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PROCEEDINGS
ROYAL SOCIETY OF LONDON.
From December 1, 187S, to June 18, 1874.
LONDON;
PKINIED BY TATLOE AND DtANCIS
112645
I
CONTENTS.
VOL. XXII.
Na 148.— Dwentier 1, 1873.
Annivenei]' MeetiDg :
Report of Auditora 1
Idit of Fsllowa daceued, Ac. aiiice last Annivenuy 1
elected 2
AddraBB of the Freaideiit 2
Fiesentatioii of the Medals 10
Etection of Council and Officers 12
Iluncul SUtemeot 14 & 16
Tniat Fonda 10-18
Account of the a^ropnAlion of the sum of £1000 onuuslly TOt«d b j Por-
lisment to the Royal Society (the QovenimeDt Grant), to be employed
in aiding the advancement of Saenco 10
Bepoit of the Eew Committee SO
December 11, 1873.
A Qnantitatire InTeatigBtion of cert^ Belations between the Gaseoua, tho
liquid, and tho Solid States of Water-Substance. By Professor James
Thomson, LL.D., Queen's College, Belfast 27
On the Action of Heat on OraTitating Uaasee. Br William Crookee,
FJl.8. &c -. 37
On the Hale, and the Stmcture of Thaumop» ptUudda. By It. tod Wil-
lemoes-Snhm, PkD., H,M.8. ' Challenger ' 42
On the Beudins of the Ribe in Forced Breathing. By Arthur Ransome,
M.D. 43
December 18, 1873.
On ttie Period of Hemisphetal Excess of Sun-spots, and Qia Sft^y Period
of TcRWtaial Uagnetiim. By 3. A. Broun, F JI.S. 43
On Ihc KeiTOus System of XrfiniVt— Part I, By rrdfi-eaor P. Mnrtin
Ihmcau, M.D. Lond., F.U.S., &c.
On certain Discrepancies in the publiahed numerical v&lua of ir. P7 Wil-
liam Shanks , 45
On Double Refraction in a Viscous Fluid in motion. By J. CleA Miuwetli
M.A., F.R.8., Professor of Eiperimental Phjsica in tho Univuisity uf
Cambridgi; 40
Liet of Presents 48
No. Ii9.—Jat>varu S, 1874.
On the Brom-Iodides. By Dr. Maxwell Sitapson, F.E.a, Profcfaor of Cho-
miatry, Queen's College, Cork 51
Contributions to the History of the Orcins.— No, IV, On the lodc.-dorivd-
tivea of the Oraina. By John Stenhouae, LL.D., F,H,S., &c
A Memoir on the Transfurmation of Elliptic Functions, By Professor
Cayley, F.R.S
On EicctrotorsioQ. By George Ooro, F.ltS G7
i/imwiry 15, ItiTi.
FieliminaiT Account of an Investigation on tlio TnuismisaioD of Sound by
the Atmosphere. By John Tyndall, D.C.L., LL.D., F.R.S
Jaimary 22, 1874.
On the Nature and Physiologiciil Action of the Poison of Koja tiimdiana
and, other Iijdian Venomous SnaJtes.— Part IT. By T. Lauder llrunton,
MlD^ ScD., M.R.C.P., and J. Fajrer, C.S.I., Hf.D., F.II.C.P. Lond,,
and, other Iijdiai
M.D^ Sc.D., M.iv.ij.r., mill J. j'Bjitr,
F.R.S.E., Sui^^eon-Major Bengal Ariny ,
Jamtary 2D, 1874.
Contributions to the Normal and Pathological Anatomy of tho Lymphatic
System of the Lungs. By £. Klein, M.D., Assistant I'rofeseor at the
Laboratory of the Brown Institution, London 133
On the Comjiarative Value of certain Geolc^ical Ages (or mups of forma-
tions) considered as itemsof Geological Tune. By A. C. liameay, LL.U.,
V,P.R.S Hfi
LiBtofPiwenU 148
No. 150.— JWn/ory 6, 1874.
On the Anatomy and Habits of the genus Thronima (Latr.). Bt John Denis
Macdonald, M.D,, F.R.S., Slaft' Sur^on R.N., Assistant Trofeasor of
KaTftl Hygiene, Netley Medical School (Plate I.) 164
On & Self'TMOTtUoff Metbod of Measaiinji; the Intentity of the Chemical
Aetioa of Totel DayligfaL Bj H. £. Roacoe, F.R.S., Ptakaaor of Ohe-
miatrj in Owens College, Uuichettet 168
Contribn&nu to the HistoiT of Ezplomre Agenta. — Second Uemoir, By
F. A. Abel, F.R.a, TVew. C.3 ICO
I^n-ary 13, 1874.
Note on the SnitheeiB of Formic Aldehyde. ■ By 3ii B. C. Brodie, Burt,
F.RS. ■; 171
On the lafluenca of Brandy on the Bodily Temperatare, the Pulse, and the
BMointions of Healthy Men. Br R A. Parkeaj U.D., F.R.8., Professor
of Hygiene, Amy Uedical School 172
Experimental Demonstrations of the Stoppage of Sound in partial Reflec-
tiona in a noD-homogeneous Atmosphere. By John Tyndall,. D.C.L.,
LL.]>., F.R.a, Frofeasoi ot Natural Philosophy in the Boyal InsUtution 190
On the IMvinon of a Sound- Wave Ip^ a Layer of flame or heated Qas into
a reflected and a transmitted Wave. By John Cottrell, Assistant in the
Phyncal Laborato^ of the Royal Institution 100
Hiivary 19, 1874.
On the Absorption of Carbonic Add by Saline Solutions. By J. Y. Buchii'
nan, Chemist cm boaid H.M.S. < Challenger ' 10?
On an Lsstrameiit tot the Compoeation of tvo Harmonic Curves. By A. E.
Donldn, U. A., F.R. A.S., Fallow of Exeter CoUege, Oxford 196
On tlie Knmher of Fiiirnrea in the Period of tlie Reciprocal of orery Prime
Number below 20,000. By William Shanks 200
Rbmar]/ 26, 1874.
The Winds of Hnrthem India, in relation t« the Temperature and Vapour-
coDstitaentof the Atmow^ere. By Henry F. Blantord, F.O.S., Meteoro-
logical Reporter to the Goremment of Bengal 210
Note on IKsplacement of the 8<Amx Spectrum. By J. H. N. IlenDOssoy,
F.R.A.8. .VTT. 210
On White lines in the Solar Spectrum. By J. n. N. Hennessey, F.R.A.S. 221
UatofPrawnta 223
No. 161.~ManA 6, 1674.
liMrfCan^dates for Election into the Sodety 228
Hie Loealinlicm of Function in the Brun. By David Fwrier, M.A., M.D.,
M.R.C.P., Profeaeor of Forenric Medicine, King's College, Ixmdon 229
Marcit 13, 1874.
Pi
Contributions to thu Pevelopmeutal IliatoiT of the MoUusca. Sections !.,
II., III., IV. By E. Eay Lantester, M.A., Fellow of Exeter College,
Oxfoid 3
Od a New Deep-Ben Theraionieter. By Henry Nogrotli and Josepb Wwwn
ZtunLro, 2
March 18, 1874.
Frelinucaiy Notice of Experigicnis concerning the CbemicBl Constitation
of Saline Solutions. By Wftlter Noel Hartley, F.C.8,, Demonstrator of
Chemistry, King'ti CoUogo, London 2
Note on the iDtmcellular Development of Blood-corpuaclea in Mammalia.
By Edward Albert Schafer 2
On the AttroctioDa of Magnets aud Electric Conductore. By Geonra Qore, _, .
F.it.s TTr. a«l
Spectniacopic Obscn-ationa of the Bnit. By J, Norman Locbyer, F.B.S., and
O. M. Scabroke, F.R.A.S 247
March 2^ 1&74,
On the Oimnization of the Fosul Plants of the Coal-measurea.— Part VL
FeniB. Bv W. C. Williamaon, F.E.S., Frofeaeoi of Natural Hiatoiy in
Owens College, Ifancheatet 248
On the Motaona of gome of the Nebule towaids oi &otn the Earth, Br
"William Hugpna, D.C.L., LL.D., F.R.8 261
Go the Annnal Variation of the Magnetic Declinatioo. By J. A. Brotin,
F.K.8. 264
Ldat of Presents 268
On the NervouB System of Actinia. — Port I. By Professor P. Martin Don-
can, M.B. Lend., F.R.8., &c. (Plates II. 4 III.) 203
No. 162.— ^prit 16, 1874.
On the Pneumatic Action which accompADiea the Aiticulatdon of Sotmda
hy the Human Voice, as exhibited by a Recording InatrumenL By W.
H. Barlow, F.R.8.,V.P.Inst.C.E. 277
Note on the Periodicity of EftinM, By J. H. N. Henneeaey, F.RA.S. . . 280
Studies on Biogenesia. By William Roberts, M.D., Manchester 280
4"^ 23, 1874
On Bome Foint* connected with the CircuUtion of the Blood, arrired at
from a Studj of the SphygmoRTaph'TTace. By A. H. Gftirod, B.A.,
Fellow of St. John's College, Cambridge : Froaector to the Zoological
Society 201
Note on the Hiante Anktmnr of the AUmentaty CanAl By Ileibert
Watney, ILA. Cantab 293
- On the lU&action d Sound br the Atmosphere. By Prof. Oabome Rey-
nolds, Owens Coll^, Manchester SOS
April 30, 1674.
The Stnctue of the Mncous Membrane of the Utcms and its Periodical
Changes. By John Williams, U.D. (Lond.)r Aasistant Obstetric Phy-
sidan to Unireraity College Hospital 207
On Leaf-^Anangement. By Hubert Airy, MA., M.D. 298
On tluLiqpiiimaient of the Spectroscope. By Thomas Qrubb, F.Ra ... . 308
Jr<9 7, 1874.
lost of Candidates for Election into the Society 310
PreliminaiT Ezperimenti on a Magnetiied Copper Wiio. By Professor
Balfoni Stewart, LU)., F.R.8., and Arthur Schuater, I^.D 311
Note on sinne Winter Thermometric Obeerrations in the Alps. By Prof.
E. Fimilklan^ P.RB f7. 317
Addition to the Paper, " Volcanic Eneigr : an attempt to develop its true
Origin and Cosmical Relations." By Ilobert Mallet, A.M., C Jl, F.R.8.,
Mfi-LA., *c 828
listofPrManti 329
On the Comparatire Value of certwnOeolodcal Ages (wgroupBof Forma-
tions) conridered as items of Geological Time. By A. 0. Itemsay,
LL,D., V.P.R.a 334
No. 163.— afoy 21, 1874.
On tbe Stmctore and Develc^ment of Piripaiut et^mtU. By H. K.
Moaeley, H.A., Naturalist to tho ' Challenger ' Ezpraition 344
The [Tnifbnn Wave of Oscillation. By John Imray, H. A., HembJnst.O.E. 360
On ComMnations of Oolonr by means of Polariied Light. By W. Spottis-
woode, M.A., Treas. ft V.P.R.S 864
Farther Experiments on the Transmission of Sound. By John Tyndall,
1>.CX., LLd., FrolMsor of Natural Philosophy in the Royal Institution 360
On Bonie recent Experiments with a Fireman's Itespiralor. By John
TyndaU, D.C.L., LL.D., Professor of Natural Philompby in the Royal
Institution , . 3G0
Election of FflloY
Jaw 4, 1874.
June 11, 1874.
1
Note on the Abwrption-Speetw of PaHtitim mi SoCiMt <* Imt Vina** ' ' -^
nturw. ByH.E.RDeaoe,F.Ra,cBdAitlHffSdiBrt«r,nJD.'(PHit»Iv;)'IBI
Note on the idleged Existence rf fiaDuIu of ft L^mnlBff ia On»4apoittl '
ofEngWd. B7Profbs»orOimjOJB^'KB.B..^ 8B4.
On the alleged Expanmon in Volgnu of nriooi SUMineoi In PMdna 1^
Befiigeration from the state erf li^dd ToAm ta that of BtAdiSeMaB.
By Robert Mallet, G.£., F.R.a •■•■••< ^
Ifote on the Excitation of tli« thalteo of tite Oenlml Bmb^hoMt \y
Induced Ourrente. By J. Budon Smdenni, M.D^ F.B.S., Pm&Mor ct
Practical PbjnologTinlTDiTan^OoUegartondon ...,.,.,,Mft
SpectroMX^ic Notes.— No. L On tl« AbMntion of smat lUdbaMM of ; >)
Metallic and Metalloidal Vaponn. Bj J. Noimaa Locikjer, FJLS. . . . . KTl
Spectroscopic Notes.— No. IL Oa As B
Structuie. Bj J. Norman Loekyer, F.fi.8. S7S
Spectroscopic Notes.— No. ItL On the Molecular Structure of Vi^urs in
. connexion with thm Denudes. By J. Norman Loclcyer, F.R.S. 374
Spectroscopic Notes.— No. IV. On a new Class of Absorption I^enomena.
By J. Norman Lockyer, F.R,8 378
June 18, 1874.
A CtnitributJon'to the Anatomy of Connective Tissne, Nerve,' and Muscle,
with special reference to tlieir couteiioa with , the Lymphatic System.
ByG.Thm,MJ>. 880
Given the Number of Figures (not exceeding 100) in the Reciprocal of *
Prime Number, to determine the Prime itoelf. By William Sbanks. . . . S81
On the Number of figures in the Recipvcal of every Prime between 30,000
nnd 30,000. By William Shanks ....884
Resentch on the Smallpox of Sheep. By E. Eldn, M.D., Assistant Pro-
fessor at the Laboratoiy of the Biown Institution, London 388
Researches in Spectrum-Analysis in connexion with the Spectrum of the
Sun.— No.rV. By J, Norman Lockyer, F.R8 891
An Account of cert^ Organisms occurriug in the Liquor Sanguinis. By
William Osier, M.D, (PlateV.) 801
On Coniferine, and its Converrion into the Aromatic Principle of Vanilla.
Dy Ferd. Tiemann and Wilh. Haarmanu 806
On the Forces caused by Evaporation &om, nnd Condensation at, a Surface.
By Prof. Osborne Reynolds, of Owens College, Manchester 401
Rese^icheB oa Exploaives.— Hred Gunpowder. Bv Owt. Noble, late RotoI
Artiller;, F.RJB., F.R.A^., F.C.S., and F. A. Abel, F.R.S., Tkm. C.'S. 408
On the Diuretic Action of DigiUdu. By T. Lauder Bmnton, U.D., D.Sc,
»Dd Hemj Power, M.B, F.R.O.a 420
Description of the Living and Extinct Racea of Gigantic Land-Tortoisea. —
FitrtaLaiidlL Introduction, and Ibe Tortoises of the OalapagoB IslaDds.
By Dr. Albert Giinther, F.R.8 421
No. \^.~^m» 18, 1874 (eimtmutd).
On Dredginin and Deep-aea Soundings in the Sooth Atlantic, in a Letter
to Admiial Richards, C.a, F.R.S. By Prof. Wyvilla Thomson, LL.D.,
F.RS., IMreetoT of the Civilian Staff on boaid H.M.S. ' ChaUeug«r.' .... 423
On the Centre of Motion in the Hunuin Eye. By J. L. Tupper 430
Some ObsArvations on Sea-water Ice. By J. Y. Buchanan, Chemist on
Board H.M.S. 'Challenger' 431
On the PhjsiolngicBl Action of the Chinolino and Pyridine Bases. By
John 0. M'Kendrick and James Dewar, Edinburgh 432
On the Calculus of Factorials. By the Rev. H. F, C. Logan, LL.D. 434
On the Employment of a Flsjiimeter to obtain Mean Values irom the traces
ofcontinuoDa''' ""----■'- *' 1. ■..n .. .. t... ^ i... ..
Scott, H.A.,
of continuoDaly Self-recordinir Meteorological Instruments. By Robert II.
°— "i.,F.R.S : : aoo
Magnetic Observations at Zi-Ka-Wei. By M. Dechevrens, Directts t^ the
Observatory 440
Experiments with Safety-Lamps. By William Galloway, Inspector of
Mhies. (Plates VL& VII.) 441
. On the AdiabatJcs end Isothermala of Wal«r. By A. W. Riicker, M.A.,
Fellow of Brssenose College, Oxford 451
Contributions to Terrestrial Magnetism.— No. XIV. By Oenerol Sir Ed-
ward Sabine, R.A., KC.B., Flt.S 461
Table* of Temperatures of the Sea at various Depths below the Surface,
taken between 1740 and 1668 ; collated and reduced, with Notes and
Sections. By Joseph Prestwich, F.R.8., F.G.8 402
On the Sun-epot Period and the Rainfall. By J. A. Broun, F.R.S 460
On the Mechanism of StrombolL By Robert Mallet, M.A., F.R.S 473
List of Presents 473
No. 155.
On the Absorption of Carbonic Add by Saline Solutions. By J. Y.
Bnehanan, Chemist on Board H.M.8.'0bBl]enger' 483
OntheUaclMiuflmofSttomboU. By Robert Unllet, MA., F.B.S. 400
ERRATA.
Page 45, line 8 from bottom, 6th group of 5 decimak, .
II II ** $f ^»^ f» »» .
„ 424, ,, 18 „ for long, 80'' 20' 8. read]
ILLUSTRATIONS.
Plate I. illustratitig Dr. J. D. Maodonald's Paper on the Anatomy and Habita
of the Oenns Fhnmima (Latr.).
PIat«s n, & in. iUuetniting Profetsoi P. Martin Dunean'a Paper on the
Nerroos Syetem of Acttitia,
Plate IV. illoatnting Messrs, H, E. Rosooe and A. Sehuater'a Paper on the
Ahsorption^pectn of Potasaiam and Sodiom at low Temperatures.
Plate V. illaBtrating Dr. William Osler'^ Paper on eertain Organisms occur-
ring in the laqnor Sangninis.
Plal«e VT. & Vn. iUustraUng William Qallowa^'s Experiments with Safetr-
Flates Vm-XL illnstiating Dr. Q. Thin's Paper on tlie Anatomj of Con-
neetiTe IWoe, Nerve, and Mnscle.
PEOCEEDINGS
THE ROYAL SOCIETY.
Decanber 1, 1873.
ANNIVEKSAET MEETING.
Sir GEORGE BIDDELL AIRY, K.C.B., President, in the Chair.
Mr. Merrifield, for the Auditors of the Tresflnrer'B Acconnta on the part
of the Society, reported that the total receipts during the past year,
including a balance of ;£447 16s. lOd. carried from the preceding year,
amoont to X4914 19*. 5d. ; and that the total expenditure in the same
period amonnta to X4221 6i., leaving a balance at the Bankers of
.£690 131. lid., and £2 19>. 6d. in the hands of the Treasurer.
The thanks of the Society were voted to the Treasurer and Auditors.
The Secretary read the following Lista : —
Fellows deceased since the last Anniversary.
On the Home Litt.
Thomas Baring.
Bichard Beamish.
John Bishop, F.B.C.S.
Lord Chief Justice Sir William
Bovill.
Thomas Shaw Brandreth.
Charles Purton Cooper, LL.D.
Frederic Crare-CalveH;, Ph.D.
Baldvrin Franris Duppa, F.C.S.
John Edye, C.B.
Eev. Geoi^ Fisher, M,A.
Charles Philip Torke, Earl of
Hardwiche,Tice-Admira],D.CX.
Sir Henry Holland, Bart., MJ).,
D.CX.
Henry Pence Jones, MJ)., D.C.L.
Bobert MacAndrew, F.L.S.
VOL, xin.
John Bobinson M^Clean, M.I.C.E.
Sir Frederick Madden, K.H.
Edward Latham Ormerod, M.D.
George Ormerod, D.C.L.
Prof. Bichard Partridge.
William John Macqnom Bankine,
LL.D.
Sir Francis Bonalds, Knt.
Bev. Canon Adam Sedgwick, M.A.
Archibald Smith, LL.D.
John Spencer Stanhope.
Paul Edmund Count de Stnselecki,
C.B.
Su- WiUiam Tite, C.B.
Samuel Wilberforee, Lord Bishop
of Winchester.
SI^HHEUi^H
J
>t Anniversari/ Meeting. [Dec. 1, 1
On ihc t'hrii.jn List. |
AuguBte De U Bive.
ChriBtopher Hansteen.
Baron Justus von Liebig,
Gustav Bose. H
Philippe Edouard PouUetier de 1
TemeiiU. ■
Hugo von Mohl.
■
Change of Name and Title. ^|
SirEobertAJeianderShafto Adair to Lord Waveney. H
The Hon. John William Strutt to Lord Kayleigh. H
Fellows elected since the last Annirereary. ^
The Eight Hon. Hugh Culhng
Eardley Child^-re.
William Aitken, M.D.
Li(3ut.-Col. J. Augustus Grant,
C.B., C,S.J.
Clements Eobert Markham, C.B.
Sir AJeiauder Armstrong, M.D.,
K.C.B.
Eobert Stuwell Ball, LL.D.
George Edward Paget, M.D.
George West Eoyatoa-Pigott, M.D,
Osbert Sal™, M.A.
John Beddoe, M.D.
The Hon. John AVilliam Strutt,
Frederick Joseph Bramwell, CJB.
Captain Edward Killwick Calver,
E.N.
Eobert Lewis John EUerj-.F.S. A.8.
M.A.
Henry Woodward, F.G.3.
James Toutig, F.C.S.
On the Foreign List.
Yninz Gustav Jakob Henle.
Charles Hermite.
Otto Wilbelm Struve.
Baron Jean Baptiat« Julien
D'OmaliuB d'Halloy.
Qeorg Adolph Erman.
Asa Gray.
The President then addressed the Society as follows ; —
Gehtleukr,
Wx meet, at length, in Apartments to the occupation ot which we have
long looked forward, and in which we hope to find scientific, literary, and
social accommodation superior to that which we have hitherto enjoyed.
And I trust that we may consider ourselves established here with a
degree of pennaiiency at least comparable to those which the Society ex-
perienced in Crtuie Court and in Somerset House. In congratulating the
Society on this important step of localization, I would express my hope
that our continoed westerly movement will not be misinterpreted.
Much of the practical vigour of the Society has always depended on the
action of Fellows engaged in the transoctionB of busy life; and our
movement from Somerset House, and in a eertnin degree from the
regions frequented or inhabited by those able men, will I trust be
■scribed to its proper cause — the difRculty of finding a suitable place in
1878.] PraUknfs Addraa. 3
those parte cS this great atj m which conimerce or manufacture is moat
active, or in which the demauds of the State are most imperative.
Our Foreign Secretary, Frofessor W. H. MiUer, has intimated to the
Council hie wish to withdraw from the duties and the labours of the
office which he has held for many years with advantage to the Society,
and for which he is eminently adapted. In offering to Professor Miller
your thanks for his long-continued services, I have to add my confidence
that the office will be well sustained by the gentleman whom the Council
submit for yonr election.
It has not be^i usual for your Presidents to allude by name to those
of your Ordinary Members whose decease the Society has had to lament
during the year last elaped. But I hope that an intimate friendship of
more than fifty years Vdll justify me, in your opinion, in alluding to one,
the only Copley Medallist in our British List lost in the last year, the
late Professor Sedgwick. I cannot sufficiently express my veneration
for the unselfishness, the love of truth, the kindliness of heart, which
^tinguished that extraordinary man ; and I cannot conceal the expres-
sion of my admiration of his general ability, and my strong ccmfidence in
the soundness of his judgment on controverted points which might come
before him. After this notice, I am bound to allude briefly to others
whose names will appear in our ofBcial Obituary. Confining my re-
marks to those who have furnished papers to our ' Transaotions,' there
are : — the Bev. G-. Fisher, first known by magnetic observations in an Arctic
Expedition, and afterwards by ids instructions to our Naval Service ;
Sir Henry Holland, the senior Fellow of the Society, equally distin-
guished by his reputation in the Medical profession, by his fame as a
traveller, by his literary records of political and personal life, and by the
mixture of science and sociality which endeared him to all who knew
him. I>r. H. Bence Jones will be remembered for his labours in
reference to urinary chemistry, — W. J. M. Bankine for his mathematical
labours in problems of engineering and in the motions of fluids, — Sir F.
Bonalds for his knowledge of electricity, his introduction (collaterally
with others) of photc^raphic self-registraticm, and his attempts at esta-
blishing a telegraph not by galvanism but by electricity, — and A. Smith,
a Boyal Medallist, for his general mathematical acumen, and for the
Application of it to the theory of the induced magnetism of iron ships.
Bat nothing prevents me from alluding to the losses among our
Fordgn Members. The Baron Liebig, a Copley Medallist, was the
founder of a branch of chemical science, not entirely new, but carried
out by him to an extent and perfection that have given it importance
which we could hardly have expected it to attain. Frofessor Hansteen
personally observed terrestrial magnetism over a great extent of country,
and was I believe the first person in modem times who endeavoured to
combine all the magnetical observations in different parts of the earth
i^ available, his own attempt to explain them being founded on an
4 Annivcrsarif Meetiny. [Dec. 1
assumption as to the action of two great nutgneta. Od llie merit* fl
Von Mohl, Ease, and Poulletier de Verneuil information will be %
by Officers oE the Societj', who can speak with greater accuracy than |
coald assume for my own st-atementa.
The Council of the Sodety, and its various Committees (for dispoi
ot the Government Grant, for the Library, for management of 1
Donation Fund, and of that appropriated to Scientific Belief), have b
working with their usual octinty. The principal grant recommendc
by the Govemment^Grsnt Committee, and sanctioned by the Coonoi
was for the construction ot a Siderostat, an instrument freqnently d
aired, but of which the expense is too great to be borne by an individi
It is believed, however, that the cost may now be materially reduced.
In my Eeport of last year I alluded to tlie Catalogue of ScieatiGc Fape
completed to 1863, and in progress to lS7!t ; perhaps the following eia-
gular instance of its value may be interesting to the Society. In settling
an international boundary, some years ago, reference was made to certais
astronomical determinations. The Government of the present day, on
taking steps for aacertiuuing the boundary so d&Bned, were unable to
discover the official report of the aslronouiical observations. On the
application of the Govemmeiit to me. I Ciircfiilly exuiiiincd (he pripers of '^
the Itoyal Observatory and those of \\v lioimJ t.f Loiigitudf ; but the M
Beport was not found. I then requested our Assistant Secretary, Ur.
White, to examine the papers v& the Boyal Society ; he was eqaaQy mi-
successful. It occurred, however, to Mr, White to refer to the CKtalogoft ot
Scientific Papers for the published works of the astronomer who vaa known
to have conducted the observatioiis in question ; and there he discorered
the desired Beport, published under circumstances of solemn aathenliiri^
in a foreign periodical. It is not improbable that the pecnniai; valne
of this discovery may have many times exceeded the whole e^qmue <tf
forming the Catalogue.
The Council have not been engaged during the past year in any coy
respondence with our own Government or with Foreign Bodice ; thejr
have, however, at the request of the President and Counol of tlie Boyal
Geographical Society, appointed a Committee to confer with a Com-
mittee of that Sodety, on the best methods of utilising for FhyaLoal
Sdence any future Arctic Ezpediticm. But the Council hare not taken
any step in urging the proposal of such an Expedition on the attention dt
Her Majesty's Government,
The Official ScientUlc Commission, of which your Home Secntanea
and other Fellows of the Society are Members, have issued an imporfaai
Bqtort on the means of making our great ITniversitieB more available ivt
the conduct of sdentific investigation. Other proposals have been paV
lished, by independent Fellows of the Society, for universal inBtmcticnt
leading to physical investigation, and for the establishment of physiea
■ervatoriei,
1878.] PresidetU'f Addreu. 5
In speaking of the scientiSc subjects which have occupied the Ordinary
Meetings of the Society, or which hare been intended for pubKcation in
its ' Transactions' or its ' Proceedings,' I may perhaps notice indiriduBUy
the following : —
In Astronomy, we h»Te commnnicationa from Messrs. Lockyer, 8ea^
broke, and Hoggins, on viewing the solar chromosphere and promiuences.
And we have the elaborate paper of the Earl of Bosse on the heat
radiated from the Moou, with all the modifications depeading on the
lunar phases and on the absorption produced by our atmosphere at
differ^it elevations of the moon.
In Oceanic Science, Mr. Wells has communicated observations on
the temperature of tlie sea between Greenland and Spitzbergen, esta-
blishing the onezpected fact that the water an the Spitsbergen coast is
considerably warmer than that on the Greenland coast ; and Commander
Wharton has ascertained with certainty that the outwards current of
the superficial waters from the Black Sea through the Bosphorus and
the Dardanelles is accompanied by an inwards current of the deeper
waters.
In Biology, we hare experiments and remarks by Dr. Bastian and
Messra. Bay and Lankester on the development of life in organic infu-
sions, bearing partly on the disputed subject of spontaneous generation ;
and wB have also a paper by Dr. Ward Bichardaon " On Muscular
Irritability after Systemic Death," with other medical and physiological
In Palnontology, Professor W. C. Williamson has continued his exa-
minations of the Btructure of fossil plants iu the Coal-meaeuree ; and
Professor Owen has extended Ma description of the Fossil Mammals of
Australia to those which may properly be referred to the same family as
the Kangaroos,
In Botany, the more complex forms of leaf-arrangement around the
parent stalk have been referred to the primary form of leaves arranged in
two opposite ranks, by mecfawiical considerations of a simple character.
In Chemistry we have numerous analyses and experiments, but, I
beliere, no establishment of new general principles.
In Optica, Meears. Steam and Lee have described the effects of pressure
on gaaea, iu altering the character of their spectra.
In Magnetism I beUere that the only memoir ia one describing the
internal magnetic influence of the largest iron tubes in existence, namely
the great tubular bridges of Bangor and Conway.
In Mechanics there is much information by Sir W. Fairbaim on the
durability of iron ships, and on the strength of riveted joints ; and, in
combination of meteorological facts with mechanical invention, Mr. F.
GiCtoD has planned a machine for indicating the best course for a ship.
I scarcely need to remark that a limited list of communications, like
that which time permits me now to offer, must be very incomplete.
The present appears, howgii, to ta ■ pwp* off^ai^iaitj iar tofUfag ''
the fttteDtkm of the Society to ft* jiiiyuM ol SahiMei^ oi 111* mm» «bn
u those which it apeciaUj kdo^ lor tiM iolijett of Hi own UwBi, M
the external world.
Commendng with ABtronoa^ii — Vl b -ntj gaUyli^ to QmfMlaBil
Astronomers to learn that ULLeVwiivlHB oDKBunkitod to tiuTMnA
Acadjmiedes Sciences (I bebm jk ««mss) Ua tbooriM of Japiterna
Satinrn.— InCVmetaT^Aatronoii^ithaaoitatrikfaigiMtialienM^setod
metocH^hower which oocnnvd'OB TfiiiWhlNii Wt, 187% FniliOB
EJinkerfues telegraphed the npoct dt ttia Aomr mA Vm w^j/aimA
course to Mr. FogBon at Madna ; id Mr. Joffnn, gwolfaiglik filMimn
in that line, discovered a oomat iwiadiiig from flw tBth, iad (lyf
rentl^ beyond doubt) the iu|in]amlaliiii of tba mUma Jaiiwf. IIW
course of this comet is so near to ttat of ttia lost Biolah omat •• to
make it probable that it is itaDf tta namti Tfr "Baggnt aone 4faaft .
since found, from Bpectrooeopio obagmtiaoa, InMss of cvboa 1b tt*
composition of comets; this has been v«rifad bf HcR-Togel and Mr.
Flummer in obserrationB of ocMMts in di6 present jear.^ — ^Dr. HaggbM
has employed the telescope sap^pSed-lir flns Society in iiiiliiHiiiwui avna
nebnls for discovery of motion or change, and in obeerrations of their
spectra, with the view of ascertaining theb apparent motion to or from
our system ; and facility has been given to this research by the proxi-
miiy of a spectral line of the nebolra to a line in the lead-spectrum:
the results have not indicated any discoTerable motion. — Father Secchi
has remarked the sudden appearance of a brilliant pmnt in the son,
which gave reversion of spectral lines, indicating ignition, with such
a distortion of a line as appears to show that the igneous matter ap-
proached us ; that is, that there was explosion. — On the constitution of
the sun there baa been much controversy. — The Transit of Venus
December 8th, 1874, has engaged much attention. The Bnssian Go-
vernment is preparing to equip twenty-seven stations, all on land;
The American Government proposes to establish three stations in the
north and four or five in the sontb. The British original scheme of five
stations has been extended, contingently, to eight : — two being r^arded
as subordinate to Honolulu, for strengthening that important stetion ;
and one, at Heard Island (if information expected from ^e ' Challenger*
shall report it practicable), or at a second point of Serguelen's Island,
for strengthening that of Christmas Harbour. The French Government
has proposed to establish five statums, and the German Government four.
Some of our colonies and cobnial observatories are taking up the matter
with intereat. It is understood that Lord Lindsay is preparing a well-
equipped private expedition to the Mauritius. For ocular observation,
the largest telescopes ore about 6 inches aperture ; with some <A these,
double-image measures of cusps, Ac. are proposed, either by belio-
meter, or by an eyepiece arranged by me many years ago. For photo—
1873.] PrenderWi Addrett. 7
graphic records, some will employ Mr. Do Ln Bae's photoheliognph ;
some wiU endeavoor to arm it with M. Jsnsaen's arrangement for taking
numerous pictares of Venus at small intervals ; some prefer a horizontal
telescope 40 feet in length, into which the sun's rays will be ^irown by ft
large plane mirror moved by a helioatat, and by which the primary
image of the sun will be photographed. A working model of the Transit
has been established at the Boyal Obserratory, by means of vrfiich the
wngnlar optical phenomena are well seen. My own estimate, and that
of my ezperienrod friends, on the amount of uncertunty, reduces it
low ; but I believe that my younger observers are not so successful. —
QennaD astronomers have proposed to make use of observations of the
Minor Planets (Flora in the present year) for measuring the Solar
Parallax ; but I conceive that Mars in 1877 will be very far superior. —
The publication of the Eclipses of 1870 and 1871 is still delayed, mainly
by troubles with engravers.— -I am happy to state that, at tha instance of
the Smithsonian Institution, and by the liberality of the Anglo-American
Company (who have declined all commercial remuneration), telegraphic
announcements of astronomical discoveries are now made direct from the
United States to Europe, and vux vend.
In Geodesy and related subjects an important repetition of Caven-
dish's experiment has been made by MM. Comu and Bailie, using, for
the attracting material, hoUow spheres filled with mercury, which was
tnnsfeiTed &om one sphere to the other; the mean density of the
earth thus obtained is 5-66. — It is proposed in France, to repeat the
obserrationB fortbe great arc of meridian. — Allusion was made in the
last two Addresses to the interruption of the TnitiaTi pendulum-observa-
tions by the death of Captain Basevi ; the pendulums (two the property
of this Society, and two belonging to the Bussian Government) have
been brought to this conntry ; and observationa of them have been made
at Eew Observatory by Captain Heaviside. It is proposed, I believe, to
combine with these observations a re-observation of Hater's double-
knife-edge pendulum.
Ge(^;raphical research has been very active. — The ' Challenger,' after
three times crossing the Atlantic, was last reported at Bahia. One result
of her operations is the establishment cS a general uniformity of depth,
averaging perhaps 2300 fathoms. A second is, the ascertaining of the
temperature at different depths ; in some places in low latitudes the
deep-sea temperature is lower than in high latitudes. A third is, the
dredging up of Crustacea of new forma. A fourth is, the ascertaining
the character of the soft bottom of the Atlantic: this will probably
require the examination of the geologist. — Dredgings made unong the
banks of the New-England coast by Mr. TerriU have given results very
similar to those of Dr. Carpenter. — The Congo expedition, fitted out, I
believe, by Mr. Young, and organised by the Boyal Geographical Society,
*aa last heard of at some distance up the counti7, at a point on the
8 Anniversary Meeting. [Dec. 1,
river which was gained, not bj passage from its mouth, but by crossing
from another landing-place. — Of the precise discoveries by Sir Samuisl
Baker, and the last year's movements of Dr. Livingstone, little seems to
be known. — Political circumstances have stimulated much research in
Central Asia. — But the interest of all these sinks before that of the
Arctic explorers. In the instance of the American ship ' Polaris,' nine-
teen men, women, and children, fortunately furnished with provisions,
lived upon an icefloe (hopelessly separated from the ship in latitude
80° 2') through the darkness of Arctic winter, drifting down Smith's
Sound and Baflin's Bay, from October 15, 1872, to April 1, 1873,
then betook themselves to a boat, and were rescued by the ' Tigress ' on
April 30, in sight of the coast of Labrador. Subsequently, eleven of
the crew who had been left in the ship, then beset in the ice, built boats
for themselves, and were picked up by the whaler * Bavenscraig,' were
transferred to the ' Arctic,' and were safely carried home. Some addi-
tions were made to our knowledge of the regions north of Smith's
Sound. — ^And another Swedish expedition, in the Polheen and Oladan,
under the direction of Professor Nordenskiold, fast locked in a bay near
^ the northern extremity of Spitzbergen, was rescued by the ' Diana.' I
must avow that the fortunate termination of these two enterprises does
not in any degree blind me to the dangers of Arctic exploration in
general.
Li Geology, while the usual activity has been shown in collecting
details, and the usual accuracy in discussing them, I am not aware of
the introduction of any new principle, except in the theory proposed by
Professor Dana, explaining the elevation of mountain-ground and con-
tinents generally by the forced contraction which must have taken place
in the crust of the earth in consequence of the cooling of the interior.
Ldl the maritime part of the publications of the Meteorological Office,
an addition to the ten-degree square mentioned last year, applying to the
regions adjacent to that square, is now in the press. Sir James £oss*s
observations south of the latitude 60° S., made in the expedition
1840-1843, have been published in an orderly form. As regards local
meteorology, a new and valuable station has been established at Stor-
noway ; the daily results of all stations are communicated, and proper
warnings given, to 129 places on the British coasts, and (at the request
of the French Government) to various ports from Dunkirk to Nantes.
In 1872, eighty per cent, of these warnings were successful. The daily
charts (first introduced by M. Le Yerrier, but now issued on a highly
extended plan by the Meteorological Office) are circulated among a large
list of subscribers. I think that comparison of the records of the various
atmospheric elements upon these charts, continued from day to day,
would be more likely than any thing yet published to throw light upon
the difficult question of causes and effects in Meteorology. — Dr. Daniel
Draper has traced the courses of rectilinear waves of cold and of storm
1878.] Praidenfs Address. 0
■CTOBS the United States. He haa alao shown that wind-atorms are
propagated from the shores of the ITnited States to the shores of Britain ;
and in eighty-six predictiona of storms to occur on the British coasts,
only three vere failures. — At the Boyal Observatory, Greenwich, a
laborious discussion of the photographic meteorological records 1848-1868
ia now far advanced.
In Anatomy, the most strilung subject appears to be Profeasor Femer's
experimental discussion of the actions of different parts of the brain,
explained at the late Meeting of the British Association.
In Natural History, much has been added to our knowledge of tnrda
by the works of Buller on New Zealand, Tiscount Walden on Celebes,
and the termination of Gould's labours on Great Britain. — Murie, Owen,
and Newton have done much on special points in Comparative Ana^
tomy. — It seems probable that considerable knowledge of the habits of
fishes may be gained from the large Aquaria lately established.
Paleontology has made considerable advances. The most important
publications are the following; — With the assistance of the Imperial
Academy of Bt. Petersburg, Professor Von Brandt has given the results
of a long series of researches on the fossil Cetacea of Europe, a work
almost forming a supplement to Cuvier's ' Ossemens Fossiles.' Aided
by the Public Museum of Buenos Ajres, Dr. Burmeister has almost com-
pletely restored the extinct epedes originally indicated by the names
Toxodon, Qlyptodon, Maorauchenia. Professor Owen, in the ' Zoological
Transactions,' has continued his restonttion of the extinct Birds of New
Zealand, and appears to have discovered evidence of the former existence
of a wingless bird of great size. The principal advances in fossil Botany
are those by Professor Williamson, already mentioned.
Medidne, in ite practical character and on the broad scale, has raised,
but has not always solved, questions of great importance. We are not
yet able to assert that contagious diseases can or cannot commence with-
ont antecedent contagion ; but the oi^anisation for tracing the course of
cont^ion is much improved, and may enable us ultimately to answer
this question. — The subject of " Nerve Storms " bos been well discussed.
— The use of self-recording instruments, and the application of the ther-
mometer, have given information which haa led to improved treatment ;
the spectroscope promises to be useful in medical jurisprudence. —
Surgery, as I understand, has been made milder than formerly ; mort^d
fluids are more easily extracted ; large ulcers are healed hy placing
healthy skin upon them ; medicines are sometimes injected into the skin ;
and there is general activity in the examination of surgical methods.
The advances of sdeutiiic Botany have been principally in the follow-
ing directions : — Dr. Hooker and Mr. Bentham continue their Catalogue
of the Genera of all known flowering plants ; Mr. Bentham has also ad-
vanced with his publication on the Australian Flora. Discussions have
arisen on the question whether Lichens are or are not parasites of a
simpler form of Alga. MbA aMullHB kw baa* gim ft» tli« AhMtm^
snd to thedr aappoaed agemy fa jWwhiBtig jntrAMau. Th»Atd»«l
reproduction of Fungi has bMS a Mibjeet «C canfaaliaB md qpewl^-
tion. The curiouB fsct appe«n tobe iaowtebsd ttat movaBtent cC (be
le^ of the Dionaa muidpuia pradaoM doetajfri j*^ ~TTIH> ■MJogBBl ts
those in the movement of musde.
In Chemistry, though a gwt nmatar «C wlyaw Ae. bftve been
made, I do not learn that ai^ alep ei lyBtMB of fmAnMoM sdenas kw
been taken, except in the drakti aqiiBMui whttho! th» gmtaHee of four
isomeric lactic acida, ftpparen^ demonsteatod by TTiiTinniirii, em be
made conaieteDt with the prenat liieoiy o( otgaaie dieBditcj.
In the sdence of Optica a amr AeA&niaaitiaa cf tlw TCkritf of Hg^
has been made by M. Coma, nriiig ttte meHiod of tmmnsaian of a nqr
of Hght first directly, and tlun bf itAeetion, betwoan A» tttA of •
rotating wheel. The velocity thw taaoA m mqmo is £98,506 ldl»-
metrea per aeoond of mean solar tioM. — M. Qidncke, in aqmimenbi on
diffraction, has shown that litere b fnquBntlj' tn oBtacpmAti aooont-
psniment of polarisation.
The practical edence of QabiBiio Telsgrapliy nsdcrgpei ""^^W bo-
prorement, especially in the power of inmsmitting namerons words in a
short time, and in the arrangement of sympathetic clocka. — But the
pdnt to which I would more particularly call attention is, that the prac-
tacatnlity of duplex telegraphy by simultaneous currents in opposite
directions appears to be established, at least in mimy circum stances. If
they are accurately simultaneous, the conclusion (previously entertained
by theorists) appears to be inevitable that the so-called correata are
waves.
M. D'Abbadie'a Magnetic Survey of Abyaainia and Brazil, made sever^
years past, has lately been published.
I have now to announce the awud of the Medals.
The Cf^ley Medal has been awarded by the Council to Frofesaor Her-
mann Ludwig Ferdinand Helmholtz, M.D., For. Memh. B.9. It would be
difficult for me, within the limits of this Address, to state the number and
the importance of the claims of Profeasor Hetmhottz; to our recognition.
H's published books on the Conservation of Energy and the Theory of
Music, and his ' Handbook on Physiological Optics,' have asdeted greatly
in the prepress of their respective sdencea. Hie memoirs have ranged
throogh nervous phyaiolt^, hydrodynamical theory, instruments (aa the
ophthalmometer and the ophthalmoacope) for exact measurement and for
medical examination of the eye, and other important subjects, and have
been generally recognized as giving real additions to our knowlet^.
PnOTiaSOK MlLLBB,
As representing the Council of the Boyal Society, I request that you
1878.] Pretidenfi Addren. 11
will place ^t our most honourable Medal in the band§ of Profeaior
Helmholts, and assure him that we appreciate very highly the serricea
which he haa rendered to Tariou« branches of science.
A Bojral Medal has been awarded to Professor Allman, F.B.9., for his
numerous soological investigations, and more especially for bis work
upcm the Tubularian Hydroida. The subject of these labours is one
upon which few persons are qualified to enter; and the Council are im-
presaed with the deUcacy of the work and the value of the scientifie
reeulta.
PRonaaos Alluak,
In the name of the Council of the Hoyal Society, I present you with
this Medal, in token of their appreciation of your valuable services to
Zoology.
A Boyal Medal has been awarded to Professor Henry Enfield Boscoe,
FJE.S., for his various Chemical Besearches, more especially for his in-
veatigationa of the Chemical Action of Light, and of the Combinations
of Vanadium.
pBonssoE BosooB,
I have much pleasure, as the organ of the Council of the Royal
Society, in presenting you with this Medal, in testimony of the value
which the Council attach to your various Chemical researches.
And now, gentlemen, I have to make an announcement which I could
wish I had been able to defer for some years. I must ask you to accept
my resignation of the office of President. I do this with great regret, for
more than one reason. I scarcely need to say that I received with great
pride your honourable call to that office, and that I should have valued even
more highly a series of repetitions of the expression of your confidence.
It is matter of much grief to me, personally, that I feel myself com-
pelted to abandon this gratification ; but I am more grieved because I
feel that the Presidential office haa not been properly sustuned, and that
% continuance of tenure by me might permanently endanger ite efficiency.
The primary causes of this failure are : — the severity of official duties,
which seem to increase, while vigour to discharge them does not increase ;
and the distance of my residence. It haa resulted from these causes
that I have been unable to attend Ooundl and Committee Meetings and
Meetings of the Society, and Trust Meetings connected with the Presi-
dency, so fully as I could have wished — that I have been unable to establish
that personal acquaintance with my colleagues which 1 hold to be almost
essential for the good conduct of a Society — and that I could not hope to
cany out any measure beyond the merest routine. The difficulties which
12 Annivertary Meeting. [Dec, 1,
I hftve mentioned m^t hare been met in Home degree by properly arranged
expenditore, if ench had been legitimately in my power \ but another
cause now comes on wbich I fear cannot ho met, a difBculty of hearing,
which iinfita me for effective action as Chairman of Council.
I reapect 3ie aentinieiit which has prompted the Society to seek for
its President a maa lA. supposed scientific character, and, perhaps in pre-
Eatence, a man in offidal scientific position ; aud I join in the unanimous
feeling of the Council that, this principle being admitted, its application
could never have been better made than in the selection of the Fellow
whom tiiey recommend to you as successor to myself. But I still think
that, practicaUf viewed, the principle is not the best that con be adopted —
and that considerations on the leisure which the President can devote
to the concerns of the yocioty, on the proiiinity which enables him at
any moment to enter into its bmiiwM, and oB Aa pvaonal ngoor <ridek
he may be expected to bring into all bu bmiBMtioaa with Vt, ob^ to
bold a very important place.
But, in retiring from tbe FnaidBn<7,iiid •gmttaa^ bam tteOoonetl,
I do not, gentlemen, retire from As Bodotf . Tben an oAer femHaOM
iu which I may hope to reodw tamob, I hno tn^Mrify been »-
quested by the Council to repnt xtpaa the chander of papers oonunani-
cated to them ; and in this capacity my power of meeting the wishes of
t&e governing body is undiminished. Perhaps other occasions will arise
in which I can continue to prove my devotion to the intereste of the
Society.
On the motion of Sir Thomas Watson, seconded by Mr. J. M. Amott, it
was resolved, — " That the thanks of the Society be returned to the Presi-
dent for his Address, and that he be requested to allow it to be printed."
The Statutes relating to the election of the Coundl and Officers having
been read, and Mr. David Forbes and Mr. Savory having been, with
the consent of the Society, nominated Scrutators, the votes of the Fellows
present were collected, and the following were decluvd duly elected as
Council and Officers for the ensuing year : —
Prmdmt. — Joseph Dalton Hooker, O.B., M.D., D.C.L., LL.D.
Treiuurtr. — William Spottiswoode, M.A., LL.D.
S*fl«(ari«— f ^^*- <=^«««B Gabriel Stokes, M.A., D.C.L., LL.D.
ateraana. | ^^^ Thomas Henry Huiley, LL J).
Foreign Secretary. — Prof. Alexander William Williamson, Ph.D.
O&er Men^>ert of the Cbunetl.— Sir George Biddell Airy, K.C.B., M.A. :
Sir B. C. Brodie, Bart., MA., D.C.L. ; Professor Arthur Caylev, LL.D. ;
John Evans, Sec. G.8., F.8.A. ; Daniel Hanbury, Treas. L.8. ; NevU
Story Maskelyne, M.A. ; Prof. James Clerk Maxwell, M.A. ; C. Wat^
kins Merrifield, Hon. Sec.LN.A.; Joseph Prestwich.V.P.Q.S.; Andrew
1878.] Number of Fellows. 13
Cromtne Ttajsuny, LLJ). ; Bear-Admiral Q. H. Bichuds, C.B. ; Prof.
Geo^e Bolleeton, M.D., MA. ; Prof. J. 8. Burdon Saadersoa, M J>. ;
William Sbarper, M.D., LL.D.; I>aiids Sibson, MJ).; Majoi^Oen.
B. Strachey, B Ji., C.S J.
The thanks of the Society were given to tiie Scmtators.
The following Table shows the progreaa and present state of the Society
with respect to the nomber of Fellows : —
Falran
and
Porfjn,
Ctom-
X4
IMaL
NoTember 30, 1872.
Since elected
Since decesied ....
4
48
- 6
278
+ 4
- 18
267
+ 12
- 11
687
+ 18
- 32
December 1, 1873.
i
43
266
268
671
Financial Statement.
[Dec. 1,
11^-
l3|
2|fl
*o3 i 9 I Si - .
ilNillfi
H ■ ■
Mm
ii
S" A't iS ..I .^1
Id4s.i;|.|
■i% ggssaas
1878.]
Financial Statement.
Hggga
51?
I".
j|S§s| 2 asESssss"
ill
I
iIiiISjji 11 r
00
»5o
00
• : :
5 s
: :
1878.]
1^
1^
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1873.] A^^ropnaUoniif the Oitveriment Grant.
Account of the apjnropriation of the sum of £1000 annually voted
by Parliament to the Royal Society (the Govemment Grant),
to be employed in uding the advancement of Science (con-
tinued from Vol. XXI. p. 85) .
1873.
1. Dr. Steohooae, for ccmtinustion of BesearcheB on the Orcins
and Varietifia of Tannins ;C100
2. W. Galloway, for Experiments bearing on the Causes of
Colliery EzplosionB 75
3. W. N. Hartley, for BeeearcheB on the effect of Heat on
Absorptdon Spectra 50
4. Dr. Klein, for Besearchea on the Lymphatic System of the
Highw Anlnnajff 100
6. J. Dewar and W. Dittmar, for Experiments on Vapoor Den-
sities at High Tempetatm«fl 50
6. A. Dupr^, for investigating the Specific Heat of MiitureB
and of Elements in the Xascent State 50
7. 'W.LaBBeU(asTrea8ureroftheEclipBe(1870)Committ«e),tor
a Spectroscope for the Eclipse Expedition ^17 10<.
8. Bev. Canon Selwyn, for continuation of bis Series of Solar
Aatographs 50
9. Dr. Frankland, Beaearches on Oigano-Boron Compounds,
and on tJie Synthesis of Organic Adds 100
10. 3. N. Lockyer, for procuring a Siderostat, to be employed
in photographing in detul the Spectroscopic Phenomena observed
m ae Solajr Disk 300
11. Sogers Field, for continuation of Experiments to determine
tite Amount of Evaporation from a Water-eurface 100
12. Prof. B. Stewart, for investigatiiig a possible connexioQ be-
tween t^e Meteorology of our Earth and the Positions of the
nearer Planetary Bodies 100
13. P. Galton, for the construction of an Instrument for com-
puting the mean Distance which a ship could sail in one day, &c . . 25
14. W. C. WiUiamson, for continuation of Besearchea int« the
Orgamcation of the Fossil Plants of the Coal-measures 25
15. Prof. P. Q. Tait, for a research on the Thermoelectric Pn>-
peitiM of Metals and Alloys 75
Cheque Book 0 10».
^1218
Report of the Kttv Commitiee.
Dr.
£ ». d.
To balance on hand,
Nov.23,1872.... 1140 0 1
To Grant from Trea-
sury (1873) 1000 0 0
BepaymentB : —
Capt. M. HaU 50 0 0
Sale of surplus copies
of "Hydnwoa" ,. 40 10 0
Interest 35 8 8
^2265 18 9
Or,
£ g. d.
By appropriattoDB as
above 1218 0 0
Balance on hand, Nov.
23, 1873 in47 18 9
Report of the Kew Commitfee for the Year eriding
October 31, 1873.
The ohlj cluuige of cOTueqaence Meeting the management of the
ObBerratoiy during the year has been caused by the resignation by
Mr. Spotliswoode of hia seat on the Committee. The vacancy thus occa-
eicaied has been filled up by the appointment of Major-Oen. Strachey,
while the Earl of Boese has been nominated as an additional member of
the Committee.
Magmtit Worh. — The series of automatic records of the several Mag-
netographs, viz. Declinometer, Horizontal-Force, and Vertical-Force instm-
ments, have been continued, and the independent absolute determinations
have been, as usua], made monthly. This latter duty has been, as hereto-
fore, performed by Mr. G. M. "Wliipple, B.Sc, First Assistant, who also
takes charge of the General Magnetic Work, In which he has the assist-
ance of Mr. Cullum. The salaries of these two gentlemen, whose time
la chiefly devoted to magnetic work, amounted during the period nnder
consideration to ^249 12«.6d., leaving a balance of about ^£350 out of the
sum of ^608 0(. 7d. received &om the Boyal Society to meet ^e general
expenses {X1979 10«. 7d.) of the Observatory. ^673 4*. 5d. of this
amount has been defrayed by the Meteorological Office ; and ^613 Oi. Id.
has been obtained from other sources, such as fees for verification of
instruments, and payments for new instruments for foreign observatories,
'eaving a balance in hand of £522 3s. lei. on the 3Ist of October.
Report of the Ktv> Committee. 21
Od the 2nd of December tbe suspeiiaioii'thiead of the Declinometer
gave vty and wbs replaced hj a new one.
Arrangements have been made to dismount the Magnetograph uutru-
mentfl in tba coarse of the enauing year, on the occasion of paintiiig
the basement story, in order to have them thoroughljr examined and
readjusted — a step which has become necessary, as their condnuous action
has not been interrupted for 15 years.
As r^ards the Magnetic Beductions, the TabulationB of Declination
have been continued to the ^id of 1872 ; and copies of the results have
been Latrusted, for discussion, to the two Sei^eants of the Boyal Artillery
who are located at Kew, as explained in the lastBeport. Msignetic daU
have been supplied to Prof. Balfour Stewart, FJE.S., Owens Coll.,
Manchester, Prof. Atkinson, B. Mil. CoU., Sandhurst, Mr. W. Gee,
Gheetham Hill, Manchester, Mr. H. Proctor, N. Shields, Mr. Beid, and
to Dr. Stein of Frankfort.
The stock of forms having become exhausted, care has been taken in
ordering a fresh supply to procure a quantity sufficient to meet possible
requisitionB from other observatories.
A Unifilar and Dip-circle, formerly in store at the Observatory, have been
repaired and set to rights, preparatory to their being lent to the Vev.
8. J. Perry for use on the expedition to observe the Transit of Venus.
MeltorologiaU Work, — The several self-recording instruments, roister-
ing respectively the Pressure, Temperature, Vapour-teDsion, Bainfall, and
Wind, have been nuuntained in constant action ondOT the superintendence
t^ Mr. T. W. Baker, Second Assistant, aided by Mr. Tig^ ; and the daily
standard eye-observations for control of the photographic records have
been made regularly.
The instmment^ txaces with hourly tabulated values are sent monthly
tothe Meteorological Office as in former years. TheBarograms and Ther-
mograms are printed off in duplicate, and one copy is preserved at Kew.
As regards the Anemogntms and Bain-records, the copy has been ob-
tained by the method of tracing.
In addition to the r^ular work of Kew as a Magnetical sod Meteoro-
logical Observatory, the duty of examining and checking the work of all
the seven Self-recording Observatories in connexion with the Met«oro-
logical Office has been carried on, in accordance wit^ the method described
in the Beport of the British Association for 1869. This portion of the
work has been performed by Messrs. Bigby and Foster.
A series of experiments are being carried on at the expense of the
Meteorological Committee, at the Pagoda in Kew Gardens, to teat the
influence of height above the ground on temperature. The thermometers
are placed at three different levels, viz. 22 feet 6 inches, 69 feet, and
128 feet 10 inches above the ground.
Copies of Meteorological data have been supplied to Mr. Q. J. Syinons
and the Beraretary of the Institute of Wining Engineers.
is Report of the Keto Committee.
Pholofi^iogrt^h, — As soon oa the experiineiita with this instrmnent
mentioned in livst Rpport were completed it was taken down, and, on
application from the ABtronomer Bojal, intmsted tc h\ja for nee at
Greenwich, in taking sun-pictures pending tlie return of the new instru-
ments to be used in observing the Traneit of Venus, The scale of equal
part*, erected on tho Pagoda in Kew Gardens, in order to teat the optical
distortion (if any) of the Kew Photoheliograph, has been taken down
by the direction of M!r. De La Bne, and any elight damage done to the
building has been made good at the expense of that gentleman, and io
the satiafactioDi of the Oerk o£ the Works at Kew. The eoale itself has
been made oi'or to the Astronomer Boyal by Mr. De La Rue.
The thanks of tho Committee have been conveyed to II.M.'e Office o£
Works for the facilities kindly afforded for the above esperiments.
The eye-observBtious of the Bun, after the method of Hofralh Schwabe,
have been made daily by Mr, Foster, when possible, as described in the
last Eeport, in order, for the present, to maintain the continuity of the
Kew recOTd of BOn-epotB.
An additiimal series o( posUivMb ftam A* K«ir ofl^tim pktolM^
is now bdng printed by • fAotognplMr, ai ti» enpsoM d Hr. S0
La Bus.
A statement, embodying the nso^ data respecting the spots Ac. on tlie
Bun'a disk, has been, ss nsn&l, published in the 'UtmtUy Notices ci.
the Boyal ABtronomical Socdety.'
Prof. Spoerer, of Anclam, hu applied tot the measmemrats f£ eaa-
Bpots for the months of January and Febmsry 1873, during the period
vX. his ovn illness ; and Mr. Se La Bue bas kindly promised to fumirii
them as soon as their reduction has been effected.
Eleetnmteter. — This instrument, tbe property of the Meteorolo^col
Committee, which was returned for readjustment to the maker, Mr.
White, of Glasgow, in September 1872 (Beport, 1872), is stall in Ms
bands. Tbe instrument, a self-recording one, has never yet been in
working order.
Verifieationa, — This department of tbe Observatory bas been in fall
activity ; and tbe work has increased largely as regards barometers and
clinical thermometers, so that almost tbe entire time of Mr. Baker and
a junior assistant is occupied therewith.
Tbe following magnetic instruments have been veiified and constants
determined ; —
A TJnifilar for the Observatory at Manila.
„ Prof. Clifton, 'SS.S., Oxford.
„ „ Dr. E. von Bijckevorsel, of Botterdam.
And in addition : —
A Dip-drcle for the Observatory at Manila,
„ „ Dr. E. von Bijc^vorael.
1
R^mri qf the Km Committee. 2S
3 Dip-drcles for Mr. L. F. C^selhi, London.
2 Kpping-iieedlea for H.H.S. ' ChftUenger.'
An Azimuth Compaes for Mr. Ney BliAS, RB.0.8.
Detenmnatiam at the Moments of Inertia have been made of two
magnets uaed by Capt. F. J. Brans, C3., F.B.S., wben swinging iron
fihipa.
Several instroments are on hand awaiting verification. Among them
may be mentioned a Unifilaraod IHp-circle received from Frof. Stewart,
for use abroad, and a set of Magnets, for determination of their con-
BtantB, destined for the obserratoiy of Bon Iaoz at Lisbon.
At the request of the Bev. B. J. Perry, a complete set of Magneto-
graphs have been ordered for transmission to Zi-ka-wei, near Shanghai,
to the £ev. A. M. Colombel, who received instruction at Kew in the year
1868.
The meteorological iuBtrument« which have been verified are as fol-
lows : —
BarometcTB, Standards 49
„ Marine and Station 110
Aneroids 20
Thermometers, ordinary Meteorological 782
„ Boiling-point Standards 20
„ Mountain 52
Oinioal 1233
In addition, nine Kew Standard Thermometers have been calibrated
and divided at Kew, and two glass tubes have been graduated to milli-
metres.
The following tniBcellaneouH instruments have also been verified : —
Bain-gauge, 1, with graduated glass,
Bobinson's Dial-anemometer, I.
AUusion was made in the last Beport to the difficulty of testing ane-
mometers, owing to the limitation of space at disposal for the purpose.
In the course of the year a grant n-as obtained from the Govemment-
Onnt Committee for the purpose of carrying on a series of such experi-
mente ; and a piece of ground in the Park has been rented. Several
anemometers, of tbHous constnictions, have been erected therein, and
experiments are still in progress.
A Freesure-plate Anemometer, by Mr. Oxiey, of Manchester, has been
tested, but not with satisfactory results.
24 Report of the Kew Committee.
Experiments were made with a spare Barograph belonging to the
Meteorologicid Gommitteey in order to ascertain ike amount of optical
distortdon, if any, produced by the lenses.
Waxed paper for photographic purposes has been supplied to the
Meteorologiod Office (3 reams), to the India Office (1 ream), and to the
Baddiffe Observatory (i ream).
InstrueHon in the use of magnetictd or meteorological instruments has
been given to the following gentlemen : —
Dr. E. van Bijckevorsel in magnetical work.
Nav. lieut. IMxon, B.N., H.M.S. < Nassau,' in magnetictd work.
Staff Gomr. Creak, B.N., made observations with a Eox's Circle for
II.M.S. < Challenger,' and with a Fox's Circle for H.M.S. < Nassau.'
G^t. Evans, C.B., E Jt.S., made some observations with a magneto-
meter constructed after his own design.
Photographs of the portable magnetic instruments, of the most ap-
proved patterns, have been taken for the use of persons seeking in-
formation.
In the month of May a request was received from Col. J. T. Walker,
F Jt.S., Superintendent of the Great Trigonometrical Survey of India,
through the Chairman of the Committee, for provision to be made at the
Observatory for vibrating pendulums.
In the year 1865 two pendulums lent by the Eoyal Society for use in
India had been vibrated at Eew by the late Capt. Basevi ; and it was neces-
sary that these pendulums should be vibrated again on their return, and
that at the same time two pendulums obtained from the Imperial Aca-
demy of Sciences at St. Petersburg should also be vibrated.
The Committee at once complied with the request ; and at the expense
of the Indian Government preparation was made for the experiments in
the south hall on the basement story, by removing for a time the appa-
ratus for testing sextants, and building up from the foundation-arches
two solid isolated supports for the Bussian dock and pendulum.
Capt. Heaviside, B.E., the officer charged with the duty of making
the pendulum experiments, arrived in England in July, and, finding all
the arrangements satisfactory, at once commenced his experiments, which
are still in progress.
Endeavours were made, in connexion with the arrangements just
mentioned, to obtain an electrical time communication between Kew
and the Boyal Observatory at Greenwich ; but the proposal &uled of
success.
InstrumeniB. — The Kew Standard Barometer, Newman 34, has been
cleaned by Messrs. Negretti and Zambra.
In January a new Minimum Thermometer by Casella was obtained to
replace the old instrument, which had been accidentally broken.
The several pieces of Mechanical Apparatus, such as the Whitworth
Lathe and Planing Machine, procured by Grants from either the Govern-
Bepoii of the Kew Commitiet. 25
ment Grant Fimd or tlie Donataon Pond, haye been kept in thorough
order ; and many of tiiein are in constuit use at the Observatory.
A snpply of filled thermometer-tubes, of Tarioua ranges, has been pro-
cured for ultimate gradnatioa as required.
The Committee hare, through their Hon. Secretaiy Mr. Bcott, who
was present at the Meteorological Coagress at Tienna in the m<mth of
September, as one of tlie Delegates from this conntiy, professed their
readiness to graduate standard thermometers for any c& the Continental
obserratoriea which may require them, on condition that the tubes
supplied for graduation are sufficiently old.
LUtrarjf. — The usual Donations of English and Foreign Sdentafic
Publications have been received, and a few standard works purchased.
Staff. — The Staff employed at Kew is as follows : — Mr. Samuel Jeffery,
Superintendent ; Q. M. Whipple, B.Sc, First Assistant ; T. W. Baker,
Second Assistant; A. J. Sigby, J. E. Cullum, J. Foster, F. figg, E.
Constable.
NoU. — Mr. F. J, Page resigned his appointment in Januaty, and
B. BenBt«d was appcnnted as Junior Assistimt. This gentleman haa also
left, and his place has been filled by E. Constable.
In accorduice with a precedent established by the Kew Committee of
the British Association, by a Besolution passed in October 1867, Mr.
B. Loewy was employed to give instruction to the Assistants. The
present Committee, in March last, resolved to resume this practice, and
Mr. G. M. Wliipple was appointed to give a course of instructioQ in
MatbematicB ; and he commenced his Lectures in April.
Mr. Bobert H. Scott, F.B.8., continues to act as Htmorary Secretary
to the Committee.
Vinton. — ^The Observatory has been honoured during the year by the
presence of several scientific men of eminence. Among these may be
mentioned : —
Prof. E. B. Clifton, F.B.S., Oxford.
B. F. Craig, M.D., Army Medical Museum, Washington.
Prof. Felix Klein.
Dr. BadcMe.
B. Bowie Walcott, H.D., Inspector of Hospitals, Barbados.
Baron von Wrangel, Hydrographic Department for the Black-Sea
Imperial Bussian Navy.
Report o/thc Kew Committee.
II f
llll If
UP
111
35S33
lllKl
ills
31 1
III ililill III
ISS £333
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i. II
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^^11
I
I
On the Gaaema, lAqmd, and SoUd State* </ Water. 87
Deember 11, 1873.
JOSEPH DAI/rON HOOKER, C.B., President, in the Cluur.
Notice was given that at the next Meeting the Bight Hon. Edward
Oardweli would be proposed for election and immediate ballot.
The Preeideiit announced that he had appointed as Vice-Presidents : —
The Troasnrer.
Sir George Biddell Airy,
Prof. A. C. Bamsay,
Dr. Sharpey,
Major-Qeneral Strachey.
St. John Beddoe was admitted into the Society.
The following commnnitatioDs were read : —
I. " A Qnantitative Investigation of certain Relations between
the Gaseous, the Liquid, and the Solid States of Water-Snb-
stance." B; Professor Jahes Thouson, LL.D., Queen's
Collf^, Belfast. Communicated by Sir William Thomson,
LLJ)., F.B.S. Received June 20, 1873.
In two communications made by me to the Britdsh Assomtion at its
Meetings at Edinburgh in 1871, and at Brighton in 1872, and printed as
abstracts in the TransactionB of the Sections for those years, considera-
tions were adduced on relations between the gaseous, the liquid, and the
solid states of matter. The new subject of the present paper constitutes
a further development of some of those previous considerations ; and a
Inief sketch of these is necessary here as an introduction for rendering
intelligible what is to follow.
Taking into consideration any substance which we can have in ths
three states, gaseous, liquid, and solid, we may observe that, when any
two of these states are present in contact together, the pressure and
temperatore are dependent each on the otber, bo that when one is given
the other is fixed. Thsn,if we denote geometrically all possible pdntsof
temperature and pressure }(nntly by p<ant3 spread continuously in a plane
surface, each point in the plane being referred to two axes of rectangu-
lar coordinates, so that one of its ordinates sh^ represent the tempera^
ture uid the other the pressure denoted by that point, we may noface
that there will be three curves — (me expressing the relation between
temperature and pressure iot gas with liquid, another expressing that for
gsa with solid, and another expressing that for liquid with so^. These
tltree curves, it appears, must aU meet or cross each other in one point
28 Prof. J. ThoniBon on iAe [Dec. 11,
of pressure and t«mperature joiutly, which may be called the triple
point •.
The cmre between gas and liquid, which may be called the boUing-Uw,
will be a eeparatiDg boundary between the regions of the plane corre-
ipondiiig to the ordinary liquid and those corresponding to the ordinary
gaaeoua etat«. But by consideration of Dr. Andrews's experimental
resulta (Phil. Trans. 1869), we may see that this separating boundary
cornea to an end at a point of t-emperature and pressure which, in
conformity with his language, may be called the crilieal point of pressure
and temperature jointly ; and we may see that, from any liquid state
to any gaseous state, the transition may be gradually e&ect«d by an
iafinite variety of courses passing round the extreme end of the boiJing-
linet.
The accompanying figure eerrea to illustrate these considerations tu
reference to transitions between the thj'ee states, the gaseous, the liquid,
and the solid. The figure is intended only as a sketch to illustrate prin-
dples, and is not drawn according to measurements for any particular
substance, though the main features of the curves shown in it are meant
to relate in a general way to the substance of water, steam, and ice.
A. X and A T are the axes of coordinates for temperatures and prea-
■ In ""fcing this statBinEnt, that it appwi that tbe Uoob aaxm moat all eron «aah
ot^r in one point, I would wish to oUbrithere (aa I preriouily did in the 1871 Britiah-
AaaooiatioD paper) anbjeot to «ome reaem in respect of conditioiia not jet known with
peiftet elsameaa and oertaintj. I hara to suggcat that ws might not be quile aafe in
BHoming that, within a oaTi^ containing nothing but pnra wat«r-aubatanoe partlj
gaieooa, the melting temperature and prewure of ice aolidifled from the gaseooa state
wouldbe the same aa the meltinglempBratora and preaaure of ioefroien from the liqiud
atat«, and in making other nippontjons, anob m that the nme quantity of heat would
beoome Latent in the melting of equal quantitiea of ioe formed in thaw two wbjs, aad in
neglooting oonociTable but, I preeume, te jet imperfectlj known diatinotionaofoapillarj
oonditiom between ioe Bmplj wet with water and ioe only moisteDed with the laet
Tcatigci of water before the whole liquid may be either evaporated or thnen. It might
be a qoeation in like manner whrthar we eon be aom that there can be theoretioall; »
oonditioti of repcae in a oavitf containing only perfeoUj pure water-iuhataiioe in whidi
(he three state* ore preeant together, eocb in eontaot with the other two, ao that Ihwe
would be ice paiil; wet with water, and partly diy in oontaot with gaaeoua water-aub-
irionoe, or *l««m m itmaybeoalled, while the water and (team were alao in oontaot with
each other. I otTer these temarki bj way of caution, «a they force tbemselTee into
notice when we attempt to iketoh out the features of the three curves under coniidero-
tion, and because Ihey may serve to suggeet queatjon* for experimental and theoretical
investigation which may have been generally overlooked before. In the present paper,
however, I proceed on aaumptiona. sooh oa are uaually tacitly made, of identity in the
thermal and dynamio eonditioni of pure ioe lolidifled in diffbrent ways, anumptiona
whii^ BO &r aa is known, may be, and probably are, perfectly true ; and I proceed on
the suppoution that there oan be theoretically the oonditioa of repcae here alluded to,
of the solid, liquid, snd gaseous state^ prteent together each in oontaot with the other
two — and consequently that the three ourvea woold meet or orasi each other in one point,
whitdi I have aaUed the tr^/le point,
t Uention of this condition has b(«n already made in a former paper by me in the
*■— edinga of the Boyal Society,' November 16, 1871, page 2.
1873.] GaaeouM, Liquid, and Solid State* (^ Water. 29
snres respectiTelj' ; A, the origin, bung taken as the veto for pnasurea
and ai the zero for tompemturefl on the Ceatigrode scale. The curve L
represents the boiling-line termmatmg in the critical point E. The line
T M represents the line between liquid and solid. It is dmwn showing
in an exaggerated d^ree the lowering of Hhe (reesing temperature of
water by pressure, the exa^eration b^ng necessary to allow small
changes of tempeiatore to be perceptible in the diagram. The line T N
represents the line between the gaseous and the solid states of water-
substance. The line L T K appeara to have been generally (in the dis-
cussion of experimental results on tbe pressure of aqueous vapour above
and below the freeEing-point) r^arded as one continuous curve ; but it
was a part of my object in the two British-Association papers referred
to, to show that it ought to be considered two distinct curves (L T P
and N T Q) crossing each other in the triple point T.
In the second of the two British-Association papers already referred
to (the one read at the Brighton Meeting, 1872), I gave demonstrations
showing that these two curves L T and N T should meet, oa shown in
the accompanying figure, with a re-entrant angle at T, not with a salient
angle such as is exemplified in the vertex of a pconted arch, and offered
in conclusion the suggestion that the reasoning which had been adduced
might be followed up by a quantitative calculation founded on experi-
mental data, by which calculation the difference of the pressures of steam
with water and steam with ice for any given temperature very near the
triple point may be found with a very close approximation to the truth.
In the month of last October (October 1872) I explained to my
brother, Sir William Thomson, the nature of that contemplated quanti-
tative calculation : I mentioned to him the method which I had prepared
for carrying oat the intended investigation, and inquired of him for some
of the experimental data, or data already deduced l^ theory from experi-
80 Prof.j:.TfcuiMm«i<fc {Ptibll,
msatB, vhidt I was Beekiog to obtain. On his attention bdng thus
tuned to the matter, ho noticed that the draired quantitative relation
oould be obtained very direclly and easily from b simple formula which
he had giroi in hia paper on the Dynamicnl Theoiy of Hpat, Transoc-
tiom of the Boyal Society of Edinbui^h, March 17, 1851, § 21 (3), to
expreu i]» second law of thermodynamica for a body of uniform tem-
perBtore tlmnighout, exposed to pressure equal in all directions.
That £i»mala b
= CM;
^i\
in vhichp denotes the amount of the preBsnro, and -^ 't^ **** "^ ™"
creaee per unit Increase of temperature, the volume being kept constant ;
0 denotes QKuot's function ; and M denotes the rate of absorption at
irtiich beat aust be supplied to the substance per unit augmcutation
of Tolums, to let it expand without varying in temperature. The body
may be either homogoneons throughout, as a continuous solid, or liquid,
or gas ; or it may be heterogoieous, as a mass of water and aqueous
Tapour (»'. e. steam), or ice and water, or ice and aqueous vapour (i. e.
steam).
Nov apply that formnla, 1st, to steam with water, and, 2iid, to steam
with ice, the temperature of the heterogeneous body in each case being
that of t^e triple point ; or we may, for the present purpose, say 0° Centi-
grade, iriiich is almost exactly the same. It is to be observed that while
in the general application of the formula the rate of increase of the pres-
sure with increase of temperature, u>A«n tht mlunu it kept eotutant, has
been denoted by -^j yet in each of the two particular cases bow
brought under consideration, it is a matter of indifference whether the
volume be kept constant or not ; because the preesure of steam in con-
tact either with water or with ice, for any given temperature, is inde-
pendent of the volume of the whole heterogeneous body ; so that the
change of pressure for change of temperature is independent of whether
there be change of volume or not. As C is a function of the tempera-
ture which has the same value for all substances at the same temperature,
it haa the same value for the two cases now under consideration. Hence,
retaining for the first case (that, namely, of steam with water) the same
notation as before, but modifying it by the use of an accent where
distinction is neceeeary in the second case (that of steam with ice), and
thus using -^ to denote the rate of increase of the pressure per unit
increase of temperature for steam with water at the triple point (0° Cen-
tigrade nearly), and M to denote the rate of absorption at which heat
must be supplied to a body consisting of steam and water at the triple
point, per unit augmentation of volume of that whole heterogeneous
body, to let it expand without varying in temperature, and using ^
187S.] GateoHi, lAqmd, and SaUd Statet of Water. 81
I rates for steun with ice at the
and M* to denote the
corresptrnding i
taiple point, we h»Te
dp
TT
U
•^^
•w
dt
The tfttrat heftt of evapomtion of one pound of water at the &eeon^
point (or triple point) into steam at the same temperature, as det^miued
by B^nault, is 606*5 thermic units, the thermio unit being here taken
as the heat which would raise the temperature of one pound of water
one degree Centigrade ; and the latent heat of fusion of ice is about 78 or
7fi of the ume thermic units. Hence, though M and M' belong each to
a cobie foot of steam at the triple point, not to a pound mass of it, atill
^L .. M . _ 606
the ratio g[. "• - 79+806-
Henoe
dt 606 ]^
■^"79+606- Ms"
This shows that for aay small descent in temperature from tiie triple
point (where the pressure of steam with ice is the same as that of steam
with water), the pressure of steam with ice falls off 1'13 times as much
as does the pressure of steam with water.
In submitting the qnantitative calculation now given, I have preferred
to adopt the method proposed and developed \>y my brother rather than
that which I had myself previously devised, because his method is simpler,
and brings oat the results more briefly by eeteblished principles from
existing experimental date. I may say, however, that the method devised
by myself was also a true method, and that I have since worked it out to
ite numerical results, and have found that these are quite in accordance
with those brought out by my brother. The two indeed may be r^jarded
as being essentially of the same nature ; and I think it unnecessary to
occupy space by giving any details of the method I planned and have
carried out. Its general character may be sufBciently gathered from the
concluding passages of the British-Association 1872 paper, as printed
in the TranuctionB of the Sections, Brighton Meeting.
In order to discover whether the feature now developed by theoretical
considerataons is to be found showing itself in any decree in the experi-
ment^ resulte of Begnault on the pressures of steam at different tem-
p^atnreB*) I have made careful examinations of hia engraved curve
(plate viii. d his memoir), and of his empirical formulas adapted to
fit veiy closely to tJie resulte exhibited in that curve, and of his final
* BagDMil^ " Dm Foroet BlattiquM de la Tapeor d'Ean tux diffirmtea Tempjra-
tnm,' HimoiTea de I'AcAdf mie de* Bdenoec, 1847.
82 Prof. J. Thomson o» ^Ae [Dec. 11,
l^ables of results at the close of hie memoir ; aud by every mode of
■crutany which I htive brought to bear on the eubjwt (in fact by each
of eome seven or eight varied modes) I have met with clear indication
of the ezietence of the expected feature ; aod by eome of them I have
found that it can readily be brought prominently into notice. The
engraved curve drawn ou the copper plate by Regnault himself is offered
by him aa the definitive expression of bia cxperimente, as being an expres-
sion which aatiafiea as wetl aa possible the aggregate of hJH observations —
subject, however, to a very alight alteration, which he ha« pointed out as
» requiaite amendment in the part of the curve immediately below the
Ereeiing-point, a part with which the invoatigntiouB in the present paper
are specially concerned.
After telling (page 681 ) of the great core nith which he had marked
the curve on the copper plate and got it engraved, he Bays ; — " Je n'ai
pas pu intec cependant qiielquea petites im^ularit-cs dnus les courbes ;
mais une seule de c*!.s iwf'gnlarites me parait assez important* pour
devoir fitre signal^. Kile se prdsente pour les basses temperatures com-
prises entreO°et —16°; la courbe creuBe trop vers 1 'axe des Jemp^ratures,
elle laisse, notablement au-dessus d'elle, tout«a lee determinations experi-
mentales qui ont iti fmtcs entre 0° et — 10°. Ainsi les valeurs, que cette
petite portion de la courbe donne pour los forcee ^lastiquea, sont nn peu
trop faibles, et j'ai en soin de les augmenter, de la qnuitit^ convenable,
dans les nombres que je donneru plus loin." Whether we are now to
think that dus bend downwards* of the curve towards the axis of tem-
peratures, involving what Begnault regarded as a small faulty departure
of his drawn curve from his actual experiments, was introduced merely
by a casual want of accuracy in drawing, or whether we may suppose
(hat possibly there may have been some experimental observationB which
attracted the curve downwards, but were afterwards rejected on a suppo-
sition of their being untrustworthy, it appears that such a bend is a
feature which the curve really ought to possess, and is one which even
after being partially smooUied off by way of correction is not obliterated,
but still reuuuns clearly discoverable in the final numerical tables of results.
This is best brought to light by means of the empirical formulie
devised and employed by Bc^^ult for the collating of his results.
He proceeded evidently under the idea of the curve being continuous iu
its nature, so that a single formula might represent the pressures of
aqueous vapour throughout the whole of his experiments; but before
seeking for snch a formula he proceeded to calculate several local for-
muhe of which each should represent very exactly his experiments
between limits of temperatire not wide apart ; and afterwards he worked
out several general formuln, each adapted singly for the whole range of
his experiments.
* Jn H. BtgnaaU'i curva the temperatures ue manured horiiontally acroei the
iheet, and preMarea «» mearared upmirde.
1873.] Gaseota, Liquid, and Solid States of Water. 83
In regard to the one of these general fonnulfe which he designates as
fonnula (H)*, he sajs that it represents the aggregate of his determiuft-
tions of the pressures of the vapour of water, referred to the air-ther-
mometer, and ext^iding between the extreme temperatures of —33° and
+232° vith su<;h precision that there could not be any hope of attaining
to representing them bettor by any other mode of interpolation, because
the differences, ho aays, between the calculated numbers and the numbers
deduced from his graphic constructions toe always smaller than the pro-
bable errors of observation. Still, for making out his final general l^ble
of pressures of steam for every degree of the ^-thermometer from —30°
to + 230°, he used three local formulte, finding that by them he could
get slightly closer agreements with his experimental determinations thui
by using the single formula (H) for the whole range. Thus between
—32° and 0° he used his formuhi designated as (K) ; from 0° to 100° he
used his formula (D) ; and between 100° and 230° he used his formula
(H). He points out (page 623) that he might have calculated this Table
throughout its entire extent by the single formula (H), and that he would
thus have got almost identically the some values by it from 100° down
to 40° as those he calculated by the formula (D), but that between +40°
and —20° the pressures given by the formula (H) would be slightly too
small. This gives indication of the existence of the feature which it is
my object at present to bring into view ; and an examination of the
column of Differences in B^nault's Table on his page 608, adapted for
comparing the pressures got from experiments as expressed by his graphic
curve with those got from the fonnula (H), shows distinctly a re-entrant
angle, or at least a flattened place, in the cune at or about 0°. Several
other like ccanparisons, by means of his other formults, give like indica-
tions ; but most of these may for brevity be passed over without further
mention hene. The most decisive indication comes out in the following
way. We may observe that for temperatures adjacent to the freedng-
point and extending both ways from It, Begnault finally adopted as fitting
best to his experiments the formula (E) for temperatures descending
from 0°, and the formula (D) for temperatures ascending from 0°. He
tried (at pages 598, 599 of his memoir) the continuing of the application
of his formula (D) beyond the inferior of the two limits 0° and 100°, for
which he had specially aimed at adapting it to his experimental deter-
minations ; and he found that in calculating by it the preaaures which it
Tould give for temperatures below 0°, these preaaures come out always
slightly in excess of those which were given by his experiments. I have
developed this mode of comparison in a more complete manner, and have
arrived at remarkable results. The formula (D) may be regarded as the
* This and other formula in H. Begnsult'i memoir are hsra referred to only by their
Ittten of rafsrence, bernue to cite the formula tbemwlvee with their aeoimaij aooom-
panying explanation!, would extend tbe present paper to too great a langUi ; and any
penon wishing to serutiniM the formnljc would oaturaUy prsier to h«Te rsooune to
34.
Prof. J. Thomson on the
[Dec. 11,
fonnula for giving the preasure p of 8t«im with water, and (E) as that
for giring the pressure ^ for stcnin with iiie. The following two Tables
show the pressures x> and p for tomperatiires, in each case, both below and
above tbo freezing-point, as calculated from theee two fomiulse ; and they
show, also in each case, the consequent differences of pressure for
1° change of temperature at several different temperatures, or, what is
the same, the values of -^ md -^ for Beveral temperatures slightly
abore and slightly below the freczing-poiut.
Table 1. By Formula (D) : Steam with Water.
Differanowforl'.
wWdiMBTBlueaof^
.Tcmperaturea.
p^,U^_y.
wltioh tlie rnluH of
^Wotig.
tcroiBnitiiret..
-3°
3-703
■280
-2i°
-2°
3-9S3
-29S
-If
-1°
4-231
-31!)
- i"
(1°
4-6110
•340
+ i°
+1"
4-040
■302
+ ir
+2°
5-302
■385
+ 2f
+3°
5-687
Table II. By Formula (E) ; Steam with Ice.
which BraTdaMof^'
taofeatana.
PK«Urt.=p'.
which the Yilqte of
temperature*
-3°
3-644
-297
-2i°
-2°
3-941
-322
-H'
-1»
4-203
■347
- i'
0"
4-610
-376
+ i°
+ 1"
4-986
-406
-Hi"
+2°
5-390
-437
■far
+3'
5-827
.] Ga$€(nu, lAquid, and 8oM 8tate$ of Water. 8S
^'
im them two Tables we obtain the following raluea of gj ae
»d from Begnault'a formulas (D) and (E),
Table m.
Tsluea deduced foe
-2i=
-1J°
- i'
+ i°
+ 1J°
+2J>'
is giroB for -r- at the freeoiiig-point the value of about 1'09 or
di
while its value brought out in the earlier part of the present
■ hy my brother's quantitative calculation was 1'13 ; and bo the
re expected showe iteelf here in B^;nault'a results almost in the
xtant in which theory shows that it ought to exist,
gnault gives in the same memoir (page 627 and following pages)
er Table, one intended chiefly for meteorological purposes, and in
I iii6 pressures are stated from —10° to +35° for every -,^^ of iv
e. In this Table the numbers inserted as representing the pressures
the freering-point are slightly different from the corresponding
in his general Table already referred to ; and he mentions that this
discrepance has resulted from the fact that the two Tables were
d at different periods, and were not calculated by the same formula ;
a remarks that the differences are insignificant, as they scarcely
at to '02 millimetre. Here, too, as in the general Table, the feature
ted shows itself, though in a diminished degree. By a careful
nation of its column of Differences for -^g of a degree, and by
ig a few small arithmetical adjustments which may be r^arded aa
d2
36 On the Gaseoits, Liquid, and Solid States of Water. [Dec. 1 1,
amendfflentB in the way of interpolation in that coIudid, I find that,
according to the experimental reaults aa they are represented in this
Table, the >-alue of __ at the freezing-point would come out to be about
'^
<U
1-05 or 1-06. We have seen by the new calculation, based oa theory, in
the present paper that it ought be 1'13 ; so here the feature ie found
showing itself in about half the degree in which, according to the new
quantitative calculation, it ought to be met with. When we consider
that Eegnault's reductions of his experimental results in the making out
of curves, formulfc, and tflbles for representing them in the aggregate
were, as we have sufficient ground to suppose, carried out under the idea,
now proved to be erroneous, of there being, for aqueous vapour, con-
tinuity in Tariations of pressure with variations of temperature past the
freering-point, just as past any other point of temperature, and when we
further consider that the quantities with which we are here concerned are
indeed very small, it ia not surprising that there should hai-e been a
tendency to smooth off this feature on the supposition that any depar-
tures of the experimental observations from the course of a continuong
or smooth curve were only slight irregularities due to experimental
errors or imperfections.
It may now, in conclusion, be remarked that if from experiments inde-
pendent of those which have been made, or may be made, directly on the
pressure of aqueous vapour at different temperatures near the freezings
point, both above and below it, very correct determinations of the values
of the quantities C, M, and M* can be made, such determinations vrill
lead to more correct evaluations of tt ^^^ -tt for aqueous vapour in
contact in the one case with liquid water, and in the other with ice, than
we at present possess. Such determinations, we may presume further,
would, if very trustworthily arrived at, conduce to the attainment of ft
more correct estimate of the density of steam at the freesing-point (or st ,
the triple point) than we now possess. In fact, in connexion with the
subject which has been here under consideration, there are various im-
portant quantities so connected that improved determinations of one or
more of them may lead to more correct evaluations of others.
1873.] Oa the Action o/Heat on Gravitating Masses. 87
II. " On the Action of Heat on Gravitating Maases." By Williau
Cbookes, F.II.S. &c. Received August 12, 1873.
(Abetract.)
The experimenta recorded in this paper have arisen from observations
made when nsing the vacuum- balance, described by the author in bis
paper "On the Atomic Weight of Thallium"*, for weigbiiig Bubstances
which were of a higher temperature than the surrounding air and the
weights. There appeared to be a diminution of the force of gravitation ;
and experiments were instituted to render the action more sensible, and
to eliminate sources of error.
In aa historical rhume of the state of our knowledge on the subject of
attraction or repulsion by heat, it is shown that in 1792 the Bev. A.
Bennet recorded the fact that a light substance de1icat«ly suspended in
air was attracted by warm bodies : this he ascribed to air-currents.
When light was focused, by means of a lens, on one end of a delicately
suspended arm, either in air or in an exhausted receiver, no motion
could be percdved distinguishable from the effects of heat.
Laplace spoke of the repulsive force of heat. Libri attributed the
movement of a drop of liquid along a wire heated at one end, to the re-
pulsive force of beat ; but Baden Powell did not succeed in obtaining
evidence of repulsion by heat from this experiment.
JBVesnel described an experiment by which concentrated solar light and
heat caused repulsion between one dehcstely suspended and one fixed
disk. The experiment was tried in air of different densities ; but con-
tradictory results were obtained under apparently similar circumstances
at different times, and the experiments were not proceeded with.
Saigey described experiments which appeared to prove that a marked
attraction exist«d between bodies of different temperatures.
Forbes, in a discussion and repetition of Trevelyau's experiment,
come to the conclusion that there was a repulsive action exercised in the
transmission of heat from one body into another which had a less power
of conducting it.
Baden Powell, repeating Fresnel's experiment, explained the results
otherwise than as due to repulsion by heat. By observing the daeent of
the tints of Kewton's Bings between glass plates when heat was applied,
Baden Powell showed that the interval between the plates increased, and
attributed this to a repulsive action of heat.
Faye introduced the hypothesis of a repulsive force of heat to account
for certun astronomical phenomena. Ue described an experiment to
show that beat produced repulsion in the luminous ore given by an induc-
ticn-coO in rarefied air.
The author describes numerous forms of apparatus successively more
<■ Fbil. Tnn*. 16T3, toI. cliiij. p. 277.
88 Mr, W. Crookea on Me [Dec. 11,
and more delicate, which enabled him to detect and then to render rery
sensible an action eserted by heat ou gravitating bodies, which ia not
duo to lUr-cuiTPnts or to nay other knomi form of force.
The following experiment with a balance made of a straw beam with
pith-ball masses at the ends enclosed in a glass tube and Cormected. with
a Sprengel pump, may be quoted from the paper; —
" The whole being fitted up as here shown, and the apparatus being
full of air to begin with, I passed a spirit-flame across the lower part of
the tube at b, observing the movement by a low-power micrometer ; the
pith ball (a, h) descended slightly, and then immediately rose to con-
siderably above its original position. It seemed as if the true action of
the heat was one of attraction, instajttly overcome by ascending currents
" 31. In order to apply the heat in a more regular manner, a thermo-
meter was inserted in a glass tube> having at its extremity a glass bulb
about 1 j inch in diameter ; it was filled with n-ater and then sealed up. . .
The water was kept heated to 70° C, the temperature of the laboratory
being about 15° C.
" 32. The barometer being at 767 millims. and the gauge at zero, the
hot bulb was placed beneath the pith ball at b. The ball rose rapidly ;
OS sooQ as equilibrium was restored, I placed the hot-water bulb above
the pith ball at a, when it rose again, more slowly, however, than when
the heat was applied beneath it.
" 33. The pump was set to work ; and when the gauge was 147 millima.
below the barometer, the experiment was tried again ; the same result,
CHily more feeble, waa obtained. The exhaustion was continned, stopping
the pump from time to time, to observe the effect of heat, when it was
seen that the effect of the hot body regularly diminished as the rarefac-
tion increased, until when the gauge was about 12 millims. below the
barometer the action of the hot body was scarcely noticeable. At
.10 millims. below it was still less; whilst when there was only a difference
eS 7 millims. between the barometer and the gauge, neither the hot-
water bulb, the hot rod, nor the spirit-flame caused the ball to move in
an appreciable degree. The inference was almost irresistible that the
rising of the pith was only due to qurrent« of ur, and that at this near
approach to a vacaum the residual air was too highly rarefied to have
power in its rising to overcome ihe inertia of the straw beam and the
pith balls. A more delicate instrument would doubtless show traces of
movement at a still nearer approach to a vacuum ; but it seemed evident
that when the last trace of air had been removed from the tube surround-
ing the balance — when the balance was suspended in empty space only —
the pith-ball would remain motionless, wherever the hot body were
applied to it.
" 34. I continued exhausting. On next applying heat, the result
k showed that I was far from having discovered the law governing these
1873.] Action o/Beat on Gtavitating MoMg^t* 39
phenomena; the pith ball roae steadily, and without that heaitaticm
which had been observed at lower raref addons. With the gauge 3 millima.
below the barometer, the ascenaion of the pith when a hot body was
placed beneath it was equal to what it had been in air o£ onUnaiy
density ; whilst with the gauge and barometer level its upward more-
ments were not only sharper than they had been in air, but they
took place under the influence of Far less beat ; the finger, for example,
instantly sending the ball up to its fullest extent."
A piece of ice produced exactly the opposite effect to a hot body.
Numerous experiments are next giten to prove that the action is not
due to electricity.
The presence of air having so marked an influence on the action of
heat, an apparatus was fitted up in which the source of heat (a platinum
spiral rendered incandescent by electricity) was inside the vacuum-tube
instead of outside it as before ; and the pith balls of the former apparatus
were replaced by brass balls. By careful management and turning the
tube round, the author could place the equipoised braes pole either over,
under, or at the side of the source of heat. With this apparatus it was
intended to ascertuu more about the behaviour of the balance during
the progress of the exhaustion, both below and above the point of no
action, and also to ascertain the pressure correspondiugwith this critical
point.
After describing many experiments with the ball in various positions
with respect to the incandescent spiral, and at different pressures, the
general result is expressed by the statement that the tendency in each
case was to bring the centre of gravity of the brass ball as near as possible
to tbe source of heat, when air of ordinary density, or even highly rar^
fied air, surrounded the balance. The author continues : —
" 44. Tbe pump was then worked until the gauge had risen to within
fi millims. of the barometric height. On arranging the ball above the spiral
(and making contact with the battery), the attraction was still strong,
drawing the ball downwards a distance of 2 millims. The pump continuing
to work, the gauge rose until it was within 1 millim. of the barometer. The
attraction of the hot spiral for the boll was still endent, drawing it
down when placed below it, and up when placed above it. The mo^'^
ment, however, was much less decided than before ; and in spite of pre-
vious experience (33, 34) the inference was very strong that the attrac-
tion would gradually diminish until the vacuum was absolute, and that
then, and not till then, the neutral point would be reached. Within one
miiliroetre of a vacuum there appeared to be no room for a change of
sign.
" 46. Tbe gauge rose until there was only half a millimetre between
it and the barometer. The metallic hammering heard when the rarefac-
tion is dose upon a vacuum commenced, and the falling mercury only
(Kcasiomlly took down a bubble of air. On turning od the battery cur-
40 Mr. W. Crookes on the [Dec. 11,
rent, there wu the fiiintest po§3ible moremeDt of the brass ball (towards
the spiial) in the dinvtion of attraction.
"48. The workinc oE the pomp was continued. On next making
contact with the batltrv, no movement could be detected. The red-hot
spinl neither sttncted uor repelled. I had arrived at the critical point.
On looking at the gauge 1 »aw it was level with the barometer.
" 47. The pump mas now kept at fidl work for an hour. The gauge
did not rise perceptibly ; but the metallic hammering sound increased in
BharpnesB, and I could sec t hat a bubble or tno of tar had been carried down.
On igniting the gpira), I t^aw that the critical point had been passed. The
flign had changed, and llie action was faint but unmiBtakable rtpvXtum,
The pump was still ki-pt going, and an observation was taken from tima
to time during several hours. The repuJaiou continued to increase.
The tubes of the pump were now waahed out with oil of vitriol*, and the
working was continued for an hour.
"48, The action of the incandescent spiral was now found to be
energetioatlyrfp^Umr, whothar it was placed above or below the brass
ball. The £ngers eierted a repellent action, as did also a warm glass rod,
s spirit-flame, and a piece of hot copper."
In order to decide once for all whether these actions re^y were dua
to air-currents, a form of apparatus was fitted up which, whilst it would
settle the question iTjili-putably, would at the same time be likely to
afford informatdon of much interest.
By chemical means the author obtained in an apparatus a vacuum so
nearly perfect that It would not carry a currant from a BuhmkorfTs coil
whoD connected with platinum wires sealed into the tube. In such a
vacuum the repulsion by heat was still found to be decided and ener-
getic.
An experiment is next described, in which the rays of the sun, and
then the different portions of the solar spectrum, are projected on to the
delicately suspended pith-ball balance, /n vacuo the repulsion is so
strong as to cause danger to the apparatus, and resembles that which
would be produced by the physical impact of a material body.
Experiments are next described in which various substances were used
as the gravitating masses. Amongst these are ivory, brass, pith, pla-
tinum, gilt pith, silver, bismuth, selenium, copper, mica (horizontal and
vertical), charcoal, Ac.
The behaviour of a glass beam with glass ends in a chemical vacuum,
and at lower exhaustion, is next accurately examined when heat is applied
in different ways.
On suspending the light index by means of a cocoon fibre in a long
glass tube furnished with a bulb at the end, and exhausting in various
ways, the author finds that the attraction to a hot body in air, and the
repulsion from a hot body in vaato are rendered still more apparent.
* This nu be efloelod without intcrferm^ irith the eiluiuUoti.
1873.] Action of Heat on Gravitating Masses. 41
Speaking of Cavendish's celebrated ei:periment, the author says that
he has experimented for some months on an apparatus of this kind, and
gives the following outline of one of the results he has obtained v —
'< A heavy metallic mass, when brought near a delicately suspended
light ball, attracts or repels it under the following circumstances : —
" I. WTten the baU is in air of ordinary density.
a. If the mass is colder than the ball, it repels the ball.
6. If the mass is Tiotter than the ball, it attracts the ball.
*' II. WTien the baU is in a vacuum.
a. If the mass is colder than the ball, it attracts the ball.
6. If the mass is hotter than the ball, it repels the ball."
The author continues: — ** The density of the medium surrounding the
ball, the material of which the ball is made, and a very slight difference
between the temperatures of the mass and the ball, exert so strong an
influence over the attractive and repulsive force, and it has been so diffi-
cult for me to eliminate all interfering actions of temperature, electricity,
Ac., that I have not yet been able to get distinct evidence of an inde-
pendent force (not being of the nature of heat) urging the ball and the
mass together.
<< Experiment has, however, showed me that, whilst the action is in one
direction in dense air, and in the opposite direction in a vacuum, there is
an intermediate pressure at which differences of temperature appear to
exert little or no interfering action. By experimenting at this critical
pressure, it would seem that such an action as was obtained by Cavendish,
Beich, and Baily should be rendered evident."
After discussing the explanations which may be given of these actions,
and showing that they cannot be due to air-currents, the author refers to
evidences of this repulsive action of heat, and attractive action of cold, in
nature. In that portion of the sun's radiation which is called heat, we
have the radial repulsive force, possessing successive propagation, re-
quired to explain the phenomena of comets and the shape and changes of
the nebulsB. To compare small things with great — to argue from pieces
of straw up to heavenly bodies — it is not improbable that the attraction,
now shown to exist between a cold and a warm body, will equally prevail
when, for the temperature of melting ice is substituted the cold of space,
for a pith ball a celestial sphere, and for an artificial vacuum a
stellar v<ud. In the radiant molecular energy of cosmical masses may
at last be found that '* agent acting constantly according to certain laws,"
whidi Newton held to be the cause of gravity.
48 Dr. A. Ranaorae on Forced Breathing. [Dec. 18,
III. " On the Male, and the Structure, of Thaumopa pelbicida."
By E. TON Willem5es-Schm, Ph.D., Il.SI.S. 'CUallenger.'
Commuaicated by Prof. Hdiley, Sec. R.S. Received October
24, 1873.
(Abstract.)
This ia an addition to the pnper on Tkawmnpt pelladdn by the sanw
author (Proceedings of Ihe Eoyal Socioly, vol. xxl. p. 2U0), cout^ning an
account of the male, iluJ sutuq corrections oE the deHcription formerly
gjvea. The specien ajipears to be widely distributed, oud to live at mode-
rate deptlts, coming to the surface at night.
IV. " On the Bending of the Bibs in Forced Breathing." By
Arthur Banbome, M.D. Communicated by Dr. Buhdon
SANDBaaoN, M.D., F.R.S. Received May 15, 1873.
(Abstract.)
In a paper "On tho Mechanical Conditions of the KeHpiratory Move-
menta,"read before tho Eoyal Society in November 1ST2", the author
endeavoured to show that there is a distinct differem-e in tlm i-licrd
lengths of a at«nial rib in the two poeitiona of fuU inspiration and
forced expiration, and that a certain degree of bending of the ribs
usually takes place in forced breathing. The measurements on which
these conclusions were based were made with a 3-plane stethometer,
the performance of which was not sufficiently accurate to satisfy the
author, who has accordingly repeated them by the aid of a new instru-
ment, the construction and use of which are described at length in the
present conununication. The author considers that the new instrument
gives fairly accurate results, which fully corroborate the conclusions pre-
viosly enunciated.
December 18, 1873.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
Pursuant to notice given at the last Meeting, the President proposed,
uid Professor Henry iFohn Stephen Smith seconded, the Bight Hon.
Edward Cardwell, M.P., Secretary of State for War, for election and
immediate ballot.
The ballot having been taken, Mr. Cardwell was declared duly elected.
The Presents received were Itud on the Table, and thanks onlerod for
them.
^^' * ProceediogE of the Bo;al Sooiet;, Nonmber 22, 1872.
1873.] iS.t.J.A.'BrounonSm-tpotaandTerrettrialMagnetum. 48
The following cominimicstioiis were read : —
I. "Od the Period of Hemispherical Excess of Sun-spots, and
the 26-day Period of Terreatrial Maguetism." By J. A.
Bboun, P.E.S. Iteceived September 13, 1873.
It appears from the interestiiig commimication to the Sayal Society,
Jane Idth, by Messrs. De La Bue, Stewart, and Loewy*, that the
difference of the area of spots on the visible northern and Bouthem
quarter-spheres of the sun seems, during periods of considerable solar
disturbance, to obey a law such that the difference is a maximum in the
same quarter-sphere duting several successive rotations of the sun, the
difierence being a maximum alternately in the northern and southern
hemisphere — the time &om mftTimiiin to "i^^TiiiFni for the same
hemisphere, bdng variable between 18 and 32 days, but hating a mean
value of about 25*2 days.
It occurs at once that if the variations of the mean t«rrestiia] mag-
netic force are connected in any way with the aolar spots, or the causes
which produce them, we might here find some explanation of the mag-
netic period of 28 days, the difference of spot-area in one hemisphere
from that in the other being related to a difference of the solar magnetic
action.
In order to determine whether such a connexion existed, I projected
first the curves of excess of spot-area given in the paper of Messrs.
De La Bue, Stewart, and Loewy, and below them the daily mean hori-
sontal force of the earth's magnetism during the same periods. The
conclusion from these projections is, that there is no rekUion whatever
hetween the two ekutet of curves. The maxima and minima of the one
agree in no way with those of the other : the greatest excesses of sun-
spot area in the one hemisphere over those in the other occur when the
earth's magnetic force is the most constant ; the greatest variations of
the earth's magnetic force from the mean occur in several instances
when the sun-spot area is equal in the two visible quart^r-spheros.
It Aould be remembered, in considering the cun-ee of sun-spot excess,
that the minima and maxima are in some cases only relative, — sometimes
Hie one, B<mietime8 the other being really cases in which there is neither
tni|Timnwi nor minimum — that is to say, cases in which the sun-spot area
is eqna], or nearly so, in the two visible quarter-spheres.
It would be hasty to conclude &om this comparison that the variations
of the mean magnetic force are really unconnected nith the mode of
distribution of the sun-spots. Other methods of grouping the spots
may perhaps be employed with advantage relatively to this and other
questjoos; for example, were the position of the centra of gravity of
the nm-spota determined for the visible quarter-spheres and hemisphere,
■ Froo. Bti;. Boc vol. ui p. S90.
44 VroL Dnacaa OH Ike ytnaui SfMltm tjf Actiain. [Dee. 18^
^ring each ipot a weight in proportton to its area, the ^-arittiaa of
thtaw potttioiM in latitude anil tangitudi-, iumI their «-^ht«, migbt ^re
A more tatinfactonr base (or tliia ■.■ompamoti ai>id fur other d^acdoiw.
It «-i]i be obrioaa al»o tliat this invintigalioa rcfen onl}' to the ruiUe
heunepbere of the sun ; an approiimatian to the ipot-<Uatributiau oa
the other hemisphere, however, will be frequeotlj pueaiMe.
II. " On the Nervous Sj-stem of Jtclinia." — Part I, By Professor
P. Martin Du.nca.v, M.B. Lond., F.R.S., &c.' Beceived
October 9, 1873.
(Abstract.)
After noticing the investigations of previoos anatomUta in the 1
tolugy of the chromatophorM, the work of Schneider and Kotteken an I
these supposed orgaus of special seuse Is examined and crilicised.
Agreeing with Kottehen iu his description, some further iuformation 1
is given respecting the nature o£ the bacilloiy layer and the minultt J
auatouj of the elongated cells called "cones" by that author. Thtt I
poBition and nature of the pigment-cells is pointed out, aud also the pent- 1
liarities of the tissues tlicv environ. It is shown thai the large re-
fi^'tilo CL-llw, which, a<.-.-or.!fijr; t,, I{„ii,-k.-FL, an- sihiut^M k■l^u■.-], Ihe
bacilli and the eones, are not invarii^ly in that position, but that badlli,
cones, and cells are often found separate. They are parta of the ecto-
thelinm, and when conjoined enable light to affect the nervous syBt«m more
readily than when they are separate. Further information is given
respecting the fusiform nerve-cells and small fibres noticed by Bottekea
in the tissue beneath the cones ; and the discovery of united ganglion-like
cells and a diffused plexiform arrangement of nerve b asserted. The
probability of a continuous pleius round the AiUinia and beneath ea^
chroroatophore is suggested, and the physiological action of the struc-
tures in relation to light is explained.
The minute structure of the muscular fibres and their attached fibrous
tissue in the base of Aeiinia is noticed ; and the nen ous system in that
region is asserted to consist of a plexus beneath the endothelium, in
which are fusiform cells and fibres like sympathetic nene-fibrila. More-
over, between the muscular layers there is a continuation of this plexus,
whose ultimate fibrils pass obliquely over the muscular filn^, and either
dip between or are lost on them.
The other parts of the Actinia are under the examination of the
author, but their details are not sufficiently advanced for publication.
The nervous system, so far as it is examined, consists of isolated fusi-
form cells with small ends (Biitteken), and of fusiform and spherical
cells which commuuicato with each other and with a diffused plexus.
The plexus at the base is areolar; and its ultimate fibres are swollen hen
and there, the whole being of a pale grey colour.
1
1873.] Mr. W. Shanks on Discrepancies in the Value ofir. 45
III. '' On certain Discrepancies in the published numerical value
of ir/* By William Shanks^ Houghton-le-Spring, Durham.
Communicated by Prof. G. G. Stokes, R.S. Received October
13, 1873.
The author's attention has been recently drawn, by Mr. John Morgan,
of Bishopbriggs, Glasgow, to two cases of discrepancy in the author's
published value of ir, and to the misprint of a figure in the value of
tan" ^ ^ (one of the arcs employed in determining w), as given in the
author's paper of April 1873. These two discrepancies in the value of
Wy which will be described presently, did not appear in the paper pre-
sented by the late William Rutherford in 1853, wherein the author's
extension to 530 decimals was correctly given.
The source of the two cases of error was easily discovered, on re-
ferring to the author's manuscript of 1852 ; for it was there found that
the 461st and 462nd decimals in the value of tan~^ ^ were, in the process
of carefid revision previous to publication, altered from 88 to 96 ; and
this alteration required the addition of 128 in the corresponding place of
the value of ir. This addition was rightly made in the value sent to
Mr. Rutherford, and given, as above stated, in his paper. It should
seem that the author unfortunately did not take a copy (for his own use)
of what he forwarded to Mr. Rutherford. At all events, from some
strange cause or accident (perhaps from being overworked) the addition
of 128 was very soon afterwards made at the 513th, 514th, and 515thy
instead of at the 460th, 461st, and 462nd decimal places. Hence arose
the double error, which remained, strange to say, undetected for upwards
of twenty years ! This mistake, however, from its nature^ in no taise
affects the accuracy of the other figures.
It is sufficient merely to state that the 75th decimal, before alluded
to, in the value of tan~^ \ should be 8 and not 7 ; but it may be well to
give the entire value of x anew : —
Value of ires 3*
14159 26535 89793 23846 26433 83*79 50*88 41971 69399 375»o 58*09 74944
59230 78164 06286 20899 86280 34825 3421 I 70679 82148 08651 32823 06647
09384 46095 50582 23172 53594 08128 481 I I 74502 84102 70193 8521 I 05559
64462 29489 54930 38196 44288 10975 66593 34461 28475 64823 37867 83165
^7120 19091 45648 56692 34603 48610 45432 66482 13393 60726 02491 41273
72458 70066 06315 58817 48815 30920 96282 92540 91 71 5 36436 78925 90360
01133 05305 48820 46652 13841 46951 94151 16094 33057 27036 57595 9^953
09218 61173 81932 61 179 31051 18548 07446 23799 62749 56735 18857 52724
89122 79381 8301 I 94912 98336 73362 44065 66430 86021 39501 60924 48077
23094 36285 53096 62027 55693 97986 95022 24749 96206 07497 03041 23668
86199 SI '00 89202 38377 0213 I 41694 I I 902 98858 25446 81639 79990 46597
00081 700S9 63123 77387 34208 41307 91451 18398 05709 85 &0.
The statement in the author^s paper of April 1873, touching Bichter'f
46 Prof. S. Clerk Maxwell on [Dec. 18,
Talue of «■ to 600 decimnls and tho date of its publication, iraa correct,
u such value was compared uith the author's giren in Mr. Rutberford'e
paper of 1853, and of course agrees with what is given above in thia.
rV. *' On Double Refraction iu a Viscous Fluid in motion." By
J. Clike Maxwell, M.A., Professor of Experimental Physics
in the University of Cambridge. Ileccivcd October 31, 1873-
According to Poisson's * theory of tho internal friction of fluids, n
viscous fluid behavet^ as an clastic solid would do if it were periodically
liquefied for an instiiut and solidified again, so that at each fresh start it
becomes for the motni.'iit like iin elaatio solid free from strain. The state
of strain of certain tDinsparcut bodies may be investigated by means of
th^ action on polarized light. This action was obsen'ed by Brewster,
and was shown by Freanel to be an instance of double refraction.
In 1866 I made sojue attempts to ascerttun whether the state of strain
in a viscous fluid in motion could be detected by its action on polariEed
light. I had a cylindi-ieul box with a glass bottom. Within this box a
solid cylinder could be made to rotate. The fluid fo bi" esaminetl was
placed in the Annnlur space between this cylinder and the sides of the
box. Polarined light was thrown up through the fluid parallel to the
axis, and the inner cylinder was then made to rotate. I was unable to
obtnun any result with solution of gum or sirup of sugar, though I ob-
served on effect on polarised light when I compressed some Canada
balsam which had become very thick and almost solid in a bottle.
It is easy, however, to observe the effect in Cuiada balsam, which is so
fluid that it very rapidly assumes a level surface after being disturbed.
Fnt some Canada balsam in a wide-mouthed square bottle; let light,
polarized in a vertical plane, be transmitted through the fluid ; observe
the light through a Nicol's prism, and turn the prism so as to cut off the
light; insert a spatula in the Canada balsam, in a vertical plane passing
through the eye. Whenever the spatula is moved up or down in the
fluid, the M^t reappears on both sides of the spatula ; this continues only
BO long as the spatula is in motion. As soon as the motion stops, the
light disappears, and that so quickly that I have hitherto been unable to
determine the rate of relaxation of that state of strain which the light
indicates.
If the motion of the spatula in its own plane, instead of being in the
plane of polarization, is inclined 4S° to it, no effect is observed, showing
that the axes of strain are inclined 45° to the plane of shearing, as indi-
cated by the theory.
I am not aware that this method of rendering visible the state of strain
■ Journal de I'fioole FoljtechQique, tome li"- <»^- 1' (1829).
1873.] Double Refraction in a Visrof/s Fhi'ul in motinn. 17
of a viscous fluid has been hitherto employed ; but it appears capable of
famishing important information as to the nature of viscosity in difEerent
substances.
Among transparent solids there is considerable diversity in their action
on polarized light. If a small portion is cut from a piece of unannealed
glass at a place where the strain is uniform, the effect on polarized light
Tanishes as soon as the glass is relieved from the stress caused by the un-
equal contraction of the parts surrounding it.
But if a plate of gelatine is allowed to dry under longitudinal tension,
a small piece cut out of it exhibits the same effect on light as it did
before, showing that a state of strain can exist without the action of
stress. A film of gutta percha which has been stretched in one direc-
tion has a similar action on light. If a circular piece is cut out of such
a stretched film and warmed, it contracts in the direction in which the
stretching took place.
The body of a sea-nettle has all the appearance of a transparent jelly ;
and at one time I thought that the spontaneous contractions of the living
animal might be rendered visible by means of polarized light transmitted
through its body. But I found that even a very considerable pressure
^>plied to the sides of the sea-nettle produced no effect oil polarized
light, and I thus found, what I might have learned by dissection, that the
sea-nettle is not a true jelly, but consists of cells filled with fluid.
On the other hand, the crystalline lens of the eye, as Brewster ob-
served, has a strong action on polarized light when strained either by
external pressure or by the unequal contraction of its parts as it becomes
dry.
I have enumerated these instances of the application of polarized light
to the study of the structure of solid bodies as suggestions with respect
to the application of the same method to liquids so as to determine
whether a given liquid differs from a solid in having a very small
" rigidity,** or in having a small " time of relaxation"*, or in both ways.
Those which, like Canada balsam, act strongly on polarized light, have
probably a small '* rigidity," but a sensible '' time of relaxation." Those
which do not show this action are probably much more '' rigid," and owe
tiieir fluidity to the smaUness of their '' time of relaxation."
The Society then adjourned over the Christmas Becess to Thursday,
January 8, 1874.
* The "time of relaxation " of a substance strained in a given manner is the time
required for the complete relaiation of the strain, suppbsing the rate of relaxation to
remain the same as ai the beginning of this time.
4S Presents. [Dec. 1 1,
Prestnts reMive<l DecnnUr 11, 1873.
Berlin : — Koniglicbe Akademie der Wissenschaften. Abhandlungeii auA
dem Jahre 1872. 4to. Berlin 1873. The Academy.
London :^Iiistitution of Cii-U Engineers. Minutes of Proceedings.
Session 1872-73. 2 vols. 8vo. London 1873. The rnstitution,
Luxembourg : — Inatitut Eoyal Grand-Ducal, Section des Sdences N»-
turellea et Mathiimatiques. Publications. Tome XUI, 8vo. Lvm-
emhourg 1873. The InBtitution.
Milan : — Keale Ifltituto Lombardo di 8cienze e Letters. Beadiconti.
Serie H. To!. V. £mc. 8-lC. 8vo. Milaiiol872. The Inatitute..
Munich: — K.b, AkademiederWissenachaften. Sitzungsberiehte. Math.r'
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hist. Clause : 1872, Heft 4, 5 ; 1873, Heft US. 8vo. Miintfu^
1872-73. Hede sur Vorfeier des alierbochsten Geburtafestes St.
Majesttkt doa Konigs Ludwig U., Ton J. von Dolliager. 4tD,
1873. Gediichtuissrede auf Friedrich Adolph Trendelenburg, ^
K, von Prantl. 4to. 1873. Der Antheil der Aiademie an d^
Entwiokelung der Electricitatslehre, von W. Eeetz. 4to. 1873.
The Academy.
Plymouth : — Devonshire Association for the Advancement of Science,
Literature, and Art, Report and Transactions. Vol. VI. Part 1.
8vo. Plymoulh 1S73. The Association.
Bydney:^ — Eoyal Society of New South Wales, Transitctious for 1870,
1871, 1872. 8vo. Sydnry 1871-73. The Sodety.
Turin : — E. Accaderoia delle SciemK. Atti. Vol. Vm. disp. 1-fi. 8to.
Torino 1872-73. The Academy.
Wurzburg ; — Physikalisch-mediciniscbe Gesellschaft. Verliandlungen.
NeueFolge. Band IV. Heft 2, 3. 8vo. Wur^urg 1873.
The Society,
Observfttione, Eeports, &c.
Coimbrai — Obsen-atoriodaUniveraidade. Ephemeridea Afitronomicas,
1875. 8vo. Coimhra 1873. The Observatory.
London: — Army Medical Department. Eeport for the year 1871.
Vol. XUI. 8vo. London 187.3. The Department.
Medical Department of the Navy. Statistical Heport on the Health
of the Navyfor 1871, 8vo. London 1873. The Department,
Melbourne: — Observatory, Results of Astronomical Observationa
made in the years ISGQ and 1870, under the direction of liobert
L. J. Ellery. 8vo. ifelbourm IS73. The Observatory.
San Fernando :— Obsorvatorio de Marina. Anales. Seccion 2*. Obser-
vacionea Meteorologicas, 1870, 1871. fol. San Fernando.
The Observatory, by the Foreign Office.
1878.] Pre$enis. 49
Damon (3. W.). F-B-S. Beport on the Fossil FUntB of the Lower
Carboniferous and Millstone-grit rormations of Canada, tiyo.
Mtmtreal 1S73. The Author.
Se GandoUe (Alph.), For. Mem. B.8. B^flexioiiB but lee Ouvragea gen^
nux de Botanique DescriptiTe. 8vo. Geneve 1873. Prodromi Sys-
tematic Naturalis Tegetabilium Historia, Numeri, Conclusio. 8vo.
Pantiit 1873. The Author.
Howard (J. EUob) BlustratioTia of the Nueva Quinologia of Pavon,
with coloured phttes by W. Fitch, fol. Loridon 1862. The Author.
Kronecker (L.) Ober die verschiedenen Sturm'achen Beihen und ihre
gegenaeitigeD Beziehuugen. Svo. Berlin 1873. The Author.
lATtet (B.) and H. Chriatj. Bflliquis Aquitanica. J)dit«d by T. Bupert
Jonea, FJt.8. Parts 12, 13. 4to. London 1873.
The Esecutors of the late Henry Christy, Esq.
Foey (A.) Nouvelle Claeaificatiou des Nuagea, suivie d'ime instruction
poureerrir^robserTatioiides Nuageset desCourantaatmoBph^riques.
Sor lea rapports eutre les tacbea aolaires et les ouragans des Antilles,
de rAtlantique nord et de I'oc^an Indieu aud. 4to. Parit 1873.
The Author.
Thirlwall (Bishop). Sir Frederic Madden, K.H. Beprinted from the
Address of the Bishop of St. David's before the Boyal Society of
litOTatope. 1873. 8vo. London. F. W. Madden, Esq.
Decanher 18, 1873.
Transactions.
Briinn : — Xaturforschender Terein. Teriiaudlungen. Baud X. 1871.
8^0. 1872. The Society.
Christiania : — Kongelige Norske Fredeiiks Universitet. Aarsberetning
for Aaret 1872. 8to. C&rwftanta 1873. Om Nordboemes For-
tnndelser med Buslaod og Tilgrtendsende Lande, af P. A. Munch.
8to. 1873. Die .£gyptischen Denkmaler in St. Petersbui^, Hel-
ungfoTB, TJpsala und Copenhagen, von J. Lieblein. 8to. 1873.
Norsk Fangst^kipperes Opd^else af Kong Karl-Land, af H,
Mohn. 8to. 1872. Aaaland.U.,af C.A.Holmboe. 8to. 1872. Bi-
drag til Knndskaben om Dyrelivet paa vore Havbanker, af G. O.
Bars. 8to. 1872. To Norske Oldsagfund, af O. Bygh. Sto. 1872.
To nyfundne Iforske Bune-Indskrift«r fra den nldre Jnmalder, af
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tesgmalmi, Gm., af B. Collett. 8to. 1872. Slsgten Latmnculns,
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til Theorien for IMssodationen, af C. M. Qnldberg. 870. 1872.
Bemerkuiuger om Formelan for Hdidemaaling med Barometer, af
C. M. Guldberg. 8to, 1872. Sur la resolution des ^uations du
TOL. xzn. B
BO Premtih. [Dec. 18,
'IVatisactione {cantinue'/i.
2", 3«« et 4"' ik'grd par la f ouction - (.r), par A. 8. Guldbei^.
8so. 1S72. Bidrag til KimilBlo(bi!ii om VegetatioHon paa Sowaja
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1872. Priis AfhandUng om den frio VUliea ForboM til Sulv-
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Ornithology of Northern Norway, by H. CoUptt. Uvo. 1«72. The
Leprous Diseases af the Eye, by O. B. Biilj and Q. A. 'Hataea.
8ro. 1873. Korek Ordbog, af Ivar Anaeu. 8vo. 1879. Om
Noreke Kongtrs Hyldiiig og Kroniug i wldrc Tid. 8to, 1873. i
Nyt Magaziu for Naturvidonsliabern^. Bind XIX., XX. H«ftl,
2. 8vo. 1572-73. Fwhwidlingcir i Vidonsknlis-K-UbntM't A«r
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memoraticii] of the mroDatioii of King Osoar XL and QliMD
Sophia at TrondhJHm, July 1S73. The Umversity,
limsbriick: — Ferdinandeum fiir llrol und Vorurlborg. Zeitschrift.
Dritt*. Folge. Heft 17. 8vo. 1872. The Insiitntion.
NaturwisBenscbaftUch-mediziuisclierVi'rfiii. Bericht*. Jnbr.S. Heft
1-3. 8vo. IS73. Tha Infttitution.
LislMJu: — Acadeinia Real das Sciencias. M^morias. Classe de Sirioncias
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thomaticas, Physicas 15 Natural. Tomo III. 8vo. 1871- SubeidioB
para a Hi'^toria da India Portugiieza. 4to. 18(i8. Corpn Diplo-
uiatico Portuguez. Tomo I.-IV. 4to. 1862-70, Leiidas Us India,
por G. Corrpa. Tomo I.-IV. 4tci. l*«58-66. Quadro Elementaf
das Bela^oca Politicas e Diplomaticas de Portugal. Tomo I.-XI.
XlWXVni. 8vo. 1842-80. llistoria dos Estabelwimentos
ScieutifiLKis, Literanos. e Artiaticos de Portugal, por J, 8. lUbeiro,
Tomo 1,-111. Bvo. 1871-73. Portugalliai Insmptionea Bomaoas.
Vol. I. fol. ie.50. Flora Cochiuchinpnsis. 2 rols. 4to. 1790.
Vest igios da Lingua A rahica em Portugal, 4to. 1789. Ovidio e
Caslilho, Os Fnst-os, Poema com amplos Commentarios. 3Jvol9.
Rvo. 1862. Teatro de Molicre (O Medico & for^a, Tartufo, O
Avarento, As SabiehonasJ, 4 vols. 12mo. 1869-72,
The Academy.
Loudon: — Eutomologii.'al Society. Transactiona for 1873. Part 3, 4.
Sto. The Society.
Institution of Naval Architects. TransaetioM. Vol, XIV. 4to.
1873. The Institution.
Koyal Agricultural LSocioty. Journal, Second Series, Vol. IX.
Part 2. Svo. 1873. The Society.
Society of Aiitiquan«8. Proceedings. Second Series. Vol. V. No.
* 7,8; Vol, VI. No. 1. 8to. 1873. The Socisty.
1878.] Present!. 51
Tr»u?action9 («m(i»n«d).
Shanghai :— North China Branch of the Hoyal Asiatic Society. Journal
for 1871 and 1S72. New Series. No. 7. Svo. 1S73. Catalc^e
of the Library. 8vo, 187i*. The Society.
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The ("ovcniinent of India.
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The Observatory.
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Greenwich : — Eoyal Observaton.-. Astronomical and Maguetical and
Meteorological Obsen'ationa made in 1871. 4to. Loudon 1873.
Astronomical Hesults, 1871. Slagnetical and Meteorological
Observations, 1?71. History and Description of the Water
Telescope. 4to. The Admiralty.
Washington :— Patent Office. Eeijorts. 186». 1S70, 1S71. 7 vols. SfO.
1S71-71 The Office.
I87S.] Dr. Maxwell Simpson on the Brom-Iodidet. 61
Tmuactioiia (amtinued).
Shanghai ; — Korth China Branch of the Boyal Asiatic Sode4|y. Journal
for 1871 and 1872. Kew Series. No. 7. 8to. 1873. Catalogue
of the library. 8to. 1872. The Society.
Obserrationa, Beports, Ac.
Calcutta : — Beport of the Met«orolc^cal Beporter to the Gh>Temment
of Bengal, by H. F. Bknford. fol. CaleuOa 1873.
The GoTemment of India.
Cape of Good Hope : — Boyal Observatory. Besnlts of Astronomical
Obseirations made in the year 1857. 8to. Cape Toum 1872.
The Obaervatory.
Christiania : — Met«oro1ogiebe Institut. Norsk Meteorologisk Aarbog
tot 1872. 6** Aai^ang. 4to. Chrittiania. The InBtitnto.
Greenwich : — Boyal Observatory. Astronomical and Magnetical and
Meteorological Observations made in 1871. 4to. London 1873.
Astronomical B«sults, 1871. Magnetic^ and Meteorolc^cal
Obseirationa, 1871. History and Description of the Water
Telescope. 4to. The Adminlty.
Washington :— Bitent OfEc«. Beports, 1869, 1870, 1871. 7 vols. 8vo.
1871-72. The Office.
January 8, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The following communications were read ; —
I. " On the BromJodides." By Dr. Maxwkli. Simpson, F.R.S.,
Profeasor of Chemistry, Qaeen's College, Cork. Beceived
November 4, 1873.
Some yean ago I ascertained that diltoide of iodine comtunes directly
vttli the. defines and the non-saturated haloid ethers in the same manner
as free chlorine or brondne. I have since ascertained that bromide of
iodine also enters into direct combination with these bodies.
In the following experiments I have invariably used a solution of
bromide of iodine in water, which was prepared by adding rather more
ttiaD a molecule of iodine in'fine powder to a molecule of bromine pre-
Tioasly mixed wiih about six times Its weight of water. The bromine
waa repeatedly agitated during the addition of the iodine, and kept cold
by being surroonded by water. An almost black liquid was thus ob-
tained, whidi was separated from the excess of iodine.
Brwnriodid* of ethjflene. — This body was formed by passing a stream
53 Dr. Maxwell Simpson an the Brom-Iodides. [Jan. 8,
of olefiant gas into the foregoing solution, which was kept cold during
the absorption of the gas. An oily liquid soon made its appearance,
which was the body in question ; it was then subjected to distillation,
having been pre\'iou8ly washed with dilute potash, and afterwards with
distilled water. Almost the entire quantity passed over without decom-
position bet\^^een 162° and 167® Cent. This gave on analysis the follow-
ing numbers : —
C 10-21 10-36
H 1-70 1-79
At the temperature of the air this is a solid body, consisting of a mass
of long white needles, which melt at 28° Cent. At 29° it has a specific
gravity =2'516« It has a sweet biting taste; on exposure to light it
becomes slightly coloured, from the separation of free iodine. When
subjected to the action of alcoholic potash, it yields iodide of potassium
and a gas burning \^dth a green flame, which is doubtless bromide of
vinyl. It is an isomer of the brom-iodide obtained by Pfaundler*, and
afterwards by Eeboult, by exposing bromide of vinyl to the action of
hydriodic acid. Pfaundler's compound boils between 144° and 147° Cent.
Bromriodide of propylene, — This body was formed by passing propylene
gas derived from iodide of allyle into the brom-iodiue solution. It was
washed with dilute potash, then with water, and distilled. The greater
part passed over between 160° and 168° Cent., suffering, however, at the
same time slight decomposition. The distillate was then analyzed, having
been previously agitated with mercury to remove free iodine. The fol-
lowing are the results : —
^^^j^' Experiment.
C 14-46 14-89
H 2-41 2-77
Notwithstanding the difference between the theoretical and experi-
mental numbers, I believe this is a definite compound, and not a mixture
of bromide and iodide of propylene. The discrepancy probably arises
from the slight decomposition which the body suffered during distiUation.
Brom-iodide of propylene is, when freshly prepared, a colourless oily
liquid ; it has a sweet and biting taste. Treated with alcoholic potash,
it yields iodide of potassium and brom-propylene (C, H, Br).
lodo-dibrom^inyl, — When the brom-iodine solution and bromide of
vinyl are brought into contact, direct combination takes place, and this
body is formed. In order to complete their union, it is ad\isable to
heat them gently in a sealed tube. A portion of the oily product thus
obtained was washed with potash and distUled ; almost the entire quan-
tity passed over bet^ieen 170° and 180° Cent. As, however, it suffered
* Jahresbericht, 1865, p. 483. t Ibid. 1870. p. 439.
1874.] Dr. J. Stenhoose on the Hiatory of the Orcitu. 68
coDsidemble decompoaition during distillatioit, I aiulTsed, in preference,
a portion of the remainder, which had not been distilled, h&ring pre*
riowAj dried it at 100°, and agitated it with metallic mercury to remove a
tmoe of free iodine. The following are the resulte of the uialTBis : —
C 7-64 7-67
H 0-96 Ml
This is a colourleM oily liquid ; like the others it has a sweet and
biting; taate. Its specific gravity at 29°C«nt. is :!-86. Heated to the
temperature of 100° in a sealed tube with moist oxide of silver it occa-
sioned a violent explosion. Heated in an open retort vrith the same
body, it evcdved carbonic add gas and bromide of vinyl.
II. " Contribationfl to the Hiatory of the Orcins. — No. IV. On
the lodo-derivatives of the Orcins." By John Stenhousb,
LL.D., F.R.S., &c. Received November 10, 1873.
A pi^iminary notice on these compounds has already appeared in the
* Chemical News,' vol. xxvi. p. 279 ; and the present paper contains a more
detaUed account of my experiments.
In 1864* I published an account of a crystalline t«riodorcin obtained
by precipitating an aqueous solution of orcin with a solution of iodine
monocUoride, but I found I was unable to prepare any other iodine
derivative of orcin by this process. It seems probable, however, that
the method devised some years ago by Prof. Hlosiwetzt, and commu-
nicated by him at the meeting of the " Naturforscher und Aerzte in
Innsbruck," would yield the lower substitution compounds. This was
found to be the case ; for on agitating an ethereal solution containing
equal molecular weights of orcin and iodine with dry precipitated mer-
curic oxide, the colour rapidly disappears, and manoiodorcin is formed ;
this may be obtained by distilling off the ether and crvatallizing the
residue from benzol, in order to separate an uncrystallizable oily com-
ponnd which accompanies it. It is, however, still contaminated with a
smaU quantity of mercuric iodide, which obstinately adheres to the sub-
stance, and can only be removed by recrystallization from a dilute aqueous
Bolation of potassium iodide ; this difHculty arises from the circumstance
that mercuric iodide is more or less soluble in most of the liquids usually
employed as sdvents. For this reason I found it advisable to substitute
plumbic oxide for the corresponding mercury compound originally pro-
posed by Hlasiweti.
Monoiodorein, CSjH,I O^ — One part of pure dry ordn is dissolved in
* Jonm. Caiem. 800. rol. xvii. p. 327. t Dent. ohem. 0«a. Ber. II. 661.
54 Dr. J. Stenhoase on the [Jan. 8,
six parfcs of ether ; then two parts of iodine are added, and the mixture
agitated until the whole of the iodine is dissolved ; nine parts of very
finely powdered lead oxide (litharge) are now introduced in small portions
at a time with frequent agitation. A marked action takes place, ac-
companied bj development of heat, and the colour of the solution rapidly
disappears. On distilling off the ether and extracting the residue with
hot benzol, the iodordn separates in the crystalline state on cooling.
Two or three alternate crystallizations from benzol and from water
suffice to render the compound pure ; but care must be taken not to boO
the aqueous solution for any length of time, as the iodorcin is thereby
partially decomposed.
Monoiodorcin in a pure state crystallizes in colourless prisms, which
melt at 86^*5, and decompose with evolution of violet vapours of iodine
when strongly heated. Concentrated sulphuric acid has but little action
on the substance in the cold ; but when gently heated with it, the iodorcin
is decomposed and iodine is freely liberated. Warm nitric acid likewise
acts energetically, evolving nitrous fumes and liberating iodine. Iodordn
is only slightly soluble in cold water, but readily in hot water. It is
very soluble in ether and in hot alcohol, moderately so in benzol and in
hot petroleum (crystallizing out from the latter almost entirely on cooling),
slightly soluble in carbonic disulphide. It is quite destitute of the pe-
culiar astringent sweet taste so characteristic of pure orcin.
Dried in vacuo and submitted to analysis, it gave the following
results : —
I. *332 gramme substance gave '311 gramme argentic iodide.
ft
U. *256 gramme substance gave *314 gramme carbonic anhydride and
•067 gramme water.
Theory.
I.
11.
C, = 84
33-00
• • • •
33-44
H, = 7
2-80
• • • •
2-90
I = 127
60-80
50-63
• • • •
O, = 32
12-80
• • • •
• • • •
260 100-00
These numbers correspond ^nth those required by the formula
C,H,IO,.
Monoiodresorcin, C^ H, 1 0,,. — This compound is prepared in a similar
manner as the corresponding ordn compound : 10 parts of resordn and
24 of iodine are dissolved in 60 of ether, and about 110 of lead oxide are
gradually added. After removal of the ether and extraction with benzol,
the iodorcin is purified by crystallization from hot water, in which it is
much more soluble than ihe iodorcin. lodresorcin crystallizes in rhom-
boidal prisms, which are very difficult to obtain colourless ; they melt at
67**, and, like those of the orcin derivative, decompose when strongly
1874.] Uittory (fftke Orcau. 65
heated. It ia mach more soluble in water than iodordn, and la very
■duble in alcohol or ether ; hot benzol dissolves it readily ; but it is only
slightly BcJuble in cwbonic disulphide. When heated with nitric or sul^
phone add, it behaves like iodorcin.
The analytical results were obtaiited from the compound dried in
WKUO, at the ordinary temperature.
L -343 gramme subet&ace gave '341 gramme ai^entic iodide.
Q. '357 gramme substance gave '354 gramme argentic iodide.
m. -265 gramme substance gave -298 gramme carbonic anhydride
and -053 gramme water.
Theory. L U. ni.
C, - 72 30-51 30-67
H, = 5 2-12 2'22
I - 127 63-81 53-73 63'68
O, ■> 32 13-66
236 100-00
The nambers agree with the formula C, II, 1 0,.
In preparing teriodorcin by the action of iodine protochloride on ordn,
it was observed that a comparatively large amount of the dilute solution
of iodine chloride could be added to the aqueous solution of orcin before
a permanent precipitate of teriodorcin was produced. It seemed possible
tliat an intermediate iodine derivative was first formed, far more soluble
than the teriodorcin, and which subsequently became converted into the
latter by the further action of the chloride of iodine. In order to as-
GertBin whether this was actually the case, a dilute solution of iodine
protodiloride was added to an aqueous solution of orcin containing one
part of orcin in fifty of wyter, as long as the precipitate redissolved in
the liquid on agitation. The addition of iodine was then stopped, and
the filtered solution agitated with ether. The ethereal solution, on
evaporation, left an oily nncrystoUizable liquid which was readily soluble
in water, and which evolved iodine when heated with concentrated sul-
phuric add : this liquid, on standing some days, deposited a few crystals
of unaltered ordn.
I cannot conclude this pi^ier without acknowledging the very efGdent
ud I have received from my aesbtant, Mr. Charles Edward Groves, in
oondnding this investigation.
56 On the Trafuformation of EUipie Functions. [Jan. 8^
III. '' A Memoir on the Transformation of Elliptic Functions/'
By Professor Caylby, F.R.S. Received November 14, 1878.
(Abstract.)
The theory of Transformation in Elliptic Functions was established by
Jacobi in the ' Fimdamenta Nova ' (1829) ; and he has there developed,
transcendentally, with an approach to completeness, the general case, n
an odd number, but algebraically only the cases n=3 and n=5 ; viz. in
the general case the formulae are expressed in terms of the elliptic func-
tions of the nth part of the complete integrals, but in the cases n=:3 and
n=:5 they are expressed rationally in terms of u and t; (the fourth roots
of the original and the transformed moduli respectively), these quantities
being connected by an equation of the order 4 or 6, the modular equation.
The extension of this algebraical theory to any value whatever of « is a
problem of great interest and difficulty. The general case should admit of
being treated in a purely algebraical manner; but the difficulties are so
great that it was found necessary to discuss it by means of the f ormulsB of
the transcendental theory, in particular by means of the expressions in-
IlK'\
volving Jacobi's q (the exponential of ^ i, or, say, by means of the
^•transcendants. Several important contributions to the theory have
since been made : — Sohnke, " Equationes Modulares pro transf ormatione
functionum EUipticarum," Crelle, t. xvi. (1836), pp. 97-130 (where the
modular equations are found for the cases n = 3, 5, 7, 11, 13, 17, & 19);
Joubert, '* Sur divers equations analogues aux Equations modulaires dans la
theorie des fonctions elliptiques,'* Comptes Eendus, t. xlvii. (1858),
pp. 337-345 (relating among other things to the multiplier equation for
the determination of Jacobi's M) ; and Konigsberger, " Algebraische TJn-
tersuchungen aus der Theorie der elliptischen Functionen," Crelle, t. Ixxii.
(1870), pp. 176-275; together with other papers by Joubert and by
Hermite in later volumes of the * Comptes Eendus,' which need not be
more particularly referred to. In the present Memoir I carry on the
theory, algebraically as far as I am able ; and I have, it appears to me,
put the purely algebraical question in a clearer light than has hitherto
been done ; but I still find it necessary to resort to the transcendental
theory. I remark that the case n= 7 (next succeeding those of the ' Fun-
damenta Nova '), on account of the peculiarly simple form of the modular
equation (1— u®Xl— v®)=(l— ut/)", presents but little difficulty; and I
give the complete formulsB for this case, obtaining them as well alge-
braically as transcendentally; I also to a considerable extent discuss
algebraically the case of the next succeeding prime value n=sll. For
the sake of completeness I reproduce Sohnke's modular equations, exhi-
biting them for greater clearness in a square form, and adding to them
those for the non-prime cases n=9 and n=15; also a valuable table
given by him for the powers of / (q) ; and I give other tabular results
jrlucli are oi asfiisiance in the theorv.
1874.] Mr. 0. Gore on Electratortion. 57
IV, " On Electrotorsion." By Geokqe GorEj F.R.S. Received
November 26, 1873.
(Abstract.)
This conuntmicatioii contains an account of a new phenomenon (of rods
and wires of iron becoming twisted while under the influence of elec-
tric curreats), and a full description of the conditioos under which it
occnrs, the necessary apparatus, and the methods of using it.
The phenomenon of torsicMi thus produced is not a microscopic ooe,
but may be made to exceed in some cases & twist of a qnarter of a circle,
the end of a suitable index moving through a space of 80 centimetres
(^31 inchefl). It is always attended by emission of sound.
The torsions ar© produced l^ the combined influence of helical and
axial electric currents, cme current passing through a long copper-wire
c(m1 surrounding the bar or wire, and the other, in an axial direction,
through the inn itsdf. The cause of them is the combined influence of
magnetism in the ordinary longitudinal direction induced in the bar by
Aie coil-current, and transverse magnetism induced in it by the axial
<xie.
The t<»«ions are remarkably symmetrical, and are as definitely related
in direction to electric currents as magnetism itself. The chief law of
tbem is — A, cMrrmt fiowing from a north to a soutA poU prodvea Uft'
handed tortwn, and a reverse one right-hattdtd tortion (i. e. in the direction
tA an ordinary screw). Although each current alone will produce its own
magnetic effect, sound, and internal mtJecular movement, neither alone
will twist the bar, unless the bar has been previously magnetized by the
other. Successive coil-currents alcme in opposite directions will not
produce torsicn, nmther will successive and opposite axial ones.
The torsions are influenced by previous mechanical twist in the iron,
by mechanical tension, and by terrestrial magnetic induction. The di-
rection of them depends both upon tiiat of the axial and of the coil-currents,
but appears to be determined most by the former. A few cases occur in
which the currents, instead of developing torsion, produce detorsion ; but
<Hily two instances, out of many hundreds, have been met with in which
torsicHi was produced in a direction opposite to that required by the law.
Single torsions vary in magnitude from 0*5 millim. te nearly 30 milBms.
of movement of the end of an index 47 centimetres long ; the smaller
ones occur when the two currents are transmitted alternately, and the
large ones when they are passed simultaneously ; the former generally
leave the bar in a twisted state, the latter do not. Thoee produced by
axial cnirents succeeding coil ones are nearly always much larger than
thoee yielded by coil-currents succeeding axial ones, because the residual
magnetism left by the coil-current is the strongest. The order of suc-
eesBi<m of tlie currents aSect« the torsions in all coses, altering their
magnitudes, and in srane few instances even their directions. In steel
58 Prof. J. Tyndall on the [Jan. 16,
all the torsional effects are modified by the mechanical and magnetic
properties of that substance.
Each current leaves a residuaiy magnetic eff^ in the bar, amounting
in iron to about one tenth of its original influence. The residuary mag-
netism of coil-currents is affected and sometimes reversed by axial ones ;
and that of axial currents is also removed by coil ones, and by a red heat.
The condition left by an axial current is smaller in degree and less stable,
in a vertical iron wire or one in the terrestrial magnetic meridian, than
that left by a coil one, partly because of the influence of terrestrial mag-
netism ; but in a position at right angles to that the effect is different.
The torsion produced by a coil-current may be used as a test, and
partly as a measure, of the residuary effect of an axial one ; and that
produced by an axial current may be employed to detect, and to Bome
extent measure, ordinary magnetism in the bar. As an opposite coil-
current at once reverses the ordinary longitudinal magnetism of a bar of
iron, so also an opposite axial one at once reverses its transverse mag*
netism.
Many instances have been met with in which the transverse and longi-
tudinal magnetic states produced by the two currents coexisted in the
same substance. The torsional influence of the excited helix is distri-
buted equally throughout its length ; so also is that of the current in the
bar. All the torsions are closely related to the well-known electric
sounds, and to particular positions and internal movements of the particles
of the iron.
Signs of electrotorsion were obtained with a bar of nickel, but not
with wires of platinum, silver, copper, lead, tin, cadmium, zinc, mag-
nesium, aluminium, brass, or German-silver, nor with a thick rod of
one, or a cord of gutta percha.
January 15^ 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The following Paper was read : —
I. " Preliminary Account of an Investigation on the Transmission
of Sound by the Atmosphere.'' By John Tyndall, D.C.L.,
LL.D., F.B.S. Received January 1st, 1874.
This notice embraces the scientific results of an inquiry on Fog-
signals, undertaken at the instance of the Elder Brethren of the Trinity
House, and communicated with their friendly concurrence to the Royal
Society.
The investigation was begun on the 19th of May, 1873, and continued
f/ll the 4th oi July. It was resumed on the 8th of October, and con«
1874.] TVofumwion of Sound by the Atmosphere. 59
tmued to the end of November. It also includes observBtiona made
durmg the dense fog wUch enveloped London on December 9 and the
eiicc«ediiig daya.
GongB and bdls were excluded from tbiB inveBtigation, in consequence
f4 their proved inferiority to other instruments of signalling. The experi-
ments were made with trumpets blown by powerfully compressed air,
with ateam-wIuBtles, guns, and a steam syren, associated with a trumpet
16 feet long.
Dsboll's h.{im, tff trumpet, had been highly spoken of by writers on
fog-aignals. A third-order apparatus of the kind had been reported as
sending its sonnd to a distance of from 7 to 9 miles against the wind,
and to a distance of 12 to 14 miles with the wind. Holmes had improved
uptm Dabdl ; and with two instruments of Holmes, not of the third but
of the first order, our experiments were made. On the 19th of May at
3 milee distance they became useless as a fog-signal ; at a distance of 4
miles, with paddles stopped and all on board quiet, they were wholly
unheard. At a distance of 2 miles from the Foreland the whistles tested
on May 19 became useless. The 12 o'clock gun, fired with a 1 lb. charge
at Drop Fort in Dover, was well heard on May 19, when the horns and
whistles were inaudible. On the 20th of May the permeability of the
atmosphere had somewhat increased, but the steam-whistle failed to pierce
it to a depth of 3 miles. At 4 miles the boms, though aided by quietness
on hoard, were barely heard. By careful nursing, if I may use the ex-
pression, the horn-sounds were carried to a distance of 6 miles. The
superiority of the 18-pounder gun, already employed by the Trinity House
as a fog-signal, over boms and whistles was on this day so decided as
almost to warrant its recommendation to the exclusion of all the other
signals.
Nothing occurred on the 2nd of June to exalt our hopes of the trumpets
and whistles. The horns were scarcely beard at a distance of 3 miles ;
sometimes indeed they faUed to be heard at 2 miles. By keeping every
thing quiet on board, they were afterwards heard to a distance of 6
milee — a result, however, mainly due to the improved condition of the
atmosphere. Considering the demands as to sound-range made by writers
on this subject, the demonstrated incompetence of horns and whistles of
great reputsd power to meet these demands was not encouraging. On
the 3rd of June the atmosphere had changed surprisingly. It was loaded
overhead with dark and threatening clouds ; the sounds, nevertheless,
were well heard beyond 9 miles. On June 10th the acoustic transparency
of the air was ^so very fair, the distance penetrated being upwards of 8|
miles. Thb subsidence of the sound near the boundary of the acoustic
shadow on the Dover side of the Foreland, and before entering tJie
shadow, was to-day sudden and extraordinary, affecting equally both
horns and guns. We were warned on June 3 that the supremacy of the
gun on OBB occasion by no means implied its supremacy on all occasions.
... .M oujn' was aL,^ain very ilr
I'lic sounds reached a inaxiiuuiu dislaiuv of ()_! iii
on n'turiiiuL,^ from the niaximiiin distaiici\ tliey \\<
;iv liad, as it were, darkened acoustically. On this da
irther their preeminence, and at OjJ miles were inferit
unds whatever reached Dover Pier on the 11th ; ai
is the close of the day that they succeeded in reach
Thus by slow degrees the caprices of the atmospher
known to us, showing us subsequently that within
le day, even within a single minute, the air, as a vehi<
^vent most serious variations. The 26th of June wac
lan its predecessor, the acoustic range being over 9|
Lon of the wind was less favourable to the sound on t
> preceding one, plainly proving that something else th
play an important part in shortening the sound-range,
the Istof July we experimented upon a rotating hon
'ect or axial blast, which proved to be the strongest, a
I miles. The soimds were also heard at the Yame
is 12| miles from the Foreland. The atmosphere 1
ily clearer acoustically, but not so optically ; for on thi
)scured the white cliffs of the Foreland. In fact, on
optical purity, the sound had failed to reach one tl
3 attained to-day. In the light of such a fact, any
)tieal transparency a measure of acoustic transparency, n
lusive. On the Ist of July a 12-inch American whistl
beard a highly favourable account, was tried in place of
whistle ; but, like its predecessor, the performance <
^nt fell behind that of the horns. An interval of 12 ho
rt the acoustically clear atmosphere of July 1 into
on the 2nd of July even ^^^^ ^'^ —
1 874.] TVantmuHon of Sound by the Atmotphere. 6 1
TiBiUe on the Ist, while the sounds were cut off at one aisth of the dis-
tsnce. At 2 tx, neither guns nor trumpets were able to pierce the
trukspuent ur to a depth of 3, hardly to a depth of 2 milea. This extraor-
dinary opacity was proved conclusively to arise from the irregular admix-
ture with the air of the aqueous vapour raised by a powerful sun. This
vapour, though perfectly invisible, produced on actmttie cloud impervious
to tiie sound, and from which the sound-waves were thrown back as the
waves of light are from on ordinary cloud. The waves thus refused trans-
mission produced by their reflection echoes of extraordinary strength and
duration. This I may remark is the first time that audible echoes have
been proved to be reflected from an optically transparent atmosphere. By
the lowering of the sun the production of the vapour was checkedi, and
the transmissive power of the atmosphere restored to such an extent tliat,
at a distance of 2 miles from the Foreland, at 7 p.m., the intensity of the
sound was at least thirty-six times its intensity at 2 f.u.
On October 8 the observations were resumed, a steam syren and a
Canadian whistle of great power being added to the list d inatnimenta.
A boiler had its steamraisedtoapresBureof 70 lbs. to the square inch; on
<^aing a valve this steam would issue forcibly in a continuous stream,
and tiie sole function of the ayren was to convert this stream into a
series of separate strong pufEs. This was done by causing a disk with
12 radial slits to rotate behind a fixed disk with the same number of slits.
When the slits coinddad a puff escaped ; when they did not coincide the
outilow of steam was interrupted. Each puff of steam at this high pres-
sure generated a sonorous wave of great intensity ; the successive waves
linking themselves together to a musical sound so intense as to be best
described as a continuous explosion.
During the earlier part of October 8 the optical transparency of the
air was very great ; its acoustic transparency, on the other band, was very
defective. Clouds blackened and broke into a rain- and hail-shower of
tropical violence. The sounds, instead of being deadened were improved
by this furious squall ; and, after it had lightened, thus lessening the
local noises, the sounds were heard at a distance of 7^ milea distinctly louder
than they had been heard through the preceding rainless atmosphere at a
distance of 5 miles. At 5 miles distance, therefore, the intensity of the
sound had been at least doubled by the rain — a result entirely opposed to
all previous assertions, but an obvious consequence of the removal by con-
densation and precipitation of that ^-apour the mixture of which with the
sir had been proved so prejudicial to the sound. On this day a depen-
dence vaa estaUished between the pitch of a note and its penetrative
power — the syren generating 480 waves being slightly inferior to the
horns, while generating 400 waves a second it was distinctly superior.
The mK-rimnm TSnge On October 8 was 9 miles. On October 9 the trans-
e power had diminished, the Tntnimum range being 7j miles. On
62 Prof. J. Tyndall on the [Jan. 16,
both these days the syren proved to be superior to the horns, and on some
occasions superior to the gun.
On the 10th and 11th, a gale having caused our steamer to seek safely
in the Downs, we made land-observations. The duration of the aerial
echoes was for the syren and the gun 9 seconds, for the horns 6 seconds.
The duration varies from day to day. We sought to estimate the influence
of the violent wind, and found that the sound of the gun failed to readi
us in two cases at a distance of 550 yards to windward, the sound of
the syren at the same time rising to a piercing intensity. To leeward
the gun was heard at five times, and certainly might have been heard
at fifteen times the distance attained to iidndvi'ard. The momentary
character of the gun-sound renders it liable to be quenched by a single
puff of wind ; but sounds of low pitch generally, whether momentary
or not, suffer more from an opposing wind than high ones. We had on
the 13th another example of the powerlessness of heavy rain to deaden
BOimd.
On the 14th the maximum range was 10 miles, but the atmosphere
did not maintain this power of transmission. It was a day of extreme
optical clearness ; but its acoustic clearness diminished as the day ad-
vanced. In fact the sun was in action. We proved to-day that by
lowering the pitch of the Canadian whistle, its sound, which had pre-
viously been inaudible, became suddenly audible. The day at first was
favourable to the transmission of the longer sound-waves. After a
lapse of three hours the case was reversed, the high-pitched syren being
then heard when both gun and horns were inaudible. But even this
state of things did not continue, so rapid and surprising are the caprices
of the atmosphere. At a distance of 5 miles, at 3.30 p.m., the change
in transmissive power reduced the intensity of the sound to at least
one half of what it possessed at 11.30 a.m., the wind throughout main-
taining the same strength and direction. Through all this complexity
the knowledge obtained on July 3 sheds the light of a principle whidi
reduces to order the apparent confusion.
October 15 was spent at Dungeness in examining the performance of
DabolFs horn. It is a fine instrument, and its application was ably
worked out by its inventor ; still it would require very favourable atmo*
spheric conditions to enable it to warn a steamer before she had come
dangerously close to the shore. The direction in which the aerial echoes
return was finely illustrated to-day, that direction being always the one
in which the axis of the horn is pointed.
The 16th was a day of exceeding optical transparency, but of great
acoustic opacity. The maximum range was only 5 miles. On this
day the howitzer and all the whistles were clearly overmastered by i^e
syren. It was, moreover, heard at S^ miles with the paddles going,
while the gun was unheard at 2^ miles. With no visible object thi^;
1874.] TVtttumuMon of Sound by the Atmotpkere. 63
eoold possiblf yield on echo in sight, the pure aerial echoee, coming
fimti the more distant southern ur, were distinct and long-continaed at
• distance of 2 miles from the shore. Near the base of the Foreland
cliff we determined thdr duration and found it to be 11 aeconda, while
that of tlie best whistle echoes was 6 seconds. On this dav three
whistles, sounded simultaneously, were pitted against the syren, and
found clearly inferior to it.
On the 17th four hmns were compared with the syren and found
inf^Hxr to it. This was our day of greatest acoustic transparency, the
•onnd reaching a maijmum of 15 miles for the syren, and of more than
16 for the gun. The echoes on this day were continued longer than on
any oUier occaaion. They continued for 15 seconds, their duration
indicating the atmospheric depth from which they came.
On October 18, though the experiments were not directed to deter-
mine the transmissive power of the air, we were not without proof that
it continued to be high. From 10 to 10.30 a.K., while waiting for the
blasts of the syren at a distance of 3 miles from the Foreland, the con-
tinned reports of what we supposed to be the musketry of skirmishing
parties <m land were distinctly heard by us all. We afterwards learned
that the sounds arose from the rifle-practice on Kingsdown beach,
fi j miles away. On July 3, which, optically considered, was a far more
perfect day, the I8-pounder, howitser, and mortar failed to make them-
aelves'heard at half this distance. The 18th was mainly occupied in
determining tiie influence of pitch and pressure on the syren-sound.
Taking the fluctuations of the atmosphere into account, I am of opinion
that the syren, performing from 2000 to 2400 revolutions a second, or,
in otlier wcffds, generating from 400 to 480 waves per second, best meets
tiie atmospheric conditions. We varied the pressure from 40 to 80 lbs.
on the square inch ; and though the intensity did not appear to rise in
proportion to the pressure, the higher pressure yielded the hardest and
most penetrating sound.
The 20th was a rainy day with strong wind. ITp to a distance of
5j miles the syren continued to be heard through the sea- and paddle-
noises. In rough weather, indeed, when local noises interfere, the syren-
■onnd &r transcends all otiier sounds. On various occasions to-d&y it
proved its mastery over both gun and horns. On the 2lBt the wind
was strong and the sea high. The hom-sounds, with paddles going,
were lost at 4 miles, while the syren continued serviceable up to 6^ miles.
The gan to-day was completely overmastered. Its puffs were seen at the
Foreland ; but its sonnd was nnheard when the syren was distinctly heard.
Heavy rain Euled to damp the power of the syren. The whistles were
also tried to-day, bat were found far inferior to the syren. On the 22nd
it blew a gale, and the 'Oalatea' quitted us. We made observations
on land tm the influence of the wind and of local noises. The shelter
of the Cowtgnard Station at Comhill enabled us to hear gun-sounds
64 Prof. J. Tyndall on the [Jan. 15,
which were quite inaudible to an observer out of shelter ; in the shelter
also both horn and syren rose distinctly in power ; but they were also heard
outside when the gun was quite unheard. As usual the sound to lee-
ward was &r more powerful than those at equal distances to windward.
The echoes from the cloudless air were to-day very fine. On the 23rd,
in the absence of the steamer, the observations on the influence of the
wind were continued. The quenching of the gun-sounds, in particular, to
windward was well illustrated. All the sounds, however, gun included,
were carried much further to leeward than to windward. The eff^ of a
violent thunderstorm and downpour of rain in exalting the sound was
noticed by observers both to windward and to leeward of the Foreland.
In the rear of the syren its range to-day was about a mile. At right
angles to the axis, and to windward, it was about the same. To lee-
ward it reached a distance of 7^ miles.
On the 24th, when observations were made afloat in the steam-tug
* Palmerston,' the syren exhibited a clear mastery over gun and horns.
The maximum range was 7| miles. The wind had changed from W.S.W.
to S.E., then to E. As a consequence of this, the syren was heard loudly
in the streets of Dover. On the 27th the wind was E.N.E. ; and ihe
syren-sound penetrated everywhere through Dover, rising over the moan-
ing of the wind and all other noises. It was heard at a distance of
6 miles from the Foreland on the road to Folkestone, and would probably
have been heard all the way to Folkestone had not the experimento
ceased. Afloat and in the axis, with a high wind and sea, the syren,
and it only, reached to a distance of 6 miles ; at 5 miles it was heard
through the paddle noises. On the 28th further experiments were made
on the influence of pitch, the syren when generating 480 waves a
second being found more effective than when generating 300 waves a
second. The maximum range in the axis on this day was 7j| miles.
The 29th of October was a day of extraordinary optical transparency
but by no means transparent acoustically. The gun was the greatest
sufferer. At flrst it was barely heard at 5 miles ; but afterwards it was
tried at 5|, 4^, and 2| miles, and was heard at none of these distances.
The syren at the same time was distinctly heard. The sun was shining
strongly ; and to its augmenting power the enfeebiement of the gun-
sound was doubtless due. At 3| miles, subsequently, dead to windward,
the syren was faintly heard ; the gun was unheard at 2^ miles. On land
the syren and horn-sounds were heard to windward at 2 to 2j| miles, to
leeward at 7 miles ; while in the rear of the instruments they were heard
at a distance of 5 miles, or five times as far as they had been heard
on October 23.
The 30th of October furnished another illustration of the fallacy of
the notion which considers optical and acoustic transparency to go hand
in hand. The day was very hazy, the white cliffs of the Foreland at the
greater distances being quite hidden ; still the gun- and syren-sounds
1874.] TVatumuaioa of Sound by the Atmosphere. 65
reached on the bearing of the Vame light-vesael to a distance of 11^
miles. The ayren was heard through the paddle-noises at 9j miles,
while at 8 j miles it became efficient as a signal with the paddles going.
The homs were heard at 6^ miles. This was during calm. Subsequently,
with a wind from the N.N.W., no sounds were heard at BJ miles. On
land, the wind being across the direction of the sound, the sjren was
heard only to a distance of 3 miles N.K of the Foreland ; in the other
direction it was heard plainly on Folkestone Pier, 8 miles distant.
Both gun and homs fiuled to reach Folkestone.
Wind, rain, a rough sea, and great acoustic opacity characteiiied
October 31. Both gun and homs were unheard 3 miles away, the
syren at the same time being clearly heard. It afterwards forced its
sound with great power through a violent rain-squall. Wishing the
same individual judgment to be brought to bear upon the sounds ou both
sides of the Foreland, in the absence of our steamer, which had quitted
ufl for safety, I committed the observations to Mr. Douglass. He heard
them at 2 miles on the Dover side, and on the Sandwich side, with the
same intensity, at 6 miles.
A gap (employed by the engineers in making arrangements for pointing
the syren in any required direction) here occurred in our observations.
They were resumed, however, on November 21, when comparative es-
peiiments were made upon the gun and syren. Both BOurcea of sound,
when employed as fc^-signals, will not unfrequently have to cover an are
of 180° ; and it was desirable to know with greater precision how the
■ound is affected by the direction in which the gun or syren is pointed.
The gun, therefore, was in the first instance pointed on us and fired,
then turned and fired along a line perpendicular to that joining Ua and it.
There was a sensible, though small, difference between the sounds which
reached us in the two cases. A similar experiment was made with the
ayren ; and here the falling off when the instrument was pointed perpen-
dicular to the line joining us and it was very considerable. This is what
is to be expected ; for the trumpet associated with the syren is expressly
intended to gather up the soimd and project it in a certain direction, while
no such object is in view in the construction of the gun. The experi-
ments here referred to were amply corroborated by others made on
November 22 and 23.
On both of these days the ' Qalatea'a ' guns were fired to windward
and to leeward. The aerial echoes in the latter case were distinctly louder
and longer than in the former. The experiment has been repeated many
times, and alwa^ with the same result.
In front of the Comhill Coastguard Station, and only 1 j mile from
the Foreland, the syren, on the 2lBt, though pointed towards us, feU
suddenly and considerably in power. Before reaching Dover Pier it had
ceased to be heard. The wind was here against the sound ; but this,
though it contributed to the effert, could not account for it, nor could the
66 Prof. J. Tyndall on the [Jan. 16>
proximity of the shadow account for it. To these two causes must have
been added an acoustically flocculent though optically transparent atmo-
sphere. The experiment demonstrates conclusively that there are atmo-
spheric and local conditions which, when combined, prevent our most
powerful instruments from making more than a distant approach to the
performance which writers on fog-signals have demanded of them.
On November 24 the sound of the syren pointed to windward ^i-as com-
pared at equal distances in front of and behind the instrument. It was
louder to leeward in the rear, than at equal distances to windward in front.
Hence, in a wind, the desirability of pointing the instrument to wind-
ward. The whistles were tested this day in comparison with the syren
deprived of its trumpet. The Canadian and the 8-inch whistles proved
the most effective ; but the naked svren was as well heard as either of
them. As regards opacity, the 25th of November almost rivalled the
drd of July. The gim failed to be heard at a distance of 2*8 miles, and
it yielded only a faint crack at 2^ miles.
Meanwhile this investigation has given us a knowledge of the atmo-
sphere in its relation to sound, of which no notion had been previously
entertained. While the velocitij of sound has been the subject of refined
and repeated experiments, I am not aware that since the publication of a
celebrated paper by Dr. Derham, in the Philosophical Transactions for
1708, any systematic inquiry has been made into the causes which affect
the inUiisUy of sound in the atmosphere. Derham^s results, though
obtained at a time when the means of investigation were very defective,
have apparently been accepted with unquestioning trust by all subsequent
writers — a fact which is, I think, in some part to be ascribed to the a
priori probability of his conclusions.
Thus Dr. Bobinson, relying apparently upon Derham, says, " Fog is a
powerful damper of sound,'' and he gives us physical reason why it must
be so. " It is a mixture of air and globules of water, and at each of
the innumerable surfaces where these two touch, a portion of the vibration
is reflected and lost.** And he adds further on, '^ The remarkable power
of fogs to deaden the report of guns has been often noticed."
Assuming it, moreover, as probable that the measure of " a fog's power
in stopping sound '' bears some simple relation to its opacity for light.
Dr. Bobinson, adopting a suggestion of Mr. Alexander Cimninghamy
states that *' the distance at which a given object, say a flag or pole, dis-
appears, may be taken as a measure of the fog's power " to obstruct the
sound. This is quite in accordance with prevalent notions ; and granting
that the sound is dissipated, as assumed, by reflection from the particles
of fog, the conclusion follows that the greater the number of the reflecting
particles, the greater will be the waste of sound. But the number of
particles, or, in other words, the density of the fog, is declared by its
action upon light ; hence the optical opacity will be a measure of the
aroustic opacity.
1 874. ] TVaiumutuM of Souad by the Aimoiphgre. 67
Thia, I »7, aipreBieB tho opinion generally entertuned, " clear itill
air" being regarded as the best vehicle for sound. We have not, u
stated above, experimented in really deiiae fogs ; but tlie experiments
actnally^made entiralj destroy the notion that clear weather is necessarily
bettv for the tnuisnussion of sound than thick veather. Some of our
days of densest acoustic opacity have been marvellously clear optically,
while some of our days of thick haze have shown themselves highly
favoorable to the transnuBsiou of sound. Were the physical cause of the
aonnd-waat« that above assigned, did tiiat waste arise in any material
degree from reflection at the limitiug surfaces of the particles of hace,
this result would be inexplicable.
Aguo, Deriiam, as quoted by Sir John Herschel, says that " falling
rain tend/r powerfully to obstruct sound." We have had repeated reversals
of tJiis ooQclusion. Some of our observations have been made on days
when rain and hail descended with a perfectly tropical fury ; and in no
ain^ case did the rain deaden the sound ; in every case, indeed, it had
predaeiy l^e opposite effect.
But falling snow, according to Derham, offers a more serious obstacle
than any other meteorological agent to the transmission of sound. We
have not extended gur observations at the South Foreland into snowy
weather ; but an observation of my own made on December 29th, in the
Alps, during a heavy snow-storm, distinctly negatives the statement of
Derham.
Beverting to the case of fog, I am unable in modem observations to
discover any thing conclusive as to its alleged power of deadening sound.
I had the pleasure of listening toa very interesting lecture ou fog-signals
delivered by Mr, Beaceley before the United-Service Institution ; and I
have carefully perused the printed report of that lecture, and of a paper
previously communicated by Mr. Beazeley to the Institution of Civil
Kigineers. But in neither of these painstaking compilations cau I find
any adequate evidence of the alleged power of fogs to deaden sound.
Indeed during the discussi<m which followed the reading of Mr. Bea«e-
le/s paper, an important observation in an opposite sense was mentioned
by Mr. Douglass, to whose ability and accuracy as an observer I am able
to bwr the strongest testimony. Mr. Douglass stated that he had found
in his experience but Uttle difference in the travelling of sound iu foggy
ta in dear weather. He bad distinctly heard in a fog, at the Smalls rock
in dke Briatot Channel, guns fired at Mdford Uaveu, 25 miles away. Mr.
Beaseley, moreover, has heard the Lundy-Island gun " at Harttand Point,"
a diataaoe of 10 miles, during dense fog. Mr. Beazeley'a conclusion,
indeed, accurately expresses the state of our knowledge when he wrote.
In winding up his paper, he admitted "that the subject appeared to be
Tery little known, and that the more it was looked into the more
qipareut became the fact that the evidence as to the effect of fog upon
■wind is ezlMmely conflicting.'' When, therefore, it is alleged, as it is
TOL. xxn. o
.....^ luiDKUtv orten occiii
optical tranHpan'Ticv. Any systiMn o\^ nicnsinvs,
the assumption that theopticaTid a-'oustic transpai
go liaiul in liand imist prove delusive.
There is but one solution of this difficulty : it is
sound 89 powerful m to be able to endure loss bj
still retain a sufficient residue for transmission. C
hitherto examined bj us the syren comes nearest U.
condition ; and its establishment upon our coasts
prove an incalculable boon to the mariner.
An account of the observations made during the
eluded in the paper shortly to be presented to \
obseryationB ^d the force of demonstration to
the paper, that fogs possess no such power of st:
hitherto ascribed to them. Indeed the melting a
cember 13th was accompanied by an acoustic darkc
sphere, so great that, at a point' midway between the
Serpentine, where a whistle was sounded, and the bri(
sessed less than one fourth of the intensity which it p
of densest fog.
Thus, I think, has been removed the last of a conge
for more than a century and a half have been associa
mission of sound by the atmosphere.
January 22, 1874,
JOSEPH DALTON HOOKER, C.B., Preside
The following Paper was read : —
\. ^'On the Nature anH T)^-
• 1
1874.] PoiaoH of Indian Venomous Snaket. 69
eolubrioe stukes, whilst thai of Daboia RtuuUii is aimll&r to that of E<shi»
eaniuUa, and kIho of the Trvtttertauri, which represent the Tiperine snakes
in India.
Jnst Bs the Ntga may be regarded on among the most virulent of the
colubrine, the Daboia is probablj as venomous as any of the viperine
snakes, it being very deadly ; whilst the Crotalidffl are but feebly repre-
sented in India by the Tfimereturi,
The venomonB colubrine snakes in India are represented by the Naja
tripudiani, OpAiopAcu/iu tlaps, Bungarus ftueiatiu, B. emruieiu, Xenure-
lop* bmtffaroida, and the Tarious spedes of Cnllophi* and Hydrophids ;
whilst among the viperine snakes the Viperids, or vipers, are represented
in India by only two genera, each with a single species, Daboia RutteUU,
BMi earimUa ; the CrotaUdie, or pit vipers, by the various Trimereiuri,
Pdtopthr, Saly», ffyptude, though these are much less active than their
American congeners.
The Daboia, however, may be considered as virulent as the most deadly
form of the Viperids of Africa, or probably as the Cmtalut or Oratpedoct-
phdlui of the pit-vipers of America and the West Indies.
In a previous commonication we have described the effect of the poison
of ilToja iripudian» upon warm-blooded animals, and have illustrated it
by e^OTiments on ttte dog, rabbit, guineapig, and fowl.
We purpose in the present paper to compao^ its action with that of the
poison of the Daboia BuaadUi, a viperine snake, to describe its effects
npon cold-blooded animals and invertebrats, and to examine in detail its
action upon the varioas organs of the body.
In onr former paper we stated that the general symptoms of pcusoning
by cobr»-veDom are depression, funtneas, hurried respiration and exhaus-
tion, lethargy, nnconscionsness, nausea, and vomiting. In dogs, guinea-
pigs, and rabbits peculiar twitching movements occur, which seem to re-
present vomiting in them; occasionally, in fact, dogs and guineapigs
(Experiment XX.) do vomit, and dogs are profusely salivated. As the
poisoning proceeds, paralysis appears, sometimes affecting the hind 1^
first and seeming to creep up the body, and sometimes affecting the whole
animal nearly at the same iime. There is loss of coordinating power
frf ^ mnsdea of locomotion.
Hsmorriiage, relaxation of the sphincters, and involuntary evacuatioQa,
not nnfrequently of a sanguineous or muco-sanguineous character, often
precede death, and are generally accompanied by convulsions.
In fowls the appearance is one of extreme drowsiness ; the head falls
forward, rests on tiie beak ; and gradually the bird, no longer able to
support itself, crouches, then rolls over on its side. There are frequent
startings, as if of sudden awaking from the drowsy state.
The following experiments upon pigeons and guineapigs show that the
general symptoms produced by the poison of the Daboia are nearly the
same ae by that of tiie Naja. The local symptoms are greator extravasatioa
70 Messra. T, L. Bruntoii and J. Fayrer on the [Jan. 22,
of blood and effusion iuto areolar tissue. In Experiment LU. it was noted
that gre-ater lethargy and less violent conviUsioos occurred in tlie pigeon
poisoned bv cobra-veoom than in that poisoned by Dahoia ; but this might
readily be duo to individual difference in the bird ; and an opposite result
is noted in Experiment VII. upon agnineapig. In one pigeon, killed by
BaJioia-venom, the blood remained permanently fluid after death ; but in
the other, and also in the guineapigs, it coagulated tirm.ly. This is an excep-
tion to the rule which has been noticed in experiments made in India,
that the blood after fttftdin-poiaoning remains fluid — La marked contradi-
stinction to death from cobra-renom, in which the blood almost invariably
coagulates. Coagulation, however, of the blood of a fowl aft«r death from
the bite of a Daboia has also been noticed by one of us (Dr. Fayrer) in
India ; and therefore the coagulation in our eiperiments was not due to
the lower temperature of the atmosphere.
Eaptmnoit I,
Aoffiist 27ih, 1873. — Three milHgrammes of dried flaioin-poison,
ceived some weeks ago from Balasore, were injected into the thigh o£
old and vigorous pigeon at 2.48,
2.53. No apparent effect, eic«pt that the bird is lame on that leg,
3.2, The bird Ja sluggish, Eespiratious hurried. Lameness con-
tinues.
3.18. Still sluggish, bat it is not deeply affected.
3.30. Disinclined to move. When placed on the table it sunk on its
breast. No nodding ot the head.
3.45, Sudden and liolont conmlsions.
3.46. Dead in 5S minutes from the time of injection.
Electrodes inserted into the spinal cord soon after death caused movo-
ments of the wings, hut not of the legs. Blood taken from the bird, just
before death, partially coagulated after death. Blood token from it after
death, coagulated more firmly— but less Knnly than some taken from
another pigeon poisoned with cobra- venom.
Ej^periment U,
A young full-grown pigeon had 3 milligrammes of dried floio ia-poiaon
injected into the peritoneum at 3,5 f.u.
At 3.13 it was observed to pass suddenly into \iolent convulsions, flap-
ping its wings strongly. It continued in this state for a minute : and at
3.14 it died, 0 minutes after the injection.
Electrodes inserted into the spinal cortl, in the neck, caused violent
muscular contractions all over the wings and legs. The cord was thus
evidently not paralyzed; but its irritability soon ceased. The blood
remained permanently fluid, and become bright red on exposure to air :
under the microscope (400 diameters) the corpuscles seemed normal.
Bigor mortis came on.
1874.] Poison a/ Indian Venomom Snakes. 71
Experiment III.
A fall-^rown yotutg pigeon had 3 milligrammes of dried cobnt-poLflon
injected into the thigh at 2.49 f.M.
2.53. The respiratioa ia reiy hurried; the bird presents a sluggish
appearance and b^ins to droop.
3.2. The eyes are now closed and the bird ia crouching ; legs extended.
3.6. ConTulsions ; head and back resting on the ground ; legs extended
wid paralysed.
3.10. Dead in 21 minutes from the injection.
Sectrodes inserted into the cord soon after death caused general coa-
'bvctions of the extremiti^, showing that the cwd was not paralyzed.
Its irritability soon disappeared. The symptoms in this bird are different
from those in the one poisoned by Daboia-viraa ; there is more lethargy,
nodding of &e head, and apparent drowsiness before the convulsions,
which are not so sudden or bo violent.
Ej^erimeat IV.
A. fall-grown pigeon had 3 milligrammes of dried cobra-poison injected
into the peritooenm at 3.6 p.ii.
3.15. The bird is sluggish, nodding its head.
3.17. Qaping ; the head is twitching, and the bird can hardly stand.
3.22. Coavolsitms. Several grains of Indian com are vomited.
3.25. Quite paralyzed. C<mTulsi<ais.
3.26. Dead in SI minutes Eroot the injection.
Electrodes in the cord bomi after death caused movements in the limbs.
The irritabiKty rapidly disappeared, and at 3.33 was entirely gone.
The blood coagulated firmly after death.
When examined after death with a magnifying-power of 400 diameters,
crenation of etune of the red COTpuscles was observed, but no other change
Avas noticed.
Experiment T.
Febrwtrif 11th. — About j-1 cuMc c«itimetre of a mixture of Dahoia-
poiaon with alcohol (1 part poison with 4 of alcohol) was injected into
the left thigh of a small gnineapig at 1.45fj(.
Immediately afterwards it becune very restless, and the nose began to
be twit«ihed inwards towards the breast.
1.48. The left leg drags somewhat.
1.54. The hind legs are jerked backwards r^ularly every few seconds.
1.55. It bites at its left 1%.
1.58. It has drawn itself tt^ether almost into a ball.
2.2. The twitching still continues.
2.23. Its hind quarters have become nearly paralyzed. It lies ou its
side, and convulsive movements occur from time to time.
2.28J. It is apparently dead. The heart continues to beat strongly.
72 Messrs. T. L. Brunton and J. Fayrer on the [Jan. 2St,
On opening it the lungs were slightly congested. Feiistaltie mov&*
ments of intestine active. The blood from the heart was allowed to nm
into a clean beaker. It was of a dark colour, but became red on expo-
sure to air. It shortly afterwards coagulated and formed a fiim dot.
Experimtnt VI,
February 11. — ^About 1 cubic centimetre of Z)a^ui-poison (1 part poison
mixed with 4 parts of alcohol) was injected under the skin of the left
thigh of a guineapig at 1.13.
1.17. Animal rubbing its mouth >^ith its fore paws. It is restless and
moves about. There are slight twitchings, and it sits on its hind legs
like a cat.
1.22. Very restless.
1.27. Head is drawn towards legs in a t>^itching fashion. Animal
bites at the left leg. When it moves about, the left leg drags somewhat.
1.45. Has been very quiet and disinclined to move for some time.
1.55. About 1 cubic centimetre more was injected into the right thig^
1.56. Both hind legs drag slightly.
1.58. The animal is very imsteady and tottering on its 1^.
2.2. Both hind legs completely paraljrzed, and, when the animal draws
itself forward \^dth its fore paws, the hind legs trail out behind it. There
are twitchings of the fore part of the body.
2.17. Hind legs and loins quite paralysed. The posterior part cxf tbe
body lies flat on the ground, the abdomen being flattened out upon it.
Paralysis seems gradually extending to the fore limbs. There is general
twitching. It tries to crawl, but cannot drag itself forward, though it can
still move the fore legs. Gnaws the bottom of the box in which it lies.
2.20. Almost motionless. Eye is still sensitive. Fluid has issoed
from the mouth. The animal can still move its head.
2.23. Convulsive movements.
2.24. Cornea insensible. Weak twitches of the trunk still occasionally
occtur ; they seem to be of the nature of respiratory movements. Heart
beats strongly.
In a minute or two afterwards the animal was opened. The heart was
irritable and contracted when touched. The ventricle did not contract
unless touched. The auricles were beating. The lungs were (I think)
slightly congested. Blood from the large trunks in the thorax was col-
lected in a vessel ; it was of a dark colour ; on exposure to air it became
bright red and formed a firm coagulum. Peristaltic movements of the
intestine were observed.
Ejcpervment VII.
February 11/7*. — About j| a cubic centimetre of milky-looking cobra-
poison was injected into the right thigh of a guineapig of moderate sise
at 2*20. It became restless immediately, and the hind legs began to
1874.] PouoH of ImSan Venomoiu Snaket. 73
twitch backwards. SborUy afterwards it again became quiet and sat
quite BtiU.
3.12. The animal did not seem to be much afFected by the ptHson.
Some more injected into left thigh.
4. Both hind legs became paralysed, and the animal lay with them
spread out behind it. The hind part of the body also sank down, so that
the abdmnen became flattened on the floor, just as with the AiAoto-poison.
4.23. Conrulsive twitches occur. The animal lies on its side. It is
more convulsed than the one killed with 2)a6oia-poison.
Action of Cobra-poison on Frogs.
"Wbea cobra-pmBon is injected under the ikin of frogs they occasionally
become very restless immediately after the injection. This, howmet, is by
no means ^waye the case ; and as similar agit&tion occurs, often to a much
greater extent, after the injection of other aubst«nces, it is to be attributed
rather to the insertion of the needle than to the action of the venom. A
gradually increasing torpor then comes over the animal, sometioies begin-
ning some time after the injection, and then proceeding uninterruptedly, at
other times being interrupted by occasional movements. The limbs are
drawn dose up to the body, and the head gradually sinks down between
tite hands in most instances; but sometimes, as in Experiment VIII., the
bead is held at first much more erect than usual. The power of motion
IB lost before that of sensation ; for the movemente caused by painful
Btamuli bectRue weaker and weaker, although they may still follow each
application of the irritant. The progressive weakness is well shonn in
the movements erf the hind legs. After the frog has sunk down and is
lying flat npon the table, pinching the toes causes it to kick vigorously ;
but by-and-by, instead of kicking, it merely draws away the foot from
the irritant with a slow wriggling motion. If it is then lifted up from
the table, so as to remove the resistance occasioned by friction, the wrig<
gUng cmtiTely disappears, and the foot is promptly and easUy drawn up
to the body when pinched. This weakness seems to depend on the
nervous system rather thm on the muscles ; for, even in this state of ap-
parent paralysis, the animal occasioni^y displays considerable muscular
power, and is able to spi^ng to a considen^le height, as in the following
experiment. A similar condition is sometimes observed in warm-blooded
animals, as in Experiment LX, The motor paralysis increases, no motion
follows the application of any irritant, however powerful ; but even then
sensation exists, as is seen from Experiment LXXVL The heart continues
to beat after all motion in the body has ceased ; but its pulsatioDS become
gradually slower, and at last cease altogether.
Experivitttt VIU.
Septtmhtr 12A, 1873. — Three frogs of nearly equal size were selected,
and a dose of dried cobra-poison dissolved in wat«r was injected into the
74 Messrs. T. L. Bninton and J. Fayrer on the [Jan. ^%f
dorsal lyinph-sac of each. The quantity injected into No. 1 was ratunatej
to be equal to three or four drops of the fresh poison, that into No. T
about a drop, and into No. 3 about half a drop. These estimateB, how^
ever, are not to he absolutely depended on.
The injection was made int^i ail three about 3 p.ii.
3.17. Nofi, 1 and 2 are sitting with the head much more erect than oioA
and the belly depressed. No. 3 has the head depressed between the f<nn
pawa.
3.22. Ko, 3 is now sitting up in the normal posture.
4. No. 1 lies quite quiet; when moved ils limbs give a slight wriggb,
Applied strong acetic acid to its legs : after many seconds it gave a ftui^
wriggle. No, 2 also lies quiet. "When its legs are pulled bock it »
still wriggle them up towards its body. When held up it can kick, well
After being placed on the table it suddenly, and without any appc
reason, sprung up to a considerable height. No. 3 presents the a
appearance as No. 2, but seems more paraljied.
4,5. No. 1 does not react at al! to any painful stimulus. Nob, 2
3 wiigglo their legs when pinched. The observation was now disi
tinned. Next morning all three were dead.
Aeiion on Lixards.
The action of cohra-poison upon lizards seems very similar to that
which it has upon frogs ; the animal becomes sluggish and difficult
to rouse ; and the bitten part is affected by paralysis, so that, if a limb
has been thus wounded, it is dragged by the animal. The paralysis
aftcniards extends to the rest of the body, and death ensues. Experi-
ments on this subject have been recorded by one of us (Dr. Fayrer) in
the ' I'hanatophidia of India.'
Effect of Herpeiit-veitom on Sna/ca.
The bite of venomous serpents, such as the cobra, IkAoia, and Bun-
garui, generally proves fatal to innocuous serpents, but not always. The
occasional escape of the latter is probably due to the quantity of poison
absorbed having been small, either absolutely, or relatively to the sise of
the bitten snake. The effect of the size of the innocuous snake upon the
time required by the poison to produce a fatal effect is illustrated by
experiment/, in which a small rat-snake was killed by the bite of a Bwi^
ganu ertruUxit (less poisonous than a cobra) in 7 hours 17 minutes, while
a large snake of the same species was not killed by the bite of a cobrm
till ^ter about 36 hours (experiment a); and another still larger one
was unaffected by the cobra-venom (experiment g). Venomous snakes
are not generally affected either by their own poison or that of another
. sort of snake, no lees than 15 drops of venom having been injected hypo-
keruiically into a cobra (Experiment r) without effect; but small ones
1874.] Potion 0/ Indian Venomoui Snaket. 75
are oocaBitmaUf killed by large iudividuBk belonging either to the same
or to a different species *.
The Bymptoms caused by the poison were the Bune in both the inno-
cuooB and the Tenomoue snakes killed by it, and cooaistod chiefly of slug-
gishness and indisposition to move, which probably signifies in the snake,
as it does in the frc^, a progressive paralysis. Only in experiment h
were convnlsiTe movements noticed. The movements of the tail in ex-
periment e, after motion had ceased in every other part of the body, are
remariuble.
The poisonons addon of the venom of the cobra, Daboia, and Bungarua
upon iunocuoos snakes is shown in the following experiments selected
from a number recorded in the ' Thanatophidia of India : ' —
Exp. o,— JtfarcA lOlh, 1868. — A rat-anake (Ptyat ntueosa), about 6 feet
in length, was bitten by a large cobra at 12.S4. Before closing the
snake's jaws on the part the sc^es were scraped off. Blood was freely
drawn by the snake's fangs from bites inflicted in two places.
1.8 pjc. Appears sluggish ; wound bleeding freely.
1.16. Perfectly active, and moves about rapidly in the cagei
1.36. No chai^.
There was no apparent change in the snake all that day or the next,
except that it may have been a little more sluggish. It died in the
night of the 11th, being found dead on the morning of the 12th.
Exp. b. — A small grass-snake (Tropidonotva qaineuneialua) was bitten
by a cobra at 1.12 p.k.
1.11. Very sluggish.
1.20. Tosses its head about in a convulsive manner.
1.25. Dead 13 minutes after the bite.
Exp. e. — Two tree-snakes {Dfndrophis picta), one about 3 feet 4 inches
long, and the other somewhat smaller, were bitten by a cobra.
1.7. The larger snake bitten. .
1.8. The smaller one bitten.
1.12. Both sluggish.
1.16. The sm^ler snake dead 7 minutes after the bite.
1.16. The lai^ier one dead 9 minutes after the bite.
They simply seemed to become sluggish and powerless ; there were no
convulsians, no writhings or ccmtortions. After they had appeared quite
dead for a moment or two, the tail of each moved slightly.
Exp. d. — A green whip-snake {PaaKrila mi/eteriiarts), more than 3 feet
long, was bitten by a cobra about 10 inches from the head, at 12.37 p.m.
12.38. Sluggish, moves less actively ; gapes, keeping the mouth wide
<^>en.
76 Messrs. T. L. Bruiitori and 3. Fayrer on the [Jan. 39^
12.39. Almoet paralyzed ; mouth now eloaed ; head lying on the eide.
The body is sivoIJen where bitten.
12.43. Dead 7 minutes after the bite. This snake was peculiaily
active and vigorous though innocuous.
Exp. e. — A green whip-snake (/*iM»eri/n m^Uris'iiu), somewhat smaller
than the former one, was bitten in the body by n Dabaia at 1.40.
l'4o. Almost powerless. It gradually became more and more ex-
hausted, gaped like the one bitten by the cobra, and at 2.2 it was dead
22 minutes after the bite. The Daloia had been in cuniiuenieut for some
time and was probably exhausted.
Exp,/. — A small rat-snake {Plyas mucosa), about 2 feet Img, was
bitten by a Bungani* arrulait 42| inches long in the muscles of the f
at 1.8 p.m; blood dran-n.
2.31), Sluggish ; has lost all its \ivadtj.
8.25. Found dead 7 hours and 17 minutes after the bile.
The occasional escape of an innocuous snake after the bite of a poisou-
ouB one is illustrated by Experiment g. Several others were mada
with a like result.
Exp. ff. — A full-groMTi rat^snako (Plya* mticofa), about 8 feet long,
was bitten by a fresh cobra about two thirds groivu and about half its
own size. About 13 minutes after the bite it seemed restless and un-
easy, but remained perfectly active, and was perfectly well on the third
day after the bite.
The power of one venomous snake to kill another appears from the
following eiperiments.
Exp. h. — A Bungarus fasciatiu, nearly-full grown, was bitten by a
very large and powerful cobra 5 feet 8 inches in length. It was bitten
twice, about 8 inches from the head, at 12,22 i'.m. The cobra took firm
hold and implanted the fangs deeply. It seemed to be unaffected ; and
22i hours after the bite it still seemed well ; but it died about the 29th
hour.
Exp. ». — A Bungarua earuleii*, 28 inches long, was bitten by a very
l&rge and powerful ccdira. It died in 40 minutes, presenting the same
symptoms as those of an innocuoue snake killed by a cobra-bite.
Exp. J, — Ayoung and very small, though lively, cobra, 14 inches long,
was bitten in the muscular part o£ the body by n lai^ krail {Buiujarua
cariilfui), 43 inches long, at 12.60.
At 1 P.M. the cobra is very sluggish.
1.8. Ho sluggish that it moves with difGculty and can be easily handled ;
it makes no effort at resistance.
1.20. Apparently dying : movements scarcely perceptible.
1.22. Dead 32 minules after the bite.
1874.] PoUon of Indian Venomma Snake*. 77
Exp. i. — July 10th, 1869. A young cobra, about 10 inches long, was
bittea at 3.45 r.u. by a fresh full-grown cobra near the tail, so that the
yiacera might not be injured. The fanga were seen to penetrate ; and
no doubt could exist that the poison was fairly inserted. Being put on
the ground it crawled away vigorously, and seemed unaffected by the bite.
On the I3th it seemed well ; but on tbe 17th it was found dead, and had
apparently been so for about 12 hours.
As this anake was young it may ha>-e died partly from wont of food,
and partly from the wound, as well as &om the effects of the poison.
Though small snakes of a venomous species may be lulled by large
ones, either of the same or of another species, full-grown individuals are
rarely injured by tbe bite of another, either of their own or another
■pedes. This is illustrated by tbe following experiments, which are
token from numerous others of the same sort.
Sxp. I. — A Bungarua faadatw was fairly and deeply bitten by a fresh
cobra near the tail ; there was no doubt of the penetration of the fangs
and inoculation of the poison. No effect was produced, and the £un-
garvt was alive and well five days after the bite.
Exp, tn. — A ^n^ortM/asetattu was thoroughly bittea in a similar man-
ner by a fresh Oaboia. The bite produced no efEect, and fire days after-
words the snake was in its normal condition.
Exp, n. — A Dahoia was bittea by a fresh cobra near the tail, the scales
hoving been previously scraped off. The snake bit fiercely and repeatedly.
Two dayv afterwards no effect could be noticed.
Exp. 0, — A large block cobra was bitten in two places 1 foot 6 inches
from the head, and aleo on the head, by a lai^ and vicious Daboia.
Blood was slightly dnwn ; ond there could be no doubt that the fangs hod
penetrated ond the poison been inoculated. Six days after the bite there
waa no change in the snake.
Exp. p. — A fall-grown cobra was bitten by another full-grown, fresh,
and vigorous cobra in two places about 6 inches from the head, and
olso in the mouth. They both bit each other freely in this situation, and
blood was freely drawn. They were both well a week afterwards,
Exp, q. — A cobra had 15 drops of his own venom injected hypodermi-
colly abont 8 inches from the head. A week afterwards it seemed sluggish ;
but this might be from obher conses.
Exp. r. — A cobra had 15 drops of the venom from another cobra in-
jected hypodermically in the same situation as the last. A week after-
words he was perfectly well.
EfeeU on Fiih.
Cobra-poiaon seems to produce paralysis, indicated by the fish turning
on its side in the water — ond also great excitement, the fish struggling
ond plunging vicdently.
78 Messrs. T. L. Bmuton and J. Fayrer on the [Jan. 22,
Krperimtiit IX,
A fish {OjihtoefptMlut mariUiits), about 10 inches in length, vi&a bitten
by & fresh rabra at 11.30 a.m. in tn-o pliices on the doiW and veatmL
surfaces.
11.22. It turned orer on its side in the water.
11.23. Stroggling and plunging violently in the water.
11.25. Turned over on its side.
11. 2C. On being roused it plunges violently.
11.40. Dead in 20 nuuutea from the bibs.
For the purpose of compariBou the following experiment with cimra I
was made. It will be seen that there was n* plunging. The failure of I
muscular action, except when a more than ordinarily powerful atimulus
from the nerre-centrea called it into piny, is very evident.
E.Tperinu7il X.
November 1873. — Injected a solution of curare under the akin of a
carp near the toil. A great part of the solution came out on withdrawing |
the needle of the ayringe.
11.25. Injection made.
11.26. The fish lies obliquely in the water, inclining to the opposite
aide from the injection. It can move when irritiited, and can remain
perfectly upright in the water ; but in a very short time its poBition be-
comea oblique again.
11.35, Injected aomo more curare. A great part of this also returned.
11.50, Liea obliquely, but can move tolerably vigoroualy when roused.
11.55, Movea more feebly when roused.
12.10. tjeemed dead, but did not lie Sat on its side, and still preaerved
the oblique position.
12.20. It suddenly started up without any apparent cauae, swam across
the vessel, a distance of several inches, and then relapsed into its former
Action on Stiails,
Cobra-venom aeema to destroy their irritability. It first causes them
to shrink within their shells, and finally lessens their movements when
stimulated.
Effect of lieagenls S;c. on the Action of tht Poison.
The actinty of the poiaon is not destroyed, and acarc«ly impaired, by
drying. We have made no comparative experiments with perfectly fresh
poison and the dried residue of a similar quantity ; but there are few, if
any, instances on record of de-ath from the fresh poison in leas than half
a minute, the time in which the dried poison killed a guineapig in
Experiment XXVIII.
The local action of the poison, however, seems to be altered by drying ;
Bfm- i;xt7:a)'j33atiDji of blood around tbe pari ivhere a snake has inserted its
1874.] Poiton of Indian Venomoua Snaiet. 79
faugB, or venom has been injected, is one of the most prominent effects
produced bj the freah poison, whereas it is very slight, or absent alto-
gether, vhen the dKed venom has been employed, except in occaeiooal
instances, soch m Experiment LVU.
Dilution seems also to have no effect in lessening the activity of the
venom, except so far as it retards absorpdon ; for it is evident that a
drop of pure poison, injected subcutaneouslf , is likely to find ite way into
the circulation more quickly than the same quantity diluted wifii a
hundred times its bulk of water.
Coagulation of the venom by alcohol does not destroy ite activity, as
we have shown in our former communication. The coagulum thrown
down by the alcohol ia innocuous, or nearly so ; but the poisonous principle
remains in solution, and the alcoholic extract posBesses similar properties
to the poison itself. A specimen of poison was received from India in a
coagulated state ; but we are uncertain whether this occurred sponta-
oeously or was produced by the action of reagents. It is probable, how-
ever, ijiat it was due to its haWug been mixed, in order to preserve it,
with alcohol, which had evaporated before we received it. It was active,
as Experiment XI. shows. Coagulation by boiling does not destroy the
activity of the poison (Experiment XII.) ; but a portion which was boiled
for more than half an hour under pressure corresponding to a tempera-
ture of 102° C, had no effect when injected under the thigh of a lark.
The notes of this experiment have unfortunately been lost. Admixture
with liquor ommonin and liquor potasste does not alter the effects of
the poison. This appears &om Experiment XIII., and from several
made by Dr. Eayrer in India. .
Experimtnt XI,
Oeto6«r 28tK, 1872. — A fresh supply of poison was received from
India. It was of a yellowish colour, and was hard and dry, like tough
cheese. About J a grain diluted with alcohol (in which it was only
imperfectly soluble), was injected into the thigh of the same guineapig
at 4" 14' 30".
4.15, Twitchings of on emprosthotonic character. The animal is appa-
rently attempting to vomit.
4.20. The twitchings continue. The animal throws up hia head. It
seeniB sluggish, and will not walk.
4.22. A mixture of 5 minims of liquor ammoniffi with 10 of water
was injected into the animal. Almost immediately afterwards it became
convulsed and fell over on its side, paralyzed,
4.25. It is dying.
4.26. Qdtedead.
4.27. The cardiac pulsations and peristaltic action of the bowels still
continue. The blood, when collected in a vessel, formed a firm coa-
golum.
i
80 Messrs. T. L. Bmiiton anJ J. Fayrcr on the [Jan. 22,
4.32. Peristaltic iicfion ditaiiiiahed. The muBclpB of the leg contract
when the sciatic nen'e is stimulated by &n induced current. Electrodes
were then placed in the cord. The muscles of the legs contracted
readily when an induced current was passed through the cord. One
cell was employed, and the distance of the secondary from the primary
coil was 44 centimetres.
Experirnenl XII.
May 19(7i. — A full dose of dried cobra-poison «-a» diluted with distilled
water, and heated until it was filled with white llocctdent coagula.
The solution was injected int« a guineapig'a hip at 3.25. Twitching
began almost immediately.
3.30. liestless. Hind leg paralyzed.
4. Twitching acute in hind leg.
4.10. Active hip-twitching, but hind leg still paralyzed,
4,15, Making efforts to vomit,
4,25, Vomiting repeatedly.
4.30, Distinct repeated convulsive attempts to vomit. Limbs becoming
weaker ; began to be convulsed ; gradually becoming more and more
paraly7ed,
4,45. In convulsions- Dead.
May 19rt. — Dried cobra-poison, dissolved in liquor ammonia, injected
into a guineapig's hip at 3.42,
Twitching at 3.43. Ecstless,
4. Twitching ; restless ; weak in hind leg,
4.8, A little more injected with a full quantity of ammonia. The
guineapig becomes immediately very restless.
4.15. Paralyzed. Going into convulsions. Pinching foot at onM
causes reflex actiou; marked reflex actions al! over the bodv.
4.20. Nearly dead. Heart disturbed ; continued to beat regularly for
some minutes after death. Lungs much cong<>stcd.
/n/fumce of Conttitation on the Action of iht Poison. Supposed JmntuHiti/
of thi Mongoose.
With cobra-Tenom, as with other poiijons, there is a general corre-
spondence between the size of the animal and the intensity of the effects
of a given quantity of poison, a small animal being more readily afEected
by it than a large one. There are, however, some exceptions to this rule ;
for a cat will resist the action of wbra-poison as much as, or mor« than, a
dog five or six times its size. (Compare Experiment LVII. with Experi-
ment XLIV.)
The mongooae(fl«jyM(MyrM«M)ha8longbeen supposed to be tmafFect#d
by the poison of venomous snakes, either on account of some peculiarity
1874.] Poiton of Indian Venomout Snaket. 81
in die coDstitatdoii of the ainiiDal, or, as the story used to run, on nccount
ofitBknowledgeof 10106 herb which it used to eat as an antidote; but such
is not die case. If fairly bitten, it succumbs like any other creature, as
proved by experiments in India (' Thanatophidia,' pp. 68, 69, and 134).
Its great activity and vigour enable it to elude the snake ; and generally,
when it is woniuled, it is merely scratched, not pierced by the £angB.
If the ptHson is inoculated, it dice.
The same is tme of the pig, which escapes probably by receiving the
wound in the foot, where absorption is not rapid or vigorous. This
animal, like others, yields to the poison when the fangs are embedded
and the vims thoroughly inoculated (vi<U ' Thanatophidia,' p. 134).
Action on Oermination.
In order to see whether cobra-poison had any effect on the germination
of seeds, the following experiments were made. It will be seen from
them that the venom does not prevent germination, but interferes with
it, especially when strong. In this it agrees with rattlesnake-poison,
^eir MitcJiell ' On Kattleanake Venom,' p. 52.)
Kxperimmi ZIV.
Apiece of flannel was doubled, and, 12 cress-seeds being laid between
the folds, it was placed in a small beaker with 10 cubic centims. of
water. Another piece, treated in the same way, was laid in 0 cubic
centimB. of wat«r and 1 of a 2-peiK«nt. solution of dried cobrft-poison.
Some time after the water had evaporated, bo as to leave the flannel
soaked with water but not covered, nine of those seeds which had been
treated with water and poison had germinated and grown to about half
an inch in length, while seven of those treated by water alone had ger-
minated and had grown somewhat larger than the others.
Experiment XV.
The preceding experiment was repeated with lettuce-seeds. Seven of
those treated with water alone had germinat«d, but only one of those
treated with water and poison. .
Eaiperiment XVL
A small piece of cotton-wool was placed in the bottom of each of two
short test-tubes, and ten lettuce- and ten cress-seeds were dropped into
each. Ten drops of a solution of dried cobra-poison, containing -0355
gramme in 3 culnc centims. of water, were then used to moist«n those
in one tube, and as nearly as possible the same quantity of pure water
for those in the other. The seeds were then covered with a few fibres of
cotton-wool ; the tubes were stopped with a plug of the same substance,
and placed in a warm room.
Three days afterwards, all the cress-seeds which had been moistened
witti water had sprouted and sent out a rndide, varying from j to j an
82 Measrs. T. L. Brunton and S. Fayrer on the [Jan. 2SM
inch in teagth. Eight out of the ten lettuce-seeds had sprout«d and sent
out a radiL-le more than ^ of bu inch loog. All the cress-seeds moistened
with poieoQ had alno sprouted, but the radicles were only about -j\[ of an
inch long. Five lettuce-seoda had begun to sprout, but the radiclea were
barely visible.
It ia not improbable that the delay caused by the poison in the germi-
nation of the seeds, in this experiment, is not to be attributed entirely to
its poisonous action ; and it may bo due in great measure to the solution
of the poison having matted the fibres of cotton-wool more closelv than
the water, and thua reudorcd the conditions of ur and moisture leaa
favourable to the seeds placed in it.
E_ffect of tkt PoUoii whfn introduced thrmiyh dijfereiit chanatU.
The action of the poison ia moat rapid when it is introduced dire
into the circulation, as by injection into the jugular vein ; and i
instances death may occur in less than a minute. When injected h
the thoracic cavity, aa in Experiment XXVIU., death occurred almost ||
quickly ; but this may hare been due to puncture of the Umg and intv
duction of the poison directly iiito some of the pulmonary vessels.
Injection into the peritoneal cavity comes next in order of rapidity,
but a good deal behind the last ; and it is followed by subcutaneous
injeclion.
"Whatever may be the effect of the venom of the viper or crotalus, the
cobra virus j>roduceB its poiaonoua effects tolerably rapidly when
swallowed, both in the frog and in warm-blooded animals, as is seen
from Experiments XA'II. and XrX,
It ia alflo abaorbed from I he conjunctiva, and produces the eharactep-
istic symptoms of poisoning. In Experiment XX. the animal, though
affected by the poison, recovered ; but in sefenU experiments made by ono
of us in India, death rapidly occurred after the application of the fresh
poison to the conjunctiva ('Thanatophidia of India,' pp. 108, 116, 127,
128, 135).
Ej^eriment XVII.
May 21*(, 1873. — 2.23 p.m. A small bit of dried cobra-poison put into
a frog's mouth and swallowed.
3.25. Yrog not much, if at all, affected.
4.5. Frog not so (igoroua. Appears to be paralyzed in fore lega. but
moves his hind legs freely. On irritating hia fore legs there are vigorous
contractions in his hind legs, but none in the fore lega.
4.10, The anterior part of tho body and fore legs seem to be quito
paralysred. No reaction is noticed in the eyelids when the cornea ia
irritated, lliud legs are still vigorous.
4.20. Hind lega vigorous. All the fore part of the body quite pant-
'■^zed. Mouth gaping. Ton^e swollen.
1874.] Fwwn qf Indian Venomoui SnakeM. 88
4J35. Hind legs now becoming weaker.
4.30. The application of add canies slight reflex movementB in the
hind le£B.
4.35. Add caases no reflex adjon. Complete paralysis and death have
thus occorred in two hours and a quarter.
4.40 ThonuE opened. Heart still contracting rhythmicallj and
steadily.
4J>6. Heart still contracting, but less vigorously. There ia no move-
ment apparent in the intestines,
6.5. Heart still contnding slowly.
5.25. Heart still contracting. The heart and liver were now removed
and given to another frog.
Erperimtnt XVIU,
The heart and liver of the former hog were given to a large and
strong frog. It was kept under observation for many days, bat did not
seem in the least affected.
Experiment XIX.
A small quantity of dried cobra-poison dissolved in water was given to
» young rabbit at 2.63 p.if. It was readily swallowed. In 7 minutes aU
the symptoms of poisoning were developed. The rabbit died in convul-
sions in II minutes, just as when the poison ia injected hypodermically.
The thorax was opened a few minutes afterwards. The heart had ceased
to beat, Bigor mortis came on very rapidly.
Experiment XX.
Sovember 28th, 1872. — 1.49. One quarter of a drop of cobra-poiaon
put into a guineapig's eye.
3.12. The eye Is much congested. The animal has twitchings.
3.14. Has been making efforts to vomit, and now vomits frothy clear
fluid. Has been poised also.
4.6. Still retdiing, but not vomiting.
Novtmber 2Brt. — Found to have recovered.
Local Action of the Poinn.
Cobra-poison acts as a local irritant, and produces chemosis c^ the
conjonctiva and swelling of the eyeEds when applied to the eye, and,
occasionally, congestion of the peritoneal vessels when injected into the
abdominal cavity (Experiments XX, and XLIV.).
It paralyzes the ends of the motor nerves, and also the musdes of the
part into which it has been injected (Experiment XXV.). The muscles
are not only deprived of their irritability, but become prone to putrefy
CBxpwimeat LVJJ..). The fresh cobra-poison prodooes great exla«va-
sation of blood around the wound through which it has been introduced ;
bat tins ia not so mailed when dried poison is used.
Toib XXII. n
81 MeBsrs. T. L. Bruntoii and J. Fayrer an the [Jan. 22,
If death do not rapidly follow, great swelling from infiltration of the
areolar tissue may occur, or, in some cases, gangrene of the skin and sub-
jacent cellular tissue and subsequent changes indicative of general blood-
poisoning.
The local action of viperine is probably more active than that of
colubrine virus.
Action of Cohra-'poison upon the Blood,
The blood of animals killed by cobra-poison generally presents a dark
colour, as death is due to failure of the respiration and not of the circa-
lation ; but it readily assumes a florid colour when exposed to air. The
same is the case with the blood of animals poisoned by Da&oia-Tenom
(Experiments II., V., and VI.).
Coagulation usually occurs readily and firmly in the blood of animals
killed by cobra-poison, while it is frequently absent from the blood of
those killed by that of the Daboia. In experiments made in India, thia
occurred almost invariably ; and it is illustrated by Experiments IL «nd
IV. In Experiments I., V., and VI., however, coagulation occurred in
the blood of a pigeon and guineapig poisoned by Daboia^Yenom ; and a
similar occurrence has been sometimes observed by one of us (Dr. Fayrer)
in fowls bitten by this snake in India*.
In numerous instances we have been unable to detect any alteration in
the blood-corpuscles after death from cobra-poison ; but in Experiments
XXI. and XXII. we observed a most distinct crenation in the corpnaclet
of rats poisoned by it. This was probably due in some degree to evapora-
tion, as in Experiment XXI. it was to a great extent prevented by sur-
rounding the preparation with oil ; but it indicates a change in the blood,
as the corpuscles did not present this appearance before the injection of
the poison — although they were prepared for observation in exactly the
same way, and were as much exposed to evaporation in the one case as in
the other.
Experiment XXI.
A drop of blood from the tail of a white rat was examined micro-
scopically. The corpuscles did not form rouleaux ; but no trace of cre-
nation could be observed in them.
12.10 P.M. '018 gramme of dried cobra-poison, dissolved in 1 cubic
centun. of water, was injected into the flank. Almost immediately the
nose of the animal began to twitch up every few seconds.
12.15. Head has sunk down. The breathing was laboured. The animal
made a sudden start forwards. The hind legs dragged behind. It did not
move readily when irritated. The breathing was laboured ; the expiration
convulsive. General convulsive movements occurred.
12.18. The animal seemed dead. The heart was still beating. A drop of
blood was taken from the tail ; and, the thorax bebg opened, another was
ThumtophidiA of India,' pp. 80, 100, 101, 104 Vids Mr. OuniiiiighAin*! Nmarta
« (
I874w] Poiaon o/ Indian Venomout Snaket. 85
tskeo from the right ventricle. On being examined microecopicsllf, the
oorpniclea in both were seen to be very much crenat«d. They did not
fonn roaleaax. Another drop was taken from the right ventricle, and
snrronnded with oil to prevent evaporation. Hardly a tnce of crenatioo
oould be oboerved in thii drop ; bat several branching crystals of a reddish
colour were observed, and soma of them appeared to grow while ondar
obaervatioD. Numeroas granular maisea were also seen,
f^crtnwnt XXU.
Auguit 27th. — Injected 1 cubic centimetre of a 2-pei>-cent. lolation <A
oobra-poiaon nnder the akin of the hip of a white rat.
1.36. Injection made.
1.37. Beapiiation quick. The end of the tail snipped off, and a drop
of blood examined bv Dr. Klein. The red corpuscles are much crenated,
and have no tendency to form rouleaux, but adhere together in flat masses.
The plasma contains numerous lumps of a granular material, probably
coogula of some sort.
2.5. The animal lies tti«tched out. Makes a curious squeaking noise.
It does not rise when the tail is pinched.
2.13. Liea with noee on ground. Convulsive movements of hind legs.
2.1G. Head sin^ to one side. Convulsive movements.
2.18. Breathing slow. Marked Interval between inspiiation and
expiration.
2.19. Stopped breathing. Heart still beating.
2JZ0. The animal lay on its back. A few weak respirations were
made, and then ceased. The heart was beating steadily. Thorax opened
and heart exposed. A little blood drawn from the ventricles by a fine
pipette was examined microscopically by Dr. Klem. It presented
exactly the same characters as those of the former specimen. Blood from
another, healthy rat showed numerous rouleaux, and the corpuscles were
not crenated.
Action on Miaelts.
Cobra-poison has the power of destroying the irritability of voluntary
moscnlw fibre when applied directly to it, either in a concentrated or
diluted condition. It does not produce any quivering of the fibres ; and
in this particular it differa ftara the poison of the rattlesnake as
dercribed by Dr. Weir Mitchell.
The local action of cobra-poison on muscle is illustrated by Eiperi-
menta XXIII., XXI7., XXV., and XXTI.
Experiment XXIII.
SejptenAer 4tA. — A frog was decapitated, and the skin removed from
both hind l^s. A longitudinal cut was then made in the mnscle of
both thighs. A ifrong solution of dried cobra-poison in distilled water,
of aoch a atraigth aa to resemble the fresh poison closely in appearance,
waa then ^pliad to the cut in one thigh, while the other was moistened
h2
86 Messrs. T. L. Brunton and J. Fayrer on the [Jan. 22j
with distilled water. Immediately after the application an almost
imporceptible trembling in the muscles occurred equdUy in both thig^ ;
but it ceased after a few seconds, and did not reappear. On testing
the muscles soon afterwards, by an induced current applied directlj to
them, those of the poisoned leg contracted feebly, but those of the noor
poisoned leg, forcibly.
In this experiment, the quivering occurred equally in both thigha, and
was therefore obviously due to the water in which the poison was dia-
solved, and not to the poison itself.
As Weir Mitchell found that the quivering produced by the poiBon of
the rattlesnake was not prevented by paralysis of the motor nerves by
curare, the previous experiment was repeated on a curarized frog.
Experiment XXIV.
September Ath. — The motor nerves having been tested and fonnd to be
completely paralyzed, a strong solution of cobra-poison was applied to %
cut in the back of the right thigh. No quivering of the muscles conld be
observed after its application. The poison was only applied to the
middle of the back of the right thigh. Alter a few minuteSy those
muscles with which it had come into contact did not contract when irritated
by the direct application of an induced current. Distance of secondazy
from the primary coO 0. The muscles of the sides and front of the
poisoned thigh, as well as those of the other thigh, contracted well when
irritated in the same wav, with the coil at 13 centimetres.
The poison paralyzes the muscles of warm-blooded animals in much
the same way as those of frogs ; and it seems probable from the following
experiment, that the paralysis of the wounded limb, which is very fre-
quently noticed in cases of snake-bite, is partly due to the local action of
the poison upon the muscles.
Experiment XXV.
September 4:th. — Injected 5 or 6 drops of a strong but not perfeetlj
concentrated solution of dried cobra-poison into the muscles of the left
thigh of a guineapig.
12.43 P.M. Injection made. The animsl immediately became much
excited, and rushed about wildly, crying loudly.
12.47. The leg seemed paralyzed and dragged behind the animal.
12.48. It ground its teeth and cried.
12.50. Began to start, and cried more loudly. Took it in mj amis.
It then became quiet.
12.52. Shivered.
12.58. Laid the guineapig on its side on the table. It lay still and
did not attempt to rise. Eespiration was still going on.
12.59. Cut off the head of this guineapig (No. 1), and immediately
aftar decapitated another, healthy guineapig of nearly the same siae (No. 2).
1874.] Pmtott of Indian VenomouM Snaket. 87
1.7. fiipoaed botit Bcutici of No. 1, and irriuted them by ao induced
mmnt.
Left kg. CoQ at 0. Ko eontnction.
Bight i^. Coil mt 17-5. Morement of toes.
The miuclM of both 1^ twitch well when irritated hj single shocka
(coil at 17*5), except those in the middle of the inside of the left thigh,
near the place to which the point of the ayringe had penetrated. These
mnsclea contract when the coil is at 3.
1.13. The mnsclea of tite hip of No, 2 twitch distinctly when irritated
b; aii^le shocks, coU at 24.
The toes more distinctly when the sciatic is irritated ; coil at 37.
1.15. The ventricles of the heart of No. 1 are firmly otmtracted and
moHonlees. The aoricles are still pulsating vigorously.
The ventricles of the heart of No. 2 are only modentefy cantincted,
and there is no pnlsation either in them or the auricles.
1.22. The toes of the right leg of Nol 1 move when the sciatic is
irritated, cdl at 18.
Those of No. 2 do so, coil at 37.
Putthedectrodes in the cervical part of the spinal cord of both guinea
pigs, and irritat«d it by an induced current, coO at 0. No contraction
took place in the bind 1^ of either animal. Contractions occurred in
the muscles of the fore 1^ with much the Bame force in both.
1.45. On irritating the muscles by single induced shocks : — left leg of
No. 1, vastoB extemus contracts, coil at 9*5 ; rectus femoris, a pale
nnsde, 12-5.
No. 1. Bi^t ieg, natns 15-5, rectus 25. No. 2. Bight leg, vastus 11,
rectos 16.
I.6S. No. 1. L^ leg, vastus at 16 ; right leg, vastus at 20: No. Z.
Jjeib leg, vastus at 20 ; right leg, vastus s^ 20. The vastus contracts
rather more strongly in the right leg of No. 1 than in those of No. 2.
2.23. No. 1. Left leg, vastus at 4 ; right leg, vastus at 11. No. 2.
Left leg, vastus at 11 ; right 1^, vastus at 1 1.
This experiment riiows that the venom paralyzes the motor nerves
' vheoi ap[died to them locally, a strong current applied to the sciatio-
caoaing no contraction in the left leg of No. 1, while a moderate one
cauaed movement in the right foot, at a time when the muscles of both
were nearly equally irritable.
Its deteteriooB action on the nrasclee, when conveyed by the blood, is
also evident in the rapid loss of irritability after death in both legs of
No. 1 as compared with No. 2, The pale muscles seemed to retain their-
irritabili^ longer tluui those having a deep colour.
The power of cobra-poison to panlyi» muscle when applied to it, even
in s diluted eonditicm, is shown by the following experiment.
£vperu)i«nf XXVI.
Jttfy 18A, 1873.— The l^s of a large frog were cut off close In the
88 Messrs. T. L. Bruuton and J. Fayrer on the [Jan. 22,
body, and the skiu removed. Each was then placed in a glass, and a
Buflk'ieut quauiity of fresh ox-blood serum poured orer it to cover it.
In one gla>s. tlie >eruiii contained about 5 centigrams of cohrar-poison
di.ssolvt\l in abour 2' » oubie centims. of serum ; but, with this exception, all
the conditions iind^r whicli the two legs were placed were exactly alike.
Jtilt/ 19///. — Aboiir in hours after the immersion of -the legs in serum
their irrita]ulit\- \va< examinevi.
m
The inu>clos c»f tlie !i*sj in the piu^ serum did not ccmtract at all when
the slroni^est irritation was applied to the sciatic nerve, but contracted
very villi )ro II slv whrn irriTatini direct 1 v. The muscles of tlie leg in the
poisoued stTiim w en.' whiter than those of the other one. They had a
faint vell(>\vi<h tintro, and wore somewhat stiff. Thev did not contract m
the lea^^t wht-n tin* strongest irritation by a Du-Bois coil was applied
either tu them or the soiatic nerve.
AViien the poison i-* iujivted directly into the circulation, op ia very
rapidly absorlu'il. so that the quantity circulating in the blood is large, it
destroys the irritaluliiy of the voluntary muscles rapidly, and, occasionally
at least, ha^^tens in a most remarkable manner the occurrence of rigor
mortis. This is wvW soon iu the E.xperiment XXV., where rigor
mortis supervtMied in half an hour after the iujection of the poison, while
the musi^le*^ of aiioihor animal killed at the same time by decapitation
retained their irrirabilitv for manv liours.
m m
Ki'jH'n.ii, lit XXVII.
Min/ Sth, 1^73. — "Hight ihiirh of a troj; liiratured, with the exception of
the sciatic nerve. Animal p(>isoiie(l by the introduction of some dried
cobra-[)oison ilissolvril in water into the lymph-sac of the back. Afterihe
animal had bei'onn' complftcly paralyzed, the gastro«'nemii of the t^o
logs were irritalt-d by an induced current (1 bichromate cell).
Loft log (poisoned i, disianct^ of coil l:Vr), contraction ; right, 24"0, con-
traction.
Eu'prrhnPiit XXVJl (^i).
Another frog prepared in the same way gave at first : — left leg (poisoned),
distance of coil 4i!*2, contraction; right (^ligatured), distance 21 '0, con-
traction.
After some time: — left leg, distance 6*0, contraction; right, distance
25*0, contraction.
Some time later: — left leg, distance 0, almost no contraction; right
leg, di^tan<-e 14'o. contra«'iion.
Jn this experiment, the poisoned muscle at first responded more readily
tr. the irritation than the one which had been deprived of blood by the
applirat i(»n of a ligal iiro : and this renders more apparent the effect of the
poison, in eausing ra]»i..l diminution and final extinction of irritability is
th«. n.u-t'-le to which it had access, since the other lost its exdtabilitT
v'rrv Hl'i-.vlv,
j
1874.] PoitOH of Indian Venomout Snake: 80
Sieperimmt XXVUI.
8tp*tiiiher 5th. — About 2^ p.m. injected | cubic centimetre of a, 2-pOT-
eent. solution of dried cobra'poison into the thoracic caritj of a ^uiift»-
pig. It wu uncertain whether the lung (right one) was pierced hy th«
point of the needle or not. Within a few seconds the ftoimal gave several
conrolsive struggles, and died in half a minute or so. The head wu then
cut off. Immediately afterwards a second guineapig was killed hj deca-
pitation. On opening the thorax of N'o. 1 (the poisoned guineapig) the
long! wne found congested. The heart was tetanically contracted and
quite stiU. The heart of No. 2 was contracting vigorously. The vena
cava contained a few bubbles of air. The lungs were pale.
2,40. Peristt^tic movements are going on very actively in the intes-
tines of both animals.
2.42. The muscles of the Nominal wall irritated by single induced
•hocks.
Guineapig, No. 1. No contraction. Coil at 0.
Guineapig, No. 2. Contraction. Coil at 14-5.
Muscles of the Mp irritated in the same way : —
' ~ if contraction of muscle. Coil IS.
1 Contraction still slight. Coil 0.
No. 1.1'^'™^'^*=*'
\ Contraction
No 2 I Contraction. Coil 37.
' I Powerful kick. Coil 0.
2.50. Bigor mortis is coming on in No. 1. The legs are quite stiff.
A trace of peristaltic movement still going on in the small intestine.
The muscles of No. 3 are quite flexible.
2.56. No. 1. Muscles of back of thigh and of abdominal wall irritated
directly as before. No contraction. Coil at 0. Muscles of the front of
tiugh twit«h slightly. Coil at 0.
No. 2. Muscles of back of thigh twitch decidedly. Coil at 37. .
3.12. No. 1. No contraction in any muscles. Coil at 0. The animal
is stiff.
No. 2. Muscles are quite limp. Muscles of back of thigh twitch de-
odedly. Coil at 25.
All the muscles do not lose their irritability with the same rapidity,
•ome of them becoming paralyzed before others. The intercostal muscles,
•errati, and abdominal muscles seem to lose their irritability fint ; and
such mnsclea of tbe limbs as have a dark colour become paralysed sooner
tiian tboae which are paler (Experiment XXV.).
Expttvnent XXIX.
8«pUtnh«rWi. — A cannula was placed in the carotid of a large guineapig,
and j cubic centimetre of a 2-pei>cent. solution of cobra-poiaon injected
into it towards the heart. The animal was seiied with violent convul-
aions, passing into complete opisthotonos in about twenty seconds, after
d>e injectioa of tbe poison, llieae ceased, and t^e animal seemeJ quite
90 Messrs. T. L. Bmnton and J. Fayrer on the [Jan. 22,
dead in rather less than a minute from the injection. The thorax was
then opened. The lungs were somewhat congested. The heart was
quite still in tetanic contraction. A strong interrupted current applied
to it caused no contraction of any of the fibres. The muscles lost their
irritability very quickly ; the intercostals of both sides^ and the serratua
and subscapularis of the right side, seemed to lose their irritability befor.*
the other muscles.
When the poison is more slowly absorbed, so that a less quantity of it
circulates in the blood, its action on the muscles is much less mariced,
as is evident from a comparison of the irritability of those in the poisoned
and non-poisoned limbs in Experiments XXXYIL, XXXYIII., XX ATX.,
XLYII. If the poison has undergone such changes as render it less
active, it has no action, or only a feeble one, on the muscles, as seen in
Experiments XI., XXX., XXXI., & XXXII., where poison^ which had
undergone partial coagulation, was employed.
Experiment XXX.
January 14^. — ^In order to test the local action of the poison on the
muscles and nerves, a ligature was tied round the base of a frog's heart
so as entirely to arrest the circulation.
12.0. About a drop of cobra-poison was injected into one leg.
1.30. Laid bare the lumbar ner>'es in the abdomen, and irritated them
by an induced current. Both legs contracted nearly equally.
ExpeHment XXXI.
January 14<^. — At 12.15. One or two drops of cobra-poison were in-
jected into the leg of a frog. The wound bled freely. Immediately after
the injection the frog became very excited and jiunped about very much*
12.20. Erog quiet. Eespiration quick.
2.30. Prog quiet, but jumps when irritated. It seems to use both lega
equally well.
January 15£7t. — The frog is not dead, but is feeble. On killing and
opening it, both legs contracted nearly equally when the lumbar nervea
were stimulated by an induced current.
ExpeAnvent XXXII.
January \biK — Tied the heart of a frog, and, 12.55 p.m., injected into the
right leg a drop of water, and into the left leg a drop or two of cobra-
poison.
1.55. Irritated the back of the frog by an induced current. Both legs
contracted nearly equally.
Exptritnent XXXIII.
May 9<A. — A frog (Rana teniporaria) was poisoned with curare. After
complete paralysis had set in, the right leg was ligatured, with the ex-
ception of the sciatic nerve. The animal was then poisoned by the in-
1874.] PatOH of Indian Venomoua Snaket. 91
trodactioii of a aolntion of dried cobn-pcdson in orator into the lymplt-aM:
on the \>Bxk, at about 12.30 pji. The irritabUitj of the muscles wu
tested l^ nng^ induced currents applied to the denuded mosclsfl, about
2.30.
Diitance of Coil.
Left leg 7-5 Contraction.
Eight leg 7-2-7-5 do.
Another frog was cnrarised and similartj prepared, with this excep-
tion— that the Teasels of the right leg only were ligatured, the muscles,
as wen as the nerre, being left free. This frog was also examined in
the same way; and the irritability of the muscles in both 1^ was
fbnikt to be almost exactly the some three to four hours after poisoning.
Both contracted with the coU at about 7'5.
Seeondary Mtion of the Poiaon on Matdei.
Hie muscles of the part into which the poison has been introduced are
very apt to ondergo rapid decomposition. We have already shown that
their irritability is either lessened, or completely destroyed, by the action of
the venom ; and it seems very probable that the mere contact of any other
foreign body, containing Bacteria or their germs (as the water in which
the cobra-poison was dissolTed in our experiments certainly did) would
suffice to explain the decomposition of the muscle without assuming any
special patrefactive action on the part of the poison; for the muscle,
whidi has been at least temporarily killed by the poison, is placed in the
body in the most fsTOuiable conditions of temperature and moiature for
the occurrence of decomposition whenever any germs are brought into con-
tact with it. However, Weir Mitchell found that the venom of the rattle-
snake had a curious influence upon muscle, which could hardly be eiplaiued
vithont ibe supposition that the poison had a peculiar disorganising
aetion upon the muscular tissue. In every instance the venom softened
the muscle in proportion to the leogtb of time it remained in contact
Trith it ; so that, even after a few hours, in warm-blooded animals,
and aft«r a rather longer time in the frog, the wounded muscle became
almost diffluent, and assumed a dark colour and somewhat jelly-like ap-
pearance. The structure remuned entire until it was pressed upon or
■lietched, when it lost all regularity, and offered, under the microscope,
the appearanceof a minute granularmass. In order to ascertain whether
oobra-pcnson had a similar action, the following experiment was tried.
ExpenmrntlXXi:^ .
Siptember 1873. — ^The gastrocnemii of a frog were removed and laid in
twtwatch-glassea. One was then covered with several drops of a solution
of dried cobra-poison, dissolved in a sufficient quantity of |-perH:ent, salt
solution to form a mixture about the consistonce of fresh poison, while
Hm a&Mt was cohered with a few drops of salt solution alone. They
92 Messrs. T. L. Brunton and J. Fayrer on the [Jan. 22,
were then protected from dust by two other watch-glasses inyerted oiver
them. The temperature of the room was moderately warm. The
poisoned muscle underwent no change. Both muscles gradually dried
up ; but at no time could one be distinguished from the other, except by
the label on the watch-glass.
The influence of cobra-poison in causing decomposition within the body
is evident from the following experiment.
Experiment XXXY.
January 17th, — About three drops of cobra-poison were injected under
the skin of the flank of a guineapig at 12.48 f.m. Immediately after-
wards the guineapig became restless and cried. In two minutes its head
began to twitch. An hour after the injection the animal was quiet, and
little or no effect of the poison could be observed. Three hours after the
injection it did not seem very well. Next morning it was found dead.
On examining it 22 hours after the injection it had begun to undergo
decomposition. The abdomen was somewhat inflated, and sulphuretted
hydrogen issued from it when opened. The hair came off readily from
all parts of the animal*s skin. The muscles were soft. There was little
ecchymosis at the spot where the injection had been made. The tissues
near it were rather watery. The heart was contracted; the lungs
somewhat congested.
Action an the Nervous System,
The most prominent symptoms of an affection of the nervous system
after the bite of a cobra, or other venomous snake, in animals or man, are
depression, faintness, lethargy, and in some cases, somnolence. There is
loss of coordinating power, and paralysis, sometimes affecting the hind legs
first and creeping over the body, sometimes affecting the whole body at
once. Death occurs by failure of the respiration, and is preceded by con-
vulsions.
These symptoms clearly point to paralysis either of the nervous centres
or of the peripheral nerves. It may be supposed that the mention of the
latter alternative is superfluous, and that paralysis of the peripheral
nerves cannot produce such symptoms, which must therefore, by ezda-
sion, be due to an affection of the central ganglia. More especially may
the occurrence of convulsions be thought to exclude the possibility of
death being due to paralysis of the peripheral terminations of motor
nerves ; for if their function is abolished here, how, it may be said, can
general convulsions, which have their origin in the nerA'ous centres, occur?
The answer to this is, that although the ends of the motor nerves are
80 far deadened that they no longer transmit to the muscles any ordinary
stimulus proceeding from the nerve-centres, their function is not so
thoroughly abolished that they cannot transmit those which are stronger
than usual. This is shown by the fact that when an animal is slowly
poisoned hv curare (as for example when that poison is introduced into
1874.] Poiton of Indian Venemout Snaket. 98
Ote Btconsch after ligatun of tlie renal veaselB), conTnldoni occur jiut
as in death from cobra-poiBon. Although the motor neirea have their
function so much impaired that they no longer transmit to the musclea
of respiiation the ordinary stimuli from the medulla, which usually keep
Qp the movementfl of breathing, they can still transmit those stronger
impulses which proceed from it when greatly stimulated by the increasing
▼enosity of the blood, and which cause the respiratory as well aa the other
muscles of the body to participate in the general convulsions. The loss of
coordination which occurs in poisoning by cobra-venom, has also b&ea
noticed by Toisin and Liouville in poisoning by curare.
That the peripheral terminations of the motor nerves are actually
paralyzed by cobra-venom is shown by Experiment XXXVI., in which the
animal was able to move the leg which hod been protected from Ihe action
of the poison for some time after the rest of the body was perfectly
motionless, as well as by Exp. XXXVII. and those succeeding it. Its
occurrence in man is indicated by the symptoms of a case described by
Dr. HilsTOi (Ind. Med. Gaz., Oct. 1873, p. 254).
But paralysis of motor nerves is not the only effect of cobra-poison on
the nervous system. The spinal cord is also paralyzed, as is seen from
Exp. XU., where motion ceased in the frog's leg which remained free
bom poison, although it answered with great readiness to a very weak sti-
mulus applied to its oerve. In some instances paralysis of the spinal cord
appeared to cause death when little or no affection of the motor nerves
could be observed (Exp. XL VII. Ac.) ; but in others the peripheral pars-
lysis was strongly marked. In no case was it more obvious, and in few
was it so distinct as in Exp. XXXTI., made with the virus itself, which
had neither become coagulated nor dried. In experiments made with the
coagulated poison, death seemed invariably to be caused by paralysis of
the spinal cord, the motor nerves being little sJffected (Exp. XI.) ; while,
in t^ose made vrith the dried venom, sometimes the action on the cord
predominat«d, and sometimes that on the nerves. In this respect, aa
well as in some of the symptoms it produces, cobra-poison agrees very
doeely with conin. This alkaloid, as Crum-Brown and Eraser have
shown, often contains a mixture of true conia and methylconia. Conia
alone paralyzes the motor nerves without affecting the spinal cord ; but
when mixed with methylconia, sometimes the one is affected first, and
sometimes the other. When the dose is small, the motor nerves are
nsaally paralyzed before the reflex function of the cord ; but when the
dose is large, the cord is paralyzed before the nerves. Methylconia also
affects both ; but a small dose of it paralyzes the cord before the nerves,
while a large one paralyzes them first. The paralysis of the hind legs,
often observed in snako-poisoning (Kxp. VI. & VU.), is probably partly
due to t^ local action of the poison in the nerves and muscles of the bitten
member, and partly to its action on the cord. This paralysis is noticed
in Qenens zlix. 1-7, where Jacob says, " Dan is an adder in the path.
--... vvi^un^-s luroiigh whii-h irritation of the iifth ue
afTected after the refiex function of the cord is nearly
the power of voluntary motion f^till exists.
The effect of the poison upon the respiratory an«
will be considered under the heads of respiration ano
Action of Cohrorpoison on Motor nen
As the contraction of a muscle, on irritation of tht
plying it, is the index by which we judge of the irrit
itself, the paralyzing effect of cobra-poison upon muscl
determination of its action upon motor nerves much
in the case of such a poison as curare, which leaves t
bility intact. For the failure of a muscle to contract
motor nerve, can be due only to paralysis of the motor
of curare ; but in poisoning by cobra-venom it may b
ment of the muscles, as well as paralysis of the nerve,
instances in which the muscles still retain their irriti
altered, and respond readily to direct stimulation after
to contract on irritation of their motor nerve, we are *
bhat the nerve is paralyzed ; and such is the case in Eb
In Experiment XXY. this action on the ends of m<
he more evident from the paralysis being most com]
("here the poison was introduced. At this part, it was
entrated state, into contact with the ends of the motor
ther parts of the body received it after dilution with
lem the paralysis was much less marked.
The paralysis of the hind legs, so often noHoa^ ^^ —
1874.] PotMon o/Indian Venomem Snakes. 95
Ktperimmt XXXVI.
A ligature was placed round the right thigh of a young frog, excluding
the Bciatic nerre.
2.43. A drop of durk fiuid cobn-poiBon (the first supply) was injected
into the donal lymph-sac. Immediately after the injection the animal
became restless.
3. It lies quietly with its eyes shut. It hardly moves when touched;
but it struggles when laid upon its back.
3.8. It can etiU draw up the ligatured leg. The other one can be
drawn up, but with a wriggling motion. When laid on its back the
BDimal no longer resists.
3.9.30. It lies quite flat. There is trembling of the leg when either
foot is touched ; and when it is pinched either leg can still be drawn up.
On suddenly touching the poisoned'leg, the frog gare a jerk with both.
BeopinttOTy movements have ceased. The exact time when they did so
WB8 not noticed.
3.17. The trog has become much lighter in colour, with the exception
of the ligatured leg,
3.45. The eyes no longer shut when touched; they remain widely
open. Dilute acetic add of 1 per cent, produces no effect when applied
to the sound leg ; but when the leg is lifted up, so as to prevent friction
■gainst the teble, it is drawn in towards the body.
4.9. On applying a strong interrupted current to the eye of the frog
tite unpoisoned 1^ jerks feebly, the poisoned one not at all.
4.13, On turning the frog on his back the non-poisoned 1^ moved,
4.20. Opened abdomen. The heart was beating, but only slowly. Irri-
tated the lumbar nerves on the left side (those of poisoned leg) by an in-
terrupted current. No contraction occurred in the poisoned leg ; but
twitching took place in the non-poisoned one. Irritated lumbar nerves
of right side. Tetanus occurred in the right (non-poisoned leg). No
movement of the poisoned leg. Laid bare the muscles of both legs, and
irritated them by a Faradic current directly applied. Those of the poisoned
leg were paler than those of the other. The muscles of both legs con-
tracted when irritated directly. Exposed the sciatic nerves of both sides
and imtaied them by an induced current. No contraction in the gastro-
Gnflmioa of poisoned leg. Tetanos in the non-poisoned leg.
4.36. The heart is no longer contracting. Electrodes were placed in
the medulla, and an interrupted current applied. Contractions occurred
in the non-poisoned I^. No contractions in the poisoned one.
The movements which occurred in the non-poisoned leg when the
lombar nerves of the other side were irritated, may have been due to re-
flex addon through the spinal cord. If this were the case, it would indi-
cate that the sensory fibres in the lumbar plexus were not paralyzed, and
that the reflex power of the cord was not quite destroyed ; but the nerves
_*»» mVUi >»l*i-T 1
luuiur lUTves of the limb si ill retaiiu'd the
paralysis of the reflex function of the eord ha
of the leg on turning the frog on his back i
higher nervous centres, through which the o]
posture was manifested, retained their power
Experiment XXXVI]
November 29^A, 1872. — ^The sciatic nerve of
exposed ; and a double ligature being passed ui
whole of the tissues except the bone were then
tween the ligatures. A fraction of a drop of (
^per-cent. salt solution, was injected into the
two hours the animal seemed paralyzed. On in
electridtj, or by acetic acid, slight movements o
and were fully stronger in the poisoned than th(
tion of the poisoned hind foot also occasioned t\(
non-poisoned foot. Twitches did not invariably
the fore paws was noticed on irritation of the hii
then passed round the poisoned hind leg, and tl
the non-poisoned one, and the animal left a li
again applied had a similar result to the former,
the non-poisoned limb were sometimes stronger t
tation applied by a strong interrupted current to
trodes inserted in it, caused very faint twitches in
tion of the lumbar nerves in the abdomen caused ^^
feet. Irritation of the exposed sciatic nerve of the
interrupted current caused afiv^r»« — ^
1S74.] Poiton of Indian Vemmoui Snaia. 97
cuued the p<MSon«l and onpoUoned muscles to contract witli &pparent1j
the ume force, shows that a stiiall dose of the poison causes a consider-
able amoant of paralyaia of the ends of motor nerves, while the mascles
ftre but little a^cted.
Bxperimtnt XXXVIII.
Jfay 14A. — The right leg of a frog was ligatured, with the exception
of the sciatic neire, and the animal poisoned by a rather small dose of
dried cobra-poison dissolved in water, and injected into the dorsal Ijrmph-
■ac at 11.45 Ajt.
12.15. The animal paralysed. Acetic add applied to the left arm
caused movements in it ; but no movementB ensued when the acid was
applied to the noae. When applied to both arms and one leg, it caused
movements in the arms and the left leg, but none in the right leg.
12^. Acetic acid applied to the left arm causes movement in it, but in
no other part of the body.
12.51 . Electrodes were placed in the spine and the cord irritated by a
Faradic current. At 15 centimetres distance of the secondary from the
primary coil there is faint twitch in right arm. At 9, distinct twitch in
both anna. At 0, distinct twitch in both arms, none in legs ; sciatica
exposed and irritated. At 50, right leg contracts distinctly. At 36,
right leg becomes tetonised. At 16, left leg contracts very faintly indeed.
At 6, left leg contracts slightly.
The muscles were then irritated by single induced shocks : — 9-8 centims.,
right leg faint contraction ; 9-8, left (poisoned) leg contraction is equally
ttraagi lO-l, left (poisoned) leg' contraction occurs. lO'l, right (liga-
tured one) does not contract.
In tjiis experiment, the irritability of the poisoned muscle is greater
than that of the other, the venom having done less injury to the mus-
cular substance than the deprivation of blood by the ligature, and conse-
qnently the paralyzing action of the poison on the ends of the motor
nervea becomes very evident.
Experiment XXXIX.
Majf 12t&, 1873. — ^A ligature was passed tightly round the right thigh
at a huge frog, the adatic nerve being excluded.
12. Bight leg ligatured.
12.12. Injected a considerable dose of a solution of dried oobrar-poison
in water into dorsal lymph~aac.
12.14. The frog has assumed a most peculiar position. The left hind
leg is drawn up, and the two fore legs are held over head with palms
tomed forwards.
12.20. Cornea sensible. Left leg is drawn up again if it be forcibly
12.31, Cornea tenaible. When the left hind foot is pressed it ta drawn
. w I i. y>^ in 1 1 1 u *.
reHcx action produced bv irritation of tht
1.24. Acetic acid ap])lied to right fon
in ri^fht hind leg alone. When applied i
movement in that arm alone.
1.35. Acetic acid applied to botb feet, 1
caused no motion anywhere. Both sciatic i
a considerable portion of their course. It
right sciatic had not been included in tht
constricted bj the fascia at the place of liga
by an induced current.
Distance of Beoondftrj
Leg. from primary ooiL
Left.
0-
No contra
Bight.
32-0
Distinct <
possible
scuitic 1
morethfl
expoeed
below tl
above th
Sight.
37-5
Distinct c<
Left.
70
No distin
muscles
ducedsh
Single shock.
7.6
they con
In this experiment, the right sciatic nerve
ration of lifi^tn"riT»*» - — ^ "
1874.] PoUoa of Indian Venomout Snakes. 99
10^7. Ligftture applied. A considerable quantity of blood was lost.
10^, A considerable quantity of dried cobra-poison dissolved in water
was injected into the dorsal lymph-aoc. Immediately after being released
the ttog jumped about, but became quiet in a minute or so.
11.28. Made some voluntary movements.
11.45. Acetic acid to fore feet causes weak reflex movements in both
fore feet; stronger in bind feet, especially in right.
11.55. Acetic acid to right forearm caused vigorous kicks of right
hind 1^. Acetic add affected right leg ui 10 seconds. No motion in
any other part of body. Acetic acid to left forearm caused kicks in both
hind 1^8, bnt much more vigorous in the right. Also movement of left
forearm by itself, but weak.
12.5. Acetic odd U> left fore leg caused wriggling motion, first in right
hind 1^ and then in left fore leg in 16 seconds. Applied to right forearm
it caaaed a weak kick in right hind leg and wriggling in left hbd leg, but
no motion in any other part.
12.27. Acetic acid applied to forearm. No reflex action anywhere.
12.30. So reflex action anywhere on application of acetic acid.
12.30. Distance of coil 8, Electrodes in the spinal cord. Slight con-
tractions in right hind and left fore legs, and also in the abdominal
muscles, though very weak. It was now noticed that tlie cord with
which the frog was attached to the board had been very tightly tied
round the left forearm and left there. The circulation was stopped there,
as the cord had not been removed.
The paralyxing effect of the poison on the motor nerves was here shown
by an involuntary experiment. On irritating the cord the ligatured leg
responded as we hod expected, but we were astonished to nee movements
in the left arm also. An examination of the limb at once showed the
cause of the phenomenon. The cord attaching it to the board had been
inadvertently drawn so tight as to obstruct the circulation, and thus pre-
vented the access of the poison to the nerves.
Experiment XLI.
May 15A. — Bight thigh of fn^ ligatured, with exception of the sciatic
nerve.
1.2. ligature applied.
1.4. A considerable dose of dried cobra-poison dissolved in wat«r
injected into dorsal lymph-sac.
2.26, Acetic acid applied to a limb causes no movement whatever in 60'.
Interrupted current. Distance 0, electrodes in spine: only weak
twitch in muscles of forearms ; no movement in hind leg.
2.30. Both sciatics exposed.
Bi^t sdatio. Distance 50, distinct contraction of gastrocnemius.
Left sciatic. Distance 0, no contraction of gastrocnemius. Single
ahocka. Both gastroonemii exposed and irritated directly.
VOL. ZXQ. I
, _ .,., I t,K — Lii orcliT to Icsf Iho action c
(Muls of tlie motor n(Tv«'S, without di^t url)iii<2: tht^ e\]
one 1(*^, two t'n\L;s were taken of as nearly as po
Both wore a erv small ; but Xo. 1 was somewhat lar^
No. 2. The sciatic nerve was exposed in one thij
placed on the hook electrodes used by Marej foi
means of a Pohl*s commutator, with the cross pieoet
rupted current could be sent at wiU through either :
of the secondary from the primary coil at which th
tion took place in the muscles of either nerve was n
Distauoe of primary firom secondary ooiL
Time. Frog 1. Frog 2.
About 1.25 17-7 22
1.40 26-3 12-3
1.46 26 18 Injected a
cobra -poi
dorsal Ij
No. 1.
2.7 31-2 24
2.27 31 18-5
2.60 24 17-8
3.10 17-5 19-2 Frog 1 m(
when the
distance (
ment occi
nerve wae
3.30 12 17-5
O 4r\ - - -
1874.] Powra rf Indian Vewmotu Siuket. 101
May 2ltt. — ^Tbo scUtica of the other legs were exposed and irritated.
30 of primuj from aea)nilw7 ooiL
XiB» Prog 1. Frog 2.
0 11*5 Frog 1, no contraction. Frog 2,
slight contraction. The ini-
tabilitj of the muscles «-u
now tested by single induced
shocks applied to them.
0 7-5 Fr(^ 1, no contraction. Fk^2,
slight contraddoD.
The disturtHng effects occasioned in the other experiments b; the
necessity of comparing a limb acted on by the poison, but retaining ita
blood-«upply, with one in which the circulation had been arrested, is here
got rid of by employing tM^ frogs of as nearly as possible the same siie.
The paralysia of nerves caused by the poison is evident.
Erp^-iment XLUI.
Dte, 4lh. — Bight 1^ ligatured, with the exception of the sciatic nerve ;
a small quantity of alcoholic extract of cobra-poiswi dissolved In water
injected into the dorsal lymph-sac.
Noon. Injection made.
1.80. The frog lies quite helpless. A spark of electricity applied to
the side causes reflex contraction of both legs. When the poisoned leg is
drawn out, the frc^ draws it up again with a wriggling motion. The
poisoned leg at once reacti when the toes are pinched; the ligatured
one does not.
When the sides of the frog are irritated by an electric sparh, all the
legs, except the ligatured one, give a twitch.
3.50. On exposing the Inmbar nerves in the abdominal cavity and irri-
tating them by an induced corrent, the poisoned leg contracted, the liga-
tured one did not.
The effect of the alcoholic extract in causing paralysis is shown by this
experiment ; but the insensibility of the ligatured leg, which was in all
probdnli<7 dne to an injniy of the sciatic nerve by the ligature, renders
it difficult to say how much of the paralysis was due to the cord, and how
miteh to the nerves. That the nerves were affected, however, seems clear
from the &ct that the muscles no longer reacted to voluntary stimuli,
but did so when an extraordinary stimulus was occasioned by pinching.
Experiment XUV.
Amg. 27d.-~A amoll dog was chloroformed, and both vagi were ex-
posed.
1235 pjL About two grains of dried cobra-poison were injected into
the pentoneat cavity.
12.42, Vat«T was thrown over the animal to revive him more com-
l2
102 Messrs. T. L. Bninton and J. Fayrer on the [Jan. 22,
pletely from the chloroform. Bowels acted. He is verj unsteady on his
legs. Looks drunk.
12.44. Dog vomits freely.
12.45. Both va^ diWded. The vomiting ceased, the breathing became
very slow, and the head was thrown up with the nose in the air.
12.53. Has become very quiet. Falls down on his side. The vomiting
has not recurred.
12.55. Dead. Artificial respiration commenced.
1.12. On laying bare the skull and trephining, slight reflex movements
occurred in the limbs.
1.17. Micturated. On irritating the exposed cerebrum by a Fanidic
current no contractions occurred in the limbs.
1*47. The spinal cord was exposed and irritated by a Faradic current.
No contractions occurred in any of the muscles, except those to which the
current was conducted, even when the strongest was employed. On
exposing the sciatic nerves and dividing one of them and applying a
Faradic current, no effect could be perceived when the electrodes were
applied to cither the central or the distal end of the nerve. The motor
nerves were thus seen to be paralyzed.
The heart continued to beat vigorously all the time. On laying
open the abdominal cavity, the intestines and peritoneum were found in
a state of intense congestion. Electrodes applied to the lumbar nerves
caused no contraction an v where.
Thorax opened. The heart was beating vigorously. The lungs were
normal. A Faradic current applied to the phrenic nerve caused no con-
traction of the diaphragm ; but when applied to that muscle directly, it
caused vigorous contractions.
The left vagus was divided and its peripheral end stimulated by a Faradic
current. The pulsations of the heart were at once arrested, but again com-
menced ; and no further irritation of the vagi had any effect on the heart.
2.2 P.M. Stomach removed. Its coats were intensely congested, as
though some irritant had been swallowed. It contained much bile. The
blood was florid and formed a firm coagulum.
This experiment clearly shows that cobra-poison produces paralysis of
the motor nen'es in warm as well as in cold-blooded animals, the sciatics
being so completely paralyzed that they did not respond to the strongest
irritation, although respiration was efficiently kept up and the circular
tion continued unimpaired. In almost all the other experiments, when
the ner>'e was irritated immediately after death, contractions were pro-
duced ; but the same is the case when the animal is poisoned with curare,
and the contractions are due to the poison not having had sufficient time
to exert its full action.
The complete cessation of vomiting after division of the vagi seems to
indicate that the poison produces emesis by acting on the periphend
termmations of the vagi, and not on any nerve-centre.
1874.] Poison of Indian Venomous Snakes. 103
Action of Cohrarpoison on Secreting Nerves,
A notable symptom of cobra-poison in dogs is great salivation ; and
this might be supposed at first sight to indicate that the poison acted
as an irritant to the secreting nerves of the salivary gland. Nausea and
Yomiting being also present, however, it is by no means improbable that
the salivation is due to the poison stimulating the secreting nerves of the
saHvary glands not directly, but by reflex action, through the gastric
branches of the vagus. Unfortunately we are unable to say in which of
these ways salivation is induced, as we have not noted whether it
occurred after division of the vagus or not. So far as memory serves us,
we are inclined to think that it was much less in these cases ; but on this
point we cannot be at all positive.
Whether cobra-poison has any stimulating action on secreting nerves
nt first or not, it seems finally to paralyze them, or at least greatly to
diminish their power.
This is evident from the following experiment.
Experiment XLV.
A dog was etherized and the chorda tympani exposed after its
separation from the lingual nerve. A cannula was then placed in the
dact of the submaxillary gland. On irritating the chorda by a weak
Earadic current, applied at intervals, saliva flowed freely. Some dried
cobra-poison dissolved in water was then injected into a vein in the leg.
Shortly afterwards the saliva began to flow much less freely than before ;
and although the current was increased in strength, only a small quantity
could be obtained.
Action on Sensory Nerves,
The sensory nerves seem to be little, if at all, affected by cobra-poison.
As appears from Experiment XXXVI. they retain their power after the
motor nerves are paralyzed; and Experiment XLYI. shows the compara-
tive effect of the poison and of want of blood both on the sensory and
motor nerves. The former were so little affected by the poison, that they
caused a ready response when those which had been deprived of blood had
nearly ceased to act. The motor nerves of the poisoned limb, on the con-
trary, were quickly paralyzed, while those of the ligatured one, although
doubtless weakened by the loss of their vascular supply, long retained
their irritability. In Experiment LX. the optic nerve and the aural and
buccal branches of the fifth nerve retained their irritability after the
cord had become nearly paralyzed ; and, in several experiments, reflex
actions could be induced by irritation of the cornea after voluntary motion
and respiration had ceased.
ExperimevU XL VI.
The right leg of a frog was ligatured, excluding the sciatic nerve, and a
ooncentrated solution of dried cobra-poison injected into the dorsal lymph-
sac at 2.3 p.m.
► « T Ky '
\\ hcii acetic acid is a])j)]ic(l to left liai
straii;]»t('in'd, and tlicrc arc stronu; {'oiitn
none ill ilu' left, and little nioveiiinit m an
Acetic acid applied to left foot causes po
Acetic add applied to the right foot hae
inserted in the spine and the cord irri
Distance of the secondary from the primar}
moyement of left hand.
At 16 centims. movement of left hand an
At 12 centims. also faint movement of le:
At 15 centims. the interrupted current wa
the muscular twitchings were more powerfi
ihMsi in the right one.
On applying the electrodes to the lumbar n
right leg contracts.
Coil at 42 centims. the left leg only twitcL
Action on the Spinal C
The spinal cord has the threefold function
impressions, a conductor of motor impressio
in examining into the nature dE the action oi
must consider the manner in which each of t]
Cobra-poison, as has already been intimate(
•ction upon the reflex function of the cord ;
Experiment XLVU., &c.
As a conductor of sensory impressions, the <
kinds, viz. tactile and painful, and thpAA h*
lOV/V
I874.J PouoM of Indian Venomota Snakeg. 105
in it amly the feebleat movement. In Experiment LX. no response
was elicited by striking, pinching, or pricking the pawa of the animal
but when the ear was tickled the cat shook its head, or moTed its paw
to ward <dl the irritant.
FrcHU these cases we think we are justified in concluding that the gny
matter of ihe spinal cord, tiirough which painful impressions are trans-
mitted, is paralysed by cobra-poison ; but the white sensory columns are
little, if at all, affected. The power of the cord to conduct motor impres-
siooa from the encephalic ganglia appears to be little, if at all affected,
until the apparent death of the animal ; for in Experiment LX. we find
that, very shortly before respiration ceased, and when ordinary reflex
action from the cord was nearly gone, purposive or voluntary movements
were still made. The absence of movements in Experiment L., when the
cord was irritated by a needle, as well oa the rapid loss of its power to
produce movement in the limbs when irritated by a Faradic current, is,
we think, to be attributed to paralysis of its function as an originator,
and not as a CMiductor, of motor impressions.
Krpenmeta XLVII.
May 19th. — The lumbar nerves of a frog were exposed and a ligature
tied roand the body, excluding these nerves.
12 (noon). Some dried cobra-poison dissolved in water was injected
into the dorsal lymph-sac.
1.45. The frog is partially paralysed ; mouth gaping ; reflex action is
still marked in all the limbs, but more in the legs than in the anna.
The heart was exposed when the ligature was applied ; it still beats,
but feebly and slowly.
1.50. Acetic add causes reflex movements when applied to either the
hind or fore feet.
1.54. Applied to the nose, acetic acid causes movements in all the
extremities, and especially in the onus.
1.56. Applied to the right hind foot it causes movements of the arms
and of the jaw, which otherwise gapes.
2.2. Applied to the left hind foot it causes no reflex action.
2.14. Heart beating very feebly, 18 pulsations per minute. Beflex
movementa still occur in all the limbs, and rather more in the legs than
in the arms.
2.30. Acetic add produces no reflex action anywhere. The heart has
almost ceased to beat, and only contracts faintly at long intervals.
2.34. All reflex action has ceased.
2.45. Eledrodes placed in the spine and the cord irritated by a Faradio
conent. At 15'5 centims. distance, faint contractions in both arms. At
0 centim. distance, no contraction in legs. Sciatic nerves exposed and
irritated. 32-5, slight contraction in left leg; sli^t contraction in
right leg.
< Ml ( iH'l't* IS no ('\ Klfl)
OV liiuscl»'s ; (It.'Mtli M|)j)**;u> (lur to |t;ii':il
caiist'd l)v the aflioii ot tin* j)(U>(Hi : I'o
i]i()ui!;li I'tH'bly, aftrr all rellex action had
Expenment XI
A ligature was passed under the right t
tied round the limb, so as to constrict th<
exception of the nerve, and completely arr
At 1.8 half a drop of cobra-poison (1st
centim. of water, was injected into the dor
1.12. The animal is sluggish.
1.15. Crawls about but sluggishly, and
drawn up close to the body.
1.20. The frog is more sluggish.
1.23. The hind limbs seem paralyzed; t]
much less than before.
1.30. Frog almost motionless. Conti*acti
occur ; but they no longer respond when pii
1.57. There is a faint motion in the limbs.
2.18. Frog is dead. Much ecchymosed.
On irritating the lumbar nerves in the abd
current, the poisoned leg contracted rather mc
On irritating the sciatic nerves in the thigl
ture, the contractions of the poisoned leg w*
those of the non-poisoned leg.
Electrodes were then placed in the spinal
by an induced current-
1874.] Pmton of Indian Venomoiu Snakes. 107
in this inatBiioe became panlyeed before the motor oervee. It is indeed
difScult to ny whether the motor nervee were paralyied in this case or
not, u the muBcles themselvee were diatioctly weakened.
Experittunl XLIX.
Dte. In, 1872. — The right 1^ ot a frog was ligatured, excluding the
Bciatac nerre, which was kept covered by a flap of akin to prevent its
becoming dr^. A ligature w^s also put round the left leg in a similar
manner, bat not tightened.
2 p.if. Colmi-p<»son injected into the abdominal rein.
The effect not being marked, the aorta was exposed. .
2.27. Some ptnaon injected into the aorta. It seemed to take effect
at onoe ; all motion ceased immediately.
2.30. The ligature was then tightened round the left leg.
2.48. The frog has since moved ; but all motion has now ceased.
2.52. Even when irritated by acetic add there is no movement. The
heart is still contracting.
No reflex action occurs when a strong interrupted current is applied
to the nose or limbs.
Lumbar nerves exposed and irritated.
ffi^t. Distinct contraction of thigh. Coil at SS-fi.
Left. Do. do.
Bight. Distinct contraction of whole leg. Coil 50.
Left. Do. do.
Sciatica exposed and irritat«d.
Bight. Contraction. Coil 77-0.
Left. Do. „ 62-0.
3.28. Bight. Do. „ 50.
Left. Do. „ 43.
The poisoned leg seems to be losing its irritability more quickly than
the other. Irrit«lHUty of spinal cord gone.
3.35. The left still contracts, with the coil at 35. The other, when
uritAted by a current of the same strength, contracts more strongly.
The loss of power occasioned by the (.'essation of the circulation In the
ligatured limb (which is used as a standard with which to compare the
other) was diminished in this experiment, by injecting the poison directly
into the circulation, so as to enable it to reach the motor nerve-ends at
once. As soon as it had taken effect, the poisoned leg was likewise
deprived of its circulation, so aa to bring the two limbs as nearly as
possible into the same conditions. The cause of death, in t^ experi-
ment, was paralysia of the cord, all reflex action having been almost
immediately abolished by the large dose of the poison injected into
the drcnlation, thongh the heart continued to beat. The motor nerves
•wen not at Bxtt afiaeted ; but after a little while paralysis appeared in
fi» p<saoaed Hmb. This experiment is especially interesting in reference
108 Messrs. T. L. Bruiiton and 3. Fayrer wi /he [Jan. 22,
tu the cause of death when a considerable quantity of poison entt^rs tlio
arterial system at once. In warm-blooded animals, as in show-n by Ei-
periment LX VTII ., the heart is arrestt^, in many iniitauoes, and death t bus
oci'aaioned; but when this is not the cose, llie appearance of jiaralysia \s
probably due to affection of the nerre-centrw.
Erperin^ent L.
Stpt. \Zih. — A ligature was placed round the middle of a frog, excluiling
the lumbar nerves.
3 P.M. Some dried cobra-poiaon dissolved in water was iujeeted into tha
dorsal Ivuiph-sac. Immediately after the injection the animal could move
all its limbs quito well.
3.3. Bestless ; moves all its limbs.
3.17. Can still move vigorously.
3.21. Can kick vigorously with its legs, especially the right. When
it moves it aeema to overreach itself and turns over, apparently front
the hind limbs remaining unaffected and the arms becoming partially
paralyzed.
3.40, Still moves voluntarily.
3,.')2. No reflex motion can be produced by touching any of the ei-
tremitles with acetic acid.
A minute or two afterwards a slight twitch was noticed in one arm, to
which acetic acid had been applied ; but whether this was greatly delayed
reflex action caused by the acid, or whether it was due to aometluDg elae,
is uncertain. A needle was now run down the apinal cord. It produced
no effect.
The legs contracted readily when the lumbar nerves were irritated.
The absence of motion in the legs when the cord was irritated by a
needle run down the spinal canal, shows that the power of the cord to
originate motor impulses had been destroyed, as it would usually have
caused violent contractions in the extremities. These having been pro-
tected from the action of the poison either on muscle or nerve, would
respond readily, as indeed they did, to voluntary motor impulses shortlj
before the death of the animal.
Experiment LI.
May 12tA, 1873, — ^The sacnun of a frog was removed, and a iigotara
passed round the body, excluding the lumbar nerves. There waa a good
deal of bleeding.
12.30. Ligature tied.
1233. A. good dose of dried cobra-poison dissolved in water was inti»-
duoed into dorsal lymph-sac. Immediately afterwards the frog spmi^
about once or twice.
1.27. Cornea insensible. On pincliiDg the fiugerof either hand, it kida
ont vigorously with the right hind leg. On squeezing the toee of n^tk
^'td foot it kicks ont ngorously with it. On squeezing toes of Um klh
1874.] Pmaom of Indian Venomom Snakes. 109
hind foot there is no morement wbatoTer. On placing acetic acid on
either forearm the frog kicks out strongly with the right hind leg.
2. Intarrapted current, tUstance 7. Acetic acid applied all otot the
frog no longer cauaee any movement whaterer. Electrodes placed in
apinal cord just below occiput. Cord irritated b; an interrupted current.
Sight leg kicks Tigorously. No motion in any other part of the body.
Experiment LII.
Jfoy 15th. — Frog ligatured round the middle, the lumbar nerrea ex-
cepted. A moderate amount of bleeding.
12.40. Ligature applied.
12.62. Frc^ springs actively ^mut when ttmched. A considerable dose
of dried cabn^-'pfOBcai dissolved in water injected into the dorsal lymph-sac,
l.lo. Cornea insensiUe. When either hind foot is pinched, it is drawn
ap with a wriggling motion when the irog is lying on the table. When
the frog is suspended the foot is drawn up at once.
1^. On applying acetic acid to both fore limbs and nose, the hind
l^s were vigorously drawn up to the body, but only after a long interval.
1.26. Strong acetic acid applied to both fore limbs and nose. Move*
nienta in all four limbs after 8 seconds.
1.36. Weaker acid applied to both fcve limbs. Movements in all the
limbs in 37 seconds.
2.20. Applied to both fore 1^. Movements in both fore limbs in 4
seconds. Worse in hind legs.
2.53. Apjdied to all the limbs and the nose. No motion anywhere.
Divided medulla.
2.58. No reflex at all in 200 seconds after appUcation of acid to all
the limbs and tite body.
Abdomen opened. Lumbar nerves irritated just below exit from spine.
DUtBoos of primarj from
Lrg. Mix>DdU7 ooil in centinu.
6-3 Left gastrocnemius contracts very
slightly ; right not.
0 Left gastrocnemius contracts slightiy;
right not. Both sciatics exposed and
irritated in the thigh some distance
below ligature.
Left 57 Tetanus of leg.
Bight 58 Tetanus. Xerve rather more firmly
applied to electrodes. Viscera re-
moved and brachial oerves irritated.
Bight 47 Contraction of foot.
Left 45 Contraction of foot.
in Qiis experiment the loss of refiex motion was gradual. It is shown
to be due to pandyaia of iho cord, and not to excitation of S^sohenow's
t o£ _
110 Messrs. T. L. BruDtOD uric/ J. Fayrer on the [Jaa.23|j
iniibitory centres, by the divUion of the medulla having no power to
crease the reflex action.
The fact that irritation of the lumbar nerves hardly caused any conti
tiou tn the legs, whUe irritation of the aciaties below the ligature
them to contract re-adily, indicates either that the nerves had been inji
by the ligature, or that the part of them lyiug between the spine
ligature had been paralyzed by the poison. The latt«r is possible ; but sb
the irog moved ita ariuB aud not its legs before death, the fonuer is more
probable.
Several years ago Setschenow showed that the optic lobes in the frog
possess an inhibitory power over the reflex acta originating in the spinal
cord. Irritation of the optic lobes greatly lengthens the time required for
the performance of any reflex act, and thus produces an effect apparently
similar to that of diminished ejcitubiht.y, or paralysis, of the spinal cord.
A diminution in reflex action may therefore be due to two very different
causes:— (1> Lessened excitability of the cord, and (2) excitement o£
Setsehenow'a inhibitory centres. These can, however, be readily
tingnishcd from one another by dividing the eord just below the medi
It is thus separated from the inhibitory eentres ; aud if the diminution
reflex action is duo to escittmeut in them it will disappear, but will bo
permanent if it is caused by pamJysia of the cord. The following ex-
periment, performed by Tiirck's method, shows that in cobra-poisoning
the diminution of reflex action is due to the latter of these causes.
Ej-penment LUI.
May 19//i, 1873. — The right leg of a frog ligatured, excluding the sciatic
nerve.
3.6. A full dose of dried cobra-poison disaoh'ed in water injected into
the dorsal lymph-sac.
3.54. The animal appears dead. Both hind legs dipped into diluta
acetic acid. Bight arm twitched.
3.57. Keflex aclion in both arms. None in the legs when the left leg is
dipped in the acid.
4, No reflex action from ligatured leg.
4.2. No reflex action from left leg in (SO seconds when it is dipped in
the add.
4.10. No reflex action from either leg in 250 seconds.
The medulla was now divided in order to separate the cord from
Setchenow's inhibitory centres.
4.35. No reflex action can be observed.
As the operation of dividing the cord somewhat lessens the excitability,
in the following experiment the division was performed on the prerious
day, BO that its effects should have passed off before the poison was inje>ct«d.
The columns headed " left " and " right" indicate the number of seconds
' ""bich lapsed before the correspondii^ leg was drawn out of the acid.
1 874.] Poison of Indian Venomous Snakes. Ill
Ea!j>eriment LIV.
May I5th, — About 3 p.m. divided the medulla of the frog.
„ 16^. — Suspended the frog by a hook in its jaw.
When touched the frog draws up its legs, an J
makes wiping movements on its flanks.
Time.
Left.
Bigl
11.17
8
8
11.44
5
6
11.59
4
5
12.6
3
7
12.10
5
3
12.25
12.30
8
10
The pomt of an aneurism needle was drawn
across the spine so as to destroy any rem-
nant of medulla. The frog at once passed
into a state of opisthotonos ; but in a few
minutes this passed o£E.
12.40
12
9
12.48
12
9
12.55
10
8
12.68
10
5
1.
8
5
1.2
• •
• •
1.5
• •
• •
1.9
11
10
1.16
10
10
1.18
• •
• •
2.35
300
300
Injected a drop of concentrated solution of
dried cobra-poison under skin of back.
It draws up legs and wipes back once or twice.
Another drop.
No reflex action in either foot. The heart could
not be seen beating till the frog was opened ;
then it was found beating slowly and lan-
guidly, 24 in a minute.
2.45 Half a drop of liquor atropi® placed on heart.
Immediately afterwards its pulsations be-
came more forcible, but were still 24.
Ea^periment LV.
May 16th, — Divided the medulla of a frog about 3 p.m.
May 16th. — Suspended it by hook through the jaws.
1.3 6 3
1.6 5 5
1.11 6 6
1.16 6 12
1.18 5 6
One Aiap of lUg^y dOntad, bnt itill iiiiiiiii
tiie akin oi Hie beck.
2.23 10 14 The foot WH twitched i^ in On add ^ than
timeo, bat the leg wu not dnwn np.
a25 150 150 No raSex eotum. Strmg RoetiD acid mnina
none. Thonx opened. Heart qinto ML
These experiments show that the time required for Uie perfonnaiioe tt
a reflex act went on increaaing, or, in otlier words, the exbltabililj of titt
cord went on diminishing, after the injection of tiie poiaon ; aitd all aim-
mntiication with the inhibitorj centres having been preriooslj oat off hf
dividing tJie medulla, this effect oonld onlj be doe to Ute .aotion ct Uw
pcMBon on the cord.
Exp4nmMt IjYL
At 1.16. Half a drop of oobr»-p(riara was injected into Ute p
cavity of a guinespig.
1.17. The animal is restleaa and twitdiing; nins about.
1.18. Micturates.
1.24. It is getting weak and Bluggisb. Thebind quarters have ai
a crouching posture. It moves when roused.
1.26. It looks dron-sy,. is disinclined to moA*e, and is jerking. The hind
le^ M« almost paralyzed. When they are retracted it draws them np
with difficulty.
1.27. Has defecated. Is convnlBed generally, but tbo convulsions are
more marked in the hind quarters.
1.32. Convulaions continue. They are not increased or ezdted bj ex-
ternal stimuU. Cornea insensible.
1.34. Mouth only twitches. Heart acting vigorously.
1.35. The animal is quite dead.
1.36. The spinal cord irritated by an induced current through electrodes
inserted in the vertebral column. The irritability of the cord seems per-
fect. (It was judged of by the contractions of the hind limbs.)
1.40. The heart continues to beat. Thorax laid open. The vagi iso-
lated, and one of them irritated. The cardiac action seems to be increased
by the irritation of the vagus. The auricles contract very rapidly, the
ventricles not so rapidly. The cord is still irritable.
1.50. The irritability of the spinal cord as affecting the lower extae-
mities is almost gone ; as affecting the upper limbs it is still retained.
Heart still contracts vigorously.
1.54. The lower limbs are no longer affected by electricity applied to
the spinal cord. The upper limbs are affected.
1.56. The spinal cord is still slightly irritable. The heart ii
^^ freely.
^^ 2. Cbrd still slightly irritable. Heart acts briskly.
1874.] Poitim of Indian Venomout Snakei. 118
2£. Heart octB as Tigaronal^ as ever. Artificial Tespintion was tried.
2-15. Artificial reapiration has been kept up, but has been of no Berrice.
The imtatnlity of the cord is mnch diminished, though not qnite eitinct.
The stroogast current causes a barely perceptible motion. The heart is
atill acting. There are spots of ecchymoaie all over tlie inteatiues,
2.40, The irritatnlitj of the cord is quite gone. The heart is still
actii^. The blood collected from the large vessels coagulated finnly.
Experiment LVII,
Aufftiet 30th. — ^A cannula was placed in the trachea of a cat, and 1^ de-
cigramme of dried cobra-poison was weighed out and dissolved in a amall
quantity (about 2 cub. centims.) of distilled water. The solution was
dear and glury, hanging in threads from the stirring-rod.
2.40. Injected about two thirds of this solution under the skin of the
right hip,
2.50. Bespiration is quicker. The cat lies down and does not like to
rise. When raised it walks toward a dark comer, dragging tiie right
feg-
2,58, Shivering (^ right 1^ and partially of body. No other symptom
than paralyms of right leg being noticed, a further injection was made.
4.26. The remainder of the solution injected in the same place. This
also seemed to produce little eSect.
6.10. Injected '02 grain dissolved in a little water, as the cat did not
•eem lUxiat to die.
6,2, Injected Ij culnc centimetre of a 2-peiw!8nt. solution of cobr&-
pmson in distilled water, partly into a vein in the back of the left hind
kg, partly into the peritoneum. The left hind 1^ seems partially para-
lyied. The respiration has a peculiar character, the diaphragm seeming
to relax with a jerk. The respiratory movements are very deep. Feri-
staltio action of bowels.
6.20. The fore legs are now becoming paralyzed.
6.25. Bespiration quick. Entirely diaphragmatic. Cornea quite sensi-
tive. The animal opens it« mouth when the tail is pinched, but not wh«i
the feet are pinched,
6.37. Sensibility of the cornea seems nearly gone. When the inside
of the ear is tickled the animal shakes its head.
6.43. Although respiratory movements still continued, artificial respi-
ration was begun. The animal was laid in an apparatus which kept it
6.45. The cat tries in vain to vomit. The cornea is almost insensible.
Abont 8.80 the heart-beats ceased. The body of the animal was ex-
Sjmned next day at noon. Bigor mortis well marked. The body of the
raTiiinnl had a strong odour of decomposition. The lungs w^« congested,
fclie right side of the heart gorged, the left empty and firmly contracted,
^y*lie perieardinm ccmtuned a quantity of dark-red serum. A considerable
li.'AO. Vomits atraiii. Tlie animal can waU
lie on its side.
2.40. C an ualk, bnt seems slightly giddy.
2.45. Vomiting and defecation.
3.12. Sensibility of the cornea nearly gor
tated the cat shakes its head. When the ey
not moye ; but when the point of a pair of fo:
fore foot is raised to push the forceps away.
3.20. The animal suddenly got up, walked a
3.22. It seems as if it wanted to yomit, but ifi
ear is tickled it shakes its head.
3.26. There is distinct reflex action on irrita
not when the fore paws are pinched.
3^2. Breathing is getting deep and slow, an
each inspiration. There is still motion of th<
mouth are tickled. A minute or two ago it got
two, and then fell. Bespiration graduiJly ceasec
in the trachea, and artificial respiration kept n
beat very shortly after. Electrodes were placed
seventh and twelfth dorsal vertebra. A Faradi
them caused contractions in the adjoining mus<
elsewhere. The left sciatic was exposed and i
tracted. About an hour afterwards curious a]
movements took place in the rigJU foot. The
posed in the right leg.
Experiment LIX.
1874.] Poiitm of Indian Venamoui Snakes. 1 15
4.4. ConviilsiYe motiong oocar, bat the animal can still run. Almost
immediately after, when laid on its side it could not get np.
4.7. The cornea is now insensible. A cannula placed in the trachea
and artificial respiration commenced.
4.15. A needle placed in heart. Pulsations quick. The artificial re-
spiration was discontinued. The pulsations became quicker.
In this experiment the paralysis began in the fore legs. There was di-
stinct loss of coordination ; but the animal could run up to the last,
although it could not walk. This indicates that the higher coordinating
centre (probably the cerebellum) was paral}ised before the lower ones, just
as in the case of a man who is drunk.
Ejsperiment LX.
August 29ihf 1873. — ^A cannula was placed in the trachea of a cat about
5.35. One decigram of dried cobra-poison, dissolved in two cubic centi-
metres of water, was injected into the peritoneal cavity.
5.39. The animal lies on its side breathing very rapidly and wagging
its tail. Bises, sits with head erect and mouth widely open.
5.45. The respiratory movements are very rapid and shallow, with
occasional deep ones. The animal sits up. Eespirations 240 per minute.
Pulse 148 per minute.
6.3. The animal was lying down and occasionally rising. Is now lying
down. The respiratory movements have an extraordinary vermicular
character. Dr. Sanderson ascertained by palpation that this is due to
the diaphragm contracting before the thoracic waUs expand.
6.7. The respirations are feeble, with occasional deep ones. The cat
walks quite well. The bowels act.
6.20. Bowels act again. Tries to vomit several times.
6.37. The cat lay on its side, and stretched itself once or twice in a
sort of convulsive manner.
6.41. Lies quietly. When the cornea is touched or poked with a
pointed instrument, or when the finger is rubbed over it, the eyelids do
not close, nor does the animal give any sign of feeling. When the hind
legs are struck, it moves its fore legs very faintly. Bespiration is quite
regular and apparently normal. The end of the tail gently moves from
side to side. When the inside of the ear is tickled the animal shakes its
head. It took a deep breath, and moved its head voluntarily. The pupil
is much contracted. When the arms are irritated by a sharp stick the
animal draws its body slightly together. A minute or two afterwards it
moved its tail from side to side several times voluntarily. The animal
was lying on its side. Lifted it up and laid it on its belly with its feet
under it. It rose up and walked several steps.
6*45. The cat again rises and walks, but staggeringly. It then falls
and lies on its side. The hind legs seem to be weaker than the fore legs.
TOL. 2xn. IL
1 16 Messrs. T. L. Bnmton and J. Fayrer pn the [Jan. 22,
6.52. Animal lying on its side. When a bright light is brou^t befora
its eyes it draws back its head. The cornea is quite insensible. When
the paws are irritated by striking, pinching, or pricking there is no re-
sponse. When the inside of the ear, nose, or mouth is tickled, the cat
shakes its head, and sometimes moves its paw to put the irritant away.
7.5. On touching the eyes it sometimes draws back its head, but there
is not the slightest motion of the eyelids. It voluntarily moved its paws
and head as if to rise, and then sank back as if asleep, and lay still an its
side.
7.6. Laid it on its bdly. It rose and Ti-alked a step or two towards a
dark comer and then fell. Immediately afterwards the musdes of the
neck gave a sort of shudder. After movement the respiration becomes
much quicker, and then rapidly becomes slow. After lying a minute or
so its respirations are 27 per minute,
7.25. Moves its paws and tries to get up voluntarily, but cannot do so.
Irritated paws and ear by sparks from a Du-Bois coil. No reaction. On
irritating the inside of the thigh in a similar manner, it stretched out its
fore legs, protruded its claws, and seemed to be trying to grasp me.
7.«'%3. The respiration ceased \dthout convulsions. The cannula in the
trachea was immediately connected with an apparatus for artificial respi-
ration, and this was kept up. While some adjustment was being made
on the apparatus the animal was obser^'ed, and its heart was found to have
ceased to pulsate about five or ten minutes after artificial respiration had
been begun.
On opening the thorax the lungs were found somewhat congested-
The right side of the heart was moderately filled. The left ventricle was
quite empty and firmly contracted. The surface of the stomach and in-
testines was much congested. The interior of the stomach was not con-
gested.
In this experiment, respiration continued for two hours after the in-
jection of the poison. The most remarkable points as regards respiration
are its great acceleration, with occasional deep breaths at first, its vermicular
character about the middle of the experiment, and its regularity towards
the end. Beflcx action seemed entirely abolished, and sensation very
much impaired ; the mental faculties seemed sluggish ; but voluntary power
was retained, and the movements of the animal were not indefinite bat
distinctly purposive.
The motor nerves and muscles were evidently not paralyzed ; but the
grey matter of the cord seemed to have lost its power of inducing reflex
actions or of conveying painful impressions. Tactile impressions, such as
laying the animal on its belly, still caused reaction. The movements
thus induced, as well as those caused by irritating the ears, &c., may all
be reasonablv ascribed to the action of the brain.
Closure of the eyelids would seem to be a purely reflex act, in which
the brain is altogether unconcerned.
1874.] PiriaoH of Indian Venomoui Snaket. 117
Experiment LXI,
Oetebv S6A, 1872. — To aacertun if a mixture of etrychaiaand woonra
prodnoed the same effect as cobra-poiBon, a giiiueapig weighing 1 lb. waa
ezperimentod upon.
2.36.30, One cubic centimetre of a solution of woorara (1 in 1000)
was injected nnder the skin of the side.
234. Aa the fint dose seemed to produce little effect, another cutuo
centimetre was injected In the same way as before.
2,56. A drop or two of Liquor Stiychnis (4 gra. to 1 fl. oz.) waa in-
jected into the side.
2.67. Twitching; motiona of the body begin. (They were not exactly
like those produced by cobra-poison.)
2.58. The animal has fallen over on ita side and ia paralyzed, but the
twitching continues.
3.2. The animal is dead. No convulsions. On opening the animal
the heart vna found contracting vigorously.
ISectrodea were inserted in the spinal column and the cord irritated by
an induced current. The limbs contracted when irritation was applied to
the cord. The iciatic nerve was exposed and irritated by an induced cur-
rent. The muscles of the limb contracted.
8.9. Heart still contracta feebly. The lungs are congested.
Action of Cobra-poiion on the Slomaek ami Intealiites,
One of the most noticeable symptoms of cobra-poisoning in dogs is
vomiting of a violent, repeated, and most distresBiug kind ; and it is also
present in cat« and guineapigs, though to a less degree. Its occurrence
in guineapigs is somewhat extraordinary, as these animals very rarely
Tomit, and, according to Schiff, only do bo after their vagi have been di-
vided ; whereas other animals which vomit under ordinary circumstances
are then unable to vomit at all. The nenous centre by «hich the move-
ments of vomiting are originated is closely connected vdtb the respiratory
centee, and it may be set in action by stimuli conveyed to it by the
branches of the vagus distributed to the stomach and other intestinal
organs, and also through the pharyngeal branches, either of the vagus or,
poBsibly, of the glosso-pharyngeal nerve. The brain can also excite it ; but
&» vomiting it produces is not usually prolonged. The vomiting which
occurs in cobra-poisoning is, in all probability, due, in part, to irritation of
the gastric or abdominal branches of the vagus — but not altogether ; for
the attempts to vomit continued in Experiment LXIV. after that nerve
had been divided in the neck ; and the failure to bring any thing up is
to be attributed to the cardiac aperture of the stomach failing to dilate
at the proper tame — a result which usually occurs after section of the
vagos.
In Experiment XLIV. there wu intense congestion of the mucous
le of the stomach ; but this does not occur in all cases. It could
I
1 18 Messrs. T. L, BnuitoD and J. Fayrer on the [Jan. J
hardly be due to the divisiuii of the vagi in this iustADce, as that operatuai J
b usuallv followed by paleness of the membroae. The intestinal mov^
ments arc quickened by the poiiwa, since there is pui^ng, which c
not be due to increased intestinal secretion, as the stools
chiefly of mucus. The movements contiuue for a considerable I
after death.
Effect of Cobra-poiaoii upon &3j)iration.
The action of cobra-poison upon respiration is perhaps the moet il
purtont of those which it exertu upon the oi^anism j for it is through th»
action that death is generally caused. The rtapiratory movements, besides
being frequently altered in form, are generally quickened after the intro-
duction of the poison ; then the number Biufes to the normal or even below
it ; they become weaker and, finally, cease altogether. The blood being
no longer aiirated, becomes more and more venous, and, by irritating either
the respirat-ory centre itaelf or some nerrous centre closely asaodated
with it, occasions general convulsions. These disappear whenecer arti-
ficial respiration is begun and the blood again at-rated; while they
reappear when the respiration is disoontiuued and the blood regains its
venous ch;iract'.'r. This condition ia to be observed io Esperimcnt LXII,
The de|>endence of the convulsions on the venosity of the blood is well
ahown by Experiment VIII. of onr former c<«amumc»tion, iriiare the otn-
ditioQ of the blood was indicated by the colour of the fowl's ctMnb, and as
this became florid, or livid, the convulsions disappeared orretomed. After
they have continued a short while the convulsions cease ; ics the Temoua
blood does not maintain the vitality of the nervous centres lofficiently to
keep them in action ; but if artificial respiration be recommenced, iha fint
effect of aerating the blood is to renew the ccmvulaions, by increasing tlia
vitality of the nervous centres, and rendering them again susceptible to
the action of a stimulus, though the conTulaions disappear sa aooa as the
arterialization has proceeded sufficiently fair.
Increased rapidity of the respiratory movements may depend either
upon greater excitability of the respiratory centre in the medullai, or
upon stimulation of some of the afferent nerves which have the power to
accelerate it. The chief of these are the pulmonary branches of then^aa,
though there are probably others proceeding from the cerebrum, throng
which the emotions influence the breathing, and others from the general
surfoce of the body.
In order to ascertain the cause of the acceleration of respiration aarenl
experiments were made. Experiment T.TTTT shows that it is not doe toUw
action of the poison on the cerebrum ; for it occurs after the oerebcil
lobes have be^i removed. The ultimate arrest of respiration is probaUj
due, in part, to paralysis of the medulla, and, in part, to paralysia at tlie
motor nerves distributed to the respiratory muscles. The complete iaaan- ^
■ihtlity of the phrenic nerve to the strongest stimuli, while the aciiliei
18r4.] Pmmm of IniUan Vemmoui Snaket. 119
and vagus still retwned a coiuidenble amount of irritability, in Experi-
ments XLIV. A LXTL, is very remarkable. The want of coordination
between the diaphragm and the thoradc muscles in Experiment LX. is
not improbably dne to paralysis of the phrenic nerve, though it may be
attributed to some alteration in the reapiratory centre. Brown~Seqaard
states that the diaphragm contains ganglia which will keep up rhythmical
movements in it after the central nervous system has been destroyed ; and
if this statement is correct, it seems probable that paralysis of the phrenic,
bj interrupting the connexion between the respiratory centres in the
medulla and those in the diaphragm, may allow the movements of the
ibonac respiratory muscles and of the diaphragm to occur one after the
other instead of simultaneously.
It is difficult to say to' what extent the stoppage of respiiation depends
on paralysifl of the medulla, or of the motor nerves, in each case. Pro-
baUy the effect of the one preponderates in some cases, and that of the
odter in others.
Eirpinmeiil LXII.
JVott. 29, 1872.-~The vagi of a cat were exposed and some dilute cobra-
pcnson injected subcutaneously. little effect bebg produced, the dose
was repeirted, and then a solution of alcoholic extract of the poison in-
jected subcutaneously and into the peritoneum. After the last injection
the animal became feebler. No vomiting. Before death slight convul-
sions occurred. After they ceased, a cannula was put in the trachea and
arttficial respiration bc^un. Slight convulsions again appeared, but ceased
as respiration was continued. They recommenced when the respiiation
was stopped, and disappeared when it was again begun. On once
more stopping reapiiation and allowing the convulsions to cease spon-
taneously, recommencement of the respiration caused them again to
appear.
Erperittuni LXIH.
Jiffy 21, 1873. — A rabbit was etherized and the cerebral lobes were
exposed and carefully removed.
3 r.u. Operation finished.
3.7. Bespirations 37 per minute.
3.8. A small quantity of cobra-poison injected into the flauk. Active
reflex movements occur on pinching the limbs and tail, and respiration
also beccanes more rapid.
3.12. Beapira^ns 98 per minute. Heart's action feeble.
3.23. Keathing hurried. BeRei force continues active.
Another quantity of cobra-poison injected, the two doses together not
mating more than a modeiate amount.
337. Bespirations very feeble. The upper part of the spinal cord, on
bmng irritated by a Faradic current, caused movemeutn in the limbs.
Beflex movements still present, but much diminished.
120 Messrs. T. L. BniDton and J. Fayrer on ike [Jon. 23,
3^8. Eeapiration ceased. Cannula Inserted iu the trachea, and arti-
ficial reHpiration commeDced.
3.40. Sciatic nerve exposed and irritated by a strong current, indi
twitcluugs in the limbs, but occasioned no reflex moTeraent
part oE the body.
'SA5. The animal seems perfectly dead. The strongest current
duces no effect either when applied to the cord or to the sciatics.
The colour of the muscles seems changed when compared with those of
the other rabbit (Experiment LXIV.) which had no poison. They are
of a less vivid colour, and altogether have an altered appearance.
In this eiperifflent the respirations became quickened from 3" to AG
per minute after the injection of the poison, although the cerebral lobes
had been preriously removed. The acceleration, therefore, could nut lie
due to emotion, or to the action of the poison on the cerebrmn. A com-
.parison with Experiment LXIV., in which the cerebral lobes were removed
without iujecting any poL-ton, shows that in the latter no acceleration
whatever occurred, and the respirations became gradually slower till they
ceased.
Experiment LXIV. ■
July 21, 1873. — A rabbit was etherized, the calvaria removed, and
cerebral lobes carefully excised. The bleeding was arrested by cotton-
wool steeped in perchloride of iron ; and by the actual cautery.
1.18. The operation concluded.
1.23. Eespirations 32 per minute, liellex movements well marked on
pinching feet or fail.
U3. Respirations 10 per minute andmuch deeper; and each oneended
with a jerk, as if of the (liaphragm.
1.35. Fore legs extended in a convulsive manner. Bespinition ceased
almost entirely ; but at long inten'als of about 15 and 20 seconds, an in-
spiration occurred,
On pinching the feet the respiratory movements became moj-e perfect,
though feeble.
1.43. Heart beats rapidly but feebly. Eespiration has ceased. Heflei
movements are still well marked.
1.44. Cannula placed in the iTachea, and artificial respiration begun.
Eeflex moveiuenta continued for some mbutes ; but then the heart ceased
to beat.
3.55. Sciatics exposed and irrilafed by a Faradic current. No con-
tractions occurred in the limbs. The muscles contracted when irritated
directly.
From these experiments it was evident that the accelerated respiration
was not of cerebral origin ; and it was therefore probably due to sti-
mulation of the pulmoiiary branches of the pueumogastric by the poison.
If this were so, the acceleration would not appear if the vagi wure
divided previously to the injection of the poison, as the stimulation of Ih^
1874.] Poison of Indian Venomous Snakes. 121
terminal branches of the nerves in the lungs would no longer be con-
ducted to the medulla. The following experiment shows that our hypo-
thesis is correct, the injection of the poison rendering the respirations,
which had already been greatly diminished in rapidity by division of the
▼agi, still slower.
Experiment LXV.
Sept, 15th. — A dog was chloroformed ; both vagi were divided, and a can-
nula placed in the trachea. On recovering from the chloroform, the
animal became very restless and retched constantly, but was unable to
Tomit. A little while afterwards he became more quiet, and his respira-
tions were counted.
3.10. Bespirations 7i per minute.
3.13. Bespirations 7 per minute.
3.15. About *01 grain of dried cobra-poison dissolved in ^ cub. centim.
of water was injected into the vein of dog*s leg.
Immediately the animal became very restless, and tried in vain to
Tomit. Bespirations 7 per minute.
3.21. Constant retching, but no vomiting. Bespirations 7.
3.23. About '02 grain more was injected.
3.27. Constant retching. Bespirations 6. The animal now lay down
exhausted, and was killed by a blow on the head.
Experiment LXVI.
July 9. — ^About 1 grain of dried cobra-poison dissolved in water was
injected into the flank of a white cat.
3.38. Injection made.
3.43. Oat seems depressed, sits with head drooping and eyes nearly
shut. Licks its lips occasionally. Pupils moderately dilated.
3.48. Bubs its ear with fore paw, and licks fore paw afterwards. Is
disinclined to move. Pupfls more widely dilated.
4.25. Another dose injected.
4.50. Another dose injected into peritoneum. As yet there is no sym-
ptom except depression and languor.
4.51. Vomiting. Lies crouched down.
5.5. Still vomiting.
5.14. Lies on its side. Movements of vomiting. When the cornea is
touched the eyes move, but the lids do not close. There is also sometimes
a movement of fore foot as if to ward off the irritant.
5.17. Whining. Pupils much contracted. When the inside of the
ear is tickled the animal scratches at its shoulder with the hind leg of
same side. It cannot stand. It shakes its head sometimes when its ear is
tickled.
5.25. Beflex movement of leg much fainter when the ear is irritated.
5.31. Tries to get up voluntarily. Gk>t up, staggered some steps.
Convulsive movements. Death. Immediately a cannula was placed
122 Messrs. T, L. Bmnton and J. Fayrer on the [Jan. 22^
in the trachea and artificial respiration begun. Sciatic nerve isolated. Irri-
tated by induced current. Eoot twitched when secondary coil was at 57
centimetres.
About 6.30. Electrodes screwed into cord about 2nd and 5th dorsal
vertebraB.
The strongest current of the coil produced contraction of the muscles
of the back, but no contraction of the limbs. The sciatic nerve, when
irritated directly, caused contraction of foot with the coil at 23.
6.50. The phrenic nerve irritated ; no contraction of diaphragm ; vagus
irritated ; heart stopped.
In this experiment the continuance of reflex action on irritation of Uie
ear, and of voluntary movements, after reflex action on irritation of the
eye had disappeared, and almost up to the time of death, are remarkable ;
as is also the paralysis of the phrenic before the sciatic and vagus nerves.
Action of Cobra-poison on the Cirexdation,
In most cases of death from cobra-poison, the fatal issue is not to be
attributed to any failure of the circulatory apparatus ; for the heart
continues to pulsate vigorously, long after all motions have ceased in the
voluntary muscles Qpd the strongest irritation applied to the spinal cord
and motor nerves fail^ to produce the slightest effect. But this only
occurs when the dose of poison is not excessive; and when a large quantity
of it is introduced, at once, into the circulation, the heart is not exempted
from its action, but is, on the contrary, most seriously affected. This is seen
in Experiments LXVIII. and XXYIII., where the poison having been
either injected into the circulation, or absorbed with extreme rapidity, the
action of the heart was at once arrested. But it is to be noted that it is
not paralysis, but tetanic contraction of the heart which is produced,
the poison, in fact, seeming to act as an excessive stimulus ; and this being
the case, we feel less surprise on finding that, in ordinary cases of poison-
ing, the cardiac action may be maintained by the use of artificial respira-
tion for more than thirty hours, as Mr. Eichards has succeeded in doing
in India. The cardiac movements cease much sooner in frogs poisoned
by cobra-venom than in those paralyzed by curare — ^the pulsations in the
latter often continuing for very many hours, or even for one or two days.
They arc also arrested by the direct application of the poison to the heart,
as in Experiment LXXII. Its action seems to be somewhat different in
degree, if not in kind, when applied to the outside of the heart, as in
Experiment LXX., and to the inside, as in Experiment LXXII. ; for in
the former case the pulsations continued for a considerable time, while in
the latter they were instantly arrested, the heart stopping in partial systole
and moderatelv contracted.
The action of cobra^poisou being exerted on the heart of the frog after
its excision, shows that it acts on the heart itself ; and its effect being
very much the same without the body as within it renders it probable
1S74.] Poumo/IntSm Venomout Snakea. 12S
that the ceubvl nerrotu ■yvtem is littls concerned in the arrest of circu-
lation bj the poioon, at least in the frog.
The stoppage of tiie excised heart may be due (1) to irritation of the
inh^ttnrf centres contained within it, or (2) to paralysis of its motor
g^"gH»t or (3) to excessive stimulation of them producing tetanus, or
(4) to the action of the poison on the muscular fibre of the oi^an. It is not
due to the first of these causes; for atropia, which paralyies the inhibitory
g*ng1i*, does not restore the ino\'ement8. The second is improbable, as
the heart does not stop in diastK^ but in systole, and resists distention
bj fluid within it. The third seems the most probable cause, as oue does
not see why the poiBan should arrest the cardiac pulsations at once when
applied to tiie interior of the organ, and not do so when placed on the
oataide, if it acted on tlie muscular fibre, whereas it may readily be sup-
posed that the poison may reach the gan^ia more readily from the inner
aide of the heut — ^though we do not venture to assert that this is the true
explanatitm of the fitcts we have observed.
The inhibitory branches of the vagus are not always paralyzed (Expe-
riment LXYL ; but sometimes the cobra-poison appears to affect them as
well OB the motor nerves ; and ut this it resembles curare, which in small
doeee does not impair the inhibitory action of the ^'agus, but in large
doaea ccmpletely deatn^s it. In Experiment LVI. irritation of the vagus
qnickeoed, instead of retarding, the cardiac pulsations — a circumstance
which indicates that the inhibitory fibres of the vagus were paralyzed by
ibe poison, hot not the accelerating ones.
The oqiilhury circulatitm is not unaffected by the poison. In Experi-
ment IV. of our former paper, the rhythmical contractions and dilatations,
altogether independent of the cardiac pulsations, which Schiff first obsen'ed
in the rabbit's ear, and which were noticed by Ludwig and Brunton in
the vessels of many parts of the body, were greaUy increased by the
injecticm of the poison.
In Experiments T.XTTV. and LXXV. the blood-press vire remained
high after the heart had ceased to beat. This shows that the art«rioles,
or capillaries, must have been much contracted, thus opposing a barrier
to the exit of blood from the arteries into the veins.
Experiment LXVII.
May iltt. — A cutnula was placed in the trachea of a large black rabbit ;
and aotna dried cobra-poison dissolved in water was injected into the hip
at 1.25 p,H.
1.50> The animal shows symptoms of poisoning. Limbs becoming
weak. There is trembling, and the body sinks donn. There is starting.
The respiration is hurried.
2, Befiex action is well marked when the animal is touched. The limbs
seem almost paralyzed ; but the animal moves the head and neck freely. It
mokes efforts to rise, but is unable tn do so. The head falls over ; the
I
124 Messrs. T. L. Brunton and J. Fayrcr on the [Jan. 22,
respiration is getting feeble. The animal seems quit* consdoua, and starts
if touched,
2.4. It ia now quite feeble. When (he (.'omea is touched the reflex
action ia less than before.
2.5, No convulsions. Artificial respiration commenced. The rabbit,
wrapped in cotton, was placed in a double tin bath filled with \nvrm
water. Temperature in reetiun 98°'8.
2.11, Hespiration discontinued for a spac^e.
2.12, Convulsivetwit^'hingsofleg.'i begin. Natural reflpiration has ceased.
ArtiJici&l respiration resumed. Pupils contracted. Reflex action on
irritation of the cornea has ceaeed.
3.16. Since the artiiiciai respiralaon has been resumed there bare bem
no more convulsive twitchings.
2.55, The heart beats rapidly, but vigorously.
Temperature 101°. The bath being rather hot, its temperature
lowered by a little cold water added to it,
2,57. The animal passed a quantify of urine tinged with blood.
3.5. Heart beats vigorously.
3,15. The eyeballs are very prominent ; pupils normal.
3.45. Heart beating u'el!, but apparently not so vigorously as befom
Teperature 100°-5,
3.55. The bath getting told ; a little hot water added to it. The heart
beating more vigorously than at 3,30,
4.20. Heart beatiug well — if any thing, more %'igorously than before.
4.40. Heart beats steadily, but apparently with less vigour. Tempera-
ture lOC-S.
5. Heart sometimes beats steadily 130-140 times per minute. Then
it gets feeble and intermits, and again beats steadily.
5.5, Heart beats more freely. Added more warm water to the bath.
5.25. He-art. beats rapidly but more feebly.
6.35. The same.
6. Heart beating rapidly, perhaps rather more feebly. Temperature
maintained at lU0°-5.
6.10. Heart beating well and more vigorously.
6.30. Heart beating well, rapidly but steadily.
The attendant, being left alone, discontinued artificial respinktion, and
the animal died. The fluctuations in the activity of the pulsations were,
in aU probability, due to the more or less perfect maintenance of the arti-
ficial respiration.
ErptritMni T.XTTTT.
A small rabbit had two drops of diluted cobra-poison injected into the
jugular vein. In 30 seconds he was in convuleions, and in 60 seconds
was dead.
The thorax was opened immediately 1 the heart had ceased to beat, and
was firmly contracted.
1874w] Ponim of Indian Venomout Snaku. ]25
A luge rein flntering the aaricle on the left side was pulsating vigo-
roiulj and rhjthmicallj, though no part of the heart itself showed the
lekat trace of motion.
Experiment LXIX.
JitiM 26, 1872. — Ha]f adiop of cobra-poison diluted nith j cub. centim.
(tf water was injected under the skin of a guincapig, weighing about 450
gTsmmeB (1 lb.).
At 12.13.15 the injection was made. Immediately the animal became
mtieii and cried constantly.
At 12.16 twitching movements began in the limbs.
At 12.1S the *ni'm*l was quiet, and would not move when touched. It
tiien became restless again, and remained so till 12.44.
12.44. The jugular vein was exposed, and J cub. centim. of the diluted
powA was injected into it (•= j drop of poison).
Id kas than 30 secands the animal appeared to be dead.
The thorax was opened, and the heart found to be motionless and the
walls o( oil its cavities firmly contracted. The lungs were ecchymosed.
12^. Electrodes were inserted into the spinal cord, and an interrupted
eoiieDt passed through it. Whenever the current passed, the legs of the
uimal jerked vigorously.
The blood which was collected &om the large thoracic vessels formed a
firm coagulum.
1.22. The cord was BtHl irritable when excited by the induced current.
Experiment LXX.
Jan. 14, 1873.— The heart of a fr<^ was excised. It beat 20 times in
1 minute. Several drops of cobra-poison were then placed upon it, and
it beat 24 times in 1 minute. When seized with forceps and placed in
eobra-p<nson it stopped in systole; but this might be due to the efEect of
the compression by the forceps.
Experiment LXXI.
Prog's heart excised. Beats, 30 in the first minute, 34 in the second.
Cobta-poison applied to it. It immediately stopped, and then began
•gain, but slowly and feebly. Then it beat 23 times per minute, less
otron^y than before. It gradually recovered and seemed little affected,
but stc^iped about 10 or 15 minutes afterwards.
Ei^eriment T.T'TTT.
A cannula was placed in the aorta, and another in the vena cava of a
frog. All branches were tied, the heart excised, and placed in connexion
with H. P. Bowditch's apparatus for keeping a stream of serum circula-
ting through the heart and recording its pulsation by means of a mano-
meter on a revolving cylinder. When fed with pure serum, the heart's
126 Messrs. T. L. Bninton and J. Fayrer on the [Jan. 22, !
contractiojia were regular and strong ; but whenever sertim containing \
dried cobra-poison in solution (in the proportion of abotit two grains J
in three lluid drachms) was introduced into the apparatua the hnart 1
fltopped almost immediately. As vriil be seen front the accompanying /
tracing, it became partially contract«d and gave one or tiro feeble beats, J
but did not dilate, and then remained still, the contraction, however, very I
slowly and gradually ii
nomcler miniiDcteil wilh l.he norli. The tmcingn all mad from right to lell.
1. Tnttdng obtAincd from the htart nipplied with pure aemm bjintwuDf atnbt
2. Trseing of the mme kind, with the addition of the line A, which iodintia the«ra
of the mercoTj. IThe tneing B, giren bj the heart, unks down to tero diiring «h1i
diwtole.
3. Tncnng ginn t^ the heart oEler it had been supplied with aeram oontamiiig a
mull quantity of eobn poieon inMlution. The heart rnkkdea few ineSbctoalattempti^
but can neither contract nor relax, and reniiune still, in a condition midway Iml wiim
oomplete ayitole and complete diaitole. The line A ii the zero to which B woold (ink
if the heart relaxed ooinplet«ly daring diastole.
Experiment LXXHI.
A cat was deprived of coneciousnesB by a severe blow on the head ; and
a cannula being placed in the trachea, artificial respiration vrss begun.
The thorax was then opened and the heart exposed. A solution of dried
cobra-poison in water was then injected into the jugular vein. At fint
the cardiac pnlsations became much quiclier, but they were also atzone.
They next became very small and rapid. Lastly, the right ventricld bfr-
came much distended, and the heart stopped. The lungs became con-
tracted ; and when force was used to distend them they did not expand
equally, but became emphysematouB in spots, so that the exterior of tbe
lung assumed a nodulated appearance. When the right ventricle was
punctured it contracted firmly. No further contraction took place wliea
it was irritated by the direct application of a Faradic current. Xlie blood
coagulated.
1874.] Pauon of Indian Venonuna Snakes. 127
Expa-ittuntLUXIV.
A ''»"""1» WM placed in the carotid of a dog and eonnected with a
kjmi^inphioii.
Hmii blood-pmnire. Pulse
Xinu. ■"ill'"" per miiia(«,
1^ 150 144 Injected some cobra-poison dis-
solved in water into the sciatic
vein. The pressure rose to 165,
165 and then sank in 7 secondB to
136 135.
1.45 60
1^ 67 ■ . Fsces passed. A dot formed in the
fantiiila and had to be remored.
1^ 70
About 1JB6 8C . . Injected some more poison.
1^1 20
1.69 55
1.601 70 .. act again formed.
2J2 76
2.7 85
2.10 85
2.1B 80 . . I«ga loosened ; but the animal did
not move. Convulsive move-
ments occurred ahnost imme-
diately afterwards.
2.17^ Cornea still sensible.
2.18 85 . . Convulsive movements.
2.19| 90 . . Convulsbns.
2.20i 80 80 No movement.
2.201 90 64 The pulse hera suddenly changed
from 80 to 64 ; and at the end of
every third beat the pressure
sank 25 millimB., while at each of
the others it only sank 5 millims.
2.21 j 98 . , Ueigbt of each single pulse-wave is
now 10 millims. instead of 5, and
every now and then it sinks 30;
but the number of beats aft«r
which it sinks is not now so re-
2.211 100 64 Convulsions.
2.22 j 105 . . There were now 8 pulsations, and
then an interval of 6 seconds,
during which the pressure went
downto 43tuillinu. Five bests
128 Messrs. T. L. Bruntou and J. Fayrer on t/ie [Jan. 22,
Mean blood -preuure. Pulie
Tims. million. pei nuQute.
moreraisedittol20. Height of
each pulse-wave about lamillitna.
2.29 30 . . The pulse ha* beea gettiiig smaller
aiid smaller, aud the intervals
longer and longer ; it is now im-
perceptible.
2.30 30 . . The pressure still seems at 30, not-
withstauding the imperceptibil-
lity of the pulse.
2.45 The heart was cut out. It stiU
eontracted wheu irritated.
The injection of cobra-polaon here caused a diminution of the blood-
pressure at first ; but a further injection agaiii raised it. In the latter
part of the experiment there is not the slightest trace of failure of the
heart's action, but, on the contrary, every evidence of powerful action.
"When the respirations failed, the heart became slow from irritation of the
roots of the vagus by venous blood : and the pulsations were gradually
weakened by the same condition. The fact that the blood-pressure sank
slowly and did not fall below 30, even after the heart bad almost entirely
ceased, shows that the arterioles were much coatncted.
Erperiment LXXV.
A cannula was placed in the carotid artery of a rabbit and connectad
with a kymographion.
The blood-pressure was 75 millims. of mercury. One cub. centim. of
a 2-per-cent. solution of cobra-poison was injected into the jugular Tein.
Almost immediately the animal began to struggle, and the pressure raae
to 95. It remained at this for a minute and then fell. The float unf<n^
tunately stuck, and the curve it should have described in falling was con-
sequently lost. On again getting the instrument to work, the pressure wai
found to be So i and this continued, although the heskft had ceased to beat
and the thorax was opened. On cutting across the aorta, the pressure fell
to lero, showing that it had not been due to any clot in the vessel.
In this experiment the poison seems to have caused tetanic contraction
of the heart, and also of the arterioles. The permanence of the prawon
at 25, notwithstanding the stoppage of the heart's action, can only Iw
ascribed to contraction of the arterioles preventing the escape of tdood'
from the arterial into the venous system.
Eavretion of Siuilce-poiton.
We have made only one or two experiments, ourselves, on the excietion
of cobra-venom ; but, from the data a&orded by the experiments and ob-
servations of others, we consider that it is excreted by the kidneys and
"Miunary glands, and probably also by the salivary gUuds and t
^74.] Paiion qf Indian Venomaui Snakes. 1%
emtvuie of the ttoouich. A case leported by Mr. Shircore, olGBlcutts,
whidi an inEuit, suckled by its mother after she had been been bitten
' a snake (species unknown), died in two hours after it had partaken of
e milk, shows that the poison is excreted by the mammary glands, and
ith oonsideraUe rapidity ; for t^e child took the breast before any marked
mptoms had occuiied in the mother*. Its excretion by the kidneys ap-
iars from an experiment of Mr. Bichards, of BaUisore, who found that
me urine from a dog poiscmed by the bite of a sea-snake (Enhydrina
ngdUnsii) killed a pigeon in 22 hours after being hypodermically in-
ctedf. Scnne saliya, which we obtained from the submaxillary gland of
dog poisoned by cobr^-venom, had no effect when injected under the
3n of the thigh of a lark ; but Mr. Bichards found that one drachm of
16 greenish liquid which flowed from the mouth of a dog poisoned by
(bnirTenom kflled a pigeon in two hours. As this fluid flowed con-
BJktij from the mouth, and the animal was paralyzed and motionless, it
ems probable that, notwithstanding its colour, it was saliva and not bile.
As the poison-glands of the snake are modified parotid glands, we
Lould naturally expect the poison to be excreted by the salivary glands ;
id we think it possible that the immunity which poisonous snakes enjoy
om the effects of their own poison or that of another species (an im-
onity which is not shared by innocuous serpents, nor even by small in-
Tiduals of a venomous species poisoned by a large dose of venom) may
due, at least in some measure, to their power of excreting the inocu-
yi venom through their own poison-glands. . We have, however, had
opportunities of trying whether venomous serpents, after extirpation
heir poison-gland, succumb to the bite of others in the .same way as
tcuous ones.
I ihe Means of preventing Death from the bites of Venomous Snakes.
the case of all poisons, snake-venom included, there is a dose which
uffident to kiU ; and animals may recover from it even after the
toristic sjrmptoms of the poison have been distinctly manifested.
as been clearly shown by Hermann that the real dose of any poison,
ither words, the quantity which is actually circulating in the fluids
erating on the tissues of the body, depends on two factors, viz.
idity with which it is absorbed, and the rapidity with which it
ted. If absorption goes on more rapidly than excretion, the
ocumulates in the blood and exercises its lethal action ; while the
in actual circulation may be reduced to an infinitesimal amount
ived of all power for evil, if the excretion can keep pace with, or
re rapidly than, the absorption. Thus it is that curare kills an
len introduced into a wound ; for the poison is absorbed from the
TO rapidly than it can be excreted by the kidneys. If placed in
ch, curare has usually no apparent action whatever ; for it is
vtophidia, p. 43. t Indian Mcdioal Guette, Maj ], 1873, p. 19.
excreted in the nrme m qmcUj-w it ia ilMxbed bjr Hie g
if sbMopticKi be quickened b7 ii
giving it on an emptf tUmaek, onme wiU have tiie ■
it is placed in a wound or itgeeted into the dnolatiai. A liko molt it
obtained by arresting its vsentiao, eiUterby ligaturing tiia nml tchA
or extirpating the kidneys. Bnake-nnom ■■ «bo poisonoaa lAen •liMftad'
by the mucous membrane of the etcmach.
On the other hand, when we wish to prerent 'tin aoeiinuilatfata cf if
pcnson in the blood and thus toanest its acti(»i,we mnat either IsMsn ttt
absorption, quicken its ezoetion, or comlnne the two means.
In the case of curare tlie former of these issoffioient; and all tlwlaff-
effects of the introduction of this pmstKi into a wound majr be praTsntadlj'
applying a ligature between the woond and the heart, and only loModag''
the bandage occaaionally, for an instant or two at a time. ISift mtUb"
obtains in snake-poisoning. In this way only a litUe of Qia pcutM it'
absorbed each time the li^tnre is slackened, and this is ezented \^ tfcs'
kidneys before another qnantity is absorbed. If tjie poison can be nnimd
from the wound itself by other means, instead of "i^Vrng the wbole of it
pass through the drculatioji, the danger it causu will, of oonrsa, be •oooar
over. Our power to quicken excretion is, in most casee, modi leaa tiisi
that to retard absorption ; and it is therefore on the latter that we mainly
rely in cases of poisoning in general, as well as snake-bites in particolar.
The ^'arious methods of met^anically arresting the introduction of t^
virus, by eiciBion, cautery, and chemical agency, bare been fully discussed
in the ' Thanatophidia of India ; ' and we purpose now to consider its excre-
tion or removal from the organism.
Before doing so, however, we must inquire whether its removal is likely
to be of any service or not ; for, aa we have already pointed oat in oor
previous communication, the action of the poison may be of two kinds.
Ist. It may resemble curare in desti-oyiiig the power of the nervous
system so long aa it is present in the blood, but leaving it in a condition
to resume its functions as soon as the poison has been removed, 2nd.
Its action may be identical with, or similar to, that of a ferment, deccnn-
posing or altering the nervous and muscular tissues in titn (in somewhat
the same way as the pancreatic or gastric ferments would decompose them
if they had been placed in the intestinal canal), and thus rendering them
utterly incapable of ever again performing their functions.
If the action of the poison is of the latter kind, no treatment can be
expected to be of any avail if the dose has been large ; but if it is of die
former, we may still entertain a reasonable hope of averting a &ital resnlt,
even when the dose of venom has been large.
We have shown in our previous communication, that, by jaoKoa' of
artificial respiration, life may be prolonged for many hours, and time
thus afforded for the excretion of some of the poison ; but the means at
our disposal have not enabled us to maintain respiration sufficiently long
1874.] Poimm of Indian Venomout Snaket. 131
to show ua whether the nen'ous and muaoul&F BjatemB regain their
fiuLCtion after the excretion of the poiBon has proreeded far enough.
The ezperimeDts oi Mr. Vincent Richards, and of a roramittce appointed
b^ the Goremment of India in Calcutta, at our siiggestioti, to investigate
the use of artificial re^iration in death hy snake-bite, being performed
under more favourable auspices, have afTorded us tbe data which ve were
unable to obtain from our own. In one instance, a dng «as bitten by a
sea snake {Enhydrina bent/nUnnit), and, t»o hours aften\'ards, died in
convulsions. Artificial respiration wha commenced ; but, four hours after-
wards, the application of a galvanic currenr caused no muscular contrac-
taons ; the eyes wore diy and glazed, and the bodr naa cold. Ke<ct morn-
ing, about sixteen hours after tbe apparent death of the animal, reaction
commenced ; the application of a galvanic ciim:nt again caused movements
of the body and expulsion of urine, and the bov\els acted spontaneously.
In five hours more reaction seemed e)<tablished and went on increasing ;
the animal appeared as if it would recover : the eyes lost their glazed ap-
pearance, tears were secreted, and a greenish-looking fluid flowed from
the mouth; reflex action became reestablished, tJie eyelids closing when
the cornea was touched or when water was jioured into the eye. At-
tempts to swallow were made when n aler u as poured into the mouth ;
and tlie application of a pan of hot charcoal to the chest caused con^-ul-
sive movements all over the body ; and these also occurred spontaneously.
Xhe animal also became more or less sensible, and the eyelids twitched
when the finger was merely brought near the eye.
These phenomena show that the muscles, the motor nerves, the secreting
nerves, the spinal cord, and the cerebnun had all recovered their functions
to a certain degree, after it had been completely aboLshed for sixteen
hours. This we think would not have been the case had the poison
acted by decomposing the tissues in the manner of a ferment; and we
are therefore inclined to hope that, like curare, it acts only while present
in the system, and that its injurious effects may be arrested by its removal.
Notwithstanding the fair promise of recovery which the use of artificial
respiration gave in this instance, the heart became weaker, and the animal
died 24 hours and 35 minutes after its first apparent decease. Nor has
the Committee been more successful in its further eiperimenta, although
life has been prolonged for even 30 hours. This result shows that, at-
tiiough artificial respiration may still prove useful in sustaining life and
affording time for the use of other measures, it alone is not likely to be of
mnch service in preventing death from snake-bite, except in those cases
where the quantity of poison is just enough to kill and no more.
It is evident from the length of time during which life may be main-
tained without the animal ultimately recovering, that the excretion of the
poison is very slow ; hut ne at one time thought to quicken it by the em-
ployment of diuretics and sialogogues, and to prevent reabserption by
drwning ofF the urine and saliva constantly. We also proposed to wash
333 On the Poison of Indittn Venoifwus Srtakes. [Jan. 29j
out the Btomach from time to time, in order to remove mit poison n-luGt
might be eJtt-'reted through the gastric walls, keeping it partially fiUej
with milk or other nutrient fluid duriog the intervals, in order to snstajii
the streugth of the animal.
We are by no means certain that sMne of the^ methods maj- not provtf
nsefal adjuncts : but as our hope of stimulating excretion, by the siliran-,'
^ands at least, baa been madt iMMoed \iy oar diaeamj Oat ttw poiMK
paralyzes the nerves of Becmtion, we an inifned to tUnk Unt^ jiamt,»ji^
the readiest method (rf Tenuning tie peiMa fram die body imj be to
allow it to flow oat tioag witb tlie Uood m wlikh it ia < '
supply the place of the poiaoned Uood tlma witlidnwii hj
(osion.
The greater part of the pcisoD pnemt in tiie system ia probaUj co^
tuned in the blood, and only a smaiD propmiian in tlie tusDea ; toe fne ct
us (I>r. Fayrer) has found that a few drops of the Uood of a dog t^lim
by the bite of a cobra or Dabata caused death in serenty-^re minalM,
when injected into the thigh at a fowl (' Thanatophidia,* pp. 80, 8^
119,120). By removing as modt blood as coold be taken without ei^taw
gering the life of the animal, a great part of tiie ptnsoD would be wit^
drawn from the system ; and, probably, any harm from the copious bleediiw
would be prevented by transfusing fresh blood immediately afterwards.
We hare tried one or two experiments with transfusion ; bnt they hare
hitherto been unsacceasful.
We are therefore by no means confident that death may be prevented
by the combined use of artaficial respiration and transfusion ; bat we
think that ther present some chance of success, and that, at all eventa,
the suggestion is justifiable on scientific and rational grounds.
The treatment of animals poisoned by cobra-TiruB by the hypodermie
injection of liquor anunonis has been frequently tried in India by one of
OS (Dr. Fayrer) (vide Thanat. pp. 89 rt »ey.), and also by Mr. Kchaida,
of Balasore, and by ourselves again in Loudon, on sevend occasionB.
The alkali has been administered internally, injected into the Bxedlu
tissue, and also into the veins, over and over again ; but no benefit has
resulted. The objection has been made that experiments of this nature,
made on animals, are not conclusive in reference to the probaUe action
of the agent experimented with on human beings ; bat this objectioQ ata
hardly be considered valid in a physiological point of view.
At auT rate the trials that have been made, of this mode of averting ttw
lethal efiectfl of the poison, in India by Dr. Hilson, Civil Surgetm of
Moradabad, do not afford any indication that the intravenous injection of
liqaor ammonia was followed by any diminution of the effect of tbe
poisons, the man in both cases having died* (vide ' Indian Med. Qaaetta,'
Oct. 1873).
The same may be said of other reputed antidotes, such as :— Tanjote
* It is unneoeawry to occupy time by describing in detail the Tarioos snlMlBaMl
1874.] On I/k Lymphatic Sj/slem of the Lumjs. 133
piD Rnd other prepu»tionB of araenic ; the hypodennie injection of Kqmw
potaiMB; quinine, ipecaciuiiha, Aritloh^ia iadica, and a vuiety af other
diuga, geaeisll; of > vegetable nature, and enjoTing a lai^e amount of
popokir confidence : all, when brought to the test of carefully conduct«d
experinunt, failed, as might have been expected, to give any favourable
reanlt.
It veema almoat auneceuary to allude to the so called Boake-stones ; they
are powerlWB for good orevil. They have also eujoyed much confidence ;
bat when Butwiitted to the test of impartial experiment and obeenation,
liteir virtnes prove as unreal as those of the antidotes above mentioned.
Witlt Teference to the mechanicsl methods of preventing the entry of
the p<Mson into the circolation after a bite, we think that the speedy
application of an elastic cord (such as is used in bloodless operations)
roond the limb, combined with the application of cups attached to an
exhauBting-«yTing8 or pump*, might be of advantage, and that it might
be made of genenl application in India.
January 39, 1874.
JOSEPH DALTON HOOKEB, C.B., President, in the Chair.
The Presents received were laid on the Table, and thanks ordered for
titem.
The foUowing Papers were read : —
I. " ContribationB to the Normal and Pathological Anatomy of
the Lymphatic System of the Lunge." By E. Klein, M.D.,
AfisiBtant Professor at the Laboratory of the Brown Institu-
tion, London. Commnnicated by Professor J. B. Sanderson,
F.R.S. Received November 13, 1873.
I propose to give in the following pages a summary of an investigation
of the lymphatic system of the lungs, in the uonnal condition as well as
in chnmic seccHidary inflammation, undertaken in counexion with the
pathological inquiries of Dr. Burden Sanderson, for the Medical Depart-
ment of tJie Privy CouncU. The research will be published at length
daring the course of the next year, in continuation of my work ' On the
Anabmy of tjie Lymphatic System,' of which the first part, " Serous
Uembnmes," has recently appeared. The present commimication is made
with the ^iproval of the medical officer of the Privy Coimcil, Mr. Simon.
A. Normal eonditiong.
(a) The endottielinm of the surface of the lungs consists, in the normal
(animal, TBgaUbla, and miiieral) Aat hare been idminutered u antidotes. Farti-
oolan maf be found in Uw 'Thanatopliidia.' where the detail* of eipnimeaU eon-
doetod tor the invMtigstion of their actions are reix>rded.
low been conatructed.
condition, of polyhedral oeUs (not 1
arranged in a single layer, lliii ia well teen m g
itinctly in rabbits, rats, doga, and cats. If Hie long u not d
endothelium of the surface vwy much resemblei an ophheGnm, As fldi
being polyhedral, or in the form of short coIomnB ; tltey kv maikaAf.
granular, and have distinct nodd. Sren in the modentelj dittgidtl
lung, the endothelium of thepleora ptdmoniim la lij no meana of tka i^ae
morphological character aa that on the costal pleura. Between the €adiK
theUum of the one and that of the otJter organ there exista dte tarns dii^:
f erence as between that of the orary and that of the peritoneam— tha 0^-
conai sting of polyhedral , or shortly colnmnar.graoitlaroeUs witii nrjmaAti
nuclei, the other of very flattened, almost hyalme, endotlieliBi rVitiri.
(b) The pleura pulmonum ia a rery thin oonnectiTe-tiarae mendBau^
prorided, like other serous membranea, with a rich netwoA of dMib
fibres. In the lungs of the rat, rabbit, cat, and dog the pleura pofawnBa
aeems to consist, for the moat part, of elastic netwtnb. In Ae mafan^
there is generally one layer of flattoned connective-tissue ompnadea to bt
found.
Beneath the proper pleural membrane, there .exists, in flie gmamplg, a
membrane which cousiatB of non-striated muscular fibres, arranged in
bundles which form a meshwork. In the normal condition the bundlea
are relatively thin, and the meshwork which tlipy form has elongated lai^
meshes. In the distended lung the inesliea nre of n much greater diameter
than in the collapsed lung ; in the latter they form a more continuous mem-
brane. The muscular bundlea have, in geiu-ml, a radiating direction from
the apex towards the basis of the lung ; and it is further to be noted that
they are most abundant on the external surface, viz. that directed towards
the anterior wall of the chest, and the internal surface, viz. that directed
towards the mediastinum ; whereas on the posterior surface the bundlea
are scanty, and become more and more so the nearer the vertebral column
ia approached. This distribution of the muscular tissue is therefore in
perfect agreement with the proportion in nhich the different parts of the
Inng participate in the respiratory movement, the fibres being most ricUy
distributed over those parts of the pulmoaary surface which are subject to
the greatest extent of excursions, and vict vers&. In rats and rabbita, aa
wdl as in cats and dogs, bundles of unstriped muscular fibres occur spa-
ringly ; at any rate there are none on the posterior surface of the lung of
these animals. As soon as the superficial parts of the lung become the
Beat of a chronic inflammatory process («. g. tuberculosis, chronic pneu-
monia), the muscular bundles increase in breadth and number to aoch
a degree, that they form a continuous membrane, chiefly in those partv of
the surface which correspond to the diseased portions of the lung.
1. Suhpleural lympTiaiict. — The meshes of the muscular membtmne of
the lung of guineapigs are lined by a single layer of flattened endothelial
cells, constituting, in fact, n coniniunicatiiig system of lymphatic sinnaea.
)874.} Me Lymphatic St/»tem of the Lungt. 136
I nil this system of lymphatics the intermMamlar or pUvral lymjthaiie*.
In the distended lung of the guineapig, these pleural lymphatic ainuses
■re Men to be covered by hardly any thing but the endothelium of the
pleur&I cavity, between which and the cavitieB of those sinuses a free
commonication exists by means of true stomata ; so that tlie endothelium
lining the sinuses is here direi-tly continuoux with that oF the pleuntl sur-
fiuse. In every case of chronic pleuritiB induced by injecting irritating
BobBtoncee (such as products of arute and chronic pyiemic processes, pro-
ducts of indurated lymphatic glands ). an active geimiuation of the endothe-
tinm anmnd those stomata takes place. This genninadon extends uot
(Kily to the endothelium of the neighbouring parts of the pleural surface,
but also to the endothelium of the intennuscular lymphatic sinuses. The
Tslatioii between the cells of the membrana propria of the pleura pulmo-
nam. and the endothelium of the surface is similar to < hat already described
by me in other serous membranes, the celJn of the jirojiria throning out
processes, which project between the endothelial elements of the free buf-
£aoe, thus forming pseudostomata. The pleural lymphatics stand in
communication with lymphatic tube?, which He in grooves, the arrange-
ment of which corresponds with thiit of Ibe most superficial groups of
alveoli of the lung. These may be called the Kiil>2>leiirnl hjmpluUKt ; they are
provided with valves, and form a network of anastomosing Ivmphatic ves-
sels. The larger trunks run along the ligamcnta pulmonum towards the
root of the Inng. This system of Ivmphatic vessels is best developed in
tbe long of the dog, in which it has been described by ^'y wodiMff ; it is
also well developed in the lungs of rabbits and cats. It receives lympha-
tic brandies, which take their origin betneen the alvcoU of the superficial
portions of the lung. The mode of origin of these iuteralveolar lymphatics
is that already described in my published work. The septa of the
alveoli contain branched connective-tlBSue corpuscles ; the spaces in which
these cells lie, forming the Ivmphcanalicular system, open into the cavities
<rf the interalveolar lymphatics, with the endothelium of which the cells
<rf Uie lymphcanalicular system are in direct continuity.
2. Ptrivaaeular l^mphalift. — Besides the system of subpleural lympha-
tics, the lung contains two other systems -. of which one takes its origin
in the alveolar septa from bnuiched cells exactly like those previously
referred to. The lymphatic capillaries of this system lead into vessels
that accompany the branches of the pulmonary artery and vein ; they run
cdther in tbe adventitia of these vessels in twos or threes, anastomosing
vrith each other, or the blood-vessel is entirelr, or only half, invaginated in
a lymphatic vessel. The branched cells of the alveolar septa, from which
the capillaries of this system of lymphatics (which we will call the
perivaieular lymphatici) originate, have an important rclaticm to the epithe-
lium of the alveoli ; for they send a process, or a greater or less portion
of their body, between the epithelial cells into the cavities of the alveoli.
These represent pseudostomata, as describi-d by myself for the serous
136 Dr. £. Klein an the Anatomy qf [Jan. 29,
membranes. As these branched cells have a corresponding lymphcuiali-
cular system, it is easy to understand why Sikorski, in his experiments,
found that carmine entered freely from the cavities of the alveoli into the
interalveolar lymphatics. But there is no other communication between
the caWties of the alveoli and the lymphatics than by means of these
pseudostomata. It can be easily understood that the pseudostomatoua
canals (viz. the canal in which lies the process of a cell projecting freely
into the cavity of an alveolus, and the lymphcanalicular system, in whidi
the interalveolar branched cells lie) may become occasionally distended, «. g»
in inflammation, by exudation, or by migratory cells. In fact, it must be
assumed that cells, such as are produced by catarrhal inflammation of
the air-passages, migrate ^m the cavities of the alveoli into the in-
teralveolar lymphcanalicular system through those pseudostomata ; and
the same assumption must be made for the well-known large granular
mucous corpuscles, in many lungs, containing carbon particles, inasmuch
as similar cells are found in the interalveolar tissue.
3. Peribronchial lyinphcUics. — The third system of lymphatics is com-
posed of lymphatic vessels which are chiefly distributed in the adventitift
of the bronchi. I shall therefore call it the system of perihnmMal
lymphatics. The vessels of this system are usually distributed around the
bronchi, anastomosing with each other, and especially with the perivascular
lymphatics. The vessels of the peribronchial system take up capUlaries,
which originate in the mucous membrane of the bronchi and penetrate
through the tunica muscularis of the bronchi. These capillary branches
originate in the usual way ; t. e. their wall is continuous with the branched
cells of the mucosa, which cells in turn penetrate, as a nucleated reticnlmn,
between the epithelial cells of the bronchus, and project on its free surface.
From this it may be understood how particles can penetrate from the
cavity of a bronchus into the peribronchial l3rmphatics, as in the experi-
ments of Sikorski. The lymphatics are always most numerous cm that
side of a bronchus which is directed towards a branch of the pulmonary
artery. In the course of each bronchus, especially those that possess only
a thin muscular tunic and no trace of cartilage, there are generally several
vasculated lymph-follicles to be met with, which are placed in continuity
with the endothelial wall of a lymphatic vessel, in such a manner that
they are surrounded by that lymphatic vessel, in the same way as the
lymph-follicles of Peyer's patches are by their lymph-sinuses. These
follicles, already seen by Dr. Burdon Sanderson, extend up to the tunica
muscularis ; in some instances they are to be traced through this latter into
the mucosa. They always lie in the wall of a lymphatic vessel, between the
bronchus and the accompanying branch of the pulmonary artery. They
are of different sizes, and are generally spherical or elliptical ; sometimes
they represent merely a cord-like thickening of the wall of the lymphatic
vessel. In the lung of the guineapig these perilymphangial follicles are
very numerous ; they are not so numerous in rabbits. It can be proved that
1874.} tHe Lgmphatie System oftheLungi. 137
% amitant growth uid reproduction of these follicles is going on. The
lymphktic Teasels of the two last-mentiooed sjatems anftBtoinose with
each other in the ligaments of the lung, and fin&lly enter the bronchial
Ijmphatic gbuds,
B. Paiholoyieal condiiiont.
I have alnaij mentioned the germination of the endothetium of
tiie surface, and the hypertrophy of the muscles, in chronic diseases of
the long.
In many chronic infiammatory proeeases of the lung (chronic pynmia,
artificiat tuberculosis, chronic pneumonia) the pleura pulmonnm becomes
tite seat of nodnles of rnrious sicea and shapes. Generally they are more
(V less ronnd, and correspond in position to those superficial portions of
tita lung ^lich have become the seat of an inflnmmatory process. These
nodules of the pleura are due to a very rapid proliferation of the branched
oonnectave-tiBsue corpuscles, simultaneously with an increase of fibrous
ConnectiTe tisane, this latt«r fact being very obvious when the nodules
haye reached a certain age. As long as they are small, they show merely
an abundance of cellul^ elements; in their later stages they become
richly supplied with capillary blood-vessels.
Lungs of guineapigs that are far advanced in the process of artificial
tnberouloaia {%, e. where the bronchial glands have already become the
•eatof cheeay deposits) show auperfidal nodules, which are in direct con-
tinuity with the subpleural lymphatics. In horir,ontal sections through
audi portions of the lung, one tinds these lymphatics filled with lymph-
oorpuades, iriiile at a later period they are occupied by an adenoid reti-
cnlnm, the meshes of which contain lymph-corpuscles, and which is in
direct continuity with the endothelium of the lymphatic tubes. The no-
dules themselves represent a network of cords, which very much resembles
adenoid tissue. The meshes of this network of trabcculce are the alveoli,
which, at an early period, contain a few lymphoid corpuscles, while the
epitJielinm is, at the same time, in a state of germination, the individual
cellt being swollen and the nucleus in a stato of division. At a latcrperiod
the alveoli are filled with small lymphoid corpuscles, while the epithelium
of the alveoli is no longer to be distinguished as such. The blood-<'apil-
laries belonging to these alveoli have undergone some remarkable changes,
of which I shall speak at length afterwards; at present I will only
mention that at a later period they are no longer permeable for the blood.
Hiese interalveolar trabccnlo) of adenoid tissue, forming the framework
of the superficial nodules, are developed from the branched connective-
tissue corpuscles of the alveolar septa. The same process extends to the
Bubpleuial lymphatics, originating from these interalveolar connective-
tissue corpuscles, in such a way that these lymphatics become con-
verted into cords of adenoid tissue connected with their endothelium.
Consequently Uiese lymphatics become converted into cndolyiuphangial
cords.
188 Dr. E. Klein on the Anatomy of [Jan. 29^
If one examines the lungs of a guineapig which is so &r advanced in
the process of artificial tuberculosis that the bronchial glands contain
cheesy deposits, one can distinguish with the naked eje two kinds of
morbid structure on the surface of the lungs : —
(a) Translucent structures of a circular or irregular shape, sometimes
projecting slightly above the surface, generally isolated, but in some
instances confluent, so as to form patches. The smallest are of the size
of the head of a small pin ; some of them are three, four, or several times
as large. In some lungs only the large structures are to be found ; the
larger kind have generally a yello\ii8h centre.
(6) Opaque patches of considerable diameter projecting above the sur-
face of the lung, some of them relatively very large (about •}■ to -jl^ of an
inch), quite white, and very firm. On sections through the lung one findtf
that the first kind of structures correspond with cords provided with lateral
nodular swellings, which accompany the branches of the pulmonary artery
and vein. The second kind of structures correspond with nodules and
patches which are irregularly distributed in the tissue of the lung. On
microscopical examination it is seen that the first kind of structures are
perivascular cords of adenoid tissue, representing the follicular tissue
which is found in the walls of the peribronchial lymphatics in the
normal condition. Many of these perivascular cords or nodules are
supplied with a system of capillary blood-vessels. The second kind of
nodules, or patches, are seen to consist, on microscopical examination, of
a framework of trabeculao which corresponds to the intend veolar tissue ;
they represent trabecula? of adenoid tissue which are in continuity with
the perivascular cords first mentioned. The meshes of this network are
more or less filled out by cells lying in the spaces that were previously the
cavities of the alveoli. The question arises. How do these two kinds of
morbid structures develop, and what is their ultimate fate ?
If one studies sections of lungs that possess very few of the first
kind of cords and nodules, one comes across a number of the lymphatic
vessels that accompany the branches of the pulmonary artery, con-
taining more or less numerous Ivmph- corpuscles. In addition to those
just mentioned, one is able to find lymphatic vessels, the endothdiom
of which is in contiuuitv with a thin short cord of adenoid tissue that
stretches along the outer wall of the lymphatic, or (as may be seen in some
places) projects into its ca>dty, thus connecting the two endothelial walls
of the lymphatic ; in other words, we have here a peri- as well as an
endolymphangial growth of adenoid tissue, connected with the endo-
thelium of the Ivmphatic. From what I have shown in the case of the
serous membranes, there can be little doubt that the above-mentioned
tuberculous cords of adenoid tissue accompanpng the blood-vessels are in
reality only peri- or endol}inphaugial outgrowths of the endothelium of
the lymphatics. It is important to state that, at the same time, the fol-
licles of the bronchial adventitia increase in size, and also that a perilym-
1874.] the LgByihoik SyMtem of the tungt. 139
ph&ngiftl n«w growth takes place on the peribronchial lyupliatica. From
the study of the nonnAl lung, it can be attcertained that not all the lai^
bntDchea of blood-Tesiets are accompanied bv lymphatics, and not even
one and the same branch for its whole length, but that in some places
they are only Burrounded by branched connective-tissue corpuscles, which
may be said to belong to their adveutitia. In a given case, one 'ndll not
be able to determine whether a certain tubercular cord hae developed by
the increase of these adventitial cells, or whether it has developed from
the endothelium of a lymphatic, either as a peri- or endol\-mphangial cord ;
for the fully developed cords have quite the same rclatiou to the blood-
vessels as if they had developed in their adventitia.
I have already mentioned that the growth of adenoid tissue in the
branches of the subpleural lymphatics extends to the connective-tissue
corpuscles between the alveoli. Exactly in the same way we see the pe-
liTascular adenoid cords spreading between the alveoli ; that is to say, the
perilymphangial growth of tracts of adenoid tissue extends from the Ivm-
pbatics to the interalveolar branched cells, with which the endothelium
of the former is indirect continuity.
The first points at which the tubercular perivascular cords of adenoid
tissue make their appearance are tho ultimate branches of the pulmonary
artery and vein, whence they spread along the lymphatics towards the
larger branches, as well as towards the interalveolar branched cells. In
general the growth in the first direction (that is, towards the larger
bntnchea) goes on much more abundantly and rapidly than in the other
direction.
It is an important fact tliat I have constantlymet with the following con-
dition of the tuberculous lungs of guiueapigH : — The ultimate branches of
tiie pulmonary artery show a genniuatioa of their endothelium, which is
already recognizable in the earlier stages of the disease, at a time when
perivascular cords are only rarely to be found. If tho process advances, the
germination of that endothelium reaches such a degree that the cavities of
the blood-vessels are almost filled with its products, only a very narrow
central canal being left free. In later stages, the tunica media of the
smaller and middle-sized vessels, that are provided with perivascular cords,
becomes very much thickened, and splits into laminse, between which lie
accumulated lymphoid cells, either free or contained in a reticulum. In
many places it can be shown that the adenoid tissue of the perivascular cords
gradually grows towards the cavities of the vessels, and finally assumes the
whole portdon of the vessel into its substance. The chief fact of import-
KDce, however, is that the capillary blood-vessels of those interalveolar
trabeculaa, into which the perivascular cords have penetrated, have become
converted into soHd nucleated bands and threads, which are in continuity
with the surrounding reticulum. These threads, although they appear
aoM, must be taken as still permeable by fluid substances ; for in lungs
the pulmonary artery of which had been previously injected with a cold
140 Dr. E. Klein on the Anattmy of [Jan. 29j
solution of Berlin blue, the cavity of many of the capillaries in the neigh-
bourhood of those iuteralveokr trabecule stops short, but the injecting
material can be traced into the nucleated filaments which enter those tra-
becule. From the study of a great number of specimens, taken from
lungs in different stages of the process of artificial tuberculosis, I haye
reason to believe that the first parts which undergo inflammatory changea
are the ultimate branches of the pulmonary artery and the capillaries next
to them, and that the morbid process extends from them to the corre-
sponding lymphatics.
I have already mentioned that, where the alveolar septa become
thickened, the epithelium of the alveoli becomes gradually changed, bo as
completely to fill the cavities of the alveoli. By this means nodulttr
or patch-like structures are formed, which may be called secondary patchea.
It may be said, in general, that the epithelial cells proliferate : tiiey en-
large; their nuclei divide ; and then the cells themselves divide. In many
alveoli there appear, besides isolated epithelial cells, with or without car-
bon particles in their substance, numerous small lymphoid corpusdea*
In some of the alveoli the enlarged epithelial cells become fused together
to one large ma«8 of granular protoplasm, which contains a number of
nuclei in its periphery ; this represents, in the true sense of the term, a
" giant cell." We may therefore say that, at an early period, these patches
consist of trabecuhe, which represent the thickened interalveolar s^taand
their meshes (the alveoli), and that the latter are filled either with small
cells or \vith giant cells, or rather with multinuclear protoplasmic cylin-
drical masses. These secondary patches gradually increase in size, by
the extension of the adenoid metamorphosis of the alveolar septa and tiie
changes of the capillary blood-vessels, indicated above.
A perivascular cord may become furnished with a number of lateral
nodules of adenoid tissue from the assumption, by adenoid interalveolar
cords, of the contents of alveolar cavities into their own tissue. Where,
however, the alveolar cavities contain giant cells, other remarkable changes
take place. These are as follows : — The cylinders of multinuclear proto-
plasm grow and divide into a number of giant cells, which gradually be-
come converted into a tissue to a certain extent resembling adenoid tissue,
but differing from it in many respects. Thus the giant cells give origin
to a more or less regular network of nucleated cells, which, consisting at
first of granular substance, soon assume the appearance of a more or less
distinct fibrillar substance ; in their meshes lie only a limited number
of lymphoid colls. This tissue spreads very rapidly, and finally undei^goes,
from the centre outwards, a fibrous degeneration, which becomes the seat
of cheesy deposits.
Different lungs are somewhat different in this latter respect. In some
cases iho transformation of the giant cells into a network of nucleated
cells goes oTi very rapidly ; and then the cheesy metamorphosis is also soon
eslablislioJ. In other cases the growth of the network of nucleated cells
1874.] the Lj/ngihatic Syttem of the Lungt. 141
ba> a Tory long dnntion, and consequently the growth of the secondary
patdiea remains acHve for a long time. The network of nucleated
oells is, at no period of its development, such a delicate reticulum as in
the adenoid tdsBOe, nor does it contain lymphoid corpuscles so r^ularly
ai this latter. Moreorer the adenoid tiHSue of the periraacular cords
or their lateral nodules never becomet the leat of a jibrotLi or tket»}f
mttamorphoni. The more the lung has advanced in the process of
aitifidal tnberculosiB, the more do we find the tissue of the lung,
in the ncdghbooriiood of the primary and secondary nodules, undergoing
inflammatory changes — consisting in thickening of the alveolar septa,
and in a granular condition of the walls of their capillary blood-vesseU,
Ae nuclei of which are in active proliferation, their number being out
of proportion large.
In the peripheral parts of the lung the most numorous secondary no-
dules are to bo met with ; and consequently the most numerous cheesy
depodta are here to be found. I have often seen a system of laige patches
pn^ectang somewhat above the surface and radiating towards the deeper
parte, as the terminal branches of a minute bronchus puss towards the
■tern.
Tba secondary process extends from the terminal branches (alveoli and
infnndibnla) to the lar^ bronchi. In these the process becomes ver}'
marled, and consists of the following changes : —
(a) The epithelium proliferates very abundantly, whereby the cavity
may finally become almost completely plugged up by the progeny of the
epithelium.
(&) A more important change consists in the proliferation of the tissue
titat we have designated above as pseudoatomata, namely the branched cells
of the tunica mucosa that extend between the epithelial cells to the surface ;
this tissue grows so as to form a very rich adenoid tissue. At the same
time ijiere goes on an active growth of adenoid tissue in the walls of the
peribnmchial lymphatics : that is tu say, there is a hyperplasia (Sander-
son) of tjie preexisting follicles, as well as a new formation. [The most
active transformation of the pseudostomatous tissue of the bronchi into
•denoid tissue I have met with was in i-abbita sufEering from chronic
pynmia ; it has been already stated that the reticulum of branched cells
vhicb stretches between the epithelial cells of the surface is better
developed in rabbits than in guinenpigs, m the normal coudilion.]
(e) In the large bronchi, which liave become involved in the secondary
process, another noteworthy change takes place, viz. the fusion of groups
of the proliferating epithelial cells, not only those of the free surface,
bat also those of the mucous glands, so as to form multinuclear proto-
plasmic cylinders and lumps (giant cells).
The secondary process, vis. that which affects the alveoli and bronchi,
and which may be justly called the catarrhal pneumonic process,
always accompanies artificial tuberculosis when it has extended to the
142 DT.E.KlmnamtkeJmiamgqf' [Jnuttl^
interalTeolar tissue ; in the earij stages of sriifieial taberadosia, mJ^ tti
perivascular lymphangtal cords mre to he md mtik.
If the infection has been established from tiie pleural oafitj, the gov
mination of the endothelium of tiie surfaoe round tiie atomat% and tta
transformation of the subpletiral lymphatics into ooids of ^vfhnmll
is the first symptom, and is fdlowed by tiie appearanoe of
adenoid cords. If, however, the lung becomes tuberoulooa bj ii
from the blood-vessels, the peritoneal cavity or the Bubentaneoaa tiiniQ,
the perivascular adenoid cords are tiie first strueturea that make tiieir aip*
pearance. In lungs which have become the seat of duronio pyuua^ the
first changes are to be found in the alveolar septa and alveoH, vis. the
formation of patches and nodules similar to thoee that I havo dnaignattiil
before as secondary; and if the process lasts Icmg enou^, ftoaa
changes take place that I have designated before aa primaiy tubemiknis
changes.
The opinion has been expressed (by Sanderson and Wilson. Eooc) tlMiJI
the process of artificial tuberculosis in the lungs of gnineapiga vaaemhleai
in its anatomical features, the tuberculous process in man. I iviB
therefore examine the process that is dinically and anatomieaUj knomi
as miliary tuberculosis in man. For this purpose I shall deaonbe the
changes that I found in three series of cases of miliary tuberculosis in
children, representing, as we shall see, three different stages of develop-
ment. In the first series the lungs exhibited all the anatomical appear-
ances of acute miliary tuberculosis. Ou microscopical examination it waa
found that the nodules were due to groups of alveoli (with the correspond-
ing infundibula) being filled with and dist^^nded by a fibrinous material
that contained granules and a few small cells ; generally these latter oo-
cupied the centre of the alveoli. The walls of the alveoli were hardly
distinguishable ; and the capillary vessels were not permeable, as shown
by the fact that, in well-injected preparations, the injection did not pene-
trate into the capiUaries of the alveolar septa. The alveoli next to these
nodules contained the same fibrinous material ; but they were not filled up
by it completely ; and their epithelium could be distinctly recognised,
having become wholly or partially detached, the individual cells being
somewhat enlarged, and some of them containing two nuclei. Here tiie
injection material penetrated the capillary blood-vessels more or less
perfectly: the alveoli of the neighbouring parts contained either a
small amount of fibrinous material, besides isolated young cells, or a ho-
mogeneous gelatinous substance that had become stained with hssmatozy-
lin. The epithelium was very distinct, its cells granular. In some of
the alveoli the epithelial membrane was more or less detached from the
alveolar septa ; the capillary blood-vessels were perfectly permeable.
In the second series of cases of miliary tuberculosis, in which the lungs
did not differ in macroscopical appearance from those of the first series, but
in which the process had lasted longer, ^^^ microscopical appearances were
1874.] ike Lyn^katic Syttem of ike Ltrnga. 148
•nmewhat diiEereDt. The nodules were seen to differ m their structure
{rom Uiose iu the former series in the following respects. In some of them
it was eaxjXa recogiUEe that they represented a number of alveoli very much
distended b; a fibrinous subatoDce similar to that described abore, which
included granular nutterial and a number of small cellular elements ; the
tnbecnln of these nodules (that is, the interalveolar tissue) were slightly
tliickened and contained young ceils, their capillary blood-vessels being not
completely permeable and not easily dLstingiii!«h able. Besides these there
ware nodules of which only the central alveoli were in the state just men-
tifmed; whereas in those situated more peripherally the fibrinous material
was no longer to be discovered, but they were filled in one or other of the
following ways ; — first, by spherical nucleated elements, many of which
could be still rec<^ized as epithelial cells, by their 8i7.e, granulation, and
nudensjand some of wluch contained two nuclei. In these places, theinter-
Klveolar trabecule were thickened in a very marked manner, exhibiting
all the appearances of an infiltrated tiNNuc — that is to say, a more or less
distinct reticulum of nucleated libres, in the meshes of which lay small
lymphoid corpuscles very readily stained by logwood or carmine. Or,
aecimdly, they were filled by one large multinucleated mass or giant cell.
In the latter case the giant cell, or rather the multi nuclear protoplasmic
cylinder, contwned the nuclei either regularly distributed in its periphery,
at all crowded together in the central part of the mass. As regatds tho
nuclei, it may be said that they xtain readily ; they are relatively small,
sharply outlined, andcontRin one or two nucleoli. The protoplasm of the
giant cell is tinted slightly yellowish, docs not stain in ha-iimtoxvlin, and is
very regularly filled with small granules of (iijual size. As regards the deve-
lopment of these giant cells and their nuclei, I ninst first contradict those
authors who say that they oripnatc generally by a free-cell formation in
the veins, as well as thos<! who make them originate in h-mphatic vessels ;
for I have folloucd their development from the epithelial cells of tho
alveoli with all possible certainty. I have been able to make out that the
whole epithelial lining of an alveolus bet-omes fused together into one pro-
toplasmic lump which fills out the alveolar cavity, and the nuclei of which
rapdlydivide.reuiMning, however, in theirorigijialplaces, viz. peripheral.
"We have here a protoplasmic cylinder the transverse section of which
■hows a peripheral ring of nuclei. But a single epithelial cell may
also become transformed into a multinuclcar giant cell: one or the
other epithelial ceil increases rapidly in size (probably at the expense of
its fellows) ; its protoplasm becomes enlarged as well as its nucleus ; then
this nucleus gives rise by cleavsgc, or by budding, to a number of small
nuclei, so that it is transformed into a number of nuclei lying in th«
middle of the cell. [I have little doubt that Klebs would be much inclined
to regard the very regular granulation of the giant cells previously men-
tioned, as being due to the presence of micrococci ; such an assumption,
however, could not easily be proved. A snlwtance filled very regularly
T.
144 On the Lyn^fkaHe l^Hem rf the Lm^. ['n^il^
.<
m
with granules is said to be flDed with mkroooooL AgMiwt tlMiA viMr.
howeyer, it can be maintnned, flnt, fliflt tiiflro are • mmiber of irmiM
tissues that appear after harfffliing to be jurt m xegobily ilBad ivilk
granules (e.g. the liver-cells of anyHtcrhaHiwMidmipirifcXM>i>»eMUfcJ^^^
that the resistance of these grmnnleB to adds and alkaliea after hntai^if
does not prove them to be mieroooccL]
Where the alveoli contain giant oeDs, the alveolar septa sre
thickened, and are seen to consiBt of a tumie tint ^wwtMna
and spindle-shaped cells, the substance of whkli baa more or Ibbi the
appearance of a fibrous lassne, their proeeeeee as weQ aa Aeir bodj
being slightly fibrillar. Between tiiese Aere are vecy few lywpjiflH
corpuscles to be found.
la a third series of lungs, wfaidi also in maoroeoopioal aspeet Si mk
differ from the former ones, it is seen tibat almost all flie T»qdntBr innntaii
giant cells, corresponding to the alveolar spaces. Theoe» howeffer, ImM
undergone changes which are ooneetljr described by Schuppel and otherii
viz. the giant cells give origin to a network of brandiednncleatodeslb^ tfl
well as toa few spherical nucleated elements that lie inita meahee, TUi
network grows at the expense of the giant ceD, which nndeigoes proBI^
ration at the same time. We have here what is generallj called a relieiilir
tubercle. From one giant cell a number of giant oeUs maj take tbeir
origin.
The nearer to the centre of a nodule the giant cell lies, the more exten-
sively and quickly does a transformation of its substance take place. It
becomes converted into a very dense feltwork of fibrillar tissue, the
nuclei of which gradually disappear, while the tissue itself dies away,
becoming firm and hard, and finally resembling a granular substance, in
which fibrils can be made out very indistinctly. While the network of the
nucleated cells continues to grow at the expense of the giant cells, the
process of necrosis spreads gradually to the peripheral parts. In this
stage of the process the thickened interalveolar trabeculsB become also
assumed into, and identified with, the tissue that originated from the giant
cells. In the neighbourhood of the nodules there are very numerous
places where the interalveolar trabecule are thickened and contain nume-
rous young cells, the epithelium of the corresponding alveoli being, at the
same time, in a state of proliferation. In general the tubercular nodulee
of both these latter series have the common character that the peripheral
zone of the tubercular nodule is a regular adenoid tissue, being composed
of a delicate reticulum which includes small lymphoid corpuscules ; this
adenoid tissue is in continuity with the tissue of the interalveolar
trabecule above mentioned. In these stages of the tuberculous process,
we find numerous branches of large blood-vessels, in the immediate
neighbourhood of the nodules, provided with the same perivascular
cords of adenoid tbsue as have been described in the tuberculous lung
of the guineapig.
1874.] Onthe Contparative Value of certain Geological Aget. 145
fitudly, it may be mentioaed that thc§e nodiiJeH also grow in drcum-
ferance, by the alveolar septa of the neighbouring alveoli gradually be*
ooming thickened, while, at the same time, the epithelium of the ooire-
aponding alveoli undergoes the changes before described. The capillary
Tesoels of these parte show the same changes as were mentioned in the cose
of the gnineapig's lung — being transformed gradually into nucleated fibres,
wluch must be supposed to be, for a certain time, still permeable by
coloured fluids.
If we summarize the results thus described, it is evident that tho
changes in the process of miliary tuberculosis in man are only to a limited
extent nmilar to those which occurr in the proi-ess of artificial tu-
berculoeiB in guineapige. In the lung of tuberculized guineapigs the
first structural changes are characterised, briefly speaking, by the appear-
ance of perivascular lymphaDgial nodules, whereas the changes of the in-
teralveolar tissue and the alveolar epithelium form only a secondary pro-
cess. In miliuy tuberculosis of man, on the other band, we see that the
firat dianges take place in the alveoli and interalveolar septa, and these
changes are followed by the appearance of perivascular cords.
It is tlierefore probable that, in artificial tuberculosis of the lung of th«
gnine^ng, the parts first attacked are the smaO branches of the pulmo-
nary artery <k pulmonary Tein, whereas in I'he miliary tuberculosis of man
the capillary blood-vessels of the alveoli seem to be the tissue from which
the action of the morbid agent starts.
n. " On the Comparative Value of certain Geological Ages (or
groups of formations] considered as items of Geological Time."
By A. C. Ramsay, LL.D., V.P.R.S. Received December 16,
1873.
(Abstract.)
The author first reviews briefly several methods by which attempts
have been made to estimate the value of minor portions of geological
time, such as: — calculations intended to estimate the age of ddtas,
founded on the annual rate of accumulation of sediments ; the astro-
nomical method followed by Mr. Croll, in connexion with the recurrence
of glacial epochs ; the relative thicknesses of different formations ; and
tiie relation of strong unconformity between two sets of formations in
connexion with marked disappearance of old genera and species, and the
appearance of newer forms. Having shown that none of these methods
^ve any clear help in the absolute measurement of time in years or
^dea of years, even when founded on well-estabhshed bets, he proceeds
to attempt to estjmate the compartUive value of long portions of geo-
lo^cal time, all of which are represented by important series of
fonnatitns.
146 Prof* A. C. Ramsay on the [Jan. 29^
The author then alludes to the subject of two papers by himself, giyen
to the Geological Society in 1871, on the £ed Kocks of England, in
which he attempted to show that the Old Eed Sandstone, Permian, and
New Eed scries were all deposited in great inland lakes, fresh or salt ;
and this, taken iu connexion with the ^ide-spreadiug terrestrial cha-
racter of much of the Carboniferous series, showed that a great con-
tinental age prevailed over much of Europe and in some other regions,
from the close of the Silurian epoch to the close of the Trias. He then
endeavours to show the value of the time occupied in the deposition of
the above-named formations, when compared >%ith the time occupied in
the deposition of the Cambrian and Silurian strata, and of the marine
and freshwater strata which were deposited between the dose of the
Triassic epoch and the present day.
After alluding to the probable mixed estuarine and marine character
of the purple and grey Cambrian rocks of St. David's, it is shown that the
Cambrian and Silurian series may be massed into three great groups: —
first, from the bottom of the purple Cambrian rocks to the top of the
Tremadoc slates ; these being succeeded unconformably by the second
group, the Llandeilo and Bala or Caradoc beds ; on which rest imcon-
formably the members of the third series, ranging from the base of the
Upper Llandovery to the top of the Upper Ludlow beds, — each uncon-
formable break in stratigraphical succession being accompanied by a
corresponding break in paljeontological succession.
These three great divisions are next shown to be comparable, in the
time occupied for their deposition, to the three dinsions of Lower,
Middle, and Upper Devonian rocks, which are considered to be the
marine representatives of the Old Bed Sandstone ; and therefore it
follows that tJu time occupied in the deposition of the latter may have been
OB long as t7w,t taken in the deposition of the Cambrian and Silurian series.
This position is strengthened by the great palseontological dilEerences in
the fossils of the Upper Ludlow and those of the marine Carboniferous
series, which seem to indicate a long lapse of time during which, in
Old Eed Sandstone areas, no direct sequence of marine deposits took
place.
The next question considered is, what relation in point of time the
deposition of the Old Eed Sandstone may have taken, when compared
with the time occupied in the deposition of certain members of the
Mesozoic formations. Through a series of arguments, lithological,
stratigraphical, and pala'ontological, the conclusion is arrived at, that the
whole of the Liassic and Oolitic series present the various phases of one
facies of marine life, and, in this respect, are comparable to the changes in
the fossil cont<mts of the various subformations of the Cambrian and
Lingula-flag series, of which the Tremadoc Slates form an upper
member. In like manner the Lias and Oolites may be compared
with the TiOwer Devonian strata ; and therefore a lower portion of the
1874.] Coa^iarative Value ef certain Geological Ayea. 147
Old Red Sandttane may have taken at lonff for its depotition at ihe vihoU
cf the time occupied in the deposition of the Jttrauie teria.
Followmg out this tnin of argument through the NeocomiaD and
CretaoeoDB stnts, the result is aniTed at that Ihe whole of ihe time
oempied in the depotilUm of the Old Red Sandtlone may have been equal
to the viMe of the time occupied in ihe deposition of all ihe Juratne,
Weedden, and Cretaceous strata eolleetively.
In the same manner the next t«nn of the Continentnl era, the Carboni-
ferouB epoch, is compared with the Eocene period, both being locally
of marine, estuarine, freshwater, and terrestrial origin, and both con-
nected with special continental epochs. Next comet the Permian series,
comparable in its lacustrine origin to the Miooene strata of so much of
Enrope, tJiongh in the case of the Permian waters the lakes were salt.
After this the TriassJc series o£ Europe alone remains o£ the old con^
tinent, tiie marine and salt-lake strata of which are not likely to have
taken a shorter time in their depOHition than the older Pliot^ne strata.
If the foregoing method be of value, we arrive at the general conclusion
that the great heal continental era, which began nith the Old Red Sandstone
and dosed with the Nevi Bed Marl, iseoniiiarable,inpointofOeohffiealTime,
to that oeeupiedin the deposition of the vhole of the Mesoioic series later than
AelfeiD Bed Marl, and of all the Cainozoic formations, and, more probably, of
aU the time that has elapsed since the beginning of the deposition of the Lias
down to the present day i and consequently the more modem continental era,
which locally began with the Eocene period and lasts to the present day,
has been of much shorter duration.
The author then pointed out that during the older continental era
there flourished two typical floras — one extending from the time of the
Old Bed Sandstone to the close of the Permian strata ; while the second,
which is largely of Jurassic type, characterized the Triaesic formations.
From the time of the Lias onward in time, we have also two distinct
typical floras — the first of Jurassic, and the second of much more modem
type, beginning with the Upper Cretaceous strata of Aix-la-Chapelle and
lasting to the present day.
In like manner the faunas connected with the land resolve themselrea
into two types : — the first chiefly Labyrinthodontian, as shown in the
CarbtmiferoaB and Permian strata ; and the second characteristic of the
Trias, with Crocodilia, many land-lizarda, Anomodontia, Deinoeauria, and
Manupial Mammalia- This fauna, as regards genera, with the exception
of Lat^iintbodontia and the appearwice of Pterosauria, is represented
Ihrongh the remaining members of the Mesozoic formations, ^from
Jurassic to Cretaceous inclusive. After this comes the Pachydermatous
MammaliaTi Eocene fauna, and after that the Miocene land-fauna,
which, in its main characters, is of modem type. From Jurassic to Cre-
taoeons times, inclusively, there was therefore, as far as we know, in
this area a land-tanna chiefly Beptilian, Saurian, and Marsupial, and
1 Ml \ III 1 J I a .'»i.u I I
. • • « 1 V.
.^irara. Of tlip ^eoloi^ical lustorv, in the v
' we |)os-;rss the last \olunit' alone, rt'latini; oiilv totwoo,
I'lir oonnoxioii of this (jiu'stion with that of the com
liffereiit geological eras is obvious, especiaUy in relation
iogical part of the question.
Presents received January 8, 1874.
FransactionB.
Bordeaux : — Acad^mie Nationale des Sciences, BeUes-L
Actes. 3« s^rie, 34« ann^, 1872-73. 1* et 2* trimest
1873.
Sod^t^ Medico-Chirurgicale des H6pitaux et Hospice
et Bulletins. Tome VI. 8vo. 1871.
Soci^t^ de M^edne et de Chirurgie. M^moires et Bi
8vo. 1873.
Soci^t^ des Sciences Physiques et Naturelles. Extra
yerhaux des Stances. 8yo. 1869.
Frankfort on the Main : — Senckenbergische naturforsc
schaft. Bericht yom Juni 1872 bis Juni 1873. 8
am Main 1873.
Jena : — Medicinisch-naturwissenschaftliche Gesellschaf
Zeitschrift f iir Medicin und Naturwissenschaft. Bi
Leipzig 1871.
Gel : — Uniyersitat. Schrift^n -"- ^
1874.] Pretentt. 149
Jonmali.
AmerinnJoniTial of Sdence and Arts. Third Series. Tol. Y. No.30;
Vrf. VI. No. 31-35. 8vo. New ffat-m 1873. The Editora.
BnUettino di Bibliografia e di Storia delle Scienie Matematiche e
Hbu^, pubblicatodaB. Boncompagni. Tomo IV. GenDUo 1871 ;
Tomo V. Die. 1872, Indici; Tomo VI. Geimaio-Maggio 1873.
4to. Boma 1871-73. The Editor.
NerwTorkMedicalJoiimal.Vol.XVn. No.6; Vol.XVIU. No.1-3.
8to. aw Tork 1873. The Editors.
Zoologiache (Der) Oarten. Zeitschrift fiir Beobacbtung, Pflege UDd
Zncht der Thiere. Jahrgang XIV. No. 1-6. 8vo. Frantfurt a.
M. 1873. The Zoologiache C^esellschaft of Frankfort.
Aooat (I'Abb^) Analyse In&ut^simale des Courbes Planes. 8vo. Pom
1873. The Author,
darke (Lieiit.-Col. A. R.), F.B.S. Compariitoii of Standards and Lengths
of Cnbits, from the Philosophical Transactions, 1866 «id 1873. 4to.
London. The Author.
Dnboia (£.) Les PasBogea de V^dus but le Bisque Solaire. 12ino. Parit
1873. The Author.
Bnmsej (Dr. H. W.) The Health and Sickness of Town Populations
considered with reference to proposed Sanitary Legislation. 8vd.
London 1846. Essays on State Medicine. 8vo. Londoa 1856. Tracts
on Sanitary Matters, 1857-73, in 1 vol. 8vo. General Medical
Council. State Medicine. 8to. 1869. The Author.
8tainton(H.T.),F.B.S. The Natural History of the Tineina. Vol.XIU.
8vo. London 1873. The Author.
Tbomas (Edward), F.B.S. Numismatic and other Antiquarian Illustra-
Uoiu of the rule of the Sassanians in Persia, A.n. 226 to 652. 8vo.
London 1873. The Author.
The Treasury of Languages: a Kudimentary Dictionary of Universal
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JaKMry 16, 1874.
l^ansactionB.
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150 Presenti. [Jan. 15^
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[Jut 89,
■Si"'
Oqra !<«<■>>•( Dr. Sd ^mtt, U&,W1
"i ':i"j' J 'ij . I i I ITia ■" fagi ■■■wlli ITii ■
fHiwiiliiw il> Slr-n^nE.
■
1874.] Prennit. 1S8
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Hngo (L.) Lea CristalloVdes complexes k sommet etoilc. 8vo. Paris
1872. The Author.
Lms (Q.). Frolegomeni alio studio dolle Burrasche del Clima di Boma.
«o. Boma 1873. The Author.
Miiller (A.) Ccmtributions to £ntomol(^:ical Bibliography up to 1862.
No. 3. 8to. Zondon 1873. The Author.
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Natural Harbours of Befuge on the Malabar coast. 8vo. Edinburgh
1873. The Author.
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Crayon Portrait of Dr. Neil Amott, F.E.S., by Mrs. Carpenter, in gilt
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Forty-aeven Original Drawings of Venomous Snakes, illustrating Dr.
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numbered Plates 1-9, 12-35, 31», 33", 35"; unmounted Drawing of
the OpKiophoffut elapa, numbered Plate 10 ; large unmounted Draw-
ing of the dusky variety of the same, Plate 8 in printed book ; nine
uncoloured Drawings of Dissections, mounted.) Dr. Fayrer-
VOI.. XXII. »
154 Dr. J. D. Macdonald on the [Feb. 5,
February 5, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
I. '' On the Anatomy and Habits of the genus Phronima (Latr.).''
By John Denis Macdonald, M.D., F.R.S., Staff Surgeon
R.N., Assistant Professor of Naval Hygiene, Netley Medical
School. Received January 15, 1874.
Of all groups of Crustacea the Amphipoda would appear to exhibit
the widest range, in the modification of their parts or organs, without
obliterating the delicate lines of natural affinity running through them
as a whole. This is well exemplified in the interesting paper of Dr. S.
Willemoes-Suhm, Naturalist to the ' Challenger ' Exploring-Expedition,
" On a new Genus of Amphipod Crustaceans" founded by him, and named
Thaumops (Phil. Trans, vol. cbdii. p. 629). This genus, although exhibiting
many characters in common with Phronima, presents some striking points of
difference traceable in the external jaw-feet, caudal appendages, the posi-
tion of the generative pore, and certain particulars in its internal anatomy.
Of the several characters given of Thaumops the presence of only four
caudal appendages is perhaps the most exceptional ; for in the generality
of the Ubopteba there are six besides the telson, which is obviously the
equivalent of the seventh abdominal segment of Macrura. Thus the six
pairs of abdominal appendages, including the tail-fins of the prawn or
shrimp, for example, are represented in Phronima aud its allies, with the
exception of Tfiaumops. The manner in which the fourth and fifth pair
of swimmerets and the caudal fins of Macrura are modified in the
XJroptera is well seen in the accompanying figures ; ^g, 2 in Phronima
and fig. 3 in a neighbouring group of Hjrperians, which also serve to
show why, at least in the former genus, only five segments have hitherto
been recognized in the abdomen.
During the exploratory voyage of H.M.S. * Herald,' in the S.W.
Pacific, numerous species which I have always been in the habit of
referring to the genus Phronima, were taken in the towing-net ; and I
may remark that the assumed parasitic habit of these creatures was
never, at least, a prominent fact to me ; they were so often taken either
perfectly free, or tenanting a nidamental case, such as that subsequently
to be described. Those who, like Dr. Suhm, are acquainted uith deep-
sea dredging are usually cautious how they refer the doubtful product
to their proper habitat ; whether it be the bottom that has been reached,
or some zone of the watery space above. Indeed it is quite possible for
1874.] JM^omjf OHd ffabiii of the GtMi* ViaoainiM. 16S
ths naznnr m* td the lallow-aniiing of the deep-sea lead to include for-
toibxulj', and carry down Phronima or any other little crustacean natu-
lallj liTing near the surface ; and contact with the bottom would finall;
pieaa it into the tallow, so aa to mislead the obseirer as to its true
liafaitat. CoaTersely, in bringing up the dredge from a giren depth, it
maj finallf eany with it anf more superficial objects casually lying in
the track which it takes.
Fig. 1 of the accompanying dranings from nature represents a species
of Phrvnima captured in hit, 30° Itf S., long. 176° 27' W., of which I
find the following description in my notes taken at the time ; —
Head exceedingly elongated from above downwards, nith considerable
enlargement of the back part, which contains two masses of transparent,
rounded?, and tapering columns, whose bases occupy the fulness of the
peril, fl^uUting a regularly facetted appearance eitemally on two rounded
protuberanoe*. The apices of these organs, on the other hand, con-
TBrgeaadUendwiththeraysof theeompoundeye, of which, indeed, they
Biay be said to form part, probably assisting nocturnal vision by the pro-
duction of himinosity. The long axis of the head is therefore at right
■n^ea witji that of the body, its form being full abore and gradually
t^>ering downwards. The aperture of the mouth is situated at the
■mailer extremity, inferiorly guarded by its mandibuls, maxillte, and one
pair of foot-jaws, appertaining to the cephalic segments. The latter
' organs are more distinctly recognizable than the others, on account of
Uieir more superficial position. They are short, apparently united at the
base^ and curved forwards, terminating in two ovate and acute appen-
dages lying side by side, serrated on the borders and beset with short hairs.
The eyes are small where the facets are Uteral, and the apices are
invested with black pigment, but large where they swell out the back of
the head, the pdnts of the same cones meeting in a red spot, quite distinct
from, and internal to the black one. This condition is also observable in
the Hyperians, and is worthy of further study in a physiological point of
view.
Two minate two-jmnted antennte arise from the head, just above and in
front of tJte eyes. The posterior or upper surface of the second joint of
these antennie is clothed with short stiff hairs.
There we seven pairs of thoracic limbs ; but the first two are separated
from the others, to some little extent, by arising on a plane anterior and
inferior to them, the first two tergal pieces being somewhat wider than
those of the succeeding segments. They are, moreover, distinguished
from the other limbs by possessing a minute apine-like movable claw,
bounded, on either side, by a short styliform process. There is also a
rudimentary manus developed upon the posterior part of the second seg-
ment above this daw, that of the first pair being the stoutest, although
the limbs themselves are the smaller of the two. Both pairs of members
BOW described, while they very distinctly belong to the thorax, act the
h2
156 Dr. J. D. Macdonald on the [Feb. 5,
part of foot-jaws as in the higher Crustacea. The five sucoeeding pairs
are more especially restricted to the thorax, the third or middle one being
stoutly chelate, normally directed backwards, with the pollex superior, and
enjoying a very considerable range of motion.
The first pair is usually thrown forwards over the head, and the last
backwards over the abdomen, the first fiexure corresponding with the
first swimmeret ; the second pair is the longest.
The fourth, fifth, and sixth thoracic segments are each furnished with
a pair of elongated and laterally compressed respiratory yesicles, connected
with the posterior and inferior part of the epimeral pieces behind the
articulation of the corresponding limbs. These vesicles increase in size
from before backwards ; and indeed a very rudimentary one may be seen
behind the third pair of limbs. The last, or seventh, thoracic segment is
of unusual length, tapering posteriorly, to correspond T^ith the narrowness
of the abdomen, in which also the segments are of greater length than
those of the thorax. It has been alr^ftdv stated that in Phronima. as in
the Macrura, there are seven segments in the posterior division of the
body ; functionally, however, three of these may be said to belong to the
abdot&en and four to the tail. The three abdominal segments bear each
a pair of swimmerets, arising near their posterior border, and consisting
of a stout or inflated foot-stalk and two narrow, acuminate, annulated
and setaceous terminal pieces.
The three anterior of the four caudal segments bear a narrow fan, con-
sisting of three pairs of slender appendages furnished with two shorl
styliform tips. The first and third of these caudal members are much
longer than the second.
The oral organs (with the exception of the jaw-feet), the large chelo,
and the foot-stalks of the swimmerets are tinted with a rich purple pig^
ment. All the other parts are hyaline and transparent.
EXPLANATION OP THE PLATE.
Fig. 1. Lateral view of Pkronima (species ?). With the exception of the antennie,
the limbs and appendages of one side only are represented, magnified about
9 times.
Fig. 2. The abdomen and tall of the same, further enlarged, to show the several s^-
ments, nmnbered (from before backwards) 1, 2, and 3, with swimmerets, and
4, 5, and 6 bearing caudal appendages, while 7 is the terminal segment or
"telson."
Fig. 3. The abdoipen and tail of a Hyperian for comparison, all the numbers haTing
the same signification *.
The evidence of Dr. Willemoes-Suhm supports my own experience, that
there is no metamorphosis in this group ; and as it is very probable that
the history of the development of Thaumops would resemble that of
Phronima^ the following observations may be of some importance,
* r, 2', 3', 4', 5', and 6' being the appendages of the corresponding segments.
Pm'»<./.to».I.XHIP;J.
1874.] Anatamn and Habits of the Genus Phrouima. 157
auTTing liie prooees a little further than it has perhaps yet been traced
by him: —
In lat. 2V 0' 8. and long, ir 45' W. off the island of Ono, Fiji
Oroap, apparently the same species of Phronima as that aboTO described
was taken in the towing-net, but with the addition of a numerous pro-
geny of young in a large gelatinous but tough nidamental case. This
interesting nest was shaped like a barrel, but with both ends open, and
the external surface was somewhat tuberculated and uneven. The wall
of the tube presented numerous round and puckered openings, observing
no very definite arrangement, but through which entering currents were
observed to pass. These openings generally, though not invariably,
pierced the tuberculations.
An external membrane, with an internal lining, were distinctly visible,
both seeming to be continuous at the rims of the tube. The space between
these layers was filled up with a pulpy substance, in which scattered
nudeiform bodies were detected \i-ith a higher power of the microscope.
I have been particular in the description of the case, as some far-
fetched guesses were made as to its real nature. The cutting, piercing,
and tearing implements of Phrtynima would very soon alter and reduce a
bell-shaped Medusa, aSalpian, or a Pyrosoma tube to the required pattern ;
for there is usually a great uniformity in the character and appearauce
of this case.
*• With regard to PArontwwi," says Mr. Spence Bate*, " oiur knowledge
is small : its habit is that of an inhabitant of the gill-ca\itie8 of some one
or more species of Medusa ; but in the Collection of the British Museum,
emtrosted to my care for examination, is a very curious case that was
sent home from Naples by S. P. Pratt, Esq., as being the one in which the
animal was taken. The structure is thick, fleshy, semitransparent, and
stndded over the surface and round the orifices — one of which is smaller
than the other — with numerous white excrescences. Examination with
the microscope shows the substance to be pervaded by bundles of fibres ;
each fasciculus is twisted together near its centre ; these, some of them
being larger than others, star the structure thickly, and still more plenti-
fully where the white excrescences appear."
However problematical the nature of the case, that its use is for nidi-
fication there can be no further doubt.
Though I have already given figures of the specimen above noticed to
my friend Major Holland, IL.M.L.I., for a paper on Phronima, published
in * Science Gossip ' (April 1869), I trust that allusion to it here may not
be out of place.
In a subsequent commission on the North-American and West-Indian
Station in H.M.S. * Icarus,' I have frequently captured " Phronima in
its bag,** as my messmates would say. In order to bring the swimmerets
into full play, the animal protrudes it« body tail foremost from the case,
ft Annmls and Maguine of Natural History (Third Series), March 1858.
lbs Mr. H. E. RoBCoe an a Method of meoiuring the [¥eh. 5,
onlj calliiig into use the fine tips of the third and fourth pairs of
thoracic limbs to hold fast its charge. When it fully retires into the
case, the claws of the two posterior pairs of legs are pressed backwards
against the lining membrane, so as still more effectuallj to secure its
hold on the approach of danger.
II. '' On a Self-recording Method of Measuring the Intensity of
the Chemical Action of Total Daylight/' By H. E. Roscoi,
P.R.S. Received November 27, 1878.
(Abstract.)
The object of the present communication is to describe an instrument
by which the varying intensity of the chemically active rays, as affecting
chloride of silver paper of constant sensitiveness, can be made self-record-
ing. The method described by the author in the Bakerian Lecture for 1865,
although it has been the means of bringing into notice many important
&ct8 concerning the distribution of the sim's chemical activity throughout
the atmosphere, as well as in different situations on the earth's sur&ce, has
not as yet been introduced as a portion of the r^ular work of meteoro-
logical observatories, owing to the fact that, in order to obtain a satisfac-
tory curve of daily chemical intensity, at least hourly observations need to
be made, and this involves the expenditure of more time and labour than
it has been found possible to give. In the present communication a
method is described, which, whilst preserving untouched the principles
and accuracy of the former method, reduces the personal attention needed
for carrying out the measurements to a minimum, and thus renders its
adoption in observatories possible.
According to this plan, a constant sensitive paper is exposed by a self-
acting arrangement for accurately known times, at given intervals
throughout the day. The insolation apparatus stocked with sensitive
paper is placed in position either early in the morning of the day during
which the measurements have to be made, or on the previous night, and
by means of an electric communication with a properly arranged dock,
the sensitive paper is exposed every hour during the day, so that, in the
evening, the observer has only to read off, in the ordinary manner, the
hourly intensities which have been recorded on the paper during the
day.
This self-recording arrangement, though apparently simple, involves
points which have rendered its successful completion a somewhat difficult
matter, owing, in the first place, to the great variations which occur in
the chemical intensity of total daylight in different places, at different
times of the day, and in different periods of the year ; and secondly,
owing to the fact that, in order to be able to estimate the chemical
intensity, the coloration acquired by the paper must reach, but not much
1874.] Intensity of the Chemical Action of Total Daylight. 159
exceed, a giyen tint. It becomes necessary therefore that on each occasion
when an observation is needed, the sensitive paper should be exposed
mechanically, not once, but for several known, but varying intervals of
time, quickly succeeding each other ; so that whatever may be the
intenaiiy of the total daylight (supposed during these intervaJs to re-
main constant), some one at least of the several exposed papers will
possess the requisite shade. This is accomplished by a duplicate ar-
rangement of a clock and insolation-apparatus, by means of which disks of
ihe constant sensitive paper are exposed each hour for successive known
intervals of tame, varying from two to thirty seconds. After an interval
of an hour, another set of disks are exposed for the same series of
intervals, and these series of insolations are repeated once every hour
during the day. The mechanical arrangements for effecting this with
aocaracy are fully described in the paper. On unrolling, at the end of
the day, tiie strip of sensitive paper which has served for the exposures,
black disks showing where the paper has been stationary for the hour
aro seen, and between each of these are found ten circles variously tinted,
from that, probably, scarcely visible, which was exposed for two seconds, to
tliat, perhaps too dark to read off, which was insolated for thirty seconds.
Amongst these, some one at least, will be found of such a shade as to
enable it to be read off by the monochromatic soda-flame, on a graduated
fixed strip, as described in former communications.
A new method of calibrating the fixed strips of standard tints neces-
sary for these measurements is next described, and the question as to the
possibility of preparing constant sensitive paper in long strips instead of
in large sheets is next experimentally discussed, the result of the exa-
mination being that it is possible to prepare silvered paper in long narrow
strips such as are used in Morse's telegraph-apparatus, so that it shall
tliroughout its length preserve the standard sensitiveness.
The time during which the disks of constant sensitive paper are ex-
posed is next ascertained for each instrument by a chronograph.
During wet weather the insolator is covered by a semicircular glass
shade, and the value of the coefficients for refraction and absorption
due to this glass shade is determined.
The latter portion of the communication contains the results of a series
of comparisons of the curves of daily chemical intensity obtained (1) ^vith
the hand-insolator, and (2) with the self-recording instrument. Com-
parisons of this nature were made during the months of May, June,
and July, 1873, by simultaneous hourly determinations in the neighbour-
hood of Manchester according to both methods. Of these observations,
six full days are selected, and the tables and curves accompanying the
communication show the close correspondence of both sets of observations.
The integrals of total chemical intensity for these days are also given, and
exhibit as close an agreement as, from the nature of the experiments,
can be expected.
160 Mr. F. A. Abel on the [Feb. 5,
III. '^ Contributions to the History of Explosive Agents.*' — Second
Memoir. By F. A. Abel^ F.R.S., Treas. C.S. Received
December 1, 1873.
(Abstract.)
The researches detailed in this memoir are in continuation of those
described in the Memoir on Explosive Agents, published in 1869*, and
relate chiefly to the investigation of the conditions to be fulfilled for
accomplishing the detonation of explosive substances, and of the circum-
stances and results which attend the transmission of detonation.
The exceptional behaviour exhibited by certain explosive compounds
with respect to their power of inducing the detonation of other sub-
stances by their explosion, which was demonstrated and discussed in
the preceding memou*, has been confirmed by further experiments. The
susceptibility of some substances to detonation, through the agency of
certain compounds, and their remarkable inertness when subjected to the
detonation of others, which at any rate do not rank lower as regards the
mechanical force and heat developed by their explosion, led the author to
suggest that a similarity in character, or synchronism, of the vibrations
developed by the explosion of particular substances, might operate in
favouring the detonation of one such substance by the initial detonation
of a small quantity of another, while, in the absence of such synchronism,
a much more powerful initiative detonation, or the application of much
greater force, would be needed to effect the detonation of the material
operated upon. This view, which has been favourably entertained by
many, as affording a reasonable explanation of the apparently anomalous
results referred to, appears to have received support from the results of
experiments recently instituted by Champion and Pellett, with iodide of
nitrogen and some other explosive compounds, which indicated that the
explosion of certain sensitive substances could be accomplished only by
vibrations of a particular pitch, and by which they also demonstrated that
particular explosions affected certain sensitive flames which were un-
affected by others, unless the volume of the explosion was proportionately
much increased.
Some few experiments were made by Champion and Pellet on the
transmission of detonation to iodide of nitrogen through considerable
spaces, by means of tubes, and some experiments of a purely practical
character have also been instituted by Captain Trauzl, on the transmission
of detonation to cartridges of dynamite, separated by spaces, in iron
tubes, by the explosion of a charge of the material placed in one extremiiy
of the tube. It appeared to the author that a systematic investigation of
the transmission of detonation through the agency of tubes, with the
employment of explosive agents less highly susceptible and more uniform
♦ Phil. Trans. 1869, vol. clix. p. 489.
t Comptet Rendiis, vol. Ixxv. pp.'210 & 712.
1874.] History of Explosive Agents. 161
and oonfltant in composition than the iodide of nitrogen, might usefully
oontribate to our knowledge of the behaviour and relation to each other
of explosire substances.
Experiments were first carried on with tubes of cast and wrought iron
of difierent diameters and lengths. The explosive agents used were gun-
ootton, in difEerent mechanical conditions, dynamite, mercuric fulminate,
and preparations containing the latter as an ingredient. Interesting
results were obtained, among others, in the course of these experiments,
demanstrating a want of reciprocity in behaviour between gun-cotton and
mercuric fulminate, as regards the transmission of detonation from one
to the other, similar to that previously observed in the case of nitro-
glycerine, chloride of nitrogen and gun-cotton, and sho^^ing also how
greatly the results, as regards transmission of detonation, may be altered
when certain limits in respect to the quantity of material employed as
tlie initiative detonator, are exceeded. Thus 7 grammes of strongly con-
fined mercuric fulminate, inserted into one extremity of an iron tube only
'152 metre (6 inches) long and '025 metre (1 inch) in diameter, was the
minimum amount required to determine the detonation of gun-cotton
placed in the other extremity of the tube, being at least fifty times the
amount requisite to ensure detonation of compressed gun-cotton when
exploded in dose contact with the latter ; but the detonation of 7 grammes
of compressed gun-cotton in one extremity of a channel 2*128 metres
(7 feet) long and '031 metre (1'25 inch) in diameter, consisting of two
iron tubes placed end to end, accomplished the detonation of fulminate
inserted in the other extremity. When 14 grammes of confined fulminate
were employed, detonation of giin-cotton was accomplished through a
channel 2*129 metres (7 feet) long and *031 metre (1*25 inch) in diameter,
while 7 grammes only just sufficed to develop detonation through a tube
of smaller diameter and only '152 metre (6 inches) long, and 10 grammes,
tlirou^ a similar tube only *228 metre (9 inches) long. The foregoing
are quoted as illustrations of the instructive results obtained in these
experiments.
A few'experiments were"made on a comparatively large scale >*ith the
above-named explosives, >^ith the view of ascertaining the influence of
ihe material composing the tube, upon the effect produced ; and some strik-
ing results were also obtained by interposing very slight obstacles {e, g,
loose tufts of cotton wool) in the path of the gas- wave, and thus checking
the transmission of detonation, \\'hich was certain when the path was
unobstructed. But these points were more closely investigated by a
series of accurate experiments upon a small scale with silver fulminate,
the tubes used being alike in diameter and thickness, but varying in
length, and consisting of different materials, >iz. glass, pewter, brass,
paper, and vulcanized india-rubber. The principal results obtained by
the larger operations with other explosives were confirmed by these small
experiments, and several additional interesting observations were made.
162 Mr. F. A. Abd on the [Feb. 5,
A great difference appeared, at first, to be established in the power pos-
sessed by tubes of different materials of favouring the transmission of
detonation, the glass tubes being far in advance of the others in this
respect. It was eventually established, very clearly, by a series of experi-
ments that this difference was not due, to any decisive extent, to ihe
physical peculiarities (in regard to sonorosity, elasticity, &c,) of the
materials composing the tubes, but chiefly to differences in the degree
of roughness of their inner surfaces, and in the consequent variation of
the resistance opposed by those surfaces to the gas-wave. Thus the
power of a glass tube to favour the transmission of detonation was
reduced, by about two thirds, by coating the inner surface with a film of
French chalk, while the facility of transmission, through a brass tube, was
nearly doubled by polishing its interior, and was increased threefold,
with a paper tube, by coating the interior with glazed paper.
The following are some of the points established by these experiments
on the transmission of detonation by tubes : —
1. The distance to which detonation may be transmitted through the
agency of a tube to a distinct mass of explosive substance is regulated by
the following conditions :
(a) by the nature and the quantity of the substance employed as the
initiative detonator, and by the natm« of the substance to be detonated,
but not by the quantity of the latter, nor by the mechanical condition in
which it is exposed by the action of the detonation ;
(5) by the relation which the diameter of the " detonator," and of the
charge to be detonated, bear to that of the tube employed ;
(c) by the strength of the material composing the tube, and the conse-
quent resistance which it offers to the lateral transmission of the force
developed at the instant of detonation ;
(d) by the amount of force expended in overcoming the friction between
the gas and the sides of the tubes, or other impediments introduced into
the latter ;
(e) by the degree of completeness of the channel, and by the positions
assigned to the detonator and the charge to be detonated.
2. The nature (apart from strength or power to resist opening up, or
disintegration) of the material composing the tube through which detona-
tion is transmitted, generally appears to exert no important influence
upon the result obtained. At any rate the differences with respect to
smoothness of the interior of the tubes far outweigh those which may
prove traceable to differences in the nature of the materials composing
them.
In the tube experiments with gun-cotton many instances occurred in
which the mass operated upon was exploded, but with comparatively
little if any destructive effect, portions of the gun-cotton being at the
same time dispersed and occasionally inflamed. Similarly, the mercuric
1874.] History of Explosive Agents, 168
fnfaniiiate was frequentlj exploded, through the agency of a transmitted
detonatKin, in a manner quite distinct from the violent detonation at other
tfaneB deyeloped. Even the silver fulminate, which under all ordinary
eireomstaiioes detonates violently even when only one particle of a mass
ia sabmitted to a sufficient disturbing influence, has on one or two occa-
Bums been exploded by the transmitted effect of a detonation of mercuric
fulminate, without the usual destructive effect.
This remarkable difEerenoe in the behaviour of one and the same explo-
iiTe Bubstanoe, under nearly similar circumstances, has been made the
subject of experimental investigation, in the course of which some in-
temting illustrations have been obtained of the manner in which varia-
tions in the resistance to mechanical motion influence the results obtained,
by sabmitting some part of a mass of explosive material to sharp blows,
by firing from a rifle (at different ranges) against masses of compressed
gUDrCotton of different weight and thickness, and either freely suspended
in air or supported in various ways. An important exemplification of the
difference between explosion and detonation was obtained in the course of
sabsequent experiments, instituted for the purpose of determining the
Telocity with which detonation is transmitted through tubes.
The influence of dilution, by solids and liquids, on the susceptibility of
explosive compounds to detonation has been made the subject of syste-
matic experiments, and some of the results obtained have already acquired
considerable importance. The dilution of a liquid and of a solid explosive
compound by inert solid substances produces very different results. Thus
the liquid (nitroglycerine) may be very largely diluted (as in the case of
difnamite and similar preparations) by inert solids, without any modifica-
tion of its sensitiveness to detonation, because this dilution does not
interrupt the continuity of the explosive substance. The initiative deto-
nator, when surrounded by such a mixture, is therefore in contact at all
points with some portion of the nitroglycerine, and the latter is in con-
tinuous connexion throughout ; hence detonation is as readily established
and transmitted through the mixture as though the liquid were undiluted.
But when a solid explosive agent is similarly diluted, there must obviously
be complete separation of its particles at a number of points proportionate
to the extent of dilution and the state of division ; the establishment of
detonation, or its transmission, is therefore impeded either by a diminution
of the extent of contact between the initiative detonator and the substance
to be exploded, or by the barrier which the interposed non-explosive
particles oppose to the transmission of the detonation, or by both causes.
Intimate mixtures of a finely divided sensitive explosive compound
with an inert solid, if compressed into compact masses, become much
more susceptible of detonation than if they be in the loose pulverulent
condition ; thus compressed mixtures of finely divided gun-cotton, with
large proportions of inert solids, were found but little inferior in sensi-
tiveness to the undiluted explosive agents. If the diluent consists of a
164 Mr. F. A. Abel on t/u: [Feb. 5i i
soluble salt {e.if. potassmm cliloride) the well-inoorporated mixture being
compressed with the aid of the solvent ('.y. water), and then dried, the
material ib obtained io a condition of great rigidity, the particles being
pemeuted together by the cr_y8talli?ed salt; it is therefore in a form more
favourable to the action of detonation than undiluted gun-cotton sub*
mitted to considerably greater compreaHion, 1
When the solid substance with which gun-o«tton is diluted consisbl <
of an oxidising agent (a nitrate or chlorate), the predbposition to chemic^
reaction butween the two substances so far increascB the susceptibility to
detonation that, operating in conjunction with the effect of the soluble
salt io imparting rigidity to the mixture, it renders the latter quite as
sensitive to the detonating action of the minimum fulminate^;ha!^ M
undiluted guu-cotton is, when highly compressed. This fact has given
additional importance to results which the author obtained some time
since in availing himself of the facility with whiL-h finely divided gun-
cotton, as obtained by the pulping process, may be intimately mixed with J
the proportion of an oxidising ^ent(sueh as potassium nitrate) required '
to completely osidtze the carbon. If about three fourths of the theoreticiJ
requirements of the salts be employed, the resulting products will perform
fully the uniount of work obtaiued from a correspouding weight of undi-
luted gun-fotton ; and an nearly one third of this suhstanoe has hwn
replaced in thorn by material nf very much li-^-^ I'ost, acoiisidentble advan-
tage is gained in point of economy. Moreover the greater rigidity of tiie
compressed mosses of "nitrated" gun-cotton, already explained, renders
them less susceptible to injury by transport and rough usage than ordinary
compressed gun-cotton.
These compressed mixtures being found quite as sensitive to detonation
by fulminate as the pure explosive compound, it became interesting to
compare their behanour with that of the latter, when exposed to the
detonation of nitroglycerine. The results demonstrated that they aie
much more readily susceptible of detonation by it than compressed gun-
cotton ; thus, in only one instance was the latter detonated by the explo-
sion of 62*4 grammes (two ounces) of nitroglycerine in close contact with
it, hut that quantity invariably detonated " nitrated" gun-cotton. The
same result was obtained with only 31'2 grammes (one ounce) of nitro-
glycerine in three out of four experiments ; in the fourth the nitrated
preparation was exphcUd, but without the destructive effect produced in
the other experiments ; similar explosions of the substance were deve-
loped by means of 15-6 grammes (0-5 ounce) of nitroglycerine. In the
case of pure gun-cotton, the results obtained were always either simple
disint^ration of the mass, or else detonation, if aufGdent nitroglycerine
were used.
To ascertain whether the different behaviour of the " nitrate " (and
"chlorate") preparations \vas due to their greater hardness and rigidity,
some corresponding experimeuls were made with compressed masses pro-
1874.] History of Explosive Agents. 165
dnoed in a precisely similar manner, but containing an inert salt, potassium
diloride, in place of the oxidizing agent. These were more susceptible
of explosion by nitroglycerine than pure gun-cotton, but decidedly less
so than the *^ nitrate ** preparations. It appears, therefore, that the ex-
plosion of gun-cotton by the detonation of nitroglycerine is, to some extent,
fiualitated by the greater resistance it opposes to disintegration when
incorporated with a salt, as described ; but that the higher susceptibility
to detonation by nitroglycerine of the " nitrate '' (and " chlorate ") pre-
pantions is probably chiefly due to some predisposing influence exerted
by the oxidizing agent.
If gun-cotton is diluted by impregnation with a liquid ^ or with a body
Bcdid, at ordinary temperatures, which is introduced as a liquid into the
mass, its sensitiveness to detonation is reduced to a far greater extent
than by a corresponding weight of a solid, incorporated as such, with the
gun-cotton. The cause of this is evidently the converse of that which
operates in preventing the reduction of sensitiveness of nitroglycerine by
its considerable dilution with an inert solifl ; the liquid diluent which
envelopes each particle of the solid explosive material isolates it from its
neighbours, and thus opposes resistance to the transmission of detona-
tion, while with nitroglycerine the liquid explosive agent envelopes the
Bolid diluent, and thus remains continuous throughout the mass.
The absorption of three per cent, of water by gun-cotton (in addition
to the two per cent, which it normally contains) rendered its detonation
doubtful by the " detonator " ordinarily used. Dry disks which had been
impregnated with oil or tallow, (^oiild not be exploded by means of one
gramme of mercuric fulminate, applied in a metal case in the usual way.
By considerably increasing the initiative charge of fulminate, damp gun-
cotton could, however, be detonated; and it occurred to Mr. Abel's
amistant, Mr. E. O. Bro^^Ti, to apply the detonation of dry gun-cotton
itaelf to the development of the explosive force of 1 he compressed material,
when in a moist state.
A series of precise experiments showed that when compressed gun-
cotton contained as much as 17 per cent, of water, it could he detonated,
though not with absolute certainty, by C-5 grammes (100 grains) of com-
pact air-dry gim-cotton explod(jd by means of the usual " detonator," in
dose contact with it. When the proportion was increased to 20 per
cent, detonation was not accomplished M'ith certainty by employing less
than 31*2 grammes (1 ounce) of the air-dry material ; and when the maxi-
mum amount of water (30 to 35 per cent.) was absorbed, detonation conld
not be absolutely relied upon vrith the employment of less than 124*8
grammes (4 ounces) of air-dry gun-cotton applied in close contact.
Moist and wet compressed gim-cotton are decidedly more readily sus-
ceptible of detonation by means of air-dry gun-cotton, freely exposed and
exploded by the usual *' detonator *^ of mercuric fulminate, than by means
of the confined fulminate applied alone : thus, when the material containcM^
166 Mr. F. A. Abel on the [Feb. 6,
17 per cent, of water, its detonation by fulminate direct was not certain
with the employment of less than about 13 grammes (200 grams),
whereas the result was absolutely certain with employment of about 10
grammes of air-dry gun-cotton.
The transmission of detonation from dry to wet gun-cotton, through
the agency of a tube, appears to take place with the same fiidlity as
though the mass to be detonated were dry ; and the same is the case with
regard to the propagation of detonation from one mass of moist gun-
cotton to others freely exposed to air, but touching each other, provided
the one first detonated contained not less water than the others to which
detonation is to be transmitted ; but this is not the case, if eyen small
spaces intervene between the separate masses, and in this respect the
moist gun-cotton behaves very differently from the air-dry material.
The "nitrated" and "chlorated" preparations of gun-cotton are as
readily detonated, in the moist- state, as ordinary compressed gun-cotton.
With respect to the mechanical effects obtained by the detonation of
these materials in the moist or wet state, numerous small and large com-
parative experiments have demonstrated that there is no idling off in tiie
work done by them when used wet.
Decided evidence has, moreover, been obtained of greater sharpness of
action, when gun-cotton and its preparations are detonated in the wet
state ; and this accords with the observations made in the earlier of these
researches, that the less susceptible a mass of given explosive material is
of compression, when submitted to the action of a sufficient initiative
detonation, the more readily will detonation be transmitted, and the more
suddenly will the transformation from solid to gas and vapour take place.
When air is replaced by water in the compressed masses, the transmission
of detonation is obviously favoured by the increased resistance of the
particles to motion, at the instant of their exposure to the detonative
force.
The freezing of wet compressed gun-cotton renders it as readily sus-
ceptible of detonation as the mixtures of gun-cotton with soluble (crys-
tallized) salts, to which the wet material obviously becomes quite similar
in structure by the solidification of the water.
Mercuric fulminate and mixtures of it with potassium chlorate, when
mixed with water to such an extent as to convert them into pasty masses
and freely exposed, are readily detonated by small quantities (0*2 grm. or
3 grains) of the confined fulminate, even when not in contact. Finely
divided gun-cotton, made up into a pulp with water, was found not to
be susceptible of detonation, even under very much more favourable con-
ditions than the above, the mixture being placed in thin metal cylinders,
open at one end, and a large disk of dry gun-cotton detonated in the
centre. But if wet compressed gun-cotton is packed into receptacles of
wrought iron, so that the initiative charge of dry gun-cotton is closely
fnuTounded by it, and the small spaces intervening between the several
1874.] History of Explosive Agents, 167
nuuNMS are filled up with water, the charge being then sabmerged, it is
exploded with oertainiy and with results equal to those furnished under
similar conditions by the dry material. Provided the escape of force, by
truiainission through the water, be retarded at the instant of the first
detoiatioiiy either by the resistance which the material of the case offers,
or by the pressure of a considerable colimin of \iiiter, the detonation of
wet gun-cotton immersed in water, and separated by thin layers of the
fluid from the contiguous masses, is accomplished with certainty. Besults
fully equal to those furnished by charges enclosed in strong wrought-irom
eases, have been obtained by the emplojnnent of sheet-tin cases or of bags,
or even of simple fishing-nets, these only serving to hold the masses
composing the charge tightly together. If, however, the latter condition
is not attended to, or the depth of the immersion of the charge is insuf-
ficient, its detonation will not take place, even if a comparatively large
initiatiYe detonator be employed.
The suddenness and completeness with which detonation was trans-
mitted through small water-spaces in the experiments with wrought-iron
cases, led the author to attempt the application of water as a vehicle for
tlie efficient employment of only small denotating charges for bursting
or breaking up cast-iron shells into numerous and comparatively uniform
fragments (and thus to employ a hollow projectile of the most simple
construction to fulfil the functions of the comparatively complicated
"shrapnel"- or " segment "-shell). The results afforded remarkable
illustrations of the transmission of force by water, and may prove of
considerable practical importance. The destructive effects produced by
small detonating charges, when exploded in shells which were filled
up with water and entiroly closed, wero proportionate, not simply to the
amount of explosive agent used, but also to the suddenness of the con-
cussion imported to the water by the explosion. Thus 7 gnunmes
(0*25 ounce) of compressed gun-cotton, detonated in a shell filled with
water, broke it up into nearly eight times the number of fragments
obtained by exploding a shell of the same kind full of gunpowder (viz.
containing 367*9 grammes => 13 ounces). When picric powder, which
is also a very violent explosive agent, though much less sudden in its
action, was detonated in one of these shells, in the same way as the small
charge of gun-cotton, 28*3 grammes (=1 ounce), or an amount four
times greater than that employed of the latter substance, burst the shell
into about the dame number of fragments as were produced by the 13
ounces of gunpowder (instead of about 8 times the number, produced by
means of 0*25 ounce of gun-cotton). Other observations of interest
wero made in the course of these shell-experiments ; they led, moreover,
to some cognate experiments which furnished interesting rosults.
In developing detonation, in a perfectly closed and sufficiently strong
Tessel, completely filled with water besides the detonating charge, the
resistance offered by the liquid at the instant of detonation may be re-
168 Mr. F. A. Abel on the [Kb. B,
garded as similar to that wiiidi would be premnted by a perCeettj solid
mass. Similarly, if the strong Tessel be oompletelj fiDed with a mixfcnie of
yrB,ter and a solid {e. g. a fine powder or a fibre reduced to a fine stale oC
division), such a mixture should also, at the instant of defamation,
behaye as a very compact solid with regard to the resistBnee which it
opposes to the detonating charge which it surrounds. If this be so, a
mixture of finely diWded gun-gotton with water, if enclosed in a shell,
should be in a condition readily susceptible of detonation^ beeanse at tibe
instant of explosion of the initiatiTe diarge, the partides of gnnrcottan
must offer great resistance to mechanical motion. Experiment has fully
established the correctness of this oondusum, having demonstrated that^
while it is indispensable to employ gun-cotton in a hig^y compressed
form, to ensure its detonation under all other oonditionB, it may, if en-
dosed in strong vessels, sudi as shells, be employed with equal efficiencj
in a finely divided state, provided the spaces between the particles be
completely filled with >^iiter, <he small detonating diarge being immersed
in the aqueous mixture.
The results obtained in the several experiments bearing on the trans-
mission of detonation led the author to attempt to detennine its vdodty,
or the rate at which it proceeds along a continuous mass, or from one
mass of an explosive body to another, under various conditions. Eor
this purpose he availed himself of the electric chronoscope devised by
Captain A. Noble, F.B.S., which had furnished satisfactory results in
determinations of the rate of motion of projectiles in the bore of a gun,
made by the Government Committee on explosive substances. The ex-
periments were carried out with compressed gun-cotton in the dry and
wet state, with " nitrated " gun-cotton, ^\ith nitroglycerine and dynamite,
and with small charges of gun-cotton inserted into tubes, with considerable
intervening spaces*. The disks of gun-cotton, dry, wet, and nitrated,
were arranged either in continuous rows or trains, the disks either
touching each other, or a definite and imiform space or interval
intenening between each. At the commencement of the row a fine in-
sulated wire, forming part of the primary circuit (by the sudden severance
of which the electric record of the rate of transmission was obtained on
the chronoscope), was tightly stretched across the first disk. Other
wires were similarly fixed at uniform distances (of one, two, four, or six
feet) from each other. In determining the velocity of transmission of
detonation through tubes, wrought iron gas-pipes of 0*032 metre
(1*25 inch) diameter were used, with small perforations at the desired
intervals, through which the insulated wires were passed ; the disks of
gun-cotton, to which detonation was to be transmitted, were inserted
into the tubes so as to be in close contact v^ith these tightly stretched
* In carrying on these experiments, Mr. Abel reoeived Taluable aasiBtanoe at dif-
ferent times from Captain Singer, B.N., Major Maitland, B.A., and Captains W. H.
Noble and Jones, B.A.
1874u] HUiory of Explosive Agents. 169
wires. The tmiiui of dynamite were arranged like those of gun-cotton,
compreeaed charges of this material, 3 inches (*0759 metre) long and 1
inch (*0253 metre) in diameter, being placed end to end or ^vith definite
spaces intenrening between them. The nitroglycerine was placed in V-
shaped trooghs of thin sheet metal, through which the insulated ^nres ^^-ere
passed transverselj at the requisite intervals, so as to be immersed in the
liquid.
A number of experiments \iith dry gun-cotton compressed, demon-
stiated that the rate at which detonation is transmitted from mass to
masSy when these are in actual contact with each other, is between 17,50<)
and 20,000 feet (5320 metres and G080 metres) per second, and that the
rate of transmission is affected by the compactness of the material, but not
bja difference in the form and arrangement of the individual masses, nor by
▼eiy considerable variations in their weight. By the experiments with
^pocM^ gun-cotton disks, it wtM demonstrated that the separation of the
masses may retard the rate at which detonation is transmitted, the extent
of such retardation being, of counte, detennined by the relation between
the siae of the individual masses and the extent of space inten'eniiig be-
tween them. With compressed gun-cotton, containing fifteen per cent.
of water, detonation was transmitted at a slightly higher velocity than
with the dry substance of the same compactness ; but when gun-cotton
satureUed with water was employed, the increase in the rate of trans-
mission was very marked, being equal to about 20,000 feet per second,
with disks which, when dry, detonated at a rate of about 17,500 feet per
second. With " nitrated ** gun-cotton the rate of transmission was, as
might have been anticipated, decidedly slower than with the pure dry
material ; it ranged between 15,500 and 10,000 feet (4712 metres aiul
4864 metres) per second.
The results obtained with dynamite and nitroglycerine presented some
very interesting points of difference from those furnished by compressed
gun-cotton, which are ascribable to the liquid nature of the explosive
material. The dynamite used was in the form of compressed rolls or
cylinders, similar in firmness or solidity to stiff but not very plastic clay.
Bows or trains of these charges, pressed together end to end, so as to
form perfectly continuous masses 2S feet (8-533 metres) and 42 feet
(12'8 metres) in length, were detonated by means of a fulminate detonator
of the kind used with gun-cotton, which was inserted into a small
cylinder of gun-cotton, or into a small cartridge of dynamite, and placed
upon one extremity of the train. The rate at which detonation
was transmitted ranged between 19,500 and 21,600 feet (5928 and
6566 metres) per second ; it was therefore decidedly higher than with
compressed gun-cotton. The separation of the individual cartridges
or cylinders by spaces of 0*5 inch (-013 metre) produced, however, a
very much greater retarding effect than was the cose with a sepa-
ration to the same extent of masses of compressed gun-cotton; the
VOL, XXIT. <>
^
170 On the Oitorp tf EsgOome JfenU. [FcIkB;
mean rate at which velodtj waa inmamilted along the q^aoad tnaMwa ti
dynamite (in an experiment remarkable £or the great imiConnitjr ot ike
records at different parte of the train) ma c«il7»6289 fiaet (1896 ]^^
per second ; the mean rate of toranamiBsifla along matioa of gim-oolAaiiof
the same weight and length as the dynamite cartridges, and aepanted by
0*5 inch spaces, was (in two experiments) neariy » lifiOO bk
(5179-9 metres) per second. When niirogtyeerine was employed in die
pure and, therefore, liquid state^ detonati(m being established afe one ex-
tremity of the trains by means of a cartridge of dynamite, the mean rate
at which it was transmitted was only abont 5500 feet (167S metrea)
per second, the same result being obtahied in two experiments, in one of
which the quantity of nitrog^yoerine, in a giTen length of tbe tnin, was
double that employed in the other*. It may be possiUe that^ by very
greatly increasing the quantity of nifooglyoerine used, the rate of trana-
mission of detonation would be increased ; bat there is no doabt that the
mobility and elasticity of the liquid, and the consequent facility with
which it yields to mechanical force when nnconfined, act antagonistioally
to the transmission of detonation in a mass of fredjf expoad mtrof^y-
cerine. The author hopes that he may haye the means and opportnnity
of extending these interesting experiments, by ascertaining the effect of
confinement, both of nitroglycerine and gun-cotton, on tiie transmission
of detonation along continuous masses of the explosive agent.
The numerical details given in the memoir afford proof of the trust-
worthiness of the results obtained in the velocity determinations, and of
the uniform rate at which detonation is transmitted along rows of con-
siderable length, composed of distinct masses of the explosive material,
even when these are separated from each other by spaces. With trains
12-16 metres to 15*20 metres (40 to 50 feet) in length, the rate at which
detonation travelled along the last few feet was equal to that obser\'ed in
the first portion of the train. This was not the case with the transmission
of detonation through tubes to widtly separated masses of gun-cotton. The
time intervening between the detonation of the initiative charge at one
extremity of the tube and that of the first distinct charge (separated by a
space of 3 feet 3 inches, or 1 metre) was somewhat variable, and ranged
between 10,000 and 13,000 feet (3000 to 3900 metres) per second ; the
subsequent transmission, from charge to charge, along the tubes proceeded
at a tolerably uniform but considerably reduced rate, the average being
1800 metres (0000 feet) per second. In one experiment, with reduced
charges, the detonation was transmitted, as usual, to the first three separate
masses ; but the fourth and succeeding charges, though they exploded^ did
not detonate ; the tube containing them was uninjured at those parts, but
the wires were severed at the seat of each charge, and the records ob-
* The amount of nitroglycerine employed in a given length of the train conre-
Bponded to that used in certain of the gun-cotton experiments, in which the imte of
traosmiwion of detonation rangrxl between 18,000 and 21,000 feet.
1874.] On the Synthesis qf Formic Aldehyde. 171
explotum
9k the nte of between 450 and 640 metres (1500 and 1800 feet) per
aeoond. These experiments with tubes showed that, when the relations
between the amount of explosive material, the diameter of the tube, and
the space intervening between the charges are such as to ensure the
transmiHHJon of detonation, its rate is about one third of that at which it
travels along a continuous mass, or continuous row of distinct masses, of
tiie same material.
The concluding part of this memoir deals \iith a subject only iuci-
dentally referred to in the former memoir on explosive agents, and which
has since that time acquired considerable importance^namely, the
manner in which the accumulation of heat in a mass of explosive ma-
terial, and other conditions, may operate in bringing about or promoting
violent explosion or detonation.
February 12, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Presents received were laid on the table, and thanks ordered for
them.
The following communications were read : —
I. '' Note on the Synthesis of Formic Aldehyde." By Sir B. C.
Bbodib, Bart., F.R.S. Received February 5, 1874.
In a former note I communicated to the Society the result of an
experiment in which a mixture of equal (or nearly equal) volumes of
hydrogen and carbonic oxide had been submitted, in the induction-tube,
to the electric action. My expectation in making the experiment had
been that the synthesis of formic aldehyde would be thus effected accord-
ing to the equation CO+H,= COH,. The only permanent gas, however,
other than the gases originally present in the induction-tube, which
appeared in the result of the experiment was marsh-gas. When a mix-
ture of hydrogen and carbonic acid gas was similarly operated upon, the
flame hydrocarbon, together with carbonic oxide, was formed. I have
now, however, succeeded, by a modification in the conditions of the latter
experiment, in attaining the object which I originally had in view.
Evidence of this is afforded by the following analysis : — The gas analyzed
was the result of submitting to the electric action about equal volumes of
hydrogen and carbonic acid. After removal from the gas of carbonic add
and carbonic oxide, and also of a trace of oxygen, 191*2 volumes of gas
remained, in which were found, at the conclusion of the analysis, 2*6
volumes of nitrogen. Deducting this amount of nitrogen, 188*6 volumes
of gas^ remain, containing the residual hydrogen in the gas, together vaih.
o2
172 Dr. E. A. Parkcs on the [Feb. 12,
any gases besides carbonic oxide formed in the experimetit. This gaa
was analysed by the addition of oiygen and subsequent detonation by
the electrif spark, the absorption of the carbonii- ai-id by potash, and the
removal of the oxygen over by pyrogallate of potash. The results of the
atudysis entirely concur with the asBumplion tliat the IflS'C volumes of
gas were constitnted of hydrogen, marsh-gas, and formic aldehyde in the
proportions given below ; —
Hydrogen 183*2
Marsh-gns 0-2
Formic aldehyde 5-2 ^
188G ■
The composition of 100 volumes of the gas beinfj.
Hvdrogen fl7'14
Marsh^pia 0-10
Formic aldehyde , . , 2'76
100-00
Another experiment was attended with similar results, only that tlisi
proportion of marsh-gn,* was somewhat greater.
The R-siiH of litis L^prrittifiit iiinv Ix' .■oiisidi.-reJ tfl !«■ i;ivoii in im*
equation CO.+2H,=:C0H,+H,0. t have reason to believe that formic
aldehyde is also formed in the reaction of hydrogen and carbonic oxide,
and that the marsh-gas found (in both erporiments) results from the
decomposition of this substance, possibly according to the equation
2C0H,— CO,+CH,. I do not now dwell upon this subject, as it is
my intention very speedily to lay before the Society, together with other
matters, the details of the various experiments which I hare made in
reference to it.
II. "On the Influence of Brandy on the Bodily Temperature,
the Pulse, and the Bespiratious of Healthy Men." By E. A.
Fahkes, M.D., F.R.S., Frofeaaor of Hygiene, Army Medical
School. Received November 29, 1873.
In the Proceedings of the Eoyal Society (Nos 120, 123, and 136) the
details of experiments are given which show that in two healthy men
pure ethyl alcohol, brandy, and claret, given at intervals during the day,
produced no eSect on the temperature of the body as measnred in the
axilla and rectum.
This result is in accordance with the experiments of Eeveral other
observers, while there are some experimenters who have noticed a de-
crease in temperature in healthy men after the use of alcohol. In some
cases of disease in men and in some healthy animala alcohol has CftOaed,
it would seem, a decided lessening of temperature.
1874.] Influence of Brandy on the Bodily Temperature ifC. 178
These difierences of statement led me to conceive that the time when
the alcohol was given might have some effect.
In the experiments formerly reported to the Eojal Society, alcohol
was osnaUy given either with or at no long interval from food. As
food raises the temperature of the body, it occurred to me that it might
mask an opposite action of the alcohol ; and I therefore determined to
repeat the experiments, and to give the alcohol about four hours after a
moderate breakfast, when the heating-effect of the food had gone off,
and when digestion was completed, and also to give it in a state of
complete inanition.
I. RvperinienU after the completion of Digestion,
The subject of the obsen'^ations is a strong healthy soldier, T. B., aged
25, height 5 feet 8| inches, weight (naked) 67*46 kilogrammes, or 148 lbs.
He has at times drunk some quantity of spirits, but not for the last two
or three years, and usually takes about two or three pints of beer daily.
The course of the experiments was as follows : — His breakfast was
taken at 6.30, was finished every day by 7 a.m. ; he took for break&st
8 ounces of bread, j ounce of butter, and 17 fluid ounces of tea with sugar
and with 3 ounces of milk. Immediately after breakfast he went to bed
again, and did not get out of the recumbent position for any purpose
until 2 o clock. He then dined on 12 ounces of beefsteak, 4 ounces of
bread, and 8 ounces of water.
After dinner he took exercise and smoked, had tea (same food as at
breakfast) at 6, and a glass of water at 9 p.m., when he went to bod.
He took daily precisely the same diet and quantity of water.
Thermometers (tested for accuracy and exactly corresponding) were
placed in the axilla and rectum at 6 o'clock, and, except at breakfast, they
were removed only for the purpose of being read at first every 30 and
then every 15 minutes, and were at once replaced, until 2 o'clock, after
which time the temperatures were only taken every t>^'o hours.
After several days' preliminary examination (during which time he
took no alcohol) the experiments were commenced and carried on for six
days without alcohol ; then during five days undiluted brandy containing
50 per cent, of absolute alcohol was given once daily, viz. at 11 a.m., four
hours after breakfast.
On the first day one fluid ounce of brandy (=j| ounce of alcohol) was
given, on the second day two ounces, on the third day four ounces, on
the fourth day six ounces (=3 ounces of alcohol), and on the fifth day
also six ounces. I had intended to give him eight ounces on the fifth
day, but the brandy made him so ill, he begged me not to increase the
quantity*.
* The effect of the six ounces of brandy taken in this way at one time and without
water waa entirely to destroy appetite, so that he could not force himself to take his
food ; it also caused a great feeling of depression, sickness, and headache, and increased
the flow of urinary water very largely for three hours. The nitrogenous elimination
174
Dr. E. A. Parkes o« the
[Feb. 13, ,
Acilla and ifartum Temperatitra.
The foUoniiig Tables give all the thennometric observations under the'
three fenois oE 6 a.m. to 11, 11 to 2, and 2 to 10 p.m.
Abulia Temperature (Fahrenheit).
Before Brandy.
Period from C a.m. to 11 a.m.
Hours.
Diyi, June 187).
...
...
.J-
.4-
.!•
6 o'clock ...
97-0
irS
9>-4
97-.
97
0
970
„■!
97
97-0
97-*
971
98'.
98-0
91
s
97a
9K-0
S.JO ..
98-.
98-.
,I-o
,8-.
,«-o
'!
97-1
,8-.
,!■•
9,6
,8-.
980
98-.
M«in of the period
5,1.
97'7
98-..
97-9
97-7
97-6
Period fron
11 A.M. to 2 P.M.
98-.
97-8
97S
,«.,
,<-.l
t>.4{ .>
»»■■
9«-o
,8-.
97-0
97-9
97-4
I1.JO ,.
,1.
980
97-84
97-«
97-6
97-5
ii+S ..
97-5
97-S
97'4
i.'S .,
9T*
1-30 „
97*4
Mi ..
,7-6
"'!
97-4
'
97-6
97-7
97-1
MainofUiojuifiod
,r,t
91=1
97'9
97-9
97-8
97-4
" Period 6
■om 2 to 10 P.M.
3 o-dock..
,!•=
97-8
,7-8
qg'>
,16
9«'.
97-8
,7-8
qli'O
9S-.
,l!'o
91-4
,8-1
,7-8
9li'K
9»'4
,!••
,!■.
98-.
98-0
9lt'K
flS-1
10
,n
9>-.
,86
,7-8
9fb
911-S
M»n of tJic pcricj
,1-,
51.5
ji-.s
97-8
9if+
9^-J
mu not increaaed, and wsi piobabl; ilighU; iMBensd ; but the Ion of appctit«^ wkieh
■Itered the ingnes of nitrogeD, on ooe day reodend th« expmineDt nOm imparfeet.
In ocder not to lengllian the praent DommuniMtioii, I raecire til detaila of the egrtm
of nilTOgen tad pboapborio acid and alMhol for uiother opportunity.
1874.] Influence of Brandy on the Bodily Temperature l^e. 175
Axilla Temperature,
Broudy at 11 &.»,
Period from 6 to 11 i..M..
HoUra.
Day
Junti7aml Julyi,
873.
*?■
»8.
9. JO.
'■
6 o-elDtV ...
g6-6
96-1
6.30 .,
97-1
97
I 97 +
97'o
7 ,f
97-0
97-0
9/
* 97 4
97-1
7-30 ..
97'»
97
97-1
97-+
9',
97'4
,«-,
7a 0
g 98'4
,M-i
9!)>
S 986
980
««'4
9!l-4
lO.JO „
m-z
■)«•+
91
"1
981
9S-0
9*1
0 98..
98-4
M«.n of tlie period I977
9772 97
58 979S
97-6
Period from 1
1 A.M. to
2 p.m.
11. IS o'clock...! 9B0
97'°
9»
0 ^i■^
98-6
11-30 ..
97-1
"■45 ..
I1.1S „
97-1
97-4
971
9/
97
97
i 97-5
8 97'i
97-9
980
977
1».J0 „
97-S
9.
97-4
IMS ..
9',
B 97-1
97-4
"■;
97'6i
9/
96'8^
97-4
i.iS ,.
97-44
V,
97'4
1.30 „
97'5
97
S 96'8
974
I-4S "
97'S
97
S 97'i
97'4
J
97-5
97
974
MMiioribeporiod
9783
97-4 97
! 1 sj'ij
97-4
Period from
2 to 10 I
M.
3 o'ulook ...
qS-o
97-6
98
0 ' 9S-2
9r6
fl«-3
9«-»
9*
. 98-4
CH-.
9iCz
9!
, 98-+
97-8
9*-.
9il-+
9»
3 1 93'4
98'4
10
97'4
97'3
99
97'4
Mean of the period
98-01
97-9+
98
3 1 98-.
97-84
Dr. E. A. Parkes on the
[Feb. 12,
Temperature of Rectuin,
Before Braiiiiy.
Period from 0 to II A.M.
Hours.
Daj», June i!7j.
*..
II. 1], 1 14.
"S-
16.
6 o'clock .,.! 97-8
97-8 ! 98-8 i 97'8
97'4
984
6.10 „ ; 97'«
">■
i ; 1*
* V,
97'4
4
91
4
7-50 .. 5«-8
9'
0 1 9t
9"
8 1 9i
0 9l
8 98-8
H
S.JO ,. OT'o
8 95
0 9!
0 1 99-0
9i
9'
4 9!
9'
0 9S-8
I ] ,1
8 , 98 !
10.30 „ 1 jB-g
9:
1 1 „ 1 9l-4
98!
98-4 1 98-8 i 98-8
98-6
MeanoFttiepenDd | 98-67
98-6
98-96] 98-6 1 9t-s
„■<.
Perioct fron
1 11 JiJt. Io2p.m.
ii.ij o-dodt
... U9-0
988
,1-1
ll.JO „
99-0
98-61] ...
988
99'
98
99-0
,«*
IJ.I5 „
990
99-0
99-0
10.30 „
99-1
11.+S „
98-z
?2.|
9lf8
i.iS ..
1.30 „
9'
58-4 ■ 98-4
I.4S ■■
?8-8
sa-a
99-0
98-8
98-4 1 98-5
!«■•
Mean of Ihepfriod 98-96
98-8 1 98-88 1 98-74! 98'6
,is«
Period from 2 to 10 p.m.
, o-dock
99-4 99*0 1 98-8
,11 1
W'.
9^
99'8 1 9!
9^
8
6
99-6 99
IDO-4 99
99-6
=
10
99-6 1 994
■ 00-4
Mean of the poriod 100-14 lOdS
99-76 99-1 99-36
99-1
1874.] Ii^ttienee (^Brandy m the BottUtf Temperaturt Ifc. 177
Temperature of Bectnni.
During Brandy.
Period from 6 to 11 a.u.
D»yt, June 17 '<• 3alj
. 1873.
noun.
.7.
.g. i 29.
3
6 o-elock
flT6
984 1 ita
98
0 97'4
6.30 ..
97'6
9U ! 9>-4
7
og-o
98x 93-4
qU
flm
!
9JC6
93-6 j 98-4
IS
♦ »!!
8.30 „
9(-6
98-6 I 98'4
9'i
4 98-8
9
99'0
99-0 ; 98-4
ll
9-JO
99-0
990 1 93-4
1^
l-i
1 99-1
10.30 „
9IIII
9>J
» 994
.. „
,H-»
99
0 991
Kfuioftheprriod
9»-4
93-64, 984s
9»
7 9!-S
Period from 1
A.M. to 2 P
SI.
,g-s
,ga
«■*
fll
J 99-4
^s-t
6 99'1
<,3-4
<,%■!>
9"
9»-4
98-6
1 g8-6
986
98 b
•>i
.!■,
,8-b
9"
0 98-6
•i*■^
9«
, , 98-6
1 „ 1 98-3
9»-i
gH-b
97
Mf^n of Ibe period , 9905
98-+; ' 98-75
98'3S 98'84|
Period from
2 to 10 P.U
} o'clock
.9-4
990 9S-8
98
4 98-6
4
99-1
99-5 996
9^
99+ IOO-6
t^
994
99a loog
10
Ibuoftheporiod
99»
99' '«>■>
»
1! 99S6
These obsen'stions will now be considered under the three following
heads : —
Ist. The mean temperature of the day.
2nd. The mean temperature of the periodi.
3rd. The lauge of the thermometer from 11 to 2 o'clock ; i. e. the differ-
ence between the 11 o'clock and the 2 o'clock temperatures.
Dr. E. A. Porkes on Iht
1. J/eioi Teinjxrature of thf f&urUen hourtwhen the w
t^iTvation.
[Feb. 12, .j
It UKU under
1-14 observations in the water days give a mean daily temperature in
the aiiUa of 'J7°-9, and 137 obserrations in the brandy days give a mean
daily temperature of OT"'"!. In the rcctinn the observations were 144
and 138 respectively, giving a mean daOy rectum temperature of 98°-89
in the non-brandy and 98'^ 78 in the brandy days.
This difference is eo slight as to fall nithia the range of unavoidable
error; but it might be that the effect of tbe brandy was only perceptible
for a ehort time. It is necessary tlkeu to take the temperature of the
periods.
2. Mean Trvipfrature of the Penoth.
Unnuilk
BsTiM
br.ndj.
br«d;.
Period&om6A.ii. toil A.)i. ...
57-Si
97°*71
Bo. of OMefTHtions pvm^ Tuean
66
SS
Period from 1 1 A.u. to i p.m. ...
jr^'ja
97=- 58
No. of obeermliou* giTing mean
49
S7
Period from i r.M. to lo p.m. ...
98=-»S
98=05
No. of obsoryfttions giving mean
19
*S
M«m rectum
t«nper»ture.
Period from 6 XH. to tl A.M. ...
98»-6j
9fS7
66
5S
Period from r i i.h. to 1 f.k. ...
9>°-73
ss-ea
«
5!
Period from a P.m. to 10 p.m. ...
996-jj
99''-46
No. of obwmtioai giving mesn
»9
*S
The differences, espeoally in the case of the rectum mean tempera-
tures, are slight eren in the hours between 11 and 2. In every case,
however, the mean of the thermometer is lower, though to a very slight
^^xtent, in the alcoboUc series. This, howeTer, is not ccmclusiTe, as will
^^1 evident from a considenitioa of the meao r^um temperatarea on the
"BmI days.
1874.] Influenee of Brandy on the Bodily Temperature ^c. 17!
Heau Tempenture of Bectum in the three houra following brandr.
No Bmnd;.
Brandy.
let day 9!o6
3Td „ ItZt
ith ,. 9874
5th „ Qg'fio
ath .. 98-S6
&d„ 9f-55
3rd „ 98-75
Bth „ 98-li
On four of the brandy days the mean temperatures were quite eqn^
to fonr of the non-brandy days ; on one day (6 ounces of brandy) the
mean wu, however, only 98°- 34, or 0°'22 below the loweat temperatura of
a water day. But this was accidental, and was owing to the thermometer
getting imbedded in a mass of fioces, which separated it from the intestinal
wall. For fear of spoiling the experiment, the man would not move
though he greatly wished to do so. That this was the real cause of the
diminution in this mean, is shown by the last day's experiment, when
with the same quantity of brandy the temperature was higher than on
four of the water days, and was 0°-l above the mean of the six water
days. It seems therefore very difficult to conclude from the mean
rectum temperature of the period that there was an actual fall.
In the period from 2 to 10 the mean brandy temperature was O^'S?
lower than in the water period. But as the observations were much
fewer at this time and were taken at much longer intervals, and as food and
exercise complicated the results, little importance can be attached to them.
Although themean temperatures do uot, then, give a satisfactory answer
to the inquiry, it may be that an effect may be found in the initial and ter-
minal temperatures of the 11 to 2 period. This is shown in the following
Table:—
3. Bange of the TemperaUire from 11 to 2 o'elocl:
Axilla Temperatures.
Temperature.
Water Pwiod. DajB. , Bratiily Period. Dsja.
,.
1.
3-
.|5.|...|..
A.
a-
4.
J-
At II o'clock ,.
At I o'clock ..
9S-,
97-6
97-6
97-8
>7f
977
97-g , 9lt-»
97"» iierS
9rs
980
97-8
981
97-D
98-4
97-4
DlfR™.
-■€
+■6
-■4
-.|-,pj->
-s
-'
-'■*
-'■°
Rectum Tempemhires.
At.i o'clock ...
At » o'clock ..
,a-4
9S-i
9S'i
99'6
93-4 |93'B
98-8 98-4
9S-8 98-!|Ua
98S .98-> '\^-t
9S-i
98-3
98-7 99-0
99-1
98-6
Difibrcnee
+•4
+..|...j-.
-'h\-h
-1 -1-3
-■6
180 Dr. E. A. Parkos on Me [Feb. 12,
The greatest fall iii these three hotira of the axilla temperature oil a
water day was 0°-6 Fahr. : the greatest fall ou a brandy day w-os F-S, and
ou another day the fall was 1", or '6 and "4 more than on any wat«rday ;
yet on the third day of brandy, when four fluid ounces ( = 2 fluid ounces
of absolute alcohol) were taken, the difiereuco was only U°'2 Fair.
In considering the rectum temperatures it is necessary to omit the
fourth day of brandy, when impacted fnjcal matter in the bowel evidently
lowered the reading of the thermometer. There M-as no fall with one
fluid ounce of brandy ( = ]J fluid ounce or 14 cub. centim. of alcohol), a fall
of O^'S with two fluid ounces (=2S-4 cub. centims. of alcohol), of only 0°'l
with four fluid ounces, and of 0°-6 with six fluid ounces. There was there-
fore no regularity with tlie increasing quantity of brandy. The greatest
fall (O^-fl) was not more than occurred on one of the wat«r days.
When these numbers, omitting the fourth brandy day of the rectum
aeries, are submitted to calculation according to the rule given by Ut.
Galloway in his Treatise on Probability, the following results are given ;^
Differrace of Temperature between 11 and 2 o'clock in Fahrenheit degrees.
Reet-am tcmper»tui*.
Wfltrr daje. Bnmdy dflye
Water ddys.
Bfandy d«y«.
Mo.afob«rvatiotis
6 S
6
4
-=''■37
Probable error of MHiilt
Truth liM bctwMn ... |
±d'-..S
-o=-j9S
+ 0°M +
-o°774
If the obaeriations are not too few to be trusted, this calculation
shows that there was a slight fall in temperature in the three hours
following brandy.
But it will be seen at once both how small the fall is, and how difficult
it is even yet to feel quite sure of the result. Taking the rectum
temperature for example, the probable errors of result ae calculated out
are O"-!! in the water and O^-Oy in the brandy days ; the results in each
series might then have been a mean fall of — 0''16 in the water series
and of — 0°-23 in the brandy series, or there might have only been a
difference of — O^-O?.
Still, looking at all these results, and especially to the fact that the
calculation is in all cases a little against the brandy series, it may
be concluded that in this man the brandy did produce a very sligbt
fall ; but that, if this is correct, the fall could not have been more than 0°'35
Falir., and may have been only '07 Fahr., in three hours.
1874.] Influence of Brands tm the BodUg Tmperatwe ^e. 18L
It may probaUjr be intoreatiiig to note the usual course of the bodOy
temperature in the water period. It was ver; nnif orm : at 6 a.m. (twelre
hours after food) the mean rectal temperatuie was lowest, vii. 98°; and
it was highest at 10 at night, when it reached 100°-I4, or a difference in
the twenty-four hours of 2°-14 Fabr.
IVom the effect produced by the breakfast, I infer that this course was
chiefly owing to food, and uot to any peculiar effect produced by the time
of day.
Thus the mean rectum temperature being 98° at 6 and 6.30 o'clock
A.1I., it rose at 7 (just after a warm breakfast) to 98°-3, and continued to
rise till 9 o'clock, when it reached 99°. It continued at this point until
10 or 10.30, when it began to fall, and at 11 was 08°06, at 1 98°-65, aud
at 3 o'clock 98°-62. Then dinner and exercise were taken, and the ther-
mometer went rapidly up, being 99°-08 at 3 o'clock, Od°-i2 at 4, B9°-83
at 0, 100°-10 at 8, and 100°- 14 at 10. It seems fair to attribute this rise
especially to the effect of food.
The mean axilla temperature followed exactly the same course, being
lowest (97°'36) at 0 a.m., rising after breakfast, falling again three and
three and a half hours after breakfast, and rising immediately after
dinner and tea to its highest point, 98'''4 ; the mean diurnal difference in
the axilla temperature was one half that of the rectal, or l°-04*.
The pulse was taken on an average twenty-three times daily, from six
in the moniiug until ten at night, the man being always in a recumbent
position, and, in fact, being in bed until two o'clock every day. The course
of the pulse before the brandy was taken was very constant ; the number
of beats per minute was raised by breakfast for t\TO hoiurs, then fell gra-
dually until dinner, and then rose greatly after dinner in consequence of
the food and exercise.
The following are the averages of the days : —
Dbjb, Before Bnndj. During Brandy.
' 76J 7S*4
Average of tbe whole water period ts'tj
.. " brandj „ 75-47
* It may be noticed, in referenni to tbe rectum temperature, tbst it is not quite
correct to uy, u i* eometime* done, that there ij no change within ahort periods. In
half an hour tbe rectum temperature haa varied u mooh a* 0°'4 Fahr., though I took
everj precaution to place the thermometer properlj and to reed it with great care.
Usually it is much leea than tbi*. The variationi within abort perioda in the axilla
were, however, decidedlj greater thso in tbe rectum, but mm seldom more than from
W-C 10 (f -8 M a
182 Dr. E. A. Parkes on the [Feb. 13, .
It will be obseired Ihat, when nil the dftVB are taken, the brandy did I
not raise the mean pulse of the whole day. It increased, howerer, th« \
rapidity of the pul^e during the three hou» after it was token, as will ba' i
soen from the following Taljle : —
Mean of the hoora &om 11 to 2 oVluk.
Dr^s. Ko Brntidf. Bmodj.
» 67-0 6-)
a ^\^6 677
3 «-9 79»
4 64-8 7IJ
5 6j-o 71-1
Wwin 65-7 Jf7
The quickening of the pulse during these hours is best seen \yf €
two days, nhit-h are fair samples of the Bcriea.
Becord o£ two days, one without and one nith brandy (C ounces), ia 1
dhow the influeiK-e of food, of movement, and of brandy.
Hour*.
Best of rulM.
Houn.
(continued).
BeatorPul*.
Brandv.
Brandj
o'dock
(6 ounces).
No
Bnuid;.
Brandy
o'clock
(6 ounce.).
61.K.
6, JO
7 (br«W«l)
g.30
9
9.3a
10. JO
6;
67
^4
i
I
66
Si
95
90
7S
74
74
11,15 P-"-
11.3a
"■45
LIS
'-JO
I -45
61
61
61
Gi
Go
71
G7
Gj
il
70
Mean or period
ei-6
T-H
98
94
99
y
Mmn uf period 71
76
u.is
11.30
"■,V(..„,
60
76
So
73
UflBn of period
,.
95
As the means of the entire day are practically the same when all the
days are token, it is clear that the acceleration of the pulse in the three
hours succeeding the taking of the brandy must have been compensated
bf. a corresponding lessening of ^equency afterwards ; and this is shown
_by the fcUowing Table : —
1874.] Zi^ftMence of Brandy on the Bodily Temperaiwe t^e. 188
FulK.
Period from Period from
6toll A.H. |lljt.ii.to2rj(.
Period from
2 to 10 r.il.
MMnof«ii4iy^l
withwrt bnmdyj
wUh brandy...)
77'»
74*
6s-7
7'7
88-9
87-0
Id the brandy period the me&a pulse was I'D per minute slower in the
after put of the day, and three beats per minute slower in the morning.
The action of the single small dose of brandy in the day was to alter the
mode of working of the heart, and not to alter the amount of work done
ID 24 hours, as far as this was judged of by the frequency of the pulse.
As far as frequency was concerned the compensation was perfect, and
the temporary quickening was balanced by an equal amount of subsequent
retardation. Frenoua experiments indicated that when large and repeated
dosee were taken, the acceleration was not thus compensated, and that
the heart beat more frequently than was natural throughout the whole
day. It was certainly very interesting to see how this healthy heart
maintained its balance, and, in spite of the alteration in action forced
upon it, accomplished in the day the same amount of work under different
conditions of diet. Whether other healthy, and especially whether
diseased, hearts would do the same is an interesting question, as is also
the point whether the temporary acceleration was, in this man, useful, or
hurtful, or indifferent, to the heart.
Respiration.
The respirations were taken at the same time as the pulse, and there
were twenty-three daily observations. To save space I give only the
mean numbers,
Bespintions.
Mean number per minute.
Before Brandy.
Period.
D»j., June 1873.
11.
la.
XI.
M-
»S-
ifi.
6 to 11 AM.
1 1 ut. to 1 r.M.
a to 10 P.II.
»r3
117
HO
ij-j
10-8
191
>9
■8
«3
13
Dr. E. A. Parkes on the
During Braudy.
[Feb. 12,
Period.
D.jfcJiii«.27l«j3ulj 1,1873.
17.
iL
99.
ja j I.
II A.M. to a r.H.
a to la f.K.
igj
so
.7!
10-;
.6'«6 ii-9
*i-4 ij
The reapiratioas in tbU man vere always extremely quieic, even when
he had been h-ing in bed for eighteen hours. The variation follows Hosely
the changes in the pulse. They increased after breakfast at 7 o'clock, and
then at 9.30 commenced to fall, and conliuued less numerous by two or
three per minute until dinner. This meal, and the exercise which was
always taken in the afternoon, raised the number. The brandy seemed
to lessen the number of respirations in the period from 11 to 2 o'clock ;
the juean of this period in the auti-brandy days was 19'86 per minute,
and in the brandy period was 17-8S. This result, if it bo real, showed a
difference between the pulse and respirations, the former being raised sii
beats per minute on a mean of all the days, and the latter being lowered
two respirations per minute in the three hours following the brandy.
The effect on the number of respirations was most marked in the two
days when six ounces of braudy was taken.
Considering, however, theratheruuuaualfrequeney of the respirations in
tlie man and the smallness of the change, I hesitate to conclude that the
Teepirations were lessened in number, but decidedly they were not
increased.
Received February 5, 1874.
II. Ej'jiirimenit ihiring mxiiiUte Inanition.
The following experiments were made to determine the effect of alcohol
after sixteen hours fasting : —
A healthy man (J. S.), 5 ft. 4 in. in height, weighing 'BG-T"* fcOo-
grammes, v,-aa kept in bed every day until 1 o'clock, at which time he re-
ceived his first meal in the day. The last meal was taken at 6 o'clock P.u.
He was consequently fasting for nineteen hours. The axilla and rectum
temperatures were taken every half hour from 6 to 10 a.m., and every
fifteen minutes from 10 to 1 p.m., the thermometers remaining in riht,
^ except for the purpose of being read. The daily food was the same,
except on two days, when the brandy destroyed his appedle and ho coidd
t not quite eat his ration.
1874.] Ii^hienee (^BrtmOg on the BotHfy Temperature ^c. 186
The ezperiioeats were carried on for six iaja : on the flist, third, uid
fiftii dajB he took no alcohol ; on the second, fourth, and nxth daja ha
took 8 fluid ounces of brandy, containing 36 per cent, of alcohol, at 10
o'clock; he therefore took 2*16 fluid oonces, or 61 cub. centims., of
absolute alcohol dxteen houn after taking food. The following Tables
gire ibo results.
Temperature of Axilla.
D-j^
.-
■■
3-
4-
s-
e.
6 o-ok
6. JO
7.30
1.30
9.30
«k A.-..
98-o'
970
97-4
III
966
97 ■>
969
97'4
97'4
97-4
97'4
973
97-6
97*4
968
968
97;4S
96.7
i
97-0
966
96-g
971
97-5
97-S
977
97-8
97-4
97'i
97-J
971
97->
97-j
97-0
97»
97'
97-»
97-0
974
97.01s
97-46
97-os
56-77
97-43
971S
Sounoa
of
bnmdj.
ti ounces
of
braudf.
6oimc«i
of
ID..5O-01CK&A.M..
10.30
">-*S ..
1 1. IS "
Il.JO
"■4S
".30
M.4.S
977
976
St
97-6
9775
97-1
97-6
976
97-5
''i
97-0
S?l
97'4
97'4
97-4
97-35
97»
977
97-4
97-S
Ill
964
9lS'8
9fi-fis
96-6
966
97'4
97-S
ST'-
97-|
97-6
97-S
97-4
97-»
974
974
96S
97-»
971
9T-'
971
97-1
97-»
97-3
97-05
97-1
97-1
97-4
MWH.
97J8
9TS9
97-]8
96654
97-16
97-<3
io'dooll-.«
4
6
,8-4
984
98a
98-1
98-44
97*
96-8
981
98-4
97 89
ti
97-4
97-4
,1,1
9»H
97-»7
97-81
98.6
97B4
'}
9S-4
9S-.
9^4
93'!
98
Jg-l
9*'44
98,9
98-=
of
brandj.
6oiin
of
brant
10.30
'0-4S ..
II. IS
11.30
11 o'clock ?,«..,
H-I5 ..
11.30
11-4S
9W"o
9*9
990
99-0
990
99-0
990
99-0
98-1
9S-1
981
98*5
98 '4
98 ■+
li
98-35
98-1
9S-3
Si
97-8
srs
9T-4
97 +
97*4
97-4
97*+
97'4
97" S
Mmd
98-833
9BJ46
9B-J.
97-66
io-cIo«kp.ii
t ;:
99;s
99-0
IK
994
99-4
99-1
99'3
"1
99-1
Haul
99'68
99.Il i oo'iS
jii.
If the rectimi temperatures, as being tu>. »
the following &re the mean daily tempenturea :-
1874.] Ii^aence ^Bnaufy m the Bodily Temperature Jfc. 187
The mean of the three water days was 98'67, and of the three days
with brandy 98-24.
There appears, then, to fae a alight iM on the brandy days. On refer-
ence to the larger Table giving the means of the periods, it will be also
noticed Qiat in the peiiods from 10 to 1 in the three hours immediately
anoceeding tiie brandy, the rectum temperature was not only lower in
two of the brandy periods, but sank twenty-sii times to fl8°-2 or below it,
■nd on one day sank to 97°'4 for more than »i hour ; while in the corro-
sponding periods without brandy, which include an equal number of oh-
aerrationB, it only sank three timea as low aa &8°'2, and never fell below
this. In other words, out of nine hours when brandy was taken, the
temperature was at 9^2, or below it, during 6] hours, while in other 9
konrs without brandy, at the same time of the day, the temperature was
at 98°-2 only for { of an hour, and was never lower. This seems conclu-
sive; for whatever conditions, independent of food and movement, may
cauae alight alterations in temperature (and the Tables show such con-
ditioDB do act), it seems impossible they should have acted twenty-six
times out of thirty-six when alcohol was taken, and only three times out
of thirty-six when alcohol was not taken.
On tracing the rectum temperatures on the se^'eral days tram 6 a.h.
to 1 P.U., the fall after alcohol is well marked on the fourth day, and is
quite perceptible on the sixth day, while on the second day it is only ob-
vioufl for an hour, and is not great. The explanation of this want of
nniformity may perhaps be that the processes in the body caoHing vario-
tions of temperature may sometimes act in the same direction with
alcohol and sometimes in the apposite, or, in other words, may sometimes
increase the fall and sometiiaes counteract it.
With r^ard to the amount of fall, the lowest rectum temperature on
the fourth day, when the effect of alcohol was most marked, was 97°'4,
while in the hours on the same day before alcohol tbe lowest was 97°-8.
If the effect of alcohol is measured by this difference, it amounts to
0°'4 F. ; if it is measured by the difference in the means of the two
periods, it amounts to 0°-39 Fahr. It seems hax to assume that 2-16 fluid
ounces, or 61 cub. centims., of absolnto alcohol produced a mean de-
pression equal to ^ of a d^ree Fahr. during three honra after alcohol
was taken.
The Faite and Se»piratu»it,
The pulse in this man was raised in frequency about five beats per
minute by the brandy, as will be seen from the following Table, where
the means of the periods only are given to save room.
Dr. £. A. Parkea on the
LFel).18i,
MMUipuke.
D.^.
■■
^'
J-
BjU,
S-
6.
Bmndj
BtlO.
From 6 to lo A.-., 1
S obserTftliona on V
taeh day J
j.iS
ss"
*677
47 '9
47'iS
4*7J
FromioA.u.toii'.ii.,'!
iiobeenstjoiuon \
jrs"
59<S
461
5''9"
+fi-i7
ss-rf
From 1 to id p.n., I
1,1
76
S9
65-6
66»
70.
Sphygniographic tracings B"ere token for me very carefully by Dr.
Hewett, Surgeou R.N., every hour ; niid forty-two were taken in sU.
I anuex a few traeiugs, which show the increased force of the heart and
the relaxations of the arterial coats.
20th January.
Tracing at 9.30 a.m., 15 j hours after food, and during rest.
Fulse 62; BeapiratioDH 15.
Tracing at 11 a.m. on the same day, during rest, 1 hour after 0
fluid ounces of brandy, 17 hours after food. Pulse 59. Bespira-
tions 11.
Tracing at 0.30 a.m., 15 j hours after food, and during rest.
Pulse 4!l. Respirations 12.
.-;——,..__.. „, ,-_ „ . il^ •, .^,„j^
1874.] Influence of Brandy on the Bodily Temperature ifc. 189
Tracing at 11 a.m. on the same day, 1 hour after 6 fluid ounces of
brandy, but with no food for 17 hours. Body at rest. Pulse 68.
Bespirations 9.
Tracing at 12.30 on the 21st January, 18 J hours after food. No brandy.
To show the effect of fasting. Pulse 48. Bespirations 11.
The respirations were slightly lessened in number.
General Condusians,
I believe the following conclusions may be drawn from the observa-
tions formerly recorded (Proceedings of the Boyal Society, Nos. 120,
123, and 136) and from those now laid before the Eoyal Society.
1. When brandy in dietetic doses (=s2*16 fluid ounces, or 61 cub.
centims., of absolute alcohol) was given to a healthy man i^ting and at
rest, a decided, though slight lowering, of bodily temperature (as judged
of by the heat of the rectum) was caused. The amount of lowering was
under i a degree of Fahrenheit ; and sometimes even this amount was not
perceptible, being probably counteracted by the opposing influence of the
heat-producing changes in the body, which cause slight variations of
temperature independent of food and movement. The greatest effect
was produced from about one to two hours after the alcohol was taken,
and the effect was evidently passing off in three hours.
2. When brandy in dietetic doses was given to a healthy man at rest
and in whom the process of digestion was completed, and whose tempe-
rature raised by tiie food was again commencing to fall, a lessening of
temperature was also proved, but its amount was not so great ; it could
not have been more than 0^*35 Fahr., and may have been only 0^*07 Fahr.
3. When alcohol was given with food, with either usual or increased
exercise, no effect on temperature was perceptible, even though the
alcohol was given in large quantities, viz. from 4 to 8 fluid ounces of
absolute alcohol (114 to 227 cub. centims.) in twenty-four hours. It is
to be presumed that the amount of heat generated from the food and
movement concealed the effect of the alcohol, which would require a more
delicate method or longer observations for detection.
4. In no case did alcohol raise the temperature.
5. The effect of alc<^ol on the pulse was uniform in the four men experi-
190 Mr. J. Cottrell on the Division of a Sound- Wave [Feb. 12,
inent«d upon. Thf pontTftctions of the heart were more frequent after
alcohol during complete rest, from five to ten beats per minute for aome
time ; and when eiercise was taken the inorease was greater. The mean
pulse of the twputy-four hours was, however, not increased unless the
amount of alcohol was large and repeated. In other words, the heart's
beats were less frequent than naturftl when the effect of the alcohol had
passed off. The pulse became both fuller and softer to the touch ; and this
relaxation of the radial artery was shown also by the sphygmi^Taph. That
the smaller vessels were relaied, was shown both by the redness of the
surface and by the erident ease with which the blood traversed the capil-
laries, as shown by the sphygmographic tracings.
6. The respirations were not increased in number by alcohol ; they
were rather lessened, and were deeper in some of the experiments ; but
the effect was not very marked.
. " Experimental Deraonst rations of the Stoppage of Sound by
partial Reflections in a n on -homogeneous Atmosphere." By
John Tyndali, D.C.L., LL.D., F.R.S., Professor of Natural
PLlloaophy in the Royal Institution.
(See Paper read Jan. 15, ante.)
IV. " On the Division of a Sound- Wave by a Layer of Flame
or heated Ga« into a reflected and a transmitted Wave." By
John Cottrell, Assistant in the Physical Laboratory of the
Royal Institution. Communicated by Professor Tyndall,
F.R.S. Received February 2, 1874.
The incompetency of a sound-pulse to pass through non-homogeneous
air having been experimentally demonstrated by Dr. Tyndali, and proved
to be due to its successive part^ reflections at the limiting surfaces of
layers of air 'Or vapour of different density, further experiments were
conducted in order to render vistUe the action of the reflected sound-
wave.
The most successful of the various methods contrived for this purpose
consists of the following arrangement. A vibrating bell contained in a
padded box was directed so as to send a sound-wave through a tin
tube, B A (38 inches long, 1| inch diameter), in the direction BF*, ite
action being rendered manifest by its causing a sensitive flame placed at
F* to become violently agilat«d.
The invisible heated layer immediately above the luminous portion of
an ignited coal-gas flame issuing from an ordinary bat'a-wing burner
1874.] by a Layer of Flame or Heated Go*. 191
was allowed to stream upwards across the end of the tin tube B A at A.
A portion of the sound-wave issuing from the tube was reflected at the
limiting surfaces of the be«t«d layer; and a part being tnuumitted
through it, was now only competent to slightly agitat« the sensitiye
flame at F.
The heited layer was then placed at such an angle that the reflected
portion of the sound-wave was sent through a second tin tube, A F (of
the same dimensioas as B A), its action being rendered nsible by it4
causing a gecond sensitive flame placed at the end of the tube at F to
become violently affected. This action continued so long as the heated
layer intervened ; but upon its witiidrawal the sensitive flame placed at
F", receiving the whole of the direct pulse, became again violently agi-
tated, and at the same moment the sensitive flame at F, ceasing to be
a&ected, resumed it-s former tranquiUity,
Exactly the same action takes place when the luminous portion of a
gas-flame is made the reflecting layer ; hut in the experiments above
described, the invisible layer above the flame only was used. By proper
adjustment of the pressure of the gas, the flame at F can be rendered
so moderately sensitive to the direct sound-wave, that the portion trans-
mitted through the reflecting layer shall be incompetent to affect the
flame. Then by the introduction and withdrawal of the bat's-wing flame
the two sensitive flames can be rendered alternately quiescent and
shrongly agitated.
An illustration is here afforded of the perfect analogy between light
and sound ; for if a beun of light be projected from B to F*, and a plate
of glass be introduced at A, in the exact position of the reflecting layer
of gas, the beam will be divided, and one portion will be reflected in the
direction A F, and the other portion transmitted through ^e glass in
the direction F*, exactly as the sound-ware is divided into a reflected and
transmitted portion by the layer of heated gaa or flame.
192 Mr. J. Y. Buchanan on the Absorption of [Feb. 19,
February 19, 1874.
JOSEPH DALTON HOOKER, C.B., Preaident, in the Chair.
The PresentB received were kid on the Table, and thanks ordered for
them.
The following Papers were read : —
I. " On the Absorption of Carbonic Acid by Saline SolutionB."
By J. y. BucHANiiN, Chemist on board H.M.S. ' Challenger.'
Communicated by Prof. Williamson, For. Sec. R.S. Re-
ceived December 11, 1873.
(AbstTBCt.)
Until lately it was beheved that the atmospheric gases disBolved in
Bfla-water could be extracted from it, as from fresh water, by boiling in
vacuo. The merit of the discoyery that such is not the cose is due to
Dr. Jacobaen, of Kiel, who found that, in order to drive out the whole
of the carbonic acid, the water must be evaporated almost to drvueBS,
and that no amount of boiling m vacMi will Bufiice to eliminate it. Being
particularly interested in the matter, I immediately commenced a series
of experiments to determine, if possible, the salt or salts to which sea-
water owea this property.
Preliminary obBerrationa satiafled me, in the first place, that sea-water
has this property, and, secondly, that solutioiu of the enlphates of mag-
nesia and of lime possess the same property. In order to gfun more
precise information, two series of experiments were made, the one auA-
lytical, the other synthetical. The former consisted in saturating saline
solutions with carbonic add, and then distilling them, the carbonic acid
passing in the various fractions being determined ; the latter, in deter-
mining the absorption coefficients of two solutions, the one of sulphate (A
magnesia, the other of sulphate of lime.
First, the analytical series. — Before proceeding to saline solutiona,
distilled water was eatur&ted with carbonic acid and distilled. The first
eighth of the distillate contained abundance, the second a trace, and the
reminder no carbonic acid. It may therefore be assumed, in the ex-
periments which follow, that the carbonic acid held simply in tolvtion by
the water passes almost entirely in the first eighth of the distillate, and
that whatever passes afterwards has been retained, in some way or
other, by the salt in solution.
Experiments were made on sdutions of sulphate of magnesia, of sul-
phate of magnesia and chloride of sodium, and of sulphate of lime, to
which were added some on sea-water itself. In every experiment the
quantity of solution operated on was 300 cub. centims., which was
boiled in a flash connected by a doubly bored cork with a Liebig's con-
denser, which was fitted at Its other end, air-tight, into a tubulated
1874.] Carbome Aeid by Saluu Solutiimt. 193
reosiTer. To the tnbnlnie wm attached a bulbed U-tnbe, and, b;
mcAoa of an atpirator, air could be constanUy sucked through. The
oarbonic acid coming off was retuned hy barfto-wster of known Btrength
distributed between the receiver and the TJ-tube ; what remained unneu-
tralized was determined hy oxalic acid, the point of neutraliution b^ng
indicated by roaolic add. The oxalic add was rather stronger than
tenth ncomal; it contained 6-478 grammes 0,H,O,+2H,O in the
}itn. One litre baiyta-water required 3235 cub. centims. oxalic acid for
neutralization.
The method of conducting the operation waa as follows : — Carbonic add
was passed through the solution until it could be assumed to be satu-
rated. The object being to determine the carbonic add retained by the
■alt, it was necessary to get rid, as much aa possible, of the simply dis-
■d.Ted gas. This waa effected by drawing six or seven litres of air
through the solution cold, then heating it to boiling, and allowing it to
bdl for a couple of minutes in a current of air. The receiver, with the
baryta solution, was then attached, and the distillation continued in a
current of air, until the contents of the flask were nearly dry. The
amount of carbonic acid was given by the remaining alkalinity of the
baryta-water.
Experiments on sulphate-of-magnesia solution, 'containing 12*3
grammes crystallized salt per litre. — As all were conducted in precisely
the same way, it will be suf&cient to give the results in a tabular form.
The first three experiments were made with one and the same solutioa ;
for the last two a fresh solution, prepared, to all appearance, in exactly
the same way as the previous one, was used. The difference in the results
shows the precarious nature of the combination.
TolamB of
■olaUoaiarfL
Tolutno of
Tolome of
ouboniaadd
in 800
OUb.MDtimik
OrunuM
osrboDiouid
in one litre.
cub. cantinu.
300
SOO
800
300
300
odU OBDtmu.
2S
10
10
16
10
onb. oentinu.
78-96
SOW
30-90
4750
si-sa
(HI04S
IH)063
0O033
fUKSS
00023
00143
O0166
frOllO
oom
0-0077
Two experiments were made with a solution prepared as follows : —
The quantity of sulphuric add necessary for the formation of 12-3
grammes crystallized sulphate of magnesia was dilated to a litre, and pul-
verized carbonate of magnesia suspended in it. Although the mixture
was allowed to stand over night, shut off &om the influence of the
atmosphere, the solution was still very add. It is well known that car-
bonate of magnesia is difficultly soluble in cold dilute adds. To have
heated the soludon would have frustrated the object of the experiment,
which was, by bringing nascent sulphate of magnesia together wiA
194 Mr. J. Y. Buchanan on (he Absorption of [Feb. 19,
□aBcent carbonic acid at ordinarr temperaturee, to gire them the be^t
opportuoitv of combining. Two expenments were made nith a sinii-
lariy prepared solution of sulphate of lime. In this case aulphurio acid
was added to tbe water in quantity sufficient to form, wilh lime, more
salt than nould dissolve in the liquid. Here neutralization took place
without difGculty ; and, aa might have been expected, the amount of
carbonic acid found was considerably greater than in the case of tbe
magoeaia salt.
Two experiments were made with an ordinary sulphata^f-mi^esia
solution, containing 2'05 grammes crystallized salt per litre.
Two further experiments were made with a aolution containing 2'05
grammes sulphate of magnesia and 30 grammes chloride of sodium per
litre. All were conducted in the way described above, and the results
are given in the following Table. The experiments with the carbonates
of magnesia and of lime were made at a couaiderably later date than tbe
others; the i-alue of 10 cub. centims. baryta- water had in coosequence
become equivalent to 32-i) cub, centims, instead of 32-34 cub. centima.
oxalic acid : —
KgC0„H,80^ I
0,. H, SO, I
+NaCl.,'
Tolume of
Tolums qF
Tolmue of
«>lut.<»i.
oxaUoruid.
ub. centimi.
cub. oentim*
300
10
30-B
300
10
309
300
10
275
300
10
27-5
300
10
312
300
10
31-3
10
31-6
300
10
31-4
0<)0.'i2
Ofl026
0-1014
0-tOU
0-OOW
000-J3
0-0016
OiXIST
01X177
0-00&3
IMW70
I
Five experiments were made with Beft-wat«r taken at the end of Porto-
bello Pier, on the Firth of Forth. In the first three it was submitt«d
immediately to the same treatment as the saline solutions ; in tbe last two
carbonic add was fint passed through it for some time. As the results
are identical, it is evident that, in its natural stat«, the water in question
was practically saturated with carbonic odd in this peculiar state of com-
Tolume of
Tolume of
Volume of
Qrammes
GrsmmM
csrbouio>md
in one litn.
bsryta-water.
•mlicadd.
in 300
cub. centim*.
onb. o(mtin».
cub. cenlins.
cub. oenUms.
300
16
39-75
0<I198
0-0660
300
10
23flO
o^H^l
0-0703
0-0208
04693
00203
10
00203
0-n«TT
1874.]
Carbottie Acid by Saline Sohiiioru.
19S
From the large unount of oi^anic matter pouied into the Forth in the
neighbourhood of Portobello, there must be an abundant production of
carbonic add in the vater itself ; and we hare Been above the effect of
bringing it together in the nascent state with sulphate of lime. Sea-
water contains on an average about 8 parts sulphate of lime in 10,000.
A saturated solution of the same salt in distilled water containa, at
1^ C, 24 parts in 10,000. Under the most favourable circumstances,
tlten, sea-water might be expected to bind about one third of the quantity
rebuned b; an equal volume of saturated gypsum eolutaon. We have
seen that a litre of this solution is cap^le of rettuning 0-338 gnn. CO^
while the same volume of sea-water contained at the most only 0*07
grm., or very little more than one fifth of that held by the sulphate of lime.
In ocean-water I have never yet found more than 0-064 grm. CO,
per litre, including both nmply ditaolved and half bound. We have, then,
in the sulphate of lime alone an agent capable of retaining much more
carbonic acid than is usually found to exist in sea-water ; and there is
besides the sulphate of magnesia ; so that whatever may be the function
of the other salts, we do not, in order to find a vera eauia for the phe-
nomenon under consideration, require to go beyond the sulphates ; and
the practical lesson to be learned is that, if we get quit of the sulphates,
the carbonic add will be more easily disengaged by heat.
This is entirely borne out by experiment. In determining the car-
bonic add in sea-water, I always add to It a suifident quantity of a satu-
rated solution of chloride of barium ; and I find that, after about the
first fifth of the distillate has passed, there is rarely a perceptible tur-
bidity in fresh baryta-water.
The synthetical experiment consisted in determining directly the
coetGdente of absorpUon of a 1-23 per cent, solution of dyBtalliied
sulphate of magnesia and of a 0-205 per cent, solution of Ga SO,
•f 2H,0. In Table I. the results of experiments on the magnesia so-
lution are given, where the obserrationa were mode without loss of time.
In Table II. the reeolts of experiments on the some solution are
given, only here the duration of the reaction was taken into account.
The first reading was made at the highest pressure after the gas and
solution hod been together for nine d«ys ; the pressure was then succes-
sively reduced, and the other readings mode at iuterrals of twenty-two,
forty-one, and twenty-five hours from each other, the last of all being
mode only after the lapse of some days. Table HI. gives the results oF
experiments on the gypsum solution, the readings in this case being
made without allowing much time for the reaction to take place.
T&BLB I.
Temperature C
Absorption ooeffioieDt ot Mg SO^ solution.
Abaorption ocwffloinit ot wiier
476-M 652-7
68114
11^
73673
196
Mr. A. E. Donkin on an Instrument for the [Feb. 19,
Table II.
Pressure in millims 832'7
Temperature C ll'l
Absorption coefficient of MgSO^ solution' 1*2467
Absorption coefficient of water 1 '3052
696-3
11-0
0-9331
1-0446
651-6
10-45
0-8823
0-8461
498-1
111
0-8974
07546
468-6
111
0-8221
0-7014
Table III.
Pressure in miUims
Temperature C
Absorption coefficient of Oa SO^ solution
Absorption coefficient of water
554-9
683-8
765'3
770-8
805-2
869-5
10-1
12-9
13-3
11-1
111
11-65
0-8845
0-9923
1-0651
1-1885
1-2191
1-2964
0-8617
0-9618
1-0624
M534
1-2048
1-2757
The general result of these experiments is, that sulphate-of-lime sola-
tion absorbs a little more carbonic acid than water, but follows the same
law of yariation with temperature and pressure; sulphate-of-magnesia
solution differs slightly from water when but little time is left for the
reaction to complete itself. If, however, the gas and solution are left in
contact for a considerable time, the difference between the coefficients
of water and of the salt solution becomes very marked, that of the latter
being less for high pressures and greater for low ones than that of water.
The details of these experiments will be found elsewhere in a more
extended paper.
II. '^ On an Instrument for the Composition of two Harmonic
Curves." By A. E. Donkin, M.A., F.R.A.S,, Fellow of Exeter
College, Oxford. Conmiunicated by W. Spottiswoode, Treas.
R.S. Received November 6, 1873.
The interest in such compound curves lies in the fact that as a simple
harmonic curve may be considered to be the curve of pressure on the
tympanic membrane when the ear is in the neighbourhood of a vibrating
body producing a simple tone, so a curve compounded of two such simplS
harmonic curves will be the curve of pressure for the consonance of the
two tones which they severally represent, and thus the effect on the ear
of different consonances can be distinctly represented to the eye.
If the motion of a point be compounded of rectilinear harmonic
vibrations and of uniform motion in a straight line at right angles
to the direction of those vibrations, the point will describe a simple
harmonic curve.
Thus a pencil-point performing such vibrations upon a sheet of paper
moving uniformly at right angles to their direction would draw such a
curve.
The same kind of curve would also be drawn by keeping the pencil
fixed and by giving to the paper, in addition to its continuous transverse
motion, a vibratory motion similar and parallel to that which the pencil
had ; and if the motion of the latter be now restored, a complicated curve
will be produced whose form will depend on the ratio of the numbers of
198 Mr. A, E, Boiikm on an Instrument for the [Feb. 19,
number of teeth, the relative angular velocities of the spindles can be regu-
lated at pleasure. The paper upon which the curve is to be drawn is carried
upon a rectangular frame, E F G- H, capable of sliding horizontallj up and
down in a direction parallel to that of the plane passing through the spin-
dles. This frame has a pair of rollers, £ F and G H, at each end connected
by tape-bands, between which the paper passes as tl^ rollers turn. In order
to give a motion of revolution to the rollers, a wheel, L, is fixed upon the
axis of one of them whose teeth gear into those of a pinion, P Q, along-
side which the frame slides, and which is itself driven by one of the
vertical spindles. A connecting-rod, D M, is carried to the frame from the
crank of this spindle, so that upon turning the latter a vibratory motion
is given to the former ; and since the transverse motion of the paper also
depends upon the same spindle, a fixed pencil-point resting on it would
draw a simple harmonic curve whose amplitude would depend on the
radius of the crank, and wave-length on the transverse speed of the paper,
which can be regulated at pleasure by means contrived for the purpose*.
A vibratory motion similar and parallel to that of the frame is given
to a small tubular glass pen, B, so arranged as to move with its point
lightly resting upon the paper. This motion is communicated by a con-
necting-rod, G N, from the other crank, which is carried underneath the
sliding-frame and jointed to the lower end of a small vertical lever, S, to
whose upper end the arm carrying the pen is attached.
The weight. W serves to regulate the pressure of the pen on the paper,
as it can be screwed in or out. T is merely a pillar upon which the
change-wheels can be placed for convenience.
If the pair of wheels on the spindles are now connected by the inter-
mediate one, it is plain that, upon turning either of the spindles by a
winch provided for the purpose, the two motions of the paper will be
combined with that of the pen, and the curve drawn will be that com-
posed of the two simple harmonic ones, which would be the result of
separately combining the harmonic vibrations due to each crank with the
transverse motion of the paper. Thus if m and n are the numbers of teeth on
the pair of wheels respectively, the equation to the resultant curve will be
y==sin nur-fsin nx.
This equation implies that not only are the radii of the cranks the same,
but also that they start parallel to each other and at right angles to the
vertical plane passing through their axes : both these conditions can, how-
ever, be altered ; and therefore the general form of equation to the curves
which the machine can draw will be
y=a sin (wM?+a) + 6 sin (na? + /3),
* It should be obserred here that the yibratory motion thus giyen to the frame is not
truly harmonic. In order to make it so, a more complicated oontriTanoe than the simple
cnvk and connecting-rod would have to be adopted ; but this would probably introduce,
through unavoidable play, an error greater than the present one, the length of the con-
necting-rods and the small size of the cranks rendering the latter nearly inappreciable. The
motionwill, however, for the sake of convenience, be considered truly harmonic throughout
1874] CompoHtioH (fftvo Hatraome Oueve$. 109
vkere a and b are the ndii of the cranks, uid a and ^ are dependent
(m tiieir relative incUnatioiiB to the above-mentioned vertical plane at
starting.
A^ an example, suppose that a^b, while theratioof m tonisasStol;
tien the above equation will repreeent the cuire of pressure tor the octave.
Similarly, if n> is to n as 1 6 to 15, the resultant curve represents the effect
on the ear of a diatonic semitone, while the ratio 81 to 80 would give
that of the comma. Jn both these curves, and more eBpe<:iall7 in the
latter, the beats which would ensue on actually sounding the two tones
together are shown with remarkable distinctness.
As the machine is provided with a act of change-wheels, many different
curves can be produced, while the form of each can be more or less
changed by altering the relative positions of the cranhs before bringing
the idle wheel into gear. It is also poesible to obtain very large valoes
of m and n in the above equation by using two idle wheels on the same
axis which shall come into gear, the upper one with the wheel on the one
spindle, the lower one with that on the other.
Thus, suppose A and B are the numbers of teeth on the spindle-wheels
respectively, C and D those on the idle wheels, and let A gear with C
and D with B ; then — = -j= . Now, by properly choosing the four
wheels, large values of m and n maybe obtained. If, forinstuice, A^sSl,
B=80,C=55,andD = 27, - = ||^, this ratio being nearly = ^,the
corresponding curve will represent the effect of an octave slightly out of
tune. The period of such curves as these being very long, it is necessary
to have a good supply of paper ; and this is arranged by carrying a reel-
full on the horizontal frame, from which it is slowly unwound between
the rollers. The rate at which this takes place has a good deal of influ-
ence on the form of the resultant curve ; the slower it is the more com-
pressed wiU the latter appear. Instead of using paper, the curves, pro-
vided the periods are short enou|^, may be drawn on slips of blackened
glass, which can be carried along between the tapes connecting the rollers ;
they can be at once placed in a lantern and thrown on a screen.
The width of contour of any curve depends on the radii of the cranks ;
these may have any value between 0 and half an inch, and therefore the
limit of possible width at any part will be two inches ; so also, by altering
the radii, a series of curves may be produced corresponding to the con-
sonances of tones not of the same intensitiei. Since the mmn'miiin width
of any curve will be double the sum of the radii of the cranks, the paper
is cut to a width of two and a half inches, within which all curves which
can possibly be drawn will be comprised.
The instrument is constructed by Messrs. Tisley and Spiller, of
Brompton Boad, to whom some improvement upon the original model
is due.
300 Mr. W. Shanks on the Period of the [Feb. 19,
III. " On the Number of Figures in the Period of the Reciprocal
of every Prime Number below 20,000/' By William
Shanks. Communicated by the Rev. Geo&ge Salmon.
Received December 2, 1873*.
The following Table, in reality the joint production of the Bev. G^rge
Salmon, F.R.S., and myself, was commenced, and indeed nearly com-
pleted, before either calculator was distinctly aware that Burckhardt,
Jacobi, or Desmarest had written or published any thing on the same
subject. This fact is perhaps to be regretted ; but it has led to the in-
dependent recalculation, by two different methods, both of Burckhardfs
( Jacobi's Table is professedly a reprint of Burckhardfs) and of Desmarest's
Table, and has resulted in the detection of several errors, which have, as
far as I know, never before been pointed out. These errors, in the first
place regarded as discrepancies, have been carefully examined ; in fact
every case has been reworked by me, with the view of either proving or
disproving the accuracy of such numbers as differ from those in our
Table. The result is, that such discrepancies are found to be errors both
in Burckhardt and Desmarest. The two lists of errors are given below.
I now proceed to give the theorems used, and some account of the
means employed by me in forming the Table.
Let P be any prime number, except 2 and 5. Then, from Fermat's
theorem, we have p ^1 ; or, adopting the usual notation, 10^"^=.!.
Again, since the number of figures in the period of the reciprocal of
all primes is not P— 1 (or, in other words, since 10 is not a primitive
root of all primes),
p-i
Let 10 ** "=1, where n is even or odd, not less than 2, and not greater
than Q • Then we have
(1) The number of figiures in the period of the reciprocal of P is either
P — 1 or a submultiple of P — 1. , ^,
(2) Let a and b be integers, and let m be the remainder from -p ;
that is, let 10*=w ; then lO-^—m*.
In practice b is never greater than 2, at least Httle or no advantage is
P-1
gained by putting b higher. Also ab need not be greater than — s— *
P-1 .
Car, When m is greater than — o — we may obviously use P — wi, or
simply — m ; for (P— m)*=P— 2Pm-hm'^m", or, because (— w)'=m*,
b being 2.
(3) Let lO'^m, and 10»=n; then 10«+*=mn.
In practice a-f-6 is never greater than P — 1.
Cor, 1. When m and n are each of them less than P, we may with
advantage use —m and — n ; that is, we may subtract m and n severally
from P ; for (P-w)(P— n)=P^-P(m4-n)4-mn=(— w)(— n).
P-1 P-1
Cor. 2. When m is > — ^ , and )* is < -g— , or vicr versd, we may use
* The part from 17,000 to 20,000 was receired January 8, 1874.
1874-.] Reciprocal of every Prime Number below 20,000. 201
— m and m, or wee vtrfd, obtainiiig a negative result, which becomes
positive by being subtracted from P. p_.
(4) Let 2c and 3r, not greater than — 3— > be submultiplea of P— 1 ;
andletlO'£s+a,and lO^sS-l; thenlO*= + l. This is evident from
(2) and (3). t^
From (1) we have 10 • s: + l, according as the submuldple of P-1 is
even or odd.
On these theorems and adjuncts my calculations have been based.
They enable us to find the remainder either from - ■ p— , or from any
Bubmultiple, such as — &-, or from any figure in -p— > and, if required,
the jiffxtre itself. Compared with other methods, such for instance as
Dr. Salmon's •, mine may seem tedious, reqiuring as it does much multi-
plication and division. All I can say Is, I did not find it so, though I
am free to admit that the calculation of such a Table as ours demands
very considerable labour.
It would be foreign to my purpose to enter upon the consideration of
primitive roots, or even of prime numbers. If wo have found 10 to be a
prinutive root of a great many prime numbers between 10,000 and
20,000, we havo contributed somethiDg, as far as I know, quite new.
In addition to this we have found the number of figures in the period of
each of the other primes between 10,000 and 20,000, and have corrected
upwards of 70 errors in Burclchardt's and Desmarest's Tables.
I beg to refer to the works of Euler, Lagrange, Legendre, Gauss, Foiusot,
Cauchy, and Jacobi (mentioned by Desm&rest), and to Desmarest himself,
for valuable information touching prime numbers and primitive roots.
Icannot, however, refrain from quoting from Desmarest's ' ThiJorie des
Nombres ' the view of Euler as to prime numbers and primitive roots :—
" On ne pent saisir entre un nombre premier et les racines primitives qui
lui appartiennent, aucune relation d'oi Ton puisse d^Juire vm teule de
ces racines, de eorte que la loi qui r^gne entre elles parait aussi profondii-
ment cach^ que celle qui eriate entre les nombres premiers oux-memes."
Not discouraged by Euler's remark, Desmarest thus writes :^" Car
pourquoi nous serait-il d^fendu d'ajouter que-nous croyons que I'intel-
ligence humaine n'a pas, sur ce point, dit son dernier mot, et que les
operations nombreuses que nous avons dQ faire sur les nombres, ne nous
ont pas convaincu de I'impossibiliti) de saisir, sinon I'ensemble, du moins
quelques-une des uineaux de la chafne mysterieuse qui unit les racines
primitives aui nombres premiers."
■ Note bff Dr. Sahnait. — The method here referred la i> explained, ' Ueegongsr of
M«tb«nMtiW (1872), p. 4». It ia founded on the remirk th«t if we havo 10'=2^,
10»£22*, wemflTdedue6ltW~'» = l. Thus, let the prime be 251. we ram at ones writa
down the equaUom 10'=-2', 2f=W, whence imraediBlely KF' = -1, 10"'=1.
In like manner from the oquations I0« = 2'3', lO'E:^2-a<, ll)'=2»3', we deduce (hat
the number of flguna in the period of the reciprocal of the prime ia
a(mr — n j)+i(np — r/) + eOq — ntji ) ,
Bj the appliraition of thaw principle* I caloulatea tlw TwiUa (ftAMiwi 'w^ ** ^*"
lowing Table aa far as 1 850ft Por dw primes above that nuwtoeT "SLt. Woa'ti w w^A-J
mponMUe; hi/mfeipmnKieof hisaccunw^givp* iiiooonftA»T\RoV(v'\v\« t«»™*>
J - -T J
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8521
355'
97
»57
II
314
8609
538
ZI
4620
i>
924
8681
4340
51
2325
II
4650
8893
4446
71
8999
8998
dbe .
9067
9066
1
ri
9187
9186
3
2471
II
4942
9397
4698
I
2540
i»
1270
9521
952
7
5106
II
»553
! 9629
4814
7
901
II
1802
9649
1206
9
5478
II
2739
9941
9940
9
5518
11
2759
I<(.I3. There are 64 errors, 3 miaprints, 2 omisi
(ions, m. 3 s
md 78
Table II. List of Errors in Burckhardt'a
and Jacobi's Tj
V« -'«
1874.] Recipreealnf ever]/ Prime Number below SO,(m. 30S
In tbs laft-tund eolnmni of X*U« m. «ra pritnM ; in the right-hand columni, iinme-
di«(dj <9pa*it«, U tlia numbw of flgtUM in Uw period of the reciprocal of cull pnioe.
s
,
1"
■ss
691
130
1109
liol
.567
1566
7
t
I'l
111
701
700
1117
n*
'57'
.570
1"7
79
709
70I
11.3
56.
'S79
.571
■3
6
311
7>9
\n
1119
564
'ill
1381
"7
16
117
lit
717
"5'
575
'597
'13
>9
13
il
»7
349
III
713
719
Ci
146
;;il
"i:
i<oi
1607
1606
19
iS
351
31
743
74*
"V
1170
.609
}■
■ 5
359
■79
75'
>»S
nil
iilo
1613
,r.i
37
3
367
iil
757
17
.,17
591
1619
4>
1
171
i>6
761
380
"91
1191
■e«t
■ Gio
41
179
37I
769
191
■617
171
47
4«
3I1
31*
'Z'
'91
iiij
.637
409
53
'1
II9
3"
7»7
393
1117
•i
Ail
59
i*
397
99
797
199
1113
61
60
401
I09
1119
ml
,667
S33
«7
7«
11
15
409
4>9
3
In
111
lio
Ito
1131
1117
4i
1669
1691
556
73
i
4»i
140
!!'J
IM
1149
108
,697
•%
79
■1
431
»5
117
4)1
11S9
115I
1699
13
41
431
43*
119
»7i
"77
638
1709
1701
■9
;j
439
119
S19
419
1179
639
1711
430
91
441
>SJ
11}
"|3
64.
1S7
4
449
3a
>57
isi
Ills
91
1731
S6$
lOJ
14
♦57
:i:
>f9
16
1*91
1190
174'
1740
53
4ii
"3
i6i
"97
1*96
■747
191
109
■ol
4«1
>54
I77
43I
1301
'300
'753
1**
t<3
467
*11
Hi
44°
1303
1301
'759
879
»7
4a
479
139
II3
t&
1307
651
"777
'776
■ !■
130
4>7
4>i
llj
1119
6S9
.783
17S1
■ 37
1
491
490
907
'5'
1311
Si
1787
«33
139
4<
499
49>
911
455
1317
1316
1789
1781
149
143
Soj
SOI
919
•i
.36.
Mo
iloi
900
1(7
;i
509
JSI
50*
919
937
,367
1373
•&
i8it
,S»3
iSio
■ 111
Jj
Si
5"J
»it
941
940
.3Si
,j,„
,831
■M
167
i6t
541
S40
947
471
1399
ij!
\lVr
173
43
547
9'
^
95*
1409
J?
179
17I
^V
•z>
311
'4»1
■i'
1I67
911
ttl
ilo
sh
all
971
970
1417
713
1I71
915
igl
95
569
at4
977
lU
'4*9
.4.1
,73
.87.
'91
iji
571
570
9S3
9S1
'413
'4J»
.877
931
197
9l
577
57«
991
4?i
1419
.»
'«S»
111
199
99
S»7
193
997
166
"447
1SS9
3I0
10
591
59"
1009
iji
■4S'
.90
1901
»»1
599
199
I013
»^a
■451
716
,907
953
i»7
113
601
300
1019
toil
'459
iGi
1913
''«
aa9
ail
foj
^'
715
1931
3S6
13s
■1»
61 J
S'
1031
lOJ
740
'933
139
7
fii7
IS
1033
1031
14S3
H7
"949
I94»
14>
10
C19
Cil
1039
5 '9
14S7
1416
"95 >
>97l
IV
»s«
50
63?
3'S
■049
5H
.4S9
148
"971
:i5
:i:
&
1»
;a:
1050
"491
■499
371
114
'979
19I7
>«|
iCS
<47
1063
1061
1511
7SS
"993
«J
171
5
<!3
?>
106^
IO«l
'5*1
761
•997
99*
»77
3
'»
k
>ol7
1086
'53>
1530
'999
,9»
ill
ill
1091
1090
'543
■S4»
lOOJ
\
>91
•a
!"
i
109J
1097
:S
'549
>S$1
MM
107
Hi
«,
3*'
HOJ
'»»
\ "'
\«A1
\ \oi-i
<*
* .
1111
III]
i I 29
1141
1143
1153
1161
"79
1203
1207
1213
1221
1237
1239
1243
1251
1267
1269
1273
L281
1287
1293
•297
.309
311
333
339
341
347
351
357
J7I
177
j8i
;83
189
93
, ^055
2621
2620
21 I 2
26',3
2632
5 3'-
2647
S3-
7ID
26,-
26ci6
2136
2659
886
2140
2663
2662
2142
2670
1335
2152
2677
223
30
2683
447
2178
2687
2686
XIOI
2689
42
2206
2693
1346
553
2699
2698
2220
2707
1353
1118
271 1
'355
IXX9
2713
2712
1121
2719
1359
2250
2729
682
''11
2268
2731
2730
2741
2740.
227a
*749
9x6
228
2753
2752
762
2767
2766
1 146
2777
2776
2296
2789
2788
2308
2791
31
583
1797
699
280X
X400
2338
2803
140X
2340
2819
28x8
1173
2833
2832
"75
2837
709
1x78
2843
142 X
2370
2851
2850
264
2857
408
476
2861
2860
2382
2879
1439
2388
2887
2886
i8>i
tinf
_o_/r
3II9
3I2I
16
3
3167
3169
318X
3187
3191
3203
3209
3217
322X
3229
3*51
3*53
3*57
3*59
327X
3299
330X
3307
3313
3319
33*3
33*9
3331
3343
3347
3359
336X
3371
3373
3389
339>
3407
3413
3433
i>S9
156
3156
15S1
3166
72
636
177
29
1 60 1
x634
X072
3220
X076
3250
54a
3256
3258
X635
3298
3300
X653
3312
553
x66i
832
3330
334*
X673
X679
x68o
3370
843
3388
169s
3406
1706
343*
3623
3631
3637
3643
659
671
673
677
691
697
701
709
719
727
733
739
76X
767
769
779
793
797
803
821
823
833
847
851
853
863
877
881
889
907
9"
9>7
919
923
jU 1 u
3622
I8I5
9^(;
1821
3658
367
3672
X838
X23O
1232
3700
3708
1859
3726
933
1246
x88o
3766
1884
3778
1264
949
X901
3820
X274
3832
3846
770
963
3862
969
X94O
'944
"953
1955
X958
653
xg6i
1874.] Recijtrocal 0/ every Prime Number below SO,COO. 205
Table III. (co^ainatd).
♦603
1301
5 "47
*S73
5689
3'6
6*47
6146
680,
3401
4611
914
5'S3
S'S»
5693
■4»3
6*57
6.56
68a3
6811
4*17
61
S'«7
s,U
570 "
5700
6163
6161
68*7
3413
4639
13 19
SI71
57"
571
6x69
6x68
6Sa9
6818
4643
1311
5179
S'78
57'7
1419
617,
1045
6833
683*
4649
7
5189
Si8g
5737
S736
6*77
'569
684,
«ss
46s.
4650
S>97
433
574'
5740
6187
6:iti
68S7
68s6
4*57
'SSI
SK>9
371
5743
57*1
6199
94
6863
686a
46*1
S117
161 J
5749
5748
630"
6869
6868
4673
4*7»
S»3'
1615
5779
1889
6]. 7
3158
687"
3435
4679
»339
5*33
S131
5783
5781
6313
3.61
688,
344"
+69.
4690
S»37
77
579>
96s
63*9
316+
6gg|
^898
4703
4701
516.
lOJI
jgo.
"45°
6337
6336
6907
"151
47»"
1360
S»73
S171
5807
5806
6343
6341
691,
3455
47*3
.361
S»79
»639
58.3
1906
6353
635»
6947
3473
47»9
1181
5.81
.64=
SUi
siio
61 S9
3'79
6949
694*
4733
■ 18]
5197
5196
S!»7
1913
6j6i
1590
tut
3479
475'
»37S
5303
5301
5839
1919
6367
6j66
3480
4759
»179
5309
S3o8
5843
1911
6373
106a
6967
6966
47»1
47S»
S3»!
1661
5849
1461
*379
aii6
6971
6970
47«7
»393
SJ33
"333
85?
'95°
6389
6388
6977
6^6
4789
iiS
5347
>673
S»57
5856
6397
78
6983
6981
4793
4791
S3SI
267s
586. .
5860
64"
1140
«99"
1495
4799
1399
5381
5380
5867
»933
64*7
1071
6997
'749
4SQI
Soo
5J87
»69J
5869
5868
6449
i6ia
7001
1 7 JO
48.3
801
S393
539»
5879
*939
645'
aijo
7013
3So6
48,7
4S16
5399
.699
588.
1940
6469
9*4
7019
70>8
4331
8=5
54°7
"801
5897
5S96
6473
647*
70*7
""71
4S61
971
54" 3
1706
5903
5901
6481
a70
7039
39'
487.
»43S
5417
54' 6
59*3
196.
649.
.198
7043
5°3
4877
ijig
54' 9
5418
S9»7
59-6
6ii.
8" 5
7057
7056
4889
1444
5431
1715
5939
5938
6S.9
1088
7069
7068
4903
.6,4
5437
'359
5953
.984
6547
1091
7079
3539
4909
.63*
5441
1710
598'
5980
655'
3*75
7103
710a
49 '9
^59
5443
907
5987
1993
6553
655*
7109
7108
493"
4935
5449
*7H
6007
8si
S'5'
»S,
7iai
3j6o
4933
1466
547'
S47
6011
5oio
6569
164,
7117
1018
4937
4916
5477
.3S9
(019
6018
6S7"
6S7°
7119
594
4943
4941
5479
»739
6037
3o.g
6577
119*
7"5"
*7S
495'
147s
5483
»74l
604J
fiS8>
1316
7"59
h;i
4957
4'3
55°'
5500
6047
I046
6599
3-99
7' 77
4967
4966
5503
550*
6053
10.6
6507
7187
3593
4969
SiS
5507
»753
60I7
3033
66.9
66.8
7' 93
719*
4973
m6
55'9
J7S9
6073
6071
ii"
474
7*07
7106
4987
J493
55»'
345
6079
1013
6653
13*6
lOJO
4993
■ 66+
55»7
55-6
6^89
76.
tip
6658
7"3
;si
4999
357
SS3>
553°
6091
ao]o
6661
6660
7*'9
5003
»ioi
SiS7
'^.6
6101
6673
667*
7**9
,..1
5009
6x6
5563
.7*"
6.13
6iti
6679
3339
7*37
40»
5011
.670
5569
1391
6iit
3=60
668?
.67*
7143
,6.1
5011
5010
5573
.786
6131
6.30
6691
6690
7*47
7246
JO13
1674
SS8.
5580
6.33
'533
6701
6700
7*51
" 7*
5039
»S'9
S59'
1795
6,41
6.4»
6703
6701
7*8j
,(,■
5051
50
5613
56"
6,5.
1015
6709
6708
7*97
.43"
5«S9
5058
5639
1819
6.6,
79
67.9
3359
7307
!i!|
S°77
.53S
564'
470
6171
1086
6731
3j66
7309
,!ol
So8i
1170
5647
tS8*
6197
3098
6717
6736
73*1
,6(0
S»87
S086
565.
5*5"
9 '99
J099
676.
1690
733"
,jM
S099
S098
5653
aii6
441
6763
161
7133
611
5101
1700
5*57
S6S6
6110
6779
677S
7349
7V
5107
»S53
5659
5658
6it7
6116
67S1
1356
7^s'
\ ^^^^ \
S"J
1704
5«9
6^8
tk.a.
6110
67,1
V Ti*"^
X^-cX
S"9
»53
S«3
1841
6»9
«76
679^
\t!.11
V2
l:.
eft
7576
7S8.
JT9S
1187
76o«
7639
7*49
7669
j67»
76I6
7«jo
769I
T-S9
li-i
-t.
■!!»
7-SS
779*
-;■■
7l.(
»»3
4^1
8-0-
!i47
4071
iT'%
Ii6>
Sr-5
8167
j;ii
S-3.
!i7l
lijo
«r37
8179
It78
*^+'
1.9?
«J«S
i"+7
<>09
4'<H
^753
S119
tilt
876.
Siii
«74o
^'-9
s 5i
j:;;
Sgo,
S' 7
4"!
S807
s=4i
4111
Jg.^
fa6l
■iSs
SSii
Sif9
■t6t
■8]l
'=?)
■l7>
»37
6=*-
tiS6
>Sl9
g!JI
U90
■8^1
*9i
107 J
■86i
£157
■19I
<86]
I
4'J5
M67
S 7
461
■887
8 3^
1041
»93
*;r.
»35»
•9"
>:>'■
4iti
«9»9
S;*.9
4i«4
t913
1,76
8941
414*
8Gb!
■Sot
■StS
I810
44"5
44K
4419
,;s Ki: n:!
9JII
4is;
«>9
4ejs
M»J
466.
93 37
Jill
9341
9340
9343
934;
9349
ju6
937'
93T"
9377
,|7«
1874.] Reciprocal ofewry Prune Number hehtw 20,000. 307
Table 111. (contintted).
1014 J
S69
10847
10846
11447
.1446
.1049
6014
11613
6306
10147
■0146
loSs)
5416
1.467
5733
11071
355
,16,9
4106
io»S3
1561
10859
10858
11471
5735
I1073
11071
,16] 7
3'S9
10159
10158
10861
10860
11483
574'
11697
4031
,164,
3.60
S>3J
10867
1811
11489
1871
11647
■ 1646
10171
79
10S83
S44'
11491
766
11,07
'foS3
11653
6316
1017]
10171
.088,
1711
"497
1,496
11109
4036
11659
.1658
10189
S144
10S9.
11503
1,501
111,3
.167.
■8.
lOJOI
10300
10903
10901
,15.9
5759
11119
6059
.1689
793
lOJOJ
34)4-
10909
11517
3841
i»'43
11141
.1697
.1696
10J.3
iOJll
10937
10936
11549
1.548
■ 1149
11.48
11703
4134
10311
.580
10939
10938
1155,
.915
11157
1016
ii;,3
11711
10351
1066
10949
10948
"579
.1578
,116.
60S0
lOJJJ
S.66
10957
J7)9
1.587
1931
,1.63
60S.
.1739
4146
■0357
10336
IC973
1743
"593
11591
,1.97
3049
11741
.1741
'0343
I034»
10979
10978
"597
5798
11103
6101
■1757
1116
"a3S7
S'78
10,87
S493
11617
1.6,6
4070
.1763
709
.0369
»S9i
10993
10991
11611
11610
6113
.1781
117S0
10391
S'9S
IIOOJ
SSOi
"<)3
.1631
,1139
6.19
11791
639s
10J99
'733
SS'3
.16,7
1,656
,114.
6.10
11799
"33
10417
5113
11047
■ 1046
'.677
583«
.1151
.1150
"si?
6404
10419
94«
11057
"056
11681
5840
"»S3
3063
11810
"HI)
I04J1
11059
11058
,1689
4B7
11163
.1161
\\t\\
.1811
1045J
5116
.1069
11068
.1699
,1698
.1169
.1168
118x9
4176
I04S7
10456
6.5
,1177
6°'o
.1841
6410
10459
I04S8
1 1083
■I47
11717
1919
mil
11853
459
10463
IO+61
11087
481
11719
i*59
.1189
384
11889
3111
10477
.746
11093
1773
1,731
11730
11301
H60
,1893
3113
10437
104I6
11113
3704
11743
"74*
11313
6161
.1899
,1898
10499
10498
I1I17
1779
11777
'■776
1.J19
3081
11907
645)
10501
3500
5!S9
«i779
39»6
"343
4114
1191.
64s S
10513
lOJIl
11130
117!)
..781
i»347
6173
119.7
6458
10519
iW
I1I49
li.+S
"7i9
117K8
"373
6.86
119.9
1,53
10531
10530
'"59
5579
11801
1950
11377
.1376
11913
646.
10559
5179
11161
JIO
11807
11806
11379
11378
11941
.1940
10567
10566
11.71
.1S.3
59o«
,139,
6195
11953
,1951
105S9
lojIS
11175
"sitl
1,811
il8to
1140
.1959
6479
'=597
5198
11177
11176
11817
5913
11409
6104
11967
41"
10601
1060
11197
1799
1183'
.69
11413
6106
11973
1,61
10607
10606
nil)
1803
1.833
.,831
11411
11410
.1979
11978
106,3
75»
111J9
56,9
11839
5919
11433
4144
11983
I19K1
.0617
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5611
.1863
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61,8
1300.
161s
1063.
53'S
11151
1150
,,867
5933
11451
.1450
13003
650.
ic6j9
5319
I11S7
1,156
11887
1.886
.1457
,1456
13007
.,co6
loSs.
10650
iii6i
1151
■ 1897
1,896
11473
.1471
,3009
116S
10657
10656
11173
U171
11903
11901
1H79
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.303)
43*4
10663
10661
11179
5639
1 1 909
.,908
11487
11486
"30)7
65,8
10667
53)3
111S7
1,186
11913
5961
11491
I1490
13043
651,
10687
106S6
11199
11198
11917
11916
11497
.1496
13049
,'061
10691
10690
n]ii
377
"933
5966
11503
11501
13063
10709
10708
ii3'7
941
11939
,.938
11511
1085
13093
10711
595
11311
I in
"94'
,1940
"49
13099
13098
10713
5)6'
11319
1888
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13101
10715
596
11351
5675
11959
5979
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1683
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11969
351
11541
4180
1311,
6560
10739
.0738
113«9
811
11971
,.970
.1547
6173
.3,17
13116
107!)
3584
1138J
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.1981
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'»SS3
11551
1)147
939
10771
"193
11391
1.987
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,1569
6184
.3151
'3'5
10781
10780
11399
5699
.1007
4001
.1577
11576
I3'59
1193
10789
10788
11411
1181
11583
.1581
,)iij
6581
10799
5399
11413
"ti
11037
3009
,1589
11588
mil
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54>5
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11041
6010
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1907
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139C2
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13907
409
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13931
13930
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13963
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13380
13967
13966
6698
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957
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13410
14009
3501
447a
14011
14010
13420
14019
14018
6720
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14031
13450
14051
1810
13456
14057
14056
13461
14071
7035
13468
14081
1760
6738
14083
7041
13486
14087
14086
13498
14107
1351
4504
14143
14141
6761
HH9
5*4
13536
H»53
14151
1936
H«59
7079
. 45"
H»73
3543
13576
14177
14176
1359
'4«97
H
3399
14207
14106
6806
1 411 1
1844
1238
14H3
7111
6813
14149
7«»4
4544
14151
14150
853
1418 1
I190
13668
14193
1191
6839
14303
14301
3420
14311
3580
4561
H3a3
1013
13690
14317
14316
45S7
4561
4563
4593
4621
4617
4619
4633
4639
4653
4657
4669
4683
4699
47«3
47»7
47*3
473 »
4737
474»
4747
4753
4759
4767
477 »
4779
4783
4797
4813
4811
4817
4831
4843
4851
4867
4869
4879
4887
242O
7280
8c9
7-95
14592
14620
73i3
14618
14631
7319
3663
14656
14668
4447
14698
1471*
7358
7361
14730
14736
14740
7373
1475*
7379
14766
1110
14778
1478a
3^9
7406
4940
1471
1483
74*1
990
7433
495^
7439
1^886
15139
15138
15727
I5U9
15148
I573I
I S161
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M733
i5'73
75S6
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15187
7593
15739
15193
15191
'5749
15199
7599
15761
15117
15116
15767
I5"7
7613
15773
15133
15131
15787
15141
3810
'579*
15259
15158
'5797
15263
15161
15803
15169
1388
15809
15171
7635
15817
»5*77
3819
158*3
15187
15186
15859
15189
1174
15877
15199
15198
15881
15307
7653
15887
«53«3
51C4
15889
«53i9
7659
15901
15319
7664
15907
'533»
5110
15913
«5349
15348
15919
>5359
7679
15913
15361
156
15937
»5373
1281
15959
»5377
15376
15971
^5383
15381
15973
'539'
7695
15991
15401
175
16001
»54»3
7706
16007
'54*7
77«3
16033
»5439
7719
16057
»5443
7721
16061
I545»
5150
16063
15461
15460
16067
ieA67
'rn^t
■ Art Art
1
I
I
1
1
1874.] Reciprocal of every Prime Number behw 20,000.
Table III. {amtimted).
6417
; 1*4)3
I 16447
16649
16653
■670J
16719
'674'
16747
167S9
1676J
167S7
16S4] 401
■"-- 1*05
1768
7'4
I7»6i
"35
17I90
1790*
179°S
"9*5
.1 8961^
13 896.
•" 8964
1793!
.... 8978
I79S9 8979
"797" 17970
"7977 856
1 7981 179*°
17987 899J
17989 599*
1E013 900G
1804"
jlo4j
18047
"8049
18059
18077 4S"9
J 8089 9044
.5?S
18719
'90)7
1J7J'
"8743
1B749
18757
.8771
1B787
18795
18797
1IB03
18819
i8Bs9
[SKti9
1SS99
189M ,,.
[89" 3 iS9l
.S9>7 -■
■ 8919
1S947
[B97J isi
■8979 18978
19001 137s
19009 47S»
I 90 I] 475)
9S'S
9518
■v'j- 6350
19069 6356
1907J 19071
19079 95J9
,9081 79r
19087 636:
I9"i" 9S6(.
19139 19138
19140
4789
95S1
6394
3S41
19118
"9*37 *8o9
19149 jiol
■9»S9 >9iS»
19167 9633
IQITI 1917*
4811
19JDI 3860
19309 19108
[9319 9*S9
'9333 4833
'9373 '*•-
19379
19381
19387
+843
1917!
1191
3S
9701
19416
'Vi»\
I 94" 7
324b
19b-, 3
32f)7
»9"S9
9^-9
I 98X9
994
194S3
9741
196 u;
9S04
19763
98*1
1 9 S 9 1
603
194X9
406
1 966 1
19600
February 26, 1874.
JOSEPH DALTON HOOKER, C.B., President,
The following Papers were read : —
I. " The Winds of Northern India, in relation to tl
and Vapour-constituent of the Atmosphere/'
Blanfobd, F.G.S., Meteorological Reporter to tl
of Bengal. Comnoiunicated by Major-General S
Received May 25, 1873.
(Abstract.)
The object of this paper is to describe the normal v
Northern India, and their annual variation, and to trace
and causes, so far as these can be discovered in the
changes of the atmosphere. After referring to the dal
conclusions are based, the author goes on to describe t
principal geographical regions of North India in di*tail.
Pabt I. Description of Winds,
1. The Punjab, — Asa rule currents from the westward
1874.] fVinds of Northern India. 21 1
and southerly, south-westerly, and north-westerly winds predominate —
the two former in the rainy months, the last in the cold and hot dry
season. In the coldest months the wind veers towards the north, and
occasionally passes a little to the east of north.
2. The Gattgetic Plain, — ^The great chain of the Himalaya, which skirts
the northern edge of this region, the elevation of which is between 150
feet above sea-level on the east and 900 feet on the west, determines in a
great measure the direction of its prevailing winds ; and those from the
north-west and south-east much exceed those from other quarters. In
the western part of the plain the north-westerly winds somewhat exceed
the easterly. In the eastern part the converse holds good. The change
from the westerly to the easterly direction accompanies the change from
the hot and dry season to the rains, and from easterly to westerly that
from the rains to the cold season. In the districts more remote from the
mountains the tendency to a westerly direction increases, and occasional
south-west winds blow, apparently caused by incursions from the Arabian
Sea. During the hot months, and during the day, the westerly winds
blow with great force, falling at night ; calms are a characteristic of the
nights, and prevail most in the colder months. As the hot season advances
the easterly winds become more frequent, and attain their maximum in
July, when the rain becomes general. The winds veer from the west
through the north to east and south-east, the opposite change being more
abrupt, and at one place of observation apparently retrograde.
3. Plateau of Majpootana. — ^This region is somewhat elevated above the
Gangetic plain, varying from 800 or 900 feet to 1800 feet above the sea-
level. Winds from the west and south-west greatly exceed those from
other quarters in the southern districts, commencing as early as February
and continuing till November, when they are replaced by northerly and
north-easterly winds. The north-east winds are comparatively weak and
unsteady, and interrupted by calms. A similarity to the winds of the
JSouthem Punjab may be observed. The northern part of the plateau of
Eajpootana partakes more of the character of the Gangetic plain in its
winds, the winds of the hot season being chiefly westerly and north-
westerly ; but the rainy season is accompanied by south-westerly winds,
and not by easterly winds as in the Gungetic plain ; and easterly winds
are always rare.
4. Central India, — This region is on an average somewhat less elevated
than that last referred to ; it is traversed by the high land known as the
8atpoora range, and is otherwise considerably broken up into valley and
mountain, so that the winds are more influenced by merely local con-
ditions than in the less hilly regions before noticed. Westerly winds on
the whole prevail. In the hot months westerly and north-westerly
winds predominate. Local inroads of south-westerly winds occur during
the rainy months on the north of the Satpoora range, and less strongly
on the south of the range ; as the rainy season ceases the winds veer
212 Mr. II. F. Blaiifoi-d on the [Feb. 26,'
through weat to north imd north-enst, which diroelioii is dominant nftor
Kovumbyr tiJl January, when the northerly tendency faiJa and southerly
winds blow, which again pass into the westerly winds oE the hot months.
This region partifiputea in the chttracttri sties both of the pliuns of
Northern India and of the Puniusulft, whii-h laet is under the influencu
of llio true aoiith-Most and north-east monsoons. During the cold
months and the rainy season respeclively, when the two great moneoons
ar« at their height, the winds of the Central India plateau are from the
north-east and south-west, \yhiJe those of the Gaugetic plain are Etohj
the north-west and Bouth-fnst, the former blowing to or from the Arabian
or Western Sea, the latter to or from the Bay of Bengnl, or Eastern l^ea.
Only in the hot season do the winds approximate, bio\ving from the dry
region to the north-west towiH^ls the thermal focus of Ceiitral India and
Western Bengal.
6. irMieoi Beni/nl. — This regioa includes the continuation of tho
plateau of Central India to the margin of the delta of the Gnngea, and
descends to the Bay of Bengal. The northern part, b«ug a compam-
tively open tableland, participates greatly as to its winds in the chanwrtfrs
of the ni.'ighhoiiriiig fJangelie jdain. The west and north-west winds of
the cold months are followed by south-west and south winds, which draw
round to south-east during the rainy season, again reverting to north-
west through west. Occasional incursions of the south-west monsoon
are felt, wliich are perceptible in the Gangetic valley. On the coast the
winds are very different. The west and north-west winds of the interior
are quite subordinate. North and north-east winds begin in October,
when the south-west monsoon ceases, becoming more northerly with the
increasing cold and the strengthening of the land-winds of the interior.
Later they again veer towards the east ; and the sea-winds blow from
Eoutb-east in January, and ultimately from the south-west. After Sep-
tember the winds fall back rapidly through south-east and east to north-
east. At places removed from the coast the wind is more westerly than
ou the coast.
6. Oantfetie Delta. — From its position this region is swept by the
currents of air passing between the Gangetic plain and the equatorial
ocean. The general course of the winds is as follows : — The winter
monsoou becomes well estabhshed in November, blowing nearly from the
north on the east of the Delta, and from north-west on the west ; near
the sea the direction is a little east of north. As the season advances
the wind draws round towards the west, where it is about February, and
eventually backs by south-west to south and south-east, in which direc-
tion it blows during the rainy season and till September. In October
tiie winds are chiefly easterly, but unsteady and apt to be stormy, alter-
tatiDg with calms In the earlier part of the month, and passing into
and north-west in the latter part.
iwMiii. — The local configuration of this valley no doubt affects its
187:1.] mnda of Northern India. 313
u'iuds, forming, as it does, an open pasBOge for the monBOons to pass to
and (rom the region north of the H^nalaya. The vinter monsoon be^s
in October, when north and north-eaat winds blow with great steadiness
till January, after which westerly winds are felt, chiefly blowing from
the Bouth-west, till in June they predominate and continue till Septem-
ber, when they in turn give way to the easterly winds. On the whole
the characteristic of Assam is the prevalence of easterly winds, which is
here aa conspicuous as that of the westerly winds over the Gangetic
plain and Punjab.
8. Araican Coast. — The observations in this region are limited to
places on the coast. The northerly winds begin in October, with 000-
sioual north-west wind, continue till March, or a month later than in the
Gangetic delta, after which they work round to the southward, and at
length to south-east by south, which is the normal mean direction of the
wind along this coast during the south-west monsoon. This mean
direction is varied at all times of the year by the land and sea breezes.
The changes of the monsoons occur sensibly later on the southern parts
of the coast than on the northern ; also the southerly winds attun less
easting, and the northerly winds less westing, in the south than in the
north. In August a sudden drawing of the wind towards the west is
observable on this const (and is also discernible in Bengal and the North-
west Provinces of India), followed by a return to the eastward, due
apparently to the influence of the true south-went monsoon of the
Arabian Sea, then at its height.
Smnmary. — From the foregoing it will be seen that the winds of
Northern India are very different from those of the adjacent seas. Id-
slcad of two monsoons from the north-east and south-west alternately
prevailing during about equal periods of the year, we find rather three
distinct seasons in which special winds prevail, the directions of which
mainly depend on the directions and relative positions of the mountain-
ranges and plains.
During the cold-weather months, November to January, light westerly
and northerly winds blow from the plains of Upper India down the
valleys oE the Ganges and Indus, and across the tableland of Central
India, and join into the north-east monsoon of the Peninsula. The
e.istcrly winds of the valley of Assam add to this current.
In April and May, as the hot weather comes on, the ninds of Northern
India become mure westerly and powerful, and take the form of the hot
winds, which are not continuous hut diurnal, blowing till sun-down and
then followed by calms, and prevailing to the eastern limits of the
Gangetic delta. At the same time southerly winds are commencing on
the coast, and are felt from Sindh across to Bengal, but only at intervals,
and feebly except near the sea.
In June the south-west monsoon, being established in the equatorial
.ocean, sets in round both coasts of the peninsula, penetrates up the
214 Mr. H. F. Blanford on the [Feb. 20,
vallej-B of the Indus, tho Xerbuddn, aud Taptee, carrying a west or
Bouth-weat piirrent over CVut-rnl India, and from the Bay of Bengal
pouring lip the fiumel-Bhapetl opening occupied by the Gangetic delta,
whence turning westward it passes np the Gangetic yalley towards the
Punjab, which sijetna to be the limit of the south-easterly winds, in
Afghanistan the dominant winds being westerly even during the summer
montha. This is the period of the rainy season of Norlbern Lidia.
In October, as the south-west mou-soon ceases, the southerly current is
reoun-ed towards the heated region along the Coromandel coast (on
which the rainfall ia till this season of the year comparatively small), and,
blowing as a south-east M-ind, causes the autiimn rains on that coast,
which some «Tit*rs have erroneously attributed to the north-east mon-
soon. With the gradual cessation of the southerly winds the westerly
tfinda of Korthem India again begin, and the cycle of the year is thus
completed.
Fakt II. lUlation of Wind* to other EUnuntt of Climate.
1. Tttnperatare. — The seasons of Norihoni Lidia present three distinct
phases: — the mW.<r«Mti, from the end of the rains in September to February
or Mnri'h : flic hit sfafnu, ch.'irarli'rizpd bv a drv iituiosphere and great
diurnal range of temperature ; and the rainy season, in which the tem-
perature is moderately high and equable, and the air vety humid. At
the close of the rains (the end of September) the temperature of Northern
India from the Punjab to the sea is nearly uniform at about 81° or 82°.
But evaporation and radiation to a cloudless sky soon reduce the tem-
perature of the interior below that of the maritime r^ona ; and in
January the Punjab is about 11° colder than Bengal, the plains of the
North-west Provinces being about midway in temperature between the
two. In March the advance of temperature in Centra) India has brought
out two thermal foci — one on the west in Bajpootona, and the other on
the east in the hilly tracts of Western Bengal. In April the Central-
Indian thermal focus is well developed. The mean temperature of
Nagpore is 7° above that of Bombay, 13° above the northern Punjab,
and 6° above tbe coast of the Gangetic delta. The hottest region has a
mean temperature between 85° and 90°, the Upper-Punjab and Upper-
Assam being from 75° to "7°. In May the thermal focus has gone
further to the north-west, and lies in the northern part of the Hajpootana
plateau. In June it has reacbed tbe Punjab, the temperature of which
continues to increase, rising to OS" and more ; while that of tbe south of
India begins to fall, consequent on the rains, which commence about the
middle of the month. In July the Punjab ranges above 90°, whUe the
greater part of Central India is below 85°. After July the temperature
again foils, so that by the end of September it is nearly equalized all over
, Northern India.
k To sum up briefly. In the cold veather there are two foci of mini-
1874.] fVin4» of Northern Trtdia. S15
miun temperature, the one in the Fonjab and the other in Assun, Knd,
with Bome exceptions, the ieothermalB nesrl^r conform to the pinllels of
latitude. In the hot months a focus of heat is formed in Central India,
round which the isotherms are bent, the temperature on the coasts and
in the northern plains being considerably lower than that of the interior.
I'^ntly, during the rainy season the seat of highest temperature is in the
Punjab, the coolest regions then being those of the maximum rninfall,
and consisting of two tracts extending from the coasts of Bombay and
Bengal, along the course of the monsoon currents.
The author then refers to the distribution of temperature in a Tertieal
direction, as ascertained from obaervations made at the monntaio-stations.
He points out apparent anomalies in the differences of temperature due
to difference of altitude in the mountains of North-western India and
thoae bordering on Bengal, and auggestfl, as a probable explanation, the
variation of hygrometrical condition of the air in the two r^ons,
remarking that the continual upward diffusion and condensation of water
Tapour must tend to equalise the upper and lower temperatures, and that
this tendency will be the greater as the approach to saturation is clowr.
The subject, however, is admitted to be one that requires further exami-
nation, and particularly with respect to the operation of nocturnal radia-
tion and diurnal absorption of heat — the remark being also made that the
avfulable observations give the local temperature near the surface of the
mountains, and do not properly represent the condition of the free
atmosphere at corresponding elevations.
2. Vajxnir-tefuion, Humidity, and SaitifaU. — In the r^ons under
dianission, the lowest vopour-tenaion occurs almost everywhere in
January, when the temperature is lowest. The lowest mean tension tor
any month is about 0'2 inch, observed in the Southern Punjab, the c(nT&-
sponding minimum in Bengal being about 0-5 inch. The increase of
tension begins early in the districts near the sea, and continueB regularly
and rapidly till the setting in of the rains ; but in the drier regions of
the interior, where the west winds prevail throughout the spring and
hot-weather months, the rise of tension is slow, probably not more than
ia due to the actual rise of temperature acting on the local vapour supply.
The increase at the commencement of the rains, in June or July, when
the southerly winds begin to be felt, is very marked and sudden ; and
equally so ia the fall after September, when the southerly is replaced by
the northerly current.
As regards variation of tension due to elevation, the conclusions of
former obBer\'erB are confirmed, that the ratio of decrement foUovs
g(^nerally the increase of elevation, but with a marked addition to the
rulative tensions at the higher stations in the hottest and wettest months.
Passing to the humidity of the air, it is shown that the period of greatest
dryness falls later in the year the greater the distance from the sea,
measuring along the course of lain-csrrying wind-cnrrent. On the eoMt
i
216 Mr. ](. F. Blauford on the [Fdi. SG,
of Bt'iigat thp lirieat month is Jftuuary, the pei'iod being Iat«r as we go
iiilanil lip the finngetic vfJIey, till it is fountl in Mny or Juno in llie
Piiiijub mill North-west I'rovinees.
In the western part oE the Gtuigstic Talley and the Punjab there is a
Bdcondary minimum of dryness, which follows a converse rule to that of
the principal minimum ; that ia, it falla earlier the f/retita- the ilistnnee
from the (tea in the sense before explained. In the Punjab this minimum
ia as early as September or October, shortly after the cessation of the
rains, gradually advancing till November at Benares, east of which it ia
not appreciable. Intermediate between the two minimum periods is n
Becoudary or winter maximum, evidently related to the n'inter rains of
the Upper Provinces, and, like the corresponding winter maximum and
rains of Europe, traceable to the descent of the equatorial (here the anti-
monsoon) current, and the low winter temperature.
The relative humidity of the air remains pretty constant at all eleva-
tions ou the Himalaya, as already pointed out by Dr. Hooker and other
writers, but not including Tibet, the conditions of which are very
dftEerent. There are, however, considerable exceptions to the general
rule ; and the local law of lariation depends much on local conditions.
The rainfall is next discussed. The author points out that there are
three principal seasons of run calling for notice. The summer and early
autumn rains (that is, those of the Bouth-west monsoon, or of the raimj
teaton commonly eo called) are the most important. In Bengal they
bc^in on an average about the middle of June, with a fall of from 9 to 15
incbes in that month. In the Upper Provinces they are later, and in
Bajpootaoa there is little rmn till July. Everywhere they have their
maximum in July. In the Upper Prorinces and Bajpootana verj' little
nun falls in October, and the nwns may be said to end in the lost week
of September. In Bengal and Central India the fall is still considerable
in October; and the rMUS there end about the middle of this last-uameil
month.
The spring rains prevail in the region over which the sea winds blow
from the Bay of Bengal early in the year. In Assam and £^teni
Bengal showers are frequent in March, and in April the fall is copious,
amounting, in those districts to windward of the eastern mouritains, to V2
or 14 inches in the latter mouth. In Western Bengal the fall is less,
and takes place with occasional thunder-storms, locally known as north-
v'titers, which extend as far inland as Xagpoor and Benares.
Thewinter rains are received most regularly and copiously in the Punjab
and Upper Provinces, Assam, and Cachar. In Bengal and the lo«er
part of the Gnngetic valley they are less regular and lighter. They begin
at the end of December, continuing till March in the North-west Pro-
Tincjs, and till April in the Punjab. The fall in these districts amounts
to about 'Lor 3 inches during the whole season. The author considers
that) fi4 they do not coincide either nith the period of greatest cold or
1874.] mndi of Northern India. 217
greatest humidity, these mns must he due to some other cftuse, which he
thinka to be the humidity of the snti-mouBoon current.
On the mountains the heaviest rainfall is on the lower and outer
slopes. The gTeat«st recorded falls are those at Cherra-Poonji over
Eastern Bengal, averaging more than 500 inches in the year. On the
Himalaya the records show falls of from 280 inches on the east to 70 or 80
inches in the North-west Provinces, and 40 to 50 inches in the Punjab.
Local circumstances of position greatly affect the quantity.
Generally the quantity of rainfall diminishes with increase of distance
from the coast ; but it increases on approaching a hill-range on the wind'
ward side when the rise Is steep, while to leeward a decrease takes place,
followed eventually by another gradual increase.
3. Atmospherie Pressure. — The available data for discussing this part of
the subject are imperfect ; and particularly the means of reducing the
pressures to the sea-!evel are not forthcoming in many cases. The fol-
lowing remarks are made subject to this ezplonatioii.
The mean pressure, reduced to sea'lerel, in the month of October is
nearly uniform over Bengal, on both sides of the bay, in the Central
Provinces, and the Gangetic valley, with a slight tendency to a higher
pressure in the North-west Provinces and Cuttack on the one side, and
on the Arakan coast on the other, which finds its expression in the
slightly converging winds of that season.
In the following months the pressure rises over the whole area, but most
in the North-west Provinces and Western Bengal ; and in December an
axis of maximum pressure lies on a line drawn from Cuttack to the
North-west Provinces in a north-west and south-east direction. The
distribution of pressure remiuns much the same till the end of February.
In March a rapid fall takes place in Korthem India ; but the line of
higher pressure still remains, extending now from North-western India
across to the coast of Arakan round the delta of the Ganges. This,
doubtless, is the immediate cause of the back to back winds described in
Parti.
In April, with a continued rapid fall, a trough of low pressure becomes
apparent, which extends from the head of the delta of the Ganges into
Central India. In May this area of low pressure is somewhat displaced
towards the north, occupying a line from Western Bengal to Nagpoor,
along the 34th parallel of latitude. In June the conditions are generally
similar, but with much reduced pressure in the Punjab, in the north-west
of which province the absolute minimum is probably to be found. The
mean difference of pressure in June between Port Blair in the Bay of
Bengal and the upper part of the North-west Provinces is not less than
■j^ of an inch, and between Port Blair and Calcutta -j^ of an inch, Cal-
cutta being about as far from Fort Blair as from the head of the Gangetio
valley, 800 miles ; the baric gradient over the Bay of Bengal, therefore, is
about double what it is over the axis of the Ganges valley, and amounts
218 On the Hinds of Northern India. [Feb. 26,
to -jlj of an inch for 400 miles over the land, and ^ of an inch over the
sea, which BufHccs to maiot^ the steady current of the Boutb-west
monsooa.
In July the minimum of preasoro is reached without important relative
diange. la August a rise begins, greater over Northern India, which
continues during Septi^mber and October, when the uniformity of
pressure is once more approximately restored.
It is apparent that thd distribuKou of preasiu^ follows, within certain
limits, that of temperature, in an inverse ratio of intensity. Thus the
region of high pressure in the cold months, which Ues across Northern
India from Boorkee to Cultach, coincides approximately with the area over
which the isothenaala, then approximately parallel to the circles of latitude,
are bent downwards, or the temperature of which ie lowest relatively to
the areas to the e-ost and west of it. Again, during the hot half of the
year, aa the isothermal lines advance, first turning their branches south-
wards and leaving an area of higher temperature in Central India between
them, which eventually is inverted towards the west over the Punjab, Bo
a pomewhat corresponding change occurs in the lines of equal pressure,
which at this sPASon may bo said ta be distributed on lines generally
following tlii> ui'TiiliiLiis, but with a loop more or Ipss deeply coucavo
towards the west.
The author then discusses at some length the manner in which these
changes of pressure arise, and to what extent they are dependent on the
changes in the proportion of aqueous vapour in the air, and concludes
that the vapour indirectly greatly influences the pressure by carrying
heat from the lower to the upper strata, and by arresting solar and ter-
restrial radiation, thus equalizing the temperature of the air-column, but
that its power of changing the density, by reason of the displacement of
the heavier air-particles, b relatively small, and in some cases unimportant.
In general terms the changes of temperature are the principal causes of
the variations of pressure.
4. Certain EffeeU of Wind*. — Inquiry is made whether any dynamic
heating or cooling of the air can be traced by reason of winds descending
to a lower or rising to a higher level, with the conclusion that no such
effects are discernible, and that certain explanations given of the winds
of India (by other writers), baaed on such a conception, are erroneous.
Evidence is adduced which is held to estabUsh that anti-nwnsooii. cur-
rents blow in the upper strata of the atmosphere, at the various seasons
of the year, and at varying elevations, causing corresponding modifica-
tions in the general temperature, the operation of all winds being to dis-
tribute the temperature peculiar to them. To the descent of the anli-
montoon current from the south, the author is disposed to attribute the
runs of the cold weather.
Attention is also directed to the greater velocity of the wind-<;urrenta
near the sea, the westerly winds increasing in force as they approach
1874.] Oa Dltplaeemmt of the Solar Spectrum. 319
Bengal, and the south-easterly winds diminishing in force as they reach
the North-west Provinces, indicating that descending and ascending cur-
rents must be formed in the upper strata, though of the return south-
ward of any descending current from the north there is no direct
evidence.
II. " Note on Displacement of the Solar Spectrum." By J.
H. N. Hbnnkssby, F.R.A.S. Communicated by Profeaaor
G. G. Stokbs, Sec. B.S. Keceived December 15, 1873.
The following experiments were made with the (new) spectroscope
(three prisou) of the Boyal Society to ascertain for this instrument the
amount of displacement in the solar spectrum from change of tempera-
tore. The spectroscope was set up on a pillar within a small tent at a
time of the year when the thermal range is considerable : the collimator
was placed horizontal, and directed through a window in the tent to a
heliostat, which was made to reflect the sun's image when required. On
closing the window darkness prevailed in the tent, so that the bright
sodium lines were easily d>tained from a spirit-lamp. Before commencing,
the slit was adjusted and the spectroscope clamped ; and no movement of
any kind was permitted in the instrument during the experiments. The
displacement was measured by means of a micrometer in the eye-end of
the telescope, reading being taken (out of curiosity) successivaly to both
dark and bright lines, >. «. to K 1002-8=0^ and K 1006-8=D^ A
verified thermometer was suspended directly over and almost touching
the prisms. The meteorological observatory referred to was some fifty
yards north of the tent.
Bejecting observation 6 (in the following Table) because the tlwrmo-
meter was evidently in advance of the prisms, we deduce
By Dark lines, displacement equal
Dr to Ds is produced by 31 'S change of temperature.
By Bright lines, displacement equal
Dr to Du is produced by 29'4 „
Mean 30
from which it appears that the displacement in question may not be
neglected in investigations made under a considerable thermal range.
Mr, J. H. N. Ilenncasey art
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1874.] WUle Linet in the Solar Speeimm. 231
III. "On White Linea in the Solar Spectrum." By J. H. N.
Hennbsset, F.R.A.S. Commuaicated by Professor Stokes,
Sec. R.S. Received December 8, 1873.
Extract from a Letter from Mr. Hennetteif to Profetior Slolcet.
"Muasoorie, No». 12. 1871
" Mr DEAB Sib, — As I camiot account for what is described and drawn
in enclosed, I hasten to place the same before you, intending to look for
the white linis in question so sooa as I move down to a lower altitude.
Amongst others, no doubt KirchhofE closely examined the region in queS'
tion, without notice of the lines ; and this only adds to my perplexity, un-
less what I see here is due (1) to altitude, or (2) is inatrumeutal. In
the latter case I cannot account for the absence of the white lines at
Sehra, where I eiamined the spectrum generally several times; I must,
however, odd that without close examination and some experience, the
lines might easily be passed over. But if instrumental, to what are they
due? I very much regret that the old spectroscope is not available at
present [it had beea temporarily sent elsewhere for a special objecf] to
enable me to verify the phenomena "
[In the drawing sent by Mr. Hennessey, the intervals between the
dark lines are coloured green, except in the place of the two white
lines. To transfer this distinction to a woodcut, an additional horizontal
band has been added below, in which only those parts of the drawing
which are left white appear as white, while in the upper part the white
of the woodcut represents the white or green, as the case may be, of the
original.— O. G. S.]
Part of Solar Speetram, drawa to Kirchhoff't scale, obeerved at Ifiueoorie,
JV^. W. Pivvineee, India, Lot. JV. 30° 28', Long. E. 78° 4' ; ffeu/ht
6700 feet above tea (aho^), v)ith the Sptetroteope hdoaging to tho
Bot/al Sodely.
Is ot" white floss silk held in the light. liie spectroscope lu
mo>t ('()nveiii(Mit; hii^hest'-power eyepiece, [)re>ents iiaai^es
thirds to seven ninths ot' those drawn in the diagnun ; the
:uggerated by reckoning to agree with KirehhoJI's millimetre
therefore be readily understood that the white lines do not
ing objects in the spectroscope, especially about the time of
I happened first to notice them ; they are best seen about
;heir resemblance to threads of white floss silk is very dose ;
1, the lines in question can always be readily detected. So
istrumental means permit, the wider line extends between
d K 1658*3 ; more accurately speaking, it &dls short of the
ther underlies the former ; the narrower white line is under-
0*3, sensibly more of the former appearing beyond the edge
)t of the latter, which presents the quaint look of a black
ite surface enclosed in a green band. These are the only
1 the spectrum from extreme red to F ; they are not bright
lines), so far as I have had opportunity to judge. Were they
the question wouldarise, why these alone should be reyersed
aboYe sea. Like the black lines the white lines grow dim
r with the slit opened wide. As seen here»K 1657*1 is sen-
than K 1667*4, whereas Klrchhoff assigns 5 6 to the former
to the latter.
ttph of the Moon, sent by the Bey. Dr. Bobinson, F Jt.S.,
the Great Melbourne Equatorial, was exhibited ; also a
- the Nebula in Argo^ made from eye-observations with the
lent.
1874.3
PreiaUi received, Febmary 5, 1B74.
Traniiactions.
Briiun : — Naturfonchender Yerein. YerbandlongeD. Band XI. 8to.
1873. . The Sodely.
CWcuttoi—AsiatioSoriety of Bengal. Journal, 1873. Ra*l,No.l,2;
Part 2, Nu. 1-3. Svo. ProceedingB, 1873. No. 2-8. 8to.
The Sodety.
Laueume : — Soci^t^ Yaudoiae des Sdences Xaturelles. Bulletin.
Yol. XII. No. 89, 70. 8vo. 1873. The Society.
London : — Mathematical Sodety. Proceedings. No. 54-63. 8to.
1872-73. The Sodety.
Odontological Sodety. Transactiona. Vol. VI. No. 1, 2. 8vo. 1873.
The Society.
Pharmaceutical Sodety. Pharmaceutical Journal and Transoctiona.
Third Series. Yol. I., II., lY. (Part 37-42). 8vo. 1870-73.
The Society.
Quekett Microscopical Gub. Journal. No. 24, 25. Eighth S«port.
July 1873. 8vo. 1873-74. The Oub.
Melbourne : — Boyal Sodety of Victoria. Progress, Beport«, and
Final Beport of the Exploration Committee. foUo. 1872.
The Sodety.
Nencfaatel ; — Sod^t^ des Sdences Naturelles. Bulletin. Tome IX.
Cfthier 2. 8to. 1872. The Society.
Paris : — Ecole des Mines. Annales des Mines. LivTuson 1—4 de
1873. 8vo. The £cole.
Faculty dea Sdences. Theses par E. Branly, G. Le Monnier, E,
Jannettaz, E. Bichat, B. Benoit, A. Sabatier, Legouia, J. Chaiui.
No. 344-351. 8yo A 4to. 1872-73. The Faculty des Sdences.
Sod^ G^k^que de France. Bulletan. 2* S^rie. Tome XXIX.
ff. 42-49 ; 3» Serie. Tome I. No. 3. 8to. 1872-73.
The Society.
Warwick : — WarwickBhire Natural-History and Arclueological Sodety.
Thirty-seventh Annual Beport. April 1873. 8to. The Society.
Barboza du Bocage (J. V.) Notice sur I'Habitat et lea Caract^res dn
Macrosdncua Coctd. 8to. ZUbomie 1873. Ten Zoological Papers
extracted from the ' Jomal de Sdendas Mathematicas, Physicaa, e
Naturaea.' 8to. Litboa 1869-73. Five Papers extracted from the
' Proceedings of the Zoological Sodety.' 8vo. 1865-70.
The Author, by Prof. Huxley, Sec.E.S.
"rMn-aclions.
Albany: — Aiiiorican Tiistitut(\ Thirtieth Annual l\oport
l^(;i)-7(>. .^vo. Alhfun/ Ls70. Tl:
New- York State Agricultural Society. Transactions. ^
1871. 8vo. Albany 1873. ^1
Boston [U.S.] : — Boston Society of Natural History. Memo
Part 2. No. 2, 3. 4to. 1872-73. Proceedings. Vol. XI
426 ; Vol. XV. Part 1, 2. 8vo. 1872-73. 1
Buffalo : — Society of Natural Sciences. Bulletin. Vol.
8vo. 1873. G
Cambridge [U.S.] : — American Academy of Arts and Scie
moirs. New Series. Vol. IX. Part 2. 4to. 1873. I
pp. 409-604. 8vo. 1872-73. Th<
American Associfttion for the Advancement of Science.
ings. Twenty-first Meeting, held at Dubuque, Iowa, A
8vo. 1873. Thei
London : — Geological Society. Quarterly Journal. V
Part 3, 4; Vol. XXX. Part 1. 8vo. 1873-74. List .
8vo. 1873. 1
Madison, U.S. : — Wisconsin Academy of Science, Arts, a
Transactions, 1870-72. 8vo. 1872 (2 copies). The
New Haven : — Connecticut Academy of Arts and Science
actions. Vol. 11. Part 2. 8vo. 1873. The
New York: — American Geographical Society. Journal. Vo
New York 1873. T
Paris : — Soci^t^ de Biologic. Comptes Eendus des Seances et
4« SpriA- Tom A TTT TV ^J . K^ aA^^ rr t tt
1874.] Pretenta. 225
Beporbs.
Albany : — Annual Mesiagei of the Qovernor of the St&te of New York,
1871, 1872. 8vo. The Govemor.
SeTenteenth Annual Beport of the Superintendent of Public In-
BtructioQ of the State of New York. 8to. 1871.
The Department.
Twelfth Annual Seport of the Superintendent of the Insurance
Department, State of New York. 8to. J871.
The Department.
TTniYereity of the State of New York. Annual Beporte of the
Begents, 84, 85. 8to. 1871-72. Annual Beport* of the TruBteea
of the New-York State Library, 54, 55. 8to. 1872-73. Subject-
Index t» the Catalogue of the New-York State Library. 8yo. 1872.
Besulte of a Series of Meteorological ObaerrationB mode at sundry
Stations in the State of New York. Second Series. By F. B.
Hough. 4to. 1872. The Eegents of the UniTerdty.
Beport of a Topographical Survey of the Adirondack Wilderness of
New York, by V. Colrin. 8vo. 1873. The Author.
Baltimore : — Peabody Institute. Sixth Annual Beport of the ProToat
to the TruBteea. 8vo. 1873. The Institute.
Bosten, U.S. :— Board of Education. Tbirir-aixth Annual Beport.
8ro. 1873. The Boarf.
Board of State Charities of Massachusetts. Ninth Annual Beport.
8vo. 1873. The Board.
Massachusetts Board of Agriculture. Nineteenth and Twentieth
Annual Beports of the Secretary, 1871, 1872. 8vo. 1872-73.
The Board.
Cambridge, U.S. :— Harvard College. Catalogue, 1872-73. 8yo. 1873.
Forty-seventh Annual Beport of the President, 1871-72. 8vo.
and other Papers. The College.
London : — Meteorological Office. Daily Weather Beport, Jan. to
June 1873. folio. Quarterly Weather Beport. 1872, Part 4 ;
1873, Part 1. 4to. Notes on the Form of Cyclones in the
Southern Indian Ocean, by C. Meldmm. 8vo. 1873.
The Office.
New York : — Cooper Union. Annual Beport of the Curator. 8vo.
1873. Fourteenth Annual Beport of the Trustees. 8vo. 1873.
The Institution.
Washington : — Bureau of Navigation. American Ephemeris and
Nautical Almanac for the year 1876. 8vo. 1873. The Bureau.
Catalogue of Books added to the Library of Congress during the
year 1871. roy, 8vo. 1872. The Smithsonian Institution.
ii-^«'l> : — Acadriiiic Ixoyali- df I^('li;i([U('. BulK'tiii. \'J' an
:> lo. 12. Svo. r>r>fj;ll,s 1>7:5. The A
Ac:i(l<iiii«' Kovak' dr Mt'dcciin'. Mrmoires Couroniu's r
Memoires. Tome II. fasc. 1. 8vo. 1873. Bulletiu. J
Tome VU. No. 5-12. Svo. 1873. The J.
iblin : — Boyal Geological Society of Ireland. Journal. V<
Part 3. Svo. 1873. The
ndon: — British Pharmaceutical Conference. Year-Book
macj, with the Transactions at the Tenth Annual Meet
at Bradford, Sept. 1873. Svo. London 1873. The Co:
Odontological Society. Transactions. New Series. Vol. T
8vo. London 1873. The
Boyal Astronomical Society. Monthly Notices. Vol. 5
No. 8, 9 ; Vol. XXXIV. No. 1-3. 8vo. 1873-74. The
Bo3ral United-Senrioe Institution. Journal. Vol. XVLI.
73. Svo. 1873. The Ini
»me : — ^Accademia Pontificia de' Nuovi lincei. Atti. Tc
Anno 3 (1849-60). 4to. Boma 1873. The J
enna : — Osterreichische G^sellschaft fiir Meteorologie. Ze
redigirt von C. Jelinek und J. Hann. Band VIU. Ni
Band IX. Nr. 1, 3. roy. Svo. Wien 1873-74. The
sbrugghe (G. van der) Sur la tension superfidelle des .'
Second M^moire. 4to. BruxelUs 1873. The
1874.] Pretentt. 227
Fthruary 26, 1874.
TranaactionB.
Amsterdam : — Koninklijke Akademie van Wetenschappen. Yerhuide-
tiugen. Deel XIII. 4to. 1873. Veralageo en Mededeelingen.
Aideeliug Nataurkimde. Tweede Beeks. Deel VII. 8to. 1873.
Afd. Letterkunde. Twe«de Beeks. Deel III. 8to. 1673. Jaai<-
boek voor 1872. 8¥0. Proceasen-Verbaal, 1872-73. 8vo. Oaudia
Doiuestica. Svo. 1873. The Academy.
Leipsic : — Konigl. SachsiBche QeBeilschaft der Wiaseiuchaftoii. Ab-
handlungen. Math.-pUp. Classe. Band X. No. 6 ; Phil.-hiat.
Claase. Band VI. No. 5 ; Band VII. No. 1. roy. 8to. Leipxig
1873. Berichte iiber die Verbandlungen. Matb.-phye. Claaae,
1872. 3, 4, Eitraheft, 1873, 1, 2 ; PhJI.-hist. Claase, 1872. Svo.
1873. The Society.
Munich : — Kdnigl. Bayerische Akademie der WiaBenBchaften. Ab-
handlimgen. Math.-phys. Classe. Band XI. Abth. 2 ; Hist. Claase.
Band Xn. Abth. 1 ; Philos.-philol. Classe. Band XIU. Abth. 1.
4to. Miiwhen 1873. The Academy.
Washington : — Smithsonian Institution. Miscellaneous Collections.
Vol. X. Svo. 1873. Annual Beport of the Board of Begents for
the year 1871. Svo. 1873. The Institution.
Beporte &c.
Paris : — D^pot de la Marine. Annates Hydrographiques, 1873.
Trimestre 1, 2. Svo. Catalogue des Cartes &c. Svo. 1873.
Annuaire des Mar^ des Cotes de France pour I'aa 1874. 12ma.
1873. Annuaire de MaHes de la Basse Cochinchine pour Tan
1874. 12mo. 1873. Des Vents observes dans I'Atlantique Nord.
Svo. 1873. Fifty-six Maps and Plans. The D4pdt de la Marine.
Washington : — United States Q«ological Survey of the Territories.
First, Second, and Third Annual Beports, for 1867, 1868, and
1869. Svo. 1873. Sisth A nnual Eeport. 8vo. 1873. Report.
Vol. I. Part 1. Contributiona to IJie Extinct Vertebrate Fauna of
the Western Territories, by J. Leidy. Vol. V. Part 1. Acrididw
of North America, by C. Thomas. 4to. 1873. Hiscellaneous
Publications, No. 1,2. Svo. 1873. The Survey.
Annual Beport of the Chief Signal-Officer to the Secretary of War
for the year 1872. Svo. 1873. The Department.
1874.] Praentt. 337
Pebniajy 26, 1874.
TmuActianfl.
Amaterdam : — Koiiiiildijke Akodeinie van Wetenschappen. Yertiaado-
lingen. Deel SHI. 4to. 1873. Veralagen en Mededeelingen.
Afdeeling Natnorkimde. Tveede Beeka. Deel VII. 8vo. 1873.
Aid. Letterkimde. Tweede Beeks. Deel III. 8to. 1873. Jaai^
boek vooT 1872. 8vo. ProcesBen-Verbaal-, 1872-73. 8vo. Gaudia
Domestica. 8to. 1873. The Academy.
Letpsic : — Konigl. Sachsische Gesellschaft der WisBenBchaften. Ab-
handlungen. Math.-plijs. Claese. Band X. No. 6 ; Phil.-hist.
Oaeae. Band VI. No. 5; Band VII. No. 1. roy. 8to. LetjMiff
1873. Berichte tiber die Verhandlungen. Math.-phys. Classe,
1872. 3, 4, Extraheft, 1873, 1, 2 ; Phil.-hist. Classe, 1872. 8vo.
1873. The Society.
Municli ; — Konigl. Bayerische Akademie der WisBenBchaften. Ab-
handlungen. Math.-phye. Classe. Band XI. Abth.2; Hist. Classe.
Band XU. Abth. 1 ; Philos.-philol. Claaee. Band XIII. Abth. 1.
4to. MiauAtn 1873. The Academy.
'Washington : — SmithBOQian Institution. Miacellaneoua CoIlectionB.
Vol. X. 8to. 1873. Annnal Report of the Board of Begents for
the year 1871. 8vo. 1873. The Institution.
Beports £c.
Paris : — D4pdt de la Marine. Annates Hydrc^raphiques, 1873.
Trimestre 1, 2. 8vo. Catalogue des Cartes &c. 8vo. 1873.
Anuuaire des Mar^ des Cotes de France pour I'an 1874. 12mo.
1873. Annuaire da Mar^ de la Basse Cochinchine pour I'aQ
1874. 12mo. 1873. Des Venta obserr^a dans TAtlantique Nord.
8vo. 1873. Fifty-eii Maps and Plans. The D^pot de la Marine.
Washington : — Unit«d States Qeological Survey of the Territories.
Mrat, Second, and Third Annual Beports, for 1867, 1868, and
1869. 8to. 1873. Sixth Annual Beports 8vo. 1873. Beport.
Vol. L Part 1. Contributions to the Extinct Vertebrate Fauna of
the West«m Territories, by J. Leidy. Vol. V. Part 1. Acrididie
of North America, by C. Thomas. 4to. 1873. Miscellaneous
PuhUcations, No. 1, 2. 8to. 1B73. The Survey.
Annual Bepori) of the Chief Signal-Officer to the Secretary of War
for the year 1872. 8vo. 1873. The Department.
Cunningham (D. D.) Microscopic lExaminationB of Air. folio. CaiouUa
1873. The Government of India.
Day (F.) Beport on the Freshwater Fish and Fisheries of India and
Burma. 8vo. CoZniMa 1873, The Oovemmwt of India.
vol.. xm. t
228 Ust of Candidates. [Mar. 5,
Jevone (W. Stanley), F.H.S. The Prindples of Science : a Treatise on
Logic Find Scientific Method. 2 vols. 8vo. London 1874.
The Author.
Eiitimeyer (L.) TJeher den Bau ron Schale iind Schiidel bei lebenden
und fossilen SchildkrcitflD. 8to, Basel 1873. The Author.
March 5, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
In pursuance of the*Stjitut«s, the names of the Candidates for election
into the Society were read as follows : — ^
Eev. Alfred Barry, D.D., D.C.L.
Edward Middleton Barry, B.A.
Isaac Lowthian Boll, F.C.S.
George Bishop, F.E.A.S.
W. T. Biantord. F.G.S.
Henry Bowman Brady, F.L.S,
Thomas Lauder Bninton, M.D,
George Buchanan, M.A., M.D.
Walter Lawry BuUer, Sc.D.
W. Chimrao,"Capt. Tt.N.
Prof. W. Kingdom Clifford.
CnthbertCollingwood,M.A.,F.L.S.
Herbert Daries, M.D.
August Dupro, Ph.D., F.C.S.
Thomas Fairbaim.
Joseph Fayrer, M.D.
Prof. Dand Ferrier, M.D.
Peter Le Nevo Foster, M.A.
Augustus Wollastou Franks, M.A.
Prof. Thomas Minchin Goodeve,
M.A.
Lewis Dunbar Brodie Gordon,
F.G.S.
Eobert Baldwin Hayward, M.A.
Prof. Olaus Henrici, Ph.D.
Preacott G. Ilewett, F.E.C.S.E.
John Eliot Howard, F.L.S.
Prof. Thomas M'Kennv Hughes,
M.A.
Bldmund C. Johnson.
Robert M'Lachlan, F.L.S.
Sir Henry Sumner Maine, C.S.I.,
LL.D.
Kichard Henry Major.
William Maves, Stafi-Commander
B.N.
Charles Meldrum, M.A.
Edmund James Mills, D.Sc.
Eichard Xorris, M.D.
Oliver Pemberton, M.R.C.S.
Eev. Stephen Joseph Perry.
John Arthur PhilHps, F.C.S.
AViUiam Overend Priestley, M.D.
William Chandler Eobcrts, F.C.S.
Henry Wyldbore Eumsey, M.D.
Henry Toung Darracott Scott,
Major-General E.E., C.B.
Alfred E. C. Selwyn (Geo!. Survey,
Canada).
Samuel Sharp. F.G.S.
Robert Swinlioe.
Sir Henry Thompson, F.R.C.S.
Thomas Edward Thorpe, Ph.D.
Charles Todd (Oba., Adelaide).
Ed«in T. Truman, M.R.C.S. "
Fmncia Henr>' Wenham, F.E.M.S.
Wildmaii Orange Whitehouse, CF:.
Charles William Wilson, Major
B.E.
Archibald ITenry Plautagenet
Stuart Worlley, Lieut. -Col.
1874.] On the localization qf Function in the Brain. 220
The Presents received were Wd on the table, and thanks ordered for
them.
The foUowlDg Paper was read : —
" The Localization of Function in the Brain." By Datid
Fbrrier, M.A., M.D., M.R.C.P., Professor of Forensic
Medicine, King's College, London. Commnmcated by J.
BuRDON Sanderson, M.D., F.R.S., Professor of Practical
Physiology in UniTersity College. Received February 20,
1874.
(Abstract.)
The chief contents of this paper are the results of an experimental
investigation tending to prove that there is a localization of function in
specif regions of the cerebral hemiapheres.
In a former paper published by the author in the 'West Sidiog
Lunatic Asylum Medical Beports,' vol. iii. 1873, the results were given
of experiments on rabbits, cats, and dogs, mode specially for the purpose
of testing the theory of Hughlings Jackson, that localized and unilateral
epilepsies are caused by irritation or " discharging lesions " of the grey
matter of the hemispheres in the region of the corpus striatum. Besides
'confirming Hughlings Jackson's views, the author's researches indicated
an exact localization in the hemispheres of centres, or regions, far the
carrying out of simple and complex muscular movements of a definite
character, and described by him as of a purposive, or expressional, nature.
Facts were also recorded tending to show that other regions of the
brain were connect«d with sensory perception, but no localization was
definitely arrived at.
Among the experiments now related are some in further confirmation
and extension of those already made on cats, dogs, and rabbits, as well
as a new series of experiments on other vertebrates. In particular,
numerous experiments on monkeys are described, for the purpose of
which the author received a grant of money from the Council of tbe
Boyol Society, In addition, the results of experiments on jackals,
guineapigs, rats, pigeons, frogs, toads, and fishes are narrated.
The method of investigation consists in the application of the stimulus
of an induced current of electricity directly to tbe surface of the brain
in animus rendered only partially insensible during the process of explo-
ration, complete antesthesia annihilating all reaction. It is supplemented
by the method of localized destructive lesions of the hemispheres.
Special attention is called to the precision with which a given result
follows stimulation of a definite area — so much so, that when once the
brain has been accurately mapped out, the experimenter can preset with
certunty the result of stimulation of a given region or centre. The
theory that the phenomena are due not to excitation of cortical centres,
but to conduction of the electric currenta to basal gangli* and motor
230 Dr. D. Ferrier on the [Mar. 5,
tracts, is considered to be disposed of by the fact of the precision and pre-
dictable characters of the results, and by the marked differences in the
phenomena which are observed when regions in close local relation to
each other are excited. Other facts are pointed out bearing in the same
direction ; among others, the harmony and homology subsisting between
the results of experiment in all the different animals.
The experiments on monkeys are first described.
Beference is continually made in the description to figures of the brain,
OD which are delineated the position and extent of the regions, stimula-
tion of which is followed by constant and definite results. A complete
statement of these results in the present abstract is impossible.
Generally, it may be stated that the centres for the movements of the
limbs are situated in the convolutions bounding the fissure of Bolando,
viz. the ascending parietal convolution with its postero-parietal termina-
tion as far back as the parieto-ocdpital fissure, the ascending frontal, and
posterior termination of the superior frontal convolution. Centres for
individual movements of the limbs, hands, and feet are differentiated in
these convolutions.
Further, in the ascending frontal convolution, on a level with the pos-
terior termination of the middle frontal, are centres for certain facial
muscles, e. g, the zygomatics <fcc. At the posterior termination of the
inferior frontal convolution and corresponding part of the ascending
frontal are the centres for various movements of the mouth and tongue.
This is the homologue of " Broca's convolution." At the inferior angle
of the intraparietal sulcus is the centre for the platysma.
In the superior frontal convolution, in advance of the centre for cer-
tain forward movements of the arm, as well as in the corresponding part of
the middle frontal convolution, are areas, stimulation of which causes lateral
(crossed) movements of the head and eyes and dilatation of the pupils.
The antero-frontal region, with the inferior frontal and orbital convo-
lutions, give no definite results on irritation. Extirpation of these parts
causes a condition resembling dementia.
No results could be ascertained as regards the function of the central
lobe or island of Eeil.
Irritation of the angular gyrus (pit eourhe) causes certain movements
of the eyeballs and pupils. Destruction of this convolution gives data
for regarding it as the cerebral expansion of the optic nerve, and, as such,
the seat of visual perception.
The phenomena resulting from irritation of the superior temporo-
sphenoidal convolution (pricking of the ear, Ac.) are indications of exci-
tation of ideas of sound. It is regarded as the cerebral termination of
the auditory nerve. The sense of smell is localized in the uncinate con-
volution. The situation of the regions connected vrith sensations of
taste and touch is not accurately defined, but some facts are given indi-
cating their probable locality.
1874.] Localizatitm of Ftttictitm m the Brian. 281
The occipital lobea do aot reset on stimulation. Destruction of these
lobes caused no loss of sensation or ToluDtary motion, but an apparent
abolition of the instincts of self-preserration.
The corpora striata are shown to be motor in function, and the optic
thalami sensory.
Stimulation of the corpora quadiigemina causes dilatation of the
pupils, opisthotonic contractions, and the utterance of peculiar cries
when the tate* alone are irritated. The nature and signification of these
phenomena are regarded as still obscure, and requiring further investi-
gitioa.
8<xne experiments have been made on the cerebellum of monkeys.
They confirm the author's previous views tA to the relation of this organ
to coordination of the optic axes, and the maintenance of bodily equili-
brium. The eiperimenta are not detailed, as they will form the subject
of a future paper.
New experiments on dogs essentially confirm those already published,
while many new facta have been elicited. Those on jackals agree in the
main with the experiments on dogs, both as to the chuacter of the results
and the localization of the centres. New experiments on cats generally
confirm, as well as further define, the results described by the author in
his former paper. The &ctB of experiment on rabbits, guineapigs, and
rats are essentially alike, and also confirm former statements.
In all those animals tbe sensory regions are defined and their position
compared with those in the brain of the monkey.
The only result obtained by stimulation of the cerebral hemispheres
in pigeons was contraction of the pupil. The region associated with this
action, situated in the postero-parietal aspect, is compared with a similar
region in the nmmnmliftn brain, and regarded as the seat of visual per-
ception.
Movements of the limbs in frogs, and of the tail and fins in fif hes (as
in swimming), can be excited from the cerebral hemispheres in these
animals. Exact localization of motor and sensory centres is not possible.
The optic lobes in birds, frogs, and fishes seem related to movements
of flight and progression, in addition to their relation with tbe eyes.
Similar phenomena result from irritation of the cerebellum; but the
significatian_of these is reserved for future inquiry.
From the data of physiological experiment a foundation is obtained
for constructing an anatomical homology of the convolutions.
Among other points in homology the fissure of Bolando is shown to
be the homologue of the crucial sulcus in tbe brain of the Camivora.
Tbe whole brain is regarded as divided into sensory and motor regions,
corresponding to the anatomical relation of these r^ons to the optic tha-
lami and corpora striata and the sensory and motor tracts.
The motor r^ons are regarded as essential for tbe execution of
voluntary movements, and as the seat <^ a corresponding motor memory
■n "^
232 Mr. E. B. LanJcester on the [Mar. 13,
motor ideas), Lhe sensory regions being looked upon as the organic seat
of ideas derived from sensory impressions. An tiplnnation is attempted
of the phenomena of aphasia, and the relation of the in:?mory of words
to the ideas they represent.
The theory that a eertjiin action, esoited by stinmlation of a certain
centre, is the result of a mental conception is i"onaidered and dispnted.
From the complesity of mental phenomena, and the participation in them
of both motor and sensory substrata, any sTStem of localiealioii of mental
faailties which does not take both faetors into account milst be radi-
cally false. A scientific phrenology is regarded as possible.
The paper concludes with a short consideration of tie relation of the
basal ganglia to the hemispheres. The yiew is adopted that they con-
ititute a subvoluntory or automatic seusori-motor mecbauism.
March 12, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
I. " Contributioas to the Developniental History of the Mollasca.
Sections I., II., III., IV." By E. Rav Lankester, M.A.,
Pdlow of Exeter College, Oxford. Communicated by G.
RoLLBSTON, M.D,, F.R.S.j Linacre Professor of Anatomy and
Physiology in the Uniyersity of Oxford. Received January 1 9,
1874.
(Abstract.)
Section I. The ovarian Eyg wtd early development o/Loligo.
The points of greatest interest to which the author draws attention in
the present memoir are : —
1. The explanation of the basketwork structure of the surface of the
ovarian egg by the plication of the inner egg-capsule.
2. The increase of the yelk by the inception of cells prohferated from
the inner egg-capsule.
3. The homogeneous condition of the egg at fertilization.
4. The limitation of yelk-cleavage to the cleavage-patch.
5. The occurrence of independently formed corpuscles (the autoplasts)
which take part in the formation of the blastoderm.
6. The primitive eye-chamber, formed by the rising up of an oval wall
and its growing together so as to form a roof to the chamber.
7. The origin of the otocysts by invagination.
8. The rhythmic contractility of a part of the wall of the yelk-sac.
1874.] - DevelopmaUal Hutory of the Molhaca. 233
9. The disappearance of the piimitaTe mouth, and the development of a
secondaiy mouth.
10. The development of a pur of lai^ nerve-ganglia by invagination
of the epiblast immediately below the primitive eye-chamben.
Oenerdl Connderatiom Telative to the Ohtervatima contained in Sections VL.,
III., IV. {tontaining the developmental hUloriei of Pisidium, Aplysia,
Ter^pes, Polyeera, taui Neritina).
In these observations the author points out briefly their bearing on two
matters of theoretical importance, viz. (1) the origin and significance of
what has been called the fiajtrttio-phase of development, and (2) the ho-
mologies or homogenies (as the author prefers to say) of the shells, liga-
ments, and internal pens of the MoUusca. More facts have to be sought
out and brought to bear on these questions ; but the author, while occu-
pied in that further search, indicates the anticipations which must guide
and stimulate it. Before doing so he mentions that there are a variety
of other matters of interest in. the facts recorded in the paper which can-
not yet be brought into any theoretical structure, but which are not on
that account kept back, as they will probably be of some service in their
isolated condition.
Kowalevsky was the first to describe, in a precise manner, the forma-
tion of the foundations of the alimentary tract in a developing embryo,
by invagination of the wall of a simple primitivo blastosphere, or hollow
ball of embryonic cleavage-^wrpuscles. He detected this mode of deve-
lopment in Amphiojrui, and subsequently in -ilscM^ia. By later researches
he was able to indicate the same mode of development in certain Vermes
(Saffitia, Euaxei, Lttmbz-ieua) ; and he mentioned incidentally that he had
observed a Bimilor development in the Heteropodous mollusk Atalanta.
At that time the author was studying the development of Pitidium and
Limax, and obtained evidence of the invagination of the primitive blasto-
sphere in those two widely separated mollnsks. Subsequently at Naples
he found the same process occurring in Nudibranchs. The probable
identity of this process of invagination with that so well known in the
Batrachians, especially through Strieker's admirable work on the subject,
became clear, to those occupied with embryologies! studies, from the facts
established by Kowalevsky ; and the " anus of Busconi " could now be re-
cognized in the " orifice of invagination " present in members of the three
large groups of Vermes, Mollusca, and Vertobrata.
The embryonic form produced by this invagination-process is a simple
aac composed of an ectoderm and endoderm, with an orifice connecting
the exterior with the cavity lined by the endoderm. It, in short, pre-
sents the typical structure of the simplest Ckelenterata, and corresponds
exactly with the so-called Planvla of the polyps and corals. Hence we
are tempted to see in this primitive invagination-form the representative
of the CcGlenterat« phase of development of the whole animal kingdom.
234 Mr. K. R. Laiikester oit the [Mar. 12,
111 a paper published iii May 1873*, coDtomJDg the aubatance of lectures
deliyei-etl in the preceding Oi-tober, the author discussed this notion at
Bomo length, and other points cuoiiected with the attempt to wwk out
the con-espondencea of the embryonal^^ll-layera of the various groups of
the animal kingdom. At the end of the year 1872, Professor Uackel'a
splendid Monograph of the Calcareous Sponges appeared, in which the
same questiouH are methodically discussed. The name GasCniia is given
by Professor Hiiokel to the embryonic form which the author proposed
to designate by the old name Planula ; and the multicellular bJastoaphere,
from which the Gaxtrula is developed, which the author had proposed to
speak of as a Pulgplast, he well christeiiB the Morala. Professor Miickol
was able to show in his monograph that &e Catcarecrus Sponges exbilHt a
beautifully definite (riw^ruif-larvn, which swims freely by means of eilia,
Lieberkiilm, Miklucho-JIaclay, and Oscar Schmidt had previously shown
that certain sponges exhibit such an embryonic form; but Professw
Hiickel described it in many cases, and showed fully its mode of deve-
lopment and structure.
This brings us to an important point in what Hackel calls the "Gas-
tnca theory "t. The Gastrala form of the CalcareouB Sponges is not formed
by invagination, but without any opening in the blastospbere mailing its
appearance ; the cells conatitutiDg its walls divide into an endoderm and
an ectoderm ; then, and not until then, an orifice is formed from the
central cavity to the exterior by a breaking through atone pole. Careful
accounts of the development of Coelenterata, with a ^iew to determine the
mode of development of the PlaMuUi or Qastrula form in regard to the
question of invagination, are not to hand in a large number of cases.
But, on the one hand, we have Kowalevsky's account of the development
of Pelagia and Actinia, in which the formation of a Qastntla by invagina-
tion is described, as in the cases already cited among Vermes, Molluscs,
Kad Vertebrata ; on the other hand, we have Allman's observations on
the Hydroids, Schultze's on Cordyhpluira, Kleinenberg'a on Hydra,
Hackel's on the Siphonophora, and Hermann roll's on the Geryonjdje,
in which the ectoderm and endoderm of the embryo (which is at first a
Planula without mouth, then a Qatlrula with a mouth) are stated to
arise from the splitting or " delamination " of a single original series of
cells forming the wall of the blastosphere. Hermann Foil's observations
are of especial value, since he shows most carefully how, from the earliest
period, even when the egg is nnicelhilar, its central part has the character
of the endodermal cells, its peripheral part that of the ectodermal cells.
The question now arises, can the Qattrvla which arise by invagina-
tion be regarded as equivalent txi those which arise by internal segrega-
tion of an endoderm from an ectoderm ? and if so, which is the typical
• AnnaU and M>g. Nat. Hist 1673, li. p. 321.
t His moat reoent tiewi on this niBltgr ure ronUinfd in i pamphlet duled Jun<! 7.
IS73, ■ Die Gaitraa-Theorie."
1874.] Developmental HUtmy of the Molbuea. 285
or ancestral mode of development, and what' relation baa the orifioe of
invagination in the one case to the mouth which, later, breaks its way
through in the other ?
It is not within the scope of the present memoir to discuss these que»-
tions at length; but the author is of opinion that we must regard the
Ocutnda~aac with its endoderm and ectoderm as strictly equivalent (ho-
mogenous, to use another expression) in the two seta c^ cases. One of
the two methods is the typical or ancestral method of development, and
the departure from it in the other cases is due to some disturbing condi-
tion. He believes that we shall be able to make out that disturbing
element in the condition of the egg itself as laid, in the presence in that
egg of a greater or less amount of the adventitious nutritive material
which Edouard van Beneden calls " deutoplasm." This and certain re-
lations of bulk in the early developed organs of the various embryos con-
sidered, determine the development either by invagination or by delami-
nation. The relation of bulk to the process of invagination may be illus-
trated from a fact established in the preceding communications. In
Loligo the large otocysts develop, each, by a well-marked invagination oE
. the epiblast, forming a deep pit which becomes the cavity of the cyst. In
Aplyiia the smaller otocysts develop, each, by a simple vaeuolation of
the epiblast without invagination. In LcUgo the chief nerve-ganglia de-
velop by invagination of the epiblast, in Aplywia by simple thickening.
Again, in Yertebrata the nerve-cord develops by a long invagination of
the epiblast ; in Tuliftx and Lumbricus the corresponding nerve-cord de-
velops by a thickening of the epiblast without any groove and canal of
invagination.
The bulkier structures in these cases are seen to develop by invagi-
nation, the smaller by direct segregation. Invagination therefore acts as
an economy of matenal, a hollow mass being produced instead of a solid
mass of the same extent.
That the presence of a quantity of deutoplasmic matter, or of a par-
tiaUy assimilated mass of such matter, in the original egg ia not accom-
panied by well-marked invagination of the blaatosphere, while the absence
of much deutoplasm is the invariable characteristic of eggs which de-
velop a Gattrula by invagination, is shown by a comparison of Aplytia
and Loligo with Piadtum and Limax, and of the Bird with the Batra-
chian. In some cases, such as Selenka has characterized by the term
" epiboly," it seems that the enclosure of the large yelk-mass by the over-
growth of cleavage-cells may be held as equivalent to the invagination
of the lai^ yelk-cells by "emboly;" and the intermediate character
which the development of Evaatt and Lumbriau present in this respect,
as described by Kowalevsky, tends very strongly to establish a transition.
But the mode of development of the Qagtrula i>t Geryonid», described
with so much minuteness by Foil, which is obviously the same as that of
the Oatlrvia of Spongiada and most Hydroids, is clearly no masked case
Mr. E. R. Lankeater on the [Mar. 12,
of iovaginatioii. There is no question o£ " epiboly " here, but a direct
and simple splitting of one cell into two ; so that vhat was a sac formed
by a layer of cella one deep, becomes a sat' formed by a layer of eells
two deep, or of two layers each one deep.
It is yet a question for much further inquiry as to how this mode
of forming a double-walled Oagtrula cau be derived from, or harmonined
with, the formation of Giutrulahy the embolic or epibolic forms of inva-
gination.
It would certuinly seem at present that the orifice o£ inva^nation of
the invaginate Oasli-ula must wot be regarded as the equivalent of the
later erupting month of the segregate Oastrula*, which is the true per-
manent mouth of the Spouge or Ccelenterate. In no case ts the oriiice
of iuvagiuation of the invaginate Oaatrida known to persist under any
form ; it appears solely to effect the invagination, and nheu that is
effected vaniBhea.
Enough has been said to show the importance of observations relating
to the GcKinda-'pha&ei of development. In the paper well-marked inva-
ginate Goiinda are described from ; —
1. Piaidiam (Lamelli branch).
2. Ttrffipes (Nudibranch).
3. Pohjcera (Nudibranch),
4. Limas (Pulmonate).
5. Limnceut (Pulmonate).
In addition to these cases of the development of invaginate Gaatndct
among MoUusca, the examination of the very beautiful figures in the
papers of Love'n on molluecan development leaves no doubt that he
has observed invaginate Qastrula: in the following cases, but has not
understood their structure ; —
6. Cardium (LamelUbranch).
7. Ci-fntlki (Lamellibranch).
Similarly, Karl Yc^'s observations on AcUeon indicate the same state
of things as the author has pointed out in Polyetra; and hence we mav
add:—
8. Aetceon (Nudibranch),
and, finally, from Kowaievsky's statement, though not accompanied by
figure or descriptiou,
fl. Aialanta (Heteropod).
The second matter of theoretical interest (namely, the early features
in the development of the shell) has not been previously discussed, since
the structures described in the paper as shell-patch, shell-groove, and
shell-plug were unknown.
If, as seems justifiable, the Cephalopoda are to be regarded as more
' In his paper in the ' AanaU' for Mbj 1873 Ibe author hai inclined to Ihe lietr
(bat it may be >o r(<gard«l.
1874.] Deoeb^meiUal HUtory of the MoUuaea. S87
nearly representuig the moUuscan type than do the other chuses, or, in
other words, more closelj reBemble the anceitnJ forms than they do, we
might look, ia the course of the developmeDt of the less typical Mollusca,
for some indication of a representative of the internal pen of the higher
Cephdopoda. We might expect to find some indication of the connexion
between this and the calcareous shell of other forms ; in fact the ori^nal
shell of all MoUusca should be an internal one, or bear indicatioos of a
possible development into that condition.
In PUidium, in Aplytia, and in Neritina the author has submitted evi-
dence of the existence of a specially differentiated patch of epidermio
cells at the aboral pole, which develops a deep furrow, groove, or pit in
its centre almost amounting to a sac-like cavity opening to the exterior.
The first (chitinous) rudiment of the shell appears as a disk on the sur-
face of this gland ; but also, in some eases, the caiity or groove is filled by
a chitinous plug.
Let the walls of the sac close and the activity of its lining cells con-
tinue, and we have the necessary conditions for the growth of such
a " pen " as that of the Decspodous Cephatopods.
At present the details of the development of the " pen " in the Cepha-
lopoda are not fully known ; but the author has evidence that it is formed
in an enclosed sac-like diverticulum of the epidermis, but he has not yet
ascertained the earliest condition of this sac. The history of its develop-
ment becomes surrounded with additional interest in relation to the shell-
gland of the other Mollusca.
The position of the groove of the shell-gland in Pitidium au^ieats a
possible connexion of its chitinoua plug with the ligament, which it will
be worth inquiring into in other developmental histories of Lamellibranchs.
The internal sheUs of other Mollusca besides the cuttlefish are cer-
tidnly not in some cases (e. g. Aplyna) primitively internal, but become
enclosed by overspreading folds of the mantle. But in the case of Limax
and its allies, it 'a possible, though the matter requires renewed investiga-
tion, that the shell is a primitively internal one representing the sheU-
plug.
There is yet one more possible connexion of this ahell-gland and plug :
this is the chitinous secretion by which TerebratvJa and its allies fix
themselves to rocks &c. The position of the peduncle exactly corre-
sponds to that of the shell-glaiid ; and an examination of Professor.
Morse's recently published account of the development of Ter^ratulina
leaves little doubt that at the pole of attachment, which very early deve-
lops its function and fixes the embryo, aa in-pushing occurs, and a kind
of shallow gland is formed which gives rise to the homy cement. The
author's own observationa on the development of TtrAratvla vitrea do
not extend to so early a period aa this.
It is perhaps scarcely necessary, in conclusion, to point out the close
resemblance of shell-gland and plug to the byssal gland and its secretion.
238 ^Messrs. Negretti mtd Zambra [Mar. 12,
They are cloaely similar structurea ; but there does nol appear to be
aiij reason for considering them " serial homologues," or more closely
related than are, sav, the hairs on the head of a man with the hairs oii
his cheat.
II. " On a New Deep-sea Thermometer." By Henry Negretti
and Joseph Warken Zambra. Commmiicated by Dr. Car-
penter, F.R.S. Received March 5, 1874.
The Fellows of the Boyal Society are perfectly aware of the assUtauee
afforded by Her Majesty's Government (at the request of the E«jyal
Society) for the purpose of deep-aea investigatjons, and have been made
acquainted with their results by the Reporla of those in* estigatioua
published in the ' I'roeeodinga of the Royal t^ociety ' aud by the in-
teresting work of Professor Wwille Thomson. Among other subjects,
that of the temperulure of the sea at various depths, and on the bottom
itself, is of the greatest importance. The Fellows are also aware that
for this purpose a peculiar thermometer was and is used", having its
hulb protected by an outt^r bulb or casing, in order that its indications
may not be vitiated by the pressure of the water at various depths, that
pressui^ being about 1 ton per square inch to every 800 fathoms. This
thermometer, as regards the protection of the bulb and its non-liability
to be affect«d by pressure, is all that can be desired ; but unfortunately
the only thermometer available for the purpose of registering tempera-
ture and bringing those indications to the surface is that which is
commonly known as the yii's thermometer — aa instrument acting by
means of alcohol and mercury, and having movable indices with delicate
aprings of human hair tied to them. This form of instrument
registers both maximum and minimum temperatures, and as an ordinary
out-door thermometer it is very useful; but it is unsatisfactory for
■cienti£c purposes, and for the object which it is now used (viz, the
determination of deep-sea temperatures) it leaves much to be desired.
Thus the alcohol and mercury are liable to get mixed in travelling, or
even by merely holding the instrument in a horizontal position ; the
indices also are liable either to slip if too free, or to stick if too tight.
A sudden jerk or concussion will also cause the instrument to give
erroneous readings by lowering the indices, if the b!ow be downwards,
or by raising them, if the blow be upwards. Besides these drawbacks,
the Six's thermometer causes the observer additional anxiety on the score
of inaccuracy ; for, although we get a minimum temperature, we are
by no means sure of the point where this minimum lies. Thus Professor
Wyville Thomson says (* Depths of the Sea,' p. 139) : — " The determina-
tion of temperature has hitherto rested chiefly upon the registration of
thermometers. It is obvious that the t«mperatnre registered
^tion of
1874.] OH a New Dt^-tea Thermometer. 289
by minimum thennometora sunk to the bottom of the bm, even tf their
registration were unaffected by the pressure, would oolj give the lowest
temperature reached aonwicAcre between top and bottom, Dot iitee*$arHy
at the bottom itself. The temperatures at various depths might indeed
(proWded they nowhere increased on going deeper) be determined by a
series of minimum thermomet«r8 placed at different distances along the
line, though this would involve considerable difEculEies. Still, the
liability of the index to slip, and the probability that the indication of
the thermometers would be affected by the great pressure to which they
were exposed, rendered it very desirable to control their indications by
an independent method." Again, at p^e 299, we find : — " I ought to
mention that in taking the bottom temperature with the Six's thermo-
meter the instrument simply indicates the lowest temperature to which
it has been subjected ; bo that if the bottom water were warmer than
any other stratum through which the thermometer had passed, the
observations would be erroneous." Undoubtedly this would be the case
in extreme latitudes, or in any spot where the temperature of the air ia
colder than that of the ocean. Certainly the instrument might be
warmed previous %a lowering ; but if the coldest water should be on the
surface, no reading, to be depended upon, could be obtained.
It was on reading these passages in the book above referred to that it
became a matter of serious consideration with ua whether a thermometer
could be constructed nhich could not possibly be put out of order in
travelling or by incautious handling, and which should be above suspicion
and perfectly trustworthy in its indications. This was no very easy task.
But the instrument now submitted to the Fellows of the Soyal Society
seems to us to fulfil the above onerous conditions, being constructed oa
a plan different from that of any other self -registering thermometers,
and containing as it does nothing but mercury, neither alcohol, air, nor
indices. Its construction is most novel, and may be said to overthrow
our previous ideas of handling delicate instruments, inasmuch as its
indications are only given by upsetting the instTument. Having said
this much, it will not be very difficult to gness the action of the thermo-
meter ; for it is by upsetting or throwing out the mercury from the in-
dicating column into a reservoir at a particular moment and in a par-
ticular spot that we obtain a correct reading of the temperature at that
moment and in that spot. Firsi; of all it must be observed that this in-
strument has a protected bulb, in order to resist pressure. This pro-
tected bulb is on the principle devised by us some sixteen years since,
when we supplied a considerable number of thermometers thus protected
to the Meteorological Department of the Board of Trade ; and they are
described by the late Admiral PitzBoy in the first Kumher of the
' Meteorelogical Papers,' page 66, published July 5th, 1867. Beferring
to the erroneous readings of all thermometers, consequent on their
delicate bulbs being compressed by the great pressure c^ the ocean, he
240
On a New Deep-sea Tliermovieter.
[Mar. 12,
gays r — ""With a ™w to obviate this failing, Messrs. Negretti and Zambra
undertook to mako a case for the weak bulbs, which should tnwismit
temperature, but resist pressure. Accordingly a tube of thick glass is
sealed outside the delicate bulb, between which aud the casing is a space
all round, which is nearly filled with mercury. The small space not so
filled is a vacuum, into which the mercury caa be expanded, or forced by
heat or mechanical compression, without doing injury to
or even compressing the inner or much more delicate
bulb."
The thermometers now in use in the ' Challenger' Expe-
dition are on this principle, the only difEerenee being Ihat
the protecting chamber has been partly filled with alcohol
instead of with mercury ; but that has nothing to do with
the principle of the invention.
We have therefore a protected bulb thermometer, like
B siphon with parallel legs, all in one piece, and having a
continuous communication, as in the annexed figure. The
scale of this thermometer is pivoted on a centre, and
being attached in a peipendicular position to a simple
apparatus (which will be presently described), is lowered
to any depth that may be desired. In its descent the
thermometer acts as an ordinary instrument, the mereury
rising or falling according to the temperature of the stratum
through which it passes ; but so anon as the descent
ceases, and a reverse motion is given to the line, so as to
pull the thermometer to the surfa*'e, the instrument turns
once on its centre, first bulb uppermost, and afterwards
bulb downwards. This causes the mercury, \i'hich was
in the left-hand column, first to pass into the dilated si-
phon bend at the top.and thence into the right-hand tube,
where it remains, indicating ou a graduated scale the ex-
act temperature at the time it was timied over. The wood-
cat shows the position of the mercury o/Ver the instrumeut "l'
has been thus turned on its centre. A is the bulb ; B the
outer coating or protecting cylinder : C is the space of
rarefied air. which is reduced if the outer casing be com-
pressed : D is a sranll glass plug on the principle of our
Patent Maximum Thermomater, which cuts off, in the
moment of turning, the mercury in the column from
that of the bulb in the tube, thereby ensuring that none
but the mercury in the tube can be transferred into
the indicating column ; E is an enlargement made in the
bend so as to enable the mereury to pass quickly from
one tube to another in revolving ; and F is the indicating
tube, or thermomfiter proper. In its action, aa soon an
1874.] On the Chemical Conetiltdion of Saline Soluiiotu. 241
the thermometer is pat in motion, and immediately the tabe has acquired
a slightly oblique position, the mercury breaks oS at the point D, nms
into the curved and enlarged portion E, and eventually falls into the
tube F, when this tube resumes its original perpendicular position.
The contrivance for turning the thermometer over may be described as
a short length of wood or metal having attached to it a small rudder of
fan ; this fan is placed on a pivot in connexion with a second, and on
this second pivot is fixed the thermometer. The fan or rudder points up-
wards in its descent through the water, and necessarily reverses its posi-
tion in ascending. This simple motion or half turn of the rudder gives
ft whole turn to the thermometer, and has been found very effective.
Various other methods may be used for turning the thermometer,
such as a simple pulley with a weight which might be released on teaching
the bottom, or a small vertical propeUer which would revolve in passing
through the water.
March 19, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Bight Hon. Viscount Cardwell was admitted into the Society.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
I. " Preliminary Notice of Experiments concerning the Chemical
Constitution of Saline Solutions." By Walter Noel Hartlit,
F.C.S., Bemonstrator of Chemistry, King's College, Iiondon,
Communicated hy Professor Stoebs, Sec. R.S. Keceived
February 3, 1874.
The author has been engaged in investigating the above subject during
the lost eighteen months, and his experiments being still in progress, he
thinks it desirable to place the following observations on record.
In the examination of the absorption-spectra, as seen in wedge-ehaped
cells, of the principal salts of cerium, cobalt, copper, chromium, didymium,
nickel, palladium, and uranium, to the number of nearly sixty different
solutions, it was noticed that the properties of the substances in regard
to changes of colour could be ascertained by noticing the absorption-
curves and bands, so that, provided water be without chemical action,
it could be foreseen what change would occur on dilution of a saturated
solution.
TJui effect of Mtat on Abiorption-i^Ktra.
When saturated solutions of coloured salts are heated to 100° C, 1st,
242 Or the Chemical Constitulim qf Saline Solaliaas. [M»r. 19,
tliere are few ctmoa in whicb no i^huige is noticed. 2udly, generally the
amount of light transmitted is diminished to a small extent by some of
the more refranKible, the leas refrangible, or both Idnds of raya being
obfltrui-t-ed. 3rdl_v, tliere is frequently a complete difference in the
nature of the transmitted light. Anhydrous salts- not depomposed,
hydratod compounds not dehydrated at 100° C„ and salts which do not
change toloiir on dehydration, give little or no alteration in their spectra
when heated.
Solutions of hydrated salts, and most notably those of haloid com-
pounds, do change ; and the alteration is, if not identical with, similar to
that produced by dehydration and the action of dehydrating hqiiids, such
as alcohol, acids, and glycerine, on the salts in crystals or solution.
A particiUar instance of the action of heat on an aqueous solution is
that of cobalt chloride, which gives a diScreut series of dark bands in
the red part of the spectrum at difEerent temperatures, ranging between
23° C. and 73° C. Band after band of shadow intercepts the red rays as
the temperature rises, till finally nothing but the blue are transmitted.
Drawings of six different spectra of this remarkable nature have been
made. The changes are most marked between 33° and 53°, when the
temperature may be told almost to a degree by noting the appearance of
the spectrum. Though to the unaided eye cobalt bromide appears to
undergo the name eliange, yet, as seen with the spectroscope, it is not of
BO curious a character, the bands being not so numerous.
With cobalt iodide a band of red light ia transmitted at low t«mperatures ;
thebandof light moves towards the opposite end of the spectrum, with rise
of temperature, until it is transferred to such a position that it consists of
green rays only. In this instance the change to the eye is more striking
when seen without the spectroscope, because the misturea of red, yellow,
and green rays, which are formed during the transition, give rise to verv
beautiful shades of brown and olive-green. Thus a saturated solution at
16° C. was of a brown colour, at — 10° C. it became of a fiery red and
crystals separated, at -t-lO" reddish brown, at 20° the same, at 35°
Vandyke brown, at 45° a cold bron-n tint with a tinge of yellowish green,
at 55° a decidedly yellowish green in thin layers and yellow-brown in
thick, at 65° greenish brown, thin layers green, and at 75° oliie-green.
An examination of this cobalt salt has shown that there are tno distinct
crystalline hydrates — the one, formed at high temperatures, has the
formula Co Clj.2HjO, and is of a dark green colour ; the other, which
contains a much larger proportion of crystalline water, Co CI,, 6H,0,
is produced at a low temperature, and its colour is generally brown,
in cold weather inclining to red.
The action of beat on .solutions of didymium is characterized hy a
broadening of the black lines seen in the spectrum, more especially of
the important band in the yellow ; and in the case of potassio-didymium
nitrate, this is accompanied by the formation of a new line. In the case
1874.} Ob the Blood-corptucUa of MrnnmaUa, 243
of didyiniuDi acetate, vMch decomposes with sepontioii of a basic salt,
tite lines thickened on heating.
Themu-chemieal Experiments.
Begnauld (Institut, 1864 ; Jahresbericht, 1864, p. 09) has shown that
on dUuting a saturated solation of a salt, as a mle there is an absorption
of heat ; but in one or two cases he noticed that heat was erolved. The
change in colour that ta1(es place on the dilution of saturated solutions of
cobalt iodide, cupric chloride, bromide, and acetate is very remarkable.
There is every likelihood that this phenomenon is due in each case to the
formation of a liquid hydrate. It is impossible of belief that accompanying
such a circumstance there should be no measurable development of heat;
and the author's experiments have proved that in the above cases, at any
rate, the heat disengaged is very considerable — amounting, for instance,
on the part of cupnc chloride, at least to about 2565 units when 1 gram
molecule of the crystalline salt is dissolved in its minimum of water at
16° C and brought into contact with sufScient to make the addition of
40 Aq. These numbers only roughly approximate to the truth. On
diluting a solution of cobalt iodide till the red colour appears, the thermal
effect must be much greater, as not only does it register several degrees
on an ordinary thermometer, but it may be perceived by the hand.
The conclusions indicated by these results are obvious, but it is beyond
the scope of this paper to refer to them. The writer hopes before long
to complete his experiments with the view of having them communicated
to the lioyal Society.
II. "Note on the Intracellular Development of Blood-corpuscles
in Mammalia." By Edward Albert Schafer. Communis
cated by Dr. Sharpbt, V.P.B.S. Received January 22, 1874.
If the subcutaneous connective tissue of the new-born rat* is exa-
mined under the microscope in an indifferent fluid, it is found to consist
chiefly of an almost homogeneous hyaline ground-substance, which is
traversed by a few wavy fibres, and has a consider^le number of exceed-
ingly dehcate, more or less fiattoned cells scattered throughout the tissue.
The cells here spoken of are of course the connective-tissue corpuscles.
They are not much branched as a rule(at any rate their branches do not
extend far from the body of the corpuscle), and they are mainly distin-
guished by the extraordinary amount of vacuolatiou which they exhibit —
by which is meant the formation within the protoplasm of minute clear
spherules, less refractive than that substance, and probably, therefore,
spaces in it containiog a watery fluid. The nuclei, of which there is
generally not more than one in each cell, are frequently obscured by the
vacuoles, but, when visible, are seen to be roimd or oval in shape and
* ^nw uumsl employed wu &e white rat,
244 On the Blood-corpvscles ofAfammalia. [Mar. 19,
beautifully clear and homogeneoua ; they commonly contain either one
or two nucleoli. It is from these cells that the blood-Tessels of the tissue
are forme^l, and within them, red, and perhaps also, white hlood-cor-
puBclea beeouio developed.
Of the vacuolated cells above described some possess a dietinct reddish
tinge, either pretty evenJy diffused over the whole corpuscle, or in one or
more patches, not distinctly circumscribed, but fading off into the sur-
rounding protoplasm. Others contain either one, two, or a greater num-
ber of reddish globules, consisting apparently of hjemoglobin. These vary
in size, from minute specks to spherules as large as, or even larger than,
the red corpuscles of the adult r in cells wbich are apparently least deve-
loped it is common to find them of various sizes in the same cell ; whereas
cells which are further advanced in development are not uncommonly
crowded with haimoglohin-glohules, tolerably equal in point of siie, and
differing from the adult corpuscle only in shape. It is important to re-
mark that there is, at no time, an indication of any structure within the
globtdes resembling a nucleus : the nucleus of the cell also appears, up to
this point at least, to undergo no change. In fact the formation of the
hsemoglobin-globulea reminds one rather of a deposit within the cell-
substance such as occurs in developing fat-eells, the difference being that
in the latter case the deposited globules eventuaUy run together int« one
drop, whereas in the former they remain distinct as they increase in size
and erentually take on the flattened form.
Before, however, this change occurs in the hsBmoglobin-globules, the
cells containing them become lengthened, and are soon foitnd each to
contain a cavity, within which the globules now lie. This cavity is pro-
bably formed by a coaleecence of the vacuoles of the cell, or, what amounts
to the same thing, by the enlargement of one vacuole and the absorption
of the rest into it. The cell now comes to resemble a segment of a ca-
pillary, but with pointed and closed extremities ; it is of an elongated
fusiform shape, and consists of a hyaline protoplasmic wall (in which the
nucleus is imbedded) enclosing blood-corpuscles in a fluid — blood, in fact.
Two or more such c^lls may become united at their ends, a communi-
cation being established between their cavities ; indeed, by aid of branches
sent out from the sides a number of ceUs may unite to form a complete
plexus of capUlaiy vessels containing blood, and situate at a considerable
distance in the tissue from any vessels in which blood is circulating.
JEventualiy, however, these last become united with the newly developed
capillaries, and the blood contained in the latter thus gets into the
general circulation.
"With regard to the mode of junction of the capillary-forming cells with
one another, and with processes from preexisting capillaries, it has seemed
to me to occur most commonly, not by a growing together of their ei-
treme points, as commonly described, but rather by an overlapping and
coaptation of their fusiform ends, which, at first solid, become subse-
1874.] On-Mi^eU and Sleetrie Gmdueton.
Queotiy hollowed by tta extension into (hem of the cftrity of ib6 cell Or
cspill^, the partition between the two being finftlly sbioriwd.
The best preparations •for demonstrating tho facts abore described or*
obtained from the subcutaneous tissoe of the upper put of the fore limb,
and from that under the skin of the back — regions in which, in the adult
rat, this tisane becomes almost entirely conTert«d into fat. Drea in the
new-bom animal some portions hare already undergone this change ; and
it is principally in the neighbourhood of such patches that the hema-
poietic cells are met with. It is only when the young rats are not more
than a few days old that the formation of blood-vessels is preceded by a
development of blood-corpuscles within the same cells ap form the vessels i
in such other animals as I have hitherto examined this phenomenon se^ni
to occur only whilst still in the foetal state. The immature condition in
which the young of the rat are brought forth is sufficient to account foe
this difference.
The observations here recorded as to the intracellular development o£
blood-corpuscles are in many respects in accordance with what has already
been described by others as occurring in the area vaieuhia and other parts
of the embryo chick. It has not, however, appeared desirable to enter
into the literature of the subject in this bt^ notice.
m. " On the Attractions of Magnets and Electric Conductors."
By Geoboe Gou, F.R.S. Beceived January 27, 1874.
Being desirous of ascertabiing whether, la the case of two paralM
wires conveying electric currents, the attractions and repulsions were
between the currenta themselves or the substances conveying them, and
believing this question had not been previously settled, I made the fi^
lowing experiment : —
I passed a powerful voltaic current through the thick copper wire of a
large electromagnet, and then divided it equally between two vertical
pieces of thin platinum wii« of equal diameter and length (about six or
seven centimetres), so as to make them equally white-hot, the two wires
being attached to two horisontal cross wires of copper.
On approaching the two vertical wires symmetrically towards tlw
vertical face of one pole of the horiEontolly placed magnet, and at equal
distances from it, so that tlie two downward currents in them might be
eqn^y acted upon by the downward and upward portions respectively
of the currents which drcuhtted nnind the magnet-pole, the one was
strongly bent towards and the other from the pole, as was, of course,
expected ; but not the least sign of alterataoa of rehttive temperature <rf
the two wires could be perceived, thereby proving that not even a small
proportion of the current was repulsed from the repelled wire or drawn
into the attracted one, as would have occurred had the attraction and
repulsion taken place, even to a aodra«t« degree, between the cnizeints
lt2
246 0)1 Maffnets and Electric Conductors. [Mar. 19,
themselves ; aad 1 therefora conclude that thi aUr^ians and rejmhioiif
of electric tomlucloi's are iiot exei-ted between the currenU thertuelvet, but
between, the svhstanees convening them.
Some importftut consequencea appear to flow from this conclusion,
eBpeoially when it is considered in connexion with Ampere's theory of
magnetism, and with the molecular changes produced in bodies generally
by electric currents and hy magnetism.
As every molecular distiu-bance produces au electric alteration in bodies,
BO, conversely, the discoveries of numerous investigators hare shown that
every electric current passing near or through a substance produces a
molecular change, which ia rendered manifest in all metals, hquid con-
ductont, and even in the voltaic arc by the development of sounds, espe-
cially if the substances are under the influence of two currents at right
angles to each other. In iron it is conspicuously shown also by electro-
torsion, a phenomenon I have found and recently made knonii in a paper
read before the Eoyal Society,
Numerous facts also support the conclusion that the molecular changes
referred to last as long as the current, De la Rive has shown Ihnt a rod
of iron, either transmitting or encircled by an elecfric current, emits, as
long as the current lasts, a diSerent sound when stnick ; and we know it
' Also exhibits magnetism. The peculiar optical properties of glass and
other bodies with regard to polarized light discovered by Faraday also
coatinue aa long as the current. A rod of iron also remains twisted as
long as it transmits and is encircled by electric currents ; and in steel
and iron the molecular change (like magnetism) partly remains after the
cmrents cease, and enables the bar to remain twisted.
That the peculiar molecular structure produced in bodies generally by
the action of electric current-s also possesses a definite direction with re-
gard to that of the current, is shown by the rigidly definite direction of
action of magnetized glass and many other transparent bodies npon polar-
ized light, also by the difference of conductivity for heat and for elec-
tricity in a plate of iron parallel or transverse lo electric currents, by
tho stratified character of electric dischai^es in rarefied gases and
the action of electric turrents npon it, and especially by the pheno-
mena of electro- torsi on. In the latest example an upward current pro-
duces a reverse direction of twist to a downward one, and a right-handed
current develops an opposite torsion to a left-handed one ; and the two
latter are each internally different from the former. As each of these
four torsions is an outward manifestation of the collective result of inter-
nal molecular disturbance and possesses different properties, these four
cases prove the existence of four distinct molecular movements and four
corresponding directions of stmcture ; and the phenomena altogether
are of the most r^dly definite character.
As an electric current imparts a definite diroction of molecular struc-
ture to bodies, and as the attractions and repulsions of electric wires are
1874.] ^ctroacopie ObterviUions t^ the 8tm. 247
betneen the wires thetneelTes and not between the cuirents, repuldon in-
stead of attraction must be due to differmce of direction ofttrueture pro-
duced by difference of direction of the currents.
Although the Amp^rean theory has rendered immense aerrice to mag-
netic science, and agrees admirably with all the phenomena of electro-
magnetic attraction, repulsion, and motion, it is in some respects defec-
tive; it assumes that magnetism is due to innumerable little electric
currente continually circulating in one unifonn direction round the mo-
lecules of the iron ; but there is no fcnown instance of electric currents
being maint^ed without the consumption of power, and in magnets
there is no source of power ; electric currents also generate heat, but a
magnet is not a heated body.
If, however, we substitute the view that the phenomena of attraction
and repulsion of magnets are due, not to continuously circulating electric
currents, but (as in electric wires) to definite directions of molecular
structure, such as is shown by the phenomena of electro-torsion to really
exist in them, the theory becomes more perfect. It would also agree with
the fact that iron and steel have the power of retiuning both magnetism
asd the electro-torsional state after the currents or other causes producing
them have ceased.
According so this view, a magnet, like a spring, is not a source of
power, but only an arrangement for storing it up, the power being re-
tained by some internal disposition of its particles acting like a "ratchet"
and termed "coercive power." The fact that a magnet becomes warm
when its variations of magnetism are great and rapidly repeated, does
not contradict this view, because we know it has then, like any other
conductor of electricity, electric currents induced in it, and these develop
heat by conduction-resistance.
According also to this ^-iew, any method which will produce the requi-
site direction of structure in a body will impart to it the capacity of being
acted upon by a magnet ; and any substance, fermginoas or not, which
possesses that structure has that capacity ; and, in accordance with this,
we find that a crystal of cyanito (a silicate of alumina) possesses the pro-
perty, whilst freely suspended, of pcanting north and south by the direc-
tive influence of terrestrial magnetism, and one of stannito (oxide of tin)
points east and west under the same conditions.
IV. " Spectroscopic Observations of the Sun." By J. Normak
LocKYEB, F.B.S., and G. M. Seabboke, F.R.A,S. ReceiTed
February 2, 1874.
(Abstract.)
This paper consisted of the observations made of the sun's diromo-
sphere and of the prominences for the period Ist September, 1872, to
31st December, 1873. Details are given of the modes of observation
adopted.
March 26, 1874.
JOSEPH DALTON HOOKEU, C.B., President, in the Chair.
The Presents received were laid on the table, and thanks ordered for
tbein.
The following Papers were read : —
I. " On the Organization of the Fossil Plants of the Coal-
measures.— Part VI. Ferns." By W. C. Williamson, F.R.S.,
Professor of Natural History in Owena College, Manchester.
Eeceived March 18, 1874..
(Abstract.)
The author call(jd attention to the various methods of classifyiug the
fem-fltems and petioles of the Coal-measures adopted by Cotta, Corda,
Brougniart, and others, and to the difGcul ties which attend those methods.
Some of those difficulties had been already felt and partially removed by
M, Brongniart. All the generic distinctions hitherto adopted were
based upon wiationB in the form, number, and arrangement of the Tas-
cvixr bundles. These elements vary so much, not only in different speraes
of the same genus, but in different parts of the same petiole, as to make
them most untrustworthy guides to generic distinctions. The consequence
has been an enormous multiplication of genera ; but, notwithstanding
their number, the author found that if he adopted the methods of his pre-
decessors he would hare to establish additional ones for the reception of
his new forms. Under these drcnmstances he decides that it will be
better to include the entire series of these petioles, provisionally, under the
common generic term of Sackiopterit. This plan dispenses with a number
of meaningless genera, and is rendered additionally desirable by the cir-
cumstance that all the petioles to which these numerous generic names
have been applied belong to fronds which have already received other
names, such as PteopUrit, Sphvnopterii, &c., only the structure of fronds
found in the shales, and their respective petioles of which we have ascer-
tained the structure, have not yet been correlated.
As a preparation for the present investigation, the author made an ex-
tensive series of researches amongst recent British and foreign fern-stems
and petioles, with the object of ascertaining not only the modifications in
their arrangementa in different parts of the same plant, but especially of
studying the modes in which secondary and tertiary vascular bundles
were derived from the primary ones. This inquiry led him over the
ground previously traversed by M. Tr^ul, and, so far as British ferns
were concerned, by Mr. Church.
The most common general forma exhibited by transverse sections ot
1874>.] FtutU Plants iff the Coal-meiuvre$. S49
these bundles in recent petioles may be teprelented by the letters H, T,
IX, and X. As a general rule, tiie seoondaiy bundles are given off irom
that part of the primary one which happens to be nearest to the secondary
rachis to be supplied. Thus in same cases the upper arms of the X will
merely be prolonged and their endt detached ; in other cases a loop pro-
jects from the side of one or both arms of the V, and becomes detached
as a ring.
The first petiole, described under the name of Raehiopleru atpera, is
one in which transverse sections of the central vascular bundle exhibit
modificationa of the H format its base, separating into two contiguouB
bundles higher up, and ultimately reverting to the V form — the gatter-
shaped bundle {en gouttiere) of M. Irecul. This is the plant to which, on
a previous occasion, the author proposed to assign the generio name o£
Edraaylon (Proc. Eoy. Soc. vol, ii, p. 438), The vessels are chiefly
reticulate, with some of the barred and spiral types. The bark con-
sists of a delicate iimer parenchyma, the cubical cells of which are arranged
vertically. This is. enclosed in a coarser middle parenchyma, and the
whole is surrounded by an outer layer, composed of intermingled paren-
chyma and prosenchyma, the latter being disposed in vertical fibrous
bands, having wedge-shaped transverse sections, and being modifications
of the Bclerenchyma of authors. The outer surface of the bark is covered
with innumerable little, obtuse, projecting cellular appendages, which ar«
obviously abortive hairs. These appendages are relatively huger in the
smaller rachis than in the larger petioles. In very young petioles trans-
verse bands of small consolidated cells traverse the bark at numerous
points, reminding us of the similar conditions seen in the Seterangium
Qrievii, described in a previous memoir. In the larger petioles these
coUular bonds have disappeared, and left in their places large intercellular
lacunn. N'umerous fragments of the terminal rachis of the above plant
have been obtained with the leaflets attached. For a long time the author
believed that he could identify these with the detached leaflet« of a JV
copterii, which are very abundant in the Oldham nodules ; but later
researches have led to the conolusion that the plant has been a ^heno-
pterit, closely allied to, if not identical wiUi, the S. HomingJuam of
Brongniart. The author proposes the provisional name of SaAu^ttrit
atpera for the above plant.
The next petiole described is one to which Mr. Binney proposed
(' Proceedings of the Literary tmd Philosophical Society of Manchester,'
Jan. 0, 1872) to give the name of StauropUrii OWutmia. This is one of
the plants of which the vascular bundle, when seen in transverse section,
exhibits the appearance of the letter X. The vessels composing this
bundle are barred ones ; t^ey are sometimes grouped in four slightly
coherent clusters, with some delicate, vertically elongated cells in or near
their central point of conjunction. The same kind of cellular tissue sur-
rounds the bundle, fonning a thia layer, which passes rapidly into a very
On the Fossil PJanli of the Coal-measures. [Mar, 2
thick layer, of coarse prosenchyma, and vrhich hae evidently been bard and
woody, as in mauy of the recent AdiantiumB. Toward§ the upper part
of the petiole the vaaeular bundle becomes distinctly consolidated into a
single cluster of crucial form ; it then passes into a somewhat trifid form,
and ultimately int-o a sraall cyliadrital one. Tlus petiole has branched
much more freely than any of the others described. Two of the estre-
mities of the crucial arms of the laecular bundle become first esJarged
and then detached us two secondary bundles, which generally have an
irregularly triangular transverse section, nith long arms to the triangle.
Theae triangular bundles are altogether different from the central aiis of
.AsterophylUtei Ae3criheAiQ& preceding memoir. The ultimate subdivisions
of these secondary branches look more like Uie terminations of cylindrical
rootletfl than of petioles — which fact, combined with the circumstance that
no traces of leaflets have been found associated with any of these ultimate
twigs, renders tlie petiolar nature- of this plant open to question, though
the arguments in favour of its being a braneliing fern-petiole preponderate
oTer those which militate against that conclusion. The author designates
this plant Ititrhinpleris Oldhamia.
The next plant described is an exqiuaitely beautiful petiole from Bumt^
island, to two detached portions of which the author has already assigned
the names of Arpexylon duplex and A. timpUx*, but which two forms he
now proves to belong to the same plant. In the matured petiole the
TEicular bundle is always a double one. There is a central bundle,
exhibiting a transverse section shaped like an hour-glass, one side of
which is truucat«d and the other rounded, with a free, narrow, crescentic
hand at the more truncate of its enlarged extremitieB. At each of these
extremities of the central bundle there is a longitudin^ groove, which is
shallow on the truncated side nearest to the crescentic bundle, but bo sur-
rounded by small vessels at the opposite convex side as often to become
converted into a longitudinal canal. The hour-glass bundle always reap-
pears in various specimens under the same aspect ; but the crescentic one
dividesinto two lateral halves, and the ends of each of these two subdivided
parts curl under their more central portions. We thus obtain two of the
creflcentic structures previously designated Arpexi/lon gimplex. These
crescentaare traced outwards through the bark to lateral secondaryrachidcs.
The Teasels thus detached from the truncated side of the central hour-
glass bundle now reappear at its opposite and more convex side, whence,
in turn, they again become detached ; so that the truncate surface with
ita crescentic appendage, and the more oblate one with Kb almost closed
canal, have alternately reversed their positions in the petiole as each
secondary rachis was given off. Alternating distichous tertiary rachides
spring from these secondary ones.
Two plants which appear to be identical with those described by M.
Sessillt, under the names of ZygopterisLaaatii and Z. Ubractiensi), are next
" Proceediiigg of the Sfijei Society, vol. xx. p. 438.
1874.] On the Motiotu of Nebula towardi or from the Earth. 26X
examined*. In these plants the eection of the central bundle exhilnt« a
form of the letter H. The Tesaels of the large central tranHTerse bar are all
reticulated ones : the greater part of those of the terminal vertical bars
are of the same character ; but the oatermost Teasels of those latter
structures are barred or qnasi-scalariform. As in the case of B. dvpUx,
already described, these outermost layers of barred vessels, accompanied
by a few reticulated ones, become detached alternately from opposite sides
of the K-shaped central bundle. Passing quickly through a tliin delicate
cellular inner bark, they eat«r the coarser parenchyma of a middle one,
as two irregular clusters of vessels with one common investment pro-
longed from the innermost bark. Onreachingtheouterbarktheybecome
two distinct cylindrical bundles, each with its own dehcate cortical
investing layer ; and thus invested, they emerge from the primary petiole
to supply the secondary rachis.
The Oldham specimens of HwAiepUrit bibradienaii agree with those
described by M. Benault in having all their vessels 'of the barred type.
The outer bark projects at numerous points iu large conical abortive
hairs, which almost assume a spinous aspect.
The author further figures and describes the sedaon of a vascular axis,
with a central cellular medulla surrounded by five contiguous crescenlic
masses of vascular tissue, whose concavities are directed outwards. This
plant appears identical with the AnartJicpteris Decaimii of Benault,
II. "On the Motions of some of the Nebulse towards or from
the Earth." By William Huggins, D.C.L., LLJ)., F.It.S.
Received January 26, 1874.
The observataons on the motions of some of the stars towards and
from the earth which I had the honour to present to the Boyal Society
in 1872 appeared to show, from the positicm in the heavens of the
approaching and receding stars, as well as from the relative velocities of
their approach and recession, that the sun's motion in space could not be
regarded as the sole cause of these motions. "There can be little doubt
but that in the observed stellar movements we have to do with two other
independent motionB — namely, a movement common to certain groups
of stars, and also a motion peculiar to each Btar''t,
It presented itself to me as a matter of some importance to en-
deavour to extend this inquiry to the nebuln, as it seemed possible
that some light might be thrown on the cosmical relations of the gaseous
nebula to the stars and to our stellar system by obserratiims of their
motions of recession and of approach.
Since the date of the paper to which I have referred, I have availed
* Aniaitm dct ScIminb KmtnrellM, 6* tlnie, Boi toms xii.
t Fi«etediiigsctftlwSo7dSod«tj,Tc^sx.p.382.
2S2 Br. W. HuffginA on the Motions of tome [Mar. 26,
myself of the nighta Bufiicieatly fine (imusually few even for our un-
favourable climate) to mate observatious on this point.
The inquiry was found to be ono of great difficulty, from the Faiutncss
of the objects and the very minute alteration in position in the spectrum
which had to ba observed.
At first the inquiry' appeared hopeleiis, from the circumstance that tJie
brightest line in the ncbuhir spectrum is not sniEdently coincident iu
oharacter and poeition ivith the brightest line in tha spectrum of nitrogen
t-o permit this line to be used as a fiducial line of comparison. The line
in the spectrum of the nebula) is narrow and defined, while the line ot
nitrogen ie double, and each component is nebulous and broader than
the lino of the nebulas. The nebular line is apparently coincideut
with the middle of the less refrangible line of the double lino of ui-
The third and fourth lines of the nebular spectrum are undoubtedly
those of hydrogen ;' but their great faintnoss makes it impossible to use
them as lines of comparison under the necessary conditions of great dis-
persive power, except iu the case of the brightest nehtUiD.
The second tine, as 1 showed in the paper to which I have referred, is
sensibly coincident with an iron line, wave-length 495*7 ; but this line ii
inconveniently faint, except in the brightest nebulte.
In the course of some other experiments my attention was directed to
a line in the spectrum of lead which falls upon the less refrangible of the
components of the double line of nitrogen. This line appeared to meet
the requirements of the cose, as it is narrow, of a width corresponding to
the slit, defined at both edges, and in the position in the spectrum of the
brightest of the lines of the nebulte.
In December 1872 I compared this line directly with the first line in
the spectrum of the Qreat Nebula in Orion, I was delighted to find this
line sufficiently coincident in position to serve as a fiducial liue of com-
parison.
I am not prepared to say that the coincidence is perfect ; on the con-
trary, I believe that if greater prism-power could be brought to bear
npon the nebulee, the line in the lead spectrum would be found to be in
a small degree more refrangible than the line in the nebulte.
The spectroscope employed in these observations contains two com-
pound prisms, each giving a dispersion of 9° & from A to H. A mag-
ztifying-pKiwer of 16 diamet«rs was used.
In the simultaneous observation of the two lines it was found that if
the lead line was made rather less bright than the nebular line, the small
excess of apparent breadth of this latter line, from its greater brightness,
appeared to overlap the lead line to a very small amount on its less
refrangible side, so that the more refrangible sides of the two lines
appeared to be in a straight line across the spectrum. This liue could be
* ProDBtdings of the Bojil Sooietj, vol, n. p, 360.
1874.] of the Nebula towards or from the Earth. 233
therefore conTeniently employed as a fiducial line in the obaenrationB I
had in view.
In my own map of the spectrum of lead this line is not giren. In
Thal^n's map (1868) the line is represented by a short line to show that,
under the conditions oF spark under which Thal^n observed, this line was
emitted hj those portions only of the vapour of lead which are close to
the electrodes.
I find that by alteratioOB of the character of the spark this line becomes
long, and reaches from electrode to electrode. As some of those conditions
(such as the absence of the Leyden jars, or the close approximation of
the electrodes when the Leyden jars are in circuit) are those in which the
lines of nitrogen of the air in which the spcurk is token ore faint or
absent, the circumstance o( the line becoming bright and long or faint
and short, inversely aa the line of nitrogen, suggested to me the possi-
bility that the line might be due not to the vapour of lead, but to some
combination of nitrogen under the presence of lead vapour. As, how-
ever, this line is bright under similar conditions when the spark is taken
in a current of hydrogen, this supposition cannot be correct,
A condition of the spark may be obtained in which the strongest lines
of the ordinary lead spectf um are scarcely visible, and the line under
consideration becomes the strongest in the spectrum, with the exception
o£ the bright line in the extreme violet.
I need scarcely remark that the circumstance of making nee of this
line for the purpose of a standard line of comparison is not to be taken
as aSording any evidence in favour of the existence of lead in the
nebulte.
Each nebula was observed on several nights, so that the whole observ-
ing time of the past year was devoted to this inquiry. In no instance
was any change of relative position of the nebular line and the lead line
It follows that none of the nebulte obsei^ed shows a motion of trans-
lation so great as 26 miles per second, including the earth's motion at
the time. This motion must be considered in the results to be drawn
from the observations; for if the earth's motion be, say, 10 miles
per second from the nebula, then the nebula would not be receding
with a velocity greater than 15 miles per second ; but the nebula might be
approaching with velocity aa great as 35 miles per second, because 10
miles of this velocity would be destroyed by the earth's motion in the
contrary direction^
The observations seem to show that the gaseous nebulie as a class
have not proper motions so great aa the bright stars. It may be
remarked that two other kinds of motion may exist in the nebulie, and,
if sufficiently rapid, may be detected by the spectroscope : — 1. A motion
of rotation in the planetary nebuln, which might be discovered by phudng
the slit of tlie infltrnment on opposite limbs of the neboloi. 2. A motasn.
g
^^H
^^H
^^^H ^^^^^^H
1
^— "^^^^^
1
254 Mr. J. A. Broun on the Annual [Mar. 26,
of translation iu the visual direction of aome portions of the nebulous
matter within tho uebuliv, which might be found by compuriiig the
difEerent parts of a large and bright nebula.
Sir William Herschel states that " nebulie wero generally detected in
certain Erections rather than in others, that the spaces preceding them
were generally quite deprived of stars, that the nebulaJ appeared some
time after among starn of a certain considerable sine and but seldom
among very small stars, that when I came to one nebula I found several
more in the same neighbourhood, and afterwards a considerable time
passed before I came to another parcel "•.
Since the existence of real nebulro has been established by the use of
;he spectroscope, Blr. Proctorf ajid Professor D'Arrestt have called
attention to tho rektion of position which the gaseous nebiUio hold to the
Milky Way and the sidereal system.
It was with the hope of adding to our information on this point that
these observations of the motions of the nebulio were undertaken.
In the following list the numbers are taken from Sir J. HerBchel'B
General Catalogue of KebuliB.' The earth's motion given is the mean
of the motions of the different days of obsenatiou.
No.
h.
H.
Otliere.
Earth's motion from Nebula.
1179
4234
4373
4390
4447
4610
4964
360
1970
2000
2023
2047
2241
iv!37.
IV. 51.
IV. 18.
M. 42
S. 5
s.'c
M.67
7 miles per second.
12 „
1 ,.
2 „
3 »
14 .-
13 „
III. "Onthe AnnualVariationof the MagneticDeclination," By
J. A. Bboun, F.R.S. Received February 11, 1874.
The first observations which seemed to show that the mean position
of the declination-needle followed an annual law were those of Cassini,
made, more than eighty years ago, in the hall of the Paris Observatory
and in the eaves below it (90 feet under ground). It cannot be said,
however, that Cassini's result has been confirmed by subsequent observa-
tions, either as regards the direction or amounts of movement from
month to month.
The extensive series of observations made in difEerent parts of the
k ■ PbiI<Mophical TraDsoctions, 17S4, p. 448.
WL t Other Worlds than Ours, pp. ^280-290.
^ { Astroiioiiiische Jfaehrioliten, Ko. 1008, p. 190.
187'4.] Variaiion of tKe Magnetic DecUnation. 255
world in modem times have given results so different that we must con-
clude either that the magnetic needle obeys different annuaJ laws at each
place, or that the differences are due to instrumental errors. The con-
sequence has been that, after long, laborious, and expensive researches, it is
still a question whether the magnetic needle obeys an annual law or not.
The results obtained at some obBervatoriea have mads it very probable
that, if an annual law exist, the range of the oscillation must bo very
small. It is therefore essential, in questioning any series of observa-
tions for this law, to be assured that the errors (instrumental or others)
are neither considerable nor systematic.
I have concluded, from sevenJ series of observations made with sus-
pension-threads bearing unmagnetic or slightly magnetic weights, that
the systematic errors due to varying temperature or humidity are very
small when the suspension-threads are carefully constructed with fibres
from which the original torsion haa been removed. Dr. Lloyd has con-
cluded that threads with fibres differently twisted may produce com-
paratively large annual variations in different directions, according to the
direction of the twist. There is little doubt, however, that the greatest
errors are due to the unequal stretching and rupture of the different
fibres which form the suspension-thread.
When the instrumental errors may be so considerable compared with
the variations to be observed, it cannot be supposed extraordinary that
instruments in different places give different results ; and it appears
essential so to eliminate the sources of error that two instruments in the
some place may tell the same story before we attempt to announce the
existence of any law.
If at sea two or more chronometers are necessary in case one may be
affected by error, it seems not less necessary in scientific researches
requiring continuous observations for years, where errors are so difficult
of detection and elimination, that two or more instruments should be
observed. These considerationa induced me to establish at Treran-
drum two declination-magnetometers of different construction, placed
under considerably different atmospheric conditions ; and it is to the
results ot sixteen years' comparative observation from these two instru^
ments that I desire to draw the attention of physicists.
Both instruments had suspension-threads made vrith the utmost care.
One, Dr. Lloyd's instrument, made by Mr. Glrubb, of Dublin, with a
m^net weighing nearly a pound, was placed in the large room of the
Trevaudrum Magnetic Observatory, which was always more or less open
to the external air ; and, although covered by a cotton-wadded hood and
a series of boxes, it was much more liable to any errors due to atmo-
spheric actions than the other. Its chief source of error was, however,
connected with small movement-s of the telescope wire, although that was
made to coincide, at varying intervals of time, with the transit-mark five
miles distant.
256 Mr. J . A. Broun on the Annml [Mar. 26,
Tlie second instrument, mado according to my own designs by Mr. P.
Adie, of London, had a magnet weighing only about one sislb of the other ;
it WHS suspended under a glass boll from whicb tlio air wiis exhausted,
and which was covered with two hoods — one with gilt surfacea, the
other with cotton wadding. This instrument was placed in a closed room
without windows or external opeuings, and with s terraced ceiling below
the obeen-atory roof. Obser\-ed from without (within the large room of
the observatory), the diurnal variations of temperature in the instrument
were not more than three tenths (0'3) of a degree Fahrenheit, while the
annual variation was under 5° Fahr.*
The compared mean positions of the two magnets for each day, derived
from hourly observations of botli instruments during eleven j'ears, and
from eight daily observations during the remaining live years, will bo
found with all other details in the volume referred to in the note to the
preceding paragraph. It will be suflicient for the purposes now in view
to give here the chief conclusions from these means.
The monthly mean declinations having boon freed from tho secular
movement, and the meana for three groups of years having been taken,
these means are represented very nearly by the following equations of
sines (fl = 0, Jan. 15);—
Tetn.
fAdie. j/=0'-033sin(fl + 135°)+0'-009sin(2e+299°).
]854tol»oy |Grubb.i(=U'-U3asiu(0+15O°) + O'-O783in(l'O+3OO'j.
IHtint^ 18(14 |-^^'«- y=0'-1908in(8 + 178°)+0'-070sin(2e+324'').
lGrubb.y=0'-099ain(fl+211°)+0'0628in(2fl+319°).
IftfiKtolRflq Z-^^^- y=0'-171 sin (fl+181'>)+0'-104sin (28+342°).
lGnibb.y=0'-0S2 8iii(e+228°)+0'-122sin(2e+322°).
In the years 1854 to 1859 the movements of Onibb'e telescope were
Tery small, the daily mean declinations from both instruments differing
rarely more than O'-l throughout the whole six years. It will be seen
that the equations for these years agree very nearly. In spite of the
greater movements of the telescope in following years (affecting chiefly
the coefficient of sin 9), the epochs of maxima and mittima derived from
the two instruments differ but little, and all the principal deviations
from the mean law for any year are confirmed by both instruments.
When the means for the whole sixteen years are token, and the equi-
* Sxperimenti wilh luapenBioii-IIircadi mnying slightly magnetic nei'ghls of nearly
one pound, shoved Oivt, the eflbct of a change of 1° fUir. on the poeition of Orubb'i
inngnet amounted to about O'OOS ( — 0"'1S) — a r««ult deduced rrom (he change! of lem-
perature from hour to liour, na well an from those from day to day. I auel refer to
the flrtt volume of the ' Trevandruin Obwrvatioiu,' now in the preu, for (he details of
^thete eiperimeuta.
1874.] Variation of the Mt^putic Declination.
Talent equations of sines are carried to four terms, the {oUowing iwulti
are obtamed : —
1864 to 1869<
Adie. y=0'-120 8m(e+175<')+0'-076eiii(2e+323'')
+ O'-Oll Bin {3fl + 299°) + 0'-022 Bin (49 + 181°).
Gmbb. y =0'-056 Bin (fl + 209°) + 0'-095 sin (29 + 316°)
+ 0'-012 sin (39 +293°) + 0'-022 Bin (4fl + 197°).
From these equations we deduce the following epochs of mftTima and
minima: —
Minima. Ma3Qraa> '
Adie. January 26 and May 19. March 14 and October 1.
Grubb. January 13 and May 23. March 18 and September 29.
The confirmation o£ the results from Adie's instroment by those from
Gnibb's, in spite of the errors of the latter, is so marked in each year
and group of years, that ve can affirm that at Trevandrum, in the south
magnetic hemisphere, the magnetic needle obeys on annual law producing
a double oscillation, having a minimum towards the end of May, t^e prin-
dpal maximum near the end of September, another minimum in January,
and a secondary maximum in the middle of March. Or, taking the results
fr<Hn Adie's instrument as most free from all error, the principcd mini-
mum occurs about a month before the June solstice, and the secondary
TTiinimiim about a mouth after the December solstice ; while the principal
mitx'm'iT'i occurs about a week after the September equinox, and the
secondary muTimiim about a week before the March equinox.
In the result obtained by me from four years' observations (1843 to
1846) at Makerstoun, in Scotland, the greatest easterly position was
attained in the end of April or beginning of May, and the greatest
westerly (or least easterly) position in September. If that result, derived
from a single iuBtrument, can be accepted*, it would appear that the
movements of the north end of the needle, in the annu&l Tariations, are
in opposite directions at Trevandrum and Makerstoun at the same period
of the year. This result agrees with that which I have found for the
decennial inequality, or that in the south magnetic hemisphere ; the law
for the south end of the magnet is the same as that for the north end of
the magnet in the north magnetic hemisphere : but it is opposed to the
result obtained by me for the twenty-six day period, in which the easterly
and northeriy magnetic forces have their muxim* at the same time in both
hemispheres.
It follows that the results which are connected with the Bun's rota-
tion on its axis are the some in both hemispheres, while those related to
* I hkTB always coniidered tlii» recult a nesr Bpproiimatjcm to the tratli, \«A it
wu not confinned by th* rery limited went* of Qbnrraliaiu mads in the three sutae-
quent ysan^ ytan of great distoifaanw.
Pregents.
[Mar. I
the earth's revolution round the sun appear oppoaito in the two hem
spheres.
It might be suppcsed, as was done for the diurnal variation of magneti
dechnation, that the directions of motion being oppoaito in the two hem.
spheres, the amount of motion should diminish, and perhaps altogetht
disappear, at the magnctie equator. This docs not seem to be the c&i
far the annual law more than for the diumal law, the range of tb
mean oscillation from four years' observationa at Makerstoun being aboi
1''0, which is little different from that found for Trevandrum (0''33), th
difference of the directive forces being considered.
The Society then odjourned t
April letb.
!■ the Eastor Eecess to Thuradaj
Prtisnli rtcHveil March 5, 1874.
Transactions.
Berhn; — Konig!, Preusaiache Akademie der Wlssenaehaften. Ma
natsberieht. February to December 1S73. 8vo. The Academy
Florence : — R. Comitate Geologico d'ltaha. BoUettino. Anoo 187*
No. 5-8, 11, 12. 8vo. Firtnst. The Inatitutioi
London : — Society of Antiquaries. Archaologia. Vol. 5X111. Part 2
Vol. XLIV. Part 1. 4to. 1873. The Society
Nijmegen :— Nederlandsche Botanische Vereeuiging. Nederlandsd
Kruidkundig Archief. Verslagcn en MededeeJingen. Tweed
Serie. Deel I. Stuk 3. fivo. 1873. The Society
Vienna : — Anthmpologische QesellschaEt. Mittheilungen. Band HJ
Nr. 1-9. 8vo. TPi<ftl873. The Societj
Iteports, Observations, &c.
Calcutta; — Geological Survey of India. Memoirs, Tol. X. Parti
8vo. 1873. Pftlieontologia Indica. Cretaceous Fauna of Souther
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1874.] Prof. F. M. Duncan on the Nervout Syitem 0/ Actinia. 268
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" On the Nervous System of Actinia." — Part I. By Professor
P. Martin Duncan, M.B. Lond., F.R.S., &c. Keceived
October 9, \%7i.
1. A Notice 0/ the Invatigatiotit of Homard, Haime, Schneider and
Sdttcken, and others on the lul^eet.
MM. MUne-Edwards and Jules Hoime* wrote as follows in 1857
concerning the nenous attributes of the group of C<elenterata called
Zoantharia : — " They (les Coralliairea) enjoy a highly developed sensibi-
lity ; not only do they contract forcibly upon the slightest touch, but they
are, moreover, not insensible to the influence of light. Nevertheless, neither
a nervous system nor oi^ans of special sense have been discovered in them.
It is true that Spix described and figured ganglions and nenous cords
in the pedal disk of Actinim ; but the observations of this naturalist, so far
as the polypes are concerned, are not entitled to the least confidence.
" Some naturalists have supposed that the ' bourses calicinales ' of the
Actinite are eyes, and M. Huschke believes that certain capsules in the
trunk of Verelilla, which contain calcareous bodies, are the organs of
hearing. But these hypotbesea do not rest upon any proved facts."
* Hist. Kat. dea Corallisire*, vol. i. p. 11.
264 Prof. P. M. Duncan on the ■
In 1804 Huxley noticed that, with regard to the CiBleiit^rata, " a noi
voua system has at present been clearly made out only in the Ctem
Homard t, an admirahie observer, contributed to the histology of th
Actinozoa in ISol. He corrected Erdl'g mistake concerning the suj
posed striation ot the mnscular fibrilliD of the tentacles, and also Quatn
fago and Leuckart's notion concerning the rupture of the tentacular end
previously to the passage of water from them. Giving very good iUiis
tratious, he proved himself to be a very reliable invesligator.
Amongst other parts of the Actinozoa, he paid especial attention to tl
minute anatomy of the " bourses ealiciuales." These bead-like appendage
situated just without the tentacles in some genera, but not in all, u
&1bo called chromatophores and " bourses marginales ; " and their heautifi
turquoise colour had rendered them attractive to pre^noua anatomists
who had, as has already been noticed, giie-saed concerning their functioi
Homard determined that they were folded eleincnta of tlio skin i
■which the capsules (nematocysts) were enormously developed. H
stated that the thread of these gigantic nematocysts was seen with diff
culty. He noticed the transparency of some large cells in the bourse:
ouJ sLatod that, m hl^ opiuiDu, there "'as " suae phytiiulogical relation Ix
tween these little organs and the light."
Jules Haime (probably in 1855) examined the minute anatomy c
Actinia mesembn/antTujitum, and his colleague, Jlilue-Ed wards, quot«
him in the ' Hist, Kat. des Coralliaires,' vol. i. p. 240. The laments
young naturalist found out that the chromatophores bore, so far as thei
number is concerned, a decided numerical relation with the number c
the tentacles. He decided that they contained but few muscular fibrei
and had navicular-shaped nematocysfs, " diversement contoumee," wit
indistinct threads within them. However, he recoguiBed large tnuLE
parent cells and pigmentary granules in them. The nematocysts of th
chromatophores aro larger than those of the tentacles. He was evi
dently not satisfied with the data upon which these coloured masses wer
decided to be of importance as organs of special sense. In all probabilit
Haime was aware of Homard's work.
Kulliker and the German histologists added about this time, and latci
to the exact knowledge respecting the histology of the muscles, akii
endothelium, and tentacular apparatus, but no advance was made to
wanls the discovery of a nervous 8yst«m in the Actinia for man;
In 1871 the popular idea of the extent of the nen-ous system ii
* Huilo;, ' Elemonta of Coraparative Anatomy,' p. 82, See Dr. Grant, F.Bil. to
on Sero'e piUiia, Zool. Trans, vol. i. p. 10. Seo also ' A Munual of the Subkingdoi
dlentcrala,' by J. R. Greene. 18G1, p. 105.
+ "Sur Ees Actiniat," Ann. dca Sciences Kat. 1851.
i Sea-side Studiee, Eliz. and A. Agusiz, 1871, p. 12.
NervoHi Syittm of Actinia. S66
.AcHnui was ezpteased by Alex. Agassi£:t> "ho wrote :r-" NotwithBtanding
ita extrsordinary MoaitiTeneu, the organs of the senses in the Actinia
are very inferior, consisting only of a few pigment-cells accumulated at
the base of the tentacles ."
But in this year a great advance was made towards discovery by
Profs. A. Schneider and Botteken*. The first-named naturalist paid
especial attention to the development of the lamelhe and septa in Corals
and Actiniie, and hi» colleague laboured in the histology of Actinia
especially.
Working at a very great disadvantage, with specimens which had been
preserved in alcohol, Botteken produced a series of researches which
added greatly to the knowledge already granted to science by Homard and
Haime. So far. as they bear on the nervous system, the result of his re-
searches may be stated as follows : — " The bourses marginales " (cbroma-
tophoree) are undoubtedly organs of sense, and, indeed, compound eyes.
They are pyriform diverticula of the body-waU, standing between the
tentacles and the outer margin of the peristome ; they are constructed
after the fashion of a retina, and the following layers of structure may be
distinguished in them : — 1, externally a cutdcular layw broken up into
"bacilli" by numerous pore-canals; 2, a layer of strongly re&actile ,
spherules, which may be regarded as lenses ; 3, cones — hollow, strongly
refractile, transversely striated cylinders or prisms rounded at the ends ;
these have hitherto been confounded with urticating capsules (nemato'
cysts) : at the exterior end of each cone there is generally one lens, and
sometimes two or three may stand in the interspaces ; 4, a granular
fibrous layer occupying the interspaces between the cones ; 5, a layer
which is deeply stained by carmine, and contains numerous extremely fine
fibres and spindle-shaped cells, probably nerve-fibrea and cells ; 6, the
muscular layer ; 7, the endothelium, which bounds the perigastric cavity.
Actinia maembryanthmium was the species examined, and the diagram
(Fl. II. fig. 16) will explun the relative position of the layers.
Botteken could not determine the position of the pigment of tbe
chromatophorea from the alcoboIiEed specimens. An examination of the
minute anatomy of the tentacles of Actinia cereut, Ellis and Solander,
determined that the refractile spherules and large cones were to be found
on the tips of these organs.
Danat, in his popular work <m Corals and Coral Islands, appears to
accept the statements quoted above. He states that " they sometimes
possess rudimentary eyes ;" and elsewhere, " they have crystalline lenses
and a short optic nerve." He th^i observes:—" Tet Actiniie are not
* Sitiangsbericht der Obsriienuohan Qeaellsohftft Tui Ifitur- und Heilkunde, U&n&
1871 (OnUieStnictamof Actii)i»a]id Oorali). Translfttod for the Ann. and Hag. of
Nat Uirt. 1871, vii. p. 437, bjr W. S. DiU^ V.h.B. ko.
t Corals and Coml lalandi, bj JamM D. Dana, hLD., 1S72, pp. 41, 39.
known to have a proper nen'ouB eysteni ; their optic nervea, where they
exist, arc apparently isolated, and not connected with a nen'ous ring
Buch as esista in the higher Badiat« onimala."
II, A Description of tin Morphology of the Chromalophoret,
During the summer of 1871 the author of thiB communication was
examining into the minute anatomy of Actinia mesemhryanihemum, and
had the advantage of possessing hving specimens. Havbg satisfied
himself of thn general correctness of Efltteken'a admirahle work, ho
relinquished the inquiry until 1873, when he resumed it.
Every one who has endeavoured to anatomize one of the Actinifo inu^t
acknowledge the esccssive ditficulties which accompany the attempt.
The irritahiiity of the muscular tissues, their persistant contraction during
manipuhitioQ, the toufusion caused by the sbuudauce of different cellular
histological elements, and the general sliraineas of the whole, render the
minut-o eianuoation very troublesome and usuaUy very unsatisfactory.
Eeageots are useful for rough examinations ; hut when the most delicate
of the tissues are to be examined they must be floated under seai-water,
and this must be the medium in which they must he examined under the
> microscope. Carmine-solution, osmic acid, and spirits of wine in wenk
Bolutiona are useful after the natural appearances have been determined,
but they exaggerate some histological elements and destroy others.
Great care must be taken in making the thin sections, and no tearing
must be allowed; for it is of paramount importance, in endeaTouring to
trace the nervous system, that the relative position of parts should be
retained.
It is useless to rely on any observations made with object^glasBea
lower than -ji^-inch focus (immersive).
In examining the chromatophores. Actinia) with very bright-coloured
ones, and other specimens with these organs dull in tint, should be
selected. Fresh subjects should be obtained, and it is not Dcccssary to
kill them first of all. The blades of very delicate scissors should be
allowed to touch the desired chromatophore close to its base, and then aa
the Actinia commences to contract, they should be brought together
gently and without wrenching the tissues. By this method the chroma-
tophore will remain on the blades. Two or three chromatophores may
be removed, n4th their intermediate tissues, without injury to the animal ;
but, of course, the excision must not be too deep, or the endothelium will
be cut into.
A dropping-tube should be used to wash the chromatophore off the
blades on to a glass slide, where a drop of sea-water awaits it.
Sections are by no means easy to make, but they are best performed
under a power of 10 diameters with fine scalpels. The forceps must not be
employed, as it crushes the tissues. If possible, very slight pressoie
Nervous Sgilem of Actinia, 267
should be exemsed on the thin glass, which is to be placed very carefully
and wet over the object. After the examinatioD, carmine should be
added, or osmic-acid solution, 1 per cent, in strength ; but no results
con be relied on which are derived from the examination imder the
influence of reagents alone, as they modify the natural appe»ance
greatly.
So far as the chromatoph ores are concerned, my investigations took the
following course: — 1. Eotteken's researches on the alcoholized ^cfinta
were followed in recent specimens. 2. The tissues of the chromato-
phores, of their margins, and of the spaces between them were examined
in a lai^ specimen of a living pale-green variety of Actinut ituiembri/tm-
ihrntum from the Mediteronean. 3. The tissues of the chromatophores
of the Actinia mesembryanihtmum were again examined with a view to
explain the differences between M. Bdtteken's and my own results.
The rounded, free, coloured, external layer of a chromatophore was
carefully disengaged from the granular tissue beneath it, so that the
baialli of Botteken, the refractile corpuscles, and bis so-called cones
were separated from the rest. This turquoise-coloured film was floated
mtd carefully placed on a glass slide, the badllary layer being inferior
and on the glass, whilst the proximal ends of the cones were free in the
water. No thin glass was placed over the film, and an object^lass of
J-incb focus was used. The appearance presented under this low power
(by transmitted light) was very remarkable, for a great number of bril-
liant paints of light were seen surrounded and separated by dark opaque
tissue. When a j-inch object-glass was used, the appearance was less
striking, for the points of light were more diffused. No trace of an
object could be seen through the refractUe tissues.
The transparent and refractile tissues were the so-called bacilU, the
globular bodies and the " cones" already noticed ; and the tissue, which
was impermeable by light, consisted of the coIouring-matt«r in sm^ dull
grannies, cells small and round in outline and granular, and also the cell-
walls of the cones.
Sections through a chromatophore were made at right angles to the
point of the greatest convexity of the surface, and thin slices were floated
off carefully from the line of section on to glass slides. The slices in-
eluded (a) the coloured outside of the chromatophore, (h) the tissue
beneath it, and (c) some muscular fibres which limit the endothelium.
Sea-water was used as the medium, and a thin glass cover was applied after
the specimens had been examined with a low power.
Externally was the baccillary layer (PI. 11. fig. 15). Botteken de-
scribes this as a cuticular layer broken up into bacilli by numerous por^-
canals. Examined, however, in the fresh subject, this ext«mal layer con-
sisted of a vast multitude (^ small rod-shaped bodies, sharply rounded but
conical at both ends, very transparent, and resembling the smallest
S68 Prof. F. M. Duncan on the
nematocyata of the tentacles without the internal thread (PI, II. fig. 2).
These are placed sido by side, and the external rounded end of each is
separated by a small Hpaco from the terminations of its neighbours.
These ends are free and are in contact with the water in which the
Actinia lives. The rods are cylinders, and are separated from each
other by a very delicate film of protoplasm, in which are numerous
dark opaque granules and a few flat simple colourless rounded cells
(I'l. II. lig. 3). The inner ends aro shaped like the CKtemai, and
are embedded in the ne^t layer of tissue. Each of Ihuao bodies is
a simple cell filled with a transparent fluid. "When a thin film
of the surface of a chromatophoro ia removed and examined imder u
-ylg-iuch, the bacilli may be observed to crowd together over a layer of
large refractile cells. The thin glass cover is generally sullicieut to crush
down the bacilli, so that their sides may be seen as f bey rest in all kiuda
of positions ou the deeper cellular layer (PI. U. fig. 17).
The bacilli are not found universally over the chromatophores, nor do
they invariably cover the layer of large rofractile globular cells.
It will be noticed, on cxamiuiug eicised portions which include two or
three chromatophorcs and their intermediate tissue, that not only are
they marked on their surface by foldings of their superficial tissue, but
that between them there are others which are microscopic. These last
rarely have badlli. Moreover, in some parts of the margins of the chro-
matophores, other pigments are visible than the turquoise, and the ted
often predominates ; the bacilli are not usually present there.
Beneath the superficial layer of bacilli and their separating protoplasm,
which is faintly granular, there is some granular tissue with a few
small spherical cells containing granules, and the inner ends of the bacilli
are embedded therein (PI. II. fig. 3).
This granular tissue ia very thin, but it covers and dips down between
the large refractile cells, which form the next layer (PI. II. figs. 4, 13,
15, 16, 17).
These cells are more or less spherical ; the cell-wall is very thin, And
the contents are transparent, colourless, and refractile. Home have a
pale grey tint, and one or more extremely faint nuclei are attached to the
inner surface of the cell-wall. The ovoid shape is occasionally seen.
These lai^ cells, which transmit light so readily, are universally found
onthe chromatophorcs J and when there are bacilli upon them.the spherical
shape is common.
At the margins of ' the chromatophores, and where the red pigment
commences, these refractile cells assume much larger dimensions and more
irregular shapes. These refractile cells are, as has already been noticed,
embedded in a tissue of granular and slightly cellular protoplasm, and
this occasionally is differentiated into some peculiar structures,
jk Where there are no bacilli this granular tissue is increased in thickness
I
I
Nervoua Sytiem (^ Actinia. 269
ftnd becomes superfidAl ; moreover the granules tlieQ contribute to the
colour of the chromatophore, and probably the^ always do bo to a cert«Q
d^;ree.
The re£mctile cells are not inTariably confined to the layer abore tho
so-called cones of Botteken, although they are often thus limited in their
position, especially iE there are bacilli covering them. In part« of the
same chromatophore, where this apparently normal arrangement is seen,
and especially on the microscopic chromatophorea between the larger
kinds, the large refractile spherules are found between and in the midst
of groups of the cones (PI. U. fig. 16).
In the chromatophores there is considerable variety in the size of the
refractUe cells ; they appear to be developed from the small ceUs with
a circular outline, which contain a few dark granules, and which are
found in considerable abundance amidst the enveloping granular tissue
(PI. n. fig. 8).
The most striking of all the histological elements of the chromato-
phores are the cones of Etittekeu, or the nematocysts with imperfectly
Yiaible threads of Homard. They are divisible into three series : —
a. Elongated simple cells, cylindrical in shape, with rounded and
somewhat pointed estremities, consisting of a tough cell-wall which ia
capable of being bent without being broken or ruptured, and of colour-
less transparent contents which are rather viscid (PI. 11. fig. 5). They
are four or five times the length of the bacilli, and three times their
width. The cell-wail is faintly tinted with the peculiar colour of the
chromatophore. These elongated cells are not conical, nor can they be
really termed cones with any propriety ; when obsened through their
greatest length, or when the light traverses their long axis, the cell-wall
appears dark and the centre very refractile. They exist in vast multitudes
over most parts of the chromatophore, and also in the intermediate tissue
and its microscopic chromatophores.
/3. Cells of the same shape as " a," but the cell-wall is faintly striated,
the appearance being very distinct under a power of 2000 diameters
(PI. 11. flg. 6). These wJls are very numerous, and were noticed by
Botteken ; they appear in the same position, and often amongst the cells
with simple walls.
y. Cells of the same shape and size as " a and fl," with a well-deve-
loped thread within them, which usually has no barb (Fl. II. fig. 7).
These cells are common where there are no bacilli, but they occur here
and there in all parts of the chromatephore circle.
In some rare instances the " Botteken bodies" (for thus I would name
these remarkable cells) ore closely approximated, side by side, without the
interv&tion of any structure ; but, usually, there is a very thm layer of
granular protoplasm, containing small cells, between them.
As the bodies are cylindrical and more or less closely applied by their
270 Prof. P. M. Duncan on the
aides, there is more space between them ia some plaees than in otherB ; and
it is in these spots, where Ihe bodies eauuot come in direct conUct,that
their intermediate structures are elongated and filiform (PJ. U. figs, 9-
14), The fliiform arrangement of the gi-anulo-cellular protoplasm is often
branched, and a set of elongated masses may unite above or below the
bodies. The cells of this intermediate tissue are small and usiialiy spheri-
cal ; in one kind there is a largi^ refractile nucleus, but in the cohimonest
Tftrieties the cells Rim])ly contain granules. It is necessary to study this
tdsHiie, because of its close agreement to what I presume to be the nerve-
structure, in some, but not in the essential, points. This tissue is clearly
continuous with that which has already been noticed ns separating and
bounding the larger refractile cells outside the Eotteken bodies, and it is
continued amongst the small closely set granular cells which underlie
these interesting histological elements (PI. II. fig. !3).
The intermediate tissue binds together the bacilli ; for it is continued
upwards and between them, the large refractile cells (which I propose to
term " Haimean bodies '"), and the " fiiitteken bodies," and it becomes lost
in the cells upon which the proximal ends of these last rest.
It contains the granulnr alTiicturea which give, in the mass, the colour
to the chromatophore, and it ia evident that the Haimean bodies are de-
veloped from it.
The proximal ends of the Eotteken bodies retain their sharp and
rounded contour amidst the dense layers of small granular cells which
everywhere underlie them.
Those granular cells form a tissue through which light passes with
difficulty under the microscope. They are regularly placed in series near
the RStteken bodies ; but deeper they become less so, and then other
anatomical elements may be obaened between them and the muscular
fibres upon which the whole chromatophore rests, and which in their
turn limit externally the endothelium.
Ill, A Notice of liottekm'a flUcovery of Futifonn Cells and of the iUffeTe»t
appearanets of the Nervout Elemtnti now first observed in the "Ple^ri-
form Tmut."
Botteken describes these nervous elements as extremely fine fibres and
spindle-shaped cells, and asserts that they are probably nen'e-fibres and
cello. But he has not traced them in conjunction, nor have the fibres
been seen of sufficient length to anastomose.
I have found the fusiform bodies and their long ends — the fine fibres
mentioned above. Jloreover the connexion of these irregular-shaped
cells has been determined in these investigations, and the anaatompsis of
their processes and their connexion with parts of a plexiforra nervous
tissue also.
These structures are in the midst of a mass of viscous protoplasm.
I
Nervoui Sgsteot of ActamA. 271
graauleB, and granulu- cells, vhich merga gradually into the close layers
of granular cells under the £otteken bodies, and they transgress hero
and there on those layers.
The fusiform cells are numerous (PI. H, figa. 18-24), and may be di-
Tided into two kinds : — (a) Those with irregular shapes and short ter-
minal processes, which are prolongations of the cell-wall and aro rounded
off. These cells contain either highly refractile nuclei, or several nudei
with granular nucleoli. The fusiform shape is not invariable, and in
Flate II. fig. 20 a large cell twice the diameter of a Eotteken body
is seen amidst the granular plasm. It has a tail-shaped prolongation and
some highly refractile nuclei.
/3. Those which are rounder in outline, and whose projections are long
and c<mtinuou8 with those of others. The outlines of these cells are
soft, and without definite and sharp margins, and the colour is a very
pale blue-grey. They contiun one or more very distinct nuclei. Our
type, illustrated in Plate II. fig. 21, haa its cells rather wider than
a Botteken body, and they are connected by a process with sharply,
defined wells — the cell, with many nuclei, having a long caudal fibril of
a pale grey colour and rather sharp marginal lines which had suffered
disruption.
A second type has large spherical or elliptical cells, which do not have
processes passing out in opposite directions, but they are reatricted to
one part. Usually the cells have only one process, but somctimeB two
exist close together (fig. 22).
These cells are granular within and have very indistinct nuclei ; the
cell-wall is extremely delicate, and the whole is of a pale grey colour.
The fibrils of these cells are particularly connected with the plexiform
tissue. In FIat« II. fig. 22 there is a cell with two fibrils^-one is
short, for it dips down and is foreshbrtened, and the other is very long ; it
bifurcates, and one end joins a rounded mass of the plexus, and the other
the nigged fibrillar part.
In Plate II. fig. 24 a cell with one fibril is shown. The fibril swells
slightly, and then passes down to join a transverse fibre belonging to the
plexus.
The plexiform tissue is probably continuous around the Actinia beneath
the chromatophores, for it is foimd between the cireular band of mus-
cular fibres and every ehromatophore. It consisfs of an irregular main
structure and of lateral prolongations, which either anastomose with the
fibrils from the Fusiform and more spherical cells, or nxe directly con-
tinuous with the cells (fig. 23).
The main structure resembles, in its iudiBtinctness of outline and its
pale grey colour and indefinite marginal arrangement, the fibre of the
sympathetic of mammtds, but it is less coherent and smaller. The
usual appearance (Plate II, fig. 23) is that of a grey film with definite
branches, and the whole has few granules here and there and a rety few
nuclei. It is intimately ftssociated with the surrounding cell-atnicturM,
but they may be separated by accident or compression. Here and
thero the structure eulargi.-a and a gangliou-lJke cell is seen (Plate II.
Sg. 22).
I have traced this structure almost across the whole field of the micro-
scope in some sections.
It appears that this portion of the nervous system of Actinia (namely,
the fuaifonn and spherical cells n-ilh fibrils and the plexiform structure)
is distinct histologically from the fibrillar and cellular structures amidst
the Haimean aud Bottelcen bodies. These structures are connectiTO and
developing ; but it must be remembered that it is possible for both seriea
to come in contact in the midst of the layers of granuhir cells which
nndorlie the Biitteken bodies.
rV, Ei-am!nation into the Phijuologwal Htlation hetwtfti iht Chroma-
topliores, the Nen'ei, and Light,
The question arises, Are these nerves of special seneo ? MM. Schneider
and Kutteken answer that the small portion of the nervous arrangement
they descrilietl, i. e. the riifliform borlip.s and their fibrilfi, are optic nerves.
They are satistied with the physical arrangement of the bacilli, Uaimeaa
and Botteken bodies, aud the nature of the colouring-matter imitating
tliat of an brgao of nsion.
The discovery of the anastomosing fibrils and the plexiform arrangement
favour this theory ; but there toe reasons to be considered which throw
much doubt on the views of the distinguished investigators. All Actinia
have not chromatophores, and closely allied genera may or may not
have them. Thus, amongst the Actinia with smooth tentacles, there is
a group with non-retractilo and another with retractile tentacles :
amongst those with non-rctractilo arms arc the genera Antmimia and
Eumenidet without chromatophores, and Coviactis and Ceralactis with
them; amongst the Actinia with retractile tentacles are Actinia with,
and Paraetit without, chromatophores.
Amongst the tubercular division, the genus Phymactis has chromato-
phores, but its close ally Ccreue has them not.
Whatever may be the value of this classification of the Actinia, it is
quite evident that to group together those niih and ^lithout chromato-
phores in separate divisions would be the reverse of producing a natural
arrangement. It is therefore diiTicuIt to belieie that these ornaments,
with something resembling an optical arrangement, can be the seat of
special sensarion.
MM. Eiitteken and Schneider have obsened the large refractile
Haimean bodies in the tentacles, nnd, as will be noticed further on,
I have found them of enormous size in the peristome.
They are surrounded in those places, but not covered, with pigment-
■■ill* -nd granaleB, and are situated just beneath the neimaf ocyst layer in
Nervous Syitem ^Actinia. 273
tbe tentacle, and beneath tt correeponding la^er, or one of badlli, in the
periatome. I hme faUed to rec<^ize any nervous elemente in the
tentacles save the fudform bodies, and there are none in the peristome
except these irregular cells.
Again, the Haimean bodies are found in the chromatophorcB, in some
places, amidst the Botteken bodies, separating them.
Nevertheless it is true that light falling on the surface of an Aettnta
will reach further into its structures where there ore Haimean bodies,
and further still if the Bottelten cells underlie them. ^Vhe^o there ii
no pigment intervening between the bodies when placed side by side, or
between the Sdttoken cells, a difhised glare of light would impinge on
the grsnulo-cellnlar layer below them, in which the nerves ramify and
the nerve-cells exist. But when the pigment-granules and cells exist,
they break up the general illumination and confine it to a series of
separate bright rays. Each of them is brighter than the corresponding
space of diffused light ; and it would appear that the bacilli, the Haimean
bodies, and the Eottoken cells in combination, concentrate light.
Two of three badlh are placed side hy side and behind each other over a
small Haimean refractUe spherical cell, and perhaps twenty or more covers
large cell (PI. H. fig. 15). TTsually a Haimean body is placed immediately
over a Botteken body ; hut, as Botteken has pointed out, this is not an
invariable arrangement, for some cover the spaces between and over
them. The refractibility of the fluid contents of the Haimean bodies
and Botteken cells appears to be the same ; but the elongated form of the
last^mentioned structures may act upon light as if their internal fluid
were more viscid.
In every instance there is a more or less opaque tissue between the
proximal end of the Botteken body and the nerve-cells ; and, moreover,
the delicate protoplasmic layer, which is slightly impervious to light,
surrounds the Haimean bodies.
In my opinion the Haimean bodies, wherever they exist, carry light
more deeply into the tissues than the ordinary epithelial stmctnres.
This is also the case with the bacilli and Bdtteken bodies, even when they
exist separately and with or without the Haimean bodies. There are
three ordinary constituents of the skin, and tbrough their individual gifts
and structural peculiarity they place the Actinia in relation with light.
"When they are brought together in this primitive form of eye, they con-
centrate and convey light with greater power, so as to enable it to act
more generally on the nervous system — probably not to enable the
distinction of objects, but to cause the light to stimulate a rudimentary
nervous system to act in a reflex manner on the muscular system, which
is highly developed. The Actinia, therefore, may feel the light by means
of the transparent histological elements when they are separate and
constitute integral portions of the ectodenn; butthis sensation thU be in*
274
Prof. P. M. Duncan on the
temified when the thres kinds of cells ore pUiced iu such order osb
been obsen-ed in tha chromatophoreB.
The evolution of an eye, which can distinguish outlines, shadowB, and
colours, probably took the p&th which ia thus faintly indicated in th^ J
Actinia, which doubtless has an appreciadou of the difference betweea I
light and darkness.
V. O.i Ihe Nerves of the hose of Actinia mesembrj-anthemum.
A large specimen of a pale green variety from the Meditcrraneitn was
examined.
The base beiug free and expanded, a rapid incision cut out a tTiangidar
piece comprehending the ectothelium, the muscular layers, and the
mucous endothelium. The apex of the triangle reached the centre o£
the base of the Actinia, and the base of the triangle, which was covered,
corresponded with the basal margin of the animal.
Sections were made parallel with the- original aspect of the base ot
the Actinia, and then some others at right angles.
The histological elements were studied separately and compared, so
that the following tissues could be distinguished readily ; —
1. A fibrous- looking tissue like ordiuary white filirous tissue with
dark nuclei, to which the muscular fibres are attached and from which
they originate.
2. A dense layer of muscular fibres, or rather fibrils, which originates
at right angles to the fibre of the fibrous tissue. Each fibril is refractile
aud nucleated. £ach is separate from its neighbours, and hes in the midst of
granules and small cells which contain granules, all being highly refractile.
In some places the fibrils are gathered together in masses, so as to _leave
areola: between them.
3. Large muscular fibres in contact laterally, so as to form a thin
layer. Each fibre is long, broad, has several pale elongate nuclei and a
distinct lateral dark line. There are no striae.
4. The elements of the endothelium and ectothelium, which, as they do
not bear on the immediate subject, will be described in a future memoir.
The object of the investigation being to discover some trace of a
nervous system, which was presupposed to resemble somewhat the traces
observed below the chromatophores, the necessity of becoming familiar
\nth the fibrous and muscular tissues, so as to decide uhat was uot
muscle and fibre, is apparent.
I have not found any isolated fusiform cells amongst the tissues of the
base ; hut under the endothelium, and also between the layers of muscular
fibres, there are structures which I feel disposed to believe must belong
to the non-ous system. 1. They are in the position of nerves. 2. Their
structure is not that of muscle or fibre. 3. Their structure resembles,
in some instances, Ihe plexiforra tissues beneath the chromatophores.
I
Nervous Syitem o^ Actinia. 275
Tha nerrous Btructures are found to present three chftncberiitio
sbapea : —
1. A thin layer of muscuUr fibriU of the BUiall and separate (seis
2 above) kind, with veil-defined dark nuclei in them, was examined.
The whole was rerj transparent and well defined under the ,^inch
objective.
Underlying this layer, and extending on either aide beyond it( so ■■
to appear in one of the meshes between groups o£ these fibrils, was a
ramified pale grey tissue, which was less pervious to light than the mus-
cular fibrils (Fl. m. fig. 26). SwoUen in one part and faintly granular
throughout, it had its margins very faintly visible. It was flat, and had
a definite resemblance to the widest portion of the plexus already men-
tioned.
2. A lai^ section of muscular tissue was examined. It consisted of
one layer of lat^ muscular fibres (see 3 above) in close lateral contact.
Bunning obliquely over the layer was an irregular but continuous cord
ramifying here and there, the branches breaking up into fibrils. In one
part the cord was swollen (Fl. HI. figs. 26 & 27). A second ramification
passed from the opposite end of the field of the microscope and broke up
into ultimate fibrils, and in this structure there was a fusiform cell.
Careful manipulation separated a portion of the upper cord &om the
muscular fibres, but a part of it evidently dropped down amongst them.
3. A layer of muscular fibres of the same kind as those just mentioned
was examined. It was marked, as usual, with the lat«ral dark lines and
pale elongated nuclei.
Three long and irregular fibres passed more or less obliquely over the
muscular tissue (PI. III. figs. 28-30). They had distinct lateral or mai^
ginol lines, were swollen out in several places, and their texture was faintly
granular.
I beUeve that these fibres were continuous with the fine twnificationi
of the plexiform arrangement just described.
4. Above the moscular layers, and under the folds of the endothelium,
I found an inosculating series of ramificatjons arising from a common
cord. It was situated upon the layer of muscular tissue, with small and
separate long fibrils.
The structure was faintly granular, pale grey in colour, with funt
outlines, and was swoUeu in some places : it covered a considerable por-
tion of the field of the microscope; and portions of it had a close resem-
blance to the ramifying structure mentioned as having been observed
below the muscular layer (Fi. III. fig. 31).
The multiplication, if it be justifiable, of these structural elements in
the other segments of the base which were not examined would give a
fair notion of the plexiform arrangement of the basal nervous tissue. I
presume that it consists of a reticuhite structure beneath the endothelium,
which sends large branches between the vacuities of the moat de^ica^
vol,. XXII. ''-
276 Prof. P. M. Duncan en Ihe Nervous iyttem of Actinia.
muscular layer, and which communicatefl with a ramifying tissue in
tact with the other muscular layers, and that this eads in long fibres
which supply the wide fibres o£ this last^mentioned layer.
The diffused nature of thia nervous tissue is what might be anticipated
would be found in annuals possessing such general irritability of tiaaue,
and probably its function is lo assist in the reficx movements of ths |
1, and to produce expansion of the disk on the stimuloa of li^t.
DESCBIPnON 05 THB PLAIBS.
Pwia n.
Fig. 1, irbioh ]» »a outline of a ohromatophore, witb two >msU onea cIom tc
mugniflcd 10 diamslen; all the rnt aredratm from nature under the
oirying-power of a j^j-inch iuimorsion lens and a, medium ejepiece.
Fig, 2. Bacilli,
Pig, 3. Qranular and cellular pratoplaam bettrsen baeiUi
Fig. 4. Large refradilo cella. Haimean bodiea.
Fig. 5. Tjpa a of a Botteken bod/.
Fig. 6, „ & „ .,
Fig, 7. „ 7 ,. „ „ with a thread.
Fig. S. Qranular and cellular tjasue between the Haimean bodiea.
Fig. 9. Same kind of tinue in oontaot with a Botteken body.
Fig. 10. Some oells with refivctile nuclei in the tissue.
Pig, 11. Portion of tisaue from amongst the Bottekon bodies.
Fig. 14. The same, with a forked end.
Fig. 12. Three portions of intermediate (issue ending in the la/er of granolar oella
which underliee the Rotteken bodiee.
Fig. 13. Haimean and Botteken bodiee and the intermediate tiaaue in position.
Fig. I&. Adiagnim, but verj close to nature, of the reUtire position of the hiitologiea]
elements of the ohromatopboree.
Fig. 16. Haimean and BoUeken bodies intermingled.
Fig. 17. Humean bodin surrounded bj pigment-oslls, and with bacilli flat opan them,
owing to pressure.
Fig*. 18 & 19. Fusiform nerre-odls.
Fig. 20. A nerve-oell.
Fig. 21 . Nerre-cells connected and with flbrea.
Fig. 22. A spherical nerre-oell with processes joining the pleius.
Fig, 23. Ramifications of the plerifonn cord.
Fig, 24. Ji'erre-cetl and fibres.
Flati hi.
Fig. 25, Nerve in relation to the small muscular fibrils of the base.
Pig. 26. Nerve rami^ing and supplying wide muscular fibre.
Fig, 27. A loop of nsrrous fibre.
Fig. 28. Terminal end* of the pleius passing over muscniar fibre.
Figs, 29 & 30. The same, more highly magnieed.
Pig. 31. The plexu* under the endothelium.
^'
1.
n
ft
l>roc.8^. Soc. Vol.XM PL 1
1 i ( ^'"
j i If
1874.] ' On the Pneumatic Actum accompanying Articuhdion. 277
Apnl 16,1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
!• '^ On the Pneumatic Action which accompanies the Articulation
of Sounds by the Human Voice, as exhibited by a Recording
Instrument.'* By W. H. Barlow, F.R.S., V.P.Inst.CE.
Received February 23, 1874.
All articulated sounds made by the human voice are accompanied by
the expulsion of air from the mouth ; and in a series of articulated
sounds the air is ejected in impulses which vary in quantity and pres*
sure, and in the degree of suddenness with which they commence and
terminate.
It appeared to me that it would be interesting and probably useful, as
tending to elucidate the process and effects of articulation, to construct
an instrument which should record these pneumatic actions by diagrams,
in a manner analogous to that in which the indicator-diagram of a steam-
engine records the action of the engine.
In considering a suitable form of recording instrument, the conditions
to be met were : — first, that the pressiues and quantities were very vari-
able, some of them being extremely smaU ; and, secondly, that the im-
pulses and changes of pressure follow each other occasionaUy with great
rapidity.
It was therefore necessary that the moving parts should be very light,
and that the movement and marking should be accomplished with as Uttle
friction as possible.
The instrument I have constructed consists of a small speaking-
trumpet about 4 inches long, having an ordinary mouthpiece connected
to a tube ^ an inch in diameter, the other end of which is widened out
so as to form an aperture of 2| inches diameter.
This aperture is covered with a membrane of goldbeater's skin or thin
gutta percha.
A spring which carries the marker is made to press against the mem-
brane with a slight initial pressure, to prevent as far as practicable the
effects of jar and consequent vibratory action.
A very light arm of aluminium is connected with the spring and holds
the marker ; and a continuous strip of paper is made to pass imder the
marker in the same manner as that employed in telegraphy.
The marker consists of a small fine sable brush placed in a light tube
of glass -jl^ of an inch in diameter. The tube is rounded at the lower
end, and pierced with a hole about i^j^ of an inch in diameter. Through,
this hole the tip of the brush is made to project, and it is fed by colour
TOL. XXII. z
278 Mr. W. H. Barlow on the Pneumatic Action [Apr. 16,
put int-o the glaaa tube in which it is held. To provide £or the escape
of the air passing through the iitstrument, a small orifice is made in the
side of the tube of the speaking-trumpet, so that the pressnre exerted
upon the membrane and its spring is that due to the difference arising
from the quantity of air forced into the trumpet and that which can be
delivered through the orifice in a given time.
There being an initial pressure upon the membrane to prevent vibra-
tory action as before deaoribed, the strength of the spring and the sine
of the orifice had to be adjusted, eo that while the lightest pressures
arising under articulation could be recorded, the greatest pressures
should not produce a movement exceeding the limit of the width of the
paper.
It will be seen that in this construction of the instrument the sudden
application of pressure is as suddenly recorded, subject only to the modi-
ficationa occasioned by the inertia, momentum, and friction of the parts
moved. But the record of the sudden cessation of pressure is further
affected by the time required to discharge the air through the escape
orifice.
Inasmuch, however, as these several effects are similar under similar
circumstances, the same diagram should always be obtained from the
same pneumatic action when the instrument ia in proper adjustment ; and
this result is fairly bomo out by the experiments.
We are thus enabled to trace to what extent the pneumatic action
varies with different articulations ; and it will be seen that although there
are instances in which considerable differences in sound do not make
much ^-ariation in the diagram, yet, as a rule, every change of sound or
articulation produces a change in the diagram, and that there are pneu-
matic actions revealed hy this instrument which are imperceptible to
ordinary observation.
Before referring to the peculiarities of the diagrams, it may be desir-
able to say a few words on the quantities of air used in articulation.
On reference to medical authorities, it appears that the average
quantity of air expelled in one respiration is estimated at 40 cubic
inches, and that the total air-space of the lungs is estimated to aven^
110 cubic inches.
I have ascertained by experiment that a balloon made of goldbeater's
skin, whose cubic content when full was 523 cubic inches, was filled
with twelve ordinary respirations, or at the rat« of about 44 cubic inches
for each respiration.
Also that by filling and emptying the lungs as completely as pr&cti-
eahle, the 523 cubic inches could bo filled with six reapirotions, or about
88 cubic inches for each respiration.
I also made the following experiment to ascertain the average quantity
of air used in pronouncing syllables.
Using the same bollooa and speaking into an elastic tube commuoi-
1874.] accompanj/u^ the ArtieulBtion o/ the Hmmam Voice. 270
eating with it, I read fnm a book until the ballocm wsa filled, taking cara
to close the elastic tube when it wu neceesiuy to take breath.
The resultfl were as follows : —
Time nquind. Va. of i^lkblM. Oubie inobea.
84 seconds 353 623
84 „ 353 623
Fhnn another part of the book 90 „ 364 623
„ „ 95 „ 364 623
Mean 86 „ 359 623
Showing tu average of about 1 j cubic inch of air for eadi Billable, and
rather more than four syllables per second, including stops.
Without stops, from five to six syllables can be pronounced in a second.
The lungs appear to be capable (A exerting considerable pressure in
the expulsion of air ; but distinct articulation becomes difficult agunst a
pressure of 2 inches of water, and I could not pronounce anj words
against a pressure of 4 inches, without considerable exerti<m.
The following diagrams made by the instrument show the d^ree of ao-
cordauceobt^ed when the same words are repeated by the samespeaker: —
One of the first features manifested in using the instrument is the
action produced by the silent diacharge of air frcnu the mouth, after a
syllable or word or a sentenw it pnmounced. This silent discharge
x3
38a Mr.W. H. Barlov On tfu: Pneumatic Action [Apr.lO^
appears to depend on the force required in the last syllable, if more tlian
one are consecntiTely uttered, and is moat developed in tiioee syllablea
terminating with the consonants termed " Dsplodents," vbetber with
or without tite silent vowel E after them.
This effect is exhibited in fig. 1.
1874.] aeerni^anyiAg the Articulation of the Hwnan Voice. ^1
In theae diagrams the part marked d is the ailent dischat^, and its
appeamnce in the diagram is under the control of the will ; for hy holding
the breath immediately aft«r pronouncing the word, this part of the
diagram can be altered and the discharge of air postponed or let off
gradually, as exhibited in fig. 2.
If, instead of t«rrainating with the " Exptodent^," another syllnble be
added to each word, making them terminate with conaonanta of softer
•ound, the air which would have been silently discharged is used to form
the syllable added, and the subsequent silent discharge is very much
diminished (see fig. 3).
There are other silent or, rather, insensible actions which occur within
certain words, as is exhibited in the difierences between the word
" Exeommvnitate" and the syllable " Ex" and the word " Communicate"
pronounced separately.
Communicale.
Eioommuniote.
Here it is seen that the part p, which is the secondary sound of the
•yllable "Ex," becomes compressed, its length being shortened and its
height increased ; so that althou^ nearly insensible as regards sound, it
becomes developed into the form p', and constitutes the most prominent
feature of the diagram when the whole word is pronounced.
Some words are shortened when a syllable is added. This eSect is
strongly exhibil«d in the word " Strettgthtn " as compared with " Strength."
" Strength " is, I believe, the only word of one syll^Ie in the English
language which contuns seven consonants, all of which are pro-
nounced.
»3 Mr. W. B. Barlow « tke pHemmmHe Aetitm [Apr. Ifl,
The diagnuns are u follow* :—
Afl a test of the npidity of odaon of the inBtnimoit, I bxn tued Hb
old nnraery words, " Ater P^ jnat«d ajweit of pideUd ptpptr'
This is Bud at the nte of six syUiUes p«r Mcond ; and ft w31 In
observed that there are two principal upward and two principal dowiH
ward moTements to many of the syllables, besides other oubsiitiaiy
actions.
Peter Piper picked & peak of ptokled pepper.
Another curious test is the continuous soond of the rough B.
The upper diagram ia pronounced by myself, the lower one by my eon.
There is a very marked difference in the quantity of air used and the
degree of compression in different words and syllables.
1874.] accoj>g>aai/inff the Articulation of the Human Voice. 288
The difference in the action between whispered sounds and tboM
spoken loud ie not bo great as might hare been expected.
384 Mr.W. H. Bariow m thePuemmatie Aetiut {Apr.Ifl;
Tbe TOrd used in the four foUoring biali U " /iiwwjwJiwMiWftjy.'*
The flnt ii vhispend Eimtlj,
The second is whiapared f orciUy,
The third is spoken at the orduuiy tone of Ute nin^
And the fourth ii spoken loudLj,
In ordnr to tihow the manner in which the diagrams oE words Ste
nflected when spoken together, I giTe four linea from Uohenlinden and
the words separately.
By torch and tnimp^t fa»t HmTeil,
Each Horxomsn drew hi* bnttip bUde :
And furioiifl e*i>rj nhari;<>r npiKlied.
To join tlie drmdful rpTplry.
886 Mr. J. H. N. HennMcy m [j^. li.
It vQI be obserred th&t the diagmoB of the npantte wordi, »M-.h«ngfc
tbey become modified whea gronped together, aze more or leu dueent-
iUe in the lines contiiiuoDBlf ipokea ; and ibe nmiluitj of ■oimd at tibe
tenniiution of the first three linea, whidi oonitatatefl tiie riiyme of tlie
verse, is represented in the sinularity of form, mr in the chaaeter o{ &m
fonn, of the t«rminAtions of the diagnma of theae three linea.
The Bubject might be pnraaed mooh farther hj showing the diorama
of Hm same words spoken bjr di&mnt individaals, the ontlinea produced
by the words and senteuoes of other langoages, &a effect prodnmd bj
change of accent, Ac
Tiiy object, howerer, has not been to porsae tiie subjeot into minnts
detail, but to show that the actienlation of the human roice is a«om^
panied by definite pneumatic actions, and that those actions, mamf <tf
which are insensible to ordinaiy obaerration, are capable <£ being
recorded.
11. "NoteonthePeriodidtyofBain&a'* ByJ.H.K.HnnnnBr,
Esq., F.R.A.S. Commniucated hj Prof. O. G. Stoebb,
Sec.R.S. Received February 24, 1874.
1. Interested in the inquiry proposed by Mr. Meldrum, as to whether
rain&ll varies n-ith the sun-spot area, I examined the register kept ftt the
office of the Superintendent of the Great Trigonometrical Survey of India,
and am enabled, through the courtesy of Colonel J. T. Walker, B.E., to
communicate the results. These are probably not devoid of peculiar
interest, from the abnormal conditions presented by the stations of
observation, which are far inland, and on, or adjoinisg, lofty mountains,
as appears frcnn the following brief descriptions.
2. MuBSOorie station is on the southernmost range of the Hlm^aya
Mountains, Ut. N. 30° 28', long. E. 78° 7', height 6500 feet ; this range
rises suddenly and forms the northern bound^ of the Dehra Doon (or
Dehra valley), which is some 18 miles wide and 40 miles long, and is
bounded to the south by the Sewalik range of hills, about 3500 feet high.
Dehn station is 2200 feet high, 10 miles south 6f Mussoorie station, and
in the Dehra valley.
3. Owing to the absence of the observers in the winter months from
Mussoorie station, the runfaU is not recorded there during that period ; '
this, however, is of little consequence to the inquiry in hand, for the total
annual fall occure almost entirely in June, July, and August. I
accordingly give in Table I. the total fall at; Mussoorie between
May 1 and October 31 of each year ; and in order to make these totals
comparable at the two stations, if desired, the fall for January, Febnutij,
March, April, November, and December is excluded from the Dehm
totals ; this quantity excluded may be set down at some 6 indtes, or only
1874.] the PeHo^eUy of BamfaU. 2^7
some 7^ per cent, of the atumal fall. Excepting five fears at Sehra and
two at MusBoorie, aU the obaerradona have been taken under my own
Bupermtendence, so that 1 can vouch for their accuracy. Bejecting
decimal places as redundant, the rainfall is as follows (in inches) for 20
years at Mussoorie and for 13 years at Dehra :—
Table I.
Sun-ipot am*.
(H>7lto
Oot31).
Bainbll, m mches, at
iUtion.
Dehra
■taliaii.
«i.,»™
1864
1856
856
867
858
859
860
1861
1862
1863
1864
1866
1866
1867
1868
1869
1870
ffi
187S
101
86
93
88
85
78
66
141
SI
82
76
81
82
61
80
84
83
S3
103
110
S*
er
75t
70
45
65
84
114
83
63
4. Adding to the &1I in the epochal year (i.«. woTiiwiiTw or iriinimnn^)
the fall for one preceding and one snoceeding year, we shall get what
may be termed Aree^ear mmi ; similarly, by including two yean on each
side of the epochal year, we find jfv^-yMr mmtXi &a lesolts ate as
follows: —
Table n.
S-jmt tamt, in incliet.
5-j<ar nima, in inolua. ]
DihM.
MoMDorie.
Dehra.
26T
as6
224
S47
190
asi
453
464
363
381
332
409
* Ttiea from a pap«r in ' JltXan,' 187% Daaeiober 13, pa^a 100, hf If orman
Loekjer, Bm]., F.B.S., Ac.
t Site of rain-gaogB ihifted.
X •HatiiM.'lSTi^S
S88 Oh the Periodieittf of Rautfall. [Apr. 18,
Ifohrithstanding the exceptional localities of tbe statioiiB, the abore
reaultB are generally in keeping with the Meldrum tbeor; : the Dritn
obserrataona for 1860 and prior yean are unfortunately waotang; hut it
will be seen in Table I. that heavy falls occurred in the two years soo-
ceeding the epochal year 1860.
5. It may, howerer, be questioned whether stations inland are ineligible
to test the theory under notice. No doubt far more rain falls on certein
porta of the globe than on othera, and Mussoorie and Dehra are included
in the former : but a large rainfall is in fact a recommendation, presenting
as it does a large measure of the periodicity in question ; bo that stations
under this condition appear highly eligible unless the rainMl is subject
to abnormal fluctuations, apart from the supposed influence of sun-spot
area; indeed, were it practicable to measure the total runfall on the
whole globe, the total results would present the most effective argument
for periodicity. Projecting the factit of Table I., with the help of ordinate*
and absdssie we obtain tbe appended diagram, where I am unable to
introduce, in lieu of the year, numerical values of 8un-spot areas from
n-ant of complete results, such as those obtained by Messrs. De La Bue,
1874.] Dr. W. Roberts on ftojrenerif. 289
Balfour Stewart, and Loewy. BecognlziDg the aun as the governor of
our syetem and the source of terrestHal heat and light, it appears certain
that at least some of the drcuiuBtances attending our globe are directly
or indirectly the resulte of solar conditions, of which we can read but too
few, and interpret still fewer rightly. In the present instance we see
that, aa is other curres, a certain rainfall maximum may be Utt than
minima not immediately preceding or succeeding ; and this alone suggests
the desirability of comparison with actual magnitudes of sun-spot areas ;
but the introduction of this more accurate test would doubtless prove a
waste of time, unless the appronmato relation at present under view can
be mainttuiied.
III. " Studies on Bic^^esis." By William Roberts, M.D.,
Manchester. Commiinicated by Hbnby E. Roscoe, F.R.S.
Received March 3, 1874.
(Abstract.)
The object of the investigation is to inquire into the mode of origin of
Bacteria and torul<ud vegetations. The inquiry is divided into three
sections.
Section 1, Onihe ttmliattion by ht^ of organic liqmdt artd mixtures.—
When beef-tea or a decoction of turnip is boiled for a few minutes and
afterwards preserved from extraneous contamination, it passes into a
state of " permanent sterility,"
This state is characterized by loss of power to originaU organisms with
conservation of tbe power of nouruAtn^ and promoting the growth of
orgamsms.
All organic liquids and mixtures seem capable of b^ng brought to this
state I^ exposure to the heat of 212^ F. ; hut the length of time during
which exposure to this heat is necessary to induce sterilisatioh varies
greatly according to the nature of the materials. Ordinary infusions
and decoctions were st«rilixed by boiling for five or ten minutes ; but
milk, chopped green vegetables in water, pieces of boiled egg in water,
and other mizturee were not sterilized unless the heat was continued for
twenty to forty minutes. Hay-infusion was sterilized, like other infu-
sions, by boiling for a few minutes ; but when the infusion was rendered
alkaline with ammonia or liquor potaass, it was not sterilized except
after an exposure to the heat of boiling water for more than an hour.
Sometiinea it germinated after two hours, and once after three hoars fA
such exposure.
There appeared to be two factors of equal importance in the induction
of sterilization — ^namely, the degree of beat and the dunUion of its appli-
cation. These two foctors appeared to be mutually compensatory in sudi
fashion that a longer exposure .to a lower temperature was equivalent to
390 Dr. W. Roberts on Biogenesis. [Apr. Id,
a shorter exposure to a higher temperature. For example, speaking
roughly, an exposure for an hour to a heat of 212° F. appeared to ba
equivalent to an exposure for fifteen iiiiDiit«s to a heat of 228° F.
Sbctios n. On the capahility of tht twnivil tUsnes antljuica to generala
Bacteria and Torulte without extraruout inftetion. — The follovring sub-
stances were examined : — egg-albumen, blood, urine, bliBter-seram, milk,
grape, orange- and tomato-juice, turnip and potato. These aubstancoB
were conveyed into previously prepared sterilized bulbs and tubes, which
were hermetiffllly sealed at one end and plugged with cotton-wool at tha
other end. Wlien the several steps o£ the experiment were quickly and
dexterously performed, the risks of extraneous contamination, although
not altogether avoided, were reduced to small proportions. The bulba
and tubes thus charged were afterwards maintained at a temperature
ranging from 60° to 90° F., and were finaUy examined at periods varying
from four to ten weeks. Out of 90 experiments performed in this way,
67 preparationa remained barren and 23 became ferHle. When the ideal
conditions of the experiment could be carried out in approximative per-
fection, as with urine, hlister-serum, orange-, grape-, and tomato-juioe •
(34 experiments), the preparations, all save one, remained barren ; but
when the rjaks of extraneous infection were (from the mechanical dif-
ficulties) obviously greater, as with blood, milk, turnip, and potato, the
proportion of fertile preparations was considerable, though even with
l^ese (except in the case of milk) the barren preparations were in a Ui;ge
majority.
The experiments seemed clearly to lead to the condusi<»i that the
normal tisBnes of plants and animals were incapable of breeding Bacteria
and ToraUx except under the stimulus of extraneous infection.
Sbttiob in. On the bearing of thefts adduced in the preetding mo-
tioM an the origin of Bacteria and Torulte, and on the real explanation of
tome of the alleged eases of Abtogenests. — Seeing that organic liquids and
mixtures sterilized by heat, and the normal juices and tissues, continued
permanently barren under the most favourable conditions of air, moisture,
warmth, and light, so long as they were preserved from extraneous con-
tamination, and seeing that the admission of ordinary air or water into
contact with them was invariably followed by germination, it was im-
possible to avoid the conclusion that ordinary air and water contain, in
addition to their proper elements, multitudes of particles capable of pro-
voking germination. The exact nature of these particles may be «
matter of dispute, but the reality of their existence is not doubtful ; nor
is it doubtful that the ordinary and common development of Bacteria sad
Torvjof is directly due to their agency.
The greatest difficulty hitherto encountered to the general acceptance
of the panspermic theory has been the appearance of Bacteria (without
the possibility of fresh infection) in certain liquids which have been
exposed for a considerable time to a boiling heat. Only two explanati<»u
1874.] On the Ctrcuialion of the Blood. 291:
of this fact Beem poiuble — either germs preexiatuig in tbem hare snr-
vived the heat^ or the organisms have arisen in them abiogenically.
These alternatives were subjected to two series of test experiments. In
the first series it was proved directly that there exist in ordinary air and
water particles which preaerre their germinal actiTity after being boiled
for five minutes in previously sterilized liquids. The second series of
experiments showed that, in the extraordinary increase of resistance to
steiilization by heat exhibited by alkalized hay-infusion, the action of tJie
alltali is to heighten the surviving power of preexisting germs, and not
to exalt the abiogenic aptitude of the infusion itself.
The issue of the whole inquiry has been to fully confirm the main
propositions of the panspermic theory, and to establish the conclusion
that Bacteria and ToruJce, when they do not proceed from visiUe parents
like themselves, originate from invisible germs fioatdng in the surrounding
aerial and aqueous media.
Nevertheless the author is nnable to withstand the impression that this
general and conunon mode of origin is poanbly Bupplemeuted, under
rare conditions, by another and ui abiogenic mode of origin. The facts
on which this impresnon rests are comparatively few. They consist in
certain instances of greatly retarded germination of Bacteria in liquids
which had been expc»ed to a boiling heat, and in two very remarkable
instances of the growth of fungoid vegetations (not identical with those
usually developed after air infection) in plugged bulbs which had been
boiled in a can of water.
If it should be hereafter established that Saeteria and fungoid vege-
tations do, under exceptional circumstances, arise abiogemcally, this would
not overturn the panspermic theory, it would merely limit the nniver-
sality of its application.
Jpnl 23, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
I. " On some Points connected with the Circolation of the
Blood, arrived at from a stndy of the SphygmogTaph-Trace."
By A. H. Gasbod, B.A., Fellow of St. John's College, Cam-
hridgt: ; Prosector to the Zoological Society. Communicated
by Prof. A. B. Garrod, M.D., F.R.S. Received March 12,
1874.
(Abstract.)
The author commences by giving a table containing a fresh series of
i
i
392 On the Circulation of the Bluod. [Apr. 2ff, '
meoeuperaenls of tlie ratio borne by the cardiosyatole * to its cotaponeob
beat in the cardiograph-trace. Those tend Btrongly to BubBtanl.iate the
law preriously published by him, yu. that the length of the cardiosystoio
is constant for any given ptilee-rate, and that it varies as the square root
of the length of the pulse-beat only — being found from the equation (
a^=20v''f. where a^=the pulse-rate, and i/=the ratio borne by the cap-
diosystole to the whole beat.
A Birailor series of fresh measurements are ^ven in proof of the law
previously published by him, that iii the spliygmograph-traoe from the
radial artery at the wrist the length of the sphygmosy stole t is constant
tor any given pulse-rate, but varies as the cube root of the length of the
pulse-beat — it being found from the equation at/'= 47 ^i', where j:= the
pulse-rate, and )/'=tlie ratio borne by the sphygmosystole to the whole
beat.
By measurement of Bphygmograph-tnicings from the carotid in the neck
and the posterior tibial artery at the ankle, it is then shown that tba
length of the sphygmosystole in those arteries is exactly the
ns in the radial ; bo that the above-stated law as to the length of thi
sphygnioByBtole in the latter apphes to them also, and must tberefoiw!
apply eqiuillv to the pulse in the aorta.
i^ucli beiug Ihu uaee, by i:uuipikriii^ tLc nqtiatioa for £u<Iiug the leugth
of the cardiosyfitole with that for finding the aortic sphygmosystole, the
relation between the duration of the whole cardiac systolic act and tbe
time during which the aortic valve remains open can be estimated with
facility ; for by subtracting the shorter sphygmosystole from the longer
cardiosystole, a remainder is obtained which can be nothing else than the
expression of the time occupied by the ventricle at the commencement of
its systole in elevating its internal pressure to that of the blood in the
aorta, which must occur before the aortic valve can open up. This in-
terval is named the " ti/tpasis." Its length is found to be constant for
any given pulse-rate, but to decrease very rapidly with increftse in
rapidity of the heart's action, becoming mi when that reaches 170 &
minute. An attempt is made to explain these phenomena.
If the above considerations are correct, certain independently obtuned
measurements ought, on comparison, to correspond ; for by reference to
one of the author's papers in the ' Proceedings of the Koyal Society,* it is
shown that the length of the there-termed second cardio-arterial interval
(which may be called the second cardio-radial interval) can only represent
the time taken by the second or dicrotic pulse-wave in travelling &Y>m
the aortic valve to the wrist. This being so, there is every d priori
reason in favour of the earlier primary wave taking the same time in going
■ Tfae cardiMgsiaU U the intfirral betveen the comineii cement at the sj'Btole and tho
clonuro of the aortic val™ in each oudiiic reTolution.
■f- The ephygmotyttoU in the interval between the opening and cloeing of the aortw
^■ntlTs in each cardiao revolution.
1874] On the MmUe Anatomy of the Alimentary Canali 293
the same distance — which can be expressed in other terms by saying that
the length of the first cardio-radial interval, from which that o£ the
syspasis has been subtracted, ought to be exactly the same aa that of the
eecoad cardio-radial interval. That such is the cose is proved by th£
measurement of the lengths of these two intervals independently ; and
it is found that in all cases they agree to tlirte places of deeimalt, which
ia great evidence in favour of the accuracy of the methods and arguments
employed.
The latter part of the paper is occupied with the description of, and the
results obtained by, the employment of a double sphygmograph, by means
of which simultaneous tracings ore taken from two arteries at difEercnt
distances from the heart. The arteries experimented on are the radial
at the wrist and the posterior tibial just behind the ankle, 29 and 52-5
inches respectively from the aortic valves. From the resulting tracings,
the time occupied by the pulae-wave in travelling the difference of
distance (52-5—20=), 23-6 inches, is found and stated to be 0-0012 of a
minute in a pulse of 75 a minute ; and it is shown that this varies very
little with differences in piilse-rate, as might have been previously ex-
pected ; it is also proved that there ia an appreciable acceUrtUioit of Ike
inovenutU of ike puhe-tvave as it ijets farther from ihe heart.
By superposing the simultaneous trace from the wrist on that from
the ankle, direct verification is obtained of the earlier proposition — that
the sphygmosystole at the wrist and that at the ankle are of exactly similar
duration. The peculiarities of the ankle-trace ore also referred to.
11. "Note on the Minute Anatomy of the Alimentary Canal."
By Herbert Watnet, M.A. Cantab. Communicated by Dr.
Sandesson, F.R.S., Profeaaor of Practical Physiology, Uni-
versity College. Beceived March 10, 1874.
The following results relating to the anatomy of the mucous membrane
of the alimentary canal were obtained in the laboratory of the Brown In-
stitution. The researches were carried out under the direction of Dr.
Klein.
1. CoHrte^ivt-listw eorpuacUt amongtt the epillielium. — In specimens
hardened in chromic acid and alcohol and stained in tuematoxylin,
structures are constantly seen among the columnar epithelium of
the intestinal tract in many animals (aa monkey, sheep, cat, d<^,
rat, rabbit) which belong to the connective tissue. These are ; —
(1) a delicate reticulum, which is continuous with that formed by the
most superficial layer of connective-tissue corpuscles (the basement
membrane) ; (2) round nucleated cells, exactly similar to those of the
mucosa.
TOL. XXII, 2 A
294 On the Minute Anatomy of the Almvntary Canal. [Aj^. 23,
This is the case at Iho pyloric end of Ihp (itoinacli, on the Wlli, orer
Peyer'a patches, and in Lieberkuhn's glwuls.
2. The lining endothelium of the lym]ih-veB8el8 of the mucosa is in
anatomical conlinuity with the reticulum of nucleated cells (connective
tissue stroma) ; so thiit it may be said the endothelial cells of the
lymphatic vessel are only transformed connertive-IiMsue corpuscles.
3. In animals killed during the absorption of fat (cream) the fat can
be seen in prepamtiona stained by osmic add as Bmall black particles : —
(Ist) arranged in lines between or around the epithelial cells ; (2ndly) in
the basement membrane ; (3rdly) as has been noticed by many previcmB
observers, in the connective-tissue stroma of the villus, whence it can be
traced mto the lymph-iessel. This indicates that the fat is absorbed by
the processes of the connective tissue which exist between the epithelial
cells, and thence finds its way by the connective-tissue stroma to the
lymph- vessel.
4. Tlie reticulum of nucleated cells of the mucosa formfl a special
sheath to the vessels and unBtriped mnscular tissue.
In the villi the muscular bundles, having approached the apei, termi-
nat<>, the connective tissue which forms their sheath being coutinaous
with the corjiuscles forming the basement membrane.
In the mucosa of the colon of the rabbit the slender muscle-bands
divide into single muscle-fibres, on which the common sheath is con-
tinued. This sheath becomes often connected with peculiar large, oval,
nucleated cells lying close under the epithelium.
5. StnU of flie -miieoxis r/laiuls of Uie torvjue in rMt ami stcrttion. —
It has been found, in accordance with the researches of Professor von
Ebner, of Graz, that there are two kinds of acinous glands in the tongue,
which have been distingiushed as serous and mucous — the former being
always found in relation to the papilla; vallataj and drcumi-allatjo, the
latter always at the root of the tongue and partially surrounding the
former.
In the coiu-se of the present inquiry it has been further found (iu sec-
tions stained in hjematoiylin and carmine, made from the hardened tongue
of ananimalwhiehbadbeenlcftforafewhours without food) that the two
kinds of glands are coloured red and blue respectively ; but in sections
of the tongue of an animal killed while feeding, both kinds of glands were
stained red, while any mucus in the duct of the mucous glantia was
stained blue — showing that, in the stateof inanition, the cells of the mncous
glands contain mucus, while, during secretion, the cell-subatonee is
affected by the staining fluids in a manner not unlike that in which ordi-
nan," cell-substance would be acted on.
1874.] On the Sejraetioa of Sound by the Atmotphere. 295
III. "On the Befraction of Sound by the Atmosphere." By Prof.
OsBOHNE Retholub, Owens College, Manchester. Communi-
cated by Prof. Stokbs, Sec.B.S. Received March 18, 1874.
(Abstract.)
The principal object of this paper is to show that sound is refracted
upwards by Hie atmosphere in direct proportion to the upward diminu-
tiou of the temperature, and hence to explain several phenomena of sound,
and particularly the results of Prof. Tyndall'a recent observations off the
South Foreland,
The paper commences by describing the explanation of the efEect <^
wind upon sound, viz. that this efEect ia due to the lifting of the
sound from the ground, and not to its destruction, as is generally sup-
posed.
The lifting of the sound is shown to be due to the different velodties
with which the air moves at the ground and at on elevation above it.
During a wind the air moves faster above than below, therefore sound
moving against the wind moves Easter be]owthanabove,theefEect of which
is to refract or turn the sound upwards j so that the " rays " of sound,
which would otherwise move horizontally along the ground, actually move
upwards in circular or mora nearly hyperbohc paths, and thus, if ther^
is sufficient distance, pass over the observer's head. This explana-
tion was propounded by Prof. Stokes in 1857, but was discovered inde-
pendently by the author.
The paper then contains the descriptian of experiments made with a
view to establish this explanation, and from which it appears that :—
1. The velocity of wind over grass differs by one half at elevations {A
1 and 8 feet, and by somewhat less over snow.
2. When there is no wind, sound proceeding over a rough sur&ce
is destroyed at the surbce, and is thus less intense below than above.
3. That sounds proceeding against the wind are lifted up off the ground,
and hence the range is diminished at low elevations ; but that the
sound is not destroyed, and may be heard from positionB sufficiently
elevated with even greater distinctness than at the same distances with
the wind.
4. That sounds proceeding with the wind are brought down to the
ground in such a manner as t« counterbalance the effect of the rough sur-
face (2) ; and hence, contrary to the experimenta of Delaroehe, the range
at the ground is greater with the wind than at right angles to its direc-
tion, or where there is no wind.
On one occasion it was found that the sound could be heard 360 yards
with the wind at all elevations, whereas it could be heard only 200 yards
at right angles to the wind, standing up ; and, against the wind, it was losb
at 30 yards at the ground, 70 yards standing up, and at 160 yards at aa
293 Oil the litfrarthn o/Sviml bj Ike Atmosphere. [Apr. '.
elevation oE 30 feet, although it could Iw heard distinctly at this lottef^
point 5 few feet higher.
As might be expected, the effect of nusiag the bell was to extend its
range to windward, to even a greater extent than was obtained by an
equal elevation of the observer.
These results agree so well with what might be expected from the
theory as to place its truth and completeness beyond queRtion.
It is thus argued that, since the wind raises the soiuid so that it cannot
be heard at the ground, by causing it to move faster below than above,
ftny other cause which produces such a difference in Telocity will lift the
sound in the same way ; and therefore that an upward diiuinution in the
temperature of the air must produce this effect ; for every degi-ee of tem-
perature between 32° and 70° adds nearly one foot per second to the
velocity of sound. Mr. Glaisher's balloon observations • show that when
the sun is shining with a clear sky, the variation from the surface is V
for every hundred feet, and that with a cloudy sky 0°-5, or half what it
is with a clear sky. Hence it is shown that "rays" of Bound, otherwise
horizontal, will he refracted upwards in the form of circles, the radii of
which are 110,000 feet with a clear sky, and 220,000 with a cloudy sky
— that ia to say, the reCmcticn on bright hot days will be double what it
is on dull days, and still more under exceptional circumstances, and com-
paring day \iith iiight.
It is then shown by calculation that the greatest refraction (110,000
radius) is sufGcient to render sound, from a cliff 235 feet high, inaudible
on the deck of a ship at Ij mile, except such sound as might reach the
observer by divergence from the waves passing over bis head ; wherefta,
when the refraction ia least (220,000 radius), that ia, when the aty is
cloudy, the range would be extended to 2^ miles, with a similar extenuon
for the diverging waves, and under exceptional circumstances the exten-
sion would be much greater. It ia hence inferred that the phenomenon
which Prof. Tyndall observed on the 3rd of July and other days (namely,
that when the air was still and the sun was hot he could not hear guns
and other sounds from the cliffs 235 feet high more than 2 inilee,
whereas when the sky clouded the range of the sounda was extended to
3 milea, and, as evening approached, much further) naa due, not to tJie
stoppage or reflection of the sound by clouda of invisible vapour, aaProf.
Tyndall has supposed, hut to the sounds beiug lifted over his head by
refraction in the manner described ; and that, had he been able to ascend
30 feet up the mast, he might at any time have extended the range of the
sounds by a quarter of a mile at least.
• Brit. Assoc. Eeport, 1862, p. 463.
1874.3 Oa the Mucous Membrane qfthe Utentt.
April 30, 1874.
Prof. ANDREW CEOMBIE RAMSAY, LL.D., Vice-President,
in the Chair.
It was announced from the Chair that the President and Coimdl had
appointed Mr. liockyer'a Paper, "Eeeearchea in Spectrum- Analysis in
connexion with the Spectrum o£ the Sud, No. 111." read Nov. 27 last, to
be the Balterian Lecture ; and Dr. Ferrier'e Paper, on "the Localization
of Function in the Br^n ," read March 5 last, to be the Croonian Lecture
for the present year.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
I. " The Structure of the Mucous Membrane of the Uterus and
its Periodical Changes." By John Williams, M,D. (Lond.),
Assistant Obstetric Physician to University College Hos-
pital. Communicated by Pr. Sharpey. Received March 3),
1874.
(Abstract.)
The paper consists of obserrations made on the uteri of nine women
who had died in different stipes of the monthly period.
lu two of the uteri the menstrual flow had almost ceased, and the
mucous membrane was wanting in the bodies of the organs. The
muscular fibre-cells were more or less exposed in the canity, and the
meshes formed by their bundles contained glands and groups of round
cells.
In one uterus menstruation had ceased three days before death, and
the muscular fibres were not exposed in the cavity of the orgnn, but im-
posed upon them was a layer of tissue composed of fusiform and round
cells. This tissue conttuned glands. The muscular tissue near the
internal orifice was devoid of glands, but nearer the fundus it contained
numerous glands.
In one uterus, in which the catameniol flow had ceased probably about
a fortnight before death, the layer of superficial tissue was thicker than
in the last; and near the internal orifice there was a marked and abrupt
distinction between it and the subjacent muscular tissue.
In one uterus the flow had ceased three weeks before death, and the
superficial layer was still thicker ; and the distinction between it and the
subjacent muscular layer was well marked, except at the fundus. The
uterine glands were tubular, ond arranged in some parts obliquely, in
others perpendicularly to the surface. They ^ were lined by columnar
ciliated epithelium.
298 Dr. H. Airy on Leaf-Arrangement. [Apr. 80^
In two uteri menstruation M^as imminent, but the flow had not begun.
In these the mucous membrane of the body of the uterus was fuUy deve-
loped, and had begun to undergo fatty degeneration. There was a
marked distinction between it and the muscular tissue throughout the
uterine cavity : it was highly congested.
In one uterus the menstrual flow had taken place for one day, and in
another for two or three days before death. In these there was extrava-
sation of blood into the mucous membrane, and the latter had in part been
disintegrated and removed.
Menstruation appears essentially to consist, not in a congestion or a
species of erection, but in gro\\i;h and rapid decay of the mucous mem-
brane. The menstrual discharge consists chiefly of blood and of the
dAris of the mucous membrane of the body of the uterus. The source
of the ha)morrhago is the vessels of the body of the uterus. The mucous
membrane having undergone fatty degeneration, blood becomes extrava-
sated into its substance ; then the membrane undergoes rapid disinte-
gration, and is entirely carried away ^vith the menstrual discharge. A
new mucous membrane is then developed by proliferation of the inner
layer of the uterine wall, the muscular tissue producing fusiform cells,
and the groups of round cells enclosed in the meshes of the muscular
bundles producing the columnar epithelium of the glands.
II. '^On Leaf- Arrangement.^' By Hubert Airy, M.A.^ M.D.
Communicated by Charles Darwin, F.R.S. Received
March 23, 1874.
(Abstract.)
This paper is offered in correction and extension of the news con-
tained in a previous paper by the same author, read 27th Februarv,
1873.
The main facts of leaf-arraugement to be accounted for are : —
(1) the division into verticillute and alternate leaf-order;
(2) in the former, the equal division of the circumference of the stem
by the leaves of each whorl, and the alternation, in angular posi-
tion, of successive whorls ;
(3) in the latter, the arrangement of leaves in a spiral series round the
stem, with uniform angular divergence between successive leaves,
and the limitation of that angular divergence (represented as a
fraction of the circumference) to certain fractional values (in most
cases only approximate) which find place most commonly in the
following convergent series (A): —
1 1 2 3 5 8 13 21 34 65 «^ ...
? 5* 5* 8* 13' 21' 3i' 55' 8D' 144' ^•' ^^^
1874.] Dr. H. Airy on Leitf-ArrartgemaU. 3J9
more rarely iu the following (B) : —
I I 3 a 5 8 13 t,. . ,„.
li' 4' f n' 16- 25- 47'*'-' ^^^
very rarely in the followiiig (C) : —
^ ^ 2 ^ ^ Ac • tr\
4- 6' ff ff 23' *^- ' ■- tC)
besides a few iaolated values, ^j, „, L &c., which would find
place in higher series. (Hofmeister, ' Allgenieine Morphologie der
Oewachse,' p. 449. Leipzig, 1868.)
Dealing first with the phenomena of alternate leaf-order, the theory ia
advanced that, in each of the series A, B, C, &c., the higher orders have
been derived from some lower order of the' same series by a process of
condensation advantageous to the species in which those higher orders are
found ; that the sceue of this condensation of leaf-order has been the
bud and other close-packed forms of plant-growth ; and that the imme-
diate gain has been better economy of space.
In support of this theory it is argued, first, that the ute of leaf-order
is to be found in that sUge of the life of a shoot in which the leaf-order
is most regular and perfect. Leaf-order is seen in perfection in dose-
packed forms of plant-growth, such aa ike bad, the balb,thB>'aidiealroielt^,
the involucre, the eompotite head, the catkin, the eime, even the tetd itself.
Therefore it must be in these forms that leaf-order is especioUy useful.
In elongated shoots, on the contrary, with long iutemodes and distant
leaves, the !ea£-order has a tendency to lose that regularity which it
enjoyed iu the bud, and is often disarranged by a twiat of the stem
or by contortion of the leaf-stalks (required for the better display of the
leaf-blodes to the light). The native arrangement of the leaves (excluding
the order ■;\ ia oft«n a positive disadvantage to them in lateral twigs.
It is only in the more vertical and unembarrassed shoots that the leaf-
blades remtun content with their distributive position. Indeed, one chief
use of the leaf-stalk seems to be to enable the leaf-blade to moke the best
of an unfavourable birth-place. (Yew, silverfir, box, and privetore in-
stanced as examples.) Hence it appears probable that the use of leaf-
order is not to be found in the elongated shoot.
Looking, then, to the above-mentioned clos»-packed forms of pkmt-
growth as the scene of the usefulness of leaf-order, it is seen that the cha-
racteristic feature which distinguishes them from the elongated forms ia
contact between neighbouring leaves (or shoots). The whole surface of the
stem is occupied by their bases, and no vacant interstices are left between
them. It is plain that the process of cell-growth bos resulted iu great
miOtttil premirt between neighbouring leaves and shoots. Becognicing
AOO Dr. H, Airy oh Leaf-Arrangfrnent. [Apr. 30,
tbis fact of mutual pressure, we can see that leaf-order ia us»?ful in these
cloee-paclicd fcraia hy securing eijunl development of leaves and therefore
economy of space. If Ihe whole space is to hi' occupied, and the leaves
or shoots are to have equal development, there muet bo orderly ar-
raugemout of aome kind. The principle of economy of apace under
mutual pressure is put forward aS of chief importance in leaf-Arrange-
ment.
It appears that economy of apace is especially demanded in a longi-
tudinal direction, for the sake of protection against vieisaitudes of tem-
perature and the attai'ks of enemiea. In s. bud, for example, it is evidently
important, on the one liand, that as many leaves aa poasible should attain
as high development aa their situation will allow, in order that they may
he ready at the first approach of spring to complete that development
and enter on their function without loaa of lime ; but, on the other hand,
it is evidently important that the embryo shoot should be as short as
possible, in order that it may be well within the guard of the protecting
Bcatea and less exposed to danger during the long period of bud-life.
These claims will be satisfied by a vertical condensation of the leaf-order,
Buch as the state of mutual pressure of the embryo leaves and shoots ia
calculated to bring about.
That the arrangements represented by the lower terms of the above-
. mentioned aeries A, B, C, Ac. would, under a force of longitudinal con-
densation, actually give rise to the successive arrangements represented
hy the higher terma of the same aeries, is shown by diagrams, in whidi
the necessary conscquenees of each step of condensation are made
apparent to the eye. In these diagrams a leaf or shoot is represented
(for mechanical considerations) by a sphere, and the spheres are numbered
from 0 upwarda. Taking, first, series A, the lowest order of that
series, „, ia represented by two vertical rows of spheres, those of each
row being in contact and alternating nith thoae of the other. If these
two rowa remain vertical, no longitudinal condenaation can taXe place.
The first atep towards such condensation must be their sponttmeona
deviation from the vertical. (Instances of such deviation in nature are
found in the genus Oaxtena and others, to he considered further od.)
The next atep required is some force of vertical compression, such as
would result in nature from the stunting of thebud-axia (due directly to
cold or indirectly to the advant^e of protection gained thereby), attended
with less, if any, stunting of the leaves. Then it is seen that the succes-
aive stages of condensation, beginnmg with the order ^, will bring sucoes-
aively into contact with 0 (zero) the following numbera, 3, 5, 8, 13, 21,
34, 55, 89, 144, &x., alternately to right and left, producing in euccesdnn
1874.] Dr. H. Airy on Leaf-Arrangement. 801
a series of orders which exactly resemble those found in nature, repr&-
sented approximately by thf aucceaaive terms of series A ; —
1 2 3 5^ 8 13 .
3' &' 8' 13' 21' 34'
The first two or three stages of this process may be illustrated by
mechanical experiment. Attach two rows of light spheres in alternate
, order on opposite sides of a stretched india-rubber baud, give the band a
slight twist, and relax tension ; the system rolls up with strong twist
into a tight complex order with three at«ep spirals, an approximation to
the order \ : if the spheres are set a little away from the axis, the order
becomes condensed into (nearly) -,, with five nearly vertical ranks ; and
it is plainly seen that further contraction, with increased distance of the
spheres from the axis, will necessarily produce in succession the orders
(nearly) s' y^ sp ^-i ^i^d that these successive orders represent sue-
cessive maxima of stability in the process of change from the simple to
the complex. These results are not invalidated by the consideration
that the natural development of leaves is not simultaneous but succes-
aive.
By other diagrams it is shown that the same process of condensation
operating on the orders represented by the lower fractions of series B (=,
P &c.\ will produce the higher orders of that series.
■ The same is also shown for series C I „ f, &c.\.
From the striking correspondence thus brought out between fact and
theory, the conclusion is anticipat«d that we have here a clue to the
secret of complex spiral lenf-order— that it is the result of condensation
operating on some earlier and simpler order or orders, the successive
stages of that condensation being ruled by tbe geometrical necessities of
mutual accommodation among the leaves and axillary shoots under
mutual pressure in the bud (t^ing the bud as the type of close-packed
forms).
From this point of view, Hofmeister's law, that every leaf is found at
that point in the circumference of the st«m which has been left most open
by the earlier leaves of the cycle, means that every leaf stands in that
position relative to its neighbours which gave it most room for develop-
ment in the bud.
Allusion was made above to deviation of leaf-ranks from the vertical
ns a necessary first step towards condensation. A series of six diagrams
shows the gradual transition presented by different species of the South-
African genus Oatteria, ftx>m a form in which the two ranks are exactly
802 Dr. H. Airy on Leaf-Arrangement. [Apr. 80,
vertical, to a form iu which they arc strongly twisted luto a oom-
plex order with angular divergence nearly ^, differing from ? by only
g- of the circumference, and endently admitting of further twist and
closer approximation to the order £ From this striking series it is
inferred that ranks originally vertical can and do acquire and transmit a
tendency to deviate from the vertical, and that this tendency admits of
augmentation to a high degree.
Assuming a twist, then, as a probable primary variation from an
originally vertical condition of leaf-ranks, it is plain that each leaf would
take a lower position, and the whole bud (with the same number of
leaves) would be shorter, than in the untwisted form. The shorter bud,
it is supposed, would Imve an advantage in cold seasons. The direct
action of cold, by stunting the bud-axis (provided it did not stunt the
leaves in the same proportion), would increase the twist. It may fairly
be supposed that this twist would bo taken advantage of and increased
by natural selection in subservience to the close packing of the leaves.
This course of modification is equivalent to the continued action of a
force of vertical compression (mentioned above as the second requisite for
condensation).
Transition similar to that in Oasteria is seen in the genus Aloe.
Compare the two vertical ranks of A, verrucosa vWth the two twisted ranks
of A. obliqua. In A. serra (^achs, * L<^hrbuch der Botauik,' fig. 144)
the change from the vertical to the strongly twisted form is found in the
same plant : the basal leaves are in order .^ ; the higher take complex
ml
order.
Exactly comparable (in thi.s respect) with Aloe serra are the common
laurel, Portugal laurel, Spanish chestnut, ivy, and others, which exhibit a
similar change of leaf-order. These instances agree in presenting the
complex order in the buds or parts of buds which occupy the most exposed
situations, while they retain the simple order -.^ in the le^s exposed
lateral buds or in their basal portion. The exposure in the former
case may be regarded as a sauiple of that which, in the course of
many generations, has (it is supposed) occasioned the condensation of
leaf-order.
It is here contended that the force of graWty (to which the two-
ranked leaf-order of lateral twigs is referred by some authors) could
not have been equally the cause of the pheuomena seen in the inclined
lateral shoot of Spanish chestnut and in the upright Aloe serra : but the
phenomena in the two cases are the same, and admit of a common
explanation by the condensation theory, if we regard the basal portion
1874.] Dr. H. Airy on Leaf-Arrangtmeni. 803
of the shoot as letaining the andeiit order, and the more exposed torminal
portion oa hsving imdei^ne protectiTO modification.
. The variouB degrees of obliquity of spiral ranks in the alternate orders
of leaf-arrangement, and the complicated numerical relations existing
between those Tarious ranks, are ail fully accounted for by the conden-
sation theory.
Analyzing the spiral arrangement seen in a sunflower-head, a dandelion-
head, a house-leek rosette, and an apple-twig, the result is found to be
that any leaf (or fruit, inthefirsttwoinstances), taken as zero, has for next
neighboursHuccesBively,inrisingatepBof complexity of order, the 1st, 2ud,
3rd, 5th, 8th, 13th, 2l8t, 34th, 65th, 89th, 144th, Ac. (in order of growth)
alternately on the right side and on tho left, producing alternately right-
and left-handed spimls in sets of 1, 2, 3, 5, 8, 13, 21, 34, 55, 89, 144,
&c. ; and these numbers are identical with those which would result
from condensatioa of one of the lower orders of series A. Similar
considerations apply to series B and C.
It is a significant relation that, in the sunflower and simihir examples,
the arrangement of the fruits in the composite head is such as would
retult from condensation oE the arrangement of the leaves on the stem.
Among the whorled orders also there is equally strong evidence of the
woiting of the same force of condensation.
First there is a series (n) derivable from the crucial arrangement.
(This is shown by diagrams.) In the orders thus formed it is seen that
conspicuous sets of parallel spirals will form the most striking feature,
and that these spirals will be found in sets of 2, 4, 6, 10, 16, 26, 42, &e.
(series a).
Instances are seen in the genera Mtrmriaiis and Sa;/ina, and the order
Di2mKaee<x, in which last the whole series a finds exemplification.
Here also it is a significant relation that the fruit-order in the com-
posite heads of DipaaatcM! is such as would result fn»n condensation of
the crucial order of theb stem-leaves. Some of these plants exhibit in
their radical leaves a minor degree of the same condensation.
In like manner it is shown that condensation of whorls of three
would produce orders with spirals in sets of 3, 6, 0, IS, 24, 39, 63, &c.
(series /3). For examples see Hofmeister, op. cit. p. 460.
Condensation (if any) of whorls of four would give spirals in sets of
4, 8, 12, 20, 32, Ac. (series y).
It is contended thatthe preceding evidence, drawn from both divisions
of leaf-arrangement (alternate and whorled), is sufficient to establish the
principle of condeniatian as having played an important port in the
history of leaf-orruigement.
304. Dr. H. Airy on Leaf- Arm /i^^ iiin.L [Apr. 80j
But tlicra are pbenomeua in leaC-arrangemont nhii-h are not explmn^
by condensation. We have still to nocouut for (1) the ori^;in o£ altei^
nate orders with 3, 4. 5, 7, 9, &o. vertical ranks ; and (2) the oripn of
the different whorled orders, with whorls of two, three, four, five, A/c
(with 4, (i, 8. 10, &c. vertical ranka).
The whole course of condensation depended on obliquity of ranks ; but
the distinguishing feature in these cases is that the ranks are exactly oe
nimost exactly vertical.
All these cases are explained on the hypothesis that there has been in the
vegetable kingdom a variability (jiersallum) in the number of leaf-r&nksj
that a plant oripjially ha**ing two vertical ranks has, by a stroke of
variation, produced shoots or seedlings with three vertical ranks ; th&t
three have varied to four, four to five, five to si.\, and so on ; and that
these " sports " have survived in some cases because of some advantage
which they enjoyed (probably the same advantage as that gained by
condensation — the accommodation of the same number of leaves in
a shorter bud).
This hypothesis is supported by the variability which is found &t tfaa^
present day in the niunber of leaf-ranks in one and the same Bpecies,
Forinstanee, 6V(/itni aearaiir/ulnre exhibits sei'ci nearly vertical ranks in order
?, or tfti' exactly rerticdl in whorla of three. FrAeinus wwJmi has uor-
mally four exactly vertical ranks in whorls of two, but may be found
viithjlve nearly vertical ranks in order ^, or with sLv exactly vertical in
whorls of three. (These three varieties may be found on shoots growing
from the same stump.) Whorls of three are often produced by plants
usually hearing whorls of two (e. g. sycamore, lilac, laurustinus, maple,
horse-chestnut, elder, ash, &c.), and whorls of four instead of three are
seen in some species of Sedam and Verhaui. Among these forms it does
not seem possible that one could be produced from another by occuma-
lative modification.
Professor Beal has found well-marked variation in the cones of larch,
spruce, &c., the majority belonging to series A, but a considerable minority
to series B or series a.
In dandelion-heada about 5 per cent, belong to series a.
DifEerent species of the same genus (e. g. Ahc verrueosaaiiA variegata,
Hatvorlhia viacosa and pentaejona, and difEerent species of Sedum and
Cactus) often exhibit differences of leaf-order which can hardly be under-
stood but as resulting from direct variation in number of leaf-ranks.
This hypothesis is also supported by analogy drawn from the animal
kingdom. Among starfishes there is variability in the number of rays :
Aiterias rubens has sometimes four or six instead of five ; A. papposa has
from twelve to fifteen. Among mammals there is some variability in tho
number of digits.
1874.] Dr. H. Airy on Let^- Arrangement. 805
Supposing, then, that, by strokea of r&riatlon, fonns have been pro-
duced with (2) 3, 4, 5, 6, Ac, vertical leaf-ranks, it is next to be con-
sidered how the arrangement of the leaves in each form would be affected
by the demands of economy of space and mutual accommodation of ranks,
supposing the ranks to be similar in point of size and number of leaves.
Tu'o vertical ranks would gain lateral accommodation by taking
alternate order ^, Under vertical condensation, with twist in either
direction, they would give rise to the auccesBive orders of series A. (Two
ranks are found in uneconomical opposite order in the genus Matmbry-
anthemum. This arrangement would be prone to fall into crucial order
under vertical compression.)
Three vertical ranks would, with least surrender of lateral accommo-
dation, assume alternate order ^ (illustrated by diagram). A slight twist
in one direction (No. 3 towards No. 1) would allow perfect lateral
accommodation. In three-ranked plants (e. g. Carex and Alnut) such
twist is usually found. Vertical condensation operating on three ranks
possessing this obliquity would produce subsequent orders of series A, If
the obliquity were in the opposite direction (No. 3 towards No. 2), con-
densation would produce successive orders of series B,
Four vertical ranks would economically fall into crucial order, the
members of each rank fittbg into the intervals between those of its
neighbours. Opposite members therefore would stand at the same
height, and would occupy one and the same node ; they would also
divide the circumference equally, and would stand over the intcnals of
the next loner pair. This crucial order under vertical condensation
would produce series a. In rare cases four ranks might assume an
alternate order .. Vertical condensation of this order :, with twist
4 4
(No, 4 towards No. 1) would produce series B ; with opposite twist
(No. 4 towards No. 3) it would produce series C.
live vertical ranks would, with least surrender of lateral accommoda-
tion, assume alternate order ?. A slight obliquity (No. 5 towards No. 2),
such as is usually found in nature, would allow perfect lateral accom-
modation. Condensation would then produce further orders of series
A. "With opposite obliquity (No. 6 towards No, 3) a new series
(i' ?' ^' W *"■) ^'"'^^ ^ produced. Pivo ranks might also take
alternate order I, which, cond^ised, would give with one twist series C,
with the other a new series ?, s, ^, r^, &c.
Six vertical ranks would economically fall into whorls of three, the
members of each whorl dividing the circumference equally, and standing
over the intervals of the nest lower whorl. Condensation would ^ve
30C Br. H. Airy on Leiif-Arranf/anenl. [Apr.30,<
series p. If sii ranks shoiUd fall iuto alternate order ~, one obli- '
qnity would lead to & series ff ji n- i^f **^'' *'^° opposite to a Benes ^
I l. ■?, Ac.
ff n' 17'
,S«i>ifn vertical ranks would take alternate order =, bdlitat«d bj I
obii()uity. Condensation wonW give series B. (It is needless to foQav I
other po«sible lines of condensation.)
Eiffht vertical ranks would fall into whorls of foar, with the <
general charaeters noted above in whorls of two and three.
would give series y.
Sine would give -. Condensation would produce series C.
Ten would give whorls of five.
Eleven would give ~.
Twelve would give whorls of six.
Thirteen would give ^ ; and bo on.
Thus it appears that the whnrled orders would naturally arise from
economic arrangement of eveit numbers (eicepf 2), and tlu- nltn-uaU
orders from economic arrangement of odd numbers (including also a), «rf
vertica] ranks.
It also appears that, in the whorled division, the members of eadt
whorl will divide the circumference of the stem equally, and that succes-
sive whorls will alternate in angular position.
It has already been showTi that in the alternate division the spiral
aTTangement of the leaves, with angular divergence limited to certain
series of fractional values (A, B, C, &c.), would follow on the hypotheaia
of condensation.
These are the " main facts of leaf -arrangement " set down on page 298
to be accounted for.
It is possible that all the varieties of leaf -order at present existing may
have been derived from an original two-ranked arrangement, partly l^
Tariation in the number of leaf-ranks, and partly by vertical condensa-
tion of the orders so formed. This view is supported by
(1) the high probability that the simplest form has been the earliest;
(2) the prevalence of the two-ranked form among lower phanero-
gamous plants (e. g, Graminete) ;
(.')) the numerous instances of transition from a two-ranted order
at the base of a shoot to a more complex order in the bigher
parts;
(4) the prevalence of the two-ranked arrangement of rootlets on
1874.] Dr. II. Airy on Leaf. Arrangement. 307
roots, token in connexicoi with their probable homology with
lateral shoots (the three ranks of rootlets in Polygtmaeta,
and the four in carrot and parsnep, illustrate rariability in
number of ranks) ;
(5) the two-ranked arrangement of leaves in the Be«dB of Mono-
cotyledonous plants, as compared with the more condensed
(though probably at first two-ranked) order in the more
highly developed Dicotyledonous embryo.
Summary, — ^The author is led to suppose : —
I. That the original form of leaf -arrangement was two-ranked.
II. That this original two-ranked form gave rise to forms with 2, 3, 4,
5, 6, 7, Ac. ranks, by " sporting," as opposed to any process of accumu-
lative modification.
UL That of the orders so formed those with an even number of
ranks (except 2) have, as a rule, assumed a whorltd arrangement, and
those with two or an odd number oi ranks have assumed an alUmate
arrangement, under the need of lateral accommodation of ranks in th^
bud (taken as type of close-packed forms).
rV. That ol! these orders have been subject to vertical condensation,
nnder the need of vertical economy of space in the bud (taken as type of
dose-packed forms).
V. (a) That such condensation, operating on a 2-ranked, or S-ranked,
or 5-ranked alternate order (^, 5, gj, has produced subsequent or-
ders of series A (-,
m 2V
».),
{b) That condensation of a 7-ranked /= I or rarely of a 3- or 4-raiilced
(I, >] alternate order has produced subsequent orders of series B
(I, I 2 i, 1, Ac.V
U' 4' V 11' 18' 7
(c) That condensation of a ©-tanked (^\ or rarely of a 4- or S-ranked
/j, pi alternate order has produced subsequent orders of series C
U' 5' »• 14' ^' 7
(d) That condensation of a 4-ranked whorled order (whorls of two)
has produced successive orders of series a, with spirals in sets of 4, 6,
10, 16, 26, 42, &x.
(f) That condensation of a &-ranked whorled order (whorls of three)
has produced successive orders of series ^, with spirals in sets of 0, 9,
15, 24, 30, &c.
(/) That condensation (if any) of an 8-ranked whorled order (whorls
of four) would produce ancoessive orders of series y, with spirals in sets
of 8, 12, 20, 32, &c. Higher numbers of ranks would lead to higher series.
Iir, "On the Improvement of the Spectroscope." By Taoi
(iRVBB, F.R.S. K«ceived April 30, 1874.
The importance, as an instrument of reaearcli, which the spectrosc
hfts reached within a few years, renders any improvement thei
a matter oE general scientific interest. Hitherto it has heen undt
disadvantage, which, though slight in amount in those cases in which
dispersive power of the instrumeut is moderate, becomes a rather sen
annoyance to the observer when a number of prisms are used in ae
combination, and the curvature of the spectral lines is proportion
increased, and only to be restrained irt appearance by usmg a nnr
breadth of the spectrum.
I have lately thought of a very simple and practical remedy (wl
may indeed have occurred to others, but which I have not seen n
tioued), whereby thoso liues are rendered palpably straight in a '
large field ; but previous to describing it, it is desirable to refer to a st
ment appearing in the ' Astronomical Notices ' for last month (March),
that the spectral lines can be rendered perfectly straight simpl]
returning them (after their first passage through a series of pri
ari-anged for minimum deviation) by a direct reflection from a p
mirror ; and, further, that this has been accomplished in a spectrosi
in construction for the Boya! Ohservatory.
Such a statement has, as might be expected, produced several inquii
in one case the querist is much interested, viz. by having a very li
spectroscope in band which, from its construction, involves the q
tion of straight or curved lines resulting. It therefore seems desii
to remove any illusion which may be entertained, by a short conaid
tion of the economy of the spectroscope, so far as the question of cu
ture is concerned.
The curvature of the upectral lines may be considered a functio
the dispersion of a prism ; it {the cun-ature) not only always ac»
panies the dispersion, but, further, its character is always the same
respect to the dispersion — that is to say, the centre of curvature wi
found invariably to lie in the same direction with respect to the direc
of the dlsiiersioa, the Unea being invariably concave towards that
of the spectrum baling the more refrangible rays*. This (which ad
of the clearest proof) is adequate to show the impossibility that, by
• Professor StokM hns indeed inveaiignlcd a form of
TSiiuUing lines are etraight, and on tlia ■amo
of courBo media of different opLioal powon)
remaining, the eurtatura might be found
law. The ourTatiirein that coin pound pri
lund priam in whic
iple no mu; eombine prisms (
■liich, with 0 halaiire of dispt
hut, this diwa not ofiect tho g«
(whicli Iras Ibe result of rarious triali
first used in tbp apECtrosoopo of IliB Great Melbourne Telescope, and now, I appro!
in pretty general Mtimation and uw) probnblj has n less proportional curniture <
line* than the simple prism.
1874.] Improvement of the ^ectroacope. 809
kind of iiiTersioii, whether by reflectionB or otherwise, we can nentralize
the curvature while donbling the dispersion.
If we examine the spectrum, as produced by a series of prisms placed
in the position of minimnm deTiation, we necessarily find that the lines
of higher refrangibility, also their centres of curvature, lie towards the
centre of the polygon which the prisma themselves affect ; and it we arrest
the rays at any ptart of the circuit, and reflect them directly back by a
plane mirror, this reflection reverses {right for left) not only the direc-
tion of tho centre of currature of the lines, but also the direction of the
spectrum itself, both which are consequently doubled in amount after
the rays have performed the second, or return, passage through the
prisms ; or (conversely) if, after the first passage through the prisms, we
reflect the rays so as to pass through a similar set in such manner as to
neutralize the curvature of the first set, we shaU find the resulting dis-
persion reduced to zero.
The writer of the article having alluded to a differraice between the
reflection as given by a plane mirror and a prism of (double) total reflec-
tion, it may be observed that, so far as the dispersion and curvature are
concerned, the cases are practically identical, the difference being that,
in the double reflection, there is a vertical inversion of the spectrum,
which, however, produces no discernible effect in either the spectrum or
curvature of the lines ; and as the spectroscope constructed with the
double reflecting prism is known to produce, with double dispersion,
double curvature, we here have an additional proof, if such were required,
that the single reflecting mirror does the same.
The remedy, or means of producing straight spectral lines, which I
have alluded to, is simply that of constructing the " slit" with curved
instead of rectilinear edges. There is but little practical difficulty
incurred in construction, and no apparent objection to its use. It may
be objected that for each variation of prism-power in use there should be
a special slit. It is, however, only in spectroscopes arranged for high
dispersion that the curvature becomes objectionable; in such there is
seldom a change required, and a single slit of medium balanciug-power
would probably remove all practical difflculty, or objectionable curvature
of the lines. I have found by trial that, when two compound prisms
were in use, giving a dispersion from A to H of nearly 14°, the spectral
lines were straight in a field of one degree, when the radius of curvature
of the slit was made 1*25 inch.
[^NbU on the above Paper.
If a ray of light be refracted in any manner through any number of
prisms arranged as in a spectroscope, undei^ing, it may be, any number
of intermediate reflections aji snrfaces parallel to the common direction
of the edges of the prisms — or, more generaUy, if a ray be thus refracted
VOL. Txn, 2 B
310
Lisl of Candidates.
[May
or reflected at the surfocea of any number of meJia bouDded by cy
drical surfaces in tbe most general sense (including, of eourwe, plane a
particular easo), the generating lines of which are piirallel, and
brevity's sake will be suppo9t.>cl vertical, and if cc be the altitude of
ray in air, a, a" , its altitudes in the media of which the rotraot
indices are /i, fi", then
(1) The Hucoessive altitudes will be determined by the eqnatiaaa
=^ , sin a = .
th^
just as if the ray passed through a set of parallel plat«e.
(2) The t!Ourse of the horizontal projection of the ray will bo the" a
as would be that of au actual ray passing through a set of media
refractive indices " , c ^_. instead of fi', ft", . . , _
a<a, the fictitious iudex is greater than the actual, and therefore
deviation of the projection is increased by obliquity.
These two propositions, belonging to common optics, place the jusi
of Mr. Gnibb's conclusion* in a clear light.— April m. Q. Q. KTOKKa
WILLIAM SPOTTISWOODE, M.A., Treasurer and Vi
President, in the Chair.
In pursuance of the Statutes, the names of the Candidates reci
mended for election into the Society were read from the Chair
follows :—
Isnac Lovrthian Bell, F.C.S.
W. T. Blanford, F.G.S.
Henry Bowman Brady, F.L.8,
Thomas Lauder Brunton, M.D.,
ScD.
Prof. W. Klngdon CTiffoid, M.A.
Augustus Wolkstou Franks, M.A.
Prof. Olaus Henrid, Ph.D.
Prescott G. Ilewett, F.R.C.S.
John Eliot Howard, F.L.S.
Sir Henry Sumner Maine, LXi,]
Edmund James Mills, D.Bc.
Hev. Stephim Joseph Perr
F.a.A.S.
Henry Wyklbore Bumsey, M.D
Alfred K."c. Selwyn, F.Q.S.
Charles William Wilson, Ma
E.E.
The Present:
■d were laid on the table, and thanks ordered
The following Papers were read :—
1874.] On a Magnetized Copper Wire. 311
I. " Preliminary Experiments on a Magnetized Copper Wire."
By Professor Balfour Stewart, LL.D., F.R.S., and Arthur
Schuster, Ph.D. Received March 30, 1874.
I. The following experimente were made in the Physical Laboratory
of Owens College, Manchester. The copper wire employed (A B C D,
1
■
see fig.) was found to contain no perceptible trace of iron, nor «a8 it
sensibly magnetic, behaving qnite in a neutral manner when tested by
the highest magnetic power at our disposal. It was covered with gutta
percha. The diameter of the wiro was 0-0487 inch. The wire was
wound fifty-three times, in one direction, round the poles of a powerful
electromagnet, the length of wire encircling these poles being about
twelve metres. The direct distance of the magnet from the galva-
nometer, G, was about twelve metres.
A ^Vheatstone bridge was employed, and a very delicate Thomson's
reflecting galvanometer by Elliott Brothers, of which the resistance was
5540 B.-A. units. A circuit-breaker was placed in the circuit at E, close
to the bridge. On some occasions, wo used one consisting of a solid
key, which might be removed, thus breaking the circuit ; but, on other
occasions, a fluid or mercurial circuit-breaker was employed.
When the left-hand pole of the electromagnet {see fig.) was made north
the arrangement was called (1), and when the other pole was made north
the arrangement was called (2). It will thus be seen, from the figure,
that the current went round the magnet in the same direction as the mole-
cular currents of arrangement (2).
Experiments were made at intervals of two minutes ; t Jd, on each
occasion, the current was allowed to pass through the Kiidge for ten
2b2
812
Prof. B. Stewart and Dr. A. SchuBter [May 7, 1
seconda, the meaaureraent being taken by the first swing of the gali>~»- '
nometer, which lasted for about eight f«oonds. Three cells of Gpove'a '
battery were used for producing this euireiit ; hut, on the other hand, aix
Bimilar cells were employed for magnetiKing the electromagnet. The
arrangements for magaetinng are not shown in the figure. The distance
of the magnet was too great to affect the galvanometer-needle so as to
alter its sensibility, the average detiection causing a difference in the
zero of about four divisions of the scale.
2. In the first experiments made, the key at E (see fig.) was not takeo
out before the magnetism wsa put on or off, in consequence of whidi Um
induction-current, due to the wire coiled round the magnet, aSoctMl the
galvanometer on these occasions ; but, after December 12th, the key waa
taken out, so that no induction-eurnmt passed.
The following is a specimen of the obserraticina made : —
December 17, 1873.
oarrcni, ii>er«*dng rcaislance in A B C D). "-rw.-
11" 11- 312 oil
13 317 off
16 311 off
17 345 (1)
19 328 off
21 306 (1)
23 : 303 off
25 293 (1)
27 300 off
29 290 (1)
31 307 off
33 283 (1)
35 292 off
37 288 (1)
39 302 off
41 292 (1)
43 309 off
It win be seen from this experiment that the^wf effeet of putting ca»
the m^netism was a marked increase of resistance ; but, with this excep-
tion, the resistance, when the m^netism was on, was leas than the meui
of the two resistances on both sides of it, representing the mag-
netism off.
3. The arrangement remained untouched, as far as we know, frtmi
December 15, when it was finally made, until December 19, when the
experiments were interrupted during the Christinas holidays ; and in all
D>t«.
FiistoE
Dec. 1« ..
.... 0
,, 17 ..
.,., 0
„ 18 .,
,... 0
„ 10 ..
.... 0.
1874.] on a Magnetized Copper' Wh-e. 313
cues tlie^rK efftei of puttiiig on the magnetism was ft marked increase
of resistance. For instance, we have —
On flret eflbct Seoond <M.
+38 on (2) +3
+34on(l) +17
+54on(l) +24
+33on(l) -18
It was soon seen that this firtt effect had some reference to the time
elapsing since the last experiments were made. For instance, in the
above Table, we see for December 18th a marked increase of resistance
when the magnet was first put on; but, on the afternoon of that day, the
experiments were repeated, and there was no apparent increase of
resistance in this Jirtt tfft^. Next, with regard to tiie average tffeel t on
Dec. 16th, 17th, and 18th, this average effect of magnetism was a decrease
of resistance; but on Dec. l&t^ there was an apparent increase of resist-
ance when the magnetism was on. We cannot say that nothing had
been done to the arrangement between the ISth and 19th of December
that might account for this change ; but whatever was done must have
escaped our recoUectioi}. Undoubtedly a good many experiments were
made during the time between the 15th and l&th of December, and tiie
direction of the magnetism was frequentiy changed. This curious
anomaly, occurring unexpectedly, induced us to limit our future experi-
ments to a definite set each day.
4. The experiments were resumed on January 7tii, the urange-
ment having remained untouched during the holidays. From this date
until January 10th inclusive, the key was taken out before beginning
experiments in the momii^ : there was no peculiar ^rvt ^eet ; while, on
the other hand, an avemge effect denoting a decrease of resistance came
out very prominentiy. On January 12th and 13th the key was only
taken out before magoetaDng, and on these occasions the Jirtt effeet,
denoting increased resistance, was sufGcientiy marked.
Our method of procedure was varied in tiie above manner up to
January 27th ; and it was invariably fonnd tiiat, whenever the key was
taken out before commuLdng experiments, there was aojint effeet; bnt
when it was kept in until before magnetizing, tins ^firsl effeet was suffi-
ciently marked. These experiments concur in proving that the ^rti
effeet has scHue reference to the previous treatment of the wire ; but they
do not prove that it is at tiie same time connected witii the putting on
of the magnetism. To determine this pcnnt we made a set of experi-
ments on January 22nd, 26tii, and 27th. When the current had become
constant the key was taken out, but the magnetism was not put on ; and
on these occasions there was no^^nt effect of the current upon itself in the
direction of increased resistance, but nther in the opponte direction. It
thus appears that the Jint ^eet which increases the resistance has not
314 Prof. B. Stewart and Dr. A. Scliustcr [May
only referoucn to th« previous treatment of the wire, but depends aJi
upon the magoetiBni being put on.
This result ja coufirmed by experiinenta miide previous to Dec. 12t
in which the key was not taken out at all. For instance, we har9<f
Dec. 9th, ^
First off. On flrat eSk^t. Scvtmi ott. H
0 +54 +45
We have hitherto only spoken of the ^rsl effect obtained aft
January 7th ; we now come to the average effect. From January 7'
to January 27th i'lclutiive, the magnetism was always put on is tl
direplion (1), and the avtrmje rfftct invariably denoted a decrease
resistance when the magnetism was on.
5. On January 28th the magnetism was reversed ; the effect during th
day wa« very irregular. On January 29th, 30th, 31st, and February 2i
the key was left in until before magnetization, The^Mf effect was no
extremely large ; but it was suspected that, during these e.tperiments, tl
contact of the key was not very good.
On January 29th the average fffett denoted a decrease of resistatic
but on January 30th, Slst, February 2nd, 4th, 6lh, the avemge ffft
denoted an increase of resistance.
6. From February flth until February 11th the wires were left hrokei
on February 11th there was a very alight _firit effect in the direction
increased resistance, and a slight avemi/e effect in the direction of d
creased resistance. On February 12th a mercury int^'rruptor was urn
instead of a metal key, both the wnres being broken by it, and its u
was continued until February 18th. The infa^rruptor was left in ov
night and the current was only broken before uingnetiKation, but ;
_firil 'ffeet was observed.
From February 19th to February 2fjth one wire onlv w'as broken
the fluid interrupter; ne^'erthelesa there was nojiml effect.
On February 12th, when the fluid interruptor was first employed, tht
was a very small average effect in the direction of increased resistanc
but, in ail the experiments afterwards, this avrroije effect \fa» in the din
tion of decreased resistance. The magnetism had been in the direct!.
(2) from January Stfth; but, during the experiment of February 25th,
was reversed and retained in this condition through the experiment
February Sttth, without appearing to affect the results.
7. From these experiments we may perhaps conclude as follows :■ —
In the Jii-st place, there is a Jirst effect in the direction of incre&s
resistance which appears to have reference to three things — -namely, t
previous state of the wire, the solidity of the circuit, and its ma
netization.
In the recond place, we have an average effect, of which the normal sla
appears to denote a decreased resistance while the magnetism is o
without reference to the directiou of the magnetism.
1874.] on a Magnetized Copper Wire. ^ 315
In the third plaet, when, in a solid circuit, the direction of the mi^;-
netism has been recently changed, there appears to be a t«mparai7
reversal of the average effect, which appears, at first, as an increase of
resistance. Besides the evidence herein detailed, we have other evidence
in favour of the third conclusion; tor in some preliminary experiments,
in which we frequently reversed the poles, we found an increase of
resistance when the magnetism was on. We have given, in a Table
appended to this paper, a synopsis of our \'ariouB experiments.
8. We are led to conclude, from other experiments besides these, that
the efEect of the magnetism is not merely confined to the part of the copper
B-ire wound round the poles, but is propagated all along the wire. On
December 2nd, for instance, the current was passed through the wire,
the galvanometer being joined as a secondary circuit. The main current
was therefore measured.
The deflections were as follows : —
297 off 300 off
300 (1) 302 (1)
297 off 301 off
300 (1)
This shows an average strengthening of the current, equal to about
one two-hundredth part of the whole. Were this strengthening due to
merely the change of resistance of that part of the wire wound round
the poles, the effect, as measured by the much more delicate arrangement
of Wheatfltone's bridge, would be much larger than was actually observed.
9. Allusion was made in article 7 to some preliminary experiments, in
which increased resistance was observed when the magnetism was put on
(1) and (2) alternately. Similar experiments were made, giving the
same result with a piece of coke and graphite, which were placed between
the poles of the magnet.
10. We have also some evidence that a copper wire, one end of which
is wound round the pole of the magnet, changes its position in the
electromotive series. Two copper wires were dipped into dilute nitric
acid and connected with the galvanometer. A weak current passed
through the galvanometer owing to a slight difference in the copper wires,
one of which was also connected with the copper wire wound round the
magnet. When the magnet was on, the current, as a rule, changed in
intensity ; but the effect was small, and the difficulty of having two
copper wires which, when joined together and dipped into nitric acid,
give a current sufficiently weak and constant, prevented us from getting
any decided results.
11. In conclusion we have to state that we regard these results which
we have ventured to bring before the Boj^ Society as preliminary, the
correctness of which will, we trust, be confirmed by the further experi-
ments which it is our intention to make.
On a Magnetistd Copper Wire.
[May
y
Dale.
1873.
Naturi' <i( Eiperiroeai.
Value of ttrst
effi»<X.
Number
of
obser»»i-
fi^t
resJi
Deo. 17.
,. IB.
.. 19.
1874.
Jan. 7.
„ e,
„ 9.
„ 10.
„ 12.
., 13.
., u.
.. 15.
.. 18.
,. 17.
.. 1!0.
„ 21.
.. 22.
., 24.
,. 20.
.. 27-
., 28.
„ 20.
„ 30.
„ 31.
Feb. 2.
„ 3.
„ 4-
„ 5.
„ 6.
„ n.
,. 12.
., 13.
„ 14.
^ 10.
,. 17.
.. 38.
.. 19.
.. 20.
., 22.
^ 24.
MfltAl ke; left in otbt niglit Uken out before
0+54+24
0+33-18
Nofirato&ct.
Ditto
Dilto
Ditto
0+47 + 18
No first effect.
0+3-6
0+17+11
No fi™t effect.
0+28 + 119
KoSrBt effect
0+7 + 1
No Qrst effect
Ditto
Ditto
Ditto
0+103+47
0+219
0+137+161
0+ 47+84
No Brat effect
Nofirit'effbct
0+7+S
No first effect
Ditto
Ditto
Ditto
Ditto
Ditto
0+11 + 18
No first effect
Ditto
15
30
.'5
1&
16
IS
15
Id
16
15
16
15
15
16
16
1&
16
13
15
16
15
IS
"is"
15
31
16
16
16
15
15
15
15
17
17
\ ^^
+
actio
Mewl 1k7 left in over night t^ten out before
MetS key Uft in orer Bight tabln out "before
Thelejwu«(aliea out beforebegiiiiiing tbe ei-
tC kej was taken out be^ro begiwing U^ ex-
periments in the morning
Tiie kef nu lakon oat before b^inniiiB the ex-
perimmils in the morning
The ke» waa Uk™ out before beginning the ei-
The key wm not uUten out until baTora mag-
netiring-'
The key was taken out (Mim« u Jan. 7)
Tiie key was not taken out (aame a Jan. 13) ...
Thekeywae taken out (Balneal Jan, 7)
The key was not token out (same as Jan. 12) ...
The eonneiions had been broken since Jan. 17 .
Thekev wu tnkm out (same as Jan. 7]
Wlien the current wus conntant the key was taken
out, but the BiBgnoC was not put on before tbe
Ditto
The roognet was put on (2) from thU day until
The magnet was put on (2), kaj l*ft in (same as
The niaenet was put on (2), key loft in (same as
Jan, 12)
The uiBguet was put on (2J, key left in (same as
The magnet was put on (2), key Wt in {same as
Tbe key was taken out and put in after aereral
ThakojwaBlalienout(eajDeBs Jan. 22)
The mercury interrupter wss kept in DTec night
The mercury intsrruplor was kept in over night
N»w mercurinl contact breaker from Elliott
Ditto keyleftin(BainBasJan.l2)
Ditto Ditto.
One wire only whs broken
One wire only was broken, key left in (same as
Jan. 12).....
One wire only was broken, key Uft in (same aa
Jan. 13)....'
Oae wire only was broken, key left in (same aa
»■/
One wire only WM broken, TD&gn<A oa (,\')
\ Wavo
1874.] On some l^ermomeiric ObtervtUiont in the A^. 317
Dec 16, 1873. For a Mcond lei-ie* of 15 on this da; do Aret effect wu found.
Jan. \b, 1874. There fne a sudden obonge of the current during tJiseiperimenta, to
which the unusuatlj small effect is moat likelj due.
Jon, 16. There wee a eudden change a! the current during the eiperimenti, to whiel)
the anusttoll; large effect is most likely due.
Jan. IT. There wae an irregulorit; at the beginning of the eiperiinenL
Jon. 20. Action somewhat irregular.
Jan. 22. There seemed to be a Brat tiStiA of the current on itself in the opposite
direction, 0-14-9.
Jan. 28. There seemed to be again a first effect ir
Jan. 27. Ditto Ditto
Jan. 28. The action was *ety irregular.
Jan. 2U. It is suspected tbat during tbe elperinieBts from Jan. 2D to Feb. 12Uie con-
tact at the Vej was not Terj good.
Feb. 3. The action wm tbtj irregular.
Feb. 4. There seemed to be two first effects of the current upon iteelf in the direction
of increased resistance.
Feb. 5. The action wna rer; irregular.
Feb. G. There seemed to be a flrst effect of decreased reeistance of current upon itadf.
Feb. 11. The wires hod been broken eince Feb. 6th.
Feb. 12. One of the wires bod got between the pole and the oare of the magnet.
Feb. 2A. After the first on (2) the magnet was olwajsput on (1).
II. " Note on some Winter Thermometric Observations in the
Alps." By E. P»A«KLAND, F.R.S.
During the past winter, I spent a fortnight at the Tillage of Davos,
Canton Graubiinden, Switserland, and had thus an opportunity of
experiencing some of the remarkable peculiarities of the climate of the
elevated valley (the Prattigau) in which Davos is situated. The village
has of late acquired considerable repute as a climatic sanitarinm i(x
persons suffering from diseases of the chest. So rapidly has its reputa-
tion grown, that while in the winter of 1865-66 only eight patients
resided there, daring the past season upwards of three hundred have
wintered in the valley.
The summer climate of Davos is very similar to that of Pontiesina and
St. Moritz, in the neighbouring high valley of the £Dgadin — cool and
rather windy ; but so soon as the FrKtt^u and surrounding mountains
become thickly and, for the winter, permanently covered with snow,
which usually happens in November, a new set of conditions come into
play and the ^jjti»T climate becomes exceedingly remarkable. The sky
is, as a rule, cloudless or nearly so ; and, as the solar rays, though very
powerful, are incompetent to melt the snow, they have little effect upon
the temperature, either of the valley or its enclosing mountMns ; conse-
quently there are no currents of heated air ; and, as the valley is well
sheltered frtan more general Ktjnospberic movements, an almost uniform
cairn prevails until the snow melts in spring.
Prof. F
According to Dufour'a trigonom-etrical meaaureineute, Davos is loo9
metres, or 5105 feet, above the sen; the measurements of the Swiss
Meteorological Sodety make the height 1650 metres, or 5413 feet ; oud
my own estimation with an aneroid gave it as 4000 feet above Zurich,
or 6352 feet above the sea. The rUlage of Davoa is thereforu about SUO i|
feet lower than the summit of the Higi.
I arrived on the evening of the 20th of December, and found the sutnr J
lying from two to three feet deep on the flat sole of the valley. On t
following morning the tbermometric observations were commenced wt^
instrumentu supplied to me by Mr. L. Casella, all of which had I
certified at the K.ew Observatory. For the corresponding readingB Wl
Greenwich I am indebted to Mr. GJaisher.
Dfctmher 2\tt, 1873.^From behind the sharp ])eak oE the Sohwan- I
horn the sun rose at the Seehof Hotel, Davoa-Diirfli, at 8.35 a.,|(,'.I
Throughout the day Ihe sun was alternately clear and obscured byffl
clouds. At Davos-PlatK it did not rise until 'J.44 a.m. At 10 a.m. tlw "
mercurial thermometer with blackened bulb in vaam showed 44° C.
(lll'-2 Fahr.) in the sunshine, and 45" C. (113° Fahr.) at 2.50 p.m. At
GreeD^ich the readings on tliis day with the blackened bulb in vaouo
placed (in the grass • in the sunshine were r— at 0 a.h.. S>°-3 C. {48°-7
Fahr,). at noon and .it 3 p.m., 21"-9 C. {IV-^ Fahr.), the maximum
during the day being 2\-i) C. (Tf-S Fahr,), The maximum tempera-
ture observed in the shade was 10°'9 C. (51°'7 Fahr.), and the miuimuni
on grass in the shade 2°-l C. (SS"-? Fahr.).
December 22nd. — A mercurial thermometer with black glass bulb wm
laid on the snow at 8 a.m. ; twenty minutes later, or fifteen miiiut«s
before sunrise, it marked — 18°-3 C. ( — 1° Fahr.). The sky was deep
blue, and almost perfectly cloudless during the whole day. Five minutes
after sunrise many of the patients at the Seehof Hot«l were walking in
the open air without any special wraps, and many of them without over-
coats. In the brilliant sunshine one felt comfortably warm sitting in
front of the hotel in a light morning coat. The following thermometrica)
observations were made on this day ; —
■ Since the above was written I have aKOrtained thnt tho readingn of this kind of in-
Btnunent ij^ much higher when it is laid on grass than when it ia clamped upon a
staff at B height of 5 feet above the ground. Thue, at SI. Lninard's^in-Sfla on the 7th
of April last, this thermometer in Bunahine stood at 42° 3 C. at 11.50 aji., when plB««d
5 feet from the ground, but when laid on (he graas it prompdj rose to SB^'S C. It u
therefore evident that the readings of tlie solar therniometcr at Qreenwicb, gma
throughout thia paper, are much too high lor fair oomparison with the Daros tempen-
ture, the thermometer at Greenwich having been olwsjs laid upon the graa>. On
the 7th of April the ekj at St. Leonard's was clear, the air warm with but littlo nrind,
and the sun bright ; nevertheless the maiiroum temperature during the day in sunshiD*
was2°'7C. lower than that observed with the same iastrument at Davos on the21atof
Dscember last.— Msj 7, 1674.
1874.] Thermometric Obaervatioiu ia the A^a. 319
I. Blackened bulb in vacuo. Ia sunshine.
8.45
8.50
9.0
9.45
10.15
10.45
l.M.
"-.""'X'"-
Light oloud
Clear.
1.45 P.M.
2l-6C
26-0 0
30-0 C
37 J C
35'3 c'ao-o c
1
41-2 C
42'4C
372 C.
43^ C.
This thermometer was clamped to an alpenstock at a height of about
five feet from the snow in all the observations recorded in this paper.
At Greenwich the readings were, with blackened bulb in vacuo : — maxi-
mum 12°-8 C. (55° Ffthr.) ; at 9 a.m., 8^-5 C. {47°'3 Tahr.) ; at noon
and at 3 p.m., 12°-8 C. (55" Fahr.). The maximum in the shade was '
10°-4 C. (SO"-? Fahr.), and the minimum on grass in the shade - l=-7 C.
(28°-fl Fahr.).
II. Plain mercurial thermometer with black glass bulb. In sunshine.
9.45. A.M.
10.15 KM.
11.15 A.1I.
NOOD.
1.45 p.K.
-1°C.
0=-6C.
3°-3 C.
3°-3C.
7°-2 C.
III. Plain mercurial thermometer with black glass bulb. In shade.
10.15 A.M.
11.15 A.M.
Noon.
1.45 P.M.
-4'-0C.
-r-oc.
- 1''0 C.
-2^0 C.
IV. Pl^ mercurial thermometer with block glass bulb, placed in a
box lined with padded black cloth and covered with plate-^lass
j inch thick.
0.45 A.if.
10.15 A.M.
Noon.
12.35 P.M.
2 P.K.
75°-0 C.
ss^-o C.
100°-0 C.
102°-8 C.
105°-0 C.
Thus in mid winter the unconcentrated solar rays at Davos ore capable
of producing, under favourable circumstances, a temperature of 221°
Fahr., — 9° Fahr. above the boiling-point of water at the sea-level, or
21° Fahr. above that point at Davos, where I found water to boil at
200° Fahr. when the barometer stood at 627-3 miUims.
320
Prof. Frankland on same Winter
[May 7,
December 2Srd. — ^The sky was again deep blue and doudlesB nearly
the whole of the day. The atmospheric pressure was 627*3 miUimB., and
the temperature eight minutes before sunrise, as shown by a black-glass-
bulb thermometer laid upon the snow, was again — 18°*3 C. (— P Faihr.).
The foUowing thermometric observations were made :—
I. Blackened bulb in vacuo. In sunshine.
90a.ii.
28»-5C.
9^A.M.
11.0 a.m.
35°-5C. 37*»-2C.
11.15a.m.
SQ'^O C.
ll.aOA.M. 12.15 p.m.
39*^-0 0.
2.0 P.M.
39<>-6C. 40°-0C.
Light clouds,
2.23 P.M.
34*»OC.
n. In the shade, the plain mercurial thermometer, with black glass
bulb, stood at -.9°-4 C. (15-1° Fahr.) at 11.30 a.m. It was freely sus-
pended in the air at a height of about three feet from the snow.
At Greenwich the readings were, with blackened bulb in vacuo : —
maximum 22*^-8 C. (73'* Fahr.) ; at 9 a.m., 4°-4 C. (40° Fahr.) ; at noon,
12°-6 C. (54°-6 Fahr.) ; at 3 p.m., 22°-8 C. (73° Fahr.). The maximum
in the shade was 8^*3 C. (46°*9 Fahr.), and the minimum on grass in
the shade - 2°-3 C. (27^-9 Fahr.).
December 24Ah, — As the Fluela pass, the highest carriage-road in Swit-
a^rland, was still open for sledges, I determined to make some observa-
tions on the summit, which is 7890 feet above the sea, and consequently
about 2538 feet above Davos. Starting from Davos at 8 a.m., I arrived
at the summit of the pass, where there is a small hotel and telegraph
station, at 10.30 a.m.
The early morning was somewhat cloudy, but, about ten o'clock, the
sky became perfectly clear and deep blue, and continued so until the sun
set behind the Schwarzhom, a few minutes past noon. The following
temperatures were recorded : —
I. The blackened bulb in vaaw marked 41°* 7 C. at 11 a.m. in the siui-
shine, 42°-3 C. at 11.30 a.m., and 42°-3 C. at 12 o'clock.
n. The' plain black glass bulb in the shade showed at noon — 7°'2 C.
when freely suspended about two feet above the snow in a brisk breeze.
The highest temperature in sunshine which I have observed at Davos
at noon, with the blackened bulb in vacuo, was 42°'5, which scarcely
differs from that read on the Fluela pass at the same hour. So far as
these limited observations go, therefore, they indicate that the solar rays
are not of appreciably higher thermal intensity at a height of 7890 feet
than at a height of 5350 feet. I may add that the thermometer in tiie
sunshine was sheltered from the wind on the Fluela pass, and was, in all
respects but oue, in a more favourable position for attaining a high tem-
perature than at Davos. The one unfavourable condition was its expo-
sure to less solar heat reflected from the snow than at Davos.
1874.]
Thartaometric Obaervalioiu in tfie Alps.
821
At Greenwich the readingH were, with blackened bulb in vacuo : —
maximum 19°-5 C. (G?"-! Fahr.) ; at 9 a.m., e°-6 C. (49°-3 Fahr.) ; at
noon, IS^-e C. (65''-5 Fahr.) ; and at 3 p.if., 19°-5 C. (e^-l Fahr.). The
mftTimiim in the shade was 10°'5 C. (50°-9 Fahr.), and the Ttiiniinnpi od
grass in the shade -3*^1 C. (26°-5 Fahr.).
Deetmber 25ih. — The sky was again deep blue and perfectly cloudless.
The sir was also apparently clear, except at about 9 a.m., when the village
and valley became immersed in a bght fog, which coneisted of minute
enow crystals. On thia and most subsequent days isolated crystals could
be distinctly seen floating in the air, by placing the eye in shadow and
then looking into the aunshine. The abundance or pandty of these
suspended and, under ordinary circumstances, invisible snow crystals .
must exercise a powerful influence upon the intensity of solar radiation.
To this cause, for instance, it was probably due that at 1.45 p.u. on this
day, although the sky was perfectly clear and the sunshine most intensely
bnlliant, the blackened bulb in vacuo only stood at 35° C. in the sun,
whereas at noon, when all the conditions were apparently the same
(except, of course, the sun's altitude), the temperature was 6° C. higher.
The following readings were taken : —
I. Blackened bulb in vaewo. In sunshine.
9.0 A.«,
froMn fog.
9.15 A.1I.,
clan.
10.20 A.M.,
cle«.
11.15 A.M.,
clear.
Noon,
dear.
1.45 P.11.,
dear.
2y-5 C.
32°-5 C.
3!"9 C.
39»-2 C.
40°-0 C.
3«°0 C.
<w eight minutes before sunrise
tde it stood at -9°-l G. Height
II. The black glass bulb on the si
marked -12=-8 C. At noon in the s
of barometer 630 millims.
At Greenwich the readings were, with blackened bulb in vacuo -, —
maximum 10°-4 C. (50°-8 Fahr.) ; at 9 a.m., 40-6 C. (40''-3 Fahr.) ; at
noon and at 3 p.m., 10°-4 C. (50°-S Fahr.). The maximum in the shade
was 7°'5 C. (45°'6 Fahr.), and the minimum on grass in the shade
-2°-7 C. (27°-2 Fahr.).
December 26<A. — Not the smallest cloud was visible during the whole
of this day. The sky was intensely blue and the mt perfectly calm.
Atmospheric pressure 630 millims. Fifteen minutes before sunrise the
thermometer on the snow marked — 16°-7 C. At 1.50 p.m. the same
thermometer in the shade stood at — 4°-l C The following readings in
the sunshine were made with the blackened bulb in vacuo -. —
8.45
9.0
lao
10.30
11.0
11.30
A.M.
.^.
12.30
1.0
2.30
3.60
P.M.
2S-0C
3i-8C.
3^-8 C
4tS'80.
d-5C
4^-70
^6C
1&1C.
(3-0 c.
af-oo.
3llC.
Prof. Franklaud on same fVinter
(.May 7.
At Greenwich the readingfl were, with blackened bulb ift vacuo : —
maKJmum8°SC. (iT^-fFahr.); at 9 a.m.. e^-JC. (44°Fahr.) ; ftt noon
uid at 3 P.M., 8°'8 C. (47°'9 Fahr.)- The maximum in the ahftde WM
8°-2C. (W-T Fahr.). and the minimum on grass in the shade -fC.
(39°-2 Fahr.).
December 27th. — A cloudless morning aiid deep blue sky. Eight
minuf«s before sunrise the thermometer on the snow iudicatfd — 1T""2C'.
At 10.25 A.K. the block bulb in vaciui registered in the simahine 3tS°-5 C
nnd at noon 38°'5 C. The afternoon woa cloudy and no observations
were made.
At Greenwieh the reodingB were, with blackened 'bulb in vaato: —
maximum 13°-6 C. (3<;°-4 Fahr.) ; at 9 a.k., 7°-5 C. (45'^S Fahr.) ; ftt
noon 6=-2C. (43°lFahr.); and at 3 p.m. 13'-6C. (56''-4Fiihr.). The
maximum in the shade was 8°4 C. (47°-2 Fatr.), and the iilinimuin oa
grass in the shade -S"-? C. (25''-3 Fahr.).
December 2S(A. — At 4.30 A.M. there was a violent stonn of wind witli
mow ; afterwards moderate wind with snow until the afternoon. The
barometer stood at 615 minima. At 2 f.m. the blaekened bulb in vaeita
registered 28°C. in sunshine.
At Gre«.nwiah the n^aJings were, with l.lm-keiieil bulb m vitcuo:—
maximum 0°-7 C. (33°-2 Fahr.); at 9 a.m., -O^'S C. (SI"-! Fahr.) ; at noon
and at 3 p.m. 0°-7 C. (33°-2 Fahr.). The maximum in the shade was 0°-6 C.
(33° Fahr.), and the minimum on grass in the shade was - 8°-4 C. {l&'-Q
Fahr.).
December 29th. — Sky deep blue and quite free from cloud during the
wholeday. Barometer 620millims. AtS a.m. the thermometer on the
snow stood at — 22°-2 C. A spirit thermometer (not verified), 4 feet from
the ground, indicated — 22°'l C. At noon the thermometer in the shade
stood at — I8°'l C. The following observations were made with the
blackened bulb in vacuo : —
9.0 A.if.
10.0 A.H.
11.0 A.X.
11.30 A.I..
Noon.
4 minutes sftor Euiuet,
3.30 P.M.
18°-0 C.
30°-0 C.
33°-7 C.
37°-0 C.
33°-7C.
. -12°-0C.
At Greenwich the readings were, with blackened bulb in vacuo ; —
maximum 28°-4C. (83°-2 Fahr.) ; at 9 a.m., - r-6 C. (29''-2Ffthr.) ; at
noon, 28° 3 C. (82° 9 Fahr.) ; and at 3 p.m., 28°-4 C. (S'6''-2 Fahr.), The
maximum is. the shade was 4°'2 C. (39°'5 Fahr.), and the minimum on
grass in the shade was - 9°-6 C. (14°-8 Fahr.).
December 30th. — Sky deep blue and perfectly free from cloud during
the whole day. Barometer 621-7 millims. At 8 a.m. the thermometer on
the snow stood at — 26°-4C. (— IS^SPahr.). A self-registerbg mioimnm
1874.]
Thermometric Obiervaiioat in the Alpt.
823
spirit thermometer (imverifled), fixed to a post 4 feet above the snow,
recorded —18° Fahr. as the minimum temperature during the night of
December 3S)-30th. At 2 p.u. the thermometer in the shade stood at
— 12°'8 C. The air was apparently equally clear throughout the whole
day. The following readings of the blackened bulb in vacuo in lunshine
9,0 *.«!.
B.30 A.K.
10.0 a.-. 11.30a.«.
12.15 P.u.
1.30 p.u.
2.0 p.-.
25°-5 C.
3Si°-3 C.
35°-0 C. 37°-5 C.
35°-2 C.
38°-5 C.
33=-7C.
At Greenwich the readings were, with blackened bulb in vacua : —
maiimom 22°-^ C. (73°-2 Fabr.) ; at 9 a.m., 2° -7 C. {36°-9 Fahr.) ; and at
3 P.M., 22°-9 C. i't2P-2 Fabr.). The maiimnm in the shade was 7°'5 C.
(45°-5 Fahr.), and the minimum on grasa in the shade was — 4°-9C. (23°1
Fahr.).
DeceiiAer Z\H. — Sky deep blue, sun quite free from clouds during the
whole day. Very light streaks of cloud appeared in the S.W. just
before sunset. Barometer 621-6 millims. At 8 a.u. the thermometer on
the snow registered — 23'''6 C. ; at noon the thermometer in the shade
stood at — 10''-C. A naked thermometer with smoked black glass bnlb
freely suspended restored only — 2°*8 C. at 9.30 a.m. in sunshine.
During the day abundance of snow crystals were frequently observed to be
floating about in the wr. The blackened bulb in vacuo was read in the
sunshine as follows ; —
9.30 4.M.
10.0 a.m.
11.0 a.m.
Noon.
12.30 p.M
2.0 P.M.
2.50 P.M.
32=0 C.
36»-5 C.
38°-7C.
39°0C.
40°-0C.
35°-0C.
21°-5C.
At Greenwich the readings were, with blackened bulb tn vacuo : —
maximum 24''-4 C. (76= Fahr.) ; at 9 a.m., 8''-1 C. (46''-6 Fahr.) ; at noon,
21°-3 C. (70''-4 Fahr.) ; and at 3 p.m., 24''-4 C. (76° Fahr.). The maxi-
mum in the shade was 10°'4 C. (50°'7 Fahr.), and the minimum on grass
in the shade was 0''C C. (33°-l Fahr.).
January \$t, 1874. — A cloudy morning. Sun only slightly visible
before 9 a.m.; afterwards brilliant between the clouds. Barometer
625 millims. At 8.15 a.m. the thermometer on the snow marked
— 13°-9C., and the unveriGed self-registering minimiuu — 17°-3C. At
11.30 A.if. the thermometer in the shade stood at-3°-3C. Thefollowing
readings of sunshine temperatures were made with the blackened bulb tn
Prof. Frankland on aome ffinter
[M.
eioudj]'
0-30 *.«,.
mn.
g.45 A.H.,
»un cl«ir,
rest of iky
cloudy.
10.0 A.>I.,
olear.
10.30 A-x,
cloudj.
ll^i-ii.
cloudj.
12.30 F
oloud
-1°-0G.
30°'SC.
43°-5C.
44''-0 C.
21*8 C.
igo-so.
ll°-5
23°
sino
The afternoon anil night were cloudy.
At Greenwich the i-eiidiijga were, with blackened bulb in vaem
maiimum 19°-e C. ((iT'-S Pahr.) ; at 9 a.m., 2°-8C. (37°Fahr.); at i
andat 3p.m., 1!)=-0 C. (fST'-S Pahr.). The ma-iimom in the shade
S°-l C. (46'-'-6 Pfthr.), and the minimum on gms« in the shade was - 1°-
(29'''9 Fahr.).
January 2nd. — -A cloudy morning. Sim not risible nntil ne
9 a.m.; afterwards clear and calm, except at about 1(1.40 Aii.,whea a
light clouds appeared. Minimum temperature during the night
measured by an unverified spirit thermometer, — 9^-2C, At 8 A.ii,
thermometer on the snow stood at — G"-? C. ; atmoapberic pres
627'8 millims. At noon the thermometer in the shade stooc
— o'C, and at 3 p.m. it registered —4°-6C. The following obse
tiona were made with the blackened bulb in naetio : —
9.0
o.ir.
...
10.0
10,30
10.40
Noon.
12.30
1.30
3.0
29°C.:3S°C.
!
40° C
41° C.
31°-5 C.
43° C
40° C.
n-c
2r-5 C.
At Greenwich the readings were, with blackened bulb in vacru
maiimum 14''-2 C. (57°-5 Fabr.) ; at i) a.m., e°-3 C. (48"-8 Fahr.) ; at i
andata P.M.,"14°'2C. (Sr-oFahr.). The maximum in the shade
10'''4 0. (50°-7 Fahr.), and the minimum on grass in the shade was 2°-
(36''-6 Fahr.).
January 3rd. — A calm but cloudy morning. At snnrise the ti
mometer on the snow registered ~(l°-9 C. The unverified spirit minin
showed the lowest temperature during the night to have been —11
Barometer 624 millims. At 11 a.m. the sun was just risible, and in
afternoon the clouds became still thinner. At 12.15 p.m. the tl
mometer in the shade stood at+0°'3C. The blackened bulb in v;
stood at 9° C. at 9 A.M. and also at 11 a.m. Between II and nooi
rose to 29° 0. At 12. 15 p.m. it marked IS^-S C, and between that b
and 2 p.m. it peached 28° C, whilst at 2 p.m. it stood at 25° C.
1871.] Thermomelrie Obtervationt in the Alpt. 325
At Greenwich the readings were, with blachenod bulb in vacuo : —
maSinmm 23°-8 C. (74<'-9 Friir.) ; at 9 a.m., 7°-2 C. (44°-0 Fahr.) ; at
noon 10°-4 C. (50°-8 Fahr.) ; and at 3 p.m., 33°-8 C. (74<'-9 Fahr.). The
maximum in the shade was 9°'2 C. (48°'6 Fahr,), and the minimiun ou
grass in the shade was - •4° C. (Sl^-S Fahr.).
During the winter of 1870-71 a series of meteorological observations
were made at Davos by Mr. Arthur Wm. Waters, F.G.9., but I am not
aware whether the instruments used were verified. The miniimiin
temperatures observed with a Hennana's metallic spiral thermometer
A. !>..«. '^-ZTcKS"
November, 1870 -10''-7 C. - 5°-5C.
December, 1870 -29°-5C. -15'=-7C.
January, 1871 -20*7C. -11°-1C.
February, 1871 -18°-7C. - 5°-0C.
The maximnro sun-t«mperatures obaen'ed with n blackened bulb tn
vtteno were :—
November, 1870 46°-3 C. 35°-l G.
December, 1870 46°-l C. 26°-0 C.
January, 1871 47='-3 C. 26''-6 C.
February, 1871 52°-2 C. SS^S C.
The chief remarkable things about the observations made lost winter
are, first, the very high suu-temperaturea prevailing contemporaneously
with very low air- or shade-temperatures, and secondly, the compar&-
tive uniformity of the solar heat from sunrise to sunset. Thus on the
29th of December, whilst the temperature of the air was — 18°-1 C, the
sun-thermometer stood at +37° C, and on the following day, with an air-
temperature not exceeding — 12'''8 C, the suurtemperature was BS^'o C
Again, the sun-temperatures observed on the 26th of December illustrate
the comparative uniformity of solar radiation during the day, when the
sky remains cloudless. Twenty-fire minutes aft«r sunrise the solar
thermometer indicated 31°-8 C. ; at noon it stood at 42''-5 C, aud at
thirty-five minutes before sunset it recorded 33°'l C.
Besides the intensity of solar radiation and its comparative uniformity
during the day, the rarity and calmness of the air are important factors
amongst the causes of the peculiar climate of Davos. With the baro-
meter standing at 615 millims. the weight of air in contact with a given
surface of the skin is about one fiftli less than it is at the sea-level. Tho
excessive dryness of the air at Davos has probably but little special influ-
ence upon the sensation of heat and cold, because the maximum proportion
of aqueous vapour present in air near 0° C. is everywhere small, and the
specific heats of equal volumes of fur and aqueous Tapoor He not widely
Tot. ixii. 2 0
386 Pror. Fraiiklaiid on some JVinfer [Mi
differeut. On thv olbt^r baud, Ihc absence of tmspeudL-il watery par
ill the air has, no doubt, very conaiderable iaflueiico in preveiitiri|
chilling of the ekin. Not only are such liquid particles present '
there is visible fog, but they often exist in great numbers when th
poBsesijeH its usuiil trouspareut appearauco. Another very importan
fluence upon the sun-temperature is the reflection of solar mys fron
Miow. The valley of Davos is about one mile wide, and has prodp'
sides and a flat sole. The liilages of Davos-Dorfli and Davos-Plat
Bituated on the north-west slope of the valley, and consequently re
the scattered solar rayn reflected from a large area of snow. 1 h&i
doubt that the sun-temperature at the opposite aide of the vail
markedly lower ; but having no second sun-thermometer, I could n<
certain this by the compariflon of simultaneous thermomctric oba
tions. When staying at Yentnor, in the vrinter of 1872-73, I no
that a not inconsiderable proportion of the total solar heat fftlling
a house on a cliff, near the shore, was reflected from the sea. M. Di
has Bince observed tlie same phenomenon betweeu Lausanne and "V
on the Lake of Gi?neva*. and has actually measured the proportioi
direct and reflected heat incident at five different stations on the norl
shore of the lake. He fauud that ihe proportion of reflected beat w
much' as 68 per cent, of the heat directly incident from the son, ■
the sun's altitude was between 4° 3B' and 3° 34'. At about 7° alt
the proportion was between 40 and 50 of reflected to 100 of direct
Even at about 16° altitude the proportion was between 20 and [
reflected to 100 of direct heat ; but when the sun was higher than
the reflected heat was hardly appreciable. It will be seen that
action of extensive reflecting surfaces of snow or water must exi
powerful influence upon the maximum temperature of places fa'
ably situated for receiving the reflected rays ; and, moreover, v
the proportion of heat reflected varies (as it has been proved to do i
case of water, and as it doubtless also does in the case of enow) inve
as the angle formed by the incident rays and the reflecting aurfaiCfl;
action nmst materially contribute, especially in winter, to the i
tenancc of an approHmately uniform sun -temperature throughom
day. At Davos and similar elevated stations, however, the compai
freedom of the air from suspended liquid and soUd particlea
obHousIy contribute, to a still greator extent, to such a result ; for as
and dry nir is transcalent and reflects light but slightly, the hor!&
sunbeams, passing through such air, would be nearly as powerful as
tical rays.
The peculiar winter climate of Davos appears, therefore, to de
upon the following conditions ; —
1 . Elfvatiott abope the tm, which causes greater rarity of the air.
I fjfoDceg de I'Acad^iiiie de« Bd
1874.] Thermometric Obaervationa in the Alps. S27
consequently lesi sbstnoHon of heat from the body. It kIso B««am
greater tnuucaleney in the atmoaphere by a pcnitdon aboTS the chief re^<ni
of aqueoufl precdpit«tion, and which is compantiTely out of the reach of
the diut and fuliginons matters that poUute the lower itiatmn of the
air. On my journey from Ixindon to Dares I never eaw the sun until I
had arrived neiirly at my destination ; and during the greater portion of
the fortnight of brilliant weather recorded above, there wai a dull leaden
sky at Zurich, about 60 miles distant.
2, Thick and {during the winter montTtt) ^nnanent gitow, which reRects
the solar beat and prevents the communication of warmth to the air, and
consequently the production of atmospheric currents. In still, though
cold, air the skin is well known to be less chilled than in much less cold
air, which impinges with considerable velocity upou the surface of the
body. The effect of motion through the air upon the sensation of warmth
and cold at Davos is very striking. Sitting perfectly atiU in the sunshine,
the heat in mid winter is sometimes almost unbearable ; on rising and
walking about briskly, a delicious feeling of coolness is experienced ; but
on drii-ing in a sledge, the cold soon becomes painful to the unprotected
face and bands,
3. A tfifltered potition favouraUe for retttving both the direct and rt-
jUctcd solar rnyt. — In this respect Davos-Dorlli, situated opposite to the
. entrance of the Dischma valley, has the advantage over DavoB-Plats, two
miles lower down the valley ; for, in the latter village, the sun rises on
the 21st December 1^ S" later, and sets about ten minutes earlier, than at
Diirfli.
All these conditions contribute not only to a high sun-temperatnre
during the winter months, but also to a comparatively uniform radiant
heat from sunrise to sunset.
In conclusion I vrill only point to the general bearing which these ob-
servations have upon winter refuges tor invalids. While the primarf .
conditions to be secured in such places must ever be fine weather and a
sheltered position, the next in importance is, undoubtedly, exposure all
day long to reflected, as well as direct, solar radiation. To accomplish
this, a southern aspect and a considerable expanse of water, or nearly
level snow, are necessary ; and it is important that the sanitarium should
be considerably, and somewhat abruptly, elevated above the reflectmg sur-
face, BO that it may receive, throughout the entire day, the uninterrupted
reflection of the sun's rays. At the sea-side, for instance, only those
houses which command such an uninterrupted view of the sea, ranging
from H.E. to 8.W., as shows the reflection of the sun throughout the
entire day, enjoy the full advantages of the place. At, or near, the se^
level, however, it is impossible, owing to the suspended matters in the
lower regions of the atmosphere, to enjoy any thing approaching to a
uniform temperature from sunrin to sunset. For this purpose it ia
necessary to leave the grosser air of the plains behind, and to ascend
•■i-M
\U: R. Malli't D,t I'olci
some 4001) or 5oOO feet into the mouatains, when, in these lati
least, the reflecting surface mnst necessarily be snow.
In the above remarks I hare confine;! myself strictly to the
aspect of the anbjei^t ; hut it is obvious that, in seeking an alp
tarium, the patient comes under new conditions of respint
breathes air comparatively free from rymotic matter — circu
which nre probably nut without profonnil influsnce upon hi?! hei
V
III. Addition to tlic I'apcr, " Volcanic Energy : an att'
derelop its tvne Origin and Cosinical Relations"
Robert Mallet, A.M., C.E., F.E.S., M.R.I.A., &
ceivcd April 3, 1874.
(Abstract.)
Eeferring to his original paper (Phil. Trans, 1873), the ai
marks here that, upoti the basis of the heat iftmnally dissipated
globe being equal to that evolved by the melting of 777 cubic
ice at zero to water at the same temperature, and of the expc
datu conlKiiied in his paper, he had demonstrated, in terms
crushed rock, the annual supply of heat derivable from the tra
tion of the meehanical work of contraction available for volcanii
and had also estimated the proportion of that amount of heat i
to support the anmml vulcanicity now active on our globe ; bnt,
want of necessary data, he hod refrained from making any cnlcu
to what amount in volume of the sohd shell of our earth tmigl \k
annually, in order to admit of the shell following down after ■
t])id]y contracting nucleus. This calculation ho now makes
sis of certaiJi allowable suppositions, where the want of datn
snch to be made, and for assumed tiiicknesses of solid shell of ]
400, and BOO miles respectively.
From 'the cnn-e of total contraction (plate x. Phil. Trane
1873) obtained by his experiments on the contraction of slag:
now deduced partial mean coefficients of conlractiou for a, redi
temperature of 1° Fahr.,for intervals generally of about 500° for t
scale, between a temperature somewhat exceeding that of tl
furnace and that of the atmosphere, or 63° I'ahr. And appl
higher of these cocfKcicnts to the data of his former paper, ao
suppositions of the present, he has obtained the ahsolut* eontr
volume of the nuclei appertaining to the respective thicknesses
shell above stated. In order that the shell may follow down an
in contact with the contracted nucleus, either its tiiickness uiu.
• RcBd June 2n, 1S72 : Phil, Trnn., for iST-l, p. 147.
1874.]
Presenli.
crease<], its volume remaiuiug couataut, or the thickuess being coostont,
a portion of the volume must be extruded. The former supposition is
not admissible, ns the epoch of mountain-building has apparently ceased ;
adopting the secoud, the author calculates the volume of matter that
must be crushed and extruded from the shell in order that it may remain
in contact with the nucleus. He tabulates these results for the four
assumed thicknesses of shell, and shows that the amount of crushed
and extruded rock necessary for the heat for the support of existing
\'olcanic action is supplied by that extruded from the shell of between
600 and 800 miles thickness, and that the volume of material, heated or
molten, annually blown out from all existing volcanic cones, as estimated
in his former paper, could be supplied by the extruded matter from a
shell of between 200 and 400 miles in thickness.
On data which seem tolerably reliable the author has further been
enabled to calculate, as he believes for the first time, the actual amount
of annual contraction of our globe, and to show that if that be assumed
constant for the last 5000 years, it would amount to a little more than s
reduction of about 35 inches on the earth's mean radius. This quantity,
mighty as are the effects it produces as the efficient cause of volcanic
action, is thus shown to be so small as to elude all direct astronomical
observation, and, when viewed in reference to the increase of density due
to refrigeration of the material of the shell, to be incapable of producing,
during the last 2000 years, any sensible effect upon the length of the
day. The author draws various other conclusions, showing the support
given by the principal results of this entirely independent investigatioa
to the verisimilitude of the \ lews contained iu his previous memoir.
PmenU r
ii'frf, Aj>rit 16, 1874.
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331 I'rof, A, C. Itnmsny oh Ccoioi/ictil Ages
"On the. Comparative Value of eertaiii Geological Ages (or groups
of Formations) considered as items of Geological Time." By A.
C. Ramsay, Lh.D., V.P.ft.S. Received December 16, 1873
There ore several metbod^ by whicb attempts have been made to esti-
mate the value of luiuor portious of geological time, one of whicb 18
founded on calculations of the probable Age of delt&s, deduced froiii>
eatimate«, more or less Accurate, of the quantity of matter ananolly
ried iu 8U8[>en3ion in rivers, in relation to the area occupied by, and the
thickness of, any given delta, such ns that of the ^Mississippi. But tut
none of these deltas are complet«d, and oa it ib imkuown when, in tlM
course of terrestrial changes, such completion may take place, no
con, as yet, successfully attempt to apply this kind of knowledge to tbe
amount of time that nas occupied in the formation of any of the ancient-
geological deltas, such, for instance, as that of tbe Purbeck and Wealdea
area.
Mr. Jame« CroU has, tvith considerable success, attempted to measura
that portion of geological time which relates to the last gnsat O-lacial
epoch, founding his conclusions on aBtronomieal data calculated back-
wards for a uiillion of years ; but, as yet, the precise beginning o£ that
epoch has not, iu my opinion, been shomi ; and in tbe absence of precise
data respecting the number of lotnl gladal episodes that may have pre-
ceded the last, and the complicated calculations that would be necessary
to measure these inten'als, even iE all these episodes were known, no
data are yet accessible for the application of Mr. Croli's method to the
greater part of geological time.
There are other ways in which the subject has been approached, bat
always, of necessity, with a total want of definitoneas with regard to their
value in the measurement of time. The relative thickness of difEermt
formations gives no clue, or only a very slight one, to the solution of
the question. Again, when in great and thick formations that spread
over wide areas, such as those of Silurian age, on upper part of the
series is found to lie quite unconformably on the lower half, it requires
but little experience iu geology to infer that the imconformity indicates
a long lapse of unknown time, unrepresented by strata over a given area.
When we link such phenomena of striking unconformity with the disap-
pearance in that area of some of the genera and most of the species in the
older strata, and their replacement by new and, to a great extent, generally
of closely allied forms, this addition to our data gives no c)e^ help in tiie
absolute measurement of time ; for no one aa yet has even dared to speculate
on the length of time that may have been necessary for the producti(Hi
of results so remarkable as those deduced from the theory of evolution.
I am well aware of much that may be said on the other side of this
particular question, such as that the incoming life of the later epoch
• Beoa Jan. 29, 1874. See nn«, p. 145.
at itema of Geological Ttme. 335
may be merely the result of migration from aomo other area or areas,
where it lived contemporaneously with the forma imbedded in the older
gtrata ; but this by no means gets rid of the question of time, with those
who may believe in an hypothesis so uncertain, if it so happen that th^
also uphold the doctrine of evolution. Looked at in this light, it in
obvious that the balance of probability is largely in favour of the greater
proportion of the specific forms in a new formation being, iu the conun<Hi
meaning of the word, of later date than those of an older formation, on
which the newer strata lie unconformably.
Neither is the main question altered by the circumstance that a pro-
portion of PaliEOioic genera are, in some parts of the world, occasionally
and nnezpectedly found along with Mesosoic associates. The fact remains,
that changes in life have been produced, during lapses of time, in specific
and consequently in generic forms, and that such contrasts of specific,
and often of generic, forms are always most striking where marked un-
conformities are found of a kind which prove that the lower strata had
previously been much disturbed, and, as land, had suffered much denudiv*
tion before being again submerged.
Seeing that speculations such as those enumerated, even when founded
on well-established facts, afford but little help in the absolute measnre-
ment of geological time, it has onxmrred to me t« look at the question
from another point of view, and, in a broad manner, to attempt to esti-
mate the &>mparative valut of long and distinct portiona of geological
time, all of which are represented by important series of formations.
In two papers* I have attempted to show that the Old Bed Sandstone, ■
Permian, and New Eed series were all deposited, not in an open sea, but in
great inland lakes, fresh or salt ; and this, taken in connexion with the
wide-spreading terrestrial character of much of the Carboniferous series,
showed that a great continental age prevuled over much of Europe and
in some other regions, from the close of the Upper SOurian epoch to the
close of the Trias. The object of the present memoir is to endeavour to
show the value of the time occupied in the deposition of the formations
alluded to above, when compared with the time occupied in the deposi-
tion of the Cambrian and Siluriui rockx, and of the marine and fresh-
water strata which were deposited between the close of the Triasslc
epoch and the present day.
Partly for the same reasons that I consider the Old Red Sandstone to
have been a lake formation, so I think it probable that the red and
purple Cambrian rocks of Scotland, Shropshire, and Wales were also
chiefly deposited iu inland waters, occasionally alternating, as at St.
David's, with marine interstratifications, generally marked by grey sla^
fossiliferous shales, somewhat in the same manner that several bands con-
• qiurterly Jaumal Geol Soo. 1871 (toI. iztiL pp. 169-198 \ 341-254), " On the
Fhyiiosl BeUtioiu of thft Nbw Bad SUrl, Blustio Beds, and Lower Luu," and " On
the Bed Bocks of Eaglsud of older date thsa ths Triaa.'
336 Pi'of'. A. C. Haiusay oa Gtologkiil Age*
tainiug mariue fossilti are iutertit ratified amoug the freshw'ater etrala of
the Miocont? rocks of SwilKerland. The probability of these Cambriaa
strata being partly of lacustrine origin is increased by the occurrence
of analogous beds beneath the Silurian strata of the Punjab. There, in
what is kuown as the Salt Bauge, I am informed by Professor Oldhain,
are certain red marly and sandy strata believed to be the general equi-
valents of our piu-ple Cambrian rocks. They contain several thick beds
of rock-salt, such as could only have been deposited by supersatunitioD
due to solar evaporation, in the manner that rotk-salt seems to have
been formed in the Keuper Marl.
If the red Cambriaa beds of Britain were partly deposited in iuluid
waters, then it appears likely that our BDurian formations, from the b&-
called Mcnevian and Lingula beds upwards, were all deposited under
marine conditiona between two continental epochs, the close of the
first of whicji is indicated by the nature of the Cambrian rocks, and tho
beginning of the second by the passage of the Upper Ludlow beda into
the base of the Old Bed Sandstone.
The physical conditioDs and lung duration of the second contineat^
epoch have been described in my two memoirs on the Red Eocks of £ng-
land •- The fimnas of tlie Cambrian and Lingula-fli^ series (which pass
conformably into each otlier). in the comparati\e paucitj' of species and
their fragmentary character, seem partjy to indicate occasional inluid
shallow seas, possibly comparable to the great inlet of the Bay of Fundy ;
and this scanty life probably gives but a poor idea of the fuller fauna of
the period, hints of which we get from the equivalent formations of
Sweden and Bohemia.
In the ' Geology of North Wales ' (IStJU) I haie shown that there is
a gradual passage between the Cambrian rocks and that portion of tho
Lingula-flag series now sometimes called Meneiian ; and, for some years,
I have held that the whole series of formations, from the lowest known
Cambrian to the top of tho Ludlow beds, mav, in Britain, be most
conveniently cUssed under three groups : Cambrian, Linguk, and
Tremadoc slates form the lowest group, succeeded niicoitfamuiblg by
the second group, consisting of the Llandeilo and Bala, or Caradoc,
beds ; above these we have the Llandovery, or May Hill, beds, over-
laid by the Wenlock and Ludlow series, the Llandovery beds lying
quite uneonfonnahhj on any and all of the formatious of older date, from
the Cambrian to the Caradoc strata inclusive. With each unconformable
break in stratigraphical succession there is a corresponding break in the
succession of species, very few (about 2| per cent, out of 68 known
species) passing from the Tremadoc slate into the Llandeilo beds, while
■ Abo in s lecture aubaequentlj given at the "RoyiA Initltulion, in nliidi this pieca
of geological liiatory was put into a more ooneecutive form, and the Bubatanoe of
which^inu published in full in the ' Can leoiporary Iteriew ' Tor Jnlv IST3, and (in
Paris) in llie ' KeTue Scientillqiie ' of 14th June.
a« ilenu of Geological Time. 337
from the Coradoc Sandstone only about 11 per cent, pass onward into
the Upper Silurian strata. These phenomena indicate gaps in geolo-
gical time unrepresented in the Silurian series of Britain by stratifled
deposits, and,^herefore, also unrepresented by genera and species, that,
did we know them, might serve to link together the life of the uncon-
formable formations in a more graduated succession of fonns. I recapi-
tulate these opinions, which were in part originally giren in my first
Presidential Address to the Geological Society (1863), because they bear
on the arguments that follow.
Like the Cambrian and Silurian rocks, the Devonian strata have also
been classified in three divisions by paleeontologiste — Lower, Middle, and
Upper. In Britain the Lower Devonian fauna is poor in numbers,
while it is rich both on the continent of Europe and in North
America. In England both the Middle and Upper Devonian fossils are
plentiful enough. According to Mr. Etheridge, out of 74 English forms
25 per cent, pass from the Lower into the Middle division ; while, out of
268 forms, 25 per cent, pass from the Middle into the L'pper Devonian
strata. No one has yet proved that these breaks in poltcontological
succession in the Devonian strata are accompanied by unconformable
stratification ; but the entire region has never been accurately mapped
according to the detailed methods of modem work. However this may
turn out, the vast thicknesses of these strata, characterized, like the great
SUurian divisions, by three marine faunas, of which the species are
mostly distinct, would- seem to indicate that the time occupied in their
deposition may be fairly compared with that occupied in the accumula-
tion of the Silurian series.
I accept the view that the Old Hed Sandstone, as a whole, is the
general equivalent in time of the Devonian formations, and probably of
a good deal more ; for our Lower Devonian beds have no defined base,
and, therefore, their predse relation to the British Upper Silurian rocks
is unknown, whereas the Upper Ludlow rocks of Wales and its borders
pass conformably, and somewhat gradually, into the Old Bed Sandstone.
If the Devonian rocks be the equivalent of the Old Red Sandstone, it
follows that the tims oeeupitd in iht dtpoiition of iht latter niny have been
oi long ai that lalcen in the <Upo»itit>n of the CanAriaa and Sihtriatt series.
This position is greatly strengthened by the thorough specific, and in
great part generic, differences in the fossils of the Upper Ludlow and
those found in the marine Carboniferous series — differences that, to my
mind, indicate a long lapse of time, represented by the deposition of the
marine Devonian strata, during which time the Old Bed Sandstone was
being elsewhere deposited in the large lakes of an ancient continent.
These palsDontological comparisons seem to me to indicate the vast
length of time necessary for the accumulaticm of these old lacustrine strata.
The next question to be considered is, what time the deposition of
the Old Bed Sandstone may have taken, when compared with the time
8t38 Prof. A. C. Ramsay on Geological AgeB
occupied in the deposition of certain members of the Mesoioic series.
This maybe attempted, partly on stratigraphical and partly on paUBonto- '
logical considerations.
The Lower Lias, at its junction with the Middle Lias, ^or Marlstoiie»
passes gradually into that formation on the coast-cliffs of Yorkshire,
where it is impossible to draw a boundary-Hue between them, either
lithologically or palsDohtologically. Both contain beds of the same kind
of ironstone ; and the marly and somewhat sandy clays, through about
twenty feet of strata, are similar in character, while a good proportion .
of the fossils in these passage-beds are common to both formations.
Higher up, where the Marlstone becomes more sandy, a suite of fossils,
to a great extent new, appears, due apparently to altered conditions of the
sea-bottom : the water was shallower and nearer shore ; and the topmost
strata of sandstone often contain many stem-like bodies, sometimes two or
three feet in length, lying on the surfaces of the beds in curved lines, the
same stems sometimes bending and crossing each other in a manner that
strongly reminds the observer of the broken stalks of Laminarian seaweeds
lying on a sandy shore, within close reach of a Laminarian mne. Taking
these thingsiuto account, there seems to be a much more intimate connexion
l)etweeTi th(^ Lower and Middle than there is between the sandv beds of
the Middle Lias and the ITi)j)er Lias clays of Yorkshire, between which,
though there is a perfect conformity, yet a sudden break in lithological
character occurs, accompanied by a nearly complete change of fossil
species. But the three divisions being conformable to each other, the
diversities of fossil contents, more or less, seem to be owing to changes
in the physical condition of the sea, caused, in the case of the Upper Lias
shale, to sudden depression of the area, which resulted in the deposition
of the muddy sediments of the L^pper Lias in deeper water than that
which received the uppermost sediments of the Marlstone. In the
Midland Counties, however, the lithological break between the Middle
and Upper Lias is not so sudden, and, in that region, there is a greater
community of species.
In Yorkshire the strata immediately above the Lias are of mixed ter-
restrial, freshwater, and marine beds ; but even there and in the middle of
England, as shown by Dr. Wright, there is a certain community of fossils
in the passage-lx^ds that unite the L^pper Lias to the Inferior Oolite.
There is no perfect stratigraphical or pahoontological break bet\i'eenthem;
and when we ])ass in succession through all the remaining members of the
truly marine Oolitic series of Gloucestershire, Somersetshire, and Dorset-
shire, no real unconformity anywhere exists. The same species of fossils,
in greater or less degree, are apt to be common to two or more formations ;
for example, such community exists between the fossils of the Inferior
Oolite and those of the (^ombrash, between those of the freestones of
the Inferior and Great Oolites, of the Stonesfield and CoUyweston flates,
and betwei.»n those of the Kimmeridge and Portland Oolites.
tu item* tff Geological Time. 339
The change (& life in the tea-bottoms vaa, so to mj, partly local, toA
due more to minor acddental physical causes than to tlyt lai^er kind ot
change that is marked by great diaturbance of a lowir set of stratm,
long-continued denudation, and the subsequent unconlprmable depo^
tion of a newer set of beds upon them, thus clearly indicating a long
lapse of tdme unrepresented by strati&ed deposits over a gi?en area. I
therefore infer that the whole of the Liassic and Oolitic series must be
looked upon as. presenting the various phases of one foctes of marine life,
belongbg to one geological epoch, marked by boundaries below and above
which depended on definite physical conditiuns over a large area. Such
a state of things in this Mesozoic epoch is comparable to the changes in
the fossil contents of the various subformations of the Cambrian and
Ijngula-flag series, of which the Tremadoc slates fonu'an upper qiember ;
and, in my opinion, the comparison holds good even partly in the
manner of their deposition, parts of both series having been locally
deposited in waters not marine. On these grounds, therefore, the
Jurassic formationa, as a whole, may be compared with these early Palso-
Eoic formations in tiie length of time octupied for the depositum of taeh.
If this inference be just, then, in like manner, they may be compared
with the Lower Devonian strata — in England poor in fossils as far as is
yet known, but rich on the continent of Europe and in North America ;
and this (assuming that the Devonian and Old Bed Sandstone strata are
equivalents) implies that a lower portion of the Old Red Sanditone may
have taken at long for it* depoaitian a» the ti'Jioh of iht timt occupied in the
depoiition of the Liauic and Oolitic series.
It is now generally allowed that the Wealden beds of England are the
freshwater and estuarine equivalents of the Lower and Middle Neo-
comian strata of the Continent, which, in a paUeontological sense, may
be said, in some degree, to be related to the uppermost Jurassic strata, in
so far that a certain proportion of the species of Mollosca are common
to both, as shown: by Forbes and Godwin-Austen ; while, in our own
country, from the Lower Greensand (Upper Keocomian) about 14 or
15 per cent, of the fossils pass on into the Upper Cretaceous strata.
The same kind of proportion, but in less degree, is found in the relations
of the Tremadoc to the Llandeilo and Bala series, and of the latter to
the Upper Silurian formations, and also of the Lower to the Middle, and
of the Middle to the Upper, Devonian strata. Those last named being
representatives in time of parts of the Old Bed Sandstone, it follows
that the whole of the time oeeupied in the deposition of the Old Sed Sand-
stone may Ttave been equal to the wJuile of the time oeeupied in the deposition
of all the Juraasie, Parbeel; Wealden, and Cretaeeoue strata collectively.
The next term of the continental era under review is the Carbonifer-
ous epoch, which, in its various conditions and numerous local subdivi-
sions, may with considerable propriety be compared to the Eocene period.
The d^ositfl of both are locally of marine, estuarine, freshwater, and
-I
310 I'rof. A. C. Ramsay on (ieohg'tral Ages
terrestrial origin, Aud both are clearly connected tvith long t
tioental epochs.
Next come thf various inembera of the Penniftu series, whirit.tfj
published conehistous are correct, were partly formed in great i^
lakes, analogous to the Caspian Sea and other aak lakes of C«iitnJi
at the present day. Having heen depottiled in lakes, thesv sttbfM
tions may, in this one respect, be compared to the lacustrine Btntt
Miocene age ; and if 0astaldi'e conclusions with regard to pari d. I
Italian Miocene beds, and my own opinions respectuig part of I
Permian strata, be correct, each series Eihona eiideuw of having induJ
a glacial episode.
Ijater than the Permian comes theNe»E€d,orTrias8ic, Heries.n^
in this region, is not directly connected with the Permian strata, ia
far that, where they occur in contact, the New Rod Sandstone u ga
rally imconformable to the Permian bods. Li the threefold dinnon
the New Ked series in France and Germany, the marine beda of i
Muschelkalk (unknown in England) may be eomparetl to the Lomt
Coralline Crag strata ; and, though the Keuper Marls of Britain ajid
much of the Continent were evidently deposited in inlaud coDtina
iftlt lakes, in the region of the Alps the St. Cassian and Hallsb
marine b«ls, being equivalent to the Keuper Marls, may in this nm
be compared to the Red Crag series. No one is, I think, likely to ci
aider that the marine strata of Triassic age took a shorter time in th
deposition than tlie marine beds of the Crag ; and, if we take the X
Red Sandstone into account, the probability is, that the whole of 1
Triassic series occupied in their deposition a much longer time than tl
taken iu the deposition ot the Plioceue marine straia.
In my opinion, a great Tertiary continental phase began with t
Eocene strata ; and that continent having undergone many phyaii
changes, has continued, down to the present day, with a certain amou
of identity; and an analogous, though not strictly similar, state of thin
prevailed for an older continent, during the deposition of a large part
the formations treated of iu this memoir.
Tf the method founded on the foregoing comparisons be of value w
then arrive at the general conclusion, ihal the (/reat Ueal contitifntal tr
tuhich bcjan with the Old Rud Sandstone and cloied with Ike Ntiv R,
Marl, is oomparahU, in point of gmlogircd time, to that oeewpietl in ti
drpotition of the whole of the Metozoie-, or Secandari/, series, later tJta* ti
New Bed Marl, and of all the Cainoioie, or Tertiary, foifnaliong, mu
indeed, of all the time that has elapsed since tlu heginniiiQ of the dtpou
t!on of the Lins down to tht present da;/. To attempt to prove thi
theorem is the special object of this paper ; .ind if I have been sue
cessful, the corollary must be deduced that the modem continenta
era which followed the oceanic submersion of a mde area, during whid
the greater part of the Chalk was Ijeing depo^itetl, has been of miicl
as items of Geological Time, 341
' shorter duration than the older contment mentioned above in italics ; and
^ which, to us, seems so ancient, when we think that the Alps and the Jura
had then no more than a rudimentary existence.
* There are other points that bear on the comparative value of
different epochs of geological time. During the older local continental
epoch there flourished four distinct floras, those of the Old Bed Sand-
stone, Carboniferous, Permian, and Triassic series. Of these the first
three, notwithstanding considerable generic and complete specific differ-
ences, may yet be said to be of one Palaeozoic type. The Triassic fiora,
as far as it is known, is of a mixed character, with generic affinities, how-
ever, that unite it more closely to the Jurassic fiora than to that of the
Permian age. The whole series may therefore be considered as resolving
itself into two types — the first extending from the Old Bed Sandstone
to the Permian times, and the second belonging to the Trias.
During the later period that elapsed, from the beginning of the
deposition of tlie lias down to the present day, we have also four
distinct floras — the first of Jurassic type, embracing the little we know
of the Neocomian fiora ; the second. Cretaceous, which, as regards the
Upper Cretaceous strata of Aix-la-Chapelle and of Greenland, is to a
great extent of modem type ; third, an Eocene, and, fourth, a Miocene
fiora — the last three being closely allied, and the Miocene flora of Europe,
in its great features, being nearly indistinguishable, except in species,
from the kind of grouping incident to some of the modem floras of the
northern hemisphere. The whole of this series may, therefore, in
European regions, be also considered as resolving itself into two types —
the first Jurassic, and the second extending from the later Cretaceous
times to the present day. In this respect, the analogy to the fioras of
two types of the more ancient continent is obvious ; and, in both epochs,
this kind of grouping is clearly connected with the lapse of time, which,
in my opinion, may for each be of approximately equivalent value.
The evidence derived from terrestrial Vertebrata is not quite so simple.
In the Old Bed Sandstone none are yet known. In the Carboniferous
rocks all the known genera (fourteen in Britain) are Labjrrinthodont
Amphibia. The same is the case, though the known genera are fewer in
number, with the Permian rocks, excepting two land-lizards of the genus
Proterosaurus, Labyrinthodonts seem to decrease still more in the number
of species in the Trias ; but Crocodiles appear, together with seven named
genera of land-lizards, ti^'o genera of Anomodontia {Dieynodon and
Rhynchosaurus), three genera of Deinosauria, and two of Marsupial Mam-
malia. As far as we yet know, therefore, this ancient continental fauna
pretty nearly resolves itself into two types ; and, just as the Triassic
tspe of fiora passed into Jurassic times, ko the Triassic land-fauna
docs the same. The oldest, or Palseozoic, type (Carboniferous and Per-
mian) is essentially Labjrrinthodontian, and the second, or Triassic is,
characterized by the appearance of many tme land-lizards and other
terrestrial reptiles, together with marsupial mammslft \ vcdi >^\% \:rs^>^
VOL. XXTI. *3LTk
Prof. A. C. Ramsay on Geological Ages
fauna, as regards genera, with the exceptioD o( LabvrinthodoatU fl
the appearance of Pt«rosauria, ia represented, pretty equally, througii
[ members of the Meaoioic formations, from Jurassic
Cretaceous inclusive. After this comes the great Pachj-dermatoua Ma
maliau Eocene fauna, and after that the Miocene fauna, which, in
a characters, is of modem type.
Tlie'guoeral result is that, from .Turaasic to Cretaceous timee inclusi
there was a terrestrial fauna in these regions, chiefly Reptiliau, Saurii
and Marsupial, and, in so-caUed Cainoioic or Tertiary times, cbie
Reptilian and Piaeent-al. In brief, the old continental epoch that lasl
from the beginning of the Old Bed Sandstone to the close of the Tri
locallv embraces two typical land-faunas — one Carboniferous and Pi
I, and one Triassic ; while the later epoch, from the beginning of I
Lias to the present day, also locally contained two typical tand-faun
the latter of which is Bpeci*ily Placental. (See Table.)
I am aware that such inferences are always liable to be disturbed
later discoveries, and I therefore merely offer the above suggestions
being in accordance with present knowledge.
Auother point remains. The earliest known marine faunas, tb<
of the Cambrian, Liugula-flag, and Tremadoc bods, include many
the eristing classes aud orders of marine life, which are much more f«
developed in the succeeding Llandeilo and Bala strata, such as Spon^i
Annelida, Echinoderroata, C'riistacea, Polyzoa, Brachiopoda, Lame)
branchiata, Pteropoda, Nucleobranchiata, and Cephalopoda, This i
portant fact was insisted on by Professor Huxley in his Anniverss
Address to the GeoSogical Society in 18G2. The inference is obvioi
that in this earliest known Taried life* we find no evidence of its havi
lived near the beginning of the zoolo^cal series. In a broad sense, co
pared \iith what must have gone before, both biologically and physical
all the phenomena connected with this old period seem to my mind
be quite of a recent description ; and the climates of seas aud lands wt
of the very same kind as those that the world enjova at the present day
one proof of which, in my opinion, is the existence of great glacial hould
beds in the Lower Silurian strata of Wigtonshire, west of Loch Ryanl
This conclusion, not generally accepted, has since been confirmed
Professor Geikie and Mr. James Geikie, both with regard to the "Wigta
shire strata aud to the equivalent beds in Ayrshire. In the words
Darwin, when discussing the imperfection of the geological record
this history, "we possess the last volume alone, relating only to two
three countries ; " and the reason why we know ao Uttle of pre-Cambri.
faunas, and the physical characters of the more ancient formations
originally deposited, is, that, below the Cambrian, strata we get at on
involved in a sort of chaos of metamorphic strata.
■ EariioBt known oioept the Huroniiui Arpidelia Thranovica and the Laorentj
Bo toon Canodtnac.
t See PhiloMipbical Magudne, vol ixii. p. 289, 186&.
as itenu 'of Geoloffkal Time,
343
The conneuoD of this queation with the principal subject of this
paper, that of the comparative value of di^^rtnt geological eras as if.-in* of
geological time, is obvious. I feel that this subject is one of great
difficulty; and, as far as I know, this is the first time that any attempt
of the kind has been made tc solve the problem. If my method be incor-
*rect, it may yet help to suggest a better way to some one else ; and iu the
meanwhile, even if partly heterodox, I hope it may deserve toleration.
Classification of Faunas (Terrestrial, Freshwater, and Estuarine)
into Groups.
Formation!. | Clan.
Otdw.
Number o( Oeaorn.
No Tertebrala tnoim eieept fiah
' r
Permiaa i
Amphibia...
BepU'iiti ...
Amphibia...
Beptilia ...
11 E.
3 C.
3 E.
1 C.
3E.
1 B.
4 E.
3 C.
1 E.
2E.
1 C.
2 E.
i
Beptilut ...
Chelotiia
CrooodLlift
4 E.
4 E.
1 C.
4E.
2 E.
pureMio
:;
Lnmrtilia
Dcinomuria
MammsUa .
Pleroaauria
3 B.
15 E.
1 C.
1
W«dd Md
Septilia ...
Chelonia
Crocodilia
DeinoMuria ...
PteroBauris
4 E.
3 E.
9E.
1 B.
''&..{
;;
Crocodilia
Lacertilia
3B.
1 E.
9 E.
Mammalia .
Chelonia
4 E.
3 E.
2E.
U E.
Many more in France.
Ho VerlebraU certain in Eng-
fauna on the Continent. chieBj
of modGni t rpe. The Pliocene
fauna* are of course still more
Uiooene
2
TbB letter B. meona English, O. Continental and notknom vi ,
phjsieal phenomena connected with the CoDttnentaltltata ia vb\dittw^ i<s«tQun&*a
the main, identjosl wiH (bote that afibot the Bn^th looks. ^u &atn>wa. Ccn^
^ /own wiBauonfiii £tuf21iU«,
e BngUth lOoks, ^n Kvio^wu OsTJomneM
Mr. H. N. Moseley on the Structure [Ma;
May 21, 1874.
WILLIAM SPOTTISWOODE, M.A., Treasurer and ■■
President, followed by Dr. SHARPEY, Vice-Presiden
the Chair.
The Presents received were laid on the table, and thanks ordei«
The following Papers were read : —
I. "On the Structure and Development of Peripalus capen
By H. N. Moseley, M. A., Naturalist to the ' ChaUec
Expedition. Coinmuuicated by Prof. Wvville Thoh
F.R.S. &c.. Director of the Scientific Civilian Staff of
Expedition. Received April 9, i874>.
(Abe tract.)
The author corameneea by expressing his obligations to Prof
Thomson, who gave him assistance in some parts of his work, and i
eDcourage.ment in the further prosecution of it.
Specimeaa of P^i-ipatus were collected at the Cape of Good ]
during the stay of H.M.S. ' CImlleuger' at Simon's Bay, with a vie
the investigation of the development of the animal. A specimen
dissected and at once skqii to be provided wilh trachere, and to co
far developed young. This led to ns careful iiu esamioat ion being ma
time would permit, and hence the present paper. The moat mc
paper on Pcrijial'ia h that of Grube*. Grube, after eiamining the
tomy of the animal, eame to the condiisiou that it was hermaphrodite
placed it among the" Bris'le- Worms" iu a separate order, Ouychop
Grube has been followed in most test-bool>s, suth as those of I
and Schmarda; but uncertainty on the matter has been generally
De Qu^itiefageat follows Gervais in placing P.njwfus in aflinity wit
Myriopods. and the result of the present investigation is to show th
is no': far wrong.
Tie species made use of appears to be Penpalus capsniU. desc
by Grub.; in the Zoological Seri-s of the 'Novara' expedition,
anin.al has invariably ssventeen pairs of ambulatory members, a
of oral pnpillffi, and two pairs of horny hooked jaws, shut in by t
lips. The specimens found vnned in leiigvh from I'G to 7 cenlim;
the contracted condition. About thirty specimens were found, i
^em but one at Wvnberg, between Simon's Bay and Cnpe Town,
anijjals appear to ba somewhat local and not very abundant ; the;
IB damp places tinder tr&es, and especially frequent rotten willow-i
• ^lilki'i Anhiv, 1S53.
t Hi&t. des A"""'"*
1874.] tmdDevelopmmiof'Ptnpd.UampaMB. M6
Tbsy bed on rottoi vood. Th^ ue noctunul in their habiti. Thsj-
coll themielves ap spir&lly like Inivt when injured. The; hareanmult-
able power of extension of the body, uid when walking stretch to nearly
twice the length they have when at rest. Tfac^y can move with consider-
able rapidity. They walk with the body entirely supported on their
feet. Their gait is not in the least like that of worms, but more like that
of caterpillars. When irritated they shoot out with great suddenneaa
from the oral papUlie a peculiarly viscid tenacious fluid, which forme a
meshwork of fine threads, with viscid globules on them at intervals, the
whole resembling a spider's web with the dew upon it. The fluid is
ejected at any injuring body, and is probably used in defence against
enemies, such as insects, which would be held powerless for some time
if enveloped in its meshes. The fluid ia not irritant when placed on
the tongue, but slightly bitter and astringent ; it is as sticky as bird-
lime : flies, when they Ugbt in it, ore held fast at once. lie fluid k
structureless, but presents an appearance of fine fibrillation when dry.
The animal ia beat obtained dead in an extended condition by drowning
it in water, which operation takes four or five hours.
Only those points in anatomy are touched on which appew to httre
hitherto been wrongly or imperfectly described.
The intestinal tract is not straight, as described by Qruba, but longer
than the body, and usually presents one vertical fold ; it presents
BOmerous irregular sinuous lateral •folds, but is not enlarged in eveiT
b^ment, as stated by (>rube. Special regions, a muscular pharynx, short
(esophagus, long Stomach, and short rectum are distinguished in the
tract. The viscid fluid ejected from the oral papillie is secreted by a
pair of ramified tubular glands lying at the sides of the stomach and
stretching nearly the whole length of the body. These glands are theae
described by Grube as testes ; they show a common glandular structure,
but no trace of testicular matter. A pair of enlorgementa on the ducts
of the glands, provided with spirally arranged muscles, serre as ejaculA-
tory reservoirs. The lateral elongate bodies lying outside the nerve-
cords, considered by Qrube to bo vessels, show a fatty structure, vtrj
much in extent, and are probably to be regarded as representing the fatty
bodies of Tracheata.
1^0 structure like that of the heart of Myiiopods waa found in the
dorsal vessel.
The tracheal system consista of long fine tracheal tubes, which reiy
rarely branch : these arise, in densely packed bunches, from short com-
mon tubes, which open all over the body by small outlets in the epi-
dermis ; these outlets have no r^ular structure and are difficult to
lae. The whole of the tracheal system, very conspicuoua in th» fresh
condition, becomes almost invisible when the animal examined has been
a short time in spirit, and the air has been thus mmoved from th»
tnoheo. Haiuw the fiikxe oi Gnb* to m» thua. Tb« tndee
346 Mr. H. N. Moseley on the Structure [May 21,
are dUtributed in niesliworks to aH the viscera. The Hpiral filament
IB very imperfectly developed. A row of larger oval spiracles esisfs
along the middle line of the under surface, the spiracles being placed
opposite the interspaces of the feet, but not quite regularly. Other
large spiracles exist on the inner sides of the based of the feet. A
large supply of trachea goes to the rectum and muscular pharDvx. In
many points the structure of the tracheal system resembles that in
Peripatus is not hermaphrodite. Out of thirty specimens about t«ii
were males. No outward distiuetion of the sexes could be discovered. The
female organs consist of a small oblong ovary situate behind the stomach,
about one siith of the length from the end of the bod? ; from tlua lead a
ptaJr of oviducts, which, at their terminations, become enlarged and per-
form a uleriue function, appearing, when filled with embryos, like a
string of sausages. In nearly all cases, even when the embryos were
far advanced, two large' masaes of spermatozoa were found in the ovary,
and others attached to the ovisacs externally. A long loop, formed by
the oviducts on each side being quite loose in the body, becomes often
thrown into a knot through the constant protraction and retraction of the
body-wull. The knot i? knoivii to =.iilors fl5 im overhand knot oq a bight.
The knot sometimes becomes drawn very tight, and then prevents the
passage of the embryos above it. A case was met with in which thia
had occurred. The upper parts of the oviducts were mortified off at the
knot, and remained attached only to the ovary. The ducts were dilated
iiif« large single sacs, the usual constrictions between the embryos having
disappeared, and were full of decomposed embryos and fatty tissue. The
knot was met with in many specimens^in some cases on both sides of
the body, in others (as in that figured) on only one. The oi-iducts unite
in a short common tube to open at the simple vulva. The male orgaoB
consist of a pair of large ovoid testes, surmounted by short tubular
prostates. The vasa deferentia are long and tortuous, forming, near the
testes, spiral coils in which the ducts are enlarged, and which may he
called vesiculee seminales. A muscular ejaculatory tube, or penis, lies on
one side of the body — sometimes on one, sometimes on the other. One
vas deferens passes across, at the end of the body, under both nerve-cords
to join the penis ; the other takes a more direct course, not pasdug
under the cords at all. In the origbal condition both ducts probably
passed one under each nerve-cord, to join the centrally placed common
terminal tube, homologous with that of the female organs.
The spermatozoa are filamentary, as in insects and in Seohpendra, but
not in Iitlus. Their development is described. They are very long, and
their tails have a spiral movement as well as an undulatory one. They
twist into all sorts of loops.
The muscular tissue of Peripatus is unstriated.
The development of Peripaius was only partially Followed. As a rule,
1874.] and Deveiopment o/Peripatus capensia. 347
&U the embryofl found in one mother are of the same age. In some
cases slight differences were found, which were very valuable for detor-
mimng the development of the part« of the mouth. The embryos lie
coiled up in simple hyaline envelopes, enclosing an ovoid cavity, within
the enlargements of the uterine tubes. In the earliest stage observed
the embryo had large round cephalic lobes and was without members, but
showed distanct segmentation about its middle ; it was coiled up spirally,
the head being free, the tail in the axis of the ceil. Later on the embryo
becomes bent round in an oval, with the tip of the tail resting between
the antenuee.
The front members are formed first : they arise as undulations of the
lateral wall of the body, which become pushed further and further out-
wards, and ore at first hollow, formed of two layers of cells, the inner of
which ia reflected over the intestine. The members form one after
another, from the head downwards. A line of segmentation is formed
across the body before the pair of members swells out, but disappears as
they develop. The wall of the digestive tract is, in the early condition,
drawn out laterally at each interspace between the pairs of members, to
become attached there to the body-wall. The cephalic lobes early show
traces of a separation into two s^ments, anterior and posterior ; from
them, anteriorly, bud out the antenuie, which gradually become more and
more joint«d. The mouth forms before the anus.
The full number of body-members is very early attained. The secoud
pair is the largest at first, but subsequently become the small oral
papillee. The first pair turn inwards towards the primitive mouth-
opening, and, developing their claws greatly, form the pair of homy jaws ;
these are covered by processes which grow down from the lower part of
the head, and which eventually unite with the tissues at the bases of the
oral tentacles and form the tumid lips, which, eventually closing in, hide
all the parts of the mouth in the adult. The head-processes are probably
homologous with the mandibles of higher Tracheata, the homy jaws vrith
the maiillffi and the oral papillee with the foot^jaws of Scolopendra ; a
regular labrum is formed by a downward growth from the front of the
head, but is eventually shut in by the tumid lips.
It is uncertain whether a corresponding structure beneath the mouth
represents the second under lip of Scolopendra or a true labium. The
foot-claws are developed in invaginations of the tips of the ambulacral
members. The young members develop five joints each, the typical
number in insects, and one which seems to be retained in the adult.
In the present state of our knowledge concerning the structure of
Peripattu, the most remarkable fact in its structure is the wide di-
varication of the ventral nerve-cords. The fact was considered re-
markable and dwelt upon in all accounts of Peripatu* befco^ the exist-
ence of trachea in the animal was known, and wheii it was thought
Mr. H. N". MoBcley on the Structure
to be hannnphrodite, but it is doubly reaawtftble now. The fact sh
oS at once all idsa of Peripntus being a degenerate Myriopod,
evidance against whieb poiaibility is overwhelm Log. The bilateral sj
metry and duplicity of the organs of the body, the absence of sH
tion in the museles, of periodical moults of the larval skin in de
lopmeot, aud of any trace of a primitive thres-legged condition, tal
in eonjunetion with the divarication of the nerve-cords, are concliis
The parts of the mouth are not to be regardud as degraded to any gt
degree ; and homologies for some of them, at least, may perbnps be foi
amongst the higher Annelnis. The structure of the stiii is not at
unlikf that in some worms, especially in its chitinoua epidermic laj
which occasionally strips off in large pieces as a thin transparent pelli
The many points of resemblance of Pcripaliu to Annelids need not be d*
upon : they led to its former placing in classification ; but it is diffii
to understand how the very unann el id-like structure of the foot-cli
did not lead others, beside De QuaToEages, to draw a line bet«-een P
palui and the Annelids. In being uDiBexual, Peripatus is like the big
Annelids, as well as the whole of the higher Traeheata. To Inw
Peripatut shows affinities in the form of the spermatozoa, and the ela
ration, structure, and bilateral symmetry of the generati* 6 organs, thoi
there is a very slight ti^ndency towards the unilaterality of Myriopodi
the male organs.
To Insects, again, it is allied by the five-jointing of the feet and (
papilla) and the form and number of its claws. It should be remembe
that spiders' feet ore two-clawed, as ore those of some Tardigrades, i
that some of these latter forms ha\e two-clawed feet in the earlv cot
tion even when they possess more claws in the adult state. In Xevrpg
well-known figure of the young hdua nith three pairs of limbs,
tips of these latter are drawn with tiuo hair-like claws; these are
mentioned in the Icit, To the ordinary lepidoplerous larva the resi
blauces of Ptripntus are striking — as, for example, the gait, the gla
(so like in their function and position to silk-glandsl, the form of
intestine, and the Jess perfect concentration of the uervous organs, a;
larval insects. To Myriopods Penp:itiL$ is allied by the great Tari
in numberof segments in the various species, 'v\ its habits, and in th
especially to luhig. The parts of the mouth perhaps show a form on
which those of Scolopiitdra were derived by modification ; but the resi
blance may bo superficial. Our knowledge is not yet sufficient to dei
mine such points. The usual difficulties occur in the matter, Segm*
mar have dropped out or fused, and their original coudition may
bo represented at all in the process of development. In structure F
patus is more like Scoli^endra than /uJiw, viz, iu the m.any joints to
antennw (in CTiiiognaths never more than fourteen), in the form
spermatozoa, and in being viviparous, as are some Scnlopftulrcf ; f
ther, in tha position of the orifices of the generatiro glands and
1874.} and Develtpmmt of Feripatas c&penBis. 848
thd less perfvot oOnmitntioa meaially of the netirs-corda in Btth-
pentlra.
PeripaUu thus shows affinitiaa, in loina poinN, to all the main bntnchM
of the family tree of Tracheata ; but a gulf is fixed between it and them
by thd divarication of the nerve-cords : tending in the aame direction are
Biicli facta as the nun- s trial ion of the muscles, the great power of extension
of the body, the arrangeitieat of the digestive tract in the early stage, the
persis'.ence of metamorphosis, and the nature of the parts of the mouth,
the full history of the manner of origin of these being reserved.
There are many speculations as to the mode of origin of thv tracheo
themselves in the Tracheata. Professer Hackel (' Biologischs Studien,'
p. 491) follows Gegenbaiir, wboss opinion is e.ipresssd in his ' Grundziige
der vergleichenden Anatomie,! p. 441. Gegenbaur concludsa that
trachex were d3veIoped from originally clo3:!d trachea! systems, through
the intervention oE the tracheal gills of primieval aquatic ioiscta now
repre32nt3d as larvie, IE Pjripitai bs as ancieat in origin u is ber»
supposed, the qondijion of the tracheal system in it throws a very
diffjren^ light on the ma^tar. Pjripitai is the only Tracbeate witb
tracheal stems opening diffusely all over the bodr. The Pro'racbeata pro-
bably had their tracheie thus diffused, and the separate small nystems after-
wards became concentrated along especial lines and formed into wide main
branching trunks. Tn some forms the spiracular openings concentrated
towards a more ventral line {luliu); in others ihey took a more lateral
position (LcpiJopt!?rou3 larvae, Ac). A concentration along two lines of
the bodv, ventral and lateral, has already commenced in Peripatws. The
original Protracheate being supposed to have had numerous small trachea
diSused all over it's body, the question as to their mode of origin ^aitL
presents itself. The peculiar form of the tracheal bundles in Peripatva,
which consist o£ a number of fine tubes opening into the extremity of a
single short common duct leading to the exterior of the body, seems to
give a clue. The traches are, very probably, modified cutaneous glands,
the homologues of those so abundant all over the body in such forms as
Bipalium or Hirudo. The pumping extension and contraction of the body
may well hare drawn a very little air, to begin with, into the mouths of thfl
ducts ; and this having been found beneficial by the ancestor of the Pro'
tracheate, further development is easy to imngine. The exact mode of
development of thetracheie in the present form must be carefully studied;
there was no trace of these organs in the most perfect state o£ Ptripatva
which I obtained.
Professor Gegenbaur^s opinion on the position of Peripatxu (' Gmnd-
ziige der vergleichendea Anatomie,' p. 199) is, that its place among
the worms is not certain, but that, at any rate, it connects ringed
worms with Arthropods and flat worms. The general result of the pro-
sent inquiry is to bear out Professor Gegenbaur's opinion ; but it poioti
to the connexion of the ringed and flat womu, by means of this inter*
360 Mr. John Imray on the [May
mediate step, with three elftsses only of the Arthropods — the Myriop
Spiders, and Insects, i. e. the Tracheata, From the primitive conditio
the tracheffl in lulut, and the many relations between PeHpatua and Si
pendra, it would seem that the Myriopods may be most nearly alliet
Peripatug, and form a distinct branch arising from it and not pas:
through Insects. The early three-legged stage may turn out as of
BO much significance as supposed. If these speculations be correct,
Crustacea have a different origin from the Tracheata. Peripatus it
may well be placed amongst Professor Uackel's Protracheata ; Gni
term Onychophora becomes no more significant than De Blainville'e M
copoda. Some notions of the actual history of the origb of ftin/n
itself may be gathered from its development.
In conclusion I would beg indulgence for the many defects in
paper, due to the hurry with which it was written (aU available time, aln
up to the last moment of our sailing for the Antarctic regions, ha'
been consumed in actual examination of the structure of PeripattLs),
due, further, to the impossibility of referring to original papers in
scientific library. At all events it is hoped that Peripatua has been sh»
to be of verv great eoologioal interest, as lying near one of the main st<
of the great zoological family tree, and that further examination of
most minute character into the structnre of this animal will be '
repaid.
H.M.B, ■ Challenger,' Simnn'a Bbj-, Cape of Good Hope,
December 17, 1873.
II. " The Uniform Wave of Oscillation." By John Ihoay, M
Memb.Iuat.C.E. Communicated by W. Frodde, M. A., F.I
Received April 11, 1874.
(Abstract.)
The results of the investigation worked out in this paper corresp
with those previously deduced by other analysts, particularly by
W. Froude, F.E.S. The paper is therefore presented, not becaos
discloses any novel result, but rather as an example of a method wl
the author has found useful in the discussion of other dynamical proble
The object of the paper ia to trace the conditions under which
separate molecules of a liquid such as water move, when a body of '
liquid is in a state of oscillatory wave-movement. It is assumed that
wave-movement is established in a channel of uniform width am
length and drpth so great that the conditions of motion are not affei
by the interference of fixed ends or a Kxed bottom.
The wave treated of haa as its characteristics permanence of form
uniformity of apparent velocity.
Ill order that these conditions may be fulfilled, it is Jie: .iriied, as b.
1874.] Un^/brm. Wave of OtciUatim. S61
cftpable of ready geometiical demoiiBtration, that idl moIeculeB which in
repoee would be at the eame leTel, move in equal and aiuiilar trsjectoriea,
but tliat each molecule towards the one hand, aa towards the right, is by
a certain interval of time in advance of the contiguous molecule on the
left. It b also taken as a necessary condition of the wave-morement
that the excursions of the molecules are periodic, and effected in closed
orbits returning into themselves.
With these general postulates, the author proceeds to investigate first
the conditions necessary to maintain continuity of the liquid, or the con-
stancy of the vertical sectional area of an elementary portion of the
liquid, in all parts of its orbit. He then traces the operation on such an
element of the forces to which it is subjected, these forces being gravity,
or the weight of the element itself, and the pressure directed on it by
the surrounding liquid.
The liquid in repose is supposed to be divided into numerous hori-
zontal strata, each stratum forming an undulating film when the wave-
movement is established. The length of any such stratum ia supposed
to be divided into numerous portions, the width of each of which ia the
distance apparently traversed by the wave in a very short interval of
time. By taking the depth of a stratum, and the interval of time which
determines the width of one of its diviaiona, such that the element of
liquid may be conaidered a parallelogram of constant area, the several
differential equations expressing the continuity of the liquid and the
effect of the forcea on the element'are developed in an integrable form.
The parallelogram representing the liquid element is determined in its
form and position by the position of the points at its four angles.
One of thoae points, namely that at the lower lBft>'hand angle, is
assumed to move in a path tjie horizontal and vertical coordinates of
which, x and y, are referred to an origin situated at a height h mea-
sured from the bottom of the liquid, and the position of the point in its
path ia taken at a time ( reckoned from the epoch when the point was
verticaUy under its origin. The point at the lower right-hand angle of
the parallelogram is referred to an origin on the same level with the
former, but separated horizontally from it by a space, vAt, where v is the
apparent velocity of the wave, and A( is the short interval of time by
which the one point is in advance of the other in its trajectory. The
coordinates x and y of the first point being functions of A and i, thoae
of the other point are the same functions of h and t+^t. The upper left-
hand point being referred to an origin which ia at a height AA above the
level of the former origiiu, but being taken as contemporaneous in ita
movement with the point below it, ita coordinates are functions of
A+AA and l; and in like manner the coordinates of the upper right-
hand point are functions of A+&A and t+At.
As it does not d priori appear that the oiigin of the upper point must
be verticaUy above that of the lower (though in the course of the invea*.
Mr. John Imray on the [May 21,
tlgation it is tbcmi that this innst bo tbe case'), the author has, in ths
first iDstance, assumed that the upper origin is somenhat in advanee of
the lou-er, the amount of such advauce being a quantity of the order Ah,
which he has taken as mAft (it being afterwards proved that m=0).
With this nomenclatare, the equation of contiaaity is dedufed in the
following terms r —
(-J)(i4f)-(»+S)l-^
A constant area independent of i.
The pressure p at the lower leff-hand angle of the element being •
fonotion of A and I, equations are deduced giving values for the horizontal
accelerating force, --^, and the vertical accelerating force including
gravity, 5 + -j^, in terms of the diSerential coefficients of j;, y, and^.
From these equations it is shown that -i:=^0, or that the pressura
along any wave-stratum is uniform ; and this result leads to the simpli-
fication of the differential equations.
From the integration of those equations it is shown that every mole-
cule of the liquid revolves with uniform velocity, and with the a&mft
angular velocity at all depths, in a truly circular orbit, the radius of
which depends on the depth of the molecule below the surface of th»
liquid. The law of variation of the radius is, that while the depths
increase in arithmetical progression, the radius diminishes in geometrical
progression, or that the logarithm of the reciprocal of the radius is
directlv proportional to the depth of the centre.
The resultant of the forces acting on a molecule is shown to be always
normal to the profile of the wave-surface of which the molecule forma a
part, such resultant being compounded of gravity, a constant forca
acting vertically downwards, and of the centrifugal force of the molecule,
also a constant force acting radially outv*"ard3 from the centre of the orbit;.
The direction and magnitude of this resultant are represented by the
position and length of a line drawn from any point in the orbit to a fixed
point in the vertical line passing through the centre of the orbit. The
hquid element in traversing its circular path varies in width and in
height to suit the varying direction of the forces acting on it, its greater
height giving a greater hydrostatic pressure at the upper part of the
orbit, where the centrifugal force is opposed to gravity, and its less
height giving a less hydrostatic pressure at the loner part of the orbit,
where the centrifugal force acts along nith gravitv. Thus the oni-
formity of pressure throughout the orbit is maintained.
As a molecule revolves uniformly round the centre of its orbit, this
centre is the mean centre of gravity of the molecule during a complete
18740
Uniform Wave of OMeillBiion.
8S8
period. It is shown that daring ware-morement thia centre is eleratod
above the level that %roald be occupied by the molecule in lepose, a
height due to the vit viva of the mole(>u1s.
The profile of anj w&ve-stratum ia a irochoid, the length of which is
the distance from hollow to hollow or from creat to crest, and the height
is the diameter of tbe orbit of the molecule belonging to that stratum.
The highest possible wave is that where tbe trochoid becomes the
cycloid, or where the length of the wave ia equal to the circumference of
the orbit. >'o trochoid of greater height is physically posaible, as such
a curve must have a looped creat, where the liquid molecules would have
to cross the paths of each other, producing broken water.
The velocity and period of a wave, and the angular and actual velo-
rities of the liquid molecules, are deduced in terms of the length of th«
wave.
The general results of the investigation are shown by the following
formulEB, in which the symbols employed are : —
L= length of wave from crest to crest.
v= velocity, or distance apparently traversed by thewiTQ in a giTan
unit of time.
T=tho period, or time occupied by the passage of the whole wave.
jf=gravity (32 feet per second).
B= radius of the orbit of a molecule at
H=height measured from bottom, and
p= radius at
A = height.
jr=: horizontal, and
y= vertical ordinate of molecule in stratum at height h and at time t,
from the epoch when the molecule is at its lowest point, or when
27=0.
Then
origin being the centre of orbit,
?=anguj&r velocity.
Mr W. Spolliswoode u
[May
III. " On Combiuatioua of Colour by means of Polarized Lig
By W. Spottibwoode, M.A., Treas. & V.P.R.S. Eece
April 8, 187-1.
The results of rombining two or mare colours of the spectrum
been studied by Ht-lmholta, Clerk Maxwell, Lord Bayleigh. and oth
and the combinations have been effected sometimes by causing
spectra at right angles to one another to overlap, and sometituee
bringing images of various parts of a spectrum simultaneously upon
retina. Latterly also W. v. Bezold has successfully applied the mei
o£ binocular combination to the same problem (Poggendorff. Jubelb
p. 585). Some effects, approximating more or less to these, may be
duced by chromatic polarization.
CompUmenl'irif Coharg.—Firat as regards complementary colours.
ve use a Nicol'a priam, X, as polarixed. a plate of quartz, Q, cut
pendicularly to the axia. and a double-image prism, P, as analyser,
shall, as is well known, obtain tn'o images whose colours are com
mentary. If we analyze these images with a prism, we shall find, n
the quarts is of suitable thickness, that each spectrum contains a (
band, indicating the extinction of a certain narrow portion of its lenj
these bniiJjt will simultaneously shift their position when the Nicol \
turned round. Now, since the colours reraaiuing in each spectrum
complementary to those in the other, and the portion of the sped
extinguished in each is eomplemenlary to that which remains, it foD
that the portion eitinguiahed in one speetrimi is complementary to
extinguished in the other ; and in order to determine what portiui
the spectrimi is complementary, the portion suppressed by a band in
position we please, we have only to turn the Xicol X until the ban
one spectrum occupies the position in question, and then to observe
position of the band in the other spectrum. The combinations considi
in former experiments are those of simple colours ; the present c
binations are those of mixed tints, vii. of the parts of the spectrum i
pressed in the bands. But the mixture (.onaiits of a prevailing col
corresponding to the centre of the band, I
of the spectral colours immediately adjacent to it t
The following results, giien by Hflmholt/ n
verified : —
LoinpleoientBrv Ccloun
Ked, Groen^blue
Orange, Cj-anic blui
Yellow, lodigo-blui
Tellow-green. Violet.
ilight admii
each side.
"When ij
will be see
le spectrum the band enters the green, i
3 the outer margin of the red and a seci
L the other a I
id at the oppc
1874>.] Q>lour'CombiHatione by Polarized L^hi. 855
end of the riolet — showiog that to the green there doea not comspond
one complementary colour, but a mLzture of violet and red, >. e. a reddish
purple.
Combination of two Colowt. — Next as to the combination of two partt
of the apectrum, or of the tints which represent those parte. If, in
addition to the apparatus described above, we use a second quarts plate,
Q, and a second doublo-image prism, P„ we shall form four images, saj
00, 0 E, EG, E E ; and if A, A' be the complementary tints ex-
tinguished by the first combination QP alone, and B, B' those ex-
tinguished by the second Q, P, alone, then it will be found that the fol-
lowing pairs of tints are extinguished in the various images : —
Imue. Tint) el
OE B'.A',
EO • B',A,
EE B, A'.
It is to be noticed that in the image O £ the combination Q, P, hu
extinguished the tint B' inst«ad of B, because the vibrations in the
image E were perpendicular to those in the image 0 formed by the com-
bination QP. A similar remark applies to the image EE.
The total number of tints which can be produced by this double com-
bination Q P, Q, P, is as follows : —
4 single images,
6 overlaps of two,
4 oveHaps of three,
1 overlap of four.
Total.. 15
CoUattral ConAinatiiyM. — The tints extinguished in the overlap
O O + E O will be B, A, B', A ; but since B and B' are complementary,
their BUppression will not affect the resulting tint except as to intensity,
and the overlap will be effectively deprived of A alone ; in other words,
it will be of the same tint as the image 0 would be if the combination
Q, P, were removed. Similarly the overlap OE-(-E£ will be deprived
effectually of A' alone ; in other words, it will be of the same tint as E,
if Q, P, were removed. If therefore the Nicol N be turned round, these
two overlaps will behave in respect of colour exactly as did the images
O and E when QP was alone used. We may, in fact, form a Table
Ans: —
Imue. Colours eitjngnuhed.
OO+BO B -l-A-hB'-l-A-B-l-B'-l-A-A
OE-I-BE B'-(-A'+B-|-A'=B+B'4-A'-=A'.
And since the tints B, B' have disappeared from each of these formoln,
it follows that the second analyser F may be turned round in Any direo-
'tion without altering the tints of the overlaps in qnestion.
S&6
Mr. VV. Spottiswoode o
In like muiner ws maj form the Table
0 0 + EE B +A+B+A'=B+A+A'-.B
OE + EO B' + A' + B'+A=B'+A+A'=K.
Hence if the Xicol X be turned round, ttese overlaps will retain tlior*
tints ; while if the analyzer Pj be turned, their tints will vary, although
always remaining complementary to one another.
There remains the other pair of overlaps, viz. : — i
00 + OE B+A+B'+A' ■
EO+EE B'+A+B-fA'. M
Each of these is deprived of the pair of complement&ries A, A', B, fft
and therefore each, as it would seem, ought to appear white of low illumi-
nation, i. e. grey. This eSect, however, is partially masked by the fact Ihat
the dark bands are not sharply defined like the Fraunhofer lines, but bars
a core of minimum or zero illumination, and are shaded off gradually on
either side until at a short distance from the core the colours appear in
their full intensity. Suppose, for inalance, that B' and A' were bright
tints, the tint resulting from their suppression would be bright ; on the
other hand, the complementary tints A and B would be generally dim,
and the imago B+A bright, and the overlap B + A+B' + A' would have
M its predamintting tint that of B+A; and similarly in other csset.
Thero are two cases worth remarking in detail, viz., first, tli&tit) vhidl
B=A', B'=A,
i. e. when the same tints are extinguish^ by the combination Q F and
by Q, Pi' This maybe verified by either using two similar quartz plates
Q, Q,, or by so turning the prism P, that the combination Q, P, used
alone shall give the same complementary tints as Q P when used alone.
In this case the images have for their formula) the following : —
00 OEO EO EE
A+A' A+A' 2A 2A';
in other words, 0 0 and E 0 will show similar tints, and E 0, £ E com-
plementary. A similar result will ensue if B^A, B'= A'.
Again, even when neither of the foregoing conditions are fulfilled, wv
may still, owing to the breadth of the iuterference-banda, have such kn
afEect produced that sensibly to the eye
B+A=B' + A'j
■ud in that case
B'+Ai=B+A-A' + A
bbB + A' + 2A-2A',
which imply thkt the images 0 0 and O E may have the same tint, bilt
that EO and EE need not on that account be complementary. They
will di&r in tint in this, that E E, having lost the same tinta u £ 0,
vill have lost also the tint A, aad will have rccsived beaidea tlie w^ditifm
of two measures of ths tint A'.
1874.] ColouT'CambpiatiOM by Polarixtd lAgkt. 857
Effed of Comhmationt of two Cohuri. — A Bimilar tntin of raaidning
might be applied to the triple overlftps. But the main intereet of theu
parte of the figure consists in this, that each of the triple overlaps la
complementary to the fourth single image, since the recombination of
all four must reproduce white light : hence the tint of each triple over-
lap 19 the same to the eye as the mixture o£ the two tints suppressed in
the remaining image ; and since by suitably turning the Nicol N or the
prism P,, or both, we can give any required position to the two bands of
extinction, we have the means of exhibiting to the eye the result of the
mixture of the tints duo to any two bands at pleasure.
Effect of ConUiintUiona of three Cahuri. — A further step may be made in
the combination of colours by using a third quartz, Q,, and a third doublo-
image prism, P,, which will give rise to eight images ; and if C C be
the complement ories extinguished by the combination Q,P^ the formula
ior the eight images may be thus written :—
000 C+B+A.
00 E C+B' + A'.
OEO C+B+A.
OEE C+B+A'.
EOO C+B+A.
BOB C+B'+A'.
BEG C+B'+A.
EEE G+B+A'.
Th« total number of comUnations of tint given by the compartments
of the complete figure will be ; —
Y ■■ 8 single imagos.
= 28 overlaps of two.
thn*.
. 10
four.
fflght.
358 On Cobmr-combmatiom by Polarized lAghi. [May SI,
The most interesting features of the figure oonsiBt in this, that the
subjoined pairs are complementary to one another, vie. : —
000
EOE
C+B+A
Cr+B' + A'
EOO
OOE
C+B+A
C+B+A'
BEO
OEE
C+B' + A
C'+B+A'
SEE
OEO
C+B-hA'
C + B' + A
And if the prisms P, P,, P, are so arranged that the separations due to
them respectively are directed parallel to the sides of an equilateral tri-
angle, the images will be disposed thus : —
OEO O
EEO EOO OEE OOE
OEO
000
EOO
OEE
EEE
EOE
The complementary pairs can then be read off, two horizontally aaid
two vertically, by taking alternate pairs, one in each of the two vertical,
and two in the one horizontal row; and each image will then lepie-
sent the mixture of the three tints suppressed in the complementary
image.
Low-tint Colours. — A slight modification of the arrangement above de-
scribed furnishes an illustration of the conclusions stated by Helmholtz,
viz. that the low-tint colours (couleurs degrades), such as russet, brown,
olive-green, peacock-blue, &c., are the result of relatively low illumina-
tion. He mentioned that he obtained these effects by diminishing the
intensity of the light in the colours to be examined, and by, at the same
time, maintaining a brilliantly illuminated patch in an adjoining part of
the field of view. If therefore we use the combination N, Q, P, Pj (t. e,
if we remove the second quartz plate), we can, by turning the prism P
round, diminish to any required extent the intensity of the light in
one pair of the complementary images, and at the same time increase
that in the other pair. This is equivalent to the conditions of Helm-
holtz*s experiments ; and the tints in question will be found to be
produced.
1874.] On E^perimenit wiih a fU'eman'i Re^nratet. 860
rv, " Furtlier Experiments oa the Tranamissioii of Soand."
By John Tyndall, D.C.L., LL.D., Professor of Natural
Philosophy in the Royal Institution. Received May 21, 1874.
The author describes a number of experiments made with het«rogene-
ous atmospheres obtained by saturating alternate layers of lur with the
TRpoursof variouH \-olatile Uquida. Starting from hia observation on the
transmissian of sound through a snow-storm on the Mer de O-lace, in
the winter of 1859, he shows the extraordinary power of sound to pass
through the interstices of solid bodies as long as the continuity of the
air is preserved. Sound, for example, penetrates through twelve layers
of a silk handkerchief, wh^e a single layer of the same handkerchief
dipped into water, so as to fill the interstices, cuta ofE the sound.
He also describes numerous experiments with artificial fogs of a
density so great that a depth of three feet suf&ced to intercept the con-
centrated beam of the electric light ; the effect of such fogs on sound
was sensibly nil. ^Experiments were also executed on the illumination
of such fogs by sudden flashes, obtained by the combustion of gun-
powder or gun-cotton, or by the alternate extinction and revival of the
electric and other lights. Such flashes promise to be extremely useful
as fog-signals.
The author corrects the mistake of supposing that, in the experiments
at the South Foreland, the lower trumpets were not compared with the
higher onea. This, in fact, was the first step of the inquiry.
He also communicated an extraordinary instance of the interception of
sound during one of the battles of the late American war.
In these experiments the author has been ably aided by his assistant,
Mr. John Cottrell. An account of the experiments will be found in a
paper now printing for the Philosophical Transactions.
V. " On some recent Experiments with a Fireman's Respirator."
By John TStndall, D.C.L., LL.D.. Professor of Natural
Philosophy in the Royal Institution. Received May 21, 1874.
In vol. cLx. of the ' Philosophical TransactionB,' 1670, p. 337, 1 refer to
certain experiments on the " floating matter of the air," which were
afterwards considerably expanded and in put described in my ' Frag-
ments of Science.* These experiments, in which my object was to obtain
optically pure air by filtration through cotton-wool, suggested to me the
notion of a fireman's respirator. Cotton-wool had been previously
employed by Schroeder and Pasteur in their experiments on spontaneous
generation.
I had heard that smoke was a formidable obstacle to the fireman, and
that cases of suffocation were not rare ; hence the desire to construct a
VOL. xin. 2 g
360 On Experiments with a Fireman^s Retpirator. [May S9
respirator. My first trials were made with cotton-wool alone, Asw>^
ciated «"itli the respirator was a mouthpiece with two valrea : through
one the inhaled air reached the lungs, having first passed through the
cottoa-wool, while through the other the exhaled air was discharged di-
rectly into the atinoaphere. The smoke was generated in smaU rooms.
and in some experiments in a cupboard ; but though the irritation of
the smoke was greatly mitigated by the cotton-wool, it was unbearable
for any considerable time.
The cotton-wool was next carefully moistened with glycerine, no oJots
which couJd intercept the wr being permitted. The respirator was
distinctly improved by the stickiness of the fibres of the wool ; still, when
the smoke was very dense, an amount of irritation continued, which
materially interfered with the usefulness of the respirator. Thinking it
certain that the mechanically suspended matter would be intercepted by
the moistened woo!, 1 concluded that this residual irritation was due to
the TOporoua hydrooirbous generated during combustion : hence tlie
thought oE associating with the cotton-wool Dr. Stenhouse's exceUent
device of a charcoal respirator. The experiment was suecessfiJ. With
this combination it was possible to remain with comparative comfort.
for half an hour, or even an hour, in atmospheres a single inhalation
of which nntbout the rcspiralor wotild bo infoleraljiy painful.
Qiptiin Sluin', of the Mt'tropoUtaa Pire £rigjidt>, ha^ it'orkoil ener-
getically towards the completion of the respirator by associating with it
a smoke-cap. Mr. Sinclair has done the same, and he informs me that
the respirator is now in considerable demuid.
Having heard from Captain Shaw that, in some recent very trying
experiments, he had obtained the best effects from dry cotton-wool, and
thinking that I could not have been mistaken in my first results, which
proved the dry so much inferior to the moistened wool and its associat«d
charcoal, I proposed to Captain Shaw to bring the matter to a test at his
workshops in the city. He was good enough to accept my proposal, and
thither I went on the 7th of May. The smoke was generated in a con-
fined space from wet straw, and it was certainly very diabolical. At this
season of the year I am usually somewhat shorn of vigour, and there-
fore not in the beat condition for severe experinients ; still I wished to
teat the matter in my own person. With a respirator which had been
in use some days previously, and which was not carefully packed, I fol-
lowed a fireman into the smoke, he being provided with a dry-wo(d
respirator. I was compelled to quit the place in about three minotes,
while the fireman remained there for six or seven minutes.
I then tried his respirator upon myself, and found that vrith it I could
not remain more than a minute in the smoke ; in fact the first inhalalion
provoked coughing.
Thinking that Captain Shaw himself might have lungs more like mine
than those of his fireman, I proposed that he and I should try the
1874.] SUcHon ofFeUowa. 861
respirators ; but he informed me that his lunga were rerj atrong.
He was, howerer, good enol^^h to accede to my request. Poctdng the
respirator with greater care, I entered the den with Captain Shaw. I
could hear him breathe long, slow inhalatioDS ; and after the lapse of
seven minutes I heard him cough. In seven and a half minutes he
had to quit the place, thus proving that his lungs were able to endure
the irritation seven times as long as mine could bear it. I continued
in the smoke with hardly any discomfort for sixteen minutes, and cer-
tainly could have remained in it much longer.
During this time I was in n condition to render very material assistance
to a person in danger of suffocation.
The smoke-cap 1 wore was one made by Mr. Sincltur, which has a
mouthpiece similar to that used in the inhalation of nitrous oiide. But,
to show the care necessary in packing the respirator, it is only necessary
to remark that, with the packing furnished to me by Mr. Sinclair, it
was not possible for either myself or Ur. Cottrell to (x>ntinue in a dense
smoke for more than three minutes ; and even these were minutes of
laborious breathing. Flannel disks are employed in these respirators,
but I cannot recommend them. Cotton-wool carefully moistened and
teased is, in my opinion, much better.
It is always possible to associate fragments of lime with the respirator,
thus, if necessary, intercepting a portion of the carbonic acid. But in
most fires we have a more or less free circulation of air ; and I venture
to think that not in one case in n thousand of actual £res would the com-
bination of smoke and carbonic add be so noisome as it was in the
experiments here described.
The Society then adjourned over the Whitsuntide Becess, to Thurs-
day, Jime 11.
Jme 4, 1874.
The Annual Meeting for the election of Fellows was held this day.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
The Statutes relating to the election of Fellows having been read, Sir
James Alderson and General Boileau were, with the consent of the
Society, nominated Scrutotors to assist the Secretaries in examining the
lists.
The votes of the Fellows present having boon collected, the following
cuididates were declared duly elected into the Sodety : —
2e2
862 Messrs. H. E. Boscoe and A. Schuster m the [June 11,
Isaac Lowthian Bell, F.G.S.
W. T. Blanford, F.Q.S.
Henry Bowman Brady, F.L.S.
Thomas Lauder Brunton, M.D.,
Sc.D.
Prof. W. Kingdon Clifford, M.A.
Augustus Wollaston Franks, M.A.
Prof. Olaus Henrici, Ph.D.
Prescott a. Hewett, F.E.C.S.
John Eliot Howard, F.L.S.
Sir Henry Sumner Maine, LL J>.
Edmund James Mills, DJ3c.
Bey. Stephen Joseph Peny,
F.B.A.S.
Henry Wyldbore Eumsey, M J>.
Alfred E. C. Selwyn, F.G.S.
Charles William Wilson, Major
E.E.
Thanks were given to the Scrutators.
June 11, 1874.
JOSEPH DALTON HOOKER, C.B., President, in the Chair.
Mr. William Thomas Blanford, Dr. Thomas Lauder Brunton, Professor
W. Kingdon Clifford, Mr. Prescott Ot, Hewett, Mr. John Eliot Howard,
Dr. Edmund James Mills, the Eev. Stephen Joseph Perry, and Major
Charles William Wilson were admitted into the Society.
The Presents received were laid on the table, and thanks ordered for
them.
The following Papers were read : —
I. "Note on the Absorption-Spectra of Potassium and Sodium
at low Temperatures.^' By H. E. Boscoe, F.R.S., and Arthur
Schuster, Ph.D. Received April 30, 1874.
In order to obtain the absorption-spectrum afforded by the well-known
green-coloured potassium vapour, pieces of the clean dry metal were
sealed up in glass tubes filled with hydrogen, and one of these was then
placed in front of the slit of a large Steinheil's spectroscope furnished
with two prisms having refracting angles of 45° and 60°. The magnify-
ing-power of the telescope was 40, and was sufficient clearly to separate
the D lines with one prism. A continuous spectrum from a lime-light
was used, and that portion of a tube containing the bright metallic
globule of potassium was gently heated until the green vapour made its
appearance. A complicated absorption-spectrum was then seen, a set of
bands (a) in the red coming out first ; whilst after a few moments two
other groups appeared on either side of the D lines, the group /3 (less
refrangible) being not so dark as the group y. These bauds are all
shaded off towards the red, and in general appearance resemble those of
the iodine-spectrum. In order to assure ourselves that the bands are not
caused by the presence of a trace of an oxide, tubes were prepared in
1874.] Adsorption-Spectra qf Potttuwm and Sodium. 863
which thfi metal wu melted in hydrogen aeveral times on succefldTe dttys
until no further change in the bright charact«r of the globule could be
perceived. On vaporiEing the metal, which had been melted dowu to a
clean portion of the tube, the bands were seen as before, and came out
even more cleu'lj, the globnle, after heating, exhibitiBg a bright metallic
surface. An analyda of the potassium used showed that it did not con-
tfun more than 0*8 per cent, of sodium, although, of Course, the double
line D was always plainly seen.
In order to ascertain whether an alteration in the absorption-spectrum
of the metal tAkes place at a red heat, fragments of potassium were
placed in a red-hot iron tube, through which a rapid current of pure
hydrogen gas was passed, the ends of the tube being closed by glass
plates. The magnificent green colour of the ^-apour was clearly seen at
this temperature, on looking through the tube at a lime-light placed at tho
other end. Owing, doubtless, to the greater thicknees or increased pres-
sure of the vapour, the bands seen by the previous method could not be
resolved by the small spectroscope employed, the whole of the red being
absorbed, whilst a broad absorption-bond in the greenish yellow was seen
occupying the place of the group y.
The poutions of the bands obtained by the first method were measured
by means of a telescope and distant scale, and the wave-lengths obtained
by an interpolation curve, for vhich well known air-lines were taken as
references. The following numbers give the wave-lengths of the most
distinct, that is, the most refrangible edge of each band. As the
measurements had to be made quickly, owing to the npid darkening
of the glass by the action of the metallic vapour, these numbers do not lay
claim to very great accuracy, but fably represent the relative positions
of the band, and show that they do not always occur at regular intervals,
although they are pretty regularly spread over the field and all are
shaded alike.
Bands of potassium shaded off towards red. Wave-lengths in tenth-
metres : —
fiS44-l
6459")
67«H
6430
fi7l()
6400
6666
1 6379 I
r 6357 f
6615
6672
6350
6534
6331
6494 J
6322)
6311 1 5949 1 5763'
6300 I a 6930 I j3 5745
6275 J 5901 J 5732
60591 6860 ■) 5712
6033 6842 1
6012 yp 6821 y
5988 I 5802 ' ■ 6674
5964J 578lJ 5667
5700
The bright potassium-lines in the red and violet n'ere not seen re-
versed, the intensity of the lime-light being too small at both extremes to
render an observation possible.
In order to ascertain whether the vapour of sodium, which, when seen
in thin layers, appears nearly colourless, exhibits similar absorption-bands.
864
Frof. Owen an the alleged EsMenee qf [Jime llj
tabes contaming the pure metal, which had been manufoctnred and pie-
served out of contact with any hydrocarbon, were prepared, the metal being
obtained free from oxide and the absorptionnspectrum being obseryed in the
manner abeady described. As soon as the metal began to boil, a series of
bands in the blue (Na y) made their appearance, and shortly afterwards
bands in the red and yellow (Na a), stretching as far as the D lines, came
out. At this perjbd of the experiment the D lines widened, Uius blotting
out a series of fine bands occurring in the orange (Na /3), some of which,
consequenly, could not be mapped. All the bands of the sodium-flpec-
trum shade off, like th€r potassium-bands, towards the red.
When the vapour of sodium is examined in a red-hot iron tube, the
colour of the lime-light, as seen through it, is a dark blue. As the sodium
is swept away by the current of hydrogen passing through, the colour
becomes lighter, and the transmitted rays can be analyzed by the spectro-
scope. At first, the whole red and green and part of the blue is cut out
entirely. The D lines are considerably widened, and an absorption-band
is seen in the green, apparently coinciding with the double sodium-line,
which comes next in strength to the D lines. All the colours, therefore,
seem to be shut out, except part of the orange, part of the green, and the
ultra-blue. As the sodium-vapour becomes less dense, more light passes
through, and the same absorption-bands are seen as are observed in the
other method. The vapour then has a slight bluish-green tint, but is
nearly colourless.
The following numbers give the wave-lengths of the more refrangible
edge of the sodium absorption-bands in tenth-metres, obtained in the
manner above described: —
6668"^
6616
6552
6499
6450
6405
6361 T
6272]
>«
6235
6192
6162
6149
>a
6105^
6092
6071
6051
6035
6016
>P
y
5999
5150^
5129
5082
5038
5002
>y
4964^
4927
4889
4863
4832
4810
I
I
Plate ly. shows the general appearance of the two absorption-spectra.
II. '^ Note on the alleged Existence of Remains of a Lemming
in Cave-deposits of England.'^ By Professor Owen, C.B.,
F.R.S. Received April 25, 1874.
In the " Report on the Exploration of Brixham Cave" (Phil. Trans.
1873) it is stated (p. 560) : — " With the appearance in the cave of the
smaller common rodents now living in this country, we have to note a
remarkable exception, that of the Lemming {Lagomys spdceus)^ And
again, in the list of animal remains as determined by Dr. Palconer and by
7{oscoe * Sckii^tep.
Proc-ItoY'^'-:ocVolXM2
i< ^ ^ *' f f
* *'
.rf^. / ^./. ». .V,. *..- ... . >. ..' >.se.. ' • y;» '.i*^** •.VJiiir.r'.n tiul jrj«rr.»L ▼*
. '/ » « /. ' '/J**'/*. , «*;^./'. ,•• '^^li ' r. \ ^t u\r>' . Tuw*
• vfHr> ',// "v.. ' ■ -'.. / '/ * '^" 'V '..^ ''O^/' /•/♦«. i,:^A!f J t^^MtM^AJLZJL)
»A v/^» f*f,**'f^ffA f f* ^-f^, h»//f*f*h'i* ♦*>; ^9at.*^cf tJ^u^j tu^ifA Uff if V0A
'ifUff*'^-** »' •* /^A^ /^"^//»r.'^ ^''A///y'A»v« <Myx/lflt«;, ff»«i » <^!^>rit
i/^ ,«/ ,. '/v v«// •^rf'>^ /^4^^ •*/«^r'V/rv, ^n^^ru^^ with fCUj/hn$ jf^m^
//*/////^ '/ '^^ // ■/.//,./#// / //r*/ #*//^«#>. ^^.i/mpi •// tf^ iMtitlly ^A " Vokw**
i Af'*i*of*fh* , »,*/> *A ' Wn-f it ' ' //^//'// <//'/^/ ; >/•<♦, 0#i-, f//it«il ff/m **lfi/5 iiur-
i\U\**t*^ y **'v' I »»;/j/'v*#* T^'/^/< *!#/; i',if/iHH (lAnUi Jtlvi, /ij(«. 12, J'J^ to
l*«. PH^'t'f/ ^'^*^•'l *'/ A'/7////v//«, Aff/J «y* Oi<j ft«if/*i$ •JHs'ri'* 'UtUinititihti
Htttt ti**ttff*l f\t ^i-y i*'j* ''^. ''/, ''1; f/i U^i ' |}riii«h K'AtiiJ Miir/jmAJii '
/I'M'^/ '^'^ «}/"'Mf'N w»\ffh.t**ji Uf mi. \ty \fr. Hwk\ikw\ wan found
\tf \U» Ih t ^* Vl iUi* t / itt V,nit\'» WnU-, '\*tri\ut^y, AfM iwhk^Um a
l«if(^' f \fft\t*t*^''ft, fA ^U* ifl"«ll Oii^ff f|»<t i>|Hw-)fiii-ii tif/iint<| ill Uid ''l(4?|K/ri''
hwNf 0#'- ihtfUnm t Hit |t lif i«/M|ifii)x M I'lltA, or UiiJJ<fifN IIai*!), ikiI a
lii itttnttttt An/I Mi' '1/ <'M/*ofNiioo of ihn tinyiimi or ilrni tivUUintvi of
f.tiifiitni/t mfofftut, untf lit Mfi- llMhitli MMMdiiff, l<«<l ifMi aIimi Uf nmiArk :—
*'\ittii»-iA M«/ ' o' <of«Mi«iif/i M iiM«o«liiif/ fl.H fliiM'oviiry, nor any rlittnud4;r
fl« «lo' 4lfl<' ^MffM ft* mUoii HI «)fMfM<«it nhilit, IlifllrAlii il. to Imi fill oMor
Im.iiii) llfMO <lf< |ii "i« *iu»\ \tt.\\i of lli«t Hitn^H, UiilfMU, Kinlil voliiN, or
VVifi* » Y^J« M hImii'I/ <I'mmiIm<1 , yi I. if iiJM|i<«:Hl)otiiilfly uMi^nU Uio former
i.aliiifiiM io I'/oi/Imo'I of II it\it.t\t.n of I'oiliiiil, wlionn ffi^iiiiN not only is
MUM )o*-' ol«<l iif lli'< jHitK.iil ijfiy III our Mrllinli fiiiiim, but hfut long
if.iftMMJ Im «-«|hI Io Noy jMifl ol IIm. roiiMiii>nl of Kiirfipn " (* Hritmh FosHii
AIihmimiiIm, |f 0 1/ llii- lft.iiiiiiiii|iii nUH iliHliirli, by tlmir multitudiuous
iiil|iittloi y •« •iiHiiM, Hii« biiMbifH'biiiiii ol hrMiiiliimviii.
1874.] i>iilinni^-T»»<iuw in Sngland. 865
Mr. Busk, there occurs (p. 656): — "IQ. Lagomyt tpeVxia. Lemming..!."
Thia is throughoat the " Beport " treated as an original diacoTery,
the importance of which ie impressed upon the Xloyal Society by the
remark : — " This cdrcumstance tends to give a greater antiquity to a por-
tion of the smaller remains than from their condition and position we
might have been disposed to assign to them" (t6. p. 560, note). These
remains are referred to " the smaUer common rodenta now living in this
country," viz. " Hare, Babbit, Water-rats," " at least two species of Ami'
eokt" (ib. -p. 548).
The auppoaed existence of remains of a Grisly Bear in the Brixham
Cave (Mr. Busk having " reason to believe that beai^remains referred
to Crtiu prUem belong in fact to Unut ferox" — an "important deter-
mination") leads to the remark: — " The presence of another small Korth-
American animal has been ascertained, viz. the Lemming " (i6. p. 556).
At the datd of publication of my ' British Fossil Mammals,' it is true
that no fossil evidence of a Lenmiing {Otoryehus, Bliger ; Lemmua, Link)
had come to my knowledge ; but I have since obtained such of species
of both Spermojphihit and Oeoryehtu, the latter nearly allied to, if not
identical with, the Siberian Lemming (Oeon/ehm aipalax), from a deposit
of lacustriAe brick-earth near Salisbury, associated with Elephaa primi-
genias. The Lemmings, I may remark, belong to the family of "Voles"
{Arvkolida), not of "Hares " (Leporidce) ; but the fossil from " the sur-
face of the cave-earth far in the Beindeer gallery " of the Brixham Cave
(Beport, p. 558) appears from the figures (plate xlvi. figs. 12, 13) to
be rightly referred to Lagomys, and to the same species determined
and named (p. 213, figs. 82, 83, 84) in the < British FosaU Mammals '
(1846). The specimen submitted to me by Dr. Buckland was found
by the Bev. Mr. M'Enery in Kent's Hole, Torquay, and includes a
larger proportion of the skull than the specimen figured in the "Beport"
from the Brixham Cave. It is evidently a Pika, or tailless Hare, not a
Lemming. And the determination of the original or first evidence of
Lagomys gpdaiu, now in the British Museum, led me also to remark : —
" None of the circumstances attending its discovery, nor any character
deducible from its colour or chemical state, indicate it to be an older
fossil than the jaws and teeth of the Hares, Babbits, Field-voles, or
Water-voles already described ; yet It unquestionably attests the former
existence in Bngland of a species of rodent, whose genua not only is
unrepresented at the present day in our British fauna, but has long
ceased to exist in any part of the Continent of Europe " (' British Fossil
Mammals,' p. 213). The Lemmings stiU disturb, by their multitudinous
migratory awanns, the husbandmen of Scandinavia.
806 Mr. B. Mallet on the alleged [Jonc 11^
in, " On the alleged Expansion in Volume of various Substancea 1
in passing by Kefrigeration from the state of Liquid Fusioa i
to that of Solidification." By Robert Mallet, C.E., P.B.&. |
Received April 28, 1874.
(Abstract.)
Since the time of Rijanmur it has been stated, with very rarioc
degreea of eridence, that certain meta5a expand in volume at
their points of consolidation from fusion. Bismuth, cast iron, antimony-;; j
flilver, copper, and gold are amoDgat the number, and to these hare
recently been added certain iron fumace-slaga. Considerable physici"
interest attaches to this subject from the analogy of the alleged fat^ta t
the well-known one that water expands between 39° F, and 32°, at whi
it becomes ice ; and a more extended interest has been given to it quite
recently by Messrs. Nasmyth and Carpontor having made the suppc
facts, more especiitlly those relative to cast iron and to s
foundation of their peculiar theory of lunar volcanic action as devolop€
in their work, ' The Moon as a Planet, as a World, and a SatoUito^
(4to, London, 1874), There is considerable ground for believing thal)^
bismuth does expand in volunie at or near consolidation ; but with
reapeet to all the other subBtancea supposed to do likewise, it ia the
object of this paper to show that the evidence is insufGcient, and that
with respect to cast iron and to the basic silicates constituting inm
slags, the allegation of their expansion in volume, and therefore that
their density when molten is greater than when solid, ia wholly
erroneous. The determination of the specific gravity, in the liquid,
state, of a body having so high a fusing temperature ae cast iron is
attended with many difficulties. By an indirect method, however, and
operating upon a sufficiently targe scale, the author has i^en enabled to
make the determination with considerable accuracy. A conical vessel of
wrought iron of about 2 feet in depth and 1-5 foot diameter of base, and
with an open neck of 6 inches in diameter, being formed, was accurately
weighed empty, and also when filled with water level to the brim ; the
weight of its contents in water, reduced to the specific gravity of distilled
water at 60° F., was thus obtained. The vessel being dried was now
filled to the brim with molten grey cast iron, additions of molten metal
being made to maintain the vessel full until it had attained its maximum
temperature (yellow heat in dayhght) and maximum capacity. The
vessel and its content of cast iron when cold were weighed agaiu, and
thus the weight of the cast Iron obtuned. The capacity of the Teasel
when at a maximum was calculated by applying to its dimensions at 60°
the expansion calculated from the coefficient of hnear dilatation, as given
by Laplace, Biemann, and others, and from its range of increased tem-
perature ; and the weight of distilled water held by the vessel thus ex-
1874.] SxpanrioH ofvariout Stibtttmett on 8oli^^fieaHm^. 867
pandad waa calcalsted from tbfi weight of its contonte when the Teeiel
and water were at 60° F.
We have now, after applying some sm^ correctionH, the elements
necesBoiy for detemuning the specific gravity of the cast iron which filled
the Tessel when in the molten state, having the absolute weights of equal
volumes of distilled water at 60° aud of molten iron. The mean spe-
cific gravity of the cast iron which filled the vessel was then det^mined
by the usual methods. The final result is that, whereas the specific
gravity of the cast iron at 60° F. was 7*170, it was only 6-650 when in
the molten condition ; cast iron, therefore, is less dense in the molten
than in the solid state. Nor does it expand in volume at the instant of
consolidation, as waa conclosively proved by another experiment. Two
similar 10-inch spherical shells, 1*5 inch in thickness, were heated to
nearly the same high temperature in an oven, one being permitted to
cool empty as a measure of any permanent dilatation which both might
sustain by mere heating and cooling again, a fact weU known to occur.
The other shell, when at a bright red heat, was filled with molten
cast iron and permitted to cool, its dimensions being taken by accurate
instruments at intervals of 30 minutes, until it had returned to the
temperature of the atmosphere (53° F.), when, after applying various
corrections, rendered necessary by the somewhat complicated conditions
of a spherical mass of cast iron losing heat from its exterior, it was
found that the dimensions of the shell, whose interior surface was in
perfect contact with that of the solid ha^ which filled it, were, within
the limit of experimental error, those of the empty shell when that also
was cold (53° F.), the proof being conclusive that no expansion in
volume of the contents of the shell had token place. The central portion
vras much less dense than the exterior, the opposite of what must have
occurred had expansion in volume on cooling taken place.
It is a fact, notwithstanding what precedes, and is well known to iron-
founders, that certain pieces of cold cast iron do float on molten cast
iron of the same quality, though they cannot do so through their
buoyancy. As various sorts of cast iron vary in speciGc gravity at
60° F., from nearly 7'700 down to 6"300, and vary also in dilatability,
some cast irons may thus float or sink in molten cast iron of different
qualitiea from themselves through buoyancy or negative buoyancy alone ;
but where the cold cast iron floats upon molten cast iron of less specific
gravity than itself, the author shows that some other force, the nature
of which yet remuns to be investigated, keeps it floating ; this the author
has provisionally called the repellent force, and has shown that its
amount is, casteris paribus, dependent upon the relation that subsists
between the volume and "effective" surface of the floati]]g piece. By
" effective " surface is meant all such part of the immersed solid as is in
a horizontal plane or can be reduced to one. The repeUent force has
also relations to the difference in tempentore between the solid and tite
molten metal on which it floats.
Dr. B. Sanderson on the Excitation of the [June
1
The author then extendti hu experimeote to lead, a metal known
contract greatly in solidifying, and, with respect to which, no one has bi
geflt«d that it eipanda at the moment of consolidation. He finds that piece*
of lead having a epecific gravity of 11'361, and being at 70° I"., float or
sink upon molten lead of the Bame quality, whose calculated specific
grarity was 11-07, according to the relation that aubsist-a between the
volume and the •' effective " surface of the solid piece, thin pieces with
large surface always floating, and vice vend. An eiphmation is offered
of the true cause of the ascending and descending current* observed in
very large " ladlea " of liquid cast iron, ag stated by Messrs. Nasmvtfa
and Carpenter. The facts are shown to be in accordance with those
above mentioned, and when rightly interpreted to be at variance with
the views of these authors.
Lastly, the author proceeds to examine the statements made by these
writers, as to the floating of lumps of solidified iron fnmace-slag upon
the same when In a luolten state ; be examines the conditions of the
alleged fact«, and refers to his ovm experiments upon the total contrac-
tion of such slags, made at Barrow Iron-works (a fuU account of
which he has given in his paper on " The true Nature and Origin of
Volcanic Heat and Energy," print<;d in Phil. Trans. 18T3 ), as eonclusivelT
proring that such rtl;ii;s are not denser in Ike molten than in the solid
ettiin), and that the jloatiug referred to is due to other causes. The
author returns thanks to several persona for ^cilities liberally afforded
him in making these experiments.
IV. " Note ou the Excitation of the Surface of the Cerehral Hemi-
spheres by Induced Currents," By J. Bubdon Sanderson,
M.D,, F.R.S., Professor of Practical Physiology in University
College, London. Received April 30, 1874.
In a paper recently communicated to the Boyal Society by Dr. Ferrieaf
(Proceedings, No. 151) it is shown that when two ends of copper wire
distant from each other not more than a couple of millimetres, and in
metallic communication vritb the terminals of the secondary coil of •
Du Bois's induction-apparatus in action, are apphed to certain spots of tike
surface of either hemisphere, and great intensity is given to the induced
currents thereby directed through the hving tissue, by previously bringing
the secondary coil into such a position that it is very dose to the primUT
coil or even partially covers it, characteristic combined movements of the
opposite side of the body are produced.
With reference to these effects, it was observed by Dr. Ferrier (1) that
excitation of the same spot always produces the same movement in the
same animal, (2) that the area of excitability for any given movement
(or, as it may be called for shortness, tite active spot) is extremely smalt
and admits of very accurate detiuition, and (3) that in different animals
1874.] Bram-tttiface by Induced Current: 869
ezcitatjona of anatomicallj correflponding spota produce Bimilar or corre-
sponding results. Prom these remark&ble facts and from otliers similar
to them relating to other parts of the brun to which I do not now advert,
it was inferred that, at the surface of the hemispheres, certain " centres "
are to be found, of which it is the function to originate combined or even
purposive movements.
To this inference objections have been recently raised by Dr. Dupny,
baaed on the results of eiperiments made by him, in which he found that,
after the ablation of those parte of the hemispheres which contain the
supposed centres, movements, similar to those described by Dr. Ferrier, can
still be produced by electrical exdtation of the cut surface. In com-
menting on these counter experiments. Dr. Ferrier has since pointed out
that the effects described by Dr. Dupuy are entirely different from those
observed by himself, and, particularly, that the movements produced in his
experiments are of an uncertain character, affecting sometimes one, some-
times several groups of muscles.
As it appeared to me that, although Dr. Dupuy has failed to prove that
the movements he described are of the same nature with those described
by Dr. Ferrier, the latter has not proved that they are different, I
thought it necessary to make a series of eiperiments for the purpose of
clearing up this uncertainty. With this view I determined to investigate
the most chaiacteristic of the comtnned movements, so accurately described
by Dr. Ferrier as produced by excitation of particular spots on the anterior
part of either hemispliere, by comparing them with those produced by
excitation of deeper ports. The results of my experiment*, in which cats
were employed, are as follows : —
1. By removing the integument, skull, and dura mater to an extent
corresponding to the anterior half of the right parietal bone and the
adjoining thin portion of the frontal bcme, an wea of the surface of the
bmin is brot^ht into view which comprises several spots by the excita-
tion of which the following charact«ristic movements can'be produced: —
(1) Betraction of the left fore paw, with flexion of the carpus, accom-
panied by similar movements of the left hind 1^. (2) Closure of the
left eye and elevation of the left npper lip. (3) Betraction of the left
ear. (4) Eotation of the head to the left side.
The active spots for these several movemente are as foUows :— For (1),
a point immediately behind tiie outer end of the crudal sulcus ; for (2),
the Buri'ace about the outer end of a sulcus which lies immediately behind
(1); for (3), the surface behind the sulcus last mentioned ; for(4),aspot
about a centim. fori^her back on the same convolution. Movements (1),
(2), and (3) can be produced in the cat with very great certainty, and ttie
active spots for them are well defined. Their limits and relations are
in exact accordance vrith the statements of Dr. Ferrier.
2. If that part of the surface of the ri^t hemisphere which comprises
the active spots above mentioned is severed from the deeper parte by a
870 On the Excitation of the Brain-»ur/ace. [June llj
nearly homoutal incision made with a thin-bladed knife, ajid the iostni-
ment ia at once withdrawn, without dialocatiou of the severed part, and
the excitation of the iictive spots thereupon repeated, the residt is tho
same aa when the surface of the uninjured oi^n is acted upoD.
If a Himiliir incision ia made in a parallel plane, but at a lower level,
this is not the case ; but on removing the flap and applying the electrodes
to the cut surface, it is found that there are on it active spots, which, aa
regards the effect of oscitation, have the same properties as the actdve
spots previously observed on the natural surface, and that the latter hayo
the same topographical relation to each other as the fonuer.
3- In a brain hardened in alcohol a needle plunged vertically, t, e. at
right angles to the surface, from the active spot for retraction o£ the
opposite ear, reaches the posterior part of the corpus slriatnm at a
depth of from 10 to 12 milluns. If a horizontal incision is made in
the living brain, at this depth, and is met by tu'O others, of which one ia
directed antero-post«riorly and the other transversely, and the part
comprised within the incisions removed, a surface of brain is exposed in
the deepest part of the n'ound which corresponds to the outer and upper
part of the corpus striaiicm'. If now the electrodes are applied to this sur-
face, the movements (I), (2), (3) are produced in the same way aa before,
but more distinctly; the active spots are ciiiitc as striclly localized, and
their relations to each other are the same as at the surface — the spot tor
the movement of the extremities being in front, that for the closure of
the eye and retraction of the upper lip being to the outaide, and that for
the ear behmd.
From these facts it appears that the superRcial convolutions do not
contain organs which are essential to the production of the combinations of
muscular movements now in question. They further make it probable
that the doctrine hitherto accepted by physiologists, that the centres for
such movements are to be found in the masses of grey matter which lie in
the floor and outer wall of each lateral ventricle, is true.
* In case it should be aecessar; U> repeat Ihie eiperimenC, it vill be found best (after
having noted the effects of exciting the surface at the several active spots and MOar-
taiDed the degree of eicitation required for tbe production of the correepondiag movB-
ments) to proceed to remove tbe part of the braio containing (bem, bo m to expose tbs
outer aspect of ^e sn1«rior part of tbe corpai i/riatum at once ; and then, as aoon M
biemorrhage bas cessed. to investigate tbe relatiTe positions of the active spots on the
surfaoe so exposed. [Since tbe attoie paper was communicated. I have ascertained that
at the lowest part of this aurfnce there is a spot, of nhich eicitation induces opening ot
the mouth and alternate protrusion aad retraction of the tongue — a group of move-
ments vhich Dr. Ferrior baa localised on tbe under surface of tbe brain, in front of the
Sjlvion fissure,— J. B. 8., June 3, 1874.]
I874.J Mr. J. K. Lockyer's Speeinmopie JVoiat.— No. I. 871
v. " Spectroscopic Notes. — No. I. On the AbsorptioiL of great
Thicknesses of Metallic and Metalloidal Vaponrs." By J.
NoKHAN LocKyKK, F.R.S. Received April 20, 1874.
It has been assuiued hitherto that a great ihidcntu of a, gas or rapour
causes its radiation, and therefore its absorption, to assume more and
more the character of a continuous spectrum as the thickness is
increased.
It has been shown by Dr. Frankland and myself that such a condition
obtains when the demity of a vapour is increased, and my later researches
have shown that it is brought about in two ways. Qenemlizing the
work I have already done, without intending thereby to imply necessarily
that the rule will hold universally, or that it exhauBts all the phenomena,
it may be stated that metallic elements of low specific gravity approach
the continuous spectrum by viidening their lines, while metallic elementa of
high epedJic gravity approach the continuous state by increasing the
number of their lines. Hence in the vapours of Ka, Ca, Al, and Mg
we have a small number of lines which broaden, few short lines being
added by increase of density ; in Pe, Co, Ni, &c. we have many lines which
do not so greatly broaden, many short lines being added.
The obsen'ations I made in India during the total solar eclipse of 1871
were against the assumption referred to ; and if we are to hold that the
lines, both "fundamental" and "short," which we get in a spectrum, ore
due to atomic impact (defining by the word atom, provisionally, that mass
of matter which gives us a line-spectrum), then, as neither the quantity
of the impacts nor the quality is necessarily altered by increasing the
thickness of the stratum, the assumption seems also devoid of true
theoretical foundation.
One thing is clear, that if the assumed continuous spectrum is ever
reached by increased thickness, as by increased density, it must be reached
through the " short-line " stage.
To test this point I have made the following experiments : —
1. An iron tube about 5 feet long was filled with dry hydrogen;
pieces of sodium were carefully placed at intervals along the whole
length of the tube, except dose to the ends. The ends were closed with
glass plates. The tube was placed in two gas-furnaces in line and
heated. An electric tamp was placed at one end of the tube and a
spectroscope at the other.
When the tube was red-hot and filled with sodium-vapour throughout,
as nearly as possible, its whole length, a stream of hydrogen slowly
passing through the tube, the line D was seen to be absorbed ; it was no
thicker than when seen under similar conditions in a test-tube, and far
thinner than the line absorbed by sodium- vapour in a test-tube, if the
density be only slightly increased.
1
372 Mt. J. N. Lockyer's Spectrcseopic Notea. — No. II. [June 1:
OiJy the longest " fundamental " line was abaorbed.
Tht line liiat thieker than the D line in the solar jiperlrunt, in which tptO"
trum all the thort lint* are reversed.
2. As it was difficult largely to increase either the temperature or tbe
density of the a odium- vapour, I have made another seriea of experiments
with iodine -vapour.
I have already pointed out the differences indicated by the spectro-
scope between the quality of the vibrations of the " atom " of a metal
and of the " subatom " of a metalloid (by which t«rm I define that mas^
of mntter which gives us a spectrum of channelled spaces, and builds up
the continuous Bpectnmi in it« own way). Thus, in iodine, the short lines,
brought about by increase of density in an atomic apectmm, are repre-
sented by the addition of a system of well-defined "beats" and broad
bauds of continuous absorption to the simplest spectrum, which is one
exquisitely rhythmical, the intervals increasing from the blue to the red,
and in which the beats are scarcely noHeesble.
On increasing the density of a very small thickness by a gentle
heating, the beats and bands are introduced, and, as the density is atill
further increased, the absorption becomes continuous throughout the
whole of the visible spectrum.
The absorption of a thickness of .') feet R inches of iodine-vapour at a
temperature of 59' F. has given mo no indication of banda, while the
beats were so faint that they were scarcely visible.
VI, " Spectroscopic Notes. — ^No. II. Ou the Evidence of Varia-
tion in Molecular Structure." By J. Norman Lockyer, F,R.S.
Received May 26, 1874.
1. In an accompanying note I have shown that when different degrees
of dissociating power are employed the spectral effects are different.
2. In the present note I propose to give a preliminary account of some
researches which have led me to the conclusion that, startiBg with a mass
of elemental matter, such mass of matter is continually broken up as the
temperature (including in this term the action of electricity) is raised.
3. The evidence upon which I rely is furnished by the spectroscope in
the region of the visible spectrum.
4. To b^in by the extreme cases, all solids give us continuous spectrs;
all vapours produced by the high-tenslou spark give us line-spectra.
5. Now the continuous spectrum may be, and as a matter of fact is,
observed in the case of chemical compounds, whereas aU compounds
known as such are resolved by the high-tension spark into their consti-
tuent elements. We have a right, therefore, to assume that an element
in the solid state is a more complex mass than the element in a state of
vapour, as it« spectrum is the same as that of a mass which is known to
be more complex.
1874.] Mr. J. N. Lockyer*fl Speciroscopie Notea.—Vo. II. 378
6. The spectroscope sapplies as with intennediate stages between these
extremes.
(a) The spectra vary as we pass from the induced current ^dth the
jar to the spark without the jar, to the voltaic arc, or to the highest
temperature produced by combustiotL. The change is always io the same
directioD ; and here, agai^, the spectrum we obtain from elements in a
state of vapour (a spectrum characterized by spaces and bands) is similar
to that we obtain from vapours of whi<^ the compound nature is un-
questioned.
0) At high temperatures, produced by combustion, the vapours of some
elements (which give us neither line- nor channelled space-spectra at those
temperaturea, although we undoubtedly get line-spectra when electridty is
employed, as stated in 4) give us a continuous spectrum at the more
refrangible end, the less refrangible end being anaIEect«d.
(y) At ordinary temperatures, in some cases, as in selenium, the more
refran^ble end is absorbed ; in others the continuous spectrum in the
blue is accompanied by a continuous specfrum in the red. On the
application of heat, the spectrum in the red disappears, that in the blue
remains ; and further, aa Faraday has shown in hu researches on gold-
leaf, the masses which absorb in the blue may be isolated from those
which absorb in the red. It is well known that many substances known
to be compounds in solution give uh absorption in the blue or blue and
red ; and, also, that the addition of a substance known to be compound
(such as water) to substances known to be compound which absorb the
blue, superadds an absorption in the red.
7. In those cases which do not conform to what has bete stated the
limited range of the visible spectrum must be borne in mind. Thus I have
little doubt that the simple gases, at the ordinary conditions of tempera-
ture and pressure, have an absorption in the ultrn-violet, and that highly
compound vapours are often colourless because their absorption is beyond
the red, with or without an absorption in the ultra-violet. Glass is a
good case in point ; others will certainly suggest themselves as opposed
to the opacity of the metals.
8. If we assume, in accordance with what has been stated, that the
various spectra to which I have referred are really due to different mole-
cular aggregations, we shall have the following series, going from the
more simple to the more complex : —
First stage of complexity 1 Lin^„^trum.
of molecule J
Second stage Channelled space-spectrum.
(Continuous absorption at the blue
end not reaching to the less refran-
gible end. (This absorption may
break up into channelled spaces.)
374 Mr. J. N. Lockyer's Speclroseopic Notet. — No. III. [Jane l)j
{Contitiiioua absorption ftt the red end
Dot readuni; to the mora refr^iH
gible end. (This absorption ia\j
break up into channelled spaces.)
Fifth stage Unique continuous absorption.
9. I shall coutput myself in the present note by giving one or fcwqr'l
inatanceR of the pnssti^ of spectra Erom one st^^ to another, beginmng^u
at the fifth stage.
From 5 to 4.
1. The absorption of the vapours of K in the red-hot tube, described
in another uote, is at first continuoufi. Ah the action of the heat ia cou-
tinned, this continuous spectrum breaks in the middle ; one i>art of it
retreats to the blue, the other to the red.
From 4 to 3.
1. Faraday's researches on gold-leaf best illustrate this ; but 1 1
that my explanation of them by massen of two degrees of complex
only is nuificient without his conclusion (' Besearches in Chemistryd
p. 4171, that they exist " of intermediat« sizes or proportions,"
From 3 to y.
1. Sulphur-vapour first gives a continuous spectrum at the blue end ;
on heating, this breaks up into a channelled space-spectrum.
2. The new spectra of K and Na (more particularly referred to in the
third note) make their appearance after the continuous absorption in t^e
blue and red vanishes.
From 2 to 1.
1. In many metalloids the spectra, without the jar, are channelled; on
throwing the jar into the circuit the line-spectrum is produced, while tlie
cooler exterior vapour gives a channelled absorption-spectrum.
2, The new spectra of K and Na change into the line-spectrum (with
thick lines which thin subsequently) as the heat is continued.
VII. " Spectroscopic Notes.— No. III. On the Molecular Stnic-
hire of Vapours in connexion with their Densities." By J.
NoEMAN LocKYER, F.R.S. Received May 26, 1874.
1. I have recently attempted to bring the spectroscope to bear upon
the question whether vapours of elements below the highest tempera-
tures are truly homogeneous, and whether the vapours of different
chemical elements, at any one temperature,- are all in a similar molecular
condition. In the present note, I beg to lay before the Boyal Society the
preliminary results of my researches.
1874.] Mr. J. N. Lockyer's SpectroteopicNotet.—tto. III. 875
2. We start with the following facts : —
I. All elements driTen into vapour by tha induced current give line-
Bpectra.
II. Most elements driven into vapour bj the voltaic arc give us the
III. Many metalloids when greatly heated, some at ordinary tem-
peratures, give us chaimelled-space spectra.
rV. Elementa in the solid state give us continuous spectra.
3. If we grant that the spectra represent to us the vibratdons of dif-
ferent molecular aggregatioos (this question is discussed in Note II.),
spectroscopic observations should furnish us with facts of some import-
ance to the inquiry.
4. To take the lowest ground. If, in the absence of all knowledge on
the subject, it could be shown that all vapours at all stages of temperature
had spectra absolutely similar in character, then it would be more likely
that all vapours were truly homogeneous and similar among themselves,
as r^ards molecular condition, than if the spectra varied in character, not
only from element to element, but from one temperature to another in
the vapour of the same element.
5. At the temperature of the sun's reversing layer, the spectra of all
the elements known to exist in that layer are apparently similar in cha-
racter— that is, they are all line-spectra ; hence it is more probable that
the vapours there are truly homogeneous, and that they all exist in the
same molecular condition, than if the spectrum were a mixed one.
6. The fact that the order of vapour-densitiea in the sun's atmosphere,
which we can in a measure determine by spectroscopic observations, does
not agree with the order of the modem atomic weights of the elements,
but more closely agrees with the older atomic weights, led me to take up
the present research. Thus I may mention that my early observations of
the welling-up of Mg vapour all round the sun above the Na vapour have
lately been frequently substantiated by the Italian observers ; so that it
is beyond aU question, I think, that, at the sun, the vapour-density of Mg
is less than that of Na.
7. The vapour-densitdoa of the following elements have been experi-
mentally determined : —
H
K
s ...
. . . 32 (at 1000°)
I ...
.. 127
Hr..-
. .. 100
N ...
.. 14
0 ...
.. 18
p ...
.. 62
a
8. To pursue this inquiry the following arrangements have been
adopted ; —
llie first experiment! were made laat December upcm Zn in a glass
TOL. XXII. 2 4
376 Mr. 3 . ti .'Locii.yet'a Spectroscopic Nolea. — No. III. [June II,
tube biased at each end with glass platca ; and I have to express my ob-
ligations to Dr. Kujiaell for allowing them to be conducted in his labora-
tory, and for miicU usBistaucv and counsel eonoorning them.
A stream of dry H was allowed to pass. The tube was heated in a
Hofmann'e gas-furnace, pieces of the metal to be studied having previ-
ously been introduced. It was found that the glass tube melted ; it was
therefore replaced by an iron one. The inconvenience of this plan, how-
ever (owing to the necessity for introducing the metal into the end of the
hot tube nhen the first charge had volatiliEcd), and, moreover, the
insufliciency of the heat obt^nable from the gas-furnace, soon obliged ma
to replace both tube and furnace by others, whicli have now been in use
for manv weeks, and which still continue to work most satisfactorily.
The iron tube is 4 feet in length, nnd is provided with a central en-
largement, suggested lo me by Mr, Dewar. forming a T-pieee by tha
screwing in of a side tube, the end of which is left projecting from the
door in the roof of the furnace. Caps are screwed on at each end
of the main tube ; these caps are closed by a glass plate at one end,
BJid have each a small side tube for the purpose of passing hydro-
gen or other gases through the hot tube. The furnace is supplied
with coke or charcoal ; an electric lamp, connected with thirty Grove's
cells, is placed at one end of the tube and a one-prism spectnwcope at the
other. The temperatures reached by this furnace may be conveniently
divided into four stages :-:—
I. When the continuous spectrum of the tube extends to the sodium-
line D, this line not being visible.
II. When the continuous spectrum extends a little beyond D, this line
being visible as a bright line.
III. When the spectrum extends into the green, D being very bright.
IV. "WTien the spectrum extends beyond the green and D becomes in-
visible as a line, and the sides of the furnace are at a red heat.
I may add (1) that I have only within the last few days been able to
employ the third and fourth stages of heat, as the furnace was previously
without a chimney, and the necessary draught could not be obtained ;
and (2) that I was informed, a little time ago, by Prof. Roscoe that, with a
white-hot tube, he had obsen'ed new spectra in the case of Na and K.
These spectra, which I now constantly see when these temperatnrea are
reached, I shall call the " new spectra."
9. The results of the experiments, so far as the visible spectrum is
concerned, between the stages indicated may be stated as follows : —
H. No absorption.
N. No absorption.
K. I have observed, either separately or together :—
(a) The line absorption-line near D.
(/3) Continuous absorption throughout the whole spectrum.
(7) Continuous absorption in red and blue at the same time,
\
1874.] Mr. J. N. Lockyer'a Spectroscopic Nole».—No. III. 377
the light being transmitted in the centre of the spectrum
(as by gold-leaf).
{S) Continuous absorption clinging on oae side or other of
the line. (This phaaomenon, which, so far aa I know,
is quite new, will be described in another note.)
(t) The new spectrum.
Na, 1 have observed, either separately or together : —
(n) D absorbed.
(/3) ContiQuous abeorption throughout the whole spectrum,
(y) Continuous abearptian clinging on one side or the other
of D.
(i) The new spectrum.
Zn. Continuous absorption in the blue. (An unknown line some-
times appears in the green, but certainly no line of Zn.)
Cd. Continuous absorption in the blue.
Ah. Xew spectrum, with channelled spaces and ^Morptiou ii) the
blue.
P. The same. (Thia, however, in consequence of the extreme deli-
cacy of the spectrum, requires confirmation.)
S. Chonnelled-space spectrum (previously observed by Salet).
As. Probable channall^-space spectrum. (Observations to be re-
peated.)
Bi. Ko absorption.
I. Channelled spectrum in the green and intense bank of general
absorption in tiie violet, where at the ordinary temperature
the vapour transmits light.
Hg. No absorption.
10. These results may be tabulated as follows : —
No visible absorption.
Line absorption.
Probable channelled-space absorption.
Continuous absorption in the blue.
Channelled-space absorption + band of
abeorption in violet.
No abeorption.
62
31
(?)
23
Line absorption.
(?)
65
Continuous absorption in the violet.
(?)
122
Channelled-space spectrum and absorption
in the blue.
32
32
Channolled-apsce spectrum.
(?)
SOS
No abiorptioD.
26%
J.N. hockycr's Spectroscopic Notes. — No, IV. [June llj
11. It will be aeeu from the foregomgatatement that if similar spectra
be taken as iudicatiug aimilar molecular conditions, then the ^'apours,
the densities of which have been determinod, have not been in the same
molecular condition among thL>mselvcs. Thus the vapours of K, 8, and
Cd, at the fourth stage of beat, gave us line, channelled-space, and con-
tinuous absorption in the blue respectively. This is also evideni-e that
each vapour is non-homogeneous for a considerable intc^^al of time, t^
interval being increased as the temperature is reduced.
VIII. " Spectroscopic Notea. — No. IV. On ancwClassof Absor]K
tion PhDnomena." By J. Nokman Lockykh, P,R.S. BecetredL'
May 2G, 1874.
1. In the eiperiments on the aba orpt ion-spectrum oE Na and K
vapour heated in a red-hot tube, to which further reference ta made in
aeparat« notes, I have observed phenomena quite new to me, some
rough drawings of which 1 lay herewith before the Boyal Society. As
the phenomena are only momentary, I cannot answer for the final accu-
racy of the drawings, nor have I been able to represent the softness of
the gradations of shaile.
2. In the drawings, the red end of the spectrum is to the left ; the I>
line common to them all is the image of a slit about half on inch long,
on which slit the light falls from an electric lamp, through the tube and
chamber in which the vapours are produced. The lower part of the
drawings would generally represent, therefore, the spectrum of the Uat
dense vapours were the vapours at rest.
3. One of the phenomena referred to consists of what may be described
as a unilateral widening of the line D : the side absorption, however, is
much less dense than that of the line ; it is bounded by D on one side
and by a curved tine on the other. Figs. 1, 2, and 3 will give an idea of
this appearance in three stages as it is frequently actually seen, i. t. as
the absorption travels up or down the line it widens as shown.
Fig.l.
\
1874.] Mr. J. N. Lockyer's Spectro$coi^c Nolet.—'No. IV. 870
4. Figs. 4 and 5 give two variations sometimes observed — fig. 4 showing
the darkeniug in the sbsorptioa and an increased steepness in the curve ;
tig. 5 the aimultaneouB existence o£ apparently different absorptions,
all boonded by D on one side, but by different curves ou the other, and
being of different intensities.
Kg. 4.
_^^
Y
Kg.S.
|PB
i
5. Altbongh, in the preceding drawings, I have represented this uni-
lateral widening exclusively on the more refrangible side of I), I have
observed it on the other, though scarcely so frequently.
6. Accompanying these appearances, but generally best visible when
the absorption with curved boundary Is visible on both sides of D, is a
brilliant boundary replacing the mere change of shade.
7. At times the brilliant boundary is continuous across D, as shown in
fig. 6 ; but I append figs. 7 and 8 to show that the phenomena on either
side of I) are independent of each other.
I'ig.fll
[June 18,
Fig. 7.
I^-l
if
•! '^^ ■ '1'
r
1
8. At times, D puts on the appearance oF the limiting line of a cbaa-
nelled-apace spectrum, the " easing otE" of the absorption being now on
one aide and now on the other.
9. Should all the^o phenomena be ultimately referred to the cauBos
which produce a channelled-space spectrum (one of which undoubtedly is
the teucleiicv to a unilateral instrad of a bilateral widening), a line-spec-
trum nil! be regnrdeil as a sjvcial ease merely, and not as an entirely
different spectrum, as it has been hitherto ; and the range of molecular
combinations in any one element from which Une-spectra may be pro-
duced is extended.
10. The question further arises, whether many of the short lines in
spectra are not remnants of channel led-space spectra.
JOSEPH DALTON HOOKER, C,B., President, in the Chair.
Mr. Henry Bowman Brady, Mr. Augustus Woilaston Franks, Prof,
Olaua Henrici, Sir Henry Sumner Maine, and Mr. Osbert Salvin were
admitted into the Society.
The Presents received were laid on the table, and thanks ordered for
The following Papers were read : —
I. " A Contrihution to the Anatomy of Connective Tissue, Nerve,
and Muscle, with special reference to their connexion with the
Lymphatic System." By G. Thin, M.D. Communicated
by Prof. Huxley, Sec. R.S. Received April 22, 1874*
• Tim Paper will appear in Ko. 155.
1874.] On the Determmatim of a Prime Number. 881
11. " Qiven the Number of Figures (not exceeding 100) in the
Reciprocal of a Prime Number, to determine the Prime itself."
By William Shanks. Commumcated by the Rey.G. Salmon,
F.R.S. Received May 19, 1874.
In a former communication (suprd, p. 200) I gave a Table showii^ the
number of figures in the period of the reciprood of every given piime up to
20,000. The Table here introduced is intended to solve the converse pro-
blem, and to show what primes have a given number of figures in their
period. It appears at once, from the ordinary rule for converting a pure cir-
culatmg decimal into a proper fraction, that if the reciprocal of a prime have
n figures in its period, that prime must be a factor in the number formed
by writing down n nines, and therefore also, generally, in the number
formed by writing down n ones. We denote that number by n ; that is
to say, 5 (in the left column), for example, =11111, except where
3, 3', 3' ... . 3' are concerned, when we have 3, for example, =899. The
problem now before us is equivalent to that of breaking np n into its
prime factors ; and the previous Table gives us great facility in doing
this, for it exhibits every factor of n which is less than 20,000* ; and if,
after accounting for all these, the remaining factor of n is less than
30,000', we may be sure that it is a prime number, and that the resolu-
tion is complete.
If we have to deal with a composite number mn, this may obviously be
writt«n down either as nt groups of n ones or as n groups of m ones. It
follows that mn contains m and n as factors. We may also state here that
12, besides the factor 9001, obviouslyhas all the factors belonging to any
submultiple of 13, e.g. 2, 3, 4, 6; and that this holdn in all other similar
cases, and need not be stated again. When we affirm that the resolution
in any case is complete (and, indeed, throughout the Table), it is to be
clearly understood that the snbmultiples have all been carefully attended
to, and thus any result may easily be verified. The high factors found
(those, we mean, above 30,000*) have involved considerable labour ; and
though we may not say absolutely that they are primes, yet we are
certun that, if composite, their component factors are primes each
greater than 30,000, and that the periods of their reciprocals have readily
been found. It only remains to add here that the left column contains
the given number of figures in the reciprocal of the prime or primes
found and placed opposite in the right column, or, in a few cases, of the
second powers of primes, and as far as the sixth power of the prime 3.
If the number of figures in the reciprocal of P be n, then the general
rulet, which may be drawn from particular cases such as the following
two, is that the number of figures in the reciprocal of P" is nP, of P* is
' In point of tact I lutTS ouried on the ckloul&tion up lo 30,000.
t See ■ MeManger of Ualhenutice,' vol. ii. pp. 41-43 (1872), tad tuI. iii. pp. 52-55
(1873),
[June 18, I
ljiiii.% the period of — = 18, &□(! siuue the remainders I
resultingfromdindinglS suth periods successively by 10 are, iu order, 15,
11, 7, 3, 18, H, 10, 6, 2, 17, 13, ft, 6, 1, 16, 12, 8, 4, U, it tdilows that
^ = 18x 19^342. The Iav of such remainders, after the first hu
been obtained, ie simple enough, and may be written down at ones.
Again, since the period of —r~^SI, also since the remainders resulting
from dividing 163 such periods, each of 81 figures, sufceBsively by 163
are, in order, 148, 135, V21, 107, 93, 79, 65, 51, 37, 23, 9, 158, 144. . . .0
(the series consisting of IG3 terms, of which tlie last is 0), it follows that
-i^ = Six 163 = 13203. The law of the above series is evident, and
the number of terms is easUy foaud to be 1G3. There is oa
obvious exception when P=3 ; then the period is divisible by P,
and the number of figures in the reciprocal of 3^ is 1, of 3' is 3, and of
3" is 3"~*. There are other exceptions also, or at all events one.
Desmarest, for instance, has remarked that in the case of P=4S7, the
period is divisible by 4S7 ; and therefore the number of fijfures in the
redprocat of 487" is the same as that in the reciprocal of 487, vis. 486.
I am not acquainted with the general theory of such exceptions ; nor do
I know what other primes (if any) besides 3 and 487 have the same
peculiarity.
With these explanations the following Table can readily be under-
stood. We mark with an asterisk those cases in which the resolution ia
complete, tiiuB 28 I 29 . 281 . 12149 9449. We ore to be understood
as affirming that 12149 9449 is a prime number.
GHbd nniDber of
PariaSofPrimei.
Prime*, Prime Factori, 4o,
3*. 333667.
9091.
11649.513159.
9901.
53,79,16537 1655.
90909 I.
, ; 58813 53"
Seems prune.
Seem a pnme.
, 1796 '•
1874.] Determination of a Pritae Nvmber.
V -^Tli! Prime*, Prime F»ctor», 4o.
99990 001.
11401 .ijSoi V*»S» "130 01-
*S9 ■ 'os8j '3049-
l*.7S7-44"33 46547 77631.
19 . igi . 11149 9449.
J191 . 16761 . io77i ojooo 95917 10406 7.
1791 . 39810 ioioi 04301 siS»' 73*75 »'■
353 .449 . 641 . 1409 .69857.
67 . 13446 »giio 31119 8373.
101 ■4°'3 ■ »'99J *333' 9-
71 , H676 18436 74776 043J3 511.
99999 90000 01. •
90909 09090 90909 091.
90090 09009 00990 99099 0991,
99990 00099 99°°° '-
8j . 1131 . 10874 80167 08045 »*7°» 4^77* 98379 31*30 ?■
7'. IJ7. 1689 .45969 1.
173 . 64"* 07578 67694 »!387 9*549 775*° 87347 46j07'
89. 11114 70797 64156 19°9-
99900 00009 99°o° 99999 90°!.
47 . 139 . 1531 . 54979 71844 91917.
SeemB prime.
99999 99900 00000 I.
10000 ooioo ooooi 00000 otooo oooio 00000 loooo 001.
151 . 5051 . 7887s 94147 1101.
611. 14696 58891 i7i"» 7°96> 00994 9S9°7-
511 . 19001 81976 77711 11417 8"-
107 . >o384 11599 '6916 17106 64589 81346 83181 41115 33748 70197 1.
99999 99990 00000 001.
1311 . 68130 8B570 01 514 75398 18144 S"09S 4'o»» 7"-
7841 . 11751 looio 10150 50376 1,
11319 . 41158 11190 53849 '0"o 5''7'° 59'44 89.
59 . 15408 11049 30661 55778 iioiS 49.
Seeme prime.
61 . 16557 16049 01641.
733 ■ 4637 ■ 3*690 11186 55567 7B491 67785 60346 38966 63414 9811}
99197 1391.
90909 09090 90909 09090 90909 09091.
10837 . 13111 . 19J45 15794 55591 00118 00680 443.
19841 . 50400 68544 93111 10780 70661 761,
90000 90000 90090 90090 90090 99090 99099 99099 991.
10989 01098 S9010 98901 I.
Seems prime.
99009 90099 00990 09900 99009 90099 01.
*77 ■ J»S*3 498»» 74693 46601 91091 53758 090M 01S40 83.
10999 88890 iiiio 08880 oooti.
Seem> prime.
' 3 '.555 6;
7153 . iijii 99847 08511 86556 01114 01639 447.
151 .4101 . 15763 98555 17191 91709 16417 09400 63151.
99009 90099 00990 09900 99009 90099 00990 I.
J137 . I7'85 4"3" 1*439 7SS75 73°I9 °7S99 s8'8o 44493 01317 17«'!
86404 43-
13* . 157 . 6397 ■ !4>« 49699 61 183 41-
117 . 6163 . 10171 . 55371 39794 64587-10197 5075» 7i9»6 68846 3<07»
31019 5*048 11389 153*6 15741 471.
Mr. W, Shanks on the Reciprocal [June 18,
'" in PriDiM, Prime Faclors, 4o.
99999 91000 00000 99999 99100 00000 I.
V ■ >6j . 9397 ■ "761 1557+ '7380 51978 03850 J93J4 1978J 10758 07<6l
797-
90909 09090 909o<} 09090 90909 09090 90909 09091,
3«ema prime-
10099 9899° "0099 9*990 ooioi.
90000 90000 90000 9090Q 90900 90900 90909 90909 90909 90909 99909
99909 9991.
90909 09090 90909 09090 90909 09090 90909 09090 91.
4,003 .11505 64319 00549 3iig6 55760 4319508116 66015 iSS*J 19000997.
617. 16105 83484 *o'i9 67584 91708 16564 01106 953,
19611 64119 50913 97453 00731 9.
547 . 14197 . I7l{37 . 64973 5B515 58148 78613 76371 1983! 67691 iiifi
17693 73769 81738 03847 7.
IZS9 . 76811 40495 741,80 7595' 11711 "8851 05500 46470 9.
9j 90090 09009 00900 90090 09009 00900 99099 09909 90990 99099 09909
90991,
94 6199. 14+31 30517 mil 15905 84364 04046 81839 8]o»7 609.
95 191 . 47110 89005 70681 09951 81717 69638 69115 1314J 30941 15*54
39841 8S481 61817 "7801.
96 97 . 10309 1783s OJ154 61S86 59793 S1443 3.
97 SeemB prime.
98 197 . 50761 41614 36553 19949 18781 71639 S9390 35533,
99 '99 ■ 397 ■ '1*57 74-717 *' S79 43369 I39I4 18173 61378 68181 11051 83191
77751 TAIl* 67,
loo 99999 99999 00000 00000 99999 99999 00000 ooooi.
Note. — In the preparation of this paper valuable assistance wa
received from the Eev. Prof. Salmon, F.E.S,, both in the way of suggea
tioDB and otherwise. — W. S.
Houghton -le-Sprin g.
April 18, 1874,
III. " On the Number of Figures in the Reciprocal of every
Prime between 20,000 and 30,000." By William Shanks.
Communicated by the Rev. Geohqe Salmon, F.R.S, Received
June 6, 1874.
In a former communication* I gave the number of figures in the
reaprocal of every prime below Srt.OOO ; the present Table is simply an
extension of the former, and has been calculated by the same method.
Towards the close of the former Table, liz. opposite the prime 19841,
ijittead of 1984 read 64. The uihoh of the former Table has kindly been
verified by the Eev. Dr. Salmon. For the accuracy of the following
Table I am entirely responsible, and believe it is free from error.
• Supra, p, 200,
1874.]
0/ every Prime behoeen 20,000 and 80,000.
In the laft-hsnd oolumn* of TaUa III. ue primM ; in the ri^t-huid oolumiu, in
diatel; opposite, U the Dumber of figuMa in Uie period <A the ndprooal ot eaoh pi
Table III.
continued).
lOOtl
6670
io6ti
10610
nil,
into
1J<03
.0901
11409
11104
1540
103. J
4144
1.8.6
11433
11431
iooil
«74
10639
10319
11117
.06.3
.0910
11441
10O19
6676
10641
ijSo
11147
1.146
11839
.0919
11+47
748*
.0047
10046
10663
10661
11169
11163
1.84I;
.0910
"453
56,3
100s ■
loop
»o68.
470
11177
.18.
i.SS"
1.850
11469
i,46i
11:063
10061
10693
739
1.183
3547
1.859
1.858
114a.
1810
10071
6690
10707
1479
1.313
ij68
i,86j
11861
11483
3747
10089
soil
10717
5"79
11317
.0658
1.87"
405
1150.
7500
107.9
34S3
11319
57
11881
1.88
115.1
..155
335"
10731
4146
11313
.066.
1.893
.0946
1153.
75.0
101.3
10743
10741
11341
4168
i.9i>
1095s
1154.
11540
S019
10747
10373
11347
10673
11919
54S1
11543
75 1*
""J
10061
10749
69,6
"377
1.376
1'937
ii936
11549
,148
101 19
10064
10753
10751
11379
3054
11943
73'4
11567
11566
10143
10071
10759
10379
1.383
11381
1.96.
"57"
45 '4
10147
'4)9
lo.ji
10771
4>54
1.391
3565
IJ977
1I976
11S73
5643
10149
10773
5'93
11397
■783
1.991
733
11613
5653
101 61
1680
10789
107K8
1.401
15
11997
.833
116.9
11618
10.73
5043
"s^
10806
1.407
1.406
11611
7540
10177
10.76
1.419
11418
11017
.1013
11637
1.318
10, gj
10 1 81
10849
10414
1.433
7'+4
11031
iio.s
116J9
"3»9
10857
10856
11467
'0733
11037
SS09
11643
1.311
10*19
1S38
10873
10871
1.481
S370
11039
3673
1165;
15.0
JOIJI
10.. s
10879
10439
11487
11486
11051
110 JO
11669
11^68
10133
10131
10887
6961
1.491
4198
11063
11061
11675
IIV^
10149
1531
10K97
10896
1.493
5373
11067
1.033
1169.
10161
10899
10898
1.499
J166
11073
11657
11696
10169
10903
1986
1.503
11501
11079
II039
44' 8
11699
1511
10187
966
10911
16.5
1.517
5379
11091
11709
11708
10197
10196
10919
436
1.51"
1151
11093
36S1
11717
5679
10313
3387
10939
10938
1.513
3587
11.09
11108
11711
.136^
10317
.0316
10947
10473
11519
1I9.
11111
1 105 5
11717
10333
1Q166
10959
499
11557
5389
11113
1687
11739
11738
103*1
406S
10963
10481
1.559
10779
11.19
5531
1174"
11740
10J47
10,73
1098,
4.96
1.563
.078.
11.33
5S33
1175"
1137s
103S3
1035,
10983
10981
..569
.0784
11.47
1.073
11769
II3>4
10357
S089
150
"577
1.576
11.53
mil
11777
7591
10359
10358
1.587
10793
11.57
S5J9
11783
11781
10369
1173
11013
5153
11589
7.96
11159
11787
11393
10389
679S
11017
11016
1.599
10799
ii
11807
7601
10393
10191
110I9
iio»8
11601
3600
IV.Vg
11811
118.0
10399
IOI99
11013
1.61.
1.6.0
11193
11191
11817
118.6
10407
11031
105 IS
116.3
.801
11119
11118
11853
57" 3
10411
10410
i|°59
1.058
116.7
1.6.6
11147
11146
11859
"X
10431
lOlIJ
4111
1,647
1.646
11159
11158
iisSi
10441
11067
3S"
1.649
11 17 1
■"35
1187.
"'43S
10443
3407
11089
105+4
11661
7110
11173
11877
5719
10477
5119
1.673
1.671
"569
1190.
11900
10479
10483
10139
10141
11107
'OS53
10560
1.683
1.70.
10841
11700
■Hi
37>3
11907
1191.
"tH
10507
10153
11139
7046
1.713
11711
11191
11190
"937
.1936
10509
10508
11143
11141
11717
11716
11303
11301
11943
11943
10511
1 140
11149
11148
11737
11736
11307
1..53
1196.
5740
losji
10166
H1S7
S189
11739
7146
11343
..171
11973
■i486
10S43
10541
11.63
3517
1175.
V^
11349
11348
11993
1199*
10S49
10548
1..69
1313
H757
10878
11367
11366
13003
II 501
105 SI
10175
11179
11 1 78
11767
11766
11369
...84
13011
IJOIO
10563
10181
11187
11773
.08S6
1138.
113S0
130.7
13016
10S9J
1871
11I91
1119
1.787
363.
JIJ91
11195
13011
13010
IOS99
10199
11193
7064
.1799
10899
11397
sm
l^-n-T
V \i."s>-i\
Wr, W. Shanks cw Me Reciprocal
T*jtI.E III. {eentinutil).
[June 1
•3019
ijoiS
13669
13668
14119
1421S
1497.
14970
1561.
15610
33039
11519
1,67.
iiS?5
14139
11119
14977
14976
15633
15631
13041
5760
13677
1.838
14147
14146
14979
8316
15639
4173
ll-JJ]
13687
13686
14151
14150
14989
1498S
156,3
iiSii
13057
mi
13689
3948
14181
1418
15013
6153
'^iv
^^lil
13059
13058
13719
11859
143.7
.115*
15031
.15.5
15667
15666
1J063
13741
13740
14319
11164
15033
1.91
15673
156,1
13071
"535
^3743
13741
14337
14336
15037
iijiS
15679
11839
^Ur
1.540
m*7
1.873
14359
11179
15057
15056
15693
6+11
a jog 7
13086
S3753
13751
14371
14370
15073
15071
15703
15701
11099
IJ098
13761
>.e8o
14373
4061
15087
15086
1S7'7
13117
5779
13767
13766
14379
8116
15097
15096
15733
11866
13131
13130
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15111
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137*9
13788
14407
.4406
15117
6179
15747
;1j;
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13801
197 s
14415
6,03
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13908
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15901
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63
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3979
14571
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8410
159.9
11959
1331 1
11660
13919
981
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15301
15300
15931
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13317
13316
13957
1,973
14611
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15301
1593J
6483
13333
1 1666
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13970
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15307
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15938
13339
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13977
13976
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8436
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15941
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1398.
13980
14659
1465 8
15311
6330
15951
'1975
13J69
1.6S4
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13991
14671
1133s
15339
8446
15969
'Itl*
13371
13370
14677
11333
15343
15341
1598'
8660
13399
.fl99
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8001
1+683
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15349
15348
15997
6499
13417
134.6
14019
1469.
14690
1S3S7
16003
13001
13431
.1715
14013
14011
14697
14696
15367
15366
160.7
8671
»3447
1134
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14018
14709
'f«^
15373
6343
1601.
.g:;
^3+59
1345S
14043
14733
6183
1519'
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11=14
14749
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16041
315s
»3497
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1406:
14060
14763
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15411
15410
1605J
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14071
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14767
14766
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13530
14077
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1.90
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11399
15453
4141
161.1
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1107 5
14907
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16188
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11458
15579
8516
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154
11459
i5';83
15581
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1*1
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141 s.
4836
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15588
16117
i*"
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7876
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14943
83'4
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i'
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149 S3
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15603
4167
16149
6561
un
ilsli
14113
14111
14^7
14966
15609
6401
16151
16150
1874.]
of every Prime between 20,000 and 30,00<).
Tabu III. {eontiwud).
aSafii
16160
16XS1
3j6o
17583
17581
iSiii
5642
18B13
\v\
16163
19. 8
16891
16890
17611
17610
18119
18817
18816
16167
13133
16893
6713
17617
176.6
18119
18218
18837
1602
16193
IT91
16903
1763.
4605
18277
.4133
18843
14411
16197
16,96
16911
I365
17647
17646
1B179
14.39
18B59
18858
16309
16917
16916
17653
69,3
1B1S3
18B67
481.
16317
.461
16947
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17673
9114
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14144
1887,
■4435
1631.
13160
169 S-
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13844
18197
1B296
18879
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16953
1695'
1J69.
9130
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1890.
F^S
26547
4391
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17696
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18308
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6589
169*.
169S0
17701
17700
18519
14.59
1S911
7130
1637.
16370
169S7
'3493
17733
4611
18349
1S348
1B917
31.4
16587
n'9i
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16991
17737
17736
18351
■4'75
18933
14466
16393
16391
170.0
17739
'3S69
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18961
14480
i6j99
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17017
17743
27741
18393
'351
18979
18978
16407
i64'.6
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17748
18403
14201
19009
14504
164.7
16416
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13511
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915
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190.7
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17058
17763
13B81
18410
19011
19010
1643.
1643
17060
17767
17766
2B4I9
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13899
18477
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1659
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18;49
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17901
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787
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14699
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4787
19401
4900
16B13
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17+87
17486
18,09
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18729
.4364
19+11
5881
16811
8940
17509
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18111
937
1875'
.150
19413
19411
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17516
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19418
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28771
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34"
17J41
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5636
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199
16863
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1947 J
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788
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7050
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9601
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1474"
l>r. E, Klein on the Smallpox of Sheep.
TiBLE III. (continued).
[June 18,
«9S0'
09500
»9!99
'4799
19717
US 58
198.,
19S.S
19881
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19517
777
90
19733
19833
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19530
19619
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19740
198J7
7459
19911
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19536
19651
19631
»9?S3
19751
5970
19917
19567
19566
»9759
19JI61
19861
19569
X464
1966,
19661
19761
496=
19S67
'4933
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19669
19668
19789
19788
1987J
19871
.»
.9^8.
19580
1967.
»4iflS
4,67
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19,89
19SB7
'4793
19683
.649
IV. " Research on the Smallpox of Sheep." By E. Klein, M.D.,
ABsistaiit Professor at the Laboratory of the Brown Institu-
tionj London. Communicated by John Simon, F.R.S.,
D.C.L., Medical Officer of the Pri\7 Council, &c. Received
June II, 1874.
Variola ovina, or emallpox of sheep, is a disease which, allbou^ it is
not communicable to man, and possesses a specific contagium of its own,
very closely resembles human smallpox, both as regards the development
of the morbid process and the anatomical lesions which accompany it.
This correapondence is so complete, that it cannot be doubted that the
pathogeny pf the two diseases is the same. The present investigation
was therefore undertaken in the confidence that the application of the
experimental method to the investigation of the ovine disease would not
only yield results of value, as contributory to our knowledge of the infec-
tive process in general, but would throw special light on the pathology
of smallpox.
The paper consists of four sections. In the first, the author gives an
account of his experimental method, which consisted in communicating
the disease by inoculation to a sufficient number of sheep, and in investi-
gating anatomically (1} the pustules produced at the seat of inoculation,
and (2) those constituting the general eruption. The lymph employed
was obtained by the kindness of Prof. Chauveau, of Lyons, and tint.
Cohn, of Breslau.
In the second section, the organisms contiuned in fresh lymph, and the
organic forms derived from them by cultivation, are described. The
author finds that fresh lymph contains spheroidal bodies of extreme
minuteness, which correspond to the micrococcus of Hallier and to the
spheroids described by Cohn and Sanderson in vaccine lymph. It also
contains other forms, not previously described, which in their develop-
ment are in organic continuity with the micrococci.
The third section contains a complete anatomical description of the skin
1874.] Dr. E. Klein on the Smallpox of Shetp. 889
of the sheep, with spei-ial reference to those puticulars in which it differs
from that of dud.
The reiDsinder of the paper b occupied with the investigation of the
changes which occur in the int^^ument at the seat of the inocnlation, and
with the anatomical characters of the secondary pustules.
The most important results are the following : —
1. The development of the primary pock may be divided into three
stages, of which the first is characterized by progressive thickening of the
integument over a rapidly increasing but well-defined area ; the second, by
the formation of vesicular cavities containing clear liquid (the "cells"
of older authors) in the rete Molpigbil ; the third, by the impletion of
these cavities with pus-corpuacles and other structures. It is to be
noted that the division inl« stages is less marked than in human small-
pox.
2. The process commences in the rete Malpighii and in the subjacent
papillary layer of the corium — in the former, by the enlargement and in-
creased distinctness of outUne of the cells, and by corresponding genui-
native changes in their nuclei ; in the latter, by the increase of size of the
papilUe, and by germination of the epithelial elements of the capillary
blood-vessels.
3. It is next seen that the interfascicular channels (lymphatic canali-
culi) of the corium are dilated and more distinct; that the lining cells of
these channels are enlarged and more easily recognized than in the
natural state ; and that, in the more vascular parts of the corium, the
channels are more or less filled with migratory, or lymph, corpuscles. At
the game time, the lymphatic vessels, of which the canaliculi are tribu-
taries, can be readily traced, in consequence of their being distended with
a material which resembles coagulated plasma.
4. About the third day after the appearance of the pock, the contents
of the dilated lymphatics begin to exhibit characters which are not met
with in ordinary exudative processes. These consist in the appearance,
in the granular material already mentioned, of organized bodies, which
neither belong to the tissue nor are referable to any anatomical type —
viz. of spheroidal, or ovoid, bodies having the characters of micrococci and
of branched filaments. These last may be either sufGciently sparse to be
easily distinguished from each other, or closely interlaced so as to form
a felt-like mass.
5. The process, thus commenced, makes rapid progress. After one or
two days, the greater number of the lymphatics of the affected part of
the corium become filled with the vegetation above described ; and on
careful examination of the masses, it is seen that they present the cha-
racters of a myceUum, from which necklace-like terminal filaments spring,
each of which breaks off, at its free end, into conidia. In most of the
filaments, a jointed structure can be made out, and, in the larger ones, the
390 Dr. £. Klein on the Smallpox ^ Sheep. [ Juue 1
contents can be distiDguished from the eocloaing membrane by their yd-^
lowisb -green colour.
0. At tbe aame tiin>? that tht^ae appearances present themselves hi tbo '
corium, those cbangea are beginning in the non' much thickened rete Ma]-
pighii which are preparatory to the formation of theiesieular caritieo
already mentioned. By a process which the author designates homy
transformation, having itB seat in the epithelial cells of the middle layer tJ
the rete Malpighii, a homy expansion, or stratum, appears, lying in a plane
paraUel to the surface, by which the rete Malpighii is divided into two
parts, of which one is more superficial, the other deeper than the homy
layer. Simultaneously with the formation of the horny layer the cells of
the rete nearest the surface of the corium undergo very active germina-
tion, in consequence of which the interpapillary processes not only
enlarge, but intrude in an irregular manner into the subjacent corium.
At the some time, the cells immediately l>eIow the homy stratum begin to
take part in the formation of the vesicular cavities, some of them en-
larging into veaii^lca, while others become flattened and acaly, so as to
forai the septa by which the veaicolar cavities ape separated from each
7. The v£'s!cles, oucp formeil, increase in form and nitmbfr. Originally
separate, and containing only clear liquid, they coalesce, as they get
larger, into irregular sinuses, and are then seen to contain masses of vege-
tation similar to those which have been already described in the lymphatic
system of the corium — with this difference, that the filaments of which
tbe masses are composed are of such eitreme tenuity, and the conidia
are so small and numerous, that the nhole possesses the characters of
Eoogltea rather than of mycelium. However, the author has no doubt
that these ^gregations are produced in the same way as the others, viz.
by the detachment of conidia from the ends of filaments. In the earlier
stages of the proi;eas the cavities contain scarcely any young cells.
Sooner or later, however, so much of the rete Malpighii as lies between
the horay stratum and the papillae becomes infiltrated with migratory
lymph-corpuscles. The process can be plainly traced in the sections. At
the period of vesiculation, t, (. at a time corresponding to the commence-
ment of the development of the vesicles in the rete Malpighii, the cutis
(particularly towards the periphery of the pock) is infiltrated with these
bodies. No sooner has the coalescence of the vesicles made such progress
as to give rise to the formation of a system of intercommunicating
sinuses, than it is seen that the whole of the deep layers of the rete Mal-
pighii become inundated (so to speak) with migratory cells, which soon
find their way towards the cavities, and convert them into microscopical
eollections of pus-corpuscles, the formation of which is proved to be due
to migration from the corium, not only by the actual observation of
numerous amoeboid cells in trantiiu, but by tbe fact that the corium itself.
1874.] On Orgatusmt in the Liquor SanffttintM. 891
before eo crowded with t^ese bodies, bacomes, as the postalaMon ftdTanceSi
entirely free from them.
8. The concluding section of the paper ia occupied with the descrip-
tioD of the secondary eruption, the anatomicftl charscters of which Torj
closely resemble those which have been already detailed.
V. " Researcbes in Spectrum-Analysis ia connexion with the
Spectrum of the Sun." — No. IV. By J. Norman Locktsb,
F.R.S. Received May 11, 1874.
(Abstract.)
Maps of the spectra of calcium, barium, and strontium hare been con-
structed from photographs taken by the method described in a former
communication (the third of this series). The maps comprise the portion
of tfae spectrum extending from wave-length 3900 to vave-length 4500,
and are laid before the Society as a specimen of the results obtainable by
the photographic method, in the hope of securing the cooperation of other
observers. The method of mapping ia described in detail, and tables of
wave-lengths accompany the maps. The vave-lengths assigned to the
new lines must be considered only as approximations to the truth. Many
of the coincidences between lines in distinct spectra recorded by former
observers have been shown, by the photographic method, to be caused by
the presence of one substance as an impurity in the other; but a certain
number of coincidences still remain undetermined. The question of the
reversal of the new lines in the solar spectrum is reserved till better pho-
tographs can be obtained.
VI. " An Account of certain Oi^nisms occurring in the Liquor
Sanguinis." By "William Oslzh, M.D. Communicated by
J. BcBDON SANnEBsoN, M.D., F.R.S. Received May 6,
1874.
In many diseased conditions of the body, occasionally also in perfectly
healthy individuals and in many of the lower animals, careful investi-
gation of the blood proves that, in addition to the usual elements, there
exist pale granular masses, which on closer inspection present a corpus-
cular appearance (Plate V. fig. 1 ). There are probably few observers in the
habit ot examining blood who have not, at some time or other, met with
these structures, and have been puixled for an explanation of their
e and nature.
2n
aeS Dr. W. Osier on Organisms [June 1«^
In BiBe they varv greatly, from lialF or quarter that of a wliittj blood-
corpuacle, to enormous maaaes occupnng a large area of the tleld or
avBii slretthiaR completely across it. Thoy usually twsume a Bouie\(hat
round or oval form, but may be elongated and narrow, or, from tint
enetenee of numerous projectiona, offer a very irregular outline,
bavc a. compact solid look, and by focusing are seen to possess eongideiM-.'
able depth ; wMIl' in specimens examined without any reagents tbo fila-
ments of 0brin adhere to them, and, entangled in their interior, while
corpuscles are not unfrequently met with.
It is not from every mass that a judgment can be formed of their true
nature, as the larger, more closely arranged ones have rather tlie appear-
ance of a granular body, and it ia with difficulty that the individual
elements can be focused. When, however, the more loosely composed
ones are chosen, their intimate composition can be studied to advantage,
especially at the borders, where only a single layer of corpuscles may
exist; and when esamined with a high power (9 or 10 Hartnack) the.se
corpuscles are seen to be pale round disks, devoid of granules and with
well-defined contours. Some of the corpuaclea generally Hoat free in tlie
fluid about the mass ; and if they turn half over their profile view faes the
appearance of a sharp dark line (fig. 5, n & 6). In water the individual
corpuscles composing the mass swell greatly ; dilute acetic acid renders
them more distinct, while dilute potash aolutiona quickly dissolve them.
Measurements give, for the large proportion of the corpuscles, a diameter
ranging from one 8000th to one in,U00th of an incb ; the largest are as
much as one 5000th, and the smallest from one 15,000th to one 24,000th
of an inch ; so that they may be said to be from ^J the size of a red
corpuscle. In the blood of eata, rabbila, dogs, guineapigs, and rats the
aiasses are to be found in variable numbers. New-bom rata are specially
to be recommended as objects of study, as in their blood the masaea ar©
commonly both numerous and large. They occur also in the blood of
foetal kittens.
Considering their prevalence in disease and among some of the lower
uiimals, they have attracted but little notice, and possess a comparatively
acaoty literature. The late Prof. Max Schultze • was the first, as far as
I can ascertain, to describe and figure the masses in question. lie speaks
of them as constant constituents of the blood of healthy individuals, but
concludes that we know nothing of their origin or destiny, suggesting,
however, at the same time that they may arise from the degeneration
of granular white corpuscles. Schuhie'a observations were confined to
the blood of healthy persons, and he seemed of the opinion that no
pitthological significance was to be attributed to them.
By far the most systematic account is given by Dr. Riess t, in an
• Archiv f. mik. Anat. Bd. i.
t Reichert u. Du Bois-Reymoud's Archiv, 1872,
1874.] in _tli€ I4qw>r Sanguinis. 898
article in which be records the results of & long leiies of obtervatiotM on
their presence in various acnte and chronic diseases. His invest^ticau
of the blood of piatients, which were much more eitensiye than an^
I have been able to undertake, show that, in all exonthems and chronic
affections of whatever sort, indeed in almost all coses attended with
disturbance of function and debility, these masses ore to be found. He
concludes that their number is in no proportion to the severity of the
disease, and that they ore more numerous in the latter stages of on
affection, after the acute symptoms have subsided. The former of theM
propositions is undoubtedly true, as I have rarely found masses lai^r or
more abundant than I, at one time, obtained from my own blood when in
a condition of perfect health. These two accounts may be said to com-
prise every thing of any importance that has been written concerning these
bodies. The following observers refer to them cursorily : — £rb *, in a
paper on the development of the red corpuscles, speaks of their presenc*
under both healthy and diseased conditions ; he hod hoped, in the be^in-
ning of his research, that they might stand, ae Zimmerman supposes (set
below), in some connexion with the origin and development of the red
coVpuscles ; but, as he proceeded, the fallacy of this view became evident
to him. Bettelheim t seems to refer to these corpuscles when hd spMka
of finding in the blood of persons, healthy as well as diseased, small
punctifonn, or rod-shaped, corpuscles of various sizes. ChristoL and
Kiener t describe in blood small round corpuscles, whose measurements
^ree with the ones under consideration ; and they also speak of their
exhibiting slight movements. Biess §, in a criticism on a work of the
next-mentioned author, again refers to these masses, and reiterotdS hil
statements concerning them. Birsch-Hirschfeldjl had noticed them and
the similarity the corpuscles bore to micrococci, and suggests that under
some conditions Bacteria might develop from them. Zimmerman ^ has
described corpuscular elements in the blood, which, with referancd to ths
bodies in question, demand a notice here. He let blood flow directly into
a solution of a neutral salt, and, after the subsidence of the coloured
elements, examined the supernatant serum, in which he found, in extra-
ordinary numbers, small, round, colourless corpuscles with weak contours,
to which he gave the name of " elementary corpuscles." Theee he met
vrith in human blood both in health and disease and in the blood of the
lower animals; and he found gradations between the smaller(alwaytcoloui>
less) forms and full-sized red corpuscles. He gives measurements (for tha
smaller ones, from one 1000th to one 800th of a Una ; the largest, one
* Tirchow'i An^v, Bd. mir.
t Wiener med. Frene, 1868, No, li
J Comptei BeDdoB, liru. 1034. Quotod in ' Caotrolhlatt^' 1869, p. 06.
§ Centnlblatt, 1673, No. 34.
I Oentralblatt, 1873, So. Sa
^ Virebam't Ardiiv, Bd. xriii.
894 Dr. W. Osier on Organisms [June 18,
sooth to one 400th of n. line), and speaks of them also as occurring in
dumpa and groups of globules. It is dear, on reading his account,
that in part, at any rat^, he refers to the eorpusclea above described,
GradatioQfl such as he noticed between these and the coloured ele-
ments I have nerer met with, and undoubtedly he was dealing with the
latter in a partially decolourised condition, I.ostorfer's • corpuscles,
which attracted such attention a few years ago from the assertion of the
discoverer that they were peculiar to the blood of syphilitic patients,
require for their production an artificial culture in the moist chamber
extending over several dnya. They appear first after two or three
days, or even sooner, as small bright corpuscles, partly at rest, partly in
motion, which continue to increase in size, till, by the sixth or seventh
day, they have attained the diameter of a red corpuscle, and may possess
numerous processes or contain vacuoles in their interior. Blood from
healthy individuals, as well as from diseases other than syphilis, has
been shown to yield these corpuscles ; and the general opinion at present
held of them is that they are of an albuminoid nature.
The question at once most naturally arose, How is it possible for such
masses, some measuring even one 400th of an inch, to pass through the
tapillfiries, unless suppowd to posocss a degree of e^tensiliititj' and
elasticity euch as their composition hardly warranted attributing to
them ? Neither Max Schultze nor Biess offer any suggestion on this
point, though the latter thinks that they might, under some conditionB,
produce embolism.
During the examination of a portion ot loose connective tissue from
the back of a young rat, in a large vein which happened to be in the
specimen, these same corpuscles were seen, not, however, aggregated
together, but isolated and single among the blood-corpuscles (fig. S); and
repeated observations demonstrated the fact that, in a drop of blood
taken from one of these young animals, the corpuscles were always to
be found accumulated together ; while, on the other hand, in the vessels
(whether veins, arteries, or capillaries) of the same rat they were always
present as separate elements, showing no tendency to adhere to onfi
another. The masses, then, are formed at the moment of the withdrawal
of the blood, from corpuscles previously circulating free in it.
To proceed now to the main subject of my communication. If a drop
of blood containing these masses is mixed on a slide with an equal quan-
tity of saline solution, J-| per cent., or, lietterstill, perfectly fresh serum,
covered, surrounded with oil, and kept at a temperature of about 37° C,
a remarkable change begins in the masses. If one of the latter is chosen
for observation, and its outline carefully noted, it is seen, at first, that
the edge presents a tolerably uniform appearance, a few filaments of
• Wiener med. PresM, 1872, p. 93, Wienermed. Woohenschriil, 1872,Ho.8. Articlo
in Arcbiv f. Dermatolog. 1872,
1874.] t» the lAgtior Sanfftdnit. 895
fibrin perhaps adhering to it, or a few email corpuBcles lying free in
the vicinity. These latter Boon exhibit appareat Browaian mOTetnenta,
frequently turning half over, and showing their dark rod-like border
(£g. 5, a, h). After a abort time an alteration ia noticed in the presence
of fine projections from the margins of the mass, which may be either
perfectly straight, or eaoh may present an oval swelling at the free or
attached end or else in the middle (fig. 2, b). It is further seen that
the edges of the mass are now less dense, more loosely arranged, or, if
small, it may have a radiated aspect. Sometimes, before any filaments
are seen, a loosening takes place in the periphery of the mass, and among
these semifree corpuscles the first development occurs. The projecting
filaments above mentioned soon begin a wavy motioa, and finally break
off from the mass, moving away free in the fluid. This process, at first
limited, soon becomes more general ; the number of filaments which pro-
ject from the mass increases, and they may be seen not only at the lateral
borders, but also, by altering the focus, on the surface of the mass, as
dark, sharply defined objects. The detachment of the filaments proceeds
rapidly ; and in a short time the whole area for some distance from tbe
margins ia alive with moving forms (fig. 2, e, and fig. 3), which spread
themselves more and more peripherally as the development continues in
the centre. In addition to the various filaments, swarming granules are
present in abundance, and give to the circumference a cloudy aspect,
making it difficult to define the individual forms. The mass has now
become perceptibly smaller, more granular, its borders indistinct and
merged in the swarming cloud about them ; but corpuscles are still to ba.
seen in it, as well as free in the field. A variable time ia taken to arrive
at this atage ; usually, however, it takes- place within an hour and a half,
or even much less. The variety of the forms increases as the develop-
ment goea on ; and whereas, at first, spermatozoon-hke or spindle-ahaped
corpuscles were almost exctuaively to be seen, later more irregular forms
appear, possessing two, three, or even more tail-like processes of extreme
delicacy (fig. 5, it). The more active ones wander towards the periphery,
pass out of the field, and become loat among the blood-corpuscles. The
process reaches its height within 2j hours, and from this time begins
almost imperceptibly to decline ; the area about the mass is less densely
occupied by the moving forms, and by degrees becomes clearer, till at
last, after six or seven hours (often less), scarcely an element ia to be seen
in the field, and a granular body, in which a few corpueclea yet exist, ia
all that remains of the maas. The above represents a typical develop-
ment from a large maas in serum, such as that seen in fig. 3*.
We have next to study more in detail the process of development
and the resulting forms. Commonly, the first appearance of activity is
* Tbe man from which thii aketchwu taken wu seen in fuU development bjnTsrkl
of the foreign viaitor* to tbe British Medial Anociatioa lut year.
[June 1^'
displayed by the small free corpuscles at the mai^ins, whidi, previoiulf i
qmeacent, begin a species of jerky irregular moiemeot, at one time wiA
tbeir pale disk-aurfsces uppennost, at another presenting their dark
linear profiles (fig. 5, a & b). Not imfrequently, some of these
with a larger or smaller segment of their circumfereuce thicker and'
darker tbau the other (fig. 5, c).
EarUest, and perhaps the most plentiful, of the forms are those of
a flpermatttsoon-like shape (fig. 5, d), attached to the mass either by the
head or tail ; while, simultaneously, long bow-shaped lilameuts appear
(fig. 5, «), haling an enlargement in the centre. Straight hair-like filaments
(fig. 5,/) may also be seen, but they are not very numerous. The time
which elapses before they begin the wavy moTcmeut is very variable, as
is also the time when they break away after once beginniug it. Filar-
ments may be seen perfectly quieewnt for more than half an hour before
ttiey move, and others may be obserTed quite as long iu motion before
they succeed in breaking away from the mass. Commonly it is in tho
smaller masses, and where the development is feeble, that filameJits re-
main for any time adherent. The spermatozoon-like forms appear, at the
head, on one \iew flattened and pale, on the other dark and linear
(fig. 5, rf|: consequently the head is diseoid, not splieroidai. The bow-
■baped filaments also present a dark straight aspect when they turn orer
(fig- 6, '}, and are by far the longest of the forms, some measutdng aa
much as one 900th of an inch. Many intermediate fo^a between the
round discoid corpuscles and those with long tails are met with in the
field, and are figured at fig. 5, g.
Small rod-ahaped forms are very numerous, most of which, however,
on one aspect look corpuscular ; but in others this cannot be detected, or
only with the greatest difficulty ; slight enlargements at each end may
also be seen occasionally in these forms (fig. 5, h).
TJaually late to appear, and more often seen in the profuse develop-
ments from large masses, are the forms with three or more tail-like pro-
oesses attached to a small central body (fig. 5, Ic). Amtmg the granule*
it is eitremoly difficult to determine accurately the number of these pro-
cesses, the apparent number of which may also vary in the different posi-
tions assumed by the element. As to the ultimate destiny of the indi-
Tidual forms, I have not much to offer ; I have \vat«hed single ones, with
this view, tor several consecutive hours without noticing any material
alteration iu them. The one represented at fig. 6 was watched for four
hours, that at fig. 7 for five, and the changes sketched. The diffi-
culty of following up individual filaments in this way is very great, not
only from the ensuing weariness, but from the obstacle the red corpuscles
offer to it.
With regard to the movement of the filaments, this, at first sight,
bears some resemblance to that known as the Brownian, exhibited bjr
I
1874.] in ths Liquor Smigmtit. 897
granules in the field, or Bometimes by the red corpasclea ; but m evident
diSerende is soon noticed in the fact tb&t, while the former (also th«
small corpuscles) undergo a change of place, the latter remain constant
in one posidoD or vary but little.
Movements like those of the ordinary rod-shaped SacUria are not
exhibited by them,
Circumstanca which inflatnce the deuelopmsnt, — In blood, without
the Addition of saline solution or serum, no change takes place in the
masses even after prolonged warming. A temperature of about 37° C.
is nece38ary for the process ; none occurs at the ordinary temperature,
with or without the addition of fluid. Fresh scrum is the medium most
favourable to the process, added in quantity equal to the amountof blood.
Not every mass develops when placed under conditions apparently
favourable ; but fur this no good reason can, at present, be offered.
P'ig. 8 represents the corpuscles among the red ones while in the
vessel \ and, as is there seen, they appear somewhat more elliptical on the
profile view, and more elongated, than in blood after withdrawal, but
present the same disk-like surfaces when they roll over. On adding
saline solution or serum, and warming the preparation, development
proceeds, but not to such an extent as from the masses. The individutd
corpuscles become elongated, some tailed, and they move about in the
vessel. At fig. 9 they are seen iu the vessel after three hours on th«
warm stage : the remarkable form seen at a was one 1300th of an
inch in length, and had moved up from the opposite end of the vessel.
It must still be confessed, with Mai Schultze, that we know nothing
of the origin or destiny of these corpuscles ; and once admit their exist-
ence as individual elements circulating in the blood, his suggestion,
and Biess's assertion that the masses arise from the disintegration of
white corpuscles, becomes quite untenable. We must also confess the
same ignorance of the reasons of their increase in disease ; nor do we
know at all what influence they may exert in the course of chronic
affections.
Finally, as there is no evidence that these bodies are in organic con-
tinuity with any other recognized animal or vegetable form, or possess
the power of reproduction, nothing can at present be said of their nature
or of their relation to Bacteria.
These observations were carried on in the Physiological Laboratory of
University College, and my thanks are due to Prof. Sanderson and Mr.
Schafer for advice and valuable assistance.
EXPLAHATION OP THE PLATE.
Fig. 1. Common fonni of (he msuM from hedthy blood. (OcuUr 3, ObjeotiTe 6,)
Fig. 2. A man from healthy blood, in nlina BolutioD, ahowjag itagea of dsrelopment:
a, at 10 i.M. ; b, at 10.30 *,*, ; o, at 11 kjt. (Onikr 8, OtigeatiTe 7.)
Messrs. Tiemann and Haarmann on
n on [June IS^rfl
slopment, kfter twa lunu^H
a show the nUtire «m>S
'. Mossfrotn blood of jo\mg rat |
warming. (Ocular 3, Objeotiva 7.)
Fig. 4. Masa (joung ral) witb blood-coipiucles about
{Ocular 3, Objertire 5.)
Pig. 5. SoniB of the developed forms as wen with No. II Harinaek. (Sea teit)
Kg. 6. Form watched for four lioura. (Oculnr 3, Objectiie 9.)
Fig. 7. Form watched for five hours. (OcuUr 3, Objective 6.)
Pig. 8. Small Tein in oonnoi'tise tiaaue from the back of o foung rat, ahowing the oor-
puacles fr«e aitiDng the red ones. (Ocular 3, Objeclire 7.)
Fig. 9. Small Tein from the connectire tissue of a rat (in serum), abawing corpuadn and
deieluped forms. (Ocular 3, Objective 9.)
VII. " On Conifcrine, and its Conversion into the Aromatic Prin-
ciple of Vanilla," By Fzbd. Tiemans and Wilh, Haarmann.
Communicated by A. W. Hofmann, LL.D., F.R.S. Received
May 11, 18?4.
The asp of the cumbiuiu of coniferous trees contains a beautiful crystal-
line glucoaide, coniferine, which was discovered by Kartig and eiamined
some years ago by Kubel, who arrived at the formula
C,, H„ 0„ + 3aq.
A minute atudy of this compound leads us to represent the molecule
of coniferine by the expression
C,„H„0, + 2aq,
the percentages of which nearly coincide with the theoretical values of
Xubel's formula.
Submitted to fermentation with emulsine, coniferine splits into sugar
and a splendid compound, crystallizing in prisms which fuse at 73°>
This body is easily soluble in ether, less so in alcohol, almost insoluble
in water ; its composition is represented by the formula
The change is represented by the equation
' C„ H„ 0. + H, 0 = C. H„ 0, + Cj, H„ 0,.
. Under the influence of oxidizing agents the product of fermentatdoD
undergoes a remarkable metamorphosis. On boiHng it with a mixture of
potassium bichromate and sulphuric acid, there passes with the vapour
of water, in the first place ethylic aldehyde, and subsequently an acid
compound soluble in water, from which it may be removed by ether. On
evaporating the ethereal solution, crystals in stellar groups are left
behind, which fuse at 81°. These crystals have the taste and odour of
vanilla. An accurate comparative examination has proved them to be idea-
,tJt.,rScr.iV.IXI!.I'iy.
% • •
% 'm
o o
o o
io
o
p ^v Ov (^ ii;
. ;),vy ■-■
'"'" ^&M'Mfl
O V 1 o
1874.] Coniferine and ita Comermm. 899
tdcftl with the ciystaUme Bnbstkuce which constdtates the aroma of Tuiillft,
and which is often Been covering the surface of vanilla-rods.
On analysis, the crystals we obtained were found to cantais
This is exactly the composition which recent researches of Carles have
established for the aromatic principle of vanilla. The transformation of
the crystalline product of fermentation into vanilline is represented hy
ttie following equation :—
C„ H„ O, + 0 =: C^ H. O + C. H, 0,.
To remove all doubt regarding the identity of artificial vanilline with
the natural compound, we have transformed the former into a series of
salts which have the general formula
C,H,MO.,
and into two substitution-products,
C.H^BrO,
and
C.H,IO„
both of which had previously been prepared by Carles from the natural
compound.
In order further to elucidate the nature of vsnillinu, we have submitted
this body to fusion with alkali. The product of this action is a well-
known add discovered by Strecker, and described by him as proto-
catechuic acid,
C,H.O„
which is thus formed —
C,H,0, + 40 = C,H.O. + H,0 + CO..
We have identified this substance by analysis, by the study of its
reactions, and also by transforming it into pyrocatechine, C, H, 0„
C, H, 0, = C, H. O, + CO..
The transformation into protocatechuic add fixes the constitution of
vanilline. This compound is the methylated aldehyde of protocatechuic
add ; its composition referred to benzol is represented by the formula
/OCH.
NOOH.
On Coniferine and Us Conversion.
[June 18,
Indeed, (ubmitted under pressure to the action of hydrochloric add,
raoiiline splits into chlorido of methjl and proto«it«ohuic aldehyde,
/OCH.
/OH
C.H
^OH
+ Ha
= CH,C1 + C.H.^0H
NCOH
^COH.
A cmrespondiDg action takea place with hjdriodic add ; but in this
case the aldehyde is destroyed.
An additioDsJ proof o£ the correctnesa of our view regarding the con-
etitution of vanilline is obtained by treating this siibstanee with acetic
anhydride and benzoyl chloride.
The action does not go beyond the formation of the compounds
/OCH,
C.H,^OC,H,0
NCOH.
r yOCH.
\ C,H,^OC,H,0 ^
■ MTOH,
showing that vanilline does not contain more than one hydroxylic
group.
The constitution of vanilline being thus made out, there could be no
doubt regarding the structure of the product of fermentation from which
vanilline arises. This compound is the ethylio ether of vanilline,
/OCH,
C,H,^OC,H,
NCOH.
That such is the constitution of the body is proved by the simultaneous
formation of ethylic aldehyde when vanilline is formed. We obtained,
however, an additional confirmation of this conception by submitting the
product of fermentation to the action of hydriodic acid under pressure,
when an alcohol iodide was formed, which we succeeded in separating
into the iodides of methyl and ethyl,
/OCH,
C,H,^OC,H. + 2HI
NCOH
/OH
= CHJ + C,H,H-C,H,^OH
NCOH.
The experiments we have described in this note were performed in the
laboratory of Professor A. W. Hofmann, to whom we are deeply indebted
for the advice and assistance he has given us in the course of these
researches.
1874.] On Swface-EvaportUum and Cotuktuation. 401
VIII. " On the Forces caused by Evaporation from, and Conden'.
sation at, a Surface." By Prof. Osbobne Reynolds^ of
Oweus College, Maucbester. Communicated by B. Stewakt,
F.R.S. Received May 16, 1874.
It has beeD noticed by several philosophers, and particularly by Hr.
Crookes, that, under certain circumstances, hot bodies appear to repel and
cold ones to attract other bodies. It is my object in tbis paper to point
out, and to describe experiments to prove, that these effects are the
results of evaporation and condensation, and that they are valuable
evidence of the truth of the kinetic theory of gas, viz. that gas consists
of separate molecules moving at great velocities.
The experiments of which the explanation will be given were as
follows : —
A light stem of glass, with pith-balls on its ends, was suspended by a
sUk thread in a glass flask, so that the balls were nearly at the same
level. Some water was then put in the flask and boiled until aU the air
was driven out of the flask, which was then corked and allowed to cool.
When cold there was a partial vacuum in it, the gauge showing from
^ to j of an inch pressure.
It was now found that when the flame of a lamp was brought near
to the flask, the pith-ball which was nearest the flame was driven away,
and that with a piece of ice the pith was attracted.
This experiment was repeated under a variety of drcum stances, in
different flasks and with different balances, the stem being sometimes oi
glass and sometimes of platinum ; the results, however, were the same in
all cases, except such variations as I am about to describe.
The pitb-bdls were more sensitive to the heat and cold when the flask
was cold and the tension within it low ; but the effect was perceptible
until the gauge showed about an inch, and even after that the ice would
attract the ball.
The reason why the repulsion from heat was not apparent at greater
tensions, was clearly due to the convection-cument« which the heat gene-
rated within tbe flask. When there was enough vapour, these current!
carried the pith with them ; they were, in fact, then sufficient to over-
come the forces which otherwise moved the pitb. This was shown by
l^e fact that when the bar was not quite level, so that one ball wag
higher tJum tbe other, the currents affected them in different degrees ;
also that a difEerent effect could be produced by raising or lowering the
positiou of the flame.
The condition of the pith also perceptibly affected tbe sensitiveness of
the balls. When a piece of ice was placed against the side of the glass,
the nearest of the pith-balle would be drawn towards the ioe, and would
eventually stop op{>oeite to it. If allowed to remain in this condition
for some time, the vapour would ccmdense on the ball near the iee.
402 Prof, O. Reynolds on Surface- Forces [June 18,
while the other ball would become dry (this would be seen to be tha
case, and waa aUo shown, by the tipping of the balance, that ball ogaiost
the ice gradually gettijig lower). It was then found, wheu the ic« waa
removed, that the dry ball u'as insensible to the heat, or nearly so, while
that ball which had been opposite to the ice was more than ordinarily
Knaitive.
If the flask were dry and the tension of the vapour reduced with tha
pump until the gauge showed | of a.n inch, then, although purely steam,
the vapour was not in a saturated condition, and the pith-balls which
were dry were no longer sensitive to the lamp, although they would still
approach the ice.
From these last two facts it appears as though a certain amount oi
moisture on the balls was necessary to render them sensitive to the heat.
In order that these results might be obtained, it u'as necessary that
the vapour should be free from air. If a small quantity of air was
present, although not enough to appear in the gauge, the eflocts rapidly
diminished, particularly that of the ice, until the cony ect ion-currents hud
it all their own way. This agrees wifh the fact that the presence of a
small quantity of air in st«am greatly retards condensation and evea
evaporation.
With a dry flask and an air-vacuum, neither the lamp nor the ice
produced their effects ; the convection-currents reigned supreme even
when the gauge was as low as j inch. Under these circumstances the
lamp generally attracted the balls and. the ice repelled them, i.e. the
currents carried them to^'ards the lamp and from the ice ; hut, by placing
the lamp or ice very low, the reverse effects could be obtained, which
goes to prove that they were the effects of the currents of air.
These eiperiments appear to show that evaporation from a surface ia
attended with a force tending to drive the surface back, and condensa-
tion with a force tending to draw the surface forward. These effects
admit of explanation, although not quite as simply as may at first sight
appear.
It seems easy to conceive that when vapour is driven off from a body
there must be a certain reaction or recoil on the part of the body ; Hero's
engme acts on this principle. If a sheet of damp paper be held before
the fire, fi'om that side which is opposite to the fire a stream of vapour
will be drawn off towards the fire with a perceptible velocity ; and there-
fore we can readily conceive that there must be a corresponding reaction,
and that the paper will be forced back with a force equal to that which
urges the vapour forwards. And, in a similar way, whenever condensa-
tion goes on at a surface it must diminish the pressure at the surface,
and thus draw the surface forwards.
It is not, however, wholly, or even chiefly, such visible motions as these
that afford an explanation of the phenomena just described. If the only
forces were those which result from the perceptible motion, they would
i
1874.] cmuei by Evaporation tmd CondeiuaHoa. 408
be insensible, except wben tbe heat on the iurEsce was sufficiently
intense to drive the vapour off with considerable velocity. This, indeed,
might be the case if vapour had no particles and was, what it appears to
be, a homogeneous elastic medium, and if, in changing from liquid into
gas, the expansion took place gradually, bo that the onlj velocitj acquired
by the vapour was that necessary to allow its replacing that which it
forcea before it and giving place to that which follows.
But, although it appears to have escaped notice so far, it follows, aa a
direct consequence of the kinetic theory of gases, that, whenever evapo-
ration takes place from the surface of a solid body or a liquid, it must
be attended with a reactionary force equivalent to an increase of pressure
on the surface, which force is quite independent of the perceptible
motion of the vapour. Also, condensation must be attended with a force
equivalent to a diminution of the gaseous pressure over the condensing
surface, and likewise independent of the visible motion of the vapour.
This may be shown to be the case as follows : —
According to the kinetic theory, the molecules which constitute the
gas are in rapid motion, and the pressure which the gas exerts against
the bounding surfaces is due to the successive impulses of these molecules,
whose course directs them gainst the surface, from which they rebound
with unimpaired velocity. According to this theory, therefore, whenever
a molecule of liquid leaves the surface henceforth to become a molecule
of gas, it must leave it with a velocity equal to that with which the
other particles of gas rebound — that is to say, instead of being just
detached and quietly passing off into the gas, it must be shot off with a
velocity greater than that of a cannon-ball. Whatever may be the nature
of the forces which give it the velocity, and which consume the latent
heat in doing so, it is certain, from the principle of conservation of
momentum, that they must react on the surface with a force equal to
that exerted on the molecule, just, as in a gun the pressure of the powder
on the breech is the same as on the shot.
The impulse on the surface from each molecule which is driven off
by evaporation must therefore be equal to that caused by tlie rebound
of one of the reflected molecules, supposing all the molecules to be of
the same siie ; thai, is to say, since the force of rebound will be equal to
that of stopping, the impulse from a ptulicle driven off by evaporation
wilt be half the impulse received from the stopping and reflection of a
particle of the gas. Thus the effect of evaporation will be to increase
the number of impulses on the surface; and although each of the new
impulses will only be half as effective as the ordinary ones, they wiU add
to the pressure.
In the same way, whenever a molecule of gas comes up to a surface
and, instead of rebounding, is caught and retained by the surface, and is
thus condensed into a molecule of liquid, the impulse which it will thus
impart to the surface will only In one halt h great as if it had rebounded.
404 Prof. 0.. Reynolds on Surface-Forces [June 18,
Hence coadensntioD will reduce the magnitude of some of tbe impulsea,
Bnd therefore will reduce the pressure on the condensing surface.
For instance, if there were two surfaces in the same vapour, ooe of
which was dry and the other evaporating, then the pressure would
be greater on the moist surface than on that which was dry. And,
■gain, if one of the surfaces was dry and the other condensing, thea
the pressure would be grejil^r on the dry surface thpn on that which
was eondenaing. Hen^e, if the opposite sides of a pith-baU in vapour were
in such different conditions, the ball would bo forced towards the cold^
These effects may be expressed more definitely as follows : —
Let 1/ be ihe velocity with which the molecules of the vapour move,
P the pressure on a unit of eurfM'e,
d the weight of a unit of volume of the I'apour,
v the weight of liquid evaporated or condensed in a second ;
'then the weight of vapour which actually strikes the unit of dry
fluifftce in a second will be •
~^' \
mnd the pressure ji ^^■i]] be given by
and / (the force arising from evaporation) will be given by
Thus we have an expression for the force in terms of the quantity of
water evaporated and the ratio of the pressure to the density of the
vapour ; and if the heat necessary to evaporate the liquid (the latent
heat) is known, we can fuid the force which would result from a given
expenditure of heat.
Applying these results to steam, we find that, at a temperature of 60°,
the evaporation of 1 lb. of water from a surface would be sufficient to
maintain a force of 65 Iba. for one second.
It ia also important to notice that this force will be proportional to the
square root of the absolute temperature, and, consequently, will be
approximately constant between temperatures of 32° and 212°.
If we take mercury instead of water, we find that the force ia only
6 lbs. instead of 66 lbs. ; but the latent heat of mercury is only -^ that of
water, so that the same expenditure of heat would maintain nearly three
times as great a force.
It seems, therefore, that in this way we can give a satisfactory ex- '
■ See Maiwsll, ' Theory of Heat,' p. 504.
1874.] catued by Svaporalion and QmdentaliotL 40S
plsoation of the experiments previouslj desciibed. When the radutted
heat from the lamp falls on the pith, ita tempenture will rise, and sa^
moisture od it will begin to evaporate and to drive the pith from the
lamp. The evaporation will be greatest on that ball which ia nearest to
the lamp ; therefore this ball will be driven away until the force on the
other becomes equal, after which the balls will come to rest, unless
momentum carries them further. On the other h&nd, when a piece of
ice is brought near, the temperature of the pith wUl be reduced, and it
wiH condense the vapour and be drawn towards the ice.
It seems to me that the same explanation may be given of Mr. Grookes's
experiments ; for, although my experiments were made on water and at
compamtively high pressures, they were in reahty undertaken to verify
thu explanation as I have given it. I used water in the hope of finding
{at I have found) that, in a condensable vapour, the results could be
o 1 lined with a greater density of vapour (that is to say, with a much less
pi<:-. 'ct vacuum), the effect being a consequence of the saturated condition
ot the vajKiur rather than of the perfection of the vacuum.
Mr. Crookes only obtained his results when his vacuum was nearly as
perfect as the Sprengel pump would make it. Up to this point he had
nothing but the inverse effects, viz. attraction with heat and repulsion
with cold. About the cause of these he seems to be doubtful; but I
venture to think that they may be entirely explained by the expansion of
the surrounding gas or vapour, and the consequent convection-currents.
It must be remembered that whenever the air about a boll is expanded,
and thus rendered lighter by heat, it will exercise less supporting or
floating power on the ball, which will therefore tend to sink. This ten-
dency will be in opposition to the lifting of the ascending current, and it
will depend on the shape and thickness of the ball whether it will rise
or fall when in an ascending current of heated gas.
The reason why Mr. Crookes did not obtain the same results with a
less perfect vacuum was because he had then too large a proportion of
air, or non-condensing gas, mixed with the vapour, which also was not in
a state of saturation. In his experiments the condensable vapour was
that of mercury, or something which required a still higher temperature,
and it was necessary that the vacuum should be very perfect for such
vapour to be any thing like pure and in a saturated condition. As soon,
however, as this state of perfection was reached, then the effects were
more apparent than in the corresponding case of water. This agrees
well with the explanation ; for, as previously shown, the effect of mercury
would, for the same quantity of- heat, be three times as great as that of
water; and, besides this, the perfect state of the vacuum would allow
the pith (or whatever the ball might be) to move much more freely than
when in the vapour of water at a considerable tension.
Of oonrse this reasoning is not confined to mercury and water; any
gas which is condensed or absorbed by the balls when cold in greater
406 Prof. 0. Reynolds on Sitrface-Forcet [June 18,
quantitiea than when warm would give the same results ; and, as this
property appears to belong to all gaBe%, it is cmlii a question of bringing
the vacuum to the right degree of tensicn.
There was one fact connected with Mr, Crookea's experiments which,
independently of the previous consideration?, led me to the conclusion
that the result was due to the heating of the pitb, and was not a direct
result of the radiated heat.
In one of the experimeuta exhibited at the Soirtfe of the Boyal Society,
a candle was placed cloee to a flask containing a bar of pith suspended!
from the middle ; at first, the only thing to notice was that the pith waa
osciJUting considerably under the notion of the candie i each end ot the
bar alternately approached and receded, showing that the candle exercised
an influence similar to that which might have been exercised by the torsion
of the thread had this been stiff. After a few niimites' observation,
however, it became evident that the oscillations, instead of graduaUr
diminishing, as one naturally expected them to do, continued ; and, more
than this, thev actually increased, until one end of the bar passed the light,
after which it seemed quieter for a little, though the oscillations again
increased until it again passed the light. As a great many people and
lights were moving aboat, it seemed possible that this might be doe to
external disturbance, and so its full importance did not strike me.
Afterwards, however, I saw that it was only to be explained on the
ground of the force being connected with the temperature of the pith.
During part of its swing one end of the pith must be increasing in tem-
perature, and during the other part it must be cooling. And it is easily
seenthatthe ends will not be hottest when nearest the light, or coldest when
furthest away ; they will acquire heat for some time after they have begun
to recede, and lose it after they have begun to approach. There will, in
fact, be a certain lagging in the effect of the heat on the pith, like that
which is apparent in the action of the sun on a comet, which causes the
comet to be grandest after it has passed its perihelion. From this cause
it is easy to see that the mean temperature of the ends will be greater
during the time they are retiring than while approaching, and hence the
driving force on that end which is leaving will, on the whole, more than
balance the retarding force on that which is approaching ; and the result
will be an acceleration, so that the bar will swing further each time until
it passes the candle, after which the hot side of the bar will be opposite
to the light, and will for a time tend to counteract its effect, so that the
bar will for a time be quieter. This fact is independent evidence as to
the nature of the force ; and although it does not show it to be evapora-
tion, it shows that it is a force depending on the temperature of the pitfa,
and that it is not a direct result of radiation from the candle.
Since writing the above paper, it has occurred to me that, according to
the kinetic theory, a somewhat similar effect to that of evaporation must
result whenever heat is communicated from a hot surface to gas.
1874.] camad by Evi^xtrtUim and Condensation. 407
The particles which impinge on the surface will rebound with a greater
velocity than that with which they approached ; and consequently the
effect of the blow must be greater than it would hare been had the sur&ce
been of the some temperature as the gas.
And, in the same way, whenever heat is communicated from a gas to a
surface, the force on the surface will be less than it otherwise would be,
for the particles will rebound with a less velocity than that at which they
approach.
Mathematically the result may be expressed as follows — the symbols
having the same meaning as before, e representing the energy communi-
cated in the form of heat, and Su the alteration which the velocity of the
molecule undergoes on impact. As before.
_dv(v + lvf—v' dtt^hv
Therefore, in the case of steam at a temperature of 60°,
■^^2000'
and in the case of air
■'^lioo'
It must be remembered that c depends on the rate at which cold
particles will come up to the hot surface, which is very slow when
it depends only on the difiuaion of the particleB of the gas inter te and
the diffusion of the heat amongst them.
It will be much increased by convection-cnrrents ; but these will (as
has been already explained), to a certain extent, produce an oppoBit«
effect. It would also seem that this action cannot have had much to do
with Mr. Crookes's eiperimenta. as one can hardly conceive that much
heat could be communicated to the gas or vapour in such a perfect
vacuum as that he obtained, unless, indeed, the rate of diffusion varies
inversely as the density of a gas*. It will be interesting, however, to
see what light experiments will throw on the question.
* June 10. — Frohanor Huwell has ahown that the diffution both of heat and of
tba gaa Tiriei invenely m the detudCy ; therefore, excepting for conTectionHnirrentB,
the amount of b««,t oonmunioted IVom a mitfaoe to a gas would be independent
of the denait; of the gat, and benee the force / would be indopendent of the demit; ;
that is to sa;, thia foroe would remain constant aa the Tacuum improTed, while the
canTectiOD.ourrents and ooonteracting foroe* would gradoallj diminish. It seema
probable, therefore, that Hr. CrookM'a reeolta are, at least in part, due to tbia foroe.
VOL. ZZIt. 2 I
408 Capt. Noble and Mr. F. A. Abel [June 18,
IX. " Rcaearcbes on Explosives, — Fired Gunpowder." By Capt.
NonLE, late Royal Artillery, F.R.S., F.R.A.S., FX.S., and
F. A. Abel, F.r'.S., Treas. C.S.*
(Abstract.)
After an historical review of the investigations and theoretical viewa
relating to the resalts produced upon the explosion of gunpowder, flrhieh
have been published during the last 150 years, the authors proceod to
describe the chief objects contemplated by their researches, which are in
continuation of some commenced by Captain Nobie in 186S, and dd-
scribed in a lecture delivered at the Boyal Institution in I87I.
These objects were as follow : —
Firtt. To ascertiun the products of combustion of gunpowder, fired
under circumstances similar to those which eiiflt when it is exploded in
guns or mines.
Sftond. To ascertain the tension of the products of cwnbustion at the
moment of eiploaiou, and to determine the law according to which the
tension varies with the gravimetric density of the powder.
Third. To ascertain whether any, and, if so, what well-defined variation
in the nature or proportions of the products accompanies a change in the
density or size of grains of the powder.
Fourth. To determine whether any, and, if so, what influence is eierted
on the nature of the metamorphosis by the pressure under which the gun-
powder is fired.
Fifth. To determine the volume of permanent gas liberated by the
explosion.
Si-rth. To compare the explosion of gunpowder fired in a close
Teasel with that of simUar gunpowder when fired in the bore of a gun.
Seventh. To determine the heat generated by the combustion of gun-
powder, and thence to deduce the temperature at the instant of ex-
plcio..
Eighth, To determine the work wbich gunpowder is capable of per-
forming on a shot in the bore of a gun, and thence to ascertain the total
theoretical work, if the bore be supposed of iudeflnite length.
The several methods of experiment adopted by the authors, and the
most important apparatus employed in their researches, are next described
in detail. The experimental operations include: — 1, Measurement of
pressure developed ; 2. Measurement of volume of permanent gases ;
3, Measurement of heat developed ; 4. Collection of gases ; 5. Collection
of solids ; 6. Analysis of the gaseous and solid products.
* We have to eiprcce our scknowlcdgrncnts of the valuable assistance ne bavo
rereiTed rrnm Mr. Charles Hutchinson in making the yfrj laboriaiie calculations, from
Mr. Q«Drge Stuart in the mechanical arranf^iente and in carrying out tbeeiperimentn
thsiQMlm, and from Dr. Kellner and MeRsrs. Deariag, Dodd, and Hobler in the ana-
lytical portion of thew raaearohes.
1874.]
on Fired Giagmwder.
409
The g^unpovder operated upon in the experiments includes five kiudj,
viz. pebble powder, rifle large-grain (cannon) powder, fine-grain powder,
and rifle fine-grain powder (all of Waltham -Abbey manufacture), and also
a apherical pellet powder of Spanish manufacture, specially selected for
experiment as prcaenting considerable difference in composition from
the English powders. The composition of the powders is shown in the
folJowiug Table : —
Table I.
lUsulli of AnaltfHU of Gunpowder* mnplayed.
Componeoti,
i per wnt.
Pebble -
Waltbam
Abbey.
RiRe
WBUham
Abbej.
Rifle
Waltham
Abbej,
Waltham
Abbey.
Spanish
powder.
7487
0^
74Wi
0'15
75-M
0-14
0-36
Pola^Kiiini aulpliHte ...
0-27
low
1212-1
?11 "-^
O-23J
0-05
10-27
low
0-25 J
MI
993
10-«7
^■'~ 1400
2(irt '*™
0-24
0-80
10«2
11-38-1
»:|? .459
0-17 J
1-48
! ^ Carbon ...
ChsrooJ "Jdrogen..
Wator
0«3 1
The qnantiticB of gunpowder exploded in the several operations ranged
from 750 grammes to 100 grammes. The following is a description of
the apparatus in which the charges were exploded : —
The apparatus consisted of a mild steel ve-ssel, of great strength, care-
fully tempered in oil, in the chamber of which the charge to be exploded
was placed. The main orifice of the chamber was closed hy a screwed
plug, called the firing-plug, fitted and ground into its place with great
exactness.
In the firing-plug itself was a conical hole, stopped by a plug, also
ground into its place with great accuracy, and, for purposes of insulation,
covered Tiith the finest tissue-paper. Two wires (one in the insulated
cone, the other in the plug) were inserted, arad joined by a very fine
platinum wire passing through a small glass tube filled with mealed
powder. By completing connexion with a Daniell's battery, the charge
could be fired.
There were two other apertures in the chamber — one communicating
with the arrangement for letting the gases escape, the other containing
the crusher^pparatuB For detennlning the tension at the moment tA.
explosion.
The pressures actually observed with the apparatos juflfc described
2i2
410 Capt. Noble and Mr. F. A. Abel [June 18,
varied from over 36 tons on the square Incli to about 1 ton on the square
The dangerous nature of the operations of explosion, carried out on ao
considerable a scale as m these investigations, rendered great precautions
necessary. Unless the explosion-cylinder was most perfectly closed, the
violent escape of gas resulted in its immediately cutting a way out for itself,
destroying the arrangement for closing the apparatus.
Special obserralHonB vere made to ascertain how long a period elapsed
after explosion before the non-gaseous products assumed the solid form.
They appeared to do this a little within two minutes after explosion, when
a charge nearly filling the vessel was used.
The method employed for collecting the gaseous products as soon as
possible after the explosion presented no special feature of novelty. On
opening the esplos ion-vessel after the gases bad been allowed to escape,
the solid products were found collected at the bottom, there being gene-
rally an exceedingly thin (in fact, with lai^e charges, quite an inappreciable)
deposit on the sides. The surface of the deposit was generally perfectly
smooth and of a very dark grey, almost black, colour. This colour, how-
ever, was only superficial, and through the black could be perceived what
was probably the real colour of the siirfaci?, a dark olive-green. Tho siir-
£ace of the deposit, and the sides of the cylinders, had a somewhat greasy
appearance, and were indeed greasy to the touch. On the smooth surface
were frequently observed very minute particles, in appearance lite soot,
but of the greasy t«xture to which allusion has been made.
The remo^-al of the deposit was generally attended with great difficulty,
aa it formed an exceedingly hard and compact mass, which always had to
be cut out with steel chisels. Lumps would frequently break ofE, but a
considerable portion flew off before the chisel in fine dust. In various
experiments, on examining the fracture as exhibited by the lumps, the
variation in physical appearance was very striking, there being marked
differences in colour, and also, frequently, a marked absence of homo-
geneity, patches of different colours being interspersed with the more
nniform shade of the fracture. There was no appearance of general crya-
tolline structure in the deposit ; but, on examination with a microscope,
and sometimes with the naked eye, shining crystals of metallic lustre
(sulphide of iron) were observed. On the whole, the general appearaace
of the deposit was attended with such considerable variations, that, for
minut« details, reference must be made to the account of the experiments
themselves. The deposit always smelt powerfully of sulphuretted hy-
drogen, and, frequently, strongly of ammonia. It was always exceedingly
deliquescent, and after a short exposure to the lur became black on the
surface, gradually passing over into an inky-looking pasty mass. As in
physical appearance, bo in behaviour, when removed from the cylinder,
there were considerable differences between the experiments. The de-
posit was transferred to thoroughly dried and warm bottles, and sealed
1874.] on Fired Gvapowder. 411
tip as rapidly as possible. In most cases, during the very short time that
elapsed while the transfeieace was being made, no apparent change took
place } but, in some, a great tendency to development of heat was appa-
rent ; and in one instance, in which a portion of the deposit (exhibiting
this tendency in a high degree) was kept exposed to the action of the ur,
the rise of temperature was so great that the paper on which it was
placed became charred, and the deposit itself changed colour with great
rapidity, becoming a bright orange-yellow on the surface.
This tendency to heat always disappeared when the deposit was con-
fined in a bottle and fresh access of air excluded.
The methods employed in the analysis of the gaseous and solid products
of explosion differed only in a few respects from those adopted by
Bunsen and SchischkoS in their investigatdon of the products of explosicm
of powder.
As regards the proportions of total solid and gaseous products fur-
nished by the several powders, remarkable oniformity was ezhituted by
the results of explosion of the same powder at different preesuiea, and no
very considerable difference existed between the proportions furnished by
the three powders chiefly used in the researches. The lai^eet gnun, or
pebble powder, yielded most gas ; the quantity furnished by &. L. G.
powder was not greatly inferior, but was decidedly more considerable
than that yielded by the smallest powder (F. Q.).
The composition of the gat furnished by the explosion of all the Eng-
lish powders was throughout remarkably uniform, but presented certain
apparently well-defined small variations, regulated by the pressure under
which the products were developed, the chief being a steady increase in
the proportion of carbonic anhydride, and decrease in that of carbonic
oxide, in proportion as the pressure was increased. The composition <d
the solid products exhibited much greater variations, cbiefiy in regard to
the state of combination in which the sulphur existed. These variatimu
were exhibited not merely by the products obtained from the different
powders, but also, and to as great an extent, by those which one and the
same powder furnished at different pressures, and apparently vrithont
reference to the pressure, excepting in the case of the very lowest
(the powder occupying 10 per cent, of the total space in the chamber).
The authors institute a comparison between the composition of the
products oE explosion obtained in their experiments and the analytical
results published by Bunsen and Schischkoff and other recent experi-
menters, and proceed to a critical examination of the methods pursued by
these for obtaining the products of the compcmtion of gunpowder, giving
reasons why the results which those methods of operation have furnished
cannot be accepted as representing the changes which powder undergoes
when exploded in a closed space.
The authors further proceed : — It is evident that the reactions which
occur among the powder-constdtuents, in addition to those which result
412 Capt. Noble and Mr. F. A. Abel [June 18,
in the deTeJopment of gas, of fairly uniform compositioa (and very uni-
form na regards the proportions which it K-ars to the solid), from powders
not differing widely in coDBtitution from eiieh other, ore susceptible o£
very eousidurable rariations, regarding the causes of which it appearti only
possible to form conjtK'tureB. Any attempt to express, even in a com-
paratively complicated chemical equation, the nature of the met&mor-
phosis whieh a gun|)owder of as^erage composition may be considered to
undergo when esploded in a oonlined space would therefore only be
calculated to convey an erroneous inipresaiou ns to the simplicity, or the
definite nature, of the chemical results and their uniformity under dif-
ferent conditions, while it would, in reality, posBess no important bearing
upon the elucidation of the theory of explosion of gunpowder.
The extensive experiments which the Committee on Explosive Sub-
stances has instituted, with English and foreign giuipowdersof very vaiioua
composition, have conclusively demonstrated that the influence exerted
upon the action of fired gunpowder by comparatively very considerable
variations in the coimtitution of the powder (except in the case of small
charges apphed in firearms) is often very small as compared vritb (or
even more than counterbalanced by) the modifying effects of variations in
the imrchiinic'il aaAjihi/aUrd' properties of the powder (i, c in its density,
hardness, the size and form of the grains or individual masses, &c.).
Hence it is not surprising to find that a fine-grain gunpowder, which
differs much more in mechanical than in chemical points from the larger
powder (E. L. G.) used in these experiments, should present decided dif-
ferences, not only in regard to the pressures which it develops under
similar conditions, hut also aa regards the proportions and uniformity of
the products which its explosion furuiKhes, On the other hand, the dif-
ferences in regard to size of individual masses, and other mechanical pe-
culiarities, between the It. L. G. ond pebble powders are, comparatively,
not so considerable, and are in directions much less likely to affect the
results obtained by explosions in perfectly closed spaces.
Again, the analysis of solid residues furnished by various kinds of gun-
powder, which presented marked dissimilarity in composition, did not esta-
blish points of difference which could be traced to any influence exerted
by such variations ; indeed the proportions of the several products com-
posing residues which were furnished by one and the same powder, in
• The desirability of BppljiDg Ihesa menna to effecting modifi cations in the action of
flred gunpowder wns poinlcd out bj Colonel (now General) Boier in a rafmorandum
aubraitted M tlieWar Office in ISTtd; and Ibe first Quvemmcnt Comoiillee on Gunpowder.
BOOH afterwards appoint^ (of which Ooneral Boier niid Mr. Abel were membera), ob-
tained Buceej^ful results, which werB reported officially ill 18IJ4. by limiting thealtera-
tionein the manufacture of gunpowder intended for use in licnvy guns to tiiudification^
in the form, siie, density, and hardness of the individiml^raitiB or uiaBs«e, tile compoBitioii
of the powder remainiog unaltered. The Committee on Biplo^ito Sulwtaneea bavo
adhered to this system in producing gunpowdersuitable for the largest Otdnanca of ttw
pieaentday.
1874.] OR fired Gm^wder. 418
distinct experiments made at varied presauree, differed, in sevenl in-
stances, quite as greatly as those found iu some of the residueB of powders
which presented decided differences in composition.
Although, for the reaeouB already given, the authors cannot attempt
to offer emj thing approaching a precise expression of the chemical
changes which gunpowder of average composition undergoes when ex-
ploded in a confined space, they feel warranted, by the results of their
experiments, in stating, with confidence, that the chemical theory of the
decomposition of gunpowder, as based upon the results of Bunsen and
Schischlioff and accepted in recent text-books, is certainly as far from
correctly representing the general metamorphosis of gunpowder as was
the old and long-accepted theory, according to which the primary products
were simply potassium sulphide, carbonic anhydride, and nitrogen.
Moreover, the following broad tacts regarding the products furnished by
the explosion of gunpowder appear to them to have been established by
the analytical results arrived at.
1 . The proportion of carbonic <Kcide produced in the explosion of a gun-
powder in which the saltpetre and charcoal exist in proportions calculated,
according to the old theory, to produce carbonic anhydride only ia much
more considerable than hitherto accepted.
2. The amount of potaitium carhonatt fonned, under all conditions
(as regards nature of the gunpowder and pressure under which it is ex-
ploded), is very much larger than has hitherto been considered to be pro-
duced, according to the results of Bunsen and Schischkoff and more recent
experimenters.
3. The j^otoMium tulpkaU ia very much smaller in wnount than found
by Bunsen and Schischkoff,Linck, and Karolyi, even in the highest results
obtained in the authors' experiments.
4. Pataisium iutphide is never present in very considerable amount,
though, generally, in much larger proportion than found by Bunsen and
Schischkoff ; and there appears to be strong reason for believing that, in
most instances, it exists in Iar^« amount as apn'ntory result of the explo-
sion of gunpowder.
5. Potassium Aifposulphite is an important product of the decomposi-
tion of gunpowder in closed spaces, though very variable in amount. It
appears probable (the reasons being fully discussed in the paper) that its
production is in SMne measure subservient to that of the sulphide ; and it
may perhaps be regarded as representing, at any rate to a considerable
extent, that substance in powder-residue — i. «. as having resulted, partially
and to a variable extent, from the oxidation, by Uberated oxygen, of sul-
phide which has been formed in the first instance.
6. The proportion of sa^hur which does not enter into the primary
reaction on the explosion of powder is very variable, being in some
instances high, while, in apparently exceptional results, the whole amount
of sulphur contmned in the powder becomes involved in the metamor-
414 Capt. Noble and Mr. F. A. Abel [June 18,
phosis. In the case oF pebble powder, the mechiuucal coadition (size and
regularity of grain) of which is perhaps more favourable to uniformity ot
decomposition, under varied eonditiooB as regards pressure, than that of
the smalier powders, the amount of sulphur which remains aa potassium
pol}%ulphide is very uniform, eioept in the producta obtained at the lowest
pressure ; and it is noteworthy that with E. L, G. powder, under the
same conditions, contparntiTely little sulphur escapes ; while in the case of
P, Q. powder, under corresponding circumstances, there is no free sulphur
at all.
7. But little can be said with regard to those producta, gaseous and
solid, which, though almost always occurring in small quantities in the
products, and though apparently, in some instances, obeying certain rules
with respect to the proportion in which they are formed, cannot be
regarded as important results of the eiplosion of powder. It may, how-
ever, be remarked that the regular formation of such substances as
potassium sulphocyanate and ammonium carbonate, the regular escape
of hydrogen and aulphydric acid from ondation, whiJe oxygen is occa-
sionally coexistent, and the frequent occurrence of appreciable proportions
of potassium nitrate, indicate a comptesity as well as an incompleteness
in the metamorphosiH, Such complexity and incompleteness are, on the
one hand, a natural result of the great abruptness as well as of the com-
parative diiEculty with which the reactions between the ingredients of
the mechanical mixture take place ; on the other hand, they favour the
Tiew that, even during the exceedingly brief period within which
chemical activity continues, other changes may occur (in addition to the
most simple, which follow immediately upon the ignition of the powder)
when explosions take place at pressures such as are developed under
practical conditions.
The tendency to incompleteness of metamorphosis, and also to the
development of secondary reactions, under favourable conditions, appears
to be fairly demonstrated by the results obtained in exploding the different
powders in spaces ten times that which the charges occupied (Experi-
ments 8, 1, and 16). It appears, however, that, even under conditions
apparently the moat favourable to uniformity of metamorphosis (namely,
in explosions produced under high pressures), accidental circumstances
may operate detrimentally to the simplicity and completeness of the
reactions. But the fact, indisputably demonstrated in the course of
these researches, that such accidental variations in the nature of the
changes resulting from the explosion do not, even when very consider-
able, affect the force exerted by fired gunpowder, as demonstrated by the
recorded pressures, &c., indicates that a minute examination into the
nature of the products of explosion of powder does not necessarily con-
tribute, directly, to a comprehension of the causes which may operate in
modifying the action of fired gunpowder.
In illustration of the analytical results obtained in these investigations
1874.] on Fired Gunpowder. 416
the following etatement u given of the percent^e composition of the
products of explosion, under one or two different pressures, of the three
principal powders used.
Table II.
Sh/>wi>iff iUuttrative Examples of the Analytical Raultt obtaitud.
Pebble. B. L. 6. F. O.
'"ST."'?'"'"'!!!.''"!} "''^ *»" "'^ ='■" »" ™-™
'JSfuT.T*!'!!*.'''.'^!"} «■*" «*= •^'" *'» "«> "i*!
PercenUge weights of solid product! □[ eiploaioQ ; —
Potassium carboiutte 65-50 6615 62-56 65-71 68-39 43-03
Bulphsto 15-02 11-03 20-47 8-52 24-22 21-00
hyposulphite 20-73 6-12 20-37 8-69 530 32-07
monosulphida 7-41 19-12 4-02 7-23 512
sulphocnnale 0-09 0-23 traoe 0'3S 0-02 023
nitrate O'iS 0-20 0-56 0-19 0-06 0-19
oDde 2-98
AmmoniDm sesquicsrbonate 0-16 0-08 0-06 0-18 0-15 0-03
Sulphur 0-61 617 1-25 9-22 5-72 0-47
Carbon trace tnwe 0-71 tnoe tnoe
Percentage volumee of gaseous producW : —
Carbonic snlivdride 46-66 49-83 48-99 6179 4741 5302
Carbonic oiida 14-76 1336 8-96 8-32 12-35 7-91
Nitrogen 32-75 3219 S5-60 34-64 32-35 3420
Sulphvdric acid 313 1-96 4-06 2-61 3-76 2-03
Harsh-gas 0-68 029 041 0-60
Hjdrogen 2-70 206 2-07 2-04 413 213
Oiygen 0-18 0-15
Table m.
Shoviiag the eompoailion by weight of the prodwit of explosion of a gramme
of powder atfumi^ted by Ae above examples.
Pebbla. B. L. O. F. Q.
Potassium carbonate -3115 -SfSJi -Sot -OT56 -^H ^d
hjpoidlpWte -1163 -0338
sulpbab) -0843 -0658
sulphide -0416 -1055
«ulphocTBnat« -0005 -0013
nitrate -0027 -0011
Anunonium sesquicarbonate -0009 -0004
ToCalsolid -5612 -5517
SulphTdric aoid -0134 -0064
Oxygen
Carboaiooiide -0519 -0473
Carbonic anhydride -2577 -2770
Marah-g«s -0012
Hydrogen -0007 "0005
Nitrogen 1161 -1139
Total guMM* •4388 -4483 -^78 -4286
■Ufift
■0*91
■0308
■1863
■1171
■0487
■1409
■1220
-tWMO
•0413
■0298
■0110"
•0021
•0001
■00 3
■0032
■0011
■0006
■00 1
-0009
-0333
0027
■5722
-6714
■5817
-6808
■0166
0077
-0154
■ooei
•0006
■0303
■0356
■0*16
•0258
■2597
■2760
■2512
'0006
■0015
■0009
-(HKlfi
■0003
■0010
■0005
■1201
■1085
■1091
■1117
416
Capt. Noble and Mr. F. A, Abel
[June 18,
Aa it was oue of the principal objects of the authors to del«rmiiie,
with as muL'h aceurafj' as posaible, not oiilv t/ie Unston o/Jired yutijiowder
vv'beu tilling I'oiiipWieiy the space in whii'h i( was expladetl, but ulso to
dettrmiue the lam acconiiiuj to which the Unaion varied with the deruiti/, the
esperimetitB tnBtitutad to ascertain these important points were both
A-aried and complete. The goneral results obtained are given in ibe
annexed Tabl&.
Table IV.
Shotfinif the pressure eorreaponding to a given density of Ae products of
exphaion of F. C/., S, L. O,, and pebble powders, at deduced Jiwn actual
observation, in a close vessel.
III
<to™p™di»g
Ilea ifvmtr
VllWC Md
Vi;s:'
pToTlJtnrfer.
tgwd«..
iwwdcn.
Ton.p<r
«SSfKi.
Taiupr
^^.SL
■10
1^47
1-47
•60
i4'3y
•20
3-26
3-26
■70
1909
18-31
■30
5-33
5-33
■80
25-03
23-71
■40
7-75
7-74
■90
32-40
30-39
■50
lO'CiU
10'59
1^00
41-70
38-52
The determination of the heat developed by the explosion was alao
made the subject of careful direct experiment, and, from the mean of
several closely concordant results, it was found that the combustion of a
gramme of the powders experimented with generated about 705 gramme-
units of heat. Bunsen and Schischkoff's assumption, that the specific
heats of the solid products remain invariable over the great range of
temperature through which they pass, is considered by the authors
untenable; they have, however,deduced the temperature(about3800''C.)
upon this hypothesis, both to facilitate comparison of their results with
those of Bunsen and Scbischkoff, and to giie a high limit, to which the
temperature of explosion can certainly not attain.
The vohmui of solid products obtained from a gramme of powder is
fixed by the authors at about -3 cub, cent, at ordinary temperatures.
A comparison is next instituted of the pressures actuaUy observed to
enat in a close vessel with tliat calculated upon the assumption that, at
the moment of explosion, about 57 per cent, by weight of the products of
explosion are non-gaaeoua, and 43 per cent, in the form of permanent
gases. The relation between the pressure and the density of the pro-
ducts of combustion may be expressed by the following equation,
_p = const. >
(3)
(a being a constant determined from the experiments) ; and a compariBon
of the results is given in the following Table :—
1874.]
•n Fired Gtmpowder,
Table V.
Sliounng the totmparima, in Urns ptr square iiuh, between At prettaret aetaallg
observed in a close veetet and those ealculated from Hie formula (3).
DnwiilT or
Vilu of p
diceutobwi.
HS
liinwtoUcf-
.1^^'lJL
-^^"'-
■M
■^I^f*^
1-50
•GO
1439
14-39
■20
3-26
3-30
■70
19^09
18-79
■30
5-3^
5-45
■80
25^03
24^38
■4U
1-7 o
7^9 1
■90
32-46
31-73
■50
10-0S>
H)^S4
1-00
41-70
41^70
The authors couaider that the accordance of this compamon with
observed results fully establiahea the accuracy of their vieirs.
The data furnished by the foregoing enable the authors to detenuiud
theoretically the temperature of exploaiou of gunpowder, which they find
to be about 2200° 0, The con-ectnesa of this theoretical eatimate they
confirm by eiperimenta! observationa on the behaviour o£ platinum when
exposed to the temperature of explosion. In all instances thin platinum
wire or foil showed signs ot fusion, but actual fusion took place only in
one instance.
The mean specif heal of the iion-gaseous products and theirprobable expan*
eion between 0° C. and the temperature of explosion are next discussed.
The means of obtaining the tensions of the products of explosion in
the bores of ordnance, aud the results obtained in this direction by the
Committee on Explosives, are then examined, as far as regards the
particular powders with which the authors have experimented.
The correctness of the view propounded by Eobins, that the work
obtainable from gun[>owder is not importantly increased by increments
to the weight of the shot, is confirmed by the authors, and the influence
upon the tension of fired gunpowder exert«d by the existence of water in
powder is illustrated.
The extent of communication of heat to the enrelope (or gun) in which
the powder is exploded is next considered, and experiments and calcu-
lations are given to show that such communication of heat varies from
about 35 per cent, of the total heat generated in the case of a small
arm to about 3 per cent, in the case of an 18-ton gun.
A comparison is instituted between the pressures actually found to
exist in the bores of guns and those which would follow from the facta
established by these researches. It is pointed out, on the one baud,
that the assumption, that all the products of combustion are iu the
gaseous state, is irreconcilable with the pressures actually observed ; and,
on the other hand, Bunsea and SchischkoS's hypothesis that the work on
the projectile is accomplished only \>j the permanent gases, without
addition or subtraction of heat, is shown to be equally irreconcilable with.
414 Capt. Noble and Mr. F. A. Abel [June 18,
phosU. In the case of pebble powder, the mechanical condition (sixe and
regularity of grwn) of which is perhaps more favourable to nnif ormitr of
decomposiriou, uader i-aried conditions as regards pressure, tfaim that of
the smaller powders, the amount of sulphur which remains as potassium
polyeulphide is veiy uniform, except in the products obtiuned at the lowest
preBsure ; and it is noteworthy tiiat with E. h. 0, ])owder, under the
same conditions, comparatively little sulphur escapes ; while in the case of
P. G. powder, under corresponding uircumstances, there is no free sulphur
ataU.
7. But little can be said with regard to those products, gaseous and
solid, which, though almost always occurring in small quantities in the
products, and though apparently, in some instances, obeying certain rules
with respect to the proportion in which they are formed, cannot be
r^arded as important results of the explosion of powder. It may, how-
ever, be remarked that the regular formation of auch substances aa
potassium sulpbocyanate and ammonium carbonat«, the regular escape
of hydrogen and sulphydric acid from oxidation, while oxygen is occa-
siooally coexistent, and the frequent occurrence of apprecjable proportions
of potassium nitrate, bdicate a eomplesity as well as an incompleteneas
in the metamorphosis. Such complexity and incompleteness are, an the
one hand, a natural result of the great nhnipfnesa m wi'l! as of the cora-
parative difficulty with which the reactions between the ingredients of
the mechanical mixture take place ; on the other hand, they favour the
Tiew that, even during the exceedingly brief period within which
chemical activity ccntinues, other changes may occur (in addition to the
most simple, which follow immediately upon the ignition of the powder)
when eiplosions take place at pressures such as are developed under
practical conditions.
The tendency to incompleteness of metamorphosis, and also to the
development of secondary reactions, imder favourable conditions, appears
to be fairly demonstrated by the results obtained in exploding the different
powders in spaces ten times that which the charges occupied (Experi-
ments 8, 1, and 16). It appears, however, that, even under conditions
apparently the most favourable to uniformity of metamorphosis (namely,
in explosions produced under high pressures), accidental circumstances
may operate detrimentally to the simplicity and completeness of the
reactions. But the fact, indisputably demonstrated in the course of
these researches, that such accidental variations in the nature of the
changes resulting from the explosion do not, even when very consider-
able, affect the force exerted by fired gunpowder, as demonstrated by the
recorded pressures, &c., indicates that a minute examination into the
nature of the products of explosion of powder does not necessarily con-
tribute, directly, to a comprehension of the causes which may operate in
modifying the action of fired gunpowder.
lu illustration of the analytical results obtained in these investigations
1874.] on Fired Gunpowder. 416
the following etatoment ii given of the percentage composition of the
products of explosion, under one or two different pressures, of the three
principal powders used.
Table II.
Shottiing iUuMrative Exampltt of the Analytical RwdU obtained.
Pebble. E. L. G. F. G.
Frenuro of eiploaion ia (otuI , .
per »qu»re inch /
Percentage weight of gueous I ^.gg ^^.g,
producW J
Percentage weights of lolid products of eiploaioD
uiArbonata 0-16 0<I8
Sulphur 0*1 617
Carbon traoo ttaco
Percentage volumee of gassoiu products :-
1-6
35-6
37
ie-2
67-22
57-14
68-I7
58-09
42-78
4286
41-83
41-92
52-56
65-71
69-39
43-03
20-47
e'52
24-22
21-00
20-37
869
630
32flT
4-02
7-23
612
tWOB
0-36
002
0-23
0-66
{H9
0-06
0-19
OiK
0-18
0-16
0-03
126
9-22
6-72
traoB
tRWW
48-99
6179
47-41
S3-09
8-ie
8-32
12-35
32-35
34'20
3-76
4-13
0-15
HitroBBn 32-75 32-19
Sulphjdrio acid 313 1-96
Hanh-gu 058
Hjdro^ 2-70 2-06
O^gen
Table lU.
Showing the atmpoiition by vieight of the producU of explosion of a gramme
of powder atfarnithed bg the above examplei.
Pebble. B. L. G. P. Q.
Potasaium carbonate -3116 -30W -»IOT -3^ '34H ^a
hypMulphite -lies -0338 -1166 -0491 -0308 -1863
Bubdiaki -0843 -Oa-iS -1171 -0*87 -1409 "1220
■ulphide -0416 -1055 -0230 -0*13 -0298
(ulphocranale -0006 -OOIS -0000 -0021 -0001 -OOIS
nitrate "0027 -0011 -0032 -0011 -0006 -0011
ojide -0173
Ammonium KHquicubonate -0009 -0004 -0003 -0009 -0009 -0002
carbon -0072
aulpbur -0034 "0340 "0041 -0527 -0333 -0027
Total Kilid -6612 -6517 -5722 -6714 -6817 6808
Sulphjdrio add -0134 -006* -0166 0077 -0164 -0081
Oijgen -0006
Carbonic oiide -0619 -0473 -0308 -0366 -0416 -0256
Carbonic anhjdride -2677 -2770 -2597 -2750 -2512 -2718
Marsh-aaa..... "0012 -0006 -0015 -0009
Hydrojwn -0007 -0006 -0006 -0003 iMlO -0006
Nitrogen 1161 -1138 1201 -1066 -1091 1117
Total pMoos -4368 •4488 -^78 -^86 -AISS -4192
420 Dr. Bninton and Mr. H. Power on Digitalis. [June 18,
X. " Oa the Diuretic Action of Digitalh." By T. LAroER
Bkoxton, M.D., D.Sc, and IIesrv Power, M.B., F.R.C.S.
Communicated by Dr. Sanderson, F.R.S. Received June 1,
1874.
It has been shown, by Mas Herrmann and Ludwig, that the rapidity of
the urinary secretion depends on the difference in pressure between the
blood in the renal glomeruli and the urine in the urinary tubulea.
At present, it is generally assumed that the diuretic action of BigitalU
is not caused by any specific influence of the drug upon the kidney, but
is due exclusively to ita power of increasing the blood- pressure in the
arterial system. .
The resiilts of some experiments made by us nearly a year ago show
that this is not the fact. On injecting a considerable dose of digitalin
(1-2 centigrammes) into the veins of .in etheriKed dog, we have observed
that the secretion of urine was either greatly diminished or ceased alto-
gether, while the blood-pressure rose, occasionally to a considerable
extent. After some time the blood-pressure ^;ain fell ; and in some of
the experiments the secretion of urine recommenced at the instant the
fall began. In other instances it did not reeouimence till the hlood-
pressure had sunk bflow the iiormdl. Occasionally the sei'retiim did not
flow with its original rapidity, but in others it was poured forth
copiously, even although the blood-pressure had suni considerably below
the normal.
If Dii/itnlis acted as a diuretic only by nusing the blood-pressure, the
flow of urine should have been greatly increased immediately after the
injection, and should have diminished with the fall of arterial teasioD.
Instead of this the secretion was least when the blood-pressure w^s
highest, and most copious when the tension had fallen below the normal.
The explanation we would offer of these phenomena is, that Bi^italU
probably stimnlat«s the vaso-motor nerves generally, but affects those of
the kidney more powerfully than those of other parts of the body. Thus,
it causes a moderate contraction of the systemic vessels, and raises the
blood-pressure in them, but, at the same time, produces excessive contrac-
tion of the renal vessels, so as to stop the circulation in the kidneys and
arrest the secretion of urine.
As the action of the drug on the systemic vessels, passes ofi they relax,
and the blood-pressure falls ; but the renal arteries probably dilato more
quickly and to a greater extent than the others. The pressure of blood
in the glomeruli may thus be increased above that normally present in
them, although the tension in the arterial system generally may have
fallen below the normal.
Additional evidence in favour of this explanation is afforded by the fact
that the urine collected after the reestablishment of secretion contains
albumen, just as Herrmann found it to do after mechanical arrest of the
circulation through the renal art«ries<
1874.] Dr. A. GSnther m Gigantic Land-Tbrtoi$e». 421
We do not overlook the possibility that the alteration in secretion may
be partly due to the direct action of the drug on the secreting elements
oE Uie kidneys, and we ore still engaged in experiments on this subject.
XI. " Description of the Living and Extinct Races of Gigantic
Land-Tortoiaes. — Parts I. and II. Introduction, and the Tor-
toises of the Galapagos Islands." By Dr. Albert Guntheb,
r.R.S. Received June 4, 1874.
(Abstract.)
The author having had the opportunity of examining a considerable
collection of the remtuns of Tortoises found in the islands of Mauritius
and Bodriguen aB30ciat«d with the bones of the Dodo and SoUtaire, has
arrived at the foil owing conclusions : —
1. These remains clearly indicate the former existence of several
species of gigantic Land-Tortoises, the Rodriguez species differing more
markedly from those of the Mauritius than these latter among them-
selves. All these species appear to have become extinct in modem
times.
2. These extinct Tortoises of the Mascarenes are distinguished by a
fiat cranium, truncated beak, and a broad bridge between the foramina
obturatoria.
3. All the other examples of gigantic Tortoises preserved in our mu-
seums, and said to have been brought from the Mascarenes, and likewise
the single species which is known still to survive, in a wild state, in the
small island of Aldabra, have a convex cranium, truncated beak, and a
narrow bridge between the obturator foramina ; and therefore ue
specifically, if not gonerically, distinct from the extinct ones.
4. On the other hand, there exists the greatest afRnity between those
contemporaries of the Dodo and SoUtaire and the Tortoises still inhabit-
ing the Galapagos archipelago.
These unexpected results induced the author to subject to a detailed
examination all the available material of the gigantic Tortoises from the
Mascarenes and Galapagos which are still living, or were believed to be
living, and are commonly called Tettudo indiea and Teituda elephantopiu,
and to collect all the historical evidence referring to them. Thus, in the
JirH {introductory) part of the paper a selection from the accounts of tra-
vellers is given, by which it is clearly shown that the presence of these
Tortoises at two so distant stations as the Galapagos and Mascarenes
cannot be accounted for by the agency of man, at least not in historical
times, and therefore that these animals must be r^arded as indi-
genous.
The Kcond part consists of a description of the Galapagos Tortoises.
The author shows that the opinion of some of the older travellers, m.
422 Dr. A. Gunther on Gigantic Land-Toriohes. [June 18,
that the different islands of the group are inhabited by different mcea, is
perfectly correct ; and he distingiushes four species, the adulfa oE wtiii-li
are characterized aa follows : —
A. Shell broad, with more or Jess corrugated plat«9. Sl-nlt with the
palatal region concave ; outer pterygoid edge sharp in its entire length
or for the greater part of ita length ; a deep receas in front of the occi-
pital condyle ; anterior wall of the entrance of the tympanic cavity con-
etricted. One of the two species is from James iHland.
1. SheU depressed, with the upper anterior profile subhorizoatal in the
male, and with the striie of the plates not deeply sculptured : sternum
truncated behind, Shdl with the facial portion very short, and with an
immensely developed and raised occipital crest. Teatado flepliantopia
(Harlan).
2. ShfU much higher, with the upper anterior profile declivous in the
male, aud with the stria; deeply scuiptured ; sternum excised behind.
Shdl with the facial portion much longer, and with low occipital crest.
Tatudo nigrita (Dum. & Bibr.).
B. Sfull oblong, smooth. Sf^U with the palatal region shallow ; the
outer pterygoid edge expanded in its whole length ; no deep recess in
front of the occipital condyle ; anterior wall of the tympanic cavity not
3. Shell with some traces of former concentric striie, compressed ante-
riorly into the form of a " Spanish saddle " in the male ; sternum trun-
cated behind. ;SJ:uZI with the tympanic cavity much produced backwards.
Testudo ephippium (0-thr.), from Charles Island. Kvtinet.
4. SJull perfectly smooth, with declivous anterior profile in the male,
and with truncated posterior extremity of the sternum. Slntll resem-
bling that of the young of the larger species, with the tympanic case not
produced backwards. The smallest species, Tatwdo microphyet (Qthr.),
from Hood's Island.
Part III. will contain the account of the still existing Tortoises of the
Mascarenes, and Fart lY. that of the extinct species.
Received June 9, 1874.
PS. The author has just received from Professor Huxley the carapace
and skeleton of anotheradult male, which evidently helongs to a fifth species
of Galapagos Tortoises. With regard to the form of the carapace, it
resembles much that of T. eUphantopw, the dorsal shell being depressed,
broad, with the upper profile nearly horizontal. Strie distinct, broad.
However, the skull differs widely from that of T. elephantopia, and has
all the characteristics of that of T. ephippium, from which it differs in
having a circular tympanic opening. The form of the sternum is quite
peculiar, the gular portion being much constricted aud produced forwards,
whilst the opposite end is expanded into the large anal scutes and deeply
excised. This species may be named Ttstado ftcina.
1874.] On Dredffinga and Deep-tea Soundings, 423
XII. " Od Dredg^iii^ and Deep-sea Soandinga in the South At-
lantic, in a Letter to Admiral Richards^ C.B., F.R.S." By
Prof. Wyvillb Thomson, LL.D., F.R.S., Director of the
Civilian Staff on board H.M.S. ' Clialleuger.' Received
May 25, 1874.
Melbourne, March 17, 1674.
Sear Admiral RicnARna, — 1 have the pleasure of informing you
that, during our voyage from the Cape of Good Hope to Australia, all
the necessary observations in matters bearing upon my department have
been made most auccessfully at nineteen prindpal stations, suitably
distributed over the track, and including Marion Island, the neighbour-
hood of the Crozets, Kerguelen Island, and the Heard group.
After Icaviug the Cape several dredgings were taken a little to the
southn'ard, at depths from 100 to 150 fathoms. Animal life was very
abundant ; and the result was remarkable in this respect, that the general
character of the fauna was very similar to that oE the North Atlantic,
many of the specia even being identical with those on the coasts of Great
Britain and K^orway. The first day's dredging was in 1900 fathoms,
125 miles to the south-westward of Cipe Agulhas ; it was nut very
successful.
Marion Island was visited for a few hours, and a considerable collec-
tion of plants, including nine flowering species, was made by Mr. Mose-
loy. These, along with collections from Kergnelen Island and from
Yong Island, of the Heard group, are sent home with Mr. Moseley's
notes, for Dr. Hooker's information.
A shallon-water dredging near Marion Island gave a large number of
spu'cies, again representing many of the northern types, but with a mix-
ture of southern forma, such as many of the characteristic southern
Bryozoa and the curious genua Serolis among Crustaceane. Off Prince
Kdward's Island, the dredge brought up many large and striking speci-
mens of one or two species of Alcyonarian zoophytes, allied to ifojum
and Tiis.
The trawl was put down in 1375 fathoms on the 29th Decemtwr, and
in IGOO fathoms on the 30th, between Prince Edward's Island and the
Crozets. The number of species taken in these two hauls was very large ;
many of them belonged to especially interesting genera, and many
were new to science. I may mention that there occurred, with others, the
well-known genera EupUctella, Hyalonema, UinhilluUiria, and FUAellum ;
two entirely new genera of stalked Crinoids belonging to the Apio-
criuidtG ; I'ourtaleitia ; several Spatangoids new to science (allied to the
extinct genus .ilnan<Ai/(M); SaUiiia; several remarkable Crustaceans; and
a few fish.
We were unfortunately unable to laud on PoBseBsiou Island on account
VOL. on. 2 K
Prof. W. Thomson on
of the weather ; but we dredged iu 210 f&thoms and ooO fftthoms, about
18 miles to the 8.W. o£ the ishmd, with a satisfactory result. We
reached Kerguelen li^laiid on the 7th of January, and remained there
until the 1st of February. During that time Dr. v. WiUemijes-SuLm
was cbieHy occupied in working out the land-fauna, Mr. Moseley col'
lected the plants, Mr. Buchanan made obsenations on the geology of
those parts of the island which we visited, and Mr. Murray and I rarriod
on the shallow-water dredging in the steam-pinnace. Many observations
were made, and large collections were stored in the difEereut departments.
We detected at Kerguelen Island some peculiarities iu the reproduction
of sevei'al groups of marine invertebrates, and particularly in the Echino-
dermata, which I have briefly described in a separate paper.
Two days before leaving Kerguelen Island, we trawled off the entrance
of Christmas Harbour ; and the trawl-not came up, on one occasion, nearly
filled with large cup-sponges belonging to the genua lUiasella of Carter,
and probably the species dredged by Sir James Clark Boss near the ice-
barrier, RosseUii aiitarelica.
On the 2nd of February we dredged in 150 fathoms, 140 miles south of
Kerguelen, and on the 7th of February off Tong Island, in both cases with
We reached Corinthian Bay, in Tong Island, on the evening of the 6th,
and had made all arrangements for examining it, as far as possible, on
the following day ; but, to our great disappointment, a suddeu change of
weather obliged us to put to sea.. Fortunately Mr. Moseley and Mr.
Buchanan accompanied Captain Nares on shore for an hour or two on
the evening of our arrival, and took the opportunity of collecting
the plants and minerals vithin their reach. A cast of the trawl
taken in lat. CO" 52' 8., long. 80° 20' S., at 1260 fathoms, was not very-
productive, only a few of the ordinary deep-sea forms having been pro
Our most southerly station was on the 14th of February, lat. 65° 42' S.,
long. 79° 49' E. The trawl brought up, from a depth of 1C75 fathoms,
a considerable number of animals, including Sponges, Alcyonariana,
Fchinids, Brj'ozoa, and Crustacea, all much of the usual deep-sea cha-
racter, although some of the species had not been previously observed.
On February 26th, in 1975 fathoms, I'mhtUularics, HolotAuna,aai many
examples of several species of the Anaiuhytida were procured ; and -we
found very much the same group of forms at 1900 fathoms on the 3rd of
March. On the 7th of March, in 1800 fathoms, there were many animal
forms, particularly some remarkable starfishes, of a large size, of the
genus Hymmaster : and on the 13th of March, at a depth of 2600 fathoms,
with a bottom-temperature of 0°-2 C, Hololhurm were abundant, there
were several starfishes and Adinia, and a very elegant little Brochiopod
occurred attached to peculiar concretions of manganese which came up
iu numbers iu the trawl.
1874.] Dredffit^s and Deep-tea Soundingt. 425
In nine successful dredgings, at depths beyond 1000 fathoms, between
the Cape and Australia : —
Sponges were met with on 6 occasions.
Anthozoa Octactiuia 7
Fol^tinia 0
Crinoidea 4
Asteroidea 8
Ophiuridea 0
Eehinidea
Holothuridea 8
Bryozoa C
Tiinicata 5
Sipimculacea 3
Nematodes I
Annelida 8
(JUyaafomum) 2
Balanoglossiu 1
Cirripedia 4
Ostracoda 1
Isopoda 7
Ampbipoda 3
Slchizopoda 5
Decapoda Macrura G
Brocbyura 2
Pycnogonida 2
Lamellibranchiata 5
Brachiopoda 3
Gasteropoda 4
Cephalopoda 3
Teleostei 0
It ia of course impossible to determine the speciee with the books of
reference at our command ; but many of them are new to science, and
some are of great interest from their relation to groups supposed to be
extinct, This is particularly the case with the Echinodermata, which
arc here, as in the deep water in the north, a very prominent group.
During the present cruise special attention has been paid to the nature
of the bottom, and to any facts which might throw light upon the source
of its materials.
This department has been chiefly in the hands of Mr. Murray ; and I
have pleasure in referring to the constant industry and care which he has
devoted to the preparation, examination, and storing of samples. I ex-
tract from Mr. Murray's notes : —
" In the soundings about the Agulhas bank, in 100 to ISO fathoms,
the bottom was of a greenish colour, and contained many crystalline par-
2k2
42(i Prof. W. Thomson on [June 18,
ticIi'H (soiuQ clai-k-colourod (iiiJ noiuo cltar) ol I'oraniiiiifera, spei.-ii>§ of
Orhidina, Ohbu/frina, and Pulvinuiina, n pretty species of Uvigtrina,
Plmiorbalinn, MilioUna, Bulimiiia, and A'ummulina. There were y&ry
fpw Diatoms.
"In the dflep soundings and dredgings before reaching the CroEets, in
1000, ]570, and 1375 fathoms, the bottom waB composed entirely of
O/'biUhia, GlohUjtrina, and Palviniditui, the same species wliich we get on
the aurfaco, but all oE a white colour and dead. Of Fonimiuifera, which
we have not got on the surface, I noticed one Rotalia and one Fohjato-
mtlla, both dead. Wome Coccoliths and Rhabdoliths were also found in
the samples from these soundings. On the whole, these bottoms were, I
think, the purest carbonate of lime we have ever obtained, AVhen the
soundings were placed in a bottle and shaken up with water, the whole
looked like a quantity of sago. The Pulviiiulimr. were smuller than in
the dredginga in the Atlantic. We had no soundings between the Cro-
zets and Kerguelen.
" The specimens of the bottom about Kerguelen were all from depths
from 120 to 20 fathoms, and consisted usually of dark mud, with an
offensive sulphurous smell. Those obtained furthest from land were made
up almost oniirely of matted spooge-spieules. In these soundings one
species of B^laliivi and one other Foraminifer occurred.
" At 150 fathoms, between Kerguelen and Heard Island, the bottom
was composed of basaltic pebbles. The bottom at Heard Island was much
the same as at Kerguelen.
"The sample obtained from a depth of 12C0 fathoms, south of Heard
Island, was quite different from any thing ^e had previously obtained.
It was one mass of Diatoms, of many sjiecies ; and, mixed with these,
a few small Glohirffrina and Eadiolariana, and a very few crystalline par-
"The soundings and dredgings while we were among the ice in 1G75,
1800, 1300, and 1975 fathoms, gave another totally distinct deposit of yel-
lowish clay, with pebbles and small stones, and a considerable admixture of
Diatoms, Badiolarians, and Gtobifferinc. The clay and pebbles were
evidently a sediment from the melting icebegs, and the Diatoms, Badio-
larians, and i'oraminifera were from the siirfato-walers.
" The bottom from 1D5U fathoms, on our way to Australia from the
Antarctic, was again exactly similar to that obtained in the 1200-fathoin3
sounding south of Heard Island. The bottom at 1800 fathoms, a little
further to the north (lat. 50° 1' 8., long. 123° 4' E.), was again pure
' Globiijerina-ocaf:,' COTnposed of Orhuliua', Globujerino', and Piilvinuliiife.
"The bottom at 2150 fathoms (lat. 47° 25' S., long. 130' 32' E.) w-as
similar to the last, with a reddish tinge ; and that at 2GO0 fathoms (Int.
42° 42' 8., long 134" 10' E.) was reddish clay, the same which we got at
like depths in the Atlantic, and contained manganese nodules and much
decomposo<l Foraminifera."
' IS/i.] Dree^inga and Deep-tea Somdings. 427
Mr. Murray hni been induced, by the observatiouB which have been
mode in the Atlantic, to combine the use of the towing-net, at various
depths from the surface to 150 fathoms, with the esamination of the
samples from the aoundings. And this double work has led him to a
conclusion (in which I am now forced entirely to concur, although it is
certainly contrary to my former opinion) that the bulk of the material of
the bottom in deep water is, iu all cases, derived from the surface.
Mr. Murray has demonstrated the presence of Globigerinct, Palvinu-
liiim, and OrbuUna throughout all the upper layers of the sea over the
whole of the area where the bottom consists of " Olohiyenna-ooze " or of
the red clay produced by the decomposition of the shells of Foraminifera ;
and their appearance when living on the surface is so totally difEerent
from that of the shells at the bottom, that it is impossible to doubt that
the latter, even although they frequently contain organic matter, are all
dead. I mean thia to refer only to the genera mentioned above, which
practically form the ooze. Many other Forainlnifera undoubtedly live in
comparatively sm^ numbers, along with animals of higher groups, ou the
bottom.
In the extreme south the conditions were eo severe as greatly tointer-
fere with all work. %Vo had no arrangement for heating the work-rooms ;
and at a temperature which averaged for some days 25° F., the instru-
ments became so cold that it was unpleasant to handle them, and the
vapour of the breath condensed and froze at once upon glass and brass
work. Dredging at the considerable depths which we found near the
Antarctic Circle became a severe and somewhat critical operation, the gear
being stiffened and otherwise affected by the cold, and we could not repeat
it often.
The evening of the 23rd of February was remarkably fine and calm,
and it was arranged to dredge on the following morning. The weather
changed somewhat during the night, and the wind rose. Captain Nares
was, however, moat anxious to cany out our object, and the dredge was
put over at 5 a.m. "We were surrounded by ieebei^, the wind continued
to rise, and a thick snow-storm come on from the south-east. After a
time of some anxiety the dredge was got in all right ; but, to our great
disappointment, it was empty, — probably the drift of the ship and the
motion had prevented its reaching the bottom. In the mean time the
wind had risen to a whole gale (force=10 in the squalls), the thermo-
meter fell to 21°-5F., the snow drove in a dry blinding cloud of ex-
quisite star-like crystals, which burned the skin as if they had been
red-hot, and we were not sorry to be able to retire from the dredging-
bridge.
Careful obsenations on temperature are already in your han<l8, reported
by Captain Nares. The specific gravity of the water has been taken daily
by Mr. Buchanan ; and, during the trip, Mr. Buchanan has determined
the amount of carbonic acid in 24 different samples— 15 from the surface,
428 On Dredffings and Deep-Sea Soundings. [Juiie 1
7 from the bottom, and 2 from interraediato depths. The srirJIe
Binoiint of carbonic acid was found in surface-water on tbe 27th Jaaoai
near Kei^elen ; it araounted to 0'0373 gramme per litre. The large
amount, 0-0829 gramme per litre, vroa found in bottom-water on the 14
February, when close to the Artarctic ice. About the same latitude t
Rmount of carbonic acid in aurfape-wat«r rose to the unusual amount
0-0651 gramme per litre; in all other latitudes it ranged betw©
0'044 and 0-054 gramme per litre. From the greater number
these samples the oxygea and nitrogen were exfci-aoted, and sealed up
The considerations connected with the distribution of tcmperohire a
specific gravity in these aouthem waters are so very complicated, that
prefer postponing any general reiamc of the roaults until there has bo
time for full consideration.
While we were among the ice all possible observations were made i
the structure and composition of icebergs. "We only regretted great
that we had uo opportunity of watching their birth, or of observing t
continuous ice-barrier from which most of them have the appearance
having been detached. The berg- and iloe-iee was examined with t
microscope, and found to contain the usual Diatoms. Careful drawin
of the different forma of icebergs, of the positions which they assume
melting, and of their intimate structure were made by Mr. Wild, a
instantaneous photographs nf se^ornl were taken from the ship.
Upwards of 15,000 observations in meteorology have been record
during the trip to the south. Most of these have already been tabulal
and reduced to curves, and otherwise arranged for reference in considi
ing the questions of climate on which they bear.
Many specimens in natural history have been stored in about seven
packing-cases and casks, containing, besides dried sijocimens, upwards
600 store-bottles and jars of specimens in spirit,
I need only further add that, so far as I am able to judge, the espei
tlon is fulfilling the object for which it was sent out. The naval and t
civilian staff seem actuated by one wish to do the utmost in their powi
and certainty a large amount of material is being accumulated.
The experiences of the last three mouths have of course been somen"!
trying to those of us » ho were not accustomed to a sea-life ; but t
health of the whole party has been pxcellent. There has been so much
do that there has Ijeen little lime for weariness ; and the arrangemei
I'lmtinue to work in a pleasant and satisfactory way.
^Signed) CuAiiLEa WirvxtLE Thomson,
w
1874.] Mr. J. L. Tupper on the Centre qf Motion in the Eye. 429
XIII. " On the Centre of Motion in the Human Eye." By J. L.
Topper. Conuntmicated by S. J. A. Salter, F.B.S. Receired
May 15, 1874.
(AbBtraet.)
The paper of which this is a short abstract premises that its argu-
ment is conditional, that it adopts all the fuudamental optical conditions
&a they are receiyed, that the received centre of motion is not one o£
these, but is supposed to be legitimately derived from them, and that tho
author disputes this and proposes ; —
1st. To show that this conclusion is inconsistent with its premises,
and that a different though indefinite conclusion is thence derivable ;
2nd. By experiment, to develop and reduce that conclusion to a de<
finite form ;
3rd. To verify it by anatomical induction.
The latest investigations (those of Prof. Donders) have placed the
centre of motion nearly two millimetres behind the centre of the globe,
and in the cornea's axis. The process of proof assumed that the centre
of motion is equidistant from the out«r and inner margins of the cornea,
and, moreover, that the eye's visual line (ordinarily at 6° with the
cornea's axis) will, by mere rotation, in turn coincide with three or more
radii of the same circle ; or that, without moving the head, we can suc-
cessively sight the lines on a graduated circular arc, seeing them as so
many points.
The paper first proves, by a geometrical diagram, that if the eye, by
simple rotation, can thus see the radii of a circle, the centre of motion
must be in the visual line, not in the cornea's axis, as hitherto supposed ;
proves next, by pairs of sights set up on the radii of a circle, and actually
Been as so many points, that the centre of motion is, in fact, in the visual
line ; and proves, lastly, by measuring (mechanically) how far the front
of tbe cornea is from the converging point of the radii thus sighted, that
the centre of motion is about ^ of an inch, instead of ^ of an inch, be-
hind the cornea's anterior surface.
Then follows a twofold anatomical corroboration of these conclusions
by examination,
Ist, of the living eye ;
2nd, of tbe dissected eye.
(Ist) If the eye rotated on a point in the antero-posterior diameter (or
cornea's axis), then any two points equidistant from tho cornea's centre
would in turn occupy the some point in apace, as assumed by Prof.
Donders. The first experiment shows that two such corresponding points
will not, OS the eye turns, fall into the same place ; whilst other examina-
tions of the living eye show not only that symmHriejdhj situated points
move asymmdricalhj, but movo asvmmetrically in such a way as would
occur if the centre of motion were externa! Ut the antero-posterior aas,
430 Mr. J. L.Tiipperon /Ac C'«!(reo/Jtfo/ion in (Ae£ye. [June 18,
or somewhere in the visual line behind Ihe nodal point, a position
which ngreea with thftt aeaigned to the centre of motion by the preceding
(2iid) The tUssected organ exhibits an asymmetrical attiwhuieiit of
the recti muacles, so that a vertical plane cutting these attachments
ia further from the external than from the internal margin of the
cornea.
The circumference of this plane would he a drele, and the attachment
of the globe's suspensory ligament, that resists the backward traction of
these muscles, is found also to be a circle parallel to, and one line further
back than, the former circle. The latter may be considered the base of
a cone, whose vertex is the optic foramen, in the surface of which cono
the recti muscles are sitiuite. The base is therefore kept in equipoise
by the symmetrical arrangement of the contracting muscles behind
and the resisting suspensory hgameut in front ; so that the contnic-
tdou of a single rectus, as it draws back the ligament on one side,
increases its fonsard traction on the other side, and moves any two
opposite points of the cone's base equally in opposite direcliona, or
rotates it on its centre, a centre which is thua the anatomical centre of
motion.
But however the recti are situate (and act) symmetrically with the base
of this cone, the base is oblique with respect to the coroea (not at right
angles to its axis), and consequently its centre will be on one side of the
cornea's axis ; and again, since Ihe cone's base is further from the outer
than from the inner margin of the cornea, its centre will Iw ouuide
the ci)mea's a\is. Kow that part of the visual line where the preceding
experiments have placed Ihe centre of motion is outside the cornea's axis,
while the base of the cone, whose centre has thus proved to bo the ana-
tomical centre of motion, is found to pass through the visual line -^ of an
inch behind the coruea, exactly in accordance with the results of the
experiment with sightt'd radii of a circle
Lastly, the obliquity of the cone's base with the base of the conieji
proves to be a consequence of the hitherto unexplamed want of lateral
symmetry in the attachment of Ihe recti muscles, thus explained ns
a moat important means of tidjusting the e\e*s Miual line to the ob-
ject ; while some further pocuharilies in (he insertion of the recti,
demonstrated in Ihe author's disseclions, conspire to attam the earn*
The author's thanks for valuable atsisianec are due to Mr J. ^'alter
F.H.8., to Mr. II. G. llowso, Demonstrator of Aiiatumv to Guv'a Hos-
pitjil, aud lo the Eev. Geo. F. Wright, of OversliHlc, liugby.
L^
1874.] TAt.J.Y.Biuihmm on Sea-water Ice. 431
XIV. " Some Observations on Sea-water Ice." By J. Y. Bdchanaw,
Chemist on Board H.M.S. ' Challenger.' Communicated
by Professor A. W. Williamson, For. Sec. R.S. Received
June 9, 1874.
Many different opinions have been expressed as to the nature of ice
resulting from tbe freezing of sea-water, oil freeing, however, in one
point, that, when nieltod, the water is uoflt to drink. During the
antarctic eriiise o£ H.M.S. ' Challenger ' I took an opportunity of exa-
mining some of the broken pack-ice, into which the ship made an
excursion on the moruing of the 25th of February, and also some ice
which had formed over nigbt in a bucket of sea-water left outside the
laboratory port.
The piece of pack-ice which I examined was, in substance, clear, with
many air-bells, most of them rather irregularly shaped. Two portions
of this ice were allowed to melt at the temperature of the laboratory,
which ranged from 2° C, to 7° C, The melting thus took place very
slovtlv, aod made it possible to examine the wal^r fractionally. My
experiments consisted in determining the chlorine in the water by means
of tenth-normal uitrate-of-BUver solution, and observing the temperature
of the ice when melting.
A lump, which, when melted, wa^ found to measure 625 cub. centims.,
was allowed to melt gradually in a porcelain dish. When about 100
cub. centime, had melted, 50 cub. centims. were taken for the determi-
nation of the chlorine; they required IS'O cub. centims. silver solution,
corresponding to 0'0483 gramme chlorine. When 500 cub. centims.
had melted, 50 cub. centims. were titrated, and required 1-6 cub, centim.
silver solution, corresponding to 0'0067 gramme chlorine. The remainder
(05 cub, centims,) of the ice was then melted and 00 cub. centims. titrated ;
they required 0'3!> cub. centim, silver solution, corresponding to 0"0014
gramme chlorine. Wo have then in the first 50 cub. centams. 0-0483
gramme chlorine, in the next 510 cub, centims, 0'067d gramme, and
in the last do cub. centims. O'OOIS gramme. Hence the whole lump
(025 cub. centims.) coattuued 0'1077 gramme chlorine, or, on an average,
U-1723 gramme chlorine per litre, A qualitative analysis of the water
showed lime, magnesia, and sulphuric acid to be present.
Another piece of the ice was pounded and allowed to melt in a beaker.
When about half was melted, the water was poured off and found to
measure 05 cub. centims. ; 75 cub. centims. were titrated with silver
solution, and required I'O cub. centim. The remainder, when melted,
measured 130 cub. centims., and required 09 cub. centim. silver solution.
Henco the first fraction of 95 cub. centims. contained 0'0085 gramme
chlorine, and the second of 130 cub. centims. 00032 gramme chlorine.
The whole quantity (225 cub. centimB.)of ice therefore contained O'OIl 7
gramme cbloriite, or, on on average, 0-0520 graipme per litre.
432 Messrs. J. G. M'Kendrick and J. Dcwar on [June ISM
From these rPBults it is evident that the ico under exaiainatioa y
very far from being an homogeneous body ; and, indeed, nothiug else
could be expected, when it is bome in mind that the ice in question
owes its existence, not only to the Inmd fule freesving of sea-water, but
abo to the snow which falls on its surface and is congealed into a
oompact mass by the salt-water spray freeKing amongst it.
The ice formed by freezing sea-water in a bucket was found to bare
formed all round the bottom and sides of the bucket, and formiug a
pellicle on the surface, from which and from the sides and bottom the ice
had formed in hexagonal planes, projecting edgewise inio the water.
The water was pourcvd off. the crystals collectod, washed with distilled
water, pressed between filteriog-paper, and one porliou melt«d. It
measured 9 cub. centims., and required 4 cub. ceutiins. silver solution,
corresponding to 0'0142 gramme chlorine, or 1-57S0 gramme per litre.
The other portion was used for determining the melting-point. The
thermometer used was one of Geissler's normal ones, divided into tenths
of a degree Centigrade, whose zero had been verified the day before in
melting snow. Tho melting-point of the ice-crystals was found to be
— 1°'3. Tho temperature of the melting mass was observed to remain
constant for twenty minutes, after whii-li no further observations were
• made.
In the same way the melting-point of the pack-ice was determined.
The fresh ice began to melt at ~1° ; after twenty minutes the ther-
mometer had risen to — 0°-9, and two hours and a half afterwards it
stood at —0°-3, having remained constant for about an hour at — 0°'4.
Another portion of the ice rose more rapidly ; and when three fourths of
the ice was melted, the thermometer stood at 0°.
These determinations of the temperature of melting sea-water ice
show that the salt is not contained in it only in the form of mechanically
enclosed brine, but exists in the solid form, either as a single crystalline
substance or as a mixture of ice- and salt-crystals. Common salt, when
separating from solutions at temperatures below 0", crystallizes in
hexagonal planes ; sea-water ice, therefore, may possibly have some
analogy to the iaomorphous mixtures occurrbg amongst minerals.
XV. "On the Physiological Action of the Chinoline and Pyridine
Bases." By John G. M'Kendrick and James Dewar,
Edinburgh. Communicated by Professor J. Bukdon San-
derson, M.D., F.11.S. Eeceived June 11, 187i.
(Abstract.)
It is well known that quinine, cinchonine, or strychnine yield, when
distilled with caustic potash, two homologous series of bases, named the
pyridine and chinoline ffiries. Bases isomeric with these may »Iso be
1874.] the Action of the ChinoUne and Pyridine Bases. 4S3
obtained by the deBtructive distillation of coal, or from Dippel's oil, got
from bone. Qreville Williams has pointed out that chinoHoe obtuned
from coal-tar differs in some respects from that yielded by cinchonine.
In this research the authors endeavoared to ascertain (1) the physio-
logical actdon of the various members of the series; (2) whether there
was any difference in this respect between the members of the series
obtained from cincbonine and those got from tar ; and (3) whether, and
if so, how, both as regards extent and character, the physiological action
of these bases differed from that of the original alkaloidal bodies.
The bases in both series are difGcult to separate from each other ; hut
this has been done as far as possible by repeated fractional distillation.
The salt employed was the hydrochlorate. This, dissolved in water, was
introduced by a fine syringe under the skin of the animal. The action of
chinoline was tested on frogs, mice, rabbits, guineapigs, cats, dogs, and
man ; but ss the effects were found to be similar in all of these instances,
the majority of the observations were made on rabbits. The experi-
ments with the other substances were mode on rabbits and frogs. The
physiological action of hydrochlorate of chinoline was first eiarained.
Its action was then compared with that of the hydrochlorates of the
chinoline series of bases distilling at higher temperatures, including
such as lepidine, dispoline, tetrahiroltne, &c. In the next place, the
physiological action of the pyridine aeries was studied, beginning with
pyridiuo itself, and passing upwards to bases obtained at still higher
boiling-points, such as plcoline, lutidine, &c. lastly, the investigation
was directed to the action of condensed bases, such as dipyridine, porapi-
coline, &c. ; and the effects of these substances were compared with those
produced by the members of the chinoline series and among themselves.
The following are the general conclusions arrived at : —
1. There is a marked gradation in the extent of physiological action of
the membors of the pyridine series of bases, but it remains of the same
kind. The lethal dose becomes reduced as we rise from the lower to the
higher.
2. Tho higher members of the pyridino series resemble in physiologi-
cal action the lower members of the chinoline series, except (1) that the
former are more liable to cause death by asphyxia, and (2) that the
lethal dose of the pyridines is less than one half that of the chinolines.
3. In proceeding from the lower to the higher members of the chino-
line series, the physiological action changes in character, inasmuch as the
lower members appear to act chiefly on the sensory centres of the
cncepholon and the reflex centres of the cord, destroying the power of
voluntary or reflex movement; while the higher act less on these centres,
and chiefly on tho motor centres, first, as irritants, cansing violent con-
vulsions, and at length produdng complete paralysis. At the same time,
while the reflex activity of the centres in the spinal cord appear to be
inactive, they may be readily roused to action l^ stiychnine.
434 Rev. H. F. C. Logan on the Calcuba qf FacloriaU. [June 18,
4. On comparing the action of aueh coinpouuds as C, RjN (clunoline^
with C, H„ N (panoline &c.), or C, H„ N (collidine) w-ith C. H„ N (conia'
from hemlock), or C„ H,, N, (dipyridine) with C„ U,, N, (nicotine, from
tobacco), it is to be obsetred that the physiological actiritj o£ the sub-
stance is, apart from chemical etmcture, greatest in those bases con-
taining the larger amount of hydrogen.
f). Those artificial bases which approximate the percentage composition
of natural bases are much weaker physiologically, bo far as can be esti-
mated by amount of dose, than the natural bases ; but the kittd of action
is the same in both coses.
6. When the bases of the pyridine series are doubled by condensation,
producing <lipyridine, parapicoline, &c., they not only become more
active physiologically, but the action differs in kind from that of tte
simple bases, and resembles the action of untuml bases or alkaloids
hating a similar chemical constitution.
7. Ail the substances examined in this research are remarkable for
not possessing any specific paralytic action ou the heart likely to cau^e
syncope ; but they destroy life either by ojthaustive convulsions, or by
p^ual paralysis of the centres of respiration, thus causing asphyxia.
8. There is no appreciable immediate ai-tion on the sympathetic system
of nenes. There is probably a secondary action, because after lar^
doses the vasomotor centre, in common with other centres, becomes
involved.
9. There Is no difference, so far as could be discovered, between the
physiological action of bases obtained from ciuchoniue and those derived
from tar.
XVI. "On the Calculus of Factorinls." By the Rev. H. F. C.
LoGANj LL.D. Comraunicatcd by Professor Cavley, P.R.S.
Received November 10, 1873.
(Abstract.)
Our present knowledge of what is called pure analysis has for its con-
crete basis the general theory of powers.
This science the author might, after Wroiiski, sanctioned by Lagrange,
have called algorithmic, but he prefers giving it the designation Caleutu*
of Powers.
The simple functions whose properties and relations it is the object
of this latter calculus to determine are, first, the three direct functiona
or algorithms, r", «', sin x ; secondly, their three inverse functions or
algorithms, ^ (or v ;), log„ r, sin"':.
The author ]>ropose8 to establish a new brjiuch of analysis or algo-
rithinie, which is based upon the general theory of factorials, aud in
which s"^^^ replaces z".
1874.] On the Meteorological Use of a Plmimeter. 435
The simple functions or algorithms whose properties and relatione it
ia ttie province of this new calculus to determine are a"''=^, (1+K)I,
{I— A)*, (1+A)~*, (1— i)~*. Bin = sin ;, and their inverse functioiu,
s" ^or a/ '/. 1*^ =1 ft logarithm taken to the Imiho (l+7i)*>or
(1— A)~iand sLn-'a sin-' s.
The calcalns so founded the author propoaes to call the Calculiiq of
Factorials.
The branches of the subioct treat«d of in the present memoir will bo
understood from the following list of the contents of the various sections
into which it is divided : —
Ch, 1, § 1. Definition and properties of s"/''^, or more generally
(fl +;)"/ Til, when M ig a whole positive number.
§ 3. Factorials with a negative whole index.
§ 3. Factorials of which the index ia a positive fraction.
§ 4. Factorials of which the index is a negative fraction.
§ 5. Factorial radicals.
Ch. II. § 1, Application of the theory of finite differences to fac-
§ 2. Differenciation * of factorial exponentials and factorial lo-
garithms.
§ 3. Development of the various simple functions into factorial scries.
XVII. "On the Employment of 8 Planimcter to obtain Mean
Values from the traces of contiunoualy Self-recording Meteoro-
logical Instnimentfi." By Kobert H. Scott, M.A., F.R.S.
Received May 23, 1874.
It is hardly necessary to remind the Fellows that the self-recording
instruments employed by the Meteorological Committee at their Obser-
vatories for the continuous registration of pressure aud temperature
furnish their results in the form of photographic traces. The usual
method of dealbg with these barograms and thermograms, as they are
respectively called, ia to measure them at certain intervals by appropriate
scales, and to treat the numerical values so obtained by arithmetical
processes so as to arrive at moan results.
This method is naturally very laborious, and its accuracj' is to some
■ The author usM thts word t« denote that trliirh in the colciilusof Unite difltrcnen
takes the plaoa of diffamtistioD in the difTsrenlUI ooloulu*.
Mr. R. H. Scott 6» Ifie [June 1
extent affected by certain peculiarities found to be very commonly pr
Bent in euch photogruphic curves, and of whiob no satisfactory explan
Hon has as yet been discovered. The most important of these is what
t-enned by us " bagging,'' tho result of which ia that the base or fiduci
line of the ciurve is no longer a struight line, but exhibits a certain d
gree of curvature, ao that the difficulty of determining the hourly i
other values by means of au engraved scale, bearing parallel etraigl
lines, is very considerable.
At the suggestion of Mr. Francis Gallon, tho Meteorological Con
mittee gave instructions that measurements should be made of tho cutti
by means of the ijistmmeut called Amsler's Plaaimeter, of which a ft
description, by Mr. V. J. Bramwell, F.B.S., ia printed in the 'Heport •
the British Association ' for 1872. The object of this invention is d
fined, in the paper quoted, to be " that the area of any figure, howeri
irregular, can be recorded iu deflnit* standard units of measurement I
the mere passage of a tracer along the perimeter of that figure."
It ia perfectly ob\*ioua that the measurement of the area of the curv
if it can be executed with sufficient accuracy, must give a far more sati
factory mode of ascertaining the value of the meau ordinate of the cut
than the calculation of the average of any number of measured individn
ordinafcB, while the economy of time ensured by the use of the plaoimet
forms a moat important recommendation for its use.
Tho mode of employing the instrument is as follows ; — The enti
perimetar of the ciure, down to the base-liue, ia measured,. and the vali
noted. Then wing the same base-lint, a rectangle of known height,
units of the scale of the curve, is next measua-d in the same way, ni
the vahie noted again.
The ratio of these two values is the mean value of the ordinate of tl
cun-e, or the meau pressure or temperature for the interval embraced 1
the curve.
It may bo remarked that I have learnt within the last few days th
the present occasion is not the first on which a planimeter has been us,
for the deduction of meteorological means. Mens, van Rysselbergli
Professor at tho School of Navigation, Ostend, has employed it in co
nesion with his new electrical Meteorograph.
The subjoined Table shows for a period of eight months the mc^ns
temperature for Kew Observatory obtained by the planimeter, as well
those yielded by the old method, both for daily and for fivLMiay mean
It will be seen that the difference in 242 determinations of daily meai
oidy amounted to 0''-5 on six occasions, and to C>°-0 in one instance ; nLi
out of 49 cases of five-day means tho greatest difference was only 0°-
and this was only ouce attoiijed.
At the end of the Table the column headed " "Wr. Eep. Plates " gl\'i
the values obtained by measurement of tho pJatea published in (1
' Quarterly "Weather Report ' for the period embraced by the measun
1874.] Meteorological Vte of a Plammeter. 4fi7
ments to which I have just alluded. It will be seeit from it that tha
five-da7 mean^ bo obtained hardly difEer from those which are yielded by
the direct meaBurement; of t^e photographic curve by means of the plani-
meter.
The plates in question are obtained by the use of Mr. Franda Galton't
Pantograph, which transfers the records at a reduced time-scale to zinc
plates, which plates are subsequently further reduced and transferred to
copper by Wagner's Fantagraph, as explained in the Beport of the Com-
mittee for 1870.
1 therefore hope that the Society will allow me to remark that sach^a
test 03 this afEords a satisfactory proof of the accuracy of the reproduc-
tions of our automatic records which are executed in the Meteorological
Office,
The result of these preliminary experiments is that the planimeter
means are practically identical with those obtained by treatment of the
values of the hourly ordinates.
It is found that the mean from the photographic record at temperature
for one day can be obtained in about the same time as is required for the
calculation of the hourly values ; while in the case of pressure the saving
of time would be considerable. In both cases the hourly values are
supposed to have been preriously measured. If, however, the five-day
mean from one of the plates <rf the ' Quarterly Weather Beport ' be
admissible, the economy of time would be very great indeed.
It does not appear that the liability to error in following the course of
the cur^'c with the tracer of the planimeter is greater than that of mea-
suring the ordinates of the curve by a glass scale ; while we escape one
serious cause of uncei^tainty in the latter operation, the difficulty of
assigning the exact ordinate to the hour at a period of rapid change of
temperature, Ac. — a case of frequent occurrence ; and we almost entirely
dispense with arithmetical calculations.
It is very unfortunate that the use of the planimeter will not enable
us to dispense with the necesBity of biking hourly readings, inasmuch as
it affords us no means of averaging any but consecutive values, and so
renders us no assistance in any determination of the march of meteoro-
logical phenomena.
A further series of planimeter measurements, for pressure and dry-
aud wet-bulb temperature, for all the observatories for three months ia
now in progress ; and if, as we hope, the results will prove as satisfactory
as those which I have the honour to submit to the Society on the pre-
sent occasion, it would appear that there is no further reason why plani-
met«r means should not be published in future by the Office.
Mr. R. H. Scott on the
Dute.
Finit Diy.
Sec<.ndD.j.
Third Dv-
SroaiaorFivcDiijr*.
'i!Ss^
PUni-
Diff,^
Tibuls-
liot...
Plmi-
mrCcr.
Difcr-
"^^
S
DIEfl
1872.
April ... 1- 6.
6M
50-4
+ 1
47-1
47-6
+■5
41-3
411
+■4
O-IO.
43-2
43-5
+"3
47-3
47-5
+ ■»
523
fi2S
+•«
IMS.
53-3
B3-2
50-1
56-4
+■3
511
51-4
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1(1-20.
497
W'O
+ ■3
45-7
40-0
+■3
42-7
430
+■3
2l-3i.
43-5
435
47-4
47-7
+ ■3
40'4
49-2
28-30.
B3-3
530
+ "3
57-5
57-0
+ ■■
51-6
&2-0
+■4
Mbt ... 1- S-
53-2
529
— '3
50-2
503
+■1
54-8
55-2
+■4
C-10.
47tf
483
+■4
604
50-8
+■+
47-3
47-8
+-S
U-li.
410
410
45'2
45-3
+-I
47-0
477
+•1
]l(.-3).
530
53-C
48-9
492
■f 3
42^)
42-3
+-J
21-25.
50-1
50'2
+■1
491
40-4
+ 'i
50O
501
+ 1
20-30.
M-1
600
61-3
60-8
— S
61-1
61-3
+ ■*
31-4.
530
534
+ "4
fi3-4
532
.'i3-4
53-C
+ ■»
Juno ... 5-0.
5(!'2
60-3
+ 1
545
651
+■6
50-8
50-8
lo-U,
&4-4
54-7
■f' 3
54-0
64-5
567
56-S
+•1
15-11).
047
640
+■»
08-7
08-7
71-4
71-1
20-at.
04-3
M8
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61-9
+ -»
59-a
59^1
+ ■3
a-i-sj.
01-9
(Ki3
+ "4
57-3
574
+ 1
579
57-0
, 30-4.
60-7
flO-8
+■1
61-5
61-7
+-1
624
027
+ J
July ... 5- 0.
69-5
69-8
+■3
67-7
C8-0
+■3
70fl
70-0
mil.
024
62-6
+ ■1
G7-0
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ft^-2
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15- W.
58-3
58-4
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+ 1
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r.7-2
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72-4
72-6
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09-8
09-9
+ 1
25-L>).
761
75-9
73-2
73-2
68-4
OS'5
+■'
30-3.
020
022
+ 1
57-0
57-7
+ ■'
GO'8
00'8
August 4- S.
M-1
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+ '
n9-2
501
612
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B-13.
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60-2
004
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+ ■*
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675
677
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61-4 I ni-3
04-8
64-8
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fil-3
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a)- 3.
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001
+ ■1
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+ -1
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5»17
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030
08-11
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8-12.
tIO-4
60-3
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13-17.
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63-7
03-4
037
+■3
18-22.
673
57-5
+ ■3
52-5
:.2-7
+ i
407
400
+ ■»
23-27.
472
47-5
+ ■3
47-8
47-7
Ot. ... 28- 2.
53-3
030
+ ■3
51 '4
51-3
I»73.
Jnn. .„ 31- 4.
avo
ar5
+■5
30-9
313
+■4
29-8
30-1
+ ■3
Fvb. ... r.- !). ; 33-2
33-4
+■»
330
331
+ ■1
37-0
37-2
+■>
111-11. a')-8
359
+■■
340
339
38-2
38-4
+ x
l.Vli). 1 W'S
40-9
+■1
38-9
39'2
+ ■3
.■)5-2
av5 1 -j-3
L1I-21. 32-0
32-2
+ 1
309
31-2
+■3
372
37-3 ' +-I
:i>- I. 375
374
40-3
4ti-j
+ *
40-3
40-0 1 +-3
March... 2- li. 1 42-7
42-9
+ z
429
42 8
49-0
liO-O \ +-1
T-ll. U-C,
44-8
+ ■»
42-1
422
+ ■1
44-9
45'!) -f-i
]-2-hi ! ;fii-3
S!)-.-)
+ 1
a->-5
av8
+ ■3
347
348 --I
17-21. 1 41-3
41-5
+*»
40-5
4U'0
+ ■1
38il
39H) +-I
:!2-2ii. 1 3.0-0
39-7
4-1
43-0
433
+■3
4,-.-4
457 -I--J
27-31. 44-4
44-5
+■'
45-2
45-5
+ ■3
4rl
47-3 +-I
+■!»
ItanC
e^KBi
+ ■'4
Uanr
iflVp™* +t4
1874.]
Meteorological Uie of a Planimeler.
Fourth Day.
PiEUiD»y.
Uemt ot the Fi»e Daja.
T^i-^
PU»i-
Diir™-
TilmU-
Pkni-
Dilttr-
TibnU-
Photo.
Pi^"^
PhoJ
oSi'..
+TUm-
+ Wr.
ti^p-FU
412
41-4
+■.
44-3
44-5
+■»
44-8
46-1
44-9
+■3
+ ■»
48'2
48-6
49-5
49-7
+ ■1
48'1
48-4
48-0
+■3
+■4
50' 1
50-2
53-5
53-6
-+■■1
52-8
52 7
62-9
— 1
41-1
41-4
+ 3
40-6
40-7
+'"
43-9
44-3
440
+ 3
+■1
487
487
51-4
010
+■»
48-0
48-1
47-7
+■'
+ 4
51 G
514
52-7
53-0
+ ■3
53-3
635
530
■f»
53'2
52-3
+■■
51-1
514
+■3
53-5
536
834
+■>
+ ■»
47-8
48-0
+■»
47-0
474
+ 4
4S-1
46'5
47-9
+ 4
+ ■6
490
50-1
+■»
506
504
46'9
469
47-0
44-4
44-G
+■»
47-6
475
473
47-4
473
+ ■1
+ ■1
f>l-7
51-8
53-2
63-1
50-8
60-9
60-8
+ '
+■'
61)'l
50-2
+■" •
58-0
585
4--5
69-1
604)
69-1
640
543
+ ■3
53-2
633
+■1
534
53-5
537
+■'
63-3
r,s-3
641
54-4
+■3
53'8
54-0
639
+■1
fil'8
82-0
+ 1
623
634
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58-0
58-1
67'8
+ ■1
+■3
70-7
70-1}
67-8
681
+'3
087
087
68-fl
S07
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666
+■'
63-6
627
02-5
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61-6
61 9
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58-7
58'«
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59-5
597
59-5
+ ■1
625
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+ 1
86-9
658
02C
027
62-6
+ 't
C3fl
C2-2
+■»
61-0
61 '2
+ ■»
06-0
86-3
66-3
+ •3
50-4
60-5
+■■
5»-l
69-1
02-6
627
62-7
+■>
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fll-2
+ ■»
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64'3
010
61-0
61-2
B8-3
684
+ ■»
70-9
711
+ i
697
69-8
69'8
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fMl-6
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+ 3
68-1
664
+ ■3
70-1
70'2
70-2
+ ■1
57-9
58-0
+■'
58'5
58-5
59-3
594
69-3
+ ■1
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SI -3
61-0
•f'3
aa-8
59-6
59fl
80-0
600
+ ■"
60-0
59-1
+■'
577
677
59-7
60-8
697
+ ■1
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fiG-1
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654
05'5
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62'6
624
+ ■1
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65-3
57-2 1 ft7-4
+ 1
68-3
58-1
60-6
00-6
60-6
+ '
56-9
56-5
-4
B6-2
659
80-7
59-6
69-8
63'3
(B-4
+ ■>
63-0
62-8
657
65-7
60-6
■f 1
6(J'4
664
65-0
654
+ 4
62-6
627
628
S7-1
57-3
+■»
013
60-9
62-2
63'1
633
43'D
439
44-0
65-8
44-0
560
+■»
48-8
49-0
49-3
+•1
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54'8
5fri
+■3
68' 1
68-2
+■'
33-2
33-3
+ ■1
36-G
357
4--1
329
332
33-3
+ ■3
o
35-5
36-n
+'S
347
34-9
+ ■»
347
34fl
349
+ ■»
37-7
37-y
+ ■»
40-2
40'3
+■'
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373
37-0
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338
+■1
336
33-9
+ "3
364
367
36-3
+ ■1
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35-fi
35-9
+■]
28-9
29'3
+ ■4
32-0
33-2
33-8
+ '3
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34-7
348
+*'
39-8
397
39-7
39-8
39-8
+ 1
4S-3
45-6
+ '3
4fr6
40-8
+ -a
44-3
444
44-3
+ ■1
3B-8
40-1
+ ■3
40-3
40-6
+ ■3
42-3
426
42'2
+ ■1
+■3
386
386
38-0
38-9
374
375
374
+■>
+■"
30'9
40-2
+ '3
369
36-9
39-5
397
39-3
+ ■»
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45-3
46 ■«
+■3
440
46-3
+'4
43-0
438
437
+■»
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505
5<W
f
49-0
49-2
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473
474
47-3
+ ■1
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)fMPl>iSa>iiM
+ 1*
II«E
•»kr«M
+■"
Hon
Diftm
+ "
+ 09
440 Magnetic Ob^ervalinns at Zi-Ka-Wei. [June 1*
XVIII. " Magnetic Observations at Zi-Ka-Wei." By M. Dechev
RENa, Director of the Obseiratoiy. Communicated by th
RcT. S. J. Peerv, F.R.S. Received Jane 15, 1874.
Mi deab .Sib, — I enclose a report of aome magnetic observatioDs mad'
at the New Observatory of Zi-Ka-Wei with instrumenta which I sen
from England some time sinc^. A complete set of self-recording mag
netograpbs have just been completed for the wime observatory by Ml
Adie, and will be forwarded to their destination this week. The Direeto
of the Observatory of Zi-Ka-Wei, as well as his first assistant, have botl
received full instructions in the use of these instruments, so we may rea
eonably hope that the science of terrestrial inftgnetism will be mucl
advanced by the foundation of this new establishment.
Tours sincerely,
S. J. Pkbrt.
O. a. Stokfi, Esq., See.R.S.
Premiers resultats roneernaiit la Variation diume de la DAi'linaison
k Zi-Ka-Wei (Chine).
Observations faites le 23-24 et le 29 Mars, 1874, le 6 et le
12 Avril, 1874.
DktM.
Point
d,d.V.rt.
M
1.^.
»•
xi^u..
Voi
U-^U
A«,p.Ut.
h,urr
D*din.
h..„
DMin.
btor.
-"■
hence
D&liB.
)SMr.ia
""J?,
i li M
",;"■
!si in
-;'■
teiwiB
fi.M
l^i-i-n
fsi^i-a.
H^ -
«
,.,..,.
,.
,.„.,.
'
IHll-TS
'
1 so *e■^9
1 £3 33-3
< «-m s
llril <
s
1 fil M'S
9
I 49 19-3
3
IHSOfl
fi-«
]M3£«
iMM-ia
B-3 9
6.«
162 27,
s..n
"■•■'
'
5.«
idosi-s
IBIWW
S.40-3 fi
[The above Table is acrompanied by a figure with the resulta pro
jeeted, and is foUowed by a magnetic bulletin for March 1874, froi
which the following mean results are extracted : —
Declination 1° 53' 59"-8 W.
Vertical intensity 7'22996
Indination 4fi'^ 13' 13"-7
Horizontal intensity 6'92833
Total intensity ]0-0ia7
G. a. S.J
1874.]
Mr. W. Galloway on Sqfetj/-Lamp».
441
XIX. "Experimenta with Safety-Lamps." By William Galloway,
Inspector of Mines. Communicated by R. H. Scott, F.R.S.
Received May 4, IS74.
MtBT the occurrence of a great colliery-explosion It b asnally rery
difGcult, and BometimeB impossible, to arrive at a satisfactory conclusion
as to what wRre the causes which probably led to the catastrophe, and
when safety-lamps have been exclusively used by the workmen its origin
seems to be shrouded in mystery. The explosions which happened at
Bisca, Morfo, Cethin, High Brooks, and Pelton Collieries between the
Ist of March, 1860, and the Slat of October, 1866, appeared to be alto-
gether inexplicable ; and, in the last t\i-o cases, when all the safety-lampa
were found lacked after the accident, no attempts were made to explain
the phenomena.
On the 12th of December, 1866, however, the great explosion took
place at the Oaks- Colliery, and fortunately several of the men who
survived could give an account of some of the circumstances which
immediately preceded it. A atone drift had been cut from near the
bottom of the downcast-shafts to within a few feet of one of the intake-
airways, and shori^Iy before the accident a shot-hole was drilled at its
inner end, and chared with a considerable quantity* of gunpowder; the
men who were about the pit-bottom were warned into a sheltered place ;
the shot was fired, and in a few seconds afterwards the shock of the
explosion was felt. It was ascertained subsequently that a part of the
rock at the bottom of the shot-hole had been blown into the intake-airway,
leaving the tamping intact, so that the concussion of the air would be
almost as great as if the tamping alone had been blown out.
A coincidence so remarkable as this attracted considerable attention,
and after every great explosion which has happened since the Oaks' a
search has evidently been made for some evidence of recent shot^firing.
The followiog Table will give on idea of the magnitude of the important
explosions which have happened within recent years, and of some of the
circumstances under which they occurred.
Synopsis of great explosions since 1860.
Diileor
Etplosion.
Name of
CoUieij.
Nurobrt
of men
killed.
Bemwki
ISflO.
76
142
47
26
dent ventilation.
TStked lighta snd nfety-lnmpe. Ou
from the goavoi oame apon the naked
ligbte.
1862.
Mr, W. Galloway on Safity-Ltmja.
[Jane]
Date of
Ntmeot
Hutnb«r
of men
killed.
CoUiery.
Bemar
1663.
October 17
1865.
30
Safetr-Iampe ; all wer« found in goo
June 16
Bedireltr
26
D«Mnibar20..
Cothin
34
1866.
OD. Cause unknown.
jBniuT7 23 .,
Eigb Brook)
30
Looked wfety-Urape; aU were foun.
looked. Cause unknown.
June 14
Dukinfleld
38
Naked lighta and aafety-Iampe. Defl
Octob«r21
Felton
24
cient Tenlilation.
Locked mfety-Umpe ; all wore fount
lockediiOiot-Bruig corned on. Cauai
December 12..
Oak.
334
Safety-lamps. A heSTily diarged sho
was inA in pure air ■ few Moondi
IWko'tfHiU..
01
Safe^-lanipa ; Bhot-Oring carried on
1867.
Augu»t20
OanwoodPark..
14
8afety-larop«. A .hot had Uown out
the tamping.
Femdale
178
Safety-lamp* ; .hot-firing carried on
Two dirtinct eiplodona took pLu<
eating only by two paamgea. and
1868.
November 25..
Hindlej Greet. ..
C2
Safety-lamps. A shot bad blown out
tlie lamping.
Haydock
26
Safety.lampB. A shot had blown out
lesQ.
the tamping.
April 1
ITighBrooka
37
Bafely-larnpe. A Aot bad blown out
the tamping.
June 10
Ferndolo
63
59
Caiue unknown.
Julj21
Ilnjdock
Sftfelylanips? An empty shot-hole was
found from which it wm supposed
the tamping had been blown; two
or more explosion, took place siroul-
tanpously in distant partsof the mine.
NoremberlS,,
Low Hall
27
SafetT-kmns. A shot had blown out
the tamping; there appew 1« haT<
1 been two Hmultaneom and *ery Tio-
1870.
lenteiploeionB.
Febriurj4 ..
0 1 Safety-lamps? A shot bud Mown out
1 the lamping.
Febriu»Tl4..
Morfa
30 1 Giu from a hirred-off eoaf iiinit«d at ■
10 1 Lamm? Cause unknown.
1» i Naked lialilH.
Ju1t7
SilTcrdal? .
July 23
Cliai-leaPit
Au«™tl9
BiynnHaU
20 Safety-la.npe? A abot had blown ont
1871.
the tamping.
Jsnuarj 10 ...
26
Safety-lamps. AshotwanAred with an
plosion. ?
F.b™»i7 2 ...
38
Locked safclT-lampe ; shot-Bring carried
on. A blower is euppoacd to hare
made the return air so eiplosiro that
it ignited at the tentilating-fumsce.
M»rch2
Victoria Pit,
19 Qao in a xt^ill worked with" a aifety
1 lamp : it is asuumed tbat a naked
light was rarried into it.
1874.]
Mr. W. Galloway on Sqfisly-Lampi.
Bite of
M>me of
Colliery.
Number
of men
kiUed.
Bemarki.
1871.
October 25
1872.
February 11 .,
March &
October 7
70
26
n
27
Safctj-l&mps. An empty ghot-holedie-
coTercd after the pits were reopened.
Csme unkuoim.
S<Jetj.l»nips. Aihotwaeflredinpiire
■ir: one eiploeion of flredunp wu
aimultaneouswith the Bhot; another
followed after a short intarral ?
Safetj-Umpa. A xhot wiu fired.
Sofely-lainpl f A abot had blown out
the tamping.
CauM unknown.
LoTer'eUne
Uorlef Mnin
It will be seen from the data given ^xive that shot-liriag was carried
oa in 17 o£ the 22 coliieries at which important eiplosions took place
aft«r the 12th of December, 1866; safety-lamps were certainly used in
12, and probably also in the 5 which are marked doubtful ; in 8 cases it
was ascertained that a shot had blown out the tamping at or about the
time of the explosion ; in 2 an empty shot^hole was found, from which the
tamping is supposed to have been blown ; and in 3 r shot had been fired
bringing down the coal or rock; finally, at Bisca, Temdale (1867), Hay-
dock (1869), Low Hall, Benishaw Park, and Seaham, two or more explo-
sions appear to have taken place simultaneously in different partrs of the
mine unconnected by a train of explosive gas. The Seaham explosion is
a remarkable one : a heavily charged shot was fired in pure air in one of
the intake-aircourses, and, according to the statement of three men who
survived, the explosion of firedamp followed the shot immediately ; one
of the men further asserted that, in several minutes more, he heard the
distinct report of another explosion.
Two methods of accounting for the simultaneousness of the explosion
of firedamp with the firing of the shot have been snggested in the
Keports of the Inspectors of Mines : one of them supposes that the fire-
damp is ignit«d directly by the shot ; the other, that the concussion of
the air caused by the explosion of gunpowder dislodges gas from cavities
in the roof and from goaves, and that this gas, passing along in the air-
currents, is ignit«d at the lamps of the workmen. In some instances,
when it has been known to be highly improbable that uiy gas existed
nearer to the shot-hole than 10, 20, or even 40 feet, the advocates of the
former hypothesis have taken it for granted that the gases issuing from
the shot-hole were projected through the air as far as the accumulation of
firedamp, retaining a sufficiently Idgh temperature to ignite it on their
arrival. On the other hand, the advocates of the latter hypothesis have
not attempted to show how the gas, which they assumed could be ^s-
lodged in quantity by a sound-wave and its refiections, could be ignited
444 Mr. W. Galloway on Safety-Lamps. [June ISn
in those caaes in which safety-laraps only were used. It is no dou
highly probable, however, that when once an exptoaion of firedamp h
been initiated in one way or another, and large bodies of air ore driveat>'|
through the passages of a mine with great velixrity, explosive accumula-
tions will be dislodged from cavities and goavea, and pressed through t^
Bafety-lamps with the velocity requisite U> pass the flame.
In the beginning of ihe year 1872, when I was giving attention to thia
Buhject, it appeared to me to be probable that the sound-wave originftted
by a b!own-out shot, in passing through a safety-lamp burning in an
explosive mixture, viould carry the flame through the roesiiiia of the wire
gauze, in virtue of the vibration of the molecules of the explosive gas.
It had long been known*, indeed, that if an explosive current w
to impinge upon a lighted aafety-lamp in ft direction perpendicular to its J
axis, and with a velocity of 8 to 14 feet per sei-ond, the flame would p
through the meahcs after a abort tiuie, and ignit« the explosive mixtui
on the outside ; but it does not seem to have been suspected that t
same result might be produced by the passage of an iulense eound-v
through a safetv-lnmp burning quietly in an explosive mixture.
explosion at Cothin Colliery in 1865 is a good example of one that n
have be<'n caused iu this way, by the firing of a shot. Several days aft*a^ 1
the explosion the safety-lamp of the overman was found, securely locked
and uninjured, lying at the distance of a few yards, within an abandoned
stall which was known to ha\'e contained firedamp : shot^firing was
carried on in this mine, and it is not improbable that a sound-wave from
an overcharged or blown-out shot had passed through this lamp and
ignited the explosive mixture shortly after the overman bad ent«red it :
moreover the Inspector of Mines says t he has no hesitation in stating
that, in his opinion, the gas in this stall had been ignited, and was there-
tore the o'rigin of the explosion ; but he is unable to state by what means
it was fired.
It is certain that, in every fiery mine, safety-lamps are placed in an
explosive mixture from time to time, either by accident (as when men
retire hurriedly, perhaps into disused places, after the fuse of a shot has
been ignited) or by design to test Ihe quality of the air, as the overman
at Cethin Colliery may have been doing ; and it is equally certain that
shots are fired, occasionally, «hieh blow out the tamping and cause a
violent concusaion of the air. if, therefore, the explanation which is
brought forward in this paper to account for the relation between explo-
sions and shot-firing be the true one, then the question as to how often
explosions of this kind are likely to occur would resolve itself into one of
probability as to how often an ordinary Davy or Clanny lamp, burning in
an explosive mixture, would be traversed by a sound-wave of a certain
amphtude of vibration.
* TransactionB of Korth of England Instiliitp or Mining Engincem, voU. i. &. x*ij,
t Kuporis of \Yk Impectore of Mince, 1W5, r- ' If^-
1874.] MT.yf,0&aovB.y on Sqfetp-Lampt. 415
Od the 16th of Januuy, 1872, 1 made the first experimmt in oonnezion
with this subject in the Fhysicftl Laboratory of TJniTernty College, London :
Profeesor G. C. Foster waa present and co-operated with me. A sheet
of wire gauee, 1 foot square, woa inclined at an angle of 70°, and a slow
current of gas and air from a Bunsen burner was directed against its
under surface. Fart of the explosive mixture thus formed passed tJirough
the meshes, and, when ignited, produced a fiat fiame on the upper surface
3 in. long by 1 in. wide, and symmotricaDy situated in regard to the
sides of the sheet. A glass tube, 3 ft. 4 in. long by 3 j in. diamet«r, was
placed with one end at a distance of 1;^ in. irom the upper sur£ace,
of the Hheet of wire gauze; its ans was horizontal, passed through
the middle point of the fiat flame, and was at right angles to the
line of intersection of a horizontal plane with the sheet. At the end of
the tube furthest from the wire gauze, a vessel, 3^ in. diameter, containing
a solution of soap in water was placed i the point at which the axis of
the tube cut the perpendicular from the centre of the liquid was 2^ in,
from the end of the tube, and at the same distance above the surface of
the liquid. An explosive mixture of coal-gas and oxygen was forced
into the solution of soap until bubbles contaiuing about 2 cub. inches
had formed on the surface. A light was then applied to the gas
at the upper surface of the wire gauze, and immediately afterwards
to the bubbles ; and after the explosion it was found that the flame had
vanished from the upper surface, and that the gas issuing from the
Bunsen burner was on fire.
In December 1872, 1 made a number of experiments similar to the
foregoing in the Laboratory of the Boyal College of Chemistry, when I
was much indebted to Dr. Frankland for his valuable suggestions. The
glass tube of the first experiment was replaced by two tin-plate tubes,
each 2 in. diameter (one 10 ft. 11 in., the other 9 ft. 7 in. loiig) ; they
were joined to form a continuous tube 20 ft. 6 in. long. The vessel
containing the solution of soap was small enough to be placed just inside
of one end of the tube, and the sheet of wire gauze was at a distance of
1 in. from the other end. The same explosive mixtures were again
employed, and the same result was obtained as before. A diaphragm,
consisting of four sheets of brown paper of ordinary thickness, was now
inserted at the junction of the two tubes ; the centre of the diaphragm
was bulged to a distance of about half an inch towards the origin of dis-
turbance. Aft«r the passage of the sound-wave, it was found that the
flame bad shifted to the opposite side of the wire gauze, and the dia-
phragm was bulged to about the same extent, but in the opposite direc-
tion. A quantity of loose cotton-wool, aufHcient to fill the end of the
tube completely for a length of three inches, was then pushed into
the end of the one furthest from the wire gauze, at its junction with
the other. After the sound-wave had passed, the flame was again
found to have removed to the opposite side of the wire gauze, and the
.Irau
\illi a iietw()rk of ^
OV.T tlu' f;l^h'uill!
I lubnl.
ill. Ifiu
lill lllL'
Till' piirl of tlie n])])!iratus whifh is surmoi
the foilawing cODBtructioa : — A round shi
meter, rests on four Bhort lega ; above this,
chnmher./. fanned of two concentric tubu
ita eitcrior Jiameter is 2| in., its interior
top ring there are twenty-four email equid
drele of 2 in, diameter. The Bcrew which i
wire gauze u carried upon projections inwi
of the chamber /. The wire gause of an
betn-een two rings in the nsnal manner, inch
gas-jot oocujiies the position of the nick in
into its place above the chamber /; the th
upper and lower rings are omitted in the fig
the plate ;/, carries a short narrow plate at
the tube h ^^'hich rests on it ; there is a strip
on eikch sidi) of this support, to prevent it
rplalivelj to the lamp. The part of the ti
gauEo is cut out, so ae to leave a clear space <
the paswige of the explosive mixture. The
chamber /, aad the pipe k supplies the jet in 1
the i^iiaotitv is regulated by screw-clips on tl
The experiment b made in the following \(
barrel is ^ Id. bore and 6 in. long, is loaded
powder, and several pieces of paper are ra
■ chargo ; the firing is done by a cap. The gas
iighttxl anil the wire gauze screwed ■"<■" ••■
; 'i^- --pie,- ^
t >l
l>
* ■!
■ ■!
. (
'l|
/
V^V^ ^^H -.-a^.-U^^H^ai^
i^ % Sac. VolJOai PL Til
i^^gSB»pB.^M«ggg
Il
ll
1874.] Mr. W. Galloway on Safety-Lampt. 4A7
oa the outside oE the lamp*. If the charge of gunpowder be increased
to '272 gramme, or be decreased to '136 gramme, the experiment does
not succeed ; and if the wire gauze has become smoked by the flame of
the inner jet being too large, the flame cannot be passed through.
In the apparatus represented in fig. 2, there are again two tin-plate
tubes, each 10 ft, long by 8 in. diameter, but they are joined to form one
continuous tube 20 feet long. At the end o there is a disk of wood,
I in. thick, with a hole in the centre for the mussle of the pistol. The
tube h (figs. 2 & 3), of tin plate, 12 in. long, has its interior isolated by
an india-rubber sheet tied over the end e, and a sheet of paper tied over
the end h. A ring, with a network of wires ^ in. thick, and with meshes
\ in. square, is drawn over the diaphragm in the same way as in the
apparatus already described. Two short tubes, of 6 in. diameter, ore
joined to fi to form a chamber lai^e enough to receive a safety-lamp ;
they are closed by flat ends, with the exception o£ a hole 3 in. diameter
in the upper one, opening into a chimney e, and an opening of 2 in.
diameter into the tube /in the lower one. The upper end of the tube
/ opens into a flat round chamber, with holes \ in. diameter and j in. apart
round about its outside ; it« position is indicated by the dotted line in
fig. 3. At the top of the chimney e there is a draught regulator, g,
which can be raised or lowered by means of the screwed spindle which
supports it. The safety-lamp to be tested is placed on the discoid
chnmber, with its top projecting into the chimney if it is so long. Gas
is supplied by a Bunsen burner at the bottom of the tube /, and, mixing
with air, it flows upn'ards through the discoid chamber into the isolated
space around the lamp. The products of combustion pass upwards
through the chimney.
The experiment is mode thus : — ^The pistol is loaded with '41 grommet
of gunpowder in the same way as before : an ordinary Davy or Clonny
lamp is lighted and put into the space d, which is afterwards closed at
the ends. Gas is then made to flow into the tube /; the lamp is observed
through the window h, and as soon as it is seen that the atmosphere in the
space (/is explosive, the shot is fired at o. The paper at it is blown out and
set on fire ; and the flame of the explosive mixture, passing backn-ards
down the tube/, ignites the gas escaping from the Bunsen burner.
The lamps which were tested with this apparatus are those known as
the Davy, Ganny, (Stephenson, Mueseler, and Eloin. The fiame was
easily passed through the Davy lamp, with rather more difficulty through
the Clanny, and not at all through any of the others.
The first experiments with firedamp were made in No. 7 Pit, Barleith,
near Glasgow. A wooden plug, with a small pipe through it, was driven
* ThiH experiment wu ahoWD bj Mr. Spottisvoode at tlie Bojal iDstitution on fiw
evening of the 17Ui of Januu^, I6TS, with the apparahu I bare deacribed. The aame
apperatuB na sflerwardi oaed at on« of the Cantor LeetnrM of the Societj of Arts.
t If the charge be in*de greater or lea» than thia b^ -15 gramme Vbe experiment
doe* not u«uallj succeed.
448 Mr. W. ti&Uoway on Safely'Lampa. [Juue 18,
into a horiEoutal borehole which had struck a blower, and the firedamp
was conducted in tubes to a colkctiag vessel at a short distAnce. I soon
found that this firedamp was very impure, as a mixture of one part of it
with thirteen parts of nir was not explosive ; however, I made a number
of eiperiments in the mine with both set-s of apparatus (tigs. 1 & 2,
Plate VI.), but did not succeed in passing the flame, except perhaps in one
doubtful instance with the larger apparatus, when the gaa issuing froni
the Bunsen burner was not set on fire.
l^he nest experiments with firedamp were made in the C Pit. Hebbom
Colliery, near Newcastle-on-Tyne. The gas, which issued Erom a bore-
hole similar to that in the Borleith Pit, va& coIlect«d in the same way,
and conveyed in the collecting vessel to a convenient place near tlie
etablea, where naked lights could bo used. The experiments with both
sets of apparatus were quite successful, the quantity of gunpowder
required being, in each case, the same as when coal-gas was used. The
Davy lamp employed in the experiments with the larger apparatus
belonged to the colliery, and was in constant use below ground. At the
fifth trial (when I had ascertained the quantity of gunpowder required)
the flame passed through the wire gauze, set fire to the paper tied over
the end k, and passing backwards down the tube /, kindled the ga«
iasuiug from the Bunsen burner. My brother, Mr. B. L. Galloway, who
was the resident viewer of the colliery at that time, waa observing the
lamp through the window A when the shot by which the flame waa
passed was fired. The flame of the wick, which was of ordinary dimen-
sions before it waa surrounded by the explosive mixture, had sent up a
long smoky point to near the top of the gauze, which showed that the
explosive mixture was composed of about 1 part of firedamp to 12 or 13
parts of air. The lamp was carefully examined after the trial, tmd was
found to be in good order.
The Directors of the Company to whom the colliery belongs were un-
willing to allow any further experiments to be made in the mine, so that
this series had to he abandoned before any more results had been obtained.
Following are the analyses of the firedamp used in the foregoing
experiments. The sample of gaa from the Barleith blower was collected
by myself at the time the experiments were being made, and analyzed by
Dr. T. E. Thorpe, of Glasgow; that from the Hebbum blower waa
collected by my brother several weeks before the experiments, and woe
aualyEed by Dr. Wright, of St. Mary's Hospital, London.
Barleith. Hebbum.
Light carburetted hydrogen 7586 85-22
Carbonic add 1-31 3-27
Olefiant gas traces
Carbonic oxide 1-36
Oxygen 2-17 1,.-,
22-83 7-98j^^^
100-00 100-00
1871.] Mr. W. Galloway m 8afety-Langu. 449
The next experiments were oa a larger scale. Through the kindaess
of Mr. Carrick, the City Architect of Glasgow, part of a new sewer in
North Woodside Bead was placed at my disposal ; and Mr. Foulis, the
manager of the Corporation Gas-Works, caused a pipe to be led into it,
and provided a liberal supply of gas. Figs. 4, 6, & 6, Plate YII., are
sections of the part of the sewer ia which the eitperiments were made ;
fig. 4 is a plaa section through the widest part, fig. 6 is a vertical cross
section showing the dimensions of the sewer (0 ft. x 4 ft. are the greatest
measurements), and fig. 6 is a vertical longitudinal section through the
highest part. Part of the sewer is a tunnel in solid rock (the diagonal
shading in fig. 0 shows the position of the rock), and part of it is built in
brickwork through the surface-drift. The length that was available for
the eiperimenta is comprised between the point A, where there was a
wide shaft to the surface, and the point C, where I caused a wooden
partition to be set up to prevent the draught of air from affecting the
lamp. B is a manhole, 3 ft. 6 in. x 3 ft. 9 in. at the bottom, and 23 in.
square at the top ; it was covered by two stones, each about 2 in, thick,
with a space about I in. wide between them across the middle of the top
of the manhole. The safety-lamp part of the apparatus (fig. 1, Plate YI.)
was set upon a board fixed across the sewer at the point L, at a height of
2 ft. 8 in. from the deepest point.
I made a large number of experiments here, but it will be sufBcd^it to
give only the principal results. The shots were fired from the same
pistol that was employed in the former experiment« at the distances from
the lamp indicated by the figures below fig. 0, Phte YII. ; they were
nearly all fired towards the position of the manhole B. Each measure
of gunpowder weighed '273 gramme ( = 4-213 grains). The number
of measures given below, corresponding to the distances from the
lamp at which the shots were fired, are those by which the flame
was passed ; uid it is to be understood that at each distance a charge
contuning one measure less was generally insnfBdent to effect the
purpose.
(1) Between C and L :—
At 37 ft. 6 measures = 1*365 gramme
S4 ft. 8 „ = 2-184 grammes
81 ft. 10 „ = 2-730
96 ft. 12 „ = 3-278
109 ft. 14 „ = 3-822
One experiment was made with the pistol pointing towards the roof at
an angle of 70° to the axis of the sewer ; the distance was 109 ft., the
charge 20 measures, = 6~460 grammes ; the muule of the pistol was
1 ft. 6 in. from the floor, and the firing was eSect«d by drawing a cord.
The flame passed through the wire gause, and ignited the gas on the
outside.
Mr. W. Galloway on Sa/efg-Lamjis.
(2) Between A aud L :—
At 33 ft. 8 measures = ^-134 gnmmea ^M
HI ft. a „ ^ 2-184 ^M
GO ft. 8 „ = 2-184 ^
It 18 remarkable that, iu these latter erperinients, it was not necessary
to iDfreflse the quanlityof guiipowiler as the distance from the lamp was
increoeed. The large uhargu required at the first station seema to have
been owing to the presence of the manhole between the lamp and the
point at which the shot was fired ; but this waste of enei^ haTing been
provided for, no further addition to the charge was required. It would
Beem as if part of the energy of the sound-wave was expended in the
space C L iu shaking the brickwork and a narrow wooden gangway
supported on cross-pieces at a height of 1 ft. Ti in. from the sole ;
whereaa in the space A L, in which no gangn*ay had been laid down, it
was conveyed through the tunnel in the solid rock without much lc«8 of
intensity.
The temperature of the air in the sewer was 55''-56° Fahrenheit ; and
there was generally a current travelling in the direction C to A at the
mt« of 5 to 10 ft. per minute.
These are the last experiments from which important results have been
oljtamcd i they were cuucludcd iu KuvemljiDr Ibi'J.
After this I made some experiments with firedamp in a Btone-mine in
No. 2 Pit, Douglas, near Glasgow. 1 filled a sheet-iron box of 18 cub. ft.
capacity with firedamp at the borehole in the C Pit of Hehhum Colliery,
and brought it to this mine. As the gas appeared to have become mixed
with MT through leakage during the transport, and would not bum
satisfactorily in the lamp of the apparatus (fig. 1, Plate VI,), the apparatus
shown in fig. 7, Plate VII,, was constructed. Two boards, each | of an
inch thick, and of the shape and dimensions of the top of the apparatDs,
are joined together by iron rods | of an inch in diameter, one at each
angle. A sheet of india-rubber, ^j of an inch thick, is then fastened
round the frame thus formed by nailing it to the boards, and an isolated
space of the form d, fig, 7, is obtained. An opening, 1| inch in diameter,
in the upper board senes as an outlet for the product* of combustion ;
and a similar opening in the lower board sen-es as an inlet for fresh air
and the firedamp from a Bunseu burner. This apparatus is placed on
two legs fastened to one of the sleepers in the roadway, and it is stayed
tightly before and behind by four stout wires in positions analogous to t,
the only one that can be seen in the figure.
A Davy lamp was lighted and placed in the inside of d,<mA block of
wood 3 inches high by 3 inches in diameter, so as to have its vrire gauce
as near as possible to the centre of the space i firedamp was then admitted
at the lower opening, and the-draught was regulated at a. The appear-
" ances presented by the lamp were observed through a glass window, h,
fastened in the sheet of india-rubber ; and as soon as the flame showed
1874.] Ob the Adiabatica and Itothertnelt of Water. 451
thftt the mixture Buirounding it was explosive, shota were fired from »
gun at a distante of 30 Tarda. The barrel of the gun which was used is
\^ of an inch in diameter, and it is rifled for a length of 3 ft. with
seven grooves ; the breech which received the charge is smooth-bored,
and 4^ inches long. Each measure of gunpowder weighed 3-822 grammes
( = 59 grains), and the charges fired ranged between 1 and 9 measiu«s ;
paper tamping was rammed down tightly, and the charge was fired by a cap.
The gun was tied to a prop in the middle of the mine, with its barrel
at an angle of about 35° upwards, pointing towards the apparatus ; tho
muKzte was 18 inches from the floor. At the part where the experimenta
were made, the si7.es of the mine are; — width at top, 4 ft.; width at
bottom, 6 ft. ; height, 5 ft. 6 in.
The sound-wave from a shot of two measures extinguished the flame
of the Davy lamp when it was placed on the outside of the apparatus ;
but when it was placed in the inside of d, the flame could not be estin^
guiahed nor passed through the meshes, even when the quantity of gun-
powder was raised to nine measures. However, after the lamp had been
allowed to bum in the isolated space for a few minutes (the supply of
fresh air not being very good), its flame could be extinguished by the
eound-wave from a shot of four measures. The whole quantity of fire-
damp was so small that there was no opportunity for enWging or varying
the apparatus.
These experiments, and one which I made formerly in the sewer with
the b tube of the apparatus, fig. 2, Plate VI., show that a very slight
obstacle n-ill interfere with the action of the sound-wave. They were
concluded in March 1874,
I woiUd add, in concluding, that the liberal grant of money which I
received from the QoTemment-Grant Committee of this Society has been
of great value in enabling me to carry out these experiments.
1 have also been much indebted for assistance to each of the following
gentlemen: — Mr. Eobert H. Scott, F.B.S.; Professor A. C. Bamsay,
F.E.S. ; Professor "W, W. Smyth, FJi.S. ; Professor Marreco, of the
College of Physical Science, Newcastle-on-Tyne ; Mr. John Galloway, of
Barleith and Dollars Collieries ; Mr. J. B. Simpson, of Kewcastle-on-
Tyne; Mr. Charles Shute, of Hebbum Colliery; and to Mr. William
Kirkwood, of the lukerman Mines, near Glasgow.
XX. " On the Adiabatica and Isothermalfl of Water." By A. W.
Rocker, M.A., Fellow of Braaenose College, Oxford. Com-
mtuiicated by R. B. Clifton, M.A., F.R.S., Professor of
Experimental Philosophy in the Umversity of Oxford.
Received June 4, 1874.
M. Verdet, in his work on Thermodynamics (' (Euvres,' vol. vii. p. 184),
enunciates the proposition " Deux courbes de nulle transmission ne peu-
452 Mr. A. W. Rucker m the [Ji
1 1
. r '■
I ■
I ■■ •
rent se couper,'' and offers a proof which rests upon the
that if a body could undergo a series of operations repreaeiiiftad ■■ ti'
changoR of pressure and volume by PQMP (where FQ is an ima/fkm
and PM, QM two adiabatics), no heat would be gained or lost ttfc aaf)
of the cycle except PQ.
It is, however, evidently impossible that the body oouldy at tha jgl
M, pass from one adiabatic to another without absorbing or enSMMigik
i. e, while fulfilling the very condition that it should not paaa fnmj
adiabatic to another ; and the question as to the poesifailitj of
section of two adiabatics must therefore be submitted to a
investigation, as it is certainly conceivable that heat might be
lost during the passage from the point M considered as lying on
curve to the point M considered as belonging to the second,
took place, as supposed by M. Yerdet, without any accompanying
of pressure or volume, or whether, as we shall see would be gensralfy
case, it could only be accomplished if the body were caused to
scries of intermediate states involving such changes.
The question admits of an easy answer if we consider tlie
bodies which can exist in two distinct states under the same
of pressure and volume ; and for the present we may confine oar
tion to water, which is the most conspicuous representative of the A
and which, at the ordinary atmospheric pressure and at tempenata
between 0° C. and 4^ C, exists in a series of states in which the Tolm
I are the same as those which it assumes if heated at the same ■
from 4° C. to about 8^ C.
Hence whereas for higher temperatures all the properties of
|. at atmospheric pressure are completely defined if we know the Yolni
niich is not the case between the limits above indicated ; but each poi
on the line of constant pressure given by jf>=l atmosphere between
intersections A^-ith the isothermals 0° C. and 4° C. corresponds to t
states of the water, or rather, since if the water-substance be oonyerl
into ice it will, if cooled suiRciently, again pass through the same
of volumes, each point corresponds to three states and is the in
of three isothermals ; and as a similar remark may be made ^^ith respi
to neighbouring lines of constant pressure, it follows that there ii
rcj^ion in the plane of pi' such that three states of the water-subatau
correspond to each point within it, and that therefore the values oi
and V given by any such point do not define the state of the water.
If, however, from every point in the plane of pv we draw perpendic
Lars to that plane, proportional to those values of some other property
the wiiter (say, in this ease, its temperature) which correspond to t
conditions 'of pressure and volume represented by the points from whi
tliey are drawn, the extremities of such ordinates will form a suzfii
which will be met once, or more than once, by any particular ordinal
according as the water can exist under the circumstances of pressu
and Tolnme defined by the point in the plane of pv tmm «
drawn in only one or in sevOTal states.
This Burfoce will be represented by the equation
uid curres may be drawn on it showing the relations between '
preasnre, volume, and temperature when the state of the water ta alto
in any determinate manner, tho prajeirtions on the plane af jw of th
represented by the equation to the surface, combined with
forming the boundaries of the region from all points in which ordiiu
can be drawn parallel to the axis of t vhich intersect the sar&ce in t
or more paints. The ordinary adiabatics drawn on the plane at ftv :
the orthogonal projoctiona of curves on the surface, each of which
defined by the condition that the water in passing through the series
states indicated by its successive points neither gains nor loses heat, i
which, to avoid confusion, will be called complete adiabatics.
Let now the line LM in the.plaDeo£^(fig. l)bethelinej>=il atx
sphere. Draw an ordinate frran L meeting the snrEace in A and
then, if different complete adiabatics pass through A and B, their p
jections on the plane of pu will intersect ; and the only hypothesis
which we cau avoid the assumption of the intersection of adiabatdcf
, that the coraplnte adiabatice are the intersections of the cbanicteris
surface _fl[|;)u()='^ wilh cylindrical surfaces, the director eur^-es of wk
are the plane adiabatics, and the generating lines parallel to the a
of I. In tliis case the saine complete adiabatic would pass tbrou
every such pair of points as A and B, which is eiideutly impossible,
in performing the cycle AQBPA the water would absorb beat alo
AQB without at any time emitting it, and yet would neither increase
internal energy nor perform any external work, since the cycle proje
into a straight line and a diacontinuoua curve meeting it in only one poi
As, therefore, a complete adiabatic cannot pass through A and B, and
a similar tram of reasoning would hold for the third point in which J
meets the surface, three adiabatics as well as three isothermals pi
throAigh the point on the plane of pv, tthich is the common projection
these points.
As this conclusion disproves -M, Verdet'a theorem, we may proceed
consider a few simple propositions based on the hj^iothesis of the po£
bility of the intersection of adiabatics ; and in so doing it will be advisa
to use a new term to distinguish between two classes oE ])oint* of int
section of the projections on the plane of pv of curves on the surfac
and reserving the usual expressions (intersect, cut, meet, &e.) for the p:
jections of points of intersection on the surface, we shall say that two cun
erou one another when they meet in a point which does not correspo
1874.] AdiabaticM and laolhermah <^ Water. 455
to an;- Buch point of intersection, but is only the common projection of
two separate points on the surface.
In the first place, tben, \re know that if water, starting from an initial
state eueh that addition of heat at constant pressure is accompanied b^
dimlnutioa of volume, be allowed to expand without receiving or emitting
heat, its temperature will rise; t. «. it will at the same time be doing
work, solely at the expense of its internal energy, and rising in tempera-
ture— a process which cannot go on indefinitely, as at lost all the internal
energy would be due to the temperature alone, and any further per-
formance of «ork would necessarily involve a fall in temperature.
Hence there must be a point of maximum temperature on the complete
odiabatic dranni through the point representing the initial state ; and the
isothermals through all other points on the same curve which lie within
the region, in which addition of heat involves contraction, must meet it
twice. The projections of these curves will also necessarily intersect in
two points ; and since when on odiabatic and isothennal meet the
tangent to the former always makes the larger acut« angle with the axis
of V (Maxwell, ' Theory of Heat,' p. 130), it follows that the two curves
must also cross at some point between their points of intersection, and
will thus form two loops.
This result holds however near the points of intersection may be
together ; and when they coincide the curves on the characteristic surface
touch one auother, and their projections on the plane of ^ir have contact
of the second order, since three points, i. €. the two points of intersection
and the crossing point, are coincident ; and, further, the isothermal which
thus touches the adiabatic is evidently that which corresponds to the
iDaximum temperature above mentioned ; and the point of contact lies on
the curve which is the boundary between the regions in which elevation
and depression of temperature are respectively the results of compression,
for at neighbouring points on the adiabatic the temperature is lowered
« hen the volume is either increased or ^minished.
All the points of maximum temperature on the complete adiabatics lie
on the curve defined by the condition
(I)-'
and since at all points on this curve the tangent planes to the surface arc
perpendicular to the plane of ^w, therefore the projections on that plane
of all curves intersecting it touch its projection, because their tangents
lie in a plane perpendicular to that of pv, aud are projected into one
line.
Hence the projection of any curve which meets this curve must at the
projection of the point of section touch an adiabatic.
But the ordinary interpretatbn put upon contact of an odd order with
an adiabatic is that tha body passing through the cycle of operations
VOL. XXII, 2 N
466 Mr. A. W. Biidter on tke [Jmia 1
represented by the curre, at the point of contact ceaMS to emit a
begms to absorb heat, or vice vertd ; and that therefore tiwrj elo)
cycle, if a continuous cnire, must hare 2n pointi of contact of an 0
order nith adiabatics, and if a discontinuous cune, 2m— r such pointa
contact and r points of discontinuity at which the carve does not eat 1
adiabatics passing through them.
This, however, evidently does not hold for a carve whidi meetg 1
curve in the plane of pv, defined by
(^}-
which is the projection of the curve in space, whose eqaatioiu are
/(^.0=0,(f)=0.
For since it does not follow that the cones in space have contact becai
their projections touch, we see that the curve in the plane of pv ni
touch an adiabatic without any change taking phtce in the ahaorpHaa
emission of heat ; and such a curve may, o>~en if continuous, hav« conti
of an odd order with an odd number of adiabatics. The pointof conia
for instance, of a cune which touches but does not intersect the llmiti
curve at nil points on which | -^ 1=0, projects into a point of contact
the third order at least ; and therefore the projected curve must
entirely between the adiabatic and projection of the limiting curre, whi
only have contact of the first order^ — i. t. it has n single point of conti
of an odd order, with an adiabatic whirh does not correspond to a char
in the absorption or emission of heat, and therefore on the whole it 1
an odd number oE points of contact of an odd order with adiabatics.
Let us now suppose that ABB' A' and afifi'a' are two adiabatics (fig.
which meet the curve l-f-f = O.andlet two isothermals.Aao'A' and 8^30"
meet the first in AA' and BB' and the second in aa and ffP" respective
We can now make the water go through Camot's cycle of operatic
between the same temperatures in four different wavs, of which we nt
only consider the cycles o'A'B'/3' and a'X'Bfl. In each of these the qui
tities of heat received along o'A' are the same, therefore the quantities
work done must be the same, i. c
area a' A'B'/3'a' = area o'A'E/3a'
=nrea a'A'B'|Sa'+area /3'B'B;3/3' ;
.-. area/a'BTJ/^/B^O.
But this area is composed of the two B'(3'ir and B/3i[, and they are
opposite signs ; for in going round the closed curve M^'B'M, th© wt
done on the body is greater than the work done by it, while in the la
MB/3M the contrary is the case ; whence wo conclude that the tm
B'i3'AI aad B/3M ai-e equal.
1874.] AdiabaHct and ItotkermaU cf Water. 467
In the figure the point 0' is represented u farther from C than M is ;
if, hotraTer, ff lies between M and C, then the croasing point of the
isothermal and adiabatic inaBt be substituted for that of the two adi»-
batics ; and in any case the areas of the two loops formed by two adia-
baticB and an isothermal which meets each of them twice are equal.
This result will still hold if we suppose that the two points of inter-
section with one of the adiabatics coincide, t. e. that it is that one which
has contact of the second order with the isothermal ; whence it follows
that the areas of the loops formed by any adiabatic and an isothermal
which meets it twice are equal ; or, in other words, that
If a body perform a cycle of operations which can be represented by
an adiabatic and an isothermal, it will on the whole do no useful work.
If we now proceed to consider the shapes of the adiabatics and
isothermals of water near their points of section ^vith the curve which
is the second boundary between the regions in which addition of heat
causes respectively increase and diminution of volume, and which corr*-
eponds for any given pressure to a local maximum as that already dis-
cussed does to a minimum volume, the applications of 'several of the
above remarks are too obvious to need any special comment ; but there ia
one isothermal the relations of which to the adiabatics which intersect it
are of a very complex order, and to which therefore it may be well to
draw attention. The isothermals of wat«r may be divided into two
classes, according as the pressure corresponding to the freezing-point is
or is not less than the maximum tension of aqueous vapour at the given
temperature.
As a type of the first we may take the isothermal corresponding to
0° G., which is represented in fig. 2. The maiimum tension of 8t«am at
this temperature is 4-6 millims. ; and as this is less than the pressure at
the f reedng-point, the vapour will be directly precipitated into ice, which
ndll in turn be converted into water, when the pressure amounts to 760
millims., the solid being thus intermediate between the gaseous and
liquid states.
An isothermal of the second class is repreBent«d in fig. 3. In thia
case the vapour is precipitated in the form of water ; and as the possii
biiity of the existence of water at the given temperature and pressure
proves that the freesing-point for the given pressure is below the tempe-
rature proper to the isothermal, and as any further increase o£ pressure
will tend still further to depress it, it is evident that the water-substance
can" never exist in the solid state at the given temperature unless at very
great pressures contraction instead of expansion accompanies solidifica-
tion. There must, therefore, be some isothermal which is at once the
boundary and limiting form of these two classes ; and if considered as
belonging to the first, it will be that for which the portion CD disappears,
I. f. for which the pressorea corresponding to the freeong- and boiling-
points ore the some.
2it3
458 Mr. A. W. Rucker on i/ie [June 18,
The form o{ this curve will therefore be that of an isothermal of the
second class ; but for the pressure corresponding to B'C the water-sulH
stance can exist in all three states ; and as the portion of the cuire in
space corresponding to B'C is a line perpendicular to the plane of pt^
its projection on that plane is the triple point of Professor James
Thomson ; and if we assume, with him, that ice, water, and steam can all
exist together at the temperature and pressure in question, it follows
that this line is both an isothermal and adiabatic ; for if we suppose the
water-substance to exist at the same time in all three states in a vessel
impermeable to heat, we can evidently by diminishing the volume con*
vert some of the steam into water, and employ the heat so set free in
melting a portion of the ice, during which operation the state of the
mixture will always correspond to a point on B'C.
Not only, however, is a single adiabatic coincident with the isothermal,
but all the adiabatics within certain limits pass through each point on
B'C, and are for a certain distance coincident with it, and therefore
with each other ; for as the conversion of ice into water is accompanied
by contraction, and that of water into steam by expansion, we can keep
the volume and pressure of a mixture of ice, water, and steam constant,
while, by supplying or subtracting heat, we alter their relative proportions.
The mixture can thus be made to go through Camot's cycle wiUiout
any change either in the pressure or temperature, the result always
being that no useful work is done ; and as in the earlier portion of this
paper it has been shown that it is possible for two adiabatics, drawn as
plane curves, to intersect, so now we have an instance of the intersection
of complete adiabatics, all three variables ^>, v, and t, to which points on
these curves are referred, being insufticient to determine the state of the
water-substance along the line B'C. . .
It is easy to determine the points at which the adiabatic corresponding
to any given mixture enters and leaves B'C.
Let (T, «, and 2 be the specific volumes of the ice, water, and steam,
r and p the latent heats of cod version of ice into water and steam respec-
tively, and V the volume of a kilogramme of the water-substance, when
the proportions by weight of steam, water, and ice are
We have then, as the temperature is constant,
and r=2{+«.v+Kl-^'-i)-
If no heat is supplied or abstracted,
dq=0 and /.(.v-.r,)+p({-£,)=0.
If we consider .v^ and f^ to belong to the initial state, two eases arise
according as
E^ is or is not >(1— .r^) -,
187i.] Adiabatics and ItothermaU of Water. 459
i. e. according as there is or is not enough steam to supply by its conden-
sation a Buificient quantity of heat to melt all the ice ; and as
which is always positive, as i — v is negative, we hare the largest and
smallest volumes given by the limits
.r=Oand l-a:-J=0,
or x=0 and£=0.
The maximum volume is therefore in any case given by
P
and the minimum volume is
(I-O ^l-^.)-pf.+, in the first
r-p
and ((-ff)!^al!l?*?+ff in the second case;
and the differences between these quantities give the range of volumes
for which the adiabatic belonging to the initial values x^, £, coincides with
the isothermal.
In conclusion it is only necessary to point out that some of the results
in the earlier part of the paper follow immediately from the ordmary
fonauliD of thermodynamics.
If Cp and C, are the specific heats at conslaut pressiure and constant
volume respectively, and if, to avoid confusion, we write the qti&ntity
which Is supposed to remain constant as a subscript to a partial differ-
ential coefficient, wo have the well-known expressioDS
""■ (S),-&;(l)/
where Q is consbmt for any adiabatic. From the first it follows that
■(I) =«.
Ha touch one anotb
i. t. the adiabaticB and isothermals touch one another at points of maxi-
mum or minimum volume.
Aiso by differentiation,
460 On the Adiabaticf and Isothemals of Water. [Jnoe
whence for all points on the ciure ■-j-=^< ^^ ^^^ '^
and therefore the contact is of the Becond order.
P.S. Since the above waa written, a paper has been publisbed in
'Annales do Cbimie et de Physique' for ALwch 1S7-1, iu which
author, M. J. Moutier, is led, from thermodynaniical considerations.
the coneiusiou that it is impossible for aqueous vapour in contact vi
ice to have the same tension as when it is in eontjict with water at
same temperature ; and as some conclusions have been pointed out in
preceding pages which follow on the assumption that at the triple p(
the tension of the \'apour is the same in each case, it may be well to sb
that his arguments do not really touch the question as to which of
two hypotheses is the true one.
M. Moutier discusses the case of a body which can exist in two <
ferent states, M and M', such as the soHd and liquid ; and supposing t'
the tension of the vapour ia different otcording as it is in contact w
the first or second, he obtjiins a general formula for the heat of trai
formation from M to M', from a consideration of the quantities of h'
gained or lost if the body is compelled to undergo a definite series
changes constituting a closed cycle (p. 34S).
The second operation in this cycle is that the body M' passes from '
pressure m to the pressure ji' ; and in the application of the gene
formula to the case of wat«r, M is taken to represent ice at 0° C,
liquid water at the same temperature, w tho atmospheric pressure, and
the tension of aqueous vapour over liquid water at 0°C. (p. 362).
If, however, the symbols have these meanings, the prescribed operat
is, in the ease of water, impossible ; for as water cannot ciiat at 0°
in the hquid state at less than the atmospheric pressure, the body
would be converted into M aa soon as the pressure m was diminish
and no conclusions can be dran'U from the cycle in question in the c
of water.
M. Moutier employs a second ai^nment which can be shown to h:
no greater weight tlian that already discussed, and which may be sta
as follows r —
If Q is the latent heat of conversion of ice into water, and L and
the latent heats of conversion of ico and water respectively into stes
then at the triple point we must havo
Q=L-L'.
L and L' are given by the well-knomi fomiidje
L=AT{f-«);J
rfi'
I'_AI(.'-»')*',
1874.} CtmtributionM to TerretMal Magnetiam. 461
where u and u' are the specific volumes of ice and wat«r, and p, p', v,
and u' the pressorea oad specific volumes of steam over ice aad water
respectively.
At the triple point v = v' and p =p' ; and M. Moutier further assumes
that ^ = —, and therefore obtains by subatitution
ilt lit
Q=AT(,.'— )f ;
and aa -^ is positive, being derived from f ormulte which have reference
to the iTiftTimiim teusiou of the vapour, and u' — u is negative, it follows
that Q, or the latent heat of water, is negative, a result which shows that
some of the premises must be false.
The erroneous assumption, however, is not the possibility of the
existence of the triple point, but is contained in the equation
dt ^ ~dt '
for Professor James Thomson has recently shown (Proc. Boyal Society,
Dec. 11, 1873) that M. Begnault's experiments, on the whole, favour ths
conclusion, which ho draws from theoretical considerations, that
dt dt
and if this equation be tnte,
\dp-
I dt
Q = AT («-w)M3-(^-u')
=AT j 0-13u-l-13tt+u' I !^ ;
whence, as at 0° C, f =210-66, while u and »' differ little from O'OOl,
it is evident that for a temperature so near lero as that of the triple
point, the expression within the brackets must be positive, and Q is, aa
it should be, positive also.
XXI. " Contributions to TerreBtrial Magnetism." — No. XIV. By
OeDeral Sir Edwakd Sabine, B.A., K.C.B., F.R.S, Be*
ceired June 18, 1874.
(Abstract.)
This paper is presented by the author as No. XIV. of his " Contri-
butions to Terrestrial Magnetism," completing the magnetic survey of
the northern hemisphere (of which No. XHI. comprised the higher lati-
tudes). It consists of a very brief explanatory introduction, followed by
Tables, in which (as in No. XIII.) the three magnetic elements are
arranged in Eones of latitude. These Tables, which form the body of the
work, are accompanied by three maps, presenting tlie resvdts graphicail;/ ,
in isogonic, isoclinal, and isodynomio lines.
463 Mr. J. Frcetwich m Tablet ^f [June 1
XXII. " Tables of Temperatures of the Sea at various Depths bdc
the Surface, taken between 1749 and 1868; collated ai
reduced, with Notes and Sections." By Josbfh Pbbsiwic
F.R.S., F.G.S. Received June A, 1874.
(Abstract.)
This paper was commenced b^ the author more than twenty yea
since, with a view to the geological bearing of the subject, but was f
some years unavoidably interrupted. It has now been broifght dov
to 1888, the date of the ' Lightning ' expedition, when the subject w
taken up by Dr. Carpenter, by whom it has since been so ardently ai
ably carried on. Nevertheless, aa Dr. Carp^^^^r's work relatm abnv
solely to recent investigations, the author considers that there is yet co
siderable interest attached to the work of the earlier obsenera from 17i
to 1868, though he feels that much of it is ncceMsarily superseded by t
great and more exact work subsequent to 18GS. He is aware that t
older observations have also not been deemed reliable on account of t
error caused by pressure on the thermometers at depths ; but this is 1
from applying to the whole of them, as that error was taken into accou
so early as lH3fJ, if not twfore, and a large number of these observatio
are equally reliable with the more nrceut ones, while the greater part
the others admit of corrections nbich r(.'uder them sufEicieutly availablt
In 1830, Gehler gave a list of 22(1 obsenations, and D'UnQle, in 18C
tubulated 421 experiments according to depths. The present paj
cootaiiH ft record of about 1300 obsurvntions, which are arranged occoi
ing to the degrees of latitude: — Ist, for the northern hemisphere; 2r
the southern hemisphere ; 3rd, iuland si-as. They are all reduced
common scales of tUermometer, measure of depth, and meridian. Thi
position is given on a map of the world, and the bathymetrical isothen
from the Poles to the Equator, based on the correct and corrected obsi
vatious, are given in a series oE ten sections. The author does not cla
for those obsenations the exact value, or the unity and completeness
plan, of the more recent ones, while, ns compared iiitli them, the depths
which tlicy were made are on the whole very limited ; still they inelu
a few at gR-ut depths ; and as they extend over much ground that 1
not been covered by the expiHlitions of the ' Lightning,' ' Porcupine,' a
' Challenger,' he trusts that tliesn Tables m.ty be of souie use as comp
mental to these later ivsenrihi's. and as bringing together and reducing t
conniion slnndard, observations st-alleri'd through a large iuuuIrt
works and memoir.". At the same time, the author would observe that
thinks it due to our many distinguished foreign eolle:igues who have be
engaged in the inquiry, and whose work seems but little known, that 1
results of their reseuR-hes should be undersfuod in this conntr)'. Th
couelusions, w hicli art* in close agivemont with those funned, entirely
1874.] Temperalurea of the Sea at variau$ Deptha. 463
dependently, upon recent and better data by Dr. Carpenter, acquire,
from this concordance, additional force and value. Theauthor was notat
all aware himself, in the earlier part of the inquiry, how much had been
done, and often found himself framing hypotheses which, on further
examination, he found had been long before anticipated by others.
The first part of the paper consists of an " Historical Xarrattve,"
which embraces an account of the character, number, and position of the
observations made by Ellis (1749), Cook and Forster (1772), Phipps
(1773), Saussure (1780), Pcron (1800). Krusenatem (1803), Scoresby
(1810 and 1822), Kotzebue (1815), "Wauchope (1816 and 1836), John
Eoss and Sabine (1817 and 1822), Abel (1818), Franklin and Buchan
(1818), Parry (1819, 1821, 1827), Sabine (1822), Kotzebuo and Lenz
(1823), Beechey (1825), D'Urville (1826), FitiEoy (1826), Blossville
(1827), Graah (1828), B^rard (1830), Vaillant (1836), Du Petit Thonara
(1836), MartinB and Bravais (1838), Wilkes (1839), James Eoss (1839),
Belcher (1843 and 1848), Aimo (1844), Kellett (1845), Spratt (1845-
1861), Dayman (1846), Armstrong (1850), Maury, S<^rs, Bache (1854-
57), Pullen (1857), Wullerstorf (1857), Kiind8on(1859), E.Leni! (1861),
Shortland (1868), Chimmo (1868).
The second part relates to the " Method and Value of the Observations ."
Wanting a reliable self-registering thermometer, the early observers, for
a considerable time, used a machine contrived by Dr. Hales to bring up
water, by means of a bucket with valves, from the depth at which the
temperature was to be taken. This was used by Ellis, Cook, Scoresby,
Wauchope, and Franklin, and one of a form improved by Parrot was em-
ployed by Lenz. Scoresby's observations in the seas around Spitsbergen are
oE much interest. He showed that while at the surface the temperature
varied from about 29° to 42°, the temperature at depths of from 2000 to
4000 feet was generally about 34° to 36° ; and there is reason to believe
that, with the very slight corrections suggested by Lens's subsequent
researches, most of them are correct mthin a fraction of a degree.
The most remarkable readings, however, token with this apparatus were
those obtained by Leus in Kotzebue's expedition of 1823. He applied to
the observations a correction founded on Blot's law of the variations of
temperature experienced by bodies in passing through mediums of different
temperature, and determined the lowest temperatures hitherto noted in
ijitertropical seas. Thus, one souuding in mid- Atlantic, 7° 21' N. lat., at a
depth of 3435 feet, gave a corrected reading of 35°'8 F., and another at a
depth of 5835 feet, in mid-Pacific, 21° 14' N. lat., gave 36°-4 F., the sur&co
temperatures being 78°'5 and 7fl°'5. His observations on the specific
gravity of sea-water are also valuable-
SauBsure and Pcron used thermometers surrounded with non-conduct-
ing substances, so that they might pass through the warmer upper strata of
« ater with little change. Saussure's experiments deserVe notice, inasmuch
as, after applying ft correction, they recorded, at that early period, for
464 Ml. J. PrcBtwichott TaAfeio/ [Juue 18,
the Mediterranean, at a depth o£ 1000 to 2000 feet, a teiuperaturo, w
nearly right, of ob°-5.
Sir iTuhQ Boaa and Admiral Spratt sometimes used SiVe thermomeitera,
ftud at others took the temperature of the silt brought up from the bottom.
The former obtained readings of 28°-5 F. for Baffin's Bay, and the Utter
of about 55° for the Grecian archipelago, agreeing therefore closely with
good thermometrical observations.
Phipps used adiSerentJal orerHow thermometer invented by Cavendish,
but it was not found to answer. This form of instrument remained in
abeyance until a greatly improved form of it was contrived by Wal-
ferdin (lArt-inomeir* d deeeriemmt) in 183ti. It was used by Mar-
tins and BravuB in the Arctic sens, and by Aime in the Medit«rnmean,
&nd was said to give very satisfactory results. Aim<5 also used aoother
BOmewbat simiTar instrument, which, at a given depth, was reversed and
then hauled up. These instnunents have the great advantage of being
free from errors arising from the shifting or immobility of the iiidei.
It is not clear why their use was abandoned, except that they were diffi-
cult to construct and not generally known.
Six described his thermometer in 1782 ; but the first person to use it
was Krusenstem, in 1803. It did not come into general use for deep-
sea observations until the ArL-tit- \oyagi's of Koss iiiiil I'nrry, iifti'r
which date it was, with the exception of Leni's and Aim^s, employed
for that purpose on all the expeditions sent out by foreign govemmenta,
as well as by our own. The necessity of protecting the instrumeat
against pressure was early insisted upon by Lenz, Arago, Biot, and
others ; and there is reason to believe that protected thermometers were
used by D'Urville and Berard, for their observations in the same Medi-
terranean area show a remarkably close agreement with those recently
made by Dr. Carpenter, with protected instruments, at and below depths
of about 200 fathoms, the results being : —
D'Urville (May 1826). Berard (Nov. 1830). Carpenter (Aug. 1870).
Surface , ... 64°- 1 F. Surface .... 67*-l F. Surface , , . . 73°-5 F.
1062 ft 54''-2 31 89 ft 55''-4 2958 ft 55°-5
3180 ft 54°-7 6377 ft 55''-4 79GS ft 54°-7
It was, however, on Du Petit Thouars's voyage of 1830 that the firat
special steps were taken to protect the thermometer against pressure.
For that purpose an improved instrument of Bunten"s was provided,
and this was eacloecd in a strong bross cylinder. Fifty-nine obser^-ations
were made, of which Arago reported that 21 might be considered perfectly
good. Temperatures of 36°, 37°, and 38° F. were recorded at depths
(900 to 1100 brassta) in both the mid-Atlantic and mid-Pacific; while
in one case, in taking a sounding at a depth of 12,271 feet near the
equator in the Pacific, the instrument came uj) crushed, but with th© index
fixed at 34^-8 F. (l^-S or l"-? C). In a certain number of cases (24) tiw
1874.] Temperutwret of the Sta tti varwu$ Depth*. 466
pressure forced water into the cylinder. For these corrections were
made.
In 1839, UM. Ujuiins and Bravais made a series of observations in
the sea between Norway and Spitzbergen with iofitrumenta carefiillf
protected against pressure hj means of glass tubes or metal cylinders,
Tbey used both self-registAring thermometers (thermom^rographet)
and Walierdin's self-registering overflow thenuometers, sending down
two to four of each in every sounding, and taking the mean of the readings.
These probably are amongst the most accurate observations on record.
To a great extent they confirm t^ose of Scoresby; and they further
showed that the bottom -temperature near the Spitsbergen glaciers was
about 29° P. None of the soundings exceeded 3000 feet.
In 1857, the lat« Admiral Fit^Boy furnished Capt&in Pullen with ther-
mometers specially constructed to resist pressure, and some very intereet-
ing, though somewhat variable results, were obtained thwewith. On two
occasions a temperature of 35° F. was recorded — one in the Atlantic,
26° 46' 8., at a depth of 16,200 feet, and the other in the Indian Ocean,
at a depth of 13,980 feet.
With regard to the many observations made with unprotected instru-
ments, they mostly admit of correction, which renders them availaUe.
Such corrections have been independently computed, with little difference,
by Du Petit Thouars, Martins, AJme, and the late Br. Miller. The
author, taking the mean of their estimates, uses as a coefficient — 1° F. for
every 1700 feet of depth.
In the third part of the paper the author shows the' " State of the
Question at the date of the Lightning Expedition." Ellis, Forster,
Peron, and others early remarked on the decrease of temperature at depths
in temperate and tropical seas, but it was not until 1823 that Lens
showed that a temperature of 35° to 36° existed at greater depths in
those seas. Notwithstanding this, D'Urville in 1826, misled by incorrect
readings obtained by previous observers with uncorrected instruments, and
in the absence of sufficiently deep observations of bis own, was led to
believe that the temperature in open seas at and below a depth of 3214
feet (600 brcutet) was nearly uniform at 39°'8 F. (4°-4 C), and that be-
tween the latitudes of 40° and 60° there is a belt of a like nearly uniform
temperature. A few years later, Arago, discussing the results obtained
by Du Petit Thouars, insisted that they effectually disproved this hy-
pothesis. Nevertheless, in 1830, Sir Jamea Boss made the same mis-
take as D'Urville, and unfortunately obtained for ,it a wider circulation,
which seems, however, to have been almost altogether restricted to this
country. Still, Boss's numerous ohsen-ations, when viewed uuder coi^
rection, are of considerable value, though the author cousiders that some
error has occasionally crept into that uniform reading, so often recorded,
of exactly 39°'5. Both D'Urville and Boss wrote under the opinion that
sea-vrater, lik« fresh water, attaioed it« maumum d^isity at a tempers-
Mt. J. i'rcBtwicli on Tabien uj [|Jmic 18
tiire of between 39° and 40°, — a point that had been investigaled ani
disproved by Marcet in 1819, a-pprosimately determined by Ermaan ii
1822, and which was finally settled by Deapreta, in 1837, at 'ia°-\ Y.
While the law of the decrease of temjjerature «-ith the depth, in botJ
the great oceaus, to a point but little above the zero of Centigrado wa
being estabHshed, experiments had been carried on in polar seas showiac
on the contrary, that the temperature at depths was higher than tJu
average Burfetce-temperature. The careful experiments of St-oresby wu
of Martins fully established this for the Arctic seas, and those of Boss
after correction, establish the same fact for the Antarctic Ocean. Ii
one part, however, of the Arctic seas this rule has not been found t<
hold good ; for, in Baffin's Bay, the eiperime.nta of John Boss, Sabine, and
Parry, at depths of from 600 to 6000 feet, agree in showing a decrease
of temperature of from 30° to 32° near the surface, to 20° and 28'''5 al
the greatest depths attained. There are also two instances given of yel
lower temperatures.
Nor were observations wanting in inland seas. Those of SaussuK,
DTJrvillo, and Bcrard had indicated generally that, in the Mediterranean,
the temperature decreased to a depth of about 1200 feet, after whicJi it re-
mained uniform at from 54° to 55" F.; and, in lS44,Aime instituted a series
of experiineuts which resulti^d in showing that the cliunial iiifluciice ceased
to be sensible at a depth of from 16 to 18 metres, and the annual variation
at a depth of from 300 to 400 metres, below which the temperature
remained constant at 12°-C C. (54°-0) ; and this he showed to be the mean
winter temperature of the area of the Mediterranean, over which his
observations extended. These obser\ alioiia were confirmed, for the
Eastern Mediterranean, by those of Admiral Spratt. His first experiments
in the Grecian archipelago shoned, ata depth of 1200 feet, a temperature
of 54°-5 to 55° F., while the later ones, at greater depths in the open aea,
give, after correction, a temperature of about 55°. In the Bed Sea,
Captain Pullen found that while the surface-temperatnre varied from 77°
to 86° F., it fell to 70° or 71°F. at 1200 to 1400 feet, below which
it remained uniformly the same to the greatest depth he attained of
4068 feet. Some curious results were obtained in 1803-6 by Dr. Homer
in the Sea of Okhotsh. The surface-temperature was 40°-4 F. ; and the
author finds (after correcting the original readings) at 360 feet a tempeia-
tureof 28°,aud at 600 feet of 28°-0, which is almost exactly that determined
by Despreta as the' temperature of sea-water at the moment of congelation.
The cause of the decrease of temperature with the depth in the great
oceans was early investigated by physicists. Humboldt concluded that
" the existence of these cold layers in low latitudes proves the existence
of an undercurrent flowing from the poles to the equator." l>'Aubuisson
and Pouillet took the same vie«-. D'Urville went further, and remarked
that " it is rather a transport uearly in mass, and very stow, of the deep
ivaters of high latitudes towards the e<iuator," and that from his xone of
1874.] Temperatures of Vie Sea at verioug Deptfu. 467
40° to 60° lat. there are two inseniible cuirentB — a lower one towards
the equator, (tnd an upper one towards the poles. Arago saw no other
explanation than " the existence of submarine currents uurying to the
equator the bottom waters of the icy seas,"
We are, however, indebted to Lens for a full and philosophical review
of tlie whole subject in 1847. After showing that all the facts proved the
existence of a temperature of from 34° to 35° F. at depths in the tropical
seas, and that this could only be maintained by a constant slow under-
current from the poles to the equator (which, on the other hand, must
necessitate the transfer by an upper current of the equatorial waters to
the poles), he proceeds to show by a series of observations, chiefly those
of Kotzebue, and by a diagram, that a belt of cooler water existed at the
equator, and that the temperature, at equal depths, was lower there
than a few degrees to the north and south of it ; and he concluded
that this arose &om the circumstance that the deep-seated polar watera
there met and rose to the surface. As corroborating this view, he
showed that the waters in the same zone were of lower specific gravity,
a fact that had been before noticed by Humboldt.
The author then proceeds to consider some " General ConelusionB."
Some of these have now been bettor established by the more recent
expeditions and by the researches of Dr. Carpenter, Taking, however,
other areas, he shows that in the Arctic Ocean the batbymetrical isotherm
of 35° is deepest on the west of Spitzbergen, while nearer Greenland and
again nearer Norway the desp waters are colder. The several isothermal '
planes of 40°, 50°, 60°, 70°, and 80° are then traced southward, attaining
their maximum depth between 50" and 40° lat., and rising thence towards
the equator. Section Ko. 2, from Baffin's Bay to the equator, shows that
the higher isotherms are not prolonged so far north as on the first line,
and that the water at the bottom of the bay is colder than in the Spit»-
bcrgen seas, approaching much nearer that of its maximum density and
of its point of congelation; whence he concludes that this is the main
source of supply of the deep-seated cold waters in the Atlantic, which,
after attaining their greatest depths between latitudes 40° to 50° N.,
are found 3000 to 4000 feet nearer the surface on approaching tho
equator,
In the South Atlantic, the bathymetrical isotherms show lesser curves ;
and while the isotherm of 40° crops out between the l»t. of 60° and 55°,
that of 35° is prolonged into high southern latitudes on a nearly imifonn
plane of 7000 to 8000 feet deep.
In the Pacific, the sections show that, notwithstanding there is no
appreciable polar current through Behring's Straits, the bathymetrical
isotherms of 60°, 50°, and 45° do not extend so far north as in the
Atlantic, while that of 35° is apparently not prolonged beyond 00° N. lat.
As the presence of temperatures lower than those which prevail in
470 Mr. J. A. Broim on the [June 18,
is the escesa or defect of spot-area for the same period of time, aud / is
a constant to be deduced from the observations.
Harittg obtained the mean spot-area for each year from 1832 to 18GT,
from Table VII. of the paper on this subject by Messrs. De La Rue,
Sten"are, and Loen'y", the meau for three periods of 11 years (1832 to
1864) was fouod etjual to G43 millionths of the snn's visible aurfaoe ; with
this quantity the values of +4 A (iu millionths of the sim'a surface) for
each year were obtained.
Mr. Meldrmn's conclasion depends chiefly on observations during these
periods in Great Britain ; and oa he has dedueed the rainfall for the first
period of minimum spots from obaep\*ations at three stations, Green^»-ich,
Carbeth (near Glasgow), and Aberdeen, I first examined the observations
nt these places together with simultaneous observations at Makerstoun
for the two periods 183i3 to 1853t. Applying the above equatii
these observations, the folloning results were obtained :—
Greenwich 4R= -0-00092 AA ;
Malfcratoun ... .iR=— 0-00020 AA ;
Carbeth AE=s +O-0O158 AA ;
Aberdeen AR= +0-00128 AA.
I
Greenwich and Mokerstoun are thus opposed to the conclusion, and
Carbeth and Aberdeen are more strongly in its favour. It should be
remarked, however, that the result for Aberdeen depends wholly on the
rainfall given for that place in 1834 (12-3 in.) being exact. Aa it is
12 inches less than the mean, while at the other three stations the defi-
ciency is only from 0-6 in. at Greenwich and Makerstoun to 1-2 in. at
Carbeth, this may be due to a leaky rain-gauge or to a clerical error of
10 inches. In any case no great weight can be given to the conclusion
from these four stationsj,
I now sought for an approximation to the mean fall of rain for Great
Britain, and for this end have employed the quantities deduced by Mr.
Symons from ten stations (British Association Report, 1865, p. 203;
1871, p. 102). The differences of spot-area from the mean, in millionths
of the sun's surface, and of the nunfall for each year are given in the
following Table :—
• Phil. Trans. 1870, p. 309.
1 The meonB for Makeretoun during the jenra 1832 to 1849 will be found in T™ns.
"Roj. Soc. Edinb. vol. lii. pt. ii. p. 108* the fnlla for the other yean are— 1850,
21-40in.; 1851, 25*57 in, ; 1852,32-20in. ; 1853, 2354 in.
} It may here be noted that the sum of the p2ui and mi'niw differences of Band tlw
mean rainfall for the four BtalionB during the twenty-two years irore —
Qreenwich. Makeratoun. Corbetb. Aberdeen.
Meanfall S4-4 in. 20'2in. 43-G in. 24-2in.
SiimsofAR 100-lin. C7-8in. 02-4in. 94-3in.
It nill be sesn that the sums of differences bare no relation to the mean fall of rain.
1874.]
Sun^ot Period and the BjunfaU.
Difierences of Baiufall for Great Britaiii and of Sim-spot a
1832 to 1867.
i Ml '
r«ir. AA. 1 iR. Year. AA. j AB. lYBat.'dA. aS.
Means.
1 ^ i 1 1
dA. AB.
i in 1 ' ' in ' ' in
in. 1
1832.-359 -Vbi ' l843.'-640' +2-66.1 1654. -501 -6-36
-467 -1-41
1833,'-558i +1-97. 1844 '-465| -4-02 ] 1855.1-5661 -4-47 ' -5401 -2-17
1834. -506, -3-22 1846, -232 +0-13i., 1856. -619' -1'85 , -452! -!■«*
183o.'+lTl' +0-82 , 1846. - 5 +1-83. ■ 1857. -428 -2-04 | - 87, +0-20
I836.'+746' +5-75 . 1847. +46S' -1-»4.| 1858. +177! -4-95.||+444 -0-38
1837, +556, -3'20.: 1848.' +395 +824 ' 1859. +756| +l>79 : +569I +1-94
1838.1+2931 -0-63.! 1849. +203' +0-77 , 1860.;+666! +5-60 ]|+384i +1-91 !
1839.l + 164i+3-53
1850.'-123 -1-39 '11861.1+659: -0'76.: +2671 +046
1840.;- 46, -3-07
1861.,+ 40 -l-Oi.,, 1862.|+530| +2-63 ,+ 174 -049
1841. -306! +5-77.
'l852.- 92 +7-7e.l| 1863. - 15] -0-81 1-138 +4'26
1842.' -429, -2-21
1 1863. -263' -0-36 „ 1864.1+245 -563»! -146' -2-73
i
' , II 1865.1-187! +l-9O.|!-409l -0-27
' 1
1 ! ||1866.|-342 +3'26« -458'-l-74
!! 1807. -468 +070.
-440|_(^34(
If we seek the value of / for the mean of the three periods of eleven
years commencing 1832 and 1835, ire find the following equations i —
1832 to 1864 AE= +00019 iA ;
1835 t« 1867 4E=+00011iA.
These results, then, are, as we expected, in conformity with Mr. Mel-
drum's conclusion ; bo that if we compare the year of largest with that of
smallest spot^area, the difference of rainfall should amount to2'61in. by
the first and to 1'5I in. by the second value of/. If we take the mean
spot-area for the years 1834, 1844, 1856, and 1866, and for 1836, 1848,
and 1861, wc find that the mean difference of rainfall for these years
should be 2-06 in. by the first and 120 in. by the second value of /, in-
stead of 8'45in. as found by Mr. Meldrum.
It will be seen also that the greatest mean differeace of rainfall is that
for the years 1841, 1852, and 1863, and this was an excess of rain for
years of spot-area deficiency ; were another such opposite difference to
present itself, it would neutralize the conclusion derived from these
means. It should also be observed that while the first and third periods
of eleven years are in favour of the connexion, the second (1843 to 1853)
is opposed to it (this is also the case for the eleven years 1857 to 1867).
It will be seen, then, that from this discussion a probable difference of
about 2 inches of rain may be expected betwixt years of greatest and
least spot-area.
This result is derived from observations at ten stations, distributed
over a very small pat«h of the earth's surface ; and it is evident that for
any serious investigation a much larger series of observations represeDt-
ing the rainfall over a great extent of country would be essential.
* Indieatea oppoaita aigni of AA. and AB.
I
472 On the Sun-stpot Period and the Rainfall. [June
I now examined observations made at diSerent stations in India ;
this esamination showed the extreme difficulty of otitaining a sattafac
result, either way, from a few stations in that country, when, in ccr
yeara, Ihe accidental excess of raiafall at some of the statjcms tii»<
4<j iacbes, even though de'ficiencies at some stations may diminiah
amount of the error.
Fri>m my ouii experience of rainfall on the Indian ghats, I sin
doubt that a mountain -station, such as Mussoorte. Ih well fitted U.
employed in this diseussioD. If a single station could he taken to w
Beat any tract of countrv, it ought to he one least liable to local auuM
variation. Among the mountains a slight change in the nrerage di
tion of the wind will cause great differences in the rainfall at stat
but little distant from each other, and to eliminate accidental variat
of 40 or 80 inches would require observations during a very loug m
of years.
The foUowing Table w-ill, however, show the quantities which may '
to be dealt with at an Indian hill-station t : —
Valnet of AB for Mahabuleahwar, 4600 feet above the sea, vrith i
corresponding values of AA.
Y«r.
AA.
AB.
Y«»,
AA.
OB.
1832.
-359
in.
-261
1843-
-640
in.
+32-7»
1833.
-558
-49-3
1844.
-465
+ 9 3*
1834.
—506
+ 443'
1845.
-232
- 3-1
1835.
+ 171
-26-3'
1846.
- 5
+35-3»
1836.
+746
- 9-4*|
1847.
+ 469
-34-2*
1837.
+556
+ 14-8
1848.
+ 395
— 8-0*
1838.
+ 293
-72-8'
1849.
+ 203
+ 85-4
1839.
+ 1C4
-I9-8-
1840.
- 46
+31-4-
1841.
-306
+ 28-0"
1842.
-429
+ 51-&-
V
From this Table we derii'e the equation
aH=-0-02in. AA,
Of that 26 inches mart rain falls for the year of lf<iit than for thi
grenlest spot-area. The examination of many series of ohservationa
shonn how difficult it will be to arrive at a conclusion for a quantifr
small as 2 iuches of rain.
It is evident that a larger tract of country than Great Britain sbi
be chosen, and the approximate rainfall be deduced from the grea
t For tlie rainfal! nt MBhabulfBhwar, 6«e Colonel SjkM'8 paper on Indian obsi
lions, Pbil. TraiiB. 1850, p. 3li7. Ths mean fall is 2530 inches.
Indicate! oppoutB ngiu o[ ^A uul ^"B^
1874.] Pretents. 478
poasible number of stations. O^rmany and France may give sufBcieut
dftfft for such a trial. Were the result well marked, there would be
reason to seek for its confirmation in other oountrieB ; but to undertake
this labour, better grounde, I think, must be found than I ha^e hitherto
been able to obtain. The admirable series of observations which Mr.
Symons is obtaining will sufGce for the future, as for the past, ten years
to give a very near approximation to the excess or deficiency of rainfall
in Great Britain.
XXIV. " Oa the Mechanism of Stromboli." By Robert Mallht,
M.A., P.R.S. Received May 17, 1874*.
The Society then adjoomed over the Long Tacation, to Thursday,
Norember 19.
IWttnta received May 21, 1874.
Transactions.
Berlin : — Physikaliscbe Gesellscbaft. Die Fortschritte der Physik im
Jahre 1869, redigirt von Dr. B. Schwalbe. Jahrgang 25. 8vo.
Berlin 1873. The Society.
Birmingham : — Institution of Mechanical Engineers. Proceedinga,
October 30, 1873. 8vo. The Institution.
London : — Pharmaceutical Society. Pharmaceutical Journal and
Transactions. Februaryto May 1874. 8yo. Calendar. 8vo. 1874.
Catalogue of the Library. 8vo, 1874. The Society.
Royal United Service Institutiwi. Journal. Vol. XVn. No. 74,
75, and Appeudii. 8to, 1873-74, Lectures addressed to Officers
of Volunteer Corps. 8vo. 1873. The Institution.
Manchester: — Geo! ogical Society. Transactions. Vol. XIU. Part 3.
8vo. 1874. The Society.
Montreal : — Natural History Society. The Canadian Naturalist and
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473 On the Sun-spot Period and the HainfaU. [June 18,
I now eiamined observftHous made at different stations in India ; but
this examination showed the extreme difficulty of obluiniug a Batiafactorr
result, either way, from a few statious in that country, when, in certain
yearB, the aci-ideuta! excess of rainfall at some of the ataliona may be
40 inches, even though deficiencies at some stations may diminish the
amount of the error.
From my own experience of rainfall on the Indian ghats, I ahould
doubt that n monntain-statioa, such as Muasoorie, is well fitted to be
employed in this discussion. If a single station could be taken to repre-
Bent any tract of country, it ought to be one least liable to local causes of
TariatioQ. Among the mountains a slight change in the average direc-
tion of the wind will cause great differences in the rainfall at stations
but little distAnt from e«ch other, and to eliminate accidental varUtionB
of 40 or 80 mches would require observationB during a very long seriea
of years.
The following Table will, however, show the qoantitieH which may hxn
to be dealt with at an Indian hill-statioiit : —
Tataes of A£ for Mahabuleshwar, 4500 feet above the sea, with the
corresponding values of AA.
Year.
AA.
AE.
Tear.
di.
AK.
1832.
-359
in.
-26-1
1843.
-540
+^2--:»
1833.
-658
-49-3
1844.
-466
+ 9-3*
1834.
—506
+ 44-3*
1845.
-232
- 3-1
1835.
+ 171
-26-3"
1846.
- 5
+35-3"
1836.
+ 746
- 9-4*
1847.
+ 469
-34-2"
1837.
+ 556
+ 14-8
1848.
+ 396
- 8-0"
1838.
+ 293
--2-8-
1849.
+ 203
+ 85-4
1839.
+ 164
-19-8"
1840.
- 46
+31-4*
1841.
-306
+28-0*
1842.
-429
+51-9*
From this Table we derive the equation
AE=-002in. AA,
or that 26 inches more rain falls for the year of leatt than for that of
greatest spot-area. The examination of many series of obsen'ations baa
shown how difficult it will be to arrive at a conclusion for a quantity so
small as 2 inches of rain.
It is evident that a larger tract of country than Great Britain should
be' chosen, and the approximat* rainfall be deduced from the greatest
+ For the rainfa!! Ht Mabsbuleahwar, «ee Colonel Sjkea's paper oo Indian oboerta-
tions, Phil. TraoB. 1850, p. 367, The mean M is WSO inche*.
IndicaUa oppoaiU signl of AA and AB,
1874.] Preaentt. 478
possible number of Btations. Oennacj and France msy give enfficient
data for such a trial. Were the result well marked, there would be
reason to seek for its confirmation in other countries ; but to undertake
this labour, better grounds, I think, must be found than I have hitherto
been able to obtain. The admirable series of observations which Mr.
Symons is obtaining will sufBce for the future, as for the past, ten years'
to give a very near approximation to the excess or deficiency of rainfall
in Great Britain.
XXIY. " Oq the MechaDism of Stromboli." By Robert Mallbt,
M.A., P.R.S. Received May 17, 1874*.
The Society then adjourned over the Long Yacation, to Thursday,
November 19.
Prttenta reetived May 21, 1874.
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• This Fqptr will ^pear iu Ko. 169.
482 Present. [June 18.
Hogg (.Tabez) The Pathological relations of the Diphtheritic Membrane
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The Author.
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Photographs of Absorption -apectra of Didymiuma and other Solutions.
W. N. Hartley.
Oh the Absorption of Carbonic Acid. 483
"On the Abaorptiou of Carbonic Acid _ by Saline Solutions."
By J. Y. Buchanan, Chemist on board H.M.S. ' Challenger.*
Conununicated by Professor A. W.WiLLiAMBONj For. Sec, R.S.
Eeceived December 11, 1873 *.
In the ezamination of sea-water, whether it be regarded from a chemical
or from a zoological point of view, the determination of and the varift-
tious in the amount of carbonic acid in different parts of ocean must
always be an object of importance. This is more especially so when a
parallel aeries of observations on the quantity of oxygen present is
carried out. At the surfaoe we should expect to find the quantities of
these gases following the law of partial pressures ; at greater depths,
however, where the water for long periods only comes in contact with
water, we should expect to find the quantity of oxygen decreasing and
that of carbonic acid increasing with the amount of animal life. The in-
vestigation from this point of view of the bottom-water, at greater and
smaller depths, presents perhaps a more interesting field of observation
than that of intermediate depths. Down to nearly 2000 fathoms life is
still abundant ; below this depth, however, the amount rapidly decreases
till, at about 2800 fathoms, it is, for carbonic-acid producing purposes,
practically extinct. We have, then, to settle the variation of the car-
bonic acid with latitude and longitude, with depth, with nature of bottom,
and with nature of atmosphere.
In order to solve these problems, it is before all necessary to have a
reliable method for the determination of the carbonic acid. For the
discovery of a cause of error in the old method, and for the invention
of a new one, we ore indebted to Dr. Jocobsen, of Kiel. Dr. Jacobsen
found that sea-water could not, as had been till then assumed, be
thoroughly freed from its dissolved carbonic add by merely boiling in
vacuo f. He found that it was necessary to boil down almost to dryness
before the last traces of carbonic acid could be expelled. Being parti-
cularly interested in the matter, I immediately commenced a series of
experiments to determine, if possible, the salt or salts to which sea-water
owes this peculiar property. A short resume of the results of these ex-
periments have been published as an appendix to Professor Wyville
Thomson's ' Depths of the Sea.'
I purpose here to give a detailed account of the experiments performed.
They consisted of two series — the one analytical, the other synthetical.
In the former I was ably assisted by Mr. George Macdougald, in the latter
by Mr. Bobert Bomanes, junior assistant in Professor Cnun Brown's
* Read Febnuuj 19, 1674. See anii, p. 192.
t Dr. Andrsfra informB me that be lud observed a iimilor pbenomODon vhen at-
tempting to determiiie the amount of atmoipberic gaaea in seo-wator, b; boiling it in
tbe Torrioelliaa vscuum after Uw manner of nponr-denii^ detorminatioiu.
VOL. XZU, % -&
484 Hr. jr. T. Bnehanan on ik$ MmffHm tf
laborfttoTf in the tTniverritjr of Edinburgli, ud I ^adDj ftTail iii j Milf of
thia oppoituQitj to tlunk thnu botii.
The analytic series connsted of ezperinuoifs oa HlatuKu of tfcs
different salts saturated with carbonic ftcid. A oeriam qiunUly <rf «Mi
ms distilled almost to dTyness, tlw steam being condaoBed in an ordmiy
Liebig's condenser, to which was fitted a tnbnlated TeoelTer, faAvii^ a
bulbed T-tube attached containing baiTta-water. The dutillaliaa «M
intermpted and the baiTta^wster changed after the iwii^Bo of amf
eighth of the distillate, the amount of carbonio add paaaed bsbig rong^
estimated bjr the apparent turbidity of the bar]rt»>wit«r. The objpet of
these experiments being to find ont which of anuroberofuliiis Mlnlii^
had the property of retaining carbonic add, and to aaontain roogfalj'wkit
length of time one most btnl in order thoroughly to expel it, an amm ite
determination of the carbonic add actually passing during t^ intanali
would hare been superflooui. Besides these, a number of qnanfitalin
determinations were made of the amount of cubonio acid actually
absorbed by different solutions.
The synthetical series consisted of experiments for the detemunatioB
of the absorption-coeffidenta of two solutions — the one of mlpliato <(
magnesia, the other of sulphate of lime.
Let us take the analytical series first. As before remarked, it ia sub-
divided into two sets, which we shall treat in their order, "in. the one
observations were made on the elimination of the carbonic add as the
distillation proceeded ; in the other nn attempt was made to determine
how much carbonic acid, in a saline solution saturated with the gas, was
actually retained or bound, or at least kept from freely exercuing its
properties as a gas, by the presence of the salt in the solution.
Finl Exptnment. — In order to have a certain standard of comparisoo
in judging the retardation caused by salts in the escape of carbonic add
from solutions on boiliog, distilled water was saturated with the gas and
distilled in the manner indicated above. During the passage of the first
eighth of distillate the gas evolution was of course abundant, during the
second a perceptible quantity passed, after which no more could be de-
tected. It may be assumed, then, that, in the experiments which followed,
the carbonic- add held simply in toliUion by the water passes almost
entirely in the first eighth part of the distillate, and that whaterer
passes afterwords has been retained, in some way or other, by the salt
in solution. In conducting these experiments no baryt»-wat«r ms
put in the reedver itself, but only in the V-tube, The water collected
was always tested with baryta-water, and with the general result that
in the firet fraction carbonic acid was present in abundance, while in
the latter ones there was rarely a trace to be detected. That the dis-
tillate consisting of pure water should contain not a trace of the ga*,
whose presence in the atmosphere above it is attested by the precipitate
Carbonic Acid by Saline Solulunu, 485
in the exit-tube, shows that, at feeble preasarea, the Bolntion of carbonic
acid requires conaiderable time for its completion.
Second Experiment, — A chloride-of-sodium solution contfiiniiig 2 per
cent. Ifa CI had a strong stream of CO, passed through it for abont ten
minutes and waa then distilled. During the passage of the second*
eighth there was still a conaiderable quantity, during that of the tdiird a
Tcry slight trace, and after that none.
Third JExperimtnt. — A chloride-of-magnesium solution contMuiug 0-25
per cent. Mg CI, vas treated in the same way as the chloride-of-sodium
solution, when the whole of the CO, passed in the first fraction,
Fovrlh ffirpeWnwnt. — A solution containing 4 per cent. Mg C), and 10
per cent. Xa 01 was saturated with CO, and allowed to stand in a closed
■ vessel over night. On distilling, it was found that carbonic add con-
tinued to be given off in perceptible but gradually decreasing quantities
until the end.
Fi/lh Experiment. — For this and the three following experiments a
solution containing 12-3 grammes crystallixed sulphate of magnesia (in
a litre?) was used. Carbonic acid was passed through some of this
solution for about 10 minutes, and the liquid allowed to stand in a
closed vessel over night. On distillation there passed during the second
fraction very little, during the third and fourth fractions decidedly
more, during the fifth again much less, and afterwards, to the end, slight
but perceptible traces of carbonic add.
Sixth Experiment. — The solution was heated to neiurly boiling, and CO,
passed into it until it was cold, the whole being allowed to stand over
night. During the passage of the second, third, fourth, and fifth frao-
tions, the amount of gas was about constant and small. It increased
greatly during the sixth, falling away again during the seventh.
Seventh Experiment.— "^^q conditions were exactly the same as those
of the fifth experiment ; and the results in the two cases agreed weU with
each other, the amount of gas coming ofE increasing slightly about the
middle of the operation. In order to see if the rise of temperature con-
sequent on concentration had any thing to do with the phenomena under
consideration, a thermometer was immersed in the Iwiling liquid. It read
at the end of the second, third, fourth, and fifth fractions 102°-5, 102°-9,
103°, and 103°-2 respectively.
Eigfiih Experiment. — The conditions were the same as in the last,
only that the solution stood two days before dlltillation. In the re-
sults there was this peculiarity, that in the fourth fraction the cai^
bonic odd disappeared altogether, reappearing, however, agitin in the
fifth.
* It is unneetMMj in the eases wliere no means were (sken to free the solution
from simplj dinolred cartmnjo scid to repeat in esoh one tbst tlie first rnction con-
tained abuudsnoo.
Mr. J. Y. Bucliannn on the Abnorption of
Ninth KrjperiiitftU. — Sea-wal«r from the Firth of Forth waa dutillwl.
Here, iw in the rase of the sulphate of ma^esia, the amount coming off
incrc&sed about the middle, falhDg away again in the fifth fraction. In
the siith, howerer. It experienced a slight increase, falling off again
towards the end of the operation.
From these eiperimenta we may conclude that, alone and in the
degree of eonceatratiou in which they occur in the sea, the two moxl
abundant salts, namely chloride of maguesium and chloride o£ sodiuni,
Bsercisc no retarding influence on the liberation of carbonic acid on boil-
ing. When mixed, however, as in the fourth eiperiment, they appear
to hare thia effect. Whether, if sufficiently diluted to represent sen-
water, they would continue to do so I was unable to ascertain, »a the
investigation of the sulphates occupied all the time at my disposal. . It
is further evident that, in the sulphatenaf-magnesia solution experimenteJ
on, wo have a solution wliich behaves towards carbonic acid in the same
way as sea-water.
Let us pass now to the second set of the analytical series — namely, the
estimation of the amount of carbonic acid retained in cousoqnence of tha
presence of the salts in (luostion. The apparatus used was the same as
that in the last set, baryta -water being contained both in the receiver
and in the V-tube.
Experiments were made on solutions of sulphato of magnesia, of lol-
phat« of magnesia and chloride of sodium, and of sulphate of lime, to
which were added some on sea-water itself. In every erperioieiit the
quantity of solution operated on was 300 c. c. The carbooic add
coming off was retained by baryta-water of known strength, the re-
maining free baryta being afterwards determined by means of oxalic
acid. Eosolic acid was used to determine the point of neutralizataon.
The oxalic acid was rather stronger than tenth-normal ; it contained
6'478 grras. C,H,0,H-2H,0 in the litre, which is equivalent to 2-259
grms. carbonic acid. 1000 c. c. baryta-water required 3235 c. c. oxalic
add for neutralization.
The method of conducting the operation was as follows :— Carixmie
add was passed through tfc' solution until it could be assumed to be
saturated. Six to seven littes of air were then drawn through it cold,
after which it was heat«d to boiling, and allowed to boil for from two to
three minut«s in a current of air. The receiver \vith the baryta-sol uticai
was then attached, fed the distillation continued in a stream of air,
until the contents of the flask were nearly dry. The baryta-water then
remaining imneutrolized was titrated, and from it the amount of ctirbaaic
add ascertained.
Experimenti on tulphate-of-magMiia solution containing 12*3 fframnut '
eryttallized talt per litre. — As all were conducted in precisely the same
■kay, it wiU be sufSdent to give the results in a tabular form. The first
Carbmie Acid by Salme Sobiiiotu. 4S7
three expenmentB were m&de with portions of one uid tiie Bame Bolu-
tion ; for the last two & fresh eolution (prepared, to all appearance,
in exactly the same way as the previous one) was aaed. The differ-
ence in the results obtained show the precarious nature of the com-
bination:—
Volume
of eolution
lued.
Volume
ofberytB-
water.
Volame
of oialio
add.
GrunmM
in300o.c
oirboDioidd
inllUre.
300 0.C
25c.c.
78 96 e. 0.
0O043
(KI143
300 „
10 „
30-0 „
0-0053
OflI65
300 „
10 ..
30-9 „
l>0033
o-ono
300 „
15 „
47-5 „
01)023
0<I077
300 „
10 „
31-32 „
0<I023
0-0077
Two experiments were made with a solution prepared as follows : —
The quantity of sulphuric acid necessary for the formation of 12-3
grammes crystallized sulphate of magnesia was diluted to a litre, and
pulverized carbonate of magnesia suspended in it. Although the mixture
was allowed to stand over night, shut off from the influence of the
atmosphere, the solution was still exceedingly acid. It is well known
that carbonate of m^nesia is dithcultly soluble in cold dilute acids. To
have heated the solution would have frustrated the object of the experi-
ment, which was, by bringing nascent sulphate of magnesia together
vith nascent carbonic acid at ordinary temperatures, to give them the
best opportunity of combining.
Two experiments were made with a similarly prepared solution of sul-
phate of lime. In this case sulphuric add was added to the water in
quantity sufficient to form, with lime, more salt than was necessary for
the production of a saturated solution of g3rpBum. Here neutralization
took place without difficulty, and, as might have been expected, the
amount of carbonic acid formed was considerably greater than in the
case of the magnesia salt.
Two experiments were made with an ordinary sulphate-of-magnesia
solution containing 2-05 grammes crystallised salt per litre.
Two further experiments were made with a solution containing 3-05
grammes sulphate of magnesia and 20 grammes chloride of sodium per
litre. All were conducted in the way described above, and the results are
given in the following Table, The experiments n-ith the carbonates of
magnesia and lime were made at a considerably later date than the
othen ; the value of 10 c. c. baryta-water had in consequence become
equivalent to 32 c. c. instead of 32*34 c. c. oxalic acid.
Mr. J. Y. Buchanan on the Absorption of
JTnturo
of
■olulion.
Volume
of (olulion
Voliuue
oflmrrta-
ToluRio
of oxolio
Mid.
carbonioadd
in 300 0. <:.
Tn 1 liU*.
H,SO, 1,
300 0.0.
10 0.0.
30-6 0.C
OiKBS
001J)7
300 „
10 „
30-9 „
O-OO'JS
" OflOSS
0. ». 1
H, SO, \
'300 „
10 ,.
275 ,.
0-1014
0-3380
300 .,
10 „
2T'6 „
0-lOH
0-3380
2^)o gm>«, (
MgSO^-t-TH, 0-^
per litre, \
3O0 .,
300 „
10 „
10 „
ai'3 „
31-3 .,
O0026
O'0O23
twwei
0-oon
Ugao.+7n,0|
300 „
10 „
318 ..
O-OOIU
tH3053
Nta 1
3fX) ,.
10 „
31-4 „
0-00£l
OOOTO
Five cxperimenta were made ivith Gca-water taken at tlie end of
Portobello Pier, on the Firth of Forth. In t!ie first three it w»s sub-
mitted immodiately to the same treatment as the saline solutions ; in tba
Isst two carbonic Bcid was first passed through it for some time. As the
results given in the folloning Table are idontieal, it u evident that, in
its natunil slate, the water iu question was saturated with carbonic odd
in this peculiar state of combination.
Experiments <
I Soa-water.
Volume
ofwntCT
UMd.
Volumfi
of barjU-
water.
Volume
of OMlio
acid.
carbonic acid
m300o.c.
Orammes
carbon io acrid
in 1 litre.
300 e.0.
15 a 0.
3*75 0.0.
0^)108
0<XiOO
300 „
10 „
23-0 „
0-0211
0-0703
300 ,.
10 „
M15 „
00-208
0OC03
300 „
10 „
23-34 .,
0K)at3
0H)677
300 „
10 „
23-34 „
0-0203
00677
Subsequent experiments inade at sea, on water from mid-ocean and
from various depths, have shown me that the above quantities are very
much in excess of the quantities usually contained in ocean-water. From
the large quantity of organic matter poured into the Forth, not for from
Portobello, there must be an abundant production of carbonic acid in the
wat«r itself, and we have seen above the efEect of bringing sulphate <£ lime
and carbonic together in the nascent state. Sea-water containn, on an
average, about 8 parts sulphate of lime in 10,000. A satorated aolntion
of the some salt in diHtilLed Nvabei contains at 15° C. 24 parts iu 10,000.
Carbonie Acid by Saline Solutions,
Under the most favour^le ciTcumBtenDei, than, one voold expect aear
water to bind about one third of the quantity retained \>y an equal
volume of sulphate-of-lime aolation. We hare seen that a litre of this
solution us capable of retaining 0*338 grm. CO,, while the same Yolume
of aea-wator contained only 007 grm., or consideiably leas than the third
of that held bj the sulphate of lime. In ocean-water I have never yet
found more than 0'064 gnn. CO, per litre, including both the simply
diuolved and the half hound. We have, then, in the sulphate of lime alone,
an agent capable of retaining much more carbonic acid than is uaually
found to exist in sea-water. Besides this there is also, at least, the sulphate
of magnesia possessing this properly. How much it would be capable of
absorbing if the carbonic acid were presented in a nascent state in a
neutral solution we do not know ; it would be interesting to detennino
the amount of carbonic acid retained by a solphate-of-magnesia solution
in which organic matter had been allowed to decay.
The practical conclusion to be drawn from the preceding eiperiment«
is that, as the carbonic acid is retmned by the presence of certain sul-
phates, the gas will be more easUy boiled out if we get quit of these
sulphates. For this purpose I always add to the sample of sea-wat«r,
in which the CO, is to be det«rmined, a sufficient quantity of a saturated
ehloride-of -barium solution to precipitate all the sulphuric acid present.
The effect has answered my expectations. Aft«r the first fifth of dis-
tillate haB passed, there is rarely a perceptible turbidity in fresh baryta-
water. In practice, however, and as it costs but little trouble, I always
distil oS from three quarters to seven eighths, and often quito nine
tenths of the solution.
The determination of the carbonic acid in sea-water is carried on on
board the 'Challenger' by means of an apparatus, a very slightly mo-
dified form of the one deacribed by Dr. Jacobsen in the ' Annalen der
Chemie und Pharmacia,' a drawing and description of which he was good
enough to give me when the ' Challenger ' was fitting out,
A flask with a capacity of about 500 c. c. receives the se^-water to be
operated on, uaually from 200 c. c. to 250 c, c. It is closed by an
india-rubber cork, through which pass two tubes ; one, reaching to the
bottom, communicates with the condenser, a cylindrical copper vessel,
10 in. high by b\ in. diameter, with a block-tin w<ffin. The lower end
of the worm ia attached to the receiver by a bent glass tube with a
flexible joint, from which a glass tube leads to the bottom of the
receiver. The flexibility thus obtained is, in practice, of the greatest
use, enabling the operator, by shaking, to expose constantly fresh sur-
faces of baryta-water to the passing gases. The receiver ia connect«d by
an india-rubber tube with two bulbed V-tubes. An aspirator enables a
stream of air to be drawn through the apparatus, a soda-lime safety-tube
being interposed between it and the T-tubes. The water running from
the aspirator is conducted outside the port by a tube which passes
490 Mr. J. Y. Suchauau on the AbtorpHoa of
through a hole in the eaeh. The flask coDtuoiag t
ported on u ring, b; a. clasp hoiding its neck. Both oi these, along
the spirit-lamp underneath the fiaak, are attached in the usual vaj 1
iron rod, which is attached to the projectiiig side of the ship 1^ an
bolt, in which it has a plaj- of rather more than an inch in the dure
of its length. The lower end of the rod sits Becurelf in a htde, let
the t«p of the working-table. When the apparatus is dismounted t^
is pushed up, tiU its lower end has freed itself from the hole and
flat along the roof, being supported at one end bf an eje-lKdt, al
other by a hook. The aspirator and the condenser are retained in
places by wooden blocks, which fit in between them and the ship's ni
the battens on the bench.
The water in which the carbonic acid is to be determined is introd
into the flask by means of a tube reaching to the bottom. Whei
carbonic acid ia to be determined in a specimen of water, the apparat
first put together and a current of air, free from carbonic add, di
through, care having been taken to see that it Is tborooghly dry in ■
parts. The corks in the receiver and V-tubes are then eased,
from 15 c. c. to 20 c. c. baryta-water, usually of about -^ no
strength, run into them. The water to be examined is introduced
the flaak through a tube reaching to the bottom ; 10 e. c, of a n
saturated solution of chloride of barium are then added, the appai
closed and heat applied. "When the liquid begins to boil, care mui
taken to lower the (lame to aioid frolhing over. A gentle eurrei
air is now conducted through the boiling liquid, and the receiver
stantly agitated. After half an hour's boiling, about 100 c. c, ^
have distilled over, and at the same time all the carbonic acid,
the latter is the case, I ascertained by changing the baryta-water at
point, and continuing the distillation, when no turbidity waa prodi
Tliat, at any rate, no appreciable amount of carbonic acid passes ;
even the first 60 c. c. water have been distilled over, may be very e
seen by tho liquid iu the receiver passing from a (nrbid, some
frothy solution, to a clear one, in which a well-defined precipitate is
peuded, and whose amount does not visibly alter as the distdlh
proceeds. Although such is the case, I liave usually, as it costs
little more time and trouble, carried on the distillation until s
eighths hai'e passed, and indeed, in many cases, until crystallization
commenced. "When proper attention ia paid to the agitation of
receiver during the first part of the distillation, the amount of oarl:
acid reaching the first T-tube is quite insignificant, and the bai
water in the second remains perfectly clear. When this operatic
finished, the contents of the V-tubes are washed into the receiver
boiled water, aud the remaining alkalinity determined with hydroch
acid of known and convenient strength. The jioint of ncutralizatit
indicated hy rosolic acid.
Carbonic Acid by SaUtie Solvtiom. 491
Syntheiieal Experimentt. — In order to cbeck the &bove experimentB, it
appeared to me to be of importance to determine the absorption-coeffi-
cients of one or more of the solutions for carbonic acid. Before knowing
any thing of the retention of carbonic acid by sea-w&tor, I had determined,
if possible before the sailing of the ' Challenger,' to investigate the solu-
tions of some of the salts occurring in sea-water, with reference to their
power of absorbing the atmospheric gases. It was well known that
sea-water, in common with most other salt-solutions, absorbed a smaller
quantity of sir than distilled water would do under the same circum-
stances ; but it had never, to my knowledge, been attempted to find out
whether this diminution of absorptive power was distributed equally
over the three gases, or was exhibited mora etroi^ly in the case of one
gas than in that of another. From a preliminary experiment in which a
2 per cent, solution of Na CI in distilled water was saturated with air and
the air then expelled and analyzed, it appeared that the oxygen was
present in slightly greater quantity relatively to the nitrogen than would
have been the case if the liquid had been distilled water. Of course, this
being the result of only one experiment, no conclusion can be drawn from
it ; but it shows the necessity of the investigations which I had proposed
to myself. 'U'nfortunat«ly, the time at my disposal was l«o short to allow
of any thing being done, except a few experiments with carbonic add and
solutions of sulpluite of magnesia and of sulphate of lime.
For this purpose I made use of a Bunaen's absorptiometer, and fol-
lowed his method, with the modifications rendered necessary by having
to do, not with a simple liquid, but with a saline solution. The carbonic
acid was introduced into the absorption-tube and measured, not in the
mercurial trough, but in the absorptiometer itself, the lid being left open.
This is a much more expeditious way, inasmuch as the gas quickly
assumes the temperature of the water of the absorptiometer ; and as the
readings after absorption are all done in this way, there can be no
object in reading the gas alone in another way. After absorption, the
instrument is always read with the lid shut, so that what corresponds
to the height of mercury in the trough is given by the height of it in the
outside graduated leg of the absorptiometer. In all of the determinations
this height is given, not in the reading on the leg itself, but in the cor-
responding reading on the absorption-tube, which can be directly
observed with sufficient accuracy with the ordinary telescope used in gas-
analysis. As after shaking the instrument and opening the stopcock
connecting the leg with the body of the instrument some of the water
frequently passed into the former, we have generally a reading marked
" water in outer leg," which forms a factor in estimating the tension of
the gas.
The solutions experimented on were, one containing 1-23 per cent,
crystallized eulpfaato of magnesia and one containing 0*205 per cent,
gypsum. It was neceesary that the«6 solutions, before \>wa% Ssixs^Asisaii.
493 Mr. J. Y. Buchanan on the Absorption of
into the absorption -tube, should be deprived of air tvithout off'
their state of concent ration. This was cffoctad in tbo following
A flask fl*aa filled up to a mark in the nock with the solutaon, Iialf
was then emptied into another flask and the two boiled, while di
water was kept boiling in a third. When the boiling had been ke
for about half an hour, the contents o£ the sMoud flask were en
into the first and woBhed out witb tho hot distilled water, the volui
the Holution being brought in this way up tu the mark, and bo for
it as was equivalent to the expansion of the solution for the differci
temperatures. A glass syringe of convenieut size was now filled
the boiling liquid and passed hot into the abaorjition-tube. This mi
may be objected to on two grounds ; iirst, tiiat there is some unoert
a!:>out the exact concentration of the solution when introduced iat
absorption-tube ; and, second, that some air may have been absorbc
the liquid in ila passage through the syringe to the tube. Aa ti
first objection, when the operation is carried out in tho way I
described, the possible diSereuee between the actual and assumed
c«ntration is ho small that it would be extremely imlikely to haT«
influence on the coefficient o£ absorption of the bquid. Ab to the ao
if the manipulations be expeditiously carried out, there is but little
that tlie liquid at so high n temperature, and exposed to the sui»U q
tity of air of diminished tension in the syringe, should be contamii
in an appreciable way. However much or little importance one
attach to these possible sources of error, they probably explain wh
whole subject has been left almost entirely untouched.
Our object in these experiments is, not to determine the abaorp
coedicient for a standard pressure such aa 7G0 miUims., but to deter
it for various pressures, the temperature being kept as luiiform as
cumstances will permit, and to compare the results obtained with I
calculated for distilled water.
Let V=volume of gas (at 0° and 700 niillims.) beiore introdui
of solution,
V,=yolume (reduced to 0'^) of gas after absorption,
Pj^pressure of this gas,
then the volume of gas absorbed will be
' 7ti0
And if A be the volume of the solution, we have for tho coefflcieu
absorption at pressure P, and tho temperatiure of obserratiou.
Two series of experiments were made on solution of eulpliati
magnesia contnining 1*23 per cent, cry staliieed salt, and one aeriet
Bulphate-of -lime solution containing 0'20j per cent, of CaS0j+2t
Carbotue Acid by SaJmc Sohtioiu.
Tbe detailed results are given in four T&blei. In the Grat are given the
original volumes of the carbonic add used in esch series, n-ith the data
for finding the same. In columns 1 and 2 are found the volumes used
in series I. and II. reapectivelj for sulphate of magnesia ; in columu 3
ia the volume for the BulphateK)f-lime experiments.
Tabu I.
Table giving the original volumes of carbonic acid used in the three
series of experiments I., II., and III.
1.
2.
8.
2
?
T
P
V
741-6
694
323
271
562
40-7
10'8
9-665
001-5
73-267
48-509
741-5
561
322
259
544
40-15
e-8
9046
618-a
73-039
47-600
738-5
686
331
255
058
4118
10-8
9-866
513
75-09
48-759
Height of water column in oaUir crlinder...
Tapour-leniion for (°
HeactingprMurefi-ii+s-T)
Volume in c. o. of b, from calibration Table
Volume (v) reduced to 0° and 760 millinu.
In series III. (Table IV.) with sulphate of lime, and in series I.
(Table II.) with sulphate of magnesia, the readings were made without
loss of time, the pressure being successively increased for each experi-
ment. In series II. (Table III.} particular attention was paid to the
length of time this gas and solution were in contact at the different
pressures, and for each experiment the pressure was successively
diminished. They were left in contact for nine days at the highest
pressure (column 1) before reading; No. 2 wos read twenty-two houn
later, No. 3 forty-one hours later than No. 2, No. 4 twenty-five hoiin
later than No. 3, and No. 5 aft«r the lapse of some days.
Haslb II.
SeterminatioDa of the absorption-coefGcient of a 1*23 per cent, solutioa
of crystallized sulphate of magnesia for carbcmic acid at the tem-
peratures and pressurea indicated. Te-46'609 o. c.
BaromeUx
ThemiomeUr
Outer lerel of merouTj
Inner lerel in abtorption-
tubo
Upper lerel of lolulion in
anorption-tube
Upper leTol of miter in outer
Bee^tant mtter column
741-5
120
568-7
314-2
293-0
234-0
2420
-104-0
102fl
352-0
-106-0
736-0
119
1825
199-0
395
123-0
-loo-o
Mr. J. Y. iiuchanan on the Abtorplion qf
Tabie II . (wniinwrf.)
1.
a.
3u
4.
Tapour-lemion torC
BesultAnt preuure on gu
VolumB in c. c. of c, from
odibration T.blB
VoluiQB B reduced to 0° and
i
P,
V,
*;
- 11-3
10-457
476-M
36043
22-100
71-218
M-275
O-7O05
O'fiWB
- 7-68
10-120
C627
ifrin
1»343
50«7a
0-9562
(H)631
- 7-07
10-389 .
68114
33-481
17-206
67-S«8
31-487
0*496
0-W55
- 7-S8
lfr3»
736-73
9*18
8-983
4a^&l
l-UMS
10718
Volume of solution iv,-t) .
,ureP,«illiu«.I;i.„.
tiil«l*™£br for same Uin-
penture and pressnw ...
Table III.
Determinaticins of the absorption-coefRcieiit o( a 1"23 per cent, solntiaa
of ciystoIliEed sulphate of iDOgneaia for the tcmperaturea and pres-
surea indicated, the duratioii of the reKtion being taken into a<xrouiit.
V=: 47-650 c. c.
I.
2. 1 3.
4.
h.
/.
w
i
V,
*:
736-5
U-l
630
174-5
40«
30
-73'0
- r,-4fi
9-867
8-327
0-905
]0'439
3D-761
20-8S6
I -2467
1-3052
737-0
II-O
257-0
2305
95-8
196-0
-72-7
- 5-37
9-793
695-3
22106
19-441
52-337
30-231
00331
1-0145
747-0
10-45
446-5
265-6
131-4
383-0
-GO-7
- 515
9-443
551-5
30-07
21-016
60-256
30-186
08823
0-M61
742-0
11-1
B06-0
277-0
143-0
440-0
-68-0
- 5-03
9-857
498-1
32-G7
20-.WB
62-841
30171
0-S974
0-7456
OuUt IbtbI of mercury
553-5
Upper leral of solution in
Upper Ipvel of wsler column
Bcsultant water ccliinm
{a f i,+c,} .
- Stt
9«SI
468-fl
36-32
23«l
88-73
3(W0)
O-Sffl
O-TClt
Exultant pressure on gru
VtSumo in 0. r. ot c, from
Volume t- reduocd lo 0° and
t
Volume of BoluKonfs.-^)...
Coelllrient of ubsorption for
Umperaturo (° and prr-s-
«urBP,niimn.B.I^.,,
tilled waUT for same Iflm-
peroturo and preesiirB
Carbonic Acid by Saline Soltiiiona.
Table IV.
Determinationa of tbe absorptioii-coefBdeDt of a 0-205 per cent, solation
of gypsum for carbonic acid at the temperatures and presBurea
iadieated. V=48-75fl c. c.
tarolneter
[hermameter
)ulor IbtbI of mercury
Iddbt 1«vel in absorp-
Jpper leTel of water
ID outer leg
iMultont watflr
column
!«,-/,-',+<,}..
IquiTalent mereurj-
column
rapour-temion for (°
iMultaoC pre»ure on
gM
calibration
rolnme'
TMe
Tolnme f reduced to 0 °
and 760millime. ...
Volume in a. o. of 6,
Tolume of solution
.. (".--;) ■■•■:■•■:■
4305
274-5
163-6
43G-0
5M-S7
35-02
47-73
27-90
- B-86
9-867
770-8
15-42
15-028
43-80
-745
- 5-5
0-857
805-2
13-87
eeO'S
10-43
Ibsorption-cocfficient
of distilled water
tor same («nipem-
ture and preoure...
Comparison of the results of series I. and II, shows the effect whicli
these sulphates have in tJtering the power of absorption of water for
carbonic acid, -when they aie allowed sufficient time for the reaction.
The subject of the abaorption-power of saline solutions is one of much
importance, and affords aa almost inexhaustible field for research, when
the effect of varying the natiuv of the salt, the strength of the solution,
the temperature, tiie pressure, and the duration of the action of the solu-
tion on the gas are taken into account. I hope, at some future time, to
be able to resume this interesting inquiry.
U.M.S. ' ChaUengttr,' Simoa'i Bay, Not. 4, 1873.
4M Mr. U. Mallet on the
" On the Mechanism of Stromboli." By Robert Mallet, MJL,
F.R.S. Received May 17, 1874*.
Stromboli and Slaaaya stand oloue, so far as observation has vet gone,
amongst, the volcanic vents of our planet, in the remarkable charactoristic
of having a distinctly rhytbmical intermittence and recurrence in their
eruptive action. Masaya, though known for about 300 years, has been
but little obBerved, so that some doubt may exist as to whether it« adicm
be truly int«rmilt«at and recurrent or not ; and if we leave it sside for
future observation, Stromboli stands unique amongst terrestrial volcnnoe*
in the rhythmical character of its eruptions, more or less accurate obser-
Tfttions as to which are upon record for above 2000 years. Every vol-
canic vent is indeed intermittent, and often recurrent, in its action, whioh
has been properly denominated paroxysmal, but no law can be traced in
the inten-ala of time elapsing between the paroxysms. A vent may sud-
denly open and a cone be thrown up, as in the case o£ Mont© Nuovo, and
after this burst volcanic effort may cease there, perhaps permanently j or,
as in the case of Vesuvius, prior to A.n. 7fl, a period of repose mav exist
in a volcanic cone already formed, exceeding human local tradition, to bo
Bueoeeded by paroxysmal efforts, rarvinp eimrmously in intensitv, and
with intiLTvals in lime bi:-(:«r"'ri ~i]rri<si\i> criiplion^ \:irvi]np from hours to
centuries. In all tliese there ia no rhytbmical recurrence, or at least none
that, upon the narrow scale open to our observation, can be viewed ■■
such. In Stromboli, on the contrary, there is a distinctly rhythmical inter-
mittence and recurrence, so regular in time, and preserving for centnriM
such a general uniformity in energy, and of such sbght violence, as to
point to some distinct train of mechanism as producing it — that me-
chanism, whatever be its nature, being comprehended vithin a moderate
distance from the surface, and not referable to the more mighty and deep-
seated forces which determine the uncertain and altogether unpredictable
paroxysms of volcanoes generally. Not that the rhythmic intervals of
Stromboli are precisely the same at all times, as has been erroneously
stated by many travellers, nor the i-iolence of its outbursts at all times
aUke ; but both vary within narrow limits during the immense historic
period that it has been observed. No satisfactory explanation has yet
been given, so far as the author is aware, of the physical and mechanical
condition constituting the mechanism upon which this extremely curioos
rhythmical action depends ; and it is the object of this paper to point ont
what appears to be its real nature. It is the more worthy of attentive
study, as Strombob is in reality the link thateonnects two widely different
phenomena — namely, the ordinary cone of eruption and the geyser.
Stromboli is, in fact, a volcano and a geyser united and acting together
in the same vent, the rhythmical action which characterizes the geyser
" Bead Juno 18, 1874. See anti, p. 473.
Mechanism of Siromboli. 497
being thtiB commnnicated, within certun limits, to the otherwise irregular
and accidental activity of the volcano.
Passing ancient accounts, Stromboli has been viaited in modem days,
amongst men of science, by SpallanEani, Dollomiea, Hoffman, Scrope,
Daubeny, and several others ; but no very full or exact description
of tbe crater and its adjuncts, much less any adequate explanatioa
of the curious mechanism of its action, has been given hj any of thesA
writers.
Hoffman's account of the phenomena witnessed by him, though far
from clear or satisfactory, is curious enough to deserve translation
here : — " The volcano appeared to have changed into a hot mineral
spring ; then at irregular times we observed that the continually deve-
loping steam be(!hme stationary, and, with a jerking uncertain motion,
rushed back into the mouth of the crater. At the same time we felt a
terrifying trembling of the ground, accompanied by visible oscillationB of
the loose crater-sides. Then followed a hollow roar, and a volume of
steam shot out of the crater, accompanied by a shrill crackling. Thou-
sands of laTar-fn^ments, which had been carried up with the steam, spread
in the air like sheaves, and then fell back, either into the mouth or on
the surrounding cinder and sand walls. "We could distinctly see (parti-
cularly on this occasion) the boiling, seething lava dash against the sidei
of the shaft, separate into two streams, and then fall back ; but the lava
ejected in bubbles flew far through the air, twisting and tearing along,
foaming drops, bright as cooled glass, clattering as they rolled down the
declivity."
Mr. Scrope makes the following remarks in his ' Yolcanos ' (second
edition, pp. 332-334) :—
" The remarkable circumstance in this small but interesting volcano is
that the column of lava within its chimney is shown, by the constant ex-
plosions that take place from its surface at intervals of from five to fifteen
minutes, casting up fragments of scoriform lava, to remain permanently
at the same height, level with the lip of the orifice at the bottom of the
crater, and therefore some 2000 feet abore the seo-level. It is evident
from this thot nearly a perfect equilibrium is preserved between the ex-
pansive force of the intumescent lava in and beneath the vent, and the
repressive force, consisting in the weight of this lofty column of melted
matter, together with that of the atmosphere above it ; consequently a
very small addition to or subtraction from the latter, such, for instance,
as a change in the pressure of the atmosphere, must to tome extent, how-
ever small, derange the equilibrium. It need not therefore surprise ns
that the inhabitants of the island, chiefly fishermen, who ply their perilous
trade day and night, within sight of the volcano, declare that it serves -
them in lieu of a weather-glass, warning them by its increased activity of
a lightening of the atmospheric pressure on the volcano — equivalent to s
fall of the mercury — and by its sluggishness giving them assurance ol ^Vi.%
Mr. R. Mnllet o
reverse. It is the tension of heated steam or water lUsiieuiiiiated through
the lava in and beneath the vent which occasioas its eruptive action, and
the boiJing-point of every drop or bubble must be sensibly affeclod by
every barometric variation
" In (lie foul weather of winter I was assured by the inhabitants that
the eruptions are sometimes very violent, and that the whole flank of the
mountain immediately below tho cr«t«r is then ^jccaaionally rent by a
fissure, which dischajgea lava into the sea, but must be very soon sealed
up again, as the lava shortly afterwards finds its way once more to the
summit, and boils up there as before. Captain Smyth found the sea in
front of this talus unfathomable, which aceounts for the remarkable fact
that the constant eruptioua of more than 2000 years have failed to fill up
this deep-sea hollow."
Dr. Daubeny (' Vole-anos,' second edition, p. 248) appears to hai'e
given but a cursory examination to the crat-er ; and in his observations ou
its phenomena only repeats SpalhuiKani, Hofim&n, and Mr. Scrope, as
(oUowa : —
" The unremittent character of tbe eruptions of Stromboli appears to
arise, as Mr. Scrope has suggested, from the exact proportion maintained
between the expansive and repressive force. The expansive arises from
the generation of a certain amount of aqueous vapour and of elastic
fluids ; the repressive from the pressure of the atmosphere, and from the
weight of the Buperincumbent volcanic products."
The mechanism, as imagined by Mr. Scrope, fails, in the author's opi-
nion, to account either for the rhythmical character of the eruptions or
for the alleged connexion between them and the state of the weather.
No equilibrium between the " expansive " and the " repressive " forces can
possibly exist at the moment of an outburst, the circumstances of which
prove an excess of pressure of many atmospheres, which has been gradually
increasing since the last outburst became quiescent.
To account for the actual facts, we must have sucli a train of natural
mechanism as shall cause a gradual, though rapid, iacreaso of steam-
pressure within or beneath the vent or tube of the volcano, imtil the ac-
cumulated pressure suffices to overcome whatever obstacles it may
encounter, solid or liquid, and by blowing these away release the pressure
itself in a burst of steam, stones, dust, &c. The conditions producing
this gradual increase of steam-pressure must be such as shall give rise to
the rhythmical recurrence, at comparatively short intervals, of fbe pheno-
mena. These conditions are certainly not to be found, either in the
general nearness of balance of any eipanaii'e and repressive forces alone,
or in any conceivable relation between these and variations of atmospheric
pressure.
Mr. Scrope has, as the author believes, greatly overrated the altitude of
the fundus of the crater in stating it at 2000 feet above the sea. But let as
suppose the height of the column of liquid lavs, between the level of the sea
Mechaninn qf StromboH. 499
and the fundus of the crater, to be one fourth of this, and the expanidve
and repressive ftgencies in the nicely balanced equilibrium assumed, what
effect could any variation of barometric pressure, within the limits ever
experienced on any part of our globe, produce in disturbing such equi-
librium ? A rise or fall o£ the barometer at the rate of a tenth of an inch
per hour is known only to occur in connexion with the most violent hur-
ricanes. A fall of half an inch in the mercury within three or four hours
exceeds probably the utmost that occurs in connexion with the most vio-
lent Mediterranean storms. But let us suppose a fall of two inches in
the barometer to take place instantaneously, how far would that affect the
equilibrium supposed of such a column, however supported, and whether
free from aeriform matter or containing vesicles thereof ? Two inches of
mercury are equivalent to about -^ of the usual pressure of the atmo-
sphere, or to less than one pound to the square inch at the sea-level. The
liquid lava supposed to fill the column may be allowed to have a specific
gravity of at least 2-000 ; a rise or fall, therefore, of a single foot in the
top surface of this column would equilibrate this exaggerated amountand
rapidity of barometric change. But the head of the column itself is de-
scribed by Hoffman as continually in oscillation upwards and downwards
through several feet. It is obvious, therefore, that changes of atmo-
spheric pressure have nothing whatever to do with the mechanism pro-
ducing the recurrent action of this volcano.
"Whatever reality there may be iu the notion, long handed down,
of some connexion between the degree of activity of this volcano and
changes of weather appears to be merely superficial, and the true inter-
pretation will be referred to further on. In any case this notion of
equilibrium within the chimney of this particular volcano, and its dis-
turbance by changes of atmospheric pressure, would be equally applicable
to every volcanic vent in the world, and fails to throw any light upon the
special phenomena which characterize Stromboli, viz. the quasi regular
recurrence of its bursts forth. The geysers of Iceland belch forth water
and steam, and occasionally stones, agd the order of recurrence is the same
whichcharacterizeatboHeof StromboH. The latter does not send forth water .
en maste, its ejecta being steam mixed with some gases, carrying up con-
siderable masses of solidified lava, chiefly iu angular blocks, mixed occa-
sionally, but not always, with torn shreds and lumps of half-solidified
lava, in a more or less plastic state, together with a preponderant volume
of dusty pulverulent matter. It is highly probable that water, not in the
state of steam, but in that of solid drops, is frequently blown from
Stromboli, and such may be felt falling to leeward after some of the bursts
forth, though not after all. It may be doubtful, however, whether or not
these drops may arise from steam condensed in the (ur.
We thus have, to the same succession of phenomena as those of the
geyser, superadded in Stromboli some of those of a volcanic vent, of feeble
but lung-continued activity.
VOL. zxn. ^ ^
&00 Mr. R. Maliet on the
The phenomena of geysers were for n long time suppoeed peculiar to
Iceland ; sad although they are now known to exist elsswliere, their
characteristics are nowhere better observable than in Iceland.
The recurrence of their outbursts, their duration and iutervnls, wem
very well described by Von Troil in his ' Lettei^ on Iceland ' in 1 772, and
have been further described by Sir George Mackeniie in 1810.
Henderson had ascertained that atones, or other obstacles, thrown into
the geyser-tube influenced the interval between two outbursts generally
by increasing it, and gave rise to augmented violence in the outburst when
it came, the stones being projected back along with the water, and rising
much higher than the latter, as might have been predicted from dynamic
considerations . Sir John Herschel suggest-ed an explanation of gersei^
phenomena, based upon modifications of the mechanism iong previously
proposed to account for those of intermittent springs. His explanation,
though tenable, certainly does not apply to all observed cases, and issearoely
likely to be the true one, because a much simpler mechanism has been
since pointed out : and it may be taken as certain that, in eiplainiog all
natural phenomena, the simplest is the true one. This was discovered
by Bunsen and Des Cloizeaux, who in 1846 esamined the geysers of Ice-
land, and ascertained the fact that towards the bottom of the tube of the
Great Geyser, at a depth of 78 feet from the lip of the basin, a thermo-
meter immersed in the rising column of water rose to 206° Pahr., or to
more than 50° above the boiling-point of water, under atmospheric
pressure only ; and these authors conclude that, as the flow of water which
replenishes the tube after an outburst causes the aqueous column gradually
to rise to the lip of the basin, the temperature of the water at the lowest
part of the column continues to rise ; and whether it receives its acceesiou
of beat from the sides of the tube or from jets of superheated Bt«am
issuing into it, no considerable volume of steam can be generated until
the boiling-point has been reached at the bottom of the column, as due
to its insistent pressure there, when a sudden and large outburst of
steam takes place, and the whole column of water is belched forth from
the tube, succeeded by the blowing-oft of the pent-up steam which ex-
pelled it, and with steam evolved from the column of water as it rises,
until that falls back to atmospheric pressure. The curious facts ascer-
twned by Professor Donny, of Ghent, that water absolutely free in^
combined air may be heated to even 275° Fahr. before it boils, and then
bursts into st«am explosively, have been appealed to as auxiliary to the
phenomena, but seem unnecessary, even were it certain that the water of
geysers is absolutely air-free. Were it so, however, there can be little
doubt that the rise in the boiling-point of such water, under atmospheric
pressure, would also take place in the same water under a head of 78 feet,
or equal to more than two atmospheres, and thus would still further aug-
ment the temperature at the bottom of the tube, and further increase the
yiolence of the outburst.
Mechaniam of Stromboli.
Bunsen is of opinion that the above is simply the mechamsm of the
Great Oeyeer ; but that to account for some of the minor phenomena of
the second, or Strokur QeyBer, some additional mechamsm, not videly
differing from that suggest«d by Herschel, may be necessary. Some of
the relatioDB which subsist between geyser-phenomena, as thus explained,
and those which he supposes to occur at yarious depths in the tubes of
active volcanic vents, have been well discerned by Sir Charles Lyell, and
are described in his ' Principles of Geology,' 10th edit, toI. ii, p. 220 ; but
he has not applied them in explanation of the rhythmic recurrence of the
outbursts of Stromboli. From Bunsen's explanation, as above sketched,
it follows that tho interval between two outbursts depends mainly on
three conditions — the depth and capacity of the tube, the rate at which
the water that fills it is supplied, and the rate at which heat, from what-
ever source, is transmitted to the water. 'Were these three all perfectly
constant, the interval between two successive outbursts would be always
the same, but it must vaiy, more or less, as any one of these three conditions
may be altered. Again, the duration of the outburst, or time occupied
in the expulsion of the column of water, and the height to which it is
sent, as well as the volume of the jet, depend upon the capacity of the
tube and the height to which the water rises within it before the blow-out
commences, and mftt therefore vary in time with these conditions. The
depth and capacity of the tube may vary secularly or be deranged sud-
denly ; the tempierature of the infiltrated water may vary, and therefore
the time of its boLJing under given conditions may alter mth the season ;
and the temperature of the sides of the tube, and of the steam blown into
it from fissures, must vary with the intensity of neighbouring volcanic
action whence these are drawn.
Before proceeding to connect the circumstances presented by Strom-
boli with the above facts in relation to geysers, it will be necessary to
adduce some facts in relation to the former, derived from personal obser-
vation.
In the latter part of the year 1864 I examined the whole of the Lipari
Islands, with the exception of Felicudi and Ahcuda, which the lateness
of the season rendered impossible. Starting from CSape Mellazo (SicUy)
in a "well-found" eperonala, with a crew of eight men, which I retained
throughout the voyage amongst the group of islands, I had the pleasure
and advantage of being accompanied for some days, and as far as Lipari
Island, Panaria, and Stromboli, by my friend Colonel H, Yule, B.E., well
known for his embassy to Siam, and recently for his noble edition of
Mai«o Polo's travels, and by various other works. Our landing at
Stromboli was difficult, from the high surf running in ; and after our
arrival the weather became so much more tempestuous as to detain
us there some time. We enjoyed the hospitality of Padre Capellano
GiuBseppe Bonsa, whose house is situated not far from the central parts
of the island, and whence a steep but not diEEcult walk leads up to the
503
Mr. E. Mallet on the
crater and to the highest point of the island. The statexnents which
have been made as to the relative heights of different points of this island
■ appear to be only derived from giiess, and are greatly in error, as I am
enabled to show, although I am not in a position to give heights which are
rigidly correct, my hypsometric mensnrements haiiug been made by
means of a single aneroid.
Diagram TCo. 1.
The pergola of Padre Banza'e house (marked A, Ragnun No, 1) wh
found to be 211 feet above the sea at St. Vincenzo, and the highest point
of the island (marked B) is 2843 feet thus measiu^d. Captain Smrth,
however, gives the height as only 2576 feet : this was probablv taken
by him by the usual nautical methods of triangulation, and if so, may not
be more exact than my own rough barometric measurement. The height
of the ridge overhanging the crater, marked C, was in like manner found
to be 1200 feet. We were enabled to clamber down from this over crags
of lava, whose irregular terraces and ledges were capped, more or less
deeply, with black volcanic sand, containing immense quantities of crys-
tals of augite, down to a point oi'erhanging the landward wall of the
crater, and at no great distance from its verge, from whence we witnessed
the phenomena of eruption. This point, marked C, I found to be 904 feet
above the level of the sea. I'rom this point the great, irregular, and
somewhat oval funnel-shaped crater was before us ; and looking seaward
the highly irregular walls bounding its edges sloped towards the sea, and
were united transversely by the sharp irregular edge or summit of the
mass of broken and in great part wholly discontinuous and angular
ejected fragments, which form a slope down to the sea, between the oppo-
site sides or jaws of the cove or reentrant angle in the coast-line called
the Scbiairazza. From the point where we stood this edge (D on Diagram)
was estimated by the eye and clinometer at about 300 feet below us ; and
the narrower width of the crater thus seen across at its brim I estimated
at from 300 to 400 feet. The form of the crater as described by Smyth
(' SicUy and its Islands,' p. 255) in 1824 was staled lo be circular, and
Meehanitm of Stromboli. 608
ita diameter about 510 feet. This statement con ooly be received aa
approximate, aa at that date the brim of the crater cannot have been
extremely different from what it was in 1864 ; and the bounding walls,
which are of material the greater part of which is as ancient as is the
island itself, can scarcely admit of its ever having been circular, or much
different from the irregular gulf it presented when I saw it. From our
position of observation, every thing around us was of the sable colouring
of black hiva and volcanic sand. We could not see with any distinctness
the fundus or bottom of the crater, a cloud of vapour issuing from its
bottom, and in places from its sides, nearly filling the cavity, and obscur-
ing the bottom even between the outbursts. This vapour smelted strongly
of hydros ulphuric-acid gas. At all the lower part, as well as I could
discern, the steep and solid walls of the crater merged into a very at«ep
funnel-shaped talus of loose materials, at the centre and bottom of which
was the aperture of the tube or " chimney " of the volcano. This has
been described by Hoffman as entering the funnel by three apertures.
Judging from the form of the column of steam, dust. Stones, <&c.,as seen
at the first moment of ejection, the aperture appeared to me to be a single
one, irregular in form, and with its longest dimension in the directiou of
the greatest width of the crater itself. Looking down from our position
over the foreshortened slope of black d^ria which plunged into the sea
900 feet below us, the two jaws of the Schiarrazza are seen to be com-
posed of huge broken-ofi beds of lava, which dip to seaward at various
depths below the surface ; these, partly by superficial decomposition,
partly by being covered with serpulie and corallines, are of a nearly white
colour ; and as we stood with the sun at our backs, the sea above these
beds, at either side of the Schiarrazza, on which the sun was shining, pre-
sented the most glorious tints, varying with the depth of tbe wat«r from
golden-yellow to the purest emerald-green, while between these, and look-
ing right dotvn over the black slope of debris, th^ deeper sea was of an
intense indigo, passing off into blackness. Nothing in the way of natural
colouring and wild outline combined could exceed the weird horror and
intense beauty of contrast when a burst from the volcano sent forth in
the midst its volumes of white st«am and dust, which, seen by the
reflected light of the sunbeams shining through it, appeared of every tint
of ruddy brown or blood-red. From what precedes, and by reference to
Diagram No. 1, it will be seen that the bottom of the crater-funnel can-
not be more than 300, or at most 400 feet above the level of the sea where
the tube or tubes enter it, and that the statement made by Mr. Scrope
(' VoieanoB,' p. 332, 2nd edition), viz. " the lip of the orifice at tho
bottom of the crater is some 2000 feet above the level of the sea," is
largely in excess of the truth. Were that a fact, the brim of the crat«r,
which is 300 to 400 feet above the bottom, would be situated within a height
of about 176 feet according to Smyth's measurement, or within about
300 to 400 feet according to my measurement of the hi^st igoint of. tW
504 Mr. B. Mallet on the
island, either of which is pbysieally imposflible. flTiiie «-e remained oti-
aerring, the outburst* from the bottom of the crater were found to be
very irregular as to time, rarying, aa timed by the watch, from a iDioiraum
of two minutea iuterral to a maximum of thirty minutes, and in one case,
after we had commeaced our descent, to forty minutes. I could not trace
a very distinct correspondent'e between the largeness of this interval and
the violence and volume of the outbursts following it, although the ten-
dency seemed to be to such a correspondence : and the dnnitiou of the
outburst was eertaiuiy greater as the iulerval between two was bo. At
each outburst a hnge volume of dust and small mati^rial, and with moiv
or less of large fragments of solidified lava, aU angular or subangular, and
with a few fragments and shreds of different sizes of tava still hot enough
to be slightly plastic while falling, were ejected ; none of the fragments
were of any great size, none appearing to exceed in weight about 500 or
600 pounds, and none of the pieces of plastic lava reaching half this
weight. The light wijid blew from us towards the sea, out over which
a portion of the finer dust was wafted after each outburst ; bat the great
mass of the dust and fragments, whether small or large, fell back into
the crat«r upon its bottom and steeply sloping funnel, a few only, and
generally of the iargest fragmeuta, being thrown out over the crest of the
crater at its sea side, and landing amidst the deliris of the elope, down
which they clattered. It was obvious that the orifice of the tube at the
bottom of the crater was greatly obstructed by the loose material forming
the funnel above it, which seemed after each outburst to be continuaUy
slipping, more or less en ituute, and so blocking up the tube, along with
the mass of ejected material which dropped hack upon the orifice ; for
it was easily remarked that successive outbursts apparently took place
from different points, distant occasionally some yards from each other, in
the bottom of the crater — the main axis of the column, or ita greatest
thickness, varying thus in position, and also more or less diverging
slightly from the vertical, sometimes one way and sometimes another, as
though the ajutage of discharge was through loose material of partly
large and entangled blocks, mixed with finer material, the positiona
of which were more or less altered after each discharge. None of
the large fragments which we saw thrown out rose higher than the posi-
tion at which we stood, and few even bo high — that is, they did not rise
more than 400 to 500 feet above the orifice at the bottom of the crater;
but occasionally the height of projection must a good deal exceed this, aa
I found many angular fragments and large shreds of lava, which bad
fallen in a leathery or plastic state, to the landward and eastward sides of
the brim of the crater, 150 feet or more above the level of our point of
observation. The black sand and dust and crystals of augito are found
in large masses still higher and further from the crater on the land side;
but much of the latter are blown inland by the strong winds from the
northward that prevail in winter. The solid mural precipices which form
JUeehamtm of StromboU. 505
the walls of the enter above the funnel of loose material consiBt of beds
of Bolid lavas and agglomerated fragments, and appear to dip more or less
towards the sea, or away from the centre of the isUnd, and were no
doubt formed by one of its great early and more central craters at a period
excessively remote. Svffioni of steam isaiie in some spots from between
these beds, and the percolation of water waa seen in places not far below
the brira of the crater. There is a perennial spring of percolated water
much higher *up upon the island, and under the steeps that mark the
posit ion of an ancient crater, so that it is highly probable that rain-water,
in greater or less quantity, finds its way into the funnel, and even the
tube, of the volcano, although the percolation of sea-wat«r is no doubt
the chief source of the supply, which is blown out as steam, and perhaps
in part as pulverized water. Each outburst, while we continued to
observe them, was preceded by several distinct low detonations, with in-
tenals between each of from 4 or 5 seconds to as much as 80 seconds :
these, though of a far deeper tone, greatly resembled the cracking
noises that are heard when steam is blown into the water of a locomotive
tender for the purpose of heating it. These detonations sensibly shook
the rock beneath our feet.
The outburst, when it comes, does not rush forth quite instantaneously
or like that of exploded gunpowder. It begins with a hollow growl and
clattering sound of breaking or knocking together of fragments of hard
material, which very rapidly increases to a roar at its maximum, continues at
about the same tension for a period varying from a few seconds to a minute
or two, and then rapidly declines, but less rapidly than the augmentation
took place. At the lirst instant of the outburst, the rock on which we
stood was very sensibly shaken, the vibrations being both vertical and
more or less horizontal ; at the end, and after the fragments have ceased
to fall and the dust has cleared away, all tension of vapour in the tube
seems for the moment at an end, uid the funnel 'A seen filled merely with
rolling clouds of vapour. The noise produced by the outburst is not very
loud, and more resembles that of the rush of a heavy railway-train over
an iron-^rder bridge, when heard at some distance off, than any other
sound to which I can compare it, but more fluffy and flat. Ou examin-
ing the existing surface of the island, it is easily discerned, by an eye
educated to the observation of extinct volcanic r^ons, that successtTe
craters have been formed, shifting their positions posterior to the pro-
duction of that great and nearly central one from which the main mass
of the island was thrown up. The existence of three such craters may
be traced ; and the existing little crater is situated at the landward or
south-eastern side of a vastly larger crater, all the north-western or sea
side of which has been destroyed and buried in deep water, and of which
the heavy beds of lava seen under water at both sides of the Schiarraraa
are the only remaias to seawards of the existing slope of d^ris. This is
represented by the Diagram No. 2, copied from my note-book, in. mtisfci.
506
Mr. R. Mallet on the
the diagoaally shaded portion represents an ideal eectioD of the ibLmd »
it now staads, taken through its highest point and the existing crater at
Stromboli, while the lines beyond indicate the probable outlines of the
island when the gruat crater was active, of which the Stromboli of to-dajr
may be viewed as Uttle more than a famnrole.
Diagram No. 2.
I way add here, in reference to the Lipan group generally, that all the
islands present more or less distinctly these chanicf en sties of craters
whose axes have shifted and formed new ones at imtneusely ancient
epochs, and with vast intervals of time intervenmg
The entire group presents, though in various degrees m the different
islands, the general character of great decadence of a once far more
powerful volcanic activity ; and, in every case, as the cone, or rather mound,
of each island increased in mass and height, the original vent thus in-
creasingly obstructed tended to move off and open new and easier venta
in directions approaching the coast-lines, just as in the ca«e of very old
and massive volcanoes on land, such as Etna, migrations have occurred of
their most ancient great craters, and, in more recent times, new ones have
opened low down upon their flanks, such as Monte Bosso &c. The epoch
of primordial activity was far from contemporaneous in all the islands ;
»nd we find in them now the most varied stages of volcanic decadence.
In the island of Vulcauo, we have an empty crater of enormous capacities
and depth (1100 to 1200 feet), the bottom of which reaches to within a
few feet of the eea-level, and is only separated from the shore-line at the
north-east of tie island by an extremely steep bank of compact tufa.
The oldest craters having been situated much more centrally and far to
the south-west, while the little crater of Vulcanello was thrown up to
seaward of the ancient coast-line and between it and the deep crater just
spoken of, boiling springs and boiling streams of superheated vapours
issue below the sea-water, and a thermometer sunk amongst the pebbles
of the beach in many spots rises to above 300° Fahr. In the bottom of
the deep crater the principal " bocca," which is several feet in diameter,
And though only blowing out superheated steam and goaes with a men-
Mechanism of Slromboli. 507
Hured Bort of rise and fall in its snorting, is red-hot to the lips, which
are of hard lava ; and the temperature at the mouth I found, in 1864,
was sulficient to melt brass wire, but not sufficient to fuse a similar wire
of bronze (i. e. copper with about 5 per cent, of tin).
The fftlling-in of any eonsideroble proportion of the walls of this grand
crater, which, on the landward side, consist of nearly horizontal beds of
volcanic rock and conglomerate, forming at that side a vast mural preci-
pice, though almost wholly of compacted tufa for the remainder of its
periphery, would easily gire rise to a renewal of volcanic energy, such
as nowhere exists now in the Lipari group.
Stromboli is the nest to this in existing energy ; but though the per-
sistence and character of its activity excite much more attenttOD, the
actual evolution of volcanic heat is greatly inferior to that constantly going
on from the unobstructed " bocea " of Vulcano, which, if again obstructed,
would produce very violent effects. In lipari Island we have the traces
of several great craters of extreme antiquity, the most recent being that
which evolved the mountainous masses of pumice and the enormous
stream of pumice and obsidian which falls into the sea at the north-east
of the island ; but the greatest sign of present activity is found on the
shore at the opposite side of the island, at II Stufl, where innumerable jet«
of hot w^ter and superheated steam with sulphurous acid issue from the
heavy beds of trachyte, which they rapidly decompose and convert into
clays and hyaLte.
In others of the islands, such as Fanaria and Saline, no sign of activity
remains, and the most practised eye with difficulty seeks to recover the
positions or outlines of the very ancient craters. Lastly, in the small
islands of Dasiluzzo, in the low rocks of Liscanera and Liscabianca, and
in the huge spire of Datola, formed of vertically parted and splintery
trachyte of the most obdurate character, we have but the last shreds of
one or more great volcanic islands which once occupied the shallow sea-
spaces between all these islands, and probably connected them into a
single vast cone. A hot spring still rises in water of 4 or 5 fathoms
deep between Liscanera and Liscabianca, which possibly mark the site of
one of the moat recent of the craters at this spot, the islands which they
formed, at a period too distant for imagination, having here almost disap-
peared under the eroding influence of the comparatively tranquil aud
tideless waters of the Mediterranean, aided perhaps by local subsidence,
but of which there is little or no evidence. It will thus be seen that the
change in position and decadence in energy ascribed to the existing crater
of Stromboli, although for 2000 years its energy has seemed to be constant
or not greatly diminished, are circumstances in complete accordance nith
the facts presented generally by the volcanic islands of the whole group.
The existing tube of Stromboli, like that which leads to the " bocca " of
Vulcano, has but a lateral and indirect and very much choked-up com-
munication with those great central ducts which oas» ^^^ -^vtA. 'vra
BOS Mr. B. Mallet en the
the products of the great craters. Lava from these, genenkUv imp«r-
foctly melted, but occaaionally in a coroflete st-ate of fusion, still finds ii»
way from these into the upper parts of the existing lube of StromboU.
but in comparatively very small quantity.
On leaving St. Vincenzo we circumnavi^ted the island of StromboU,
nnd examined the slope of debris in Schjarrazza cove : the actual average
angle of slope is much overrated by Mr. Kcrope at 50° ('Volcano*,'
page 32). By the clinometer it proved to be from 34° to 36° with the
hori7X)ntal. The slope consists almost wholly of angular fragments,
averaging but a few hundredweight each, and of shreds and tails of lata
that have fallen in a semifused condition. Mixed with these, in a wholly
irregular manner, are here and there siauouH and twittted flakes of lava.
These have been oft«n taken for dykes of lava forced out by hvdrostatic
pressure through the bank of debris, when the crater has boen assiuoed
brim-full of liquid lava; but I am not aware of any endonce whatever
in support of the notion that this crater ever has been so fUled. It*
steep walls present no traces of the contact of liquid lava at any time
eaatx their formation ; and it can scarcely be doubted that had the crater
ever been filled with liquid la^-a to the brim, the loose and incohereut
slope of dobna would have boea utterly uuuhle to sustain tho protaure,
and must have been forced bodily into the sea, into which tbb mass of
liquid lava must have followed it. The base of the slope appears to con-
sist of solid and, no doubt, comparatively water-tight beds of lava, like
those described, as seen from above, at both sides of the Schiarraaza ; and
but for these the existing crater could have never been formed, or its
activity preserved, for it must have been drowned out by the inroad of the
sea, as so many other and recent craters in the other islands prove to
have been. The sinuous masses of lava seen at various parts of the slope
of debris appeared to me no more than huge splashes of very liquid lavs,
which, in outbursts of greatly more than usual intensity (such aa was one
of those witnessed by Hofiman) and with a larger supply of lava than
usual, were blown out over the crest of the slope and fell amongst the
blocks of debris. Fresh deposits of debris obscure the features of most
of these plashes ; but I observed, in some cases, that the lava had distinctly
moulded itself, like a mantle, to the sinuosities between and the forms of
the blocks upon which it fell. Within a yard or two of the base, or
water-Une, of the slojie were tuo blocks of ltcv& of exceptional magnitude,
the larger having a volume of 8 or 10 cubic yards. These blocks wwe
confidently affirmed to us to have been projected during some violent
burst forth and thrown clean over the crest of the slope, and to be in fact
bloet rtjelit thrown from the bottom of the crater ; examination proved
that they could be nothing of the sort. They were sharply angular, and
all the surfaces had the crystalline texture of dark pyroxenic lava ntrt
very long fractured, except in some places, where distinct signs of wea-
thering were evident in tbe larger block. Had they been bloet rgeUt
Mechanian qf SlromboU.
509
thej would lUTe presented on all their surfaces and edges the more or leu
rounded outlines and eitreme induration and closenesB of grain due to
long-continued torrifaction, which are the invariable characteristicB of such
blocks. The true history of these great blocks is, that they had been
detached by the shakings of the outbursts from one of the steep cliffs of
the ancient crater-walls which overhang the crests of the slope, and had
thence rolled down to the position in which we found them at about F in
Diagram No. 3, which is a section of the slope of debris and of the sea-
bottom in line extending from its base. In this line we took a few sound-
ings at distances from the water-line at the base of the slope, which we
had to guess. These distances, as guessed by me, exceeded those guessed
by Colonel Tule, though not very greatly ; and I have preferred to adopt
those derived from his military experience in guessing distances t^ the
eye rather than my own.
Diagram No H.
It will be seen from these soundings that the statements made by the
islanders, and wroi^ly attributed to Captain Smyth (see his ' Sicily ' in
loco), that the sea outside Schiarrazza cove is unfathomable, and hence
swallows up the d^ris of mora than 2000 years, is wholly erroneous.
Indeed8myth'ssoundings('SicilyanditBlBlands'),aB well oa the Admiralty
Chart, sufficiently indicate that for some miles in the offing here the
Mediterranean does not exceed 100 fathoms in depth. The bottom along
which I took these soundings consists of huge irregular and ovoidal
masses, of 10 to 20 tons in weight, of volcanic rock, old and water-
rounded. What, then, does become of the d^ris ? Its quantity, in reality,
is extremely small in a given time. A very large proportion of it consists
of mere dust and glassy or angular lapillEe, and these, if blown seaward,
hil at a considerable distance away, and are lost in the depths ; those
which &tU nearer, including the fragments th&t totm \!ti& v)«tMisa 111&B& <fi-
510 Mr. R. Mallet on the V
the slope, ue slowly r^mov^d and carried out iuto deeper vrat^r br Iti^ -
uodur ton of the heavy ee&s in winter, sod are loet in the cUnks and
cre*ices between the huge blocks at the bottom, which I found to be m
deep &nd tortuous as often to render the extraction of the BOUDding-Ipad
wiiich bad entered tbem difficult. The lara ejected by Stromboli, whelluT
in the floUdified or half-melted state, is eitremelr dark-coloured, ktaost
black. It IB highly pyroieuic and crystalline, and its fusibility is greatly
in<:re&sed by an intin)At« iutennisture of d&rk obaidianii: g:las9, of which
portideH as well as Hlrings are met uith ererywhere. It is still lastjtnr
or plastic at a temperature considerably below a rc-d heat, risible in day-
light, and is probably in tolerably liquid fusion at a temperature not
much exceeding 1200° Fahr. Ita compoaitioo is by no tDeotis invariable.
BB may be seen on the slope of dftnis ; and when the glassy material ia
very abundant, as from time lo time secma to be the ease, or from
any of the cauMes which inHuence periodically the flticluations of t^mf*-
rature more or leas observableat all volcanic vents, this lava would become
extremely liquid and be blown about by the outbursts in the way some-
what obscurely described by Hoffman, as well as urged in liquid flaken
over the brim of the crater, Thecrystals of augitv which are deposited
ill such abuiiJaiK'i,' with the dust blown out may preexist in the lai-a, but
appear to me, more probably, to be mainly formed by the disintegration of
the hot lava by contact and churning up with water, under a considerable
pressure and therefore high boiling-point, and perhaps by separation and
recombination from solution of its constituents. The crystals, which
are often an inch or more in length and frequently macled or cuneiform,
have scarcely any lustre ; and when the surfaces are closely examined n^th.
a lens, they aro oft«n seen to be minutely pitted with microscopic cavities.
We now come to collect and correlate our facts and draw such conclusions
as they warrant iu explanation of the mechanism which produces the
phenomena of Stromboli. The supply of wat^r producing the immense
volumes of ateam constantly blown off at the rate, on the average, of three
or four outbursts per hour may be derived in part from percolated fresh
water ; but this source alone, derived from the small gathering area of
the island, would be wholly insufficient; and, were that the sole source, it
would almost wholly fail towards the end of the dry season, so that a
marked annual change in the volcanic phenomena must result, and could
not fail to be observed. The supply of water, honever, is manifestly
regular, and very nearly constant at all times, and therefore is derived
from the sea, and thus must enter the tube «f the volcano below the sea-
level^that is to say, more than 400 feet below the lip of the tube at the
bottom of the crater-funnel. Whatever be the source of supply of the
lava, therefore, it can never fill the tube as a solid column of melted mat-
t«r reaching up to its lip ; for in that case, whatever be the mechanism
of the volcano at each outburst, the whole of this immense column of
melted matter of more than 400 feet in height must be blown completely
Mechamna of StromboU, 511
out of the tube, which actually is emptied, at the end of each outburst, of
evervthiog but gaaes and vapours, and these at a tension not greatly ex-
ceeding that of the atmosphere. We do not know the average section
of the tube, and therefore cannot calcuhite the-volumeof tavathat would
be propelled thus out of the tube, if previously filled by each outburst ;
but it is manifestly so great that it would wholly change the character of
the phenomena exhibited by the Tolcano, and must, during the last 2000
years, have produced a mass of ejected matter of enormous magnitude
instead of the insignificant amount of mixed lava and debris which alone
are to be seen.
Liquid or semiliquid lava does, however, continually make its way into
the bottom of the crater-funnel and amongst the fragments collected there,
which it more or less solders together, and along with which it is blown
out at the outburst. Some may ooze into the tube lower down, and may
more or leas obstruct, but can never completely fill it. The walls of the
tube, and those of all the fissures or cavities below the level at which the
more or less fused lava reaches them, can scarcely have a lower tempera-
ture, and are most probably at a higher one than the lava itself. If the
tube of the volcano were the main, or only, ajutage through which the
liquid lava, as well as the steam to blow it out, were supplied — if, in fact,
the tube were the main duct into the lowest depths of which both the
liquid and vaporous matters entered — then, at irregular intervals, the tube,
and even the crater, must become filled, and the whole phenomena of
eruption would not differ in character from the highly irregular paroxysmal
efforts of any common volcano of like energy. The tube, then, here
plays a different part from what it usually does, and constitutes an addi-
tional element in its machinery, upon whose action in producing expulsion
the rhythmical recurrence of the outburst depends.
We can now discern the very simple mechanism by which the actual
phenomena are produced, a description of which will be rendered more
intelligible by reference to the ideal Diagram No. 4, in which A is the
lower part of the funnel of the crater, filled more or less with the frag-
mentary mass which has fallen back into it from the preceding outbursts.
B is a lateral duct conveying more or less liquid lava into the bottom of
the crater. C is the tube leading to the bottom of the funnel from a
depth considerably below the sea-level, supposed to be, at the line L, at
about 400 feet below the upper lip of the tube. D is a duct communica-
ting with the sea, and enabling sea-water to find access to the interior of
the tube, and to rise therein^if otherwise unimpeded, to the aea-level.
E is either a lateral duct or a continuation of the tube itself, through
which steam at a high temperature and tension enters the tube at some
point much below the level of the sea. The lava- and steam-ducts, B
and E, may be supposed to come from the ancient great volcanic channels
still remaining under the more central parts of the island, and which
supplied its great ancient craters. The duct D may consist of manY
All of the three ducts, £, G, aD<
vaHed to ahntrnt any extent, provic
poaitions, And these only within
Diagram No. 4. Suonosinn »- —
Mechanism of Stromboli. 513
d^ris shall have some sort of landing-place and support for the l&i^r
portion of the mass, ho as not all to drop into and permanently block the
tube. The lava oozing from the duct, or ducts, B, escaping amongst these
fragments, solders them more or less together ; and in proportion as its
rate of supply is greater or less, some of it may overflow and drop, in a
more or less liquid stat«, into the tube C and into whatever water it may
contain. The tube, however, is emptied at the outburst of nearly all
that it contains, and the tension therein being that of the atmosphere, or
little more, the sea-water again begins to fill it by the ducts D. This
water is already probably considerably warmed in the d,uct« D ; it receives
accessions of warmth from the sides of the tube and from the continual
blowing into it of superheated steam and vapours through the ducts £,
whose temperature is probably not far different from that of the lava at B.
The column of sea-water rises in the tube to a level, we will suppose S, by
which time the boiling-point has been reached at the lowest point of the
column, namely, that due to the stetical head of water, and to all such
obstructions above the lip of the tube as tend to hinder the escape and
so increase the tension of the vapours and gases occupying the otherwise
empty upper part of the tube. At such on instant, the whole column
may be lifted through a few inches or feet vertically by the steam locally
generated at the bottom of the tube ; and as this incipient evolution of steam
escapes upwards the whole column of liquid will be suddenly dropped
back upon the bottom of the tube, to be again similarly lifted, and so on
until every portion of the column of water has acquired the full boiling-
point due to its depth, Ac. This is the cause of the detonations heard
before the outburst. As soon as this has been reached, the whole mass
of water below S is driven violently upwards, and partly by its impulse,
but mainly by actual steam-tension, drives before it the mass of obstructing
matter filling the bottom, of the funnel at A, and the whole is driven
forth together in a mingled cloud of dust, stones, shreds of half-melted
lava, steam, and pulverized water. When the tube is left empty, and
after the fall back of the fragments, the whole apparatus is ready for a
repetition of the process. It is obvious that the depth of the tube below
the level of the sea, and the temperature of its sides and that of the
steam entering at £, determine the force of the outburst, that the rate
of supply of water and steam determine the intervals between the out-
bursts, and that the proportion between the volume of steam and that
of pulverized water, at each outburst, depends upon the capacity (that is,
the greater or less section) of the tube C. If that be narrow in proportion
to its total depth, as is probaBly the fact, then very little water will be
ejected in any state but that of st«am. It is not necessary that the
temperature of the column of wat«r in any part of the tube G should
ever reach the tension due to a temperature equal to that of the lava
escaping from B ; it only needs to be such as shall raise it« own column
to the lip of the tube and overcome the obstructions there encountered
with ft sufBdent residual tension left to blow tbmft & ^[KAite'E <n \•!Aft^liet^^^
51-i Oh the Mechanism qf Slroniboli.
into the air. The «ugite tTyotals are probably formed within the tnbe,
from small portiona of lava dropping la a liquid state into the wat*r it
contains,
Bfverling uow to the remarks mad(- at the beginning npon the relation*
trnditionally Bind to exist between the phenomena of tliis -volcano anil
the state of the weather. It ia obvious that the notions of nieely balani'wl
equilibrium in a tube always filled to the lip with liquid lava can no
more act^ount for any such relation with the weather thau it can exploiji
the rhythmical recurrence of the outburats themBelves ; and if euppused
relations with changes of weather, as alleged to be indicated by Stromboli.
could be thus explained, every constantly active volcano in the world
would be equaUy a " weafher-glaas.'' Kilama, for example, mnst present
upon an o.vaggerated scale all the weather-prognostics attributed to
Stromboli. In examining the v^ue statements mado upon thia subject,
we should hear in mind the extreme incapacity of ignorant peoples to
observe phenomena with accuracy, their proneuess to exaggeration, and
the readiness with which they accept traditional statements, however
improbable. The statements made to me by several of the more intelU-
gent people of Stromboh as to the height to which stones were alleged to
be thrown, viz. far above the highest point of the island, as to the filling
of the crater hri Ill-full vith liquid kv.i (wliii Ii. b<i«i-v^r. no orn.- had ;iftu:illv
himself seen), and the forcing through the slope of deTiris of vertical dykes
thereof, as well as the projection of the huge blocks we saw at the bottom
of the slope, and such hke, should be home in mind before we attempt to
square theoretic views with statements of facts that probably have no
real existence. The only intelligible statements that I could gather from
the inhabitants of Stromboli as to relations between the weather and
their volcano resolved themselves really into two propositions : firat, that
in fine weather the light reflected upwards from the crater was more
brilliant, and apparent at a greater distance, than in windy or uncertain
weather ; secondly, that in cold and broken weather the light waa dimi-
nished, and a heavy cloud of vapour hung more or less over the crater.
These are intelligible facts, and admit easily of being accounted for on
well-known meteorological principles. A tendency, though not a marked
one, to the production of sea- and land-breezes in the morning and even-
ing is observable in these islands, the sun-heat during the day being
often very great, as alao the nocturnal radiation. These, taken in con-
nexion with the prevailing direction of the wind at a given time, vii.
whether it sweeps over the island and over the highest points from the
southward and eastward, or blows against its steep north-western feee
and into the crater, will, by altering the state of the atmosphere above
the latter, tend to produce changes both in the light and in the vapour'
cloud of the volcano. But that there is any real connexion, in the way
of direct cause and effect, between the energy or frequency of the out-
bursts and the state of the weather, or fluctuations oi barometric presaure,
or vice versd, seemB de\oii ol «fi^ ^ovmiB.'nnQ.-vta.tftTer-
On Omneetive Tissue, Nerve, and Muscle. 515
" A Contribution to the Anatomy of Connective Tissue, Nerve,
and Muscle, with special reference to their connexion with
the Lymphatic System." By O. Thin, M.D. Conmiani>
cated by Professor Hoilet, Sec. R.S. Beceived April 22,
1874*
I pnblialied in the ' Lancet ' of the 14th February of this year a paper
entitled " On the Lymphatic System of the Cornea," in which I endea-
voured to show that the canals in that structure in which the nerves lie
communicate with the lacuna), that the straight canals and lacunte are
connected by means of a continuous layer of flat cells, the margins of
which are indicated by the well-known action of nitrate of silver, and
that these cells are not the anastomosing so-called comea-corpuscles, but
that the flat cells line the lacuna, while the branched cells fill the cavity.
I have lately undertaken a series of further Investigations on the same
subject.
In order to corroborate the results yielded me by the nitrate of silver,
I availed myself of the well-known property which hiematoxylin pos-
sesaes of specially staining the nuclei of cells. I allow the cornea to
remain in the solution until it is perfectly saturated. Subsequent mace-
ration In acetic acid removes the luematoi^tin from the fibrillary sub-
stance before it bleaches the nuclei. On comparing a cornea so treated
with successful preparations of the comea-corpuscles as obtained by
chloride of gold, it is fouud that the number of cells demonstrated by
the hfematoxylin exceeds by several times that found in the gold prepara-
tion, affording direct proof of the existence of other cells in the cornea
than those known as the comea-corpuscles.
If a vertical section of the cornea is so treated by hematoxylin and
acetic add, in many of the clefts in the fibrillary substance, in which, as
is well known, the comea-corpuscles are situated, several nuclei are seen,
proving in another way the existence of a greater number of cells than
those hitherto accepted by anatomists.
But in addition to the proof afforded by staining the nuclei of the
cells, I have, by the application of a new method, been able to isolate
(and thus demonstrate beyond all further possibiUty of doubt their exist-
ence in the cornea) a large number of cellular elements, the varied size
and shape of which distinguish them not only from the comea-corpuscles,
but from any anatomical structures that have been as yet described.
If a cornea is placed in a saturated solution of caustic potash, at a
temperature between 105° and llo° Fahrenheit, it is reduced, iu a few
minutes, to a white granulated mass of about a fourth of its previous
bulk. In a small piece of the diminished comea, broken down with a
needle and examined under the microscope in the same fluid, it is found
that the only visible elements are a great number of cells. If the con-
•Scad June IS. 1874. SMantl.^.^n.
TOL, xni, 4 -a.
516 Dr. G. Tliin on the Analomy of
jundiTftl epitheliiun of the comca hae not been previoaely remored, lb*
cells o£ that structure cau be recognized amongst the others ; and if tha
mass under eiamination has not been too much broken up in manipii-
lating, groups of them may bo aoeu in direct anatomical continuity with
Icmg narrow flat cells, which belong to the elements that have been for
the first time brought to light by tho potjish solution.
But the cells of the anterior or siirfoce-epithelium form a very Bnull
proportion of the number. The sniaUest piece that can be removed by
the needle frwm a cornea which, before being put into the solution, haa
had this epithelium scraped off and Deacemet's membrane remored, shows
nnder the microscope a multitude of cells. Of the branched corpU9c3e»i
the fibrillary substance, and nerves, not a trace ia visible.
The form of these cells ia so various that it would be difficult to con-
struct a. scries of types under which every individual cell could 1»
brought. They seem in their development to have assumed any modifi-
cation of form that ia necessary to enable them to fit accurately tb*
cavities and fibrUlary bundles to which they are applied.
Those whose outlines do not permit their being accurately described as
belonging to a strictly defined type, are many of them somewhat qiu-
draiiguiar or triangnlar in form, or club-shaped, with a short or long
projecting process. Of fixed niid iHlnite 1\-po>J are Jong narrow rod.*,
ending obliquely at the point, and oblong cells intersected at one end by
a notch, which receives the extremities of two of the long cells tbalt lie
parallel to each other.
I do not attempt to give an eshauBtive account of the varioiu fonu
aasumed by these ceUs. A better idea than can be given by any dfr
scription will be got by an examination of figs. 1, 2, 3, Plate TUX, bt
vhich many of them are represented ; but an examination of the first
prepared cornea will show that there are many forms and modiflcatiail
which have not been drawn.
The cells are granular in appearance, with sharp clear outlines. The
terminal surfaces of the long cells can often be seen to be finely BOTTBted ;
and so closely do they fit each other- at these points, that sometimes a
high magnifying-power is necessary to^ discover the suture-like line by
which the junction is indicated.
The nuclei of all the cells have nearly the same length, but in tiie
narrower cells the nucleus is oft«n much compressed transversely.
The long cells are many of them OOQ millim. long and from 0'006-
0-003 nuUJm. broad ; the shorter cells are broader. Those 0-06 millim.
long are generally about 0-009 millim. broad. A length of 039 milliiiin
with a breadth of about 0-015 millim. is common ; others are 0-03 milliffl.
long and O'OIS millim. broad.
I hare chiefly examined the cells in the cornea of the ox, sheep, and fro^
and have found no important differences either in shape or arrangranetit.
In ezamining ^rtioiu ol t^« cotroaa ^frUch. hare been as little dif
Connective Tinue, Nerve, and Mtucle. 517
turbcd as ie consistent vitfa the nutintenaQce of traDsparency, groups of
cells are found massed together ih sttu, as they have been left hj the di»<
solving out of the fibrillarj aubetuice by the potash; these are found
chiefly in tvo forms, TransTerse tnasses of the anterior epithelium are
found sutured to long narrow cells, which sometimeB seem to join them
at an angle.
Further, flat quadrangular masses of a single layer of cells are found
formed in the following manner : — Of two opposite sidee the external
rows are formed of more or less rounded and angular cells, to which are
joined long narrow cells that lie parallel to each other. Those from each
side respectively meet in the centre, where they join. The remaining
sides of the quadrangle are formed by a side view of these vaipeus cells,
where they have been detached from the adjoining ones in the breaking
down of the cornea mass.
The coincidence between the breadth of the long narrow cells and the
fibrillary bundles of the cornea-substance, as seen when prepared by the
ordinary methods, is evident, the continuous planes formed by their junc-
tion indicating that they form layers between which it is enclosed.
According to this view, the ground-snbstance is everywhere encased in
a sheath of cellular elements.
Bowman's corneal tubes I believe to include both the straight canals
described in the paper above referred to and the spaces between the
long cells widened by injection, chiefly the latter.
Although I have nothing to add to the description of the mode of pre-
paration which I have already given, I must state thatthere are conditions
of success, as to the nature of which I have not yet come to a definite con-
clusion. Sometimes the same solution, applied at the same temperature
to different comece, succeeds in one and fails in another, and sometimes
a solution prepared with every precaution has failed to afford me any
result. The two essentia conditions to' success are complete saturation
and temperature. I have never succeeded with a temperature above
120°, nor with one below 102° ; and so sensitive is the solution to mois-
ture, that preparations sealed in it with asphalt seldom keep longer than
one or two days, except in rery dry weather. On a damp day I have
known a successful preparation left on the object-glass disappear in six
hours. The c(»neal mass may be kept unaltered for at least some weeks
in the solution by running sealing-wax round the stopper of the bottle,
A perfectly successful preparation shows nothing but the cells. Un-
successful preparations, especially those prepared with too hot solution,
show globular masses unlike any anatomical element ; others, especially
those prepared at too low a temperature or with imperfect saturation,
show masses of hexagonal crystals like those of cystin.
To sum up, I believe that there exists in the cornea : —
I., the fitnillary ground-substance, which is pierced by straight canals
and honeycombed with csyitiee ;
51*8 Dr. Gt. Thin on the dkatm^ ^
XL, ist cells, which evexywheie cover flia' fibrilhurjr bandka of Ab
former and line the entire system of the latter ;
I£L, the comea-corpufldes of Toynbee and Yiidunr ; and,
iy.y the nerve-structures of the tissue.
The cornea-corpuscles and the nerves lie free intbeoanab andeavitis^
and between them and the epithelium there is a fluid-filled apaoe irUch
permits the passage of lymph-corpusdee.
It is therefore proper to r^ard the canals, cavitjes, and intw^
fibrillary spaces as forming a continuous and integral part of the lyoh
j^hatic system, the latter having to the fdnner the same rdatioa tint
blood-capillaries have to the veins.
The junction of the flat cells of the flbriUary subBtanoe iviCh die
epithelium of the surface justifies the inference tiiat the interoeDiiltr
spaces in the anterior epithelium of the cornea omimmuoate with die
lymph-spaces in the ground-substance, and that tiie position of nene-
fibrilla between the epithelium is a continuation of the Bimilar nlatioa
that has been demonstrated in the substance of the structure.
#
It is a reasonable hypothesis that what can be definitelj eataUished
for the cornea holds good for the other forms of connectiTe tisane.
I have accordingly submitted tendon to an examination bj differsnt
methods, with the view of obtaining evidence of the existence in tiist
structure of cells other than those arranged longitudinally between the
bundles, the nature of which has lately been carefully investigated bj
Boll, Spina, Ranvier, and others.
If the tcndo Achillis of a frog, or the tendons of a mouse's tail, fixed
according to the ingenious method described by Ran\ier in his first
paper*, are treated by nitrate of silver, care being taken to avoid friction
of any kind, it is found that every part of the free surface of the bundles
is covered by a continuous epithelium. In the tendo Achillis of the frog
I have seen lymphatic capiUaries distributed over this surface ; and the
epithelial markings can be traced from the cells covering the bundles
into those of the vessels. A preparation from the tail of the mouse,
showing this epithelium, is represented in fig. 4, Plate IX.
If sections of tendon are placed for several hours in a strong solution
of extract of logwood and alum, and the dye then washed out bv concen-
trated acetic acid, it is found that while the fibrillary substance becmnes
clear and transparent, the nuclei retain their colour. This is best done
under a cover-glass and under the microscope, as the effect of the add,
if kept too long in contact with the preparation, is to discolour the
nuclei also ; the weight of the covering-glass is sufficient to prerent the
otherwise invariable distortion of the preparation by the acid. If the
preparation is intended to be permanent, all traces of the acid must be
removed bv a current of distilled wat-er.
The effect of this treatment is to show that there exists in tendon a
* Archives de Physiologie, 1869.
Connective Ti»»ue, Nerve, iotd Mutcle. 610
£ar greater number of cells than can be seen in the most sncceesful gold
preparations. The figures illustrating the structure of tendon usually
given by investigators account for only aportion of the cells whose exist-
ence is thus proYed — that portion, namely, which consists of the rows of
cells occupying the stellate spaces, and which colour easOy in gold and
carmine. In longitudinal sections, prepared by the method I have above
deacribed, not only are the nuclei much crowded together, but two are
frequently seen on the same level, and applied to the opposing surfaces
of contiguous bundles. In transverse sections a similar arrangement
is found. The nuclei between the bundles are very numerous; two are
often found together on opposite bimdles ; and in one stellate space three
and four nuclei can often be found at the same level.
This is clearly a condition to which the so-called division of the
nucleus is not applicable.
If we believe that each of these nuclei represents a cell, the
conclusion is inevitable that, in addition to the cells hitherto de-
scribed and occupying the centre of the stellat« spaces, thei« exists
another and very numerous class of cells applied to the surface of the
bundles.
This effect of tuematoxylin and subsequent action of acetic acid on
sections of tendon is perfectly analogous to that similarly produced in
sections of cornea.
The treatment of tendon by the potash solution has seldom yielded me
satisfactory results ; but when it has succeeded, I have found confirmation
of the inferences I draw from the effect of the saturated solution of
htematosylin. A reference to figure 7 (Plate IX.) shows that while many
of the cells isolated by the potash correspond to those found on the sur-
face, others are similar to the long narrow cells that cover the fasciculi
of fibrillary tissue in the cornea, and do not resemble in shape, even
approximately, the superficial elements defined by nitrate of silver. Al-
though I have not succeeded, as in the cose of the cornea, in reducing
tendon to a mass of these ceUs, I consider it a fair inference that the
long narrow cells I have seen are samples of cells that invest the fas-
ciculi of fibrillary tissue.
The comparative difficulty in successfully treating tendon by potash
is probably due to the denseness of its structure.
It is in regard to the branched cells, which I hold to be the analogues
of the branched eomea-cells (corpuscles), that the important fact demon-
strated by Spina, that it is on the surface of the cells that the fibres of
elastic tissue are formed, specially applies.
In the centrum teudineum of the rabbit the continuity of the flat
cells, which in silver preparations are considered to indicate lymphatic
vessels, with cells covering the fibrillary substance can be shown to a
greater or less extent, according to the success which has attended this
difficult manipulation. That it often. succeeds in patches, is shown by
5:iii Dr. G. Thiu on Ike Anatomy of
tbo plates that illustrat* worta on this aubject, although the mfluenrr
of Von EecklinghftueeQ'B doctrine (namely, tliat wherever au epithelium
is found n lymphatic capillary must be supposed to exist) haa led to wbtt
I believe to be their tnio nature being overlooked.
From a similar cause to that eocountered in tendon., the complete re-
duction of the dense corium of maminals by potssU is rery diflicalf ; but
by treating thin sections of fresh cutis, isolated flat cells aj« found.
In the cutis of the frog, the bundles oE fibrillary tissue are arranged in
parallel layers, and the corium being thin, the demonstmlion of flat wll»
is ejisier. And here the continuity of these eeliB with those of the rvte
Malpighi is erident, in the same way as the cells of the anterior epithe-
lium of the cornea ore continuous nith the flat cells of the interior of
the structure.
Figures 11 and 12, Plate X., represent flat cells from the skin of die
01 and frog.
I make the same inference in regard to the communication of ihe
spaces between the cells o£ the rote Malpighi with the lymph-spaces ("f
the corium, that I make in regard to the similar arrangement in the cornea,
both AS regards anatomical continuity and in regard to the position of
the nerves in the spaces, Langerhans has described the network of
nerve-fibres in the rcte Malpighi, and, in that of Ihe cutis of the rabbit,
tlio rii'h iiftMiDrk in the sjiaces between the cells is not very difficult lo
demonstrate. In the skin of the finger, I hare traced a medullated mm
as high OB the third layer.
Eanvier, in that part of his essay which treats of the element! mB»-
laires du tissu conjonctif l&die, describes an entirely different an&tomiot
element from that on which the authorities with whom he is in contro-
versy had fixed their attention. The cells figured by him* are the aame
as those isolated by potash when very thin pieces of skin or areolar tissos
are operated on. As described by him, they are applied closely to tlw
bundles. But when he attempts to show that the conQectdve-tisaue cor-
puscle of Virchow does not exist, and that the appearances by whit^ it ii
distinguished depend on an optical delusion, I believe him to be nustaken.
In skin and subcutaneous tissue the chloride of gold brings out in tbe
clearest manner the existence of nucleated ceUs with long projecting pro-
cssses stretching between and around the bundles, the whole of tha
eeUs being connected by the anastomoses of their processes. So com-
plete is the analogy between skin and tendon, that it would be easy to
find parts of a successful gold preparation of akin where the diagnooia
between skin and tendon might be difficult.
Figures 13 and 14, Plate X., illustrate the appearances presented by
the branched cells in skin.
A history of the opinions held regarding the structure of the con-
nective tissues since the time of Schwann is equally.beyond the scope (rf
^ • L,e. p. 483.
Coimective Tistug, Nerve, and Mtucie.
thii paper and my acquamtanoe with the Utoratme of the subject. It
is, however, well known that while twenty years ago the so-called con~
nectivfr-tJBSue oorpnacles weA believed to be concerned in the formation
of elastic tissue, with the development of Virchow's doctrine of cel-
lular pathology, this opinion seems to have been gradually abandoned,
even by those who, like Vinbow himself, had originally maintained it.
Banvier, whose investigations seem to have been conducted in singular
independence of contemporary theories, holds that the first step in the
appearance of elastic tissue is the formation of "granulaiumt ri/nngenta"
traceable in the fully developed fibres.
In the spring of 1673, while investigating the structure of the touch-
corpuscles of the finger, I found that the much-discussed cellular ele-
ments of these bodies, which colour in gold and carmine,' anastomose with
each other by means of fibres that resist prolonged maceration in con-
centrated acetic and dilute mineral acids, and I described them, in the
account I gave of the results of my investigation, as " elastic tissue fibres."
At the same time I found that similar cells and fibres form a thick net-
work in the cerium. Simultaneously, Spina made his exhaustive study
of the connexion of the elastic fibres in tendon with the walla of the
cell, to which I have already referred.
Since that time, I have continued to subject the skin and subcutaneous
tissue to treatment by different methods, and the results have been con-
firmative of those I obtained in Vienna. Shortly expressed, the con-
clusion I have come to is, that, in skin, all the branched cells form elastic
tissue on their surface and on their processes, and that there is no elastic
tissue anywhere that is not so formed.
The cells found in connective tissue are divisible, as I believe, into two
distinct classes. There are, first, the flat cells which never branch, and
which, when treated by nitrate of silver, present appearances identical
with those produced when the flat cells of serous membranes are simi-
larly treated ; secondly, there is the system of branched cells in its va-
rious forms. As contrasted with each other, they may be described simply
as the flat and branched ceUs of connective tissue*. Between these
two classes of cells there is no transition and no anatomical continuity.
The forms of the branched cells embrace all the gradations between the
fine network of a lymphatic gland and the anotitomoHLng network of the
strong fibres in skin and tendon. They are distinguished by their pro-
cesses, their capacity to form a substance that resists acetic acid — the
power, namely, of forming the resisting element specially characteristic
of elastic tissue. That they do not all exercise this latter power to
the same degree, does not constitute a sufficient difference to make
it necessary to regard them as separable into classes essentially distinct.
The ligunentum nucha may be taken as the type of the stronger forms
■ To flst sells Om Urm plaeotdt hs* bem applied b; Dr. Burdon Ssndsrxm, Oit
e^nbalent <rf ths QsnnsofbAm,
522 Dr. O. Thin m ike Jbi&tamf ^
of elastic tissue ; and I select it fortius reason to proffe tiie ^"^"n^ ooffk
tit its fibres.
If a thin piece of the ligamentnm nnchiB is Strang^ ookmred bj cUorids
of gold and genti j teased in gljcenne, tiiero will be fodnd a «"»"b^ cf
otbI nuclei lying loose amongst the fibres^ Bat careful
shows similar nuclei stiU adhering to manj of the latter; and'in
instances the remains of the protc^lasm of tiie cdl can be seen aromd
the nucleus and adherent to the fibre. The nndeos and oeDriemaina an
often found at the point of the division of a fibre into two, and nwliffilft
the original processes of the cell in the embryonic state.
If a portion of the same gold-stained ligament is farther placed in a
very strong solution of hsDmatoxylin and alum for twelve boiirs^ and
then carefully spread out for examination, the appearances will be fbond
to have considerably changed. If the preparation has not been lOD^dy
handled, the astringent effect of the latter solution has caosed the dear
outiines of the individual fibres to disappear, and, in tiieir stead, then are
flat bluish bands in which fine dark lines connecting oval swelliiigB are
seen. The latter are the nuclei, and the lines are* permeable canals in
the elastic fibres, which have become filled witii the hematoxylin aoloEtioiL
Both these conditions are depicted in figures 15, 16, and 17, Plate X.
The formation of the elastic substance on the surface of the cell, as
described by Spina in tendon, applies universally, and also holds good for
the cell-processes. But the part of the cell-body that does not enter into
the formation of this resisting substance, so far from sharing the strength
of the new tissue, becomes more easily disintegrated than at an earher
period of its development, and can be found only when the tissue is
cautiously manipulated. But sufficient staining with gold, and care in
operating, will demonstrate the cellular origin of elastic fibres in whatever
tissue they occur.
Virehow, as is well known, vindicates for his connective-tissue corpus-
cles the character of a connected chain of plasmatic canals, and I have re-
marked above regarding the tubular nature of the fibres of the ligamentum
nuchsD. That every elastic fibre is permeable to fluid is highly probable,
though not yet proven. This tubular nature of the larger fibres has pro-
duced one of the difficulties of the recognition of the connexion of the
fibre with the cell. The chloride of gold colours the protoplasm of a cell,
with which a fully developed fibre is continuous, a faint purple ; and when
the tinting is continued into the process, it is the contents of the tubular
space that are coloured. The elastic fibre, unless carefully examined in
a good light, is apt either to escape observation, or seems to run past the
cell without being in continuity with it.
This difficulty has been increased by a chemical difference between the
cell and the elastic tissue to which it gives origin, so that many reagents
and modes of treatment, that by potash-lye for instance, dissolve the cell
but leave the fibre untouched. Hence the methods that have been most
Connective TUtw, Nerve, and AfmcU. 623
used for establieluDg the mdividiul ch&ractarB of elaatio tissne hftT« been
instrumental in producing eironeouB notiona as to its origin.
Thus we have in skin, as in tendon, bundles of fibrillary tissue eveiy-'
where corered with flat cells, and, in the interstices of the bundles, the
analogues of the brani^ed cells of the cornea, producing a ramifying net-
work of elastic tissue.
In gold preparations of the skin, the blood-vessels and nerves can be
followed between the larger fasciculi, analogously to the position of the
nerves in the cornea.
Fascia differs from skin and tendon only in so far as its flatness permits
and necessitates a change of forin in the flat ceUs, and the easy study of
their arrangement and nature by nitrate of silver. If a half per cent,
solution'is injected under the skin of a mouse's back and the animal killed
. in from five to ten minutes afterwards, and the skin of the back disBect«d
off, the fascia which has been in contact with the silver is recognised by
its milky whiteness and (edematous condition. If spread out car«fully
on the object-glass in glycerine and exposed to sunlight, it is seen to be
plated over with oblong or slightly rounded cells with large nucla.
Figure 8, Plate TS.., is a sketch from a part of a preparation so obttuned.
The cells separated from the same structure by potash are represented
in figure 9, Plate IX. ; it will be observed that they are identical in
appearance. Figure 10, PUite IX., illustrates the very lai^ flat cells,
with their nuclei, that cover the fascia of the muscles of the thigh of the
frog.
Frequently, bat not so constantly, the branched cells are also stained
by the silver, and they are generally found at a different focus.
Kanvier ('Archives de Physiologie ') has described flat cells on the
sheaths of nene-fasciculi and the investing membrane of nerve-bundles
as constituting a lymphatic sheath.
By means of the saturated potash solution I have been able to satisfy
myself that, not only are the nerve-bundles surrounded by lymphatic
sheaths, but that each meduUated nerve-fibre is invested with a layer '
of flat cells. This layer is closely applied to the medulla, and is
internal to the sheath of Schwann, It is composed of eitremely fine
and delicate cells, and their demonstration by potash succeeds less fre-
quently than does that of the cornea-cells ; they are (as far as I have
seen) without exception long and narrow, often tapering to an exceedingly
fine point. In the finest forms their cellular nature is only to be distinctly
made out by a magnifying-power of 700 or 800 diameters. Figure 18,
Plate X., represents varieties of these cells and their relation to the
medulla. Their length varies from 0'075 to 0'036 millim, ; many of them
are not more than O'OOld mdlim. broad. Appearances are sometimes seen
that would seem to indicate that the sheath of Schwann (tubular mem-
brane) is lined by a layer of flat cells, distinct frofn that covering the
medulla (white substance). Themedulla,^heati«eft«&\y3'$^:^MSb,^'wt«SQhb
624 Dr. O. Thin m the JtmHrng ^
% leriet of bulgiiigs, so thsfc its kteml (optiofti) bordeif am dM^gaaloily
irregolarlj waYing lines. One set ctf deUcste oeDi euL ba aaen nloislj
f oOo wing tiie unnosities ctf the snhstuuse, while another eat^ mosia ^"Tlwrd,
lie in a straight direction parallel to the longitadinal axia of tiia fibn^
Where the medulla is constricted, tiiere is a dear apaoa botwai tkHi
two sets of cells, which are in contact at the conTantiaa ^nn^^ \fj ^
bolgings.
B7 adhering to the broad principle that wherever tfaeia ia a nndew
there is a cell, the eidstence of a great number of cellfl aurrotmding ths
medulla of a nerve-fibre can be demonstrated in another wa^. If a nerve
is placed in absolute alcohol for twentj-f our hours and then Tavj ymfly
dimtangled from the sheath in glycerine, a oover-glass pat on and aoliitiflB
of hematoxylin drawn through the field by filter-paper, tibe nooiki of the
fibres stain first, and their number soon becomes yety stxildng. IE ths
field is allowed to become saturated and obscuro with ilie dje, and tlMn
subsequently deared up by aoeiic add, those fibres whidi have not
suffered by the manipulation are literally dotted over witii nndaL Hw
number is so great as at once to dispd the idea that they can be aoooonted
for by the sheath of Schwann. The nudd of the sheath oan oftsn hs
distinguished from the others by their more external poaituin rdathne to
the nerve and a deeper tint. Figuro 19, Plate X., is drawn from a pre-
paration made in this way.
The ring which, as Eanvier was the first to show, snares the medullaM
fibre is well seen when the nerv^e is treated by absolute alcohol or tiw
saturated potash solution, both of which leave the medulla untouched.
As at the seat of this constrictioQ the medulla is deficient, and as the
nerve-fibre is bathed in lymph, it is evident that there must be at these
points a very intimate connexion between the lymph-fluid and the axis-
cyliuder of the nerve. This has been already indicated by Banvier in his
essay on the lymphatic nature of the nerve-sheaths, and receives greater
force now that we know that flat cells, indicative of lymphatic structures,
are situated on the fibres themselves.
The use of hsDmatoxylin is as advantageous in demonstrating the large
nuclei of the flat cells of the nerve-sheaths as it is in showing those of
tendon.
Banvier has observed that in transverse sections of nerves the sheaths
and connective tissue surrounding the fibres stain more deeply \i'ith car-
mine than the surrounding tissue does. 1 have made a similar observation
in the nerv'es of the skin in gold preparations which had been macerated
in acetic acid. In this dMB the concentrically arranged connective tissue
of the nerves is conspicuous by its pearly whiteness. But as we know
that the surrounding corium is equally rich with the nerve in lymphatic
structures, the cause of the difference in colour must be sought elsewhere,
and will probably 1^ found in relative differences in regard to the ar*
xangement of the elastic tissue*
Cmmeettet Tbtne, Nerte, and Mtuck. 625
By comtniiing sevenl m^ods of inTettagaiion, I beliere I hare suc-
ceeded in cleftring up some points in the anatomy of muiciUar fibre,
by which it will be seen that, as regards the lymphatic system, muscle
occupies a position almost identical with tendon and connectiTe tissue
generally.
If fresh muscle is deeply stained with hicmatoxyliu and then treated
by acetic acid and gently teased, the perimysium of the bundles and it« vary
fine continuation around each fibre are seen to be studded with hu^ round
nuclei, which are far more numerous than those of the branched cells,
which are also seen. The round nuclei belong to the flat cells of the
perimysium.
I have been able to demonstrate the character of the cells ^j teasing
the living muscle of the frog Id aqueous humour, and thence truuferring
the separated fibres to the nitrate-of-silver solution. The usual sinuous
lines are then seen both on the general and special perimysium. This is
represented in figures 5 and 6, Plate XZ.
When muscle is treated by the saturated solution of potash, as above
described, the fibres are found unaltered, the striated appearance being
well marked. There is no vestige left of the perimysium. On the naked
surface of the sarcolemma, a number of round distinct nuclei aro seen ; and
when they happen to be on the edge of the fractured fibre, it is seen that
they are situated on its outer surface.
If the saturated potash solution in which the muscle is placed is kept
for about an hour at a temperature of 110° Fahrenheit, and then allowed
to cool gradually, we find a further effect has been produced. '
On breaking down a piece of the muscle into its individual fibres, we
find that although some of these are unaltered, others have lost all their
nuclei, and present the appearance of a coarse granular cylinder. But
there is sometimes a transition stage seen of peculiar interest. On the
surface of the fibre the outlines of a series of quadrangular cells make
tbemselrea visible, each cell having a distinct nucleus ; and it is easy to
satisfy one's self that the nuclei of the cells are identical with the nuclei
seen previously distributed over the surface of -4ihe sarcolemma. These
cells are sometimes also seen free in the solution, in which case they are
generally more or less broken up, but sometimes they are seen isolated
in perfect condition. Figure 21, Plate XI., shows the ct^Ue becoming de-
marcated on the fibre, and figure 22, Plate XI., their appearance when
isolated entire. The sarcolemma is sometimes seen freed both from the
' cella and th^ contents ; and in this case the striped cylinder which may be
seen near it is beset with small perforations. -
The aarcolemmaof muscle is thus covered with flat cells, regular in appear-
ance and outline, which resist the action of a saturated solution of potash.
But the action of the potash teaches us something more. A fibre is
flometimes found apparently un^tered, smooth in it« c«mt<mr, and atill
showing ftomething of the striated appeaiamoa, \»A ibsrarSs^ -&» Tfo&ssk.
526
Br. 0« Thin m the JMMtmnif 4/
One or more rgimd holes are, however, seen on (lie pieces of brok^
cylinder, the more conspicnous becftuse the nndei are wimmA ; the]
about the size o£ the blood-corpasde of the frog. Bj dumgiiig the t
it is seen that each hole is only on one side of the fibre. The 1
deamess of their outline shows they are not artefiu^, bat spaoee in n
the sarcolemma is wanting (figure 23, Plate XL). A forttier rndk
potash is seen when a muscular fibre is found channelled with one or i
canals parallel to the long axis of the fibre. The' canals thoa seen
imif onn in breadth ; they are formed by rows of vacnoles, whidi oc
spond in shape and size to the nuclei of cells. (I had observed in sti
ing the cornea that the first stage of the destruction of the flat oeUsy in
potash solution, is a vacuole taking the place of the nucleus.) By chaoj
the focus, it is seen that these channels are in the substance o£ the fi
Smaller channels and single vacuoles are seen in di£Eerent planes.
A more extended degree of the action of potash on a fibre is when
central canal has no longer sharp outlines and is seen to contain gran
ddbris. -
Treatment of muscular fibre by hiematoxylin gives, as regards nn
results confirmatory of those got by potash, in so far as a still gre
number of nuclei are seen internal to the sarcolemma than is indict
even by that method. To obtain the best results from hsematoxylin,
fibres should be isolated before being dyed. The excess of colour \x
removed by acetic acid, the nuclei become distinct ; they are seen t
arranged in long rows, those of one row being in the same plane. Isob
nuclei are seen in different planes. An idea of their number is 1
formed from the appearance presented by the broken end of a fibre w
it is turned upwards, giving a view equivalent to a transverse sect
The whole thickness of the fibre is then seen to contain nuclei, in the
rangement of which something of a concentric disposition can gener
be observed. The nuclei are large and oval, and contain one or 1
distinct nucleoli. If the substance of the fibre has been teased, it is s
that the fibrillae are arranged in bundles which have an equal thickn<
and isolated nuclei are seen adhering to their surface.
The inferences that are irresistible from these appearances prepare
way to readily understanding the more decided effects of an appropri
treatment by chloride of gold. The conditions of a successful exami
tion of a muscular fibre by gold include the detachment of the perimysi
from the fibre without injuring the latter, the obtaining good transvc
views in the preparation, and the requisite degree of colouring. As it is :
possible to ensure beforehand a combination of these favourable con
tions, it is evident that, with equal care, success is not uniform. 1
results which I now give were obtained by teasing the muscles of
thigh of the frog in aqueous humour before staining with gold.
Li the most perfect preparations thus obtained, the structure of a mi
cular fibre is seen to be almost identical with that of a fasciculus
Cottnective Tiuue, Nerve, and Mutele. 627
teudun. Longitudmally the fibre ie Been to couHist of parallel buadles
of uniform width, separated by apAces thftt are indicated by distinct lines ;
and, distributed at intervals in the lines, are oblong naolei, the long axis
of which ia parallel to that of the fibre. The breadth of the bundles is
aboat the same as that of a secondary bundle in tendon ; their surface
is smooth and bomogeneoos (figure 25, Plate XI.).
A transverse view, corresponding to that of a cross section of tendon,
shows tbe muscular substance intersected by stellate spaces, in some of
which nuclei are seen, and, branching out from the spaces, a rich anasto-
mosing network of fine dark lines divides tbe substance of the fibre into
a number of compartments. Between the appearance I have just described
and that of a cross section of tendon similarly prepared, the only difference
is that, in muscle, the fields enclosed by the dark lines are dotted over by
minute points, which may indicate the fibriUee.
Nuclei are always seen in fibres successfully stained with gold, and
especially when the fibre is separated by teasing into the bundles of
fibrillffi ; but their number is much less than that seen when htematoxylin
is used. We have seen how, in the cornea, gold when it has deeply stained
the nucleus of the branched cells leaves that of the flat cell invisible,
while hiematoxylin colours them both. So it is generally in tbe capil-
laries of blood-vessels'. I have found that, in the capillaries of the muscles
of the frt^, these invariably consist of two layers — an internal epitholial
layer, the outlines of whose cells are defined b; nitrate of silver, and an
external layer, into whjch a fine system of branched cells enters. Uaimn-
toxylia brings out the nuclei of the cells of both layers. The deep stain-
ing with gold, while it differentiates the kyora by staining the internal
(epithelial) more intensely than it does the outer (adventitious) layer, shows
no nuclei in the epithelium, while the nuclei in the outer layer are well
marked.
In applying to muscular fibre the experience thus acquired, we ore
warranted in concluding that the nuclei coloured in gold are those of cells
that belong to the branched system, and which are the characteristic
nuclei seen in the transverse view of a gold-stiuned muscle, while the
great majority of those stained by btematoxylin belong to the flat cells of
the lymphatic system.
The isolation of these cells is surrounded by difficulties, which are, how-
ever, surmountable. In fibres deeply stained by gold I have isolated long
thin flat cells, lying amongst the fibrillce, which are identical in shape
with similar cells in the cornea. They were coloured uniformly deep
purple, and a distinct nucleus was not visible. They are represented in
figure 27, Plate XI.
Immediately investing the bundles composing a muscular fibre is the
sarcolemma, which is externally, as I have shown, covered with flat cells.
The property possessed by this membrane of resisting acetic acid is the
cause of a characteristic appearance presented by a muscular fibre under
528 Dr. G. Thin m ike Jtialmi^ tf
its influence. From the hroken end a krge nneifen vmm pEofandM vitt
thick eyerted lips, bending back over the memtanne wfaidi taanm a atiaa
gukting band round the neck of the protmiioin. When thia ahoath ii
ruptured at difbrent parts, the gehitmous snbstanoe, nUeh Conna alaigs
proportion of the contents of the fibre, bulges out in inasina aa tt avrik
The fibrill», which do not swell under the add, and wUdi an im-
bedded in this mass, can be often seen, in teased gold or hsainalmjlin
preparations, lying unaltered at one part of tiie field, irkQe displaesl
masses of gelatinous substance are seen at another. (It is the diapoHfn
of this gelatinous substance in parallel bundles which is the caoae of Aa
peculiar effect of chloride of gold, represented in figure 25, Plata XL)
The astringent effect of chloride of gold on the sarool«mna prodnflesa
Terj characteristic appearance. In manipulating a fibre, as aprelinrinaiy ts
its being hardened by gold, it sometimes happens that the menilnaiia nd
the layer of musdeHBubstanoe adhering to it is rent longttadinally froai
the sur&ce to the centre. In the gold solution it loses ita cjliadiiied
form, and spreads itself out as a broad band. This perfectly flat hand is
marked longitudinally with parallel lines, which are straight and aqin*
distant from each other. The prolonged action of acetic aeid doea nofc
alter the appearance of these lines or their mutual relations, but it makes
visible a not very thick layer of gelatinous substance, which protrudes
from imder the edges of the band.
Without comparing this peculiar appearance in its most exquisite forms
with the transition stages sometimes seen, in which one end of a fibre
still retains its cylindrical form while the other end is flattened out, the
observer might certainly doubt that he was looking at a muscular fibre.
Interstices between the lines, and, in them, occasictnal oblong nuclei are
sometimes visible.
The loiigitudinal lines are the optical expression of the septa between
the bundles, which are seen through the transparent sheath ; and that
the fibres in these septa are formed by elastic tissue, is shown by thdr
persistence when treated by acetic acid.
They differ in no respect from the septa and their contained nuclei,
which are seen in muscular fibres that have retained their cylindrical form
when the chloride of gold has produced that appearance.
Another occasional effect of the astringent action of gold is an exag-
geration of the dimensions of the central canal. The upturned end of a
fibre is sometimes seen in which there is the appearance of a wide central
cavity, around which the contents of the sarcolemma form a thick rim.
The mechanism of this appearance is explicable by the assumption that
the sarcolemma becomes sufficiently unpelding to form an immovable
surface, towards which the more yielding substance is drawn as the
shrinking caused by the gold proceeds.
The sarcolemma is probably in very intimate connexion with the elastic
network, the more superficial cells of which, with their prolongations, are
Conntetive TUatte, Nerve, md MutcU. 629
situated directly under uid apptuentiy in contact with it ; and the nn-
meraiu foramina seen in the cylindrical rod left by the potash solution,
vhen the membrane has been loosened from it, ue probably the pcsnts
vhere the elastic fibres penetrate.
A muscular fibre is thus composed of a number of bundles resembling
those of tendon, arranged parallel to each other, each bundle giring
shelter to a number of fibrillte, and separated from the neighbouring bundles'
by a space lined with flat cells. In the larger spaces lie tnnnched ceDs,
and in the smaller the projecting processes vt the elastic fibres given out
by the latter.
The large holes I have described in the elastic sheath afford passage to'
the nerves. When these have been traced, it is reasonable to infer that,
here as well as elsewhere, they will be foimd to follow the lymph-channel i.
These holes not only permit the passftge o£ nerves, but allow free com-
muuitution between the lymphatic spaces within the fibre and those
between the perimyBium and the sarcolemma.
The abundance of gelatinous sabstance in a muscular fibre accounts,
for the phenomenon known as transverse cleavage, which is produced by
the action of very diluted hydrochloric acid. I regard it as essentially
equivalent to the effect produced in tendon when by similar treatment a
bundle divides transversely into the flat plates known as the " Sonde-
rische Bander," after the distinguished histologist who first described
them.
To sum up these views regarding the structure of muscle in a few
words, it might be said that a muscular fibre is a fasciculus of tendon in
the bundles of which the primitiTe fibrillffi ore imbedded longitudinally.
The small spaces a^ the points of junction of flat cells which colour
deeply in silver, and to which allusion has been made by histologists, are
seen in all tissues. They are always present when the colouring has been
intense, and should, I believe, be regarded as playing an important part in
the mechanism of the lymphatic system. They are especially well defined
in the rete Malpighi of the fn^, where it would be impossible to regard
them as artefacts.
It is evident from the various anatomical facts above detailed, that the
tissues inay be said to be in an almost unbroken continuity with the
lymph-system*. "When a blood-corpuscle escapes from a capillary it is
into the cell-lined spaces of this system that it directly passes, and there
is manifestly no obstacle to the passage of the contents of the lymph-
channel into the blood other than that formed by the <A'all of the capil-
laries, which alone separates the fluids of the lymphatic and vascular
systems. We know that white blood-corpuscles can make their way
* In this eonnezian I quote from Rsnvier'i etuj {I. e. p. 486) the following tea-
tence : — " L'eti«l«iiM, duis le tiiiu csllulnire >om-cutuii, de cei cellules plates, div
po*£«s I U Boriice dw biaoeans, ns notu toggjre-t-elle paa l'id£e de voic dans le
tinu eonjonetif nn vsste espsce doisotml, analogue aox caniUt ttnuMb'V''
530 Dr. G. Thin o« (Ac Analogy of
through at the points of junctiou of the angles of the capillary cells*, wd
it is reasouable to suppose that these points &k always permeable te
fluids.
We have seen that thpre is a rich supply o£ lymphatic channela ia the
interior of a muscnkr fibre, and that the axia-cyliuder of a nerve ia pro-
bably in free eommunication with the lyraph. Tho term " inv^ination,
aa applied to the relation of the nerves and blood-vesseU of particular
organa to the lymphatics, has no special physiological meaning, as it only
impUea that at certain parts* condition that is unirersal can, by special
modes of procedure, be made capable of more easy demonstration. Every
nerve-fibre and every blood-vessel is invaginated in lymphatics.
That there ia a plasmatic circulation infinitely more comprehenaire
than that expounded by Tirchow. ia, as has been already remarked by
Eanwer, a fact which anatomy has placed on an incontroverlible basi?.
EXPLANATION OF THE PLATHa.
The Drawings were eicciitfd by Mr. J. C. Ewirt from mj prepanlions. The
obj»:tivcs and ocular glusn n>ferred to sa indicating the luagnirjing-powBri
I are thow of Hartnarli, with the eiceplion o[ the TUd. XII. imniersion-leiu
I Uied in > few instance*, whieh win nmde by Virict, nnd bu the potter
assigned lu tliat tminber in his BcnK.. Tlius 3. Vllt. n>«uis eippiew No 3
and objeotiTe So. VIII.
Pmib vm.
Kg. 1. Cells from the oomsa of a frog which wu treated by the saturated lolatiaD of
potash. 3. Tm. Tube out.
Vi%. 2. Cetla from the oomea of (he ox treated by «olution of potaah, 3. Till.
Tube out.
Fig. S. Cells from tbe cornea of the sheep treated by iolulton of potash. 3. nil.
Tub© oul
Platr IX.
Fig. 4. Tendon from a mouse's tail coloured by nitrate of silver. 3. TIL Tnbe out.
Fig. 5. Perimysiumof muioleof frog. Silver preparation. 3. Vn. Tube out.
Fig. 6. Perimysium of a muscular fibre of frog. Silver preparstioii. 3. TTL Tube out
Fig. 7. Cells from tendo Achillis of frag by solution of potash. 3. Tm. Tube ouL
Fig. e. Fascia from dorsal musclea of the mouse. Nitrate-of-silrer preparation.
3. Tin. Tube out. •
F^. 9. Cells isolated from the fascia of the dorsal muscles of the mouse by ebtution of
potash. 3. Tnr. Tube out.
F^. 10. Continuous layer of flat cells investing the fWicia of the muscles of the thigh
of the frog. Nitrate-of-mlver preparation. 3. Till. Tube oat.
Plate X.
Fig. II. Cells of ths cutis of Ihe frog isolated by solution of potash. 3. TTTT, Tube
Fig. 12. Cells isolated from the skin of the 01 by solution of potaah. 3. TIH. Tobeout.
Fig. 13. The anastomosis of the cells by means of the elastic fibre*. Gold preparation
from finger, macerated in acetic acid. 3. XII.
* EndolheUum en Emigratie door Dr. Laidlaw Furves. Utrw^t, 1873.
'c^'^M.wawi.i^M
.'C Ei.»T i^ -l\-MW,tU,tuh
:■/ .vji. r: V.
JCXwaitM.. wmi^iUjUth.
Proc. Ray Sac. VolJXII. R XI.
JC£imHj4L WSIfa'tr'A
Connective Tietue, Nerve, and Mtucle. 581
Fig. 14. Elaatdo flbrra irith oelU. Section ttom guld praparatioQ of (kill of adult
rabbit treated by oonoentnted aoetio odd. Si Tin. Tube oat-
Fig. 15. Fibna from the ligsmentum nucbiB of a three-dajsHild foal. Gold prepan-
tion. The noclei and remuns of the protoplaon of the cell ■tained. 3. TUL
Tube out.
Kg. 16. Ligamentum nQch» of tbree-daji-old foal stained in gold and hiematoijlin.
The central oanal of the fibres indicated by the haematorrtin. 3. Till.
Tube out ■
Fig. 17. Fibre from the same pi^pantion aa fig. 15. 1, XQ. Tube out.
Fig. 18. Cetla from the fibm of the sciatic oerre of the frog. Isolated by the eaturated
solution of potash, 3. VU. Tube out.
Fig. 10. IferTO-Sbre from the sciatic nerre of the moiue. Treated by absolute alcohol,
djed irith hiematoiylin, and the ercess of Colour removed by acetic acid.
3. Tin. Tube out.
PtATB XI.
Fig. 2tX Ferimysiam of a musoular fibre of frog stained in luEmatoiylin. Flat oelli
seen. 3. Til. Tube out.
Fig. 21. Muscle of mouse subjected to prolonged action of warm potash solutJOD. The
cells on the sarcolemma indicated. 3. Till. Tube out.
Fig. 22. Flat cells from the sarcolemma of muscuLu- fibre of oi. Isolated by pro-
longed action of warm potash solution. 3. Till, Tube out.
Fig. 23. Muscular fibre of mouse treated by solution of potash. The boles in the sar-
colemma seen. 3. Tin. Tube ouL
Fig. 24. Muscular Glire of frog trmtsd by eotulion of potash. Canals indicated by
nuclear vacuoles. 3. Tni. Tube out.
Fig. 25. Muscular fibre of frog. Gold preparation. Sarcolemma rent longitudinally
and flattened. Sepia diriding muscular subatanco risible. 3. Til. Tube
Fig. 28. End lieir of musoular fibre of frog. Gold preparation. Stellate spaces with
nuclei and processes of branched cells, haTing the signification of elastic
fibres, between the bundles. 3. Til. Tube out.
Fig. 27. Muscular fibre of frog. Qold preparation, Tho fibrillEe separated by leasing
into bundles, betweenwhich long narrow fiatcellearescen. 3. Til. Tubeout.
Fig. 28. Muscular fibre of frog. Oold preparation. The central cavity seen mueh
enlarged by the astringent action of the gold. 3. TH. Tube oat.
" On the Refraction of Soond by the Atmosphere." By Prof.
OsBORME Revnoldb. Communicatcd by Prof. G. G. Stokes,
Sec.E.S. ReceiTcd March 18, 1874*.
My object in tbie paper is to offer eiplanatioDB of aome of the mora
common phenomena of the transmission of sound, and to describe the
results of experiments in support of these eiplanations. The first part
of the paper is devoted to the actvm of wind upon touitd. In this part of
the subject I find that I have been preceded by Professor Stoies, who
in 1857 gave precisely the same explanation as that which occurred to
me. I have, however, succeeded in phuring the truth of this explanation
upon an experimental basis ; and this, together with the fiwt that my
work upon this part of the subject is the cause and foundation of what
>• Bead April 23, 1W4. Bee onM, p. 295.
TOL. xxn. 2 B
682 Prof. O. Beynolds on Ike
I have to saj on the s30ond part, most be my ezouse for introduciiig it
here. In the second part of the subject I have dealt with the eflbct of
the atmosphere to refract sound upwards, an effect which is due to tlie
yariation of temperature, and which I beHeve has not hitherto been
noticed. I have been able to show that this le&actioii explaina the
well-known difference which exists in the distinctneBS of sounds bj day
and by night, as well as other differences in the transmiiwtion of sound
arising out of circumstances such as temperature ; and I have applied
it in particular to explain the very definite results obtained by Profeasor
Tyndall in his experiments off the South Foreland.
The Effect of Wind upon Sound
IB a matter of common observation. Oases have been known in which,
against a high wind, guns could not be heard at a distance of 550 yards*,
although on a quiet day the same guns might be heard from ten to
twenty miles. And it is not only with high winds that the efEect upon
sound is apparent ; every sportsman knows how important it is to enter
the field on the lee side even when the wind is very light. In lig^
winds, however, the effect is not so certain as in high winds ; and (at any
rate so far as our ears are concerned) sounds from a small distance
seem at times to be rather intensified than diminished against very light
viinds. On all occasions the effect of \iind seems to be rather against
distance than against distinctness. Sounds heard to windward are for
the most part heard with their full distinctness ; and there is only a
comparativoly small margin between that point at which the sound is
perceptibly diminished and that at which it ceases to be audible.
That sound should be blown back by a high wind does not at first
sight appear to be unreasonable. Sound is kno\ni to travel forward
through or on the air ; and if the air is itself in motion, moving back-
wards, it will carry the sound with it, and so retard its forward motion —
just as the current of a river retards the motion of ships moving up the
stream. A little consideration, however, ser^'es to show that the effect
of wind on sound cannot be explained in this way. The velocity of
sound (1100 feet per second) is so great compared with that of the
highest wind (50 to 100 feet per second), that the mere retardation of the
velocity, if that were all, would not be apparent. The sound would
proceed against the wind with a slightly diminished velocity, at least
1000 feet per second, and with a but very slightly diminished intensity.
Neither can the effect of wind be solely due to its effect on our hear'
ing. There can be no doubt that during a high wind our power of
hearing is damaged ; but this is the same from whatever direction the
sound may come ; and hence from this cause the wind would diminish
the distance at which sounds could be heard, whether they moved with
it or against it, whereas this is most distinctly not the case. Sounds at
* Proc. Boy. Soc. 1874, p. 62.
Refraclion of Sound by the Atmosphere. 533
r^ht angles to the wind ore but little affected by it ; uid in moderate
winds aounds can be heard further with the wind than when there is
none.
The same msj be said against tbeoriea which would explain the effect
of wind aa causing a heterogeneous nature iu the air so that it might
reflect the sound. M\ such effects must apply with equal force with and
against the wind.
This question has bafBed investigators for so long a time, because they
have looked for the cause in some direct effect of the motion of \he air,
whereas it seems to be but incidentally due to this. The effect appears,
after all, not to be due simply to the wind, but to the difference in the
velocity tcith which the air trarels at the surface of the ground and at a
height above it; that is to say, if we cotild have a perfectly smooth
snrface which would not retard the wind at all, then the wind would not
obstruct sound in the way it does, for it would all be moriug with an
equal velocity ; but, owing to the roughness of the surbce and the ob-
structions upon it, there is a gradual diminution in the velocity of the
wind aa it approaches the surface. The rate of this diminution will
depend on the natiu« of the surface; for instance, in a meadow the
velocity at 1 foot above the surface is only half what it is at an ele-
vation of 8 feet, and smaller still compared with what it is at greater
hnghts.
To understand the way in which this variation in the velocity affects
the sound, it is Qecessary to consider that the velocity of the waves of
sound does depend on the velocity of the wind, although not in a great
degree. To find the velocity of the sound with the wind we must add
that of the wind to the normal velocity of sound, and against the wind
we must subtract the velocity of the wind from the 1100 feet per second
(or whatever may be the normal velocity of the sound) to find the
actual velocity. Now i£ the wind is moving at 10 feet per second
at the surface of a meadow, and at 20 feet per second at a height of
8 feet, the velocity of the sound against the wind will be 1090 feet
per second at the surface and 1080 feet per second at 8 feet above
the surface ; so that in a second the same wave of sound will have
travelled 10 feet further at the surface than at a height of 8 feet. This
difference of velocity would cause the wave to tip up and proceed in an
upward direction instead of horizontally. For if we imagine the front
of a wave of sound to be vertical to start with, it will, after proceeding
for <mc second against the wind, be inclined at an angle of more than 46%
or half a right angle ; and since sound-waves always move in a direction
perpendicular to the direction of the front (that is to say, if the waves
are vertical they will move horizontally and not otherwise), after one
second the wave would be moving upwards at an angle of 46° or more.
Of course, in reality, it would not have to proceed for one second before
it began to move upwards : the least forward motion would ba {K>'i!t.<y««&
534 Prof. O. BeynoldB on the
by an inclination of the front backwards, and by an upward motion d
the wave. A similar effect would be produced in a direction opposite to
that of the wind, only as the top of the wave would then be moving
fiister than the bottom, the vr^\es would incline forwards and move
downwards. In this way the effect of the wind is to lift the waves
which proceeded to Mindward, and to bring those down \i'hich move
with it.
Thus the effect of wind is not to destroy the sound, but to raise the
ends of the wave, which would otherwise move along the ground, to such
a height that they pass over our heads.
When the ends of the waves are raised from the ground they vidll
tend to diverge down to it, and throw off secondary waves, or, as I shall
call them, divenjiny waves, so as ]:o reconstitute the gap that is thiu
made. These secondary waves N\ill be heard as a continuation of the
sound, more or less faint, after the primary waves are altogether above
our heads. [This phenomenon of divergence presents many difRculties,
and has only as yet been dealt vi-ith for particular cases. It may, how-
ever, bo assumed, from what is known respecting it, that in the case of
sound being lifted up from the ground by refraction, or, what is neariy
the same thing, passing directly over the crest of a hill so that the
ground falls away from the rays of sound, diverging waves would be
thrown off very rapidly at first and for a considerable distance, depending
on the wave-length of the sound ; but as the sound proceeds further the
diverging rays would gradually become fainter and more nearly i)arallel
to the direct niys, until at a sufTicient distance they would pnictically
ceas(? to exist, or, at any rate, ho. no greater than those which cause the
diffnu't ion-bauds in a ])encil of light*. The divergence would introduce
bands of diffraction or interference within the direct or geometrical path
of the sound, as in the case of light. These efftu'ts would also be com-
plicated by the rellection of the diverging waves from the ground, which,
crossing the others at a small angle, would also cause bands oi inter-
ference. The results of all these causes would 1h' very conij)licated, but
their general eff(H't \^ould be to caus(^ a rapid weakening of the sound
at the ground from the point at which it was first lifted : and as the
sound became weaker it would be crossed bv bands of still fainter sound,
after which the diverging rays, as \\ ell as the direct rays, would he lifti-d,
and at the ground nothing would be heard. — Sej^tUmher 1874.]
If we leave out of consideration the divergence, then we mav fonn
some idea as to the path which the bottom of the sound, or the rays of
sound (considered as the rays of light), would follow. If the variation
in the speed of the \\ind were uniform from the surface upwards, then
* Taking sound of 1 foot wave-length, and comi^aring it v^ith light whose wave-
length is the 5().0()0th part of an inch, then tlio divergence of the sound at a mile from
the point at which it left tlie ground would bo compai-alively the same as that of the
light at ,\, of an inch from tlie aperture at which the pencil was fomied.
R^aetimo/Soand by the Atmotphere, 536
the rays of aound would at firet move upwards, very nearly in circles.
The radii of these circles may be abown to be 1100 x . where
V, and f, are the velocities of the wind in feet per second at elevations
differing by h feet. In fact, however, the variation is greatest at the
ground, and diminishes as we proceed upwards, so that the actual path
would be more that of a parabola.
Also, owing to this unequal variation in the velocity, those parts of the
waves immediately adjacent to the ground will rise more rapidly than
the part immediately above them ; hence there will be a crowing of the
waves at a few feet from the ground, and this will lead to an intensifying
of the sound at this point. Hence, notwithstanding the divergence, we
might expect the waves to windward to preserve their full intensity so
long as they were low enough to be heard. And this is in accordance
with the fact, often observed, that sounds at short distances are not
diminished but rather intensified when proceeding against the wind.
It will at once be perceived that by this action of the wind the dis-
tance to which sounds can be heard to windward must depend on the
elevation of the observer and the sound-producing body. This does not
appear to be a fact of general observation. It is difBcult to conceive how
it can have been overlooked, except that, in nine cases out of ten, sounds
are not continuous, and thus do not afford an opportunity of comparing
their distinctness at different places. It has often astonished me, how-
ever, when shooting, that a wind which did not appear to me to make
the least difference to the directiou in which I could hear small sounds
most distinctly, should yet be sufficient to cover one's approach to par-
tridges, and more particularly to rabbits, even until one was within a tew
feet of them — a tact which shows how much more effectively the wind
obstmcte sound near the ground than even a few feet above it.
Elevation, however, clearly offered a crucial teat whether such an action
as that 1 have described was the cause of the effect of wind upon sound.
Having once entertained the idea, it was clearly possible to put it to
the test in this way. Also, if the principles hold in sound, something
analt^us must hold in the case of waves on the surface of a running
stream of water — for instance, waves made near the bank of a river.
I had just reached the point of making such tests when I discovered
that the same views had been propounded by Professor Stokes so long
ago as 1857*. Of course, after such a discovery, it seemed almost un-
necessary for me to pursue the matter further ; but as there were one
or two points about which I was not then quite certain, and as Prof.
Stokes's paper does not appear to be ao well known as it might be (I
do not know of one writer on sound who has adopted this explanation),
it still seemed that It might be well, if possible, to put the subject
on an experimental basis. I therefore made the experiments I am
• Brit Amoo. Beporl, 18&7. Tmot. of Beat. p. 83.
Sae Fn>£. O. Beyuolda on the
(bout to deseribe ; nd I am glad that I did not iwt eontent wiOont
them, for they led me to what I beliere to be tjw dbcoroy of Ntnc-
tion of sound bf the atmoephere.
Fig.l.
The results of my first obserration are shown in fig. 1. Hiis repe-
sents the shape of the wares aa they proceeded outwards from a pouit
near the bonk of a stream about 12 feet wide. Had the water bean at
rest there would have been semicircular rings ; as it was, the front
of the waves up the stream mode an obtuse angle nith the wall, which
they gradually left. The ends of the waves, it will be observed, gradually
died out, showing the effect of divergence. The waves proceeding down
the stream were, on the other hand, inclined to the wall, which they
aji preached.
1 was able to make a somewhat better observation in the Medlock,
near the Oxford Rood Bridge, !Maii(.'hestt5r. A pipe sent a succession
of dro[)s into the water at a few inches from the wall, which, falling
from a considerable height, made very definite n-aves. Fig. 2 represents
a sketch of these waves, made on the spot : the divcrgii^ vaves from the
entU of the dire.-t waves, and also the bands of interference, are very
Befraction of Sound by the Atmoaphere. 537
clearly seen. Both these figures ngtee with what has been explained
as the effect of wind on sound.
In the next place I endeavoured to ascertain the effect which eleva-
tion has on the distance to which sound can be heard against a wind.
In making these eiperiments I discovered some facts relating to the
transmission of sound over a rough surface, which, although somewhat
obvious, appear hitherto to have escaped attention.
My apparatus consisted of an electrical bell, mounted- on a case con.
tuning a battery. The bell was placed horizontally on the top of the
case, so that it could be heard equally well in all directions ; and when
standing on the ground the bell was 1 foot above the surface. I also
used an anemometer.
These experiments were made on four different days, the 6th, 9th,
10th, and 11th of March. On the first of these the wind was very light,
on the others it was moderately strong, strongest on the second and
fourth ; on all four the direction was the same, vis. north. On the two
last days the ground was covered with enow, which gave additional in-
terest to the experiments, inasmuch as it enabled me to compare the
effect of different surfaces. On the first two days I was alone, but on
the last two I had the assistance of Mr. J. B. Millar, of Owens College,
whose ears were rather better than mine, although 1 am not aware cJ
any deficiency in this respect. The experiments were all made in the
same place, a flat meadow of considerable extent.
The Qraeral Raalts of the Eit^periiMiUt.
De La Eoche*, in his experiment, found that the wind produced least
effect on the sound at right angles to its direction, t. e. sounds could be
heard furthest in this direction. His method of experimenting, however,
was not the same as mine. He compared the sounds from two equal
bells, and in aU cases placed the bells at such distances that the sounds
were equally distinct. I, on the other hand, measured the extreme
distance at which the sounds could be heard, the t«8t being whether or
not the observer noticed a break in the continuity of sound, a stoppage
of the beU. The difference in our method of experimenting accounts for
the difference in our results. I found in every case that the sound could
be heard further with the tvind than at right angles to its direction; and
when the wind was at all strong, the range with the wind was more than
double that at right angles. It does not follow, however, nor was the
fact observed, that at comparatively short distances the soimd with the
wind was more intense than at right angles.
The explanation of this feet, which was fully borne out by all the ex-
periments, is that the sound which comes in immediate contact with the
ground is continually destroyed by the rough surface, and the sound from
above is continually diverging down to replace that which has been
* Annalea de Chimie, vol. i. p. Ml QlftV^V
688 Profi O. Beynoldi m the
destroyed. These diyerging waves are in tiieir torn destroyed ; 80 that
there is a gradual weakening of the intensity of the waYes near tlw
ground, and this weakening extends upwards as the waYes piooeed.
Therefore, under ordinary drcumstanoes, when there is no wind the
distant sounds which pass above us are more intense than those wliieh
wo hear. Of this fact I have abundant evidence. On the 6th, when the
wind was light, at all distances greater than 20 yards from the bell the
sound was much less at the ground than a few feet above it ; and I was
able to recover the sound after it had been lost in every direction fay
mounting on to a tree, and even more definitely by raimng the bell on to
a post 4 feet high, which had the effect of doubling the range of the
sound in every direction except with the wind, although even in this the
range was materially increased.
It is obvious that the rate at which the sound is destroyed by the
ground will depend on the roughness of its surface. Over grass we
might expect the sound at the ground to be annihilated, whereas over
water it would hardly be affected. This was shown to be tiie case fay
the difference in the range at right angles to the wind over grass, and
over the same ground when completely covered with snow. In the
latter case I could hear the sound at 200 yards, whereas I could only
hear it at 70 or 80 in the former.
Now, owing to the fact that the sound is greater over our heads than
at the ground, any thing which slowly brings dowTi the sound will
increase the range. Hence, assuming that the action of the wind is to
bring down the sound in the direction in which it is blowing, we see
that it must increase its range in this direction. And it must also be
seen that in this direction there will be less difference in the intensity of
the sound from the ground upwards than in other directions. This
was observed to be the case on all occasions. In the direction of the
wind, when it was strong, the sound could be heard as well with the head
on the ground as when raised, even when in a hollow with the bell hidden
from view by the slope of the ground ; and no advantage whatever was
gained either by ascending to an elevation or raising the bell. Thus,
with the wind over the grass the sound could be heard 140 yards, and
over snow 360 yards, either with the head lifted or on the ground ;
whereas at right angles to the wind on all occasions the range was
extended by raising either the observer or the bell.
It has been necessary to notice these points ; for, as will be seen, they
bear directly on the question of the effect of elevation on the range of
sound against the wind.
Elevation was found to affect the range of sound against the wind in
a much more marked maimer than at right angles.
Over the grass no sound could be heard with the head on the ground
at 20 yards from the bell, and at 30 yards it was lost with the head 3 feet
from the ground, and its full intensity was lost when standing erect at
i
Refraction of Sound by the Atmosphere. 539
30 Tarda. At 70 yards, wlien standing erect, the sound was lost at long
intervaJs, and waa only faintly heard even then ; but it became continuaua
again when the ear was raised 9 feet from the ground, and it reached its
full intensity at an elevation of 12 feet.
Over the snow similar efEecta were observed at very nearly equal
distances. There waa this diSerence, however, the sound was not
entirely lost when the head was lowered or even on the ground. Thus
at 30 yards I could still hear a faint sound. Mr. Millar could hear this
better than I could; he, however, experienced the same increase on
raising his head. At 90 yards I lost the sound entirely when standing
on the ground, but recovered it again when the ear waa 9 feet from the
ground. Mr. Millar, however, could hear the sound very faintly, and at
intervals, at 160 yards ; but not with his head on the ground. At this
point 1 was utterly unable to hear it ; and even at an elevation of 25 feet
I gave it up as hopeless. However, as Mr. Millar by mounting 10 feet
higher seemed to hear it very much better, I again ascended ; and at an
elevation of 33 feet from the ground I could hear It as distinctly as I
had previously heard it when standing at 90 yards from the bell. I
could not hear it 5 feet lower down ; so that it was the last 5 feet which
had brought me into the foot of the wave. Mr. Millar experienced the
same change in this 5 feet. As the sound could now bo heard as strong
as at a corresponding distance with the wind, we thought we had reached
tiie full intensity of the waves. This, however, was not the case ; for
the least raising of the bell was followed by a considerable intensifying
of the sound ; and when it was raised 6 feet I could hear each blow of the
hammer distLoctly, although just at that time a brass band was playing
in the distance. It seemed to me that I could hear it as distinctly as at
30 yards to leeward of the bell. All these results were repeated on
both days with great uniformity.
When more than 30 yards to the windward of the hell, the raising of
the bell was always accompanied by a marked intensifying of the sound,
and particularly over the grass, I could only hear the boil at 70 yards
when on the ground ; yet when set on a post 5 feet high I heard it
160 yards, or more than twice the distance. This is a proof of what I
previously pointed out, that the waves rise faster at the ground than they
do high up, and crowding together they intensify. In all cases there was
an unmistakable greater distinctness of the sound from short distances to
windward than to leeward or at right angles.
Except when the sound was heard with full force it was not uniform.
The bell gave two sounds (the beats of the hammer and the ring) which
could be easily distinguished ; and at times we could hear only the ring,
and at others the beats. The ring seemed to preserve itself the longest ;
whereas near the ground at short distances the ring was lost first. This
is explained by the fact that the rate at which sound-waves divei^
depends upon t^eir note : the lower the note the moce wULt^iK^ 4K4<b-c^.
640 Prof. O. Reynolds m the
Thus the beats diverge more rapidly than the ring, and conaequentiy
out sooner ; whereas when the head is on the ground near the bell it is
only the diverging waves that are heard, and here the beats have the
best chance. The intensity of the sound invariably seemed to waver ;
and as one approached the bell from the windward side, the sound did
not intensify uniformly or gradually, but by fits or jerks ; this was the
result of crossing the rays' interference, such as those shown in fig. 2.
During the observations the velocity of the wind was observed &om
time to time at points 1 foot and 8 feet above the sur&oe.
On the 9th, that is over grass, it varied from 4 feet per second at
1 foot and 8 feet per second at 8 feet, to 10 feet at 1 foot and 20 feet at
8 feet, always having about twice the velocity at 8 feet that it had at
1 foot above the ground.
• Over the snow there was not quite so much variation above and below.
On the 10th the wind varied from 3 feet at 1 foot to 4 feet at 8 feet*. On
the 11th the variation was from 12 at 1 foot and 19 at 8 feet to 6 at 1 foot
and 10 at 8 feet. Thus over snow the variation in the velocity was only
about one third instead of half.
Since the foregoing account was written, I have had an opportunity of
experimenting on a strong west wind (on the 14tii of March) ; and the
results of these experiments are, if any thing, more definite than those of
the previous ones. The wind on this occasion had a velocity of 37 feet
per second at an elevation of 12 feet and of 33 at 8 feet and 17 at 1 foot.
The experiments were made in the same meadows as before, the snow
having melh^d, so that the grass was bare.
With the wind I could h(jar the boll at 120 yards, either with the bell
on the ground or raised 4 feet above it. At right angles to the direction
of the wind it ranged about 60 yards with the bell on the ground, and
80 yards when the bell was olovat(?d.
To windward, with the hell standing on the ground (which, it must be
rememliered, means that the bell was actually 1 foot above the surface),
the sound was hoard as follows : —
Full. Lost.
AVith the head close to the ground. . At 10 yards. At 20 yards.
Standing >» 30 „ ,» 40 „
At an elevation of 25 feet Not heard at 90 yards.
With the bell at an elevation of 4 feet G inches : —
Full Lost
Head to the ground At 18 yards. At 30 yards.
Standing up », 40 „ „ 60 „
At an elevation of 12 feet »i 90 „
At an elevation of 18 feet „ 90 „
These results entirely confirm those of the previous experiments ; and
the intensifying of the sounds to windward by the raising of the bell was
* The wind fell rapidlj towards the close of Ihe obserrations on this day.
Refraction qf Sound bp the AtmotpHere. 641
erea more marked than before ; for at 90 yards to windward, with the
bell raised, I could bear it much more dintiactly thau at a corresponding
distance to leeward. This tact calls for a word of special explanation ; it is
clearly doe to the fact that the variation in the velocity of the air is much
greater near the ground than at a few feet above it. When the bell is
on the ground all the sound must pass near the ground, and will all be
turned up. to a nearly equal extent ; but when the bell is raised, the rays
of sound which proceed horizontally will be much less bent or turned up
tttan those which go down to the ground ; and consequently, after pro~
oeeding some distance, these raya will meet or cross, and if the bead bi
at this point tbey will both fall on the ear together, causing a sound of
double intensity. It is this crossing of the rays also which for the most
part causes the interference seen in fig, 2.
These experiments establish three things with regard to the transmia-
aion of sound : —
1. That when there is no wind, sound proceeding over a rough surface
is more intense above than below.
2. That as long as the velocity of the wind is greater above than
below, soimd is lifted up to windward and is not destroyed.
3. That under the same drcumstauces it is brought down to leeward,
and hence its range extended at the surface of the ground.
These experiments also show that there is less variation in the velocity
of the wind over a smooth surface than over a rough one.
It seems to me that these facta fully confirm the hypotheses propounded
by Prof. Stokes, that they place the action of wind beyond question, and
that they aSord explanations of many of the anomalous cases that have been
observed ; for instance, that sounds can be heard much further over wat«r
than over land, and also that a light wind at sea does not appear toaffect
sound at aU, the fact being that the smooth water does not destroy either
the Bound or the motion of the air in contact with it. When the wind
and sea are rough the case is different.
The Effect of Variations of Temperature.
Having observed how the wind acts to lift the waves of sound by
diminishing their velocity above compared with what is below, it was
evident to me that any other atmospheric cause which would diminish
the velocity above or increase that below would produce the same effect,
viz. would cause the waves to rise.
Such a cause must at certain times exist in the variation in the condi-
tion of the air as we proceed upwards from the surface.
Although barometric pressure does not affect the velocity of sound,
yet, as is well known, the velocity of sound depends on the temperature',
* It THieauUi«*qtuirerootof K- — tt—, and ooTueqiMnUy u the square root of tJie
642 Pnrfl O. Bejmoldi m tke
and everj degree of tempentuie between SSPand 70^ adds mpfproxanaUif
1 foot per second to the yelodtjr of sound. This vdocity also increases
with the quantity of moistore in the air; bnt the quantity is at all times
too small to produce an appreciable result. This yapomr nererthdess
plays an important part in the phenomena under consideratioii ; for it
gives to the air a much greater power of radiating and absorbing heat^
and thus renders it much more susceptible of changes in the acCaoo of
the sun.
If, then, the air were all at the same temperature and equally satorated
with moisture, the yelocity of sound would be the same at all elevations;
but if the temperature is greater, or if it contains more water below than
above, then the wave of sound will proceed quicker below than above,
and will be turned up in the same way as against a wind. This action
of the atmosphere is, strictly speaking, knalogous to the refraction of
light. In light, however, it is density which retards motion ; temperaturs
and pressure have little or nothing to do with it ; and since the density
increases downwards, the rays of light move slower below Uma they do
above, and are therefore bent downwards, and thus the distance at whidi
we can see objects is increased. With sound, however, since it is tempo*
roture which afiPects the velocity, the reverse is the cose ; the rays are
bent upwards, and the distance from which we can hear is reduced.
It is a well-known fact that the temperature of the air diminishos as
we proctH?d upwards, and that it also contains less vapour. Hence it
follows that, as a rule, the waves of sound must travel faster below than
they do abovo, and thus be refracted or turned upward.
The variation of temperature is, however, by no means constant, and a
little consideration serves to show that it will be greatest in a quiet
atmosphere when the sun is shining. The sun's rays, acting most
powerfully on that air which contains the most vapour, warms the lower
wtrata more than those above them ; and besides this, they warm the sur-
face of the earth, and this warmth is taken up by the air in contact with
it. It is not, however, only on such considerations as these that we are
in a position to assert the law of variation of atmospheric temperature.
Mr. Glaisher has furnished us with information on the subject which
places it beyond the region of siumise.
I extract the following from his " Eeport on Eight Balloon Ascents in
18()2" (Brit. Assoc. Rep. 18(;2, p. 402) :—
" From these results the decline of temperature when the sky was
cloudy
For the first 300 feet was 0°-5 for every 100 feet.
From 300 to 3400 „ 0°-4
„ 3400 to 5000 „ 0°-3 „ „
" Therefore in cloudy states of the sky the temperature of the air
decreased nearly uniformly with the height above the surface of the earth
nearly up to the cloud.
Refiaction of Sound by the Atmotphere. 548
" When the akj was putiallj cloudj the decline of tfimpenture
In the frat 100 feet was 0°'9
From 2900 to 5000 „ 0°-3 for every 100 feet.
"The decline of temperature near the earth with .a partially clear sky
is nearly double that with a cloudy sky,
" In some cases, as on July 30th, the decline of temperature in the first
100 feet was as large as l"-!."
"We may say, therefore, that when the sky is clear the variation of
temperature as we proceed upwards from 1 to 3000 feet will be more
than double what it is when the skyis cloudy. And since for such small
variations the variation in the velocity of sound, that is the refraction, is
proportional to the temperature, this refraction will be twice as great with
a clear sky as when the sky is cloudy.
This is the mean difference, and there are doubtless exceptional caaes
in which the variations are both greater and less than those given ; during
the night the variations are less than during the day, and again in winter
than in summer.
This reasoning at once suggested an explanation of the well-known
fact that sounds are less intense during the day than at night. This is a
matt«r of common observation, and has been the subject of scientific
inquiry. F. De La Boche discusses the subject, and exposes the fal-
lacies of several theories advanced to account for it. Amongst others
there are some remarks by Humboldt, in which he says that the dif-
ference is not due to the quietness of the night, for he had observed
the same thing near the torrid zone, where the day seemed quieter than
the night, which was rendered noisy with insects.
It is, however, by the experiments of Prof. Tyndall that this fact has
been fully brought to light ; and from their definite character they afford
an opportunity of applying the explanation, and furnish a t«Bt of its
soundness.
Neglecting the divergence of the bottom of the waves, a difference of
1 degree in the 100 feet would cause the rays of sound, otherwise hori-
Eontol^ to move on a circle, the radius of which by the previous rule
= 1100 . ■1^»110,000 feet. A variation of one half this would cause
them to move on a circle of 220,000 feet radius. From the radii of these
circles we can calculate the range of the sound from different elevations.
With a clear sky, i. e. with a radius 110,000 feet from on elevation of
236 feet, the sound would be audible with full force to 1-36 mile ; the
direct sound would then be lifted above the surface, and only the di-
verging sound would be audible. From an elevation of 15 feet, however,
the direct sound might be heard to a distance of '36, or ^ mile further,
so that in aU it could be heard 1-72 (1 j) mile.
Witli a cloudy sky, t. e. with a radius 220,000 feet, the direct «stsiA
644 Prof. O. Beynolds m ike
would be heard to 2*4 miles from an elevation of 15 feet, or 1*4 tunes what
it 18 with the clear skj. These results have been obtained bj taking the
extreme variations of temperature at the surface of tiie ettrth. At
certain times, however, in the evening, or when it was raining, the wiatioiL
would be much less than this, in which case the direct sound would be
heard to much greater distances.
[So far I have only spoken of the direct or geometrical rays of aoond,
that is, I have supposed the edge of the sound to be definite, and not
fringed vidth diverging rays ; but, as has been already explained, the
sound would diverge downwards, and from this cause would be heard to
a considerable distance beyond the point at which the direct rays first
left the ground. Erom Uiis point, however, the sound would become
rapidly fainter until it viras lost. The extension which divergence would
thus add to the range of the sound would obviously depend oa the re-
fraction— that is to say, when the direct rays were last retracted apwards,
tiie extension of the range due to divergence would be greatest. It is
difficult to say what the precise effect of this divergence would be; but we
may assume that it would be similar to that which viras found in tihe case
of wind, only the refraction being so much smaller the extension of the
range by divergence would be greater. On the wh(^ the results calcu-
lated from the data furnished by Mr. Glaisher agree in a remarkable
manner with those observed ; for if we add | mile for the extension of
the range by divergence, the calculated distuice with a clear sky would
be two miles from a cliff 235 feet high. — September 1874.]
Now Prof. Tyndall found that from the cliffs at the South Foreland,
235 feet high, the minimum range of sound was a little more than
2 miles, and that this occurred on a quiet July day with hot sunshine.
The ordinary range seemed to be from 3 to 5 miles when the weather
\i'as duU, although sometimes, particularly in the evening, the sounds
were heard as far as 15 miles. This was, however, only under very ex-
ceptional circumstances. Prof. Tyndall also found that the interposition
of a cloud was followed by an almost immediate extension of the range
of the sound. I extract the following passages from Prof. Tyndall s
Eeport : —
'* On June 2 the maximum rauge, at first only 3 miles, afterwards ran
up to about 6 miles.
'' Optically, June 3 was not at all a promising day ; the clouds were
dark and threatening, and the air filled with a faint haze ; nevertheless
the horns were fairly audible at 9 miles. An exceedingly heavy rain-
shower approached us at a galloping speed. The sound was not sensibly
impaired during the continuance of the rain.
'* July 3 was a lovely morning : the sky was of a stainless blue, the air
calm, and the sea smooth. I thought we should be able to hear a long
way off. We steamed beyond the pier end and listened. The steam-
clouds were there, showing the whistles to be active ; the smoke-puffs
BefractioH of Sound by the Atmosphere. 545
were there, attestiug the activity o£ the guns. Kothiug waa heard. We
went nearer ; but at two miles horna and whistles and gims were equally
inaudible. This, howerer, being near the limit of the sound-shadow, I
thought that might hare something to do with the effect, bo we steamed
right in front of the atatiou, and halted at 3| miles from it. Not a
ripple nor a breath of air disturbed the Htillness on board, but we heard
nothing. There were the ateam-puffs from the whistlea, and we knew
that between every two puffs the hom-souuds were embraced, but we
heard nothing. We signalled for the guns ; there were the smoke-puffs
apparently close at baud, but not the slightest sound. It was mere
dumb-show on the Foreland. We steamed in to 3 miles, halted, and
listened with all attention. Neither the boms nor the whistles sent us
the slightest hint of a sound. The guns were again signalled for ; five
of them were fired, some elevated, some fired point-blank at us. Not one
of them was heard. We steamed in to two miles, and had the guns
again fired ; the bowitser and mortar with 3-lb. charges yielded tbe
faintest thud, and the 18-pounder was qiiite unheard.
" In the presence of these facts I stood amazed and confounded ; for it
had been assumed and affirmed by distinguished men who had given spe-
cial attention to this subject, that a clear, calm atmosphere was the beat
vehicle of sound : optical clearness and acoustic cleomesa were supposed
to go hand in hand * * *.
"As I stood upon the deck of the 'Iren^' pondering this question, I
became conscious of the exceeding power of tbe sun beating against my
back and heating the objects near me. Beams of equal power were
foiling on the sea, and must have produced copious evaporation. That
the vapour generated should so rise and mingle with the air as to form
an absolutely homogeneous mixture I considered in the highest d^roe
improbable. It would be sure, I thought, to streak and mottle the
atmosphere with spaces, iu which tbe tur would be in different degrees
saturated, or it might be displaced by the vapour. At the limiting sur-
faces of these spaces, though invisible, we should have the conditions
necessary to the production of partial echoes, and the consequent waste
of sound.
" Curiously enough, the conditions necessary for the testing of this ex-
planation immediately set in. At 3.15 p.u. a cloud threw itself atliwart
fte sun, and shaded the entire space between us and the South Fore-
land. The production of vapour was checked by the interposition of this
screen, that already in the air being at the same time allowed to mix
with it more perfectly ; hence the probatnJity of improved tnuumiasion.
lo test this inference the steamer was turned and urged bock to our
last position of inaudibility. The sounds, as I expected, were distinctly
tiioogh faintly heard. This was at 3 miles distance. At 3| miles we
had the guns fired, both point-blank and elevated. The faintest thud
WIS all that we heard ; but we did hear a thud, whereas we bad i}K'da>u.\^
546 Prof. O. Bejmolds m the
heard nothing, either here or three qnarteni of a mile nearar. We
steamed out to 4| miles, when the sounds were for a moment hinOj
heard, but thej fdl away as we waited ; and though the greatest quiet-
ness reigned onboard, and though the sea was without a ripple, we ooold
hear nothing. We could plainly see the 8team-pu& which azmonnoed
the beginning and the end of a series of trnmpet-Uasts, but the blasts
themselves were quite inaudible.
'^ It was now 4 p.m., and mj intention at first was to halt at this dif
tanoe, which was beyond the sound-range, but not far beyond it, and see
whether the lowering of the sun would not restore the power of the
atmosphere to transmit the sound. But after waiting a little, the an-
choring of a boat was suggested ; and though loth to lose the anticipated
reviyal of the sounds myself, I agreed to this arrangement. Two men
were placed in the boat, and requested to give all attention, so as to hear
the sound if possible. With perfect stillness around them, they heard
nothing. They were then instructed to hoist a signal if they should hear
the sounds, and to keep it hoisted as long as the sounds continued.
'* At 4.45 we quitted them and steamed towards i^e South Sand Head
light-ship. Precisely fifteen minutes after we had separated from them
the fiag was hoisted. The sound, as anticipated, had at length succeeded
in piercing the body of air between the boat and the shore.
** On returning to our anchored boat, we learned that when the flag was
hoisted the hom-sounds were heard, that they were succeeded after a
little time by the whistle-sounds, and that both increased in intensity as
the evening advanced. On our arrival of course we heard the sound:}
ourselves.
** The conjectured explanation of the stoppage of the sounds appeared
to be thus reduced to demonstration ; but we pushed the proof still
further by steaming further out. At 5 j miles we halted and heard the
sounds. At 0 miles we heard them distinctly, but so feebly that we
thought we had reached the limit of the sound-range; but while we
waited the sound rose in power. We steamed to the Yarne buoy, which
is 7 j miles from the signal-station, and heard the sounds there better
than at G miles distance.
" Steaming on to the Vame light-ship, which is situated at the other end
of the Vame shoal, we hailed the master, and were informed by him that
up to 5 P.M. nothmg had been heard. At that hour the sounds began to
be audible. He described one of them as ' very gross, resembling the
bellowing of a bull,' which very accurately characterizes the soiuid of the
large American steam-whistle. At the Vame light-ship, therefore, the
sounds had been heard towards the close of the day, though it is 12|
miles from the signal-station."
Here we see that the very conditions which actually diminished the range
of the sound ^^ere precisely those which would cause the greatest lifting
of the waves. And it may be noticed that these facts were observed and
■Refraction of Sotmd by tfu Atmosphere. 947
recorded by Prof. Tyndall with his mind altogether tmbimed nith any
thought ot eHtabliahiiig this hypothesis. He was looking for an expla-
nation in qoite another direction. Had it not been so he would probably
have ascended the inait, and thus found whether or not the sound was
all the time passing orer his head. On the worst day an ascent of
30 feet should have extended the range nearly ^ mile.
The height of the sound-producing instruments is apparently treat«d
as a subordinate question by Prof. Tyndall. At the commencement of
his lecture, he stated that the instruments were mounted on the top and
at the bottom of the cliff ; and he subsequently speaks of their being
235 feet above him. He does not, however, take any notice of the com-
parative range of those on the top and those at the bottom of the cliff ;
but wherever he mentions them he speaks of them as on the cliff, lead-
ing me to suppose that for some reason those at the bottom of the cliff
had been abandoned, or that they were less efficient than those above.
If I am right in this surmise, if the sounds from below did not range so
far as those from above, it is a fact in accordance with refraction, but of
which, I think, Prof. Tyndall has offered no explanation.
[Besides the results of Prof. Tyndall's experiments there are many
other phenomena which are explained by this refraction. Humboldt
could hear the falls of Orinoco three times as loud by night aa by day
at a distance of one league ; and he states that the same phenomenon has
been observed near every waterfall in Europe. And although Humboldt
gave another explanation*, which was very reasonable when applied to
the particular case at Orinocot, yet it must be admitted that the circum-
fltances were such as would cause great upward refraction ; and hence
there can be but little doubt that refraction had a good deal to do with
the diminution of the sound by day.
In fact if this refraction of sound exists, then, according to Mr,
Glaisher's obsenafions, it must be seldom that we can hear distant
sounds with anything like their full distinctness, particularly by day;
and any elevation in the observer or the source of the sound above the
* " That the lun itcts upon the propagation and inteosit; of aound by the obatAcles
met incmmits of air of different densitf, aod by the partial unduJatioas of the atmo-
■l^ere arinng'f^^jm uneqiinl heating of different parts of the Mil During the
iaj there a d ludden interruption of dengitj whereTeramaUatreamletBofairof ahigh
temperatiiTe riae orer parts of the aoil uneqiudlj heated. The aonoroui undulations are
divided, as the rajs of light are refracted wherever strata of air of unequal denritj are
eoDtigoone. The propagation of sound ie altered when a stnttum of hjdrogen gas is
made to rise over a atrntum of atniospherio air in a tube closed at one end ; and H.
ffiot has well explained, by the iuterpositionof bubUee ofcafboaio acid gas, why a glow
filled with champagne is not aonorous so long aa that gas is evolved and paaauig through
the strata of the ]iqmd:'—Humioldea IVavels, Bohn'a Series, vol. ii. p. 264.
t The sounds proceeded over a phuie covered with rank vegetation interspersed with
black rocks. Then latter attained a very considerable elevation of temperature under
tlie eflitcts of the tropical sun, asmueh as 48° C, while the air was only 28°; and hence
over each rock there would be a (xdumn of hot air Moen^ttg.
TOL. nil. ^ "S
548 On the RtfracluM ofSomdbg tke Atmotpbere.
interreniiig ground will increase tbJB ruige and diKtinctneas, as niU a)>o
a gentle niod, which brings the eoitnd doui) and so oount^nifta the
effect of refraction. And heuoe we have an explanation ot the snrpnsiiig
diatoncee to which sounds can gometimei be heard, particularlv' th^ ex-
ploaion of meteors, as well as a reason for the cnstom of eleratiag churvb-
bells aad souuda to be heard at great distanoua, — SejiUmbrr 1S74.]
INDEX TO VOL. XXII.
AbBL (F. a.), oontrfbutlona to the
hiEtoiTof (OWMtTe want*: MOond ntft-
moir, 160.
and Sable (Oapt,). nMu-diw oo
explodTei : Seed gimponder, 406.
Absorption phonomann, on k new dnn Qf,
378.
. — speotn of potanum and todium at
low («iDp«mtiirM, on ths, iSOS.
Actinia, <uith»j)tirToanjd»atot: FurtL,
44,283.
Addreu of the Preadent, 2.
AdiabaUos and itothennali of wat«r, on
the.4fil.
A^ta, onaxploai
&il
AlimenlAiT oanal, on the minnte anatomT
ofthftWS.
AUmaii(pTof.), TO^ medal awarded to, 1 1 .
Alps, on Boma winter thermometiio ob-
■eiratioD* in the, 317.
Anatomy of the geniu PArontno, on the,
154.
. .1 of tbeljmphaCioiyiteDiof thelnngi,
oontributiona to the normal and patho-
logioal,133.
Annireraarj Meeting, Deo. 1, 1879, 1.
Atlantic, South, on drediriDgi and deep-
■ea toundingi in the, 423.
Atmoephera, non-homogeneoua, on the
■toppaEe of Mund bj partial refleotioni
ina,^.
—, on the nfinotion of Hund br the,
265, C31.
, prelimiiuuy tMOU&t of an inTeeti-
^51
Auditon, Beport of, 1.
ed.297.
Barlow (W. U.) on the pneumatie lutioii
which aooompaniei the articulation of
loundl bj the human Tcdoe, na exhibited
b;r a Tcoording inaCrument, 277.
Beddoe (J.), admitted, 27.
Blanford (W. T.), admitted, 362.
(H. P.), the windi of Horthern
India, in lelation to the tempeiatura
and Tapour-oonatituent of the atmo-
■phere, 21 IX
Blood, on some poinla oonnected with the
dnmlatioQ or the, oniTed at from a
•tad; of the >phv|mogra^h-tra«e, 201.
oorpuades m Mammalia, on the in-
tnoellular development of, 243.
Bodily tsmperatuie, Ac, of healthy men,
on the iaSuence of biandy on ths, 172.
Bmdj (a. B), admitted, 380.
Btaio, on the looaliiation of function in
the, 229.
Bnudy, on the inSucnce of, on the bodily
temperature, the pdIh^ and the rMpf-
rotiona of healthv men, 172.
Brodie (Sir B. 0.) on Ibe ^nllutli of
formic aldehyde, 171.
Brom-iodidee, on the, 51.
Broun (J. A.\ on the lumaal vaiiadon of
the magnetic deolination, 254.
on the period of hemispheial (ooeM
of lun-Bpota, and the 29-day period, 43.
on the imi«>ot period via lite taiu-
fWll,460.
Brunton (T. L.), admitM, 362.
and Payrer (J.) on the nature and
phyiiologiral action of the poiaon of
Mfja Mpudiant and other udian Ta-
nomoue nukM ; Put IL, 68.
and Power (H.) on the diuretic
action of DigUalit, 420.
Buchanan (J. 7.) on the absorption of
carbonic ooid bj Mlioe wilationjk 192,
483.
, lonLG obeervationi on aea-water ice,
431.
Calculus of factorioU, on the, 434.
Candidat«* for election, lilt of, Moreh 6,
1874, 228.
wlwted, liat of, Moy 7, 1874, 810.
2t2
550
IXOEX.
OAriKHue aod, on the timorpdtm oi, bt
nlme Mlntkiu. 19S, 4^
Oudwdl QU. Hon. E.X dMtcd, 42; ad-
iiuttod,211.
Onre-depofiu of Eki^bnd, on the aDmd
cxutenee of rnnuBt of alcDmimg in, &1.
CMcj (Prof.), a memoir on the tnnt-
/ormation of cUiptie fmietioni, 56l
Centre of motion in the hmnan ere, on
the, 429.
Cerebnd hemiipherei, on the cxotatian
of the farfree of the, bj indueed ear-
icntat 9qo«
Chemiol action of total dajU^, on the,
156.
— eoutitntion of Mhne eolntioni^ on
the, 2».
Chinoline and pyridine Imam, on the pfaj-
giolficied action of the, 432.
Clif<nnf (W. K.). admitted, 382.
Coal-iminw, on the foail planta of the.
Colour, on the combiiiaHone of, bj meant
of polaiiaed light. 3ML
Coniferine, on, and ita eonrernon into
the aromatic principle of vanilla, tM.
Connectire timne. nerre, and mvcde, on
the anatomy of. with ipecial refemee
to their eonnenon with the Innphatie
mtem. 380, 515.
Contributions to the historr of the orrinfi :
Ho, TV. On the iodo-deriratiTee of the
orcins, 53.
to the hietorv of explosiTe ogents :
Bccond uxnnoir, l60.
to the deTelopniental historr of the
Mollusca : Sections I.-IV., 232'
■ to terretl rial magnetism : "So. XIV.,
401.
Copley medal awarded to H. L. F. Hebn-
holtz, 10.
Copper wire, preliiiiinanr experiments on
a magnet ixed, 311.
Cottrell (J.) on the division of a eound-
waTe by a layer of flame or heated gas
into a reflected and a transmitted ware,
190.
Coundl, list of, 12.
Crrxikes (W.) on the action of heat on
grayitating masses, 37.
Croonian Lecture announced, 297.
Daylight, total, on a self-recording me-
tliod of measuring the intensity of the
chemical action of, 158.
Decherrens (M.), magnetic obflerrations
at Zi-Ka-Wei, 440.
Declination, on the annual rariation of
the magnetic, 254.
Deep-sea thermometer, on a new, 238.
Development , on the, oi Pcrivatus capen-
iM,344. I
DigUJia, on the diniccie nelkm oC 4SDl
oftbe
211R.
tkn of AyAtfi^ OB tbe. 4S0L
Donkan (.A. B.) on an inH H fiir thi
minncMtinn of two
IMl
BonUe TClbMtiQB. an,
m mouona 4flL
DivdcDMi and deco'^en aoonoinasi m tin
South AthBtiCi on, 42S.
Donean (P. IL) on tlie aerraoa ayiCcB of
FM L, 44, 989.
Buth. on th* motioni of ^vna of tht
nebobe towaide or fvom tfaa^ SSL
Election of FdlowB, 961.
Eleetiie condiieton» on the ■liiitii— of
on, 57.
Klliptic fimftioWfc on the
0^56.
Ezpenmcnta with nCetr-lampa, 441.
Ezploeire agents, contributions to the
history of: second memoir, 160.
Explosives, researches on : fired gun-
powder, 41^?.
Factorials, on the calculus of. 4M.
Fayrer (J.) and Brunt un (T. L.) on the
nature and ^hyeiolcigioal action of the
poison of ^aja trijntdians and <<ther
Indian renomous snakes : Part II.. 08.
Fellows deceased. 1 ; elected, 2, ^'Gl ;
number of. 13.
Ferrier (DX the localisation of function
in the brain. 22*A
Financial statement. 14, 15.
Fireman's respirator, on eome recent
experiments with a. Syx
Forced breathing, on the bending of the
ribs in, 42.
Forces, on the. caused by CTaporation from,
and Condensation at.' a surfiM^e. 44>1.
Formic aldehyde, on tbesyntheeis of. 171.
FoMil plants of the coal-moosurea, on the
or^nization of the : Part VI. Ferns,
24d.
Frankland (£.) on eome winter thermo-
metric obeenrations in the Alpe, 317.
Franks (A. W.). admitted, 380.
Function in the brain, on the looalixation
of, 229.
Qalapagoe Islandst on the tortoisea of the.
421.
Qallomy (W.), eiperimmU wilh i»fety-
lamp«,441.
Owrod (A. H.) on aome poiata oonneoUd
nith the drcuUtion of the blood, nr-
lired at from a, atudj of the aphjgmo-
graph-traoe, 291.
Cwological Bgee (or groupc of formatioiiB),
on the compaTatiTe value of certain,
COondered as item* of Reolceical time,
145.334.
Oore (Q.) on electrotoraon, 57.
on the ottnctioDi of nuigneta and
dectrio eonduoton, 245.
(Joremment Qrant, account of appropri-
ation of, 1873, 19.
Gravitating maaBee, on the action of h»at
on, 37.
Grabb (T.) on the jroproremeat of the
Gunpowder.'on fired, 40e.'
Gunther (A.), deacription of the liTing
and eitinot raoee of gigantic lond-tor-
toiaee : Farts I. & II. Introduction, and
the tortoises of the Oalspagos lalanda,
421.
Haannann (W.) and Tiemann {P.) on eo-
niferine, and its conTenion into the
aromatie priiujiplB of vanilla, 398.
Habits of the genus Phrtnima, on the,
154.
Hamonic curves, i
the chemical
ons, 241.
Hnt, on the action of, on gravitating
mssse>, 37.
Helmbolti (H. L. F.), Copley medal
awarded to. 10.
Hemispheres, cerebral, on the excitation
of the surface of the, bf induced cur-
i-spots, on the
HemiBpheral excess of
period of, 43.
Hemmeej (J. H. N.) on displacement of
the >oUr spectrum, 219.
on nbite linee in the solar cpectrum,
321.
n the periodicity of rainfall, 286.
Howard (J. E.), admitted,
Huggins (W.) on the motions oi some oi
the oebulie towards or from the earth,
_261.
Human eye, on the centre of motion in
the, 429.
— < — — voice, on the pneumatic action which
aooompanice the articulation of sounds
l^ the, as exhibited liy a r^oording in-
~ mrav (J
300.
India, on the winds of northern, in rela-
tion to the temperature and vapour-
constituent gf the atmosphere, 210.
Indian venomoua snakes, on the poison
of, 68.
lodo-derivatives of the orcins, on the, 53.
Isothermals and adiabatics of water, on
the, 451.
Eew Committee, report of the, 20.
Klein (B.), contributioiu to the normal
and pathological anatomy of the lym-
phatic system of the luugg, 133.
on the smallpoi of sluep, 388.
lAnd-lortoisn, on the livini and extinct
noes of: Parts L & II. Introduction,
and the tortoises of the Qalapagos Is-
lands, 421.
Lankeeter (E. B.), oontributions to the
developmental history of the Mollusoa ;
Sections L, U., HI., IV., 232.
Leaf -arrangement, on, 298.
Lemming, on the allied existanFe of re-
mains of a, in cave-<upoeits of England,
Liquid funon, on the alleged expansion in
volume of various substances in passing
by refrigeration from the state of, to
that of solid ideation.. 3G6.
Liquor sanguinis, on certain organisms
occurring in the. 391.
Lockyer (J. N,), rwearchee in spectrum-
annlygis in oonneiion with tbe spectrum
ottheiun: No. IV-, 391.
, spectroscopic notes : No. I. On the
absorption of great thioknenes of me-
tallic and metalloidal vapours, 371 ; No.
11. On the evidence of variation in mo-
lecular Btructure. 372 ; No. 111. On tiie
molecular structure of vapoure in con-
nexion with tfafir densitica, 374 ; No.
IV. On a new claM of absorption phe-
obserrations of the i
Logan (H. F. C.) on the calculus of (ac-
torials, 434.
Ijungs, contributions to the nonuol and
pathological anatamy of thu lympbntic
B;i1«moftbe, 133.
Lymphatic system, on the anatomy of
connective tissue, nerve, and muscle,
with special refcrenco (o their oon-
li the, S
), 515.
Macdonald (J. D.) on the analom; and
habits of the genus Fkrcmima (Lair.),
552
INDEX.
H'Eendrick (J. O.) and Dcwar (J.^ on the
pbjBiologioal action of the chinolme and
pyridine bases, 432.
Magnetic declination, on the annual Tari-
ation of the, 254.
obseryationB at Zi-Ka-Wei, 440.
liagnetiBm, on the 26-da7 period of ter-
restrial, 43.
Hagnetixed copper wire, experiments on
a, 311.
Magnets and electric conductors, on the
attractions of, 245.
Maine (Sir H. 8.), admitted, 380.
Male of Thaumois pHtucida, on the, 42.
Mallet (R.). addition to the paper "Vol-
canic energy : an attempt to develop
its true origin and cosmical relations,'
328.
■ on the alleged expansion in voliuno
of Tarious substances in passing bj re-
frigeration from the state of bquid
fusion to that of solidification, 3G6.
"■'— on the mechanism of Stpomboli, 473,
496.
Mammalia, on the intracellidar derelop-
nient of blood-corpuscles in, 243.
Maxwell (J. C.) on uouble refraction in a
viscous fluid in motion, 46.
Met'liauism of Stroraboli, on the, 473, 496.
Medals, presentation of the, 10.
Metallic and mctalloidal vapours, on
tlie absorption of great tliicknesscs of,
371.
Meteorological use of a planiraeter, 435.
MiUs (E. J.), admitted, 362.
Minute aiuitomy of the alimentary canal,
on the, 203.
Molecular structure, on the evidence of
variation in, 372.
' of vapours, on the, in connexion
witli their densities, 374.
MoUusca, contributions to the develop-
mental liistory of the, 232.
Moseley (11. N.) on tlic structure and de-
vclopiiiout of Pcripafv.s capnisis. 344.
Mucous mcmbrnuo of tlio uterus, on the
structure of the, and its pcriocUcal
changes, 297.
Kaja fripvdians and other Indian venom-
ous snakes, on the nature and physio-
logical action of the poison of, 68.
Nebulip, on tlio motions of some of the,
towards or frr)ui the oarth, 251.
Ncgrotti (TI.) and Zarabra (J. W.) on a
new deci)-f»oa thonuomcter, 238.
Korvous pvstcm of Actinia^ on the, 4-1,
^ 2(;3.
Kohlc (C.ipt .) and AIk.-1 (F. A.), ri'scan'lios
on explosives: fired gunpowder, 408.
Kumeric.'J vnhie of tt, on certain discrc-
pancies in the published, 45.
Obitnarr notioM of FbUowb deoeMed:—
Archibald Smith, i.
Obwrratioiif, ipeotro0oopie^ of tht m,
247.
Orcina, oontributionato tha hirtory of the:
No. rV. On the iodo-deriTmtirei of Um
onrins, 53.
Organisma, on certain, oocurxing uk the
uquor Banguinia, 391.
OsciUation, on the uxuform wst6 of, 350L
Osier (W.), an account of certain atptt
isma occurring in tha liquor w^ig""^
o91.
Owen (B.) on the alleged existenoe of n*
mains of a lemming in CBTo-deporiU of
Enghind, 364.
Parkes (E. A.) on the influence of brandy
on the bodiljr temperature, the pulie,
and the respirations of healthy men,
172.
Periodicity of rainfall, on the, 286.
Peripafus capenme, on the Btmcture and
development of, 344.
Perry (S. J.), admitted, 362.
Phronima, on the anatomy and habits of
the genus, 154.
Planimeter, on the employment of a, to
obtain mean values from the traces c^
continuou.«ly self-recording meteoro-
logical instruments, 435.
Poison of Naja fripudians nnd other In-
dian venomous snakes, on the nature
nnd physiological action of the, 68.
Polarized light, on the combinations of
colour by means of, 354.
Potassium aud sodium, on the absorption-
8i>eotra of, at low temperatures, 3»52.
Power (II.) and Bnmton (T. L.) on the
diuretic actiim of Dii/tfalis^ 420.
Presentjition of the medals, 10.
Presents, list of, 48, 148, 223, 258, 320,
473.
President's Address, 2.
Prestwieli (J.), tables of temperatures of
the sea at various depths bi'low ibo
surface, taken between 1740 and ISiW:
collated and reduced, ^ith notes and
sections, 402.
Prime, on the nimiber of figures in the
reciprocal of everv, between 20,000 and
30,000. 384.
number below 20,000, on the num-
lx>r of figures in the period of the reci-
procal of everj-, 2tX).
-, given the nuiiil>er of fipircs
(not exceeding UK.)) in the retMpnx^il of
a. to dotennine the prime itself. 381.
Pyridine nnd eliinoline bases, on the pht-
biologioal action of the, 432.
Kaiufall.^ou the periodicity of, 286.
Boinrall, on tbo nm-tpot period utd the,
469. r- r- -^
Bamuy (A. C.) on tlie oompusUre ralue
at certain gMilogical UM (or group* of
fonoatioiii) oonn^end m itemi of geo-
logioal time, 14&, 334.
ItanBome (A.) on the b«nding of the ribs
in foraed brotthing, 42.
Beport of Auditor*, 1.
of the Kew Committse. 20.
BflMarchu In ■pectnim-uiBlfgle in con-
nerion with lie ipertrum of the sun:
No. IV., 391.
Bopirator, on aoma recent experiments
with a fireman's, 359.
Bejnolds {O.) on the refraotion of iound
bj the atmosphere, 295, 531.
, on the forces oauied bj erapotation
from, and oondnuation at, a surfaoe,
401.
be (W\ atudies on bioeenMii. 289.
1 (H. £.), Boyal medol awanied to,
- — ' on a telf-reoording method of mea-
suring the intensity of the chemical
action of total dajlisht, 158.
— and Bohuster (A.) on the absorption-
spectra of potassium md sodium at low
temperatuK*, 362.
Bojal medal awarded to Prof. AUnan
and Prof. H. B. Boaooe, 11.
Biieker (A. W.) on the adi^otioa and iso-
thermals of water, 451.
Babine (Sir B.), contributions to terres-
trial magnetism : So. XIT., 461.
Safetj-lampe, experiments with, 441.
Ssline solutions, on the abaorption of tti-
bonicaddby, 192,483.
, preUminary notice of experi-
ments ooneemins the chemioal ooustl-
tuUon of, 241.
Selrin (O.), admitted, 38a
Sanderson (J. B.) on the natation of the
(ni&oe of the oerebral hemispheres by
Sehafer (B. A.) on the intraceUular deve-
lopment of blood-oorpusclea in Ubiq-
nialiu,243.
Schuster (A.) and Boscoe (H. B.) on the
abeorption-spectin of potasrium and
sodium at low temperatures, 3G2.
and Stewart (B.J, preliminary ei-
Seriments on a magnetized copper wire,
11.
Scott (B. n.) on the employment of a
planimeter to obtain mean tsIum from
the traces of oontinuously self-recording
meteorologieal instruments. 435.
Seo, lemperaturcB of the, at various depths
below the surface, taken between 1749
and 1868; ooUated and reduced, with
note* and sections, 463.
Sea-water ice, some obnerrations cm, 431.
"-'—'- (G. M.) and Looker (J. N,),
loopio Dbwrrations of tne sun.
, given the number of figure* (not
exoeeding 100) In the redprooal of a
iirime number, to determine the prime
taelf. 381.
on the number of Sgii
dprocal of erery prime M
and 30,000, 3S4.
Sheep, on the small-pox of, 388.
fiimpson (M.) on the bron-lodidM, 61.
Smith (A.), obituary notioe of, i.
Snakes, Indian Tenomoua, on the poison
of, 68.
Sodium and potassiuni, on the absorption-
speetm of, at low temperatuna, 3o2.
Solar spectrum, note on diiptaoement of
the,2l9.
, on white lines in tlut, 231.
Solid states of water-substance, a quantita-
tive investigation of certain relations be-
tween the gsseouB, the liquid,'and the.27.
Bound, on the refraction of, br the atmo-
sphere, 295, 531.
, on the stoppage of, I^ partial re-
fleotions in a non-homogeneout atmo-
sphere, 190.
, on the transmiMion of, I7 the atmo-
sphere, 58, 369.
wave, on the division of a, by a layer
of flame or heated gas into a refleoted
and a transmitted wave, 190.
Sounds, on the pneumatic action which
aoDompaniea the articulation of, bj the
human voios, 277.
Speotrosoope, on the improvement of the.
Bpeotroaoopic notee; So. I. On the ab>
sorptJon of great thioknuses of metallio
and mMAlloldal vapours, 371 ; No. II.
On the oridence of variation in mole-
cular structure, 372 ; No. III. On the
moleoular structure of vapours in con-
nexion with their densitiee, 374 ; No. IT.
On a new class of absorption pheno-
mena, 378.
Spectrum-analyiie, researches in, in oon-
neiion with the spectrum of the sun :
Ko. IV., 301.
neotad w^tbe dronlatiaDVClibeUMd.
■rrind It from a itn^ of lh^ 391.
Spottinrooda . (W.) on oomMnafiiw o(
ocdonr In idmim of polarind li^^ SM.
SUnlioQM (J.), oontrilwiBant lolbeliHtoiy
of tha OM^ : No. lY. On tlu iodo-
' deiintini of the orcuu, GS.
Btomrt (B.) Mid Bdiiatar (A.), pn-
ooppeririTB, 311.
BtrwnDoli, on tlie madutniim of, 473^496.
Stroebin and dDTsIopmaDt of Ptr^atui
capmuk, on Oie, 344.
of nmnupf waK«ia,oattw,42.
BtadiM «n biagdMia. 38ft
BnbrtMwai, on the aUcgad enaarion of
TaitotM, oo KilidiSatfioa, 30&
Bun, ipaetroaeopio otMarratkoa of ttic^
247.
^— ipat period end the ntn&U, on tlw,
469.
— •■pota, on the nariod of iMmirnhnml
eiM*« of, and ttte SB-day panod of
terraatttel Eugnetinn, 43.
SnrfiuM-napon^on and eondtnpaHon, m,
401.
Temneratone of the mb at TUJont depth*
below the mrfiioe, 4«2.
TerreBtrial raagnetiim, oontributioni to:
No. XIT., 461.
, on the 26-day period of,
43.
Thauvwpt peUadda, on the male, and Ihe
struct are of, 43.
Thennometer. on n ne« depp-tea, 238.
Thennomctrio obserTntioiu in tbe Alps,
on >ome winter, 317.
Thin (O.), a contribution to tbe anaUiniy
of conneotiTe tiuue, nerre, and muaole,
with special reference to their oonnoiion
with the lyniphaUo Bjetem, 380, 515.
ThomBOTi (J.), a quantilatiTe infeetigBtion
of certain relations between the gaseous,
the liquid, and Ihe solid stotee of water-
eubatance, 27.
(^0 on dredgings and deep^ea
soundings in the South Atlantic, 423.
~" m (F.) and Haarmann ^W.)
.niferln
n into Uie
aromntio jtrinoiplo of TaniUa, 308.
Tronsfonnation of elliptic functions, on
the, f>G,
Trust fands, 13-18.
Tuiiupr (J. L.) on the ranire of motion in
the huiDan e;o. 429.
Tpulall (J.),(!Xpprimenta1dFm(nislnilliKii
of the stoppage of soimd by partial
Water, on the adtabatiw and isothnnud*
of, 451.
subatanoe, a quantitaiiTe inTestiga-
tion of oertun relations between Ifae
gaseous, the liquid, and the solid stain
of, 27.
Watnej (H.) on the minute anatomy of
the alimentary canal, 293.
WaTe of oscillation, on the uniform. 350.
White Uues in the sol&r Bpedrum, m,
221.
'Willemdes-Sulmi (S. Ton) on the mile
and the structure of Tltaiiniops pd-
lueida, 42.
Williams (J.) on the structure of the
mucous membrane of the ulerus and its
W periodical changes, 297.
dliamson (W. C.) on tha organiutioD
of the fossil plants of the coal-measures:
Part VI. Ferns. 248.
Wilson (C, W.), admitted, 362.
Winds of Northern India, on the, 210.
Zambra (J. W.) and Negretti (H.) on a
new deep-ssa thermometer, 238.
S-Ea-Wei, magnetie obaemtions at, 440.
rsn or tub TWSNTr-BBcoNB tomjme.
PBlNTEn BT TATLOB AHD FBAKCI9,
BID LlOa CODBT, FLBCT STBnr.
OBITUARY NOTICES OF FELLOWS DECEASED.
Abchibald SbAth, only bod of James Smith, of Jordanhill, Benfrew-
ahire, woa bom on tho 10th of August, 1813, at Qreenhead, Glasgow, in
the house where his mother's &ther lived. Hie father, who also was a
Fellow of the Hoyal Society, had literary and sdentific testes with a
strongly practical turn, fostered no doubt by bis education in the Uni-
Tersity o£ Glasgow and bis family connexion with some of the chief
founders of the great commerdal community which has grown up by its
side. In published works on various subjects he left enduring monu-
ments of a long life of actively employed leisure. His discovery of
different species of Arctic shells, in the course of several years' dredging
from bis yacht, and his inference of a previously existing colder climate
in the part of the world now occupied by the British Islands, con-
stituted a remarkable and important advancement of Geological Science.
In his 'Voyage and Shipwreck of St. Paul,' a masterly application of
the principles of practical seamanship readers St. Luke's narrative more
thoroughly intelligible to us now than it can have been to contem-
porary readers not aided by nautical knowledge. Later he published a
'Dissertation on the Origin and Connexion of the Gospels;' and ha
was engaged in the collection of furirher materials for the elucidatioii of
the same subject up to the time of his death, at the age of eighty-five.
Archibald Smith's mother was also of a family distinguished for intel-
lectual activity. Her paternal grandfather was Dr. Andrew Wilson,
Professor of Astronomy in the University of Glasgow, whose specula-
tions on the constitution of the sun are now generally accepted, especially
since the discovery of spectrum-analysis and its application to solar
physics. Her uncle, Dr. Patrick WUson, who succeeded to his father's
Gh^ in the University, was author of papers in the 'Philosophical
Transactions ' on Meteorology and on Aberration.
Archibald Smith's earliest years were chiefly passed in the old castle of
Boseneath. In 1818 and 1819 he was taken by his father and mother to
travel on the continent of Europe. Much of his early education was
given him by hie father, who read Virgil with him when be was about
nine years old. He also had lessons from the Boseneath parish school-
roaster, Mr. Dodds, who was very proud of his young pupil. In Edin-
VOL, xsii. h
u
burgh daring the winters 1820-22 he went to a day-sdiobl ; and aft
that, living at home at JordanhiU, he attended the Giammar School
Glasgow for tiiree years. As a boy he was extremely actiTe,and fond
eyerything that demanded skill, strength, and daring. At Boeeneath 1
was constantly in boats ; and his &yourite reading was any thing aboi
the sea, commencing no doubt with details of adyentorers and booo
neers, but going on tonarratiyes of voyages of discovery, and to the be
text-books of seamanship and navigation as he grew older. He had i
coarse the ordinary ardent desire to become a sailor, incidental to bo]
of this island; but with him the passion remained through life, an
largely influenced the scientific work by which he has conferred never4(
be-f orgotten benefits on the marine service of the world, and made ooc
tributions to nautical science which have earned credit tar Englau
among maritime nations. He was early initiated into practical seamaz
ship under his fether^s instruction, in yacht-sailing. He became -a
expert and bold pilot, exploring and marking passages and anchOTagc
for himself among the intricate channels and rocks of the West Hig^
lands, when charts did not supply the requisite information. His moi
loved recreation from the labours of Lincoln's Inn was alvrays a craii
in the West Highlands. In the last summer of his life, after a natural!
strong constitution bad broken down under the stress of mathematics
work on ships' magnetism by night, following days of hard work in hi
legal profession, he regained something of health and strength in sailin
about with his boys in his yacht, between the beautiful coasts of the Frit
of Clyde, but not enough, alas, to carry him through unfavourable influ
ences in the winter that followed.
In 1826 he went to a school at Bedland, near Bristol, for two years
and in 1828 he entered the University of Glasgow, where he not onl
began to show his remarkable capacity for mathematical science in th
classes of Mathematics and Natural Philosophy, but also distinguishe
himself highly in Gassies and Logic. Among his fellow students wer
Norman Macleod and Archibald Campbell Tait, with both of whoi
ho retained a friendship throughout life. After completing his fourt!
session in Glasgow, he joined in the summer of 1832 a reading part}
under Hopkins, at Barmouth in North Wales, and in the October fol
lowing commenced residence in Trinity College, Cambridge.
While still an undergraduate he wTote and communicated to th
Cambridge Philosophical Society a paper on Fresnel's wave-surfaa
The mathematical tact and power for which he afterwards became cele
brated were shown to a remarkable degree in this his first pubUshe
work. Fresnel, the discoverer of the theory, had determined analyticall
the principal sections of the wave-surface, and then guessed its algebrai
equation. This he had verified, by calculating from it the perpendicula
from the centre to the tangent plane ; but the demonstration thus ob
tained was so long that he suppreased it in his publkhed paper. Ampere
bf sheer labour had worked out a direct analytical demonstration, and
published it in the 'Annates de Cbimie et de Phyeiqne'*, where it occupies
thirtj-twe pages, and presents so repulsive an aspect that few mathemati-
cianB would be pleased to face the task of going through it. With these
antecedents, Archibald Smith's inreatigation, bringing out the desired re-
sult directly from FreBuel's pOBtulat«8 by a few short lines of beautifully
symmetrical algebraic geometry, constitutes no small contribution k> the
elementary mathematics of the undulatory theory of light. It was one
of the first applications in England, and it remains to this day a model
example, of the symmetrical method of treating analytical geometry,
which soon after (chiefly through the influence of the 'Cambridge Mathe-
matical Journal') grew up in Cambridge, and prevailed over the un-
symmetrical and frequently cumbrous methods previously in use.
In 1836 he took his degree as Senior Wrangler and first Smith's FriEe-
man, and in the same year he was elected to a Fellowship in ^inity
College.
Shortly after taking his degree, he proposed to his friend Duncan
Farquharson Gregory, of the celebrated Edinburgh mathematical £imily,
then an undergraduate of Trinity College, the establishment of an
English periodical for the publication of short papers on mathematical
subjects. Gregory answered in a letter of date December 4th, 1836,
cordially ent«riug into the scheme, and undertaking the office of editor.
Being, however, on the eve of the Senate-House examination for his
degree, he adds, " But all this must be done after the degree; for ' business
before pleasure,' aa Bichard said when he went to kill the king before
he murdered the babes." The result was, the 'Cambridge Mathematical
Journal,' of which the first number appeared in November 1837. It
was earned on in numbers, appearing three times a year under the
editorship of Gregory, until his death, and has been contiaijed under
various editors, and with several changes of name, till the present time,
when it is represent«d by the ' Quart«riy Journal of Mathematics ' and
the ' Messenger of Mathematics.' The original ' Cambridge Mathe-
matical Journal' of Smith and Gr^ory, containing as it did many
admirable papers by Smith and Gregory themselves, and by other able
contributors early attracted to it, among whom were Greatheed, Donkin,
Walton, Sylvester, EUia, Cayley, Boole, inaugurated a most fruitful
revival of mathematics in England, of which Herschel, Peacock, Babbage,
and Green hod been the prophets and precursors.
It is much to be r^retted that neither Cambridge, nor the university
of hia native city, coidd offer a position to Smith, enabling him to make
the mathematical and physical science, for which he felt so strong an
inclination, and for which he had so great eapadty, the professional
■ Tolume for 1828.
b2
IV
work of his life. Two years after taking his degree he commenced reading
law in London ; but his inclination was still for science. Belinquishing
reluctantly a Trinity Lectureship offered to him by Whewell in 1838, and
offered again and almost accepted in 1840, resisting a strong temptation
to accompany Sir James Boss to the Antarctic regions on the scientific
exploring expedition of the * Erebus * and * Terror ' in 1840-41, and re-
gretfully giving up the idea of a Scottish professorship, which, during his
early years of residence in Lincoln's Inn, had many attractions for him,
he finally made the bar his profession. But during all the long years of
hard work through which he gradually attained to an important and
extensive practice, and to a high reputation as a Chancery barrister, he
never lost his interest id science, nor ceased to be actively engaged in
scientific pursuits ; and he always showed a lively and generous sym-
pathy with others, to whom circumstances (considered in this respect
enviable by him) had allotted a scientific profession.
About the year 1841 his attention was drawn to the problem of
ships' magnetism by his friend Major Sabine, who was at that time
occupied with the reduction of his own early magnetic observations
mode at sea on board the ships 'Isabella' and 'Alexander' on the
Arctic Expedition of 1818, and of corresponding magnetic observa-
tions which had been then recently made on board the * Erebus*
and 'Terror' in Capt. Boss's Antarctic Expedition of 1840-41. The
systematic character of the deviations, unprecedented in amount, ex-
perienced by the ' Isabella ' and * Alexander ' in the course of their
Arctic voyage, had attracted the attention of Poisson, who published in
1824, in the ' Memoirs of the French Institute,' three papers containing a
mathematical theory of magnetic induction, with application to ships'
magnetism. The subsequent magnetic survey of the Antarctic regions,
of which by far the greater part had to be executed by daily observations
of terrestrid magnetism on ship-board, brought into permanent view the
importance of Poisson's general theory ; but at the same time demon-
strated the necessity for replacing his practical formulaB by others, not
limited by certain restrictions as to symmetry of the ship, which he had
assumed for the sake of simplicity. This was the chief problem first put
before Smith by Sabine ; and his solution of it was the first great service
which he rendered to the practical correction of the disturbance of the
compass caused by the magnetism of ships. Twenty years later the
work thus commenced was referred to in the following terms by Sir
Edward Sabine*, in presenting, as President of the Boyal Society, the
Boyal Medal which had been awarded to Archibald Smith for his in-
vestigations and discoveries in ships' magnetism: — ♦ ♦ ♦ "Himself
" a mathematician of the first order, and possessing a remarkable facility
" (which is far from common) of so adapting truths of an abstract cha^
* Proceedings of the Boyal Society, Not. 30, 18G5, vol. xiv. p. 499,
" racter as to render them available to leas highly trained iatellecta, hu
" derived at my request, from Polsson's fundamental equatione, simple
" and practical formube, including the effects both of induced magnetism
" and of the more persistent magnetism produced in iron which haa
" been hardened in any of the processes through which it has passed.
" The formube supplied the means of a sufGciently exact calculation
" when the results were finally brought t<^tber and coordinated. They
" were subsequently printed in the form of memoranda in the account
" of the survey in the ' Philosophical Traosacttons ' for 1843, 1844, and
" 1846.
" The assistance which, from motives of pHvato friendship and sden-
" tific interest, Mr. Smith had rendered to myself, was from like motives
" continued to the two able officers who had successively occupied the
" post of Superintendent of the Compass Department of the Navy; and
" the formulie for correcting the deviation, which he had furnished to
" me, reduced to simple tabular forms, were published by the Admiralty
" in successive editions for the use of the Boyal Navy.
" As, in the course of time, the use of steam machinery, the weight of
" the armament of ships of war, and generally the use of iron in vessels,
" increased more and more ; the great and increasing inconvenience
" arising from compass irrogntaritiea were more and more strongly felt,
" and pressed themselves on the attention of the Admiralty and of
" naval officers.
" An entire revision of the Admiralty instructions became necessary ;
" Mr. Smith's assistance was again freely given ; and the result was the
" publication of the ' Admiralty Manual ' for ascertaining and applying
" the deviations of the compass caused by the iron in a ship.
" The mathematical part of this work, which is due to Mr. Smith,
" seems to exhaust the subject, and to reduce the processes by simple
" formula and tabular and graphic methods, to the greatest simplicity of
" which they are susceptible, Mr. Smith also joined with his fellow-
" labourer, Capttun Evans, F.B.S., the present Superintendent of the
" Compass Department of the Navy, in laying before the Society several
"valuable papers containing the results of the mathematical theory
" applied to observations made on board the iron-built and iron-plated
" ships of the Eoyal Navy."
This is not an occasion for explaining in detaU the elaborate investiga-
tions sketobed in the preceding statement by Sir Edward Satnne ; but
the writor of the present notice, having enjoyed the friendship of Arehi-
bald Smith since the year 1841, and having had many opportunities,
both in personal int«rcourse and by letters, of following the progress
through thirty years of his work on ships' magnetism, may be permitted
a brief reference to some of the points which have struck hirn as most
remark^Ie : —
VI
1. Hannonic reduction of observations.
2. Practical expression of the full mathematical theory.
8. Heeling error.
4. Dygograms.
5. Eule for positions of needles on compass card, with dynamical and
magnetic reasons.
1. Harmonic reduction of observations, — The disturbance of the compass
produced by the magnetism of a ship is found by observation to be the
same, to a very close degree of approximation, when the ship's head is
again and again brought to the same bearing, no great interval of time
having intervened, and no extraordinary disturbance by heavy sea or
otherwise having been experienced in the interval. Overlooking these
restrictions for the present, we may therefore say, in Fourier's language,
that the disturbance of the compass is a periodic function of the angle
between the vertical plane of any line fixed relatively to the ship, and
any fixed vertical plane, when the ship, on " even keel " or with any con-
stant inclination, is turned into different aadmuths — ^the period of this
function being four right angles. Hence also the disturbance of the
compass is a periodic function of the angle between the vertical plane of
the chosen line moving with the ship, and the vertical plane through
the magnetic axis of the compass. The line moving with the ship being
taken as a longitudinal line drawn horizontally from the stem towards
the bow, and the fixed vertical plane being taken as the magnetic meri-
dian, the angle first mentioned is called for brevity " the ship's magnetic
course" and the other " the ship's comjpass course.^*
One of Smith's earliest contributions to the compass problem was the
application of Fourier's grand and fertile theory of the expansion of a
periodic function in series of sines and cosines of the argument and its
multiples, now commonly called the harmonic analysis of a periodic
function. To facilitate the practical working out of this analysis, he gave
tables of the products of the multiplication of the sines of the " rhumbs "
by numbers, and by arcs in degrees and minutes ; also tabular forms and
simple practical rules for performing the requisite arithmetical opera-
tions. These tables, tabular forms, and rules, just as Smith gave them
about thirty years ago, are in use in the Compass Department of the
Admiralty up to the present time. From every ship in Her Majesty's
Navy, in whatever part of the world, a table of observed deviations of the
compass, at least once a year is sent to the Admiralty, and is there sub-
jected to the harmonic analysis. The observations having been accu-
rately and faithfully made, a full history of the magnetic condition of the
ship is thus obtained, and want of accuracy, or want of faithfulness, if
there has been any, is surely detected. The rigorous carr}nng out of this
system, with all the method and business-like regularity characteristic
of the scientific departments of our Admiralty, has undoubtedly done
more than any thing else to promote the usefulness of the mmpaes, and
to render its use safe throughout the British Navy. Smith's tables aud
forms for harmonic analysis have proved exceedingly valuable in many
other departments of practical physics besides ships' magnetiem. The
writer of tMs article found them most useful fifteen years ago in re-
ducing for the Boyat Society of Edinburgh Forbes's observations of the
undei^roond temperature of Calton Hill, the Experimental Gardens,
and Craigleith Quarry, in the neighbourhood of Edinburgh ; and the
forms, with a suitable modification of the tables, have proved equally
useful in the harmonic analysis of tidal otwervatioos for various parts of
the world, carried out by the Tidal Committee of the British Association,
with the assistance of sums of money granted in successive years from
1888 to 1872.
2. Pnutieal ftrprewton of the full mailumatieai (heory. — Foisson him-
self, in making pcw^ical application of his theory, had simplified it by
assuming particular conditions as to symmetry of the iron in the ship,
and even with these restrictions had left it in a form which seemed to
require further simplification before it could be rendered available for
general use. Airy, in taking up the problem with tikis object, at the
request of the Admiralty in the year 1839, founded his calcuLationB on a
supposition that, " by the action of terrestrial magnetism every particle
" of iron is converted into a magnet whose direction is parallel to that of
" the dipping needle, and whose intensity is proportional to the intensity
" of terrestrial magnetism," This supposition, which is approximately
true only for the ideal case of the iron of the ship being all in the shape
of globes placed at such considerable distances from one another as
not to exercise mutual influence to any sensible degree, leads to a law
of dependence between the ship's force on the compass needle, and the
angular coordinates of the ship, which differs from that of the complete
theory, as shown afterwards by Smith, only in the want of his constant
term A of the harmonic development,— a difference which, in ordinary
cases, does not vitiate sensibly the practical application. In introdudug
the supposition. Airy correctly antidpated that it would in general lead
to results sufficiently accurate and complete for practical purposes. But
he said "it would have been desirable to make the calculations on
" Poisson's theory, which undoubtedly possesses greater chums on our
" attention (as a theory representing accurately the facts of some very
" peculiar cases) than any other. The difliculties, however, in the appli-
" cation of this theory to complicated cases are great, perhaps insuper-
" able." These difficulties were wholly overcome by the happy mathe-
matical tact of Archibald Smith, who reduced the full expression of
Poisson's theory, including the effect of permanent magnetism, the great
practical importance of which had been discovered by Airy, to a few
simple and easily applied formuln. [See Appendix to this notice.] These
vm
formula are now in regular use in the Compass Department of the
Admiralty, for the practical deduction of rigorous result-s from the har-
monic analysis already referred to. In fact the full expression of the
unrestricted theory, as given by Archibald Smith in Part III. of the
* Admiralty Manual,' is even simpler and more ready for ordinary use
than the partial and restricted expressions which Poisson and Airy had
given for practical application of the theory.
3. Heeling error. — Poisson's general formulsB express three rectangular
components of the resultant force at the point where the compass is
placed, due to the magnetism induced in the ship by the terrestrial
magnetic force. To these Airy added the components of force due to
permanent magnetism of the ship's iron, which, though not ignored by
Poisson, had been omitted by him, because, considering the probability
of scattered directions of the magnetic axes of permanent magnetism in
the isolated masses of iron existing in wooden ships and their arma-
ments, he justly judged that permanent magnetism could not seriously
disturb a properly placed compass in a wooden ship ; and iron ships were
scarcely contemplated in those days. This general theory of Poisson and
Airy expresses the resultant force in terms of three angular coordinates,
specifjring the position of the ship. In the practical application these
coordinates are most conveniently taken as :— (1) the ship's " magnetic
course," defined above ; (2) the inclination of the longitudinal axis of
the ship to the horizon ; (3) the inclination to the horizon of a plane
drawn through this line perpendicular to the deck. The second co-
ordinate has no name and is of no importance in the compass problem ;
for under steam, or even under sail, the average inclination of the longi-
tudinal axis (chosen as horizontal for the ship in still water) is never so
great as to produce any sensible effect on the compass disturbance, and
the magnetic effects of pitching in the heaviest sea are not probably ever
so great as to produce any seriously inconvenient degrees of oscillation in
the compass card. The third coordinate is called the "heel ;" and its mag-
netic effect on the compass is called " the heeling error." The heeling
error was investigated by Airy in his earliest work on the compass disturb-
ance ; but at that time, when iron sailing ships were comparatively rare,
he confined his ordinary practical correction of compass error to the case
of a ship in different azimuths on even keel. Since that time the heeling
error has come to be of very serious practical importance, on account of
the great number of iron sailing ships, and of screw steamers admitting
of being pressed by sail to very considerable degrees of " heel." Archibald
Smith took up the question with characteristic mathematical tact and
practical ability, and gave the method for correcting the heeling error —
which is now, I believe, universally adopted in the Navy, and too fre-
quently omitted (without the substitution of any other method) in the
mercantile marine.
4. Dytjogratns. — This is the name given by Smith to diagrams eihibitiug
the m^nitude and direction of the resultaut o£ tho t«rreBtriaI magnetic
force and tho force of the ship's magnetism at the point occupied by the
compass. The solution of the problem of Snding for a ship in all
amnuths on even keel the dygogram of the whole resultant force ie
gifen by him in the chapter headed " Ellipse and Circle," of the * Ad'
miialty Manual,', Appendix 2 (3rd edition, 18((9, page 1I>9-171). But it is
only for horizontal components of force that he has put dygograma into
a practical form ; and for this caae, which includes the whole compass
problem of ordinary navigation, bis dygograms are admirable both for
tlieir beauty and for their ntility. " Dygt^ram Number I." is the
curve locus of the extremity of a line drawn from a fixed point, 0, in
the diiectioD, and to a length numerically equal to the magnitude, of the
horinMital component of the resultant toree experienced by the needle
when the ship is turned ttirough all asfmnths. This curve (however
great the deviations of the compass) he proves to be the Lima^on of
Pascal — that is to say, the curve (belonging to the family of epitrochoids)
described by the end of an arm rotating in a plane round a point, which
itself is carried with half angular velocity round the circumference of a
fixed orde in the same plane. The length of the firet-mentioned arm is
equal to the maximum amount of what is called (after Airy) the
quadrantal deviation ; the radius of the circle last mentioned is the
maximum amount of what Aiiy called the polar magnet deviation, and
Smith the semudrcular deviation. (When,aathe writer of this article trusts
befcRO long will be universally the case*, the quadrantal deviation is
perfectly corrected by Airy's method of soft iron correctors, the dygogram
Number I. wiU be reduced to a circle.) Besides the form of the curve
in any particular case, which depends on the ratio of the first-menticmed
radius to the second, to complete the diagram and use it we must know
■ the position of the fixed point through which tho resultant radius-vector
is to be drawn, and must show in the diagram the m^netic bearing of
the ship's head, for which any particular point of the curve gives the
resultant force. Smith gave all these elements by simple and easily
execated ccoistructionB, in the first and second editions of the ' Admiralty
Manual.' In the third editi<m he substituted, for his first method of
constructiDn of the dygogram curve, a modification of it due to Lieut.
Colongue of the Eusaian Imperial Navy and of the Imperial Compass
Observatory, Oronstadt, and added several elegant constructions, also
due to Lieut. Colongue, for the geometrical solution of various compass
problems, by aid of the dygi^nun Number I.
* The barrier against thia being done hitherto has been the pemicioualj' great length
of the compaes Dsedlee Died at aea.tho ihortest being about ail inches. Y
eompan the needles ought Dot to be more than half an inch long.
The Annexed digram is the dygogrsm Number I. for the "j^fV^
drawn accurately (by lud of a drcuhtr board rolling upon a ^^^ Ad-
board of equal diameter, in the manner described by Smith in ^_
miralty Manual,' Appendix H., under the heading " ***''**"*Tj„ced
atroction of Dygogram No. t"), accoi^ng to the foUowii^ data aeo _^
from observationa inadR at Spithpad in October 1 Sfil . Tte untatwo •
RuUfoi- aaiiuj Dygogram Ao.I.— In the diagram Q is „ c
the " Ltraa^c/' called " the pole of the dTgogram " it P"^"* °^
axis of symmetry, which is indicated by a dotted lin at "^ ^^^
are two hnes throuph Q at right angles to one anoJk '*^' ^Q™"
are two points, in positions fixed by the ship's mapn *^' ^^ ^' ^
The length OP represents " mean force on comoaas^U*' ^'ementa.
Take any point R on the curve, such that NOR is " , f*,"'^'' "(XH).
" magnetic course ;" then is KOP the " deviation '■ of th *''*' ^""P*
and OR represents the horizontal coniponeiit of the tor *^™P*«8,
C, fit Ci is that which wab introduced by Smith when he first subBti-
tuted the rigoroua formula) for the Approidmate harmonic formuls
which had preriously BufGced : it ia explained in the Appendix to this
notice.
Dygogram Number 11. may be deduced from djgogram Number I. by
attaching a piece of paper to the half-speed revolving ann, and letting
the tracing-point of tfie lima^on leave its trace also on this paper, which
will be a rircle, while at the same time the fixed point from which the
resultant radins-vector is drawn will trace another circle on the moving
paper. The fresh diagram thus obtained consists of two circles. Mark
one of tliese circles (the second in the order of the preceding descrip-
tion) with the pcintB of the compass*, like a compass card ; or (bett«r)
mark simply degrees all round from North taken as eero ; and mark
with degrees coonted in rererse direction tjie other circle, which, for
breri^, will be called the auziliai; circle. Mark the ship's c<»npaBs
course on the circumference of the ideal cranpass card. From this
point to the corresponding point on the auxiliary drdo draw a straight
line. The direction of this line shows by the parallel to it, through the
centre of the ideal compass aad, the compass course correspon^g to
any chosen magnetic course. The length of the line, diswn in the
manner described, represents the horisontal resnltsnt force of the earth
and ship, at the pmnt occupied by the ccanpass needle, in torms of the
radius of the ideal compass card, as unity. The writer of the present
article beHevee that this construction will yet prove of very great practical
ntility, although hitherto it has not come into geneml uset- Its geo-
metrical beauty attracted the notice even of Cayley, who has ccmtributed
to the Admiralty Compass Manual a Bec<Hul method of solving, by
means of it, one of Smith's compass problems.
Construction from ship's and earth's m^;netic elements. With O m
centre and OH equal to "mean force on compass to north "(MI) describe
a circle. Blake
NL=S, OB=-B; BC=-€:; CD=-»; DAs-C;
with C as centre describe a circle through A.
The following diagram shows (for an ideal cose, as possibly a turret
ship of the future, with very large values of the usually small magnetic
elements 2 and G) the Dygogram of two circles, modified to suit the
Chinese compass (or needle imloaded with compass cord, which is un-
doubtedly the compass of the future). This modification ia also conve-
■ The ancient Sfltcm of marking 32 poinU on ^he compua caid, and sp«cir;ing
coumn in terma of them, has alwafa been Ter; inoonToaiont, and U now beginning U>
bo genrriillv perceived to be >o.
t A sliort demonatrMion of it, deduced dircuttj from Siiiitli'a fundiimetilnl forniulv,
IH appended (o the present iirticlc for the aake of mathenialiukl readcrn wbo ma; not
have the Admirallj Compnaa Uanual at hand.
nient for the theoretical explaDation and proof appended to the present
notice.
Dygogram No. XL.
Use. — Make hm equal in angular value to NH ; then OK, parallel and
equal to mL, ehowa direction of needle and magnitude of horiKontftl
component force on it when correct magnetic north ia in direction
ON, and ship's head OH r NOH being ship's " magnetic courBC,"
KOH is the corresponding " compass course. '
5. Ride for position* of needles an oampasa card, with dyitamiral and
magnetic reatom. — In 1837 a Committee, consisting of Captain Beaufort,
Hydrographer to the Admiralty, Captain Sir J. C. Ross, K.N., Captain
Johnson, B.N., Major Sabine, E.A., and Mr. S. H. Christie, uiis appointed
to remedy defects of the compasses at that time in use in Her Majesty's
fleet, and to organi7:e-a system of compass management ashore and afloat.
The labours of that Committee have conferred signal benefit, not only on
the British Navy, but on>the navies and mercantile marine services of all
nations — in the ' Admiralty Standard Compass,' and in the establishment
in 1843 of the British Admiralty Compass Department. The qualities of
the magnetic needles and their arrangement on the card occupied much
attention of the Committee. Smith's attention was called to the subject
by Us friend Sabine ; and he gave a rule for placing the needles, which
wu adopted by the Committee, and has ever since been followed in the
construction of the Admiralty compass. The rule is, that when there are
two needles used they should be placed with their ends on the compass
card at 60° on each side of the ends of a diameter ; and that when (as
in the Admiralty Standard Compass) there are four needles, they should
be placed with their ends at 15° and 45° from the ends of the diameter.
The object of this rule was to give equal momenta of inertia round all
horizontt^ axes, and so to remedy the " wabbling" motion of the compass
card when balanced on iia pivot, which has been found inconvenient.
Captain Evans, in a letter recently received from him by the writer of
this notice, says that th? " wabbling " motion has been satas&ctorily
corrected by this arrangement of needles ; " it is transformed into a
' (u'unmit)^' motion."
About twenty years later it was discovered that the same arrangement
gives, by a happy coincidence, a very important magnetic merit to the
Admindty compass, which had not been contemplated by Smith when he
first gave his rule. To explain this, it must be premised that practical
compos B-^justera had experienced difficulties in correcting the compass
deviation of certain ships by Airy's method (which consists in using soft
iron to correct the qnadrantal deviation, and permanent magnets to
correct the semicircular), and had reported that in such cases they had
found it advantageous to substitute compasses with two needles for a
single-needle compass. The attention of Captain Bvans was drawn to
this subject by the observations made in the ' 0reat Eastern ' on her
experimental voyage from the Thames to Portland, and afterwards when
she was Ijdng at Holyhead and Southampton, &om which he found that
although the deviations had been carefully corrected by Mr, Gray, of
liiverpool, with magnets and soft iron, and were in fact nearly correct
on the cardinal aad quadrantal points, there were errors of between
5° and 6° on some of the intermediate points. These observations indi-
cated the existence of a considerable error, which was neither semicircular
nor quadrantal, and thus apparently some source of error which had not
been taken into account by Airy in his phin for correction. To explain
the cause of these and similar rosults in other ships, previously considered
to be anomalous. Captain Evans instituted a series of experiments with
compasses, and magnets and soft iron placed in different positions with
respect to them. He soon found that the greatness of the supposed
anomaly in the ' Great Eastern ' depended on the unusually great length
of the needles of her standard compass (two needles* of 11 j inches in
* Compau Deedles becoming larger with the shipe, bja procen of " Arliflciol Selec-
tion " unguided b; intelligence, hav^ Bometimea AttAined to the monstroua length of
10 inchee, or eien more, in aome of the gnat modern paswngiir-Bteamcn BtteA out by
onners regardless of eipenw, md onlf desiring efficiency, trusting to inatrument-maJben
xiv ■
length, placed near each other on the card). The results of the obeton-
tions and experiments, reduced by add of Napier's graphic method, and
subjected to a thorough harmonic annljsis, are describt.>d in a joiat paper
by Smith and Evans, published in the Transactions of the Royal Society
for 1861. They show, in the expression for the deviation, sextantal aud
octantal terms* very large in the case of the ' Great Eastern,' and com-
pantiTely small when the Admiraltj standard compass was tested in cir-
cumstances otherwise similar. Whether single needles or double needlea
were osed, it was found that the smaller the needle the smaller were tie
sextantal and octMital terras. Single needles gave greater terms of this
class than double needles of the same magnitude, arranged as in the
Admiralty compass.
The merit of giving abnoet evanesoeat sextaotal and octactal tenus.
of the hjgbeit name. Heremton to the old Cbincae species, with nnsle neodle Icsi than
an incli long and unloaded hj a compui cord, would be sa impniTemont on the pre-
Hnl otdinuy ixage of fint-clas ocean alennion.
The directjon at part of the reactioaar; iinproTement required is clearly poml<d out in
the following note on the compaj^tive meriu of Infge and aaaii cumpiimnr. eitracMd from
C^jMam Evaiis'i ■ Elementary Manual fer the Deriation of the Compow in Inm Sbipe:' —
" Of lata jcan much dliemily in pmolioe Ilu preiailed as to the «iio of oompaasca for
" uae on board ship. The AdmimJtj Standard eord of 7} iniihes diameter, foreiaiuplh
"u fitted witli npodles tlio mniimum Irn^gtha of Kbich nri- 7^ i!i,-L.--s. nliilo In large
" pMMogcr eteam-Taancli (he needlea are fraqnantlj 12 to 16 inehea, and eren longer.
" Ibt chief ot^ect id the emplojment of luge oomjMsea ii to enable the helmamtn
" to iteer to degnwe ; and a more aocuiato ooune ia thua preaomed to be piueui led."
" With veferenoe to thi« inewaacd aiie, it muat be obaerted that competent authoritiee
" limit the length of effloietit oompaat needles to 6 or 6 inehea ; bejond thia limit an
" inereaae of length ia alone accompanied bf an increase of directiTe power in tbe
" aame proportion ; and if the thirhiena of tba needle be preaerred, the wei^t, and
" oooaeqnently the friction, incn«ae in the nme ratio. No advantage of direa^ie
" power is therefore gained b; increase in length ; but with the increaaed weight pf tba
" card and appendagea the inereaae of friction probably far eioeeda the inereaie of direc-
" tive force : Bluggiahneaa ia the result, which is further eiaggenited by the nxbone aloir-
" Iteaa of oscillation of long needles compared with abort needles."
" lArge carda, however convenient in praotioe, are therefore not without danger ; tor
" Uie course stAered may deoeive the Mamen bj seeming right to the fraction of a
" degree, but which avoila little if the card ia wrong half a point, and the ship in oon-
" aequenoe hazarded. In the opinion' of the writer the present Admiralty staidard
" card it M large aa should be used for the purposes of naviffafiini, and tha^ as regards
" safety in the long, ateadj, and (oat ship, the choice il really between the Admiral^
" card and a smaller one^ In short tbe case may be thua alaled : the smaller a card
" tbe more correctly it poiule ; tbe larger a card the more accurately it can be read."
When the needlea of a standard compaaa are reduced to aomething like half an inch
in length, and not till tiien, will the tbeDretioal perfection and beauty, and Iha great
practical merit, of Airy*! correction of theoompBaa I^aoft iron and permanent mogneti
(which theoretically assumes the length of the needle to ba infinitely small in propor-
tion to il* distance from the nearest iron or steel) be uniTersoUy recognised and havs
full justioe done to it in practice.
* Hut is to say, terms consisting of coefficienta multiplying the sines or cosines of
MX Unci and of eight tJmes the ship's magnetic oiimuth.
diflcoTeied in the Admiralty Btandard compase, " suggested the idea, that
" the amngement of the needles in that compass might produce, in the
" case of deviations caused by a magnet or mass of soft iron in close
" proximity to it, a compensation of the sextantal and octantal deviations ;
" and this, on the subject being mathematically investigated [on the
" approximate hypothesis that the intensity of magnetization is uniform
" through the length of each needle, and equal in the different needles],
" proved to be the case, this particular arrangement of needles reducing
" to tan the coetBcIente of the terms invoUing the square of the ratio
" of the length of the needle t« the distance of the disturbing iron ; so
" that this remarkable residt was obtained, that the arrangement of
" needles which produces the equality in the moments of inertia is, by a
" happy coincidence, the same as that which prevents the sextantal devia-
" tion in the case of correcting magnets, and the octantal deviation in
" the case of soft iron correctors. The consequence is, that with tie
" Admiralty compass cards, or with cards with two needles eoch 30°
" from the central line, correcting magnets and soft iron correctors
" may be placed much nearer the compass than can safely be done with a
" single-needle compass card, and that the large deviations found in iron
" ships may be thus for more accurately corrected."
It will be understood that the preceding statement, even as an index
of subjects, gives but a very incomplete idea of Smith's thirty years' work
on magnetism. Further information is .to be found in his papen in the
Transactions and Proceedings of the Boyal Society, some of them contri-
buted in conjunction with Sabine <xc with Evans, others in his own name
alone. In 1850 he published separatoly* an account of his theoretical and
practical investigations on the correction of the deviations of a ship's
compass, which was afterwords given as a supplement to the Admiralty
" Practical Rules " in 1856. The large deviations found in iron-plated
ships of war " having rendered necessary the use of the exact instead of
" the approximate formulie," this article was rewritten by Smith for the
Compass Department of the Admiralty. It now forms Part HI. of the
' Admiralty Manual for the deviations of the Compass,' edited by Evans
and Smith, to which are added appendices containing a complete mathe-
matical statement of the general theory, proofs of the practical formulie,
and constructions and practical methods of a more mathematical cha-
racter than those given in the body of the work for ordinary use. A
separate publication, of " Instructions for correcting the Deviation of the
Compass," by Smith, was made by the Board of Trade in 1857.
It is satisfactory to find that the British Admiralty ' Compass
Manual,' embodying as it does the result of so vast an amount of labour,
guided by the highest mathematical ability and the most consummate
■ TnatructionB forCompntation ofTabtMof DevialioiiB, b; ArchibBldSmitfa. Pub-
lished for Ihe Hjdrographic Offloe of the Admiralty.
XVI
(4
practical skill, has been appreciated as a gift to the commonwealth of
nations by other countries than our own. It is adopted by the United
States Navy Department, and it has been translated into Bussian, Ger-
man, Portuguese, and French. Smith's mathematical work, and particu-
larly his beautiful and ingenious geometrical constructions, have attracted
great interest, and have called forth fresh investigation in the same
direction, among the well-instructed and able mathematicans of the
American, Bussian, French, and German Navy Departments.
The laborious and persevering devotion to the compass problem,
which has been shown by British mathematicians and practical men, by
Sabine, Scoresby, Airy, Archibald Smith, by Captains Johnson and Evans
of the Compass Department of the Admiralty, and by Townson and
Bundell, who acted as secretaries to the Liverpool Compass Committee,
has been an honour to the British nation in the eyes of the world.
Beferring particularly to the Liverpool Compass Committee, Lieut.
Collet, of the French Navy, the French translator of the * Admiralty
Manual,' in a history of the subject which he prefixes to his translation,
says : — " Aid^ par des liberalit^s particulieres, soutenu surtout par
cette sorte de tdnacite passionnee, tout particuli^re h la nation anglaise,
qui, en inspirant les longues et patientes recherches conduit s&rement
'* au succes et sans laquelle tous les moyens d'action sent impuissants k
" surmonter les obstacles, ce Comite fit paraitre successivement trois rap-
" ports qui fix^rent d'une mani^re definitive la plupart des questions con-
trovers^s, et qui indiqu^rent nettement, pour celles qui restaient k
rc^soudre, la marche qu'il fallait sui^Te et les vdritables inconnues du
"probleme." And in an official publication by the American Navy
Department, containing an English translation of Poisson's memoir,
followed by the whole series of papers, theoretical and practical, on ships'
magnetism, which have appeared in this country, we find the following
passage, which must be gratifying to all who feel British scientific work
and appreciation of it by other nations, to be a proper subject for national
pride : — " * * With the complex conditions thus introduced, and the
" more exacting requirements of experience in their practical treatment,
" came the necessity for constantly aiming at that complete analysis of
" the magnetic phenomena of tJie ship which has been so prominent and
" characteristic a feature of the English researches."
The constancy to the compass problem in which Smith persevered with
a rare extreme of disinterestedness, from the time when Sabine first
asked him to work out practical methods from Poisson's mathematical
theory, until his health broke down two years before his death, was cha-
racteristic of the man. It was pervaded by that ** tcnacite passionnee "
which the generous French appreciation, quoted above, describes as a
peculiarity of the English nation ; but there was in it also a noble single-
mindedness and a purity of unselfishness to be found in few men of any
nation, but simply natural in Archibald Smith.
it
Honourable marka of appreciation reached him from various quarters,
and gave him the more pleasure froia being altogether unsought and un-
expected. The "Admiralty, in 1862, gave him a wateh. In 1864 he
received the honorary degree of LL.D. from the University of Glasgow.
The Soyal Society awarded to him the Boyal Medal in the year 1SG5.
The Emperor of £ussia gave him, in I8G(!, a gold Compass emblazoned
with the Imperii Arms and set with thirty-two diamonds, marking the-
thirty-two points. Sis months before his death Her Majesty's Govern-
ment requested his acceptance of a gift of £20{iO, as a mark of their ap-
preciation of " the long and valuable scnices which he hod gratuitously
" rendered to the Naval Service in connexion with the magnetism of iron
" ships, and the deviations of their Compasses." The official letter in-
timating this, dated Admiralty, July 1st, 1872, contains the fallowing
statement, communicated to Smith by command of the Lords of the
Admiralty : — " To the zeal and ability with which for many years you
have a[jjp]ied yourself to this difficult and most important subject, My
Lords attribute in a great degree the accurate information they possess
in regard to the influence of magnetism, which has so far conduced to
the safe navigation of iron ships, not only of the Soyal and Mercantile
Navies of this country, but of all nations."
The writer of this notice has obtained I^n veto quote also the following
from a letter from the First Lord of the Admiralty, Mr. Ooschcn, of date
February 23rd, 1872, announcing to Mr. Smith that the GovemmeTit
had determined to propose to Parliament that the sum of £2000 should
be awarded to him " as a mark of recognition of the great and successful
" labours" which he had " bestowed on several branches of scientific eo-
" quiry of deep importance to Her Majesty's Navy."
" I am aware that you have treated your arduous work in this direction
" as a labour of love ; and therefore I do not consider that the grant which
" Parliament will be requested to sanction is in any way to be looked
" upon as a remuneration of your services I trust you will
" regard it as a mark of recognition on the part of the country, of your
"great devotion to enquiries of eminent utility to the public, conducted '
" in the leisure hours which remained to you in a laborious profession."
The followingletter, which was addresaedto the Editor of the 'Glasgow
Herald,' and published in that paper last January, will be read with
interest by others as well as those for whom it was originally written : —
" As an intimate friend of the late Archibald Smith of Jordanhill, I
" desire to call your attention to a passage in your article of the
" 30th December upon him, which might perhaps convey a wrong im-
" presaion to the minds of your readers.
" You say that ' mathematics ... in its application to practical navi-
" ' gation was the amusement of his lighter hours.' The truth is, that
" the profession of a Chancery barrister, which the claims of a large
" famUy forbade him to abandon, occupied his beBt energies from C3cl<{
TOL. XIII. 0
xvm
" morning till late in the evening — ^in other words, what would in the
" case of most people, be called ' his whole time ; ' and compass investi-
" gation of the most minute and severe nature, undertaken after mid-
*' night, and carried on far into the morning hours bv a man whose brain
** had been working all day, and must work again the next day, can
" hardly be called * the amusement of lighter hours/ The same remark
" applies to vacations, during which his magnetic papers were constantly
" with him — on railway journeys, on board the yacht, the last subject of
" his thoughts at night, the first in the morning, at one time depriving
" him, to an alarming extent, of the power of sleep ; for, unlike the
" labours of law, these abstruse subjects cannot be dismissed at will.
'* The fact is that, in addition to the love of science for her own sake,
" he was penetrated by the conviction of the usefulness of his work.
" His splendid abilities, supported by a constitution of unusual vigour,
" were freely and heartily devoted to the service of his country, and the
good of his fellow-creatures. * Think how many lives it will save,' was
his answer to an anxious friend who begged him to relinquish labours
" so exhausting, and to give himself ordinary rest. But the inevitable
" result followed ; and though in earlier days it had seemed as if nothing
** could hurt his constitution, and his friends might anticipate for him
the length of days for which many of his family had been remarkable,
yet the continued mental strain did its work too surely, and in 1870
he was compelled to give up his profession with shattered health, to
spend two short years with those he loved, and then sink into a pi'ema-
" ture grave. You observe that * from the very commencement of his
" career Her Majesty's Government (to their credit be it said) appreciated
" the supreme importance of his researches.' In justice to the Govem-
** ment, it ought also to be mentioned, that they asked [twelve years ao-o]
" what acknowledgment should be made to him for work undertaken at
" their request, and when Smith named a watch, it was presented to him bv
** the Admiralty. The testimonial presented to him during the past year
" * not as representative of the money value of his researches, but as a
" * mark of their appreciation of their worth,' and still more, the graceful
" letter in which Mr. Goschen intimated to him that it was awarded
" gave him pleasure, and his friends must always be glad that it did not
** come too late.
" The truth is, Sir — and it is for this reason that I address you — that
" services such as his, rendered at such heavy cost to himself and his
" sorrowing friends, deserve the highest reward which can be given,
** namely, the gratitude of the nation."
One more extract in conclusion. The following from the * Solicitors'
Journal and Eeporter' of January 11th, 1873, contains a brief statement
regarding the estimation in which Smith was held in relation to his legal
profession, and concludes with words in which the writer of this article
wishes to join, and therefore gives without quotation marks : —
" When Mr, Jamea Parker was mode Vice-Chancellor he appointed
" Jlr. Smith his Secretary ; and he was also Secretary to the Decimal
" Coinage Commission, which made its final report in 1859, In that
" report there is a remme of the subject by Mr, Smith ; and one may see
" there not only the speciftl knowledge which he had collected on the
" matter in hand, but an example of his thorough and exhaustive style,
" close, compressed, and rich with fruits which it had cost him long
" labours aod careful thought to mature. Ungrudgingly and without
" parade he used to offer the products of his toil ; ' This,' be said to the
" writer, pointing to one half page of figures in his book, ' cost me six
" ' weeks of hard work.' It was thus he ever worked : no pains seemed
" to be too much ; and consequently a marvellous neatness and elegance
" adorned all that he did. In his profession, although he did not attain
" the same exceptional eminence as in science, there was much that
" deserves notice. His mental characteristics were of course more or
" less apparent here. As a draughtsman few could compare with him
" for conciseness and perspicuity. His opinions were much esteemed;
" and his arguments, though far from brilliant in manner, had in them
" BO much sound law and careful aud subtle Euialysis that they were
" always of interest and value, and commanded the respect and attention
" of the judges. The important change which substituted figures for
" words as to dates and sums occurring in bills in Chancery was made,
" it is believed, at his suggestion. The well-known case of Jamer v.
" Morrit (on appeal 3 D. F, & J. 45, 9 W. E, 391), is an instance of one
" of his successful arguments ; and the ease of Dtare v, Soittten (9 L. E.
" Eq. 151, 18 W, E, 203), in which the former case was reconsidered
" and confirmed, illustrates the research and industry which he was wont
■' to'use in all matters which came before him, A judgeship in Queens-
" land was ofiered to him about the year 1864 ; but he declined it."
In private life those who knew Archibald Smith best loved him most ;
for b^ind a reserve which is perhaps incident to engrossing thought,
especially when it is concerned with scientific subjects, he kept ever a
warm and true heart ; and the affectionate regrets of his friends testify
to the guileless simplicity and sweetness of his disposition, which nothing
could spoil or a£Eect, About the close of 1870 he was compelled by ill-
ness to give up work ; but two years later he had wonderfully rallied,
and, building too much on a piurtial recovery of strength, had recurred
imprudently to some of his old scientific pursuits. A few weeks before
his death he revised the instructions for compass observations to be made
on board the ' Challenger,' then about to sail on the great voyage of
scientific investigation now in progress. The attack of illness which
closed his life was unexpected and of but a few hours' duration. In
1853 he married a daughter of Vice-Chancellor Sir James Parker, then
deceased ; aud he leaves six sons and two daughters. He died on the
26th of December, 1872.
.Ifhrmillintl ^
1. Sinilh'i DMitction of Pnutical Formidir from /'oiMon't MitthrmatiaU
Theory.
Lot the components of the terrestrial magnetic force*, parallel to three
rectangular lines of refyrence fixed wilh reference to tbe ship, be denotwl
by X, Y, Z; the components at the point occupied by tho compaast of
combined magnetic force of earth and ship by X', T', Z' ; the componeut*
of that part o£ the ship's action depending on " pennaneot " or " snbpei^
maneut" magnetism, by P, Q, E, qnanKtiea which mathematically must
be regarded" na slowly varying parameters, their variations to bo deter-
mined for each ship by obsen-ation ; and the componenta of that part, of
the ship'n action which depends on transiently induced magnetism by
P, 1,'", BO tbat we have
X'=X+i»+P, T=T+j+Q, Z'=Z+r+E (1)
Laatiy, let (y», a,-), (?, x), (r, x) be the values which p. q, r would have if
the earth's force were of imit intensity, and in the direction of jt;
(p. .V). (7- y). (•;;/) the same for i/ : andjp.c), ('/,:), (r, s) the same for r.
By the elementary law of superposition of magnetic inductions tbe actual
value of p will be(j>,x)X + (p, y) T + (p, i) Z ; and corresponding ei-
pressioQS will give q and r. Hence, and by (1), we have
X' = X + (p,^)X + (j,,y)T + (p,:)Z+F, 1
T' = Y + (5,*)X+(9,i/)T + (v,y)Z + Q,L .... (2)
Z'= Z + (r,a;)X+ (r, 7j)Y + (r, z)Z + -R.}
These equations were first given by Poisson in 1824, in the fifth volume
of the Memoirs of the French Institute, p. 533. From these Smith
worked out practical formulie for the main case of application, that of a
ship on even keel, thus ; let
H be tho earth's horisroatal force ;
II' tho resultant of the earth's and ship's horizontal forces ;
0 the dip ;
a the ship's " magnetic course ; "
a' the ship's " compass course ; "
i = i—i' the deviation of the compass.
• Thut I«(osnj,tln> force experienced bj« unit magnetic polo. Thedinction of the
force is taken as tlmt of tlie force experienced by s aouth polo, or (according to Gilbert's
original nomenclature) tlie pnlcof ■ mngnet which is repelled from tbe soutliem regions
nf the oirth. British instrumcnt-mnkers unhappilj mark the north pole with S and
the south with N.
f Tbe length of the needle issuppowd in finitely «m all in conpariaon with the diatanM
of the nearest iron of the ship from the omtre of the oompan.
Then, if the diroctions of « be longitudinal from stem to head, y trans-
verae to Btarboard, r yertkally downwnrda, we have
X = H COS f,
X' = H'coai',
T =-
Y' = -
Hsinf,
H'Binf.
Besolving along and perpendicular to the direction of H we find, after
some reductions.
x^"'-«+»
int+Ccoi
t+B
.m2{+eco.2C,
ir
m
J=l+B
io.t-e.iii
t+»
C0.2J
-e.m2:.J
where
k =
.1 + (P, ') + (?■»),
a=
X
-(J>,S),
»■
-i[^'"'»'+IJ
e-
1[<"
«)-.+ §]
B
i(ft»)
! '
e-
Kii
't "■•'"■
Dividing the first by the second, of (3) we find
_3H-B sin<+Cco3f+Bain2C+gcf
,2{
"l+Bco8f-C8inf+BcoB2f-esin2{
(3)
(5)
which gires the deviation on any given magnetic course, i, when the
five coefficients 9, 33, C, fi, ft are known. Multiplying both numbers
by the denominator of the second member, and by cos i, and reducing,
we find
n3=aco3a+B8ini'+Cco8r+fi»in(C+O+ecoB(f+0.
(fl)
8iQ5=flcoB2+18sinf + a;coai'+B8in(2{'+3) + ecoB(2r+3). . (7)
These give the deviations expressed nearly, though not wholly, in terras
of the compass courses.
When the de>iations are of moderate amount, say not exceeding 30°,
equation (6) or (7) may be put under the comparatively simple and con-
venient form
Ss=A+B sin f'+Coos f+D sin 2;'+E COB 24^,
. (8)
in which the deviation is expressed wholly in tenna of the compass
courses ; and this will be sufficiently exact for practical purpoaeB,
- It will be seen that the '&, B, C, 9, ff are nearly the natural ainea of
the angles A, B, C, D, E.
2. Dyyoyraitu af Clou 11.
Tahe lengths numerically «jual to X, Y. Z and X', T', Z' for the «»-
(HiliiutM of two pointa. T)u> axes of (wonluiAt«s being fixed r^tirdr
to the ship, eoacKife the ship to be tnmed utto aU positions round b
fixod point Taken aa the origin of coordinates ; or for siropljcitr imapne
the bhip to 1k' fixed and the direction of the earth's ivsultant force to lake
mil ponilion*. it« ma^ilude remaining constant : the point (X. T, Z) will
ilways lip on B apbencal surface, [(i)) below); and the pobt (X', T", Z')
will alwayB lie on an ellipsoid fixed relntively to the ship. For we ha¥o
X-+T'+Z'=l', (9)
wbero I denotes the earth's resultant force. Now by (2) tolnd for
X, T, Z, WB express these quantities as linear functions of
X-P. T-Q, Z'-R.
Substituting these expressions for X, T, Z, in (9) we obtain a homoge-
neoiiH quadratic function of X'— P, Y" — Q, Z— R, equated to I", which
u the equation of an ellipsoid having F, Q, R, for the coordinates of its
centre.
It i- Tiotcworliiv that the point (X', T'. Z') is the position into which
the point (XTZ) of an elastic solid is brought by a translation (P, Q, R),
compounded with a homt^neous strain and rotation represented by the
matrix
^l + ip,^), {p,y), (P,^),-)
(9-^). l + (?, y)> (?,=).[ (10)
(r,^), (r,y), l+(r,r).|
Instead of drawing at once the dygogram surface for the resultaot of
the force of earth and ship (X', T', Z), draw according to precisely the
same rule, the dygogram surfaces for (X, T, Z), the earth's force, and
(X'-X, T'-T, Z'-Z), the force of the ship. The first of these will be
a sphere of radius I. The second will be an ellipsoid having its centre
at the point (P, Q, R). Let ON and OM be corresponding radius vectors
of these two surfaces. On OM, ON describe a parallelogram MOXK.
OK is the resultant force of earth and ship at the point occupied by the
ship's compass. Vary the construction by taking a "triangle of forces"
instead of the parallelogram, thus : — Produce MO through 0 to m, making
Cm equal to MO ; in other words, draw the dvgogram surface represent-
ing (X-X', T-T', Z-Z'); and of it Jet Ombe the radius vector cor-
responding to OM of the spherical -surface dygogram of the esrth's force.
Join Nm; through O draw OK equal and parallel to Nm, OK (the
same line as before) is the radius vector of the resultant dygogram sur-
face, corresponding to ON of the spherical dygogram. The law of cor-
Fespondence between N ou the spherical surface and m on the ellipsoid
is, according to (2) above, that m is the position to which M is brought —
translatioii ( — P, — Q, — B) and strain • with rotation, represented by
the matrix
](?.'). ft. J). (?,*[ (11)
Take any plane section (large or small circle) of the spherical surface.
The corresponding line on the ellipsoid is aUo a plane eection, but gene-
rally in a different plane from the other. For example, let the ship
revolve round a vertical axis OZ ; in other words, relatively to the ship
let ON revolve round OZ in a cone whose semi- vertical angle is fl, the
dip. The locus of N is a horiuiDtal circle whose radius is K, the hori-
zontal component of the earth's magnetic force. The corresponding
locus of m is an ellipse, not generally in the plane perpendicular to OZ —
that Is to say, not generally horizontal. This ellipse and that circle are
Smith's "Ellipse and Circle" {Admiralty Manual, 3rd edition, 1869,
App. 2, page 168). The projection of the ellipse on the plane of the
circle is the dygogram of what is wanted for the practical problem, namely
the horiiiontal component of the ship's force.
By a curious and interesting eonatruction (Admir^ty Manual, page 176)
Smith showed that, when 3 and C are zero, the ellipse and circle are
susceptible of a remarkable modification, by which, instead of them, an
altered circle and another circle (generally smaller) are found, nith a
perfectly simple law of corresponding points, to give, in accordance with
the general rule stated above, the magnitude and direction of the resul-
tant of horizontal force on the ship's compass. But in point of fact the
comparison with Dygogram No. I., by which (pages 168, 169) Smith in-
troduced Dygogram No. II., taken along with his previous mechanical
construction of Dygogram No. I. (pages 166, 167), proves that Dvgogram
No. II., simplified to two circles, is not confined to cases in which Sf and
<£ vanish, and so gives to this beautiful construction a greatly enhanced
theoretical interest. It is to be also remarked that, although the necessity
for supposing S and tt zero has been hitherto of little practical moment,
as their values are very small for ordinary positions of the compass in all
or nearly all ships at present in existence, the greatly increased quantity
of iron in the new turret ships, and its uosymmetrical disposition in ttra
newest projected type (the ' Inflexible '), may be expected to give unpre-
cedentedly great values to tt and 9. The happy artifice by which Smith
found two circles to serve for the " ellipse and circle " consisted in alter-
ing the radius of the first circle from H to XH. If, further, we alter it
■ Thin ttnin must include refleiioD id a pisns mirror » ai not to eiclude DrgatiT«
Tallin exceeding certam limita in the conatituenia of the matrix. It is to be borne ia
mind that, imaginaij Taluea of the elementa being excluded, atratn and refleiioil cm
only alter ^herce or ellipaoida to ipherea or alLpMod*, not to bjperbalouSa.
■^
Ui owigoihide wjd direyrtion, auil m.ike it repn-aent the rcAultaur itf Mt
to north and 31 to east, thus iaduding pwt of the ship's frnw. Daiu»-Jv
(A— l)IIlonortliand 3 toPttst, alcmgwith the eMth's horiKOHt»] fonv in
o<ie circiilar dygogram, the ivsidue of the hoiisoutat ooiniwnenl. of ihf
ship's fonx has also s circular dvgogram. The constnirtion lhu» ublaiiied
is fuUv described and illustrated by a diagnm uudiT the hetwliug '■ Dv-
gognm Ho. 11., shore. The proof gf this is very simple. The follow-
ing is the anJj-tical proWcm of uhich it is the solution: — In the genera!
eauations (2) suppose Z to be constant, and put
X'-(j..z)Z-P=X-, Y'-(,,=)T-(J-T- (12)
We havi
(13)
X-=tI+C(.,x)]X+(p,.,)T. ,
T"= (,.,)X+p+(,,s)]Tj
es (ellipses or circles) to be constructed
y') given by the equations
Now imagine hio dygogram cii
as the locus of points (a",?.), (a
3r=X+(nX+/3T5;
y=X"-X-(aX-f^Y);
and let it be required to find a
circles; we have four equmtic
Then, Bs
y=T+(yX+aT); I . . (14)
y-=T"-Y-(yX + JT);J
(i, y, t Hojliat these two currea may be
IS for these four unknown quantities.
=X", y'+y=T;
the resultant of the radius vectors of the two concentric circles thus ob-
tained is the resultant of the constituent (X", Y") of the force on the
compasB; and by (12) we have only to shift the centre of one of them to
the point whose coordinates are (j>, a) Z -|- P, (7, z) Z -f- Q, to find two
circles such that the resultant of corresponding radius vectors through the
centre of one of them shall be the whole horizontal component of the
forc« on the compass. Thus we have Smith's beautiful and most useful
Dygc^ram of two Circles. — W. T., Jaiiuary 1874.
To avoid fine, thb book should be returned on
or before the date Ust stamped below
jui 1 3 no
1
I