Full text of "Proceedings of the Section of Sciences"

See other formats

Univ.or
Toronto
Liprary

| ey

¢e

: Onn
dp Sh rs

KONINKLIJKE AKADEMIE
VAN __WETENSCHAPPEN
-- TE AMSTERDAM =:

PROCEEDINGS OF THE
eee llON OF SCIENCES

VOLUME Xv
= 2° PART —}

JOHANNES MULLER. — AMSTERDAM
: DECEMBER 1912:

(Translated from: Verslagen van de Gewone Vergaderingen der Wis- en Natuurkundige
Afdeeling van 25 Mei 1912 tot 30 November 1912. Dl. XXI.)

dings of the Meeting of May 27

November 30 »

1912

: > > » June 29
>» > > » September 28 os
ae > » October 26 »
+73 > »

CONTENTS.

123
281
433

675

{

Digitized by the Internet Archive
in 2009 with funding from
University of Toronto

htto://www.archive.org/details/p 1 proceedingsofs 15akad

a font
t ae
i.

-KONINKLUKE AKADEMIE VAN WETENSCHAPPEN
TE AMSTERDAM,

PROCEEDINGS OF THE MEETING
of Saturday May 25, 1912.

DOGS

President: Prof. H. A. Lorentz.
Secretary: Prof. P. Zeeman.

from: Verslag van de gewone vergadering der Wis- en Natuurkundige
Afdeeling van Zaterdag 25 Mei 1912, Dl. XXI).

e. ©, Be Easy 2 S: =

fo. M. J. vAN Uven “Homogeneous linear differential equations of order two with given relation
between two particular integrals” (5th Communication). (Communicated by Prof. W.

____ Kaprern), p. 2.
i J. W. Le Hevx: “On some internal unsaturated ethers”. (Communicated by Prof. P. vax
; 2a -Romevren), p. 19.
__E. H. Biicuyer: “The a eeeatees of rubidium and potassium compounds”, II. (Communicated
° i =, by Prof. A. F- HoLLeMAn), p. 2
_ J. C. Kivrver: “On a differential equation of ScHAr i’, p. 2
TT. van Lonuizen: “Series in the spectra of Tin and Antimony”. (Communicated by Prof.
_-P. Zeeman), p. 31. (With one plate).
i. ~ Kapreyn: “New researches upon the centra of the integrals which satisfy differential
equations of the first order and the first degree” (2nd part), p. 46.
PF. A. H. ScureineMAKkErs and J. Mirrkan: “On a few oxyhaloids”, p. 52.
¢ L. S. Ornster: “Accidental deviations of density in mixtures”. (Communicated by Prof. H. A.
; LorEntz,, p. 54.
Ge VRIES: “Calculus rationum” (2nd Part). (Communicated by Prof. JAN DE Vries), p. 64.
Bs; ‘E W. Rosenserc: “Contribution to the knowledge of the development of the vertebral column

sf of man”, p. 80.

Ph. Kounystamm: “On vapour-pressure lines of binary systems with widely divergent values

“i of the vapour-pressures of the compenents.” (In connection with experiments of Mr.
Karz) (Communicated by Prof. J. D. van DER WAALS), p. 96.

Ee E. J. Brouwer: “On looping coefficients”. (Communicated by Prof. D. J. Korrewee), p. 113.

Mathematics. — “/lomogeneous linear differential equations of order
two with given relation between two particular integrals.”
By Dr. M. J. van Uven. (Communicated by Prof. W. Kapreyn).
(5% communication).

(Communicated in the meeting of April 26, 1912).

The equations (8) and (29) (see 1s* comm. p. 393 and 398) show
us in the case that the equation /’(a,y,z)—=O represents a conic
(see for the notation: 4 comm. p. 1015):

2° Az?* [ide
SS = — = CI
‘ f (n—1)?F,* g° 3
where c is put equal to 1.
From this ensues

Let us further put:
"op en a ue
we then find:

ey gS yo
[re ae
or
S
PSS 0 ee el Oe eee
: (73)
The equation (62) (see 4% comm. p. 1015) runs now as follows:
2 5 4 2 274 9 273 2
ffir 365 = 7 ae (— 4,5 A,,276° + 2a,,Az70? — a,, Az’),
or making use of the notation (59) (4% comm. p. 10083),
7 Ne ene fall 1 RG Ne ae Ieee

so $' is likewise an elliptic function of t. Its invariant has the same
value (68) as that of the function w= /? (compare (67) *) (4° comm.
p. 1006).

We can now deduce out of the equation

Aa — Ay = V-A,g? + 2Aq2-Aa,,2* = Va,,A . 2 V--AS4 4207-1 (75)
(see 4° comm. p. 1005 at the bottom)

A,,« — Ay = 22Va,,d.. Gee a Saeneend 3 (76)
‘) In the 4" comm, in the table on p. 1014 and in the enumeration of the
cases on p. 1015 >; =e? and “, =e-i¥ must be replaced by 3, = e—tt, 55 = ets,

»
WwW

ite from (73) follows

nm
~ ‘

- @,,@ + a,,y = a,,2(6°—1),. . . . . . (77)

we find with the aid of (76) and (77)

ist it a34,,) « « = (A—a,,A,,) « = A(L—i’) « =

er = = {2a,,Va,,A. C + @,,4,, 6" —=L} 2,

: (1.4 1s+%34,5) y = (A —a,,A,,) y =A (1—A’) y =

im =| —2a,,Va,,A. s + 4,,A,, (6’—1)} z.

: 7a In this way we have expressed 2 and y as functions of r with
the aid of the function ¢. It is now still our task to determine
as function of tr. Let us now put in

= — Qu? = u? — 36u? + 824 (1—A) u

(eee dth comm. p. 1016)

(78)

% u=T?=860+12,..:... . (79)
ont we flieh find

Soy EEA oN

: ee a7 oy
by applying the ordinary notation
1432? 9/7—1
eee Sane Ee 27 am i (80)

.. we then find
E v= D(T 955 9)

1
r=+6]// peinin+ >. Ri eitthe ee)

s i
eo BE sy Tal a5 eh eee ee)

Before transforming the p-function of Wetrerstrass we wish to
remind the readers that the roots of “= 0 are

i | u, = 0, u, = 18(1-+A), u, = 18 (l—A),

Ma eit’ for the roots of v= 0 (see (79)) we find

‘3 7 po eee me

eee EE ETA 6

——

We shall now investigate the relative value of these roots in the
eitincs eases LCE tA ow), IV (+1>14>0), VI @=W’)

2 (00 4th comm. p. 1014).

ee + PeOce Ws Err lkao to

1 2s
> ate % > 5? Ne Greeny

The roots are all real. Let us call them in the ordinary way in
descending order e¢,, @, @,, we then find

14-84 1 132
of Fer Oph ee ee aS pase . . ° . Gs
Case IV: +1 >1>0.

Per ie 1
Ui Te eee ar tte Be ois teat a

The roots are here, too, all real and run when arranged :
143, 1 BR

Ci == = 5Cg =e IV

Fy Lapa aa
Case VI: A=i'.
The roots v, and v, are now conjugate complex. If we follow

J
a

the notation generally assumed, we then write: .
1 143i! ey
mee. oe ae Gia ee 5 ed ae ee

When reducing the p-functions to the, elliptic functions of Jacosi
we make use of the following formulae of reduction: *)

sn(v = (eae ny) == P(t) cet dn(v) = P(t) —¢,
») Y see le Vy Sao Beaks Vagos

— = C6 €,— 6
2 3 1

Pe 0 ae eS
e 4 €,—e,

—e;, cn*(p)
sake " sn?(p) . sn2(v) . dn?(v) ‘
—Be,'+ 2V (e, —es )(¢. — ¢,)
4V/(e,'—e,)\e,'—,/)

(ts ey se4'se,') = 4! + =

y=—7) (e,'— e, \(e, — é,) ’ —

’

pr + 8e, +2V(, —e, )(e,—e,) V—%e 2’ +4(e,'—e,') (e,'—e, ')
AV (e,'—e,')(¢,'—e,)) AY (e,'—e5')(C,'—e,')
The expression for §:$ becomes in this way:
in case II

, k= —

$ V pir ) —< dn(v)

ae 39o) ¢ == = — 7

S mee 93) — 0, — = Vie oe sn(v) | P==T Ve,—e,,

in case IV

: case L\ pao pis 1
pee P(t; 9,.9,)—¢, = Ve, ee Cis 4 €, =e
$ ‘: sn(v) |

) See i i. a M. Krause: Theorie der elliptischen Funktionen (Leipzig, Tsusyer
(p. 135, 186, 147, 148).

eR eer
= get
et “- : _ ts -
sa 5
mee 2
-~
Jae VE
<u = |
¢. [A+ —e, en(v)
—_ E56; 6550, ey = * nv ;
: ie Az VB 1983) e—e5" - 4ikk' sn(v).dn(v)

V —9e,?+ 4(e,'—e,)(e,'—e,),
V (e,,—e,')(e,'—e, '’)

i ay (e,'—e,'\(e,'—e,') fo) es

or, after having expressed’ the roots ¢,, ¢; 23/1235 2 in A:
a

in case I
a:
aa dn{v) — ecu pee LE
pee) tees 2A fs ry tes
in case IV
ee fife te tae ade ak,
ae 2 Trin i ae a Shae, ~ 14a"
(83
' in case VI
P. Vis." en(v) eh V1422
ea ‘ sn(v) . dn(v) - r=] / eta
ae ot ee phe Oe
ei eo ee ae

Let us substitute these expressions in (14), we then find successively

t 1+en(r) te, 1
YA sn(v) : oe ae a

1
“in case IV &, =; Vaan en(v) + dn(r) pass

sn(v)

WA(L-Ei) dn(v) pnts.

Be ys = 5 2 == SS
aie eC Sa

Let us now choose

ree 1
P= + af / poe: on) ag

| and for $ the expressions 6, with the upper sign, we find:

ve, i
ae *
ye: ne 2

. fer
ea

ye _ Ai pease )
eT eee Ci ’ pth ’ — ey ’
+i lpe(r) ,_tieniidaly) dn(v)
a V2 a sn(v) ae nv)
f oa ee ee 1+,
Ty Sees “pre
wae ee 2A
Se ee |
Sek L+A ene) td), 11 +4) enn) dno) (\ (84)
ee Nery tay sn(v) Le De ern)
Va" cn(v) ve V1+47
sae mea Fe - 2 * sn(v).dn(v)’ Re Ve Dace
ke a a —14+V 143"
Ce BV TEER a oy ok eee
eo 4(1 +4") dn(v) rn V1I+A? en(v)
soe i’ “sn(v) | NM sn*(v)

Let us restrict ourselves to real points (2, y) of the conic, then
follows from (78) that Va,,4.§ must always be real.
Case II (in which 2 is real) appears only with the hyperbola fan
which holds A,,< 0; so we have here
Aa 0
7 ; Arey A,,
From this ensues that in case II we shall find ¢ always imaginary,
{1 + en (v)} dn (v)
sn* (vp)
Case IV is found with the hyperbola as well as with the ellipse.
As here too 4 is real we find
IVa. with the hyperbola (A,, << 0) a,,4 <9, so ¢ is imaginary or
cn (v) + dn (vr)

sn* (v)
IV+. with the ellipse (A,, >0) a,, >0, so § is real and

and therefore

is real ;

real ‘

en(v) + dn (vr)

sn® (v)

is purely imaginary.

Also case VI appears with the hyperbola as well as with the
ellipse. On account of A being purely imaginary, thus 4? negative,
holds :

Vila. for the hyperbola (A,,< 0) a,, A >0O, hence real, and

aa Ke - 7

Vib. for the ellipse (A,, > 0) a,,4 < 0, thus purely i inaemnery and
en (0)

“aly sn? (0)

From the preceding we see that » must move in its complex

_ plane on the sides of the rectangles of the net formed by the lines

. Bat purely Mea and »v = nik’ + real.

yy + Oy

_ The value of ¢* = ————— + 1 is evidently positive on
a as33

ig Beihai side of the polar line y=0O of O with respect to the conic
where O lies itself; on the other side ¢? is negative. The polar line
fg = 0 of O astes therefore the plane into two parts: in one (in
_. which O lies) §-is real, in the other ¢ is imaginary.

In the points of contact R, and R, of the tangents out of O to
ithe conic § is 0, so =o.

o>. In the points at infinity S, and S, we find that ¢ aa $ are both
infinite and / is also equal to «.

_ The diameter passing through O (A,,7—— A,,y=0) intersects the
x conic in two points 7, and 7, for which $—0, thus [=0.

a a If we substitute the expressions (84) for § and ¢ in the formulae
: a (78) we at last arrive at z and y as functions of rt.

- With a view to VA,, being real or not, we shall deal with the cases
of IV and VI separately. Farthermore we shall express 2 every where

e 1— = 7
mo. in o= Da’ thus in the anharmonic ratio of the four points

Se R,, R,, S,, S,. We shall give the formulae for « only. The expres-
sions for y we can easily find by replacing a,, in those for w by
/——@,, and A,, by <A,,.
, We then find at last:

purely imaginary.

pet J 1--en (v) ‘8

LN ie 7 ee |- (1+) Fae Mra Tila ney,
— 1—d"

es. Te |

2 1 en(v) + dn(v) oe Ay, Fe

: LVa ————— 30° me (1 +d) S47 wa % \den(v) ot d On
s ia ah
At ; ae

ay 2d i sn? (v)

e a; = 1 en(v)-+dn(v) | - —* i fd en(v) + dn |.

: __ Zen (v) w G33 ae A,,
Via a ere i + 2 cos 4 tn |,

y= ——_ , J =e! 1 og OS

w
VA cos ai

2 cn (vw A
Vib “a= | ey {eng bp wen Sion) |
t sn? (v) 2 VA,, 4° A

Fe teers eee ; d= e-#, pmilogd.

Vz cos id
2

When point (x,y) describes the conic, the variable » will deseribe
a certain curve in its complex plane. This curve we shall investigate
in the five cases mentioned above whilst at the same time we shall

indicate how the functions ¢, § and J bear themselves during that
motion.

Case Il. Point O lies in the domain of the conjugate hyperbola;
the diameter through O does not intersect the curve, i.e. the points
T, and 7, are imaginary. On the contrary the points R, , Rk, , S,, 8,
are all real.

eee : See ae ets

'»| © |purely imag. | 2iK’ Ease real 2K+2iK 2K-+p.imag 2K real

t| © | pos. real | vs pees imag. oa pos. real | 0 | pos. imag. Be
=

fa Bi | pos. imag. +5 2 pos.imag.| © “neg. imag. —5 neg. imag.|

[| wo | neg. imag. | o | neg. real © |pos.imag.| o | pos. real|

| |

Here the curves are sketched which are described by » and J in
their respective complex planes.

The points where / turns its direction of motion are arrived
at by putting /=0. We then find the values of / corresponding
to. “the roots, of #=0; these are #0, Sao, a

Bae iy) 95 4h) pea eee: Laat aol 2,

——— —_——
7

o | ‘Seu ‘dou 0 ‘Seu ‘sod co | [val “sau 00 ‘Seu ‘dou 0 ‘Beu ‘sod | @ | jwar‘sod | o | 7

co | ‘Seu ‘sod 0 ‘Seu “Sou wo ‘Seu 'sod oy ‘Seu ‘sod 0 “Seu “Sou é “Seu 'SoU| 0 2

‘ { ZA Y aacicit ; Sean a ee euines ;
o> © Jea1 ‘sod =IA+ CA ea1 ‘sod o) Seu ‘sod 0 ear ‘sod ERA [ear ‘sod Q |*seu‘sod| o 5

R, Sz
ik v-plane
Be +K Fz
Si) Be plane of
Wit amy

sn(v) YA

Ss,

Ry _tco

Fig. 1

1—i A—1 dn (v)
=F — = 61 ; the quotient assumes in those
sy 2 2 sn (v)

points successively the values 0, «, +4’, +2k. The corresponding
values of » are congruent (mod. 2K and 27K’) with A+ 74K’, 0,
K and ik’. (see fig. 1).

Case 1Va. Point O lies in the domain between the hyperbola
and the asymptotes. The points R,, R,, S,,S,, 7 and 7, are all real ;
T, and 7, lie both on the same side of the polar line of O as O
itself. We shall assume that the polar line intersects that branch on
which 7’, lies. The order of the singular points is then S,, R, , 7,, R,,
Bees y's 3

14-4 1}
ane yaiues J;=—0, 7. ig, 1 =6|/—,1=6| 7 -
1

correspond resp. to the values of 0, #, +1 and +f for

sn (vp)
thus to the values of » which are congruent (mod. 2K and 27K’)
resp. with 7K’, 0, K and K+ ik’. (see fig. 2).

— és ;
= :
~J ia ae
le ae
hs
a /. ele 11
a
* eee
.
he /
all »

v-plane

plane of

l wad. «2,
511 Mee

Fig. 2.

Case IVb. Point O lies inside the ellipse; 7’, and 7, are real,
&AR,, R,,S, and S, are imaginary.

Wwe in 7; | on 77» in 7p | on 7p7; in 7; |
;

| | ~ >

£ 0 | pos. real | 0 neg. real | 0 |

The points where the motion of J changes its sign are according
are S. 1
_ to what was found in /Va the points for which —=+ hf, thus

. sn (v)
— vw=K-+iK’ (mod. 2K and 27K’) (see fig. 3).

Fig. 3.
Case Via. Point O lies on the concave side of the hyperbola:
S,, S, 7, and T, are real, R, and #&, are imaginary. Let 7, be
the point of intersection of the diameter through O lying on the

same side of the polar line as QO itself.

p-plane
+i cnt py
S; plane of WONG
sn(v) . dn(v)
+00
5;
-toost
Fig. 4
1471 aay!
The. values. 1,370,172 == 0,1 =—=6 VA uss ty a
amd
correspond here respectively to the values 0, «, + ELT and

1—ih' en(v)
+77 To. 7 f r OF tare thus to the values of » which are
congruent (mod. 2K and A+ 7K’) with K,0, 4 (K-+37K’), 4 (K-+7K"
(see fig. 4).

Case ka Point O lies outside the ellipse; R,, R,, 7,, and T,
are real, S, and S, are imaginary. The point of intersection 7’, may
lie on acs same side of the polar line as OQ itself.

For the particular values of / and the corresponding values of
py we can refer to Via. (see fig. 5).

13
Ww —_—__
a Sie ais ea 0 wiles
+ 8 8 8 + o i
sce =—2 e
ae Bs
re s he: . ‘
ee 2 Se e 5 a ae
Y ay Eo a Ge a a S
a : re 3S ESE £ o
| Cs Pea ES -_ = = &
apiece : E
= ope 2 = wn
ro) ° x
° Qa, ° cD) ° °
so a. ae ee Ea, Ee
_- _ +
aw || SAI. |e
N | ray = oO) ianie< |
\| + it SS aR = cr
i= | we | = + |= |
—£ i] <A = | Se |
fect S| | “SN |
| fe ss | ae
fe | 3s es y e| 32% 3
FA's 7 er (SS o alte Wa RE! hee
A c. ae i= & — ome _ :
. ba . = ~ reYa) ey) on
= pea ae ee r) Sra Y
rs) x Seine ee lhe 5 2 5
8 o || 8
x Re a ~In
| a a: a =i ae ae
& = x
ue a Sor = a 28
= = = 2 v ee = 2 = e
5) = - —
as a a oe Qa. ~ =
aeoeeee Sal ee
| =)
ag \
Te 25 cx || SAI
Hee Ne cm co ! vu | o- 6
SE: | (peas = lj
| NE eA
== |
] + —— -- S
= — — —— — on — y
ES s s K ceo
_ a hh aoa ae = Set 2 ee
¥) o : : « P< arts tae
pee the oko OD: kl an nM
i=] ro) =
° a = & hed vi meetin
8 =) || Res |
_—= . ~ IAN
A a ie = pe:
c 8 8 | aS a i 8
4 = ae
= a SST a NT: ~ = > See ~
= >

| — ee : =

Before investigating the cases of degeneration III] and V we shall
occupy ourselves for a moment with the relation (53) (4 comm. p. 1011),
existing between / and /*. In the case of the conic it takes the
shape of (65) (4 comm. p. 1018). The curve it represents is as
can be expected symmetrical with respect to the X-axis (X = /’).
To simplify the reasoning we shall translate the curve ® (X,Y) =
® (J?, /)=0 parallel to the X-axis and we shall decrease it and
that by the formulae of transformation

-plane tle 1 f en(v)
»P cise gy aie sn(v) . dn(v)

I? — 18 = 36,
_— 67.
The equation of the curve transformed in this manner runs as
follows :
72
CASS Wine ragea

the curve is therefore a rectangular hyperbola. In the cases II and
IV the §-axis is the real axis, in case VI the y-axis is the real axis.
Each point of the conic /’(v, y) =O corresponds to one point of this
rectangular hyperbola whilst to one point of ®=0O two points of
#=0O are conjugated. The points for which /—0O have as absciss
§ — — 4. The line § = — } does not intersect the curve ® in case
II, but it does in the cases IV and VI. The point at infinity on
§ + 2,=0 represents the points S, and S,; the point at infinity on
5 — 7 = 0 represents the two points R, and R,. The points 7’ and
7’, are represented by the points of intersection of ®=0 with

§ = — }. The images of the points 7, and 7, are in case VI united
in the point of intersection of §= — 4 with the branch of ®=0

lying under the §-axis. The images of 7, and 7, are always points
where the motion changes its sign along the curve ®,

Now we have to investigate the cases of degeneration.

Case III. h=-41, J, =9, a,, and a,, not disappearing at the
same tune.

The point O lies on one of the asymptotes, without coinciding
with the centre. So this position occurs with the hyperbola only.

Here equation (71) bolds, in which is put tr, = 0,

Pe EE eee ee

Equation (62) (4" comm. p. 1015) passes, on account of the relation

(1 Pe: lipeet

and with the aid of (72), into

9 9 (¢? —1)3
BE eg tox ye OR
S Re
from which ensues, in connection with (71),
6 3i (C71
sin T B
or
t(l4 cost
sin T
We choose for ¢
. _l— cost Hy
Gr =. 2 ——=-+ttg—, ... .». « (85)
sin T 2 :
and find in this manner
1 ©
C= + — sec? ape

Now the equations (76) and Be are incompatible. If they depended
on each other we should have A,, =O, which has not been sup-
posed to be the case. .

Equation (77) now runs:

Ay,@ + G,,Y = — Gy,2 sec”

(86)

Bringing this equation into connection with / (zx, y, 2) = 0, we find

T T T
2A,, sec? — .a = {a,,a,, sec* — —a,,”|{ 2 sec? — —1
S 2 y)
T t
9 f Pari4 — aap win oe 2 ———s
2A,, sec 5 + Y = 341105, sec" — aie ee sec” 1)} i
-_

These formulae can be used unless either fh or A,, is zero.
Therefore we will mention also the expressions for « and y for the
gase. A. =; Then we have a,,= 0. on account of a;,A,, +
+ a,,4,,—=90. We then find immediately out of (86) the expression
for x, out of the second equation (87) in which A,, is replaced by
a,,4,, the expression for y. So the solution is:

nee - ,
GQ, == — d,,2 - sec

2 t 4 be 3 9 2 . i
20,40;, sec rat a A, 1,43, SEC mo. ayy 5éC my = =
-_ =

Case 111°, a,,=
The point O coincides with the centre.

Now we have
I= 0.

The expressions for « and y are of the form:
xz — (ae + ale—*)z,
y = (Be + Bem) z.
In order to have F = a,,«? + 2a,,ey + a,,y? + @,,2° = 0, we must put:
ao (—a,,+V—A,;), a’ = oO (—a,,—VY— A;;);
B = 6a,, ’ > —e6a,
with the condition

In the case of the real ellipse we have A,, >0 and —22 Sod) ayes
a

11
then can put:

Mas pha i — a3 x
2 a,,A;,
So we find
1 — : : j :
£m — Seve : {— ix (e* te—it)t iV A,,-(e" —-e—i7)} ——
2 a,,A,,

=| 2 (a, eon — Ay sin) ‘ (88)
a,,Ayg,

1 a, 4,143,
— __ we 4. It = ey WIRE GO
y : Vlews “a etna ve i Be vs

We can use the same expression if we have to deal with a

hyperbola not intersecting the z-axis. For then A,,< 0 and >0,

so o=o' real. We prefer to write —/—A,, . sh (it) for Vs sint
=—ip-A,,.sint and ch (it) cos fort. Then real points of the hyperbola
correspond to purely imaginary values of tr.

If the hyperbola does intersect the z-axis we have A,, << 0 and

a . :
<0, so =o’ imaginary.

a),

We then put s= —o = —

2 “and get in this manner
my a,,A,,

1 ay : : : 5 \ a
eK tea 0) $V Ay bee |
(88)'

= ae {— a,, sh(it) + VA,, ch(iz)} z,

1 ta As, . . 4,143
y= — ——— .a,, (e* —e-") ze = Var . sh(it) . 2
2 a,,A,, As,

Here also r must describe in its complex plane the imaginary axis.
For a,,=0, we get (2a,,7+a,,7) y + a,, = 0.
A solution of this is given by

—1]

9
ad, 9

i —

(a, ,¢'* + a,,e—**),

= er,

Here also only purely imaginary values of r come in consideration,
as might be expected.

The second case of degeneration (IV) presents itself for 2— 0,
i. e. J, = +1. Here we must distinguish three subdivisional cases, viz.

IV“. a,, =9: the point O lies on the conie,

LV. A,,; =O90: the conie is. a parabola,

IV¢. a,, =0 and A,, =O: the point O lies on the parabola.

Case 1 V«. Here we have (70a) (4 comm. p. 1017); substitution
of tr, = 0 furnishes

T= + 3y2.th 7, noite: Tener ee a e
so
é 3
——
pitee
V2

Now the equations (62) and (63) (4t* comm. p. 1015) teach us

RTE IN 1
C0 ee Cry ; = -

3A, Jae j2
ch? ——
2
2aei 4 f\? 1 4 L\? 1
AeA, yy =V —Ayag FRO g2 =|“ See fe eS
Jai f hs T Ay h? T
Cc V2 c 7)
] e
2Az wave:
7 cme
ope
2
sO we get
22 x \)
v= <p A,,+4,,; VA,, ° sh v2
A, ,ch?——
V2
(89)
< az A iad F t
—— ae 4153 — 3 es ae
A, ,ch?—
V2 j
2

Proceedings Royal Acad. Amsterdam. Vol. XV.

18 -
=:

In the case A,, <0 we prefer to write 71V — A;, a, —

and cos — for ch —

—+Y— Ay, sin 7 for VA,, ot hes WE a a

whilst the formulae (89) are specially suitable for the ellipse

So,
we do better in using for the hyperbola

a
a = (At 131 Tog — pa ° sin ns)

has cos /6
s \
2
y —= ——. (4— a1; V —Asz, - sin ol
: iv 2
ay. cos” 5 V.
Vs |

Consequently the real points of the hyperbola correspond to purely

imaginary values of T.

Case [V*. Putting tr, = 0, (700) as comm. p. LO17) we find

j ee st oe a (70'b)
and therefore
——
t
ch?—=
V2
So the formulae (62) and (63) now give
D442 Gy, tf
g=a4,,¢ + a,,y +.4,,2= = i =F ch? ya"
1.e.
Qant
i a me “(a Vi — 2)
and
A,,« -A,,y = V 2Agz—a;,,2 —Va,,A
so we find
Aes Va,,A T Gagln t ;
pee | A 5 sh 2 + eer G V2m 2| 7
(90)

ress : T 4 GaAs J T 9
p= ‘ sh ———| ch? —~ — .
7 A Yo" 2A \ 2 ) |

Case 1V¢. Here we have 4
T= +342

The equation
P= a7,2" + 2a, ,y 1

a 2

13 2 '
y* + 2a,,¢ + 2a,,y = 0
ai,

or
(4,,7+4,,4)° + 2a,,(4,,7+4,,y) = 0

passes by the substitution

a,,% + 4,4 = 2a,,5 (91)
a,,0 + a,,y = — 2a,,4
into
y=S,
a solution of which (see 2"? comm. p. 590) is
5 —<V2
G7 gar 2 : "= é (92)
Out of (91) and (92) we deduce
2a = é
= — (ane v24-a,e s
13
(93)

2 Se aS
— (aus v2 +1 a,,e |

These formulae are always applicable, as the supposition A,, = 0
would imply the degeneration of the parabola.

Chemistry. — “On some internal unsaturated ethers’. By J. W.
LE Hevx. (communicated by Prof. van Rompurex).

(Preliminary communication).
(Communicated in the meeting of April 26, 1912).

By the action of formic acid on mannitol Fauconnrer obtained a
‘mixture of formic esters of this hexavalent alcohol, which submitted
to dry distillation, yielded among other products a liquid of the
composition C,H,O, boiling at 107°—109".

Van Maanen (Dissertation, Utrecht 1909) who investigated this
“substance and mentions it as a liquid boiling at 107° proposed as
the most probable structural formula :

CH,—CH—CH—CH=CH—CH,
Sy

As the mode of formation of this substance does not give acom-

plete insight into its structural formula, Prof. van RomBurGs proposed to

me to prepare the various possible oxides of hexadiene by other
2*

methods which show more satisfactorily the progressive change of
the reactions, and thus to find out the real structure of the sub-
stance prepared by FAuconninr.

As starting material was used the doubly unsaturated glycol
CH, =CH—CHOH—CHOH— CH=CH,, which Griner prepared by
reduction of acrylaldehyde, divinylglycol.

Advantage was taken of the property of acetyl chloride to act on
divalent aleohols in such a manner, that of the two alcohol-groups
the one is converted into the hydrochloric, the other into the acetic
ester.

The reaction product of acetyl chloride on divinylglycol is obtained
as a colourless liquid, which after repeated fractionation under a
pressure of 18 mM. boils at 84°—88°. I have not yet obtained it
in a perfectly pure state as the chlorine content was found a little
too high. On keeping, the liquid darkens after a few days and then
shows an acid reaction.

In order to prepare the oxide from the chloroacetine it was shaken
for some time with strong aqueous sodium hydroxide and then dis-
tilled under reduced pressure (to prevent as much as possible, poly-
merisation). Of the distillate, which consists of two layers, the upper
one is again distilled a few times over sodium hydroxide and finally
over finely divided calcium in an atmosphere of hydrogen in order
to obtain the product completely free from halogen and water.

The so prepared divinylethylene oxide

_CH,=CH—CH—CH—CH=CH,
MA
QO

is a very mobile, colourless liquid, boiling at the ordinary pressure
at 108°—109°, with a very pungent odour characteristic of allyl
compounds,

mine = 144942. di. = 0,8834.

Once obtained in a pure state the oxide is permanent and only turns
pale yellow on long keeping; under the influence of alkalis it resini-
fies when in contact with the air. When brought into contact with
hydrogen chloride, this is absorbed immediately ; on warming with
water, divinylglycol is regenerated.

The ring —C—C— is also opened comparatively easily by

Q)
aunines.
For, if divinylethylene is heated with allylamine for a few hours

a4 compound is formed of 1 mol. of oxide and 1 mol. allylamine.
By distillation and recrystallisation from petroleum ether, | obtained
white needles melting at 37,5°. The oxide when heated with am-
monia also gave a crystallised amino-aleohol.

Another method often applied to arrive at internal ethers consists
in addition of hypochlorous acid to an unsaturated hydrocarbon and
subsequent elimination of hydrogen chloride from the chlorhydrine
formed. Before applying this method to hexatriene which micht yield
an oxide of the formula C,H,O, I first tried the action of this acid
ou a hydrocarbon with only one conjugated system of double bonds.

CH,
The hydrocarbon Pe ton. isoprene, which is now
| rey ae ke ae:
readily prepared in a pure condition by means of the so-called
Harries isoprene lamp, was cooled in ice-water and shaken in the
dark with a solution of hypochlorous acid in such proportion that
1 mol. of acid was used for 1 mol. of isoprene.

The hypochlorous acid disappears spontaneously and the isoprene
dissolves. After saturation of the liquid with common salt, ether
extracts from this solution a compound boiling at 142°—145°, the
chlorine content of which points to its having the composition
C,H,OCI. By removing from this compound hydrogen chloride by
means of strong aqueous potassium hydroxide, I obtained a liqnid
with an ethereal odour b.p. 80’—82° which, however, still contained
a trace of halogen.

Brought into contact with hydrogen chloride the latter is at once
absorbed ; when dissolved in carbon tetrachloride, the substance
decolorises, although slowly, a solution of bromine.

“If now we consider to which position in the isoprene molecule
the HOCI can be attached the three following possibilities may occur.
1. The hypochlorous acid is attached to the double bond 1=2.

2. The hypochlorous acid is attached to the double bond 34.
3. or, because the two double bonds are in conjunction, the linking
has taken place at the carbon atoms 1 and 4 with the appearance of
a new double bond between the carbon atoms 2 and 3. In the latter
ease a 5-ring would, probably, have been produced from the chlor-
hydrine thus formed, namely a methyldihydrofurane. The ready
absorption of hydrogen chloride does not, however, support the latter
view.

I hope to be soon able to make further communication on this
subject with which I am still occupied.

Utrecht, April 1912. Org. Chem. Lab. University.

Chemistry. — “The radioactivity of rubidium and potassium com-
pounds.” Il. By Dr. E. H. Bicaner. (Communicated by Prof.

A. F. HoLlEeMan).
(Communicated in the meeting of April 26, 1912).

Some time ago I described a series of experiments undertaken with
the object of demonstrating .the radioactivity of rubidium and even-
tually of other alkali metals by the photographic method *). I then
only noticed an action on the sensitive plate with rubidium sulphate ;
the salts of other alkalis produced no effect. I have repeated these
experiments and, as announced previously, I have inquired more in.
particular, whether the phenomenon might be attributable to a
previous exposure of the salt to the light; in that case there can
be no question of a real radioactivity, but we should have here
an analogism of the wellknown experiments with calcium sulphide.
According to NrEWENGLOwsKI, this substance acts on a photugraphic
plate by means of rays which penetrate through aluminium, but
only when it has been previously exposed to the light. In the
present meaning of the word we cannot call calcium sulphide
radioactive, because an external influence is at work; if the same
happened with rubidium and potassium, these substances could neither
be included among the radioactive ones. And because they differ in
various respects from the other active substances, there is still some
doubt left about this matter. It was, therefore, desirable to carry
out some experiments in this direction.

For this purpose I have exposed, simultaneously, in one box, some
photographic plates to the action of RbCI, RbNO, and Rb,SO, in.
the manner described previously, but of each salt two specimens
were taken; one of these had been kept in complete darkness from
4 to 5 months, the other had been exposed to broad daylight for
some days previous to the experiment. When developing after 90
days, no difference was found between the action of the two
specimens, both having affected the plates in the same manner. Hence,
it again becomes more probable that we are dealing here indeed
with true radioactivity. ;

For the rest I have been able to confirm my previous results. Again,
I have not succeeded in geting an action on the sensitive plate
either with salts of potassium or with salts of caesium, sodium, and
lithium, but on the other hand rubidium did affect the plate. With
RbCl and RbNO,, also with Rb,SO, I found that the plate had

1) These Proc. 1909, p. 154.

darkened distinctly on those spots, where little holes or figures had
been cut in the sereen of copper foil which had been placed between
the salt and ihe plate. The action is strongest with the chloride and
weakest with ihe sulphate. I attribute this io the greater absorption
which the rays undergo in the sulphate itself, for this salt has a
higher density than the chloride and, therefore may be expected to
show a greater absorption. This explanation can also serve for a
few deviating results. In two experiments, it appeared that Rb,SO,
had produced no effect; now in these cases the salt had accidentally
been used in the form of fairly Jarge crystals and not in powder, as
usual. The surface of the powder is, of course, larger and conse-
quently more rays will reach the plate than in the case where
erystals are employed. Perhaps, this reasoning may explain also the
results of Srrone*) who, in the exposure of different potassium salts
to photographic plates, observed effects of very varying intensity ;
for instance strong action with potassiumeyanide and_ practically
none with the urate.

The rubidium salts investigated by me were obtained from difle-
rent dealers (Merck, Kauispaum, Dr Harn, Scuucnarpt): the fact
that they show no difference in action goes to prove that the phe-
nomenon must be attributed really to rubidium and not to some
impurity.

2. Other investigators have already shown that the radiation of
potassium and rubidium consists mainly, probably even exclusively,
of p-rays. Now, e-rays may, however, elude observation sometimes,
as they act but faintly on sensitive plates and consequently practically
not at all with slightly active substances. Moreover when we are
dealing with «-particles of very small velocity and corresponding small
penetrating power, only an exceedingly small portion of the «-parti-
cles will arrive in the surrounding gas and the ionisation current,
generated by them, which is measured with the electroscope, will
be very weak; it may even be of little importance in regard to the
eurrent caused by. the #-rays. If now we may apply the results
obtained with strongly active substances to feebly active compounds,
the a-rays, if present here, may be expected to possess a slight
velocity, since we may assume as a rule: the larger the activity of
a substance, the greater the velocity of the «-particles. A possible
occurrence of a-rays demands an investigation all the more, because

‘the absorption of the radiation in different substances, like tin foil

1) Amer. Chem. Journ. 42, 127.

for instance, cannot be represented by a simple exponential formula;
on the contrary, it seems as if the radiation is composed of a part
decidedly penetrating and of another one less so; the latter is then
only of slight importance.

In two ways, I have attacked the problem of the presence of
«-rays; firstly by observing whether zine sulphide became luminous
andér the influence of the salts. This method has the advantage that
we can bring together the salt and the zine sulphide as closely as
we like, and reduce as far as possible the absorption which the ea-
particles undergo in the air; consequently we may, perhaps, find in
this manner a-rays of very slight penetrating power which would
not be detected by other means.

We know that light emitted under the influence of a-particles
possesses a peculiar character and that, when examined under the
microscope, it breaks up into numerous points which are formed
at the spots, where the a@-particles meet the zine sulphide; each
scintillation, therefore, indicates an a«-particle. In order to show the a-
particles eventually present, an object-slide with a little KCl was put
under the microscope; above it at a distance of about 2 m.m. was
placed another slide which was coated at its lower surface, by means
of Canada balsam, with a layer of zinc sulphide. The whole arrange-
ment is placed in the dark; it is, however, advisable, in imitation
of Recener, to faintly illuminate a portion of the field of vision (for
which purpose a “‘VERKADE waxine’”’ light is very serviceable) in order
to facilitate the adjustment. In this manner, we can readily show
‘the a-particles of pitchblende, uranium oxide, and thorium oxide ; we
shall be able to observe also all «-particles which can traverse a
distance of at least 2 m.m. in the air. Neither with KCl, nor with
RbCl, however, any scintillation was noticed in different experiments,
though the observation lasted each time ten minutes. I then made
the experiment in another way: to render the distance between the
salt and the zine sulphide as small as possible, I mixed the two
compounds. But even then I did not succeed -in observing a single
flash of light. These experiments thus confirm the results communi-
cated by Hxnriot*) in a paper which appeared after my experiments
were closed, namely that rubidium and potassium do not emit a-rays.

3. There is yet another way to demonstrate the emission of a-
particles. It is well known that the heat generated by radium and
other radioactive substances originates in the kinetic energy of the
a-particles, which are stopped in the surrounding matter. A large

1) Comptes Rendus, 152, 1884 (1911).

portion of the a-rays gets already absorbed in the emitting substance,
because they penetrate into solid matter but a few hundredths of a
m.m.; consequently the active substance is heated above the tempe-
rature of the surrounding air and, of course, remains warmer, because
the radiation process proceeds continuously. «-Particles which do
not possess a sufficient velocity to ionise gases, or to render the
zinc sulphide luminous, may still have a considerable kinetic enerey :
and when they are absorbed, their energy being converted into heat,
they might raise the salt from which they originate to a higher
temperature. This argument has also been applied by GREINACHER ?
during an investigation on the radioactivity of several ordinary
substances; he, however, did not study the salts which are now of
particular interest to us.

I have investigated this question by placing in a large galvanised
iron basin, on pieces of cork, two silvered vacuum flasks of about
1’/, litre capacity. The basin was placed in another and the
space between was filled with ice; the whole was placed in a
wooden box isolated by means of slag-wool. A third bath serves as
a cover, which was also filled with ice and covered with blankets.
In this manner, the flasks are entirely surrounded by ice, and it
may be assumed that the surrounding air possesses a constant tem-
perature. Every two days, the accumulated water is drawn off and
fresh ice is added. The flasks are filled with about 2 kilogrammes
of potassium or sodium chloride respectively, and closed with a
solid plug of cotton-wool, upon which is poured a layer of paraffin.
Through this seal penetrates a very thin-walled glass tube which
reaches to the centre of the bulb and contains one of the junctions
of a thermo-couple copper-constantan. The constantan wire con-
nects directly the junctions, the copper wires are carried away
through an opening in the box and connected to the galvanometer
which is suspended according to Jutivs and read off by means of a
mirror and a telescope.

If now potassium chloride emits «@-rays, it may be expected to
reach a higher temperature than sodium chloride and, owing to a
thermoelectric force the galvanometer will deviate; by gauging with
a definite difference in temperature it may be found with how many
degrees corresponds a deviation of, say, 1 mm.; this proved to be
0.003°. As soon as the circuit is closed a deviation of the galvano-
meter is observed, but without further discussion we may not con-
clude to a difference in temperature between the two salts. There
are, necessarily, always some places of contact between different

') Ann. der Phys. [4] 24, 79 (1907).

metals which, perhaps, have not exactly the same temperature and
therefore also yield a thermo-current. This influence may be elimi-
nated by placing between the galvanometer and the thermoelement
a commutator; on commuting, only that part of the current which
has to be measured, namely the current of the thermoelement itself,
takes another direction ; it may, therefore, be determined from the
difference. Only care must be taken that no differences in tempera-
ture occur in the commutator itself. As such served two three-limbed
glass tubes well wrapped up in cotton-wool and placed in a little
box, which was suspended and moveable round a horizontal axis.
In both tubes was poured a little mereury, while in each of the
limbs were introduced wires which effected communication with the
galvanometer and the thermoelement, respectively. By inclining the
box to 45° in any direction, the current is closed, but this, in both
cases, passes through the galvanometer in a different direction. There
is still another source of error due to the thermoelement itself whose
wires are often not quite homogeneous; and if there should be no
equal temperature over their whole length, a thermo-current may be
generated. Althongh these irregularities seem to occur but rarely.
with copper wires (and only these were here at different tempera-
tures), care was taken al! the same that they should not influence
the final result, by changing the junctions in the two flasks after
a series of measurements.

We then must take again the difference of the resulting figures:
of different series to obtain the thermo-electric force of the copper-
constantan and to calculate thence. the- difference in temperature
between the potassium and sodium. chloride. I refrain from giving -
a detailed communication of the results. of the measurements because,
anyhow, my conclusion must be that the two salts do not show a
difference in temperature, at least none exceeding 0,001°. As I look
upon this figure as representing the accuracy attained, I do not
attach any importance to the fact that the final result showed sodium
chloride to be about 0.001° warmer than potassium chloride. Four
experiments were carried out, the junctions of the thermoelement
being changed after each; an experiment consisted of five to six
measurements which were each composed of three to seven readings,
carried out one after another with continuous commutation.

_ From these experiments also, I must conclude to the absence of
a-rays in potassium compounds; this result did not afford reason to
make also an experiment with rubidium chloride.

My best thanks are due to Dr. A. H. W. Aren, who placed his
galvanometer at my disposal for these experiments:

Inorg. Chem. Laboratory University of Amsterdam.

Mathematics. — “Qn a dijjerential equation of Scuuivi.” By
Prof. J. C. Kiuyver.

As a suitable example of the method of solution due to Prarr
ScaiArit has determined the general integral of the equation

a, (%,P3;—5p,)° ae a, (7,P,—2,p,)’ =| Gs (v, p,- —#,p,)* <7
(Annali di matematica pura ed applicata, serie 2, t. II, p. 89-—96
and in his Theorie der partiellen Differentialgleichungen Mansion
has repeated the calculation of Scaiari. As Mansion remarks this
treatment of the equation does not allow to maintain the symmetry
with respect to the variables; therefore we will show in the fol-
lowing lines that it is possible to obtain the complete integral of
the equation with preservation of the symmetry by means of Jacosi’s
method.

By putting
&oP3 — &.P, = A,,
GsP ie HPs — A,,
Camere ta A,
the given equation passes into
f= AY aA, + aA? — 10.
The system of simultaneous differential equations to be considered
here becomes
da, dp,

xi a,p,A4,—a,p,A, fi
One derives from it immediately
dix, dA, tf A OAL, Se

ele

Sea — We Cth | a” |, 0.8) O

a,v,A,—a,v,A,

“ee ¢ ©

a,v,A,—a,x,A, ~~ (a,—a,) A,A, es = 0 i 0
This furnishes two integral equations
Si =p, “i s&s z% Ps —m* = 0,
ne AS Ae = 0.
The two functions f, and /, are in involution. For we have
[47,p7]=9, [A.*,p.7]=4Aip.ps [A,"p."] = — 4 AiPaPrs-
From this ensues
-[A;?, Sp;7] = 0
and furthermore also
[As Sf] = 9-
So one has to solve the partial derivatives p,, p., p, out of the
three equations
ee), = OF Fr, ==. 0
and to integrate afterwards the differential equation
dz = 2p, dz,.
A direct solution of p,, p,, p, cannot be given. Therefore we

remark that the three quantities A,, A,, A, are entirely determined
as functions of z,,2,,2, by the three equations
BAAS, BO AN, tA == 0
and now We express 7,; Ps, Ps iN 2, €, 23, Ay, Ay, As.
So by eliminating p, and p, out of the equations

«,p, — &p, —A,,

LP, — &sPy —=A,,

Pi + Ps + ps Sm
we find that p, is determined by the equation

pat 2 (Age Ae) — ee A,

from which follows after some reduction

ee At Pen te ; Se ae ae Seay
p= : | Asn A,«, + aVm S«,°—k*}).

aa
1
We find for p, and p, similar expressions; by putting
eae,
we get the total differential equation
de, dw, dz,|

di Lik eres
An A. | a Vine
u

Biba
In order to transform the differential
\dve, da, da,|
i
qi | AA
u? |
w, &,
we consider three functions §,, §,, §, of A,, A,, A;, satisfying the

condition ‘
ZAC = 0,

but otherwise arbitrary.
Putting moreover

Lp (4,§,— Ass); Us (A,5,—A4,&;), q; —- (A,§,—4,§,):
te 5. S|
4 = | un UE: Vs ’
AAS eae
we get

SE, = 0, (SAS AS SS ae
We still introduce two quantities U7 and V determined by the
equations
Ze. §, =U, at,
By adding to these the equation

Sie AL
ait Ara By,

“*

and solving 2,, z,, 2, out of them we find
men Us, Vy, oA Ue, + Vn,, 2, A= khUE, + Vn;
‘from which ensues immediately
a =a 2 (U°?k?+ V?),
A
and also
Ao ds, = 4 Udh + V4, ds,
A2z,dy, = — kh U7,d§, + 4 Vdd,
A (V2a,ds,— UL z2,dy,} = (U7? + V*) Sy, dé, .
The reduction of the differential dH now takes place as follows,
We have

pasvderdms|-(6- 6, &, | =§,de, 2y,dx, LSA,dz,
P| | | | iis
dH#=—\A, A, A,|.\", 1% %|=—-| 0 0
N | 1 2 3 | | li M2 "Ns | IN k
pate swe be AA. | U ¥ 0

and therefore
ka dd a a6. dV—Zx,dy,

SS
; wu? | LeU, ie
k?(VdU— UdV) ke? ate
dH = -—— PL? aEVs = 1,45, »

so finally
| a, d&, dé, |
Z 1

ES ae Bt SEs Se) 8 is See Se
Sata tea]

The second term of the righthand member corresponds in form
entirely to the original form dH; however the independent variables
#,,2,,2, are replaced now by &,,&,,§,, functions of A,, A,, A,.

On account of the equations

Ae ee os SG A,
we may consider A,,A,,A, as functions of one variable ¢ only,
which implies that also §,, &,,§, appear as functions of that variable
t, whilst this variable itself is determined by the equation
SA 0)
as a function of 2,, 2,, 2.
Substituting the expression found for dH we now find

| dg, dé, dg,
|
|

ae ake air Sa aes
dz = kd tang— Th +. 5B: RAW. Pag le Vm u?—k

and

; S2,(A,§,—A,8,) Be iti ap
24+ C=k tang =— = - +f = dt +-

k 22,6, aie: Ae taA. A,

5. §: §:

+ Ym? S02?—k? + k sin— :
wy Pes
mV Sa?

So a solution of the given differential equation containing three
constants of integration C, m, k has been obtained; we can now
stil! investigate in what manner this solution can be transformed
by means of a suitable choice of the functions §,, §,,§, into the
most simple form.

The only condition §,,§,,§, have to satisfy is

S45, =—0.
So we may put
§, =Ai@e@=1y fe, = Ao) 3 6 Ae
or
5, = Ab, ’ Ss, = A,b, ’ §,= A,b,
The equations

can be replaced by
2438, SSA seo
_ and these two are satisfied by putting
A, = A =
V'(b,-b,)(t-+6,6,) V(6,-b,)(¢-+856,)
ka A ay k
V(b,-b,)(t+- 6,6.) V-(b,-b,)(b,-b,)(6,-B,)
where ¢ is supposed to be determined by the equation
Sx, V(b,—b,)(t+b,6,) = 0.
By eliminating A,, A,, A,,§,,&,&, out of the solution found above
we get finally

dt
s+ O=-Hyh,b, J. ee — ee
VAC bb \(E+ 50,450.)
Sa,V—(b,-b,) (++0,0,) (40. stot ned ASA s
-ktang—}. a ( = 3) (rhs) + V m? dw ?-k*? + ksin—! uA
2x, b V (b,-b,) (t+b,b,) m a2,"
By this the differential equation is solved and in this solution the
symmetry with respect to the independent variables is preserved.

Te ee
*

31
Physics. — “Series in the spectra of Tim and Antimony’. By T.
vAN Lonuizen. (Communicated by Prof. P. Zeman).

(Communicated in the meeting of April, 26 1912),

In my Thesis for the Doctorate, which will shortly appear, I have
used a spectral formula, which expresses this fundamental thought:
“For every series the curve obtained by using the parameters (1, 2,
3, etc.) as abscissae and the reciprocal values of the wave-lengths
as ordinates, is exactly the same, only referring to another system of
axes’. This curve is the curve of the third degree :

im which y= 1!0°A—!, « is successively: 1, 2, 3 etc., and N is
the universal constant which occurs in the formulae of Rypsere,
Ritz, and Mocenporrr—Hicks, the universality of which, somewhat
more intelligible after the physical meaning which Rtrz*) has given
to it, can hardly be doubted any more. Transferred to one and the same
system of axes the general spectral formula becomes for all series :
ne eee ey
3 [(w—a) cos y—b siny—10° A—! sin y}?

in which a and 0& are the ordinates of the origin of the original
system of axes, and y the angle of rotation. As I shall demonstrate
more at length in my Thesis, the formula may be reduced to:

108 A-! = 6 — —_________
[e+ a'+c)—1/

for small values of y.

This approximated form closely resembles Rirz’s formuia, which
may; therefore, be considered as an approximation of the one given
by me. Also the formulae of RypBerG (c =O) and of Baumer for
the hydrogen series (a =O and c=O) are implied in it as special
cases. Accordingly it is also further closely related to the original

_ formula of Ryppere. This, too, expresses that the curve is the same
for all series, but the important difference is that RypBerG gives the
system of axes only a translation, whereas according to my formula
there generally appears a — mostly small — rotation of the curve.
- The thought of one curve for all series has been embodied in a
model which I have had constructed for this purpose, aud which
contains the most important part of the curve:

3) Magnetische Atomieider und Serienspektren. Ann. d. Phys. 25 p, 660 et seq. 1908.

109675.0

a ae a?

and also the axes of the system to which it refers. By a fine divi-
sion with vernier it is possible to determine the first four figures of
the oscillation frequencies expressed in five figures (10° A—!, A expres-
sed in AU).

[t deserves notice that also RypBerG has designed his curve by
means of one model. He says‘): ‘Toutes les courbes ont éte tirees
a l’aide du méme calibre’.

This model has proved to be a great help in detecting new
series for elements for which no series had been observed up to now.
For this investigation I have first chosen the spectra of those ele-
ments for which Kaysgkr and Ronee’) had found ‘eine andere Art
der Gesetzmassigkeit”. Kayser points out already there that when
we pass from one MENDELEJEFF group to the next, the series move
to the region of the small wave-lengths. He says’): ‘Es ist also recht
cut modglich, dass fiir weitere Elemente, die Serien im unzugang-
lichen Gebiet der Schumannschen Strahlen liegen’’.

From what I have found, the results of which for Z%n and Anti-
mony I communicate here (I hope to publish the results for the
other three elements Pb, As, and Bi later) I think 1 may infer
that in general this conclusion is correct, but that the beginning of
a great number of series is found in the already investigated region.

Whereas for the other elements the finding of series was facilitated,
because the parts where the lines converge, had been observed, while
later the first terms were added by the discoveries of PAscaen and
others in the ultra red, exactly the opposite takes place for the
elements considered here. The initial terms have been observed, and
they lie together of all kinds of series; the part where the series
begin to converge clearly lies outside the region of observation. So
the difficulty was to accomplish the discovery of the series from the
few terms that have only been observed of most of these series.
Only very few observations on the Zepman-effect for Tin and Antimony
have been made, so that at present they do not yet afford sufficient
data for the finding of series. It would be desirable that investigations
for these elements on the magnetical splitting up of the spectral
lines lying more in the ultra violet were carried out. They might
throw more light on the series found by me. So as these data were

') Kon. Svensk Vetensk. Akad. Hand. Vol. 23 p. 152. 1890.

*) Ueber die Spektren der Elemente VII. Abh. Berl. Akad. 1894. Cf. also
Kayser. Handbuch der Spektroskopie. Vol. lI, p. 578 et seq.

§) l..c. p. 578.

not at my disposal, I have tried to find the series by means of my
mudel, somewhat led by the estimations of the intensity given by
Exner and Hascuex’). As these authors give widely divergent and contra-
dictory differences from those of Kayser and Runge”), I have thoueht
that 1 ought to prefer the former, because they extend over the
whole of the spectrum observed by them.

The obtained results follow.

I must not omit mentioning that besides the said estimations of
the intensity, also the constant frequency differences found by Kayser
and Runeg *) have furnished a first basis for my investigation.

In the spectrum of Zim I have found a series which is represented
by the formula :

109675.0

10° A—1 = 45307.40 — i dhs bal eehh onl 3
(a + 1,651360 — 657,42 A—!)

mea eo.
the results of which are:

ci | jars dy Aw—p | al | Intensity
SS pp lL. lll a a

1 | 3655.92) | 3655.92 0 0.03 | §

2 |, 2185.14 | 2785.14 | 0 | 0.03 3

3 |) 2524.05 | 2524.08 | 0 0.05 !

4 +, 2408.27 | 2408.71 —0.44 a |

No more terms have been observed of this series, which need not
astonish us, if we consider that in their tables Exner and HaAscurK
indicate by 1 the lines of the least intensity, and that therefore the
following lines have probably been too faint. Now this four-term
series would have little conclusive foree, if it was not in con-
nection with other series, which I have ealled Translation series in
my Thesis for the doctorate, because they are obtained by a pure
y-translation of the curve, and so only differ in their asymptotes.
Such translation series are easily shown, as I have proved there, in
the spectra in which series are known. By a translation 5187.03
(one of the two differences of frequency discovered by Kaysrr and

1) Die Spektren der Elemente bei normalem Druck, II, p. 232 and 235.
By les:
8) l. c.

_ 4) Exner and Hascuex, |. c.

Proceedings Royal Acad. Amsterdam. Vol. XY.

2uNGE), we get a series with the formula :
109675.0

10° 2—1 = '50494,43 —
Kis ¥ (@ + 1.651360 — 657.42 4-1)?

ae Nee
So the series differs from the others only in its asymptote.
find the following lines :

: x | dy 1b | sp Lint | Intensity
4 aoe | 3073.15 | rons | Bs | i
2 | 2433.581) | 2433.57 40.01 0.03 | 1
3 | 2931.80 | 2231.80 | 0 | oso |b <=
4 | 2141.1 | 2141.19 | —0.09 | 0.20 | =
5 | 2001.7 | 2002.30 | =0.6c0 | oso. |. =>
6 | 2063.8 | 2063.79 | + 0.01 0.50 | =

23073.15 for «1 does not occur in the arc-spectrum of tin. The
spark-spectrum has the line 2 3071.9, which is given as diffuse and

broad- There appears to be good agreement for this series.
terms for «= 7.8 ete. are outside the region of observation.
@he translation 5618.84 gives the series with the formula:
109675.0
(2 + 1,651360 — 657,42 4—')?

108 A-1 = 50926.14 —

7 ——

which yi@ds:

Ill
ae — dy | - yap | pies f Intensity —
1 | 3032.90) | 3032.90 iia paren eer
2 2408.27 | 2408.27 go hes gad at 1
3 | 2209.78 | 2210.55 | —0.77 | “0.10 _
4 | 2121.5 | 2121.57 |. 0.07. | 0.20 a
5 | 2073.0 2073.50 | —0.50 | 0:50 ss

For A= 2209.78 Livenc and Dwar found 2 — 2210:7, =

~The

gives a difference of + 0.15. with the value found by me. ‘There is
2

I) ened: aa Hascuer 1, ¢, 240 pis a

‘i

- we

ae
'

a
.*

_—

.
at

j
7
va

af
m4

further again good agreement here, 7 — 6 falls just outside the region

of observation.

The translation 6923.26 (the other difference of frequency found

by Kayser and Runer), yields:

19675
10° A—) — 52330.66 — LUIGI S.0 .

(e + 1,651360 — 657.42 1!)

S = Sy are
2 a
ae ae Aw | Ap | to 5) t athey | Intensity
igh ae 2917.48 | Sep eae 4 =. 5
2 | 2334.89 | 2334.93 | So.ercke 0.08
3 | 2148.7 | 2148.59 40.11 0.20 i?
4 | 2063.8 | 2064.12 | —0.32 0.50 ~)

“z==5 is outside the region of observation. 4 2917.48 has not been

observed.
The translation 8199.87 yields the formula:

109675.0
TOS an ES E10 > sa aa lm Sa pee
(« + 1.651360 — 657.42 )—1)?

toe
« | Ay dy es cea Limit of age
| | pei!» €FLOrs ’
1 | 2812.72| 2812.72 | 0 | 0.05 | 3
Za he. 2267. SOs 2267.33 —0.03 | 0.05 |
’ 3 | 2091.7 | 2091.23 | Meer 40 V0.8: Vib =

xz = 4 is outside the region of observation.

The translation 8617.50 yields a series with the formula:
109675.0
(x + 1,651860 — 657,43A—*)

10° A—! — 53924.00 —-

eet of
£ | Aw | Ab | “0B | etre Intensity
\ 1 | 279.02 | 2780.06 | —0.14 0.03 4
2 | 2246.15. | 2246.06 | +0.09 | 0.10 | —
3 | 2073.0 2073.12 ite Oaks

x = 4 is outside the region of observation.

1) Exner and Hascuex l.c.

Besides these six series, which are connected by a simple trans-
lation, I have found some more in the tin spectrum that are con-
nected. The first series of this group may be represented by the formula:

109675.0

See a oe ee ee
Fis: (@ + 1.384406 + 446.70 11):

pa
oa ES ST Ls
Vil l ae
x day dy | hy—y | prt) | Intensity
i Lea
1 | 3801.16 9801 AG |S | OSE OMe at. 186
2 | 2850.72 | 2850.72 | 0 |- + 0.03.3, 24753 - 40
3 | 2504.49 | 2594.49 | 0 |. -0.08 >.>} 3
4. 2483.50 9482.58 >| 4402077, F) (aOale & oa 3
5 | 2421.78 | 2422.24 | 0.46 0.03 5
| !
6 | 2386.96 | 2385.98 40:08. ape. 9
- |

Why Exner and HascHek give so great an intensity for A 2421.78,
whereas this line is fainter than any of the others according to
Kayser and Rvuner, I do not know. 2 2386.96 only occurs with
Kayser and Ronee with the indication “sehr unscharf’. Exner and
Hascuek have not got this line at all, which is very strange, indeed,
in connection with the intensity 5, which Kayser and Runes give.

Of this series I have found two translation series, which corre-
spond with the two differences of frequency found by Kaysgr and
LUNGE.

The translation 5187.03 yields the series:

109675.0

108 2-1 = 49012 08 - oe NES Cte
(w + 1.384406 +. 446.70 212

ea Tee
VII Ste Suu =: a

x i ds eee os | aa z | Intensity

1 | 3175.12 | 3175.13 0.01 0.03 | 100

2 | 2483.59 | 2483.49 +0.01 0.03 --| 3 }
3 \ 2286.75 1) | 2286.75 0.00°° {> -peasceel ib 6
4 2199.46 | 2199.32 +0.14 | 0.10 |

5 2151.2 | 2151.54 —0.34 | 0.20 _-

1) Exner and Hascuex |.c,

The translation 6923.26 yields the formula:
109675.0

108 a- 1 = 50748.26 — feos she
a + 1.384406 + 446.70 3-1/2

Veep een
: x Aw 4b Ap—*b Wy aahel Intensity
LS al ee ae a
1 | 3009.24 3009.24 0.00 0.05 50
2 | 2380.82 | 2380.88 | —0.01 |. 0.05
J3 | 2199.46 | 2199.42 40.04 0.10

42118.43, which we found for c= 4 and the following lines have
not been observed. Possibly their intensity is too slight.

These two groups of translation series are represented on the
annexed plate, arranged in succession according to the vibration
frequencies of the first lines of these series. The figures mean:
freq. X 10°. The arrow indicates tle limit of the region of observation.

The first line in the fourth red series for Tin must be dotted. The six
series that were treated first, have been indicated by the same colour
(viz. red), in the same way the three last by black. The succession
cowed VIL Ih, TL IX, IV, V5.VE-

Not until further investigations on the Zzerman-effect have been
carried out, will it be possible to determine further what place
these series occupy in the whole system. In the arc-spectrum of
Tin there are further indications for series, which have, however,
not yet been examined by me.

In the spectrum of Antimony | have found a series which has as
formula:

109675.0

(« + 1.568667 + 237,63 A—l)?

108 A—! — 45365.69 —

—— 1

- ; ae os Limit +m
7 “9 4 Reese of uae Intensity
awe | ama | 0.00. | 0.0 8
2 2692.35 2692.35 0.00 | 0.03 3
3 2480.50 | 2480.50 0.00 | 0.03 | 2
4 | 2383.731)| 2383.93 | —0.20 | 0.03 | 24
5 ee s eS

— | 2330.95

1) Exner and HascHex l.c.

2 2330.95 has not been observed, its intensity is possibly too slight.
It lies in the neighbourhood of 4 2329.19 of Kayskr and Runes,
which, however, does not oceur at all with Exner and HascHEKk.
The two following series are in connection with this by translation.
The former of them has as formula:
109675.0

8 J! = 43296.20 — — ace Ene
a ee Ne a eeseer ae esa >

ea
+ aera eee reer ee eee ee eee Sa
ha ae : RTE

; : ae imit .

z dig dy | ee Ae EErars | Intensity

i | 3637.94 — |..3637:95 © |.. 0.01 #1) oe0c03: ana eee

2 | 2651.20 - |: 2851.21 |" 9.01 | 0.03 | 5

3 | 2614.74 | 2614.74 | 0.00 | 0.03 | 1

4 | 2507.90 ) | 2507.74. 1 306 2) — Ss:

12507.74 does not occur in the are-spectrum.
In the spark-spectrum, however, we find 4 = 2507.90 which cor-
responds with this. Further terms have not been observed on account
of their slight intensity.
The other translation-series has as formula:
109675.0

{08-J1 3 1908/91 <> aes a eee
ae c (@ + 1.568667 - 237,63 Ae

Pea as ak,

tt eee aa oo ee
zo) dw AL | Awe | Lint : | Intensity
1 | 2770.04 2710,04: |. 0:00 » “| = nonus 10 u
2 | 2289.09 2289 .09 0.00 | 0.10 =
3 | 2137.21 2195.07. | Paget a aaa =
4) ‘osnosral) 20e2!26- |. - oe ee =

0.r. 0. means outside the region of observation.

Further there are some more indications for other translation
series, which lie further in the region of ScnuMaNN, viz. that with
the asymptotes : .

93251.07 to which 4 2673.73 (Int. 5 ) and A 2220.85 belong, and

94951.35 to which 4 2554.72. (Int. 1) with 4 2139.89 may be
counted. For a= 3 4 2003.88 is therefore o. r. o.

1) Exner and Hascuex l.c. Vol. LI.

In the Antimony spectrum I found further a second group of
translation series, the former of which has as formula:
109675.0
(2 + 1.616567 — 332,37 1-12

£08 A—! — 47810.99 —

21.2

XIII 4 | ’ ut Me Limit of | :;
x Aw Ab Aw—4b Errors || Intensity
1 | 3267.60 | 3267.60 0.00 0.03 | 30 u
2 | 2574.14 | 2574.14 0.00 | 0.03 2
3 | 2360.60 | 2360.60 0.00 | 0.03 as
4 | 2262.55 | 2964.49 | —1.94 | 0.20 2.
5 | 2212.54 | 2212.51 | 0.03 | GeiGe Pa, ke re

Remarkable is the very great deviation for «= 4, while 7=5
is again in perfect harmony. Earlier investigators Harriey and ADENEY
found 4 2263.5 for this line, which lies just between the value found
by Kayser and Runee and mine.

By translation we may obtain the series:

109675.0

10°A—! = 45741.50 — |
(@ + 1.616567 — 332.37 1—1):

i ae ee
X1V ) SaaS Tae

1 | 3504.641)| 3504.64 | 0.00 | < 3

2 | 2719.00 | 2719.00 | 0.00 0.03 | 3
| | |

3 | 2481.81 2481.81 | 0.00 0.03 | !
| }

4 0.1.0. 2375.74 | x = &

4 2375.74 lies near A 2373.78, which has been observed, and for
which Exner and Hascugk remark : 2 +1, so diffuse. Possibly this diffuse-
ness is caused by the faint line 2375.74 in the immediate neigh-
bourhood.

Of a number of translation series, which lie for the greater part
in the ScHuMANN region, indications are available, which I will give
together in the following table with their respective asymptotes, and
for each of them one calculated vaiue in the as yet uninvestigated region.

1) Exner and Hascuex |. c. p. 322.

xV- =

XIX Asymptote 53986.13 | 54354.11 | 54005.34 | 55696.37 57039.02
ae = 1 Fa 2719500 2692.35 2652.70 2598.16 2510.60
|
=F | 222075 2203.13 | 2175.99 | 2139.89 2079.55
| |
r=3 2044.78: 2021.96 | 1990.20

1938.83

| 2060.25
The valnes for «= 8 lie all in the not investigated region.
Further I have found a third group of translation series in the

spectrum of Antimony, the first member of which has as formula:

109675.0

10° A-! = 44790.00 — : 2b test ea
(@ + 1.269826 +- 1757,48 1—))?
(eee) ee ae
XX Tate a oe
x | Aw Ab Aw—4b | ae | Intensity
| | |
1} 13282.61 3232.61 0.00 0.03 30
2 | 2652.70 | 2652.70 0.00 0.03 4
3 | 2478.401)| 2477.45 | +0.95 | 2 2
4 2395.31 2395.31 0.00 0.03 1
5 n.o. 2349 .50 — _ ~
2.2549.50 has not been+observed any more, which tallies with the

course of the intensity, as J indicates the faintest lines according to
Exner and Hascuek.
The following form was found as corresponding translation series:

ee 109675.0
£0? 4 =A 5208997 a=
(2 + 1,269826 4- 1757,48 A—1)?

" Ixner and Hascuex loc. cit. p. 282.

while there have been found two indications of series of translation
in the region of ScHUMANN viz.

aaa
XXIII Asymptote= | 53402.61 54744 .87
a 2528.60 (Int. 20) 2445.59 (Int. 2)
22 | 2159.32 2098 .47
os 2042.40 (0.r.0.) | 1987.30 (0.r.0.)

The found series in the Antimony is indicated on the annexed
plate, coloured in groups, just as that of the Tin.

The first group of translation series is coloured black, the second
group red, the last mentioned group blue. The succession of the
black one is: XI, X, XII; that of the red one XIV, XIII, XV, XVI
ete.; that of the blue one XX, XXI, XXII and XXIII.

So it appears from this investigation that in the spectra of Tin
and Antimony the series have been considerably shifted towards the
side of the small wave-lengths, and so that they lie for the greater
part in the ScHUMANN region. At the same time it has appeared from
it that the intensity of the lines of one and the same series greatly
decreases, so that only a limited number of lines has been observed.
But though the number of lines is limited, yet the mutual relation
that exists. between the different members of one translation group,
sufficiently proves the existence of series in the same form‘) as we
meet with them for other elements. Though the series there are at
once far more pronounced, yet the translation series exists there too,
as I shall show more at length in my thesis for the doctorate.

How we must distinguish the series found as principal and subor-
dinate series etc. cannot be decided for the present. Not until a
sufficient number of magnetic splittings up have become known in
the ultra-violet spectrum of these meials, this investigation can be
undertaken. The few things that are known about the Zueman-effect
of Sn and Sb, have been found by Purvis?). We will summarize
it here.

Purvis has measured the magnetic splitting up of the following
lines in our tables.

1) RypDBERG’s statement, therefore (Rapports Paris 1900. T. II. p. 220) that Sn, Sb
and some other elements present spectra built according to other laws, cannot
be maintained. ;

2) Purvis Untersuchungen tiber die ZeEMAN-Phinomene. Physikal. Zeitschr.
p. 594, 1907. and the literature mentioned there.

dp
4 | 2
|
Tin |
+ 2.12 s
3032.90 een)
— 2.16 s
+ 1.22 s
; 3801.16 Oe
| | — 1.22 s
| 4+ 1.30 s
2850.72 OD hap
— 1.30 s
+ 2.12 s
1 boi 0 ?
— 2.13 s
+ 2.00 s
3009.24 Or, Dp
— 2.02 s
Antimony
+ 2.1ls
+ 0.99 p
3637.94 0
— 0.99 p
— 2.l1ls
+ 1.76 s
3232.61 Maar kr)
— 1.75 s
| + 1.20 s
2770.04 Ors ap
— 1.20 s
| =F Lillss
3267.60 | 0 ap
| — 1.19 s
| + 1.60 s
2598.16 oO >
— 1.60 s
+ 1.59 s
2528.60 0 >
— 1.59 s

In this table s denotes vibrations normal to the field, p vibrations
parallel to the field. Of the lines of the Table only Sn 3801 and
Sn 2851 belong to the same series. They are both blurred, in con-
nection with this the agreement in magnetic splitting up is sufficient.

Sb 3638 becomes a quadruplet. According to Purvis it is identical
with that of Cu 3274 and Ag 3383 and so of Na 5896. It will
have to appear from the further investigation of the magnetic field
whether this numerical result has a deeper meaning.

In conclusion I will point out some objections, which might be

raised when the above series are studied. In some eases we find,
namely, a value given under 2, which occurs in two series. The
corresponding values of 2 are then somewhat different as a rule.
It is now the question :

“Do the observed lines belong to two series, or have we to do
with two lines close together, one of which is difficult to distinguish
from the other >”

Befcre answering this question | will first draw attention to this
that this phenomenon is also met with in the spectra of other
elements. Thus we find in the spectrum of aluminium *) 4 2204,73
classed as nm =8 in the 1st subordinate series, and as n =7 in the
2nd subordinate series; in that of Zinc *) 4 24380,74 as n—=8 inthe

2nd component of the 1st subordinate series, and as n=4Q in the 1st

component of the same series. In the spectrum of Calcium *) we
find 23101,87 as n=8 in the 3rd component of the 2nd subordi-
nate series, and as 72 —=—9 in the 1st subordinate series. These few
examples may suffice to show that the phenomenon that presents
itself a few times in the series found by me, is met with elsewhere.

Let us now try to answer the question raised led by the examples
which present themselves in our case.

Let us begin with the spectrum of Tin.

For 2, 2483.50 we find 2, = 2412.53 in VII and a; = 2482.49 in
VIII,. Examining the observation of this line we find given by KaysEr
and Runer*): “2 umgekehrt”’, and by Exner and Hascuex §): “3
unscharf, umgekehrt’”. It is not impossible that here two different
lines must be observed. Also what follows pleads in favour of this :
In VII we find successively the intensities: 30, 10, 3, 3. That for
«=A the intensity is not found smaller than 3 may find its explanation
in this, that two lines of slighter intensity give this increased intensity.

For 2, 2408,27, which is given in I, with 4, = 2408,71, in III, with
A, = 2508.27, a similar explanation may hold. Kayser and Runes find *):
“3 umgekehrt”’, Exner and Hascuek *): “4 unscharf.’ The course of
intensity in I is: 5.3.1.1. Probably /, = 2408.71 agrees therefore
with a very faint line beside 4 2408,27, which belongs to III.

4» 2199.46, which has been given in VIII, with A, = 2199.32,
and in IX, with A, = 2199.42, we find in Kaysrr and Runge *) with
the indication: “1 umgekehrt”, and in Exner and Hascuexk °) in the

}) Kayser, Handbuch der Spectroscopie. Vol. Il, p. 547.

2y-1..¢.. p. 542.

sel: @.. p. 536.

4) Ueber die Spekiren der Elemente. VII. Abh. Berl. Akad. 1894.
Bele." Vol. II:

oF). é. Vol. IL

sparkspectrum (the are-spectrum of Tin they have observed no
further than 42267): 42199.41 “4 unscharf’ and 4 2199.68 “1
unscharf’”. So the two lines very clearly appear here very closely
side by side.

i,, 2091.7 oceurs with 74, 2092.30 in U, and with 4; 2091.23 in
V.. This line has not been observed by Exner and Hascuek.

‘In Kayser and Ronee ») we find “3 umgekehrt (?)”. So they doubt
whether or no they have to do with a reversal here. So the surmise.
is justified that we have to do here with two separate lines, which
surmise is supported if the course of the intensity in II is examined
according to the observations of Kaysrr and Runeg. Starting from
z—=2 this is namely 5, 3, 1, 3, 3. The increased intensity 3 for
z—5 is again accounted for by the assumption of two lines close
together. In the same way the increased intensity of the line 2063.8,
which as z—=6 occurs in the same series, may be accounted for
by our finding 4,= 2064,12 in IV,, which is given there also with
i}, — 2063.8. It is a line which has been given by Kayser and
Runce’”) with a limit of errors 0.50, so which could be observed

less accurately.

After this extensive discussion of the spectrum of Tin, a few in-
dications will suffice for that of Antimony.

22719.00 we find in XIV, and XV,. The intensity in XIV is
3.3.1, so somewhat too high for z=2. This line is found in KaysEr
and RunGcE reversed, but not in Exner and Hascuexk*). This is also
the case for 42692.385, which occurs in X, and XVI,, and with
-2.2652.70 in XX, and XVII,. :

22614.74 we find as XI, and XXI,. It occurs in both observers
as a single line. Noteworthy, however, is the difference in intensity.
In Kaysrer and Runee*) this line is one of the strongest lines (inten-
sity 5, while 6 is the greatest intensity that occurs), whereas in
Exner and Hascuek *) it is one of the weakest (intensity 1, highest
intensity 30). 4 2098.47 has not been observed by Exner and Hascnek.
We find it given in XXI, and XXIII,. In conneetion with the A,
which I found for XXI,, namely 2097.76 I still want to remark that
this value lies between that found by Kayser and Runge, and that
of Hartley and Apgnry, who give for it: 4 2096.4.

I should further like to make another remark. When the list on

1) 1. c. Vol. III.
¥)\ 1. ¢.
1, ¢.
4 1c,

p. 42 with the given magnetic separation is examined, the question
naturally rises :
“Why do 4 3032.90 (III,) and 4 3175.12 VIII,) occur in different
series for Tin, though they exhibit the same splitting-up ?”
The same question applies also for Antimony 4 2770.04 (XII,) and
4 3267.60 (XIII,), and also for Antimony 2 2598.16 (XVIII,) and
4 2528.60 (XXII).
To answer this question I have traced every time two lines as
10°4-' and examined by means of my model without giving it a
rotation, what would be about the frequencies of the other terms of
the series that is perfectly determined without rotation by these two
points. In this way I have arrived at the following results:
If we consider Sn 4 3175.12 as e=3 and Sn23032.90 as x= 4,
we get 10°A—-' — + 28400 for x=1, which does not agree with
any observed line. (The nearest lines have the frequencies 27353.20
and 30023.63).
If we consider these lines as «=3 and «r=5, we find
10% A-! = + 32450 for «= 4, which does not agree with any line.
@©=2 yields 10° 4-' = + 29500, which might then possibly be
30023.63. But this is not very probable either, for the line which
Le a ae
+ 1.22 p

agrees with this (4 3330.75) exhibits a quadruplet') 0 in the
— 1.22 p
—1.79s

magnetic field, and so very certainly does not belong to this eventual
series. In this way I have ascertained that the lines in question
cannot be ranged together with others in one and the same series.

I have obtained corresponding results with the other lines which
show the same splitting-up. This has rendered it very probable that
the rule: “All the terms of one and the same series present the
same resolution in a magnetic field’, cannot be reversed, and so
it is my opinion that the argument that I have not ranged lines
which present the same splitting up in the same series, cannot be
advanced as an objection to.the classification of the Tin- and Antimony-
spectrum given by me.

1) Purvis. Proc. Cambridge Phil. Soc. 14. 1907, p 220.

Mathematics. — «New researches upon the centra of the mtegrals
which satisfy differential equations of the first order and the

jirst degree.” (Second Part). By Prof. W. Kapreyn.

8. Assuming in the third place
a’ + ¢=i(a+e)

aa’ — ec = (b—ib') (a+c)

2b' = 3a + de
or putting b= 7p
2a' = — i(8a—2B8-+ 8¢e)
2¢e' = 7 (5a —28 4+ 5e)
26' = 3a+ 5e.
We have
g, =a’ — i (Ba42') = — — (15a—28-4-180)

q, = 2a + 80 —ib = = (18a+28-+ 15e)

pes 5 (86a! + 26a8 + 179ace — 48? + 288e + 99c?)
1

Se (45a? — 36a8 + 84ac + 48? — 32Be + 39c*)

r= = 5 (1300a" — 6a -+ 265ac — 48? —8f8e +137c?)

1 -
r= 75 (42la® + 11603 + 972ac — 128" + 120 8c + 567c*)

and for the coefficients of P,

8, = (5a4 20) r, + a'7,
2s, — 4s, = (864 2c') r, + (4a4 4b') vr, 4+ 2a'r,
ds, — ds, = der, + (6b+4 3c) r, + (8a+6b') r,43a'r,
4s, -— 2s, = 2er, + (4b+-4c') r, + (2a4 8b') 7,
— 8, = cr, -+ (2b+-5e) r,. .
To determine the next condition we introduce the two following
polynomia
P= tov, + tyaty + tw*y” Es tu? y* ty = ty"
P, = uya® + ujary + uety? -p u,a?y® + u,e?y* + uny® +ugy’.
The coefficients of the first are determined by the relations

i t, = (6a+ 2b') s, + a's,
2t, — dt, — (106 + 2c’) s, + (5a+-4b') s, + 2a's,
Bi, — 44, = des, + (8b+-3c) s, + (4a +66) 8, + 3a's
4t, — 3t, = des, + (6b+-4c') s, + (8a+8b')s, + 4da's
ot, — 2t, = 2cs, + (46-+-5c)s, + (2a+10B) s,
— t,=cs, + (26+ 6c')s,
which may always be satisfied, and the coefficients of the second are
related to those of the first by the following system
u, =(7a+2b')t, + at,
2u, — 6u, = (126+ 2c’) t, + (6a +4 46') t, + 2a't,
du, — du, = det, + (1064 3c) t, 4+ (5a+ 6b')t, + 38a't,
4u, — 4u, = 4et, + (8b+4 4c’) t, + (4a4 8b’) t, + 4a't,
5u, — du, = det, 4+- (66+ 5c’) t, + (8a+100') t, + 5a’ e, -
6u, — 2u, — 2ct, + (46+ 6c) ¢, + (24+126't,
— u,—ct, + (26+7c) t,.
This system is impossible unless

du, + (3u,—5u,) + (5u,—s3u,) + 5 (—u,) = 0

or
(35a+-106'+ 5c) t, + (5a'4-1064 3c’) t, + (5a+60'4+ 3c) t, +

+ (Ba' + 6b-+5c’) t, + (8a+108'+5c) t, + (Sa' +1054 35c) #, — 0
which may be written
At,+B (2t,—5t,)+C (3+,—4t,) + D (4+, —3t,) + E (5t,—2t,)+ F ( -t,)=0
if

A == (Td $140 be) BS Gaon by),

1 1 ee
C == (574106419) , D=— = (19a+-108'+ 5c).
B=! 1 26 4 Te Pee) ted = (17a 140! +70).

Thus, choosing as before s,— 0, the sought condition takes this form
s,[ vA + (5a+ 4b!) B+ (8b43c’) C + 3c D]
+s, [2a B+ (4a+ 61') C 4+ (664 4c) D 4+ 2c FE]
+s, [8a'C + (8a+ 8b') D+ (4b +5c) E+ cF]
+ s, [4a'D 4+ (24+ 100') E + (26+46c) F] = 0.
Writing this equation
eas A fs 8a Se *y + i, =O
and eliminating a’ 6’ c’ we obtain

201 : 4; ;
eres 8a+84+8c) , B= —2(5a+3c) , ea, (08 —B+410c)

; Ei
DSS ed (l7a+1l5c) , H=4i(4a—B8-+-4e), Sheweh i. = (19a-+ 21c)
iS ee (13a+108+11ce) = 19 (ate) gq,
fy = 304 (a+ ¢) (8a— 28+ de) = 10 (a+c) g,
f, = — 10 (a+e) (8la—2B+41c) =10(a4+o)9,
f, = — 107 (a+e) (61a—148+59e) = 10 (a+ 0) g,.

Now, omitting the factor 10 (a-+ c), we get
91% +92 + 958 + 9.8, = 0
‘herein the values s may be expressed in function of 7 in this way
2s, — (16a + 10c)r, —i(8a—28-+3¢e)r,
2s, —=i(5a+ 68+ 5c)r, + 10(a+e)r, —2(8a—2B-+ 380e)r,

2s, — —2er, —i(25a—68-+ 25¢)r,

u
2s, = — (5a + 68+5c)7, + (5a-+ 60), + 4 (T+ 28+ 70) 7,4 (Ta4-10e) 7,
Substituting these values, and putting

G,=13a4+ 108+ 1le , G,=9a— 6B +4 15e,

G, = 3la — 28+ 4le, G,==6la— 146 2 oer
we find
1
r,[— (16a4+-10c) G, — (5a+ 68 + 5e) G+ 9 Oe ORT de) Gy]
+ ir, [(3a—28-+ 8c) G, + 10(a +e) G, — (5a + 6c) G,]
1
+ r,[(8a—28 + 8c) G,-+ 2c G, +- 5 (een G,]

+ i, [((25a—6p-+ 25c) G, — (7a +-10c) G,] =0
which may be reduced to
1 ;
iat [—20la*— 72a8— 252ac—126°— 36fe — 75c?]
+ wm[-176a?+ 14a8— 349ac —208*+ 328e—171e?]
1
+—>9,[ 48la"— 48a%+1108ae— 48% - 84Ge + 667c*]
+ «w,[ 348a?—138a8+ 77%ac + 128? — 156pe + 435¢?] = 0
Writing this result
1 ’ . ry. 1 .
ree T,t+,T,+ ri Te +u,7T,;=0
and assuming

z ; a if
i g fo nian ; "2 eee tage
we obtain

et BRT cl SIRT. — RP. —410
which after reduction gives finally the condition
12 (a + c) (a — 28 — c) (3 a—28 4+ 5e) = O.
This condition breaks up into three others from which the first
a-+c=O has already been examined in Art. 2.

9. Introducing the second, we must examine the case where

2a’ = —- i (8a — 28 + 3c)
2c = i(5a— 28 + 5e)
Ab ==) 3a+- 5e
2b >=. a—e

or, remembering that 6=78

a’ = —i(a + 2¢)
cé= i(2a+4 3c)

265 38a+ 5e

26 == ~4 (a= ¢).

This case has already been met with in Art. 7.

10. Finally we have the relations

2a' = — i (38a — 28 + 3c)
2c = 1t(5a — 28 + 5e)
26; = + 8a-+ de
2p === on -- be
which are identical with
a=—t
c =

2b = 21b' = 1 (3a + 5c).
The differential equation reduces in this case to

dy —«a + tex? + (3a + 5c) ry + tay’
da - y +: aw? +1 (8a + 5c) ey + cy’

whose general integral may be constructed from the two particular
integrals

1
(a + 8c) (w — iy)? + 2i(@ + wy) + Trt, 0
and

(a + 80) (a — iy)? + 3i(e? + y?)=0
which are easily found. —
This general integral
eee ee
1 8
ate

= const.

(a + 80) (@ — iy)? + 2i(@ + iy) +

Proceedings Royal Acad. Amsterdam. Vol. XV.

may be expanded for small values of # and y in the form
eityt F,+ F,+.... = const.

which proves again that the origin is a centrum.

11. Resuming we may conclude that where
(ate? ti(dicf=0.
the differential equation
dy —a+a'e’ 4+ 22'ey 4+ cy?
dz y + az +- 2b ay + ay?
has a centrum in the origin of coordinates only in the following cases
ta oe 0 en a Ae .
fia 1? == 4 (a +o) en ev
IIL. 2a = + i(a— 20' +0), 2 =+iCa+ W 40, 2=+iaa—dD
IV.ad = +i, ¢d= +a, 2b'=>3a+4 be, 2b=—3a-- Be
for it is easily seen that in the last three cases everywhere 7 may
be replaced by —z?.
The results obtained in our former paper show that the origin is |
also a centrum in the three following cases
V2 a=), io bo coves e ee
hia =e. 0, o' = 6— 90
Vil. ad t+ ¢=0, a= 6b, 2b = 8a 56, 2a = eee
We found there one case more viz.
atc), dt and «es

but this is included in I.

12. To compare these results with those of Duac, we will
transform our differential equation

dy _ —exta'e’? + 2b'ay+ ey? Wy ese 8
dz ytax*+Qbay+cy? yx
in his form. This may be done by the substitution
A§ZS =a iy ky = « — yy.
This gives
hd& kdy
ytX+ i(—at Y) iy y + x —i(—@#+ VY)
where
y —ta@ = — hs, y + 12 = thy
X + 1¥ = — i(A—B) h?§* — 21 (C—C’) hkSy — i1(D - £) Px?
X —1¥ = —1(D+ B) WS — 21 (C4 C) AkEq — 1 (A4-B) x?

and

= ape), B=

*: (a’'—2b—c'), C=-
r 1 I— =— 4 (a-t-c)
p= = (a— 280), E= = (any BEG jy “Gr =e : (a +.
4 4 rd

Thus we find generally

ES h(A—B) & + 2k (C-C’) & + — (DE) 1? pe
t

* =
| n= b+ B) 4” — 2h (C+ C') 4 — = (D+ En) | ds = 1)
and when C’=0 or a’ +c’ =0

E + h(A—B) 4 20S 4+ > (D—B) y |
- E — k (A+B)? — 2hC%y —— (4.8) § | di=0 (B)
where
i 2(a'—b) , (a+)
— > = ——= Se OS
AS (a + 26'-c), B ri C n
2 (a' +b)

j= 5 (a—2b'-c), E=

If now we compare with (B) the first equation (1) of Art. 1 we

have
ke?
h (A—B) = 1, Bit, —— ze (D—E) = v
u
h?
—k(A+B)=1, —2hkC=pn, — z (D+ E) =p
which may be satisfied by taking 4 = -~/ and
fe Oe FP == 0
or

ne Oe)
This first equation therefore belongs to our class VI.
In the same way we may infer that
(2) belongs to class V
(3) is a special case of class |
(4) belongs to class VII
(7) is a special case of class I
(9) is a special case of class VI
(11) is a special case of class I.
If now C’==0 we compare with (A). This gives for the fifth

equation of Art 1
4*

h(A—B)=1, 2k(C—C)=0, = (D-H) =0
L

}2
—k(A+B)=0, —2a(C+C) =r, — 7 (D+£)=pv

which may be satisfied by
A 4- B=; D—E=), C—C'=0
or
2a' = i(a—2b'+c), 2c =i(a+20'+c), 2b =i (a—-).
Thus (5) belongs to class II.
In the same way it is seen that
(6) is a special case of class II
(8) belongs to class IV
(J0) is a special case of class III.
The eleven equations given by Durac are therefore contained in
the preceding 7 classes.

Chemistry. — “On a few oxyhaloids.” By Prof. F. A. H. Scnreine-
MAKERS and Mr. J. MILIKAN.

Of the chlorides, bromides, and iodides of the alkaline earths
several oxy-salts have already been described; in order to further
investigate the occurrence or non-occurrence of these salts, to deter-
mine the limits of concentration between which they exist and, if
possible, to find other oxyhaloids, different isotherms have now been
determined and by means of the “residue method” ') the compositions
of the solid phases have been deduced therefrom. Here, we will
discuss only the solid substances that can be in equilibrium with
solution.

The system CaCl,—CaO—H, 0. "

Temperature 10° and 25°. At both these temperatures occur,
besides CaCl,.6H,O and Ca(OH),, as solid phases the oxychlorides:

CaCl, .3 CaO .16H,O. and CaCl, .CaO .2 H,0
the composition of the second salt may be expressed also as:
Ca OH: HO

This latter oxychloride has already been found previously by a

determination of the isotherm of 25°7); the first one was then

') F. A. H. Schrempmakers, Die heterogenen Gleichgewichte von H. W. BAKHUIS
Roozesoom. [Ile 149.

*) P. A. H. ScurememaKers and Tu. Freer, Chem. Weekbl. 683 (1911).

53
already known’). From their determinations, ScureinemMakers and
Ficet thought they might conclude that the other oxy-salt should
have the composition
CaCl, .4 CaO .14 H,0

As the region of existence of this salt at 25° was, however, still
but very small, a slight error in the determination of this composi-
tion was still possible.

Temperature 50°. At this temperature occur, besides CaCl, . 2 H,O
and Ca(OH),, also the two pees

Cad 1
a Ob: $H,O and Cat OE:

as solid substances in proximity to their saturated solutions. The
first one already exists at 10° and 25°, the last one had not been
described, as yet.

The system: CaBr,—CaO—H,0.

In this system, only the isotherm of 25° has been determined ;
as solid phases occur, besides CaBr,.6H,O and Ca(OH),, the oxy-
bromides :

CaBr,: 3 CaO .16H,O and 3 CaBr,.4CaO.16 H,O

The latter salt was not known up to the present; the first one has
been described previously. ’)

The system: BaCl,—BaO—H, V.

In this system the isotherm of 30° has been determined’); as
solid phase occurs here, besides Ba Cl, .2H,O and Ba (OH), . 8H,O,
the oxychloride :

2 H,O

: 2 / Cl
a bat). B : De : O
Ba Cl, . BaO .5H,O o1 Ny H 2H.¢

This salt had already been prepared and described previously *) ;
the two oxychlorides :
Ba Cl (OH) . 3'/, H,O and Ba Cl (OH). 2Ba Cl,
also described previously, were not found at 30°.
The system: Ba Br,—BaO—H, 0.

In this system the isotherm of 25° has been determined; as solid

1) Rose, Schweigers Journ. 29, 155.
_Ditre. Compt. rend. 91, 576.
AnprRE, Compt. rend. 92, 1452.
2) E, Tassitty. Compt. rend. 119, 571.
Ann. Chim. et Phys. [7] 17, 38.
3) F. A. H. Scuretvemaxkers. Zeitschr. f. Phys. Chem. 68°88 (1909).

_ 5) Beckmann, Ber. 14 2151 (1881)

André, Compt. rend. 98, 58; 98, 572.

phase occurs, besides Ba Br, .2H,O and Ba(OH),.8H,O, the oxy-
bromide :

Br
Ba Br, . BaO . 5H,O or BX Oy . 2H,O

This salt has already been described previously *); the other oxy-

bromide:
Ba Br(OH) . 3H,O

which has also been described *) was not found at 25°.

The system: Ba I,—BaO—H, 0.

In this system also, the isotherm of 25° has been determined; in
addition to Bal, .7H,O, Bal,.2H,O and Ba (OH), .8H,O the oxy-
iodide:

]
Ba I,.. Ba 970" or Ba on .4H,0

also described previously, occurs as solid phase. *)
Besides the above systems, various other ones are now being
investigated; the results of this research will be communicated later.

Physics. — “Accidental deviations of density in mixtures”. By .Dr.
L. S. Ornstern (Communicated by Prof. H. A. Lorentz).

The theory of accidental deviations of density in mixtures does
not differ, as for the principles, from that of the deviations of density
‘in systems containing only one kind of molecules. To calculate these
deviations I shall apply the canonical ensembles of Gisps °*).

1. Let us suppose a mixture of & substances to be in a volume
v, n, being the number of molecules of the kind 1, n, that of the
kind zx, and mn, that of the kind &. Besides the coordinates and-
moments of the centres of gravity, a number of internal coordinates
and moments can be used to characterize the state of the mole-
cules. Let us imagine a canonical ensemble built up of those systems. |
We shall denote by a1, yi, Z1-.--- Zing the coordinates of the
centres of gravity for the molecules of the first kind, those of the
z-molecules will be represented by a1 .. . Zn -

In order further to characterize the system, we shall introduce

1) BecKMANS, J. f. prakt. Chem. N. F, 27 132 (18883).
2) BECKMANN. Ber. 14, 2156.
E. TassiLLy, Compt. rend. 120, 1338.
5) 1 shall confine myself to a single phase, the coexistence of phases offering
no particular difficulties. | dealt with this question in my dissertation (comp. p. 114).

the moments belonging to the coordinates (the internal ones and
those of the centres of gravity) mentioned above. Now, suppose (2;
to represent an element of the extension in phase of the internal
coordinates and moments. Consider the integral

(fer #/ae,, mali thatnl aes

where « is the total energy « diminished by the energy of the
progressive motion of the centres of gravity. The integration with
respect to the coordinates of the centres of gravity must be extended
over the 3(n, + ..n--+ nz)-dimensional space v32n, , whereas all
values that are possible without dissociation of the molecules are to
be ascribed to the internal coordinates and moments.

If, in the case considered, there exists a sphere of repulsion such
as there is with rigid, perfectly elastic molecules, then the conse-
quence will be that «' takes an infinite value for certain contigu-
rations, and therefore the parts of the integral corresponding with
these configurations will not contribute to it. Just as in the case of
a simple substance and in that of a binary mixture‘), one can show
in this case that the integral may be put into the form

k
a Ry
feodny... Dy: . Np). 0}
Wize 6:
’ where Dx = 7; i. e. the number of molecules of the kind x pro
unit of volume.

The function @ may be determined if the structure of the mole-
cules is given; but for our purpose it is sufficient for us to know
that the integral can be reduced to the form mentioned above.

2. We now imagine the volume V to be divided into a great
number of equal elements of volume J,.. V;.. Vi. and we want
to know the number of systems in a canonical ensemble for which
the element V, contains respectively 7,.. n,.. mj of the diffe-

rent molecules. We have for the numbers 7,,
l
= Uj Nz.

ihe total number of A cei ‘of each kind being given.
This number of systems &, which I shall call the frequency of the
systems eae s: is ag by the formula

11 \6-0n0 »1]

1) Comp. my dissertation and these Comm. 1908, p. 107.

Ily) ,

- (1)

@) (D1X- - Ber - Dg) Vi)

n, !

m, denoting the mass of a molecule of the kind x. We now can
ask, for which values of the numbers 7,, this frequency is a maxi-
mum. In this way we find for the & conditions to which the den-
sities in the most frequently occurring system are submitted :

l J log wy
— log ny, + & (na) ee OP = Fes a Te A
1 xd

x from 1 to k&. These conditions can be satisfied by means of a
homogeneous distribution of each of the x kinds over the volume
V. Further the second variation of ¢ or of log§ has to be negative.
If we denote by 7, the values in the most frequently occurring
system, then the frequency Sa of the system in which these num-
bers have the values 7,,-++ 1, can be represented by
—Q
So = So é ee : ee te gt Lk eee (3)

The quantity Q is a homogeneous quadratic function of the numbers
t,,. Taking the sum of §4 with respect to all possible values of
these numbers i.e. from —o to +0, we obtain > $4 = N, from
which ¥% can be calculated.

Proceeding in this way we find

2 ony

a ae k Rais
2
e : = iB (22@m,) {w(n, . Dx =. DE), > ee
1

In calculating YY, which is equivalent to the free energy, we
must neglect a factor of the order of unity. However, the formula
is rigorously exact, the above-mentioned being a mere verification
of the equation (3). For keeping in mind the definition of Gisss,
we have for

oO 36
e —— fe m,Gi,, : =~ Ge, aa;

Ya — 2 + m,2,,°

and therefore

u k 3 €
O 2 O
e = [] (227 Om,) F AG. os cn Sige
I

and we see that according to the definition of the function , the
formula given for Y holds exactly ’).

If we would have as a separate system of volume V; the n,, .. Ma.
i,, molecules being now in the volume Vj, then the free energy
of this system would be given by the formula

1) Comp. also my dissertation p. 56, 112, 126.

t
~J

W; 3

—Nin}

== k
7) 2
a = {| (227Om,) fw (ny) » « Dyy- - Dy) Vy} Nx.
l

The function Y, may be used to transform the formula for the
frequence §. For, applying the theorem of SrirLinc, we can write ¢
in the form

ae 3
— =~ Obie
oO ig, te »)(0,>...0%)) Vi) my
we A Oxemy aot [| (eels
1 1 Ny)
and therefore, introducing %, we obtain for ¢
8 pe og |
QO n Ny NI. 0) 1
aN Gg WS ne Mg ge IH el | é l]
1 | 1 Ps Wixk S

For the further discussion we shall not use the free energy Y%,
but a function y,'), closely connected with it, and being defined
by the equation

!) We can somewhat more closely explain the introduction of the function y) (comp.
also my dissertation p. 52 s.). We shall compare the free energy of the system
considered above to ihe free energy of the same system in gaseous state and in
a volume so great that it can be considered as an ideal gas. We now can easily
show the free energy of the mixture in the gaseous state to be equal to the sum
of free energies of the components, if each of them occupies the same volume as
their mixture. Further we can suppose that the volume of each of the substances
(which now occur as simple substances in k& separate volumes), is changed in such
a way, that the number of particles pro unit of volume which is to be taken very
great, amounts to » (arbitrarily chosen) for all & systems. The volume occupied

Y
that («(v)n**4) may be put equal to unity.
We therefore find for the free energy of each of the components, originating
from the element a

Ny) Ny \Nxd
by the th component now amounts to —. In this state (2) will be so great
Y

Les 3

—Ny)

0 2
e = (2 x Om,) (

Ny) Ny) «

And for their total free energy :

2a lad k

is ae ue Zn, _*
1

Oo ar es Ny) \Nx)
A —e = (2 x Om,) | | =
]

bo| 09

For the difference between the free energy in the state from which we started
and that in the zero-state considered we find

(a=).

Introducing the function y», we obtain * C
YY 3 ] W

a Sa Aft TAG [le Cs Oe 2" RE 4 :

The volume being given, the function wp is a function of the
densities n,, for

ay Ie
—— = 2 n, {log w (n, ..0,.. ng) — log nx} =
Spee

k
V & {n, log w (n, .. ny. . ng) — log u,}
1

3. We shall use the form now given to § to put the question of
probability of deviations in such a form that the deviations of density
appear from our formulae. We then have to examine for which
values of the densities /oyS will be a maximum. Suppose n,, to
represent these values and vy, to represent the deviations of densities

for other systems, then
l

= Ox = 0.
For dlog§ we have
1f! & ow, 120.074)
Lo. — — Se y — >) 44 oe
J 5 | 2 l On,» ¢ +3 l Pere 5
| ae 2 Ow, SaaS | ja
. a On, One), 01) 02) -- ee o- e . . . . ( )
As conditions of equilibrium we now find
Jw)
ne =f, A-from_1 tod 3 Se
Further
mp Make Vora CL 0 8
a ( e e
27 lon? EL ae On}),0ng) ~ G1102. + a co
l
ZY;

YS yy") 1
— eee Dy) ved | Mxd Mad ea aoe
5 EG yp = '¢ pl

the quantity y nee an ie. constant aot any physical meaning; £y*
?

however, being connected with the difference of free energy from the zero state
defined above.

The left member of this inequality consists of / terms, each of
which relates to an element of volume v;. If we take into conside-

v) 1 ae
ration that > Say yw, then it is seen that we have
Vv

oy, 1dy
dn,,? 1 On2
and
Fw, 1 iy |
edna emir Say eee” (9

The coefficients of all / forms therefore will be the same for all
corresponding terms. In order to find the condition which is to be
fulfilled by the coéfficients in (8), we will consider the case

QD = — ev ,
all other v’s being 0. For this case we have for all possible values
of the o’s

On) = — Ux! 3) UR — Gki!

O° Pw
——91,7 + 2—— 9] ga +... 0
On,? Sp Onan a” . ae
only the index 4 occurring.
The conditions, necessary for this to be true, are that 1. the

discriminant A

Bea d*y Op |
Onyr On, On, On, dny!
. | 0° 07 ow |
== f ogee Fe
| a On, On, dn} Meal (10)
07 ew d°y
On, On}. Onj-0n1: Oni

whereas the same must be true for the determinants originating
from the discriminant if we successively omit the right-hand column
and the last row. The conditions under which the system is really a
maximum and therefore stable, agree with the well-known thermody-
namical conditions of stability.

4. We are now able to determine the mean values of the squares
of deviations 97,, and of the products 9,19, *).

As is easily seen we have

SST ig eee Pee | a er en
and
1) Mathematically speaking, our problem is one of correlate probability, my

formulae agreeing with formulae Prof. J. GC. KaptetsN communicated to me after
1 had solved this problem.

Ox), O27), = Oxi! Uz'! + . . Baus . . (11a)

To define 9”,, e.g., we have

Ont
11 : 1 = 0?y se a 5 0 w
TD io 2) — —_—- O° 2 oe a = 2A 1 Oo A ee
+ : 261 , dn,? * 1 On,on, *” V2
{ fue dg,,.» dgzt-
ee se
+a +a a v7y+. Cine es Yl) G2)

pel 7 bana
D
fos : ee dg +. 5 Agel

Now, = vi, =O, etc. In order to take this into account in deter-
mining g’,,, Wwe introduce new variables instead of Q,,.. gi... Qi:

i!
on —e'h — poy ea h from 2 to l.

Then we hare
l
= pn = 8;
1 2
We also introduce for gi, .. g,; new variables in a similar way.
The exponents of the integral then can be expressed by

1 Ow 1
re “ae. 1 Lo. =
41 a is =i) fe

210

0°y i 1 07h , 35 3
ee Caged oe. | + 5) Oita amy as + : ‘

where C’ is a quadratic function in the g'1, v'2, (A 2 to J).
Now, taking into account the conditions +9‘, = 0, we can integrate
with respect to the variables 0’,, i.e. with respect to the elements

2..4../; the result in the numerator being cancelled by that in
the denominator. In this way we find

Oy
ap 2 Qin On jae

+ be spats oe
f-fern- doy, - - 19K

Os; =— a re
1 dey dw
wo +c = 105 Se ee a
3: - ae, (J—1) a) 11 On, 2 ar Qi 921 On,0n,
| | . Qi: dyke

According to a well-known theorem (comp. Gisss El. Pr. in Stat.
Mech. p. 205) we have

: BP Si. ge Oe |
5s 2 @(l—1) Esc yb dg ss On,On, ot Or) x
| e do,, Ov, a dvr, =
ena
laa S|
Be OE Gs hot at OB

where A is the determinant defined by (10). Differentiating the

2
“Uy

=, we find

logarithm of (13) with respect to -

On,
Ss je 7
ng ee (.—1) 0 rs
and in general
v4) @ 16" (14)
A
whereas at the same time we find
‘aie ee Ay
Ori Urs == (l—1)O (14a)

The quantities A,, and A,, represent in the usual way the minor
determinants in A,
If / is great with respect to 1, then we can replace /—1 by /,

ry’

A Geen, t 23 R
and this quantity by = and keeping in mind that 0 = ae have

Seow nP, VR, %
Uz — No A e . ° , . Fy e ( 2)
Fee Vee

Czy Gr = NI ose (152)
= A

where ¢, and @, are used to denote o, and oz.

We can still modify these equations by introducing the free energy
for the unit of volume filled with the given density. As p = Vy,
we obtain A= V«A (A then relating to the determinant (40) for
wp). Ay, = Vk A,, ete. and we find

ae Se? iy,
POND
ne. * i
ees. Tel. LS,
Ce = ee
V3, N A

Taking into account that 1,,, being the deviation from n,, , amounts
to Vie, we find

RT Ay
Th = Va Sees
5 Meo:
For the frequency & of a deviating system we have
l 2 2
1 ke Ow : O7w

—— = }.— 0)’ eo ee
See 201 1 (dn,? o dn,On, ° ‘o

The probability of a system is proportional to C,, and the logarithm
of thus defined probability is, as I formerly showed, equivalent to
the entropy’). The difference of entropy of the stationary and the
deviating state therefore amounts to

R Allow
: sai |e +
or
ae Gy Oy
ae ot = ‘= op” + -+2 Te 013.02)
The energy taken by the transition ean therefore be expressed by
dhe = Sige » 07
gp On? °Y He 2 pe ebeD «|
The mean value of this energy is
rae
2N
the absolute value being
1 0° 0°yw
zs = aa 1 Pes —s 3
Rr A yw Ow
Wad 1 at ae ae |=
RT
2N

This result agrees with that found on p. 852 of the quoted communication.

5. If x is some observable quantity depending on the densities
Nj)-.N,..n,, in the elements },, then with the help of the given
formula we can easily calculate the probability of a set-of values
wi +-%--%, and the mean squares of deviations. For ys, we have
(limiting ourselves for a moment to a single element and therefore
omitting the index)

0; 05 0
Ks — be = 5, + 5, Ot 5 ee

and so we have

') Comp. Entropy and probability, Proceedings 1912 p, 840.

dn,
From which it appears, that
pees = ET (st) 4. eee ti
Vi, N A (\0n, dn,0n, **
which may also be written
= RE ¥ |
LE ay a ea een ol (ag Min ore. OORee
In the formula D represents the determinant
Bs HOR LH By 1 OB
On, On, One =|

4 dp dp d7y
On, dn,? On,On, On, dng
| ox O*w Ow op
| on, On,dn, On, dn,0nj,
ox vp dy Ow
On; On,Onz On,Onz On;?

With the help of the given values of ¢, and of transformations
which to some degree answer to those already performed, we can
show that the probability of a system in which the deviations of
4%, §,--§--§, are between § and § + d&,, amounts to

onal 2 2
wit® — wie wed de dee ley.

W:
For Jf gee we therefore have

(eae toate Sey)

21D
The mean value of this quantity is
wets 2 AS, IRE
meinen We ID is Oe

It appears from this, that © /og a = @ log a The probability

Eq e
of a state defined with the help of the quantity x therefore also
agrees with the entropy, at least as far as the mean values which
generally are only of importance, are concerned. Instead of the /
partial densities also the function ~ of them can serve therefore to
define the entropy of deviating systems. In the quoted communication

on entropy and_ probability this has been shown for arbitrary
observable parameters. The mean energy of deviation did not depend
on the nature of the parameters, but on their number only; and
also in the case considered it is not the partial density in the elements
but only the number of elements discernible for observation which

plays a part.
Groningen, April 1912.

Mathematics. — “Calculus rationum.” (2.4 Part). By Dr. G. DE
Vries. (Communicated by Prof. JAN DE VRIEs.)
(Communicated in the meeting of March 30, 1912).

§ 16. If in the following remarkable root

0)" = p90, 1)
nv) | v 1
we put vw, the left member assumes the form 1° apparently
indefinite; the right member becomes "—!(u)". Introducing the sign
R for the ratio of two values of a variable lying infinitely close
together, we can write:

Ry | Re ="—(a)r for y="().

This is a mutual root of two ratios lying infinitely close to unity.
If it is now even obvious to introduce in agreement to the preceding
a rational radix as measure for the field of ratio, then the signifi-
cance of a mutual root of exponential numbers is strengthened by
the fact that of the following forms

at
lin — ; limat|b;
ra) he fa)

the latter has no sense, the former has.
If for the comparison of two variables a third is introduced as
independent variable and if we then put
a = ef)
then from this can be deduced:

Az A : Az
eS) = lim wv (1 SE —*) » eF'®) = lim (: — =").
v y

When joining these we find that Az disappears when one of the
mutual roots is caleulated.

ei Pe ee x ALt
eb'"(2): f(z) = lim (1 +- 2) | (1 + =~) = lim yt Ay ‘
y av ¥y

: ype) 5

Introducing for the rational radix the sign ~ R

65
dLx dky
Ry = Ry | Ra = lz,

Without causing confusion we can omit for two variables the
root exponent, and when repeating the operation we can write
[ag A cae Sea

For the rational defined in §6 the above mentioned quantity is
constant, just as the differential coefficient of the logarithms is.

§ 17. General rules for the rationalising are easy to fix; thus
V hw Ru. Rr;
Ruy = (v,~“Ru).(u,~Rv) 5 “Rulv =f, Ru) 3 (u, -R v)} | 2(v);

u--v

VR(ut+rv) =v (Ru). (Rv);
VRe=ell-Ry.
Then the following rational radices often appear:

VRAc)y > = "lal,

UR Le =e 2;

UR at pao (ae

VR srzx =e cre == (arz)—!;
URire = Gin hr x) :

V fiian rs =| ¢.7(x) ;

where we are reminded of the meaning of ¢7, mentioned in § 8;
tan—'r represents here the opposite.

We mention as peculiarity that the exponential function remains
unaltered in this operation.

UR at = ar.

§ 18. As starting point for the development in series of the product

we choose:

wo p!
e—ellv P(x),
1

which formula immediately follows out of
o lpr
oe
ro pl
In a general way we can also deduce the analogon of MAcLatrin’s

series :
wo p! b
09 IT( P(x), UR y1)3 ec ce Pee ee (J)
1

in which the index 1 refers to the values of the function and deri-

vatives for 1. If the ratio in which the independent variable increases

becomes r,, if the corresponding accretion of ratio of the dependent
2

Proceedings Royal Acad. Amsterdam. Vol. XV.

66
variable is called 7,, then the series corresponding to Tayzor’s

is:

serie

ao db! p
yry = flarr) = fle) 0 [VW P(rz), WR f(s)]. . - - ()
1

It can be of service in geometrical investigations of particular
points.

Whilst now z, cannot be developed in a series of sum, it is
possible te find a series of products:

wo p!
Co = @ TIN ado:
1
; at wah ge é
For the following development exists the limitation : 7 il ae
o Pp p—l
Lex). = TV Pe) ee
1

§ 19. For a maximum or minimum holds:
fig =;
From series II (§ 18) follows, that in the immediate vicinity of
the point the change of y depends on the factor:
(rz), P Ry
whose first. efficient is always greater than one, so that the second
efficient decides whether in the point there is a maximum or a

minimuin. +
For the second rational radix we find deduced:

hy ery", Ry :7( Ry).
From this ensues as condition of an inflectional point
Ry v- heg ee
A rational inflectional point is characterized by
i hg A.

In such a point the curve has with the touching rational 3 points
in common. That now the two curves osculate each other follows
easily from the equation of the rational (§ 7).

y'=s A(A—1) ; e@=W Ry ; 80: Ve ey’ = *(- Ry): Vas
so that the preceding condition is satisfied.

The rational of contact in (#,, y,) is given by:

7 = »u Ry,.

7] 1 v 1

When asymptotes (rationals) are at hand, the following formulae

for z, or 7, infinite or zero tend to a definite value
A= Ry, andm= y, : 2,, Ry.

By rational subtangent of a curve we understand the ratio of the
absciss to the absciss of the point of intersection of the rational of
contact with the axis OX,; it is given by

y|\-~ Ry.

The envelope of a series of curves is found in the same way as

in the differential calculus.

§ 20. There exists an integrating operation which reduces the
functions obtained by means of rationalization to the original ones.
It can be regarded as the limiting product of mutual powers, of
which one of the efficients lies infinitely close to unity. It shall be
named mu/tiplcal(-potence); its form is:

A LydLx
‘lim IT (».(1 + = a aad ; F
: Hi

For an indefinite multiplical a constant factor must be added; e.g.

n+
P(x)dLe a eth

P(e'x)4Ll+ — Lic, x)

zt
padi vis (=)
é

P(erx)¢l4 = ¢. srx.
For definite multiplicals the constant disappears; we have to take
into consideration the following rules:

3 2 3
Pydlx— Pydlx,Pyilz , , , . . . . (2)
i 2

72 i 2

keels Padig Shoo, CEE)
7 9p HA

§ 21. A rational is determined by two points: the director exponent

4 = tgp follows out of:
i —_ (2)
ye

If now (x,y,) is a point out of which the rational distance (@) is
measured, then holds

cos 9 sing 2/ a -
| ae ca = EF - =@, and (=) ; (*) =a (D).
vo Yo X, Yo

' For the ratio of two such distances on the line we find:

65
£082 x sins y i
2 ee
z, 4, ?,

This can also be represented by a definite multiplical, of which
the indefinite form is:

V digF Lae? z AA ee
moor P+ aly =tim mal (1+ —)-(1+=)].
2 z y

For the rational this becomes:

va)

It is obvious that we can give to S the name of rational length

of arc. \t represents therefore for an arbitrary curve the limit of
the product of the rational distances taken from point to point; where
thus FR continually changes into the following form:

2 2
S= PL 12° Ry) 4.
i 1 2

For a line parallel] to the X-axis this has the simplest form, viz. -

2
7 *
i az.

The multiplical mentioned in § 20 then becomes if y= y, (constant):

2 z
Py siz = - ’ Ye:
i 1
This represents the rational area of the rectangle determined by

the above mentioned coordinates. For the rational trapezium bounded
by y,, y, and a rational we have

2 z z

P ytlt = —, WY, 9, = Yes
Z, =
when y, is the mean proportional. We can also take that multi-
plical as a power of a ratio of area, when we write:

(2)
x.y)

Also for an arbitrary curve that multiplical will be called the
rational area; it is entirely determined by the limiting coordinates.

§ 22. From the notion “rational area’ is deduced that of “rational
angle” (already mentioned in § 8). In fig. 8 the rational MB determines
with MWA and the logarithmic circle a sector whose rational area is
going to be calculated. The multiplical extended over ABDM is

if namely we put

Lez
f =< cos—l 7

It is evident from the preceding that the first factor is the rational

- area of AMBD. With a view to the equation

PQ PQ SQ
EQ” 8Q~* EQ’
the 2°¢ factor will indicate the rational area of AMBP.
PONSIz dat
lim HT x =(+ a), 7(r)
Extended over the quadrant AMC the multiplical becomes:

e2,1-(r) = (Ur);
so that holds for sector BMC:

70
It is easy to see that the multiplical over MBF is:

P(BMF) = P(BMC): P(FMC) =V 2 =m
u

The rational angle comprised between two rational radii through
M is the second power of the rational area of the figure enclosed
by the radii and the logarithmic circle with radius e and centre
Vf. For the rational area of a logarithmic circle holds:

2 (r) T
For rational length of chord and circumference we find:
r,wand r 2

3y two rationals of centre sectors are cut out of concentric
logarithmie circles whose rational areae form with the second
eradations of the radii a logarithmic proportion. Such figures are in
rational sense congruent.

§ 23. Besides the rational circle functions the rational hyperbolic
functions are of importance. Just as in difference geometry they
appear in the simplest way by the consideration of areae of the
logarithmic equilateral hyperbola with equation:

a(S (9) ee .

Side by side with the current notation of the ordinary functions

we can write: .

bm
|

0 L (a) (x) a
Fig. 9,

1
ch Lu =} (« + =) ; shIlu=} (» — =}
u u

If a is again the parameter the area of a sector is given by:

eee es
eae
——" 71
+z ¢ a > 2]
) ar :. f= Yu or +e
es in connection witb this holds the definition for the “rational
functions”
“ee l :

‘ chr u — hl — (ye)! w ; shr u — eshLu —(ye ete.
= By the substitution

= ad chru 3 ga; shru
“the rational area e TPA (fig. 9) is determined.
: ee
ee ‘Py =Va,y: (Ving 2).
Sa

Now the numerator of the 2"¢ member again represents the rational
: ares of PMA so that the denominator is that quantity for PMT.
The argument of the function is therefore determined by the rational
area of sector M/PTQ. Simpler are the relations for a =e; then

#
| ee (ay L avy = “a= Lay = toes aoe
‘te u y
= out of which again the following relations are formed:

a Se : chru XX shru=e* ; chru:shru= ey
Development of series furnishes

j co 2p! aw (2p—1)

— chr u =e Tu) o snre —— TF
aq 1

2p_,(u).

§ 24. If the eae is calculated for the logarithmic equilate-
ral hyperbola in the equation on the asymptotes, then these functions
appear again.
4 : 7 . »
ay="@) 3 Pyle = ,%0);
2 y a=e leads to a new form for 73 ae
Re P lls Pe | x)dlx,
é€ é€

If this (shortened by P;) is introduced as argument, then

: et isy > skr Pe Vs

fiom which ensue easily the properties; as i.a.

chr P,” — "(chr P;) . *(shr Pz).
The above mentioned curve forms a part of the elementary eo gs
in the roottield. The general equation of these ‘gradation curves” is:

y =m, (w)

In the supposition 2 > 1 we find

x I+1 y I+1
Pytlz—Va,y ; Pe Vy
1 1
So that we find, calling the multiplicals for short P, and P,:
P, | \ 2a — e.

The gradation curves divide the rootfield in such a way that the
mutual root of the rational areae measured along the curve has a
constant value.

§ 25. An equation, in which besides the variables also rational
radices or the rationals of the functions appear, is called a rational
equation. In some cases equations can be solved in which besides
the above mentioned quantities still differential coefficients appear.

I. Required is the curve for which the rational subtangent is
constant. The equation runs :

a ay = a.
In succession we write:
tz |a=Ty\y
P(e\a)¢l« = P(ely)tly
a,(ela = Lic,y)
Yale

This represents the logarithmic curve of arbitrary order.

II. To find the curve for which the rational radix is proportional
to the differential coefficient. Out of the condition :

follows as answer :
é
y =e*= i cpandy =— 2.
P

The last answer is the singular solution and those which by
means of an integrating power can be reduced to such. Fartheron
the rationalisation under the multiplicative sign for which it is easy
to compose the formula.

§ 26. Some of the above mentioned formulae can be extended,
as ia. the 3'¢ formula of § 17.

>>
1 (up)

VRE = (up) =|/ mR ye

If the sum passes into an integral, this formula becomes :

. [yde
UR [yd SS OW EY

From the preceding we can gather that in all respects the field
of difference with the corresponding functions represents the loga-
rithm of the field of difference with the corresponding rational
functions. This can be carried further consistently as regards angles
and areae. By means of a simple “transformator’ we pass from one
field to another, thus we arrive by substitution of

c= e*; y= e* and a=—eA
-in the equation of the logarithmic hyperbola
geass) Nay AS,
at that of the ordinary hyperbola.

Also ambiguous fields can be considered; i. a. the “semi-rational
field’, in which the absciss ascends with differences, whilst the
ordinate changes by ratios. Thus the consideration of the semimulti-

plical :
Patt — 6)
(0) é

has led me to the equation:
P
limp: Vp !\ =e;
io 2)
one thing as well as the other in connection with the “geometrical-

arithmetrical series’.

§ 27. The rational in fig. 8 brought through a point J(a,d)
equidistant with MB, for which we write Jf’ B’ | MB, has as equation:

y oe Ce ae: ;
| SS) i — te
b a : bk a

If a logarithmic circle is drawn having MM’ as centre, r as
radius, then the rational area of the sector, described by JM’ 5’ and
MM’ X’ (|| MX,) proves to be:

: ole
' LAr), tan ¢ (¢ | =) ;

hence the rational angle is

tan—| » e’.
This is as large as the one between MBS and MC, the equation
of MB being

“me.

y
So we can also see, that:

74
BMF See
if namely I’ F’||| ZF and the separation by means of the commas
indicates the rational angle. In one formula we write
PR as A
‘These angles must not be confounded with those of the tangents).
~ Three rationals determine a rational triangle the sides of which
are the rational distances of the points of intersection. These shall

be represented as follows:

3 x 3
led : (). ele.
1 1

By interchange of the letters the value is reversed.
Thus holds:

Be a == CE, 5s
likewise
PHP = &

If the angles are indicated by w,, wu, and w, and if equidistant

rationals are drawn through the vertices, e.g. P,, Q||P,,P,,
L #39, QS, ease

As these are completed by w, to a rational stretched angle, we

find that:

U, us ue ee

. e

2 alias 2 |
% ae Il! i

“4 3 |

A rational right angle is the root out of a rational stretched angle.
If 4, and A, are the director exponents of two rationals, then holds
for the rational angle formed by these:

tru = (e2:e1) | e.(e2, 64) ;
so that the condition for a rational angle becomes:

1 4. Ak.

(6:
§ 28. To get a good insight in the significance of the field of
ratio it is important to name some more theorems out of rational
planimetry.
The rational area of triangle P,, P,, P, is given in:

1 ; diz 2 diz 2 CL
P(m, a2) . P(m, a): P(m, x)
3 1 3

After a few reductions we find the following symmetrical form:

2 3 l £ pe oe
Po PO Pe P= (32). Yo =). i. — ‘
I 2 3 Ly v, ee A
In case P, coincides with M (1,1) the form becomes:
boyy ©) 24ta> a)

If three points lie on one rational, then its value becomes one,
as is easy to see.

For the rational area P, of the rational parallellogram (fig. 10)
holds :

ees 4 2 aya 369 1 2 4 2
fo eer tke PoP = (P > P) : (P: P)
$501 4 La 4.'8 a oy cae
l
in which for short for the multiplicals one letter is taken, e.g. P
3

for area (P,, P,,2,,.7;). Out of the equidistance of the sides follows
immediately :

Ue a SE) Sd Pie Pini) i) Pi
so that two opposite rational sides are equal:

Tae 2 y 2p 2 y
ee 2 Lite = (=) @eae
te ers =] 4 t,)] \Y, ihe

The analogon of the theorem of PytsaGoras can be deduced in
the simplest way out of the equation of the logarithmic circle. For
a rational rectangular triangle placed arbitrarily we have but to
apply revolution about the axis (see § 15). Thus we find also easily
the rational area of a triangle, which is the root out of the mutual
power of a rational side and the rational height let down out of
the third vertex on to it. The considerations of the rational vector-
analysis lead in a shorter manner than the ways indicated here to
the results required.

A word or two must still be said about polar coordinates. The
equation of the rational becomes:

Gr ——0;;
U,

when o is the rational distance M(1,1) to the point of the line and

uw the corresponding rational angle, whilst 9, and w, relate to the

perpendicular-rational out of J.
For the rational area of a logarithmic circle sector we find:

Pr *(g)tl4 = 1(y), —.
Ug bala” 5
The rational, i.e. the multiplical over an infinitesimal sector of a
logarithmic circle is therefore:
2 (vy).
Applied to the triangle J/, P,, P, mentioned in § 28 we find that
multiplical integration furnishes, when P,, P,, P, is a right line:
7(Q,), &r us =*(0,); (G3 | 0,) =e ,9,,.

§ 29. Fig. 11 can give us a good idea of two equal skew ratios.
If P, and P, are points of a rational, we then find two points with
equal rationai distance on an equidistant rational by transferring
successively the abscissae and ordinates or reversely. So here is

34 7, — &,:a@, ; yy 7 Yg = U3 Vass

Fig. 11.

which two proportions are summarized in:
Pei? == eae
The rectangles having P, P, and P, P, as diagonals, are congruent
now in a rational sense. With a view to the above mentioned

proportions the rational sides are equal and likewise as immediate
consequence, the rational areae:

Os) Ya get Ya

’
goth a, Ys
By means of proportional translation we can always construct

5
(i

by way of points a figure which is rational congruent with a given
figure. Rational congruence is of course originated by means of
potential augmenting of the ratios. If in fig. 11 the ratio of the
abseissae is equal to that of the ordinates we have ordinary congruence ;
the points C and D then coincide with 0.

§ 30. In case two of the just mentioned four points coincide,
the points are ‘“corrational” ; the middle point is then situated mean
proportionally. A more general relation for corrational points is

Pee here. or (2: Rj — (R: Q):

R divides the rational distance P,Q logarithmical proportionally

according to:
es =| P
Cee Re AA 2

By drawing the root the logarithms of the rational weights (a, b
and a+ 6) can be varied so that a+6=1. In fig. 11 the points
P torm the vertices of a rational parallelogram of which P, satis-
fying:

A ae ye ae ae 2
is the centre; this point is the geometrical mean of the diagonals.
If now the point ratio is cailed the “freerational vector’, then the
rational distance P,, P, = P,4£: must be regarded as “bound rational
vector” (§ 27).

In the tield of difference a point ratio has no significance, the
product of points only when the exponents are missing. It will
therefore be right to furnish the rationai product with a multipli-
cative sign. By ascending to the rooifield the mutual root of two
points, having no importance for the field of ratio, will represent a
free vector. The product of two free vectors is again a free vector;
this can then be regarded as a resultant of the two. This is easy
to see when we move one of the vectors until one end coincides
with one of the ends of the other vector.

§ 31. It is easy to see the following theorems.

II. The product of point and free vector is a point.

Il]. The mutual power of a point with a free vector is a bound
vector :

P
eee ea tas ha Pas Pe

1
That for three points of a rational holds simultaneously :

3 P;
Per and PoP aaaP ky

78
can be seen by bringing the members of the first equation with P,
in mutual power; we then find:
P,, P,=1:P,,P,=P,,P..
1V. The mutual power of two free vectors is called “‘bivector.”’
This is connected with the rational area of the rational triangle
enclosed by the vectors made to coincide in a point, and the vector
connecting the ends:

ray eas) Sé (PF) x (23):
BoP, P, P, eee
Vv. A bivector is represented by the product of 3 bound vectors.
Simultaneously we find again for a rational triangle
Fe ge Po ae ee
N= (P,; POX Cs F383 Vee Pp ae
VI. A bivector is equal to the product of two equal, equidistant
hound vectors with reciprocal values (fig. 10).
2 Ds
ee (Fr): & ae & P| xX C2 Cn ee ae
VII. The mutual power of point and bivector is a bound triangle;
at the same time the mutual power of a free vector with a bound one
, (Z ; 3) ==(Pe4 Pz ale gs nae ge
VIII. The product of a bound vector with a bivector is again a
bound vector:

(e rx (F er: P
1? 2 PPR) re 3) 4° -

IX. The product of two bound vectors with the same origin is
again a bound vector.

X. Each point in the field of ratio can be replaced by the
product of three points, each provided with an exponent representing
the logarithm of the weight. This can be seen in different ways:

P=E 4 XK £2 X £,® 3 ~a, +a, +4,—1.

We might replace e* by g, we then find:

9, =(P,, £,, £,) | (Z,, E,, £;) ete.

The weights (having the character of numbers), are logarithmically
proportional to the rational areae of the opposite triangles. If P is
the centre of gravity of the fundamental triangle, then the weights
are mutually equal to Be.

§ 32. We must then still mention the difference which must be
made between the outer and the inner power of two rational vectors,
of which the latter is always a scalar. It is natural to take in the

further considerations 2 as base vector; for continuous change the
ends form the logarithmic circle. If then still the mutually perpendicular
vectors 2, and @, are introduced we can write for a free vector:

P, Pp = i <q
BN 1) = 0 = (01) ex) K (Yas &y)s

corresponding to the previously mentioned equation :

#, = vs Ny, (%:)
=a “N
P, av, Y,

For the outer power, which is, indeed, a bivector, holds:

tC) = *(ey) a= ee (Ex ey) — (e, e,)—1 = )
or reversely, according to the choice of the positive sense of revolution,
which is evident from the determination of the multiplical:
— € e — — l 1 1
(ex, ey) = es — [«], = eae (ey, €x) — FP ily = Ly], ieee
é€ C
When introducing the rational angles we arrive for the outer
power and the inner respectively at the following equations:

= U ==
2

(9, 9.) = 9; Q2, S7 vt ’ [9,, 0, | — 0, 9,4, 7 oe 5
1 d

Of this important applications can be made.

§ 33. In the plane the mode of reckoning with complex powers
‘is not inferior to the one with vectors. To determine the situation
of a point in the field of ratio we can use:
Lu

: z(1 a
es =i —— o, eet
é

Z=@O,cru 5; yYy=—O,sru.

1 [-e

1
re eC)

from which ensues:

The multiplication of two directed areae (or vectors) mentioned
in §8 leads to the rational cosinus formula:

w\e
o— 4 ko - *(Q,) - (0. Q., ¢r *:) |
= 3

the mutual power to the analogon of pe Motvrr’s formula:

O11 Oo = 911 Og: Ca VT,
From this can again be deduced
Meru. sr? u) = er (u”) . sri (u”),
besides

N(eMs V—1) =. ou", V—l

b]
which can again serve for the deduction of rational goniometric
relations and for the development in series of product.

Anatomy. — ,,Contribution to the knowledge of the development of

the vertebral column of man”. By Prof. Dr. KE. W. RosEnBere.

(Communicated at the meeting of March 30, 1912).

The investigation, about which I wish to make a communication,
was in the first place made by me with the intention, to test
by new material my view regarding the existence of processes of
transformation. in the vertebral column of man, because this view,
thongh it has been affirmed by several investigators, has been
repeatedly contradicted, also of late years.

Furthermore I wished to make my investigation owing to a plan,
communicated by me a long time ago, to utilize the work in the
preparation-room for a purely scientific purpose °).

In view of both intentions it was necessary to obtain a knowledge
as complete and exact as possible, of the differences in form and
composition, that the vertebral column of full-grown man can
show, and moreover in such a way, that always the whole verte-
bral column and not only a part of it is examined. Neither was it
allowed to make a choice among the objects that were at disposal,
whereby preference was given to rare or more interesting observa-
tions; all the available vertebral columns, provided that they were
complete, were to be used for the investigation. But on account of
the anthropological side of the scientific work in the preparation-
room, I had to put aside the vertebral columns of anonymous per-
sons and of persons belonging to other nations than the Dutch.

Consequently my investigation regards the vertebral columns of
born Dutchmen.

On account of the small number of corpses that were at my
disposal at Utrecht, I was obliged to collect during a period of
time, running from the autumn of 1888 to the end of 1899, in
order to get 100 vertebral columns that satisfied the requirements.

In the period from 1900 till the present day a second hundred
has not yet been obtained.

In the treatment of the vertebral columns I have not followed
the usual method of preparation by which maceration is applied,
because small parts are easily lost when is followed this method and
because in adjusting again the bones of a vertebral column, isolated
by maceration, arbitrariness and inaccuracy cannot be avoided.

1) B. RoseNRERG, Eine vergleichende Beurtheilung der verschiedenen Richtungen
in der Anatomie des Menschen. Antrittsvorlesung, gehalten in Utrecht d. 28.
Sept, 1888. Leipzig 1889, p. 43—47.

E. Rosenserc, Ueber wissenschaftliche Verwerthung der Arbeit im Praeparirsaal,
Morpholog. Jahrbuch, Bd. XXII, p. 561—589. 1895.

I have preserved the objects in alcohol, and prepared them myself
with knife and pincette, by which operation the bones remained
connected by natural ligaments. The preparations are placed in alco-
hol and a number of the drawings have been copied at an enlarge-
ment of °/, °).

If one can agree to the view that transformation-processes take
place in the vertebral column, the examined 100 vertebral columns
can be divided, on account of certain peculiarities of these proces-
ses, into two groups.

One group contains 80 specimens, the other 20. These figures
indicate already, that the first mentioned group is the more import-
ant one. This be therefore discussed first.

Not one of the 80 vertebral columns is perfectly identical with
another. '

Most points of difference are little deviations in form, which how-
ever morphologically are not without signification. If one leaves these
aside, and pays only attention to differences that are so great, that
they can influence the formula of the vertebral column, one sees,
that in the group of 80 vertebral columns ten difierent forms are
represented, which can be indicated by formulas. These are the
formulas Jf to //a and J//e to J//b of the subjoined list; vide
page 82.

As an explanation of these formulas it be pointed out, that the
vertebrae are indicated by figures, denoting their place in the column.
The counting starts from the atlas as the first vertebra.

The vertebrae in different vertebral columns that are indicated
by the same figure, are morphologically equivalent, because it has
appeared, that in case of transformations of vertebral columns no
vertebra falls out of the series, or is newly formed in the series
between vertebrae, that exist already.

According to their form the vertebrae are taken in groups — the
regions of the vertebral column — and the vertebrae in each region

are indicated by letters corresponding with the names of the regions.

The vertebrae of the cervical region are indicated by cv. In the
normal vertebral column this region contains the first vertebra up
to the 7 included.

The vertebrae of the dorsal region are indicated by d. There are
12, consequently the 8 up to the 19" included. They are charac-
terized by the fact, that each vertebra is provided with one pair of
ribs movably united to it.

1) These drawings were demonstrated at the meeting; they will be published
on another occasion. ,
6
Proceedings Royal Acad. Amsterdam. Vol. XY.

The vertebrae of the lumbal region are indicated by /. There are
5 of them, consequently the 20 up to the 24" vertebra included.
Their peculiarity is, that reduced ribs are completely coalesced with
the transverse processes, consequently projecting parts are formed
which are called processus laterales.

The vertebrae of the sacral region are indicated by s. There are
5 of them, consequently the 25" up to the 29" vertebra inclusive ;
they have processus laterales of the same morphological value as the
lumbal vertebrae. But the sacral vertebrae have these processus fused
together at the lateral extremities on either side of the body. This
occasions the formation. of the pars lateralis sacri, with which the
girdle of the lower extremity articulates. The bodies of these verte-
brae fuse likewise together at the formation of the os sacrum.

The vertebrae of the caudal region are indicated by cd. There

LIST OF FORMULAS OF THE VERTEBRAL COLUMN.

IV 1. -1. cv athe 19.23. I 24.—28. s - 20.—32. ca
(If 1.—7. cv Sted 19 ag 24, 28, s 29.—33. cd)
(Ile 1.—1. cv 8. 18. d 19.—23. 1 24.—28. s 29. scd 30.—33. cd)
(Id 1.—1. cv Sige 19,—23. 7 2499: s 30.—33. cd)
(lle 1.—1. cv 8.—18. 219. drab. 23 24,—29. s 30.—33. cd)
IIb 1.—1. cv § 19a 20 soe 24.—29. s 30.—33. cd
Ila 1.—1. cv 21050 20.—23. 124. ls 25.—29. s 30.—33. cd
HE -V.—Isep 8.—19. d 20.—24. 1 25-90. 1s 30.—33. cd
If 1.—1. cv 8.—19. d 20.—24. 1 Cee S 30.--34. cd
He 1.—1. cv 8.—19. d 20.—24. 1 25,—29, s 30. scd 31. -34. cd
Itd 1.—1. cv S19 ed 20 25.—30. s 31.—34. cd
fle 1.—1..cv 8.—19. d 20. di 21.—24. 1 25.—30. s 31.—34. cd
IIb 1.—1. cv 690; 21.—24. 1 25.—30. s 31.—34. cd
Ha 1.—1. cv 8.—20. d 21.--24. 125. ls 26. 30. s 31.—34. cd
i. A—1-c 8.—20. d 2195 7 26.— 39. s 31.—34. cd
fee wees Bat 8-20" 5 a? 26.—30. s 31.—35. cd
(le 1.—1. cv 8.—20. d Mia 26.—30. s 31. sed 32.—35. cd)
07 ES ee Da 8.—20. d A, eat ol 2631s 32.—35. cd)
(le 1.—1. cv 8.—20. d 21. dl 22. - 25, 1 26.—31. s 32.—35. cd)
(6 1—1. ct Gee 22,25. 1 9631s 32 —35. cd)
(la 1.—T. cv 8.—2l. d 22.—25. 1 26. ls 27.—31. s 32.—35. cd)

(J 1—7. cv 8.—21. d 22.— 26. l 27.—31. s 32.—35, cd)

are 4 of them, consequently the 30 up to the 334 included, They
are characterized by a very reduced form.

On the boundaries between the regions vertebrae may be found
showing the peculiarities of vertebrae of two regions.

Between the dorsal region and the lumbal region a vertebra may
occur, bearing on one side of the body a small rib and on tha Sitiee
a processus lateralis. Such a vertebra is called dorsolumbal vertebra
and indicated in the formula by d/.

Between the last typical lumbal vertebra and the first sacral vertebra
a vertebra may exist, touching either on the right or the left with

its thickened processus lateralis the pars lateralis of the sacrum or

uniting with it. This is a lumbosacral vertebra indicated by /s.

Between the sacrum and the first caudal vertebra a vertebra may
exist, not showing on one or on either side the connection with the
pars lateralis, yet being united with the body of the preceding
vertebra. This intermediate form is called a sacrocaudal vertebra
and is indicated in the formula by sed.

Now the ten forms of the vertebral column that are represented
in the group of 80 specimens can be regarded more closely.

One of these forms is the “normal vertebral column” : it has the
formula ///.

The nine otbers differ among each other and with regard to the
normal vertebral column especially in that part that contains the distal
part of the dorsal region with the sternum and the areus costarum
and further all following regions in a distal direction.

In the cervical region likewise differences are to be detected, they
are however not so great, as to influence the formula. Though these
differences are by no means without signification, I shall not discuss
the cervical region, in order not to take up too much time, and
I shall likewise pass over in silence the areus costarum and
confine myself to that part of the vertebral column that begins at
the 18 vertebra; this is in a// specimens the 11" dorsal vertebra.

By many authors the different forms of the vertebral column
occurring beside the so called normal vertebral column, are in a
certain respect contrasted- with the latter.

They are looked upon as variations or varieties or fluctuating
modifications that are a result of the variability of the organism.
These deviating forms are consequently regarded as_ oscillations,
surrounding a constant form, representing the central point — i.e.
the normal vertebral column — either at equal distances or in an
irregular manner.

In my opinion this view which of late years has still been defended
e.g. by Dwicut'), BARDEEN *), FiscHEL *) is not very satisfying.

In opposition to this view I wish to hold another, at which one
arrives when making use of the notions of comparative anatomy
and certain results of embryology.

If we cast a look at the above ten formulas, we are struck by
the difference in the number of vertebrae as regards both the whole
vertebral column and the praesacral and the dorsal part.

In a vertebral column of the formula // 35 vertebrae are extant
in toto, among which are 25 praesacral and 13 dorsai ones.

On the contrary we find in a vertebral column of the formula ///}
in toto 33 vertebrae, 23 of which are praesacral and 12 dorsal.

Now comparative anatomy teaches, that if we leave out of consi-
deration the stages of the vertebral column, which form the beginning
of the phylogenesis of this organ, a comparatively greater number
of vertebrae characterizes a more primitive state. Consequently a
vertebral column of the formula /f is more primitive than a column
answering to the formula ///d.

And as embryological investigation *) has shown us, it is true, that
a lumbal vertebra can be transformed into a sacral vertebra, but
the opposite process has not been demonstrated, and further, because
the study of the development of the vertebral column of man has
proved, that a little rib can fuse with the transverse process of a
vertebra, and consequently can contribute to the formation of a
processus lateralis, but never has anything been observed, which

1) Tu. Dwieur, Description of the Human Spines showing Numerical Variation
in the Warren Museum of the Harvard Medical School. Memoirs of the Boston
Sociely of Natural History vol 5. N. 7. 1901 p. 237—312.

Ta Dwieur, Numerical Variation in the Human Spine, with a Statement con-
cerning Priority. Anatom. Anzeiger. Bd. XXVIII p. 33—40; 96—102. 1906.

*) Ca. R. Barpeen. Numerical vertebral Variation in the human Adult and
Embryo. Anatom. Anzeiger. Bd. XXV 1904 p. 497—519.

Cu. A. Barbers, Studies of the development of the human skeleton. With 13 pl.
American Journ of Anatomy. Vol IV N. 3 p. 265—392 Pl. 1—XIIL 1905.

Compare likewise the chapler written by Barpeen: ‘Die Entwicklung des Skeletts
und des Bindegewebes” in the Handbuch der Entwicklungsgeschichte des Menschen,
herausgegeben von fF’. Keren und I’. P. Matt. Bd. | Leipzig 1910 p. -326,
p. d60—362.

*) A. Viscuet, Untersuchungen tiber die Wirbelsiiule und den Brustkorb des
Menschen, Anatom. Hefte. Herausgegeben von F. Merxet und R. Bonner. Bd.
XXXI p. 459—588. M. Tf. 51—60. 1906.

') Regarding the observations to be taken into consideration here, vide : E. ROSENBERG,
Bemerkungen tiber den Modus des Zustandekommens der. Regionen an der Wir-
belsiiule des Menschen Morpholog. Jahrbuch Bd. XXXVI H. 4 p. 609—659. 1907.

might prove that a vertebra without any ribs is being provided
with the latter in the course of ontogenesis, so, in view of these
facts, a vertebral column of the formula // is more primitive than
others that have fewer praesacral vertebrae and fewer dorsal vertebrae.

Consequently we may take the vertebral column // as our starting-
point when considering the above mentioned 10 formulas.

If now in a vertebral column of this form the 35" vertebra is
completely reduced, the result is a vertebral column of the formula //
which, otherwise, with regard to the composition of the regions,
corresponds with the vertebral column /7. When comparing the
illustrations, however, one can see that in the vertebral column //
the 13 pair of ribs consists of smaller bones and that the processus
lateralis of the 25'" vertebra are thicker, and that they are likewise
nearer to the pars lateralis sacri.

These are but little differences of form, but they are forerunners
of greater ones.

This is already seen in the specimen, representing the formula //a.
Here the 25 vertebra is a lumbosacral vertebra. :

This state of things becomes intelligible, when we consider, that
the sacrum is formed, because the girdle of the lower extremities
rests on the vertebral column and that therefore a number of vertebrae
fuse. Further one must pay attention to the fact that the girdle of
the extremity, (being the ossa coxae), is not connected with the
whole extent of the pars lateralis but only with a proximal part of
it. This fact shows, that the pars lateralis did not come into existence
at once in its whole extent, but developed successively, and the part
of the pars lateralis that in a given vertebral column is in connection
with the ossa coxae, has been formed later or is younger, than the
part lying more distally; this part was previously connected with
these bones, but lost this connection because the girdle of the extremity
was displaced in a proximal direction.

At first sight this view seems to be a very hypothetical one, but
it can be proved.

Let»us suppose that the girdle of the extremity in a vertebral
column of the formula // be removed only a little in a proximal
direction, then the 25 vertebra is more strongly influenced by the
ossa coxae. The more intense functional requirements cause a stronger
development of the processus laterales, which can soon increase so
much, that on one side of the body the thickened processus lateralis
touches the pars lateralis and unites with it. In this way the
25t vertebra can become a lumbosacral vertebra.

This has been the case with the vertebral column //a, where the

thickened processus lateralis is already connected with the right hand
os coxae. Moreover the vertebral column //a shows, that the 13" pair
of ribs is still more reduced; they are still only little pieces of bone
which are however movably united with the processus transversi.

In the vertebral column J/c we see, that the 25" vertebra is on
both sides of the body attached to the pars lateralis and has con-
sequently become the first sacral vertebra. And as in the distal part
of the vertebral column no important modification has taken place,
we find now a sacrum consisting of six vertebrae. At the same time
at the 20% vertebra on one side the rib has fused with the vertebra,
on the other side the rib has remained extant. Consequently the
vertebra has become a dorsolumbal vertebra. Now there are only
4 lumbal vertebrae extant, as is likewise the case in //a.

The next form, //d, develops, when, on both sides of the body,
at the 20% vertebra rudimentary ribs have disappeared as independ-
ent parts. This vertebra has now become the first lumbal vertebra ;
there are again 5 lumbal vertebrae, and in the praesacral part the
arrangement has taken place that characterizes the normal vertebral
column. In the sacrum there are however still 6 vertebrae to be found.

In vertebral columns of the form //e the praesacral part is con-
form to that of //d. At the distal extremity of the sacrum, however,
now peculiarities can be observed, showing that the 30'" vertebra
is loosened from the sacrum. [n the specimen represented the pars
lateralis is interrupted between the 29" and the 30 vertebra on
the right side of the body, in other specimens this is the case on the
other side or on both sides; in these cases the 30% vertebra is only
connected with the sacrum by its body. In all these cases the 30th
vertebra has become a sacrocaudal vertebra.

If now the 30% vertebra is separated from the sacrum also with
regard to the body, then a vertebral column is formed that is indi-
cated by the formula //f. This has a sacrum composed again of 5
vertebrae. But now of course 5 caudal vertebrae are extant, because,
as already in the form //, the 34 vertebra still closes the series.

The consequence of a complete reduction of the 34'> vertebra is
a vertebral column of the normal form; the formula is indicated by
/I/, which has been done for good reasons.

If we compare namely the formula /// with the formula /7, it
appears, that the dorsolumbal boundary, the lumbosacral boundary,
and the sacrocaudal boundary have all three been displaced one
vertebra in a proximal direction, and that at the end of the vertebral
column one vertebra has disappeared.

It is not for the first time that in the so-called normal vertebral

column displacement of the boundaries of the above-mentioned regions
has caused the existence of 5 lumbal, 5 sacral and 4 caudal vertebrae
but, as can be shown with great probability, it is for the third time
in the course of the phylogenetical development of the human ver-
tebral column. In vertebral columns of the formula // it is the
second time that such an arrangement has taken place. This follows
from observations in a vertebral column, in which, in so far as at
present the history of the human vertebral column is known to us,
for the first time groups of 5 lumbal, 5 sacral, and 4 caudal ver-
tebrae have appeared. These observations will be cited afterwards.

This induced me, to divide the formulas into groups indicated by
figures. This facilitates the general survey and gives, as will after-
wards prove, still another advantage.

Now .we have still to look at the formulas ///a@ and J/Tb.

From the formula ///a it appears, that now the 24t vertebra
has obtained a lumbrosacral form. And the illustration shows, that
the 12" pair of ribs is a little shorter than in the vertebral column
[11. This points to a beginning reduction of the mentioned pair of ribs.

The form ///a is evidently analogous to the form //a and, like
this, the vertebral column ///a shows that a removal in a proximal
‘direction of the girdle of the extremity occasions a modification in
the composition of the regions, and that the formation of a lumbo-
sacral vertebra is again the first act in the progress of the trans-
formation-process.

The formula ///6 and the sketched specimen represent a further
advancement of the process. The 24 vertebra has now become the
first sacral vertebra, we can, however, easily conelude from the form
of this vertebra that from a lumbal vertebra it has been transformed
to a sacral vertebra. Of course there are now again 6 sacral vertebrae,
as in the case of the sacra of //c and //d. In vertebral columns
of the form ///b we see distinctly. that the 12" pair of ribs has
been reduced still more; in one of the specimens it is almost as
little as the 13% pair of the vertebral column /7.

If we take now a survey of the ten forms of the vertebral column
just discussed, we may, in my opinion, assert that the view as if
nine of these forms should only be insigniticant oscillations of the
organisation, surrounding as variations or varieties a constant form
— the normal vertebral column — in an irregular way, does not
explain the stated facts in a satisfactory manner. On the contrary
these facts confirm the view I have defended long since.

It is so clear, that the discussed forms of the vertebral column
are parts or links of a morphological succession or chain (morpho-

logische Reihe) that when deseribing the forms I could hardly help
assigning a share in this description to the part of the phylogenetical
development that is to be inferred from this chain. |

Because the separate forms can be joined together freely and in
a definite direction to a morphological succession, it is clear, that
there is no contrast between a normal form of the vertebral column
and varieties. All these ten forms are principally of equal value;
they are representatives of stages of development, following each
other successively.

The so-called normal vertebral column is the form that is at
present numerically predominant.

Vertebral columns representing the formulas /f to /// are retarded
forms that have stopped at different stages, preceding stage //J.

And of course forms with a formula as ///a or ///b must be
regarded as forms of a higher development than the normal vertebral
column, having the value of future forms.

It seems to me that this view is more satisfying than the oles
and at the same time admits of the possibility of a certain appli-
cation, which the other does not allow.

The application, I] mean, becomes evident, when we pay attention
to the fact, that the stages of development hitherto stated distinguish °
themselves, with only one exception, by only one phenomenon of
transformation that can be indicated in the formula. The distance
between each other of these stages of development is consequently
in a morphological sense the same.

- This is the case with the stages Jf to //a and J/e to IIb.

If however we compare the forms //a and //c, we see that in
the latter two phenomena of transformation are present, namely
a transformation of the 25'" vertebra into a first sacral vertebra,
and of the 20 vertebra into a dorsolumbal vertebra.

The distance between these two forms is consequently greater
than between the others. This suggests the supposition, that between
the stages //aw and J/c a stage might exist, characterized by the
fact that the 25 vertebra has already become a sacral vertebra,
whilst the 20° vertebra has still remained the last dorsal vertebra.

To this answers a formula //6, which I have inserted into the
series provisionally as an hypothetical one. I have in vain looked for
such a form among the 100 vertebral columns under consideration.
When studying the specimens, which I am collecting for the second
hundred, t have however found the designated form of the vertebral
column and even three times.

The formula //4 is therefore no longer an hypothetical one,

fey

The confirmation of one deduction of such a nature causes us
to construe others from the observations we have made.

Now that the series of formulas from If to 111b shows no longer
an hiatus, it is possible, proceeding from the extremities of the series,
to follow to a certain degree the process of transformation forward
and backward, and to indicate the stages. by hypothetical formulas.

The formula ///d is analogical to the formula //+, and in analogy
to the formula //c we can add to the formula ///4/ a formula ///c,
indicating that the last dorsal vertebra of ///4, the 19" of the
series, has become a dorsolumbal vertebra.

When, by reduction of the rib still existing on one side of the
19%" vertebra, this becomes a first lumbal vertebra, then we have
the form J//d, in which, as in ///4 and ///c, a sacrum consisting
of 6 vertebrae must be extant.

Now we can imagine, that the 29 vertebra becomes a sacrocaudal
vertebra and thus the formula ///c is given.

And when now this 29 vertebra has passed into the series of
the caudal vertebrae, the result is a vertebral column having the
formula ///7, which, as the formulas I1f and /f, is characterized by
the existence of 5 caudal vertebrae, the last, however, is now the
33° of the series.

The reduction of this 334 vertebra gives a formula / V, an anologon
to formula ///, and now once more the dorsolumbal boundary, the
lumbosacral boundary and the sacrocaudal boundary have been
displaced one vertebra in a proximal direction, and at the distal
extremity one vertebra has disappeared. Consequently for the fourth
time successive groups of 5 lumbal, 5 sacral, and 4 caudal vertebrae
would be extant.

I have not hesitated to mention these conclusions. because formula
IV may indeed not be considered to be a hypothetical one. A verte-
bral column of this composition has been described more particularly
by Texcuint') in Parma, who however adheres to the then already
refuted doctrine of excalation, and supposes, that the 12 dorsal
vertebra with its ribs is entirely missing. A similar vertebral column
has also been observed and briefly described by Brancui*) in Siena.

Whether this process whill continue further, cannot be said with
certainty ; it might be possible.

1) L Tencuint, Mancanza della dodicesima vertebra dorsale e delle due ultime
coste etc. L’Ateneo Medico Parmense, Anno 1. Fasc. 2 p. 97—132. Parma 1887.

2) S. Brancnt, Sulla frequenza delle anomalie numeriche vertebrali nello scheletro
dei normali e degli alienati. Atti della R. Accad. dei Fisiocritici in Siena. Ser. IV,
yol VII Fasc. 1—2. p. 29, osservazione V. Siena 1899.

Now, proceeding from the actually observed form //, one might
cast a look into a comparatively ancient period of the history of
the vertebral column.

If in analogy of the formulas ///f to // one were to construe
succeeding formulas to the formula //, the first in succession would
be a formula, denoting the 31s vertebra as a sacrocaudal vertebra: Je.

The latter must be preceded by a form of the vertebral column
in which the 31st vertebra is the last and moreover the sixth sacral
vertebra: Jd. Here the 2J8* vertebra must be the first lumbal vertebra
as in the formulas //c to Te.

Inasmuch as now a first lumbal vertebra is developed from a
last dorsal vertebra, after it has passed through the stage of a
dorsolumbal vertebra, the next following more primitive form must
possess the 21‘ vertebra as dorsolumbal vertebra, as is indicated in
the formula /c.

And this must have been developed from a form in which the
91st vertebra is the last and moreover the 14‘! dorsal vertebra, which
characterizes the formula /6. In this formula the 26 vertebra is the
first of a sacrum, consisting of 6 vertebrae. A first sacral vertebra,
however, develops from a last lumbal vertebra, after it has been
lumbosacral vertebra.

Consequently we can imagine a formula, showing the 26 vertebra
as lumbosacral vertebra, in which at the same time 14 dorsal vertebrae
and 4 lumbal vertebrae are extant, besides a sacrum, consisting of
five vertebrae. This is indicated in the formula /a.

And if now we go one step more backward, then it must be
possible to find a vertebral column in which the 26 vertebra is
the last and moreover the 5 lumbal vertebra, then a sacrum of 5
vertebrae must follow and 4 caudal vertebrae must succeed to this,
the last of which is the 35 vertebra of the series. This gives the
formula /.

With regard to the formulas /e to /a I must admit, that they
are purely hypothetical; with regard to formula J, however, I
should wish to cite an observation, answering almost entirely to this
formula.

First I must, however, briefly fix the attention to a peculiarity,
occurring in vertebral columns standing on the ten stages mentioned.

If a special stage is represented by more than one specimen we
see in these specimens differences that have a morphological signification.

As an example I wish to cite the stage ///a, which is represented
by three vertebral columns.

One glance at the illustrations is sufficient to see that these three

91 6

specimens form a morphological progression, demonstrating a beginning
of the reduction of the 12™ pair of ribs.

At the same time it is very clear that these three specimens cannot
be directly derived the one from the other, that consequently they
do not form what might be called a descensional succession.

This shows the 24 vertebra. In specimen 1 the contact with the
sacrum has been formed on the right side of the body, in the two
other specimens on the /eft side. These three specimens consequently
belong at least to two successions that have diverged, be it only in
a slight degree.

And if in the specimens 2 and 3 we carefully examine the pars
lateralis, then it appears from observations, which we cannot enter
into particulars upon here, that the specimen 3 which, with regard
to the twelfth pair of ribs, is higher developed than the specimen 2,
is, with regard to the facies auricularis, more primitive than the
specimen 2. Thus, likewise between these two specimens, there exists
a slight divergence of development. All three specimens are conse-
quently the extremities of three independent progressions of develop-
ment, though they may be only very short.

As a second and last example the two specimens representing the
stage ///b may serve.

We see that the reduction of the 12'" pair of ribs has reached a
higher degree; in the specimen 2 these ribs are already so little
that they look much like much reduced 13 ribs. Together with
the specimens of the stage ///a these two specimens exhibit, in the
most convincing manner, the gradual reduction of the 12'" pair of ribs.

The 24 vertebra is in the stage ///6 first sacral vertebra, and
it is obvious that, in specimen 1, it is transformed in a slighter
degree than in specimen 2.

With regard to these points (I leave other points out of discussion)
specimen 2 is doubtless the higher developed one. That this specimen
does not after all directly continue the line of development of spe-
cimen 1, but deviates from it divergently, appears from the position
of the facies auricularis, which in specimen 2 is a less transformed
one than in specimen 1. This is likewise seen, when considering
the 30% vertebra. In specimen 2 this vertebra has still cornua coce-
eygea, whereas these have already almost completely disappeared in
specimen 1. This points likewise to divergent development.

This divergency of development is shown by all specimens belonging
to any stage. It is however so slight that the specimens remain un-
mistakably within the boundaries of the separate stages.

It is however of importance to ascertain this divergency, because

- 92

it enables us to interpret the vertebral columns in the second, smaller
group.

One need only suppose, that the divergency of the direction of
development increases more or less, then forms must originate that
do no longer fit in the frame of the separate stages, but are con-
nected with every stage as accessory forms, as they might be called.

These forms remain by local, relative retardation or by local
acceleration of the transformation, either below the stage, to which
they belong, or they are a little more developed. But always they
diverge from the direction that leads from one special stage to the
other, and thereby they form. as it were, side-branches, which are
however very short, because the several accessory forms are, as a
rule, only represented by one single specimen.

The second group contains 20 vertebral columns, and these represent
17 different forms that can be denoted by formulas.

Only as one single example I wish to cite an accessory form,
belonging to stage //. In this stage the 20% vertebra is the 13%
dorsal vertebra; if this vertebra through comparatively too rapid
transformation becomes a first lumbal vertebra, whilst the other parts
of the vertebral column remain unaltered, then a vertebral column
has been formed with 6 lumbal vertebrae. And we see that this
column has not followed the line of development leading to stage //a,
because to this stage only 4 lumbal vertebrae belong. It has followed
a side-path that leads away from the main-route and soon ends.

Let me mention a second example.

In the list of formulas stage ///b is followed by a hypothetical
stage ///c, in which the 19 vertebra is a dorsolumbal vertebra.
1 have now found a vertebral column, belonging to the second group,
in which the 19" vertebra has this form. To the left exists a pro-
cessus lateralis and to the right a rudimentary 12 rib, which is
about to fuse with the vertebra.

Further we find 4 lumbal vertebrae and a sacrum, consisting of
6 vertebrae, the 24 tothe 29", as must be the case ina stage ///c.
In so far everything agrees with what is indicated in the hypothe-
tical formula. But the vertebral column I am dealing with, has only
3 caudal vertebrae and not 4, as the formula requires, the 32°4
vertebra is the last.

Consequently I cannot regard this vertebral column as a repre-
sentative of a stage ///c; but it may be conceived as an accessory
form to such a stage. By acceleration of the transformation at the
distal end the 33°¢ vertebra has been reduced comparatively too early.

It seems to me that this observation makes it very probable tbat

it will. be possible, to find the stage ///e, which for the present is
still hypothetical.

Principally in the same way the probability of the existence of
the most primitive stage / can be shown.

This appears from observations I was allowed to make on a ver-
tebral column in the anatomical institute of Leiden. *)

On account of the existence of articular planes on the 20% and
the 21s' vertebra it is certain that these vertebrae were provided
with movable ribs that were missing in the preparation.

So here 14 dorsal vertebrae are to be found as formula |
requires. Further we see 5 lumbal vertebrae, the 26 vertebra is
the last lumbal one, then follows a sacrum, consisting of the 27" to the
31st vertebra, as the formula indicates. The caudal vertebrae of the
preparation are defective, so that we cannot know whether the 35
vertebra was the last. The 32°¢ and the 33" vertebrae are extant
in the preparation, they have however a sacrocaudal form.

Consequently this vertebral column does not answer entirely to
formula /, it is a little more primitive and* may be regarded as an
accessory form to a stage /.

The examples cited show that the aecessory forms can likewise
be explained, if we admit the view, that the various forms are not
irregular varieties, but the consequences of special processes of devel-
opment.

Having this view, we need no longer explain the existence of the
various forms by the so called variability. This does indeed not give
an explanation at all, neither does it make us understand that the
great majority of the vertebral columns forms a_ morphological
progression.

The observations I have made, become however intelligible, if we
consider that when a species, consisting of many individuals, is ina
state of phylogenetical development, it would be highly improbable,
that all the individuals should be transformed with exactly the same
rapidity.

If there is, however, a difference of rapidity or intensity of the
transformation, then it is evident, that, at a given period, in indivi-
duals living at the same time, very different stages of the process
of development of the whole species will be represented by groups
of the individuals.

And this is what we have seen.

At the same time it is clear now, why the great majority of the
1 E. Rosenserc. Ueber eine primitive Form der Wirbelsiule des Menschen
Morphol. Jahrbuch Bd XXVII, H. 1. p. [—118, Tf. E—V. 1899.

individuals form a continuous progression of stages of development.

If we survey the whole progression, we can observe that the
difference, existing between the most primitive stage and the highest,
is greater than the differences in the composition of the vertebral
columns not only in some species, but even in several genera of
Primates.

Consequently it is not an unimportant part of the history of the
human vertebral column that the formulas allow us to survey.

Three dorsal vertebrae have successively become proximal lumbal
vertebrae, three distal lumbal vertebrae have the one after the other
been lodged in the proximal part of the sacrum, and from the distal
extremity of it gradually tree vertebrae have passed into the caudal
region, which bas lost three vertebrae at the extremity. :

The diminution of the number of praesacral vertebrae does,
however, not necessarily involve a shortening of the trunk; by
measurements we can come to the conclusion, that in the higher
stages the bodies of the vertebrae become higher and this occasions
a compensation. ;

In the sternum and the arcus costarum, too, analogous modifications
take place. 3

All these observations justify the notion, that in the region of the
trunk an important transformation is working; the processes in the
vertebral column can certainly not take place, if the parts of the
body, surrounding this extensive organ, do not participate in the
transformation.

The knowledge of these processes must consequently exercise an
influence on the descriptions which systematical and topographical
anatomy give of the composition of the trunk. Both branches of
science pay too little attention to the transformation of the organism.

I cannot enter into further details on this subject now; in con-
clusion I wish only to point out in a few words the importance of
the series of formulas with regard to anthropology.

This becomes apparent when we consider, how the vertebral columns
are arranged by the series of the stages.

The result appears from a graphical representation *).

On horizontal lines, answering to the stages, the specimens belonging
to each stage are indicated by dots.

At the end of each line the accessory forms are indicated by marks,
placed either a little lower or a little higher, further is denoted, what
characterizes each accessory form.

The rows of the representatives of each stage have been placed

') This will be published in another communication.

7 *

_ Bos

symmetrically in relation to a line, indicating the route or course
that is followed by the transformation of the species. If we consider
this representation, it is in the first place remarkable that the so-called
normal vertebral column has not the absolute majority, but only a
relative one. There are in the stage /// 26 vertebral columns

Further the attention is drawn by the fact that the stages //e and
TIf contain a rather great number of specimens.

In the stage //e the 30° vertebra is a sacrocaudal vertebra. The
loosening of this vertebra from the sacrum is morphologically a com-
plicated process; it is therefore clear that it is not so soon finished,
and that consequently a rather great number of individuals are at
the same time in stage //e. There are 23 of them.

In stage //f 5 caudal vertebrae are extant, the last is the 34%
vertebra. This must be reduced, then the stage /// is attained. The

reduction of this vertebra is morphologically a comparatively simple

process, consequently there are fewer specimens found in this stage
than in stage //e. This reduction, however, is physiologically of little
importance; this may be a reason of retardation of the process, so
that after all as many as 14 individuals have stopped in this stage.

It stands to reason that the more primitive and the most modified
forms are found only-in small numbers in the relative stages.

As the series of the formulas allows of an arrangement of the
examined vertebral columns, this series gets the value of a scale or
standard by which we can ascertain the degree of development,
reached by the examined organ for every group of men that can
anthropologically be distinguished.

It is true the number of 100 vertebral columns is not sufficient
to pronounce a decisive opinion in an anthropological regard,

But in a methodological regard the result we have obtained is, in
my opinion, sufficient to confirm the conviction, that, by this method,
when many individuals are examined, it is possible to fix for every
nation the degree of development, attained with regard to the organ
examined or to other organs, provided that for each a series of
stages be established.

So I am of opinion that it would be worth while applying this
method of investigation to races of men that in anthropological
regard stand widely apart from each other.

This might be done, if in preparation-rooms of various countries,
provided with the required number of corpses, the same investigations
were made. ;

It is very likely that rather different arrangements of individuals
by the scale of the formulas would be found, and that it would

be possible to characterize anthropologically the different races of men
by indicating the differences in the character and the intensity of
the processes of transformation.

And if the vertebral column should be chosen for such an inves-
tigation, an opinion about the degree of organisation attained would
certainly not rest on too narrow a basis, as the vertebral column is
in contact with many organs that surround it, and actively or
passively participate in its transformation.

Physics. — “On vapour-pressure lines of binary systems with widely
divergent values of the vapour-pressures of the components.”
(In connection with experiments of Mr. Katz). By Prof. Pu.
KonnstamM. (Communicated by Prof. vAN DER WAALs).

§1. General character of the vapour-pressure lines derwed from
the differential quotients. The theory of the p,c-lines of binary mixtures
was developed by van per Waats in Verslagen Kon. Ak. v. Wet.
(3) 8 p. 409 and These Proc. III p. 163 (See also Cont. H p. 120
et seq.) on the supposition that the quantity «,, occurring there may,

qd —

dx : ae
be represented by —-—— , and so is only dependent on the critical
av

temperature of the mixture taken as homogeneous. VAN DER WAALS
showed later on that a further approximation may be obtained by
the introduction of the quantity p., the vapour-pressure of the
mixture taken as homogeneous. Then:

while 4

In a recently published paper’) I showed that a number of
particularities of the vapour-pressure lines follow from these equations.
Since then Mr. Karz’s investigations *) and the results communicated

obtained was °/, 2. lt was mentioned during the discussion at the Conseil Sotvay,
Noy. 1911 that Professor Kamerunen Onnrs and myself had undertaken an inves-
tigation of y,,, by Kuypr’s method for hydrogen at temperatures down to that of
liquid hydrogen, but this investigation has not yet been completed.

1) ‘Zschr. f phys. Ch. 75 p. 527.

*) These Proc. Vol. XIII p. 958.

in a paper by Mr. Timmermans and myself *) have drawn my
attention to some other conclusions from the formulae derived
].e. particularly with regard to systems the components of which
differ much in vapour pressure. I shall deal with this in the following

pages.

will ascend or descend with increase of x, according as

Let us first give the formula? which we shall want. A p,t,-line

dp,
di

positive or negative. Let us call the substance with the Jarger value
of bethe second component (z= 1), and put:

=a Aha. a." = Pa,a,
tly a 1 i i
—=9 —h 2, — m, —=—
b, b, ky T';,
then
dl of
( 4 —— ay Mes cae +2(kl—1—29) . . , (1)
adr Jr m, 7

dlp, 2 l f
== =—— {| 1--h—— } + 2([ 1—2h—_-] = . (2)
daz z—"* m, k k

The question whether the p,z,-line is concave or convex downward

at the border, depends on the sign of

lpe

will have the same sign as —

dlp. . : d*p
- in this way that a

aL a

for a line that ascends from the

border, or if it descends so long as 7, >’/,, resp. 1—r, > 4(1—z2,).
If z,<*/,#, resp. l—«,<('/,(1—<,), the vapour-pressure line is convex

d?l

when

Gr te .
is negative, and concave when

d?lp,.

is positive. Also the

stability or unstability of the liquid phases depends on this quantity.
We are, namely, on the verge of stability when:

d?lp.

1 + 2, PY ea = 0

= hae?

So we are certain to be in the stable region everywhere where

d?lp,

then (for not too small value of #1—z«

- ta 2 dl € 4
ee positive; if on the other hand = has a large negative value,
& Lc

we shall be in the unstable

region, i.e. unmixing will take place. Expressed in the quantities
defined just now we find for the required value at the two borders:

5) These Proc. Vol. XIII p. 865.

Proceedings Royal Acad, Amsterdam, Vol, XV.

| db
d?lp-_ ie : da*
oPe\ + |2+489?+8g9——— +4.2k*—lk(4 + 8g)\ +
da = a—0 m, b, 1
d*b
p ar
Bet ame dete wi ries oT See see
1
d*b |
d?lp, A paws? 7 ans ot
== — —+ |24 8h?—8h— ——(4—8h)\ +
( da? = m, each b, + ke? ok ( » |
d*b
Al — te gh? 2 Sia da? (4)
== x — i = L 2 a b . . 5 ° .

2
Now we arrive at a surprising result when we apply this formula
to systems whose molecules differ much in size. If e.g. 6, is = 100 3,,

b :
then ae becomes — 22.4 according to the well-known formula of

Lorentz; so g = 21,4 and h = 0.776. If we further suppose 4 = 20,
1 1
so: that. 7, = 47%, P= 55 Pky and m, = 7m equations (1) and

(2) become:

lp. af
( 4 =" ~ 7 (a—22.4) + 2 (kl—43.8).-. . . (la)
— m,

da —-

dlp. 27 I l
—_ 4 [0,224 = | 222 reo ee
(Ze) =m, (04g) A(R) ee

dlp,
So we find /—1.04 for the value of / which makes ( P )
dx z—0

equal to O for a temperature m,—=4 and the supposition f= 7;

Ip, . = :
for smaller values of / (- Ps) is then positive at this temperature,
at /xz=0

for larger values negative. Equation (2a) shows further that for
values of /< 4 the p,a-line ends descending for the second com-

. ap : Pe
ponent. So = has the same sign on both sides for /= 1.05. But
&

between a region of non-miscibility will be found. For with the
values mentioned equation (3) passes into:
I? lp,
@ =) — — 14/4525—3504 1} + 801-1600 2 + 4237 . (3a)
av” /xr=0

With a value of / in the neighbourhood of 1 the lefthand member
becomes of the order 10—!; so the curve is at first concave down-

SH,

7
V ward, but already for a value of « of the order 0.0001 unstable
esis es are reached. On the other hand equation (4) passes into:

am: iS

eB
a = — 56 {— 0.507 - 0.11041} 4+ 0.21 — 0.017 + 0.581 (da)
i

‘<
=

and so this value becomes (with / about 1) of the order + 20. So
on the righthand side the p,c-line will be concave downward, and
_ we shall have to get very far from the border before meeting with
a region of unmixing.

If we put 6,=10006 instead of b,=1004, we get the equations:

(€£)s- (il—156) + 2 (ll ~ 831 ag eee)

= — + (0.165 —)—2(0.608 + z): ae ee |
ia

a, fal
be Pe\ _ __ J (917800-4-24*—192418) 44k — 40°? 424° -+.215000. (38)
~~ ‘ da? 0 my,

2 @lpe f D) l 1 2 2

| yy ae 67 4

. ( da* )= m,| a 4 ge Bieter

and if we now suppose = 638, so that again 7),—= +77, all our
_ conclusions remain of force, and the peculiarities which we pointed
— out (insolubility on the side of the small molecule ete.) are still more

b, .
pronounced. And also values of = considerably smaller than 100 still
1

yield the same results.
Summarising them we must say that or the systems considered
with a value ‘of about /—1 the p,z,-line begins at the side of the
small molecules slightly ascending concave downward, that, however,
already with exceedingly small concentration a region of unmixing
is reached, which lies very asymmetrically in the lefthand side of
the figure, and that the p,z,-line after having left this region of
- unmixing, continually descending and finally convex downward reaches
the line for the second component.

§ 2. The experimental results of Mr. Karz.

Now it is very remarkable, that this course entirely agrees with
_ that of the vapour-pressure lines determined by Mr. Karz for the
majority of “swelling’’ bodies, those with limited imbibition- power.
Here too on the side of water an exceedingly small line (generally
so small that it cannot even be determined experimentally) is found

__ for the solution of the swelling substance in water, and on the other

100

side of this very asymmetrically situated region of unmixing just
such a line as was described just now.

No doubt we are not justified in concluding from this agreement
that the substances to which Mr. Katz’s figures refer, satisfy all the
conditions that we bad to put in order to be able to arrive at our
conclusions; to apply the law of corresponding states to casein and
haemoglobin must certainly be called a very bold generalisation,
even apart from the other suppositions on which our formulae are
founded. Still I thought this agreement striking enongh to justify a
closer investigation for the solution of the question in how far the
experimental particularities found by Mr. Katz would have to be
expected in virtue of the simplest theory for a mixture of two per-
fectly normal components, when the ratio between the size of the
molecules, ‘x/,,, becomes very great. Mr. Katz was so kind as to
summarize the results of his measurements for me as follows :

1. If we draw the water-vapour tension of the swelling substance
as function of the molecular percentage (vAN DER WAALS’s p, .7-curve),
we get a line which (ef. fig. 1, which represents the line for inulin
in proper proportions *)):

a. lies for not very small values of « (pure water) under the
value which the vapour tension would have if van ’r Horr’s law
p=p, d—2) held for all concentrations.

6. begins almost horizontally for « about 1, and does not begin
to rise abruptly until past «= ’/,.

c. turns its convex side downward for a about 1, then gets a
point of inflection (for smaller 2), and finally turns its concave side
downward for very small value of z.

d. presents an excentrically situated region of unmixing for very
small w, so excentrically as has not been observed anywhere else as
yet. Pretty well pure water «= 0.00001 coexists with «= 0.002 or
Q.006. The lines for casein (albumen) and inulin (polysaccharide) may
serve as an example. For both substances the minimum molecular
weights have been taken (casein = 4000, inulin = 1800) in all these
calculations. If higher values are used, the above-mentioned properties
are evell more pronounced.

*) In this figure of Mr. Karz the component with the smaller molecule (water),
has, however, been thought on the right hand, whereas in the text it has been

assumed, where the contrary has not been expressly stated, that the molecular
weight increases from left to right.

0.90

0.60

0.50

0.20

— ES ee ee

0.80 0.70

Inulin

Pf,
Bs

0.962
0.914
0.853
0.788
0.596
0.410
(.176
0.022
0.01

101

0.60 0.50 0.40 0.30 0.20 0.10

0.004
0.014
0.018
0.021
0.024
0.031
0.041
0.062
0.178
0.29

( ase

0.962
0.917
0.853
0.788
0.596
0.410
0.176
0.022
0,01

102

9. The heat of mixing (generation of heat when 1 er. of dry
substance absorbs 7 gr. of water) is strongly positive, and is very
well rendered by a hyperbola:

3. The volume contraction ¢ by tne mixing (in cm*. when 1 gr.
of dry substance absorbs 7 gr. of water) is strongly positive, and fol-
lows a line which closely resembles a hyperbola.

c pele os ; , é
4. If we compute = for small 7’s (lim. 7=0), we find that this

quotient is of the same order of magnitude for the most different
swelling substanees viz. between 10 and 25 >< 1O-+*, and that this
quotient is of the same order of magnitude as for mixtures of sul-
phurice acid, phosphoric acid, and glycerin with water.

The analogy of the latter substances with the swelling substances
is the more striking, because they present all the properties described
under 1 (a, 6, and c), under 2 and under 3 exactly as for the swelling
substances. There is only one difference: they are miscible in all
proportions, whereas some swelling bodies exhibit the characteristically
excentric region of unmixing described under 1d. Other swelling
substances have an unlimited power of imbibition, but behave for
the rest as described above. So this difference will not be essential.

Limited or unlimited miscibility, it seems, may depend on small
factors, as closely allied substances may belong to different types. Further
quantitatively there exists this difference that for the swelling sub-
stances the vapour pressure line begins to ascend much less steeply,
the lines for the volume contraction and for the heat of mixing on
the other hand much more steeply than in the usual case. We may
express the latter also in this way that for swelling substances the
quantity 6 in the equation of the hyperbola for the volume contrac-

ion. ¢ = ai is remarkably small, just as the quantity £ in the for-

; 2

mula of the heat of mixing.

§ 3. The integral equation of the vapour pressure line, Let us
begin our investigation with the vapour pressure lines, To investigate
whether they agree with the experimentally determined ones also
with respect to the peculiarities not yet treated in § 4, it is easier
to use the integral relation between p and 2 instead of the differential

103

relation used there. We find for this"), when the vapour pressure

of the second component may be neglected which is certainly the

case here:
d loe Ie

=p,(l—«)y

p=p, (1 — 2)e

So everywhere, where the exponent of ¢ is positive, the vapour

pressure line lies below the straight line which would represent the

vapour pressure when the law of van ’t Horr held for all concen-
trations. When this exponent is negative the real vapour pressure
lies-below this straight line. If we now apply van per Waats’s formula
for p-, and if we assume as above 4,=1004,, b,,=2244,,
= 1004a,, 4,, = 20a, we get: y= 10-4 forz = 0.5 and y = 0.25
for x= 0.2. So we really see the same course as given under a, 4,
and ¢*). But on these suppositions the region of unmixing is not so
narrow as is required in d. For y becomes = 2.5 for x—0O.1,
and as for absolutely stable states the vapour pressure in the mixture
cannot be greater than the sum of the vapour pressures of the com-
ponents *), we must be in the region of unmixing already here.

If, however, we take a,—1000a, and a,,=25a,, we get

b,
oe — Ob tor z— OF and y=1-.22 for z— 0.01. If 7: is still greater

than 100, we may even find much narrower regions of unmixing.

b
Thus e.g, y= 0.95 for c= 0.01 with ae 1000 and the correspond-

: b
ing —*— 166, while a,is put = 100004, and a,,=105a,. That

,
1

there exists still a region of unmixing, however, appears from the
value y= 1,04 for = 0.001. If a,, is taken somewhat greater still,
the region of unmixing disappears.

1) Compare the second volume of the Lehrbuch der Thermodynamik, which will
shortly appear, p. 178.

2) That a point of inflection must occur follows from the fact that the vapour-
pressure line is turned convex downward at first, and then concave downward in
the region of unmixing, as it has a maximum there. No general rule can, however,
be derived as to whether this point of inflection will still lie in the absolutely
stable, or in the metastable region. In virtue of the very slight breadth of the
plait, however, which leads us to expect that we are already quite close to the
maximum of the vapour-pressure line on the verge of unmixing it may be consi-
dered as exceedingly probable that the point of inflection still falls in the absolutely
stable region.

8) Cf. the footnote p. 111.

104

We shall presently return to these results, but we may now
already state that with suitable values of a,, and a, really vapour
pressure lines are obtained which perfectly agree in type with the

experimentally determined ones. It deserves notice that this result is
> 2

in the first place the consequence of the great value which =
av

assumes according to our suppositions (great value of ; and validity
if

of Lorentz’s formula for 4,,). If we take 4 as linear function of 2,

as is often permissible for small values of ; nothing remains of these
1

results. The obtained vapour-pressure lines are namely characterised

by this that uw", is strongly positive for values of x near 1, which
leads to the strongly convex pz-line, whereas near r=0O wu’; is
strongly negative, which circumstance gives rise to the region of
unmixing. If, however, we take 4 as linearly dependent on z, change
of sign of «”, becomes impossible '). This quantity must have the same
sign throughout the whole breadth of the figure; then we can have
unmixing with negative value of w",, but then the vapour pressure
line ends also concave downwards on the side of the slight vapour
pressures. This is accompanied by an extension of the region of
unmixing over the full width of the figure as in the case of mercury-
water. When the vapour-pressure line ends concave downward,
however, on the side of the small vapour pressures, uw’; must be
positive, and then unmixing is impossible. And this holds whatever
values one may choose for a, and a,,. Only for very large values of

; as they follow from the formula of Lorentz for great values of
ae

b Pie : asi:
— a region of unmixing can occur in a pa-line which is convex on

1
the other side. Whether this region of unmixing then occurs, and how

wide it will be, will depend on the a@’s, and more particularly on
. a . *. . .
the ratio of —*. We have seen this already in the foregoing discus-
a,
sion, and we shall find confirmed in what follows that only a very
small change of this quantity is required to make a mixture with
an exceedingly narrow region of unmixing on the side of the small
molecule pass into a system that is miscible over its full breadth.
This is in accordance with Mr. Katz’s remark “limited or unlimited
miscibility, it seems, may depend on small factors, as closely allied

1) Cont, Il, p. 152,

105

substances may belong to different types’. Of course it would be
entirely premature now that we are still altogether ignorant about

the causes that govern the value of the quantity 2 even for. the

a
best known systems, to pronounce an opinion about the qecakian why
for some systems the value is such that a very narrow region of
unmixing appears, whereas for others there exists complete miscibility,
Even quite apart from the fact that it does indeed follow from what
precedes and what follows that the experimental peculiarities found
by Mr. Katz can all appear for perfectly normal substances, but
that it does not follow by any means, of course, that not all kinds
of other circumstances might be found for the systems investigated
by him, which do not affect the general character of the lines, but
might have a very considerable influence on the numerical values
of the quantities to be calculated. For this reason I have abstained
from endeavours to find the numerical values of a’s and 4’s, and
have confined myself to the general course of the investigated lines.

§ 4. The volume-contraction. Further on we shall return to the
vapour-pressure lines, but for a reason which will soon become clear,
we shall first speak about the volume contraction. According to
Mr. Katz it may be represented by a hyperbola:

b43

in which ¢ is the contraction in em’* when 1 gr. of dry substance
absorbs 7 gr. of water. What does the theory of the normal mixtures
teach us about this quantity > If we may assume that the tempera-
ture has been chosen so low that we may put the limiting volume
b for the liquid volume, the increase of volume Av in consequence
of the mixing of J/, (1—z) gr. of water and WV, 2xgr. of dry sub-
stance becomes :
Av=b;— b, (1 — «) —b,a = — «(l—a)(6, + 6, —2b,,). . (5)

From this we must derive the relation between ¢ and 7. Now
evidently :

Av
Me
follows from the definitions, c and Av taken for the same concentration.

If we further mix 1 gr. of dry substance and 7 gr. of water resp.
M, with M, 7 ger., the number of molecules are evidently in the

M, .
ratio 1 :—Z so:
M,

106

i M

1
= gee Se, ee
Mi M,+ Mi (6)

and
i Mii
— «= ——_—_..
M, == My
So equation (5) becomes :
i
<=. 3
M,+ My
so really a hyperbola.
Also the second above mentioned peculiarity of the c,7-lines that
the quantity 6 in the equation of the hyperbola becomes much
smaller than is usually the case, is found confirmed here. For

M,.. Saat :
— is found for this quantity.

ae |

The heat of mixing. Mr. Karz has already pointed out’), that the
hyperbola found by him is in accordance with a formula given by
vAN per Waats in the Théorie Moleculaire. But this formula was
derived on the supposition of linear dependence of 6 on & (4,-+-6,=20,,)
and we saw already that both the experimental vapour pressure and
volume contraction lines and the theory exclude this supposition in
our case. If we, however, again assume the supposition, on which
the said formula of vAN prr WaAALs is also founded, that viz. the

(Oe Ee 6

ae
—, we find
b;

for the increase of the potential energy or the absorbed quantity of
heat when M,r gr. of dry substance is mixed with J/, (1—2) er.
of water : =

al—a)( 6,, b, Gy eae
A = ———— } 2a, — 4+ a, — —2a,,—a,— 2 — — |(6,+6, - 2,.)| (7)

potential energy of a mixture may be represented by

b b, b, Beebe
3etween A and the quantity W used by Mr. Karz the relation
; A :
W=— ap exists again, and of course, equation (6) holds again.

So it appears that we do not get a hyperbola for W, but a curve
of higher degree than the second.

In how far this involves a deviation from the experimenial data,
we shall examine presently ; first we must see what conclusion may

. . . 28 . C . °
be derived from the limiting ratio 7 for very small values of 2

b) leic.ap,: 270,

~107

determined by Mr. Katz, so values of x which are nearly equal to 1.
With such values of x the terms multiplied by (4, + 6, — 24,,) now
predominate on the lefthand side; so we find for the required ratio:

If this expression is to be independent of the order of magaitude
of 6,, we must conciude that in general a increases proportionally
* 2 . . . i a . .
with 4° for increasing values of 4, so that - remains of the same

order of magnitude.
: ; A
Also with a@ proportional to 4 the coefficients res would remain
equal, they all being zero then. This supposition does not eall for
any further discussion, also because the critical temperature rapidly
ses for all known bodies with great increase of 4, whereas the
critical pressure remains of the same order of magnitude,

. . a . * a bd ,
§ 5. Supposition that pa OF the same order of magnitude for

the components. So we shonld have to conclude from this that we
have assumed the increase of a for certain increase of 4 too small
in § 1 and 3. And now the question should be solved whether what
was found above for the vapour-pressure line continues to hold also
with the now supposed great increase of 7. For this purpose I once
more examined the course of the vapour-pressure line with the aid
of the above formula, now on_ the suppositions 6,—1004,,
b,, = 22.46, a, =10000a,. For a,,—=150 we find then that the
region of unmixing has quite disappeared ; with a,, = 140 on the
other hand we find y=1.03 for «= 0.01. So if we take z slightly
higher, we shall find exactly the required width of the region of

unmixing already with ”: = 100. So all Mr. Kartz’s results mentioned
under 1, 3, and 4 can be derived from our theory.

So if finally remains the question in how far the result under
2 is incompatible with the simplest theory developed here. If we
take the last mentioned example, viz. 4, = 100 4,, 6,,=22.44,,
a, = 10000-a, and a,, —140a,, we find for the heat of mixing the
expression :

r(1—s
A= — 11362 + 5563.82). . . . . (7a)

108

Ai
This is in conflict with the hyperbolical line as é

-, for this
+2

leads to an expression of the form:
iz 2 SES eet oe eee ai
C+-De

For a course from «=O to e=1 equations of these two types
ean certainly not perfectly accurately agree; it is, however, the
question in how far they deviate within the region in which the
observations lie («=01 to «=04). H now for =01, 02,

bean
136.245563.82

and if we divide the result by the value for «= 0.4, we find:

0.7342, 0.8223, 0.9110 and 1.0000

0.3, 0.4 we calculate the value of the expression

these values do not ascend linearly, but they differ from the purely
linearly ascending ones :
0.7336, 0.8223, 0.9110, 0.9997

everywhere less than 1°/,,, the experimental errors certainly amount-
ing to a few percentages. So it is clear that the discrepancies which
exist between a formula of the type (7) and of the type (8), are
much too small in the considered region to allow of an experimental
decision. We must conclude that a formula of type (7) represents
the experimental data as well as a formula of type (8)°). Farther
reaching conclusions are of course excluded, as we already remarked

1) Perhaps we may go still further and say that in the general case a formula
as (7) represents the experimental relations better than (8). For according to the
latter formula the total heat of mixing W and also the differential heat of mixing

dW ,
Tin must always retain the same sign, while en the other hand for certain values
di

of the a’s and b’s a reversal of sign is possible according to formula (7). And this

3 dy ‘ :
change of sign -of Th” which can never take place for a hyperbolical formula,
di

seems indeed to appear in reality in some cases e.g. for inulin, as appears from
the subjoined table.

i W in Cal.

0 0

0.052 11.8

0.095 16.7

0.116 19.0 .
0.223 22.4

0.293 23.0

1.05 21.8

It is also in connection with this deviation of the theoretically required formula

‘

LO9

above, by the absence of accurate numerical values of all the as,
b’s, and even the molecular weights.

So summarizing we must say that a// the experimentally found
particularities can appear exactly in the same way for mixtures of
perfectly normal substances which behave according to the sim-
plest theory.

§ 6. Deviation from the law of van ’t Horr even in case of
extreme dilution. There is another particularity in connection with the
absence or presence of unmixing, to which it may be desirable to
draw attention. I mean departures from the well-known vapour-
pressure formula of vAN ’t Horr for extreme dilutions

dp
pde,

=— 1.

This formula, which may be expressed geo-

A metrically by saying that the vapour-pressure
line *) in its limiting direction points to the

opposite angle (direction AB in figure 3), is

considered of general validity for systems

whose components differ widely in volatility.

And indeed if we understand by this latter

B vs

; condition that
Fig. 3. x

= 0, at the limiting value,
1

from a hyperbola that the property mentioned in the last lines of § 2 can be
cal.

0.50 1.00
Fig. 2.
proved in a simple way for the volume contraction, but not for the heat of mixing.
1) Of course the total vapour-pressure line is meant here. For the partial vapour

110

i.e. that the ratio of the concentration of the second component in
ihe vapour and in the liquid is very small, this rule can be perfectly
rigorously derived for the limiting value purely thermodynamically
in the wellknown way. Purely thermodynamically, because we have
then only to do with the logarithmic part of the thermodynamic
functions, and need not know anything more about the system. But
this definition of “difference in volatility” is not the only possible
one, and not the only one that naturally suggests itself. We might
as well, perhaps better, understand by this idea, that one pure
component has a very much lower vapour-pressure than the other
at a definite temperature. And these two detinitions by no means
always coincide. Let us e.g. take a system for which the equations
1—-4 hold. On the supposition f=7 and 7);,—47%, it follows that
the quantity p,/p, is of the order 10~'8 at a temperature of '/,7;,.
So there seems, indeed, to be every reason to say that the second
component is much less volatile than the first. Yet by no means

oo : Ae Ee” ae =

lin. ~=0. On the contrary, if we put /=1, it follows from the
L,

above that the p,#,-line begins ascending, so #, > .2,; in the begin-

ning the second component is present in the vapour in greater

quantity than in the liquid, and van ’t Horr’s law by no means holds

any longer even for the extremest dilutions. Exactly the same thing

applies for other values of 2% So we must supplement the condition
1
for the validity of van ’r Horr’s law also for the extremest dilutions
as follows, that the components differ greatly in vapour-pressure,
and that there be no region of unmixing in the neighbourhood.
For if this were not the case we should already soon get a vapour
in which the partial pressure of the second component would be
greater than the total pressure of the component at the chosen
temperature, and this is not possible for absolutely stable states‘).
So where the rule of van ’r Horr does not hold with great difference
in vapour pressure, this will be in the closest connection with this

pressure lines on the side of their component it always holds that they point to
the opposite angle with their initial direction, as immediately follows by differentia-
tion of the equation on p. 103.

) We used this thesis already above to conclude to the existence of unmixing. It
may be proved as follows. It follows from the differential equations of the two
partial vapour-pressure lines (Cont. II, p. 163) that they will possess a maximum
or a minimum only on the borders of the stable and unstable region. So if there
is no unmixing, the partial vapour-pressure line of the first component is always
descending, that of the second always ascending. If there is a region of unmixing,

ae
Pt

tit

that the liquid phase becomes unstable and unmixing appears already
at very slight concentrations. So we shall have to expect that
vAN ‘T Horr’ law does hold for substances with unlimited imbibition
power. And our formulae prove in harmony with this. As we namely
saw it is required e.g. in the case 6, = 1004, and 7 not far from

a
1 that — does not lie far below 35. Then, however, we find for
a,

x about — 380, and so lim a of the order 10—'5°, On the other
zr sok

hand for substances with limited imbibition power van’? Horr’s law

may hold, but this is by no means necessary, or even probable, and

we shall undoubtedly have to take this circumstance into account

in attempts to derive the molecular weight of these substances from

the properties of their solutions.

§ 7. Other systems with great difference in vapour pressure of the
components. 1 already pointed out the possibility of such departures
from van *T Horr’s rule in an earlier communication published in
These Proceedings, mentioned in the beginning of this paper. What
was said there, will’ bave been made sufficiently clear by the foregoing
discussion. So I shall only add a few calculations here for systems
as the one discussed there (aniline or nitrobenzene with isopentane
or hexane). These systems agree in so far with the systems discussed
in the foregoing that there exists a very large difference in vapour
pressure between the two components, though not nearly so great
as in the cases examined by Mr. Karz, where the second component
nowhere shows a measurable vapour pressure. But for the rest the
difference is great; whereas in the systems discussed up to now the

b : ;
ratio — reaches very great values, the ratio here is not far from 1,
1

the partial vapour pressure of a component in
ihe maximum can of course considerably rise
above the value for the component itself (see
fig. 4), but then this is always in the metastable
or unstable region. For the partial vapour pressures
must be the same in the two coexisting liquid
phases. So the point A must lie on the same
level as B, and as both between A and C, and
between B and D the partial vapour pressure line
can only be ascending, the partial vapour pressure
must be smaller than DE throughout the region
Fig. 4. of the absolute stable mixtures.

412 :

and the substance with the greater vapour pressure has here even
the greater molecule. Instead of in the righthand half of the general
isobaric figure of vAN DER Waals we are now in the lefthand part.
Accordingly ihe unmixing found here must not be ascribed to the

same cause, the high value of re but (so long as we assume that
),
1

we have not to do with abnormal systems, and with the systems
mentioned we may do so to all probability) to a smaller value of /
than generally occurs.

Let. us take as an example the system aniline-hexane. 5, is here

4 b
0.006113, = — 0,007849, so 4, =1,284, and =e — 1,136 follows

1 1

d*b

from the formula of Lorentz, so 40,1153, and | = 0,017.

2 2
Further a, = 0,04928 and a, = 0,05282, so k = 0,9659. If we sub-
stitute these values in the equations (2) and (4). we get:

dlp. 2 gles :
(2) — __~ (0,8847—1,035) + 2(0,7694—1,0351). (2c)
dz Je m,
and ;
d?lp, 7 <
= — + (3,31—3,19]) + 4141 — 4,297 + 0,22. (4e)
dx? xz—1 mM,
‘ dlp, : a 2
So we get (S s)=—12 for /=1 with f=7 and My
—

T;. hexane = 235° and the temperature of the upper mixing point
= 68°,9). So we have not to expect unmixing, at least in the
neighbourhood of the border, nor for greater concentrations,

d?lp, d'lp-
because ——— must at least be — 4 to make 1+2(1—~2)
dz? r=

: ee eege ee
negative. In agreement with the complete miscibility = = 2,62, and so
aL
l—z, 1
1—z, 4 10 :

with pretty close approximation. As soon, however, as / becomes

and accordingly van ‘Tt Horr’s law is _ fulfilled

dlp.
smaller, this is changed. For /=0.9 we get - = 0.66, and so
& :

1—z. ] -
; —>-s: and the lowering of the vapour pressure of the second

component by addition of the first will therefore amount to only
d?lp,

da?

has the

half of what van ’t Horr’s rule would require. But as

113

value — 4,08 already now, we see clearly that there is a region of
unmixing at hand, and it will already have appeared with some

. dl Ven
decrease of temperature. For /= 0,85 finally P< has already got the

at
. : dlpe
negative sign oto 0,3) at the chosen temperature; so the
ae

vapour-pressure line does not descend from the side of the most
volatile component, but ascends; there is a maximum vapour pres-
d’lp,

sure. But then the value of am has fallen to almost —6, and we
may expect that even for not very great concentrations unmixing
will take place. .

The calculations given here, will, I hope, have sufficiently eluci-
dated the thesis which I pronounced in the cited paper that van *v
Horr’s rule need not hold, even as a limiting law, for systems whose
components differ very much in vapour-pressure, when viz. these
substances do not mix in all proportions, or at least a region of
unmixing is close at hand. They also set forth again’), how much
greater the influence is of slight deviations in the value of / from
unity, than in those of or = and that such deviations are able to

1 1

modify the course of phenomena entirely, so that certainly only a
small part of all the possible cases is observed when we start from
the supposition that the relation /=1 should be always rigorously
fulfilled. On the other hand they also show that in all the systems
known to us, we have to do with values of / which are contained
within narrow limits, and that we have not a single indication to
think values possible for the value of / of the same order as

b a
undoubtedly occur for = and also for —.

1 1

Mathematics. — “On looping coefficients.” By Dr. lL. E. J. Brouwer.
(Communicated by Prof. D. J. Kortrwze.)

(Communicated in the meeting of February 24, 1912).

Let us suppose in Sp, two non-intersecting simple closed curves
k, and &, furnished with a sense of circuit. Then /£, possesses with
respect to &, a looping coefyjicient answering to the intuitive notion

1) Cf. the paper in the Zsch. f. phys. Ch. 75 cited in the beginning of this
treatise.
5
Proceedings Royal Acad. Amsterdam. Vol. XV,

114
of the number of times that kh, circulates around k,, and generally

defined as us ‘< the variation corresponding to a circuit of /, of the
solid angle projecting /:, out of a variable point of &,.

A first objection to this definition is, that without further agreement
it can be applied only to special categories of simple closed curves.
For, as soon as e.g. a simple closed curve & intersects of a sheaf s
all the ravs contained in a certain finite solid angle, the solid angle
projecting i: out of the vertex of s, has no more a definite value.

A second objection to the definition is, that it cannot be generalized
to a notion of “looping coefficient in Spr of a two-sided closed Spp
with respect to a two-sided closed Spr—r—1 not intersected by Spp.”

In the following we shall give a definition for which these two
objections bave been annulled.

On each of the two curves */, and &, we construct a scale of
measurement:), and we consider the set / of pairs of points consisting —
of a point of &, and a point of &,. A part of R determined by an
element?) of #, and an element of #, we shall call a parallelo-
element. It appears as a continuous one-one image ofa parallelogram.
Each of these image parallelograms can be divided into four triangles
with a common vertex inside the parallelogram and with their bases
in the sides of the parallelogram. Accordingly we can divide each
paralleloelement of & into four two-dimensional elements, and with
this we attain that the whole set & is divided into two-dimensional
elements which by their mode of being joined cause R to appear
as a closed two-dimensional space. *)

Let p be a paralleloelement of A, d, resp. d, the corresponding
element of /, resp. &,, A, resp. 5, the negative resp. positive end-
point of d,, A, resp. B, the negative resp. positive endpoint of d,,
we then define the row of pairs of points (A,A,), (4,B,), (B,B,) as
a positive indicatrix of the partitional simplex *) of p determined by
those pairs of points, and with the aid of it we fix the positive
indicatrix of the four elements of R belonging to p*). In this way
we determine of all elements of & the positive indicatrix, where for

t) Mathem. Annalen 71, p. 98—100.
*) ibid., p. 97.
8) ibid., p. 98.
4) jbid., p. 100.
6) ibid., p. 101.

115

two arbitrary elements having a side in common these indicatrices
satisfy the relation prescribed for two-sided spaces‘).

So & is a closed two-sided two-dimensional space.

The set of the vector directions of Sp, forms likewise a closed
two-sided two-dimensional space (of the connection of the sphere
which we shall represent by 6. The positive indicatrix of the spheres
of Sp, (and with it at the same time the positive indicatrix of B) we

determine by regarding them as boundary of their inner domain *

If we conjugate to each pair of points consisting of a point of
k&, and a point of &, the direction of the vector connecting the two
points, we determine a continuous one-one representation a of R on
&. To this representation belongs a finite integer c independent of
the mode of measurement of F, and therefore also of the mode of
measurement of £, and &,, which is called the degree of the repre-
sentation, and possesses the property that the image of R covers
positively each partitional domain of 5 in toto ¢ times *),

It is this degree of representation which we define as the looping
coefficient of k, with respect to k,.

By exchange of £, and &, we find that on one hand the indicatrix
of FR changes its sign, but on the other hand each image point on
B is replaced by its opposite point. So the looping coefyicient of k,
with respect to k, ts equal to the looping coefficient of kh, with respect
Oe eos

We shall now show ‘that for rectifiable curves the looping coeffi-
cient of &, with respect to /, can be expressed by the formula:

1
if Pa GinOde” (OSt;, 0S, eee ol eee ee

This integral namely can be interpreted for rectifiable curves as
follows: We construct in &, resp. 4, a simplicial division *) z, resp.
z,. To this corresponds a simplicial division z of &, whose base
simplexes *) are determined in connection with the base arcs‘) of

1) ibid., p. 101.

2) ibid., p. 108.

3) ibid., p. 106.

4)ibid.; p. 101.

5) That here the base simplexes are found by division of a paralleloelement,
not as |.c. by division of an element, has of course no influence on our reasoning.
Moreover, after HapAMARD (comp. J. Tannery, “Introduction a la théorie des
fonctions d’une variable’, Vol. I, p. 463) a simplicial division of the parallelo-
elements can be subdivided to a simplicial division of the elements.

6) i.e, one-dimensional base simplexes.

= 446

ik, and &, in the same way as we have determined above the elements
of R in-connection with the elements of &, and &,. Each base are
of z, resp. z, we replace by the corresponding Nee: i.e. by the
straight line segment with the same endpoints. Let x, be the chord
corresponding to the base are , of: “x ilie chert corresponding
to the base are @, of &,, r the distance of their midpoints, then
x, and x, regarded as vectors determine together with a vector of
size r-2 in the direction of the straight line connecting their mid-
points, a certain volume product. Of the volume products appearing
in this way for the different pairs (*,,%,) we take the sum S; our

1 ee . :
integral is to be regarded as a x the limit of S for infinite con-
: ‘1 4

densation of z, and 2,.

Let us on the other hand represent each pair of points consisting
of a point of a chord of £, and a point of a chord of &,, by the
endpoint of a vector with fixed origin QO, and having the size and
direction of the vector connecting the corresponding pair of points.
Then for infinite condensation of z, and z, the ratio of the element
of S corresponding to #, and x, to the value of the solid angle
projecting out of O the parallelogram representing the chords ~,
and z,, approaches indefinitely to unity, and so does: the ratio of the
element of S corresponding to x, and x, to the partsof B covered
for the simplicial approximation *) of @ corresponding to z, by the

“base parallelogram’ resulting from , and 8.

As farthermore on account of the rectifiability of 4, and hk, the
sum of the absolute values of the elements of S for infinite con-
densation of z, and z, cannot exceed a certain finite value, re
converges indeed io the looping coefficient defined as the degree of
the representation «.

On the other hand for rectifiable curves holds also the defimtion
of the looping coefficient as a variation of a solid angle mentioned
in the beginning, and we easily see also this definition to be equivalent
to the expression (1).

5 3.

Let now in Sp, be given a two-sided closed /-dimensional space
9, and a two-sided closed (2—/--1)-dimensional space @, not cutting
¢,, each provided with a positive indicatrix. We make 9, as well

!) Mathem. Annalen 7], p. 102.

117

as 9, measurable’), and we consider the pairs of points consisting
of a point of 9, and a point of g,. A part of R determined by an
element of 9, and an element of 9, we shall eall a paralleloelement.
It appears asa continuous one-one image of a (4, —h—1)-simplotope *).
Let us call a division of a simplotope 2 into simplexes with one
common vertex inside 2, whilst the remaining vertices lie in the
boundary of z, a “canonic division’, then we can brine about such
a canonic division by first executing it for the two-dimensional limits,
then for each three-dimensional limit by projecting the divisions of
its two-dimensional limits out of an arbitrary inner point, then for
each four-dimensional limit by projecting the divisions of its three-
dimensional limits out of an arbitrary inner point, and so on.
Accordingly we can divide the paralleloelements of R into (n—1)-
dimensional elements in such a way, that by their mode of being
joined they cause # to appear as a closed (n—1)-dimensional space.

Let p be a paralleloelement of &, d, resp. d, the corresponding

element of 9, resp. 9,, A,A,....A,'") a positive indicatrix of d,,
A,A,....A,"—*-)) a positive indicatrix of d,, we then define the
row of pairs of points (4,A,), (A’,A,),....(A,A,), (A,\MA’,),....

_(A,{A,7-*-)) as a positive indicatrix of the partitional simplex of
p determined by those pairs of points, and with the aid of it we
fix the positive indicatrix of the elements of R beionging to p. In
this way we determine of all elements of F the positive indicatrix,
where for two arbitrary elements having an (n—2)-dimensional limit
in common these indicairices satisfy the relation prescribed for
two-sided spaces.

So Ff is a closed two-sided (n—1)-dimensional space.

The set of the vector directions of Sp, forms likewise a closed
two-sided (n—1)-dimensional space (of the connection of the (mn—1)-
dimensional sphere) which we shall represent by &. The positive
indicatrix of the spheres of Sp, (and with it at the same time the
positive indicatrix of 6) we determine by regarding them as boundary
of their inner domain. :

If we conjugate to each pair of points consisting of a point of @,
and a point of o, the direction of the vector connecting the two

1) ibid., p. 98—100.

2) Let in Sp,—1 be given a plane /i-dimensional space v and a plane (n—h—1)-
dimensional space w. Let S, be a simplex in v, S, a simplex in w. The set of
those points of R,—; which in the direction of w project themselves on v in Sy,
and in the direction of v project themselves on w in Sy, form by definition an
(h, n—h—1)}-simplotope. Of a simplotope the limiting spaces of any number of
dimensions are likewise simplotopes. (Comp. P. H. Scuoute, *Mehrdimensionale
Geometrie”’, Vol. Il, p. 45).

118

points, we determine a continuous one-one representation a of R on
B. To this representation belongs a finite integer c independent of
the mode of measurement of R&R, and therefore also of the mode of
measurement of @, and @,, which is called the degree of the repre-
sentation, and bas ihe property that the image of F& covers positively
each partitional domain of B in toto ¢ times.

It is this degree of representation which we define as the looping
coefficient of 9, with respect to @,.

Exchange of oe, and e, has only this consequence that the indi-
catrix of R changes its sign in some cases, and that each image point
on B is replaced by its opposite point. So the loeping coefficient of
, with respect to 9, and the looping coefficient of 9, with respect
to @, are either equal or opposite.

We shall now show that if eg, and eg, are evaluable, i.e. if they
have a definite finite /-dimensional resp. (7—h—1)-dimensional volume,
the looping coefficient of @, with respect to 9, can be expressed by

the formula :
: af Vol. prod. (di,, di,,ri—"). . . . . . ()
where fh, represents the (n-—1)-dimensional volume of an (n—1)-
dimensional sphere described with a radius 1 in the Euclidean Sp,.
If namely e, and e, are evaluable, this integral can be inter-
preted as follows: We construct in e, resp. @, a simplicial division
z, resp. 2,. To this corresponds a simplicial division z of R, whose
‘base simplexes are determined in connection with the base sim-
plexes of e, and e, in the same way as we have determined
above the elements of in connection with the elements of e, and
,. Hach bas2 simplex of z, resp. z, we replace by the plane simplex
with the same vertices. Let z, be the plane simplex corresponding
to the base simplex ?, of e,, *, the plane simplex corresponding to
the base simplex ?, of 9,, 7 the distance of their centres of gravity,
then x, and x,, the former regarded as an /-dimensional, the second
as an (n—/—1)-dimensional vector, determine together with a line-
vector of size r'—" in the direction of the straight line connecting
their centres of gravity, a certain volume product’). Of the volume

a
s

‘) The sign of this volume product we determine as follows: Afler having
formed in the manner described above out of (—1)’X the positive indicatrix of x,
and the positive indicatrix of , an indicatrix of a simplotope s parallel to +, and
xz, we add to the latter indicatrix the endpoint of a linevector described out of a
point of s in the direction of the straight line connecting the centres of gravity of
x and x ;. Tue sign of the n-dimensional indicatrix found in this way determines
he sign of our volume product.

119

products appearing in this way for the different pairs (x,,%,) we

; : ; l
take the sum JS, our integral is to be regarded as the limit of

fm»

S for infinite condensation of z, and z,.

Let us on the other hand represent each pair of points consisting
of a point of a plane simplex determined by 2, and a point of a
plane simplex determined by z,, by the endpoint of a vector with
fixed origin OV, and having the size and direction of the vector con-
necting the corresponding pair of points. Then for infinite condensation
of z, and z, the ratio of the element of S corresponding to x, and x,
to the value of the solid angle projecting out of O the simplotope repre-
senting the simplexes x, and z,, approaches indefinitely to unity, and
so does the ratio of the element of S corresponding to %, and x, to
the part of 4, filled for the simplicial approximation of @ corre-
sponding to z, by the ‘‘base simplotope” resulting from #, ond @,.

As farthermore on account of the evaluability of 9, and 9, the
sum of the absolute values of the elements of S for infinite conden-
sation of z, and z, cannot exceed a Certain finite value, Ue conver-

ges indeed to the looping coefficient defined as the degree of the
representation «.

§ 3.

Let us now consider in Sp, two sets of points g', and gy’, which
have no point in common and are successively a continuous one-
one image of an /-dimensional two-sided closed space g, and of an
(‘n—h—1)-dimensional two-sided closed space e,, then for these all
the considerations of the former § remain of force. Let farthermore
0," be a second continuous one-one image of 9,, and let eg,” be a
second continuous one-one image of e,, then there exists a quantity
y with the property that if the distance of two corresponding
points of g,' and g," as well as the distance of two corresponding
points of 9,’ and 9,” is smaller than 4, the looping coefficient of
9,’ with respect to-9," is equal to the looping coefficient of 9,’ with
respect to @,.

From this ensues that in Sp, the looping coefficient of an )-dimen-
sional two-sided closed space ¢, with respect to an (m—/h—1)-dimen-
sional two-sided closed space 9, not intersecting 9, is equal to the
value of the integral

1
~ vol prod. (dt, , di, , r—)
Cn

120

for an arbitrary simplicial approximation’) a_(9,) of ¢, and an
arbitrary simplicial approximation a (9,) of Q,.

Let A, and K, be in Sp, two spheres lying outside each other,
a(o,) a simplicial image of @, lying inside A,, e(g,) a simplicial
image of g, lying inside K,. The looping coefficient of «(@,) with
respect to a(g,) is then zero; for, by transferring K, -with a(9,)
outside K, to infinity, we can vary this looping coefficient only
continuously, thus not at all.

We can now transform «(¢,) continuously into a(e,) by causing
the base points*) of @(g,) to describe continuous paths, and we can
choose for these base point paths such broken lines that in none of
the intermediary positions of « (¢,) an (4—1)-dimensionai element limit of
a(o,) has a point in common with «@(o,), neither an (mn—h—2)-
dimensional element limit of @(9,) has a point in common with a (Q,),
whilst those intermediary positions of @(e,) which correspond to the
angles of the base point paths, hae no point in common with a (@,).

Then for this variation of a@(9,) the looping coefficient of a (@,)
with respect to «@(g,) increases by a unit as often as an element
e, of a(g,) is traversed by an element , of @(9,) positively, i.e. in
such a way that the volume product of ¢,, %,, and the direction of
motion of the traversing point is positive according to the above
definition.

If on the other hand we understand by na (e,) resp. ra (g,) a two-
sided (n—h)-dimensional net fragment’), limited by a(e,) resp. a@(g,)
and crossing a@(9,) only in a finite number of points, belonging neither
to an (4—1)-dimensional base limit of a(9,), nor to an inner (7—h—1)-
dimensional base limit of na(g,) resp. na(e,), whilst such a crossing
is called positive, if in the crossing point the n-dimensional indicatrix
composed of (—1)" >< the positive indicatrix of a@(g,) and the positive
indicatrix of na{o,) resp. ne#(e,) is “positive, then for the above-
mentioned variation of a(o,) the algebraical sum of the number of
positive and the number of negative crossings of a(e,) and na(g,)
increases likewise by a unit each time that a@(o,) is traversed by
a(Q,) positively.

From this ensues that the looping coefficient of 9, with respect to
e, can also be defined as the algebraical sum w {1(9,), na(Q,)} of the
nuiber of positive and the number of negate crossings of an arbitrary
simplicial approximation a(9,) of 9, and an arhitrary (n—h)-dimen-

1) Mathem. Annalen 71, p. 102 and p. 316.

*) ibid., p. 317.

5) ibid., p. 316.

121

sional net fragment na (9,), limited by an arbitrary sumplicial approwi-
mation a(9,) of @,.

That this algebraical sum is unequivocally determined by 9,
e,, can also be shown by a direct proof.

If, namely, we have two different net fragments na o,) and
n’a(9,), limited by the same simplicial approximation a (o,), and if
we represent the net fragment obtained out of n/a (e,) by inversion
of the indicatrix, by n'a (g,), then na(e,) and na (o,) form together
a two-sided closed net’), so that w {a (o,), na(9,) + n'a (o,)} must be
equal to zero, thus w {a (9,), n’a (9,)} = w fa | (0,), na (Q,)}.

If farthermore we have two different simplicial approximations
a(g,) and a’ (9,) corresponding to one and the same mode of
measurement of @,, two different simplicial approximations a (o,)
and a’ (9,) corresponding to one and the same mode of measurement
of 9,, and two two-sided net fragments na (e,) and na’ (@,), which,
leaving their rims out of consideration, have the same base points,

then for continuous transformation of a’ (9,) into a (

and

we have:

Q 1)
aw ya (9,), na (9,)} SS (a (9,), na (9.)},

and for continous transformation of a'(g,) into a (o,):
w {a’ (0,), na’ (@,)} = w {a’ (9,), na (9,)}.

If finally we have two different modes of measurement mu, and
uw’, with corresponding indicatrices of 9,, and two different modes of
measurement mg, and mw, with corresponding indicatrices of 0,, then
on account of the theorem, that a continuous one-one correspondence
between two closed spaces useeeses the degree + 17), there exists
a simplicial approximation a'(9,) corresponding to w',, covering a
simplicial approximation a(9,) corresponding to uw, with the degree
one, and asimplicial approximation a'(9,) corresponding to p’,, covering
a simplicial approximation a (g,) corresponding to fu, with the degree
one, from which ensues immediately :

@ {a' (Q,), NA (O,)} = & {a (9,), na (Q,)},

0,);

with which the proof that the abovementioned algebraical sum
depends exclusively on 9, and g,, is completed.

In close connection with the looping coefficient is the notion of
enlaced spaces recently introduced by Lesuseun*). Two spaces enlaced

1) ibid., p. 316.

2) ibid., p. 324 and p. d98.
5) G. R., 27 mars 1911.

122

according to LEBESGUE, possess in our terminology with respect to each
other an odd looping coefficient. But to justify his definition LepesGuxr
has neglected to prove that the being enlaced or not of two spaces is
independent of the manner in which they are measured, which
property is established only by the above reasonings.

The developments joined by Lxsrscur to his definition can mean-
while be made entirely rigorous by replacing the notion “enlaced”
by: “enlaced for a definite mode of measurement.”

(June 25, 1912).

KONINKLIJKE AKADEMIE VAN WETENSCHAPPEN
TE AMSTERDAM.

PROCEEDINGS OF THE MEETING
of Saturday June 29, 1912.

IOCe

President: Prof. H. A. Lorentz.
Secretary: Prof. P. Zeman.

(Translated from: Verslag van de gewone vergadering der Wis- en Natuurkundige
Afdeeling van Zaterdag 29 Juni 1912, Dl. XXI).

S eae ay es:

H. J. Waterman: “Mutation in Penicillium glaucum and Aspergillus niger under the action
of known factors”. (Communicated by Prof. M. W. BrisEerinck), p. 124.

G. P. Frets: “On the external nose of Primates”. (Communicated by Prof. L. Bork), p. 129.

G. P. Frets: “On the Jacobson’s organ of Primates”. (Communicated by Prof. L. Bork), p. 134.

' P. Martin: “The magneto-optic Kerr-effect in ferromagnetic compounds and metals”, III.

(Communicated by Prof. H. E. J. G. pu Bors), p. 138.

Davin E. Roperts: “The effect of temperature and transverse magnetisation on the resistance
of graphite’. (Communicated by Prof. H. E. J. G. pu Bots), p. 148.

T. van Louuizen: “Translation series in line-spectra”. (Communicated by Prof. P. Zermay),
p. 156. (With one plate).

F. E. C. Scnerrer and J. P. Trevus: “Determinations of the vapour tension of nitrogen

- tetroxide”. (Communicated by Prof. J. D. vAN DER WAALS), p. 1€6.

P. ZEEMAN and C. M. Hoocrxsoom: “Electric double refraction in some artificial clouds and
vapours”. (3rd part), p. 178.

A. Ssmts: “On critical endpoints in ternary systems” If. (Communicated by Prof. A. F.
HOoLiemay), p. 184.

H J. Zwiers: “Researches on the orbit of the periodic comet Holmes and on the pertur-
bations of its elliptic motion”, V. (Communicated by Prof. E. F. van DE SANDE BakuuyZzEN),
p. 192.

E. L. Exre: “The scale of regularity of polytopes”. (Communicated by Prof. P. H. Scuovrte),
p- 200. f

A. P. N. Francuimont and J. V. Dussxy: “Contribution to the knowledge of the direct

nitration of aliphatic imino-compounds”, p. 207.

BérsEKeN and H. J. Waterman: “A biochemical method of preparation /-Tartaric acid”.

(Communicated by Prof. M, W. BrtvErrINck), p. 212.

J. BorsEKEN: “On a method for a more exact determination of the position of the hydroxyl
groups in the polyoxycompounds” (4th Communication). (Communicated by Prof. A. F.
HOLLEMAN), p. 216.

G. A. F. Morencraarr: “On recent crustal movements in the island of Timor and their bearing
on the geological history of the Hast-Indian Archipelago”, p. 224.

Max Weser aud lL, F. pe Beaurort: “On the freshwater fishes of Timor and Babber”, p. 235.

W. H. Kexsom: “On the deduction of the equation of state from BoLTzmann’s entropy prin—-
ciple”. (Communicated by Prof. H. KAMERLINGH ONNES), p. 240.

W. H. Kersom: “On the deduction.from Borrzmany’s entropy principle of the second virial-
coefficient for material particles (in the limit rigid spheres of central symmetry) which
exert central forces upon each other and for rigid spheres of central symmetry containinz
an electric doublet at their centre”. (Communicated by Prof. H. Kameriincu OnnEs), p. 256.

H. Kameriincn Ones and C. A. Crommenin: “Isotherms of monatomic substances and of
their binary mixtures. XIII. The empirical reduced equation of state for argon”, p. 273.

Proceedings Royal Acad. Amsterdam. Vol. XV.

124

Microbiology. — “Mutation in Penicillium glaucum and Aspergillus
niger under the action of known factors.” By H. J. Waterman.
(Communicated by Prof. M. W. BersErtNckr).

(Communicated in the meeting of May 25, 1912).

A. Penicillium glaucum.

In solutions of p- and m-oxybenzoie acid a spontaneous growth
of mould had developed at the air. From this material, which
floated on the liquid, a pure culture of Penicillium glaucum was
obtained by isolation on malt agar, which culture was used in the
biochemical investigations described by Prof. BOEsEKEN and WaTERMAN.’)
It looked quite normally green and had the peculiar ‘mould smell”.
The culture was transferred some times in the course of a year;
mostly to protocatechetic acid, and a few times also to p-oxybenzoic
acid as sole carbon food.

After about a year, white, jelly-like spots were observed in a great
number of the films floating in ErLenmever-flasks of 200 cc. Seen~
under the microscope these spots proved to have produced but few
spores, whereas the mycelium and hyphae were normally developed.
The phenomenon became still more prominent if considerable quan-
tities of other substances retarding the growth, such as salicylic and
trichloracrylic acid were added to the p-oxybenzoic acid. ;

1) Bo#sexEn and Waterman. These Proceedings Vol. 14, p. 604, 608, 928, 1112.
2) Salicylic acid retards the growth more than trichloracrylic acid.

125

It was supposed that the observed alteration in the mould film
might be explained by mutation, which was proved true by the
biological method. By isolation on malt gelatin two forms could be
obtained from these cultures. One of these was very lightly coloured

-in consequence of the small number of spores. This form will be

indicated as ‘the mutant’. The other had preserved the dark green
colour and had evidently remained identic with the original culture.
The difference between the two forms was very marked.

So it cannot be doubted, that at prolonged cultivation in presence
of p-oxybenzoic acid mutation does indeed take place. With proto-
catechetic acid as carbon food the same was observed. Furthermore,
Table 1 shows that salicylic acid and trichloracrylic acid promote
this process.

In the floating mould layer the extent of the mutant was greatest
in those flasks where the said antiseptica were most concentrated.

At a continued cultivation on malt agar the thus obtained mutant,
which in all the said cases seemed the same, remained constant.

If the mutant and the original form were again transferred to a
p-oxybenzoic acid solution with the anorganic food named in the
table, they also preserved their properties.

Under the microscope the mutant produced considerably fewer spores
than the primitive form‘) and its mycelium had a greater tenacity,
which was repeatedly stated.

There was besides a peculiar difference in smell, as the original
form gave out the well-known “mould odour’, which the mutant
did not.

The growth of the mutant on para-oxybenzoic acid was considerably
slower than that of the primitive form.

In the laboratory a third form of Penicillium glaucum was present,
distinguished from the original form of my experiments by darker
green spores and which served for the subsequent experiments.

It was first cultivated during four days on p-oxybenzoic acid
where the growth was very slow; it was then transferred to a
new flask with the same medium, and now the growth was much
accelerated, which proved that in these few days accommodation
to the para-oxybenzoic acid had taken place. Furthermore it was
observed that also here, after a prolonged cultivation on p-oxybenzoic
acid mutation occurred. Substances such as tetrachlor-propionamid

CHCI,CCI,C=0 ) and pentachlor-propionamid/CCI,—Cvul,—C=0 ),

xu) ( xi)

1) Whether the difference in the number of spores was accompanied by a

difference in intensity of colour is not settled as yet.
o*

126

likewise compounds which retard the growth, again favoured the
mutation, so that this process seems rather general.

The smaller number of spores and the less rapid growth evidently
lead to explain the properties of this mutant by a loss of character-

istics or gens. *)
B. Aspergillus niger.

We started for this investigation from a pure culture of the la-
boratory collection, which was first cultivated some time on a 2 °/,
suecinie acid solution. In several inoculations in ERLENMEIJER-flasks
with different culture media, a considerable alteration of this black
mould occurred.

Using a 2°/, solution of galactose it was observed that in this
medium, beside the primitive form with black spores, a brown and
a white one appeared, which three forms may be called I, II,
and II].

On a 2°/, rhamnose solution of for the rest the same composition
tapwater, 0,05°/, NH,Cl, 0,05°/, KH,PO,, 0,02°/, MgSO,) the black
and the brown forms (I) and (Il) were distinctly present, the white
form (III) wanting. A tube, to which beside the food consisting: of
0.3°/, p-oxybenzoic acid, 9 mgr. (per 50 c.c.) dichloraerylic acid
‘CH=CCI]—C=0 had been added, showed after about a month
( Cl er
a quite brown mould layer. Later experiments proved that in nutrient
solutions with 2°/, glucose as source of carbon, under the influence
of 1°/, boric acid likewise mutation occurs.

The three forms from the galactose solution were isolated on
malt agar; II and III distinctly gave fewer spores than I, and III
fewer than II]. They were transferred to media of tapwater-agar to
which beside 0,05 pie NH, NO, and 0,05 “ke KH, PO; 2 “he galactose
was added. On this plate the appearance of the mutants was different
from that on the malt agar. From this galactose plate I, I, and III
were again transferred to malt agar; the latter cultures were used
for the examination of the plastic aequivalent of the carbon, where-
unto we return below.

lt was clear under the microscope that besides a smaller quantity
of spores, there was also a decrease of colour intensity of these
spores in II and III, which had become brown instead of black.
The question whether Ill might also be obtained without any spores

') Compare M. W. Bevertcx, Mutation bei Mikroben. Folia Microbiologica,
1912, p. 5.

127

at all must be answered negatively, as is shown by the subsequent
experiments.

By starting every time from a single spore, cultures were obtained
which remained identic to the material used for the sowing. If the
mycelium, carefully separated from the spores was separately sown,
no difference appeared between the product obtained from it and
that from the spores.

Possibly form II is the same as the brown form obtained some
months ago by Fri. ScHreMANN *) under the action of kaliumbichromate.

In earlier experiments on the metabolism of Aspergillus nijer
irregularities had been found, which then could not be accounted
for, but which can now be explained by the observed mutations.
In the said experiments it was determined what percentage of the
assimilated quantity of carbon was at a given moment bound in the
body of the mould and what percentage was excreted as carbonic
acid by respiration or otherwise. The first percentage may be called
“plastic aequivalent”’ of the carbon, in accordance with the term
used in researches on the luminous bacteria by Professor BusERtNck °)
whereas the percentage of the carbon which at a given moment is
respirated will be called “respiration aequivalent’’.

On a 0,3°/, paraoxybenzoic acid solution (anorg. food : tapwater,
Mie NOL 005 °/, KH. PO, 0,02 9 MeSO,; t= 382—33°C))
was found after 45 days a plastic aequivalent of the carbon of 34 °/,.
In other cultures likewise on para-oxybenzoie acid and obtained
by inoculation with the said culture, whose plastic aequivalent was
34°/,, this number amounted after 27-28 days respectively to 20
and 16 °/,.

As this lowering of the plastic aequivalent under the influence of
the p-oxybenzoic acid might possibly be ascribed to the above mentioned
mutation the question arose: Do forms I, H, and III quantitatively
differ considerably in their metabolism ?

The experiments resumed in Table II prove that this is really
the case.

The differences are, as we see, enormous and they sufficiently
explain the described irregularities.

By this method we are thus enabled to conclude to mutation even
then when visible external differences between the cultures are
wanting.

Likewise as for the mutation of Penicilliiwm glaucum we see in

1) Ber. d. Deutsch. Bot. Gesell. 1912 Heft 2, 28 Marz. =
*) Aliment photogéne et plastique. Archives Neérlandaises, T. 24, p. 1 1891,

128
TABLE II.

200 cc. ERLENMEUER-flasks of Jenaglass with 50 cc. tapwater, in which 0.05 0/, NH,Cl
0,05 °', KH, PO,, 0,02°/) MgSO, and 150 mgr. para-oxybenzoic acid,
temperature about 32°—33°.

the bere described mutation a loss of characteristics or gens, for
beside the loss in colour intensity we stated a. decrease in the
number of spores.

On the other hand it was observed, that the new forms were dis-
tinguished from the primitive one by a much more vigorous combustion
of the p-oxybenzoic acid to carbonic acid, their “respiration aequi-
valent” being found to amount from 71—72°/, in I, to 82°/, in II,
and even to 85 °/, in III.

If, as in the case observed, all other carbon-containing secondary
products are wanting, the sum of the two aequivalents is of course =100.

The here introduced aequivalents only relate to the element carbon,
whereas the hitherto used coefficients refer to the number of grams
of dry substance, to the number of grams of assimilated carbon, or
‘to the carbonic acid evolved during the life of the related organism’).

The here introduced aequivalents are to be preferred to the other
terms referred to, because the chemical composition of the food, of
the constituents of the organism, and of the carbonic acid are so
widely divergent. :

Finally I bring my thanks to Mr H. C. Jacosssn, assistant to the
Laboratory for Microbiology, for his kind help in these experiments.

Laboratories for Microbiology and Organic Chemistry
of the Technical University at Delft.

1) See for instance: KunstrMANN, Ueber das Verhaltnis zwischen Pilzernte und
verbrauchter Nahrung. Dissertation Leipzig, 1895. Also: Natuansonn, Stoffwechsel
der Pflanzen, 1910.

129

‘

Anatomy. — “On the external nose of Primates”. By G P. Frets.
(Communicated by Prof. Dr. L. Box).

The distinction of monkeys into Platyrrhini and Catarrhini is
of ancient date and generally adopted. It seems to be little known
by whom this distinction has first been made, in the systematical
works at least the name is not mentioned. The object of the present
communication is to premise the description of this classitication, as
it has been given by Burron and E. Grorrroy St. Hinatre and
amended by Is. Gxorrroy Sr. Hinaire, and to test by this formular-
ization the result of an investigation I have made.

About 1765 bBurron was the first to use the external nose as a
systematic characteristic for the classification of monkeys, which
coincides with their geographical dispersion over the two continents *),
He writes:*) “les singes de lancien Continent ont la cloison des
narines étroite, et ces memes narines sont ouveries au-dessous du
nez comme celles de ’homme” and ‘les singes du nouveau monde
ont tous la cloison des narines fort épaisse, les narines ouvertes sur
les cétés du nez et non pas en dessous.”

In 1812 Er. Guorrroy Sr. Hitatre*) divides the monkeys in his
Tableau des Quadrumanes into catarrhinins, catharrini or monkeys
of the Old World and platyrrhinins, plathyrrhini or American monkeys.
He borrows Burron’s description and adds to it, that with catarrhine
monkeys the nose-bones dissolve before the shedding of the teeth
(p. 86) whilst with platyrrhines the suture between these bones
disappears only at a later age. Later French authors sometimes
bring out still more distinctly that the characteristic has been derived
from the external nose. So DesMargst *) writes : ‘‘les singes catarrhinins
ou singes de Vancien monde (ont les) narines rapprochées lune de
Pautre’” and “les singes platyrrhinins ou singes du nouveau continent
(ont les) narines écartées l’une de l'autre”. In the same way G. Couvizr
(ed. 1829 I p. 99) F. Cuvier’), DE Buainvitiz *), P. Gewais’), Brocac®).

1) Compare Is. G. St. HitArRe, Mém. du Muséum, T. 17, p. 129; 3828,

2) Burron, Oeuvres complétes; ed. 1837 IV, 2, p. 687, 1,

8) E. G. St. Hitarre, Annales du Muséum, T. 19, 1812.

4) DesMAREST, Mammologie 1, Partie, p. 30, Paris.

5) G. Sr. Hinarre et F. Cuvier, Hist. Nat. des Mammiféres, T. 1, Paris 1824.
6) DE BLAINVILLE, Ostéographie des Mammiferes, T. 1, p. 6, Paris 1839—64.
7) P. Gervais, Hist. nat. des Mammiféres, p. 8 and p. 113, Paris 1854,

8) Brocac, L’Ordre des Primates, Mém. d’Anthropologie, T. Ill, p. 11, 1877,

130

Likewise Scuincen'). Less exact descriptions are given by GinBEI.’),
Criaus*), and M. Weser‘*).

In order to preclude incorrect representations, it is necessary to
premise that the classification of monkeys into Catarrhini and Platyr-
rhini is based on external distinctive features namely on the distance
and the location of the nostrils. Catarrhini or monkeys of the Old
World are monkeys with small distantia internarina and nostrils
turned downward, Platyrrhini or monkeys of the New World have
a large distantia internarina and nostrils turned sideways.

Isiporrk Grorrroy St. Hinatre‘*) takes the classification of Burron
and of his father as point of issue for his investigations. He comes
however to the conclusion that the distinction of monkeys according
to their external nose, without more, does not coincide with their
eeographical dispersion over the two continents. According to him
Eviodes, Lagothrix and Nyctipithecus, all of them American monkeys,
agree, with regard tu their’ nostrils, almost entirely with the monkeys
of the Old World; on the other hand Semnopithecus and especially
Miopithecus come very near up to the monkeys of the New World.
Is. G. Sr. Hinarre therefore proposes the following compromise: “Il
est permis de conserver a ces caracteres toute leur généralité, a la
condition d’en modifier l’expression, la cloison internasale étant tou-
jours mince ou médiocrement épaisse jamais large chez les Singes
de lAncien Monde, a quelque tribu qu’ils appartiennent; large ou
médiocrement épaisse, jamazs mince chez les Singes americains.

I have controlled this view by a great number of individuals.
In my opinion it is not correct; when examining many monkeys,
we see that the external nose of Platyrrhini with ‘Ja cloison inter-
nasale médiocrement épaisse’ can always be distinguished from
Catarrhini with a similar distantia internarina. It is true that it is
difficult to express this difference in a single sentence.

Let us first pass under review the shape of the external nose of
typical representatives of the two groups. The different species of
Cebus have all a large distantia internarina and nostrils turned side-
ways; between these lies a superficial fossa internarina. The nostrils
are rather wide oval, the oral part is the wider; from above and
medial the processus naviculares of the maxilloturdinale penetrate

1) H. ScuteceL, Muséum d’Histoire naturelle, p. 3 and 4, Leyden 1876.

2) GIEBEL, Die Sidugetiere, 1859, S. 1025.

$) CLAus. Lehrbuch der Zoologie, 3 Aufl. If, S. 1199, 1876.

4) M. Wezer, Die Siiugetiere, Jena 1904, p. 771 and 776.

6) ls. G. St. HiLarre, Extr. d’Archives du Muséum d’Hist. nat. T. 2, p. 6 and
p. 39, Paris,

131

into them. Consequently the opening of the nose is kidney-shaped,
with the convexity to the outside. The cartilaginous nose consists of
the two cartilagines alares and the cartilago triangularis. The cartilago
alaris is a rather broad, shell-shaped cartilage blade, surrounding the
nostril at the top, medially and orally. The dorsal, lateral angle of
the cartilago alaris is continued in the processus navicularis. If we
prepare the median parietis of the carit. alares separately and spread
them out, we can follow the downward extremity of the cartilago
triangularis that is continued in the foremost edge of the septum.
The septum does not protrude free from between the cartt. alares. The
proportions of Chrysothrix and Hapale are exactly like those of Cebus.

The form and composition of the cartilaginous nose of Plathyrrhini
ean easily be derived from its form in the embryo. There it is the
uninterrupted continuation of the internal nose, its frontal termination.
The septum is gradually transformed into two cartilaginous blades,
which at the top medially and orally limit the nostrils. In older
foetal stages both the cartt. alares and the cartilago triangularis take
their origin from these blades.

The slight prominence of the nose of Platyrrhini (DesMargst) is
caused by a slight protuberance of the region of each nostril separately.
By their. boundary the nostrils are more independent and wider
open than those of Catarrhines; the cartt. alares are thicker. There
is a sharp oral boundary of the nostril with regard to the upper-lip.

The external nose of Catharrini, as e.g. of Macacus, M. sinicus,
M. rhesus is characterized by a small distantia internarina and down-
ward directed nostrils. Instead of a fossa internarina a sulcus
interalaris is often found here. The nostrils are in the direction of the
lips not separated from these. They lie at the distal end of the cartt.
alares and are enclosed by the latter only medially and not at the
inferior side; therefore there is, between the two nostrils, a free
duplicature of the skin, a septum mobile, that extends more or less on
the upper-lip and forms here a slight protuberance. In the septum
mobile a projecting part of the cartilago alaris, crus mediale, extends ;
I found this likewise in microscopic preparations of the full-grown
nose. The region of the ecartt. alares is often a little arched, as if
it were inflated. The nostrils are narrow oval and long, the two
rims almost touch each other, also on account of the thinness and
flabbiness of the cartt. alares. Medially the beginning of the processus
navicularis arches into the opening of the nose from the maxillotur-
binale, which originates from the upper part of the cartt. alares.
The cartt. alares are narrower and less curved than those of Platyr-
rhini; they run pretty well parallel. The sulcus supraseptalis

132

terminates in the cartilago triangularis. If one prepares the cartt.
alares separately, and spreads them out, one sees that the cartilago
triangularis extends between them as front edge of the septum nasi
and protrudes a little to the front. Cereopitheci of which I examined
several specimens are of exactly the same structure as these deseribed
Macacus.

If now types with a distantia internarina ‘‘mediocrement épaisse”
are compared with these two types, one sees that the American
monkey always represents the platyrrhine type, the monkey of the
Old World always the cathyrrine type. Is. Grorrroy St. HIbaire
mentions Semnopithecus and Mvopitecus (talapoin) as monkeys of the
Old World with a rather large distantia internarina. In Semnopithecus
namely in a specimen of Lophopithecus melalophos (s. Semnophitecus
melalophos) I found the greatest distantia internarina of monkeys of
the Old World. In the mentioned Lophopithecus this distance was
0.6 cm., over against 0.55 cm. in an Ateles, to be mentioned
by-and-by. Yet one recognizes by the prominence of the whole nose,
by the absence of the separation of the nostrils with regard to the
upper-lip, by their regular narrow oval shape the eatarrhine nose. On the
other hand the nose of an examined Afeles grisescens with a distantia
internarina of 0.55 em., with the sharply limited nostrils opening
spontaneously indicates the, platyrrhine monkey. The physiognomy
of Nyctipithecus trvirgatus, likewise mentioned by Is. Grorrroy
Sr. Hinaire, is greatly different from that of the other Platyrrhini.
The animal has a prominent nose and nostrils directed downward
-and sideways. A fossa internarina lies on the inferior part of the
nose. The distance between the upper part of the nose and the rim
of the upperlip is short. The nosirils have for the rest the sharp
limitation of Platyrrhini.

With the prepared nose the distinction of the two forms is also

always possible. With Semnopithecus the nostrils do not lie — as
with Macacus -— any longer on the oral but on the lateral extremity

of the cartt. alares, they are however not enclosed in a labial direction,
but a little crus mediale extends into the septum mobile. The cartilago
alaris of Platyrrhini is stronger and more curved than that of
Catarrhini.

The shape of the nose in the different tribes of Platyrrhini is
little divergent. Only Nyctipithecus forms an exception. With Afeles
the distantia internarina seems to vary considerably. So Is. G. Sr.
Hitaire mentions Lagothrix Humboldt, belonging to the same family,
as a specimen with rather small distantia internaria; it was not the
case with the specimen that I examined. Of Catarrhini some species

133

have a more or less one-sidedly specialized nose. So with Cynocephalis

_ (C. porearius, hamadryas, sphinx, mormon) the nostrils are to the front,

they lie at the oral extremity of the eartt. alares; these have a crus
mediale. A detailed description of Semnopithecus nasicus has been
given by WreDERsHEIM’). With Colobus (Cursinus, C. Pennanti, @. Kirkii)
the prominent part of the medial rim of the nostril, which extends
inwardly into the processus navicularis of (he maxilloturbinale, is

strongly developed ; the nose is flabby, the medial rim covers almost

the nose-opening. With a Colobus ursinus the distantia internarina
was “rather large’, 0.55 em. Of Catarrhini the external nose of
Semnopithecus is least differentiated.

With Cebus the distantia internarina varies between 1,2 and 1,4
em.; with Ateles between 0,55 (Ateles grisescens) and 1,15 cm.;
with Macacus between 0,15 and 0,3 (1 specimen 0,4) cm.; with
Cercopithecus between 0,3 and 0,4 cm. ; with Seinnopithecus between
0,3 and 0,55 (Lophopithecus melanophos 0,6 em.).

Anthropoides are catarrhini like man. In the opening of the nose
no Processus navicularis protrudes. Hylobates has entirely the nose
of Catarrhini. The form of the nostrils is lengthened oval, the
medial side however regularly curved; as no processus navicularis
penetrates into the opening of the nose; the nostrils are not limited
with regard to the upperlip. The flabby cartt. alares possess a
crus mediale, which extends into the septum mobile. In two young
specimens of Simia satyrus | found in the angle cartilago triangularis
a small cartilaginous piece, a cartilago sesamoidea (of the human
anatomy). There is here a vestige of a wing of the nose, the latter
does not contain any cartilage. The oval nostrils lie in the plane of
the face. The external nose of a specimen of a new born human
being which I examined, agrees very much with that of a young
Chimpanzee ; in the latter the nostrils are likewise turned somewhat
downward and to the front. In the new-born and young human
beings the cartilago alaris extends still very regularly into the crus
mediale. Only in the full-grown individual the crus mediale passes
with a sharp deflection, angulus pinnalis, into the remaining part of
the cart. alaris, crus laterale. Cartt. alares minores lie in the lateral
continuation of the cartilago alaris (major). The wing of the nose
does not contain any cartilage. Cartt. sesamoideae lie as with Orang

between cart. alaris and cart. triangularis.

For Is. Georrroy St. Himarre the result of his comparative examin-
ation — consequently his conclusion, that the gulf between Catar-

') Zeitschr. f. Morph. und Anthropol. Bd. IIIf S. 300.

134

rhini and Platyrrhini was almost entirely bridged over both by some
Catarrhini and some Platyrrhini with a middling distantia inter-
narina — was a support for his transformistical conception of the natural
development. This was incorrect, as, I suppose, I have shown: the
external nose of the monkeys of the Old World always differs from
the nose of those of the New World. This fact can be connected
with a supposed common descent, if we admit that in a mutation
period of the ancestors, the two forms of the nose came into existence.

Anatomy. — “On the Jucobson's organ of Primates”. By G. P.
Frets. (Communicated by Prof. Dr. L. Bork).

When examining older stages of development of some platyrrhine
monkeys, Chrysothriz, Cebus, Ateles(?) and Mycetes I always found
a well developed Jacobson’s organ. In some of these foetuses I
ascertained the innervation by olfactoriusfibres. In embryos of 40 mm.
of Macacus cynomolyus and Semnopithecus maurus no Jacobson’s organ
is extant, but a well-developed basal cartilage, of which the Jacobson’s
cartilage forms a part. Very young embryos of catarrhine monkeys
have always a Jacobson’s organ. I made microscopic sections through
the regions of the nose of two fullgrown specimens of Cebus hypoleucus.
A well developed Jacobson’s organ was extant‘) (Fig. 1). It terminates
in the ductus nasopalatinus. A nerve-bundle (Fig. 1 n.J.0) is in
connection with the mucous membrane. I ascertained in series of
older embryos, as I said before, that the nerve for the Jacobson’s
organ belongs to the olfactorius, and consequently I am of opinion
that I may admit, that the nerve found in the full-grown animal is
an olfactorius-bundle. The nerve nasopalatinus of the second branch
of the trigeminus runs through the canalis nasopalatinus and in a
groove between the processus palatinus of the maxilla and the lateral
part of the Jacobson’s cartilage (Fig. 1, . mp.). A lamina praeductalis
‘an be distinguished at the basal cartilage — before the ductus
nasopalatinus —, continuations of which extend to the interior and
to the front. The continuation to the interior and medially is the
Jacobson’s cartilage.

Of Catarrhini,1 examined microscopic sections of the nasal region
of a young Macacus rhesus and a Semnopithecus entellus. In both I
find a well developed basal cartilage ; the Jacobson’s organ however
is missing. In Macacus rhesus, of which I examined a hardly inter-
rupted series, a groove separates itself on both sides of the ductus

') Herzretp found a Jacobson’s organ in Hapale.

135

nasopalatinus, which can be followed to a distance of 36 sections of
25 mw. and lies nearly on the spot of the entrance of the Jacobson’s

Fig. 1.

Cebus hypoleucus. Full-grown. Enlarged 25> 2/3. J. 0. =Jacobson’s organ;

n.J.0. =nerve for the organ; J.k.=Jacobson’s cartilage; n.np.= Nerv.

nasopalatinus; S.”2.—Septum nasi; #.s.—=mucous membrane of the

medial parietis of the nose-cavity; g.s.—= mucous membrane of the palate
V = Vomer; m= maxilla; V = Veins.

organ into the ductus nasopalatinus of Platyrrhini. This groove may
be a rudiment of the Jacobson’s organ; in embryos of Catarrbines
with young cartilage skeleton however, the Jacobson’s urgan, which
is then still extant, lies more dorsal.

All the mentioned foetuses of Platyrrhini possess likewise a small
lamina terminalis dividing the hindmost part of the nose-cavity into
a reduced regio olfactoria and a regio respiratoria.

The Jamina terminalis is found in all mammals with a well devel-
oped olfactoria organ. It separates in the hindmost part of the
nose-cavity from its lateral parietis, divides the nose-cavity into two
parts situated the one above the other, and fuses with the vomer.

136

The independent regio olfactoria, formed in this way, which contains
the olfactoria-conchae, terminates at the end blind against the frontal
part of the praesphenoid.

In an almost fullgrown specimen of Afteles ater I found likewise
an independent regio olfactoria, half a centimeter deep; it is also
extant both in a museumpreparation of Cebus fatuellus (Fig. 2) and
in a specimen of Hapale jacchus which I prepared myself.

Cebus fatuellus. Museum-preparation 1906, N. 3. Frontal dish from the

hindmost part of the nose-cavity, seen from behind. Enlarged 3/, X 3/4.

l.cr. =lamina. cribrosa; G=palata; //=Jlamina terminalis; v. 7. = its

free rim to the front; 7.0. = regio olfactoria; 7.7. = regio respiratoria;

mt = maxilloturbinale; c.m. = concha media; f.c.a. = fossa cerebri anterior;

s. fr. = sinus frontalis, s.m = sinus maxillaris; 0. f. = os frontale; 0. 2. =
os zygomaticum; ™ = maxilla.

Among Catarrhini embryos of Semnopithecus do not show a vestige
of lamina terminalis. Neither does an embryo of 47 mm. of Macacus
cynomolgus do so; in younger Macacus-embryos I found sometimes
a very little independent regio olfactoria. Nor has a young specimen
of Semnopithecus entellus a vestige of lamina terminalis; a young
animal with a shedding dental system of Macacus sinicus possesses
on the frontal parietis of the praesphenoid a little protuberance, a
last remainder of the lamina terminalis.

So we see, that in Platyrrhini a Jacobson’s organ is extant
and a reduced independent regio olfactoria, whilst in Catarrhines
both are missing. Consequently the question presents itself whether
this fact can give any information about the signification of the
Jacobson’s organ. By cauterisation of the organ of a cat and

some rabbits v. Mrmancovics') has tried to discover the function:
the animals continued to live in the same way. Here, with the
monkeys, nature has made the experiment: Plathyrrini have a
Jacobson’s organ, Catarrhini miss it. No communication is known
to me that, e.g. in taking their food, Platyrrhini behave differently
from Catarrhini. In the latter a compensation-apparatus for the
missing Jacobson’s organ might exist. The hypothesis about the
signification of the Jacobson’s organ, most generally defended, is that
it might be of use as a smelling organ in the mouth by tasting
food (vide e.g. Wrprr’) p. 153). If this hypothesis were correct,
it would be possible to indicate in Catarrhini the compensation
apparatus. In makrosmatical mammals the regio olfactoria is separated
from the regio respiratoria by the lamina terminalis. This is not the
ease with Catarrhini; here the cavity of the mouth is in much
better connection with the olfactory region by means of the lamina
terminalis, consequently a separate organ of smell communicating
with the mouth cavity through the canales incisivi is not so much
required, and therefore the loss of the Jacobson’s organ might
be compensated by the disappearance of the secluded independent
regio olfactoria.

HERZFELD *) however communicates a fact which is very unfavoura-
ble to the above mentioned hypothesis. According to this author
horse, ass, giraffe, and camel possess a Jacobson’s organ, but no duc-
tus incisivus communicating with the mouth-cavity. It is likewise
known, that among Chiropteres the Jacobson’s organ is often missing,
— this holds e.g. for Pteropus (Herzreip, ZucKERKANDL *) — whilst
the preparation of this animal shows that it possesses a capacious
independent regio olfactoria.

In virtue of these facts I am of opinion that in the simultaneous
disappearance of the Jacobson’s organ and the independent regio
olfactoria in Catarrhini, and the continued existence of both in a
reduced form in Platyrrhini, we must see a parallel phenomenon,
an indication of the general reduction of the olfactory organ.

1) V. v. Mraatcovics. Anatomische Hefte. XI Band, S. 78, 1898.

2) M. Weser. Die Siugetiere, 1904.

8) P. Herzreip, Zoologische Jahrbiicher, 3 Bd., S. 551.

4) E. ZUCKERKANDL. Sitzungsberichte. Wien. Bd. 117. Math. phys. Cl.

138

Physics. — “The magneto-optic Kurr-effect in ferromagnetic com-
pounds and metals.” UI. By Pierre Martin of Geneva. (Com-
munication from the Bosscna-Laboratory). (Communicated by
Prof. H. pu Bots). |

The purpose of the following work was the extension of the
investigations of Loria’) on the magneto-optical properties of the
newly obtained ferromagnetic compounds and alloys. I limited myself
to the determination of the dispersion of different manganese and
iron compounds, and to a repetition of the measurements for the
case of the three chief metals. The literature has been fully discussed
by Loria so that it is not necessary to introduce it here; his experi-
mental arrangement has been again adopted, for a description of
which I may therefore refer to his publication. The direct vision
monochromator, with high illuminating power, was subjected to a
new calibration. Throughout, pole end-pieces (V) with rectangular
bore were used, the profile of. which (2,5>< 4mm.) was nearly
always exceeded by the size of the mirrors: the latter were irregu-
larly shaped and fixed by means of plaster of Paris.

As a simple relation between the optical constants and the disper-
sion curve was sought for in vain by Lorta, I have not on this
occasion determined the former. In general, for my specimens the
extinction was good and consequently the ellipticity only very slight;
considering the very small rotations in most cases, its determination
appeared as yet scarcely possible of execution although certainly to
be desired.

MATERIALS INVESTIGATED.

Manganese compounds. “Mn 65,Sn 35” = Mn,Sn, and “Mn 35,
Sb 65” = Mn Sb nearly, were very kindly given to me for investigation
by Prof. Tammann. The relations between the amounts of the metals
combined together correspond, according to Honpa, to the most
ferromagnetic compound or alloy respectively ’). Besides these, I
investigated a specimen of MnSb and MnB from Prof. Werpbrkinp
and also Mn Bi from Dr. Hitpert. The metal manganese was found
inactive by Lorta.

Iron compounds. A piece of a carbon alloy consisting substantially
of cementite (Fe,C) was kindly prepared for me by Dr. Hipert.
For normal pyrrhotine (Fe, S,) I am indebted to Prof. P. Weiss of
Ziirich. In addition to these compact magnetic pyrite and amorphous

1) SranisLaw Loria. These Proceedings Vol. 12, p. 835 and Vol. 14, p. 970.
4) Koraro Honpa. Ann. der Phys. 32, p. 1003, 1910.

139

iron sulphide from the laboratory collection were investigated. A
piece of cerium-iron was also subjected to observation.

Metals. For electrolytic iron and also for pure cobalt and nickel |
am again indebted to Prof. Wetss'), who has investigated their
saturation values of magnetisation.

The dispersion of the Kerrr-effect in the metals has been moreover
previously determined by pu Bots *).

I beg here to express my best thanks to those gentlemen who
have assisted me by supplying the materials.

In the following tables are given: 7, the wave-length of the observed
light in wu. A, the double rotation as observed in mm. on the scale
after reversal of the current. ¢, the simple rotation in minutes, de,
the mean error in minutes and percent respectively. V the number
of readings taken for each direction of the current.

MANGANESE COMPOUNDS.

Manganese boride*’ (Mn B). In this case, my attempts to observe
any rotation gave but negative results. Although the material was
porous and on that account the mirror not very bright I was able
to convince myself that if a rotation existed it was less than 0,3’.

Manganese-tin. (Mn 65; Sn 35 = Mn, Sn). The dispersion curve
here remains entirely in the region of negative values (Fig. 1). The

io - 450 550 RGGOni: aa? 065m <Gsewe

Fig. 1.
curve, which in the violet falls rather steeply, reaches a numerical
minimum in the blue and then gradually rises again. The rotation
always remains of a small order as one would expect from con-
sidering the small magnetisability of the material.

Two mirrors on the same piece, obtained by grinding at right
angles to one another, gave results in good agreement as is shown
by tables 1 and 2.

1) P. Weiss, Journ. de Physique (4), 9, p. 373, 1910.

2) H. ru Bors, Wied. Ann. 39, p. 25, 1890. Phil. Mag. (5) 29 p. 253, 1890.

5) E. Wepexinp. Zeitschr. fiir Physik. Chemie 66, p. 614, 1909.

Proceedings Royal Acad. Amsterdam. Vol. XY.

140

TAS LUE aL
e== Fla) Mn4Sn. (saturated) TAMMANN
N | d(4) | A(mm) = (min.) : + dz
|
20 | 435 — 14,8 — 2,24' 0,07= 31),
20 | 466 — 5,0 — 0,75 0:038=4' 5,
20 »\=- 503 4). = tO. anielis 0,02=1,4 ,
205) 561 | 20,2 als 0,02 =0,7 ,
20 | 615 — 28,4 — 4,26 0:02 015 =
20 | 675 —- 36,8 — 5,52 O13 = 0125,
TAA TB AGEs 22,
==7 (4) Mn4Sn (saturated) TAMMANN
N |} ier) A (mm) 2(min.) - + de
15 | 466 — 5,0 -- 0,75' 0,05'= 6,7°'p
1osh 530 — 13,3 — 2,00 0,03 = 1,35,
12 | 567 — 20,0 — 3,00 0,04 ==41,3;,,
15 {e “615 — 28,4 — 4,26 0/04 —
|
|

— Manganese-antimonide (Mn 35, Sb 65 = Mn Sb nearly). The material
of Prof. Tammann showed a strong negative rotation which reached its

(WedeKind)

(Tammann)

Mn Sb

141

numerically highest point in the blue-green and then fell steeply in
the green passing through a minimum at about 580 yu; it then
slowly increased again as it approached the red (Fig. 2).
TABLE &.
pg V) MnSb (saturated) TAMMANN

N | i(42) | €(mm) | -(min.) vats

40 | 435 | — 148,9 | —22,35' 0,15’= 0,759,
35 | 466 | —153,5 | — 23,02 0,06 = 0,25 ,
25 | 483 | — 1547 | — 23,21 0,04 = 0,17,,
2 | 503 | —154,6 | — 23,19 0,03= 0,13,
40 | 530 | — 136,4 | — 20,46 0,03 = 0,15,
21 | 567 | —115,7|—1736 | 0,01—0,06,
2 | 615 | — 119,0 | —17,86 0,02 =0,11,
35 | 675 | —125,0 | — 18,75 0,02 = 0,11,
|

A second specimen of MnSb coming from Prof. Werpekinp gave a
similar dispersion curve agreeing in character with the above. The
rotation however always remained smaller than in the case of the
first specimen. It can therefore probably be assumed that this
corresponds better to the ferromagnetically best compound Mnsb,
whose existence has lately been established with great probability by
Hivpert and DiEcKMANN ‘*).

TABLE 4.
e—= FO} MnSb (saturated) WEDEKIND
N | i (4) | A (mm) | :(min.) | + de
30 | 435 | —961 | 1441") 0,16'= 1,1%
25 | 466 | —97,1 | —1451| 0,09=06,
20 | 503 | —970 |°—1455| 0,05=03,
21 | 530 | —910 | —1353| 0,03=02,
20 | 567 | — 80,9 | 1214 0,01=9,1,
20 | 615 | —81,7 | —1225| 002=02,
a1 | 675 | — 87,5 | — 13,14 | 0,05 = 0,4 ,

1) Cf. Koraro Honpa loc. cit. E. Wepex:xp, Chem. Ber. 40 p. 1266, 1907
S. Hitpert and Tu. Dieckmann, Chem. Ber. 44 p. 2833, 1911.

142

Manganese-bismuthide*) (MnBi). The rotation, which was negative at
both ends of the spectrum (Fig 3), reached a positive maximum at
530 uu. Points of inversion were found at 468 uz and 617 qe.
Although the mirror was not very bright I was yet able to measure
the rotation fairly accurately in spite of its small amount.

TABLE 5.
J fe Mn Bi (saturated) HILPERT
N | d(4r) | 2 (mm) = (min.) +4
| |

95° |: 435. |) SSO | sso! | 0,13 = 1),
pgs | 480 2|) gaa odio nad as
50 -|\.2A66.0| 231i 20a 2] <s0Md epi
os | 483 | eee a ne oss
21 503 | + 84 b 24126 | 003 =2->
21 | 530. | 4 10,0] 2h 4g 41003 =? c»
21 | 567 | + 63 | +0,94 | 0,03 =28 »
70 | 615 | +03 | 40,045] 0,015 =333>
30° || 6% 4 2 abo bee | ee

IRON COMPOUNDS.

Tron carbide (Fe,C, Cementite). As the material contained for the
most part cementite in needle-like crystalline layers mixed with other
substances, the mirror was treated with sulphurous acid so that the
cementite surfaces did not change their reflecting power while the
other constituents were strongly darkened. Measurements carried out
on six different parts of the surface yielded somewhat different
results. All the curves however show a certain similarity viz. a very

1) S. Hmperr and Tu. Dieckmann, Chem. Ber. 44 p. 2831, 1911. E, Wepexinp
and A. Verr, Chem. Ber. 44 p. 2665, 1911.

145

strong negative rotation having a numerical maximum in the violet
and indicating a decrease towards the ultra-violet. It falls steeply in
the blue region until the green or yellow-green is reached and then
increases again towards the red. The carbon atom of the carbide
accordingly produces a considerable change in the dispersion curve,

compared with that of pure iron (table 12). Four of the curves are

represented in fig. 4 and tab. 6 to 9. The two other places gave a
smaller rotation. A consideration of the etched figures on the surface
show that a better agreement for such a complicated structure can
hardly be expected. On this account the investigation of alloys appears
altogether more difficult than in the case of well defined compounds.

TABLE 6.
e= f(*) Tron carbide (saturated) HILPERT
N | Aun) | £ (mm) |- =(min.) $3:
30 | 435 | —201,9 | —30,28'| 0,05'=0,17%y
25° |° 450 | — 200,0 | —30,00 0,03 =0,10,,
20 ‘ 466, | —196,3 | —29,42 | 0,02=0,07,,
20 483 | — 1808 | —2848 | 0,02=0,07,
20 | 503 | —180,8 | —27,13 | 002=007,,
26 | 530 | —1763 | —2645 | 0,01—004,,
20 | 567 | — 1760 | —2640 | 0,02—0098,,
20 | 615 | i717 | —26,66 | 0,01 =0,4,,
20 | 675 | — 1801 pa euet | 0,03=0,11,,
|

144

LAB Esk
N i(4r) | £ (mm) | :(min.) +e
25 435 | — 161,4 | — 24,20 0,10'= 0,49 9
25 466 —166,1 —24,91 0,05 = 0,2 ,
20 | 503 | —157,8 | — 23,66 0,07=0,3,
20 =| 580.) —— 14a ae 005012
20-| 567 | —1360| —20,40| 002=0,1,
20 | 615 | — 130,64" = 20,51 0,02 =0,1,,
20 6715 | —1468 | — 22,02 0,04 =0,2,,

| |

TAS Lewes
N d4(u¥) | L (mm) | = (min.) +:
95 | 435 | —170,0 | —25,50'| —0,05'= 0,29,
25 | 450 | ~171,7 | — 25,75 003=0,1,
20 | 466 | =e |) 25h 0,03 = 0,1,
0 | 493 | —171,7| —25,5!/ 003=0,1,
20 | 503. | tesa = oat 0,03 = 0,1 ,
20 | 530 | 15034) 2255 0,02 =0,1,,
20 | 567 | — 1431 | —21,46 0,02 =0,1,
20 | 615 | —1494| —22,40 0,03 = 0,1,
20 | 675. |) “= 4161,0' |. ean 0,03 = 0,1,

TABLE 9.

a
N (4) 4 (mm) = (min.) + 0:
mc a

30 435 | —181,0 | —27,15' 0,07'= 0,3 %/
25 466 | —178,7 | —26,79 0,03 =0,2 ,
30 503 | —161,0 | —2414 0,04=0,1 +
25 530 | —147,5 | —2213 0,01 = 0,04 ,
25 567 | —145,4 | —21,81 0,01 = 0,05,
20 615 | —150,0 | —2250 0,01 = 0,04 ,
20 675 | —156,3 | —23,44 0,03=0,1 ,

145

Normal Pyrrhotine (Fe,S, = (FeS), Fe,S,, from Morro Velho, Brazil).
The piece. with which I made my measurements was polished, in
the first case, parallel to the magnetic plane and in the second case
in a plane normal to this and to the direction of easiest magnetisation °).
The first mirror, as was to be expected, showed no rotation whatsoever.
On the second surface however a positive rotation of the order
of one minute was to be observed for the whole region of the
spectrum. Even at ihe ends of the spectrum no indication of an
inflection in the dispersion curve could be found: (perhaps a trace
of an increase in the violet). I repeated the same measurements
thereupon more accurately, the slit of the monochromator being
widened, using a brighter yellow and blue illumination. The field here
amounted to at least 12 kgs.

A BEE 10:
e==f() Normal Pyrrhotine (saturated) WEIss

N | i(@#) | £ (mm) | (min) ie

35 435 |. +66 | +0,98'| 0,04'=4)),

30 > Le 00 0,05 =5>
25 466 | +63 | + 0,94 0,04=4 >
20 46g.) 6G.) 4: 0:97 0,04=4>

20 503 | +64 | +0,95 0,03 = 3»
20 | 5390 | +65 | +0,96 0.03 =3>
20 567 | +64 | +0,95 0,02 = 2»
20 | 615 | +66 | +097 0,03 =3 >»
% | 6 | +63 | +10, 0,04 = 4»

30 7 oe. Ge | +097 | 003=3>
20 ~blau | +64 | +0,94 0,02 = 2 »
is ge) hn" | 10,01-— 1 >
20 | gelb | +64 | +095 | 0,02=2>
ae +65 | +0,96 C0t— fs

Compact magnetic pyrite (presumably from Obermais, Tyrol). A
naturally reflecting surface was previously found by bv Bors to show

1) According to the above formula this substance ought to be regarded as Sulpho-
-pentaferroferrite. P. Wess, Journ. de Phys. (4) 4 p. 469, 1905 finds for the
saturation value of magnetisation about 60 to 75 G.G.S.

146

no effect: this was irregular and moreover parallel to the magnetic plane.
In the present work, as in the case of pyrrhotine, a mirror was
obtained by grinding, normal to the above. It gave a small positive
rotation of some tenths of a minute.

Amorphous tron sulphide (Fe §). This substance, which is not ferro-
magnetic, was also investigated by pu Bots ].c. in 1889: The same
mirror now also gave a negative result. Should a rotation exist, it
must be smaller than 0,3’.

Cerium-iron. The dispersion in the case of pyrophorous cerium-
iron of unknown composition exhibited nothing exceptional. The
rotation increased a little on passing from violet to red. The material
was not quite saturated.

TASS
e = f(i) Cerium-iron (nearly saturated)
N | 2%») | Q(mm) | <(min.) | +e:
25 435 — 336", |" > 500" | 0,05'=1 %
20 466 eile ee 0,04 = 0,7,
20 503 22395 yl = ad 0,02 =0,3,,
20 530 eee hse eee 0,01 =0,2,,
20 567 —427 | —641 | 0,01=0,2,,
20 615 | —435 |-—652 | 0,02—03,,
25 675 | —440 | —6,60 0,03 = 0,4,,
LA BL Ea
s=f() Iron (unsaturated) WEIss
N | (42) | Q(mm) | :(min.) | + é:
25 435 | — 126,4 ted 18,96'| 0,10’ = 0,5 %
20 483 | —131,0| —1965) 0,05=0,25,
20 530 | —136,6| —20,47 | 0,03 = 0,15 ,
20 567 “| °— 141,7 | -— 21,25 | 0,02 = 0,09 ,,
20 615 | —1495| —2242| 0,02=0,09,

20 675 | --164,6| —24,70| 0,03=0.12,

147
METALS.

Tron (electrolytic). The dispersion curve remains throughout in the
negative region, numerically increasing from violet to red with an
indication of-a minimum in the ultraviolet. The iron investigated by
pu Bots, loc. cit., showed a dispersion of a similar but more marked
character. The material was not saturated.

Cobalt. The curve showed a flat numerical minimum in the blue-
green near 530 yu. Otherwise there is nothing particular to be
noticed. .In the case of the impure cobalt investigated by pu Bots the
minimum was even less marked.

TABLE 13,

a7 (2) Cobalt (unsaturated) WEIss—
N | (4) | 4 (mm) | z(min.) | + ¢:

25 | . 435 | 1417 | — 21,25'| 0,12’ = 0,560/,
20 | 483 | — 1346 | — 20,20 0,05 = 0,25,

20 | 530 | — 1315 —19,74|} 0,02=0,10,

20 | 567 | —1328 | —19,92 0,01=0,5,

20 | 615 | —1353| —20,28 0,01=0,05,

20 | 675 | —141,0} —21,15| 0,03=0,14,
|

Nickel. The curve showed a minimum in the yellow but otherwise
no singularities. The dispersion of the original nickel-mirror of
pu Bois was exactly proportional to this. The metal was not completely
saturated.

‘hk A. Bl Et.
e== f (0) Nickel (nearly saturated) WEISS
N | 4(#) ees (mm) | -(min.) | +0:
}
20 | 435 | —57,6 | —864' | 0,05'=0,56/,
Doe. dee | = S560: | —830 0,02 = 0,24,
eel 530, 12546. | = 8.15 0,01 =0,12,,
20 567 | —53,3 | —8,00 0,01 0,12,
20 615 | —55,5 | —8,32 0,01=0,11 ,
20 675 | —59,7 | — 8,96 0,02 = 0,22,
‘ i

148

Physics. — “The effect of temperature and transverse magnetisation
on the resistance of graplute.” By Davw EK. Rosgrts. (Com-
municated by Prof. H. E. J. G. pu Bots),

The investigations of Grunmach and Wueipert'), Parrerson’) and
others on the effect of transverse magnetisation on electrical resistance
show that paramagnetic and diamagnetic metals exhibit an increase
of resistance when magnetised, while the three ferromagnetic metals,
at least in sufficiently strong transverse fields, show a decrease.
Although as yet no simple relation may be given between the order
of magnitude of this effect and the corresponding magnetic suscep-
tibility, it may be noticed that the effect increases in the ratio of
one to a hundred as we pass from paramagnetic tantalium to dia-
magnetic cadmium and suddenly again a thousandfold as we pass on
to bismuth. This element, as is well known, possesses rather a high
diamagnetic specific susceptibility (— 1,40.10~¢). Soon after Morris
Owen *) found Ceylon graphite to show the highest value yet observed,
Dr. W. J. pe Haas was led, by analogy, to anticipate that graphite
might exhibit a variation of resistance of an even higher order when
magnetised and suggested to me to search for the effect. The
preliminary experiments‘) performed with powdered graphite pressed
into a thin plate, with irregularly shaped pieces and with ordinary
pencils amply satisfied expectation and justified an extended investi-
gation of the phenomenon.

Well defined crystals of graphite are exceedingly rare and could
net be procured ; the ordinary material occurs in lamellar agglome-
rations, cleavable with great ease along surfaces parallel to the base
of the hexagonal system. From a chemical point of view the structure
is possibly very complicated; graphite is generally considered, above
372°, the most stable of the three allotropic carbon modifications.

The conductivity for heat of this substance has lately been studied
by Kornicspercer and Weiss*). The resistivity as formerly determined
by several observers ") is as follows:

1) L. Grunmacn and F. Weimert, Ann. der Phys. 22 p. 141, 1907.

*) J. Patrerson, Phil. Mag. (6) 3 p. 6438, 1902.

5) Morris Owen, Versi. Afd. Natuurk. 20 p. 673, 1911. Ann. der Physik. 37
p, G57, 1919.

4) When magnetised transversely in a field of 20 kilogauss, the compressed
powdered Ceylon graphite gave an increase in resistance of 52 °/); an irregularly
shaped piece gave 219°/); HB and 5B pencils by A. W. Faser gave only 3°/p
increase,

*) J. Koeninaspercer and J, Werss, Ann. der Physik. 85 p. 27, (911. Verh. d.
Deutsch. physik. Ges. 14 p. 9, 1912.

6) See Handb. der Anorg. Chemie 3 (2 Abtl.) p. 54, 1909.

149

Graphite from Ceylon at O° ' 12.10-4 ohm per em?
% MSS tie AIO oi vjaghse
- wee erernland..;, 150s) 410-4. se

The best of my samples gave a resistivity as small as 0,5.10-4,
ie. roughly about half that of mercury (0,96.10-4 at 18°): this zn-
creased with rise of temperature by about 0,001 per degree. The
resistivity of amorphous carbon has always been found to be much
larger and is well-known to decrease with rise of temperature; the
coefficient diminishes, however, as the transformation into the graphitic
modification proceeds’), although it has never been observed to
change its sign.

With regard to the effect of magnetisation Parrerson |. c. found
the resistance of a glow-lamp filament to increase by 0,027 percent
in a transverse field of 25 kilogauss. According to Ciay®*) the resis-
tivity of such a filament decreases by 24°/, on heating from — 255°
to 0°. Laws’) has investigated the effect for transverse magnetisation
of glow-lamp filaments, pencils and graphite without finding it to
be of a high order. He found, at ordinary temperatures, the increase
of resistance of the graphite in a field of 11 kilogauss to be about
1°/, of the resistance when outside the field, while at the temperature
of liquid air the effect was increased threefold. Within this small
range the increase of resistance was found proportional to the square
of the field and between the temperatures 18° and —186° inversely
proportional to the absolute temperature. As will be seen these results
are not in agreement with those found in the present research.

EXPERIMENTAL ARRANGEMENT.

The specimens most used in this investigation were prepared from
the same Ceylon graphite as that used by Owen in his researches
on its thermo-magnetic properties; a chemical analysis has not yet
‘been made. Short rectangular pieces (7—10 mm. long, 1—2 mm.
wide and 0,1—0,5 mm. thick) were obtained by careful cleavage
and those selected for investigation which appeared of most pro-
nounced and uniform crystalline structure. For the determination of
the effect of transverse magnetisation they were, in general, supported
in the magnetic field so that the cleavage planes were perpendicular
to the field i.e. the crystallic axis was parallel to the lines of force.
On supporting the pieces freely in a magnetic field it was observed

1) See Handb der Physik 4 p. 380, 1905. G. Wiepemann, Elektrizitaét, 1 p. 539,
Aa2.. -

*) J. Guay. Dissert., Leiden 1908.

3) S. C. Laws, Phil. Mag. (6) 19, p. 694, 1910; his graphite was obtained from
the Morean Crucible Co., London.

150
that they moved so that the crystallic axis set itself perpendicular -
to the field, this axis thus coinciding with the direction of maximun
diamagnetic specific susceptibility, which according to Owen may
reach -—15 millionths.

The magnetic field of the latest large type model of the pu Bots
half-ring electromagnet was used. To obtain the higher fields at
ordinary temperatures special prism-shaped pole end-pieces were
used — 13mm. long and 1,2 mm. wide. — With these end-pieces
(0,7 mm. apart) and a pair of extra polar coils a field of 50 kilogauss
could be easily attained. For observations at low and high temperatures
the same arrangement was used as that adopted by bu Bois and
Wits in conjunction with the large type electromagnet’). The
magnetic fields were measured by means of an exploring coil and a
ballistic galvanometer ’) in the usual way. It was assumed provision-
ally that the fields were appreciably the same at all the tempera-
tures used for a given current through the electromagnet.

The resistance of the graphite specimens, both in and out of the
field, was determined by -a potentiometer method *), being compared
directly with known resistances (0,1—1,0 ohm). The current through
the graphite during a series of measurements was varied between
2 and 0,5 milliamperes according to its resistance. In order to
eliminate thermo-electric junction effects the current in the main
circuit as well as the potentiometer connections were successively
reversed. The changes of resistance involved being considerable it
was found necessary to adjust the sensitiveness of the potentiometer
arrangement during a single series of readings; this was initially
sufficient to detect differences of */,,,.. ohm. Small irregular variations
in the resistance of a particular specimen were observed after it was
subjected to the action of magnetic fields or to widely different
temperatures. This change, however, amounted in general to less
than 1°/,. Through the kindness of Dr. Horrmann the resistance of
specimen G,15 — that used in the experiments at different tempera-
tures — was re-determined at 18° in the Phys. Techn. Reichsanstalt
by means of DresseLnorst’s ‘compensation apparatus’ *) and a
differential galvanometer; good agreement was found. Some of
the preliminary measurements had been made with WHEaTsSTONE’s
bridge method and, when repeated potentiometrically, practically the
same results were obtained.

1) H. vu Bots. Ztschr, fiir Instr.kunde 81, p. 362, 1911.

*) H. pu Bois. The magnetic circuit in theory and practice, p. 300, London 1896.

8) F. Koutrauscn, Prakt. Physik. 11 Auflage p. 422, 1910. ;

4) H. Diessetnorst, Zeitschr. fiir Instr.kunde. 26 pp. 173, 297, 1906; 28 pp. 1,
38, 1908. :

“~_oAS es UP

By deft

> ial
ee ae

vf oe

151
EXPERIMENTS AT ORDINARY TEMPERATURE [18°].

About twenty specimens of Ceylon graphite were investigated,
which all gave variations of resistance of a high order, the increase
of resistance in a field of 20 kilogauss varying however between
300 and 500°/, of the resistance in zero field. Considering the
difficulty of obtaining specimens of graphite of definite crystalline

‘structure and having regard to the impurities occurring in the natural

substance these variations in the magnitude of the effect are not
surprizing. About five specimens, which gave a variation of resistance
of greatest order were investigated more particularly; by analogy

with the well-known behaviour of more or less pure bismuth *) the

assumption appeared justifiable that these were more likely to be
pure and perhaps of more uniform crystalline structure. Some of the
specimens were supported free between thin mica or glass plates;
when imbedded in sodium silicate, collodion or Canada balsam allowed
afterwards to solidify they did not experience any change in the
magnitude of their increase of resistance in the magnetic field, thus

eliminating any doubts that the effects were due to bodily strains

in the graphite. In the final experiments at different temperatures
the graphite pieces were supported by fine flexible wires between
thin mica plates so as to avoid any strain due to possible expansion
or contraction. The specimens could be mounted with their connections
so that the total thickness amounted to less than 0.7 mm, thus
enabling them to be examined in fields up to 50 kilogauss. Some of

R _ ISOTHERMAL CoRVES. 6-/%*
TRANSVERSE Magne TISATION,

Seecimen RB

$4 | Qtt3de
$0. \Q080..
$i \aer6 2

G 12. \aey3.

§ /§ \0032..

SS)

= Pace ce a ao Bee
ee

Cand fil

152

the isothermal curves obtained for different specimens, at 18°, with
the cleavage plane normal to the field, are shown in Fig. 1.
Attempts to identify the curves with such equations as
Hb pe eae: +...
ik, tie c c .
failed; it was found however that all the curves obtained at ordinary
temperatures could, well within experimental errors, be represented

by the formula

R R
Bo Ses oe ere. eee
where &,, resistance at O° for = 0,
te ss tO? tor 2 —_ a
t'; - ,, O° in transverse field 9.
A,n Constants.

Owing to the difficulty of determining the dimensions of the
specimens it is unfortunately impossible to give their absolute resistivity
with any exactitude.

From equation (1) we have, taking logarithms

R'—R
ee

log

which can be represented by a straight line, the coordinates being
log (R’—R) R, and log §.

The values of log(R’—R)R, and log, corresponding to the
curves shown in fig. 1, when plotted were found to lie on straight
lines practically parallel to one another, indicating that m is the
same constant for each of these specimens. In the case of specimen
G. 15 — the one which gave an increase of the greatest order —
equation (1) did not hold as well as for the other specimens although
the mean value of m was the same for this as for the others.

LABEL

Isothermals at 18°

Specimen | Ro R'/Ro = RIRo + An

G.4 | 0.0430 ohm. | 1.01 +-0.0171 wt.748
| G10 | 0.0792, | 1.01 -+ 0.0205 m1.74°

G.11 | 0.0162, | 1.004 + 0.0162 w1.748
2 | 0.0430 , | 1.014-+.0.0188 gt.745

5 0.0316

Eee
—_—|— _

» | 1.02 + 0.0214 yl.745

_—
on. <a ly
=
he

2
« ~
«
_

*,
+ peu
5

- .
-“
=
7 te
a

" ~—_
<r
a

et
ae -

f 2
c a

a
-

or n= 7/4.

153

‘The values of A and n obtained for the different specimens are

given in Table 1. For each specimen n = 1.74°?).
A specimen was also prepared for investigation from another piece

of Ceylon graphite out of the laboratory collection. This graphite

very easily split up along its cleavage surfaces but pieces of uniform
structure of suitable form were difficult to obtain. The best piece
I could prepare gave an increase of resistance of only 182°/, in a
field of 20 kiloganss, the resistance out of the field being 0.0427 Ohm.
A piece of graphite from Himbuluwa (Ceylon), which was investi-
gated, on the other hand, gave quite different results. The upper
side of this graphite possessed a quite smooth and polished surface
underneath which however it appeared to be of a fine granular
structure. A thin piece of this upper layer was removed and the
variation of its resistance found when transversely magnetised. An
increase of resistance of 220°/, was observed in a field of 20 Kgs,
the resistance out of the field being 0.0786 ohin. A thin piece removed
from the under side of the same material, and having a high natural
polish on both of its cleavage surfaces gave the anomalous results.
Its resistance outside the field was several hundred ohms and diminished
very rapidly with increase of temperature. In a magnetic field however
no change in its resistance could be observed, while rough experi-
ments indicated that it was apparently paramagnetic; no test for the
presence of ferroginous impurities was made.

‘Specimen G 12 was also tested with its cleavage plane parallel
to a transverse field, the crystallic axis being therefore at right
angles to the lines of force. In a field of 26 kgs the value R’/R,
was found to be only 1,15 while for the usual position this ratio
is rather more than 6. This evidently proves the necessity for very

accurate adjustment of the angle between the crystallic and field

axes*): an analogous question is known to arise in the behaviour
of nickel and other ferromagnetic wires.

EXPERIMENTS AT LOW AND HIGH TEMPERATURES.

Observations were taken at temperatures of — 179°, 0°, + 18°,
-+ 95° and + 179°, the field being varied from 0 to 40 kilogauss.

1, Within the experimental errors the exponent may also be n=V 3 =1,732

*) The effect of longitudinal magnetisation was also observed. The increase of

resistance involved was found to be independent of the direction of the current

and of the same order as that observed in this last described position. Experiments
are in progress to study the effect in both these cases at different temperatures.

154

The method of measurement was the same as at 18°; the deter-
minations afforded no difficulty, the resistances being quite steady.
At the lower and higher temperatures thermo-electric effects were
sometimes evident but by successive reversals these were eliminated.
It was incidentally observed that these thermo-electric effects — when
occurring at the connections of the graphite and therefore within the
magnetic field — were also influenced by the field *). Thus in one case
the thermo-electric effect was increased fourfold by a field of 38 kgs. For
all the specimens examined (with the exception of the piece from
Himbuluwa) the resistance of the graphite out of the field was found
to increase with the temperature, the coefficient of increase of resi-
stance being of the order 0,001 per degree. The ordinary temperature
curve R= funet. (6) for =O is given in Fig.2 for G15. Very

REsisTANCE Rw O4MS

CHANGE of Resistance

TEMPE RATURE

TEM PERATUREO

Fig. 2.

nearly the same type of curve was obtained in the case of specimen
G11. It is interesting to compare this with the curves obtained by
KaAmertincH Onnes and Nernst’). The temperature during a series
of readings, the graphite being in the field, was determined as
follows. Before commencing, the current required to be sent in the
reverse direction through the magnet to reduce the residual tield to
zero, was determined. Then, to measure the temperature, the graphite

1) These effects are being subjected to further detailed investigation.
2) H. Kamerunen Onnes, Versl. Afd. Nat. 19. p. 1187, 1911. W. Nernst, Sitz.
Ber. Berl. Akad. p. 306, 1911.

155

being in position, this reverse current was set up and the resistance
of the graphite found. The temperature of the graphite was then
deduced from the temperature curve ($= 0) fig.2. Owing to the
difficulty of exactly getting rid of the residual field without setting
np a field in the opposite direction, and on account of the small
change of resistance with temperature, this method of determining
the temperature does not seem to be susceptible of great accuracy.
The isothermals at low and high temperatures were determined for
G1i and G15. Except for the difference in the magnitude of the
changes of resistance concerned similar results were found. The
results obtained with specimen G15 are shown as isothermal curves
(fig. 3) from which the so-called isopedic curves (J) = constant) may

TsormenmatCugves, GS
Transverse. SISGHETISATION.

Fig. 3.

easily be deduced. As will be seen, the increase of resistance is
much greater at low temperatures. At the temperature of liquid air
the increase is 9300°/, for a field of 38,8 kgs, the increase at 18°
being 1250 °/,.

The isothermal curves for the lower temperatures cannot be re-
presented by an equation of the form (1); at higher temperatures
this seems to be the case, although more accurate measurements
appear desirable.

11
Proceedings Royal Acad. Amsterdam. Vol. XV.

156

Physics. — “Translation series in line-spectra.” By T. van LOHUIZEN.
‘Communicated by Prof. P. ZrEmay).
(Communicated in the meeting of May 25, 1912).

In my preceeding communication ') I told already how I had suc-
ceeded in discovering series in the spectra of Tin and Antimony by
makine use of a model which was the result of a spectral formula
found by me empirically, which formula was based on the fundamen-
tal thought: ‘‘Every series in a line-spectrum of whatever element
can be represented by one and the same curve when the frequen-
cies are considered as function of the parameter, and the curve
refers every time to another system of axes.”

I will now show how this fundamental thought may be serviceable
to arrange the series of systems of the different elements in better
order. It is true that some order has already been brought in the
great material of observation*) by the discovery of numerous
series by Rypperc, Kayser and Ronee and others, and recently
particularly by the “Kombinationsprinzip”, discovered by Rrrz, but
it is exactly this great number of series and combinations that
threatens to destroy the order and bring confusion. If we consult,
e. g. a treatise by Dvcyxz*) which was recently published, - we
find there a great quantity of material of observation arranged
according to Rirz’s spectral formula and the ‘‘Kombinationsprinzip”’,
but it appears already very soon that specially for the numerous
- combinations the order leaves a good deal to be desired. It is impossible
to have a survey of the matter. That this way of arrangement is
not the only one, is shown by Mocrnporrr *) in his communication
on “Summational and differential vibrations in line-spectra’, in which
most of the combinations are indicated as summational and differential
vibrations. Though the system is by no means lucid here either,
yet we will for a moment retain the idea of differential vibrations.
Already before PascHen *) had about the same idea when he says:
“Die Linien eines Seriensystems sind darstellbar durch eine Anzahl
von Termen, deren Differenzen die Wellenzahlen (bzw. Schwingungs-
zahlen) existierender Linien geben.”

The first thought of this sentence is already found in RyppgEre,
where he takes the asymptote of the principal series as a special

1) These Proce. p. 31.

2) Gf. Kayser, Handbuch der Spectroscopie Bd. V and Exner and Hascuex, Die
Spektren der Elemente bei normalem Druck.

8) Unsere Kenntnisse von den Seriengesetzen der Linienspektra.

4) Proc. Royal Acad. Amst. Nov. 25, 1911.

5) Jahrbuch der Radioaktivitét und Elektronik Bd, 8, Heft 1.

157

value of the fraction which occurs in the formula of the 2°¢ sub-
ordinate series. LORENTZ *) too holds the same idea in his theory on
the ZremAn-effect, where he says: “In connection with this, it should
also be noticed that, in Ryppere’s formulae, every frequency is
presented as the difference between two fundamental ones”. A more
independent meaning is assigned to these fractions by Hicks *), who
gives them the name of ‘‘sequences”’.

He distinguishes viz. four kinds of them:

1. Principal (P) sequence.

2. Sharp (S) sequence.

3. Diffuse (D) sequence.

4, Fundamental (/’) sequence.

In agreement with the theory given by Rirz*) Hicks expresses himself
as follows *):

“Tt appears, that, whatever the kinetic configuration may be, which
-is the source of the vibrations, the light periods depend on the differ-
ence of frequency of two systems each with distinguishing train
of frequences’’.

In Dunz*) we find the values of these systems calculated and
indicated as mp, ms, md, and m&p, in which we recognize Hicks’s
sequences, and about which we may notice that when we confine
ourselves to one component, al/ the series and combinations are
formed from these four “sequences”.

In the following manner this system may at once be reduced to
order, so that it is easy to survey:

All the series and combinations may be graphically represented
by one and the same curve, which is subjected to four different
rotations with regard to the original system of axes. All the series
that are represented by curves of equal rotation, belong together
and differ only in asymptote. They may be changed into each other
by a translation of the curve parallel to the-y-axis. We shall there-
fore call them Translation series. The asymptotes may be found
from a curve with the same or with another rotation. So every
spectral line is determined by its number on the curve and by the
asymptote of this curve.

Before entering into a fuller explanation by means of the annexed
plate, I should first point out the necessity of the introduction of

1) Theory of Electrons etc. p. 128.
2) Phil. Trans. 210 A 1911 p. 57 et seq.
3) Magnetische Atomfelder und Serienspektren Ann. d. Phys. 25. 1908 p. 660 et seq.
aE cp. 96.
5) |. c.
3d Se

158 -

an all-including notation. This necessity already appears on a cursory
examination of the notations used by PascHEen (Ritz’s notation),
Hicks (a modified RyppBere notation), and Mocernporrr (in the cited
communication), while, as we saw above all three entertain
about the same idea about the differential action. Let us now try
to bring unity in this by considering the thought they have all in
common, viz. that in accordance with Rrrz’s theory *) on the magnetic
atomic fields, every spectral line is brought about by the difference
of Two actions.

"So in the notation of every spectral line it should be expressed,
with what member of what two series (sequences) it is related. For
the designation of these series the nomenclature introduced by Hicks”)
is the most convenient, because the notations mp, ms etc. exist al-
ready also with Rirz’s formula.

So we distinguish :

1. Principal series or Pe (e=1 aoe)
2. Sharp series or See = 1 aa ee)
3. Diffuse series or Da @= 1S ae

4. Fundamental series or Fr @@=1.2.3...)

The form of these series is somewhat different for the different
spectral formulae, but yet there is close agreement. The numerators
are the same for all three, (Ritz, Mocgrnporrr-Hicks, and mine),
viz. the universal constant 109675,0. The roots from the denomina-
tors are threeterms. The first term of it is the parameter (m or 2),
the second a constant (a, p; 5, dor, 4), the coefficient of the third
term being denoted by (6,2,9,¢ or y). Let us now also bring
agreement in this, and in imitation of Ritz introduce different, but
corresponding symbols for the different series, so for the constant
terms resp. p,s,d, and /, and for the last coefficients resp. x, 6, d,
and ¢p.

Then the meaning of. Pr, Sx ete. will be according to the formulae
of Rirz, (2), of Mocunporrr-Hicks (ZH), and according to my
formula (£): (see table p. 159).

X may be put here: 1.2.3... The notation, as Ritz introduced
it for the 2"¢ subordinate series (1,5; 9.5: 35.5. .) should be dis-
carded. It makes the matter difficult to survey. Though for some
metals we do get the impression that we have to do with x + 0,5 +
a certain fraction, this is by no means the ease for all, and I
entirely coneur with the conclusion of Hicks‘), who has inquired
into this matter more closely :

159

: .

| R MH L
Pex 109675.0 109675.0 __109675.0°

| (x+e+35): (z+p+—) (t+Pp+77)
Sr = | __109675.0 | __—:109675.0 _ 109675.0

(2+s+3) (2+5+2) (7+ s+7-y)
Dr= | ___109675.0 * | 109675.0 _ 109675.0 —

ay é\? oy
ee ey ee), | rer or
| 1096750 | _109675.0 109675.0

ae — | o\2 ae * oes =
(e+r4+2) | (24r4t) | StF

|
I

“Also it shows conclusively that such difference cannot be 0,5,
a supposition, which has suggested the idea that the P and S are
similar series, P with even numbers and S with odd”.

About the Fz we may remark that / differs very little from a
whole number, and that g becomes practically equal to zero. So
the denominators differ very little from 37, 4’, ete.

After we have ascertained this, the designation of every spectral
line is self-evident. We must, namely express in the designation,
of what two terms of what two series its frequency is the dif-
ference. So the second line of the principal series is represented

\ by S,—P,, the whole principal series by S,—Pv. So we may omit
the sign — for simplicity, and write S, P, resp. S, Pe.
A priori the following series are possible:

|
Up to now only one or more lines have been observed of the
series printed in big type.
The series in column I we call Principal series. They form together
a group of Zranslation series (cf. p. 157), and differ only in asymptote.
ee ep 77.

160

As asymptotes are known up to now P, and §,, whicb both also
occur in the Natrium system, which has been drawn on the adjoined
plate. To the Sharp series, as we shall call all the series belonging
to column II, the same thing applies. They too form a translation
group, in which P,, P,, and P,, occur as asymptotes, with all three
of which we meet again also for the Natrium. The translation group
of the Diffuse series, which all belong to column III has as asymp-
totes: P,, P,, P,, S,, and S,, the four first-mentioned of which occur
in the Na-spectrum. Column LV contains the Mundamental series, which
have as asymptotes P,, S,, D,, D, and F,. Only P,, D, and F,
occur in the Natrium spectrum.

In case one should object to the names of Diffuse and Sharp
Series, because not all the lines of all the diffuse series are diffuse,
and not all those of all the sharp series are sharp, we may also
simply speak of D- resp. S-series. In this connection I will quote
an expression of Hicks °) :

“Regarded from this point of view, we may look upon P as
standing for positive, D for difference and S for semi’.

To make clear the connection between the old and the new names,
this table may serve: (see p. 161).

If a series is composed of several components, they may be
distinguished by accents,, e.e: P, Dz, Pl Da; PD: It Asai
worthy of note that the different components of the S-, D-, and F-
series resp. belong to the same translation group. Only for the P-
series it is slightly different. There the asymptote remains the same,
but the curve for the two components has a somewhat different
position. So S,P'z, which denotes the 2°¢ component of the principal
series, belongs to the same translation group as P,'P'z, which group
however, differs somewhat from that of the P-series. They occur
both also for Natrium, but have been omitted on the plate for
clearness’ sake.

If we examine this plate, we notice ‘first of all, that al the recorded
curves were drawn off the same pattern curve, which consists of a
thick brass plate, into which according to my data the curve:

109675.0
i =

has been inciged in an exceedingly careful way, so that «= 1 is repre-
sented by a distance of 4¢.m., while y= 10*4—'! (A expressed in A.U.)
has been taken so that 1 m.m. corresponds to a frequency 100.
The other sides of the templet constitute the two axes of the system, on
which the curve has been drawn. Both sides are provided with a

l) lc. p. 96.

161
SL me
New | ete ee =
appellation | Symbol | Old appellation or symbol !)
Principal P, Px Comb *): 2p —3p; 2p — 4p; 2p — 5p; 2p — 6p; etc.
series
(P-series) | 5S, Pr Principal series.
Sharp | P, Sx 2nd Subordinate series.
series P, Sx | Comb: 3p —1.5s; 3p —2.5s; 3p —3.5s.
(S-series) | Ps Sx | Comb: 4p—2.5s; 4p —3.5s.
| P, Dx “| Ist Subordinate series.
Diffuse P, Dx Comb: 3p — 4d; 3p —5d; 3p — 6d.
series is Fy Dex Comb: 4p —4d; 4p — 3d.
(D-series) | S, Dx Comb: 1.5s —3d; 1.5s — 4d; 15s —5d; 1.5s — 6d.
SS; Dx Comb: 2.5s — 3d.
By Ex Comb: 2pb—4¢p; 2p—5/p; 2p—6rp
Spandamental AS at 2 Comb: 1,5s—6/p.
‘ D, Fx Bergmann series.
series
© eae) D, Fx Comb: 4d—4/p; 4d—5vp.

FEF Comte, = 20025 *
vernier one of which corresponds with a division in mm. ona brass
ruler 1 m. long (to be used along the y-axis), and the other with
a division in 0,1 z (= 4 mm.) on a rectangle also of brass for the
asymptotes. Everything has been executed with the utmost care in the
Factory of Scientific Instruments, P. J. Kipp and Sons, J. W. Gittay
suce. Delft.

On the plate we find a system of axes OXYZ, and the YOZ-
plane is turned over to the left. Here the curves:
Pee yas. y= SZ. and y = Dz
have been drawn.
All the #-curves and F-asymptotes have been indicated by

» ” yg ” ”? y ”» ”? ”? 3? »”? Te
> >”) S > > S 33 ”? bP] 3? 33 fee ee te
” » D » ”? D ” 2 39 By ”

1) Cf. Dunz. l.c.
*) This series was called third subordinate series by Saunpers before. Proc.
Amer. Acad. 40, p. 439, 1904,

162

The four mentioned eurves are all four the same, but each in
another position. For z=1.2.3 the curve y= Pz, yields the values

P., P,, P,, which indicate three P-asymptotes (——w—) in the
YOX-plane. In the same way the S,-asymptote (_._.—_), the D,-
asymtote (__..__..__) and the F,-asymptote (—) is obtained. In

other spectra D,,S, ete. can also appear as asymptotes. We now
find the following curves in the YOX-plane, in which I have now
once more given the meaning in the new and the old nomenclature.

y= S,P, Principal series with S,-asymptote. Principal series.

y= P.S; Sharp ‘ ee a e3 2°4 Subordin. series.
—— Pop: Diffuse a & re os 1st met zs
y = P,P, Principal = mae = » an » »
y = P,F, Fundamental _,, ae 24 c Comb : 2p—mAp.
y— P,S, Sharp a 38 = Comb : 3p—ms.
y= i Ds Diffuse > = Pe =< Comb : 3p—-md.
y= P,S, Sharp ~ sj Slee » . Comb : 4p—ms.
y= P,D, Diffuse 3 eae! 5 2 Comb : 4p—md.
y = D,F, Fundamental ,, Same So Ee Bergmann series.
N
y= F,F, Fundamental ,, mag 2 Comb : zs Ap,

and further the curve y= o0/;, so this is the original curve on its
original system of axes. :

In the above table I have arranged the curves according to their
asymptotes. We can now also easily arrange them in Translation

groups.
w= 1; and y= Pees form together the Translation group P
g= 78,5 J = Passe ae 5 : -s 9

y a Dy = PD: fA E oe eer
aa hes DD, Fie See ee eS es e i

All the curves representing series which belong to one and the same
Translation group, have been indicated in the same way, so:

All the members of the Translation group P by —— —

>» 3) 2) >) > 9) 9) S >) Soe et eSore en omeed
>) >) 3 3 2) 39 > D bed <a ar —F
+P 3) > 9 9 >) o> F >

All the curves indicated in the same way can be made to cover
each other by merely a translation // Y-aais.

If we wish to make a spacial representation of the whole system
of series, we need only think the YOZ-plane rotated back to its
original position, then the different curves will lie in different planes

163

//YOX-plane. All the series with asymptotes P,S,D, then get into
the plane z=1, those with asymptotes P,, D, ete. in the plane
2==2 etc.

By means of this plate we can now easily demonstrate, how the
whole system may be built up, when only some spectral lines are
known.

Let us suppose e.g. that 3 lines of the P series with S, asymptote
S, Pz or Principal series have been observed, then the curve Y= S, P,
ean be drawn in the YO X-plane and the curve Y = P. inthe YOZ
plane. The latter yields for z= 1 the asymptotes P,, P,, P,, which
may be drawn in the YOX-plane. S, and P, being known, the S
series with P, asymptote (P, S, or 2°¢ subordinate series) is given
_ for the greater part (i.e. without the rotation). If one more line is
known of this series, the curve Y= P, S, is perfectly determined,
and so also the curve Y= P,S, and Y=P,S,. If we now draw
the curve Y=, in the YOZplane, the former yields at once the
asymptotes S, , S, ete.

If one line is known of a Diffuse series, e.g. that with P, asymp-
tote (P, D, or 1% subordinate series), then the curve Y= P, D,
may be drawn in its main features (so without rotation), and it is
perfectly determined by a second line. So all the D series are known,
and all the D asymptotes may be found by drawing the curve
Y= D. in the YOZplane. Now all the asymptotes of the Funda-
mental series are known, so they may all be drawn without it being
necessary that one knows one line of it by observation. So the whole
system of series is known through six lines, provided only one com-
ponent be used, as has been expressly stated. We draw attention to
the fact, that this is possible only by the idea of unity, by which
we are guided:

For all the series the curve by which they may be denoted in
the indicated way, is the same-

Besides the easy survey of the whole system of series and the
well-arranged whole, which we owe to this way of considering
the matter, our plate can teach us several things more.

It shows us in what region there are still lines wanting in the
spectrum, and where endeavours to find new lines have a great
chance of success.

Reversely, if new lines have been found from the experiments
in a certain spectral region we can by marking their frequencies
on the Y-axis and by drawing lines // X-axis, determine the points
of intersection of these lines and the traced curves, and see which
of these points of intersection then coincide with the linesz=1.2.3.,

164.

etic. We know then at once to what series they belong, and so what
place they occupy in the whole system. If a meeting as discussed
above should not take place for a line, we should consider that the
line may belong to a series for which no other member has been
found as yet for that element. Then the whole system of asymptotes
(Pail = S,,5,---D,,D,...f,, F,..-) should be’ drawn, after
which the templet should be made to run successively along these
asymptotes, in which way it is easy to find to what asymptote the
considered line belongs. From the X-translation, which the templet
then has, one can derive at once to what translation group the series
belongs. In_ this way our pattern curve can be very serviceable in
detecting and arranging new lines.

I should like to draw attention to another point. When we draw
the systems of series for the different elements (I have, of course,
only been able to select one for the adjoined plate), all kinds of
different types are found. Gradual changes take place when we
proceed from one element to another in the same column of the
table of Menpe.rnrr, and also when we pass on to the other columns,
ihe occurring changes in the type are very great. I bope to publish
the results of a more extensive study on these changes later on.
I will make some remarks ~ about this already here. On the
annexed plate we find e.g. the asymptote S, of the P series lying
above the P, asymptote of the S and D series. We also see that
S, P, is pos. and P, S, neg. for ¢ = 1. The absolute value of the two
ordinates is the same.

We find the same behaviour in the systems for the other alkali-
metals, and also H, He, and O. If we compare this with a diagram
of the Thallium system or some other heavy metal, we observe
exactly the reverse. Now the S, asymptote of the P series lies under
ihe P, and P,’ asymptotes of the two components of the S and D
series. Moreover .S, P, and S, P,’ are now negative and P, S, and
PS, are the same, but positive. I will not enter just now into
other points of difference between the two types. I will only draw
attention to the following points:

As appears from the diagram, the negative frequencies naturally
occur here. So, as we are here almost compelled by the principle
of continuity, to assume negative frequencies, I consider the objections,
entertained by Mocrnporrr *) against formulae with negative frequen-
cies, entirely unfounded.

In the same way the objection that Mocrenporrr*) advances to the

1) Thesis for the doctorate, Amsterdam, p. 39.
?) loc. cit. p. 39.

165

formula of Rirz that the succession of the lines is irregular, is quite
removed by the introduction of the negative frequencies and the
continuity obtained through it.

Further our plate of the Natrium system throws light on the so-
called summational and differential series, discussed by Mocunporrr *).
We find two P-series in the spectrum of Na, viz. P, Pe and S, Pr.
The corresponding terms of the two series show the constant diffe-
rence of frequency S, P,, which also represents the frequency of
the first term of the P series with S, asymptote.

According: to Mocrnporrr *) the series P, Px is now a differential
series of S, Pv and S, P,, or as we may briefly write:

iS Pr—S, Te = vie Px:

Such a relation can also be easily shown between other trans-
lation series e. ¢.

Po Da— Pi Pe PP. De.

Here it are the two D series: P, Dr and P, Dz, of which the
corresponding terms show the constant difference in frequency which
exists between their asymptotes, viz. P, P,, which is also the 24
term of P, Px; according to Moaunporrr the 1** line of the diffe-
rential series. As appears from the plate, however, (the observed
lines are indicated by 0), this line has not yet been observed, though
it (4 7510) lies in a region very well accessible to observation. So
it will probably have a very slight intensity. That this line would
give rise to a whole series of differential vibrations, seems, indeed,
somewhat strange to me. From the asymptotes of one Translation
group we can write all kinds of constant differences of frequency,
for which a line is often to be found then. In this way we can
indicate the members of one Translation group in all kinds of ways
as summational and differential series. So we get simply here
Rirz’s ‘“Kombinationsprinzip”’,. in somewhat modified form, for which
PascHEN *) has already given a scheme for the Potassium spectrum,
according to which scheme Dunz‘*) has calculated the systems of
series for different elements. These systems, however, share the
drawback of Mogrnporrr’s system of being confusing and difficult
to survey, which drawback is entirely removed by the introduction
of the Translation series.

») Summational and differential vibrations in line spectra. Proc. Kon. Akad.
v. Wet. Amsterdam. 25 November 1911 p. 470.

aA. p. 474.

8) Jahrbuch der Radioaktivitat und Elektronik Bd 8 p. 174. 1911.

einen C.D. 39.

166

Chemistry. — “Determinations of the vapour tension of nitrogen
tetrocide’. By Dr. F. E. C. Scnurrer and J. P. Trevs. (Com-
municated by Prof. J. D. Van per Waais).

(Communicated in the meeting of May 25, 1912).

1. In a previous treatise’) we communicated the results of an
inquiry into the vapour tensions of nitrogen tetroxide. In these deter-
minations we made use of a method which had been applied before
by different investigators (LaprnBurG, Ramsay and Youne, BoDENsTEIN,
Jounson and JACKSON) in measurements of vapour tensions of substances
which could not be brought into contact with mercury. Of the forms
of the manometer proposed by the said investigators. we chose that
described by Jackson, because this manometer can be very easily
constructed, and the accuracy which we wanted to reach, can be
easily obtained by means of this apparatus. Moreover by means of
this manometer it seemed possible to us to devise a method to determine
the vapour pressures of substances attacking mercury up to the
critical pressure. As a sequel to the determinations to three atmos-
pheres given in the preceding paper, we shall give a description here
of this method for higher pressure, and state the results which make
the vapour tension line of the nitrogen tetroxide up to the critical
temperature known to us.

2. Critical temperature. Before entering upon the description of
the vapour tension determinations at higher pressure, we will first
mention a determination of the critical temperature, which we did
not carry out with the measurements of the vapour tension, but in
another way independent of these. A thickwalled tube of combustion
glass provided with a capillary constriction was connected by means
of a ground glass junction with the reservoir with nitrogen tetroxide.
Afier the tube had been evacuated by means of the GagpE-pump (with
cooling of the nitrogen tetroxide with a carbonic acid alcohol mixture),
and the connection with the pump had been melted off, the tube
was filled by the liquid being distilled over, so that the liquid took
up a volume that was somewhat smaller than half that of the tube.
Then the latter was melted off at the capillary constriction, and
heated in a bath of paraffin oil.

The liquid, which is almost colourless in the neighbourhood of

1) These Proc. Vol. 14, p. 536.

—

167

the melting-point, and has a yellow brownish colour at the tem-
perature of the room, becomes darker with rise of temperature; at
about 50° it is already dark brown, and the transparency diminishes
gradually with ascending temperature. The vapour which has a
lighter colour at equal temperature on account of its slighter density,
also gets darker with increasing temperature, so that above 100° the
meniscus between liquid and vapour can hardly be distinguished.
Hence the critical phenomenon of this darkbrown liquid and vapour
has not been directly observed. The only value of the critical
temperature recorded in the literature, has, accordingly, not been
determined by an optical, but by another way.

For the determination of the critical temperature NaprsprNe ') made
use of a very ingenious method, which, however, has not yielded
accurate results. A tube was provided with a balance-knife in the
middle so that it could execute regular oscillations round the state
of equilibrium. If now the tube is filled with nitrogen tetroxide,
regular oscillations are impossible, the tube inclines to the side where
the liquid is. With rise of temperature above the critical however,
the tube fills homogeneously, and gets in equilibrium. The tempera-
ture, at which this setting in of the equilibrium takes place, was
considered to be the critical temperature; it amounted to 171,2°C.

We have, however, succeeded in observing the critical phenomenon
directly optically. With incident and transmitted light there is nothing
to be observed of the. critical phenomenon in our tubes of about
3 mm. bore (thickness of the wail 3mm.). Even the use of an are
lamp did not bring a change. When, however, we threw the light
on the tube (in a bath of paraffin oil), and directed our eye so
that the light that was reflected on the inner wall of the tube, could
reach our eye, we could clearly distinguish the demarcation between
liquid and vapour. In one of the tubes we saw the meniscus quickly
shift to one of the extremities on rise of temperature, and disappear
suddenly. In another tube, the volume of which pretty well agreed
with the critical volume of the filling, the line of demarcation dis-
appeared suddenly about in the middle of the tube. Both tubes
yielded 158,2° C. for the temperature at which the demarcation
between liquid and vapour disappeared. We have repeatedly carried
out these determinations independently of each other; the obtained
values agreed within 0,2°. So the critical temperature amounts to
158,2°, and accordingly differs considerably from the value given by
NADEJDINE.

1) Beibl. 9, 721 (1885).

168

3. The vapour tension determinations. The apparatus used by us
for the vapour tension determinations, is represented in fig. 1. The
manometer, which is fused
into the tube A, differs from
the one described in our
previous communication only

E in this that it is more elon-

: 8 gated and smaller; the length”

of the curved part amounts

to three or four em., while

the tube A has an external

A diameter of 10 mm. and a

length of 22 or 23 em. The

entire apparatus serving for

the measurements has a length

of about 28 cm. after the

Fig. 1. constriction at # has been

melted off. On the outer tube A two marks have been made, so that the

end of the needle is just between the two marks when the internal and

external pressure is the same. The manometer can resist an excess of

pressure of one atmosphere, and can therefore be evacuated ; then the

end of the needle reaches the inner wall of A in some of the apparatus

used by us. The sensitivity reached with this shape of apparatus
varies between */,, and '/,, atmosphere.

Before the apparatus was filled the reservoir C with the
nitrogen tetroxide was cooled by means of a mixture of carbonic
acid-alcohol, and evacuated by means of a GaEDE-pump through D.
Then the constriction J was melted off, and a quantity of nitrogen
tetroxide was distilled over through the U-tube with phosphorus-
pentoxide into £4; for this purpose a cilindrical vessel was placed
round the tube 4A by means of a cork, which vessel could be filled
with alcohol cooled by carbonic acid. When a sufficient quantity of
liquid was distilled over, the apparatus was separated from the filling
apparatus by melting off at ZH, after the nitrogen tetroxide in Band
C' had been brought to — 80°.

We have applied two different methods for the determination of
vapour tensions.

a. For our first determinations we made use of the arrangement
indicated in Fig. 2a.°The apparatus AB was slid into a thickwalled
combustion tube, so that it rested on the constriction at C’ with a
copper spiral, which is not drawn in the figure. At the lower end
of the combustion tube a combustion capillary D of 3 mm. bore

169

and with a wall of 3 mm. thickness was fused to the apparatus,
which was cemented into a mounting for CaILLerer experiments.
The upper end of the combustion tube was fused to by means
of an oxygen gas flame. After evacuation with a water-jet pump
the combustion tube was filled with a glycerin-water mixture, and
screwed into a CatLietrr-pressure-cylindre filled with the same
liquid. Then a cilindrical glass jacket was put round the combustion
tube by means of a rubber stopper prepared for high temperatures,
in which jacket different liquids were electrically heated under varying
pressure till they boiled (by means of the heating wire wrapped

round the tube and drawn in fig. 2a). The rubber stopper was
protected against the action of the boiling liquid by a layer of mercury.
The condensation ring of the boiling liquid was always raised to
above the extremity of the combustion tube, the temperature was

170

read on an Anschiitzthermometer (which had been compared with a
normal thermometer) the mercury bulb of which was ata level with
the nitrogen tetroxide.

For the determination of the pressure this was regulated by means
of a CalLLeTeT-pump in such a’ way that the needle was exactly
between the marks on the tube A, and read on a ScuArrer and
BuDENBERG metal manometer gauged by means of a pressure-balance.
The liquids which we have used for heating, were successively
alcohol, toluene, xylol, and aniline; the bumping was prevented by
a stream of air-bubbles, which were sucked in through the tube
that passed through the stopper. :

The results obtained by this method, will be described in § 4.
The experiments arranged in this way always finished up with an
explosion; the highest pressure we reached was 67 atmospheres. .
The critical pressure, however, lying higher, we were obliged to
have recourse to another method for the determination of the higher
vapour-tensions.

b. In our further experiments we abandoned the use of a com-
bustion tube, and replaced it by a copper tube. In this we had first
of all to face the difficulty to arrange it in such a way that the
reading of the position of the manometer needle was possible. For
this purpose near the end of the tube two transverse tubes were
adjusted, which could be closed by means of perforated screws, one
of which (/) has been drawn in fig. 2b. The hole through these
screws was closed with a glass plate, which was pressed to the tube
by the screw. To make this arrangement tight at high pressure was
at first attended with great difficulties. We tried to reach this by
screwing the glass plates to the tube between rings of leather; it
was, however, impossible to get a sufficient closure in this way.

Then we pressed the plates between plaster of Paris, and between
copper, made soft by being made red-hot, always, however, with a
negative result. After these futile attempts we cemented the plates in
loose steel mountings, and screwed these mountings with copper plates
into the tube. As cement we tried first a mixture of soluble glass,
zine oxide, and magnesium oxide; once we succeeded in this way to
obtain a sufficient closure up to 100 atmospheres, generally, however,
the soluble glass showed cracks, which allowed the liquid in the copper
tube to get through on increase of pressure. At last we succeeded
in cementing the glass plates into the steel mounting by means of
an enamel obtained by melting from natrium- and potassium ecar-
bonate, silicium oxide, and lead oxide. By heating with a-Tecluburner
this enamel melted, and entirely filled the narrow opening between

che

171

glass and steel, and continued to close after it had been cooled, up
to a pressure of 150 atmospheres.

Now the apparatus AB was slid into the tube; it rested on the
constriction C’ by means of a loose glass tube that tightly fitted in
the copper tube; the length of this tube was chosen so that the end
of the manometer needle was exactly between the two glass plates
in the holes in the screws, so that it was possible to read the
position with an incandescent lamp placed behind it. The narrow
copper tube D, which formed the connection with the Cam.eret-
pump, was fastened to the lower end of the copper tube by means

_of a screw. Now the tube was quite filled with the glycerin water

solution, and closed at the top with a screw.

So in this way we had obtained an arrangement which could
resist pressures of about 150 atmospheres. It only remained to us
to find a method to heat this copper*tube to varying temperatures.

We have tried to use an oil-bath for the heating, and to place
the tube in the bath in such a way that the end in which the glass
plates were, projected above the bath. This was required for the
accurate reading of the needle, and to have at the same time an
opportunity to clean the glass panes when in course of time the
screws began to leak a little in consequence of the increase of tem-
perature. This method of heating, however, appeared to give un-
reliable results in spite of different modifications. It appeared that
the part that projected above the liquid caused a loss of heat,
so that the temperature of the nitrogen tetroxide remained lower
than the temperature in the oil-bath, so that at a definite tempera-
ture always too low pressures were found compared with the
results according to the method a.

At last we were more successful with another quite different
method of heating. The copper tube was quite surrounded by
two tightly fitting spirals of hard lead. Through both these
spirals an oil-stream was passed, so that the two streams ran in
opposite directions; one stream flowed spirally round the tube from
below upwards, the other in the opposite direction. The oil-stream
was obtained by means of a rotating pump worked by an electro-
motor, which pressed the cil from a pan heated by two Tecluburners
through the spirals. The tube and the heating-spirals surrounding it
were first enveloped witn thick asbestos cord, and then with a
thick layer of cotton waste to prevent emission of heat as much as
possible; the inlet and exit tubes were isolated in the same way.

The temperature was read on an Anschiitz thermometer, which
was placed between the spirals and the tube and of whieh the part

Proceedings Royal Acad. Amsterdam. Vol. XY.

172

of the seale that was to be read, was placed behind an opening in
the isolation material. Besides this thermometer opening only two
small apertures were made in the isolation layer, through which
the two small panes remained visible.

4. Results. The results obtained by the methods described in the
preceding paragraph, have been collected in Table I. They have
been made with five apparatus; the determinations in the neighbour-
hood of the critical temperature have been carried out with an
apparatus which was about half filled with liquid at the ordinary
temperature, and the volume of which was therefore somewhat
smaller than the critical volume. From our determinations at the
femperatures in the immediate neighbourhood of 7, we have deter-
mined the critical pressure graphically. The extrapolation that is
required for it, can» certainly be executed within the error of one
atmosphere. Yet we think that we must consider the critical pressure
accurate up to two atmospheres. We have namely no perfect certainty
that the observations at the highest temperatures refer to the hetero-
geneous equilibrium. The possibility cannot be entirely excluded that
these observations represent a line in the homogeneous liquid region,
though these determinations yield a practically continuously progressing
curve with those at lower temperatures ; if this should be the case,
the deviation from the real vapour-tension curve is so shght, that
the accurate value of the critial pressure could only be found by
means of an extrapolation formula, drawn up from observations at
lower temperature. In this, however, we also meet with difficulties,
as then the extrapolation would have to take place over a greater
range of temperature; we return to this extrapolation in a following
paragraph. So we find 100 atmospheres for the critical pressure, in
which we must consider a maximum deviation of two atmospheres
possible. It will, moreover, be difficult to reach a greater accuracy,
as it will not be possible to observe the critical pressure at the
same time with the measurement of the pressure without complicating
the arrangement considerably. Besides this would give rise to new
experimental difficulties, because the critical phenomenon in itself
is so very difticult to observe. A manometer which was filled for
about two thirds with liquid, presented a sudden deviation from
the vapour tension line at about 140°; the pressure rose abnormally
rapidly (about 6 atm. per degree) with slight rise of temperature,
much more rapidly than the vapour tension line, even in the neigh-
bourhood of the critical circumstances. So this apparatus is quite
filled with liquid at 140°, and the abnormal rise of pressure. was

TABLE |.

t p Method foes lee pf Method
54.25 | 4.1 | a (alcohol) 109.8 | Setar sheets aeatoN)
59.6 4.95 | a (alcohol) 110.2 26.8 b
64.95 | 6.1 a (alcohol) 110.3 |. 27.0 a (xyiol
10.1 1.3 a (alcohol) | 110.8 | 27.2 b
72.7 8.0 | b Peeps a=} -- 40.8 a (xylol)
14.7 S:1..|°. *@ (aicohiol)+*.| .- 115.5 31.3 a (xylol)
78.3 9.7 a (alcohol) 115.7 | 31.6 a (xylol)
78.3 9.6 b He a 35.3 a (xylol)
er | 10.1 | b 120.0 | 35.7 b
81.7 10.8 a (toluene) 120.5 | 36.3 a (xylal)
82.7 11.1 b PE 1e5 | ate a (xylol)
86.7 12.9 b 15.5 | 41.8 a (xylol)
87.1 13.0 b iis" | > 48.8 a (xylol)
88.5 13.6 | a (toluene) | 131.5 | 49.3 b
92.3 15.3 | b 134.9 | 54.4 a (xylol)
ae. | 16,1 | a (toluene) | 139.1 | 60.5 a (aniline)
98.15 18.6 a (toluene) 142.6 | 66.6 a (aniline)
100.7 20.3 a (xylol) 42.9 | 66.4 | b
eet ons' | a (xylol) re | ena | b
101.45 | 20.5 b ie. 4 fs 8 | b
101.6 20.7 a (toluene) 156.27 _.| 93.6 | b
104.5 | 22.6 a (toluene) | 157.4 | 97.2 | b
105.6 | 23.3 a (xylol) | 7, 158.2 | P.100 | extrapolation
105.9 | 23.7 a (xylol) | | |

| | |

therefore owing to the heating of the homogeneous liquid at constant
volume. .

With every determination in Table [ the method used for the
observation is given; the pressures are given in atmospheres. In the
first four determinations and in the sixth the pressure was not
determined by means of a ScHirrer and BupENBERG manometer, but
with an air-manometer (air-isotherm of AMAGAT).

12*

174

It will be clear from the table and the corresponding graphical
representation (fig. 3) that there is sufficient harmony between the
results obtained by the two methods of observation.

Aw Pee = = =
— - - ed

60 80 100 120 140 160 7
Fig. 3.

So
ine)
=)
>
—)

By way of control of the pressure measurements we have exposed
one of our manometer tubes, after being opened, in the copper tube
to the same pressures and temperatures as occurred in our deter-
minations. Then it appeared that in none of the observations a
correction was required for a change of the zero position.

5. As for the nitrogen tetroxide we have to do with a substance
which is in dissociation, for which the values of the degree of the
dissociation appreciably vary both in the liquid state and in the
vapour state corresponding with it — for the vapour we already
gave some values for the degree of dissociation in our preceding
communication —- it seemed desirable to calculate the value of 7 from
VAN DER WaAALs’s empirical equation with the aid of our observations.
If for this purpose in the equation:

175

-we substitute the values p,—= 100 and 7). = 158.2 + 273 — 431.2,
our observations yield values of / varying with the temperature, as
will be clear from the subjoined table II.

TABLE IL
1.0 enriy. f Uei Wt 4.2% 100.5 | 373.5 20 4.5
21.2 294.2 1 4.3 123.8 sons: | 40. | 46
]
166 319.6 3 4.35 138.8 | 411.8 | 60 [4.7]
79.4 352.4 10 4.5 150.0 | 423.0 | 80 [5.0]

The value of / appears really to reveal the dissociation; it lies,
namely, much higher than that of normal substances (+ 3), even
higher than that of substances as water and alcohol. It appears at
the same time that 7 rises with the temperature, whereas the reverse
takes place for water and alcohol.

So the inclination of the /—/7-line increases more rapidly with
rising temperature than for a normal substance.

In the graphical representation, which occurs in the Theoretische

Chemie of Prof. Nernst’), in which —- log £- is taken as ordinate,
Pk

oa as abscissa, nitrogen tetroxide yields therefore a line, which

in opposition to that of water and alcohol is concave seem from

below, and yields a branch of the fanlike sheaf of lines, which lies

still higher than all those indicated in the graphical representation.

We have put the last two values for / in table II between paren-
theses, as these change resp. 0.1 and 0.2 by a change of one
atmosphere in the value of P;, and are therefore distinctly inferior
to the preceding ones in accuracy.

6. As appears from the change of colour of liquid and vapour
with rising temperature the increase of the degree of dissociation
is accompanied by an increase of darkening of the colour according
to table IV of our former communication. Hence the supposition
naturally suggests itself, that the brown colour is owing to the split
molecules, whereas the unsplit molecules are colourless. This suppo-
sition has been confirmed by the investigation of Sater’), who has

1) p. 237 (1909).
2) (. r. 67. 488 (1868).

176

succeeded in getting quantilative data about the homogeneous equi-
librium by a colorimetric method, which data accord well with the
determinations from the vapour densities. As the colour of the liquid
and the vapour gets darker and darker towards the critical temperature,
the degree of dissociation will probably be great at 7.

In order to get a criterion about the degree of the dissociation
we have calculated the values of a and 6 from the equation of
state (as the result of a discussion of one of us with prof. VAN DER
Waats). By substitution of 7; = 4381.2 and Pe =100, we find:

7 Te
is Eee) = 0,0105 and
64.273? Pr
Ty
Lt ees 0,00197.
8.273 Py

Jf to get an approximative estimation we now consider the 5 as
an additive quantity, we can calculate the theoretical 6 for NO,
resp. V,Q, from the tables of the 4-values, and compare them with
the values found above.

From the values for nitrogen and oxygen we find in this way
for NO, and N,O, resp. 0,00226 and 0,00452. .

Calculation with the aid of the data about nitrogen oxide and
oxygen, resp. nitrogen mon-oxide and oxygen, yields for NO, and
N,O, 9,00186 and 0,00372, resp. 0;00200 and 0,00400.

So we draw the conclusion from these values, that the fluid phase
for the critical circumstances consists for by far the greater part of
split molecules.

7. The complex behaviour of the nitrogen tetroxide leads us to
expect an intricate equation for the P7-line. Calorie data, which
can be of use to us to find the vapour tension equation, are not
sufficiently known. For this we must of course know the heat of
evaporation and the specific heats along the border-line. The specific
heats which are known, refer to unsaturate vapours as far as the
vapour state is concerned. Accordingly they would have to be corrected
in accordance with the change of the degree of dissociation with the
pressure. The heat of dissociation in the homogeneous vapour is
known pretty accurately, and so this correction might be applied
at those temperatures for which the degree of dissociation in the
saturate vapour is known (see preceding communication Table IV).
The specific heat of the liquid is almost quite unknown. So even if
the heat of evaporation at one temperature were known with sufficient
accuracy, the unknown dependence of the specific heats on the

177

temperature would yet render the drawing up of a formula by the
aid of the caloric data impossible.

We will only calculate the value of the heat of evaporation from
our vapour-tension determinations by the aid of the equation of
Ciapryron, which can only be applied for low pressures, because
the specific volumes along the border line are unknown at higher
pressure. From the equation:

,aP Q
G0 Fae
we find, neglecting V; with respect to V,,; and applying the law
of Boyir-Gay-Lussac :
Ey eke,
in which 2 represents the degree of dissociation
of + 2) RT? GP

Q PF. dT

In order to calculate a have represented our determinations

at low pressure by an empirical formula. By the aid of the data:

t= — 23, p=10m.M.;t=11,0, p=463m.M; t= 48.7, p = 2478 m M.

from our former communication we derive the values a= 1325.6,

b = 3.354 , c = — 0.8950 for the constants a, 4, and c in the equation:
logp = —- i + hblogT +c

This equation represents our observations of the preceding com-
munication very well. It may be remarked here in passing that this
expression can represent the observations at higher pressure even up
to about 120° and 36 atmospheres. At higher pressures the curve
calculated from the equation deviates slightly towards lower pressure ;
in the immediate neighbourhood of 7), the deviations become greater ;
still even at 7). the deviation amounts only to about three atmospheres.
It is remarkable that this formula drawn up from observations below
3 atmospheres, is able to represent the vapour-tension line of this
complicated substance so accurately.

If we now differentiate the obtained expression we find:

iS RR, es CRY panei
nae = eT? T
which yields after substitution :
1325.6
ae 0.4343

(1 + #) R + 3.354 (1 + 2) RT.

: 178
If in this expression we substitute the values R= A985: i Bi
and «= 0.15, which two last refer to the boiling point, we find for
the heat of evaporation at the boiling-point:
9200 calories.

The experimental determinations of BrrtHEeLoT and Ocrsr *) appre-
eiably differ from this value. From a number of values which differ
pretty considerably from each other, which, however, all of them
lie lower than the above mentioned one, they consider 8600 calories
the most probable. We, however, think that we have to prefer our
calculation, the more so as the determinations which have served
for our calculation, just lie in the temperature region over which
Ramsay and Youne’s investigation extended, and the determinations
of the latter do not practically differ from ours.

In conclusion we wish to avail ourselves of this opportunity to
express our thanks to Prof. Smrrs for his advice in the experimental
difficulties experienced by us, and for the interest shown by him in
our work.

Anorg. Chem. Laboratory of the
University of Amsterdam.

Physics. — ‘Electric double refraction in some art:ficial clouds and
vapours.” (Third part). By Prof. P. Zeeman and C. M. Hooernpoom.

18. The results obtained with the sal-ammoniac fog might be
explained by postulating the existence of two varieties of sal-ammoniac
erystals. This hypothesis was put forward in § 17. In the textbooks
on crystallography, which were at the disposition of the authors,
nothing however, relating to dimorphism of sal-ammoniac could be
found. This seemed rather unfavourable to the proposed explanation.
We are much indebted therefore to Dr. F. E. C. Scuerrer, who
gave us some references to the chemical-crystallographical literature,
from which it appears that the dimorphism of sal-ammoniac is a
well-known fact (see v. Grots, Chemische Kristallographie. Band I.
S. 167. 1906). ‘tte

Stas *) while sublimating NH,Cl had observed a phenomenon closely
resembling the transformation of polymorphous substances; he did
not try however an explanation and it seems that he did not think
of dimorphism.

1) Ann. de Ch. et de Ph. (5) 30 398 (1883).
*) Sas. Untersuchungen tiber die chemischen Proportionen u.s.w. deutsch von
Aronstein. S. 54, Leipzig 1867.

sips

LrHMaNn') was the first to suggest that the ammonium salts are
dimorphous and he tried to prove it by experiments on crystallization
of solutions, containing simultaneously two or three of the three
halogenous ammonium salts. His result was: “dass hier ein sehr
eigenthtimlicher Fall von Dimorphie vorliegt, insofern anzunehmen
ist, dass alle drei Kérper in je zwei Modificationen krystallisiren, und
zwar beide regulir, beide in Wiirfeln, nur insofern unterschieden,
als die der niedrigeren Temperatur entsprechende Modification in
salmiakahnlichen Skeletten, die der héheren entsprechende in scharf-
kantigen vollkommenen Krystallen auftritt.”

For our purpose it was of particular interest to know whether
the two modifications of sal-ammoniac appear also after sublimation.
As will be proved below (see § 19) all the phenomena which we
described (§ 14, 15, 16) can be obtained with sublimated sal-ammoniac
also; the transition of one modification to the other one might then
be accompanied with a change of the sign of the electric double
refraction.

In this connection an investigation of GossNER*) merits our atten-
tion. Gossnrrk among other things. repeats an experiment of Stas
and we may be permitted to give here his description :

“Im Gegensatze zu Lesmann halt Retcers*) die Dimorphie der
Ammoniumhalogenide nicht fiir bewiesen. Sras’s Beobachtungen ent-
sprechen zwar ganz den Vorgéngen, die bei polymorphen Umwand-
lungen zu beobachten sind, doch erklart Stas selbst die Erscheinung
nicht durch Dimorphie. Nachdem mancherlei Krystallisationsversuche
zur Entscheidung der Frage ob der Salmiak dimorph ware ohne
Resultat verliefen, wurde der Versuch von Stas in ahnlicherweise
wiederholt. In ein 2.8 ¢e.M. weites Glasrohr von 70 ¢c.M. Lange
das am einem Ende verschlossen war, wurde ein ca. 15 cM. lange
Schicht Salmiak gebracht, der durch Sublimiren vollstandig getrocknet
und gereinigt war. Die Schicht war nach dem offenen Ende zu mit
Glaswolle abgeschlossen, da die Beobachtung ergeben hatte, dass beim
Sublimiren im Vacuum feste Salmiakteilchen mitgerissen wurden.
Das vordere offene Ende wurde in eine enge Rohre ausgezogen, mit
der Saugpnmpe in Verbinding gesetzt. Der leere Theil der Réhre wurde
dann unter fortwahrendem Saugen circa zwei Stunden lang sehwach
erhitzt um alle Salmiak Keime daraus zu vertreiben. Als sodann bei

1) Zeitschr. f. Krystallographie 10. 321. 1885.
2) GossveR, Zeitschr. fiir Krystallographie u. Mineralogie herausgegeben von
GrotH. 38. 128. 1903.

3) Arzruni, Die Beziehung zwischen Krystallform u.s. w.; in GRAHAM-OTTO’S
Lehrbuch der Chemie 1898. 1 (3). 321. 3 Aufl.

180

einem Drucke von 15 mm. die Salmiakschicht langsam erwarmt wurde,
sublimirte NH, Cl in den leeren Raum und setzte sich in winzigen
lebhaft glainzenden Krystallchen, die allmahlich zu einem dicken
Ringe sich vermehrten, an den Glaswanden ab. Die Krystallchen
erwiesen sich im parallelen polarisirten Lichte als einfachbrechend.
Doch war eine genauere Beobachtung tiber Krystallform und Aus-
bildung nicht mdglich. Bei Unterbrechung des Versuches begann
plitztich der Ring vom kalteren Ende aus sich zu triiben und
undurehsichtig zu werden. Die Grenze zwischen der triiben und der
sehr lebhaft glanzenden urspriinglichen Partie schritt langsam auf
Kosten der letzteren weiter und war dabei scharf zu verfolgen,
genau wie bei der Umwandlung eines charakteristisch dimorphen
K6rpers. Dabei entstanden zahlreiche Risse in der ganzen Masse.
Der Vorgang war mit einer bedeutenden Volumenanderung. ver-
bunden, was sich durch ein lebhaftes Knistern dusserte, abnlich wie
wenn ein ziemlich starkwandiges Glasrohr zerspringt. Leider war es
nicht méglich Krystallchen langere Zeit zu erhalten. Meist traten die
eben beschriebenen umwandlungsartigen Erscheinungen schon wahrend
des Versuches ein. Immer aber trat die Umwandlung wahrend des
Abkiihlens ein. Es war deswegen eine physikalische und krystallo-
graphische Untersuchung des ersten Sublimationsproductes nicht még-
lich. Doch besteht zwischen den typischen Umwandlungserscheinungen
und den bei diesen Versuchen beobachteten Erscheinungen, wie schon
erwabnt eine vollkommene Aehnlichkeit. Es ist daher der Schluss
sehr wahrscheinlich gemacht, dass wir es hier mit einer polymorphen
Umwandlung zu thun haben und dass das Chlorammonium in zwei
Modificationen existirt.”

We have verified these results. It appeared, however, that it was
unnecessary to produce a vacnum.

After having observed once the transition, experimenting according
to Stas’ precepts, we had no difficulty in obtaining the phenomenon
at atmospheric pressure also. We made use of a tube of 2 em. width
and of 30 cm. length; the tube being closed at one end and charged
with some sal-ammoniac purified by previous sublimation. It is to be
recommended to give a preliminary heating to the place where the sal-
ammoniac is to be solidified again, in order to decrease the velocity
of transition. This procedure also applies to the evacuated tube.

19. Our observations on electric double refraction were conti-
nued with the same optical arrangement, described above, but with
sal-ammoniac fogs prepared by two methods, differing from the ones
used above.

181

a. A current of air was passed successively through bottles with
a NH, solution and with a HCI solution. The tubes did not reach
below the surfaces of the solutions.

The fog, originating in the HCl bottle, was introduced into the
basin with the exterior condenser plates (see § 10). It was rather
difficult to regulate the density, so that the field of view was obscured
nearly immediately. The fog was partly precipitated after the inter-
ception of the air current and the dark band (§ 3) became visible;
the establishment of the field (+ 9000 volts) made the band jump
upwards.

In this case we were unable to observe a downward motion of
the band.

In the present experiment the rotation of the plane of polarization
(see $11), i.e. the dichroism was very small, so that it was difficult
at first to determine the sign of the rotation. It proved to be, how-
ever, the same as the one formerly observed.

In other experiments with the same kind of fog larger rotations
were observed.

6b. Dried air was passed over heated, previously sublimated sal-
ammoniac and then introduced into the basin with exterior con-
denser plates.

The air current and the heating of the sal-ammoniac being well
regulated the throwing on of the electric field caused a downward
displacement of the band, accompanied witb a rotation of the plane
of polarization. After stoppage of the air current, the band after a
while exhibited the upward displacement. In some experiments the
downward displacement could not be observed, and only a rotation
was seen. This especially happened, if the density of the fog was
initially very great so that the field of view became dark. After
partial precipitation of the fog the throwing on of the field caused
an upward displacement of the dark band.

20. The results now obtained and those recorded in the former
‘parts of this paper clearly point to the existence of two modifica-
tions of sal-ammoniac, the one which is originated first exhibiting
a positive, the second modification a negative electric double refraction.

That we may speak of a “direction” of change of the sal-ammo-
niac modifications is shown by the fact that the positive double
refraction is always observed in the first place, and only afterwards
the negative refraction; we never observed with a given fog first
an upward and then a downward motion of the band.

182

In some cases the phenomena were only incompletely visible, but
this can be always explained.

The downward motion of the band sometimes happened to be
absent. This is the case if the air current is very slow. The tran-
sition of one modification to the other has already taken place before
‘the introduction of the fog into the condenser.

The upward motion of the band will be imperceptible, if before
the entire transition of the fog, the precipitation has been such that
the effect becomes too small to be observable.

21. We have tested also a hypothesis, communicated privately
to us by a friend, and which would afford a possibility of explaining
the observed phenomena, discarding the assumption of two sal-
ammoniac modifications.

The orientation of a crystal depends upon the surrounding medium
and may change with it.

Would it not be possible that in the case of positive double
refraction the gas surrounding the particles is different from that
present in the case of negative double refraction? For instance hy-
drochloric acid or ammonia gas in the first case, in the second
air with traces only of the mentioned gases. If then the dielectric
constant of the environment is not much different from that of the
particles, a new orientation might ensue, which would expiain the
phenomena.

Indeed all the preparations which. we used allow of an initial
excess of either NH, or HCl; in the experiment with sublimation
(§ 19) an excess of one of the constituents might be due to the
difference of the velocities of diffusion of the two gases. But in
this last experiment air must be abundantly present. In order to
look for a possible influence of the surrounding medium, the experi-
ment of § 19 was arranged somewhat differently. A current of air
was passed over a solution of NH,, the gases then were dried, and
afterwards introduced into the tube, which contained the hot sal-
ammoniac and lastly into the space with the condenser plates.

The excess of NH, in the gas delivered from the apparatus was easily
shown. The phenomena were the same as those described in § 190).

A similar experiment was tried with HCl in excess. The phenomena
remained the same. It is preferable to use instead of air passing over
a solution of HCl, a current of pure hydrochloric acid, obtained by
dropping sulphuric acid into hydrochloric acid.

22. We have also established the fact that NH, or HCl gas in the

183

sublimation tube ($ 18) does not prevent the transition of one modifi-
cation of sal-ammoniac to the other one.

23. From the experiments of §§ 2l and 22 we may conclude,
that the observed change of sign of the electric double refraction
cannot be explained by a change of orientation of the particles
constituting the fog.

24. It seemed interesting to investigate the behaviour of a fog
obtained by blowing finely powdered, not very recently sublimated
sal-ammoniac into the observation tube, the analogon of the experiment
described in § 8 with glass and different tartaric acid salts. The
displacement of the dark band ought to be now upward. We could
confirm this expectation.

25. Recently Prof. Voter has been occupied with Lancevin’s theory.
He kindly communicated to us a result, which admits of experimental
verification *). From the orientation hypothesis Vorer deduces, that
an absorbing substance must change its power of absorption for
natural light.

We have songht for an action of this kind using the sal-ammoniac
cloud and we think we have discovered it. The nicols and the glass
bar of our arrangement were removed. Between the lamp and the
lens one cr more plates of ground glass were introduced in order
to diminish the superfluous intensity of the souree of light. A dense
sal-ammoniae fog was blown through the observation tube, the field
of view becoming of a red hue. Initially the establishing of the field
gave no change; after interruption of the air current it caused a
brightening of the field of view, later this became darker under the
influence of the electric forces.

The first brightening apparently is due to the precipatation of
particles on the condenser plates; if the field is made zero again
nothing happens. During the later phase very probably an electro-
optic effect is observed. The field of view changes from pale yellow,
to more red hues. This effect could be observed again and again when
the field was put on and off.

26. In the last part of our investigation we will investigate whether

1) Since the above was written Voret’s paper, Ueber elektrische und magnetische
Doppelbrechung. I. was published in Géttinger Nachrichten 1912.

i84

it is possible to determine by the electro-optic method a transition
temperature of the two modifications of the sal-ammoniac fogs, which
we have discovered. Other examples will be tried also.

(To be continued).

Chemistry. — “On critical end-points in ternary systems. Il. By
Prof. A. Smits. (Communicated by Prof. A. F. Honiemany).

In two previous communications I already discussed some parti-
cularities which may occur in ternary systems obtained by the
addition to a system of the type ether-anthraquinone of a third
substance which presents critical end-points neither with anthraquinone,
nor with ether’). An example of this was naphtaline-ether-anthra-
quinone, which was examined by Dr. Apa Privs’). p

Though some more cases were afterwards theoretically examined
by me, the publication was postponed not to anticipate too much
on the experimental investigation, which was greatly delayed by
want of time.

Now however just recently we have met with the very welcome
circumstance that the petrographer-mineralogist Nieeii not only has
seen that the phenomena which are found for the said systems, are
of fundamental significance for petrography and particularly for the
chemistry of the magna, but that moreover he has had the courage
to enter upon an investigation of this territory, which is so compar-
atively difficult to explore *).

In virtue of this it seemed desirable to publish our results already
now, the more so as I may cherish the hope fo facilitate the experi-
mental study of others somewhat in this way.

Having discussed one of the possible types pretty fully in my last
communication on this subject, a more general discussion of the
classification of the different cases which might be distinguished for
ternary systems with critical end-points may suffice here.

1 Case. In the first place I will mention the ease that critical
end-points occur for only one of the three binary systems; this case
was discussed by me before, and tested by an example by Dr. Apa Prins.

If we call the components A, 6, and C; and if critical end-points
occur only in the system A—C, we know that the ternary system

1) These Proc. 25 Sept. 1909. 182.
; » 24 Sept. 1910. 342.
*) These Proc, 24 Sept. 1910. 353.
5) Zeitschr. f. Anorg. chem. '75. (1912).

185

will possess a critical end-point
curve pg, Which projected on the
concentration triangle can have a
shape as indicated in fig. 1 by
the curve pg, the temperature of
which rises in the direction indi-
eated by the arrows.

If in the same triangle we draw
the projection of the eutectic vapour
and liquid lines, along which the
temperature also rises in the direc-
tion indicated by the arrows, we
‘see that in the case considered here none of the eutectic lines comes
into contact with the critical end-point curve pq.

24 Case. In the second place we shall suppose that in two of
the binary systems critical end-
points occur, but in such a way
that in the symbol for the critical
end-point S-+-(G=I), the solid
phase S is the same in the two
binary systems. Let the component
C’ be here this solid phase, then
we get the following simple pro-
jection on the supposition that the
system AZ does not possess either
a minimum or a maximum critical
temperature.

Let us consider the case that 6 possesses a much higher critical
temperature than A, then the temperature of the critical end-point
p’ will probably be higher than that of p, and hence the temperature
will continually rise from p to p’. In this case the temperature along
the g-line may rise from q’ to q, but the reverse is also very well
possible; the former has been assumed in the figure. If the system
AB had a minimum critical temperature, the critical end-point lines
might get a greater distance, and in the case of a maximum critical
temperature depressions can occur which may even give rise to a
closed portion, so that a region is formed where no critical end-points
occur any more.

34 case. The phenomena become much more interesting when the
eritical end-point curve comes in contact with a eutectic line. This
case may be found when in two of the three binary systems critical
end-points occur, but so that the solid substance S in the symbol

Fig. 2.

186

of the critical end-point S-++ (G=L) is different in the two binary
systems.

So we suppose now that in the two binary systems AB and AC
critical end-points occur, in such a way that the critical phenomenon
appears by the side of solid B in the system AJ, and by the side
of solid C in the system AC. A meeting of a eutectic line with a
critical end-point curve of course means this that the critical pheno-
menon occurs at the temperature of the meeting by the side of
two solid substances, and so it is clear that-a eutectic line must
always meet two critical end-point curves sunultaneously, namely the
critical end-point curves which belong to the solid substances to
which the eutectic line refers.

Let us now assume for the sake of simplicity that the melting-
point figure of the system LC’ possesses a eutectec point. We can
then state at once that by the side of the conglomerate of solid
B+ solid C critical phenomena can appear only when the eutectic
temperature of the system LC lies above the critical temperature of
the component A, and the greater this difference is the greater will
be the chance that the case in question can be realized.

V4 To get a better insight into the
peculiarities of such a system it
is necessary to make use of a
ternary V, X-figure, as was used
V by me before.

This ), X-figure is pretty simple
so that it is possible to give at
once the projection of the principal

£ limes of equilibrium on the V, X-
Z plane of the binary system B—C.

Below the eutectic temperature
the V,X-figure of the system B,C
C consists of two lines ace and bc,
which indicate the mol. volumes
and the concentrations of the
vapours, which can coexist with solid B resp. solid C.

Now it is of importance to show what equilibria would appear
when as we proceed aiong the isotherm ac resp. bc the deposition
of solid C' resp. of solid B did not take place.

This case I examined before in the p, z-section for another purpose,
and the sections discussed then quite agreed with the V, X-fig. of
the system 5, C drawn above’).

1) These Proc. 30 Dec. 1905. 568.

Fig. 3.

187

If on compression the deposition of solid C failed to appear in
the vapour coexisting with solid 4, the solubility-isotherm acg,/,
shows that in this case a metastable three-phase equilibrium between
vapour, liquid, and solid B might occur, the coexisting phases of
which are indicated by the points g,, /,, and d.

The figure also shows that if the vapour that coexists with solid
C could be compressed without solid B being formed, a metastable
three-phase equilibrium between vapour, liquid, and solid ¢ might
appear, indicated by the points g,, /,, and e.

If we now think the third component A added, and placed in
the third angle of the base of the trilateral prism, and if we assume
that the chosen temperature lies above that of the first critical end-
points in the systems ABS and AC, it is possible that the stable
ternary JV, X-figure simply consists of two isothermal solubility
surfaces which intersect along a line which originates in the point c.
Along this ternary solubility isotherm solid B-+ solid C+ vapour
coexist. Now it is clear that a two-sheet liquid-vapour surface extends
within the said solubility surfaces, which begins on the binodal vapour
and liquid line in the plane for BC. The two sheets of this liquid-
vapour-surface will continuously merge into each other in space,
and this continuous transition takes place on the critical isotherm,
the projection of which on the BC-plane is indicated by the line £,.

When the said liquid-vapour-surface lies entirely inside the two
isothermal solubility surfaces, no critical phenomena can occur in
stable condition, and in this case no particularities occur. Now we

know that at temperatures lower than those assumed here stable

hquid equilibria must occur, and this must also happen when we
raise the temperature, and in this way approach the eutectic tempe-
rature of the system B—C. With decrease of temperature we shall
see liquid appear as stable phase, because then the liquid-vapour-
surface extends more quickly in space than the solubility surfaces.
The consequence of this is that at a certain temperature the three-
phase solubility isotherm for Sg +Sc-+ G just touches the liquid-
vapour-surface. So at this moment Sg + Sc +L-+G must be able
to coexist for the first time, from which follows that this contact
must take place in a point of the critical isotherm of tbe liquid-
vapour surface so that liquid and vapour are identical there, and a
critical phenomenon makes its appearance.

In connection with this the following things may be remarked.
Starting from the pairs of points g,,/, and g,,/, two continuous
curves pass over the liquid-vapour-surface, the former of which
indicates the vapours and liquids coexisting with solid 5, and the

Proceedings Royal Acad. Amsterdam, Vol. XY.

188

latter of which contains the vapours and liquids which can be in
equilibrium with solid C.

If the liquid-vapour-surface touches the solubility isotherm of
Sp +Sc, it is clear that also the lines starting from the nodes g,, /,
and g,/, must touch, which accordingly takes place on the critical
isotherm. ;

If we now think the temperature still a little lower, the just
mentioned contact will change into an intersection, and so two points
of intersection will occur, one of which indicates the vapour phase,
and the other the liquid phase of the four phase equilibrium
Sg +Sc+L+G.

The intersection of these lines, which are indicated in projection
by 929, P: 4,4, and 9,9, p2/,/,, means of course that the liquid-
vapour surface intersects the solubility surfaces, in consequence of
which the liquid-vapour equilibria get partly into the stable region.
These stable liquid-vapour equilibria lie within the two intersecting
lines g,p, 1, and g,p, /,. The first intersection line, which refers to
the liquid and vapour phases which coexist with solid 6, possesses
a critical end-point in p,, and the second intersection line, which
indicates the liquid and vapour phases which can be in equilibrium
with solid C, possesses a critical end-point in p,. The points g, and
1, denote, as was already said, the vapour and liquid coexisting
with Sg-+Sc, and so it is evident that through these two points
the line must pass which has its origin in C’, and indicates
the coexistence of a fluid phase with a conglomerate of Sg
and Sy . :

If we lower the temperature still more, the points g, and /,, and
also p, and p, move more and more apart, whereas on rise of tem-
perature they draw nearer and nearer together, and coincide in the
double critical end-point, for which the symbol is Sg-+ So + (L=G). .
At temperatures above this double critical end-point there will exist
only fluid phases or coexistence between fluid phases with solid 5
resp. with solid C, or with the two solid substances at the same
time. It is, however, clear that as was already observed, liquid will
have to appear again in the ternary system before the eutectic tem-
perature of the system L—C' is reached, and so we see that when at
lower temperature a double critical end-point has appeared, a second
double critical end-point will occur at higher temperature, so that then
at rise of temperature a repetition will take place of what has happened
at lower temperature, but in the reversed order. So after the second
double critical end-point has appeared, the stable part of the liquid-
vapour-surface will continually increase in extent. To this is added

189

another particularity in the system
bB—C' at the temperature of the
eutectic point, viz. that the vapour-
points cg,g, and g, coincide just
and /,.
Now that this projection has

as the liquid points Z,, Z,
been briefly discussed, it is very
easy to project the indicated spacial
lines on the concentration triangle,
as has been done in fig. 4.

We see from this figure that

Fig. 4. the two continuous vapour-liquid
lines of the two three-phase equilibria S3 +-L+G and Ss + L+G,
indicated by the letters g,9,p,/, resp. 9.9, P./, intersect in two
points g, and /,, where four-phase equilibrium prevails, and where
accordingly also the fluid line of the three-phase equilibrium Sg —--Soe-+-F
runs, which is denoted by the symbols cg, /,. It is further note-
worthy that the liquid branches of the three-phase equilibria
Ss+L+G and Sc +L+G are cut by the critical isotherm £4,,
so that p, and p, are two critical end-points.

If we start from a temperature lying a little above that of the
first critical end-points in the systems B—A and C—A, we know
that on rise of temperature not only the critical end-points p, and
P2 but also the vapour point g, and the liquid point /, of the four
phase equilibrium Sg + Se +1L+G will approach each other till
they coincide in the double critical end-point. As g, is a point of
the ternary eutectic vapour-line and /, a point of the ternary eutectic
liquid-line it follows from what precedes that these two ternary eutectic
lines will have to pass continuously into each other in the double critical
end-point. In the first double critical end-point ? the continuous
eutectic line possesses in conse-
quence a temperature manmum.
At higher temperature the second
double critical end-point Q occurs,
and from this temperature the liquid
and vapour points of the second
continuous part of the eutectic line
recede more and more from each
other, so that the second double
critical end-point is at the same
time the temperature minimum
of the second continuous part of Fig. 9.

2D
a

190

the eutectic line. If we represent this in a diagram, i.e. if we
draw the projection of the pq-lines and that of the eutectic lines in
the concentration triangle, we get fig. 5, in which the arrows again
indicate the direction in which the temperature rises.

It is clear, that it is also possible that the two continous p q-lines
do not intersect. In this case there are no double critical énd-points,
and so the eutectic lines proceed undisturbed up to the ternary
eutectic point.

4th case. In the fourth case we might suppose that each of the
binary systems presents critical end-points. To realize this case we
shall have to choose three substances, the critical temperatures of
which lie apart as far as possible, so that in each binary system the
triple point of one component lies far above the critical temperature
of the other. If then double critical endpoints occur, we get a com-
bination of fig. 2 and fig. 5.

5th Case. It is elear that the appearance of mixed crystals in the
system 5—C does not bring about
any change in the foregoing con-
siderations, when this system has
a eutectic point; if this is not the
case, modifications appear which
are most considerable when the
components B and C are miscible
in all proportions, as in the system
SO,+Hgbr,—HeJ,. examined by
Nicer). The projection of the eriti-
cal end-point lines runs then as is
schematically represented in fig. 6. Fig. 6.

Now it should be pointed out, however, that when the melting-
point line of the system S—C' has a very marked minimum, a
closed portion can be formed in the middle of the figure, so that no critical
endpoints occur there then. If on the other hand the said continuous
melting-point line has a very marked maximum, the special case might
be found that though no critical endpoints occur in the binary systems
A—B and A—C, they do occur in the ternary system. We can
imagine that this case arises from the ordinary case fig. 6 by the
points p, and g,, and also p, and q, approaching each other and
coinciding, in consequence of which the two critical end-point lines
merge continuously into one another. If then this continuous curve
contracts still further, we have obtained a closed critical end-point
curve, which lies quite inside the concentration triangle.

1!) Niae@ui, The projection.

131

6th Case. If a binary compound appears as a_ solid phase,
different cases may be distinguished, the most interesting of which
I will discuss here. In the first place we shall suppose that the com-
ponents B and C do not give critical end-points either with A, nor
with the compound BC, but that this compound gives critical end-
points only with the most volatile component A. It is clear that when
this case occurs, the triple point temperature of the compound BC
will probably le far above that of the components 6 and C.

If we draw the projection of
the vapour and the liquid line of
the three-phase equilibria Sgo + L
+ G and that of the critical iso-
therm on the concentration triangle
corresponding to a temperature
lying above the critical tem-
perature of A and a little above
the highest eutectic temperature
of the system B—C, Fig. 7. is
formed.

Fig. 7. The isotherm 4,4, is convex

seen from A, as it is supposed
here that the compound BC'is less
volatile than the components 5
and C. When the liquid vapour
surface in the ternary v-z-figure
recedes more on rise of tempera-
ture than the surface of nodes for
the liquids and vapour coexisting
with solid BC, the critical isotherm
will touch this surface of nodes
at a given temperature; then the
liquid and the vapour line of this surface of nodes merge continuously
into each other. At a still somewhat higher temperature a closed
portion is formed in the surface of nodes, in consequence. of
which two ternary critical end-points have appeared, as fig. 8 shows.

If we think the temperature as gradually rising, the critical end-
points will recede from each other in the beginning, and they will
also move towards the plane LC, but before the triple point tem-
perature of the compound has been reached the points p, and p,
will approach each other, and they will coincide, because when we
approach the triple point temperature, the surface of nodes of the
liquids and vapours that coexist with solid LC will have to con-

192

ZB tract more rapidly than the liquid-
vapour surface, for this surface of
nodes entirely disappears at the

: triple point temperature of BC.
So if we draw the ternary critical
BC end-point line in this case, we get

‘ a closed eurve, as is drawn in
‘0. fig. 9 with a temperature mini-
mum and maximum.

A C If critical end-points occur also

Fig. 9. in one of the binary systems AB

or AC’ or in both, other cases may occur, but they are easy to

derive from what precedes. If also ternary compounds are included

in our considerations, the cases get somewhat more complicated, as
I hope to show on a following occasion.

Anorg. chemical laboratory

Amsterdam, June 27 1912. of the University.

Astronomy. — “Researches on the orbit of the periodic comet
Holmes and on the perturbations of its elliptic motion”. V.
By Dr. H. J. Zwirrs. (Communicated by Prof. E. F. van DE
SANDE BAKHUYZEN).

In January 1906 I communicated to this Academy the most probable
elements I had derived for the return of the comet Holmes in 1906—
O7. In a later paper, November 1906, I discussed the then known
three photographic observations of the comet by Prof. Max Wotr
at Heidelberg, and from these derived corrections to the mean longitude,
to the inclination and to the longitude of the ascending node of the
orbit. The elements obtained were:

Epoch 1906 January 16.0 M. T. Greenw.
M, = 351°47'36".838
u = 517" 447665
log a = 0.5574268
p= 24°20'25".55
1 ="-20 49 062
a= 346 231 .63 , 1906.0
Sb = 331.4437 85
These elements left the following errors O—C in the three observed
places :

193

1906 Aug. 28.55 Aa = + 08.095 Ad = — 0".33
Sept. 2Ok == a O99 = + £26
Oct. 10.35 =e te fe = —1 .15

So the obtained elements very satisfactorily represented the obser-
vations, and might therefore be adopted for the apparition in 1906,
until by a rigorous calculation of the perturbations this apparition
may be exactly combined with the previous ones.

On December 7, however, Prof. Wour succeeded in taking another
observation, this time with the great reflector of 28 inches aperture.
It was, however, exceedingly difficult to obtain trustworthy measure-
ments from this last plate. First of all the image of the comet was not
sharply defined; ‘das bild ist verwaschen, aber deutlich’’, Prof. Wor
wrote already on Dec. 8. A much greater difficulty arose owing to
a peculiarity of the photographic star images, especially on plates
taken with reflectors of this shape. The following quotation from a
letter of Prof. Wour of 1906 Dee. 27 may serve to characterize the
phenomenon, indicated by him with the name “Verzeichnung”’.

“Die relative Verzeichnung, ein von mir eingefiihrtes Wort, ist
“der grésste Feind und wichtigste Fehler der photogr. Positions-
“bestimmungen. Sie besteht darin, das fiir jede Sternhelligkeit der zu
“messende (Mittel-)punkt des entstehenden Sternscheibchens an anderer
“Stelle des Scheibchens zu suchen ist. Also z. B. liegt beim Reflektor
“der geometrische Mittelpunkt eines Sternes Y'** Grésse in der Nahe
“des Gesichtsfeldrandes um mehrere Bogenminuten, soviel ich bis
“jetzt schaitzen kann, von dem Punkt entfernt, anf den man die
“Position eines schwachen Objektes (Cometen) beziehen muss. Fiir
“jede Sterngrésse andert sich dies, ebenso fiir jeden Radius ab
“optischem Centrum, also A= //f(r,m). Bei Brashear 6 ist die rel.
“Verzeichnung erst in 6° radius merkbar. Bei Brashear a schon in
“3°—4° ry, Beim Reflector schon in 10’ —20’ r.”

On the 18t of Dec. Prof. Worr wrote to me:

“Aus A. G. Cambr. 1572 und 1584 erhalte ich fiir den Kometen
@is06.0 3°38™503.41 di906.0 + 51°16'52".7 1906 Dez. 7 7°8™.1 MZ. Kegst.
Grosse 16.

“Ob die relative Verzeichnung ganz richtig eliminiert ist, weiss
“ich aber nicht. Ich bringe es auch vorerst nicht heraus. Mir

“scheint deshalb, dass das Gewicht dieser Beobachtung etwas
“geringer ist, als das der ersten Beobachtungen.”

With the scarcity of the material this observation too demanded
the necessary attention but after wlrat has been said above I need

194

hardly mention that I commenced the calculations for it with little
hope of success.

For the reduction to apparent place I found:

in @: +5s.112 in d: + 9."75
and as correction for parallax :
in a: — 08.247 in Jd: + 0.72

The observed apparent place thus becomes:

1906 Dec. 7.273046 : a = 3538" 558.275 d = + 51°17'3"17
Time of aberration: 0.011279 day.

This observation has further been treated in exactly the same way
as the three preceding ones in my communication of Nov. 1906.
As starting-elements I again adopted those given in my paper of
January 1906, p. 677, after increasing 4/ with 50". I obtained as
differences Obs.— Comp. :

1906 Dec. 7.27: Aa=-+ 18.065 A d= + 15'.53

For the derivation of the differential quotients of @ and fd with
respect to J/, ¢ and §% the computed places were then derived 1. with
AM =-+ 40" (instead of + 50"); 2. with Az =-+ 10"; 3. with
AQ=+10". Thus this fourth place yielded the two following
equations of condition:

From a: + 0.2288 AM — 0.0372 4:— 0.0114 AN, =+ 138.065

From d6: + 0.426 AM+1.3874 Azi+ 0.03838 Ag, =+ 15"53.

The first equation was again multiplied by 15 cos d and just as
ieee ae
before aie was introduced as unknown quantity instead of AQ;

moreover I gave half weight to both equations. Thus I obtained 2
new equations, in addition to the former six, given in my paper
Researches IV (Nov. 1906):

from the R. A.:

A
0.18128 AM + 9.39236, Az + 9.87872, — = 0.84917

from the declination :

AS
10

9.47889 AM + 9.98747 Az + 9.36799 = 1.04067

in which all co-efficients are logarithmic.
From the total of 8 equations of condition there follow the normal
equations :

195

- 442.3299 AM — 0.47796 Ai — 4.9039 ie — — 17.461
— 047796 ,, +51423 ,, — 2.3300 ,, =-+ 58.562
— 49039 ,, —2.3300 ,, +44680 ,, = — 26.733.
These give the following values for the corrections of the elements:
AM = — 2".6793
Ai=+ 9 .29
AS = — 40 .78

By means of substitution in the equations of condition we find
that these corrections leave the following errors O—C in the obser-
vations :

1906 Aug. 28.55 Aa = — 03.190 Nd == — OF1
Sept. 25.51 — 0 .207 ++ 0 .72
Oct. 10.35 — 0.510 — 2 .26
Deg 0.27 + 1.559 + 5.25

The now found corrections of the elements do not differ considerably
from those determined before, but a comparison of the remaining
errors shows that the introduction of the uncertain fourth place in
the calculation cannot be said to have improved matters. Therefore
I continue to regard the elements given at the beginning of this
paper and agreeing absolutely with those from the ‘Proceedings’ of
Nov. 1906, as the most accurate for the present moment.

For the approaching return of the comet I have kept these ele-
ments unaltered since there was no time to calculate the pertur-
bations. I have only reduced the elements 7, a and $v to the ecliptic
and the aequinox of 1912.0. So the employed elements are :

Epoch 1912 June 15.0 M. T. Greenw.
M = 328°25'19".269
uw = 517" 447665
— 191s January 20:695 M.'T. Gr.
log a = 0.557427
gp == 24°20'25".6
~== 2049 3.3
346-7352 .9 ---1912.0
Sh = 351 4942 1
According to these elements circumstances are not quite so favour-
able this time. The perihelion passage occurs shortly before the con-

196

junction with the sun so that the comet is then at a great distance
from the earth and its place in the heavens is moreover not far from
the sun. The circumstances are more favourable at the opposition in
1912, although the comet then remains invisible for our northern
regions owing to its considerable southern declination. In order to
calculate an ephemeris for that opposition I have first derived the
following expressions for the heliocentric co ordinates : .

x = [9.99 3799] sin (v + 77°42'18".3).
y = [9.87 6101] sen (v — 20 52 48 5)
z = [9.83 2770] sin (v — 1 4355 .6)

The rectangular solar co-ordinates have been taken from the
Nautical Almanac and reduced to the mean aequinox of the beginning
of the year.

The resulting mean places of the comet were reduced to the
aequinox of the date by means of the constants f, g, G@ of the
Naut. Alm.

The following table gives the apparent places of the comet for
Greenwich mean noon; column # gives the theoretical brightness

according to H =-. It may be remembered, that the value of 7
7B

for the time of the photographs by Wo.r in 1906 varied between
0.032 and 0.088.

Apparent places of the come

197

t from 1912 June 15
for O& mean time at Greenwich.

to 1913 Jan. °

1912 4 log < H
|
h m-s PP ie at
ante 15. |2210223 29-74 | -= 49 16 38.2 0.24 0106 | 0.0473
FE} 21 41.65 20 43.5 | 0.23 6066 |
19 | 19 46.28 23 59.7 29204 | .0497
21 17 44.08 96 21.6 0.22 8530
pe As 15 35.55 21 43.9 5051 0519
5 13 21.29 Ig = 32 1779 |
27 11 1.95 21 16.6 0.21 8719 0541 |
29 8 38.22 25 21.3 5878
| July 1 | 6 10.91 O29 14." 3263 0561
3 | 3 40.82 17 54.9 0878
5 | b (g282 12 19.3 0.20 87132 0580.
7 | 18 58 35.69 5 26.4 6828
9 | BG. Pes dos 48 5715.7 5172 0596
11 53 29.71 4] 47.7 3764
13 50 58.71 Si. 25 2608 0611
15 48 30.30 2% 0.2 1706
17 46 5.39 11 42.4 1058 0622
19 43.44.82 | — 4157 11.1 0660
21 41 29.38 41 30.6 0510 0631
23 39 19.87 24 42.5 0603
25 37 16.84 6 50.5 0935 | =.0637
ale 35 20.86 — 46 47 58.3 1504
29 | 33 32.44 28 9.8 2302 0640
31 31 52.05 7 29.1 3322
Aug. 2 | 39 20.08 — 45 46 0.3 4558 0641
4 | 28 56.87 23, 47.6 6004 | |
6 | 27 42.67 0 55.1 7651 0639
8 | 9% 37.69 | — 44 37 26.8 9492
10 | 25 42.13 13 26.9 0.21 1522 0635
12 | 94 56.14 | — 43 48 59.5 3728
14 24 19.80 24 8.9 6103 0629
16. 93-58 11. \(=-42 58-58.7 8634
18 23 36.05 33 32.6 | 0.22 1309 0620
20 | 23 28.54 7 53.4 4124
22 | 93 30.42 | — 41 42 4.6 7065 0611
24 | 23 41.53 16 8.9, 0.23 0124
26 | 94 1.68. | — 4050 8.9 3291 0600
28 | 24 30.72 24 6.4 6559
30 | oe 8.35.. | S. 39758. 3.5 9918 0588
| Sept. 1 |> 25 54.37 32 1.8 0.24 3360
3 26 48.58 Ga el 6879 0576
5 97 50.86 | — 3840 7.0) 0.25 0470
7 29 0.94 14 16.3 4121 0563
9 30 18.57 | — 37 48 31.3 7825
11 31 43.54 92 52.8 0.26 1575 0549
13 33 15.68 | — 36 57 21.1 5370
15 34 54.72 31 56.2 9197 0536
{T.| 36 40.39 6 38.2 | 0.27 3049
19 38 32.44 | — 35 41 27.3 6921 0522
a.) 40 30.62 16 23.7 | 0.28 0810
23 42. 34.68 | — 34 5h 27.2 4709 0509
5 44 44.37 26 37.3 8613
27 46 59.46 153.7 | 0.29 2518 0496
29 AGO. = So Sb 15.3 6423

a 3 log Pp H
| j h m Ss fe} / " |
| Oct. 1 1851 44.96 | — 33 12 41.9} 0.30 0324] 0.0483 |
3 54 14.99 | — 32 48 12.8 4217
5 56 49.62 23 47.3 8098 0470
| 7 | 59 28.72 | — 31 59 24.6| 0.31 1966 |
9 | 49 2 12-10 35 4.0 5817 | .0458
11 459.57 10 45.0 9648 |
13 | 750.95 | — 30 46 26.7! 0.32 3455 0446
| 15 | 10 46.07 OF. S16 7235 |
17. | 13 44.73 | — 295749.5 | 0.33 0986 | -.0434
19 16 46.75 35 28764 4707 |
21 19 51.95 9 5.6 | 8397 | .0423
23 23 0.18 | — 28 44 40.0 | 0.34 2052 |
25, | 26 11.28 20 10.3 5672 0412
97 | 29 25.12 | — 2755 36.0 9257
29 99 41 5a-e 30 56.3} 0.35 2807 .0402
Si al 36 0.47 | 6 10.7 6320
Nov. 2 | 39 21.75 = 26 41 18.4 | 9795 | 0392 |
4 | 42 45.30 | 16 18.9 0.36 3231
6 | 46 11.01 | — 25 51 11.4 | 6626 | 0383
8 | 49 38.74 25 55.3 9981
10 53 8.41 030.1) 0.37 3294 .0374
12 | 56 39.92 | — 24 34 55.3 | 6564
14] 20 0 13.14 9 10.4 | 9789 0365
16 | 3 47.93 | — 23 43 14.4! 0.38 2970
18 | 7 24.20 173264 6107 .0357
20 11 1.85 | — 22 50 49.6 | 9198
22, | 14 40.78 24 20.0 0.39 2245 .0349
24 | 18 20.90 | — 21 57 38.1 5248
26 | ge Pea be 30 43.8 8206 0342
28 | 25 44.40 3 36.9 0.40 1120
30 | 2997 67s = BPB6-17.4 4 3990 .0334
Dec. 2 | 33 11.89 844.1 | 6817
4 | 36 56.98 | — 19 4057.7. 9600 | -.0327
6 40 42.88 .12 57.6 | 0.41 2337
8 44 29.53 | — 18 44 43.6 5029 .0321
10 48 16.89 16 15.6. 76717
| 12 | 52 (4.877 |= 17 8733.61 > 0:42 275 0314
14 | 55 53.40 18 37.7 2833
16 | 59 42.42 | —~16 49 27.9 | 5342 .0308
| 18.) 213 31200 20 4.2 | 7808
20 | 7 21.77 | — 15 50 26.8 | 0.43 0229 .0302
22 | 11 11.94 20 35.7 2605
24 | 15 2.38 | — 14 50 30.9 | 4937 0297
26 | 18 53.14 20 12.6 | 7227
| 28 | 9944.16 | — 13°49 41,0. 9474 .0291
30 | 26 35.41 18 56.1 0.44 1679
Jan. 1 | 30 26.86 | — 12 4758.2 | 3842

.0286 |

The following table gives the variations of @ and d in two suppo-
sitions: 1st that the comet reaches its perihelion 4 days earlier,
2nd that it reaches it 4 days later.

> | —

199

Variations of « and d for altered times of perihelion passage.

OT =— 4d

1912/13

m s
— 8 46.83
— 8 59.63
— 9 10.67
— 9 19.43

=OtmA OM 1N'oO

éixer 2016 2 -b 2 aw

10 O- rhea kar)
10 NI
Orit n- ODO
NANNAATA eS
ied ef | P|
tOomoma;rnw
SSRBSLSSS
IN DDO ANI
AQAA

19 $10 1H DIS

et CO al
SOmuonton-
ONAAAATAIAN

SF deloaicten

m—r- 1010 O©r10-
CcCoOnMmnoowoo iw;

CONAGHAOH
AIM CO COMI 18

DAAAAIADN SO

“tb ++

oMmowmn O10

Dm DH i 10 10 1010
r= Ot = 1010 DD
oOo- fo |

QIN TIVO D FOS
ice) 1 10

ooooocons:
NAN SK KH ANNAIA

Aichi

AAI AT 09 08

A110 CO D sh 10
stm ino ONO =
NAAT

bs ae)

— >> = =o =
OAINI NAN
Hig Ol ©

NNAA A

spi a

m=O min DOH
HOoCcNnoor-

Om ODIO AS
Cee SCN it

(coco )Ke.oK/0)] taal all all Son

+++4+++++

NOOMtOAIO OS
met St OI CI OD

+++}

0910 010 © 0) cD
OD DD OD SH et tH OY)

SNUSH~OO
HOA 19 HO

OOO O10 1010

Mm Hr HO 10

o) eee. “Cora ee

Cer Cs me a Cer

SOKA Fi9 al
Aa 1 HCD

RIB HOH GHG

tp i

ST T= oO Sh CO CO =
OOM OM rmin rn

SrAAnHGsan
aI 10 OD 09

10 10 1.0 1.0 HSH SH sH

SeyetaleT eal:

=OMm10 DODO

1D S00 SS 0 0
10 m1
BBA MADEH

(i ORME Sale A eee

THA OMInS
mT HANA

BEDE DCO

++++++4++4+

[meio )itee}le opr) tral) tmatl eye)
On NS Or
Pei Oi © 16 =
ANAL AS ee 1010

SS ST SSH CD CPD

Se iri

07
15
51
99
15
54
64

— 3 39
— 3 35

OOntt AIO

mae HAITI AIC
SH SH St Sh << <f

1N 0) Dn 10 ©
N01 © OOO

rHODSIDO
HH cD CO AIA

Om 09 6 0 6) CDC

aegis:

| Sept.

1 D CD Qn
See | NI

_ Oct.

Nes Teas
mee AIA

— 42 41.8

— 3 23.88

Jan.

+ 3 23.84 | + 43 16.8

Leyden, June 1912.

200

Mathematics. — “The scale of regularity of polytopes’. By Dr.
E. L. Exre (Meppel). (Communicated by Prof. P. H. Scuovre).

In my dissertation*).it was my aim to determine the semiregular
polytopes, i.e. the polytopes analogous to the semiregular polyhedra.
So this investigation had to be based on a definition of the notion
“semiregular polytope’. Now ordinarily a semiregular polyhedron is
defined as follows: “A semiregular polyhedron has either congruent
(or symmetric) vertices and regular faces o congruent faces and
regular vertices. So there are two kinds of semiregular polyhedra
which we will call with Catalan’) “semiregular of the first kind”
and ‘semiregular of the second kind”; those of the first kind are
enumerated in the following table. For any of these polyhedra this
table gives the numbers of vertices, edges, faces and indicates which
faces pass through each vertex and which couples of faces pass
through each kind of edges. Here p, denotes a regular polygon
with n vertices.

Faces through Faces through

Notation) N”. ‘Vertices | | Faces eres the edges

lpn , 3p3 Pn P3 | P33

2
3
4
5
6
7
8
9

1) “The semiregular polytopes of the hyperspaces”, Groningen, 1912.
*) “Mémoire sur la théorie des polyédres”, Journal de l’Ecole Polytechnique, ~
Cahier 47.

201

The semiregular polytopes of the second kind are the polar-reci-
procal figures of those given in the table with respect to a concentric
sphere.

The definition of semiregular polyhedron given above had to be
modified in order to make it applicable to polydimensional spaces.

We say that a polyhedron possesses a “characteristic of regularity”,
if either all the vertices, or all the edges, or all the faces are equal
to each other. Equality of vertices signifies that the polyangles
formed by the edges concurring in each vertex are congruent (or
symmetric); equality of faces consists in the congruency of the
limiting polygons. But the equality of edges includes two different
parts which can present themselves each for itself: equality in length
of the edges and equality of the angles of position of the faces
through the edges. So all the polyhedra of the table have edges of
the same length but —- with exception of the numbers 6 and 7 —
more than one kind of angles of position, whilst quite the reverse
présents itself with the corresponding polyhedra of the second kind.
If the equality of edges is realized only partially — as in the case
of the polyhedra of the table — we speak of a “half characteristic”
so that these polyhedra admit 1} characteristics. By bringing this
result in connection with the circumstance that a polyhedron can
admit 3 characteristics, the epitheton “semiregular’” obtains a Literary
signification. As the polyhedra N°. 6 and N°. 7 of the table possess
both the half characteristics of the edges, these polyhedra must be
called ‘“?/,-regular’ according to our system.

We remark that the characteristics of a semiregular polyhedron
of one of the two kinds are lacking in the corresponding polyhedron
of the other. Moreover that we are obliged to observe a quite
determinate order of succession in counting the characteristics of a
polyhedron of defined kind and, beginning at the commencement, to
count successive characteristics only, i.e. in the case of polyhedra
of the first kind to take into account successively equality of vertices,
equality in length of edges, equality of angles of position round
edges, equality of faces, and reversely in the case of polyhedra of
the second kind. Jf this order of succession was not observed e. g.
with respect to the two half characteristics of the edges a beam
with different length, breadth, and height would appear as a semi-
regular polyhedron of the first kind on account of equality of ver-
tices and angles of position, whilst a double pyramid formed by the
superposition of two faces of two equal regular tetratredra would
appear as a semiregular polyhedron of the second kind, to which
enunciations fundamental objections can be raised.

202

Now the definition of “degree of regularity” extended to higher
spaces runs as follows:

“The degree of regularity of an 7-dimensional polytope is a fraction
with 2 as numerator and the number p of the successive charac-
teristics of regularity as denominator, this number p being counted
in the case of a polytope of the first kind from the vertex end, in
the case of a polytype of the second kind from the end of the limiting
n—1-dimensional polytope.”

In my dissertation 1 have contined myself to polytopes of the
first kind, the degree of regularity of which is 4 at least. For the
methods employed in unearthing these polytopes I must refer to
that memoir.

In discussing my dissertation my promotor Dr. P. H. Scnoure
remarked that if all the fractions representing possible degrees of
regularity of an n-dimensional polytope are reduced to the denomi-
nator 2n the numerators 1 and 2n—1 will be lacking, on account
of the fact that the first and the last characteristic have not been
subdivided into two halves; so in this sense my scale contains
something superfluous. .

Indeed the classification of the polyhedra according to my scale
is indicated in the diagram

0 — 1

|
I

|
|

ee ie R

3 4
6 6

— | or

where the numbers 1—5, 8-—15 at the midpoint and 6,7 at the
right designate the polyhedra bearing these numbers in the table,
whilst 7 and # stand for quite irregular and regular polyhedra and
P cither for the beam or for the double pyramid mentioned above,
according to the scale corresponding either to polyhedra of the first
or to polyhedra of the second kind. Indeed the points of division

1 5 . Ags
= and ne are unoccupied and in SS, the analogous. characteristic
; : £ 1
property presents itself with respect to the points of division —
an
2n—1
and :
an

It goes without saying that we can take away the superfluity
indicated (of the two points of division adjacent on either side to
the extremities) ezther by counting each of the two extreme charact-

203

eristics, that of the vertices and that of the limiting »—1-dimensional
polytopes, for half a characteristic, 07 — what comes to the same —
by counting each of the two extreme characteristics and each of the
two halves of the remaining intermediate characteristics for one. So
the scale relating to our space passes into

1 2 3
0 us = es 1
4 4 4
|-—— | —— | ——__ |
v4 P 1—5, 6,7 R
8—15

where the numbers and the letters have the same meaning as above.
An n-dimensional polytope of the degree of regularity = according
U

to the scale given in my dissertation will be qualified, for 1 < p <n — 1,
pP—2

——

this degree would acquire the same value for both scales in the
cases p=O and p=n, i.e. for entirely irregular and for regular
polytopes. For in the cases 1<p<n—1 a polytope loses in the
first of the two possibilities indicated by ezther and or a half characte-
ristic, whilst the total number of available characteristics diminishes
by a half at either side which changes the denominator n into n—1.

by the degree of regularity

according to the new scale, whilst

In this paper I wish to take position with respect to the modifi-
cation of my scale due to Dr. Scnoutre. Thereby I will have occasion
to point out three different moments.

1. Besides for entirely irregular and for regular polytopes the
two scales coincide with respect to semiregular polytopes proper.
For the supposition

gives.
2p(n—1) = n(2p—1),

i.e. p= 4n and therefore
1 OC ee

5
2
So, if we arrange the polytopes of space S, in three groups, for
which the degree of regularity is successively smaller than a half,
equal to a half and larger than a half the modification proposed
brings no alteration in these groups. Otherwise: in passing to the
new scale the polytopes with a degree of regularity equal to a half
14
Proceedings Royal Acad. Amsterdam, Vol. XY.

204

do not stir, whilst — if we use scales of the same length — the
others execute a movement enlarging their distance from the centre.
So the polytopes with a degree of regularity of at least a half
found by me present themselves quite as well if we use the new
scale; so in this respect I have not the least objection to accept this
new scale. *)

2. However one may not flatter oneself with the hope, that the
new scale shall not contain superfluous points of division with respect
to either of the two kinds of polytopes considered for itself. In space
S, already we find with respect to the polytopes of the first kind

in this new scale, agreeing with the old one for n= 3, the point
ISA

. . . v0 .
of division = unoccupied. For we have

1 D 3 4 5
0 ze af = ae = 1
6 6 60 6 6
- | | a
I P e,8(5) e,8(5) ce, S(5) R

where / and R have the same meaning as before, whilst P represents
a rectangular parallelotope with edges of four different lengths and
e,S(5), e,S(5), ce, S(5) indicate three polytopes deduced from the
regular simplex |S (5) of S, in the notation given by Mrs. A. Boone
Stott ”).

3, As the new scale contains no unoccupied points of division in
the case n==3 only, it would not be worth while to substitute it
for mine, which has the advantage of treating all the groups of

limiting elements — vertices, edges, faces, etc. and the limits with
the highest number of dimensions — on the same footing, if it did

not possess a second advantage, in my opinion of great importance.
We will treat this somewhat in detail.

In the determination of the semiregular polytopes of the first kind
I consider of any polytope the corresponding ‘‘vertex polytope”’ *).
In general the vertices of the latter are those vertices of the former
joined by edges to a vertex of this original polytope. In an appendix
to my dissertation I state the rule, that a polytope with edges of

\) Dr. Scuoure requests me to communicate that the primitive idea of this new
scale for .S, presented itself to him in an intercourse with F. Zernixe, candidate
in mathematics and physics at the University of Amsterdam.

2) “Geometrical deduction of semiregular from regular polytopes and space
fillings’, Verh. Kon. Akad. v. Wetenschappen, Amsterdam, 1st series, Vol. XI, n°. 1.
3) Not to be confounded with the polytope of vertex import of Mrs. A. Boouz Srorr.

205

the same length*) admits one characteristic of regularity more than
its vertex polytope, i.e. if the latter is n-dimensional and admits the’

hes 43 : ;
degree of regularity —, the former must admit the degree of regularity

pt+l
n--
does not bring any alteration. If we build up an n+1-dimensional
polytope by starting from a given n-dimensional vertex polytope,
the n+1-dimensional polytope will possess all the characteristics of
regularity of the n-dimensional one, eacb of these adapted to limiting
elements of one dimension higher, and moreover it obtains at the
beginning of the series two new halves of characteristics, i.e. equal
vertices and edges of the same length. Finally the denominator like-
wise increases by unity, the new polytope admitting one dimension
more than its vertex polytope.

In my dissertation I had to point out an exception to this rule,

presenting itself in the case p=0O, i.e. when the vertex polytape
ab

. In this rule the indicated modification of the scale evidently

instead of

0
is irregular. For in that case — passes into
n

n ntl
So the vertex polytope of the semiregular polyhedra of the table
— ie. “the vertex polygon” here — is an isosceles triangle for the

numbers 1-—5 and 14, an isosceles trapezium for 8, 9, 15, ascalene
triangle for 10, 11, a symmetric pentagon for 12, 13 and therefore
l

ses: 13
the degree of regularity = of the vertex polygon has to lead to m == 4

in the cases enumerated. This exception now disappears by intro-
duction of the new scale of Dr. Scnoutr; for according to this scale

0 1
i passes into = in these cases.

On account of the latter important advantage of the new scale
over the old one I wish to accept the first. Therefore I insert
finally a second table in which the polydimensional polytopes with
a degree of regularity equal to or surpassing } are enumerated with
addition of their degree of regularity according to the new scale.

The superscripts S, represent the number of the n-dimensional
limits of the polytope. The character of these limits is indicated by
notations, the meaning of which is partially clear by itself or by
the first table of this paper. Moreover we may state the meaning
of the following symbols :

1) The latter has been supposed tacitly on p. 129.
14*

206

Degree Notation S> | Si | So S3 S4
4:6 | tCs 10| 30| (10+ 20)p5 50+5T
Biro |tGs 32| 96) 64p3 + 24p,4 8CO+16T
6 | to, 96| 288, 96p3 + 144p4 | 24CO + 24C
4:6 | tCgo) | 720| 3600) (1200+ 2400)p| 6000+ 1201
3:6 | tCyo) 1200] 3600) 2400p, + 720p; | 120ID-+ 600T
3:6 30! 60} 20p3 + 20f5 10tT
3:6 288] 576) 192p3-+ 144 pg, 48 tC
3:6 20! 60} 40p3 + 30p4 10T + 20P,
3:6 144| 576] 384p;-+288p, | 480+ 192P,
a6 n2| 2n2) n2p4-+-2npy 2n Py
5:8 | Ss2 20| 90 120 ps B0ir 13010, 12 tCs
6:8 | HM; 16) +80 160 ps (80 +- 40) T 16:G,- 10\Cx6
4:8 | Sst 15| 60) (20-+60)ps; 30 T +150 GCr ar GitGs
4:8 | Crs! 40| 240] (80+ 320) ps; 160 T+ 800 824C,--.10 Ci,
4:8 | Crs2 80| 480] (320 +320) p5 80 T + 200 0 B2tCs 1 10'Co,
e10| Wao 712| 720 2160 ps 2160 T 432 Cs + 270 Cig
6:10) HMg 32| 240 640 ps (160 +- 480) T 192°C. 60'Cig
8: 10| Voy 27) 216 7120 ps 1080 T 216 Cs + 432 Cs
10:12] Vs 56| 756 4032 ps 10080 T 12006 C;,
8:12] Vio6 126 | 2016 10080 ps 20160 T (4032 ++ 12096) C;
Oe12! Vern 576 |10080 40320 p3 (30240 ++ 20160) T 116128 Cs +- 7560 Cy6
8: 14 Vorgo » 12160 169120 483840 ps3 1209600 T (241920 +-967680)C;
12:14) Vo4o 240 | 6720 60480 pz 241920 T 483840 Cs

54 HM;
32 Ss + 12 HMs
72'S 27. Cre
(2016 + 4032) S;
4032 Ss +- 7156 Crs
2016 Sx +-2268HMs
483840 S;-+-60480Crs
483840 S;

516 Sg + 126 Cr¢
576 Sg + 56 Vor
126HM5 +56 Vr. |
138240S,-+ 6720 Voy]

(69120-4-138240)S¢6| 17280 S7 +-

17280 Sy -

=
'

240 Vi 26
2160 Cry

207

dae ,, tetrahedron,

C » hexahedron (cube),

O » octahedron,

Ce. » fourdimensional five-cell,

ec: * fs sixteen-cell,

c; “ Ps twinty four-cell,
Sn ',, m-dimensional simplex,

Cr, = > cross polytope.

The cases in which we have to deal with a half characteristic
are also indicated in this table. So e.g. the first polytope of the table
is limited by. equilateral triangles of two different kinds, presenting
themselves in the numbers 10 and 20.

Meppel, June, 1912.

Chemistry. — “Cuntribution to the knowledge of the direct nitration
of aliphatic imino compounds’. By Prof. A. P. N. Fraxcuimont
and Dr. J. V. Dussxy.

In the January meeting 1907 I had the honour to give a survey
of the action of absolute nitric acid on saturated heterocyclic com-
pounds whose ring consists of C and N atoms. This originated in
the fact observed and described by Dr. Donk, that the so-called

H
glycocollanhydride H,C—N—CO, in which the group NH is placed
|

o¢_N—¢a,
H
between CO and CH,, nitrated with difficulty, with much more difficulty
than I had expected because a number of other heterocyclic com-
pounds with rings of five or six atoms in which the group NH is
placed in the same manner may be readily nitrated with absolute
nitric acid at the ordinary temperature. This was not the case here;
only a treatment of the nitrate with acetic anhydride or, as I showed
*with Dr. Frrepmann, of the glycocoll anhydride with acetic anhydride
and nitric acid gave a mono- and a dinitroderivative.
CH,
H
With the so-called alanine anhydride HC—N—CO and with the

| |
OC—N—CH
H |
CH,

a-amino-isobutyrie anhydride (CH,),C—N—CO FRIEDMANN and I

| |
OC—N—C(CH,),
H

found something similar, with this understanding, however, that the
nitration always took place with more difficulty, which can be attributed
to sterical influence.

At the same meeting, I also called attention to the fact previously
noticed by me that the group NH placed in a ring between two
eroups CO cannot be nitrated with absolute nitric acid, neither when
it is placed between two saturated hydrocarbon groups. The expec-
tation that one of the eleven isomers of the so-called glycocoll anhy-
dride which Dr. Joxexres had prepared for me, namely tminodia-

H
cetic imide —-H,C—N—CH, in which one NH-group is placed between

|
We res
H
two CO-groups and the other one between two CH,-groups, would
not be capable of direct nitration by absolute nitric acid, was not
realised in so far that it appeared indeed to give a nitroderivative
but with some properties differing from those observed up to the
present with nitramines and nitramides, so that it was questionable
whether the nitrogroup is attached to the nitrogen or to the carbon.

Owing to the peculiar properties of the nitroderivative the chance
of answering that question in a direct manner, for instance by
reduction to hydrazine, was but a very slight one.

Moreover, the starting material, the imide, is obtained with diffi-
culty and then only in small yield so that a great economy is
necessary in the research. Two indirect ways could, however, be
pursued, namely by starting from substances in which either the
hydrogen at the N, or that at the C is replaced by other groups
and to test these compounds RN(CH,—CO),NH and HN(C(R),—CO),NH
as to their behaviour on nitration.

The last way is undoubtedly the best although even there
we may meet with difficulties, for instance a difficult nitration owing
to sterical hindrance as has already been demonstrated by me
and FRIEDMANN.

Of the first process a few examples will be given here, namely
acetyl and methyl derivatives, which, however, do not justify a
final conclusion. The surmise that the NO,-group is placed at the N
can be supported somewhat by the results of the nitration of the

209

acyclic compounds from which the imide is derived, such as imino-
diacetonitrile, iminodiacetic acid, its ester and imide. This at the
same time also furnishes a contribution to our knowledge of the
nitration of acyclic imino compounds from which it is again evident
that the nitration of one NH-group placed between two CH,-groups
(residues of saturated hydrocarbons) depends also on other consti-
tuents attached to these hydrocarbon residues.

The results obtained are as follows :

Iminodiacetonitrile HN(CH,CN), yields with ordinary nitric acid a
nitrate in beautiful glittering needles which melt at 138—140° with
decomposition. The formula was determined by analysis and titration
of the nitric acid. It is readily soluble in cold water, soluble in hot
methyl alcohol, ethyl alcohol and benzene. On slowly cooling a hot
alcoholic solution it yields very beautiful crystals. If this nitrate is
dissolved in absolute nitric acid (which is accompanied by a slight
evolution of heat) and the acid is allowed to evaporate in vacuo
over lime, the residue when triturated with absolute alcohol gives
a crystal-paste which, after being dried and recrystallised from dry
benzene, forms splendid snow-white needles melting at 100—101°.
Their analysis points to the nitro-derivate NO,N(CH,CN), nitro-imi-
nodiacetonitrile. It gives the reaction of the nitramines with zine and
an acetic acid solution of a-naphtylamine. On warming with water
decomposition sets in.

Iminodiacetic acid HN(CH,CO,H), gives a nitrate already described
in 1865 by Heintz. When this nitrate is dissolved in absolute nitric
acid and evaporated in vacuo over lime it is recovered unchanged.
It is insoluble in ether, benzene and acetic ether. If, however, the nitric
acid solution is heated to boiling a nitroderivative NO,N(CH,CO,H),
nitroiminodiacetic acid is formed, which is left behind after evaporation
of the nitric acid in vacuo over lime. It is soluble in methyl and ethy!
alcohol in acetone and acetic ether, also in cold water. Crystallised
from acetic ether it forms broad, flat needles mutually joined like a
fan. Its melting, or rather decomposition point appears to lie at
about 153°. Its aqueous solution is strongly acid and gives the above
nitramine reaction. A neutral potassium salt was prepared which
readily crystallises on addition of absolute alcohol to the watery solution;
it is decomposed at about 195° with explosion. The acid potassium
salt which is not easily soluble in alcoho! and yields beautiful crystals
was also prepared. From the ethyl ester of iminodiacetic acid described
by Mr. Jonekers there was also prepared a nitrate, which is very Jittle
soluble in alcohol and crystallises in silky needles, which melt at

210

198—199°. By treating this nitrate, in the manner described, with
absolute nitric acid in the cold xt is recovered unchanged but if the
solution is heated to boiling the nitroderivative NO,N(CH,CO,CH,),
is formed which is not, or but little, soluble in cold water so that
it may be precipitated by pouring the nitric acid solution into coid
water. From acetic ether, in which it is soluble, it is obtained in
silky delicate scales which melt at 63°.5. _

Iminodiacetamide HN(CH,—CONH,), gave with one mol. of NO,H
a nitrate which was obtained from the aqueous solution, by addition
of absolute alcohol, in beautiful lustrous leaflets which melt at 206°
with decomposition. If this nitrate is placed in absolute nitric acid,
an evolution of gas takes place after a short time, as in the case
of all amides of N,O; when this has ceased, or has been accelerated
by warming, the nitro-iminodiacetic acid is obtained.

Iminodiacetimide HN(CH,CO),NH, which was made according to
the directions of JONGKEES, also gave compounds with acids. We
prepared: (1) the HCl compound in lustrous, beautiful erystals which
are decomposed on heating above 180°; (2) the NO,H-compound, also
white crystals with a strong lustre, which when heated above 180°,
are decomposed and turn a bluish-green. Both compounds contain
one mol. of acid.

When iminodiacetimide or its nitrate is dissolved in absolute nitric
acid and the solution evaporated in vacuo over lime a crystal-cake
is obtained which may be recrystallised from boiling dry chloroform
in which it is very little soluble. It then forms beautiful colourless
needles which have the empirical composition of a mononitroderivative.
This nitroiminodiacetimide NO,N(CH,CO)NH spontaneously turns a
dark blue, especially in not quite dry air and its aqueous solution
on warming first turns green, then blue and deposits an almost
black amorphous substance soluble only in strong sulphurie acid
with an indigo-blue colour. *

In order to render it more probable still that the nitro-group
is attached to the nitrogen situated between the CH,-groups, the
acetyliminodiacetimide CH,CON(CH,CO),NH was prepared first of all
by subliming in vacuo acetyliminodiacetamide, which according to
JONGKEES decomposes at 203°. On recrystallising the sublimate from
methylaleohol splendid small crystals were obtained which melt at
167—168° and according to analysis, have the empirical composition
of acetyliminodiacetimide. They are insoluble in benzene, petroleum

ether and acetic ether. The same substance was prepared by boiling

iminodiacetimide with acetic anhydride. This acetyl derivative was
dissolved in absolute nitric acid and the solution evaporated in vacuo

211 =

over lime. The residual crystalline mass, after being recrystallised
from methyl alcohol, proved to consist mainly of unchanged acetyl
derivative. The mother liquor, however, exhibited colour phenomena
which may raise a suspicion that a small fraction of the acetyl group
has been replaced by the nitro-group.

Finally, also a few derivatives of methyliminodiacetic acid
CH,N(CH,CO,H, were made, in which the hydrogen atom of the NH-_
group which is placed between 2 CH, has been replaced by methyl]. First
of all the diamide by acting on the methyl ester of the said acid
for some time, with NH, in methyl! alcoholic solution. This diamide
CH,N(CH,CONH,), forms beautiful, large crystals melting at 162—
163°; it is readily soluble in cold water, methyl- and ethy! alcohol,
very little so in acetic ether, acetone, ether, petroleum ether, chloro-
form and benzene. It was recrystallised from boiling methy] alcohol.

From the diamide the imide was prepared by sublimation under
a pressure of 17—18 m.m. at 200 —220°. The methyliminodiacetimide
CH,N(CH,CO),NH thus obtained was first recrystallised from boiling
acetic ether in which the amide is practically insoluble, then from
boiling acetone and finally from a little boiling methyl alcohol. It
then forms white, glittering crystals which melt at 106°. This imide
gives crystallised compounds with one mol. of HCl or NO,H. The
first is decomposed by heating above 235°; the second by heating
above 130°; treated with absolute nitric acid an oxidation seems to
take place slowly at the ordinary temperature, at least after being
some time in vacuo over lime a decidedly strong evolution of red
fumes took place and from the residual swollen mass no well-defined
product could, as yet, be isolated.

Although the question as to the position of the nitro-group in
nitroiminodiacetimide is not yet quite solved, as this position will
be determined fully only then when the analogous isobutyrice acid
derivative HN(C(CH,),CO),NH has also been tested as to its behaviour
on nitration, yet it has been rendered very probable by the results
obtained, the publication of which was rendered desirable owing to
to the departure of Dr. Dusky.

The direct nitration capacity of the above acyclic aliphatic amino-
compounds, also the differences in the readiness of this nitration
point to a connection with what has been found in the case of
aromatic N-compounds where the nitration capacity, or otherwise
the formation of nitramines by direct nitration, has been first shown
by van Rompureu.

This connection is quite in harmony with what I have demonstrated

212

previously as to the direct nitration capacity of aliphatic carbon
compounds, by nitrating malonic acid and its esters, methylene-
tricarboxylic ester etc. from which it follows that the direct nitration
capacity is caused by the adjacency of so-called negative groups of
definite strength.

In this manner were also discovered the aliphatic nitramines and
nitramides, by nitrating the amides wherein occurs also a negative
group and it now appears that an aliphatic secondary amine (dime-
thylamine) may also undergo direct nitration when in the alkyl
groups are present the group CN or CO,H, so distinctly negative
groups.

I, therefore, put to myself the question whether the phenyl or
nitrophenyl-group would also be able to give the same result as
CN or CO,H. This, however, does not seem to be the case, for
dibenzylamine HN (CH,C,H,), yielded only dinitrodibenzylamine nitrate,
but no nitramine on boiling with absolute nitric acid. |

The ready nitration capacity of iminodiacetonitrile and of imino-
diacetie acid and its derivatives is striking especially when we com-
pare it with that of other substances as shown in the subjoined list.

CH3.NH.CH3 not CN . CH2.NH.CH,2. CN readily
CH3.NH.CO.CH3 readily | CO,H.CHg.NH.CH2.CO:H readily
CH;.CO.NH. COCHs readily | COQ .CH3.CH). NH.CH).CO;,CH3 readily
CH. NH. CO.CH3 iar | GaH NO) NH. Cs. CHNO. not
CH3.CO.NH. CO,CH3 readily | aa NH. CH3 readily
CH; . €O, . NH GOxeny not CyHa(NO,)3 . NH . CgH_(NO»)3 not
Biochemistry. — “A biochemical method of preparation of -Tar-

taric acid.” By Prof. J. Boeseken and Mr. H. J. WaTERMAN.
(Communicated by Prof. BetsERiNck).

In our investigations on the assimilation of carbon nutriment by
different kinds of mould it was found necessary to get some more
information as to the manner in which the carbon was retained in
the body of the plant either temporarily or permanently.

For this purpose one of us (H. J. W.) carried out a large number

213

of carbon determinations of the mould that formed on a definite
organic compound used as exclusive carbon nutriment, while at the
same time the amount of unattacked substance in the nutrient base
was determined. The further particulars of this research will be
communicated by him elsewhere, when the significance of the survey
thus obtained of the course of the plastic equivalent or assimilation
quotient of the carbon*) will also be explained: here we will call
attention to some observations on the growth of Aspergillus niger
and Penicillium glaucum on the tartaric acids.

Aspergillus niger grew hardly at all on /tartarice acid, but very
well on the d-acid, so that a 2°/, solution of the latter provided
with the necessary inorganic nutriment was, after the lapse of six days
used up by the mould. A 4°/, solution of uvie acid provided with
0.15 °/, NH,NO,, 0.15°/, KH,PO, and 0.06°/, MgSO, and inocu-
lated in the usual manner with Aspergillus niger and cultivated at
33°—34° gave after six days a maximum /-rotation; this then
began to decrease slowly, showing that the /-tartaric acid also gets
consumed.

This maximum rotation observed with the saccharimeter of Scamipt
and Harnscu for white light in a 20cm. tube, amounted to — 1°,0
corresponding with a solution of about 1,2°/, /-tartaric acid.

As a 4°/, solution of uvic acid can only give at most a 1.88°/,
solution of /-tartaric (on account of the disappearance of the d-acid
and the water of crystallisation of the uvic acid) this maximum
rotation corresponds with a yield of fully 60°/,.

In order to isolate the /-tartaric acid the liquid after removal of
the film-of mould, was precipitated with lead acetate. The precipi-
tate, after being washed was decomposed with hydrogen sulphide
and the filtrate evaporated.

From 4 grams of avie acid was obtained 0.8989 gram of l-tartaric
acid = 56°/,.

The acid crystallises readily.

0.100 gram consumed 8,6 cc. of baryta water of which 4.66
were equivalent to 0.100 gram of salicylic acid: Mol. Weight =
149.3 (calculated 150)

0.2719 gram was dissolved in 50 ec. Polarisation in a 40 em.
tube = — 0°.8, that is, for a solution in a 20 em. tube = — L°,5,
while a 2°/, solution of pure d-acid gave + 1.°6.

As a part of the /-acid is consumed and as this is connected with

1) Compare. Waterman, Mutation with Penicilliwm glaucum etc. These Proc.
29 June 1912, p. 124.

214

the increase of the mould material, it is desirable not to subject *)
large quantities of uvic acid to this operation all at once, but to
distribute it into a number of small flasks (containing not more than
50 ec.). Operating in this manner we prepared from 40 grams of
uvie acid, distributed into 20 flasks, nearly 9 grams of pure /tar-
taric acid.

The question, which is more of a biological than of a chemical
nature, how the /tartarie acid is decomposed, could be answered
by the determination of. the above quoted assimilation quotient of
the carbon, in that sense that it takes part, in the same degree as
the d-acid, in the construction of the organism. This could not be
proved in a direct manner, because the pure /acid promoted the
growth of the inoculating material too slowly, but it could be
determined from the values obtained in the growth on uvie acid
compared with that of d-tartaric acid.

The “acid is evidently attacked only a little slower. If we mix
d-acid with uvie acid this will not much affect the absolute con-
sumption of the acid because the total amount of mould material
formed in the same time will be approximately the same. As, howe-
ver, we can only subject to the operation a solution not exceeding
6°/,, the quantity of /tartarie acid is smaller from the commence-
ment and the yield will have to be low. If, for instance, we mix
1'/, gram of d-tartaric acid with '/, gram of uvie acid, practically
no /-acid will be left when all the d-acid has disappeared.

These experiments with Aspergillus were carried out in conjunction
with others, because we had noticed that Penicillium glaucum,
which was used for many of our observations exhibited towards
the tartaric acids a but little pronounced power of selection. This
will be seen at once from the subjoined table.

The three acids behave nearly similar in regard to a same Penicil-
lium culture; only during the first days the growth on the Lacid
is somewhat less than on the two others.

It seems remarkable that, in consequence of the great concentra-
tion of the hydrogen ions, the retardation which in a 2°/, solution
of /- and d-acid is very plainly perceptible after six days *) does not
set in at all with the anti-acid. This is quite in harmony with the
smaller dissociation constant of this acid*) owing to which, in a

1) When using larger flasks, the surface in regard to the capacity is as a rule
more unfavourable than when small flasks are used, so that the aeration becomes
insufficient.

*) BOEsEKEN and Waterman. These Proc. 30 March 1912, p. 1112.

5) Biscnorr and W atpen. Ber. D. Ch. G. 22, 1819 (1889).

215
TABLE 1.

Development of Penicillium glaucum in 50 ce. tapwater, pro-
vided with 0.05°/, NH, Cl, 0.05 °/, KH, PO, and 0.02 °/, Mg SO,.

f ys
| added acid Piarelopricn: in stated number
| | in mg. | . of days.
|
No d-tartaric acid | 2 | ee 6
50 i ie
2 100 + +> | ++
3 300 es Se pet SS
4 500 rer’ beck eee
(5 1000 | He sae ly
l-tartaric acid |
6 50 ea al rane
ee | 100 eee = ae eg
8 300 + ae 4-4
9 500 | 2 oe toes
“10. 1000 | 2 + as
Antitartaric acid 1) |
11 50 Sera ote ie ea
| 12 100 | - — | ——
13 300 fet pas 2B
(14 500 = }+ | ++
t 1000 | + +> | ++
|

2°/, solution thereof, the harmful concentration of the H-ions for
Penicillium is not yet reached.

For the rest, these small differences in growth at lower concen-
trations are somewhat unexpected because the specific character of
the two anti-podes has been determined by Pasreur first of all with
Penicillium glaucum. But it may be very well assumed that the

1) Aspergillus niger gives practically no growth on antitartaric acid.

216

organism used by us has been another form than that employed by
Pasrrur in his classic experiment and the continued investigations
of one of us*) (H. J. Waterman) have exactly demonstrated that the
phenomena of growth are dependent in a high degree on the variation.

Delft. Laboratory, Org. Chem. Techn. High School.

Chemistry. — “On a method for a more exact determination of
the position of the hydroxyl groups in the polyoxycompounds’’.
(4t Communication on the configuration of the ring systems).’)
By Prof. J. Borsexen. (Communicated by Prof. A. F. Honiemay).

The investigations as to the action of the polycompounds on the
conductivity of boric acid were started to furnish a contribution to
our knowledge as to the situation of the carbon atoms, and the
groups attached thereto, in benzene.

This object has been attained to a certain extent, but, in addition,
the measurements have also taught us something about the position
of the hydroxyl groups in the saturated polyvalent alcohols.

The influence of polyoxycompounds and boric acid on each other
has been known for a long time.

So, for instance, the increase of the acidic properties of boric acid
by means of glycerol was made use of in the titration of that acid
and, reversely, the large increase in rotation exerted by boric acid
on mannitol went to demonstrate that this polyatomic alcohol was
indeed optically-active *). These few empirical data were very con-
siderably added to by G. Macnanini*); at the same time an experi-
mental foundation was given to the surmise that these phenomena
might be due to the formation of compounds.

He demonstrated that mannitol strongly increased the electric con-
ductivity power of boric acid and that, although to a less extent,
this was also the case with oxy-acids such as tartaric acid, salicylic
acid, lactic acid, glycerine acid, gallic acid, mandelic acid and gly-
collie acid. He thus proved the formation of complex ions, conse-
quently of a chemical combination between the two components.

Van ’t Horr’), on account of these investigations, was of opinion

1) H. J. Waterman. These Proc. 29 June 1912, p. 124.

2) Recueil 30, 392; 31, 80 and 86.

8) Vienon. Ann. Chim. Phys. 5e S. If 433. (1874).

4) Gazz. chim. 20, 428; 21, II, 134, 215. Zeitschr. phys. Chem. 6. 58. -
») Lagerung der Atome im Raume. 3e Ed. p. 90.

217

that a compound can only then be formed when the conditions are
favourable for the formation of a 5-ring (and eventually of a 6-ring).
A substance like mannitol might then unite readily with one or more
mols. of boric acid, because the position of the hy droxyl groups would
favour the formation of 5- or 6-rings.

In the case of a hexatomic alcohol like mannitol, the conditions
for the ring formation are, however, probably favourable, because
to each carbon group is attached a hydroxyl group and because of
the very great probability that two of these with the two carbon
atoms attached thereto, are situated at the same side and in the same
plane ; and this especially because it is a saturated non-cyclic substance.

It occurred to me that a further study of the influence of these
compounds.on boric acid might become of more importance still, if
the more simple alcohols were chosen for that purpose.

Now, with the polyoxyderivatives of benzene the conditions are
exceedingly simple.

When in the benzene derivatives the six carbon atoms with the
groups attached thereto, are situated in one plane, the orthodioxy-
compounds only (eventually also the erthooxyacids have a configu-
ration that offers the best chances for the formation of the said
cyclic systems.

In fact, the measurements carried out by myself and A. vAN
Rossem (I.c.) have shown that of the polyoxyderivatives of benzene
only the orthocompounds exert a very great positive influence on the
conductivity of boric acid.

The specific conductivity of */, mol. solution of this acid at 25°
is increased :

by '/, mol. pyrocatechol from 25.7 & 10-® to 553.2 & 10—§

eee apyromaillols 22-1 we . 6608. DK AOR
Pere epyrecatechol:, 27. 2... .- . ATO Oe AO-*
eae Py ronalol 7... Oe BO | KIO
pee as. t-2-dioxynaphialene... ..- - LD Se AO *

(measured iy “Mr. J. D. Roys)

on the other hand, the meta- and paraderivatives exerted an insigni-
ficant negative influence. The spec. conductivity was lowered :

by '/, mol. resorcinol from 25.7 « 10-® to 25.0 x 10-6
a ahydrodainone. i... ..-.-., 2a dO-*
Po ee pnaroeluemol.5 9. .,.. + Ree ea Ges

Gallic acid and protocatechuic acid also suffer a considerably larger
increase in conductivity by addition of boric acid than would agree
with this acid’s own conductivity.

: 218

1/, mol. protocatechuic acid had at 25° a specitic

}

conductivity = 7031 20
1/, mol. boric acid = lola
Found a conductivity of the mixture = S47 nO s 5

Increase = 118.9 SC AO ss8

1/, mol. of gallic acid had at 25° a spec. conductivity = 750.7 K 10-®
1/, , of boric acid =~ 25.7 <i
Found for the mixture = 917 S10

Increase = 141.2 & 10-6

From this influence on the conductivity we may conclude that
with the polyoxybenzene derivatives an important reaction only then
takes place when the hydroxyl groups are situated in the ortho-
positions in regard to each other,

Of a specific aromatic influence there can be no question because
it would then be difficult to understand why resorcinol, hydroquinone
and phloroglucinol do not exert an increasing action whereas mannitol,
pentaerythrol and glycerol do increase the conductivity (MAGNANINI,
BOESEKEN and van RosseEm I. ¢.).

We are constrained, as stated above, to look for the cause in the
favourable situation of the hy —— groups in regard to the boric
acid molecule.

Now, the peculiar property of pyrocatechol and other orthodioxy-
(and also of amido-oxy and diamido-) compounds of benzene and
other ring systems to readily absorb another atom and to form with
this, as a rule, very stable compounds has been known for a long time.

This is attributed to the exceedingly ready 5-ring formation, there-
fore to the favourable position of the ortho-placed groups.

Without troubling, provisionally, about the configuration of the
compounds formed between boric acid and the polyoxyderivatives,
we may take it as very probable that an analogous cause determines
their origin.

The importance of demonstrating the influence of the polyoxy-
compounds on the conductivity of boric acid is not related to the
fact itself but lies in the sensitiveness of the method and its simple
application.

It enables us to announce the formation of compounds without
having to isolate the same and even more: from the degree of
influence we can draw important conclusions as to the position of the
hydroxyl groups im the original polyoxycompound.

If, for instance, we find that the increase of the specific conductivity
at 25° caused by:

219

=
es)
=

. glycol on~ 2 a boricsacid == GOs 10
. glycerol SSE Or ey ca na el Pek ee
PpEmeMeMAcryihrOks -y.%s5 |< caine yes. == DOLD KX 107%
P eemeperdentcebOl a! 6. 5 ses 4 SEAT OE 10-6
‘/, n. dulcitol oo 2 SSeOl Gee eee
we may conclude therefrom that in pentaerythrol, at least two of
the hydroxyl groups are situated rather favourably, but not by a
long way so as in the case of pyrocatechol; that in dulcitol more
than one pair of hydroxyl groups exert an influence on the boric
acid; that in glycol, they are very unfavourably situated and that
they are also unfavourably situated in glycerol although three of
them are present. This is shown in a still more striking manner
when we compare the trivalent pyrogallol with glycerol at a some-
what greater concentration of the alcohol:
1 n. pyrogallol on */, n. boric acid = 911.3 x 10-6
Pere: SlyCerol eee nee Eerie se La Le

In the determination of the tence exerted on the conductivity
we possess a very simple and sensitive method to get some infor-
mation as to the situation of the hydroxyl groups in regard to each
other without strongly attacking the molecule and so disturbing the
existing equilibrium.

In consequence of the preceding we submit the following suppositions:

1. If the hydroxyl groups, as in pyrogallol or in pyrvcatechol, are
situated in the same plane and at the same side of the carbon atoms
to which they are attached and if there is no entering atom as in
the case of resorcinol, hydrochinone or phloroglucinol, the influence
is very great.

2. This influence becomes less when the OH-groups are leaving
this favourable position.

The simple glycols as yet investigated by us: aethylene glycol,
pinacone, propanediol 1,3, butanediol 1,4°), do not increase the
conductivity of boric acid.

We surmise that the hydroxyl groups in these molecules repel
each other and then, in consequence of the mobility of the saturated
molecule, get situated as far as possible from each other, still in the
same plane but at the opposite side of the carbon atoms to which
they are attached.

We will see whether a more extensive experimental material
confirms these suppositions.

—

ws
=)

1) Butanediol (1.4) can be prepared very readily by reduction of succinicdiethyl
ester according to the directions given by Harries for the preparation of methyl
(2) butanediol (1.4) from pyrotartaricdiethy] ester.

Proceedings Royal Acad. Amsterdam. Vol. XV.

220

The influence of glycerol is certainly in harmony with these views.
As we have stated this influence is very slight; two of the OH-groups
are therefore, most likely, not situated so favourably as in pyrocatechol.
But still they are not situated so unfavourably as in the simple
elycols and this cannot be otherwise, for even when the three OH-
eroups repel each other as far as possible the situation of these
eroups viewed two by two must still be more favourable than in
the said bivalent alcohols.

The fact that on the other hand the position of the hydroxyl groups
in pyrocatechol and in dioxynaphtalene is so particularly favourable
must be attributed to the ring-system of the benzene, which forces
them to remain in the plane of the ring and at the same, or outer, side.

The fact that, according to MaGNANINI’s measurements, the a-oxy-
acids and salicylic acid affect the conductivity of boric acid positively,
points to a position of the hydroxyl groups, in regard to each other,
which is more favourable than in the glycols. This is very com-
prehensible when we consider that the OH-group of the a-carbon’
atom finds at the other side of the acid OH-group of the carboxyl
group an oxygen atom, and not the hydrogen atoms of the glycols.

If the number of hydroxyl groups in saturated compounds is greater
than two, it is obvious that the chances of a favourable position
increase and in harmony therewith we find that erythro] exerts a
stronger influence on the conductivity of boric acid than glycerol
and that the action of mannitol and dulcitol is more important still.

For ‘/, mol. of the alcohols on */, mol. of borie acid was found:
K > to)

Glycerol E Erythrol Mannitol | Dulcitol
8.7 | 64d ba eG Ss | 717

In the case of these saturated polyalcohols it is, at the present,
still somewhat difficult to point out the most probable position of
the hydroxyl groups by means of a determination of the influence
exerted on the conductivity.

This is much more easy in the case of cyclic systems where the
mobility of the molecule has been lessened to a considerable extent
by the closing of the ring thus causing the position of the groups
to become much more defined. We have already made use of this
property in criticising the action of the polyoxycompounds of benzene ;
but the action of sucrose is also that which may be expected from
this molecule.

221

The influence of sucrose on the conductivity of boric acid is very
trifling, and reversely, also that of boric acid on the rotatory power
of sucrose.

' 1
The change of a sucrose to = N borie acid = +0

3b4. IG
1
” ” ” 3.49 N ” ” : . : . = —- ed 10 —6
: 1 k ‘ |
” ” > rain » ” . . . . a —3x10-6

The change in the rotation for these concentrations kept below
0,13° and like that of the conductivity was exceedingly small indeed.

Pia If now we observe the subjoined symbol of

WC Soh ae sucrose in space, which is considered by

ae : Hoc , Touiens and E. Fiscuer’) as the most probable

noch / ee one, we notice that of the eight hydroxyl groups

Hc HG only those indicated by (1) and (2) can have

He oH(1) sees a favourable position, that is to say, in the
CH, 0H(2)

same plane and at the same side of the carbon
atoms to which they are attached and undisturbed by other atoms.

It was, however, to be expected that these two OH-groups will
not be situated favourably, for they possess a freedom of motion
analogous to that in the simple glycol and if in the latter the OH-
groups repel each other it would be difficult to understand why they
should not do so in the sucrose molecule.

The almost complete indifference of sucrose towards boric acid
(and probably towards many other compounds) now finds in its
configuration a very simple explanation.

These observations thus confirm the configuration of the sucrose
as well as the value of the process for the more exact determination
of the hydroxyl groups of organic compounds. I have been able to
employ the method for determining the configuration of e- and 8-dextrose.

Eee. aay ae ay
wc Sof Ko

oH(=)

It is known that the above contigurations are now imputed to
both these isomers. If this be correct they must behave differently
in regard to boric acid.

1) E. Fiscner, B 45, 461 (1912).
Lae

222

One of them, represented by (I) must, in consequence of the
favourable position of the hydroxyl groups (a) and (/), influence the
conductivity more forcibly than the other one and because in aqueous
solution they are converted into each other up to a definite equili-
brium, the conductivity must decrease until this equilibrium-mixture
is attained.

In the other represented by II the conductivity must increase
until the same limit value is attained.

The preliminary measurements executed by Mr. C. E. KLamEr now
have led to the result :

1. That a-dextrose had, at 25°, a considerable positive influence
on the conductivity.

2. That this decreased slowly so as to attain a definite limit
value after 24 hours.

3. That the positive influence of @-dectrose (up to the present
not obtained in a perfectly pure condition) was much slighter than
that of a-dextrose.

4. That it kept on increasing slowly to finally reach nearly, but
not quite, the same limit value as in the case of the «-dextrose.

After repeated recrystallisations the conductivity of a 6.5°/, solution
of a-dextrose at 25° was on an average 5 X6~-®, ofa15°/, solution
7< 10-5, that of a 6.5 °/, solution of 3-dextrose obtained by reery-
stallisation from pyridine 10><10-°, presumably it still contained
‘a little pyridine.

The increase of the conductivity caused by a

6.5 °/, a-dextrose solution on 2'/,°/, H,BO,= 42 10-6
falling to 30 xX 10-6
The increase of the conductivity eaused by a
15°/, a-dextrose solution on 2'/, °/, H,BO, = 106 & 10-6
falling to 90 >< ieee

The increase of the conductivity caused by a

6.5 °/, @-dextrose solution on 2'/,°/, H,;BO0,; = 20 10-6
rising to 29 xX 18=

Without anticipating the result of the final measurements with
the sugars we may safely conclude that this method which, of course,
is capable of extension in many directions can give us further data
as to the more delicate structure of the molecules.

In other respects also, the formation of complex compounds of
boric acid with organic polyoxycompounds is of great importance.

We know that boric acid is used as an antiseptic; this is based
on the retarding action which this substance exerts on the growth
of moulds.

According to the researches of H. J. Waterman and myself
described in these Proc. (80 Dec. 1911 and 30 March 1912)
retardation is usually associated with a strong solubility in fat or
with a too large concentration of hydrogen ions.

Now, boric acid is much more readily soluble in water than in
olive oil and is moreover an exceedingly feeble acid so that these
two properties cannot, therefore, explain to us why boric acid so
very much retards the growth of penicillium glaucum as we have
indeed observed.

The formation of compounds with the polyalcohols which play
such an important role in-the living beings, compounds which can,
moreover, be much more strongly acid than boric acid itself, offers
a very simple explanation of the powerful action of this apparently
so innocuous substance. :

Under the influence of the development of the chemistry of the
colloids, the origin of physiological processes has been perhaps
searched for a little too much in purely physical phenomena: diffu-
sion, change in surface tension, discharge of negative-charged colloids
by positive ions and reversely, etc. Undoubtedly, all these actions
play an exceedingly important role, but in many cases a chemical
phenomenon is involved; it is like this with boric acid and so it
will be, presumably, with the toxic action of many metals (I further
refer to a communication from H. J. WarrrmMan and myself in the
“Folia microbidlogica’’).

The question whether the strong action of some of the hydroxyl
compounds is associated with an easy ring formation, as surmised
by van ’T Horr, has, as yet, been discussed by me only casually.

Last year, Fox and Gaver (Trans. Chem. Soc. 1911, 1075) have
succeeded in isolating mannitoboric acid and in preparing some of
its salts, but as it appears from the analytical figures that there is
present one molecule of water in excess of that required for the
5-ring closure, the configuration still remains uncertain.

As pyrocatechol causes a very strong increase of the conductivity
I have endeavoured to obtain pyrocatecho-borie acid. Although we
have not succeeded in doing so, we have yet managed to prepare
a series of readily crystallizable complex salts some of which are
characterised by a very slight solubility, so that they may, presumably,
serve for the quantitative separation of boric acid.

A full description of these salts, also of the experiments mentioned
above, which have been carried out mainly by Mrs. N. H. Stewerts
VAN Rexsema, C. EK. Kuamer and J. D. Ruys, will be given later.

Delft, May 1912. Org. Chem. Lab. Techn. High School.

224

Geology. — G. A. F. Mo.encraare: “On recent crustal movements
in the island of Timor and their bearing on the geological
history of the East-Indian archipelago.”

The occurrence of elevated coralreefs on the islands of the eastern
portion of the Kast-Indian archipelago, amongst others on the island
of Timor, has attracted the attention of many scientists, because it
proves that in a geological sense not long ago, these islands have
been considerably raised above the level of the sea.

The ‘Timor-expedition*) particularly studied these elevated reefs
and their results may throw some light on the question of the
character and correlations of the recent crustal movements in the
East-Indian archipelago.

The following brief remarks, therefore, are intended as introduction
to the history of these reefs.

The strata of the island of Timor were greatly folded at a time,
which is known to be post-eocene and pre-pliocene, but which cannot
at present be more precisely defined. Among these strata besides schists
of unknown age various formations ranging from the Permian to the
Eocene are represented, the whole of which will be here indicated by
the name of the Perm-Eocene-series or simply as the older formations.

This period of folding and tilting was most probably followed by
a period of prolonged and considerable denudation, because it is
observed that a later-tertiary formation of neogene age is found
resting unconformably on the much denuded (peneplainized) older
formations. The oldest strata of these neogene deposits consist of pure
Globigerina-limestone, a pelagic sediment devoid of the elements of
terrigenous origin, which must have been formed in an open sea
far distant from the land.’)

From the time of deposition of the Globigerina-limestone important
crustal movements had set in, which resulted in the forming of basins
graben), in which the soil was deposited slowly but continuously
and thus filled up these true depressions *).

‘) Messrs. H. A. Brouwer, F. A H. WeEcKHERLIN DE MAREZ OYENS and the
author as leader, formed the Timor-expedition, during which geological explora-
tions were made in the eastern half of the Netherlands-Timor in the years 1910—1912.

2) | am not inclined to regard this formation as a deep sea deposit, although
it must have been formed in the open sea far from the land, but believe, that it
may have deposited under similar conditions as the white chalk of Europe, to
which this late-tertiary Globigerina deposit bears petrologically a remarkable resem-
blance.

3) Only the most important of those graben or depressions, which have been
of such vital importance in the development of the later-tertiary deposits, are
mentioned in this paper.

As the German terms “graben” and “horsten” are frequently used in this paper,

225

Beyond the “graben”, in the adjoining ‘‘horsten’’, a slow upheaval
of the: land took place, in consequence of which the sea became
shallower thus causing the growth of coralreefs upon the Globigerina-
limestone. Foraminifera are found abundantly in these reefs whose
preliminary determination points to a probable miocene age, although
such an assumption must be confirmed by further palaeontological
examination. Sometimes small pebbles are found in these reefs and
in places thev pass into littoral conglomerates. It appears that coral-
reefs have been formed continuously during the long period of slow
upbeaval of these “horsten”. So in proportion to their age so they occur
at different levels, the oldest or first formed lying in the highest
level, those which are younger gradually somewhat lower. These reefs
therefore form together a slowly sloping more or less terraced covering
or coating of coral-limestone. The entire thickness of this neogene
formation from beyond the basins does not exceed 60 Meters.

Inside the “graben”? where the neogene beds attain a much greater
thickness, elements of terrigenous origin make their appearance in
the upper portion of the Globigerina deposit and gradually it passes

ee ae hve OE = = es

Fig. 1. Sketchmap showing the area covered by the later-tertiary
deposits in Middle-Timor. Scale 1 : 2.560.000

f-—-

it may be as well to explain that in case adjoining strips of land are affected by
antagonistic movements and are separated one from the other by faults, the down-
thrown strips or blocks are called “graben”, whereas the upthrown strips or blocks
are called “horsten”’.

226

into a sandy limestone, or even into a grit with calcareous cement,
Thus the influence of land gradually increases and the higher strata
consisting of marly claystones and marly sandstones are observed to
contain numerous shells of the zone of shallow water which are
regarded as of pliocene age *)

The above-mentioned basins or “graben” trend in a direction
approximately parallel to the longitudinal axis of the island of Timor
(fig. 1). In a portion of Middle-Timor, as e. g. between Kapan and
Niki-Niki, one single undivided ‘graben’ exists which might be
termed the median neogene basin, although generally, the structure
of the “graben” is more complicated being subdivided by ridges
(“‘horsten’”’) or islands of older formations, which are elongated as
well in the direction of the longitudinal axis of the island. Thus in
the eastern portion of Middle-Timor the later-tertiary basin is divided
by the Mandeo-mountains into two troughs, the Talau-Insana-basin and
the Benain-basin *), while the latter more to the West again is sub-
divided by a narrow ridge of older formations into a northern Benain-
Noilmoeti-basin and a southern Noil Lioe-basin. Faults of considerable
character occur at the walls of the “graben”, which by their influence
have caused the younger tertiary strata in the basin to become suddenly
curved and bent upwards near the edges. In many places a crush-
breccia is found between the older formations and the tertiary strata
thus indicating the position of these marginal or lateral faults.

During the formation of these “graben” by the slow subsidence
of their deposits they remained always fairly well filled up with an
accumulation of late tertiary sediments, from the character of which
it may be gathered that the sea, although having occupied those
basins, never attained a great depth.

These late-tertiary strata besides being tilted near the walls of the
“oraben”’, also show in places slight disturbances. The entire thickness
of this formation in the “graben” is unknown although in my
opinion in the Benain-basin it may safely be estimated at more than
500 metres.

True littoral formations such as conglomerates, oysterbanks, coral-
reefs, ete. lie directly upon these pliocene deposits, and their thickness
is at least 200 metres in the central axis of the larger or Benain-

1) The pliocene age of these deposits is proved by MARTIN, who has examined
the fauna of the marls of Fulumonu in the Talau-basin, which is identical with
the fauna of the fossiliferous strata in the basin of the Benain. K. MARTIN. Tertiaer
von Timor. Beitrige zur Geologie Ost-Asiens and Australiens. Serie I, Band III,
p. 305, Leiden 1883—1887.

*) These two basins are united again West of the Mandeo-Mountains.

227

“oraben”. One of the coralreefs in the Benain-basin (fig. 2) is of
great thickness (70 Meters) and of considerable extension, being con-
sequently an element of importance in the configuration of the land-

Fig. 2. Section across a portion of the Benain-basin in Middle-Timor.

Claystone and marl! with shells, Pliocene.
Marls and sandy marls, containing in places marine organisms,
. Conglomerate.

. Sandy marl with Placunna.
. Coralreefs, Jate-Phocene or Pleistocene.
. Oysterbanks.

Seale. 1 : 14.000. Altitudes in Metres above sealevel.

o> or

‘
scape; on these coralreefs is again deposited a succession of layers
of sandstone, conglomerates, oysterbanks, etc., all significant of a
littoral origin. From tbeir considerable thickness we must infer that
these deposits were formed during a period of slow subsidence, which
must have occurred at the end of the pliocene or at the beginning
of the pleistocene age.

These reefs and other littoral deposits although getting thinner
towards the edges (walls) of the basins, are not always confined to
the “graben”, but in places they spread over a great area in Middle-
Timor and overlap the older formations from which they are often
separated by a well developed coarse basal conglomerate ; conse-
quently they are also found resting unconformably upon the Globi-
gerina-deposits where the latter are locally tilted at the edges of the
“oraben’. It is obvious that these coralreefs of late-pliocene or
early-pleistocene age have been formed outside the ‘“‘graben”’ in close
proximity, although generally at a somewhat lower level, to the
above-mentioned older reefs of probable miocene and pliocene age.
It was not proved possible to discriminate in the field between these
reefs of different ages, with certainty, but probably a future exami-
nation of the Foraminifera contained in them may lead to more
accurate results.

In the “graben” there is no break in the succession or unconfor-
mity visible between the pliocene strata and the overlying reefs and

228

littoral deposits; and there can be no doubt that the last mentioned
reefs both inside and outside the “graben” all belong to one and
the same continuous formation, the connection of which has only
been interrupted by later erosion.

During and just after the formation of these coralreefs a great
portion of Middle-Timor must have been covered by a sea full of
coral-islands and reefs. The higher mountain-groups ,Moetis, Lakaéan,
Mandeo etc.) emerged as islands from this sea, and the conglome-
rates, formed simultaneously with and_ posterior to the coralreefs,
prove that the islands must have been steep and high and that the
running water must have transported a considerable amount of debris
from them towards the surrounding sea.

It may be accepted that the majority of the big coralreefs were
thus formed in late pliocene or early pleistocene times as they overlie
and clearly therefore indicate a younger age than the marls with
pliocene shells.

Further, as these reefs were already formed, a general upheaval
of the island of Timor took place which possibly still continues.
This upheaval, however, was not equally strong everywhere, conse-
quently the elevated coralreefs are no longer found in a horizontal
position but feebly sloping. .

It appears that the upheaval of the central portion of the island
has been from the beginning somewhat stronger than that of the
southern and northern coastal regions.

In fact the reefs of the Diroen-ridge south of the Lakadn near the
central axis of the island occur now at an altitude of 1283 Meters,
about 680 Meters higher than those on the hills of the north coast
at Babilo. The big reef also of the Gempol-cliff in the central portion
of the island not far from Kapan has an altitude of 1250 Meters
above sealevel, whereas in the southern mountainranges near Niki-
Niki the highest altitude at which coralreefs are found is only
750 Meters.

Moreover, the upheaval of the land has been stronger at the edges
of the basins (‘‘graben’’) than in the basins themselves. Consequently
the coralreefs which rest on the pliocene strata in the “graben” are
no longer found in their original horizontal plane of deposition, but
assume a feebly basin- or trough-shaped position and are besides
split up into blocks of slightly different altitudes. If may be that this
latter circumstance is caused by compression and the squeezing out
of the soft and more or less plastic plivcene strata underlying the
heavy compact coral limestones, although it might just as well be
suggested that it is caused by a feeble continuation of the crustal

229

movements which had been present to account for the formation of the
pliocene ‘“‘graben” and “horsten’’.’)

During the prolonged period of recent upheaval the running waters
were obliged to cut their courses with strong and increasing gradients.
Narrow deep valleys, often true gullies (caions) were formed which
are characteristic of the topography of the greater part of the island.
Numerous terraces are tound along the courses of the rivers as well in
connection with those rivers which have developed their systems within
the late-tertiary basins, as also with those, where the systems lay entirely
outside of the basins. This proves that the entire island of Timor took
part in the recent upheaval, although not everywhere to the same extent.

This unequal or differential upheaval of the land has caused the
rivers which flow within the tertiary basins to generally transverse,
somewhere in their course, one or more of the strong layers of reef-
limestone, at those places where those are comparatively little elevated.
Thus the Benain has, in the central portion of the Benain-basin near
the native village Neke, at an altitude of 296 M. cut a narrow deep
gorge of more than two miles in length through a thick stratum of
coral limestone. In one portion of this gorge the running water
undermined a portion of the coral limestone, and thus formed over
the current, which is very deep and strong a natural arch or bridge
which is now a much frequented road of communication.

1) My conclusions differ slightly from those of VerBeeK (R. D. M. VerRBEEK,
Molukkenverslag. Geologische verkenningstochten in het oostelijk gedeelte van den
Ned. O.-[. Archipel. Jaarb. van het Mynwezen XXXVII. Batavia 1908). According
to VERBEEK the coralreefs of the Talau-basin are of different age, and were all
formed during the gradual upheaval of the land as fringing reefs, which are now
found to be the older because of their higher level above the sea (lc. p. 777).
The highest, those of the Diroen-ridge at an altitude of 1283 M. above sealevel
are regarded as of miocene age, those of Lahoeroes at an altitude of 569 M. of
somewhat later date, and the lowermost, those of l’atoe Lamintoetoe at an altitude
of 300 M. of pliocene age. These coralreefs diverge the older they are proportionally
more from their original horizontal position; thus the oldest show a dip of 89,
those which are at a lower level of 5°40’, whereas those which occur still further
below dip only 3°50 (l.c. p. 357 and p. 778).
Although admitting that outside of the ‘“‘graben’’, coralreefs of probably miocene
age are found and that these ancient reefs occupy the highest levels now, I am
of opinion that the majority of the elevated reefs i.e. the bulk of those which
occur within the area of the “graben” including the Talau-basin, and also a part
of those which are situated beyond the limits of the ‘‘graben”, were formed before
the commencement of the latest period of emergence (upheaval) of the island of
Timor and consequently must be of the same late-pliocene or early-pleistocene
age; and the above mentioned, feebly synclinal and somewhat disturbed and frac-
tured position of the reefs, which spread continuously over large distances within
the “graben”, would be an explanation for the fact that these reefs are found
at present in different altitudes, decreasing towards tbe central axes of the “grapen”’.

230

In the same way the Talau-river just below its confluence with
the Baukama at an altitude of 245 M.*) above sea-level, has cut a
gorge which at present is 55 M. deep, across a high bank of coral
limestone.

Theoretically one might expect, that during this prolonged period
of upheaval, which possibly is still in progress, a series of fringing
reefs had been formed all round the area of elevation. The current
opinion is, of course, that the elevated coralreefs of Timor were
formed in such a way from miocene times until now, during a
continuous movement of upheaval of the land ’). The fact is, however,
that not a trace of elevated fringing reefs is found along the
north western and southeastern coast, where the island of Timor
adjoins the eastern continuation of the deep depression of the Savoe-
sea and the equally deep depression of the Timor-sea. The western-
most portion of the island, on the contrary, where it borders the
shallow water which separates it from the island of Rotti, is covered
with elevated fringing reefs.

If we look for an explanation of this remarkable fact, it is of
importance to bear in mind that the island of Timor appears to be
suddenly truncated and broken off by faults just along the north-
western and southeastern coasts which border deep basins of the sea
coming up close to the shore.

The late-tertiary or early-quaternary reefs and littoral deposits which
form the uppermost portion of the neogene series of the Talau-basin,
on the mountain-ridge of the northcoast for instance near Babilo,
abruptly terminate with their full thickness in a steep cliff, facing
the sea at an altitude of about 610 Meters. Evidently the strata
once extended much further towards the North, but afterwards
became detached. Between this point and the actual coast no trace
of elevated coralreefs is found, whereas at the beach in the surf
small reefs of living corals are abundant. This circumstance as well
as the fact that along the north coast the hills rise with an un-
commonly steep slope from the sea, tends to prove that the island
of Timor is broken off towards the North. More convincing evidence
still, is afforded by the south coast, where in the district of Amanatan
the parallel ridges of the Amanoeban-mountainchain, which is mainly
composed of Jurassic strata striking OLON-W105 (a direction differing
about 12° from the general trend of the coast line), follow each other
abruptly abutting against the coast and terminating in high cliffs.

1) VERBEEK, in his description of the tertiary basin of the Talau-river, also
mentions this gorge l. c. p. 348.
*) R. D. M. Versegx, |. c. p. 777.

231

The sea deepens suddenly all along this coast and no trace of islands
or shoals are found which might be regarded as the submarine
continuation of those ridges. All observatidns made along this coast
give support to the opinion that the island terminates here against
a fault facing the Timor-sea.

I think it quite possible that the faults which thus terminate the
island of Timor both towards the North and the South have been
the cause of the absence of elevated reefs along those coasts of upheaval.

If we accept the existence of these breaks, the question arises:
What has been detached towards the North and the South? Clearly
it must be the sunken blocks of land which are found in the deep
basins of the Timor-sea and the Savoe-sea.

To the North of the island of Timor the eastern continuation of
the Savoe-sea has a depth of 3255 M. near the island of Kambing;
to the South the depth of the Timor-sea is 3109 M. and this con-
siderable depth is found much nearer to the coast of Timor than to
the Sahul-bank which forms part of the continent of Australia.

Not only Timor, however, is thus bordered at both sides by deep
sea-basins, but it is a coincidence which holds good for the majority,
if not for all of the islands of the eastern portion of the archipelago,
consequently, the origin of the deep sea-basins and the elevation of
the islands in the eastern portion of the archipelago may be regarded
as a simultaneous process between which a genetic connection must
have existed.

The genesis of adjoining sunken and tilted blocks must be the
result of one and the same crustal movement, which in my opinion
would be the cause of a process of folding at great depths.

If the question were raised as to what might be seen at the earth’s
surface if an area were folded by crustal movement at a certain
depth, I should be inclined to reply that its appearance would be
similar to what obtains at present in the eastern portion of the Indian
archipelago '). It is a well known fact that the folding of rock-strata
is only possible under high pressure; it may therefore be inferred
that folding can only originate at certain depths below the earth’s
surface. At the surface, in the zone of fracture, where the rocks
cannot be plicated, the phenomena of deeply seated thrust and folding
would be indicated by the presence of “graben” and “horsten”, the
former corresponding to the troughs, the latter to the saddles of
the deeply seated folds. Generally speaking every range of tilted

1) ABENDANON has arrived at a somewhat similar conclusion, in his analysis of
the topography of the island of Uelebes. E. G. ABbenpanon, Celebes en Halmaheira,
Tijds. K. Ned. Aardr. Genootsch. 2, XXVII. p. 1149, Leiden 1910.

232

blocks, or islands in our case, as well as every range of sunken
blocks, or deep sea basins in our case, must indicate the position
and the trend of the major folds, which ure in mode of formation
at a certain depth; thus the character of the deeply seated folds
would be found reflected in the surface topography.

But then one has to take into account also, the submarine topo-
graphy ') and fortunately the excellent deep sea chart of the Siboga-
expedition enables us to do this *).

The most salient feature on this map is the striking difference
which exists between the western portion (the Java-sea and _ its
surroundings), and the eastern portion (the Molucca-sea). The latter
exhibits a complicated topography and great variations both in the
depth of the sea and in the heights of the numerous islands, which
generally emerge boldly from the sea; whereas the western area
shows a slight and very uniform depth of the sea and smooth out-
lines of land which rises with a very gentle slope from the coast °).

1) In my opinion it is imperative to study the submarine topography, because the
part of the surface of the earth hidden beneath the sea in this archipelago is so
much greater than that of the islands. This itself is a favourable circumstance,
because it tends to prove, that the basins until now were comparatively little
filled up by products of erosion brought from the land, and consequently the
surface topography originated by the recent crustal movements has been fairly
well preserved at the bottom of the sea. The upraised islands of course are
smaller and less high now than they would have been, were it not that the
erosion had from the start counteracted the results of the upheaval. In or near
large continents the chances for the preservation of a salient topography are
much smaller, because the original features would have been much sooner oblite-
rated by the effects of erosion and sedimentation. Thus in a portion of Northern
Germany 2nd the Netherlands, geologically not long since, crustal movements
formed a surface topography, certainly not less complicated than that of the East-
Indian archipelago, in which the levelling processes have been so powerful, that
its original topographical details has become obliterated, with the result that at
present only a trace of them can be seen at the surface; indeed we have to
imagine the quaternary and a portion of the tertiary deposils removed to be able
to realize tle complexity of this topography. ~

*) G. A. F. Typeman. Hydrographic results of the Siboga-expedition. Chart 1.
Part Ill of M. WeBer. Siboga-Expeditie. Leiden 1903.

Soundings which have been made in the archipelago since the results of the
Siboga-expedition were published, have proved, that the submarine topography is
still more complicated than that shown on the chart. Very probably, the most
important result of the researches of the Siboga-expedition i. e. the existence of
a strikingly complicated submarine topography in the eastern parts of the Kast-
Indian archipelago, wil! be more accentuated by future researches.

3) VERBEEK has already drawn attention to this striking difference between the
western and the eastern portion of the archipelago and he pleads a causal origi-
nation for the presence of the deep sea-basins and the islands with elevated

233

This western portion with the tranquil topography both of the land
and the sea-bottom, has not taken part in the more recent crustal
movements ; since the upheaval which raised the miocene sandstone
formation in Central-Borneo to a level of more than 1000 M. above
the sea, no movements of the soil have been recorded there, probably
with the exception of the area immediately bordering the Street of
Macassar. In the eastern portion of the archipelago, where a com-
plicated topography of the land and the sea bottom prevails, deep
sea-basins have been formed by subsidence; and, during the same
time, ranges of islands have been elevated above the sea, caused by
antagonistic movements which are probably still in course of progress.
It thus appears that in the latest geological period the crustal move-
ments, im the geosynclinal ov movable area between the Australian
and the Asiatic continent, have been confined to the portion, immediately
adjoinina the Australian continent, t.e. between Borneo and Australia.

In tropical regions generally, a coating of coral-limestone is formed
along an elevated coast, as long as there are no causes to counteract
or annihilate the results of the growth of successive fringing reefs
during the period of upheaval.

This easily recognisable coating of coral-limestone (series of fringing
reefs in different levels one above the other) in tropical regions,
affords an excellent criterion from which may be judged whether a
coast has been elevated in proportion to the level of the sea.

Now in the entire western portion of the archipelago with its
undisturbed topography i.e. the land surrounding the Java-sea where,
according to my opinion, no movements of the land in relation to
the level of the sea have taken place in the latest geological time,
raised coralreefs have not been recorded °).

In the eastern portion of the archipelago with its complicated
topography, where crustal movements have occurred, elevated coral-
reefs are found on the great majority of the islands.

L believe, that generally speaking it may be accepted, that where
coralreefs (l.c. p. 817). VERBEEK, however, believes in an indirect cause for such
a phenomenon. In his opinion the upheaval of the islands took place only after
the deep sea-basins had already been formed, by the subsidence of landmasses ;
pressure exercised by the sunken blocks caused later folding at a great depth, as
well as the upheaval of the islands (l.c. p. 816). In my opinion, however, the
causal origin was of a direct nature; the subsidence of tlie deep sea-basins
and the elevation of the islands took place at the same time, and both anta-
gonistic movements were the resulls of one and the same phenomenon of thrust
and folding at a certain depth.

1) Java, especially the southern coast, would have been subjected again to the

crustal movements, which had occurred at the border belween the Indian Ocean
and the Kast-Indian archipelago.

234

a deep sea chart shows a complicated topography the adjoining
coasts must show signs of upheaval (in tropical regions, as a rule,
elevated coralreefs), and where this ts not the case one must expect
no evidence of importance in favour of the upheaval of the adjoining
coasts.

If my suggestion is correct that folding at a certain depth is the -
cause of the simultaneous origin of both deep sea-basins and the
elevation of the islands, the followmg phenomena would result:

1. The elevated islands would be grouped in rows, for they are
nothing but the elevated though fractured strips of land on top of
the saddles of the deeply seated folds. The trend of the rows of
islands would indicate the line of strike of such folds, examples of
which may be seen in the rows at Soemba-Timor-Timorlaut-Kei-
Ceram-Buru; as also at Soembawa-Flores-Wetter -etc.

2. The deep sea-basins would be elongated in one direction more
or less exactly parallel to the adjoining rows of islands, because
they are formed on top of the troughs of the deeply seated folds.
For example I may quote the case of the Savoe-sea, the depth near
the island Kambing, the Timor-sea, the Weber-depith, ete.

3. Near the surface, in the zone of fracture, one would also expect
.to find faults, which had broken the connection in the sides of the
folds. Such faults would exist between the deep sea-basins and the
elevated islands; and where the faults had repeatedly cut away the
land at the coast, the development of elevated fringing coralreefs
would have heen hampered. This has taken place both at the north
and the south coast of the island of Timor, and also at the islands
of Moa and Leti. |

4. All the islands of one row would be elevated, but the upheaval
would have been very unequal, as can be observed if tbe islands
are compared one with the other, or if an examination be made of
different portions of one island. This is indeed the case in all the
elevated islands, as can be principally deduced from the desriptions
in VERBEEK’s Molukken-verslag.

5. There is no reason why faults should occur between adjoining
islands belonging to one and the same elevated range (saddle of a deeply
seated fold), which would hamper the development of elevated
coralreefs. It is possible that this circumstance might explain why,
at the western extremity of Timor, elevated fringing coralreefs
appear to be so well developed.

6. Where the deeply seated fold, shows sudden bends or curves,

235

or where two systems of folds interfere’) exceptions to the above
mentioned rules and complicated cases may be expected. The deep
sea chart of the Siboga shows good examples of this fact.

Zoology. — “On the Freshwater Fishes of Timor and Babber.” By
Max Weber and L. F. pr Beavrort.

The Timor Expedition, under leadership of Prof. G. A. F. Moen-
GRAAFF, returned to Holland with extraordinarily rich mineralogical,
palaeontological and geological collections and its leader has already
communicated some important preliminary results, which are of great
importance, not only to our knowledge of Timor, but also to the
geological history of the whole indo australian archipelago. As they
throw new light on the youngest phases in the development of the
archipelago, they are of special importance to the zoogeographer too.

Therefore it is a memorable fact, that Prof. MoLENGRAAFF consented
to our request to make a collection of freshwater fishes, when
time and circumstances permitted, as thus important light is thrown
on at any rate the younger phases of the evolution of the indo-
australian archipelago.

We are glad to seize this opportunity to thank him as well as
his collaborator Mr. F. A. H. Weckoeriin pE Marez Ovens for the
collection of well preserved specimens of fish, brought together by
the lastnamed in different rivers of Timor and the island of Babber.

As far as we know, Babber was — ichthyologically — a terra
incognita. The following fishes were collected by Mr. W&cKHERLIN
pE Marez Oyens in the rivers (Jer), which are mentioned next to
the name of the fishes.

Anguilla mauritiana Bunn. Jer Lawi, 7 Km. above mouth. Jer
Toilila near Tepa, 500 M. above mouth.

Caranx carangus Bu. Jer Lawi, 7 Km. above mouth.

Gymnapistus niger C. V. Jer Lawi, 7 Km. above mouth.

Eleotris gyrinoides Buxr. Jer Toilila near Tepa, 500 M. above
mouth. Jer Lawi, 7 Km. above mouth.

1) The East-Indian archipelago is situated in the area of junction of two systems
of folding of the earth’s crust, the alpine and circumpacific system, vide E. Have.
Les géosynclinaux et les aires continentales. Bull. de la Soc. Géol. de France.
1900. 8. Sér. Vol. 28 p. 635. Whereas E. Haue refers in this area to an “embran-
chement” of the two systems, SARASIN goes further and speaks of an actual conflict:
“Ich habe noch immer den Eindruck; dasz es sich im malayischen Archipel um
einen Konflikt zwischen den Kettensystemen der Tethys und denen der pazifischen
Umrahmung handle’. P. Sarasin. Zur Tektonik von Celebes. Monatsberichte der
deutschen Geol. Ges. 1912. p. 215.

Proceedings Royal Acad. Amsterdam. Vol. XY.

236

Eleotris (Culius) fusca Bu. Jer Toilila near Tepa, 500 M. above mouth.

Eleotris (Belobranchus) belobranchus’ C. V. Jer Lawi, 7 Km. above
mouth.

Gobius spec. Jer Toilila near Tepa 500 M. above mouth.

Sicyopterus micrurus Burr. Jer Lawi, 7 Km. above mouth. Jer
Toilila near Tepa, 500 M. above mouth.

Sicyopterus cynocephalus C. V. Jer Lawi 7 Km. above mouth.

On the fishfauna of Timor BLEEKER') wrote 7 papers between the
years 1852 and 1868. There is not much to be learned from them
for our purpose, however. Any exact account of the localities
where they were taken, is lacking. Doubtless by far the greater
part was captured in the litorai waters of Kupang and Atapupu. The
following 7 only are specially recorded from a river near Deli:

Megalops indicus C. V. = Megalops cyprinoides Brovss.

Anguilla austrahs RicHarps.

Atherina lacunosa Forst. = Atherina Forskali Ropp.

Mugil brachysoma C. V. = Mugil sundanensis Bur.

Acanthurus matoides C. V.

Caranz forsteri C. V.

Eleotris Hoedtiu Bur.

The locality and the nature of the fishes make it probable, that -
they were caught not far from the mouth of the river:

In 1894 the first named of us*) published a more extensive list of the
fishes of Timor, chiefly due to Prof. A. Wichmann, who was kind
enough, during his stay in Timor in the spring of 1889, to collect
the following fishes in the river Koinino and other small streamlets
in the neighbourhood of Kupang, as well as in the river near Atapupu.

Mugil (Bleekeri Grur.?) river Koinino.

Kuhlia marginata C. V. river Koinino.

Ambassis buroensis BuKR. river near Kupang.

Ambassis batjanensis Bukr. river Koinino.

Therapon jarbua Forsk. river near Kupang.

farane hippos li. river near Kupang.

Eleotris hoedti Bukr. river near Atapupu.

Eleotris fusca Bu. Scan. river near Atapupu.

Gobius celebius C. V. rivers near Kupang.

Gobius melanocephalus Bukr. river Koinino.

Ibid. XIII, 1857. p. 387-390. Ibid. XVII, 1858 p. 129—140. Ibid. XX, 1859. p. 442—
445. Ibid. XXII, 1861, p. 247—261. Ned. Tijdschr. Dierk. I, 1863, p. 262—276.
2) Max Weser. Zool. Ergebnisse einer Reise in Niederl -Indién. ITI, 1894. p-433.

237

Then Dr. H. ren Karr collected a few freshwater fishes, which
have been published by Dr. C. L. Revvens'). These are:

Anguilla bengalensis (Gray) Gthr. = Anguilla mauritiana Benn.
from a Jake near Baun.

Anabas scandens Dald. near Amarassi and from lake Nefko near
Oikaliti. ’

Lastly Mr. H. A. Lorentz was kind enough to collect in August
1909, when passing Kupang on his way to New Guinea, the following
fishes from the river Koinino:

Eleotris (Belobranchus) belobranchus ©. V.

Gobius celebius C. V.

Gobius melanocephalus Burr.

The great value of the fishmaterial collected by the Timor expedition
lies in the fact, that it comes from the interior of Timor, far away
from the sea, and from altitudes varying between 200 and 900 M.
It gives a picture of the fishfauna in the upper course of the rivers,
while the previously known material came from the lower course
of the rivers. The collection consists of the species mentioned below,
from the following localities:

1. Mota Berluli, District Djenilu, Belu, 1 Km. above mouth.

2. Noil Enfut (= Noil Mauden) between Wikmurak and Oi
Lollo, District Insana, area of the river Noil Benain, about 200 M.
above sea.

3. Area of the river Mota Talan, from streamlet without name near
camp Naitimu, Belu, about 250 M. above sea.

4. Noil Bidjeli (= Noil Noni!, near camp bidjeli, upper area
of the river of Noil Benain, District Mollo, about 350 M. above sea.

5. Noil Aplaal (= Noil Besi), near camp Aplaal, District Miomaffo,
about 500 M. above sea.

6. Noil Besi near path from Fatu Seinaan to Bonleo, about 900 M.
above sea.

7. River Bele, near the source of the river Noil Tuke, District

Amanzebang, about 700 M. above sea.

Anguilla mauritiana Brxn., Noil Besi, River Bele.

Anguilla celebesensis Kaur, River Bele.

Aplocheilus celebensis M. Wes., Area of the river Mota Talau.
Mugil spec. Mota Berluli.

Aeschrichthys Goldiei Macuray, Noil Bidjeli.

Kuhlha marginata C. V., Noil Bidjeli, Noil Aplaal.

1) C. L. Revvens. Fresh and brackish water fishes from Sumba, Flores, Groot-
Bastaard, Timor, Samaoe and Rotti. Notes Leyden Museum XVI 1895, p. 154.
16*

Mugil spec. juv.

In Timor. ers
eas Si = ® hae :
= 2 ou Distribution outside
a. eye Gh eee Timor.
pot |N co)
Seat $1 Be
< as ies | =
Megalops cyprinoides Brouss. 5" — tees Indopacific.
Anguilla celebesensis Kaup — + Eastern part of indo-
australian Archipelago to
| | = Fe Westpacific islands.
illa mauritiana Benn. — + |\\g 2 From East Africa to
ae ag F a 3 Westpacific islands.
A illa australis Richards. oe _ ~4 From India to Australia
aa and New-Zeeland.
Aplocheilus celebensis M. Web. _ + no Celebes.
Atherina Forskali Riipp. os — yes From Red Sea to West-
| pacific islands.
get == = =
Mugil (Bleekeri Gthr.?). = + brackish} Banka, Aru-islands.
water
Mugil sundanensis Bleeker +. yes Indo-australian Archi-
| pelago.
Aeschrichthys Goldiei Macleay — + no South New Guinea,
| | Philippines.
Anabas scandens Dald. a | + no From Ceylon through
| indo-australian Archipel.
| to Halmahera and Batjan?
Kuhlia rupestris C.V. ae | no From East Africa to
| Westpacific islands.
Kuhlia marginata C.V. = + | yes Indo-australian Archipel.
to Westpacific islands.

- Toxotes jaculator Pall. + = no Indo-australian Archipel.
Ambassis buroensis Bleeker = +- yes Indo-australian Archipel.
Ambassis batjanensis Bleeker — aca) aves Indo-australian Archipel.
Lutjanus fuscescens C.V. oe +. brackish Indo-australian Archi-

water ,pelago to Westpacific
- islands and China.
Therapon jarbua Forsk. ios + yes | Indo-pacific.
Therapon cancellatus C.V. — + yes Indo-australian Archipel.
Acanthurus matoides C.V. ae — yes Indo-pacific.
Caranx forsteri C.V. == = yes Indo-pacific.
Eleotris Hoedti Bleeker ae + brackish) Brackish and freshwater
water | from India to Westpacific.
Eleotris belobranchus C.V. oe + |brackish) Brackish and freshwater
| water | of Indo-australian Archip.
Eleotris fusca Bl. Schn. — + |brackish| Brackish and freshwater
water | of Indopacific.
Eleotris gyrinoides Bleeker — 4+ |brackish| Brackish and freshwater
| water |of Sumatra and Celebes.
Gobius celebius C.V. = oe yes Seas and rivers of Indo-
australian archipelago.
Gobius melanocephalus Bleeker — a yes Seas and rivers of India
and Indo. australian Archi-
pelago.
Sicyopterus Wichmanni M. Web. _ + no Flores.
Sicyopterus cynocephalus C.V. — + [pet RO, Indo-Australian Archipel.

239

Kuhlia rupestris Lacke., Noil Aplaal.

Lutjanus fuscescens C. V., Mota Berluli.

Therapon cancellatus C. V., Noil Aplaal.

Eleotris (Ophiocara) Hoedti Buxr., Mota Berluli. :

Eleotris gyrinoides Buxr., Mota Berluli, Noil Enfut.

Gobius celebius C. V., Mota Berluli.

Gobius melanocephalus Brkr., Mota Berluli, Noil Enfut.

Sicyopterus cynocephalus C. V. Noil Enfut, Noil Besi.

The zoogeographical importance of all the species hitherto known
from the freshwater of Timor will be more pronounced in a table
in which is mentioned at the same time whether the species are known
to inhabit the sea, in which case it is proved that salt water does
not constitute a barrier against their distribution. Furthermore the
distribution of the mentioned species is noted in our table.

From this table the following may be deduced:

1. Contrary to expectation Timor misses every australian or papuan
element in its freshwater fishfauna. We mean by that the JJelanotae-
niidae, which are only known from Australia, New Guinea, Waigeu
and the Aru islands and which are still represented on lastnamed
islands by Pseudomugil and Rhombatractus, and further such forms as
Neosilurus, Eleotris aruensis M. Wes., E. Mertoni M. Wes., FE. mogurnda
RicHarps, which are also found on the Aru islands.

2. On the other hand a few fishes: Anabas scandens Daup. and
Aplocheilus celebensis M. Wes., occurring in the freshwater fauna of
Timor, are forms which are entirely lacking in the freshwater of
the australian or papuan region.

3. The most striking fact however is, that 15 of the 28 enumerated
species occur as well in the sea, temporarily (Anguillidae) or perma-
nently, and 6 of them also in brackish water. The 7 remaining are
hitherto only known from freshwater. From these 7 Aeschrichthys
Goldiet Macu., Kuhlia rupestris C. V., Sicyopterus Wichmanni M. Wes.
and Sicyopterus cynocephalus C. V. are closely related to forms for
which salt water, or at least brackish water does not form a hindrance
in their dispersion.

In other words the freshwater fisbfanna of Timor has a marine
character, it is almost totally composed of immigrants from the sea.

This very remarkable phenomenon can be explained by what the
geological history of Timor teaches, as conceived by MOoLENGRAAarr.
To us the following is of importance.

Timor was covered by sea during a very great part of the pleisto-
ceen. The high mountains however (Mutis, Lakaan etc.) projected
above the sea. They must have been comparatively high at that time

240

too, as the water, running in torrents from their sides, carried down
much gravel. It was evidently a landformation not very apt to lodge
a freshwater fauna of any importance. It is difficult to ascertain
whether elements of this fauna still survive in the present fauna.
This might possibly be the case with Aplocheilus celebensis M. Wes.
and Anabas scandens DALD., which form a special element in the present
fauna. One of these, Aplocheilus belongs to the family Poecilidae,
several genera of which are known from the early tertiary; and
Anabas scandens has a very wide range of distribution, from the
continent of Asia to the eastern part of the indo australian archipelago. —

The recent fishfauna only came to full development when Timor was
raised to its present level in post pleistoceen times. This very young
land developed a system of rivers, which could only be populated
by such fishes, as are not, hindered by salt water in their distribution.
Timor, when rising, was surrounded by sea. The ichthyological
material tends to prove that this was originally a shallow sea, possibly
surrounding other greater or smaller islands in the neighbourhood,
as, for several elements of the freshwaterfauna of Timor, a deep sea
with a high salinity would form an unsurmountable barrier. Such
a sea could only have been formed after the immigration in the
freshwater was accomplished for the greater part.

We are of opinion that this is in accordance with the views
of Moneneraarr, who thinks that the formation of the deep seas
along the north and south coast of Timor took place in connection
with the final upheaval of the island, and that this has been the
latest event.

Physics. — ‘On the Deduction of the Equation of State from Boutz-
mann’s Entropy Principle.” By Dr. W.H. Kessom. Supplement
No. 24a to the Communications from the Physical Laboratory
at Leiden. (Communicated by Prof. H. Kamertinen Onngs).

(Communicated in the meeting of April 26, 1912).

§1. Introduction. Since the two great advances made by van
per Waats in deducing his equation and in developing the theory
of corresponding states therefrom, the theoretical investigation of the
equation of state for a single component substance has been developed
in various directions, particularly by van per Waats himself; these
developments have cleared up and enriched our knowledge of various
circumstances which influence the equation of state, and which had

241

been left out of account in the first deduction of the equation. For
example, we may refer in particular to the recent researches of
VAN DER Waats on the influence of apparent association. On the
other hand, there has been collected much valuable experimental
material, which has already, on various occasions, been compared
with the results obtained from theoretical assumptions. In the mean-
time, while these researches are being continued, it seems desirable
and opportune to undertake a systematic investigation of the equation
of state over a region in which not only reliable experimental data
can be obtained, and are in fact already accessible in part, but
which also permits of a rigorous theoretical investigation.

KAMERLINGH ONNes*) has started to systematically collect, arrange
and incorporate into his empirical equation the experimental results
already accessible over the whole region which has been already
investigated for the equation of state. Amongst other effects of this
empirical equation is that it makes it easy to compare different
substances from the point of view of the principle of similarity,
and in this respect it has already led to a number of valuable
conclusions. For a general review of these conclusions we may refer
to an article on the equation of state which is to appear in the
Encyklopddie der Mathematischen Wissenschaften and is now passing
through the press; we shall refer to this paper as Suppl. N°. 23.

In investigating the most suitable expression for the equation of
state preference was finally given (cf. Comm. N°. 71 § 3) to a series
of increasing powers of v—! (omitting the odd powers above 2
and closing the series with v—§). With a small deviation from the
notations of Comms. N°. 71 and 74 we may write the equation in
the form

v5 a haere 2 SD Ta og
Se eS SS ee
Vv v Vv Vv v
(cf. Suppl. N°. 23).

The form of this equation shows that, from an experimental point
of view, the method most immediately indicated for proceeding to
obtain correspondence between theory and experiment is to successively
determining, both theoretically and experimentally, the various
virial-coefficients A, B, C etc., over a temperature region as extensive
as possible for substances for which one would expect it necessary to
make the least complicated assumptions regarding molecular structure

1) H. Kamertinco Onnes, Comm. No. 7! (June 1901), No. 74, Arch. Neéerl. (2)
6 (1901), p. 874.

242

and molecular action. This is especially the case with the first
coefficients A, B and C, as their values can be experimentally
obtained with pretty high accuracy quite independently of any
special assumptions which may be made regarding subsequent terms;
while, from the theoretical point of view, the means are at hand
for deducing these virial-coefficiets from various special assumptions
regarding the structure and action of the molecules’).

- With regard to the first virial-coefficient A we may remark that
one may write

(R is the gas constant, 7’ the temperature on the KeELvtn scale) for
non-associative substances over the whole temperature region hitherto
investigated. With regard to the question as to whether such sub-
stances would exhibit another law of dependence upon temperature
in another region (e.g. at the lowest possible temperatures) we may
refer the reader to Suppl. N°. 23.

Both the present and the following paper aim at making a
beginning with the dednetion of the second virial-coefficient, 5,
from certain special assumptions, having in view its completion in
subsequent papers by a comparison with results obtained from
experiment.

In his Elementary Principles in Statistical Mechanics Gress deve-
loped methods which in principle enable us to deal with any mole-
- cular-kinetic problem concerning the equation of state, as long as we
limit ourselves by the assumption that the mutual actions of the
molecules conform to the Hamtironian equations. ORrNSsTEIN *) adapted
this method to the deduction of the equation of state and applied it.
In Suppl. N°. 23 the method indicated by Bourzmann in his Gastheo-
rie I] § 61 and based immediately upon the BoLTzMaNn entropy
principle is developed in general terms. This method, too, seems
suitable for the solution of all problems concerning the equation of
state of systems in which the mutual actions of the molecules con-
form to the Hamtonian equations. It has been shown by Lorentz *)

1) In this connection it must be remembered that, as noticed in § 1 of Comm.
No. 74, the virial-coefficients in the polynomial (1) differ from those of the corres-
ponding infinite series in which all the positive powers of v—! are present. The
more attention must be paid to this point, the higher the coefficients concerned ;
it will be quite appreciable with C on account of the absence of the v—* term in
(1), while D in (1) can no longer be regarded as approximating to the coefficient
of v4 in the infinite series (cf. Gomm. N’. 74 § 1).

2) L. S. Ornstein. Diss. Leiden 1908.

8) H. A. Lorentz. Physik. Z. S. 11 (1910), p. 1257.

243

that it leads to the same results as the Gisss method of the canonical
ensemble. Although the two methods can therefore be regarded in
principle as equivalent, the Botrzmann method seems to possess certain
advantages over the other, e.g. its terminology can be more directly
applied to the physical conception. *)

As Suppl. N®. 23 is not yet published we may here give a short
general account of this method, which forms the basis of the sub-
sequent developments.

§ 2. General formulation of the method of obtaining the equation
of state of a single component substance from the BOLTZMANN entropy
principle. In the general formulation of the method we shall follow
Bottzmann, Gastheorie I. § 36, and determine the momentary state
(PLANCK’s micro-state’*)) of a system of molecules whose motions,
under the influence of their mutual forces, can be regarded as
determined by Hamitron’s equations *) in terms of a finite number
of generalised coordinates and the corresponding momenta for each
molecule. We shall define a mzcro-complexion *) as a state in which,
for instance, the coordinates g,...qs and the momenta p,... ps of
the first molecule lie between the limits qi; and q:;-+ dqii, gai and
gai + dqai gsi and qi + gsi, pri and pi; + dpri, poi and px; + dpa, eps:
and psi+ dps, those of the second molecule between qi; and
gij +dq; ete.

In this, the micro-differentials*) dqi; ete. must so be chosen that
the specified distribution of molecules according to generalised coordi-
nates and momenta is sufficient to fix the energy of each molecule
in the micro-complexion as lying between definite limits which, in the
problem under consideration, may be regarded as coincident, and
also to enable one to ascertain if possible special conditions (e.g.
mutual impenetrability, in the case of molecules supposed rigid) have
Beene tulfilled, We assume that dq,,—... = dq,i=dq,; =... dq,»
a... ap. =... dp; = dp,;.= dp,. ete. or, at least, that the

1) And also in this that by this method the most provable distribution of molecules
according to definite coordinates or momenta is at the same time determined, and
also an expression is found for the Botrzmann H-function for the particular case
under consideration.

*) M. Piuanck. Acht Vorlesungen p. 47 sqq

3) In the application to collisions between molecules which are regarded as rigid
bodies we shall, if necessary, regard the collision as a continuous motion subject to
very great accelerations.

4) Derived from BoLtTzMANN’s “Komplexion’”’. Comp. L. BoLrzMann. Wien Sitz.-
Ber. 76 (1877), p. 873; Wiss. Abh. 2, p. 164.

5) M. Puanck. Acht Vorlesungen, p. 59.

244

different elements of the 2s-dimensional space involving the coordinates
p and the momenta qg (the micro-elements) are of the same size.

We consider now, in general, states of the system of molecules
which are defined by certain conditions — formulated in detail for
each special problem — in such a way that the number of mole-
cules or of groups of molecules is determinate for which e.g. certain
coordinates, mutual distances or orientations of the molecules, their
momenta or their relative velocities lie between limits previously
assigned. The formulation of these special conditions and the choice of —
limits must so be made that the supposed numbers of molecules ete., are
sufficient to determine, in so far as the particular problem under
discussion is concerned, the state of the system as seen by a macro-
observer at the particular moment for which those numbers are given.
In this we are in no case concerned with the individuality of the
molecules (we assume throughout that we are dealing with a single
component substance). The limits to which we referred must, moreover,
be so chosen that the macro-state thus determined can be realised
trom a very large number of different micro-complexions.The assemblage
of these micro-complexions we shall call a group macro-complexion’).

As a foundation for further development we shall now assume
that all micro-complexions represent cases of equal probability *). From
this it follows immediately that the probability, W, of the occurrence
of any group macro-complexion is proportional to, or, if we care to
neglect an arbitrary factor, is equal to the number of micro-com-
‘plexions contained in the group macro-complexion *).

In many cases it will facilitate the calculation of this number to
first obtain the number of micro-complexions contained in an individual

1) For constructing a clear molecular kinetic interpretation of a definite macro-
state, in particular regarding the number of the different micro-states by which it
can be realised, we regard here as in the Gress method at any particular moment
an assemblage (ensemble) of systems, independent of each other identical as regards
number, structure and actions of their component particles and as regards their
exterior coordinates, each of these systems forming a definite micro-complexion
realising that macro-state. Cf. Bortzmann, Wiss. Abh. 1, p. 259; 3, p. 122;
MAXWELL, Scient. pap. 2, p. 713. [Note added in the translation.]

2) In the present paper we shall not justify this assumption, which, in so far
as it affects the choice of micro-elements, is founded upon LioUVvILLE’s theorem,
but for it we may refer to the writings of BOLTZMANN, PLANCK (e.g. Acht Vor-
lesungen, p. 56), and others. (Compare also Art. IV 32 by P. and T. EHRENFEST
in the Math. Encykl., particularly note 170).

*) In order to conform to the common definition of probability as a fraction
between © and 1 in value we should have to divide by the assumed value of the
constant total number of micro-complexions possible, which would have to include
all possible values of energy and volume which occur in our considerations. This
constant is of no importance in any of our considerations, so we shall omit it.

245

macro-complexwn. The definition of the latter complexion follows
from that of the group macro-complexion by taking account of the
individuality of the molecules. The number of micro-complexions in
the individual macro-complexion has to be separately determined for
each special problem, and this, multiplied by the number of individual
macro-complexions contained in the group macro-complexion gives
the number of micro-complexions contained in the group macro-com-
plexion. The number of individual macro-complexions contained in
the group macro-complexion, which is readily obtained from the
theory of permutations, we shall call the permutability index of the
macro-complexion *).

From the value thus obtained for the probability of a group macro-
complexion one can ascertain which group macro-complexion is the
most probable in a self-contained system of molecules of given energy
and volume. According to Bortzmann the distribution of molecules
according to the coordinates ete. determining it, obtained for this
macro-complexion, corresponds macroscopically to a state of equilibrium
of the system of molecules.

BoLTzMANN’s entropy principle can now be formulated in such a
way that the entropies of different macroscopically determined states
are, if we omit an arbitrary additive constant, proportional to the
logarithms of the probabilities of the different group macro-complexions
corresponding to those macro-states. In this it is understood that these
macro-complexions are determined with the same limits (equal
elements of corresponding spaces) for the coordinates ete.

In the simple case, in which the same number of micro-complexions
is present in each of the individual macro-complexions, as in the
deduction of the equation of state for molecules whose dimensions
and mutual attractions are neglected *), the entropy is then simply
proportional to the permutability index of the macro-complexion.

In general we may write

f S = kp log. W. o iggteiee aes
in which S represents the entropy, and kp = Ry/N where Ry is
the molecular gas constant and WN is the AvoGapro number (i. e.
the number of molecules in the gram molecule). We then obtain for
the entropy in the state of equilibrium of a gas whose molecules are
regarded as having no dimensions and as exerting no mutually attractive
forces, a function of volume and temperature which agrees with the
thermodynamic expression for the entropy.

1) Differing slightly from L. Botrzmany, loc. cit. p. 243 note 4.
7) Comp. M. Puanck, Warmestrahlung, p. 140 sqq.; Acht Vorlesungen, Vierte
_Vorlesung.

246

If, by introducing special assumptions regarding the molecules and
their mutual forces, one calculates, in the manner here indicated,
the entropy S in the equilibrium condition for given energy U and
volume V, one obtains directly a fundamental equation of state from
which both the specific heats and the thermal equation of state can
be deduced.

§ 3. Deduction of the virial-coefficient B for rigid, smooth spheres
of central symmetry and subject to VAN vuR Waats’ forces of
attraction. |

Although this problem has already been repeatedly treated, first
by van DER Waats himself in the deduction of his equation of state,
and since then, in particular, by Pianck') by a method which is
essentially the same as that here developed, we may yet utilise
this simple case as an introduction to our treatment of the succeeding
more complex cases. The description of these can then be shortened
by referring to corresponding definitions and operations in the present
problem.

Determination of the macro-complexion :

Two states which a macro-observer can distinguish as different
may be regarded as having their differences arise from the presence
in definite elements of volume of different numbers of molecules in
the two cases, and also from different distributions of speed in those
volume-elements. To determine a macro-complexion we _ therefore
take the three-dimensional spaces which are available for each
molecule with respect to its coordinates «, 7,2 and the velocities §, 4, 5
of its centre, and divide them up into equal elements (dv,dy,dz, =)
dv,, dv, ... dvz, and (d§,dy,d6, =) dw,, dw, ... dwy.

In this we make dv,... so great that each contains on the whole
a great number of molecules, and yet sufficiently small for the density
variations within those elements of volume to escape the notice of
the macro-observer; the elements dw,... are also chosen so great
that to each corresponds a large number of molecules in dv,... and
yet so small that d3,,dy,,d¢,... are small in comparison with the
mean speed.

The group macro-complexion is now determined by the conditions that

n,, unspecified molecules “are present” in dv, dw,

(4)

ME : ‘ r » ny A, dy .
Determination of the micro-complexion :
As far as velocities?) are concerned, the micro-complexion can be

1) M. Puanck, Berlin Sitz.-Ber. 32 (1908), p. 633.
2) As the velocities differ from the momenta only by a constant factor, we may

determined from the same elements of the proper space as the maecro-
complexion. With regard to the distribution of the molecules throughout
the space we must distinguish between various elements of volume,
which are supposed small in comparison with the dimensions of a
molecule, for, in ascertaining if a certain micro-complexion occurs in
the macro-complexion determined by (4), it is of importance to know
if the centre of any particular molecule lies within or without
the distance sphere of any other molecule. Hence we divide
the volume-elements of the macro-complexion into smaller volume-
elements, thus

dv, into x equal volume-elements dw,,... dw,
dv, By ” ” » dw,, Sate dws,
ete.

A micro-complexion is now determined by specifying for each mole-
cule in which of the elements dm and dw it is present at the par-
ticular moment under consideration (understanding that a molecule
is present in the micro-volume-element dw, when its centre of mass
is there).

W is now the number of micro-complexions thus determined present
in the macro-complexion given by (4); in this we must remember that
all micro-complexions are excluded in which the distance separating
the centres of any two molecules is smaller than the diameter of a
molecule. '

For the permutability index of the macro-complexion we obtain

ni!

O° es) sae ead a ae OY

As we shall have to deal only with such macro-complexions as
correspond to states of equilibrium or to states differing but little
therefrom, it follows from the conditions laid down regarding the
magnitude of dv and dw, that for each element dvjdw; of the 6-
dimensional space in which, for any specified state, molecules may
be present, the number ;; will be large. We shall, in the mean-
time, be obliged to compare macro-complexions whose total volumes v
are not the same’), for instance in the development of the thermal
equation of state. This can be done if, in the determination of the
macro-complexion, we also take account of volume-elements lying

in this case use equal elements in the velocity diagram for determining micro-
complexions of equal probability.

1) When, as in the present instance, we consider states in which the substance
is not split up into different phases, we shall indicate the volume ete. by small
lelters v.w,s, which, when referred to 1 gram of the substance, can then be
regarded as spec‘fic quantities.

248

outside the volume v. A similar remark holds regarding the energy
u. The conditions represented by (4) must then be so understood that
the number of molecules in each of these outlying elements of the
6-dimensional space is zero, and for each of these elements the
figure 1 must be put in the denominator of the permutability index.

We have still to calculate the number of micro-complexions contained
in the individual macro-complexion; this is determined by specifying that

n,, specified molecules are present in dv,dw,
: (5)
Nkl 33 A i r: ,, dvydwi.
These micro-complexions_ differ only in the different dispositions of the
n, = 7n,, +...m; molecules in the volume-element dv, ete. The diffe-
rent volume-elements are here to be regarded as independent of each
other. We then obtain the total number of micro-complexions by cal-
culating the number of different ways in which the n, molecules
can be placed in the volume dv,, the same then for dv, etec., and
by then multiplying these numbers together.
Let us first put the first of the n, molecules in dv,. For this there
are x places available. For the second molecule there are then left

4 i
—70°!

x fi ———|places available. Of these there is a comparatively small
H v,

number for which the distance between the centres of molecules
is such tbat the distance spheres of the two molecules partially
overlap. In placing the third and succeeding molecules we shall omit
these cases, for bringing them into the calculation would introduce
terms of the second order of small quantities compared with the
principal terms of W, and would have no effect upon the value of
the virial-eoeffivient 6. The influence of these terms would have to
be more closely investigated only in the determination ‘of C and
succeeding coefficients. The number of places available for the third

is caat
' arc |
molecule can then be written “{i—2.— J. Proceeding in this
vy
fashion we obtain
| —10°
n =n,—1 3
a2 ee ] I—t
—s dv,

different dispositions of the n, molecules in dv,. Doing the same for
dv, ete., we obtain the number of micro-complexions in the individual
macro-complexion.

249

After multiplying by the permutability index, a little reduction
in which use is made of Srirtina’s formula, gives with sufficient
approximation

: a ;
log W= — = &J n,, logen,, -— > — Sh: ets 6 Gem
dv dw @ dv, dv @

In this, terms have been omitted which remain constant when n

is constant and the division into elements remains the same. > and >
dr dw

indicate summations taken over all the elements dv and dw. Use has
also been made of the fact that the elements dv are all of the same size.

The expression which one obtains for Botrzmann’s H-function by
reversing the sign of (6), agrees to the degree of approximation
here given, with the expression given by OrnstEIN’) for this case.

State of equilibrium:

This is determined by the condition that for constant v and w,
W is a maximum. The condition v = const. is fulfilled by varying
only the values of n,,, etc. which occur in (6), and keeping
M,+-.--2=n constant. With regard to the condition «= const.
the assumption that the molecules behave as if they were rigid
smooth spheres, of central symmetry (so that their density is constant
or only a function of the distance from the centre, and therefore
their mass centres and their geometrical centres coincide) enables us
to disregard angular speeds about axes through their mass centres.
To enable us to find an expression for the potential energy we
shall assume that the macro-volume-elements are great in comparison
with the sphere of action of a molecule. With reference to the
potential energy we shall, in conformity with the assumptions under-
lying the van DER WAALS attractive forces, further assume that, in
states of equilibrium and in states closely approximating thereto,
each sphere of action can be regarded as being uniformly filled
with the number of molecules which that sphere would contain if
the molecules were uniformly spread over the whole macro-volume
element. In making this assumption cover even the molecules which
lie near the boundaries of the volume-element we neglect the influence
of capillary forces. Calling the potential energy of mn molecules
uniformly spread over the volume v, — ae with a, constant, we may

;
write the whole potential energy contained in the element dv, as
dwn,”

n*dv,

1) L. S. Ornsrer. Diss. 1908, p. 60.

. The condition for the energy then becomes

250

Oy Sige

Ee EG)

OGL gis) ais ea
dv dw dv n? dv,

1 . .
in which to, = at (§,? + 7,° + $,°) represents the kinetic energy of

translation of a molecule whose velocity lies in dw,.
The condition for a maximum, in conjunction with (7) and
n = const.’) gives

4 3
ee 20, Wt,
— loge n,, — 2, ——h|{ ty, - —]|-+ log,c=0,. (8)

dv, n°dv,
in which / and ¢ are constants. A few reductions lead to
7
Rn == — dt,
v
and (9,

n(hm ‘lz — hy,
22 = e dv, dw,,
11 9 1 1
vo\ 2a

the well known conditions for equilibrium: macroscopically uniform
distribution throughout the space, and Maxwet1’s distribution of
velocities with the same constant for each macro-volume-element.
This constant h can be found by obtaining an expression for the
energy wu

pe ge
CT Soe es 3. er
From (6) and (9) we obtain for the state of equilibrium
ln 4
logg W =n loge v — Se loge h+-h wy — a n aoe

in which w,, represents the total kinetic energy, and certain constants
are omitted. In conjunction with (3) this gives

— k lode Y= SS k 7 lo e h =~ k ji Sh ds = nm —H : ] 1
— f/; ) . "yn ¥ ) u w (6) . .
s I mv . 9 : I : ; Z v 3 ( )

On eliminating h between this equation and (10) one obtains a
fundamental equation of state expressing w as a function of s and
v,or s as a function of w and v, which Pranck calls the canonical
equation of state. On keeping v constant and differentiating (10) and

“ :
(11) with respect to /, since Tess one easily obtains
Uv

1
(— ee ee
kp h

1) It will be seen that in the case of the most probable distribution the total
momentum and the total moment of momentum vanish for each macro-volume-
element. If one wished to evaluate the entropy for states in which these magni-
tudes were not zero one should have to introduce here suitable conditions to allow

for them.

;

251

from which with (11) it follows that

if 8 n P 4 37 oe ag TOE es
p—u — —_ = — — log. v + — — logge h — — + -n —wo’.
ky h h D es v 2 he 8

Using (12) and the relation 4, = R/n, in which FP is the gas con-
stant for the quantity under consideration, this equation is trans-
formed into

3 a ep
= —RT loge v — SRT log. joan 9
v

Basia, See

; 1 4
in which 6, has been written fox — ra. xo and a linear function

of 7 has been omitted.

. . . Vv --p
From this equation one obtains the value = R for the specitic

heat at constant volume, while the thermal equation of state becomes

Fiat b by ay
pee fe ye
v v v

Hence (cf. § 1) ,

een ote SS Sed
R1

§ 4. The virial-coefficient B for rigid ellipsoids of revolution subject
to VAN DER WAALS attractive forces.

Determination of the macro-complexion.

We shall first assume that in collision between two ellipsoids the
speed of rotation around the axis of revolution can also vary. To
make sure that HAmilton’s equations are sufficient to determine the
mutual action of two such ellipsoids (cf. also p. 245 note 5) we
shall make it essential that the surfaces of the colliding bodies which
we are considering can never exert other than normal forces upon
each other at their point of contact. We shall, however, assume that
it is found on closer investigation that the surfaces of the ellipsoids
are not perfect surfaces of revolution but show, it may be, a uni-
versal wave-formation; but in the meantime we shall assume that
deviations from the true shape of an ellipsoid of revolution are so
small that they may be altogether neglected except in so far as they
give rise to a moment around the “axis of revolution” during colli-
sion. Hence in formulating the condition that the energy has a given
value, we shall also have to allow for the speed of rotation around the
axis of revolution. To express that condition, then, it is desirable to
determine the macro-complexion as was done in § 3 and also
with respect to the speeds of rotation around the three axes of
. 17
Proceedings Royal Acad. Amsterdam. Vol. XV.

i)
Or

inertia, Pr, Gr 7r, in which pr represents the speed of rotation around
the axis of revolution.

The group macro-complexion is now determined by specifying that
2,,, unspecified molecules are present in dd, dw, dw,

Nor1 . %9 : Mr) Sateen, Serres tee SSP)
in which dw, represents an element of the space involving the
coordinates p.,g-, and 7,; these elements are also assumed to be equal.

Determination of the micro-
complexion :

For this it is necessary to spe-
cify the position of the ellipsoid.
To do this choose a fixed system
of axes XYZ, and through the
origin draw a line OA parallel
to the axis of revolution; we shall
determine the position of the ellip-
soid by the angles AZX =a,
AOZ = 060 and the angle x
between the plane AOZ and a
fixed meridian plane of the ellipsoid (Fig. 1).

Angular momenta: We may represent the kinetic energy ane rota-
tion, Z,, by the formula

Pigeal.

L= Ape $48, G4). 2.
in which A,— the moment of inertia about the axis of revolution, and
‘Bia 2 ipa » an equatorial axis.

We shall choose the equatorial axis to which q, refers, OL, in
the plane AOZ, OC perpendicular to OA and OB in such a
direction that a rotation from A towards B seen from C is in the
sane direction as a rotation from X towards Y seen from Z.

It is seen that

Pr=p osO+y
qr = p sinO Mae ts eo rn
m~=—O

in which the dots represent differentiation with respect to the time.

If we call the angular momenta with reference to ~, 4, %, ¢ D, 6, "i

respectively, we then obtain
G = A; cos O. py + B, sin O. qs
6=—B,r, ayy
%= Ar Pres

in which p,, qr, and 7, have the values given in (17).

Instead of determining the micro-complexion by dp d@ dx dy dé dy
we shall introduce a slight modification. From (18) we find

253

dp d6 dy = A; B,? sin 0 dp, dq, dr,
if we stipulate that the sign of equality in this and similar expres-
sions means that in the integral the expression on the left may be
replaced’ by that on the right with the proper modification of the
limits of integration.

Let us further write do for an element of the surface of the sphere
of unit radius, by points on which we can indicate the direction of
the axis of revolution of the ellipsoid; we then obtain

do
sin @

dp dd =

Hence
dp dO dy dg dO dy = A, B,? do dy dp, dg, dr;.

We shall therefore obtain micro-elements of equal probability (cf.
p. 246 note 2) if we measure equal dw’s, equal dw’s, equal do’s,
equal dy’s and equal diw,’s, and combine them.

If each molecule is assigned to a particular micro-element, then
the micro-complexion is completely determined.

The number of individual macro-complexions in the group macro-
complexion is

111 ! Nites ! pe ies
(compare what was said concerning the corresponding expression in § 3).

The number of micro-complexions in the individual macro-complexion
is determined as follows:

The various volume-elements dv are again independent of each
other (cf. §3). Let us consider the 7,*molecules in dv,. To each
molecule we ascribe its proper speed of translation €,7,¢ and speed
of rotation p,,qr,7r determined by (15). We then “place” the first
molecule in one of the » elements dy, then in one of the x ele-
ments dw and lastly in one of the uw elements do. This can be done
in xuv different ways.

We now dispose of the second
molecule. For this we have still »
elements dy at our disposal, but
for the other coordinates there
are fewer places available than
was the case with the first mole-
cule. Outwards along the normal
to each point of the first ellipsoid
mark off a distance a (equal to
half the major axis) (Fig. 2),then
each dw outside the surface thus

17*

254

obtained is a possible position for the centre of the second ellipsoid,
and in any of those positions all orientations of the axis of revo-
lution of this ellipsoid are possible. Calling ve the volume enclosed
by the outer distance surface thus obtained, then the above volume-

elements give rise to xj

Ve TOE EAI
1 -—) possibilities.
dv,

Along the normal to each point of the ellipsoid mark off a distance
/ (equal to half the minor axis), we thus obtain a surface within which
no centre of another molecule can lie. We shall call this the znner
distance surfuce, and designate by v, the volume which it encloses.
In the shell enclosed between these two distance surfaces the centre
of the second ellipsoid can be placed, but then all « orientations do
are not possible, but only a portion of them, which can be deter-
inined in the following fashion (Fig. 3). Let A be the first ellipsoid
which we shall regard as immovable. Let ? be a point of the shell
determined by the coordinates relative to A: x in the direction of the

Fig. 3.

axis of revolution, y in the direction perpendicular to it. Now place
the second ellipsoid with its centre at P, and, keeping its centre
fixed, allow it to roll on the surface of A; during this rolling the
point of contact & describes a trace on the surface of A. We can
write for the solid angle of the cone which is described during the
rolling by the semi-axis of revolution, PQ, 2 ay if the ellipsoid is
prolate, 22 (1—v) if oblate, in which g is a function of x and y;
there are then m«(1—v) orientations do possible for the ellipsoid
pene

B with its centre fixed at P. Altogether we shall have xur i
1

cases, where
B=Ss0ie st iydw. oes) 4.) = ee

the integration being taken throughout the shell.

255

B may be regarded as the mass obtained taking the volume con-
tained within the inner distance surface as having unit density,
and adding to it the sum of the volume-elements contained within
the shell between the two surfaces, each multiplied by its own
density v.

The placing of iv , Pipe se cio, ek

placing of the third molecule can be done in xn /! 2
1
ways if one takes no account of the complication introduced by the
approach of three molecules (cf. § 3). Finally we get

ae. n! ‘—n,—1 B
W = (eur)? ———_ TT _ IT 1—t— }.

Miyil s+ dv c= dv,

Omitting constants this gives

3 = ios 3
one Wa on loge n.,) aa
d. dw dw,. dy 4a dv,

Subsequent treatment of this problem differs from that given in

§ 3 only in so far as the energy condition, under the same assump-

tion as was there made regarding the potential energy, must now
be written

= = = Miia 4 m (55° bm," +$,’) =f

dv dw dw.

1o|h

Ayp,* + 4 By (qe? +72); —

2
ys tw

med 2
dy n’dv,

S=ODDER Ss = = tae ay. $(20)

The result then follows that the specific heat at constant volume
for these rigid (but not smcoth). ellipsoids is 3/2, while as regards
the thermal equation of state equation (14) gives the value of B if
we substitute
byt (21)
. Wiss 2 z “

. As far then as concerns the term with the virial-coefficient B,
we find the sam2 equation of state as for rigid spheres’), only with
the ellipsoids, 6, is not such a simple function of the volume of
the molecules as with rigid spheres. .

‘ We shall now introduce the assumption that the ellipsoids are
perfectly smooth, so that the velocities of rotation around the axis
of revolution undergo no change on collision. We shall also assume
that the attractive forces cause no modification in these angular
speeds. In that case it is not necessary to allow for the value of

1) This may be regarded as a particular case of the general proposition indicated
by Bottzmann (Gastheorie IL §61), for molecules which behaye as solid bodies
of shape other than spherical,

256

p: in the equation for the constant energy; hence we shall also
take no account of p, in the determination of the macro-complexion.
The group macro-complexion is then specified thus:

,,, unspecified molecules are present in dv, dw, (dq, dr;),

Niis 2 ” >” ” See 5 CICS ee: (22)
in which (dq, dr,), represents one of the different elements (supposed
equal) of the space involving the coordinates g, and 7,. The equation
for given energy then becomes
= ny om 6s aie a Gs Bae ot ,°)} — =

dv n'dv,

dwn,”
= const,

As far as the thermal equation of state is concerned the result is
the same as that obtained for rough ellipsoids, but the specific heat

oe
at constant volume is different, viz. A R, for smooth ellipsoids.

Physics. — On the deduction from Bout7Mann’s entropy principle
of the second virtal-coefyicient for material particles (in the
limit rigid spheres of central symmetry) which exert central
forces upon each other and for rigid spheres of central-sym-
metry containing an electric doublet at their centre. By Dr. W. H.
Kzrsom. Supplement N°. 24° to the Communications from the
Physical Laboratory at Leiden. (Communicated by Prof. H.
KAMERLINGH ONNEs).

(Communicated in the meeting of April 26, 1912).

§ 5°) The deduction of the second virial-coefficient, B, for material
points (in the limit rigid spheres of central symmetry) which exert
central forces upon each other.

In this section we shall deduce the eqnation of state, as far
as the second virial-coefficient, 6, is concerned (cf. § 15, for a
system of molecules which act upon each other as if they were
material particles (in the position of the centres, which are also the
centres of gravity of those molecules) and with forces which are
given invariable functions of the distance. All mutual actions other
than that just described will be excluded. The case in which the
spheres can be regarded as rigid spheres of central symmetry (§ 3)
exerting central attractive or repulsive forces upon each other which
are a function of the distances between their centres, will be treated
as a limiting case.

') To facilitate reference to Suppl. N'. 24a sections, equations and diagrams
in the present paper are numbered as continuations of those in Suppl. N% 24a.

257

This problem has already been discussed by Botrzmann') and by
Remcanum’), both of whom applied BorrzMann’s distribution law to
the deduction of the pressure from the equation of the virial, and
by OrnsTEIN’), who used Grsss’s methods of statistical mechanics. In
this § our treatment of the problem will be based upon the BorrzMann
entropy principle, and at the same time we shall obtain an expression
for the BortzmManNn /7/-funetion for this case, while the BouTzMANN
distribution law for this case will also result. In § 6 we shall
conclude with a discussion of a system of rigid molecules of central
symmetry, each with an electric doublet at its centre.

The reader is referred to Suppl. N°. 24a, § 2 and 3 fora general
exposition of the method which forms the basis of the present inves-
tigation, and for an application of this method to rigid spheres of
central symmetry exerting VAN DER WaAats attractive forces upon
each other.

In the case now under discussion the macro-complexion must first
be determined as in § 3 by the conditions laid down in (4). In order
to be in a position, however, to write down the energy equation
for the present problem it is necessary to know how many pairs
there are amongst those molecules, the distances between whose
centres lie between certain definite limits. We shall assume that we
have to differentiate only between molecules within whose sphere of
influence are no other molecules and those within whose sphere of
influence one other molecule is present; that is, that molecules which
have two or more other molecules within their sphere of influence
are of such infiequent occurrence in those states of the molecular
system which we shall consider, that we may entirely neglect their
influence. This supposes that the force exerted by any molecule is
appreciable only over a finite sphere of influence which is small
compared with the space in which the molecules are moving. We
assume that the elements, dv, which are taken to determine the
macro-complexion (cf. § 3) are large compared with this sphere of
influence. We now divide the radius of the sphere of influence, rt,
into a great number of equal elements dr,, dr,, etc., which are so
small that we may neglect the change in the potential energy of a
pair of molecules during a change equal to one of these elements
in the distance separating them. We shall subdivide the n,, molecules
contained in dv, dw, into

1) L. Botrzmann. Wien Sitz.-Ber. [2a] 105 (1896), p. 695, Wiss. Abh. 3, p. 547.
In that paper the general result is also applied to the special case of repulsive
forces varying as Kr-5.

2) M. Remincanum. Ann. a. Phys. (4) 6 (1901), p. 533.

3) L. S. Ornstein. Diss. Leiden 1908, p, 70 sqq.

258 |

Ny, single molecules (with no other molecule within their sphere

of influence)
y3,, Molecules belonging to pairs which are separated by a distance
lying between r, and 7, 4+ dr,,
yy,2 Molecules belonging to pairs separated by a distance lying f
between 7, and r,-+dr,, ete, . . . (23)
the z,, molecules in dv, dw, we shall subdivide into

Ng, single molecules ete.

The group micro-complexion is determined by these numbers 7),
ete., when no account is taken of the individuality of the molecules.

Determination of the micro-complexion :

Each of the equal elements dv is divided into x equal volume-
elements dw whose linear dimensions are still small in comparison
with the dr, ete. which we have just introduced. Otherwise the deter-
mination of the micro-complexion is just the same as in $§ 3.

The number of individual macro-compiexions in the group macro-
complexion is

! / /
Nyja: M15] - MyUWA- +. No! otehe

The number of micro-complexions in the individual macro-complexion
is found in this way: All the volume-elements dv, etc. are independ-
ent of each other, so that we can obtain the total number of micro-
complexions by finding the number for each volume-element dv, and
multiplying these together. We shall first assign to each of the

my == My, + Min + Mue + --- + min +... =~ ~ Aa
molecules in dv, its place in the micro-volume-elements dw, . . . daz,
and thereafter give it its proper speed as obtained in the determi-
nation of the individual macro-complexion. The latter operation will
not give rise to any change in the number of micro-complexions.
In dv, therefore we have got to place
n, specified molecules.

Of these:
N\q specified molecules are to be single
161 i z- are to belong to pairs whose distance apart

lies between 7, and 7, + dr,
ni etc,
where
me Rac haiy he he) ae ee
Ms) = Nas + M1951 +--+
The first of the 14 molecules gives rise to x possibilities according
to which of the elements dw it is placed in. When the first

259

4
| = ar'|
molecule has been placed there is a volume dv, h — rare left
av, |
available for the second of the njq single molecules. The second mole-
4
= "|
cule, therefore, gives rise to the factor x a Sag ey in the num-
a v1

ber of micro-complexions. The third of the 7, molecules gives *
4 3
as CLG

3
“Fa
number of micro-complexions the spheres of influence of the first two
molecules partially overlap, as these complications need only be
allowed for in the calculation of the C and subsequent virial-coefti-
cients (cf. § 3). Proceeding in this fashion the 7, single molecules give

the factor

p= oO. in this no account is taken of the fact that in a

We must now place the 7,,; molecules which belong to pairs whose
distance apart lies between 7, and 7, + dr,. In order to see in how
many different ways this may be done we must first notice that one
of these molecules can go to form a pair whose distance apart lies
between the proper limits only in combination with another of the
same group (this does not strictly hold if the molecule in question
is placed on the boundaries of dv, ; if, is sufficiently great, however,
the effect of this” may be neglected). The 7,; molecules can then
combine to form pairs in

different ways. Let us take one of these combinations. Take one of
the pairs and place it; this is done by first assigning a place to one
of the pair. As it must be placed outside the sphere of influence of
any of the ,, single molecules already in position there are left
qe

x )l —n, ——
dv,

places available. Having placed the first molecule of the pair in

260 d

question in one of these places there are, since the second of the
pair must come within a distance between r, and r, + dr, of the
first,
Anr,?*dr,
x ——— -—-
dv,

places available. This is so at least for all those cases in which the
first molecule is placed within a distance not less than r+ r, of
any of the 2, molecules already in position. When that distance is
not exceeded complications are introduced by the fact that a portion
of the shell 477,?dr, lies within the sphere of influence of that other
molecule. If we wished to confine ourselves strictly to cases in
which one molecule is acted upon at any time by no more than
one other molecule, then these portions of the shell which are over-
lapped by other spheres of influence ought not to be included in the
summation.

But cases in which these complications occur form but a small
fraction of the whole, both for this and for subsequent pairs of

n,.—a0*

molecules, the order of magnitude being a eis which is very
vy :

2
"

dr
— give rise to terms in log, W which are of the
vy

first order of small quantities, and which we shall have to take into
account. Subsequent terms, however, may be omitted, and in that
case we may also neglect the effects of the complication referred
to above. Likewise we shall for the same reason neglect corresponding
complications for subsequent pairs, of which the placing of the first
molecule already gives rise to a factor which we change ina corre-
sponding manner.

As the method here described gives all the positions possible, after
the 2, single molecules have been disposed of, for the first pair of
molecules whose distance apart lies between 7, and 7, + dr,, the
placing of this pair gives rise to

An
small. The terms x

3
2
4ar,*dr,

dv,

x“? J1— 1,

possibilities. In this expression we shall introduce a factor 1—(n,, + 1)
4

— at’

ne these factors, too, of which there is one for each pair of mo-
v, :

261

lecules, do not influence terms of the first order of small quantities.
By treating all the pairs of molecules contained in dv, in the same

way, and then all the pairs of molecules in dv, ete., we obtain for

the number of micro-complexions in the group macro-complexion

+
eee)
n! c=m—1 |
ft |.
Ma! Mw! ++ Mga +++ dv c= dv,
M1
Ayal Azur dr,\ 2
IT (26)
dr 181 dv,

goa fer t\
2

Retaining the principal and first order terms in the expression for
loge W, and abandoning higher orders of small quantities as well as
all terms which remain constant under all the considerations involved,
we obtain the expression

4
23 zer*
n
loge W=—nila loge nila —Mi101 loge M1141 «».-— SS —- ——— +
done av,
4ar,*d
fee Seeing, | | | (27)
dv dr 2 2 2 3 dv,

If the sign of this expression is changed, it becomes a form of the
BottzmMann H-function for this case.

The state of equilibrium:

Let us write — ¢(r,) for the potential energy as dependent upon
the mutual forces exerted by a pair of molecules at a distance 7,
apart, and let us assume that for separating distances greater than
t the potential energy of a pair of molecules may be taken to
be =0; we may then write the energy condition in the form

w= J Tn, te — § FS Sry G(r,) = const. . « « (28)
dv dw dy dr 3

(for the significance of w,1 cf. § 3).
The condition that loge W is a maximum together with this equation
(28), and the condition » = const., and equations (24) and (25) give

4
— ar
—loge M1. —N, — — huy) + loge c = 9
v;
x
nee , (29)
3 Azxr,*dr,
—loge M1151 —N, + 4 loge min “+ lage se
dv, % \ dv,

—uUyi—h i3¢(r,)} + logec = 9

262 '

ete., in which ¢ and / are constants. If we retain only the terms
of the rank of principal or first order terms in log, W, we get, since

4 :
n, ae is small compared with dv, :

4 \
| — ar
: 3 —huiy)
Nila = C | 1—n, é
dv, | :. de Oe
( ie —hiuwi—tg(r,)}
73311 — ¢| 2161. —_—_— e
dv,

The constant c¢ is determined by the condition that the total
number of molecules must be equal to n. Let us writec = c’dw, =
= ¢'d3, dy, dS,, and then summation (integration) of (80) with
respect to dw, gives

of aE es a
Te ———_— elif) ,
hm dv,

Summation with respect to 7, and addition of the value of 1,
yields an expression for 7, which leads to the conclusion that the
distribution of the molecules in space in the state of equilibrium is
uniform in the macroscopic sense. c’ is next determined by summation
with respect to dv,. We then obtain

7
n

ny = = 4a? dr, CM) de, si ae
v

If we divide this by 2 it gives us, to a first approximation, the
number of pairs of molecules whose distance apart lies between 7,
and 7, + dr, in the state of equilibrium. This expression is in
agreement with that given by Bottzmann (p. 257 note1) which was
also used by REINGANUM (p. 257 note 2).

We find, moreover, that
2 3
n hm ‘ls = ee, ,
v Jt

so that the velocity distribution is the same for molecules in each
other’s neighbourhood as for single molecules.
For the number of single molecules we get

n (hm ?!2
5) —
v\2n

P= {Oda de oS

eel dv, OW, (20m 6° ee

n
1—— P
v

in which

-
rs

265

if we replace summation with respect to d by an integration.
To determine 4 we derive the total energy, u

3n 1 n? 0 :
“4 = — — —— , 0, eae ee es eee
2h Nie (35)
in which
Q= felHy0) a | ees en ar aie SY 1,
0

If we now calculate the expression for log, W from (27), allowing
for (33), (82) and (31), retaining only principal and first order
terms we get from (3) and (35) for the state of equilibrium

3 1 n® (4 :
s = nkp Inv — = nkp Inh +- kp hu——kp — a xt — P (37)

a a 1

On elimination of / by means of (35) this equation yields what Planck
calls the canonical equation of state. And just as in $ 3, noting
: dP
that P and Q are related to each other by the equation Q=—
0
we now recover equation (12) from (35) and (37), a result to be
expected and consequently affording a desirable control.
Introducing the temperature 7’ as defined by (12) and also the
gas constant Ff (cf. § 3) we obtain
3 RT n (A
w — — RT log. v — — RT loge T +-— .~|~—ar?—P] . (38)
2 v 2\3
The specific heat at constant volume y, is now found to be
dependent upon the volume. Putting v = in the expression for y» we
obtain the specific heat at constant volume in the Avocapro state *)
7.2. ;
For the thermal equation of state we obtain

fee ye Oo es ae et OP)

with the second virial coefficient

5 f
B==—=n
9
0
1

in which 2 may be replaced by = 4
P

CT. Oro xs j0 5:

1) Cf. Suppl. N°. 23, Nr. 39a.
2) This result agrees with that given by OrNSTELN, Thesis for the Doctorate, p. 73.

264

By introducing for ¢(r) a definite function which vanishes for
7 >t, or, at least approximates to zero with sufficient rapidity as r
increases, we should obtain from (40) the value of the virial-coef-
ficient B for that particular law of force. The case mentioned in
the beginning of this section of molecules which can be regarded
as rigid spheres of central symmetry exerting upon each other
central attractive forces‘) which are a function of the distances
between their centres, can be obtained from this result by allowing
g(r) to approximate- to — o for r less than o (6= diameter of a
molecule). We then get

4 +
B= a | ehw = ot hf eey (r). so dr}; .. * a
in which v=g@(o), so that —v represents the potential energy of
a pair of molecules which are in contact.

In this expression for B the first term represents the collision
virial which, as first shown by Remncanum, becomes, on account of
the attractive forces, e” times greater than the value found in $3;
the second term represents the attraction virial, and is negative since
g' (r) is negative for attraction.

for @ i). = - *), in which g is greater than 3, and for which

c 5
v =—.,, this becomes
o7

Pee ey Fo See
——— SSS ED —
‘eeeces fo8 2 Bags

5 (hi). (42)

“Ye 1
which gives, on replacing h by ——, a series of ascending powers

kpT
of, 7,

§ 6. The virial-coef ficient B for rigid smooth molecules of central
symmetry, having at their centres an electric doublet of constant
moment.

In this section we shall regard the molecules as rigid smooth

1) These formulae also hold for repulsive forces and for forces which are for
certain distances attractive, for others repulsive.

2) The force which two molecules exert upon each other as a ie is then
proportional to r—(g+1). On the supposition of forces operating according to the
above law between the volume-elements of spherical molecules supposed homo-
geneous the resultant could not be regarded as a function r—9 (with g constant)
of the distance between the centres.

265

spheres of central symmetry, each having at its centre an electric
doublet; we shall assume that thg distance between the two poles
of the doublet is negligible compared with the dimensions of
the molecule, while the moment of the doublet is nevertheless so
large that it must be allowed for by introducing terms into the
equation of state to represent the mutual action between the doublets.
In all considerations introduced into the present section we shall
regard the moment of the donblet as constant. A model of a mole-
cule which, in so far as its externa! action is concerned, could be
regarded as approximating closely to such a doublet, would be given
by a non-conducting sphere with a uniform distribution of positive
electricity (or with the charge distributed in concentric shells, each of
constant density) in which there is an immovable electron at a very
small distance from the centre (the centre coinciding with the centre
of gravity). The terminology of this section, however, will be chosen
with reference to the supposition of two poles infinitely close to
each other ‘electric doublet) at the centre of the sphere. External
action will be calculated as if only electrostatic forces were invol-
ved. In this supposition the mutual action of two molecules may
be treated as being governed by the HamiLton equations. The
assumption would have to be more closely verified in the further
development of the theory of the action of a model such as the one
just described.

Van peR Waats Jr.*) has considered such a system as the one
here described, and calculated the mean attraction between two
molecules when these have assumed orientations with respect to the
axes of the doublets which are in accord with the condition for heat
equilibrium; he showed that the law of decrease of this attraction with
increasing distance must be more rapid than r—+,

The object of the present section is to deduce the virial-coefficient
B by the method indicated in § 2.

The group macro-complexion is first determined by (22) as in the
treatment for smooth ellipsoids in § 4.

In order to be able to evaluate the potential energy it is necessary
to subdivide the n, molecules present in the volume-element dv,
into n,, single molecules (cf. § 5), and 7, molecules which belong
to molecular pairs, and exert forces upon each other of such magni-
tude that they must be allowed for in the determination of B. We
shall once more assume that cases in which one molecule is acted
upon by more than one other molecule with forces sufficiently

1) J. D, van DeR Waats Jr., These Proceedings June, Oct. 1908, March 1912,

266

large to influence the result are of such rare occurrence that they
may be neglected altogether. In so far as the fact that the field of
a doublet does actually extend to infinity introduces difficulties into
the treatment, we shall, where necessary, conceive that the field is
annihilated at distances greater than r= oo so that we may regard
x as the radius of the sphere of influence of the doublet.

Nb - . :
The —> pairs we shall have to separate into various groups. We

shall determine a definite pair of molecules in the following way:

1 by the distance 7 between the centres,

2 by the angles 6, and 6,, which the axes of the doublets make
with the line joining their centres. In this we shall choose the direc-
tion of a line joining the centres of two molecules as positive for
the first molecule when it goes towards the other, and as_ positive
direction of the axis of the doublet the direction towards the positive
pole. The angle concerned will be taken as lying between O and a;

3 by the angle g between the two planes each of which con-
tains the axis of one of the doublets and the line joining their centres.

pi ae
s
3

oe a eS

Fig. 4.

Values lying between O and 227 will be given to this angle. We
can specify the angle g uniquely for any pair of doublets in the
following way: Let AA’ and LB’ (fig. 4) represent the pair of
doublets, A and B being the centres of the molecules, and A’ and
B’ being in the positive direction along the axes of the doublets.
Let us now take up our position either at A or B, say at A, and
project AA’ and BB’ upon a plane passing through £6 and perpen-
dicular to AB; the angle g is then that angle through which the
projection of BS’ must turn in the positive direction as seen from
A in order to coincide with the projection of AA’.

The number of pairs of molecules which ‘are present” in a
definite element of the space determined by the coordinates 7, @,,
6,, , that is to say, the number of molecule pairs with a definite
“space freedom (drd6, d0, dp), we shall indicate by putting the

267

number corresponding to this freedom immediately after the index /.
The group macro-complexion is then determined as follows :

in dv, dw, (dq, dr,;), “there are” my, single molecules
M1 Molecules belong-

ing to pairs of molecules with

the freedom (dr d6, d6, dy),, ete.

(43)

Determination of the micro-complexion :

For this as in the treatment of smooth ellipsoids at the conclusion
of § 4 we subdivide the respective spaces into equal dw’s, equal diw’s,
equal do’s, equal dy’s, equal dp,’s and equal (dq; dr;)’s. If these are
determined for the position of each molecule, we have then a.definite
micro-complexion. We may refer to § 4 for the proof that the micro-
complexions thus determined represent cases of equal probability.

The number of individual macro-complexions in the group macro-
complexion is

Myj10/ (aggre! cuace &

The number of micro-complexions in the individual macro-complexion:

To determine this the macro-volume-elements are again to be
considered as independent of each other. Let * represent the number
of equal micro-volume-elements dw,,... in dv,, « the number of
equal elements of surface of the unit radius sphere, points on whose
surface give the directions of the axes of the doublets, r the number
of equal elements dz (y= the angle representing the rotation of the
molecule around the axis of the doublet), and wv’ the number of equal
elements dp, (p; = the speed of rotation around the axis of the doublet).

We shall first ascribe to each molecule its dm, its do, its dy, and
its dp, for each micro-complexion ; we shall then give it its div and
its dq, di, as specified by (48). The latter is then without influence
upon the number of micro-complexions.

In dv, we have to place n, specified molecules :

My = May TMs Pees + Ma eee «ea oe (44)

Of these 7, specified molecules are single

Ni : é belong to pairs with the freedom
: (dr dé, dé, d¢),
if Nig = Nj} 14 -— Ny19q + >» N14 — a ar

2 (45)
My = Naw + Num -- Maw - - -
The placing of the 2, molecules (for the approximation here

18
Proceedings Royal Acad. Amsterdam. Vol. XIV.

268

employed cf. § 5) gives rise to
4

x sy Na IT 1 —
(xurr ) Fa ] t a

possibilities.

Let us now place the m,; molecules. Again we may remark that
one of these molecules can go to form a pair only with another
molecule of the same group. These pairs can be formed in

nye /

nibl

9 2 181 !
2
different ways (cf. § 5),
Let us consider the first pair of molecules in one of these com-
binations in particular. For the first molecule there are

( 4
3
SS LEG

x |l— nr. uvy'

VY)
places available in the proper space (cf. § 3). When the first molecule

has thus been placed and given a definite orientation, there are on
account of the freedoms d6, dr

227° sin 6,d0,dr
4
dv

places in space available for the second molecule. On account of
the freedoms d6,dy there are

sin 6,d0 dep sin 0,46 ,dyp
do Sore .
0 4x

orientations possible for this second molecule for each of its positions
in space.

y and p; in addition give rise to the factor ry’. We thus obtain
on the whole

Ste an 6, sin 0, dr dO, dO, dg -

dv, 2 dv,

(zu vr’)? | 1—n,

possibilities for this pair of molecules, to which we affix the factor

269

— re"

oe (ist 1) dv
st

other pairs of molecules, we finally obtain

, 4s was done in §5. Doing this in turn for the

4 3
: ni t=n,—1 3 shit
a pe ta
Maia! Mi! +--+ dv c= dv,
"101
mis! r sin O, sin 0, dr dO, dO, dg 3
em (a 4 Ee a 3)
79, 9y9 "141 2 dv,

2 M1)
ss 1
2 (=e),
where 7 indicates that the product must be taken for all freedoms
7,949
(elements in a corresponding space) determined by 7,6,,90, and ¢
respectively. The notation of this expression has been simplitied by
omitting the index which is used to indicate the special freedom
(dr dé, d0,dy) except in the notation referring to the number of
molecules. From (46) we obtain (cf. §5 for the omission of terms)

loggW = — 12 l0Je M14 —N1111 loge Ni +++ — > —

Nyy) Nyy) Nyy) r° sin @, sin 0,drd6,d6 dep ;.
+> loon — — + —log. —— _____* > * 4

Changing the sign we obtain an expression for the BoLtzMANNn
fi-function for this system.

~The equilibrium state:
The energy condition gives
Us SL (Mya + Mi +--+.) uw + LY L{ mn ms = const. (48)
dv dw dv r6,$x2
where
Uli = 4m (§,° + 4,7 + 6,7) + 4 Br (qr? + 1’) represents the kinetic

Me”
and uw, = 7 (2 cos, cosO, + sin, sinO,cosg) the potential energy

m is the mass of a molecule, B; the moment of inertia around an

axis perpendicular to the axis of the doublet, and m,. the moment

of the doublet. From the condition for a maximum value of log, W,

together with -the conditions (48) and n = const. and the equations
18*

270

(44) and (45) the deduction of the distribution in the state of equi-
librium and the calculation of the entropy are mutatis mutandis made
as in § 5. We shall give only the following results :

The number of pairs of molecules with freedoms dr, d0,, d6,, dp
is obtained from

n? In, r® sin O, sin 6 ,drd6,d0,dp

N41 — py? é 9 dv, > eer (49)
on division by 2.
From
n? (hm ‘zh By —hu.4,+u,,) 778in8 ,sin8 ,drdO ,dO,dp
niu 5 J ae wil Tél rg ae Pe ee (50)

it follows that the distribution of the velocities (including q, and ry)
is independent of the position of the molecules relative to each other.
We aiso find that

n (hm hB; n hu
eget || aye gna rie Ple dv,dw,dq,4rr4, + (51)

in which

on t 270

/ —hu
P= if {fe "9? sin 0, sin O,drd0,d6,dp,. . . (52)

000

- where the summation with respect to 7, @,,0,,@ has been replaced ©
by a corresponding integration.
Macroscopically the distribution throughout space is uniform.
Elimination of A from

5 uf -
s = nkpln v Sree kplnh + kphu + se ee Pe aes
v

2v 3

= 5n 176 i232)

a ee ere ee ee eee

j 2h 2
in which

tn mt 270

1 his) ae

Q == e wu, 7 sin 0, sinO, drdO,dO,dp .« . «. « « (94)
¢00 0

gives the canonical equation of state.

From (53) we again obtain 7 =

kp h-
The specific heat at constant volume in the AVvoGADRO state, y-A,

271

5
becomes — Rk, in agreement with the circumstance that both g, and
=

r,, but not p,, participate in the heat equilibrium in consequence of
the torques exerted by the doublets upon each other.
For the thermal equation of state we again get (39), with 5 now

equal to
1 P vy
a oy n ae —" |, (55)
in which
{aed LS ei |
a if {{[e —-1) r? sin O, sin O,drdO0,d0,dp . . (56)
¢ 00 0

P’ is convergent for ro, so that as far as (55) is concerned
the assumption is no longer necessary that the field of the doublet
is annihilated at distances greater than t (the same is true for
(53) if P’ is introduced in the expression for s).

In order to evaluate the integral P’ we shall write 2 cos 6, =
gcosw and sm0,=gsny (9 20,0 p<a), so that

2 cos A, cos 0, + sin 6, sin @, cos ~ = g (cos W cos A, + sin W sin A, cos (p).

In the plane containing the line
BA and the axis of the doublet at
A draw an angle CBE=y, and
introduce the angles HAD = & and
CED = gq as the new independent
variables instead of 0, and g '). The
integration with respect to g' gives 227.

Fig. 5. Integration with respect to # can
also be done with ease. Let us then substitute g as independent
variable instead of 6, and we get

in which
2
2 dg

= ——= | —— (¢9—e-9 — 2c9),
Y3d Y7—l i
; 1

1) This comes to the same thing as introducing the angle between the axis of
the doublet B and the field at that point caused by the action of the doublet A.
Cf. Van per WaAALs JR. These Proceedings June 1908.

272

hm.* : oe
—. We can, ina way similar to that used by vAN DER

if ‘¢ is) hexe ===
ss

Waats Jr. in solving the integral developed in his paper, evaluate G
in terms of a series by expanding eY —e ‘7 into a series of ascending
powers of g. The proof of convergence can be given in the same
way as by vAN DER Waals Jr.

If we write

Me”
ye

a (57)

for the potential energy of two molecules in contact with the axes
of their doublets parallel and at the same time perpendicular to the
line joining their centres and if we take as our upper limit r=
we obtain

1k aay, 1 ie is ;

Bs cee 0 ta q, (hv)? — 35/9 (hv)* — |]
(58)

11 agit d

aay tee arg et os ane

in which

nal+l.5.8 =2
1 1 24
, Pee ae ei ate ha cee =
1 ES =. Le a nee
i ae ae ge Se a as
1 1 4
g = gt ian 8S see? ne ieee a ae
or
yee tee 1 2 hse te See fis (Av)*...}-9-) (ag)
2 5) 3 75 55125

1 :
in which / should be replaced by eae if 5 is to be obtained as a
=

function of 7. We now obtain a series containing only the even
powers of T—! ‘ef. § 5).

Just as in § 5 we can now separate the terms which represent
the collision virial and the attraction virial in B.

Should the law of dependence of 5 upon temperature for a dia-
tomic substance in the region for which y,4 =‘/, 2‘) be found expe-

1) In Communication N°. 109a@ § 7 (March ’09) the dependence of B upon.tem-
perature is given for hydrogen as deduced from the isotherms of KAMERLINGH
Onnes and Braak. With regard to the specific heat, however, we must remark
that measurements made by Evcken, Berlin Sitz-Ber., Febr. 1912, p. 141, of the

a
ho

273

rimentally to agree with that deduced from (59) one could get a
fair conception of the molecule which would at least give this Jaw
of dependence upon temperature by calculating v from the tempe-
rature of the Boye point (if within the specified region) and 6 from
the terms in the expression for £ which are independent of 7’, and
then me, the moment of the doublet; from this one could, for in-
stance, calculate the distance of the electron from the centre in the
case of the molecular representation indicated at the beginning of this
section. Further discussion of experimental results, however, must
be postponed till a later paper.

Physics. -— /sotherms of monatomic substances and of their binary
mictures. XIII. The empirical reduced equation of ‘state for
argon. By Prof. H. KAMErtineu Onnes and Dr. C. A. Crommenin.
Comm. N°. 128 from the physical laboratory at Leiden.

In a previous paper*) we indicated the desirability of obtaining
from the mean reduced empirical equation of state for a number of
normal substances which we have ealled VII. 1.*), a mean reduced
empirical group-equation applicable to the monatomic substances. As
a first step in that direction we now give a special reduced empi-
rical equation for argon which we shall call VII. A. 3. and which
embraces data obtained from observations made in both vapour and
gaseous states. °)

In previous communications similar special equations have been
published, viz. one for carbon dioxide *) in gas, vapour, and liquid
states, and one for hydrogen *) which embraced all available obser-
vations on the gaseous state. The important part as convenient sum-
maries of all available experimental data played by such special

increase of temperature undergone by a quantity of gas contained under high
pressure on the addition of a measured quantity of heat showed that even at
200°K. y,4 is for hydrogen considerably below °/. R, while at 60° K. the value
obtained was */, R. It was mentioned during the discussion at the Conseil Soxvay,
Nov. 1911, that Professor KamertincH Onnes and myself had undertaken an inves-
tigation of y,, by Kunpt’s method for hydrogen at temperatures down to that of
liquid hydrogen, but this investigation has not yet been completed.

1) Proc. March 1911. Comm. N°. 120qa.

2) Suppl. N’. 19 p. 18.

3) Proc. Dec. 1910, Comm. N°. 118) and C. A. Cromuetiny, Thesis for the doc-
torate, Leiden, 1910.

4) Arch. néerl. (2). 6. 874. 1901, Comm. N°. 74.

5) Proc. April 1909, Comm. N’. 109q.

274

equations in all sorts of thermodynamical calculations concerning the
particular substance within the limited range through which the
equation holds, makes it essential to obtain the best possible agree-
ment between the equation and the results yielded by experiment.
As the form VII. 1. was chosen for this equation with a view to its
relationship to other investigations concerning the equation of state,
it was fortunate that, for the comparatively smal] region of tempe-
rature covered by the argon observations, there were still the same
number of coefficients available for the equation as had been found
required to give good average agreement over the whole region
covered by the equation of state for various different substances.

In the paper’) whicb contained the isotherm determinations for
argon we have already given preliminary values: for the individual
virial coefficients 44, B4, ete. of the equation

Bar a. ae Bi ack
VA ay or oe ay
as directly calculated from the observations for each individual isotherm.

The reduced virial coefficients 3, &, ete. have now been calculated
from the virial coefficients By, C4 ete. as functions of the reduced
temperature ft, which comes to the same as the evaluation of the
constants in the equations

P= A, aa

7
en

6 b 6
Oita sa eat es Ge

¢ C ¢
S=¢f+¢+—4 — :
t od

t® ete.

By this the coefficients are adjusted to the observations with respect
to both temperature and density.

We may here give a short resumé of the.manner in which these
calculations were carried out.

As in the present instance the final terms of the polynomial

B
pug Ag+ At etc. exert but a slight influence and therefore
vA

can ~be calculated only approximately from the observations, it was

1) Proc. Dec. 1910. Comm. N®, 1185 and C. A. Crommenin, Thesis for the
doctorate, Leiden 1910.

*) Proc. June 1901, Comm. N°. 71 and Arch. néerl. (2) 6. 874 1901, Comm.
N°, 74.

As can be seen a 5th term has been added to the equations there given. For
the formulae connecting By and 3, Cy and G, etc., reference may be made to the
former paper. In the present paper we shall use chiefly the reduced virial coeffi-
cients which are to be preferred for the adjustment of the values of the coefficients.

275

best to begin with the adjustment of these terms. The fairly great
changes which these terms as a rule undergo, have but a slight
influence upon the values of the initial coefficients, while, on the
other hand, small changes made in the initial coefficients in the
process of adjustment occasion appreciable alterations in the coefficients
- of the final terms, and so the adjustment of the values of the final
coefficients would become more difficult than it is as a rule at small
densities.

In the case of argon the coefficients © and § need not be taken
into account, for their valnes have been adopted from VII. 1.*) and
consequently they have already been adjusted to the observations.
Our calculations therefore began with the adjustment of D, which,
as a glance at the values of Dy, already published’) will clearly
show, had to be done in a somewhat arbitrary manner. Some of
these D4’s have been taken from VII.1. The values of Dy, at the
lower temperatures, which were very irregular, were now plotted,
while for t—=6 the Dy, value from VII.1 was included. In this
way values of D4 or D were graphically smoothed, and then the
deviations of these smoothed values from VII.1. were represented
as functions of the reduced temperature by a linear equation

AD = Ad,t + Ad,
(in which

AD =D, — Dvii.

Ad, = Sia — OVI

Ad, = 02.4 — de.vit.1)

In this way 9;,, and teq were calculated as functions of the redu-
ced temperature, while 3.4, 4, and 55., were taken from VII.1.

The values of ®D adjusted in this way were then converted into
D, and were used in the first place to get an idea of the mag-
nitude of the corrections to be applied to the values of 3 and €so
as to give the best possible agreement with the observations. When
this was done we could then proceed to the adjustment proper of
the values of By and (4, or rather of 3 and € according to the
formulae (Ij.

As can be*seen from what follows, this process yielded values of
the coefficients which, especially as regards the ¥ coetficient, did not
differ much from those of VII.1. while, at the same time, a compa-
rison with the experimental data of the reduced equation of state

1) Suppl. N°. 19 p, 18.
2) Proc. Dec. 1910, Comm. N® 1180.

276

thus obtained gave thoroughly satisfactory results. The results of all
these calculations viz. the coefficients 6,, 6,, 6,, 6,, 6,,¢,,¢, etc., of the
equation VII. A.3., the virial coefficients obtained from these, and
finally, the comparison of VII. A.3. with the experimental data
are given in the following tables.

The figures italicised in the tables are those which have been
taken from VII. I.

TABLE |. Coéfficients of the equation VIII. A. 3.

6 >< 103 | + 137.193 | — 146.732 | — 505.734 | 4+ 94.358 | — 17.8488
c>< 1011 | + 97.9740) — 528.608 | + 836.166 | — 315.182 | + 77.4006
d< 1018 | + 236.30 | + 421.825 | — 903.004 | + 367.7055; — 178.5625
e< 1025 | —r588.948 | +5725.652 | —4331.720 | + 864.610 | + 40.449
f>< 1032. | +7685.000 | —6477.876 | +6019.629 | —1s12.028 | + 144.537
TABLE II. Virial coéfficients of equation VII. A. 3.
s Ay B 4X 103 C 4X 108 D 4X 1012 EAA
+ 20.39 | + 1.07545 | — 0.60178 | + 0.76768 | + 6.78079 | + 7.6045 | — 4.35430
0.00 | + 1.00074 | — 0.76763 | + 0.91203 | + 5.93894 | + 8.7327 | — 4.98937
— 57.72 | + 0.78922 | — 1.30257 | + 1.50907 | + 3.28679 | + zo. 5255 | — 5.02409
— 87.05 | + 0.68174 | — 1.62411 | + 1.92013 | + 1.18908 | + zo. 5566 | — 3.93044
— 102.51 | + 0.62511 | —1.81201 | + 2.16108 | + 0.72267 | + zo. 4013 | — 3.10842
— 109.88 | +0.59810 | — 1.90692 | 4+ 2.28115 | + 0.20350 | +- z0. 3251 | — 2.69045
— 113.80 | + 0.58372 | — 1.95896 | + 2.34653 | — 0.09396 | +- 10.2947 | — 2.47655
— 115.86 | + 0.57617 | — 1.98675 | + 2.38134 | — 0.25708 | + 20.2837 | — 2.35600
— 116.62 | -+ 0.57340 ; — 1.99711 | + 2.39431 | — 0.31873 | + 10.2806 | — 2.31432
— 119.20 | +0.56393 | — 2.03255 | + 2.43867 | — 0.53362 | + 10.2759 | — 2.17669
— 120.24 |-+0.56012 | — 2.04701 | + 2.45677 | — 0.62312 | 4+ 10.2764 | — 2.12239
— 121.21 | + 0.55658 | — 2.06056 | + 2.47376 | — 0.70808 | + 20.2783 | — 2.07246
— 130.38 + 0.52296 | — 2.19283 | + 2.64178 | — 2.10863 | + zo. 3966 | — 1.66293
| — 139.62 /+ 0.48909 | — 2.33484 | + 2.83477 | — 2.41358 | + 10.8045 | — 1.42979
— 149.60 | 4 0.45252 | — 2.50118) + 3.10431 | — 2.78849 | 4- 11.8440 — 1.53961

es a

277

nn ns Sp
eect |

TABLE III. Comparison of equation VII. A. 3 with observation.
rs a
- = d Oo a ee 0—C d O—C
A in % A in% | in % in %
+ 20°.39 0°.00 — 57°.72 — 87°.05
20.499 | — 0.07| 2).877| + 0.05 | 23.509) + 0.11} 25.152| +0.17
25.759 | + 0.01 | 26.581 | — 0.02 | [28.575 | — 0.16] 34.467 | + 0.02
32.500 | + 0.14} 32.302 /+ 0.05 | 33.793 | — 0.05 | 55.822 | — 0.10
35.330 | — 0.09 | 37.782 | — 0.06 | 48.116 0.00 71.444 | — 0.06
35.759 | — 0.13 | 51.840 | — 0.15 | 64.948 | +0:06| 94.625 | — 0.14
47.319 | — 0.04 | 65.325 | — 0.21 | 90.695 | + 0.11 | 119.84 | + 0.19
59.134 | ++ 0.07 |
59.250 i 0.06 | |
| |
— 102°.51 | — 109°.88 — 113°.80 — 115°.86
25.571 | + 0.19 | 26.242 | -+ 0.14! 67.078 | — 0.16 | 69.947 | — 0.23
35.077 | 0.00 | 34.807 | + 0.26 | 88.889 | —0.13| 91.308 | — 0.18
(47.893 | + 0.47]| 65.142 | — 0.54 | 106.68 | — 0.34! 108.02 | — 0.35
[53.752 | + 0.48}]| 66.530 | — 0.29 | 129.17 | — 0.25 | 131.51 | — 0.38
62.240 | — 0.05 | 87.176 | + 0.01 | 152.71 | — 0.14 | 155.12 | — 0.27
[69.954 | + 0.50]|} 102.76 | — 0.20; 155.40 | — 0.07 179.94 | — 0.06
84.002 | — 0.08 | 125.56 | — 0.09 | 182.13 | + 0.37 | [183.35 | + 2.40]
95.802 | — 0.17 | 148.32 | + 0.03 | 184.82 | + 0.27 | 235.47 | + 1.16
115.88 | — 0.17} 152.79 | — 0.26 | 212.99 | + 1.02 | 319.52 | + 0.20
135.65 | — 0.01 | 180.84 | + 0.37 |
158.01 | -+ 0.13 | |
| | |
\e
— 116°.62 | — 119°.20 | — 120°.24 | — 1219.21
| |
26.480 | + 0.25 | 26.871 | + 0.24! 72.627| — 0.04! 27.326 | + 0.24
34.939 | — 0.01 | 34.965 + 0.24 82.816 | + 0.10 35.283 + 0.25
68.630 | — 0.13 | [70.314 | — 0.25]) 99.246 + 0.03 71.459 — 0.10
90.563 | — 0.21 | 70.481 | — 0.66 | 118.51 | —0.10 85.580 — 0.05
110.19 | — 0.46 | 70.580 — 0.56 | 136.31 | — 0.02 100.33 — 0.03
133.69 | — 0.39} 83.257 | — 0.63 | 165.79 | — 0.09 [123.85 | — 0.19]
159.71 | — 0.25] 96.834 | — 0.31 | 206.57 | + 0.82 | 148.95 | — 0.10
161.75 | — 0.35] 98.863 | — 0.83 | 280.25 | + 3.22 | 170.05 | — 0.16
[186.15 |--+ 0.13]| 124.97 | — f.10 | 338.95 | + 0.89 | 234.13 | + 1.73
210.02 + 0.64 [143.71 | — 0.44] 333.15 | =f 1.93
260.61 | + 1.74]| 156.36 | — 1.07 |
331.29 | — 0.46:|[172.25 | + 0.07]
| 222.69 | — 0.04
275.02 | + 1.11
| 356.892) == 1.72" |
|
= 1300.38» _| a el — 149°.60
| | |
27.394 | + 0.30} 28.122} + 0.12 | 29.183 |; — 0.03
[31.583 |. — 0.44]| 35.573 | — 0.10 | 34.646 | — 0.14
34.726 | + 0.24 | |
55.807 | + 0.20 | | |
65.125 + 0.14 | |
77.821 | + 0.77 | | |
; — 0.81], |

- +300

278

The accompanying diagrams exhibit the reduced coefficients 3 and
© as functions of the reduced temperature t within the region of
observation for argon, that is, from f= 2, to t= 0.8. The curves
drawn through the circles refer to the special argon equation VIL. A. 3,
those through the triangles to the mean reduced equation VII. 1. and
those through the squares to the special equation for carbon dioxide,
Vi Bale)

As the experimental data at present employed are very limited in
scope we must, in the meantime, be somewhat chary of drawing
conclusions as to the mutual actions of molecules when they come
within each other’s immediate neighbourhood from a comparison of
VII. A. 3. with the equations for the other substances shown in our
diagrams. In the case of the % coefficient the absence of data at
small values of t is specially felt *), while as far as © and the special
argon equation are concerned it is the absence of data towards the
side of high densities. Equation VII. A.3 can, therefore, be regarded
only as a first step towards the formation of the empirical equation
of state for argon.

COMONTL.A2 eCOWS1 A
6y eee = 2S sui

aif

+350

+250

1) Arch. Neérl. (2), 6, p. 874, 1901. Comm. N°. 74.
2) We hope to be able to publish shortly some experimental results to supply
this deficiency.

nt iD A ie ea Be

TC,
sa
|

a 4,90 4,50 4,70 1,60 4,50 1,40 1,30 4,20 110 1.00 0.90

We may still take it, however, that we have advanced a step

since our previous papers’). It was there found that deviations of

the isotherms in the gas state were systematically connected with
deviations of the diameter and of the vapour pressure curves (with
which the deviations of the latent heat of vaporization etc., are
connected by thermodynamical formulae), while in the present case
a much simpler survey is obtained of the deviations of the isotherms
at densities at which the virial coefficient D need not be taken into
account. These are shown in the two curves for 3 and ©, which
therefore play pretty much the same part in this particular region
as the boundary curve for equilibrium between liquid and vapour.
And it is again striking how the various substances arrange them-

1) Proc. March 1911,-Comm. N°. 120 and Proc. July 1911, Gomm. N°. 1210,

280

selves as far as these deviations are concerned according to the more
or less complicated structure of their molecules. The curves for VII. 1
in the region of reduced temperature to which the diagrams refer
are obtained chiefly from isopentane and ether, substances which
have very complex molecules; after these come, in the order given,
carbon dioxide, with an undoubtedly less complex molecule, and
finally argon. Clearly, just as was the case with the deviations which
were encountered in a previous paper‘), one must look for the
explanation of this in a real or apparent compressibility which
diminishes in magnitude as the molecule becomes less complex in
shape or structure, or in a characteristic behaviour of the attraction
potential determined by this peculiarity.

We hope to present further communications shortly giving results
of calculations of various thermodynamical quantities which may be
made from the equation now given within the limited region for
which it holds.

1) Proc. July 1911. Comm. N°. 1210.

(September 2, 1912).

KONINKLIJKE AKADEMIE VAN WETENSCHAPPEN
TE AMSTERDAM.

PROCEEDINGS OF THE MEETING
of Saturday September 28, 1912.

DOC

President: Prof. H. A. Lorenrz.
Secretary: Prof. P. Zeeman.

(Translated from: Verslag van de gewone vergadering der Wis- en Natuurkundige
Afdeeling van Zaterdag 28 September 1912, Dl. XXI).

CO Sa A ES:

J. Syaprer: “Comparative researches on young and old erythrocytes”. (Communicated by Prof.
H. J. Hampurcer), p. 282.

W. J. pe Haas: “Isotherms of diatomic gases and of their binary mixtures. X. Control
measurements with the volumenometer of the compressibility of hydrogen at 209° C. p. 295,
XL. On determinations with the volumenometer of the compressibility of gases under low
pressures and atlow temperatures”. (Communicated by Prof. H. KAMERLINGH ONNES), p. 299.

H. Kameriincu Onnes and Bencr Beckman: “On the Hatt-effect and the change in the
resistance in a magnetic field at low temperatures. I. Measurements on the Ha.t-effect
and the change in the resistance of metals and alloys in a magnetic field at the boiling
point of hydrogen and at lower temperatures”, p. 307. — II. ¥“The Hari-effect and the
resistance increase for bismuth in a magnetic field at, and below, the boiling point of
hydrogen”, p. 319.

H. Kameruincu Onnes and E. Oosreruutis: “Magnetic researches. VI. On paramagnetism at
low temperatures”, p. 322.

Hi. pu Bors: “A theory of polar armatures”, p. 330.

C. A. PeKkeLaarinc: “Influenee of some inorganic salts on the action of the lipase of the
pancreas’, p. 336.

C. E. A. Wicumayn: “On rhyolite of the Pelapis-islands”, p. 347.

L. E. J. Brouwer: “Continuous one-one transformations of surfaces in themselves”, (5th
Communication), p. 352.

A. Smirs: “Extension of the theory of allotropy. Monotropy and enantiotropy for liquids”.
(Communicated by Prof. A. F. HoLLEeman), p. 361.

A. Smits: “The application of the theory of allotropy to the system sulphur”, IL. (Communi-
eated by Prof. A. F. HoLLtEman), p. 369.

A. Sits: “The inverse occurrence of solid phases in the system iron-carbon”. (Communicated

by Prof. A. F. Hortemay), p. 371.

E. C. Scuerrer: “On the system ether-water”. (Communicated by Prof. J. D. vAN DER
Waats), p. 380.

E. C. Scuerrer: “On quadruple points and the continuities of the three-phase lines”.
(Communicated by Prof. J. D. van DER WAALS). p. 389.

H. Kameriincn Onnes and W. J. pe Haas: “Isotherms’ of diatomic substances and of their
binary mixtures. XII. The compressibility of hydrogen vapour at, and below, the boiling
poinv’, p. 405,

Ww. H. Keesom: “On the second virial coefficient for di-atomic gases”. (Communicated by
Prof. H. KAMERLINGH ONNES), p. 417.

Errata, p. 431.

19
Proceedings Royal Acad. Amsterdam. Vol. XY,

282

Physiology. — ‘Comparative researches on young and old erythro-
cytes.’!) By J. Snapper. (Communicated by Prof. H. J.
HAMBURGER.)

(Communicated in the meeting of June 29, 1912).

1. Introduction.

Of late years various investigations have been carried out with a
view to ascertain if there are differences between newly formed red
blood-corpuscles and those which have already circulated for some
time. For this purpose the blood was examined of animals which
had been made anaemic in some way or other. Since the loss of
blood must be made up for by fresh red blood-corpuscles, we may
depend upon it that the differences existing between the blood before
and after the artificial anaemia was effected, are caused by the new
formation of fresh red blood-corpuscles.

According to recent*) investigations there is. a difference between
new red corpuscles, formed after bleeding, and those formed after
blood has been lost by injections with blood poisons. -This difference
manifested itself especially when the capacity of resistance of the
blood-corpuscles was tested by means of hypotonic salt-solutions.
Whilst the blood-corpuscles of an animal which had been made
anaemic by poison-injections resisted the hypotonic salt-solution better
than the blood-corpuscles of a normal animal, this was said not to
be the case with those animals of which the anaemia had been
caused by bleeding.

There are indeed reasons to assume that the regeneration after
poison-injections will be stronger than after bleedings. Yet it is im-
probable that the young red blood-corpuscles formed after bleeding,
should not be distinguished in the same way from the old erythro-
cytes — though it may be in a slighter degree — as those formed
after poison-injections. These slighter differences too, may be of im-
portance, however. As we know, the anaemia effected by injections
of poison causes the number of blood-corpuscles to decrease so
strongly that sometimes only 16°/, of the original number are left.
It is not improbable that after such an extreme loss of blood the
regeneration may be an abnormal one. On the other hand the pro-
perties of new red blood-corpuscles, formed after a smaller loss of
blood will bear a greater resemblance to the properties of young
red blood-corpuscles formed under physiological conditions.

1) A more detailed account of these investigations will be published elsewhere.
2) Irami and Pravt, Biochem. Zeitschrift, Bd. 18.
SATTLER, Folia Haemat, 1910.

283

In order to discover these minuter differences it was necessary to
subtilize the method. For this purpose the foliowing considerations
were held in view. In the experiments mentioned above only the
maximum and minimum capacity of resistance of the young erythro-
cytes had been determined.

The determination of this capacity is, as is generally known,
based on the following facts.

When red blood-corpuscles are suspended in a salt-solution with
an osmotic pressure less than 0,9°/, NaCl, they absorb water which
causes them to swell. The lower the osmotic pressure of the salt-
solution, the more water they will absorb. At last they burst and
the haemoglobin, contained in them, enters the solution. The lower
the osmotic pressure of the medium in which they can only just
maintain themselves, the greater the capacity of resistance of the
red blood-corpuscles. Seeing that not all the blood-corpuscles have
the same capacity of resistance the minimum capacity of resistance
of the blood is expressed by the most concentrated Na Cl-solution
which already causes haemolysis. In this solution the weakest blood-
corpuscles lose their haemoglobin. The maximum capacity of resistance
of the blood is determined by the NaCl-solution in which the hae-
molysis is complete, aud which cannot be resisted even by the
strongest blood-corpuscles. On/y these two salt-solutions have been
determined in the above-mentioned investigations: as to the degree of
haemolysis caused by the intermediate solutions every detail is wanting.

By determining this degree we succeeded in discovering some
qualities by which blood-corpuscles, newly formed after blood has been
lost, are distinguished from the other, remaining ones. It was also
found possible to study the mechanism of the regeneration more
closely. The experimental method may be described as follows.

2. Experimental method.

The blood experimented upon was always that of rabbits. It was
obtained by a slight cut in the ear and defibrinated by being beaten
with 2 glass rods. A series of centrifugating tubes was filled with
5 em’ NaCl-solution in progressive concentrations, the difference
between two successive concentrations being 0.02 °/,. To these 5 em*
0.1 cm* of blood was added and the mixture was shaken thoroughly.
Then the solutions were left exposed to the temperature of the room
for a few hours; subsequently they were centrifugated. In the tube
where red blood-corpuscles no longer settle at the bottom, the haemo-
lysis is complete. In the other tubes, where blood-corpuscles have

19*

284

remained intact, less haemoglobin has been dissolved. T’he degree of
haemolysis in these tubes is eapressed by the proportion between the
haemoglobin concentration in these tubes and the haemoglobin concen-
tration of the tube with complete haemolysis. These proportions can
be easily calculated by making use of the colorimetrical method
first suggested by Arruenius’). Thus a series of values is obtained
expressing which percentage of the complete haemolysis is caused
by each salt-concentration. (Table A). The progress of this haemolysis
may be expressed by a curve, the absciss of which is formed by
the NaCl-concentrations and the ordinate by the degrees of haemo-
lysis effected by each concentration. (Fig. 1).

Haemolysis
100%

90%

a1
oOo
oy

ea ee ee ee oe see ae ee ee EE ee ee
0.49% 0.51% 053% 055% 057% 0.59% 0.61% 0.63% a
Sol.

Fig. 1. Graphical representation of Table A.

TABLE A. Denoting the haemolysis caused by each
NaCl concentration.

0.63 > NaCl solution caused 9° haemolysis

0: 61s Ss > > 9» >
0.59 >» » > > 9» >
0.571 2. > > 42 » >
0.55 » > > > 55 » >
0.53.3), 3 > > 73 » >
1 Wa) AO > > 91 > >
0.49 >» » > > 100 » >

3. The capacity of resistance of old and new erythrocytes
against diluted salt-solutions.

The blood of an animal which has been made anaemic by bleeding,
may be examined in the same way as that of a normal animal.

1) ARRHENIUS and MapsEN, Zeilsehr. fiir Physikal. Chemie 1903.

285

After every bleeding the degree of haemolysis, caused by the
different salt-solutions, is determined. (Table B). When we also
represent these values graphically, the curve after every venesection
is found to have moved in the direction of the lower concentrations.
(Fig. 2). In the normal animal 80°/, is set free at a concentration of
0.49°/, NaCl. After one venesection the same solution causes 66 °/,
of haemolysis and after 2 venesections only 25°/,. In other words
whilst only 20°/, of the blood-corpuscles of the normal animal could
resist a NaCl-solution of 0.49°/,, the composition of the blood is
changed to such an extent after two venesections, that 75 °/, of the
blood corpuscles can still bear this concentration. Moreover, the
haemolysis was complete in the case of the normal animal at
0.47 °/, NaCl. After two bleedings the same 0.47 °/, NaCl solution
caused an haemolysis of 40°/, only. Hence there were in the blood
of the anaemic animal 100°/,;— 40°/,=60°/, blood corpuscles
which could withstand a less concentrated salt-solution than the most
resistant blood-corpuscles of the normal animal. These 60 °/, are,
therefore, blood corpuscles which were not met with in the non-
anaemic animal. They have been newly formed artter the bleeding;
they are the new blood-corpuscles which are to replace the lost ones.
Also the young blood-corpuscles, formed after a venesection, have an
increased capacity of resistance *).

1) About the quantity of haemoglobin new erythrocytes contain, more particulars
might be discovered by counting the number of erythrocytes which remain in
every concentration. If we compare this with the quantity of haemoglobin set free,
then it may be decided whe'her the old erythrocytes contain more or less haemo-
globin than the new ones. If for instance the old, that is to say the blood corpuscles
with smaller resistance contamed more haemoglobin, then in the more concentrated
solutions more haemogiobin would proportionately be set free than in the less
concentrated ones. Generally speaking, however, the values are found to agree
very well.

It is impossibie to settle this question conclusively, the method of counting, as
suggested by Zreiss-THoma, allowing of no closer determination than with an error
of 5°/). This causes deviations in the agreement of the values.

By means of the haematokrit-method it can be determined whether there are
any differences between the volumes of old and new erythrocytes. For this purpose
the volume of the cells, left after each concentration, was compared with the
number of erythrocytes left. Though here too, the values were found to agree, the
method employed in counting gave rise again to important inaccuracies
_ Besides, an equa] average volume of new and old blood corpuscles would be
the more remarkable since according to unpublished investigations of this institute
made by HamBuRGER and Kooy, the diameter of new blood corpuscles is greater
than that of old ones. ~

It would follow from this that new and old erythrocytes differ in shape.

286

Haemol.
100%

90%
80%
10%
60%
50%
40%
30%
20%

10%

041% 0.43% 0.45% 0.47% 0.49% 0.51% 0.53% 055% 0.57% sl
Sol.
1st Bleeding 26-III-1912, ------- 2nd Bleeding 1-IV-1912, =. =.= 3rd Bleeding 3-IV-1912,
Fig. 2. graphical representation of Table B.

TABLE B, denoting the haemolysis caused by each NaCl-concentration in the
normal and the anaemic animal.

4. New erythrocytes are built up from old ones.

The values and curves of fig. 2 may also be viewed in another
way. On the first day, for instance, a solution of 0.57 °/, NaCl causes
12°/, haemolysis, whilst at 0.55 °/, NaCl 18°/, of the erythrocytes
had disappeared. Hence there were then 18 °/, — 12 °/, = 6 °/, blood-
corpuscles which were just unable to withstand a solution of 0.55 °/,
NaCl. For 6°/, of the blood corpuscles 0.55 °/, NaCl is just the
minimum concentration they can bear.

287

0 I | a 6 ‘eke “ “ I p . 0 «“ “ «“ « “ a a“ “ «“ “ “ ts
« €Z a“ L aie a“ “ Pp . 0 « “ “ a “ a «“ “ a“ « “ “
a“ Lz “ 6 oo “ a“ Gp . 0 a“ “ “ a “ a“ « “ “ «“ «“ “
a“ c | “ 6 “ 02 a“ “ LP . 0 a“ a“ “ “ a“ a a“ “ a a“ a“ a“
“ .o I “ 62 a“ ron “ “ 6P . 0 « “ a“ “ “ a“ a“ “ “ a“ “ “
‘yd 0 I “ 9 I “ CZ “ “ I G . 0 « “ « “ a“ “ a“ a “ a“ a «
—_ a“ P “ WA “ “ CG . 0 « a“ a“ a“ “ “ a a“ “ a“ “ «“
— a ¢ a“ 9 a “ (efe) . 0 “ “ a a“ “ a “ “ a“ «“ “ «
— ‘19d ZI | 19d zI IDBN ‘JDd LG'O 7e ysang Ady} UOIeAyUIDUOD AaSUO.NS ATYSYs v vag [[IS uvd Ady} YS[IY AA
SS a en,
UO!IPISOUIA PIE UOIaSIUaA pug! UOTaSaUaA js] |

‘d Aqey pur Z “B]4 sv yiqqei ames ‘Dy ATGVL

288

Thus it ean be established for every concentration, which percentage
of the bloodcorpuscles lose their haemoglobin in one particular solution,
whilst they could withstand a solution which was 0.02 °/, stronger.

If, therefore, we analyse in this manner the values obtained with
the anaemic animal every day, then we shall find for which percentage
of the erythrocytes every salt-solution represents the minimum con-
centration. (See Table C). The 3 series of values obtained, may be
expressed again in curves (Fig. 3). There are always one or two
salt-concentrations representing for the greater number of erythrocytes
the minimum concentration they can bear. On the first day these
maxima are found at 0.53 °/, and 0.51 °/, NaCl, on the second day
at 0.49°/, NaCl, and on the third day at. 0.45 °/, and 0.43 °/, NaCl.

These maxima too move in the direction of the less concentrated
solutions.

30% 4

20%

10%

0.41% 0.43% 0.45% 047% 0.49% 0.51% 0.535% 0.55% 0.57% Mis
ol,

lst Venesection ------- 2nd Venesection §.—.—. — 3rd Venesection

Fig. 3. Graphical representation of Table C.

It follows from this

2nd Venesection 3rd Venesection

Bloodcorpuscles bursting just at 0.55 pCt. NaCl | equal decreased

“ . Ay sO a decreased ‘

m af ee Bs) lames = $ .

~ _ » iy O.49- ,, i increased k

- cs a 4 O41. ; decreased increased

- + i ke eae es newly formed .

+ . Pr = ee ‘ . _

~ = ip (04 4 . equal

Hence the number of strong blood-corpuscles increases as the
number of weak ones decreases. This increase on the one hand and

289

decrease on the other, run so exactly parallel, that we are at once
tempted to trace a connection between them.

Moreover the weaker ones are found to decrease much more
strongly than can be explained by mere loss of blood only. If no
regeneration were to take place, the proportion between the weaker
and the stronger blood-corpuscles would not be modified at all. At
the regeneration, therefore, the number of weaker bloodcorpuscles
must become relatively smaller since it is just the new bloodcorpuscles
which have a great capacity of resistance. Even if the entire loss of
blood had been made up for, this strong decrease of the weaker
ones cannot be explained. The rabbit weighed 2000 grammes, con-
tained, therefore, */,,, X 2000 = 160 gr. of blood. After 2 bleedings
of 15 ceM. (that is about 20°/, of the whole) of the 80°/, erythro-
eytes which are destroyed at 0.49°/, NaCl only 25°/, are found
back. These weaker bloodcorpuscles decrease, therefore, much more
strongly than can be explained by loss of blood only: they must be
used in some way or other. Since, moreover, the increase of the
stronger bloodcorpuscles runs parallel to the decrease of the weaker
ones, we may with a great amount of probability assume that the
young red bloodcorpuscles are built up out of the weaker ones.

Now it can also be explained why the young blood corpuscles
develop a greater capacity of resistance as more blood is withdrawn.
The weaker bloodcorpuscles decreasing very strongly after every
bleeding, the old bloodcorpuscles, which in the anaemic animal serve
to build up the new ones, are already much stronger than the old
bloodecorpusecles which are disintegrated in the normal animal for
this purpose. As the material out of which they are built up grows
stronger and stronger, the young blood-corpuscles are stronger too
after each venesection.

This also supplies us with one of the chief causes of the difference
between erythrocytes, formed after bleeding, and those formed after
poison-injections.

Owing to the abnormally strong decrease of the number of blood-
corpuscles after poison-injections, the newly formed cells could not
but become very strong — much stronger than after a few bleedings.

5. Also in the blood the regeneration greatly surpasses the loss.

Finally a conclusion may be arrived at as regards the degree of
the regeneration. After 2 venesections about 20 °/, of the blood
of the rabbit had been withdrawn. At the third bleeding 60 °/,
bloodcorpuscles were found with a greater capacity of resistance

290

than the strongest of the normal animal. After 20°/, blood has
been withdrawn at least 60°/, new cells are formed. In this case too,
the rule of Weicrrt, applicable in general pathology; holds good: the
regeneration surpasses the loss by far. Only with regard to blood
it cannot be deduced from the number of bloodcorpuscles, because
for each new bloodcorpuscle an old one has to be disintegrated.
Hence the absolute number of bloodcorpuscles per m.M*. can increase
but slowly.

Yet this strong regeneration of the blood-corpuscles too, has probable
a beneficial effect upon the organism. Though there is no difference
as regards size or haemoglobin-percentage, Morawitz has pointed
out the fact that while blood in normal circumstances can bind
chemically hardly any oxygen, the anaemic blood consumes rather
large quantities of O,’). Hence the new blood-corpusceles differ
qualitatively from the old ones, which appears besides from their
increased capacity of resistance.

6. LHifect of the serum on haemolysis.

a. The serum ts replaced by 0.9°/, NaCl.

Before drawing the conclusions, mentioned above, zt was necessary
to determine the effect which the serum has upon haemolysis. Mostly
we read that the serum contains substances which impede haemolysis”),
_ for when the blood-corpuscles have been washed with 0.9°/, NaCl-
solution, their capacity of resistance has decreased. If these substances
were really present, it might have a considerable effect upon the
capacity of resistance of anaemic blood. In anaemic blood there is
relatively more serum than in normal blood: the greater quantity
of serum would impede haemolysis more strongly, and this might
give an impression of a greater capacity of resistance.

It is indeed found that the capacity of resistance of the blood ts
lessened when it is washed with 0.9°/, NaCl. (See Fig. 4).

b. The serum is replaced by 4°/, glucose.

That this is not due, however, to the effect of the serum having
disappeared, but probably to osmotic changes, follows from the fact
that washing with an isotonic glucose solution (4°/,) does not modify
the capacity of resistance (See Fig. 4).

*) Morawirz, Archiv f. exper. Pathol. u. Pharmacol. Bd 60.

*) Gros. Ztschr. f. exper. Pathol. u. Pharmacol. Bd. 62.
SATTLER l.c,

291

Seeing that glucose cannot enter the blood-corpuscles, no ions can
leave them. A solution leaving intact the osmotic equilibrium does
not modify the capacity of resistance. Hence the removal of the
serum by washing the blood-corpuscles need not alter the capacity
of resistance.

The serum contains, therefore, no substances which impede haemolysis.

Haemolysis

100%

0.39%

blood which has not been washed
=—.—.== blood washed with 4% glucose.

0.41%

0.43% 0.47%

0.49% 0.51%

0.53% 0.55% 0.57% NaCl

wasce-= blood washed with 0.9% NaCi

Fig. 4. Graphic:] representation of Table D.

TABLE D. When the blood has been washed with 0.9 pCt. NaCl-solution, the same
NaCl-concentration effects more haemolysis than it does in blood which
has not been washed.

Blood, washed with a 4 pCt. glucose-solution has mo decreased capacity
of resistance.

Blood which had Blood washed — Blood washed
not been washed with 0.9 pCt. NaCl with 4pCt. glucose

At 0.57 pCt. NaCl

”

0.55
0.53
0.51
0.49
0.47
0.45
0.43
0.41

” ”

11 pCt. = y
11 ” cx | 7)
n

31 ” ra a
>)

44, 33 pct | 5
ae 3, )8
66 30 =
2

eae 6, |e
°

— 80 , =
oI

a 100 ” G

292

7. In the osmotic disturbance, caused by washing with 0.9°/, NaCl,
the tons of Ca play a prominent part.

This disturbance of the osmotic equilibrium of the blood-corpuscles,
caused by washing with 0.9°/, NaCl, is not effected if we wash
with 0.9°/, NaCl -+ 0.1 °/, CaCl, What was pointed out before in
the case of leucocytes, viz. the importance of ions of Ca’), is also
found to apply to the erythrocytes. Though only traces of Ca are
found in the erythrocytes, yet their capacity of resistance is con-
siderably modified if osmose causes these few ions to disappear.
Haem, 100%

90%
80%
70%
60%
50%
40%
30%
20%
10%

0.43% 0.45% 0.47% 0.49% 0.51% 0.53% 0.55% 0.57% 0.59% NaCl
Blood which has not been washed. ------- Blood washed with 0.9% NaCl
ea Blood washed with 0.9% NaCl +0.1% CaCl,.
Fig. 5. Graphical representation of Table E.
TABLE E. Blood which has been washed with a 0.9 pCt. NaCl-solution has a
decreased capacity of resistance.

Blood which has been washed with a 0.9 pCt. NaCl-+ 0.1 pCt. CaCl,-
solution has mo decreased capacity of resistance.

Blood which had Blood washed h Bleed set NaCl

ae been washed}with 0.9 pCt. NaCl +0.1 pCt. CaCl,

At 0.59 pCt. NaCl | = |. -"40-pCtr-— a
Re ey Pent | = re Se: eee
Bee eer | tt pct ae | 10 pct J ®
S.C. as Ae ie | 33> 4 | G0, Pee cme. >
Pye Bt at | ont oie oe ig IB ne 40, ° =
at Rees aera ea [ eaogt me ons te
Mare tee 1, eee h =100° ae
Ost) See Pel gare | = | 2 o ee
1 US ae} fe fe | 2. | = L “so 5
or ae) ae | 100, | = ioe

1) HAMBURGER and Hexma Biochem. Zeitschrift Bd. HI and Bd. VII.

Conversely the capacity of resistance does not change if the Ca is
prevented form leaving the blood-corpuscles though all the other metal-
ions should disappear.

8. Also washed new erythrocytes have a areater capacity of

resistance than washed old erythrocytes.

At any rate the objection to the results of the examination of
anaemic blood is removed: the fact that anaemic blood contains
more serum than normal blood can have no effect upon the capacity

Haem. 100%
90%
80%
10%
60%
50%
40%
30%
20%
10%

0.43% 0.45% 0.47% 0.49% 0.51% 0.53% 0.55% 0.57% 0.59%
Washed blood of the norma! animal.
------- Washed blood of the same animal at the 3rd Venesection.

Fig. 6. Graphical representation of Table F.

TABLE F. Denoting the course of haemolysis in the normal and
the anaemic animal after the blood-corpuscles have been washed
with 0.9 pCt. NaCl.

a PE a

Normal blood Anaemic blood
(washed) (washed)

At 0.59 pCt. NaCl. S'pCt. ss: 63
SOS. 2 for =; = =
A055 a 16: =, | TYopct 9g
Osa oy AG. 20ers 3
nn la Gar. 20) =" Saeed
Otic ae 100, A 50, ee
Pes ss = eae, Ge:
ole | a LBD E
arise ss: ex sig” PS
7) ee = oF 4.2

294

of resistance as the serum contains no substances which impede
haemolysis.

Moreover it may be observed that also the washed blood-corpuscles
of an anaemic animal possess a greater capacity of resistance than
the washed blood-corpuscles of the same animal in a normal condition.
See Table F and Fig. 6.

Summary.

The colorimetrical determination of the haemolysis, (ARRHENIUS)
caused by diluted NaCl-solutions, suggests a means to compare the
qualities of blood-corpuscles, differing as regards their capacity of
resistance.

With the aid of this experimental method the following results
were obtained.

1. New erythrocytes resist diluted NaCl-solutions better than old ones.

2. It must be assumed that new red blood-corpuscles are built up
out of the old ones.

3. After venesections the regeneration greatly surpasses the loss.
(Rule of WetGert).

4. Washing the blood-corpuscles with a NaCl-solution of 0,9 °/,
renders them less capable of resisting diluted NaCl-solutions.

5. The conclusion drawn from this by several workers that this
phenomenon is caused by the removal of unknown substances, found
in the serum, which substances impede haemolysis, is incorrect.
Experiments have shown that if a 4°/, glucose-solution is used
instead of a NaCl-solution 0,9 °/,, this decrease in capacity of resis-
tance does not manifest itself.

6. The phenomenon, mentioned sub 4, should rather be viewed
in the light of an osmotic disturbance, the principal factor of which
is the loss of Ca, suffered by the blood-corpuscles. Indeed the capacity
of resistance is not modified if 0,1°/, CaCl, is added to the NaCl-solution.

7. New erythrocytes, washed with NaCl-solution 0,9 °/,, have a
greater capacity of resistance than old ones which have been treated
in the same way.

May 1912. Groningen, Physiological Laboratory.

295

Physics. — ‘‘Jsotherms of diatomic gases and of their binary
mixtures. X.. Control measurements with the volumenometer of
the compressibility of hydrogen at 20° C. By W. J. pe Haas.
Communication N°.127a from the Physical Laboratory at Leiden.

(Communicated by Prof. H. Kamertincu Ones).

(Communicated in the meeting of April 26, 1912).

X. The compressibility of hydrogen at 20° C.

§ 1. Introduction. In Communication IX. “Control measurements
with the volumenometer’, (Comm. N°. 121a, Proc. May 1911) a
discussion based upon experimental data was given of the degree of
accuracy attainable in determinations with the volumenometer. A
determination of the compressibility of hydrogen at ordinary tem-
perature has now given an additional desirable test of the accuracy
with which the various experimental conditions in their mutual
relationships have been fulfilled.

The investigation is based upon the Leiden measurements of the
compressibility of hydrogen at pressures up to 60 atm. The accurate
piezometers (Comm. N°. 50) and the sectional open manometer (Comm.
N°. 44) specially designed by Kameriincn Onnzs for that investigation
rendered a very high accuracy attainable in those measurements.
Considering this degree of accuracy, we may therefore take ScHALK-
WlJk’s measurements with those apparatus at 20° C. to be quite
accurate, and ascribe the small difference between his formula and
that deduced from Amacat’s results to a lower degree of accuracy
in one_ or other of AMAGAT’s measurements (perhaps in his determination
of the normal volume, which can be done more accurately by
KamerLincH Onnes’s method). This conclusion is also supported by
the fact that ScHALKwik’s formula is confirmed by the results obtained
by Kamertincn Onnes and Hynpman (Comm. N°. 78).

We may therefore write at 20°C.

pva = 1.07258 + 0,000667 d4 + 0,00000099 d4*

in which p is the pressure, v4 the volume in terms of the normal
volume and dy, is the reciprocal of v4. On account of the small
densities which occur in measurements made with the volumenometer
(in which dy, is at the most 1.1) the d4* term may be neglected.
The compressibility at 20°C. is then given by

296

pua =Ag + Bag dg
in which Az = 107258 aes ta Se vs
Ba = 0.000667

Again, on account of the small densities at which the volumeno-
meter is used, the second of the terms on the right of the sign of
equality plays but a small part in the result; it varies from 7.10—4
of pva at density 1.1 to 1.10~-4 of pv, at density 0.15. The question
to be investigated in the proposed test was if compressibility deter-
minations with the volumenometer could give values of pv, to within
240+.

As appears from the table at the end of § 3 giving pv, as obtained
from experiment and dy, as calculated, the accuracy attained in the
compressibility determinations is as a rule somewhat greater than
that which we desired. (Comm. No. 121, § 1). To show more clearly
the nature of the remaining deviations, values of 44 determined by
formula (I) have also been calculated from the volumenometer results
by themselves; in doing this, of course, a sufficiently good approxi-
mation can be obtained only at the highest densities.

§ 2. Summary of the experimental methods. To get as good an
idea as possible of the reliability of the volumenometer determinations
of compressibility at temperatures between — 252°C. and — 259° C.
the compressibility was first measured at ordinary temperature within
the same pressure limits as would be chosen or were to be expected
at the lower temperatures. Measurements were made with two
distinct quantities of distilled hydrogen. For the first series a pressure
of half an atmosphere was chosen as the starting point, and it was
desired to ascend to a pressure of 1.1 atm. while in the second
series the limits chosen were 0.16 atm. to 9.5 atm. The apparatus
was filled in the usual way (cf. Comm. No. 94/) after repeated
evacuations and washings with hydrogen.

For the determination at higher pressures measurements were
made in the neck m, (see Plate I, Comm. No. 117) and pressures
were obtained from the manometer @Og—O, and the barometer
6:—6p. In this an artificial constant pressure practically equal to
the barometric pressure was maintained in the manner usually
adopted in the Leiden Laboratory by means of the ice pot &. To
eliminate changes due to temperature fluctuations the four menisci
to be observed were read twice in reverse order. Measurements were
then made in the necks m, and m, (Pl. I loc. cit.). To do this the
tap /, was closed, and, keeping %, closed, communication was esta-
blished with a mereury pump through &,,, &,,. After careful evacu-

297

ation the pressures of the volumes close to the necks m, and mM,
were measured, using the manometer as an indicator. For this two
of the telescopes of the large Société Genevoise cathetometer were
focussed upon the menisci in the volumenometer and manometer,
and the heights were read each time from the standard metre S.

In an identical fashion measurements were made with a smaller
quantity of gas in the necks m,, m,, and m,.

For further experimental conditions and precautions reference may
be made to Comm. No. 121, § 4 and 5 and also to my dissertation,
which is to be published shortly.

§ 3. Calculation and values of pv.

The final value of the gas density for each of the two series of
measurements, each with its own definite quantity of gas, was
obtained by means of equation (I) from the observed final pressure
after the application of the correction necessary for the small differ-
ence between 20°C. and the temperature at which the measurements
were made. The pressure coefficient used was 0,0036627 (Comm.
N°’. 60). On account of the smallness of the temperature difference
for which a correction has to be applied no correction is needed for
the dependence of this pressure coefficient upon the pressure. The
observed volumes vy for each measurement follow from the v,4’s
obtained from the final density and from the ratio of the volumes
in each series measured at 20°C. to the final volume. Table I gives

| TABLE I. H;. Values of pu

|
pugobs. | O—C |

No. | t | Pp | agcale. | |
1 (20°C, 0.46780 | 0.43603 | 1.07278 | — 0.00009
ae | 0.58113 | 0.54162 | 1.07295 | + 0.00001 |
3 | > | 1.12867 | 1.05161 | 1.07328 |
| | | | |
| 1 20° cl 0.16310 | 0.15205 | 1.07247 | — 0.00021 |
| 2 | » | 0.2008 | 0.18885 | 1.07248 | — 0.00022 |
3 | » | 0.99313 | 0.36645 | 1.07282 | |

the values of pva,and those of d4 as calculated from p by means

of equation (I).
20
Proceedings Royal Acad. Amsterdam. Vol. XV.

298

From this it is evident that an accuracy of one in four thousand
to one in five thousand is attained at the lower pressures, while in
the series of measurements made at higher pressures the accuracy
reached is greater than one in ten thousand.

§ 4. Calculation of Ba. From the former of the two series con-
tained in Table I (pressures varying from 1.1 to 0.46) B,4 can be
calculated. Instead of B 42:0 = 0,00067 it gives

B 4200 = 0,00074 so that O—C = 0,00007,

in which only the fourth decimal is significant. In the second series
the percentage error expected in 6, is too great to allow of a
calculation of Sy itself. Only under more favourable circumstances
could one count upon an accuracy of one in ten thousand or more
in the values of pv4; the error in pv, becomes greater at smaller
pressures; in #4 it is magnified four or five times and at small
densities the utmost value of the whole term AByd,4 for that series
is 0,00026. In the meantime it may be remarked that a comparison
of the positive differences found here between observation and cal-
culation (+0,00138) with the corresponding positive difference in the
first series seems to indicate a possible systematic error which makes
its presence specially felt at the lower pressures ’).

In order to be able to compare the results obtained with others
which just had in view the determination of the compressibility at
ordinary temperature we must reduce the results to a common basis.

Take first the measurements made by Lepuc’*) at 16°C. and at
pressures varying from 1 to 1.5 atmospheres. From the numbers
which he obtains from his experiments after the incorporation of
other data for the compressibility at O° C. we find to correspond
with his result

Basoo0 = 0,0007 and therefore O—C = 0,0000.

The figure last given does not necessarily lead to the conclusion
that the Leiden determinations with the volumenometer are the less
accurate. The degree of accuracy of Lxpvuc’s results is indicated by
the fact that he goes only to the fourth decimal place (for CO,
Cuapputs') and Lepvc differ by 0,0002). And the pressures used by
Leptc in this determination, which is accurate to 1 in 10000 were
very much more favourable (the smallest density was twice as great
as that of the first series of Table I) than those which are expe-

1) Possibly a small constant error arising from a change in the correction for
the capillary depression since the control measurement of Comm. N° 121a.

*) A. Lepuc, Recherches sur les gaz. 1898.

299

rienced in experiments at liquid hydrogen temperatures and at which
my measurements had to be made.

Determinations made by Cuappuis') and by Ray.eien, in each case
with apparatus designed to attain a higher degree of accuracy than
that of the Leiden volumenometer, also afford a basis of comparison.
CHAPPUIS measured compressibilities at O° C. between 1.4 and 1.8
atmospheres. His results give B49 = 0,00058, from which, using the
figure given by KameriLincGH Onnezs and Braak*) for the difference
between Buicoo and L4oo we get

Bax0 = 0,00064 and O—C = —0,00003.

The values deduced from the two single observations distant by
about half the pressure difference from each other, in which the
errors are increased, differ by 0,0001. .

Finally, Lord RayLeicH’s*) measurements were made with an appa-
ratus specially designed to give an accurate comparison between pv.
at half an atmosphere and its value at double that pressure. From
them we get B4io.7 = 0,00054 from which, using again the KAMERLINGH
OnneEs—Braak result just given, we obtain

Bao00 = 0,00057 and O—C = —0,00010.

So that comparison between the results now given with those
yielded by these different researches shows a satisfactory agreement.

In the proposed determination of 44 at hydrogen temperatures
circumstances will be much more favourable than at ordinary tem-
perature, for B4d,4 will then be 15 to 20 times greater at the same
pressure. We may regard the value obtained for B, in this way at
—252°C. as accurate to within 2°/,, and to within 10 °/, at —259° C.

Physics. — ‘“Jsotherms of diatomic gases and of their binary
mixtures. XI. On determinations with the volumenometer of
the compressibility of gases under small pressures and at low
temperatures.’ By W. J. pe Haas. Communication N°. 127°
from the Physical Laboratory at Leiden. (Communicated by
Prof. H. KAamMertincH ONNss).

(Communicated in the meeting of May 25, 1912).

§ 1. Criticism of the pressure equilibrium between the piezometer
and the volumenometer. In the investigation of the compressibility
of hydrogen vapour with which a subsequent paper by Prof. Kamrr-

1) P. Cuapruis, Nouvelles études sur le thermométre a gaz.
2) Comm. no. 1000, These Proceedings Dec. '07.
8) Lord RayLeieH, Proc. Roy. Soc. 73 (1904). Ztsch. phys. Chem. 52 (1905),

20*

300

TINGH Onnes and myself will deal, the volumenometer described in
the previous Communication was used to measure the quantity of

hydrogen contained under different pressures in a reservoir —- the
piezometer reservoir — which was immersed in liquid hydrogen and

connected with the volumenometer by a capillary and tap. The
pressure of the gas in the piezometer reservoir was then given for
each measurement by the pressure of the gas in the volumenometer
in pressure equilibrium with it. It was shown in Communications
N°. 124¢ (Proc. May 1911) and N°. 1272 (These Proc. p. 295) that the
accuracy with which the pressure, volume and temperature of the
quantity of gas contained in the volumenometer could be determined
was sufficient to allow of the evaluation of the virial coefficients B
at low temperatures for hydrogen vapour from determinations of
the compressibility of that vapour. More particular attention must
now be bestowed upon the question of pressure equilibrium between
the volumenometer and the piezometer.

In the course of the above experiments it was repeatedly necessary
to adjust the mercury in the volumenometer to one of the lower
necks (for instance, m,, m,, or m,. Cf. Comm. N°. 117, Pl. I, Proe.
Febr. 1911). The quantity of gas contained in the volumenometer
was in those cases always less (though not many times) than that in
the piezometer of 110 ce. capacity and at a temperature of —252°
to — 258° C., so that the gas in the piezometer was of a density
from 12 to 20 times greater than that in the volumenometer. On each
side of the capillary, therefore, which had to be long on account
of the construction of tbe cryostat and narrow on account of the
uncertainty of the volume correction to be applied for it, there are
relatively large quantities of gas. On account of friction in the
capillary, pressure equilibrium will be but slowly attained. A preli-
minary experiment had shown the desirability of a means to decide
from the measurements themselves when exactly this pressure equi-
librium had been attained. In order therefore to obtain the necessary
data for this, the behaviour of the pressure in the volumenometer
was systematically observed during the final experiments upon the
compressibility of hydrogen vapour at low temperatures (June 23
and 24, July 8, 14, and 18, 1911) on each occasion on which the
meniscus was adjusted to one of the necks m,, m,, m,, m, — this
of course only after satisfying the experimental conditions to be fulfilled
for equilibrium (regulation of cryostat and of volumenometer thermo-
stat, constancy of room temperature). At intervals, as a rule every
5 minutes, the difference between the levels of the mercury in the
manometer and in the volumenometer was read and corrected, from

301

tables prepared beforehand, for changes occurring during the measure-
ment in the quantities determining the corrections (such as change
in the temperatures of the volumenometer, the piezometer, the dead-
space, change in the capillary depression, etc.).

In this way the actual change in the difference between the pres-
sure and the equilibrium pressure was known at all stages of the
measurement. During the measurements a curve was drawn with
this pressure difference as ordinate and time as abscissa, and the
observation was regarded as at an end as soon as the plotted points
began to fluctuate about a line drawn parallel to the abscissa axis.
The accompanying diagram (unit ordinate representing 0.1 mm.
mercury) is taken from the above investigation and refers to the
adjustment of the pressure equilibrium on July 18, 1941, an occasion
on which circumstances were particularly unfavourable. The observed
pressure differences, increased by a certain fixed quantity, are re-
presented by circles. At the end of § 3 we shall return to this diagram.
20 a] Se | ard ie ;

2422°m 3h

Fig, 1.

§ 2. Calculation of the pressure change jrom the experimental data.

The curve giving the change in the pressure difference between
the two communicating vessels as a function of the time was now
calculated from the dimensions of the apparatus and from data
determining the temperature distribution along the glass capillary.
As will be seen from the end of § 3, calculation is in complete
agreement with observation, and is therefore suitable for checking
the smallest pressure difference experimentally determined by the
above method in the case discussed in §3. The reduction of the
theoretical calculation to formulae has the result that it not only
covers this particular case, but it can also be applied to gauge the
degree of pressure equilibrium in similar cases in which capillary
connections occur in experiments at low temperatures.

302

The influence of gravity upon the gas is left out of account in
the caleulation, as is also the pressure difference which KNUDsEN’s
researches show must exist. If necessary both corrections may be
applied to the observed pressure at which equilibrium is attained ’).
The influence of slipping along the walls of the capillary is also
left out of account, while the volume of the capillary has been regarded
as negligible compared with that of the reservoir and of the volu-
menometer. It is also assumed that the speed may be regarded as to
remain the same over a short period of time, and that the speed is
small (far below the critical); further that the temperature, 7’, and the
pressure, p, may be regarded as uniform over any cross-section,
so that if z is the length and y and z two axes at right angles to
it and to each other, p is independent of y and z; and, finally, that
the speeds v and w in the directions of y and z may be taken to
be zero. A flow is therefore assumed such that in a tube at constant
temperature throughout and for a substance whose density is inde-
pendent of the pressure PortsevILLe’s law should hold, and such as
may be regarded as subject to this law over any element of length,
dz, of the capillary when the values of the pressure gradient, the
density g and the viscosity 4 at that particular place are inserted.
Working out the equations of motion subject to the given assump-
tions*) at once leads to the result 3

iol Sa dp

i ey y dz (1)

where m is the mass of the gas contained in the reservoir, and hence

dm i : ;
re the mass which flows per unit time across any section of the
It
capillary.

We assume 7 to be independent of the pressure so that 7 = f(T),
and for 7 (7) we take SuTHERLAND’s formula

1) As a general rule, however, both corrections may be neglected. For the
lowest pressure occurring in the course of the experiments for which this cal-
culation was made the KNUDsEN correction just reached that limit at which the
calculations by KAMERLINGH OnNeEs for the capillaries of his hydrogen and helium
thermometers show it would begin to be appreciable.

2) Cf. O. E. Meyer, Pogg. Ann. 127. p. 253, 353.

303

in which C is a constant. As an approximation for vapours we may
write p=ao-+ bo? in which a and 0 are functions of 7. These
and all other quantities occurring in the present calculation were
expressed in absolute measure (the C.G.S. system was chosen). If
T be given as a function of 2, equation (1) can at once be integrated.

As a further simplification for this integration we shall regard /
as negligible on account of the smallness of 60° compared with ag.
If the pressure difference between the ends of the capillary is small,
deviations from Boyir’s law may, to the same extent, be allowed
for. For further information on this point I may refer to my disser-
tation.

It may be further remarked that we may differentiate between
three different portions of the capillary. The first part projects above
the eryostat, and has throughout its whole length the same tempe-
rature, that of its surroundings (room temperature); for the pressure
at the upper end of this portion we shall write p, and for the
pressure at the lower end p,. In the second part of the capillary
the temperature changes from the room temperature to that of the
cryostat bath. The pressure at the upper end of this part is p,, and
for the pressure at the lower end we shall write p,. The third
portion of the capillary is wholly within the cryostat bath, and over
its whole length has the temperature of the bath. p, is the pressure
at the upper end, and we shall write p, for the pressure at the
lower end.

With the object above indicated of not only calculating for the
particular case discussed in § 3, but also of obtaining simple formulae
applicable to analogous cases I have endeavoured to find a simple
form for the function expressing the temperature of the middle portion
in terms of the length; in order that four terms in this would
suffice I have imagined a sudden change in the temperature at the
junction of the second and third portions of the capillary, in other
words I assume that at that point the temperature changes rapidly
over a length which is large compared with the diameter of the
capillary but is still small compared with its length.

The calculation is therefore made for a temperature distribution
other than that which actually exists, but, as will be seen, the
difference between the two cases does not affect the result.

The temperature distribution over that portion of the capillary in
which the temperature is variable is thus represented by

e==¢-+ L.T + m,T? + Tig D tu.) bial he aN (2)

In the experiment further discussed in § 3 the temperature change

304

at the surface of the bath would be one of from 7,—=26° K. to T.—15K.
With «a7,

7 C
F T 973 Pe 8 dm :
SS = ——
V273 a ah* dt @)
(1) now gives
1
for the first portion A ———— (p,?—p;”)} - - »- +» + (4)
2a Nl
and for the third portion A——=———(p,?—p,?), . . . . . (8)
2A,n,T
while the substitution of
DE = CP vers | se Sa ae

gives
Pp, — ps) = 4Aa, ky Cs (Fr), — (0 7) 22
in which

E 2m—-3
| i E Giese to’a -+- (1 — 2mC + 3nC*)

tga toa tga
oe ES SoG) ee
5) 3) 1

so that p, and p, can be expressed in terms of p, and p,. From
(4), (5), (7) it is seen that for a case such as that discussed in § 3
for which 7, = 15°K. and 7’, = 295°K, p, does not differ appreciably
from p,, so that one need not be very particular about the lower
limit in the integral of (7) and (8), and the small jump in the tempe-
rature is of no influence within the limits of accuracy desired; this
indeed is obvious if one considers that the gas flows about
20 times more slowly in the cold portion while the viscosity is also
about as many times smaller.

With the temperature function now obtained for the interchange
of pressure in a gas of known C,y, and a, through a capillary of
radius Rk, and for a given temperature distribution, we obtain

dm, xR
dt — 8Ka,

mess: 7

C= PA . oe Oa > Sane (9)

in which m, is the mass of gas in the volumenometer, and
k= In, (fp —F7,) = My,), fT, aie Wat Ts
where the quantities Z, 1/ and JN follow at once from (4), (5) and (7).

The first member of the expression for A refers to the portion of
the capillary in which the fall of temperature occurs, and the second

305

and third members to those portions in which the temperature is
uniform.
If we further write

, mM—m, |

fl, -—— Roa) eo tions) 4,
v; Vv,

in which v, represents the volume at the lower temperature, v, that

at ordinary temperature, and mm the total mass, and then integrate

(9) we obtain, with the omission of an integration constant
ia

(m—m,) + aos m,
0,0, ate aha,
2 a \ i
rm — log ry = — >t . iE . (11) )
LT jm Deg AK
m—m,) — m,
1X9

The ease discussed in § 3 and graphed in fig. 1 gives an example
of the curves given by this equation.

§ 3. Application to a special case. Deductions.

From measurements made during the experiment of 18" July 1911
temperatures were to be taken as

—258°C. for 10 em. in the liquid bath
ae Sal em:
=) 5S Pe ty eit
— 25° ee vem.

Room temp. at + 22° » 22 em. projecting outside the cryostat.
For the calculation of (2) the temperature of each portion is
regarded as the temperature at its centre.
Meemeuerciore, fet 42 — 10, 24,=-11, 7,=15, 7,= T,= 295;

4
and from «=10 to = 49 equation (2) holds with the values

g=166 /,=0.389 m,=—0,00278 n,= 0,00000682 ;

1) In the simpie case in which p,;-+p, may be regarded as constant, and
T,=T7T,, m=v, d+ »,d in which d is the common density in both vessels,
substitution of (10) in (11) gives

ms og Ms ay OR
C(ey"2) PP ;

The subscript 4 is here replaced by 2.
This is the formula given by RAyLetcH Scientif. papers Vol. LV 1892—1901
p. 53. This formula does not hold for instance for the evacuation of a vessel by
a pump through a capillary, to which (11) is applicable as long as the pressure
is not so small that the mean free path becomes comparable with the diameter

of the capillary.

306

while, as was already remarked, the temperature jump assumed to
take place at the surface of the liquid has no influence upon the
result. We also find

m — 0,017, v, = 110, v, = 1035.

The line drawn in fig. 1 has been calculated from these data.
The observed pressures, indicated by circles, agree well with the
results of calculation.

Between half-past four and five more liquid gas was admitted into
the cryostat. The readings during which the resulting pressure inter-
change was stopped by means of a valve are not marked in the
figure. A ‘slight temperature fluctuation occasioned by the refilling
is clearly seen in the diagram. A small pressure increase at 5%5™
dies down about six o’clock quite in accordance with the calculated
curve. (See 3'27™. At this point the temperature also increased).

As can be seen, it took more than an hour for the last 1.8 m.m.
pressure difference to die down to 0.02 m.m. (the whole pressure
was 9 cm.).

The calculations show that the assumed distribution of temperature
along the capillary is, in the main, correct. It gives a very welcome
estimate of the time requisite for the last appreciable interchange
of gas.

To establish pressure equilibrium as rapidly as possible in such
experiments it is necessary that:

1. as little of the capillary as possible should project above the
cryostat, and that the stem within the eryostat should be kept as
cold as possible ;

2. the upper part of the capillary should be wider than the lower,
as is the case, for instance, in the helium thermometer of KAMERLINGH
Onnes, or better still, the connecting capillary should be gradually
narrowed. (In fig. 5 Comm. Suppl. N°. 216 *) compare the tube which, in
the experiments by KamERLINGH ONnNEs on the attainment of the lowest
possible temperatures, had to carry off helium vaporised under a
pressure of 0.2 mm. with the least possible reduction of pressure;
the dimensions of this tube were calculated according to the principles
of § 2). :

(To be continued).

1) Bericht tiber den II. Internationalen Kaltekongres, Wien, October 1910, Bd. Il.

307

Physics. — “On the Hau effect and the change in the resistance
in a magnetic field at low temperatures. 1. Measurements on
the Haut-effect and the change in the resistance of metals and
alloys in a magnetic sield at the boiling point of hydrogen
and at lower temperatures’. By H. KameruincH Onnes and
Benet Beckman. Communication N°. 129° from the Physical
Laboratory at Leiden.

(Communicated in the meeting of June 29, 1912).

§ 1. Introduction. An investigation of the Hatt effect and of the
change of resistance produced by a magnetic field was carried out
by van EverDINGEN at Leiden some time ago down to liquid air tem-
peratures *), but the fundamental importance of these phenomena in the
theory of electrical conduction has long made it desirable fo extend
this investigation to the much lower temperatures which have been
freely available since the successful development of methods of
obtaining accurate series of observations at liquid hydrogen tempe-
ratures. The problem, however, has been forced aside by other
researches which could not be delayed, until the study of it and of
allied problems for various metals at the lowest possible temperatures
has been rendered essential to the further development of the theory
of electrons by the discovery of the fact that the resistance of
pure mercury disappears at liquid helium temperatures. We have
therefore been occupied for some time with various aspects of
the investigation of these problems at hydrogen temperatures, and,
while we propose to continue this investigation systematically and,
if possible, to make some measurements on the more important points
at those temperatures which are obtainable with liquid helium, we give
in the present paper some results which have already been obtained,
and which may be considered to be themselves of some importance.

The investigation has been extended by one of us (B. Beckman)
with the same experimental material to temperatures obtainable with
liquid ethylene, liquid oxygen, and liquid nitrogen, and these results
will be discussed in a later paper.

We wish to record our heartiest thanks to Mrs. A. Beckman for
her assistance in the course of the measurements.

1) The results for bismuth (and antimony) given in the dissertations of LEBRET
(Leiden 1895) and van EverpDINGEN (Leiden 1897) and in Communications Nos. 19,
26, 37, 40, 53, 58, 61 have been confirmed by Biuaxke, Ann. d. Physik. 28, 449,
1909 and Lownps, Ann. d. Physik 9, 677, 1902. Lownps investigated rods cut
in different directions from bismuth crystals, and extended his investigation for one
direction down to liquid air temperatures. He found that with the crystalline axis

perpendicular to the field the Hatt coefficient is negative at higher temperatures,
while as the temperature is lowered it vanishes and then becomes positive.

308
I. Bismuth.

§ 2. Change in the resistance of a wire of electrolytic bismuth.

This part of the investigation was made with a wire of electrolytic
bismuth provided by Hartmann and Braun 0,3 mm. thick, and iden-
tically the same as that used by Kameriincu Onnes and Cray in
their determination of the change of resistance (Comm. N°’. 99). The
Konrrausch method of overlapping shunts was used. At ordinary
temperature and at the boiling point of hydrogen the main current
was + milliamps, but at — 259° C. it had to be reduced to 0.1 a
0.2 milliamps on account of the effect of heating upon the resistance.
In the following Table w’ represents the value of the resistance in
ohms in a magnetic field of strength H, wr is the resistance with
no field on, and w, is the resistance at O° C. with no field.

We may notice that we have not obtained the maximum in the
isopedals observed by Brake. It will be seen from the forthcoming
paper on the change of resistance with magnetic field at liquid air
temperatures that Biake’s bismuth wires which showed the maximum
exhibited a smaller change in the resistance than ours and were
therefore probably not so pure. It is possible that as the purity in-
creases the maximum in the isopedals is displaced towards the lower
temperatures.

| TABLE I.
Resistance of Big 7 as a function of the temperature and of the
field strength.

x | T = 290° | T = 20°,3 | T = 15°
| | ir
on fw l[ef~le [© le
Wo Wy Wo
0 2.570 1.057 || 0.588 | 0.242 0.526 | 0.216
2160 || 2.770 | 1.140 || 11.5 | 4.73 |
3850 || — pa |e aes 19.9 | 8.185
5540 || 3.110 | 1.280 | 32.8 | 13.50 34.9 | 14.35
| 7370 || 3.473 | 1.388 || 54.7 | 22.50 55.9 | 23.00
9200 || 3.635 | 1.495 | 76.7 | 31.55 |
|

113.2 46.55 116.4

| | 47.90
13600 || 4.248 | 1.746 | 141.5 | 58.20 || 143.1
|

58.85
12.25
82.00

| 172 10.75 175.6
17080 || | 196.5 | 80.85 199.3

|
|
|
| 80.8 33.25

309

The general character of the isotherms is also conserved at hydrogen
temperatures ; the field at which the resistance begins to increase
practically proportionally to the field itself is about 12000 gauss just
as at liquid air temperatures. The gradual transformation from the
change at small fields to the practically linear change in strong fields
takes place in the same way at each temperature.

§ 3. The Hatt-ejfect and the increase of resistance for plates of
compressed electrolytic bismuth. Experimental method.

The method adopted was that developed and applied by Lesret and
vAN EverDINGEN in their dissertations (see Suppl. N°. 2); in it all
disturbing influences are eliminated. A diagram is given in Plate 3
of the Supplement quoted, and for all matters concerning the arran-
gements for measuring we may refer to Chapter I of that paper.
Circular plates were used to which were soldered with Woon’s alloy
the primary and Hatt electrodes as well as two auxiliary electrodes
(placed on the diameter in the direction of the main current). All
were point electrodes *).

Choosing our notation to correspond with that of the Supplement
quoted let us write e for the potential difference between the Hai
electrodes, / for the main current and d for the thickness of the
plate. The Hatt constant & is given by

__ ed

==:
Let us also write F#, for the resistance of the secondary circuit outside
the plate, 7 for the resistance of the shunt of the compensating
circuit, g for a constant determined by the differential galvanometer
employed, and Ay for the resistance determined by

er 1 1
[ejb a Bey

in which Ry and Rg are magnitudes obtained from the resistances
of the compensating circuit with reversal of the main current when
the field commutator stands in each experiment in the positions A
and 6 respectively; we then obtain

Ss
=
The change in the resistance was also measured as well as the
Hau effect.
At ordinary temperature the bismuth plates showed no asymmetry

1) Van EVERDINGEN has solved the problem theoretically for point electrodes with
circular plates.

310

in the Hatt-effect, but they showed it very clearly and sometimes
very strongly at hydrogen temperatures, giving considerable differences
between 4 and Fz. In the following tables twice the asymmetry
is given by the side of the mean Hatt-constant; for the method of
evaluating the asymmetry we may again refer to Chapter I of Suppl.
N°. 2. All quantities except w are expressed in C.G.S.

The current in the main circuit was / = 0.15 amp. A WirpEMANN
galvanometer was used. The bath of liquid gas in the magnetic field
was obtained in a silvered vacuum vessel by the method of Comm.
N°. 114.

§ 4. Results of the measurements.

Bit, Bint, Bi, represent three plates of 10 mm. diameter pre-
pared from the same Harrmann and Braun electrolytic bismuth.
Bi,; was compressed from a thin rod in a steel mould. 2,77 and
Bi,171 were prepared by first grinding the bismuth to a fine powder
in an agate mortar and then compressing in the same mould as Bi,7.
In the preparation of £2,777, which was otherwise the same as that
of Bi,z; and 42,7, the grinding operation took place in an meet
of carbon dioxide.

| TABLE II
= The HALL constant, asymmetry and resistance change for Bip y-
||
| T = 289° | T = 20°,3
= | rw’ Tw
| | hee aie PR Weal RA 2x Asym. | —R ies
oe 2
| |
2060 | 13.9>X103 | 0.4><103 | 6.75 | 1.06 || 91. 4><103 39. ed 44,.35| 10.1
| 3450 | 20.9 0.2 6.06 | 1.12 | 166.5 48.25} 21.7
| 5660 || 29.1 1.1 15.14 | 1.21 || 308 54 54.40] 39.3
7160 || 33.2 0 4.64 | 1.29 || 385.5 114.5 53.90] 52.0
9880 || 40.3 1.8 4.08 | 1.45 || 563 199 57.00) 78.2
11090 || 42.6 2.3 3.84 | 1.50 | 640 243 51.70, 89.5
| | w= 0.00044 0
0 w= 0.00209 2 w
| T CO 55 ee |
| 980K |

With no field the ratio of the resistance of Ai,7 at hydrogen
temperature to that at ordinary temperature is almost the same as
the same ratio for the bismuth wire Jigz; but in a magnetic field

By L8¥00'O = “mr U 68E00°0 = 8%m
——_—_—— Ae es De ae ee | ee
1° (cL ‘LO 02 gig || sz°9 | 6°LS QOT OOL || L8z'I | 61°S bl
Lo’9 | 1°89 II ccy || OL°S | ¥'°8¢ 16 G'L¥O || Oct | 1r's 80
Lp’s | S'69 02 L89 || 12'S | 0°6S 6L egg || zz | 99°S Z'0
-- -- ~ — 8S'b | 0°6S OL €0S || 98I'T | s1°9 8°0
1d ey de Pl a rl 60S || 6° | €°09 0S Z' Ich || ShI'I | PPO £0
e — -- _— _ ez's | 8°19 G’L¢ L'6bS || SOIT | SOL r'0
CY
Zb'a =| 6'SL Gq’ goe'|| 1¢:¢> L799 62 Cee uiCLco" tT LTS z2°0
eer'l | SIS | cOIX<E |eOIXS'L9l IL'l | 1°bL | c01X< bz \e01 X9°ZSI || €z0'T | 80°6 | c0l X20
J) A) | x— | waswe | > He za] w—|-utswe | ony | 7] )) y— | utevxe
9ohl =L €'003 = L 068 =L
I hig JO} oURYSISAI JO asuRvYD puB AxyomwAse uejsuoo-TIVH “YT ATAVL

8°29 || 06021

S6°6S |) OGOTI

6°SS || 0886

GI°2G || 0298

1°9P || OOTL

68°66 || 0996

Z'8z || OShE

c0I X<L'S8I || 0902
HM

—|| H

312

the ratio of the resistance at hydrogen temperature to the zero
resistance is less for the disc than for the wire Bzy;, so

dise wire

w’ w’

for = 11090. ab S203 ee
W, Ws,

In the case of 42,7; both the negative temperature coefficient and

the smallness of the change of resistance with magnetic field indicate

the presence of impurities.

FABLE AV.

The HALL constant, asymmetry and resistance
change for Bipiiy:

fe"
H |
|| RH —R | Asym | [=|
| w IT |
2850 | 247 & 103 | 86.6 | 137 X 103 2.16
4700 426 90.7 210 2.91
6675 || 624 | 935 | 280 3.67
8275 || 814 98.5 346 4.44
10160 | 1007 99.2 400 5.12
11100 | 1105 99.4 425 5.49 :
12220 | 1216 99.5 | 460 5.87

With the dise 42,737 measurements were made only at hydrogen
temperatures, but we give the results here as, just as with 52,7, R
increases with H, and approaches a limiting value, approximately
100; this is the highest Haut coefficient yet obtained for bismuth.

All the coefficients we have obtained for bismuth plates are negative.
Circumstances which give rise to positive’) coefficients occur only in
certain positions of the crystalline axis and therefore, since all posi-
tions of the axis occur at random, they are obscured by those which
give rise to negative coefficients.

ll. Other Metals.

§ 5. Experimental method. This was just the same as for bismuth.
A Tuomson differential galvanometer was used for observing the HAL
effect. Now the contacts were not soldered with Woop’s alloy, but
with tin.

| 1) Here total coefficients are considered, cf, Gomm. N?. 129c. [Note added in
the translation].

313

> 6. Han. erect for Gold. The plate Aw,; was prepared from a
dutch 10 fl.-coin; this was dissolved in aqua regia, precipitated by SO,,
melted in a porcelain crucible and rolled between steel rollers. During
the last operation and afterwards it was treated with various acids.
ee the decrease with temperature of the resistance with no magnetic
d (see Table V) it is seen that this plate was made of purer gold
isn that which composed the wire Aw, of Comm. N°. 99, which
gave W790] p=s73 — 9,045 and was known to contain 0,03 °/,
eeestty.

d was 0,101 mm., / approximately 1.2 amp., and R,—0,6 to
07 ohms.

ewe found :

TABLE V.
The HA. effect for Gold Au, r
| T = 290° F=ms° |} T=14°5 |
H | ee ae | i
| RH eee Ey RH CR. 84 RH — R.104
i
rT |
a 641. 727 |) 157). 979 156 | 9.78
| {| |
9500 |) 6.75 711 | 9.32 | 981 | 9.22 | 9.71
| 811..| 732 || 10.91 | 984 || 11.03 | 9.96
10 885 | 7.25 || 1198 | 981 || 1200 | 9.82

ae e Haut effect for Silver. The plate Ag,; was prepared from

TABLE VI. |
The Hatt effect for Silver Ag].

7-200" K: T=20°.3K. | T = 14°95 K,

RH | R.10° || RH | R.10! || RA | R.104

aq7-|. 804 || — a = =
581 | soi || 739 | 10.18 || 722 | 995 |
7.23 | 798 |} 9.22 | 10.17 898 | 9.91
8.16 | 795 10.34 10.07 10.12 | 9.85 |
17310-59147 10 0 0.925 X 10-6. |
1.065 | 0.00905 | 0.0057 |

21
Pro ceedings Royal Acad. Amsterdam~ Vol. XV.

« - =

314

silver for which we are indebted to the Master of the Royal Mint,
Dr. C. Horrsema. The silver was found to be practically the same
as that of the wire Ag; of Comm. N°. 99, which had 0,18 °/,
impurity, and for which W799 W 7973 = 90,0089 (ef. wy in Table).
The thickness of the plate, d= 0,096 mm.

§ 8. Hatuefect for electrolytic Copper. The electrolytic copper
was supplied by Fenren and GuiLLaume; d was in this case 0,057 mm.
We found :

TABLE VII.
The Hatt effect for Copper City /-

T= 290°K. 20 f—=1 5K

H | - -
RH | R.10 || RH | R.10* || RH | R.108
| 7260 || 359 | 495 || 4.79 6.60 | 4.79 6.60
| 9065 || 442 | 487 || 603 | 6.65 5.94 6.55
10270 | 5.08 | 4.95 | 6.78 6.60 6.71 | 6.54
w 312.10-6 a 2.94.10-6 0 2.83.10-6
w/w | 1.065 0.0103 | 0.00907 |

§ 9. Hat effect for Palladium. The plate Pd,7 was supplied by
Heragcs; d= 0,100 mm. We found:

TABLE VIII. |

| The Hatt effect for Palladium Paty.
| T = 290 | T=203 =i T= 1495
}
H eae: |
| | RH | R | RA | R |) Pee R
ae ! | , :

8250 | 561 | 680<10-4 11.42 | 1383X10-4) 11.54 | 13.98<10—4)
9065 6.04 «6.66 ea er = fot ed

9360 sey = || 12.71 | 13.58 12.96 | 13.84
} } | 1]
9760 6.64 | 6.80 -- = | =
' \|
10270 ||. =e Oe See 13.65 14.09 13.74
1} |
w 1262x1050 | 611K1050 || 571<X1058
= 1.065 0.0515 0.0485

3Lo

The plate was annealed and was kept from contact with the liquid
hydrogen in the bath by a coat of celluloid dissolved in amyl acetate.
By immersing the same plate unprotected in the bath, so that it
absorbed a large quantity of hydrogen it was found that the occlusion
of hydrogen constantly diminished the Hani coefficient, as is evident
from a comparison of the following data with those of Table VIII.
It was observed that the change of resistance with temperature
diminished at the same time. We found :

ie ee = 12, 0,10—-* w= 5310-7 Ohm,
then oe = a)” fo Grol O— w= ACT. “WOs
an@.aeain ,, (= 14°.5 Pip ed

eo P10 440. wa 69.10%
finally: 2p-7,,-2' == 290° w= 109. -10-*

§ 10. Summary of results dealing with the change in the Hau.
coefficient for various metals. In the two subsequent Tables we give
figures for the change in the Hai coefficient when the temperature
sinks to hydrogen temperatures and in the region of liquid hydrogen
temperatures; /? is the mean value taken from the previous tables
at each definite temperature for each substance. |

- TABLE IX.
= fas cone R at ayes SEE eS

Ty | Apr Pe lea eel

]

200° 1.24 10-4) 8.00 10-4 4.92 x 10-4] ex

20°.3 | 9.81 (10.14 6.62 13.68
14.5 9.82 | 9.91 | 6.56 ee
; 2S al

Rr |
| Rog90K
| on cooling to and in the region of liquid
| So SEs
Tt | ye | 480 | Spr | Pept

Change of the HALL coefficient

| |

es 1.355 | 1.265 | 1.345 | 2.03
cal al 1.24 | a 2.05 |

290° | vr ay oe

21%

316
The change of the Hat coefficient on cooling to the temperature

Rr=se :
of liquid air aT=* has been found by SmitH') to be
Rr=293

1.03 for Au, 1.095 for Ag, and 1.205 for Cu.

It seems to be of great importance that the change in the Hai
coefficient for Ag and Aw takes place chiefly below —190° C. and
becomes practically constant again in the region of liquid hydrogen
temperatures. This is also seen to be the case for palladium on
comparison of the results of experiments by Bexer Beckman upon
palladium at liquid air temperature, which are not in agreement
with those given by Smitu, and which will be published in the forth-
coming paper by Berner Beckman. In connection with the different
behaviour for copper, for which Brckman has already found an
increase in liquid air although smaller than that given by Swiru, the
question arises if this cannot be accounted for principally by the
influence of impurity. Experiments which we have already under-
taken upon alloys — in § 12 we give one set of results — will
enable us to decide the point.

§ 11. Change of resistance of Au,z1, Pd,z, Cu,r, in a magnetic
field.

From the measurements with these plates only approximate results
can be obtained for this change on account of the smallness of the
change in the already very small resistance. In the following table
results which were obtained in fields of from 10000 to 11000 gauss
are reduced to a standard field of 10 kilogauss.

| TABLE XI
| Change of resistance in a magnetic field
Sor ae |
aj =
H TO) Aa es fa
: : =

10 Kilogauss 20°3K | 1.017. 1.14 | 1.0015 |
10 ¢ 1495 | 0 <4

While at ordinary temperature the change caused in the resistance
by the field is extremely small, at hydrogen temperatures it becomes
quite appreciable.

1) A. W. Smita, Phys. Review, 30, 1, 1910.

317
ll ] - Alloys.

§ 12. Gold-Silver.

On account of the usually great influence of

admixture upon the Harr effect and upon the magnetic change of
resistance it was thought desirable to investigate various kinds of
alloys. We are already in a position to communicate details of the
behaviour of one solid solution, viz. an alloy formed by fusing 2°/,
by volume of silver with gold. The exact analysis we shall publish

later. d was here 0,073 mm.

TABLE XII.

|
HALL-effect for a gold alloy |
| | T= 290° T = 2093 T=1495 |
H || :
RH | R RH | R RH R
pi pees AS ee eee . i
| 8250 | 570 | 6.91X<10-4 | 5.60 6.79<10-4 | 5.44 6.60<10—4 |
9065 6.31 | 6.96 hs of = oe mo
| d
9360. || -— aa 646 6.90 = ae
| 9760 || 6.75 | 6.91 ee = 6.44 6.60
10270 | 7.08 6.90 71.01 | 6.83 6.80 6.62
| | w = 3.81<10—4 2 || w = 1.083104 2), w = 1.08010—-4 0
0 | :
a =045 \Y — 0,298 w= 9-907
Wy 0 Wo
Here we have
Rr—=.:
ies ay ORs
Rr =290
R == 5
poe = 955
Rr=290

The observations show that down to hydrogen temperatures and

in that region itself the Hat. coefficient
changes however are so small that they do
the probable error,

decreases slightly ; both
not exceed the limits of

318
POSTSCRIPT.
[V. Bismuth crystals.

§ 13. Hatr-effect in bismuth crystals. We were not very successful
with some of our measurements upon the rods cut in various direc-
tions from a erystal which had been formerly used by van EvERDINGEN
in his researches, and we had therefore meant to postpone the com-
munication of ouv results until we had obtained a complete series
of determinations for various positions of the axis; just as we goto
press, however, the important paper by J. BecqurrEL in the Comptes
Rendus for 24th June 1912 reaches us, so that we now publish the
result which we had already obtained for the case treated by Lownps;
it is given in the following Table.

TABLE XIII.

HaLL-effect in a Bismuth crystal with the axis perpendicular to the field.
T2902 | P= 20°93 |
ea yA as 3 |
ie |e ee | R | H | RH R
2010 | 20.0103 —9.95 || 1850 | 18.0103 | +972 |
3140 30.6 gis: | 3700 | 26.0 | 47.03 |
| | |
| 5870 | 38.6 —658 || 5800 | 33.6 | +5.79
8250 | 42.1 beet i | 8100 43.7 |. 5.02
10270 44.3 25481 11080 53.1 | +4.79

At hydrogen temperatures / is positive and approximates to a
constant value; at ordinary temperature it is AH corresponding to
negative values of # which approaches a constant value. It is possible
that small impurities exert considerable influence upon these changes, -
and it would therefore be risky to conclude from the fact that the
value of A at hydrogen temperature which we have found is not
greater than that found by Lownps for one direction in liquid air, that
no change of any importance takes place between tbe latter tempe-
rature and that of liquid hydrogen. (The resistance measurements
show that Lownbs’s bismuth plate was freer from impurity than ours).

319

Physics. — “On the Hat. effect and the change in the resistance
in a magnetic field at low temperatures. Il. The HAL-effect
and the resistance increase for bismuth in a magnetic field at,

-and below, the boiling point of hydrogen”. By H. Kamer.incu
Onnes and Bener Beckman. Communication N°. 129° from the
Physical Laboratory at Leiden.

V. Linear variation in strong fields.

§ 14°). Linear variation of the Haun. effect for bismuth in strong fields.

a. As was suggested by J. BecqurreL’,, the fact that the Hauer effect
for bismuth in strong fields can be represented by a linear function
of the field strength may be regarded as resulting from the compo-
sition of the effect from two separate components. One of these is
proportional to the field, and was found by us (see Comm. N°. 129¢
§ 4) to be always negative for plates of compressed electrolytic
bismuth. The second approaches a limiting value, and, with our
plates, was found to be constant at hydrogen temperatures, in fields
greater than 3 kilogauss.

That is to say, the law of linear dependence upon the field is
rigidly obeyed by the first component of BecQuEREL, within the limits
of experimental error in fields greater than 3. kilogauss. As an
example we give in Table XIV values calculated from

RH=dH+U' :
in which a’ — 54.3 and b' = 42.10?
(with both a’ and 6’ in absolute units), and alongside these we put
values for T= 20°.3 K. taken from Table III.
‘The linear form is found to be just as rigidly obeyed in the
experiments made by Berner Beckman upon the same experimental
material at the temperature of liquid air; for an account of these
experiments we may refer to § 3 of the Commnmnication N°. 130qa.

It is noteworthy that, in the case of the second component, satura-
tion is most easily attained at low temperatures. In this respect this
component is analogous to the magnetization of a ferromagnetic sub-
stance. The linear dependence of the first component upon the field
strength recalls the behaviour of diamagnetic polarisation. In the
region of very low temperatures the very rapid variation of a’ with
the temperature can be represented by a simple empirical formula
which was obtained by compounding the data given by Beckman for
liquid air temperature (see Communication N°. 130a). From this it
was found that

(3)

1) The sections of this paper are numbered in continuation of those of Comm.
No. 129a.
2) G. R. 154, 1795, 1912.

TABLE XIV. |

Linear variation of the Hatt effect |
for “ell in strong fields T= 20°.3 K.

| |

H | RH Obs. RH Calc.
3450 230><103 229<103
| 5660 350 352 |
| |
7160 431 434
8520 503 507 |
9880 583 582
11090 647.5 647
| 12090 700 702
a=a eB. i Fd eee (4)

within the temperature region 90° K. ee 14° kK. A much more
complicated formula would be required to embrace the observations
at higher temperatures as well.

On going down to liquid hydrogen temperatures the constant b’,
the maximum value of the second BrcquEREL component, which is
negative at ordinary temperature becomes positive in the case of
Bi, and Bi,771. BUCKMAN’s investigations upon the same plates at the
temperature of liquid air show that the reversal of the sign must
take place below 72° K.

}. With regard to crystals we have already stated in § 13 that,
when tne crystalline axis is perpendicular to the field, the Hau effeet
is negative at ordinary temperature, and approaches a limiting value.
To this we may now add that with another rod also with its axis
perpendicular to the field we found, at ordinary temperature, a maxi-
mum at 47 = 9500, and then a decrease (10-3 RA fell from 37 to
35,4); this leads us to suspect that proceeding to stronger fields than
those we employed would have brought to light the same behaviour in
the case of the rod quoted in § 13. At hydrogen temperatures the sign
of the Haut effect reverses and becomes positive, increasing linearly with
the lield for fields above 3 kilogauss*). From this it appears that in

J. Becqu REL draws attention to the fact that at low temperatures RH
becomes very large. The values we here give for hydrogen temperatures make
this all the more striking. For Bip we obtained RH = 500.103 for H = 8500.

With this plate, indeed, at the temperature 7’ = 90° K. we get a higher value
(RH = 214.10% for 7 = 8500) than that given by BrcqueREL for his_ plates.
From his data (loc. cit.) we calculate for the temperature of liquid air RH = 168.108

(or R=+19.8) for H=8500.

321

the case of the axis perpendicular to the field, the positive effect
must be much weaker at ordinary temperature than the negative,
and begins to be appreciable only at very low temperatures. What
we haye found for the case of the axis perpendicular to the field
is analogous to what BrcqurreL obtained with the axis parallel to
the field.

With our crystalline rod placed in a definite position the value
of the field at which the second component attains saturation at
hydrogen temperatures is the same as that at which a plate con-
sisting of crystals of various orientations (for instance, a plate of
compressed electrolytic bismuth) reaches saturation. That is to say, on
going down to hydrogen temperatures, the saturation field appears
to be independent of the orientation.

§ 15. Linear variation of the increase of resistance of bismuth
mn strong fields.

In § 2 we remarked that in strong fields the resistance varied
directly as the field. For fields of 12000 gauss upwards we find

!
w

te eee Pes GL S| oe ene)

Ww
(ef. fig. 1 of the Communication N°. 1380a by Berner Beckman) where
the values of.a and / vary greatly with peculiarities of the bismuth
employed (wire or various plates made from compressed electrolytic
bismuth).

Tt is worth noting that the coefficient a of the linear variation
of resistance, and the coefficient @’ of the linear variation of the
Haut effect can, for temperatures below that of liquid air, be repre-
sented by the same functions of the temperature, so that we may write
eee: tac eee 5.) Se te eg ES)
This is found to be the case when we use the values given by
Benet Beckman for the ‘temperature of liquid air (see sections 2 and
3 of the Communication N°. 130@) in conjunction with those con-
tained in Tables I, Il, and IIIf. If we remember that the values of
8 and 3’ can differ greatly for the different plates,

(for Bi,7 B=O0,023 and p' = 0,023
Biu 8 = 0,014 3 2k —=' 066

a big PO O27)
it is evident that we can as yet give no answer to the question
as to whether the values of @ and )' are the same or not for pure
bismuth, and the agreement in the case of 7,7 can quite well be
accidental.

The constant 4, which is very small at ordinary temperature,
becomes large and negative at hydrogen temperatures.

322

Physics. — “Magnetic Researches. VI. On paramagnetism at low
temperatures’. By H. KAMERLINGH ONnNEs and E. OostErauis :
Communication n°. 1292 from the Physical Laboratory at
Leiden.

(Communicated in the meeting of June 29, 1912).

§ 1. Introduction. In the present experiments which form a conti-
nuation of those discussed by KaMERLINGH OnNzEs and Perrier in Comm.
Nos, 122* and 124" we have again measured the attraction exerted by a
non-homogeneous field upon a long cylinder of the experimental sub-
stance. Unless where we state otherwise, the experimental substance
was finely powdered and contained in a glass tube just as was done
in the researches referred to. In the present experiments, however,
we adopted a device which had only been tried a few times in the
former series, and, in order to eliminate the effect of the glass, the tube
was taken twice as long as the part of it which contained the
powder, so that the two halves were the same except that one was
evacuated and the other held the powder; the evacuated part was
separated from the other by a plug of cotton wool which was placed
in our experiments at about the centre of the field of our Werss
electro-magnet. We now balanced the attraction by gravity, and
instead of allowing the tube to be drawn down by the attraction
of the field and to be raised to its zero position electromagnetically,
the tube was now drawn up by the action of the field and was
brought down again to its zero position by weights. The modified
form of the apparatus allowed much greater forces to be measured
without involving any considerable alteration; we shall return to its
description whenever a detailed account is given of the apparatus
used in the former experiments.

§ 2. Anhydrous Ferrous-sulphate. Comm.’ No. 124a_ stated that
it was intended to investigate this substance at temperatures available
with liquid nitrogen, so as to fix more definitely the temperature at
which y attains its maximum value, which lay according to the
experiments then made between 148° K. and 20° K. While this
particular investigation was our principal aim, at the same time we
repeated the measurements previously obtained at other temperatures.
The salt was dried by heating for some time in vacuo to 280° C.
special care being taken with this operation. We obtained the
following results: (see table I, p. 323).

If we compare these with the results given in Comm. No. 124a
for ferrous-sulphate which was practically anhydrous we see that a
small admixture of water diminishes the value of y, and that to a

023

TABLE |
Anhydrous ferrous-sulphate I.

ig z%.10° zy. 1.10% Limits of H Bath
290°.2 K 67.6 19617 14000 — 16000 Room atmosphere
169.6 107.2 18181 14009 — 17000 Liquid ethylene
71.3 200.4 15491
70.4 215.1 15143 14000— 17000 Liquid nitrogen
64.8 221.3 14729
20.1 402 8080
17.8 379 6746 > 10000 — 16000 Liquid hydrogen
14.4 335 4824

very large extent at hydrogen temperatures. For while the increase
in the value of x brought about by more efficient drying is only a
few percent at ordinary temperature, it is as much as 50°/, at 20° K.
That we must really look in this direction for an explanation of the

TABLE II
Ferrous-sulphate III. not quite anhydrous

7 —-z.108 | Limits of H Bath
289°.5 K 62.1 8000—17000 Room atmosphere
169 .6 95.7 9000—17000 Liquid ethylene
yg es 169.8
70 .4 182.0 | 5000—15000 = Liquid nitrogen
64 8 189.8
20 .1 231.4
LEAS 220.6 | 4000—17000 | Liquid hydrogen
14 4 204.8

differences between the numbers given in November 1911 and those
now communicated is evident from an experiment in which the
quantity of moisture present in the ferrous-sulphate was purposely
increased slightly (the quantity of water present being probably a
little greater than that of ferrous-sulphate II, by which we designate

324

the specimen used by KAMERLINGH Onnes and Perrier). For this not
quite anhydrous ferrous-sulphate HI we found the data given in table II

p. 323).

§ 3. Deviations from Curtr’s law. In previous Communications
an attempt was made to establish a law other than Curte’s (which
from Table I does not hold for anhydrous ferrous sulphate) to
represent empirically the variation of x with temperature ; for this was
given the law yV 7’=const., which did quite well indeed represent
the various observations then under consideration. The analogy of
phenomena exhibited by ferric sulphate, which lead one to believe
that this substance exhibits ferromagnetism at low temperatures,
suggested to us to express y—! as a function of the temperature,
and we found that the formula x¥(7+A’)= C’, which has also been
used by Weiss and Fokx’)*) was worth trying with positive values
of A’ and C’. As long as we keep above — 208°C. this formula is
quite satisfactory for the representation of the deviations from Curir’s
law at low temperatures found by KameriincH OnnEs and PERRIER
and by us up to the present; we shall give several instances of this
in § 7. The variation of x as a function of the temperature can then
be expressed for ferrous sulphates of different degrees of dryness by
ascribing different values to A’. below the maximum y—! remains
still linear, at least to a first approximation, but the constant, C",
which replaces the Currie constant in that region, is negative, as is
also A", the constant which replaces J’.

The results obtained for ferrous sulphates I, iI, and HI are shown

1) Starting with the idea of corresponding states for para- and ferro-magnetic
substances, we were led to the formula x (7’+A') =C' by an attempt to deter-
mine the absolute temperature © of the possible GuRIE point with the help of
experimental data in the suspected region of the “magnétisme sollicité”. We found
© negative, which brought to our minds the notion of the inverse field by which
Vorer has tried to explain certain peculiarities of the ZEEMAN effect as shown by salts
of the rare earths. It was only after we had represented the deviations from CuRIE’s
law shown by paramagnetic substances at low temperatures by means of this
molecular diamagnetic field that we noticed that Werss and Fox had in the same
way represented the behaviour of ;-iron and the nickel alloys above the CURIE
point. Wetss and Fox show that there is no prima facie cause why the WEIss
molecular field could not occur with the opposite sign. It speaks well for the
reasonableness of the hypothesis that we should be led to it for entirely different
substances and under circumstances in which the quantity = fundamental in
paramagnetism, is so much greater than in the experiments made by WEISS and Fox.

*) After this communication was printed in dutch, we received the dissertation

of A. Preuss, Ziirich 1912, in which there is found also a negative molecular
field for the alloys of Fe with less than 16°/, Go. [Note added in the translation. ]

i 325

a ‘graphically in Fig. 1. C’ and C” are seen to be practically equal

17500

15000

a Fig. 1.

for the different degrees of dryness, while 4’ (31° for ferrous sul-
phate I) and A” differ and increase in magnitude with the quantity
of moisture present in the salt.') The difference between the values
of (’ and C”’ for different degrees of dryness is so small that it
practically coincides with the limits of accuracy of the observations.
On the present representation the temperature at which x attains its

1) For crystallized ferrous sulphate the line, according to Table [!, Comm. 122a
of KAMERLINGH ONNES and Perrier, is passing almost through the origin, 4’ being
2° only. So, interposition of a small number of water molecules seems to increase

a’, of a great number to reduce it to a very small value. (Note added in the
translation).

326

maximum value is given by the point of intersection of the two
lines, which are determined by the constants C” and 4’, in the first
disturbed paramagnetic state (we shall designate that state normal
in which the Curm law holds), and by the constants C’’ and A’’
in the second disturbed paramagnetic state. The temperature of the
maximum therefore alters with the quantity of moisture contained
in the salt. It lies just above the boiling point of hydrogen, so that
a new arrangement of the experiment is necessary before the correctness
of this deduction can be tested and at the same time an investigation
made as to whether the formula given holds good up to the maximum
or not. That this is probably so is corroborated by the fact that on
cooling ferrous sulphate I down to 20° K. x would increase continuously
until it began to fluctuate about its mean final vaiue, while on
cooling ferrous sulphate [HI y clearly overstepped its maximum value
before the temperature of the bath was reached, just as is to be
expected from the diagram.

§ 4. Anhydrous ferric sulphate down to — 208°C. Anhydrous
ferric sulphate was also investigated at the same time as the ferrous
sulphate to ascertain any possible influence of the valency of. the
iron atom, and to see if x for ferric sulphate also reached a maximum
value. Down to the temperatures available with liquid nitrogen and
in that temperature region we found perfectly regular behaviour
corresponding to what we have termed the first disturbed paramag-
netic state. We found:

|
64 .9 | Tia 16980

Valency, which plays such an important part in solutions, has
here but a very slight influence down to and at nitrogen temperatures ;

327

the difference between the molecular susceptibility of anhydrons
ferric sulphate and that of ferrous sulphate I is only about 3°/,.
We may note that A’ is the same for both anhydrous ferrous
and ferric sulphates.
For the behavionr of ferric sulphate at hydrogen temperatures we
may refer to § 8.

§ 5. Manganese chloride. Manganese chloride was used which
had been freed from water as far as possible; it was not possible
to make it quite anhydrous. As can be seen from the following
table it obeys Curiz’s law exactly at temperatures above —208° C.;
values are also given for hydrogen temperatures for which the law
no longer holds.

TABLE IV.
Manganese chloride [, pulverised, not quite anhydrous.

T ¥.106 ~.7.106 Limits of H Bath

290°.8 K 106.5 30970 6000--17000 G room atmosphere

169 .6 183.4 31100 5000—17000 liquid ethylene |

TPA 403 31190 5000—16000
| liquid

70 5 440 31020 7000— 16000 |

| nitrogen |

64 .9 480 31150 5000—16000 |

air % The & =

20°.1 1419 28520 5000—16000 |

} liquid |

17 8 1589 28280 3000—10000 ?

hydrogen |

14 .4 1881 27090 | 3000 —16000

§ 6. Gadolinium sulphate. The observations of KAMERLINGH ONNES

TABLE V.
Crystallised gadolinium sulphate II.

|
|
; - = : ail
£ y10° | ~7.10°| Limits of H Bath

328

and Prrrimr were supplemented by those included in table V (p. 327)
which further confirm the validity of Curin’s Jaw and the absence
of saturation phenomena.

This result, on account of the large number of magnetons present
in gadolinium sulphate and «f the resulting large value of the a of
LANGEVIN at this low temperature is of importance to LANGEVIN’s
theory, according to which saturation phenomena are here still outside
the limits of experimental accuracy.

§ 7. Summary of the deviations from Curir’s law. We here append
the representation of the experiments of KaMERLINGH Onnes and PERRIER
on dysprosium oxide (Comm. N°. 122%) by the formula x (7+ A’)=C’.

TABLE VI.
Dysprosium oxide
represented by the formula
x(T+ aJ=C'; 2'= 16

7: | 308) Al yareee)
28895 K | 220.2 69790
170 374.6 69670
[132 .79 445.7 66320]
20.25 1915 - 69420
17 .94 2032 68970
15 95 2173 69430
13 .93 2334 69860

With the exception of the measurement made with liquid ethylene
boiling under reduced pressure, which is rendered doubtful by the
otherwise good agreement between observation and formula, the
differences do not exceed the limits of experimental error.

If we collect the various data hitherto given in this paper the
following different cases are seen to occur.

Gadolinium sulphate follows Curt’s law over the whole region of
low temperatures down to the lowest hydrogen temperature, 14° K,
throughout the whole of this region we may call it a normal para-
magnetic substance.

ver the whole region of low temperatures and down to the lowest
hydrogen temperature dysprosium oxide obeys the law x(7'+ A') = C’

329

with 4’ and C’ positive. Over the whole of this region it shows
therefore a disturbance of the first kind, which is to be ascribed
to the occurrence of a Werss molecular field of opposite sign.

Down to —208° C., and perhaps lower, manganese chloride is
normal. At hydrogen temperatures it deviates in a manner which
may to a first approximation be represented by 7(7'+ A’')= OC, or,
in other words, the disturbance throughout this region is of the first
kind. Crystallised ferrous sulphate behaves in exactly the same way.
(Comm. N°. 1227).

Both anhydrous ferrous sulphate I and ferrous sulphate not quite
anhydrous (see § 3) show a disturbance of the first kind down to
— 208°C. and probably to about — 250°C.; at hydrogen tempe-
ratures they show a disturbance of the second kind (both A” and
C" negative).

At low temperatures down to — 208° C. anhydrous ferric sulphate
exhibits the same disturbance of the first kind as anhydrous ferrous
sulphate. At hydrogen temperatures it exhibits the deviations which
are discussed in the following section.

§ 8. Ferric sulphate at hydrogen temperatures. For the first time
in the course of our observations we here found a dependence of
the susceptibility upon the magnetic field which leads one to presume
the existence at these temperatures of ferromagnetism in a substance
which at ordinary temperatures is paramagnetic. We must in the
meantime confine ourselves to this general remark. Accurate data
giving magnetisation as a function of the field at different tempera-
tures cannot be immediately deduced from the attractive force exerted
upon a long cylinder in a non-homogeneous field, as long as y remains
an unknown function of #7. The investigation has therefore in the
first place been continued with a cylinder of short length (a disc)
of ferric sulphate placed in a certain part of the field at which
both H and a are known.

We must refer to a subsequent paper for the results obtained and
for the deductions which may be drawn from them.

22
Proceedings Royal Acad. Amsterdam. Vol. XV.

3080

Physics. — “A theory of polar armatures.” By H. pu Bots. (Com-
munication from the Bosscha-Laboratory).

A well-known partial theory for truncated cones was given by
SrrraN and applied to the isthmus-method by Sir ALFrep Ewine. As
a first approximation the magnetisation of the poles is everywhere

Fig. 1.

assumed parallel to the a-axis (Fig. 1) and thus polar elements have
to be dealt with on the terminal surfaces only.

Now the magnetic field due to coils of various shapes has been
thoroughly investigated in every detail by various authors, whereas
that produced by ferromagnetic pole-pieces is only known for parti-
cular points in a few special cases. I believe it is now useful to
develop a more general and complete theory for arbitrary points
in the field, regard being also paid to protruding frontal surfaces,
such as I have been using since 1889 (see fig. 1).

Considering the increasing introduction of prismatic pole-pieces,
e.g. for string-galvanometers and other applications, I have also
calculated equations for these, generally exhibiting a formal analogy
with the conic formulae. Instead of a meridian section, Fig. 1 in
this case represents a normal section, the generatrices being directed
normally to the plane of figure and parallel to the z-axis.

For the determination of attraction or repulsion the first derivatives
of the field with respect to the coordinates have to be considered ;
e.g. for gradient-methods in measuring weak para- or diamagnetic
susceptibilities and also for extraction-magnets, such as those used
in ophtalmologic surgery and in ore-separators.

Besides the intensity of the field its topography, especially its
more or less uniform distribution appears more and more important
in quantitative work and ought to be investigated. Here the second
derivatives of the field also come in.

The following equations may occasionally serve as well for certain

331

electrostatic problems showing the same geometrical configuration,
on account of the well-known general analogies. The details aud
proofs are to be given elsewhere.

Round armatures. Considering in the first place surfaces of
revolution, more especially cones, the coincident vertices of which
both lie in A, the field in this point is known to be

= ~ . ~~ s B
N° =H, + H, — 4a J sin vers B + 4a J sin? a cos a log rach (I)

The notation sufficiently appears from Fig. 1. Both terms are
generally of the same order practically; the first corresponds to the
truncated frontal planes, the second to the conic surfaces; the latter
shows a maximum for @ = tan—!V2 = 54°44’.

In order to judge of the field’s uniformity we now consider the
second derivatives, which are related to one another by LaApLacr’s
equation and the symmetry of the case. The z-component, ‘,, of
the field is everywhere meant, though the index z is mostly omitted
for simplification. For the centre A, where the first derivatives
evidently vanish, the following values are found

Bo OD 5 OD,

., 3 sin? Bcos® B . 2 sin‘ B cos B
—— 2 oo = 4a § ———_—- = 4a § —————_ (1)
Ou? 07? 02? a® b?

Now the term 9, always shows a minimum in the centre 4,
when passing along the longitudina! z-axis, corresponding to a
maximum along the equatorial transverse axes, because the numerator
sin? B cos*B remains positive for 0 < 8 < 2/2; in particular this is
a maximum, and accordingly the non-uniformity is greatest, for
6 = tan—V2/, — 39°14’.

The term , behaves exactly in the opposite way, its second
derivative vanishing for that same angle. This well-known result also
follows from the general formula, which I now find, viz:

os == =2 es —-2 OD. = Ase ae a cos a (5 cos? «-3\( 5 - ze
On? 07? 02? ee rahe. is bP EP

As B > 5b this expression evidently is + for @ as cos} {/*/, == 39°14’;
accordingly , shows a longitudinal minimum and transverse maximum
for smaller semi-angles, whereas for larger ones the reverse holds,
so as to make the field weaker on the axis than in its lateral
surroundings. Finally for the total field

0? (D, =e §,) as
Ox? cA B?

22*

3 is
An S ae E sin‘ 8 cos 8 + sin* acos a(5 cos? a-3) (2 + z) |

dod

Equalizing the contents of the square brackets to zero gives a
relation between @ and #. In most practical cases 6°/5" may be

neglected and we find

60°

ao for | = sau 54°4 a | 57? 63°26’
the value: B= 90° 79°96" | 76°32. | 12°49" 163 26°

as corresponding sets. For the most favourable semi-angle a = 54°44’
it is thus possible to combine uniformity and intensity of the field.
For a— 63°26’ the same value is obtained for 8 and we have the
ordinary non-protruding truncated cones. These results, somewhat
at variance with current ideas, were shown to be correct by
measurements with a very small test-coil, for which I am indebted
to Dr, W. J. pe Haas.

For excentric axial points, at a distance « from the centre A, the

value of the first term is

E Ane ata a—w ) (4)
J, (x) Seay ( WV (a a eo 2V (a—a)? +b? e 5

That of the second term for one single cone

B-x sin acosa+ V B?-2 Bz sin acos ata’ sin’? a

5 (a) = 225 sin® aos a| log $$
; b-x sin a cos a + V b?—-2b2 sina cosa + x? sin?a

t ee

V B?—2Besinacosa+ x sin*a Vb? —2basin acosa + a sin® a

xtga—2B xvtg a—2b
- (5)

This formula was developed by CzermMak and HAUSMANINGER in a
somewhat different form.

By (4) and (5) the total field for any axial point may be calculated,
whether the vertices coincide or not. However a cone is a magnetic
“optimum-surface” relatively to its vertex only.

For excentrie points on an equatorial y-axis the first term becomes

$,(y) = 23 | 10
0

a(ry cos @—a*?—+’) i!)

ey 6
lene sin? OV a? +y?— 2ry cos 0+ r?|r=0 °)

which is reducible to elliptic integrals. For the second term a still
more complicated integral is found, of which the first part also
leads to elliptic integrals of the third kind; whereas the logarithmic
term can only be expressed by series of elliptic integrals, a result
kindly worked out by Prof. W. Kaprryn. In fact for two concentric
cones we find

333

b + a4 26 s A s cos A
i. (4) 5 sin* ceone {| 2 _y con. G) sin” @ is € 2 ae
> 2
(1-sin?acos? 7) }2 “Db yein? coum eens

0
B+ (y — 2B cos @) sin® a cos 6

ee (il — sin* acos* 0) V B? — 2 By sim? a cos 0 i y? sin? \
—— y sin® acos @ -+- VB ae By sin” acos @ + =a sin 7a

=
y

Oe y? sin® a
b — y sin® a cos 0 — 5? — 2 by sin? acos 0 + 7? sin? @

coat = Saas
B— y sin® acos6 — VY B? — 2 By sin’ acos@ + y? sin®

+ log
b — y sin? a cos O +- VE — 2 by sin? @ cos

If the point considered neither lies on the z-axis nor on the
y-axis the equation for , (7, y) becomes more complicated still.

By applying (4) to pole-shoes having parallel frontal planes only
the field for any axial point is easily found; after integration and
division by the polar distance the mean value is found to be

= x Techie ev (il Be
eee | ppd A oe ee spe eee Co

2 a

As a matter of fact the uniformity in such cases is generally
rather satisfactory. It may even be improved within a larger range
by hollowing out the front surfaces. If a spherical zone be considered
of radius fk, perforated in its centre; if the visual angle of the
periphery be 2y, that of the aperture 2y' as seen from the sphere’s
centre, then at a distance x from the latter the field is

Qa} ja‘ —2R! + (2R* - a*)Ree cos 0+ Rea? sin® O)=7
32° | £V a {R20 cos 0 b=

(9)

The sign depends upon whether the point considered lies on the
"coneave or convex side («#«< Kor >). By (9) the field in any
axial point of a centered pair of spherical zones may be calculated,
the interferric space having the shape of a biconvex, biconcave or
concave-convex lense; without aperture we have y' = 0. The formula
for 0°)/d2* becomes rather complicated; this derivative vanishes for
concentric concave hemispheres, for which we find after considerable
simplification

es Sa ek. on OY ee Nan
24 J (10)

independent of 2, i. e. a perfectly uniform field, a result following
moreover from known properties. The same holds more generally for
a spheroidal cavity in the midst of a ferromagnetic medium, rigidly
magnetised parallel to the axis of symmetry; we then have

334

ee ay cos—l m)) ix, Des
La V1—m?

here m denotes the ratio of the axis of revolution to a transverse

axis of the spheroid; such a case might be approximately realized if

the necessity arose.

The attraction exerted upon a smali body inan axial point is pro-
portional to 0/dx in case of saturation, or to $. 0$/de if a magnetisation
proportional to the field be induced in it. It may therefore be found
by differentiation of the expressions (4), (5) or (9), though this gene-
rally becomes rather intricate.

Prismatic armatures. If we denote the length at right angles to
the normal section (Fig.1) by 2c, then we have for c=, 1. e.
practically for prisms of sufficient length, if the inclined planes have
one mutual bisectrix through A

B
S° = Ho Sy 8 ja SS sin @ 005 alog = > 7. ee

For shorter prisms the first term becomes

b c? |
(2302 | 7
Ds one a a? +b? -+1-¢? ( )

and the second term

ie bares bay
‘Bs 1 + ——_— — 1
B ( — sin? & )

N, = 83 sinacosa| log — —log —

b > ae
‘ aves =< ~ 1)
_ c sin’ a —

The subtractive term in brackets vanishes for c = o; then evidently
05,/da vanishes for a—=45°, which is the most favourable angle
in this case, giving the strongest field ; for shorter prisms however
a > 45°.

The uniformity along the z-axis is complete for prisms of sufficient
length, i.e. 0°5,/d2? = 0; for this case we find

OD <0, Os sin 28 cos? 8B sin? B sin 28

— = $3 ——_ 85 ee eee
On? Oy? J a2 J b? ( )

. (14,2

This expression remains positive and passes through a maximum
for 8 = tan //'/, = 30°, the non-uniformity consequently being
greatest for this angle.

The term , again behaves inversely, its second derivative vani-
shing for this same angle; in fact cos 3a then vanishes in the formula

335

07.0, 07D, 1 1
——- = 85 sin® a cos 3a{—— —]}. . . .(2*)
etatante(e—f) sw
As B> Ob this expression is + for aS 30°. For the total field
we finally have
0? 1 b?
228 =— oy 7 sin? B sin 28 + sin® acos 3a (: -— i . (3*)
Equalizing the bracketed terms to zero gives a relation between
a and 8; neglecting 6’/4* we find
e.g. for a= 30" | - 45° 48° | 50°46’ 54°44’ | 60°
ihe yaine= p— 40 |°82738" |-79°S9’ | -77°9’ =| 72°26’ | 60°’
as corresponding sets. For ¢ = 60° we obtain the same value for 8,
i.e. non-protruding frontal rectangles.
In excentric axial points at a distance z from the centre A the
value of the first term is

2ab

ay iS —_ x
(x) — 45 tan 1 as ae . . . ° . ° (4 )
That of the second term for one pair of inclined planes
ae B? —2Bersinacosat 2’ sinra
N,(«) = 25 sin a cos a | log
b? — 2bz sin acos a+ a’ sin? a (5+)
; 5
b—«esinacosa B—e«sinacosa
+ 2 tga tan— —tan—1—________—
a“ sin® a & sin? a

By means of (4*) and (5*) the total field may be calculated for
any axial point, whether the 4 inclined planes intersect in one line
_ or not; only in the former case do they form an ‘“‘optimum-surface”’
with regard to A. ;

For excentric points on an equatorial axis of y we find as the
first term, for c= 2

a ae (6*)
=A S\tan— ;
D(y SD a? aa b? a= y?
and as the second term for two pairs of inclined planes
B+ 2Bysiv? ast y’' sinta
= § st log ———— 4

aly) Mime i oe Bs + 2by sin? a+ y* sin’? a Xx |

B* — 2By sin’? a+ 7’ sin’? a .y sin? a + b a

—____________+______ + 2tga@| tan—+—————_ +, (%*)

b? — 2by sin? a + y’ sin’? a a y sin @cos at

Ww sin? a — b
n+

sinrtat B ysin?-a— B
+ ta a eS eer —tan—!—_____——_

y sin @ C03 & y sin acosa y sin & COs &

The distribution of the field is thereby completely determined ; in

336

the symmetric equatorial plane it is everywhere directed parallel to
the z-axis. The most general case of any arbitrary point in the
field leads to an expression for #, (2, y’, capable of integration but
more complicated still than (7*). By differentiation 06./dy may also
be obtained, though this also turns out rather intricate. In much the
same way the distribution of , along the z-axis may be calculated
for prisms of finite length and the integrals.

~ ~ 1
zo =

[ §,(z)dz and | §?,(z)dz

cal Al

may be computed, of which the latter is of importance e. g. in the
study of transverse magnetic birefringency. The case of an air-space
shaped like a cylindric lens is of less practical importance and

may here be omitted.

Physiology. — “Influence of some inorganic salts on the action of
the lipase of the pancreas.” (By Prof. Dr. C, A. PEKELHARING.)

Hydrolytic fat-splitting by the lipase of the pancreas, the only
enzyme that will be considered here, may be aided by a number
of inorganic salts as well as by bile acids. It does not follow however
that this action is always due to the same cause, to the process of
activating the enzyme.

It has been proved by Racurorp as early as 1891 that bile aids
the action of the lipase of the pancreas especially on account of the
presence of bile salts. The fat-splitting power of rabbit's pancreatic
juice was increased by the addition of a solution of glycocholate of
soda nearly as much as by the addition of bile*). According to the
researches of more recent investigators, especially TERROINE *), it is
highly probable, that the action of bile acids is based on a direct
influence on the enzyme, so that here we might speak of an “activator”
in the real sense of the word. The fact that various electrolytes also
aid the hydrolysis of fat by the lipase, has-been demonstrated: by
Porrryin*) and more in detail by Txrromnr‘*); afterwards also
by Minamr*). However, the mode of action of the electrolytes is still
unknown, as has been clearly pointed out by TrRroine. The investi-
gators | mentioned used for their experiments pancreatic juice or a

1) Journ. of Physiol. Vol. XIl. p. 88.

2) Biochem. Zeitschr. Bd. XXIII. 8, 457.

8) Compt. rend. Acad. d. Sciences, T. CXXXVI, p. 767.

4) 1. c. S. 440.

5) Bioch, Zeitschr. Bd. XXXIX, S$. 392,

glycerin extract of the pancreas, liquids containing, besides lipase, a
great quantity of other substances, chiefly proteins, and moreover
some electrolytes. Trrroine has tried to remove the electrolytes from
the pancreatic juice by dialysis, but this did not bring him nearer to
his end, the dialysis causing the juice to lose its lipolytic activity.

RosenHEmm has discovered‘), that this was not due to deleterious
action on the enzyme by the dialysis, nor to the diffusion of the
lipase through the wall of the dialyser, but to the removal of a co-
enzyme that readily diffuses, that withstands boiling and is soluble
in alcohol.

If the diffusate is evaporated and again added to the contents of
the dialyser, its fat-splitting power is as great as before. The co-enzyme
can “be separated from the lipase not only by dialysis but also, as
RosenHerm demonstrated, by diluting the glycerin extract of the
pancreas with water, the result being a precipitate containing the
enzyme, while the co-enzyme is left behind in solution.

RosENHEIM’s suggestions induced me to use for my experiments
lipase prepared in the following way:

Fresh pig’s pancreas was minced up, then mixed with about twice
its weight of glycerin and percolated after 24 hours. By filtration
through a compressed pulp of filterpaper a solution can be obtained
that is only slightly opalescent, whose lypolitic power however is far
‘inferior to the original extract. Besides it yields after dilution with
water a much smaller quantity of precipitate containing lipase. In
preparing the enzyme I therefore used the extract only percolated
through fine linen. This extract is highly opalescent, but little or no
precipitate settles even after standing long. Part of this, mostly 30 ee,
was mixed with ten times its quantity of distilled water. The liquid
is very milky; however a satisfactory precipitate is not always
obtained.

To this effect a very faintly acid reaction, by addition of a few
~ drops of diluted acetic acid, is required so as to colour sensitive
“blue litmuspaper faintly red. A stronger acid reaction would also
cause a rather considerable amount of trypsin and trypsinogen to be
precipitated. Next day the perfectly clear liquid is cautiously de-
canted off fromthe residue and exchanged for 300 cc. of water; if
Necessary the water is acidulated with a few drops of acetic acid.
After precipitation the decantation is repeated. The remaining fluid
together with the precipitate is put on hardened paper in a Brcnner
filter and filtered off under pressure. The precipitate is repeatedly

) Proc.: Physiol, Soc. Febr. 19, 1910, Journ. of Physiol, Vol. XL.

338
washed in distilled water on the filter. It is then a greyish white
mass which, after being thoroughly deprived of the superfluous water,
can be easily removed from the filter and is now sufficiently free
from electrolytes. After incineration the substance dried at 110°C.

0.1521 erm. yielded 0.0004

gr. of ash
and 0.2761 grin. yielded 0.0010 gr.

of ash.

The solution of this ash in boiling hydrochloric acid was yellow,
which colour disappeared on dilution with water. This solution
got vividly red with potassium sulphocyanate and did not give any
calcium reaction. It was evident therefore, that the ash was chiefly
composed of iron phosphate, which was not present before but only
formed during incineration. ‘

The matter precipitated by dilution of the glycerin extract with
water is soluble in highly dilute alkali. However, it also dissolves in
glycerin without alkali. To effect this the precipitate, taken from the
filter, was rubbed up in a mortar with pure glycerin. The solution
gets clouded, nevertheless practically homogeneous. It preserves its acti-
vity also after standing for a long time. Filtration makes it quite clear
again, but deprives it of much of its activity. That is why I used
the unfiltered solution. To dissolve the precipitate from 30 ce. of
pancreatic extract, 20 cc. of glycerin was used, after which process
the concentration of the enzyme — considering the inevitable loss of
matter — was about equal to that of the original extract. The
proteolytic and the amylolytic enzymes have been all but eliminated
by the washing. The glycerin solution hardly attacks boiled starch
and fibrin, not even after addition of some calcium chloride. It
contains however a considerable amount of lipase. Still, the action
of the enzyme is extremely weak without the addition of other
substances.

As Rosgnueim detected, its activity is raised by mixing with the
washwater (concentrated by evaporation), which has been separated
from the precipitate, also when the evaporation occurs at a high
temperature. Whereas in this respect Rosenneim’s statements were
fully confirmed by my experiments, I have been able to prove that,
contrary to RosENHEIM’s results, the power to aid the lipolysis is not
lost through combustion. It is necessary, however, to dissolve the ash
with a small quantity of boiling hydrochloric acid. When mixed
with the neutralized solution, the glycerin solution of the enzyme
(which further on I shall call only “lipase’’) evinces intense lipolysis.

It is especially (though not exclusively) the calcium present in the
ash that increases the activity of the enzyme. The bearing of very

339

small quantities of lime salt on the lipolysis is not hard to test:
Some drops of commercial olive oil are mixed with highly diluted
soda and a few drops of lipase. After thorough intermixture by which
the enzyme, left in solution by the weak alkali, is equally distributed
in the fluid, and after addition of a little phenolphthalein, equal
portions of the emulsion are put in two tubes, after which to the
one calcium is added, for instance 1 drop of CaCl, 1°/, to 5 ce.
of the fluid. The red colour will disappear, at least will get much
fainter. Subsequently the fluid is made as red again as that of the
other tube by cautious addition of sodium carbonate. When both
tubes are heated to the temperature of the body, it will be seen that
the one with calcium soon loses its red colour while its acidity is
gradually increasing, whereas the colour of the other hardly changes
or does not do so at all, in an hour’s time. The reaction should be
made very slightly alkaline, because the enzyme, especially at the
temperature of the body is soon destroyed by alkali.

It thus appeared that, in order to confer activity on the almost
inactive lipase, the only salt in it being a little sodiumcarbonate,
we do not want the addition of the mixture of substances dissolved
in water from the pancreatic extract, but that calcium chloride will
do for the purpose.

For a more exact investigation of the lipolysis | proceeded as
follows: 3 to 4 cc. of the lipase was mixed with about double the
quantity of a 0.2°/, solution of Na,CO, and on addition of ten drops
of phenolphthalein diluted with water to 200 ce. This slightly opa-
lescent fluid of reddish coloration was equally distributed among
four bottles of 150 cc. capacity each; to each bottle 1 ce. of neutral
olive oil was added, the oil being liberated from fatty acids by
shaking up the ether solution with sodium hydrate. Beforehand the
bottles were furnished with the substance whose action on the lipase
was the object of our research. When OH-ions were fixed by the
investigated matter, the pink colour was equalized in all the bottles
by means of Na,CO,. Hereupon the well-corked bottles were put
in the thermostat at 38° C. and turned slowly round an horizontal axis
mostly for 6 hours, so as to ensure a constant regular intermixture
of their contents. After 50 cc. of 92 °/, alcohol had been added to each

ees = Ace Se
bottle, the amount of acid was determined by titration with z NaHo.

_It now invariably appeared, that some acid had also been set free
in the bottles containing only lipase, some sodium carbonate, water
and oil. The quantity varied in different preparations of the enzyme,
but was the same in each preparation on different days. It can hardly

340

be supposed that the lipolysis, in this case, depended on bacteria and not
on the lipase of the pancreas. It came forth also when 10 ce. of
toluol was added to the fluid and it was arrested without toluol
even when the quantity of acid was extremely small. The greatest
amount of acid was in a great number of experiments found to be
still Jess than */,,, normal. SéHnGEN') found that the activity of the
lipase of bacteria can be destroyed only by */,, ” lactic acid.

Rosenuem holds that the fact that the lipase of the pancreas remains
active even without addition of co-enzyme, is to be ascribed to its
not being sufficiently purified. Considering that electrolytes had been
all but completely removed from the lipase prepared by me, and
again that the electrolytes of the pancreas (more especially the cal-
cium salts) are alone sufficient to aid the activity of the lipase, I
have tried to find another plausible explanation.

Since several observers have demonstrated that lipase, including that
of the pancreas, is able not only to split fat but also to synthetize
fat from fatty acid and glycerin, we may be justified in supposing
that the action of this enzyme consists in favouring an equilibrium
reaction, a supposition borne up by Drrrz’s’) laborious investigations.
Now, when the lipase decomposes oil in presence of calcium. salt,
it is very remarkable that, while the bottles are being turned round
in the thermostat, a considerable amount of calcium soap is carried
out of solution, partly as a solid precipitate lining the wal! of the
bottle, partly as gelatinous lumps in the liquid. It is therefore per-
missible to conclude, that fat-splitting is stopped as soon as a small
quantity of fatty acid has been separated; again, that in consequence
of this the lipolysis in the salt-free solution is indeed not wanting,
but that it soon ceases; and finally, that the action of the calcium
salt results in separating the fatiy acid in insoluble condition, as it
is4set, free.

The following experiments wvill illustrate the influence of CaCl,.

Every bottle contained 1 ce. of lipase in 50 cc. of water with
pbenolphthalein and just enough soda to evolve a very light pink
colour of the fluid. After six hours’ shaking in the thermostat at
38° C. the following results were arrived at by titration:

I without addition 2s 3o erg sae Sees ; NaHo
with 2 ¢.c-CaCh 1 i+ Pe hs 8 ue ae ee i
IL without addition set ee ee ee Pe

1!) Folia microbiologica. I, p. 199.
*) Zeitschr. f. Physiol, Chem, Bd. LU, 8. 279.

B41

pouemenU eet. (CAO eq ein ae oi oe ew we AA: ; NaHo
ina 5 See Pete ees a, a ®
III without addition Sra WER are ee | Ore x
MOR OAS, we ee ww OO -
IV without addition Jp EOI a ee | A ies a
mute Mera 2s Sle OG ,, 3
en ee 4, . Sagi ic ttt em ees TY aes ,,
a hs alee Le 3 ee eee Py. aes ra

I was not astonished to find, that the lipolysis did not increase
in the same degree as the amount of lime salt, nor that it did not
increase regularly, since the quantity of fat contained in the gelat-
inous deposit of calcium soap varies and in virtue of this a varying
quantity of fat is abstracted from the influence of the enzyme. The
precipitate also comprises free fatty acid, as it appeared necessary
during titration to shake the fluid well. Thereby the tough calcium-
soap was crumbling away and passed into coarse flakes collecting,
after standing a short time, on the surface of the alcoholic fluid.
When the calcium soap was broken up, alkali disappeared as was
evident from the disappearance of the red colour.

That CaCl, had indeed been decomposed by the fatty acid, may
also be concluded from the greater amount of H-ions in the fluid,
the determination of which I owe to Dr. Rincer.

A solution of 4 cc. of lipase with a little sodium carbonate in
400 ce., was distributed in 4 bottles, and 1 cc. of neutral oil was
added to each bottle. After digestion for 6 hours 50 cc. was pipetted
off from each bottle to determine the H’-concentration. The remaining
50 ce. containing about all the calcium soap was titrated.

a without addition, 0.6 er, NaH®,: ¢7 84'5< 10-8

6 with 10 mgr. CaCl, 1.0 ,, e eg 6.6 >< 10-7
C 33 25 > > 1.4 bP) bP)
d oe) 50 ” »” 1.6 ? ” CH 2.6 ~ 1p-¢

The apparatus only allowed to work with three H-electrodes at
a time, so that no H’-determination was made of c.

Though the greater part of the titratable acid was left in the
bottles, acidity, increasing with the amount of CaCl,, was distinetly
noticeable in the fluid pipetted from 4 and d. Thus the fluid contained
a strongly dissociated acid, which in this case was sure to be hydro-
chloric acid.

342

The lipolysis is also aided by lime salts that are very difficult to
dissolve.

4 ce. of lipase, after addition of 6 ec. of Na,CO, O.2 °/,, diluted
with water to 200 ec., is distributed in 4 bottles. To a only 1 cc. of
neutral oil was added. To 2} moreover, 2 ec, of CaCl, 1°/,, to ¢
2 ec. of CaCl, 1°/, as well as 3 ce. of an equivalent solution of
K,C,O, and to d the centrifugalised washed precipitate obtained by
mixing 2 ec. of CaCl, 1°/, with 3 cc. of the same solution of calcium -
oxalate. After digestion for six hours I found:

7
a uses 0.2 ce. ee NaHO

b 33 2.0 33 bP]
co op TOMAS 3
d 3) 1.0 b>] bP)

Calcium carbonate works likewise. The experiment also showed that
CO, was set free. .

200 cc. solution of 4 ce. of lipase, with a little soda in 4 bottles
a, 6, c, and d 50 ce. each. Beforehand I had put in ¢€ and d
+200 mgr. of freshly precipitated CaCO, which was obtained by
precipitating a water solution of 300 mgr. of CaCl, with Na,CO,
and repeatedly washing the precipitate with water in a centrifuge.

The fluids, each with 1 ce. of oil, were digested for six hours.
Immediately after this @ and c were titrated. Through 6 and da
current of air free of CO, at 25° C. was passed for an hour and carried
off through 50 ec.n/50 of barytic water. Subsequently also 6 and d
were titrated. The barytic water through which the air in d was
carried off had got very turbid, that of 6 hardly clouded. After
precipitation of the barium carbonate formed, 40 cc. of the limpid
fluid from each bottle was titrated with n/5 HCl. The result was:

7
a uses 0.6 ce. r NaHO

eee (1 Water eek yields 0,14 ec. 7 CO,

C5 ead ee ae 5
d 33 3.7 3) 9? > 3 1.18 3’) bP)

A rather considerable quantity of carbonic acid had therefore been
liberated from the calcium carbonate. The total acidity of d was 4.88,
that of c being 4.2. Though, in the titration of the digested cloudy
fluid, errors of 0.1, nay even of 0.2 cc. may pussibly occur, this
difference lies beyond the limit of the errors. The reason is obvious.
While the air passed through the liquid it was heated to 25° C. to

343

drive off the carbonic acid. Consequently the lipolysis could proceed
again for the very reason, that by expelling the carbonic acid the
equilibrium in the fluid was disturbed. Fatty acid could now be
precipitated again through presence of the excess of calcium carbonate.

As regards the action of calcium salts my results are not quite
the same as those of Trkrrotwwe, who found no or hardly any increase
of the lipolysis by calcium chloride. The nature of Terrorr’s ex-
periments however differed from mine. This experimenter made use
of dog’s pancreatic juice of which 5 cc. was digested with 5 ec. of
olive oil. This mixture, even without any addition, contained lime,
and besides other electrolytes, a large quantity of colloid substances
and comparatively little water, whereas for my researches the lipase,
as much as possible freed from the other constituents of the pan-
creatic extract, especially from the electrolytes, was dissolved in
glycerin and strongly diluted with water. This method enabled me
to study the action of the electrolytes all the better.

Indeed, Trrroise found the lipolysis inereased after addition of
magnesium- and barium chloride. This supports the belief that the
action of the enzyme is promoted by precipitation of the liberated
fatty acid. In this respect my results agreed with Terrorne’s as may
appear from the following instances:

Again 4 ce. of lipase was dissolved with a little sodium carbonate
in water to a volume of 200 cc. and divided into four equal portions
of 50 ec. To three of them equivalent quantities of CaCl,, BaCl, or
MgCl, were added. The faint pink colour which disappeared, returned
after the addition of some soda.

After six hours’ digestion I used:

ecihout addtipued:.. +. - ... 0.6 ce. : NaHO
Pam Mere Awl oe. fo. . 14, ;
Oe eA ee ee. AB, a
eC rare eee BRT, ee
Memmi andinione Ss s 3. 3 . . . O58 , te
Pi emmere wee 7 ', 3. , |. DO) 4, a
Ee i i 1: ine i
Pee eee ee OT, a

DP MIHNOULAGGIION* 9s. -. 2c. so. ee 4 OB y -
Sone Onemor: ORI neh. «ws OD, cs

PE mre EA Obey eA... tk! a BARS i

99 185 9 MgCl, ee Gs. nt bee he »” ”

344

The magnesium soap which was formed, was not so tough and
gelatinous as the calcium and the barium soap and could therefore
not take up so much of the oil. Consequently less oil was protected
against the action of the enzyme. I think the more powerful action
of the magnesium chloride is owing to this fact.

As known, sodium salts also aid the lipolysis. Here also, I think,
the action is caused by the separation of fatty acid from the fluid,
as insoluble soap. Sodium oleate is precipitated by solutions of different:
sodium salts of sufficient concentration, whereas in very weak
salt solutions as well as in water they dissolve with opalescence.

In order to arrive at an approximate estimation as to the degree of
solubility, I made a solution of sodium oleate by dissolving pure
oleic acid in alcohol and adding to it sufficient sodium hydrate to
produce distinct alkaline reaction. Several mixtures were made of
5 drops of this solution with 20 cc. of salt solutions varying in
strength. This mixture was at once filtered. The filtrate was found
to be less cloudy according as the precipitation had been more

complete.

Na@l 04 ot OR ee ee ta eee eae

ys Ds. ate ae) ee , slightly opalescent
NaBr: )26%/32. ee ae ee ee *. ao .@lear

a Bl? * BORIS Bie Es aan , slightly opalescent
se Die MIE iS Ge See Aaa » cloudy .
NaI) “FER R Es i> | Pe ie eee sou) elear

zs oes 2k) A Sie ee » cloudy
NaF Diy 2) 2h) eS ee 77 Clear!

_ 1:59) Ae. “ES Le ee » cloudy

CaGl~ 0.2)/,— 0 ae Se eee so clear

- OAS ge ex ts Sn se oe ee » clear

an) 5015 4 Perens, ee edie elie oS » very cloudy

i Oe Oe Pica Sure eee dane «Bee , hear

Oo teat as ee eee ;,- clear

bs IM be Pe eR Ret Fs, |. > elear

KC] A fe tase is cn So > choudy

> Pine Mack » very cloudy

By these researches the positive bearing of these salts (except
that of Nal and NaF) on the lipolysis was ascertained. KCl, which
does not precipitate soap by far so well as sodium salts, also exerted
much less influence upon the lipolysis. The experiments were made
in the usual way. Every time 50 cc. of a lipase and oil mixture,
with or without addition of salt was digested for 6 hours and sub-
sequently titrated. I used:

B45

Peewiinout addihom . =... 3. 0.8 ce. ; NaHO
Grin ori, Wate on sna Se 2.4 ,, r
Po ands 55 et) on tae Lo re
aS ear ae Fetal be ne 4.4 ,,
tLewinout addiien. . . . . , . 0.8 ,,
ineR ene 5). Ok, O.9 .; :.
a” are ag ee eg i ee
6 ye 2.0 z
Mi-without addition . . - -. . >. 0.5
Weert NA: se. fo. 5,
tel ioe ed Eo 2 oe PO. 7
tee ik eC ag Tk ee :
EV withigutadditioy ~° 2. . 2... Oss «,.
Witheo SRM NAC Se PS -s Be x es
ce ONE Paes. 3 A ras y,
Path Pee ec S74. %

When the fluid contained Nal it got slightly yellow during digestion.
That the lipolysis was very insignificant every time was no doubt
owing to the liberation of iodine. NaF, indeed, aided fat-splitting in
some degree, but much less than NaCl and NaBr.

The above experiments led to the conclusion, that the electrolytes
under investigation did not aid the lipolysis by conferring activity
on the enzyme itself, but by neutralizing one of the products of the
splitting, viz. fatty acids.

I have tried to test this also in another manner. An activator of
the lipase, in the real sense of the word, may be expected to exert
its influence as well in the synthesis of fat from fatty acid and
glycerin as in fat splitting. Such indeed is the case with respect to
bile acids as Hamsik has demonstrated '). If however the action of
electrolytes consists only in the precipitation of soap, they cannot
promote the synthesis, a counteraction is rather to be expected.

I proceeded as follows :

Glycerin was digested with oleic acid and lipase in the thermostat
at 38° C., while being shaken slowly but incessantly. Toluol was
added because the experiments generally lasted 24 hours or even
longer. Originally I tried to determine the acidity of the fluid at the
beginning of the experiment, by titrating a measured portion of it
directly after mixing.

However, serious errors ensued, because of the impossibility to

i) Zeitschr. f. Physiol. Chem. Bd. LXV, S. 232.
23
Proceedings Royal Acad. Amsterdam. Vol. XV.

346

keep the fluid well mixed during the pipetting even after shaking
it thoroughly. Therefore mixtures of oleic acid and glycerin of the
same composition as those that were to be digested, were prepared
separately and immediately after the acidity was determined by
titration. These samples were taken in duplicate in order to discover
eventual errors in the measuring of the oleic acid.

In every experiment I used: 10 ce. of glycerin, 2 ec. of oleic
acid, 2 ec. of lipase and 3 ce. of toluol with or without addition
of salt. The following are some of the results obtained :

nr
ee. — NaHO
¢ ; a

Addition Immediately. After 24 hours. After 48 hours.

| 23.9
ee
4 0 / 23.6 g Wer 133
200 mer. CaCl, 23.1 23.4
. (23.0 b
El 0 }23.5 18 19.5
100 mer. CaCl, 23.3 23.0
Addition. Immediately. After 24 hours
: 23.5 Ld.
EEE: 0 33 6 16.9
10 mgr. CaCl, 19.3
as > 5, £ 20.4
BU aes FA 22.1
: 23.6 oe
Le 0 on 17.2
10 mer. BrCl, 18.8
i a - 22.0
100: F: 23.0

It is evident therefore that the synthesis was not increased. It was
even strongly inhibited, just the reverse result as was obtained after
addition of bile salts, prepared from oxbile affer PLarrner’s method.

n
ec. —NaHO
4

Addition. Immediately. After 10hrs. After 24hrs. After 48 hrs.

i 0 co 151 14.9
20.6
100 mer. bilesaits 10.4 9.5
i] 0) ao 19.8 16.7
(23.5 3

100 mer. bilesalts. 14.2 11.2

D47

It cannot be doubted therefore, that with regard to the activity of
the lipase calcium-, barium-, magnesium- and soda salts play a part
totally different from that of bile acids. It seems to me that from
the above the conclusion may be drawn, that the said salts separate
fatty acid from the solution as soap, and for that reason increase the
fat-splitting power of the enzyme.

Geology.—‘On rhyolite of the Pelapis Islands.’ By Prof. A. WICHMANN.

The Pelapis Islands rise between the Westcoast of Borneo and the
Karimata Islands about 1°17’S. 109°10’ EK. and consist, besides a
few small islets, of the four high uninhabited and not easily
accessible islands 1st Pelapis Tiang Balei, also called Pelapis Hangus,
or Pelapis Ajer Tiris, 2°¢ Pelapis Rambai or Pelapis Ajer Masin,
3'¢ Pelapis Genting and 4" Pelapis Tekik '). They reach a height of
399 m.”). Their total surface amounts to about 13 km’.

The group of islands was visited in 1854 by the mining-engineer
Rh. Everwiix, who communicates the following particulars about their
geological condition.

“In the Pelapis or Melapis Islands both neptunian and plutonic
formations are found. The former are clay-rocks which are so much
metamorphosed by granite and a rock analogous to syenite that it
is often difficult to recognize its original character. In these islands
plutonic rocks contain a small quantity of magnetic iron-ore and
iematite *).”7

The Mineralogical and Geological Institution at Utrecht received in
1895 among others through the kindness of the Royal Physical Society
(Kon. Natuurk. Vereeniging at Batavia) as a present a specimen of
the metamorphosed clay-rocks collected by Evrrwin ‘).”

1) J. P. J. Barra. Overzicht der afdeeling Soekadana. Verhandel. Batav. Genoot-
schap van K. en W. L. 2. Batavia 1897, p. 61.

2) M. CG. van Doorn. Verslag omtrent de opname van Straat Karimata. Meded.
betr. het Zeewezen XXII.2. ’s-Gravenhage 1882, p. 12. — Gids voor het bevaren
van Straat Karimata. Batavia 1884, p. 31.

,°) Onderzoek naar tinerts in de landschappen Soekadana, Simpang en Matan en
maar antimoniumerts op de Karimata-eilanden. Natuurk Tijdschr. Ned. Ind. IX.
Batavia 1855, p. 63. Reprinted with map in the Jaarboek van het Minwezen
N.O. Indié, Amsterdam 1879. 1, p. 64.

+) As Everwisn mentions nowhere (not even on the label) on which island he
has collected the above-mentioned rock, we give here a statement of the geological

condition of the islands according to his map:
23*

348

It appeared immediately that the above-mentioned specimen has
nothing to do with clay-slate, but is a genuine eruptive-rock showing
excellent piperno-structure. The dark brownish-red faint colour of the
chief mass seems to have given rise to Everwisy’s error. Characteristic
are the numerous lens- or disk-shaped “Schlieren” ending in a point,
which, being arranged more or less parallel, contrast sharply with
the groundmass. The specimen is distinguished from the typical
piperno by the much more intimate connection between “Schlieren”
and groundmass, and by its inferior porosity.

The analysis of the rock (1), for which I am indebted to Prof.
Dr. M. Drrrrica of Heidelberg gave the following result:

I II
SiO? -. 2 eS SSeS eee
TiO?) 2 oo SS ee Cee eee —
APO®.=.). 3 Bo eee ee
ree
Fe0 - 2 pees oS Oe See =
Ma'Q@ : .. 3@ 2222 ee ee eee —
CaO. oto. Jo Ss ee a eee
MeO: ..% 284 ¢ 93 OA ee ee ee
K2Q 2. os oes. TE eee ee ee eee
Na**O . o£ 2
COs retest Re Rae ee —

{under 110°... 0,56
| over L102. 2s
100,38 99:89

HO loss of incandese. 0,94

From this analysis it appears that among all the rocks that have
hitherto been found in the Indian Archipelago, the above-mentioned
eruptive rock is richest in potash. From the —— alas incomplete —
analysis [1 communicated at the same time’) appears further its

Pelapis Tiang Balei granite and in the N.W. part clay-rocks
Pelapis Genting ES 5° Aa iene Ay .
Pelapis Rambai x ii Wo Soe Se e
Pelapis Tekik (Pelapis Tukang Kluwar) _,, ih a) A ee Mi
Pelapis Suka se

Pulu Dua and Pulu Bulak clay-rocks.

This does not imply, of course, that all that was called by Everwisn clay-slate,
sh uld be classed with the rhyolitie rocks.

') Cart von Haver. Rhyolith aus dem Eisenbacher Thal. Verhandl. k. k. geolog.
Xeichsanst. Wien. 1868, p. 386. :

O49

close affinity with the rhyolite of Etsenpacn near Vichaye ‘) in
Hungary.

According to the method of W. Cross, J. P. Ippinas, L. V. Pirsson
and H. S. WasHineton’) the calculation of the mineralogical com-
position gave the following result:

SiO2 TiO2) Al203 |Fe203 FeO MgO K20 | Na2O
Orthoclase 38.88 — 11.02 — - — 10.17 -- 60.07
Albite O.07 ~- 0.05 — — — _ 0.03 0.25
Corundum — -- 1.65 — — — — — 1.65
Ilmenite — |0.70; — — |0.31| — — = 1.01
Hematite — — — 6.47 — — — _— 6.47
Hypersthene 1.68 — — — 0.19 0.99 — — 2.86
Quartz 21.69 a _- —_ — — -- — 27.69

68.42. | 0.70 | 12.72 | 6.47 | 0.50, 0.99 | 10.17 | 0.03 | 100.00

salic : femic :
Orthoclase 60.07 Ilemenite 1.01
Albite 0.25 Hematite 6.47
Corundum — 1.65 Hypersthene 2.86
Quariz 27.69
89.66 10.34

To the rock in the chemical system consequenily a place must
be assigned in:
Sel 89.66 7

Fem 10.34 ae. Olass 1-.Persalane.
Fem 10347 1 Class I. Persalane

QFL e

ae Se tS Ao ee = Subclass I. Persalone.

Oe ALG 5) |

r= aa ae => a Order 4. Britamare.

Ge ¥a?Q 6 8.0

eee ee poe Rang I. Liparose.
CaO 1 trace

1) Not Vichnye, as J. Rorn (Beitrige zur Petrographie der plutonischen
Gesteine. Abhdlg, k. Akad. d. W. 1869. II. Berlin 1870, p. LX XXIII) and all
those who copied him, communicate.

2) Quantitative Classification of Igneous Rocks. Chicago 1903, p. 110 et seq.

390

: qin -
ed ia a = Subrang 1. Lebachose.
Na’O 0.08 1 :
Although the analysis points to a rather high percentage of quartz
the SiO? percentage is rather low fora rhyolite, it approaches already
more that of trachytes. With regard to this fact and taking into
consideration the high percentage of Fe?O*, the specific weight is
very high for a rhyolite namely 2.623.

It cannot be said that there is a similarity of any significance
between the real mineralogical composition and the one calculated
from the analysis. For this too few individuals have separated from
the magma. So we discover under the microscope only a very slight
quantity of more or less rectangular sanidine-plates, besides very few
lath-shaped plagioclases, and likewise very rarely some augite-crystals.
The groundmass is amorphous, chiefly microfelsitic. On the spots where
it has become erystalline no distinguishable constituents occur. Occa-
sionally spherulitic formations are detected. It is however very rich
in ore-particles, by far the greater quantity of these should be classed
with hematite, though they are only exceptionally plate-shaped. As
a rule one discerns only black and irregularly shaped particles, and
it is these that accumulate in the “Schlieren” and make them appear
black at first sight. Besides this difference which has already come
off at the differentiation of the magma the main mass of the rock
does not vary in the least from the “Sehlieren”’. E. KALKowsky when
examining the genuine piperno which in a mineralogical and che-
mical respect differs so much from the rock originating from the
Pelapis Islands, had already come to the same result.’)

“Wer koénnte an der Lavennatur des sonderbaren Piperno zweifeln?”
once exclaimed Lreop. von Bucn.?) He was mistaken, for at all events
during the last decenniums objections have been made against this
view. Besides A. Scaccut*), Luigr DELL’ERBA‘), P. Franco *), especially

') Ueber den Piperno. Zeitschr. d. Deutschen geolog. Gesellsch. XXX. Berlin
1878, p. 673.

2) Geognost. Beobachtungen auf Reisen. IL Berlin 1809, p. 209, reprinted in
Gesammelte Werke [. Berlin 1867, blz. 459.

3) This was still his opinion in 1849. Afterwards he regarded the piperno as a
metamorphosed volcanic conglomerate (A. Scaccur. La regione vulcanica fluorifera
della Gampania. Atti Acc. Se. fis.e. Mat. (2) IL. Napoli 1828, No.2 p. 103).

') Gonsiderazioni sulla genesi del Piperno. Atti Accad. Se. fis. e Mat. (2) V. Napoli
1893, N’. 3, [1891] p. 1—22, reprinted in Giornale di Mineralog‘a, Cristallografia e
Petrografia Il. Milano 1892, p. 28—54.

*) Il piperno. Boll. Soc. Naturalisti. Napoli 1901, p. 34—52 (Geol. Centralbl.
Vil. Berlin 1905—6, p. 98).

551
H. J. Jounston-Lavis, who very emphatically contended for the tufa-
character of the piperno, and who attempted to give a peculiar
strength to his argument by writing:

“All geologists who have attempted to explain these principal
“neculiar characters, have utterly failed to do so, and had [ space
“to enumerate many minor ones, the difficulty would be still greater.
“Unfortunately, most of these inclusions have been jumped at, as
“the result of that useful instrument though unfortunate misleader
“of geology, the microscope, which has caused investigators to forget
“that it is only one means to an end, and that field investigation is
“of far greater importance.” *)

On account of the aversion which Jounston-Lavis has to the
microscope it will be impossible to convince him of the difference
between a piperno and a pipernoid tufa. But we point out the fact,
that it was exactly the “field-geologists’ who, as yet, not knowing
anything of the application of “that useful instrument” to the domain
of petrography, have ascertained that piperno was an eruptive rock.
Besides Lrop. von Buch we need only mention Scipio BreisLaK *),
H. Asicu*), J. Rotx, G. Guiscarpi*). It is likewise a fact known
long since that a tufa may obtain a pipernoid structure in the way
surmised by Jonnston-Lavis, but the investigators knew, also without
the help of the microscope, how to distinguish such like rocks from
‘real piperno. °)

The rhyolite of the Pelapis Islands is a stronger evidence of the
fact that the piperno-structure is not connected with a tufa-formation
as the porosity of the main mass of the rock is as insignificant as
that of the “Schlieren” whose form has as little resemblance to that
of voleanic ejections.

1) Notes on the Pipernoid Structure of Igneous Rocks: Natural Science II]. London-
New-York 1893, p. 219.

*) Voyages physiques et lythologiques dans la Campanie. II. Paris An. IX (1801)
p. 42—47.— Institutions géologiques. II. Milan 1818, pp. 154—156.

5) Ueber die Natur und den Zusammenhang der vulkanischen Bildungen. Braunschw.
1841, p. 39.

4) Il piperno. Rendic. Accad. Sc. fis. e Mat. VI. Napoli 1867, p. 221—226.

») J. Ror, Der Vesuv und die Umgebung von Neapel. Berlin 1857, p. 512. —
G. vom RatH. Mineralogisch-geognostiscte Fragmente aus Italien, Zeitschr. d.
Deutschen geolog. Gesellsch. XVII, 1866, p. 633—654,

Mathematics. “Continuous one-one transformations of surfaces in
themselves’. (5 communication ')). By Prof. L. EK. J. Brouwrr.

In Cre.ie’s Journal, vol. 127, p. 186 Prof. P. Bont has enun-
ciated without proof the following theorem proved by me (as a
particular case of a more general theorem) in vol. 71 of the Mathe-
matische Annalen (compare there page 114):

“Werden die Punkte einer Kugeloberjliche wieder in Punkte der
Kugeloberjliche iibergefihrt und geschaieht diese Ueber fiihrung durch
stetige Bewegung, welche den Mittelpunkt nicht beriihrt, so kehrt
mindestens ein Punkt in seine friihere Lage zuriick. Unter einer stetigen
Bewegquna ist hier eine Bewegung verstanden, bei welcher die recht-
winkligen Koordinaten. stetige Funktionen der Zeit und der Anfangs-
werte sind.”

Now I shall show here in the first place that the theorem enun-
ciated and proved in the first communication on this subject *), 1. e.
that each continuous one-one transformation with invariant indicatrix
of a sphere in itself possesses at least one invariant point, may be
considered as a particular case of the quoted theorem of Bout *).
To that end I shall establish the following theorem : ;

“Any continuous one-one transformation @ with invariant indicatrie

of a sphere in itself can be transformed by a continuous modification *)-

into identity” *).

In order to prove this property we choose in the sphere two
‘opposite points ?, and /, determining a net of circles of longitude
and latitude and passing by «@ into Q, and Q,. By means of a
continuous series + of conform transformations of the sphere in
itself we can transform Q, and Q, into P, and P,. Let ¢ be an
arbitrary circle of latitude, described in such a sense that P, pos-
sesses with respect to c the order*) + 1, and c’ the image of ¢ for
at, then P, possesses also with respect to c’ the order + 1.

1) Compare these Proceedings XI, p. 788; XII, p. 286; XIII, p. 767; XIV,
p 300 (1909—1911).

2) These Proceedings XI (1909), p. 797.

5) This | indicated already shortly Mathem. Ann. 71 (1911), p. 325, footnote *).

4) Under a continuous modification of a univalent continuous transformation we
understand in the following always the construction of a continuous series of uni-
valent continuous transformations, i.e. a series of transformations depending in
such a manner on a parameter, that the position of an arbitrary point is a con-
tinuous function of its initial position and the parameter.

°») That this theorem wants a proof is shown by the fact that e.g. for a torus it
does not hold,

‘) Compare e.g. J. Tannery, ‘Introduction a la théorie des fonctions dune
voriable”, vol. Il, p. 438.

Let P be an arbitrary point coinciding neither with 7, nor with
P, and passing by ar into A, and let Q be the point corresponding
in latitude with P and in longitude with ?. Then by transforming the
different points /# continuously and uniformly along circles of longitude
into the corresponding points @ we define a continuous series 0 of
univalent continuous transformations of the sphere in itself with the
property that of none of the points & the path passes through 7, or /,.
So an arbitrary curve c’ is transformed by 9 into a curve c", with
respect to which PP, possesses likewise tiie order + 1, so that c”
covers the corresponding circle. of latitude ¢ with the degree*) + 1.

From this ensues that an arc of a circle of latitude connecting
an arbitrary point P with the corresponding point Q defines une-
quivocally -for any point P an are of circle of latitude PQ whose
variation with P is uniformly continuous, so that it is possible to
construct a continuous series g’ of univalent continuous transformations
of the sphere in itself, transforming each point ( into the corre-
sponding point P, and thereby the transformation «rg into identity.
But then tree’ is the looked out for continuous series of transfor-
mations, transforming « into identity.

We shall say that two transformations belong to the same class,
if they can be transformed continuously into each other. We then
can state the theorem proved just now in the following form :

Tueorem 1. All continuous one-one transformations with invariant
indicatrix of a sphere in itself helony to the same class.

As the continuous one-cne transformations with invariant indicatrix
form a special case of the univalent continuous transformations of
degree + 17%), the question arises whether perhaps theorem 1 is a
special case of the more general property that all the univalent
continuous transformations of the same degree of a sphere in itself
belong to the same class. We shall see that this is indeed the case;
we shall namely show that any univalent continuous representation
of degree zero of a sphere « on a sphere mw can be transformed by
continuous modification into a representation of « in a single point
of mw’, and that any univalent continuous representation of degree
nz0 of a sphere w on a sphere pg’ can be transformed by continuous
modification into a canonical representation of degree n, i.e. into a
representation for which —1 non intersecting simple closed curves
of j are each represented in a single point of w’, whilst the 1

1) Mathem. Ann. 71 (1911), p. 106.
2) Mathem. Ann. 71 (1911), p. 106 and 324.

oo4

domains determined by these curves are each submitted to a
continuous one-one representation on w’, and that either all with
degree +1 or all with degree —1. By means of an indefinitely
small modification a canonical representation can be transformed
into a simply ramified Riemann representation, 1.e. into a represen-
tation which in the sense of analysis situs is identical to a simply
ramified representation of a Riemann surface with n sheets and of
genus zero on the complex plane. That all simply ramified Riemann
representations belong to the same class, follows, according to a
remark made by KierN*), out of a known theorem of Lirora—C xsscn.

In order to transform an arbitrarily given univalent continuous
representation « of « on w into a representation in a single point, resp.
into a canonical representation, we first modify it continuously
into a simplicial approwimation®) ae’, to which we have imparted,
by means of eventual subdivisions of the corresponding simplicial
divisions of ms and w, the property that any base triangle of
w covers in wv’ either a single base triangle, or a single base side,
or a single base point; we then investigate the possibility of finding
two base triangles of u, one positively and the other negatively
represented, allowing that we pass from the one to the other by
transversing exclusively base sides of u not represented in a single
point. If this be the case, u will possess a positively represented
‘base triangle ¢, and a negatively represented one ¢, both represented
in the same fundamental triangle ¢ of w’, allowing us to pass from
the one to the other by transversing exclusively such base sides of
as are represented in the same side s, of ¢’. The base triangles
,t,-1 of mw crossed on this way leading from f, to ¢, are

Mt,
Bg
then also represented entirely im sy.

Let s, and s, be the other two sides of ¢ ; by a continuous modi-
fication of «@’ and a suitable farther subdivision of ¢,, ¢,, .--fr—-1, tis
we can generate a representation @” for which all the triangles
t,,t,,---,tn—1, 4, are represented entirely in s, and s,, and which
possesses still the same property as @’, viz. that any base triangle
either a single base triangle, or a single base side,

Sn lg

of # covers in 2’

or a single base point.

In the same manner as we transformed «’ into @”, we transform
«' if possible into «”, and we continue this process until after a

!) Compare: ‘Ueber Riemann’s Theorie der algebraischen Funktionen und threr
Integrale’. Leipzig, 1882.

4) Mathem. Ann. 71 (1911), p. 102.

finite number of steps we have reached a representation «/”) no more
allowing a suchlike modification.

We now construct on uw all those polygons formed by base sides
belonging to @?) which are represented by «”) in a single point.
These polygons divide mw into a finite number of domains /,, 4,, ..., ge.
Each domain g,, which by ¢” is not represented nowhere dense.
admits the property that there is no polygon lying entirely within it
or partly within it and partly on its boundary, which is represented
by e in a single point‘). Any two base triangles belonging to the
same domain y, can be connected within y, by a path transversing
only base sides nof represented in a single point, so that of the base
triangles of g, either no one is represented negatively or no one
positively. :

As each coherent part of the boundary of y, is represented on qu’
by a single point, «’ is covered by the image of y, with a certain
degree which we will suppose to be positive. Then there are no
negative image triangles, but there are in general singular image
triangles with two coinciding vertices.

By considering each coherent part ;,- of the boundary of y, as a
single point P.., g, is transformed into a sphere sp,, and we can
deduce a simplicial division of sp, from the simplicial division of y,
belonging to «#”, by bisecting all those base sides of g, which touch
the boundary but do not lie in the boundary, dividing by means of
these bisecting points each base triangle one side of which lies in the
boundary, into a triangle and a trapezium to be considered as a
base triangle of sp,, and dividing those of the remaining base tri-
angles of which sides have been bisected, into new base triangles
corresponding to those bisecting points. The simplicial representation
a) of g, on w’ is then at the same time a simplicial representation

of sp, on w’, whilst by suitable subdivisions of the simplicial divisions

‘

1) For, as this property holds for polygons formed by base sides, any base
triangle of g» possesses at most one base side represented in a single point.
Therefore each broken line, lying in a single base triangle and not in a single
base side, which is represented in a single point, must necessarily lie entirely in
a straight line segment connecting two points of the circumference not coinciding
with vertices. So a polygon represented in a single point must either consist ex-
clusively of base sides, or it can transverse only such base sides as are represented
in one and the same base side of xu’. In the latter case however the series of the
base triangles of . crossed in this way would have to be represented in that
selfsame base side of z', so that each of the two limiling polygons of this series
(of which at most one can be illusory) would be a polygon formed by base sides
and represented in a single point of yu’.

356

of sp, and mw’ we can effectuate that any base triangle of sp, covers
in w’ either a single base triangle, or a single base side.

By choosing one of the base sides of sp, represented by @” in
a cele point, and considering it as a single point and accordingly
the two base triangles adjacent to it as line segments, sp, passes
into an other sphere sp,’ represented likewise simplicially by a?
In the same way we deduce from sp,’ an other sphere sp," if this
be possible, and we continue this process until after a finite number
of steps we obtain a sphere sp.) no more possessing for a? any
singular image triangle.

Let us denote by B and D the two base points of sp,{™—\
identified for spf and by a and c¢ the two base triangles of
sps@-) contracted into line segments for sp”. Then the triangles
a and c have either only the side 4) in common, or moreover a
second side, which we may assume to contain the vertex B:

In the first case we represent the third vertex of a, resp. c, by
A, resp. ©, and the domain covered by @ and ¢ together, by d.
At least one of the base points B and D, say D, does noé coincide
with a point P... We then connect in sp,—' outside d the points
A and © by an are of simple curve @ situated in the vicinity of
the broken line ADC, and we represent the domain included
between § and the broken line ADC, by d’. By means of a
continuous series of continuous one-one transformations leaving the
points of @ invariant and transforming each point of AB and BC
into points coinciding with it on sp”, we can reduce the domain
J +d’ with its boundary continuously into the domain d’ with its
boundary. If we represent by «,(”) an arbitrary univalent continuous
representation of sp” on w’, then to the continuous reduction of
d+ d’ to d’ corresponds a continuous series of univalent continuous
representations of sp.("—) on spJ” transforming the representation
obtained by the identification of 4 and D, into a continuous one-one
correspondence —j,@,—1 In Which the points P,. correspond to them-
selves, thus also a continuous series of univalent continuous repre-
sentations of sp,” on uw’, leaving invariant the images of the
points P,., and transforming «,” considered as a representation of
sp—) on p’, into that representation a{=—!) of sp,” on pg
which follows from «,% by means of ném-i.

In the second case we represent the third vertex of aandc by FP,
choose on the side DI of a, the side DF’ of c, and the common
side BF’ successively three such points A, C, and G, as in passing
from spi" to sp) are brought to coincidence, connect A within a
rectilinearly with B and G, C within ¢ reetilinearly with 5 and G,

357

and apply the operation of the first case to the pairs of fundamental
triangles ABD and CBD; BCG and FCG; BAG and FAG
successively ‘).

By applying this operation successively to sp,™, sp.°—),..., sp") and
sp’, we experience that the representation a”) of sp, on uw’ can be
transformed by a continuous modification leaving the images of the
points ,- imvariant, into a representation a, of sp, on wu’, which
follows from e«) by means of a continuous one-one correspondence
between sp, and sp,. As sp,™ can be divided into elements each
of which is submitted for «&” to a one-one representation of degree
+1 on a base triangle of w’, it is clear that sp, can be divided into
elements each of which is submitted for a, to a one-one representation
of degree +1 on a base triangle of uw’. The representation «, of
sp, on w’ is therefore a Riemann representation, and eventually it
may be transformed by an indefinitely small modification leaving
the images of the points /,- invariant, into a simply ramified
Riemann representation.

By executing this process of modification for all the values of » for
which it is applicable we arrive at a representation @ being for
any of the spheres sp,,sp,,..-,spx either a simply ramified, positive
or negative Riemann representation, or a representation nowhere dense.

In each domain g, we approximate the boundary parts y,- by
simple closed curves z,- not intersecting each other. Each x,- includes
with the corresponding y,- a domain q',-, and the ~z,- situated in the
same domain g, include together a domain g’,. The domains g’,- be-
longing to the same t form together a domain g’:. By means of a
continuous series of univalent continuous representations of g, on
sp, we can transform identity into a representation which for
g., with the exclusion of its boundaries is a continuous one-one
representation on sp,, whilst z,- and g',- are represented in P,,. By
doing this for all values of » we transform a@ into a representation
a, being for each of the domains y', and yg", after contraction of its
rims into points either a simply ramified, positive or negative Riemann
representation, or a representation nowhere dense.

The domains g', and g’-, which will be represented henceforth
by §,,93, - - 9, are determined on mu by a finite number of simple
closed curves not intersecting each other.

1) If we dropped the condition of the invariancy of the images of the points
P.~ (introduced only for the sake of clearness), this second case might have been
treated of course in the same manner as the first,

308

We choose an arbitrary domain g., and suppose in the first place
that a is for the sphere 6, into which g, is transformed by contrac-
tion of its rims into points, a simply ramified Riemann representation.
We then draw on w a system of ramification sections belonging to
this representation and corresponding to a system of simple closed
“ramification curves’ on o,. By first leaving the ramification sections
on w invariant and varying eventually continuously the ramification
curves on 6, in such a manner that after that they contain no more a
point corresponding to a rim of ,, and then leaving the ramification
curves on 6, invariant and contracting the ramification sections
on # continuously into points, we can transform the representation
of 6, on w determined by « continuously into a canonical representation.
During this continuous modification the points representing the rims
of a, vary also in general. Let 7; be such a rim and q.- the residual
domain of gs, on mw determined by 7-. We then can follow the con-
tinuous variation of the image point of 7; by a continuous series of
continuous one-one transformations of «’ in itself to which corresponds
a continuous modification of the representation of g,-on pw’ determined
by a@;. By applying this modification to the representations of all the
residual domains of 9, we generate a representation a@; of uw on -w!
into which «, can be transformed continuously, and which is a
canonical representation for 6,.

In the second place we suppose «@, to be for 6, a representation
nowhere dense. Then we can modify the representation of 6 on w'
determined by «, into a representation in a single point. The varia-
tion of the image points of the rims of 4, implied by this modifica-
tion, can be followed once more in the way described above by a
continuous modification of the representation of the residual domains
of c,, furnishing us with a representation @,; of uw on w into which
« can be transformed continuousiy, and which represents 6 in a
single point.

By executing this operation for all values of » successively, we

vet a representation a” of won w, into which « can be trans-

i
formed continuously, and which represents each of the domains
§,, S,,-..% either after contraction of the rims into points eanoni-
cally, or in a single point. The sphere « is now divided by a finite
number of non intersecting simple closed curves into a finite number
()

of domains d,, d,, .. . ., d, in such a way that for a each of these

domains is submitted either after contraction of the rims into points
{0 a continuous One-one representation, or to a representation in a
single point. Thus the degree of these representations is U, + 1, or

BOY

—1, according to which we distinguish domains of the first, the
second, and the third kind.

If for the representation «@*’, which may be denoted henceforth

by ay, all domains d, are of the first kind, we have attained our
aim ; for then we have transformed « continuously into a represen-
tation of gw in a single point of uw’. So we further confine ourselves
to the case that among the d, there are domains of the second or of
the third kind, and we will suppose that there occur moreover
domains of the first kind. Then there is certainly a domain d, of
the first kind adjacent to a domain ds of the second or third
kind. The domain formed by d, and ¢/: together, may be indicated by
d,z, the sphere deduced from d,z by contraction of its rims into
points, by djs. We then can modify the univalent continuous repre-
sentation of d,: on mw’ determined by e, continuously into a conti-
nuous one-one representation of d,s on w’. The variation of the
image points of those rims of d,:; which originate from d,, necessarily
implied by this modification, can once more be followed in the man-
ner described above by a continuous modification of the representa-
tion determined by ef of those residual domains of d,s which origi-
nate from d,, furnishing us with a representation a’ distinguishing
itself thereby from ay that a domain of the first kind and a domain
of the second (resp. third) kind have been united into a single
domain of the second (resp. third) kind.

By repeating this operation as many times as possible we arrive
after a finite number of steps at a representation a, distinguishing
itself thereby from ay that all the domains of the first kind have
been absorbed by domains of the second and of the third kind.

If there are for the representation « ©),

henceforth by a, domains of the second as well as of the third kind,
we consider a domain d. of the second kind separated by a simple
closed curve 7,, from a domain d. of the third kind, and we repre-
sent the domain formed by d; and d. together, by d.., and the
sphere deduced from d,, by contraction of its rims into points, by
J... Moreover we represent by P, the image point of 7. for @,, by
P, the opposite point of P, on uw’, and we modify the representa-
tion of d,, determined by «, into a representation of d-. in the
single point P,, by diminishing the polar distances measured from 7,
continuously and proportionally to each other to zero. The variation
of the image points of the rims of ¢@:, necessarily implied by this

which may be denoted

360

modification, can be followed in the manner described above by a
continuous modification of the representation of the residual domains
of d.. determined by @,, furnishing us with a representation a,’ dis-
tineuishing itself thereby from a, that a domain of the second and
one of the third kind have been united into a single domain of the
first. kind: this domain however, if it does not occupy the whole
sphere gu, ean be absorbed in the manner described above by an
adjacent domain of the second or of the third kind, by which process
a, passes continuously into a representation a’, distinguishing itself
, that a domain of the second and one of the third
kind have been absorbed together by a domain of the second resp.
of the third kind.

By repeating this operation as many times as possible we arrive
after a finite number of steps at a representation «>) for which the

thereby from ¢

domains d, are either all of the second or all of the third kind. So
this representation is a canonical one, and we have proved :
Turorem 2. All univalent continuous transformations of the same
degree of a sphere in itself belong to the same class.
A proof of the inverse theorem has been given Mathem. Ann. 71,
p. 105.

In carrying out the ideas sketched in the second communication
on this subject’) I experienced that in some points of the course of
demonstration indicated there, still a tacit part is played by the
Schoenfliesian theory of domain boundaries criticized by me),
so that the theorems 1 and 2 formulated p. 295 and likewise the
“oeneral translation theorem’? founded upon them and enunciated
without proof Mathem. Ann. 69, p.178 and 179, cannot be considered
as proved*), and a question of the highest importance is still to be
decided here.

The “plane translation theorem” stated at the end of the second
communication (p. 297) and likewise Mathem. Ann. 69, p. 179 and
180, has meanwhile been proved rigorously by an other method.*)

1) These Proceedings XII (1909), p. 286—297,

2) Compare Mathem. Ann, 68 (1910), p. 422—434.

3) Already the property of p 288 that the transformation domain constructed
in the way indicated there determines at most two residual domains, vanishes for
some domains incompatible with the Schoenfliesian theory.

') Compare Mathem. Ann. 72 (1912), p. 37—54.

361

Chemistry. — “Kvtension of the theory of allotropy. Monotropy

and enantiotropy for liquids.’ By Prof. A. Smits. (Commu-

eated by Prof. A. F. Honieman).

The extension meant above concerns the case that the pseudo-
binary system exhibits the phenomenon of unmixing in the liquid state.

Fig. 1 X.

Let the §,z-line be schematically represented
by fig. 1 at the temperature and pressure at
which the phenomenon of unmixing takes
place. Then in the first place it is noteworthy
that 7, and /, are the coexisting liquid phases
of the psendo-binary system, and that more-
over there exist two minimum points L,
and L, representing the liquid phases which
may be formed when the system gets in
internal equilibrium, and consequently be-
haves as a unary substance.

The two liquid phases are not miscible,
and when they are brought into contact
the metastable liquid ZL, will pass into the

stable liquid phase Z,, so that this operation means the same thing
as seeding the metastable liquid. As fig. 1 shows the metastable
unary liquid point ZL, lies inside, and the stable unary liquid point
L, outside the region of incomplete mis-
cibility, and now it is of importance to

examine what

happens when we move

toward such a temperature that the critical
phenomenon of mixing occurs in the pseudo-

binary system. The coexisting phases /, and
/, have drawn nearer and nearer to each other,

and finally coincided in the critical mixing-
point, and the §,z-line has then changed into a
curve with only one minimuin, as fig. 2 shows. E
It is now, however, of importance for
our purpose to consider the way in which
the §,z-line has changed its form from that Wie, 2 ¥.
of fig. 1 to that of fig. 2.
It is known that before the points /, and /, coincide, the maximum

Proceedings Royal Acad. Amsterdam. Vol. XY.

362

M = vanishes in consequence of the coin-
cidence of this point with the minimum
L,, at which moment a point of inflection
appears with horizontal tangent. At this
moment the. possibility of the existence
of a metastable unary liquid ceases, so
that this condition has already become
impossible before the critical mixing point
has been reached in the pseudo-system.
This consideration is in itself already
sufficient to indicate in a 7Vxz-diagram the
situation of the liquid lines in the unary
system with respect to those in the pseudo-
binary one. If we assume that the pseudo-
system, just as the system nzcotine-water,
presents an upper and a lower critical
Fig. 3 2. mixing point, fig. 3. is formed.

The closed line PP, indicates the coexisting liquid phases in the
pseudo-binary system. Outside the region enclosed within this conti-
nuous curve, runs the line £4,, on which the stable internal liquid
equilibria are found, and inside this region lie the metastable internal
liquid equilibria on the line 2’, &, 4+). In the points #', and /’ this line
passes continuously into the locus of the maximum points J/ of

the ¢.r-lines, and as in these points @re just as for the stable
&/ P,T

2
and metastable unary equilibria, but (53).<0. we may call the
3 )
locus of the maximum points M the line of the unstable internal
equilibria.

The theory of allotropy attributes the phenomena of monotropy
and enantiotropy to the occurrence of different kinds of molecules
of one substance, and says that when there exist two or more solid
states of a substanee, the differences in properties are owing to the
situation of the internal equilibrium which will be different in the
two solid states.

Now we saw just now that when a substance occurs in two
different liquid states, this phenomenon must also be ascribed by the
theory to the existence of two different internal equilibria between
different kinds of molecules of the same substance. So according to

1) The lines of the internal equilibria have here a very peculiar shape, which is
dependent on the phenomenon of unmixing. | shall return to this subject later on.

363

this new view there is no essential difference between the occur-
rence of different solid and different liquid phases of one substance
and as in the case considered here we have two liquid phases, one
of which is afvays stable with respect to the other, we are justi-
fied in speaking here of the phenomenon of monotropy for a liquid.

Now it is of importance to examine what will take place when
the region of incomplete miscibility comes into contact with one of
the melting-point lines of the pseudo-binary system.

Beforehand I will, however, remark that Dr. Scnorvers '), who
undertook the same problem at Baknuis RoozEBoom’s instigation, but
took no notice of the $-z-lines, could only draw by chance a line
for the stable unary liquid equilibrium, as shown in fig. 4.

Fig. 4X. Fig 5 X.

If we suppose that the region of incomplete miscibility comes in
contact with the melting-point line of the component with the higher
melting-point, we get the 7, x-figure 5.

Now it is of importance to determine the continuity between the
iwo pieces ed and cb of the interrupted melting-point line of the
pseudo-component #4, and also the continuity which is connected with
it, between the mixed crystal lines ef and mf. Now it is the
question where the liquid lines of the unary system will meet those
1) Thesis for the doctorate. ;

24*

364

of the pseudo-binary system. In the first place we see that the
stable unary liquid line meets the melting-point line of the pseudo-
system in JZ, so that there a total solidification will take place, at
least if phenomena of retardation fail to appear.

The solid states, which are in internal equilibrium below this
temperature, and so belong likewise to the unary system, lie on
the line SS,. It is further noteworthy that one of the two meta-
stable parts of the melting-point line of the pseudo-component B,
intersects the metastable liquid line of the unary system in L’.

At the temperature of this point of intersection an intersection
must also take place of the metastable produced parts of the mixed
crystal line mf and of the line for the solid internal equilibrium S,5S,
which intersection is denoted by the point S’.

It follows from this that when the metastable unary liquid is
cooled down, and no retardation takes place, at Z’ total solidifica-
tion to the metastable unary solid phase S’ will set in, which,
however, becomes stable at SS. So what is remarkable about this,
is that the metastable point of sodification lies higher than the stable
one, and this is due to this that here there is no monotropy in the
solid state but monotropy in the liquid state, in consequence of
which-we get the reverse of what we are accustomed to, as is
immediately clear, when we draw the P, 7-fig. Our 7’, X-fig. 5,
however, reveals more. We see namely from it that when the
metastable part of the region of incomplete miscibility extends far
enough below the eutectic point of the pseudo-system, the metastable
unary liquid line can also be cut by the metastable prolongation
of the melting-point line of the pseudo-component A, so that the
possibility also exists that in Z” total solidification of the metastable
unary liquid to the metastable unary solid substance S” sets in,
which solid phase will then follow the line S"S," at lower tempe-
ratures. So one of the peculiarities of this case consists in this that
the metastable unary liquid possesses #wo metastable points of solidi-
fication, and that when this liquid is not converted to a stable one,
it ean solidify to a solid substance which is at first metastable and
at lower temperatures stable when it is first heated above a definite
temperature, and then cooled down. If the temperature is not raised
so high, the -metastable unary liquid solidifies to another solid
substance, which remains metastable, at least when no transition
equilibrium occurs in the solid state.

Now it should, however, be pointed out that the two mentioned
points of solidification of the metastable unary liquid need not neces-
sarily exist. The upper point of solidification may be absent, in con-

365

sequence of the partially metastable, partially unstable middle portion
of the melting-point line of the pseudo-component #4 no longer
intersecting the metastable unary liquid line, but running round this
eurve. And the lower point of solidification may be absent, when the
same curve lies entirely above the metastable prolongation of the
melting-point line of the pseudo-component A.

When the question is considered in what way in case of liquid
monotropy, the metastable phase can be obtained from the stable
one, one arrives at the conclusion that this will have to take place
by rapid condensation of the vapour, which in concentration is nearer
the metastable than the stable liquid.

Whether substances have already been found which belong to the
above-described type, is still open to doubt, though in the Hterature
statements are found, which might lead us to suppose so.

As is known, it was believed for a long time that the pseudo-
system of sulphur had to possess a region of unmixing, because it
was thought that some phenomena observed in the investigation
furnished indubitable indications in this direction. This view was
first pronounced by Baxkuuis Roozesoom, and supported by Krvyr,
on the ground of his own observations’). After SmirH c.s.*) had
made it probable that the quasi-unmixing was to be ascribed to a
difference of temperature, | succeeded last year in conjunction with
Dr. ve Lrzuw®*) in ascertaining with perfect certainty that the phenome-
non in question has nothing to do with a phenomenon of unmixing,
and is really brought about by a difference of temperature, which
gives rise to a quasi-unmixing when tubes with more than a certain
inner diameter are used.

Moreover it appeared that the point of solidification of states of
sulphur fixed at higher temperatures could not give support to the
old view, so that. not a single reliable experimental datum is now
known that speaks in favour of the existence of a region of incom-
plete miscibility in the pseudo-system.

That the shape of the line for the stable unary liquid equilibrium
resembles that of the line £Z in Fig. 5, is of course, of not the
slightest importance, for also when the pseudo system possesses no
region of incomplete miscibility in the liquid state, the said line can
have such a shape. Besides, the system sulphur, as I already stated,
is at least pseudo-ternary, which view is in harmony with the

1) Z. f. phys. Chem. 64, 513 (1908).
ne » 57, 685 (1907).
3) These Proc. Oct. 1911, p. 461.

366

results of the investigations of Rotensanz') and Arrn?). In a more
complicated case, in which a line of equilibrium is the resultant of
three or more lines of equilibrium a line of equilibrium with a
clearly marked point of inflection will of course exceedingly easily
arise, as is, indeed, the case for the aldehydes *).

Fig. 6.

2. Let us suppose in the second place that above the temperature
of the three-phase equilibrium Sg+ L, + Z, the S-z-line of fig. 1

1) Z. phys. f. Chem. 62, 609 (1908).

*) See Versl. Kon. Ak, 28 Sept. 1912, p. 396. This paper will shortly appear

in These Proceedings

8) Z. f. phys. Chem. 77, 269 (1911).

367

changes in such a way that the minimum point Z, gets higher than
L£,, so that a change of stability takes place. Under these circum-
stances we get what I discussed before for the solid phase. At the
moment that the minimum points lie at the same height, the unary
liquid phase will suddenly he changed into one of different concen-
tration, if no retardation takes place.

So in this case we have enantiotropy for a liquid or a liquid
with a point of transition,

The (T,x)p-fig. of the pseudo-binary and unary system can then
have the form as indicated in fig. 6, when the equilibria with solid
substance are omitted.

- We see from this that the two stable unary liquid lines £2, and
Lk, ave continuously connected with each other by a-partially
metastable, partially unstable middle portion, and that in accordance
with the theory of allotropy the equilibrium between the two phases

Fig. 8.

£, and L, is perfectly comparable with the equilibrium between
two solid phases at the temperature of transition.
If we now examine what may happen when the region of incom-

368

plete miscibility in the pseudo system comes in contact with one of
the melting-point lines, we may distinguish different cases. In his
Thesis for the Doctorate Scnorvers gives the following figure 7,
adding that when on loss of heat the phase z has been entirely
converted to y, the ordinary phenomena will occur at lower tempe-
ratures.

By ordinary phenomena Scnorvers understands the deposition of
one of the two components in pure state. The theory of allotropy,
however, says that from the liquid which is in internal equilibrium,
a solid substance will deposit, which is also in internal equilibrium,
so that this solid phase will contain the two pseudo-components. If
we express this in a drawing, we may get among others fig. 8,
which is at once clear without any further elucidation. It is, however,
necessary to point out that it is also possible that the line for the
internal liquid equilibrium L,LL’L" does not intersect the stable
part of the melting-point line of the pseudo-component B, but that
of the pseudo-component A. Besides it is possible that coming from
higher temperatures the line for the internal liquid equilibrium does
not meet the region of incomplete miscibility for the first time on

069

the righthand side, but on the lefthand side, in which case fig. 9
gives one of the possible situations. The region of incomplete misci-
bility lies too high here to give the second lower metastable unary
point of solidification.

All these 7',x-figures can be accurately determined by means of
the ¢-z-lines, which has been omitted here for want of space.

It may finally be remarked that the phenomenon of enantiotropy
for liquids has never been observed as yet, but the possibility of
this phenomenon is beyond all doubt.

Anorg. chem. laboratory of the University.
Amsterdam, Sept. 20, 1912. |

Chemistry. — “The application of the theory of allotropy to the
system sulphur’. UU. By Prof. A. Smrrs. (Communicated by
Prof. A. F. Honuemay).

In a preceding communication ') [ already pointed out that the
theory of allotropy requires that the system sulphur must be consi-
dered to be at least pseudo-ternary.

On that occasion a 7,x-figure was projected by me, which as I
stated already then, had still to undergo a simplification by the
omission of the region of incomplete miscibility 7). But the figure
had to be modified also in another respect, for in the meantime
SmitH and Carson *) had determined the melting-point line of a third
crystallised moditication of the sulphur, the so-called soufre nacre
(mother-of-pearl sulphur), which had been discovered by GrErNez *).

To keep the representation as simple as possible for the present,
the modification required to insert this third crystallised condition of
sulphur into our figure, has been accomplished by assuming in the
pseudo binary system Sp— Sy and Siy—S,°) above the eutectic point
a discontinuity in the monoclinic mixed crystals. In consequence of this
the line for the internal liquid equilibrium in the plane for the pseudo-
binary system Sr— Sj meets the stable melting-point line of one kind
of monoclinic mixed crystals in /,, and the metastable branch of the
melting-point line of the other kind of monoclinic mixed crystals in
1, the same line of equilibrium cutting the metastable part of the

1) These Proc. XIV 263.

er s:, XIV 461.

3) Zeitschr. f. phys. Chem. 77, 661 (1912).

4) Journ. de phys. 3, 76 (1884).

5) By Sr, Sa, Sz the pseudocomponents are meant here.

370

melting-point line of the rhombic mixed crystals in Z,. lf we have
once premised this in the plane for Sre+ Su, we find the ternary }
T,#-figure in the same way as was explained in my first communi-
cation on this subject, if viz. the fact is allowed for that the transi-

|
|
|

=~ ; \ -

SSS
> —
=—>

q
tion point is lowered by the third component, which follows from the
experiments carried out by Dr. DE Leeuw at my request ’*). .

1) See Versl. Kon. Ak. 28 Sept. 1912, p. 488. This paper will shortly appear :
in These Proceedings. 3 ;

371

In this 7,7r-figure L and S denote the coexisting phases at the
unary point of solidification of the monoclinic sulphur, and in the
same way the points L’’ and 8’ indicate the coexisting phases at
the unary point of solidification of the monoelinie sowfre nacré, L’
and S’ referring to the unary point of solidification of rhombic sul-
phur, and 8, and §
point of transition.

In conclusion I will emphatically point out that it is very well
possible that in many respects the real 7,7-figure of the system sul-
phur deviates from the diagram given here. The system sulphur may
be pseudo-quaternary, or even still more complicated. Moreover it is
very well possible, indeed it is even probable, that in the pseudo-
binary systems no eutectic points occur etc., but, however strange
this may seem, this is just now of minor importance.

At present the only end in view can be this to find a means to
express the fundamental thought, that we meet here with a system
that is composed of more than two kinds of molecules, and of which
not only the unary vapour- and liquid phases, but also the unary
solid phases are states in which these different kinds of molecules
are in equilibrium. Starting from this idea the figure given here was
drawn up, which will probably appear to be able for the present to
account satisfactorily for the observed phenomena.

, to the coexisting solid phases at the unary

Amsterdam, Sept. 25 1912. Anorg. chem. lab. of the University

Chemistry. — “The inverse occurrence of solid phases in the system
_tron-carbon.” By Prof. A. Smits. (Communicated by Prof.
A. F. HOLLEMAN.)

Through an investigation made by Rurr’) concerning the comple-
tion of the T,x-figure of the system iron-carbon I came to the con-
clusion some time ago that stable carbides probably occur in this
system’). Shortly after there appeared an abstract of a preliminary
investigation by Wirtorr®*), written in Russian, which seemed to
confirm this surmise. When what seems very probable to me, the
results of Wirrorr are correct, we meet in the system iron-carbon
with a pecularity, as I demonstrated before, which has been met
with up to now only in the system ceriumsulphate-water. This
peculiarity consists in the inverse occurrence of solid phases. One of

1) Metallurgie 458, 497 (1911).
2) Z..f. Elektr. Chem. 18, 362 (1912).
3) Russ. phys. chem. Ges. 43, 1613 (1911). Compt. rend 1912, 1091.

372

the phases which shows this phenomenon in the system iron-carbon,
is graphite. Graphite is the second component, and when there was
no deviation from the ordinary state of things the succession of the
solid® phases, which coexist with the saturated solid and liquid solu-
tions, would be such that the carbon content continually increased
in one direction. Starting at the ordinary temperature we find, how-
ever, this that first graphite, and then carbides are formed, which
latter however will finally have to give way before the graphite
again.

Now it wouid follow from the preliminary investigations of WiTTorE,
when namely the equilibria examined by him are stable, that twice
such an inverse deposition takes place in the system 7ron-carbon,
for with rise of temperature he found this succession :

C—-Fe,U—FeC—Fe, C—Fe,C ?
from which it appears that a solid phase with a hiyher percentage
of iron succeeds not only C, but also Fe C.

This phenomenon of inverse occurrence of solid phases is still so
strange to us that it is expedient theoretically to enter a little more
deeply into this matter.

To throw the peculiar element into strong relief, I shall discuss
the phenomenon led by the same example as I used as an illustra-
tion in the Zeitschr. f. Elektrochemie. So I shall suppose for a
moment that the succession of the solid phases which coexist with
saturated liquid solutions with rise of temperature, is this:

C — FeC — FeC, — C.

If we now suppose that the situation of the lines for the three-
phase equilibrium with one of these solid phase, so forS + L-+G,
is as has been represented in fig. 1, the easiest way to find the
situation of the other three-phase lines is to prolong the two three-

Fig. 1.
phase lines bc and de metastable through the point of intersection
c, till we meet the metastable middle portion of the three-phase
line for C++ L + G in g resp. f.

373

Let us at first only consider the two three-phase lines for C+-L+G
and FeC + L + G, which are once more drawn separately in fig. 2.
Then it is noteworthy that 4 and g are two quadrupie points, where
vapour, liquid, graphite aud the carbide FeC coexist. There is,

Fig. 2.

however, a difference between these two quadruple points, and the
most essential difference is this that whereas in the first quadruple
point 6 with supply of heat graphite with the vapour and the liquid
phase is converted to FeC, in the second quadruple point the very
reverse takes place.

If the case supposed here actually existed, we might account for
it in the following way. The simplest supposition we can make is
that along the three-phase line for C + L+G the concentration of
FeC in the vapour and in the liquid phase continually increases
from a to 4, because the carbon concentration increases, and because
besides we probably have here the endothermic process:

C + Fez FeC

In consequence of the shifting of the above mentioned equilibrium
to the right, the liquid and the vapour phases in the quadruple
point 6 have just become saturate with FeC, and they are still just
saturate with graphite. With an infinitely small rise of the tempe-
rature the two phases, which are still supposed to be in contact
with graphite, become swpersaturate with regard to FeC, and wn-
saturate with regard to graphite, from which follows that on supply
of heat graphite will dissolve and FeC deposit in the quadruple
point 4, till all the graphite is gone.

So the symbol for the conversion, which takes place in the qua-
druple point 6 on supply of heat is as follows:

C + Fe— FeC in the homogeneous gas-

- | and liquid phases. D fe eee CEN
C FeC
solid solid

a eal.

O74

It is clear that if the reverse happens in the quadruple point g,
the condition must have become different in so far that the homo-
geneous gaseous resp. liquid phases, which were before saturate with
regard to FeC and unsaturate with regard to C, must be saturate
again in g with respect to both the solid phases, and infinitely little
above the temperature of the quadruple point g the gaseous and
liquid phases in contact with solid FeC must become unsaturate with
respect to FeO, and supersaturate with respect to graphite, so that
solid FeC is dissolved, and graphite is deposited, till all the carbide
is gone.

So in the quadruple point g we get for the transformation on
supply of heat the symbol

C+ Fe<—FeC in the homogeneous gas-

| {and liquid phases. oe
C FeC
solid solid

So the transformation given here must be endothermic in the
direction of the arrows. We have to call attention to the fact that
we assumed for shortness’sake that the formation of FeC in the
coexisting gas and liquid phases is endothermic along the three phase
line for C+L+G' from a to 6. Now, however, we know only
with certainty that the total transformation (1) is attended with
absorption of heat.

When in the process of condensation resp. solidification of FeC
from the coexisting phases more heat was developed than was absorbed
in the process of evaporation resp. melting of graphite *), the process
in the homogeneous phases would undoubtedly be endothermic, but
in the opposite case the total transformation (1) could be endothermic,
whereas the reaction in the homogeneous gas and liquid phases was
exothermic. But in this ease we should have to inquire how it is
possible that the gas and liquid phases, which were unsaturate with
respect to FeC on the three-phase lines between the points a and 6,
have become saturate with respect to this compound at 6. This is
easy to see. We must namely consider two influences here whicb
can displace the equilibrium : in the first place the temperature, and
in the second place the concentration of the reacting components.
On rise of temperature in the absence of graphite the equilibrium
in the homogeneous gas and liquid phases would shift to the left,
but in the presence of graphite just the reverse would take place,
when namely the increase of solubility of graphite predominates over

') The heat of mixing included.

.the influence of the temperature on the homogeneous equilibrium on
rise of temperature.

Thus we may not conclude from the circumstance that the trans-
formation (2), which refers to the second quadruple point g is endo-
thermic, that the conversion in the homogeneous phase proceeds
endothermically in the direction of the arrow.

If we make the same supposition as we did just now, viz. this
that in the process of evaporation resp. melting of FeC more heat
is absorbed than is developed by the process of condensation resp.
solidification of graphite, the total heat of transformation (2) might
be endothermic, also when the homogeneous process in the direction
of the arrow was exothermic.

In the opposite case, however, the reaction in the homogeneous
phases in the direction of the arrow would certainly be endothermic.

Thus we come to the conclusion that the case of inverse depo-
sition of solid phases supposed here is possible, when the conversion :

C+ Fes FeC

taking place in the homogeneous phases between the points g and é
has become less greatly endothermic ov exothermic.

As is known, a change in the heat-effect with the temperature is
a phenomenon of general occurrence, which owes its origin to the
circumstance that the specific heat is a function of the temperature.
Repeatedly great changes of the heat of reaction with the temperature
have been observed, so much so that a reversal of the sign of the
heat took place, from which accordingly follows, that the possibility
of the here supposed case was to be expected on the ground of our
present knowledge.

Now we shall proceed to the discussion of the other three-phase
lines, which likewise start from the two quadruple points 6 and g.
In the first place a three-phase line for C + Fe C + G still starts
from the point 6. To determine the direction of this curve we may
make use again of VAN per Waats’ theory of binary mixtures.

If we denote graphite by 5S, and carbide by 5,, the following
relation follows from the theory mentioned for the three-phase line

for C+ FeC+G:

— Hs, aa lg -:
: Wee 2 Cw
Ip Ls, —Ly
Ba, = ~- hte a eS
S,S2G V7 aes Ls, ee V.
Sig $26
Use —&q

In the quadruple point 6 numerator and denominator indicate the

376

heat-effect and the change of volume, which attends the transfor-
mation (1). If we first consider the denominator, we see that V,,,
and V.,, are both negative and differ little. And as further 2,—
—iy > ws, —&, We see immediately that the denominator will be
positive.

About the numerator we know that it is negative in b, so that

: d
it follows from the sign of numerator and denominator, that 7 7

is negative, and that the three-phase pressure will descend with
rise of temperature, at least in the neighbourhood of 6.

With a view to the further discussion it is desirable to examine
the numerator somewhat more closely. W,,, and Ws,, are the quan-
tities of heat which are developed when a gr. mol. of S, resp. S,
evaporates in an infinitely large quantity of the coexisting vapour
phase. We can divide both quantities into two others, viz. into a
molecular heat of evaporation and a molecular differential heat of
mixing e.g.

Weg =(Ws9), + Wo,

The heat of evaporation (IV’s,,) is negative. If now we further

s
assume that the formation of FeC is endothermic at 6, so
C+ Fe =FC —a Cal,
which is more probable, the heat of mixing Was will also be nega-
tive, so that Ws, is also negative then.
For Wg, we may write:

Weg = (Wayy)z + Waa

The molecular heat of evaporation (IVs,,)_ is again negative. The
differential heat of mixing Wo. will consist almost exclusively in
the heat effect of the conversion:

FeC—Fe+C+aCal
which as has been indicated here, is positive at 6, so that Wag
can be also positive, and Ws,, negative or even positive. So we see
from this how it is possible here that notwithstanding the fraction
US, — &q : r Pe . ° :
eg 1 the quantity Ws,, predominates in equation (I), so that
the numerator is negative.

It is now clear that when on rise of temperature the heat of
formation of FeC becomes smaller negative in the gas phase, and
finally passing through zero, assumes a positive value, the negative

value of W.,, will continually decrease, and that of WW. will in-
crease. From this it follows that the numerator which is at first
negative, will likewise pass through zero and become positive. This
happens before the second quadruple point g has been reached, for
in that point the numerator must be positive already. So we arrive

' dp E ‘
at the conclusion that 7 = for the three-phase line S, + S,+ G4

starting from 4% is negative, then passes through zero, and has a
positive value in g, so that the said three-phase line, which joins
the two quadruple points 4 and yg, possesses a minimum pressure,
as is indicated in fig. 3.

The considerations given here may be directly applied to the
fourth three-phase line of the mentioned two quadruple points, viz.
to that for S,+ S,+ LZ. The equation, which we want in this case,
is quite analogous with equation (1), and we need only substitute
the letter / for g to obtain the true relation, so:

Hig — ae
W.1—— “Wut -
dp eee
Ti = = Sea ee ae eee
dT] 5.5L ¥ Ls, —2|
Vi — <o-tae Pe,
vs, —L] ¥

The discussion of the numerator is perfectly identical with that
just given, but now the denominator requires further consideration.

We were convinced that Vg, and J's, are negative, but about
the quantities Vs; and J’s,; we must make the following remarks.
The known increase of volume, -which takes place in iron-carbon
mixtures on solidification leads us to expect that this property is to
be attributed to the presence of the component carbon, which behaves
probably in the same way as the substance water. In consequence
of this not only carbon, but also carbon-compounds will exhibit in-
crease of volume on solidification, specially when the compound

25
Proceedings Royal Acad. Amsterdam. Vol. XV.

378

contains comparatively much carbon, whereas compounds with a
smaller percentage of carbon will probably behave like iron.

If we now assume that Vs; and Vs, are both positive, then it

is possible that the denominator of equation (II) is negative, and the

: . dp\ . a:

numerator also having a negative value at 4, 1( =) will begin in

dT’ )s,5,L
this case in & with a positive value. In the second quadruple point
g the numerator is positive, as I showed before, and consequently

dp f
r( : ) will be negative.

dT S\ Sob
Reasoning in the same strain as before in the discussion of the

three-phase line for S, +58, -++G it foliows that the three-phase line
for S,-+S,-+L will possess a pressure maximum, as has been
schematically represented in fig. 4.

When on the other hand Vg, is positive and Vg, negative, the
< d
denominator has a positive value, and 7 (#) will consequently be
S,SoL
negative at 6 and positive at g, in consequence of which the P,T-
figure becomes as it has been drawn in fig. 5.

A metastable minimum cannot occur here, because the three-phase
lines for C+ FeC+G and for C-+ FeC +L pass continuously

into each other by means of two cusps in the way indicated in
fig. 5’). Finally it may still be pointed out that it is possible that in
the last case the denominator passes through zero, which would
bring about a combination of the figures 4 and 5.

If we now apply the results obtained here to our original case
indicated in fig. 1, we arrive easily at the correct result, when we
omit in our thoughts first the three-phase line for FeC, + L-+ G,
and then that for FeC-+L+G. We then get two intersecting
figures, in which we can easily distinguish the stable equilibria from
the metastable ones.

Fig. 6 gives the P,7-projection for the case that we have twice
the same type as fig. 4. |

yo 6

Fig. 6.

The three-phase lines for C+ FeC+G and C+ FeC,+G
intersect in A, where a new quadruple point is formed, from which
two more three-phase lines start, viz. hk for C + FeC + FeC, and
he for FeC + FeC,+G. The point & is the point of intersection
for the three-phase line /in'y for C+ FeC + L, and of the three-

') Comp. the paper of Dr. ScHEFFER, These Proc. p. 389.

25*

380

phase line jfm,'d for C+ FeC, +L, and so this latter three-phase
line, which starts from the metastable quadruple point 7, becomes
stable at #, and then after having reached a maximum, it runs to
the quadruple point d. So the point & is also a quadruple point,
where besides the two mentioned three-phase lines, two others meet
viz. the three-phase line for FeC+-FeC,-+-L and that for C+-FeC+FeC,.
It is clear that the situation could also have been such that the
three-phase line for C + FeC + L possessed a stable maximum, but
this does not give rise to essential modifications. If we examine a
combination of twice the type of fig. 5, the case is less remarkable.

Anorganic Chemical Laboratory

Amsterdam, September 8, 1912. of the University.

Physics. — “On the system ether-water.” By Dr. F. E. C. ScHurrer.

(Communicated by Prof. J. D. vAN DER WaAats).

1. In his Thesis for the doctorate (1912) Dr. Rreprrs described a
number of experiments which were undertaken with a view to the
experimental realisation of the phenomenon of double retrograde
condensation, which had been predicted by Prof. vAN Der WAALS.
Both the systems which were used for this investigation, carbonic acid
and urethane, resp. carbonic acid and nitrobenzene exhibited three-
phase pressures, which at the same temperature, were lower than
the vapour pressures of the carbonic acid. In neither of the systems
the direct observation of the said phenomenon has been possible. In
my opinion Dr. Reepers justly ascribes the failure of this observation
to the fact that the difference in volatility of the components of both
systems is so great that the vapour phase under three-phase pressure
practically consists of pure carbonic acid, and consequently the
quantity of the liquid layer, poor in carbonic acid, which is formed
during the retrograde condensation, is so small that it escapes obser-
vation. The critical points of the upper layer lie for both systems
at concentrations which are smaller than 2 mol. percentages of the
least volatile substance, and hence the concentration which is to
present the double retrograde condensation contains still less of the
second component.

When Dr. Rrepers told me his results a long time before the
publication of his Thesis for the Doctorate, it did not seem impossible
to me that a system, in which the volatility of the components

381

differs less, might offer a greater chance to the realisation of the
said phenomenon. Such systems, however, are pretty rare. For
“normal” substances such a behaviour will probably seldom occur.
The system ether-water, on the other hand, which as appears from
KvUENEN’s observations, possesses three-phase equilibria which extend
to the critical neighbourhood of the ether, satisfies the requirement
that the vapour under three-phase pressure contains an appreciable
quantity of the least volatile component, in casu the water, the
vapour tension of the water amounting to about 14 atms. at the
critical temperature of ether (critical pressure 36 atms.). That this
system differs from those used by Rerprrs in this that the three-
phase pressure lies higher than the pressure of saturation of the two
components at the same temperature need not interfere with the
appearance of the phenomenon. Therefore I carried out some expe-
riments about a year ago with a view of examining whether double
retrograde condensation can be observed in the system ether-water.
However, this system too appeared unsuitable for the observation.
It is true that the critical point of the upper layer lies at a concen-
tration of about 30 mol. °/, water, and that it is therefore not so
one-sided as for the mentioned systems of carbonic acid, but an
altogether different difficulty prevents the observation, viz. the invi-
sibility of the lower layer for comparatively small quantities. So
after some futile attempts I discontinued the observations with this
system. Hence a direct observation of the phenomencn in question
has not succeeded as yet, and will, it seems to me, be always
attended with great experimental difficulties.

2. Of late attention has been drawn to the system ether-water
in consequence of an investigation by Prof. Van per Waats. In his
17th contribution to the theory of binary mixtures Van DER Waats
discusses this system fully as an example of that series of systems
for which under three-phase pressure the concentration of the vapour
phase lies between that of the two coexisting liquids. As far as the
system ether-water is concerned, this investigation led to a number
of conclusions, some of which could be experimentally tested through
the investigations mentioned in § 1, as was already stated by Prof.
Van per Waats in the cited paper. As it was, however, of impor-
tance to examine this system more closely with a view to the.
remaining conclusions, I have taken up again the interrupted in-
vestigation. In the following pages I intend to discuss the results
obtained for so far as they are necessary as a test of the above-
mentioned conclusions.

382

3. Preparation of the mixtures, method of observation.

Commercial ether (Pharmacopoeia Néerlandica) was twice shaken
with strong sulpburie acid, and dried first on sodium sulphate, then
on sodium. It was preserved in this condition; for the preparation
of every mixture part of this stock was distilled. As second component
distilled water was used. For the preparation of the mixtures use

Fig, 1.

was made of the apparatus represented in fig. 1. Each of the com-
ponents was weighed in a small thin-walled glass bulb provided
with a capillary stem, and put in the tubes A and &, which were
then fused to at their tops. The Cailletet test tube of combustion
class ED was connected with the filling apparatus in reversed
position by means of a rubber tube surrounded by a mercury joint.
Near its end D the tube is widened to enlarge the volume, which
enabled us to perform the experiments with a comparatively large
quantity of substance. This was necessary, because exclusively concen-
trations on the ether side were examined for this investigation; if a
Cailletet tube of the ordinary shape had been used the quantity of
water used would have been too small for accurate observations.
The part of the apparatus represented in fig. | was connected
by means of the glass spiral M with two tubes with cocoa-nut
carbon, a Geissler tube, and a water-jet pump, which served to

383

bring about a sufficient vacuum‘). When the whole apparatus had
been exhausted, the bulb with water was broken by cooling with
carbonic acid alcohol, that with ether by heating, and the contents
of both were condensed in C and D by means of liquid air. The
air dissolved in the liquid in the bulbs could then be removed by
the cocoa-nut carbon. Then the mercury which had been boiled in
vacuo was conveyed from G in small drops through the constriction
H into the Cailletet tube, which was then screwed into the pressure
cylindre in the known way after having been separated from the
filling apparatus at F’.

In some experiments the stem of the bulb filled with water was
put into the opening of the plug of cock A, and broken after the
evacuation of the apparatus by rotation of A. This method of working
proved very convenient for the realisation of concentrations of definite
amount. Then there was no necessity for the bulb to be filled so
far with water as is necessary for bursting in consequence of solidi-
fication and the weighing of a definite quantity of substance was
rendered a great deal easier thereby.

At last the Cailletet tube was surrounded with a jacket, in which
nitrobenzene was electrically heated till it boiled under varying
pressures *). .

4. Discussion of the results.

In the cited paper the shape of the plaitpoint curve in its 7'-,
and its P,7-projection was examined by Prof. van per Waats. It
then appeared that after some modification fig. 43 of the series of
contributions mentioned can account for the phenomena which appear

1) Cf. e.g. These Proc. XIII p. 831 and fig. I on p. 830.

2) To obtain constant temperatures | made use of a steam-jacket, which is
different from the one generally used. A wide tube is provided with a smaller one
on either side which are closed with rubber stoppers prepared for high tempera-
tures. On the constriction at the bottom rests an inner tube, which ends about
10 cm from the upper constriction. The stopper on the bottom side has one
perforation for the Cailletel tube, which is entirely inside the inner tube, two for
the supply of the electric current, and an aperture through which a tube is put
for sucking up and letting out the boiling-liquid. The heating is effected by means
of a nickeline wire adjusted in the inner tube and wound spirally. The boiling
liquid rises in the inner tube, condenses in the upper part of the outer tube, and
flows down in it. in the inner tube two branch apertures have been made close
to the bottom to keep the liquid at the same level inside and outside the inner
tube. A glass tube through the stopper at the upper end brings about the con-
nection with water jet pump, manometer, pressure regulator etc. If we proceed
in this way there is no difficulty whatever in keeping the temperature constant for
any length of time.

384

in the system ether-water’ In fig. 43 the case has been drawn that
the three-phase line would just terminate at the minimum critical
temperature; in the 17 contribution, however, it is pointed out
that this end-point of the three-phase line, which we will designate
by the name of “critical endpoint” in our further considerations,
may occur both on the branch AQ, and on the branch Q, Pia.

Hence we shall have to distinguish three cases as regards ‘the
relative situation of the critical end-point and the minimum critical
temperature, viz. :

1. If the critical end-point lies on the branch AQ,, the critical
line in its P,7-projection will have the shape as has been drawn
in fig. 51 of the paper that has already been cited several times.
Then the minimum critical temperature is found in the metastable
region, and cannot be experimentally realized except by the appear-
ance of phenomena of retardation.

2. If the three-phase line terminates exactly in the point Q,
(fig. 48), the minimum critical temperature would occur just on the
boundary of metastable and stable phases, and so it could be demon-
strated by experiment. The P,7 projection for this case has been
represented in fig. 50.

3. If lastly the three-phase line terminates on the branch Q, Piz,
the critical end-point lies on the righthand of the minimum critical
temperature. Accordingly the latter, if really present, will lie in the
stable region, and might be found experimentally. If, however, it is
not present, it might be imagined to lie outside the figure, and the
plaitpoint curve on the side of the ether would have to exhibit the
tendency to this minimum. At last as transition case we might still
suppose that the minimum critical temperature would just coincide
with the critical point of ether, and that therefore it could just be
still demonstrated. As far as the P,7-projection is concerned, the
presence or absence of the minimum critical temperature would have
to manifest itself in a strong negative rise with vertical tangent,
resp. in a very strong positive rise on the ether side.

From the above-cited experiments by KuENEN it may be already
inferred that the system ether-water is a case as mentioned under
3. The critical temperature of the upper layer lies, namely, at
higher temperature than the critical temperature of pure ether. So
the critical end-point lies on the ascending branch in the 7'2-pro-
jection.

In the cited treatise case 3 has therefore been fully examined,
and Prof. vAN per WaAats arrives at the conclusion that it is possible
that the three-phase line before terminating on the critical line, first

385 :

intersects it in its P,7-projection. With regard to this last case again
three cases may be distinguished. We may, namely, imagine that the
three-phase line without previous intersection terminates on the cri-
tical line, that intersection takes place before this end-point (see
fig. 48), and thirdly that the intersection takes place exactly in the
end-point, i.e. that in the critical end-point the three-phase line touches
the critical line (fig. 49). This last case is again to be considered as
the transition case between the two first-mentioned ones.

5. To enable us to decide which of the possible cases discussed
in the preceding paragraph presents itself in the system ether-water,
the P,7-projections of the plaitpoint line and the three-phase line
had to be experimentally determined. For it is possible to derive
from the situation of the plaitpoint line whether or no a minimum
critical temperature occurs (vertical tangent), and from the relative
situation of the said lines a conclusion may be drawn as to whether
or no an intersection occurs. So the determination of the P,7-
projections of the two lines might suffice; the three-phase line can
be determined by means of one mixture, provided it do not possess
a concentration that lies too much on one side. For the determina-
tion of the critical line the 7, and P, found for different mixtures
should be combined together to one line. So for every mixture
practically nothing but the critical pllenomenon need be observed,
and of a single one the three-phase line in the neighbourhood of
the critical end-point.

However, I have not been satisfied with this. To obtain as much
certainty as possible I have observed part of the three- and two-
phase equilibria of every mixture. The great advantage yielded by
these observations, is the following. If a mixture should contain a
slight quantity of admixtures, and the presence of air is the most
probable, this mixture would bring about an error in 7, and Px,
and so it might furnish a point which might cause the course of
the critical line to deviate from the correct one. In the determina-
tion of the three-phase pressure, which must show the same value
for all the mixtures used, we have, however, a criterion of purity.
With none of the mixture, for which this test could be applied, a
deviation was found exceeding 0,1 atmosphere.

But besides this, the observation of the two-phase equilibria furnished
another advantage. We want to decide, among others, whether inter-
section takes place between the three-phase line and the critical curve.
If we now put the case that this intersection really occurs, the part
of the critical line between the point of intersection in question and

386

the critical end-point lies at higher pressure than the three-phase
line. So two-phase equilibria must be possible at these tempera-
tures between liquid rich in ether and vapour at pressures higher
than the three-phase pressure. If, therefore, only one point of end-
condensation of the ether layer was found to lie higher than the
three-phase pressure at the same temperature, the intersection would
have been proved. So we see that in the observation of the two-
phase equilibria we may find a second decision on the presence or
absence of the point of intersection in question.

Now what concerns the observation of the two-phase equilibria
we have already seen in § 1, that the liquid which is rich in water
is sometimes not observable in the mixtures. This, however, does not

Fig. 2.

affect the decision in question. For every mixture I determined the
initial and the final condensations of the ether layer in the neigh-
bourhood of the critical temperature. If in one of the two a layer
is present, visible or invisible, which is rich in water, the pressure
must be the same as the three-phase pressure. Now it follows from

387

Ether | (Ae hoes (1) x — 0.024
|
I]

ip | (2) x = 0.051 || (3) x 0.118 |(4) x = 0.1925
= |

l} ;
Seen tf het tet.) Poe bal ¢ lg

| | |
156.9 | 20.0 | 150.3 | 21.2 || 160.75 | 22.2 || 165.5 | 24.9 |/ 163.1 | 25.5 | 164.15 26.95
160.9 | 21.45}| 155.9 | 23.5 || 165.5) 24.0 || 173.45 | 28.3 |] 169.7 | 28.4 || 175.45 | 32.7

165.5 23.1 ||161.5 (26.0 || 170.5 | 26.05) 179.35 31.15]]177.9 |32.5 || 184.1 | 37.65

171.1 | 25.3 |/165.9 28.1 | 174.85 279 | 185.7 34.3 |}185.1 |36.4 ||192.7 | 43.05 |
171.3 27.9 ||170.15 30.45) 180.2 30.4 | 189.3 36.1 |] 189.55 38.9 ||196.5 | 45.55)

180.8 29.55 )/174.5 32.8 | 184.6 3255]}193.55 38.4 ||191.5 | 40.05|)1964 | 45.3
185.3 31.7 ||179.55 35.75) 1895 35.0 ||1941 38.6 |]193.0 40.95] 196.15 45.0
Sls SEs) Seles 191.75 362 1198-7 |98.2 |] 194.7 |419 eke
193.9 361 || 190.15 42.65|/192.7 36.7 || 192.85 37.651|194.85 41.9 || 193.75 | 43.2

| 193.3 37.0 || 191.7 36.95 | 193.85 40.95 || 193.0 | 42.55

194.7 | 45.9 |

199.1 49.2 |/1940 37.3 ||190.2 36.1 || 192.1 30.65 190.9 | 41.0

202.2 51.8 ||193.5 | 36.9 | 190.05 | 38.3 |
191.9 35.9 | |
190.15 35.0 | |

(5) x = 0.226 | (6) + = 0.260 | (1) x = 0.275 || (8) x = 0.298 || (9) x = 0.300 10) + =0.316

|
| | |

Pejole|ofelo| ele] + |e t |p
| |

\} |

| | | | |
| 164.2 | 27.2 ||176.7 | 33.9 || 157.9 | 24.3 || 178.7 | 35.15|/ 176.7 | 33.9 | 163.1 | 26.8
| |

174.9 | 32.8 || 185.0 | 39.0 || 169.1 29.8 || 186.75 | 40.3 | 188.1 41.15 182.5 | 37.6

| 182.3 | 37.2 |}189.9 | 42.1 |1185.7 | 39.6 | 194.35 45.5 | 191.5 43.55 || 186.9 | 40.4
1959 39.35|1947 4545|1893 420 | 198.3 484 | 195.65 46.5 || 193.9 | 45.25
(190.35 42 15] 198.75 48.4 }1925 44.2 2008 50.4 | 200.1 49.95 196.9 | 47.55
(192.5 | 43.65//199.35 48.9 || 195.1 46.0 ||199.5 49.3 201.0 ) 199.15 49.3
| 194.85 | 45.2 1197.6 47.5 ||2001 (49.7 || 197.1 | 47.4 |/200.2 | 49.95|/201.9 | 51.55
197.6 47.1 |] 194.05 44.85 || 198.65 48.5 | 193.45 44.75 || 198.65 | 48.75 || 200.55 | 50.35

1195.1 | 45.8 || 189.55 42.0 | 195.8 | 46.6 || 198.85 | 49.0

197.35 46.9 || 189.85 41.8
(195.6 45.5 192.7 | 44.05, || 193.25 | 44.7

192.05 42.85 190.0 42.2 | }191.4 (43.4

388

the observations given in figure 2 and table I of pure ether of the three-
phase pressure determined with a mixture of about equal quantities by
weight, and of some ten mixtures of the concentration given in the
table, that not a single end-condensation of the ether layer can be
realized which took place at higher pressure than the three-phase
pressure. This shows us in an indirect way, what we also see directly
from the locus of the plaitpoints, that there is no intersection between
plaitpoint line and three-phase line. The relative position of the two
lines is, however, snch that we are here quite in the neighbourhood
of the above-mentioned transition case. The inclination of the two
lines in the critical end-point differs so little that we may practically
speak of contact here. In the P,7 projection the lines of the initial
and final condensation of the ether layer have been indicated by
ithe same numbers as the corresponding mixtures in the adjoined
table.’) It is clear that the mixtures 6, 7, 8, 9, and 10 in the neigh-
bourhood of 160° have yielded the three-phase line as end-condensation.
In ascending order this was the case up to higher and higher
temperature. For the mixtures 1 to 5 the end-condensation pressure
was lower than the three-phase pressure over the whole range of
temperature; hence there was no question of the occurrence of
three-phase equilibria with these mixtures. The intersection of the
line of the end-condensations and the three-phase line must be looked
for here at lower temperature.

It is, moreover, clear, from figure 2 that the critical line at the
critical point A of the ether rapidly proceeds to higher pressure, as
Prof. vAN DER WAATS anticipated. Whether the inclination is infinitely
great or very great in the direct neighbourhood of 7), of ether, could
not be ascertained. Also in this respect we may again speak of a
transition case for this system. For we cannot state with certainty
whether the minimum critical temperature lies in the figure or on
the axis, or whether it would lie just outside the figure. The last
seems, however, the most probable from the given observations.

When the plaitpoint line is considered in its other projections, it
appears that in the 7\x-projection the inclination on the ether side
is very slight, almost zero, and that it continually increases up to
the critical end-point on imereasing concentration. In the graphical
representation the P,x-projection appears to deviate very little from
a straight line.

1) In the table the critical data have been given in bold type, above them we
find the values of the end-, below them those of the begin-condensations of the
ether layer.

389

If we finally consider the relative situation of the phases on the
three-phase line, it appears from what precedes that the vapour phase
lies between the coexisting liquids up to the highest temperature,
that the vapour branch, however, closely approaches the branch of
the liquid rich in ether already before the critical end-point. It is
in agreement with this that a P,z-section brought through the P,7,2-
surface e.g. for the critical temperature of ether yields two curves
which show decreasing values of ~ starting from the critical pressure
of ether, that tbe intersection with the three-phase line, however,
appears just before the maximum pressure is reached, at which the
concentrations of liquid and vapour would become the same.

So in the system ether-water the minimum critical temperature
predicted by Prof. van Der Waats lies in the immediate neighbour-
hood of the axis, and the remarkable point of intersection at the
critical end-point.

I intend to repeat this investigation for another system hoping that
I shall be able to demonstrate both peculiarities experimentally when
the situation is a less one-sided one.

Anorg. Chem. Laboratory of the University.
Amsterdam, Sept. 13 1912.

Chemistry. — “On quadruple points and the continuities of the
three-phase lines.” By Dr. F. E. C. Scuerrer. (Communicated
by Prof. J. D. vAN DER Waazs).

1, In a previous paper’) I examined the continuous connection of
the three-phase lines, which occur in Bakavis RoozEBoom’s spacial
figure on tbe most simple suppositions. It then appeared that the
three-phase lines Sag +5Sp +L and S,s+5g3-+@ pass continuously
into each other, and that in the P,7-projection this transition takes
place by means of a partly metastable, partly unstable curve with
two cusps, in both of which two three-phase branches touch. I have
now extended this investigation to the other quadruple points which
can occur in binary systems; I have, however, postponed the publi-
cation of it for a long time, because the phenomena which present
themselves in the most interesting case, are much more complicated
than in the above mentioned case, and a full description would
require a great many intricate figures. Without treating the cases

1) These Proc. 1910, p. 158.

320

fully I have, however, managed to give a survey of the phenomena
which in general present themselves in quadruple points. It seems
to me that the construction of the figures referring to a definite
case will not present any difficulties, if this survey is consulted.

In the first place I will assume in the following considerations
that continuity only takes place between liquid and gas phases. So
I preclude an eventually present continuity between solid and fluid.
If it should appear that van Laar’s theory, which leads to this con-
tinuity, is valid, this transition will also have to be reckoned with
for a complete treatment. On the appearance of a quadruple point
S,+5,+5,-+5, the four solid phases could then pass continuously
into each other. Until, however, the existence of the continuity in
question shall have been experimentally realized, it seems better to
me not to take it into account to prevent our entering into an ela-
borate consideration of a great many cases which may appear later
on to be physically impossible.

In the second place I exclude a continuity between solid phases.
Their occurrence has indeed been ascertained, but until certainty
has been obtained as to how the crystallographic orientation in the
equation of state of the solid substance is to be taken into account,
it seems impossible to me to obtain certainty about the connection
of the three-phase lines in consequence of this continuity.

If we now consider that in a binary system unmixing in the
gaseous state has never been found as yet, and never more than
two simultaneous liquid layers, it appears that in all six different
quadruple points can occur:

1, & -S. 4+ 65.5. 8.5) 4)5 a Se ee
29.16, 16 LO as 4 Se 6 eS 2 ae

In the quadruple points 1, 2, and 4 no continuities can appear
between the three-phase lines, in which liquid and gas phases par-
ticipate. Of the three cases 8, 5, and 6, which accordingly remain
for our consideration, the case 5 has already been fully examined
in the cited paper.

Case 8 only differs slightly from 5. In the quadruple point 8 the
the three-phase lines S, +8, -+1,, $,+5,-+1L,, 5, -+ L, + L, and
S,+L,+ 1, occur, of which only the two first are in continuous
connection with each other. It is easy to see by the aid of the V,2-
projection, that this connection again takes place by means of an
unstable branch with two cusps in the P,7-projection, just as this

391

was shown before for the case 5 with regard to the three-phase
lines 8, +5,-+1L and §8,+58,+6G').

' Tf, however, we compare the three-phase lines 5, + L, + L, and
S, +L, + L, of case 3 with the corresponding lines S,+L-+G and
S,+1+6G of case 5, it is clear that in the latter case the two
lines terminate in the melting-points of the two components, at least
if we have a case of the ordinary spacial figure. In case 3 on the
other hand, the binodal line of the two liquids can be an entirely
closed curve with two plaitpoints. Each of the three-phase lines
S,+L,+L, and §,-+ L, +L, will then possess two critical end-
points in the /P,7-projection. Yet this difference between the cases
3 and 5 is not so great as one would be led to expect at first sight.
The occurrence of critical end-points is not confined to the case 8 ;
also in case 5 it is possible that the three-phase lines 5, -+ L+G
and 8,+L+G do not reach the melting-point, but come into con-
tact with a critical line. This case, which is pretty well the prevailing
one in case 8, has been shown by Smits for case 5 in the system
ether-anthraquinone.

2. The quadruple pomt S+ L,+ L,+ G.

So we have seen that the quadruple points 3 and 5 give rise to
analogous phenomena; the only remaining case 6, however, deviates
from what we discussed in many respects. Where in the quadruple
points 8 and 5 continuity is always only possible between two
phases we have three phases L,, lL, and G, in the quadruple point
6, which all three may pass continuously into each other. So the
phenomena become more complicated here, and it is already a priori
clear that the connection between the three-phase lines may take
place in different ways. What cases we have to distinguish for this
quadruple point can be easily derived from Prof. vAN Der WaAats’
investigations on unmixing. It is known that the critical line can
present very different shapes when a longitudinal plait exists on the
w-surface.

In the first place we may imagine that at low temperature solely
a transverse plait occurs on the w-surface, that on rise of tempera-
ture a longitudinal plait is formed (inside the transverse plait), that
on further rise of temperature it makes its way outside the transverse
plait, and that it afterwards again retreats inside the plait, and dis-
appears at a temperature which lies lower than the lowest critical
temperature of the transverse plait. This case, to which we shall

t) false § &

392

refer as the first in our further considerations, yields a critical line,
which consists of two entirely detached portions, one of which, lying
at high temperature, presents the normal shape, and the other is in the
P,T-projection a closed figure with two heterogeneous double plait-
points, which represents the locus of the critical points of the longi-
tudinal plait.

In the second place it is possible that the longitudinal plait, which
has got outside the transverse plait in the same way as above,
continues to exist far above the temperature at which the transverse
plait gets detached on one of the two sides. Then a transition takes
place at a certain temperature in the connection of the plaits; the
longitudinal plait, which was entirely closed at low temperature,
then merges into a part of the transverse plait, while simultaneously
the portion of the transverse plait on the side of the component with
the lower critical temperature gets isolated, and retreats inside the
former at rise of temperature, and disappears. This case is referred
to as the second in what follows.

I have now examined the question what phenomena may appear,
when a tangent plane for solid-fluid is rolled over the y-surfaces in
question, and it has appeared to me that the behaviour in both cases
can be ascertained by a comparatively simple train of reasoning. In
these considerations | have contined myself to those cases, for which
only the components occur as solid substances.

3. The first case.

When we consider the case that was called the first in the pre-
ceding paragraph, we can get a survey of the phenomena by means
of figure 1. In this figure it has been assumed that (dp/dz), is always
positive, in other words that we are in the lefthand part of the
isobaric figure. The longitudinal plait here possesses two critical
points P, and P, where contact takes place with the spinodal line.
Further only the liquid binodal line has been drawn of the transverse
plait; the vapour branch, which lies at large volumes has been
omitted in the diagram; it possesses a ridge, the two end-points of
which indicate the phases coexisting with A and 4. About the rela-
tive situation of longitudinal and transverse plait we know that at
low temperature the longitudinal plait lies entirely inside the trans-
verse plait, at higher temperature the former passes the border of
the transverse plait, and at still higher temperature it retreats again
inside the latter. In this temperature range the transverse plait covers
the whole width of the figure, as we remain all the time below the
critical temperature of the components.

We shall now imagine that a tangent plane for solid-fluid rolls
over the y-surface, and we choose as solid substance the first com-

; ss

Fig. 1.

ponent. At very low temperature the curve which is described by
the tangent plane on the y-surface, will lie entirely on the right-
hand side of the figure. So if will not come in contact with the
longitudinal plait, if it should be present already. This condition has
been represented by the curve a in figure 1; it intersects the bino-
dal of the transverse plait, and this point of intersection indicates
the liquid of the three-phase equilibrium S+ L, + G (we denote
by L, the liquids lying on the righthand of the longitudinal plait).
Now on rise of temperature the possibility presents itself that the
binodal solid-fluid comes in contact with the longitudinal plait. If
this is the case contact will take place, and this can happen no-
where else than in the plaitpoint. This is easy to see, as in case of
contact in another point of the longitudinal plait a second liquid
would have to coexist with the solid substance, and so no contact,
but intersection would have to take place. This condition of contact
has been represented by curve 4. So the fluid phases coexisting with
solid yield. a line 4, which passes through the stable plaitpoint of
the longitudinal plait, and intersects the transverse plait in two
points, of which again only the liquid point has been indicated in fig. 1.

Then at higher temperature an intersection follows in four points.
Two points of intersection with the longitudinal and two with the
transverse plait then lie on the line solid-fluid; so at this tempera-
ture there are two stable three-phase equilibria $ + L, +L, and

26
Proceedings Royal Acad. Amsterdam. Vol. XV.

394

S+1L,+G (linec); the equilibrium L, + L, + G isstill metastable.
This condition continues to exist till the line for the fluid phases
coexisting with solid gets into contact with the liquid branch of the
transverse plait in A, and then also passes through the righthand
cusp in the vapour branch of the transverse plait (line d). This is
followed by a range of temperature, in which six points of inter-
section with the transverse plait, and still two with the longitudinal
one occur. At these temperatures five three-phase equilibria then
appear in all. This range terminates at the temperature of the curve
f, where again contact with the liquid branch of the transverse
plait is found (in B), and the line for fluid by the side of solid
passes through the lefthand cusp of the vapour binodal curve. In
this temperature range we find the quadruple point, the behaviour
of which is given by the curve e. Above this range of temperature
four points of intersection again occur, till the temperature is raised
to that of g, where contact with the longitudinal plait takes place.
Then eight points of intersection again follow, six of which, however,
now lie on the longitudinal plait. This continues to be so till the
condition / is reached, above which again two intersections with
the longitudinal, and again two with the transverse plait take place
(curve 7). At last in / the temperature is reached at which contact
in the hidden plaitpoint ?, takes place. At still higher temperature

Fig. 2.
there is no longer contact of the fluid line with the longitudinal
plait, and the latter will recede within the transverse plait.
After this discussion it will be easy to construct the P, 7-projection
of the three-phase lines, which has been given in fig. 2. The tem-

odo

peratures for which the intersections in fig. 1 were studied, have
been indicated in fig. 2 by the same letters. The three-phase line
L,+1,+G retairs therefore the shape which it has when no
solid substance occurs; one part has, however, become metastable
here. Just as the line L,+ L,-+G the three-phase line S+L, +L,
possesses two plaitpoints, one of which is stable, and the other
metastable or unstable. Besides the former possesses a ridge, which
lies entirely in the non-stable region, the ends of which correspond
with the points where the lines y and / of fig. 1 cut the spinodal
curve. The two other three-phase lines 5+ L,+G and 8S+L,+G
are continuously connected by means of such a ridge, the end-points
of which correspond with the points A and 4 of fig. 1. That really
ridgelike figures occur here, with contact of every time two branches
in the end-points is easy to see; this will always be the case when
two binodal lines touch in a point of the spinodal line (plaitpoints
excepted). If we choose the temperature very little different from that at
which contact takes place, then if the direction of the change of tempe-
rature has been correctly chosen, an intersection will appear of the bino-
dals; then in the J’, .-figure there are two three-phase-triangles present,
the angular points of which draw near to each other on approach of the
temperature of contact, and coincide when this temperature is reached,
If e.g. we have the intersection of a line between (d and e with the
transverse plait in fig. 1, then the two phases L,, the two phases
G, and the two solid phases will coincide at a lower temperature.

ap. -. ee ee We
Now the value for :3 for both the two three-phase equilibria is
Q

given by the equation :

; nh G => a Ll :
: yf Gly <a mre ta WSL,
dp ee £5 — £1,
Ch LG — £L,
AES aves “SIy

TNS eee is

in which all the quantities of the second member refer to the three
coexisting phases. It is now clear that on approach of the tempe-
rature of contact the two phases L,, the two phases G, and the
two solid substances differ less and less in properties, and that at
the temperature at which contact takes place, the quantities of the
second member refer to identical phases. For the two three-phase

_ dp
branches the value of ar becomes exactly the same at the tempe-

rature of contact, and so contact oecurs.
26~

396

_d :
It may be further pointed out that the value of = at this contact

does not in general become infinitely great. This would be the case,
if in the point of contact also the condition:

eee oS a

LG — £], 25 ale

was satisfied.
It is easy to see from fig. 1 that this will not be the case in the

point A.

4. In §3 we assumed a very decided relative displacement of the
fluid line with respect to the longitudinal plait for the derivation of
fig. 2. It will be clear that the relative displacement of the said
binodal curves can also take place in another way than that described
above. If we want to ascertain how great the number of possibilities
is that may occur, we should first of all bear in mind that our first

dp ise 2
assumption was, that (7) was positive on the y-surface. Further
ae
we took the first component as solid substance. If we now exclude

: dp : :
the appearance of a line ({r) = 0, it will be clear that we can
az),

be) dp pei f 7
survey all the cases if we take ) always positive, and choose
ae,
. sea a.) es
the two components as solid substances. For if 7) 38 negative,
e/}y
and the solid substance is the second component, we get the same
dp\ , fe
phenomena as in the case where Ft positive, and the first
Cty.
component appears as solid phase.
ney dp rc ere eee
So if we keep a always positive, the situation of the longitu-
av vo

dinal plait is always as indicated in tigure 1. The differenees between
the cases which may occur, are accordingly caused by the fact that
both components can occur as solid phase, and by the relative
displacement of the solid-fluid line with respect to the longitudinal
plait.

If we confine ourselves to the ease that the first component is the
solid phase, we see a second possibility in figure 1, if we suppose

es ; P dp
') The transformed denominator of the above expression for =

397

that the line for solid-fluid retains its shape @ to higher temperatures,
and that then on rise of temperature a longitudinal plait arises on
the righthand of a, which plait extends and overtakes the line for
solid-fluid. It is clear that then contact takes place in the unstable
plaitpoint P, at low temperature, and that with rising temperature
the intersections with the longitudinal plait may take place in reversed
order as has been described above. In this case in opposition to
fig. 2 the three-phase line L,-+ L,-+G is stable at temperatures
below the quadruple point, and at temperatures above it metastable,
and the stable part of S-+ L, + L, possesses a positive value for

dp
= This, however, does not affect the connection between the three-

phase lines S++ L, + G and 5+ L,+G, and the two other three-
phase lines retain their critical points just as in fig. 2.

Finally we may assume that the line for solid-fluid forces its way
inside the longitudinal plait in the way represented in fig.1 by the
line p, and this line can again be displaced in two directions with
respect to the longitudinal plait, so that either the stable or the
metastable plaitpoint is situated at the lower temperature.

So we get in all four different quadruple points, when the solid
substance is the first component, and as many when the second
component appears as solid substance, so that we have to conclude
to eight different types of quadruple points, at least if we disregard
the appearance of ordinary pressure and temperature maxima, which
occur, if the situation of the three-phase points satisfies the conditions:
ee ss tae 3 ed

—= 0 resp. = *— (),

wv 1 L 2 == 1 a 1

Lav, Ls

I will not enter into the further treatment of these cases, because
for all these possibilities the result already obtained in §3 always
remains intact that the two three-phase lines S+ L,-+G and
S+1,+G are in continuous connection, and that on the two other
three-phase lines two critical points occur. Nevertheless it seemed
desirable to me to give a survey of these possible cases, because
the appearance of these quadruple points will not be rare; they will
occur in almost any system where unmixing continues to exist below
the melting-points of the components.

5. The second case.

In the second case we have supposed that the longitudinal plait
continues to exist to above the lower critical temperature of the
transverse plait. So one of the components has then become critical,

398
and at these temperatures only the appearance of the other compo-
: : ' ; dp
nent as solid phase is possible. So again supposing az to be posi-
ry

tive, only the first component can appear as solid substance because
then the second component will generally possess the lower critical
temperature. We know that in this case a transformation in the
connection of the plaits takes place, as is indicated in fig. 3. We
must now suppose that at low temperatures the behaviour does not

differ from what was discussed in §3 (lines a, 6, and ¢ of fig. 1),
that then, however, the transformation of fig. 3 makes its appearance.
If this takes place before the condition g of figure 1 has been
reached, it is clear that the liquid points of the three-phase line
S+L,+1L, lie on the longitudinal plait at low temperature, but
that when the transformation takes place the branch on which L,
and L, lie gets into connection with the vapour branch. Henee on
rise of temperature the three-phase line S-++ L,-+ lL, merges conti-
nuously into S+ L,-+ G. Then the points L, and G of the three-
phase line S+L,+G which lie on the transverse plait at low
temperature, are both found on the closed portion in the trans-
formation; hence the three-phase line 5 -+ L, + G terminates in the
hidden plaitpoint ?,, where the line for fluid by the side of solid
touches the closed portion. Without our entering into any further
particularities, it will be clear in my opinion, that fig. 4+ indicates
the P,7-projection holding for this case. That again a transition takes
place by means of an unstable ridge, can be shown in perfectly
analogous way as in the transition described in § 3.

Fig. 4.

6. It will be clear that the number of cases possible compared
with those of the first case of §3 and §4 will be smaller bere, as
only one of the components can appear as solid substance, but that
on the other hand the transformation of the plaits gives rise to a
complication.

If we again take the case of § 5, the transformation can take
place before the state y has been reached, as described above. If,
however, the temperature of y is lower than that of the transfor-
mation, then just as before, the three-phase line S-+ L, + L, con-
tinues to terminate in the hidden plaitpoint ?,, and so, though the
shape of the critical line is entirely different from that in § 35, we
have the same connection of the three-phase lines 5+ L,-+ G and
S+L, + G, and two critical points on S + L, + L, and L, + L,+G.

In analogy with §4 we can also imagine that the longitudinal
plait makes its appearance and is transformed after the solid-fluid
line in the figure has been shifted some distance to the left, and
then overtakes the solid-fluid line. In this case we shall again have
to distinguish two cases, viz. that the transformation appears before
or after the state ¢.

In the first case the three-phase line, which begins in the unstable

400

plaitpoint, will terminate in the critical point P, of the transverse
plait, which has detached itself from the side, and a stable critical
end-point occurs with the properties described by Sts in the system
ether-anthraquinone. The three-phase line S-++ L,-+G then merges
continuously into the three-phase line 5+ L,-+ L,. If, however,
the transformation takes places after the state g, the three-phase line
that has started from P, will pass into S++ L, + L,, and terminate
in the stable plaitpoint ?,. Then the three-phase lines S + L, + G
and S+L,+G are continuously connected, and the latter ends
again in a critical end-point on the closed transverse plait, which
has detached itself.

Finally we should. still take into account the possibility that the
line for fluid can possess the shape of line p in fig. 1, and also for
this case we get four types of quadruple points, which, however,
differ only shghtly from the preceding types.

All the possibilities, however, agree in this that either two critical
points oceur on the three-phase lines 5+ L,-+L, and L, + L, + G,
and the continuous connection takes place between S-++ L,+G and
S+ L, + G, or one of the three-phase lines S + L + G is in
conuection with S + L, + L,, and the other three-phase line S + L+G
possesses one or two critical points.

7. In the preceding paragraphs we have pretty completely
discussed the types which can possess quadruple points, in which the
components occur as solid phases. The occurrence of mixed crystals
and compounds does not give rise to essential modifications. All the
same different types should be distinguished for these cases ; this
follows, namely, already from the fact that with the discussed
quadruple points the solid substances always possess either the
greatest or the smallest concentration, and so the possibility was
excluded that the concentration of the solid substance lies between
that of the coexisting liquid and vapour phases. To form an opinion
of these cases the most rational way would be to have recourse to
the w-surface ; this alone can give a complete insight into the pecu-
liarities that oecur for a definite case. Generally, however, we can
avoid this course; but then the danger is great to assume possibi-
lities, which would appear to be physically impossible if the y-surface
was consulted. To escape this danger, and to avoid on the other
hand the more laborious way via the y-surface, I] will here draw
attention to a rule which gives a_ relation between the relative
situation of the three-phase lines and the concentrations of the coexisting
phases.

401

The simplest way to state this rule is in my opinion as follows.

The region that docs not possess metastable prolongations of three- -
phase lines in the P,T-projection is that of coexistences of phases of
consecutive concentration.

Perhaps the clearest way to set forth the meaning will be by
means of fig. 2.

If we produce the four stable three-phase lines through the
quadruple point, as has been done in fig. 2, it appears that no
metastable prolongations occur in the region between S + L, + L,
and L,-+ L,+G. The region in question indicates the coexistence
of S+L,, L, +1, and L,+G. These coexistences refer every
time to two phases consecutive in concentration, i. e. if the four
phases are arranged according to their w-values, the succession is
SL,L,G. That this is really the case in fig. 2, is clear since it

dp f me ee.
has been assumed there that (2) is positive, that by L, the liquids
- v
were denoted which lie on the lefthand of the longitudinal plait, and
that the first component appears as solid substance.

8. To prove the rule in question we will indicate the phases
arranged according to their z-values in the quadruple point, by 1,
2, 3, and 4, so disregarding altogether what state of agregation
the phases possess. The four three-phase lines 1+ 2-+35, 1424-4,
1+3+4 and 2+3-+4 divide the space round the quadruple
point in the P,7-projection into four parts, which every time indi-
cate pressures and temperatures of two-phase regions. We know
besides that every three-phase line forms the boundary of three
two-phase regions, and so that on one side of the three-phase line
one, on the other side two regions occur, where every time a com-
bination of two of the three phases are in equilibrium. In the first
place it is now clear that none of the tsvo-phase regions can have
an angle at the quadruple point which is greater than 180°. If this
were so we should be able to produce one of the bounding three-
phase lines through the quadruple point. This metastable prolonga-
tion would tben lie in the region where two of the three phases
could coexist in a stable way; then, by the side of these two the
third could also occur stable on the three-phase line, which is
evidently impossible, because the prolongation represents metastable
States.

Every quadruple point which contains a two-phase region with
an angle that is larger than 180° is therefore impossible. If we take
this into account, the thesis in question can be simply derived. For
this purpose we first take the coexistence of the phases with the

402

extreme v-values, so 1 and 4, then the two-phase region 1 + 4
will occupy all the available width in the spacial figure; this region
forms a space which has the full width of the four-phase line as
boundary. So with the same pressure and temperature no other
stable two-phase equilibrium is possible there. The two other two-
phase equilibria 1+ 2 and 2+ 4, which lie by the side of the
three-phase line 1+ 2-4, and the equilibria 1 + 3 and 3+ 4,
which lie by the side of the line 1+ 3-4 4, lie therefore always
on the other side of the lines in question in the P,-7 projection.
So in fig. 5 the situation of the region
1 + 4 determines that of the two three-
phase lines AO and BO, and at the same
time that of the regions 1+ 2, 2+ 4,
1+ 3, and 3+ 4. So it now remains to
decide what the situation is of the two
remaining three-phase lines. It is now easy
to see that the line OC lying on the right
must represent the coexistence of 1 +2+3

Fig. 5. and the line OD that of 2+ 3-+ 4. The
line OC, namely, must bound on one side either the region 1 +3
or the region 3+ 4. This can only take place by the three-phase
line 1+2-+3, because in the other case besides 3 + 4, also the
region 2-3 would have to le on the same side of the three-
phase line, which can evidently not be the case. So now, the
situation of the phases is quite determined. So it appears that one
two-phase equilibrium occurs in the region AOS, two in the regions
BOC and DOA, and three in COD.

Now the angle AVS must contain the metastable prolongations
of the two three-phase lines CO and DOU. Suppose namely, that the pro-
longation of C’'O should fall in DOA, then the region 1 + 2 should
present an angle which is greater dan 180°; if the prolongation of
DO lay in COB, then the region 3 + 4 would possess an angle
greater than 180°. So it has been proved that only such a situation
is possible that no prolongation falls in the angle COD. And this
proves the stated rule.

It will, moreover, be clear from the above proof, that the thesis
might also be stated as follows :

If the phases, arranged according to their 2-values, are expressed
by 1, 2, 3, and 4, the angle without metastable prolongations lies
between the three-phase lines 1+ 2+ 3 and 2+ 3-4-4.

9. The application of this rule can naturally be twofold. At

403

certain values of the concentration it is easy to distinguish, what
quadruple points can occur and what cannut. And in the second
place it furnishes a simple means to read directly the consecutive
order of the concentrations from the observations of the three-phase
lines.

The former kind of applications is of course far more numerous
than the second. There are, namely, only few cases as yet, in which
the situations of all four three-phase lines at the quadruple point are
determined.

To elucidate the former kind of applications, I will briefly examine
what the rule requires for some known quadruple points. The qua-
druple point of the ordinary spacial figure, in which the suecession
ot the phases is 5,GI.S,, has to fulfil the demand that the region
between 5S, +G+1L and G+L-+5S, does not contain metastable
prolongations.

If we consider the quadruple point of two salt-hydrates by the
side of liquid and vapour, in which the order of the concentrations
is GLH, H,, the rule in question demands that no metastable pro-
longations occur between the three-phase lines G+ L+H, and
L+H,-+H,. This rule both holds for the ordinary case that the
hydrate H, rich in water is transformed into that which is poor in
water on rise of temperature and for the “inverse melting-points’,
where the reverse takes place. For the former case the rule requires
among others that the prolongation of H, LG lies at lower pressure
than the stable part of H, LG, and reversely, which must really be
the case, as is known.

What type of quadruple points must be expected in the case of
an “inverse melting-point’, will be discussed a little more fully here.

If we think the transformation of the two salt-hydrates to take
place in such a way that the one rich in water exists at higher
temperature than that poor in water, then the quadruple point will
have to satisfy besides the above-mentioned demand, also the con-
dition, that at temperatures below the quadruple point the three-
phase line G-+L-+H,, above it the line G+ L+H, is stable. If
we further consider that on the three-phase line L—+ H, + H, the
transformation H,-+L—-H, occurs on isobaric supply of heat, and
this will probably be accompanied with volume-contraction; that on
the three-phase line G+ H, + H, the transformation H, + G—H,
occurs on supply of heat, and that this is certainly accompanied
with volume-contraction, then we know that probably both, but
dp

certainly the line G+ H,-+ H, possesses a negative value for 7a
tf

404

If we take this into account for both lines, then it will be clear
that this quadruple point will present the shape of fig. 6, where
the angle between L+ H,-+ H, and
G +L -+ H, does not contain metastable
prolongations. I sball postpone a discus-
sion of the further peculiarities which
appear for inverse melting-points, to a
later occasion. *)

Another example, in which the rule
enables us to infer easily what quadruple
points are possible, we find among others
for a dissociating compound in solid

Fig. 6. state by the side of the least volatile
component, liquid and vapour; then we know that this quadruple
point can occur on different branches ot the three-phase line :
compound +- liquid + vapour.

Let us consider the case that the pressure continually decreases
from the first to the second component; then the quadruple point
can lie in the first place on the three-phase line so that neither
melting-point, nor maximum sublimation point appear stable. If this
is the case then the order of the phases is GLVS5S, in which V
denotes the solid compound, 5 the solid second component. The
angle without metastable prolongations lies therefore between G-+-L+V
and L+V-+5, and in this the coexistences G+ L, L+ V and
V +5 occur according to the first formulation of the rule.

If, however, on the three-phase line of the compound the melting-
point occurs, but the maximum sublimation point does not occur,
the succession has become GVLS, so that just as in the preceding
case we cannot meet with metastable prolongations in the angle
between G+ V+ Land V+ L-+5, and now find the coexistences
G+V,V+L and L+5 between the two lines. As is known this
ease is found among others when a salt-hydrate (before its transition
to the anhydrous salt or to another hydrate) possesses a melting
point.

If the compound has both a melting-point and a maximum point of
sublimation, the order has become VGLS, and no metastable pro-
longation occurs in the angle between V + G+L and G+L-5,
where the coexistences V + G, G+ L, and L+S are found.

Led by these considerations we can easily construct the quadruple
points under discussion.

') A similar type of quadruple points we find also in the system Iron-carbon.
Smits. Z. f. Elektrochemie 18. 362 (1912).

405

In conelusion one of the few applications of the second kind may
be briefly mentioned here.

In my first communication’) concerning the system hydrogen sul-
phide-water I have fully determined the situation of the quadruple
point S (hydrate) by the side of two liquids (LL, and L,) and gas (G)
with the three-phase lines terminating there. If this rule had been
known to me already then, I could have directly inferred from the
figure of the cited communication that between the three-phase lines
S+L,+G and $+1L,+1L, no metastable prolongations occur, that
there the coexistences :

S+L, (angle < 180° between 5+ L,+G and S+1h,-+1,)

Lb --G: ,, a + S+h,+G and L,+1L,-+ G) and
S+1L, Pa re ry S+h,+G and 8+1h;-+1,)
occur, and that therefore the order of the phases must be GL,SL,, if
the mentioned coexistences are to take place between phases that
are consecutive in concentration. The gas of these phases containing
the greatest quantity of hydrogen sulphide, it is clear that the
hydrate contains less water than L,, and that therefore the liquid
L, lies on the side of the water. From determinations which |
carried out later on, and which I have communicated in my second
paper?) on this system it appears that this conclusion is really valid.

Anorganic Chemical Laboratory of the University.

Amsterdam, September 18, 1912.

Physics. — “Jsotherms of diatomic substances and, of their binary
mivtures. X11. The compressibility of hydrogen vapour at, and
below, the boiling point.” By H. KameruincH Onnes and W.

J. pE Haas. Communication N°. 127¢ from the Physical Labo-
ratory at Leiden.

(Communicated in the meetings of May 25 and June 29, 1912),

§ 1. Introduction. To the region covered by the investigations
which have been made for many years past in the Leiden laboratory
upon the equation of state for bydrogen at low temperatures (for
the latest paper see Comm. N°. 100a, Proc. Dec. 1907) the present
Communication adds the region for hydrogen vapour lying between
—252° C. and —258° CU. While the lowest reduced temperature

1) These Proc. January. 1911. p. 829.
2) These Proc. June. 1911. p. 199.

406

attained in the measurements of KAamMeRLINGH ONNES and BrAAK was
about ¢ == 2.2, in our present investigation we were able to calculate
the second virial coefficient 4 for the further region from ¢ = 0.7
to about t= 0.5; by this means, since interpolation between ¢ = 0.7
and t= 2.2 is not a matter of any difficulty, 4 becomes known
over a very. extensive region of reduced temperature (from t = 0.5
to t > 12). The second reduced virial coefficient is therefore known
for a single substance over a much more extensive region of tempe-
rature than has hitherto ever been the case. This extension was
especially to be desired as, in the first place, it allows a better
comparison from the point of view of the lai of corresponding states
of 4 for hydrogen with its value for various other substances,
and this will become of particular importance when the comparison
ean be extended so as to embrace monatomic substances (a commu-
nication by KamertinGH Onnes and CromMenin will shortly appear
dealing with the 5 for argon at low reduced temperatures). In the
second place it allows us to put to the test theoretical deductions
concerning / (for instance, the connection between the peculiarities
of 4 with the peculiarities of the specific heats and of viscosity, and
also of the dielectric constants and of penetrability by electrons).
This is all the more important as / is related to that state which
according to REINGANUM can be called the planetary gas state in
which, in allowing for the influence of collisions between moiecules,
only two molecules need be considered, as the possibility of the
proximity of others may be neglected.

From 4, moreover, one can calculate the experimentally deter-
mined corrections of the hydrogen thermometer scale to the AVOGADRO-
scale, which have hitherto been known only down to — 217° C.,
down to the lowest temperatures which can be measured with the
hydrogen thermometer. (Cf. Comms. Nos. 1016 and 1020).

The uncertainty in the adjustment of a cryostat bath to an accurate
definite temperature and in the measurement of that temperature is
much greater than that with which a temperature, once steadied, can be
maintained constant. Since, now, uncertainty in the determination of
the temperature is of great influence upon the values of 5 obtained
from the observed pv,, it was decided to proceed with isothermal
measurements so as to be as independent as possible of thermome-
trical measurements. A further advantage of constancy of temperature
in the Comparison of values of pv, at different pressures lies in the
circumstance that the possible difference between the temperature
of the gas in the piezometer and that of the thermometer in the
bath is constant throughout. The advantages of isothermal measure-

—

STERRN NNN SS ANN

iy YI. |
ff (ATLA

t
ten
j be "
“VY \ Lx
{i}
fr f
} ; A
4
Ay, F
ware f
| J
| |
yale Me IT a
- . i| | ie
e
| |
aD eae
“ I = Ir

408

ments would have been far greater for us bad we not frequently
been obliged to aim at obtaining the same reading of the resistance
thermometer instead of at the maintenance of a definite temperature.

The investigation was carried out at three temperatures, approxi-
mately — 252°.6 C., — 255°.5 C. and — 257°.3 C. A lower tempera-
ture than — 257°.3 was not desirable as the smallest pressure to be
measured at this temperature had already sunk as low as 5 em. and
further progress in this direction would have necessitated another
apparatus.

For each isotherm the densities were so chosen that the ratio of
the extreme densities was about two to one in each ease. By this
means it was brought about that in the solution of Ly from the
two equations

pod, Aa + Ba dy, + Ca da,’

pu 4,-= Aa + Bg da, + Ca da,’
the coefficient of B4 was approximately 1. In this solution C4 was
taken as a correction term from the equation of state VII. H,.38
(formula (16) Comm. N°. 109a).

Finally, for practical reasons, it was necessary to remain as far
as possible away from the region of condensation, as a sudden flue-
tuation of the temperature could quite well occasion condensation to
take place upon the walls of the piezometer, and particularly of the
capillary, and this, in view of the excessively slow liberation of
liquid and vapour from the glass, would render the measurements
valueless.

The measurements were made with a piezometer immersed in a
bath of liquid hydrogen and connected through a capillary with the
volumenometer studied in detail in Comm. N°. 127a (See Fig. 1,
p. 407). The piezometer was first evacuated and a quantity of gas
measured in the volumenometer; the valve between the two was
then opened. Pressure equilibrium was then allowed to establish
itself at the desired value, and then the pressure and the quantity
of gas remaining in the volumenometer were determined.

§ 2. Arrangement of experiments. Auciliary apparatus.

The experimental arrangements are shown in fig. 1, p. 4077). One
portion of the apparatus had already been utilised in the investiga-
tion of the diameter for oxygen, and is described in Comm. N°. 117,
Proc. Febr. 1911. The left hand part of fig. 1, p.407 is an impro-

') In the drawing some details of no importance are incorrectly represented, viz:

the ice ought to cover the bottle R, the air-trap Z/ is in reality much smaller,
the safety-tube Ys; is of course not wholly filled with mercury.

409

ved copy of the left hand part of Pl. I of that Communication, to
which we may in the first place refer. The improved diagram
embraces the modifications which were introduced later, and which
are described in Comm. No. 121@. Identical parts are indicated by
the same letters in fig. 1 and in Comms. Nos. 117 and 1214a, parts
which have undergone modification are distinguished by accents,
while parts which are new or are now lettered for the first time
have new letters attached to them. We may refer to W. J. pe Haas’s
thesis for further details concerning the water circulation, IW, which,
supplied from the thermostat, keeps constant and uniform the tem-
perature of the volumenometer and of the manometer.

The volumenometer is connected to the auxiliary reservoir /”
through the taps #4, and /,. This allows one to add gas to the
measured quantity contained in the volumenometer, or to temporarily
abstract a measured quantity from the volumenometer. This was
essential in our experiments as the volume of the piezometer, in
which the gas density was sometimes practically 20 times as great
as that in the volumenometer, was 110 ¢.c. and that of the volumeno-
meter was not more than 1250 c¢.c. Hence, if, for instance, the
volume is adjusted to the smallest volume in the volumenometer
(the neck m, in the figure) at a pressure of one atmosphere, then
even when the volumenometer is completely filled (to the neck m,
in the figure) the second equilibrium pressure of half an atmosphere,
which, according to § 1, is desirable in this case, is not vet attained.
The admission of gas from the volumenometer to /” and vice versa
ean be of use in another way, viz. in the transition to another tem-
perature and in the adjustment of pressure equilibrium. In the course
of our experiments, however, we have not been able to make such
free use of the auxiliary reservoir as we should have liked. The
volumenometer can be evacuated through the valves &,,/,,4,,; and it
can be connected to the barometer and to the constant pressure
reservoir, R, (Comm. No. 60, Pl. VI) through &,, &,, &,,, 0, 4, Ais.
When the volumenometer adjustments and the value of the pressure
permit of it, the valve /, may be closed and the pressure then deter-
mined from the manometer J/ alone, the space above which is then
evacuated through /,. We may refer to Comm. No. 121la by W. J.
DE Haas for further details concerning the pressure measurement.

To ascertain when pressure equilibrium has been attained we applied
the method already described in Comm. No. 127; the pressure in
the volumenometer was under constant observation, and from the
curve expressing the pressure as a function of the time, we deduced,
during the observations, the time at which the pressure difference

Proceedings Royal Acad. Amsterdam. Vol. XY.

410

originally existing between the volumenometer and the piezometer
lad sunk to a value that was insignificant. The reliability of this
method is shown by the caleulations published by W. J. pe Haas
in Comm. No. 127a. For assistance rendered in the application of
this method and for further help given in the course of this research
we should like to express our indebtedness to Mrs. DE Haas-LORENTz.

Readings were taken with a very fine Société Genevoise catheto-
meter with three telescopes’), each with a micrometer eyepiece and
level. A scale with very accurate subdivisions (Comm. N°. 60) was
used for the readings with the micrometer eyepieces.

Communication between the volumenometer and the piezometer
see the right hand portion of the diagram) was obtained through
the tap &,, the glass 7-piece (closed on’ the other side by £,) over
which a connecting tube is cemented, a copper capillary g, (to give
a certain elasticity to the connections), the steel taps 4,,%,, a steel
capillary g, and a glass capillary /,. The steel taps 4,,4,,4,, were
provided with selected cork packing and were kept for about half
an hour at a pressure of 50 atm. They closed perfectly. Connections
between steel and glass capillaries were also made with the greatest
care. This connection was made by means of a brass screw soldered
to the glass capillary, the capillary being very slightly rounded and
projecting about */, mm. beyond the screw; this joint sustained a
high vacuum for a long time. The rounded end of the glass capillary
was covered with a packing ring made of fibrous plate, and could
be screwed with force into the brass nut soldered to the steel
capillary.

The diagram does not show the wool with which all the principal
parts of the apparatus were wrapped. The barometer was wrapped
with the greatest care in wool, and was, moreover, surrounded by
a double layer of paper so as to eliminate all convection currents.

") Compare the similar adjustments of Comm. No. 95e, Table I.

The difference between the levels of the top and the edge of the meniscus and
between the top of the meniscus in one of the necks and the central line on a
screen (Cf. Comm No. 84, Pl. Il, Proce. March 1903) can be obtained with sufficient
accuracy and more quickly from the catethometer scale than with the standard
scale and level and the micrometer eyepiece. In the majority of cases it is sufficient
and much simpler still to estimate these differences of level from the standard scale
wilhout focussing the micrometer upon the divisions of the standard seale at all.
lor an error of 10°/, in the determination of the height of the meniscus leads to
an error of 1°/, in the capillary depression; and an error of 1 mm. in the estima-
tion of the height of a line on the sereen induces an error of only 16 or 17 mm3,
in the volume, which makes a difference of only 1 in 60,000 in the volume of
gas usually employed.

41}

Neither are the numerous thermometers shown in the diagram which
were suspended along the whole apparatus.

Finally, the connections Z%,, Zk,, lead to the hydrogen resev-
voir Z,. To this reservoir is attached a side tube with a valve,
Zk, through whieh the whole apparatus can be filled with hydrogen:
it is also provided with a purifying chamber 4j, througin which the
gas passes on its way to the measuring apparatus and consisting of
a tube filled with glass wool surrounded by a Dewar flask containing
liquid air. After the measurements the gas can be collected in Z,
through Z4:,, Z/;,,. :

We may refer to Comms. Nos. 83, 94c, 94d, 94e, and 121a for
descriptions of the thermostat, the water circulation and the cryogenic
bath and auxiliary apparatus.

§ 3. The hydrogen. The apparatus was filled with distilled hydrogen
by means of the arrangement described in Comm. N°. 94¢, § 2: the
tap Zk:,(see fig. 1) was utilised for the repeated evacuations and washings
with hydrogen.

§ 4. The temperatures. The thermostat supplied the water circu-
lation, JW, with water at very uniform temperature. (See Comm.
ht 21a).

Stirring was continuous during the measurements. A thermometer
divided into 20-ths of a degree and calibrated by the Reichsanstalt
was attached to the stirrer of the voiumenometer, the mean tempe-
rature being thus obtained. The influence was studied beforehand of
fluctuations in the room temperature upon that of the water in the
jacket surrounding the volumenometer, and it was found sufficient
to keep it constant to within one deg. Cent. This was always done.
(For further details see dissertation by W. J. pe Haas). Every deter-
mination of the volumenometer temperature can then be regarded
as certain to within 0°.02 C,

The temperature of the cryostat was regulated in the usual way ;
great care was devoted to keeping it constant by Mr. G. Hoxst,
whom we wish to thank for his assistance. It would take up too
much space here to give all the curves of this temperature regulation,
but as an example we may state that in the determination of the
isotherm at — 255°.5 C., made on the 24'' of June, and on the 8? and
14 of July, 1911, the values of the differences at five points from
the first determination were

0.005, 0.012, 0.010, 0.000 degrees Centigrade.

This corresponds to an uncertainty of 0.00004 in the value of pe .
7-7 bag

412

The temperature of the bath was furnished by the determinations
themselves. See § 6.

§ 5. Calibration, Constants and calculation of corrections.

a. Pressures.

The corrections, and in particular the optical corrections, for the
apparatus have already been discussed in part in Comm. N°. 1214.

The pressures were always reduced to the normal atmosphere of
45°N. For this the value of the Leiden atmosphere, 75.9463"), was
used. The following corrections were applied to the pressures :

1. A temperature correction for the inequality between the tem-
peratures of the mercury in the manometer and in the volumeno-
meter (Comm. N°. 121a).

2. A correction for the standard meter which is 999.91 mm. at
0° C. (Comm. N°. 70).

3. An optical correction for the refraction of light by the glass
windows (Comm. N°. 121a) and by the manometer tube.

4. A correction for the capillary depression. These corrections
were tabulated for various widths of tube, being obtained from
Kenyiy’s graphical construction and from LOouNsrTEin’s *) formula.

5. A correction for KNUDsEN’s transpiration pressure *).

6. A correction, where necessary, for the pressure of the air
column between the lower barometer meniscus and the manometer
meniscus.

7. A correction for the aerostatical difference between the pressure
in the volumenometer and that in the piezometer was neglected.

A discussion of the degree of accuracy attained in the determination
of the pressure has already been given in Comm. N°. 121a.

h. Volumes.

teference may be made to Comm. N°. 121¢@ for the calibration
of the volumenometer.

The volumes as measured were always corrected at their cali-
bration temperature. This correction was always very small.

A correction for the compression of the glass vessels was applied
by means of the formula

IVS 4) eee

>
V et et 2 d
1) This value has been caleulated with the number for the gravily at Leiden
used in Comm. N‘. 60, Sept. 1900, p. 304, and guomm = 981,625 according to
Suppl. N’. 23, *Emheiten” a. (Nolte added in the translation).
2) I’, Lonnsrers. Ann. der Physik (4) 33 (1910), n°. 2.
8) M. Knupsen, Ann. der Physik (4) 31 (1910), n”. 3.

413

in which E = 6500 K.G./mm’., uw = 1/
(See Comm. N°. 88).
In the caleulation of the volumes, the volumes of the mereury
menisci were taken from the table given by Scnren and Hevsn ’).
As regards the accuracy of the volumes measured we may remark
that a variation of one degree in the temperature causes a change
of only 1 in 40000 in the volume. The correction for the compres-

SOR S39 em.; d= 0b

an for 7 at the lowest pressure measured (5 cm.).
If this correction is applied, the remaining uncertainty is certainly
fess: thane) Fo:

As regards the volume of the mercury menisci as, for instance,
in the case of 24 = 14.8 mm. where the volume is 179.4-mm*: for
a meniscus height of 1.6 mm., and 192.2 mm’. for a height of
1.7 mm., the error for heights lying between these two values is
certainly not so great as 10 mm*. This is certainly negligible in a
volume which would, at ordinary temperature, be at least 1200 em’.
seeing that the volume of the piezometer is 110 ¢m*. and contains
gas of density from 12 to 20 times the normal. The same may be
said of the uncertainty in the volume of the dead space. Such
portions of this as were not separately calibrated with mercury
(steel and glass capillary, see dissertation pe Haas’ were volumeno-
metrically calibrated. The total dead space was about 10 ¢m*. An
error of 1°/, in the calibration or of 3 degrees in the temperature
causes an uncertainty of 100 mm’. This is only 1 in 12000 of the
1200 cm’. just mentioned. The volume calibration, however, was
much more accurate, while, as was stated above, the room tempe-
rature was kept constant to within a degree.

These comments are also all applicable to the determinations of
Comm. N°. 121a.

The accuracy attained in the calibration of the piezometer was
greater than 1 in 10000 (ef. dissertation DE Haas). The volume was
corrected for the temperature of the cryostat by means of the formula

t as ;
——) +-ivk - kt - fOs-6
eee [ | | ani) a ce | |

k, = 2348
k, = 272
(See Comm. N’. 950, §1). The error arising from this method can
only be very small.
Temperature corrections for the gas in the glass capillary were

sion gives

in which

1) K. ScHEeL and W. Heuss. Ann. d. Phys. (4) 33 (1910), n°. 2

414 =

applied in the manner published in Comm. N°. 97a § 8. For this, the
iemperature distribution along the stem was iaken from Comm. N°. 95e.
That this temperature distribution is approximately correct was
apparent, moreover, from the time it took pressure equilibrium to
be established. Cf. Comm. N°. 127a.

Collecting all these, we may regard the volumes occupied by the
cooled gas as certain to within 1 in 10000. Allowing for what we
have already stated regarding the pressure, but not taking tempera-
ture uncertainty into account, we may expect an accuracy of 0,60002
in the pva’s, or, at the highest pressure to within one fivethousandth,
and at the lowest pressure, to within */,,,,'" of the value of pv4.

§ 6. Calculation and Results. The quantities of gas were always
expressed in terms of the normal volume. For this purpose equation
I of Comm. N°. 127a was used:

pv Asoo’ = 1.07258 + 0.000667 d4a00c.

Using, where necessary, an approximate temperature as a correc-
tion factor for the piezometer, the measurements vielded values of
d4, the density of the gas in the piezometer under the observed
pressure. The temperature of the gas in the piezometer for each
series was obtained from the pv 4 itself for that particular series.
For that purpose values of Cy in

pra = Ag + Bad, + C4d4°
were used in the calculation which were obtained for each (at first
approximate) temperature from the special reduced equation of state
for hydrogen VIL. H,.3 given in Comm. N°. 109a@ equation (16)
which was deduced from the observations of KAMERLINGH ONNEs and
Braak and adjusted to a temperature of — 217°C. A4 and By
then follow from our observations and also pra at the same tem-

perature for the density of the gas in the hydrogen thermometer of
1100 mm. zero pressure. From this with

(pra )is == (pr), (1— 0.0036627 ¢t,)
we finally obtain the temperature on our hydrogen thermometer of
1100 min. zero pressure.

The temperatures obtained in this way yield a calibration on the
hydrogen seale of the resistance thermometer whose readings serve
as a guide to the regulation of the temperature of the bath. This
resistance thermometer was also calibrated with the hydrogen ther-
mometer independently. The two calibrations are not quite in agree-
ment. A subsequent paper by Kamertinca Onnes and Horst will
return to the question of this difference.

We obtained (where ¢, is the temperature on our hydrogen ther-
mometer of zero pressure 1100 mm.):

—
ee ee

bn ee ad

415

TABLE I. Hg. Values of pv 4:

Series NO, f ? d4 pv, O=6

S
I. I 0.34786 | 4.7568 0.073129
| 23 and 29 June 1911 \- 252° .63
| 2 0.60358 8.4597 | 0.071348
‘ 1 0.10964 | 1.6918 | 0.064216
2 | 0.20672 | 3.2560 | 0.063469 0.000031
24 June
3 |}—255°.46 0.27759 | 4.4133 | 0.062898 0.000012
8 and 14 July 1911
4 0.31318 | 5.0026 | 0.062603 0.000008
5 0.31294 4.9992 | 0.062598

Il.

| | 0.06698 | 1.1582 0.507834
14 and 18 July 1911 — 257° . 26
2

0.13153 2.3031 | 0.057104

The second series was represented by
pva = 0,065043 — 0,00489 dy + Cada?
deduced from Nos. 1 and 5, with (4 as before, and the column
O—C€ gives the differences between observation and calculation. These
differences are smaller than those corresponding to the observed
‘temperature fluctuations of the bath (see §4), which is in agreement
with the assumption that it is the mean temperature of the bath
which must be taken as the temperature of the gas in the piezo-
meter. This series also supports the use of the assumed C4. Series
I and III, lacking the controls possessed by series II in itself, ave
less reliable. Various circumstances have obliged us to postpone our

| TABLE IL
| Hy. Individual virial coefficients B ,

|
| for hydrogen vapour

fs B At
= 2522.65 0.000481
— 255°.46 0.000489

— 257°.26 0.000638

416

experiments for some time to come, so that for the temperatures of ‘
series IT and Lil we have not been able to give such extensive series
of measurements as in series II. ]

From Table I we finally obtain Table I (see p. 415)

§ 7. Smoothed values of the virial coeffpcents, and corrections of
the international hydrogen thermometer to the absolute scale.

-These corrections are to be determined from the virial coefficients
By by the method employed by KamertincH Onnes and Braak in
Comm. N°. 1014. For this, however, it is desirable to use smoothed
values. This was tried by plotting log 6 as a funetion of log 7.
Taking account of the accuracy of the various measurements there
seemed to be much to recommend the smoothing given in Table III
in which the temperatures O=T —213:09" are given in’ KELVIN
degrees, Table IV having been used for the calculation).

TABLE Il.
H,. Smoothed virial coefficients

}
|
|

' B , for hydrogen vapour.
6 l= a
— 252°.47 — 0.00047
— 255°.32 — ().00049
— 257°.10 — 0.00055

In Table IV these values of B47 have been used to supplement by data
for —— 252° C., — 255° C. and —=257-° Co the lisk given in Comer
N°. 1014 of experimental corrections Af;—= 6 — ¢; of the international
hydrogen thermometer to the absolute scale.

TABLE IV.

Corrections of the international
hydrogen thermometer to the
absolute scale.

t; ft, in degrees K.
— 252°.59 C. | +0.118
— 255°.45 + 0.125
— 2579.24 | + 0.144

417

Physics. — “On the second virial coefficient for di-atomic gases’.
By Dr. W. H. Krrsom. Supplement N°. 25 to the Communications
from the Physical Laboratory at Leiden. (Communicated by
Prof. H. KAMpRIINGH ONNEs).

§ 1. Jntroduction. Synopsis of the more important results. In
Supplements N°. 24a (§ 1) and 4 (§ 6), in which the second virial
coefficient was deduced from different particular assumptions concern-
ing the structure and action of the molecule, a comparison was
contemplated between the results then obtained and such experi-
mental data as are at present available. The present paper will
discuss some results obtained by carrying out such a comparison in
the case of di-atomic gases. The importance of such a comparison,
as well as of a comparison of the second virial coefficients for
various gases, especially for di- and mon-atomic gases, from the point
of view of the law of corresponding states, was emphasized in
Comm. N°. 127c, § 1 (these Proceedings p. 405). That such a comparison
can now be made with any fruitful result is due to the extensive
series of accurate isotherm determinations made by KAMERLINGH ONNES
and his collaborators, Braak, Crommenin, and W. J. pr Haas.

In the present investigation a beginning is made with the di-atomic
gases, especially with hydrogen, for these reasons: In the first place
the most immediately indicated simplified hypothesis that can be made
concerning the genesis of molecular attraction and can give any
hope of agreement with experimental results’) is that first intro-
duced by Remnecanum, which represents it as originating in the mutual
electrostatic action of doublets of constant moment immovably attached
to the molecules at their centres; this, together with the assumption
that the molecules collide as if they were rigid spheres of central
symmetry, leads to a value of the specific heat which agrees most
closely with that of the di-atomic gases dissociating with difficulty at
ordinary temperature; for these gases a law of dependence of /:
upon the temperature quite definite, and therefore ready to be tested,
was deduced in Suppl. N°. 246 §6 from the above assumptions. In
the second place, values of 4 for hydrogen are known over a much
more extensive temperature range than for any other gas with the

") See M. Rermyaanum, Ann. d. Phys. (4) 38 (1912), p. 649 for the rejection of
the explanation of molecular attraction by gravitation, or (at least of the total
molecular attraction, cf. p. 429 note 2) by the magnetic aclion of series of tnag-
netons assumed to be present in the molecules of paramagnetic and ferromagnetic

substances.

418

exception of helium, but for helium values of 6 for temperatures
below the Boy1x point are still comparatively uncertain.

The most important results yielded by the present investigation
ean be summarised as follows. The experimental results concerning
the second virial coefficient for hydrogen above — 100° C. (the
observations reaching + 100° C.) are consistent with the above
assumptions of Suppl. N°. 24h § 6 (rigid spheres with constant
doublets’. Below — 100° C. hydrogen exhibits deviations from this
behaviour which finally become considerable. Below the Boyze point
(the corresponding region of observation is from — 180° C. to — 230° C.
for H,) hydrogen is found to correspond with argon, and also with
helium in so far as the experimental data for helium at: present
available allow of any definite conclusion. It appears therefore that
between — 100° C. and — 230° C., as far as B is concerned the
thermal behaviour of hydrogen also approaches that of a monatomic
substance and eventually becomes the same, as was found by EvckEn’)
tobe the case with its caloric behaviour. This conclusion is supported
by the results for the coefficient of viscosity.

It was also found that, as far as the second virial coefficient is
concerned, the thermal behaviour of oxygen between 0° and 200° C.,
as deduced from AMAGAT’s observations®) corresponds with that ofa
system of rigid spheres of central symmetry, each with a doublet of
constant moment at its centre.

For nitrogen, on the other hand, within the same temperature
region (0° to 200° C., Amacat’s observations) important deviations
were found from the behaviour of rigid spheres of central structure
each with an electric doublet of constant moment at its centre. With
nitrogen in that temperature region, the dependence of 4 upon the
temperature corresponds to that dedueed from the assumption that
the vAN pEeR Waats quantities aw and by are constant (Suppl.
N°. 24a § 3); but then, however, the values given by BEsTELMEYER
and Varentiner for 6 from 81° to 85° K. differ greatly from this.

§ 2. Method. Logarithmic diagrams were employed for the com-
parison of the experimental values of 6 with those deduced in
Suppl. N°. 24 from various assumptions (ef. Suppl. N°. 23, Math. -
Enc. V 10, Nr. 38a). For this purpose log by was plotted as a
function of log 7 upon transparent squared paper to a_ scale of
1 mm. = 0,005. Here, following Suppl. N°. 23, Ly represents the

*) A. EuckEN. Berlin Sitz.-Ber., Febr. 1912, p. 141.

*) Cf. p. 428 note 1.

419

second virial coefficient when the empirical equation of state is written
in the form:
Cx . Dx Ey Ix

By
aS 6

pun = Ay {1 + A Se
UN UN UN UN UN”

(1)

while the subscript j indicates that the volume is expressed in terms
of the normal volume as unit (ef. Suppl. N°. 23, Chapter on “Units’’)
Values of Ly were taken from the corresponding individual values
of Ly which were given in previous communications by KamErLINcH
Onnes, and by him in collaboration with Braak, with Crommenn, and
with W. J. pe Haas. As we must remember that the latter coefficients
Bs, belong to the empirical equation when written in the form of
equation (II) of Comm. N*. 71 (June ’01), and that the subscript
a bas there a meaning quite different from that attached to it in
Suppl. N°. 23, they will be in the sequel distinguished as 4+;
The reduction is then made by means of the relationship

250 es Se ee oe era)

It was first examined for each of the different gases if the tempe-
rature variation of 5 is in agreement with that deduced on the
assumption of rigid molecules (ef. Suppl. N°. 24a § 3 for spheres of
central structure, § 4 for ellipsoids, cf. also p. 255 note 1 of that
Suppl.) and van ber Waats attractive forces. This assumption gives

avN |
nc dae

(ef. Suppl. N°. 24a §3 equation (14)), where ayy, dwn and fy are

By = byn {! (3)

constants. For this investigation /, = log (1—r), in which po= ee :

. 2 bywNRxXT
is now plotted as a function of log on transparent squared paper
to the same scale as before. but log r is now taken as increasing
in the opposite direction to that in which log 7 increases in the
previous diagrams.

For comparison with the assumption that the molecules of a gas
behave as if they were rigid molecules of central structure each
with an electric doublet of constant moment at its centre, equation
(59) of Suppl. N°. 244 § 6 was written in the form:

29
55125

Here / and v have the same significance as in Suppl. N°. 244 $6,
and bywy.z is the factor which, for the units now employed, must

l ]
By = bwna {1 — = (Av)? — — (hv)* - LATE. Paes a C9)
: 15

1 4
replace the factor nT A, xo* of Suppl. N°. 24) § 6.

420

29 ; :
55195 cD ore Soe |
is now plotted as a function of log iv, where again log hv is taken
increasing in the direction opposite to that in which log 7’ increases
in the log By, log 7-graph. Where necessary in (5) terms up to and
including (hr)'* were used in the calculation.

As in Suppl. N°. 25 Nr. 38 (ef. note 399 of that Suppl.) where
the argument of the logarithm is negative, the absolute value of the
logarithm is plotted, and the corresponding portion of the curve is
marked by (7).

To ascertain if the experimental values of by correspond to one
or other of the equations (3) and (4), is now the same as trying if the
corresponding log Ly, log 7-curve can be made to coincide as a whole
or in part with the corresponding F,, logr, or F,, log hv-curve by
moving it over the other, keeping the coordinate axes of the two
graphs constantly parallel *).

‘ 1 1
Fy = log {1 — — (hv)? — a5 (Av)* —
v ‘

§ 3. Hydrogen. a. The individual virial coefficients for hydrogen
were taken from Comm. N°. 100a (Dee. ’07) table XXII and
from Comm. N°. 1004 (Dec. ‘O7) by Kamertinen Onnes and Braax
‘ef. Comm. N°. 1014 (Dec. ’07) table XXV for the reduetion of the
temperatures to the AvoGapro scale), and from Comm. N°. 127c (these
Proceedings) table IV by KamertincnH Onnes and W. J. pe Haas’).
6. On moving the log By, log T-diagram for hydrogen over the
log #,, log t-diagram, which I shall call in what follows the diagram
for ay and fw constant, it was evident that it was not possible to
get them to coincide over any extensive temperature region (see
fig. 1). From this it is again (ef. Suppl. N’. 23 Nr. 44 for the
general case) evident that constant values of aw and /yw cannot be
used to represent even the planetary gas state (which, cf. Comm.
N*. 127c, these Proceedings, § 1 by KamertincH Onnes and W. J. pr
Haas, can be more closely defined as that state in which only the
L-term is still of influence in the equation of state) for hydrogen,
over a temperature region of any appreciable extent.

One could now try to determine values of aw and bw which on
the assumption that ay and dy are constant over any limited region

') This method corresponds to the log B, dlog B/dlog T-method of Suppl. N°. 23
note 399.

*) The individual virial coefficients for hydrogen calculated from the observations
of AMaGat, and given in Comm. N'. 71, June ‘01, p. 143, do not agree sufficiently
with those given by the Leiden measurements and are therefore unsuitable for
extending the temperature variation of By to higher temperatures.

+21

of temperature for these regions would give by equation (3) values
of 6B in sufficiently good agreement with the experimental values ;
this is done by so moving the curves with respect to each other
that the curve joining the experimental points touches the /’,, log r-curve
within the limits of each particular region‘). In fig. 1 the one curve
is moved over the other so as to give agreement at the BoyLe-point *).

igo |

a7, 00 Hydrogen

Se A) £ by COMSt

|
|
|

D> | 1,5 2,0 | Stage

Ba ras 98-10 | fog t
Fig. 1.

In this the point log 7’7— 2,0, log by =6,5—-10 coincided with
the point log r=0,024, 7,—9,412—10. From this in conjunction with
Ayooc=Aa71)=0,99942*) we find awn = 0,473 .10-3 and dbwxy =

1) With these values of ay and bw we could, as in Suppl. No. 23 Nr. 38,
for each temperature determine values of the critical reduction quantities for the
planetary gas state of the substance under investigation, if we choose as standard
for comparison a fictitious substance whose ay and dy are assumed to be constant

*) One can easily see how the criterion of contact must be modified for this case.

3) In Comm. No. 100), Dec. ’07, 0.99924 is printed by mistake (as is at once
seen from the value of Baov7zi).

te
wo
ND

oho

He Sel: Micon ies

Ta
ND
=

arog age

Fig. 2.
1,224.10-°; these values, therefore, on the assumption that these
magnitudes are constant, will give the closest possible agreement
with the experimental thermal equation of state, at least for the
planetary gas state, at the particular temperature under consideration,
which is here found to be 106° K. *) ?).

1) The values of ax and Wwyyx given by Braak, Diss. Leiden 1908, p. 82 were
obtained by a method of calculation which is essentially the same as the log B,
| g C-nethod of Suppl. No. 23, Nr. 38, applied to the comparison of hydrogen with
a fictitious standard wilh constant ay and by. The difference between these and
the results obtained by the log 6, dlog B/d log 7-method here, show that
complete correspondence does not exist between hydrogen and the fictitious standard
with constant ay and by even over a limited temperature region, if one is not
confined to the planetary state.

*) The deduction of similar values of ay and by for other temperatures which
might be followed by the development of deviation functions as for instance
indicated in Suppl. No. 23, Nr. 88, was not made.

423

ce. On moving the log By, log T-diagram for H, over the /,,
log Av-diagram, which | shall refer to henceforth as the diagram
for constant doublets, it was found that comparatively good coinci-
dence was obtained at temperatures above the Boye point, see
Fig. 2. At temperatures below the Boyie point, differences, which
begin to be noticeable even at the point —164°C. still above the
BoyLE point, become very marked,.so that below a certain tempe-
rature not even local coincidence (contact between the two curves
ean be obtained.

If we look upon these differences at the lower temperatures as a
consequence of a deviation, which increases regularly towards those
temperatures, of the behaviour of the H,-molecules from that which
is assumed in the hypotheses from which the constant doublets
diagram is constructed, there is then reason for superposing the
diagrams in a manner slightly different from that shown in Fig. 2,
viz. so that the points indicating the highest ‘observed temperatures
should lie upon the curve of constant doublets. The log by, log 7-dia-
gram does then, in fact, exhibit a deviation from the constant
doublets diagram, increasing regularly towards the lower tempera-
tures, and already appreciable at — 139°C. At higher temperatures
as far as the observations extend, that is, up to 100° C., and taking
into account the accuracy with which 4 can be deduced from the
observations, we may say that as far as & is concerned the thermal
behaviour of hydrogen in the planetary gas state may be represented
by that of a system of rigid spheres of central structure, each with
an electric doublet of constant moment at its centre. The caloric
behaviour of H,, in which differences clearly occur earlier, is, to a
first approximation, consistent with this at the higher temperatures
of the region under consideration.

From this method of superposing the diagrams we may easily
deduce values of o, the diameter of a molecule, and of v, the
potential energy (v being 0 for r=) of two molecules in contact,
when the axes of the doublets are respectively parallel and perpen-
dicular to the line joining the centres of the molecules (ef. Suppl.
N°’.. 245 § 6). On superposing them so that the H,-points for the
highest three temperatures fell upon the line for constant doublets,
then the point log hv = 0,2, /,—=9,7—10 coincided with the point
log T = 2,075, log By = 6,540—-10. From this, together with the value
kp = 1,21.10—'6 (Suppl. N°. 23, note 174) taken from Perrrin’s
observations we obtain

w = 2,28 -10—'4 [erg].
From this too, we get for four times the molecules own volume

424

ou the assumptions here made, expressed in terms of the normal
volume as unit, bwx, = 0.692 .10~%. This value, which can also be
regarded as to be obtained by extrapolation to very high temperatures,
is markedly smaller than the value obtained above on the assumption
that wy and dw may be regarded as constant over a small region of.
temperature, and it is also much smaller than that given by Braak,
Diss. p. 82 and 83. We shall return to the variation of dw with
the temperature when we come to consider the viscosity.

From yn we obtain the diameter of the molecule using the
relation
a Wine)
oy une

—_ e

bwWNo Anvoe Oy =

In this @y = 22413 |em*.)*) is the theoretical normal volume of
the gram molecule, and V = 6,85.10"* *) is the AvoGapro number.
We find

== 2,241.07 * ems:

From the values of wv and 6 we further obtain the moment of
the doublet

me = 4,96.10—'" [electrostatic unit. em. |].

Assuming that each pole bears a charge equal to that of a single
electron, the distance between the poles should be 1,17.10~—* em.’),
that is, about one twentieth of the diameter of a molecule; within
the interior of a molecule there is therefure plenty of room for such
a doublet. At the temperatures here considered the mean speeds of
rotation assumed by the molecules are such that the electromagnetic
force exerted by the molecules upon each other need not be taken
info account, and this confirms the assumption previously made

1) Cf. Suppl. N’. 23, note 23, and ‘Kinheiten” a.

2) Taken from Perrin’s researches; cf. Suppl. NY. 23, note 173.

3) From the energy required to ionise the gas RutHeRKoRD and Mc KLIne,
Physik. ZS. 2 (1900), p 53, obtained the same order of magnitude. So, too, did
REINGANUM, Physik. ZS. 2 (1900), p. 241, Ann. d. Phys. (4) 10 (1903), p. 334,
and loc. cit. p. 417 note 1, from the dependence of viscosity upon temperature
(cf. $6), from the tensile strength of metals, and from the latent heats of vapori-
sation of liquids, while the same order of magnitude for the moment of the mole-
cule was oblained by Desise, Physik. ZS. 13 (1912), p. 97, from the variation

with temperature of the dielectric constants of certain liquids.

425

(Suppl. N°. 244 § 6), that we need only allow for electrostatic forces. *)
Consideration of the viscosity lends some support to the result
obtained above that hydrogen behaves at higher temperatures in the
planetary gas state as a system of hard spheres of central symmetry,
each with an electric doublet at its centre, but deviating considerably
therefrom at lower temperatures. On this point we may refer to § 6.
d. Comparison of the log B, log 7-diagram for hydrogen with
that for argon affords an important insight into the behaviour of H,
below the BorLe point which is closely related to the deviation
found in ¢ fur the H, diagram from that for constant doublets*). The
individual virial coefficients for argon

{O58 sy _ aoe were taken from Comm. N°. 1184
ay? |O E _ (Dec. 1910) by Kamertinen Onnes and
Gee ~~ _— Crommeiin. From their measurements a
| | | | portion of the branch (7) of the log B,
— | Ee . log Y-curve lying below the Boye
o? 7 | | | point is accurately known.
L % — 1 On superposing the log By, log T-
| Pe | | curve for hydrogen on that for argon
[toe | 161 | it is evident that the latter quite well
U2 1 eae _ fits the corresponding part of the hy-
4 — | drogen curve, see Fig. 3°).
Oe From this it follows that, in so far
Be abydragen © as the second virial coefficient of the
6.8 AA Tego % thermal equation of state is concerned,
a ee eg! the thermal behaviour of hydrogen from
1,9 24 M&M __180° ©. to at least — 230° C. (the
Fig. 3. temperature for hydrogen which corre-

1) The length of the axis of a doublet may also be neglected in a first approx-
imation, as has always been done here. In a more accurate calculation, however,
this would have to be allowed for.

?) The deviations from the law of corresponding states occurring in B and C for
hydrogen when compared with their values for other substances, such as oxygen,
nitrogen, carbon dioxide, ether and isopentane, for which, as well as for hydrogen
at very high reduced temperatures, the mean reduced equation VII.1 (Suppl. N’. 19,
p. 18) holds, first found definite expression in the special equation VII.H,.3
(Comm. N°. 109a@ equ. (16)), which was introduced for this purpose; marked diffe -
rences occur between the 9% and © of this special equation and those of the mean
equation VII.1. The continuation of the investigation of the nature of these diffe-
rences which was commenced in Suppl. N’. 23, Nr. 38, was left to me by Prof.
KAMERLINGH ONNES.

3) Then the point log 7 = 2,4, log By =7,2—10 for argon coincided with the
point log T= 1,869, log By = 6,908 for hydrogen.

Proceedings Royal Acad. Amsterdam. Vol. XY.

426

sponds to the lowest observed argon temperature) corresponds to
that of a monatomic substance *)’).

In Nr. 38 of Suppl. N°. 23 hydrogen is compared with hélium.
From fig. 15 of that Suppl. it is evident that from the BoyLxe point
downwards good correspondence is obtained between He and H, in
so far as any conclusion is possible from the small number of helium
points which were available for the construction of that particular
branch of the log B, log Z7-curve*). To the figure just quoted we
may now add the helium point 4°,29 K. from Comm. N°. 119
March 1914) § 5, which, in that figure, comes above the argon-
hydrogen line. A suitable displacement *), however, of the helium
diagram brings this point (whose degree of accuracy, however, is
not so high as that of the points.forming the H,-A-curve), too, on
to the hydrogen-argon curve.

From fig. 16 of Suppl. N°. 23 one can see further that, when
superposing the hydrogen and helium curves so that the branches
below the Boyne point coincide, those above the Boy.r point deviate
markedly from each other, from the figure quoted and from the
table referring to it in note 399, that coincidence between the
branches above the BoyLe point can be obtained only over a very

limited region ®). So that at these higher temperatures appreciable

deviations from correspondence between He and H, exist. ~

1) The preliminary values of By obtained for helium in the corresponding region
-do not conflict with the suspicion that this is the case down to much lower
temperatures (see @).

2) From the data given on p. 425 note 3 for the sigacernent necessary to
obtain coincidence between the A-curve and the H,-curve, and from the value
T;; =.150.65 for argon (C. A. GromMELIN, Comm. N° 115, May 1910), we can
calculate Ty... 4) = 25,25 for the critical reduction temperature for hydrogen
with respect to argon as standard for comparison (cf. Suppl. No. 23, Nr. 38D).
pe ae with the eritical temperature for hydrogen on the one side, with
Tx (Hy :No,0,) = 48 (Suppl. No. 23 note 399) on the other side leads to the con-
fasion! that the virial coefficients for hydrogen and argon higher than the second
do not correspond perfectly, though the deviation from correspondence between
the two substances within the region of temperature under consideration is much
smaller than that between H, and Ny or Oy.

°) The third virial coefficient, C, then corresponds as well (see fig. quoted). In
good agreement with this is the finding of a constant value for Tyr (He:H,), 4!
the points ty, —=— 253° and — 259°, which does not differ much from TT. ic
(Suppl. No. 23 note 399).

‘) In this there is no longer any notice taken of the correspondence between
the C coefficients, as is also the case in the other diagrams discussed in the
present paper.

*) Comparison with fig. 15 shows that the third virial coefficient, C, would then
exhibit wide deviations from correspondence. ‘

Se ae

497

jf. If we combine the results obtained in d and e with those given
in c we reach the conclusion that, as far as BP is concerned, between
— 100°C. and —180°C. the thermal behaviour of hydrogen, which,
between — 100° C. and + 100° C. is that of a system of rigid
spheres of central structure each with an electric doublet of constant’
moment at its centre, and acting upon each other according to the
ordinary laws of mechanics and of the electromagnetic field, now
changes to that which characterises a monatomic substance, and that
between — 180° C. to at least — 230° C. this behaviour is completely
followed *). On this account we shall postpone further considerations
of the second virial coefficient for hydrogen in this region until
monatomic gases are discussed in a subsequent communication.

From the above it is accordingly evident that the thermal behaviour
of hydrogen exhibits a strict parallelism with its caloric behaviour
as deduced from Evckrn’s measurements of the specific heat at constant
volume. As we suspect, in accordance with the theories of Nrrnst’*)
and Erste *), that the decrease in the specific heat at lower
temperatures will find an explanation in the application of the
hypothesis of finite elements of action to the rotations of the mole-
cule, the parallelism here observed at once leads to the question
as to whether the explanation of the pecularities of the thermal
equation of state for hydrogen obtained in the present paper may
not profitably be sought in the same direction. For instance, one can
imagine that the hypothesis in question would lead to the assumption
that, on approaching one another, the molecules have not such
orientations and are not so distributed with respect to their mutual
distances, as is required by the laws of statistical mechanics according
to ordinary dynamics and electrodynamics, and that therefore the
mean attraction would be smaller at lower temperatures‘) than would
be the case if these laws were obeyed at these temperatures as well.

From the fact that 6 is negative at those temperatures at which the
di-atomic hydrogen begins to behave as a monatomic substance, and
that there is consequently some attraction still left which does not
decrease much more even with the temperature (cf. 4), it follows
that the quantum hypothesis applied to this region would not have

1) The temperature regions here given are not to be regarded as sharply bounded,
still less are they to be considered as sharply defined by the observations at
present available.

2) W. Nernst. ZS. f. Elektrochem. 17 (1911), p. 265.

8) A. Etnstetn. Discussions of the Sotvay Congress, Noy. 1911.

4) A similar diminution of the attraction was assumed in Comm. No. 119 in
order to explain the maximum observed in the density of helium.

428

to lead to a large decrease of the whole of the attraction, but only
to that of a part of it. This, then, would again lead to the hypothesis
that at higher temperatures only part of the attraction is to be
ascribed to the mutual action of the doublets of constant moment,
another part being ascribed to a mutual action of the molecules
corresponding to the mutual attraction of monatomic molecules (cf.
Suppl. N°. 23 Nr. 84d). The answer to the question as to whether
treatment on these lines would lead to a still better agreement with
observation than that obtained inc must, in the meantime, be postponed
till a later Communication.

§ 4. Oxygen*) The individual virial coefficients for oxygen were
taken from Comm. N°. 71, p. 143.

From Fig. 4 it is evident that the oxygen
points (90) lie well upon the curve (——) for
constant doublets, so that in this particular region
(0°—200° C.), as far as B is concerned, and sub-
ject to the reserve of note 1, the behaviour of
oxygen may be regarded as that of a system
of rigid spheres of central structure each with
a doublet of constant moment at its centre. From
the following data concerning the superposition
of the diagrams (ef § 3c) we obtain the accom-
panying results: the point log T = 2,6, log By =
= 6,5 —10 for oxygen coincides with the point
log hy = 0,204, #, = 9,628 — 10 on the curve
for constant doublets, hence :

» = 7,71.10—!4, bywno = 0,745.10-3, 6= 2,27.10-8, m = 94.

On the assumption that each of the poles of the doublet bears
a charge equal to that carried by a single electron, the length
of its axis should consequently be one tenth of the diameter of the
molecule. The oxygen molecule should accordingly be about as large
as the hydrogen molecule, but the moment of its doublet should
be about twice as great as that of the hydrogen doublet.

§ 5. Nitrogen’). The individual virial coeffcients deduced from

1) The lack of agreement between the observations of Kamerttnen Onnes and
Braak upon hydrogen and those of Amacat (cf. p. 420, note 2) shows how desi-
rable it is that new observations should extend our experimental data over a wider
range of temperature and give a control upon the values of B deduced from
Amacat’s data for oxygen and nitrogen as well as for hydrogen. In the meantime

429

AMAGAT’s observations covering the region 0° tot 200°C. were taken
from Comm. No. 71, p. 148. From the observations of BesteLMEYER
and VALENTINER*) it is possible to obtain still another value for By.

At T= 51,01 we get By .73) = — 3,411.10-*, from which with (2) By
follows.

Look Comparison of the nitrogen dia-

& | gram with the curve for constant

a sie | doublets and with the hydrogen

IO | diagram shows that nitrogen devia-

bo OO dbikragen tes markedly from the other two

5 — oH, € & cost especially in the neighbourhood of

28 | tne Boy.e-point *). Comparison with

| from AwaAGAT’s observations can be
| brought into pretty close agreement

at with the curve, while the point given
~#0 | re by BresteLMEyeR and VALENTINER lies
a= a then pretty far above it (see Fig. 5).

\ | In Fig. 5 the point
? log r= 0,004, 4, = 9,731—10

94 |? pire |
' coincides with the point
ot | log T = 2,5, log By = 7,05,

OL y : the curve for aw and bw constant
Ne shows that the four points taken
8

14 | from which we get, for the region

2A | fagAF covered by Amacat’s observations :
03 93425 awn = 2,44.10-3, bwn — 2,08.1 eee
Fig. 5

§ 6. Coefficient of viscosity *). It seemed of importance to inves-
tigate whether the results obtained in § 3 find confirmation or not
in the manner in which the coefficient of viscosity varies with the
temperature. The second column of the following Table, which, on

it appeared not quite devoid of interest to utilise the data at present available
for these two gases subject to such reserve as may be necessitated by future
control and extension, for comparing with the results of Suppl. N°. 24.

1) A. BesTELMEYER and S. Vatentiner. Ann. d. Phys. (4) 15 (1904), p. 72.

2) The different behaviours of N, and O, from the point of view of the law of
corresponding states was illustrated by the two corresponding Tables of Comm.
No. 71. The influence of the magnetic properties of oxygen will be investigated later.

3) An investigation of viscosity at low temperatures has been in progress at
Leiden for some time, Papers by KamerLincH Ones and DorsMan on the viscosity
of hydrogen and by KAMeRLINGH Onxes and S. Weser on helium will soon be
published.

430

the theory of rigid spheres without attraction, should show the
figure 1,000 at each temperature, gives results taken from the obser-
vations of Markowski') and of Kopscn?); in column 3, dw is the

3 RT
quantity which, multiplied by the factor > a> gives the collision
r Z v

virial; in accordance with the splitting indicated in Suppl. N°. 246

§ 6 of the whole virial of the mutual forces between the molecules

into the collision virial and the attraction virial, by o>c/bw is eal-
culated from *)

1 4 \ 1 I 1

bw 5 ty 18 }! ae af (ho)? + LE (hv)i + = g,(Av)*.. | bare

3 5

(for g,, 92... see Suppl. N°. 246 §6), or
29

pits
11025 “*”)

4 sy | 1 } ) 1 (1 43 8
-— XO + —(hv)?+—(Av)*+
EG aan 55 Lv) (8)

Although the theory of viscosity, and, in particular, of the
influence of molecular attraction upon it, is not yet sufficiently
worked out to draw quite certain conclusions therefrom, yet comparison
of these two columns seems to show that the behaviour of hydrogen
above O° C. is in pretty good agreement with that of a system. of
rigid spheres of central structere each with an electric doublet of

yj ga Troe bwooc
t | Nooc ? bw
hydrogen | const. doublets

184.2 1.108 1.104
100.5 1.058 1.074

0 1.000 1.000

— 78.73 0.940 0.865

— 194.9 0.827 0.236

constant moment at its centre, but that below O° C. it deviates con-
siderably therefrom. Comparison of hydrogen and argon shows that

') H. Marxowski. Ann. d. Phys. (4) 14 (1904), p. 742,

*) W. Kopscn. Diss. Halle 1909.

°) For the corresponding ay we obtain a series with only odd powers of hu
beginning with the first; the first term is consequently proportional to 7—! (ef.
Suppl. No. 23, Nr. 48c) while the subsequent terms become small with compa-
ralive rapidity. -

431

the viscosity of hydrogen at — 192°.7C. and that of argon at 0° C.
deviate from correspondence by only 6°/, (taking the coefficients of
similarity from §3 d), but that the viscosity of hydrogen from — 198° C.
upwards increases much more slowly with the temperature (corre-
sponding to a more rapid increase in the attraction in the case of
hydrogen within the region of transition) than corresponds to the
increase in the viscosity of argon. This confirms in some degree the
conclusions reached in § 3.

Contirmation would have been attained in a higher degree if
corresponding to § 4 agreement had been obtained between the
temperature variation of the viscosity of oxygen and by oo/bw as
given by (8), using the value of v obtained in § 4. This, however,
is not at all the case. That temperature variation can, indeed, as
far as observations’) go, be represented with the aid of bw! of
(ouut then =we find w= 2,79 .10—"* instead of the 7,71 .10—4
deduced in §4 from the coefficient 4. Unless the agreement obtained
in § 4 is wholly fortuitous we must conclude from this that a
deviation from the temperature variation of the viscosity of oxygen
as deduced upon the assumption of rigid spheres each with a constant
doublet at its centre is occasioned by some circumstance whose
influence upon / vanishes, or is at least extremely small. As such,
for instance, one could regard deviations from sphericity in the
molecular shape.

ait

1) By H. Marxowskl. p. 450, note 1. (The observations by E. V6LKER, Diss.
Halle 1910, on the coefficient of viscosity of O; down to — 152°.52 C., which
came to my notice only after the Dutch original of this paper was printed, join
those observations at 0’—14°.65 C. Below 0° C. they show a deviation from bw -!
for constant doublets in the same sense as that exhibited by Hy. At — 40° C.
this deviation is already distinct and it finally becomes very marked. (Added in the
English translation).

Pe Be Ae PA.

In the Proceedings of the meeting of June 29, 1912.
p. 258 |. 9 from the top: for micro-complexion read macro-com-
plexion,
peecot. |. 1 .,, », bottom: for w,,, —h{sg(r,)} read h fty,—3¢(7,)}.
Be260-1. 5 ,, i Set 108 Oo read ©.
meark bh 13; , bottom: for LBD read EBB’.

(October 24, 1912).

KONINKLIJKE AKADEMIE VAN WETENSCHAPPEN
TE AMSTERDAM.

PROCEEDINGS OF THE MEETING
of Saturday October 26, 1912.

———Doce-—

President: Prof. H. A. Lorentz.
Secretary: Prof. P. Zeeman.

(Translated from: Verslag van de gewone vergadering der Wis- en Natuurkundige
Afdeeling van Zaterdag 26 October 1912, Dl. XXI).

2 NN EEN ES:

3. R. Karz: “The antagonism between citrates and calciumsalts in milkcurdling by rennet.
A contribution to the knowledge of the relation between structure and biologics al action”.
(Ist Communication). (Communicated by Prof. A. F. Hortemay), p. 434.

J. R. Karz: “The law oe surface-adsorption and the potential of molecular attraction”. (Com-
municated by Prof. J. D. van DER Waats), p. 445. ;

C. Braak: “The Boca between atmospheric’ pressure and rainfall in the East-Indian
Archipelago in connection with the 3,5 yearly barometric period”. (Communicated by Dr.
J. P. van DER Srok), p. 454. ;

L. Rutren: “On orbitoids of Sumba”. (Communicated by Prof. C. E. A. Wicumayy), p. 461.

-F. A. H. Scnrememakers and Miss W.C. pr Baar: “On the quaternary system KCI =CuGi i:
BaCl,—H.0”, p. 467.
F. A. H. Scmreremakers and_J. C. Tuoyxts: “The system HygCl, —CuCl.—H, 30”, p. 472.
W. Remspers and S. pe Lance: “The system Tin—TIodine” (Communicated by Prof. F.
H. ScureisEMAKERS,, p. 474.

W. Rempers and PD. Lery Jr: “The distribution of dyestutfs between two solvents. Con-

tribution to the theory of dyeing”. (Commnniecated by Prof. F. A. H. Scmremrmakrrs),
482. 7

Hk. op Vries: “On Ieee congruences and foeal systems deduced from a twisted eubic and
a twisted biqnadratic. curve’ [, p. 495.

C. van Wissetincu: “On the demonstration of carotino:ds in plants. First communication:
Separation of carotinoids in erystaliire form”. (Communicated by Prot. J. W. Morr) -p ol:

N. Scnertema: “Determination of the geographical latitude and jongitude of Mecca and
Jidda, accomplished in 1910-1911”. (Conminnic ated by Prof. I. F. van DE SANDE BAKHUYZEN,
Part I, p 527. (With 1 plate), Part II, p. 540, Part III, p. 556. (With 2 plates).

a i W. "ATEN: “On a new modification of sulphur”. (Commanic: ated by Prof. A. F. Hotr-
EEMAN), p. 572.

H. L. pe Leeuw: “On the relation between the sulphur modifications”. (Communicated by Prof.
A. F. HoLiteman), p. 584. ‘

A. F. Hotreman and J. P. Wisact: “On the nitration of the chlorotoluenes’’, p. 594.

P. Zeeman: “On the polarisation impressed upon light by traversing the slit of a spectroscope
and some e:zrors resulting therefrom’’, p. 599.

J. D. vaN DER WaaLs: “Contributioa to the theory of binary systems. XXI. The condition
for the existence of minimum critical temperature”, p. 602.

J. J. van Laar: “The calculation of the thermodynamic potential of mixtures, when a com-
bination can take place between the componenis”. (Communicated by Prof. H. A. Lore NTZ),
p- 614.

J. W. Mort and H. H. Janssonivs: “The Linnean method of describing anatomical structures
Some remarks concerning the paper of Mrs. Dr. Marie C. Stores, entitled: Petrifactions
of the earliest European Angiosperms’, p. 620

(©. E1gkmayn: “On the reaction velocity of micro-organisms”, p. 629.

‘Vv. H. Keresom: “On the second virial coefficient for monatomic gases, and for hydrogen
below the BoyLe-point’. (Communicated by Prof. H. KAMeruincn Onnes), p. €43.

Benct Beckman: “Qn the Harr effect, and the change in resistance in a magnetic field at
low temperatures. I!T. Measnrements at temperatures between + i7° C. and — 260° C.
of the Haut effect, and of the change in the resistance of metals and alloys ina magnetic
field”. (Communicated by Prof. H. KAwerimen Oxxes), p. 649. IV. Continuation! ), p- 659.

H. KameriixscH Oxnes and Bexner Beckman: “On the Hatr-effect and the change in
resistance in a magnetic field at low temperatures. V. Measurements on the Har “effect

= for alloys at the boiling point of hydrogen and at lower temperatures”, p. 664,

C. A. Crovmein: “On the triple point of methane”. (Communicated by Prot. H. Kameriincu
ONNES), p 666.

_E. Marutas, TL KaMERLINGH Onnes and C. A, Crommeriy: “On the rectilinear diameter for

argon’, p. 667.

Erratum, p. 673,

434

Biochemistry. — “The antagonism between citrates and caleiumsalts
in milkeurdling by rennet. A contribution to the knowledge
of the relation between structure and biological action’. + First
communication). By J. R. Karz. (Communicated by Prof.
A. F. Honiemay).

(Communicated in the meeting of April 26, 1912).
Introduction.

A small quantity of neutral citrates prevents the coagulation of
blood; various salts which precipitate calcium as an insoluble com-
pound, e.g. oxalates and fluorides, have an analogous action. The
peculiarity of the case is however that citrates do not precipitate
diluted solutions of calciumsalts, but remain entirely clear; notwith-
standing this, they have neutralized the effect of the calcium.

A similar antagonism between citrates and calcium has been found
in various biochemical and pharmacological processes.

Citrates in small quantity prevent the curdling of milk by rennet;
various immunochemical reactions are prevented by citrates, as the
laking of red bloodeorpuscles by animal hemolysines (eelserum
cobralecithide, normal complement); here also the action of citrates
is prevented by the addition of calciumsalt*).

Recently Prof. Hampurerr has shown that the phagocytic power
of the leucocytes is inhibited by citrates and is reactivated by calcium-
salts and that fluorides and oxalates too prevent phagocytosis.

The pharmacological action of citrates shows the same antagonism
with ecalciumsalts, e.g. JANUSHKE*) has found that the paralysis of the
heart and the paralysis of the nervous system caused by intravenous
injection of citrates, is removed by injection of calcium. Busg and
Pacnon *) showed, that there exists antagonism between the action
of citrates and calcium on the heartmuscle, and Mac Caio *)
observed that the purgative action of citrates is inhibited by addition
of calciumsalt.

It seems perfectly clear, that substances as fluorides and oxalates
which precipitate calcium as a nearly insoluble compound, are anta-
gonists of calcium, but how shall we explain, that citrates have the
same action, although they do not precipitate calciumsalt?

As this property of citrates is used more and more in hema-

‘) Genaou, Arch. Intern. de Physiologie 7 (1903).

9) Arch. f. Exper. Pathol. u. Pharmak. 61. p. 8363—875.

8) C. R. 148 p. 575—578.

*) Americ. Journ. of Physiol. 10, p. 101—110.

435

tological and immunochemical reactions, it has drawn attention from
various sides. Sappatant') thinks, that ifs aetion might be cansed by
the diminution of the number of free calciumions; Artuus *) and
Gerncou *) showed, that citrates have an antifloceulant action on finely
divided suspensions, and asked whether the biological action should
not rather be attributed to the latter. Finally M. H. Fisener ‘)
proved recently that citrates inhibit to a large extent the swelling
(imbibition) of proteids by acids and by alkalis and that some phar-
macological properties of these salts (e.g. their influence on glaucoma)
are related to this. Each of these theories is supported by a number
of experiments; possibly all three contain a part of the truth; under
these circumstances a choice between the different explanations does
not seem possible as long as the biological action of citrates has
not been more extensively analysed.

Analysis of the biological action of citrates by comparison
with the action of substituted citrates.

For such an analysis the finding of the active groups in the citrate-
molecule seems particularly adapted. For it seems rather improbable
that the different actions of the citrates are all caused by the same
groups. Then this research will give an indication which actions can
be compared, which not.

In order to find which are these groups, I have followed the
ordinary pharmacological method. A number of derivatives of citric acid
were prepared in which the probably active groups were changed
in different ways. As all acids which precipitate calcium in the
manner of fluorides and oxalates inhibit the curdling of milk, this
secondary complication should be excluded. On this account | have
made a control with all acids examined in order to see if the
solution of the neutral salt of the acid used, precipitated a diluted
solution of calciumsalt. Only those, which did not were used for
the investigation. As solution of calciumsalt I chose a solution of
gypsum (saturated solution, diluted 1:5 with distilled water).

OH COOH

a ei aN .
Citric acid, COOH .CH,.C.CH, . COOH, contains 4 groups whieh
may be considered as the active ones: three carboxylgroups COOH
and one aleoholgroup OH. The hydroxylgroup can be made inactive

1) Atti della R. Acad. di Torino 36, p. 27—53; Memorie [2] 52, p. 213—257,
2) C. R. Soc. de Biol. 36 (1901).
S) 1,7 @
+) Das Oedem.
29*

436

by acetylation; of the carboxylgroups one, two, or three can be
removed by preparing the mono-, di- and tri-amides, or mono-, di-
and tri-esters *).

a. The alcoholgroup made inactive.

C,H,O, COOH

The acetyleitric acid COOH. ee COOH
Anhydrous citric acid was boiled with acetylehloride ae-
cording to EastTerreLp and Sexi ?); the acetylcitric anhydride
formed is purified by washing with acetylchlovide and dried
in the exsiceator above sodium hydroxide. Immediately before
use, this substance was recrystallised with chloroform until
it had the exact melting-point. A weighed quantity of this
substance was dissolved in water of 50° C., when the anhy-
dride changes into acetyleitric acid, and then was neutralized
with titrated sodium hydroxide solution. Three equivalents of
sodium hydroxide were used pro molecule acetyl-citrie an-
hydride, as should be the ease when no acetie acid is split
off. Such a solution is relatively very stable at ordinary
temperature and only becomes acid after several weeks (by
breaking up into acetic acid and citric acid).
When the alcohol-group of citric acid is made inactive, the substance
has become comparable with other miulti-basic aliphatical acids
without alcohol group. It therefore is interesting to compare some
of these acids with acetyleitric acid as to their action on milk-
curdling *).
For comparison were chosen :
COOH
aconitic acid COOH. CH, dj = CH SO0GH
Purity controlled by melting point.

COOH COOH

isoallylentetracarbonic acid COOH . CH, .C .CH,COOH.
The tetra-ethylester of this acid was prepared by conden-
sation of malonic ester with 2 molecules of monochlor-acetic-

') 1 am indebted to Dr. J. Branxsma for his amiable advice in synthetical
difficulties.

*) Journ. of the Chem. Soc. 61, p. 1003—1012.

*) In order to prevent secondary cemplications | have for comparison chosen
acids which differ as litthe as possible in structure from the original ones Acids
in which the carboxylgroups are nearer to one another than in the citric acid-
molecule were excluded, because in such cases other properties so often appear.

acid ester. This tetra-ethylester was saponified in alcoholic
solution according to the method of Biscnorr '); addition of
BaCl, precipitated the bariumsalt. This starchy looking salt
could not be sucked dry; it was purified by repeated decan-
tation. The free acid was prepared by adding the calculated

* quantity of- sulphuric acid; if was extracted with ether and
recrystallised with anhydrous ether until it had the right
melting-point (this never was quite exact because of the
decomposition on melting). :

H COOH

; saa hotae ee
tricarballylic acid COOH .CH,.C.CH, .COOH

b. one carboxrylgroup made inactive.

OH CONH,

Symmetrical citric monoamide COOH . CH, . C. CH, .COOH.

To pure acetondicabonicacid-diethylester prussic acid was
added in statu nascendi; the cyanhydrine was saponified with
strong sulphuric-acid, after dilution of the H,SO, with ice
the diethylester of monoamide-citric acid was extracted with
chloroform. This was purified by pressing between unglazed
porcelain plates, dissolving in chloroform and precipitating with
ligroine, until it had the required melting point and was
colourless.

To a weighed quantity of this substance a small excess of
normal sodium hydroxide solution was added; after 24 hours only
the 2 estergroups were saponified as was proved by titration.
The amide is very resistant to diluted solutions of sodium
hydroxide at ordinary temperature’).

Such a substituted citrate, in which one carboxylgroup has been
made inactive, was compared with some acids with two carboxyl-
groups and one or more hydroxylgroups. As such were chosen:

OH
|

the malic acid COOH. CH. CH, . COOH
OH OH

the tartaric acid COOH .CH .CH . COOH
OH OH OH

the trioeygqlutaric acid COOH. CH. CH. CH. COOH.

1) Lieb. Ann. 214, p. 61— 67.
?) Scuroeter, Berl. Ber. 38, p. 3199.

438

Pure arabinose, prepared from arabinose was oxydised at
35° C for 24 hours with 24 parts of nitrie acid (spec. grav.
1,2). The superfluous HNO, was removed in the waterbath
and the residue dissolved in 25 parts of water. This liquid
was saturated at its boiling temperature with calciumcarbonate
and filtrated while hot. The calciumsalt separated on cooling.
The potassiumsalt was formed by adding the calculated quantity
of potassiumearbonate, decoloured with animal charcoal and
purified by recrystallisation. As the calciumsalt is soluble only
to a small extent, the acid could only be used in diluted
dilution’).

c. The alcoholyroup and one carboxylgroup made tmactive.
CH,—O

Real
0 C=O

The methylencitrie acid COOH .CH, an . COOH.
Methylencitrie acid is formed by treating citric acid with

formaldehyde and separating from the unchanged citric acid.
I was presented with this substance in a very pure condition
(as neutral sodiumsalt) freshly prepared by the Pharmaceutical
Laboratory of the Elberfelder Farbenfabriken (Bayer)’).

This compound was compared with some other dibasic acids

without alcoholgroup :

succiuc acid COOH.CH,.CH,COOH.

glutaric acid COOH.CH,.CH,.CH,COOH

pimilinic acid COOH (CH,),-COOH.

suberic acid COOH.(CH,),.COOH.

d. two or three carboxylyroups made inactive.
OH COOH

Symmetric citric acid dimethylester GOODE. CH. CH COOH
100 er. of citric acid were dissolved in 500 gr. methyl-
alcohol and boiled for one hour after addition of 4 er. H,SO,;
this mixture was diluted with limewater, neutralized with
CaCO, and filtered. The filtrate was concentrated in vacuo.
After addition of HCl. the ester crystallized and was recry-
stallized from water. Melting-point (not very sharp) 125-127° C.’).

') Kiurant, Berl. Ber. 2), p. 3007.

°) | am = sincerely indebted to the Elberfelder Farbenfabriken for this kindness.
*) SCHROETER Berl. Ber. 35, p. 20586.

rae

439
OH COOH

Citrodiamide (symmetric 7) CONH,.CH,.C.CH,,CONH,,.

The motherliquor of the citramide (see below) was acidified
with nitric acid and precipitated with alcohol. The citrodiamide
is gained as a white crystalline powder'). Usually the
compound is mixed with its ammoniumsalt.

OH COOCH,
SS
Citric acid trimethylester . COOCH,.CH,.C.CH,.COOCH,,.

One part of citric acid was dissolved in one part of methy|
alcohol and the solution saturated with HCl-gas. On cooling
the ester crystallized and was purified by recrystallizing from
methylalcohol. Purity controlled by melting-point. °

OH CONH,

Citramide COON ee ea
Citric trimethylester was dissolved in 5 parts of strong ammonia
(spec. grav. 0.88); soon the citramide precipitated and was
recrystallized from water’).
Diethylester of monoamide-citric acid
OH CONH,

BoC HACE fen.coben,
preparation described on page 437: purity controlled by
melting-point.

The action of these substituted citrates was compared with the
action of other organic compounds, having none or only one car-
boxyl group, but one or more hydroxylgroups.

We choose for comparison :

CH OH
; :

monoethylester of tartaric acid COOC,H, . CH . CH. COOH

preparation of MERcK.

isoamylalcohol CH, .

CH, . CH, . CHOH
ue

CH,
1) When no erystals of this substance are obtainable, it may last months before
crystallization begins.

*) BeEdRMANN und Hormany, Berl. Ber. 17, p. 2684.

440
glycerine CH,OH . CHOH .-CH,OH
erythrite CH,OH .CHOH CHOH CH On
mannite CH OH. (CHO) — CEZ0H
glucose CH,OH . (CHOH), .COH

Injluence of substituted citrates on curdling by rennet.

It seemed natural to begin the investigation with that bioche-
mical or pharmacological process, the nature of which seemed mosi
simple and by which the smallest number of complicating circum-
stances might be expected.

To begin with, pharmacological actions may be excluded. For,
an intravenously injected substance only acts after having been
taken up by the tissues; the really acting concentration therefore
is not only determined by the injected quantity (calculated pro kilo-
gram of bodyweight) buc also by the partition-coéfficient tissae-blood,
which is very different for different substances.

The same difficulty complicates the investigation of immunity
reactions; here also the partition-coefficient leucocytes-serum or
erythrocytes-serum varies considerably for various substances.

Zemains the coagulation of blood and milk-curdling by rennet.
Milkcurdling seems to be a so much simpler process than blood-
eurdling, the substances one has to work with, so much more
stable, that milkcurdling seems to be the natural process to begin
with. It is my intention to study later immunochemical and phar-
macological processes with this method.

In order to find the influence of citrates on the curdling of milk,
I first observed how much the curdling-time was lengthened after
addition of increased quantities of neutral citrate of sodium. I prepared
a‘/,, normal solution of sodiumeitrate, to which 2 drops of litmus-
tincture were added and which by addition of a few drops of dilute
hydrochloric acid or sodium hydroxide were brought to the same
colour as distilled water witb the same quantity of this indicator.
140 normal solution obtained in this way, was diluted to an 1/80
N, 1/100 N, 1/200 N, 1/500 N and 1/1000 N. I convinced myself
that all these solutions remained neutral.

In order to determine the curdling-time, 10 cc. of raw milk were
pipetted into a test-tube, 2 ce. of distilled water, resp. a solution of
citrate .of different streneth, were added, the test-tube was closed
with a cork or a stopper of cotton-wool, well mixed and placed ina
waterbath of 37° C. until it had reached this temperature. Then
0.5 ce. of a solution of commercial rennet in distilled water (1 : 17)

441

-was added with a pipet, the contents of the test-tube quickly rever-

sed several times and again put into the waterbath. By carefully
moving the test-tube from time to time, the moment when the milk
became thicker, could be observed. When this change began, eurd-
ling was very near. The test-tube then was taken out of the water-
bath and carefully inclined, so that some of the contents slowly
moved along its wails, till at a certain moment floccules of about
‘4, m.m. suddenly appeared in the milk which adhered at its walls.
This point was taken as the curdling-point. “As milk-curdling is
delayed by shaking and by cooling, care was taken to avoid all
unnecessary movement and cooling. With some practise it is easy
to reduce both factors to a minimum and then the curdling-time can
be accurately determined. In the case of milk without citrate, the
curdling-time seldom varied more than 15 seconds Gn a curdling-
time of 2*/, minute); usually the observations differed less. After
adding salts which only give asmail delay, analogous differences were
obtained ; in the case of strongly delaying salts, the differences were
somewhat larger, but always agreed sufficiently. Every curdling-time
was determined in duplo or in triplo and the exact values found
by taking the average. Curdling-times of more than 2 hours cannot
be trusted because of the possibility of bacterial action.

It was found, that the kind of milk invesligated on subsequent
days with the same solution of rennet (1:17) gave curdling-times
which varied little. In order to make observations on different days
as well comparable as possible, the solution of rennet was aiways
taken somewhat more or less diluted till a curdling-time of 2 minutes
18 seconds exactly was obtained, this being the value on the first day.

The lengthening of curdling-time found when the milk contained °
the quantities of citrate given below, is seen from the following

figures :

O.QO016 N delay 17 séeonds |) 0.0020 N delay 289 seconds
0.00032 N 4 5 Sis 0.0030 N ao 27 min.(27')
0.0008 N ¥ 105 .,, |0.0040N 4 BE: us

0.0016 N ‘025 ee 0.0080 N e 9 hours.

These figures give the following curve (see p. 442).

Which is the best concentration to compare citrates with the
substituted products’ When the- concentration is sufficiently large
all salts inhibit milk-curdling. The characteristic of citrate-action is
the fact that curdling is prevented in concenivations in which other
salts give a scarcely perceptible delay. In general therefore the
results of the comparative investigation will be the more correct,

449

the smaller the concentrations used. On the other hand the difficulty
of accurately determining very small lengthenings of curdling-time,

min.

citrate-concentration
0.001 0.002 0.003 0.004

‘forms another limit. The best concentrations proved to be 1/125 N
and 1/25N; citrates in this concentration practically inhibit milk-
curdling, while indifferent salts as sodium chloride, sodium formiate
among others show none or very little influence.

In order to find the influence of salt on milk-curdling, 1/80 gram-
molecule‘) of the acid was neutralized with titrated natron, with
addition of two drups of litmustincture till the colour was the same
as distilled water with the same quantity of indicator.

Then the volume was brought to 50 ee. with distilled water. In
this way a neutral solution was obtained, containing '/, grammolecule
of neutral salt per liter. In the same way or by diluting the */, N.
solution '/,, N. solution of the neutral salts was obtained.

The curdling-time was determined as described above; only 2 e.e.
of the salt was added instead of the 2 cc. of distilled water. After

') Not 1/80 equivalent, but 1/80 molecule; therefore of a tribasical acid with

mol. weight 200 gr. were dissolved.
SU

445

all had been mixed and brought to the right temperature, again

*/, ec. of diluted rennet was added. ')

I found the following lengthenings of curdling-time :

a. The alcoholygroup made inactive.

Acetyleitrie acid 5 ae

compared with

Aconitic acid fers
1/

Tricarballylic acid

125
Isoallylentetracarbonie acid ‘/,,.

N 3'/,’ + N qi Ki
N 2*/,' fon N G/

T raat ae 1/ T Q3/ /
N 2/ oN 99/.
7 y/ 1 Ty Qi /
5 bs | ss ~ a) IE

b. One Carhoxylyroup made inactive.

Symmetric citricacid-

monoamide rf oes a Ss wha od Beare
compared with
Malic acid of oe Sag i Be wy aes Sea
Tartaric acid apres i Se aay ie a 3 (ep
Trioxyglutaric acid Peicn 1 Sie. t= 2)
ce. The alcoholgroup and one carbouylgroup made inactive.
Methylencitric acid Bee oN ()’ oy Be | the
compared with
Suecinic acid SN ()’ Wee | i
Glutarie acid ee ()’ py eves i
Pimilinic acid RAN ()’ "cg i os es
Suberic acid Deo IN ()’ ) for te. SNS
d. two or more carboxrylgroups made inactive.
Citric acid dimethylester '*/,,, N ()’ of eee 3 Ba ot
Citrodiamide 5 P| of eaten i
Curie acid trimethylester:.*/;,, N —*/,’ ‘/,,N-°- —%)
Citramide eed» ()’ of eg feat
Diaethylester of the

citric acid-monoamide heer N ()’ yep ap.| 5

compared with :

Monoaethy lester of

tartaric acid of See “3 pre. gh
Isoamy laleohol maze IN ()’ S| one cis
Glycerine ese ee ()’ a ee | ()’
Erythrite = cae | ()’ yas ()
Mannite fae. () 14, N —7/,'
Glucose soit OF YR 0)’

1) I am indebted to Mr. Ross van
of the investigation.
2) Not examined because of the small

Lennep for his valuable help in this part

solubility of the calciumsalt.

5) Not sufficiently soluble to be examined in this concentration.

444

When we consider that the unchanged citrate both in */,,, and
in */,, N solution delays the curdling more than 2 hours, it appears
from the above table, that the action of citrate is very much weakened
as soon as we substitute one of the active groups of the citricacid-
molecule, that it totally stops as soon as we make 2 or 3 groups
inactive. In the case of tartaric salts we find the same influence of
eroups ; when the aleoholgroups are made inactive (by acetylation)
or one of the carboxylgroups (by esterification), the inhibiting action
has disappeared (has fallen to the order of magnitude of all kinds
of indifferent substances as is shown by the following figures}.

When one group which is substituted, is an alcoholgroup, we-get
a delay of 3'/,’ with an '/,,, N and of 9°/,’ with */,, N. It seems
very remarkable that the compared: 3-basie acids without aleohol-
group give ‘a delay of the same order of magnitude, viz. 24}—3’
with. */,,, N and 9*/,—-37/, with */,5 0

When, the one group that has been substituted, is a carboxyl
group, we get a delay of 17/,’ with */,,, N and of 6°/,’ with */,,; N.
while with the bibasic acids compared, with 2 carboxylgroups and
1 or more alcoholgroups, these figures are 1—1'/,’ with */,,, N and
6—6'/,’ with */:, N. Here also we find a remarkable agreement.

When 2 or more of the active groups of the citrates are taken
away, the lengthening of curdling-time diminisbes to O a */,’ with
1/4, N and 7/, a I'/,’ with */,, N, figures which can be obtamed
also with the compared substances but are in the same order of
magnitude as with various indifferent salts. It is therefore better to
say, | think, that when 1 or more groups are taken away, the
characteristic action of citrate has quite disappeared.

We can get a better insight into the relations here described, if
we calculate what would be the concentration of citrate, necessary
to give the same lengthening of curdling-time as a substituted citrate.
For according to the figures on page 441 this lengthening increases
much faster than in proportion to the concentration.

We find then that a lengthening of curdling-time
of 9'/,—9/,’ corresponds with a citrate-concentration of 0.0023 N.
66” 0.0021 N.

” l4 re Ev) ” oe) ” ”

+) LY be) > ” 9 29 9 0.0003 RN:

We can state therefore, that the characteristic citrate-action 1s
diminished to about 6°/, of its original value, when one group has
been taken away and is diminished to about 1°/,, when two groups
are substituted. We have found, that an analogous influence on the
curdling-time belongs to all salts which possess either three carboxyl-

445

groups and one or more aleoholgroups. It is the combination in one
molecule of these two groups, which each delay curdling-time to a
certain extent, which increases this power in the case of citrates so
strongly (up to 16 times). It is remarkable that the alcoholgroup is
as much necessary for the citrate action, as the carboxylgroups.
Summer of 1911. Delft, Hygienic Laboratory of

PE At a ;
the Technical University.

Biochemistry. — ~The laws of surface-adsorption and the potential
of molecular attraction.” By J. R. Karz. (Communicated by
Prof. J. D. v. p. Waats). (Introduetion).

(Communicated in the meeting of June 1912).

Exclusion of secondary complications.
Surface-adsorption or adhesion plays an important part in biolo-
gical and biochemical processes, but very little is known of its laws.
Especialiy for the solving of some questions about swelling (imbibi-
tion) if is desirable to study this phenomenon more closely. There-

fore I have made — although the subject really belongs more to
physics than to biochemisiry — some researches which are only

intended as a first introduction to the study of this subjeet.

The confusion which is still reigning here, comes, I think, for a
large part from the fact, that two different things again and again
are mixed up: surface-adhesion at substances which have some
other action on the adsorbed fluid (formation af a solid solution, swelling,
formation of a chemical compound among others) and uncomplicated
surface-adsorption. Among the authors who in the course of the
19th century have studied surface-adsorption, not a single one seems
to have earried through this distinction as far as might be wished.
And even the two latest investigators of this subject, Trouron *) and
FREUNDLICH *), still treat the adsorption of water-vapour at glasswool
and the adsorption at cotton- or woolfibres, as the same phenome-
non; although glass does not take up water between its smallest
particles, whereas wool and cotton do this to such an extent that
the dimensions of the fibres become perceptibly larger (swelling).

Therefore 1 think it above all necessary in the experimental
study of surface-adsorption, fo choose a solid which has no action
on the fluid studied. | chuvose water as the fluid to be investigated,

1) Proc. Roy Soc. 77 (1906) en 79 (1907).
*) Kapillarchemie.

446

because of the facility with which its vapour-tensions can be deter-
mined with the method to be explained below.

Dr. Day, Director of the Geophysical Laboratory of the Carnegie
Institution in Washington, who has great experience of silicates, ad-
vised me to begin with synthetical quartz and synthetical anorthite
(Calciumaluminiumsilicate) as adsorbent solids, because these sub-
stances, when in mass, certainly do not take up water as a solid
solution and have very little inclination to react chemically with
water. Dr. Day had the kindness to have both substances prepared
for me in the most pure condition and to have them powdered in
a motor-driven agate-mortyr as finely as is possible. The material
then was sieved through the finest metal sieve (SO meshes pro centi-
meter). In this way the surface of the solid was made as large as
possibly can be attained; in this way the best chance was obtained that
sufficiently large quantities of adsorbed fluid could be observed in
the case of a solid substance which agrees as well as possible with
the above requirement.

In order to get an impression how finely divided the substances
were, I have suspended a weighed quantity in a known volume of
water and have determined with the counting-apparatus for blood-
corpuscles of Thoma, how many microscopically visible particles
this suspension contained pro m.m*. In this way it was found, that
1 mer. of quartz contains 140 million particles and I mer. of
anorthite 120 million. Extraordinarily finely divided powders therefore !

I have determined for both substances the amount of water adsor-
bed as a function of the vapourtension. Nine portions of this powder
of 1 to 2 er. each were carefully weighed in crystallizing dishes;
these were treated as described below, in order to bring them in
the same condition and then were placed above 9 different mixtures
of sulphuric acid and water, of which the vapourtension was known.
There they remained until constant weight. Ignition in a porcelain
erucible showed the amount of water contained in the material used.
Controls showed, that the adsorption at the surfaces of the dishes
was too small, compared with the adsorption at the surface of the
powder, to have influence of importance.

Injluence of the preliminary treatment of the powder: the
adsorbed layer consisting of vapour or of fluid.
Theoretically there exist two possibilities, when a vapour-condenses
on the surface of a solid. Hither it is condensed as vapour only, or
the layer of fluid is formed on the solid.

447

That indeed different curves are obtained in the case of a solid
which is covered with a thin laver of fluid or one by which this
layer has been removed by intensive drying, is shown by the expe-
riments of Trouton on the adsorption of water at glasswool *). When
the glasswool had been dried during 7O hours at 160°C) in vacuo
over phosphorpentoxide (so that we may presume that the adhering
waterlayer had been removed) curves were obtained as shown in
the subjoined figure. *)

: | Tes
}
Bd Fan i—y
sek 2 ie, oe) all pnt |
amie ie a orer a fe aoulcalca |
8 pt ————s pp =
Tey aol OE al ee ba
Aw Agim Bs iat os OF cae
$ hi i | ! | | | eh | |
bry iat eapensf eal sl 7 eel ee) ae] a Fs ij
j | fa } |
Jere ewer ee er ey
5 hi ae ae lta tos aL ee
| |
A SE SSS SSE iat Fi
| | | | | |
eee sina iey ET tL
pie mae
012345678901 23456789W1234567689WIZ345578SWI2Z3456
Feeds

Fig. 1.

The abscissae represent the amounts of water (in arbitrary units)
which are adsorbed at the surface of the glass, the ordinates represent
the vapourtension, which is in equilibrium with these. This curve was
obtained when going from the driest towards the moister side. The
curve rises quickly at the smaller values of the abscissae and
turns its concavity downward, then shows a very curious maximum
and minimum and finally quite continuously becomes a line, which
in the main seems to agree with the line obtained when a layer
of fluid water covers the surface of the glass.

Trouton has realised this last case only in an impure form, pro-
bably because he had to meet the difficulty, that in his experimental
technic the curves could only be followed from the driest to the
moister side. As driest substance he used glasswool dried at room-
temperature over phosphorpentoxide until the vapourtension just
had become zero. He then obtained the curve shown below. *)

1) Proc. Roy. Soc. 79, p. 383—390.
2) 1. c. p. 385.
8) l. c. p. 388,

448

This curve begins almost horizontally (the first one vertically !) and
then has its converity below; with larger abscissae it has its conca-
vity below.

The curve still shows however something like a maximum and —
a minimum. Trouton ascribes this to the fact, that a part of the
glasswool is really dry, which means in our conception that a part
of it has lost its adherent layer of fluid water. Two different pheno-
mena are thus measured t gether. ; *

It would be very interesting to know how the curve would be a
in the other extreme case, viz. when it is certain, that all the glass-_ ;
wool is covered with a layer of fluid water, because, as we shall
see, just in this case it can be predicted by approximate calculation ——
how the shape of the curve will be.

Description of my own experiments.

In order to be sure, that a layer of fluid water covers the par- {
ticles of the powder, weighed quantities of the powder were placed —
during several days in a bellglass above a 1°/, solution of sulphuric —
acid in water (vapourtension "*/,,, of the maximum tension of water)?). —
Then the dishes were placed over the different mixtures of acid- “¥
water till they were of constant weight, in a room which (situated
on the north and provided with double windows) had variations of
temperature as small as possible. ai
The following was found as the relation between vapourtension

') Pure water would have given too irregular condensations. _ an

449

and quantity of adsorbed fluid (¢ being the quantity of gr. of water,
absorbed by 1 gr. of dry powder).

QUARTZ | ANORTHITE |
Pip, | ix 102 Pip. | id< 102 |
0 0 | o | 0
| 0.020 | 0.29 | 0.020 | 1.79
| 0.048 | 0.31 | 0.048 | 1.85
| 0.122 | 0.33 0.122 | 1.87
| 0.306 | 0.34 | 0.306 | 1.88
| 0.525 | 0.39 | | 0.525 | 1.89
| 0.718 | 0.40 os | 1.91 |
| 0.857 | 0.41 0.857 | 1.99
| 0.915 | 0.42 | 0.915 | 2.04
| 0.965 | 0.61 | 0.965 | 2.53

By graphical representation the following curves were obtained :

Pipo quartz Pipo anorthite
1.00 1.00

0.75 0.75

¥ 0-50 ¥ 0.50

OR25 - 0.25

E :

A 0.005 0.010 0.015 0.020 0.025
Both curves begin with a more or less horizontal part, then have
the convexity below, with larger 7 first have a flexible point, then
have the concavity below; they therefore have the shape of an S.,

Thermodynamical relation between vapourtension and potential
of molecular attraction.
Prof. vAN DER Waats now called my attention to the fact, that
in the following manner an approximate theory of the shape of this
30
Proceedings Royal Acad. Amsterdam. Vol. XY.

450

curve can be obtained. When a layer.of fluid covers the surface and
this is thick fenough for us to assign to it the properties of fluid
in mass, there exists a simple thermodynamical relation; at least
when there is a discontinous change in density of the layer of fluid
and of the coexisting vapour (which is allowed as a first approxi-
mation) and when we neglect the very small compressibility of
the water.

Then there exists for the vapourtension p, coexisting with fluid
water at a distance 7 from the solid wall, the relation:

RT nt =k
Po
where & is the potential of the attraction of the solid wall on a
distance /, p, the maximumtension of water at the absolute tempera-
ture 7, and R the constant of gases. °*)

If the potential of molecular attraction were known, it would be
possible to predict how the vapourtension, which is in equilibrium
with a layer of fluid of the thickness 7, depends on 7. And be-
cause the quantity of adsorbed water 7 (in gr. of water pro 1 gr.
of dry powder) is related to the surface O according to the formula

it would be known at the same time, how the quantity of adsor-
bed water depends on the vapourtension.

The potential function of Lord Rayiuien and Prof. vAN DER WAALS.

Prof. van pER Waats proposed, that [ should see how far we
come with the potential function, which Lord Rayneten and he had
adopted in course of their studies about capillarity. They assumed

1) This relation is easily deduced from the general property (VAN DER WAALS—
KounstammM, Lehrbuch der Thermodynamik I, p. 197) according to which in a
system, subjected to the action of external forces, the total potential of a sub-
stance possesses the same value through the entire system. When zp is the potential
of watervapour, »’ the density-potential of water in the point / (that means the value
which the potential of the water would have with the same density but without
external forces) and & the potential of the molecular forces at a distance /
at the solid wall, we have.

wtkau.

When the compressibility of water can be neglected, » = RTin po, while

# = RTin p. It follows from this, that

k= RTIn= ;

en hh a a hs

=
ee Se ee ae

in
. la

451

that the potential on a distance / from a plain surface (pro unit
of weight of adsorbed fluid) is represented by

where / is a large ‘positive constant and 4 is a number of the order
of magnitude of the diameter of one molecule.
This leads to the relation.

Rape = fe?
Pe
or
RT In * == =e a
Ps

Discussion of this function gives a curve which begins about hori-
zontally, having its convexity below, then gets a point of inflection;
with a still larger 7 if has its concavity downward, and_ finishes
about horizontally. So exactly what has been found experimentally.
On the relative values of the coefficients / and 4 it depends how
large the horizontal beginning will be. One could be in doubt
for a moment, whether the formula deduced for a plain surface is
valid for the particles of a powder. But as long as these particles
are large, compared with the molecular dimensions, an error is
made, which is not of importance. And how fine the powders of
Dr. Day may be, the diameter of the particles is always still large
compared with the diameter of a molecule.

Is it possible to determine from experiments on surface-adsorption
how the potential function of molecular forces
depends on distance?

Finally an interesting question. We have seen, that the vapour-
tension p and the potential of the molecular forces / (on a distance
/ from the glass-surface) are related to one another according to the
formula

k= RT In’.
Po
If the theory of Prof. vAN per Waats is really a sufficient approxi-
mation, then it will be possible to calculate £ from the measured
vapourtensions. So we get the relation between # and the adsorbed
quantity of water 7. We should like to know the manner in which
3U*

452

i. depends on distance. In order to calculate / from 7, we must
know the total surface of the powder. It is impossible to measure
this accurately, but where an estimate is sufficient, we can try to
calculate it from the number of particles pro mgr. as deseribed on
page 446.

We then assume, that the particles are spheres of equal dimensions
and must know the specific gravity of the sclids. In this way I have
found for the surface of 1 gr.

quartzpowder 3260 cm?
anorthitepowder 3150 cm?

In this way I have found for the relation between potential and
distance the following numbers (4 expressed in cal. pro mol. adsorbed
water) *):

water -quartz (Si O,) | water-anorthite (CaAl silicate)

=f i Lin10-cm.| —k a Lin 10-6 cm.
328 0.0031 0.95 =| 328 0.0185 5.87
228 0.0633 POT) 996 0.0187 5.94
128 0.0035 POT~ sl 4 28 0,0188 5.97
69.8 0.0039 Lisbon 0.0189 6.00
36.0 0.0040 Re eM oe 0.0191 6.06
16.7 0.0041 sy i 0.0199 6.32
9.62 0.0042 1.28-"|; 9162 0.0204 6.48

3.86 0.0061 1.86 | 3.86 0.0253 8.03

These tables represented graphically, give the figures shown below;
it is, I believe, the first time, that it has been tried to determine
experimentally the form of the law of moiecular attraction. Many
assumptions are made about it in theoretical physics, but nobody has
so far tried to determine its form by actual measurement. The shape
of the curve obtained, is not dependent on the exactness of the
estimate of the surface of the powder; an error in this estimate can
only lengthen or shorten the figure in the direction of the abscissae.

It appears, that the potential diminishes rapidly with increasing
distance and has a rather well defined “radius of the attraction-
sphere’ *). For the size of this radius we find:

a). Por, £7236.

2) We therefore come to the conclusion that the layer of fluid is almost in the
whole course of the curve less thick than this radius. The supposition that the
fluid has the properties of fluid in mass therefore only is exact as an
approximation.

453
—k quartz
400
cal.
| |
300
200
100
Z in 10—* em?
je 2.74 4.42
—k anorthite
400
cal.

300 ae
200 =e
: ei,

en 1 in 10-8 cm?

1.59 3317 4.76 6.35 1.95

water-quartz fc « 1O- © cm:
water-anorthite 6.2 x 10~® em.
while Inmore*) has found in an analogous method (weighing with
a very delicate balance the increase of weight of a plain surface of
known size in a moist atmosphere)
water-brass 0.27 « 10~-° cia.
water-steel 0.61 * 10~-° cm.
water-nivkel 0.99 « 10—-® cm.
water-rock-cristal 0.0 till 6.0 x 10—-® em.
water-platina O.0y =" 3:2 % 0c": cm:
water-Jenaglass 0.3 ,, 4.0 >< 10° cm.

1) Wiedem. Arn. 81, p. 1006—1014. (1887).

454

Corresponding in order of magnitude with my figures.

There seems to exist no relation with the density of the solid.
But it seems that substances with many atoms in the molecule have
a larger radius.

Although the results found may still need correction from the fact,
that the boundary of the waterlayer and the vapour is not so sharply
defined as has been supposed, and because the compressibility of
liquid water has been neglected, the results seem interesting enough
to call attention to them. Perhaps then some one more competent on
this subject, will deduce a less approximate theory. This theory will
also have to answer the question, what is the relation between the
maximum and the minimum in TrovuTon’s curves with the maximum
and the minimum in the isotherm of vAN Der Waats, and if the
supposition is right, that it is possible to calculate the maximum
and the minimum of the equation of state from the minimum and
maximum in TRoUTON’s curves.

The importance of these investigations for the problem of swelling
(imbibition) will be treated later.

Meteorology.
Rainfall in the LEast-Indian Archipelago in connection with

“The Correlation between Atmospheric Pressure and

the 3,5 yearly barometric period’. By Dr. C. Braax. (Com-
-municated by Dr. VAN DER Stok).

(Communicated in the meeting of June 29, 1912).

The regularity of the East-Indian climate renders it eminently fit
for clearly revealing weather variations of longer period. There the
interest in the weather of next day is quite subordinate to the question
whether the coming season will bring much or litile rain and since
predictions for the immediate future are not wanted, full attention
can be paid to those for a more distant future. And this the more
so as the circumstances there promise a much better chance of
success for a prognosis of the seasons than elsewhere.

That the variations from one year to another are very considerable
and an investigation of their character and origin is important, may,
perhaps superfluously, be proved by the following summary: (p. 455)

One naturally looks for a relation between the oscillations in the
rainfall and the barometric changes of long period.

These variations of the atmospheric pressure are of the same
character over an area extending from British India over the Indian

ee bd

TOTAL RAINFALL IN M.M. IN THE MONTHS JULY, AUGUST, AND SEPTEMBER

Wet East monsoons Dry East monsoons
Batavia | Ternate | Koepang | Batavia | Ternate | Koepang
1880 363 | 599 | 0 1881 | 121 | 268 | 0
82 144 | 485 | 36 83 | 30 | 254 | 0
89 148 | 475 4 Soe). 228 or Ghee Oo
90 290 452 18 a | ee iW
92 248 | 353 | 1 91 | 102 | 321 | 0
95 262 470 | 44 96 «=| ol 393 © | 0
98 162 402 | 10 1902 16 38 0
1900 146 370 82 05 119 261 22
04 340 145 16 11 155 133 0
06 364 434 | 3 |
09 PA 697 | 37 |
10 258 305 | 5 | |
Average | 245° “432° | xop 72 197 | 3 ;
| |

Archipelago as far as Australia. They are regular and can with
great approximation be represented by a series of waves with periods
of 3 to 5 years; the other periods are quite subordinate. As a
typical example we mention the amospheric pressure at Port-Darwin
where not only the amplitude is maximal, but also the variations
are characterised by an extraordinary regularity’). For this reason
in what follows the rainfall in various parts of the Archipelago has
been referred to the indications of the barometer at this station.

The stations whose observations are regularly published by the
Batavia Observatory under the title ‘Rainfall observations in the
Dutch East Indies’ were arranged in groups, containing places of
approximately similar situation. These contain from 1 to 5 stations
and are:

1 North Sumatra, 2 North East Sumatra, 3 East Middle Sumatra,
4 Padang Highlands, 5 West Middle Sumatra, 6 South East Sumatra,
7 South West Sumatra, 8 West Borneo, 9 South Borneo, 10 North
coast of West Java, 11 the Preanger district, 12 North coast of

1) Cf. Meteorologische Zeitschrift, Heft 1, 1912, p. 1.

456

Middle Java, 13 Madioen, Kediri, Blitar and Malang, 14 North coast
of East Java, 15 the Lesser Sunda Islands and Timor, 16 West
coast of South West Celebes, 17 East coast of South West Celebes,
18 South coast of North Celebes, 19 North coast of North Celebes,
20 Amahai, Banda, Ambon and Saparoea, 21 Wahai and Kajeli,
22 Ternate.

For our analysis the period 1883—1908 was chosen.

For each group the deviations of the monthly means were calcu-
lated from the monthly means of all the years of observation,
including 1908. Since probably the oscillations in the rainfall have
a retardation of about two months with respect to those of the atmos-
pheric pressure*), the barometric deviation for January, February
etc. was always compared with the rainfall for March, April ete.
Being only a small fraction of the total period, this shifting is indeed
of secondary importance, but still it has the advantage of eliminating
the pressure variations of short duration, which as a rule last a
month or less and probably are not without any influence on the
formation of rain.

In order to express mathematically the relation between rainfall
and atmospheric pressure, the correlation factors between them were
calculated for each group and for the twelve months. Denoting by
UV, &,2,...X the deviations of the separate monthly averages from
the general monthly mean for the rainfall and by 4, y,y;.-.Yn for
the atmospheric pressure, the correlation factors are represented by *):

= ry
V Se? *K Sy

The values of 7 have been collected in the following table.

From these data the following conclusions may be drawn:

An influence of the mountain ranges on the correlation cannot be
proved with certainty. For the Preanger district behaves in the same
way as the coast stations of Java and the stations of group 13,
lying between high volcanoes. Also the West and East coast of
South-West Celebes (except in January, February, March, and
May), the South and North coast of North Celebes (except in
April) and the stations to the North (group 21) and to the South
(group 20) of the mountains of Ceram and Buru (except in February
and April) behave generally in a similar way; besides, during

1) Cf. Natuurk. Tiydsch. voor Neder]. Indié, Vol. LXX, p. 110.

*) Cf. R. H, Hooker: An elemeutary explanation of correlation... , Quarterly
Journal Royal Met. Soc. Vol. 34, p. 277, 1908 and the extract by Feurx M. —
in Meteorol. Zeitschr. June 1910, p. 263.

457

CORRELATION FACTORS

Atmosph. pressure at Port-Darwin — Rainfall in the Archipelago.

Febr. |March April| May | June | July Aug. | Sept. | Oct. | Nov. | Dec.

1) 0.04\—0.10—0.11—0.00 0.07 0.14 0.22—0.18—0.09 0.16 0.10, 0.07
a} .o6|— .32\— .35|— 21] 05] .17|- .28| .09| | .33|— .09|— .10|— .07
sl .o2|— .o7|— .50| 45] .23|— .32|— .45|— .12|— 06.13.46] 19
4) .44| .4ol— 15] 23] .00/ 17} .06-— .26| 09 121.19] .08
5] .19| 20/40} .12| 38, .02|— .05|— 10) .23|— .14|— .05| 01
e| .22) .ot|— 30) .19| .05|— .12|— .12\— .29|— .23|— -52\— .o|— 17
11— .15| .49| .03|— .04| 28 .19|— .32|— 43\— .31)— .53|— .25|— .14
8} .41| .25/— 06 40, 19) .23, | .02|— .29|— .30)._ .04) .00| 34

29] 20) .o2|— .05|— .14|— .241— asl .30|_ sal .25
- eae 42, 38 — .20\— .14|— 221 .341— .37|— .46|— AL — .10
il 18 40-191 30.18 22 t2\_ .37\— .431— .35|— 401.30
i9|— .46|— .22|— .37|— .04 .4o|—_ .31|_ .25|— 40|— ss|— .35|— 37] «18
oo) 11} 12} .32/— .33|— .sol— .38\__ .33|_ .54l_ .36|— .18|— .37|--.35
21) oo} .48) 47] .42|— .36\— .27|— .30|— .37/— .28|— .231— .55|— .24

a as a7|—= 40|— .28— .co'\— .38'— .33|— .39|— .37|— 1 53|\— .26
| |

the bracketed exceptional months the minus sign prevails on the
South coast of South West Celebes and the plus sign on ithe
East coast, while the stations of group 21, similarly situated with
respect to the monsoons as the West coast, have the plus sign and
those of group 20, situated like those on the East coast, the minus
sign, which is exactly contrary to what one would expect if the
mountains determined the sign.

458

On the other hand we clearly perceive a variation of the corre-
lation with the geographical longitude and latitude and with the
season. Leaving aside for the present the western part of the archi-
pelago north of the equator, we find in the remaining part in the
East monsoon with a few unimportant exceptions negative correla-
tion, increasing in amount from West to East. In the West monsoon
the negative sign still prevails in the East, in the West however the
positive sign appears almost without exception, so that there a surplus
of rain falls during the barometric maximum.

The explanation suggests itself that this change of sign of the
correlation depends on the wind, which has also opposite directions
in both monsoons. Now the relation between the barometric changes
and the force of the monsoons is such that during the maximum of
atmospheric pressure (caused by the relatively large amplitude of the
barometric oscillation over Australia) the wind is reinforced during
the East monsoon and weakened during the West monsoon, while
at the minimum the opposite occurs*). From this we conclude that
strengthening of the monsoon, either Last or West, impedes the for-
mation of rai. This phenomenon must be partly ascribed to the
development of fewer local showers when a stronger wind prevails,
partly, especially in the East monsoon, but perhaps also in the West,
to the circumstance that the air, when it moves in a quicker current,
remains a shorter time above the sea.

The stronger negative correlation in the East would indicate that
here, besides the influence mentioned above, stil] another factor
makes itself felt, as well in the West as in the East monsoon.
Very likely we have here a more direct influence of the neighbour-
ing active centre in North Australia, causing drought during the
maaimum by falling air-currents, rain during the minimum by rising
currents.

Though the variation of the correlation finds in this way a natural
explanation for the greater part of the Archipelago, the matter is
less simple for the remaining North-western part. There, as in Java,
the correlation is, generally speaking, opposite for both monsoons,
but it is negative when Java has a positive correlation and vice versa.

It is possible that the Barisan range, which in the northern part
of Sumatra lies straight across the path of the monsoon, makes its
influence felt. Also another explanation can however be given.

While during the maximum the influence of Australia increases
the pressure difference in other places, it is quite possible that here

1) Cf. Natuurk. Tijdschrift voor Ned. Indié, Vol. LXX, p. 105.

ea Se ee ee —— ee

— —

a -

ee.

459
the opposite occurs. The difference namely of the barometric devia-
tions at Batavia and Singapore changes in an irregular manner and
points to a transitional region between these two places, whereas the
difference between the deviations at Port-Blair (Andaman Islands),
and those observed at Singapore, runs parallel with the barometric
deviations at Port-Darwin, although with a small correlation (r=0,15).

While the atmospheric pressure goes through its 3 to 5-yearly
eycle, during the maximum in the South, Middle and East air-
currents from the South would be superposed on the general flow
of the monsoon and in the North-East, although to a smaller extent,
from the North and currents from opposite directions during the
minimum. Between the two currents a rising or falling movement
should appear. The predominant positive correlation during the whole
year in the Padang Highlands and in group 8 (Pontianak and Sing-
kawang), which are approximately situated on the border line, might
be a consequence of this vertical movement of the air. The corre-
lation factors in the North-western exceptional region are small
however, so that not much importance must be attached to these
speculations.

Nor can we expect much for this region in the way of predictions,
at any rate on the lines here developed. Matters are quite different
for the remaining part of the Archipelago, where the correlation under-
goes regular changes and reaches fairly considerable values.

The great question thus remains how we can obtain sufficient cer-
tainty about coming changes in the atmospheric pressure. Very likely
we shall have to pay less attention than was done until now to the
sun and the changes occurring there, but we shall have to look
especially for a terrestrial cause and shall have to study the coope-
ration of metereological phenomena over the whole world.

For the temperature changes, observed in British India, the Archi-
pelago and Australia find a natural explanation from the jluctua-
tions in the general circulation of the atmosphere, accompanying the
barometric changes, while it ts difjicult to bring them into relation
with changes in the solar radiation, which surely would reveal
themselves in a direct manner in temperature changes.

These temperature changes are of a twofold nature:

1. In this tropical region, where long-period changes in the
atmospheric pressure are brought about not dynamically, but enti-
rely thermally, these must be accompanied by simultaneous tem-
perature changes of opposite sign in the air-column above the
spot of observation. In agreement with this we find e.g. from a
comparison of the changes in atmospheric pressure at the mountain

460

station Kodaikanal (height 2340 m.) in the South of British India
with those at the base-station Peryakalam (290 m.) that the average
temperature of the intermediate layer undergoes oscillations of about
0,7° C., opposite to the simultaneous barometric changes at the base-
station. The correlation factor between the two is r=0O,75. The
station Kadaikanal evidently still lies in the stratum in which these
temperature changes occur, for the temperature there changes in
the same way as in the layer underneath. The correlation factor
between the two temperature changes is 7 = 0,69.

With an amplitude of the atmospheric oscillation of 0,6 mm. at
sea-level and of the temperature oscillation of 0,7° C., the air-stratum
in which both changes would be in harmony would lie at about
1000 m. above the mountain station. The temperature changes are
in this case restricted to the condensation level.

The results of Enior’s investigations’) would show that this is a
general phenomenon. From a comparison of the barometric changes
at the mountain stations in British India with those of the stations
in the plains, he deduced that during the barometric maxima at
sea-level, an abnormally large quantity of air is found below the
level of the mountain stations and an abnormally small quantity
during the minima. The temperature changes that determine the
barometric pressure here occur in the lower 2000 tot 3000 metres
in the region where the heat of condensation plays an important part.

2. In the very lowest strata of the atmosphere the oscillation of
the temperature is of a different nature. Over the whole of the area
here considered the temperature of the stations in the plains follows
namely very regularly tbe identical barometric change with a lag
of about six months’). This oscillation of the temperature must have
had a disturbing action on the observed barometric oscillation, since
the phase differs by about a year (i.e. more than ‘/, period) from
the value required for the formation of the barometric oscillation
(see 1). Still no disturbance is observed and the curves representing
the barometric oscillation and these temperature changes generally
show great similarity. This must probably be ascribed to the small
thickness of this layer, which consequently has to be considered as
a thin transition layer resting on the surface of the earth.

The temperature oscillations mentioned sub 1 and 2 are in com-
plete agreement with the following scheme of changes :

If we suppose the general circulation of the air to be subjected
to fluctuations in such a way that it is increased by the barometric

') Indian Metereological Memoirs VI, p. 102.
*) Cf. Metereol. Zeitschrift loc. cit.

461

minimum in India and Australia and weakened by the maximum,
as must undoubtedly be the case, the successive stages may be ima-
gined fs follows. During the barometric minimum an_ increased
mixing takes place with the cool air from higher latitude together
with an increased supply of cold water. By these causes after the
barometric minimum a temperature minimum is developed in the
lower strata of the atmosphere. In the upper strata, however, by
the greater heat of condensation, resulting from the increased ascend-
ing motion of the air, a temperature maximum will develop simul-
taneously with the barometric minimum and this maximum will in
its turn determine and strengthen the barometric minimum. This
latter process will continue until the progressive sinking of the tem-
perature of the water and the air below, cause the condensation to
diminish and the atmospheric pressure to rise by a smaller supply
of water-vapour and greater density of the air and in this way the
following phase is prepared.

The energy required for keeping up this process is partly supplied
by the increased heat of condensation during the barometric minimum
and may for another part be derived from the interaction with the
active centres of higher latitude where the deviations, once started,
reinforce themselves, contrary to the tropical system of circulation
where they are self-regulating *).

Weltevreden, May 10, 1912.

Geology. —- “On Orbitoids of Sumba’. By Dr. L. Rurrey. (Com-

municated by Prof. A. WicHMany).

(Communicated of the meeting of September 28, 1912).

From Professor Wicamann I received a short time ago a small
collection of specimens of rocks and fossils belonging to a collection
gathered by Mr. H. Wirkamp, geologist of the Bataafsche Petroleum-
Maatschappy in the southern part of the Islend of Sumba.

I beg to communicate here some particulars about the Orbitoids
found in this collection. In 5 of the samples sent to me I discovered
Orbitoids ie. in 4 numbers (81, 114, 166 and 167) the subgenus
Orthophragmina, and in 1 number (105) the subgenus Lepidocyclina.

1) Cf. Metereol. Zeitschr. loc, cit.

462
Orthophragmina.

Previous findings in the Dutch East Indies.

The first Orthophragmina were described by R. D. M. VeErpexrx ')
from South-East Borneo. A few years afterwards his material was
investigated by Von Fritscu’), who determined 5 species. A short time
after K. Martin*) reported the existence of Orbitoids with Num-
mulites of the river Teweh in South Borneo, whilst Tu. Posrwirz
had collected in the neighbourhood of Muara Teweh analogous
Orthophragmina as VeERBEEK had gathered in South-East Borneo ‘*).

In recent times H. Dovvi1£*) and Irene ProvaLe‘) have again
described Orthophragmina of South Borneo whilst the latter determined
moreover a series of Orthophragmina of Udju Halang on the Upper-
Makaham (Central Borneo) ‘).

Of West Borneo we know through Jennines *), and R. B. Newton
and R. Hor.anp *) some findingplaces of Orthophragmina.

In Java Orbitoides with rectangrlar median chambers have been
found at the surface in the residences of Bagelen, of Djokjokarta
and of the Preanger*’) Regencies, whilst also in a boring near
Ngembak (Recidency of Samarang) a few Orthophragmina were
found *°).

Y) R. D. M. Verpeex. Die Nummuliten des Borneo-Kalksleines. Neues Jahrbuch
fiir Mineralogie etc. 1871, p p.. 1—11.

*) K. v. Fritsca. Einige eociine Foraminiferen von Borneo. Jaarboek van het
Mijnwezen in Ned.-Indié. 1879. 1. p.p. 236—281,

8) K. Martin. Neue Fundpunkte von Tertiiirgestemen im Indischen Archipel.
Samml. Geol. Reichsmuseums. Leiden. (1). 1. 1881—83, p.p. 181—198.

4) Tu. Posewirz. Das tertiire Hiigelland bei Teweh. Nat. Tijdschr. van Ned.-
Indié XLIIL. 1884, pp. 169—175. — Tu. Posewitz. Borneo. 1889. p.p.383—384.

5) H. Dovuvitré. Les Foraminiféres dans le tertiaire de Bornéo. Bull. Soc. géol.
de France. (4). 5. 1905, p.p. 435—464.

6) I. Provate. Rivista italiana di Paleontologia. 15. 1909. p.p. 65—96.

7) I. Provate. Rivista italiana di Paleontologia. 14. Perugia 1908, p.p. 55—80.

8) A. V. Jenninas. Geological Magazine (3). 5. 1888. p p. 530—532.

9) R. B. Newton and P. Hottanp. Annals and Magazine of Natural History. (7).
3. 1899, p.p. 245 —264.

1) R. D. M. Verseex, Tijdschr. Ned. Aardr. Genootschap. 1, Amsterdam 1876,
p-p. 291 et seq.

K. Martin. Samml. Geol. Reichsmuseums. Leiden. (1). 1. 1881—83. p.p. 105—180.

R. D. M. Venpeex. Natuurkundig Tijdschrift van Nederl.-Indié. 51. 1892. p.p. 101 — 138,

R. D. M. Verseex et R. Fennema. Description géologique de Java et Madoura.
1896. Tome 2.

C. Scutumperaer. Bull. Soc. géol. de France. (4). 3. 1903. p.p. 293 et seq.

H. Dovvitie. Samml. des Geol. Reichsmus. Leiden. (1). 8. 1904 —12. p.p. 279—294.

‘) K. Martin. Samml. des Geol. Reichsmus. Leiden. (1). 8. 1887. p.p. 327 et seq.

463

For a short time past Orthophragmina of Nias') are known,
whilst in the eastern part of our archipelago they were found in
West Celebes*), West Timor, the new island near Ut, Great Kei,
Kilwair, Tofuré, in New-Guinea eastward of the Etna Bay, Rend-
juwa *) and in West Buru ‘).

With the great number of very often incompletely described species
of Orthophragmina that are known from the Dutch East-Indies, it
will often be difficult to decide with which species a special form
must be classed; fortunately this difficulty did not present itself with
regard to the Sumba material, as the Orthophragmina in question
belong to 2 wellknown species, O. javana Verb. and QO. dispansa
Sow., as will appear from the description.

Orthophragmima javana VERBEEK.

Syn. papyracea Boubée, in von Fritsch 1879?

papyracea Boubée, var. javana in Verbeek. T. A. G. 1.
papyracea Boubée, var. javana in Verbeek 1892 and 1896.
dispansa Sow. in Martin 1881 (partim).

javana Verbeek in Douvillé 1905.

. javana Verbeek in Douvillé 1912.

Discocyclina discus Riitimeyer in Verbeek 1908. p. 304.

Sei cre

From the finding-place n°. 105 I received 5 isolated Orthophragmina,
which, though they are very different in size (diam. 6, 12, 14, 24
and 27 mm.), cannot be separated from one another and must be
classed with one species.

The pretty well conserved fossils have the form of regular lenses,
showing either no central chamber at all or one which is but little
pronounced in its youth; most of them are symmetrically thickened
towards the centrum; the specimen of 27 mm. diameter had a
thickness of 6 mm. The surface of the fossils is somewhat disin-
tegrated, so that the fine-granular, dense, and very symmetrical
granulation cannot very well be seen. Three horizontal sections
were made, from which it appeared that the larger specimens of
24 and 27 mm. diameter were microspheric and the one of 12 mm.

_ 1) H. Dovvitté. Samml. des Geol. Reichsmuseums Leiden. (1). 8. 1904—12.
p-p. 253—278.

2) H. Douvitté. |.c. 1905.

R. D. M. Verseex. Molukkenverslag. Jaarb. van het Mijnw. Wetensch. Ged.
XXXVI. 1908, p.p. 54, 80, 81.

3) R. D. M. Verseex. lc. 1908. p.p. 398, 625, 613, 616, 255, 474, 754 en 304.

4) J. Wanner. Centralbl. fiir Mineralogie, Geologie und Paldontologie. 1910,
p- 140.

464

diameter was megalospheric. With regard to the two first-mentioned
specimens I did not succeed in including the little embryonal chamber
into the preparation.

1. Megalospheric form.

The median plane is but little curved: the median chambers form
frequently incomplete circles round the very large embryonal cham-
bers, whose maximal and minimal diameters are 2500 u and 1800 u.
The parietis of the embryonal chamber is thin. The peripherical,
median chambers of the first round are larger than those situated
more outward: |
4st round diameter of the chamber radiary 190 u, tangentially 55—75 u
more peripherically maxim. diameter radiary 150 p, tangentially 60 uw.

2. Microspheric form.

In these large Orbitoids of exterior regular lensshape the median
plane shows a strong saddle-shaped curve, as in the median hori-
zontal section only narrow ligaments of median chambers running
hyperbolically have been struck (comp. VERBEEK and Frnnema 1896.
P]. 10, Fig. 150).The radiary diameter of the median chambers increases
from the centre of the periphery, though constantly smaller chambers
are scattered among the larger ones. The normal dimensions of the
chambers are about:

At 2 mm. from the centre: radiary 45-75 wu, tangentially 35-55 u.
Nearer to the periphery : » 135-190 p, 95 30-09 ML.

The grouping of the intermediate skeleton-columns to which of
late, for a systematical purpose, DovviL1e (J.c, 1912) attaches such
a great value can distinctly be observed. Their thickness in tan-
gential diameter is 55—95 4, it may be however that very near the
periphery they are a little thicker. As a rule columns are only sepa-
rated from each other by a single row of spacious lateral chambers.

Consequently the exterior habitus and structure of these Formani-
fera correspond very well with the forms described by VERBEEK
(1896) as O. papyracea var. javana and witb those described by
Dovvitié (1912) as O. javana, only the megalospheric form of this
species was not yet known hitherto.

From the finding-place near Mount Madu (n°. 81) I received
two Orbitoids (diam. 14 and 380 mm.) which correspond very
well with the former, and the larger of which was again micro-
spheric. 1 succeeded in including into the preparation the very
small embryonal chambers round which the first peripherical cham-

465

bers are grouped in circles. The tangential diameter of these
first rounds of peripheric chambers is larger tnan the radiary one
(comp. VERBEEK 1896, pl. 10 f. 157). The columns are here a little
thicker (100—180 uw) than with the forms described above; they
show both in a transversal and in a longitudinal section a very
distinct, fibrous structure. The lumen of the lateral chambers is in
a vertical direction very wide and their horizontal parietes are
very thin.

From the finding-place N°. 167 a I received likewise a specimen
of O. javana.

Orthophragmina dispansa Sowerby.

Syn. QO. dispansa Sow. in von Fritscu 1879?
O. dispansa Sow. in VERBEEK 1892 and 1896.
O. dispansa Sow. in Martin 1881 (partim) and 1887.

QO. dispansa Sow. in Dovvin1é 1912.

The rock N°. 16 is entirely filled up with Orbitoids which, by
disintregation, are partly laid bare, so that their exterior habitus
can be studied. The maximal diameter amounts to 9 mm, the height
to 3 mm. The fossils are considerably thickened in the centre,
whilst at the periphery they have an excessively thin edge. The
surface is strongly granulated; the granulae however are not sym-
metrically divided over the whole surface. They are largest on the
central tubercle (100—190u), towards the periphery they become
very small, but on the very thin edge again larger granulae are
perceptible.

Though in general the granulae are separated by a single row of
spacious lateral chainbers, it often occurs that there are two rows
of chambers between them.

In sections only macrospheric individuals were found. The dimi-

nutive size and the spacious lateral chambers make this form corre-
spond entirely to O. dispansa Sow, as DovviLL£é described them a
short time ago (1912).
Rare specimens of Calcarina and little Nummulites are found in
the limestone N°. 238, together with these Orthophragmina, whilst
it is by no means impossible that still another very thin Orthophrag-
mina is met with: the material was however insufficient to decide
in this respect.

o1
Proceedings Royal Acad. Amsterdam. Vol. XIV.

466
Lepidocyclina.

The brecciated rock N°. 105 contains many but fragmentary
fossils, among which Lithothamnium, Cycloclypeus, Heterostegina,
and Lepidocyclina can be recognized.

The individuals of the latter genus seem to reach a size of about
10 mm.; the median chambers are spatulated to rhombic. It is
impossible specifically to determine them for want of orientated
sections, and isolated specimens.

Since VersBrek’s publication of 1892, nearly all authors on Indian
Orbitoids agree that Lepidocyclina and Orthophragmina never occur
together in one stratum, and that the latter are characteristic of
the Eocene, the former of the Upper-Oligocene and Miocene.

J. Provate U. ec. 1908) holds a different view, she describes
Orthophragmina and Lepidocyclina of Udju Halang in Central Borneo,
which are said to proceed from one stratum, whilst G. Osimo’) has
mentioned rare Lepidocyclina of West Celebes (Donggala) that are
reported to eccur with eocene Nummulites. These assertions should,
however, be accepted with some reserve.

In the first place at Udju Halang Lepidocyclina and Orthophrag-
mina are not found in one and the same rock (Provare |. c. 1909
p- 75)*), so that it is likely that they occur in the proximity of
each other, but not in the same stratum.

The same possibility, however, exists for the findingplaces near
Donggala, the more so as VERBEEK (I. c. 1908, p.p. 58, 59) ascertained
for the surroundings of Pangkadjéné and Maros, northward from
Makassar the existence of eocene limestone with Orthophragmina,
and of oligo-miocene limestone with Lepidocyclina the one in the
proximity of the other.

For the present we may consequently certainly stick to the old
view that in India Orthophragmina characterizes Eocene, Lepido-
cyclina on the other hand the Upper-Oligocene, so that from the
above we may make the conclusion that in Sumba both Eocene and
Miocene must be found. The limestone and marls of Sumba that are
known up to the present (VERBEEK J. c. 1908) originated from the
northern part of the island and were usually very young; the older
ones were most likely classed with Miocene.

Buitenzorg, August 1912.
1) G. Osmo. Rivista italiana di Paleontologia, 14 Perugia 1908, p.p. 21—54.

*) I. PRovALE indicates in this place the age of the Orthophragmina as ence
that of the Lepidocyclina as oligocene. (?)

467

Chemistry. — “On the Quaternary system : KCI—CuCl,—BaCl,—
HO.” By Prof. F. A. H. Scurememakers and Miss W.C. pg Baar.

(Communicated in the meeting of September 28, 1912).

In the previous articles’) we already discussed the equilibria

occurring at 30° in the quaternary systems :
NaCl — CuCl, — BaCl, — H,O
and NH,Cl — CuCl, — BaCl, — H,O

In the first system no double salt is formed, in the second

occurs the double salt CuCl, .2 NH,Cl.2H,O. As in the system :
KCl — CuCl, — BaCl, — H,O

two double salts may appear, we have now investigated this system

also.

The two double salts are:

D; 20 == CuCl, KCl. 2 H,O
and Dit =— CuCl, aKCL,

The equilibria. occurring have been investigated at 40° and 60°;
these temperatures have been chosen purposely because at the first
temperature (40°) only one of the double salts (Dj 22) still occurs;
at the other temperature (60°) both double salts appear.

In the ternary system KCl — BaCl, —H,O occur as solid sub-
stances, at 40° and 60° KCi and BaCl,.2H,O so that the isotherms
also consist of two saturation lines.

The monovariant (P) equilibria occurring in the ternary system
KCl — CuCl, — H,O have been described previously by W. Meyer-
HOFFER’); the isotherm of 30° has been determined by H. Funrepo*),

From these investigations it follows that below 57°, in addition
to KCl and CuCl,.2H,O also occurs the double salt Dj 22, between
57° and 92° the double salts Dj22 and D;; and above 92° only the
double salt Dy 4.

The isotherm of 40° therefore consists of the saturation lines of:
KCl , CuCl,.2H,O and Dj 22, that of 60° of the saturation lines of
mel. Cu€l,.20.0, Dies and D1.

The equilibria appearing in the quaternary system may be repre-
sented in space, in the well known manner with the aid ofa tetra-
hedron, whose four apexes indicate the four components : KCI, CuCl,,
BaCl, and water. In Figs. 1 and 2 is found a projection of the

1) F. A, H. Scurememaxers and Miss W. C. pve Baat. Chem. Weekbl. 1908.
2) W. Meyeruorrer. Z. f. Phys. Chem. 3 336 (1889).
m8 > o- OF (1890).

8) H. Fitippo. Not yet published.

468

spacial representation on the side plane KCl—BaCl, —CuCl, of the
tetrahedron which projection may be easily deduced in the well
known manner from the representation in space *).

Fig. 1 gives a schematic representation of the equilibria occur-
ring at 40°.

The equilibria occurring in the ternary system BaCl,—CuCl, —
Water are represented by the curves ab and dc situated on the
side plane BaCl],—CuCl, —Water.

ab is the saturation line of the CuCl,.2H,O
ial ares A: 33° 26. 4 aOl.. 2020

The equilibria occurring in the ternary system : KCl—BaCl,— Water
are represented by the curves cd and de situated on the side plane:
kK Cl—BaCl,—-Water.

cd is the saturation line of the BaCl,.2H,O
dé’, 45 Uae Bll 5. eek:

The solution d is saturated with both salts.

The curves ef, fy and ga situated on the side plane KCI—CuCl,—
Water represent the equilibria in the ternary system KCl—CuCl,——
Water.

e f is the saturation line of the K Cl.
W 9 ener + yo Ss.
Gx aoe le, ry fe HOUOL Ss, ee:

Hence the solubility’ line of the double salt Dj22—= Cu Cl,.2K Cl.
2H, 0 is limited in point f by the occurrence of solid K Cl and in
point g by the occurrence of solid Cu Cl, . 2 H, O.

1) Z. f. Phys. Chem. 65, 563 (1909).

469

In the quaternary system occur solutions saturated with one, two
and three solid substances.

Those saturated with one solid substance only are represented by
a plane, tbe saturation plane of that substance.

Plane I or abhg is the saturation plane of the CuCl, .2H,0.

peer oe G2 Feo gs ix ad ase oy ee OD
ee 6 OE ie ys ms 53 Ore yc ek Oa > Se ae
” FY ”» Sg hi ” »” ” ” ” ” Di 22.

The intersecting lines of these saturation planes indicate the solu-
tions saturated with two solid substances; thus we find:

Curve 6h is the saturation curve of CuCl,.2H,O+BaCl,.2H,0.

a is % os. KCI--BaCh,.2H.0.
” fi BB) AE, ” ”? ”? KCI+Dj; 99

55 ih Dero. ae 3 + 3 Dj 22 +BaCl,.2H,O.
_ IEP 3, 2 +» Di22-+ CuCl,,2H,0.

The solutions saturated with three solid substances are represented
by the points of intersection of the saturation planes;

ar fh a Ac Se a5 KCl+BaCl,.2H,O+D; 29

If we remember that the equilibria represented in Fig. 1 apply
only to one definite temperature 7’ and to one definite pressure P,
we notice occurrence of the following equilibria:

A. Invariant (P. 7.) equilibria (2 Components in 7 phases)
1. binary: the point a, ¢ and e;
2. ternary: ewe 0d, F and.¢:;
3. quaternary: -,;) 5° 2 and A.

B. Monovariant (P. 7.) equilibria (n Components in »—1 phases)
1. ternary: the Curves ad, be, cd, de, ef, fg and ga.
2. quaternary: the Curves bh, hi, id, if and gh.

C. Divariant (P. 7) equilibria (2 Components in n—2_ phases.
1. quaternary: the planes /, //, //Z and JV.

The equilibria occurring at 60° are represented schematically in
fig. 2; this is distinguished from fig. 1 in so far that between
the saturation plane / and /V of fig. 1 another saturation plane V
has introduced itself so that the following saturation planes oceur.

Plane /, or ablk, the saturation plane of CuCl, 2H,O

” LF » € d We ” ” ” », KCl
mathe. chil ped. ,. =) 5 a is, ea 2G)
” (BA ” Sg h i, ” ” ” ”» Di22

” ue » J hlk ” 2 ” ” Di

470

If we compare the figs 1 and 2 we notice that the equilibria in
the two ternary systems CuCl,—BaCl,—Water and KCl— BaCl,—-
Water, do not show appreciable differences at 40° and 60°, but that
these are observed in the ternary system CuCl,—KCl—Water and
in the quaternary system.

At 40° (Fig. 1) the isotherm of the ternary system KCl
CuCl,—H,O consists of:

ef, the saturation line of the KCl
TGF 6 “ 5 hap Sees
and ga, ,, * so 5 2 (Ca BRS

whereas this consists at 60°, (Fig. 2), of:

Fig. 2.

ef, the saturation line of the KCl

TO. = is i sp Sees
gk, ” » 9 »» ed Bee
and ka, ,, ‘3 7 os = eUCl are
Whereas at 40° only 5 quaternary saturation curves occur, seven
ave found at 60°, namely.

Curve 0/, the saturation curve of CuCl, .2H,O + BaCl, . 2H,O

es “ » 9» KCl-+ BaCl,..2H,O
53 Fa Gates 53 » 9» KCl+ Di2e
“aerate: rn » », BaCl, .2H,O + Dj22
ela (1 Fane 43 » op Diss 4D

ales (| Pane “= »- » Dia=-+ BaGl, 20,0
tee x » yy Dit OnGk Soe:

The saturation curve gh of fig. 1 (at 40°) is, therefore replaced
in fig. 2 (at 60°) by the three saturation curves gh, hl and lk.

At 40° (fig. 1) we find only two, at 60° (fig. 2) however, three
quaternary saturation points, namely :

471

Point 7, the saturation point of KCl + BaCl, .2H,O + Dj 22

2 ae 29 » 9» BaCl,.2H,O + Di22 + Dit

Sh Sar 55 » 9 BaCl,.2H,0 + CuCl,.2H,0 + Dy,

As the equilibria represented in fig. 2 only apply to one definite
temperature 7Z’ and one definite pressure P, we have at 60° the
following equilibria:

A. Invariant (P. 7’) equilibria.

binary : the point a, ¢ and e.
ternary : 2 oe Ord, og and. &.
quaternary : ,, Be? of ang. f;

. Monovariant (P. 7’) equilibria.

ternary : the curves ab, bc, cd, de, ef, fy, gk and ka.
quaternary: _,, Sool EL, Weal, ha; fe and id
Divariant (P. 7’) equilibria.

quaternary : the planes I, I, III, IV and V.

icy Sees ay ee

It is evident that between the Figs. 1 and 2 there exist transi-
tion forms, which must occur between 40° and 60°. If we start
from fig. 2 and lower the temperature, the saturation surface V gets
smaller until at 57° the points g and / coincide. The saturation surface
then has a triangular form of which one apex rests against the side
plane W—CuCl,—-KCI of the tetrahedron. As in this apex the
saturation surfaces I, 1V, and V meet, the equilibrium:

Cu Clo.2H20 -- Di 29 a Di

occurs in the ternary system KCl — CuCl, — Water at 57’.

On lowering the temperature still further the saturation surface V
becomes smaller still and surrounded by the saturation surfaces /, [//
and JV to finally disappear in a point within the tetrahedron, so
that the relations drawn in fig. 1 occur. The moment the saturation
surface V disappears, or rather that it becomes metastable, the
surfaces J, I//, 1V, and V pass through one point so that only one
single point of the surface V represents a stable solution. This then
signifies that in the quaternary system occurs the invariant (2) equi-
librium :

Ba Cl2.2H20 + Cu Cle.2H20 + Dy2.2 + Di + Solution.

This as deduced from the thermic determinations, happens at
+ 55,7°.

Between the above 5 phases a phase reaction may take place at
595.7°, on increase, or decrease of heat.

472

If, for the sake of brevity, we call Ba Cle.2H20 = Bag and Cu Cle.
2H20 = Cue, the reaction is then:
Bag ~- Cue2 = Diez Dy. 1 a Solution
Ba Cu D,. 1 Sol.
Bas + Cte + Draa+ 801 | pp en ee
Baz Cae + Diz2 a Di. | Cuzg + Di22-+ Di1 + Sol,

Hence, of the invariant (P) equilibrium two monovariant (P)
proceed to lower and three to higher temperatures, or if we only
consider the systems in which a solution occurs, one to lower and
three to higher temperatures.

The system proceeding to lower temperatures: Bag ++ Cug +
Di22+ sol. still exists at 40° and is represented in fig. 1 by the’
point 4. The system proceeding to higher temperatures: Cuz + Di 22
+ D,; + solution terminates at 57°, when the solution only still
contains the three components CuCl, KCl and water.

The other two systems proceeding to higher temperatures still
exist at 60°; the solution of the system Bag + Cug + D,; + solution
is represented in fig. 2 by the point / and that of the system:
BaCle + Dj 22+ Dy, is indicated in fig. 2 by the point A.

Chemistry. — “Zhe system HgCl,—CuCl,—H,0O.” By Prof. F.
A. H. ScurertneMAKers and J. C. THonts.

(Communicated in the meeting of September 28, 1912).

In order to ascertain whether or not the salts HgCl, and CuCl,
form a double salt, the isotherm of 35° was determined; the result
of this investigation is that, at 35° no double salt was found but
that the salts HgCl, and CuCl,.2H,O can exist by the side of
each other.

In fig. 1, the experimentally
determined isotherm of 35° is
represented schematically; the
apexes W, HgCl, and CuCl, repre-
sent the three components, and
the point Cu, the hydrate CuCl,.
2 H,0.

The isotherm consists of the
two branches ac and be; ac indi-
cates the solutions which are
saturated with the hydrate CuCl, .
2H,O, be those saturated with

73
HgCl,; the point of intersection ¢ of the two saturation lines repre-
sents the solution saturated with CuCl, .2H,O + HeCl,.

The solubility curve be of the HgCl, has a peculiar form; for a
tangent may be drawn to it parallel to the side W.CuCl,. This
means, in our case, that the solubility of HgCl, first increases and
then decreases with an increased CuCl,-content of the solution. From
the Fig. 1 it is shown that the solubility of HeCl, is much increased
by addition of CuCl,; from the table we see that the solubility of
HgCl,, which in pure water amounts to 8.51 °/, can increase to
fully 52°/, by addition of CuCl,.

The isotherm represented schematically in fig. 1 can be drawn
with the aid of the determinations communicated in the table. As
not only the compositions of the liquids, but also those of the corre-
sponding “residues” have been determined, the composition of the
solid substance may be deduced therefrom. We find that the solu-
tions of branch ac are saturated with CuCl,.2H,O and those of
be with HeCl,.

Compositions in % by weight at 35°.

of the solution of the residue

= solid phase
%y CuCly | % HgCly | %/y CuCl, , %/ HgCl,

44.47 Gi a aero | = CuCl, . 2H,0
33.5 21.03 | 51.0 | 13.04 |
26.01 | 37.3 55.82 | 16.97

23.31 | 44.47 | 54.71 | 19.70 :
21.49 | 50.45 | 43.60 | 36.63 CuCl; .2H.0 + HeCl,
2h ae tans | ase |, ok,
21.54 | 50.37 - == Pee ie os
19.40 | 52.44 | 3.0 | 91.94 HgCl,
18.48 | 52,54 | 4.6 | 87.57 ‘
18.06 | 52.81 | 3.17 | 90.06 ;
14.73 | 51.03 — _ ”
5.94 | 49.5 - ae ;
aa eet cme Se | :

474

One of us has previously deduced the rule’) that the meta-
stable continuations of the branches ac and 6c must fall both
together either within or without / Cae 2be Ol Wiel gease
occurs here is difficult to prove experimentally as both branches, in
the vicinity of point c practically coincide with the sides of the
angle Cu,.c.HgCl,. Moreover, the saturation line bc of the HgCl,
exhibits a very peculiar form. The metastable continuation must, of
course, terminate somewhere on the side HgCl,—CuCl, of the tri-
angle; from the course of the stable part in the vicinity of ¢, it
appears, bowever, that this will not be possible without a point of
inflexion appearing somewhere on the metastable part or on the
stable part situated in the vicinity of c.

Chemistry. — “Zhe system Tin-[odine’. By Prof. W. Reinpers
and S, pe Lancer. (Communicated by Prof. SCHREINEMAKERS.)

(Cummunicated in the meeting of September 28, 1912).

1. Of tin and iodine two compounds are known, stannous and stannic
iodide. As regards the preparation and properties of these compounds
there exist in the literature different conflicting statements. By the
older investigators?), for instance, it is stated that on heating tin with
iodine, stannous iodide is formed. Henry‘), however finds a mixture
of SnI, and SnI, and Personne’) SnI, only. The melting point of
SnI, is given by Personne *) as 145° (solidifying point 142°), by
Emicn*) 143°. The boiling point according to Personne is at 295°,
Emicn finds 341°. Henry, however, states that it sublimes at 180°.

Of Snl, the melting point is given both at 2467) and at a dull
red heat (PERsonNE) and the boiling point both at 295°") and at the
temperature of molten glass (PERSONNE).

For the knowledge of the binary systems of a metal and a metal-
loid a renewed investigation was therefore desirable.

2. Snl, was prepared in two ways, a. by treating granulated tin
for some days with a solution of iodine in carbon disulphide and

1) |". A. H. Scurememaxers, Die heter. Gleichg. von Baxnuts Roozeroom. III’. 268.
2) Ia. Berzentus, Traité de chimie; Rammetsperc, Pogg. Ann. 48, 169.

3) Phil. Trans. 185, 363 (1845).

4) Compt. rendus. 54, 216 (1862).

ay aL ec:

6) Sitzungsber. der K. Ak. v. W. Wien 118, I[b, 535 (1904) ( Monatshefte 25, 907.
7) Conen, Abegg’s Handbuch d. anorg. Ch. Ul. 2, 571.

ae -

475

evaporating the solution obtained, 6. by melting iodine with a small
excess of tin. The weighed out quantities were introduced in small
portions into a glass tube and if necessary, beated a little to start
the reaction; the tube was then sealed, heated for some time at
250°, then placed vertically and cooled slowly. The orange-red ery-
stalline mass obtained was then separated from the tin and the
bottom layer of crystals and reduced to a fine powder. Both methods
gave according to analysis, pure SnI, without any SnI, whatever.
Found : 18,95—18,99 °/, of Sn; theory 18,99 °/,.

For the preparation of Snl, is recorded a. addition of SnCl,-solu-
tion to KI-solution *) 6. dissolution of tin in concentrated hydriodic
acid 7).

The first method seems the most simple one. It has the disadvantage
however, that in this reaction besides the red SnlI,, double salts
with KI may be formed also, whilst it is still uncertain whether
a protochloro-iodide (Henry), or mixed crystals with SnCl, are per-
haps obtained in addition. The first method was, therefore, aban-
doned and the second process used instead. The action of tin on HI
proceeds slowly and was carried out in a round bottomed flask
attached to a refluxcondenser. The red crystals obtained ‘were dried
in a vacuum desiccator, first for a few weeks over sticks of KOH,
then for a few months over P,O,. Found 31,83 and 31,87 cf ait 3
on; theory 31,92 °/,.

Another mode of preparation will be mentioned presently.

3. The melting point of Snl, was found 143,°5, therefore in agree-
ment with Emicu, who gives 143°.

The solidifying point determinations of I-SnI,-mixtures took place
in the usual manner by cooling in the apparatus van Ex. In order
to prevent strong undercooling we constantly stirred with the ther-
mometer during the cooling.

The results are united in the subjoined table (p. 476) and
represented graphically in Fig. 1.

Hence we have a simple melting point line with a eutecticum at
79°,6 and 60°/, by weight of SnI, (12,06 at. °/, Sn).

4, In the preparation of SnI,, it had already been shown that
SnI, could be heated for a considerable time with Sn at 250°
without any perceptible reaction setting in with formation of Sn J,.
_ The possibility had, therefore, to be considered whether Sn and

1) Bouttay, Ann. d. phys. et chim. (2) 34, 337 (1827); Personne, 1. c.
2) Personne l.c.

476

Composition of the liquid
Initial
gr. Snly per | at. Sn per | Solidifying point
100 gr.Snly+1 100 at. Sn-+-1 |
0 | 0 ais
10 | 2.02 109.0
20 4.04 104.7
30 6.05 99.7
40 8.06 94.7
50 10.06 87.6
55 11.06 83.0
60 12.06 79.6
65 13.05 83.5 (eutecticum 79°.6)
70 14.05 89.8
80 16.04 108.4
90 18.02 127.0
100 20.00 | 143.5

Sn I, might not really be in stable equilibrium with each other
and that Sn I, might be at high temperature a labile compound that
would dissociate into Sn + Sn I,. Looking at the fact that the number
of halogen atoms, capable of combining with an element, generally
decreases with the atomic weight of the halogen, the probability of
this was not great, and it was even to be expected that SnI, would
be very permanent.

In order to decide this, weighed quantities of Sn, SnIJ,, and Sn I,
were heated in a sealed tube during 14 hours at 360°. Starting from
12.5 grams of Sn I,, 7.7 grams of Sn I, and 2.4 grams of Sn there
were obtained about 9.6 grams of SnI,, 10.5 grams of SnI, and
1.6 gram of Sn. Consequently, there was a very appreciable decrease
of Sn and Sn I, and an increase of Sn I,.

The reaction Sn-+SnI,—25nI,, therefore, actually does take
place, although very slowly. The contradiction between the statement
of Pursonne that from Sn-++ I no Sn I, is formed and that of Henry,
who states that a mixture of SnI, and SnJI, is formed, is now
explained. Hrnry has evaporated SnI, with an excess of fine tin
powder and so obtained a partial conversion into Sn I, which was

477

J 2 4 6 81012 14 16 18 20 22 24 26 28 30 32 34 at. % Sn
Sn lq Sn,

Pies i.

left on evaporation. Prrsonne allowed but a short time for the
reaction and took no particular care to accelerate the same by
addition of an excess of fine tin powder, and so he got no appre-
ciable quantities of Sn I,.

By this conversion is now indicated also another method for the
preparation of SnI,, namely, prolonged heating of Sn-+ SnI, in a
sealed tube at a high temperature (360°).

It appears that Sn I, and Sn 1, then form two liquid layers, a bottom
layer of SnJ, and an upper layer of SnJI,. In order to promote the
reaction it is, therefore, necessary to keep on shaking the tube so as to
bring the Sn I, into contact with the Sn. By placing the tube, at the end
of the heating operation, in a vertical position, and then allowing it to
cool, we obtain, after solidification a crystalline stick which can be
readily removed from the tube and breaks up along a fairly sharp
meniscus into a SnI, and a Snl, piece. By strongly heating in a test
tube of hard glass, the SnI, can be freed from the adhering SnI,.

478

The analysis of the Sn I, thus prepared gave 31.6 and 31.2°/, of
tin instead of the theoretical quantity (31.9).

5. The melting point of SnI, was determined by heating and
cooling in a small electric furnace consisting of a cylindric little pot
of porous earthenware, surrounded by a nickel heating wire and
placed in a similar larger pot which was then filled up with asbestos.
The melting point was found at 319°—320°.

The boiling point of Sn I, was determined in a 25 em. long hard
glass tube 3—4 cm. in diameter, the upper part of which was
thoroughly isolated by a thick layer of asbestos and could be heated
electrically by a nickel wire, whilst the lower part, which contained
the SnI, was heated strongly either electrically or with the blow-
pipe. The temperature was measured with a standard Pt-PtRh
thermocouple.

The mean of many determinations was 720°.

6. Addition of SnI, or Sn had no perceptible influence on the
melting point of SnI,. These substances, when by the side of
Sn I,, form a second liquid phase, so that above 320° there are two
regions of decomposition, one between SnI, and SnJ, and one be-
tween SnI, and Sn. The fused SnI, lies in a narrow region of
homogeneous mixing.

In order to determine the limits of these regions of decomposition,

Sn I, and SnI, were heated in a narrow sealed tube and shaken for
an hour at 350° in an electric tube furnace. The apparatus was
then placed. in a vertical position, the tube was removed and rapidly
cooled in a current of air. The solidified Sn I, and Sn I, layers were
separated from cach other, well scraped and then analysed.

The Sn I, layer. The total tin content was 18.95 and 19.02, mean
18.99, which corresponds to pure SnJ,. The solubility of SnT, in
Sn I, is therefore, practically m/. This result was confirmed by
dissolving a portion of the upper layer in carbon disulphide and
after adding iodine, titrating the excess of the latter with sodium
thiosulphate; only 0,06 °/, of Sn I, was thus found.

The SnI, layer. The total tin content amounted to 31.2 and
30.9°/,, mean 31.1°/,; SnI, requires 31.9 °/, of tin. This analysis
therefore points to a 6°/, SnI, content. This figure must probably
be considered as a maximum. During the fusion the Sn I, penetrates
between the glass and the SnI, layer so that after cooling, this is
enveloped by a thin layer of SnI, which might be not completely
removed in some places. The fact that addition of Sn I, does not

479

perceptibly affect the melting point of Sn I, shows that the solubility
of Sn I, in this Jayer is very trifling.

The SnI, layer saturated with Sn. SnI,, prepared by shaking
molten SnI, with Sn, did not differ in colour from that which had
been prepared by the net process and fused afterwards. A solubility
of Sn in SnI, did not make itself conspicuous by a darker colour,
or as Lorenz*) describes it by a ‘“Metallnebel’’. The analysis of
fused Sn J, which had been heated with Sn for some time at
300°—-400° and then poured off from the molten metal, also did not
differ perceptibly from that of pure Sn I,. The solubility of Sn in Sn I, is,
therefore, exccedingly small. This is in agreement with the determi-
nations of the solubility of Sn in SnI, by R. Lorenz’), who found
that at 629° this is only 0.13°/, more than at 400°, so that, at
390°, it may be safely taken as practically nl.

7. The boiling point of SnI, was determined at 340°; Emicu has
stated it to be at 341°. These determinations therefore tally, and the
previous statcment by Prrsonne (295°) must be rejected as being
inaccurate.

8. The boiling points of mixtures of I
and Sn I, were determined in the apparatus
drawn in Fig. 2. This consisted of a round-
bottomed flask A of + 100 ce capacity,
half way filled with the boiling mixture
and protected by an asbestos case in the
bottom of which a circular opening was
made. The boiling flask can then be heated
over the naked flame without danger of
snperheating.

To the flask was sealed a vertical tube
surrounded by a jacket which was heated
up to 140° by xylene vapour from 5. This
prevented the vapour from A from forming
a solid deposit in the tube; it conden-
sed to liquid and was collected again in A.

If, after long boiling, the iodine vapour
had diffused too much towards the upper

Fig. 2, part of the apparatus, the heating of A
was suspended and all the iodine reentered the flask. The apparatus

1) R. Lorenz. Die Elektrolyse geschmolzener Salze.
2) R. Lorenz. Die Elektrolyse geschmolzener Salze Il, 77.

480

gave great satisfaction. Not a trace of vapour was lost and by adding

every time weighed quantities of SnI, or I and starting from the
pure components or of a mixture of naan composition, a whole
series of determinations could be carried out.

The temperature was recorded by means of a previously stand-
ardised thermo-couple of silver-constantan which was plunged into the
boiling liquid.

The results are united in the following table.

Composition of the liquid.
| Boiling
gr. Snl, per | at. Sn per point.
100 gr. Snl,+1 | 100 at. Sn+I
0 0 183
10 2.02 184
20 | 4.04 187
30 | 6.05 190
40 8.06 193
50 | 10.06 198
60 | 12.06 204
70 | 14.05 214
15 | 15.05 | 219.5
80 | 16.04 228
85 | 17.03 | 249
90 | 18.02 267
95 | 19.01 296
100 | 20.00 | 340°

9. Finally, we endeavoured to determine the composition of the
saturated vapour which coexists with the different Sn I, — I mixtures.

For this purpose the liquid was heated to boiling in a 25 ¢.m.
long circular tube surrounded at its upper end by a thick asbestos
jacket. In the vapour space was then placed a long suction tube
with a pipette-like enlargement of 1—-2 c.c., capillarily drawn out
and bent upwards at the lower end. By means of this tube some
vapour close above the surface of the boiling liquid was withdrawn ;
this condensed for the greater part in the pipette and was then

481

analysed. Although these determinations have only a qualitative value,
we still think it worth while to communicate the result.

Composition of the liquid. Composition of the vapour.
Boiling
pase in °/) Sn in ,, Snl
0 ; ; o/ ire, ‘ ° 0;
by weight in at. 9/, Sn by weight in at.°/, Sn
185 13 2.6 2 0.4
189 27 5.4 5 1.0
201 55 11.0 14 2.8
210 66.5 13.3 is 3.6
230 81 16.2 28 56
270 91 18.2 48 9.6

Summary of results.

1. The melting point of Snl, is 143,°5, the boiling point 340°.
The melting point of SnI, is 320°, the boiling point 720°.

2. In the action of Sn on I, there is at first an exclusive for-
mation of SnlI,. The reaction SnI, + S5n—25nl, takes place with
extreme tardiness and even at 350° it still proceeds at a very
slow rate.

3. The melting point line of mixtures of SnI, and I consists of
two branches with a eutecticum at 79°,6 and 60 °/, by weight of
Snl, (12,06 at. °/, Sn). The boiling point line takes a regular course
without a maximum or a minimum.

4. Fused SnI, and SnJ, form two liquid layers, the composition
of which at 350° is: SnI, with traces only of SnI, and SnI, with
at most 6°/, of SnI,. As Sn also is not perceptibly soluble in molten
SnI,, this lies in a very narrow region of homogeneous mixing
which, at 350°, extends from 33,3 at.°/, Sn (pure Snl,) to 32,5 at.
°/, on (SnI, + 6 °/, by weight of Snl,).

Inorg. Chem. Laboratory
Technical High School.
Delft, Jane 1912.
32
Proceedings Royal Acad. Amsterdam. Vol. XV.

482

Chemistry. — “The distribution of dyestuffs between two solvents.
Contribution to the theory of dyeing.” By Prof. W. Rernpers

and D. Lrety Jr. (Communicated by Prof. F. A. H. Scarere-
MAKERS.)

(Communicated in the meeting of September 28, 1912).

For the explanation of the absorption and retention of dyestuffs
by fibres there exist three theories; the chemical theory, the theory
of solid solution, and the mechanical or adsorption theory.

According to the first theory ') the colouring matter enters into a
chemical reaction with a constituent of the fibre with formation of
an insoluble product, which is retained in the fibre. This constituent
—according to Kyecut, lanolinic acid in wool and sericinie acid in
silk — is supposed to have the character of an amphoteric electrolyte
and, therefore, to be capable of forming a salt with the base of the
basic dyestuffs as well as with the acid of the acid dyestuffs.

An important argument in favour of this theory is the observation
that when dyeing with basic dyestuffs there first occurs a dissociation
into base and acid, the former then being absorbed by the fibre and
the latter retained in the bath.

But it appears, however, that this dissociation also takes place in
the absorption of dyestuffs by cotton, by pure cellulose *) and by
inorganic matters such as glass, asbestos, silicates*), and carbon ‘*)
in which substances we surely cannot assume the presence of an
acid capable of forming a salt with the dissociated base.

Moreover, the occurrence of such a dissociation in the case of acid
dyestuffs is still doubtful *), and it also does not take place with the
substantive colouring matters which are absorbed in their entirety.
The chemical method of explanation is here a complete failure.

We also might be led to expect that the amount of colouring
matter that can be absorbed by a certain fibre would be determined
by the quantity of acid or base in that fibre. Only so much colouring
matter ought to be taken up as is equivalent to this content in acid
or base and a further addition of colouring matter to the bath should
not cause any further absorption of the dyestuff by the fibre. More-

1) Knecut, Berl. Ber. 21, 1556, 2804; 22, 1120 (1889). Surpa, Sitzungsber. der
K. Akad. d. Wiss. Wien. 113 Ifg, 725 (1904); Z. f. angew. Chem. 1909, 2131.

*) Knecut, Fiirberzeitung 18, 22 (1893/94).

°) Georatevics, Fiarberzeitung 19, 9, 129, 188, 286 (1894/95).

*) Freunpucn und Losev. Z. f. physik. Chem. 59, 284 (1907); Losev, Inaug
Dissert. Leipzig 1907, p. 45.

5) Losey, 12. p:~ 67:

over, the formation of the insoluble precipitate in the fibre could only
start when a certain concentration had been attained in the bath.

Neither of these phenomena have, however, been observed. ‘The
absorption of the dyestuff increases regularly with ifs concentration in
the bath and there is no question of a discontinuity in this absorption.

The chemical theory is, therefore, an improbable one and is, in
fact, rejected by the majority of the investigators of dye absorptions.

The theory of the solid solution has been proposed first by O.
N. Wirt?) and was at first universally accepted. Wirt, by a number
of examples has rendered it indeed plausible that the condition in
which the colouring matter is present in the fibre is perfectly com-
parable with that of a substance in solution, that there is an equi-
librium between the dyestuff in the fibre and in the aqueous solution
and that the changes in that equilibrium, caused by the addition of
another solvent such as alcohol, or of acids or salts, agree qualita-
tively, exactly with those in the equilibrium between two non-miscible
liquids in which a third substance is dissolved.

In the quantitative investigation as to the distribution of the
dyestuff between the fibre and the bath, it has been found,
however, that this distribution does not take place according to
Henry’s law, but that the adsorption-formula == act must be
applied.

Mainly on account of this, WaLker and AppLEyArD*) as well as
Scumipt*), Frreunptich and Losrv *), Groreievics *), PELet-JOLIvET °)
and others conclude that Wirt’s theory cannot be correct and that
the colouration is, in the first instance, an adsorption phenomenon ‘).

Hence, a very high value is attached to this utterly empirical and
very elastic formula, which in FReonpricn and Losrv’s determinations

1) Fiirberzeitung 1890/91, 1.

2) Journ. Chem. Soc. 69, 1334 (1896).

3) Zeitschr. f. physik. Chem. 15, 56 (1894).

4) lc. and Freunpiicu, Koll. Zeitschr. 3, 212 1908).

B} le:

6) L. Pexet-Jouiver, Die Theorie des Fiarbeprozesses, 1910.

7) According to Freunpuicu and Losev the fixation of the dye after its absorption.
tikes place because the colouring matter was either dissolved in a colloidal state
and then rendered insoluble by coagulation by the fibre (in the case of substantive
dyes), or was dissolved molecularly but converted in the fibre into an insoluble
or colloidal non-diffusing substance. As regards this last change the action of
another adsorbed substance (the mordant) or of the fibrous matter would, however,
have to be considered eventually.

Peter-Jouiver also regards the fixation of the dye chiefly as a coagulation of
colloids.

32*

484

had actually to be modified so as to agree with the figures obtained.

The question now arises whether this is really justified.

Is the compliance with this formula really such a certain criterion
for the presence of a surface condensation, or can we meet with a
similar relation in the distribution of a dyestuff over two non-
miscible liquids ?

Again, are the other properties of the dyed fibre in harmony with
the adsorption theory ? Is the colouring matter really present at the
surface only or must we assume that it has penetrated also in the
interior of the same ?

We will consider these questions successively.

How is the dyestuff distributed in the fibre ?

Some years ago this question was fully discussed by Hueo
Fiscuer'), who has most strongly protested against the implicit belief
in internal surfaces in colloids. He calls attention to the fact that
with starch granules, for instance, the colouration is perfectly homo-
geneous and argues in detail and on several grounds that the assump-
tion that we are dealing with an adsorption is very improbable. He
points out that the appearance of the coloured granule as wellas the
progressive change of the colouring process with a slowly acting dye
stuff such as congo-red makes altogether the impression that this colou-
ration is a phenomenon of solution and not a surface condensation.
Svipa *) in his investigations on the dye absorption of starch granules,
also states that they are coloured quite homogeneously. The fact that
when a dyestuff in the solid condition has a colour different to that
of its solution, the fibre always presents the colour of the latter and
not that of the former*) also shows that the dyestuff is present ina
condition which corresponds with solution.

In the case of several other phenomena which have been described
as adsorptions, a doubt now begins to arise whether this view is
really quite correct. Van BrmMeLen *) has already pointed out that.
with the gels the line between ad- and absorption is difficult to draw.
Davis *) found that the amount of iodine taken up by carbon increases
with the time of action. The iodine diffuses slowly towards the
interior of the carbon. Mc Bain °) noticed the same in the absorption

1) Z. f. physik. Chem. 68, 480 (1908).

*) Sitzungsber. der K. Akad. d. Wiss. Wien 113 IIp, 725 (1904).

8) O. N Wirz, l.c.

4) Z. f. Anorg. Chem. 28, 321 (1900).

6) Journ Chem. Soc. 91, 1666 (1907).

$) Z. f. physik. Chem, 68, 471 (1909).

485

of hydrogen by carbon and concludes that a portion is really adsorbed
and that another portion forms a solid solution.

GeorGinvics'), in his later investigations as to the absorption of
dilute acids by wool, has also come to the conclusion that in many
cases adsorption and solid solution occur together. From very dilute
solutions, acids as well as different colouring matters with a constant
division factor are absorbed so that this absorption may be considered
as a true solid solution.

Adsorption and solution, therefore, go hand in hand and in most
eases it is difficult to make out what part appertains to each of
these phenomena.

When the nature of the absorbing material causes the diffusion
towards the interior to take place with extreme difficulty, as in the
ease of carbon and silicates, the formation of a solution will take
place in the external layers of the substance only and one will get
the impression of dealing with a mere surface action or adsorption.
In some cases, however, it appears that the colouring matter has
penetrated further into the substance. Silicates coloured by fuchsine
and methylene blue exhibit a distinct pleochroism *), which shows that
the dyestuff has distributed itself homogeneously 7to the silicate and
has not deposited merely on the surface.

Cases of true adsorption will occur when the snbstance is dissolved
in the colloidal state and does not dissolve molecularly in the absorp-
tion medium. We may then expect either no absorption at all or a
complete absorption as colloidal solid solution, or else a complete
separation of the colloid at the border layer; this then constitutes
adsorption. Instances of this are found in the adsorption of colloidal
gold by carbon or by BaSO,*), of As,S,-solution by carbon or by
BaSO,, of a very fine carbon suspension by paper‘) and also in the
dyeing of wool or cotton with some undoubtedly colloidal dye
solutions such as that of the blue acid of congo-red. This colouration
however, is not permanent and can be completely removed by washing’).

How does a dyestuff distribute itself over two solvents?

In this direction but few determinations have been made. Only
in the case of picric acid the distribution between water and

1) Koll. Zeitschr. 10, 31 (1912),

2) 'T. Cornu, Tschermak’s Mineralogische und Petrographische Mitteilungen 1906,
453.

3) L. Vanino, Berl. Ber. 35, 662 (1902).

4) Sprinc, Beobachtungen iiber die Waschwirkung der Seifen. Koll. Zeitschr.
4, 161 (1909).

5) Petet-Jouiver, Die Theorie des Fiirbeprozesses, p. 141

456

various organic solvents such as amyl alcohol, benzene, chloroform,
bromoform ard toluene has been investigated and it has been found

Alcohollayer
400

380
360
340
320
300
280
260
240
220
200
180
160
140
120 y
100 Ae ylene pe D ea
80 a
60
40

———
—
et ie

Crystal ponceau
2S = — pee ots ae Ee

100 200 300 400 500 mgr/L
aqueous layer

that on increasing the concentration an proportionally smaller part
remains in the aqueous layer’). With methylene blue, between
- aniline and water, the division coefficient is constant *).

We have now measured for a number of dyestuffs the distribution
between water and isobutyl alcohol (b.p. 106°). The determination
of the colouring matter was effected colorimetrically. The temperature
was 25°. The results are united in tables 1—19. The concentrations
are indicated therein in mgs. per litre.

From these tables and better still from the curves in fig. 1 it
appears that with all these colouring matters, the division coefficient
Ca

decreases with the increase in the concentration. If the adsorption
Cw

In ; 1 ae:
relation Cq = one is applied we find that — varies from 0.3 (with
7
erythrosine A) to 1 (alkali blue and crystal ponceau). In most eases,
however, this exponent increases with the rise of the concentration.
This result is surprising. As the investigations of recent years have
1) W. Herz, Der Verteilungssatz, Sammlung chem. und chem.-techn. Vortrage
15 (1909).
*) Peter-Jotiver, Revue gén. mat. col. 1909, 249.

847

1. Methyleneblue G. conc. (Basel). 4. Methyleneblue D (Basel).
(Basic dyestuff). Neutral.
C | Ca | — |\logCw log Ca| — erate md
w | Gay oece es Cal Cu Ca Cw | ) log Ca n |
| | 1 ; - 7) = iy
1.6} 4.3] 2.70 || 0.20 | 0.633]| 6.8| 5.2| 0.76 |}0.832! 0.716]
| | || 0.56 | 0.72
5.8} 8.7} 1.50 || 0.76 vt 15.0 6.9 0.46 || 1.176 0.839)
15.4) 15 | 0.97 || 1.19 | 1.176]| 34 | 15.5] 0.45 ||1.531/1.190||
37 | 24 | 0.65 || 1.57 | 1.38 | 184 54 | 0.30 ||2.265! 1.732)”
78 | 50 | 0.64 || 1.89 | 1.70 || 460 108 0.24 ||2.663 2.033]
} | } |
1140 | 72 | 0.51 || 2.14 | 1.85: || $1
| 0.72
464 | 156 0.34 | 2.66 2.19 |)
| | i
5. Methyleneblue D.
: With 2 equivalents of HCL.
2. Methyvleneblue G. conc.
Aqueous layer 0.33 n. HCl. ie } Py. a ,
Cw Ca — |logCwilog Cal} —
| Ca 1 w || | ae
Cece Ca | cw loeCw og Cal =r = —<—<———— —
| | 7 7.5 1.07 || 0.845 | 0.875||
i | | 0.65
0.32 2.27 7.09 0.505-1 0.356 15 10.5) 0.70 |} 1.176 | 1.021 ||
| 0.75
or 9.0 | 2.75/0.505 | 0.954 38 22.4 0.60 || 1.580 1.350 |
| | | )
FPG) 22-5 |-1.95)'1.064 | 1.352]! 165 79 0.48 ||2.217 | 1.898
| 1 ar | 0.84
29.6 | 43.0 | 1.45/|1.471 | 1.642 440) 192 0.44 || 2.643 2.283 ||
| : |
130 86140 1.08,2.114 | 2.146
304 2680.88 2.483 2.498||
Sa ang
6. Fuchsine.
(Basic dyestuff).
3. Methyleneblue G. conc.
Aqueous layer 0.003 n. KOH. ae rer beat MCE ee
Cw | Ca a a log Ca} —
| | |
é
Cw Ca = logCw log Cal a — er =
Cw | | 7 | _ |
— oon e fens ) 24e 0. .87-1 1.25
0.4
4.0, 18.0 4.50 | 0.602 1.255 | 2:5.) 735" |‘) 14-0 0. 40 1.54
| 0.75 4
9.0. 32.5 3.61 || 0.954, P. 5k 8.0 62 7.75 }0.90 1.79
25 | 70 | 2.80 |}1.398|1.875|| 24 | 103 | 4.30/1.38 | 2.01
120 |200 | 1.67|}2.079|2.301]| ” 110 320 © 2.91|12.04 | 2.50
} | , | Out
300 (500 | 1.67 ||}2.477 | 2.699 320 620 42.0 | 2.79

488

10. Crystal ponceau.

7. Fuchsine. (Acid dyestuff).

With 7 equivalents of HCl.

eae a J
Cw Ca — |ogCw log Ca — | | Cw Ca a log lg Ca ae
| ) |
| 5.3 42] 8.0 \o.724 1.6281 ea 20 | 1 fone 1.301 0.00 he
| | ¢ ? OO
| 14 118 | 8.4 |] 1,146 | 2.072 | 49 1.7 0.0351! 1.690 | 0.230
| 25 | 232 | 9.3 |/1.398 2.365|| 195 | 6.0 0.031|/2.290 0.778|| ”
52 | 450 | 8.65 |/1.716|2.653|| ~ 480 | 15.0 0.031 ||2.681 1.176]| ”
| : » |
‘140 | 1108 | 7.91 2.246) 3.045
| |
8. Crystal violet (Basel). : ;
(Basic dyestuff). 11. Patent blue (Hochst).
(Acid dyestuff).
Ca
Cw |.Ca | — |logCwilog Ga. — C.
| Cw | Gy) Ge he logCwllog Cal
| i Cw n
0.9} 17 | 18.9 |0.95-1) 1.23 .
| | 0.5 4.2, 1.0/0.24 || 0.62 0.00
2.0) 25 |12.5 |0.30 | 1.40
| | 8.5] 2.1/0.25 || 0.93 | 0.32
5.3| 43.5 0.72 | 1.64 0.6
| 46 | 5.40.12 || 1.66 | 0.73
19.5|104 | 5.3 |l1.29 | 2.02 0.82
| 184 | 18.0.0.098!| 2.26 | 1.25
100 |360 | 3.6 |i2.00 | 2.56 ~ ae
| | : 0.9 410 | 45.4|0.095|| 2.67 | 1.66 |
245 820 | 3.35]/2.49 | 2.91 1.25 |
ie | 1140 150 |0.13 || 3.06 | 2.18
22 5 17 2.57 a
50 13 0. 3.35 | 2.
9. Neufuchsin (Hochst).
(Basic dyestuff).
| G
Cw | Ca a logCw log Cal =
—— 7 i 12. Erithrosine A. (Hochst).
| Acid dyestuff).
2.0| 12.5] 6.5 || 0.30 | 1.10 Oe ee
0.5 a
4.0, 17.5 4.4 || 0.60 | 1.24 cw \ca | lhoeculos ea
Cw | n
9.4, 30 | 3.2 || 0.97 | 1.48
“al | |
28 | 68 | 2.4 || 1.45 | 1.83 1.4) 14.0) C720: Hee t4e 08
120 | 250 | 2.1 || 2.08 | 2.40 4.0) 16.8 | 4.2 ||0.602) 1.225 |
|
290 | 600 | 2.1 || 2.46 | 2.78 10.7| 23.4 | 2.2 ||1.020/1.369|} ”
780 1560 2.0 || 2.89 3.19 | 38.5| 27.7 | 0.72 |/1.587/1.44211 ”
1600 3000 1.9 113.20 3.48 178 | 42 | 0.24 ||2.250| 1.6231) ”
| 1.0 |
3200 5700 1.8 || 3.50 3.76 460 | 63 | 0.14 ||2.663/1.799]| ”

13. Roccellin (Basel).

(Acid dye stuff).

=) | Ca
Cw | Ca ie HogCalog Ca =
| | |e
1.62) 11.77) 7.27 |/0.210 1.061 |
| 0.52
4.38 19.5 4.45 |0.641 1.290/)
| 14.2 | 42.6 3.0 ]1.152/ 1.6291]
30.4 | 73.6 | 2.4 11.483! 1.867||
65 |138 | 2.1 |I1.813 2.140]
| | | 0.80
179 300 ras [eee ea
| S ae se
14. Quinoline yellow (Fr. Bayer).
(Acid dyestuff).
Ca || | 7
Gr} Ca = |logCw log Cal os
Go [eee re al“
| | cece |
11.5) 18 | 1.60) 1.06 | 1.25 |
| HO
123 | 38 | 1.64 |] 1.36 | 1.58 ||
} :
60 100 | 1.67 || 1.77 | 2.00 ||”
}120 | 200 | 1.67|| 2.08 | 2:30 ||”
a | 425 | 1.7 || 2.38 | 2.63 ||”
630 | 964 | 1.53 |] 2.79 | 2.98 ||
15. Quinoline yellow.
With 10 equivalents of HCL.
-
Cw | Ca ad logCu tg Cal al
Go [Peele a
6.5} 36| 5.5 | 0.81 | 1.56
| | | 1 : 0
12.5| 74| 6.0 || 1.10 | 1.87
31 | 200 6.45) 1.49 | :
61 | 390 | 6.40 || 1.78 | 2.59 | ;
125 | 800 | 6.40 || 2.10 | 2.90 || ”
320 2) 6.39 || 2.51 24) i
|

489

16. Quinoline yellow.

With 10 aequivalents of KOH.

ool Ga | lhnete lone
Ww a nae) oO
Cw | soba Pied
1 | 17 |1.40l} 1-08 | 1.23]
| BG i!

25 33, | 1.92']| 1.40 | 1.52
70 | 80 | 1.14 || 1.84] 1.90 ]| ”

140 | 160 | 1.14 |] 2.15 | 2.20] ”

280 | 320 | 1.14 | 2.45 | 2.51 fs

720 | 800 | 1.11 || 2.86 2.90 | :

— — = = | — | a

17. Alkali blue 6 B. (Bayer).
(Acid dyestuff).
ba ier einen
25

Ca |= Ca Cw Ieee log oF =
7.9 105 | 13.3 ||0.897| 2.021 ||

feat 212+ 1-14.01), t- £79 2 326 |

30.2 | 425 | 14.1 il. .480 2. el 4

18. Congo-red (Bayer).
(Substantive dyestuff).

(Gaalte Ca | osteall : ieee
ie a C eee 4 aa
9.0 2.2) 0.24 lo. 954 0. -342|| |

| 7

19 3.3 | 0.17 || 1.2791 0.518

48 6.5 | 0.13 ||1.681|0.813]| ”

94 12 0.13 || 1.973/1.079]| ~”

180 | 21 0.12 |12.255/1.322]]} ”

480 | 42 0.09 | 2-681 1.623]| ”
19. Congo-red.
With 4 equivalents of KOH.

ae Ca || Bente

Ew | Ca a liege Si
6.6| 2.4 | 0.36 0.819 0.380 a

17.4) 5.4 | 0.31 ||1.240/0.732]] ~

44 | 10 0.23 1.643 1.000]} ”

180 | 27 0.15 ||2.255/1.431}} ”

456 0.13 | 2.654 TBI.

490

shown that different dyestufis, particularly the basic and the acid ones,
are dissolved molecularly in aqueous solution and, as shown by the
conductivity of those solutions, are fairly strongly dissociated electro-
lytically, whereas the dissoviation in alcobolic solution is but trifling,
ae might expect that the transition into the alcohol layer would
inmerease with a rise of the concentration.

In order to explain this small exponent we can make different

suggestions :

4. The molecular size of the colouring matter is greater in the
aqueous solution than ia the alcoholic one.

This view finds support in the determinations of Krarrr*) on the
lowering of the freezing point in aqueous and alcoholic solution.
From these the following molecular weights are deduced:

in water in aleohol — theoretical
Fuchsine 520—617 320— 344 oor
Methyl violet 804—870 403—421 408
Benzopurpurin 38000 — 724
Diamine blue 3430 —- Shs,

Hence, the two first basic dyestuffs would possess in water twice
as great a molecular weight as in alcohol. These determinations,
however, are not in harmony with the measurements of the con-
ductivity power of most of the dyestuffs, dissolved as salts, which
is about equal to that of a strongly dissociated binary electrolyte.

2. The dyestuff (BS) in aqueous solution is partly dissociated
hydrolytieally. By the alcohol the neutral ‘molecules are strongly
absorbed, the ions are not. In the case of a basic dyestuff the mols.
BOH ana BS therefore pass into the alcohol layer.

The hydrolysis equilibrium can be written as

B: + H,O @ BOH + H-:
hence
CBOH X cit = #, ¢B-
or also, because
cCROH = CH
cBoH = V&, ¢2

To the ordinary electrolytic dissociation of the dye salt applies

the formula:

Cy, = k, CB < i — ke CR

1) Berl. Ber, 82. 1608 (1899).

49]

If for the dye salt in the aqueous solution, we take it for granted
that there is practically a complete dissociation, the concentration of
the dye in the aqueous layer C, may be considered as equal to
cg. If now we eall the division coefficients for the molecules BOH
and BS 4, and /, we obtain:

Ca = ky cpon + &, cuz = Kk, Ch + K, C

The first term will be of influence particularly with small con-
centrations; the second will apply more in the case of increased
concentrations.

1
On applying the adsorption formula, — _ will, therefore, increase
nr
with the rise of the concentration. It will start with a value <1
then become = 1 and may subsequently rise to above 1. The line
indicating the dependence of the concentration in the alcohol layer
on that in the aqueous layer will at first turn its concave side down-
wards, then exhibit a point of inflexion and finally turn its concave
side in an upward direction.
Sou $0): 1
A similar variation of — has indeed been observed with a great
n
many dyestuffs even though with most of them no higher values than
1 were obtained. Only with ‘patent blue” this value was exceeded

1
and — rose to 1.3.
7

In agreement therewith it also appears that in the case of basic
dyestuffs, the transition into the alcohol !ayer is promoted by addition
of a base and in the case of acid dyestuffs by addition of an acid and
in such a manner that finally everything passes into the alcohol
layer (see Table 20).

Reversely, however, by adding acid to a basic dyestuff, or a base
to an acid dyestuff, the transition thereof into the alcohol layer is not
diminished. Frequently, this even causes an increase in the concen-
tration of the alcohol layer.

This may be partly explained by the diminution in the hydrolysis,
and the increase in the concentration of the non-dissociated salts
caused thereby. From the changes in colour on increasing the
concentration of the acid added, it seems, however, that the reactions
are often much more complicated.

Let us take as an example crystal violet. This is a_ basic
dyestuff. Formula {(CH,), N .C,H,}, C = C,H, = N(CH,), Cl. In a
neutral or faintly alkaline solution the colour is violet. On addi-
tion of acid the colour turns blue, then green and with still

492

PA BLES 20:

Name of dye.

Distribution in
neutral solution

Distribution in
acid solution

Distribution in
alkaline solution

Methylene blue
(basic dyestuff).

Crystal-violet
(basic dyestuff).

Chrysoidine
(basic dyestuff).

Fuchsine
(basic dyestuff).

“Neufuchsin”
(basic dyestuff).

Erythrosine
(acid dyestuff).

“Wasserblau blau-
lich” I

(acid dyestuff).

Rose Bengale

(acid dyestuff).

Quinoline-yellow
(acid dyestuff).

Eosine
(acid dyestuff).

Roccelline
(acid dyestuff).

Patent blue
(acid dyestuff).

Crystal-ponceau
(acid dyestuff).

Congo-red

(substantive dyestuff).

Alkali blue 6 R.
Forms a colloidal
solution in water,
but littie coloured,
reddish blue and
opalescent.
“Indulin spritlis-
lich?
In water an almost

| hol

| tribution.

Both layers about | Same asinneutral
_ solution.

_ equally blue.

Much more in the -|

alcohol layer. Both

| layers violet.

Alcohol layer dark
yellow to brown.
Bottom layer pale
yellow.

More in the alco-
hol layer. Both
layers red.

More in the alco-
layer. Both
layers red.

About equal dis-
Alcohol
layer more orange

| like, the aqueous

| layer more red.

About equal distri-
bution ; both layers
blue.

Equal distribution.
Alcohol layer yello-

wish brown, aqueous

layer orange.

Equal distribution;

both layers yellow.

colourless colloidal

Se oe ee

About equal dis-
tribution.

Both layers red.

Most in the alco-
hol; both layers
blue.

Little in the alco-
hol layer ; aqueous
layers red.

Both layers red.

Alcohol layer dark
blue; aqueous so-
lution colourless.

All with blue co-
lour in the alcohol
layer; aqueous layer
colourless,

More in the alco-
hol layer. This is
violet, the aqueous
layer green.

Same as in neutral |

solution but the
colour is more
brownish.

Most in the alco-

is much darker.

Most in the alco-
hol layer. Colour
red.

All in the alco-
hol layer. Colour
orange.

Much more inthe

alcohol layer, blue. |

All in the alcohol |

layer; light brown.

Much more inthe |

alcoh. layer; yellow.

All in the alcohol
layer ; yellow.

All in the alcohol
layer ; red.

All in the upper
layer. The colour
slowly changes to
mauve.

All in the alcohol
layer. Colour violet.

All in the alcohol
layer. Colour dark
yellow.

_ The colour vanishes.
hol layer. Colour |

All dark brown in
the upper layer.

As in neutral solu-
tion.

All in the alc. layer.
Colour orange,after-
wards colourless.

Much more in the
alcohol layer; red.

Much more in the
alcoh. layer ; yellow.

As in neutral solu-
tion.

Both layers red but
much darker than in

_ neutral solution.

Upper layer dark- |

er, aqueous layer
more greenish.

Much more inthe
alcohol layer.

All in the aqueous
layer. Dark blue.

Little in the alcohol
layer; aqueous layer

_ more brownish.

Blue deposit on |
the plane of de- |

marcation.

As in neutral so-
lution. Aqueous
layer § somewhat
tinged.

Nearly all in the |
alcohol layer, blue; |

aqueous layer some

| what tinged.

All in the alcohol
layer ; red.

All in the alcohol
layer with slight
reddish colour.

All with violet co-
lour in the alcohol
layer ; aqueous layer
colourless.

pree Sl

493

more acid yellow. From these solutions, however, it always passes
into the alcohol layer with a violet colour. The only explanation
we can give is this, that the dye adds an H-ion to its 2-valent N-
atoms. These additive products might then be blue, green, or yellow,
the non-dissociated salt, however, violet. In the alcohol layer the
H-ion concentration is much less than in the aqueous layer and so
these additive products are formed with -more difficulty. By a large
excess of HCl the upper layer turns green also. The green solutions
also regain their violet colour by strong dilution : the added hydrogen
ions are again split off by dilution.

“Patent blue” exnibits a similar behaviour ; a very little acid causes
the concentration in the alcohol layer to increase, on addition of more
acid it again decreases, while the aqueous layer turns first green
and afterwards yellow. When the aqueous layer is already yellow,
the alcohol layer is still green.

The influence of acid and base was investigated quantitatively
with methylene blue, quinoline-yellow and fuchsine.

From table 1, 2 and 3; 6—7; 14, 15 and 16 we notice that with a
large excess of acid or base the course of the division curve is quite
analogous to that in the neutral solution.

The influence of increasing quantities of acid or base is shown in
the following table where in the first column is indicated the number
of equivalents of acid or base in solution with one equivalent of
eolouring- matter. The total quantity of dyestuff taken was always
the same.

fT Ace ED 20.

Methylene blue D with Cy Cale. | Ca: Cw
very much acid 130 149 1.08
8 eq. acid 140 120 0.86
4, 5 160 80 0.50
7 ae : 170 70 0.41
i. . 170 70 0.41
neutral 170 70 0.41
0.8 eq. KOH 170 70 0.41
ZG. - 150 86 0.57
G.2°3 : 128 160 1.25

| eee 7 90 300 3.33

494

If now we compare the distribution of dyestuffs between water
and aleohol with that between water and fibres or other absorbents
it appears that :

1. As in the case of the colour absorption by fibrous matters, the

; 1
so-called adsorption-equation in which — <1, also applies to the
nm

distribution beiween water and alcohol.

2. Addition of a base to the solution of basic dyestuffs and of an
acid to acid dyestuffs strongly promotes the absorption by fibrous
matter?) as well as the entry into the aleohol layer.

3. Wool and silk dyed with basie dyestuffs in which the base only
has been retained are very readily decolourised by extraction with
alcohol. The solubility of the free base, which in water is slight, is
large in the fibre and also in the alcohol *).

4. According to Losrv*) no dyestuffis absorbed by paper fibre from
a solution of crystal-violet when this substance is dissolved in butyl
alcohol, amyl alcohol, aniline, chloroform or anisaldehyde; the
absorption is perceptible from a solution in nitrobenzene, anisol, ethyl!
malonate or amyl nitrite and strong from the aequeous solution.

If now, we observe the distribution of this dyestuff between water
and those solvents it appears that with the first group of solvents it
practically disappears from the aequeous layer and that with the
second group it distributes itself somewhat evenly over the two layers.

Nitrobenzene makes the only exception as it removes nearly all
the dye from water although, according to Losgy, no colouring matter
is absorbed from it by paper.

This behaviour is now quite comprehensible if we look upon
dyeing as being tantamount to dissolving the colouring matter in
the fibre. For crystal-violet the fibre is a good solvent and water a
bad one; the organic solvents of the first group are good, those of
the second group are ‘bad solvents. In the distribution of the dyestuff
over the fibre and the organie solvent, less dyestuff will be absorbed
in the fibre and more will be retained in the solvent, according to the
greater solubility of the dyestuff in the latter. The division coefficient

fibre fibre org. solvent

—- will be the quotient of that between and ———_—_—.
org. solvent water water

5. Frevunpiich and Losey have found that the order of adsorption
is independent of the nature of the adsorption medium. With carbon

1) See i.a. Pevet-Jourvetr, Koll. Zeitschr. 2, 225 (1908).
*) Freunpiicn and Losey, loc. cit. p. 303.
’) Losev, Inaug. Dissert. p. 64.

eT. ee Oe Toe

495

as well as with silk, wool, cotton and cellulose the order of the
three following dyestuffs was: crystal-violet, “neufuchsim’, patent blue.

The same order, however, is noticed in the distribution of these
dyestuffs between water and alcohol. Here again is shown the great
analogy between the absorption of the dyestuff in fibres and the transition
of the colouring matter into another solvent, which leads to the
assumption that the absorbed dyestuff is present as a solid solution
in the fibre.

We, therefore, conclude that the dye absorption in fibres is mainly
a phenomenon of solid solution and that the assumption of a surface
adsorption is in many cases unnecessary and should, therefore, be
discarded.

Delft. Inova. Chem. Lab. Technical High School.

Mathematics. — “On loci, congruences and focal systems deduced
from a twisted cubic and a twisted biquadratic curve”. 1.
By Prof. Henprik DE VRrigs.

(Communicated in the meeting of September 28, 1912).

1. In the Proceedings of the Meeting of this Academy on Saturday
Sept. 30, 1911, p. 259, Mr. Jan pe Varies has investigated the locus
of the points sending to three pairs of straight lines crossing each other
three complanar transversals, and in the Proceedings of the Meeting
of Nov. 25, 1911, p. 495, Mr. P. H. Scuoure has made the same
investigation for the points sending to (n+ 2), pairs of straight
lines crossing each other (7+ 2), transversals lying on a cone of
order n. In the following pages one of the three pairs of lines will
be replaced by a twisted cubic, the two others by a quartic curve
of the first kind. Through a point P? one chord « of &* passes and
two chords 6 of £* pass; we ask after the locus of the points P for
which the line a@ and the two lines 6 lie in one plane.

We imagine a chord a of &*. Through an arbitrary point P of
this chord pass two chords 6,,6,* of &* and in the plane a, lies
one chord 6, which does not meet 6, on /* itself, in ab,* one such-
like chord 6,*; if for convenience sake we call the points of inter-
section of 6, and ,* with a both @, then in this way to each point
P two points Q correspond. However, it is clear that to each
point Q also two points P correspond, so that on a a (2,2)
correspondence arises with four coincidences, and for these it is evident
that the triplet a+ 2b is complanar. However, it is easy to see

496

that the four coincidences coincide two by two; for, if we call one
of the two chords 4 through such a point 6,, then the other is 6,,
but if we call the Jatter 6,*, then 6, 6,*, so that really the coin-
cidences coincide two by two. Furthermore it is easy to point out that
in general the two coincidences do not fall in the points of intersection
of a and £*; for, both chords 4 throvgh such a point will in general
not lie with @ in one plane.

So out of these considerations follows that @ intersects the demanded
locus outside /* in two more points; ¢f therefore we point out that
k* is a nodal curve, then we have proved that the demanded locus is
a surface 2° of order 6. Now through a point P of 4° pass two
chords 4 and in the plane through these lie two chords a; so each
point of 4° is a nodal point for the surface.

2. We again determine the order of @* by considering a chord
}, of &*. Through a point P of 6, passes one a and in the plane
ab, lies one 6,; if the latter intersects 6, in Q then to each point
P one point @ corresponds. Inversely through Q passes one 4,,
but in the plane 4,4, lie three chords a; so on 6, we find now a
(1,3) correspondence with four coincidences, and these do not coincide
two by two. For, through each coincidence passes one a and one 6,
but of course these cannot be exchanged. Neither does a single
coincidence fall on ‘4*; for through a point of intersection P of 6,
_and f* passes one a and the line connecting the two remaining
points of intersection of plane ab, and £* does of course in general
not pass through P. So a chord of £* cuts 2° outside £* in four
points more; therefore k* is for 2° a single curve.

This last result has something unexpected, for if we regard &* by
itself we arrive at quite a different result. Through a point P of &
passes one a and in an arbitrary plane through this lie three chords
6 through P; so that each point of 4* regarded by itself satisfies the
given question an infinite number of times; if however we also take
into consideration the points outside 4°, then we find according to
the above mentioned a surface 2° for which 4‘ is only a single curve.

That 4* is just a single curve is made clearer by the following
consideration. The curve /* is the section of two quadratic surfaces
®,, ,, and the plane of the two chords 6,,6, is at the same time
the plane through P and the line of intersection s of the two polar
planes a, a,, of P with respect to ®, and ®, ; if now P falls exactly
on é*, then a,, a, become tangential planes in P to ®,, ®,, so their
line of intersection s becomes the tangent ¢ in P to &*; among all
the planes through ? only those through ¢ come into consideration,

497

and as now the plane throngh ¢ and the chord a through P is deter-
mined unequivocally, and as in this plane only two chords @ lie,
point P counts only once.

3. Through /* pass four quadratic cones whose vertices we shall
eall 7’ ....7',. These vertices too behave themselves somewhat irregularly
with respect to the question put originally, for an arbitrary plane
e.g. through the line @ passing through 7’, contains always two chords
b, so that also the four vertices of the cones regarded by themselves
satisfy the given question an infinite number of times; nevertheless
these points are for 2° only single points.

This can be proved most easily with the aid of the edges of the
tetrahedron 7’,....7’,. Let us consider e.g. 7,7’, and let us_ regard /*
as the intersection of the two cones having 7) and 7’, as vertices. All
points P of 7,7, have with respect to the first cone only one polar
plane z,, viz. the plane 7,777, and likewise with respect to the
second cone only one polar plane 2,, viz. 77,7, ; the line of inter-
section 7,7’, is therefore the line s forall points ? of 7, 7,, or in other
words the planes Ps (or Pb,/,) for all points of 7,7, forma pencil
of planes around the edge 7,7’, The question is to find the points
P of T,T,, for which the chord a of é° passing through / lies in
the plane Ps and to this end we have but to intersect each plane Ps
by 4*, by means of which we find in each suchlike plane three
chords a forming altogether a scroll &* of order four with # as
a nodal curve and s as a single directrix. For, through a point of s only
one chord a passes, whilst in a plane through s three of suchlike
chords are lying, and through a point of &° evidently two chords a
pass intersecting s. Now this scroll 2* intersects 7’, 7’, in four points,
but to these 7’, and 7’; themselves do not belong, because no reason
whatever can be given why of the three chords a in the plane 7, 7,7’,
e.g. just one should pass through 7; so we find on 7’, 7, four points
of intersection besides the two vertices of the cones, and as the latter
of course likewise belong to the surface they count once on 7,7,
and therefore likewise in general.

If we determine the points of intersection of 2° with the chord a
through 7, then we find that the two points which this chord has
outside /* in common with the surface (§ 1) coincide with 7,, which
with a view to the preceding means that a touches the surface in 7}.
We endeavour also to acquire on this specia! chord a@ the (2,2)
correspondence of § 1, which is easily done and where we have but
this to remark, that in the plane 4,4, as well as in the plane 6,*4,*
the four points of &* lie two by two on two lines through 7’. If

Proceedings Royal Acad. Amsterdam. Vol. XY.

498
now the point of intersection P? of 6, and a is to coineide with the
point of intersection Q of 6, and a then the four points of £* in the
plane ab,), must form a complete quadrangle with P and 7’, as two
of the three diagonal points, and this is only possible if the ne oS
thus a, lies on a special cone of order two, which will in general
not be the case. In an arbitrary plane through 7, le namely four
points of £*, forming a complete quadrangle ; one of the three dia-
gonal points is 7’,, the two other ones lie in 7,77, and evidently
describe here when the plane varies a conic through 77, 7,,7,. If now
a happened io lie on the cone projecting this conic out of 7,, then
two coincidences of the (2,2) correspondence would lie on the conic
and the two others in 7,; in every other case however all four
coincidences must coincide in 7), and so a must touch the surface

San 7,

4. We now proceed to determine the points of intersection of
2* with an entirely arbitrary line 7. To that end we allow a point
P to travel along the line / and we investigate how often the chord
a passing through P lies in plane Ps. According to § 3 the chords a
issuing from the points P of 7 form a seroll of order four with
nodal curve /* and single directrix /; the lines s belonging to the
points P of / form a regulus and the planes Ps envelope a develop-
able of class 3. If namely point P describes the line / then the two
polar planes a, and 2, of P with respect to ®, and #, (comp. § 2)
revolve around the two lines /7,,/, conjugated tu /, and crossing each
other in general; thus the line s describes a regulus with 1, and 1, as
bearers.

Now the surface enveloped by the planes Ps. We imagine an
arbitrary point V in space, we choose a point P on /, we determine
the corresponding line s and we find the point of intersection Q of
the plane Os with 7; in this manner to each point P one point Q
corresponds. If reversely we wish to know how many points P cor-
respond to @, we draw the line connecting O and Q and we
intersect it by the regulus of the lines s just found; through each
of the two points of intersection passes one line s whose corresponding
point P lies on /, so that to one point Q two points P correspond.
Between the points P and Q on 7 there exists a (1, 2) correspond-
ence; for the three coincidences the plane Ps passes through O;
so the planes Ps be longing to the pounts of a line l envelope a
developable of class three.

We now add to the figure an arbitrary plane a@ and we determine
‘the section of this plane with the scroll of order four, formed by

—

499

‘the chords of 4° resting on /, as well as with the developable just
found of class three; the former is a rational curve of order four
with three nodes in the points of intersection of @ and /* and a
single point in the point of intersection of « and /, the second a
rational curve of class 3 with a double tangent.

Through an arbitrary point of the curve of order four passes one
chord a, intersecting / in P, and through P passes one plane Ps,
so that in this way to each point of the curve /* of order four one
tangent of the curve &, of class three corresponds, whilst in the
same way we can see that to a node of /* two different tangents
of k, correspond. In the same easy way we can conyince our-
selves that to each tangent of 4, one point of /* corresponds and
to the double tangent two different ones; so the result is that there
exists a (1,1) correspondence between the points of 4‘ and the tangents
of #,; the question now is how many coincidences this correspondence
possesses.

Let us take a point P on £#* and jet us determine the corresponding
tangent ¢ of &,, cutting /* in four points Q; reversely through one
point Q pass three tangents f, and to each of these one point P
corresponds; so between the points ? and Q exists a (3, 4) corre-
spondence and, as the bearer is rational, the number of coincidences
is seven. One of these must necessarily be the point of intersection
of / and «; for, through this point taken as point P of /, passes a
chord a and likewise a plane Ps cutting @ of course according toa
line passing through P?, however without it being necessary for a
to lie in the plane Ps. So we have here a coincidence in the plane
« to which no incidence of @ into the plane /’s corresponds; if we
set this case apart six coincidences remain which are each the conse-
quence of a point of intersection of / and 2°.

For the sake of completeness we add to the preceding that the
regulus of the rays s belonging to the points P of / contains the
four vertices of the cones 7,,..., 7, (comp. § 3); for 7, has as
polar plane with respect to ®, as well as to ®, the plane 7,7',7%,
so inversely the two polar planes of the point of intersection of / with
this plane pass through 7, and so coes therefore their line of
intersection s.

The developable of the planes Ps is of class three, so through
each point P of / itself three planes Ps must pass; indeed two
rays s of the regulus cut / and to these two points P of / cor-
respond; so through / pass two planes Ps and these must for
each point of / be added to the plane passing through that point
but not through /.

33*

500

5. As we have seen before 4‘ is for the’ surface 2‘ a single curve,
j° a nodal curve, and the surface cannot contain other nodal curves
for, if a point 0 is to be a double point, then through this point either
more than one chord a or more than two chords 6 must pass; the
former is only possible for the points of 4°, the latter only for those
of J*, and these two curves we have already investigated. On the
other hand the surface contains a number of single lines crossing
each ether, as many as twenty; the chords of k* namely form a
congruence of rays (4,3), those of £* one (2,6), and these congruences
have according to the theorem of HarpHen 1.2 + 3.6 = 20 rays in
common. Through a point P of such a ray passes one chord a, one
chord 4 coinciding with a and one chord 4 more; so it is a single
point for 2°. Two of these lines cannot possibly intersect each other
outside £°, for in that case two chords a would pass through one
point, which is impossible; it is not impossible for them to intersect
on 2°, but this requires a peculiar situation of 4° and 4* with respect
to each other, which we will not presuppose.

An arbitrary plane through one of the twenty lines cuts 2°
besides in this line still according to a curve of order five which
has with the line in common its two points of intersection with 4°
but not those with 4/', because the latter are but single points for
the surface. However besides the two points of intersection on £*
the curve must have three points more in common with the line,
in which points the indicated plane must therefore touch the surface;
so the surface 2° possesses an infinite number of threefold tan-
gential planes, which are arranged in twenty pencils of planes, around
the twenty lines of the surface as axes.

7.8.9
1.2.3
in general single conditions; we shall investigate for how many
single conditions 4*, 4*, and the twenty lines of the surface count.
The curve £* must be a nodal curve; so we try to construct a surface
of order 6 having #* as a nodal curve. In an arbitrary plane @ we
assume eighteen points quite arbitrarily ; we determine the three

A surface of order 6 is determined by —1= 83 points or

points of intersection of «@ with 4°, and we construct a plane curve
of order 6 having these last three points as double poinis and at
the same time containing the 18 points above mentioned; as a double
point counts for tbree single data and a curve of order 6 is deter-
mined by 4.6.9=27 points, we have in @ just enough data to
determine the curve of order six.

In a second plane 3 we assume arbitrarily only 12 points,
and we add to these the six points of intersection with the curve

5O1

lying in @; then we can also find in 3 a curve of order 6 which
must lie on the surface. Finally in a third plane y we have now
of course to assume arbitrarily only 6 points and then the surface
is determined; for every arbitrary fourth plane cuts the three curves
lying in a, ,y together in 18 single points, and 4° in three points
which must be double points, by which the section of the surface
to be constructed is determined. Besides 4° we therefore want
18 + 12 + 6= 86 points to determine the surface; so the condition
that £? isa nodal curve is equivalent to 83 — 36 = 47 single conditions.

If #4 is to lie on the surface of order six, then we have to take care
that it must have twenty-five points in common with the surface ; so
k® as a double curve and £&' as a single curve absorb 47 +- 25 = 72
single conditions, so that but 85—72—11 conditions are left. Now
a common chord of 4? and 4* bas with every surface of order six
passing twice through /* and once through /* in its points of inter-
section with both curves exactly six points in common with this;
thus by distributing the eleven points which are left among eleven
of the twenty common chords, we can be sure that also these
eleven chords will come to lie on the surface. However, we know
that on our surface 2° all the twenty common chords lie; so we
can state the following theorem: the twenty common chords of k*
and k* lie on a surface 2° of order 6 passing twice through k* and
once through k*; it ts the locus of all the points of space for which
the triplet of chords a + 26 is complanar.

6. The first polar surface of an arbitrary pomt © of space
with respect to 2° is a surface 77,’ of order five passing once
through £?; the complete section with 2°, which must be of order
thirty, breaks up into /* counted twice and a residual section 7**
of order twenty-four, from which ensues immediately that the apparent
circuit of 2° out of an arbitrary point of space on an arbitrary plane
is a curve of order twenty-four.

The curve 7** has as is easy to see twelve points in common
with ?. The second polar surface of O, viz. a surface J7,* of order
four, does not contain /*, so it intersects it in twelve points; these
are the points which £* and 7?* have in common. If namely we connect
QO with an arbitrary point P of 77‘, then OP is a tangent in P of
2': now if P lies on &* then OP touches in P one of the sheets
of 2° passing through /?, but in consequence of this on the line
OP lie united in P three points of 2°, and therefore two of /7,, and
one of Jf,. Each of these twelve points counts for three coinciding points
of intersection of 2° with its two polar surfaces; for, if we intersect

502

yj? +724, the section of 2° and 7, by 7,, then every point of inter-
section with 4° counts for two, with r?* for one; therefore each of
the twelve points under discussion counts for three. As the complete
number of points of intersection of the three surfaces is 6.5.4 = 120,
outside £° there are 120—3.12— 84. lt is wellknown that the tan-
vents in these points to r** pass through QO: thus the apparent circuit
0 f 2° possesses eighty-four cusps.

To determine the class of 2° and with it of the circumscribed cone,
resp. the apparent circuit, we assume a second point O’, and we
coustruct the first polar surface 7/,’; this, too, passes through £*° and
intersects the curve 7?! just found in 120 points of which twelve
however lie on #*, and count singly, because 7** is a single section
of 2° and JF, and £* is again a single curve of 77,; so outside /°
the three surfaces have 120 — 12 —108 points in common, so that
the class of 2° amounts to 108.

By applying the Pricker formula rv = gu (u—l) — 2d — 3x to the
apparent circuit, we find

25 = uw (u—1) — vp — uz = 24.23 — 108 — 38.84

or
J = 96: ;

The projecting cone out of O contains therefore 96 double edges,
the apparent circuit 96 nodal points.

The PLtcker equation dualistically related :

u = v (vp—1) — 21 — 381,
applied to the apparent circuit furnishes us with
2x + 81 v (yp—1) — w = 108. 107 — 24 = 11532,
whilst the third formula: « — z= 3 (»—un) furnishes for t
e— 84+ 3(108—24) — 336;

so we find. 2x = 11532 —S.. 356 = 10524 s6r. c — a2e

Now however we have to remember that the planes through O
and the twenty lines of 2° are threefold tangential planes of the
cone, that their traces are therefore threefold tangents of the apparent
circuit and that therefore they count together for sixty double tangents.
If we subtract these from the entire number 5262, then for the uppa-
rent circuit remain 5202 real double tangents completed by 20. three-
fold ones.

A cusp in the apparent cireuit is generated by a principal tangent
a tangent with contact in three points) of the surface passing through
; these principal tangents form a congruence, of which according
to the above mentioned the first characteristic (number of rays through
a point) is eighty-four, The second characteristic indicates the number

503

of rays in a plane; in order to find this we have but to determine
the number of inflexions of a plane section of 2°. We have already
seen that this plane section is of order 6 and of class 24, and that it
contains 3 double points, whilst the number of cusps is 0; from this
ensues easily that the number of inflexions is 54, the number of
double tangents 192. the congruence of the principal fangents of
2° has therefore the characteristics 84 and 54, those of the double
tangents 5202 and 192.
7. Through each point P of 2° passes a plane 2, in which are
situated one chord a of %* and two chords 4 of /*; we wish to
study the surface which is enveloped by those planes 2. The class
of this surface ean be determined in different ways; we shall deduce
this number in the first place by asking how many planes 2 pass
through a chord a of 4°. Through the point of intersection A, of
a with k* passes one plane a which in general however does
not pass through a, and the same holds for the second point of inter-
section A,. Besides these two points a has still but 2 points S,, S,
in common with 2°, and through ‘hese passes a plane 2 containing
a; for S, eg. is a point of 2° exactly for this reason that the
chord a lies with two chords 4 of 4* in a plane x. So to each
of the two points S,, 8S, a plane a through @ corresponds.

However planes 2 can also pass through a without it being
necessary for the point of intersection P of the triplet a + 2/ to
lie exactly on a itself. If we make a plane e to rotate round a, it
contains in each position 2 more chords @ and 6 chords 6, forming
a complete quadrangle. The two chords a describe the two quadratic
cones by which &* is projected out of the two points A, , A,, the
diagonal points of the complete quadrangle describe a twisted curve
possessing in each plane « three points apart from the points lying
on a itself and which are nothing but S, ,.S,; so the diagonal points
form a twisted curve 4° of order 5 resting in 2 points S, ,.S, ona,
(and containing evidently the four vertices 7,,.., 7',, § 3). Let us
consider a point of intersection of this 4° with one of the just men-
tioned quadratic cones, we tien have evidently obtained a point of
2* and at the same time a plane 2 through a. Now 4° intersects
each cone in ten points, but among these are S, and S, ; so outside
a lie only sixteen points of intersection and if we again add SS, and
S,, counted once, we then find that the surface enveloped by the planes
x bearing a triplet a+ 2b is of class eighteen. We shall indicate
it by &,,.

As easily we can determine the class of 2,, by means ofa chord

504

h of £4. If it euts &* in B,, B,, we must bear in mind that these
points according to § 2 are for the surface £2° single points only, from
which ensues that through those points only one plane a passes
which comes in consideration if we make, as is done here, a point
P to describe the surface and if we ask after the surface to be
enveloped by the planes 2; this one plane however does not pass
in general through 6. Besides b,, 6, 6 has with 2° four more
points S in common; through each of these evidently passes a plane
a containing 6.

However, there are of course now again planes a through 6,
whilst point P lies outside 6. A plane 6 through 6 contains three
chords a and these describe when ~# rotates round 6 a seroll of
order four with /® as a nodal curve and 6 as asingle directrix (§ 3).
The plane @ contains moreover 6 chords of £*, of which however
one coincides with 6, so that one diagonal point lies on 6 and two
outside 6. These describe when £ rotates round 4 a twisted curve
of order four, resting in 4,, 6, on 6; if namely p touches £* in
B, or B,, it is easy to see that one of the two diagonal points lying
in general outside } coincides with the point of contact. This curve
of order four intersects the just mentioned scroll of order four in
sixteen points, to which however belong 5, and /, as these lie in
h and therefore on the scroll too; if we set these aside, because
they do not satisfy the question, fourteen are left, and these added
to the four points on 4, which do satisfy the question, give us again
the number 18.

We can also determine by the way followed here the eighteen
tangential planes of @,, through an entirely arbitrary line /. The
chords of 4° resting on / lie again on a surface of order four, and
the diagonal points of the complete quadrangles in the planes 4 through
/ lie on a curve of order five resting in two points on /; for, the
chord a of 4* which we discussed above is for /* an arbitrary line,
so it contains as many diagonal points as in the general case. The
curve and the surface intersect each other now in twenty points,
but to these belong the two points of intersection of the curve
with /, which do not satisfy the question; so there are again
eighteen left.

8. An arbitrary plane through one of the twenty common chords
of 4° and ** contains beside this chord, representing an a as well
as a /, one chord 4 more, cutting the other outside 4“, and therefore
it is a plane a to be counted once; so through each of the twenty
chords pass an infinite number of tangential planes of 2,,, from

505

which ensues that the twenty common chords of k’ and k* are single
lines of &,,.

The plane a issuing from a point of %° contains two chords a
and so if counts twice as tangential plane of 2,,, whilst reversely
it is easy to see that 2,, can have no other double tangential planes
than these; for, in such a plane must either lie two chords a,
which leads to the curve £*, or more than two chords /, which
is the case for the points of 4*, but as for the latter only the plane
through the tangent and the chord a comes into consideration (§ 2),
the last possibility disappears and only the points of /* are left.
The double tangential planes of 2,, are therefore the planes x
corresponding to the points of k*; they envelope a developable 4, of class 9.

In order to find this number we look for all the double tangential
planes passing through an arbitrary point 6, of 4‘. Such a plane
then must contain a chord of £* passing through #, intersecting 4°,
and it can thus be obtained for instance by intersecting 4* by the
eubie cone projecting £* out of £,, which furnishes 9 points of
intersection, or inversely by intersecting /* by the cubic cone projecting
k* out of the vertex 6,, which furnishes 12 points of intersection,
of which three however coincide with ££, and must be taken
apart. If now we call A such a point of intersection lying on /3
then really through this point passes one double tangential plane of
2,, containing point 4,; so the class of the developable is nine.

Through a point 4 of £* pass likewise 9 tangential planes of A, ;
for. one of these points A itself is the point from which start the
two chords 4 of &*, in the eight other planes on the other band
the chords / start from an other point; from this ensues that through
A pass altogether ten chords of 4* which start from the point of
k* and which at the same time lie in the tangential planes of A,
corresponding to those points; the locus of those chords is a surface
2” of order twenty for which lk? ts a tenfold curve.

For, an arbitrary chord of /° meets in each of its 2 points
of intersection with /* ten generatrices of the scroll to be found,
and is intersected outside 4* by no chords of 4°.

In a tangential plane of A, lie also two chords / intersecting 4’,
viz. in point A to which that tangential plane corresponds; Jet us
also ask after the locus of these chords 4. Through each point of 4°
pass iwo, through each point of /* nine, because (see above) the
cubic cone projecting /* out of that point is intersected by /* in
nine points; let us now determine the points of intersection of the
scioll to be found with a chord 4, of 4*, then of these in each of the
two points of intersection of 4, with /‘ lie nine united. If further-

506

more we make a plane £ to rotate round 6, then the chord 6, in that
plane, which cuts 6, outside £*, describes a scroll having six points
in common with £*; through each of these passes a chord 4, which
euts £° and b,; the scroll to be found is therefore a surface 2** of
order 2X 9+ 6= 24. It has k’ asa nodal curve and k* as a ninefold

CUrvVe.

9 The surface 2*° found in the preceding § possesses no other
manifold curve than #*. Each scroll of order 2 contains namely a
nodal curve which is cut by a generatrix in n—2 points, because a
plane through a generatrix contains as residual section a curve of
order n—1, and of the n—1 points of intersection of this curve
with the generatrix only one acts as a point of contact, so that all the
remaining ones are due to a nodal curve. Now a plane through a genera-
trix of 2*° contains a residual section of order nineteen with two
ninefold points on /*; these together form eighteen points of inter-
section of the generatrix with the nodal curve, so that the latter is
complete with %* only. On the other hand the surface contains twenty
double generatrices, viz. the common chords of k* and k*, as is easy
to see, and these same lines are double generatrices of 7+.

The surface 2%! contains besides the nodal curve /* and the ninefold
curve £* still a new nodal curve which is cut by each generatrix in
five points: for, a plane through a generatrix contains a residual
section of order twenty-three with two eightfold points on £* and
a single point on 4°, forming together seventeen points; so the gene-
ratrix must contain five points more of an other nodal curve. And
indeed, if we make a plane to rotate round a generatrix 6,, it then
possesses in each position still one chord 6, of 4* not meeting +,
on /*; this chord describes a regulus intersected by 4£* in six points,
of which one however coincides with the point of intersection of d,
and /*; through the remaining five passes every time one generatrix
of 2** meeting 4, outside 4° and 4*, thus in a point of the new
nodal curve.

We can find the order of this new nodal curve with the help of the
theory of the permanency of the number. We conjugate an arbitrary
generatrix of 2’* which we call g to all others which shall then
be ealled/, and in this way we find * pairs of lines gf to which
we will apply in the first place Scuupert’s formula:

£6 —2 .&B8 —2. 6g").
The letter ¢ indicates the condition that two rays g and h/ of a

1) Scuupert: “Kalktil der abz. Geom.”, p. 60, N°. 22,

— ee

SOT

par lie at infinitesimal distance without intersecting each other, 6
on the other hand indicates that they intersect each other without
coinciding; the combination «6 therefore indicates the number of pairs
the two components of which lie at infinitesimal distance and cut each
other at the same time. This can take place in our case as follows.
We know that the double tangential planes of /* are simply the
tangential planes of the four quadratic cones cutting each other in
k*; k* has with these four cones twenty-four points in common and
through such a point pass evidently two generatrices satisfying
the condition so and forming together one pair satisfying this con-
dition. These generatrices are the torsal lines of 2** and their points
of intersection with k* are the cusps. The surface 2** contains however
also twenty double generatrices, viz. the common chords of 4° and
i+, and these too must evidently be regarded as satisfying the indi-
eated condition; the number «6 is therefore — 20 + 24 — 44.

The symbol «g indicates the number of pairs of rays which
coincide and where g (or 4, which is of course the same) intersects
a given line; now that given line intersects the surface in twenty-
four points: so eg is twenty-four. We thus find:

2.e8 —~ so + 2.89 = 44 4+ 48 — 92,
so
E> == 46.

The symbol ? indicates the condition that the two rays of a pair
‘intersect a ray of a given pencil, thus the symbol «3 indicates the
condition that those two rays lie moreover at infinitesimal distance
withont intersecting each other; so the quantity «2 indicates in our
case evidently exactly the class of a plane section of 2**. If now
we remember that such a section contains in general no cusps, we
then find for the number of double points :

2d = 24. 23—46 = 552—46 = 500,
80:
d = 2038.

Now we know of these 253 double points the followmg: 1. the
three points of intersection with 4°; 2. the four points of intersee-
tion with £*, each. of which is a ninefold point and therefore absorbs
1.9.8—36 double points; 3. the points of intersection with the
twenty double generatrices, so together 3+ +.36 + 20 = 167 ;
the order of the new nodal curve is therefore 253 — 167 = 86.

A plane curve of order twenty-four can possess at most $ . 23 . 22
= 253 double points, just the number of our case: 2** is therefore
a rational surface,

508

We control this result by using a second formula of Scuusert

viz ').
op +89 + B= + gh + h,,

where op indicates the number of pairs whose components without
lying at infinitesimal distance intersect each other, whilst the point
of intersection lies in a given plane, thus evidently in our case
the order of the complete nodal curve, however taken twice, be-
cause each ray can be a g as well as an /, and therefore each
pair of rays satisfying the condition 6p counts for two pairs; gp
designates the number of pairs where the line g passes through
a given point, a number which is evidently zero in our case,
because all our rays belong to a surface and can therefore not
pass through a point taken arbitrarily; for the same reason we
find h, zero. On the other hand gh designates the number of
pairs where g intersects a given line /, and # a given line /,,
« number which in our case evidently amounts to 24.24 = 576,
because /, is intersected by twenty-four generatrices g, /, by twenty-
four generatrices /, and each line of one group can be joined to
each of the other. As eg—24, «846, op becomes 576—24—46=506,
and as the order of the nodal curve is half of it, we find back the
quantity 2538.

In the formula:

Ge + 8g + &8 = ge + gh + he,*)

which is dualistically opposite to the last but one, oe indicates the
number of pairs of rays whose components intersect each other
and whose plane passes through a given pvint. Now, too, each pair
we find is counted double, because each ray can be gy as wellash;
so ice is the class of the developable, enveloped by the double
tangential planes of 27'. The quantity gy, indicates the number of
pairs where the ray g lies in a given plane, and fh, indicates the
same for 4; both numbers are in our case evidently zero; and from

this ensues oe = op = 506, so that the class of the doubly cireum-
scribed developable of 2°* amounts to 20D.

For the sake of completeness we shall discuss in short the sur-
face formed by the chords of 4° resting on #£*. Through any point of
k* passes one, so that /* is a single curve: through any point of #°
on the other hand eight pass, because the quadratic cone projecting
k* out of that point is intersected by 4* in eight points; so #° is
an eightfold curve. From this ensues again that an arbitrary chord

aie. p. 60, iN 239
2) Le. p. 60, NO. 24.

509

of £* intersects the demanded surface in each of its two supporting
points with 4° in eight points and no more, because two chords of
k* cannot intersect each other outside 4°; the demanded surface is thus
of order sixteen, and it has k* as an eightfold curve, k' asa single curve.
That 4° is the only manifold curve follows again out of the cireum-
stance that two chords of 4° can meet each other only on the curve
itself; on the other hand the twenty common chords of k*® and kt are
again double generatrices. As an eightfold point counts for 4.8.7 = 28
double points, the complete number of double points of a plane section
is 3.28-+ 20=— 104; a plane curve of order sixteen can however
contain at most $.15.14—= 105 double points; so the sur face is of
genus 1.

10. Through a point 7? of space pass two chords / of k* situated
in the plane a through P and the line of intersection s of the two
polar planes of P with respect to the two quadratic surfaces ®, , @,
(§ 2) intersecting each other in 4*; we shall conjugate this plane a as
focal plane to P and we shall discuss the focal system that is formed
in this way. Lach point of space has then one focal plane (so
a=1")), with the exception of the points of k* having cw focal
planes, viz. all the planes containing the tangent in that point.

In order to find inversely the number $ of the foci P of an arbi-
trary plane 2, we intersect that plane with ®, and #,; this gives
rise to two conics /,?,#,?, and with respect to these we take the
polar lines p,,p, of an arbitrary point P of z. The polar planes of P
with respect to ®,, ®, then pass through p,,p, and the line s con-
jugated to P contains the point of intersection of p, and p,; if s is
thus to be situated in plane 2, then p, and p, must coincide, and this
takes place only for the vertices of the polar triangle which /,* and
k,”? have in common; so 8 is = 3.

The third characteristic quantity, y*'), indicating how often a focus
P lies on a given line, whilst at the same time the focal plane 2
passes th rough that line, is found as follows. When P deseribes
the line / the two polar planes rotate round the two lines /,, /, con-
jugated to / with respect to ,,,; their line of intersection s
describes a regulus with /, ,/, as bearers, and passing through the
vertices of the four doubly projecting cones of 4" ; this regulus intersects
/ in 2 points, through which every time one line s passes, and the
foci conjugated to these lines lie on / as is in fact the case for all
lines s of the regnlus; for these two foci however the focal plane
x = Ps passes through /; so y = 2.

\) Sturm, “Liniengeometrie” I, p. 78.

510

Through the points P of space the polar planes a, , 2, with
respect to ®,, ®, are conjugated one by one to each other; so we
ean regard the lines s as the lines of intersection of conjugated planes
of two collinear spaces, and we then find immediately that the lines
s form?) a tetrahedral complex, for which the tetrahedron of the
four vertices of the cones of k* is the surface of singularity, in such
a sense that each arbitrary ray through one of the vertices or in one
of the faces of that tetrahedron is a complex ray, whilst in general
the tetrahedral complex being quadratic a point has but a quadratic
complex cone, a plane a quadratic complex curve. As namely the two
polar planes of the vertex of a cone coincide in the opposite face of the
tetrahedron, each line in this face can be regarded asa ray s, and as
of a line / through 7, e. g. the t wo conjugated lines lie in 7,7, 7,
inversely the two polar planes of the point of intersection of those
conjugated lines pass through /, so that / is a complex ray s. The
complex cone of a point P in 7,7,7,—=r, breaks up into two
pencils, one with vertex P and lying in 1,, the other with vertex P
and lying in a certain plane through P and 7’; and likewise the
complex curve in a plane through 7’, degenerates into 2 points, viz.
7, itself and a certain point in the line of intersection of that plane and rt.

A ray s being the line of intersection of the polar planes 2, , x, of
a certain point 7 with respect to ®, , ®,, inversely through an arbitrary
ray s two planes 2, , 2, must pass having the same pole 7; if however
a line lies in a plane, then the conjugated line passes through the pole
of that plane; thus for s the ¢wo conjugated lines s,,.%, must pass
through P and must intersect each other in P; so we can also dejine
the rays s as those rays of space whose two conjugated lines with
respect to P,, ®, intersect each other. In this we have also a means
to determine the focus of an arbitrary ray s; we have but to find
the point of intersection of s, and s,.

The rays s conjugated to the points of an arbitrary line / form
a regulus as we have seen above; those conjugated to the points of
a ray s must thus form according to the preceding a quadratic cone,
and this is evidently the complex cone for the focus P of s, by
means of which a construction for that cone has been found; we
take the ray s conjugated to ?, we allow a point to describe that
ray and we determine for each position ihe two polar planes; the
line of intersection of these describes the complex cone when the point
describes the ray s. Just as the regulus for a line /, so each com-
plex cone contains the vertices of the four doubly projecting cones ;

1) Sturm |.c. p. 342.

a ee

51)

and as the two conjugated lines of a ray s lie likewise on the com-
plex cone of the focus 7, they themselves are again rays s.

The complex curve lying in a plane @ we find by regarding the
two poles A, and A, of a. The conjugated lines /,,/, of the lines /
of @ pass respectively through A, and A,, and are conjugated by the
rays / one by one to each other, so that two projective nets of rays
are formed ; the locus of the points of intersection of rays conjugated
to each other is a twisted cubic through A, and A,, and furthermore
through the four vertices of the cones 7,...7,; for, the two conju-
gated lines of the line of intersection of « with 7,77, are A,7),
A,T,. The rays s conjugated to the points P of that twisted eubie
as foci lie in @ and envelope the complex curve; and as each line
of the plane 7,,7,7', can be taken as a ray s conjugated toe.g. 7’,
so also the line of intersection with «, the complex conic will touch
the four surfaces of the tetrahedron.

Botany. — “On the demonstration of carotinoids in plants’ (First
communication): Separation of carotinoids in crystalline form.
By Prof. C. van WisseLincH. (Communicated by Prof. Mout).

(Communicated in the meeting of September 28, 1912).

Many of the chemical, physical, and microscopical investigations
on the yellow and red colouring matters of the vegetable kingdom
which are grouped under the name carotins*) or carotinoids’) bear
witness to great care and originality. They have, bowever, not all
led to similar results. Especially the microscopical investigation has
led to very divergent results which sometimes seriously conflict with
those obtained by chemicai and physical means. The investigators
might be divided into two groups; one is inclined to consider all
carotinoids identical; believing that the differences observed are not
of a chemical nature. The other group distinguishes several carotinoids.

T. Tammes*) is especially a representative of the first group. After
investigating a fairly large number of plants, she comes to the
conclusion that the yellow to red colouring matter of plastids, in
green, yellow variegated and etiolated leaves, in autumn leaves, in
flowers, fruits and seeds, in diatoms, green, blue, brown and red

1) Czapex, Biochemie der Pflanzen, |. p. 172.

2) M. Tswertt, Uber den makro- und mikrochemischen Nachweis des Carolins,
Ber. d. d. bot. Ges. 29. Jahrg., Heft 9, 1911, p. 630.

3) T. Tammers, Uber die Verbreitung des Carotins im Pflanzenreiche, Flora,
1900, 87. Bd. 2. Heft, p. 244.

512

algae, completely agrees in chemical and physical properties with
ihe carotin from the root of Daucus Carota.

The most recent macrochemical investigations of carotinoids, namely
that by Wutusrirrer and his pupils have not confirmed Tammss’
results. Wittstitrer and Mire?) isolated two carotinoids from the
leaves of the stinging nettle, namely, carotin (C,,H,,) which substance
was found to be identical with the carotin from the root of Daucus
Carota and xanthophyll (C,,H,,O,), whilst Witistirrer and Escuer *)
obtain from tomatoes another carotinoid, lycopin (C,,H,,) isomeric¢
with Daueus-earotin. From two objects three different carotinoids
were thus obtained, namely, two hydrocarbons and one oxygenated
substance.

The great difference between the results of microscopical and
macro-chemical investigations determined me to try various methods
which have been recommended for the demonstration of carotinoids
by microscopical means.

These methods are sometimes divided into direct and indirect ones.
The direct ones depend on the addition of reagents which bring about
colorations, such as, for example, the beautiful blue coloration with
sulphuric acid; the indirect methods are based on the separation of
the carotinoids in crystalline form in the cells or tissues. Only in a
few cases do the carotinoids occur as crystals in the cells; generally
they are combined with, or dissolved in a substance that is fluid,
fatty and saponifiable by alkalies*), This substance occurs in the
plastids, or forms, as in the case of lower organisms, oily drops in
the cells *). The aim of the indirect methods is to free the carotinoids
and to erystallize them out. The following methods belong to this
category.

Potash Method.

This method invented by MoriscH*®) was used originally for the
demonstration of xanthophyll or carotin in green leaves. Fresh leaves

1) R. WiristArrer, Untersuchungen tiber Chlorophyll, IV. Ricsarp WitistATTer
und Water Mira, Uber die gelben Begleiter des Chlorophylis, Justus Liebig's
Annalen der Chemie, 355. Bd. 1907, p. 1.

2) Ricnarp Wiutstirrer und Heir. H. Escuer, Uber den Farbstoff der Tomate,
Hoppe-Seyler’s Zeitschrift fiir Physiol. Ghemie, 64. Bd. 1910, p. 47.

3) F. G@. Kont, Untersuchungen tiber das Carotin und seine physio]. Bedeutung
in der Pflanze, 1902, p. 118 et seq.

‘) W. Zorr, Zur Kenntnis der arbungsursachen niederer Organismen_ Erste
Mitteilung, Beitriige zur Physiol. und Morphol. niederer Organismen, Erstes Heft,
1892, p. 35. Zweite Mitteilung, 1. c. Zweites Heft, 1892, p. 5.

®) Hans Mouiscu, Die Krystallisation und der Nachweis des Xanthophylls (Caro-
tins) im Blatte, Ber. d. d. bot. Ges, Bd. XIV, 1896, p. 19.

513

or parts of them are placed in alcoholic potash containing 40°/, by
volume of alcohol and 20°/, by weight of potassium hydroxyde ;
they are left in the mixture for several days while light is excluded,
until all the chlorophyll has been extracted. With green leaves the
potash method gives good results, but also in many other cases, for
example, with etiolated, autumn, and variegated leaves, flowers,
fruits, algae, ete. We may assume that generally the carotinoids are
separated in those cells in which they occur in the living plant.
Sometimes the carotinoids wander and form aggregations of crystals
in apparently arbitrary places or outside the objects. As a rule the
method gives positive results; only in a few cases does it fail.

In order to obtain an idea of the way in which the crystal-formation
takes place, I have in a few cases studied the effect of Moniscn’s
reagent on the living material under the microscope. The crystallisation
wiil be illustrated by a few examples.

Large yellow plastids are found in the corolla of Calceolaria rugosa.
The carotinoid occurs dissolved in a substance, fluid and easily
saponifiable, which forms a yellow peripheral layer in the plastids.
On the addition of Mouiscn’s reagent the plastids sometimes form
yellow globules with a sharp edge, which quickly change into globules
or masses which show a less well-defined contour and are products
of saponification. Often saponification proceeds still more rapidly, so
that globules with sharp outline are no longer seen, but the saponi-
fication-products appear immediately. They dissolve and out of the
solution there grow.in a few minutes orange-yellow acicular or narrow
band-shaped crystals, often very long and strongly curved and some-
times fissured.

In the ligulate florets of Gazania splendens large orange-coloured
plastids occur in which can be distinguished globules that are in
constant movement. When Motiscu’s reagent is added they rapidly
form orange balls with sharp outline. These arise out of the union
of the globules described above. The phenomenon is not the result
of saponification, as Koni.*) assumes, for warming in water or a
stay in dilute spirit (70°/,) has the same effect. In my opinion it is
caused by the cells dying and the plastids losing their structure. In
Gazania splendens saponification of the globules formed proceeds very
slowly. After being in Motiscn’s reagent for 20 days (in vitro), I
saw only orange globules in the cells which were coloured dark-blue
by sulphuric acid. When I investigated the flowers after 24 days,
I again found many orange globules, but at the same time there

1) F, G. Kont, |. ¢. p. 122.
34
Proceedings Royal Acad, Amsterdam, Vol, XY.

514

were also many well-formed crystals, orange crystal-plates with
rounded ends and aggregates of the same crystal-plates. The crystals
sive the various colour-reactions of carotinoids and the same is the
ease with the orange globules, in proof, that all the carotinoid has
not yet crystallized out.

The formation of crystals by the potash method is easily explained.
In the living plant the carotinoids occur in solution. They are dissolved
in a fluid, fatty substance. When Moniscu’s reagent is added the plas-
tids are destroyed and the fluid substance forms globules, which are
coloured orange-yellow or orange by the carotinoid. Mo.iscs’s reagent
farther brings about saponification and solution. The oily substance
is saponified and the cells are filled with a solution of the saponi-
fication-product in which the carotinoid is soluble. This solution is
diluted by the reagent in which the objects are placed and the caro-
tinoids, which are not soluble in Momiscu’s reagent, separate in the cells.

By reason of the above facts, [ assumed that the carotinoids must
be soluble in soap-solutions. This was indeed found to be the case.
If, for example, after being washed out with water, preparations, in
which carotinoids occur in the form of crystals, are placed in soap-
spirit (Spiritus saponatus Pharm. Nederl. Ed IV without oil of laven-
der) the crystals dissolve.

As is evident from the examples described above, the saponification
of the fatty substance and the separation of crystals sometimes takes
place rapidly and sometimes very slowly. According to the nature of
the object minutes, hours, days, weeks, or months are required for the
separation of the crystals. Among objects which require much patience
are the following in addition to the ligulate florets of Gazania splen-
dens those of Hiéracium aurantiacum, Doronicum Pardalianches and
Taraxacum officinale, in which erystals were observed after 24, 48
and 74 days respectively. In the ligulate florets of Hiéracium murorum
and Inula Helenium and in the petals of Viola cornuta no crystals
were perceived after 60, 39 and 29 days respectively. That the
carotinoids do not separate out in these last examples, must be attri-
buted to the fact that the oily substance is not saponified and holds
the carotinoid in solution. The yellow or orange-yellow globules,
which are seen in the cells, are coloured blue by sulphuric acid,
transient blue by bromine water and green by iodine in potassium
iodide; this proves that the carotinoid is still present.

I do not think that-the long continued action of Momiscu’s reagent
is accompanied by any disadvantage. I have no indication that the
carotinoids are destroyed by it and often fine crystallisations are finally
obtained. | have tried Moxisci’s potash method in about 40 cases and

— -.—. 7s

ew Se Oe ee

O15

only in the 3 last-mentioned was there no erystallisation of caro-
tinoid. It is however possible that in these cases also a still more
prolonged action might have had the desired result.

Tames ') and Kou’) maintain that all the crystals, which are
obtained by the potash method consist of carotin, however they may
differ in colour and shape. The colour would only depend on the
thickness of the crystals and of the angle at which they are seen.
BECKE *) however, considers as a result of crystallographic investiga-
tions that the crystals obtained by Mou.iscn’s method are not identical.
I myself have come to the following conclusions. Before proceeding
] wish to remark that_the names of the colours which I use are in
agreement with those of Kiincksieck et Varetrn’s Code des Couleurs,
1908. Often the numbers, given to the colours in the book, have
also been mentioned.

In many cases the crystals differ greatly in colour and shape. In
general, with respect to the colours the crystals can be arranged in two
groups, namely, orange-red and red (Kl. et V. 91, 76, 51, 46) to
which the violet-red (Kl. et V. 581) of the fruit of Solanum Lyco-
persicum are allied and a second group composed of orange-yellow
and orange crystals (Kl. et V. 176, 151, 126, 101). The colour is
also influenced by the thickness of the crystals. Red is always pre-
sent in the first group, but not in the second.

However different the shape of the crystals may be, it is still
true that colour and form are often connected. Among the red
crystals, as a rule well-developed plates are found which have the
shape of small parallelograms and sometimes also of rhombs. Generally
small plates are formed which are several times more long than broad
or narrower ones which resemble pointed needles. The parallelograms
and rhombs are often imperfect. Parts may be wanting, angles and
sides may be rounded. Very often the red crystals form aggregates.
The root of Daucus carota and the fruit of Solanum Lycopersicum
belong to the objects in which carotinoids occur in the form of crys-
tals. In Daucus the carotin has formed in addition to well-developed
red parallelograms and rhombs all sorts of other crystals which are
even curved band shaped. In the tomato lycopin is found in the form
of red-violet needles.

The orange-yellow and orange crystals are also very varied.
Especially in those cases in which the carotinoids crystallize out
slowly, little plates of crystal are often found which are generally

1) lc. p. 242, 244.
2) 1. c. p- 33 et seq. and p. 67.
3) Hans Moutseu, |. c. p. 24.

34%

516

several times more long than broad, rarely about as long as broad. The
ends are for the most part rounded, occasionally pointed, irre-
cular or more or less straight. Often oval and whetstone-shaped
crystals are found. Once they were seen as rhombs with rounded
sides. In a few cases the crystals showed large surfaces of indefinite
shape, in other cases the surfaces were narrow, long and slightly
curved. The multifarious ribbon- and needle-shaped crystals that
occur are allied to this last-mentioned form. These are generally
much curved. Straight needles are rare. The ribbon-shaped erystals
are often branched or split up into separate curved needles. Finally
connected with the curved, needle-shaped crystals there are filamentous
ones, which may be very much twisted and often form clews. The
erystal plates often form aggregates.

When leaves are treated with Mottscn’s reagent aggregates of
crystals are generally formed in the cells which contain chlorophyll ;
they are composed of orange-yellow plates and red crystals resembling
needles.

The shape of the orange-yellow and orange crystals often differs
in one and the same object. In the flower of Dendrobium thyrsiflorum
I found orange-yellow (KL. et V. 151) whetstone-shaped plates and
orange-yellow (151) thread-like crystals, also aggregates of fine needle-
shaped crystals coloured bright orange (101) and to some extent
orange-red (81). In the flower of Cucurbita melanosperma I found
thread-like erystals and very thick, almost completely straight, flat
needles in the hairs.

The shape of the crystals is sometimes very dependent on external
circumstances, as for example, on the quantity of Motiscn’s reagent
into which the object is put. In the petals of Chelidonium majus,
for example, I got thread-shaped crystals whenever I placed them
in a flask with a large quantity of Motiscn’s reagent, and crystal
plates when a petal was placed in a small quantity of Mottscn’s
reagent between a cover-slip and a slide.

However diverse the crystals may be there is an important point
of difference between the red and orange-red on the one hand and
the orange-yellow and orange crystals on the other hand, namely,
that when the carotinoids have separated out in the form of plates,
among the former well-shaped parallelograms are nearly always
formed and these are not met with among the orange-yellow and
orange crystals.

In the leaves of Urtiea dioica I was able to observe that the
quantity of the reagent may influence not only the shape of the
crystals but also the place where they are formed. By using much

ee oe ar

317

of Mo.tscn’s reagent a small aggregate of orange-yellow and red
crystals appears in every cell; with little of the reagent I got large
red and yellow aggregates of crystals in various places in the tissue
or outside it. This last result need cause no surprise. The carotinoids
are soluble in the solntion of the saponification-products formed and
not in Motiscu’s reagent. When a small quantity of the reagent is
used no quick dilution of the soap-solution occurs and the carotinoids
will have the chance of changing their place in the tissue. In general
it is therefore preferable not to use too small a quantity of the reagent,
unless for any reason large aggregates of crystals are desired, —

I have applied the potash method of Moniscn to the followine
objects. ;

Flowers: Trollius caucasicus Stev., Nuphar luteum Sm., Chelido-
nium majus L., Meconopsis cambrica Vig., Corydalis lutea DC.,
Erysimum Perofskianum Fisch. et Mey., Sinapis alba L., Isatis tine-
toria L., Viola cornuta L. var. Daldowie Yellow, Cytisus sagittalis Koch
(Genista sagittalis L.), Cytisus Laburnum L., Spartium junceum L.,
Thermopsis lanceolata Rh. Br., Cucurbita melanosperma A.Br., Ferula
sp., Inula Helenium L., Doronicum Pardalianches L., Doronicum
plantagineum. L. excelsum, Calendula arvensis L., Taraxacum offici-
nale Wigg., Hiéracium aurantiacum L., Hiéracium murorum I.,
Gazania splendens Hort., Asclepias curassavica L., Calceolaria rugosa
Hook., Dendrobium thyrsiflorum Rcehb. fil., Iris Pseudacorus L.,
Narcissus Pseudonarcissus L., Clivia miniata Regel, Tulipa hortensis
Gaerin., Fritillaria imperialis L., Lilium croceum Chaix, Hemeroeallis
Middendorffii Trautv. et Mey.

Green leaves: Chelidonium majus L., Taraxacum officinale Wige.,
Urtica dioica L., Triticum repens L., Selaginella Kraussiana A.Br.

Yellow variegated leaves: Sambucus nigra L. fol. var., Grapto-
phyllum pictum Griff., Croton ovalifolius Vahl.

Fruits: Sorbus aucuparia L., Solanum Lycopersicum Tn.

Root of Daucus Carota L. |

Algae: Cladophora sp., Spirogyra maxima (Hass.) Wittr., Haemato-
coecus pluvialis Flot.

It must be noted that in four of the above-named objects in their
natural state carotinoids already occur in the form of crystals, namely
in the root of Daucus Carota, the fruits of Sorbus aucuparia and
of Solanum Lycopersicum, and in the flower of Clivia miniata.

Acid method.

By treating parts of green plants with dilute acids Frank ') observed

1) A. Tscumrcu, Untersuchungen tiber das Chlorophyll, Landwirtsch. Jahrbiicher,
XIII. Bd., 1884, p. 490. Hans Mouiscu, l.c. p. 26.

518

the formation of red or reddish yellow crystals, especially in the
stomata. MoriscH’) repeated the experiment with the leaves of
Elodea and also observed such crystals which according to him,
correspond to the crystals he obtained by his potash method. Tamers’)
experimented on a great number of plants and various parts of
plants with dilute acids, as, for example, hydrochloric acid, oxalic
acid, tartaric acid, chromic acid, picric acid, acetic acid, and hydro-
fluorie acid. Picrie acid was used in a solution of alcohol, the other
acids in aqueous solutions of various strengths. The investigation
yielded positive results in the case of leaves, and other green parts
of plants, flowers, green algae and Fucoideae. In all the cases inves-
tigated, over 30, crystals were obtained after some hours or days
which, according to the above-mentioned writer, agreed completely
with the erystals which had been obtained by the potash method
and were found to consist of carotin. With yellow variegated, yellow
autumn and etiolated leaves the experiment was without result, a
fact which Tammrs*) is unable to explain.

When plants or parts of plants which contain chlorophyll are
investigated with dilute acids allowance must be made for the action
of the acids on the chlorophyll. When Morniscn’s reagent is used the
chlorophyll dissolves with saponification of the ester, separation of
phytol and formation of chlorophyllin potassium *), but the action of
acids on the chlorophyll produces insoluble derivatives. WiLLsTATTER,
who treated alcoholic extracts obtained in the cold from dried plants
with acids, obtained, when the magnesium had been eliminated,
phaeophytin *), which like chlorophyll *) consists of two component
parts, namely, phaeophytin a (phytylphaeophorbide a) and phaeo-
phytine b (phytylphaeophorbide b). Earlier investigators also already

: Gp. 20;

c. p. 216 et seq. and p. 242 et seq.

2p. 2a,

RicHaRD Wiistarrer, (Untersuchungen tiber Chlorophyll), Il. Zur Kenntnis
der Zusammensetzung des Chlorophylls, Justus Liebig’s Annalen der Chemie, 350.
Bd. 1906, p. 48.

Ricuarp Whitsrirrer und Ferrpivanp Hocueper, III. Uber die Einwirkung von
Sauren und Alkalien auf Chlorophyll, 1. ec. Bd. 354, 1907, p. 205.

») R. Wiutstiirrer, I. Zur Kenntnis der Zusammensetzung des Chlorophylls, | c.

R. Wiustirter und F. Hocueper, |. c.

Ricnarp Wutsritter und Max Ister, XX. Uber die zwei Komponenten des
Chlorophylls, 1. c. Bd. 390, Heft 3, 1912, p. 269.

6) Ricuarp Witstirrer und Max Urzneer, XVI. Uber die ersten Umwandlun-
gen des Chlorophylls, 1. c. 382. Bd. p. 129.

R. Wisrirrer und M. Isuer, |. c¢.

)

)
*)
) 1
*)

519

obtained products produced by the action of acids on chloropliyll.
Hopps-Sey.er ') obtained from grass by extraction with boiling alcohol
a crystalline chlorophyll derivative, which he subjected to a number
of operations in order to separate it from other substances and to
purify it. He named it chorophyllan. Tscrircn *) states that when
parts of plants that contain chlorophyll are treated with acids, chloro-
phyllan erystallizes out in the cells. Witistirrer, Ister, and Hue *)
have after further investigation compared the chlorophyllan of Hoppr-
SEYLER to phaeophytin. In the opinion of these investigators it is not
a pure compound but chlorophyll more or less decomposed by plant
acids and allomerised by treatment with solvents. For this reason
they consider the name chlorophyllan unsuitable for the chlorophyll
derivative obtained by means of acids.

Tames *) also discussed the action of acids on chlorophyll and
comes to the conclusion that the formation of chlorophyllan offers
no hindrance to the demonstration of carotin, because, although it
must be admitted that the crystals obtained may perhaps be conta-
minated by some chlorophyllan, yet in the main they are composed
of carotin. Koun*) evidently agrees with Tammes. He writes : “Mehr
oder minder unbewusst ist die Saéuremethode schon friiher von einigen
Forschern angewandt worden, unbewusst insofern, als das auskrys-
tallisirende Carotin irrtiimlich fiir Chlorophyllan gehalten und nur in
einzelnen Fallen als solches erkannt wurde.” I consider TAMMEs’ rea-
soning inconclusive, whilst Koni does not further explain his views.
A simple investigation of the crystals shows that they are very diffe-
rent from carotin-crystals and there is even no reason to assume
that they contain any carotin.

I exposed fresh plants and parts of plants containing chlorophyll
to the action of acids at the ordinary temperature, oxalic acid from
1°/, to 10°/,, hydrochloric acid of 5°/,, tartaric acid of 10°/, and
hydrofluoric acid of 2°/,. Without exception after a day crystals had
separated out. They form small aggregates attached to the chroma-
tophores. The crystal aggregates resemble spherical bodies, but with
high magnification the constituent crystal plates can be distinguished.
Only in one case, namely in Cladophora, did I see long whip-shaped
erystals projecting from the crystal aggregates. The crystal aggregates
are not yellow, orange yellow, or red, but brown. In acetone they

1) F. Hopre-Seyier, Zeitschr. f. physiol. Chemie 3, 1879, p. 339.
2) A. Tscuircu, Untersuchungen iiber das Chlorophyll, l. c. p. 441.
8) R. Wuustitrer und M. Ister, |. c. p. 287 et seq. and p. 337.
4) lic. p. 217 and 218.

) lc. p. 47.

520

are easily soluble, slowly in glacial acetic acid. With concentrated
or somewhat dilute sulphuric acid, for example 66°/,°/,, they are
not coloured blue, but green (Ku. et V. 326). The colour never.
resembles the blue colour which the crystals of carotinoids assume
with sulphurie acid, and which never shows a green, but sometimes
a slightly violet tint. The ereen-coloured crystal aggregates are soluble
in sulphuric acid. The brown crystal aggregates are also coloured
ereen by concentrated hydrochloric acid (specific gravity = 1.19);
afterwards they dissolve slowly. With concentrated nitric acid they
are not, as is the ease of carotinoids, temporarily coloured blue; they
deliquesce and form globules, which when gently warmed, gradually
become colourless and presumably consist of phytol. Nor do they,
like carotinoids, become temporarily blue in bromine water; the
brown colour at first remains unchanged. Towards caustic potash
ihe brown aggregates of crystals also behave quite differently from
the crystals of carotinoids; they are entirely scluble in it; they also
are completely soluble in dilute aleoholic caustic potash, as, for
example, in Mouiscn’s reagent, in which the crystals of carotinoids
are of course insoluble. Since they leave nothing behind on solution
there is no reason for thinking that they contain carotinoids.

The behaviour of the brown aggregates towards reagents shows
that they are composed of a chlorophyll derivative. Phaeophytin *)
gives the same reactions, and sometimes more or less clearly shows
erystalline structure. Tammes and Koni have confused carotin with a
chlorophyll derivative. Tammes’ drawing N°. 22 of Elodea canadensis
in particular clearly shows that such a confusion has taken place.
In each cell a number of brown, round crystal aggregates are figured
attached to and on the chromatophores. The crystalline structure is
not indicated in the figure, but is not always easily distinguished
in the full cells. Besides these crystal aggregates, I found in many
cells, though not in all, red aggregates of crystals which resemble
carotin and which are coloured blue by concentrated or somewhat
dilute sulphuric acid, namely of 76°/,. These crystal aggregates are
however not figured by Tammes, nor are they mentioned.

Now it is somewhat explicable why Tammes’*) obtained negative
results with yellow variegated, yellow autumn and etiolated leaves.
These objects or the yellow parts of them contain no chlorophyll
and are therefore unable to produce brown crystal aggregates of a
chlorophyll derivative. But this does not, however, clear up every-

4) R. Wittstatrer und F, Hocueper, |. ce. p. 222 and 223.
) 1. c. p. 220.

524

thing. For the non-green leaves and the parts which are not green,
yet contain substances which belong to the carotinoids. How is it
that these were not found by Tames, whilst in other non-green
parts of plants such as flowers, TamMes obtained after some days in
all the eight cases investigated well-formed crystals which with
reagents showed the reactions proper to carotin. | am convinced by
the use of Motiscn’s reagent that carotinoids exist in the yellow
parts of yellow variegated leaves. Sometimes I obtained separation
of orange-yellow crystals, in other cases they were orange-yellow
and red, but all gave the reaction proper to carotinoids. Kon °*),
with etiolated leaves, arrived at a different conclusion from that
of Tammes. I cannot refrain from remarking that Kout does not
always correctly reproduce the results of Tames, with whom he is
in entire agreement. The following is quoted from Tammes*): Ich
habe auch gelbbunte, herbstlich gelbe und etiolirte Blatter in ver-
diinnte Sdurelésungen gebracht, aber stets mit negativen Resultaten.
And from Koat*): Durch die neueren Untersuchungen der etiolirten
Pflanzen mit Séauren, welche T. Tammes in grosser Zahl ausfiihrte
und welche ich, um in die unsicheren Anschauungen einige Klarheit
zu bringen, planmassig fortgesetzt habe, ist es nun mit Sicherheit
erwiesen, dass in allen etiolirten Pflanzenteilen, so weit sie gelb
gefarbt, mit verdiinnten Saduren Carotin-Krystalle zur. Ausscheidung
gebracht werden kénnen.

I treated objects, both with and without chlorophyll, such as green
and yellow variegated leaves, yellow, orange-yellow, and orange
flowers, and algae, with dilute acids at the ordinary temperature,
namely, with 1°/,, 2°/, and 10°/, oxalic acid, 1°/, and 5°/, hydro-
chloric acid, 10°/, tartaric acid and 2°/, hydrofluoric acid solutions.
The treatment often lasted oue or two months. The objets which
were subjected to this investigation, were the same as those investigated
by the potash method of Monisca.

In the case of green leaves I obtained with the dilute acids
the above mentioned brown crystalline aggregates of a chlorophyll
derivative which were formed in each cell containing chlorophyll,
and here and there in the tissue red crystals, loose plates or
ageregates. In the case of flowers, of which I investigated about 25,
I generally obtained no crystals with dilute acids. Only in two
cases was there a positive result, namely, in Asclepias curassavica,
where red crystals separated and in Calceolaria rugosa where orange-

1) 1. c. p. 48.
4) 1. c. p. 220.
5) lc p. 48.

yellow ones appeared. In one of the yellow variegated leaves, namely,
of Graptophyllum pictum I obtained the separation of small orange-
yellow crystals in the yellow portion of the leaf. The crystals which
had separated behaved towards reagents and solvents exactly as
did the corresponding crystals obtained by the potash method.

With regard to the investigation of flowers with dilute acids,
Tammers’') results and mine differ. Whilst she obtained well formed
crystals in all cases, I obtained them only exceptionally. Our in-
vestigations were however mostly concerned with different flowers.
I propose if possible to examine with acids those flowers which
have been studied by Tammes, but not yet by myself, in order to
reach greater certainty on this point of differenve. Whatever the
ultimate results, I nevertheless already venture to state, that the
method of inducing crystallisation of the carotinoids in plants by
means of acids cannot in general be recommended. Often the yellow
carotinoids in particular do not crystallize. Red crystals very often
form in the tissue but not in all cases in which they can be obtained
by the use of the potash method. This is the case, for example, in
the flowers of Nuphar luteum, Isatis tinctoria, Cytisus Laburnum and
Thermopsis lanceolata as also in the peduncles of Trollius caucasicus.
In these many oranje-yellow and a few red crystals were obtained
by Moriscn’s reagent, whilst in the flower of Asclepias curassavica,
in which, as stated above, red crystals had been separated out by
means of acids, Moniscu’s reagent produced many red as well as a
few orange-yellow crystals. When the carotinoids which yield red
crystals are present in great quantity, they can therefore be demon-
strated by acids, but when they are present in small quantity, they
escape observation.

Another drawback to the acid method is that the carotinoids
which yield orange-yellow crystals are very liable to decompose.
Continuous treatment with acids as is necessary with the acid
method, often is very harmful and may lead to complete decom-
position of the carotinoids. They are much more liable to decompo-
sition by acids, while they are still in solution in the fatty substance
of the plastids, than when they have been separated as crystals
by some other method. According to HutskMANN*) WACKENRODER
pointed out this decomposition so far back as 1832. In the treatment
with acids I have sometimes found decomposition to occur even in
the first few days. The colour of the flowers becomes paler and the

We Me re p. 243,

2) A. Husemanny, Uber Carotin und Hydrocarotin, Ann. der Chem. u. Pharm,
Bd, CXVII, 1861, p. 200,

-M

523

yellow or orange oily globules and masses, which have been for-
med in the cells and which contain the carotinoid, also lose more
or less of their colour. Sulphurie acid then no longer colours them
blue or much more feebly than at the beginning of the experiment.
The carotinoid decomposes without crystallising out. This decompo-
sition is easily confirmed in Chelidonium majus, Narcissus Pseudo-
narcissus, Doronicum Pardalianches and Tulipa hortensis, for instance.

Resorcinol Method.

Tswert ’) has described a method of crystallising the earotinoids from
plants and parts of plants under the microscope. The objects are
placed on the microscope slide in a concentrated solution of resorci-
nol, containing 10 to 12 parts of resorcinol in 10 parts of water.
I have used this method in eight cases, namely, in the leaves of
Urtica dioica, in the flowers of Chelidonium majus, Erysimum Perof-
skianum, Gazania splendens, Calceolaria rugosa and Narcissus Pseu-
donarcissus, in Cladophora sp. and in Haematococcus pluvialis. In
five cases, namely, in Urtica, Chelidonium, Calceolaria, Narcissus
and Cladophora crystals separated rather quickly. In Chelidonium,
Calceolaria and Cladophora crystals appeared in the cells, in the

other two cases in and around the preparations. Erysimum, Gazania

and Haematococcus which had given positive results with the potash
method, gave negative results with the resorcinol solution. In the
case of Haematococcus pluvialis JacoBseN’*) was also unable to obtain
separation of erystals.

The shape of the crystals differs greatly. When with Motiscn’s
reagent red and orange-yellow crystals were obtained, crystals of the
same colour were formed with Tswerrt’s reagent in those cases in
which the experiment gave a positive result. With respect to reagents
the crystals behave in the same way as the carotinoid crystals obtained
by the potash method.

TsweTt’*) has also pointed out the variation in the erystals and
has shown in Lamium by his adsorption method that different che-
mical bodies are present, carotin and xanthophyll. It seems to me
that Tswert’s method will be applicable with success to many cases.

1) M. Tswerr, Uber den makro- und mikrochemischen Nachweis des Carotins,
Ber. d. d. bot. Ges. 29. Jahrg. Heft 9, 1911, p. 630.

2) H. C. Jacossen, Die Kulturbedingungen von Haematococcus pluvialis, Folia Micro-
biologica I, 1912, p. 25,

oy te

- 594
Other methods.

Koni *) has remarked that possibly other substances also might be
used to bring about the crystallisation of carotin. He surmises that
chloralhydrate might be used for the purpose and intends to inves-
tigate this possibility. When the solvent action of chloralhydrate
upon the various constituents of cells is considered and it is seen
that carotin crystals in contrast to those of xanthophyll are fairly
resistant, then it is natural to suppose that chloralhydrate may
offer a suitable means of separating carotin as crystals. I have
experimented with the leaves of Urtica dioica in a concentrated
aqueous solution (7 in 10) of chloralhydrate. We know from the
investigations of WiLisTArTer and Misc *) that these leaves contain
carotin and xanthophyll. When I placed a small piece of the
tissue containing chlorophyll in a_ solution of chloralhydrate and
observed it under the microscope, I could soon detect changes in the
chromatophores and the formation of a globule in each cell, which
gradually dissolved and left behind a small aggregate of red carotin
crystals. Orange-yellow crystals of xanthophyll were not separated.
As was to be expected therefore the method is of no use for
the separation of xanthophyil because decomposition takes place. I
cannot moreover recommend it for the separation of carotin-crystals,
because carotin is also attacked by chloralhydrate and small quantities
therefore may escape observation.

According to Wu.ustaArrer and Mire *) xanthophyll is “spielend
loslich” in phenol. Having in mind the solubility of many substances
in liquefied phenol and having confirmed the fact that carotin dis-
solves much more slowly than xanthophyll, it occurred to me to try
liquefied phenol for the separation of carotin or allied carotinoids. I[
used two mixtures, one of 10 parts by weight of phenol in loose
crystals and 1 part by weight of water, the other consisting of 3 parts
by weight of phenol in loose crystals and 1 part by weight of glycerine.
I prefer the latter mixture, because it mixes more quickly with the
water contained in the objects. I examined the flowers of Erysimum
Perofskianum, Asclepias curassavica, the leaves of Urtica dioica and
the ligulate florets of Taraxacum officinale. With petals of Erysimum
Perofskianum the potash method yielded no beautiful result, and the
acid method a negative one. I placed parts of the petals in the above
mixtures between a miscroscope slide and a cover-slip. Under the

925

microscope I saw that the brightly coloured orange-yellow plastids
quickly formed orange-yellow globules; crystals soon appeared in
these globules. While the globules dissolve the crystals remain behind.
These are orange-red plates and aggregates which very slowly dissolve
in the phenol mixtures. To investigate these, the preparations can be
washed out successively with dilute alcohol (70 °/,) and with water.
With reagents they give the reactions characteristic of carotinoids.

When parts of the flower of Asclepias curassavica are placed in
the mixture of phenol and glycerine, there quickly appear in all
the cells numerous light- and dark red or orange-red (KI. et V. 11,
46, 51, 71, 91) crystals, in the same way as in Erysimum Perofs-
kianum, among which were many plates and aggregates. They do
not dissolve in the phenol solution; at any rate after three days they
were still unchanged. When investigated with reagents in the way
indicated above, they show the reactions proper to carotinoids. In Urtica
dioica orange-red (81) crystal aggregates are formed here and there
in the tissue, which after three days are still present in the mixture of
phenol and glycerine. In the ligulate florets of Taraxacum officinale
yellow globules soon arise; in this case no crystals occur; the globules
completely dissolve. Clearly in these four objects carotinoids occur,
which differ greatly with respect to their solubility in a mixture of
phenol and glycerine (3 to 1), and are either insoluble or dissolve
slowly or readily. In the last case the carotinoids do not separate.

Witistitrer and Mira’) have dealt with the question whether,
in addition to carotin, xanthophyll is also present as such in the
living plant and have answered it affirmatively. Both substances,
can indeed be separated with simple solvents, carotin from dried
leaves with petroleum ether, xanthophyll from alcoholic extracts of
fresh leaves according to the ‘“Entmischungsmethoden” of G. SToxss,
u. Kraus, H. C. Sorsy and R. Sacussr’). It is therefore reasonable
to assume that in some cases the use of simple solvents in which
the carotinoids themselves are but little or not soluble, might lead
to the erystallisation of these substances. In a few cases I have
indeed succeeded in doing this.

With the ligulate florets of Taraxacum officinale and Doronicum
Pardalianches I did at first not succeed in crystallising even a
part of the carotinoid by means of the potash method. It remained
in solution in the yellow or orange-yellow globules which had formed
in the cells) When 1 had treated the ligulate florets for a very
short time with absolute alcohol or a certain quantity with very

No 5. p.510:

*) See WILLsTATTER und IsLER, l.c. p. 275 et seq.

526

little absolute alcohol, I ascertained, that the oily substance which
retained the carotinoid, was dissolved and that part of the latter had
separated more or less crystalline and gave the reactions charac-
teristic of carotinoids. Direct treatment of the florets with absolute
alcohol led to similar results. When the treatment with absolute
aleohol is prolonged or when too much of it is taken, the carotinoid
dissolves completely.

In a few cases I succeeded in obtaining even with dilute spirit
the separation of carotinoids in crystalline form. After being placed
for one day in 70 °/, spirit the corolla of Calceolaria rugosa was
seen to contain orange-yellow crystals, loose plates and aggregates.
The petals of Chelidonium majus when soaked for a month in
20°/, spirit are found to contain not only orange-yellow and yellow
drops and globules but also orange-yellow needle and thread-shaped
crystals, some straight and some very much curved. They are often
attached to the globules and give the impression of having grown
out of them. In the flower of Narcissus Pseudonarcissus crystallisation
of the ecarotinoid took place already after one day in 20°/, spirit.
Long continued treatment with dilute spirit may cause the complete
decomposition of the carotinoid; this was already the case in Narcissus
Pseudonarcissus after a few days.

Finally I wish to point out that on account of ARNavD’s ') inves-
tigations it must be assumed that the results sometimes depend greatly
on the season of the year. ARNAvD found, for instance, that the leaves
of the chestnut and the stinging nettle contain most carotin during the
flowering time (May). I also found that the separation of crystals
in one and the same species was not always the same. This was
especially the case in Cladophora, in which treatment with Momisca’s
reagent sometimes resulted in the separation of many orange-yellow
and a few red crystals, and at other times yielded many red and
a few orange-yellow ones. It is desirable to point out this difference.
When these experiments are repeated by other investigators it must
be taken into account.

It must be admitted that the results of the above crystallisation
experiments point strongly to the frequeni occurrence of several
distinct carotinoids in a plant. In a subsequent communication the
behaviour of carotinoids with respect to reagents and solvents will
be dealt with and the results of the direct and indirect methods will
be summarised.

1) A. Arnaup, Recherches sur la carotine; son réle physiol. probable dans la
feuille. Compt. rend. CIX, 1889, 2, p. 911.

527

Astronomy. — “Determination of the geographical latitude and
longitude of Mecca and Jidda executed in 1910—'11.” By
Mr. N. Scuertema. Part I. (Communicated by Prof. E. F.

VAN DE SANDE BAKHUYZEN).
(Communicated in the meeting of May 25, 1912).
Il. Lntroducton.

Mecca as we know is the holy city and the meeting-place for
Mohammedan believers. Yearly some 200.000 gather there from
different parts of the world in order to make their pilgrimages and
many of them stay there for a couple of years to gain a thorough
knowledge of the doctrines of their religion.

From an economical and political point of view as well as for
the history of religion Mecca is a place of great significance. Moreover
it forms an important starting-point for the geography of the interior
of Arabia. Hence it is not surprising that constant efforts have been
made to obtain closer and the most accurate possible knowledge
about this centre of the Islam; but great and peculiar difficulties
are connected with these endeavours on account of the fact that
entrance into the “holy domain” is_ strictly prohibited to non-
Mohammedans. Only now and again a few Eurepeans succeeded in
stealthily penetrating into it and spending there some time.

It is well known that among these stands first our compatriot the
present professor Dr. C. Snouck HurGronsr, who spent some eight
months in Mecca and put down his exhaustive researches in his
standardwork about this town. It stands to reason that my position
as Consnl of the Netherlands at Jidda, the harbour of Mecca, often
brougbt me into contact with this scholar, and it was he who in
the course of our talks drew my attention to the fact that so much
scientific work might be done in the Hedjaz. In particular he pointed
out that even the geographical position of Mecca was not accurately
known and he raised the question if I might not supply this deficiency.

Others had succeeded in making fairly accurate plans of the town
but its absolute position had not yet been determined with sufficient
exactness. Lack of good instruments, which are not easily transport-
able and the necessity of taking care that no attention was drawn
in the vicinity had generally prevented astronomical observations.

The only person by whom direct determinations of the latitude
and the longitude of Mecca have been published is Aut Bey EL ABAssI,
or at any rate the man who under that name travelled in many

528

oriental countries from 1803 to 1807 and in the latter year also
visited Arabia and Mecea. His ‘Travels’ were published in London
in 1816"). He made his astronomical observations with a reflecting-
circle of 10inch diameter with 4 verniers by Troughton and an
achromatic telescope by Dollond of 2'/, feet, with the aid of two
chronometers by Brooksbanks and Pennington (see Vol. 1, p. XVII,
Vol. 2, p. IX). The latitudes were determined by meridian altitudes
of the sun and stars, the longitudes by the transporting of chrono-
meters, by lunar distances and by observations of eclipses of the
satellites of Jupiter. Of his determination of the position of Mecea
it is mentioned in particular that it was accomplished by means of
altitudes of the sun and of lunar distances (2, 94)”); in the meantime
the chronometer by Brooksbanks had been broken, while probably
shortly afterwards, that of Pennington was stolen at Mina in
the neighbourhood of Mecca, so that the determinations of longitude
could not be continued. Ai Bry’s results, especially his longitudes
such as they have been published can only be of little accuracy.
Taking, however, into account the good instruments he had at his
disposal, it is probable that a renewed calculation might amend
matters, but his original observations are not likely to have been
preserved.

Besides from direct observations the position of Mecca might also
be derived from that of Jidda by means of journeys between
the two places with noted directions and distances, as the latter
place has at present been accurately determined by the obser-
vations of the English hydrography. Of these itineraries Husrr’s*)
seems to stand first; it has been accurately calculated and discussed
by J. J. Hess. Yet Hess‘) himself must attribute to his results for
the longitude and latitude of Mecca mean errors of resp. + 3’.2 and
+ 3’.8,

So even after this last investigation the position of Mecca was very
unsatisfactorily determined and Prof. SNouck Htreronge’s proposition
to try and obtain greater accuracy attracted me greatly. In the
summer of 1909 I therefore applied to the director of the Leyden
observatory, Prof. E. F. vAN DE SANDE BAKHUYZEN, Who was much
1) Travels of Aut Bgy in Morocco, Tripoli, Cyprus, Egypt, Arabia, Syria
and Turkey between the years 1803 and 1807, written by himself. London 1816
2 vols.

2) Erroneously J, J. Hess says in his Geographische Lage Mekkas that ALI
Bry’s longitude of Mecca is based on eclipses of the satellites of Jupiter.

3) CHARLES Huser, Journal d’un voyage en Arabie. Paris 1891.

4) J. J. Hess, Die geographische Lage Mekkas und die Strasse von Gidda nach
Mekka. Freiburg 1900. ;

~~ oe

529

interested in my plans and kindly promised me help and advice.
The execution of the work was now rendered possible and by the
kind dispensation of His Excellency the Minister of Foreign Affairs,
to whom I here respectfully render thanks, I received a royal
commission to execute astronomical observations in the Hedjaz.

Let me say first of all in what way I intended to set about the
proposed plan. As it was quite impossible for me to enter Mecca
and make observations, the help would be asked of Mr. A. Sani,
Pupil-Secretary-Interpreter of the consulate. As a Mohammedan be was
perfectly free in his movements within the holy domain and having
finished the 5 years’ course of the Secondary School at Batavia, he
was sufficiently well-grounded to successfully make the astronomical
observations. Let me add that Mr. Sani showed an eager interest,
when | communicated my plans to him.

According to the consultations with Prof. BakHuyzen a more detailed
plan was now made out for the execution of the observations. For
the determination of the latitude of Mecca circummeridian-altitudes
of stars were to be observed and the same was to be done also at
Jidda, partly for practice, partly for the examination of the instru-
ment and of the employed method of observation and finally to
mutually control the results obtained by the English hydrographers
and by ourselves. Secondly the difference of longitude between Jidda
and Mecca was to be determined by transporting some chronometers
to and fro between the two places, if possible a couple of times,
while during the stay in each place as many determinations of time
as possible would be made by altitudes of stars in the east and in
the west. All the observations at Mecca having to be accomplished
by Mr. Sauim, also the corresponding determinations of time at Jidda
wanted for the derivation of the difference of longitude were to be
executed by him. All the observations were to be made with a small
altazimuth.

First of all I now tried to use the rest of my furlough to practise
making observations at the Leyden observatory. The exceedingly
unfavourable summer of 1909 gave, however, only very rare oppor-
tunities for observations and so I had to leave again for Jidda at
the end of July without having acquired sufficient skill in observing.

Consequently the observations | accomplished after my arrival at
Jidda left much to be wished for in arrangement as well as in
accuracy. Besides, other circumstances, among which an extremely
busy time at the consulate, concurred in impeding the work. Owing
to all this the material collected in the winter of 1909—10 has so
little value that we can henceforth leave it out of account.

So)

Proceedings Royal Acad. Amsterdam. Vol. XY.

530

Fortunately the next year was in all respects more favourable
for my enterprise. During my furlough in the summer of 1910 I
again had the pleasure to work for three weeks at the observatory
under the guidance of Prof. vAN DE SANDE BakuUyzeN, and this time
the heavens often gave an opportunity for observations. After my
stay at Leyden I was moreover able to practise quite by myself
for a few weeks in Gelderland with the instrument I had taken
with me.

Under good prospects I therefore returned to Jidda towards autumn,
and when early in November the greatest heat and also the busiest
time at the consulate were over, I could begin regular observations
and also Mr. Sam could practise systematically under my supervision.
Soon we were able to execute determinations of time and of
latitude alternately on succeeding days. But now we met with another
mischance. The chronometer employed for the observations began to
accelerate very much and very irregularly and at last it stopped
altogether (December 2). Since no observations could be made with
any of my pocket-chronometers, the only thing left to do was to
stop our observations until another box-chronometer could be for-
warded from Leyden. .

Owing to this ill luck and on account of the irregular connexion
between Holland and Jidda, a delay was caused of more than six
weeks. Not till the end of January 1911 could we resume the obser-
vations and with a view to the advanced time, it seemed best that
they should further be done by Mr. Sauim alone.

Thanks to his ability and zeal the series of observations undertaken
could be brought to a satisfactory result between January 25 and
March 23 1911. During this time three journeys were made to Mecca.
Before the first journey and after the 1**, 2>¢ and 3"¢ the corrections
of the chronometers were determined at Jidda on 23 nights and
during the journeys 14 determinations of time were accomplished
at Mecca. Besides, the latitude of Mecca was determined on 10
nights and that of Jidda on 13 nights, while for the last mentioned
place already 7 determinations of latitude had been accomplished by
the two of us in Nov.—Dec. 1910.

Finally, a journey from Mecca to Jidda made on foot by Mr. Sati
with the determination of distances and directions enabled him to
make a map of the road between the two places.

As much as possible we calculated our observations ourselves,
also to continually control our instruments, but of course the accurate
calculation and the systematic derivation and discussion of the results
could not take place until after my return to Holland.. These have

531

been done at the observatory at Leyden under the supervision of
Prof. vaAN DE Sanpe Bakunuyzen, who also investigated the best methods
of combining the observations. The extensive calculations have been
for far the greater part executed by Mr. H. W. Hammrsma, late chief
mate of the Royal Dutch Navy.

In this way results have been obtained for the geographical position
of Mecca which certainly exceed in accuracy all that has been
known up to this time and therefore I take the liberty to offer a
paper on this subject to the Royal Academy of Sciences.

I. L/nstruments. Stations of observation.

The instrument with which our observations were made was the
universal-instrument Pistor and Martins N°. 905, belonging to the
Technical University at Delft and kindly lent to me by Prof. Heuvetink.
The same instrument had formerly been employed by Mr. S. P.
L’HonorE Naser of the Royal Dutch Navy for his observations for the
demarcation between the republic of Liberia and French Congo.

The telescope of the instrument is at the end of the horizontal axis,
while for the observation of small zenith-distances a reflecting prism
ean be brought before the ocular. The circles are read with verniers,
the diameter of the vertical circle is 130 mm. and that of the
objective is 28 mm. The value of a division of the level attached
to the alidade-circle is about 8”. During my first stay at Leyden the
spider-lines were broken. They were replaced by two horizontal
threads only, at about 6’ distance from each other.

For a moment we had thought of employing instead the small
universal instrument of the Leyden observatory, which has the same
dimensions but is read with micrometer-microscopes. The consideration,
however, that it is advisable in the damp and warm climate of Jidda to
make as little use as possible of spider-threads especially of movable
ones, made us give up this idea.

In the choice of the chronometers to be used, particular attention
had to be paid to the peculiar circumstances attending the transport
from Jidda to Mecca, which is done by camels, so that shocks cannot
be altogether avoided. Moreover the road is far from safe; nearly
every year a caravan is attacked and robbed by Beduins and it is
therefore desirable not to take any conspicuous boxes. To carry these
on foot would be altogether impossible. Discussing this point with
Prof. VAN DE SANDE Bakuuyzen and Mr. C. F. J. Cosyn, Chief of the
bureau of instruments of the Royal Navy, the latter drew our atten-
tion to the pocket-chronometers of Leroy, the so-called chronometres-

Do2

torpilleurs. These had been used by Mr. Naper in the above mentioned
observations and had proved very satisfactory (see his communication
in Marineblad, vol. 24), while also at Mr. Cosyn’s bureau they had
been found to go very regularly.

Through the kind permission of the Admiralty six of these
watehes have been lent to me, while the Home Office took the
risks of their carriage to and in the Hedjaz. I here express my
respectful thanks to their Excellencies the ministers.

In order to carry these six watches Mr. Naser had had a wooden
box made with six pigeonholes, which was again to be packed into
a leather bag to be carried knapsack-wise. This box and this bag
we were allowed to employ, and transporting the watches in this
way we could be pretty sure that they were free from disturbance.

The observations, however, could not be made directly on their
very low ticks (5 per second) and therefore I had from the Leyden
observatory the loan of a box chronometer by Cummins. As I have
said before, however, this chronometer got out of order in Nov.
1910, and then Prof. Baknuyzen sent me another chronometer, by
Dent, so that the greater part of our observations has been made
with this one. /

Finally my equipment contained an aneroid-barometer marked :
Holosteric 7225 with an attached thermometer, a separate thermo-
meter for the external temperature and a magnetic boussole. The
correction of the barometer was determined at Leyden, through a
comparison with the normal barometer of the observatory and was
found to be —1™™.5 in Dec. 1909 and — 2™™.8 in Aug. 1911.
No dependence on the reading of the barometer was appreciable and
so I corrected all my readings with — 2™™". As corrections of the
attached thermometer and of the other one I found respectively
+ 1°.0 and — 0°.5, which corrections have always been added.

In the beginning there was some difficulty in getting the universal
instrument well stationed at Jidda. The observations could not be
made in the open because that would have been very conspicuous
and we should certainly have been molested by the population, while
no doubt difficulties would have arisen with the Turkish authorities.
A fairly large enclosure next to the consulate, which I had been
thinking of, proved to be impracticable, since the ontlook to the west
was too far intercepted by the consulate.

So there was nothing else for it but to find a place on the roof
of the consulate. This seemed to be easy, since here, as everywhere
else, there was a flat roof offering sufficient room. Such a roof,
however, rests on fairly thin beams over which matting is spread

covered with a layer of cement, so that it trembles when walked
upon. Yet I succeeded in constructing a fairly stable mounting; near
one of the corners of the roof on two walls that crossed each other
and were raised a few centimeters over the roof, two heavy beams
were laid and cemented down and on the top of these two thin beams
were nailed on which the tripod of the instrument could be placed.

For further illustration see the picture on plate I. This shows that
the tripod was made heavier by a big block of stone and we took
eare not to touch the supporting beams, although we had to adopt
rather uncomfortable poses for some of the positions of the telescope.
We soon got used to this, however, and the end was attained. We
could now walk round the instrument, even stamping our feet, without
causing the bubble of the level to move in the least. Afterwards
Mr. Sautim™ arranged his station as Mecca in exactly the same way
on the roof of a house rented by me.

The only thing sometimes preventing pleasant and quiet working
was the noise in our neighbourhood. Regularly every evening at
about 8 o’clock there was a musical performance by the Turkish
military band at Jidda, and even more troublesome was the noise often
occurring in the evenings in my neighbour’s house and occasioned
by an ice-machine making almost two turns per second. All we
could do was to wait till quiet should return, although sometimes
stars were lost in this way.

We had also made a point of determining, if possible every night,
the zenithpoint of the instrument on a signal at some distance. This
was done in order to continually control the mutual stability of the
parts of the instrument, and also to facilitate the computation of the
observations and to trace immediately eventual errors, e.g. in the
reading of full degrees or in the employed star. At Jidda we used
as signal a lantern with a circular hole placed on the roof of the
sufficiently far off French consulate. At Mecca the observer used a
black spot on the wall of a post situated on the Jebel Abu Kobeis
a hill quite close to the town.

3. Value of the parts of the level. Zenithpoint of the instrument.

The divisions of the alidade-level are numbered in such a way
that if the reading of the bubble is too low, the reading of the
verniers must be increased. The value of a division was measured
a couple of times by displacing the alidade, the instrument being
clamped.

534

In Oct. 1909 11 determinations in 9 days gave 1 d.= 7.85 + 0".20
in Oct. 1910—March 1911 15 determinations
1 19 dayS .. 0. fies te Roe eee

while all the determinations together would yield 1 d. = 8".46 + O".17

Will it be better to use for our observations the value 8”.91 or
8".462 Since 8.7 had been actually used for the calculations, there
did not seem to be any reason to change. The influence of an error
in the value of a division on our final results is but small. A change
in the adopted value by 0".5 would alter the results for the latitude
of Meeca and of Jidda with less than 0”.2.

The zenithpoint was with a few exceptions determined every
evening and each time for both the horizontal threads. In the following
table have been collected the means of the two results together
with their differences, i.e. the mutual distance of the threads. (See
the table on p. 535).

For each period there have been added the means of the daily
results; in forming these means we have left out of account Nov.
18 and 24, the results of which days are divergent.

From this table it appears that in each period the zenithpoints,
determined on different evenings, mostly agree satisfactorily, but that
after every journey the reading for the zenith has become a little
higher. After the last journey back from Mecca it has considerably
increased, with about 4’.5, probably owing to a displacement of the
level-tube with regard to the alidade. A few oscillations seem to
appear in the thread-interval, while two very diverging results occur
in Nov. 1910.

4. Determination of the geographical latitude of Jidda
and of Mecca.

Coming to the observations proper I will now first communicate
the latitude determinations executed at Jidda and at Mecca and the
results derived from these. For their reduction we must naturally
know the corrections of the chronometer used, just as knowledge of
the latitude is required for the reduction of the time determinations.
I will, however leave the tables containing the chronometer-cor-
rections till the next paragraph.

With a few exceptions each latitude determination consists in the
observation of a northern and of a southern star, each in the two
positions of the instrument. Every time two pointings were made,
one on each of the two threads; the level was always read before
and after the reading of the verniers.

‘
j

‘

4
.
.
4

ee ee eee ee

939

ZENITHPOINT DETERMINED ON THE SIGNAL.

Mean | Thread- Mean Thread-
zenithpoint interval zenithpoint interval
Observations 1910 3rd period Jidda
SCHELTEMA a
_.\ ae a Febr. 18 90° 12'17''4 5'56'1
| ah 20) 18.8 49.3
Nov. 18 90° 12'20"0 eLs] = ey 4.9 44.8
‘ 2a) | 8.1 56.9 019112 cq
: Be 79 513 Mean 90° 12'13''7 5'50'1
pe ae | 16.7 oe 06-4. ; =
a od | 15.8 53.9 4th period Mecca
Mean 90°12'11"9" |.-- 5'54"6 :
ae OF 4 Febr. 24 90° 12'16"4 | - 6'5'0
SALIM pes. 16.2 4.1
Ve lai. 16.7 13.6
ies (ih iid (ain aia freee 18.6 12.9
Nov. 24 90° 11522 5'18"1 Mean 90° 12'17'0 6 8'9
ee 20 69.9 41.2 ee : ae
ws oo 54.1 | 39.6 a : :
Mean 90°12’ 2°0 | -5’40"4 5th period Jidda
~ ae see | ie aaa to a
; March 2 90° 12'21"4 5'40'3
Observations 1911 z 3 5.1 51.0
: ; $ a 28 .2 51.8
Ist period Jidda : 3 247 46 1
=e o.oo aie. go Mean 90° 12'24'8 5' 47'3
Jan. 23 CO? Th 537 5'44''4 a wots er
ss 25 60.2 54.6 :
é 6 473 50.0 6th period Mecca
- 28 58 .0 49.7 : = <n a a
» 30 57.8 48.1 Marchl1 90° 12'24’'8 6! 92
" 31 55.8 39.4
t “ae 31.9 bs
Febr. 1 52.0 50.9 9 9
= eae Zoo 8.2
3 60.2 | 53.8
= eee Soa 7.8
” 6 Till A 48.6 S
= fs fn 16 38.3 5.0
a | 54.2 | 34.4 17 35 .6 6.2
8 48.5 | 46.8 yi :
: 12 | 56.8 51.0 Mean 90° 12' 312 6' 7'9
Mean ; 90991155" 5'47'6 = ae = a =
A Sa ee ee z Tth period Jidda
2nd period Mecca a iehiee ee: sve,
Se a March 19 90° 16'53'"4 5'49"1
ci tA 67.0 52.5
Febr. 15 90°12'10°2 | 5'52"5 an tA 49.6 70.0
mm 16 17.0 61.4 i oe 55.6 64.8
Mean a Sue 12) 136s = 25'57"0 Mean 90° 16’56"4 | Sa

In reducing the observations that value of the zenithpoint was
used, which had been determined on the day itself. In the very
rare cases that the signal had not been observed the zenithpoint
has been derived from the determinations of preceding and subsequent
days.

536

We have always tried to choose the two stars for one evening
in such a way that their absolute zenith-distances would not be
too great and almost equal, in order to practically eliminate from
the result of each evening the flexure of the instrument and the
systematic division-errors of the cirele. We have been fairly success-
ful in this and find:

Z Zn — Zs Mean (zx — 7 )
Jidda 1st series 37° to 56° — 38° to + 4° —1°.5
z gua s AOD se 440 A eee a
Mecea Je ae 4 eee 200

while one evening only the zenithdistance has exceeded 45°.

Both the chronometers employed in the observations (as well as
the Leroy-watches) had been regulated after mean solar time, and
so their readings, after having been corrected, had still to be reduced
to sidereal time. In all our calculations account was taken of course
of the variation of sidereal time at mean noon with the longitude.

The pointings were mostly arranged fairly symmetrically with
regard to the meridian. The reduction to the meridian was computed
with the aid of ALsprecut’s tables; the term dependent on sin* 4 ¢
has always been taken into account if it exceeded O".05. The star-
places were taken from the Nautical Almanac, and besse1’s refraction
~was used.

Below I shall first give as an example the detailed observations of
one night, viz. February 25, 1911, at Mecca.

The given temperatures and barometer-readings are corrected
ones. The level-readings given are each time the mean of the
readings before and after those of the verniers, which nearly always
agreed fairly well iter se. They represent the deviations of the
position of the bubble from the middle of the graduation, whereby
the sign is taken positive when the reading of the bubble was too
low and the reading of the verniers had to be increased.

In the table the 1st and 2"¢ column contain the star and the
position of the instrument; the 3°¢ column contains first the chrono-
meter time of the pointing, then the hour angle derived from it; the
4th gives the readings of the two verniers, the 5‘ the employed
zenithpoint. The remaining columns need no further explanation.
Finally we have given the results for the latitude, such as follow
from the observations of this night.

lA. 2b je ot

a ee

ial a i rte i ii i et Ee a a

North star

537

DETERMINATION OF LATITUDE.
Mecca, 1911 February 25.
Z 24°29’.

a Aurigae

South star € Orionis 2o 2d.
T.ext. TT. Bar. Barom. Level
a Aurigae T.L. 28.3 28.9 735.1 + 1745
+ 1.45
Pike t 21.8 28.3 fae. (2.05
— 2.6
COrionis T.R. 27.8 28.3 7353) + 1.3
+ 0.95
Tot, sat. 28.1 735.5 —18
— 1.6
Star | Instr. pe ee Verniers Zenithpoint Refr. Red. on Latitude
Hour angle | merid.
N. | T.L.| 18365, 65°38 20" 90° 97142 24"1 —1'36"7 21925'21"1
— 537.0 245 38 30
22 14.0 65 45 30 L518 .3; |-24.0) | —. 12:0 4.9
—1 58.9 245 45 45
fr: Re. 30 24.0 114 46 20 15 18.3 | 24.1 | —1 58.2 27.9
+6 12.6 294 46 40
| 34 33.0 114 43 50 914.2 24.1 —5 29.4 21.2
+10 22.3 204 44 10
S: al. Bee 44 23.5 | 113 41 35 |90 15 18.3 | 22.9 | —2 40.8 | 21 25 3.4
—5 55.1 | 293 42 5
48 11.0 | 113 33 20 9 14.2 | 22.9| — 20.6 9.4
—— 2 P08. 295) Sar 50
T.L.| 5616.5 | 664225) 9 14.2 22.9| —2 45.2 10.4
+ 5 59.9 | 246 42 45
0 20.5 66 43 0 15 18.3 | 23.0 | —7 45.4 32.9
+10 4.6 | 246 43 30

Latitude North star 21°25’20’’3

”

South star
Mean

14. 0
21°25/17''2

538

RESULTS OF THE DETERMINATIONS OF LATITUDE AT JIDDA.

Nonthys tar Sion the ota
North+South
pat. ¥ ; 2
| De bs eel bs Mean ii ad Ce a2 Ake. Mean
First Series
1910 21929! | 21920! 21° 21°29' | 21°20’ 21° 21°

Nov. 18 |Sch; 16"1 32"9 | 29'24"5 8"3 12°7-| 29105 4) 2917S

ee Se 178| 18.8|| 22.6 70| 148] ts
> eset re }saied0 cape 8.6
» 25 |sch| 298 |—20/° 13091 76 | 2021 ig8]) Ge |
>». 21Sa| i5.1-| 333] 2421) t98 | 594 VO) aSe
so) ie 27.1 3.0| 15.0|| 84 | 30.0| 192\| 174 |
>» 30|Sch| 5.4 712| 63] 27 | 173] 195] 129 .
Dec aisisa A eS — 05 10.3

1.1 27.61) 132. aie

Second Series

1911 Sa | 21°29") 21929! Z12 PAIS |e 21°28) Pic pi AS!

Jan. 25)» 158 29"8 | 2922"8 300 3°6 2016"8 | 29019"8
» Be | o- S546 8/225 Ue 12.4
f- Ses | 24 | aes eee 18.8 i
> 301s | 97% | 95S) Saee 73) 343.1 208] 494 i
> 31/3 | 209 | 469 | 2840 Se lt oct ieee aia
Febr. 1| > | 31.6 | 12.6 |- 22.1 5.0/ 186 | 11.8|| 17.0
> 3l|> | 25.7 | 124 | 180] S01 lee34 oe] oom
» 6]> | 21.7 | 226 | 222] 153] 1344 44.41) Gee ;
> T/> | 20.0 | 2996 | 24849491 46 | 144 1)- gome
: >| 35541) 903 ere 53| 208 | 13.0] 204
> 20/> | 308 | 220 | 264] 35.2] 124 | 23.8]| 64
S et. a as 10.6 I= 14] as 6.9 8.8
March23|> | 168 | 22.7 | 19.8] 264] 70 | .16.7]) 182

hed in Aaa a eens Seek tle od ~

N. SCHELTEMA. “Determination of the geographical latitude and longitude of
Mecca and Jidda executed in 1910—’11”’. Plate I.

Proceedings Royal Acad. Amsterdam. Vol. XV.

539

Secondly there follow the results from all latitude determinations
first from those at Jidda, subsequently from those at Mecca. In these
tables have been collected the results from ‘Telescope left’ and
“Telescope right” for the north star and for the south star; the
values given are the mean results of the pointings on the two threads.

On Dec. 1 and Febr. 21 no zenithpoint had been determined.
For Dec. 1 we have used 9/9".4 and 14’43".5 and for Febr. 21 the
mean of the results of Febr. 20 and 22. For Nov. 23 too a mean
has been employed of that date itself and of Nov. 25, 28 and 30.
On Nov. 23 and on Febr. 21 one star had not been observed in
the two positions of the telescope.

For the few days on which the observations were not complete,
we have in order to deduce mean results employed the systematic _
differences found hereafter. (See the table on p. 538).

RESULTS OF THE DETERMINATIONS OF LATITUDE AT MECCA.

Nom tines tat Sionttheso. baer
oes eee ise < ane North+South
| 2 ;
rio |i. IR |--Mean ie ir. Kee) Mean
1911 Zle25 eZ 1O25! 21° ZLO25 I 21025! 21° 21°

Bebr. [5 | Sa}. °21"5 11"5- -1-2516"5 39 S001 | 25970) 25'16"S

meiG}s | 9 | 21) 55) 126 | 341 | 2.4] 24.4
Bete Piao rere | 203) 216 |) 64 | 140] 172
oes a78 | 151 21.4 |) 23.1
eh hie | 2650 24 .4 2572 20 .0 10 .4 15:2 20 .2

Marchii| » | 22.4 | 53.4 | 37.9|| 368 | 272 | 320]] 35.0
pers 21.8 | 135 | 206|| . 223
Peres ors Fo es | i490] 22.9 | 47.3 | 35.1 25.0
eer a | ie | 198 || 144 | 33.8 |: 26.1 23.0
iets | 235 |°287-|. 26.1 || 21.2 | 196 | 204]) _ 23.2

(1o be continued).

540

Astronomy. — “Determination of the geographical latitude and
longitude of Mecca and Jidda executed in 1910—11.” By
Mr. N. Scueutema. Part Il. (Communicated by Prof. E. F.
VAN DE SANDE BAKHUYZEN).

(Communicated in the meeting of June 29, 1912).

4. Determination of the geographical latitude of Jidda and Mecca.
(Continued).

About the results given in the two preceding tables it must still
be- noted that some of them in the first series at Jidda depend on
one pointing only. These are: Nov. 23 North star T. R., Nov. 29
North star T. L. and T. R. and Nov. 26 and Dec. 1 South star
oi cand Vite |

In the first place we shall now see what may be deduced about
the accuracy of our observations as regards chance errors, from a
comparison of the individual results.

If the mean error of one pointing on a star be . . . .m
of one pointing on the signal be. . . . . M

>> > 39?

then we have

: : ; : L >
m. error of the zenithpoint for the mean of the two threads 5
(m. error)? of a zenithdistance derived from two pointings

a: 1 1
on the star in one position of the telescope .. pitts +7.

We may now consider the m. error of a latitude gy to be equal
to that of the zenithdistance from which it has been deduced and
thus we obtain:

1 1
mn. e.)? of gy from one posit. = | = Pee = M
4 1 1
3. Of {9,2 Op e— fl = 7m’ + — Mf
1 oe
Brae 3 : (¢, tog) =W= 7”
4 if 1
” of 2 (Py— Ps ) — IV — g m? é
ee is
3 Oh —(9_ P3)= Van, }

from which: I] + Ul=

DT S22

| YY ool

54)

We now deduce the values of I, IH, and Ul by comparing the
individual results with their mean, first of all for the observations
at Jidda and Mecca separately, afterwards for all together. In order
to deduce in the latter case the values of II (just as afterwards o
IV) the general mean of the gy, —y, (and later on of the Pu— Pg)
has been employed. The result was, however, practically the same
when the two separate means were used. The first series of obser-
vations at Jidda has been left out of account throughout this investigation,
as it was less homogeneous and besides contained Mr. Sauim’s first
observations, when he had had little practice as yet.

JSidda Mecca Zogether

(=O. 66)? — 11'7-96-(4- 10.91)? = 119.08 (+ 10".88)? = 118.44
Me ated je —— Ja 00 (wo .Jo) = 69.40 (+ 8".99" = 80.74
a On 9 (a i OD) == 49.71 (+ 6".09)!. = 37.48

From this appears very satisfactorily that Il + I11—TI, while we
find in the three cases :

Pe (S10)? = 65.60+ (+ 47.44)? = 19.69 (+ 6".60)? = 43.61.

We can now compare inter se the values of m and M. As the
signals at Jidda and Mecca were of a different kind the two values
of M must not a priori be accepted as equal. The differences found
between the m and M for the two places are, however, evidently
not real, and we may only conclude from the general results that
m and M are about equal, only possibly J/ slightly greater than m,
which wouid also a priori be probable.

This investigation raises the question whether it would have been
better to employ for the zenithpoint mean values from longer periods
instead of the individual results, and although the value of the
zenithpoint is generally eliminated, I still wanted to examine this.
Therefore the observations have also been reduced with the zenith-
point from the whole of the period in which the instrument remained
at one station, and then the squares of the mean error [| and II
have again been determined. As the last 3 isolated nights of observation
at Jidda have not been used here, the values of I and II were also
deduced again after the first way of calculation.

Thus we found:

Jidda Mecca Together
With individual zenithpoints
Peete O07 = 2421.02 10". 91)* = 119.08 (+ 10".96)* = 120.06
I (+ 10 .02)? = 100.45 (+ 8 .33)?= 69.40 (+ 9 .22)7>= 84.93
With mean zenithpoints

et -99)7 99.88" (-F 11".68)-— 136.54 Ge 10°87) = s.21
Peco .01)7 = 79.3t (CE 9 32)? 86.95 (4 9.12)? =— S312

]

542

So no improvement is found for all the observations together ;
and although this is indeed the case for those at Jidda, the value
of Il remains still considerably higher than the one found for III,
which shows that even when mean values are used the mean error
of the zenithpoint has not yet become really small.

We shall now consider the values of IV and V, which, not taking
into account the influences of flexure and division-errors, must be equal

1 i ae ;
io ie Now these two errors must have been almost eliminated
5 Fey race = .
1 Laat
in the = (yy +s) owing to the nearly equal zenithdistance of North-

: 1
and Southstar, but they may be considerable in the 5 (Pn--Fs);

and as on different nights couples of different zenithdistance were
observed, the value of [VY must also have been increased by that
influence.

SEE:

bo|

We now find, adding for comparison the values of

Jidda Mecca Together
IV (4.3".36)) = 11.26 (44857 =23-51 (4. 4214)? = ee

Vo (4414 =17.19 (£5 06) = 25.60 (44 56) = 20

Fisalaty

4.99)? = 24.86 (44 31)? = 18.56

1
= gee 8 Oe

So we see that the values found for 1V are not only not higher

but on the contrary somewhat lower than those of V and that both
1 See

are almost equal to — .III, on which flexure and division-errors

»)

must have had some influence too. From this we may conclude
that the two influences cannot have been great.

Coming now to a consideration of the mean results for g in the
different positions, we shall first compare those with the telescope
left and right. ?

Denominating the correction of the employed zenithpoint 47 then
we see that

Northstar..7 LL." Awe = et

Ly RE, p= ee ?, — Op = + 2s
Southstar 7. L. Ag=+tAZ ;

I OR Khe Sees P,—Pp=—24Z

Ths: oh, caylee ee (P,— Pp y(~v-s) = +244

543

In this way we find
from all observations AZ=+1"54+1".2
from those of 1911 only +10+14

The value of 4Z is fairly small and almost equal to its mean
error. The 3 partial results Jidda 1910, Jidda 1911 and Mecca have,
however, the same sign. In order to correct one-sided observations
we have employed the value deduced from 1911, Jidda and Mecea
together, + 1”.0. :

In the second place we shall consider the differences between the
results from the North and the Southstar. Except on one night in
1910 the zenith-distances of the observed stars lie between 10° and
45° and the mean z is about 30°. The yy—vysg therefore contain
twice the flexure for a zenith-distance of about 30° and the influence
of the systematic division-errors cn an are of about 60°.

We now find:

Jidda 1910 yu —%5=— + 1".7 weight 5.5

pl Ok # ee eay pl td
Mecca _,, x ai) 8
from which follows for
all observations together + 3".0+1'.7

for the observations in 1911 +3 441.9

So the differences are not great. That the flexure of the telescope
would be small was to be expected. but our results prove also that
the systematic division-errors of the circle cannot be great. For the
reduction of the incomplete observations we always employed (even
in 1910), according to the results for 1911

5 (¢y— Ls y= 4 1".%

In this manner we deduced for all observation-nights values for
4(gy +), and the means taken from these, giving half weight to
the nights on which only one star had been observed, were considered
our final results. Moreover mean values have been formed from the
results in the separate positions and from the separate stars, again
giving half weight to incomplete observations.

So we found:
: Nth+ St
Northstar Southstar plac sth
+k T_E Mean Peds To “Mean
Jidda 21°
Sa SSA ay a a ee | 13°O -16"3. 14°7 29' 14"5
Siren feos 19.2. * 20.9 15.7. 16.3 16.0 29 18.5

544

Mecca 21°
22"1 24"5 233 20"9 24"2 = 22"5 25' 23"1
The results from the two series for Jidda are:
21° 29° 14.5 7
29 18 541 3
The difference between them a little exceeds the sum of their mean
errors. Forming for the first series separate results for the two
observers we obtain :
ScHeLteMa 21° 29'15"1
SALIM 13.9
which are in good accordance.
After full consideration the two series have been united according
to their weights and so our final results are :
g Jppa = 21° 29'17".0+ 1".0
g Mecca 21° 25'23".1+1'.5

5. Results of the determinations of time.

The determinations of time were always made by observing tlie
altitude of a star in the east and of one in the west. Each star was
observed in the two positions of the instrument and each time the
transits over both the horizontal threads were noted, the instrument
remaining clamped. Hence the zenithpoint for the mean of the two
threads was employed in deducing the zenith-distance, and for the
mean of the two instants the hour angle was then computed after the
usual formula

COS Z
COS ===

sin ¢ sin J

cos ¢ cos b

In Nov.—Deec. 1910 the chronometer of Cummins and since the
2" half of January 1911 that of Dent was used for the observations.
The rates of Cummins were very great and irregular until it
stopped altogether. I therefore omit the communication of the
chronometer-corrections and rates for the first period. They were
only used for the reduction of the latitude determinations and they
were sufficiently accurate for that purpose.

About the determinations of time in the second period I shall first
give the necessary data to form a judgment of the accuracy reached
as regards systematic and accidental errors. The two following tables
contain for this purpose the 4 separate results obtained each night.

As appears from these tables there is only one determination of
time at Mecca (Febr. 26) which is not based on an eastern and

545

a western star, while on another night (Febr. 25) 2 eastern and 2
western stars were observed. Further, on Febr. 14 (Mecca) and
Febr. 21 (Jidda) no zenithpoint was determined and this was derived
from preceding and following days.

RESULTS FROM THE DETERMINATIONS OF TIME AT JIDDA.

Stari East Star West

ieee ; = =: — E.—W.

5S ao lee Mean Es E. in ee Mean

1911 4+ 2h 4+. 2h
Jan. 25 7837 9589 23m 8363 8585 | “8530 | 23m8s58 | + 0s05
» 26| 15.71 | 14.46 15.11 13.86 | 13.12 13.48 | + 1.63
: 08 24.64 23.56 24.10 || 25.57 | 23.91 24.74 | — 0.64
» 30] 33.36 | 34.11 33.73 || 31.42 | 33.93 32.67 | +1.06
Benet | --38!6t -| 37:24 37.93 36.00 38.05 37.02 | +0.91
Febr. 1 41.61 40.44 41.02 | 40.34 | 41.05 40.70 | +0.32
Pas 48°04. | 47.88 41.96 || 41.41 | 41.78 47.59 | +0.37
, 6}| 0.47 | 59.27 | 59.87 || 59.72 0.14 59.93 — 0.06
ie | 5.08 4.51 | 24 4.82 5.08 4.80 | 24 4.94 | —0.12
=| 10:03 8.16 9.10 7.96 9.15 8.56 | + 0.54
Peat?) 25.25} 27.80 28.06 || 28.51 | 29.36 28.94 | — 0.88
, 18| 2.59 | 3.06 | 25 2.83 || 3.84 | 2.67 | 25 3.25 |—0.42
me} 14.12 | 14.84 14.48 14.19 | 15.81 15.00 | — 0.52
Py) 20.23 | 18.35 19.29 18.53 | 20.72 19.62 | — 0.33
» 22| 26.11 | 25.42 25.71 25.14 | 25.63 25.39 | +-0.38
Mrch 2. 10.84 10.14 26 10.50 9.21 9.80 | 26 9.51 | +0.99
ood | 13.80 | 14.17 14.03 14.70 | 13.83 14.26 | — 0.23
» 7} 30.96 | 30.37 30.67 | 30.23 | 29.85 30.04 | + 0.63
Pe-98 |}? 36.39 | 34.11 35.25 | 34.94 | 35.47 35.20 + 0.05
~ 19| 27.96 | 27.28 | 27 27.62 || 26.29 | 29.18 | 2727.74 | —0.12
eee) 32:53 | 33.26 | 32.89 || 34.41 | 32.78 33.60 | — 0.71
eat | 37.60 | 31.72 31.66 || 37.55 | 38.17 37.86 | — 0.20
> 23|. 47.84 | 48.75 48.30 || 48.32 | 47.84 48.08° | +.0.22

Proceedings Royal Acad. Amsterdam. Vol. XY.

546

RESULTS FROM THE DETERMINATIONS OF TIME AT MECCA.
eT ee =

|
1}

| Star East | Star West |

ie | E.—W.

pO TR Mean eae eat bs Teak: Mean

iol | pee) 4. 2h
Febr.14 2091315853. | 27m17883_ || 16806 | 19538 | 27m17572 | + O51]
A ib | 24 2 ope 4 hs eu | 22.04 | 23.87 22.96 | + 0.61
, 16| 28.24 96.49 | 27.37 || 28.73 | 28.86 28.80 | —1.43
_ o4| 11.99.| 13.10 | 28 12.49 || 12.92 | 11.26 | 28 11.79 | + 0.70
95,| 17,40 Ne ag4o aa | 18.30 | 17.10 17.70 | Oem
| 17.69 | 18.24 | 18.02 | 18.55 | 18.09 18.32 | [See

928 | | 91.33 | 22.88 22.10
21| 28.61 | 29.46 29.04 | 28.85 | 27.86 28.35 | + 0.69
Mrch11 | 22.53 | 24.28 | 29 23.41 || 24.60 | 23.63 | 29 24.11 | —0.70
, 12| 27.07 | 28.05 | 27,66 || 27,00. | 26.89 27.00 | +.0.66
» 14| 38.92 38.22 | 38.57 || 38.71 | 38.44 38.57 | 0.00
, 15 | 43.49 | 42.58 | 43.04 || 42.41 | 42.30 42.36 | + 0.68
, 16| 45.88 | 46.47 | 46.18 || 47.51 | 45.42 | 46.46 | — 0.28
, 17 | 50.40 | 50.29 50.34 || 50.32 | 49.17 | 49.75 | + 0.59

We must now first compare the results obtained in the two
positions of the instrument. If the observed corrections of the chrono-
meter are Az, and the correction of the employed zenithpoint is
designated by 47, then we find:

: Aitiz,— At

Eastern star A Z=-+a 3 a
hy, == ha

Western. star A Z=—@ = tL, 5 R

in which, if 4¢ is expressed in seconds of time and A Zin seconds
of arc, the mean value of the factor a is 13.8.

Leaving out of account the two days on which the zenithpoint
had not been determined and reversing the signs for the western
stars, we find as mean result:

ANG ge ag aN
alee 9 IR — 4 05.07

547

from which follows AZ—= + 1".0, i.e. tho same value as was found
from the determinations of latitude

Secondly the results from the eastern and the western star have
been compared iter se and the mean values obtained were:

Jidda 23 nights E—W =-4+ 03.13
Mecca 13 be + 0 .08
Together 36 o E—W =—-+ 05.11

If this difference is produced by a constant error in the measured
zenithdistances, then we find for its amount Az = + 0".8, while
+1".7 had been found from the determinations of latitude in
which the average zenithdistance was somewhat smaller. From a
comparison of the separate values for E.—W. with their general mean
we find, however, as mean error of the difference found in a single
night + 08.68, hence of the result from 36 nights + 0s.10, which is
equal to the mean difference itself. The obtained results are, howe-
ver, satisfactory, as we may conclude that no great unknown sources
of error have been at work.

Disregarding a possible systematic personal error, we may further
consider the mean error of }(E-+-W) as equal to that of 4 (E—W),
and we thus obtain as mean error of a chronometer-correction from
an eastern and a western star + 08.32.

At each time-determination the Leroy watches were compared
with Dent. In the meantime Leroy 5180 — Dutch navy 3 had
stopped and on the journeys to Mecca only 2 or 3 watches were
taken (2 on the first and second journeys, 3 on the third) for fear of
a possible mishap. Prudence demanded this, although now that
everything went off well, I regret that all the watches were not
taken each time. Naturally the mean errors of the observed corree-
tions of the watches will be somewhat greater than in the case of
Dent, owing to the errors of comparison.

The following tables contain the observed corrections for Dent and
the Leroy-watches and the thence derived daily rates; the first, two
tables according to the observations at Jidda, the next two according
to those at Mecca. On Febr. 25 Leroy 4129 = Dutch navy 77 was wound
up too late after it had already stopped (see the tables on p. 548—550),.

It is clearly: visible from the daily rates contained in the preceding
tables that the time-determination of Febr. 26 at Mecca, based on
one star only, has been less accurate. The same appears with even
greater force for the one of Febr. 21 at Jidda, although the ob-
servations of that night are apparently irreproachable.

For a closer investigation of the regularity of the watches we
shall use the rates which have been obtained during the stay at

36*

548

CORRECTIONS DETERMINED AT JIDDA.

March2

3
-

LeRoy 5192 || Leroy 4129
pe D. N. 7 | Dae
. {|
|
M.Time| Corr. | D. R. ||MTime, Com | D. Rj) “Cor. | (Deie
| } | || |
+ 2h — 0h || — 2h
Th 4m 23m 8560 | gh31m 2m13s86 | 9m 3382 |
| += 5s53 | + 0s24 || + 2510
7 49 14.30 |: eos a ae ee 1.85
+ 4.98 || See Sy | + 3.88
8 34 24.42 ||, PB 28-40 || 8 54.11
| + 4.51 | + 1.02 | + 3.42
Ay 33.20 8 71| 6.66 | ° 47.25
| +--4.33 || + 1.80) + 4.46
6 58 317.47 | | 9 10 4.78 || 42.59
eres 20 | + 2.51|| Bie 2:
7 38 40.86 | 9 394)~ ~2:20 || 38.66
S48 + 2.68 | + 418
7 20 41.71 | 913 1 56.90 |} 30.50
Fee ey | 2.47 +- 3.34
6 56 59.90 929 | 49.45 | 20.44
40718 | + 2.41 + 4.84
7156 | 24 4.88 | 1 7] 47.28 | 16.08
+. 4.11 | + 1.59 | 3.8
6 58 8.83 10 6| 45.49 12.48) ~
+ 4.85 | + 2.26 || + 3.56
8 16 28 .50 10 11 | 36.45 58.24
| |
+ 5.68 | + 1.87 + 4.09
10.16.) 25° Buea 10 48 | 25.21 33.60 |
+ 5.92 | + 1.94 + 4.83
9 30 14.74 1059 | 21.31 23.91 |
be Seer + 0.74|| | + 3.93
9 32 19.45 10 9} 20.60 | 20.99 |
+ 6.61 | + 2.74) + 5.41
1 48 25.58 935| 17.93 | 15.71 |
| + 5.48 + 1.13|| — Ou
||
10 26 26 10.00 1122] 8.84 | 51 20.24 |
ee | — 0.54 || + 4.68
9 52 14.15 1022) 9.36) \ 15.764
+ 4,12 + 0.09 | + 4.52
8 20 30.36 9 38 9.00 | 50 57.80
+ 4,53 | =—.14) + 4.35
10 35.23 fi 7 9.13 | 53.18
4 AB | — 0.21 | + 5.12
| 41 1 | 27 27.68 if 27 |. alas | 49 56.82
+ 5.90 — 0.66 || + 5.64
9 38 33.24 11, AAs 12208 |} 51.28
+ 5.04 = 02) + 4.83
a8 317.76 748| 12.70 | 47.10
+ 5.19 |
7 23 48.19 |
1|

com. ©

549

LERoY 3565

LeRoy 4127 LeRoy 4128
D. N. 80 D. N. 81 D. N. 84
M.Time| Corr, | D.R. || Corr. | D.R. || Corr. | DR.
aa 2h eat all
Qh3im 18m34s56 2644561 57m42s23
+ 1825 — 6s — 0546
S=-35,)- 35273 50.86 42.66
| + 2.49 =, 58 + 0.78
7 58 40.70 27 2.50 41.10
a oi — 5.60 = 621
8 71 | 44.65 | 13.74 41.64
| | + 1.90 | — 4.06 + 0.44
| 910 | 46.63 17.98 41.18
| So 85 — 6.35 “| — 0.08
| 939 | 48.54 24.46 41.26
| + 2.61 — 5.16 + 0.19
9 13 53.71 34.69 40.88
ae 2. Ot — 5.76 + 0.28
9 29 59.76 52.02 40.04
+ 2.42 — 5.38 + 0.42
Tr oP) oO el 94 56.87 39.66
| + 1.58 — 5.88 ta
103 6 4 Seale 28 3.48 40.07
| -—- 1.81 Sete ee + 0.06
10 11 10.96 | 25.04 39.83
| | + 0.47 = 5.02 — 0.09
10 48 13.80 55.30 | 40.40
+ 0.65 == 18 + 0.25
10 59 15.10 29 5.70 | 39.89
0.12 — 6.69 sie
10 9 14.41 12.16 | 41.38
255) Ses ED a)
9 35 15.88 15.92 | 40.31
A Bese, — 4.57 + 0.08
22s =. 86858 52.83 39.63
serif 21 | — 5.35 eas
2 a te 57.96 39.95
| + 1.68 519 — 0:86
9 38 34.41 | 30 18.58 40.18
+ 1.89 pate: + — 0.19
i esse, 36.42 | 24.18 | 40.38
| — 0.02 | A TY + 0.47
fie Jeo), 236.18 31 16.02 35.21
+ 0.15 | | — 4.52 + 0.35
6 a | 36.33 20.46 34.87
== 0-48 — 4.64 | + 0.22
7 48 35.91 24.48 34.68

590

CORRECTIONS DETERMINED AT MECCA.
wae 2t LeRoy 5192 LeRoy 4129
DENT 2521 D.N.7 po wi

M.Time| Corr. D. R. ||M-Time| Corr. |. D. R. Corr. | DR.

ee nn eee en ee
1911 sph. + oh = hy 4
Febr.14 | 10h40m) 27m17s78

+ 5591
3245" | 855 23.26
+ 4.73
MG | Be 28.08
4+. 5.54
24) 8 32 | 28 12.14 12h47m 1m]19s56 4m32s64
4+. 5.70 +. 0594 || — oh
Ehae"| 25.38 17.86 816 | 20.32] 49 6.80.
4+. 4,30 15,9 4+. 3815
ee |) kee 22210 1258 | 20.64 3.03
+. 5.40 | 44:67 + 4.03
pd abd oO 28.69 14 6 22.39 | 48 58.81
+ 4.68 + 0.36
Mrch 11 7 44 | 29 23.76 8 17 26.65
43753 + 0.40
8 27.33 835 | 27.05
“78.98 + 0.15
=) hh: eee 38.57 13 0 27.38
+ 4.01 — 2.45
ie (4 Cd 42.70 113 28| 24.88
4+ 3.63 — 1.39]
, 16 | 12 16 46.32 1315 23.50
| + 4.62 + 0.09
mae hue ee 50.05 8-18 | 23.57 |
en _____________
Leroy 4127 Leroy 3565 | Leroy 4128
D. N. 80 D.N.8! || D. N. 84 '
— As E =
M. Time) Corr, 9 |—DARS ie ior: 4) Ba: ! Corr. } | Dae
1911 4 2h | = Bi ory
Febr. 14 | 11h 5m) 21m47s67 | 25m58353 |
| + 0354 — 5558 |
ww 1S | at 47 48.23 | 26 4.27
| | + 0.15 = "501
» 16 | 13 56 48.39 | 11.91
+ 0.99
March 11 S17 2240387 55m 6393
| — 0.02 + 0875
54 ae 8 35 10.85 6.17 |
4- 0.43 | + 1.45
' 14 | 130 11.79 3.00 |
| + 0.28 + (1.26
45 | 13°88 12.08 | 1.71 |
ee | =
- 16 | 15-15 11.70 | 2.81
— 0:46 | | + 0.73

a | 6.98 1 asi | | | east

551

Jidda. First we find as the mean daily rates during 4 periods of from
-4 to 6 days each separated by journeys to Mecca:

Denn? 7 Doe @ Dina CC DN: 80: DN. Sk DN, Bet
Febr. 6—12 +472 + 2516 + 3°68 +1585 — 548 + 0:03
» 48—22 45.77 +184 +453 +053 —5.22 + 0.02
March 2—8 + 4.21 —0.05 +451 +164 — 5.23 — 0.18
» 19-28 +533 — 0.69 +5.26 —015 —458 + 0.29
Secondly the accidental deviations have been examined, first by
he
forming the mean value —WZLAA of the differences A between
n
two subsequent daily rates, and afterwards by comparing the rates
between Febr. 6 and March 23 themselves with their mean value
fog Aces
for the whole period and deducing the mean deviation —Y2A’'.
n
Both these mean deviations I and II follow here.

Dent DN.7 DN.77 DN.80 DN.81 D.N.84
ae Oct 091 ~+ 097 —+ 060 +095 + 061
me OG, 129 069 -- 0% +039 4.0.29

For D.N. 81 the mean deviation I becomes + 0857, if one time-
determination is excluded.

The striking things in these comparisons are in particular the con-
siderable acceleration of D.N. 7, owing to which also the mean
deviation II is very great; and secondly tke regularity of D. N. 84.

6. Derivation of the difference of longitude Jidda—Mcecca.
) J

From the corrections and rates of our watches given in the pre-
ceding paragraph we must now deduce the most probable value for
the difference of longitude between Jidda and Mecea. Apart from
the desirability of knowing the result yielded by each of the watches
an immediate combination of the results of all would be impossible,
because of the fact that on the different journeys different watches
were taken and only Dent 2527 was used throughout. We shall
therefore derive separately the results to which the 6 employed
watches have led, and only afterwards we shall endeavour to derive
from the whole of this material the most reliable final result.

Whereas each group of observations at Jidda or at Mecca usually
includes time-determinations on 4 nights, determinations on 11 nights
at Jidda, viz. from Jan. 25 to Febr. 12 immediately precede the

552

first journey to Mecca. But of however much value this long series
is for the investigation of the watches and of the observations them-
selves, it cannot be of any immediate use for the derivation of the
longitude. The longer the periods that are discussed the greater does
the uncertainty become in the calculated rates and corrections of
the watches, and soon its influence surpasses that of the errors of
the observation. The great difficulty lying here in the answer to the
question at what distance from the journey determinations of time
may still be used to advantage, this will certainly not be the case
for the observations in January. Finally only the observations of
Febr. 6-—-12 have been used as a first group.

In the following we shall indicate Leroy’s watches with the
numbers they have in the Dutch Navy.

a. Chronometer Dent 2527.

This was taken by Mr. Sam on all his journeys to Mecca and
we have therefore at our disposal 4 groups of observations at
Jidda, each including 4 nights, and between these 3 groups at Mecca
with resp. 3, 3 and 6 determinations of time. Hence the discussion
of the results obtained with this chronometer offers the best oppor-
tunity for comparing the different methods that may be followed
for the deduction of the difference of longitude.

This deduction must be based on the comparison of observed
chronometer-corrections at one place with interpolated corrections
with regard to the local time of the other, whether that interpolation
is made directly or in such a way, that we represent the corrections
found for both stations by formulae differing only in the value of
the constant term

An exhaustive criticism of these methods of calculation has been
given by W. Srruve on the occasion of his discussion of the results
of the chronometer-expeditions ') executed between Pulkowa and
Altona. He arrived at the conclusien that for observations made
during a long period with a great number of journeys in both
directions, as in his case, the representation by one formula, which
must then contain a rather great number of powers of the time,
would be unpractical. Our case, however, is somewhat different.
The number of journeys and the duration of each was much less,
and, whereas our determinations of time were much less accurate,
we had attempted to make up for this inferiority by observing on
several nights each time at each station.

1) F, G. W. Srruve. Expéditions chronométriques entre Poulkova et —_
St.-Pétershourg 1844, p. 117—128.

553

It therefore was difficult for us to decide whether the different
journeys would have to be discussed each by itself, or whether it
would be preferable to take two or three together. And so finally
it seemed best to follow both ways or rather try a number of
different methods of calculation.

As the smallest group of observations discussed together we have
always taken those obtained during the stay at one station combined
with those from the preceding and the following visit to the other
station. Then only a real interpolation is possible, and there is besides
another circumstance demanding this. The rate of a chronometer may
not only be subject to chance perturbations during the transport,
but there may also take place a systematic retardation or acceleration,
which continues thronghout the duration of the transport. So a
chronometer-correction calculated by means of extrapolation would be
subject to systematic errors. On the other hand it is easy to see
that in the calculation of a chronometer-correction for instance
during a stay at Mecca from preceding and following observations
at Jidda, the ahove mentioned error will be altogether eliminated
for a moment exactly between those of the observations and that it
would be small for other moments.

In this respect therefore such a group of observations can yield
accurate results. A uniform retardation or acceleration, however,
cannot be taken account of in this way but very imperfectly. This
will become clear when we represent the chronometer-corrections
by formulae. These will then contain terms with the square of the
time, and it will be easily seen that in a combination Jidda—Mecea
Jidda the influence of such a term and that of an error in the
difference of longitude will not differ greatly. If, however, a com-
bination Mecca—Jidda—Mecca is also discussed then the influence
of a quadratic term on the difference of longitude will have the
reverse sign. Hence it will be possible to eliminate that’ influence
by forming combinations of the two kinds and taking the mean of
their results. This approaches already the calculation of a quadratic
formula from a longer period.

I shall now communicate the numerical results obtained by means
of Dent 2527 using the different methods of calculation.

1. Results from the separate journeys.

Journeys to Mecca (J.—M.—J.). Determinations of time in Mecca
compared with interpolated values between the observations at Jidda
immediately before and after the journey.

554

4st journey 22d journey 34 journey
+ 2m + 2m 9m

Febr. 14 37535 Febr. 24 35:44 Mrch 11 34575
bs shocked on 3. Qe eo oo geal 2 dacoe
7) 26 36:60 ,» 26 34.49 » 14 34.55
Mean 37217 » 2 34.39 = MSS3i77
Mean 34:99 » 16 32.66

ye T8255

Mean 33°63
Mean of the 3 journeys + 2™ 35°26.

Journeys to Jidda (Me—J—Me). Treated in exactly the same way
they gave the following results.

1st journey 22d journey
oa 3m — Qm

Febr. 18 36529 March 2 32512
a ga aces i PO eee
Lele eaorent fee
io 822° Ba700 S20: 4200
Mean 35889 Mean 33857

Mean of the 2 journeys + 2™ 34573.

The combinations Jidda—Mecca—Jidda have also been calculated
by means of linear formulae, i.e. the corrections of the chronometer
~ determined at Jidda and at Mecca have been represented resp. by
formulae a -—+ 4(t—t,) and a’ + 4(¢—+,), from which the unknown
quantities were solved after the method of least squares. The difference
a’—a gives us the difference of longitude, or when a provisory value
for this difference had been applied, the correction needed by that
value. Of the 3'¢ group of observations at Jidda March 2 and 3
have only been used for the 2"¢ journey to Mecca, March 7 and 8
only for the 34,

So we found:

1st journey + 2” 35862 (+ 117)

2nd “f 35.62 (+ 0.65)

3rd - 02.93 (+ 0.91)
Mean + 2™ 34872

The values in brackets are the mean residual errors in the
observed chronometer-corrections, when they are represented by the
calculated formulae.

2. Results from the whole of the material.

We have represented the observations by formulae of the second

and third degree

ny +b (t—t,) 4 € (t=4,)?

and
a + Et) + 6 (tt)? + d(e—t,)?

from which the values of the unknown quantities have been deduced
by the method of least squares.

Five solutions have been found.

I by means of quadratic formulae

II by means of formulae of the 3'¢ degree

III by means of quadratic formulae, correcting the data beforehand
for the supplementary “transport-rale”’.

IV like I, but giving half weight to the 6 observations of the
3d series at Mecca.

V Like II, but giving half weight to the 6 observations of the
3°d series at Mecca.

Defining the supplementary “transport rate’ E. as the excess of
the daily rate during transport on that of the stationary chronometer
and putting t for the duration of a transport, we have as supplemen-
tary correction of the chronometer after each journey

A corr. — Agar corr. = suppl. corr. = tv. E.

Now A corr. could be determined from the time-defermination
next preceding and next following the transport, and yet be found,
for the mean of two journeys to and tro, independent of an assumed
value of the difference of longitude, while 4y,q; corr. could be derived
from the daily rates in the intervals next preceding and next
following the transport.

In this way we found for the suppl. corr. after each transport:

1st journey to M. and back -+ 2822
Qnd ees ate 3 : + 1.54
2 ae + ee . + 1.60

Mean influence of one single journey -+ 1579
i.e. the transport caused a retardation. This value was employed to
correct the data for solutions UI and V.

The solutions IV and V were executed not to give undue weight
to the 3° stay at Mecca with 6 observation-nights, overagainst the
1st and 2™¢ with 3 and 4 nights, since for each stay there are clearly
left systematic errors. Febr. 26 was left out in all solutions, The 5

solutions gave for the difference of longitude. a

556

I + 2m 33:73 (++ 1,84)
Il 33.80 (+ 1.85)
Ill 33.92 (+ 1.58)
IV 34.23 (+ 1.73)
V 34.38 (+ 1.47)

The mean errors in brackets have the same meaning as above ;
in solutions IV and V they refer to observations with weight unity.
Of all these solutions the 5 seems to me certainly to be preferable.
I have, however, communicated also the other results, since they
show the intluence of the different ways of treating the observations.
On the other band IJ shall not give the results of a discussion of 2
successive journeys to Mecca together. The thus obtained formulae
do not represent the observations better than the formulae deduced
from the 3 journeys together.

The final result for Dent 2527 I should like to deduce as follows:

The 3 journeys J.—M.—J. 1st meth. -++ 2™ 35:26

2nd meth. 34.72

Mean + 2™ 34°99

The 2 journeys M:—J.—M. +2 34.73
Mean + 2™ 34586

General solntion +2 34.38
Adopted final result + 273462

(To be continued).

Astronomy. — “Determination of the geographical latitude and
longitude of Mecca and Jidda executed in 1910—11.” By
Mr. N. Scuerrema. Part III. (Communicated by Prof. E. F.
VAN DE SANDE BAKHUYZEN.)

(Communicated in the meeting of September 28, 1912).

6. Deriwation of the difference of longitude Jidda- Mecca.
(Continued).
6° Watch N= 7:

Watch N°. 7 was taken on the 2>¢ and 3'¢ journeys to Mecca.
During the whole period of the observations it clearly showed a
progressive acceleration. Any direct influence of the transport, how-
ever, was not clearly visible; nor was this so much to be feared for our
carefully transported pocket-chronometers as for the box-chronometer
of Dent.

557

From the observations with this watch results for the difference
of longitude have again been derived in different ways.

1. From the separate journeys.
a. Journeys Ji—Me.—Ji.; Jidda-time interpolated between the
last time-determination before and the first after the journey.

2d journey 3° journey
2m + 2m
Febr.-24 35:08 March 11 36889
» 20 34.92 5 AD SOG
5 20. cap-O9 es AA tS
> 2 34.46 2 die 3o50
Mean + 2™ 34859 so thGie: yaaa
Omitting Febr. 26 34.82 Rov is “BAUsG
Mean + 2™ 35593

b. Journey Me—Ji—Me; discussed in the same manner.
Mareh 2) + 2™ 932527

- eO 39.13
aw: 34.20
tae 34.72
Mean + 2™ 33°58

c. Journeys Ji—Me— Ji; all observations (including Febr. 26)

represented by linear formulae
2>d journey + 2™ 35:22 (+ 2948)
ae is 36.46 (+ 1.05)

As the formulae for the second journey to Mecca represent the
observations unsatisfactorily, I adopt as the result of this journey
that of the direct interpolation excluding Febr. 26; for the 3'¢ I
adopt the mean of the results a and c, hence:

2nd journey + 2™ 34582
3rd ‘ 36.20

Mean + 2™ 35551
Combining this result with equal weights with result 6 we obtain
—- 2™ 34s 54.

2. From general solutions by means of quadratic formulae.

Of such solutions based on the whole material four have been
executed; I and IL respectively excluding and including Febr. 26;
Ill and IV as I and II but giving half weight to the six observations
during the 3'¢ stay at Mecca, for the same reason as in the case of Dent.

In this manner we found

058

I + 2™ 34564 (+ 0:90)
Il 34.59 (+ 0.88)
Ill 34.77 (+ 0.80)
1V 34.70 (+ 0.78)

1 adopted the mean of the results II] and IV, viz. + 2™34s74

and then as final result for watch N°. 7 the mean of the results
from (1°) the individual journeys and 2°) the whole material together
+ 2™ 34°64

c. 'Waick NA -7e

This watch was taken on the 2°¢ journey to Mecca, but unfortunately
it stopped between the observations of Febr. 24 and 25, as it had been
forgotten to be wound. Fora comparison of the corrections determined
at Mecca with corrections to Jidda-time we can therefore only use
extrapolated values .

So we found:

Febr. 24 + 2" 33-41

Py 36.77
En eaG 35.10
Peek 34.57
Mean I + 2™ 34596
Ba 34.56
i 34.51

The first mean value was obtained by giving equal weights to
the 4 days; for the 2°¢ we adopted weights inversely proportional
to the interval of time, for which extrapolation had taken place;
for the formation of the 3'4 we moreover gave half weight to Febr. 26.

After all it seemed best to ignore the smaller weight of the
last-mentioned time-determination, but to take into account the
intervals of extrapolation and | therefore adopt as final result:

1 2m 34556
d. Watch N°. 80.

This watch was taken to Mecca on the 1%* and 34 journeys. It
did not seem advisable to immediately connect these two, which are
separated by an interval of nearly one month. There is the same
objection against forming the combination Me—Ji—Me. Hence we
can only discuss two journeys Ji—Me—ZJi each by itself, but then
we meet with the difficulty that with linear interpolation the results are
not free from the influence of a progressive variation in the daily

559

rate of the watch. If e.g. a daily acceleration of 03.10 takes place,
then a linear interpolation in the middle between two time-determinations
with an interval of 12 days will yield a result that is 18.8 in error
and from a journey Ji-—Me—Ji the difference of longitude will be
found so much too great.

Now it appears, however, that the change of rate of N°. 80 was
more complicated. When it was transported after a period of rest,
it showed a considerable acceleration and then it continued for some
time to show this accelerated rate unaltered. In such a case the error
committed by linear interpolation will be much smaller, but it will
not be easy to account for. Finally I have deduced results by
means of quadratic formulae as well as by linear interpolation.

We thus found:

1st Journey.
a. By interpolation between the last preceding and the next
following observations at Jidda

Febr. 14 -- 2™ 35875

15 35.83

16 39.48

Mean + 2™ 35869
b. By linear formulae + 2™ 37585 (+ 41863)
Cs By quadratic formulae —-+ 2™ 35505 (+ 0872)

As the linear formulae represent the observations very unsatisfactorily,
the result thus obtained was rejected and we adopted as the result
yielded by the 1s* journey the mean of the results a and c

4 2m 358,37.

37¢ Journey.
a. By interpolation between the nearest ubservations at Jidda

March 11 + 2™ 34551

12 34.51
14 35.49
15 35.80
16 35.44
ty 35.33
Mean + 2™ 35518
b. By linear formulae + 2™ 3569 (= 0559)

c. By quadrati¢ formulae -++ 2™ 33592 (+ 0°49)

560

For the solutions 4 and ¢ only March 7 and 8 were used as first
Jidda-group, as the next preceding observations are 4 days earlier.
I adopted the mean of the 3 results a, 6 and ¢
+ 2™ 34593
As the final result yielded by N°. 80 I adopt the mean of the
results from the two journeys
+ 2™ 35:15

e. Watch N°. 81.
This watch was taken on the first journey to Mecca. About that
time it seems to have gone fairly regularly,
The following results were found for the difference of longitude.
First we obtain by means of comparison of the results obtained
at Mecca with those interpolated between the last preceding and the
next following observations at Jidda:
Febr. 14 + 2™ 36s74
15 36.17
16 33.99

Mean + 2™ 35563

Further 4 general solutions have been executed, I and UI by -
quadratic, II and IV by linear formulae. Only for HI and IV the
deviating result of Febr. 21 at Jidda was excluded.

I + 2m 35584 (+ 0588)
ll 35.39 (+ 0.85)
Ill 35.78 (+ 0.83)
IV 35.22 (+ 0.83)

It appears here, as before, that the exclusion of a deviating time-
determination between others has but little influence. As results from
the quadratic and from the linear formulae I adopt the mean of I
and IlI and that of II and IV

+ 2™ 35580
and + 2 35.30
and as final result the mean of the results obtained by the three
methods, direct interpolation, lear and quadratic formulae

+ 2™ 85558

f. Waich N°. $4.

This was taken on the 3'¢ journey. According to the investigation
of the results at Jidda its rate was very regular; it showed no progressive
variation and only small accidental deviations. During the stay at

561

Mecea, however, it had a daily rate, in the mean + 0%.78, which
differed much from that at Jidda and was moreover very irregular,
while during the journeys themselves the rate seems to have had
about the same value as at Jidda.

The following results were derived from this watch:

1st by interpolation between the nearest determinatons of time
at Jidda.

March 11 + 2™ 32510

Dpalegh 32.38
i ee 34.52
Nema 25, 35.30
x 46 33.77
as 33.98
Mean + 2m 33°68

2nd by means of quadratic formulae. Using also the observations
of March 2 and 3, which are further away from the time of the
journey, or leaving them out, we obtained

4+ 2m 34°72 (+ 1:03)
or 32.83 (+ 1.08)

3 We obtained in the same two manners by means of linear
formulae :
+ 2™ 33°08 (E1827)
or 30.64 (+ 1.02)
Of the results by the quadratic formulae the mean of the two
has been adopted; of those by the linear formulae it seemed best
to adopt the second.
Giving finally equal weight to the results of the 3 methods, the
final result becomes ;
+ 2™ 33°70

differing rather much from those yielded by the other watches.
g. General result from the 6 watches.

For the derivation of the difference of longitude according to each
of the employed watches, given in the preceding paragraphs, different
methods of calculation were followed, which had all of them special
advantages and disadvantages, and in most cases the mean of the
results found by these different methods was adopted. Naturally in
this procedure some arbitrariness could not be avoided ; its influence
on our final results, however, will not be great.

Proceedings Royal Acad. Amsterdam. Vol. XV.

Now there remains to be decided what weight must be given to
each of the 6 results. Although it seemed at first that for each watch
we should have to adopt a different accuracy peculiar to it, it
appeared after all very difficult to determine this intrinsie accuracy.
So e.g. for N°. 84 we should have had to adopta rather high weight
according to the observations at Jidda and yet it went very irregu-
larly during the journey to Mecca. So ultimately I adopted the same
intrinsic accuracy for each of the watches; nor could greater weight
be given to the chronometer of Dent, as a travelling instrument,
than to Leroy’s watches.

Hence I have given weights to the 6 results proportional to the
number of journeys in which each watch had been used, and besides
only a weight of 0.5 to watch 77 owing to the discontinuity during
the stay at Mecca.

So I obtained :

DIFFERENCE OF LONGITUDE JIDDA—MECCA.

Dent 2527 + 2™34°62 Weight 3

W AtcH si 34.64 os 2
i. 77 34.56 » 0.5

- 80 35.15 emt.

3 81 35.58 4 ae

84 33.70 ca et

3
From the agreement of these six values iter se there follows as
mean error for weight unity + O*.66 and the final result from the
6 watches is found to be
Difference of longitude + 2" 34°74 + 022.

It is clear from the foregoing that a derivation of the difference
of longitude from partial results for each journey must lead to a
less advantageous combination of the observations. Yet I want to
show that a final result obtained in this way does not differ much
from the above given.

We then obtain, indicating the journeys Ji——Me.—Ji. and Me.—
Jii—Me. respectively by M. and J.

MI M Il M Ill 4 J
Dent 3640 35:30 33528 35589 33957
i 34.82 36.20 33.58
77 34.56(4)
80. 35.87 34.93
81 35.58
84 33.70

Mean 35578 34°96 3455 35°89 33898:

563

Combining these 5 results with equal weights we should find
+ 2™ 345.95

which agrees with the final result adopted by us just within the
limit of its mean error.

7. Reduction of the results to known points in the two cities.

Longitude of Mecca from the meridian of Greenwich.

The situation of the observation-station at Jidda, (the Dutch consulate)
relative to the Mecca--gate has been measured four times by
Mr. Sauim by means of the determination of the direction and the
length of the 4 parts of the road, the first by the boussole, the last
by counting the steps, the length of which was found to be equal
to 0".768. To the directions counted from magnetic North to East
first of all must be added, to reduce them into astronomical azimuths,
the magnetic declination for which, according to the English admiralty
chart, — 2°.4 was adopted. The thus corrected results, however,
appear to be still in need of a correction of + 1°.6’) according to the
results obtained with the same instrument about the road from Jidda
to Mecea, of which we shall treat hereafter. So the total correction
of the lectures of the boussole was — 0°.8.

- From the directions and distances the rectangular co-ordinates have
been derived taking as axes the parallel and the meridian. The mean
results of the 4 measurements expressed in meters were as follows
(see Plate II, tig. I, the scale of which has been given in hectometers) :

Ax Ay
h—a — 94m + 350™
c—b — 313 a ea
d—-c 0 = 2-44
e—d eae Fi5S = 9
Sum — 465" + 401™

The sums of the two first Av and Ay give as co-ordinates of the
Medina-gate relative to the Mecca-gate — 407" and + 442™, for
which is found — 368™ and + 349” according to the English ad-
miralty-chart /idda with its approaches. 1 adopted the mean of the
two results and thus found as co-ordinates of the Dutch consulate
relative to the Mecca-gate :

1) The accurate result is +27.0, but this difference is here immaterial.

ai*

564

A «2 = — 446™ Ay=-+ 355™')
or expressed 1A seconds of longitude and latitude :
AV=Tes Wiest Ag ==11" o>" North:

For the determination of the relative situation of the observation-
station Mecca and the Kabah we have a report of Mr. Satm that
the latter is at 187 steps $.S.W. of the former. After this indication
it has been tried to identify the observation-spot in the plan of
Mecca by BurckHarpT, as revised by SNnouck HtureronJe, of which the
scale las been given in steps. As the most likely place we have
found the spot indicated on Plate Hl, Fig. 2, as point III, which is
situated at a distance of 192 steps from the Kabah, indicated as
point I, in a direction 18° East of the North.

The rectangular co-ordinates of the observation-station reiative
to the Kabah thus are:

A x= -++ 35™ Ay=+ 144m
or AA =1".2 Kast A p.= 4".7 North

As regards the mean errors of the values for Az and Aq, I
believe that they are not undervalued if we adopt + 2".5 for both
co-ordinates for Jidda and + 1".5 for Mecca.

So we obtain :

Latitude Jidda Mecca-gate 21° 29'5'5 + 2'7

Latitude Mecca Ka’ bah 21°25) (BAe a

Difference of longitude 38' 244 + 44 — 2™ 33°63 + 0:29

The thus obtained latitude may be compared with the result found
in 1876 by Comm. Wuarton, on which the Adm. chart is based.

The point determined by him is situated on Geziret el Mifsaka
and the latitude he found was + 21°28'0". Further we find by meas-
urement on the chart that the latitude of the Mecca-gate is 2197™ =
= 1'11".4 greater. Hence it becomes 21°29'11".4 i. e. 6" greater than
the value found by us, an agreement which, if we take into account
the reductions that had to be added to both results before their
comparison, may be considered satisfactory.

In the second place Wuarton’s result for the longitude of Jidda
may be employed to determine the longitude of Mecca from the
meridian of Greenwich. He found as longitude of his observation-
spot 39°11'25"; according to the chart the Mececa-gate is situated

!) These vesulls may be compared witii the co ordinates of the English consulate,
Which is next to the Dutch, measured on the adwiralty-chart, as accurately as was
possible: : Ax = — 542m pny =-+ 344m,

Our plate II, fig. 1 is based solely on Mr. Sautmw’s measurements.

565
2010m = 1'9"8 further eastward, hence:
Longitude Jidda. Mecea-gate 39°12’34.8 = 2" 36" 50°.32
and consequently :
Longitude Mecca Kabah 39°50/59".2 = 2h 39" 23:.95.

We have still attempted to find out the basis of Wuarron’s long-
itude and whether the telegraphic determinations of the longitude
of Aden and Suez have been employed for it. But although Rear-
admiral C. J. pe Jone, Chief of the Dutch Dept. of Hydrography
has with the greatest kindness put all the available charts and other
data at our disposal, we have not succeeded in obtaining certainty.

Direct data as to the basis of WuHarrton’s longitude were not to
be found. Then we tried to attain our end by consulting the charts
of Aden, Suez and Alexandria and by comparing the longitudes
given there with the results of the telegraphic determinations. These
had been executed principally in connection with the transit of Venus
in 1874, and have been discussed by Airy *), CopELAND *) and Auwers °).
We did not find any certainty in this way either, as in the first
place it is not sure that the bases for the longitude in the different
charts agree inter se, and moreover uncertainty as to the exact
situation of the observation-spots prevented an accurate determina-
tion of the longitude errors of the charts.

Therefore it seemed impossible to find out with any probability
the eorrection needed for the longitude of Jidda adopted in the
Adm. Chart. Consequently I must regard the longitude of Mecca as
deduced above, as the most reliable value for the present.

In order to find the total mean error of the Jongitude of Mecca
from the meridian of Greenwich, we should have to know that of
the adopted longitude of Jidda, and it is impossible even to estimate
this. In the total mean error an unknown value 77,7 has therefore
been included.

Thus our final results for the geographical position of Mecca
Kabah become
Latitude -+ 21°25'18'4 + 2'.1
Longitude 39°50'59".2 + V 4".4)° + mr

or 2°39" 23°95 + (0:.29)+m,* East of Greenw.

ie 2)

1) G. B. Arry: Account of observations of the transit of Venus, 1874, Dee.
London 1881.

2) Dun Echt observatory publications. Vol, I[f. Dun Echt 1885,

5) A. Auwers: Die Venus-Durchgiinge 1874 und 1882. Bd. 6. Berlin 1896.

566

The results obtained by J. Hxss from the itinerary Jidda-Mecca were :")
Latitude = 20° 20 Wiese" 303
Longitude 39°52'5 + 31.2
i. e. agreeing with our result within the given mean errors, which
are still rather considerable. So we may conclude that by our
work, the accuracy attained has been a great deal increased.
Finally we shall compare our results for Jidda and Mecea with
those of Ar Bry. The following are the corrections needed by the latter

Ly ie
Jidda SE 278 Ae sG'B5"
Mecea Bae) ss be 94! 4"

Ai Bey’s errors in latitude are for both places about —3’; the
errors in longitude are great and irregular, which need not surprise
us, as they are the results from observed lunar distances (for the lon-
citude of Jidda also 2 observations of eclipses of Jupiter-satellites
have been taken into account). Att Bry also determined the latitude
of a number of other places in Arabia. Perhaps these also need a
3’ and may then be fairly reliable. I dare not,

correction of about
however, decide this question here.

8. Road from Jidda to Mecca.

In this last paragraph I shall discuss the results obtained by
Mr. Samm in surveying the road between the two places, on a
journey on foot from Mecca to Jidda, undertaken for this special
purpose. This survey was made by means of observations with the
boussole and by counting the steps.

The boussole, of which mention has been made before, was a very
handy little instrument by Casella, belonging to the Leyden observatory.»
It has a little telescope in which also the divisions of the azimuth-
circle (full degrees) are made visible by reflexion.

The following table contains the results of these observations and
their further reduction. The road was divided into 92 parts, for each
of which the direction and the length were determined. For the two
terminal and 13 of the 91 intermediate points special names could
be indicated in the first column. The 2°¢ and 3¢ columns contain
for each of the parts of the road the direction @ read on the boussole
and the length / expressed in steps.

The directions @ are counted from magnetic North to East, South

1) Hess started from the following co-ordinates of Jidda, Mecca-gate : Longitude
39° 11' 47" KE; Latitude + 21°29'11”, while the Adm. Chart Ed. 1905 gives
39° 12° 35"; +21°99' 11”, ie. a longitude of 48” greater.

567

/ ic A - J

<P carat S Pca a corrected corrected

1 Entrance Mecca

i—2 337°| 496; — 166/+ 350|— 130/+ 299
2 Kahwat al-mu‘allim
pees o45 | 606|— 586|+ 132|— 489/-+ 128
S54 991 | 160!— 1148/4 321|— o56|-+ 304
4— 5 240, | 320) — 1359/4 187| — 1138|}-+ 197
5— 6 964 | 230|— 1536] + 161|— 1287|-— 180
6:7 307 | 595 |— 1918/4 425|— 1601|+ 413
Hy 8 306 | 2090 — 3276 + 1327 — 2716/4 1212
g 56 98g 1418 | — 4341 | + 1624 | — 3602 | + 1493
9—10 265 2100 — 5966 + 1413 — 4976|+ 1363
10—11 75 | 484| — 6344/4 1430|— 5292| +4 1388
11 Umm ed-dad |
11—12 275 | 699 — 6888 + 1454 — 5749/4 1425
12-13 991°| 959 | — 7413'| + (921 |— 6206|+ 991
13—14 243 | 310| — 1664/-+ 719) — 6421}+ 880
14—15 o50 | Git. | = 8110) -— 613 |— 6801 | + 753
15—16 236 | 818 — 8623 + 235 — 7244/4 451
16—17 261 | 1284| — 9621/-+- 141|— 38086|-+ 401
17 Maktala |
17-18 267 | 1623 | — 10881| + 22|— 9148}-++ 337
18—19 o35 | 12718 | — 11672| — 583|— 9832}— 148
1920 249 | 2907 — 13754 — 1483 — 11608 — 844
20—21 o4g | 1254 | — 14631 | — 1918 | — 12359 |— 1184
21 Kahwat Salim |
21—22 255 | 1400 | — 15673 | — 2245 | — 13244 | — 1427
2223 289 | 2531 — 17565 | — 1680 — 14819 — 898
23 ‘Alameyn |
2324 908 | 4710 — 20878 — 93 — 17559|+4+ 534

24—25 314 | 1150 — 21549 + 503 — 18105 + 1055

x y xr y
‘ st ae sally sy! corrected corrected
25 Shumési | |
2526 315° | 1427 | — 22368 | + 1256 | — 18772| + 1712
26—27 319 | 1102 | — 22958 ! + 1881 | — 19250 + 2255
27—28 280 | 402 | — 23268 | + 1922 | — 19509 | + 2208
28 29 252 | 350 | — 23524 + 1927 | — 19727 + 2226
29—30 269 806 | — 24151 | + 1790 | — 20256") 4- 2212
30—31 258 | 922 — 24848 + 1611 | — 20847 + 2084
314.30 950 | 687 | — 25343 + 1407 | — 21269 | + 1926
3233 246 614 — 25772 + 1194 | — 21636 + 1760
33—34 255 | 320 | — 26018 | + 1117 | — 21845 | + 1702
34—35 265 970 | — 26768 + 1019 | — 22478 | + 1642
35 small kahwah | |
35—36 250'| 567 | — 27171 | + 851 | — 22897 | + 1513
36-37 272 | 2189 | — 28884] + 839 | — 24263 | + 1552
31 Hadda | |
37—38 268 | 1202 | — 29818 | 4 Je6:-| — 250514 seas
38—39 239 | 443 | — 30107| + 576 | — 25209] + 1367
39—40 950 | 845 | — 30717 | 4 325 | — 25819 | + 114
40—41 244 | T12)| = 31247) 4 30° | = -o6n74d! tae
41—42 234 | 336 | =--31452||-— 124.) = @e45i-)| ee
42 43 250 | 906 — 32106 — 393 | — 27009| + 611
43—44 257 | 1994 | — 33605|.— 806 | — 28281| + 307
44—45 235 | 706 | — 34043 | — 1141 | — 286590] 4+ 39
45— 46 230 | 785 | -- 34495 | — 1554 | — 20052 | — 296
46—47 225 | 1930 | — 35514 | — 2662 — 20041 | — 1197
47— 48 223 | 506 | — 35771 | — 2962 | — 30166 | — 1442
4849 217 | 491 | — 35989 | — 3277 | — 30358 | — 1701
49—50 220 | 2782 | — 37313 | — 4905 | — 31521 | — 3106
50 Bahra
50—51 240 | 271 — 37495 | — 5110 | — 31679 | — 3198
51—52 225 | 318 | — 37663|| — 5293 | — 31825 | — 3347

a |

O69

: a Jy x Jy
— __, corrected corrected

52—53 240° 250 | — 37828 — 5398 31966 — 3430
53 - 54 238 755 | — 38314 — 5731 — 32385 | — 3696
34—55 | 250 1153 | — 39146 — 6073 — 33095 — 3959
55—56 | 261 1205 | — 40067 — 6259 — 33875 — 4088
56—57 280 | 4594 | — 43618 — 5786 — 36847 — 3586
57—58 270 150 | — 43735 — 5791 — 36946 | — 3587
58—59 281 519 — 44135 — 5730 — 37280 | — 3524

59 Kahwat al-‘abd |
59— 60 281 210 — 44297 | — 5705 — 37415 — 3498

60—61 | 253 | 356 — 44559| — 5797 | — 37638 | — 3569
61—62 317 | 1056 | — 45146 | — 5219 | — 38115 | — 3065
62—63 - | 312 | 583 | — 45496| — 4930 | — 38401 | — 2811
63—64 | 207 | 502 | = a5esa.} — 4767 | — se60s | — ones
64—65 | 305 2296 — 47360 — 3801 | — 39985 — 1807
65—66 | 319 | 1392 | — ast06 | — soi2 | — 40590 | — 1193
; 66—67 295 716 — 48664 — 2780 — 41002 — 911
67—68 250 | 1743 — 49921 | — 32908 | — 42074 — 1309
68—69 267 | 780 | — 50527| — 3355 | — 42585 | — 1340
69 ~70 295 | 1733 | — 51715 | — 2836 | — 43619 | — 867
10—71 292 | 610 | — 52223| — 2677 | — 43991 | — 720
71 Kattana
172 306 | 438 | — 52508 — 2488 | — 44226 — 552
12-73 290 | 1575 | — 53679 | — 2117 | — 45199; — 206
73—74 275 .| 317 | — 53026 | — 2106 | — 45407} — 190
4-75 295 | 453 | — 54252 | — 1970 | — 45677] — 66
15—16 296 | 390 — 54530; — 1848 | — 45907, 4+ 45
16—T1 2900 1490 — 55638 | — 1497 — 46828 + 372
Tl—18 310 | 1084 — 56308) — 981 | — 47377| + 826
78 Jarada
78 —19 310 1930 — 57501, — 63 | — 48353 | + 1633

79— 80 280 416, — 57822, — 20 , — 48622 | + 1678

z ‘ SP = ie = 2 2 ae ! a eae
= ne = |
s0—81 265° | 1470 | — 58959 | — 167 = 49582 | + 1589
81—82 256 | 1225 | — 508715 | — 438 | — 50360 + 1388
82—83 280 | 3400 | — 62503 — 88 | — 52560 {| + 1759
83 Raghama

83—84 288 | 1024 | — 67779 | -+ 1385 | — 56952 | + 3152
84—85 2999 5866 — 71869 + 3435 — 60332 | + 4995
85— 86 290 | 1233 — 72785 +- 3725 | — 61094 | + 5266
86—87 289 4440 — 716103 + 4716 Ea 63855 | + 6197
87—88 284 | 460 | — 76455 + 4788 | — 64149. + 6268
88—89 287 366 — 16731 -+ 4860 | — 64378 | + 6337
s9—90 293 780 — 77300 -+ 5074 | — 64850 | + 6533
90—91 281 424 | — 71627 | + 5124 | — 65124 | + 6585
91-92 285 | 583 | — 78071 | + 5223 | — 65495 | + 6681
92—93 283 | 330 — 78324 + 5271 — 65705 | + 6729

93 Jidda, Mecca-gate

|
|
|

and West, from 0° to 360°. They had first to be reduced to astro-
nomical azimuths counted also from North to Kast and for this
purpose the magnetic declination was taken from the Adm. Chart
of Jidda. For 1911 it was assumed to be 2°55’ West — 11 & 3’= 2°.4
West, and this value was considered to hold good for the whole of
the road. As length of the step 0.78 was adopted as given by
Mr. Sati, and the length of the parts of the road expressed in
meters shall be designated by /’. The 4 and 5" columns contain the
93 relative to point 1,
taking as axes the parallel and the meridian, so that we have

co-ordinates « and y¥ in meters of points 2

es 2 Meine) 9 = = hose
in which for point n the summation has to be extended over all the
parts between point 1 and n.

The two values in the last line of the 4 and 5 columns of
the table are the co-ordinates of the Mecea-gate at Jidda relative to the
Entrance of Mecca. These may be compared with the corresponding
differences deduced from the astronomical determinations. For. this

N. SCHELTEMA. “Determination of the geographical latitude and
longitude of Mecca and Jidda executed in 1910-—11”. Plate II.

Observation-station at Jidda.
a Mecca-gate,
c Medina-gate.
abe Part of the rampart.
e Observation-station, Dutch Consulate.
Scale in hectom.

Observation-station at Mecca.

I Kabah.
II Entrance to the town on the Jidda side.
Ill Observation-station.

Scale in hectom.

Proceedings Royal Acad. Amsterdam. Vol. XV.

O71

purpose the situation of the point designated as “Entrance Mecca”
had first to be determined. We adopted as such point II in the plan
of Mecca, plate II fig. 2, and according to this its co-ordinates relative
to the Kabah are

Az = 638m. = 22'02 West

Ay = 253 m. = 8".2 North

Using these values we obtain as relative co-ordinates of points 93

aid 1 according to the astronomical determinations
X = — 38’ 2".2 = — 65705 m
Y= —. *3'3809 = + 6729 m
while the results from the observations on the journey were
e=— 78324m y=-+ 5271 m.

As the errors in the astronomical results may be regarded as
small compared with the accumulated errors of the observations on the
journey, we may conclude that the latter results need corrections
Az = + 12619m Ay=-+ 1458 m. We may regard these corrections
as owing to an error in the accepted value for the length of a step
and to a constant error in the deduced azimuths.

We then obtain, designating the true length of a step in meters
by 0.78 (1 —p) and the constant error of the azimuths by d, the
two equations

Az = — (p cos bd + 1 — cos d) « + (A—p) y sin d = + 12619
Ay = — (p cos d + 1 — cos db) y — A—p) e«smd=-+ 1458
The solution of the two equations vields
p cos J = eh — a 0.15913
(1—p) sin d = b-= + 0.02932

So the true length of a step and the constant error of the azimuths

are found to be

(1—p) 07.78 = 0".6563 é= + 2°0’
while the values found for @ and 4 may be used to correct the
co-ordinates of cur 92 points. These corrected co-ordinates are found
in the two last columns of our table.

At the same time they have also been drawn, and with them the
Jidda, in our plate III. No seale has been

whole of the road Mecca
appended, but in the map itself lines have been drawn at distances
of 2’ in longitude and latitude of each other. These have been drawn
perpendicular to each other, and as length of a second of latitude
and longitude in meters we have accepted after Brssen’s dimensions
of the earth 30™.753 and 28.789, the latter value holding rigorously
for g¢ = 21°27’. As the absolute longitude from the meridian of

572

Greenwich may still need a correction, we have reckoned the longitude
and also the latitude on the map from Jidda, Mecca-gate.

At the conclusion of this paper, which has proved that much
advice and help has come to me from many sides, the only thing
left for me to do, is to express my sincere gratefulness to all those from
whom I have received this help.

Postcript.
(November 1912).

In order to investigate the accuracy of our time-determinations
we had compared the results from the eastern and the western star,
but in doing this no attention lad been paid to the fact, that in most
cases the times of observation of the two stars lie too far apart to
neglect the rate of the chronometer in the interval.

Theretore this comparison has been made anew after correcting
the differences E—W;; the results, however, have not been materially
changed. We now obtained

Jidda 23 nights E—W = + 05.12

Meccai3 _., + 0.25
Together E—W = + 05.16 + 03.10
against before + 03.11 + 0°10. The constant error in the zenith-

distances would be found now 4z2—=-+ 1".2 against before + 0.8,
but just as before it is small.

As mean error of the difference from one night we now found
+ 08.58 and therefore as mean error of a time-determination from
two stars + 08.29 against before + 0°.32. The accordance of the two
stars was somewhat improved.

Chemistry. — “On a new modification of sulphur’. By Dr.
A. H. W. Aten. (Communicated by Prof. HoLiemay).

Communicated in the Meeting of September 28, 1912.

This investigation originated in an observation by Aronst#In and
MEInUIZEN *), who noticed that when a solution of sulphur in sulphur
chloride (S,Cl,), supersaturated at the temperature of the room, is
heated to 170°, no sulphur erystallises on cooling. I have afterwards
repeated this experiment and demonstrated that the solution of S$ in
S.Cl,, which has been heated to 170° not only fails to deposit sulphur
at the temperature of the room, but is even capable of dissolving a

1) Verhandelingen Kon. Akad. Wet. Amsterdam, 1898. 1,

~ Pe
ie

“

considerable quantity of sulphur, about as much as the solution
saturated at 20° originally contained‘). It also appeared that the
conversion, which has taken place here retrogrades very slowly, for
after 20 days the quantity of dissolved sulphur had decreased but
very little.

The sulphur which was added originally as rhombic sulphur and
consequently was present in the liquid as 5, apparently undergoes
some conversion or other on heating, for after the heating some
5; has disappeared. The question now arises: what has become of
this S,° Does it pass into another modification of sulphur or is
there a compound formed of 5 with 5,Cl,’ At one time I thought
I ought to arrive at the latter conclusion, because in other solvents
metaxylene for instance, the same phenomenon could not be observed.
Krvuyt*) on the other hand is of opinion that the cause of the dis-
appearance of S) is situated. in a transformation into amorphous
sulphur S,. From what follows it will appear that neither of these
views is correct.

1 have again resumed the investigation of the above phenomenon
in consequence of a publication by Rotrsanz*), in which are com-
municated the results of the determinations of the viscosity of sul-
phur at different temperatures with and without addition of iodine.

With molten sulphur without iodine, the course of the viscosity,
as function of the temperature to which the sulphur has been heated,
may be readily explained, because a transformation S$, 225, takes
place which proceeds comparatively slowly, so that with more rapid
changes in temperature there exists no equilibrium between the two
kinds of molecules. On rapid cooling, for instance the condition is
such as corresponds with an equilibrium at a higher temperature. If,
however, we endeavour to apply the same explanation to molten
sulphur to which a trace of iodine has been added, we meet with
difficulties as will be shown in a more elaborate article to appear
shortly. The course of the viscosity cannot be explained here by
the assumption that in the molten sulphur the above transformation
5,225, takes place. Presumably, a third modification of sulphur
occurs here, as an iodine-sulphur compound does not exist, at least
not in the solid condition. The same may now happen with mixtures
of sulphur and sulphur chloride.

The investigation was, therefore, directed in the first place to
decide what becomes of the 5; when this is heated with S,Cl, to a

1) Z. fir physikalische Chemie. 54. (1905). 38.

*) Z. fiir physikalische Chemie. 64. (1908). 545.
3) Z. fiir physikalische Chemie. 62. (1908). 609.

574

suitable temperature. As has already been observed it is possible
that either a compound of S with 5,Cl, is formed or else another
sulphur modification. That, in this latter case, there can be no
question of the formation of 5, is shown readily from the following
experiments.

On heating S with S,Cl, we can obtain very concentrated sulphur
solutions. If this were caused by the formation of S,, this ought to
have a great solubility, or the separation of 5, ought to take place
very slowly when, by heating, a concentrated solution of 5, has
been obtained. Neither of these phenomena occur, however. If sulphur
which, owing to heating and rapid cooling, contains a certain quantity
of S, is brought into contact with S,Cl, a turbid liquid is formed
immediately. This turbidity of 5, is permanent at the ordinary tem-
perature, but on warming for a few minutes at 100°—110° it disappears.
On cooling, however, the turbidity at once reappears. Hence, it is
shown that the solution and subsequent separation of Sz is a process
which takes place withou tappreciable retardation. At the temperature
of the room, the solubility of S, is very trifling, for the experiment
just described may be carried out with a very little S,. Ata higher
temperature the solubility is apparently fairly large. At 100°—110°
an appreciable, rapid transformation of 5, takes place, presumably
into S,, for if the above experiment is repeated a few times, the
turbidity of 5,, finally, does not reappear.

Not only in pure $,Cl, but also in $,Cl, containing S$; the solubility
of S, is but small, although the solubility of 5, in $,Cl, is increased
by addition of S;. For, on adding to 5,Cl, which is turbid by 5, a
large quantity of 5;, the turbidity disappears, but only when very
little S» has been added. The possibility of the formation of S, in
considerable quantities in solution is therefore excluded.

In order to ascertain what is formed from the 5; originally present,
the proper way would be to determine the melting point line of the
system S-+5,Cl, after heating. It appeared, however, that nothing
else but rhombic sulphur or S,Cl, was separated. The newly formed
product does not separate at all. As, moreover, no suitable chemical
method could be found to separate the new product from the other,
systematic determinations were carried out of the solubility of sulphur
in mixtures that had been heated to a suitable temperature. From
this it can also be shown whether a new modification or a compound
has formed.

The system S-+5,Cl, must be treated as a ternary system, as
besides 5, and $,Cl, a third kind of molecule is present. The com-
position of a mixture that has been heated for a certain time must,

€

ae
fo

therefore be represented in a triangle the apexes of which indicate :
S;,, 5,Cl,, and the compound, or the new modification.
Let us take first the case of a
MOR BEE compound, for instance, $,Cl,; the
composition may then be expressed
by a point of the triangle PQR
in Fig. 1. As unity of the com-
pound has been taken '/, 8,Cl, ;
this has the advantage that we
can now deduce the — gross
composition, i. e, the relation
5:5,Cl, in a simple manner from
a a! = 5 the real composition (5 +S,Cl, : */,
Je Ole 5,Cl,), namely by projection on
the side PR.
If 0 is the real composition, a mixture of this composition O
contains PT SRUS,Cl, and UT'/, S,C,. The gross composition
is now :

total S 2x EY i ae z{9.
ie a Ck-— RU UT. RO:

Hence, 0’ gives the gross composition. This is also the composition
which one may determine experimentaliy by an estimation of the
total sulphur. Not, however, the true composition (, for there is no
means of determining the quantity of $,Cl,.

The question now arises: If we heat the mixture of varying
sulphur content to a given temperature and then cool to a definite
temperature, how then does the composition of the solution saturated
after warming, vary with the original composition? This is readily
indicated with the aid of fig. 2.

Let the line PBHR represent the equilibrium S + 5,Cl, 22 5,Cl,
at a temperature 7’,.

Let 7DFU represent the solubility line of S; in mixtures of S,Cl,
and S,Cl, at the temperature f,. The point 7’ then represents the
soubility of 5, in §,Cl,.

When now a mixture of S and $,Cl, of the gross composition A
is heated long enough at 7’, the equilibrium S + 8, Cl, 25, Cl,, which
belongs to the temperature 7, sets in. The inner composition is,
therefore, given by a point of the curve PBHR, which is found by
drawing a line 1 PF in the gross composition of A. The intersecting
point of this perpendicular line with PSHR gives the looked for
real composition. If one now cools rapidly to /, the composition

O76

will not alter if the equilibrium at 7’, remains the same. This liquid

now must separate sulphur at ¢,; the saturated solution must lie on

* S,Cly

oa, o

Fig. 2a.

the line 7 DFU. Its composition is found by drawing from FR a
straight line through B until this intersects the solubility line 7DPU.
In this manner we find for the real composition of the saturated
solution 2), the corresponding gross composition is D,.

100

Composition of the
saturated solution
after heating

Composition of the original
mixture.

Fig. 2b

577

We can carry out this construction for different gross compositions
and then put down the composition of the solutions saturated at 4,
after heating at 7’, as function of the original composition. We then
find the line PA in Fig. 20.

When we determine the solubility line at a higher temperature &, the
line QC is found. If we heat at a higher temperature 7’, and again
determine the solubility at ¢, and ¢,, the lines PB and QD are found.

We see that these lines, at 100 at. °/,S of the original compo-
sition, approach to a certain limitation value which is different for
different temperatures of heating and of solubility. This limitation
value can give a larger as well as a smaller sulphur content than
corresponds with the composition of the compound.

The first is the case when the compound is but little dissociated
and the solubility of the sulphur is great, the latter when the disso-
ciation is great and the solubility small.

Quite different becomes the course of these solubility lines when
a new modification of sulphur is formed. In this case, the compo-
sition of a ternary system is given by a point in a triangle the
apices of which indicate 5, Cl,,5, and the new sulphur modification. .
We then obtain the gross composition (for instance D, in Fig. 3a

Fig. 3a.

by drawing a line // QR through D which indicates the real com-
position. The line indicating the inner equiliorium between S; and
38
Proceedings Royal Acad. Amsterdam. Vol. XY.

“rn
Oe

the new modification of sulphur will now have the course of PBhG Y
in Fig. 87 for a temperature 7’. The solubility line of 5; in mixtures
of S,Cl, and the new modification will be TDF V at the tempe-
rature ¢,.

We can now deduce in exactly the same manner as in Fig. 2¢

100 A R
5)
ox
SS-18
qe
ORS
—
CS
= 3
es
a.
Es
Oo -=
60; P =
77)

P Composition of the original mixture.
20 40 — 60 60 100
Fig. 850

what is the gross composition of a given mixture, which after heating
to 7, is saturated with S, at ¢4,. If we do this with different com-
positions we find that the composition of the saturated solution asa
function of the original composition is given by the line PAF in
Fig. 8°. If we repeat the same construction for mixtures which are
heated to 7’, and for solubilities at ft, and ¢, we find the lines PBR,
QCR and QDR. These lines all converge in one point. At J00 at.
°/, S of the original composition, the composition cf the saturated
solution is also 100 at. °/, S the temperature to which the mixture
was heated or independently of temperature at which the solubility
has been determined.

Hence, there exists a characteristic difference between the course
of the solubility line with a compound and a new modification.
Therefore, it was expected that in this manner we migbt decide
with which of the two cases we are dealing here.

Before proceeding to the actual solubility determinations it was
ascertained at what temperature the transformation of 5, becomes

319

perceptible and how long the heating must be continued before the equi-
librium js attained. It now appeared that a very perceptible conversion
already occurs at 100°. Whereas, at 0° the solubility of S; in S,Cl, with-
out previous heating amounts to 36.1 at.°/, of S, this, after heating to
J00°, becomes 55.7 at. °/, of S for a 50 at.°/, mixture. The heating,
therefore, causes a considerable increase in solubility. It also appeared
that at 100° 1’/, hour was required for the equilibrium to set in.
This reaction, therefore, proceeds at LOO? comparatively slowly and
it may be expected that by 1apid cooling the equilibrium can be
fixed at 100°. Above 100° it is different. Because, as a rule, the
velocity of a reaction for every 10° of rise in temperature becomes
2—3 times greater, the setting in of the equilibrium will, at 140°,
require about 5 minutes and at 170° less than one minute. Here
we shall not be able to cool so rapidly that the equilibrium becomes
fixed and hence we shall find, after heating to 170°, somewhat
fluctuating values for the solubility. This explains why the deter-
minations previously carried out at 170° agreed badly. At a lower

TAREE OE

Original | Composition of the saturated ‘solution at
Pepe aes (=n (4 cates
0 Roe ae. 11.6
10.0 Bae ah 40.1 18.1
28.7 | 62.0 | 47.4 31.9
49.6 | = er, a
49.9 | 66.6 | 56.0 42.9
60.1 69.4 | 59.9 41.7
69.1 72.8 | = =
79.4 — | 2.0 65.2
80.1 al | 11.6 66.1
89.9 82.1 = =
90.1 — 80.5 =
94.6 | 87.7 ae ae
97.4 ig. 9t-0 = es
98.0 93.5 | — =

38*

580

temperature than 100°, the completion of the equilibrium takes a
longer time and it can be fixed with still greater certainty.

The method of investigation is very simple. A mixture of sulphur
and sulphur chloride is heated for a sufficient time at the desired
temperature. The liquid is then cooled rapidly, sulphur is added if
the solution is not already saturated and the whole shaken at the
temperature at which we want to know the solubility. When the
solution is saturated a sample of the liquid is taken and its com-
position determined. This determination is carried out by oxidation
with aqua regia and bromine, evaporation of the volatile acids and
titration of the residual sulphuric acid.

In the first place, mixtures of varying composition were heated
to 100° and the solubility determined at 25°, 0° and — 60°.

The results are united in table I. (see p. 579).

<0
Soe
= O24
O in
100 DAD
FD) =
—_—
wv SS yo !
WO NSsHS
= Oe =
Ss ES B
ey a eS) 0
co fou a 5
GO aes SS 2
nawBee E
ae | :
a.
70 Eas
Oo §

Atom °/, S Composition of the

1+ x original mixture.
0 TO T2008 OV RZOVT SOR COP TO 80 90 f00
Fig. 4,

If we represent graphically the relation between solubility and
original composition we obtain the lines shown in Fig. 4.

A comparison of these lines with those of Figs. 2 and 3% shows
that they correspond with the lines of Fig. 3% which are drawn in
case a new modification is present. The solubility line for 25°, in
particular, proceeds very distinctly towards 100 at °/, of S.

In the second place, mixtures of varying composition were heated

581

2 5.b.E IE
—_—— : - ae
Original | Composition of the solutions saturated at 25° in at./5S,
composition after heating to
in at.%JyS | 50° 75° 100° | 125°
0 a 53.5 53.5 53.5
10.0 Sy ey 57.9 57.6 57.9
28.1 — — 62.0 —
30.9 60.7 61.5 — 63.2
50.3 63.2 64.4 _ 67.6
60.1 65.0 66.7 — yA:
69.1 66.6 70.9 72.8 74.1
81.4 70.6 — — ~
83.7 — 75.0 -- 80.1
89.9 _ — 82.1 —
94.6 — -- 87.7 -
94.9 -- — — 91.5
96.8 _ — — 93.6
97.4 -- — 91.0 —
98.0 _ a 93.5 =
98.1 _ — — 95.6
100 saPEs
=i. © Pa
= aS 1G ~ 4]
oe :
o
0 re S
Le
ea
== B
pl =
32 75K
9) f
-o
Ons
<a
Mer an 6
aoe :
3 ~ ae
60

fe. OR“ °/, S Composition of the original mixture

@t0 20 30 40 530 60 7@ 8 30 10
Fig. 5,

582

to 125°, 100°, 75° and 50° and the solubility determined at 25°.
The values found are given in table II.

From the line of 125° we see, still more distinctly than from
that at 100°, that this proceeds towards 100 at. °/, 5 in accordance
with the line deduced in case a new modification is formed.

No experiments could be carried out with quantities of sulphur
larger than indicated in the table. Not at 50° and 75° because the
liquid at these temperatures was not homogeneous. Not at 100° and
425° because the liquids rich in sulphur are very viseous and, there-
fore, cannot be separated from the crystals by centrifugal action.

The line drawn for 25° has not been determined experimentally,
but has been found by extrapolation of the values at 50°, 75°
and 125°. We notice from this line that even at 25° a considerable
amount of the new sulphur form must be present. A comparison of
the lines for 25°, 50°, 75°, 100° and 125° shows that the quantity
of the new modification increases at a higher temperature and that
this increase for each 25° difference, is greatest below 100°; from
100° to 125 the solubility increases but little. For this reason, when
the liquids are heated at 175°, we find but a small increase in
solubility, as shown by the two points drawn in Fig. 5. We must,
however, bear in mind that at 175°, the equilibrium will not be
tixed. If such were the case a somewhat greater solubility would
have been found.

The existence of a new modification of sulphur, has not, however,
been proved with absolute certainty by the course of the lines in
Fig. 5. It might yet be possible that a compound was formed very
rich in sulphur, such as §,,. 5S, Cl, which contains 94 at °/, of
sulphur. In such case the existence of these liquids rich in sulphur
would be explained. The line in Fig. 5 then ought not to proceed
in the extrapolated part towards 100 at. °/, of S, but turn to the
right and attain say at 96 or 98 at. °/, of S their limitation value.

That, however, a new modification is actually formed is shown
in the following manner.

When in mixtures of sulphur and sulphur chloride a new modi-
fication is formed on heating, this must also be the case with pure
sulphur although perhaps in smaller quantities than in mixtures with
S,Cl,. Moreover it may be — and there is reason to suppose so —
that the conversion of the new modification into 5;, or reversely,
proceeds more rapidly when no or little S,Cl, is present. This might
be the reason why the formation of that new modification in pure
sulphur could not be demonstrated.

583

We have succeeded however, in demonstrating that the new modi-
fication is formed in pure sulphur also. When sulphur is heated to
125°, rapidly pourec out and powdered and then placed into $,Cl,
the solubility is larger than that of rhombic sulphur alone.

In this way was found :

1. Sulphur after heating to 125 and rapid cooling mixed with
el to 69.2 at. °/, of S., Solubility = 56.0 at..°/, -of S.

2. Id. Mixed with §$,Cl, to 73 at. °/, of S. Solubility = 56.5 at. of S.

&. Id. Mixed with S,Cl, to 80.9 at. °/, of S. Solubility 58.5 at. °/,
of 5S.

The solubility at 25° for sulphur, which has not been heated, is
only 53.5 at. °/, of S. The heated sulphur has, therefore a consi-
derably larger solubility than the non-heated rhombic sulphur, which
proves that in the heated sulpbur another modification is also present.
It has already been explained above that this cannot be amorphous
sulphur. But it is also shown by the fact that the sulphur content
of the saturated solutions is all the greater when more sulphur is
added. Now, the solutions 1—3 indicated above are all saturated
with amorphous suiphur for this was present in large excess. If now
the increase in solubility were caused by the amorphous sulphur
getting dissolved, the solubility from 1—38 ought to be the same. To
make more sure, the solubility of a mixture of rhombic and amorphous
sulphur at 25° was determined also. For this was found 54.5 at. °/,
of S. Even after 24 hours the solution was still somewhat turbid
owing to amorphous S. The figure 54.5 at. °/, of 5 is therefore too
high. Hence, it appears again that the solubility of amorphous sulphur
is very slight and cannot explain the increase of solubility in expe-
riments 1—».

In connection ‘vith his theory of allotropy, Prof. Swrrs has pointed
out, that the system sulphur must be a ternary system. The possible
relation between the sulphur medification we were dealing with,
and that assumed by Prof. Smits, will be discussed in a following
paper, as well as the results of investigations on the molecular weight
and the permanency of the modification, which are row being
carried out.

Amsterdam, Chem. Lab. University. August 1912,

584

Chemistry. — “On the relation between the sulphur modifications.”
By Dr. H. L. pr Leeuw. (Communicated by Prof. A. F. HoLieman).

(Communicated in the meeting of September 28, 1912).

Prof. Smits has authorised me to criticise a recently published
report of a lecture by Kruytr delivered before the Deutsche Bunsen
Gesellschaft (Z. f. Elektr. Chem. 1912, 10, 581) and to make use for
this of the experimental data obtained during a research conducted
by me as private assistent. Before proceeding to this it seems to
me desirable to mention very briefly some points in historical order.

SmitH and his coadjutors were the first to assume dynamic isomery
with sulphur. They determined the course of the equilibrium line
S,—S, and also the solidification line of the monoclinic sulphur.
Krvyt, in addition, determined the initial melting points of rhombic
sulphur which, at different temperatures, had got into equilibrium
with S,, the melting point line of Smita being used as the method
of analysis. Moreover, he concluded to the existence of a metastable
region of demiscibility contrary to Sir and his co-workers who
rejected this. ;

By Prof. Smrrs it was pointed out already in 1910 that the results of the
sulphur investigation contain data which support his theory of allo-
tropy. Krvyt, for instance, had stated that when starting with rhombic
sulphur, which has placed itself in equilibrium at 90° and then
determining the melting point of the sulphur in this condition, according
to Socn’s method, 110°.9 was found whereas, in the same method
of working, a melting point of 111°.4 was observed when the S had
come into equilibrium at 65°. From this result it, of course, follows
that we are dealing here with an inner equilibrium in the solid
state, therefore with mixed crystals, and that the line for the
inner equilibrium in the solid condition proceeds on increasing the
temperature, to a greater S, content, as in the liquid. Prof. Smits
therefore changed the 7’, x-figure (fig. 1) into that indicated in fig. 2.

Afterwards, A. Smita and Carson (Z. f. phys. Chem. 1911, 77,
661) have determined the solidification line of Sp, also making use
of the lines determined previously. This line differs a little with
the curve of Kruyr. Moreover, they also found a third melting point
line, that of the ‘“soufre nacré”’. In the same time Krvuyr (Chem.
Weekblad 1911, 647) announced that all the values of the transition
temperature (7’—>), with varying quantities of S, are situated lower
than Reicuer’s value (95°.6) and also that the dimensions of the
mixed crystal-region are not such that the influence thereof on his
calculations exceeds the experimental errors.

585

In the meanwhile it had been pointed out by Prof. Smrrs that the
theory of the allotropy leads us to expect that the previous history

Fig. 1.

might exert an influence on the situation of the transition point.
Specially conducted experiments confirmed this surmise completely
(A. Smits and H. L. pr Leruw, On the system sulphur, Proc. 1914).
The 7’— was determined according to Rericner’s method with this
modification that the upper end of the dilatometer was not sealed.
The transition temperature was consequently determined at 1 atm.
pressure, whereas with Rercnpr the pressure amounted to 4 atm.
The influence which the pressure exerts on the transition temperature
is calculated by RetcuEer to be equal to */,,° rise per atm. pressure
increase. This tallies, as instead of 95°.6 observed by Reicner, I
found 95°.45.

Now in order to find 7’— when S, was present the sulphur was
heated to boiling in the dilatometer and then rapidly cooled so that
a great-part of the S, formed remained intact. Then the dilatometer
liquid (a mixture of 9 vol. of turpentine and 1 vol. of CS, which
had been boiled for a long time with sulphur’ and showed no longer
an evolution of gas) was added and the transition point determined
by ascertaining at which temperature one was above and when one
was below T’—. In the first case the level of the liquid rises at
a constant temperature (conversion Sp,— Siz), in the second case
it falls (conversion Sj — Sz;).

Here it was shown that already at a much lower temperature than

586

95°.45 could be observed a conversion of rhombic into monoclinic
sulphur, which could be made reversible by lowering the temperature;
hence there must be a transition point. A conversion of S, into erystal-
line S could not account for that reversible behaviour as then either
Sy or Spr, was formed owing to which the volume ought to always.
decrease and no temperature should be found at which the volume
increased. As stated in the communication from Prof. Smits and
myself, the S, present in the mixed crystals will be converted con-
tinuously into S, from which it follows that when an increase in
volume is noticed, the conversion Sp,— Ss, predominates‘). So
as to make sure that the phenomena observed were not due to the
not yet complete equalization (after about 10 minutes) of the each time
differently chosen temperature of the thermostat, a second dilatometer
containing SS which had been in equilibrium for weeks and gave
a 7’ of 95°.45 was placed in these experiments, by way of a
check, next to the dilatometer, which contained sulphur with much
». Below follows with full details the result of one of the experiments.
In the first column is given the temperature of the thermostat. The
second column gives the time elapsed after placing the dilatometer in
the thermostat. In the third column is found, first the change in the
dilatometer with the S, and below that in the control dilatometer.

From this we see that 2'/, hours after the heating the control
dilatometer at 71° did not further rise in 15 minutes, but the other
one did, showing that a conversion took place with change in volume,
which ean never be explained by conversion of S, into Sy, or Sy as
this causes the volume to decrease. The only possible thing, therefore,
is that Spr, — Sy, that is to say the transition point has been
lowered by S, to below 71°. This fall depends on the quantity of
S, which will decrease gradually. The baa: which take place in
presence of each other are S, —> Spr, S,—> Sy and Sy Spraq. The
decrease of S, may be seen from the rise in 7’—. After 4'/, hours,
no more change in volume at 71° could be observed, whilst after
6°/, hours the Jiquid in the dilatometer distinctly fell. The transition
temperature then appeared to lie between 71° and 72°’). In this way

') The forming or augmentation of a second phase rich in S, should also cause
the volume to increase. Whether a part of the depression in this manner has to
be explained, is on trial. Tt is however sure, that even when #t were so, the lowering
of the transition point by S,, has to be considered as certain.

*) This is not quite correct on account of the always continuing conversion
Sy» —> crystalline S in consequence of which, on decrease of the volume, a slight
conversion of SRhk—> Sv can take place. For the sake of brevity we will disreea
this, howeyer,

587

Total lapse of time

Temperature Time in which the rise

of bath gh pce tan or Rise in mm. was observed.
ee aaa

71° 2y,hours | t2 | 15 min.
ale rie 10,
Gl x; hs ie,
16° 25. x Th after 12 m. 10: 45
78° eau +2! after 15m. 12,
243), y T8tht a.
Ce ae aL eee
pee Hil | ae
903), - res tou
atin 4, cies 2 15,
86° 481/oy ae (after 12m IS y
86° 491, +2 after 15 m. (eas
87.5° Bees rath} jay
53> a 10°*
LL peal a oe
91.5° 73 - ex: after 14m. 12 ,
Way he [ses
Pallas Ji 15;
161, , s 1st
78 . A is.
94° 78/2» Tit after 12m. 20 »
168%; ea sae
95 .2° 1681/2, th 20h...
160° <, a Linea
95 .3° 1691/._, pane: falling {a8
95.4° 1693/, , - ia,
(7 or eee
95 .6° 1704, Tie ig;
fi. 3 ine 200,

588

the rise of 7’—> could be readily traced, from which it appeared
that this, with ever decreasing velocity, rose until 95.45° was
reached, which temperature is the true unary transition tempe-
rature. Hence, we see that 7’— can be lowered by S, fully 20°.
In harmony therewith is also the fact that starting from S,-free
sulphur, RetcHer (Dissertation) obtained, as he thought, diverging
results, namely first a transition temperature of 97° which tempera-
ture he found in course of time on the decrease until the unary
transition temperature 95°,45 was reached at which S, is present.’)

Simultaneeusly with the result mentioned above several experiments
were communicated which contrary to Kruyrt’s investigation (Z. f.
phys. Ch. 64 513) removed all grounds for the assumption of a
metastable region of demiscibility in the pseudo system. It appeared
that the occurrence of two layers is due to the difference in tem-
perature which between the two layers may amount to even from 10
to 30°. When the heat conductivity was improved by the introduction
of platinum wire or small gauze this phenomenon occurred less dis-
tinctly or not at all. Quite in harmony therewith is also the influence
which an alteration in the diameter of the sulphur tubes exerts on
the appearance of two layers. That we are not dealing here with a
metastable region of demiscibility appeared, contrary to Krvyt, also
from the fact that in the presence of NH,, which is a positive catalyst,
that apparent unmixing occurred still better, notwithstanding we
now follow the equilibrium line. While Kruyr believed that there
existed a constant three-phase temperature S, with two liquid layers
at 110° (intersecting point of the solidifying line of Sj, with the
region of demiscibility, point d of Fig. 4), this also did not prove
correct as, on inoculation with monoclinic sulphur, solidification
temperatures of 108° and 109° were observed and, when starting
from pure Sz, even 106°.

As the last publication I mention Krvyv’s lecture which contains
pretty well the same as the article in the Chem. Weekblad except
that Fig.8 occurs also.*) From this we notice that KrvyT now assumes
that C (7— of S,-free sulphur) lies at 94°.8, GH at 95°.6 (unary
temp. really 95°.45). In what manner these experiments have been
carried out, is, however, not communicated. They must be fauity or

1) Gernez also gives too high values (97°.6—98°.4). As GERNEz only observed
SRik— Sa and not Si —> SRa his figures are likely to be too high and do not
prove much.

2) In the Fig. Kruyt draws the S» to the right. The reason that | always
place it to the left is that I do not want to depart from the custom to place the
substance with the lowest m.p., therefore, _presumably Sy, to the left.

589

interpreted wrongly for it is a fact that addition of S, lowers the
transition point. The highest point given by Krvyr for the metastable
equilibrium Sp Sj is 96°. Above this, Sg when passing into Sy,

Fig. 3.
ought to begin to melt. This statement is rather remarkable when
we read that Kruyr in the Chem. Weekbl. 648, (1911) actually states
that all values for the 7—, on change of S,-content, lie dower than
95°.6. I should like to ask, how that temperature has been found ?
Also, the high values (97°.6 and 97°), deterniined by GeERNEz and
Rercaer, find no room in Krvyt’s Figure.

Hence, it is faulty without any doubt to let CG proceed to higher
temperatures; this line falls. If, however, we draw CG sinking we
obtain a Figure which is identical with a figure previously given
by Prof. Smirs (Proc. 1911, 264) and represented here by Fig. 4.
This identity becomes perfect if we leave out the dissociation region
drawn therein (which as stated in a note ought to be discarded as
not a single experimental fact points to its existence). In this way we
obtain Fig. 5. What Krvyr (fig. 3) calls CG is in fig. 4 and 5 op ete.

The deduction of the transition point of the sulphur with the aid
of the equilibria lines of the solid substance is therefore not due to
KRvyt.

590

591

Krvyt draws no region of demiscibility, but states that for the sake of
brevity he discards the probable occurrence of the region of demiscibility.
It would have been more correct to state that nothiny pleads for its
existence and that therefore it was omitted. In connection herewith |
will observe the following. If we prolong the lines AD and BE,
as indicated by Kruyt (Zt. phys. Chem. 64, 513) they intersect each
other at about 106°, so far above 96°. GH/ would then lie at 106°
which cannot be. If now we call to our aid a region of dissociation
(see Fig. 2) this difficulty, of course, does not occur, but this alone does
not justify the assumption of a region of Jdemiscibility, particularly
if we remember that the mode of representation is not correct.

The matter may indeed be explained readily when, as required
by Prof. Smits’s theory, we not merely assure two kinds of sulphur
S, and S,, but (at least) three kinds of molecules which we will
indicate briefly by S,, Sy, and Sp,. Because there exists a transi-
tion point Ssy = Sra we must also assume a pseudobinary system
Spr—Sm. The whole S-diagram then becomes ternary of which
already a schematic figure has been constructed (Proc. XIV, 266)
Prof. Smits has now modified the former ternary figure by omitting
the region of demiscibility and keeping account with the third crystallised
modification, the sowfre nacré'). This drawing is given in Fig. 6. The
above mentioned difficulty does not arise here at all. The lines AD
and BE from Fig. 3 are lines which in the ternary figure run over
the surfaces /,S, ZS and /,S, ZS’ and therefore are spacial curves which
may deviate much from the right ones. If we assume that the equili-
brium Sj, = Sr, sets in with infinite velocity there is formed from
the pseudo ternary figure the pseudobinary Fig. 5, in which the curves
justmentioned have undergone an intricate projection, whereby a
crossing may turn into an intersection so that the above mentioned
intersection at 106° need not signify anything.

Hence, it is incorrect to assume, as Kruyr, Smirn, and others,
that we can deduce from the unary solidification temperature of the
Sr, the S,-content with the aid of the line of equilibrium, since in
the projection the situation cf the lines in regard to each other is
totally changed. Also it is not permissible, as Kruyt has done, to
first determine the melting point of the rhombic modification and
then to determine the composition with the aid of the melting point
when the substance has become monoclinic, for AD and BE need
not, of course, be situated in one plane. Kruyt’s experiments on the
melting point of rhombic sulphur clearly indicate this.

1) See These Proceedings XV p. 369.

592

Krvyt has, in fact, not determined BE, but LL’, that is to say
the initial temperatures of fusion’). The line BE has been determined

q
4

1) He says, for instance, in his dissertation p. 48, of a mixture that at 112°.4
it just commenced to melt and then takes that temperature as melting point
temperature.

by SmituH; it differs somewhat and ought to lie somewhat higher
Now, Krvyr allows the sulphur to become monoclinie¢ and then again
determines the initial melting point, but according to bis figure, this
is totally impossible, when we notice that HL” is situated nearly
totally between AD’G and AD./, so that, starting from points of
BE we arrive into the region monoclinic sulphur-liquid, owing to
which the substance must be partly melted and consequently no
initial melting point can be observed.

This is the result of the incorrect assumption that UG rises, owing
to which AG nearly always gets situated quite to the left of BA,
If CG is drawn falling (lowering of the transition: point) in which
case we again obtain Fig. 5 this difficulty does not arise.

Summarising, I arrive at the following conclusions which- differs
case we from that of Kroyr:

1st The modifications introduced by Kervyr in the previous Fig.
of Prof. Smits (Proc, XIV, 264) are incorrect.

2nd By addition of S, the transition temperature S, <> Spi is
lowered.

3d Fie. 3 (from Krvyt) is not in harmony with the phenomena
observed (also see ad 7). Even [xrvuyt’s own experiments are in
disaccordance with it.

4th Kruyr has determined not the line BH from Fig. 3, but the

line BE’.

5th The system sulphur is not pseudobinary, but at least pseudo-
ternary.

6t In consequence of this, the true direction of the lines from
figs. 3, 4, and 5 is another one than that assumed by Krvytr. The
significance of the intersecting points of the lines drawn by Krvuyr
also differs from that attributed to them by that investigator.

7% There exist no grounds for the assumption of a region of
demiscibility.
Inorg. Chem. Lab. University.
Amsterdam, September 1912.

1) The difference has to be explained by the different method of working.
Freezing points are easily found too low, melting points too high especially in the
case of mixed crystals.

29
Oe

Proceedings Royal Acad. Amsterdam. Vol. XY.

594

Chemistry. — “On the nitration of the chlorotoluenes”’. By Prof.
A. F. Honueman and Dr. J. P. Wiavr.

When two substituents are present in the benzene nucleus, both
have a certain influence on the place where a third substituent
enters. Which of the possible trisubstituted isomers will be obtained
in a larger quantity depends, as I have shown elsewhere, on the
velocity of substitution which both of the groups cause.

If we consider for instance a monochlorophenol, the new entering
substituent places itself nearly exclusively on the ortho- and para-
places with regard to hydroxyl and not on these places with regard
to chlorine, because the velocity of substitution, which OH causes
is much larger than that caused by chlorine.

By considering all the cases of substitution in the bisubstituted
benzene derivatives, I found, that the velocity of substitution to
meta-places is always much slower than that to para-ortho-places,
and that the substituents that direct a new substituent to the latter
places cause a velocity of substitution which deereases in the
following order:

OH>NH, >halogens >methy1

As the halogens and methyl cause no large difference in the
velocity of substitution, it should be expected, that the entrance
of a third group takes place para-ortho as well to the halogen as
to methyl. Indeed, Couen and Dakin proved in an excellent and very
laborious research that in the chlorination of orthochlorotoluene all
the four possible chloro-o-chlorotoluenes are formed and in the chlorin-
ation of p-chlorotoluene the two possible dichlorotoluenes, whereas with

CH! CH® meta-chlorotoluene the same operation

howe C] a procured the isomers I and II, but not the

| I | and | II | | symmetrical dichlorotoluene, just as might

| Y, Cl ey Cl be expected, because neither chlorine

C] _ nor methyl direct a substituent to meta-
places.

In order to get an insight in the ratio of these velocities, it is
necessary quantitatively to determine the proportions in which the
isomers are formed; and as nitrations are generally not attended with
production of secondary products, we resolved to study again the
nitration of the monochlorotoluenes. Through former investigations it
was known, that o-chlorotoluene yields the product CH,,Cl,NO, = 1,2,5
(Gotpscumipt, Hoénia, B. 19, 2440), m-chlorotoluene yields the isomers
CH,,CLNO, =1,3,4 and 1,3,6 and para-chlorotoluene yields the
isomers CH,,C]NO, =1,4,2 and 1,4,3. The latter nitration had been

already quantitatively studied in my laboratory by van DEN AREND,
who had found that 58°/, of the isomer 1,4,2 and 42°/, of the
other one (1,4,3) are formed.

As we supposed that the nitration of ortho-chlorotoluene would
yield all the four possible mono-nitroderivatives, the first thing to do
was to prove this. The nitration product presents itself as a yellow oil
which commences to congeal only at about +1°; on the other hand, the
eutectic temperature of the binary mixtures of the isomers CH,,Cl,
NO, = 1,2,3-1,2,4 was found at 8°.2; of 1,2,.3+1,2,5at+1.1;
1,2,44-1,2,6 at 17° .2; 1,2,5-++1,2,6 at 7°.2. It was therefore evident, that
the nitration product could not be a mixture of only two isomers,
but must contain still a third and perhaps also a fourth. Of
course, this conclusion only holds good, when the nitration product
contains only the mononitrocompounds. This was proved to be so by
fractional distillation and the determination of the refraction of the
first passing drops and of the residue, which showed both the same
refraction as the principal portion of the distillate.

As it proved to be impossible to separate the isomer nitro-o-chloro-
luenes themselves, we reduced them; the chlorotoluidine CH,,CI,NH,
= 1,2,5, melting at 81°, separates easily in large quantities. The
oily mixture which remains then was acetylated, because we stated
that the acetyleompounds of the two vicinal chlorotoluidines CH,,
Cl, NH, = 1, 2,3 and 1, 2,6 are sparingly soluble in cold benzene.
Indeed, by treating the mixture of acetyleompounds with this solvent,
these two isomers were easily isolated and identified; the presence
of the isomers CH,, Cl, NO,=1,2,3 and 1,2,6 in the nitration
product was thus proved.

It was far more difficult, to prove also the presence of the
fourth isomer 1,2,4. After about six months of strenuous labour,
in which a great many methods were tried, we succeeded at last
in the following way: about 100 grams of the nitration product
was reduced. After separation of the isomer -1,2,5, the residue was
acetylated and the vicinal isomers isolated by treatment with ben-
zene. The products that remainec in the benzenic solution were
saponified; from the mixture of chlorotoluidines so obtained. a
great deal of the isomer 1,2,5 separated again on cooling. The liquid
residue, again converted into acetylcompounds, yielded again on treat-
ment with benzene a considerable pertion of the vicinal compounds.
After all these operations, there remained about 9 grs. of a mixture
of acetamino-2-chlorotoluenes, in which the compound 1,2,4 must be
accumulated. By dissolving this mixture in a little quantity of ben-
zene and by fractional precipitation of this solution with petroleum

596

ether, the first fractions are still essentially the isomer 1,2,5; but
at last, a fraction was obtained, melting at 70°—75°, whose melting
point rose to 95°, when it was mixed with an equal quantity of
the acetaminocompound 1,2,4. Though the latter could not be isolated
in a perfectly pure state from the mixture, this test proves nevertheless
with certainty its presence. This was still corroborated by treating
an artificial mixture of the four isomers, containing them in nearly
ihe same proportion as the nitration product (see below) in the same
way; it showed quite the same peculiarities and neither from this
mixture could the isomer 1,2,4 be isolated perfectly pure. The pro-
portions of solubility of this compound and of many of its deriva-
tives in comparison with those of the isomers are too unfavourable
to allow its extraction.

After having proved that really the four possible nitro-o-chloroto-
luenes occur in the nitration product of o-chlorotoluene, we proceeded
to estimate the relative quantities in which these isomers are formed.
The nitration itself was executed as follows. To 10 gr. o-chlorotoluene
was dropped 40 ers. of nitric acid sp.gr. 1.52 while stirring mechani-
cally; the temperature being kept between —-1° and + 1°.

For ihe analysis of the nitration product, the melting point method
was applied in ihe medification described by VaLrron. When looking at
the six binary melting curves, which are possible with the four isomeri¢
nitro-o-chlorotoluenes, one perceives, that these curves coincide over a
considerable range of temperature. For instance, considering the
binary curves for 1, 2,5-+ 1, 2,3 and 1,2,5 +1, 2,4, we see that
the branches at the side of the isomer 1, 2,5 coincide practically,
and it is the same in the other cases. We have then to do with
so called “ideal melting curves”; they show the property that the
lowering of the freezing point, say of the isomer 1, 2,5, is the same
for the addition of a certain percentage of any of the other isomers
or of mixtures of them, unless their sum comes again to the same
percentage.

Wishing now to determine quantitatively one of the isomers, say
1.2,5, we add to a known weight of the nitration product so much
of that isomer (of course also weighed) that it crystallizes at the
first freezing point of the mixture and we determine this point. We find
then with the aid of one of the melting-point curves the total amount
of this isomer in the mixture and it is now only a simple arithmetic
operation to calculate the amount of the isomer in the original
nitration product. In the same way, the quantity of the other
isomers is determined.

By this method, we found that the nitration product of o-chloro-

597
toluene contains:

Isomer | 1, 2,5 | f,204 pene 6 |) 23
ET ee oe Gs i a

in which the figure for 1, 2,3 is obtained by subtraction. It may be

observed, that this method of analysis was first tried with good

result on artificial mixtures of the four nitro-o-toluenes. ;

For the application of this method of quantitative analysis, it is
necessary to possess the isomers present in the nitration product in
a perfectly pure state. This presented some difficulty with the nitration
product of m-chlorotoluene, the nitro-m-chlorotoluenes being hardly
known and surely not obtained chemically pure until now. I shall not
give a description of their preparation and purification here, but
only mention that the isomer 1, 3, 6 (CH, = 1, Cl = 3) solidifies
at -24°.9, the isomer 1,3,4 at 24°.2, the isomer 1,3,2 at 23°.4,
and the isomer 1, 3,5 at 58°.4.

The quantitative nitration of m-chlorotoluene was executed in the
same way as is described for o-chlorotoluene. By applying the
method Vazxton on the nitration product, we found for its composi-
tion the following figures:

Isomers jas Asta el we i Aes agra

Percentage | 58.9 o2.¢ | 8.8

The figure for the isomer 1, 3,2 is the difference of the sum of the
two isomers from 100, the method VaLrron giving only more exact
results as the quantities to be determined are larger. On the other
hand however, we found by direct determination an amount of
8.3 °/,. We believe it therefore proved with certainty that this isomer
is present in the nitration product, and that the isomer 1, 3,5 is
not present in it in an appreciable quantity. The presence of the two
other isomers was already known by an investigation of Rrverpin.

From the figures obtained in analyzing the nitration products of o-,
m-, and j-chlorotoluene we may now draw the following conclusions.

In o-chlorotoluene, methyl directs the entering substituent to the

wax places 4 and 6, chlorine to the places 3 and 5. They act
"SCL therefore independentiy of one another, the little quantity
i of m-compound that is formed in the nitration of toluene

beingt left out of consideration.

When the velocity of substitution, caused by methyl and chlorine
were the same, the isomer nitro-o-chlorotoluenes would be formed

in the same proportion as in the nitration of chlorobenzene on one

598

hand and of toluene on the other hand. It must only be taken into
consideration that one of the ortho-places both of methyl and of
chlorine is occupied and so the remaining o-places will be substituted
in the same ratio as if both o-places towards CH, and Cl were free.
One should therefore expect a ratio of the isomers as follows:

1, 223) “TA glee silo. 6

30+2: 38: 70+2: 58
because the nitration of toluene gives 58°/, 0-, 38°/, p- and 4°/,
meta-compound and the nitration of chlorobenzene gives 30 °/, 0-
and 70°/, p-chloronitrobenzene. Of course the 4°/, of meta-compound
formed in the nitration of toluene, must be divided equally between
the places 3 and 5.

I deduced however that chlorine causes a larger velocity of sub-
stitution than methyl. If we call the ratio of these velocities 7, we
find for the proportion in which the isomers must be formed:

1, 3,2 a i a Pas eB 6
3072+ 2 : 38: 70x42 : 58

With the same reasoning we find for the proportion in which the

isomer nitro-p-chlorotoluenes must be formed :
LA, 143
58: 44+ 302

CMs for also in this case methyl and chlorine act independently

of each other.

ae Equalling these figures with those found by experiment,

c. we get the equations:

302 + 2:38: 70x + 2:58 = 19.2:17.0: 48.3: 20.5 and

58 : 302 + 4— 58 : 42
from which « may be calculated. As mean value of 2 we find in
this way:

= 1.401
expressing that chlorine causes a velocity of substitution 1.491 times
as fast as methyl.
Calculating now with this value of « the proportion in which the
isomers are formed, we get:

CH, CH, CH, CH,
23.3 “> Cl «208 mes (| a ae ee 58
Be Bad
Aol onal 4 | a> ee
42.7 18.7 19.2 44.6 49
Dera oe NS) Bes
133 ace Ct or

caleulated found caleulated found

599

Calculating however with the same value of w the proportion of
the nitro-m-chlorotoluenes formed by the nitration of m-chlorotoluene,
there is no such gratifying concordance. This is due to the fact,

ie that in this case the two substituents act no longer independ-
J) ently of each other, but that both methyl and chlorine
| 3| direct the entering nitro group to the places 2, 4, and 6.

\7~ Now we must not simply add the figures for the isomers,
but we must take the resultant of their action, as is indicated in
the scheme below, in which it is assumed that the benzene nucleus
is a regular hexagon.

If we calculate in this way the proportion of the isomers, we find
indeed a gratifying concordance between calculation and experiment:

CH, CH,
592/199 sof!

2 30 3.01

Va ri
25.9 32

calculated found

Amsterdam, org. chem. lab. of the Univ. October 1912.
Physics. — “On the polarisation impressed upon light by traversing

the slit of a spectroscope and some errors resulting there-
from.” By Prof. P. Zeeman.

In a communication “The intensities of the components of spectral
lines divided by magnetism’ '), I drew attention to the fact that
by the polarizing action of the grating the ratio of the observed
intensities of the components of a triplet differs considerably from °

1) These Proceedings, October 26 1907,

600

ihe ratio present in the light as it is emitted by tne source. In some
cases the observer sees only a faint central component and two
intense outer Components, whereas the true ratio is just the reverse.
In order to obtain in the image the true ratio of the intensities I
suggested to introduce before the slit of the spectroscope a quartz
plate of such a thickness, that the incident light is rotated through
an angle of 45°. *)

Besides the mentioned polarizing effect of the grating there is a
second cause tending to make the ratio of the intensities of com-
ponents of different direction of vibration in the image different
from that corresponding to the constitution of the emitted light.
I] mean the polarization impressed upon light which traverses fine
slits. Since Fizgau *) this effect is well-known, but the errors which
may ensue from it in investigating spectral lines magnetically resolved
have not yet been pointed out.

The following simple experiment is easily made. A vacuum tube
charged with mercury is placed in a horizontal magnetic field. The
emitted light is analysed by means of a spectroscope securing great
illumination and high resolving power. The slit must be under the
control of the observer at the eye-piece. The two yellow mercury
lines, which are resolved into triplets or the green mercury line,
which splits into three groups each of three lines may be observed.
If the slit is rather wide then the central components of the yellow
triplets may have twice the intensities of the outer ones; the three
groups of the green mercury line have about the same integral inten-
sity if not wholly resolved. If the slit (made of platinoid) be narrowed
gradually, the intensity of all components decreases, but that of the
central component or group more than that of the outer ones. At last
the central components of the triplets and even the middle group of
the brilliant green line can. be made to disappear entirely *), whereas
the outer components remain visible. From these observations we
cannot but conclude that the vibrations perpendicular to the slit at
last hardly traverse the narrow slit.

The correctness of this explanation may be inferred from the fact
that the ratio of the intensities changes gradually during the narrowing
of the slit.

The view may be controlled by the following observations. If a

1) ie. p. 231.

2) Fizeau. Ann. de Chim. et de Phys. Vol. 63 p. 385. 1861.

8) This extreme case involves the use of an exceptionally narrow slit rarely
employed in practice.

——s *

a et ea ss ie,

601

quartz plate, rotating the plane of polarisation through 90° be intro-
duced before the slit of the spectroscope, then only the outer com-
ponents of the resolved spectral line can be made to disappear.

A second observation was made with the slit only of the spectros-
cope. The lens of the collimator being removed the slit of the spec-
troscope could be seen distinctly while viewing along the axis of the
spectroscope. Looking through a calespar rhomb the slit appears
double. With a wide slit, illuminated by the radiating tube, the two
images exhibit the same intensity ; a narrowing of the slit gradually
makes the image due to the vertical vibrations more brilliant than
the other one.

I will mention two cases in which errors may be introduced by
the polarization impressed by the narrow slit. This happens in the
first place in the case mentioned above of the comparison of the
intensities of resolved components vibrating in different planes. In
the second place when the resolution of lines originally diffuse toward
one side of the spectrum is investigated, apparent shifts and dissym-
metrical separations may result. Is the original spectral line diffuse
toward the red then a decrease of the intensity of the central line
of a triplet will cause an appavent shift relatively to the outer com-
ponents toward the violet. The reverse will be the case if the
original line is diffuse toward ibe violet.

The apparent shift now under consideration has had no influence in
the experiments concerning a change of wavelength by magnetic forces
of the line Hg 5791, which the author‘) and (independently) Gmemin*)
discovered at the same time. Its existence could be demonstrated
also by the method of Fasry and Perrot, a method not dependent
upon the use of a narrow slit.

It is a favourable circumstance that a quartz plate introduced
before the slit of the spectroscope and giving a rotation of the plane
of polarization of 45°, eliminates at the same time as well errors
due to the polarising action of the grating as those caused by the
narrowness of the slit.

1) ZEEMAN, Change of wavelength of the middle line of triplets. These Preceed-
ings February 29, 1908, in print in the Dutch edition March 12, 1908, in the
English March 29, 1908.

2) P. Gwetin. Uber die unsymmetrische Zerlegung der gelben Quecksilberlinie
5790 im magnetischen Felde. Physik, Zeitschr. p. 212 (eingegangen 24 Febr. 1908)
appeared April 1, 1908.

602

Physics. — “Contribution to the theory of binary systems. XXI. The
condition for the existence of minimum critical temperature.”
By Prof. J. D. van Der Waats.

Already in the theory of binary systems concerning perfectly
miscible substances we repeatedly found the case of a minimum
critical temperature, and already in my ‘Théorie moléculaire’ I
derived the condition for the existence of such a minimum, and ex-
pressed it in the form:

a “ and
b, b,

In my investigations of recent times, in which I chiefly intended
to ascertain the conditions for the only partial miscibility, my
attention was again directed to the possibility of the existence of a
minimum (7;,, and I have come to the conclusion that there is
also question of such a minimum (7%), for the mixture ether-water,
but that the value of « for 7), minimum lies very close to the ether
side. If as second component we always take the substance with
the greater value for the size of the molecules, so ether in the
case under consideration, the value of « is 1 or nearly 1. In
‘the experimental investigation by Dr. Scuurrer my expectations
have proved to be correct, and he has even succeeded in observing
the course of the p,7-line for given value of v up to a certain
distance from the ether side, and found it in perfect harmony
with the course predicted by theory for completely miscible sub-
stances. He has even succeeded in reaching the value of 2 at which
the plaitpoint entirely coincides with the critical circumstances for
such a mixture taken as homogeneous. According to this experimental
investigation, of which I express my sincere admiration, the value
of zw at wkich the minimum value of (7%), occurs, is so close to
the ether side that we may put this value —1, and the second value
mentioned of z is at a distance of more than 0,8 from the ether
side, so that we may put it smaller than 0,7. For smaller value of .
« the non-miscibility, as a new circumstance occurring in_ this
system, prevents the observation of the course of the ordinary plait-
point line. .

In my investigation of the causes of imperfect miscibility and of
the different forms which can occur for only partial miscibility, I
was led to apply a simplification in the theory, which I thought that
though certainly of influence on the quantitative accuracy, would
be of little or no influence on the qualitative course of the pheno-

603

mena. In how far this is the case further investigation will have to
decide. The simplification consisted in this that for the value of b,,
which according to the theory is equal to 4,(1—a)+2h, ,a1—x)+5, 2°,
I assumed the value

by. == b, + @ (6,—b,)

With the simplified form 4, numerous calculations appeared to be
easily feasible which otherwise would lead to too intricate computations.

The simplification of 4, comes to this that we put 24,, = 6,+4,.
The theoretical value of 6,, can be calculated and leads, whether
one starts from the idea that ) is determined by the increase of the
number of collisions in consequence of the dimensions of the mole-
cules or by means of the theorem of the virial, to the same result.
By both ways one finds 6,=4 times the molecular volume of the
1st substance, in the same way 6, —4 times the molecular volume
of the 2°¢ substance, and 5,, = +4 times the molecular volume of a
fictitious substance consisting of molecules the dimensions of which
are between those of the two substances. If the molecules could

be regarded as spheres the radii of which we take =7, and 7r,,
4 1 4
yep 0, == = orca rir) —andke:b, ==>. ane ee (r,)*; then
ji r,t+r,\? ee an
> ae “(25 ‘y. If we put 0,=nb,, then 6,,—= 3 ) be

The three quantities 6,, 6,, and 6,, are therefore determined by the
distances of the centres at the collision of the similar and the dissimilar
molecules. Hence according to the theory 6,+-6,—2b,, is not equal to 0,

3
but equal to ee: We subioin some values of this

quantity for values of m between 1 and 3.

Vn Al 12 3 14 15 1,6 17 ey eS 19 2

n 1331 1,728 2,197 2744 39375 4,098 4,913 596 5,882 6859 8
& Misi 138) 1,521. 1728 1,953 2,197 244 (26 2744 3,048 3,375
1

l+n as Boe: am Kae een a plas POY en as a
5) 1,1655 1,364 1,5985 1,872 2,1875 2,598 2,96 3.18 3,416 3,928) 45
aes eels 0,0158 0,064 0,155 0,288 0,469 0,704 1,03 1,18 1,844 L177 225

n+1 b
“= for —2 instead
1

It is seen from these values that if one puts

1+PBn
of i: a =) for a value of 2 which is not great, the difference is

not much, but that the difference is already considerable for n greater
than 5, to which I concluded for the system ether-water.

604

1 1+ n\*
For n = 5,36 we have is = 3,18 and le ae.

.
—_

Let us- examine what influence this has on the expectation whether
minimum (7%), will occur for a given system or not.

a
qe
If this oecurst hen ae is negative for z — 0 and positive for 2 = 1.’)
av
2(a,.— a 2(6,,—b
Hence 7s De ( = ) for e—0. Let us think the value of az
a, 1

given thus:
dy =a, + 2(a,, — a,)e# + (a, + 4, — 24,,) 2”,

and #, in a similar form:

b, = 6, + 2(b,,— },)¢ + (6, + 6, — 2b,,)a?

a a
d— dl —
The quantity — has the same sign as ——. For 2=0 we have
dx ds
a b a a
therefore —*< —* or —"<—. We find for z=1
a, b, Dick

tie ro ot te) 2s ee
b

2 2
or
a, — Masts a by.
a, b,
or
‘aes
Or b,

I concluded already to these relations in my “Theorie moléculaire”.

. . a
For the existence of a maximum (7%), ne would have to be greater
)
ae
a a
than — and) =:
) )

1 2

1) In this investigation 1 have assumed that RT =o According to an
earlier communication (These Proc. XIII p. 1216) I demonstrated that
RTt, = ne = and that (7s) will have to lie somewhat below 8. So if I put
To ee 1 neglect — ate which may perhaps give rise to an error

of importance for widely differing components.

605

i F a a 2 y \
If we write a,, =/ //a,a,, ack 3 leads to the following equation :
13 DO)
ly V 4,4, Vb,, ay
Yb, b, Bis b,

or
Px. (LP n-+-1)°
7p ae
key 8Yn

5 a
And in the same way a

13
(Kaa, (6,0. a,
0b. be b,

Tr, Pa)
a :

8Yn
oa . a .
Now we can put two extreme cases, viz. that F continually

decreases till at 21 the minimum value has just been reached,
or that the minimum value begins at =O and that the quantity

a
rs becomes greater for all successive values.

In the first case, which is entirely, or almost entirely realized

Bn+1)
for the system water-ether, Waews Zs see. and
Syn

Sgcx. (PB Puy -
L ee Sn
‘In the second case

Y= rs gia)
Ty, ms Syn

Ty, (hn+1)*
— :
Tk, 8Yn

In both cases the higher critical temperature is in the numerator

Be Tr,
in the expression pe or ae where the sign = occurs
lea ley

and the formula:

and

606

A Vy (Bn-+1)
l ee ——
‘3 T, or ae 8Yn

may be considered as See the highest ratio of the critical tem-
peratures of the two components at which minimum critical tempe-
rature is still found.
If this ratio is smaller, there is a lowest value of 7% for certain
value of wv. At exactly the ratio given by the formula, this lowest
value is either at z=O or at e=1. And that in these two cases
the ratio of the critical temperatures: is the same, is the consequence
(B“n-+-1)° 1

-— to have the same value for — instead of
Vn n

for n. Only if 7 should have a different value, the equality of

woe * and Ve 2 would no longer hold.

of a property of

Hence it is necessary to calculate WAS Ts, © to find
b
—*_. In the above given table, in which the values ee — have
Vb,5, i,

Meee

been given for different value of m, we must divide —_ byVn: And
b,

this greatly reduces the value for large value of 7, but it always remains

larger than 1. It follows from this that 6,, >0,0,. For small values
of n it is nearly 1. For the above given values of Pn, I have calculated

b : puss :
the value of — and that of 7, and given it in the following table.

on 1,331. 1/28 2,197 2744 3375 4,098 4,913 536 5,832 6859 8
2 1,1576 1,981 1,521. 1,728 1,958 2,197 244 26 2744 3048 aie
Vn 1,1576 1,318 1,482 1,656 1,937 2,023 223 232 241 262 2829
a 1,01. 1,027 1,044 1063 17086 1,094 112 1,134 LI = aoe
V bybs
Before applying the formula Aes = to the system water
1s |

ether, I first wanted to examine what S tae would follow for / with
the values a,, a,, and mn, at which I had arrived in a previous
investigation. I had concluded to an exceedingly small value for «,,
and to a value little below 6 for ¢,, while I had come to a value
lying between 5 and 5} for 1.
If we again put a,, = /Va,a, and a, = 1 + «, and a, = n*(1-peg
Gi, 0%. lyfa,a, mcr ly (t str) a Os

in ——— we ge OL =
ie Mae er sea

607
. - | b,, > o :
For n = 5,36 we have 5 i 2,6, and V7 being = 2,65 we find:
1
2,6
{= ——
2,65
: : Aar - l+n
which is very near 1 viz. 0.98. With 4,, = 5 we should have
3,18 .
found cane so about 1,2. And as I have, indeed, repeatedly met
i009

with 7/< 1, but never with /> 1, this is the reason that has induced
me to try whether the theoretical value of 6,, would harmonize better
with the observations than the simplified assumption, which implies
that b= 6, $1 + (n—1)z}. And the result obtained with the theoretical
value of 65,, even leads us to consider the quesiion for a moment,
whether if we could always introduce it, / would not always appear
to be =1. But we have first to examine in how far the values of
€,&, and m put by me for the ratio of the size of the molecules of
water and ether, will appear to be correct. Thus for n = 4 the value

i) s

of = would be equal to about 2.19 with the same value of ¢, and
1

«,, and hence

or
b= 0.81
Now as I recently demonstrated (see among others Arch Neéerl.
Serie III A. Tome 1 p. 136 etc), we can calculate the value of a
for a substance pretty accurately. We then found :

(ADs)?

—
e

f—1

Pk
And as for all substances, only with the exception of methyl

i ee

6
alcohol, the value of =s5,, we have:

re
27 (RT .,)?
EE SSS °
64 pe
638
For water with R7., = -
: al

Ady — 0,01204

467 e
And for ether with RT. = aa and per = 9395 the value of:

and p-, = 190, this yields the value of:

me«

Geth == 90,0358.

608

For “) Wwe find with this 2,932 and |Y2 = 1.712. Hence
a,

a,
Slee B sae
7. Sn
That I put 1-+¢«,—=7 and «, almost 0 was the consequence of
my opinion, which some circumstances had led me to accept, that 7

ty ah
ae becomes equal to
a,

Ite Sto c
would be about 5, for "being = Ea it follows from n= 5 that
n* 30
n? 95 ea >
ee a (et
3,513 3,518

We have, however, not been able to find a formula for the accu-
rate determination of 4, for a substance. We can, indeed, give the
form :

Evie

But about rs, for which 8 is an approximate value, we know
only that this product is <8, and probably the smaller, as b is
more variable and decreases more rapidly with decrease of v. If
we attribute this change of 6 to the compressibility of the molecule,
rs will be the smaller as the molecule is the more compressible.

0,0123 0,0488
We then find (09). = cau for water and (Oa)e = , for ether.
TS) rs)e
b 0,0488 (rs).» tl ee
For ——7 ae — 3.92 Neither for ter nor
or as 0,0123 (v8), oe ither for water nor

for ether, however, is the investigation exhaustive enough to enable
us to conclude to the value of 7s with perfect certainty. And so we
can only assume a value of about 4 for m with some reservation.
That I assumed 2» to be a little more than 5 before, was because
I only intended then to investigate the behaviour of a binary mix-
ture that should behave in somewhat the same way as the system
ether water.
2,197

With n al to 4,098 we found fro = for: Fl
ith n equal to 4, we found from L712 = 4,098 ol 1e

value 0,91.
If after this digression we return to the equation
(Ta Va
(7 Nes 8Yn
we shall have to find the same value for /, because we have put
the value of (7s), = (rs). in our former calculations. It appears from
everything that from this equation we can calculate the highest value

609

( Tr), ( Tr).
A Of
(Pi), (Th)
rather high degree of approximation. But the uncertainty, or rather

at which minimum value of (7%), can ocenr with a

our ignorance of the value of / prevents a sharp determination.
What precedes is of use at least in so far that it gives the reason
why in the first experimental investigation about binary mixtures,
for which the value of 7), differed so little for the two components,
minimum (77), was of such frequent occurrence.

Let us now proceed to the determination of the value of « at
which the plaitpoint coincides with the critical point for the mixture
taken as homogeneous. For this mixture the p,7-figure is not rounded,
but the vapour and the liquid branch touch each other in the plait-
point; they also touch the p,7-line of the plaitpoints and the p,7-

: ue : (EES 64-
line of the critical points. From — = 5. 4 follows :
P al

Zar 1 dp da
Tder Pp da adx
and with —-—=A4(rs), if we neglect the variation of (rs) follows :
P
dT 1 dp db

Pas a p da bda

— = /f;, we find by division :

as I assumed already before but without a rigorous proof, and
without demonstrating that on account of the probable variability of
(rs) the relation only holds with a high degree of approximation.

If we have two componerts for which the value of / does not
differ much, /f,, which will probably lie between /f, and /,, will
not differ much either. For the mixture water-ether / may be put
= 7 approximately, at least not far from the ether side, hence we
must determine w from the equation :

2 (a,,— 4,) + 22 (a,+4a, —2a,,)
a,+2(a,, 4,)2# 6 (a, +a,—-2a,,) 2” ¥
5 2(b,,—6,) + 2a (6,4+6,—26,,)
EiGb; to 2 O,— Oa Fa OF UP ,)
40

Proceedings Royal Acad. Amsterdam. Vol. XV.

610

a, a = maig ih 2
With — = 2,932 or | /S=1,712and/=0,91 and with 5 = 4098
a, a, 1
this equation becomes:
0,5579 + 0,816 2 5) 1,197 + 0,702 «

1+ 1,1158e-£ 0,8162* 61+ 2,394.2 + 0,702 a?

For «1 the first member is equal to 0,468, and the second

a
member ( withou the factor =) equal to 0,464, so almost the same.
8) :

For «—O the first member —0,5572, and the second member
equal to 1,197. To obtain equality the factor wouid have to be

1 :
smaller than ou For «= 0,6, the first member becomes equal to

0,535 and the second member equal to 0,6, so that the factor would
be equal to 0,89, which would be slightly too great according to the

srobable value of f,. With /,—=7, —— is equal to 0,83: ScHEFFER’s
| : |

observations, therefore, yield a value for « somewhat greater than
the value of « which satisfies the given equation. Possibly the
constants occurring in this equation, may have to be revised, and
n put somewhat smaller than 4,098. The value of p, for ether,
which was found by Scurrrer larger than 35 (viz. 36,1), would
also point in the same direction. But then / is also reduced to a
smaller value than 0,91.

As may be supposed as known, the plaitpoints on the p,7-lines
for constant value of « do not lie at the highest value of 7. Be-
tween the value of x for the minimum critical temperature and that
of the remarkable point they lie on the vapour branch, and in the
remarkable point they are transferred to the liquid branch. But for
the values of « which differ littlke from this point, the distance
between vapour branch and liquid branch is very slight, and in the
point itself the distance is zero. From the values printed by Dr.

Idp , prods age
ScHEFFER in large type the value of — for the plaitpoint line in

P @
the neighbourhood of the remarkable point can be, therefore, calcu-
: ff rs Lp ee
lated with close approximation. Then, however, ae 9,4 is found
pe

even for the highest value of the water-content, and so certainly
higher than fr. From the course of the three-phase pressure this
value is found to be 7,08 at the highest temperature, and this goes
to support the expectation that the three-phase line touches the
plaitpoint line. But at the same time this shows that the remarkable

611

point lies at somewhat higher water con(ent than that at which
Dr. ScHerrer has been able to continue his observations.
If the highest point of the three-phase pT-line is taken as the
(RT)? 64
p27
with 7’ = 202,2-+ 273 and p=91,8. The value assumed by us for
dz above, viz.:

remarkable point, one finds the value 0,024 for a, from Ls;

dy =a, {1 + 1,1158 x + 0,816 we? }
or

2,022 =1-4 1.1158 ¢ + 0,816 2?
would yield 0,627 for the value of x, and hence for « reckoned
from the 2d component, the value 0,373.

But small differences in the data change x considerably.
a,
~a value
a,

of «= 0,68 is calculated, and so «—0,32 reckoned from the
ether-side, which is only slightly higher than the « to which
Dr. Scuerrer carried up his observations. And that the value of «
for the remarkable point lies higher, appears also from the value of
T dp
on

If the ratio of the critical temperatures of the components is below
the above given limiting value, then minimum 7%. is found at certain
value of «2. As has already been stated only just there where

1 da 1 db
———=--—,, when (rs) has the same value for the two components
a dz h dx

and for the intermediate mixtures taken as homogeneous. If (7s) differs,

h da db d(rs) Baril P hiel 1 da 1 db
: ae a OF BNC Mixture tor which — — == —~——
et ade bdo (rs)de é:da b de’
dT. d(rs ee Ue

aes AEM hence the minimum has slightly been shifted to the
T da rs de

component for which (7s,

small difference, we can derive the following rule for the place of
minimum 7. Then:

So with /=0,9, hence also slightly changed value for

which still has the value 9 instead of 7.

is smallest. But if we disregard this probably

Ll da 1 db,

a de be the

or
(a,, —4@,) a (a, +a, —2a,,)@ ae (6,,—,) ai (6, +6, —26, ,)a
a, +2(a,,—4,)a + rea je" b, +2(6,,—b,)e + (6, +b,—2b,,)a?

40*

612
If both members are multiplied by 2, and subtracted from 1,
we get:

a, + (a,,—a,) #

a, + 2(a,,-—a,)e + (a,+ a, —2a,,)a? ee

From the equation derived from this, :

(a,,—a,) + (a, +a,—2a,,)z i (6,,—b,) + (6,+6,—26,,)a

a, + (a,,—4a,) 6b, +(6,,—6,)
or
(a,,—4,)(1—#) +(a,—a,,)7 _ (6,,—b,)(1—2a) + (6,—b,,) @
a, (1—a#) 4+ a,, 2 ou) b(t 2) be
or

a, (1 — 2), a, baa) oe
a,(l—a) + a,,2 6, —2)+5,,2

—— a a , ryyY a)
For the case that ~—— or 7;,— 7;,, we find «= and
ees iP - 14 Yn
71
1—a eos
1l+ypn

Let us put the difference of 7, and 7, such that 2=—41, just as
for the system water-ether. Let us keep 7, constant, but let us
take 7, variable. With decrease of 7, the minimum has got outside
the figure, and properly speaking (7;)min no longer exists. With
increase of 7’, the minimum enters the figure, and moves towards
smaller wv. If 7, has increased so much that it has become equal
0 7,, 2 has become equal to oars If we then keep 7, constant,

1t+Vn
so retaining the value which we had assigned to 7’, at first, and if
we now make the critical temperature of the first component decrease,

1
the minimum lies at still lower value than ———, and when we
+Vn
make this value decrease to the amount that we had originally
assigned to 7, « has become =. So the minimum always lies on
1

that side where 7; is lowest, reckoned from # = -———

ltyn-

If —~ is put below the limit for which there still exists minimum
2

7’, and if with the same value of n 7, > 7, is taken in the first

x a
case, and 7',> 7, in the other case, the values of ee = dif-
—

ferent. There is, however, a simple relation between these: values,

613

: x PP fiz ; ; sa
a - We arrive at this relation by writing
1 2

mT,b, for a, and the value m7\h, for a, in the equation

If then 7, and 7, are Caan the given equation is verified.

bd ry’ ry? v & .
Only in the case 7',=— 7, (, -) and & ) are of course equal
1 3

—

yes tn oa 1
and the value of this quantity is found equal to ——, as was found
V

above. If 7, = 0,
The two equations, from which the given relation can be derived

are in the first case, if we put : —_— N;,:
—wL,
mT’ .b..—a rey
N> eis aae ee yn (T,—T,) + iow 17 _
b, b,
and in the 2¢ case:
mlb eal 215
N,? saat ie (7,— , 2) fee pe = — ().
1 9

The second equation multiplied by such a factor that in this
too the known term becomes equal to that of the first equation,
micas 1V, NV, — —

The increase of pressure, if the system is entered from the ether

side, is, however, not so considerable as has been found by Dr. ScHEFFER.

A
The quantity =, which appeared to be almost constant, had for
eA

15,45 :
«z=0,316 the value age = 48,9. It is true that strictly speaking this
did not refer to the value of the pressure which we call p,,. But
the difference cannot be great for «= 0,316. From the three-phase

pressure which we have calculated, terminating at «= 0,373, the

value

or Bp yt Dios
= 42,1 would follow for —~. The quantity — for pe,
ile Lea Le

ean, of course, not be constant. For water this pressure is 190, and
for greater value of x (reckoned from the ether side) the quantity

614

Ap : ; eter hes
~ must rapidly increase. If minimum 7’, is exactly on the ether

&
1 da 1 db,
1d P 1 db. }

side, then and so at first the approximate value of

—_— == ———., But if (rs) differs appreciably from 8, an appreciable
P daz by daz
deviation can also occur in this. We find, namely, for pz not exactly
a log. 04 dpi: 1 da db, d(rs)
—__— but p, = —-——-—— and so —— =— — —- 2-—_ — 2, . As
27 bq? PE 97 ba? (rs) pkde adx — bjdx — (rs)dx
Ida = 1 db, -d{rs)
a dx by dx (rs)dax
dpi: 1 dby (rs)
pede oO b, dx (rs)\da
for water the observations at 7’,,. are not sufficient to allow us to
judge about the variability of 6, it must be considered impossible
for the present to decide whether (rs) differs for these substances,

holds for minimum 7, also

the relation 0 =

As, however, at present, both for ether and

dp*
and if so for which of them (7s) is greater. The value of 2 ;
prdx

. 1 db,
which seems greater than — --—— would lead us to expect that (7s)

dy av
is smaller for water than for ether. If this variability of 4 is attributed
to the compressibility of the molecule, the water molecule would be
more compressible than the ether molecule in spite of ifs simple
structure.

Physics. — “The calculation of the thermodynamic potential of
inietures, when a combination can take place between the
components.’ By J. J. van Laar. (Communicated by Prof.
H. A. Lorentz.)

1. In Dr. Hornen’s Thesis for the Doctorate recently published *)
the usual method of calculation also followed by me in the Areh.
TryLer ?) and elsewhere is eritised on p. 2—4, with which criticism
I cannot entirely concur.

In the cited paper in Tryter the problem in question has been
treated briefly and not very clearly (in a footnote of a few lines),

') Theorie der thermodynamische functies van mengseis met reageerende com-
ponenten en hare toepassingen in de phasenleer; Nijmegen, L. C. G. MALMBERG,
1912:

*) Théorie générale de l'association de molécules semblables et de la combinaison
de molécules différentes; Arch. TEYLER (2) 11, 3me partie, p. 1—97.

615

so that what has been said there can easily give rise to misunder-
standing.

But for this very reason I have afterwards once more fully dis-
cussed the matter in the Chemisch Weekblad'), This paper, however,
seems to have escaped the notice of the writer of the Thesis.

Fortunately he admits (see p. 4) that a correct formula has been
used by me, which leads to correct results. 1 should have been quite
satisfied with this, if not some objections called for further elucida-
tion so as to remove any doubt of the validity of the method fol-
lowed by me in imitation of Gipps, VAN per Waats and others,

2. It is clear that we may alevays write {for convenience’sake
we consider again the formation of a compound (association) of the
equal molecules of an associating substance, which compound
decomposed to an extent ~—— but the considerations would, of course,

apply to any compound, also of wnegual components | :
V.2

eee ‘| ub dw) dp re
Woh VE f a)" (ap) A a Secu a

X'9,30
| |

because the free energy y is a function of both v and ’ (7’ taken
constant). The quantities v, and ~, refer to an arbitrary condensed
gas or liquid state; the quantities V and ? to a very large gas
volume, where accordingly ~ approaches 1.

Equation 1 is always valid, for the integration is carried out along
the line of equilibrium, so that the functions w then always refer to

states of equilibrium, but then fe is always equal to zero in con-
t v

sequence of this equilibrium, ey we have simply :

Ow 1a
Woo, % — WV, Sea ® ‘ ; 3 F : 5 ( )

Vo>) 1)

(98 | :
In this | — }——p, hence applying van ber Waats’s equation
a

of state, we may write: ’)

(1+) RL a
yes = 2 - lv, . ° e ° 14
w, @)/70 y Ve {| y iy 1? te ( )

1) Beschouwingen over eenige fundamentecle eigenschappen van den thermody-
namischen potentiaal; Chermisch Weekblad 1969, N’. 51, p. 1—S.
2) Kor convenience’sake we ee viz. dissociation of double molecules to

simple ones, in which 2, —= — 1 2, =28,. 21S Pe, Se

616

in which the quantity B changes every moment, namely between the
limits of integration 8, and 3, during the integration (see also p. 5
of the paper in the Chemisch Weekblad).

But on account of this variability of 8 the calculation of (1”) is
rather laborious. because now also ? as a function of »v and 7’ is to
be substituted, and the integration can then give rise to difficulties.’)

3. It is therefore of importance to sketch a second method of
calculation of Ys, in which the said difficulty is evaded. There is,
of course, not the slightest objection to the method discussed just
now; against the method that will be given now an objection may
be raised, though it leads to correct results, as Dr. HomNEN admitted.

We have namely also:

é 2/70

(ow Op). dp] .
Wr, == wy ecm ee a =| dv, . . . (2)
|

"0)/70
0

in which, therefore, in the case of expansion to a very large volume
V the degree of dissociation p is kept constant, viz. equal to that of
the condensed mixture @,, Which is in internal equilibrium. Now we

dw
do not have c —() under the integral sign, for during the
08 /,
oe de : d3
expansion the internal equilibrium is disturbed, but — = O, be-
av
cause B remains constant. Just as above we have also here :
gers
(ow
a — ae ew ; »
Wr, 20 — Wy 2/70 jG de J = 4 : : * (2¢)
7"9:/20
Op : i : : ; :
or also, aa being again = — p, after substitution of the value
Vv 3 -
t
for p:
V Po
Ae er ee
Wr, = WV.Ao + a = 2 dv . ; . : (24)
J 4 v—b vy?

Yor/70
That (1°), to which no objections can be raised, and (2°) against
which an objection might be advanced lead to entirely identical results,
I have demoastrated in the cited paper in the Ch. W. (p. 7—8),
which furnishes at the same time an ¢éndirect proof also of the

‘) For also a and b are sill functions of 8.

617

validity of (2”), and it shows that practically the possible objections
to the validity of the second method are unfounded.

4. This objection consists in this that now we do not integrate
along the states of equilibrium, and that it is therefore questionable
whether it is allowed to substitute the known expression of the
mixture 3, as a function of v and 7’ for wy.:,.

Dr. Hornen says: strictly speaking it is not allowed, but after
some extension of the definitions of the thermodynamic functions, it is.

I will not argue about this, but will only draw attention to what
follows.

In my Opinion it is namely not of the least importance in the
calculation of the function yw for a mixture whether the components
happen to be in equilibrium or not. For what would else be the
meaning of the statement: In case of equilibrium yw must be a minimum!
How can a function be a minimum when the values outside the
minimum, where therefore there is no internal equilibrium, are
declared invalid ¥

Nobody has as yet taken any notice of the said objection, neither
Gipps in the calculation of the state of dissociation of N,O,, nor
VAN DER Waats') in his numerous calculations on these subjects, and
in my opinion justly.

For we write the value of the function w for an arbitrary mixture
of the components, even though there should be no internal equili-
brium, and then determine the specia/ values of 3 for which y becomes

hee: Ow : :
minimum, {| from seh Oe by which the required concentration

of equilibrium is obtained.

It is namely also possible to regard the mixture fictitiously as
non-reacting (this fiction is realized in many cases of retardation and
similar ones), and write the expression of y which the mixture would
have if the components really did not interact. For ancther value of
the ratio of mixing § there is another value of wp and for a
definite value of ? (independent of the constants of energy and
entropy determining the equilibrium) yw will have a smallest value.
Then there is really equilibrium, and now no change in the condition

‘an set ui even after ages.

5. Finally I will just reproduce the calculation of § 7 of the cited
paper in the Ch. W. (p. 7—8), in which the identity of the methods,
represented by the formulae (1%) and (2°), is proved.

Y Cf also VAN DER WAALS-KoHNSTAMM, p. 159 et seq.

618

Let us introduce the function § (the thermodynamic potential)
instead of the function w (the free energy); then we have to calculate:

Vp
(+8) 4 ae
a ee aa a — p( vy Gh) 4a
V0; fo
and
Vs
Pes tai k
Si, o Sy, 39 t ip \ Z ) ee p(V- Ua) oi tue Eee (2°)
v
"9, 0

For the simplicity of the calculation of (19, where we have to
integrate with variable 8, we suppose that also the state v,, 8, is a
gas-state, to which the simple law of Boye applies.

a. Calculation of (1°). As according to a well-known property :

0s os
[=n + n, ‘
On, On,
we get:
$= (1 =P) i, Se 2 tt, — Hy, aS pl Hy a 2u.),
C
with —-—=yp, and —=—yp, (u, and mw, are therefore the molecular
On, ny
potential: of the components), and with n, =1-— B, n, = 2p.
Now on account of the equilibrium (in (1°) we have namely
always states of equilibrium) — u, + 2u, =O"), hence simply:
c=u,,

i.e. the fofa/ potential of the mixture is equal to the molecular
potential of the first (the dissociating) component |or also equal to
twice the potential of the second component].
For «#, we may now further write at the large gasvolume JV:
u, = C,—RT log V + RT + RT log (1--9),
in which C, is the known temperature function. Hence we may
write for (1°):

= = |
Si, 80 aie | ¢,

Now for perfect gases (this follows from the condition of equili-
brium —u, + 2u, = 0):

ee hae dv — p(V—2,).

Vo5/70

: 5 OS dn, 0S dn, 4
1) For ~~ =O is identical with — —- + —— —— = 0, i. e. with

0p On, dp On, a3
uw, (—1) + w, (2) = 0, or with — p, 4+ 2n, = 0.

B* ;
i—s — ix (} er . ° . ° ° * . a (a)
hence after logarithmic differentiation :
2—p dv
ag =
8 (1—8)

so that the integral becomes:
V3

Vp
1+-8)(2—8 3 2 _a\
(+8) ( ab) — E +- 2 log | = (8—3,) + ly ( 3 (I Bo) :
1—, : B,?

p (1 ==) ( 1— 8)?
"0,80 2'0,/20
In this according to (a)

| p? jee Kv
(1-p) 1—@'

‘ V 1—3
= (S—p L loc - ce
7 J=@-A + (= =).

and so finally :

i je. — RT logV + RT -+- RT log 9) | Me

hence

V i=
Bt | er (8—B,) + RT log — + RT log = — RT (B-- p,),
Vo es
because pV — (1-4-6) iT and pv, = (1 + p,) RT.
Hence:
Gre Zo (= ia Cy RT log v, + RT + RT log (1—~,), : (12)

the known expression for § or uw, when also v,, %, refer to a gaseous
State.
If the state v,, 3, had been a liquid state, the correct expression

would bave been found too, but in this case the integration would
have given rise to great difficulties.

B. Calculation of (2°). Let us write this equation in the form:

aS Ip
: ae Py aaa ads Ip <i s RT
$11, — SyV.2 - = == (01) = (<7, — (27,),) tl,

0s
then for the molecular potential 1, = — holds:
On,

V (0
“RI
(U1), == (44) V4 "| ri dv ax (1 Ke 1) RT,
r

reo
: s diag 2s 0.00. die:
because for perfect gases —= =—— => is no longer dependent
. . v Paes nett? v ‘
; 1 1 1

on the molecular values 7, ete. ‘

Hence:

: V
(U)v0.Fo — (81) V4) RI log a
1)

6
and therefore, if we may again put

(u,)V,a = C, — RT log V+ RT + RT log (1 — 8,)
for (",)y,2,, also when’ there is no equilibrium at the degree of asso-
ciation ~,, finally:

G0. = We = 7 ET ogy, RT eT log (ee (2¢)
quite identical with (1%). |For (r,),,2, may namely be written §,,4,,
because v,,3, represents a state of equilibrium, and hence §= 4,
(see above) |.

This way, which is much shorter. than the preceding, and there-
fore the prevalent one, leads therefore — in spite of (@,)V7,2, being
changed into its value, if the mixture @, is considered as an arhi-
trary one, 1. e. apart from the presence or absence of internal equi-
librium between the reacting components -— to the perfectly accu-
rate expression, which we have found in (1¢) by the much more
lengthy but perfectly unobjectionable way.

Baarn,, Oct. 21, 19123

Botany. — The Linnean method of describing anatonical structures.
Some remarks concerning the paper of Mrs. Dr. Marie C. Sropss,
entitled : “Petrifactions of the earliest European Angiosperms.”
By J. W. Mott and H. H. Janssonivs.

In our ‘Mikrographie des Holzes der auf Java vorkommenden
Baumarten”’ we are trying to show that important results in systematic
Botany can be obtained by anatomical investigations concerning the
wood, if these are conducted with sufficient care. For this purpose
descriptions of the anatomical structure are necessary, made with
careful observance of the rules given by Livny for describing the
external appearance of plants. Of course some additions to these rules
and some alterations have been necessary, because anatomical and
morphological facts belong to somewhat different orders of things
and because the microscopic method presents peculiar difficulties.
But in the main it is the Linnean method we apply.

The results obtained in the two first volumes of our work are
from a systematic point of view most satisfactory, which we hope
will become still more apparent, when after some years the work
will be finished. Families, genera and in many cases even species

621

are easily recognisable from the anatomical structure of their wood
alone.

The method used by us, though extremely simple and well known
in its principles, by aiming at a complete survey of the anatomical
structures, an analysis leaving no rest, becomes a very laborious
task, taxing rather heavily the psychical energy of the student. But
a somewhat wide experience in these matters has taught us that
only by the help of this method, results really worth while are to
be attained in anatomical investigations of every kind.

Thus it is our conviction that the eyes of students in anatomy
must be gradually opened to this truth. But we feel very well
that this is not a result easily to be obtained. It is a_ notion
widely spread among botanists, that every one having some general
anatomical knowledge can, without making use of any special
method or form, construct with great facility a good and useful
description of anatomical structure. Literature more and less recent
abounds with proofs of the truth of what has been said here. Des-
criptions are to be found everywhere, unripe, incomplete, abounding in
repetitions and omissions, referring to many things with which the
reader is not in the least concerned, unsteady and supported by lots
of necessary and unnecessary drawings. *

We cannot see however that up to this date the example we try
to give has procured us many followers. Nevertheless we want some
because there are most important problems, only to be solved by
the cooperation of many botanists using this samme Linnean method
of micrography.

Therefore we try to avail ourselves of every opportunity offered,
to show the value of our method in obtaining results, vainly aimed
at otherwise.

Thus some time ago we studied the wood of Cytisus Adami and
its two components C. Lahurnum and C. purpureus*) and were able
to show that the wood of C. Adami is that of Laburnum, very
slightly altered, it is true, but by no means in a direction tending
to the structure of the wood of C. purypureus. This result could in
the main have been anticipated from the splendid work of WINKLER
and Baur on this subject and in so far may not be accounted very
interesting. But it was valuable as a testimony for the usefulness
of our method, because several other botanists had tried in vain to
identify this wood.

1) Alph. De Candolle. La Phytographie végétale.
2) Recueil d. trav. bot. Néerl. Vol. VII[- 1911. 333,

622

Now. again a similar opportunity is offered by the publication,
some months ago, of an elaborate paper by Mrs. Mariz C. Stopxs,
entitled: Petrifactions of the earliest European Angiosperms’).

In this paper detailed anatomical descriptions are given of 3
specimens of fossil wood belonging to the collections of the British
Museum of Natural History. These specimens are from the Lower
Greensand, a formation of the Cretaceous Period and are considered
by the author as representing the oldest European Angiosperms,
known up to this date. For this reason a careful study of the inter-
esting specimens was commenced, and descriptions were made, so
far as the condition of the specimens permitted.

By far the best preserved specimen was that called Aptana
radiata, gen, et spec. nov. We will only treat of this one.

Reading on p. 90 of the paper the discussion of the affinities of
Aptiana radiata, the prospect does not indeed seem very hopeful.
Mrs. Sroprs points out that no branch of modern botany is in a
more chaotic condition than that dealing with the anatomy of
Angiosperms, which from a taxonomic point of view must certainly
be admitted.

She considers that it is entirely premature to attempt any dis-
cussion of the possible affinities of this fossil. “In evidence of this
“I may mention, that for more than a year I have been showing
“this fossil wood to many of the leading botanists of this country,
“Europe, and America, and that among the numerous opinions kindly
“offered, I have been told it resembled closely nearly every family
“ranging from the (netiles on one hand to the JMa/vales on the
“other. This is not to be interpreted to mean that the woods of all
“these families are alike, and that consequently classification of them
“is impossible, but it is due to the comparatively few samples that
‘any one individual studies and to the great range of variations
“between the woods of so-called species of so-called genera.”

Mrs. Stopes concludes: ‘The genera which I was able to examine,
“which showed most points of likeness to the fossil, were some
“species of Lonicera, of Viburnum, of Magnolia and of Liriodendron.
“Qn this however | lay no stress and consider that for the present
“more definite statements regarding possible affinities would be purely
“theoretical and unprofitable.”

We have quite another opinion. After the reading of Mrs. Sroprs’
paper, it occurred at once to us, that Aptiana could very well
belong to the family of the Zernstroemiaceae. And knowing, that

1) Phil. Trans. 0. t. Roy. Soe. B. Vol. 203. 1912. Pp. 75—100 and Plates 6—8,

with the help of our method we could hope to obtain certainty in
this matter, we proceeded at once to testing our hypothesis.

For this purpose the first thing we needed was a Linnean de-
scription of the wood of Aptana in order to compare it with the
several summarizing descriptions of the wood of whole families,
already published in our ‘Mikrographie des Holzes’”. Having done this
we found, that our first impression had been correct and that Aptiana
was no doubt a plant belonging to the family of the Ternstroe-
miaceae, very nearly allied to the genus Eurya, if not belonging
to it indeed.

In order to give the reader the means of judging for himself, we
will now go somewhat more in detail, first giving the Linnean
description of Aptiana, mentioned above, then a translation of our
description of a species of Hurya, given in the ‘“Mikrographie des
Holzes”’, and ending with a discussion of the results obtained.

The Linnean description of the wood of Aptiana now following
was of course abstracted from the paper of Mrs. Stopes. The data
thus gathered were arranged in the Linnean fashion, according to a
form for the description of secondary xylem, which we always
use as a basis of our description '). As far as possible Mrs. Stopss’
own words were used and the pages where they are to be found
were mentioned. But in some cases, where our interpretation dis-
agreed with that of the writer or where characters were described
only to be seen in the drawings or photos, this was of course im-
possible. These passages were printed in italics and if necessary a
footnote explains why it was desirable to alter the writer's statement.

Micrography of the wood of Aptiana radiata,

M. C. Sroprgs, Phil. Trans. Ser. B vol. 203, p. 75.

A stem or braneh thick about 3,5 ¢.m,

Topography.

Annual rings structurally recognisable *), the limit of some of the
rings a little difficult to determine; thick about 0.6 mm. (p. 85).
The number of vessels and their transverse dimensions, also the
cavities of the fibre-tracheids in the inner part of the annual ring

1) This form has been published with many others in: ‘J. W. Mott. Hand-
boek der Botanische Micrographie”. Groningen. 1907. p. 49.

2) On p. 85 is added: ‘but not clearly marked by any noticeable change in
the character of the wood or size of the vessels.” By studying Pl.6 Photo 4 and
Pl. 7 Photo 6 we have come to an opposite opinion, to that mentioned in the text.

624

larger than in the outer; the breadth of medullary rays sometimes
smaller in the inner part of the ring. Vessels for the rest uniformly
distributed; with a few exceptions isolated and standing separated
from each other in the radial rows of fibre-tracheids (Plate 6 Photo
4. Plate 7 Photo 6, Plate 8 Photo 10 and text-fig. 1); in one or two
eases 2 vessels standing adjacent in the tangential direction, but such
pairs are rare (p. 85) and disturb remarkably little the radial rows
of the fibre-tracheids (p. 86). #ibre-tracheids: the wood appearing
be entirely composed of fibre-tracheids; arranged with considerable
regularity in radial rows (p. 86). Wood parenchyma scarce and
possibly wanting; several times lying just behind vessels, spanning
the distance between the rays (text-fig. 1 and p. 86). Medullary rays*)
in 2 kinds. The most numerous principally 1-seriate, 4 to 10 cells
in height and simple (hinfache Markstrahlen, Mikrographie I. 59).
The other kind 4 cells wide — a few 3 or 2 — a dozen cells in
height *), often composite (Zusammengesetzte Markstrahlen, Mikro-
sraphie I. 59)*), consisting of 3. stories. Between the multiseriate
rays innumerable 1-serate rays (p. 86). The medullary rays running
between almost every 2 radial rows of tracheids and vessels (p. 84)
and in such a way that nearly every fibre or vessel is in direct
contact with them (p. 86, see also p. 90). The cells of 1-seriate rays

1) A character, described by Mrs. Stopes (p. 87) as a noticeable feature, is the
way of dying out or dwindling down to 1 cell thick in transverse- section of the
broader rays (PI. 6 Photo 3 and 4 dm and text-fig. 4). The authoress says herself:
“while it is very possible that, as both Prof. Ottver and Dr. Scorr have suggested
“to me, this is due to the rays therein lymg somewhat oblique, in a radial sense,
“so that any transverse section passes through them, yet it remains an unusual
“feature in the truly transverse section of the wood, and gives it the character
“shown in text-fig. 4, which separates it from any wood with which I am acquainted.”
Witliout doubt the explanation given by Prof. Ontver and Dr. Scorr is the right
one. In our investigations we have very often met with the same phenomenon,
which is represented in a considerable number of our figures, e.g. 16, 24, 34,
38, 40, 41 ete., also in that of Eurya acuminata, given below.

2) Plate 6 Photo 5 shows that these rays can be at least 3 times this number
of cells in height.

5) The term zusammengesetzte Marrstrahlen was first used by us in our Mikro-
graphie as cited above. The definition of the term is given there as follows :
“aus in senkrechter Richtung tibereinander gestellten, regelmiissig abwechselnden
1- und mehrschichtigen Teilen zusammengesetzt. Die einschichtigen Teile fast
immer aus aufrechten Zellen aufgebaut ; stets das oberste und unterste Stockwerk
bildend. Die mehrschichtigen Teile fast immer aus liegenden Zellen aufgebaut.”

The study of p. 87 of Mrs. Sropgs’ paper, text-fig. 3 and 5, Plate 6 Photo 5
and Plate 8 Photo 11 will convince the reader, that our description, as given in
the text, is correct.

625

having the same shape as those of the 1-seriate stories of the com-
posite rays (Pl. 6 Photo 5).

Description of the elements.

I. Vessels. R. and T. 28 to 40 uw, about 33 u
being the commonest size. Roughly circular cylinders.
Transverse walls placed very obliquely; with scalari-
form perforations and horizontal rungs, see fig. 1°)
Walls thickened, but not remarkably so and the
lignified wall much thinner than that of the adjacent
cells (fibre-tracheids); —— with irregularly placed
simple round or slightly oval pits (p. 86).

II. Fibre-tracheids R. and T. 15 to 50 (@) yw, the
radial dimension often somewhat smaller than the
tangential; 4- to 6-, generally 6-angular. Wadls in
most cases thickened, the lumen of the cells ‘/, or
less that of its whole diameter (see P]. 8 Photo 10
and text-fig. 1); -— with bordered pits, on the

eek tangential walls at least as numerous as on the radial

Aptiana radiata (p. 86, Pl. 8 Photo 10, and text-fig. 1); arranged
Stopes. Transverse in 1 and in a few cases in 2 slightly irregular rows,
chao. not very closely arranged in vertical position, each
foration.Reproduct- being spaced at a distance from its neighbour roughly
ion of textfig-2 of equal to its own diameter; borders of pit-chambers
Mrs. Stopes’ paper.

circular (p. 86).

Ill. Wood parenchyma. Cells on a_ transverse section somewhat
elongated in the direction of the circumference of the vessels. (Pl. 8
Photo 10 and text-fig. 1). Walls thickened; — with only simple pits.
Contents more blackened than that of other cells (p. 86).

IV. Cells of medullary rays. Walls thickened; pitted (see Pl. 8
Photo 10 m, and p. 89).

Having completed this description we compared it with the general
descriptions of the wood-anatomy of the several families, published
in the two first volumes of our “Mikrographie des Holzes’’. It was soon
found that the only family with which the characters of Aptiana
coincided and did so in a very satisfactory manner, was indeed that
of the Vernstroemiaceae.

1) On p. 86 Mrs. Stopes says: “In longitudinal section not many of the vessels
show the character of their walls, but those that do, have broad, simple scalariform
pitting (see text-fig. 2)”. If a regular Linnean description had been made, this
mistake would no doubt have been avoided.

Proceedings Royal Acad. Amsterdam. Vol. XY.

626

We now sought in this family among the species of which a full
description was given, for that which corresponded in the largest
number of most essential characters with Aptiana. We found that
this was the case with Hurya acummata and we reproduce here a
literal translation of this description, as given in our Mikrographie,
but somewhat shortened for the reader’s convenience, by omitting all
those characters of which no mention is made in the description of
Aptiana.

If the reader will compare the two descriptions with each other,
he can judge for himself of the validity of Aptiana’s claim to be
considered as a member of the family of the Vernstroemiaceae.

Micrography of the wood of Eurya acuminata,
DC. Mém. Ternstr. 26.

A stem or branch of about 7 em.

Topography. (See fig. 2).

Annual rings, especially in the sample
most minutely examined, fairly distinet ;
0.35 mm to 2.5 mm thick. In several
rings a period in the number of vessels
and the transverse diameters of vessels,
fibre-tracheids and wood parenchyma cells,
in the 2 last named elements especially
of the radial diameter; the maximum of
this period about in the middle of the

m!: ring, the minimum in the outer lower
Wk than in the inner part, especially for the
CH radial diameter of the fibre-tracheids. The

‘\ eS limits of the rings sometimes more distinct,

_...jtmm bY the number of vessels in the different
Fig. 2. rings being unequal. On the limits of the

Eurya acuminata. Transverse rings the medullary rays mostly somewhat
aS ag Pg ae : broader. Vessels for the rest regularly
Wood parenchyma; Ms Medull- distributed ; almost always isolated, only
ee very seldom in pairs. Fvbre-tracheids con-

stituting the groundmass of the wood; only now and then in radial
rows. Wood parenchyma scarce, scattered between the fibre-tracheids ;
when bordering on vessels, on the inner side of these only. Medul-
lary rays in 2 kinds. The most numerous generally 1-, in the middle
sometimes 2-seriate, 6 to 30, mostly 10 to 15 cells in height and

627

simple. The second kind 3- to 6-seriate, up to 150 cells in height,
often composite and consisting of 3 stories. The absolute height of
the first kind of medullary rays smaller than that of the latter.
Between 2 multiseriate medullary rays mostly some 1-seriate. The
medullary rays laterally separated by 1 to 4 rows of fibre-tracheids
often adjoining vessels. The cells of the J-seriate rays resembling
those of the 1-seriate stories.

Description of the elements.

I. Vessels. R..25.to 80 gw, T. 20 to 70 un. Elliptical and circular
cylinders or multilateral prisms with rounded edges. Transverse walls
placed very obliquely, showing scalariform perforations with 50 to
125 horizontal rungs. The scalariformly perforated part of the trans-
verse walls sometimes 500 « in length. Walls 1.5 w thick ; — with
numerous transversely elongated bordered pits, when adjoining each
other; — with very numerous elongated bordered pits, when adjoining
fibre-tracheids ; —- with a few simple and numerous elongated one-
sided bordered pits, when adjoining wood parenchyma cells and
upright ray-cells; — with unilateral bordered pits, when adjoining
procumbent ray-cells.

Il. Fibre-tracheids. R. 20 to 30 w, T. 25 to 35; 4 to 8-angular.
Walls thick 6 to 8 «; — with numerous elongated bordered pits,
when adjoining vessels or each other; these pits more numerous on
the tangential than on the radial walls; borders of pit-chambers
circular or somewhat elongated in a vertical direction, e.g. 5 by 6 uw.

II. Wood parenchyma cells. Those adjoining vessels mostly elon-
gated in the direction of the eircumference of the vessels. Wa//s
thick 1.5 ~; — with a few simple, and numerous elongated 1-lateral
bordered pits, when adjoining vessels; with elongated 1-lateral bor-
dered pits, when adjoining fibre tracheids ;— with simple pits when
adjoining each other or ray cells. Contents: sometimes a few starch
grains and some red brown mass on the transverse walls.

IV. Cells of medullary rays. Walls thick 1.5 « or more; pits the
same as in the wood parenchyma cells.

A simple comparison shows, that there is a coincidence in almost
every particular, such as cannot be the outcome of accidental cir-
cumstances and as in classifying systematic botany must needs lead
to identification. As leading features in this comparison we consider
the very oblique transverse walls of the vessels, with their scalari-
form perforations; the groundmass of the wood consisting of fibre
tracheids; the excessive scarcity of woodparenchyma and the oc-

+1*

628

currence of composite medullary rays —all of which are characters
not found in many families and coinciding only in that of the
Ternstroemiaceae, Staphyleaceae and in some of the Olacineae. But the
two last could be excluded Ly differences in several other characters.
The objection might perhaps be made, that in our “Mikrographie
des Holzes’ we have studied only a comparatively small number
of families, viz. 33, up to this date, and that it would by no means
be impossible, that afterwards another family might be found coin-
ciding as well or even better than that of the Ternstroemiaceae
with the characters found in Aptiana. But we are going right through
the system, following the Genera Plantarum of BentHam and Hooxnrr.
Thus this objection implies the probability, that in a region of the
system far distant from the Ternstroemiaceae a family will be
found showing an anatomical structure of the wood coinciding in
almost every particular with that of the Zernstroemiaceae. Our
experience in wood matters leads us to tax this probability as
infinitely small. But we do not know what lengths some botanists
might go in such a matter. The argumentation stated above thus led
us to the scientific conviction that Aptana belongs to the Ternstroe-
miaced.

Having reached this point, we tried, making use of the analytical
key for the identification of the species in our Mikrographie and
comparing the descriptions of the species whether some nearer ally of
Aptiana than Lurya acuminata could be found. If the reader does
the same, he will be led to Hurya japonica and E. glabra. There-
fore we think that the genus Lurya may safely be considered as a
most near ally of Aptiana, leaving it undecided whether both could
be united with each other in the genus Hurya, which however to
us does not seem improbable.

In conclusion we want to say some words on the work of Mrs.
Sroprs and on the character of the observations made by us. In the
foreground must be placed the fact that for the whole of our know-
ledge of Aptiana we are indebted to the careful work of Mrs.
Sroprs. But we can go farther and trust, that the reader will not
have mistaken our work for a criticism of Mrs. Sropgs’ paper. If
we had not indeed considered this paper as a very fair specimen
of what at this time may be called good anatomical work, we could
not have written as we have done. That bad work does not produce
eood results is a truth, which we by no means want to prove. We
do not criticize a special paper, but the method or rather the want
of method still prevailing in almest all anatomical work published at
this day. And we think that we have shown how a research on a

629

very interesting subject, bringing to light a most interesting palae-
ontological result and ably conducted, might have bronght us still
nearer to the truth if the Linnean method had been used in making
the descriptions.

This method indeed asks much of the investigator’s time and
energy and the use of it can only be learnt by patient study. But
we mean to say, that at some future time a botanist of Mrs. Sroprs’
power will not be satisfied with descriptions of anatomical structures
made without the use of the Linnean principles of micrography.

Groningen, Oct. 21 1912.

Bacteriology. -— “On the reaction velocity of Micro-organisms’’.
By Prof. C. Erskman.

(Communicated in the meeting of September 28, 1912).
I. Velocity of disinfection.

Micro-organisms have been the object of various researches as
regards the velocity of their reaction, when exposed to external
agents. From the experimental evidence brought forward it appeared,
that. considerable differences exist between individuals of the same
species, of the same stock, nay of the same culture: they do not
react all about at the same time, but the reaction proceeds in an
orderly manner.

It is especially the orderly progress of disinfection of bacteria,
under the influence of germicidal agents, either chemical or thermal,
which, in- virtue of its vital importance for theory as well as for
practice, has recently been studied by several investigators.

Attempts have even been made to find a mathematical formula
for this gradual process. As I stated before’) Mapsun and Nyman
arrived at the conclusion’) that in the disinfection of anthrax spores
the reaction proceeds according to the equation for the so-called
“unimolecular reactions”. This view found favour with most experi-
menters.

When the reaction is illustrated graphically by plotting the results
(abscissae representing the times and ordinates the numbers of survivors),
a “curve of survivors’ is obtained, having the shape of \.. This

- 1) Proceedings of the Meeting of 27 Feb. 1909.
2) Z. f. Hyg. u. Inf. Kr. Bnd. 57, 1907.

630

being an exponential curve, will become a straight line inclining
to the abscissae, if we take the logarithms of the numbers of
survivors instead of the numbers themselves.

By expressing the results of the experiments logarithmically, we
can see at a glance whether, and how far, they are in accordance
with the formula, or whether they depart from it; the absolute
values being immaterial in this case, I used for my calculations
Briea’s logarithms in place of natural logarithms. (ef. H. Cuick).

In order to account for their results Mapsen and Nyman regard
anthrax spores aS an aggregation of individuals of differing resistance.
If however this dissimilarity were decisive, a totally different type
of “curve of survivors” could be expected, as I demonstrated in the
Biochem. Zeitschrift (Bnd, 11. 1908). Conformably to the frequency-
curve of QUETELET-GALTON au accumulation of deaths could then be
expected at an average moment of the process, the rest of the spores
with a lower or higher resistance, dying before or after it in gradually
lessening numbers. Consequently the curve of survivors would neces-
sarily assume the ~_-form or, when represented logarithmically, the
“form and not the shape of \. (see also fig. 6, page 637).

Experiments with bacillus coli, published by me in a previous
paper really brought forward a curve very much like it, which
however differed from the one expected in not being symmetrical,
as the first half of the germs were killed in much shorter time than
the second.

In the case of anthrax spores I obtained since that time results
in fair accordance with Mapsen and NyMan’s experience, just as
H. Cuick '), RercHenBAcn *) and others did.

a. Experiments with anthrax spores.

Fig. 1 shows the results of three experiments on disinfection
at 80°, 84° and 90°, expressed logarithmically. Their accordance
with the formula may be called very satisfactory. The deviations
from the straight lines, inclining to the abscissae, are indeed
slight. An exception is noticed only at the beginning of the experi-
ment at 80°, where there is hardly a fall in the number of bacteria
during the first few minutes. The same had occurred very regularly
in my previous experiments with Bacillus coli. This period of lag
1 then took to be an incubation. I learned since, that an analogous

1) The Journal of Hygiene, Vol. VIIL 1908, Vol. X, 1910.
*) Z. f. Hyg. u. Inf. Kr. Bnd, 60, 1911,

631

phenomenon is observed in purely chemical reactions, and is called
“induction” *).

For my experiments I used again suspensions of spores. Of every
sample, selected at definite intervals of time, 4—5 parallel cultures
were plated, of which | took the average. If the numbers did not
mutually agree the experiment was considered to have failed.

of survivors.

Logarithms of concentration

. 1. Disinfection of anthrax spores by heat.

TABLE I. Anthrax spores at 80°.

Time, Numbers on plates Number =tarting
| — Mean Dilution number logjo
| ae ae ele Ber | 1000

1 | 440| 422) 456 | 454/| 454) 445 1] 4895 1000 = 3.000
3 | 431) 4385 408 454 448 435 11 4785 977 | 2.990
6 | 366; 343) 365) 386 406 373 11 4103 838 | 2.923

10 | 597 604 605 614. 613) 607 6 | 3642 | 744 | 2.872
20 | 724) 756 665 729 788) 732 3 | 2196 | 449 | 2.652
30 | 935) 950 937 946 921) 938 2 | 1876 | 383 | 2.583
50 | 1159 | 1081 | 1077 1022 1024| 1073 1 | 1073 | 219 | 2.340

1) Bunsen and Roscoe, Pogg. Ann. Bnd. 96, 1805,

632

For an easy survey and comparison of results I started in my
eraphical illustration from 1000 living bacteria, the numbers obtained
by the experiment underwent a corresponding reduction.

Table I contains the numerical data resultmmg from an experiment.

As I stated before, Mapsen and Nyman’s interpretation of the
conformity in- the process of unimolecular reactions and the disin-
fection of anthrax spores is open to doubt. With greater consistency
H. Cnick avers not only that the two processes agree outwardly
but are even completely analogous :

“The fact that the individuals do not die all at once but at a
“rate proportional to the concentration of the survivors at a given
“moment, is to be attributed to temporal and rhythmical changes
“in resistance, which by an analogy with chemical processes, may
“be supposed to be due to temporary energy changes of the con-
“stituent proteins.”

Thus putting bacteria on a level with molecules has raised some
objections: ReicHeL*) remarks that this is admissible only if the
chances of the germs being attacked by the active mass of the
disinfectant were not the same for all bacteria, which in an homo-
geneous liquid is possible only for particles commensurable as to
number and size, such as molecules, not however for micro-organisms
and molecules. RetcHenpacH thinks so too. He can hardly imagine,
that considering the vast difference in size, not all bacteria should be
under the same circumstances, relative to the molecules of the germicide.

Still less can it be maintained that the bacteria must reach the’

thermal deathpoint in succession. Moreover considering, that the type
of the curve of survivors is not at all determined by the character
of the noxious agent, Rricnenpaca is induced to think, that the cause
is to be looked for only in the micro-organisms themselves, i.e. that
differing resistance decides the order of their destruction. The same
observer adduces theoretical and experimental evidence to prove,
that resistance depends chiefly on the “age” of a generation and
shows, by a mathematical treatment, that a culture, having been
developed in a definite manner, may contain generations, which,
when classified according to their ages form a geometrical series.
Assuming moreover that the individual resistance of the cells in-
ereases with the age of the generation, this would afford solid ground
to aceount for the orderly progress of disinfection.

It seems to me that this attempt to settle the question is some-
what artificial, its weak point being that RercHenBacu, on the basis

1) Biochem, Z. Bnd. 1i, 1908.

6388

of his supposition, shows only how a geometrical series can come
forth, not however why it always must do so, for example in the
case of anthrax spores, in spite of varying conditions of growth.
This points to a regularity as to the age-distribution, which of itself
requires an explanation. In my opinion, the one put forward by
REICHENBACH is inadequate.

It would seem then that, if we have to find an explanation, the
only way would be to consider the progress of disinfection to be
mainly a physico-chemical phenomenon. Mapsen- and Nyman and
Cuick lend further support to this view by agreeing that van ’t Horr’s
temperature coefficient appears to be applicable in this ease.

It may indeed be called in question, whether this material allows
of a mathematical treatment, since it can hardly be worked with
without committing serious experimental errors. Consequently, as I
pointed out in my first paper, the experimental data of the researchers
just mentioned, were far from accurate. Their results however, having
been corroborated by several other observers, their opinion that the
process of disinfection exhibits some analogy to a unimolecular
reaction, can no longer be disputed. Setting aside experimental errors,
divergencies from the regular process should then be ascribed to
individual differences in resistance.

b. Bacillus coli.

It seems that the individual differences mentioned above are more
frequently displayed by vegetative forms than by spores, anyhow
they show many more departures from the regular process.

H. Cuick found no less than three types of the curve of survivors
for the disinfection of staphylococcus pyogenes aureus with hot
water. I also refer to Figs. 2 and 3, giving the logarithmic curves
for the disinfection of bac. coli respectively by heat and with 0,5°/,
phenol. It will be seen from Fig. 2 how three coli-cultures A, B
and C, though taken from the same stock, when killed by heat,
yield very different types. 6 is the only one that corresponds with
the type of the unimolecular reaction. C’ shows a marked departure,
A only a slight one in the opposite direction.

In order to give an idea of the degree of accuracy of this kind
of investigations I once more subjoin all the quantitative results of
an experiment in Table Il. We know that plate-culture is not a
very precise quantitative method. Sets of parallel cultures not seldom
yield essential differences, even though the sampling may have been

634

performed with the greatest caution. Our results however, as may

“ay

Logarithms of concentrations of survivors

Minutes

Fig. 2. Disinfection of Bae. coli.

A, B, and C are different cultures.

be roughly concluded from the table are most likely not more in-
accurate than those of other investigators on this subject.

TABLE II. Disinfection of B. coli (culture C) by heat at 47.5°.

Disinfection

Numbers on plates

Oa:

oF [arecice Mean

coli with phenol also

Starting
number logyo

= 1000
1000 3.000
740 2.869
120 2.079
61 1.785
35 1.544
33.5)) 12525

yielded types of loga-

635

rithmic curves of survivors that differed for
various cultures. (Fig. 3.),

Both divert from the straight line, so the
reaction- or disinfection velocity is not con-

Logarithms of concen-
tration of survivors

stant: that of A increases in the progress
of the process, whereas that of C diminishes *).
The same types were also observed by H.
Cuick in the case of vegetative organisms.
Type C was also found by ReicaenBacn
(ef. tab. XIV—XVI 1.c.), who worked with
very young paratyphus cultures that were
killed off by heat at 47—49°. When the
culture was older than 13 hours, the expo-
nential curve became smoother, once how-
ever it assumed the shape of type A.
ReICHENBACH attributes the tendency to
depart from the straight line in very young
cultures to the relatively large number of
low-resistant individuals present. It is remark-
able, that H. Cuick’s experience is just the
reverse: the value of / diminishes in the

Minutes
Fig. 3. Colicultur 4)059, Course of the process for the older cultures,
g. 3. uy
» B(phenol whereas for the younger ones / is smaller
at 22°

and approximately constant.

As for my own experiments (with Bacillus coli), for the sake of
uniformity in my material I invariably worked with very young
cultures and found, as shown in Figs. 2 and 3 departures in either
way. Added to the contradictory results of the observers mentioned
above, this seems to suggest that the age of the culture does not
determine the form of the curve of survivors.

ce. Yeast cells.

It being possible that large cells might lead to other results than
small ones, I also made some experiments with yeast cells.

There is perhaps some reason to suppose that speaking generally,
in disinfection experiments, whether with thermal or chemical agents,
the individuals are destroyed, because the cells, suspended in the
liquid, are attacked by molecules, whose caloric velocity exceeds

1) The cultures referred to in Fig. 3 and Fig. 2 are not identical, though from
the same stock.

636

a certain limit. A slow process would induce us to think, that these
active molecules with a caloric velocity far beyond the average,
are only small in number, all the rest being comparatively indiffe-
rent. The micro-organisms are then as it were exposed to a contin-
nous shower of bullets (the active molecules) and if this shower be
not too dense they will be destroyed in succession and in obedience
to the mass-law. Thus the analogy with the unimolecular reaction
would be rendered intelligible.

Now, just as in a shower of bullets, the number of “hits” in our
case depends on the size of the targets, the larger the individuals
are, the more regularly the hits wiil be distributed among them.
We were therefore justified in supposing that, whereas the smaller
organisms behave in analogy to the unimolecular reaction, the
individual differences of resistance existing among the larger ones
become more prominent and express themselves in the form of the
curve of survivors.

I do not mean to attach great importance to this illustration, nor to
offer its validity as a point to be discussed. I only wanted to set
forth why I extended my experiments to larger organisms also.

Numbers of

germs ee alla Numbers of germs == s- ~~--- log.
1000 3.00 1000
goo 2.50 goo
800 2:00) ©ood
700 1.50 700
600 1.00 600
900 0.50 500
400 0.00 400
300 300
200 200
PERG.
9 > fe)

Minutes Minutes

Fig. 4, Rose yeast killed at 47°. Fig. 5. Rose yeast with 0.69/) Phenol at 25°,

637

First of all experiments were made with Blastomyces rosea, a
fairly uniform material, consisting of well isolated cells; their size
exceeds that of anthrax spores 90 times in volume and twenty times
in surface. The curve of survivors corresponds with type A of
Bacillus coli, i. e. the value of & increases continuously during
the experiment (Figs. 4 and 5).

The same type appeared invariably also in working with a pure
culture of press-yeast.

Numbers of
germs On Suppose the structure of the cul-
1000 3-09 tures according to various degrees

of resistance had in this case deter-

2.00 mined the shape of the curve of
survivors, it would not accord

1.00 entirely with the law of fluctuating
variability (QuETELET-GALTon). If it

o did, the curves would look like those
in Fig. 6. Intermediate between these
and the types of the unimolecular
reaction are the curves found for
yeast cells.

800

d. Small and large spores.

ReicHenBacH published experiments with the spores of a small
saprophytic bacillus. The results differed from those with anthrax
spores. The order of dying was not in accordance with the formula
for the unimolecular reaction, whether disinfection had taken place
by heat or with sublimate. During the process the value of &
increased progressively.

As a specimen of small spores I selected those of bacillus subtilis ;
in all my experiments the results obtained evinced a fair accordance
with the formula of the unimolecular reactions. Only towards the
end of the reaction / was always inclined to decrease slightly.
This peculiarity is indeed also noticeable in my experiments with
anthrax spores (cf. Fig. 1). It is much more conspicuous with large
spores (see Fig. 8 and Table III). Here we had to do with spores
of a particularly big bacillus obtained by chance from the dust settled
in a room. Their dimensions are about twice as long as those of anthrax
spores. Four experiments, in which the spores were disinfected by

638

heat showed invariably that there was at a given moment a rather
great fall in the disinfection velocity (Fig. 8).

Numbers of
spores
T1000

goo

800

Numbers of
spores

700

600

Minutes Minutes
Fig. 7. Small spores at 90°. Fig. 8. Large spores at 90°.

This result clashes with the reasoning on page 635, which rather
implied a gradual rise in the value of 4, just as with yeast cells.

TABLE III. Large spores at 90°.

Numbers on plates

Time Number) Starting
Facer a Tm ae a =i SS) eT Dilution number logo
(min.) 1 | 9 3 4 5 per cc. | —J000
: |
1 | 940] 843] 826! 830] 826| 853 75 | 63975
| | | 1000 | 3.000
3 2610 | 2624 2600 2603 2571 | 2602 | 25 | 65050 |
6 | 420; — | 501, 431) 487) 460 | 11 | 5060 78.5) 1.895
10 | 520] 481 | 492| 441} 481/° 483 6 | 2808 | 45 | 1.653
20 | 586 | 530/| 593 | 554] 438) 540 1 1 Sa 8.4 0.924
| }
30 | 163 151 | 157] 146| 112] 146 1 146 | 2.3] 0.362
| |

639
II. Velocity of germination.

Germination of spores is to be looked upon as a reaction to
the favourable conditions of the nutrient medium. As will appear
later on, this reaction can be very rapid at the beginning and is
very sensitive either way: in a negative as well as in a positive
sense. For when favourable and inhibitory influences coincide, the
spores are not to be decoyed from their tents: they do not develop.
It seems problable therefore that they permanently keep in touch
with their medium, from which they are not isolated by their mem-
brane as completely as is commonly admitted.

According to Koca and others, who watched the process under the
microscope, spores take rather a long time (one or more hours)
to germinate. Still in this respect individuals differ greatly. When
examining the suspended drop, we shall see after some time besides
fully developed spores, others still in their original state, and,
between these two extremes, others again in various stages of
germination.

We alluded to the possibility of indications of growth being given
at the very outset. Wei‘), among others, discovered that after
10 minutes’ sojourn in broth at 37°, out of 8600 anthrax spores
only 60 remained resistant, when heated up to 80° for a short time.
This rather surprised him, as he deemed it not likely that the greater
portion of the spores should have germinated so rapidly and hence
should have become vulnerable at a temperature of 80°. Yet, as also
FiscHOEDER*) remarks, this is the best way to account for WEIL’s
experience, which seems to prove that germination can begin very
soon, when the circumstances are favourable. Similarly FiscHoEDER
found in his microscopic observation of some spores, already after
5—10 minutes, such alterations in their appearance and in their
behaviour towards colouring matter as pointed to germination in an
initial stage.

The large spores worked with in my experiments on disinfection,
published in this paper, were also now selected for my material.
Their very size enables us to perfectly control the process of germi-
nation. Their growth optimum is 37° C.

The results I obtained, fully confirmed the observations of Weu,
and Fiscnorper. I agree with the latter, that the decrease of resistance
towards heat after a short incubation in broth or serum at a favourable

1) Arch. f, Hyg. Bnd. 39, 1901.
2) C.f. Bakt. I. Bnd. 61, 1909.

640

temperature, is to be considered as the initial indication of a germi-
nating process, not only on the basis of microscopic observation,
but also because of the fact, that there is no decrease, when ger-
mination is arrested, for instance by adding to the broth */, °/, phenol,
or by raising its temperature to 50°.

Weit’s and FiscaorpEr’s numerical data do not practically point
to an orderly progress of the germination, which was indeed evidenced
by our experiments. ;

Fig. 9, where logarithms of numbers are plotted against time,
illustrates graphically the decrease of the thermostable spores in
broth. The logarithmic curves, represented by straight lines, prove
that germination proceeds in accordance with the formula for uni-
molecular reactions.

When germination does not take place at the temperature optimum,
in consequence of which the process will be slower, again a period
of induction is distinctly noticeable. At 50° there was not any
decrease of the resistance, throughout the whole experiment.

ST
SUSHIL
~~ 2

qT
ee

0.3°

Logarithms of numbers of spores.

1.50} 4 =

z a Fa al
37 ° 1. Bay
:
oa; Jl ale j i | Ew | [ee a =
oO © 6 © 6 TS “oOmorio monroe ° '
CRF AO MAENO BDAC HR aAMYE HO
3 eS oe ow al
Minutes

Fig. 9. Large spores in broth at 20.8°
31.5°, 37.38°, 46° and 50°.

The results of one experiment are tabulated in Table IV. Before
plating the samples were heated for about five minutes up to 78°,

641

TABLE IV. Germination of large spores at 31.5°.

Time Numbers on plates Starting
Mean number Jogi
(min) 2 3 4 1000
l 489 541 560 534 531 1000 = 3.000
5 476 583 492 541 523 985 2.993
15 313 | 340 | 347 | 319 330 621 2.793
45 76 90 if) 74 79 149 | 2.173
90 18 16 14 19 17 32 1.505

The results obtained with small spores were entirely
with the above. In Fig. 10 the logarithins of the numbers

against time.

On the other hand anthrax spores beiave differently as

the curves of Fig. 11.

Log. of numbers of spore

‘OL “Sq

SOJNUTTA,

o8& pue ope ye YJoaq ut satods Tews

Proceedings Royal Acad. Amsterdam

Number of

5. spores

1000

700

600

analogous
are plotted

showh in

2.00

O 10 20 30 40

Minutes

Wig. 11. Anthrax spores in broth at 34°.

VOL RY.

642

The experiments taught that the value of & is not well nigh
constant, but diminishes progressively, so that the logarithmic curve
is convex on the side of the abscissae. (Fig. 11).

Since it was evident from Fig. 1 that anthrax spores were vulne-
rable at a temperature of 80°, the samples were heated up before
plating to 70° only.

Ill. Conclusions.

1. As regards disinfection of micro-organisms (vegetative forms
as well as spores) some species are killed off in an orderly progress
analogous to the process of a unimolecular reaction.

In the case of other species the velocity of disinfection is not
constant, but either decreases or increases in the course of the process.
However with them a certain regularity is also to be observed, viz.
apart from the period of induction, the value of / alters in the same
experiment continuously in the same sense.

Most often every species has a definite type expressing the orderly
progress of its disinfection. Some there are however affording different
types in different cultures of the same species; for this variability
no satisfactory interpretation can be given.

It is stil a matter of doubt, whether the progress of disinfection is
chiefly a physico-chemic phenomenon, or whether differing individual
resistance of micro-organisms of the same culture play a principal
part in the process.

2. <A striking analogy is to be observed in the orderly progress

Disinfection Germination

Small spores

Anthrax sp res

Large spores

VAs
Pay aged

Fig. 12. Types of logarithmic curves.

643

6f germination of spores to that of disinfection. Three species were
examined. With two of them development took place in accordance
with the formula of the unimolecular reactions.

The reaction-(germinating) velocity of the third species however was
not constant, but decreased progressively.

For the same species the orderly progress of disinfection and
germination do not always agree as to their types (fig. 12).

Physics. — “On the second virial coefficient for monatomic gases,
and for hydrogen below the Boyie-point’. By W. H. Krrsom.
Supplement N°. 26 to the Communications from the Physical
Laboratory at Leiden. (Communicated by Prof. H. KamERLINGH
()NNEs). ;

§ 1. Introduction. In Suppl. N°. 25 (Sept. °12) a comparison was
made between the experimental data at present available concerning
the second viriai coefficient, 4, for monatomic gases, and the relations
for the variation of 4 with temperature deduced in Suppl. N°. 24
(June °12) from certain definite assumptions concerning the structure
and the mode of action of the molecules. In continuation of that
investigation the present paper supplies a similar comparison for the
monatomic gases, and also, in view of the correspondence obtained in
§ 3¢ of Suppl. No. 25 between these gases: and hydrogen below
the Boy.e-point, for hydrogen, too, in that region of temperature.
Until such time as the theories introduced by Nernst and E:Nsreinx
concerning the application of the quantum hypothesis to the rotations
of the molecules have been further developed, only the suppositions
made in Suppl. No. 244 § 5 are of any account as_ simplified
assumptions if the specific heats of those gases are taken into
account; according to those assumptions the molecules behave as
if they were smooth rigid spheres of central structure, attracting
one another with a force which is a function of the distance
between their centres and is directed along the line joining their
centres. As was done towards the end of §5 of Suppl. No. 244,
this function is more closely specified by assuming that the attraction
potential may be put equal to ~-r~7 where g is a constant‘). It

1) For the present comparison is postponed with the assumption made by
TannER, Diss. Basel 1912, in which, for simolicily, the action of the attractive
force is supposed to be completely localised in a thin concentric spherical shell
surrounding the molecule supposed spherical.

42*

644

is true that without further evidence one is rather disinclined to
regard such a distance law tor the attraction potential as a funda-
mental property of the monatomic atom, and, should agreement with
experiment be obtained with any definite value of g, one would
like to obtain a deeper insight into the structure of the atom which
would lead to the same law of distance for the resultant of the
probable electric forces originating at various points of the atom ;
yet it is still clear that the results eventually obtained in the present
paper for the index g can give important indications of the direction
in which ene must look for the development of the correct atomic
model.

§ 2. A comparison was first made between the experimental data
and the hypothesis of rigid spheres of central structure exerting
central attractive forces upon one anotber proportional to 7—@+!)
where g is a constant (potential energy proportional to —7—%). This
was done, following § 2 of Suppl. No. 25, by moving the log Sy,
log 7-diagram for the experimental substance over the J, log hv-
diagram, where, following equation (42) of ie No. 246,

ae ial 3 Le aks ; 3 hy)
yh og gan Ronee (h v) eo (hv) Bi itis P (1)

For the meaning of / and v reference may be made to § 5 of
Suppl. No. 244. The scale was again 0.005 to the mm. and log hv
was again drawn increasing in the direction opposite to that in
which log 7’ increases.

In this connection it is to be noted that when g is just shghtly
greater than 3, and then v must be taken small in comparison, the
terms of equation (1) involving the square and higher powers of
hv ave small in comparison with the preceding term. The variation
of B with temperature then becomes the same as in the ease of the
assumption of constant ay and 6, . Hence comparison of experiment
with the hypothesis of constant values of ay and 5, can be made
the same as comparison with the present assumption concerning the
attraction potential with a value for gq which is but slightiy greater
than 95.

§ 3. Argon, and hydrogen below the Boyin-point.
at. In the case of argon ‘) the deviations of the experimental points

1) As in ‘Suppl. No. 25 § 3d the individual virial coefficients of Comm. No. 118d
have been used. In Comm. No. 128, June 1912, KAmEerRLINGH ONNES and
CROMMELIN gave values of Bac71) adjusted according to the temperature polyno-
mial of the empirical equation of state; in these were included the lowest three
temperatures, for which only a few points of the isotherms were observed and
for which, individually, no sufficiently reliable values for the coefficients could be
calculated; these, therefore, must be regarded as known with less certainty than

645

from the curves for ¢ slightly greater than 3 (ay and 4, const.), for gy=4,
and for ¢=5 were all found to be relatively small. With the expe-
rimental material at present available for this gas it is difficult to settle
the question as to which of these three values gives the best agreement
(ef. Fig. 1). An extension of the temperature region for which # is
known for argon, particularly towards the region of lower temperatures,
as is already contemplated by KamrErLincH Onnes and CRromMMELIN,
will be ef. Fig. 1) of the greatest assistance in settling the point.

5. From Fig. 1 *) it is evident that the best agreement is obtained
for hydrogen below the Boy.i-point (see in particular the points
representing the lowest three temperatures) on putting g = 4. (Compare
fig. 1 of Suppl. N°. 25, on which may be placed fig. 3 of the same
paper for the argon points so as to

3 ¢ jaar : :
34 a ae 7 exhibit the degree of agreement for ¢
\ | | . ‘
eee alia hp Ty} Slightly greater than 3). Hence, as
a) swe, Me | | far as / is concerned, the behaviour
> ks S “sa
ee > t —— of hydrogen below the Boyin-poin
| | | « e
\e| | | appears to be in pretty good agree-
eS ment with the assumption of rigid
f2\ ia ? Or
| Bh EN spheres of central structure wiih an
a LN e —— attraction potential *) proportional to
S X re —r-4,
> | {) ® | ' = ; *
ae ie 4 If we assume that, as far as B
A | pe } P .
73 | Q Mt _ is concerned, hydrogen behaves in
3) Qi-10 | cS :
Ee r | +a manner similar to the monatomic
* ee eee Q | argon not only (as in Suppl. N°. 25
JO Vie UGE. | a | me Settee oh ;
L } x Sr § 3d) witbin that region of tempera-
AA Cvigon ‘<Doag Sks e : ;
“J \ —@ | ture corresponding to the respective
| Vega | . : ,
——— ear {observational region for argon, but
er -| oz logs ;
Soll "32 2 toa Sj x) also towards lower temperatures,
(425) (qeyy I~ ey ne ats
so that the series of argon points
= may be supplemented by means of

the others. As the calculations of the present paper may be regarded as another
method of adjusting the virial coefficients, it seemed more reasonable to effect a
direct comparison of the equation with the individual values. Comparison of the
deviations occurring in this method which are independent of the adjustment to
the empirical temperature polynomial, with those obtained by the latter method
can then afford a basis of judging whether the deviations are greater or less than
the degree of accuracy of the observations (cf. p. 646 note I).

1) In this the point log 7 = 2,0, log BN = 6,5 — 10 for H, coincides with the
point log hu=9,551 —19, $F’; = 9,488 —10 when q=4, and with the point
iog Av = 9,815 — 10, Fs; = 9,495 —10 when q=5-

2) Braak, Diss. Leiden 1908, p. 85, finds for Hy at these low temperatures a

646

hydrogen below the Boyix-point, then it follows from fig. 1°) that
the attraction potential for argon is also proportional to —r 4; but
this conclusion must always be subject to reserve concerning the
validity of the assumption just made down to the lowest temperatures,
which has not yet been submitted to the test of experiment in the
present case.

c. Following § 6 of Suppl. N°. 25, the accompanying table gives
the temperature variation of 47’~'> (y is the coefficient of viscosity)
as given by the measurements of Kopsca*) compared with values
of byw! from

byw = Re? 3 Bl as, he ee (2)

The latter relation appears on the separation of the attraction virial
from the collision virial, as is indicated in equation (41) of Suppl.
N°. 246. For v the value 1.46.10—-'4 is taken from the data given
on p. 645 note 1 for the superposition of the diagrain for H, , A
upon that for the attraction potential -—7—? with ¢=4 (for the
relative positions of the H, and the A diagrams see p. 425 note 3
of Suppl. N°. 25).

ae byooc
7 To0¢
yo oe Miers eae
00C attraction
potential — r—¢
ee v= 1.46. 10—14
0 1.000 1.000
pes 40.17 0.949 0.927
— 18.82 0.883 0.836
ee gap 0.729 0.660
— 183.17 0.606 | 0.406

corresponding value for the index of 7 in the law of distance governing the force.
From the ratio of the potential (heat of exparsion) to the virial, REINGANUM, Ann.
d. Phys. (4) 6 (1901), p. 546, deduces that the force is proportional to from
CE TG For

1) The deviations of the individual values of BN from g =4 are of the same
order of magnitude.and are throughout in the same sense as their deviation from
the values adjusted according to the empirical temperature polynomial.

*) W. Kopscu. Diss. Halle 1909.

647

Comparison of the second and third columns would lead one to
desire a smaller value for v, and this in turn would lead one to
fix") the index y more closely as lying between 3 and 4, but nearer
4 than 3°). (Reference should be made, however, to the reserve of
§ G of Suppl. N°. 23 qualifying the validity of these conclusions
drawn from the influence of molecular attraction upon viscosity).

d. The log B, log T-diagram for argon could not be made to
coincide with the curve for constant doublets (Suppl. No. 25 § 3c);
this is in agreement with § 3d and ¢ of Suppl. No. 25 (and in
particular with Figs. 2 and 3 of that paper) and also with the known
‘aloric behaviour of this substance.

§ 4. Helium’). Helium shows, at the higher temperatures, a
deviation from all the hypotheses introduced in Suppl. No- 24 and
tested in Suppl. No. 25 and in the present paper, for the maximum
exhibited by 6 at these temperatures (cf. Figs. 15 and 16 of Suppl.
No. 23, Math. Enc. V 10) is not given by any of these assumptions.
It can well be that the peculiarity ascribed by KaAMERLINGH ONNEs
to the helium afom at low temperatures is also present at these
higher temperatures, so that one would have to assume the helium
atom to be compressible, or to assume a relatively large increase in
the attraction (cf. also note 4 on this page.

Moreover, the points for the lowest three temperatures cannot be
regarded as known with the same degree of certainty as the others.

From both these circumstances it follows that the moving of the
helium diagram over that for rigid spheres with an attraction potential
—1—! (y = const.) can be made to take place in a manner toa very
large extent quite arbitrary. Fig. 2 shows a superposition for the
case g=4. In this the point log 77—1,3, log By = 6,5 — 10
coincides with the point log ve = 9,478 — 10, /, = 9,688 — 10.

With the exception of the highest temperatures *) the coincidence is

1) The data given in note 1 p. 645 for the superposition in Fig. 1 would yield
v = 2.68.10—l for g =5.

2) Cf. also C. BRAAK, loc. cit. p. 645 note 2.

3) The individual virial coefficients for He are taken from Table JL of Comm.
No. 1024 by KAMeRLINGH OnNes; these are supplemented by the virial coefficients
for — 252.072 and — 258.°82 U., which have not yet been published but have
kindly been placed at my disposal by Prof. KAMERLINGH ONNEs (they have already
been used for the construction of Figs. 15 and 16 of Suppl. No. 23) and also by
the value for 4.929 K. taken from Comm. No. 119 § 5é.

4) At these temperatures Prof. KAMERLINGH ONNEs tells me there is some uncer-
tainty ; improved values are being obtained.

645

not to be regarded as wholly bad, so that at the lower temperatures
‘below —- 100° ©.) the experimental results at present available for

6,0 AI ie
oo Mefum.
20) | |
55 AA ? i f Log J)
0,0 45-10 9,0 HOG 4. V

helium are, as far as / is concerned, compatible with the assumption
of rigid spheres of central structure with an attraction potential
proportional to —7r +.

Having now reached the end of the considerations advanced in
Suppl. N°. 24, 25, and 26 it is my pleasant duty to thank Prof.
KAMERLINGH ONNES for having invited me to participate in the inves-
tigation of the second virial coefficient for gases of low critical
temperature, which he had undertaken with the object of reaching
some conclusion regarding the structure and mode of action of the
molecule, in particular with the help afforded by the application
of BonrzMann’s principles, and also for his kindness in leaving to
me the continuation of the investigation within the particular region
which I have treated in this series of papers.

649

Physics. — “On the’ Haus effect, and the change tit resistance in
a magnetic field at low temperatures. IIT. Measurements at
temperatures between +-17° C. and —200° ©. of the Hawn
efiect, and of the change im the resistance of metals and alloys
m a maynetic jield”. By Bexet? Beckman. (Communicated by
Prof. H. KAMERLINGH OnNkEs). Communication No. 130a from the
Physical Laboratory of Leiden.

(Communicated in the meeting of September 28, 1912).

§ 1. Lntroduction. A communication was nade by KameruNcu
Onnes and the present writer to the meeting of June 29th 1912, of
the results of measurements of the Hatt-effect and of the increase
of resistance in a magnetic field made by us at liquid hydrogen tem-
peratures. In the present paper those results are extended fo the tem-
peratures which are obtainable with liquid ethylene and_ liquid
oxygen, with the same experimental material and following the same
experimental methods. It is of great importance that observations made
‘with any particular substance should be distributed as uniformly as
possible over the region of temperature under investigation. The
measurements now completed make it possible for the results obtained
ai liquid hydrogen temperatures to be compared with those of former
experimenters, who, without exception, proceed only to liquid air
temperatures.

For a description of methods and material we may refer to the
above Communication N°. 1292. In order to complete the diagrams of the
present paper the results for liquid hydrogen temperatures in the
paper quoted are also indicated without making specific mention of
the fact on each occasion. The present paper is confined to a diseus-
sicn of the results obtained with bismuth.

I. Bismuth.

§ 2. Change in the resistance of a wire of electrolytic bismuth. The
resistance of the bismuth wire 4/7; was measured in eight different
fields at tive different temperatures: 7 = 290? Kk, 170° K, 139°.5
kK, 90? K, 72° K. These results are given in Table I. // is the field
strength in gauss, w’7 the resistance in olms in the magnetic field
at the absolute temperature 7, 7 the resistance without field at that
temperature, and 7, the resistance without field at 0? C.

Fig. 1 shows the increase of resistance as a function of the field
at constant temperature (Isotherms), and fig. 2 the increase of resis-
tance as a function of the temperature under constant field (Isopedals).

650

TAA CB ee

Resistance of Bi yy as a function of the temperature and of the field.

| \| |

H H T= 290°. =e | T = 139°.5 T= 90° T= r°

| .ain | Z | |
| Gauss |) w’ | — tot) ee ante th taeol et Seas | ws
Wo Wy | Wo | Wo

0 2.570) 1.057 1.570) 0.646 | 1.365) 0.562! 1.075 es! 0.989, 0.407
2160 || 2.770) 1.140), 2.366) 0.973); 2.571 1.058 || 3.92 | 1.613) 4.68 | 1.926

}
|

5540 3.110) 1.280 3.657 1.504!| 4.414 1.816. 9.24 | 3.80 [12.28 5.052
7370 ||3.473/ 1.388) 4.612 1.897, 5.894 2.425 14.20 | 5.84 /19.10 7.86
| 9200 | 3.635) 1 495 | 5.613 2.310. 7.605) 3.128 ||19.74 | 8.12 126.6 10.94 |
| 11850 || 4.002| 1.646 7.299 3.003 10.56 4.346 | 29.82 |12.27 \41.2 (16.95

| 13600 4.248 1.746 8.506 3.500 12.596 5.180 38.60 15.88 '52.4 21.6
| 15670 | 4.540 1.868 10.204 4.199 15.51 6.380 48.05 19.77 61.2 27.65 |

17080 || — | — |{11.412)4.695;/17.78 | 7.316 | 55.80 22.96 17.8 32.0
| | | |

In Table HH are collected some results obtained by different
experimenters for the increase of resistance in a magnetic field. It

SA REO Neo eae Se Ra .
contains values of —~—-and——- in a field of 16 kilogauss at the
W 9730 K w

temperature of liquid air.

LA eds old

Increase of resistance in a field of 16 kilogauss.

Observer

0.42—0.44 81°K. 13.3 BLAKE !)
— 81° | 18.3 BLaKEe:5b |
=o 83? 23.8 Du Bois and WILLS 2)

90° | 20.9
0.43 | BECKMAN
2. 18a
0.36 88 ° Bye DEWAR and FLEMINGS)

1) P. CG. BLake: Ann. d. Physik. 28, 449, 1909.
*) H. pu Bors and A. P. Witts: Verh. d. Deutsch. Phys. Ges. 1, 169, 1899.
°) J. Dewar and J. A. FLeminG: Proc. Roy. Soc. 60, 72, 1896 and 425, 1897.

651

Fig. 1 and 2.

The measurements by Dewar and FLEMING give the largest results for

we! ‘ WE30 K
— and at the same time the smallest results for —. They
Uw, #2739 K

were probably obtained with extremely pure material. BLake worked
with a large number of different bismuth wires. One of these, labelled

ant

54, gave a larger value for — than the others tor which he gives
Ww,

| a mean value. The wire with which I worked gives exactly this

652

7
nea , but a greater value for Bae at the tempe-
W2730 K Wy
rature of liquid air. At higher temperatures there is also agreement
between BLAke’s values for the latter ratio and mine.

The maximum in the isopedals found by Brakn to lie at 36600
gauss at the temperature 7 = 99° kK. and which, for lower tempe-
ratures, ought to be found at lower fields, was not observed in the

present experiments.

mean value for

In the weaker fields the isotherms are convex towards the axis
of abscissae; from 12 Kilogauss upwards they become straight. For
H > 12000 the relationship

ee dd SD oh eee” 1 ee (1)
holds, where a and # are constants, while, at lower temperatures
i aeer 2 Pek ee

to a first approximation. The following Table shows to what degree
of approximation this relationship holds.

TABLE III.

a for Bi gy
sf a | a
obs. | “calc.
170 1.94 1.95

90 18.3 17.1
72 29.7 21.9
20 iS 7| 114
15 121 131

Even at the boiling point of oxygen @ is already clearly negative
—- 26.5). As the temperature falls the absolute value of 4 increa-
ses rapidly, and at hydrogen temperatures it reaches the value — 110.

§ 3. Vhe Haut. effect and the increase of resistance of plates of
compressed electrolytic bismuth. Tables 1V and V contain the results
of measurements made at ordinary temperature and at two liquid
oxygen temperatures with the plates Bi, and Li,y. R is the Han

0°S?

PG b'6l GS
£°S? co 61 L’ GV
£'? 0°61 L°S¢
=") Sool 6°l
= C012 6°8

— | o¢‘9z2 | c0I1X<8'0

ot Fd
co O61
961
9° 601
Leah
c0LXE' S

0) ik 2) i
09"S” «| S36

cP 9

lee 0

U B 60Z00'0 = 8m
| ;

= = me | Ost |¥8's | Vl 9°aP
| GPF €¢ Q°ZPI || GPT | 80°F 6°0 © OP
LPI Z LI L°SOl | 61 rob 0 g£0
aie cote ges || tet | PI's! el 162
PSI L'S Geo || ZI°t |90°9 10 6°02
| ¢z'1z \sotXo"e | c0lX<erer || 90'T |SL°9! eOIXZ'O \c01X6'SI
Era!

See are: He a \¥-| @ Hel

‘Al

006 = L

gq joj o8uvyo aourysisar pur ArjutuAse

da Tav i

Yoyo TIVE

0686 = L

0906

654

;

2060
3450
5660
7160
8520
9880
11090

12090

18.7103, 0.1108

28.2
39.8
46.1
52.1
59.9
59.9

62.8

Wog90

T = 289°
D oR ea
9.08 1.023
Q.1 8.17) 1.057
0.2 | 7.05) 1.108
0.2 | 6.44) 1.148
0.4 | 6.12) 1.186
0.1 5.66) 1,222
0.4 5.41) 1.260
0.7 | 5.19) 1.287

= 0.00889 49

TAL BeE Eran,

HALL effect, asymmetry and resistance change for

110.7
155.2
185.8
214.2
243.0
267.3

288.0)

| 74.3><108) 0.9>X103) 36.1

1.5

Wago

T=90°

—R

Oe, 1
27.4
25.95
(toa Te
24.6
24.1
23.8 |

= 0.00444

Bi pI
T = 713°

RH D —R
94.4><103, 1.3>X103, 45.8 |

139.5 | 3.5 | 40.4

205 8.5 36.2
248 13.7 34.6 |
289 16.5 33.9 |

330.5 20.5 33.5
367 24.2 68.15]

0.76
0.73
0.75
0.78

0.82

2.355
Rae
| 3.255
3.718
4.12
| 4.483

coefficient in) (. GS.
quantity

B55

D is the asymmetry and

0 2000 4000
raster C

8000 10000 12000 14000Gauss

Fig. 3.

Q is the

Figs. 3 and 4 show the resistance increase, and fig. 5 the Han.
effect as functions of the field for various temperatures ').

The isotherms of the magnetic increase of resistance are of the
same nature as those for /a;, but the rectilinear portion of the
curve now begins at 7 kilogauss. Equation (2) also holds in this case

Ed
1) Remembering that RH = - where E is the HAuw potential difference, d the

thickness of the plate, and J the main current, we see that RH is the HAL

potential difference for d=1 ard J

656

for the rezion 90° K< 7>>15°K. This is evident from Table VE
The diminution of the resistance at low temperatures without a
magnetic field is practically the same for both bi,; and Biaz.

90 1.69 |. 1.77. ))°90° | 29.3 ).31

2.55 || 13? | 35.8 | 34.4
20.3) 9.2 1 9-1 20°.3) 47.3 | 47.3
14.6 48.3 49

657

In Jiquid air the magnetic increase of resistance, however, appears

to be much greater for Bia), just

liquid hydrogen *).

as was found to be the case in

40% 4
wor -G-0. — : — 2
| j
| |
‘s) ale | "
$00 A Pee a | oe
t | de | 446
| ! i
- ‘ {
106—-— 9 Biryoy : ie ‘
; I-40
ae) ie
5 F169
600 — : ~- {46-5
\ XM
erm i
} } fis
500} pea 5) we ae a
|
| a
; Aue 28! |
400 — f{——.——L £ 4 : —1.,
| | ee | ti
| i Ma ae : wa |
of fel Vi } es |
300} a st Pe
A LAH ees oe 90°0
pif ya ys iG \
ey ay, | yi LA :
fer. Agee ale A ae
LO ae > a ge IAS
: eae | poe a | wa ao |
Wr wee eel GeO
100 | ft a a OL. t
| es ao ei, | ee eas
sd if Le ee eae eae
fe) ee pare
ee! 5005 7501) 1000% 42500 Goues
— of
Fig. 5
For H = 11090 we find at
Big Bi] Bi,
dd P p
° w! ¥ rs -
eA 2 IE == 11-6 1,0 3,20
w
0
: : w'
ft == 20.3 IC a 19,7 4,7
. w

For Bi, the resistance temperature coefficient with no magnetic
field is negative, which undoubtedly points to the presence of impurity.
At 7 = 289° K the specific resistance of 7,7 is about 1,5 x ‘Lite
and for Bi,7; 2,3 < 10° C.G:S.

\) H. KamertincH Onnes and Benat Beckman, Comm. N°. 129a

Proceedings Royal Acad. Amsterdam, Vol. XY.

658

The magnetic change of resistance is much smaller for Bi,1 parti-
cularly so at low temperatures.
Just as in the experiments in liquid hydrogen, for H > 3000, RH
becomes a linear function of the field
RH =a BA aw se ee eee
Following J. BrcquereL') we may regard the Hatt-effect for
bismuth as resulting from two components. One of these is propor-
tional to the field, and was always negative for the plates (5z,7, 52,7) I
used. The other is constant or, as one may say, saturated, for these
plates from H = 3000 upwards.
Within the temperature region
20° Ke 2ew la we
a’ can, to a first approximation, be satisfactorily represented by
a =asenPhi as eh ee eee (4)
The agreement for 7—= 90° &K between observation and calculation
from (3) with a’ = 20.6 and 6'= 39,3 < 10° for the plate Bz,77 is
exhibited in Table VII, while Table VIII shows how far the relation-
ship (4) holds.

TASS VIL

Linear variation of the HALL effect
in strong fields for
Big] Ate a —O0C ee

a RH ops, RA atc.

3450 110.7103) 110.4 103

5660 | 155.2 155.8
7160 185.8 186.8
8520 | 214.2 214.8
9880 243.0 242.8
11090 | 267.3 267.8
12090 —- 288.0 | 288.3

The constant 4’ which gives the value of the second component
of the effect in the state of saturation is commonly negative. Only
for 57,; at hydrogen temperatures does it become positive. With

1) J. BecQUEREL: C. R. 154, 1795, 1912.

659

Bin U' is almost constant for 7< 90°; with bi b' is very small
and for 7’ > 72° K is practically constant.
In strong fields the constant R approaches a limiting value in

TAB YT. By Va.

| 90° 12 AR 12:1 |) 90°? 4)206 | 22-0
|
| 74.5) 17.7 PTA 189 20:8 | 27.6

| 20.3 | 62.1-| 62.6 |] 20.3 | 54.3 | 57.3
| | |
| 14.6 | 64.5 62.4 |

accordance with equation (3). In weak fields RH for Bi,,, is in-

versely proportional to the temperature at 7 — 289° K, 90° _K, 74°,5 K.
: D

Tables IV and V also contain the quantity Q—=——. For

ie fal

HT> 7000, Q is either a linear function of the field, or a constant’).

Physics. — “On the Hat effect and the change in resistance
in a magnetic field at low temperatures. IV. Measurements
at temperatures between ae 17° C. and — 200° C. of the Haun
effect, and of the ee in the resistance of metals and alloys
in a magnetic field.” By Berner Brockman. Communication
N°. 1300 from the Physical Laboratory at Leiden. (Communic-
ated by Prof. KAamERLINGH ONNEs).

(This Communication is a continuation of Comm. N° 130@ in
whieh the behaviour of bismuth was discussed.)

Il. Gold, Silver, Copper, Palladium.

§ 4. Ua effect for Gold. From the temperature decrease of the
wT=20 Se
— = 0,035, it is to be sup-

WT7=290
posed that this plate is composed of purer gold than that of the wire

resistance without magnetic field *),

1) Cf. E .v. Everpincen, Leiden Communications Suppl. no. 2. p. 57.
2) H. KAMERLINGH ONNES and Benat Beckman.; Comm. N°. 129a.

45%

-
660 |
Au, of Comm. N°’. 99, which was known to contain 0,03 °/ impurity.
The thickness of the plate was 0,101 mm.
TABLE IX.
Hatt effect for Gold Au, I: )
T = 290° K. T=90°K || T=TIPK
H RH —Rxi08 H | RH —Rx108 H | RH —Rxt04
| | |
7130 | 5.62 | 7.27 || 7130 | 5.82| 7.53 || 4940 | 3.75 | 7.59 .
9500 6.75 7.11 9500 7.24 7.62 9065) 6.95 7.67
11080 | 8.11 | 7.32 ||/11080 | 8.53 | 7.70 ||10270 | 7.72 | 7.59
12200 8.85 7.25 12200) 9.24) 7.58
| 1}
| i
§ 5. Hawt effect for Silver. The plate Ag,; was found to be of
practically the same purity as that of the wire Ag, of Comm. N°. 92
which contained 0,18°/, impurity. The thickness of the plate was ;
0,096 mm. ;

TABLE X.
HALL effect for Silver Ag, I:

!
ee K. T = 90° K.
H RH —Rx10# RH = —Rx104 |
IH | /

4940 3.97 8.04 | 4.10 8.30 .

7260 | 5.81) 8.01 || 5.92 8.15 | |

9065 | 7.23) 7.98 || 1.45 8.22

10270 | 8.16) 7.95 8.28" he
| |

Woo90 = 173 x 10-5 Wo90 = 37x10 n

§ 6. Hari effect for electrolytic wi oan The thickness of the
plate Cu,, was 0.057 mm,

661

| TABLE XI,

HALL effect for Copper Cu pr
T = 290° K. T=S902K.
H = ee eS — — a ——
RH — Rx 104 RH | —Rx104
_ -— a Lea 4) —s
7260 || 3.59 | 4.95 | 4.05 5.58
9065 | 4,42 4.87 5.04 5.56
10270 5.08 4.95 5.66 5.5]

§ 7. Hawi effect for Palladium. The thickness of the plate was
0,100 nm.

TABLE XII.
| Hatt effect for palladium Pay y-

T = 290° K. | T=90°K.

H | RH |—Rx 104 H RH —Rx 104

8250 5.61 | 6.80 8250 | 5.85 | 7.10
9065 | 6.04 6.66 9065 | 6.35; 7.01
9760 | 6.64 6.80 9760 | 6.77 | 6.94

10090 | 7.06 | 7.00

§ 8. Summary of the variation of the Hari. coefficient for different
metals. The results obtained in § 4—7 are collected in Tables XIII
and XIV. For R is taken at each temperature the mean of the
values‘) for the different fields.

1) It has not been possible to determine the thickness of the plates with a
greater accuracy than about 3°/), which of course influences the absolute values
of the Hatt coefficients. This inexactitude, however, makes no difference as to the
temperature coefficient of the Hatt effect, the measurement of which has been the

principal object of this investigation.

662

TABLE al
HALL coefficient R.

ar: A ‘pI ASp] Cus) Pay |

290°K. 7.24 10-4 8.00 10-4 4.92 10-4) 6.75 & 104 |

igcuee 7.61 8.21 5.56 6.99
77° 7.62 = -— | — |
TABLE XIV.
Variation of the HALL coefficient es
290°K
= Ss | :
= Be cael :
290°K. | 1 I Pie epee >
90° 105 | 1.02 | 113 | 1.035 |

77° 1.05 aa Sf TA Fe

From these observations, therefore, the Hatt coefficient for Azz,
Ag and Pd is almost constant from ordinary temperature down to
that of liquid air. A distinct increase is first observed on proceeding
to hydrogen temperatures‘), which amounts to 25—35 °/, for Gold,
Silver and Copper, and 100°/, in the case of Palladium.

: <<
A. W. Sirs?) gives the following values for the ratio

Au Ag Cu Pd
1.03 1.095 1.205 1.27

This gives agreement in the case of Aw, but with Ag and Cu,
and particularly with Pd, Smirn’s results deviate considerably from
mine. In the case of Cu and Ag the lack of agreement may perhaps
be ascribed to the presence of impurity.

The relationship

293° K

on
R, = ——
; SNe

deduced for the Hai effect by R. Gans*) has been utilised by

1) H. KAMERLINGH OnNnES and Benet BeckMaAy, l. c.
®) A. W. Smita, Phys. Rev. 30. 1. 1910.
8) R. Gans, Ann. d. Phys. 20. 293. 1906,

668

J. KognigsBerGer and J. Weiss*) to obtain the variation of the electron
density (V) from the temperature coefficient of the Hai effect. From
this relation it should follow that the density of the electrons in Au,
Ag, Cu, Pd varies very slowly with the temperature, much more
slowly than V 7.

WI. Alloys.

§ 9. Gold-silver. The: alloys investigated contained 2°/, of silver

by volume.

TABLE XV.
HALL effect for a gold alloy.

| | T= 290° K. T= 90° K,

H }

| RH | — Rx 104 RH — Rx 104
8250 || 5.58 Gl UP 5.40 6.54 |
9065 ~=—«-6..18 6.82 6.01 6.63 |
9760 | 6.61 6.77 6.44 6.59
10270 ||), 6-94.) |: 6.76 - || 6.86 6.67

0 : Woq90 = 3.81 x 10-4 9 Wo90 = 1.77x 10-40

Hence the mean value of F is for
T= 2902: - tn 6134 10-4
90° i= 6.61
The hydrogen experiments gave *) for
T=20°3 K R=669X 10-4
E145 R= 6.48

Hence the Hatz. coefficient for this alloy is almost constant; on
proceeding to low temperatures it begins to exhibit a slight decrease.

1) J. KorniasBperGer and J. Weiss, Ann. d. Phys. 35. 1. 1911.
2) H. KamMERLINGH Onnes and Benet Beckmay, l. ¢.

664

Physics. — “On the Hatt effect and the change in resistance in a
magnetic field at low temperatures. V. Measurements on the
Haut eject for alloys at the boiling point of hydrogen and
at lower temperatures.” By H. Kameriincu Onxes and Brnor

BeckMAN. Communication N°. 130° from the Physical Labora-

tory at Leiden.

VI. Gold-siver alloys.

§ 16'). In § 12 of Comm. N°. 1297 observations on the Haus
effect for an alloy of gold and silver (Au-Ag), with 2 atom °/, of Ag
are published. We now give the results of our measurements on two
Au-Ag alloys, containing greater percentages of silver.

The alloy (Auw-Ag),, coniained 10,6 atom °/, of silver”). The
thickness of the plate was 0.049 mm. The Hatt effect was measured
at the temperatures 7’—= 290°, 20°,3 and 14.5° K.

We found:

T ABLE oa
| The Hatt effect for (Au—Ag),7
P
T = 290° K. T=0°93K | T= 14.5° K.
H | 7 hee
RH ial RH | Rx 104} RH = —Rx104,
= EO as Be. — tes = \ |
8250 4.59 5.57 || 3.07 3:72 -|[- 6-04 3.69
9360 || 5.47 5.61 3.47 3.11 | 8523 ee
10270 || 5.70 | 5.55 | 3.82 | 3.72 N= 2:88 <1" Bag
‘ ll uN |
|| w= 8.06x 10-4 9 | w= 4.58x 10-40 Pere
|e wh = 0.585 | = 0.58
| Wo || 0 | 0

The alloy (Au-Ag);;, contained 30 atom °/, of silver. The thickness

of the plate was 0.078 mm.
We found:

1) The sections of this paper are numbered in continuation of those of Comm.
N°, 129c. (Sept. ’12).
4) The exact analysis being made now the composition is given in atom %,

FRELE RVI.
The HAL effect for (Au—Ag) WI

T = 290° K T=20°.3K T=15°K
H ey ee eee '
| RH |—Rxict|| RH |—Rx104\)) RH |—Rx104|
8250 || 4.62 | 5.60 3.00 3.64 3.12 3.78
9369 | 5.23 5.59 3.30 3.53 3.42 3.66

—
i—)
bho
—!
Oo
or
rn
—!
or

53 3.713 3.63 3.81 3.71

Uv Wo Wy

The results of measurements on gold and on the three gold-silver
alloys are brought together in the tables XVII and XVIII.

LASS L EXVIL

The HALL coefficient for gold and gold-silver alloys.

E Aus) (Au—Ag), (Au Ag) | (Au—Ag) 77

290° K | 7.2x10—-4 | 6.8x10—4 | 5.6x10-4 | 5.6x10—4
|
| 20:3 9.8 6.7 Peg 3.6
| atSse | 9.8 | 6.50 ag ST

T-ASE, XVUE.

FF
Change of the HALL coefficient Fas ae cooling
290°K.

to and in the region of liquid hydrogen temperatures,

sige] 3 |
1% 1 Atty (Au—Ag), |(Au— Ag); 7 (Au--A8)
2909K. | 1 } 1 ee | 1
20.3 1.355 | 0.985 | 0.665 | 0.646
15 | 1.355 | 0.955 | 0.665 | 0.667

T=20 a ae .
Thus, ———— diminishes by greater percentages of silver. For pure
T=290

666

gold Ry=203 > Rr=es0, but for alloys with more than 2 °/, of silver
by volume Ry—s03 << Rr=290.

The curve that represents the relation between the Hatt coefficient
R720. and the percentages of silver is of a shape analogous to that
representing the conductibility or the temperature coefficient of the
resistance as a function of percentages of silver. The curve for
Ry—203 at first descends very rapidly for small admixtures of Ag;
at higher concentrations it becomes flatter.

The Hats coefficient Rz—s0.3 is approximately a linear function

ie ;
of the quantity “="" for alioys with less than about 8 °/, by
OT 973
volume of Ag.

The Hau. coefficient /7—se9 diminishes too, though much more
slowly than R7=20,3, when the percentage of Ag increases.

Physics. — “On the triple point of methane’. By C. A. CRoMMELIN.
Comm. N°. 1316 from the physical Laboratory at Leiden.
(Communicated by Prof. H. KAMERLINGH ONNES).

The measurements made by Prof. Maruias, Prof. KAMERLINGH ONNES
and myself on the diameter for argon’) afforded an opportunity
of determining the pressure and temperature of methane at its triple-
point. For, when the cryostat was filled with liquid methane, and
the pressure was reduced so as to give a temperature of about
—183° C. the methane was covered with a solid crust. A slight
increase of the pressure caused the solid methane to spread itself in
small pieces throughout the liquid. While these pieces were kept in
constant motion through the liquid by means of the stirrer, the
following triple point constants were observed :

t— — 183.15 K. p=71 Cem.

On account of the manner in which these figures have been determined
they must be considered to be very accurate.

As far as I am aware there has hitherto been only one other
determination of these data — that of Oxtszewski 7) — who found

t= —185.°8 and p=8.0 em.

*) Comm. No. 131a.
*) K. Ouszewski, GC. R. 100, page 940, 1885.

66%

Physics. — “On the rectilinear diameter for aryon. By E. Marutas,
H. Kamertincn Onnes and C. A. Crommenin. Comm. N°. 1314
from the phys. Lab. at Leiden.

§ 1. Introduction. The present paper forms. a continuation of
the investigation of the diameter for substances of low critical tempe-
rature with which a beginning was made with oxygen.') The
importance of this and of similar investigations was indicated in the
introduction to the Communication referred to, so that we need not
discuss the point further here.

We chose argon for the present investigation since the isotherms
for that gas had already been determined to within the neighbourhood
of the critical point, while the critical pont itself, the vapour pres-
sures and even preliminary values of the densities of the coexisting
vapour and liquid phases were aiready known ®*) the monatomic
nature of the gas, moreover, will undoubtedly enhance the value of
the results.

§ 2. Apparatus. The apparatus was essentially the same as that
employed in the investigation of oxygen. The arrangement for com-
pressing the argon and also the volumenometer have, however,
undergone some modification since that time, so that it seemed
desirable to take this opportunity of publishing a new diagram of
the whole apparatus (Fig. 1).

The modifications of the volumenometer and of the auxiliary
apparatus belonging to it have already been described in full detail *).

The use of such a costly gas as pure argon necessitated, however,
a completely new arrangement of the pressure connections. The
copper tubes of which all the connections were made were chosen
as narrow as possible so as to reduce the quantity of gas in the
dead space to a minimum. The argon was contained in the steel
cylinder A which was completely immersed in oil; so too were
all the taps and coupling pieces which contained compressed gas. *

Through the taps C,, and C\,, the gas passes to the spiral Sp;

1) Proc. Febr. 1911. Comm. No. 117. G. R. 151, 213 and 477, 1910,

2) Proc. May 1910, Comm. No. 115, Proc. Dec. 1910, Comm. No, 118, G. A,
CROMMELIN, Thesis for the doctorate, Leiden. 1910.

8) Proc. May 1911 Comm. No. 121la, Proc. Sept. 1912 Comm, No. 127¢ and
W. J. De Haas, Thesis for the Dociorate, Leiden 1912, in which diagrams of
the modified volumenometer are also given. Certain small errors in these diagrams
make it desirable to publish a diagram here in which these errors are corrected.

4) Proc. June 1905 Comm. No. 94). The value of this device for the detection
of leaks has already been repeatedly emphasized

Ky
rie — ee eae
Ry, a rs Ce (( a -
On
ie ‘A I Wy
yo} cos 1
aN :
Ran ~) Ww, a
} fie
re | Ons\ wnt
. Oe
f
5H
: (
, al:
INC, 4

Fig.

=
.

669

here the argon is dried by immersing this spiral in aleohol and
cooling it down to its melting point by means of liquid air. Through
k, and ’:,, the gas then reaches the compression tube A, within the
compression cylinder A,'). In this compression tube the mercury is
forced by means of compressed air from the steel cylinder B; by
this the required amount of argon is compressed into the dilatometer
on closing the tap /, and opening /, and /:,. This arrangement for
compressing pure gases has already been fully described in previous
Communications *); moreover, its mode of operation is easily seen
from the accompanying diagram.

Through the tap C), it was possible to establish communication
between the air compressor and our accurate closed hydrogen mano-
meter *), and by this means we were able during the actual measu-
rements to obtain a few further determinations of the vapour pressure,
which will be published shortly. .

The cryostat Cr was the same as that used in the investigation
of oxygen, the sole modification being the introduction of a different
type of stirrer, Ag, provided with valves. *).

As the appendix of the dilatometer formerly used was found to
be too narrow, another dilatometer Di/, very accurately calibrated,
was employed with an appendix sufficiently wide to allow of the
suitable measurement of the small volume of the liquid coexisting
with the vapour.

A GAEDE vacuum pump was used, and we found it of the greatest
utility, particularly during the actual measurements, in ensuring the
continued absence of leaks,

Two platinum. resistance thermometers were introduced into the
cryostat to serve forthe regulation und measurement of the temperature.

The argon used for the present measurements was taken from
the same supply as that employed in the previous investigations
already quoted. The impurity in this argon is certainly less than 0.1 °/, °).

§ 3. Heperiments. We may now give a short description of the
sequence of operations involved in the measurements :

1) At the cylinder A is connected the glass manometer P, for high pressures
and of small volume, especially constructed for the use of such cylinders as reser-
voirs for the rare gases.

*) Proc. April 1901 Comm. No. 69, Proc. March 1907 Comm. 97a.

5) April 1902 Comm. no. 78, Proc. March 1907 Comm. no. 97a.

4) Proc. June 1911. Comm. no. 123.

5) For a detailed description of the preparation and of the analysis of this
argon see CG. A. Cromme.in, Thesis for the Doctorate, Leiden, 1910,

670

4. All the apparatus and connections were reduced to a high
vacuum and then washed out with argon.

2. The cryostat was filled with the liquid gas desired (O,, CH,,
or Crit),

3. The argon was admitted to the compression tube A, and then
pumped into the dilatometer.

4. The argon meniscus was adjusted to the upper part of the
stem of the dilatometer, and the tap 4, was closed.

5. When the temperature is constant the position of the argon
meniscus is read, the temperature is measured, and also when requi-
red, the pressure registered by the hydrogen manometer.

6. By reducing the pressure in the eryostat transition is made to
a lower temperature, the same measurements are repeated; a lower
temperature is then installed and so on until the meniscus has sunk
below the subdivided portion of the stem.

7. Sufficient argon is then allowed to escape into the volumeno-
meter to bring the meniscus to the lower part of the appendix
below the dilatometer ; the temperature, pressure and volume of the
escaped gas are measured.

8. The measurements of 5° and 6° are repeated in the reversed
order of temperature until the meniscus reaches the upper part of
the appendix.

9. The argon still remaining in the dilatometer is transferred to
the volumenometer, and the measurements of 7° are repeated.

It is clear that these measurements yielded the data requisite for
the calculation of the liquid and vapour densities at all the experi-
mental temperatures. To these calculations we shall return in the
succeeding section.

The dimensions of the dilatometer were so calculated that one
could finish off the temperature range for any particular substance
by successive measurements; in this way only two measurements
with the volumenometer were required to give both the liquid and
vapour densities.

§ 4. Calculations. In many respects the calculations were made
in the same way as those of Comm. No. 117. It was of great
advantage to us that so many data are already available for argon,
and that we could already make use of the reduced equation of
state, VII. A. 2&.'). We shall, however, here give a short summary
of the method adopted in the calculations.

Working from the very accurate calibration of the dilatometer,

1) Proc. June 1912, Gomm. no. 128,

671

the liquid volumes were first calculated directly from the positions
of the meniscus top in the stem and in the appendix, without
applying any correction. To the numbers so obtained the following
corrections were then applied:

1. A fairly large correction for the diminution of the volume at
low temperature, seeing that the calibration of the dilatometer had
been reduced to + 20° C.; the correction was obtained by means
of a formula from a former Communication

2. A correction for the increase of volume due to the pressure,
For this correction, which was so small as to be negligible in almost
every case, approximate values were calculated from data contained
in two previous Communications ”).

3. A correction for the volume of the argon meniscus. KELvin’s
graphical method *) was employed for the evaluation of this by no
means negligible correction. To obtain the volume of the menisci it
was usually sufficient for our purpose to regard the surface of the
liquid as half of an oblate ellipsoid of revolution. Only at the higher
temperatures was it necessary to apply Gttpin’s theorem to the

KerLvIN diagram in order to determine the body of revolution.

1) Proc. Sept. 1906, Comm. no. 95b.

2) Proc. April 1902, Gomm. no. 78, Proc. March 1907, Comm. no. 97a.

5) The capillary constant for argon and its variation with temperature must be
known for the construction of these diagrams. Now Baty and Donnan (Journ.
of the Chem. Soc. Trans. 81. 907. 1902) have determined capillary constants for
liquid argon but only between — 189 C°. and — 183° C. so that the question
now arose as to how to interpolate in the most rational manner possible from
— 183°. C. to the critical temperature. A comparison between the results giving

the reduced capillary constant (see J. D, van DER Waa s, Cont. I. p.

W.
T)./spy'ls
176) as a function of the reduced temperature by Baty and Donnan (l.c.), for
argon, by DE Varies (Ziitingsversl. Febr. 1893, Comm. no. 6, and Thesis for the
doctorate, Leiden 1893) for ether, by VeRSCHAFFELT (Zilttingsversl. Juni 1895,
Comm no. 18) for carbon dioxide and nitrous oxide was fruitless, seeing that the
last three correspond well, while argon deviates strongly from them. A suitable
rational method is given by the assumption of the validity of the Eérvés formula
(Ann. d. Phys. und Chem. 27 (1886) p. 448) according to which the quantity

NE. 99
2 ( )e is a linear function of the temperature. According to BAty and Donnan
Yliq
te

M \?
we get for argon w-, r = 2.020 (145.44 — T); from this formula our esti-

Oliq
mates have been made except that for the highest temperature, + — 125° C., at
which one is so close to the critical temperature that the Eérvés formula no
longer holds, and for which interpolation was resorted to in correspondence with

the curves given by other substances.

672

Having thus calculated all the liquid volumes, we were able, taking
the first two of the above corrections into account, to obtain the
volumes of the saturated vapour. In this it was assumed that the
temperature of the bath extended to a distance of 2 cms. above the
surface of the liquid.

The following method was adopted of reducing the gaseous argon
in the glass and steel capillaries from the point of the capillary just
mentioned up to the tap &, to terms of the normal volume. The
portion of the glass capillary within the cryostat was divided into
different parts for each of which the mean temperature was known
from previous papers’). The temperatures of the part of the glass
capillary outside the cryostat and of the steel capillary up to the
tap &, were obtained from thermometers during the measurements.
The volumes of all these portions were known from the calibrations
and the pressures from the vapour pressures already published ”)
together with those added by the present measurements.

In order now to cbtain the normal volume of all these portions
at different temperatures we again make use of the modified series

pun = Ay {l + BO) p + Cp? 4+....}

J
—and Ay = Anoce. (1 + aad, it follows that

Since vy = x
+

pV
N SS ee eee
: Anorc (1 + aa t) (1 + BO) p + CO) p?]

The virial coefficients necessary for the employment of this
equation were taken from the equation VII. A. 3. In all these
calculations the coefficient C’) could be neglected.

We may again refer to previous papers *) for the corrections
which have to be applied to the volumenometric determinations.

For the normal specific mass of argon we used the value given
by Ramsay and Travers *) 0.001782.

‘)

1) C. Braak, Thesis for the doctorate, Leiden. 1908. p. 16,
2) Proc. May 1910, Comm. N'. 115.

8) In these formulae p is the pressure in atmospheres, vy the volume expressed
in terms of the normal volume as unit, N the normal volume, V the actual expe-
rimental volume and z,, the coefficient of expansion in the AvoGADROo state,
0.0036618. For the notation see also Suppl. No. 23.

4) Proc. May 1911, Comm N?® 121a. Proc. Sept. 1912 Comm. N°. 127¢ and
W. J. ne Haas. Thesis for the doctorate, 1912.

5) W. Ramsay and M. W. Travers, Proc. R. S. 67. 329, 1900.

673

We may further state that at the lowest three temperatures the
vapour densities were not measured but ealeulated: in view of the
degree of accuracy desired this is quite permissible. The calculation
was made by means of the above series in which, however, C'” is
now no longer negligible. (To be continued).

ERRATUM.

In the Proceedings of the meeting of September 28, 1912.

p. 415 1. 10 from the top: for 0.507834 read 0.057834.

(November 28, 1912).

r ®
‘
P 2
i = ~
e
<
~~
,
.
i a
>
sd *
.
a“
iw
nl
«
"
$
—_—

KONINKLIJKE AKADEMIE VAN WETENSCHAPPEN
TE AMSTERDAM.

PROCEEDINGS OF THE MEETING
of Saturday November 30, 1912.

a 6s

President: Prof. D. J. Korrrwna.
Secretary: Prof. P. Zeeman,

(Translated from: Verslag van de gewone vergadering der Wis- en Natuurkundige
Afdeeling van Zaterdag 30 November 1912, Dl. XXI).

Cera [Ea as ES.

A. Sits and H. L. pe Leeuw: “The system tin”. (Communicated by Prof. A. F. HoLLEMAy),
p. 676.

A. Sirs and S. C. Boxuorsr: “The phenomenon of double melting for fats”. (Communicated
by Prof. A. F. Horieman), p. 681.

A. Sits and A. Kerryer: “On the system ammonium sulphocyanate thioureum water”. (Com-
municated by Prof. A. F. HoLtteman), p. €83.

C. van WissELincGH: “On the demonstration of carotinoids in plants. Second communication:
Behaviour ot carotincids with regard to reagents and solvents’, p. 686. Third communi-
cation: “The leaf of Urtica dioica L., the flower of Dendrobium thyrsiflorym Rehb. fil.
and IIaematococcus pluviales Flot”. (Communicated by Prof. J. W. Moi), p. 693.

F A. H. Scurememakers: “Equilibria in ternary systems” I, p. 700.

J. C. Scuoure: “Dichotomy and lateral branching in the Pteropsida”, p. 710.

Hk. DE Vries: “On loci, congruences and focal systems deduced from a twisted cubic and
a twisted biquadratic curve” I, p. 712.

L. J. J. Muskens: “The posterior longitudinal fascicle, and the manege movement”. (Com-
municated by Prof. C. WiNKLER), p. 727. ‘With one table).

H. A. Brotwer: “On the formation of primary parallel structure in lujauritcs’ (Commani-
cated by Prof. MoLENGRAAFF), p. 734.

I. J. H. M. Kvessens: “Form and function of the trunkdermatome tested by the strychnine-
segmentzones”. (Communicated by Piof. WiNKLER), p. 740. (With one plate).

IL J. Waterman: “Action of hydrogenious, boric acid, copper, manganese, zinc and rubidium
on the metabolism of Aspergillus niger”. (Communicated by Prof. M. W. Beiserincn),
p. 753. (With one table).

ERNESTINE DE NEGRI and C. W. G. Mieremetr: “On a micro-organism grown in two cases
of uncomplicated Malignart Granuloma”. (Communicated by Prof. C. H. H. Sproncx), p. 765.
(With one plate).

J. F. Sinks: “Measurements on the ultraviolet magnetic rotation in gases”. (Communicated by

Prof. H. KaMERLINGH ONNES), p. 773.

44
Proceedings Royal Acad. Amsterdam. Vol. XV.

676

Physics. “The system tin’. By Prof. A. Suits and Dr. H. L. pg Lerow.
(Communicated by Prof. A. F. HOLLEMAN),.

(Communicated of the meeting of October 26, 1912).

As is known when molten tin is cooled down, the tetragonal modi-
fication deposits under ordinary cireumstances, which form was first
described by Mitiur') in 1843. This form shows a point of transi-
tion at 18°), below which the gray tin is the stable modification.

In the years 1880 and 1881 TrecHMANN *) and Fovurton *) disco-
vered moreover a third modification, viz. a rhombic one, which can
be formed when molten tin is exceedingly slowly cooled down, and
which is brittle.

It was now natural to assume that this form of tin forms at higher
temperature from the tetragonal modification, for it had been known
for a long time that tin heated to about 200° becomes 6rvitle, and
that in England this circumstance has been profitably used to obtain
the so-called corn tin or grain tin. In this process tin is heated to
some degrees under the melting-point, after which it is dropped from
a great height on a stone plate, on which the metal breaks up into
picces resembling basalt. The above-mentioned supposition was further
supported by observations by Katiscuer®), in which it appeared that
when tin is heated to about 200°, the aspect changes, and the metal
assumes the appearance of moiré métallique.

As Scuaum-) already observed these experimental data make the
existence of a point of transition at about 200° very probable, and
as the spec. gravity of the tetragonal and rhombic modification,
which amount to 7,25 resp. 6,55 at 15° differ pretty much, it seemed
the natural course to take to try and find this point of transition by
a dilatometrical way. Conen and GoLpscumipt’s’) experiments with an
oil-dilatometer, however, (in which ne difficulty was experienced from
any generation of gas) did not furnish the least indication for the
existence of a point of transition, for the expansion, represented as
function of the temperature, appeared to be a perfectly straight line
from 175° to 210°. Though these experiments had yielded a negative
result, already a year before Wertein, Lewkoserr and TamMANn *) had

't) Phil. Mag. (8) 22, 263 (1834).
2) ConEN-vAN Eyk, Z. f. phys. Chem.
3) The mineralogical magazine and Journal of the Mining Soc. 8, 186 (1880).
4) Verh. der k. k. geologischen Reichsanstalt 1881, 237.
Jahrb. der k. k. geologischen Reichsanstalt 1884, 367,
5) B.B. 15, 722 (1118),
6) Lieb. Ann. 808, 18 (1899).
7) Z. f phys. chem. 50, (1904).
3) Drud. Ann. 10. 647 (1908).

(4
found indications which seemed to point to a point of transition in
the neighbourhood of 200° in a determination of the velocity of
eftluxion of some metals, among which tin, at different temperatures.
Their results were the following :

temperature | velocity of effluxion

—_—_—————

162.8 0.6 + 0.3
173.4 1.74 0.3
183.8 3.9 + 0
193.5 8.2 + 0.1
203.8 12.1 + 2.1
204.0 3.2 + 0.3
214.8 ie
eG Ae 10-%-E 0.4
235.1 | 112.3

The above-mentioned investigators make the following remarks
about this result:

“Von Interesse sind noch die beim Zinn bei 200° deutlich auf-
tretenden Abnormalitéten in der Temperaturabhingigkeit der Aus-
flussgeschwindigkeiten. Beim Zinn fallt bei jener Temperatur plotzlich
die Ausflussgeschwindigkeit. Der Grund hierfiir kann nur in der
Bildung einer neuen Kristallart, also im Auftreten eines Umwandlungs-
punktes gesucht werden. Von Zinn ist bekannt, dass es bei 200°
sprode und pulverisierbar wird. Genauer sind diese Umwandlungs-
punkte hisher nicht untersucht worden.”

Why in reference to these experiments Conen and GoLpscHMiptT
give 195° for the point of transition in question in the ‘“Chemisch
Weekblad”’, and 170° in the Zeitschr. f. phys. chem. is quite unac-
countable. Their assertion: ‘“Bringt man die in Tabelle 4 (the above
table) gefundenen Werte in Zeichnung, so entstehen zwei Kurven,
welche sich bei etwa 170° schneiden, somit auf einen Umwandlungs-
punkt bei dieser Temperatur hinweisen’’, is decidedly erroneous, and
proves that they have not understood the significance of this curve.

In view of the fact that the experiments on the velocity of effluxion
render a point of transition at more than 200° very probable, it
was very desirable to get certainty on this point by another way,
the more so as the experiments about the velocity of effluxion refer

44*

to pressures of 500 kg. per cm’*. There was therefore every reason
to rejoice that Mr. Drerens, when revising his Thesis for the Docto-
rate: “Legeeringen van tin en lood” (Alloys of tin and lead) wanted
to make another attempt to find the expected transition between
tetragonal and rhombic tin in a dilatometrie way, though his prede-
cessors had only obtained negative results.

As Mr. Drerens found it impossible to obtain reliable results
with paraffin oil, which had been used as dilatometric liquid by
Conen and GoLpscHmMipT, in consequence of the generation of gas,
however slight, one of us (Smits) advised Mr. Drcens to use an
air-dilatometer with a twice bent capillary. To prevent any injuricus
decomposition of the dilatometric liquid, mercury was used by Mr.
Decens, {o include the air in the dilatometer, although in this way
there was, of course, a possibility that during the experiment, espe-
cially when it had to be continued for a long time, appreciable
quantities of gaseous mercury could be absorbed by the tin. Mr.
Drcens, bowever, expressly states that “it was never observed that
the metal was attacked by mercury vapours’’.

By the aid of this air-dilatometer Mr. Drcens really found an
iidication about the existence of a point of transition, viz. at 161°.

Siuce we have been occupied with the tin-problem, we have begun
to mistrust this temperature, because different phenomena led us to
expect a point of transition at + 200°. And as it seemed very
desirable in connection with the already partially published investi-
gation about the system tin, to know the exact situation of the
point of transition between tetragonal and rhombic tin, an investi-
gation was undertaken also by us to determine this point dilato-
metrically.

When we repeated Mr. Drcens’ experiments we found first of
all that by this way of procedure a point of transition can really
be demonstrated, but that in successive experiments this point of
transition descended. This pointed to an absorption of gaseous
mercury by the tin during the experiment. On investigation of the
tin used it appeared clearly that the tin contained appreciable quan-
lilies of mercury, which to our great regret condemned Mr. Drcsns’
method. We regretted deeply that we had to come to this conclu-
sion, particularly because Dr. Degens was known {o one of us
(Smits) as a man full of enthusiasm for his work, who carried out
his investigations with great experimental skill, in the conviction of
having left no means untried to test the validity of his results. In
this case, however, he has been mistaken.

In order to’ take the experiment in such a way that the results

679

obtained were entirely reliable, we turned back to the ordinary dila-
tometer, and tried to attain by means of the oil of the vacuum pump of
GorpE, which seemed to be very suitable as dilatometrice liquid, that
no generation of gas took place at temperatures up to the melting-
point of tin. By thoroughly boiling the oil in the vacuum of the
pump, by then allowing it to flow into the dilatometer vessel, and
afterwards heating the whole 20° above the melting-point of tin we
managed to prevent any generation of gas even above the melting-
point of tin *).

With the dilatometer filled in this way curves of expansion and
of contraction were determined as accurately as possible by putting
the apparatus in a thermostat with oil resp. a molten mixture of
KNO, and NaNO,, by raising the temperature every time 10°, resp.
lowering it, and by then reading the position of the oil tevel after
15 minutes. Though the obtained lines have not appeared to be per-
fectly straight, as Coney and Gonpscumipr found, yet no indication
of a point of transition was to be detected. As according to Mr. Drcens’
method, by the same procedure a point of transition was found
for tin containing mercury the mercury seemed to be a positive
catalyst for the conversion in the point of transition. In connection
with this we proceeded to the determination of the transition point
of tin to which small quantities of mercury had been added.

In this it was not only found that for every mixture very clearly
a transition point occurred, but also that the transition peint was
greatly lowered by mercury, which is in accordance with the slight
heat of transition.

We found :

at. % Hg
of the mixture

= -

|
| transition temperature
| |

1 | 0.12 | 173°
2 0.22 | 151°
3 0.34 133°
4 0.49 133°

The third and fourth determinations point to the existence of three-
phase equilibrium, which is also in harmony with this that the transition

- 1) Not to lose the oil during the heating up to this high temperature, the upper
end of the capillary was provided with a wider yessel,

680

points 8 and 4 do not lie on the line drawn through 1 and 2%).

If we use the first two observations to extrapolate to the compo-
sition 0 atom °/, Hg, which is, of course, a rather inaccurate method,
we find 200°,5 for the transition point of pure tin.

At all events it appeared from this that the transition point of pure
tin must lie in the neighbourhood of 200°, and as it had appeared
from the preceding experiments that the conversion in the transition
points of mixtures containing Hg is attended with a distinct though
small diminution of volume, it must also be possible to find the transition
point for perfectly pure tin by dilatometrical way.

It was clear that the conversion in pure tin proceeds slowly, and
that at every temperature we should have to wait long to attain
reliable results.

When the thermostat, in which the dilatometer which contained
250 gr. of tin, was placed, was first regulated at 240°, so that the
tin melted, and when then comparatively rapidly the thermostat was.
brought to 190°, it appeared that after the dilatometer had assumed
the temperature of 190°, no change of volume worth mentioning took
place even after 24 hours, from which it was inferred that on soli-
dification exclusively the tetragonal modification had been formed,
and that therefore the tin had solidified at the metastable point of
solidification.

In agreement with this experiment it appeared that when the bath
was regulated at 206°, and also the tin had assumed this temperature,
an increase of volume took place, which could not practically be
considered as completed until after 48 hours. If then the thermostat
was again put at 190°, a diminution of the volume set in again at con-
stant temperature.

This phenomenon, which points to the conversion :

tetragonal tin = rhombie un,

shed a great deal of light on the fact of tin becoming trittle at about
200°, on the preparation of corn tin, and also on IK. ALISCHER’S obser-
vation, particularly because it is very probable that the above
conversion proceeds most slowly in pure material.

It further appeared from these experiments, just as from those
made with tin containing mercury, that the difference in specific
cravity between the tetragonal and the rhombic modification is much
smaller at + 200° than at the ordinary temperature, as the variation
of volume found, which, it is true, had probably not yet reached its

') This investigation is being continued to get to know more about the system
lin-mercury.

681

maximum value, amounted only to about 0,3 em*., which variation
of volume corresponded with a displacement of the oil-level of
+ 6 em. in the capillary.

With a purpose of determining the accurate situation of the tran-
sition point the experiments described above were repeated several
times, which resulted in a final determination of the transition point,
which had been sought so long in vain, at + 202,8°, for at this
temperature no variation of volume had taken place even after four
days, whereas below it a diminution of volume and above it an in-
crease of volume was observed. The inaccurate extrapolation which
was mentioned before, and which gave 200,5° for the transition
temperature, yielded, therefore, a result which was pretty near the truth.

As we have always got the impression in this investigation that
even on slow cooling of pure liquid tin exclusively or almost exclu-
sively the tetragonal modification, which is metastable aboye 203°,
is formed, and that even with pretty slow heating of the tetragonal
form the conversion to the rhombic modification fails to appear, it
seemed pretty certain that only the metastable unary melting-point
of tin was known. To find the stable unary melting-point the curve
of heating was determined of tin which had been heated for 48
bours at 220° in a thermostat. The result yielded by this investi-
gation and the particularities of the pseudo system derived from it
will be communicated in a following paper.

Anorg. laboratorium of the University.

Amsterdam, Oet. 23, 1912.

Chemistry. — “The phenomenon of double melting for fats”. By
Prof. A. Smits and S. C. Boxnorst. (Communicated by Prof.
A. F. HoLueman).

(Communicated in the meeting of October 26, 1912).

Guru *), who has been extensively occupied with the preparation
of simple and mixed glycerin esters of fatty acids, has observed the
phenomenon of double melting for several of these fats. Thus we
hear about tristearin that the crystallised tristearin has only one
melting-point at 71°.5, whereas the tristearin that has first been
melted, then cooled in a capillary, and then solidified, first melts at
55° on supply of heat, then solidifies again, and then melts again
at 71°.5 on further supply of heat. On the ground of these pheno-
mena GuTH has come to the result that the melted and rapidly

1) Z. f. Biol. 44, 78 (1902).

682

cooled mass has not yet crystallised, and is therefore in a glassy
metastable state. On supply of heat the metastable state would pass
into the stable one, in which so much heat is liberated that small
quantities are thereby completely melted, which later solidify again,
but which melt again when the melting point has been reached for
the second time on supply of heat.

Keeis and Harner’) have repeated Guta’s experiments and found
iem perfectly confirmed, but what rouses our great astonishment
is this that they entirely concur in GurTH’s view of the matter.

Without entering into GutxH’s explanation, which is, putting it
mildly, very improbable, we will state here very briefly what has
been the result of an investigation which we have carried out with
the purest ¢ristearin of KAHLBAUM.

It is clear from what precedes that in GurtH’s opinion the tempe-
rature of 55° cannot he called a melting point of tristearin. Our
experiment, however, has shown that GuTH has stated the truth,
in spite of himself, and that we have, indeed, to do here with two
melting-points. It has namely appeared that the observed peculiar
phenomenon is caused by the existence of two different crystallised
modifications of tristearin, of which the metastable one appears most
readily. The velocity of crystallisation of the stable form is still
very small, even a few degrees below the point of solidification of
the metastable form, and much smaller than that of the metastable
modification. Hence when the liquid is cooled down to below the
point of solidification of the metastable form, the latter is always
made to crystallise.

If the hquid is kept for some time at a temperature between the
two melting-poimts, the stable form crystallises, but with a_ very
slight velocity.

If we start from the metastable modification obtained by compara-
tively rapid cooling of the liquid, and if this metastable modification
is placed in a bath the temperature of which rises slowly, the meta-
stable unary melting-point appears at 34°.5; if the temperature of the
bath is carried up to 63°, and if this temperature is kept constant for
some time, crystallisation sets in slowly, and only after 2 or 3 hours
everything has become solid and has passed into the stable modification.
If the temperature of the bath is made to rise still further, the stable
unary melting point occurs at 70°.8. The phenomena described just
now have also been studied under the microscope, in which our
views were perfectly confirmed in all respects.

1) B. B. 36, 1123.

683

In conclusion we will still remark here that the system ¢ristearin,
which according to our investigation exhibits the phenomenon of
allotropy, and is probably monotropic, has also furnished a confir-
mation for the theory of allotropy, as it has appeared here again
that the solid phases are states of internal equilibrium. Particularly
for the metastable modification it could be clearly demonstrated that
the solid substance which has assumed equilitrism at lower tempe-
rature, melted already below the metastable unary melting-point in
case of rapid heating.

Henze it follows from what precedes that we have to assume two
kinds of molecules « and 8 for the systera fristearin, and that the
differences between the two crystallised states are owing to the diffe-
rence in situation of the internal equilibria.

That the phenomenon of double melting observed for other fats,
will have to be accounted for in the same way, is more than probable.

Anorg. Chem. Laboratory of the University.
Amsterdam, Oct. 25.

Chemistry. — “On the system ammonium sulphocyanate-thioureum-
water.’ By Prof. A. Smirs and A. Kettner. (Communicated
by Prof. A. F. Hottieman).

(Communicated in the meeting of October 26, 1912).

A recently published paper by Atktys and Werner’) induces us
briefly to communicate already now the results of an investigation
which is not yet quite completed.

The pseudo binary system NH,CNS — CS (NH,), was examined.
The melting-point figure found for this system (fig. 1) pointed with
great probability, to the existence of acompound NH,CNS.4CS (NH,),
because the curves of cooling on the right of this concentration did
not give a single indication for a eutectic point at +105°, whereas
this was the case for mixtures on the lefiside uf this concentration.
Atkins and WerNeR are, however of opinion that the compound
NH, CNS.3CS(NH,), follows from the melting-point lines found by
them, which show a close resemblance to ours °*).

To get perfect certainty about the existence of the compound 1 4,

1) Journ. Chem. Soc 101, 1167 (1912).
2) On account of the rapid conversion of GS (NH), at high temperature, the
mixtures with more than 70°%/, CS (NH,‘, had to be investigated by Socn’s capil-
lary method,

684

the study of the ternary system NH, CNS — CS (NH,), —- H,O was
taken in hand after the melting-point diagram had been determined,
ii which a method of analysis was worked out which enabled us

the

ONKACNS 5h Naens, 4 CSW) CHV),
AG
Fig. 1.

quantitatively to determine the ammonium sulpho-eyanate and the
thioureum by the side of each other with sufficient accuracy.

The solubility-isotherms found at 25° and the investigation of the
eoexisting solid phases, in which the residu-method was applied for
the determination of the binary compound (see fig. 2) afforded a
proof for the validity of the conclusion drawn from the melting-point
figure, so that the existence of the compound 1.4 may now be con-
sidered as conclusively proved.

Moreover the knowledge of the peculiar situation of the solubility
isotherms led us to a simple explanation of the method of prepa-
ration of thioureum from ammonium sulphocvanate according to
Reynonps and Wernzr'), which method had been unaccountable
up to now.

The process of preparation is as follows: ammonium sulphoecyanate
is heated for some time up to 160°, then the liquid is poured into

1) Journal Chem. Soc, 83, 1 (1903).

685

cold water, and then the solid substance obtained by evaporation
is recrystallised.

B C5(NH),

NH,CNS

According to FinpLAy’s') experiments, and also according to ours
the internal liquid equilibrium that sets in when ammonium sulpho-
cyanate is heated up to 160° for some time, has the following compo-
sition 75°/, NH, CNS and 25°/, CS (NH,),. When the liquid is poured
into cold water, this state is fixed. If we suppose that everything
is solved at 25°, the obtained state lies in our figure on the line
that joius the points P and A, and in the unsaturate region. If we
now begin to make the liquid evaporate, the isotherm of the com-
pound NH,CNS.4CS(NH,), will be passed, i.e. we may enter the
region which is supersaturate of the compound 1,4 indicated by the
point V, so that the latter deposits. If we now separate the solid
substance from the mother liquor and if we solve the compound V
in a new quantity of water, the obtained liquid will again lie in
the unsaturate region, but now on the line that connects point V
with A. This joining line accidentally does not cut the isotherm of
the compound JV, but that of the thioureum (4), so that on evapo-
ration of the solution, not the compound V, but thioureum will

1) Journal Chem. Soc. 85, 403 (1904).

686

deposit. It is clear that to obtain thioureum from the compound V
it is not even necessary to dissolve the latter first entirely. It already
suffices to bring the compound in contact with water, because the
pure saiurated solution of V is metastable, and will deposit thioream
specially on seeding with a crystal of this substance, which con-
version continues till the compound has quite vanished.

With regard to the exact relation between the pseudo-binary and
ihe unary T, x-figure of the sysiem NH, NCS—CS(NH,), we may
state that it is being investigated, and that we hope that we shall
soon be able to give it with perfect certainty. °)

Anorg. Chem. Laboratory of the University.
Amsterdam, Oct. 25, 1912.

Botary. — “On the demonstration of carotinoids in plants. Second
communication: Behaviour of carotinoids with regard to
reagents and solvents.” By Prof. C. van WisseLinca. (Commu-
nicated by Prof. J. W. Mo11).

(Communicated in the meeting of October 26, 1912).

The reagents by means of which coloration is brought about in
earotinoids are the following: concentrated sulphuric, sulphurous and
concentrated nitric acids, bromine water, concentrated hydrochloric
acid with a little phenol or thymol, and iodine in potassium iodide
or chloralhydrate solution. All these reagents cause blue coloration,
except the iodine reagents which generally produce a green colour,

In this paper the use of sulphuric acid, bromine water and iodine
in potassium iodide solution will be dealt with as well as two new
reagents for carotinoids, namely, concentrated solutions of antimony
trichloride and of zine chloride both in 25 °/, hydrochloric acid.
Solvents as well as reagents can also be successfully used in the
microscopic investigation of carotinoids, and they also are dealt with
in this paper.

Sulphuric acid.

T. Tammes*) in her investigation of carotin used concentrated

1) This relation is probably pretty complicated, because different crystallized
modifications exist of both pseudo-components. This was already known of NHy
CNS, but for CS (NHg); it was revealed for the first time by this investigation.

*) T. Tammes, Ueber die Verbreitung des Carotins im Pflanzenreiche, Flora
1900, 87. Bd. 2. Heft, p. 213.

687

sulphuric acid, concentrated hydrochloric acid containing a little
phenol, concentrated nitric acid and bromine water, and she com-
pletely dried the preparations over sulphuric acid in a dessicator.
She maintains that with sulphuric acid and hydrochloric acid con-
taining phenol, this is absolutely necessary and is to be recommended
in the case of nitric acid and of bromine water. Tamms says that
when the preparations are even slightly moist, the reaction sometimes
does not take place, and she attributes this, especially in the case of
sulphuric acid, to the presence of traces of water. When investigating
the crystals which have been separated out in the cells and tissues
as also when working with plants and parts of plants, which have
not yet been treated with other reagents, Tames prescribes the
careful drying of the preparations. Kon. ‘) completely agrees with
this. My impression is, however, that he does not support his opinion
by experiments. G. and F. Tosrer *) state moreover that the assertion
that the reaction with sulphuric acid succeeds only with anhydrous
objects, is not correct. 7

With respect to Tammes’ method of procedure it must be remarked
that a thorough drying is not a suitable method for obtaining beau-
tiful preparations, and there is no theoretical explanation why this
drying is necessary, for concentrated nitric acid contains 50 °/, water,
concentrated hydrochloric acid 75°/, and bromine water being a
saturated solution of bromine in water contains nearly 97 °/, water,
whilst concentrated sulphuric acid also always contains a certain
percentage of water, 4—6. Only when concentrated sulpburie acid
is used can I imagine that the smail quantities of water in the
preparations can be of influence, but in this case a much simpler
means can be used than the thorough drying of the preparations,
namely, the use of fuming sulphuric acid, so that the water with
which it comes into contact is converted into sulphuric acid
(H,S,O, + H,O = 2H,SO,). Thus fuming sulphuric acid has a
stronger action than the concentrated acid.

The assertion that traces of water can interfere with the reaction,
is wholly incorrect, as I shall further prove. On the contrary the
best results are obtained with somewhat diluted sulphurie acid. By
mixing concentrated sulphuric acid of 95°/, with 10, 20, 30, 40
and 50°/, water, I obtained dilute sulphuric acid of 85'/,, 76, 66°/,,

1) F. G. Kont, Untersuchungen tiber das Carotin und seine physiol. Bedeutung
in der Pflanze, 1902, p. 44.

2) G. und F. Tosier, Untersuchungen tiber Natur und Auftreten von Carotinen,
Ill. Zur Bildung des Lycopins und iiber Beziehungen zwischen Farb- und Speicher-
stoffen bei Daucus, Ber. d. d. bot. Ges. 30. Jahrg. Heft I, 1912, p. 33.

688
57 and 47'/,°/,. | have experimented with sulphuric acid of varying
strength in about forty cases with flowers, leaves and algae. The
earotinoids, which rarely in nature occur in crystalline form, were
previously separated out as crystals by means of Morisca’s reagent,
and were successfully obtained, except in a few cases. | allowed the
sulphuric acid to flow to the preparations which were in water
under the cover-slip or I applied it to the preparations which lay
in a minimal quantity of water on a slide, Mixing therefore always
took place between the mixture used and the water in which the
preparations were, and consequently there was a slight dilution of
the mixture. The result of this series of experiments was that the
fine blue coloration due to sulphuric acid was always shown. In
most cases the reaction succeeded already with sulphuric acid of
65'/, or 76°/,, it was seldom necessary to use sulphuric acid of
85'/, °/,, and in some cases the blue colour appeared on using sulphuric
acid of 57°/,, eg., in Narcissus Pseudonarcissus and Cladophora.

When stronger sulphuric acid, namely, 95°/, is used, various
subsidiary phenomena generally occur. Sometimes the crystals are
seen to dissolve, forming blue cloudlets in the fluid, or they lose
their shape and unite to form blue drops of liquid. Sometimes they
dissolve and in their vicinity a precipitation of small blue drops is
seen. Often the blue coloration is observed to become fainter and
disappear. Commonly some of these phenomena occur together. It is
difficult to say to what extent the differences in the action of sul-
phurie acid are caused by accidental circumstances or are connected
with the chemical nature of the carotinoids, but it is certain that in
the course of the reaction the latter plays an important part.

It happens, for example, in many plants, that in the same cells
two kinds of erystals are separated out, which behave differently with
regard to sulphuric acid. Before the action of sulphuric acid takes
place, the two kinds of crystals ean already be distinguished by their
colour and shape, especially by the colour, which is orange-yellow
or orange, and red or orange-red. The difference is, that the blue
colour does not appear equally quickly in both kinds of erystals or
indeed that a different degree of concentration of the sulphuric acid
is required to produce it. Under the action of sulphuric acid of 66’/,
or 76°/, the orange-yellow or orange crystals are immediately coloured
blue and the red or orange-red ones not at all or much later. When
these different crystals have about the same thickness and are in
proximity in the same cells, it may be assumed that the action of
the sulphuric acid takes -place under the same conditions. Since the
different behaviour with regard to sulphuric acid is accompanied by

689

differences in colour and shape and the erystals also differ in respect
to other reagents and solvents, as will be further indicated, it may
be assumed that the phenomenon is connected with differences of a
chemical nature.

The action of concentrated sulphuric acid on dried preparations
shows no trace of the different behaviour of the crystals with regard
to sulphuric acid. The reaction takes place so quickly that it some-
times completely escapes observation. The treatment of dried prepar-
ations with concentrated sulphuric acid is to be deprecated, for such
a method of working greatly decreases the value of the elegant
reaction, which is so well suited for microscopical investigation.

The bright colour which the reaction produces is usually called
blue, sometimes also blue-violet. It may be called blue, aithough a
faint violet shade is sometimes unmistakable (compare KLINcksIECK
et VatetTtE, Code des Couleurs, 426 and 451).

I have found no explanation of the reaction in the literature.
HuseMANN ') states that water causes the blue colour to disappear and
unchanged carotin remains. If the blue crystals are treated with a
large quantity of water, then they resume their original colour,
orange-yellow or red. Sulphuric acid brings the blue colour back again.

The objects with which I have studied the sulphuric acid reaction
in the manner described are the same as those with which Momiscn’s
potash method was investigated (see the list in the first communication).

Zinc chloride and Antimony trichloride.

It is not only with somewhat diluted sulphuric acid, but also with
saturated solutions of both zine chloride and antimony trichloride
in 25°/, hydrochloric acid that the erystais of the carotinoids which
occur naturally in the cells or are artificially produced there, can
be given a beautiful dark, persistent, blue colour. These two solutions
have hitherto not been used as reagents for carotinoids. | tried them
in about twenty cases. I allowed the solutions to flow to the prepa-
rations under a cover-slip. When a solution of zine chloride was
used, the preparations lay in water, but when I used a solution of
antimony trichloride I first placed them in dilute hydrochloric acid
in order to obviate the formation of insolulable antimony oxychloride.

The reaction did not occur equally quickly in the case of all the
erystals. The orange-yellow crystals become blue before the red ones.
When the zine chloride solution was used the red crystals did not

1) A. Husemann, Ueber Carotin und Hydrocarotin, Ann. der Chem. u. Pharm.
Bd. CXVII, 1861, p. 226.

690

always become blue. With the solution of antimony trichloride all
the crystals finally became dark-blue. Generally the colour is pure
blue (Ku. and V. 426), but at the beginning of the reaction it is
sometimes bluish-violet (476, 451). Occasionally in the use of con-
centrated sulphuric acid, subsidiary phenomena appear, such as the
flowing together of the crystals into blue drops, solution and separa-
tion of blue droplets from the solution.

When the crystals coloured blue by means of zine chloride or
antimony trichloride are treated respectively with water or with
dilute hydrochloric acid and water, the original orange-yellow or
red colour reappears, although it may be somewhat less pure.

Sulphuric acid and zine chloride solution in a more or less con-
centrated state strongly aitack the cell-walls, but this is much less
so in the case of antimony trichloride solution. This to some extent
may be reckoned an advantage of the latter reagent.

There follows here a list of the organs and plants on which I
have tested the two new reagents for carotinoids.

Flowers: Trollius caucasicus Strv., Chelidonium majus L., Isatis
tinctoria L., Spartium junceum L., Thermopsis lanceolata R. Br.,
Cucurbita melanosperma A. Br., Ferulasp., Asclepias curassavica I..,
Calceclaria rugosa Hook., Dendrobium thyrsiflorum Rens. fil., Iris
Pseudacorus L., Narcissus Pseudonarcissus L., Lilium croceum Caarx.

Green leaves: Chelidonium majus L., Urtica dioica L.

Fruits: Sorbus aucuparia L., Solanum Lycopersicum Try.

Root of Daucus Carota L.

Algae : Cladophora sp., Haematococcus pluvialis Fror.

Bromine.

The behaviour of bromine water with respect to the carotinoid
crystals was studied in about twenty cases. The crystals were for
the most part separated out by using Mo.isca’s reagent. Without
exception a fugitive, greenish-blue colour was obtained. Generally
the blue colour was clearly perceptible and only to a slight extent
showed a greenish shade. In a few cases the coloration passed off
quickly and the green predominated. This was so with Chelidonium
majus and Spartium junceum. In the crystals of the fruit of
Solannm lLycopersicum 1 saw the reddish-violet (Kn. and V. 581)
colour successively change into bluish-violet (476), blue, greenish-
blue (386) and green, and finally this last colour faded away.

In the following cases, the crystals were investigated with bromine
water.

691

Flowers: Chelidonium majus L., Corydalis lutea DC., Erysimum
Perofskianum Fiscn et Mey., Isatis tinctoria L., Cytisus sagittalis Koc
(Genista sagittalis L.), Spartium junceum L., Thermopsis lanceolata
R. Br., Cucurbita melanosperma A. Br., Doronicum Pardalianches L.,
Hiéracium aurantiacum L., Gazania splendens Horv., Asclepias curas-
savica L., Calceolaria rugosa Hook., Dendrobium thyrsiflorum Reus.
fil., Iris Pseudacorus J.., Clivia miniata Rreen, Lilium croceum Cary.
Hemerocallis Middendorffii Traurv. et Mey.

Leaf of Urtica dioica L.

Fruits: Sorbus aucuparia L., Solanum Lycopersicum Try.

Root of Daucus Carota L.

Algae: Cladophora sp., Haematococcus pluvialis For.

Todine.

With carotinoids iodine forms addition products. In about twenty
cases the behaviour of iodine in- potassium iodide solution was in-
vestigated with respect to the crystals of the carotinoids. By means
of the potash method the latter were separated out in most cases.
With iodine they became nearly always green.’ Often they were
distinctly green, in other cases less so, and frequently they were
yellowish green. In many cases the green colour appeared immedi-
ately, and sometimes not at once, but only gradually, as, namely,
in the flowers of Chelidonium majus and Spartium junceum, and
in the red crystals obtained in the flower of Asclepias curassavica
and the leaf of Urtica dioica. Sometimes no green coloration what-
ever could be observed, not even after 24 hours. This was so with
the flower of Dendrobium thyrsiflorum where, in addition to orange-
yellow crystals, aggregates of orange or orange-red crystals separated
out, which did not become green. The objects experimented upon
with iodine in potassium iodide solution were the same as those on
which bromine water was tried.

Solvents.

The most suitable solvents for the microscopical investigation of
the carotinoid crystals are those which can be mixed with water.
The preparations can then be brought direct from water into the
solvent or the solvent can be allowed to flow under a cover-slip to
the preparations which are in water. Solvents which fulfil this
condition are, for example, alcohol and acetone. In addition use can
be made of an alcoholic soap-solution (soap-spirit of the Dutch Pharm.
4h edition, without oil of lavender) and of chloralhydrate solution

Proceedings Royal Acad. Amsterdam. Vol. XIV.

692

7 in 10). With these two solutions I succeeded, in establishing for
instance that in the leaves of Urtica dioica, the orange-yellow crystals
dissolve more quickly than the red ones. The best results I obtained
with phenol solutions.

According to WitistAtter and Mre¢') xanthophyll is “spielend
léslich” in phenol. When liquefied phenol (10 parts by weight of
phenol in loose crystals to one part by weight of water) is added
under the cover-slip, the orange-yellow crystals are generally seen
to dissolve very quickly, whilst the solvent becomes orange-yellow.
The process of solution is often preceded’ by a flowing together and
the formation of orange-yellow globules and masses. Other crystals,
generally the red and the. orange-red, the reddish-violet in the fruit
of Solanum Lycopersicum and the orange ones which are separated
out by Moriscn’s reagent in the flower of Dendrobium thyrsiflorum,
dissolve much more slowly. In some preparations they are dissolved
after some hours, in others, kept in the solvent for several days,
crystals can still be detected.

Because it is so difficult to mix with water phenol that has been
liquefied by water, I have preferred for microscopic investigation a
mixture of three parts by weight of phenol in loose crystals and one
part by weight of glycerine. The phenomena observed are the same,
but the mixing and dissolving proceed more quickly. With this solvent
IT have been able to show in a number of cases that the various
crystals which had separated out, differed greatly in solubility. This
was, for instance, the case with the flowers of Asclepias Curassavica
and Dendrobium thyrsiflorum, as also in the leaf of Urtica dioica.

In a few cases I experimented with a saturated aqueous phenol
solution (solubility of phenol in water about 1 in 12'/,). With the
orange-yellow crystals I often observed a slow deliquescence to
orange-yellow globules which did not dissolve in the phenol solution.

As is stated in my first paper, the microscopical observation and
separation of the crystals of carotinoids already show that there are
many reasons for thinking that in the vegetable kingdom several
varieties of carotinoids occur. The results obtained with various
reagents and solvents, sulphuric acid, zine chloride, antimony tri-
chloride, bromine, iodine, and phenol solutions have further confirmed
this. In my opinion the results of microscopic and micro-chemical
investigations have thus been brought into agreement with macro-
chemical results.

') Richarp WILLSTATTER und WALTER Mine, IV. Ueber die gelben Begleiter
des Chlorophylls, Jusrus Lreste’s Annalen der Chemie, 855. Bd. 1907, p. 1.

693

Botany. --— “On the demonstration of carotinoids in plants. Third
communication: The leaf of Urtica dioica L., the jlower of
Dendrobium thyrsiflorum Rehb. fil. and Haematococeus pluviales
Flot.” Prof. By C. van Wissrtincn. (Communicated by Prof.
J. W. Mot).

(Communicated in the meeting of October 26, 1912).

In the first and second communications I have shown that earotinoids
in plants present differences in the colour and shape of the erystals
and in their behaviour towards reagents and solvents. It is obvious
that the presence of different chemical bodies cannot be assumed
when the crystals only differ in colour and shape or when only a
slight difference can be observed on the addition of a reagent or
a solvent. When, however, important differences in colour and shape
accompany avery remarkable difference of behaviour towards reagents
and solvents, then such a conclusion may be justified. I will show
by means of a few striking examples that the latter case applies to
the carotinoids found in plants.

Leaf of Urtica divica L.

The substances accompanying the chlorophyll of the stinging-nettle
have been accurately investigated chemically. We know from the
investigations of Wiuiustirrer and Mire’) that two carotinoids are
present in the leaves of the stinging-nettle, carotin identical with
Daucus-carotin, and xanthophyll. These chemists found four times
as much xanthophyll as carotin.

When leaves of Urtica dioica or leaf fragments are placed in
Moniscu’s reagent and examined after a few days, there is found in
each cell containing-chlorophyll an aggregate of red crystals resembling
small parallelograms or needles and of orange-yellow plates, which
are several times more long than broad and show more or less rounded
ends; sometimes a few orange-yellow curved filamentous crystals
project from the aggregate. We readily observe that the orange-
yellow crystals form the greater part of the aggregates. If the crystals
are investigated with reagents and solvents, differences become evident.
When they are treated with sulphuric acid of 76°/, they all
finally become blue, but the orange-yellow ones are coloured first.
The red ones often retain their own colour for a long time. The

1) RicHarp Wi.usratrer und Watter Miec, IV. Ueber die gelben Begleiter des
Chlorophylis, Justus Lizsie’s Annalen der Chemie, 355. Bd. 1907, p. 1.
45*

694

different crystals are then distinguished very clearly with sulphuric
acid of 66'/,°/,, only the orange-yellow crystals become blue.

If preparations with crystals separated by the potash method are
placed on the slide in a solution of chloralhydrate (7 in 10) then
after a time, for example, 1'/, hours, the aggregates appeared much
changed; the orange-yellow crystals had been dissolved and the red
needles or small parallelograms remained behind, sometimes still
united. After 24 hours they had not wholly disappeared from the
preparations.

With soap-spirit also (Pharm. Nederl. Ed. IV, without oil of
lavender) a great difference in solubility was proved. After being one
day in soap-spirit the orange-yellow crystals had disappeared from
the preparations, whilst the red remained behind.

I obtained a still more striking result with a solution of phenol
in glycerine (3 to I). If this mixture is allowed to flow under the
cover-slip, the orange-yellow crystals are seen to dissolve quickly
whilst the red ones are unchanged even after 24 hours.

The investigation of the orange-yellow and red crystals can be
facilitated in the following manner. Leaf fragments are placed for
two hours in a 10 °/, solution of oxalic acid and then put into
Mouiscn’s reagent. In the tissue large red and yellow crystal-agere-
eates are, thus formed, which can easily be studied. |

On consulting the paper of WitisTArrer and Mrre*) on carotin
and xanthophyll, we must conclude that, of the crystals described,
the red are carotin and the orange-yellow xanthophyll.

As in the leaves of Urtica dioica so in many other cases, in
flowers, leaves and algae, I have been able to distinguish yellow,
orange-yellow or orange-coloured crystals and red or orange-red ones,
of different shape, which behave differently towards reagents and
solvents and indeed in a more or less corresponding way. I do not
doubt that in all these cases the plant contains different carotinoids
side by side, in many cases probably a carotin together with a
substance which belongs to the xanthophylls. I think it not
improbable that the same ecarotin and the same xanthophyll are
often found together, but I also consider that in a number of cases
another carotin or xanthophyll is present. WILLSTATTER and EscHeEr *)
have already established the presence, in the fruit of Solanum Lyco-
persicum, of a carotin, lycopin, differing chemically from Daucus-carotin.

os ae
2) RicHArp WILLSTATTER und Hetnr. H. EscHer, Ueber den Farbstoff der
Tomate, Hopps-SryLpr’s Zeitschr. fiir Physiol. Chemie, 64. Bd. 1910, p. 47.

695
The flower of Dendrobium thyrsiflorum. Rehb. fil.

The flower of Dendrobium thyrsiflorum Rehb. fil., is an example
of an object containing a carotinoid, differing from those so far
described. After treatment by the potash method, I found in the
cells orange-yellow (Kuinckstnck et Vanerre 151) much curved fila-
mentous crystals, orange-yellow (151) whetstone-shaped plates and
Jarge and small aggregates of brightly coloured orange (101 though
inclining towards orange-red 81) thin acicular crystals. The difference
in colour is very striking. Some cells are more especially filled with
one shape, others with the other shape. In this case I could observe
no difference on using sulphuric acid of varying strength, nor with
bromine water, but on the other hand iodine in potassium iodide
solution brings it out. With the latter reagent the orange-yellow
crystals at once become a fine green. The orange-yellow aggregates
suffer no change of colour whatsoever, not even after 24 hours.
The contrast in the colour of the crystals is very striking. So far
as concerns their solubility in a solution of phenol in glycerine (3
to 1) the erystals also differ much. When the solvent is allowed
to flow under the cover-slip, the orange-yellow crystals are at once
seen to deliquesce, and form with the solvent yellow globules which
dissolve entirely. On the other hand the orange-coloured aggregates
do not at first show any signs of dissolving. Sometimes they are
seen in the midst of the globules that are formed. Finally all the
Orange aggregates can be seen in the yellow solution of the orange-
yellow crystals. Slowly the orange crystals dissolve also. If the
preparations are placed for one day in the mixture of phenol and
glycerine, the orange crystals also dissolve.

Because of the difference in colour, different behaviour towards
iodine in potassium iodide solution and different solubility in phenol,
I conclude that two different carotinoids occur in the flower of
Dendrobium thyrsiflorum. The one of these which is to some extent
reddish-orange in colour, is a carotinoid that is not common in plants.
Such a carotinoid I have found only in Dendrobium thyrsitlorum,
Its colour and other properties makes me inclined to think that it
belongs to the xanthophylls rather than to the carotins.

Haematococcus pluvialis Flot.

The colouring matter of this interesting alga has been investigated by
Zorr'). The result of his enquiry was that it possesses not one but two

1) W. Zopr, Couy’s Himatochrom ein Sammelbegriff, Biologisches Centralblatt,

XV. Bd. 1895, p. 417.

696 .

colouring matters, which must be considered to be carotinoids. Zopr
found a vellow carotinoid such as is commonly found in green
plants and a ved one to which the alga is indebted for its frequently
dark blood- or brown-red colour and for its name. Zopr succeeded
in separating the two colouring matters in the following way. The
erude alcoholic extract of the alea was saponified with caustic soda.
The chlorophyll was thus changed into a sodium compound, the fat
into a soap and glycerine, the yellow carotinoid was set free and
the red one converted into a sodium compound insoluble in water.
When the saponification products after dilution with water, were
treated with petroleum ether, the yellow carotinoid was removed,
whilst the sodium compound of the red one separated out. After
purifying the sodium compound the carotinoid was set free ty means
of dilute sulphuric acid, it was taken up in ether and investigated
spectroscopically. The red carotinoid differs spectroscopically from
the yellow, in colour and in the colour of its solutions, and also in
its power of combining with alkalis and alkaline earths.

Haematococcus pluvialis has recently also been investigated by
JacogseN'). By means of Moniscu’s potash method he obtained sepa-
ration of crystals, but on the other hand he was unsuccessful with
dilute acids and with Tswert’s resorcinol solution. The accuracy of
Zorr’s results remained undecided.

Mr. JacopseN was kind enough to send me a culture of Haemato-
coceus pluvialis on agar, and thus I was given an opportunity of
studying this remarkable alga and of confirming the above mentioned
conclusions of Jacopsen. As is clearly shown by his beautiful plates,
the aplanospores differ very much as regards colour; some have
a green content, in consequence of the chlorophyli they contain,
others are green at the periphery and red in the centre, whilst in
others again the green of the chlorophyll is entirely masked and
there seems to be only a red content. The red colouring matter is
combined with a liquid fatty substance or, more‘ accurately, is
dissolved in it. This substance occurs in the form of globules in the
cell-content.

As is to be expected, aplanospores which at first sight show
differences, yield different results on investigation. In the green spores
orange-yellow crystals were quickly separated out by Moriscn’s rea-
vent; generally these are shaped like curved needles, which are
often united into bundles; sometimes orange-yellow crystal plates
were also observed. In addition to these plates, there were also a

1) H. €. Jacosson. Die Kulturbedingungen von Haematococcus pluvialis, Folia
Microbiologica, I, 1912, p. 24 et seq.

697

few small red plates, shaped like parallelograms. On the addition
of sulphuric acid of 66'/, or 76°/, the orange-yellow crystals become
blue without any deliquescence to globules or solution being observed.
This takes place when sulphuric acid of 95°/, is used. The small
red crystals, shaped like parallelograms are not so quickly colcured
blue as the orange-yellow ones or a more concentrated acid must be
applied in order to colour them blue. The erystals also behave dif-
ferently with respect to phenol glycerine. The orange-yellow quickly
dissolve in it whilst the red remain undissolved. The orange-yellow
crystals behave therefore like xanthophyll-crystals and the red ones
like carotin-crystals. The investigation of the green aplanospores
therefore gives no special result. Two carotinoids are found to accom-
pany chlorophyll, an orange-yellow one and in small quantity a rved
one, as is usual in green plants.

In those aplanospores which are more or less red in dates there
are found after treatment with Moziscn’s reagent reddish-violet crystal
aggregates and, frequently, curved band shaped crystals. I now
leave out of further consideration the small red crystals shaped like
parallelograms. The crystals do not seem to be so easily separated
out in the red aplanospores as in the green ones. It is advisable to
allow Motiscn’s reagent to act for at least some days in order to
decompose the fatty substance which tenaciously retains the colouring
matter. If any of the fat remains behind, the investigation becomes
more difficult in consequence.

_ By means of sulphuric acid of 66'/, the reddish-violet crystals
become blue, also with 76°/, sulphuric acid, but in this case the action
is accompanied by partial solution, which sometimes is preceded by
deliquescence. The surrounding medium becomes blue. The behaviour
of the reddish-violet crystals towards sulphuric acid of varying
strength is therefore different from that of the orange-yellow crystals.
In a solution of phenol in glycerine (8 to 1) the reddish-violet
erystals easily dissolve, and colour the solvent dark reddish-violet.

The crystals were not at one time of an orange-yellow colour,
and at another time reddish-violet, but in many cases they oscillated
between the two colours. Orange-yellow and reddish-violet crystals
were never observed side by side in the same cell. These facts and
-the solution in 76°/, sulphuric acid, as described, led me to suppose
that the reddish-violet crystals were perhaps mixed crystals composed
of two carotinoids. I then tried to separate them with solvents, and
succeeded. The crystals often completely dissolve in acetone or
absolute alcohol; the orange-yellow carotinoid remains in solution,
but the other quickly separates out again in the cells in the form

698

of numerous small violet platelets. The experiment can be made in
a test tube and also on a microscope slide. Under the microscope
the process of solution, the yellow-coloration in and round the cells
and the separation of the violet platelets can be seen.

The phenomena observed can be explained in the following way.
The orange-yellow carotinoid is fairly easily soluble in acetone or
absolute alcohol; the other one is practically insoluble, but its solu-
bility is increased by the presence of the orange-yellow one, with
which it forms mixed erystals. A solution of both is produced in the
cells, and is quickly diluted, and this brings about that the carotinoid
insoluble in acetone or in absolute alcohol separates out. I am con-
firmed in this opinion by an observation ef Zopr '). When he extracted
the yellow carotinoid from the aqueous solution of the saponification
products with petroleum-ether, the other separated out beneath the
petroleum-ether.

I cannot distinguish any definite form in the violet platelets. They
behave in the following way towards reagents and solvents. With
sulphuric acid of 66'/, ‘/, the colour is not modified or only slightly
so, but with 76°/, suiphurie acid the erystals quickly take a blue
colour and this is speedily followed by dissolution. In a saturated
zine chloride solution in 25°/, hydrochloric acid and in a saturated
antimony trichloride solution in 25°/, hydrochloric acid they become
blue, then the erystals generally deliquesce to blue globules and
dissolve. The solutions are bluish-violet or blue. With bromine water
a very transitory bluish-green colour is observed. In a solution of
phenol in glycerine (8 to 1) the crystals dissolve, whilst the solvent
becomes bright reddish-violet.

If the reddish-violet crystals obtained from the red aplanospores
by means of Motiscn’s reagent are compared with those separated
out from alcohol and acetone and with the orange-yellow ones
obtained from the green aplanospores by Momiscu’s reagent, then the
first mentioned erystals, so far as their properties are concerned,
must be placed between the other two, and this strengthens my
belief that they are mixed crystals.

| must here remark that according to Zopr?) the violet-red or
blood-red carotinoid enter into combination with potassium hydroxide.
On this account it should be assumed that the reddish-violet crystals,
separated out with Moriscn’s reagent contain the potassium compound
of the carotinoid and that the crystals obtained with acetone and
alcohol consist of this compound. In the microchemical investigation

699

I have obtained no indication which points to this. When I treated
the crystal platelets got from acetone or alcohol, with dilute sulphuric
acid for 24 hours at the ordinary temperature I found them un-
changed and moreover their solubility in various solvents remained
the same. However this may be, Zopr’s results and mine obtained
by different methods agree in this that in Haematococcus pluvialis
more than one carotinoid occurs. According to Zorr there are two,
whilst I have succeeded in crystallising out three in the cells and
in separating each from the other two.

Finally I must add a few experimental details. By cultivating
Haematococcus pluvialis in various solutions, I obtained cultures with
different aplanospores, both green and red. I cultivated the alga in
the two following solutions: KNO, 0.01, (NH,), HPO, 0.01, MgCl,
0.01, Na,SO, (hydrated) 0.01, H,O 100 and NH,NO, 0.02,-K,HPO,
0.02, MgSO, 0.02, H,O 100’). In the former solution most of the
aplanospores had a green content, in the latter a red one, and this
was an advantage in the investigation. I used a centrifuge for trans-
ferring Haematococcus from one solution to another and for washing
out the material, which sank to the bottom on centrifuging so that
the solution to be replaced could be poured off.

It results from this paper and the two previous ones, that my
conclusions differ completely from those of Tammus and of Kout.
The assumption, that only one carotinoid occurs in the vegetable
kingdom, is not based on sufficient evidence. It was the result of
microscopic and micro-chemical research. Nevertheless I believe that
such investigation may contribute to our knowledge of carotinoids,
provided that it be carefully carried out. I have found, for instance,
that when different carotinoids occur in a plant ov organ, it is in
many cases at least possible, to distinguish them, that unknown ones
can be detected (Dendrobium thyrsiflorum) anc that sometimes a
greater number can be demonstrated than has hitherto been possible
by other means (Haematococcus pluvialis). The results I have obtained
are in agreement with the macro-chemical investigation (Urtica dioica).
When the quantity of material is insufficient for the application of
other methods, a microscopical and micro-chemical inquiry is still
practicable and moreover demands comparatively little time. The
botanist who concerns himself with such work, should however
consider, that it is impossible to solve by means of a few colour-
reactions difficult chemical problems, such as, for example, the

1) H. C. Jacossen, |. c. p. 8.

700

identification of the carotinoids of different plants. As Zopr') justly
says eareful macro-chemical investigation alone can lead to decisive
results in such cases.

Chemistry. — “Equilibria in ternary systems [”. By Prof. F. A. H.
SCHREINEMAKERS.
(Communicated in the meeting of October 26, 19.2).

On the equilibria oecurring in ternary systems between liquid and
vapour different theoretical *) and experimental*) investigations have
already appeared previously. We will now discuss a few cases where,
in addition to liquid and vapour, solid substances occur also.

The syster FL G.

We choose for / a ternary compound and will assume that the
three components occur in the vapour.

We now choose at a definite constant temperature T such a
pressure P that no vapour can form. The isotherm can then consist
only of the saturation line of the solid substance F. This saturation
line is a closed curve surrounding the point F like the closed curve
of Fig. 1, for instance. |

On reduction of P a gas region appears somewhere and at the same
time a heterogeneous region separating the gas region from the liquid
region. In Fig. 1 the gas region is indicated by G, the liquid-region
by L: the drawn line is the liquid-line, the dotted one the gas- or
vapour line of the heterogeneous region. The straight lines drawn
in this heterogeneous region unite the liquids with the vapours with
which they can be in equilibrium.

We now have in Fig. 1 two homogeneous regions, namely the
liquid region lL. and the gas region G; in addition we find two
heterogeneous regions.

In one of them a mixture dissociates into L+G; we will eall

1) W, Zopr, Zur Kenntnis der Farbungsursachen niederer Organismen (Dritte
Mitteilung), Beitrage zur Physiol. u. Morph. niederer Organismen, 1892, Erstes
Heft, p. 36.

*) J. D. vAN DER WAALS. These Proc. Vol. JV p, 448, 539, 681; Vol. V p.1,
121, 225. (1902).

F, A. H. ScorernemaKers. Zeitschr. f. phys. Chem. 36 257, 413, 710 (1901) 37
129 (1901) 38 227 (1901) 48 671 (1903)

Bb. M. van Datrsen. Dissertation, Amsterdam. (1906).

3) F. A. H. Scuremnemakers. Zeitschr. f. Phys. Chem. 39 485, 40. 440, 41.

331 (1902), 47 445, 48 257 (1904).
B. M. van Bice l.e.

701

this the heterogeneous region LG. In the other takes place a disso-

ciation into solid Ff and a liquid saturated with F of the saturation
line of F; we will call this the heterogeneous region FL.

J If we imagine the liquid- and vapour surface

q L of the ¢-surface to be introduced above Fie. 1, it

is Obvious that the solid substance F can be also

g in equilibrium with a whole series of ternary

ee vapours, which equilibria, however, are in the

ae present case all metastable yet. It is also obvious
pee ie

= that these vapours must form in Fig. 1 a closed

curve surrounding point F, which curve, however, has been omitted
from the figure. We will cail this curve “vapour saturation curve”
of the solid substance F. This curve surrounds the heterogeneous
region FG which, however, is still quite metastable.

Hence in Fig. 1 we distinguish :

the saturation line of F.

the vapour saturation line of F (metastable).

the vapour- and liquid-line of the heterogeneous region LG.

the vapour region (G) and the liquid-region (L.)
and the heterogeneous regions LG, LF and GF, the latter of
which is metastable.

_ The vapour region G can form within as well as without the
saturation line of F; on further reduction of the pressure there may
occur also several vapour regions first isolated from each other and
afterwards amalgamating. Moreover, in the system liquid + gas
there may occur either binary or ternary vapour pressure maxima or
minima or stationary points so that different cases are to be distin-
guished. We will first take the case that there occurs neither a binary
or ternary maximum or minimum nor a stationary point so that the
gas region appears in one of the apexes of the component-triangle
and the liquid region disappears in one of the other apexes.

In Fig. 1 the gas region is, therefore, formed outside the saturation
line of F; on reduction of the pressure, the different curves of Fig. 1
will change in form and position. As a rule, a small change in pres-
sure only causes an exceedingly small change in the solubility of a
solid substance; hence, the saturation line of F will alter but little on
change of pressure within very wide limits. This, however, as we
will notice presently, becomes different when we get near to the
melting point of F so that the saturation line of F is only still a
small curve.

702

The influence of a change in pressure on a

a fees liquid and vapour region is, however, great in
comparison with that on the saturation line of F.
g When the pressure decreases, the gas region
ie extends and the liquid region contracts; the

€ €

heterogeneous region L G shifts, therefore, in Fig. 1
Fig. 2. towards the heterogeneous region FL. Hence, on
reduction of pressure, there will occur a pressure as represented in
Fig. 2 where the liquidline and the saturation line of F will meet
in a point M so that the equilibrium F + Ly + Gy, appears. The
three points F, M, and M, as follows readily from the indieatrix theorem,
are situated on a_ straight line. With the aid of the two sheets of
the ¢-surface it is also easy to see that the non-drawn vapour saturation
line of F in Fig. 2, must meet the vapour line in M,.

On further decrease of the pressure, the
saturation line of F and the liquidline intersect
each other in two points; these intersecting
points are represented in Fig.3 by a and b;
in the solid substance the letter F is omitted.

From a contemplation of the liquid sheet
and vapour sheet of the ¢-surface it follows at
once that with each intersecting point of the
saturation line of F and the liquidline is
Fig. 3. conjugated an intersecting point of the vapour

saturation line of F and the vapour line. As the saturation line of
F and the liquidline intersect each other in the points a and b, the
vapour saturation line of F and the vapour line must intersect each
other in the two points a, and b,. The curve a, b, is the vapour
saturation line of F, the vapour line consists of the two parts e, b,
and a, d, which are, of course, connecied with a metastable branch
not drawn in the figure.

At the pressure contemplated here, two three-phase equilibria
kf + L-+G therefore occur, namely :

F+L,+ G,, and F+ Ly + Gp,

On further reduction of the pressure, the heterogeneous region
],G shifts more and more in such a direction that the vapour region
becomes larger and the liquid-region smaller. At a certain pressure,
the liquidline will pass through the point F, after which this gets
situated within the heterogeneous region. We then obtain an isotherm
as in Fig. 4 which does not differ essentially from that of Fig. 3.

703

On further decrease of the pressure, the points a and b and con-
sequently a, and b, will at a definite pressure coincide ; here we
first assume that F then still lies within the heterogeneous region
LG. We then obtain an isotherm like in Fig. 5 in which we must

a
a \
%
Fe
Coe
Fig. 6

imagine m to be formed by the coincidence of a and b, and m,
by the coincidence of a, and b,. It is obvious that m,, F and m
must le on a straight line and that the non-drawn and metastable
saturation line of F must meet the curve de in m and that the
vapour saturation line of F must meet the curve d, e, in m,.

On further decrease of pressure the saturation and vapour satu-
ration curves of F arrive quite within the heterogeneous region LG;
F cannot, therefore, occur any longer in the solid condition but
splits into vapour + liquid; the compositon of the vapour is now
represented by a point of the vapour line d, e,, that of the liquid
by a point of the liqnidline de. Both points le with F on a
straight line.

On reducing the pressure still further we obtain, when the gas
region has extended itself over the point F, isotherms like those in
Fig. 6. Tbe vapour saturation line of F has now disappeared, the
saturation line of F can, however, still exist but then represents
only metastable solutions and has, therefore, been omitted from
the figure.

From the foregoing views, it now follows at once that the liquid
as well as the vapour of the system F + 1L- G trace a closed
curve, like in Fig. 7 and that on each of these lines occurs a
point of maximum and of minimum pressure. As the points of
the curves of Fig. 7 all appertain to a same temperature but to
different pressures, we may call Fig. 7 an isothermic — polybaric

diagram.

704

The curve Mam b represents the solu-
tions which, at a given temperature are
saturated with F under their own pressure;
the compositions of the vapours are indi-
cated by the curve M, a, m, b,. We may,
therefore, call the curve M amb, the iso-
thermic saturation line of F under its own
vapour pressure and M, a, m, b, its con-
jugated vapour line; where no mistake is possible we will omit
the adjunct “isothermic’’.

As a rule, the saturation line of F at a certain constant pressure
P and the saturation line of F under its own vapour pressure will
differ but little, so that, practically, we may substitute the one for
the other; as to exceptions for temperatures in the vicinity of the
melting point of the compound F to them we will refer later.

We have already stated above that the saturation line of F, under
its own vapour pressure, must exhibit a point with a vapour pres-
sure maximum and another with a vapour pressure minimum; the
first is represented in Fig. 7 by M, the second by m. On the con-
jugated vapour line, there occur, of course also two points M, and
m, of which M, represents the vapour with the vapour pressure maxi-
mum and m, that with the vapour pressure minimum. The arrows
on both curves indicate the direction of the increasing vapour pressure.

The points F, M and M, are, of course, situated on a straight
line and agree with the isothermic-isobaric diagram of Fig. 2; the
points F, m and m, which are of course also situated on a straight
line, agree with the isothermic-isobaric diagram of Fig. 5.

We have assumed above that on lowering the pressure the diagrams
3, 4 and 5 succeed each other, or in other words that the points a
and b of Figs.3 and 4 had already coincided in a point m of Fig. 5
before the vapour region had extended to over F. If, however, the
vapour line has already passed point F before aand b of Fig. 3 or4
coincide we get an isotherm as in Fig. 8 which, however, does
not differ essentially from Fig. 3 or 4. On further reducion of the
pressure Fig. 3 is converted into Fig. 9. The vapour saturation line
of F now meets the vapour line e, d, in m,; the saturation line of
F not drawn in Fig. 9 meets the liquidline ed in m. The vapour
saturation line of F represents the stable, the saturation line of F
the metastable conditions. The points F,m and m, are, of course,
again situated as in Fig. 5 on a straight line; as, however, these
points are situated, in the-two figures, differently in regard to each

705
other, the reaction between solid F, liquid m and gas m, is in these
two cases also different. .

Fig. 8. Fig. 9. Fig. 10,

On reducing the pressure still further, the two regions LG and

FG separate and diagrams as in Fig. 10 are obtained. The non-

a drawn saturation line of F represents metastable

mconditions only; solutions saturated with F ean.

ent therefore, occur only in the metastable condition
v Gat this pressure.

ae, The case is, however, different with the vapours
M, : saturated with F; these all occur in the stable

Fig. 11 condition and are represented by the closed vapour
saturation line of Fig. 10.

By a further fall in pressure this vapour saturation line of F
becomes continuously smaller; at the vapour pressure of the com-
pound F it contracts to a point, namely point F, and on further
reduction in pressure it disappears.

Hence, the liquid as weli as the vapour of the system F + L+G
again trace a closed curve (Fig. 11). Mamb is the saturation
line of F under its own pressure, M, a, m, b, its conjugated vapour
line. On the one curve the pressure in M is maximum and in m
minimum, on the other curve in M, and m,; the pressure thus
increases in both in the direction of the arrows.

The two Figs. 7 and 11 exhibit a great resemblance to each
other; yet they differ in different respects such as for instance, in
the situation of the points F, m and m, in regard to each other.
This causes that in Fig. 7 the point F is situated outside and in
Fig. 11 within the vapour line.

When deducing the previous diagrams we have assumed that on
change of pressure, the liquidline of the heterogeneous region moves
more rapidly than the saturation line of F or what amounts to the
same that the vapour line of the heterogeneous region I.G moves
quicker than the vapour saturation line of F.

706

Although this is the case generally, it no longer holds good if
we take a temperature close to the melting point of F. The satu-
ration line of F then surrounds a comparatively small region which
on change of pressure, can rapidly extend, cr possibly contract.
The saturation line of F will then move more rapidly than the liquid-
line of the region LG. We will now distinguish two cases in one
of which the substance expands on melting whilst in the other case
it contracts.

F expands on melting. An increase in pressure (at constant T)
will cause a solidification of the molten F, a decrease in pressure
a fusion of solid F. On decrease in pressure, the isothermic satu-
ration line of F will consequently contract rapidly and disappear
in the point F. We now start from Fig. 1 and assume that, on
lowering the pressure, the saturation line of F contracts at first
rather slowly and then more rapidly; its movement is more rapid
than that of the liquid line of the heterogeneous region LG.

If now the movement of the saturation line of / is slower than
that of the liqnid line, Fig 1 may be converted into Fig. 2 and then
into Fig. 3 from which are then formed either the Figs. 4, 5 and6
or the Figs. 8, 9 and 10. If however, after the isotherms have
assumed a form as in Fig. 3, the movement of the saturation line
becomes more rapid than that of the liquidline, then, after the appear-
ance of the isotherms of Fig. 3, those of Fig. 2 and 1 reappear.
On reduction of the pressure we then get a series of isotherms such as:

fig. | — fig. 2 — fig. 3 — fig. 2a — fig. la
in which the figures occurring after fig. 3 are indicated by 2a and
da. Fig. 2 and 2a resemble each other with this great difference,
however, that in fig. 2a the saturation line of F is much smaller
and that the liquid and vapour lines of the heterogeneous region lie
more adjacent to F than in fig. 2. The same applies to fig. la in
regard to fig. 1. Between fig. 2 and 2a there is also still this diffe-
rence that Fig. 2 applies to the maximum and Fig. 2a to the minimum
pressure of the system F + 1-+G. We will therefore assume that
in fig. 2a the letters M, and M of fig. 2 have been replaced by

m, and m.

From the previous considerations it now
F follows at once that the saturation line of F
under its Own vapour pressure must be situated
as in fig. 12; contrary to this same curve in
fig. 7 and 11 it does not surround the point
14, F which represents the solid phase with which
its solutions are saturated. We will, therefore

707

call the saturation line of F in tigs. 7 and 11 a circumphased and
that of fig. 12 an exphased one.

F contracts on melting. An increase in pressure (at constant T
will, therefore cause a fusion of solid F, a decrease of pressure a
solidification of molten F. On decrease of pressure the isothermiec
saturation line of F will consequently form first of all in F and
then extend at first rapidly and then slowly.

We now start from such a pressure that a heteroveneous region
I, G@ does exist, but not yet the saturation line of F. We then have
fig. 1 from which we must, however, leave out the saturation line
of F. On lowering the pressure, the liquid line shifts towards F and
we assume that it has already just passed the point F when the
saturation line of F appears in the point F. The isotherm then has
a form as in fig. 5 or 6 in which, however, we must assume the
curve de to be very close to F. On further reduction of pressure
the saturation line of F now rapidiy extends round the point F and
overtakes the liquid-line so that at a definite pressure they come into
contact with each other. We then obtain an isotherm as in fig. 5
or 9. In fig. 5 however, we must imagine the saturation and the
vapour saturation lines of F to be drawn and in such a manner
that the first curve comes into contact with e d in m, the second
curve with d, e, in m,. In Fig. 9 we must also imagine the satu-
ration line of F coming into contact with the curve d e in m.

On further reducing the pressure fig. 4 or 8 are formed and as
the velocity of the saturation line of F now becomes smaller than
that of the liquid-line, these are again converted into fig. 5 or 9.
Hence on reduction of pressure we obtain a succession of isotherms
such as:

fig. 5 — fig. 4 — fig. 5a or fig. 9 — tig. 5 — fig. Ya.

in which fig. 5a differs from fig. 5, and fig. 9a from fig. 9 in this
way, that in the figures indicated by a the liquid line ed is removed
further from point F. Also, as the fig. 5 and 9 occur at higher
pressures than the fig. 5a and Ya the letters m and m, must be
considered as being replaced by M and M,.

From these considerations it now follows
that the saturation line of F must exist
under its own pressure as in fig. 13, hence
exphased; the correlated vapour line may
be exphased as well as circumphased and
may also be situated on the other side of F.

The case may also occur that the satu-

Proceedings Royal Acad. Amsterdam. Vol. XV.

708

ration line under its own pressure and its correlated vapour line get
each reduced to a point. Both these points then lie with F on a
straight line.

This case will occur when the saturation line of F and the liquid
line when meeting each other in a point (fig. 2 in M, in fig. 5 and
9 in m) move at that moment from that point towards and from F
with the same velocity. The same then applies to the vapour line
and vapour saturation line of F which also meet in a point (M, in
fig. 2 and m, in fig. 5 and 9). This equality of velocity has, of course,
also a physical significance, which we will look for.

We represent the composition and the volume of the solid substance
F by a, 6 and 2, that of the liquid by 2, y and V and that of the
gas by 7, y,V,.

The equation of the saturation line of F is then given by:
[(a—a)r + (@— ys] da + [(a—a)s + (By) dy =— A V.dP (l)
and that of the liquid line of the heterogeneous region LG by:

[(e —2,)r + (y¥ —4,) 8] da + [(e@— 2,)8 + (y—y,)t] dy = Vor dP (2)
in this:
0V ov
AVE V2 Hae — ay pa
0 # Oy
0oV 0V
Vo a Vo Walger eet ae oe
& y
As the two curves (1) and (2) come into contact with each other
x and y in (1) and (2) are the same and then we have:

i—) ad as

= — We
G—e# 2@,—-# a—ua,
If now we write (4) and (2) in the form:
AV
(r + us) de + (s + ut) dy = — dP
a—wzt
| Vol
(r + us) dx + (s + put) dy = dP
ce— wv

1
we notice that the above mentioned circumstance will appear as:
AV Vo.

a—w &

vy
After substitution of the values AV and Vo we can write for
this also:
(a—wv,) V + («—a) V, + (a, -— «) v= 0
or (6—1,) f + (y—P) ee = (y, re y) v= 0.
This means that the change in volume which can occur in the
reaction between the three phases #, Z, and G', which are in equi-

TO9

libriam with each other is ni/. The reaction between the three phases
therefore takes place without a change in volume. We will return
to this later.

We may summarise the above as follows:

The isothermic-isobaric saturation and vapour saturation curves of
a solid substance F are, at all temperatures and pressures, circum-
phased and disappear (are formed) in the point F.

The saturation curves of a solid substance F under their own
vapour pressure are at a lower temperature circumphased; at a
definite temperature, one of them passes through the point F after
which, at higher temperatures, they become exphased, then they dis-
appear in a point, if in the reaction between the three phases no
change of volume occurs. This also applies to the vapour lines
appertaining to the saturation lines under their own pressure which
can, however, be already exphased at lower temperatures.

In fig. 14 are drawn some saturation lines under their own vapour
pressure with their appertaining vapour lines for different tempera-
tures. On each of these curves
occurs a point with a maximum
and one with a minimum vapour
pressure which, however, are
not indicated in the Fig. although
the arrows indicate the direc-
tions in which the pressure in-
creases. These points are situated
of course, in such a manner,
that the line which unites two
Fig. 14. points with a maximum or

minimum pressure of curves of the same temperature, passes through
the point F. The saturation line under its own vapour pressure
disappears in the point M; the appertaining vapour-line in the point
M, both points lie with F on a straight line. ;
In fig. 14 the curves of different temperatures are al! united in
a plane; if, however, we imagine a temperature axis drawn per-
pendicular to this plane and also the curves in space according
to their temperatures, two surfaces are formed, namely the
saturation surface, under its own pressure of F and the appertaining
vapour surface. The first has its top in M, the second in M,; the
line MM, is situated horizontally. It is evident that the point F does
not coincide with the top M of the saturation surface under its own
vapour pressure but is situated somewhat lower and that the points
M, M and F lie in a same vertical plane. (Lo be continued).
46*

710

Botany. — ‘Dichotomy and lateral branching in the Pteropsida’.
By Mr. J. C. Scnouts. (Preliminary communication). *)
(Communicated in the meeting of Oct. 26, 1912).

In 1900 and more recently ?) Jerrrey argued that the correspond-
ence in structure of Filicales, Gymnosperms and Angiosperms jus-
tified the union of these three groups into a higher group, that of
the Pteropsida.

Palaeontological research has later rendered this conclusion more
probable *).

When on this account we assume a Closer relationship between
these groups, there naturally still remain many great differences
between them; one ‘of these is in the method of branching. For
whilst the Gymnosperms and Angiosperms without exception branch
by means of axillary buds (apart from adventitious buds), we find
the ferns are typically dichotomous ‘*). Merrenius *) described long
ago in ferns lateral buds in every kind of position (axillary,
next to the insertion of the leaf, under the insertion, half on the
stem and half on the petiole) but all this has been explained by
VeLenovsky as due to the formation of “stable adventitious buds ‘).
The distinction between dichotomy and lateral branching has always
been considered by all writers to be of great phylogenetic importance.

An investigation on branched tree-ferns has led me to the idea
that there may perhaps be no difference in principle between these
various modes of branching; in other words, that dichoto-
mous branching would be, in its essence, the same as the lateral
branching of ferns or Angiosperms. The fine material, mostly col-
lected by Mr. Koorpvrers, on which this investigation has been made,
will be described exactly in the detailed publication. Here I only
remark that in these trees ordinary dichotomy can sometimes take
place, as a reaction fo certain pathological processes, with a normal

1) A detailed paper, illustrated by plates, will appear on this subject in the Recueil
des Travaux botaniques néerlandais.

2) E. CG. Jerrrey. The Morphology of the Central Cylinder in the Angiosperms ;
Canadian Inst. Trans., Vol. 6, 1900. -— The Structure and Development of the
Stem in the Pteridophyta and Gymnosperms; Philos. Trans. R. Soc. London, Vol.
195, 1902.

3) See e.g. D. H. Scorr, Studies in fossil. Botany, 2nd Ed. London 1908/09,
p. 638,

ay Jd. VELENOVSKY. Vergleichende Morphologie der Pflanzen. Prag 1905, p. 245.

°) G. Merrentus. Ueber Seitenknospen bei Farnen, Abhandl. math-phys. Classe
k. Siichs. Ges d. Wiss. Bd. 5, 1861, p. 611.

6) l.c. p. 247.

711

angular leaf, such as, according VELENOVSKY, characterizes dichotomy
in ferns *).

In this process however, one of the two branches may also be
smaller than the other, in which case the larger branch places itself
entirely in the prolongation of the base. These cases gradually pass
into such in which one branch forms in every respect a prolongation
of the base, and the other is placed next to an ordinary leaf of the
stem as a thin branch or small lateral bud; this leaf we may then
still regard as the angular leaf of the dichotomy.

From these observations we may deduce that probably all bran-
chings in ferns, including those by means of VrLENovsky’s “stable
adventitious buds’, are to be referred to one and the same process
and also that it is not permissible to consider the lateral buds of
ferns as adventitious buds. It then further becomes highly probable
that the axillary branching of Gymnosperms and Angiosperms is due
to the same process. The only points of difference between the lateral
branching of ferns and that of these groups, are that in ferns the
bud is not always placed above the insertion of the leaf and that
by no means all leaves produce buds.

In the Conifers we find already an intermediate stage to the extent
that by no means all leaves have axillary buds, whilst in the cycads
another intermediate stage seems to the found, for in this group the
rare non-adventitious buds appear to be placed, not above, but next
to the corresponding leaf °).

If this is so then, the normal dichotomy, which occurs in rare cases
among Angiosperms’*) is a different, new process, a dichotomy of
the second order, as it were.

4} Lc. p- 246.

2) E. Warminea, Undersogelser og Betragtninger over Cycadeerne. Oversigt K.
Danske Vidensk. Selsk. Forh. 1877 p. 91. — H. Graf von Sotms LaAusacu, Die
Spoorsfolge der Stangeria und der tibrigen Cycadeen. Bot Zeitung 48, 1890, p. 197.

3) See my article ‘Ueber die Veristelung bei monokotylen Baumen II. Die
Veriistelung von Hyphaene’’, in Recueil des Trav. botan. Néerl. Vol. 6 1909p, 211.
The opinion expressed there on p. 232 that the dichotcmy of Hyphaene is the
first case described in the literature of dichotomy in a phanerogam is incorrect
since CHURCH in his ‘Relation of phyllotaxis to mechanical laws’ (London i904)
in the “notes and errata” at the end of the book (p. 352) already described the
dichotomy of fasciated heads of Helianthus.

712

Mathematics. — “On loci, congruences and focal systems deduced
from a twisted cubie and a twisted biquadratic curve’. I.
Communicated by Prof. Hk. DE Vrigs.

(Communicated in the meeting of Oct. 26, 1912).

141. We found in § 1°) a surface 2° as locus of the points P
for which the chord a of &* and the two chords 6 of &* are com-
planar; in the plane of those three chords then lies a ray s of the
tetrahedral complex discussed in the preceding § 7), so that the rays
s corresponding to the points P of 2° form a congruence con-
tained in the complex; we wish to know this congruence better.

Through an arbitrary point P of space pass six rays of the con-
gruence, thus w=6; for all rays s through that point form a
quadratic cone, the complex cone (§ 10), and the foci correspond-
ing to the edges of this cone lie on the ray s of P; this intersects
2 in 6 points and the rays s conjugated to these pass through P.
The number uw is called the order of the congruence.

Exceptions we find only for the points of £* and in the 4 cone
vertices. If P lies on #* then the conjugated line s is the tangent
in P, which now belongs itself to the complexcone of P, for it is
generated as line of intersection of the two polar planes of P itself
with respect to @,, ®,, which planes coincide with the tangential
planes to the two quadratic surfaces. The tangent s to 4* is now
however at the same time tangent to 2° and it contains therefore
besides the point of contact only 4 points of 2°; thus besides the
tangent only 4 rays of the congruence pass through P, from whieh
ensues that the tangent itself counts double.

The four cone vertices bear themselves quite differently. To 7,
e.g. are conjugated as rays s all the lines ofthe plane 7,7,7,=r,,
which plane intersects 2° in a curve &° of order 6 containing
T,,T,,7, as single points, the points of intersection with 4° on the
other hand as nodal .points; to each point of the curve a ray s
through 7’ is conjugated, so that through 7’, pass an intinite number
of rays of the congruence forming a cone. This cone can be deter-
mined more closely as follows. As of an arbitrary line s, in 1, the
two conjugated lines pass through 7;, the ray s, corresponding to
the points of that ray s, form a quadratic cone; now s, intersects
the curve £° in 6 points, thus the quadratic cone must intersect
the cone to be found in 6 edges.

Let us consider the point of intersection of s, with the edge 7,7;

1) See Proceedings of Oct. 26th, 1912, p. 495.
2) 1. c. p. 509.

713

of the tetrahedron. The two polar planes of this point now pass not
only through 7’, but also through 7, because the point itself lies
now not only in rt, but also in r, = 7,777; so the quadratic cone
contains the edge 7,7, and of course for the same reason 7,7’, and
T,T,. These same edges lie also on the cone to be found and that
as fourfold ones, which is easy to see when we consider e.g. the
line 7,7. This line intersects 4° in 7,,7, and in four points more;
to 7’, all lines of r, are conjugated and thus also particularly all
lines of +, through 7’, so that this plane (and for the same reason
the two other tetrahedral planes through 7’) separate themselves
from the cone; however, for each of the 4 remaining points of inter-
section the conjugated ray s is determined and identical with 7,77,
so that this line is indeed for the cone under discussion a. fourfold
edge. So the quadratic cone and the cone under discussion have in
common :

1. the three fourfold edges of the latter, 2. the 6 rays s, conju-
gated to the points of intersection of s, with 4°, thus altogether
ox<4+6= 18 edges; so the cone under discussion is of order nine.
If finally we see that this cone possesses three double edges too,
formed by the rays s conjugated to the three nodal points of 4°
lying in £®, we can comprise our results as follows:

For the congruence of the rays s corresponding to the points of 2°
the four cone vertices are singular points, as through these points pass
instead of 6, as in the general case, w' rays of the congruence ; these
form at each of those 4 points in the jirst place three pencils situated
m the three tetrairedral planes through that point, and in the second
place a cone of order nine with three double edges and three four-
fold edges, the latter coinciding with the three tetrahedral edges through
that point.

The cone of order nine must intersect the tetrahedral plane
*,= 1,T,T, in nine edges, four of which lie united in 7,77, four
others in 7',7,, so that only one is left; the latter is to be regarded
as the line s more closely conjugated to point 7), and it will
change its position if 4° changes its form, and passes through 7’, in
an other direction.

The complete nodal curve of the surface of tangents of £* consists
of four plane curves of order four lying in the four tetrahedral
planes and every time with 3 vertices of that tetrahedron as nodes;
let us now regard in particular the nodal curve lying in f,.
Through a point P of this pass two tangents of £* representing
the two chords 0 through that point; the line connecting the two
contact points passes through 7, and is an edge of the doubly

714

projecting cone having this point as vertex, and from this all follows
easily that that edge of the cone is the line s conjugated to the point P
of the nodal curve. The nodal eurve now intersects &° in 24 points,
of which 6 however coincide two by two with 7,, 7;, 7’, ; the lines s
conjugated to the 18 remaining ones are tbe lines of intersection
of the cone of order nine with the doubly projecting cone at the
veriex 7’.

The surface of tangents of £* is of order eight, it contains the 4
just mentioned plane curves of order 4 as nodal curves and the four
cone vertices as fourfold points; it intersects 2° in a curve of
order 48 having the cone veruces as fourfold points, the 24 points
of intersection with £* and the 4 times 18 points of intersection on
the 4 nodal curves as nodal points. For an arbitrary point of this
curve a chord a of &* and 2 chords 6 of &* are complanar; one of
these two chords 4 however is a tangent of &*. For one of the 24
nodal points on £° the same holds, as is easy to see; for each of
the 418 remaining nodal points on the other hand a chord a of
k® is complanar to 2 tangents of &*.

12. We now determine the second characteristic number, the
class » of the congruence formed by the rays s conjugated to the
points of 2°, i.e. the number of rays of the congruence in an
arbitrary plane. The locus of all foci of all the rays s lying in
an arbitrary plane « is according to § 10 a twisted cubic through
the four cone vertices; this intersects 2° in 18 points, but to these
belong the four cone vertices. To each of the 14 remaining ones
One ray s is conjugated, lying in the assumed plane; to a cone
vertex on the other hand all rays of the opposite tetrahedral face
are conjugated, and therefore also the line of intersection of that face
with a@, so that if we like we can say that in each plane lie 18
congruence rays, among which, however, then always appear the
lines of intersection with the four tetrahedral planes. So we prefer to
say that im an arbitrary plane tie 14 congruence rays and that from
the complete congruence the 4 jields of rays situated in the four
tetrahedral planes separate themselves. .

In § 8 we found that the double tangential planes of the surface
2,, discussed in § 7 of class 18 envelop a developable A, of class
9; they are nothing else than the focal planes of the points of 4%. :
The lines s they contain belong to the congruence we are discussing,
and these rays count double in the congruence because &* is for
2° a nodal curve; let us find the locus of these double rays.

If a point P describes the curve £*, then each of its two polar planes

715

X,, 7, with respect to ,,, envelops the reciprocal figure of a
cubic curve, i.e. a developable of class 3, and the tangential planes
of these two developables are conjugated through the points P one
by one to each other; for, a tangential plane 2, of the first devel-
opable has only one pole P and this again only one polar plane
with respect to ®,. Now the lines s are the lines of intersection of
the conjugated tangential planes of the two developables; they form
a scroll the order of which appears to be 6. Let us namely assume
a line 7; through a point P of this line pass 3 tangential planes me
of the first developable, and to these three planes z, are conjugated ;
if these intersect the line / in three points Q, then to one point P
three points Q are conjugated, but of course inversely too; through
each of the 6 coincidences passes one line s, so the line / intersects
the demanded surface in 6 points.

For each of the three points of intersection of &° with one of
the four tetrahedral faces the corresponding line s passes through the
Opposite vertex; the four cone vertices are therefore threefold points
of the surface. Moreover the surface possesses a nodal curve cut by
each generatrix in 6—2=4 points and which proves to be of
order 10; the four cone vertices are as points of intersection of 3
generatrices of the surface also threefold points of the ncdal curve.

The order of the nodal curve we determine again as in § 9 with
the aid of Scuusert’s formula:

2.é3 = 06 + 2. «9,

by conjugating each generatrix of the scroll as ray 7 to all others
as rays h. The symbol eg, the number of coinciding pairs where g
intersects an arbitrary line, is 6, viz. equal to the order of the sur-
face; the question is now how great is «0, the number of pairs gh
of which the components lie at infinitesimal distance and intersect
each other; these are evidently the torsal lines of the surface. We
shall show that their number is 8.

The rays s conjugated to the points of a line / describe a regulus
through the four cone vertices (§4) and so they cross each other all,
then too when they ‘lie at infinitesimal distance; they can intersect
each other only when line / is itself a ray s (§ 10); however, they
then intersect each other all and that in the same point, viz. the
focus of s. If thus two rays s corresponding to two points of &*
are to intersect each other, then their connecting line must be a
ray s; and if moreover these rays are to lie at infinitesimal distance
then the line connecting the points must be a tangent of 4°; so the
question is simply this how many tangents of 4° are rays of the

716

tetrahedral complex. Now according to one of the theorems of
HaLpHEN a complex of order p and a scroll of order n have pn
generatrices in common; the tetrahedral complex is quadratic, the
surface of tangents of 4° is of order 4 and so the number of common
rays is 8; so e6=8. From this ensues 2.¢8-=—8+ 2 6= 20,
«3 = 10. Now «3 represents the class of a plane section of our scroll
of order 6; by applying the first PLicker formula for plane curves
§9) we thus find d=16, a number we can control with the aid of

6p+eqteB=—agh (§9); viz.
op + 64+10= 36
6p = 20,

and this is twice the order of the nodal curve as we proved in§9.
Summing up we thus find: Zhe nodal rays of our congruence fori
a scroll of order 6 with 8 torsal lines and therefore also 8 pinch
points lying on a nodal curve of order 10 which is intersected by each
generatriz in 4 points and having the vertices of the four doubly
projecting cones of k* as threefold points.

§ 13. We shall inquire in this § into the scroll of the rays s of our
congruence, resting on an arbitrary line / and in particular on a
ray s. All rays s intersecting / form a congruence (2,2); for the
quadratic complex cone with an arbitrary point of space as vertex
intersects 7 in 2 points, so that through that point 2 rays of the
congruence pass; and an arbitrary plane contains of the complex cone
of the point of intersection with / likewise 2 rays, so that in an
arbitrary plane lie likewise 2 rays of the congruence. An exception
is made by the points on /, which are vertices of quadratic cones
of rays of the congruence and the planes through 7 containing an
infinite number of rays of the congruence, which evidently envelop
a conic because two of them pass through any point of the plane.
Among these planes are four, which are distinguished ‘rom the others,
because the conic which they bear breaks up into a pair of points,
and dualistically related to these are 4 points on 7 whose quadratic
cone breaks up into a pair of planes; the planes are those through
/ and the 4 cone vertices, the points are the points of intersection
of / with the four tetrahedral planes. In the plane /7, eg.
according to § 10 all the rays through 7’, belong to the com-
plex, so the conic in this plane must degenerate into 7’, and one
other point; or expressed in other words: of the two rays of the
congruence through a point of this plane one passes through the
fixed point 7’, so the second must also pass through a fixed point.

717

This point is a certain point of the line of intersection of the plane
(7, with the face rz, lying opposite 7; for, for an arbitrary point
P of tr, the complex cone breaks up into the pencil with vertex P
lying in t, and a pencil with vertex P lying in a certain plane
through P and 7’, and inversely for a plane through 7’,
our plane /7,, the complex conic breaks up into point 7’, and a
second point lying on the line of intersection of that plane with 7,
(§ 10). So the four singular points on / are therefore nothing else
but the points of intersection with the four tetrahedral planes.

Two congruences according to the theorem of HaLpnnn possess in
general only a finite number of common rays; however, the con-
gruence discussed above and the one deduced out of the points of
<2" possess an infinite number, therefore a scroll; for al/ complex
rays s cutting / belong to the former, and every time 6 of these
through a point of 7 belong according to § 4 to the second; the
two congruences have thus a scroll in common for which the line /
is a sixfold line. As furthermore according to §12 there lie in each
plane 14 rays of the second which as rays s cutting / also belong
to the former (and therefore, as we now discover, envelop a conic)
the scroll to be found is a 2” of order twenty and with a nodal
eurve which by each plane through the sixfold line / is ent in
4.14.13 —= 91 points not lying on /.

If a point P describes a line /, then the corresponding line s
describes a regulus through the 4 cone vertices (§ 4); and if we
wish to construct for that same point P the complex cone, then
according to § 10 we must determine the lines s which correspond
to the points of the line s conjugated to 7; from this ensues that
the regulus formed by the lines corresponding to the points P of 1
is the locus of the points P whose conjugated rays form the congru-
ence of the rays s which intersect 1. And so furthermore from this
ensues that the curve hk of order twelve alona which that regulus
and 2° intersect each other, is the locus of the poimts P whose
conjugated lines s form the just found surface 2*°.

Each generatrix s‘of the regulus contains 6 points of 2° or there-
fore of £’*; the corresponding lines s are the six generatrices of 2*°
issuing from the focus conjugated to the generatrix P of the regulus
on the sixfold line 7. The curve £'*? admits 6 nodal points, viz. the
points of intersection of the regulus with k*; the line s of the
reeulus through such a point intersects £2° in two coinciding points,
from which ensues that through the point ? on / conjugated to that
line s really only 5 rays s pass instead of 6; one of these, however,
viz. the one corresponding to the nodal point of /"*, is a generatrix

so e.g.

718

of the surface of the double rays of the congruence ($ 12), and
thus evidently a double generatrix of 2°. So: the 6 points of inter-
section of 1 with the surface of the double rays of the congruence
deduced from 2° are double generatrices of 2°.

The curve 4%? passes through the 4 cone vertices and the lines s
corresponding to them fill the tetrahedral faces lying opposite ; so we
can ask how &*° bears itself with respect to those faces. We now
have separated in § 12 of the complete congruence deduced from 2°
the four fields of rays in the tetrahedral faces; if we thus follow
4 through the vertex 7’, then to all points on either side of 7, every
time a completely determined ray intersecting / is conjugated; by
this also in +t, One ray is determined, so that 2*° has simply one
ot its generatrices in r, and therefore this plane as an ordinary tangential
plane. The cone vertices on the contrary are themselves singular
points ot 2*°. Our curve #** namely cuts t, in 12 points lying
on a conic and at the same time on the section £*° of 2° with r,,
to which belong the three cone vertices 7, 7,, 7’; the rays s corre-
sponding to these lie, it is true, according to the above, respectively
in T,, T;, T,, but they do not pass through 7’ (if let us say s conjugated
to 7’, had to pass e.g. through 7, it would have to pass for the same
reason through 7’, and 7’), however the rays corresponding to the
remaining 9 points of intersection do; so in the plane 7\/ nine
generatrices of 2°° pass through 7; they are the lines of intersection
of this plane with the cone of order nine, on which lie according to
§11 the rays s which are conjugated to the points of intersection of 2
with t,. The same holds of course for the planes through the remain-
ing vertices and /.

In such a plane the conic which must be touched by the 14
generatrices of 2°" degenerates, as we have seen at the beginning
of this §, into a pair of points; so in each of these four planes not only
nine generatrices pass through a cone verter, but also the five remain-
ing ones pass through another fived point, lying in the opposite face.
The vertices are thus for the nodal curve of 2? 4.9.8 =36-fold points,
the other points }.5.4—=10-fold points. lf we add these 36 + 10
points to the 45 points generated by the intersection of the two groups
of 5 and respectively 9 generatrices lying in a plane through a cone
vertex and /, we find back the 91 points of the beginning of this §.

If we add to the figure, as we are now studying it, another arbitrary
line m, then to this also belongs a regulus through the 4 cone vertices
cutting the regulus conjugated to 7 in a curve of order four through
the vertices; this biquadratie curve has with 2° twenty-four points
in common among which again the cone vertices; if we set these

719

apart for reasons more than once mentioned, then there remain
twenty; the rays s corresponding to these rest on 7 as well as on m,
i.e. the rays resting on 7 form a surface 27°. This in order to
control the result.

§ 14. We shall now try to determine the order of the nodal curve
of 2*, which is according to the preceding equal to 91, augmented
by the number of points unknown for the present, with which that
curve rests on /7; this number is connected with other numbers
which we must also calculate to be able to find the former, and to
this a deeper study is necessary of 2°, as well as of the figures
which are in relation with this surface.

A scroll possesses in genera! a certain number of pinch points and
torsal lines, and those of £*° can be divided into two kinds which
bear themselves very differently in the following considerations. To
the first kind we reckon the torsal lines whose pinchpoint lies on 7
but whose torsal plane does not pass through /; to the second kind
the dualistically opposite, thus those whose pinchpoint does not lie
on / (thus on the nodal curve to be investigated), but whose torsal
plane for it does pass through /.

A third kind might be a combination of the two others, torsal-
lines, whose pinchpoint lies on / and whose torsal plane passes
through 7; we shall however show that these do not appear on 2°.

We can get some insight in the appearance of these torsal lines if
we return to the regulus and the curve £* of the preceding §;
k** contains the foci of all generatrices s of 2*°, and the regulus is
the locus of all the rays s, which are conjugated to the points P
of /. Moreover lie in a plane throngh / fourteen generatrices of 2?°
and the foci of these lie on a cubic curve through the four cone
vertices. Let us now consider the generatrices of the regulus and the
eurve 4'*. A generatrix s, of the regulus intersects 2° in six points
and these lie on £'?, for 4°? is the intersection of 2° with the regu-
lus; the rays s corresponding to these six points are the generatrices
of 2°, which pass through a same point P of /, viz. the focus of s,.
If however s, has two coinciding points in common with /'*, then
two of the six generatrices through /P coincide, and this can
Lappen in two ways. The curve /** has namely 6 nodal points (viz.
on &?), and through each of these passes a line s, which has with
k*? besides the nodal point only four points in common; of the six
generatrices of 2*° through the focus P of s, two coincide and that
in a double geueratrix of 2*°, the number of which, as we know,
(§ 13) amounts to 6. Those double lines can be regarded as “full

720

coincidences’ in the sense of SCHUBERT, 1. e. as coinciding lines whose
point of intersection as well as whose connecting plane is indefinite ;
so they satisfy the definition we have given above of torsal lines of
the first kind.

[n the second place now however an s, can touch the curve £";
in this case the two coinciding rays s conjugated to the point of
contact form a ‘single coincidence’, i.e. two coinciding rays whose
point of intersection and whose connecting plane beth remain de-
finite; the point of intersection lies on /, the connecting plane however
does not pass in general through /, for then it would be necessary that
in the point where s, touches the curve £’? at the same time also
one of the cubic curves through the vertices were to touch that
curve, which can of course in general not be the case; so we find
torsal lines of the first kind. However, if tiere really were torsal lines
of the third kind, then there would have to be among the points of
contact of the rays s, with 4’? also some where at the same
time a cubic curve were to touch £'?; these particular points of
contact would then give rise to the torsal lines of the third kind.

The cubic conjugated to a plane 4 through / may have with &*°
two coinciding points in common; in this case two generatrices
lying in the same plane 4 coincide. This happens in the first
place for those planes 2 whose conjugated cubic passes through one
of the six nodal points of 4'?, and so we find again the nodal tines
of 27°; this, however, also takes place if a cubie touches /**, and
then we find a torsal line of the second kind; for the two rays s
conjugated to the point of contact coincide whilst their connecting
plane 4 remains definite. Their point of intersection lies in general
not on /, because the point of contact of £'° with the cubie is in
general not a point of contact of 4’? with a generatrix s, of the
regulus ; for those points however where that might be the case we
would find torsal lines of the third kind.

We calculate the complete number of points, where a line of the
regulus has two coinciding points in common with £'*, with the
aid of the formula of ScHuBert :

e=p+q—g')
which relates to a set of «' pairs of points. We can now indeed
obtain such a set by conjugating on each line of the regulus each
of the six points £"*, regarded as a point p, to the five others, which
are then named q ; each line of this kind bears then thirty pairs, because
each of the six points of /'? tying on it can be conjugated succes-

') Scoupert 1. c. p. 44,

721

sively as point p to the five others (which are then called qg), and
the whole number is o'. The quantity p in the formula points to
the number of pairs, where the point p lies in a given plane;
now this plane intersects %'? in twelve points, which we ean all
regard as points p; through each of these passes one line of the
regulus containing still five other points of £'*, which we shall call
q; it is then clear that there are 60 pairs py whose component p
lies in a given plane. The symbol q has the same meaning as jp, in
this case for the points g; however, as in our case each point of i"?
can be a p as well asa g, the quantity q is also = 60.. Finally
the letter g indicates the number of pairs whose connecting line
intersects a given line; now that given line intersects only two lines
of the regulus, on each of which 80 pairs pq are situated; g is
therefore 60, and in this way we find for ¢, the number of coincidences,
e = 60 + 60 — 60 = 60.

So there are sixty lines of the regulus containing two coinciding
points of £’*; 6 of them correspond to the double generatrices of
&2**, but a closer investigation shows us that these must be counted
double ; the remaining forty-eight are tangents of £4‘? and correspond
to torsal lines: so 2” contams forty-eight torsal lines of the jirst kind.

The formula ¢=p-+q— g, or written as: p-+q=g9-+¢, is namely
‘deduced by assuming a system of o' pairs of points p,g and by
projecting ihese out of a line /. If a plane 4 through / contains
p points p, we can connect the points g conjugated to these
by planes with /, so that. p planes are conjugated to 4; if inversely
a plane 4 contains g points g, then to this plane y others are con-
jugated, and thus is generated a correspondence (p,q) with p+ y
coincidences, which are evidently furnished by means of the coinci-
dences of the pairs of points themselves (¢) and by the pairs of points
whose connecting line intersects /.

Let us now apply this to our case. A plane / intersects /*? in twelve
points p; to each of these the five points 7 are conjugated lying
with p on a generatrix of the regulus, so that to 4 sixty other planes
are conjugated. A plane 4 through a nodal point DV of 4° however
contains of £'? besides D only ten more points, which give rise to
fifty planes; so the ten remaining ones must be furnished by D
itself. Now the gereratrix of the regulus through PD intersects 2°
besides in D only in four points more, the planes through these
and / count double in the correspondence, because PD itself counts
double in the plane /D, but this furnishes only four planes counting
double, or eight single ones; so the two missing ones must coincide
with the plane /D, i.e. /D is a double plane counting double (and

722

likewise a fourfold “branchplane’) Q. E. D. In § 17 we shall see
a confirmation of the considerations given here.

§ 15. In order to be able to point out the eventual existence of
the torsal lines of the third kind, we must include a new auxiliary
surface in our consideration, which we deduce from the tetrahedral
complex. All complex rays lying in one and the same plane envelop
a conic which also touches the four tetrahedral planes, and indeed
in § 138 we have already drawn attention to the fact that the
‘ourteen. generatrices of 2*° lying in a plane / through / are the
tangents of a conic; the auxiliary surface which we must introduce
to find the torsal lines of the third kind is the locus of these conies,
thus the locus of the complex conics lying in the planes 4 through J.
In each plane 2 lies one and through each point of 2 pass two of these
conics, as is easy to prove. For, let us imagine an arbitrary plane 2 and an
arhitrary point P on /, then 4 intersects the complex cone of P in
two rays s, and these are the tangents out of P to #* lying in 4;
therefore if 4° is to pass through P then the two tangents out of P
must coincide, and this takes piace in the two tangential planes
through 7 to the complex cone. The locus to be found is therefore an
2* with double line 1.

If a surface possesses a double line it is an ordinary pheno-
tenon that only a part is efficient, the rest parasitical; so applied
to our case that through certain points of / two real conics go,
through others two conjugated imaginary ones, and through the limit-
ing points between both groups two coinciding ones ; for the surface
we have here under discussion those limiting points are the points of
intersection of / with the four tetrahedral planes. Let us namely assume
the point of intersection s, of / with t,. The complex cone of S,
breaks up into two planes, viz. t, and a plane through S, and 7,
cutting t, along a line s, through S,; s, is nothing else but
the generatrix which 2° has in common with t,. Now the tangen-
tial planes through / to this degenerated cone coincide in the plane Js,,
which bears a complex conic touching t, in S, (with tangent s,) ;
this conic is the only one passing through 5S,.

Of great importance for our surface 2‘ are furthermore the planes
through / and the four cone vertices. We know i.a. that of the
fourteen generatrices of 2*° in the plane /7, nine pass through 7,
and the other five through a point 7,* lying in 1,, and really the
complex conic in this plane breaks up into the pair of points 7%,
7’,*, which means for the surface 2* that it is intersected by the
plane /7, (except in the nodal line 7 of course) in the line

723

7 zi i ‘ . °
T,7T,*, counted double, whilst the tangents to this conic degene-
rated into a double line, thus the complex rays in this plane can

only go through 7, and 7,*; the four planes IT; (i=1,...., 4
touch 2* along the four lines T, T;*(i=1,.... , 4), and the 8 points
i Li*@=1,....,4), are nodal points of 2*.

The nodal point 7',* lies in rt, and is characterized by the property
that its complex cone breaks up into the plane t, and the plane
T,*, so that each ray through 7,* cutting / is a complex ray. Let
us assume e.@. the plane 7)*, 7,*, 7,*; this cuts / in a certain
point Z and according to the preceding the lines L7,*, L7,*, L7y*
are complex rays. But if three complex rays lying in one plane pass
through the same point, then the complex curve in that plane must
degenerate into a pair of points, and this takes place only for the
planes through the four cone vertices; so the plane 7,* 7,* 7,7
passes through a vertex, in our notation 7’. And with this we have
proved the following property: the eight nodal points of 2 can bi
mae rimoeivo groups of four, 7,,....;T, and T,*,...., 77,
and the four tetrahedra having these points as vertices are simulta-
neously described in and around each other.

The surface $§2* is one of those already found and described by
Pricker in his ‘Neue Geometrie des Raumes’, Part 1, § 6,
p. 193 ete., on the occasion of his general investigations of quadratic
complexes. :

We shall now intersect the surfaces 2* and 2° with each other.
The section which must be of order 80 consists in the first place
of the line 7 to be counted twelve times, because 7 is for @* a
double line and for &?° a sixfold line; the residual section is thus a
curve of order 80 — 12 = 68. Now there lie in a plane 4 through
1 fourteen generatrices of 2’°, and these touch a conic lying on 2*;
so the residual section is a curve having with a plane 4 through /
fourteen points in common. However, we must keep in view that
the two surfaces touch each other in every ordinary point which
they have in common outside /; so the residual section must be a
curve to be counted twice, from which ensues that its order must
be 34; as it has outside / with a plane 4 only tourteen points in
common, it must have with / itself 20 points in common. It then
goes 9 times through each of the four points PE. :..72, see
5 times through each of the four points 7;* (c= 1,....,4) because
these points are respectively 9- and 5- fold points of £2*° (§ 13) and
nodal points of 2‘; the curve counted double has then 18- and
resp. 10-fold points, as should.

How does now a point of intersection of the curve found just

Proceedings Royal Acad. Amsterdam. Vol. XV.

724

now with 7 make its appearence? An arbitrary point is gene-
rated when in the plane 4 through that point and / a generatrix
of 2°° and a conic of &* touch each other; so a point on /is gene-
rated when in a certain plane 4 through / a generatrix of @° and
a conic of 2* touch each other exactly on /; then through the point:
of contact, however, pass two coinciding tangents of the conic, thus
two coinciding complex rays; or, in a better wording, whilst in an
arbitrary plane 2 through each of the 14 points of 7 lying at the
same time on generairices of 2*° two complex rays pass one of which
does not belong to £2*°, in the case under discussion the last
ray coincides with the former, so tbat it might look as if here a
torsal line of the third kind was generated; but it would have to be
possible to show that in the plane through 7 and such a line only
twelve other generatrices of 2*° were situated, or that whilst tend-
ing to such a plane two generatrices were tending to each other,
for which there is no reason whatever; so we conclude that 2
does not possess torsal lines of the third kind, and we shall find this
conclusion justified in future in different moments.

16. In a plane 4 through 7 lie fourteen generatrices of 27°;
through each of the points Z in which these generatrices intersect
/ five other generatrices pass which in general determine with 7 70
different planes; we shall conjugate these to 4. In this manner the
planes through / are arranged in a symmetrical correspondence of
order 70; we wish to submit the 140 double planes d of this
correspondence to a closer investigation. Such a plane is evidently
generated if for a certain point Z of / two of the 6 generatrices s
through that point lie with / in the same plane; the point Z is then
evidently at the same time a point of the nodal curve of 2*° lying
on /, for this double curve is the locus of the points of intersection
of all generatrices lying in a plane 4 through /. We shall now,
however, show that each suchlike plane as a matter of fact represents
two coinciding double planes. Let us assume to that end a plane 4
in which two generatrices s,,s, are lying, cutting / in two points
L,,L, lying close together. Through each of these last pass five
generatrices not lying in 2, and that in such a way that one of the
generatrices through ZL, lies in the vicinity of s, and inversely, whilst
the remaining ones lie two by two in each other's vicinity. If
we allow 4 to transform itself gradually into d, then that one gene-
ratrix through £4, coincides with s,, and inversely, whilst the remaining
ones coincide two by two in four double planes of the second kind

725

to which Jd corresponds as “branch plane’ '); if we remember that in
d, besides s, and s,, lie only twelve other generatrices of &?°, then
to d are conjugated 12*%5+2*4—68 planes not coinciding
with d. The two missing ones /o coincide with d, so that dis really
a double double plane. .

It is easy to see that the reasoning given here is literally applicable
to the six double generatrices, but not to the torsal lines of the first kind,
and much less to those of the second. The plane 4 through a torsal
line of the first kind is, it is true, a double plane J, but only a
single one, for besides that torsal line there are now in d still 13
other generatrices of 2*° (because namely the torsal plane does not
pass through /), and through the pinehpoint pass four generatrices
not lying in Jd; so to d are now conjugated 13% 5+4—69
planes, so that only one coincides with Jd. And as for the torsal lines
of the second kind, these give no rise whatever to double planes, but
only to branch planes. Let us assume again, as above, a plane A, in
which lie two generatrices s,,s, which almost coincide, but in such
a way, that their point of intersection lies at finite distance from
1. Through Z, and ZL, pass again every time five generatrices not
lying in 2, but now lying neither in the vicinity of s, nor ofs,, and
when 2 transforms itself into the plane through / and the torsal line
of the second kind, those ten generatrices coincide two by two; so
the torsal plane becomes a fivefold branch plane, but not a double plane.

Let us now draw the cenclusion from these considerations. If we
assume the double curve of 2*° to have w points in common with /,
then our correspondence contains #-—+- 6 (namely on account of the
double generatrices) double planes counting twice, and 48 (on account
of the torsal lines of the first kind, see § 14) double planes counting
once, so that the equation exists:

2 (7 + 6) + 48 = 140
out of which we find: 2 = 40.

So the double curve of 2*° rests in 40 points on 1 and is there-
fore of order 404+ 91 = 131.

A plane section of *° contains however not only 131 double
points, but 131 + 6 +15 — 152, viz. 6 on the generatrices and a
sixfold point on /; so it is of class 20 19— 2 152 = 76, so
that if we again apply the formula

e6—2.sPp—2.é9
we must substitute for «8 the number 76; and as ey = 20, because
the line of the condition g intersects 2* in 20 points, we find.
4) Em. Weyr, “Beitrage zur Curveniehre,’ pp. 9, 10.

47*

726

¢6—2.76 —2.20—112.

This number comprises all pairs of lines of the surface whose
components lie at infinitesimal distance and intersect each other,
thus the 6 double generatrices, the 48 torsal lines of the first kind
and the still unknown number of torsal lines of the second kind:
so 2° contains 58 torsal lines of the second kind.

For a congruence is characteristic, besides the number of rays
through a point (in our case 6) and in a plane (in our ease 15),
the number of pairs of rays which belong with an arbitrary line
to a pencil, the so-called rank; according to the preceding this number
is nothing but our quantity 2, thus 40; the congruence deduced from
2?" is therefore a (6, 14, 40).

The results found above allow being controlled, by our finding
the 4131 —524 points of intersection of the surface 2* with
the nodal curve of 2%. The greatest number of these points we find
united in the points 7; and 7;*, the eight nodal points of 2*. A
point 7; is a 36-fold point of the nodal curve (§ 13) and counts
thus for 72 points of intersection; a point 7;* is a tenfold point of —
the curve and counts thus for 20 points of intersection, together
4 >< 92 = 368. In the 40 points where the nodal curve rests on /,
the curve meets the double line of £*; so this gives 80 points. Ina
pinch point of a torsal line of the second kind the nodal curve traverses
2* in a single point of intersection. Let us assume e.g. a plane 4
through / and such a torsal line as well as two planes /, and 2, on
both sides of 4 and in the immediate vicinity of 4; then in 4, e.g.
two generatices of £*° will nearly coincide, so their point of inter-
section will almost lie on the conic of &* lying in this plane; in 4
itself this point of intersection really falls exactly on 4’, and in 4,
the two tangents have become conjugate imaginary ; their point of
intersection has nevertheless remained real, i. e. the nodal curve
naturally continues its course but now lies inside £?; so it has inter-
sected the surface. As 2%" possesses 58 torsal lines of the second kind
we find 58 new points of intersection.

We must finally discuss the 6 double generatrices of 2*° which
bear themselves as regards the nodal curve about the same as torsal
lines of the second kind do. We must not lose sight of the fact that
a double edge d of 2° is a singular ray for the congruence but not
for the complex; so if it intersects / in D, then the complex cone
of D shows in no way anything particular; the plane 4 through
/ and d contains thus two different generatrices of that cone, of
which d is one. The consequence is that the conic of @* in 2 must
touch the line ¢ in some point or other not lying on /, through

727

which point the nodal curve passes, just as with a torsal line of the
second kind; and indeed the plane 4 through d contains besides d only
twelve generatrices of ?°, intersecting each other mutually in
4.12.11 = 66, and d in 12 points counting double, which amounts
together to 66-+ 24—90 points of the nodal curve; so one is
missing, but is the point of intersection in a closer sense of the two
generatrices coinciding in d, and according to the above this cannot
lie on /. In passing we learn from this consideration that the nodal
curve of 2*° touches each plane through | and either a torsal line of
the second kind or a double edge in twelve points lying either on that
torsal line or on that double edge.

That a double edge, however, does not bear itself altogether as a
torsal line follows from a repetition of the above given consideration
with the three planes 4,, 2, 2,; for now in 2, as well as in 2, two
real generatrices of 2° will lie. Nevertheless the nodal curve has
here with 2* not only a contact by two points, but even one by
three points, so that the plane of osculation of the nodal curve
coincides with the tangential plane of 2‘, and the nodal curve touches
one of the two branches of the section of £* lying in the tangential
plane.

Indeed, it is clear that besides the 368 + 80 + 58 = 506 points
of intersection already found no others are possible than the 6 points
on the double edges, which occupy us here; for each point of inter-
section not lying on / must be the point of contact of a generatrix
of 2? with a conic of &*, so a pinchpoint of a torsal line of the
second kind, or of a double edge; as there are 6 of the latter sort
in evidence and 524 — 506 = 18 points missing, each of those six
points must be counted three times.

Physiology. — “The posterior longitudinal fascicle, and the manege
movement.’ By Dr. L. J. J. Muskens. (Communicated by Prof.
C. WINKLER).

(Communicated in the meeting of October 26, 1912).

In a series of experiments in cats by means of different needles
a lesion was caused in the cerebro-spinal axis, between the posterior
commissure and the vestibular nuclei, avoiding the .V-vestibularis, of
which the lesion invariably causes such vehement rolling movements
to the side of lesion, that the observation of the manege-movements
is impossible. The microscopical control of the lesion and its results
was performed after the method of Marcut.

728

In three cases both posterior longitudinal fascicles were cut. With-
out exception the posterior longitudinal bundles were found degene-
rated, as well above as below the lesion, but not always equally
heavily. Especially to the oral side the number of strongly stained
fibres rapidly diminishes, reminding of Grr and Toorn’s observation °),
which particularly strikes one in 114, where within the domain of
the oculomotor nuclei the lesion was performed. As well the ascend-
ing as the descending degeneration involves in these cases the whole
area of the longitudinal bundle.

The physiological result is naturally different, according to the
additional lesion of the cerebral stem. The spontaneous locomotion is
always seriously interfered with. Forced movement, in the form of
manege-movement, is as a rule absent and the stature of these animals
answers to the description of the attitude after exstirpation of both
labyrinths. Only in case 90 as an exception manege-movement to the
right was observed, which in this case should be attributed to the
fact, that a bloodextravasation had happened at the cross-section of
the left longitudinal bundle, which had caused during some days
an asymmetrical irritation. This is inferred from the results after
unilateral section of the longitudinal bundles.

In a second series of experiments a unilateral lesion of the
longitudinal bundle was applied, with little or no lesion of the Drrrmrs
Complex. In these three cases regularly an ascendent degeneration
of the lateral part, especially of the severed longitudinal bundle was
observed. Downward equally degeneration in the middle part of
the cross section of the bundle was found, whereas also on the other
side in the same field some degeneration was noted. Equally regu-
larly in these cases manege-movement to the side of the non-sectioned
longitudinal posterior bundle was observed during life; solely on 144
also the allied symptom of conjugated deviation of head and eyes
was noted.

In a third group a unilateral lesion of the Drrrers Complex was
caused. In this series of animals the results were neither anatomic-
ally, nor physiologically so easy to understand as in the two first
groups. Regarding the degenerated fibres in the posterior bundle,
they are in all cases far less numerous, compared with direct lesion
of the bundle; also here it holds good more than for group 2, that
degeneration, limited on one side only, is a rare occurrence; but in
all cases very decided predominance of the degeneration on one side
was found. Of these (7) animals in one (158) a total longitudinal
lesion was performed at the left side of the left longitudinal fascicle,

1) Brain 1898.

729

in such a way, that all fibres from the left Drirers Complex towards
the posterior bundles and the raphe, had been eut leaving the left
longitudinal bundle practically intact. Solely in this animal both
longitudinal fascicles were upward degenerated, on the right side more
heavily than on the left side. In three animals the lesion struck
the Drirers nucleus (118, 113 and 99), In these eases in the contra
lateral longitudinal bundle a limited degeneration was found. In
three animals (95, 93 and 111) the most proximal-dorsal cell group
of the vestibulary-complex (BrcHTerew’s Nucleus) was struck; in
this series a very limited degeneration on the side of the lesion
in the lateral part of the bundle, rather mixing with the fibres ot
the fasc. Durrers ascendens (WINKLER *‘), could be followed up. All
these ascendent degenerated (more medially in the areal of the
longitudinal bundle after lesion of Derrrmrs nucleus, more ‘laterally
afier lesion of Brcaterew’s nucleus) fibres can be followed up to
the oculomotor nuclei, where as in all cases, some strands of fibres
could be traced up to the nucleus of the posterior commissure. ‘The
descending degeneration after lesion of the Dkrrrers complex is
usually not very extensive, but present on both sides, regularly
stronger on the side, where there is more marked ascending degene-
ration.”) These fibres occupy, lower down, more and more a ven-
tral situation and can be traced down to the cervical medulla and
lower down. For reason of comparison one of PRrosst’s experiments *)
has been added to the table.

The degeneration found in these cases seems to prove, that solely for
the distal nuclei of the vestibulary complex (especially the triangular
part) Fusn’s dictum holds good, that the structural connection between
the Duirers-complex and the longitudinal bundle is a crossed one.
Here the results, obtained by GupprN’s method, are reinforced by
those of Marcui’s method. On the other hand with the latter method
it appears hardly subject to doubt, that the connection between brcn-
TEREW’S nucleus and the longitudinal bundle is mainly a homo-lateral
one, these fibres mixing with the fase. Drivers ascendens.

Regarding the phenomena observed during life, it is surprising
that, equally regularly as in group 2 manege-movement was observed
to the non-sectioned side, equally regularly also in these animals

1) Central Course of the nervus octavus. Verhandelingen der Koninkliyke Aka-
demie van Wetenschappen. Tweede sectie 1907.

2) This detail seems to be able to support Ramon y Cayat’s and Monakows
contention, that the fibres from the Detrers-complex to the posterior longitudinal
fascicles all split up in an ascending and descending branch.

5) Jahrbiicher f. Psychiatrie 1901. P. 7 of the separate paper.

730

manege-movement was noted to the side where the P. L. B. shows
the least degeneration (the lesion being on the same or on the other
side). Some reserve I have to make here for the homo-lateral dege-
neration in the longitudinal bundle after lesion of BecaTEREw’s nucleus.
For in 95, being the animal, that produced the most classical circus-
movements to the left, a very local lesion was found in the middle
part of the ingoing fascicles of the N. vestibularis. It can a priori
not be excluded, that such a direct and local lesion of the nerve may
cause manege-movement to the other side, in the same way as usually
any lesion of the vestibulary nerve causes vehement and long lasting
rolling movements to side of the lesion’). Such an interpretation seems

however very improbable indeed. As to 111, the lesion was here

accompanied by an haemorrhage and rather extensive. The physio-
logical analysis of the Drirers-complex can go, I think, a little further,
in that a lesion of the caudal part of the complex, e.g. on the right
side, as well as a lesion of the proximo-dorsal part (BECHTEREW’S
nucleus) of the left side resulted in an ascendent degeneration in the
P. L. B., of the left side, and also produced equally circusmove-
ments to the right. This cireus movement to the right side being
clicited from an anatomical entity on either side, we are led to believe,
that a double sided connexion of either horizontal semicircular canal
with Deirers nucleus and a proper exteusion of Ewa.ps experiments
might clear up this point.

From these results I think it must be admitted, that the physio-
logical function of the P. L. B., or at least one of its functions, is
intimately related to the coordinated locomotion in the horizontal plane
of eyes, head, trunk and extremities. A similar suggestion of sucha
relation is often found in literature, but about the precise form and
direction resulting from such coordination none of these researches
give information (EDINGER) *).

In a fourth group of experiments (in 6 animals) a lesion was applied
in the region of the corpora quadrigemina anteriora, of the commissura
posterior and of the red nuclei. In four cases descending degeneration
from that region into the posterior longitudiual bundle, exclusively
on the side of lesion, was found. This degeneration, sometimes amount-
ing to no more than a few fibres, is lost sight of high in the medulla
oblongata, especially in the region of the abducens-nuclei. In 2 of
these cases accurately the origin can be followed in the series and
it appears that the nucleus of the posterior commissure is involved

1) Compare: Studies on the foreed movements. Journal of Physiology. XXXI.
Ne. 3 and 4. 1904.
*) Vorlesungen. 1912, P. 110,

Group LESION

T Both P. L. B. sectioned:

Lesion high, in region of corp. quad. post. 114
low, in the vestibulary region 92
” »» » » ” ' (with an hae-}| 90
morrhage on the left P. L. B.)
II | One P. L. B. sectioned:
Pons-region Right | 139
” Left 91
: Left 119
Hemisection of midbrain ine
Probst !)
Ill | One-sided lesion of vestibulary nuclei
Left vestibulary nuclei cut off from raphe (with exstir- 158
pation of left frontal hemisphere)
Right nucleus Deiters (pars triangularis) 118
Right nucleus Deiters (pars triangularis) 113
Left nucleus Deiters (pars triangularis?) 99
Right nucleus Bechterew (+ N.? vestib. ?) 95
Right nucleus Bechterew 93
Left nucleus Bechterew 111
IV | Lesion of upper quadrigeminal region with exclu-
sively descending degeneration in the P. L. B.
Nuc. commissurae post. Right | 107
Superficial lesion Corp. quad. ant. Right | 106
Lesion of lateral part of red nucleus Right | 108
Nuc. commiss. post. Right | 109
” ” r Right 98
Lesion of region of red nucleus Left 61
V_ | Lesions of cerebral hemisphere.
Ablation of frontal region Right | 127
” ” " » Right | Cat I
(Probst)
Ablation of tot. hemisph. (with thalamus-lesion) Left 186

') Jahrbiicher f. Psychiatrie 1901. P. 72 (of separate paper).

Ascending degen®

Total (+ F. Deiters
asc.)

Tot. (med. part esp.)

Total (latero-dorsal
part esp.)

Lateral

Diffuse and little
(partially descend.)

Moderate (med. part,
higher esp. lateral)

Strong (idem)

Total

gn of P. L. B. Descending degeneration of P. L. B.
Circus ; (distally to the lesion)
a Duration

movement

Left Right

Total, lower down(in Total, lower down (in
medulla) ventro-med.. medulla) ventro-med.

edial especially 0 Total lower down Total, lower down

er F. Deit. asc.) ventro -medial ventro-median

tal and strong To Right 9 days | Total, lower down | Strong and complete,

(+ F. Deit. asc.). ventral lower: ventral

rong, esp. lat. part 5 Lett 1D a Little Ventro-median part
(to lumbar region)

yme fibres » Right ae Total, lower down | A few fibres

ventro-median

me fibres » Right Oars Tot., median part esp. | Moderate

2generation pn ete ZU 0 Degeneration
|

teral part ene Tile “es Lateral part (strong) Medial part, rather
| diffuse

teral part » Right 1 day Medio-ventral (till | Lateral(+F.Deit asc.)

dorsal region)

asc. Deit. asc. » Right 8 days * -

»w fibres eweit Wks te 0 Few fibres (med.), to
j dors. part of medulla
w fibres (+ Fasc. ,, Left Ss 0 Latero-ventral, to
Deit. asc.). cervical region
em 5) eel 6+ 0 Little, lateral, to low
in medulla spinalis
0 » Rignt Doe Latero-ventral Few fibres
|
» Right (35 aa Medio-dors. (not lower
than striae acust.)
0 Few fibres
oer) 2a _ Fasc. interstitialo-
| spinalis
» Right 1 day | Few fibres
» Right Is | Very little
» Left 3 days | Well degenerated (to Little (medial), to

medulla oblongata;, tmedulla; there more
there more ventral)! ventral)

0 0 | 0
0 0 | 0
To Left ean Some fibres to exit |

of N. Trigeminus

731

in the region of the direct lesion or of the local malacy. My supposition
that this nucleus must be regarded as the origin of this commissuro-
medullary bundle, gains in probability by the findings in 2 cases
(106 and 108), where this bundle was not degenerated. In 106 the
lesion involves exclusively the superficial layers of the anterior corpus
quadrigeminum, but leaves the nucleus of the commissure intact. In
108 an extensive sagittal lesion in that region was found. Here from
the surroundings of the red nucleus a strand of degenerated fibres
can be followed in the homolateral posterior bundle, which however
does not disappear at the level of the n. abducens, but can be traced
far lower down, as far as in the dorsal spinal cord. Problably we deal
here with the homolateral tecto-spinal bundle of Prossv.

As to the forced movements, it is remarkable, that all these four
animals with the degeneration of the commissuro-medullary bundle
performed circus-movements for a skort period to the side of the
lesion, whereas the animal with lesion in the corpus qudrigeminum
anterius solely, and that with lesion of the nuc. ruber exclusively
did not do so.

In relation with these cases we have to mention two animals with
extensive lesion of the cerebral hemisphere. Whereas in 127 solely
an extensive exstirpation of the anterior pole was performed, leaving
the thalamus opticus intact, in 186 the whole hemisphere was exstir-
pated and also the thalamus wounded. Only in this latter animal on
the operated side some degenerated fibres were found, of which the
course is exactly that of our commissuro-medullary bundle. This latter
animal showed decidedly circus-movements to the operated side during
some days.

From these results we conclude, in agreement with current anato-
mical notions, that the posterior longitudinal bundle contains fascicles
of different source and end-station. At any rate in the medial portion
of the P. L. B.-formation 3 bundles must be distinguished, two
ascendent and a descendent one dealing with the coordinated locomotion
in the horizontal plane. Innermost within the medial portion of the
P. L. B. we find the descending commissuro-medullary bundle ; next
comes the crossed ascendent Driters P. L. B.-bundle, then comes the
homolateral BecntErEW-P. L. b. bundle, containing fewer fibres than the
crossed one. The latter bundle lies entirely within WiINKLER’s Fase.
Deiters ascendens. In a next paper ihe physiological analysis of the rest
of the P. L. b. formation wil! be dealt with. There are many prepara-
tions in my collection, which tend to prove (as far as Marcal-work is
entitled to do so), that, as is suggested by the authors, the vestibulary-
P. L. B. fibres, as well the crossed as the homolateral ones, in the

732

P. L. B. formation bifureate, one limb ascending to the oculomotor
nuclei and the nuc. of the posterior commissure, the other passing
down to the cord.

The descending bundle has its origin exclusively, so it appears,
in the nue. commissurae posterioris (VAN GEHUCHTEN, Propst) and
can be traced as far as the homolateral abducens nucleus. The oral and
distal final stations of both coordinating bundles are therefore found
in the same level, a detail with seems particularly inviting to study
here the physiology of the bundle as a common final path (SHEr-
RINGTON). For the study of the mechanism of the circus and rolling-
movements undoubtedly labyrinth- and neck-reflexes described by
Magnus and Dr. Kiryn’) as well as Baranyi’s experiments?) have
to be considered.

As to the function it can be hardly considered accidental, that
in my experiments the animals with ascending degeneration in the
P. L. B., on one side (e.g. on the mght side) performed circus-
movement to the other side, to the left; whereas the animals with
a (from the Nuc. comm. post) descending degeneration e.g. on the
right side, did their manege-movements to the diseased side. Prosst’s
law *) that ‘‘a hemisection of the brainstem anterior to the red
nuc. caused maneze-movements to the diseased side; a hemisection
caudal to the red nucleus to the healthy side’, seems therefore,
well founded, but with this important restriction, that the nue. com-
missurae posterioris and not the red nue. is the origin of the commis-
suro-medullary bundle, and that not hemisection, but a simple lesion
of one longitudinal bundle will suffice, to cause the cireusmovements.

By comparison with a number of other series and subtraction
of the phenomena during life, it can be proved, that lesion of the
great descending tracts (pyramidal, rubro-spinal, tecto-bulbar, vesti-
bulospinal, and ponto-spinal tracts), of the most important ascending
systems (Gowers’s and FLecusie’s tract) the lemniscus and cerehello-
rubral tracts have nothing to do with this function. I am not in a
condition to deny nor to affirm CLAarke and Horsixy’s supposition ‘),
that the ponto-cerebellar connections should have to do with the
“mouvement de manege” but I do think as long as there is no proof
forthcoming, regarding a centre for equilibration in the temporal
lobes, that after these experiments there is no need to fall back upon
any such conjecture.

1) Archiv. f. d. gesammte physologie, 1912. Bd. 145. S. 455.
*) Neurologischer Centrallblatt. 1912.

8) Loc. cit. p. 41.

*) Brain 1905

In the course of these experiments, having specially in view the
posterior longitudinal bundle and the Deirrrs-complex, it appeared,
that — at least for this system — in relation to the disturbances observed
during life one has to distinguish three different modes of traumati-
eal lesion. 1. Total destruction of a cell-complex or bundle through
the instrument used, with renders the structure irrecognizable, the
tissue being totally or partly replaced by a moderate bloodextravasation.
After this lesion invariably a total degeneration of all fibres arising
from or passing this region oecurs, if care be taken, that the specimen
does not stay too long in Mcuixrs fluid. 2. Malacy of a region
which causes in a selective way some systems of fibres to degenerate,
whereas other systems apparently continue to be nourished and pro-
bably also continue their function’). In view of Konnstamm’s and
Monakow’s findings it appears, as if the great, the middle-sized and
the small cells of the Derrers-complex suffered unequally in their
nourishment, if this structure happens to be involved in such a
malacy. 3. If an extensive haemorrhage occurs and exerts compression,
irritative symptoms appear of the same order”) but more vehement,
than those which are caused hy the dissolution of the medullary sheath
and the moderate irritation, caused by this process.

In judging about the physiological consequences, it must be kept
in view, that every lesion after 1. and 3. is always found sur-
rounded by a zone of malacy, and finally, that in a case with volu-
minous haemorrhage in the brainstem the general brain-compression
may mask completely the forced movements.

It is quite natural, that in different experiments the vestibulary
P. L. B.-complex was repeatedly wounded on more than one loca-
lity. Regarding the physiological effect it appeared, that a lesion of
the N. vesiibularis itself predominates above a lesion of its nucleus,
and the latter again dominates above a lesion of the posterior longi-
tudinal bundle.

1) So I found in 102, that the left longitudinal bundle passed such a malacy in
the upper pontine region. The descending commissuro-medullary bundle was degene-
rated and the animal had shown the physiological consequence of this degeneration;
the ascending vestibulary-P. L. B. fibres were not degenerated.

2) It is interesting to note, regarding the nucleus of the posteror commissure,
tbat afler E. SacHs’ experiments (Brain 1909, p. 180) direct electrical stimulation
of this region causes conjugated deviation to the opposite side; which evidently
corresponds to the effect, described in this paper, of the stimulation exerted on the
nucleus of the posterior commissure by the degeneration of a number of ascend-
ing fibres, running in the P. L. B. and ultimately arriving in this nucleus. The
circus movement in many of my experiments was accompanied by conjugated
deviation to the same side; both phenomena evidently being narrowly related,

734

Geology. — “On the formation of primary parallel-structure in
lujaurites.” By Dr. H. A. Brouwer. (Communicated by Prof.
G. A. F. MoLeNnGRrAaFr).

(Communicated in the meeting of October 26, 1912).

In an important memoir of the late Professor N. V. Ussine *)
we find a detailed discussion on the question of the origin of schis-
tose structure in lujaurites. It is explained as a consequence of
fluctuation, in contradiction to Ramsay’s*) view, who admits a slow
cooling and undisturbed crystallization of the magma for the rocks
of the peninsula of Kola.

In my description of the Transvaal nepheline-syenites*) the name
lujaurite was extended to rocks without parallel-structure, charac-
terized by the oceurrence of fine-needle-shaped crystals of aegirine
in abundance. The parallel-structure where it occurs was explained .
as aconsequence of a crystallization influenced by one-sided pressure,
which view will be now more explicitly explained.

(reological connection with accompanying rocks.

In the peninsula of Kola no remains of the roof of the intruded
batholite have been preserved and thus it is not certain whether
the lujaurites are the first products of consolidation in the marginal
zone of the igneous mass. In the Pilandsbergen (Transvaal) the
schistose varieties are often still surrounded by a border of nephe-
-line-syenitic or syenitic rocks, whilst in the Greenland intrusions
which have been very carefully examined, the lujaurites form the
lowermost rocks of a stratified batholite which has been denuded.
The last mentioned rocks are covered by a very coarse-grained
foyaitic rock (naujaite) the erystals of which are sometimes a few
decimeters large; it is characterized by sodalite poikilitically surround-
ed by all other minerals. Pegmatitic segregations are found chiefly in
a horizontal position, whilst in the rock itself a more or less hori-
zontal stratification in thick layers is indicated. Towards the upper
portion the naujaite gradually passes into a sodalite-foyaite, whilst
downwards it is connected with the underlying lujanrites by a breccia-
ted zone of transition. This breccia-zone is formed by strata of lujau-

1) N. V. Usstne, Geology of the country around Julianehaab, Greenland. Med-
delelser om Gronland, vol. XX XVIII, and Muséum de Min. et de Géol. de |’Univer-
sité de Copenhague, Communications Géologiques N® 2, 1911.

2) W. Ramsay, Das Nephelinsyenitgebiet auf der Halbinsel Kola, | and Il. Fennia
11 and 15, N.2. Helsivgfors 1894 and 1899.

5) H. A. Brouwer, Oorsprong en samenstelling der Transvaalsche nephelien-
syenieten. ’sGravenhage, Mouton & Co, 1910.

ee I
==
* om

735

rite entirely surrounding the lenses of naujaite and increasing
in number towards the bottom, so that a structure is formed which
reminds of the “Augenstructur”’ of some gneisses if this were thought
many times magnified. Commonly the lujaurites of the breecia-zone

are black (arfvedsonite-lujaurites), but occasionally —- and this is of
importance for the genesis — we find also green aegirine-lujaurite,

bounded on either side by black arfvedsonite-lujaurite, thus proving
that cifferentiation has taken place.

The rocks of the lujauritecomplex of Greenland, which is more than
600 m. thick, are, as a rule, more fine-grained than those of Kola
and Transvaal and contain a greater quantity of dark constituents.
Complexes of kakortokites alternate with the lujaurites; these are
foyaitic rocks, distinguishing themselves from the normal foyaites by
a greater percentage of dark minerals; they are more coarse-grained
than the Injaurites, and their average composition corresponds pretty
well with that of the latter. Light-coloured, red and dark strata al-
ternate, and it is peculiar that the same succession constantly returns,
and, in the thickest parts of the complex, repeats itself about forty
times. As in the breccia-zone of the lujaurites, the kakortokites likewise
envelop fragments of naujaite.

The above-mentioned variations originating from the same parent
magma are likewise met with among the Transvaal rocks; their
mutual connection here, however, is more irregular, and can less
clearly be observed in the field because they are in most places
covered by other rocks.

Mechanism of the intrusion of the Pilandsbergen.

It is peculiar that in the territory of the Pilandsbergen effusive
rocks are found in large quantity between the deep-seated *) whereas
they do not occur in the surrounding granites and norites.

It is very likely that, in the Pilandsbergen and its environs origi-
nally a roof of volcanic rocks has covered the deep-seated rocks,
because elsewhere in the igneous complex of the Boschveld a thick
voleanic series still forms the roof of the deep-seated rocks, which
is intersected by dykes of tinguaitic and camptonitie rocks °*).
In connection with the intrusion of the foyaitic magma which is
younger than both the granites and norites, the roof has locally sunk

1) H. A Brouwer, loc. cit. p. 16.
2) H. A. Brouwer, loc. cit. p. 35 and 89.
P. A. Waaner, Note on an interesting dyke intrusion in the upper Water-
berg system. Transactions Geol. Soc. of South Africa 1912, p. 26 sqq.

736

down, and whilst it has disappeared everywhere else in the neigh-
bourhood by erosion, we see the remains preserved just on these
sputs where the roof has given way.

Consequently the massive of the Pilandsbergen does not belong
to that important class of intrusions, to which tangential pressure
in the portion of the earthcrust in which the intrusion takes place
is necessarily connected, which is proved moreover by the existence
of a great number of vertical dykes of vast extension. Blocks
sinking elsewhere cannot have been the cause of the intrusion
of the magma, as the roof has sunk down exactly on_ those
spots, where the foyaitic magma has risen. Certainly pressure and
faults are directly connected with the mechanism of the older chief
intrusion of the Boschveld*), and also the young foyaitic intrusions
are chiefly restricted to those spots where tension has taken place,
and consequently the pressure has been diminished.

Thus both the sinking down of the roof and the intrusion are
regarded as consequences of the same common cause, which occasioned
the relief of pressure; the question in how far the sinking down of
fragments of the roof into the magma underneath has contributed to
the batholitic invasion (DaLy’s “overhead stoping’) is in this respect
of secondary importance; we must however admit that sinking down
and intrusion took place partly simultaneously. .

Similar conditions are found likewise in the Greenland rocks.

Formation of the schistose stuctures.

The formation of these structures in consequence of flow in the
crystallizing magma is improbable for the following reasons:

1. For a great verticai distance the direction of the plane of schis-
tosity by parallel-structure remains the same. Consequently we should
have to admit in a_ batholite for a considerable height a gradual
decrease of rapidity in the flowing magma. Ramsay has already pointed
out the improbability of this theory.

2. The aegirine-needles lie for the greater part parallel to the plan
of schistosity but in it they are irregularly distributed. In a flowing
magma the needles would have a tendency to arrange themselves
parallel to the direction of the flow. Indications of such an arrangement
are missing.

3. The lujaurites vary and by transitions are connected with other
rocks without parallel structure. If we admit flow-structure, then other

1) G. A. F. Motenaraarr, Geology of the Transvaal. Johannesburg 1904, p. 50
sqq. A. L. Hatt, Ueber die Kontaktmetamorphose an dem Transvaalsystem im
dstlichen und zentralen Transvaal. Min. u. Petr. Mitt. XXVIII, Heft 1, 2, 1909.

737

rocks being crystallized almost simultaneously as well above as below
with the lujaurites, likewise ought to show a parallel structure.

4. In the breccia-zone between the Greenland lujaurites and the
naujaites differentiation towards the marginal zones occurs. As the
lujaurites between the naujaite-blocks distinguish themselves from
the others only by the fact that the parallel arrangement of the
composing minerals follows planes which bend round the naujaite-
blocks, a continual current ought necessarily to have taken place also
between the naujaite-blocks, which would have prevented the diffe-
rentiation.

An other explanation for the strongly varying structures we have
described will now be suggested.

The parent magma of all these rocks is characterized. by a high
percentage of pneumatolytic gases and connected with it a strong
power of crystallization and a thin fluidity maintained to a compara-
tively low temperature. As the different foyaitic rocks of Greenland
and most likely also those of the Pilandsbergen have crystallized
with only very slight differences in time, the temperature can only
be a secondary factor in the mode of formation of these greatly
varying structures. The differentiations caused by fractional crystal-
lization or by separation according to the specific gravity may
likewise be left out of account, as they modify chiefly the compo-
sition and not in the first place the structure of the rocks.

From such a magma coarse granular varieties will be formed
under undisturbed conditions of crystallization, whilst poikilitie strue-
tures can be explained by differences in power of crystallization, in
connection with affinity and with the relations between the quantities
and the solubilities of the components. For the fine granular varieties
a rapid mode of crystallization is essential, but movements in the
magma are not required. This rapid erystallization can be caused
by the escape of gases from the magma which remained thin fluid
down to a low temperature on account of the great percentage of
pneumatolytic gases kept in solution, whereas by the escape of the
gases it suddenly becomes viscous, so that large crystals cannot
develop themselves any more.

If now during the crystallization a one-sided pressure prevails, this
pressure — transformed in the thin fluid magma into an all-sided
one —- will be able to make its influence felt. Consequently it is
not accidental that exactly the fine-granular lujaurites show a great
inclination to parallel-structure. /n the viscous magma no strong
currents can take place; no parallel structure can thus be formed
in it. In case Jarger feldsparcrystals had already been formed before

(5)

the relief from pressure, they will be placed parallel one to the
other and be surrounded by a felt of aegirine-needles (Kolarocks) ;
in case no one-sided pressure prevails, a rock will be formed
distinguishing itself from the normal foyaites by the habitus of
aegirine and arfvedsonite.

The viscosity of the magma will check the escape of gases, and
ihe gradual supply of gases from the underlying magma will ocea-
sion a transition into rocks of the habitus of the kakortokites, which
are of an almost identical chemical composition and distinguish them-
selves from the lujaurites mainly by the increase of the size of the
grains, by the absence of parallel-structure and by the needleshaped
habitus of aegirine and arfvedsonite. The again increased pressure in
this thin fluid magma is converted into a pressure from all sides.

The regularly returning succession of different variations of kakor-
tokites was already expla:ned by Ussins by a periodically repeated
relief of pressure assisted by separation according to the specific
gravity. The appearance of narrow transition zones without deviating
structure between the different variations, and the comparatively
trifling thickness of the strata prove that the relief of pressure was less
pronounced during the crystallization of the lujaurites.

The enclosing of the naujaite-fragments in the breccia-zone can be
explained by a sinking of the roof, simultaneously with the decrease
of volume and the erystallization of lujaurites, causing an increase
of pressure which is favourable to the development of parallel-structure.
During this process the parallel arrangement of the minerals will take
place in planes which will bend round the naujaite blocks.

With a less regular sinking down of the roof, such as seems
to have taken place in the Pilandsbergen, the pressure and the
arrangement of the different structures in the batholite becomes
likewise irregular. The suecessive periods of relief of pressure and
the simultaneous escape of gases from the magma may have been
accompanied by voleanic eruptions of varying intensity.
Similarity in structures between the crystalline schists and the contactrocks.

In rocks accompanying Injaurites, we find a great variety of sieve-struc-
tures which were discussed at large in a former communication *).

Sieve- and parallel-structures are found also both in crystalline
schists and contactrocks. This explains why travellers of the first
half of the 19 century have mentioned chloriteschists and gneisses
among the rocks of Greenland, and why Cart Mavcr’) enumerates

1!) H. A Brouwer, On peculiar sieve-structures in igneous rocks, rich in alcalies.
These Proceedings XIV, p. 383.

*) G Maucnu. Reisen in Siid-Afrika (1865— 1872). Ergiinzungsheft N°. 37 zu
PETERMANN’s Geogr. Mittheilungen, p. 14, 1874.

739

gneisses among the rocks of the Pilandsbergen, This great similari-
ty of structure points to analogy in the genesis: the principal
factors for the formation of contactrocks are abundance of pneuma-
tolytic gases, and crystallization at a low temperature, whilst recrys-
tallisation under pressure in firm rock, as takes place in crystalline
schists, will lead to a similar structure, as a sudden and rapid crystal-
lization does under pressure in an already viscous magma, circum-
stances under which the normal laws ruling crystallization in a
slowly cooling magina are no longer in force.

The varieties of lujanrite rich in aegirine or arfvedsonite, in
which the feldspars are only developed as small crystals, show e. &.
a great outward resemblance to some amphibolites. Characteristic
of both of these is a simultaneous crystallization through the entire
magma, or a simultaneous recrystallization through the entire rock,
the consequence of which is the simultaneous formation of many
little crystals. It will, however, generally be possible to distinguish
between them, because in the igneous rocks with the habitus of
erystalline schists the minerals that had already crystallized as pheno-
erists under the influence of affinity, chemical equilibrium and relative
solubility of the components, before the conditions of rapid crystalli-
zation set in, will continue to exist as such, whilst with the crystalline
schists the entire preexisting mixture of minerals must adapt itself to
ihe new circumstances and recrystallize at the same time, in conse-
quence of which the formation of idiomorphic crystals is checked
althrough the rock, and this is also the case in the genesis of
contactrocks. A greater mclecular mobility however often still allows
the development of idiomorphic crystals and of a succession of
erystallizations in a cooling igneous magma. These differences can
often distinetly be observed in the sieve-structures which are met
with in both groups of rocks.

Defining the crystalline schists as metamorphic rocks, the lujau-
rites do not belong to this group; neither do many other rocks
often regarded as crystalline schists. As such may be mentioned
the rocks of numerous gneiss-areas situated outside large folded
mountain-ranges which just as the above described nepheline-syenites
show strongly varying types, whereas traces of dynamometa-
morphism after the consolidation are entirely wanting.

Finally the above mentioned facts and reasonings illustrate the
importance of the agencies which are at work in the cases of
piezocrystallization and piezocontactmetamorphism, with ‘regard to the
genesis of rocks of the habitus of the crystalline schists. ;

Proceedings Royal Acad. Amsterdam. Vol. XV.

740

Physiology. — ‘form and function of the trunkdermatome tested
hy the strychnine-segmentzones”’ '). By: J. J. H. Mo Kussseng:
Communicated by Prof. WINKLER.

(Communicated in the meeting of October 26, 1912).

The theoretical trunkdermatome of man ard mammals is a trape-
zium. the short basis of which lies in the dorsal diameter, and the
lone basis of which lies in the ventral diameter. This statement dates
aiveady from Turck, who called the attention to the fact that dorsally
a same number of posterior roots provides for the skin covering the
thoracal-vertebrae, whilst ventrally they do so for a much larger
part of the skin, extending from the manubrium stern to the sym-
physis pubica.

It seems that the anatomically. prepared dermatomes (BOLK ’),
Grosser and FronnicH *)) support this view.

The root-fields experimentally fixed according to the “remaining
aesthesia’” method, that Snerrincton *) found with Macacus rbesas,
have likewise a form answering to the theoretically postulated one.
SHERRINGTON writes, that the string formed by the dermatomes on the
trunk is, ‘somewhat wider near its ventral than at its dorsal end’.
And passim: “each zone is narrowest at its dorsal end”. Yet
SHERRINGTON remarks that the periphery of the dermatomes feels
stronger than the central part, so that going from the border towards
the centre for the fixation of sensibility, occasionally the sensibility
suddenly appears to become much sharper.

A similar fact was stated for the dog by C. WINKLER and van
UJNBERK °). They saw namely that the sensible isolated zone generally
deviated in extent and form from the theoretical dermatome. These

1) According to investigations made in the physiological laboratory of the Uni-
versity of Amsterdam.

2) L. Boutx, Die Segmentaldifferenzirung des menschlichen Rumpfes und seiner
Extremititen. I—1V. Morphologisch Jahrbuch Bd. XXV. XXVI. XXVII. XXVIII.
Leipzig 1897—1900 and: 1. BoLK. Een en ander uit de segmentaal anatomie van
het menschelyjk lichaam. Ned. Tid. v, Geneeskunde. Amsterdam. 1897. Vol. I. p.
982. Vol. II. p. 366.

3) O. Grosser und A. FROHLICH. Beitr. z. Kenntniss der Dermatome der mensch-
lichen Rumpfhaut. Morphol. Jahrb. XXX. 8. 308. Leipzig 1902.

') C. S. SHERRINGTON. Examination of the peripherical Distribution of the fibers
of the posterior Roots of some spinal nerves I Transactions of the Royal Society
of London. B. Vol. 184. p. 691. London. 1892.

5) CG. WINKLER and G. vAN RuyperK. On function and structure of the trunk-
dermatoma I-IV. Proc. of the K. Akademie van Wetenschappea te Amsterdam.
1902-1905, Amsterdam, and: CG. Winker. Ueber die Rumpfdermatome. Ein
experimenteller Beitrag z. Lehre der Segmental-Innervation der Haut. Monatschr.
f. Psychiatrie und Neurologie, Bd. XUIL S. 161. Berlin. 1993.

741

deviations were greater in proportion as the operative trauma for
the investigation had been larger. Moreover they found a permanent
regularity in the way in which the deviations presented themselves.

These facts brought them to the view that the isolated root-field
that could experimentally be ascertained, can never have the entire
extent of the theoretical dermatome. They supposed therefore that
even in the most favourable experiments beyond the limits of the
sensible zone, always another little strip of skin must be admitted
as belonging to the dermatome. This strip they called “Marginal area’’,
and pronounced ia. the hypothesis which for the rest was no further
elaborated, that this strip is not capable of independent sensation (i.e.
without the assistance of the sverlapping). This isolated sensible zone
they called “central area”. In the experiments of W. and v. R. the
form and extent of this zone appeared to be extremely variable and
dependent on the postoperatory conditions of the isolated root and
of the spinal cord. With a large operative trauma the form of the
central area was no more than a “caricature” and its extent much
smaller than might be expected from the dermatome. W. and y. R.
call this part of the dermatome, that was found to be insensible
likewise ‘‘marginal area’. If we summarize W. and v. R.’s views, we
find that even in the most favourable experimental isolations the
zone that is found to be sensible does not constitute the whole theo-
retical dermatome, but only a central area of it shut in between two
marginal zones that cannot be indicated. In unfavourable cases, when
the central area becomes a caricature, the marginal area is widened
at the expense of the central area.

In W. and v. R.’s experiments the latter phenomenon always
occurred first and strongest in the ventral zone of the dermatome.
As an explanation of the fact that the sensibility in the ventral zone
appears to be feebler W. and v. R. adduce two hypotheses : 1s that
the ventral part is the most excentric part of the dermatome (i.e.
most distant from the C.Z.S. spinal cord and spinalganglion)*) and
20d that on account of the “stretching” of the skin between manu-
brium sterni and symphysis the extremities of the nerves had to
extend over a larger surface than in the dorsal zone. :

On the occasion of a systematic examination of the strychnine-

1) Compare likewise: G. vAN RigNBERK. On the fact of sensible skin dying away
in a centripetal direction Proc. of the K. Akademie v. Wetenschappen te Amster-
dam 1903, and G. vaN RunsBerk. Beobachtungen iiber die Pigmentation der Haut
bei Scyllium catulus und canicula und deren Zuordnung zu der segmentalen Haut-
innervation dieser Thiere. Petrus Camper. Nederl. Bijdragen tot de Anatomie.
DI. Ill. p. 1387. Haarlem. 1904.

48*

742

seomentzones of cats ®., of which I hope to make detailed communi-
cations on some subsequent occasion, | found some facts which, in
connection with the questions mentioned above, I suppose to be of
sufficient importance to be separately communicated here. My expe-
riments are made on cats that by a high transverse section had been
converted into spinal-cord animals. I apply then strychnine in the
place where a root enters, and cut besides cranically two roots.
Consequently I make use of a combination of the remaining aesthesia
method and that of the local strychnine-poisoning of the spinal cord.
I do so to be sure, that though there may perhaps exist some doubt
about the decidedly local application of the poison, at all events, no
stimuli of the skin ean reach the spinal cord from roots situated
beside those, of which I intend to fix the skin-zone.

By a slight touch of the skin with a pencil we look then further
for hypevreflexion*): usually this can already be shown a few
minutes after the poisoning.

A peculiar fact that I have regularly stated at the determination
and fixation of the zones, is that hyperreflexion appears first and
strongest in a definite string-shaped zone, which however soon widens
because cranially and caudally a strip of skin which at first was not
hyperreflectory, becomes so now, though in an inferior degree to
the zones that could first be indicated. When the entire strychnine-
seementzone has reached its largest extent, this difference of intensity
still continues to exist, so that we can distinguish a central zone
with stronger hyperreflexion from a narrower peripheric strip with
less strong hyperreflexion.

This stryehnine-segmentzone can consequently be divided into a

strong hyperreflectory inner-zone which can soon be indicated, shut in
by two feebler outer-zones appearing a little later.
These facts show an unmistakable correspondence with those men-
tioned above communicated partly by SHERRINGTON, partly by W.
and v. R. I shall try to elucidate this peculiar behaviour of strych-
nine-segmentzones in connection with what has been found by the
above-mentioned authors, chiefly on account of indications ascertained
with a eat (marked 32) where, under specially favourable cireum-
stances, successively three strychnine-segmentzones could be fixed,
namely to the left Th. VIII and Th. XI to the right Th. VIL.

1) Compare J. G. DusseR DE BARENNE. Die Strychninwirkung auf das Zentral-
nervensystem. I—IV. Folia Neurobiologica. Bd. IV. V. VI. Haarlem. 1910-1912.

2) With this form of strychnineapplication no Tetanus takes place, but only
hyperreflexion,

745

1. Strychnine-segymentzone Th. VIL left.

After the cat had been- made a spinal-cord-animal by a transverse
section at Thor. II a piece of thoracal spinal cord is laid bare in the
usual way, and the place of introduction left of Th. VIII moistened
with strychnine. Moreover the dorsal roots of Th. VI, VII, IX and
X are cut intradurally. Soon it is possible to ascertain a strongly
hyperreflectory zone of the skin, wich gradually widens and a few
minutes after the poisoning reaches its maximal extent. It is then
still very easy to distinguish an inner-zone and two outer-zones.

a. Description of the inner-zone.

The ¢ ntral-zone is almost string-shaped. The cranial and caudal
limits first run parallel to each other, perpendicular to the axis of
the body. On the centre of the lateral surface the cranial limit makes
however a curve convex to cranial. A similar phenomenon‘is scarcely
indicated in the caudal limit. *)

The bordering lines continue to run parallel and perpendicular
as far as the ventral surface. Here they converge slightly, so that
the central zone that was at the d. d. 30 mm. wide, measures in
the v. d. only 283 mm. The central zone however goes beyond the
v. d. and finishes, sharply limited, about 4 mm. overlapping the
crossed side. Here the hyperreflexion is somewhat slighter than in
the rest of the zone. (A dorsal crossed overlap could not be fixed
on account of the median skin-section).

The zone hitherto described is surrounded by a ventrally strongly
widening outer-zone which being itself less reflectory than the inner-
zone, contrasted however strongly with the'adjoining areflectory resp.
normally reflectory zone. The outer-limits of the outer-zone are of
course at the same time the boundary of the totai strychnine-segment-
zone, which I am going to deseribe now.

b. Description of the total strychnine-segmentzone (vuter-limits of

the outer-zone).
Searcely to be recognized at the d. d., running closely along the

1) A similar fact is often indicated by W. and R. Compare e.g. their fig. 27
of their I[lrd communication. Here the 13th and 16th spinal roots were isolated.
The caudal zone of the ventral part seems to be considerably shrunk, whilst
cranially the lateral outward curve of the central area breaks through the anaesthetic
zone. To explain these phenomena they admitted a widenirg of the ceutral area
in the lateral part, whilst at the same time it is supposed that here a relative
minimum of sensibility is found. As now a similar removal of the border existed
cranially and not caudially Jikewise with my cat, this fact may perhaps also be
regarded as a peculiarity of the 16th root-field.

744

foremost limit of the inner-zone, the cranial limit of the total zone
soon assumes a course directed more towards cranial, so that the
cranial outer-zone, in the d. d. scarcely a few mm. wide, is in the
v. d. 10 iam. wide.

The caudal boundary-line continues to run at the d. d. almost
tovether with the caudal limit of the imner-zone ; it is here hardly
a oe mm. to the outside. Its further course however is like that
of the cranial limit strongly divergent, consequently here in a strong
eaudal direction, so tbat, especially in the ventral zone, a wide
outer-zone appears, which in the v. d. is 21 mm. wide. The caudal
onter-zone is consequently almost twice as wide as the cranial one.

If we regard now this large extent, and the shape that the total
strychnine-segmentzone obtains by the addition of the so wide outer-
zones, we should be inclined to admit that almost the whole theo-
retical, ideal dermatome has appeared here. If now we remember
W. and v. R.’s conclusion:

“Isoliert man experimentell ein Dermatom so entspricht der erhaltene
sensibele Bezirk nie weder der Ausdehnung, noch der Gestalt nach,
dem theoretischen oder anatomischen Dermatom,” *) then the com-
bined strychnine-isolation method applied by me affords doubtless
better results than the simple “remaining aesthesia method”. For
under the influence of the strychnine poisoning the limited value for
the reflexion diminishes so much that there can hardly anymore be
question of a marginal area in the sense of W. and v. R.

2. Strychnine-segiment zone Of Th. SINE

After the rootfield of Th. VIII had in this way ‘een fixed and
measured, the root Th. XI was isolated in the same way by cutting
the dorsal roots of Th. XII and XIII, and locally poisoned with
strychnine.

The hyperaesthetical zone that appeared here likewise, had a steep
trapezium shape, and was when the total extent had been reached,
at the d. d. 34 mm., at the v. d. 49 mm. wide. Here the cranial
limit could however only be fixed, after the Th. VII, isolated in
the preceding experiment, had been cut. For it appeared that the
eranial limit of Th XI crossed the caudal limit of Th. VIII in the
level of its lateral cranial curve.

a. Description of the central zone.
The central zoue of Th. XL occupies dorsally also again almost

1) G. van RunperK. Versuch einer Segmental-Anatomie. Ergebnisse der Ana-
tomie. Bd. XVIII. Wiesbaden 1910. 8. 544.

745

the total extent of the strychnine-segmentzone. Its limits have here
likewise a parallel and perpendicular direction. On the lateral and
ventral surface they assume also a distinctly converging course so
that when they reach the ventral diameter, they are only 16 mm.
distant from each other, whilst at the dorsal diameter the inner-zone
is about 32 mm. wide.

b. Description of the outer-limits of the outer-zone. Total strych-
nine-segmentzone).

The cranial limit lies in the dorsal zone, scarcely perceptibly
cranially from the cranial limit of the inner-zone. On the lateral
surface however when the cranial limit of the inner-zone begins to
converge, (consequently begins to move in a caudal direction), it
deviates strongly diverging (consequently in a cranial direction). The
outer-zone hereby becomes rather wide; at the v. d. it attains a
width of 21 mm. The caudal limit of the outer-zone follows that
of the inner-zone as far as the lateral surface, then about the place
where likewise the cranial limits of outer- and inner-zone deviate
from each other, it takes also a diverging direction (consequently
follows a caudal course). In the level of the axil-groinfold line the
outer-zone reaches its greatest width. From here it continues in a
ventral direction pretty well perpendicular to the axis of the body.
The caudal outer-zone is at the v. d. only 12 mm. wide.

If now we cast a glance at the entire strychnine-segmentzone, i.e.
both inner- and outer-zone, we obtain the fimpression, that the
two zones by which it is formed (both inner- and outer-zone) show
an inclination to shrinking. In favour of this view plead: 1. the
stronger converging of the limits of the inner-zone towards the ven-
tral diameter, which reminds us of W. and y. R.’s central area;
2. the fact that the cranial outer-zone exceeds the caudal-zone espe-
cially in the ventral region; 3. the disappearance of a distinct ‘“‘ventral
erossed overlap’; 4. the fact that at the d.d. the zone is as wide
as the former (VIII Th.) and is here 34 mmi., whilst at the v. d.
the width is here 49 mm., consequently 6 mm. less.

If we may admit here on these grounds a first beginning of
shrinking, then we are struck by the fact that the zone undergoes
this diminution exactly in its most excentric part, namely in the
“ventral-crossed overlap” and farther in the caudo-ventral region.
In this way we obtain an insight into the manner in which the
shrinking begins, and must observe then, that this shows conformity
with what Snerrineron and W. and vy. R. saw already in their
root-fields.

746

We may consequently admit, that both the dermatomes and the
strychnine-segmentzones, when they shrink, do so in the same manner,
and both have their weakest point in the ventral-crossed overlap-
region and in the caudo-ventral part.

3. Strychnine-segmentzone of Th. VIL right.

As after the expiration of the above-mentioned determinations, the
eat was still in a very good condition, I undertook the poisoning cf
another root, now on the right side of the spinal cord. I selected
for this operation Th. VII, where I performed the application of the
strychnine as carefully as possible, and did not cut the adjoming
roots. I had previously convinced myself that to the right there
was not a vestige of byperreflexion in the skin. At the same time
the first isolated root Th. VIII to the left was cut.

After the poisoning soon a distinctly hyperreflectory zone appeared
that could easily be limited.

The zone had a great extent now, and no distinct contrasts between
the inner- and the outer-zone could be discovered.

Description of the total zone of Th. VIT right.

The cranial limit leaves the d. d. at about the level of the pro-
cessus spinosus of the 7" thoracal vertebra, and runs almost per-
pendicularly to the axis of the body, with slight convexity in a caudal
direction on the lateral surface. On the ventral surface it deviates
again somewhat more in a cranial direction. The v. d. is reached
10 mm. ecranially from the cranial limit of the left VIII thoraeal
zone. (Comp. figure 3).

The caudal limit leaves the d.d. about 30 mm. caudally from the
former and runs almost parallel with it with a slight inclination to
diverging in a caudal direction. It reaches the v. d. together with the
caudal limit of the left VIII thoracal zone. (Compare the description
given above and fig. 3). In the v. d. the width of the whole zone
amounts to 43 mm. A ventral-crossed overlap could not be ascer-
tained. This fact and likewise the comparatively slight width of the
zone can justify the supposition that we have here to do with a be-
ginning of shrinking, at all events the zone as strychnine-segmentzone
has not the maximum extent which it can have. (Th. VIII on the
left side was much wider). Although we have here not even to do
with an optimum, I found, when exaetly fixing the limits in the
fixed bone-points under the skin, that the extent on the lateral surface
answered already to above 3 ribs and the spaces between 3 ribs.

747

Such an extent is now the same as Merrens could preparatorily
ascertain as the norm for the trunk-dermatome of man.

The trapezium-shape answers likewise to the anatomical dermatome:
all these proportions consequently plead strongly for the fact that
my method is superior to the usnal isolation methods, and strengthen
the view, that the strychnine-segmentzone represents in fact the whole
rootfield: the theoretical dermatome. If this is so indeed, we may
likewise conelude that W. and v. R’s view, that the central aren
and the whole dermatome have the greatest width in the lateral part,
is not correct, but that the greatest width is reached at the v. d. °),

At last we can try, by a comparison of the dimensions of the
zones which we have found, to get an insight into the overlappings
of the rooi-fields. With a view to this I begin to represent here all
the dimensions found by me in a table likewise indicating those of
the areflectory zone of the left side, situated between the isolated
Th. VIII and Th XI.

1) Compare: V. E. Mertens. Ueber die Hautzweige der Intercostalnerven. Anatom.
Anzeiger Bd. XIV. S 74 Jena. 1891. Mervrens describes here the extent ia. of
the 4th intercostalnerve of man. He found: that the zone provided for by it: .. .
“sich iiber drei Intercostalriume, und ebensoviel Rippen erstreckte, und zwar
begann es mit dem dritten Intercostalraum, und endete auf der sechsten Rippe”’.

748
As it is known W. and vy. R. indicate the overlapping of the central-

of the extent at the d. d. Further they found, in some

qo |

area as
of their cases, that the width of the analgic zone, the consequence
of the cutting of two roots, was as wide at the d.d. as the sensible
zone of one isolated root.
Let us now compare the results of the strychnine-segmentzones.
With regard to the proportion of the width of one total segmentzone
to that of the areflectory zone of two cut roois we see that the
proportion is here 30:15, thus instead of 1:1 they beara proportion
of 2:1. Of greater importance however is the overlapping of the
strychninezones in their entirety, or, where they have taught us to
consider them, identical with the theoretical dermatomes, the over-
lappings of the entire rootzones. W. and v. R. could not determine
them, as is self-evident, because they always found large “marginal area”.
If we apply now the method of caiculation of the covering as
indicated by the above-mentioned authors we find, if we call the
overlapped field of the root-zones « and the not overlapped part y,
that at the d.d. holds for the whole hyperreflectory zone
2¢ + y= 35 mm.
and the areflectory zone must be expressed as:
2y + 2=11 mm.
From this we can calculate the values of x and y
22 + y = 35 20 + y = 105:3 w+ 2y = 33:3
2yt+a=—11 r+y= 46:3 ut y= 46:3
du + 3y = 46 x ==" Has y =— 13:3

From which follows that

If now we suppose the whole root-zone = 1, then is

9
22 + y = 2x — Pei 1, consequently 16% = 9, and «= Th

From this follows that the rootfields cover each other at the d.d.
9 9
for =n W. and y. R. had estimated it at about Tk which agrees
) v
pretty well with my resuit.
e. 4) it appears that in the dorsal
trunkskin, parts are alternately provided for by two and by three

From the construed figure (fig

749

roots. In the middle of each dermatome meet each other the outer
extremities of the two adjacent zones, which overlap each other bere for
»

16°
the rest of the dermatome only two fields overlap each other.

Here conseqnently a threefold root-innervation takes place. In

Let us now execute the same calculation for the v.d. Here, as
will be remembered, no areflectory zone was found. We can however
make an analogous, though somewhat more complicated calculation,
taking into account the ascertained overlapping of the zones of

Eh. VIL amd "PR XT:

If we express now the width of the whole dermatome in the v.d.
in the above indicated symbols, the width of arootfield AL = Ab —
AS 1A aoa, 1h Gig —_— 27 ane y.

In the figure zone I represents consequently Th. VIII and zone
IV Th. XI. As Th. VIUl and XI overlap each other 10 m.m. |
may suppose pg =10. If now we call wv the overlapping of two
adjacent zones, and y the overlapping of two alternating zones, then
we find for pq:

pg = Co—Cp = C a—bB as Cp=bB

pg = y—(AB— Ab) as CYa=y (namely the overlapping

of onvhly,

pa = y -(22--y—2)

pg =y—e + y= — e+ 2y=10 mm.

From this follows:

2a—y = 55") = —a+2y = 10
—2x+4y = 20 4% —2y = 110

oY = 75 32 = 120

(1 xz = 40

The overlapping of the immediately adjacent root-tields (v) is consequently

1) [ take here for the calculation the width of Th. VII[ and not that of Th. XI,
because I suppose that this zone had somewhat shrunk.

Fig. 4.
Scheme of the mutual overlappings of the dermatomes at
the d.d. and at the v.d. (The dorso-ventral dimension bas
not been taken proportionally correct,

40) 8 : : ; :
cee and the overlapping of a root-field with the third next one (y) is
Bo
25 5) : : 4 ; :

roe At last the overlapping of a rootfield with the fourth (pq) :
dy»)

10 2

Se Lh

W. and v. R. supposed that the rootzones overlap each other for
one half, so that zone 1 should stand against zone 3. Consequently
each skinpoint would be provided for by only two roots. From my
statements it appears that the overlaps are much stronger, and that
in some places even as many as four rootfields overlap one another.
The arrangement is thus at the v.d. so, that here strips that are
provided for by 2 borders of rootzones and by 2 more central
parts of these, alternate with strips provided for by the more peri-
pheric parts of three rootfields.

If we repeat the calculations given above likewise for the ‘‘inner-
zones’ of my strychnine-segment zones, then the overlapping of these

l 1
at the d.d. appears to be not —, as W.and v.R. supposed, but —.
-

At the ventral median line where W. and vy. R. did not find an
overlap of their central areas, the overlaps of the inner-zones appears

1 E
to be about —. From this great difference between the results of
3) ‘i

I. J. H. M. KLESSENS. “From and function of the trunk-dermatome
tested by the strychnine-segmentzones”’.

Fig. 1. Left side of 32. Inder- and outer-zones of
Th. VIII. (a d p gq) and of Th. XI. (e f m n).
(Indicated the arcus costarum and the scapula and the crista ilei)

Fig. 2. Ventral side of cat 32. To the left the inner- and
outer-zones of Th. VIII (pq) and of Th. XI (7d).
To the right the total zone of Th. VII.

Fig. 3. Richt side of cat 32. Strychnine-
zone of Th. VII.
(Indicated the arcus costarum and the scapula).

Proceedings Royal Acad. Amsterdam. Vol. XV.

751

the usual method of isolation and mine appears again how strong a
diminution of the limited value of stimuli is obtained by strychnine.

So far the facts. Now it seems not impossible to me to investigate,
with the help of my- results, somewhat closer some questionable
points of the segmental innervation.

Let us begin with the well-known so called “LANGELAAN lines’.
According to this author‘) one finds in the skin of normal persons
hyperaesthetic lines and strings, which are said to exist in the inter-
segmental limits. From my calculations of the overlaps it might
follow on the contrary, that there is a better foundation for admitting
this hyperaesthesy in those strips of skin where always three (at
the d.d.) dermatomes overlap each other. These strips however do not
lie intersegmental in the sense of two immediately succeeding zones,
but exactly opposite to the axis of a rootfield. At the same time
they form the so-called intersegmental limit of each third dermatome.
From this may, at the same time, be concluded that the distance
between two “LANGELAAN lines” does not amonnt to the width of a
dermatome, but to half the width. At the v.d. the proportions are
too complicated for an analogous interpretation to be ventured.

For the much discussed territory of pigment-stripes of vertebrae
the knowledge of the innervation-proportions of the skin, as it is
now somewhat more detailed by the study of the strychnine-
segmentzone, might prove useful. I have here specially in view
the dark stripes of so many animals. SHERRINGTON’) has already
called the attention to the fact that with zebra and tiger they seem
to be segmentally arranged. Van RiNperk*) considers the dark stripes
as an expression of the stronger innervation which in his opinion
can be observed in the intersegmental limits. by the overlaps of the
central area a “summation” of the innervation is supposed to exist.

It is clear that to this view may be applied likewise what I said
already above with regard to the “Langelaan-lines’. Then van
RuNBeRK’s excess-contrasts might be arranged in those strips where
the extreme borders of the alternating dermatomes overlap one another.

At last we may here fix the attention of the proportion in length
of the short basis of the trapezium-shaped dermatome (in the d.d.)
to that of the long basis in the v.d. This proportion is in Th. VIII

1) J. LANGeELAAN. On the determination of sensory spinal skinfields in healthy
individuals. These Proc. of 2 Sept. 1909 Vol. III.

2) C. S. SHERRINGTON. |. c. p. 737.

3) G. van RignperK De huidteekeningen der gewervelde dieren in verband met
de segmentaalleer. Verslagen der K. Akademie v. Wetenschappen te Amsterdam,
30 Sept. 1905.

752

zone here described, as 2:3. (In reality the proportions were 35 : 55).

It is certainly peculiar, that this proportion 2:3 expresses exactly

the “stretching” of the ventral skin (from manubrium to symphysis)

with regard to the dorsal one from the first to the thirteenth thora-

calvertebra. I could find for the cat about the same proportion,

given by SHERRINGTON for Macacus. :
Summary :

I. Jn favourable cases the strychnine-segmentzone has the exact
shape, and most likely also entirely the same extent as the theore-
tical dermatome. It has then the shape of a trapezium, the short basis of
which lies in the dorsal, and the long oasis in the ventral body-diameter.

Il. The strychnine-segmentzone consists of two parts which are

sharply to be distinguished: an ‘‘inner-zone” that becomes sooner

hyperreflectory, and remains stronger, and an ‘‘outer-zone” that
appears later and remains less hyperreflectory. This behaviour of the
stryclinine-zone is consequently analogous to what SHERRINGTON and
especially W. and v. R. communicated aiready about the sensibility
in the dermatome that they had investigated by the isolation-method.

III. The vulnerability of the strychnine-segmentzone shows likewise
great correspondence with that of the isolated root-field ; they begin
to shrink in the ventral overlapzone, and in the caudo-ventral part
of the zone. Moreover they offer like the root-fields the peculiarity, that
when shrinking, the innerzone analogous to the nucleusfield, becomes
smaller, to the advantage of the outer-zone, analogous to the border-zone.

IV. In consequence of all this we may admit that the other pro-
portions-found for the strychnine-segmentzone, hold likewise for the
dermatomes, that is to say :

9 8
the overlapping of the d.d. amounts to Fe and at the v.d. Pit By

3,
this the skin is alternately provided for: at the d.d. for ae by three
D
5
roots, and for 7 of each dermatome by two roots ; and at the v.d. for
9

Ae Sees
Fi by four roots, and for a of each dermatome by three roots.

V. The “Langelaan lines” and van Ruperk’s “excess-contrasts” by
summation most likely answer to the strips of skin, where, at the dorsal
diameter, the innervation takes place through three roots. If this hy po-
thesis might be confirmed we should in the mentioned skin-stripes
really possess a means of fixing the dermatome limits, as between
every two such like alternating stripes, exactly a dermatome would
be situated.

753

Microbiology. — ‘.letion of hydrogenious, boric acid, copper, man-
ganese, zine and rubidium on the metabolism of Aspergillus
niger’. By Mr. H. J. Warrrman. (Communicated by Prof. M.
W. Beertncr).

(Communicated in the meeting of Oct. 26, 1912).

Ravnin’s object when examining the culture conditions of Asper-
gillus niger*) was to obtain the greatest possible weight of mould.

The experimenters who after him occupied themselves with this
question, likewise only considered the dry weight.

Such an investigation must needs be partial as the process of the
metabolism is only roughly determined by the weight of mould. For
a good insight into this process it must be observed that for instance
the spore formation produces differences in the chemical composition
of the obtained mould materials.

Hence, the changes of the plastic aequivalent or of the assimi-
lation quotient should be determined many times in the course of
the development; first of all of the carbon then of the other elements.

In an earlier paper’) i proved that changes of temperature and
concentration do not modify the metabolism of the carbon and _ that
only the velocity of this process is subject to modification.

At present I have studied the influence of various chemical
compounds.

1. Action of different rates of hydrogenions.

The results of the referring experiments ave found in Table I.

We see from it in connection with the incorrectness of these
observations, caused by the small quantity of mould, that the plastic
aequivalent of the carbon, in spite of the slackening of the growth
and sporefourming, caused by the hydrogenions, does not undergo
a convincing change.

2. Action of different boric acid concentrations. *)

Analogous results as for the hydrogenions were found with boric
acid as seen in Table II.

In lower concentrations of about 0,06°/, the plastic aequivalent
remains almost unchanged.

The slight lowering observed at higher concentrations may be

1) J. Raunin, Etudes chimiques sur la végétation, Paris 1870,

2) H. J. Warerman, Beitrag zur Kenntnis der Kohlenstoffnahrung von Asper-
gil/us niger, Volia Microbiologica, Holliindische Beitriige zur gesammten Mikrobiologie
1912 Bd. 1 p. 422.

3) Also compare: J, BésseKen and H. J. Waterman, Folia Microbiologica | (1912)

p. 342.

754

LA Beet

Culture liquid: 0,15 gr. paraoxybenzoic acid p. 50 cm’ tapwater. Temp. 32—33° C. Anorganic-
food: 0,059 NH4Cl, 0,05 KH,PO,, and 0,02% MgSOx,.

Expressed | a oe ; ape ; ~~ leeee
H-ions in in c.m3, Course of development!) after Mastic Ae aan

grams p.L. N. H.SO, ed : 2 ee SS eee

NO. : ad
given as p. 100 cm® of |
sulf acid. the culture Dy <a 9 27,28 40 271—28 90 days
liquid |
l 0 0 +i: ioe a aa a ne | 5%
many spores | 9
2 0 oe} Sa]! aay “1, |
|
3 0,4.10-5 O19 ++ +444 =2 (2. | 55%
3
“| eels 058 | +4+\/44+++) =3 ae 49,
ae
5 || 1,8. 10-5 097 9 ++ 4444+ 444449 eS 48,
ropa:
| eh 1,17 Specter te) actor aa So 44,
few spores on &
ai,
7 2,8. 10-5 1,56 + a a Ee) = = | “ae
few spores = °
z
3} 33.10 .9 1,96 =m oa +t+ 2) zie 46 ,
few spores 2 Es
9 3,9. 10-5 2,35 be ae eee) =e 43,
few spores ou
: e sz
10 | 4,4.10-5 2,74 == = ? = 6
= §
|

11 5,7. 10-5 3 92 — - —

TAB eae

50 cm3 tapwater, in which dissolved i gr. glucose, 0,159, NH4NOs,
0,15" EES a0ES be Temes 33 34° C.

=i
Weight of Development after | Plastic aequiv. of

Nr. oe ae we the carbon after
in "/, 2 6 7 days

1 0 +++ vig. growth, many spores 36%

2 0,01 +++), er » 36,5 y

3 0,02 +4+ , n° eee " 35 y

4 0,06 te ane » 34 y

5 0,2 TEE | Tei her " 31 y

6 0,5 ++ +++-++, few spores 50> 5

7 1,0 + +++, no spores _

') The differences in vigour of mycelial growth are indicated by ,+”, ,++’ a etc.
*) The mycelium is yellow.

759
explained by the formerly described mutation ') occurring under the
influence of boric acid.

From these observations it follows that the metabolism of the
carbon, in opposition to the velocity of the growth and spore pro-
duction, changes little by the said chemical influences.

3. Action of copper.

Whilst Raviin?), proved that coppersulfate in strong concentrations
is noxious to the development of Aspergillus niger, Ricurer and Oxo
put the question whether copper in very dilute solutions may act
favourably.

ANDREAS RIcHTER *), who stated that in absence of zinc even addi-
tion of a gr.mol. coppersulfate per L. caused the weight
of mould to decrease, answers this question negatively.

N. Ono *) came to an opposite result.

The observations of Ono and Ricuter need not, however, be in
contradiction with each other as it is not certain that they cultivated
under the same circumstances, although Ono endeavoured to do so.

Ono’s experiments especially are deficient in as much as the
velocity and the nature of the metabolism are not sufficiently sepa-
_rated. For this reason I have once more made an analogous in-
vestigation.

The chemicals used were of KAnHLBAUM’s and of great purity.

The distilled water was once more purified by redistillation in an
apparatus of Jena glass joined by a glass tube to a tin cooler *), and
then kept for use in Jena flasks. The cultivation took place in
ERLENMEYER flasks of Jena glass of 200 cm’*. capacity.

The composition of the culture liquid was:

0.15 °/, ammoniumnitrate

0.1 ,, potassium-chloride

0.1 ,, magnesiumsulfate (crystallised)
0.05 ,, calciumnitrate (free from water)
0.05 ,, fosforic acid (crystallised)

2 ,, glucose.

1) H. J. WateRMAN, These proceedings, June 1912. Vol. XV, p. 124.
ay Lic. pa dat

-3) A. RicuTer, Centralbl. f. Bakteriol. 2e Abth. Bd. 7 (1901) p, 417.
4) N. Ono. Centralbl. f. Bakteriol. 2e Abth. Bd. 9 (1902) p. 154.

5) Corks and such like material were avoided.

49
Proceedings Royal Acad. Amsterdam. Vol. XV.

756

Each culture tube was filled with 50 cm’. of the above liquid
and coppersulfate was added in different concentrations.

After boiling spores of Aspergillus niger (Form I) *) were inoculated.

The observed development is described in Table III; the formation
of but few spores is caused by the use of the said chemicals free
from manganese, as is further explained in Table. V.

T ACB LSE. An
Temp. 34—35° C.

Coppersulfate added
(Cu SO4.5 Aq.)

l
Course of development after
Nr. | = |

aa:-. |In Gr. mol. | |
| In milligr. |p. Litre | 3 5 | 9 days
| rather vigorous, y; orous, hardl i orous, onl
1} Control | — 4+ | hardly any [18 ) ¥) NISOrOnS,)
| spores any spores few spores
8 vigorous, very
SSS = = 1 =o g )
: os 10000000 | + | few spores
8 vigorous, hardly
3 ever eee —2
: o1 | Too0000 | * | any spores
4 | 10 | nea leas at Pai joes hardly |++ ++, hardly
) 100 000 as | any spores any spores
z s 2,8 | ++, hardly |+-++4, hardly
i oe 10 000 ic “Fe | any spores any spores
427 | 4+t4, hardly |++4+4+-4, hardly
: : 10 000 a ca any Spores any spores
b 3 Peay | ++, hardly |-++4+4+4, hardly
09 1000 a5 | Bae any spores any Spores
Aas Se ee eae pate ++, few +++, hardly
F 1000 spores any spores
ee _ ++, few +++, hardly
: a 1000 fe ae spores any Spores
|
10| 252 dae = | 2 +, hardly any
100 spores
11 505.5 KA a 1 oe after two months’ growth,
ii 100 but probably with mutation
|
12 1000 me ae me as
100

') Compare H. J. WarErMAN. These Proceedings June 1912.

diminishes the production of spores.

The velocity of the mycelium formation as well as the assimilation
of glucose are also slackened by the coppersulfate (Comp. Nr. 4 and
the following Nrs with Nrs 1-3).

By determining the quantity of dry substance ') and the carbonic
acid obtained from it by combustion on one hand, and on the other,
by determining the polarisation*?) and the reduction number by
litration after Frnuinc, by which tbe assimilated glucose could be
computed, the plastic aequivalent of the carbon could be fixed.

In Table IV the results of these experiments are united,

TABLE IV3),

Metabolism of Aspergillus niger under influence of
different coppersulfate concentrations. Nine days
after inoculation.

Obtained | Mgr. CO2 at | a cimitated | Plastic

eG | Me mot isons inl ee
| material | |

ry ene. | sans) Stoo 36,0,

2) 3185 | 556 «=| «= 100—Sts«*d' 38,0,

3| 325.5 563,5 100 385 .

ab 377 | 643,5 | 100 44,0 -

St pe Mudge be Poie i)? sae sae

6 | 190,5 331 57 «30,5, aa

Th 83 146 31 (Sates [eae

Seng 1925 | 32 /41 ,

9} 89,5 ego eaieeg <1 | 44,5,

(oie ake Ele ea A aaa

il | _ = | agate rae

| = = | Ge cenit <=
| |

1) Dried at 105° to constant weight.

2) Determined by the saccharimeter of Scumipt and HaeEnscu. It is proved
that in the Nrs. 1—6 a small quantity of a hitherto unknown polarisating sub-
stance occurred, not reduced by ‘FEHLING”’.

3) Compare Table III.

49*

758

8
We thus cbserve that the addition of van mol. coppersulfate

considerably enhances the weight of mould after 9 days; it is more
than 70 milligr. greater than that obiained without addition of copper.
Already before’) I explained that the non-formation of spores
commonly coincides with the accumulation of glycogen in the mould
and with a high plastic aequivalent of the carbon.
This we find confirmed here, compare for instance Nrs. 1, 2, 3. 4.
The values of the then following numbers are not very exact.
That they are notwithstanding mentioned is to make clear that even
considerable copper concentrations (N°. 9) do not change the character
of the metabolism. The decrease in quickness of the assimilation
of glucose is very obviously caused even by slight quantities of copper.
Whether the greater mould production may be called favourable is
doubtful, the sporeforming being retarded.

4. Action of manganese.

BertranpD and JaviLuer®*) found that addition of manganese enhances
the weight of mould whilst it was also stated that this element is
fixed in the organism. It also proved necessary for the spore forming’). ©

By a very minute examination BERTRAND succeeded in showing tkat

1
‘en addition of = manganese made the weight of mould
eta 10000000000 5 8 ;

rise considerably. As will be seen from Table V the addition
of manganese had especially brought about changes in the velocity
of the glucose assimilation. For the rest, my experiments with manganese
have confirmed those of BerTRAND and JAVILLIER.

The composition of the nutrient liquid was:

very pure distilled water in which dissolved:

0.15 °/, ammoniumnitrate

0.1 ,, potassium chloride

0.1 ,, magnesiumsulfate (crystallised)
0.05 ,, calciumnitrate (free from water)
0.05 ,, ammoniumfosfate

0.05 ,, fosforie acid (crystallised)

2.— ,, glucose

1) H. J. WATERMAN, Folia Microbiologica I. (1912) p. 422.

*) BERTRAND et JAvILLreR. Influence du manganése sur le développement de
l’ Aspergillus niger. C. r. 152 (1911) p. 225; Ann. de I’Institut Pasteur T. 26 (1912)
25 Avril p. 241.

*) BertRaANnD. Extraordinaire sensibilité de l’Aspergillus niger vis a vis du
manganese. C. r. 154 (1912) p. 616.

759

Into each ErLenmever flask of Jena glass (200 cm* capacity) 50 em*
of the above liquid was introduced and manganese in different
concentrations was added.

For the result see Table V.

Quite as in the preceding experiment every nr. consisted of several
flasks. Taking this into consideration, the extreme sensibility of
Aspergillus niger as to manganese, already observed by Brrrranp,
was with certainty confirmed. Without manganese hardly any spores
are formed afier four days.

In spite of the observed favourable influence of manganese on the
production of spores no important modifications in the metabolism
of the carbon occur (Table V).

We may thus conclude that the numbers given by Brrtranp ‘)
for the dry weight with and without addition of manganese relate
only to the velocity of the metabolism.

is it necessary or desirable to distinguish elements such as man-
ganese from others as carbon, nitrogen, ete. which occur in the
organism in great percentages? Have we to reckon manganese
among the purely catalytic elements, in opposition to carbon as a
plastic one? In my opinion there is no sufficient reason for such a
marked separation. The only important difference is that elements
as manganese form an extremely small permanent percentage of
the organism. It is, however, very well possible that this difference
is only apparent. The circulation of manganese may for instance
be much quicker than that of carbon, so that the concentration in
One special cell may for a time have been relatively high. It is not,
however, possible to detect this by analysis of the whole mould layer.

5. Action of zine.

Since Ravnin had already supposed that zine acts favourably on
the weight of mould, Javier’) showed with certainty that small
quantities of zinc considerably increase this weight. At the same
time he proved that zinc is fixed in the mycelium *). Moreover,
BerRTRAND and JavilLier *) studied the joint action of zinc and man-

1) BERTRAND GC. r. 154 (1912) p. 616. .

2) JAVILLIER, Sur l’'influence favorable de petites doses de zinc sur la végétation
de l’ Aspergillus niger, C.r. 146 (1907) p. 1212.

Also compare BERTRAND et JAVILLIER, Sur une methode permeltant de doser de
trés petites quantités de zine C. r. 143 (1906) p. 900; 145 (1907) p. 924.

8) Sur la fixation du zine par /’ Aspergillus niger. GC. r. 146 (1908) p. 365.

4) BERTRAND et JAVILLIER, C. r. 152 (1911) p. 900; C. r. 153 (1911) p. 1337,
Cf. also Ann, de I’Inst. Pasteur T. XXVI (25 Juillet 1912) p 515,

760

ganese, which proved more favourabie than that of each of these
elements separately.

In his last communication Javitiier ') mentioned that the constant
relation between the assimilation of sugar and the production of
mould, which is nearly 3:1, sometimes became 8:1 by leaving out
zine, that is to say, addition of zine should allow the organism to
use less food; besides, the assimilation of nitrogen and of the other
anorganic elements changed according as zine was added or not.

Hitherto I have not been able to confirm JAviLLInr’s results.
Addition of zine caused but little change in the metabolism of
the carbon, but again the velocity of the glucose assimilation was

modified.

75
Addition of stronger zine concentration: ——~— er. mol. ZuCl,

100000
p. L. caused a distinct, albeit slight increase of the plastic aequiva-
lent of the carbon, but it was accompanied by non-formation of
spores.

In many respects, thus, the action of zine resembles that of cop-
per. As with this element the addition of slight quantities of zine,
which exerts no perceptible influence on the production of spores,
causes hardly any change in the weight of mould.

7 it
3 ‘ient solutions taining ~~. > A ;
So, nutrient solations, conlainite | in ann.000 ° 10000lsmin a

____-_. er, mol. ZnSO, 7 Aq. p. 1. produced after’ fourm
1.000.000 ?

respectively 407, 410 and 417 milligrs. of dry material, whilst analogous
experiments, without addition of zinc, produced 406 and 408 milligrs.
The fact that stronger concentrations of zinc check the forming
of spores (see above) which had also been observed by Sauron’) and
Javiniier®), Bertranp*) tries to explain by the relation existing
between the quantity of manganese present on one side, and the
produced mould on the other. | |
Thus Bertrand says: “Lorsque au milieu nutritif on n’ajoute ni fer,
ni zine, ou seulement du fer ou du zine, les mycéliums qui pren-
nent naissance sont si réduits que le rapport du manganese, introduit
yolontairement on non, au poids de matiere organique formée, peut

1) JavitLier, Influence du zine sur la consommation par l’ Aspergillus niger.
de ses aliments hydrocarbonés, azotés et minéraux, C. r. 155 (1912) p. 190.

2) B. Sauron, C. r. 151 (1911) p. 241.
8) M. Javinurer et B. Sauton, Cr. 153 (1911) p. 1177.
4) G. Bertranp, CG. r. 154 (1912) p. 331,

TA’
Temp. -

Influence of manganese on the spore-fo

Added

MnCl, . 4 Aq. Course of development after
Milligr. | Crammol. 2 3 | 4 |. -
; pals y

vigorous, hard- vigorous, very ?
0 . se bag ot ly any spores few spores it! Spores
vi hard- vi few r
9 jae = : gorous, hard- vigorous few | rather ma
20,0001 are eahsheng ly any spores spores | _—s spores
vigorous, be- vigorous, |
3 0,001 |——— +4 1 |ginning spore- rather | many spore
3 10 000 000 Tepes form. many spores :
! |
*} PE /aa00 000: | cael meme iden
5 0,1 id i
i? hee (00000 |) a ee idem ; .
|
7 ae = i i
| 000d. | ete ae idem a
|
| 0,5 :
are: 100° = 7 teem idem idem " ”
8 10 | : id its
: 1000. - jar ett e eee idem ; ;
9 | 25 mae id i
2 1000 Soa | idem idem i .
5 | |
10 | 50 i000 + +++ idem idem . :
11 | 100 i | id
100. | idem iaem : f
25 ;
12 | 250 100 +4+4++ idem idem re *
5 se |
13. 500 fa +4 4-4+-+ | idem idem a ”
| | |
14 1000 io ++-+4-- idem idem s ”
|

Jry weight obtained after

4 £5 days

ndetermined undetermined

410 “

424 | f

418 | s

ndetermined |

s 292
294
- 290
* undetermined
e 302
“ 306
; | 321
> 318

the mould

material after);

35 days

438

undetermined

477

485

484

undetermined

510

pCt. after

nearly 100 pCt.

undetermined

100 pCt.

nearly 100 pCt.

undetermined

|
|

Milligr. CO, at! Assimilated glucose in
combustion of

35 days

49d 00]

Plastic
Aequivalent
ofthe carbon

after

35 days

30 pCt.

v é
1s
a
i ' : we
x # =
cs i
* \ ie ‘ *
+e
on :

761

etre suffisant & la formation des conidies.” On the contrary the
greater the proportion of the quantity of mould material with respect
to the manganese present, the smaller the production of spores.

This explanation is not, however, in accordance with my obser-
vations as the produced quantity of mould was only very little
increased by the addition of zine. .

But like Bertranp I have observed that by adding manganese, in
spite of the presence of zinc, the production of spores is furthered.

Notwithstanding Bertranp’s excellent investigation only few of the
factors are known which determine the formation of spores.

It is proved, however, that in the hitherto treated cases siackening
of the spore formation is combined with a great plastic aeguivalent
of the carbon.

6. Substitution of rubidium to potassiuin.

In 1879 Nicer1*) made some experiments with rubidium and
caesium *) on the metabolism of Aspergillus niger from which he con-
cluded that these elements could replace potassium.

BENECKE *‘, who studied this question more in detail, proved that
by replacing potassium by rubidium the production of mycelium was
normal, but that sporeformation was inhibited.

He found that the dry weights of the rubidium moulds at the
lower Rb.concentrations were somewhat higher, in other cases again
lower than those obtained ina medium containing potassium. In stronget
concentrations rubidium retarded the growth and only insignificant
coats of mould appeared which did produce spores, which fact BeNECKE
could not account for. Probably the presence of potassium, if large
quantities of rubidium salt are used, then becomes of importance in
relation to the small weight of mycelium.

The results obtained by NAGri1 and Beyecke are here chiefly
confirmed as appears from what follows.

If instead of potassiumchloride rubidiumchlorid is used the formation
of mycelium remains the same. The “rubidium moulds”, however,
are distinguished from those cultivated with potassium by their being

1) CG. v. Niagewi, Sitzungsberichte d. math. phys. Classe d. k. b. Akad. d. Wiss.
zu Miinchen vom 5 Juli 1879.

2) I have proved that caesium canfot replace potassium.

8) W. Benecxe, Ein Beitrag zur mineralischen Nahrung der Pflanzen, Ber. d.
deutschen botan. Gesellschaft 1894 S. 105.

‘Die zur Ernahrung der Schimmelpilze notwendigen Metalle, Jahrbiicher fiir wis-
senschaftliche Botanik Bd. 28 (1895) S.. 487.

762

eovered with only a small quantity of spores; the rubidium
mycelium is moreover more intensely yellow than in normal cases,
when it often is nearly colourless.

The presence of rubidium in the said concentrations when kalium
(0,1°/, KCl) is present has no influence on the spore formation and
on the yellow-colouring of the mycelium. (See Table VI). Here it
may be added that also the addition of 0.05 °/, manganesechloride
accelerates the spore production.

For the experiment I prepared two culture media of the fol-
lowing composition.

Medium A: ; Medium B:
Distilled water in which dissolved Composed like A.; only instead
0.2 °/, ammoniumfosfate of 0.1 °/, KCl, 0.L°/, RbCl was
0.1 ,, potassiumehloride added.

0.07 ,, magnesiumsulfate

0.035 ,, calciumchloride

2 » glucose

Some drops of a dilute fosforic acid solution.

In the careful investigation of Benecke there is wanting an exposition
of the relation between the assimilated food and the weight ot
mould in connection with time.

The results of more exact experiments are united in Table VII.

T. A B 22275
Temp. '33°°E.

‘50 cm’. of the above solutions were introduced into 200 cm*. Erlenmeyer-flasks of
Jenaglas and after boiling inoculated with Aspergillus niger.

Composition of the Growth and spore forming after

') In triplo

*) In duplo.

°) The beginning of spore formation (Nr. 3) is probably caused by the presence
of but slight quantities of potassium.

“UOHN[OS oy} Wor, pasvaddesip sey asoonys ayy [ily (;

| | MOT[VA
MO]JOA WNIT) wintpaoAut s| |
| ‘satods | -a0Aur'satods) ‘saiods Aur soiods |
Maj Joyyer | sSAep p Aue Ajpaey Ajpaey ‘sno. JOA Jou
62 bP 902 | ‘snoJoSIA | Joye SP ‘SHOIOSIA | -OSIA Joyyet ‘}--+--+-+4 + | 100M “ to |
| | moped | moqas |
uinpaoAU wunipaoAw |
‘sarods ‘saiods Aue so.iods
| SAep % Aue Ajpaey (Ajpaey ‘sno. JoA yOu
"GIP ‘609 LLE Jaye se | ‘snodosiA |-O81A Joyyet| “-++- | + | 1D0qN “ T'0 | ¢
saiods | WHO} Sa.tods) — satods soiods Aur sa.iods | |
Aaa rayye.| Suruurseq | Aue A[pavy Aypaey ‘sno. JoA Jou
%/,G'G? PLE LIZ | ‘snoso8ta._| ‘snos031a | ‘snososta |-o81a soyyes} “+++-- | + | om “ 10) 2
| ‘ult0} sarods) — sa.iods saiods Aue soiods |
Suruurseq | Aue AyTpavy |Appaey ‘sno. JoA Jou
"/oS‘OF | 6S | OSE | | ‘SnoJosiA ‘SnNOJOSIA |-O8IA Jayyes) “+--+ a IOM % 10 | 1
| |
! |
RP |
vag Pe Bele hate sale et 9 Jaye) skep (81 (9 b € z I doqye
| | |
: |
jelsoyew pappy JIN
UOGIBD dU} JO. : |
prnow ayzjo | yystam Aap s ‘
is /uolsnquios | paureyqo UuUOTJBVWIOJ OIOdS puB YYMoUNH
dV IN4SBId (ye “QD SW ,
- : ; :

Toga 10 40 TOM “oO J9y}IO poppe Uday} ‘sse]s BUoL JO SySe]} MALIAWNATAY pouvsyo Ay[Njosed oyur paonpo.yur
SBM UO!N[OS VAoqe dy} JO ,WIO OG ‘(4aJBM WOAJ ddIJ) VSOONTS °/) Z ‘(“A9JBM WOAY daIj) oPespULMIOTeD "/y [{Q “(pastppeySAs9) ayeyyns
-winisouseu %/,[{9 “(pasiypeysAso) plow oojsoj °/,¢0'0 ‘ayes UOWWUR "/pG]‘O : PAATOSSIP YOIYM UL JazVM paT]ysip sind Aya,
‘2 of —pe “dway
Th “aah GW a

764

From these it follows that the nature of the metabolism of the
earbon does not change by substituting rubidium to potassium. Tke
rubidium mycelium only proves to contain more glycogen as is
shown by the greater plastic aequivalent of the carbon.

We likewise perceive that also without production of spores the
digestion of the intermediary products is possible, for in spite of the
fact that after 18 days at the rubidium experiment only few spores
appear, the plastic aequivalent of the carbon is lowered from 41.5 to 29°/,,

Summary.

1. Addition of 2.85 cm* normal sulfuric acid per 100 cm? culture
liquid and of 0.5°/, boric acid but feebly influences the plastic
aequivalent of the carbon. In the case of the boric acid we must
ascribe the observed changes to mutation.

2. The action of the factors that govern the development of
Aspergillus niger must not be partially judged; thus, a high weight
of mycelium cannot always be called favourable. This is not suffi-
ciently taken into consideration by Ono, Ricnrer, BerrranD and
JAVILLIER. So it was proved for the action of certain concentrations
of coppersulfate, zincchloride and zincsulfate, that these salts considerably
increase the plastic aequivalent of the carbon, whereas the increase
of the weight of mould is proportional to the retarded spore production.

- = . : : 7
Very dilute zine solutions Caanen —~ 7000000 2 mol .ZnSO,,.

7 Aq p. L.) have no influence. Coppersalts counteract the spore form-

ing in all concentrations.

3. Presence of manganese in minimal quantities does not change
the plastic aequivalent of the carbon; it only acts on the velocity
of the metabolism.

The quantities of dry substance found by Brrrranp should be
considered as values indicating the velocity of the process.

4. By replacing potassium by rubidium thespore formation is coun-
teracted, the weight of mould is increased, and the metabolism of
the carbon (i. e. the change of the plastic aequivalent and of the
respiration aequivalent in connection with time) remains unchanged.

Finally my hearty thanks to Professor Dr. M. W. Briertck and
Professor Dr. J. Boxseken for their assistance in this investigation.

Laboratories for Organic Chemistry and
Delft, October 1912. Microbiology of the Technical University.

Ae
(69

Pathology. -— “On a micro-organism grown in two cases of un-
complicated Malignant Granuloma.” By Exxxstine pe Near and
C. W. G. Mirremer. (Communicated by Prof. (. H. H. Sproncr).

(Gommunicated in the meeting of September 28, 1912).

In recent years Malignant Granuloma, also called Lymphomatosis
granulomatosa or Hopakin’s disease, has occupied the attention of
many writers and researchers, in consequence of which some more liolit
has been thrown upon the subject after a long period of obscurity,

For all this, the etiological evidence brought forward in the study
of this incurable disease is still extremely limited.

In 1832, it is true, Hopexin') published the history of some eases
and autopsies which may, to a certain extent, bear on the disease
we are about to discuss, but its etiology was not dwelt on in the
literature before many years later.

No attempt whatever had been made to distinguish by differential
diagnosis the various diseases, characterised by glandular swellings
and enlargement of the spleen, until Vircaow, in 1845, described
leukaemia as a well defined disease. Next, in 1865, Connuem distin-
guished pseudoleukaemia as a disease of the lymphatic apparatus
resembling leukaemia, but differing from it by the absence of the
typical bloodpicture. Since Connuem the term pseudoleukaemia has
again and again been misapplied to a congery of glandular diseases;
others again added the epithet “tubercular” to it, so that in spite of
Connueim’s discovery, the confusion was again as great as before.

Neither did Brittrora’) confine the term ‘‘malignant lymphoma”,
a name often given to malignant granuloma, to one special affection
of the glands, as he himself says in his paper on Multiple Lymphome.

_STERNBERG*) was the first to describe in an elaborate histological
investigation a definite group of cases, thereby leading the way for
later workers. He was likewise the first to discuss at length the
etiology of the disease, as appears distinctly from the title of his
publication: “Ueber eine eigenartige unter dem Bilde der Pseudo-
leukamie verlaufende Tuberkulose des Lymphatischen Apparates.”
However the etiology, suggested by the title, is not nearly ascer-

1) 1832 Hopexin. On some morbid appearances of tiie absorbent glands and
spleen. (Med. chir. Transact. Vol 17).

3) 1871 Busrotrx. Multiple Lymphome. Erfolgreiche Behandlung mit Arsenik.
(Wien. Med. Woch. N°. 44 5. 1065).

8) 1898 Srernperc. Ueber eine eigenartige unter dem Bilde der Pseudoleukaemie
verlaufende Tuberkulose des Lymphatischen Apparates. (Zeitschr. f. Heilk. Bd

XIX 8, 21).

766

tained in this writing, though we must admit, that the nature of
the available cases were adapted to tempt the writer to draw his
conclusions. For in the great majority of cases, reported by STERNBERG,
there was tuberculosis, besides the special granulation tissue described
by him. As moreover in most cases tubercle bacilli were found in
the histological preparations and only seldom cocci, which had caused
no local reaction, so that he supposes them to have multiplied post
mortem, he coneludes: ‘“dasz es eine eigenartig verlaufende Form
der Tuberkulose des lymphatischen Apparates gibt”.

The fact that there appears the peculiar granulation tissue, as
described by him, and not a pure tubercular tissue, STERNBERG believes
to be probably due to higher or lower resistibility of the patient or
to the virulence of the tubercle bacillus.

At the “Siebente Tagung der Deutschen Pathologischen Gesellschaft’,
held in 1904, where this subject was discussed, Benpa') advanced
the theory that here we have to do with ‘ein sich den malignen
Neubildungen naherndes Granulom welches nicht durch einen spezi-
fischen Infektionstrager, sondern durch die modifizirten oder abge-
schwiichten Toxine verschiedener Infektionstrager hervorgerufen wird”’.
Askanazy believes the etiology to be wholly unknown. Cutart and
YAMASAKI consider the process as a chronic inflammaiion whose etiology
has not been ascertained, but should not be mistaken for tuberenlosis.
ASCHoFr arrives at the conclusion, ‘“dasz es sich nicht um die gewohn-
liche Form der Tuberkulose handelt”, appealing to his failure in produ-
cing tuberculosis in 5 typical cases by inoculation of caviae. Also STERN-
BERG qualifies his assertions when he writes: ‘‘Wenn auch die seither
publizirten Falle diese (his) Auffassung meist bestatigten, so réume
ich doch gerne ein, dasz die damals von uns gewahlte Bezeichnung
“eigenartige Tuberkulose des lymphatischen Apparates” vielleicht zu
weil geht. Immerhin glaube ich, dasz ein Zusammenhang zwischen
dem diesen Fallen zu Grunde liegenden Entziindungsprozess und der
Tuberkulose nicht von der Hand zu weisen ist”.

A most valuable addition to our knowledge of malignant granu-
loma was furnished by KE. Framnxen and H. Mucn’s?)*) discovery
of “eranulare Stabchen”, which they found to be antiformin-resistant
and Gram-positive. This at first seemed in a high degree confirmatory

1) 1904 Benpa. Zur Histologie der pseudoleukaemischen Geschwiilste. (Verhandl.
der D. Path. Ges. 7e Tagung 26—28 Mai).

*) 1910 EK. Frarnker u. H. Mucu. Bemerkungen zur Aetiologie der Hodgkinschen
Krankheit und der Leukaemia lymphatica. (Miinch. Med. Woch. n° 19).

*) 1910 id. id. Ueber die Hodgkinsche Krankheit (Lymphomatosis Granulomatosa)
insbesondere deren Aetiologie. (Zeitschr. f. Hyg. u. Infekt. Kr. Bd. 67).

767

of STERNBERG’s conception, considering that morphologically the granular
“rods” could not be distinguished from the non-acidfast Mvcu-form
of tubercle bacilli. Experimental inoculation of caviae afforded con-
elusive evidence against Srernperc’s opinion. Caviae injected with
granulation tissue obtained from uncomplicated cases were not affected
by tuberculosis.

FRAENKEL and Mvcn do not hesitate to call their granular rods
the causative agent of malignant granuloma; however they are not
decided about the question of their affinity with tuberculosis: “Die
Lymphomatosis granulomatosa ist eine Infektionskrankheit, die durch
granulare Stabchen hervorgerufen wird. Diese granulire Stabchen
sind antiforminfest aber nicht siurefest; sie sind durch verschirfte
Gramfarbung darstellbar, und stehn dem Tuberkulose-virus zum
mindesten sehr nahe. Die Jymphomatosis granulomatosa ist nach
unseren Erfahrungen nur ausnahmsweise mit typischer Tuberkulose
vergesellschaftet.”

At a meeting held at Hamburg January 1912 Frarnket ‘) announced
his discovery of “granula” or “granular rods’ in 16 out of 17 cases.
Availing himself of the additional evidence brought forward by
Meyer, Dr Josseuin DE JonG*)*) (who decidedly inclines to deny the
identity of the tubercle bacillus with the virus of malignant grann-
loma both on the basis of his own experimentation and on the
inoculation experiments of many other researchers), SimmMonps and
JAKOBSTHAL, FRAENKEL writes as follows:

“Ks liegen jetzt iiber mehr als dreiszig Falle Hodgkinscher Krank-
heit von den verschiedensten Beobachtern herriihrende mit den
unsern vOllig iibereinstimmende Aufgaben vor. [mmerhin, das will
ich offen bekennen, ist auch durch unsere Untersuchungen eine
vollige Klarung der Aetiologie der Hodgkinschen Krankheit noch
keineswegs herbeigefiihrt.””, And further on: ‘“‘Es musz die nachste Auf-
gabe sein Reinkulturen der fraglichen Gebilde zu erzielen, und im
Tierversuch weiter zu kommen”.

It is evident that these researches did not throw more light upon
the relation of the rods to the tubercle bacillus, as FRANKEL *) him-

1) 1912 E. Fraenxer: Ueber die sogenannte Hodgkinsche Krankheit (Lympho-
matosis granulomatosa). (Deutsche med. Woch. n°. 14 S. 637).

2) 1909 R. pe Josseuin ve Jone. Bijdrage tot de kennis der pseudoleukaemie.
(Geneesk. Bl. 14e reeks I en II).

3) 1911 id. Over acuut maligne granuloom (Lymphomatosis granulomatosa).
(Ned. Tijdschr. v. Gen. II helft n°. 22).

4) 1912 E. Fraenxet u. Srernserc. Ueber die sogenannte Pseudoleukaemie.
Bericht tiber die XVe Tagung der Deutschen Path. Ges. in Straszburg vom 15-17
April. (Centralbl. f. Alg. P. u. Path. An. Bd. 23, No. 10).

768

self declares in the meeting of the Deutsche Pathologische Gesell-
schaft in April 1912: «Die Frage der Stellung der Granula zu den
Tuberkelbazillen ist noch offen; aetiologisch ist die Lymphogranulo-
matose unklar.”

The death of a boy v. DD. S., 7 years of age, suffering from
malignant granuloma, clinically uncomplicated with tuberculosis,
whose autopsy took place on the 4 of June 1912, 8" 30™ post
mortem gave us an opportunity to cultivate the “rods”, so often
alluded to above. At the autopsy no trace whatever of tuberculosis
was detected, only alterations pointing to malignant granuloma.
The histologic examination of the spleen, a great number of glands,
the bone marrow and the liver, led to the discovery of the granu-
lation tissue which, according to STERNBERG, characterises the disease,
whereas the typical alterations due to tuberculosis were not found.
Nor were caviae, injected with an emulsion of the granulation tissue
attacked by tuberculosis.

In smears of the spleen we could demonstrate numerous rods
fully corresponding with FRragenkeEL and Mvcn’s description of the
granular rods that are found in the typical granulation tissue of the
majority of such cases as were studied for this purpose. No other
micro-organisms could be detected in any of the preparations.

We have been successful in demonstrating the bacteria in only a
few histologic preparations, as was the case with other workers on
the subject. Whether or not this was due to the small number of
organisms present, we are unable to say.

In order to obtain the wished-for result, we have sown from the
spleen on a large number of varying media and we have been
fortunate enough to grow at once, in all the media used, a pure
culture of a micro-organism, which proved in every respect similar
to Fraenkel. and Mucu’s rod.

It was especially on the blood-glycerine-potato-agar plate, used by
BorpEt to cultivate the whooping-cough bacillus, that we obtained
already after 2 < 24 hrs a strongly developed culture, which proved
to consist of rods morphologically in no way differing from the
granular rods.

Before entering upon a description of our micro-organism we point
out the fact, that we succeeded in obtaining from a jugular gland
(patient 5, twenty years old), sent to us for diagnosis, a micro-orga-
nism similar to that obtained post mortem from the spleen of v. D.S.
The histologic examination of this gland made us decide upon
malignant granuloma in making the diagnosis of the typical tissue.
Tubercular changes could not be detected in the preparations, neither

“a

769
were they in any way suggested clinically. Pirauet was negative.
Description of the Micro-organism.

Morphology.
We observed the following forms varying according to the media
and the age of the cultures:

Plump short rods: length 1 yw, breadth */, uw. The short-
ness of some reminds us of coccobacilli of less than 1 mw dia-
meter (a minority on LoxrrLEr’s serum; in eight-week-old
cultures on Bordet medium almost exclusively ; a majority
on agar-plates a few days old).

Small fine rods: polar staining, length from 1'/,—2 u,
breadth + */, w (in every medium of any age).

Rods of from 2—3 mu with polar granules, or more granules
(they are far predominant in the older cultures on LOEFFLER’s
serum).

Comma-shaped rods: in many cases to be divided into
two shorter rods, length + 1°/, u, breadth '/, uw (on Bordet
medium, ascites-agar, and LorrrLeEr’s serum ; in the first ascites-
agar-culture longer and finer than in the later).

Granular rods of different dimensions; length varying
from 5—7 uw, breadth from */,—1'/, u. This considerable breadth
concurs with a prickly shape found on the Bordet-medium,
the rods being broader in the middle and becoming more
pointed towards the extremities. The greater breadth is in
many bacilli due to the irregular arrangement of the protuberant
granules.

In older cultures some giant forms, which however have
not at all lost their original structure, i.e. a distinet body, in
which the granules are seen.

Occasionally branching forms were observed in various
media (Bordet-medium, fluid and solid, Lorrrier’s serum, and
canesugar-nutrose).

Rows of granules: only granules arranged as in the
granular rods but without a visible cell-body. The arrange-
ment is not regular, the granules being placed longitudinally
in different directions relative to the long axis of the granular
rod or row.

-Involution-forms: clubbed or swollen ends (in old enl-
tures) and spheric forms to 2 uw.
Motility is lacking

770

Staining peculiarities: The microbe stains easily with the ordinary
dyes for bacteria. After Gram the small rods show pclar coloration,
positive or negative, according to the medium; the comma-shape always
positive, the body of the granular rods negative, the granules positive.

After Mucn’s modification of Gram’s methods the results agree
with those obtained with the Gram-stain.

With Ziwur’s stain they are not acid-fast.

The microbe is facultative anaérobe, however it grows much better
in presence of oxygen. Growth is sluggish in deep stab-cultures,
covered with agar, and in a hydrogen-atmosphere.

Injluence of temperature on the growth.

The growth optimum is in the neighbourhood of 32° C.

The highest temperature at which growth is demonstrable is 39° C.;
at 40° C. it ceases altogether.

The lowest possible temperature for growth is between 10° and
8°. 6) At. 5° Cex it- is non-existent.

Reaction of media: alkaline reaction is more conducive to growth,
which however is not inconsiderable with acid reaction.

Growth. .
~Gelatin-stabculture: not liquefacient, slight growth in
the track made by the needle, threadlike, getting thinner
lower down.
Smear-culture: growing evenly in moderate amount.
Plate-culture (after 24 hours): cultures elevated on the
surface, dark grey (later greyish-yellow to ochraceous), round,
smooth-rimmed, homogeneous, dewdrop-shaped, dim-glistening.
Later on the colonies are finely granular and the edge gets
finely crenated.
garstabeulture: slight growth in the track, threadlike,
ragged, getting thinner lower down.
Smear-culture: growing evenly in fair amount.
Plateculture (after 24 hours): cultures elevated on the
surface, yellowish, round, smooth-rimmed, somewhat granulous,
granules finer near the rim than in the centre, where a dark
stain is visible, dewdrop-shape, highly glistening, condensation
water cloudy, no pellicle is formed.
Ascitesagarplateculture: sluggish and slight growth ;
colonies finely granular, later here and there more coarsely
granular especially at the periphery, so that the rim, being
smooth at first, now becomes finely lobulated; elevated above
the surface; fluorescence.

771

Young colonies dewdrop-shaped; highly glistening, conden-
sation water as in agar-cultures.

Broth-eculture: slow growth, cloudy with sediment, which
squirms up like a slimy flagellum when shaken, and may be
equally distributed. No pellicle is formed, as is the case in
broth mixed with horse-serum, yeast-decoctum or ascites-fluid.

LOkFFLER’s serumsmear-culture, growing abundantly

in 24 hours, even, very slimy.
Plateculture (24 hours): highly elevated above. the
surface; colour deep canary-yellow, later in part brownish-red,
round, smooth-rimmed, uniformly finely granular, dewdrop-
shaped, moist-glistening, condensation water very cloudy; no
pellicle.

Milk is not coagulated ; ultimately a pinkish coloration.

Glycerin-potato-culture: growing badly ; hardly visible,
light yellow; dim-glistening.

Blood-glycerin-potato-agar (Bordet medium) :
Smear-culture: abundant growth in 24 hours; theculture
first obtained was greenish, afterwards rather brown to brown-
ish-black, chocolatelike, elevated above the surface; very
slimy; easy confluence of colonies; glistening; condensation
water cloudy.

Sporeformation not noted.
Resistance to:

Desiccation: cultures in fluid media did not lose vitality
at room-temperature 1] weeks after drying.

Heating for half an hour at 60° C. kills off the culture ;
when heated for 5 minutes at 80° C. they are also destroyed.

Cold: cultures exposed for 4 hours to a temperature of —60° C,
did not lose vitality. ;

Light: diffuse daylight does not kill the microbe; nor does
it affect growth.

Lifetime: After 16 weeks the cultures have not yet died away.
Chemical conversions.

Formation of Gas: none in broth with glucose or lactose,
neither in nutrose with canesugar.

Acid-production: in nutrose with glycose, mannite, mal-
tose or canesugar.

Alkali has been detected in broth with yeast-decoct. After
5 weeks 1 cem. ‘/,, n. acetic acid on 9 ¢.c. of broth with
yeast-decoct. appears to be just neutralised.

H,S is not produced.

50
Proceedings Royal Acad. Amsterdam. Vol. XY.

772

No more is Indol.

Nitrates are not reduced to Nitrites.

Diastatic fermentation is absent.

Chromogenesis :

Canary-yellow mainly on LOEFFLER’s serum; less intense
on the other solid media (except Bordet-medium); also in the
fluid media.

Muddy green: the first cultures on Bordet-medium.

Chocolate colour on Bordet-medium.

Faint fluorescence on ascites-agar.

Brownish-red in all older cultures except ascites-agar.

Poisonous products could not be demonstrated.

Thus far the microbe did not prove to be pathogenic for animals,
but even now we wish to lay stress on the fact that all our labora-
tory-animals, among which a large number of caviae, some injected
with organic emulsion, others with cultures, remained free from
tuberculosis.

Summary.

The bacterium we have been describing, is to be classed as a
corynebacterium on account of:
its septed structure,
its sometimes peculiar shape with pointed or clubliike extrem-
ities,
its tendency to branching,
its lack of acid-resistance (after Zmut) but great affinity for other
bacterium stains.

We feel assured that this corynebacterium is identic with FRAENKEL
and Muvcn’s rods, observed by them and others in the tissue of
malignant granuloma in a large number of cases.

In describing them Framnket and Mucn mention their peculiar
morphology, their affinity for stains, and the antiformin-resistance.

The morphological description of their rods agrees entirely with
the morphology . of our bacterium, as regards both the smears
from the spleen and those from the cultures.

The Zient- and the Gram-stain ave the same for either bacterium.

As to antiformin-resistance we discovered that it cannot be considered
as a quality peculiar to this bacterium, though we too found some
rods in antiformin-sediments of organic emulsion.

We do not intend to enter into further details in this short space.
Further investigation will have to decide whether or not our coryne-

Fe ety Se oe
Ney

E DE NEGRI and C. W. G. MIEREMET. ,,On a micro-organism grown in two
cases of uncomplicated Malignant Granuloma”.

Figs:
5 Fig. 2

Fig. 4.

Fig. 5. Fig, 6.

Proceeding Royal Acad. Amsterdam. Vol. XV.

773

bacterium occurs invariably in malignant granuloma. In our opinion
this seems to be the case, as may be concluded from the literature
that appeared hitherto. Still, even if this be so, it would perhaps
not by itself entitle us to consider that corynebacterium, beyond a
shade of doubt, as the etiologic moment.

We purpose before long to write more at length about this subject
in another publication.

EXPLANATION OF THE PLATE.
Fig. I Smear from the spleen v. d. S. Gram-stain with counterstain.

» il 48 hours’ Bordet-culture, cultivated directly from the spleen of y. d.S.
Gram-stain with counterstain.

» ill 18 hours’ Bordet-culture after one transplantation. Gram-stain without
counterstain.

» IV Rod with branches from fluid Bordet-medium. Gram-stain with counterstain.

» WV 5X24 hours’ ascites-agar-culture, grown directly from ‘the spleen of
v. d. S. Gram-stain with counterstain.

» VI LorrriLeR’s serum-culture transplanted after 12 weeks from original
LOEFFLER’s serum-culture, obtained from a gland of patient S.

Physics. — “Measurements on the ultraviolet magnetic rotation in
gases.’ By Dr. J. F. Sirxs. (Communicated by Prof. Kamer-
LINGH ONNES.)

(Communicated in the meeting of October 26, 1912).

1. To get an idea of the relative values of the various theories which
have been developed to explain magnetic rotation, measurements may
be made in the neighbourhood of absorptionbands and -lines in the
visible spectrum with a view to ascertain whether the rotation has
the same’) or opposite sign’) on either side of the absorptionband. With
perfectly transparent substances one could extend one’s observations
over a much wider region of the spectrum so as to ascertain if the
experimental results obtained in the ultraviolet, for which the rotatory
constants are much greater, can be more satisfactorily represented
by the one theory than by the other, and if, perhaps, a strong increase
in the rotation takes place on approaching the ultraviolet region.

With gases, and in particular with hydrogen, where, on account
of their simple molecular structure ordinary refraction of light can
well be represented by the assumption of a single kind of ultraviolet
electrons *), and for which the value of ¢/, may be obtained from the

1) Vorat, Magneto- und Elektro-optik p. 133.

Drupe, Hypothese des Hall-effektes, Lehrbuch der Optik p. 429, 1906.

*) Drupg, Hypothese der Molekularstréme, Lehrbuch der Optik p. 419.

8) ABRAHAM, Theorie der Elektrizitét II, p. 261, 1908.
50*

774

magnetic rotation in the manner indicated by Srmrtsema’), the question
arises as to whether ultraviolet measurements would not enable one
to ascertain if this value of @/, is actually constant, and thus justify
such a simple assumption for the case of hydrogen. As the ultra-
violet magnetic rotation has hitherto been investigated only for solids
and liquids’), I was glad to accept the invitation extended to me
by Prof. KamprnincH Onnes to endeavour to extend SisrTsEMa’s *)
measurements to the ultraviolet region of the spectrum with the
same apparatus as the latter had used.

2. In order to obtain good results from the use of this apparatus
absorption of the ultraviolet rays had to be prevented, hence quartz
was chosen instead of glass as the material for the covers, lenses and
prism, while the canadabalsam-nicols were replaced by Guan’s air
layer nicols.

For preliminary experiments I used a fluorescent eyepiece filled
with aesculin solution, but this was found unsuitable on account of
the small intensity of the light. When I had a spectrograph at my
disposal I was able to photograph the dark rotationband which
occurs in the BrocH-WiEDEMANN method and which SiertseMa had
used for purposes of adjustment, but in the ultraviolet the band
was too broad and the spectrum was too feeble to allow the centre
to be determined to the desired degree of accuracy. I decided there-
fore to follow Lanpav and use a half-shadow method.

In this method a half-shadow analyser divides the field into two
halves, whose planes of polarisation make a small angle of 2d° with
each other; if now a_ rotating substance is placed in the path of
the rays between the nicols, and the rays from the analyser are
received in a spectroscope, two spectra are formed, one above
the other, in which the dark rotationband does not occupy the
same position. If the angle of rotation for the position of the band
in the one spectrum is @°, then in the other spectrum the band is
at a place where the rotation is (a+ 2d)°. At a point at which the
rotation is (@-+ d)°, there is, for a special wavelength, the same
intensity in the two spectra. On rotating the polariser the position

1) SIERTSEMA, These Proc. Vol. V, p. 413.

*) VAN SCHAIK, Proefschrift Utrecht 1882. Jousiy, Ann. Chim. Phys. S. 6, T.6,
p. 78. 1889. Boret, Arch. des Sc. Phys. et Nat. Genéve, 16, p. 24, 1903. Lanpau
Phys. Ztschr. 9, p. 417, 1908. Darmois, Ann. Chim. Phys. S. 6, T. 22, p. 247,
495, 1911.

*) Siertsema, Versl. K. Ak. v. Wet, 24 Juni 1898, p. 31; 26 Jan. 1895, p. 230;
28 Maart 1896, p. 294; 24 December 1898, p. 280; 27 Mei 1899, p. 4.

oki
(io

of equal intensity of illumination is displaced along the spectrum.
When using a discontinuous spectrum ‘iron are, or Herarvs quartz
mercury arc) equal intensity has to be obtained between the halves
for a definite line of the spectrum. From a series of photographs
for different positions of the polariser Lanpav obtained that particular
position in which there was equal illumination for a special wave
length; the current was then reversed and the series of photographs
repeated. Such a method of operating is tedious, but it has the
great advantage of giving the required angle of rotation direct from
the photographs without the measurements, which are required for
determining wavelengths in a continuous spectrum.

3. In order to adapt Lanpavu’s method to the investigation of gases,
the following modifications of SimrTsemMa’s apparatus had to be made:

a. The polarising nicol had to be replaced by a half-shadow nicol, to which the
slit was attached. When the halfshadow was used as analyser, the great length
(about 230 cm) of the high pressure tube brought the slit too far from the
source, and the light was then too feeble.

b. Equal intensities had to be obtained by varying the current, as the hallf-
shadow nicol attached to the rotating end of the experimental tube had to be
maintained in a fixed position.

It was now possible, by slightly varying the current for successive
photographs, to determine accurately, for different lines of the spectrum,
the particular current, at which equal intensities were obtained. These
currents are inversely proportional to the rotatory constants, and the
constants can be expressed in terms of a standard line as unit.

A preliminary investigation was made to see if it was not possible
to arrange the nicols outside the experimental tube. As the quartz
covers were ordered of equal but opposite rotations, the measurements
would have been simplified by attaching the analyser with a divided
circle to the spectroscope, for I should then have been able to read
the rotations directly. With the quartz plates placed between the
nicols, however, perfect extinction could not be obtained, so that
for the determination of Verprt’s constant in absolute measure I
was obliged to have recourse to a comparison with water, for which
the constants have been determined by Stertsema') and Lanpav. It
was of advantage then that there was nothing but gas between the
nicols, thus eliminating the influence of repeated reflections and of
the magnetic rotation in the quartz plates.

- 4. A diagram of the apparatus is given in Fig. 1.
L is a Heragus quartz mercury lamp, A a collimator, C and D the coils, PF

1) SrertseMaA. Arch. Néerl. (2) 6. p. 825. 1901.

776

the high pressure tube, B the small rotating endpiece, containing the half-shadow
nicol and slit, E the large fixed endpiece, containing the analyser, G ascrew with
a wheel, by which with the steel wire and the weight J the endpiece B
may be rotated, PQ the spectrograph.

In series with the coils are:

The main switch A,, two dial resistances Wy and Wu indicating to 001 ohm
coupled in parallel, a manganin resistance across which is shunted a resistance box

om _
[-——=y

pint fh

(a
| i Gi

\f wf
i

)
E WAS

eI
AN

of—|
s
(Cl a

H
q
fj

Fig. 1.

in series with a moving coil galvanometer (clock model) by HARTMANN and BRAUN,
an auxiliary switch By in parallel with a sliding resistance, through which the
current is switched before being broken so as to diminish the intensity of the spark.

ene

In the measurements the current varied from 10 to 40 amp. and
was obtained from three 60 volt batteries of accumulators, coupled
in parallel.

For the absolute determination of Verbrr’s constant the current
was measured with an ammeter having three ranges (O—2, 0-20,
O—50 amp). This ammeter was calibrated on the potentiometer,
and, moreover, when taking. the photographs, the variation of the
current was so chosen that the pointer of the instrument coincided
with the graduations as during the calibration, so that the current
is known with certainty to one-tenth of an amp. (one seale division
== 059 amp.)

The pressure was measured on a ScHArrer and BupENBERG metal
manometer with a circular scale of 16 cm diameter, reading up to
150 kg/cm’ by steps ot */, kg/cm’. The greatest difference between
two independent calibrations did not exceed 0,1 kg/em*. We assumed
therefore that the pressure is accurate to 0,1 kg/cm’.

The manometer was coupled directly to the experimental tube,
and, along with it, could be shut off from the rest of the appara-
tus by means of a tap. The rest of the apparatus consisted of
a gascylinder and an airpump (a GarpE vacuum kapsel-pump) ;

Fig. 2.

there was also an exit tap for the gas in the experimental tube, as
it would not have been good for the nicols to expose them to
the high pressure for days on end.

778

To euard against any displacement of the coils, the Ingh pressure
taps which were mounted before on the base of the coils, were now
placed on a separate table. The temperature of the gas was regulated
by that of a water jacket between the coils and the experimental
tube. (These details are easily distinguishable in the accompanying
photograph of the work room).

5. The following remarks may be made concerning the optical

part of the investigation :

The collimator placed in front of the mercurylamp contained a single laevoro-
tatory quartz lens, of 36cm. focal length for the yellow mercurylight, and 3,6 cm.
diameter. The breadth of the slit was 1 mm, and its length was reduced by means
of a brass plate to 2 mm. so as to prevent troublesome reflection from the inner
wall of the experimental tube. A circular opening of 1 mm. diameter was _substi-
tuted later for this slit.

The quartz covers were 11 mm. thick, and their diameters were 26 and 22 mm,
respectively,

The half-shadow (aperture 12 mm. by 12 mm.) with air separation, according to
Guan, had a half-shadow angle of about 2°. It was fixed in a brass mount, and
this fitted closely into a brass cover, whose ribbed sides were soldered im a cylin-
drical tube. The gas had free access to the nicols through the openings, thus
removing any possibility of displacement. To enable one to set the separating line
of the half-shadew horizontal, the cylindrical tube was arranged so as to rotate in
a ring attached to the endpiece. A tube, with a slit 11 mm. long and !/, mm.
wide, perpendicular to the separating lme, was attached to the half-shadow half
of the nicol.

A Guay-nicol, aperture 20 mm. by 20 mm. was used as an analyser; it was
mounted in the same way so as to rolate in the larger endpiece of the experi-
mental tube. The mount was provided with a circular scale of 180 subdivisions
which was used in setting the nicols at a special angle to each other. For the
absolute measurements the construction of the nicols was somewhat modified as
the water entered the airspace, and the nicols no longer polarised. A brass window
(‘/, mm. thick) was cemented between the halves of each nicol, and in this way
the space between the nicols was protected on all sides by a layer of cement from
ingression of gas or liquid.

As spectrograph was used a Société Genevoise spectrometer with a Cornu
quartz prism. The telescope tube contained a single quartz lens, of 36 cm. focal
length for yellow mercurylight, and of 3.6 cm. diameter. The eye-piece was
replaced by a camera, which was constructed in the workshop of the Delft laboratory
by the master instrumentmaker Mr. P. vAN DEN AKKER; the accompanying
diagram shows the arrangement drawn to a scale of one half:

B is a horizontal arm attached to the telescope stand; C is a fixed semi-cylin-
drical brass drum, and D a similar semi-cylinder rotating about an axis coincident
with the vertical central line of the photographic plate, by means of which it
is possible to set the plate at an angle (usually 50°) to the axis of the camera

779
lube; EF is the sliding holder for the dark slide (0,2 by 8,4 em) and ean be

raised by means of a vertical screw (not shown) of 1 mm. pitch. The drums were
slitted in such a way that only a strip of the sensitive plate 30 mm, long and

——

SON) NNENAARRANRRAAR

7H
SS SSSA ASSSSSSSS SSS Sanna

3 mm. broad was illuminated at each exposure. The double spectrum formed was
about 1.5 mm. broad and was 25 mm. long for the range 4358 A.U. to 2805 A.U.
Nineteen photographs could be taken one below the other on a plate 4.5 cm. by
6 cm. (Lumiére Agfa-plates specially sensitive to extreme ultraviolet). The exposures

780

ranged from 1 to 18 minutes. Parts of the mercury-spectrum were photographed,
and the cameratube was usually so adjusted by means of the divided circle of
the spectrometer that the mercuryline to be photographed appeared in the middle
of the plate. Immediately after the development of the plates it was examined in
which photo the intensities of the halves were equal for a special line. This
could be properly observed only when the illumination of the half-shadow slit was
uniform, and for this reason the mercurylamp had to be kept burning in a ver-
tical position.
On account of absorption photographs were taken

for oxygen up to and including 2654 A.U.
,, hydrogen hat Oe re DoT On ss
eECATDON-CiIORIC Cae eee 4 2482 _,,

For ultraviolet absorption by oxygen I find it stated!) that Liveine and Dewar
found absorption from 2745 A.U. upwards in a tube 165 cm. long at a pressure
of 85 atm. and from 3360 A.U. upwards in a tube 18 m. long at a pressure of
sO atm. In my experiments the oxygencolumn of 230 cm. at a pressure of 80
kg/em? just let the line 2805 A.U. through and no more, while for a pressure of
40 kg/cm? the limit of absorption was 2654 A.U.

6. Measurements of the rotatory dispersion were commenced with :
Oxygen.

Before the experimental tube was filled and closed, the nicols were
set at an angle previously calculated. The cameratube was then
replaced by a telescope in order to ascertain what current strength
gave equal intensities of the halves of the green or the violet mercury
line. By a slight torsion of the experimental tube equal intensity
was usually obtained for the blue-violet line 4358, with a current
of about 385 amp, a gas pressure of 85 kg/cm? and an angle of
J2° between the nicols. The necessary current strengths for the ultra-
violet lines could then be calculated roughly by extrapolation from
the dispersionformulae given by Srertsema. If / is the value of the
current thus calculated, photographs were usually taken with currents
of from (f— 2) and to (f+ 2) amp. and a series of careful exposures
were then made at intervals of 1/,, or ‘'/;, /amp. between the values
of / given by the first photographs. A current of 1 amp. gave a
galvanometerdeflection of 1 em. so that with the currents used a
change of 3 to 8 mm. in the galvanometerdeflection could just be
distinguished on the negative by an appreciable difference in darkness.

As the original negatives were too weak for reproduction, I prefer
to give a drawing of a series of 7 photographs of a portion of the
mercuryspectrum (4047—2755 A.U.) with hydrogen at 19°,5 and

1) Kayser, Handbuch. Band III. p. 357.

(81

(6 atm.*). Equal intensities for the line 3130 (in the centre of

the plate occur between the 4th and 54 exposure trom above. The

variation of the current was °/. amp.

Fig, 4.
As the ammeterreadings, or the galvanometerdetlections corrected
to angular deflections, are, for constant gasdensity, inversely propor-
tional to the required VeERpeET’s constants, the relative rotatory con-
stants can be calculated from such photographs; in this the constant
for the violet line 4358 A.U. is usually chosen as unity. The relative
rotation is then obtained from:
R; I a,

l) The line 2805 is the second from the right, not the first as 1s erroneously
shown in the figure. Horizontal distances are magnified four times, and vertical

distances about seven times. Differences in intensity are indicated by differences

in breadth.

782

in which FR, is Verpet’s constant, /, is the current in amp, @, is
the corrected galvanometerdeflection for the wavelength 4358 A.U.,
and R,, J, and a, relate to the other mercurylines. As, owing to small
leaks and to temperature fluctuations, the readings of the manometer
did not remain perfectly stationary, the dispersion was calculated
from

hy, cee ad, _ oP (1+ 8h) _ &o Po
Rowdy ap, (1+ 6t,) ae ae oes

Oo —
0
in which d, is the density, p, the pressure and ¢, the temperature
of the gas during the measurement with the line 4858, the subscript
2 denotes the other wavelengths, 6 is the pressurecoefficient (taken
from AMAGAT’s observations), and /; is equal to p; {1-++ 8 (¢,—4)}.
Since P; does not differ much from p,, deviations from Boyur’s
law need not be taken into account. For the reduction of the ob-
servations at the lower pressure from 2805 to 2654 A.U. the rotation
for the line 2805 was first taken to be unity, and the relative dis-

2805

persion was then obtained by multiplication by
0

The oxygen used was supplied by the “Oxygenium’” Company,
Schiedam. It was analysed in a Hemper absorptionbulb filied with
copper gauze, moistened with a solution of ammonia and ammonium
carbonate. For the gas with which the most reliable results were
obtained, 97 °/, of oxygen was found.
_ The following table is from the photographs, obtained on the 21st
to the 25% of May :

Tf ASB Bea:
_—________— eS
a. _ pressure temp. _galv. deflect.
Ain ASS rasa aie AL eC, | mm. | ‘
| {
4358 83.8 <4. 335.9 | 1.00
4047 83.8 Mire 304.9 1.10
3665 83.29 il 258.2 lol
3130 84.9 16.9 184.2 | -4.7@8
2805 82.5 17.4 152.3 cles
|
2805 40.9 16.7 314.1 | —
2155 41.3 Wife 301.9 2.31

2654 41.05 16.5 280. 1 | 2.50

783

The pressurecoefficient was taken to. be 0.0046 for an initial
pressure of 84 atm. and 0.0042 for a pressure of 41 atm. These
values were obtained by extrapolation from AmaGar’s observations °),

Hydrogen.

7. The first series of measurements were made with double
purified hydrogen, supplied by the “Oxygenium’ Company ; analysis
in a HempeL explosionbulb showed no impurity. With a view to
absolute determinations measurements were subsequently made with
a cylinder of very pure hydrogen which had been prepared in the
Leiden laboratory by freezing out the impurities at low temperature.

Measurements dated 244 to 295 of May with the first gas gave
the following results:

hia BeL. EW.
. pressure temp. galv. deflect.

Ain AU.) “in atm. | in °C. mm. R,/Racar
4047 54.1 15.8 373.8 1.00
3665 56.8 Lee2 288.1 1.239
3130 597 14.9 197.1 1.79
2805 52.8 | 15.7 159.6 2.40
2654 57.8 15.9 126.9 2.759
2535 56.1 16.5 {15.2 3.14

4 107.0 3.355

2482 |.) | 56.4 16.

The nicols were set beforehand at an angle of 92°. The exposures
varied from 1.5 to 10 minutes. The pressurecoefficient was taken
to be 0.0087 and no correction was applied for deviations from
Boy.e’s law.

A higher pressure was obtainable with the Leiden hydrogen, and
the nicols were accordingly set at an angle of 92°.5 for that series
of measurements. Currents were measured with the ammeter already
described. (range 0 to 50 amp, 1 scale division = 0,5 amp).

The exposure for the last two ultraviolet lines 2399 and 2378 A.U.
was 18 mts; the current was kept constant at 10 amp. for an hour.
On account of the heating of the coils not more than three expo-
sures could be made in any one series. The following are the results
of these measurements :

1) Wiittyer. Experimentalphysik. 5te Aufl. Band II. Tab. p. 138.

784

TAB E Ul

4358 | 93.85 | 18.6 | 35.74 1.00

4047 | 93,9> &| d833 | 30.18 1.18

3665 00.0: deere || abees a sees

3130 Boa = 4c Ages 17.70 2.145

3130 76.0 (9.5: | . 205 see

2805 75.2 19.8 | 15.69 | 2.88

2654 715.5 19.7 13.44 3.29

2535 74.9 20.9 (2.10, 591) Baan

2482 | 75.0 20.5 11.44 | 3.908
9399 | 74.7 19.3 10.44 4.27
2378 74.8 19.3 10.19 Arr ius

By calculating values of f,/f,,,, from these measurements we
can compare the results obtained with the Leiden and with the
Oxygenium hydrogen:

TA BL EA.

| R/Raoagz | Rj/Raoar

sin AU. “Teiden Oxygenium
4047 1.00 £700
3665 1.23 1.235
3130 1.815 1.79
2805 2.39 gee
2654 2.78 2.7155
2535 3.105 3.14
2482 3.30 3.355

As the photographs for the last ultraviolet lines were much sharper
for the Leiden hydrogen, 1 have used the values obtained with it
for the construction of the dispersion curves.

Carbon-dioaide.

8. For this the rotatory constants are greater than for the other gases..
The measurements were made at a pressure of 27 atm. as at higher
pressures small temperaturefluctuations gave rise to currents in the
gas, which rendered the image of the slit indistinct.

785

Commercial carbon-dioxide was used after purification by distil-
lation ; analysis in an absorptionbulb, filled with iron cauze and
potassium-hydroxide, showed 96°/, CO,.

The results of the experiments are here given:

TA. BE: V.
pres ee ) a [Fae Ga rec
Le (il
4047 | 25.39 16.1 SO0%n 1.00
3665 Piles. Mino 211.9 1.225
3130 Paths: afta. 189.9 1.79
2805 ie Wie 149.8 2.275
2654 PA aA 16.5 129.6 2.019.
2535 Peles: 16.2 114.6 Pade ts:

Exposures ranged from 1,5 to 10 mts. An additional series of photo-
graphs of the green and the blue-violet mevcurylines was also made
upon Agfa-chromatic plates in order to afford a comparison with
SIERTSEMA’S results. The correspondence was found to be very good:

TAB LE .Vi

R,/Rs461

A in AU. R;/Rs461 (after SIERTSEMA)

5461 1.00 1.00
4358 1.605 1.60
4047 1.87 1.87

Determination of the absolute rotatory constants.

9. It has been mentioned already that the arrangement of the
apparatus for the half-shadow method does not allow of a direct
measurement of the angle of rotation, so that a calibration with water
is necessary for an absolute determination of the rotatory constants.
If the rotatory constant for the wave-length 4 at a definite pressure
and temperature is yg for hydrogen and Ry for distilled water
and if the currents used for the two photographs were /j7; and. Ly
amp. respectively, then

Ry=s fw Ry.
TH

786

In this formula the currents must be known with the same rela-
tive accuracy. As the rotation by water for the mercuryline 4358
A.U. is about 25,3 times greater than for hydrogen(100 kg/em? 17.°5),
the ammeter ranges used were 0 to 2 and O to 50 amp. After
filling the experimental tube with water I found, contrary to expec-
tation, that the 230 cm. column transmitted the ultraviolet only up
to the wavelength 3665 A.U., while Lanpau with a waterlayer of
1 em. was. still able to obtain photographs of the iron line
2496 A.U. I finally used only the line 4558 for these measurements.
The exposures were two minutes for hydrogen and five for water.
On account of the repeated fillings of the experimental tube the pres-
sure obtainable from the Leiden cylinder of hydrogen sank to
75 ke/em?, so that the currents used for the gas were about 34
times those required for the water photographs.

In this way I obtained for :
Hydrogen (73.9 atm. 16°.9.) /77 = 37.72 amp.
Distilled water Iw =1.145 amp.

According to SrertseMA yy = 0.02495’ for 4 = 43858. From my
measurements we may calculate /77=: 32.88 amp. for a pressure
of 85 ke and a temperature of 9°.5, whence it follows, that Ryz(85

787

kg/em* 9°.5) = ‘869 & 10-5)’. This agrees well with the value given
by Srertsema: (863 < 10-®)’, ;

1. This led me to anite my results for the three gases with
SIERTSEMA’S, and to plot the dispersioncurve for each for the
visible and ultraviolet regions. The rotatory constant for the yellow
mercuryline (mean wavelength 5780 A.U.) was taken to be unity:
along the axis of abscissae are plotted wavelengths in mu, and
along the axis of ordinates the following relative rotations:

Pe ACES EE Vil.

RJRsis
teh Oxygen edi Hydrogen

578 1.00 1.00 1.00
546 1.08 1.125 1.125
485 1 .26° 1.439 1.44
436 1.50 1.805 1.815
404.5 1.655 2.10 PAG ts.
366.5 1.969 EJAY | 2.64
313 2.695 3.76 3.90
289.5 3.369 4.77 5.14
265.5 3.759 5.49 5.975
2555 6.195 6.67
248 7.09
240 7.76
238 1.94

The dotted line at 423 wp gives the limit of SrertseMa’s obser-
vations.

It is to be remarked that the oxygen-curve deviates considerably
from those for the other gases, but that there is no sudden change
as the ultraviolet absorptionregicn is approached, and that the
difference between hydrogen and carbon-dioxide begins to be good
appreciable in the ultraviolet region.

On the assumption that ultraviolet refraction in hydrogen satisties
a formula of the type

~ Proceedings Royal Acad. Amsterdam. Vol. XV.

in which 2,,, the wavelength of the ultraviolet free vibration, is
taken to be 0,087.7), the following values have been calculated

for e/m: ’ we
Zin up éfm *~10-* for H, (85 kg 9°.5)

589 dea
405 acTsS
53) i Beal
265 1.85°
245 1.86
238 137"

The increase here found for e/m does not accord with the assump-.
tion of a single ultraviolet free vibration.

I must, in conclusion, offer my warmest thanks to Prof. Dr. H.
Kamerninch Onnes for inviting me to undertake this investigation
and for placing the necessary high-pressure apparatus at my disposal
and also to Prof. Dr. L. H. Srertsema for granting such excellent
facilities for the work and for the unflagging interest with which he
has followed the investigation. a

Delft, October 1912. Physical Laboratory of the
Technical University.

1) SteRTSEMA and pE Haas. These Proc. Vol. XIV. p. 603.

(December 30, 1912). Q

'
1
wr H
'
j ”
‘ . "
P st
r F 7
: Y
7 ey ¢
‘
’ i \ *
“ ‘
§
: i di
\ a

aes
a Ah 4

% i

av
pe ae ear it
Yo ek Ae Le Op Vera, Hs
Tae Ne ns, diy te

ips Fy, i j ;
« a any C=

w
‘

a? =

ae nde eS Su

pes tS

wise
re zr
>
-—

pepe t , J ‘ t ie tly ‘ ‘
ks . ay
S ‘ Ryans y ; . ‘
$ 7 ‘ s = Z
; , 1 . %
j ‘
> r Ml * ‘ «< x f ‘ ’
4 4 — i] =~ m hs t »
ws i * ‘ AY ;
. ba ®i 7 Sey .
i } ry ‘
ne ' ck , rt i , ; a Mths :
“¥ aa 'rt - ay Poe ae
a» rr af . . Par) tw :
Bt 250, a | . ‘ . o> , a ‘
'
i : “ 4 “ ¥
' ' ‘
. , .
’ - ;
" '
] .
. "
‘
a
; . .
‘ fl 5 '
» . %
n ‘i »
« iY ‘
’ i — ‘ . ‘
. ‘
4 : . " ‘ \
a v4 ’ s bes
. f 4 .
vf , - -
, ‘ i . =
: . 4
’
‘ N —_ ;
‘ . ~ al 7
r . . ; <
> , ay ¢ “uy . =
- i
; rr le! = 4 ~
- a
- r . .> .
. “| * . r ae
' ing " is ss -
=

Q Akademie van Wetenschappen,

vt Amsterdam. Afdeeling voor
AL8 de Wis-— en Natuurkundige
v.15 Wetenschappen

pt.l Proceedings of the Section
Physical & Of Sciences

Applied Sci.

Serials

PLEASE DO NOT REMOVE
CARDS OR SLIPS FROM THIS POCKET

UNIVERSITY OF TORONTO LIBRARY

STORAGE

rg en :

a P ¥ as Seen AP « : 77 vent Sw” s - , z ’
ee eee En | Se a a nae Dlg OREN AIP PSE ae eae ms gt
. “ . . . ’ re = . '

wy aS 4° ogee seed natal ion y Salat

= he

Internet Archive Audio

Featured

Top

Images

Featured

Top

Software

Featured

Top

Books

Featured

Top

Video

Featured

Top

Mobile Apps

Browser Extensions

Archive-It Subscription

Save Page Now

Full text of "Proceedings of the Section of Sciences"

See other formats