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,A  &&•• 


To 
Fellow  Workers  in  the  Biological  Sciences, 

Architects  of  Progress, 
Who  Hew  the  Stone  to  Build  Where  Unseen  Spires  Shall  Stand 


6?  D 


CONTENTS 

PREFACE  TO  THE  THIRD  EDITION ix 

PREFACE  TO  THE  FIRST  EDITION xiii 

CHAPTER  I 

INTRODUCTION  AND  THE  SIMPLER  EQUILIBRIUM  EQUATIONS  FOR  ACIDS 
AND  BASES 1 

CHAPTER  II 
SOME  SPECIAL  ASPECTS  OF  ACID-BASE  EQUILIBRIA 35 

CHAPTER  III 
OUTLINE  OF  A  COLORIMETRIC  METHOD 62 

CHAPTER  IV 
CHOICE  OF  INDICATORS 67 

CHAPTER  V 
THEORY  OF  INDICATORS 99 

CHAPTER  VI 

APPROXIMATE  DETERMINATIONS  WITH  INDICATORS 119 

CHAPTER  VII 
THE  APPLICATION  OF  SPECTROPHOTOMETRY,  COLORIMETRY,  ETC 141 

CHAPTER  VIII 
SOURCES  OF  ERROR  IN  COLORIMETRIC  DETERMINATIONS 177 

CHAPTER  IX 
STANDARD  BUFFER  SOLUTIONS 192 

CHAPTER  X 

OUTLINE  OF  THE  "HYDROGEN-ELECTRODE"  METHOD 221 

CHAPTER  XI 

ON  CHANGES  OF  FREE-ENERGY 230 

CHAPTER  XII 

THEORY  OF  THE  HYDROGEN-ELECTRODE 251 

CHAPTER  XIII 

POTENTIAL  DIFFERENCES  AT  LIQUID  JUNCTIONS 264 

v 


VI  CONTENTS 

CHAPTER  XIV 
HYDROGEN  HALF-CELLS 281 

CHAPTER  XV 

CALOMEL  AND  OTHER  STANDARD  HALF-CELLS 303 

CHAPTER  XVI 

THE    POTENTIOMETER,    NULL-POINT    INSTRUMENTS    AND    ACCESSORY 
EQUIPMENT 317 

CHAPTER  XVII 

HYDROGEN  GENERATORS,  WIRING,  INSULATION,  SHIELDING,  TEMPERA- 
TURE CONTROL,  PURIFICATION  OF  MERCURY 350 

CHAPTER  XVIII 

OXIDATION-REDUCTION  POTENTIALS 367 

CHAPTER  XIX 

THE  QUINHYDRONE  AND  SIMILAR  HALF-CELLS 404 

CHAPTER  XX 

METAL-OXIDE  ELECTRODES.  THE   GLASS   ELECTRODE.    THE   OXYGEN 
ELECTRODE 423 

CHAPTER  XXI 
SOURCES  OF  ERROR  IN  ELECTROMETRIC  MEASUREMENTS 434 

CHAPTER  XXII 

TEMPERATURE  COEFFICIENTS 448 

CHAPTER  XXIII 

STANDARDIZATION  OF  PH-MEASUREMENTS. 461 

CHAPTER  XXIV 

STANDARD  SOLUTIONS  FOR  THE   ROUTINE   CHECKING   OF  HYDROGEN 
ELECTRODE  MEASUREMENTS 483 

CHAPTER  XXV 
THE  THEORY  OF  DEBYE  AND  HUCKEL 489 

CHAPTER  XXVI 
SUPPLEMENTARY  METHODS 513 

CHAPTER  XXVII 
AN  ALTERNATE  METHOD  OF  FORMULATING  ACID-BASE  EQUILIBRIA 519 


CONTENTS 


Vll 


CHAPTER  XXVIII 
ELEMENTARY  THEORY  OF  TITRATION 530 

CHAPTER  XXIX 
NON-AQUEOUS  SOLUTIONS 539 

CHAPTER  XXX 

APPLICATIONS 549 

BIBLIOGRAPHY 587 

APPENDICES 

TABLE  A.  ARBITRARILY  STANDARDIZED  VALUES  FOR  HALF-CELLS  ....  672 

TABLE  B.  RELATION  OF  [H+]  TO  pH ' 673 

TABLE  C.  FACTORS  FOR  CONCENTRATION  CELLS  0°C.  TO  70°C 674 

TABLE  D.  CORRECTION  OF  BAROMETER  READING  FOR  TEMPERATURE.  .  675 

TABLE  E.  BAROMETRIC  CORRECTIONS  FOR  H-ELECTRODE  POTENTIALS  .  676 

a.  a 

TABLE  F.     VALUES  OF  LOG  AND  OF  LOG MULTIPLIED  BY 

1  -  a.  I  -  a 

THE  TEMPERATURE  FACTORS  FOR  CONCENTRATION  CELLS.  677 

TABLE  G.    DISSOCIATION  EXPONENTS  OF  ACIDS 678 

TABLE  H.    DISSOCIATION  CONSTANTS  AND  ASSOCIATION  EXPONENTS 

OF  BASES 679 

TABLE   I.    DISSOCIATION  EXPONENTS  AND  ASSOCIATION  EXPONENTS 

OF  AMINO  ACIDS 680 

TABLE   J.    HALF  TRANSFORMATION  POINTS  OF  ALKALOIDS 681 

TABLE  K.    RELATION    OF    PERCENTAGE    REDUCTION    TO    POTENTIAL 

AT  CONSTANT  pH 682 

TABLE  L.    E'0  VALUES    FOR  SEVERAL  OXIDATION  REDUCTION  INDI- 
CATORS AT  30°C 683 

TABLE  M.     SYMBOLS  AND  CONVENIENT  FORMULAS 684 

TABLE  N.    DEFINITIONS  FOR  THE  MOST  PART  NOT  INCLUDED  IN  THE 

TEXT 684 

TABLE   O.    TABLE  OF  LOGARITHMS 690 

INDEX  OF  AUTHORS 693 

INDEX  OF  SUBJECTS  . .  . .  •. 703 


PREFACE  TO  THE  THIRD  EDITION 

Within  the  past  twenty  years  methods  of  determining  hydrion 
concentration  have  served  well  in  the  exploration  of  many  and 
divers  subjects.  But  the  period  of  general  exploration  is  drawing 
to  a  close  and  long  ago  there  were  begun  exact  studies  of  equilibria, 
or  of  kinetic  events  in  which  hydrions  participate.  Refinement 
of  technique,  variety  of  method  and  elegance  of  formulation  are 
in  greater  demand.  Accordingly  there  have  been  added  in  this 
edition  chapters  or  sections  bearing  upon  each  of  these  aspects, 
and  the  old  text  has  been  almost  entirely  rewritten  to  conform 
to  the  revised  presentation.  There  results  a  superficial  appear- 
ance as  of  a  more  exhaustive  treatment.  However,  the  require- 
ments of  a  new  age  have  far  outrun  the  range  of  subject  and  the 
depth  of  treatment  that  can  be  encompassed  with  adherence  to 
the  more  or  less  discoursive  style  of  presentation  which  it  has 
seemed  best  to  use.  Consequently  this  enlarged  edition  remains 
more  elementary  in  relation  to  the  needs  of  today  than  was  the 
first  edition  in  relation  to  the  needs  of  its  period. 

The  expansion  has  not  led  to  a  wholly  satisfactory  product. 
For  the  faults  of  comprehension  or  of  exposition  I  need  ask  no 
charity.-  It  cannot,  or  should  not,  be  given  in  such  matters.  But 
I  feel  compelled  to  shift  to  the  times  some  responsibility  for  one 
or  two  of  the  major  faults  of  this  book. 

So  varied  and  extensive  are  the  applications  of  the  methods, 
the  details  of  technique  and  the  special  forms  of  theory  that  it  is 
become  about  as  ridiculous  to  attempt  to  recount  all  aspects 
within  one  text  as  it  would  be  to  note  all  the  uses  of  the  thermom- 
eter, all  types  of  data  to  which  is  affixed  the  symbol  °C.  and  at 
the  same  time  to  exhaust  the  theory  of  thermometry.  But, 
having  set  out  to  glean  from  the  literature  important  informa- 
tion which  I  think  is  still  desired  in  one  text,  I  believe  the  reader 
will  be  interested  in  a  survey  incidental  to  this  task  and  de- 
scribed by  the  accompanying  chart. 

The  data  were  compiled  as  follows.  The  number  of  papers 
for  each  of  the  years  from  1910  to  1920  was  taken  from  the  bibli- 

ix 


PREFACE    TO    THIRD    EDITION 


ography  of  the  second  edition.  Estimates  for  each  of  the  subse- 
quent years  were  made  as  follows.  Several  numbers  of  Chemical 
Abstracts  for  each  year  were  taken  at  random  and  carefully 
searched  in  all  sections  for  papers  which  seemed  to  conform  to 
the  types  included  in  the  bibliography  of  the  second  edition. 
From  the  number  of  pages  searched  and  the  number  of  pages  for 
the  year  the  number  of  such  articles  for  that  year  was  calculated. 
Of  course,  a  serious  question  of  personal  judgment  enters.  This 
need  not  be  discussed,  for  I  trust  the  reader  to  recognize  in  the 
chart  what  he  himself  must  have  felt  is  happening  in  his  own 
specialty. 


1500 

1400 

1300 

1200 

to  1100 

£  1000 

£  90° 

**"  800 

0  700 
K  600 
<n  500 

1  400 
Z    300 

200 
100 


frrr 


YEAR 

The  situation  has  made  obsolete  some  of  the  old  ideals  of 
scholarship.  It  has  made  trivial  all  available  facilities  of  library, 
abstract  and  review.  It  has  made  the  monograph  almost  futile. 
It  has  made  ridiculous  him  who  claims  to  combine  thorough 
investigation  with  thorough  re-search. 

Undoubtedly  the  mediaeval  scholar  felt  oppressed  by  the  mag- 
nitude of  his  specialty  in  his  time  and  looked  forward  with  mis- 
giving to  the  "impossible"  tasks  of  the  future;  and  yet,  with  no 
vacation  such  as  Sir  Ernest  Rutherford  whimsically  prays  for 
as  a  need  of  the  present,  scholarship  survived  then  and  doubtless 
will  now.  However,  there  was  one  disease  of  mediaeval  times 
that  had  to  be  cured  before  the  intellect  came  to  renewed  health 
and  to  vigor  adequate  for  enlarged  tasks.  I  fear  that  we  may  be 


PREFACE   TO   THIRD    EDITION  XI 

reinfected.  It  was  the  pursuit  of  "vanishing  particulars"  and 
the  employment  of  conveniences  suited  to  a  purpose.  A  new  age 
has  brought  new  purposes  and  an  equal  sincerity  of  a  new  type 
that  makes  us  sometimes  scorn  the  old;  but  amid  the  abundance 
of  our  learning  the  instinct  of  mastery  has  driven  us  to  take 
refuge  in  specialization  wherein  we  are  at  liberty  to  make  our 
neighbors  the  victims  of  our  conveniences.  They  are  the  con- 
veniences of  special  terminologies  suited  to  the  immediate  need  of 
the  specialist  but  barriers  to  earnest  seekers  of  the  contents  of 
the  specialty.  They  are  the  conveniences  of  special  formulations 
suited  to  the  immediate  needs  of  the  case  but  barriers  to  the 
widespread  use  of  the  meaning  of  the  case.  While  I  have  tried 
to  avoid,  so  far  as  possible,  discussion  of  the  less  significant  in- 
stances, I  conceive  it  to  be  the  function  of  this  book  to  tell  about 
a  few  of  the  more  important  matters  in  terms  agreeing  essentially 
with  those  which  the  reader  will  have  to  know  in  his  study  of 
the  literature.  Partly  because  the  literature  is  what  it  is,  the 
subject  is  not  here  presented  as  I  conceive  some  genius  will  some 
day  present  it — with  brilliant  simplicity  and,  withal,  rigidly. 

To  those  who,  in  philosophic  mood,  would  question  what  I 
mean  by  simplicity  and  rigidity  I  will  answer  that  the  pro- 
nouncements of  genius  determine  this,  that  we  recognize  it  when 
it  comes  and  dream  of  it  before  it  comes.  And  come  it  must  if 
those  who  labor  with  life  chemistry  are  ever  to  apply  effectively 
all  the  pertinent  information  being  gathered,  often  with  lack  of 
systematic  thoroughness  and  being  recorded  with  ever  increasing 
inavailability. 

In  undertaking  the  difficult  task  of  revision  I  have  sought  and 
have  been  generously  given  the  aid  of  many  friends  and  authori- 
ties. Since  none  of  these  has  seen  the  manuscript  in  final  form 
I  shall  not  note  the  subjects  on  which  advice  was  given,  lest,  per- 
chance, the  mishandling  of  the  advice  reflect  upon  the  giver. 
I  hope  that  this  will  not  seem  to  detract  from  the  gratitude  I 
have  or  from  the  credit  due  to : 

Mr.  C.  E.  Abromavich  Dr.  Lloyd  Felton 

Mr.  Alan  Bernstein  Dr.  F.  Fenwick 

Dr.  William  Blum  Dr.  H.  D.  Gibbs 

Dr.  Barnett  Cohen  Dr.  A.  Grollman 

Dr.  N.  Ernest  Dorsey  Dr.  Louis  J.  Gillespie 


Xll  PREFACE   TO   THIRD   EDITION 

Dr.  A.  Baird  Hastings  Dr.  W.  A.  Perlzweig 

Dr.  Leslie  Hellerman  Dr.  A.  H.  Pfund 

Dr.  Morris  Kharasch  Dr.  Julius  Sendroy,  Jr. 

Dr.  H.  R.  Kraybill  Dr.  George  Scatchard 

•  Dr.  Victor  K.  LaMer  Dr.  S.  E.  Sheppard 

Dr.  E.  K.  Marshall,  Jr.  Dr.  Edgar  T.  Wherry 

Dr.  George  Morey  Dr.  D.  D.  Van  Slyke 

Dr.  Leonor  Michaelis  Dr.  G.  W.  Vinal 

and 

the  publishers. 

Needless  to  say  I  have  drawn  freely  upon  the  literature.     I  hope 
that  I  have  given  adequate  credit  at  the  proper  places  in  the  text. 
Baltimore,  Maryland 
Easter  Sunday,  1928 


PREFACE  TO  THE  FIRST  EDITION 

Poincare*  in  The  Foundations  of  Science  remarks,  ( 'There  are 
facts  common  to  several  sciences,  which  seem  the  common  source 
of  streams  diverging  in  all  directions  and  which  are  comparable 
to  that  knoll  of  Saint  Gothard  whence  spring  waters  which  fer- 
tilize four  different  valleys." 

Such  are  the  essential  facts  of  electrolytic  dissociation. 

Among  the  numerous  developments  of  the  theory  announced 
by  Arrhenius  in  1887  none  is  of  more  general  practical  importance 
than  the  resolution  of  "acidity"  into  two  components — the  con- 
centration of  the  hydrogen  ions,  and  the  quantity  of  acid  capable 
of  furnishing  this  ionized  hydrogen.  For  two  reasons  the  hydro- 
gen ion  occupies  a  unique  place  in  the  esteem  of  students  of 
ionization.  First,  it  is  a  dissociation  product  of  the  great  majority 
of  compounds  of  biochemical  importance.  Second,  it  is  the  ion 
for  which  methods  of  determination  have  been  best  developed. 
Its  importance  and  its  mensurability  have  thus  conspired  to  make 
it  a  center  of  interest.  The  consequent  grouping  of  phenomena 
about  the  activity  of  the  hydrogen  ion  is  unfortunate  when  it 
confers  undue  weight  upon  a  subordinate  aspect  of  a  problem  or 
when  it  tends  to  obscure  possibilities  of  broader  generalization. 
Nevertheless,  such  grouping  is  often  convenient,  often  of  im- 
mediate value  and  frequently  illuminating.  Especially  in  the 
field  of  biochemistry  it  has  coordinated  a  vast  amount  of  material. 
It  has  placed  us  at  a  point  of  vantage  from  which  we  must  look 
with  admiration  upon  the  intuition  of  men  like  Pasteur,  who, 
without  the  aid  of  the  precise  conceptions  which  guide  us,  handled 
"acidity"  with  so  few  mistakes. 

In  the  charming  descriptions  of  his  experimental  work  Pasteur 
has  given  us  glimpses  of  his  discernment  of  some  of  the  effects  of 
"acidity"  in  biochemical  processes.  In  the  opening  chapter  of 
Studies  on  Fermentation  he  noted  that  the  relatively  high  acidity 
of  must  favors  a  natural  alcoholic  fermentation  in  wine,  while  the 
low  acidity  of  wort  induces  difficulties  in  the  brewing  of  beer. 
He  recognized  the  importance  of  acidity  for  the  cultivation  of 

xiii 


XIV  PREFACE    TO    FIRST   EDITION 

the  bacteria  which  he  discovered  and  was  quick  to  see  the  lack  of 
such  an  appreciation  in  his  opponents.  In  describing  that  process 
which  has  come  to  bear  his  name  Pasteur  remarks,  "It  is  easy 
to  show  that  these  differences  in  temperature  which  are  required 
to  secure  organic  liquids  from  ultimate  change  depend  exclusively 
upon  the  state  of  the  liquids,  their  nature  and  above  all  upon  the 
conditions  which  affect  their  neutrality  whether  towards  acids  or 
bases."  The  italics,  which  are  ours,  emphasize  language  which 
indicates  that  Pasteur  was  aware  of  difficulties  which  were  not 
removed  till  recently.  Had  Pasteur,  and  doubtless  others  of  like 
discernment,  relied  exclusively  upon  volumetric  determination  of 
acidity  they  would  certainly  have  fallen  into  the  pitfalls  which 
at  a  later  date  injured  the  faith  of  the  bacteriologist  in  the  meth- 
ods of  the  chemist.  Was  it  reliance  upon  litmus  which  aided 
him?  Perhaps  the  time  factor  involved  in  the  use  of  litmus 
paper,  which  is  now  held  as  a  grave  objection,  enabled  Pasteur 
to  judge  between  extremes  of  reaction  which  the  range  of  litmus 
as  an  indicator  in  equilibrium  does  not  cover.  At  all  events  he 
recognized  distinctions  which  we  now  attribute  to  hydrogen  ion 
concentrations.  Over  half  a  century  later  we  find  some  of 
Pasteur's  suggestions  correlated  with  a  marvelous  development 
in  biochemistry.  The  strongest  stimulus  to  this  development 
can  doubtless  be  traced  to  the  work  of  S0rensen  at  the  Carlsberg 
Laboratory  in  Copenhagen  and  not  so  much  to  his  admirable 
exposition  of  the  effect  of  the  hydrogen  ion  upon  the  activity  of 
enzymes  as  to  his  development  of  methods.  At  about  the  same 
time  Henderson  of  Harvard,  by  setting  forth  clearly  the  equilibria 
among  the  acids  and  bases  of  the  blood,  indicated  what  could  be 
done  in  the  realm  of  physiology  and  stimulated  those  researches 
which  have  become  one  of  the  most  beautiful  chapters  in  this 
science. 

Today  we  find  new  indicators  or  improved  hydrogen  electrode 
methods  in  the  physiological  laboratory,  in  the  media  room  of  the 
bacteriologist,  serving  the  analyst  in  niceties  of  separation  and 
the  manufacturer  in  the  control  of  processes.  The  material 
which  was  admirably  summarized  by  Michaelis  in  1914,  and  to 
which  Michaelis  himself  had  contributed  very  extensively,  pre- 
sents a  picture  whose  significance  he  who  runs  may  read.  There 
is  a  vast  field  of  usefulness  for  methods  of  determining  the  hydro- 


PREFACE    TO    FIRST   EDITION  XV 

gen  ion.  There  is  real  significance  in  the  fruits  so  far  won. 
There  remain  many  territories  to  explore  and  to  cultivate.  We 
are  only  at  the  frontier. 

In  the  meantime  it  will  not  be  forgotten  that  our  knowledge  of 
the  hydrogen  ion  is  an  integral  part  of  a  conception  which  has 
been  under  academic  study  for  many  years  and  that  the  time  has 
come  when  the  limitations  as  well  as  certain  defects  are  plainly 
apparent.  While  there  is  now  no  tendency  nor  any  good  ground 
to  discredit  the  theory  of  electrolytic  dissociation  in  its  essential 
aspects,  there  is  dissatisfaction  with  some  of  the  quantitative 
relationships  and  a  demand  for  broader  conceptions.  It  requires 
no  divination  to  perceive  that  while  we  remain  without  a  clear 
conception  of  why  an  electrolyte  should  in  the  first  instance 
dissociate,  we  have  not  reached  a  generalization  which  can  cover 
all  the  points  now  in  doubt.  Perhaps  the  new  developments  in 
physics  will  furnish  the  key.  When  and  how  the  door  will  open 
cannot  be  foreseen ;  but  it  is  well  to  be  aware  of  the  imminence  of 
new  developments  that  we  may  keep  our  data  as  pure  as  is  con- 
venient and  emphasize  the  experimental  material  of  permanent 
value.  We  may  look  forward  to  continued  accumulation  of 
important  data  under  the  guidance  of  present  conceptions,  to 
distinguished  services  which  these  conceptions  can  render  to 
various  sciences  and  to  the  critical  examination  of  the  material 
gathered  under  the  present  regime  for  the  elements  of  permanent 
value.  These  elements  will  be  found  in  the  data  of  direct  experi- 
mentation, in  those  incontrovertible  measurements  which,  though 
they  be  but  approximations,  have  immediate  pragmatic  value 
and  promise  to  furnish  the  bone  and  sinew  of  future  theory.  In 
the  gathering  of  such  data  guiding  hypotheses  and  coordinating 
theories  are  necessary  but  experimental  methods  are  vital. 

The  time  seems  to  have  come  when  little  of  importance  is  to 
be  accomplished  by  assembling  under  one  title  the  details  of 
the  manifold  applications  of  hydrogen  electrode  and  indicator 
methods.  It  would  be  pleasing  to  have  in  English  a  work  com- 
parable in  scope  with  MichaehV  Die  Wasserstoffionenkonzentra- 
tion;  but  even  in  the  short  years  since  the  publication  of  this 
monograph  the  developments  in  special  subjects  have  reached 
such  detail  that  they  must  be  redispersed  among  the  several  sci- 
ences, and  made  an  integral  part  of  these  rather  than  an  unco- 


XVI  PREFACE    TO    FIRST    EDITION 

ordinated  treatise  by  themselves.  There  remains  the  need  for  a 
detailed  exposition,  under  one  cover,  of  the  two  methods  which 
are  in  use  daily  by  workers  in  several  distinct  branches  of  bio- 
logical science.  It  is  not  because  the  author  feels  especially 
qualified  to  make  such  an  exposition  that  this  book  is  written, 
but  rather  because,  after  waiting  in  vain  for  such  a  book  to 
appear,  he  has  responded  sympathetically  to  appeals,  knowing 
full  well  from  his  own  experience  how  widely  scattered  is  the 
information  under  daily  requisition  by  scores  of  fellow  workers. 

For  the  benefit  of  those  to  whom  the  subject  may  be  new 
there  is  given  in  the  last  chapter  a  running  summary  of  some  of 
the  principal  applications  of  the  methods.  This  is  written  in 
the  form  of  an  index  to  the  bibliography,  a  bibliography  which 
is  admittedly  incomplete  for  several  topics  and  unbalanced  in 
others,  but  which,  it  is  believed,  contains  numerous  nuclei  for 
the  assembling  of  literature  on  various  topics. 

The  author  welcomes  this  opportunity  to  express  his  apprecia- 
tion of  the  broad  policy  of  research  established  in  the  Dairy  Divi- 
sion Laboratories  of  the  Department  of  Agriculture  under  the 
immediate  administration  of  Mr.  Rawl  and  Mr.  Rogers.  Their 
kindness  and  encouragement  have  made  possible  studies  which 
extend  beyond  the  range  of  the  specialized  problems  to  which 
research  might  have  been  confined  and  it  is  hoped  that  the  bread 
upon  the  waters  may  return.  To  Dr.  H.  A.  Lubs  is  due  the  credit 
for  studies  on  the  synthesis  of  sulfonphthalein  indicators  which 
made  possible  their  immediate  application  in  bacteriological 
researches  which  have  emanated  from  this  laboratory.  Acknowl- 
edgment is  hereby  made  of  the  free  use  of  quotations  taken 
from  the  paper  The  Colorimetric  Determination  of  Hydrogen  Ion 
Concentration  and  Its  Applications  in  Bacteriology  published  in 
the  Journal  of  Bacteriology  under  the  joint  authorship  of  Clark 
and  Lubs. 

The  author  thanks  his  wife,  his  mother,  Dr.  H.  W.  Fowle  and 
Dr.  H.  Connet  for  aid  in  the  correction  of  manuscript  and  proof, 
and  Dr.  Paul  Klopsteg  for  valuable  suggestions. 

It  is  a  pleasure  to  know  that  the  publication  of  the  photograph 
of  Professor  S.  P.  L.  S0rensen  of  the  Carlsberg  Laboratory  in 
Copenhagen  will  be  welcomed  by  American  biochemists  all  of 
whom  admire  his  work. 

Chevy  Chase,  Maryland 
March  17,  1920 


CHAPTER  I 

INTRODUCTION 

AND 
THE  SIMPLER  EQUILIBRIUM  EQUATIONS  FOR  ACIDS  AND  BASES 

In  a  country  rich  in  gold  observant  wayfarers  may  find  nuggets  on 
their  path,  but  only  systematic  mining  can  provide  the  currency 
of  nations. — SIR  FREDERICK  HOPKINS. 

INTRODUCTION 

"Acid"  still  means  sour,  like  vinegar.  This  common  meaning 
preserves  the  ancient  flavor  of  the  word  and  recalls  the  fact  that 
the  modern  highly  technical  meaning  had  its  origin  in  the  grouping 
of  substances  by  type.  In  this  there  is  a  resemblance  to  the  pro- 
cedure of  the  botanist  who  in  the  last  analysis  determines  a 
species  by  reference  to  a  type  specimen.  But  once  we  pass  beyond 
the  mere  origin  of  the  modern  meaning  we  may  trace  persistent 
searches  among  the  sour  or  vinegar-like  substances  for  the  nature 
of  that  community  of  properties  which  came  to  be  regarded  as  of 
much  more  fundamental  interest  than  the  classification  itself. 
Each  attempt  bears  the  imprint  of  its  age.  By  Paracelsus  the 
community  of  properties  was  supposed  to  reside  in  the  Acidum 
primogenium.  By  Lavoisier,  the  discoverer  of  the  true  nature  of 
oxygen,  it  was  associated  with  oxygen.  Mills,  in  philosophic 
mood,  called  it  a  function.  In  the  age  of  structural  and  atomic 
chemistry  it  was  hydrogen  so  placed  in  a  compound  as  to  be 
replaceable  by  a  metal.  Fortunately  no  categorical  distinction 
between  property,  function,  substance,  etc.,  deterred  the  searchers. 

Among  the  properties  common  to  the  sour  or  acid  substances 
is  their  submission  to  the  "killing"1  effect  of  alkalies.  "Alkali" 

1  The  word  "kill,"  taken  from  the  vernacular  discussion  of  the  phenom- 
enon in  question,  is  much  more  appropriate  to  this  stage  of  the  discussion 
than  certain  other  words  like  "neutralize"  which,  in  the  parlance  of  the 
laboratory,  have  acquired  meanings  so  specialized  and  at  the  same  time  so 
diverse  as  to  obscure  meaning  very  successfully. 

1 


2  THE    DETERMINATION   OF   HYDROGEN   IONS 

is  said  to  originate  in  an  Arabic  word  meaning  the  ashes  of  plants. 
From  this  origin  has  arisen  a  variety  of  meanings  illustrating  ad- 
mirably another  search  for  an  account  of  another  community  of 
properties.  From  wood  ashes  has  been  isolated  potassium,  a  metal 
having  properties  in  common  with  lithium,  sodium,  etc.  This 
series  is  now  known  as  that  of  the  "alkali  metals."  To  a  certain 
degree  their  properties  extend  to  the  group  of  metals  known  as 
the  "alkaline  earths."  Metals  of  either  group  act  vigorously 
upon  water  and  the  resulting  solutions  have  preeminently  a 
property  in  common  with  the  leachings  of  wood  ashes.  They 
"kill"  the  acidity  of  acid  solutions.  They  are  "alkaline." 

An  alkali  upon  interacting  with  an  acid  forms  a  salt,  for  example 
caustic  potash  and  hydrochloric  acid  form  the  salt  potassium 
chloride.  In  a  chemistry  which  elevated  the  importance  of  the 
metals,  the  potassium  in  potassium  chloride  held  the  center  of 
interest.  It  was  considered  the  base  of  the  salt.  But  "base"  in 
this  sense  is  going  out  of  common  usage.  Again  a  property,  the 
basic  property,  has  been  abstracted  and  "base"  is  now  the  pre- 
ferred word  with  which  to  denote  all  substances,  organic  as  well 
as  inorganic,  which  act  like  the  leachings  of  wood  ashes  in  killing 
acids. 

There  are  many  evidences  of  the  mutual  destruction  (complete 
or  partial)  of  properties  of  the  two  groups,  when  acids  and  bases 
interact.  Attempts  to  systematize  these  evidences  have  had  their 
important  part  in  developing  a  classification  of  specific  substances 
into  acidic  and  basic  compounds.  Some  of  the  systems  of 
classification  have  extended  far  beyond  the  bounds  of  their  con- 
crete origin.  We  need  not  recreate  for  ourselves  the  perplexities 
which  arose  during  attempts  to  make  the  classification  of  acids 
and  bases  scientifically  definite.  But  in  passing  we  may  recall 
that  the  older  theories  were  reduced  by  the  "practical"  chemist 
to  meet  his  demand  that  an  acid  solution  turn  litmus  red  and  an 
alkaline  solution  turn  litmus  blue.  The  ghost  of  this  delight- 
fully simple  basis  still  lingers  about  the  laboratory,  although  the 
litmus  test  is  now  recognized  as  hopelessly  inadequate  for  analysis, 
for  organic  synthesis,  for  biochemistry,  and  for  a  host  of  industrial 
processes.  If  we  ignore  the  older  classifications,  it  is  not  be- 
cause there  is  any  occasion  to  disclaim  our  debt  to  the  early  in- 
vestigators. They  provided  the  foundations  of  our  far-reaching 


I  ACIDS   AND    BASES  3 

subject.  From  these  foundations  have  arisen  some  concepts  and 
some  specific  data  of  such  importance  as  to  merit  our  entire 
attention.  The  purely  historical  we  shall  leave  to  the  historian. 

We  need  only  note  that  the  process  of  abstraction  has  progressed 
until  a  property  common  to  wood  ashes,  alkali  carbonates,  hy- 
droxides in  general  and  a  host  of  organic  compounds  has  been 
elevated  to  unique  distinction.  A  similar  abstraction  has  occurred 
in  the  treatment  of  acids;  and  at  last  we  associate  properties  with 
material  entities  again.  The  entities  appear  in  the  following 
definitions,  and  their  associations  with  properties  appear  in  those 
manifold  consequences  which  will  be  touched  upon  throughout 
this  book. 

For  present  purposes  we  may  define  an  acid  as  any  substance 
which  is  capable  of  supplying  to  its  solution,  or  to  another  sub- 
stance, hydrogen  bearing  a  positive  electric  charge.  An  instance 
is  hydrogen  chloride,  HC1,  which  splits  to  form_H+  and  Cl~. 

Likewise  we  may  define  a  base  as  any  substance  which  is 
capable  of  supplying  to  its  solution  or  to  another  substance  the 
electronegative  group  OH~.  An  instance  is  sodium  hydroxide, 
NaOH,  which  splits  to  form  Na+  and  OH~. 

Like  the  Greeks  who  personified  the  virtues,  we,  having  em- 
bodied the  acidic  and  the  basic  properties,  have  lifted  to  our 
Olympus  the  hydrogen  and  the  hydroxyl  ions,  H+  and  OH~. 
Furthermore  the  current  conception  of  the  nature  of  acids  and 
bases  bears  the  imprint  of  the  age  of  electricity. 

Having  touched  upon  the  electrical  aspect  we  might  be  tempted 
to  carry  the  theme  forward  into  the  whirl  of  current  concepts 
regarding  the  electrical  nature  of  matter.  Some  of  these  con- 
cepts will  be  used  in  later  chapters;  but,  for  the  most  part,  they 
will  not  be  essential  to  our  present  theme.  Without  necessarily 
losing  sight  of  adjacent  subjects,  we  may,  (as  we  are  entitled 
to  do)  establish  a  province  for  our  own  subject.  We  may  draw 
from  the  adjacent  subject  helpful  pictures;  but  as  our  theme  pro- 
gresses it  will  be  perceived  that  our  task  is  to  formulate  a  set  of 
phenomena,  that  the  organization  of  the  material  within  the  chosen 
province  is  our  subject  and  that  any  reconstruction  of  the  physical 
meaning  of  the  terms  will  affect  but  little  the  essential  organiza- 
tion with  which  we  are  concerned. 


THE   DETERMINATION    OF   HYDROGEN   IONS 


All  too  briefly  we  shall  touch  first  upon  the  adjacent  subject. 

According  to  current  conceptions,  the  atom  of  hydrogen,  the  simplest 
of  the  chemical  elements,  concentrates  the  greater  part  of  its  mass  in  a 
nucleus  having  unit,  positive,  electrical  charge.  (See  figure  1,  a.)  Fre- 
quently this  nucleus  is  called  the  proton.  About  this  rotates  an  electron, 
the  unit,  negative,  electric  charge.  This  apposition  of  the  unit  charges  of 
opposite  sign  renders  the  atom  as  a  whole  electrically  neutral. 


a 

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FIG.  1.  SCHEMATA  OP  ELEMENTS,  MOLECULES  AND  IONS 
Nuclei  with  +  charges;  electrons  with  —  charges,     a,  hydrogen  atom; 
6,  hydrogen  molecule;  c,  carbon  atom;  d,  methane  molecule;  e,  chlorine 
atom;  /,  hydrogen  chloride  molecule;  g,  hydrogen  ion;  h,  chloride  ion. 

Atoms  of  other  elements  are  built  of  nuclei  having  several  excess  positive 
electrical  charges  and  of  extra-nuclear,  planet-like  electrons,  the  total 
number  of  which  in  the  electrically  neutral  atom  must  be  equal  to  the  net, 
nuclear,  positive  charge.  (See  figure  1,  c  and  e.)  This  number  is  the 
.so-called  atomic  number  of  the  element.  For  example  the  atomic  number 
of  carbon  is  6  and  of  chlorine  17. 

It  is  profitable  to  assume  that  the  essential,  structural  aspect 
of  compound  formation  is  a  sharing  of  the  outer  electron  orbits 


I  ELECTRONIC   STRUCTURE  5 

of  the  component  atoms  such  that  not  only  is  the  compound  as  a 
whole  electrically  neutral  but  that  an  element  such  as  carbon  or 
chlorine  completes  a  stable  octet  of  electrons  in  its  outer  shell. 
Thus  the  structure  of  methane  is  suggested  by  the  formalistic, 
static  diagram  in  one  plane  shown  in  figure  1,  d.  Since  the  outer 
electron  orbits  are  considered  all-important  in  the  formation  of 
such  compounds,  all  parts  of  carbon  except  the  outer  electrons 

can  be  represented  by  C,  atomic  carbon  itself  by  -O  and  methane, 

H 
for  example,  by  H:C:H.     Likewise  hydrochloric  acid  is  repre- 

ii 

sented  by  :C1:H,  and  the  chlorine  molecule  by  :C1:C1:.     The 

hydrogen  molecule,  being  stable  with  a  pair  of  electrons  shared  by 
the  two  protons,  is  represented  by  H:H.  The  hydrogen  ion 
appears  as  a  proton  stripped  of  electrons. 

Physical  theory  demands  rotation  of  the  planet-like  electrons,  while 
chemical  theory  demands  some  sort  of  resultant  effect  which  will  account 
both  for  the  positions  of  elements  relative  to  one  another  when  in  chemical 
combination  and  for  that  curiously  vague  yet  definite  something  called 
valence.  Pending  the  results  of  attempts  to  meet  both  demands,  it  has 
become  the  custom  to  picture  the  spatial  and  valence  aspect  by  repre- 
sentations such  as  those  of  figure  1  or  their  abbreviations  given  above;  but 
it  should  be  remembered  that  the  apparently  implied  static  positions  of 
the  electrons  merely  represent  effects  which  come  within  the  range  of  ele- 
mentary chemical  demands. 

The  picture  given  above  and  in  figure  1  will  be  found  elaborated  upon  in 
Valence  by  G.  N.  Lewis,  1923.  It  is  critically  discussed  by  Andrade  (1927) 
in  whose  popular  book  The  Structure  of  the  Atom  will  be  found  references 
to  the  more  important  papers  on  the  subject.  The  chief  success  of  the 
theory  in  the  field  with  which  we  are  concerned  has  been  an  attractive, 
orderly  redescription  of  well  known  fact  with  a  few  predictions  of  minor 
importance.  The  student  should  be  very  careful  to  use  the  picture  as  a 
convenience,  subject  to  radical  change  if  required  when  the  gap  between 
the  demands  of  chemistry  and  physics  is  bridged. 

In  some  of  the  compounds  of  hydrogen  the  sharing  of  electrons 
may  be  so  complete  as  to  make  difficult  the  detachment  of  the 
hydrogen  nucleus ;  in  other  compounds  the  electron  of  the  hydro- 
gen atom  may  occasionally  be  captured  and  the  proton  be  left 
free  to  escape;  in  some  cases  the  capture  may  be  complete  and 


6  THE  DETERMINATION  OF  HYDROGEN  IONS 

decisive.  In  the  last  case  it  would  appear  that  only  the  electro- 
static attraction  of  the  oppositely  charged  parts  might  keep  the 
compound  intact  and  that  an  environment  tending  for  any 
reason  to  favor  dispersion  would  favor  complete  dissociation. 
Thus  the  dissociation  of  HC1  (fig.  1,  f)  would  furnish  H+  (fig.  1,  g) 
and  Cl~  (fig.  1,  h)  in  high  degree. 

Whether  all  or  only  a  very  few  of  the  hydrogen  nuclei  (protons) 
in  a  mass  of  a  given  compound  escape,  those  which  do  escape  act 
as  discrete  entities  contributing  their  part  to  the  osmotic  pressure  of 
a  solution  and  to  all  the  other  so-called  colligati  ve  (bound  together) 
properties  of  a  solution  such  as  the  lowering  of  the  freezing  point, 
rise  in  the  boiling  point,  etc.  These  effects  are  discussed  in  all 
texts  of  physical  chemistry  and  need  not  be  reviewed  here.  In 
aqueous  solution  the  escaped  hydrogen  nucleus  may  combine 
with  water  molecules;  but  the  charge  is  preserved.  Therefore, 
under  the  stress  of  an  electric  field,  the  particle  will  travel  toward 
the  cathode.2  Hence  it  is  called  an  ion  (traveler),  more  specifi- 
cally a  cation,  and  quite  specifically  it  is  called  the  hydrogen  ion 
or  hydrion.3 

In  cases  rarely  encountered,  for  instance  in  the  compound  LiH, 
the  hydrogen  nucleus  not  only  tends  to  hold  its  own  electron  but 
may  take  the  lithium  valence  electron  from  the  environment  of 
the  lithium  nucleus.  On  dissociation  of  this  compound  there  is 
formed  the  negative  hydrogen  ion.4  In  gaseous  form  molecules  of 
hydrogen  (H2)  may  become  charged  and  thus  become  gaseous  ions. 
Neither  of  these  two  types  is  to  be  considered.  It  will  be  under- 
stood that  the  term  hydrogen  ion  or  hydrion  as  used  in  this  text 
refers  to  the  species  H+.  When  using  this  symbol  we  ignore  the 
water  of  hydration.  (See  page  540.) 

It  is  suspected  that  the  development  of  this  subject  may  show 

2  Frequently  there  will  be  occasion  to  introduce  a  technical  term  the 
meaning  of  which  is  understood  by  the  majority  of  readers.    To  interrupt 
the  exposition  by  introducing  definitions  of  all  the  technical  terms  which 
will  be  used  would  not  be  practical.     It  might  prove  distracting  to  the 
novice  and  irritating  to  the  more  advanced  student.    As  an  imperfect 
compromise  there  are  assembled  in  appendix  N  definitions  of  the  more  im- 
portant technical  terms  used  in  this  book  and  not  defined  in  the  text. 

3  The  two  terms  will  be  used  without  discrimination  in  order  to  make  the 
reader  familiar  with  each  as  they  occur  in  current  literature. 

4  See  Klemenc  (1921)  on  negative  hydrion. 


I  IONIZATION  7 

that  such  a  readily  dissociable  compound  as  hydrogen  chloride 
has  a  structure  radically  distinct  in  type  from  that  of  so  stable  a 
compound  as  methane.  The  latter  must  suffer  drastic  treat- 
ment before  it  yields  evidence  of  dissociation.  Nevertheless  the 
tendency  of  compounds  to  throw  off  or  surrender  hydrions,  as 
measured  in  terms  presently  to  be  described,  grades  without  any 
serious  discontinuity5  from  that  high  degree  displayed  by  hydro- 
gen chloride,  through  the  comparatively  weak  yet  very  distinct 
tendencies  displayed  by  many  carboxylated  compounds  (e.g., 
acetic  acid),  on  to  the  barely  measurable  tendencies  in  certain 
alcohols.  Even  beyond  the  measurable  lie  cases  for  which  the 
presumption  of  ionizable  hydrogen  is  often  useful. 

In  dealing  with  these  matters  we  shall  find  ourselves  fully 
occupied  with  the  laws  governing  dissociation  in  mass  and  we 
shall  not  be  concerned  with  the  architecture  and  the  electronic 
structure  of  the  individual  molecule.  We  must  circumscribe  our 
subject  matter  and  we  may  begin  its  exposition  either  with  the 
acceptance  of  the  evidences  for  ionization  or  by  introducing  the 
fundamental  concepts  as  pure  postulates.  Indeed  it  is  significant 
that  many  modern  authors  go  to  no  trouble  to  justify  these  con- 
cepts before  introducing  them  in  a  manner  which  would  lead  the 
logician  to  the  conclusion  that  they  are  pure  postulates.  The 
reason  is  simple.  The  best  evidences  of  the  realities  to  be  con- 
sidered are  found  in  those  quantitative  relations  which  can  hardly 
be  appreciated  before  the  method  of  formulation  is  developed. 

Let  it  be  said  here  most  emphatically  that  our  first  formulation 
will  be  as  a  map  drawn  for  a  locality.  If  extended  far  it  will 
need  to  be  drawn  with  additional  devices  comparable  with 
Mercator's  projection  for  the  use  of  navigators.  Like  the  map 
of  a  locality,  our  map  is  good  for  restricted  conditions.  Like  the 
projection  of  Mercator,  the  corrected  map  is  good  for  distant 
voyages  even  if  it  distort  reality.  It  is  of  more  importance  to 
indicate  how  certain  experimental  devices  yield  results  which 
appear  to  be  in  substantial  agreement  locally  and  in  conflict 
extralocally.  This  is  because  these  devices  operate  in  ways  as 
distinctly  different  as  the  sextant  and  the  compass.  Surveys 

5  There  have  been  several  expressions  of  the  opinion  that  a  statistical 
study  would  show  a  more  or  less  distinct  "break"  between  the  frequencies 
of  occurrence  of  "strong"  and  "weak"  acids. 


8  THE  DETERMINATION  OF  HYDROGEN  IONS 

by  sextant  or  compass  can  be  made  from  the  same  base  line ;  and 
either  map,  without  correction  to  the  terms  of  the  other,  is  valid 
locally.  Difficulties  arise  if  the  distinctly  different  natures  of 
the  two  methods  are  not  recognized  when  the  traveler  is  on  dis- 
tant voyages,  or  in  the  presence  of  local  perturbations. 

THE    CONCEPT   OF   EQUILIBRIUM 

Reversibility 

Imagine  an  acid  of  the  type  HA  dissociating  into  the  cation 
H+  and  the  anion  A~. 

HA  ^  H+  +  A-  (1) 

Arrows  in  place  of  an  equation  sign  were  introduced  by  van't 
Hoff  to  indicate  not  only  the  ^equivalence  expressed  by  the  usual 
equation  sign  but  reversibility.  In  other  words  there  occur  among 
the  large  number  of  anions  and  cations,  present  in  any  ordinary 
aqueous  solution  of  the  acid,  recombinations  of  the  ions  the  while 
some  of  the  HA  molecules  are  dissociating. 

This  conception  of  a  "reaction"  as  labile,  continuous  and  re- 
versible is  of  profound  importance.  So  long  as  analysts  are  con- 
tent to  balance  the  two  sides  of  such  a  written  form  for  the  purpose 
of  expressing  stoichiometrical  relations  of  ordinary  analytical 
importance  the  equation  sign  suffices  and  the  implications  sym- 
bolized by  the  arrows  may  be  neglected.  But  as  a  matter  of  fact 
it  is  of  particular  importance  to  analysis  to  regard  reactions  as 
not  necessarily  going  to  completion  in  one  direction.  The  con- 
cept of  reversibility6  is  particularly  applicable  to  the  ionization  of 
acids  and  bases  and  to  many  reactions  in  which  acids  and  bases 
take  part.  So,  in  terms  of  reversible  reactions,  the  geologist 
describes  the  laying  of  the  limestone  stratum  and  the  return  of 
the  "everlasting  hills"  to  the  "eternal  drift." 

Our  modern  views  of  chemical  reversibility  supplement  the 
ancient  views  of  mechanical  reversibility  which  Mallock7  has 
paraphrased. 

6  This  is  not  to  be  confused  with  reversibility  in  a  strict  thermodynamic 
sense. 

7  Mallock,  hu$retius  on  Life  and  Death. 


I  EQUILIBRIUM 

No  single  thing  abides,  but  all  things  flow, 
Fragment  to  fragment  clings;  the  things  thus  grow 

Until  we  know  and  name  them.     By  degrees 
They  melt,  and  are  no  more  the  things  we  know. 

Nothing  abides.    Thy  seas  in  delicate  haze 
Go  off;  those  mooned  sands  forsake  their  place; 
And  where  they  are  shall  other  seas  in  turn 
Mow  with  their  scythes  of  whiteness  other  bays. 

As  if  playing  a  joke  on  Fate,  Life  seems  to  have  seized  upon 
delicate  balances  in  just  such  processes  as  determine  the  destiny 
of  mountains  and,  unlike  the  Inanimate,  has  made  these  balances 
the  internal  environment  of  its  potentially  immortal  cells. 

In  the  ceaseless  interplay  of  the  components  of  a  given,  re- 
versible reaction,  the  following  situation  may  occur.  The  reac- 
tion may  proceed  no  faster  in  one  direction  than  in  the  other.  An 
indication  of  this  state  is  the  absence  of  change  in  the  quantities 
of  the  components  of  the  system.  Statistically  the  system  is  at 
rest.  This  is  the  state  of  equilibrium. 

THE    EQUILIBRIUM   EQUATION    FOR    ACID    DISSOCIATION 

At  the  start  let  there  be  no  attempt  to  describe  all  the  factors 
which  increasingly  refined  technique  forces  into  view.  Let  there 
be  imagined  an  ideally  simple  system  in  which  each  component 
represented  in  equation  (1),  while  free,  behaves  as  if  it  were  un- 
affected by  the  presence  of  the  other  solutes.  Let  a  variation  of 
the  concentration  of  any  component  not  affect  the  imagined 
constancy  of  the  environment. 

Let  brackets  about  a  symbol  indicate  concentration  of  the 
species  which  the  symbol  represents  and  let  concentration  be  ex- 
pressed in  moles  per  liter  of  solution.  Trra»-[HA]  represents  x 
moles  of  residual  undissociated  apid,  HA,  per  liter. 

We  need  not  enquire  concerning  the  forces  or  the  circumstances 
which  occasion  the  ionization  of  the  individual,  acid  molecule. 
We  need  only  assume  that  occasionally  the  molecule  acquires  the 
ability  to  ionize  and  does  ionize.  Then,  since  enormous  numbers 
of  molecules  are  present  in  solutions  even  of  high  dilution,  we 
may  trt  u  the  subject  in  a  crude,  statistical  way  and  imagine  that 
each  m  1<>  has,  on  the  statistical  average,  the  same  span  of 


10  THE    DETERMINATION    OF    HYDROGEN    IONS 

life.  Then  the  velocity,  Vi,  with  which  the  concentration  of  HA 
is  decreasing  at  any  instant,  is  proportional  to  the  concentration 
[HA]  at  that  instant. 

Vl  =  ki[HA]  (2) 

In  (2)  ki  is  a  proportionality  factor.  Its  value,  as  we  shall  see 
presently,  need  not  be  determinable. 

The  velocity  of  the  reverse  reaction,  wherein  ions  combine  to 
reconstruct  HA,  is  likewise  dependent  on  the  concentrations 
[H+]  and  [A~]  and  in  the  following  manner. 

Suppose,  to  begin  with,  that  there  were  equal  numbers  of 
>ydrions  and  anions.  Then  imagine  that  the  number  of  hydrions 
in  a  given  volume  were  tripled.  The  number  of  collisions  be- 
tween hydrions  and  anions  would  be  tripled.  If  the  original 
number  of  hydrions  remained  and  the  number  of  anions  were 
tripled  the  number  of  collisions  would  be  tripled.  But  if  the 
hydrions  were  tripled  and  the  anions  were  tripled  simultaneously, 
the  number  of  collisions  would  be  nine  times  the  original.  Thus 
the  number  of  collisions  is  proportional  to  the  product  of  the  con- 
centrations. Combination  may  not  necessarily  be  determined  by 
collision  alone.  A  favorable  orientation  during  collision  may  be 
necessary.  A  heightened  energy  may  be  necessary.  But,  if  we 
idealize  the  situation,  we  may  suppose  that  successful  combination 
is  that  constant  fraction  of  collisions  which  is  determined  by  a 
particular  environment  and  by  the  specific  natures  of  the  ions 
concerned.  Then  in  equation  (3)  the  proportionality  factor  k2 
expresses  not  only  proportionality  of  combination  to  collisions  but 
proportionality  to  other  factors  which  are  idealized  as  constant. 

We  have  then  for  the  velocity  of  combination 

V2  =  k2  [A-]  [H+]  (3) 

Having  already  defined  the  state  of  equilibrium  as  that  at 
which  the  velocity  of  phange  in  one  direction  equals  the  velocity 
in  the  opposite  direction,  we  let  Vi  and  v2  be  those  velocities  which 
occur  at  the  attainment  of  equilibrium  and  accordingly  we  equate 
the  two.  Whence  from  (2)  and  (3)  there  is  obtained  (4). 

^  =  T  =  K»  ^ 

[HA]  k2 


DISSOCIATION   CONSTANT 


11 


e  ratio  of  two  constants  in  (4)  there  is  substituted  the 
one  constant  Ka,  which  is  properly  called  the  equilibrium  con- 
stant. It  will  be  noted  that  the  ion  concentrations  are  placed 
in  the  numerator  of  (4).  Had  they  been  placed  in  the  denomi- 
nator the  equilibrium  constant  would  be  the  reciprocal  of  Ka. 
When  the  convention  used  in  (4)  is  followed,  the  constant  (i.e., 

Ka)  is  called  the  dissociation  constant.     Its  reciprocal,  ^-,  is 

J\a 

called  the  association  constant. 

The  dissociation  constant  is  sometimes  described  as  a  measure 
of  the  "strength"  of  an  acid.  Thus  the  following  comparison 
may  be  made. 


CLASS 

COMPOUND 

I\2  (APPROXIMATE) 

Strong  acid  

HC1 

About  10+7 

Moderately  strong  acid    

Dichlor  acetic  acid 

About  5.  X  10~2 

Weak  acid 

Acetic  acid 

1  8  X  10~B 

Very  weak  acid  

Phenol 

1.0  X  10-10 

Extremely  weak  acid 

Glucose 

4      X  10  ~13 

Vanishingly  weak  acid  

Methane 

Approaches  0 

For  tables  of  dissociation  constants  see  appendix  tables  G,  H, 
I,  and  J. 

To  indicate  that  a  dissociation  constant,  as  used  in  these  ap- 
proximate equations,  applies  to  a  limited  set  of  conditions,  it  is 
frequently  written  K'.  K  is  then  reserved  for  the  "true"  disso- 
ciation constant,  which  can  be  estimated  by  the  method  of 
Chapter  XXV. 

It  is  readily  perceived  that,  when  actual  numerical  values  are 
given  to  the  concentrations  of  the  several  "species"  occurring  in 
the  equilibrium  equation,  care  must  be  taken  to  use  a  consistent 
unit  of  concentration.  If  grams  per  liter  in  one  case,  moles  per 
liter  of  solution  in  another,  moles  per  1000  grams  of  solvent  in 
another  and  millimoles  per  liter  of  solution  in  another  case  were 
used,  the  equilibrium  constants,  while  well  defined  in  each  case 
separately,  would  not  be  comparable. 

Of  course,  if  there  be  reason  to  believe  that  an  acid  like  HC1,  or  a  salt 
like  NaCl,  is  ionize  '  )st  completely  in  dilute  solutions,  there  is  little 
point  in  attempts  to  apply  to  experiment  the  treatment  which  follows  the 


12  THE    DETERMINATION    OF   HYDROGEN   IONS 

derivation  given.  As  noted  later,  the  application  of  the  type  equilibrium 
equation  to  a  case  like 

[Na+]  [C1-]  [H+]  [C1-] 

INaClJ  [HC1]  Ka 

has  no  practical  value.  In  the  first  place,  if  the  quantity  in  the  denomi- 
nator of  the  type  equation  should  approach  an  infinitesimal,  the  most  ex- 
treme accuracy  would  be  required  to  satisfy  the  equation  experimentally. 
Furthermore  the  simple  equation  is  founded  upon  an  idealization,  and 
in  the  case  specified  the  utmost  accuracy  would  be  required  to  detect  and 
to  measure  the  several  factors  which  might  interfere  with  the  applicability 
of  the  ideal  equation.  But,  in  the  second  place,  the  introduction  of  a 
concentration  of  a  molecule  like  NaCl  or  HC1  would  be  to  confess  one's 
ignorance  of  the  fact  that  the  evidence  is  against  the  existence  of  the 
molecule  NaCl  and  (for  aqueous  solutions)  against  the  existence  of  the 
molecule  HC1.  (See  page  58.)  A  dilute  solution  of  hydrochloric  acid 
may  be  regarded  as  one  extreme.  A  solution  of  methane  is  a  case  at  the 
other  extreme.  In  the  first  case  Ka  approaches  infinity;  in  the  second 
Ka  approaches  zero.  In  either  circumstance  the  type  equation  has  little 
practical  value. 

APPLICATION   TO   A   SIMPLE   ACID   SOLUTION 

Since  the  concentrations  of  the  various  "species"  are  treated 
like  the  x,  y,  z  of  any  ordinary  algebraic  equation,  it  may  be 
interesting  to  note  at  this  point  a  special  application  of  equation 
(4)  which  will  involve  some  simple  algebra. 

Consider  a  solution  containing  the  acid  as  the  only  solute  and 
neglect  the  ions  which  may  come  from  water.  The  simple  acid 
HA  partially  dissociates  into  equal  parts  of  H+  and  A~.  Hence 

[H+]  =  [A-] 

Let  the  concentration  of  total  acid  [S]  be  defined  by 
[S]  =  [HA]  +  [A-], 

i.e.,  the  sum  of  the  concentrations  of  undissociated  and  dissociated 
acid.  Equation  (4)  may  now  be  written  as  follows 

fTTJIO 

=  K.  (5) 


[S]  -  [H+] 

Equation  (5)  may  be  solved  for  [H+]  by  the  usual  process  of 
"completing  a  square."     There  is  thus  obtained 


(6) 


I  EQUILIBRIA   IN   MIXTURES  13 

When  Ka  is  small  in  relation  to  [S] 

[H+]  ^  -\/Ka  [S]  (7) 

Example:  Given  Ka  =  1  X  10~5;  calculate  [H+]  when  [S]  =  0.1 
molar. 


(H}  (10-0 
Approximately: 


[H+]  =  V  10-6  =  10-3  =  0.001  normal 

Application  of  (6)  to  the  case  of  the  acid  having  the  value  10~5 
for  Ka  will  show  that  the  approximation  of  (7)  introduces  a  sig- 
nificant error  when  [S]  is  less  than  0.001  normal.  For  dilute 
solutions  and  for  solutions  of  very  weak  acids,  account  must  be 
taken  of  the  hydrions  coming  from  the  water  as  will  appear 
presently. 

GENERAL  EXTENSION  OF  THE  EQUILIBRIUM  EQUATION  TO  MIXTURES 

When  an  anion  originates  by  the  dissociation  of  the  acid  HA 
or  by  the  dissociation  of  some  admixed  salt,  such  as  NaA,  it  may 
combine  with  any  hydrion  irrespective  of  the  source  of  this 
hydrion.  Therefore  equation  (4)  holds  even  in  mixtures, — with 
the  qualification  that  the  actual  value  of  Ka  may  vary  some- 
what even  in  solutions  of  the  same  solvent  and  of  the  same  tem- 
perature, if  the  components  of  the  system  vary  sufficiently  in 
concentration  to  alter  appreciably  the  environment.  This,  in 
our  idealization,  we  demanded  should  be  constant. 

To  embrace  the  situation  to  be  considered  when  salts  of  the 
acid  are  present,  let  [S],  the  concentration  of  total  material  con- 
taining the  acid's  main  group  in  the  form  of  ions  or  ionogens,  be 
defined  by 

[S]  =  [A-]  +  [HA]  +  [«]  (8) 

Here  [s]  represents  the  sum  of  the  concentrations  of  all  those 
salts  of  the  acid  which  are  in  an  undissociated  state. 


14          THE  DETERMINATION  OF  HYDROGEN  IONS 

Equations  (4)  and  (8)  yield  (9)8 


[S]       Ka  +  [H+]  IB] 

It  can  be  said  at  once  that  if  (9)  be  applied  to  experimental  data 
it  will  appear  as  if  [s]  should  be  considered  a  variable  of  significant 
magnitude.  On  the  other  hand  there  are  frequently  good  reasons 
for  believing  a  salt  to  be  practically  completely  ionized  and  in 
these  cases  it  is  permissible  to  let  [s]  =  0.  Indeed,  effects  which 
might  be  attributable  to  the  formation  of  undissociated  salt 
molecules  are  now  attributed  to  the  attraction  between  its  charged 
ions  and  are  dealt  with  by  the  special  methods  of  Chapter  XXV. 

It  should  not  be  assumed  that  there  are  no  cases  in  which  there 
is  undissociated  salt.  However,  we  shall  continue  as  if  for  cases 
in  which  it  can  be  assumed  that  the  concentration  of  undisso- 
ciated salt  is  so  small  as  to  be  negligible.  Then  [s]  in  equation 
(9)  is  considered  zero  and  (9)  reduces  to  (10) 


[S]       K.  +  [H+] 

[A~1 

In  either  case  the  ratio  -7^7-  is  called  the  fraction  of  dissociation 

LbJ 

or  degree  of  dissociation.     This  refers  not  to  the  acid  alone  but 
to  all  the  ionogens  capable  of  supplying  to  the  solution  the  specific 
ion  A~~.     This  ratio  is  so  frequently  used  that  it  is  a  convenience 
to  give  it  the  symbol  a.     Percentage  dissociation  =  lOOa. 
Then  (10)  is  written: 

-irniFi  (10a) 

Equation  (lOa)  emphasizes,  in  a  very  direct  way,  the  fact  that 
changes  in  the  hydrion  concentration  of  a  solution  indicate  altera- 
tion of  a,  the  degree  of  dissociation,  —  that  is,  the  degree  to  which 
the  specific  acid  under  consideration  is  present  in  the  dissociated 
state.  This  is  the  key  equation  unlocking  the  door  to  most  of 
the  reasons  for  interest  in  methods  of  determining  hydrion  con- 
centrations. For,  since  [H+]  indicates  or  in  a  specific  case,  [H+] 

8  Since  the  term  (1  —  ~)  in  (9)  is  to  be  eliminated  the  student  is  advised 

[SJ 
to  develop  the  simpler  equation  (10)  by  neglecting  [s]  in  equation  (8). 


I  LOGARITHMIC    EQUATION  15 

indicates  the  degree  to  which  properties  associated  with  the  anion 
or  properties  associated  with  the  undissociated  residue  will  be 
manifest  in  mass. 

This  simple  equation  sums  up  the  main  feature  of  most  that 
follows.  However,  it  is  more  convenient  in  logarithmic  form. 

LOGARITHMIC    FORMS   OF   THE   FUNDAMENTAL   EQUATIONS 

Because  the  values  of  [H+]  may  vary  so  greatly  that  charting 
on  a  linear  scale  is  impracticable  and  because  of  other  better 
reasons,  it  is  both  convenient  and  logical  to  use  a  logarithmic 

function  of  [H+].     That  chosen  is  logio  yg^j.     To  this  is  given 

the  symbol  pH  (see  page  36). 

For  the  sake  of  simplicity  continue  with  the  assumption  that 
M  in  equation  (9)  is  so  small  that  it  may  be  considered  zero. 
Equation  (lOa)  is  then  applicable  and  may  be  transformed  to  (11) 

[H+]-K.^^  (11) 

a 

Taking  the  logarithm  of  the  reciprocal  of  each  side  of  (11)  we 
have  (12)  which  is  merely  another  form  of  the  key  equation 
(lOa)  and  is  the  most  generally  useful  of  all  the  equations  with 
which  we  shall  deal.  The  greater  part  of  the  subject  can  be 
developed  with  the  aid  of  this  equation. 


Analogous  to  the  expression  pH  =  log  j^j-p:  is  the  expression 
pKa  =  log  —  •    Since  the  current  literature  cannot  be  under- 

Ka 

stood  without  an  appreciation  of  the  meaning  of  pKa9  we  shall 
not  hesitate  to  adopt  this  symbol.     Then  (12)  may  be  written: 

pH  =  PKa  +  log  ~-  (12a)10 

1  —  a 

9  Bjerrum  (1923)  calls  pKa  the  dissociation  exponent. 

10  This  is  the  most  important  equation  of  the  book.     The  student  is 
advised  to  calculate  pH  with  any  given  value  of  pKa  and  values  of   a 
ranging  from  0.1  to  0.9  at  intervals  of  0.1,  and  to  chart  the  results  as  in 
figure  2. 


16 


THE   DETERMINATION   OF   HYDROGEN   IONS 


It  will  be  remembered  that  a  is  the  degree  of  dissociation.  If 
we  can  assume  that  a  mixture  of  equivalents  of  acid  and  base 
forms  a  salt  which  dissociates  completely,  a  should  be  1  for  such 
a  mixture.  If  the  acid  is  so  very  weak  that  its  dissociation  is 
negligible  compared  with  that  of  the  salt,  we  can  assume  (as  an 
approximation)  that  a  is  approximately  the  same  as  the  corre- 
sponding degree  of  "neutralization"11  i.e.,  salt  formation.  In 


1 

2 
3 
4 
5 
6 
7 
8 
9 

to 

11 

12 
pH 
13 

14 

\ 

\ 

1 

14 

13 
12 
11 
10 
9 
6 
7 
6 
5 

^ 

x. 

7 

\ 

^ 

^ 

V 

2 

^^ 

\ 

^^ 

1 

\ 

A 

^ 

B 

y_ 

X 

\ 

^ 

^f 

^^^ 

\ 

>? 

N 

Y 

\ 

\ 

\ 

i 

^ 

N, 

2 

\ 

^ 

^ 

^ 

3 
'pOH 

1 

0 

\ 

Y 

\ 

\ 

\ 

\ 

0.2       0.4       0.6       0.6       1.0       0.2       0.4  .    0.6       QA       1.0 
a.  Acid  dissociation        o.o  a.  Base  dissociation 

FIG.  2.  (A)  RELATION  BETWEEN  pH  AND  THE  DEGREE,  a,  OF  THE 

DISSOCIATION  OF  ACIDS;  (B)  RELATION  BETWEEN  pH  AND  THE 

DEGREE,  a,  OF  THE  DISSOCIATION  OF  BASES 

other  words  the  curve  relating  a  to  pH  may,  under  the  specified 
conditions,  be  closely  comparable  with  the  curve  relating  degree 
of  neutralization  to  pH.  Equation  (12a)  may  then  be  written 
in  approximate  form  as: 

*H--*+i*S        (i2b) 

This  equation  will  be  derived  again  later. 

11  "Neutralization"  is  here  used  in  the  loose  sense  that  each  equivalent 
of  base  destroys  the  acidic  nature  of  one  equivalent  of  acid. 


I  BASES  17 

The  geometry  corresponding  to  equation  (12)  or  (12a)  is 
shown  by  figure  2  A.  All  the  curves  are  identical  in  form.  The 
position  of  any  one  is  det ermine (Tby  the  value  o£j)Ka,  for,  since 
[H+]  =  Ka  when  a  =  0.5,  the  midpoint  of  the  curve  is  deter- 
mined by  pKa. 

BASES 

Before  dwelling  more  at  length  upon  equation  (12)  and  upon 
the  corresponding  geometry,  there  will  be  considered  the  funda- 
mental equation  for  the  equilibrium  state  in  the  dissociation  of  a 
base. 

It  has  been  customary  to  regard  oxides  such  as  K20,  which  on 
solution  in  water  give  tests  for  alkalinity,  as  if  they  became 
hydrated  to  compounds  of  the  type  BOH  (e.g.,  K2O  +  H20-» 
2KOH).  The  alkalinity  of  the  solution  is  then  assumed  to  be 
due  to  the  ionization  of  BOH  to  furnish  some  definite  concentra- 
tion of  the  hydroxyl  ion,  OH~. 

For  the  reversible  reaction : 

BOH  ^±  B+  +  OH- 

there  may  be  written  the  equilibrium  equation: 
[B+]  [OH- 


[BOH] 


=  Kb  (13) 


Equation  (13)  is  to  be  regarded  as  the  type  equation.  It  is  not 
applied  in  practice  to  a  base  such  as  KOH  which  is  practically 
completely  dissociated  in  dilute  solution.  Such  a  case  is  best 
treated  in  another  manner.  (Compare  page  12.) 

Applying  to   (13)  the  same  sort  of  mathematical  treatment 
accorded  (4)  we  reach  in  turn  (14),  (15),  and  (15a). 


pOH  =  pKb  +  log  ~—  (15a) 

1  —  a. 


18  THE    DETERMINATION    OF   HYDROGEN    IONS 

In  the  latter  cases  pOH  symbolizes  log  rrvc,  ,  and  pKb    = 

[(Jti.  \ 

log  ib 

The  geometry  of  (15a)  is  illustrated  by  the  curves  of  figure  2  B. 
Again  this  equation  gives  a  family  of  curves.  Any  one  curve  is 
fixed  in  its  position  by  the  value  of  pKb. 

For  a  reason  presently  to  become  clear,  values  of  pOH  in 
figure  2  B  are  plotted  in  a  direction  opposite  to  the  direction  of 
increasing  values  of  pH. 

THE   WATER    EQUILIBRIUM 

Up  to  this  point  no  relation  has  been  shown  between  the  acid 
systems  and  the  base  systems  nor  between  pH  and  pOH.  If  we 
confine  our  attention  to  aqueous  solutions  we  may  now  introduce 
the  fact  that  water  yields  both  hydrions  and  hydroxyl  ions  in 
accordance  with 

HOH  ^±  H+  +  OH- 

For  the  equilibrium  state  of  this  reaction  write : 

[H+]  [OH-] 
[HOH] 

Anticipating  a  conclusion  to  be  mentioned  in  Chapter  II,  we 
may  state  that  water  is  so  little  dissociated  that  no  serious  error 
will  be  made  in  regarding  the  concentration  of  the  undissociated 
residue,  [HOH],  to  be  equal  to  that  of  the  total  water.  Further- 
more this  may  be  considered  constant  for  limited  ranges  of  dilute 
solutions.  Hence: 

[H+]  [OH-]  =  Kw  (16) 

Properly  Kw  is  an  ionic  product,  but  it  is  commonly  called 
the  dissociation  constant  of  water.  Like  all  the  other  so-called 
equilibrium  constants,  it  is  only  a  constant  by  grace  of  the  main- 
tenance of  a  constant  environment.  Its  value  is  subject  to 
change  with  change  of  temperature,  salt  concentration,  etc.  For 
descriptive  purposes  Kw  may  be  considered  to  have  the  rounded 
value  10~14. 


I  WATER    EQUILIBRIUM  19 

From  (16)  there  is  readily  derived  the  following; 


pH  +  pOH  =  pKw  (17) 

and,  since  the  value  of  Kw  may  be  rounded  off  to  10~14, 

pH  +  pOH  =  14  (17a) 

It  is  this  relation  which  was  used  in  aligning  the  pH  and  pOH 
values  of  figure  2. 

MORE    DETAILED    EQUATIONS 

It  is  unnecessary  for  purposes  of  general  treatment  to  develop 
separate  equations  for  acid  systems  and  for  base  systems.  This 
will  be  shown  in  Chapter  II.  Therefore,  we  shall  confine  atten- 
tion to  the  equations  for  acid  systems  in  a  discussion  of  more 
detailed  equations. 

In  considering  the  following  treatment  the  student  is  advised 
to  pay  little  attention  to  the  mathematical  derivations  of  equa- 
tion (19)  or  (20).  They  are  stated  in  their  elaborate  form  for 
convenience  of  discussion.  In  this  discussion  there  will  be  shown, 
by  one  numerical  example,  conditions  under  which  certain  of 
the  quantities  as  they  occur  in  the  equation  can  be  neglected. 
This  will  aid  in  the  justification  of  the  useful  approximation  to 
follow  in  the  next  section. 

In  the  derivation  of  equation  (12)  there  were  introduced  —  in 
addition  to  the  idealistic  assumptions  at  the  very  origin  —  two 
approximations.  One,  the  neglect  of  the  undissociated  salt  [s], 
we  have  already  mentioned.  The  other  was  the  neglect  of  the 
hydrions  and  hydroxyl  ions  coming  from  the  solvent,  water. 

In  addition  to  the  familiar  equation 


_ 


[HA] 

and  the  summation  (8)  which  is 

[S]  =  [A-]>[[HA]  +  [«] 


20  THE    DETERMINATION    OF    HYDROGEN    IONS 

it  now  becomes  itecessary  to  employ  equation  (18)  which  will 
automatically  take  account  of  the  hydroxyl  and  hydrions  arising 
from  the  water. 

[H+]  +  [B+]  =  [A-]  +  [OH-]  (18) 

This  new  equation  expresses  the  electro-neutrality  of  the  solution 
as  a  whole,  it  being  required  that  the  total  number  of  positive 
charges  of  whatever  source  (ions  from  water  included)  must  equal 
the  total  number  of  negative  charges.  [B+]  is  the  concentration 
of  the  cation  of  the  salt,  for  example  [K+]  in  a  solution  of  potas- 
sium acetate.  [OH~]  can  be  eliminated  from  expressed  inclusion 
in  the  equations  by  using  the  equation  for  the  water  equilibrium, 

[H+]  [OH-]  =  Kw    or    [OH-] 


[H+] 

These  equations  can  be  combined  to  yield  (19)  which,  in  loga- 
rithmic form,  is  (20) 


Ka    =    -  ~~  (19) 

[S]  -  [B+]  -  [H+]  +  ^  -  W 


[S]  -  [B+]  -  [H+]  +  -=-  _  [8] 

pKa  =  pH  +  log  -  (20) 

DH  +  [H+]  - 


Let  equation  (20)  now  be  applied  in  a  specific  case  in  order  that 
the  relative  importance  of  each  term  may  be  shown  numerically. 
We  shall  use  the  data  of  Walpole  (1914)  for  mixtures  of  acetic 
acid  and  sodium  acetate.  The  compositions  of  the  solutions  and 
the  measured  values  of  pH  which  Walpole  gives  are  found  in 
table  1.  Lest  false  interpretations  of  the  treatment  be  made,  it 
should  be  emphatically  stated  that  the  values  called  pH  are 

not  strictly  those  of  log  -  .     Partly  for  this  reason  and  partly 

[H+] 

for  the  reason  described  in  Chapter  XI  the  constants  as  calcu- 
lated should  not  be  expected  to  be  exactly  the  same  for  all  ratios 


ACETATE    SYSTEM 


21 


of  acetate  to  acetic  acid.  In  Chapter  XXV  corrections  will  be 
discussed.  With  this  caution  we  may  proceed  as  if  the  cited 
values  truly  represent  hydrion  concentrations. 

Again  we-  shall  proceed  with  the  assumption  that  the  con- 
centration of  undissociated  salt,  [s],  in  this  instance  [sodium 
acetate],  is  negligible.  This  at  once  simplifies  the  treatment,  be- 
cause it  not  only  eliminates  this  specific  term  but  it  also  makes  it 

TABLE  i 

Calculation  of  pKafrom  Walpole's  data  for  mixtures  of  acetic  acid 
and  sodium  acetate 


(1) 

NaAc 

MOLAR 

(2) 
HAc 

MOLAR 

(3) 
pH 

(4) 
[H+] 

(5) 
[B+]  +  [H+] 
X 

(6) 

'^T'- 

Y 

(7) 
X 

LOGY 

(8) 
PKa 

(9) 
pKa 

BY  AP- 
PROXI- 
MATION 

0.000 

0.200 

2.696 

0.00201 

0.00201 

0.198 

-1.994 

4.690 

CD 

0.005 

0.195 

3.147 

0.00071 

0.00571 

0.1943 

-1.532 

4.679 

4.739 

0.01 

0.19 

3.416 

0.00038 

0.01038 

0.1896 

-1.262 

4.678 

4.695 

0.02 

0.18 

3.723 

0.00019 

,0.02019 

0.1798 

-0.950 

4.673 

4.677 

0.04 

0.16 

4.047 

0.00009 

0.04009 

0.1599 

-0.601 

4.648 

4.649 

0.06 

0.14 

4.270 

0.00005 

0.06005 

0.1399 

-0.367 

4.637 

4.638 

0.08 

0.12 

4.454 

0.00004 

0.08004 

0.12 

-0.176 

4.630 

4.630 

0.10 

0.10 

4.626 

0.00002 

0.10002 

0.10 

0.000 

4.626 

4.626 

0.12 

0.08 

4.802 

0.000016 

0.12 

0.08 

0.176 

4.626 

4.626 

0.14 

0.06 

4.990 

etc. 

0.14 

0.06 

0.368 

4.622 

4.622 

0.16 

0.04 

5.227 

0.16 

0.04 

0.602- 

4.625 

4.625 

0.18 

0.02 

5.574 

0.18 

0.02 

0.954 

4.620 

4.620 

0.1925 

0.0075 

6.024 

0.1925 

0.0075 

1.409 

4.615 

4.615 

0.1975 

0.0025 

6.518 

0.1975 

0.0025 

1.898 

4.620 

4.620 

possible  to  consider  [B+]  equal  to  the  concentration  of  total 
sodium  acetate.12  Therefore  the  values  of  [B+]  -f-  [H+],  found  in 
column  5  of  table  1,  are  readily  calculated  from  the  experimentally 
determined  values  of  [H+],  column  4,  and  the  values  for  total 
sodium  acetate,  column  1. 

The  reader  may  readily  calculate,  by  using  the  value  10~14 

T£" 

for  Kw,  that  the  values  of  TTpr  are  so  small  as  to  be  negligible  in 


12  No  undissociated  base,  NaOH,  is  supposed  to  remain. 


22          THE  DETERMINATION  OF  HYDROGEN  IONS 

the  sum  in  equation  (20).     Equation  (20)  now  reduces  prac- 
tically to  (21) 

~  ,,      [S]  -  [B+]  -  [H+]  (    . 


With  this  there  are  made  the  remaining  calculations,  which  are 
summarized  in  table  1  and  which  lead  to  the  values  of  pKa 
found  in  column  8. 

There  are  cases  in  which  values  for  rTT ,,  are  significant  while 

[H+J 

those  for  [H+]  are  insignificant  (alkaline  solutions).  In  rare  cases 
both  terms  have  to  be  considered.  The  latter  occur  when  the 
measurements  are  near  "neutrality." 

It  will  be  noted  in  table  1  that  values  for  [H+]  in  the  lower  part 
of  the  table  affect  the  magnitude  of  the  sum  [B+]  +  [H+]  so  little 
that  the  effect  is  there  negligible.  We  can  readily  imagine  two 
cases  in  which  this  neglect  would  be  serious.  One  case  would 
be  that  of  a  stronger  acid  maintaining,  during  the  course  of  its 
treatment  with  a  base,  values  of  [H+]  large  in  relation  to  [B+]. 
Another  case  would  be  a  solution  so  extremely  dilute  that  [B+] 
would  approach  the  magnitude  of  [H+]. 

A   USEFUL   APPROXIMATION 

If  we  confine  attention  to  the  cases  like  that  illustrated  in 
table  1  we  may,  for  purposes  of  approximation,  neglect  [H+]  as 
it  occurs  in  the  sum  [B+]  +  [H+].  Then  equation  (21)  is  further 
simplified  to  equation  (22). 

pKa  =  pH  +  log  [S]  "^  (22) 

which  may  be  rewritten 

pH  =  pKa  +  log       _  (22a) 

This  is  virtually  , 

pH  =  PV+log  — ^L  (23) 

[residual  acidj 

This  is  frequently  called  the  Henderson-Hasselbalch  equation. 
Compare  (23)  with  (J2b)  on  page  16  and  see  column  9,  table  1. 


I  a-CURVES   AND   TITRATION   CURVES  23 

We  might  return  to  the  complete  equation  (20)  and  discuss  in 
the  general  language  of  algebra  the  effects  to  be  expected  if 
probable  values  for  the  concentration  of  possibly  undissociated 
salt  [s]  were  introduced.  The  danger  of  this  is  two-fold.  We 
would  be  discussing  quantities  which  are  experimentally  evaluated 
with  such  difficulty  and  uncertainty  that  we  would  find  the 
mere  algebraic  discussion  rather  academic.  In  the  second  place 
we  might  be  led  to  emphasize  a  method  of  treating  salts  which  is 
less  profitable  than  that  which  will  be  discussed  in  later  chapters. 

DISTINCTION   BETWEEN  ^-CURVES   AND   TITRATION   CURVES 

Equation  (12a)  is 

a 


PH  =  pKa  +  log 


1  -  a 


The  "approximate  equation"  developed  in  a  preceding  sec- 
tion is 


It  has  been  shown  in  the  case  of  acetic  acid  that,  for  a  given 
set  of  conditions,  there  is  a  fair  degree  of  agreement  in  the  applica- 
tion of  these  two  equations.  However,  if  a  be  considered  zero 
before  any  alkali  has  been  added  to  an  acetic  acid  solution  in 
the  course  of  its  titration,  it  is  obvious  that  the  dissociation  of 
the  acetic  acid  is  being  neglected.  No  correspondence  between 
the  atrcurve  and  the  actual  titration  curve  should  be  expected 
near  the  beginning  of  the  titration. 

This  lack  of  correspondence  becomes  more  and  more  emphasized 
as  the  "strength"  of  the  acid  being  titrated  increases.  The  case 
of  hydrochloric  acid  is  the  extreme.  In  this  case  it  is  advisable 
to  regard  the  acid  as  practically  completely  dissociated  in  dilute 
solution,  and  to  be  gradually  eliminated  as  acid  during  the 
course  of  the  titration. 

This  matter  could  be  gone  over  again  in  detail  with  the  aid  of 
the  equations  discussed  in  previous  sections.  However,  the 
student  will  probably  find  it  more  profitable  at  this  point  to 
compare  the  a-curves  of  figure  2  and  figure  11  (page  47)  with  the 
titration  curves  of  figure  92  (page  531). 


24 


THE  DETERMINATION  OF  HYDROGEN  IONS 


AN   EXAMPLE    OF   DILUTION 

There  may  now  be  considered  another  aspect  of  the  acetic  acid- 
sodium  acetate  mixtures.  In  table  2  are  tabulated  Walpole's 
data  for  various  dilutions  of  a  solution  equimolecular  with  respect 
to  both  the  sodium  acetate  and  the  acetic  acid  used  in  construct- 
ing the  mixtures. 

By  the  approximation  formula  (23)  an  observed  value  of  pH 


should  equal  pKa,  since  the  ratio 


[salt] 
—  rr: 


. 

is  fixed  and  is  equal  to  1. 


In  the  calculations  of  pKa  shown  in  the  table  there  has  been 
used  the  more  nearly  complete  formula  (21).     Its  use  in  place  of 

TABLE  2 

The  apparent  change  of  pKa  with  dilution  of  a  solution  equimolecular1  with 

respect  to  both  acetic  acid  and  sodium  acetate 

(Data  from  Walpole  (1914)) 


TOTAL, 
ACETATE 

NaAc 

HAc 

pH 

[H+] 

xio* 

[B+]  +  [H+] 
X10* 

Y 

[S]  -  [B+]  - 
[H+] 
X  105 

X 

LOG  Y 

pKa 

0.4 

0.2 

0.2 

4.606 

2.48 

20,000+ 

20,000- 

0.000+ 

4.606 

0.2 

0.1 

0.1 

4.623 

2.38 

10,000+ 

10,000- 

0.000+ 

4.623 

0.08 

0.04 

0.04 

4.646 

2.26 

4002.0 

3998.0 

0.000+ 

4.646 

0.04 

0.02 

0.02 

4.663 

2.17 

2002.0 

1998.0 

0.001 

4.662 

0.032 

0.016 

0.016 

4.673 

2.12 

1602.0 

1598.0 

0.001 

4.672 

0.02 

0.010 

0.010 

4.684 

2.07 

1002.1 

997.9 

0.001 

4.683 

0.01 

0.005 

0.005 

4.706 

1.97 

502.0 

498.0 

0.003 

4.703 

0.004 

0.002 

0.002 

4.737 

1.83 

201.8 

198.2 

0.008 

4.729 

0.002 

0.001 

0.001 

4.758 

1.75 

101.75 

98.25 

0.015 

4.743 

the  first  approximation  (equation  (23))  is  not  significant  in  this 
instance,  except  for  the  higher  dilutions.  Even  then  its  use  pro- 
duces little  improvement  in  the  constancy  of  the  "constant"  pKa. 
In  general  it  is  well,  when  dealing  with  highly  dilute  solutions,  and 
especially  with  acids  of  low  pKa  values,  to  consider  the  more 
complete  formula.  However,  there  remains  a  strong  suggestion 
that  account  should  be  taken  of  the  undissociated  salt.  We  shall 
see  in  Chapter  XXV  that  this  question  is  now  being  dealt  with 
by  unique  methods  and  that,  starting  with  the  postulate  of 
practically  complete  dissociation  of  salts,  the  effect  we  now  have 


DILUTION 


25 


in  mind  is  accounted  for  by  interionic  forces.  This  is  sometimes 
described  as  a  force  which  produces  an  ionic  clustering.  These 
only  remotely  resemble  true  salt  molecules.  Therefore,  we  had 
best  not  try  to  get  the  complete  answer  to  our  problem  from  the 
elaboration  of  an  equation  which  was  established  in  the  first  in- 
stance on  simplifying  assumptions  and  in  ignorance  of  the  de- 
tailed nature  of  specific  solutions. 


PH 


cc 


8        10 


FIG.  3.  TEN  CUBIC  CENTIMETERS  0.2  N  ACETIC  ACID  TITRATED  WITH 

0.2  N  NaOH 

Experimental  data  shown  by  centers  of  circles  (hydrogen  electrode). 
Type  curve  is  shown  centered  at  pH  =  4.73  the  ideal  position  as  corrected 
for  solutions  of  zero  ionic  strength.  See  page  507. 

Equation  (23)  may  be  considered  a  first  approximation  useful 
for  the  treatment  of  weak  acids.  Equation  (21)  may  be  con- 
sidered a  first  approximation  useful  when  [H+]  becomes  of  appre- 
ciable magnitude  relative  to  [S]  and  [B+]. 

Figure  3  shows  the  experimental  data  for  0.2  N  acetate  mix- 
tures and  also,  in  a  displaced  position,  the  type  curve  drawn  with 
the  aid  of  equation  (21).  The  placement  of  this  type  curve  was 
made  with  a  value  of  pKa  taken  from  conductivity  data  for 


26          THE  DETERMINATION  OF  HYDROGEN  IONS 

the  dissociation  constant  of  acetic  acid.  As  indicated  in  table  2, 
the  value  of  pKa,  varies  with  the  dilution.  We  shall  also  see  that 
it  varies  with  the  salt  content  and  with  the  standard  of  reference 
chosen.  However,  the  general  form  of  the  curve  and  its  ap- 
proximate position  are  now  our  chief  interests. 

ACIDS  WITH  MORE  THAN  ONE  REPLACEABLE  HYDROGEN 

Since  it  is  not  within  the  province  of  this  book  to  outline  all 
types  of  acid-base  equilibria  which  are  met  in  the  application  of 
methods  for  determining  hydrion  concentrations,  the  main  princi- 
ples have  been  illustrated  by  considerations  of  simple  acids  and 
.bases.  The  outline  is  easily  extended  to  acids  with  more  than 
one  replaceable  hydrogen  and  also  to  those  compounds  which 
contain  both  acidic  and  basic  groups  and  which  are  called  "ampho- 
teric  ionogens"  or  more  usually  "amphoteric  electrolytes'7  or 
"ampholytes."  The  extension  will  be  illustrated  graphically  ;  but, 
to  indicate  the  manner  in  which  equations  corresponding  to  the 
geometry  are  handled,  one  simple  example  will  be  given. 

Assume  an  acid  of  type  HAH  dissociating  stepwise  to  HA~ 
and  A. 

HAH  ^  HA  +  H+ 
HA  ^  A  +  H+ 

The  equilibrium  equations  are  : 


First  step  =  Kl  (24) 

Second  step  ^  =  K2  (25) 

LrlAJ 

If  secondary  considerations  discussed  during  the  treatment  of  the 
simple  systems  are  neglected,  there  is  need  to  employ  only  one 
additional  fundamental  equation,  namely  that  giving  the  sum 
[S]  of  the  concentrations  of  all  species. 

[S]  =  [HAH]  +  [HA]  +  [A]  (26) 


I  MULTIVALENT   ACIDS  27 

By  defining  the  degree  of  the  first  step  of  ionization  by 

^itF = ai  (27) 

and  the  degree  of  the  second  step  by 

[A--; 


[8]        *  (28) 


there  are  derived  from  the  above  the  following : 

K!  [H+] 


Oil 


iK,  +  K!  [H+]  +  [H+p 


(29) 


i2 .     . 

"  K.K2  +  Ki  [H+]  +  [H+P 


The  degree  of  total  ionization,  at,  is  evidently 

Cti   +   0(2 


Inspection  of  equations  (29)  and  (30)  shows  that,  since  their 
denominators  are  the  same,  the  relative  values  of  Ki[H+]  and  of 
KiK2  determine  whether,  at  a  given  value  of  [H+],  oti  or  1  +  az  shall 
be  the  targer  proportion  of  at. 

The  effects  of  varying  the  difference  between  KI  and  K2  can 
be  shown  best  indirectly  by  resorting  again  to  logarithmic  rela- 
tions expressed  graphically.  However,  actual  calculations  are 
performed  most  easily  with  the  equations  given  above.  In  figures 
4  to  6  are  charted  the  curves  for  three,  multivalent  acids.  Differ- 
ences between  the  pKa  values  are  such  as  to  show  in  figure  4  no 
serious  deviations  from  the  picture  which  three  independent  acids 
would  give.  In  figures  5  and  6  are  indicated  "overlappings"  to 
different  degrees. 

AMPHOLYTES 

For  amphoteric  electrolytes  (i.e.,  electrolytes  containing  acidic 
and  basic  groups)  a  relation  of  great  importance  may  be  illus- 


28 


THE    DETERMINATION    OF   HYDROGEN    IONS 


KH2P 


to 


KJHP 


C.C. 


100 


ISO 


FIG.  4.  TITKATION  CURVE  OF  PHOSPHORIC  ACID 

Fifty  cubic  centimeters  of  M/10  H3PO4  titrated  with  N/10  KOH.     Shows 
step-wise  "neutralization"  of  three  hydrogens. 


PH 


C.C. 


10 


FlG.    5.    TlTRATION   OF  THE  "DlBASIC"    AdD,    PffTHALIC  AdD,    WITH  KOH 

Shows  step-wise  neutralization  but  "overlapping"  of  titration  curves 


AMPHOLYTES 


29 


strated  by  the  conduct  of  the  simple  ampholyte,  p-amino  benzole 
acid.  The  acid  dissociation  constant  Ka  is  6.8  X  10~6  and  the 
basic  dissociation  constant  Kb  is  2.3  X  10~12  (Scudder).  Trans- 
lating these  into  the  corresponding  pK  values  we  have  5.17  and 


3 
4 
5 
6 

pH 

7 

^ 

N 

. 

"Ns 

..  x 

V 

v- 

\ 

-->s 

N^ 

V. 

<^ 

'N; 

<^ 

\ 

\ 

_                   2..                         « 

Equivalents  of  NaoH 

FlG.   6.    TlTRATION   OF  THE  "TRIBASIC"    AdD,    ClTRIC  AdD 

Shows  that  the  pKa  values  are  sufficiently  close  to  obscure  the  curvatures 
of  the  idealized  curves  for  each  step.  (After  Hastings  and  Van  Slyke 
(1922).) 

2.36. 1S    If  we  regard  the  compound  as  if  it  were  made  up  of  an 
acid  and  a  base  with  the  above  dissociation  constants  and  each 


NHS 


p-amino  benzoic  acid 


Cation 
in  acid  solutions 


COO 

Anion 
in  alkaline  solutions 


independent  of  the  other,  we  can  plot  the  dissociation  curves 
of  each  with  the  aid  of  equations  (12a)  and  (15a).  In  each  case 
the  dissociation-residue  curves  are  the  complements.  These  are 
plotted  in  figure  7  with  heavy  lines.  It  is  seen  that  they  cross 
at  pH  3.77.  This  means  that  at  pH  3.77  there  is  a  maximum 
of  undissociated  residue.  Now  if  the  salts  are  more  soluble 
18  See  page  48. 


30 


THE  DETERMINATION  OF  HYDROGEN  IONS 


than  the  free  compound  itself,  there  should  be  a  minimum 
solubility  at  pH  3.77.  Michaelis  and  Davidsohn  (1910)  found  a 
minimum  solubility  at  pH  3.80. 


FIG.  7.  DISSOCIATION  CURVES,  A  AND  B,  AND  DISSOCIATION-RESIDUE 

CURVES,  A'  AND  B',  FOR  P-AMINO  BENZOIC  ACID 

Treated  as  if  this  amphoteric  ionogen  were  composed  of  an  acid  with 
pKa  value  of  5.17  and  a  base  of  pKb  value  denned  by  pKb  =  pKw  —  2.36. 

Turning  to  the  light  lines  A  and  B  of  figure  7,  we  see  that  their 
intersection  is  at  a  point  where  the  percentage  of  the  compound 
ionized  as  an  anion  is  equal  to  the  percentage  ionized  as  a  cation. 
In  other  words  the  amount  carrying  a  negative  charge  is  equal  to 
the  amount  carrying  a  positive  charge.  Because  of  this  equality 
the  point  where  it  occurs  is  called  the  isoelectric point. 

If  we  still  maintain  the  simple  conditions  postulated  in  this 
elementary  treatment,  we  can  calculate  the  isoelectric  point  from 
the  dissociation  constants  of  an  amphoteric  electrolyte. 

Consider  an  amphoteric  electrolyte  of  the  type  HROH  for 
which  we  have  the  following  equilibrium  equations : 


[HR+]  [OH-] 
[HROH] 

IROH-]  [H+] 

[HROH] 


Kb 


(31) 


(32) 


I  ISOELECTRIC   POINT  31 

When  [HR+]  =  [ROH~]  (isoelectric  condition) 
[HROH]  [HROHI 

KbloiT    KaliTfT 


Hence  [H+]  =  /  Kw  (34) 


In  the  case  cited  above  [H+]  =  i/  2  3  x  KJ-H  10~" 


or  pH  =  log  =  3.77 

Furthermore  from  equations  (31)  and  (32) 


If  we  let  [HR+]  -f  [ROH~]  =  X,  X  becomes  a  minimum  when 


/K 
=  0,  a  condition  fulfilled  when  [H+]  =  A/ -~  Kw 

r  -*-*•!> 

In  other  words  the  sum  of  the  anion  and  cation  concentrations 
is  a  minimum  at  the  isoelectric  point. 

Only  in  case  Ka  =  Kb  will  the  isoelectric  point  correspond  with 
the  ' 'neutral  point,"  pH  7.0. 

It  is  at  once  evident  that  the  isoelectric  point  of  an  amphoteric 
electrolyte  is  a  point  at  or  near  which  there  should  tend  to  occur 
maximal  or  minimal  properties  of  its  solution.  Indeed  at  such 
points  have  been  found  to  occur  minimum  solubilities,  minimum 
viscosities,  minimum  swelling,  optimum  agglutinations,  etc. 

Lest  this  exposition  obscure  matters  of  importance  to  the 
treatment  of  complex  ampholytes,  the  reader  should  consult  such 
papers  as  that  of  S0rensen  and  Linderstr0m-Lang  (1927). 

See  Levene  and  Simms  (1923)  on  calculation  of  isoelectric 
points. 

In  figure  7  the  treatment  is  as  if  for  two  distinct  substances,  one 
an  acid  and  the  other  a  base.  Actually  the  acidic  group  and  the 


32 


THE  DETERMINATION  OF  HYDROGEN  IONS 


basic  group  are  in  the  same  molecule.  When  the  simultaneous 
equations  are  solved  for  the  identical  dissociation  residue  and  this 
is  charted,  its  curve  will  follow  B'  and  A'  for 'the  most  part  but 
will  pass  from  B'  to  A'  a  little  below  the  intersection  of  B'  and  A'. 

Figure  8  gives  another  set  of  cases. 

It  will  be  noted  that  this  elementary  outline  of  the  subject  of 
ampholytes  has  been  presented  with  the  aid  of  a  specific  case  in 
which  the  ion  formed  is  probably  the  univalent  anion  or  the 
univalent  cation  according  to  the  pH  .value  of  the  solution. 
Many  ampholytes  probably  ionize  in  such  a  way  as  to  form 
"hybrid"14  ions  of  the  type  +NH3-R-COO-  These  are  called  in 
the  German  Zwitter-Ionen,  signifying  hermaphroditic  ions.  They 


2        3        4         5        6         7        8         9        10       11        12      13        14 


FIG.  8.  REPRESENTATION  OF  THE  DISSOCIATION  CURVES  OF  HEXONE  BASES 
(After  Foster  and  Schmidt  (1923)) 

are  often  called  ampholyte  ions  with  the  implication  of  the  above 
special  significance  of  opposite  gender  or  of  hybrid  nature. 
Perlzweig  (1926)  uses  the  term  "amphoteric  ion." 

As  previously  suggested,  experimental  methods  do  not  always 
show  clearly  whether  an  acid  or  a  base  is  being  handled;  and  by 
the  same  token  it  is  often  uncertain  whether  an  ionization  constant 
assigned  to  an  ampholyte  from  the  measurements  has  been 
properly  formulated  as  an  acid  constant  or  should  be  reformu- 
lated as  a  basic  constant.  Thus  the  reformulation  of  the  so-called 
acid  and  basic  constants  of  certain  amino  acids  will  depict  these 

*4Kolthoff  and  Furman  (1926,  p.  49),  use  the  term  "hybrid  ion." 


STRONG   ACIDS 


33 


compounds  as  existing  as  hybrid  ions  at  the  isoelectric  point 
instead  of  as  undissociated  molecules.  For  a  more  detailed  dis- 
cussion of  this  matter  see  Bjerrum  (1923). 

It  should  be  emphasized  that  the  foregoing  relationships  have 
been  developed  from  very  simple  conditions.  When  these  con- 
ditions have  been  approached,  experimental  verification  has  been 
found.  The  insight  thus  gained  has  led  to  a  better  understanding 
of  complex  ampholytes,  the  complete  equilibria  of  which  can  be 
seen  only  in  broad  outline. 


14 


0     10  20  30  40   50   GO  70   80  90  100 
^Neutralization 

FlG.  9.  TlTRATION  _CURVES  OP  HYDROCHLORIC  AdD  AND  POTASSIUM 

HYDROXIDE 


"STRONG"  ACIDS  AND  BASES  AND  THEIR  SALTS 

Many  acids  like  hydrogen  chloride  (and  bases  like  sodium 
hydroxide)  are  so  near  complete  dissociation  in  dilute  solution  that 
a  first  approximation  in  their  treatment  can  be  accomplished  by 
assuming  complete  dissociation.  The  hydrion  concentration  is 
then  assumed  equal  to  the  concentration  of  the  substance.  If  a 
solution  of  hydrogen  chloride  is  under  consideration  and  is  pro- 
gressively undergoing  "neutralization"  by  potassium  hydroxide, 
there  is  obtained  actually  a  picture  of  the  relation  of  pH  to 
degree  of  "neutralization"  similar  to  one  or  the  other  of  the 


34          THE  DETERMINATION  OF  HYDROGEN  IONS 

curves  in  figure  9.  These  curves  were  calculated  on  the  assump- 
tion that  [H+]  =  ["unneutralized"  HC1].  A  similar  curve  for  the 
titration  of  KOH  is  also  shown  in  figure  9. 

However,  if  the  solution  vary  in  its  initial  content  of  one  or 
another  neutral  salt,  or  vary,  as  it  actually  does  during  titration, 
in  the  proportion  of  neutral  salt,  a  distinctly  appreciable  de- 
parture from  the  approximately  calculated  relations  noted  above 
will  be  found  when_jbhejiydrogen  electrode  method  of  measure- 
ment is  used.  FundamentaTIy~tKe  etfecT^s^olTve'ry  different 
from  the  "residual  error"  already  noted  when  hydrogen  electrode 
measurements  are  carried  into  the  elementary  treatment  of  a 
mixture  of  a  weak  acid  and  its  salt.  But  in  the  present  instance 
we  are  dealing  with  a  strongly  dissociating  acid  and  in  respect  to 
the  high  degree  of  dissociation  the  acid  is  like  salts  such  as  KC1. 
The  high  concentration  of  the  acid's  charged  ions  produces  an 
effect  as  truly  as  the  highly  dissociating  salts  produce  their 
effects.  Therefore,  the  displacement  of  the  actual  curve  from 
that  approximately  calculated  cannot  be  ascribed  solely  to  a 
"salt-effect."  Rather  should  it  be  called  an  evidence  of  the  con- 
duct of  strong  electrolytes  in  general. 

This  is  a  subject  which  has  stimulated  many  investigations 
and  has  led  to  still  incomplete  but  very  illuminating  results. 
The  modern  treatment  is  unique  but  a  discussion  of  it  must 
be  postponed.  However,  we  need  not  be  troubled  for  the 
time  being.  Although  we  have  introduced  simplifying  assump- 
tions restricting  too  free  and  generalized  application  of  the 
equations,  these  serve  admirably  to  outline  the  main  features  of 
the  subject.  To  only  a  little  less  degree  are  we  safe  in  outlining 
the  conduct  of  solutions  of  strong  acids  and  bases  by  the  assump- 
tion of  complete  dissociation.  Later  we  shall  return  to  detail. 


CHAPTER  II 

SOME  SPECIAL  ASPECTS  OF  ACID-BASE  EQUILIBRIA 
Words  are  the  footsteps  of  reason. — FRANCIS  BACON. 

Many  relations  implicit  in  the  general  equations  of  acid-base 
equilibria  do  not  appear  vivid  and  do  not  find  their  way  into 
everyday  practice  until  they  are  reargued,  reformulated  and 
named.  A  consequence  is  a  special  terminology  which  must  be 
understood  if  the  literature  is  to  be  followed  intelligently;  for 
sometimes  a  whole  subdivision  of  our  subject  is  summed  up  in 
a  single  expression. 

THE   pH    SCALE 

As  a  normal  solution  of  an  acid  has  been  defined  as  one  con- 
taining in  1  liter  of  solution  the  equivalent  of  1.008  grams  of 
acidic  hydrogen,  so  the  normal  solution  of  the  hydrogen  ion  was 
defined  to  be  one  containing  in  1  liter  of  solution  1.008  grams 
of  hydrogen  ions. 

Thus  an  acid  solution  may  be  described  in  terms  of  its  normal- 
ity with  respect  to  total  acid  or  in  terms  of  its  normality  with 
respect  to  hydrions. 

To  distinguish  between  these  two  components  with  their  com- 
mon unit  it  has  been  suggested  that  we  call  "normality"  in  its 
older  sense  the  quantity  factor  of  "acidity"  and  the  hydrogen 
ion  concentration  the  intensity  factor.  This  may  serve  to  em- 
phasize a  distinction,  but  the  suggested  analogy  with  the  quantity 
and  intensity  factors  of  energy  is  confusing  when  we  retain  for 
each  a  unit  of  the  same  category.  Nevertheless  the  two  com- 
ponents remain  in  a  restricted  sense  the  quantity  and  intensity 
factors  of  "acidity."  The  one  is  the  total  quantity  of  available 
acid.  The  second,  the  concentration  of  the  hydrogen  ions,  repre- 
sents the  real  intensity  of  "acidity"  whenever  it  is  the  hydrogen 
ion  which  is  the  more  directly  active  participant  in  a  reaction. 
This  is  admirably  expressed  when  we  use  for  hydrogen  ion  con- 
centrations a  mode  of  expression  which  links  it  with  the  potential 

35 


36          THE  DETERMINATION  OF  HYDROGEN  IONS 

of  a  hydrogen  electrode.  It  so  happens  that  in  determining  the 
hydrogen  ion  concentration  with  the  hydrogen  electrode  the 
potential  of  this  electrode  is  put  into  an  equation  which  reduces 
to  the  form : 

Potential  1 

=  log 


numerical  factor  [H+] 

Later  we  shall  see  that  this  potential,  expressed  in  volts,  is  the 
intensity  factor  in  the  free-energy  change  involved  in  the  trans- 
port of  hydrions  from  a  concentration  of  one  normal  to  another 

given  value  of  [H+].     Thus  the  expression  log  -      -  is  a  linear 

function  of  an  intensity  factor  of  energy-change  and  in  this  sense 
it  can  be  called  an  index  to  acid  intensity. 

On  the  other  hand  the  association  of  the  words  "potenz"  and 
"puissance"  with  pH  arose  in  a  totally  different  manner.  In  his 
original  article  S0rensen  (1909)  says: 

.  .  .  .  ,  la  grandeur  de  la  concentration  des  ions  hydrogene  s'exprime 
par  le  facteur  de  normalite  de  la  solution  par  rapport  aux  ions  hydrogene, 
facteur  indique  sous  la  forme  d'une  puissance1  negative  de  10. 

Dans  tons  les  cas  traites  dans  le  present  memoire  .... 

.  .  .  .  le  facteur  de  normalite  de  la  solution  sous  le  rapport  des  ions 
hydrogene  ou,  en  d'autres  termes,  le  nombre  d'atomes-grammes  d'ions 
hydrogene  par  litre  est  plus  petit  que  1  et  peut  etre  pos6  egal  a  10~p,  ou 
pour  le  nombre  p  je  propose  le  nom  d'exposant  des  ions  hydrogene  et  la 
designation  pH.  Par  exposant  des  ions  hydrogene  (pj)  d'une  solution,  nous 
entendons  done  le  logarithm  Brigg  de  la  valeur  reciproque  du  facteur  de 
normalite  de  la  solution  relativement  aux  ions  hydrogene. 

Comme  il  n'est  d'ordinaire  pas  question  de  solutions  d'ions  hydrogene 
plus  fortes  qu'une  solution  normale,  j'ai  choisi  la  definition  ci-dessus  de 
1'exposant  des  ions  hydrogene,  qui  par  suite  sera  generalement  un  nombre 
positif;  il  ne  sera  negatif  que  dans  les  cas  bien  rares  ou  Ton  a  affaire  & 
des  solutions  plus  fortes  que  la  normale. 

Thus  PH  is  denned  by  the  relation: 


As  a  matter  of  typographical  convenience  we  shall  use  pH  in 
place  of  the  original  p^  and  PH. 

1  "Potenz"  in  the  German  translation,  i.e.,  power  (mathematical). 


II 


pH-SCALE 


37 


If  we  follow  S0rensen's  original  suggestion,  pH  may  be  called 
the  hydrogen  ion  exponent.  Its  numerical  magnitudes  have 
been  called  "S0rensen  values,"  "reaction  numbers,"  etc.  The 
term  exponent  (puissance,  Potenz,  power)  is  employed  because 
the  relation 

pH  =  logic 


or 


[H+] 


pH  =  -  logw  [H+] 


may  be  written  [H+]   =   10~pH.     Here  —  pH  appears  as  an  ex- 
ponent. 

TABLE  3 

Relation  of  [H+]  to  pH 


[H+] 

pH 

[H+] 

pH 

10+1 

-1 

io-» 

7 

10±0 

0 

10~8 

8    ' 

10-1 

+1 

10~9 

9 

10~2 

2 

lO-io 

10 

io-« 

3 

10-" 

11 

io-< 

4 

10-u 

12 

10-' 

5 

etc. 

io-« 

6 

A  caution  may  now  be  noted.  A  difference  of  sign  occurs 
between  a  given  value  of  pH  and  the  exponent  found  when  the 
normality  of  the  corresponding  hydrogen  ion  concentration  is 
written  in  the  usual  way.  For  example,  —7  is  the  exponent  in 
10~7;  but  the  pH  value  corresponding  to  [H+]  =  10~7N  is  +7. 

The  gross  relation  of  [H+]  to  pH  is  shown  in  table  3.  See  also 
table  B,  appendix  (page  673). 

The  convenience  of  pH  over  [H+]  is  manifest  when  we  compare 
the  numerical  values  encountered  in  chemical  and  physiological 
studies.  For  instance,  one  enzyme  may  operate  most  actively  at 
a  hydrogen  ion  concentration  of  0.01  normal  while  another  is 
most  active  at  0.000,000,001  normal.  While  convenient  abbre- 
viations of  such  unwieldy  values  are  1  X  10~2  and  1  X  10~9, 
there  remains  the  difficulty  of  plotting  such  values  on  ordinary 


38  THE    DETERMINATION    OF   HYDROGEN   IONS 

cross-section  paper.  If  the  difference  between  0.000,000,001  and 
0.000,000,002  is  given  a  length  of  one  millimeter,  the  difference 
0.01  to  0.02  when  plotted  on  the  same  scale  would  be  ten  kilo- 
meters, ten  kilometers  distant.  Evidently  the  logarithmic 
spacing  should  be  followed  and  fortunately  it  is  the  logarithmic 
plotting  of  hydrogen  ion  concentration  (in  terms  of  pH)  which 
correctly  depicts  the  fact  that  the  difference  between  1  X  10~9 
and  2  X  10~9  may  be  as  important  to  one  set  of  equilibria  as  the 
enormously  greater  difference  between  1  X  10~2  and  2  X  10~2  is 
to  another  set  of  equilibria.  This  is  revealed  in  the  charts  on 
previous  and  subsequent  pages. 

Thus  both  convenience  and  the  nature  of  the  physical  facts 
invite  us  directly  or  indirectly  to  operate  with  some  logarithmic 
function  of  [H+j. 

It  is  unfortunate  that  a  mode  of  expression  so  well  adapted  to  the  treat- 
ment of  various  relations  should  conflict  with  a  mental  habit.  [H+] 
represents  the  hydrogen  ion  concentration,  the  quantity  usually  thought 
of  in  conversation  when  we  speak  of  increases  or  decreases  in  acidity. 
pH  varies  inversely  as  [H+].  This  is  confusing. 

The  normality  mode  of  expression  has  historical  priority  and  conse- 
quently conventional  force.  Since  there  is  a  hydrogen  ion  concentration 
for  each  hydroxyl  ion  concentration  it  became  the  custom,  following 
Friedenthal  (1904),  to  express  both  acidities  and  alkalinities  in  terms  of 
[H+].  This  gave  a  scale  of  one  denomination  and  the  meaning  of  "higher" 
and  of  "lower"  became  firmly  fixed.  Later  we  meet  the  new  scale  with 
its  direction  reversed.  The  inconvenience  is  unquestionable  and  partly 
because  of  this  the  pH  scale  has  been  criticized. 

Wherry2  (1919,  1927)  and  others  have  proposed  changes  of  one  kind  or 
another  which  they  believe  introduce  greater  simplicity  or  convenience. 
Wherry  (1927)  in  particular  has  urged  the  use  of  his  "active  acidity" 
[antilog  (7.0  —  pH)]  and  the  descriptive  terms:  super  acid  (pH3to4),raecfo'acid 
.(pH  4  to  5),  subacid  (pH  5  to  6),  minimacid  (pH  6  to  7),  neutral  (pH  7), 
minimalkaline  (pH  7  to  8),  etc.  His  purpose  is  admirable  and  his  case  well 
stated.  It  is,  in  short,  an  attempt  to  "humanize"  the  statement  of  acidity 
for  the  benefit  particularly  of  botanists. 

It  will  presently  be  indicated  that  we  are  not  denying  the  excellence  of 
the  purpose  if  we  classify  Wherry's  proposal  with  others.  We  may  pass 
over  the  fact  that  the  functions  offered  are  arbitrary  and  artificial.  The 
same  may  be  said  of  pH.  We  may  pass  over  the  fact  that  one  or  the  other 

2  Compare  Wherry  and  Adams  (1921)  with  reply  by  Clark  (1921).  See 
also  Giribaldo  (1925),  Derrien  andFontes  (1925),  Guillaumin  (1926),  Richter 
(1926),  Kolthoff  (1926),  Lambling. 


II  SUBSTITUTES    FOR    pH  39 

of  these  newer  functions,  offered  as  a  convenience,  would  entail  the  extreme 
inconvenience  of  recasting  in  a  new  mold  a  vast  amount  of  accumulated 
data  now  recorded  in  terms  of  pH.  The  fundamental  difficulties  with  all 
the  new  functions  so  far  proposed  are  these.  Some  of  them  involve  a  new 
basis  of  reference  when  we  are  having  difficulty  enough  with  the  con- 
ventional basis  (see  Chapter  XXIII) .  It  might  be  said  that  the  choice,  for 
instance,  of  "neutrality"  as  a  reference  point  is  made  without  involving 
those  refinements  which  acquaint  us  with  the  shifts  of  the  "neutral  point" 
and  is  made  for  purposes  of  approximate  descriptions  only.  As  in  all 
matters  of  definition  the-  choice  is  permissible.  However,  its  proposal  is 
as  much  as  to  say  that  the  proposer  has  no  anticipation  that  his  follower 
will  see  farther  than  he  sees  and  will  have  no  need  to  reestablish  contact 
with  the  refinements  he  has  ignored.  Those  substitutes  for  pH,  which 
have  been  proposed  so  far,  employ  so  many  unacknowledged  complexities 
and  tacit  assumptions  that  they  have  not  commanded  assent. 

If  simplicity  be  desired,  it  were  better  to  ignore  the  special  meanings  of 
pH,  [H+],  aH,  etc.,  which  these  various  authors  have  used  in  deriving  their 
new  functions;  it  were  better  to  ignore  the  almost  useless  "neutral  point," 
and  to  develop  the  themes  of  Chapters  XI  and  XXVII.  It  would  probably 
not  satisfy  the  novice  merely  to  tell  him  that  a  pH  value  is  to  be  used  as 
an  arbitrary  number  representing  the  state  of  acids  in  solution  but  if  he 
will  use  indicators  as  type  acids  he  can  visualize  something  of  what  the 
numbers  mean.  He  would  then  be  relieved  of  the  puzzling  question  of 
how  a  concentration  of  1,000,000  N  can  so  profoundly  affect  the  things  he 
deals  with  and  he  might  consent  to  use  the  numbers  with  the  conventional 
name  of  pH.  Because  the  subject  is  important  too  much  effort  cannot 
be  spent  upon  making  the  presentation  direct,  simple  and  at  the  same 
time  representative  of  actuality.  This  is  certainly  not  accomplished  by 
piling  one  convention  upon  another,  one  mathematical  function  upon 
another,  one  difficulty  upon  another.  Until  a  really  fundamental  and 
simple  change  is  proposed,  attempts  to  alter  what  has  become  established 
convention  should  be  vigorously  opposed  and  the  convenience  of  pH  should 
be  preserved. 

In  passing  it  may  be  noted  that  occasionally  a  mind  is  found  which 
honestly  distrusts  the  use  of  a  logarithmic  function  of  [H+]  because  it  is 
logarithmic.  Apparently  it  demands  [H+]  itself  from  a  sense  of  absolutism. 
One  possessed  of  this  obsession  might  profitably  consider  the  innumerable 
phenomena  which  are  most  vividly  described  by  use  of  logarithmic  func- 
tions. See,  for  example,  the  absorption  of  light  by  an  indicator  solution 
as  described  in  Chapter  VII.  But  see  in  particular  Chapter  XXVII. 

A  new  symbol,  paH,  has  been  suggested  by  S0rensen  and  Linderstr0m- 
Lang  (1924)  to  indicate  a  function  of  hydrion  activity  in  contrast  to  pH 
which  is  a  function  of  hydrion  concentration.  This  will  be  discussed  on 
page  479. 

While  discussing  "pH"  we  may  note  that  a  symbolization  originating 
in  S0rensen's  pH  is  coming  into  wide  use.  In  Chapter  I  it  is  noted  that, 


40  THE   DETERMINATION   OF   HYDROGEN   IONS 

when  a  dissociation  constant  occurs  in  an  equation  in  the  form  log  — , 

Ka 

it  has  become  the  custom  to  write  log  —  as  pKa.    So  also  the  custom  is 

l^a 

spreading  to  similar  functions  and  we  find,  for  instance,  pl~,  indicating  the 
logarithm  of  the  reciprocal  of  iodide  ion  concentration. 

THE   EFFECT   OF    DILUTION 

The  effect  of  dilution  upon  the  hydrogen  ion  concentration  of  a 
solution  may  be  briefly  generalized  by  some  approximations. 

Consider  an  acid  of  the  type  HA  for  the  dissociation  of  which 
we  have  the  equilibrium  equation: 

[H+]  X  [A-] 
[HA] 

If  Ka  is  small  there  must  obviously  be  a  large  reserve  of  undis- 
sociated  acid  so  long  as  the  concentration  of  total  acid  is  high. 
As  the  solution  is  diluted  this  reserve  dissociates  to  keep  Ka 
constant;  but  there  is  a  readjustment  of  all  components  which  can 
be  conveniently  followed  only  by  means  of  the  simple  algebraic 
equation  expressing  the  equilibrium  condition. 

If  the  acid  alone  is  present  in  the  solution  we  may  assume  that 
[A-]  =  [H+].  Also  if  [Sa]  =  the  total  acid,  [HA]  ==  [SJ  -  [H+]. 

Substituting  these  in  the  above  equation  and  solving  for  [H+] 
we  have: 


[H 
When  Ka  is  small  in  relation  to  [Sa] 

[H+]  ^ 

Compare  the  equation  on  page  13.  On  these  assumptions  the 
hydrogen  ion  concentration  should  vary  with  dilution  of  the 
solution  (diminution  of  Sa)  only  as  the  square  root  of  Ka[Sa]. 

If  there  is  present  a  salt  of  the  acid  we  can  apply  the  equation 
derived  on  page  22  which  shows  that  the  hydrogen  ion  concen- 
tration of  a  mixture  of  a  weak  acid  and  its  highly  dissociated  salt 


II 


DILUTION 


41 


is  determined  approximately  by  the  ratio  of  acid  to  salt.  Since 
dilution  does  not  change  the  ratio,  such  a  mixture  should  not  suf- 
fer a  change  of  hydrogen  ion  concentration  beyond  the  limits  set 
by  the  approximate  treatment  with  which  this  relation  was 
derived. 

Therefore,  except  for  solutions  of  high  hydrogen  ion  concentra- 
tion induced  by  the  presence  of  unneutralized  strong  acids,  the 
hydrogen  ion  concentration  should  vary  with  dilution  somewhere 
between  the  zero  change  indicated  by  the  last  approximation  and 
the  square  root  relation  first  indicated. 

If  an  acid  be  one  which,  in  pure  solution,  is  completely  disso- 
ciated, the  hydrion  concentration  is  equal  to  the  analytical  or 
stoichiometrical  normality  of  the  acid.  This  will  not  be  shown 
precisely  by  the  hydrogen  electrode  method  of  measurement  since 
this  device  measures  energy  changes  which  are  not  strictly  propor- 
tional to  concentration  changes.  This  appears  in  a  striking  way 
when  a  solution  of  hydrochloric  acid  is  concentrated.  At  some 
dilutions  the  hydrion  concentration,  as  calculated  with  the  aid 
of  the  uncorrected  formula  for  the  concentration  cell,  will  appear 
to  be  higher  than  that  of  the  available  acid.  This  aspect  will 
be  discussed  later. 

In  the  case  of  mixtures  of  weak  acids  and  their  salts,  dilution 
may  in  many  instances  produce  changes  in  hydrion  concentra- 
tion too  small  to  be  detected  by  any  but  refined  methods.  Ad- 
vantage of  this  is  taken  in  the  dilution  of  solutions  otherwise  too 
dense  optically  for  the  application  of  the  indicator  method. 

The  effect  of  dilution  should  be  reconsidered  after  reading  the 
last  part  of  Chapter  XXV. 

TABLE  4 

Effect  of  dilution 


MOLKCULAK  CONCEN- 
TRATION OF  GLY- 
COCOLL 

PH 

MOLECULAR  CONCEN- 
TRATION OP  A8PAR- 
AOINE 

PH 

1.0 

6.089 

1.0 

2.954 

0.1 

6.096 

0.1 

2.973 

0.01 

6.155 

0.01 

3.110 

0.001 

6.413 

0.001 

3.521 

0.0001 

6.782 

0.0001 

4.166 

42          THE  DETERMINATION  OF  HYDROGEN  IONS 

For  bases  and  amphoteric  electrolytes  relations  similar  to  those 
discussed  above  may  be  deduced. 

One  or  two  actual  cases  may  be  of  interest.  S0rensen  has 
given  the  accompanying  table  (table  4)  of  the  pH  values  of  dif- 
ferent dilutions  of  asparagine  and  glycocoll. 

The  dilution  here  is  ten-fold  at  each  step,  yet  the  increase  in 
pH  is  very  small  while  the  solutions  are  between  l.OandO.Ol  M. 

Walpole  (1914)  besides  giving  data  on  the  hydrogen  electrode 
potentials  of  various  dilutions  of  acetic  acid  and  "standard  ace- 
tate," has  determined  the  effect  of  a  twenty-fold  dilution  of 
various  acetic  acid-sodium  acetate  mixtures.  The  change  of  pH 
on  twenty-fold  dilution  of  standard  acetate  is  about  0.08  pH; 
and  for  mixtures  of  acetic  acid  and  sodium  acetate  which  lie  on 
the  flat  part  of  the  curve  the  change  of  pH  is  of  the  same  order 

of  magnitude.    When  the  ratio      acetlc  acid      reaches  19/1  the 

sodium  acetate 

change  is  about  0.3  pH. 

See  Cohn  (1927)  and  page  509  on  the  dilution  of  phosphate 
solutions. 

The  brief  outline  given  above  takes  no  account  of  changes  of 
equilibrium  which  sometimes  occur  in  colloidal  solutions. 

"NEUTRALITY"  AND  VALUES  OP  Kw 

It  was  shown  in  Chapter  I  that,  under  ideal  conditions,  the 
product  of  the  hydrogen  ion  concentration  and  the  hydroxyl  ion 
concentration  of  an  aqueous  solution  is  constant 

[H+]  [OH-]  =  Kw 

Therefore,  aqueous  solutions,  even  those  containing  large  excess 
of  hydrogen  ions  (i.e.  strongly  acid  solutions)  must  contain 
sufficient  hydroxyl  ions  to  maintain  the  constant  relation  shown 
above.  Likewise  aqueous  solutions,  even  those  containing  large 
excess  of  hydroxyl  ions  (i.e.  strongly  alkaline  solutions),  must 
contain  sufficient  hydrogen  ions  to  maintain  the  constant  rela- 
tion shown  above.  Obviously,  there  will  be  one  point  at  which 
the  concentration  of  hydrogen  ions  will  equal  the  concentration 
of  the  hydroxyl  ions,  that  is  [H+]  =  [OH~].  Using  for  Kw  the 
rounded  value  10~14,  we  find  this  point  as  follows. 

[H+]2  =  [OH-]2  =  10~14  or  [H+]  =  [OH~]  =  10~7 


II 


NEUTRALITY  43 


In  other  words,  equality  of  hydrion  and  hydroxyl  ion  concentra- 
tions occurs  at  pH  =  7.  This  is,  as  stated,  an  approximation. 
Here  no  account  has  been  taken  of  the  variation  of  the  value  of 
Kw  with  variation  of  temperature,  salt-content  of  the  solution, 
etc.,  nor  of  the  precise  meaning  of  the  values  called  Kw  as  they 
are  derived  from  experimental  measurements  of  very  different 
types. 

Considerable  confusion  will  be  avoided  if  there  is  maintained  a 
categorical  as  well  as  an  obviously  numerical  distinction  between 
Kw  and  the  pH  value  called  "neutrality." 

The  pH  value. 7.0  is  a  convenient  reference  point  with  which  to 
differentiate  "acid"  from  "alkaline"  solutions  in  ordinary,  crude 
descriptions.  Otherwise,  it  is  of  little  practical  significance.  To 
be  sure,  it  is  the  pH  value  of  pure  water  and,  therefore,  an  interest- 
ing value  to  calculate  as  a  derivation  from  water's  characteristic 
constant,  Kw.  But  pure  water  itself  has  seldom  been  seen  and  is 
of  little  use.  Its  hydrogen  ion  concentration  has  no  general 
relation  to  the  hydrogen  ion  concentration  at  the  equivalence  point 
sought  in  the  "neutralization"  of  an  aqueous  solution  of  an  acid 
by  an  aqueous  solution  of  a  base.  This  will  be  made  plain  in 
the  discussion  of  the  theory  of  titration  (Chapter  XXVIII)  but  it 
also  appears  in  several  of  the  figures  of  Chapter  I.  "Neutrality" 
is  also  of  no  interest  whatever  in  the  study  of  ampholytes.  See 
Chapter  I. 

In  contrast  to  the  pH-value  7,  Kw,  the  ionic  product  of  water, 
is  frequently  employed  when  formulations  of  equilibria  involve 
both  hydroxyl  and  hydrogen  ions.  The  relation  [H+]  [OH~]  = 
Kw  enables  one  to  eliminate  either  [OH~]  or  [H+]  when  desired. 
Usually  the  necessity  of  this  transformation  may  be  avoided  as 
will  be  shown  in  the  discussion  starting  on  page  46. 

Kw  has  been  determined  by  a  variety  of  methods  and  with 
substantial  agreement.  The  following  are  some  instances. 

Kohlrausch  and  Heydweiller  (1894)  determined  the  electrical 
conductivity  of  water  approaching  very  near  to  purity.  On  the 
assumption  that  the  conductance  is  proportional  to  the  numbers 
and  mobilities  of  the  hydrogen  and  hydroxyl  ions,  that  these  are 
present  in  equal  concentrations  and  that  the  mobilities  of  the 
hydrogen  and  hydroxyl  ions  are  known,  there  can  be  calculated 
the  value  of  Kw.  Wijs  (1893)  used  the  results  of  a  study  of  the 


44 


THE    DETERMINATION    OF    HYDROGEN    IONS 


relative  rates  of  hydrolysis  of  methyl  acetate  by  hydrions  and 
hydroxyl  ions  and  applied  these  data  to  the  case  of  the  hydrolysis 
of  methyl  acetate  by  water.  There  have  also  been  studies  of  the 
hydrolysis  of  salts,  studies  on  the  hydrogen  potential  in  acid  and 
alkaline  solutions  (e.g.,  Lewis,  Brighton  and  Sebastian  (1917))  and 
many  other  studies  leading  to  substantially  the  same  order  of 
magnitude  for  Kw. 

Kolthoff  (1921)  has  compiled  the  following  table  5  showing  the 
"dissociation"  constant  of  water  at  different  temperatures  as 
given  by  different  authors.  Lewis,  Brighton  and  Sebastian 
(1917)  found  Kw  =  1.012  X  10~14  at  25°C.  Hence,  [H+]  =  1.006 

TABLE  5 

Ion-product  (dissociation  constant}  of  water  at  different  temperatures 
(After  Kolthoff  and  Furman  (1926)) 


TEMPER- 
ATURE 

AUTHORITIES 

1 

2 

3 

4 

0 

0.12  X  10-" 

0.14  X  10-" 

0.089  X  10-" 

18 

0.59  X  10~" 

0.72  X  10-" 

0.74  X  10-" 

0.46    X  10-" 

25 

1.04  X  10-" 

1.22  X  10-" 

1.27  X  10-" 

0.82    X  10-" 

50 

5.66  X  10-" 

8.7    X  10-" 

100 

58.20  X  10-" 

74.0    X  10-" 

48.0      X  10-" 

1.  Kohlrausch  and  Heydweiller  (recalculated  by  Heydweiller)  (1909). 
2>.  Lorenz  and  Bohi  (1909). 

3.  Michaelis  (1914),  p.  8,. 

4.  Various  investigators. 

X    10~7   (practically,   pH    =    7.0).     Lewis  and  Kandall   (1923) 
give  Kw  =  1.005  X  10~14  at  25°C. 

The  following  values  of  pKw   (log  — )   given  by  Michaelis 

Kw 

(1922)  (see  table  6)  were  obtained  on  a  basis  somewhat  different 
from  that  used  by  Lewis,  Brighton  and  Sebastian. 

Here  it  may  be  said  that  Kw  appears  as  a  constant  because,  in 
its  derivation,  there  was  introduced  at  the  very  beginning  the 
postulate  that  the  environment  is  to  be  constant.  If  the  solu- 
tion be  altered,  as  by  the  addition  of  a  certain  quantity  of  neutral 
salt,  there  is  the  possibility  that  Kw  will  have  a  new  value  under 


II 


IONIC    PRODUCT   OF   WATER 


45 


the  new  conditions.  It  is  only  on  the  expectation  that  the  altera- 
tion will  be  slight  in  ordinary  changes  of  composition  that  we  are 
justified  in  neglecting  the  corrections  which  modern  theoretical 
methods  have  brought  to  light.  However  figure  10  will  illustrate 

TABLE  6 

Interpolated  values  of  —  log  Kw 
(After  Michaelis  (1922)) 


TEMPERATURE 

i 

LOO^r- 

Kw 

pH   OF  NEUTRAL  POINT 

•c. 

16 

14.200 

7.10 

17 

14.165 

7.08 

18 

14.130 

7.07 

19 

14.100 

7.05 

20 

14.065 

7.03 

21 

14.030 

7.02 

22 

13.995 

7.00 

23 

13.960 

6.98 

24 

13.925 

6.96 

25 

13.895 

6.95 

26 

13.860 

6.93 

27 

13.825 

6.91 

28 

13.790 

6.90 

29 

13.755 

6.88 

30 

13.725 

6.86 

31 

13.690 

6.85' 

32 

13.660 

6.83 

33 

13.630 

6.82 

34 

13.600 

6.80 

35 

13.567 

6.78 

36 

13.535 

6.77 

37 

13.505 

6.75 

38 

13.475 

6.74 

39 

13.445 

6.72 

40 

13.420 

6.71 

what  is  to  be  expected.     Note  the  specific  effects  of  salts  so  similar 
as  are  sodium  chloride  and  potassium  chloride. 

At  this  point  it  is  appropriate  to  remark  that,  since  in  exact 
treatments  of  equilibria  a  correction  term  for  Kw  (or  varying 
activity  coefficient  for  water,  see  later  chapters)  must  be  taken 
into  consideration,  it  will  be  well  to  formulate  the  elementary 


46 


THE  DETERMINATION  OF  HYDROGEN  IONS 


aspects  of  our  subject  by  avoiding  forms  which  include  Kw 
wherever  that  is  feasible.  This  will  be  our  policy  in  dealing  with 
bases,  although  the  classical  equations  will  also  be  shown.  The 
variation  of  Kw  constitutes  one  of  very  many  reasons  for  avoiding 
several  of  the  schemes  which  have  been  suggested  as  substitutes 
for  the  pH  scale  (see  p.  39)  and  which  involve  Kw  in  their 
derivations. 

Although  a  correction  term  must  be  applied  in  refined  formula- 
tion and  although  this  correction  term  varies  with  every  change 
in  the  composition  of  the  solution,  the  rounded  values  of  Kw  as 
given  by  Michaelis  (1922)  and  shown  in  table  6  may  be  used  for 
ordinary,  approximate  calculations. 


1.6 

1.5 

1.4 

"2    ,.3 


1.2 


I, 


1.0 


0.5  1.0  1.5 

SQUARE    ROOT  OF  CONCENTRATION 


FIG.  10.  VARIATION  OF  V  Kw  WITH  CONCENTRATION  OF  SALT 


FORMULATION  OF  EQUILIBRIA  IN  SOLUTIONS  OF  BASES  WITH 
AVOIDANCE    OF   THE   USE   OF    [OH~]    AND   Kw 

In  Chapter  I  figure  2  was  constructed  by  first  formulating  the 
equilibria  of  acids  and  of  bases  separately  and  then  aligning  the 
two  sets  of  curves  by  use  of  the  relation 

pH  +  pOH  =  pKw^14 

In  such  a  system  of  formulation  the  transformation  of  a  given 
value  of  pOH  to  a  corresponding  value  of  pH  (or  vice  versa)  may 
be  made  whenever  desired  by  use  of  that  numerical  value  of  pKw 
which  is  applicable  to  the  specific  conditions.  Therefore,  it  is 
convenient  in  general  discussion  to  neglect  pOH  and  to  use  pH 
uniformly. 


II 


FORMULATION   WITHOUT   [OH" 


47 


Now  consider  figure  11  in  conjunction  with  figure  2  (page  16). 
In  figure  11  there  is  shown  by  curve  C  the  relation  between  pH 
and  percentage  dissociation-residue  for  an  acid  having  the 
dissociation  curve  B.  Obviously  curve  C  has  the  form  of  the 
dissociation  curve  for  a  base.  Its  position  on  the  pH  scale  is 
made  evident  by  the  legend  of  figure  11. 

Thus,  if  it  suits  our  convenience,  we  may  proceed  to  deal  with 
the  cation  of  a  base  as  if  we  were  dealing  with  the  dissociation 


50 


cV 


pH3          4  5  6  78          9  10 

FIG.  11.  DISSOCIATION  CURVES  AND  DISSOCIATION  RESIDUE  CURVES 

A.  Dissociation  curve  for  acid,  pKa  =  8.0. 

B.  Dissociation  curve  for  acid,  pKa  =  4.8. 

C.  Dissociation  curve  for  base,  pKb  =  14  -  4.8  =  9.2  or  dissociation- 
residue  curve  for  acid  pKa  =  4.8. 

* 

residue  of  an  acid.  Likewise  we  may  deal  with  the  dissociation 
residue  of  a  base  as  if  we  were  dealing  with  the  anion  of  an  acid. 
Likewise  if  our  knowledge  of  a  compound  tells  us  nothing  of  its 
acidic  or  basic  nature  and  if  a  series  of  measurements  can  be 
formulated  by  equation  (12a)  or  by  equation  (15a)  we  shall  not 
be  able  to  tell  by  these  measurements  and  their  formulation 
whether  we  are  dealing  with  an  acid  or  a  base. 

However,  there  is  a  more  direct  way  of  arriving  at  a  uniform 
method  of  formulation.  Consider,  for  instance,  equilibria  in 
solutions  of  ammonia. 

Ammonia,  NH3,  is  usually  considered  the  parent  of  the  base 


48  THE    DETERMINATION   OF   HYDROGEN   IONS 

NH4OH,  a  hypothetical  substance  supposed  to  be  formed  by  the 
hydration 

NH3  +  H20  ->  NH4OH 
A  basic  dissociation  constant  could  be  defined  by 

[NH4+]  [OH-] 
[NH4OH] 

If  this  were  used,  we  would  proceed  in  the  classical  manner. 
Ammonia  systems  may  equally  well  be  treated  in  accordance 
with  the  following  formulation3 

[NHS]  [H+] 
[NHt] 

3  It  is  instructive  to  note  the  following: 
For  the  hydration  equilibrium: 

[NHJ  [H.O] 


[NH4OH] 
For  the  dissociation  equilibrium: 

[NHt]  [OH-] 
[NH4OH] 

Combine  these  two  equations  to  yield: 

[NHJ  [H20] 


=  Kh 


Kb 


[NHJ]  [OH-]       Kb 
Introduce  [H+]  [OH~]  =  Kw 

[NHJ  [H+]         Kh  Kw 


[NHJ]          Kb  [H20] 
If  [H2O]  is  regarded  as  a  constant 

[NHJ  [H+]  _ 
[NHt] 


II  FORMULATION   OF   BASES  49 

There  are  many  amino  compounds  which  are  substituted 
ammonias,  —  primary,  secondary  and  tertiary  ammonias.  These 
may  be  considered  to  add  hydrions  and  the  equilibrium  equation 
can  be  formulated  as  is  done  in  the  last  equation  above.  We  have 
also  to  consider  the  quaternary  ion,  R^RsRiN^.  In  this  case 
it  would  seem  more  logical  to  formulate  the  basic  dissociation 
as  follows 

[R1R2R3R4N+]  [OH-] 
[RiR2R3R4NOH] 

But  the  quarternary  ammonium  hydroxides  are  exceedingly 
strong  bases.  Frequently  they  are  so  strong  that  complete  dis- 
sociation may  be  assumed  as  it  is  in  the  case  of  sodium  and 
potassium  hydroxides.  Under  such  circumstances  equations  of 
the  ordinary  type  are  of  little  practical  value  as  stated  on  page 
12.  The  majority  of  the  weak  organic  bases  may  be  treated  as 
the  ammonia  system  is  above  and  the  equilibrium  equation  may 
be  written 


[RiR2R3N+H] 


Thereby  one  avoids  the  necessity  of  considering  either  [OH~] 
or  Kw. 

The  important  point  is  that  in  general  either  mode  of  treat- 
ment can  be  adapted  to  convenience.  When  a  more  comprehensive 
formulation  capable  of  extension  to  all  sorts  of  non-aqueous 
solutions  is  desired,  those  presented  by  Br0nsted  (1923)  and  by 
Lewis  in  Valence  will  be  found  useful.  See  also  Lowry  (1924). 


This  is  the  equation  given  in  the  text  where  Ka  is  substituted  for  the 
constant 

KhKw 


Kb  [H20] 

This  way  of  avoiding  an  account  of  the  changing  properties  of  the 
solvent  is,  in  a  sense,  only  a  "dodge." 


50  THE    DETERMINATION    OF   HYDROGEN   IONS 

BUFFER   ACTION 

If  we  were  to  add  to  1  liter  of  perfectly  pure  water  of  pH  7.0, 
1  cc.  of  O.OlN  HC1,  the  resulting  solution  would  be  about  pH  5.0 
and  very  toxic  to  many  bacteria.  If,  on  the  other  hand,  we 
were  to  add  this  same  amount  of  acid  to  a  liter  of  a  standard 
beef  infusion  medium  of  pH  7.0,  the  resulting  change  in  pH  would 
be  hardly  appreciable.  This  power  of  certain  solutions  to  resist 
change  in  reaction  was  commented  upon  by  Fernbach  and 
Hubert  (1900)  who  likened  the  resistance  of  phosphate  solutions 
to  a  "tampon."  The  word  was  adopted  by  S0rensen  (1909)  and 
in  the  German  rendition  of  his  paper  it  became  "Puffer"  and 
thence  the  English  "buffer."  There  has  been  some  objection4 
to  this  word  so  applied,  but  it  now  possesses  a  clear  technical 
meaning  and  is  very  widely  used.  By  buffer  action  is  meant  the 
resistance  to  change  of  pH  exhibited  by  a  solution  when  it  is  sub- 
jected to  gain  or  loss  of  acid  or  alkali.  The  elementary  theory  of 
buffer  action  is  already  clear  if  the  implications  of  the  simple 
equations  of  Chapter  I  are  understood. 

Returning  to  figures  4  to  6  we  see  that  along  the  flat  portion  of  a 
titration  curve  considerable  alkali  has  to  be  added  to  produce 
much  change  in  pH.  Conversely,  the  addition  of  a  strong  acid 
would  not  have  anywhere  near  the  effect  at  this  flat  portion  of  the 
curve  that  it  would  have  near  either  end.  Thus  it  is  evident  that 
a  mixture  of  an  acid  and  its  salt  will  tend  to  stabilize  the  pH 
of  the  solution  only  within  certain  narrow  zones  having  vague 
boundaries.  Mixtures  buffering  the  solution  within  such  a  pH 
zone  are  often  referred  to  as  "regulator  mixtures."  They  are  of 
very  great  value  to  the  analyst  and  the  physiological  chemist  in 
that  they  furnish  a  means  of  stabilizing  the  hydrogen  ion  con- 
centration within  a  predetermined  zone.  The  middle  point  of 
this  zone,  where  the  strongest  buffer  action  is  exerted,  is  deter- 
mined approximately  as  shown  on  page  17  by  the  dissociation 
constant  of  the  acid  or  base  concerned.  Other  things  being 
equal,  the  choice  of  mixtures  is  thus  revealed  in  a  table  of  disso- 
ciation constants. 

*  "Moderator"  is  sometimes  preferred.  Moore,  Roaf  and  Whitley  were 
employing  the  concept  as  early  as  1905  under  the  term  "balanced- 
neutrality." 


II 


BUFFERS 


51 


Henderson  (1908)  and  Washburn  (1908)  simultaneously  utilized 
the  principle  that  an  equimolecular  mixture  of  an  acid  and  its 
salt  will  stabilize  the  hydrion  concentration  of  a  solution. 

Emphasis  may  be  placed  upon  one  or  another  aspect  of  buffer 
action  by  means  of  the  following  examples. 

A  1  per  cent  solution  of  Witte  peptone  was  found  to  have  a 
pH  value  of  6.87.  To  equal  portions  of  the  solution  were  added 


/ 

^ 

— 

— 

f 

7 

^ 

— 

5 

J 

/ 

/^ 

/ 

\ 

*/ 

/ 

/ 

• 

7 

P 

/ 

/ 

/ 

8 

/ 

/ 

/ 

/ 

! 

a 

| 

/ 

1 

42024 
C.C. 

FIG.  12.  TITEATION  CURVES  OF  1  PER  CENT  ANDJ>  PER  CENT  PEPTONE 

SOLUTIONS  yjjj 

Ten  cubic  centimeters  of  peptone  solution  titrated  with  0.1  N  lactic 
acid  (to  right)  and  with  0.1  N  NaOH  (to  left). 

successively  increasing  amounts  of  O.!N  lactic  acid  and  the  result- 
ing pH  was  measured  in  each  case.  There  were  also  added  to 
equal  portions  of  the  solution  successively  increasing  amounts  of 
O.!N  NaOH  and  the  resulting  pH  was  measured  in  each  case. 
The  pH  values  were  then  plotted  on  cross  section  paper  as  ordi- 
nates  against  the  amount  of  acid  or  alkali  added  in  each  case  as 
abscissas.  This  gave  curve  1  shown  in  figure  12.  The  other 
curve  shown  in  this  figure  was  constructed  with  data  obtained 
with  a  5  per  cent  solution  of  Witte  peptone. 


52 


THE  DETERMINATION  OF  HYDROGEN  IONS 


Figure  12  shows  that  the  buffer  action  of  a  solution  is  dependent 
upon  the  concentration  of  the  constituents.  The  5  per  cent  solu- 
tion is  much  more  resistant  to  change  in  pH  than  the  1  per  cent 
solution. 

It  will  also  be  noticed  that  in  either  case  the  buffer  action  is 
not  the  same  at  all  points  in  the  curve.  In  other  words  the  buffer 
action  can  not  be  expressed  by  a  constant  but  must  be  determined 
for  each  region  of  pH.  This  is  illustrated  even  more  clearly  by 
the  titration  curve  for  phosphoric  acid  (fig.  4,  page  28).  At 
the  point  where  the  solution  contains  only  the  primary  phosphate 


c.c. 


20 


40 


60 


FIG.  13.  TITRATION  OF  A  BEEF-INFUSION  CULTURE  MEDIUM 
One  hundred  cubic  centimeters  of  medium  titrated  with  0.2  N  HC1 
solution  in  one  case  and  with  0.2  N  lactic  acid  solution  in  the  other  case. 

and  again  where  it  contains  only  the  secondary  phosphate  there 
is  very  little  buffer  effect  indeed. 

Furthermore  the  buffer  action  of  a  solution  may  not  be  due 
entirely  to  the  nature  of  the  initial  constituents  titrated  but  also 
to  the  nature  of  the  substance  with  which  it  is  titrated.  This 
point  may  be  illustrated  by  titrating  a  beef  infusion  medium  in 
the  one  case  with  hydrochloric  acid  and  in  the  other  case  with 
lactic  acid,  both  of  the  same  normality  (see  fig.  13).  It  will  be 
seen. that  at  first  the  two  curves  are  identical.  As  the  region  is 
approached  where  the  dissociation  of  the  lactic  acid  (a  weak  acid) 
is  itself  suppressed  because  of  the  accumulation  of  lactate  ions 
(and  the  hydrogen  ions)  further  addition  of  this  acid  has  com- 


II  BUFFERS  53 

paratively  little  effect.  The  "strong"  acid,  hydrochloric,  on  the 
other  hand  continues  to  be  effective  in  changing  pH  until  at  high 
hydrion  concentrations  the  logarithmic  function  suffers  less 
change.  As  already  noted  in  Chapter  I,  hydrochloric  acid  may 
be  considered  in  approximate  treatments  as  completely  disso- 
ciated. The  flattening  of  the  titration  curve,  of  which  pH  is  the 
ordinate,  is  therefore  inherent  in  the  nature  of  the  case;  but  it 
must  not  be  presumed  that  a  mere  mathematical  limitation 
obscures  the  reality  of  a  physically  significant  buffer  effect. 
Imagine  an  acid  which  is  not  totally  dissociated  but  which  has  a 
high  dissociation  constant.  The  degree  of  its  dissociation  remains 
a  function  of  pH  and  if  we  are  to  suppress  its  dissociation  com- 
pletely we  might  have  to  run  the  pH  value  of  the  solution  into 
negative  values  by  adding  high  concentrations  of  very  strong 
acids.  Ultimately  we  reach  a  limit  in  the  "strength"  of  the  acids 
available  and  can  use  only  higher  total  concentrations  of  those 
acids  which  approach  complete  dissociation  in  dilute  solution.5 

These  examples  will  suffice  to  make  it  evident  that  the  buffer 
action  of  a  solution  is  dependent  upon  the  nature  and  the  con- 
centration of  the  constituents,  upon  the  pH  region  where  the 
buffer  action  is  measured  and  upon  the  -nature  of  the  acid  or 
alkali  added. 

The  main  aspect  of  the  subject  is  summed  up  in  the  relation 

that,  so  long  as  the  ratio  does 


rr  rrrr  , 

[HAJ        [M  J  L-tlAJ 

not  depart  far  from  unity,   [H+]   cannot  depart  far  from  the 
constant  Ka. 

Buffer  action,  that  is  resistance  to  change  of  pH  upon  addition 
or  loss  of  acid  or  alkali,  cannot  always  be  so  easily  formulated. 
For  instance,  suppose  that  there  is  present  in  a  solid  phase  some 
material  which  adsorbs  from  the  solution  a  component  of  the 
solution's  acid-base  equilibrium.  That  substance,  by  reason  of  its 
ability  to  take  up  or  give  off  the  adsorbed  component  according 
to  the  concentration  of  the  component  in  the  liquid  phase,  may 
act  as  a  buffer.  Henderson  (1909)  called  attention  to  this.  Bovie 
(1915)  and  others  have  shown  the  buffering  effect  of  charcoal. 

5  Later  we  shall  encounter  the  case  of  an  acid  dye  which  behaves  as  if 
it  has  a  dissociation  exponent,  pK  =  1.5.  To  obtain  what  appeared  to  be 
complete  dissociation  there  was  used  36  per  cent  HC1  solution! 


54 


THE  DETERMINATION  OF  HYDROGEN  IONS 


When  a  component  of  the  acid-base  equilibrium  of  a  solution 
reaches  such  a  concentration  that  it  precipitates  and  forms  a 
solid  phase  in  equilibrium  with  the  liquid  phase,  the  zone  of  pH, 
within  which  buffer  action  would  be  expected  from  the  relations 
for  homogeneous  solutions,  may  be  considerably  altered.  The 
direction  which  the  treatment  then  takes  is  outlined  on  page  582 

Since  the  types  of  such  cases  are  numerous,  we  shall  not  pause 
to  discuss  the  detail;  but  it  should  be  noted  that  the  subject 
is  of  fundamental  importance  to  many  problems  of  physiology, 
analysis,  etc. 

There  are  occasions  when  a  more  elegant  definition  of  buffer 
action  leads  to  very  useful  formulas.  Thus  Van  Slyke  (1922), 


.3 


.2 


PH 

FIG.  14.  BUFFER  ACTION 
Change  of  pH  on  addition  of  base 

in  an  independent  development  of  a  treatment  first  attempted 
by  Koppel  and  Spiro  (1914)  (cf.  Lehmann,  1922,  and  Michaelis 
and  Perlzweig,  p.  106)  proposes  the  following. 

Let  there  be  charted  as  in  figure  14  the  relation  between  pH 
and  the  equivalents  of  base  per  liter  added  to  a  given  solution. 

Between  the  points  A  and  C  the  ratio  -TT-^T  gives  the  slope  of 


the  line  AC.  This  is  only  a  rough  indication  of  the  order  of 
magnitude  of  the  slope  of  a  tangent  to  the  curve  in  this  region. 
The  slope  of  the  tangent  obviously  changes  between  its  position 
at  A  and  its  position  at  C.  To  obtain  the  slope  at  any  point 
use  is  made  of  the  infinitesimals  dB  and  d(pH). 


II  BUFFER   INDEX  55 

Van  Slyke  then  describes  a  unit  for  the  buffer  effect.     "The 

JT>    «^V**' 

unit  adopted  is  the  differential  ratio  -,.  T,.?  expressing  the  rela- 


tionship  between  the  increment  (in  gram  equivalents  per  liter) 
of  strong  base  B  added  to  a  buffer  solution  and  the  resultant 
increment  in  pH.  Increment  of  strong  acid  is  equivalent  to  a 
negative  increment  of  base,  or  —  dB.  In  these  terms  a  solution 
has  a  buffer  value  of  1  when  a  liter  will  take  up  1  gram  equivalent 
of  strong  acid  or  alkali  per  unit  change  in  pH.  If  base  is  added 
to  a  solution,  pH  is  increased,  so  that  both  dB  and  d(pH)  are 
positive.  If  acid  is  added  both  dB  and  d(pH)  are  negative. 

The  ratio  ,,        is,  therefore,  always  a  positive  numerical  value." 


To  summarize  Van  Slyke  's  treatment  we  shall  proceed  as  follows  : 
For  the  convenience  of  the  mathematical  treatment  equation 

(12a)  of  Chapter  I,  namely, 

/—•-£*• 

_ 

pH  =  pKa  +  log 


is  rewritten  with  natural  logarithm  as  (1) 


pH  =  pKa  +  0.4343  In  —  —  (1) 

1  —  a 


The  derivative  is 


=  0.4343    —    d    -—  (2) 

a         \l  -  a) 

Whence 

=  2.303  a(l  -  a)  (3) 


da 
When  a  —  0.5,    ,         =  0.576.    This  value  is  the  maximum  ob- 


tained  by  a  univalent  acid. 


1 


56         THE  DETERMINATION  OF  HYDROGEN  IONS 

Now  under  limited  conditions,  explained  in  Chapter  I, 

_  Base  added  _  [B]  d[B] 

Total  acid   :=  [S]    J  ''    [S] 

Hence 

^r  =  2.303  «(1  -  «)  [S]  (4) 

Also 

Ka 


Ka  +  [H+] 
Hence 


For  brevity  ,/  J.  is  called  /3  by  Van  Slyke.     In  figure  15  equa- 
a(pJti) 

tion  (5)  is  used  to  obtain  part  of  the  curve  showing  the  relation 
of  /3  to  pH  in  the  cases  of  0.1  M  and  0.2  M  acetic  acid.  Equation 
(5)  gives  that  part  of  each  curve  shown  in  the  figure  by  the 
central,  peaked  portion  and  continued  as  dotted  curves  near 
pH  2  to  3.5.  In  the  region  lower  than  pH  3.5  correction  must  be 
made  for  the  buffer  effect  of  the  strong  acid.  Likewise  beyond 
pH  10  the  effect  of  a  strong  base  should  be  considered. 

These  additional  buffer  effects  are  calculated  as  follows. 

Consider  a  strong  base  added  to  water.  Assume  that  the  base 
is  completely  dissociated.  Then  d[B]  =  d[OH~]  and 

4B]  dIOH-] 


d(pH)       d  log  [OH-] 
Likewise  for  the  case  of  a  strong  acid  added  to  water  we  have : 

d[E]    =  2.303  [H+]  (7) 


II 


BUFFER   INDEX 


57 


The  buffer  effect  in  strong  acid  or  alkaline  solutions  is  the  sum  of 
these  two  effects;  i.e., 

d[B] 


rf(pH) 


=  2.303  ([H+]  +  [OH-]) 


(8) 


This  is  illustrated  in  figure  15. 

Between  pH  2  and  pH  3.5  a  resultant  of  the  /5  of  the  acetate 
system  and  the  (3  of  the  strong  acid  prevents  the  buffer  index 
from  falling  to  zero. 


0.12 


0.10 


0.08 


0.06 


0.04 


0.02 


0.00 


0.2 IT  acet.c  acid 


M   \\\ 


0.1  M  ace 


tic  acid 


/9-duetofel 


1         2         3        4        5        6        7        8        9        10       11        12       13 

pH 

dB 

FIG.  15.  VALUES  OF OR  /3  FOR  MIXTURES  OF  ACETIC  ACID  AND  ACETATE 

dpH 

(After  Van  Slyke  (1922)) 

For  further  details  see  the  original  articles  by  Van  Slyke  (1922), 
Koppel  and  Spiro  (1914)  and  Taufel  and  Wagner  (1926). 

One  very  distinct  advantage  in  the  use  of  Van  Slyke's  buffer 
values  arises  from  the  fact  that  the  buffer  values  of  various  com- 
ponent systems  of  a  complex  system  are  additive.  When  the 
individual  values  of  component  systems  can  be  precisely  formu- 
lated, much  can  be  predicted  of  complex  systems. 

A   FURTHER   REMARK   ON   STRONG   ELECTROLYTES 

The  reader  who  is  seeking  an  outline  of  our  subject  will  doubt- 
less be  willing  to  proceed  with  the  approximate  treatment  which 


58 


THE  DETERMINATION  OF  HYDROGEN  IONS 


was  accorded  strong  acids  at  the  close  of  Chapter  I  (page  34) 
and  to  postpone  a  reconsideration  of  the  effects  of  those  highly 
dissociating  salts  formed  by  the  addition  of  strong  bases  to  weak 
acids.  Since  it  has  been  intimated  that  the  simple  relations  pre- 
sented so  far  are  inapplicable  to  strong  acids  and  bases,  an  addi- 
tional remark  on  strong  electrolytes  may  be  appropriate  here, 
pending  the  development  in  later  chapters  of  more  suitable 
methods  of  approach  and  formulation. 

In  the  introductory  section  of  Chapter  I  brief  mention  was 
made  of  the  electronic  architecture  of  atoms  and  molecules. 
There  it  was  stated  that  certain  compounds  behave  as  if  one  of 


FIG.  16.  REPRESENTATION  OP  A  PORTION  OF  A  CRYSTAL  OF  SODIUM 

CHLORIDE 

Sodium  ion  represented  by  dots;  chloride  ion  by  circles 

the  component  atoms  has  completely  captured  the  valence  elec- 
tron or  electrons  of  the  other  component  with  the  result  that  the 
compound  is  virtually  an  association  of  ions.  For  example,  it  is 
believed  that,  whatever  may  be  the  orbits  of  the  electrons  in 
sodium  chloride,  the  chlorine  there  found  has  captured  an  elec- 
tron to  complete  its  own  octet,  while  the  sodium  has  lost  an  elec- 
tron. Consequently  the  sodium  chloride  molecule  might  be 
represented  by  (Na+,  Cl~)x.  Indeed  x-ray  analysis  of  the  crystal 
suggests  this.  An  interpretation  of  the  x-ray  "reflection  spectrum" 
of  sodium  chloride  crystals  yields  the  conclusion  that  the  sodium 
and  the  chloride  ions  are  arranged  as  shown  in  figure  16.  In  this 
picture  there  is  no  indication  of  the  molecule  NaCl  or  of  any 
"molecule"  short  of  the  crystal  as  a  whole.  There  is  only  evi- 
dence of  a  spatial  arrangement  which  can  reasonably  be  accounted 


II 


STRONG   ELECTROLYTES  59 


for  by  the  assumption  that  chloride  and  sodium  ions  are  each 
attracting  the  ions  of  opposite  charge  with  no  exclusive,  one-to- 
one  pairing.  A  variety  of  data  supports  this  view. 

When  the  components  of  the  crystal  are  dispersed,  as  in  water 
solution,  it  would  certainly  be  expected  that  the  only  discrete 
particles  persisting  as  individuals  would  be  the  sodium  and  the 
chloride  ions  (undoubtedly  combined  with  water  molecules). 
Indeed  evidence  has  been  molding  opinion  to  this  view  until  it 
is  rather  widely  although  not  universally  accepted.  Thus  many 
treatises  start  with  the  assumption  of  the  "complete  dissociation 
of  strong  electrolytes." 

This  view  by  no  means  excludes  the  persistence  of  the  attractive 
force  which  is  so  strongly  manifest  in  the  crystal.  The  operation 
of  this  force,  theoretically,  can  not  become  completely  negligible 
until  the  thermal  agitation  becomes  exceedingly  great  (infinite 
temperature)  or  the  dispersion  by  the  solvent  becomes  exceed- 
ingly great  (infinite  dilution).  In  short,  it  must  be  supposed  that 
at  any  given  concentration  of  the  sodium  chloride  solution,  and 
notwithstanding  the  thermal  agitation,  there  occur  situations  in 
which  a  sodium  ion  is  surrounded  by  more  chloride  ions  than  by 
sodium  ions  or  a  chloride  ion  is  surrounded  by  more  sodium  ions 
than  chloride  ions.  This  is  to  be  regarded  as  an  expression  of 
the  orienting  force. 

Thus  there  should  exist,  statistically,  groupings  very  different 
in  nature  from  the  sodium  chloride  molecule  specified  in  the 
classical  equation: 

[Na+]  [C1-] 
[NaCl] 

If  one  is  convinced  of  this,  he  might  say  that  an  attempt  to  apply 
the  above  equilibrium  equation  proceeds  in  ignorance  of  the 
nature  of  sodium  chloride  and  is  no  test  whatever  of  the  mass  law. 
With  this  interpretation  of  the  data  on  crystal  structure  and 
with  the  support  of  various  other  types  of  evidence  it  is  con- 
venient to  regard  salts  such  as  sodium  chloride,  and  also  acids 
such  as  HC1,  as  completely  ionized  in  solution  and  to  take  account 
of  the  constantly  changing  associations  of  the  ions  by  methods 
quite  different  from  those  which  are  employed  in  treating  the 
cases  where  true  molecules  are  probably  formed. 


60  THE   DETERMINATION   OF   HYDROGEN   IONS 

We  owe  to  Milner  and  particularly  to  Debye  and  Hiickel  the 
way  in  which  statistical  mechanics  may  be  applied  to  this  situa- 
tion. The  theory  is  outlined  in  Chapter  XXV.  However,  it 
should  be  well  understood  that  Debye  and  Hiickel  attempt  to 
take  account  only  of  the  effect  of  the  electrical  forces  between  the 
oppositely  charged  ions  and  that  their  theory  has  nothing  to  say 
about  several  other  factors  which  may  interfere  with  the  applica- 
tion of  the  postulates  entering  the  derivation  of  the  simple,  ideal, 
equilibrium  equation.  Since  these  factors  are  many  and  varied, 
it  may  be  said  that  the  student  has  the  choice  of  attempting  the 
impracticably  rigid  all  at  once  or  of  setting  up  an  ideal  as  a  guiding 
principle  in  some  such  way  as  that  which  we  have  here  attempted. 

There  is,  however,  another  way  of  approaching  the  subject. 
We  shall  see  that  some  of  the  methods  to  be  described,  notably 
that  of  the  hydrogen  electrode,  are  methods  which  measure 
energy  changes.  It  is  sometimes  assumed  that  there  is  some 
definite  relation  between  two  concentrations  of  hydrions  and  the 
energy  necessary  to  bring  a  mole  of  hydrions  from  one  of  the 
given  concentrations  to  the  other.  In  this  assumption  trouble 
begins.  It  could  be  avoided  if  we  were  content  not  only  to  leave 
the  results  of  the  measurement  in  terms  of  energy  changes  but 
also  to  formulate  equilibrium  conditions  in  these  same  terms  and 
to  eschew  the  employment  of  equations  cast  in  terms  of  concentra- 
tion. Since  current  thought  is  not  yet  wholly  receptive  to  the 
extreme  of  this  method  of  formulation  we  have  the  rather  interest- 
ing situation  that  the  so-called  rigid  formulations  of  the  day  are 
fundamentally  those  of  the  energy  changes,  but  there  is  introduced 
a  term,  called  the  activity,  which  has  been  rather  inaccurately 
described  as  a  sort  of  corrected  concentration. 

In  place  of  the  equation 


[HA] 

where  []  represents  concentration,  there  is  used  the  equation 

(H+)  (A~) 
(HA) 

where  ()  represents  "activity." 

Then  the  equations  reduce  to  the  forms  we  have  been  using 


II  SIGNIFICANCE    OF   pH  61 

but  with  "activity"  replacing  "concentration."  Formulation  by 
"activity"  is  a  defined  application  of  rigid  thermodynamics  but 
the  value  of  the  activity  of  a  substance  varies  with  every  change 
of  condition  and  practically  makes  concrete  knowledge  of  the 
details  largely  empirical.  Formulation  by  concentration  is  an 
idealistic  application  of  molecular  theory  but  then  the  equilibrium 
"constant"  varies  with  every  change  of  condition  and  again  the 
detail  remains  largely  a  matter  of  empiricism. 

We  shall  proceed  with  "concentrations"  and  molecular  theory 
and  shall  return  in  due  time  to  a  consideration  of  energy  changes. 

THE   SIGNIFICANCE   OF   CERTAIN   pH   VALUES 

There  is  no  hesitation  in  attributing  a  significance  of  actuality 
to  hydrion  concentrations  arising  from  the  dissociation  of  strong 
acids.  There  is  little  disposition  to  question  the  essential  reality 
of  hydrion  concentrations  arising  from  the  dissociation  of  moder- 
ately weak  acids.  However,  there  is  good  reason  to  doubt  the 
physical  significance  of  hydrion  concentrations  said  to  be  of  the 
magnitude  of  10~7N,  10~13N,  etc. 

We  shall  postpone  a  discussion  of  this  very  pertinent  question 
to  a  later  chapter  because  there  will  then  be  an  opportunity  to 
include  material  discussed  in  the  intervening  chapters.  We  may 
here  state  that  if  the  questioned  values  be  considered  as  numbers, 
they  serve  admirably  and  conveniently  as  indices  to  states  of 
equilibrium  among  relatively  large  quantities  of  materials.  If 
the  doubting  reader  is  not  content  to  accept  this  for  the  moment 
as  a  dogma,  he  should  at  once  read  the  first  part  of  Chapter 
XXVII. 


CHAPTER  III 

OUTLINE  OF  A  COLORIMETRIC  METHOD 

In  a  short  time  you  will  improve,  my  friend, 
When  of  scholastic  forms  you  learn  the  use; 
And  how  by  method  all  things  to  reduce. 

Mephistopheles  to  the  Student  in  Goethe's  Faust. 

While  the  word  "indicator"  can  have  various  meanings,  —  as 
current  indicator,  pressure  indicator,  etc.,  —  we  shall  use  it  as  a 
generic  name  for  substances  which  "change  color"  when  the  pH 
values  of  their  solutions  change. 

We  shall  postpone  to  a  later  chapter  a  closer  analysis  of  what 
is  meant  by  "change  of  color"  and  shall  use  the  expression  as  it  is 
commonly  understood. 

Each  indicator  exhibits  color-change  within  a  characteristic 
zone  of  pH.  We  shall  consider  here  only  those  indicators  which 
have  one,  or  at  most  two,  characteristic  zones.  Beyond  one 
indefinite  edge  of  such  a  zone  one  characteristic  color  appears. 
Beyond  the  other  indefinite  edge  the  other  characteristic  color 
appears.  Within  the  zone,  the  color  may  be  treated  as  if  it  were 
a  mixture  of  the  two  characteristic  colors.  Because  the  edges  of 
the  zone  are  indefinite  the  color  or  color  mixture  in  the  center  of 
the  pH-zone  constitutes  a  useful  point  of  reference.  The  value 
of  pH  at  the  50  per  cent  transformation  is  called  the  indicator's 
pK  value.  This  originates  in  the  use  of  the  equation 


and  in  the  treatment  of  the  indicator  as  a  simple  acid. 

The  color  chart  is  useful  as  a  crude  representation  of  the  colors 
of  various  indicators  at  various  values  of  pH.  The  pK  values 
are  indicated. 

The  color  chart  exhibits  only  intermediate  colors.  When  the 
pH  value  of  a  solution  containing  any  one  indicator  is  lower  than 
the  pK  value  by  about  2  units  pH,  what  is  conveniently  called 

62 


Ill  OUTLINE   OF   COLORIMETRIC   METHOD  63 

the  "acid  color"  appears.  When  the  pH  value  of  the  solution  is 
greater  than  the  pK  value  of  the  indicator  by  about  2  units  pH, 
what  is  conveniently  called  the  "alkaline  color"  appears.  "Acid" 
and  "alkaline"  used  in  this  sense  have  no  reference  to  a  line  of 
demarkation  between  "acid"  and  "alkaline"  solutions.  Theory 
associates  the  "acid  color"  with  the  "acid-form"  and  the  "alkaline- 
color"  with  the  "alkaline-form"  of  the  indicator  substance. 
These  terms  are  conveniences. 

In  ordinary  titrations  (see  Chapter  XXVIII)  conditions  are 
so  chosen  that  when  the  "end-point"  of  the  titration  is  reached 
the  pH,  value  of  the  solution  plunges  through  the  entire  range  of 
the  indicator's  color  transformation.  A  pronounced  change  of 
color  occurs  on  the  addition  of  a  very  small  amount  of  acid  or 
alkali.  The  intermediate  colors  even  if  observed  are  not  em- 
phasized. However,  the  intermediate  colors  are  important  to 
our  present  purpose. 

They  can  be  maintained  by  buffer  solutions  which  maintain 
constant  values  of  pH.  Thereby  reference  standards  may  be 
prepared.  Standard  buffer  solutions  are  described  in  Chapter  IX. 
In  their  use  it  is  essential  to  remember  that  the  buffer  solution 
controls  only  the  ratio1  between  the  concentrations  of  "acid" 
and  the  "alkaline"  color-forms  of  the  indicator.  Therefore  the 
preparation  of  a  standard  color  tube  to  be  judged  by  eye  includes 
the  use  of  a  definite  concentration  of  indicator  substance  and  ob- 
servation through  a  definite  depth  of  solution. 

Suppose  that  the  phosphate-buffers  are  employed  in  the  range 
pH  6.0  to  pH  7.0  with  the  indicator  brom  thymol  blue.  If  these 
standards  are  to  be  used  in  comparison  with  an  unknown  solution 
it  is  essential,  not  that  any  particular  amount2  of  indicator  be 
used,  but  that  the  same  concentration  be  used  in  both  standard 
and  unknown.  It  is  furthermore  essential  that  standard  and  un- 
known be  observed  through  equal  depths  of  solution.  It  is  then 

1  If  instead  of  the  ratio  for  the  two  color  forms  we  use  the  ratio  of  the 
concentration  of  the  alkaline  color-form  to  the  concentration  of  total 
indicator  we  may  call  this  a  and  use  the  equation 

pH  =  pKa  +  log  — - — 

1    —    OL 

8  The  amount  becomes  very  important  in  studying  poorly  buffered  solu- 
tions. See  page  190. 


64          THE  DETERMINATION  OF  HYDROGEN  IONS 

clear  that,  if  standard  and  unknown  have  produced  the  same  ratio 
of  the  two  color-forms  of  the  indicator,  the  appearance  of  the 
two  tubes  will  match.  The  first  approximation  of  the  theory 
concerned  is  that  equal  ratios  of  the  two  indicator  forms  will  be 
produced  by  solutions  of  the  same  pH  value.  Therefore,  if  the 
color  of  the  unknown  match  that  of  standard  "pH  6.6"  it  is  pre- 
sumed that  the  pH  value  of  the  unknown  is  6.6. 

In  case  the  approximate  value  of  the  unknown  is  undetermined 
a  preliminary  test  may  be  made  as  follows.  The  indicator  brom 
thymol  blue  will  differentiate  solutions  having  pH  values  greater 
or  less  than  7.0.  If  then,  a  drop  or  two  of  brom  thymol  blue 
gives  a  distinctly  yellow  color  one  knows  that  the  solution  has  a 
pH  value  less  than  about  5.6.  Imagine  that  brom  cresol  green 
is  next  tried  and  that  there  is  found  an  intermediate  color  suggest- 
ing to  the  memory  pH  4.4  or  4.6.  Standards  for  this  range  are 
set  up  with  phthalate  buffers  (table  35)  or  citrate  buffers  (table  39) 
and  brom  cresol  green.  The  standards  are  compared  with  the 
unknown.  It  is  remembered  that  equality  of  concentrations  and 
views  through  equal  depths  are  essentials.  Suppose  color  match 
is  not  perfect  at  "4.4"  or  at  "4.6"  but  that  the  unknown  appears 
as  if  it  would  match  an  intermediate  between  standard  "4.4" 
and  "4.6."  Unless  extreme  accuracy  is  desired  4.5  may  be  said 
to  be  the  value  for  the  solution  under  measurement. 

In  case  an  extensive  set  of  standards  is  set  up  it  is  well  to 
employ  volumes,  etc.,  systematically.  Thus,  10  cc.  of  each  buffer 
are  added  seriatim  to  each  of  a  set  of  uniform  test  tubes  and  to 
each  of  these  are  added  5  drops  of  a  stock  solution  of  the  proper 
indicator.  Mixing  should,  of  course,  be  insured.  Now  when  an 
unknown  is  to  be  compared,  10  cc.  of  this  solution  are  placed  in 
a  tube  of  the  same  bore  as  those  of  the  standards  and  5  drops  of 
the  stock  indicator  solution  are  added  and  mixed.  Change  of 
stock  solution  is  obviously  inadvisable. 

When  one  is  familiar  with  the  colors  of  the  indicators  at  known 
pH  values,  very  fair  estimations  may  be  made  without  the  aid 
of  the  standards;  but  there  is  no  way  as  satisfactory  as  the 
setting  up  of  the  standards  for  the  establishment  of  a  correct 
impression  of  the  relations  of  the  various  indicators  on  the  pH 
scale.  On  the  other  hand;  the  author  has  discovered  in  his 


Ill  COLOR   CHART  65 

conversations  that  there  are  many  investigators  who  would  like 
to  use  indicators  for  the  occasional  rough  measurement  of  pH 
but  who  are  discouraged  by  a  pressure  of  work  which  prevents 
them  from  taking  the  time  to  carefully  prepare  the  standard 
solutions.  To  furnish  such  investigators  with  a  demonstration  of 
the  general  relations  of  the  various  indicators  and  to  furnish 
rough  standards  the  attempt  has  been  made  to  reproduce  the 
colors  in  figure  17. 

It  must  be  remembered,  however,  that  in  undertaking  a  repro- 
duction by  means  of  the  printer's  art  the  publishers  are  to  be 
commended  for  their  courage  and  are  not  to  be  held  responsible 
for  the  inadequacy  of  the  result.  Aside  from  the  inherent  dif- 
ficulty in  freeing  a  printed  color  from  the  effect  of  the  vehicle, 
there  remains  the  utter  impossibility  of  reproducing  with  paper 
and  ink  the  effect  observed  in  a  liquid  solution.  The  funda- 
mental phenomena  are  quantitatively  very  different  in  the  two 
cases.  Therefore,  the  user  of  the  chart  of  colors  will  have  to 
use  discretion  and  some  imagination.  If  he  does  not  attempt 
to  .make  the  reproductions  take  the  place  of  the  standards  he 
should  find  them  useful  for  class  room  demonstrations,  for  refresh- 
ing the  memory  and  for  rough  standards. 

For  class-room  work  it  is  advantageous  to  show  the  position 
of  the  several  indicators  on  the  pH  scale  by  cutting  the  chart  and 
relining  each  series  so  that  corresponding  pH  values  overlap. 

Many  users  of  the  color  chart  have  not  only  failed  to  note  the 
warning  given  above  in  previous  editions  of  this  book  but  have 
failed  to  realize  how  the  best  use  may  be  made  of  the  chart. 
By  certain  mechanical  improvements  in  the  art  of  production  the 
gradation  of  the  color  has  been  improved.  This  feature  serves 
as  a  very  helpful  guide.  Too  much  emphasis  should  not  be 
placed  upon  the  color  quality.  These  brief  reminders  give  re- 
lease to  the  exercise  of  judgment  which  is  all  that  the  chart  can  aid. 

In  each  case  the  colors  were  designed  to  match  standards  in 
tubes  16  mm.  internal  diameter  containing  10  cc.  of  buffer  solu- 
tions and  the  following  proportions  of  indicators. 

Thymol  blue  (T.B.  ac)  1.0  cc.  0.04  per  cent  solution 
Brom  phenol  blue  (B.P.B.)  0.5  cc.  0.04  per  cent  solution 
Brom  cresol  green  (B.C.G.)  0.5  cc.  0.04  per  cent  solution 


66  THE   DETERMINATION   OF   HYDROGEN   IONS 

Chlor  phenol  red  (C.P.R.)  0.5  cc.  0.04  per  cent  solution 
Brom  cresol  purple  (B.C.P.)  0.5  cc.  0.04  per  cent  solution 
Brom  thymol  blue  (B.T.B.)  0.5  cc.  0.04  per  cent  solution 
Phenol  red  (P.R.)  0.5  cc.  0.02  per  cent  solution 

Cresol  red  (C.R.)  0.5  cc.  0.02  per  cent  solution 

Meta  cresol  purple  (M.C.P.)  0.5  cc.  0.04  per  cent  solution 
Thymol  blue  (T.B.)  0.5  cc.  0.04  per  cent  solution 


CHAPTER  IV 

CHOICE  OF  INDICATOKS 

We  are  now  forced  to  increase  the  number  of  compounds,  not  merely 
in  order  to  prepare  new  substances,  but  to  discover  natural  laws. — 
R.  FITTIG. 

From  the  enormous  number  of  colored  compounds  found  in 
nature  and  among  the  products  of  the  laboratory  many  have 
been  called  into  use  as  acidimetric-alkalimetric  indicators.  Few 
have  been  chosen.  Among  indicators  of  plant  origin  litmus  and 
alizarine  are  the  more  familiar.  One  indicator  of  animal  origin, 
cochineal,  an  extract  of  an  insect,  was  formerly  used  to  some  ex- 
tent. Walpole's  (1913)  treatment  of  litmus,  Walbum's  (1913) 
study  of  the  coloring  matter  of  the  red  cabbage  and  some  of  the 
more  recent  work,  have  given  us  some  data  on  properties  of  plant 
and  animal  pigments  which  are  applicable  to  hydrogen  ion  deter- 
minations. But  for  the  most  part  indicators  of  natural  origin 
have  been  neglected  for  the  study  of  "synthetic"  compounds. 

Litmus  has  played  so  important  a  role  in  acidimetry  that  it  is 
worthy  of  brief,  special  mention. 

litmus  is  obtained  by  the  oxidation  in  the  presence  of  ammonia 
of  the  orcin  contained  in  lichens,  generally  of  the  species  Roccella 
and  Lecanora.  The  material  which  comes  upon  the  market  is 
frequently  in  the  form  of  cubes  composed  of  gypsum  or  similar 
material  and  comparatively  little  of  the  coloring  matter.  The 
coloring  matter  is  a  complex  from  which  there  have  been  isolated 
many  compounds,  chief  among  which  are  azolitmin,  erythrolitmin, 
erythrolei'n  and  spaniolitmin.  Of  these  the  azolitmin  is  the 
most  important.  Scheitz  (1910)  found  the  azolitmin  of  com- 
merce to  be  of  uncertain  composition  and  it  may  well  be  so  now, 
for  the  composition  of  the  crude  material  varies  with  the  source 
and  with  the  extent  of  the  complex  action  of  air  and  alkali  on  the 
original  materials. 

The  following  method  of  preparing  a  sensitive  litmus  solu- 
tion is  taken  from  Morse  (1905). 

67 


68          THE  DETERMINATION  OF  HYDROGEN  IONS 

The  crushed  commercial  litmus  is  repeatedly  extracted  with  fresh  quan- 
tities of  85  per  cent  alcohol  for  the  purpose  of  removing  a  violet  coloring 
matter  which  is  colored  by  acids  but  not  made  blue  by  alkalies.  The  resi- 
due, consisting  mainly  of  calcium  carbonate,  carbonates  of  the  alkalies 
and  the  material  to  be  isolated,  is  washed  with  more  hot  alcohol  upon  a 
filter  and  then  digested  for  several  hours  with  cold  distilled  water.  The 
filtered  aqueous  extract  has  a  pure  blue  color  and  contains  an  excess  of 
alkali,  a  part  of  which  is  in  the  form  of  carbonate  and  a  part  in  combination 
with  litmus.  To  remove  the  alkaline  reaction  the  solution  is  heated  to 
the  boiling  point  and  cautiously  treated  with  very  dilute  sulfuric  acid 
until  it  becomes  very  distinctly  and  permanently  red.  Boil  till  all  CO2 
is  dispelled.  Treat  with  a  dilute  solution  of  barium  hydroxide  until  the 
color  changes  to  a  violet.  Filter,  evaporate  to  a  small  volume  and  pre- 
cipitate the  litmus  with  strong  alcohol.  Wash  with  alcohol  and  dry. 

Dr.  P.  Rupp  (private  communication)  prefers  to  make  a  final 
washing  with  water  which  removes  much  of  the  salt  at  the  expense 
of  some  dye. 

"Synthetic"  indicators  have  for  the  most  part  displaced  those 
of  natural  origin  until  litmus  and  alizarin,  turmeric  and  cochineal 
are  becoming  more  and  more  unfamiliar  in  the  chemical  labora- 
tory. Indeed  Bjerrum  (1914)  states  that  the  two  synthetic  indi- 
cators, methyl  red  and  phenolphthalein,  particularly  because  of 
the  zones  of  hydrogen  ion  concentration  within  which  they  change 
color,  are  sufficient  for  most  titrimetric  purposes. 

But  the  two  indicators  mentioned  above  cover  but  a  very  lim- 
ited range  of  hydrogen  ion  concentration  so  that  they  are  insuf- 
ficient for  the  purpose  we  now  have  under  consideration.  A  sur- 
vey of  indicators  suitable  for  hydrogen  ion  determinations  was 
opened  in  Nernst's  laboratory  in  1904  by  Salessky.  This  survey 
was  extended  in  the  same  year  by  Friedenthal,  by  Fels  and  by 
Salm  and  the  results  were  summarized  in  Salm's  famous  table 
(cf.  Z.  physik.  Chem.,  57,  471). 

Then  came  the  classic  work  of  S0rensen  (1909)  of  the  Carlsberg 
laboratory  in  Copenhagen.  The  array  of  available  indicators  had 
become  so  large  as  to  be  burdensome.  S0rensen  in  an  extensive 
investigation  of  the  correspondence  between  colorimetric  and 
electrometric  determinations  of  hydrogen  ion  concentrations  re- 
vealed discrepancies  which  were  attributed  mainly  to  the  in- 
fluence of  protein  and  salts.  He  chose  those  indicators  which 
were  relatively  free  from  the  so-called  protein  aiid  salt  errors, 
constructed  solutions  of  known  and  reproducible  hydrogen  ion  con- 


IV  INDICATOR   HISTORY  69 

centrations  and  thus  furnished  the  biochemist  with  selected  tools 
of  beautiful  simplicity.  It  is  well  to  emphasize  the  labor  of 
elimination  which  S0rensen  performed  because  without  it  we 
might  still  be  consulting  such  tables  as  that  published  by  Thiel 
(1911),  or  the  ponderous  table  8,  pages  76-86,  and  be  bewildered 
by  the  very  extensive  array. 

S0rensen's  work,  coupled  as  it  was  with  a  most  important  con- 
tribution to  en'zyme  chemistry,  gave  great  impetus  to  the  use  of 
indicators  in  biochemistry.  His  selection  was,  therefore,  soon 
enlarged  by  additions  of  new  indicators  which  fulfilled  the  criteria 
of  reliability  which  he  had  laid  down.  Alpha  naphthol  phthalein, 
a  compound  first  synthesized  by  Grabowski  (1871),  was  shown  by 
S0rensen  and  Palitzsch  (1910)  to  have  a  range  of  pH  7-9  and  was 
found  useful  in  biological  fluids.  Methyl  red  (Rupp  and  Loose, 
1908)  was  given  its  very  useful  place  by  the  investigations  of 
Palitzsch  (1911).  Henderson  and  Forbes  (1910)  introduced  2-5 
dinitrohydroquinone  as  an  indicator  possessing  several  steps  of 
color  change  and  therefore  useful  over  a  wide  range  of  pH. 
Walpole  (1914)  called  attention  to  several  indicators  of  potential 
value.  Hottinger  (1914)  recommended  "lacmosol,"  a  constituent 
of  lacmoid,  and  Bogert  and  Scatchard  (1916)  advocated  the  use 
of  dinitrobenzoylene  urea. 

Lund  (1927)  and  Kolthoff  (1927)  report  some  data  obtained 
with  certain  very  interesting  indicators  of  the  triphenyl  methane 
series.  These  indicators  are  colored  in  acid  solution  and  color- 
less in  alkaline  solution.  They  are  numbers  99a,  99b  and  102a 
of  table  8.  No.  102a  is  described  as  requiring  a  time  interval  for 
the  color  change.  The  others  are  described  as  useful  for  a  variety 
of  purposes.  Their  unique  color  changes  should  be  of  service 
in  some  cases. 

Additions  continue  to  be  made  every  little  while;  sometimes 
with  accompanying  data  of  value  to  our  subject.  Only  the  cases 
for  which  pH  measurements  of  some  kind  are  available  can  be 
included  in  the  following  tables.  For  this  reason  the  tables  do 
not  include  those  vast  arrays  of  material  waiting  to  be  explored. 

In  1915  Levy,  Rowntree  and  Marriott,  without  applying  the 
tests  of  reliability  which  S0rensen  had  employed,  used  phenol 
sulphonphthalein  in  determining  the  pH  of  the  dialyzate  of 
blood.  This  compound,  first  synthesized  in  Remsen's  laboratory 


70          THE  DETERMINATION  OF  HYDROGEN  IONS 

by  Sohon  (1898),  received  considerable  attention  from  Acree  and 
his  co-workers  because  it  furnished  excellent  material  for  the 
quinone-phenolate  theory  of  indicators.  To  further  such  studies 
Acree  and  White  had  synthesized  new  derivatives  of  phenol 
sulphonphthalein  at  the  time  when  the  work  of  Levy,  Rowntree 
and  Marriott  attracted  the  attention  of  Clark  and  Lubs.  The 
latter  were  looking  for  more  brilliant  indicators  for  use  in  bacterial 
culture  media  and  were  attracted  by  the  well  known  brilliance 
of  phenol  sulphonphthalein.  Through  the  courtesy  of  Professor 
Acree  some  of  the  derivatives  which  White  had  prepared  were 
obtained.  Many  new  homologs  were  synthesized  by  Lubs. 
There  was  then  undertaken  an  extensive  study  of  the  applica- 
bility of  these  and  numerous  other  indicators  to  the  study  of 
biological  fluids  and  of  bacterial  culture  media  in  particular.  See 
Clark  and  Lubs  (1916-1917).  They  finally  selected  a  series  of 
indicators  which,  for  the  most  part,  was  made  up  of  sulfon- 
phthaleins.  Two  azo  compounds  were  included,  methyl  red 
(cf.  Palitzsch,  1911)  and  propyl  red  (Clark  and  Lubs,  1915). 
Propyl  red  precipitates  too  easily  from  buffer  solutions  and  was 
soon  discarded.  Methyl  red  continued  in  the  series  until  the 
work  of  Cohen  (1922)  [see  especially  Cohen's  paper  of  1927]  made 
available  several  new  sulfonphthaleins. 

In  the  course  of  their  investigations  Clark  and  Lubs  resurrected 
ortho  cresol  phthalein  (Baeyer  and  Fraude,  1880),  found  it  quite 
as  reliable  as  phenolphthalein  and  more  brilliant  with  a  color 
better  adapted  to  titrations  in  artificial  light. 

In  spite  of  the  fact  that  S0rensen  rejected  the  greater  number 
of  the  indicators  which  he  studied  and  that  Clark  and  Lubs,  after 
a  resurvey  of  the  subject  and  the  preparation  of  many  new  com- 
pounds, listed  but  few  indicators  as  reliable,  there  has  recently 
appeared  a  tendency  to  resurrect  the  rejects.  Many  of  these 
are  useful  in  special  cases  and  undoubtedly  there  is  an  occasional 
individual  to  be  found  in  the  lists  which  has  been  insufficiently 
studied  and  unjustly  rejected.  Nevertheless,  the  indiscriminate 
use  of  miscellaneous  indicators  may  lead  to  gross  errors  or  at 
least  to  such  a  diversity  of  data  that  their  correlation  will  become 
complex  during  the  coming  period  when  the  specific  salt-effects 
and  general  conduct  of  the  individual  indicators  are  still  being 
determined. 


IV  SELECTED   INDICATORS  71 

It  is,  therefore,  advisable  to  use  the  more  thoroughly  studied 
indicators.  Three  lists  of  these  are  given  (tables  10,  11,  and  12). 
The  indicators  therein  listed  should  suffice  for  all  ordinary  needs. 
S0rensen's  list  is  given  in  table  10  and  to  this  are  appended  S0ren- 
sen's  comments.  For  general  purposes  the  indicators  named 
in  table  11  will  be  found  the  most  satisfactory  especially  because 
of  their  brilliancy.  Each  of  these,  however,  has  its  own  special 
limitations  as  every  indicator  has.  For  the  study  of  colorless 
solutions  where  salt  errors  are  to  be  reduced  the  nitrophenols 
listed  in  table  12  should  be  valuable. 

In  table  8  are  a  few  indicators  which  are  undoubtedly  reliable 
but  little  used,  a  few  which  are  definitely  unreliable  though  often 
used,  and  very  many  of  uncertain  character  and  for  the  most  part 
bearing  the  stamp  of  disapproval  by  competent  judges.  Since 
the  indicators  in  tables  10,  11  and  12  cover  all  ordinary  require- 
ments it  seems  hardly  worth  while  to  venture  upon  an  analysis 
of  table  8  except  to  note  by  a  star  one  or  another  compound 
which  seems  promising  or  has  received  more  or  less  careful  study. 

TYPE    STRUCTURES 

Since  it  is  impractical  to  give  structural  formulas  for  all  the 
indicators  of  the  general  list  (table  8),  a  few  typical  structures 
will  be  given  as  guides.  The  grouping  in  table  7  is  that  of  table  8 
and  the  numbers  are  the  index  numbers  of  table  8. 

COMMENTS  ON  THE  GENERAL  LIST 

Table  8  is  taken  from  International  Critical  Tables,  Clark  (1926) . 
A  few  additions  have  been  made.  The  lists  on  which  it  is  based 
were  originally  compiled  with  the  aid  of  Dr.  Barnett  Cohen  and 
Dr.  Elias  Elvove  with  several  purposes  in  view.  In  the  first 
place  there  exist  in  the  older  literature  a  great  many  observations 
recorded  in  terms  of  the  color  of  a  given  indicator.  These  data 
can  often  be  translated  into  modern  terms  if  the  pH  range  of  the 
given  indicator  is  known.  In  the  second  place  there  are  circum- 
stances when,  for  one  reason  or  another,  it  becomes  necessary 
to  draw  upon  the  list  of  miscellany.  It  should  therefore  be  avail- 
able. Lastly,  and  perhaps  most  important,  our  review  of  the 
literature  and  of  indicator  labeling  has  shown  that  there  is  great 
confusion;  and  an  initial  step  in  the  clarification  of  the  subject 


TABLE  7 
Type  structures  shown  by  examples 


EXAMPLES 

GE  NERAL  STRUCTURE 

Nitro  group 

12. 

p-Nitro  phenol 

HO^       ^>NO2 

16. 

Nitramine  ; 
2,4,  6-trinitrophenyl- 
methyl-nitroamine 

O,N<^      ^>N(  J 

Mono-azo  group 

44.  Methyl  orange; 

p-benzenesulfonic  acid- 
azo-dimethylaniline 

59.  Methyl  red; 

o-carboxybenzene-azo- 
dimethylaniline 


<(        )>-N=N-<(        ^> 
C02H 


Dis-azo-group 


87.  Congo  red; 

Diphenyl-disazo-bis-o:- 
naphthylamine-4-sul- 
fonic  acid 


-<^        ^>N= 


NH 


Triphenylmethane  group 


97.  Methyl  violet  6B  (penta- 
methyl  constituent) 


72 


TABLE  7— Continued 


GENERAL  STRUCTURE 


Phthalein  group 


120.  Phenol  phthalein; 

dihydroxyphthalophenone 


•o 


H 


OH 


c 


vo 


Sulfonphthalein  group 


142.  Phenol  red 


C 


OH 


O 


Quinoline  group 


151.  Quinoline  blue; 

1 , 1  '-di-iso-amyl-4, 4'- 
quinocyanine  iodide 


-N  =C-  N— 


\. 


H 


Indophenol  group 


152.  Indophenol; 

Benzenone-indo-phenol 


Azine  group 


158.  Neutral  red; 

Amino-dimethylamino- 
toluphenazonium 
chloride 


H3C 


N(CH3)2C1 


Oxaiiine  group 


160.  Alizarine  green  B; 

Dihydroxy-dinaphthaz- 
oxonium  sulfonate 


73 


74 


THE    DETERMINATION    OF   HYDROGEN   IONS 
TABLE  7— Concluded 


GENERAL  STRUCTURES 


Anthraquinone  group 


O 

H       OH 

166.  Alizarin; 

/v  Y>H 

1  ,  2-dihydroxy-anthra- 

quinone  ; 

SA  A/ 

c 

0 

Indigo  group 

0 

II 

0 

168.  Indigo  carmine; 
Indigotin-5,5'  disulfonic 

C 
HOsS^V  \ 

/C\/\SO,H 

acid 

U\  /c~c" 

\  /  V 

N 
H 

H 

will  be  taken  if  there  is  available  a  tabulation  of  existing  data  to 
serve  as  a  basis  for  revision. 

In  examining  a  large  collection  of  indicators  the  labeling  was 
found  to  be  insufficient  in  a  large  percentage  of  cases.  On  study- 
ing the  literature  we  find  evidence  that  others  have  encountered 
the  same  difficulty  without  stating  so,  for  in  many  instances  the 
indicator  names  given  were  evidently  provided  by  one  or  another 
dealer  who  cared  so  little  for  the  scientific  uses  of  his  commodity 
that  he  left  from  the  label  the  designation  essential  to  its  identifica- 
tion. This  habit  had  become  more  or  less  prevalent.  In  some 
instances  our  own  uncertainty  may  be  due  to  an  arbitrary  ad- 
herence to  the  nomenclature  found  in  various  editions  of  Schultz. 
For  instance  when  we  see  the  indicator  croce'ine  listed  and  refer 
to  Schultz  (1914)  we  find  four  croce'ines  with  various  distinguish- 
ing marks  and  seven  other  compounds  for  the  names  of  which 
"croce'ine"  is  used  in  one  or  another  combination.  Eut  Schultz 
lists  no  croce'ine.  We  are  not  helped  in  going  back  to  the  lists 
of  Schultz  and  Julius  (1902).  Now  we  might  assume  that 


IV  INDICATOR   LABELING  75 

"croceme"  was  used  in  Salm's  table  as  a  term  having  a  definite 
meaning  outside  the  dye  industry.  On  this  principle  we  should 
find  that  "helianthine"  has  been  employed  in  accordance  with 
scientific  usage.  However  we  find  that  an  old  sample  of  helian- 
thine from  Salm's  dealer  is  not  the  helianthine  of  methyl  orange 
but  corresponds  in  pH-range  to  Salm's  Helianthine  I,  which, 
together  with  Salm's  Helianthine  II  we  have  not  identified. 

There  are  other  difficulties  such  as  are  illustrated  by  the  case 
of  Tropaeolin  OOO  No.  1  and  Tropaeolin  000  No.  2.  No.  1  is 
prepared  from  p-sulfanilic  acid  and  a-naphthol.  No.  2  is  prepared 
from  p-sulfanilic  acid  and  (3-naphthol.  In  this  there  is  agreement 
by  Schultz  and  Julius  1902,  Green  1904  and  Beilstein  (third  edition). 
In  accord  with  this,  S0rensen  describes  his  a-naphthol  prepara- 
tion as  Tropaeolin  000  No.  1.  In  the  second  edition  of  Indi- 
cators and  Test  Papers,  Cohn  (1914)  has  given  synonyms  for  the 
a  and  0  compounds  which  agree  with  Green,  but  has  reversed 
the  No.  1  and  No.  2  at  the  headings  of  his  descriptions  and  uses 
"No.  1"  and  "No.  2"  inconsistently  in  the  text,  Prideaux  (1917) 
has  called  the  /3  compound  Tropaeolin  000  and  gives  the  range 
as  7.6-8.9,  which  looks  suspiciously  like  S0rensen's  7.6-8.9  for 
the  a  compound.  Prideaux  uses  the  synonym  Orange  II  for  the 
j8  compound  in  harmony  with  Green;  but  on  the  next  page  de- 
scribes the  a  compound  as  Orange  II.  The  identity  of  Salm's 
Tropaeolin  000  is  not  clear.  It  was  evidently  different  from 
the  Tropaeolin  000  No.  1  used  by  S0rensen.  We  find  that  an 
old  sample  with  the  label  "Tropaeolin  000"  agrees  with  neither 
S0rensen's  nor  Salm's  data. 

Many  other  instances  might  be  cited  to  show  the  confused 
state  of  the  subject.  Because  it  is  serious  the  reader  will  have  to 
use  the  following  tables  with  caution,  and  he  need  not  be  sur- 
prised if  a  sample  of  indicator  which  he  tests  does  not  give  a 
pH  range  corresponding  to  that  recorded.  Since  the  publication 
of  the  list  in  the  second  edition  only  one  person  has  called  our 
attention  to  a  correction.  In  this  case  the  information  was  oral 
and  unverified  and  hence  is  not  applied.  Established  corrections 
will  be  welcome. 


TABLE  8 

General  list  of  indicators 
After  Clark  (1926) 

The  following  list  of  indicators  includes  all  those  for  which  data  on  the 
pH-ranges  have  been  found.  Many  of  the  data  of  this  table  are  to  be 
regarded  with  caution,  because  in  some  cases  the  names  proposed  are 
inadequate  for  complete  ^identification,  and  in  other  cases  names  have 
been  given  to  materials  of  uncertain  composition. 

The  Schultz  (S )  and  Rowe  (R....)  numbers  are  taken  from  the 

1923  and  1924  editions,  respectively,  of  these  works.  Delicate  shades  of 
meaning  in  the  color  nomenclature  have  been  avoided,  as  data  regarding 
the  purity  of  the  compounds  have  often  been  lacking.  The  abbreviations 
used  are  as  follows:  b,  blue;  br,  brown;  c,  colorless;  f,  fades;  fl,  fluorescent; 
g,  green;  o,  orange;  p,  pink;  pu,  purple;  r,  red;  v,  violet;  y,  yellow.  pK 
is  the  pH  at  which  there  is  an  apparent  half-transformation  of  the  indicator. 
*  indicates  that  the  indicator  has  been  studied  in  sufficient  detail  to  be 
used  in  supplementing  the  lists  of  tables  10,  11  and  12. 


INDEX 

NUM- 
BER 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Nitro  compounds 


1 

2,4,6-trinitrophenol;  Picric  acid 
[S  5;  R  7] 

c    0  0-  1  3  y 

C15  21) 

2 
3 

2,6-dinitrophenol  [Michaelis'  ft]  .  . 
2,4-dinitro-a-naphthol;         Man- 
chester vellow  [S.  6;  R.  9]    ... 

c    2.0-  4.0y 
v    2  0-  4  0  v 

(15,  20,  21) 
(3a) 

4 

4a 

2,  4-dinitrophenol  [Michaelis'  a]  ... 
4,6-dinitroguaiacol  

c    2.6-4.4y 
pK  =  3  4 

(17,  20,  21) 
(10   17) 

5 

Dinitrohydroquinol 

3-10 

m26) 

6 

Nitrohydroquinol  

3-11 

(26) 

6a 

3,5-dinitrocatechol  ..              .   . 

[     pKi  =    3.25 

/ 

L       (17) 

7 
8 
8a 

2,3-dinitrophenol  [Michaelis'  «]... 
2,5-dinitrophenol  [Michaelis'  7]... 
2  ,  4-dinitroresorcinol 

\     pK2  =  10.39 
c    3.9-  5.9  y 
c    4.0-  5.8y 
pK  =  4  22 

(15,  20,  21) 
(15,  20,  21) 

(17) 

9 

2,6-dinitro-4-aminophenol;     Iso- 
picramic  acid 

p    4  1-  5  6  v 

(36) 

10 
11 

3,  4-dinitrophenol  [Michaelis'  5]... 
4-nitro-6-aminoguaiacol  

c    4.3-  6.3y 
y    4.5-  8.0  r 

(20,  21) 
(18) 

12 

p-nitrophenol  

c    5.6-7.6y 

(15,  20,  21,  32) 

13 

o-nitrophenol  ...         .           ... 

c    5  0-  7  0  y 

(26) 

13a 

2-nitroresorcinol  

pK2  =  6.47 

(17) 

14 

*Dinitrobenzoylene  urea  

c    6.0-  8.0  y 

(2,  10) 

15 

m-nitrophenol 

c    6  8-  8  6  y 

(15,  20,  21) 

16 

2,4,  6-trinitrophenyl-methyl- 
nitroamine  ;  Nitramine    .... 

c  10.8-13  0  br 

(15) 

17 

sym.-trinitrobenzene  

c  12.0-14.0o;f 

(10,  29) 

18 

2,  4,  6-  trinitrotoluene  

p  11.5-14.0  o 

(3a) 

76 


IV                                                       INDICATOR  LIST                                                      77 
TABLE  8—  Continued 

INDEX 

NUM- 
BER 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Mono-azo  compounds 

19 
20 

21 

22 
23 

24 
25 

26 
27 

28 
29 

30 
31 
32 
33 

34 
35 

36 

37 
38 
39 

p-toluene-azo-phenyl-aniline  .  .  . 

1.0-2.0 
r    1.0-  3.0  y 

1.1-  1.9 
p    1.2-2.1y 

r    1.2-2.3y 
v    1.4^2.6o 

r    1.4r-2.6y 
1.4-2.9 

1.6-2.6 
1.6-2.8 

1.9-2.9 
y    1.9-  3.3y 
r    1.9-3.3y 
r    1.9-  3.3y 

r   2.0-  4.0y 
p   2.3-  3.3  y 

r    2.6-  4.0y 

r   2.6-  4.6y 
r   2.9-  4.0  y 
r   2.9-  5.8y 
mid-point  2.  9 

(31,  32) 
(3,  33) 

(31,  32) 
(32) 

(32) 
(31,  32) 

(32,  33) 
(31,  32) 

(31,  32) 
(31,  32) 

(31,  32) 
(31,  32,  33) 
(31,  32,  33) 
(32,  33) 

(3b) 
(32) 

(32,  33) 

(3a) 
(32,  33) 
(34) 
(33) 

p-carboxybenzene-azo-dimethyl- 
aniline;  Para  methyl  red 

p-toluene-azo-phenyl-a-naph- 
thylamine  

Benzene-azo-diphenylamine  
m-benzenesulfonic  acid-azo- 
diphenylamine  ;  Metanil  yellow 
[S.  134;  R.  138J  

Benzene-azo-phenyl-a-naphthyl- 
amine 

p-benzenesulfonic  acid-azo-di- 
phenylamine;    Tropaeolin    OO 
[S.  139;  R.  143] 

o-tuluene-azo-o-toluidine  ;  Spirit 
yellow  R  [S.  68;  R  17] 

p-toluene-azo-benzyl-o!-naphthyl- 
amine  

p-toluene-azo-benzyl-aniline  

Benzene-azo-benzyl-a-naphthyl- 
amine  

Benzene-azo-aniline;  amino-azo- 
benzene  [S.  31  ;  R.  15]  
p-benzenesulfonic     aeid-azo-ani- 
line 

p-benzenesulfonic    acid-azo-ben- 
zylaniline  -    . 

m-carboxybenzene-azo-dimethyl- 
aniline  

Benzene-azo-benzylaniline  
p-benzenesulfonic  acid-azo-m- 
chlorodiethylaniline 

m-nitrobenzene-azo-^-naphthol- 
3,6-disulfonic  acid;  Orange  III 
[S.  47;  R.  39]    .     . 

Benzene-azo-dimethylaniline  ; 
Topfer's  indicator  [S.  32;  R.  19]. 
o-carboxybenzene-azo-a-naph- 
thylamine 

p-benzenesulfonic  acid-azo-o- 
toluidine  

78 


THE    DETERMINATION   OF   HYDROGEN   IONS 

TABLE  8— Continued 


INDEX 

NUM- 
BEB 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Mono-azo  compounds — Continued 


40 

p-benzenesulfonic  acid-azo-m- 
xylidine  

mid-point  2  9 

(33) 

41 

o-carboxybenzene-azo-diphenyl- 
amine 

p    3  0-  4  6  y 

(3b) 

42 
43 

p-benzenesulfonic  acid-azo- 
methylaniline  
p-benzenesulfonic  acid-azo-ethyl 
aniline 

r    3.1-  4.2y 
r    3  1-  4  4  y 

(31,  32,  33) 
(31   32   33) 

44 

p-benzenesulfonic  acid-azo-di- 
methylaniline  ;  Methyl  orange 
[S.  138;  R.  142]  

r    3  1-  4  4  y 

(32,  33) 

45 
46 

p-benzenesulfonic  acid-azo-di- 
ethylaniline  ;  Ethyl  orange  
o-benzenesulfonic  acid-azo- 
dimethylaniline  

r    3.5-  4.5y 
mid-point  3.5 

(31,  32,  33) 

(33) 

47 

p-benzenesulfonic  acid-azo-m- 
toluidine  

mid-point  3.5 

(33) 

48 

p-benzenesulfonic  acid-azo-p- 
xylidine 

mid-point  3  6 

(33) 

49 
50 

*  p-sulfo-o-methoxybenzene-azo- 
dimethyl-a-naphthylamine  
p-benzenesulfonic  acid-azo-a- 
naphthylamine  

b    3.5-  4.9  o 
r    3.5-  5.7  y 

(23) 
(32,  34) 

51 

p-benzenesulfonic  acid-azo- 
phenyl-«-naphthylaniine  

v    3.5-  6.5  o 

(34) 

52 

o-carboxybenzene-azo-phenyl-a- 
naphthylamine  

v    3.5-  6.5  o 

(34) 

53 
54 
55 

Benzene-azo-a-naphthylamine  .... 
p-toluene-azo-a-naphthylamine.  .  . 
o-carboxybenzene-azo-methyl- 
aniline  

r    3.7-  5.0  y 
3.7-  5.0 

r    4.0-  6.0  y 

(32,  34) 
(31,  32) 

(3b) 

56 
57 

Benzene-azo-m-phenylenedi- 
amine  ;  Chrysoidine  [S.  33  ;  R.  20]  . 
o-carboxybenzene-azo-ethylani- 
line 

o    4.0-  7.0  y 
r    4  2-  6  2  y 

(3a) 
(3b) 

58 
59 
60 

o-carboxybenzene-azo-n-propyl- 
aniline  
o-carboxybenzene-azo-dimethyl- 
aniline;  Methyl  red  [R.  211].  .  .  . 
o-carboxybenzene-azo-diethyl- 
aniline  ;  Ethyl  red  

r    4.2-  6.2y 
r    4.2-  6.3y 
r    4.4-  6.2y 

(3b) 
(4,  32,  33) 
(3b,  33) 

IV 


INDICATOR   LIST 


79 


TABLE  8— Continued 


INDEX 
NUM- 
BER 


COLOR  AND  USEFUL 
RANGE  pH 


LITERAtCRE 


Mono-azo  compounds — Continued 


61 

*  o-carboxybenzene-azo-di-n- 
propylaniline  ;  Propyl  red..   .. 

r    4  6-  6  6  y 

(3b) 

62 

o-carboxybenzene-azo-m- 
phenylenediamine  

o    4  fr-  7  6  y 

(3a) 

63 

Benzene-azo-dimethyl-a-naph- 
thvlamine 

48-55 

(31   32) 

64 

p-benzenesulfonic  acid-azo-di- 
methyl-a-naphthylamine  

r    5  0-5  7  o 

(31,  32,  34) 

65 

o-carboxybenzene-azo-a- 
naphthlyamine  

p    5  6-  7  0  y 

(3b) 

66 

o-carboxybenzene-azo-(di  or 
mono?)-amyl  aniline 

o    5  6-  7  6  y 

(3b) 

67 

o-carboxybenzene-azo-dimethyl- 
a-naphthylamine 

r    5  6-  7  6  o 

(4  34) 

68 

4-sulfo-a-naphthalene-azo-o:-naph- 
thol;  Naphthylamine  brown  [S. 
160;  R.  175] 

o    6  0-  8  4  p 

(3a) 

69 

Tropaeolin?  

y    7  0-  9  o  r 

(29) 
^) 

70 

6-sulfo-a-naphthol-l-azo-m- 
hydroxybenzoic  acid 

f     o    7.0-  8.  Ob 
\     v  12    -13     r 

|        (36) 

71 

Curcumine?  

y    7  4-  8  6  b 

(15) 

72 

p-benzenesulfonic  acid-azo-a- 
naphthol;  Tropaeolin  OOO  No.  1 
[S.  144;  R.  150] 

y    7  &-  8  9  p 

(32) 

73 

p-benzenesulfonic  acid-azo-/9- 
naphthol;  Tropaeolin  OOO  No.  2 
IS.  145;  R.  151] 

76-8  9(?) 

(25) 

74 

m-nitrobenzene-azo-salicylic  acid  ; 
Alizarin  yellow  GG  [S.  48;  R. 
36]  

c(?)  10  0-12  0  y 

(20,  21) 

75 
76 

77 

p-nitrobenzene-azo-salicylic  acid  ; 
Alizarin  yellow  R  [S.  58;  R.  40]. 
a-naphthylaminosulfonicacid-azo- 
0-naphthol;RedI[S.  161;  R.  176]. 
a-naphthalene-azo-/8-naphthol- 
3,6-disulfonic  acid;  Bordeaux 
B  [S.  112;  R.  88]  

y  10.0-12.1  y 
10.5-12.1 

p  10.5-12  5  o 

(32) 
(31,  32) 

(3a) 

77a 

Isonitrosoacetyl-p-amino-azo- 
benzene 

see  p  583 

(24) 

78 

p-benzenesulfonic  acid-azo-re- 
sorcinol;  Tropaeolin  O  [S.  143; 
R.  148]  

y  11  1-12  7  o 

(32) 

80 


THE  DETERMINATION  OF  HYDROGEN  IONS 


TABLE  8— Continued 


INDEX 
NUM- 
BER 


COLOR  AND  USEFUL 
RANGE  pH 


Mono-azo  compounds — Continued 


79 

Benzene-azo-/?-naphthol-6,  8-di- 
sulfonic  acid;  Orange  GG  (S. 
38;  R.  27]  

y  11  5-14  0  p 

(3a) 

80 

Crocein? 

p  12  0-14  0  v 

C291 

80a 

Isonitroso-p-toluazo-p- 
toluidine 

see  p   583 

(24) 

81 

Helianthin  (Griibler)?  

o  11  0-12  0  r 

(3a) 

82 

Helianthin  1? 

o  11  0-13  0  r 

(29) 

83 

Helianthin  II?  

y  13  0-14  0  v 

(29) 

84 

Curcumein?             

f     o    0.0-  1.0  y 

J         (29) 

|     yl3.0-15.0g 

Dis-azo  compounds 


85 
86 
87 
88 

89 

Ditolyl-disazo-bis-/3-naphthyl- 
amine-6-sulfonic   acid;  Benzo- 
purpurin  B  [S.  365;  R.  450]  
Ditolyl-disazo-bis-a-naphthyl- 
amine-4-sulfonic  acid;  Benzo- 
purpurin  4B  [S.  363;  R.  448].  .  .  . 
Diphenyl-disazo-bis-a-naphthy!- 
amine-4-sulfonic  acid;  Congo  red 
[S.  307;  R  370]                     .     .  . 

[     b    0.3-  1.0  v 
v    1.0-  5.0  y 
[     y  12.  0-14.  Or 

v    1.3-  4.  Or 
b    3.0-  5.  Or 

v  10.  5-11.  5  p 
f     mid-point  7.  3 
\     mid-point  7.  6 

(29) 

(15) 
(29) 

(3a) 
(28) 
(9) 

Ditolyl-disazo-bis-a-naphthol-4- 
sulfonic  acid;  Azo  blue  [S.  377; 
R.  463]  

CurcuminW  [probably  Rowe,  364]. 

Triphenylmethane  derivatives 

90 
91 

92 
93 

Methylated  pararosaniline  ;  Crys- 
tal violet  [S.  516;  R.  681]  
p,  p'-tetramethyldiamino-tri- 
phenylcarbinol;  Malachite  green 
[S  495-  R  657] 

g    0.0-  2.  Ob 

I     y    0.0-2.0g 
b  11.  5-14.  Of 

g    0.0-  2.  Ob 
y    0.0-2.6g 

(3a) 
(29) 

(3a) 
(3a) 

Hofmann's    violet;    methylated 
rosanilines  and  pararosanilines 
[S  514*  R  679] 

Tetraethyl-diamino-triphenyl- 
carbinol;  Brilliant  green  [S.  499; 
R  662]                            

IV                                                       INDICATOR   LIST                                                      81 
TABLE  8—  Continued 

INDEX 

NUM- 
BER 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Triphenylmethane  derivatives—Continued 

94 
95 
96 
97 

98 
99 

99a 
99b 
100 

101 
102 

102a 
103 
104 
105 

106 
107 

Heptamethylrosaniline;      Iodine 
green  [R  686] 

y    0.0-2.6b 
y    0.0-  3.6b 
y    0.3-2.  Ob 

yO.15-  3.2  v 
0.4-2.7 

pu    1.2-  3.  Of 
v    1.2-  3.2c 
p   2.6-  4.6c 

p    3.6-  6.0  c 
o    3.8-  6.5  v 

b    4.7-7.0c 
r   5.0-7.0c 
br    6.9-  8.  Or 
v   9.4r-14.0  p 

b  10.  0-13.  Op 
b  11.  0-13.  Or 

r  12.  0-14.  Of 

(3a) 
(3a) 
(15) 

(32) 
(31,  32) 

(3a) 
(16) 
(16) 

(3a) 
(15) 

(3ft) 

(16) 
(32) 
(3a) 

(3a) 
(3a) 

(29) 

Hexaethylpararosaniline;     Ethyl 
violet  [S.  518;  R.  682]  
Ethyl-hexamethyl-pararosaniline; 
Ethyl  green  [R   685] 

Methyl    violet    6B;    benzylated 
tetra-    and    pentamethyl-para- 
rosaniline  [S.  517;  R.  683]     

Gentian  violet;  mixture  

Aniline  red;  rosaniline  and  para- 
rosaniline  [S.  512;  R.  677]  
2,4,2',4',2"-pentamethoxytri- 
phenylcarbinol  

2,4,2',4',2",4"-hexamethoxytri- 
phenylcarbinol  

Red  violet  5RS;  di-  and  tri-sul- 
fonate  of  ethylrosaniline  [S.  525; 
R.  693]  

Resazurin  [R.  727  note]  . 

China  blue  [S.  539;  R.  707];  mix- 
ture   

2,4,6,2',4',2",4"-heptamethoxy- 
triphenyl  carbinol  

Rosolic  acid  [S.  555;  R.  724];  mix- 
ture 

Alkali  blue  4B  [S.  536;  R.  704]; 
mixture  ... 

XL  soluble  blue  [S.  538;  R.  706]; 
mixture  

Poirrier's  blue 

Acid  fuchsin;  di-  and  tri-sulfonic 
acids  of  rosaniline  and  para- 
rosaniline  [S  524;  R  692] 

Phthaleins  and  related  compounds  (see  also  Thiel  and  Diehl,  1927) 


108 

Diethyl-m-amino-phenolphtha- 
lein;  Rhodamine  B  [S.  573;  R. 
749]  

o    0.1-  1.2  p 

(3a) 

109 

Pyrogallol-phthalein;  Galle'in  [S. 
599;  R.  781]  ... 

variable  0—14 

(29) 

82 


THE  DETERMINATION  OF  HYDROGEN  lONg 


TABLE  8— Continued 


INDEX 

NUM- 
BER 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Phthaleins  and  related  compounds  —  Continued 

110 
111 

112 
113 

114 
115 
116 
117 
118 
119 
120 
120a 

121 
121a 
122 
123 

124 

125 
126 

Tetrabromofluorescein;      Eosine 
Y  S  [S.  587;  R.  768]  

y    0    -3.0fl 

o    0.0-  3.6fl 
p    1.4r-  3.6r 

y    3.6-  5.6fl 
y    4.0-  6.6fl 
y    8.9-9.5g(f) 
y    7.0-  9.  Ob 
c    8.0-9.0v 
c    8.5-  9.0  pu 
c    8.2-  9.8r 
c    8.  3-10.  Or 

c    8.4r-  8.8b 
c    8.  9-10.  2  b 
c    9.  2-10.  Ob 
c    9.3-10.5b(f) 

p  10.  5-14.  Oy 
c    8.4r-10.0v 

c    8.6-  9.8  v 
c    9.0-lO.Ov 

(3a) 

(3a) 
(3a) 

(3a) 
(3a) 
(8) 
(32) 
(25) 
(1,  14) 
(3b) 
(20,  21,  32) 

(7) 
(8) 
(7) 
(32) 

(3a) 
(12) 

(12) 
(12) 

Erythrosin     (iodeosin);    di-    or 
tetra  fluorescein  [S.  591,  592? 
R.  772,  773?]  

Phloxin  red  B.H.  (Griibler)? 

Dihydroxyfluoran;  Uranin  (fluo- 
rescein) [S.  585;  R.  766]  

Dichlorofluorescein  

o-a-naphthol  phthalein  . 

p-a-naphthol  phthalein  

Tetrabromophenol  phthalein 
o-cresoltetrachlorophthalein  
o-cresolphthalein  

Phenolphthalein  [R.  764]  

Dibromothymoltetrachloro- 
phthalein  

*  1,2,3-xylenolphthalein  

Thymol  tetrachlorophthalein 

Thymolphthalein    

Dibromo-dinitrofluorescein;  Eosin 
BN  [S.  590;  R.  771]  

R=  SCH3     ^^      /<CZy>OH 
R=SC4HJ/N  \      [\^        ^>OH 
R=SC6H60  =  C—  0              R 

Sulfonphthaleins 


127 

Catecholsulf  onphthalein  

f     p.   0.2-  0.8o 
\     y    4.0-  7.0  g 

[       (22) 

128 

m-cresolsulfonphthalein;  Meta- 
cresol  purple  

v    8.5-10.2  b 

f     r    1.2-  2.  8  y 
1     y    7.4-9.0pu 

}        (5) 

129 

Thymolsulf  onphthalein  ;  Thymol 
blue  

f     r    1.2-  2.  8  y 
\     y    8.0-  9  6b 

}       (3b). 

130 
131 

Tetranitrophenolsulf  onphthalein. 
Tetrabromophenolsulf  onphtha- 
lein; Bromphenol  blue 

y    2.8-  3.8r 
y    3  0-  4  6  b 

(3b) 
(3b) 

132 

*  Tetrachlorophenolsulfonphtha- 
lein 

y    3  0-  4  6  b 

(3b) 

IV 


INDICATOR  LIST 


83 


TABLE  8— Continued 


INDEX 
NUM- 
BER 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Sulfonphthaleins — Continued 


133 

*  Dichloro-dibromo-phenol-sul- 
f  onphthalein;  Brom-chlorphenol 
blue                 

y    3  0-  4.6  b 

(5) 

134 
134a 

Tetrabromo-m-cresolsulfon- 
phthalein;  Bromcresol  green  — 
Tetrachloro-m-cresolsulfon- 
phthalein                                  .  . 

y    3.8-  5.4b 
y    4  0-  5  6  b 

(5) 
(5) 

135 
136 

Dichlorophenolsulf  onphthalein  ; 
Chlorphenol  red  
Dibromo-o-cresolsulf  onphthalein; 
Bromcresol  purple 

y    4.8-  6.4  r 
y    52-68  pu 

(5) 
(3b) 

137 

138 
139 

Dibromophenolsulf  onphthalein  ; 
Bromphenol  red 
*  Diiodophenolsulf  onphthalein  .  .  . 
Dibromothymolsulf  onphthalein  ; 
Bromthymol  blue 

y    5.2-  6.8r 
y    5.7-  7.3  pu 

y    6  0-  7  6  b 

(5) 
(3a) 

(3b) 

140 

*  Brom     xylenol     blue,     dibrom- 
inated  No   145        

y    6  0-  7  6  b 

(5) 

141 
142 

Phenol-nitrosulf  onphthalein  
Phenolsulf  onphthalein;      Phenol 
red 

y    6.6    8.4pu 

y    6  8-  8.4  r 

(3b) 
(3b) 

143 

144 

o-cresolsulf  onphthalein;  Cresol  red 
Salicylsulf  onphthalein  

y    7.2-  8.8r 
y    7.2-  9.2  p 

(3b) 
(3a) 

145 

*  1.4-dimethyl-5-hydroxyben- 
zenesulf  onphthalein;     Xylenol 
blue                                 

y    8.0-  9.6  b 

(4) 

146 

a-naphtholsulf  onphthalein 

y   7  5-  9.0  b 

(3b) 

147 

Carvacrolsulf  onphthalein  

y    7.8-  9.6  b 

(3b) 

148 

Orcinsulfonphthalein       .       

y    8.6-lO.Ofl 

(3b) 

149 

Nitro-thymolsulf  onphthalein  

v    9.  2-11.  5  y 

(3b) 

Quinoline  compounds 


150 

a-  (p-dimethylaminophenylethyl- 

ene)-quinoline  ethiodide;  Quin- 

aldine    red.    Eastman    Kodak 

Co.  No.  1361  

C,  1.0-2.0  r 

'  (18) 

150a 

Pinacyanol  [R.  808]       

pK  =  3.7 

(10,  18) 

150b 

Ortho-chrom-T  [R  807] 

pK  =  6  7 

(10,  18) 

151 

Quinoline    blue     (cyanin);    1,1' 

di-iso-amyl-4,  4'-quinocyanine 

iodide  IS.  611;  R.  806]  

c    7.0-  8.0  v 

(31,  32) 

84 


THE  DETERMINATION  OF  HYDROGEN  IONS 


TABLE  &— Continued 

Index  no.  152    Indophenols  (6) 

Color  changes:  from  brownish  or  clear  red  in  acid  to  deep  blue  in  alkali. 
All  indophenols  are  somewhat  unstable 

5'     6'  56 

HO/ ^N  =  <T    I^>  =  0 
\ /  \ / 

3'     2'  32 

Indophenol 


SUBSTITUENT8 


pK 


2,6,3'  tribromo- 5.1 

2,6-dibromo-3'-chloro- 5.4 

2,6-dibromo-3'-methyl- 5.4 

2,6-dichloro-3'-chloro- 5.8 

2, 6-dichloro-3'-methyl- 5.5 

2,6-dibromo-3/-methoxy- 5.6 

2,6-dichloro- 5.7 

2,6-dibromo- 5.7 

2, 6-dibromo-2 '-methyl- 5.9 

2, 6-dibromo-2'-bromo- 6.3 

2-chloro- 7.0 

2-bromo- 7.1 

3-bromo- 7.8 

Indophenol 8.1 

2-methyl- 8.4 

3-methyl- 8.6 

2-methoxy- 8.7 

2-isopropyl-5-methyl- 8.8 

2-methyl-5-isopropyl 8.9 


5'     6' 


34 


3'     2' 


o 


Orthoindophenol 


SUBSTITUENTS 


3'  bromo- 

Orthoindophenol . 
2'-methyl- 


7.1 
8.4 
8.8 


IV 


INDICATOR   LIST 


85 


TABLE  8—  Continued 

H03S  5      6 


H0<^  ~^>N  =  \  /  =  0 

/    S       3   2 

Indonaphthol-3'-sulfonic  acid 

8UBSTITUENT8 

pK 

2,6di 
Indon 
2-metl 

chloro-  

6.1 

8.7 
9.0 

aphthol-3'-sulfonic  acid  

tivl- 

INDEX 
NUM- 
BER 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Azines 

153 
154 

155 
156 

157 

158 

159 

Safranine  (which?)  .... 

b-0.3-  l.Or 

pu    0.0-  1.2  v 
0.1-  2.9 

p    3.0-  4.  On 
b    5.6-  7.0  v 

r    6.8-  8.0y 
9.3-10.2 

(29) 

(3a) 
(32) 

(29) 
(3a) 

(32) 
(31,  32) 

Amino-dimethylamino-phenyl- 
diphenazonium  chloride;  Meth- 
ylene  violet  B.N.  [S.  680;    R. 
842]  

Amino-phenylamino-p-tolyl-ditol- 
azonium   sulphate;   Mauve  [S. 
688;  R.  846]...:  

Magdala  red;  mixture  amino-  and 
diamino-naphthyl-dinaphth- 
azonium  chlorides  [S.  694;  R.  857] 
Induline,  spirit  soluble  [S.  697; 
R.  860];  mixture 
Amino-dimethylamino-toluphen- 
azonium  chloride;  Neutral  red 
[S.  670;  R.  825]  

Dimethylamino-phenyl-naphtho- 
phenazonium  chloride;  Neutral 
blue  [S.  676;  R.  832]             .    . 

Oxazine  compounds 


160 

Dihydroxy-dinaphthazoxonium 
sulfonate;  Alizarin  green  B  [S. 
657;  R  918] 

f    v-0.3-  1.0  p 
\     y  12  0-14  0  br 

N                                     9 

|       (33) 

161 
162 

Diethylamino-benzylamino- 
naphtho-phenazoxonium     chlo- 
ride; Nile  blue  2B  [S.  654;  R.  914]. 
Diethylamino-aminonaphtho- 
phenazoxonium    sulfate  ;    Nile 
blue  A  [S.  653;  R.  913].  ......... 

b    7.2-  8.  6  p. 
b  10.  2-13.  Op 

(3a) 
(3a) 

86 


THE  DETERMINATION  OF  HYDROGEN  IONS 


TABLE  8— Continued 


INDEX 

NUM- 
BEK 

INDICATOR 

COLOR  AND  USEFUL 
RANGE  pH 

LITERATURE 

Anthraquinones 

163 

164 
165 
166 
167 

1  ,  2-dihy  droxy-anthraquinone-0- 
quinoline;   Alizarin  blue  ABI 
[S.  803;  R.  1066]  

[     p    0.0-  1.6y 

1     y    6.0-  7.  6  g 
f     y    0.0-  4.0  o 
\     o    4.0-  8.  Op 

y    3.7-4.2p 
f    y    5.5-  6.8r 
1     vlO.l-12.lpu 
various  6-14 

[       (3a) 
}       (3a) 

(36) 
}    (.31,32) 
(25) 

1,2,  4-trihydroxy-anthraquinone  ; 
Purpurin  [S.  783;  R.  1037]  

Alizarin  sulfonic  acid;  Alizarin 
red  S  [S.  780;  R   1034] 

1  ,  2-dihy  droxy-anthraquinone  ; 
Alizarin  [S.  778;  R.  1027] 

Alizarin  blue  S  

Indigos 

168 

Indigo  disulf  onate  ;  Indigo  carmine 
[S.  877;  R.  1180]    .. 

b  11.  6-14.  Oy 

(3a) 

Miscellaneous  and  natural  indicators 

169 
170 

171 
171a 

172 

173 

174 

175 
176 
177 
178 
179 
180 
181, 

182 
183 

184 
185 

Echtrot?....  

y    0    -  l.Or 
various  0-14 
r    2.4r4.5g 
various  2-11 

c    2.7-  3.7  pu 

o   2.8-  3.9  y 
(    y    3.0-  6.  Or 
\     rlO.O-13.0c 
r    4.4-  5.5b 
r    4.4-  6.2  b 
r    4.5-  8.3b 
y    4.8-  6.2  v 
p    5.6-7.6v 
c    6.0-  8.0  p 

y   7.3-8.7g 
7.7-9.6 

y    7.8-  9.2br 

8.3-10.0 
y    8.5-9.8g 

(29) 
(25) 
(35) 
(19) 

(36) 

(36) 
}       (25) 

(13) 
(31,  32) 
(31,  32) 
(31,  32) 
(3a) 
(3a) 

(36) 

(32) 

(15) 

(31,  32) 
(31,  32) 

Logwood  [S.  938;  R.  1246]  

*  Red  cabbage  extract 

Blue  cabbage  extract  

1-oxynaphtho-quinomethane  ; 
Nierenstein's  indicator  
Troger    and    Hille's    indicator, 
CuHisNiSOsH  

Phenacetolin 

Lacmosol  

Lacmoid  [R.  908  note] 

Azolitmin  (litmus)  [R   1242] 

Cochineal  [S.  932;  R.  1239]  
Archil  (orchil)  [S.  934;  R.  1242]... 
Brazilein  [S.  935;  R.  1243] 

Di-o-hydroxy-styryl  ketone  ; 
Lygosine  

Mimosa  flower  extract  

Turmeric  (curcuma)  [S.  927;  R. 
1238] 

Alkannin    [R.     1240,    note]    cf. 
alizarin 

a-naphtholbenzein  

IV  INDICATOR  NAMES  87 

TABLE  8—  Concluded 

(1)  Arnold  (1924).  (18)  McClendon  (1924). 

(2)  Bogert  and  Scatchard  (1916).         (19)  Milobedzki  and  Jajte  (1926). 
(3a)  Clark,  Cohen  and  Elvove  (see       (20)  Michaelis  and  Gyemant  (1920). 

text,  page  71).  (21)  Michaelis  and  Kr tiger  (1921). 

(3b)  Clark  and  Lubs  (1915-1917).  (22)  Moir  (1920). 

(4)  Cohen,  A.  (1923).  (23)  Moir  (1923). 

(5)  Cohen,  B.  (1927).  (24)  Naegeli  (1926). 

(6)  Cohen,  Gibbs  and  Clark  (1924).  (25)  Prideaux  (1917). 

(7)  Cornwell  and  Esselstyn  (1927).  (26)  Prideaux  (1924). 

(8)  Csanyi  (1921).  (27)  Rowe  (1924). 

(9)  Fels  (1904).  (28)  Salessky  (1904). 

(10)  Hegge  (1925).  (29)  Salm  (1906). 

(11)  Henderson  and  Forbes  (1910).  (30)  Schultz  (1923). 

(12)  Holt  and  Reid  (1924).  (31)  S0rensen  (1909). 

(13)  Hottinger  (1914).  (32)  S0rensen  (1912). 

(14)  Hundley       and       McClendon  (33)  Thiel    Dassler.  and    Wiilfkin 

(1925).  (1924). 

(15)  Kolthoff  (1923).  (34)  Thiel  and  Wulfkin  (1924). 

(16)  Kolthoff  (1927).  (35)  Walbum  (1913). 

(17)  Laxton,    Prideaux  and    Rad-      (36)  Walpole  (1914). 

ford  (1925). 

TABLE  9 
Common  synonyms  of  indicators 

Among  synonyms  given  in  this  table  are  several  which  apply  to  dyes 
which  are  not  listed  in  preceding  table  or  which  have  been  applied  to  two 
or  more  of  the  indicators  listed.  Such  cases  are  indicated  by*.  Num- 
bers are  index  numbers  of  table  8. 

Acid  bordeaux,  77  Alkanet,  184 

Acid  brown  R,*  68  Alkalin,  Alkannin,  184 

Acid  fuchsin,*  107  Alphanaphtholbenzein,  185 

Acid  magenta  II,  107  Alphanaphtholphthalein,*  116 

Acid  roseine,  107  Amido-azo-benzol,  30 

Alizarin,  166  Amido-azo-toluol,  26 

Alizarin  blue  ABI,  163  Amino-azo-benzene,  30 

Alizarin  blue  S,  167  Amino-azo-toluene,  26 

Alizarin  blue  X,  163  Amyl  red,  66 

Alizarin  carmine,  165  Anchusin,  184 

Alizarin  green  B,  160  Aniline  orange,*  31 

Alizarin  red  S,  165  Aniline  red,  99 

Alizarin  sulfonate  or  S,  165  Aniline  yellow,*  3,  25,  30 

Alizarin  yellow  GG,  74  Archil,  179 

Alizarin  yellow  R,  75  Aurin,  103 

Alkali  blue  4B,  104  Azo-blue,  88 


88 


THE  DETERMINATION  OF  HYDROGEN  IONS 


TABLE  9— Continued 


Azolitmin,  177 

Azoresorcin,  101 

Benzopurpurin  B,  85 

Benzopurpurin  4B,  86 

Benzyl  violet,  97 

Beta  naphthol  orange,  73 

Bitter  almond  oil  green,  91 

Blauholz,  170 

Boettger's  indicator,  184 

Bordeaux  B,  77 

Brasilein,  brasilin,  brazilin,  180 

Brazil  wood,  180 

Brilliant  green,  93 

Brilliant  yellow,*  89 

Brom-chlor-phenol  blue,  133 

Brom  cresol  green,  134 

Brom  cresol  purple,  136 

Brom  phenol  blue,  131 

Brom  phenol  red,  137 

Brom  thymol  blue,  139 

Brom  xylenol  blue,  140 

Butter  yellow,*  26,  37 

Cabbage  red,  171 

Campeachy  wood,  170 

Carmine,  178 

Carminic  acid,  178 

Catechol  sulphonphthalein,  127 

China  blue,  102 

Chlor  phenol  red,  135 

Chrome  printing  orange  R,  75 

Chrome  printing  yellow  G,  74 

Chrysoidine,  *  56 

Chrysoine,  78 

Coccus,  178 

Cochenille,  cochineal,  178 

Congo,  87 

Congo  red,  87 

Corallin,  103 

Cresol  red,  143 

Cresolphthalein,*  119 

Cresolsulphonphthalein,  *  143 

Crismer's  indicator,  101 

Crocein,*  80 

Crystal  violet,  90 


Curcuma,  183 

Curcumein,*  84 

Curcumin,*  183 

Curcumin  W,  89 

Curcummin,*  183 

Cyanin,  151 

Dechan's  indicator,  109 

Degener's  indicator,  174 

Dianil  red,*  87 

Dichlorofluorescein,  114 

Diethylaniline  orange,  45 

Dihydroxyanthraquinone,  166 

Dimethylaniline  orange,  44 

Dimethyl  orange,  44 

Dimethyl  yellow,  37 

Dinitroaminophenol,  9 

Dinitrohydroquinone,  5 

Echtrot,*  169 

Echtrot  A,  76 

Echtrot  B,  77 

Eosine,  110 

Eosine  BN,  123 

Eosine  YS,  110 

Erythrosine, *  111 

Ethyl  green,*  96 

Ethyl  orange,  45 

Ethyl  red,*  60 

Ethyl  violet,  95 

Fast  red  A,  76 

Fast  red  B,*  77 

Fluorescein,  113 

Formanek's  indicator,  160 

Fuchsia,  154 

Fuchsin,*  99 

Fuchsin  S,  107 

Galeine,  109 

Gallein,  109 

Gentian  violet,  98 

Golden  orange,  44 

Haematein,*1  170 

Haematoxylin,*1      haematoxylon,* 

170 

Helianthine,*  44,  81,  82,  83 
Hematein,*1  hematine,*1  170 


1  Haematoxylin  is  the  leuco-compound  of  Haematein  or  Hematine  as 
obtained  from  logwood  although  the  name  is  sometimes  givon  to  the  oxi- 
dized form.  Haematein  or  Hematine  should  not  be  confused  with  Hem- 
atin  of  the  blood  pigment. 


IV 


INDICATOR   NAMES 


89 


TABLE  9— Continued 


Hematoxylin,*1  170 
Henderson  &  Forbes'  indicator,  5 
Heptamethoxy  red,  102a 
Herzberg's  indicator,  87 
Hexamethoxy  red,  99b 
Hofmann's  violet,  92 
Holt  &  Reid's  indicators,  124-126 
Indigo  carmine,  168 
Indigo  disulphonate,  168 
Indophenols,  152 
Induline  spirit-soluble,  157 
lodeosine,*  111 
Isopicramic  acid,  9 
Iodine  green,  94 
Kosmos  red,  87 
Kroupa's  indicator,  99 
Kriiger's  indicator,  113 
Lackmoid,  lacmoid,  176 
Lacmosol,  175 
Lacmus,  177 
Litmus,  177 
Logwood,  170 
Luck's  indicator,  120 
Lunge's  indicator,  44 
Lygosine,  181 
McClendon's  indicator,  11 
Magdala  red,  156 
Magenta,*  99 
Malachite  green,  91 
Manchester  yellow,  3 
Martius  yellow,  3 
Mauve,  mauveine,  155 
Mellet's  indicator,  70 
Meta  cresol  purple,  128 
Meta  methyl  red,  33 
Metanil  yellow,  23 
Metanitrophenol,  15 
Methyl  blue,*  105 
Methylene  violet  BN,  154 
Methyl  green,*  96 
Methyl  orange,  44 
Methyl  red,  59 
Methyl  violet  5B  or  6B,  97 
Methyl  yellow,  37 
Michaelis'  nitro  indicators,  1,  2,  4, 
7,  8,  10,  12,  15 


Mimosa  flower  extract,  182 

Moir's  "Improved  methyl  orange," 

149 

Moir's  polychromatic  indicator,  127 
Monobenzyl  orange,  32 
Monoethyl  orange,  43 
Monoethyl  red,  57 
Monomethyl  orange,  42 
Monomethyl  red,  55 
Monopropyl  red,  58 
Naphthol  benzein,  185 
Naphthol  orange,  72 
Naphtholphthalein,*  115,  116 
Naphthylamine  brown,  68 
Neutral  blue,  159 
Neutral  red,  158 
Nierenstein's  indicator,  172 
Nile  blue  A,  162 
Nile  blue  B,  161 
Nitramine,  16 
Nitroaminoguaiacol,  11 
Nitrobenzene  (tri),  17 
Nitrobenzoylene  urea,  14 
Nitronaphthol,  3 
Nitrotoluene,  18 
Oil  yellow,*  37 
Oil  yellow  B,  30 
Orange  G,*  79 
Orange  GG,  79 
Orange  I,  72 
Orange  II,  73 
Orange  III,*  36,  44 
Orange  IV,  25 
Orchil,  179 
Orseille,  179 
Ortho-chrom-T,  150b 
Parahelianthine,  44 
Para  methyl  red,  20 
Paranitrophenol,  12 
Paraphthalein,  120 
Pentamethoxy  red,  99a 
Pernambuco,  180 
Phenacetolin,  174 
Phenol  red,  142 
Phenolphthalein,  120 
Phenolsulphonphthalein,  142 


90 


THE  DETERMINATION  OF  HYDROGEN  IONS 


TABLE  9— Concluded 


Phloxin  red  BH,  112 
Phosphine  substitute,  78 
Picric  acid,  1 
Pinacyanol,  150a 
Poirrier's  blue  C4B,  106 
Poirrier's  orange  III,  44 
Propyl  red,  61 
Purpurin,  164 
Pyrogallol  phthalein,  109 
Quinaldine  red,  150 
Quinoline  blue,  151 
Red  I,  76 

Red  cabbage  extract,  171 
Red  violet  5R,*  92 
Red  violet  5RS,  100 
Red  wood,  180 
Resazurin,  101 
Resorcin  blue,*  176 
Resorcin  phthalein,  113 
Resorcin  yellow,  78 
Rhodamine  B,  108 
RiegePs  indicator,  87 
Rosaniline,  99 
Roseine,  99 
Rose  magdala,  156 
Rosolane,  155 
Rosolic  acid,  103 
Rotholz,  180 
Rubine  S,  107 
Safranine,*  153 
Salicyl  yellow,*  74 
Schaal's  indicator,  166 
Soluble  blue  3M,  2R,  102 
Soluble  red  woods,  180 
Spirit  yellow,  30 


Spirit  yellow  G,  30 

Spirit  yellow  R,  26 

Tetra  brom  fluorescein,  110 

T.  N.  T.   18 

Thymol  blue,  129 

Thymolphthalein,  122 

Toluidine  orange*  (ortho),  39 

Toluidine  orange*  (meta),  47 

Toluylene  red,*  158 

Topfer's  reagent,  37 

Tournesol,  177 

Troger  and  Hille's  indicator,  173 

Tropaeolin*,?  69 

Tropaeolin  D,  44 

Tropaeolin  G,*  23,  72 

Tropaeolin  O,  78 

Tropaeolin  OO,  25 

Tropaeolin  OOO  No.  1,  72 

Tropaeolin  OOO  No.  2,  73 

Tropaeolin  R,  7 

Turmeric,  183 

Turnsole,  177 

Uranin,  113 

von  Miiller's  indicator?,  25 

Weselsky's  indicator,  101 

Water  blue,  102 

XL  Soluble  blue,  105 

Xylenol  blue,  145 

Xylenol  phthalein,*  121 

Xylidine  orange*  (meta),  40 

Xylidine  orange*  (para),  48 

Yellow  B,  37 

Yellow  T,  78 

Zellner's  indicator,  113 


SELECTED  INDICATORS 


Table  10  is  S0rensen's  list, 
sen  remarks: 


Concerning  these  indicators  S0ren- 


Not  all  these  indicators  furnish  equally  well  defined  virages  and  above 
all  they  are  not  of  equal  applicability  under  all  circumstances.  In  the 
choice  of  an  indicator  from  among  those  which  we  have  been  led  to  recom- 
mend it  is  necessary  to  use  judicious  care  and  especially  to  take  into  con- 
sideration the  following  facts; 


rv  S^RENSEN'S  INDICATORS  91 

a.  The  indicators  of  the  methyl  violet  group  (nos.  1  and  2)  (see  table  10) 
are  especially  sensitive  to  the  action  of  neutral  salts;  furthermore  the 
intensity  of  color  changes  on  standing  and  the  change  is  the  more  rapid 
the  more  acid  the  medium. 

6.  The  basic  indicators  (nos.  3,  6,  9,  11,  14)  are  soluble  in  toluene  and  in 
chloroform.  The  first  four  separate  partially  on  prolonged  standing  of 
the  experimental  solution. 

c.  In  the  presence  of  high  percentages  of  natural  proteins  most  of  the 
indicators  are  useless  although  certain  of  them  are  still  serviceable;  nos. 
1,  2,  13,  16,  17,  18. 

d.  In  the  presence  of  protein  decomposition  products  even  in  considera- 
ble proportions  the  entire  series  of  indicators  may  render  real  service. 
Yet  even  in  these  conditions  some  of  the  acid  azo  indicators  may  give 
notable  errors  (nos.  4,  5,  7,  8,  10)  in  which  case  one  should  resort  to  the 
corresponding  basic  indicators. 

e.  When  only  small  percentages  of  protein  or  their  decomposition  prod- 
ucts are  concerned  the  acid  azo  indicators  are  more  often  preferable  to 
the  basic  for  they  are  not  influenced  by  toluene  or  chloroform  and  do  not 
separate  from  solution  on  standing. 

/.  In  all  doubtful  cases — for  example  in  the  colorimetric  measurement 
of  solutions  whose  manner  of  reaction  with  the  indicator  is  not  known, 
the  electrometric  measurement  as  a  standard  method  should  be  used. 
Then  the  worth  of  the  indicator  will  be  determined  by  electrometric 
measurement  with  colorimetric  comparison. 

In  table  11  will  be  found  the  selection  of  Clark  and  Lubs,  modi- 
fied by  the  rejection  of  methyl  red  and  the  inclusion  of  Cohen's 
contributions.  These  indicators  are  marketed  both  in  the  form 
of  the  dry  powder  and  in  stock  solutions.  In  cases  where  the 
acidity  of  the  free  acid  dye  does  not  interfere  with  accuracy  and 
when  alcohol  is  not  objectionable  the  alcoholic  solutions  of  the 
dyes  may  be  used.  Clark  and  Lubs  prefer  to  use  aqueous  solu- 
tions of  the  alkali  salts  in  concentrations  which  may  be  con- 
veniently kept  as  stock  solutions.  These  are  diluted  for  the  test 
solutions  used  in  the  dropping  bottles. 

For  the  preparation  of  these  stock  solutions  one  decigram  (0.1 
gram)  of  the  dry  powder  is  ground  in  an  agate  mortar  with  the 
quantities  of  NaOH  shown  in  column  A  and  footnote  in  table  11. 

If  there  be  no  particular  reason  to  maintain  exact  equivalents 
it  may  be  found  easier  to  dissolve  the  dyes  in  1.1  equivalents  of 
alkali  instead  of  one  equivalent  as  indicated  above.  See  page  190. 

To  place  the  dyes  upon  a  comparable  basis  the  final  dilution 
should  be  nearly  the  same  when  calculated  upon  a  molar  basis 


92 


THE  DETERMINATION  OF  HYDROGEN  IONS 


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SC^RENSEN'S  INDICATORS 


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THE  DETERMINATION  OF  HYDROGEN  IONS 


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IV  SULFONPHTHALEINS  95 

and,  by  reason  of  the  great  change  in  molecular  weight  caused 
by  the  introduction  of  bromine  and  other  group  substituents, 
equal  molecular  concentrations  will  be  very  far  apart  in  per- 
centage concentration.  For  all  ordinary  purposes,  however,  this 
may  be  neglected  and  solutions  of  a  concentration  of  0.04  per 
cent  will  be  found  satisfactory  for  use  in  testing  10  cc.  of  a  solu- 
tion with  about  five  drops  of  indicator. 

From  various  sources  have  come  complaints  that  the  method 
outlined  above  for  the  preparation  of  the  aqueous  alkali  salt 
solution  of  brom  cresol  purple1  leads  to  a  solution  of  much  lower 
tinctorial  power  than  when  the  same  material  is  taken  up  directly 
in  alcohol.  No  such  difficulty  was  experienced  with  the  material 
described  by  Lubs  and  Clark  but  it  has  appeared  not  infrequently 
since.  The  source  of  the  difficulty  is  not  yet  definitely  traced, 
but  is  suspected  to  be  due  to  impurities.  If  so  it  should  be 
avoided  by  purchasing  the  highly  purified  material  which  is  now 
made  specially. 

Since  the  range  of  an  indicator  depends  to  a  considerable  extent 
upon  the  manner  in  which  the  indicator  is  used,  it  is  of  interest 
to  note  the  ranges  assigned  by  Saunders  (1923)  on  the  basis  of 
his  ability  to  detect  changes  of  0.02  pH  unit. 

Brom  cresol  purple 5.8  -6.4 

Brom  thymol  blue 6.4  -7.2 

Phenol  red 7.1  -7.9 

Cresol  red 7.65-8.45 

Thymol  blue 8.4  -9.2 

Phenolphthalein,  or  orthocresolphthalein,  and  methyl  red, 
which  are  valuable  indicators  for  titrations,  may  be  used  for  this 
purpose  in  alcoholic  solution  unless  exacting  requirements  are  to 
be  met. 

Since  the  requirements  of  titration  are  so  varied  no  separate 
lists  for  this  process  have  been  compiled.  The  theory  of  titration 
is  outlined  in  Chapter  XXVIII.  There  reference  will  be  made  to 
the  color  chart  (page  65)  for  the  selection  of  various  end-point 

1  The  effect  of  excess  alkali  on  sulfonphthaleins  is  still  more  or  less 
uncertain.  See,  however,  Hubbard  and  Meeker  (1924),  Brown  (1923), 
Brightman,Hopfield  andJMeacham  and  Acree  (1918) .  AJsp  search  the  papers 
of  Orndorff , 


96  THE   DETERMINATION   OF   HYDROGEN   IONS 

colors  to  be  used  in  conjunction  with  figures  93  and  94  (page  535). 
There,  also,  reference  is  made  to  the  indicator  constants  of 
table  11  which  are  used  for  more  refined  work. 

Michaelis'  selection  of  "one-color"  indicators  is  given  in  table 
12.     Discussion  will  be  found  in  Chapter  VI. 

TABLE  12 

Michaelis'  indicators  and  their  ranges  as  used  in  the  method  of  Michaelis  and 
Gyemant  (see  Chapter  VI) 

Picric  acid colorless  0.0-  1.3  yellow 

2,  4-dinitro  phenol colorless  2.0-  4.7  yellow 

a  dinitro  phenol 

2,  6-dinitro  phenol colorless  1.7-  4.4  yellow 

0  dinitro  phenol 

2,  5-dinitro  phenol colorless  4.0-  6.0  yellow 

y-dinitro  phenol 

m-nitro  phenol colorless  6.3-  9.0  yellow 

p-nitro  phenol colorless  4.7-  7.9  yellow 

Phenolphthalein colorless  8.5-10.5  red 

Alizarin  yellow  GG colorless  10.0-12.0  yellow 

Salicyl  yellow 


MIXED   INDICATORS 

Mixtures  of  indicators  are  used  for  two  purposes.  The  modifica- 
tion of  color  is  discussed  in  Chapter  VII.  In  that  chapter  will 
be  found,  in  terms  of  absorption  spectra,  an  example  of  the  re- 
sultant effect  of  pH-change  upon  the  simultaneous  changes  in 
degree  of  dissociation  of  each  component.  The  more  usual  pur- 
pose of  a  mixture  is  to  extend  the  pH  range  which  can  be  covered 
by  one  test  solution. 

In  one  sense  indicator  mixtures  are  comparable  with  those 
indicators  which  have  several  ionizations  each  associated  with  a 
color  change.  Henderson  and  Forbes'  (1910)  employment  of 
dinitrohydroquinone  provided  one  of  the  earlier  instances  in 
which  use  was  made  of  a  compound  of  several  stages  of  dissocia- 
tion. With  this  one  indicator  they  were  able  to  cover  roughly 
the  range  pH  3  to  pH  9. 

Prideaux  and  Ward  (1924)  describe  the  "universal  indicator' ' 


IV 


MIXED    INDICATORS  97 


put  out  by  the  British  Drug  Houses  as  having  the  following 
color  changes: 

pH 4.2          4.8  5.4  6.8 

color red    yellow-       orange        yellowish 

ish  red        yellow        green 

pH 7.3  9.1          10.3        11.5 

color sap  greenish    violet    reddish 

green        blue  violet 

Bogen  (1927)  describes  a  mixture  with  a  range  of  from  pH  1  to 
pH  10.  His  receipt  is  as  follows. 

Phenol phthalein,  100  mgm.;  methyl  red,  200  mgm.;  dimethylaminoazo- 
benzene,  300  mgm.;  bromthymol  blue,  400  mgm.;  thymol  blue,  500  mgm. 
Dissolve  in  500  cc.  of  absolute  alcohol.  Add  tenth  normal  sodium  hy- 
droxide solution  until  the  red  disappears  and  the  solution  becomes  yel- 
low (pH  6.0). 

The  colors  produced  resemble  those  of  the  spectrum,  thus: 
Red       indicates  about  pH    2.0     (very  strongly  acid) 
Orange  indicates  about  pH    4.0     (strongly  acid) 
Yellow  indicates  about  pH    6.0     (weakly  acid) 
Green    indicates  about  pH    8.0     (weakly  alkaline) 
Blue       indicates  about  pH  10.0     (strongly  alkaline) 

Moir  (1917)  is  cited  as  using  a  mixture  of  methyl  red,  naphthol 
phthalein  and  phenolphthalein.  To  this  Carr  (1922)  adds  brom 
thymol  blue  or  cresol  phthalein,  or  cresol  red. 

Niklas  and  Hock  (1924)  are  cited  as  employing  the  following 
mixture:  one  volume  0.04  per  cent  brom  cresol  purple,  4  volumes 
0.04  per  cent  brom  phenol  blue,  6  volumes  0.02  per  cent  methyl 
red  and  4  volumes  0.04  per  cent  brom  thymol  blue.  Range  pH 
3.5  to  7.6. 

Felton  (1921)  used  equal  parts  of  methyl  red  and  brom  thymol 
blue  for  the  range  4.6  to  7.6  (unsatisfactory  between  5.6  and  6.2) ; 
methyl  red  and  brom  cresol  purple  4.6  to  7.0;  methyl  red  and 
thymol  blue  (rough)  1.2  to  9.0. 

Lizius  and  Evers  (1922)  cite  the  following: 


98 


THE  DETEEMINATION  OF  HYDROGEN  IONS 


ARBITRARY  NAME 

COMPONENTS 

pH  RANGE 

COLOR 

Methyl-thymol  blue 

Methyl  red  (1  part), 

4^10 

red-yellow-greenish 

. 

thymol     blue      (3 

blue 

parts) 

Phenol  violet 

Phenolphthalein     (1 

8-10 

yellow-blue-violet 

part),  thymol  blue 

(6  parts) 

Phenol-thymol 

Phenol  phthalein  (1 

8.3-11 

Colorless-pink- 

phthalein 

part),      thymol 

violet 

phthalein  (6  parts) 

Thymol  violet 

TropaeolinO  (1  part), 

9-13 

Yellow-green-blue- 

thymolphtnalein 

violet 

(4  parts) 

See  also  A.  Cohen  (1922),  Lizius  (1921)  and  Kolthoff  (1927)  on  mixed 
indicators. 

INORGANIC   INDICATORS 

Grunberg  (1924)  notes  that  complex  platinum  compounds 
behave  as  acid-base  indicators.  A  number  of  other  inorganic 
systems  have  been  used  either  as  involving  a  species  precipitated 
within  a  certain  zone  of  pH  or  as  involving  a  color  change.  See 
Houben  (1919),  Daniel  (1927). 


CHAPTER  V 

THEORY  OF  INDICATORS 

It  requires  a  long-necked  observer  to  see  the  whole  firmament  out 
of  one  window. — J.  ARTHUR  THOMSON. 

INTRODUCTION 

Indicator  theory  is  a  cross-roads.  Here  the  organic  chemist 
fetches  structural  formulas,  group  names,  and  correlations  be- 
tween molecular  architecture  and  "color."  The  physicist  brings 
his  account  of  the  radiant  energy  absorbed,  methods  for  its 
measurement,  and  schemes  for  its  translation  into  color.  The 
psychologist  pauses  here  to  philosophize  on  color  and  to  reflect 
upon  the  eye  as  a  differentiating  instrument.  The  physical 
chemist  has  called  the  cross-roads  his  own  for  he  has  tried  to 
bridge  the  gap  between  the  knowledge  supplied  by  chemistry  and 
that  supplied  by  physics;  but  his  sole  outstanding  contribution 
has  been  to  formulate  what  can  be  formulated  by  equilibrium 
equations.  The  colloid  chemist  has  occasionally  tried  to  direct 
the  traffic.  He  possesses  valuable  information  the  submission 
of  which  is  welcomed  as  a  service.  The  botanist  has  left  on  the 
roadside  the  historically  important  indicators  and  the  entomologist 
has  furnished  cochineal.  The  bacteriologist  has  brought  some  of 
the  first  records  of  dye  reduction  and  has  asked  of  the  plant  physiol- 
ogist what  part  acidity  and  what  part  reduction  plays  in  the 
beauty  of  the  autumn  landscape.  The  analyst  has  camped  here 
to  acquire  for  his  daily  use  the  information  that  comes  this  way. 
And  he  who  has  imagined  the  chemistry  to  come,  illustrated  with 
electron  orbits,  seeks  in  the  passing  throng  the  bearer  of  the 
Rosetta  stone  that  will  translate  speculative  ideas  concerning  the 
electronic  nature  of  organic  reactions  into  reasonable  certainties. 
Beside  him  stand  the  biochemist  and  pharmacologist,  awaiting 
the  formulation  of  what  neither  structural  chemistry  alone  nor 
physical  measurement  alone  seems  to  suggest  half  so  well  as  the 
imagination  which  has  been  fired  by  the  contributions  of  all. 
For  the  indicator  has  been  shown  to  be  a  labile  thing,  responsive 


100         THE  DETERMINATION  OF  HYDROGEN  IONS 

to  radiant  energy  and  to  the  pressures  of  protons  and  electrons, 
subject  to  structural  changes  and  physical  changes  in  delicate 
response  to  changes  in  the  environment.  It  is  the  embodiment  of 
sets  of  phenomena  having  an  "  all-togetherness"  with  which  our 
intellectual  methods  have  hardly  attained  the  power  to  cope. 
The  indicator  reminds  the  biochemist  of  many  things  in  the  chem- 
istry of  life  that  exhibit  an  analogous  "togetherness."  He  hopes 
that  a  complete  mastery  of  indicator  theory  may  take  its  part  in 
the  understanding  of  the  unity  and  lability  of  life  -chemistry. 

But  our  present  task  is  limited  and  commonplace.  We  must 
separate  and  assign  to  another  chapter  the  physical  phenomena 
of  light  absorption.  We  must  relegate  to  the  treatises  on  organic 
chemistry  details  of  structure  and  the  proofs  thereof  which  the 
thoughtful  student  will  require.  We  must  pass  over  the  fascinat- 
ing story  of  indicator  history  with  its  contributions  to  theory. 
In  short  we  must  select  only  that  which  is  essential  to  the  use  of 
indicators  for  the  measurement  of  hydrion  concentration.  Hence 
there  will  be  found  in  this  chapter  little  of  what  is  sometimes 
called  indicator  theory. 

OSTWALD'S  THEORY 

Let  us  deal  first  with  the  simple  theory  of  Ostwald  which  was 
constructed  on  the  primd  facie  evidence  that  indicators  do  behave 
as  acids  or  bases,  the  molecules  of  which  have  abilities  to  absorb 
radiant  energy  of  one  spectral  band,  and  the  ions  of  which  have 
abilities  to  absorb  radiant  energy  of  another  spectral  band. 

If  we  start  with  this  as  a  postulate,  it  is  evident  that  the  "color" 
of  an  indicator  should  change  with  the  pH  of  a  solution  exactly 
as  depicted  by  one  of  the  dissociation  curves*<iescribed  in  Chapter 
I.  If,  for  instance,  the  indicator  is  an  acid,  colorless  in  the  un- 
dissociated  form,  but  colored  when  dissociated  as  an  anion,  then 
the  change  of  color  with  the  hydrogen  ion  concentration  should 
conform  to  the  equation: 

Ka 


where  Ka  is  the  dissociation  constant  of  the  acid  indicator  and 
a.  is  the  degree  of  dissociation.     Assuming  that  such  a  relation 


OSTWALD'S  THEORY 


101 


does  hold,  let  us  determine  Ka  for  a  series  of  indicators  in  the 
following  way. 

From  the  above  equation  when  a  =  J,  Ka  =  [H+].  That  is, 
at  a  hydrogen  ion  concentration  corresponding  numerically  to  the 
dissociation  constant,  the  acid  is  half  dissociated.  At  such  a 
hydrogen  ion  concentration  a  colorless-to-red  indicator,  such  as 
phenolphthalein,  should  show  half  the  available  color;  and  a 
yellow-to-red  indicator,  such  as  phenol  red,  should  show  the  half- 
yellow,  half -red  state.  We  can  match  the  half-way  state  of  this 
first  solution  by  superimposing  two  solutions  each  of  a  depth 
equal  to  the  first,  if  we  have  in  one  of  the  superimposed  solutions 
only  the  yellow  form  and  in  the  other  only  the  red  form,  each 
concentration  equaling  half  the  concentration  in  the  first  solution. 
Such  an  arrangement  is  shown  diagraphically  in  the  following 
figure : 


Alkaline  solution 
(full  red)  5  drops 
indicator 

Known  pH  stand- 
ard 10  drops 
indicator 

Acid  solution  (full 
yellow)  5  drops 
indicator 

Water  blank 

We  may  not  know  at  the  beginning  at  what  pH  the  half  trans- 
formation may  occur,  so  we  vary  the  pH  of  the  standard  solution 
until  a  match  with  our  superimposed  solutions  does  occur.  Then 
we  have  found,  presumably,  the  hydrogen  ion  concentration  the 
numerical  value  of  which  is  that  of  the  dissociation  constant  of  the 
indicator.  Values  so  obtained  by  Clark  and  Lubs  (1917)  are 
given  in  table  13. 

This  is  the  method  of  Salm  (1906). 

Of  course  it  is  not  necessary  to  confine  attention  to  the  case 
where  each  of  the  superimposed  tubes  at  the  left  in  the  diagram 


102        THE  DETERMINATION  OF  HYDROGEN  IONS 

contains  the  same  quantity  of  the  indicator.  Various  divisions 
between  the  solutions  inducing  the  full  "alkaline  color"  and  the 
full  "acid  color"  may  be  made;  and  in  each  instance  a  color- 
match  may  be  made  by  adjusting  the  standard  buffer  until  the 
ratio  of  the  "acid  form"  to  the  "alkaline  form"  is  that  of  the 
artificial  division  between  the  acid  and  the  alkaline  solutions. 


TABLE  13 
Approximate  apparent  dissociation  constants  of  indicators 


INDICATOR 

Ka 

PK 

Phenol  sulf  on  phthalein  

1.2  X  10- 

7.9 

o-Cresol  sulfon  phthalein 

5  0  X  10- 

8  3 

Thymol  sulfon  phthalein  

1.2  X  10- 

8.9 

Carvacrol  sulfon  phthalein      .   .   . 

1  0  X  10" 

9  0 

a-Naphthol  sulfon  phthalein  

5.3  X  10" 

8.2 

Tetra  bromo  phenol  sulfon  phthalein 

7  9  X  10~§ 

4  1 

Di  bromo  o-cresol  sulfon  phthalein  

5.0  X  10~7 

6.3 

Di  bromo  thymol  sulfon  phthalein  

1.0  X  10~T 

7.0 

Phenol  phthalein  

2.0  X  10~10 

9.7 

o-Cresol  phthalein  

4.0  X  10~10 

9.4 

a-Naphthol  phthalein  

4.0  X  10~9 

8.4 

Methyl  red 

7  9  X  10"6 

5  1 

Ethyl  red  

4.0  X  10~6 

5.4 

Propyl  red  

4.0  X  10~e 

5.4 

Thymol  sulfon  phthalein  (acid  range)              

2.0  X  10~2 

1.7 

Thus  it  is  possible  to  determine  various  values  of  a  and,  by  means 
of  equation  (1)  or  (la),  to  determine  whether  the  simple  require- 


pH  =  pK  +  log 


a 


1  -  a 


(la) 


ments  of  the  Ostwald  theory  are  met  formally.  Figure  18  shows 
some  examples.  In  this  figure  the  experimental  points  are  shown 
lying  on  or  very  near  type  curves  drawn  to  correspond  to  equa- 
tion (la)  and  placed  with  reference  to  the  pH  axis  by  using  the 
average  value  of  pK  calculated  from  the  known  pH- values  of  the 
buffers  and  the  measured  values  of  a. 

As  indicated  in  Chapter  I  the  determination  of  the  dissociation 
curve,  or  of  the  half  transformation  point,  does  not  tell  us  whether 
we  are  dealing  with  the  dissociation  curve  of  an  acid  or  the  disso- 


INDICATOR   CONSTANTS 


103 


elation-residue  curve  of  a  base  or  vice  versa.  Thus  methyl  red 
is  treated  in  table  13  as  an  acid  and  plotted  in  figure  19  as  if  the 
color  were  associated  with  the  undissociated  form.  Methyl  red 
however  could  be  treated  as  a  base. 

Figure  19  shows  at  a  glance  that  an  indicator  of  the  simple  type 
we  have  assumed  has  no  appreciable  dissociation  and  consequently 
exists  in  only  one  colored  form  at  pH  values  beginning  about  2 
points  below  the  half  transformation  point,  while  at  the  same 
distance  above  this  point  the  indicator  is  completely  dissociated 
and  exists  only  in  its  second  form.  Between  these  limits  the 


Pep  cent  dissociation 
ooSSSSSc^Sg 

*. 

- 

•~ 

•%?• 

^f 

' 

38^, 

:^' 

~vf 

^ 

^ 

'  *^> 

Y 

/' 

^ 

jj/ 

/> 

, 

& 

y 

/ 

/ 

"/ 

/ 

% 

/# 

^ 

/ 

/ 

, 

& 

]t 

v 

% 

£d 

ir 

X 

& 

/ 

4 

p 

& 

% 

y\ 

& 

^ 

<6 

t 

A 

» 

7 

«? 

2 

y 

"  Broro-cpcsol  orccn'aL  38* 
•  Brom-cpesol  6re«nal  20* 
•  Chlop-phcnol  pcd  it  38* 
o  Chlop-phenol  red  at  20* 
*  6rom-cr>csol  purple  &L  38* 
+  Bronocpcsol  pupplc  &t  20* 
o  Phenol  red  at  36'zuid20* 

/ 

/ 

ti 

y 

/ 

7 

/' 

4 

'' 

%. 

'/ 

s 

1 

S 

*"' 

" 

' 

"" 

16  3.8  4.0  42  4.4  46  W  SO   U   S.4    5.6  5.J   6D  62   &4    66  tt   TO   12   T4    16   T8   S0    82   S.4    8.6  8.8    9.0  92  9.4 

pH 

FIG.  18.  CALCULATED  AND  OBSERVED  DISSOCIATION  CURVES  FOR  INDICA- 
TORS, USED  IN  URINE  pH  DETERMINATION 
(After  Hastings,  Sendroy  and  Robson  (1925)) 


color  changes  may  be  observed.  The  useful  range  of  such  an 
indicator  is  far  less  than  4  pH  units  for  optical  reasons  which  will 
be  discussed  in  Chapter  VII. 

The  illustration  (fig.  19)  will  show  how  in  choosing  a  set  of  indi- 
cators it  is  advantageous  to  include  a  sufficient  number,  if  reli- 
able indicators  can  be  found,  so  that  their  ranges  overlap.  It 
shows  that  each  of  the  indicators,  when  considered  to  be  of  the 
simple  type  we  have  assumed,  has  an  equal  range.  It  also  shows 
that  the  half  transformation  point  of  each  indicator  occurs  nearer 
one  end  of  the  useful  range,  the  useful  range  being  indicated  by 
the  shaded  part  of  the  curve,  This  aspect  will  be  discussed  later. 


VlO  MCI 


AS?ERGILL0S 
LIMIT 


B.PARA  TYPHI 

B.TYPHI  AOOL. 
B.COLI4.WIT 
PWEUHOCOCCOS  A&CL. 


BLOOD 


NH4OH 


100 


FIG.  19.  INDICATOR  CURVES  AND  SIGNIFICANT  pH  VALUES 

Shading  indicates  useful  range 

104 


V  TAUTOMERISM  105 

It  is  evident  that  if  the  actual  color  change  of  an  indicator 
varied  with  pH  in  accordance  with  a  curve  such  as  those  in  fig- 
ure 19,  and  if  the  true  dissociation  constant  were  accurately  known, 
then  the  hydrogen  ion  concentration  of  a  solution  could  be  deter- 
mined by  finding  the  per  cent  transformation  induced  in  the 
indicator.  Indeed  the  dissociation  constants  of  some  few  indi- 
cators have  been  determined  with  sufficient  accuracy  to  permit 
the  use  of  this  method  when  the  proper  means  of  determining  the 
color  intensities  are  used.  This  will  be  discussed  in  Chapters 

VI  and  VII. 

TAUTOMERISM 

The  following  sketch  of  tautomerism  is  purposely  made  brief. 
Its  consideration  leads  to  equations  which  reduce  to  the  forms 
used  with  the  Ostwald  theory.  Further  consideration  would  lead 
to  very  many  points  of  interest  but  these  are  involved  in  the  use 
of  indicators  which  are  ordinarily  rejected. 

Without  following  the  detail  of  the  reasoning  we  may  say  that 
certain  reactions  of  isatin  suggest  the  formula 

O 

c' 

C6H4          C=0 

\  / 
N 
H 

while  other  reactions  of  isatin  suggest  the  formula 

O 


C6H4  C—  OH 


Since  the  study  of  this  case  there  have  been  found  many  com- 
pounds which  act  now  in  one  way  and 'again  in  another,  according 
to  the  conditions  used  and  the  reagents  with  which  they  are 
attacked.  To  account  for  a  case  like  that  of  isatin  it  has  been 


106        THE  DETERMINATION  OF  HYDROGEN  IONS 

assumed  that  a  hydrogen  atom  moves  from  one  position  to  the 
other,  that  the  two  forms  are  in  dynamic  equilibrium  and  that 
when  a  reagent  attacks  one  form  the  other  rearranges  to  main- 
tain the  dynamic  equilibrium  and  thus  maintain  a  supply  of  the 
reacting  form. 

Among  the  types  are  those  with  the  lactam  and  lactim  struc- 
tures and  those  with  the  keto  and  enol  structures. 

—  C=0         —  C—  OH         —  O=0         —  C—  OH 

I  II  I  II 

—  NH  —  N  —  CH  —  C— 

I 
Lactam  Lactim  Keto  Enol 

From  one  and  the  same  compound  have  been  formed  derivatives 
corresponding  to  the  enolic  or  to  the  ketonic  structure.  The 
two  forms  of  the  original  substance  are  isomers;  but  to  emphasize 
their  labile  nature  Laar  (1885)  called  them  tautomers.  To  denote 
each  and  every  shade  of  meaning  in  explanations  which  differ,  we 
now  find  more  terms  than  we  can  afford  space  to  define.  We 
shall  use  the  word  tautomerism  to  denote  labile  isomeric  changes 
of  whatever  nature. 

Frequently  tautomeric  rearrangements  are  associated  with 
change  of  color.  The  argument  is  as  follows.  In  those  beautiful 
and  often  very  elaborate  series  of  syntheses  by  means  of  which 
the  organic  chemist  attains  an  orderly  view  of  structures,  it  is 
noted  that  color  is  associated  with  various,  particular  structures. 
When  a  colorless  ionogen  is  converted  into  an  ion,  a  colorless 
ion  might  be  expected.  But  the  fact  that  the  ion  is  colored  is 
the  occasion  for  believing  that  a  rearrangement  takes  place  with 
the  production  of  one  or  another  of  those  structures  which  have 
been  associated  with  color  production.  Groups  which,  by  their 
presence,  "produce"  color  are  called  chromophores.  Important 
chromophores  are: 


>C=0;>  C=S;>  C=N—  ;—  NO;—  N02;—  N=N—  ;= 


TAUTOMERISM 


107 


Of  particular  importance  to  our  subject  are  groups  such  as 
—  NH2,  —OH,  etc.,  which  are  not  chromophores  per  se  but  which 
may  have  a  profound  influence  upon  the  calling  forth  or  the 
suppression  of  the  appearance  of  color. 

Now  consider  the  case  of  crystal  violet.  The  "free  base"  will 
be  represented  by  formula  I.  It  contains  no  chromophore.  It 
is  colorless.  However  it  contains  substituted  amino  groups  and 
a  hydroxyl  group.  Therefore  it  is  an  ionogen,  potentially,  at 
least.  Imagine  that  the  free  base  is  brought  into  a  solution 
containing  hydrogen  ions  at  a  concentration  just  sufficient  to 
convert  one  of  the  groups,  and  one  only,  to  an  ion.  Perhaps  the 
first  result  will  be  the  addition  of  a  hydrion  to  one  of  the  three 
symmetrically  placed  dimethyl  amino  groups  as  represented  by 
formula  Ha.  Or  perhaps  the  first  result  will  be  the  stripping  of 
the  hydroxyl  group  from  the  carbon  to  leave  the  ion  lib.  Either 
ion  could  rearrange  to  form  the  ion  He,  the  first  by  elimination 
of  water  and  shift  of  electrons;  the  second  by  shift  of  electrons 
alone.  Now  He  contains  the  chromophore  group,  the  quinone 
group,  which  "accounts  for"  the  color  of  the  ion.  It  is  therefore 
the  preferred  way  of  representing  the  ion. 

We  may  now  note  a  matter  of  considerable  importance.  If  in 
fact  there  be  a  rearrangement  which  resembles  the  transformation 
of  Ha  or  lib  into  He,  the  rearrangement  is  spontaneous  and  repre- 
sents the  persistance  of  the  more  stable  form.  Its  direct  control 
is  often  beyond  our  power,  although  it  may  be  possible  by  taking 
advantage  of  the  slowness  of  rearrangement  in  a  rare  instance  to 


(CH3)2N 


N(CH3). 


C— OH      (CH3)2N 


H+ 

N(CH3)2 


(CH3)S 


N(CH3)S 


Ha 


108 


THE    DETERMINATION    OF    HYDROGEN    IONS 


N(CH3)2 


(CH 


IV 


form  a  derivative  which  rearranges  less  readily  than  the  original 
tautomer.  On  the  other  hand  the  first  step,  whereby  the  ion  is 
formed,  appears  to  be  under  control  by  the  hydrion  concentration 
of  the  solution.  It  must  not  be  assumed  that  a  measurement  of 
the  "ionization  constant"  evaluates  the  primary  ionization  alone. 
The  rearrangement,  being  spontaneous,  leads  to  the  formation  of 
the  more  stable  tautomer  and  the  process  of  rearrangement  is  an 
integral  part  of  the  whole  process  of  which  the  initial  and  final 
steps  are  only  parts.  Later  we  shall  see  that  an  ionization  con- 
stant is  a  function  of  ionization  energy.  In  the  case  at  hand  there 
may  be  energy  involved  in  the  rearrangement.  Our  measurements 


V  TAUTOMERISM  109 

are  incapable  of  separating  the  two  energies,  and  we  shall  find 
ourselves  describing  the  total  energy  change  between  I  and  He 
as  if  it  were  that  of  an  ionization  of  I  directly  to  He. 

Of  course  we  must  assume  that  any  one  of  the  forms  shown  is 
capable  of  existence,  in  small  amounts  at  least,  under  any  con- 
ditions. It  is  assumed  that  acetic  acid  molecules,  for  instance, 
occur  in  minute  amounts  in  very  alkaline  solutions  of  acetate. 
Nevertheless  there  remains  a  radical  distinction  between  the 
ionogen  and  any  one  of  the  ions  depicted  above.  The  latter  are 
true  tautomers,  the  dominance  of  any  one  of  which  is  determined 
by  the  stability  of  the  internal  configuration.  The  ionogen  or  a 
tautomer  thereof  differs  from  the  ion  or  a  tautomer  thereof  by 
the  energy  involved. 

There  may  now  be  noted  a  rather  interesting  matter.  By 
following  the  elementary  principles  for  the  writing  of  formulas 
as  given  for  instance  in  Valence  (G.  N.  Lewis,  1923),  we  arrive  at 
the  following  configuration  for  the  group  attached  to  the  quinone 
ring  of  He. 

H  +  H 
H:C:N:C:H 

ii ::  ii 

:C: 

The  nitrogen  and  each  carbon  are  surrounded  by  octets  of  elec- 
trons. However,  carbon  has  a  charge  of  -f-  four  to  be  neutralized, 
nitrogen  has  a  charge  of  +  five  to  be  neutralized  and  hydrogen  a 
charge  of  +  one  to  be  neutralized.  Not  only  does  this  group 
lack  one  electron  required  to  fulfil  these  neutralizations  but  the 
ion  as  a  whole  lacks  one  electron  required  to  complete  the  neutral- 
ization at  all  points.  Therefore  lib  and  He  differ  only  in  the 
positions  of  the  electron  pairs  and  of  the  odd  electron.  If  one 
is  willing  to  place  any  significance  in  this  rather  crude  way  of 
depicting  the  situation,  he  has  already  accepted  some  degree  of 
shift  of  an  electron,  if  lib  and  He  are  to  be  called  tautomers  in 
dynamic  equilibrium. 

There  have  been  attempts  to  relate  such  electron  shifts,  which 
might  be  oscillations  capable  of  resonating  with  radiant  energy, 
to  color.  The  modern  spectroscopist  would  doubtless  not  consent 


110         THE  DETERMINATION  OF  HYDROGEN  IONS 

to  this  for  various  reasons.  Indeed  the  gap  between  the  in- 
formation supplied  by  structural  chemistry  and  that  demanded 
for  a  solution  of  the  problem  in  terms  of  spectroscopy  is  so  large 
that  it  would  be  inappropriate  to  our  present  purposes  to  enter 
the  discussion  and  recount  the  many  partial  theoretical  ad- 
vances. However  it  would  appear  that  a  structural  formula  for 
a  "tautomer"  may  be  merely  an  expression  of  a  limiting  state,  a 
state  which  perhaps  represents  crudely  a  main  feature  important 
to  the  rationalization  of  chemical  reactions  but  nevertheless  a 
state  which  is  perhaps  of  no  particular  importance  to  our  present 
purpose.  We  shall  detect  a  hint  of  this  in  a  further  treatment 
of  the  equations. 

In  the  meanwhile  let  us  proceed  as  if  the  molecule  or  ion  re- 
adjusts in  large  jumps  to  those  configurations  which  are  usually 
described. 

Consider  the  case  of  crystal  violet  further.  Assume  that 
further  increase  in  the  hydrogen  ion  concentration  will  drive 
hydrions  upon  the  comparatively  weak,  substituted  amino  groups 
forming  successively  the  ions  III  and  IV.  Adams  and  Rosen- 
stein  (1914),  by  an  analysis  of  the  absorption  bands,  correlate 
the  changes  of  color  with  the  stepwise  addition  of  hydrions  to 
the  dimethyl  amino  groups. 

To  indicate  more  specifically  the  structures  assigned  to  particular 
systems  we  may  deal  briefly, with  a  few  of  the  other  important 
indicators. 

The  case  of  phenolphthalein  is  often  represented  as  follows: 


OH     OH 


— C—0  f   \COOH  (    \COO 


V  TAUTOMERISM  111 

The  lactone  form  V  is  a  tautomer  of  VI  which  may  undergo 
primary  ionization  at  the  carboxyl  or  phenolic  group.  The 
resulting  ion  can  be  represented  as  rearranging  in  several  ways. 
A  probable  form  is  VII.  This  or  its  tautomer  can  then  suffer 
secondary  ionization  and  if  the  primary  ion  is  VII  the  result  is 
VIII 


o-    o- 


coo  /\-  coo 


VIII 

If  this  is  rewritten  with  the  extra  electrons  situated  as  far  as  possible 
from  the  center,  carbon  is  left  positive  and  is  satisfied  by  addition 
of  hydroxyl.  Hence  IX  is  sometimes  used  to  represent  the  color- 
less carbinol  found  in  very  alkaline  solutions. 

According  to  Acree  and  his  students  (Acree,  1908)  (Acree  and 
Slagle,  1908)  (Lubs  and  Acree,  1916)  the  chief  color  change  in 
phenolphthalein  is  associated  with  the  presence  of  a  quinone 
group  and  with  the  ionization  of  one  of  the  phenol  groups.  In 
the  sulfon  phthalein  series  of  indicators  Acree  and  his  students 
(White,  1915,  and  White  and  Acree,  1918)  have  found  much  the 
same  sort  of  condition. 

In  the  sulfonphthalein  group  of  indicators  we  have  to  deal 
with  poly-acids;  but  as  Acree  has  shown,  the  dissociation  con- 
stant of  the  strong  sulfonic  acid  group  is  so  very  much  greater 
than  that  of  the  weak  phenolic  group,  with  which  the  principal 
color  change  is  associated,  that  there  is  no  serious  interference. 
As  shown  in  Chapter  I  we  may,  therefore,  plot  the  curve  for  the 
chief  "color-change"  as  if  we  were  dealing  with  a  univalent  acid. 


112  THE    DETERMINATION   OF   HYDROGEN    IONS 

The  structures  of  all  the  sulfon  phthaleins  are  analogous  to 
that  of  phenol  sulfon  phthalein  (phenol  red)  whose  various  tau- 
tomers  are  given  by  Lubs  and  Acree  (1916)  in  the  following 
scheme : 

C6H4OH 
I 
C6H4— C(C6H4OH)2  ->  C6H4— C— C6H4OK  ->  C6H4— C(C8H4OK) , 

I  II  II 

S02  —  0  S02  —  O  S02  —  0 

A  colorless  B  colorless  C  colorless 


C6H4OH  C6H4OH  C6H4OH 

I  I  I 

C6H4— C:C6H4:0    ->    C6H4— C:CCH4:O    ->    C6H4— C:C6H4:0 

I  I  'I 

S02— OH  S020-  +  H+  S020-  +  K+ 

D  slightly  colored          E  slightly  colored  F  slightly  colored 

i 

C6H4O-  K+  C6H40-  +  K+ 

I        I      I 
C6H4— C:CcH4:0  C6H4— C:C6H4:0 

I  I 

S020-  +  K+  < — >        S020-  +  K+ 

H  deeply  colored  G  deeply  colored 


Of  course  such  a  table  represents  possibilities  (some  of  them 
remote)  and  says  nothing  about  the  relative  probability  of  any 
specific  form.  This  must  be  very  carefully  argued  by  a  series  of 
analogies  and  by  all  the  manifold  devices  of  organic  chemistry. 

In  the  case  of  an  azo  indicator  such  as  methyl  orange,  X,  in 
alkaline  solution, 

s  ^  /  \ 

X 

we  find  the  chromophore  group  —  N  =  N—  associated  with  a 
yellow  color.  On  driving  a  hydrion  into  this  structure  (by 
decrease  of  pH)  there  would  be  expected  XI 


TAUTOMERIC   EQUILIBRIA  113 

N(CH3)2  H+  XI 


which  may  rearrange  to  XII 

H  , x   + 

s— N— N=<          >  N(CH3)2  XII 


with  quinoid  structure  and  red  color.     See  Stieglitz  (1903). 

The  question  now  is  this.  Given  these  tautomers,  will  their 
inclusion  in  the  equilibrium  equation  affect  the  end  result  of  the 
Ostwald  theory? 

EQUATIONS  INVOLVING   TAUTOMERS 

In  a  previous  section  it  was  assumed  that  the  theory  of  indicators 
may  be  treated  in  the  simple  manner  outlined  by  Ostwald.  His 
theory  does  not  embrace  the  possibility  of  a  radical  change  in 
structure  with  distinctive  properties  pertaining  to  each  structure. 
In  the  section  immediately  preceding  this,  the  concept  of 
tautomerism  was  briefly  and  inadequately  outlined.  There  we 
found  that  the  ionization  of  one  group  may  be  followed  by  a 
rearrangement  of  the  molecule.  If  the  tautomer  is  a  distinct 
entity  there  may  be  ascribed  to  any  ionogenic  group  that  it  may 
contain  a  distinctive  ionization  constant.  Let  us  therefore  formu- 
late the  acid-base  equilibria  of  these  systems  by  including  the 
ionization  constants  of  the  separate  tautomers  and  follow  the 
consequences  to  the  rather  curious  end. 

Merely  to  illustrate  a  principle  in  outline  assume  two  tautomers 
HTi  and  HT2  and  let  HTi  alone  ionize  as  an  acid.  The  equilib- 
rium state  for  the  ionization  is  described  by 

[THIH+] 

lirT"       a 

For  the  equilibrium  of  the  tautomers 

[HTl!        K  to) 

[HTJ=  KT 
The  combination  of  (2)  and  (3)  gives: 

[HT21          K°  KT  =  K  " 


114  THE   DETERMINATION   OF   HYDROGEN   IONS 

Now  suppose  that  Tf  furnishes  one  color  and  either  HT\  or 
HT2  another  color.  Since  (4)  has  the  form  of  the  ordinary  equa- 
tion (K'a  replacing  the  ordinary  Ka)  it  is  obvious  that  the  color- 
change  will  depend  on  [H+j  in  the  manner  already  described. 
Regarding  the  matter  from  another  point  of  view  we  perceive 
that  a  determination  of  the  equilibrium  constant  from  the  data 
for  the  color-change  would  not  reveal  whether  this  constant  is  a 
simple  acid  dissociation  constant  (Ka  of  2)  or  a  complex  constant 
(K'.  of  4). 

In  one  sense  this  situation  is  not  unlike  that  which  obtains  in 
the  case  of  an  '  'ordinary"  acid.  There  may  be  no  occasion  to 
ascribe  a  tautomeric  form  to  one  of  these  "ordinary"  acids  but  it 
would  require  considerable  skill  to  demonstrate  that  there  are  no 
tautomeric  forms.  There  is  every  reason  to  believe  that  dif- 
ferent states  of  hydration  occur  and  a  complete  equation  should 
contain  the  equilibrium  constants  for  the  hydration.  We  simply 
agree  to  ignore  this  as  we  agree  to  ignore  the  hydration  of  the 
hydrion  in  ordinary  formulations.  See  also  page  561  for  a  dis- 
cussion of  the  use  of  the  sum  of  the  concentrations  of  HaCOa  and 
COs  in  formulating  carbonate  equilibria. 

The  too  simple  treatment  given  above  must  now  be  elaborated  ; 
for  the  ionization  of  the  second  tautomer  was  neglected  and  may 
modify  the  conclusion.  With  slight  changes  of  notation  we  shall 
follow  the  treatment  given  by  Noyes  (1910). 

The  three  fundamental  equations  are: 
Ionization  of  tautomer  1; 

[TT1  [H+] 

Kal 


=  Ka2  (6) 


Ionization  of  tautomer  2  : 

[T2~] 


[HT2] 
Tautomerism : 

[HT2] 
[HTJ 


V  TAUTOMERIC    EQUILIBRIA  115 

Multiply  (6)  by  (7),  add  (5)  to  the  product  and  for  [HTJ  in  the 
denominator  of  the  resulting  equation  substitute  its  equivalent 
[HTJ  +  [HT2]  which  can  be  obtained  from  7>  There  resultg 


[H+]  ([17]  +  [IT])  =  K..  +  K.,  KT  = 
[HTJ  +  [HTJ  1  +  KT 

Now  if  [T~]  represents  the  sum  [Tr]  +  [Tr]  and  if  [HT]  repre- 
sents the  sum  [HT:]  +  [HT2],  we  have; 

[T-]  [H+]  _  ,  , 


Again  we  have  in  (8)  an  equation  of  the  usual  form.    Applying 
to  it  the  derivation  given  on  page  14  we  find 


K' 

a 


K'  +  [H+] 

where  a  is  now  the  ratio 


[T-]  +  [HT]      [Tr]  +  [TTJ  +  [HTJ  +  [HT,] 
or 

sum  of  all  ions 


a  = 


sum  of  all  forms 


The  ordinary  dissociation  curve  will  then  represent  the  degree 
of  color- transformation  only  when  the  sum  [Ti~]  +  [T2~]  is  prac- 
tically equal  to  either  [Ti~]  or  [T2~],  according  to  which  tautomer 
is  associated  with  the  color.  A  suggested  explanation  of  the 
fact  that  such  curves  do  represent  closely  the  color  degree  in 
certain  instances  is  that  KT  is  very  large  or  very  small.  Formal- 
istically,  at  least,  an  equally  good  suggestion  is  that  [Ti~]  + 
[Tj~]  or  [HTi]  +  [HTJ  is  merely  an  expression  of  a  formal  sum 
of  two  limiting  states  the  shift  between  which  is  only  a  part,  but 
nevertheless  an  integral  part,  of  a  phenomenon  with  which  there 
may  be  associated  absorption  of  radiant  energy. 

Assuming  the  first  and  more  usual  suggestion,  we  then  find 


116  THE    DETERMINATION    OF   HYDROGEN   IONS 

that  the  consideration  of  the  tautomeric  equilibria  only  modifies 
the  original  Ostwald  treatment  to  this  extent :  the  found  dissocia- 
tion constant  is  a  function  of  the  several  equilibrium  and  ioniza- 
tion  constants  involving  the  different  tautomers.  It  is  what 
Acree  calls  the  "total  affinity  constant,"  or  what  Noyes  calls  the 
"apparent  dissociation  constant."  As  Stieglitz  (1903)  and  others 
have  pointed  out,  it  is  the  state  of  these  compounds,  their  exist- 
ence in  a  dissociated  or  undissociated  condition,  which  determines 
the  stability  of  any  one  form. 

But  there  remains  a  view  of  the  together-ness  of  the  whole 
set  of  phenomena  which  cannot  be  well  formulated  when  we  start 
with  the  assumption  of  independent  entities  having  independent 
ionization  constants.  The  simpler  view  is  perhaps  the  better  in 
that  it  permits  us  to  conceive  of  the  departure  of  the  hydrion  and 
the  rearrangement  as  a  unified  process  and  the  hydrion  associa- 
tion and  re-rearrangement  as  a  unified  process.  Then  the  energy 
of  ionization  is  linked  inseparately  with,  or  rather  is,  an  integral 
part  of  any  energy  change  involved  in  the  rearrangement  of  the 
molecule.  Because  of  this  together-ness  we  appear  to  be  dealing 
with  a  most  simple  case  of  a  simple  dissociation  when  we  measure, 
by  the  means  described  above,  the  apparent  ionization  constant. 

MULTIVALENT  INDICATORS 

Many  indicators  will  not  conform  to  the  treatment  of  a  uni- 
valent  acid  because  there  are  two  or  more  distinctive  groups  which 
may  ionize  either  near  the  same  level  of  pH  or  at  different  levels 
of  pH. 

An  instance  of  the  first  is  phenolphthalein.  It  was  shown  by 
Acree  (1908)  and  by  Wegscheider  (1908)  that  the  dissociations  of 
the  carboxyl  and  of  a  phenolic  group  occur  near  together.  The 
proper  equations  to  apply  in  such  a  case  were  developed  by  Acree 
(1907,  1908)  and  by  Wegscheider  (1908,  1915). 

In  the  case  of  a  sulphonphthalein  the  "strong"  sulfonic  acid 
group  is  already  ionized  when  the  phenolic  group  undergoes  its 
transformation.  The  "spread"  between  the  dissociation  curves 
is  then  sufficient  to  permit  the  drawing  of  the  curve  of  chief  color 
change  as  if  of  a  univalent  acid,  the  undissociated  portion  of 
which  is,  however,  the  sulfonate  ion. 

There  are  also  indicators  with  two  or  more  basic  groups,  e.g. 


V  TIME   CHANGES  117 

crystal  violet;  and  indicators  of  amphoteric  nature,  e.g.  methyl 
orange. 

In  case  any  two  ionization  constants,  expressed  in  comparable 
terms,  have  values  of  the  same  order  of  magnitude,  it  is  necessary 
to  use  the  complete  equation  and  to  avoid  the  inevitable  error 
that  would  be  involved  in  a  treatment  as  if  of  a  univalent  acid 
or  base. 

MORE   COMPLEX   EQUILIBRIA 

A  displacement  of  the  position  of  and  an  alteration  of  the  form 
of  a  dissociation  curve  occurs  when  one  of  the  components  of  a 
system  precipitates.  The  precipitate  is  a  special  case  of  an  aggre- 
gate which  may  remain  in  suspension.  Imagine  then  an  indicator 
of  high  molecular  weight  tending  to  form  aggregates  which  bring 
its  "solutions"  within  the  category  of  colloidal  "solutions." 
The  presence  of  the  aggregate  per  se  interferes  with  simple  formu- 
lation. In  addition  there  may  occur  surface  phenomena  and 
various  types  of  adsorption.  These  effects  will  be  superimposed 
upon  the  basic  equilibrium  relations  in  an  inseparable  way  and 
with  the  failure  of  a  simple  quantitative  formulation  the  flood- 
gates of  speculation  open.  Many  indicators  such  as  congo  red 
must  be  turned  over  to  the  students  of  colloid  chemistry  before 
a  full  account  of  their  conduct  can  be  given.1  Until  that  account 
is  clear  these  indicators  and  partial  accounts  of  their  conduct 
had  best  be  studiously  avoided  except  as  objects  of  research. 

THE   TIME  FACTOR 

In  the  application  of  indicators  we  take  advantage  of  the  accom- 
modating way  in  which  they  adjust  their  equilibria  practically 
instantaneously  and  it  hardly  ever  occurs  to  us  to  imagine  the 
embarrassing  predicament  we  would  be  in  if  they  did  not  adjust 
instantaneously.  Yet  there  are  such  indicators  and  one  must  be 
on  his  guard  if  the  occasion  arises  in  which  they  are  put  to  use. 
S0rensen  has  one  or  two  in  his  list.  "China  Blue"  used  by 
Bronfenbrenner  (1918)  is  another,  and  a  disconcerting  indicator 
it  is  found  to  be  when  the  very  different  rates  of  transformation  of 
different  commercial  samples  are  compared.  Equilibrium  equa- 

1  See  also  Zsigmondy  (1924)  on  the  degree  of  dispersion  of  some  dyes 
which  have  been  used  as  indicators. 


118  THE   DETERMINATION    OF   HYDROGEN   IONS 

tions  are  inadequate  to  deal  with  this  "time  effect"  and  equilib- 
rium studies  are  easily  put  in  jeopardy  by  the  use  of  such  indi- 
cators. For  discussion  of  the  time  changes  we  refer  the  reader 
to  the  very  numerous  papers  of  Hantzsch  and  his  co-workers. 
Indicators  involving  a  time  adjustment  are  most  frequently  en- 
countered among  the  triphenylmethane  dyes. 


CHAPTER  VI 
APPKOXIMATE  DETERMINATIONS  WITH  INDICATORS 

//  you  can  measure  that  of  which  you  speak,  and  can  express  it  by  a 
number,  you  know  something  of  your  subject;  but  if  you  cannot 
measure  it,  your  knowledge  is  meagre  and  unsatisfactory. — LORD 
KELVIN. 

The  distinctive  advantages  of  the  indicator  method  are  the 
ease  and  the  rapidity  with  which  the  approximate  hydrogen  ion 
concentration  of  a  solution  may  be  measured.  The  introduction 
of  improved  indicators,  the  charting  of  their  pH  ranges,  better 
definition  of  degree  in  "acidity"  or  "alkalinity,"  and  the  illumina- 
tion of  the  theory  of  acid-base  equilibria  have  developed  among 
scientific  men  in  general  an  appreciation  of  how  indefinite  were 
those  old,  favorite  terms — "slightly  acid,"  "distinctly  alkaline," 
"neutral,"  etc.  There  is  now  a  clear  recognition  of  the  distinct 
difference  between  quantity  and  intensity  of  acidity;  and  for 
each  aspect  there  may  be  given  numerical  values  admitting  no 
misunderstanding. 

Furthermore  the  clarification  of  the  subject  has  brought  a 
perspective  which  may  show  where  accuracy  is  unnecessary  and 
where  fair  approximation  is  desirable.  In  such  a  case  the  in- 
vestigator turns  to  the  indicator  method  knowing  that  even  if  his 
results  are  rough  they  can  still  be  expressed  in  numerical  values 
having  a  definite  meaning  to  others. 

A  very  good  approximation  may  be  attained  by  color  memory 
and  without  the  aid  of  the  standard  buffer  solutions  or  of  the 
systems  presently  to  be  described  in  which  the  standard  buffer 
solutions  are  dispensed  with. 

An  excellent  procedure  for  rough  measurements  is  to  utilize 
the  colors  of  indicators  with  overlapping  ranges.  For  instance, 
Cohen  (1923)  gives  the  following  table. 

119 


120 


THE  DETERMINATION  OF  HYDROGEN  IONS 


INDICATOR 

COLOR  AT  pH— 

4.5 

5.0 

5.5 

6.0 

6.5 

Methyl  red  

red 
yellow 
yellow 
yellow 

red 
green 
yellow 
yellow 

orange 
blue 
yellow 
yellow 

yellow 
blue 
orange 
yellow 

yellow 
blue 
red 
green 

Brom  cresol  green  

Brom  phenol  red 

Brom  thymol  blue     

The  reader  may  elaborate  such  a  table  by  use  of  the  color 
chart  (page  65). 

To  establish  a  color  memory,  as  well  as  to  refresh  it,  a  set  of 
"permanent"  standards  is  convenient.  These  may  be  prepared 
with  the  standard  buffer  solutions  in  the  ordinary  way,  protected 
against  mold  growth  by  means  of  a  drop  of  toluol,  and  sealed 
by  drawing  off  the  test  tubes  in  a  flame  or  by  corking  with  the 
cork  protected  by  tinfoil  or  paraffin.  For  temporary  exhibition 
purposes  long  homeopathic  vials  make  very  good  and  uniform 
containers.  They  may  be  filled  almost  to  the  brim  and  a  cork 
inserted,  if  a  slit  is  made  for  the  escape  of  excess  air  and  liquid. 
The  slit  may  then  be  sealed  with  paraffin.  A  hook  of  spring- 
brass  snapped  about  the  neck  makes  a  support  by  which  the  vial 
may  be  fastened  to  an  exhibition  board.  A  neater  container  is 
the  so-called  typhoid-vaccine  ampoule  which  is  easily  sealed  in 
the  flame.  Standards  having  considerable  permanency  are  made 
by  sealing  buffer-indicator  mixtures  in  Pyrex  glass  tubes  and  steril- 
izing them  by  the  ordinary  intermittent  method. 

If  one  of  a  series  of  standards  so  prepared  should  alter,  the 
change  can  generally  be  detected.  But  if  all  in  a  series  should 
change,  it  may  be  necessary  to  compare  the  old  with  new  stand- 
ards. Because  such  changes  do  occur,  "permanent"  standards 
are  to  be  used  with  caution.  The  sulfonphthalein  indicators 
make  fairly  permanent  standards  but  methyl  red  which  is 
an  important  member  of  the  series  of  indicators  recommended  by 
Clark  and  Lubs  (1917)  often  deteriorates  within  a  short  time. 

As  an  aid  to  memory  the  dissociation  curves  of  the  indicators 
are  helpful  even  when  used  alone.  The  color  chart  shown  in 
Chapter  III  is  a  still  better  aid  to  memory  and  within  the  limita- 
tions mentioned  the  colors  may  be  used  as  rough  standards. 


VI  GILLESPIE    METHOD  121 

COLORIMETRIC  DETERMINATION    OF  HYDROGEN  ION  CONCENTRATION 
WITHOUT  THE   USE   OF   STANDARD    BUFFER   SOLUTIONS 

We  have  already  seen  that  if  an  indicator  is  an  acid,  its  degree 
of  dissociation,  a,  is  related  to  the  hydrogen  ion  concentration  of 
the  solution  by  the  equatkm 

1  -a 


[H+]  =  Ka 


a 


We  have  also  seen  that  if  Ka,  the  true  dissociation  constant  is 
replaced  by  the  so-called  apparent  dissociation  constant,  K'a, 
which  is  a  function  of  Ka  and  of  the  constants  of  tautomeric 
equilibria,  then  a  represents  the  degree  of  color  transformation. 
We  then  have 


K'a  —  — 


or  the  more  convenient  form 


PH  -  PK'a  +  log  --  (1) 

1  —  a 

where  a  may  now  be  considered  as  the  degree  of  color  transforma- 
tion. If,  for  instance,  an  indicator  conducts  itself  as  a  simple 
acid  having  the  apparent  dissociation  constant  1  X  10~6  (pK'a 
=  6.0),  we  can  construct  the  dissociation  curve  with  its  central 
point  at  pH  =  6.0.  Then  there  can  be  read  from  the  curve,  or 
calculated  from  the  corresponding  equation,  the  percentage  color 
transformation  at  any  given  value  of  pH.  Proceeding  with  these 
simple  and  sometimes  unjustifiable  assumptions  we  can  now 
devise  a  very  simple  way  of  measuring  the  degree  of  color  trans- 
formation. The  following  is  quoted  from  Gillespie  (1920). 

We  may  assume  that  light  is  absorbed  independently  by  the  two  forms 
of  the  indicator,  and  hence  that  the  absorption,  and  in  consequence  of  this 
the  residual  color  emerging,  will  be  the  same  whether  the  two  forms  are 
present  together  in  the  same  solution  or  whether  the  forms  are  separated 
for  convenience  in  two  different  vessels  and  the  light  passes  through  one 
vessel  after  the  other.  Therefore,  if  we  know  what  these  percentages  are 
for  a  given  indicator  in  a  given  buffer  mixture,  we  can  imitate  the  color 
shown  in  the  buffer  mixture  by  dividing  the  indicator  in  the  proper  pro- 
portion between  two  vessels,  and  putting  part  of  it  into  the  acid  form  with 
excess  of  acid,  the  rest  into  the  alkaline  form  with  excess  of  alkali. 


122 


THE  DETERMINATION  OF  HYDROGEN  IONS 


Gillespie  sets  up  in  the  comparator  (see  page  171)  two  tubes, 
one  of  which  contains,  for  example,  three  drops  of  a  given  indicator 
fully  transformed  into  the  acid  form,  and  the  other  of  which  con- 
tains seven  drops  of  the  indicator  fully  transformed  into  the  alka- 
line form.  The  drop  ratio  3:7  should  correspond  to  the  ratio  of 
the  concentrations  of  acid  and  alkaline  forms  of  ten  drops  of  the 
indicator  in  a  solution  of  that  pH  which  is  shown  by  the  disso- 
ciation curve  of  the  indicator  to  induce  a  seventy  per  cent  trans- 
formation. If  then  the  two  comparison  tubes  and  the  tested 

TABLE  14 

Gillespie's  table  of  pH  values  corresponding  to  various  drop-ratios 


DROP-RATIO 

BROM- 
PHENOL 
BLUE 

METHYL 
RED 

BROM- 
CRE80L 
PURPLE 

BROM-- 
THTMOL 
BLUE 

PHENOL 
RED 

CRESOL  RED 

THTMOL 

BLUB 

1:9 

3.1 

4.05 

5.3 

6.15 

6.75 

7.15 

7.85 

1.5:8.5 

3.3 

4.25 

5.5 

6.35 

6.95 

7.35 

8.05 

2:8 

3.5 

4.4 

5.7 

6.5 

7.1 

7.5 

8.2 

3:7 

3.7 

4.6 

5.9 

6.7 

7.3 

7.7 

8.4 

4:6 

3.9 

4.8 

6.1 

6.9 

7.5 

7.9 

8.6 

5:5 

4.1 

5.0 

6.3 

7.1 

7.7 

8.1 

8.8 

6:4 

4.3 

5.2 

6.5 

7.3 

7  9 

8.3 

9.0 

7:3 

4.5 

5.4 

6.7 

7.5 

8.1 

8.5 

9.2 

8:2 

4.7 

5.6 

6.9 

7.7 

8.3 

8.7 

9.4 

8.5:1.5 

4.8 

5.75 

7.0 

7.85 

8.45 

8.85 

9.55 

9:1 

5.0 

5.95 

7.2 

8.05 

8.65 

9.05 

9.75 

Produce 
acid  color  < 
with 

1  cc.  of 
0.05M 
HC1 

1  drop 
of 
0.05M 
HCJ 

1  drop 
of 
0.05M 
HC1 

1  drop 
of 
0.05M 
HC1 

1  drop 
of 
0.05M 
HC1 

1  drop  of 
2  per  cent 
H2KPO4 

1  drop  of 
2  per  cent 
H2KPO4 

solution  are  kept  at  the  same  volume,  and  the  view  is  through 
equal  depths  of  each,  the  two  superposed  comparison  tubes  should 
match  the  tested  solution. 

Barnett  and  Chapman  (1918)  applied  this  method  with  one 
indicator,  phenol  red,  but  without  using  the  dissociation  curve. 
Gillespie  (1920)  extended  the  procedure  to  several  other  indicators 
and -made  use  of  the  dissociation  curves  so  that  he  was  able  to 
smooth  out  to  more  probable  values  the  experimental  data  re- 
lating drop  ratios  to  pH.  This  is  important  because  the  experi- 
mental error  in  judging  color  is  not  inconsiderable  and  if  the 


VI  GILLESPIE   METHOD  123 

purely  empirical  data  he  made  the  sole  basic  standardization  of 
the  method  there  may  be  involved  a  systematic  error,  which, 
added  to  the  error  of  the  individual  measurement  may  make  the 
cumulative  error  unnecessarily  large.  That  this  had  already 
occurred  was  indicated  by  Gillespie's  comparison  of  the  values 
for  the  drop  ratios  of  phenol  red  given  by  Barnett  and  Chapman 
on  the  one  hand  and  the  report  of  the  bacteriologists'  committee 
(Conn,  et  al,  1919)  on  the  other  hand. 

Gillespie  found  the  correspondence  between  the  experimental 
and  the  theoretical  results  predicted  on  the  basis  of  the  simpli- 
fying assumptions  mentioned  above  to  be  very  good  for  the  sul- 
fonphthaleins,  doubtless  because  of  the  reasons  mentioned  in 
Chapter  V.  He  also  showed  good  correspondence  in  the  case  of 
methyl  red  but  reiterated  the  fact  that  phenolphthalein  cannot 
be  treated  by  means  of  the  simple  dissociation  curve  for  a  mono- 
acidic  acid,  as  was  mentioned  in  Chapter  V. 

In  table  14  are  given  the  pH  values  corresponding  to  various 
drop  ratios  of  seven  indicators  as  determined  by  Gillespie.  At 
the  bottom  of  the  table  are  shown  the  quantities  of  acid  used  to 
obtain  the  acid  color  in  each  case.  Acid  phosphate  instead  of 
hydrochloric  acid  is  used  in  two  cases  because  the  stronger  acid 
might  transform  the  indicator  into  that  red  form  which  occurs 
with  all  the  sulfonphthalein  indicators  at  very  high  acidities. 
The  0.05  M  HC1  is  prepared  with  sufficient  accuracy  by  diluting 
1  cc.  concentrated  hydrochloric  acid  (specific  gravity  1.19)  to 
240  cc. 

The  alkaline  form  of  the  indicator  is  obtained  in  each  case 
with  a  drop  of  alkali  (two  drops  in  the  case  of  thymol  blue). 
The  alkali  solution  used  for  this  purpose  may  be  prepared  with 
sufficient  accuracy  by  making  a  0.2  per  cent  solution  with 
ordinary  stick  NaOH.  The  indicator  solutions  may  be  made  up 
as  described  on  page  91.  Gillespie  prefers  the  alcoholic  solution 
in  the  case  of  methyl  red  and  specifies  it  for  soil  work. 

Gillespie  proceeds  as  follows: 

Test  tubes  1.5  cm.  external  diameter  and  15  cm.  long  are  suitable  for 
the  comparator1  and  for  the  strengths  given  for  the  indicator  solutions. 

1  See  page  171. 


124  THE   DETERMINATION    OF   HYDROGEN   IONS 

It  is  advisable  to  select  from  a  stock  of  tubes  a  sufficient  number  of  uni- 
form tubes  by  running  into  each  10  cc.  water  and  retaining  those  which  are 
filled  nearly  to  the  same  height.  A  variation  of  3  to  4  mm.  in  a  height  of 
8  cm.  is  permissible.  Test  tubes  without  flanges  are  preferable.  The 
tubes  may  be  held  together  in  pairs  by  means  of  one  rubber  band  per  pair, 
which  is  wound  about  the  tubes  in  the  form  of  two  figure  8's. 

It  is  convenient  to  use  metal  test  tube  racks,  one  for  each  indicator, 
each  rack  holding  two  rows  of  tubes,  accommodating  one  tube  of  each 
pair  in  front  and  one  in  back.  For  any  desired  indicator  a  set  of  color 
standards  is  prepared  by  placing  from  1  to  9  drops  of  the  indicator  solu- 
tion in  the  9  front  tubes  of  the  pairs  and  from  9  to  1  drops  in  the  back  row 
of  tubes.  A  drop  of  alkali  is  then  added  to  each  of  the  tubes  in  the 
front  row  (2  drops  in  the  case  of  thymol  blue),  sufficient  to  develop  the 
full  alkaline  color  and  a  quantity  of  acid  is  added  to  each  of  the  tubes  in 
the  back  row  to  develop  the  full  acid  color  without  causing  a  secondary 

change  of  color  (see  table  14  for  quantities) The  volume  is  at 

once  made  up  in  all  the  tubes  to  a  constant  height  (within  about  one  drop) 
with  distilled  water,  the  height  corresponding  to  5  cc. 

These  pairs  are  used  in  the  comparator  and  matched  with  the 
tested  solution.  This  tested  solution  is  added  to  ten  drops  of  the 
proper  indicator  until  a  volume  of  5  cc.  is  attained  and  the  tube 
is  then  placed  in  the  comparator  backed  by  a  water  blank. 

Gillespie  describes  the  use  of  the  comparator  (page  171)  and  a 
modification  for  the  accommodation  of  sets  of  three  tubes  used 
when  colored  solutions  have  to  be  compared.  He  also  discusses 
a  number  of  minor  points  and  cautions  against  the  indiscriminate 
comparison  of  measurements  taken  at  different  temperatures. 
For  the  details  the  original  papers  should  be  consulted.  Were  it 
not  that  the  writer  has  seen  evidence  that  the  method  has  been 
applied  with  neglect  of  volume  or  concentration  relations  called 
for  by  the  theory  involved  and  carefully  specified  by  Gillespie, 
it  would  seem  unnecessaiy  to  advise  that  the  principles  be  under- 
stood before  the  method  is  used.  Certain  other  misconceptions 
of  theory  and  practice  found  in  a  treatment  of  the  method  by 
Medalia  (1920)  have  been  corrected  by  Gillespie  (1921). 

A  very  judicious  appraisal  of  the  value  of  the  method  was  given 
by  Gillespie  in  these  words: 

The  method  should  be  of  especial  use  in  orienting  experiments,  or  in 
occasional  experiments  involving  hydrogen  ion  exponent  measurements, 
either  where  it  is  unnecessary  to  push  to  the  highest  degree  of  precision 
obtainable,  or  where  the  investigator  may  be  content  to  carry  out  his 


VI 


BICOLOR   STANDARDS 


125 


measurements  to  his  limit  of  precision  and  to  record  his  results  in  such  a 
form  that  they  may  be  more  closely  interpreted  when  a  more  precise  study 
of  indicators  shall  have  been  completed. 

For  the  elaboration  of  certain  manipulative  details  see  Van 
Alstine  (1920). 

TABLE  15 
Table  for  preparation  of  bicolor  standards  with  0.016  per  cent  brom  cresol 

green,  0.002  N  HCl,  and  0.001  N  NaOH 

Brom  cresol  green.    pK'  =  4.72  at  38°  and  20° 

(After  Hastings,  Sendroy  and  Robson,  1925) 


PH38°  and  20° 

ALKALI  TUBE 

ACID  TUBE 

Dye 

Alkali 

Dye 

Acid 

cc. 

cc. 

cc. 

cc. 

4.00 

0.40 

24.60 

2.10 

22.90 

4.10 

0.49 

24.51 

2.01 

22.99 

4.20 

0.58 

24.42 

1.92 

23.08 

4.30 

0.69 

24.31 

1.81 

23.19 

4.40 

0.81 

24.19 

1.69 

23.31 

4.50 

0.94 

24.06 

1.56 

23.44 

4.60 

1.08 

23.92 

1.42 

23.58 

4.70 

1.23 

23.77 

1.27 

23.73 

4.80 

1.38 

23.62 

1.12 

23.88 

4.90 

1.51 

23.49 

0.99 

24.01 

5.00 

1.64 

23.36 

0.86 

24.14 

5.10 

1.77 

23.23 

0.73 

24.27 

5.20 

1.88 

23.12 

0.62 

24.38 

5.30 

1.98 

23.02 

0.52 

24.48 

5.40 

2.07 

22.93 

0.43 

24.57 

5.50 

2.14 

22.86 

0.36 

24.64 

5.60 

2.21 

22.79 

0.29 

24.71 

5.70 

2.26 

22.74 

0.24 

24.76 

5.80 

2.31 

22.69 

0.19 

24.81 

Hastings,  Sendroy  and  Robson  (1925)  have  systematized  the 
Gillespie  method  as  follows.  The  indicator  solution  specified  in 
each  of  the  following  tables  (15  to  18)  are  added  to  each  tube  from 
a  micro  burette.  Then  either  0.001  N  HCl,  0.01  N  or  0.001  N 
NaOH  solution  is  added  to  bring  the  volume  to  25  cc.  "The 
tubes  are  stoppered  or  sealed  and  kept  in  a  dark  cupboard.  When 
sealed,  the  solutions  are  stable  for  several  months." 


126 


THE    DETERMINATION   OF  HYDROGEN   IONS 


The  stock  indicator  solution  (0.1  per  cent)  are  prepared  by  the 
procedure  noted  on  page  91.    These  are  diluted  as  follows. 


FINAL 
CONCENTRATION 

STOCK  SOLUTION 
DILUTED  TO 
200  CC. 

Phenol  red  

per  cent 

0.0075 

cc. 

15 

Brom  cresol  purple           

0.008 

16 

Chlor  phenol  red 

0  010 

20 

Brom  cresol  green    

0.016 

32 

TABLE  16 

Table  for  preparation  of  bicolor  standards  with  0.01  per  cent  chlor  phenol 

red,  0.001  N  HCl,  and  0.01  N  NaOH 

Chlor  phenol  red.    pK'  =  5.93  at  38°,  and  6.02  at  20° 

(After  Hastings,  Sendroy  and  Robson,  1925) 


pH38o 

ALKALI  TUBE 

ACID  TUBE 

pH20° 

Dye 

Alkali 

Dye 

Acid 

cc. 

cc. 

cc. 

cc. 

5.00 

0.26 

24.74 

2.24 

22.76 

5.09 

5.10 

0.32 

24.68 

2.18 

22.82 

5.19 

5.20 

0.39 

24.61 

2.11 

22.89 

5.29 

5.30 

0.48 

24.52 

2.02 

22.98 

5.39 

5.40 

0.57 

24.43 

1.93 

23.07 

5.49 

5.50 

0.68 

24.32 

1.82 

23.18 

5.59 

5.60 

0.80 

24.20 

1.70 

23.30 

5.69 

5.70 

0.93 

24.07 

1.57 

23.43 

5.79 

5.80 

1.07 

23.93 

1.43 

23.57 

5.89 

5.90 

1.20 

23.80 

1.30 

23.70 

5.99 

6.00 

1.35 

23.65 

1.15 

23.85 

6.09 

6.10 

1.50 

23.50 

1.00 

24.00 

6.19 

6.20 

1.63 

23.37 

0.87 

24.13 

6.29 

6.30 

1.75 

23.25 

0.75 

24.25 

6.39 

USE   OF 


INDICATORS 


If  an  indicator  has  only  one  color,  for  instance  if  it  is  yellow 
in  the  alkaline  form  and  colorless  in  the  acid  form,  it  is  evident 
that  the  method  employed  by  Gillespie  may  be  used  with  the 
elimination  of  one  of  the  sets  of  tubes.  Thus  if  10  cc.  of  a  tested 
solution  containing  1  cc.  of  para  nitrophenol  matches  10  cc.  of 


VI 


BICOLOR   STANDARDS 


127 


an  alkaline  solution  containing  0.2  cc.  of  the  same  solution  of  the 
same  indicator,  it  is  known  that  the  tested  solution  has  induced 
a  20  per  cent  transformation  of  the  indicator.  Then  a  is  0.2. 
If  now  K'a  has  been  determined,  and  if  it  has  been  shown  that 
the  simple  dissociation  formula  holds  for  the  indicator  in  use,  the 
following  equation  may  be  solved  for  pH. 

PH  ==  pK'a  +  log 


1  -a 


TABLE  17 
Table  for  preparation  of  bicolor  standards  with  0.008  per  cent  brom  cresol 

purple,  0.002  N  HCl,  and  0.01  N  NaOH 

Brom  cresol  purple.    pK'  =  6.09  at  38°,  and  6.19  at  20° 

(After  Hastings,  Sendroy  and  Robson,  1925) 


pH38o 

ALKALI  TUBE 

ACID  TUBE 

pH20o 

Dye 

Alkali 

Dye 

Acid 

cc. 

cc. 

cc. 

cc. 

5.60 

0.61 

24.39 

1.89 

23.11 

5.70 

5.70 

0.72 

24.28 

1.78 

23.22 

5.80 

5.80 

0.85 

24.15 

1.65 

23.35 

5.90 

5.90 

0.99 

24.01 

1.51 

23.49 

6.00 

6.00 

1.12 

23.88 

1.38 

23.62 

6.10 

6.10 

1.26 

23.74 

1.24 

23.76 

6.20 

6.20 

1.40 

23.60 

1.10 

23.90 

6.30 

6.30 

1.55 

23.45 

0.95 

24.05 

6.40 

6.40 

1.68 

23.32 

0.82 

24.18 

6.50 

6.50 

'1.80 

23.20 

0.70 

24.30 

6.60 

6.60 

1.91 

23.09 

0.59 

24.41 

6.70 

6.70 

2.01 

22.99 

0.49 

24.51 

6.80 

6.80 

2.09 

22.91 

0.41 

24.59 

6.90 

6.90 

2.16 

22.84 

0.34 

24.66 

7.00 

This  procedure  has  been  developed  by  Michaelis  and  co workers; 
Biochem.  Z.  (1920)  109,  165;  Biochem.  Z.  (1921)  119,  307;  Deut. 
med.  Wochenschr.  (1920)  46, 1238;  47,  465,  673;  Z.  Nahr.  Genussm. 
(1921)  42,  75;  Z.  Immumtatsf.  (1921)  32,  194;  Wochenschrift 
Brau.  (1921)  38,  107. 

The  following  revisions  of  their  tables  are  taken  from  the  1926 
edition  of  Praktikum  der  Physikalischen  Chemie  by  Michaelis. 

In  the  cases  of  phenolphthalein  and  Alizarine  Yellow  GG  the 


128 


THE  DETERMINATION  OF  HYDEOGEN  IONS 


TABLE  18 
Table  for  preparation  of  bicolor  standards  with  0.0075  per  cent  phenol  red, 

0,001  N  HCl,  and  0.01  N  NaOH 

Phenol  red.    pK'  =  7.65  at  38°,  and  7.78  at  20° 

(After  Hastings,  Sendroy  and  Robson,  1925) 


pH38° 

ALKALI  TUBE 

ACID  TUBE 

pH20° 

Dye 

Alkali 

Dye 

Acid 

cc. 

cc. 

cc. 

cc. 

6.70 

0.25 

24.75 

2.25 

22.75 

6.83 

6.80 

0.31 

24.69 

2.19 

22.81 

6.93 

6.90 

0.38 

24.62 

2.12 

22.88 

7.03 

7.00 

0.46 

24.54 

2.04 

22.96 

7.13 

7.10 

0.55 

24.45 

1.95 

23.05 

7.23 

7.20 

0.65 

24.35 

1.85 

23.15 

7.33 

7.30 

0.77 

24.23 

1.73 

23.27 

7.43 

7.40 

0.90 

24.10 

1.60 

23.40 

7.53 

7.50 

1.04 

23.96 

1.46 

23.54 

7.63 

7.60 

1.18 

23.82 

1.32 

23.68 

7.73 

7.70 

1.32 

23.68 

1.18 

23.82 

7.83 

7.80 

.46 

23.54 

1.04 

23.96 

7.93 

7.90 

.60 

23.40 

0.90 

24.10 

8.03 

8.00 

.73 

23.27 

0.77 

24.23 

8.13 

8.10 

.85 

23.15 

0.65 

24.35 

8.23 

8.20 

.95 

23.05 

0.55 

24.45 

8.33 

TABLE  19 

One-color"  indicators 


COMMON  NAME 

CHEMICAL  NAME 

COLOR 

pKAT 

18° 

RANGE 

SOLUTION 

j8-dinitrophenol  

l-oxy-2,  6-dinitroben- 

yellow 

3.69 

2.2-4.0 

0.1    gram    in    300    cc. 

zene 

water 

a-dinitrophenol  

l-oxy-2,  3-di  nitroben- 

yellow 

4.06 

2.8-4.5 

0.1    gram    in    200    cc. 

zene 

water 

y-dinitrophenol  

l-oxy-2,  5-di  nitroben- 

yellow 

5.15 

4.0-  5.5 

0.1    gram    in   200    cc. 

zene 

water 

p-nitrophenol  

l-oxy-4-nitrobenzene 

yellow 

7.18 

5.2-  7.0 

0.1    gram    in    100    cc. 

water 

m-nitrophenol  

l-oxy-3-nitrobenzene 

yellow 

8.33 

6.7-  8.4 

0.3    gram    in    100    cc. 

water 

Phenol  phthalein  .  .  . 

phenol  phthalein 

red 

(9.73) 

8.4-10.5 

0.04  gram  in  30  cc.  al- 

cohol +  70  cc.  water 

Alizarin  yellow  GG 

• 

(salicyl  yellow)  .  .  . 

m-nitrobenzene-azo- 

yellow 

(11.16) 

10.0-12.0 

0.05  gram  in  50  cc.  al- 

salicylic acid 

cohol  +  30  cc.  water 

ONE-COLOR   INDICATORS 


129 


TABLE  20 
pK  values  of  "  one-color"  indicators  at  different  temperatures 


TEMPERATURE 

/3-DINITRO- 
PHENOL 

(1:2:6) 

a-DINITRO- 
PHENOL 

(1:2:4) 

7-DINITRO- 
PHENOL 

(1:2:5) 

P-NITRO- 
PHENOL 

1:4 

m-NITRO- 
PHENOL 

1:3 

0 

3.70 

4.16 

5.24 

7.39 

8.47 

5 

3.76 

4.13 

5.21 

.7.33 

8.43 

10 

3.74 

4.11 

5.18 

7.27 

8.39 

15 

3.71 

4.08 

5.16 

7.22 

8.35 

18 

3.69 

4.06 

5.15 

7.18 

8.33 

20 

3.68 

4.05 

5.14 

7.16 

8.31 

25 

3.65 

4.02 

5.11 

7.10 

8.27 

30 

3.62 

3.99 

5.09 

7.04 

8.22 

35 

3.59 

3.96 

5.07 

6.98 

8.18 

40 

3.56 

3.93 

5.04 

6.93 

8.15 

45 

3.54 

3.91 

5.02 

6.87 

8.11 

50 

3.51 

3.88 

4.99 

6.81 

8.07 

TABLE  21 

Relation  of  apparent  degree  of  color,  a,  to  pH 
Phenolphthalein 


a 

pH 

a 

pH 

a 

pH 

0.01 

8.45 

0.16 

9.10 

0.55 

9.80 

0.014 

8.50 

0.21 

9.20 

0.60 

9.90 

0.030 

8.60 

0.27 

9.30 

0.65 

10.00 

0.047 

8.70 

0.34 

9.40 

0.70 

10.1 

0.069 

8.80 

0.40 

9.50 

0.75 

10.2 

0.090 

8.90 

0.45 

9.60 

0.80 

10.3 

0.120 

9.00 

0.50 

9.70 

TABLE  22 

Relation  of  apparent  degree  of  color,  a,  to  pH 
Alizarin  yellow  GG 


a 

pH 

Of 

pH 

0.13 

10.00 

0.56 

11.20 

0.16 

10.20 

0.66 

11.40 

0.22 

10.40 

0.75 

11.60 

0.29 

10.60 

0.83 

11.80 

0.36 

10.80 

0.88 

12.00 

0.46 

11.00 

130 


THE  DETERMINATION  OF  HYDROGEN  IONS 


color-change  does  not  follow  the  type  a-curve  for  a  univalent 
acid.  Tables  21  and  22  give  the  empirical  values  for  a  for 
use  with  the  ideal  equation. 

Calculations   are   aided  by  the  use  of  a  table  relating  a  to 


log 


Such  a  table,  somewhat  more  elaborate  than  that 


1  -  a 

required  for  this  special  purpose,  will  be  found  on  page  677  of 
the  Appendix. 

TABLE  23 

Composition  of  color  standard 
m-nitrophenol 


Tube  number  

1 

?, 

3 

4 

6 

6 

7 

8 

9 

Cubic  centimeters  of  indicator.  . 
pH.. 

5.2 

8  4 

4.2 

8  ? 

3.0 

8  0 

2.3 

7  8 

1.5 

7  6 

1.0 

7  4 

0.66 
7  ?, 

0.43 
7  0 

0.27 
6  8 

p-nitrophenol 


Tube  number 

10 

11 

1? 

13 

14 

15 

16 

17 

18 

Cubic  centimeters  of  indicator.  . 
pH 

4.05 

7  0 

3.0 

6  8 

2.0 
6  6 

1.4 
6  4 

0.94 

6  ?, 

0.63 
6  0 

0.4 
5  8 

0.25 
5  6 

0.16 
5  4 

2, 5-dinitro phenol  (7  dinitro phenol) 


Tube  number  

19 

?,0 

?,1 

?,2 

23 

24 

25 

26 

Cubic  centimeters  of  indicator  . 

6  6 

5  5 

4  5 

3  4 

?,  4 

1  65 

1   1 

0  74 

pH  . 

5  4 

5  ?, 

5  0 

4  8 

4  6 

4.4 

4.2 

4.0 

2, 4-dinitro  phenol  (a  dinitro  phenol) 


Tube  number 

27 
6.7 
4.4 

28 
5.7 
4.2 

29 
4.6 
4.0 

30 
3.4 

3.8 

31 

2.5 
3.6 

32 
1.74 
3.4 

33 

1.20 
3.2 

34 

0.78 
3.0 

35 

0.51 

2.8 

Cubic  centimeters  of  indicator.  . 
pH 

With  these  data  we  are  now  prepared  to  measure  pH  values 
without  the  use  of  standard  buffer  solutions. 

Test  tubes  must  be  of  equal  bore.  A  measured  amount  of  the 
solution  to  be  tested  (e.g.  10  cc.)  is  mixed  with  the  proper  indicator 
in  such  amount  that  a  rather  weak  color  is  developed.  To  a 
second  test  tube  containing  9  cc.  0.1  M  Na2C03  (for  nitro phenols 
only)  there  is  added  such  a  volume  of  the  indicator  solution  that 
the  color  developed  approximately  matches  that  of  the  first  tube. 
The  volume  of  the  second  tube  is  now  made  up  to  the  volume  of 
the  first.  If  the  two  tubes  do  not  match  in  color,  another  trial 


VI 


MICHAELIS'   METHOD  131 


is  made  with  more  or  less  indicator  until  a  color  match  is  obtained. 
The  amount  of  fully  transformed  indicator  in  the  second  tube  then 
corresponds  to  that  amount  of  indicator  in  the  first  tube  which 
has  been  transformed  to  the  colored  tautomer.  Let  us  assume 
that  1.0  cc.  was  added  to  the  tested  solution  and  that  a  color  match 
occurs  when  0.1  cc.  of  the  same  indicator  solution  was  placed  in 
the  second  alkaline  tube  and  made  up  to  the  volume  of  the  first. 
Then  the  percentage  color  transformation  induced  by  the  tested 
solution  was  10. 

Hence  a  =  0.1  and  log  —2—  =  -  0.95. 
1  —  a 

If  the  indicator  used  was  p-nitrophenol  and  the  temperature 
was  20°C.  pH  =  7.16  -  0.95  =  6.21  (6.2). 

For  routine  work  in  the  range  pH  2.8  to  8.4  Michaelis  (1921) 
recommends  the  following  system.  See  table  23. 

To  uniform  test  tubes  are  added  seriatim  the  volumes  of 
indicator  solution  given  in  table  23,  the  indicator  solution 
being  prepared  by  diluting  the  stock  solutions  (page  128)  ten 
times  with  0.1  M  Na^COs  solution.  Each  tube  is  now  filled  to 
a  7  cc.  mark  with  the  soda  solution.  (In  the  original  paper 
Michaelis  and  Gyemant  describe  dilutions  with  N/100  NaOH 
solution.) 

The  test  tubes  are  sealed  and  when  not  in  use  are  protected 
from  the  light. 

To  test  a  solution  for  its  pH  value,  6  cc.  are  taken  and  1  cc. 
indicator  solution  added.  The  solution  is  then  compared  with 
the  standards  in  a  comparator,  see  page  171,  figure  29. 

Empirically,  Michaelis  finds  that  if  there  be  placed  over  the 
comparator  holes  a  ground  glass  and  a  glass  of  cobalt  blue,  the 
color  quality  of  two  tubes  will  be  very  different  when  there  is  no 
match.  This  increases  the  differentiating  ability  of  the  eye  and 
makes  the  use  of  the  nitrophenols  with  colored  solutions,  such  as 
urine,  much  more  satisfactory.  The  glass  of  cobalt  blue  should 
be  selected  by  trial  for  a  satisfactory  density. 

For  finding  the  pH  values  of  waters  Michaelis  (1921)  operates 
as  follows : 

A  stock  solution  containing  0.3  gram  pure  m-nitrophenol  in 
300  cc.  distilled  water  is  diluted  before  use  by  adding  to  1  cc. 
of  the  stock  9  cc.  distilled  water.  There  are  used  flat  bottom 


132  THE   DETERMINATION   OF  HYDROGEN   IONS 

tubes  of  about  25  cm.  height  and  14  mm.  internal  diameter 
having  such  uniformity  that  40  cc.  of  water  will  stand  at  a  height 
of  between  22  and  23  cm.  To  six  such  tubes  are  added  seriatim 
0.25;  0.29;  0.33;  0.38;  0.45  and  0.50  cc.  of  the  diluted  m-nitro- 
phenol  solution.  To  each  tube  are  added  40  cc.  of  an  approxi- 
mately N/50  NaOH  solution  freshly  prepared  by  dilution  of  an 
approximately  normal  solution.  These  are  the  standards. 

To  test  a  water,  40  cc.  are  added  to  a  tube  of  correct  dimensions 
and  to  this  is  added  sufficient  indicator  to  develop  a  color  within 
the  range  of  the  standards,  preferably  near  the  brighter  of  the 
standards.  Comparison  is  now  made  as  in  Nesslerization,  after 
having  waited  two  minutes  for  completion  of  the  mixing. 

TABLE  24 
Effect  of  salt  on  pK  of  m-nitrophenol 


MOLECULAR  SALT  CONTENT 

log^I 

0-0.01 

8.33 

0.05 

8.28 

0.10 

8.23 

0.15 

8.22 

0.20 

8.18 

0.3-0.6 

8.17 

to  1.0 

8.15 

The  amount  of  indicator  in  the  alkaline,  matching  standard 
corresponds  to  the  amount  transformed  to  the  colored  form  by 
the  tested  solution.  Therefore,fthe  cubic  centimeters  of  indica- 
tor in  the  standard  divided  by  the  cubic  centimeters  in  the  tested 
solution  is  a,  the  degree  of  color  transformation,  or  when  multi- 
plied by  100,  the  percentage  color  transformation. 

Michaelis  and  his  co-workers  have  tabulated  corrections  for 
temperature  and  for  salt  concentrations.  The  operator  should 
determine  for  himself  not  only  the  order  of  accuracy  required  in 
his  problem  but  his  own  ability  to  make  readings  with  that  pre- 
cision which  will  make  corrections  significant.  He  may  then 
refer  to  the  original  papers  for  tables  giving  corrections  for  salt 
effects  and  for  temperature.  The  order  of  magnitude  of  these 
corrections  may  be  seen  in  tables  20  and  24. 

For  ^m-nitrophenol  Michaelis  and  Kriiger  give  the  values  of 


VI  MICHAELIS'   METHOD  133 

log  —  at  17°C.  in  solutions  of  the  indicated  salt  concentrations 

shown  in  table  24. 

In  spite  of  the  fact  that  the  nitro-compounds  used  by  Michaelis 
and  Gyemant  are  of  wan  color  and  those  tried  in  the  survey  made 
by  Clark  and  Lubs  were  neglected  for  this  reason,  Michaelis  and 
Gyemant  describe  the  application  of  their  method  to  colored 
solutions.  In  this  use  the  colored  glass  is  essential. 

Advantage  is  taken  of  the  fact  that  many  solutions  are  inappre- 
ciably altered  in  pH  by  diluting  five  or  even  ten  times  (see  page 
40).  For  dilution,  Michaelis  and  Gyemant  use  freshly  boiled 
NaCl  solution  of  a  concentration  approximately  that  of  the  test 
solution.  If  on  dilution  the  natural  color  still  interferes  with 
the  use  of  an  indicator,  the  natural  color  may  be  duplicated  in 
the  standard  by  the  use  of  supplementary  dyes  such  as  S0rensen 
uses.  Or,  if  addition  of  alkali  does  not  alter  the  natural  color  of 
the  solution  under  test,  the  standard  may  be  made  up  with  an 
alkaline  solution  of  the  tested  solution  itself.  In  this  case  it  is 
necessary  to  be  on  guard  against  the  buffer  action  and  to  add 
alkali  until  no  increase  in  the  color  of  the  indicator  is  observed. 

Without  doubt  the  preferable  procedure  to  follow  when  apply- 
ing the  Michaelis  and  Gyemant  method  or  any  other  method  to 
colored  solutions  is  to  use  the  "comparator"  described  on  page 
172  and  illustrated  in  figure  29,  page  171.  The  blue  glass  (see 
page  131)  is  held  before  the  holes  by  a  pair  of  clips. 

The  method  of  Michaelis  and  Gyemant  is  fundamentally  the 
same  as  that  of  Gillespie  and  should,  therefore,  be  used  with  the 
qualifications  which  Gillespie  has  stated.  There  is  a  distinct 
advantage  in  the  use  of  the  nitrophenols  for  they  have  been  found 
to  have  relatively  small  "protein"  and  salt  effects,  and  do  not 
show  the  errors  with  alkaloids  that  appear  with  the  use  of  sulfon- 
phthaleins.  It  is  sometimes  necessary  to  use  very  high  con- 
centrations of  the  indicator,  and  in  such  circumstances  one  must 
be  on  guard  against  the  effect  of  the  indicator  itself  or  of  im- 
purities. Only  the  purest  grades  of  nitrophenols  should  be 
used.  Impure  samples  are  almost  useless. 

Inasmuch  as  the  method  inherently  is  capable  of  high  accuracy 
it  may  be  asked  why  its  description  is  relegated  to  a  chapter 
entitled  "approximate  determinations."  If  the  reader  will  reflect 


134  THE   DETERMINATION   OF   HYDROGEN   IONS 

he  will  remember  that  any  numerical  value  reached  by  the  ap- 
plication of  this  method  depends  upon  the  value  of  the  disso- 
ciation constant.  There  remain  larger  discrepancies  in  the  values 
for  some  of  the  indicators  than  are  warranted  by  the  accuracy  of 
available  methods  if  applied  to  the  same  solutions.  But,  as  we 
shall  see,  a  dissociation  constant  formulated  by  the  classical 
methods,  is  subject  to  some  change  in  value  as  the  nature  of  the 
solution  (e.g.,  salt  content)  changes.  It  is  therefore  preferable 
to  recast  the  equations  into  terms  of  activities  (see  Chapter  XI) 
and  when  this  is  done  the  true  dissociation  constant  may  have  a 
very  different  numerical  value  than  has  the  apparent  constant 
at  a  given  salt  content  of  the  solution.  As  this  edition  goes  to 
press  the  period  is  just  beginning  when  the  characteristic  con- 
stants of  indicators  are  being  redetermined  both  with  the  aid  of 
spectrophotometric  accuracy  and  with  the  aid  of  modern  re- 
formulation. Pending  the  outcome  we  must  regard  the  applica- 
tion of  the  method  in  question,  when  performed  with  the  data 
available,  as  having  been  standardized  by  reference  to  the  standard 
buffer  method  and  with  all  the  systematic  errors  attendant  upon 
a  secondary  standardization. 

Indicator  papers.  Although  a  favorite  form  of  indicator  is  the 
deposit  on  a  strip  of  paper  (for  example  the  familiar  litmus  paper) 
it  is  to  be  avoided  unless  the  use  of  an  indicator  solution  is  pre- 
cluded. It  is  to  be  avoided  because  the  factors  involved  in  the 
reaction  between  solutions  and  indicator  are  made  complex  by 
the  capillary  action  of  the  paper  or  the  material  entrained  in 
these  capillaries.  On  the  other  hand  there  are  occasions  when 
an  approximate  measure  of  pH  is  sufficient  and  when  an  indicator- 
paper  is  to  be  preferred.  On  such  occasions  it  is  desirable  to 
know  the  difficulties  to  be  encountered. 

We  are  indebted  to  Walpole  (1913)  and  others  and  particularly 
to  Kolthoff  (1919,  1921)  for  investigations  on  this  subject.  Kolt- 
hoff  has  given  particular  attention  to  the  sensitivity  of  indicator 
papers  when  used  in  titrations,  a  situation  where  there  is  generally 
but  little  buffer  action  near  the  end-point.  Under  such  circum- 
stances there  are  to  be  regarded  a  number  of  details  which  are 
described  at  length  in  Kolthoff's  papers.  Several  of  these  details 
will  be  perceived  if  we  describe  some  of  the  more  important  aspects 
of  the  indicator-paper  method  of  determining  pH. 


VI  INDICATOR   PAPER  135 

In  general  one  must  ride  either  horn  of  the  following  dilemma. 
The  paper  is  sized,  in  which  case  the  buffer  action  of  the  tested 
solution  must  be  strong  enough  and  allowed  time  enough  to  over- 
come the  buffer  action  of  the  sizing.  Or  the  paper  has  the  quali- 
ties of  filter  paper,  in  which  case  the  solution  tested  will  spread 
and  leave  rings  of  different  composition  formed  by  the  adsorp- 
tive  power  of  the  capillaries. 

Kolthoff  found  that  various  treatments  and  selections  of  filter 
paper  are  of  secondary  importance,  so  the  choice  lies  between 
sized  and  unsized  paper.  Certain  coloring  matters  are  adsorbed 
by  filter  paper  so  that  a  separation  is  possible  and  the  clear  solu- 
tion can  be  found  in  a  ring  about  the  point  of  contact  between  a 
tested  colored  solution  and  the  indicator  paper.  But  beyond  this 
ring  is  a  much  more  dilute  one  and  unless  one  knows  the  properties 
of  the  system  under  examination  it  is  not  easy  to  estimate  cor- 
rectly the  pH  of  the  solution  from  the  appearance  of  the  paper. 

In  any  case  the  paper  should  be  left  in  contact  with  the  tested 
solution  a  generous  length  of  time,  for  the  establishment  of 
equilibrium  may  be  very  slow  (Walpole),  and  there  must  be  in- 
stinctively exercised  a  mental  plotting  of  the  time  curve. 

If,  after  having  exhausted  all  other  methods,  it  is  found  that 
the  indicator-paper  method  is  the  better  adapted  to  a  particular 
set  of  circumstances,  the  procedure  should  be  calibrated  to  the 
purpose  at  hand  rather  than  forcec}  to  render  accurate  pH  values. 

Rebello  (1922)  replaces  paper  by  cotton  thread  which  he  draws 
through  the  tissue  he  examines.  Wulff  (1926)  uses  transparent 
membranes  of  cellulose  derivatives. 

See  Kolthoff  and  Furman's  book  Indicators  for  further  discus- 
sion of  indicator  papers. 

Dilution.  As  indicated  in  Chapter  II  a  well  buffered  solution 
may  often  be  moderately  diluted  without  seriously  altering  the  pH. 

When  dealing  with  complex  solutions  which  are  mixtures  of 
very  weakly  dissociated  acids  and  bases  in  the  presence  of  the 
salts,  and  especially  when  the  solution  is  already  near  neutrality, 
dilution  has  a  very  small  effect  on  pH,  so  that  if  we  are  using  the 
crude  colorimetric  method  of  determining  pH,  a  five-fold  dilution 
of  the  solution  to  be  tested  will  not  affect  the  result  through  the 
small  change  in  the  actual  hydrogen  ion  concentration.  Differ- 
ences which  may  be  observed  are  quite  likely  to  be  due  to  change 
in  the  protein  or  salt  content. 


136         THE  DETERMINATION  OF  HYDROGEN  IONS 

For  accurate  work  with  dilutions  there  should  be  involved  the 
principles  discussed  in  Chapter  XXV. 

The  salt  content  of  the  standards  undoubtedly  influences  the  indi- 
cators and  should  be  made  as  comparable  as  is  convenient  with 
the  salt  content  of  the  solutions  tested  when  these  are  diluted  to 
obtain  a  better  view  of  the  indicator  color. 

In  the  examination  of  soil  extracts  colorimetrically  little  could 
be  done  were  the  "soil-solution"  not  diluted.  Whatever  may  be 
the  effect  it  is  certain  that  the  correlations  between  the  pH  values 
of  such  extracts  and  soil  conditions  is  proving  of  great  value  (see 
Chapter  XXX).  Wherry  has  developed  a  field  kit  of  the  sulfon- 
phthalein  indicators  with  which  he  has  found  some  remarkable 
correlations  between  plant  distribution  and  the  pH  of  the  native 
soils.  This  field  kit  is  now  on  the  market. 

A  good  example  of  the  application  of  the  dilution  method  is 
given  in  a  paper  by  Sharp  and  Mclnerney  (1926).  They  dilute 
milk,  whey  and  cream  with  as  much  as  nineteen  volumes  of  water 
in  order  to  lower  the  turbidity  adequately.  They  then  apply 
their  statistical  study  of  corrections  to  be  made  to  bring  the 
colorimetric  readings  into  conformity  with  the  hydrogen  electrode 
measurements  of  the  undiluted  solution.  They  tabulate  these 
corrections  for  convenience  in  routine  examinations. 

The  use  of  indicators  in  bacteriology.  Perhaps  no  other  science 
requires  such  continuous  routine  use  of  indicators  as  does  bac- 
teriology. This  use  is  chiefly  in  the  adjustment  of  the  reaction 
of  culture  media  and  in  the  testing  of  the  direction  and  limits  of 
fermentation.  While  these  are  but  examples,  the  frequency  with 
which  they  become  matters  of  routine  warrants  a  brief  outline  of 
special  procedures. 

If  experience  has  shown  that  the  pH  of  the  medium  may  lie 
within  a  zone  about  0.5  unit  of  pH  wide,  it  is  sufficient  to  add  un- 
standardized  acid  or  alkali,  as  the  case  may  be,  until  a  portion 
of  the  medium  tested  with  the  proper  indicator  in  proper  concen- 
tration approximately  matches  that  color  standard  shown  in  the 
color  chart  of  page  65  corresponding  to  the  pH  value  to  be  ap- 
proximated. This  requires  experience  in  overcoming  the  con- 
fusing effect  of  the  natural  color  of  the  medium  and  also  a  well 
established  sense  of  color  memory.  The  beginner  should  proceed 
in  some  such  way  as  the  following. 


VI  SPECIAL  USES   OF  INDICATORS  137 

It  is  desired,  for  instance,  to  adjust  a  colorless  medium  to  pH 
7.5.  The  medium  as  prepared  is  somewhat  below  the  final  vol- 
ume. A  quick,  rough  test  at  room  temperature  shows  that  the 
pH  value  lies  between  6.0  and  6.5.  Therefore,  alkali  must  be 
added.  The  alkali  solution  to  be  used  need  not  be  standardized 
but  may  be  about  1  normal.  An  exact  one-in-ten  dilution  of  this 
is  run  into  5  cc.  of  the  medium  to  which  have  been  added  5  drops 
of  phenol  red  solution.  Titration  is  continued  until  the  color 
nearly  matches  10  cc.  of  standard  buffer  "7.5."  The  tube  of 
medium  is  now  diluted  to  10  cc.  so  that  a  color  comparison  may  be 
made  between  test  solution  and  standard,  each  containing  the 
same  concentration  of  indicator.  The  tubes  are  viewed  through 
equal  depths  of  solution.  If  the  desired  point,  7.5,  has  been 
overstepped,  another  trial  is  made.  If  7.5  is  not  reached  a 
moderate  addition  of  alkali  may  be  made  without  serious  viola- 
tion of  volume  requirements,  and  a  second  reading  is  taken. 

After  making  estimates  of  the  pH  values  in  the  two  readings 
an  interpolation  is  made  of  the  amount  of  dilute  alkali  required 
to  bring  the  medium  to  exactly  pH  7.5.  From  this  is  calculated 
the  amount  of  the  stronger  alkali  required  for  the  main  portion. 
After  adding  this,  a  check  determination  is  made.  When 
finally  adjusted  the  medium  is  diluted  to  its  final  volume  Most 
culture  media  suffer  alterations  of  their  pH  values  during  sterili- 
zation and  consequently  allowance  for  this  must  be  made  if  the 
final  pH  value  is  to  be  exact.  This  allowance  will  vary  with  the 
medium  but  can  easily  be  determined  for  a  standard  medium 
prepared  under  uniform  conditions. 

When  the  color  or  turbidity  of  a  tested  solution  interferes  with 
direct  color  comparisons  proceed  as  above  but  make  comparisons 
by  means  of  the  Walpole  compensation  method  described  on 
page  171. 

It  need  hardly  be  said  that  if  the  requirements  of  an  organism 
are  such  that  the  desired  pH  value  cannot  be  obtained  with  phenol 
red  a  more  suitable  indicator  is  selected  from  table  11  and  if  the 
medium  requires  the  addition  of  acid  an  unstandardized  acid 
solution  approximately  normal  (or  stronger)  and  an  exact  1:10 
dilution  of  this  are  substituted  for  the  alkali  solutions  mentioned 
above. 

In  testing  fermentations  it  often  happens  that  the  final  hydro- 


138  THE    DETERMINATION    OF   HYDROGEN   IONS 

gen  ion  concentration  is  of  more  significance  than  the  amount  of 
acid  or  alkali  formed;  but  the  two  distinct  types  of  data  are  not 
to  be  confused  to  the  complete  displacement  of  either. 

It  is  sometimes  convenient  to  incorporate  the  indicator  with  the 
medium,  provided  the  indicator  is  not  reduced  or  destroyed  by 
the  bacterial  action.  The  sulfonphthaleins  are  particularly  use- 
ful for  they  are  not  reduced  except  by  the  more  active  anaerobes. 
Brom  cresol  purple  replaces  litmus  in  the  common  milk-fermenta- 
tion tests  without  introducing  that  confusion  which  the  reduction 
of  litmus  causes.  It  reveals  differences  in  pH  even  beyond  the 
range  of  its  usefulness  for  ordinary  measurements,  passing  from  a 
greyish  blue  in  normal  milk  to  more  and  more  brilliant  yellows 
with  the  development  of  acidity,  and  to  a  deep  blue  with  the 
development  of  alkalinity.  For  further  details  see  Clark  and 
Lubs  (1917). 

In  the  method  of  Clark  and  Lubs  (1915,  1916)  for  the  differenti- 
ation of  the  two  main  groups  of  the  coli-aerogenes  bacteria,  as 
well  as  in  the  similar  method  of  Avery  and  Cullen  (1919)  for 
separating  streptococci,  the  composition  of  the  medium  is  so 
adjusted  to  the  metabolic  powers  of  the  organisms,  that  the 
reaction  is  left  acid  to  methyl  red  in  one  case,  and  alkaline  in  the 
other.  No  exact  pH  measurements  are  necessary.  In  cases 
where  large  numbers  of  cultures  falling  within  the  range  of  one 
indicator  are  to  be  tested,  the  cultures  may  be  treated  with  the 
indicator  and  compared  by  grouping.  A  careful  determination 
made  upon  one  member  of  a  homogeneous  group  will  serve  for  all. 
In  this  way  large  numbers  of  cultures  may  be  tested  in  a  day. 

Special  uses.  While  on  the  subject  of  approximate  determina- 
tions with  indicators  a  word  may  be  said  about  the  usefulness  of 
the  quick,  rough  test. 

Almost  every  investigator  has  come  to  realize  that  among  the 
mistakes  in  labeling  chemicals  the  more  frequent  are  cases  in 
which  a  basic  salt  is  labeled  as  an  acid  salt  and  vice  versa.  A 
solution  of  NaaHPO4,  for  example,  has  a  pH  value,  which,  while 
easily  displaced  (see  fig.  4),  distinguishes  it  definitely  from  a  solu- 
tion of  NaH2P04  or  Na3P04.  Indeed  some  idea  may  be  obtained 
of  the  degree  of  impurity  if  the  pH  value  of  a  dilute  solution  is 
displaced  definitely  from  about  pH  8.5.  Some  serious  accidents 
have  occurred  in  medical  practice  by  the  use  of  solutions  purported 


VI  MICRO   METHODS  139 

to  be  neutral  and  too  late  found  to  be  acidic.  One  short,  swift 
test  with  an  indicator  could  have  revealed  the  situation,  and 
averted  the  accident. 

Indeed  there  are  a  great  many  substances  solutions  of  which 
have  either  a  buffered  and  definite  pH  value,  as  in  the  case  of 
acid  potassium  phthalate,  or  else  a  pH  value  easily  displaced  by 
impurities  from  that  of  the  absolutely  pure  substance  but  still 
falling  within  limits,  as  in  the  case  of  the  primary  and  secondary 
phosphates.  When  properly  defined,  such  values  can  be  made 
part  of  the  specifications  for  purity.  Especially  in  the  case  of 
drugs  which  are  often  used  beyond  the  reach  of  the  assay  labora- 
tory a  simple  indicator  test  should  prove  helpful  as  suggested  by 
Evers  (1921)  and  especially  emphasized  by  Kolthoff  (1921). 

MICRO   COLORIMETRIC   METHODS 

The  majority  of  micro-methods2  follow  the  main  principles 
hitherto  described  but  with  greater  or  lesser  reduction  in  the 
dimensions  of  the  vessels.  Such  are  the  capillary  tubes  employed 
by  Walther  and  Ulrich  (1926),  Needham  and  Rapkine.  Rap- 
kine's  capillary  tubes,  used  for  comparison  with  a  single  cell 
which  has  been  injected  with  an  indicator,  are  made  of  varying 
diameter  in  order  that  there  may  be  selected  a  portion  of  the 
capillary  of  the  same  diameter  as  the  cell.3  Vies  (1926)  describes 
a  micro  colorimeter  for  use  on  the  microscope  stage. 

Spotting.  When  only  small  quantities  of  solution  are  available 
or  when  highly  colored  solutions  are  to  be  roughly  measured,  their 
examination  in  drops  against  a  brilliant  white  background  of 
"opal"  glass  is  often  helpful.  In  the  examination  of  colorless 
solutions  comparisons  with  standards  may  be  made  as  follows. 
A  drop  of  the  solution  under  examination  is  mixed  with  a  drop 
of  the  proper  indicator  solution  upon  a  piece  of  opal  glass.  About 
this  are  placed  drops  of  standard  solutions  and  with  each  is  mixed 
a  drop  of  the  indicator  solution  used  with  the  solution  under 
examination.  Direct  comparison  is  then  made.  Felton,  who 
developed  details  in  this  method  for  the  examination  of  small 
quantities  of  solutions  used  in  tissue-culture  investigations,  found 

2  See  also  Pfeiffer  (1927),  Vies  (1926)  and  Lindhard  (1921)  on  micro- 
colorimetric  methods.     Cf.  Ellis  (1925). 

3  Personal  communication. 


140         THE  DETERMINATION  OF  HYDROGEN  IONS 

mixtures  of  indicators  of  particular  value  for  orientation.  (See 
page  96.)  Mixtures  are  used  only  as  "feelers."  The  opal  glass 
or  porcelain  upon  which  the  tests  are  to  be  made  should  be  care- 
fully tested  for  the  absence  of  material  seriously  affecting  the 
acid-base  equilibria  of  the  material  under  examination.  Errors 
due  to  unequal  drops,  evaporation  and  impurity  of  indicator  are 
to  be  watched  for.  For  further  details  see  Felton  (1921). 

To  what  extent  the  mixture  of  as  much  as  50  per  cent  by  volume 
of  indicator  solution  and  tested  solution  causes  an  error  can  only 
be  judged  in  the  specific  case. 

From  the  spot-plate  with  flat  surface  and  drops  of  any  size 
that  can  be  made,  we  come  to  the  spot-plate  with  depressions  to 
hold  larger  quantities;  and  then  to  small  glass  cells  such  as  Brown 
(1923)  employs  and  such  as  the  LaMotte  Co.  uses  in  one  of  their 
commercial  sets. 

PRECIPITATING  INDICATORS 

Naegeli  (1926)  employs  the  principle,  briefly  noted  on  page 
583,  that  precipitations  may  occur  within  narrow  ranges  of  pH. 
He  therefore  selects  organic  acids  the  undissociated  forms  of 
which  are  very  little  soluble. 

The  variation  of  the  precipitation  point  with  the  buffer  suggests 
a  restudy  in  terms  of  activities.  See  page  583. 


CHAPTER  VII 

THE  APPLICATION  OF  SPECTROPHOTOMETRY,  COLORIMETRY,  ETC. 

How  that  element  washes  the  universe  with  its  enchanting  waves! 
....  'Tis  the  last  stroke  of  Nature;  beyond  color  she  cannot  go. 

— EMERSON. 

INTRODUCTION 

The  marvelous  color-change  of  an  indicator  invites  scrutiny  of 
the  internal  structure.  Why  should  the  mere  act  of  ionization 
initiate  a  radical  change  in  the  response  to  radiation?  Theory 
relating  structure  to  absorption  of  radiant  energy  has  not  yet 
attained  the  certitude  that  will  doubtless  arrive  in  time.  There- 
fore, we  had  best  resist  the  temptation  to  look  into  this  tantalizing 
subject  lest  our  attention  be  diverted  from  the  present  task, 
which  is  to  formulate  the  fact  of  absorption  of  radiant  energy  in 
a  manner  which  will  contribute  to  exactitude  in  measurement  of 
pH-values. 

ABSORPTION 

As  radiant  energy  of  any  wave-length  advances  through  a 
material  medium  it  suffers  some  absorption.  Visible  radiant 
energy  is  absorbed  but  little  by  water  and  by  optical  grades  of 
glass;  but  in  refined  measurements  absorption  by  these  relatively 
"transparent"  materials  must  be  taken  into  account.  Usually 
absorption  by  solutions  is  somewhat  selective.  Absorption  is 
both  selective  and  effective  in  solution  of  those  "dyes"  which  are 
used  as  indicators.  Thus,  if  an  alkaline  solution  of  cresol  red  is 
viewed  through  a  spectroscope,  there  appears  in  the  spectrum  a 
dark  band,  the  position  of  which  indicates  that  the  stimuli  of  the 
colors  yellow  and  green  have  been  very  effectively  obstructed. 
So  far  as  relative  absorption  of  the  radiant  energy  is  concerned, 
this  is  shown  quantitatively  by  the  curves  of  figure  20  where  the 
ordinate  is  a  measure  of  relative  absorption  and  the  abscissa 
is  divided  in  such  a  way  as  to  show  approximately  the  relative 
positions  of  lines  of  various  wave-length  as  distributed  in  the 

141 


142 


THE    DETERMINATION    OF   HYDROGEN    IONS 


spectrum  of  a  prism  instrument.  From  this  curve  it  is  evident 
that,  in  addition  !to  Relatively  great  absorption  centered  at  the 
wave-length  (X)1  of  mju  =  572,  there  is  appreciable  absorption  by 


...     650  700 
Violet  Blue  Green  Yellow  01-41136  Red 

FIG.  20.  ABSORPTION  CURVES  OF  INDICATORS 

cresol  red  within  the  range  m/*  450  to  m^  610.     Quantitative 
measurement  of  absorption  and  the  charting  of  the  absorption 


1  X  =  general  symbol  for  wave-length,    m/x 
X  10~9.    One  m/i  =  10  Angstrom  units. 


milli  micron  =  meters 


VII  ABSORPTION  143 

band  provides  data  for  identification  of  an  indicator  and  for  tests 
of  purity.  A  special  application  of  the  data  to  the  determination 
of  pH  values  will  presently  be  outlined. 

Neglect  for  the  moment  absorption  by  the  solvent  and  by  the 
glass  walls  of  the  container.  Consider  the  absorption  which  occurs 
when  radiant  energy  of  one  definite  wave-length,  X,  passes  through 
a  homogeneous  solution  of  some  absorbing  substance  contained 
in  a  cell  the  end-plates  of  which  are  plane-parallel,  the  propagation 
through  the  cell  and  solution  being  rectilinear. 

In  advancing  through  an  infinitesimal  length,  dl,  of  the  solu- 
tion, the  radiant  energy  of  the  given  wave-length  suffers  the  loss 
of  some  certain  fraction  of  its  power,2  P.  Within  the  next  in- 
finitesimal length  the  remaining  power  is  reduced  by  the  same 
fraction.  Accordingly,  the  decrease  of  power  per  element  of 
length  is  proportional  to  the  power  of  the  radiant  energy  in  this 
length. 


Now  let  the  power  incident  at  the  first  surface  of  the  solution  be 
PI  and  that  emergent  at  the  second  surface  be  P2.  When  these 
limits  are  used  in  the  integration  of  equation  (1)  there  is  obtained 
equation  (2) 

-Zn|2  =  k'l  (2) 

-tl 

In  this  equation  In  (logarithmus  naturalis)  symbolizes  (natural) 
logarithms  to  the  base  e. 

The  decline  of  radiant  power  within  any  infinitesimal  length 
of  the  solution  should  be  proportional  to  the  number  of  absorbing 
molecules  encountered.  This  number  may  be  considered  propor- 
tional to  the  concentration,  c,  of  the  dye  under  a  given  set  of  con- 
ditions. Therefore,  (1)  becomes  (3).  Integration  of  (3)  between 
the  limits  PI  and  P2  yields  (4) 

'T> 

=  kcP  (3) 


2  Since  ratios  of  powers  are  to  be  used,  intensity  might  be  substituted 
here  for  power. 


144         THE  DETERMINATION  OF  HYDROGEN  IONS 

-  ln  |»  =  kcl  (4) 

The  ratio  ^  is  that  fraction  of  the  power  of  the  incident  radiant 

energy  which  emerges.  This  ratio  is  called  the  transmittance  and 
is  symbolized  by  T.  Introducing  T  and  changing  the  constants 
of  (2)  and  (4)  to  correspond  with  the  conversion  of  natural 
logarithms  to  common  logarithms  we  have  from  (2)  and  from 
(4)  equations  (5)  and  (6)  respectively. 

-logTx=lK'x      (Lambert's  Law)  (5) 

-logTx  =  IcKx     (Beer's  Law)  (6) 

The  subscript  X  is  used  to  emphasize  the  fact  that  specific  values 
for  the  indicated  terms  depend  upon  the  wave-length  (X)  of  the 
radiant  energy. 

Here  it  may  be  noted  that  any  relation  between  the  transmit- 
tance at  a  given  wave-length  and  the  wave-length  is  determined 
by  the  specific  properties  of  the  absorbing  system.  In  other 
words  the  position  and  shape  of  the  absorption  curve  is  charac- 
teristic of  a  given  system.  With  the  cause  of  this,  or  with  the 
empirical  formulation  of  a  relation  between  TX  and  X  as  X  varies,  we 
are  not  now  concerned.  We  are  concerned  only  with  the  accept- 
ance of  the  fact  as  a  specificity  to  put  to  our  present  uses.  For  a 
brief  discussion  of  variation  of  TX  with  variation  of  X  see  Thiel 
and  Diehl  (1927)  page  517  ff.  but  especially  the  Report  of  the 
Committee  on  Spectra  and  Constitution,  1926,  British  Asso- 
ciation. 

Equation  (5)  is  an  expression  of  Lambert's  law  of  absorption  and  is  be- 
lieved to  be  universally  applicable.  Equation  (6),  which  involves  concen- 
tration of  the  absorbing  species,  must  be  used  with  caution;  for,  although 
there  will  presently  be  noted  cases  in  which  apparent  deviation  from  this 
so-called  Beer's  law  is  readily  explained  and  indeed  put  to  use,  there  are 
cases  in  which  observed  deviations  have  not  been  explained. 

When  the  length,  1,  and  the  concentration,  c,  are  each  unity 

-  log  T  =  K 

K  is  called  the  specific  transmissive  index.  Its  value  as  determined  by  a 
measurement  of  T  at  a,  given  wave-length  will  of  course  depend  upon  the  unit 
adopted  for  1  and  c.  The  unit  of  length  is  usually  the  centimeter;  but  the 


VII  EXTINCTION   COEFFICIENT  145 

unit  of  concentration  is  frequently  changed  to  the  convenience  of  special 
problems.  Were  c  the  concentration  of  total  dye,  as  it  is  in  the  usual  state- 
ment of  Beer's  law,  and  were  one  mole  per  liter  the  unit  of  concentration,  K 
would  be  the  molar  transmissive  index.  The  term  absorption  index  arises 
from  the  fact  that  the  magnitude  of  K  is  a  measure  of  the  extent  of  the 

r>  ~p 

relative  absorption.     If  — -  is  T,  the  transmittance,  1  —  — ^  may  be  called 

r\  .       *  i 

the  absorptance  A,  a  term  little  used. 

The  term  "extinction  coefficient"  arises  in  the  following  way.  Were  all 
the  radiant  power  incident  at  the  first  surface  to  be  absorbed  (extinguished) 

r> 

when  the  radiation  reached  the  second  surface,  —  would  be  zero  and  then, 

Pi 

by  equation  (5),  K'  or  1  would  have  to  be  infinity.  Since  K'  has  a  finite 
value,  the  length  would  have  to  be  infinity.  To  avoid  this  difficulty 

imagine  the  value  of  1  to  baadjustedso  that  K'  equals  unity.     Then  —log 
•p         I 

T  =  1  or  T  =  —  =  — .     Under  these  conditions  K'  appears  as  that  coeffi- 
tr\       10 

cient  the  value  of  which  determines  the  distance,  1,  within  which  the  radiant 
power  is  one-tenth  extinguished,  hence,  "extinction  coefficient." 

As  specified  in  their  derivation,  and  as  indicated  by  means  of  the 
subscript  X,  equations  (5)  and  (6)  are  applicable  only  when  the 
wave-length  is  specified.  In  practice  very  narrow  bands  of  the 
spectrum  are  used.  Using  these  narrow  bands  and  determining 
at  successive  wave-lengths  the  specific  transmissive  indices  we 
can  chart  so-called  absorption  curves.  (See  figs.  20  and  24.) 
For  regions  of  the  spectrum  in  which  the  wave-length  is  lower 
than  the  wave-length  of  visible  radiant  energy  photographic 
methods  are  employed.  For  regions  in  which  the  wave-length  is 
larger  than  the  wave-length  of  visible  radiant  energy  thermo- 
electric methods  are  used.  Undoubtedly  the  most  fundamental 
data  will  be  obtained  when  indicators  are  examined  with  radiant 
energy  of  a  wide  range  of  wave-length,  but  the  immediate  task  is 
to  make  use  of  visible  radiant  energy. 

SPECTROPHOTOMETERS 

A  brief  description  of  a  remarkably  direct-reading  instrument, 
the  Keuffel  and  Esser  Color  Analyser,  will  show  how  the  trans- 
mittance of  a  solution  may  be  measured.  Figure  21  is  a  diagram- 
matic representation  of  the  instrument.  See  Keuft'el  (1925). 

Radiant  energy  from  tungsten  lamps,  12,  in  the  "integrating" 
sphere,  1,  is  diffusely  reflected  from  two  blocks  of  magnesia  held 


146 


THE  DETERMINATION  OF  HYDROGEN  IONS 


at  6  and  7.  The  two  beams  of  radiant  energy  pass  through  the 
slit  17  of  the  collimator,  and  are  brought  by  the  collimator  to  the 
prism  19.  The  position  of  this  prism,  which  can  be  rotated  by 
the  drum  with  wave-length  scale  4,  determines  the  narrow  band  of 
the  spectrum  in  the  photometric  field  at  the  eye-piece  21.  By 
means  of  the  biprism  20  placed  over  the  lens  18,  there  is  produced 
the  photometric  field  of  the  type  illustrated  by  9.  The  energy 
in  one -half  of  this  field  comes  by  one  of  the  beams  and  that  in  the 
other  comes  by  the  second  beam. 


1.  Spherical  Light  Source. 

2.  Photometer. 

3.  Spectromter. 

4.  Wave  Length  Scale. 

5.  Photometer  Scale. 

6.  Holder  for  Standard  Sample. 

7.  Holder  for  [Reflection  Sam- 

ples. 

ft.  Hold  erf  or  Transparent  Sam- 
ples. 

9.  Field  of  View  thru  Eye  Slit. 

10.  To  Vacuum  Ventilator. 

11.  Plug  for  Vacuum  Ventilator 
li.  400  Watt  Lamps. 

13.  Lever    for    Kaising    Photo- 

meter. 

14.  Sector  Discs. 

15.  Universal  110  Volt  Motor. 

16.  Speed  Control  Rheostat. 

17.  Entrance  Slit. 

18.  Collimator  Objectives. 

19.  Dispersion  Prism. 

20.  Bi-Prism. 

21.  Eye  Slit. 

22.  Cast  Aluminum  Base. 


Diagram  of  K    A,  E    COLOR  ANALYZER 


FIG.  21 
(Courtesy  of  Keuffel  and  Esser  Company) 

The  one  beam  passes  through  the  solution  which  is  under  ex- 
amination and  which  is  held  at  8.  The  other  beam  passes  through 
a  tube  of  the  same  length  and  similar  glass  end-plates  (also  held 
at  8)  but  containing  the  solvent  alone.  The  power  in  the  given 
narrow  section  of  the  spectrum  as  seen  at  the  eye-piece  is  now  cut 
down  by  the  rotating  sector,  14,  until  photometric  match  is  ob- 
tained. The  openings  of  the  sector  are  controlled  in  an  ingenious 
way  while  the  sector  is  rotating.  The  drum  controlling  these 
openings  is  so  marked  (scale  5)  as  to  indicate  directly  the  per- 
centage transmission. 


VII 


SPECTROPHOTOMETERS 


147 


Since  the  transmission  by  the  solvent  and  by  the  end-plates  are 
compensated  by  placing  in  the  path  of  the  second  beam  a  similar 
tube  of  like  length  and  solvent,  the  percentage  transmission  ob- 
served is  that  of  the  solute,  conditioned,  of  course,  by  the  solvent. 

The  percentage  transmission  is  one  hundred  times^the  trans- 
mitt  ance  T. 

In  some  instruments  the  photometric  match  is  obtained  by 
altering  the  actual  or  virtual  distances  of  two  sources. 

One  of  the  most  frequently  used  devices  is  the  Konig-Martens 
photometer,  the  principal  features  of  which  are  indicated  by 
figure  22. 


a.  .A 


D-  Ji  -O— I 

~t*       II  II  "U2    !    " 

s 

FIG.  22.  (Above)  PRINCIPAL  FEATURES  OF  THE  KONIG-MARTENS  PHO- 
TOMETER; (Below)  ARRANGEMENT  OF  TUBES  IN  PHOTOMETER 

Two  beams  of  radiant  energy  coming  through  apertures  A  and 
B  are  to  be  reduced  to  equal  power  at  the  eye-piece  O.  The 
beams  are  converged  by  the  biprism  C  to  the  collecting  lens  D  and 
thence  pass  through  the  Wollaston  prism  W.  The  Wollaston 
prism  is  a  crystal  of  calcite  so  cut  as  to  separate  the  "ordinary" 
and  "extraordinary"  rays  of  the  double  refraction  and  deliver 
them  polarized  in  planes  mutually  perpendicular.  Each  of  the 
original  beams,  a  and  b,  is  thus  divided  into  two  and  each  of  these 
is  redivided  by  the  biprism  F.  Thereby  eight  images  correspond- 
ing to  the  two  apertures  A  and  B  are  formed.  The  polarization 
of  each  is  indicated  in  the  figure.  All  but  one  pair  of  these  images  is 
screened  or  absorbed  by  the  walls  of  the  instrument.  In  the  pair 
selected  the  polarizations  are  in  planes  mutually  perpendicular. 


148 


THE  DETERMINATION  OF  HYDROGEN  IONS 


At  N  is  a  Nicol  prism  which  can  be  turned.  At  one  position  it 
reduces  to  zero  the  amplitude  of  vibration  in  the  ray  that  gives 
image  A'.  At  90°  from  this  position  it  reduces  to  zero  the 
amplitude  of  vibration  in  the  ray  that  gives  image  IV. 

If  the  power  at  A  equals  the  power  at  B  and  there  are  no  inci- 
dental polarizations  at  the  surfaces  of  the  optical  parts,  and  if 
there  is  no  inequality  of  absorption  in  the  paths,  there  will  be 
photometric  match  between  A'  and  B'  when  the  Nicol  is  turned 
45°  with  relation  to  either  of  the  extinction  settings. 

But  assume  that  the  radiant  power  at  A  is  not  equal  to  that 
at  B.  The  angle  at  which  the  Nicol  must  be  turned  is  related  to 
the  ratio  of  the  powers  at  A  and  B  as  follows: 

Suppose  beam  a  is  polarized  in  the  direction  OA,  figure  23.  Let 
the  amplitude  of  the  vibrations  be  represented  by  the  distance 


FIG.  23 

OA.  If  the  Nicol  be  turned  so  that  its  optic  axis  conforms  to 
OA  it  will  not  affect  the  amplitude.  If  it  be  turned  90°  from  OA 
it  will  reduce  the  amplitude  of  vibration  in  beam  a  to  zero.  At 
any  angle  6  the  amplitude  of  the  vibrations  in  beam  a  which 
will  be  transmitted  by  the  Nicol  will  be  represented  by  the  dis- 
tance OC.  Likewise  for  beam  b  the  amplitude  of  the  vibrations 
transmitted  by  the  Nicol  will  be  OD. 
Geometrically  we  have 


OC  =  OA  sine  B 
OD  =  OB  cos  6 


or 


OD      OB 


(7) 
(8) 

(9) 


Again  consider  figure  22  in  which  the  photometer  with  aper- 
tures A  and  B  is  placed  in  train  with  the  beams  a  and  6  which  pass 
through  tubes  of  absorbing  solution  and  solvent  respectively. 


VII  PHOTOMETER   EQUATION  149 

For  purposes  of  generality  we  shall  assume  that  the  light  source, 
S,  delivers  to  the  absorbing  tubes  energy  of  unequal  power  Pal 
and  Pbi-  For  simplicity  of  exposition  we  shall  imagine  that  the 
solvent  and  solution  are  held  in  like  tubes  of  equal  length.  Also 
we  shall  imagine  that  the  solute  is  removed  from  the  solution  tube 
and  placed  in  a  space  of  the  same  dimensions. 

The  various  Ps  in  the  figure  represent  the  powers  of  the 
radiant  energies  at  the  several  points. 

The  ratio  of  the  powers  of  two  beams  equals  the  ratio  of  the 
squares  of  the  amplitudes. 

Therefore, 

¥  =  =  do) 

Pb3      ODa 

Photometric  match  is  determined  by  adjustments  to  the  con- 
dition that  Pa4  =  Pbs.  Using  this  relation  and  equations  (9)  and 
(10)  we  obtain 

L  =  tan20  (11) 

OA2 

Since 


OA2          Pa3 

^-2  =  tan2  0  (12) 

Pa3 

The  transmittance  of  the  solute  is  given  by: 

T  =  |^  (13) 

The  transmittance  of  the  solvent  is  given  by  the  identities 


JL  al  -Tbl 

Combination  of  equations  (12),  (13),  and  (14)  yields: 


Pbi 


tan2  9  (15) 


150         THE  DETERMINATION  OF  HYDROGEN  IONS 

If  no  absorbents  were  in  the  train,  (T  =  1),  photometric  match 
would  be  obtained  at  a  new  angle  8'  of  the  Nicol  in  place  of  6 

P  P 

of  equation  (12)  and  the  ratio  -^  would  be  replaced  by  =£1. 

*a3  Pal 

Hence  for  the  "zero  setting"  of  the  instrument 

^  =  tan°9'  (16) 

ial 

Substitute  this  in  (15)  and  obtain: 

T  =  cot2  6  X  tan2  tf  (17) 

If  the  instrument  conformed  to  the  theory  given  above  and  if 
the  light-source  were  such  that  Pai  =  Pbi,  (16)  would  become 

1   =  tan2  0'  (18) 

or 

B'  =  45°,  135°,  225°  or  315°. 

If  the  instrument  alter  the  amplitude  of  the  vibrations  in  either 
ray  by  slight  polarization  at  glass  surfaces,  it  is  equivalent  to 
altering  the  relative  powers  Pal  and  Pbl.  Thus,  for  example,  a 
"zero-setting"  may  occur  at  46°  instead  of  45°  even  if  Pai  =  PM- 

In  (17)  0',  it  will  be  remembered,  is  the  angle  at  "zero-setting" 
while  B  is  the  angle  with  absorbents  in  train. 

In  case  the  tubes  are  reversed  we  have 

T  =  tan2  0  X  cot2  0'  (19) 

According  to  equation  (17)  or  (19)  the  transmittance  desired 
is  determined  as  follows.  First  make  photometric  match  with 
no  absorbents  in  train.  Read  the  angle  B'.  Second  make  the 
reading  with  tubes  of  solvent  and  solution  in  train  and  read  the 
angle  0.  In  each  case  the  angle  is  that  at  photometric  match. 

It  has  been  tacitly  assumed  that  energy  of  one  wave  length  or 
narrow  spectral  band  has  been  used.  The  spectrometer  deliver- 
ing this  to  the  eye  is  usually  placed  beyond  the  photometer. 
This  virtually  accomplishes  the  desired  limitation. 

For  further  information  on  spectrophotometers  consult :  Walsh 
(1926). 


VII 


ABSORPTION   CURVES 


151 


BROM 
PHENOL 
BLUE 

1=5.0  em. 
c-0.02  g.  per 


THYMOL 
BLUE 

AC. 
1=5.0  cm.       I   RED 

C  =  0,04  o.          |1  '5.0cm. 
per  tOO cc.  -\c*0.(U5g.  \\vs// 
per  100 


BROM 

THYMOL 

BLUE 


BROM 
CRESOL 
PURPLE 


1  =  5.0  cm. 
c  =  0.032  g.  per 
lOOcc 


1  =  5.0  cm. 
C=0.04£.  per 

100  cc. 


1  =  5.0  cm. 

C  =  0.016  g.  per 

100  cc. 


1=5.0  cm. 

c  =  0.032  g.  per 


1  =  5.0  cm. 
c  =  0.01a.  per 


440   480    520    560    600 


480    520    560    60O    640 


460     520    560   600 


WAVE  LENGTH.  M/AS-MILLIMICRONS^  METERS  x  io~9 

FIG.   24.  ABSORPTION   CURVES   OP  SEVEN   SULFONPHTHALEINS,    METHYL 

RED  AND  PHENOL  PHTHALEIN 

(After  Erode  (1924)) 


152  THE   DETERMINATION    OF   HYDROGEN   IONS 

ABSORPTION   CURVES 

By  use  of  a  spectrophotometer  the  value  of  a  transmittance,  T, 
or  the  value  of  —log  T  at  any  given  wave-length  or  narrow 
section  of  the  spectrum  within  the  range  of  visibility  is  deter- 
mined. When  determinations  are  made  at  successive  wave- 
lengths the  results  may  be  charted  and  a  curve  drawn  through  the 
points.  Such  a  curve  is  called  an  absorption  curve  or  a  trans- 
mittance curve,  according  to  the  manner  of  charting,  or  choice. 

Typical  transmittance  curves  are  shown  in  figure  24.  Each  curve 
represents  the  relation  of  —log  T  to  X,  expressed  in  m/z,  when 
the  indicator  was  kept  in  a  solution  of  the  pH  value  indicated  by 
the  number.  These  curves  were  determined  by  Erode  (1924). 
Each  individual  curve  in  figure  24  was  determined  while  the 
solution  was  held  at  a  constant  value  of  pH  by  means  of  a  buffer 
solution.  In  each  instance  the  pH  number  is  indicated.  Any 
such  curve  can  be  called  an  "isohydric  transmittance  curve." 
Thiel,  Dassler  and  Wulfken  (1924)  call  them  ''isobathmen." 

It  is  evident  in  figure  24  that  the  isohydric  absorption  curve 
changes  in  some  regular  way  when  the  pH  value  of  the  indicator 
solution  is  changed.  We  naturally  ascribe  this  to  the  change  in 
the  degree  of  dissociation  of  the  indicator,  and  since  the  curve  for 
a  very  low  pH  value  is  distinctly  different  from  that  for  a  com- 
paratively high  pH  value  we  are  led  to  attribute  to  the  ion  and 
to  the  undissociated  molecule  a  qualitative  difference  in  their 
abilities  to  absorb  radiant  energy. 

According  to  equation  (6)  the  effect  of  doubling  the  concentra- 
tion c  can  be  compensated  by  halving  the  length.  Therefore, 
to  make  the  argument  simple,  let  it  be  imagined  that  all  the  ions 
are  forced  into  the  first  half  of  the  tube,  and  all  the  undissociated 
molecules  into  the  second  half.  The  final  effect  will  be  unchanged 
but  we  may  now  consider  separately  the  transmission  by  the 
ions  and  by  the  undissociated  molecules. 

Let  the  radiant  power  incident  at  the  first  surface  of  the  solu- 
tion containing  the  ions  be  PI  and  that  leaving  this  solution  be 
P2.  Then  up  to  this  surface 


Pi 


VII  ABSORPTION   CURVES  153 

where  KI  is  the  molar  transmissive  index  of  the  ions,  c  is  the  con- 
centration of  the  indicator  in  the  undivided  solution,  1  is  the  length 
of  the  whole  solution  and  a  is  the  degree  of  dissociation.  In  the 
half  of  the  divided  solution  c  has  been  doubled  but  1  has  been 

halved  l-2co;  =  L 


For  the  second  part  of  the  path  of  the  radiant  energy  let  P3 
be  the  radiant  power  leaving  the  solution  of  the  undissociated 
molecules.  Then 


where  Ku  is  the  molar  transmissive  index  of  the  undissociated 
molecules.  The  total  transmittance  equals  •*_?.  Hence 

-  log  T  =  lc[«Ki  +  (1  -  a)  KJ  (20) 

If  a  =  1,  —  log  T  =  IcKi.  Thus,  if  the  pH  value  of  the  solution  is 
such  as  to  cause  complete  dissociation,  the  observed  transmittance 
is  that  of  the  ions  alone  and  the  measurable  value  of  Ki  at  a  given 
wave-length,  or  the  absorption  curve  relating  Ki  to  X,  becomes 
characteristic  of  the  ions.  Likewise,  if  a  =  0,  —  log  T  =  lcKu; 
and  now  the  isohydric  absorption  curve  becomes  characteristic 
of  the  undissociated  molecules. 

It  frequently  happens  that  as  the  wave-length  changes  in  one 
direction  the  values  of  Ki  and  Ku  approach  and  at  some  one 
value  of  X  become  equal.  Then  by  equation  (20) 


-  log  T  =  IcKi  =  lcKu  (21) 

In  (21)  the  degree  of  dissociation,  a,  does  not  appear.  This 
means  that  each  isohydric  curve  should  pass  through  some 
common  point  as  most  of  them  are  seen  to  do  in  figure  24.  This 
point  Thiel,  Dassler  and  Wlilfken  (1924)  call  "der  isobestischer 
Punkt."  Prideaux  (1926)  adopts  "isobestic  point." 

It  may  be  noted  that  the  isobestic  point  is  not  merely  a  point 
of  intersection  between  the  curve  characteristic  of  the  ions  alone 
and  the  curve  characteristic  of  the  molecules  alone,  but  that  it  is 
a  point  of  intersection  between  all  isohydric  curves  whatever  the 


154  THE    DETERMINATION    OF   HYDROGEN   IONS 

value  of  the  degree  of  dissociation.  Consequently  the  probability 
of  its  occurrence  is  low  unless  two  "colored"  components  and  two 
only  have  some  intimate  relation  as  have  the  ions  and  undissociated 
molecules  in  our  equilibrium  equation. 

If  then  the  instrumental  accuracy  of  the  spectrophotometric 
measurements  be  adequate  to  establish  the  actual  rather  than  the 
apparent  occurrence  of  an  isobestic  point,  it  would  be  presumptive 
proof  that  two  absorbing  components  of  the  dye  system  and  two 
only  are  related  to  the  hydrion  concentration  of  the  solution, 
within  the  range  of  pH  where  the  point  suffers  no  displacement. 

Not  infrequently  there  are  to  be  observed,  in  the  published 
charts  and  tables  of  indicator  absorption  data,  indications  that 
there  is  a  true  isobestic  point  for  a  limited  range  of  pH  values  but 
that  an  extreme  change  of  pH  throws  the  absorption  curve  out  of 
conformity.  This  suggests  the  formation  of  a  new  absorbing 
species.  If  so,  nonconformity  to  the  isobestic  point  should  be 
used  as  a  warning  that  the  argument  to  follow  should  be  modified, 
and  that,  in  the  spectrophotometric  method  of  determining  pH 
values,  on  isohydric  curves  that  do  not  conform  to  the  isobestic 
point  are  to  be  avoided. 

SPECTROPHOTOMETRIC   DETERMINATION    OF    DISSOCIATION 
CONSTANTS 

Let  it  be  assumed  that  equation  (20)  is  applicable.  Let  the 
pH  value  of  the  solution  be  changed  in  one  direction  until  the 
values  of  —  log  T  no  longer  change.  It  is  then  to  be  presumed 
that  a.  has  become  either  1  or  0,  according  to  the  acidic  or  basic 
nature  of  the  indicator  and  the  direction  of  the  change  in  pH.  Let 
the  pH  value  of  the  solution  now  be  changed  in  the  other  direc- 
tion until  the  values  of  —  log  T  no  longer  change.  It  is  of  course 
impossible  to  tell  from  the  spectrophotometric  measurements 
whether  an  acidic  or  a  basic  indicator  is  being  used  but,  as  indi- 
cated in  Chapter  I,  the  data  in  either  case  can  be  treated  as  if 
for  an  acid.  Inspection  of  the  absorption  curves  for  the  disso- 
ciated and  undissociated  indicator  shows  whether  or  not  there  is 
a  wave-length  at  which  either  KI  or  Ku,  as  it  appears  in  equation 
(20),  is  negligible.  This  wave-length  should  be  as  near  as  prac- 
ticable to  the  peak  of  the  curve  for  the  chosen  species,  provided 
that  it  does  not  depart  far  from  the  region  of  good  visibility, 


VII  DETERMINATION   OF   INDICATOR   CONSTANTS  155 

presently  to  be  discussed.  Let  us  assume  that  the  ion  is  the 
chosen  species  and  that  the  wave-length  is  such  that  (20)  approxi- 
mates closely  to 

-  log  T  =  lea  Ki  (22) 

Determine  —  log  T  when  it  is  certain  that  the  alkalinity  of  the 
solution  is  sufficient  to  make  a  practically  unity.  Then  —  log 
Tm  =  IcKi,  at  a  specific  value  of  X  where  Tm  indicates  minimum 
transmittance  (maximum  absorption).  Now  change  the  pH  value 
of  the  solution  till  it  is  within  that  range  where  a  lies  between 
0.9  and  0.1;  and,  having  measured  the  pH  value  of  the  well- 
buffered  solution  without  the  indicator,  determine  (for  the  same 
wave-length  previously  used)  the  new  value  of  —  log  T.  This 
will  be  designated  by  —  log  Tx.  Then 

(23) 


—  log 

In  some  cases  it  contributes  to  accuracy  of  measurement  if  the 
concentration  or  the  tube  length  is  varied.  In  that  case  there 
can  be  used  the  equivalent  of  equation  (23),  namely: 

=  lm  cmKi  logT, 
lxcxKi   logTm 

Remembering  that  we  are  using  one  wave-length,  we  can  cancel 
KI  from  equation  (24).  Also  the  exact  concentrations  cm  and 
cx  need  not  be  known  if  the  ratio  be  known. 

The  values  of  a  having  been  determined  in  a  number  of  cases, 
there  is  used  the  familiar  equation 

pH  =  pK  +  log 


1  -  a 

pH  values  being  known  from  the  buffers  used,  pK  is  now  cal- 
culated. 

Holmes  (1924)  uses  the  transmittances  of  both  ion  and"  undis- 
sociated  molecules  in  the  following  manner.  Select  two  wave- 
lengths Xi  and  X2,  preferably  in  regions  of  good  visibility,  one 
preferably  near  the  peak  of  the  curve  for  the  ion  and  the  other 
preferably  near  the  peak  of  the  curve  for  the  undissociated  mole- 


156  THE   DETERMINATION   OF   HYDROGEN   IONS 

cule.  If  it  happens  that  these  wave-lengths  are  such  that  in  one 
case  KIM  =  0  and  in  the  other  case  Ku\2  =  0,  equation  (23)  will 
apply  to  the  ions  and  a  similar  equation  will  apply  to  the  undis- 
sociated  molecules.  To  distinguish  the  cases  the  subscripts  i\i 
and  u\2  will  be  used  with  obvious  meanings. 

[log  TjjXi  ,    . 

=  Ri  (25) 


-  a  = 


=  Ru  (26) 


pK  is  found  directly  from  the  relation  : 

PH  =  pK  +  log|i  (27) 

Ku 

As  Holmes  (1924)  notes,  the  change  in  the  concentrations  of  the 

•p  . 

ions  and  the  ionogen  both  contribute  to  the  ratio  ^  and  con- 

Ku 

sequently  the  use  of  this  ratio  is  preferable,  where  practicable. 

In  case  there  cannot  be  selected  a  wave-length  at  which  the 
absorption  is  due  practically  to  the  ion  or  the  ionogen  alone, 
equation  (20)  must  be  used.  The  resulting  equations  for  a  by 
either  of  the  above  principles  becomes  somewhat  more  com- 
plicated (cf.  Vies,  1925),  but  this  in  itself  is  not  serious.  The  real 
difficulty  lies  in  the  accurate  estimation  of  KI  and  Ku  which  can 
no  longer  be  eliminated.  The  determination  of  a  transmissive 
index  requires  a  pure  compound  used  in  known  concentration. 
If  the  pure  compound  is  not  available  the  apparent  transmissive 
indices  must  be  determined. 

SPECTROPHOTOMETRIC   DETERMINATION   OF  pH 

There  is  to  be  used  the  equation: 
pH  =  pK  +  log 


1  -  a 

The  value  of  a  is  to  be  determined  by  the  ratio  .         *  where 

log  Tm 

Tx  is  the  transmittance  of  the  tested  solution  containing  the 


VII 


DETERMINATION   OF   pH 


157 


indicator  partially  transformed  and  Tm  is  the  transmittance  of 
the  indicator  fully  transformed.  Therefore  pK  must  have  been 
previously  determined  by  the  method  described  in  the  previous 
section  and  by  the  use  of  buffers  which  now  become  the  standard 
of  reference.  See  table  25. 


TABLE  25 

pK  values  and  absorption  maxima  of  sulfonphthaleins 
A.  =  solution  used  for  full  transformation. 
Solutions:  1.  Between  20  and  36  per  cent  HC1. 

2.  M/20  borax. 

3.  M/2  trisodium  phosphate. 

Formulas:  a.  pH  =  pK  —  log 


b.  pH  =  pK  +  log 


1  -  a. 

a 


log  T, 


1  -  a  log  Tm 

Standards  of  reference:  Clark  and  Lubs'  buffer  solutions. 


INDICATOR 

pK 

WAVE-LENGTH 
OF  MINIMUM 
TRANSM  ITT  ANCE 

A 

FOR- 
MULA 

m-cresol  purple  (acid  range)  

1.51 

533  (Cohen) 

1 

a 

Thymol  blue  (acid  range)       

1  5 

544  (Erode) 

1 

a 

Brom  chlor  phenol  blue 

3  98 

596  (Cohen) 

2 

b 

Broin  phenol  blue     

4.10 

592  (Erode) 

2 

b 

Brom  cresol  green  ( 

4.68 

614  (Holmes) 

2 

b 

Chlor  cresol  green  

4.67 

4.8 

617  (Cohen) 
612  (Cohen) 

2 

b 

Chlor  phenol  red                        

5  98 

573  (Cohen) 

?, 

b 

Brom  phenol  red  

6.16 

574  (Cohen) 

2 

b 

Brom  cresol  purple             

6  3 

591  (Erode) 

?, 

b 

Brom  thymol  blue 

7  0 

617  (Erode) 

3 

b 

Phenol  red         

7.9 

558  (Erode) 

3 

b 

Cresol  red                                        

8  3 

572  (Erode) 

3 

b 

m-cresol  purple  (alkaline  range)  

8.32 

580  (Cohen) 

3 

b 

Thymol  blue  (alkaline  range)  .         .     \ 

8.91 

596  (Holmes) 

3 

b 

8.90 

596  (Erode) 

3 

b 

Establish  by  trial  that  strength  of  the  standard  indicator  solu- 
tion which,  with  the  tube  length  selected,  will  give  a  transmit- 
tance of  0.2-0.1,  when  the  indicator  is  fully  transformed  to  the 
"alkaline"  (or,  if  preferred,  to  the  "acid")  form.  Establish 
accurately  the  value  of  log  Tm.  Then  with  the  same  indicator 


158  THE   DETERMINATION    OF   HYDROGEN   IONS 

solution  added  in  the  same  proportion  to  the  tested  solution  deter- 
mine log  Tx.  Introduce  the  values  into  the  above  equation  and 
with  the  given  value  of  pK  solve  for  pH.  To  facilitate  such  cal- 
culations there  is  given  in  Appendix  F  (page  677)  values  of  log 

— for  various  values  of  a. 

I— a 

There  can  be  used  also  the  ~  values  as  discussed  in  the  pre- 

Ku 

vious  section. 

In  table  25  are  given  the  wave-lengths  at  which  maximum  ab- 
sorption of  several  indicators  are  reported.  It  is  well  to  select 
a  wave-length  near  such  a  "peak."  There  might  have  been  in- 
cluded the  extinction  coefficients  for  these  stated  wave-lengths. 
However,  extinction  coefficients  are  misleading  in  practical  appli- 
cations of  the  method  because,  to  be  of  universal  significance, 
they  would  have  to  apply  to  these  rare  articles  of  commerce — 
pure  indicators.  One  hundred  per  cent  purity  of  indicator  and 
perfection  in  the  construction  of  a  standard  solution  of  known 
concentration  cannot  always  be  depended  upon  and,  as  shown, 
are  unnecessary  to  the  method  when  a  wave-length  can  be 
selected  at  which  the  equations  permit  the  elimination  of  one  or 
the  other  extinction  coefficient. 

For  the  production  of  the  full  transformation  of  the  indicator 
the  same  precautions  must  be  used  that  are  applied  in  the  Gil- 
lespie  method.  Data  for  the  sulfonphthaleins  are  found  in  table 
14  (page  122). 

A  fundamental  assumption  in  the  method  as  described  is  that 
the  specific  absorptive  property  of  the  ion  and  of  the  ionogen 
are  not  affected  by  change  in  the  general  composition  of  the  solu- 
tion, e.g.,  alteration  of  "salt"  content  by  addition  of  neutral  salt 
or  change  in  buffer  composition.  That  this  assumption  is  not 
justified  in  strictness  is  shown  by  Halban  and  Ebert  (1924). 

Of  the  method,  Holmes  (1924)  remarks: 

"With  judicious  selection  of  indicators  and  technique  the  spectrophoto- 
metric  method  affords  the  maximum  accuracy  possible  in  indicator 

methods The    phenomena    of    dichromatism,    encountered   with 

many  indicators,  introduce  no  interference.  The  presence  of  such  degrees 
of  color  and  turbidity  as  are  ordinarily  met  in  solutions  to  be  evaluated 
does  not  affect  the  accuracy  with  which  the  ratios  may  be  measured, 


VII 


DETERMINATION   OF   pH 


159 


since  the  technique  of  spectrophotometric  practice  is,  or  may  be  made, 
such  that  an  exact  compensation  for  their  effects  is  obtained  automati- 
cally. The  difficulties  introduced  by  excessive  color  or  turbidity  may  be 
overcome  by  increasing  the  concentration  of  the  indicator  and  decreasing 
the  thickness  of  the  layer  of  solution  employed  in  the  measurements. 
The  resort  to  thin  layers  of  solution  should  also  render  it  possible  to 
determine  the  ratio  of  a  solution  when  only  a  few  drops  of  material  may  be 
available  for  examination." 

A  fuller  discussion  of  the  effect  of  turbidity  would  be  welcome. 
In  passing  it  is  well  to  note  how  well  the  values  of  a,  determined 
spectrophotometrically,  conform  to  the  type  curve  corresponding 
to  the  simple  equation 


URGENT  TRANSFORMATION 

8*  0>  OB  0 
O  O  O  O 

pH  =  pK  +  log  - 
1  —  a 

/ 

rf^ 

/ 

< 

I 

7 

/ 

t 

1 

/ 

S 

^ 

/ 

10        II 


pH 


FIG.  25.  RELATION  OF  pH  TO  PER  CENT  TRANSFORMATION  OF  BROM  CRESOL 

GREEN  (pK  =  4.68)  AND  OF  THYMOL  BLUE  (pK  =  8.91) 

(After  Holmes  and  Snyder  (1925)) 

Determinations  by  Holmes  and  Snyder   (1925)   are  shown  in 
figure  25. 

Other  references  to  the  use  of  spectroscopy  in  indicator  work  are : 
Birge  and  Acree  (1919),  Baker  and  Davidson  (1922),  Brue're 
(1925),  Henri  and  Fromageot  (1925),  Hildebrand  (1908),  Buch 
(1926),  Lund  (1927),  Moir  (1916),  Morton  and  Tipping  (1925), 
Paulus,  Hutchinson,  and  Jones  (1915),  Prideaux  (1925),  Siegler- 
Soru  (1927),  Stenstrom  and  Reinhard  (1925),  Vies  et  al.  (1922- 
1927).  Adams  and  Rosenstein  (1914),  Brightman  et  al.  (1918- 
1920),  Hirsch  (1925). 


160 


THE    DETERMINATION   OF   HYDROGEN   IONS 


EFFECTS  OF  ABSORPTION  ON  THE  STIMULUS  AS  IT  REACHES  THE  EYE 

•p 

Transmittance,  is  merely  the  fraction  ~,  the  fraction  of  the 

-t  i 

power  incident  at  the  surface  1  which  emerges  at  the  surface  2. 
It  has  been  particularly  noted  that  this  fraction  varies  with  the 

TABLE  26 

Relative  visibility  of  radiant  energy  of  different  wave  length  and  spectral 
distribution  of  relative  radiant  energy  for  standard  white  light 


WAVE 
LENGTH 

RELATI\  B 
VISIBILITY* 

RELATIVE 
RADIANT 
ENERGY  — 
STANDARD 
WHITE  LIGHTf 

WAVE 
LENGTH 

RELATIVE 
VISIBILITY* 

RELATIVE 
RADIANT 
ENERGY  — 
STANDARD 
WHITE  LIGHTf 

mp 

mn 

400 

0.0004 

53.33 

550 

0.995 

100.95 

410 

0.0012 

60.00 

560 

0.995 

100.00 

420 

0.0040 

66.67 

570 

0.952 

99.05 

430 

0.0116 

69.52 

580 

0.870 

97.14 

440 

0.023 

77.14 

590 

0.757 

95.24 

450 

0.038 

86.19 

600 

0.631 

94.29 

460 

0.060 

92.38 

610 

0.503 

93.33 

470 

0.091 

96.19 

620 

0.381 

92.38 

480 

0.139 

99.05 

630 

0.265 

91.43 

490 

0.208 

100.48 

640 

0.175 

90.48 

500 

0.323 

100.95 

650 

0.107 

89.52 

510 

0.503 

101.43 

660 

0.061 

87.62 

520 

0.710 

100.95 

670 

0.032 

86.19 

530 

0.862 

100.95 

680 

0.017 

84.29 

540 

0.954 

100.95 

690 

0.0082 

82.86 

700 

0.0041 

80.48 

*  Provisionally  adopted  by  the  International  Commission  on  Illumina- 
tion, Geneva,  July,  1924.  See  Gibson  et  al.  (1925). 

t  Average  noon  sun  at  Washington.  Used  as  standard  white.  See 
Gibson  et  al.  (1925). 

wave-length.  It  must  now  be  emphasized  that  the  values  of  the 
incident  power  at  different  wave-lengths  vary  with  the  source. 
In  table  26  are  shown  relative  intensities  at  different  wave-lengths 
of  the  radiant  energy  of  white  light.  The  values  given  are 
proportional  to  the  relative  powers.  By  means  of  the  relative 


VII  LUMINOSITY  161 

p 

value  of  PI  and  the  value  of  the  fraction  =^  (i.e.,  T)  there  can 

-T2 

now  be  calculated  the  value  of  P?  for  any  wave-length.  P2,  as 
evaluated  in  relative  terms,  is  the  destined  stimulus  as  it  leaves 
the  solution  on  its  way  to  the  eye. 

Now  the  visibility  of  radiant  energy  varies  greatly  with  the 
wave-length.  Standard  values  of  relative  visibility  provisionally 
adopted  in  1924  by  the  International  Commission  on  Illumina- 
tion as  quoted  by  Gibson  et  at.  (1925)  are  shown  in  table  26. 
The  product  of  the  relative  visibility  and  the  relative  value  of  P2 
at  a  given  wave-length  is  the  relative  light  or  the  luminosity  for 
the  wave-length  under  consideration. 

At  this  point  attention  may  be  called  to  our  previous  avoidance 
of  the  word  "light."  It  is  a  word  which  is  in  such  common  use 
that  no  committee  can  ever  dictate  its  good  and  proper  usage. 
Yet,  in  an  exposition  of  such  technical  matters  as  those  now 
under  discussion  there  is  a  distinct  advantage  in  adhering  to  the 
nomenclature  of  the  Colorimetry  Report  (Troland,  1922)  wherein 
the  physical  aspects  of  radiation  are  kept  distinct  from  physio- 
logical effects.  There  it  is  stated,  that  light  is  to  be  regarded  as  a 
"Psycho-physical"  quantity.  It  is  defined  "as  the  product  of 
absolute  power  and  visibility  measures  for  any  given  sample  of 
radiant  energy," 

"Relative  light  quantities  are  called  luminosities.'" 

The  only  immediate  concern  which  we  have  for  luminosity, 
in  the  application  of  the  spedrophotometer  is  that  the  luminosity 
shall  be  sufficient  to  make  possible  accurate  measurements  in 
which  the  eye  is  the  detector  of  inequalities.  On  the  other  hand, 
further  consideration  of  this  quantity  reveals  relations  of  con- 
siderable importance  to  the  direct  visual  observation  of  indicator 
solutions.  An  instance  of  this  will  be  shown  in  the  next  section. 

DICHROMATISM 

Consider  for  instance  a  solution  of  brom  cresol  purple  which 
at  pH  7.6  gives  the  transmittance  curve  indicated  in  figure  24. 
By  means  of  the  data  of  table  26  and  the  values  of  T  read  from  a 
large  scale  drawing  of  figure  24  there  are  calculated  and  plotted 
as  curve  A  of  figure  26  the  variation  of  luminosity  with  wave- 


162 


THE    DETERMINATION    OF   HYDROGEN    IONS 


length.  Now  let  either  the  concentration  or  the  length  of  the 
brom  cresol  purple  solution  be  increased  ten  times  and  for  the 
new  condition  let  there  be  plotted  curve  B. 

In  the  first  case  (low  concentration,  or  short  tube),  the  luminos- 
ity is  greatest  in  the  "blue"  and  "blue-green."  There  is  still  a 
marked  luminosity  in  the  "red."  The  combined  effect  is  "purple." 
In  concentrated  solution  or  deep  layers  as  shown  by  curve  B  there 
is  very  little  luminosity  for  the  "blue"  and  the  luminosity  for  the 
"red"  is  dominant.  The  effect  approaches  "red."  Thus  a  change 
of  concentration  or  length  causes  a  distinct  change  of  color.  This 


440       480       520       560        600       640       680 
Blue         Green   Tfetlow  Orange  Red 

FIG.  26.  LUMINOSITY  CURVES,  CALCULATED  BY  MEANS  OF  THE  TRANS- 
MISSION, THE  RELATIVE  RADIANT  ENERGY  OF  STANDARD  WHITE 

LIGHT  AND  THE  RELATIVE  VISIBILITY 

Curve  A — brom  cresol  purple  in  dilute  solution.     Curve  B — brom  cresol 
purple  in  ten  times  the  concentration  of  case  A. 

is  called  "dichromatism."  It  can  readily  be  observed  with  the 
proper  concentration  of  brom  cresol  purple  by  observing  it  in  a 
test  tube,  first  side  wise  and  then  lengthwise  of  the  tube.  It  is 
of  very  great  importance  in  the  determination  of  pH  values.  In 
the  first  place,  two  solutions  of  like  pH  value  containing  brom 
cresol  purple  will  give  distinct  differences  in  "color"  quality  if 
there  is  an  error  either  in  the  concentration  of  indicator  or  in  the 
depth  of  view.  Secondly,  if  a  solution  containing  suspended 
material  be  compared  with  a  clear  standard,  an  error  may  arise 
from  the  fact  that  in  the  turbid  solution  much  of  the  radiant  energy 
reaching  the  eye  may  not  have  traversed  the  whole  depth  but 


VII  DICHROMATISM  163 

may  have  entered  from  the  side  and  having  been  scattered  by 
the  particles  may  have  traversed  only  a  shallow  layer  of  the 
solution.  Indeed  turbid  solutions  containing  this  indicator  often 
appear  "bluer"  than  the  standard  having  the  same  pH  value  and 
having  the  same  concentration  of  the  indicator.  With  milk  the 
red  tone  of  brom  cresol  purple  is  almost  undetectible  unless  re- 
flected light  be  screened  off. 

This  effect,  dichromatism,  is  operative  to  some  extent  with 
most  indicators  but  it  becomes  distinctly  troublesome  only  with 
indicators  such  as  brom  cresol  purple,  and  brom  phenol  blue,  the 
absorption  curves  of  which  are  located  in  such  a  position  that 
effective  amounts  of  radiant  energy  are  transmitted  in  the  region 
of  visible  "red"  on  the  one  hand  and  visible  "blue"  on  the  other 
hand. 

Since  the  luminosity  is  determined  in  part  by  the  spectral 
distribution  of  the  relative  power  of  the  source,  the  luminosity  at 
a  given  wave-length  will  vary  with  the  source.  Artificial  illu- 
minants,  as,  for  instance,  the  tungsten  lamp  furnish  radiant  energy 
the  power  of  which  at  different  wave-lengths  is  much  less  uniform 
than  that  of  sunlight.  Such  illuminants  are  commonly  de- 
scribed as  deficient  in  "blue"  or  relatively  rich  in  "red."  Thus 
a  dichromatic  indicator  appears  much  "redder"  under  a  tungsten 
lamp  than  in  daylight. 

In  dealing  with  dichromatic  indicators  which  give  trouble  in 
direct  visual  observations,  it  sometimes  helps  to  change  the  source 
of  illumination.  For  instance,  it  is  an  appreciable  although  not 
an  entirely  satisfactory  aid  in  the  use  of  brom  cresol  purple  to 
screen  off  the  "blue"  in  the  source  of  illumination.  This  can  be 
done  crudely  as  follows.  In  an  ordinary  box  of  convenient  size 
are  mounted  three  or  four  large  electric  lights.  A  piece  of  "tin" 
serves  are  reflector.  The  box  may  be  lined  with  asbestos  board. 
A  piece  of  glass,  cut  to  fit  the  box,  is  held  in  place  on  one  side  by 
the  asbestos  lining  and  on  the  other  by  a  few  tacks.  This  glass 
serves  only  to  protect  the  screen  and  is  not  essential.  The  screen 
is  made  from  translucent  paper  known  to  draughtsmen  as  "Econ- 
omy" tracing  paper.  It  is  stretched  across  the  open  side  of  the 
box  and  painted  with  a  solution  consisting  of  5  cc.  of  0.6  per  cent 

phenol  red  and  5  cc.  of  — KH2PO4  (stock  standard  phosphate 

o 


164  THE    DETERMINATION    OF   HYDKOGEN   IONS 

solution).  While  the  paper  is  wet  it  is  stretched  and  pinned  to 
the  box  with  thumb  tacks.  If  a  dark-room  is  not  available  for 
observations,  exterior  light  may  be  shut  off  with  a  photographer's 
black  cloth. 

Blue-yellow  indicators  which  retain  a  dichromatic  red  may  be 
observed  by  mercury  arc.  Its  emission  is  poor  in  "red"  but 
"yellow,"  "green"  and  "blue"  lines  fall  in  the  spectrum  where, 
for  instance,  shifts  in  the  absorption  bands  of  brom  phenol  blue 
occur. 

The  absorption  spectra  of  all  the  indicators  of  the  sulfon 
phthalein  series  are  such  that  the  appearance  of  dichromatism 
must  be  expected  under  certain  conditions.  It  will  be  observed 
with  phenol  red  in  illumination  relatively  poor  in  "red"  and  rich 
in  "blue,"  for  example,  that  of  a  mercury  arc;  and  with  thymol 
blue  in  illumination  relatively  poor  in  "blue"  and  rich  in  "red" 
for  example,  ordinary  electric  light. 

OBSERVATIONS   BY   THE    COLOR-BLIND 

Curiously  enough  the  author  never  has  heard  this  problem  dis- 
cussed until  he  raised  the  question  himself,  a  fact  which  suggests 
that  few  people  have  such  insuperable  difficulties  with  the  indi- 
cator method  that  they  are  conscious  of  possible  personal  limita- 
tions. It  may  be  said  at  once  that  an  adequate  discussion  of 
this  problem  would  require  a  clear  recognition  of  the  various  types 
of  color-blindness  and  that  the  author  is  not  competent  to  deal 
with  the  subject  except  superficially.  One  aspect  is  clear.  The 
physical  phenomena  are  definite.  The  absorption  bands  are 
usually  broad  enough  so  that  some  alteration  with  change  of  pH 
occurs  at  wave-lengths  at  which  eyes  of  limited  deficiencies  are 
still  sensitive.  Consequently,  changes  are  detected.  It  is  a 
matter  of  no  fundamental  importance  that  the  deficiencies  lead  to 
wrong  names  of  colors.  The  serious  aspect  is  deficient  sensitivity 
in  the  region  of  greatest  indicator  change.  When  this  occurs 
there  may  be  manifest  (in  certain  instances)  avoidance  of  red- 
yellow  indicators  and  preferance  for  blue-yellow  indicators  or 
vice  versa  (compare  Saunders  (1923)).  Preferences  arising  from 
real  physiological  deficiencies  and  not  from  esthetics  deserve  more 
study.  Such  problems  became  important  when,  as  frequently 
happens  in  industrial  work,  extensive  measurements  become 


VII  DIFFERENTIATION   BY   EYE  165 

routine  and  rapidity,  accuracy  and  ease  of  measurements  should 
be  encouraged. 

DIFFERENTIATION   BY   EYE 

Let  us  also  consider  the  range  of  an  indicator  as  it  is  deter- 
mined by  the  differentiating  power  of  the  eye.  An  approximate 
treatment  of  this  is  all  that  will  be  attempted. 

Use  the  equation  : 


( 

On  differentiation  the  rate  of  increase  in  a  with  increase  of  pH 
is  found  to  be  : 

-Jfe-  2.3  «(!-*). 

d(pH) 

When 

d*a  I 

0,  a 


d(pH)>  2' 

In  other  words  the  maximum  rate  of  increase  in  dissociation  is  at 
the  half  transformation  point.  This  fixes  a  reference  point  when 
indicators  are  to  be  employed  in  distinguishing  differences  in  pH. 
The  question  now  arises  whether  or  not  this  is  the  central  point 
of  the  optimal  conditions  for  differentiation  of  pH  values.  It 
may  be  said  at  once  that  it  is  not,  because  the  eye  has  not  only 
to  detect  differences  but  also  to  resolve  these  differences  from  the 
color  already  present.  Experience  shows  that  the  point  of  maxi- 
mum rate  of  increase  in  a  is  near  one  limit  of  the  useful  range  and 
that  this  range  lies  on  the  side  of  lower  color.  Thus,  in  the  case 
of  the  one-color  indicator  phenolphthalein,  the  useful  zone  lies 
between  about  8.4  and  9.8  instead  of  being  centered  at  9.7  which 
corresponds  with  the  point  of  half -transformation.  -In  the  case 
of  a  two-color  indicator  such  as  phenol  red  the  same  reasoning 
holds,  because  the  attention  fixes  upon  the  very  dominant  red. 
With  other  two-color  indicators  the  principle  holds  except  when 
there  is  no  very  great  difference  in  the  command  upon  the  atten- 
tion by  one  or  the  other  color. 

It  should  be  mentioned  however  that  these  more  or  less  empiri- 


166  THE    DETERMINATION    OF   HYDROGEN   IONS 

cal  relations  are  observed  in  comparing  colors  at  equal  incre- 
ments of  pH  when  the  indicator  concentration  is  adjusted  to 
emphasize  the  differences  among  the  less  intensely  colored  tubes. 
By  suitable  dilution  of  the  indicator  the  differences  among  the 
tubes  having  the  higher  percentage  color  may  be  emphasized 
and  the  useful  range  of  the  indicator  slightly  extended.  In  prac- 
tice this  is  a  procedure  which  requires  care  for  it  is  easy  to  be- 
come confused  when  dealing  with  different  concentrations  of  the 
same  indicator. 

The  fixing  of  the  lower  pH  limit  of  usefulness  of  a  given  indi- 
cator involves  another  factor.  There  is  the  question  of  the  total 
indicator  which  may  be  brought  into  action.  A  dilute  solution 
of  phenolphthalein  may  appear  quite  colorless  at  pH  8.4  while 
a  much  stronger  solution  will  show  a  distinct  color  which  would 
permit  distinguishing  8.2  from  8.4.  But  the  concentration  is 
limited  by  the  solubility  of  the  indicator  and  this  must  be 
taken  into  consideration.  In  short  there  is  no  basis  upon  which 
to  fix  definite  limits  to  the  pH  range  of  a  given  indicator,  and 
those  limits  which  are  given  must  be  considered  to  be  arbitrary. 
On  the  other  hand  the  apparent  dissociation  curve  is  quite  defini- 
tive; and  were  it  not  for  the  greater  convenience  of  the  "range  of 
usefulness"  it  would  be  preferable  to  define  the  characteristics 
of  an  indicator  in  terms  of  its  apparent  dissociation  constant. 

COLOR 

Translation  of  the  data  of  transmittances  into  luminosities 
requires  the  data  of  table  26.  But  if  an  attempt  is  made  to  carry 
the  matter  further  into  a  description  of  the  psychological  affair 
called  color,  additional  data  are  required.  This  is  beyond  the 
scope  of  this  treatise,  and  since  it  is  we  have  taken  liberties  in 
preceding  paragraphs  and  have  named  stimuli  by  the  names  of 
the  effects,  e.g.,  "red." 

In  no  part  of  our  subject  is  color  quantitatively  evaluated.  As 
we  shall  see  presently  the  ordinary  colorimeter  is  misnamed. 

On  the  other  hand,  when  we  use  two-color  indicators  like  the 
sulfonphthaleins,  and  have  normal  eyes,  we  undoubtedly  utilize 
color  distinction,  which  stands  us  in  good  stead  and  often  becomes 
the  sole  criterion  of  distinctions  when  turbidity  and  other  factors 
interfere  with  the  judgment  of  relative  intensities.  See  also 


VII  COMPAKATOR  167 

page  131  on  the  utilization  of  color-quality  in  observations  of 
"one-color"  indicators. 

THE  "COLORIMETER,"  I.E.,  COMPARATOR 
Beer's  law  is: 

-  log  TX  =  lcKx 

(see  page  144)  where  T  is  the  transmittance  at  a  specified  wave- 
length, X,  1  is  the  length  of  the  absorbing  layer,  c  is  the  concen- 
tration of  absorbing  substance  and  K\  is  a  constant  characteristic 

of  the  absorbing  substance  for  the  specified  wave-length  X.     The 

•p 

transmittance  is  the  ratio,  -=?-,  of  the  power  of  the  radiant  energy 

Jti 

emerging  from  the  solution  to  the  power  incident  at  the  first 
surface. 

Imagine  two  solutions  receiving  from  a  source  the  same  radiant 
power  Pi  at  wave-length  X  and  containing  a  substance  character- 
ized by  the  absorption  constant  K\.  Let  the  length  1  of  one  solu- 
tion or  its  concentration  c,  of  absorbing  material,  be  adjusted 
until  the  emergent  power  P2  is  equal  to  that  of  the  second  solu- 
tion. The  transmittances  will  be  equal  in  each  case.  Then  by 
applying  the  above  equation  to  the  two  cases,  indicated  by  sub- 
scripts 1  and  2,  and  solving,  we  have: 

-  log  Tx  =  lidKx  =  12C2KX;  whence:  lid  =  I2c2 
or 

Cj   =    1^ 
C2          li 

The  ordinary  "colorimeter"  of  the  Duboscq  type  is  a  device 
whereby  the  length  of  absorbing  layers  li  and  12  can  be  varied 
and  measured,  until,  by  an  optical  device  for  bringing  the  photo- 
metric fields  into  juxtaposition  it  is  seen  that  the  transmittances 

are  equal.     If  Ci  is  known,  and  the  ratio  ^  is  measured,  c2  is 

li 
determined. 

In  the  treatment  given  above,  it  was  tacitly  assumed  that 
absorption  by  the  solvent  could  be  neglected.  This  assumption 
is  not  serious.  The  specification  that  there  is  to  be  used  radiant 
energy  of  one  wave-length  ("monochromatic  light")  is,  of  course, 


168 


THE  DETERMINATION  OF  HYDROGEN  IONS 


not  usually  met.  And  yet  it  is  essential  to  the  strict  applicability 
of  the  laws  involved.  We  need  not  repeat  here  the  discussion, 
given  in  a  previous  section,  of  the  variation  in  "color-quality" 
made  very  evident  in  solutions  of  "dichroic"  indicators  as  the 
concentration  of  indicator  or  the  length  of  absorbing  layer  is 
varied.  Suffice  it  to  say,  that  if  a  "colorimeter"  is  used  with  two- 
color  indicators,  the  variation  in  "color-quality"  with  variation 
in  the  ratio  of  tube  lengths  will  be  so  disconcerting  as  to  make  the 
use  of  the  ordinary ' ' colorimeter"  quite  useless  for  pH  measurements . 
Gillespie  (1921)  brought  into  prominence  a  principle  which 
promises  to  be  of  considerable  value.  It  is  illustrated  diagram- 
matically  by  figure  27.  The  vessels  A,  B,  C  and  E  are  of  colorless 
glass.  The  bottoms  should  be  optically  plane-parallel.  A  and 
C  are  fixed  while  B  may  be  moved  up  or  down.  The  position  of 


B 


FIG.  27.  DIAGRAMMATIC  SECTION  OF  GILLESPIE'S  COLOR  COMPARATOR 

B  is  indicated  on  a  scale  the  zero  mark  of  which  corresponds  to 
the  position  of  B  when  B  and  C  are  in  contact  and  the  100  mark 
of  which  corresponds  to  the  position  of  B  when  B  is  in  contact 
with  A.  If  now  there  is  placed  in  B  a  solution  of  the  acid  form 
of  an  indicator  and  in  C  a  solution  of  the  same  concentration  of 
the  indicator  transformed  completely  to  the  alkaline  form,  it  is 
obvious  that  the  position  of  the  vessel  B  will  determine  the  ratio 
of  the  two  forms  of  the  indicator  which  will  be  within  the  view. 

For  comparison  a  solution  to  be  tested  is  placed  in  E  together 
with  that  concentration  of  indicator  that  occurs  in  the  optical 
system  B-C.  For  colored  solutions  tubes  A  and  D  are  used  as 
in  the  Walpole  system,  which  will  presently  be  described.  As 
Gillespie  has  indicated,  this  "colorimeter"  should  be  useful  for 
certain  general  work  where  the  exact  principles  of  color  comparison 
have  often  been  neglected. 


VII 


COMPARATOR 


169 


170         THE  DETERMINATION  OF  HYDROGEN  IONS 

An  instrument  embodying  the  principle  which  Gillespie  used 
was  described  by  Mines  (1910)  under  a  title  concerning  the  action 
of  beryllium,  etc.,  on  the  frog's  heart.  Wu  (1923)  and  Gerretsen 
(1924)  have  employed  the  principle.  The  instrument  made  by 
the  Bausch  and  Lomb  Optical  Company  for  Dr.  A.  B.  Hastings 
is  shown  in  figure  28.  It  has  the  advantage  of  auxiliary  cups  H 
useful  in  the  compensation  of  natural  colors  of  solutions. 

COLOR-WEDGE 

Another  principle  which  has  been  put  to  use  is  embodied  in  the 
"color- wedge"  of  Bjerrum  (1914).  This  is  a  long  rectangular 
box  with  glass  sides  and  a  diagonal  glass  partition  which  divides 
the  interior  into  two  equal  wedges.  One  compartment  contains 
a  solution  of  the  indicator  fully  transformed  into  its  alkaline 
form,  the  other  a  like  concentration  of  the  indicator  transformed 
to  the  acid  form.  A  view  through  these  wedges  should  imitate 
the  view  of  a  like  depth  and  concentration  of  the  indicator  trans- 
formed to  that  degree  which  is  represented  by  the  ratio  of  wedge 
thicknesses  at  the  point  under  observation.  Compare  Barnett 
and  Barnett  (1921)  and  Myers  (1922).  Myers  apparatus  has 
been  developed  commercially  and  is  now  on  the  market.  Wherry 
has  reproduced  Bjerrum's  color-wedge  with  celluloid  walls 
and  made  of  it  a  very  helpful  field  kit. 

McCrae  (1926)  Kolthoff  (1924)  have  also  employed  the  wedge 
principle. 

In  the  use  of  the  wedge  the  relation  between  wedge  thicknesses 
and  pH  values  are  determined  by  the  relation 

,   .      thickness  1 

pH    =    pKa  +  log  —T- 

thickness  2 
provided,  of  course,  the  indicator  has  been  properly  used. 

COMPENSATION   FOR   NATURAL   COLOR   OF  A   SOLUTION 

There  have  been  two  chief  methods  of  dealing  with  the  interfer- 
ing effect  of  the  natural  color  of  solutions.  The  first  method,  used 
by  S0rensen  (1909),  consists  in  coloring  the  standard  comparison 
solutions  until  their  color  matches  that  of  the  solution  to  be 
tested,  and  subsequently  adding  to  each  the  indicator. 


VII 


COMPARATOR 


171 


S0rensen's  coloring  solutions  are  the  following: 

a.  Bismarck  brown  (0.2  gram  in  1  liter  of  water). 

b.  Helianthin  II  (0,1  gram  in  800  cc.  alcohol,  200  cc.  water). 

c.  Tropaeolin  O  (0.2  gram  in  1  liter  of  water). 

d.  Tropaeolin  OO  (0.2  gram  in  1  liter  of  water). 

e.  Curcumein  (0.2  gram  in  600  cc.  alcohol,  400  cc.  water). 
/.  Methyl  violet  (0.02  gram  in  1  liter  of  water). 

g.  Cotton  blue  (0.1  gram  in  1  liter  of  water). 

The  second  method  was  introduced  by  Walpple  (1910).  It 
consists  in  superimposing  a  tube  of  the  colored  solution  over  the 
standard  comparison  solution  to  which  the  indicator  is  added, 
and  comparing  this  combination  with  the  tested  solution  plus 
indicator  superimposed  upon  a  tube  of  clear  water. 

THE   BLOCK   COMPARATOR 

A  somewhat  crude  but  nevertheless  helpful  application  of  Wai- 
pole's  principle  may  be  made  from  a  block  of  wood.  Six  deep 
holes  just  large  enough  to  hold  ordinary  test  tubes  are  bored 
parallel  to  one  another  in  pairs.  Adjacent  pairs  are  placed  as 
close  to  one  another  as  can  be  done  without  breaking  through  the 
intervening  walls.  Perpendicular  to  these  holes  and  running 
through  each  pair  are  bored  smaller  holes  through  which  the  test 
tubes  may  be  viewed.  The  center  pair  of  test  tubes  holds  first 
the  solution  to  be  tested  plus  the  indicator  and  second  a  water 
blank.  At  either  side  are  placed  the  standards  colored  with  the 
indicator  and  each  backed  by  a  sample  of  the  solution  under  test. 


LIGHT  LIGHT 

CONTROL  O®O  CONTROL     CONTROL  OO 
STANDARD  O®O  STANDARD   ACID       OO  W 

£Y£  ALKALINE  OO  UNKNOWN 

EYE 


FIG.  29.  SIMPLE  COMPARATORS 


172  THE    DETERMINATION    OF   HYDROGEN   IONS 

This  is  the  so  called  "comparator"  of  Hurwitz,  Meyer,  and 
Ostenberg  (1915).  Before  use  it  is  well  to  paint  the  whole  block 
and  especially  the  holes  a  non-reflecting  black.  To  produce  a 
"dead"  black  use  a  soft  wood  and  an  alcohol  wood-stain. 

This  comparator  is  shown  in  two  forms  in  figure  29.  Form  A  is 
used  with  the  unknown  X  +  indicator,  backed  by  a  water  blank, 
W,  in  the  center.  On  either  side  is  placed  the  standard  buffer  + 
indicator,  backed  by  a  tube  of  the  unknown  (control)  to  com- 
pensate for  the^  natural  color  or  turbidity  of  the  unknown.  Form 
B  is  used  with  the  Gillespie  method.  The  unknown  +  indicator 
is  backed  by  two  tubes  of  water.  The  acid  solution  of  indicator 
and  the  alkaline  solution  of  indicator  are  backed  by  a  tube  of  the 
untreated  unknown  (control)  to  compensate  for  the  natural  color 
or  turbidity  of  the  unknown. 

There  have  been  described  many  elaborations  of  this  simple 
device.  Several  provide  mechanical  means  of  rapidly  exchanging 
tubes  in  the  field  of  view,  see  for  example  Cooledge  (1920). 

In  the  operation  of  this  comparator  with  "one-color"  indicators 
(nitrophenols)  Michaelis  uses  a  screen  of  blue  glass.  See  page  131. 

COMPENSATION   FOR   TURBIDITY 

Turbidity  often  presents  a  difficult  problem.  S0rensen  (1909) 
has  attempted  to  correct  for  this  effect  by  the  use  of  a  finely 
divided  precipitate  suspended  in  the  comparison  solution.  This 
he  accomplishes  by  forming  a  precipitate  of  BaS04  through  the 
addition  of  chemically  equivalent  quantities  of  BaC^  and  Na2S04. 
Strictly  speaking,  this  gives  an  imperfect  imitation,  but  like  the 
attempt  to  match  color  it  does  very  well  in  many  instances.  The 
Walpole  superposition  method  may  be  used  with  turbid  solutions 
as  well  as  with  colored,  as  experience  with  the  device  of  Hurwitz, 
Meyer  and  Ostenberg  has  shown.  In  passing,  attention  should 
be  called  to  the  fact  that  the  view  of  a  turbid  solution  should  be 
made  through  a  relatively  thin  layer.  When  the  comparison  is 
made  in  test  tubes,  for  instance,  the  view  should  be  from  the  side. 

There  are  some  solutions,  however,  which  are  so  dark  or  turbid 
that  they  cannot  be  handled  with  much  precision  by  any  of  these 
methods.  On  the  other  hand  a  combination  of  these  methods 
with  moderate  and  judicious  dilution  [as  was  indicated  in  Chap- 
ter II  this  may  not  seriously  alter  the  pH  of  a  solution],  permits 


VII  FLUORESCENCE  173 

very  good  estimates  with  solutions  which  at  first  may  appear 
"impossible."  Some  of  the  deepest  colored  solutions  permit  reason- 
ably good  determinations  and  when  sufficiently  transparent  per- 
mit the  application  of  spectrometric  devices.  Turbidity  on  the 
other  hand  is  sometimes  unmanageable.  Even  in  the  case  of 
milk  where  comparison  with  a  standard  is  out  of  the  question  a 
two  colored  indicator  presents  a  basis  for  judgment.  See  also 
page  136. 

REFLECTIONS 

Buckmaster  (1923)  has  suggested  using  films  of  tested  solution 
and  of  buffer  standards.  The  comparison  is  to  be  made  by 
reflected  light.  He  does  not  describe  the  principles.  Since  they 
are  rather  complex  and  since  the  procedure  seems  not  to  be  of 
immediate  importance,  the  citation  will  suffice. 

FLUORESCENT  INDICATORS 

A  number  of  substances,  among  them  fluorescein,  not  only 
suffer  changes  in  the  grosser  aspects  of  their  color  in  solution  when 
the  pH  value  of  the  solution  passes  through  a  certain  range,  but 
also  fluoresce  within  and  above  one  zone  of  pH  and  not  below 
the  zone. 

True  fluorescence  is  described  as  follows.  Radiant  energy  of 
one  or  another  wave-length  is  absorbed  by  the  substance  and  the 
energy  is  given  forth  as  radiant  energy  of  another  wave-length 
usually  greater  than  that  of  the  exciting  radiation.  Fluorescence 
is  therefore  best  observed  indirectly  as  if  one  were  considering  the 
substance  the  source.  An  extensive  discussion  is  given  by  Pring- 
sheim  (1923)  and  Wood  (1921). 

Since,  in  some  cases,  there  appears  to  be  a  direct  relation  be- 
tween the  degree  of  fluorescence  and  what  might  be  expected  to 
be  the  degree  of  dissociation  as  controlled  by  buffer  solutions, 
measurement  of  the  degree  of  fluorescence  provides  a  method  of 
measuring  hydrion  concentration.  In  figure  30  is  a  graph  taken 
from  the  work  of  Desha,  Sherrill  and  Harrison  (1926)  which  shows 
the  relation  between  the  pH  values  of  the  solution  and  the  degree  of 
fluorescence  of  2  naphthol,  3,  6-disulfonic  acid.  The  fluorescence 
is  very  easily  influenced  by  chlorides.  Included  in  the  paper 
mentioned  above  are  data  for  other  substances  such  as  quinine. 

See  also  Mellet  and  Bischoff  (1926)  and  Robl  (1926). 


174 


THE    DETERMINATION    OF   HYDROGEN   IONS 


20 


80      100 


40       60 

PERCENT 
FIG.  30.  RELATION  OF  pH  TO  PER  CENT  MAXIMUM  FLUORESCENCE  OF 

2-NAPHTHOL,3,6-DISULFONIC   AdD 

Center  of  curve  at  pH  9.45.     (After  Desha,  Sherrill  and  Harrison  (1926)) 
ARTIFICIAL   COLOR   STANDARDS 

There  is  an  inherent  simplicity  in  the  use  of  standard  buffer 
solutions  and  indicators  themselves  which  would  seem  to  pre- 
clude attempts  to  use  artificial  standards.  And  yet  there  seems 
to  be  an  insistent  demand  for  artificial  standards.  Even  color 
charts  are  in  demand!  See  page  65.  These  should  be  used 
with  due  precautions. 

Grieg-Smith  (1924)  tells  us  that  he  makes  his  own  water  color 
standards  for  use  with  the  spot-plate  method  and  that  he  has  seen 
similar  standards  at  the  Lister  Institute.  They  can  be  prepared 
by  a  good  artist  better  than  by  the  printer's  art.  The  original 
color  chart  which  Professor  Max  Brodel  did  in  water  color  for 
reproduction  in  the  first  edition  of  this  book  was  a  beautiful 
piece  of  work :  but  it  could  not  be  reproduced  accurately  and  was 
used  only  as  a  guide.  The  artist's  eye  is  not  the  eye  of  the 
spectrophotometer  or  of  the  camera  or  of  the  printer. 

In  the  same  category  of  artificial  standards  fall  the  organic 
or  inorganic  solutions  such  as  those  proposed  or  discussed  by 
Haskins  (1919),  Kolthoff  (1922),  Risen  (1924),  Janke  and  Kro- 
pacsy  (1926),  Brue*re  (1926),  Taub  (1927),  J0rgensen  (1927).  See 
also  comments  on  inorganic  standards  by  Breslau  (1925). 

Sonden  (1921)  has  used  colored  glasses  (see  also  Anon.  (1927), 


VII 


MIXED    INDICATORS 


175 


/.  Sri.  Inst.  4,  327).  Incidentally  it  is  interesting  to  note  how  the 
old  Lovibond  tintometer  with  its  colored  glasses  has  become  quite 
out  of  date. 


MIXED   INDICATORS 


Mixtures  of  indicators  are  employed  for  two  very  distinct  pur- 
poses, only  one  of  which  justifies  their  description  in  this  chapter. 


0.0 


440    480     520    560    600   640     680 

WAVE  LENGTH 

FIG.  31.  ABSORPTION  CURVES  FOR  THE  MIXED  INDICATOR:  0.015  GRAM 

METHYL  RED  +  0.04  GRAM  BROM  THYMOL  BLUE 

(After  Erode  (1924)) 

Sometimes  a  rational  selection  of  indicators  having  different  ab- 
sorption bands  or  the  admixture  of  an  indicator  with  a  dye  which 
is  not  itself  an  indicator,  results  in  color-changes  more  easily 
distinguished.  A  case  in  point  is  described  by  Hickman  and 
Linstead  (1922)  who  use  xylene  cyanole  F  F  as  an  "internal  light 
filter"  in  conjunction  with  methyl  orange  (1  part  methyl  orange 
to  1.4  part  cyanole  in  500  parts  50  per  cent  alcohol).  The  result 


176  THE    DETERMINATION    OF   HYDROGEN   IONS 

t 

at  pH  3.8  is  a  grey  intermediate  color  which,  these  authors  claim, 
increases  the  ease  of  detecting  end-points  in  titrations.  The  ab- 
sorption bands  showing  the  rationale  of  the  combination  are  given 
in  the  original  paper. 

For  a  very  different  purpose  is  admixture  of  indicators  to  ex- 
tend with  one  test  solution  the  range  of  pH  values  determinable. 
While  recognizing  some  advantage  in  this,  the  author  has  never 
felt  it  to  be  a  distinct  advantage  to  ordinary  pH  measurements. 
In  certain  titrations  the  ability  to  detect  two  or  more  end-points 
widely  apart  on  the  pH  scale  is  a  distinct  advantage  of  indicator 
mixtures. 

A  spectrophotometric  analysis  of  one  mixture  is  shown  in 
figure  31.  This  analysis  by  Erode  (1924)  illustrates  a  mode  of 
attack  which  should  be  profitable  in  cases  where  specific  results 
are  to  be  achieved. 

Several  references  to  mixed  indicators  are  given  in  Chapter  IV. 

PHOTOELECTRIC    CELLS 

Now  that  the  photoelectric  cell  is  coming  into  more  general 
use  it  will  doubtless  be  applied  in  a  variety  of  ways  in  our  subject. 
Reimann  (1926)  describes  its  use  in  titrations  and  Miiller  and 
Partridge  (1927)  apply  it  to  the  automatic  control  of  titrations. 
The  selenium  cell  has  been  applied  by  Hjort,  Lowey  and  Black- 
wood  (1924)  in  end-point  work  with  indicators  absorbing  in  the 
orange  and  red.  In  following  absorption  in  the  ultra-violet  certain 
types  of  photoelectric  cell  have  been  very  useful.  See  for  instance 
Halban  and  Geigel  (1920),  Halban  and  Siedentorff  (1922)  and 
Kaplan  (1927).  There  may  be  rare  instances  when  minute  de- 
flections of  the  galvanometer  mirror  in  potentiometric  measure- 
ments have  to  be  detected.  The  photoelectric  cell  has  been  used 
to  amplify  such  minute  deflections. 

For  a  discussion  of  photoelectric  cells  as  applied  to  colorimetry 
see  Campbell  and  Gardiner  (1925)  and  also  the  book  on  spectro- 
photometry  by  Walsh. 


CHAPTER  VIII 

SOURCES  OF  ERROR  IN  COLORIMETRIC  DETERMINATIONS 

A  series  of  judgments,  revised  without  ceasing,  goes  to  make  up  the 
incontestable  progress  of  science.  —  DUCLAUX. 

INTRODUCTION 

There  are  errors  of  technique,  such  as  incorrect  apportionment 
of  the  indicator  concentration  in  tested  and  standard  solution  and 
the  use  of  unequal  depths  of  solutions  through  which  the  colors 
are  viewed,  that  may  be  passed  over  with  only  a  word  of  reminder. 
Likewise  we  may  refer  to  certain  of  the  optical  effects  mentioned 
in  Chapter  VII  and  then  pass  on  to  the  more  serious  difficulties 
in  the  application  of  the  indicator  method. 

At  the  very  beginning  it  will  be  well  to  emphasize  the  distinc- 
tion which  should  be  maintained  between  discrepancies  attrib- 
utable to  the  neglect  of  factors  which  may  be  evaluated  by 
some  general,  if  arbitrary,  formulation  and  discrepancies  attrib- 
utable to  the  sum  of  what  is  ordinarily  called  "error"  and  spe- 
cific phenomena  beyond  the  range  of  any  convenient  formulation. 

Up  to  this  point  in  the  development  of  the  subject  there  has 
been  used  as  the  fundamental  type-equation  the  following: 


[HA] 

For  convenience  of  discussion  consider  separately  the  constant 

[A~] 

Ka,  the  ratio  rTJA1  and  [H+]. 
|MAJ 

In  the  derivation  of  the  equation  it  was  assumed  that  it  is 
primarily  the  density  of  the  number  of  particles  in  the  solution- 
space  that  determines  the  equilibrium  state.  As  the  subject 
develops  it  will  be  found  necessary  to  introduce  appreciable 
corrections  to  this  formula  because  it  was  deduced  on  assumptions 
far  too  ideal  to  meet  the  varying  conditions  of  actual  solutions. 
If  we  then  insist  on  using  the  above  formula,  variation  of  condi- 

177 


178  THE    DETERMINATION    OF   HYDROGEN   IONS 

tions  will  make  it  appear  as  if  the  so-called  constant  Ka  were 
subject  to  appreciable  variations.  If  under  one  set  of  conditions 
there  is  used  a  value  of  Ka  standardized  for  another  set  of  condi- 
tions an  error  will  be  introduced. 

It  is  reasonable  to  assume  as  a  close  approximation  that  the 
ratio  of  the  concentrations  of  two  forms  of  the  indicator  will  be 
determined  by  the  "color"  as  described  in  Chapter  III.  However, 
see  Halban  and  Ebert  (1924).  Their  objection  will  now  be 
neglected.  Therefore,  and  in  accordance  with  the  theory  of 

Chapter  V,  we  use  the  ratio  ;g-rr  as  it  stands  uncorrected   in 

the  equation.  On  the  other  hand,  we  shall  see,  after  having 
studied  the  theory  of  the  hydrogen  electrode,  that  there  is  no 
exact  relation  between  the  potential  of  a  hydrogen  cell  and  the 
hydrogen  ion  concentrations.  However,  there  is  an  approximate 
relation. 

Later  there  will  be  used  the  convenient  equation 

(H+)  (A-)  _  [H+]  [A-]  jrHA_ 

(HA)  [HA]         K"7H.7A- 

Where  ()  indicates  "activity"  and  y  represents  the  "activity  coeffi- 
cient." Now  it  is  doubtless  a  very  close  approach  to  fTJA1  that 

|rLA| 


is  measured  colorimetrically;  it  is  (H+),  or  [H+frn+i  and  not 
[H+]  that  is  measured  electrometrically  and  ascribed  to  the 

buffer  system;  and  it  is  Ka  -~  that  is  determined  under  one 

specific  set  of  conditions  and  applied  rather  indiscriminately  to 
all  conditions. 

The  situation  requires  careful  "unscrambling"  which  cannot 
well  be  done  until  the  developments  in  subsequent  chapters.  In 
the  meanwhile  the  interpretation  of  indicator  conduct  will  be 
considered  to  be  standardized  by  the  use  of  standard  comparison 
solutions  having  the  pH  values  assigned  in  Chapter  IX. 

Because  investigators  have  been  content  to  proceed  with  this 
system  of  comparison  and  have  not  imposed  upon  themselves  in 
all  cases  the  accuracy  demanded  of  the  systematic  type  of  study 
later  to  be  indicated,  most  of  the  more  directly  applicable  tables 


VIII  SALT   EFFECTS  179 

of  corrections  are  rather  inaccurate.  They  will  be  cited  to  indi- 
cate orders  of  magnitude  found  by  the  methods  used.  The  reader 
will  do  well  to  watch  current  literature  for  better  systematized 
data  which  will  probably  be  published  extensively  in  the  near 
future. 

In  the  ordinary  method  of  comparison,  discrepancies  have  often 
been  traced  so  clearly  to  two  definite  sources  that  they  have  been 
given  categorical  distinction.  They  are  the  so-called  "protein" 
and  "salt"  effects. 

From  what  has  already  been  said  in  previous  pages,  it  will  be 
seen  that,  if  there  are  present  in  a  tested  solution  bodies  which 
remove  the  indicator  or  its  ions  from  the  field  of  action  either  by 
adsorption,  or  otherwise,  the  equilibria  which  have  formed  the 
basis  of  our  treatment  will  be  disturbed.  An  indicator  in  such  a 
solution  may  show  a  color  intensity,  or  even  a  quality  of  color, 
which  is  different  from  that  of  the  same  concentration  of  the  indi- 
cator in  a  solution  of  the  same  hydrogen  ion  concentration  where 
no  such  disturbance  occurs.  We  could  easily  be  led  to  attribute 
very  different  hydrogen  ion  concentrations  to  the  two  solutions. 
This  situation  is  not  uncommon  when  we  are  dealing  with  protein 
solutions,  for  in  some  instances  there  is  distinctly  evident  the 
removal  of  the  indicator  from  the  field.  In  other  cases  the  dis- 
crepancy between  electrometric  and  colorimetric  measurements 
is  not  so  clear,  nor  can  it  always  be  attributed  solely  to  the  indi- 
cator measurement. 


If  two  solutions  of  inorganic  material,  each  having  the  same 
pH- value,  are  tested  with  an  indicator,  we  should  expect  the  same 
color  to  appear.  If,  however,  these  two  solutions  have  different 
concentrations  of  salt,  it  may  happen  that  the  indicator  colors  are 
not  the  same.  As  S0rensen  (1909)  and  S0rensen  and  Palitzsch 
(1913)  demonstrated,  this  effect  of  the  salt  content  of  a  solution 
cannot  be  logically  tested  by  adding  the  salt  to  one  of  two  solu- 
tions which  have  previously  been  brought  to  the  same  pH-value. 
The  added  salt,  no  matter  if  it  be  a  perfectly  neutral  salt,  will 
change  the  pH-value  of  the  solution.  Comparisons  had  best  be 
made  between  solutions  of  the  same  pH-value. 

So  long  as  hydrogen  electrode  measurements  are  made  the 


180 


THE  DETERMINATION  OF  HYDROGEN  IONS 


standard,  it  is  convenient  to  throw  the  burden  of  the  "salt  effect" 
upon  the  indicator;  but  neutral  salts  are  known  to  displace  elec- 
trode potential  differences  from  the  values  estimated  from  the  ex- 
pected hydrogen  ion  concentration. 

A  standardization  procedure  may  be  illustrated  as  follows.  The 
pH-value  of  the  unknown  is  measured  potentiometrically.  Let  it 
be  6.73.  A  portion  of  the  same  solution  is  now  treated  with  the 
indicator  and  a  color  match  is  found  with  a  standard  buffer 
having  an  electrometrically  determined  pH-value  of  6.70.  The 
"error"  is  —0.03  pH  unit  and  the  correction  necessary  to  bring 
the  apparent  colorimetric  reading  to  the  electrometric  is  +0.03. 

Bjerrum  (1914)  gives  an  example  of  a  case  where  the  influence 
of  the  neutral  salt  is  evidently  upon  the  buffer  equilibrium  rather 
than  on  the  indicator.  An  ammonium-ammonium  salt  buffer 
mixture  and  a  borate  buffer  mixture  are  both  made  up  to  give 
the  same  color  with  phenolphthalein.  On  the  addition  of  sodium 
chloride  the  color  of  phenolphthalein  becomes  stronger  in  the 
ammonium  mixture  and  weaker  in  the  borate  mixture. 

Let  it  be  kept  in  mind  that  while  neutral  salts  displace  the 
electrode  equilibrium  and  lead  to  different  pH  values  of  the 
standard,  it  is  the  measurement  of  the  particular  standard  used 
that  is  usually  taken  as  a  standard  of  reference  in  the  colorimetric 
comparison.  The  following  illustrates  a  procedure  with  solu- 
tions of  the  same  general  nature.  S0rensen  and  Palitzsch  (1910) 
were  studying  the  salt  effects  of  indicators  in  sea  water.  They 
acidified  the  sea  water  and  passed  hydrogen  through  to  displace 
carbon  dioxid,  and  then  neutralized  it  to  the  ranges  of  various 
indicators  and  buffer  mixtures  and  compared  colorimetric  with 
electrometric  measurements.  In  this  way  they  found  the  follow- 
ing "errors." 


INDICATOR 

BUFFER 

PARTS  PER   1000   OF  SALTS   AND 
CORRESPONDING  ERRORS 

35 

20 

5 

1 

p-Nitrophenol  

Phosphate 
Phosphate 
Borate 
Phosphate 
Borate 

+0.12 

-0.10 
+0.22 
+0.16 
+0.21 

+0.08 
-0.05 
-fO.17 
+0.11 
+0.16 

0 
+0.03 
-0.04 
+0.05 

0 
-0,07 
-0.14 
-0,03 

Neutral  red 

a-Naphthol  phthalein.  .  .< 
Phenolphthalein  

TABLE   27 

Salt  effect  of  indicators,  after  Kolthoff 


INDICATOR 

SALT 

SALT 
CONCEN- 
TRATION 

CORREC- 
TION 

REMARKS 

Tropaeolin  OO 
(Orange  IV)  

KC1 
KC1 
KC1 
KC1 

0.10  N 
0.25  N 
0.50  N 
1.00  N 

-0.05 
-0.01 
+0.06 
+0.23 

Indicator    suitable.     NaCl 
has  about  same  influence 

Methyl  orange  
Butter  yellow  

KC1 
KC1 
KC1 
KC1 

KC1 

0.10  N 
0.25  N 
0.50  N 
1.00  N 

0.10  N 

-0.08 
-0.08 
+0.02 
+0.23 

—0.08 

Indicator     suitable.     NaCl 
has  about  same  influence 

Same     errors      as     methyl 

orange  but  indicator  floc- 
culates with  salt 

Thymol  blue  (acid 

KC1 
KC1 
KC1 

0.10  N 
0,20  N 
0.50  N 

-0.06 
-0.06 
—0.04 

NaCl  has  same  influence 

KC1 

1.00  N 

+0.05 

Brom  phenol  blue.. 

KC1 
KC1 
KC1 
KC1 

0.10  N 
0.25  N 
0.50  N 
1.00  N 

-0.05 
-0.15 
-0.35 
-0.35 

Corrections  large  at  weaker 
concentration  of  salt 

Brom  cresol  purple  .  . 
Phenol  red  

NaCl 
NaCl 

0.50  N 
0.50  N 

-0.25 
—0.15 

At  small  concentrations  of 

Thymol  blue  

NaCl 

0.50  N 

—0,17 

salt  correction  of  opposite 
sign 

Methyl  red  

NaCl 

0.50  N 

+0.10 

p-Nitrophenol  
Azo  yellow  3G  

NaCl 
NaCl 

0.50  N 
0.50  N 

-0.05 
0.00 

Phenolphthalein  

NaCl 

0.50  N 

-0.17 

KC1 
KC1 

0.10  N 
0.25  N 

-0.06 
-0.12 

NaCl  has  about  same  influ- 
ence 

KC1 
KC1 

0.50  N 
1.00  N 

-0.10 
-0.29 

181 


182 


THE   DETERMINATION   OF   HYDROGEN   IONS 


If,  for  example,  sea  water  of  about  3.5  per  cent  salt  is  matched 
against  a  standard  borate  solution  with  phenolphthalein  and 
appears  to  be  pH  8.43  the  real  value  is  pH  8.22.  Compare  table 
44,  page  213  and  McClendon  (1917). 

TABLE  28 

The  salt  error  of  cresol  red  at  salinities  from  5  to  85  parts  of  sea  salts  per  1000 
(After  Ramage  and  Miller) 


Salinity  

5 

6 

7 

8 

9 

10 

11 

12 

Correction 

-0.11 

-0.13 

-0.14 

-0  15 

-0  16 

-0  17 

-0  18 

—0  19 

Salinity 

13 

14 

15 

16 

17 

18 

19 

20 

Correction  

-0.20 

-0.21 

-0.21 

-0.22 

-0.22 

-0.23 

-0  23 

-0  24 

Salinity  

21 

22 

23 

24 

25 

26 

27 

28 

Correction 

-0  24 

-0  24 

-0  25 

-0  25 

-0  25 

-0  25 

-0  26 

-0  26 

Salinity 

29 

30 

31 

32 

33 

34 

35 

Correction  

-0.26 

-0.26 

-0.26 

-0.27 

-0.27 

-0.27 

-0.27 

TABLE  29 

Salt  effects 
(After  Parsons  and  Douglas  1926) 


1  molar 

2  molar 

3  molar 

Thymol  blue  (alkaline  range)  

-0.22 

-0.29 

-0.34 

Cresol  red 

-0  28 

-0  32 

—0  37 

Phenol  red                                              

-0.21 

-0  26 

-0  29 

Brom  thymol  blue  

-0.19 

-0.27 

-0.29 

Brom  cresol  purple                                 .    .  . 

-0  26 

-0.33 

-0.31 

Brom  cresol  green              

-0.26 

-0.31 

-0.29 

Brom  phenol  blue 

-0  28 

-0  37 

-0  43 

Thymol  blue  (acid  range)             

-0.10 

-0.13 

-0.12 

Methvl  red.  . 

-0.04 

-0.01 

+0.12 

CORRKCTION 


Such  calibration  is  one  of  the  very  best  ways  to  deal  with  the 
salt  errors  since  it  tends  to  bring  measurements  to  a  common 
experimental  system  of  reference. 

The  following  table  taken  from  Prideaux  (1917),  illustrates  the 
order  of  magnitude  of  the  "salt  error"  in  some  instances. 


VIII 


SALT   EFFECTS 


183 


INDICATOR 

BUFFER  USED 

CHANGE  OF  pH 

IN  PRESENCE  OF 

0.5  N  NaCl 

p-Benzene  sulphonic  acid  azo  naphthylamine  — 
p-Nitrophenol                                          .   . 

Phosphate 
Phosphate 

-0.10 

-f  0  15 

Alizarin   sulphonic  acid  

Phosphate 

+0  26 

Neutral  red           .                            .... 

Phosphate 

—0  09 

Rosolic  acid  

Phosphate 

+0.06 

p-Benzene  sulphonic  acid  azo  a-naphthol  
Phenolphthalein  

Phosphate 
Phosphate 

+0.12 
+0.12 

Kolthoff  (1922)  gives  table  27  page  181  showing  the  correc- 
tions to  be  applied  for  the  "salt  error"  of  various  indicators.  It 
should  be  noted  that  Kolthoff  includes  in  this  table  data  obtained 
when  the  hydrogen  electrode  potentials  were  taken  as  standard 
and  also  data  in  which  the  pH  values  were  calculated.  The  two 
sets  are  not  strictly  comparable  and  therefore  must  be  used 
with  caution  in  theoretical  work.  We  have  eliminated  from 
Kolthoff's  table  Congo  red,  Azolitmin,  and  Tropaeolin  0  (Chry- 
soi'n)  which  Kolthoff  describes  as  having  salt  errors  so  large  that 
these  indicators  are  useless. 

Michaelis  and  his  coworkers  have  determined  the  salt  errors 
for  a  number  of  the  nitrophenols,  but,  since  the  corrections  are 
often  intimately  related  to  the  constants  used  in  Michaelis' 
method  of  operating,  the  reader  is  referred  to  the  original  litera- 
ture for  the  details.  See  Chapter  VI. 

TABLE  30 

Salt  effect.    New  sulfonphthaleins 

(After  Cohen  (1927)) 

[The  values  given  below  are  corrections  to  be  added  to  the  colorimetric 
pH  determinations  to  bring  the  values  to  the  electrornetric  pH  of  the  corre- 
sponding Clark  and  Lubs'  buffers.] 


MOLAR 
CONCEN- 
TRATION 
SALT 

m-CRESOL  PURPLE 

.     BROM 

CRESOL 
GREEN 

BROM 
PHENOL 
RED 

CHLOR 
PHENOL 
RED 

BROM 
CHLOR 
PHENOL 
BLUE 

Acid  range 

Alkaline 
range 

1.0 

-0.14 

-0.29 

-0.32 

-0.26 

-0.26 

-0.33 

0.5 

-0.09 

-0.22 

-0.26 

-0.22 

-0.20 

-0.28 

0.2 

-0.02 

-0.16 

-0.16 

-0.12 

-0.10 

-0.16 

0.005 

+0.11 

+0.09 

+0.09 

+0.25 

+0.23 

+0.14 

184 


THE    DETERMINATION    OF   HYDROGEN    IONS 


Ramage  and  Miller  (1925)  after  a  comparison  of  their  own  and 
Wells'  (1920)  data  for  cresol  red  give  table  28  for  use  in  the  study 
of  sea  water. 

Parsons  and  Douglas  (1926)  give  a  table  (table  29)  for  "average" 
corrections  which  they  suggest  using  in  order  to  bring  pH  measure- 
ments of  solutions  of  the  indicated  concentrations  of  NaCl  to 
conformity  with  the  values  of  Clark  and  Lubs'  standard  buffers. 

Cohen  (1927)  publishes  table  30. 


2  3 

Electrometric 

FIG.  32.  VARIATION  OF  THE  "PROTEIN  ERROR,"  IN  THE  COLORIMETRIC 
DETERMINATION  OF  pH  AS  THE  pH  VALUE  OF  GELATINE 

SOLUTION  CHANGES 

O  =  bromphenol  blue  and  1.0  per  cent  gelatine.  •  =  Thymol  blue 
and  1.0  per  cent  gelatine.  +  =  bromphenol  blue  and  0.4  per  cent  gelatine. 
X  ss  Thymol  blue  and  0.4  per  cent  gelatine.  (After  St.  Johnston  and 
Peard  (1926).) 


EFFECTS 

The  magnitude  of  "protein"  effects  may  be  roughly  judged  from 
the  following  tables.  The  data,  which  could  only  be  summarized 
in  this  way  by  neglecting  some  variation  in  the  salt  content  of 
the  solutions,  include  to  some  degree  a  salt  effect. 

Since  it  is  not  often  that  protein  errors  are  presented  in  a 
systematic  way,  figure  32  by  St.  Johnston  and  Peard  (1926)  is 


TABLE  31 

"  Protein"  effects  of  indicators 
(Data  from  Sprensen  (1909)) 

Corrections  to  be  added  to  apparent  colorimetric  reading  to  bring  read- 
ing to  the  electrometric  standard. 


INDICATOR 

CORRECTIONS 

In  2%  peptone 
0.3  'N  salt 

In  2%  egg- 
white  0.07  — 
0.3  N  salt 

Methyl  violet  

-0.02 
-0.04 
-0.06 
-0.27 
-0.30 
+0  01 
-0.22 

-0.41 
-0.08 
-0.18 
-0.02 
-0.03 
-0.06 
+0.13 
+0.08 
-0.12 
-0.01 
+0.01 

-0.19 
-0.19 
>-0.90 
>-1.40 
>-1.40 
>-0.80 
>-0.80 

-0.53 

+0.15 
-0.04 
+0.68 
+0.44 
+0.10 
+0.18 
+0.40 
+0.29 
-0.30 

Mauve                                                ...         .... 

Benzene-azo-diphenyl  amine  

Tropaeolin  OO  

Metanil  yellow 

Benzene-azo-benzylaniline  

p-Benzene  sulfonic  acid-azo-benzylaniline.    .  .  . 

p-Benzene-sulfonic       acid-azo-w-chlorodiethyl 
aniline    

Topfer's  Indicator                                  .      ... 

IVIethyl  orange 

Benzene-azo-a-naphthylamine     

p-Benzene  sulfonic  acid-azo-a-naphthylamine.  .  . 
p-Nitrophenol      

Neutral  red 

Rosolic  acid  

Tropaeolin  OOO  no.  1      .              

Phenolphthalein 

Thymolphthalein  

Alizarin  yellow  R 

TroDaeolin  O... 

TABLE  32 

"  Protein"  effects  of  indicators 
(Data  from  Clark  and  Lubs  (1917)) 

Corrections  are  to  be  added  to  colorimetric  readings  to  bring  readings 
to  electrometric  standard. 

CORRECTIONS 


INDICATOR 

Peptone- 
infusion 

10% 
gelatine 
sol. 

2  %  egg- 
white 

Urine 

Brom  phenol  blue     

0.05 

Methyl  red 

-0  10 

0.24 

0.05 

Brom  cresol  purple  

0.01 

0.04 

0.01 

Brom  thymol  blue      

0.10 

0.04 

0.02 

Phenol  red 

0  04 

0  20 

0.00 

Cresol  red 

0  03 

0  20 

Thymol  blue  

6.04 

0.20 

Cresolphthalein  .  . 

-0.03 

0.20 

185 


186 


THE  DETERMINATION  OF  HYDROGEN  IONS 


TABLE  33 
"Protein"  effects  of  indicators 

(Data  of  Cohen  (1927)) 

[The  values  listed  are  the  corrections  to  be  added  to  colorimetric  pH 
readings  to  bring  them  to  the  electrometric.] 


INDICATOR 

IN  5  PER  CENT  WITTE 
PEPTONE 

CLARK  AND 
LUBS* 

Series  1 

Series  2 

m-Cresol  purple  (acid) 

-0.20 
-0.19 

-0.28 
-0.28 
-0.10 
+0.09 
+0.11 
+0.11 
+0.34 
+0.24 
+0.02 
+0.03 
+0.09 

-0.20 
-0.20 
-0.43 
-0.43 
-0.13 
-0.07 
-0.10 
-0.10 
+0.07 
-0.01 
-0.03 
-0.02 
-0.03 

+0.05 

+0.01 
+0.10 
+0.04 
+0.03 

+0.04 

Thymol  blue  (acid)  

Brom  phenol  blue       .    ... 

Brom-chlor  phenol  blue  

Brom  cresol  green  

Chlor  phenol  red 

Brom  phenol  red  

Brom  cresol  purple  

Brom  thymol  blue  .    . 

Phenol  red 

Cresol  red  

m-Cresol  purple  (alk.)  

Thymol  blue  (alk.) 

*  In  a  1  per  cent  peptone-beef  infusion  broth. 

TABLE  34 

Protein  errors  with  neutral  red  and  with  phenol  red 
(After  Lepper  and  Martin  (1927)) 


NEUTRAL 

NEUTRAL 

PHENOL  RED 

PHENOL 

RED 

RED 

RED 

PSEUDO- 
GLOBU- 
LIN 

DEVIA- 
TION FROM 
ELECTRO- 

ALBUMIN 

DEVIA- 
TION FROM 
ELECTRO- 

PSEUDO- 
GLOBULIN 

DEVIATION 
FROM 
ELECTRO- 

ALBU- 
MIN 

DEVIA- 
TION FROM 
ELECTRO- 

METRIC 

METRIC 

METRIC 

„  TT 

METRIC 

PH 

pH 

pH 

pH 

per  cent 

per  cent 

per  cent 

per  cent 

0 

0.00 

0 

0.00 

0        (7.38)     0.00 

0.00 

0.00 

0.17 

0.00 

0.23 

0.00 

2 

0.00 

0.03 

0.00 

0.33 

0.00 

0.047  (sic) 

0.00 

4 

+0.02 

0.06 

-0.02 

0.67 

-0.05 

0.095  (sic) 

+0.10 

8 

+0.03 

0.13 

-0.03 

1.35 

-0.15 

0.19 

+0.20 

12 

+0.04 

2.70 

-0.25 

0.38 

+0.30 

0        (7.93)     0.00 

4.09 

-0.45 

0.75 

+0.40 

1.75 

0.00 

5.40 

-0.60 

1.5 

+0.51 

3.5 

+0.02 

8.17 

-0.73 

3.0 

+0.58 

7.0 

+0.09 

10.80 

-0.83 

11.0 

+0.12 

16.35 

-0.85 

VIII  SYSTEMATIC   TKEATMENT  187 

rather  interesting.  The  apparent  error  is  lowest  near  the  iso- 
electric  point  of  gelatin  (4.7).  Table  34  shows  some  cases  in 
which  the  effect  of  the  concentration  of  the  protein  is  evident. 

SYSTEMATIC  TREATMENT 

We  owe  to  Br0nsted  (1921)  the  separation  of  the  several  differ- 
ent sorts  of  quantities  appearing  in  the  equation 

IH+]  [A-]  7HA 

[HA] 


briefly  mentioned  earlier  in  this  chapter.  He  applied  certain  of 
his  equations  for  the  estimation  of  the  correction  terms  and  ob- 
tained in  some  cases  a  rather  striking  agreement  between  ob- 
served salt-effects  and  calculated  salt-effects.  A  more  recent 
development  will  be  mentioned  in  Chapter  XXV  (see  page  511). 
There  it  will  appear  that  salt  effects  are  probably  subject  to 
much  more  systematic  treatment  than  they  have  hitherto  re- 
ceived. It  will  also  appear  that  specific  salt-effects  remain.  How- 
ever, the  first  order  corrections  can  be  estimated  by  use  of  the 
Debye-Hiickel  equation  described  in  Chapter  XXV.  Also  the 
principle  concerned  can  be  put  to  good  use.  For  instance, 
Hastings  and  Sendroy  (1924)  employ  0.154  M  NaCl  solution 
for  the  dilution  of  plasmas  to  be  compared  colorimetrically  with 
phosphate  standards.  The  ionic  strength,1  /*,  of  this  sodium 
chloride  solution  is 

1/2  (0.154  X  I2  +  0.154  X  I2)  =  0.154/1 

At  6.8  the  ionic  strength  of  the  M/15  phosphate  buffer  is  ap- 
proximately 

1/2  (.0333  X  22  +  .0333_X  I2  +  0.1  X  I2)  =  0.1330 
HP04  H2P04  Na+ 

At  7.8  the  ionic  strength  is  about  0.190/1.  Hence  there  is  not  a 
great  difference  between  the  ionic  strengths  of  the  diluted  plasma 
and  the  buffer  standard  and  consequently  little  difference  in 
"salt  error." 

1  See  pages  490  and  559. 


188  THE    DETERMINATION    OF   HYDROGEN    IONS 

It  were  much  better  to  begin  the  systematization  of  salt- 
effects  on  such  a  basis  than  to  continue  longer  with  the  pure 
empiricism  which  has  characterized  the  data  of  the  past.  Un- 
fortunately there  are  available  as  yet  few  systematic  data  and 
consequently  the  older  tables  are  given  in  the  foregoing  pages. 
But  see  page  511  and  figure  90. 

It  is  not  improbable  that,  even  if  the  protein  error  cannot  be 
precisely  formulated  with  the  aid  of  the  Debye-Hiickel  equation, 
its  description  can  be  rationalized  by  the  procedure  suggested  for 
the  salt  effects. 

SPECIFIC   ERRORS 

The  "protein"  effect  and  the  salt  effect  have  been  given  prom- 
inence in  the  literature  partly  because  both  have  to  be  taken  into 
consideration  in  dealing  with  biological  solutions,  and  partly 
because  there  is  to  be  perceived  underlying  the  salt  error  a  most 
interesting  phenomenon  of  rather  general  theoretical  importance. 
However,  this  emphasis  should  not  obscure  the  fact  that  there  are 
specific  conditions  for  each  indicator  which  render  that  indicator 
useless  for  the  determination  of  pH.  For  instance  alizarin,  in 
passing  from  the  phosphate  to  the  borate  buffer  mixtures,  exhibits 
a  sudden  transition  which  has  all  the  appearances  of  a  specific 
effect  of  the  borate  upon  the  indicator.  And  alizarin  is  not 
alone  in  this  peculiarity.  This  same  alizarin  in  the  presence  of 
aluminium  may  form  a  lake  and  with  proper  pH  control  may  be 
made  a  useful  reagent  for  aluminium  in  place  of  a  very  poor  acid- 
base  indicator,  cf.  Williamson  (1924).  Zoller  (1921)  has  called 
attention  to  the  incompatibility  between  certain  dyes  and  the 
phthalate  buffers.  Kolthoff  (1926)  notes  an  especially  large 
error  when  methyl  orange  is  used  with  phthalate  buffer.  Arndt 
and  Nachtwey  (1926)  note  errors  with  pyridine  solutions  and 
Michaelis  (1926)  states  that  sulfon  phthaleins  show  errors  with 
alkaloids  that  are  not  observed  with  nitrophenols. 

Some  indicators  precipitate  with  certain  cations,  for  instance 
Orange  IV  and  Congo  with  alkali  earths. 

S0rensen  (1909)  paid  particular  attention  to  the  extraction  of 
an  indicator  from  the  aqueous  phase  by  excess  of  chloroform  etc. 
used  as  antiseptics. 

Many  indicators  precipitate  more  or  less  slowly  from  standard 


VIII  SPECIFIC    ERRORS  189 

buffer  solutions.  When  this  is  not  noticed  immediately  it  may 
lead  to  deceptions.  Propyl  red  was  rejected  from  Clark  and  Lubs' 
original  list  for  this  reason.  Some  indicators  fade  in  light.2 

Other  indicators  are  reduced  by  suspensions  of  living  cells. 
Some  of  these  are  useful  as  oxidation-reduction  indicators;  but 
the  two  classes  should  be  so  sharply  distinguished  that,  when 
possible,  the  one  property  will  not  be  used  under  conditions  in 
which  the  other  operates.  In  litmus-milk,  for  instance,  the  reduc- 
tion and  the  acid-base  change  of  the  litmus  may  occur  together 
and  introduce  complexity  of  interpretation  as  noted  by  Clark 
and  Lubs  (1917).  They  recommend  that  brom  cresol  purple  be 
substituted  for  litmus  in  the  acid  test.  Compare  Reiss  (1926). 
There  should  also  be  distinguished  the  reversible  oxidation- 
reduction  indicators  and  the  irreversible.  For  a  discussion  of 
oxidation-reduction  indicators  see  references  found  in  Chapter 
XVIII  and  Appendix,  tables  K  and  L. 

Some  indicators,  especially  several  of  the  triphenylmethane 
series,  undergo  some  of  their  color  changes  slowly.  Ignorance  of 
this  may  lead  to  serious  error. 

Several  common  indicators,  notably  Congo,  do  not  form  true 
solutions  and  degree  of  dispersion  contributes  to  the  color.  These 
indicators  show  abnormally  large  errors  due  partly  to  variations 
in  degree  of  dispersion.  They  should  not  be  expected  to  follow 
the  ordinary  equations  except  in  a  very  approximate  manner,  if 
at  all. 

In  short  all  possibilities  must  be  watched  lest  the  investigator 
venturing  upon  the  study  of  some  new  solution,  be  misled  by  the 
mark  of  reliability  placed  upon  an  indicator  tried  under  limited 
circumstances. 

Wherever  possible  it  is  good  practice  to  test  doubtful  cases 
with  two  indicators  of  widely  different  chemical  composition. 

TEMPERATURE   EFFECTS 

Let  it  be  supposed  that  the  simple  equilibrium  equation  is 
applicable.  A  condition  in  its  derivation  was  that  the  tempera- 
ture should  remain  constant.  If  the  indicator  constant  is  deter- 

2  Cullen  (1922)  reports  that  color  standards  may  fade  in  the  course  of  a 
week  to  the  extent  corresponding  to  about  0.02-0.04  pH  unit. 


190  THE    DETERMINATION    OF   HYDROGEN    IONS 

mined  by  reference  to  some  standard  buffer  solution  it  is  implied 
not  only  that  the  constant  found  applies  only  at  the  temperature 
used  but  that  this  same  temperature  was  a  condition  determining 
the  state  of  the  standard  buffer  solution.  If  a  new  temperature 
is  used  it  determines  the  states  of  both  the  buffer  and  the  indi- 
cator systems.  If  now  the  pH  values  of  the  buffer  solutions  at 
different  temperatures  are  to  be  made  the  basis  for  determining 
the  temperature  coefficient  of  the  indicator  constant,  the  method 
of  comparing  pH  values  at  different  temperatures  becomes  of 
fundamental  importance.  Unfortunately  it  will  be  found  from 
the  discussion  of  Chapter  XXII  that  there  is  considerable  con- 
fusion in  regard  to  this  point.  Therefore,  we  find  various  methods 
of  determining  so-called  temperature  coefficients  and  if  in  a  given 
case  the  specific  method  is  not  duplicated,  an  error  is  made  in  the 
sense  that  the  specified  specifically  standardized  correction  for 
temperature  has  been  wrongly  applied. 

In  Chapter  VI  are  found  temperature  coefficients  for  nitro- 
phenols  by  means  of  which  the  error  due  to  temperature  changes 
may  be  estimated  when  the  procedure  specified  is  used.  Further 
discussion  is  postponed  to  Chapter  XXII,  page  448. 

ON  MEASUREMENTS   OF   POORLY   BUFFERED    SOLUTIONS 

The  extreme  of  a  poorly  buffered  solution  is  a  solution  of  a 
strictly  "neutral"  salt  such  as  KCL  Were  an  indicator  added, 
the  indicator  system,  however  dilute,  would  function  as  the  buffer 
and  would  "indicate"  only  its  own  state  of  equilibrium. 

In  the  ordinary  applications  of  indicators  it  is  assumed  that 
the  buffer  strength  of  the  solution  is  so  great  as  practically  to  be 
unaffected  by  the  addition  of  the  small  quantity  of  indicator 
acid,  indicator  base,  or  indicator  salt. 

Now  in  the  ordinary  use  of  an  indicator  which  is,  for  instance, 
an  acid,  either  a  solution  of  the  acid  form  itself,  of  one  or  another 
of  its  salts,  of  the  partially  neutralized  indicator  or  of  the  over- 
neutralized  indicator  is  used.  In  applying  such  solutions  to 
poorly  buffered  solutions  there  may  be  extensive  interaction  and 
the  indicator  color  merely  represents  the  position  of  the  new 
equilibrium.3  This  has  been  a  very  troublesome  source  of  error 

3  Apparently,  and  unless  1  misunderstand  their  treatment.  McBain, 
Dubois  and  Hay  (1926)  have  neglected  this  aspect. 


VIII  POORLY    BUFFERED    SOLUTIONS  191 

in  numerous  practical  applications  of  indicators  to  solutions  which, 
although  poorly  buffered,  are  conveniently  characterized  by 
pH  values. 

A  method  frequently  applied  is  as  follows.  Estimate  by  par- 
tially neutralized  indicators  the  approximate  pH  value  of  the 
solution  to  be  tested.  Then,  if  the  addition  of  more  of  the  par- 
tially neutralized  indicator  alters  the  color  as  compared  with  a 
like  well  buffered  standard,  the  assumption  is  that  the  indicator 
solution  and  unknown  had  not  the  same  pH  value  and  therefore 
reacted  upon  each  other  to  a  new  point  of  equilibrium.  If  the 
displacement  of  color  was  toward  a  greater  proportion  of  the  acid 
form  of  the  indicator,  it  is  assumed  that  the  tested  solution  had  a 
lower  pH  value  than  the  indicator  solution.  Accordingly  adjust 
the  indicator  solution  in  this  direction  and  again  compare  after 
adding  different  amounts  of  the  indicator,  in  each  case  comparing 
the  resulting  color  with  that  of  a  well  buffered  standard  containing 
the  given  quantity  of  indicator.  By  this  "trial  and  error" 
method  there  are  at  last  established  isohydric  solutions  which  on 
admixture  in  different  proportions  should  not  affect  the  equilib- 
rium of  either  system  except  in  a  minor  and,  for  present  purposes, 
negligible  degree.  Obviously  a  salt-effect  remains  to  be  con- 
sidered, see  also  Dawson  (1925). 


CHAPTER  IX 

STANDARD  BUFFER  SOLUTIONS  FOR  COLORIMETRIC  COMPARISON 

//  arithmetic,  mensuration  and  weighing  be  taken  from  any  art} 
that  which  remains  will  not  be  much. — PLATO. 

The  standard  solutions  used  in  the  colorimetric  method  of 
determining  hydrogen  ion  concentrations  are  buffer  solutions 
with  such  well  defined  compositions  that  they  can  be  accurately 
reproduced,  and  with  pH  values  accurately  defined  by  hydrogen 
electrode  measurements.  They  generally  consist  of  mixtures  of 
some  acid  and  its  alkali  salt.  Several  such  mixtures  have  been 
carefully  studied.  An  excellent  set  has  been  described  by  S0ren- 
sen  (1912).  This  set  may  be  supplemented  by  the  acetic  acid — 
sodium  acetate  mixtures  most  careful  measurements  of  which 
have  been  made  by  Walpole  (1914),  and  restudied  by  Cohn, 
Heyroth  and  Menkin  (1928).  The  set  may  also  be  supplemented 
by  Palitzsch's  (1915)  excellent  boric  acid-borax  mixtures,  or  by 
one  or  another  of  the  several  series  of  mixtures  which  have  been 
described  in  more  recent  years.  A  few  of  these  will  be  mentioned 
but  details  will  be  given  only  for  those  mixtures  which  are,  in 
the  writer's  limited  knowledge,  the  more  widely  used. 

In  assigning  values  to  these  buffer  solutions  different  authors 
have  made  somewhat  different  assumptions.  See  especially 
Chapter  XXIII  and  those  sections  which  deal  with  the  hydrogen 
electrode. 


Clark  and  Lubs  (1916)  have  designed  a  set  of  standards  which 
they  believe  are  somewhat  more  conveniently  prepared  than 
are  the  S0rensen  standards.  Their  set  is  composed  of  the  follow- 
ing mixtures: 

Potassium  chlorid  +  HC1 
Acid  potassium  phthalate   +  HC1 
Acid  potassium  phthalate  +  NaOH 
Acid  potassium  phosphate  +  NaOH 
Boric  acid,  KC1  +  NaOH 
192 


IX  STANDARD    BUFFERS  193 

Clark  and  Lubs  published  their  data  for  KC1-HC1  mixtures  as 
preliminary  data.  Although  these  data  were  retained  in  previous 
editions  they  have  now  been  rejected  and  replaced  by  table  35a. 
The  pH  numbers  in  table  35a  are  calculated  with  the  assumption 
that  7n+  =  0.84  for  these  mixtures  of  constant  ionic  strength 
(/*  =  0.1).  The  assumption  is  not  entirely  justified;  but,  for  con- 
venience in  the  comparison  of  calculations,  the  third  decimal  of 
the  pH  numbers  is  given.  The  uncertainty  affects  the  second 
decimal  place. 

In  table  35  the  compositions  have  been  recalculated  from  the 
original  data  with  the  elimination  of  corrections  made  with  the 
Bjerrum  extrapolation.  This  should  bring  the  numbers  into 
conformity  with  the  specifications  of  Chapter  XXIII. 

For  a  discussion  of  these  mixtures,  the  methods  used  in  deter- 
mining their  pH  values,  and  the  potential  measurements  we  refer 
the  reader  to  the  original  paper  (Journal  of  Biological  Chemistry, 
1916,  25,  no.  3,  p.  479).  -We  may  proceed  at  once  to  describe  the 
details  of  preparation. 

The  various  mixtures  are  made  up  from  the  following  stock 
solutions:  M/5  potassium  chlorid  (KC1),  M/5  acid  potassium 
phosphate  (KH2PO4),  M/5  acid  potassium  phthalate  (KHCsH^CX), 
M/5  boric  acid  with  M/5  potassium  chlorid  (H3BO3,  KC1),  M/5 
sodium  hydroxid  (NaOH),  and  M/5  hydrochloric  acid  (HC1). 
Although  the  subsequent  mixtures  are  diluted  to  M/20  the  above 
concentrations  of  the  stock  solutions  are  convenient  for  several 
reasons. 

The  water  used  in  the  crystallization  of  the  salts  and  in  the 
preparation  of  the  stock  solutions  and  mixtures  should  be  redis- 
tilled. So-called  "conductivity  water,"  which  is  distilled  first 
from  acid  chromate  solution  and  again  from  barium  hydroxid,  is 
recommended,  but  it  is  not  necessary. 

M/5  potassium  chlorid  solution.  (This  solution  will  not  be 
necessary  except  in  the  preparation  of  the  most  acid  series  of 
mixtures.  See  table.)  The  salt  should  be  recrystallized  three  or 
four  times  and  dried  in  an  oven  at  about  120°C.  for  two  days.  The 
fifth  molecular  solution  contains  14.912  grams  in  1  liter. 

M/5  acid  potassium  phthalate  solution.  Acid  potassium  phtha- 
late may  be  prepared  by  the  method  of  Dodge  (1915-1920)  modified 
as  follows.  Make  up  a  concentrated  potassium  hydroxid  solu- 


194  THE    DETERMINATION    OF   HYDROGEN   IONS 

tion  by  dissolving  about  60  grams  of  a  high-grade  sample  in  about 
400  cc.  of  water.  To  this  add  50  grams  of  the  commercial  re- 
sublimed  anhydrid  of  ortho  phthalic  acid.1  Test  a  cool  portion  of 
the  solution  with  phenol  phthalein.  If  the  solution  is  still  alka- 
line, add  more  phthalic  anhydrid;  if  acid,  add  more  KOH.  When 
roughly  adjusted  to  a  slight  pink  with  phenol  phthalein2  add  as 
much  more  phthalic  anhydrid  as  the  solution  contains  and  heat 
till  all  is  dissolved.  Filter  while  hot,  and  allow  the  crystalliza- 
tion to  take  place  slowly.  The  crystals  should  be  drained  with 
suction  and  recrystallized  at  least  twice  from  distilled  water. 

Crystallization  should  not  be  allowed  to  take  place  below  20°C., 
for  Dodge  (1920)  states: 

A  saturated  solution  of  the  acid  phthalate  on  chilling  will  deposit 
crystals  of  a  more  acid  salt,  having  the  formula  2KHC8H4O4-C8H6O4. 
These  crystals  are  in  the  form  of  prismatic  needles,  easily  distinguished 
under  the  microscope  from  the  6-sided  orthorhombic  plates  of  the  salt 
KHC8H4O4. 

Dry  the  salt  at  110°-115°C.  to  constant  weight. 
A  fifth  molecular  solution  contains  40.836  grams  of  the  salt 
in  1  liter  of  the  solution. 

M/6  acid  potassium  phosphate  solution?    A  high-grade  com- 

1  While  phthalic  anhydride  is  now  prepared  commercially  in  very  high 
purity  and  has  become  comparatively  inexpensive,  dealers  will  sometimes 
furnish  material  which  is  grossly  impure.    Among  the  more  serious  con- 
taminants are  benzoic  acid,  naphthols  and  possibly  quinones.    See  Conover 
and  Gibbs  (1922).    The  best  method  of  purification  is  that  of  sublimation 
in  an  apparatus  of  the  type  invented  by  Gibbs  (1924) .    The  better  grades 
of  phthalic  anhydride  are  now  made  in  remarkable  purity  by  the  vapor 
phase,  catalytic  oxidation  of  naphthalene;  a  process  discovered  by  Gibbs 
(1918).    Unless  some  purification  is  made  when  one  has  to  use  the  lower 
grades  of  the  anhydride,  it  may  be  necessary  to  recrystallize  the  potassium 
salt  of  the  acid  ten  or  more  times  before  a  sample  is  suitable  for  satis- 
factory hydrogen  electrode  measurements.    A  great  deal  of  trouble  is 
avoided  by  purchase  of  the  highest  grade  anhydride  in  the  first  place. 

2  Use  a  diluted  portion  for  the  final  test. 

3  The  original  measurements  of  Clark  and  Lubs  were  made  with  samples 
of  phosphate  which  gave  no  clouding  or  floes  in  their  dilute  solutions. 
Since  then,  and  especially  within  recent  years,  the  writer  has  had  difficulty 
in  obtaining  phosphates,  dilute  solutions  of  which  will  not   show  this 
sign  of  impurity.    No  reasonable  number  of  recrystallizations  seem  to  rid 
the  material  of  the  contaminant.    It  appears  to  be  an  aluminium  com- 


IX  PEEPARATION   OF   SOLUTIONS  195 

mercial  sample  of  the  salt  is  recrystallized  at  least  three  times 
from  distilled  water  and  dried  to  constant  weight  at  110-115°C. 
A  fifth  molecular  solution  should  contain  27.232  grams  in  1  liter. 
The  solution  should  be  distinctly  red  with  methyl  red  and  dis- 
tinctly blue  with  brom  phenol  blue. 

M/5  boric  acid  M/5  potassium  chlorid.  Boric  acid  should  be 
recrystallized  several  times  from  distilled  water.  It  should  be 
air  dried4  in  thin  layers  between  filter  paper  and  the  constancy 
of  weight  established  by  drying  small  samples  in  thin  layers  in  a 
desiccator  over  CaCl2.  Purification  of  KC1  has  already  been 
noted.  It  is  added  to  the  boric  acid  solution  to  bring  the  salt 
concentration  in  the  borate  mixtures  to  a  point  comparable  with 
that  of  the  phosphate  mixtures  so  that  colorimetric  checks  may 
be  obtained  with  the  two  series  where  they  overlap.  One  liter 
of  the  solution  should  contain  12.4048  grams5  of  boric  acid  and  •/- 
14.912  grams  of  potassium  chlorigL ^  ~f~ 

M/5  sodium  hydroxid  solution.  This  solution  is  the  most  diffi- 
cult to  prepare,  since  it  should  be  as  free  as  possible  from  carbon- 
ate. A  solution  of  sufficient  purity  for  the  present  purposes  may 
be  prepared  from  a  high  grade  sample  of  the  hydroxid  in  the 
following  manner.  Dissolve  100  grams  NaOH  in  100  cc.  distilled 
water  in  a  Jena  or  Pyrex  glass  Erlenmeyer  flask.  Cover  the 
mouth  of  the  flask  with  tin  foil  and  allow  the  solution  to  stand 
over  night  till  the  carbonate  has  settled.  Then  prepare  a  filter 
as  follows.  Cut  a  "hardened"  filter  paper  to  fit  a  Buchner  funnel. 
Treat  it  with  warm,  strong  [1:1]  NaOH  solution.  After  a  few 
minutes  decant  the  sodium  hydroxid  and  wash  the  paper  first 
with  absolute  alcohol,  then  with  dilute  alcohol,  and  finally  with 
large  quantities  of  distilled  water.  Place  the  paper  on  the  Buch- 
ner funnel  and  apply  gentle  suction  until  the  greater  part  of  the 

pound.  A  large  sample  of  phosphoric  acid  which  Dr.  Ross  prepared  for 
the  writer  by  the  method  of  Ross,  Jones  and  Durgin  (1925)  was  converted 
to  acid  potassium  phosphate.  This  has  been  entirely  satisfactory. 

4  Eoric  acid  begins  to  lose  "water  of  constitution"  above  50°C. 

6  This  weight  was  used  on  the  assumption  that  the  atomic  weight  of 
boron  is  11.0.  The  atomic  weight  has  since  been  revised  and  appears  as 
10.82  in  the  1927  International  Table  of  Atomic  Weights. 

Because  the  solutions  were  standardized  with  the  above  weight  of  boric 
acid  this  weight  should  be  used. 


196 


THE    DETERMINATION    OF   HYDROGEN   IONS 


water  has  evaporated;  but  do  not  dry  so  that  the  paper  curls. 
Now  pour  the  concentrated  alkali  upon  the  middle  of  the  paper, 
spread  it  with  a  glass  rod  making  sure  that  the  paper,  under 
gentle  suction,  adheres  well  to  the  funnel,  and  draw  the  solution 
through  with  suction.  The  clear  filtrate  is  now  diluted  quickly, 
after  rough  calculation,  to  a  solution  somewhat  more  concentrated 
than  N/l.  Withdraw  10  cc.  of  this  dilution  and  standardize 
roughly  with  an  acid  solution  of  known  strength,  or  with  a  sample 
of  acid  potassium  phthalate.  From  this  approximate  standardiza- 
tion calculate  the  amount  required  to  furnish  an  M/5  solution. 


FIG.  33.  PARAFFINED  BOTTLE,  WITH  ATTACHED  BURETTE  AND  SODA-LIME 
TUBES  FOR  STANDARD  ALKALI 

Make  the  required  dilution  with  the  least  possible  exposure,  and 
pour  the  solution  into  a  paraffined*  bottle  to  which  a  calibrated  50 
cc.  buret  and  soda-lime  guard  tubes  have  been  attached.  See 
figure  33.  The  solution  should  now  be  most  carefully  standard- 
ized. One  of  the  simplest  methods  of  doing  this,  and  one  which 

6  The  author  finds  that  thick  coats  of  paraffin  are  more  satisfactory  than 
the  thin  coats  sometimes  recommended.  Thoroughly  clean  and  dry  the 
bottle,  warm  it  and  then  pour  in  the  melted  paraffin.  Roll  gently  to  make 
an  even  coat  and  just  before  solidification  occurs  stand  the  bottle  upright 
to  allow  excess  paraffin  to  drain  to  the  bottom  and  there  form  a  very  sub- 
stantial layer. 


IX  STANDARD    ALKALI  197 

should  always  be  used  in  this  instance,  is  the  method  of  Dodge 
(1915)  in  which  use  is  made  of  the  acid  potassium  phthalate 
purified  as  already  described.  Weigh  out  accurately  on  a  chemical 
balance  with  standardized  weights  several  portions  of  the  salt  of 
about  1.6  gram  each.  Dissolve  in  about  20  cc.  distilled  water 
and  add  4  drops  phenol  phthalein.  Pass  a  stream  of  C02-free 
air  through  the  solution  and  titrate  with  the  alkali  till  a  faint 
but  distinct  pink  is  developed.  It  is  preferable  to  use  a  factor 
with  the  solution  rather  than  attempt  adjustment  to  an  exact 
M/5  solution. 

If  one  should  be  fortunate  enough  to  find  that  the  concentrated 
sodium  hydroxid  solution  had  clarified  itself  without  leaving 
suspended  carbonate,  the  clear  solution  might  be  carefully  pi- 
petted from  the  sediment.  Cornog  (1921)  describes  another 
method  as  follows : 

Distilled  water  contained  in  an  Erlenmeyer  flask  is  boiled  to  remove 
any  carbon  dioxide  present,  after  which,  when  the  water  is  cooled  enough, 
ethyl  ether  is  added  to  form  a  layer  3  or  4  cm.  in  depth.  Pieces  of  metallic 
sodium,  not  exceeding  about  1  cm.  in  diameter  are  then  dropped  into  the 
flask.  They  will  fall  no  further  than  the  ether  layer  where  they  remain 
suspended.  The  water  contained  in  the  ether  layer  causes  the  slow  forma- 
tion of  sodium  hydroxid,  which  readily  passes  below  to  the  water  layer. 

Cornog  depends  upon  the  evaporation  of  the  ether  as  a  barrier 
to  CO2.  There  are  various  ways  in  which  the  protection  can  be 
made  more  sure,  and  there  are  also  various  ways  in  which  the 
aqueous  solution  may  be  separated  from  the  ether. 

From  time  to  time  there  appear  in  the  literature  suggestions 
regarding  the  use  of  barium  salts  to  remove  the  carbonate  in 
alkali  solutions. 

In  the  author's  opinion  the  next  step  to  take,  if  the  separation 
of  carbonate  from  very  concentrated  NaOH  solutions  is  not  con- 
sidered refined  enough  for  the  purpose  at  hand,  is  to  proceed 
directly  to  the  electrolytic  preparation  of  an  amalgam.  Given 
a  battery  and  two  platinum  electrodes  this  is  a  simple  process. 
A  deep  layer  of  redistilled  mercury  is  placed  in  a  conical  separa- 
tory  funnel.  The  negative  pole  of  the  battery  is  led  to  this 
mercury  by  a  glass-protected  platinum  wire.  Over  the  mercury 
is  placed  a  concentrated  solution  of  recrystallized  sodium  chlorid 
and  in  this  solution  is  dipped  a  platinum  electrode  connected 


198  THE   DETERMINATION   OF   HYDROGEN   IONS 

with  the  positive  pole  of  the  battery.  The  battery  may  have  a 
potential  of  4  to  6  volts.  Electrolysis  is  continued  with  occasional 
gentle  shaking  to  break  up  amalgam  crystals  forming  on  the 
mercury  surface. 

Boil  the  CO2  out  of  a  liter  or  so  of  redistilled  water,  and,  while 
steam  is  still  escaping,  stopper  the  flask  with  a  cork  carrying  a 
siphon,  a  soda-lime  guard  tube  and  a  corked  opening  for  the 
separatory  funnel. 

When  the  water  is  cool  introduce  the  delivery  tube  of  the  separa- 
tory funnel  and  deliver  the  amalgam.  Allow  reaction  to  take 
place  till  a  portion  of  the  solution,  when  siphoned  off  to  a  buret 
and  standardized,  shows  that  enough  hydroxid  has  been  formed. 
Then  siphon  approximately  the  required  amount  into  a  boiled- 
out  and  protected  portion  of  water.  Mix  thoroughly  and 
standardize. 

M/5  hydrochloric  acid  solution.  Dilute  a  high  grade  hydro- 
chloric acid  solution  to  about  20  per  cent  and  distill.  Dilute  the 
distillate  to  approximately  M/5  and  standardize  with  the  sodium 
hydroxid  solution  previously  described.  If  convenient,  it  is  well 
to  standardize  this  solution  carefully  by  the  silver  chlorid  method 
and  check  with  the  standardized  alkali.  Standard  solutions  of 
hydrochloric  acid  are  also  prepared  from  constant  boiling  mix- 
tures. See  data  and  references  by  Foulk  and  Rollings  worth 
(1923). 

The  only  solution  which  it  is  absolutely  necessary  to  protect 
from  the  C02  of  the  atmosphere  is  the  sodium  hydroxid  solution. 
Therefore  all  but  this  solution  may  be  stored  in  ordinary  bottles 
of  resistant  glass*.  The  salt  solutions,  if  adjusted  to  exactly  M/5, 
may  be  measured  from  clean  calibrated  pipets. 

These  constitute  the  stock  solutions  from  which  the  mixtures 
are  prepared.  The  general  relationships  of  these  mixtures  to 
their  pH  values  are  shown  in  figure  34.  In  this  figure  pH  values 
are  plotted  as  ordinates  against  X  cc.  of  acid  or  alkali  as  abscissas. 
It  will  be  found  advantageous  to  plot  this  figure  from  table  35 
with  greatly  enlarged  scale  so  that  it  may  be  used  as  is  S0rensen's 
chart  (1909).  The  compositions  of  the  mixtures  at  even  intervals 
of  0.2  pH  are  given  in  table  35. 

In  any  measurement  the  apportionment  of  scale  divisions 
should  accord  with  the  precision.  Scale  divisions  should  not  be 


IX 


STANDARD    BUFFERS 


199 


4fe— 


B 


10 


PH 


50 


X-C.C. 

FIG.  34.  CLARK  AND  LUBS'  STANDARD  MIXTURES 

A.  Fifty  cubic  centimeters  0.2  M  KHPhthalate  +  X  cc.  0.2  M  HC1. 
Diluted  to  200  cc. 

B.  Fifty  cubic  centimeters  0.2  M  KHPhthalate  +  X  cc.  0.2  M  NaOH. 
Diluted  to  200  cc. 

C.  Fifty  cubic  centimeters  0.2  M  KH2PO4  +  X  cc.  0.2  M  NaOH.    Diluted 
to  200  cc. 

D.  Fifty  cubic  centimeters  0.2  M  H3BO3,  0.2  M  KC1  +  X  cc,  0.2  M 
NaOH.    Diluted  to  200  cc. 


200 


THE   DETERMINATION    OF    HYDROGEN    IONS 


TABLE  35 

Composition  of  mixtures  giving  pH  values  at  20°C.  at  interval  of  0.2 
Phthalate-HCl  mixtures 


2. 

2 

50  cc.  M/5  KHPhthalate 

46.60cc.  M/5HC1 

Dilute 

to  200 

cc. 

2. 

4 

50  cc.  M/5  KHPhthalate 

39.60cc.  M/5HC1  ' 

Dilute 

to  200 

cc. 

2. 

6 

50  cc.  M/5  KHPhthalate 

33.00cc.  M/5HC1 

Dilute 

to  200 

cc. 

2. 

8 

50  cc.  M/5  KHPhthalate 

26.50cc.  M/5HC1 

Dilute 

to  200 

cc. 

3. 

0 

50  cc.  M/5  KHPhthalate 

20.40cc.  M/5HC1 

Dilute 

to  200 

cc. 

3. 

2 

50  cc.  M/5  KHPhthalate 

14.80cc.  M/5HC1 

Dilute 

to  200 

cc. 

3.4 

50  cc.  M/5  KHPhthalate 

9.95  cc.  M/5  HC1 

Dilute 

to  200 

cc. 

3. 

6 

50  cc.  M/5  KHPhthalate 

6  00  cc.  M/5HC1 

Dilute 

to  200 

cc. 

3. 

8 

50  cc.  M/5  KHPhthalate 

2.65cc.  M/5HC1 

Dilute 

to  200 

cc. 

Phthalate-NaOH  mixtures 

4. 

0 

50  cc.  M/5  KHPhthalate 

0.40cc.  M/5NaOH 

Dilute 

to  200  cc. 

4.2 

50  cc.  M/5  KHPhthalate 

3.65cc.  M/5NaOH 

Dilute 

to  200 

cc. 

4, 

,4 

50  cc.  M/5  KHPhthalate 

7.35cc.  M/5NaOH 

Dilute 

to  200 

cc. 

4 

.6 

50  cc.  M/5  KHPhthalate 

12  00  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

4 

.8 

50  cc.  M/5  KHPhthalate 

17.50  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

5.0 

50  cc.  M/5  KHPhthalate 

23.  65  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

5 

.2 

50  cc.  M/5  KHPhthalate 

29.  75  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

5 

.4 

50  cc.  M/5  KHPhthalate 

35.25cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

5 

.6 

50  cc.  M/5  KHPhthalate 

39.  70  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

5 

.8 

50  cc.  M/5  KHPhthalate 

43.  10  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

6 

.0 

50  cc.  M/5  KHPhthalate 

45.  40  cc.  M/5  NaOH 

Dilute 

to  200  cc. 

6 

.2 

50  cc.  M/5  KHPhthalate 

47.00  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

KH2PO4-NaOH  mixtures 

5 

.8 

50  cc.  M/5  KH2PO4 

3  66  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

6 

.0 

50  cc.  M/5  KH2PO4 

5.64  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

6 

.2 

50  cc.  M/5  KH2PO4 

8.55cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

6 

.4 

50  cc.  M/5  KH2P04 

12.60cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

6 

.6 

50  cc.  M/5  KH2PO4 

17.74  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

6 

.8 

50  cc.  M/5  KH2PO4 

23  60  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

7 

.0 

50  cc.  M/5  KH2PO4 

29.  54  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

7 

.2 

50  cc.  M/5  KH2PO4 

34.  90  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

7 

.4 

50  cc.  M/5  KH2P04 

39.34  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

7 

6 

50  cc.  M/5  KH2PO4 

42.  74  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

7 

.8 

50  cc.  M/5  KH2P04 

45.17  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

8 

.0 

50  cc.  M/5  KH2P04 

46.  85  cc.  M/5  NaOH 

Dilute 

to  200 

cc. 

IX 


STANDARD    BUFFERS 


201 


TABLE  35— Concluded 

Boric  acid,     KCl-NaOH  mixtures 


7.8  50  cc. 
8.0  50  cc. 
8.2  50  cc. 
8.4  50  cc. 
8.6  50  cc. 
8.8  50  cc. 
9.0  50  cc. 
9.2  50  cc. 
9.4  50  cc. 
9.6  50  cc. 
9.8  50  cc. 
10.0  50  cc. 


M/5  HsBOs, 
M/5  H3BO3, 
M/5  H3BO3, 
M/5  H3B03, 
M/5  H3BO3, 
M/5  H3BO3, 
M/5  H3B03, 
M/5  H3BO3, 
M/5  H3BO3, 
M/5  H3BOS, 
M/5  H3B03, 
M/5  H3B03, 


M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 
M/5  KC1 


2.65cc. 

4.00  cc. 

5.90  cc. 

8.55  cc; 
12.00  cc. 
16.40  cc. 
21.40  cc. 
26.70cc. 
32.00cc. 
36.85  cc. 
40.80  cc. 
43.90  cc. 


M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 
M/5  NaOH 


Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 
Dilute 


to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc. 
to  200  cc 


It  is  important  to  check  the  consistency  of  any  particular  set  of  these 
mixtures  by  comparing  "5.8"  and  "6.2  phthalate"  with  "5.8"  and  "6.2 
phosphate"  using  brom  cresol  purple.  Also  "7.8"  and  "8.0  phosphate" 
should  be  compared  with  the  corresponding  borates  using  cresol  red. 

TABLE  35a 

HC1-KC1  MIXTURES  OF  CONSTANT  IONIC  STRENGTH,  ju  =  0.1 
Calculated  on  assumption  that  7H+  =  0.84 


KC1 

MOLAR 

HCl 

MOLAR 

pH 

COMPOSITION  FOR  0.1  pH  UNIT  INCREMENT  OF  pH 

STOCK  KC1:  0.2  MOLAR 
STOCK  HCl:  0.2  MOLAR 

KC1 

solution 

HCl 
solution 

pH 

cc. 

cc. 

0.00 

0.10 

1.07tfa      0.00  +  59.5 

dilute  to  100  cc. 

(1.0)  Gu  =  0.119) 

0.01 

0.09 

1.120  '     2.72  +  47.28 

dilute  to  100  cc. 

1.1 

0.02 

0.08 

1.175     12.45  +  37.55 

dilute  to  100  cc. 

1.2 

0.03 

0.07 

1.231     20.16  +  29.84 

dilute  to  100  cc. 

1.3 

0.04 

0.06 

1.298  1  26.30  +  23.70 

dilute  to  100  cc. 

1.4 

0.05 

0.05 

1.377 

31.18  +  18.82 

dilute  to  100  cc. 

1.5 

0.06 

0.04 

1.474 

35.03  +  14.95 

dilute  to  100  cc. 

1.6 

0.03 

0.03 

1.595 

38.12  +  11.88 

dilute  to  100  cc. 

1.7 

0.01 

0.02 

1.774 

40.57  +     9.43 

dilute  to  100  cc. 

1.8 

0.09 

0.01 

2.07£a 

42.51  +     7.49 

dilute  to  100  cc. 

1.9 

0.095 

0.005 

2.377 

44.05  +     5.95 

dilute  to  100  cc. 

2.0 

0.098 

0.002 

2.77-5 

45.27  +    4.73 

dilute  to  100  cc. 

2.1 

0.099 

0.001 

3.075 

46.24  +     3.76 

dilute  to  100  cc. 

2.2 

a  See  page  472. 


202         THE  DETEKMINATION  OF  HYDROGEN  IONS 

The  original  data  for  mixtures  in  table  35  were  obtained  with  a  saturated 
KC1  calomel  electrode  as  a  working  standard.  This  was  compared  with  a 
group  of  tenth-normal  KC1  calomel  half -cells.  In  calculating  pH  values 
for  previous  tables  (see  earlier  editions  and  compare  Clark  and  Lubs 
1916,  1917)  there  were  included  Bjerrum  extrapolations.  These  were  es- 
pecially large  in  the  case  of  the  HC1-KC1  mixtures.  The  original  data 
have  now  been  used  in  recalculations  in  accord  with  the  specifications  of 
Chapter  XXIII. 

so  coarse  that  interpolations  tax  the  judgment  nor  so  fine  as  to 
be  ridiculous.  What  scale  divisions  are  best  in  the  method  under 
discussion  it  is  difficult  to  decide,  since  the  precision  which  may 
be  attained  depends  somewhat  upon  the  ability  of  the  individual 
eye,  and  upon  the  material  examined,  as  well  as  upon  the  means 
and  the  judgment  used  in  overcoming  certain  difficulties  which 
we  shall  mention  later.  S0rensen  (1909)  has  arranged  the  stand- 
ard solutions  to  differ  by  even  parts  of  the  components,  a  system 
which  furnishes  uneven  increments  in  pH.  Michaelis,  (1910)  on 
the  other  hand,  makes  his  standards  vary  by  about  0.3  pH  so 
that  the  corresponding  hydrogen  ion  concentrations  are  approxi- 
mately doubled  at  each  step.  Certain  general  considerations 
lead  to  the  conclusion  that  for  most  work  estimation  of  pH  values 
to  the  nearest  0.1  division  is  sufficiently  precise,  and  that  this 
precision  can  be  obtained  when  the  nature  of  the  medium  per- 
mits if  the  comparison  standards  differ  by  increments  of  0.2  pH. 

If  smaller  increments  are  desired  it  is  permissible  within  limits 
to  interpolate;  but  see  table  43. 

It  is  convenient  to  prepare  200  cc.  of  each  of  the  mixtures  and 
to  preserve  them  in  bottles  each  of  which  has  its  own  10  cc. 
pipet  thrust  through  the  stopper.7  It  takes  but  little  more  time 
to  prepare  200  cc.  than  it  does  to  prepare  a  10  cc.  portion,  and 
if  the  larger  volume  is  prepared  there  will  not  only  be  a  sufficient 
quantity  for  a  day's  work  but  there  will  be  some  on  hand  for  the 
occasional  test. 

Unless  electrometric  measurements  can  be  used  as  control,  we 
urge  the  most  scrupulous  care  in  the  preparation  and  preserva- 
tion of  the  standards.  We  have  specified  several  recrystalliza- 
tions  of  the  salts  used  because  commercial  samples  are  not  always 
to  be  relied  upon. 

7  No  serious  error  will  be  made  if  the  tips  of  the  pipettes  be  broken  to 
permit  rapid  delivery. 


ix  S^RENSEN'S  STANDARDS  203 

S0RENSEN?S    STANDARD   BUFFER   SOLUTIONS 

S0rensen's  standards  are  made  as  follows.  The  stock  solutions 
are: 

1.  A  carefully  prepared  exact  tenth  normal  solution  of  HC1. 

2.  A  carbonate-free  exact  tenth  normal  solution  of  NaOH. 

3.  A  tenth  molecular  glycocoll  solution  containing  sodium  chlo- 
rid, 7.505  grams  glycocoll  ancL'5.85  grams  'Nad  in  1  liter  of 
solution. 

4.  An  M/15  solution  of  primary  potassium  phosphate  which 
contains  9.078  grams  KH2P04  in  1  liter  of  solution. 

5.  An  M/15  solution  of  secondary  sodium  phosphate  which 
contains  11.1876  grams  Na2HP04,  2H2O  in  1  liter  of  solution. 

6.  A  tenth  molecular  solution  of  secondary  sodium  citrate  made 
from  a  solution  containing  21.008  grams  crystallized  citric  acid 
and  200  cc.  carbonate-free  N/l  NaOH  diluted  to  1  liter. 

7.  An  alkaline  borate  solution  made  from  12.404  grams  boric 
acid  dissolved  in  100  cc.  carbonate-free  N/l  NaOH  and  diluted 
to  1  liter. 

The  water  shall  be  boiled,  carbon  dioxid-free,  distilled  water, 
and  the  solutions  shall  be  protected  against  contamination  by 
C02. 

The  materials  for  these  solutions  are  described  by  S0rensen  as 
follows. 

Glycocoll  (glycine) 

Two  grams  glycocoll  should  give  a  clear  solution  in  20  cc. 
water  and  should  test  practically  free  of  chlorid  or  sulfate.  Five 
grams  should  yield  less  than  2  mgm.  of  ash.  Five  grams  should 
yield,  on  distillation  with  300  cc.  of  5  per  cent  sodium  hydroxid, 
less  than  1  mgm.  of  nitrogen  as  ammonia.  The  nitrogen  content 
as  determined  by  the  Kjeldahl  method  should  be  18.67  ±0.1  per 
cent. 

Primary  phosphate, 


The  salt  must  dissolve  clear  in  water  and  yield  no  test  for 
chlorid  or  for  sulfate.  When  dried  under  20  or  30  mm.  pressure 
for  a  day  at  100°C.  the  loss  in  weight  should  be  less  than  0.1  per 
cent,  and  on  ignition  the  loss  should  be  13.23  ±0.1  per  cent. 
When  compared  colorimetrically  with  citrate  mixtures  the  stock 


204         THE  DETERMINATION  OF  HYDROGEN  IONS 

phosphate  solution  should  lie  between  "7"  and  "8  citrate-HCl." 
On  addition  of  a  drop  of  tenth-normal  alkali  or  acid  to  100  cc. 
the  color  .of  this  phosphate  solution  with  an  indicator  should  be 
widely  displaced. 

Secondary  phosphate  NazHPO^,  2  H20 

The  salt  with  this  content  of  water  of  crystallization  is  pre- 
pared by  exposing  to  the  ordinary  atmosphere  the  crystals  con- 
taining twelve  moles  of  water. 8  An  exposure  of  about  two  weeks 
is  generally  sufficient.  The  salt  should  yield  a  clear  solution 
and  yield  no  test  for  chlorid  or  sulfate.  A  day  of  drying  under  20 
to  30  mm.  pressure  at  100°C.  and  then  careful  ignition  to  constant 
weight,  should  result  in  a  25.28  ±0.1  per  cent  loss.  The  stock 
solution  should  correspond  on  colorimetric  test  with  "10  borate- 
HC1"  and  should  be  displaced  beyond  "8  borate-HCl"  on  addi- 
tion of  a  drop  of  N/10  acid,  and  beyond  "8  borate-NaOH"  with 
a  drop  of  alkali  to  100  cc. 

Citric  acid,  C6HB07,  H20 

The  acid  should  dissolve  clear  in  water,  should  yield  no  test 
for  chlorid  or  sulfate  and  should  give  practically  no  ash.  The 
water  of  crystallization  may  be  determined  by  drying  under  20 
to  30  mm.  pressure  at  70°C.  On  drying  in  this  manner  the  acid 
should  remain  colorless  and  lose  8.58  ±0.1  per  cent.  The  acidity 
of  the  citric  acid  solution  is  determined  by  titration  with  0.2  N 
barium  hydroxid  with  phenolphthalein  as  indicator.  Titration  is 
carried  to  a  distinct  red  color  of  the  indicator. 

8  There  have  been  occasional  complaints  of  the  difficulty  of  preparing 
or  keeping  S0rensen's  salt  with  a  definite  water  content.  See  for  example 
Clark  and  Lubs  (1916)  and  Cohn  (1927).  Naegeli  (1926)  has  brought 
together  a  number  of  references  and  a  table  of  vapor  pressures  of  the 
several  hydrate  systems  which  indicate  that  the  subject  is  not  yet  in  a 
satisfactory  state.  Naegeli  prefers  to  make  his  buffer  solutions  with 
the  heptahydrate,  solutions  of  which  are  standardized  gravimetrically. 
S0rensen  states  that  he  had  no  difficulty  in  obtaining  the  salt  by  exposure 
of  the  heptahydrate  to  the  dry  atmosphere  of  cold  winter  days.  It  should 
be  noted  that  S0rensen  took  his  usual  care  by  determining  the  water  con- 
tent. This  is  advisable  in  variable  climates. 

Certain  samples  sold  for  the  preparation  of  standard  buffers  and  called 
"S0rensen's  Phosphate"  are  wrongly  labeled  Na2HP04. 


IX 


STANDARD    BUFFERS 


205 


O.C.-A 

1098 


\ 


6 


8         9        10 


01         2345 
C.C.-B 

FIG.  35.  S0RENSEN's  STANDARD  MIXTURES,   WALPOLE'S  ACETATE  SOLU- 
TIONS AND  PALITZSCH'S  BORATE  SOLUTIONS 
Mixtures  of  A  parts  of  acid  constituent  and  B  parts  of  basic  constituent 


206 


THE  DETERMINATION  OF  HYDROGEN  IONS 


I1 

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IX 


S0RENSENJS   STANDARDS 


207 


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208 


THE   DETERMINATION   OF   HYDROGEN   IONS 


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IX 


S0RENSEN'S   STANDARDS 


209 


TABLE  38 

Sprensen's  borate  —  HCl  mixtures 

(Walbum's  values) 

Borate:  12.404g  H3BO3  +  100  cc.  N  NaOH  per  1. 
HCl:  0.1  TV 


Temperature 

10° 

20° 

30° 

40° 

50° 

60° 

70° 

8.86 

10.0  Borate    

9.30 

9.23 

9.15 

9.08 

9.00 

8.93 

9  5  Borate  +  05  HCl 

9.22 

9.15 

9.08 

9.01 

8.94 

8.87 

8.80 

9.0  Borate  +  1.0  HCl  

9.14 

9.07 

9.01 

8.94 

8.87 

8.80 

8.74 

8.5  Borate  +  1.5  HCl  

9.06 

8.99 

8.92 

8.86 

8.80 

8.73 

8.67 

8.0  Borate  +  2.0  HCl  

8.96 

8.89 

8.83 

8.77 

8.71 

8.66 

8.59 

7.5  Borate  +  2.5  HCl 

8.84 

8.79 

8.72 

8.67 

8.61 

8.55 

8.50 

7.0  Borate  +  30  HCl 

8.72 

8.67 

8.61 

8.56 

8.50 

8.45 

8.40 

6.5  Borate  +  3.5  HCl 

8.54 

8.49 

8.44 

8.40 

8.35 

8.30 

8.26 

6.0  Borate  +  4.0  HCl 

8.32 

8.27 

8.23 

8.19 

8.15 

8.11 

8.08 

5.75  Borate  +  4.25  HCl... 

8.17 

8.13 

8.09 

8.06 

8.02 

7.98 

7.95 

5.5  Borate  +4.5  HCl 

7.96 

7.93 

7.89 

7.86 

7.82 

7.79 

7.76 

5.25  Borate  +  4.75  HCl... 

7.64 

7.61 

7.58 

7.55 

7.52 

7.49 

7.47 

TABLE  39 

Sjrensen's  citrate—  HCl  mixtures 

Citrate:  21.008g  Crystn.  Citric  Acid  +  200  cc.  N  NaOH  per  1. 

HCl:  0.1  tf 

Temperature  18  °C. 

CITRATE 

HCl  ' 

pH 

CC. 

cc. 

0.0 

10.0 

1.038* 

1.0 

9.0 

1.173 

2.0 

8.0 

1.418 

3.0 

7.0 

1.925 

3.33 

6.67 

2.274 

4.0 

6.0 

2.972 

4.5 

5.5 

3.364 

4.75 

5.25 

3.529 

5.0 

5.0 

3.692 

5.5 

4.5 

3.948 

6.0 

4.0 

4.158 

7.0 

3.0 

4.447 

8.0 

2.0 

4.652 

9.0 

1.0 

4.830 

9.5 

0.5 

4.887 

10.0 

0.0 

4.958 

Note  inconsistency  with  table  35a. 


210  THE   DETERMINATION   OF   HYDROGEN   IONS 

TABLE  40 

Sfrensen's  glycocoll—HCl  mixtures 
Glycocoll:  0.1  M  Glycocoll  +  0.1  M  NaCl  per  1. 
HC1:0.1AT 

Temperature  18°C. 


GLTCOCOLL 

HCl 

PH 

CC. 

CC. 

0.0 

10.0 

1.038* 

1.0 

9.0 

1.146 

2.0 

8.0 

1.251 

•  3.0 

7.0 

1.419 

4.0 

6.0 

1.645 

5.0 

5.0 

1.932 

6.0 

4.0 

2.279 

7.0 

3.0 

2.607 

8.0 

2.0 

2.922 

9.0 

1.0 

3.341 

9.5 

0.5 

3.679 

Note  inconsistency  with  table  35a. 


TABLE  41 

S$rensen's  phosphate  mixtures 
Secondary:  11.876g  Na2  HPO4  •  2  H20  per  1. 
Primary:  9.078g  KH2P04  per  1. 
Temperature  18  °C. 


SECONDARY 

PRIMARY 

pH 

CC. 

CC. 

0.25 

9.75 

5.288 

0.5 

9.5 

5.589 

1.0 

9.0 

5.906 

2.0 

8.0 

6.239 

3.0 

7.0 

6.468 

4.0 

6.0 

6.643 

5.0 

5.0 

6.813 

6.0 

4.0 

6.979 

7.0 

3.0 

7.168 

8.0 

2.0 

7.381 

9.0 

1.0 

7.731 

9.5 

0.5 

8.043 

IX 


WALBUM  S    DATA 


211 


Boric  acid, 

Twenty  grams  of  boric  acid  should  go  completely  into  solution 
in  100  cc.  of  water  when  warmed  on  a  strongly  boiling  water  bath. 
This  solution  is  cooled  in  ice  water  and  the  nitrate  from  the  crys- 
tallized boric  acid  is  tested  as  follows.  It  should  give  no  tests  for 
chlorides  or  sulfates.  It  should  be  orange  to  methyl  orange.  A 
drop  of  N/10  HC1  added  to  5  cc.  should  make  the  filtrate  red  to 
methyl  orange.  Twenty  cubic  centimeters  of  the  nitrate  evap- 
orated in  platinum,  treated  with  about  10  grams  of  hydrofluoric 
acid  and  5  cc.  of  concentrated  sulfuric  acid  and  reevaporated, 
ignited  and  weighed,  should  yield  less  than  2  mgm.  when  corrected 
for  non-volatile  matter  in  the  HF. 

Tables  36-42  give  the  S0rensen  mixtures  with  the  corre- 
sponding pH  values.  Mixtures  whose  pH  values  are  considered 
by  S0rensen  to  be  too  uncertain  and  which  he  has  indicated  by 
brackets  are  omitted  from  these  tables.  The  third  decimal  of 
S0rensen's  tables  are  given  by  S0rensen  in  small  type. 

TABLE   42 

Sfirensen's  citrate — NaOH  mixtures 

(Walbum's  values) 

Citrate:  21.008g  Crystn.  Citric  Acid  +  200  cc.  N  NaOH  per  1. 
NaOH:  0.1  AT 


Temperature                               .   . 

10° 

20° 

30" 

40° 

50° 

60° 

70° 

10.0  Citrate  

4.93 

4.96 

5.00 

5.04 

5.07 

5.10 

5.14 

9.5  Citrate  +  0.5  NaOH.. 

4.99 

5.02 

5.06 

5.10 

5.13 

5.16 

5.20 

9.0  Citrate  +  1.0  NaOH.. 

5.08 

5.11 

5.15 

5.19 

5.22 

5.25 

5.29 

8.0  Citrate  +  2.0  NaOH.. 

5.27 

5.31 

5.35 

5.39 

5.42 

5.45 

5.49 

7.0  Citrate  +  3.0  NaOH.. 

5.53 

5.57 

5.60 

5.64 

5.67 

5.71 

5.75 

6.0  Citrate  +  4.0  NaOH.. 

5.94 

5.98 

6.01 

6.04 

6.08 

6.12 

6.15 

5.5  Citrate  +  4.5  NaOH.. 

6.30 

6.34 

6.37 

6.41 

6.44 

6.4* 

6.51 

5.25  Citrate  +  4.75  NaOH 

6.65 

6.69 

6.72 

6.76 

6.79 

6.83 

6.86 

WALBUM'S  DATA 

Walbum  (1920)  has  determined  the  pH  values  for  the  S0ren- 
sen  mixtures  at  temperatures  of  10°,  18°,  28°,  37°,  46°,  62°  and 
70°C.  and  has  interpolated  data  for  intervening  temperatures. 
He  finds  that  the  alteration  of  pH  with  temperature  is  for  the 
most  part  negligible  for  the  phosphate  mixtures,  the  glycocoll-HCl 
mixtures  and  the  citrate-HCl  mixtures.  In  his  tables  will  be 
found  S0rensen's  values  at  18°.  Tables  39,  40  and  41  are  taken 
from  S0rensen's  paper  of  1912. 


212 


THE    DETERMINATION    OF   HYDROGEN   IONS 


S0rensen  and  Walbum  used  the  Bjerrum  extrapolation  which 
results  in  making  the  pH  numbers  of  the  more  acid  solutions  less 
than  they  would  be  had  the  specifications  of  Chapter  XXIII  been 
used. 

HASTINGS  AND  SENDROY7S  DATA 

For  the  special  purposes  of  urine  and  blood  analysis  Hastings 
and  Sendroy  (1924)  required  smaller  increments  of  pH  than  are 
usually  provided  in  tables  of  buffer  systems.  They  also  desired 
standardized  values  at  20°  and  38°.  Table  43  contains  their  data. 


TABLE  43 

M/15  phosphate  mixtures  at  20°  and  88° 

(Hastings  and  Sendroy  (1924)) 
0.1  N  HC1  :  pH  1.08  used  as  standard  of  reference 


M/15 

Na2HPO4 

M/15 

KHzPO4 

nH  DETERMINED 
AT  20° 

pH  DETERMINED 
AT  38° 

cc. 

cc. 

49.6 

50.4 

6.809 

6.781 

52.5 

47.5 

6.862 

6.829 

55.4 

44.6 

6.909 

6.885 

58.2 

41.8 

6.958 

6.924 

61.1 

38.9 

7.005 

6.979 

63.9 

36.1 

7.057 

7.028 

66.6 

33.4 

7.103 

7.076 

69.2 

30.8 

7.154 

7.128 

72.0 

28.0 

7.212 

7.181 

74.4 

25.6 

7.261 

7.230 

76.8 

23.2 

7.313 

7.288 

78.9 

21.1 

7.364 

7.338 

80.8 

19.2 

7.412 

7.384 

82.5 

17.5 

7.462 

7.439 

84.1 

15.9 

7.504 

7.481 

85.7 

14.3 

7.561 

7.530 

87.0 

13.0 

7.610 

7.576 

88.2 

11.8 

7.655 

7.626 

89.4 

10.6 

7.705 

7.672 

90.5 

9.5 

7.754 

7.726 

91.5 

8.5 

7.806 

7.776 

92.3 

7.7 

7.848 

7.825 

93.2 

6.8 

7.909 

7.877 

93.8 

6.2 

7.948 

7.919 

94.7 

5.3 

8.018 

7.977 

IX 


PALITZSCH'S  STANDARDS 


213 


PALITZSCH'S  STANDARD  BUFFER  SOLUTIONS 

Palitzsch  (1922)  designed  his  standards  for  the  special  con- 
venience of  those  investigators  whose  interests  center  upon  the 
determination  of  the  pH  values  of  sea  waters. 

TABLE  44 

pH  values  of  borax-borate  mixtures  at  18°C.  and  "salt-effects"  for  phenol- 
phthalein  and  a-naphtholphthalein 

(Palitzsch  (1922)) 

Borax  solution:  19.108gramsNa2B4O7.10H2Oinl  1.  Boric  acid  solution: 
12.404  grams  H3BO3  +  2.925  grams  NaCl  in  1  1. 


STANDARD 

TRUE  pH  VALUES  OP  SEA  WATER  CONTAINING  S  PARTS  PER  1000 

SOLUTIONS 

SALINITY  AT  COLOR-MATCH  \VITH  STANDARD 

a 

0^ 

<O 
CO 

8 

o 

N 

oo 

S 

0 

CO 

-i< 

M 

^ 

0 

'!'§ 

W 

II 

n 

II 

it 

II 

n 

II 

II 

ii 

II 

n 

w 

w 

a 

CQ 

CQ 

CQ 

03 

CQ 

CQ 

CQ 

CQ 

02 

GQ 

CQ 

cc. 

cc. 

6.0 

4.0 

8.69 

8.48 

8.49 

8.50 

8.52 

8.54 

8.57 

8.59 

8.63 

8.66 

8.69 

8.72 

5.5 

4.5 

8.60 

8.39 

8.40 

8.41 

8.43 

8.45 

8.48 

8.50 

8.54 

8.57 

8.60 

8.63 

.S 

5.0 

5.0 

8.51 

8.30 

8.31 

8.32 

8.34 

8.36 

8.39 

8.41 

8.45 

8.48 

8.51 

8.54 

-s  3 

4.5 

5.5 

8.41 

8.20 

8.21 

8.22 

8.24 

8.26 

8.29 

8.31 

8.35 

8.38 

8.41 

8.44 

§£ 

4.0 

6.0 

8.31 

8.10 

8.11 

8.12 

8.14 

8.16 

8.19 

8.21 

8.25 

8.28 

8.31 

8.34 

0?  i-£3 

3.5 

6.5 

8.20 

7.99 

8.00 

8.01 

8.03 

8.05 

8.08 

8.10 

8.14 

8.17 

8.20 

8.23 

f2 

4.5 

55 

8.41 

8.19 

8.20 

8.21 

8.23 

8.25 

8.28 

8.32 

8.37 

8.40 

8.45 

8.48 

4.0 

6.0 

8.31 

8.09 

8.10 

8.11 

8.13 

8.15 

8.18 

8.22 

8.27 

8.30 

8.35 

8.38 

pj 

3.5 

6.5 

8.20 

7.98 

7.99 

8.00 

8.02 

8.04 

8.07 

8.11 

8.16 

8.19 

8.24 

8.27 

2 

3.0 

7.0 

8.08 

7.86 

7.87 

7.88 

7.90 

7.92 

7.95 

7.99 

8.04 

8.07 

8.12 

8.15 

i 

2.5 

7.5 

7.94 

7.72 

7.73 

7.74 

7.76 

7.78 

7.81 

7.85 

7.90 

7.93 

7.98 

8.01 

2.3 

7.7 

7.88 

7.66 

7.67 

7.68 

7.70 

7.72 

7.75 

7.79 

7.84 

7.87 

7.92 

7.95 

o 

2.0 

8.0 

7.78 

7.56 

7.57 

7.58 

7.60 

7.62 

7.65 

7.69 

7.74 

7.77 

7.82 

7.85 

1 

1.5 

8.5 

7.60 

7.38 

7.39 

7.40 

7.42 

7.44 

7.47 

7.51 

7.56 

7.59 

7.64 

7.67 

& 

1.0 

9.0 

7.36 

7.14 

7.15 

7.16 

7.18 

7.20 

7.23 

7.27 

7.32 

7.35 

7.40 

7.43 

0.6 

9.4 

7.09 

6.87 

6.88 

6.89 

6.91 

6.93 

6.96 

7.00 

7.05 

7.08 

7.13 

7.16 

S 

0.3 

9.7 

6.77 

6.55 

6.56 

6.57 

6.59 

6.61 

6.64 

6.68 

6.73 

6.76 

6.81 

6.84 

The  stock  solutions  are:  an  M/20  Borax  solution  containing 
19.108  grams9  Na2B407  10  H2O  in  1  liter;  and  an  M/5  Boric  acid, 
NaCl  solution  containing  12.404  grams9  H3B03  and  2.925  grams 
NaCl  in  1  liter. 


9  The  values  given  by  Palitzsch  were  calculated  upon  the  basis  of  11.0 
as  the  atomic  weight  of  boron.  Since  this  was  the  value  used,  the  new 
value  of  10.82  given  in  the  atomic  weight  table  of  International  Critical 


214 


THE   DETERMINATION    OF   HYDROGEN   IONS 


Since  the  buffer .  solutions  are  used  more  frequently  for  the 
study  of  sea  water,  table  44  includes  the  values  of  the  salt  effects 
of  sea  water  on  two  indicators.  For  salt  effects  in  general  see 
Chapters  VIII  and  XXV. 

MCILVAINE'S  STANDARD  BUFFER  SOLUTIONS 

Mcllvaine  (1921)  employs  a  mixture  of  0.2  M  disodium  phos- 
phate and  0.1  M  citric  acid.  The  citrate  system  functions  as  a 
buffer  in  the  region  of  pH  between  that  buffered  by  the  phosphoric 

TABLE  45 
Mcllvaine' s  standards 


pH 

0.2MNa2HPO4 

0.1  M  CITRIC  ACID 

pH 

0.2  M  Na2HPO4 

0.1  M  CITRIC  ACID 

cc. 

CC. 

cc. 

CC. 

2.2 

0.40 

19.60 

5.2 

10.72 

9.28 

2.4 

1.24 

18.76 

5.4 

11.15 

8.85 

2.6 

2.18 

17.82 

5.6 

11.60 

8.40 

2.8 

3.17 

16.83 

5.8 

12.09 

7.91 

3.0 

4.11 

15.89 

6.0 

12.63 

7.37 

3.2 

4.94 

15.06 

6.2 

13.22 

6.78 

3.4 

5.70 

14.30 

6.4 

13.85 

6.15 

3.6 

6.44 

13.56 

6.6 

14.55 

5.45 

3.8 

7.10 

12.90 

6.8 

15.45 

4.55 

4.0 

7.71 

12.29 

7.0 

16.47 

3.53 

4.2 

8.28 

11.72 

7.2 

17.39 

2.61 

4.4 

8.82 

11.18 

7.4 

18.17 

1.83 

4.6 

9.35 

10.65 

7.6 

18.73 

1.27 

4.8 

9.86 

10.14 

7.8 

19.15 

0.85 

5.0 

10.30 

9.70 

8.0 

19.45 

0.55 

acid-mono  phosphate  system  and  that  buffered  by  the  mono 
phosphate-diphosphate  system.  Consequently  the  range  pH 
2.2-pH  8.0  is  covered  by  mixtures  of  but  two  stock  solutions.  If 
samples  of  the  salt  and  acid  are  well  characterized  this  combina- 
tion is  convenient  for  many  purposes. 

Mcllvaine's  data  are  summarized  in  table  45. 


Tables  should  not  be  used  in  calculating  the  composition  of  the  specific 
solutions  given  by  Palitzsch. 


IX 


STANDARD    BUFFERS 


215 


OTHER   STANDARD    BUFFER    SOLUTIONS 

Walpole's  (1914)  data  on  acetate  solutions  were  included  in 
the  reconsideration  of  acetate  solutions  by  Cohn,  Heyroth  and 
Menkin  (1928).  Their  data  are  shown  in  tables  49A  and  49B. 

Atkins  and  Pantin  (1926)  have  described  some  buffer  solutions 
composed  of  boric  acid,  potassium  chloride  and  sodium  carbonate. 
Range:  7.44-11.0. 

Prideaux  and  Ward  (1924)  propose  a  buffer  mixture  in  which 
is  found  phenyl  acetic  acid  (pK  =  "4.27"),  phosphoric  acid 

TABLE  46 

Alkaline  soda-borax  buffer  solutions  of  Kolthoff  and  Vlesschhouwer 

(1927}  at  18° 

See  page  477  for  note  on  standard  of  reference.  Solution  A:  5.30  grams 
Na2CO3  per  liter.  Solution  B:  19.10  grams  Na2B4O7-10  H2O  per  liter. 


MIXTURE 

PH 

Cubic  centimeter  A 

Cubic  centimeter  B 

0 

100 

9.2 

35.7 

64.3 

9.4 

55.5 

44.5 

9.6 

66.7 

33.3 

9.8 

75.4 

24.6 

10.0 

82.15 

17.85 

10.2 

86.9 

13.1 

10.4 

91.5 

8.5 

10.6 

94.75 

5.25 

10.8 

97.3 

2.7 

11.0 

(pK  values:  "1.96,  6.85,  11.52")  and  boric  acid  (pK  =  "9.22"). 
The  object  of  this  combination  is  to  provide  a  "universal  buffer" 
(cf.  table  45).  Acree  and  his  co workers  have  worked  on  the  same 
idea.  The  principles  concerned  in  overlapping  the  buffer  effects 
of  different  systems  are  discussed  in  systematic  form  by  Van 
Slyke  (1922). 

Kolthoff  and  Vleeschhouwer  (1926)  have  published  data  on 
mixtures  of  mono  potassium  citrate  with  HC1,  NaOH,  and  with 
citric  acid  and  borax.  See  corrections  by  Kolthoff  and  Vleesch- 
houwer (1927). 


216  THE    DETERMINATION   OF   HYDROGEN   IONS 

Kolthoff  (1925)  has  described  buffer  mixtures  of  succinic  acid 
and  borax  and  of  acid  potassium  phosphate  and  borax. 

Avery,  Mellon  and  Acree  (1921)  describe  buffer  mixtures  the 
salts  of  which  are  put  up  in  tablet  form.  If  properly  prepared 
and  preserved  these  might  be  especially  useful  for  field  work  and 
for  the  occasional  rough  measurement. 

The  following  tables  of  Kolthoff  and  Vleeschhouwer  (1927)  give 
pH  values  for  alkaline  regions  of  pH.  The  standard  of  calcula- 
tion was 

pH  =  2.038  for  0.01  N  HC1  +  0.09  N  KC1  at  18°. 

TABLE  47 

Alkaline  phosphate  buffer  solutions  of  Kolthoff  and  Vleeschhouwer 

(1927}  at  18° 

See  page  477  for  note  on  standard  of  reference.  Solution  A:  17.81  grams 
Na2HFO4-2  H20  per  liter.  Solution  B:  0.1  N  NaOH. 


MIXTURE 

pH 

25  cc.  A  H 

h    4.13  cc.  B,  dilute  to  50  cc. 

11.00 

25  cc.  A  H 

h    6.00  cc.  B,  dilute  to  50  cc. 

11.20 

25  cc.  A  H 

-    8.67  cc.  B,  dilute  to  50  cc. 

11.40 

25  cc.  A  H 

h  12.25  cc.  B,  dilute  to  50  cc. 

11.60 

25  cc.  A  H 

h  16.65  cc.  B,  dilute  to  50  cc. 

11.80 

25  cc.  A  H 

h  21.60  cc.  B,  dilute  to  50  cc. 

12.00 

CORN'S   SYSTEM   OF   BUFFER    STANDARDS 

An  excellent  innovation  in  the  construction  of  buffer  standards 
has  been  introduced  by  Cohn  (1927)  and  Cohn,  Heyroth  and 
Menkin  (1928). 

As  ordinarily  prepared,  buffer  solutions  vary  appreciably  in 
ionic  strength.  The  ionic  strength  is  determined  by  multiplying 
the  concentration  of  each  ion  by  the  square  of  that  ion's  valence 
number,  summing  all  such  products  and  dividing  by  two.  See 
page  490.  As  a  consequence  of  the  variation  in  ionic  strength  the 
corrections  to  a  common  basis  of  reference,  which  may  be  calcu- 
lated by  the  Debye-Hiickel  equation,  vary.  (The  Debye- 


IX 


COHN  S   SYSTEM 


217 


Hiickel  equation  is  discussed  in  Chapter  XXV.)  Furthermore 
there  are  occasions  to  employ  buffers  of  different  known  ionic 
strength. 

TABLE  48A 

pK'  values  of  phosphate  system 
(After  Cohn  (1927)) 
Temperature  18°C. 


TOTAL 
PHOS- 
PHATE 

MOLE  FRACTION  OF  TOTAL  PHOSPHATE  AS  K2HPO4 

0.1 

0.2 

0.3 

0.4 

0.5 

0.6 

0.7 

0.8 

0.9 

M 

0.1 

6.788 

6.781 

6.774 

6.769 

6.765 

6.760 

6.755 

6.753 

6.752 

0.2 

6.676 

6.679 

6.679 

6.682 

6.685 

6.687 

6.688 

6.692 

6.698 

0.3 

6.596 

6.608 

6.616 

6.631 

6.640 

6.651 

6.658 

6.668 

6.682 

0.4 

6.530 

6.553 

6.570 

6.593 

6.611 

6.628 

6.642 

6.659 

6.681 

0.5 

6.472 

6.505 

6.531 

6.564 

6.590 

6.615 

6.634 

6.659 

6.688 

0.6 

6.420 

6.463 

6.498 

6.540 

6.574 

6.606 

6.632 

6.664 

6.702 

0.8 

6.325 

6.390 

6.441 

6.503 

6.553 

6.6CO 

6.639 

6.684 

6.737 

1.0 

6.238 

6.324 

6.393 

6.474 

6.540 

6.602 

6.653 

6.712 

6.781 

1.2 

6.157 

6.265 

6.351 

6.450 

6.533 

6.609 

6.672 

6.746 

6.830 

Cohn  finds  that  the  pH  values  of  phosphate  buffer  solutions 
may  be  calculated  by  means  of  the  formula. 


In  place  of  pK  -f  log  —  may  be  substituted  pK',  the  values  of 

which  are  found  in  tables  48A  and  48B. 

For  example:  a  mixture  making  0.1  M  KH2PO4  and  0.3  M 
K2HP04  would  be  0.4  M  with  respect  to  total  phosphate  and  the 

0  3 
mole  fraction  of  total  phosphate  as  K^HPCX  would  be  ^-r  =  0.75. 


0.4 


Interpolation  in  table  48A  shows  pK'  =  6.651. 

0.3 


pH  =  6.651  +  log 


0.1 


7.128 


218 


THE    DETERMINATION   OF   HYDROGEN   IONS 


TABLE  48B 

pK'  values  of  phosphate  system 
(After  Cohn  (1927)) 
Temperature  18  °C. 


IONIC 
STRENGTH 
OF  PHOS- 
PHATE 
SOLUTION 

MOLE  FRACTION  OF  TOTAL  PHOSPHATE  AS  KzHPO4 

0.1 

0.2 

0.3 

0.4 

0.5 

0.6 

0.7 

0.8 

0.9 

n 

0.1 

6.813 

6.824 

6.831 

6.837 

6.841 

6.844 

6.846 

6.848 

6.850 

0.2 

6.709 

6.731 

6.745 

6.757 

6.765 

6.771 

6.775 

6.779 

6.783 

0.3 

6.634 

6.667 

6.688 

6.706 

6.718 

6.727 

6.733 

6.739 

6.745 

•0.4 

6.573 

6.617 

6.645 

6.669 

6.685 

6.697 

6.705 

6.713 

6.721 

0.5 

6.520 

6.575 

6.610 

6.640 

6.660 

6.675 

6.685 

6.695 

6.705 

0.6 

6.472 

6.538 

6.580 

6.616 

6.640 

6.658 

6.670 

6.682 

6.694 

0.7 

6.428 

6.505 

6.554 

6.596 

6.624 

6.645 

6.659 

6.673 

6.687 

0.8 

6.387 

6.475 

6.531 

6.579 

6.611 

6.635 

6.651 

6.667 

6.683 

0.9 

6.348 

6.447 

6.510 

6.564 

6.600 

6.627 

6.645 

6.663 

6.681 

1.0 

6.310 

6.420 

6.490 

6.550 

6.590 

6.620 

6.640 

6.660 

6.680 

1.1 

6.274 

6.395 

6.472 

6.538 

6.582 

6.615 

6.637 

6.659 

6.681 

1.2 

6.238 

6.370 

6.454 

6.526 

6.574 

6.610 

6.634 

6.658 

6.682 

1.3 

6.204 

6.347 

6.438 

6.516 

6.568 

6.607 

6.633 

6.659 

6.685 

1.4 

6.170 

6.324 

6.422 

6.506 

6.562 

6.604 

6.632 

6.660 

6.688 

1.5 

6.137 

6.302 

6.407 

6.497 

6.557 

6.602 

6.632 

6.662 

6.692 

1.6 

6.281 

6.393 

6.489 

6.553 

6.601 

6.633 

6.665 

6.697 

1.7 

6.260 

6.379 

6.481 

6.549 

6.600 

6.634 

6.668 

6.702 

1.8 

6.366 

6.474 

6.546 

6.600 

6.636 

6.672 

6.708 

1.9 

6.353 

6.467 

6.543 

6.600 

6.638 

6.676 

6.714 

2.0 

6.460 

6.540 

6.600 

6.640 

6.680 

6.720 

2.1 

6.454 

6.538 

6.601 

6.643 

6.685 

6.727 

2.2 

6.448 

6.536 

6.602 

6.646 

6.690 

6.734 

2.3 

6.534 

6.603 

6.649 

6.695 

6.741 

2.4 

6.533 

6.605 

6.653 

6.701 

6.749 

2.5 

6.607 

6.657 

6.707 

6.757 

2.6 

6.608 

6.660 

6.712 

6.764 

2.7 

6.611 

6.665 

6.719 

6.773 

2.8 

6.669 

6.725 

6.781 

2.9 

6.673 

6.731 

6.789 

3.0 

6.738 

6.798 

TABLE  49A 

Interpolated  values  of  —log  7  for  mixtures  of  acetic  acid  and  sodium  acetate 

(After  Cohn,  Heyroth  and  Menkin  (1928)) 

Temperature  18°C. 


CONCEN- 
TRATION 
OF  TOTAL 
ACETATE 

MOLE  FRACTION  OP  TOTAL  ACETATE  AS  CHaCOONa 

0.1 

0.2 

0.3 

0.4 

0.5 

0.6 

0.7 

0.8 

0.9 

-log  y 

M 

0.05 

0.034 

0.045 

0.053 

0.060 

0.064 

0.069 

0.071 

0.075 

0.073 

0.10 

0.047 

0.062 

0.071 

0.078 

0.084 

0.088 

0.091 

0.093 

0.089 

0.10 

0.065 

0.082 

0.092 

0.099 

0.105 

0.108 

0.109 

0.109 

0.101 

0.40 

0.088 

0.106 

0.115 

0.119 

0.123 

0.123 

0.120 

0.118 

0.100 

0.60 

0.105 

0.120 

0.127 

0.130 

0.129 

0.125 

0.119 

0.112 

0.089 

0.80 

0.118 

0.130 

0.136 

0.134 

0.130 

0.123 

0.112 

0.102 

0.072 

1.00 

0.129 

0.139 

0.140 

0.134 

0.127 

0.117 

0.102 

0.088 

0.052 

1.20 

0.138 

0.144 

0.141 

0.133 

0.123 

0.109 

0.090 

0.071 

0.030 

1.40 

0.146 

0.148 

0.143 

0.130 

0.116 

0.099 

0.075 

0.054 

0.007 

1.60 

0.153 

0.152 

0.142 

0.126 

0.108 

0.086 

0.061 

0.035 

-0.016 

1.80 

0.159 

0.153 

0.142 

0.121 

0.100 

0.075 

0.044 

0.016 

-0.040 

2.00 

0.166 

0.155 

0.139 

0.115 

0.090 

0.061 

0.028 

-0.005 

-0.065 

TABLE  49B 

Interpolated  values  of  —log  7  for  mixtures  of  acetic  acid  and  sodium  acetate 
(After  Cohn,  Heyroth  and  Menkin  (1928)) 
Temperature  18°C. 


Wl'KJllJNUTH. 
OF 
ACETATE 
SOLUTION 

0.1 

0.-2 

0.3 

0.4 

0.5 

0.6 

0.7 

0.8 

0.9 

-log  7 

0.02 

0.065 

0.061 

0.061 

0.060 

0.059 

0.059 

0.058 

0.058 

0.056 

0.04 

0.088 

0.082 

0.080 

0.078 

0.077 

0.077 

0.075 

0.075 

0.071 

0.06 

0.105 

0.095 

0.092 

0.090 

0.089 

0.088 

0.086 

0.085 

0.080 

0.08 

0.118 

0.106 

0.102 

0.099 

0.098 

0.096 

0.094 

0.093 

0.087 

0.10 

0.129 

0.114 

0.110 

0.106 

0.105 

0.103 

0.101 

0.099 

0.092 

0.12 

0.138 

0.120 

0.115 

0.112 

0.110 

0.108 

0.105 

0.103 

0.095 

0.14 

0.146 

0.126 

0.120 

0.116 

0.114 

0.112 

0.109 

0.107 

0.098 

0.16 

0.153 

0.130 

0.124 

0.119 

0.117 

0.114 

0.111 

0.109 

0.099 

0.18 

0.159 

0.134 

0.127 

0.123 

0.120 

0.117 

0.114 

0.111 

0.101 

0.20 

0.166 

0.139 

0.131 

0.126 

0.123 

0.120 

0.116 

0.114 

0.102 

0.40 

0.202 

0.155 

0.142 

0.134 

0.130 

0.125 

0.120 

0.116 

0.098 

0.60 

0.155 

0.139 

0.128 

0.123 

0.117 

0.110 

0.105 

0.083 

0.80 

0.147 

0.127 

0.115 

0.108 

0.101 

0.093 

0.088 

0.063 

1.00 

0.090 

0.083 

0.074 

0.067 

0.040 

1.20 

0.045 

0.015 

1.40 

0.021 

-0.011 

1.60 

-0.005 

-0.038 

1.80 

-0.065 

219 


220  THE    DETERMINATION   OF   HYDROGEN   IONS 

In  table  48B  are  values  of  pK'  at  different  ionic  strengths.     In 

the  above  example  the  ionic  strength  is  given  by  L      — — 

2 

=  1.0.     Interpolation  in  table  48B  gives  pK'  =  6.650. 
For  acetate  systems  there  may  be  used  the  equation: 

TT  [Acetate] 

pH  =  4.73  +  log  rf-        —!—  +  log  7 
[Acetic  acid] 

if  the  S0rensen  value  of  the  "0.1  N  calomel  half-cell"  is  used;  or 

pH  =  4.77  +  log  [A[A?etate],,  +  log  7 
[Acetic  acid] 

if  the  value  of  the  "0.1  N  calomel  half-cell"  corresponding  to 
0.3357  at  18°  is  used. 
In  either  case  values  of  log  7  are  given  in  tables  49 A  and  49B. 


CHAPTER  X 
OUTLINE  OF  THE  "HYDROGEN  ELECTRODE"  METHOD 

Let  a  noble  metal,  such  as  gold  or  platinum,  be  coated  with 
platinum  black  or  palladium  black.  Let  this  metal  be  placed 
in  a  solution  containing  hydrogen  ions,  under  a  definite  partial 
pressure  of  hydrogen. 

This  combination  of  metal,  hydrogen  and  solution  constitutes 
a  hydrogen  half-cell,  commonly  called  a  "hydrogen  electrode. " 

When  two  such  half-cells  are  placed  in  liquid  junction,  as 
illustrated  in  figure  36,  a  complete  cell  is  formed.  Its  metallic 
terminals  will  exhibit  an  elect rical^o^^tial  difference  at  E. 
This  can  be  measured  by  impopng^an  electromotive  force  of 
opposite  direction  and  of  such  magnitude  as  to  prevent  current 
flowing  through  the  cell  in  either  direction.  This,  the  potentio- 
metric  method,  is  described  in  Chapter  XVI. 

It  will  be  convenient  to  regard  the  potential  difference  at  E, 
between  the  metals,  as  the  algebraic  sum  of  potential  jumps  at 
the  interface  between  each  metal  and  the  contiguous  solution  and 
of  a  potential  jump  at  the  liquid  junction  (L  of  figure  36). 

There  is  no  general  and  at  the  same  time  simple  way  in  which 
this  liquid  junction  potential  can  be  related  to  the  composition 
of  the  two  solutions.  However,  there  is  good  reason  to  believe 
that  the  interposition  of  a  saturated  solution  of  potassium  chloride 
will  greatly  reduce  the  magnitude  of  this  liquid  junction  potential. 
For  present  purposes  we  shall  make  the  bold  assumption  that  this 
device  reduces  the  liquid  junction  potential  to  a  small  constant 
value.  Indeed  we  shall  regard  this  value  to  be  so  small  as  to 
be  negligible  in  the  first  consideration. 

With  this  understood,  we  have  left  for  our  consideration  the 
two  potential-jumps  at  the  metal-solution  interfaces.  Suchjin 
interface  is  called  an  electrode^-With  the  understanding  that  a 
potential-jump  or  potential  difference  is  meant,  we  may  speak  of 
an  electrode  potential. 

An  electrode  potential  cannot  be  used  for  our  present  purposes 
unless  it  be  obtained  under  conditions  which  we  call  equilibrium 

221 


222 


THE    DETERMINATION    OF   HYDROGEN   IONS 


conditions.     These  are  discussed  in  later  chapters.     Here  we  shall 
assume  that  they  exist. 

There  is  no  sure  way  of  measuring  the  value  of  the  potential- 
jump  at  any  single  electrode.  Therefore,  an  arbitrary  standard 
hydrogen  half-cell  is  selected  and  its  electrode  potential  is  called 
zero.  When  this  is  done  the  potential  of  the  whole  cell  is  allo- 
cated to  the  half-cell  which  is  joined  to  the  standard. 


FIG.  36.  DIAGRAM  OF  Two  HYDROGEN  HALF-CELLS  IN  LIQUID 
JUNCTION  AT  L 

For  historical  reasons  the  nature  of  this  arbitrary  standard 
hydrogen  half-cell  is  defined  in  a  manner  which  it  is  very  difficult 
to  conform  to  experimentally.  We  shall  dodge  the  discussion  of 
this  standard  for  the  present.  We  shall  simply  refer  to  it  as  the 
"normal  hydrogen  half-cell"  and  shall  assume  that  someone  has 
constructed  it  and  has  instituted  a  series  of  direct  comparisons 
with  other  hydrogen  half-cells. 

Suppose,  for  instance,  that  a  solution  tenth  molar  with  respect 
to  acetic  acid  and  tenth  molar  with  respect  to  sodium  acetate  has 
been  used  in  a  hydrogen  half-cell  with  one  atmosphere  of  hydro- 


OUTLINE    OF    HYDROGEN    ELECTRODE 


223 


gen  and  in  conjunction  with  the  "normal  hydrogen  half-cell." 
It  has  been  found  that  at  18°C.  the  E.M.F.  of  this  cell  is  0.267 
volt  and~that  the  platinum  on  the  acetate  side  is  negative  to  the 
platinum  of  the  "normal  hydrogen  half-cell."  If  we  agree  to 
call  the  potential  of  the  normal  hydrogen  electrode  zero  and  to 
give  the  sign  of  the  metal  to  the  potential  of  the  other  electrode 
we  may  speak  of  the  potential  on  the  acetate  side  as  —0.267 
volt.  Potentials  so  referred  to  the  normal  hydrogen  half-cell 
are  indicated  by  the  subscript  h  in  EH. 

The  hydrogen  half-cell  with  the  "standard  acetate"  solution 
can  now  be  used  as  a  secondary  working  standard.  Suppose 
solutions  a,  b  and  c  are  to  be  studied.  They  are  placed  in  turn 

at  position  X  in  a  cell  described  as  follows. 

— i 


Ft,  H2(l  atmos.) 


X 


KC1 


0.1  N  Acetic  acid 


H2,  (1  atmos.) 


A    B 


0.1M  Na  Acetate 
C  D 


Pt 


This  reads:  Platinized  platinum  under  one  atmosphere  pressure 
of  hydrogen  is  placed  in  contact  with  solution  X.  The  latter  is 
separated  by  a  saturated  solution  of  KC1  from  the  mixture  of 
0.1  N  acetic  acid  and  0.1  M  sodium  acetate.  In  the  latter  solu- 
tion is  a  platinized  platinum  electrode  under  one  atmosphere  of 
hydrogen.  Potential-jumps  occur  at  A,  B,  C  and  D. 

We  have  agreed  to  neglect  the  potential  differences  at  B  and  C. 
We  have  agreed  to  accept  the  value  Eh  =  —0.267  at  18°  for  the 
potential  at  D. 

When  solutions  a,  b  and  c  are  in  turn  placed  at  X  the  electro- 
motive forces  are,  for  example,  those  indicated  in  the  last  column 
below. 


E.M.F.  of  cell  for     "Potential' 
standardization 
(standard  acetate)  Eh 


"Electrode' 


Cell     E.M.F.  of  Cell 


0.267 


f 

-  0.156 

L   -  0.267     " 

-  0.467 

-  0.768 


"normal  hydrogen" 


standard  cell 
b 
c 


:.] 


=i-i 
-I 


0.111 
0.200 
0.501 


224         THE  DETERMINATION  OF  HYDROGEN  IONS 

It  is  obviously  necessary  to  determine  whether  the  platinum 
of  electrode  a,  for  example,  is  positive  or  negative  relative 
to  the  platinum  in  the  "standard  acetate."  It  is  then  a  simple 
matter  to  arrange  the  "potentials"  "Eh  relative  to  that  of  the 
normal  hydrogen  electrode  in  the  correct  order.  See  figure  40, 
page  259. 

It  is  obvious  that,  so  far  as  a  comparison  between  two  solutions 
is  concerned,  the  selection  of  a  standard  is  of  no  consequence. 
The  difference  between  electrodes  b  and  c  is  0.301  volts  with 
b  positive  to  c  and  this  difference  remains  whatever  the  ul- 
timate standard  of  reference.  However,  if  we  are  to  agree  upon 
the  meaning  of  numerical  values  assigned  to  single  electrodes, 
agreement  on  a  standard  is  necessary. 

Each  of  the  "potentials"  in  the  above  set  of  examples  may  be 
considered  characteristic  of  the  solution.  As  such  these  poten- 
tials would  suffice  for  many  correlations  with  the  degree  to  which 
the  property  of  a  substance  placed  in  these  solutions  appears. 

For  historical  reasons  these  potentials  themselves  are  not  used. 
Instead  any  such  potential,  Eh,  is  divided  by  -0.000,198,322  T 
where  T  is  the  absolute  temperature  (273.1  +  t°C.  =  T).  Values 
for  this  expression  at  various  temperatures  centigrade  are  found 
in  appendix  C,  page  674. 

The  result  of  this  division  is  called  pH. 

E 
-0.000,198,322  T  "  pK 

Thus  for  the  potentials  given  in  the  above  series  we  have  the 
following  values  of  pH. 


POTENTIAL  AT  18°C. 

Eh 

pH 

0 

0 

-0.156 

2.70 

-0.267 

4.62 

-0.467 

8.09 

-0.768 

13.30 

USE   OF   CALOMEL  HALF-CELLS 

In  the  previous  section  cells  composed  of  two  hydrogen  half- 
cells  were  considered.     It  is  usually  more  convenient  to  use  as  a 


X  OUTLINE    OF    FORMULAS  225 

working,  or  comparison,  half-cell  a  so-called  calomel  half-cell 
Such  half-cells  are  described  in  Chapter  XV.  The  types  in 
widest  use  are  the  half-cell  in  which  0.1  N  KC1  solution  is  used 
and  the  half-cell  in  which  saturated  KC1  is  used.  The  latter  is 
the  more  convenient;  the  former  the  better  standardized.  In 
each  instance  pure  mercury  is  the  metal  of  the  electrode  and  pure 
calomel  (Hg2Cl2,  usually  written  HgCl)  is  present  in  solid  form. 
The  beginner  is  advised  to  use  the  following  cell 


Pt,  H2  (1  atmosphere) 


Solution  X 


KC1 

(sat.) 


KC1 ,  HgCl 

(sat.) 


Hg 


B  C 


Hydrogen  half-cell  Connect-      "Saturated 

ing  calomel 

solution       half-cell" 

In  the  first  instance  solution  X  is  made  one  of  the  standards 
described  in  Chapter  XXIV.  For  convenience  certain  values 
assigned  to  A  are  given  on  page  672. 

With  these  values  at  A  accepted,  a  measurement  of  the  E.M.F. 
of  the  cell  permits  the  calculation  of  the  sum  of  the  potentials 
at  B  and  C.  This  is  to  be  used  as  the  working  standard  and  the 
potential  at  B  is  to  be  considered  not  to  vary  as  solution  X  is 
changed.  Then  as  solution  X  is  changed  the  value  at  A  can  be 
calculated  from  the  potential  of  the  whole  cell  and  the  standardized 
value  of  B  -f  C.  A  standardized  value  for  pH  is  then  calculated 
as  follows. 

E.M.F.  of  cell— Potential  (B  +  C)  = 
0.000,198,322  T 

For  example:  The  observed  E.M.F.  is  0.648  volt.  Potential 
B  +  C  has  been  found  by  the  process  of  standardization  to  be 
0.246  volt.  The  temperature  is  25°C.  (25°  +  273°.l  =  298°.l 
=  T).  Hence 


226 


THE    DETERMINATION    OF   HYDROGEN    IONS 


OUTLINE    OF   PROCEDURES 


Although  it  is  impracticable  to  describe  at  this  point  the  details 
of  a  complete  system  for  the  measurement  of  hydrogen  ion  con- 
centration, an  outline  may  be  given  with  which  to  coordinate 
the  main  features  as  they  will  develop  in  subsequent  chapters. 


FIG.  37.  A  SIMPLE  ARRANGEMENT  FOR  POTENTIOMETRIC  MEASUREMENT 

OF  pH 

Figure  37  illustrates  a  simple  system  which  may  be  put  together 
from  inexpensive  material.  It  is  not  a  system  which  can  be 
recommended  for  even  rough  measurements,  but  it  will  work  and 
is  well  adapted  to  show  the  principles  concerned. 

Hydrogen,  prepared  by  one  of  the  methods  described  in  Chapter 


X  USE   OF  POTENTIOMETER  227 

XVII  passes  into  the  hydrogen  electrode  vessel  A  and  escapes  at  B. 
Connected  with  this  vessel  by  the  siphon  S,  filled  with  a  saturated 
KC1  solution,  is  the  calomel  electrode  M  consisting  of  a  layer  of 
mercury  covered  by  calomel  under  a  saturated  solution  of  KC1. 
The  hydrogen  electrode  H  consists  of  a  piece  of  platinum  foil 
covered  with  platinum  black.  It  is  welded  to  a  platinum  wire 
which  is  sealed  into  the  glass  tube. 

Hydrogen  is  bubbled  through  the  solution  in  A  until  solution 
and  electrode  are  thoroughly  saturated  with  the  gas. 

The '  difference  between  the  potential  at  the  mercury-calomel 
junction  and  the  potential  at  the  hydrogen  electrode  is  now 
measured  by  means  of  a  potentiometer.  A  simple  form  of  this 
is  illustrated. 

A  storage  battery  P  sends  current  through  the  rheostat  R,  the 
calibrated  resistance- wire  K-L  and  the  fixed  resistance  L-F.  By 
properly  setting  the  switch  O  a  Weston  cell  W  having  an  electro- 
motive force  of  1.018  volts  can  be  connected  to  K  and  F,  the 
-f  pole  of  the  Weston  cell  being  connected  to  the  +  side  of  the 
battery  current.  The  rheostat  R  is  now  varied  until  there  is 
no  deflection  of  the  galvanometer  or  electrometer  E.  Then  the 
difference  of  potential  between  K  and  F  is  equal  to  the  E.M.F. 
of  the  Weston  cell.  The  resistance  K-L  is  such  that  when  the 
above  adjustment  is  made  the  difference  of  potential  between  K 
and  L  is  one  volt.  A  scale  properly  divided  is  placed  beside  the 
wire  K-L.  When  the  sliding  contact  X  is  at  K  there  will  be  no 
difference  of  potential  between  X  and  K.  When  X  is  at  L  the 
difference  of  potential  between  X  and  K  will  be  one  volt.  When 
X  is  at  some  intermediate  position  the  difference  of  potential 
between  X  and  K  will  be  that  fraction  of  one  volt  indicated  by 
the  scale. 

After  the  potentiometer  is  adjusted  by  means  of  the  standard 
Weston  cell,  the  switch  O  is  thrown  to  connect  the  calomel 
electrode-hydrogen  electrode  system  and  X  is  slid  in  one 
direction  or  the  other  until  the  galvanometer  E  shows  no  de- 
flection. Then  the  difference  of  potential  between  X  and  K  is 
equal  to  the  difference  of  potential  between  mercury  and  platinum. 

The  temperature  is  read  and  the  data  put  into  the  equation 
given  above. 

Neither  measured  E.  M.  F.  nor  Weston  cell  should  be  left  in 


228  THE    DETEKMINATION    OF   HYDROGEN   IONS 

circuit  for  more  than  an  instant.  While  switch  O  can  be  used 
for  this  momentary  completion  of  circuit,  it  is  more  convenient 
to  use  a  telegraph  key  in  the  galvanometer  circuit. 

If  care  be  taken  to  maintain  the  hydrogen  at  barometric  pres- 
sure, the  effects  of  minor  variations  of  the  barometer  from  sea 
level  conditions  and  of  displacement  of  hydrogen  by  water  vapor 
may  be  neglected  in  rough  measurements.  A  discussion  of  the 
barometric  pressure  is  found  in  Chapter  XII. 

In  all  cases  where  two  unlike  solutions  are  joined  as  in  figure  36, 
there  will  develop  a  local  potential  difference  at  the  liquid  junction. 
To  deal  with  this  precisely  is  the  most  difficult  of  the  problems 
encountered.  The  subject  is  discussed  in  Chapter  XIII.  In 
very  many  instances,  however,  the  employment  of  a  saturated 
solution  of  KC1,  as  is  specified  in  the  apparatus  illustrated  in 
figure  37,  reduces  the  liquid  junction  potential  difference  to  an 
order  of  magnitude  which  is  negligible. 

Since  variations  may  occur  in  the  calomel  electrode  or  in  the 
reliability  of  the  hydrogen  electrode  it  is  well  to  check  the  system 
frequently  by  means  of  measurements  made  with  the  standard 
solutions  previously  mentioned. 

In  the  use  of  the  potentiometer  the  elementary  principles 
must  be  understood  lest  standard  cells  or  half-cells  be  injured 
or  quite  erroneous  results  obtained.  Therefore,  these  principles 
are  discussed  in  Chapter  XVI. 

Were  it  not  for  the  fact  that  several  experimenters  have  tried 
to  make  hydrogen  electrode  measurements  by  use  of  conductivity 
instruments,  it  would  seem  hardly  necessary  to  say  that  the 
measurement  of  conductivity  or  its  reciprocal,  resistance,  is  a 
procedure  entirely  different  from  the  measurement  of  electro- 
motive forces  or  potential  differences.1 

If  the  beginner  is  puzzled  by  the  array  of  apparatus  described 
in  the  following  pages  he  may  welcome  the  following  suggestion. 
The  main  outline  of  a  problem  can  often  be  defined  by  the  use 
of  the  immersion  electrode  used  in  connection  with  the  saturated 
calomel  half-cell  and  by  using  as  a  potentiometer  the  voltmeter 

1  The  surprising  number  of  cases  in  which  this  confusion  has  been  re- 
vealed may  be  an  interesting  psychological  result  of  the  emphasis  hitherto 
placed  upon  conductivity  measurements,  sometimes  to  the  entire  exclusion 
of  any  reference  to  potentiometric  measurements. 


X  DISCUSSION   OF  APPARATUS  229 

system.  This  set  of  apparatus  is  illustrated  on  page  325.  *  It 
not  infrequently  happens  that  the  outlining  of  a  problem  with 
this  or  a  comparable  system  will  indicate  that  further  refinement 
would  be  useless  or  confusing.  It  also  frequently  happens  that 
the  errors  suggest  phantom  relations  or  obscure  existing  relations 
of  importance.  It  is,  therefore,  advisable  whenever  possible  to 
keep  the  accuracy  of  measurements  just  ahead  of  the  immediate 
demands.  To  meet  this  requirement  the  investigator  must  gain 
the  ability  to  judge  for  himself  the  apparatus  required.  It  is  to 
contribute  toward  this  and  the  pleasure  of  work  that  the  follow- 
ing chapters  are  written  in  some  detail.  If  the  reader  does  not 
care  to  work  out  the  peculiar  requirements  of  his  problem  he  is 
advised,  after  having  outlined  his  problem  with  the  system  men- 
tioned above,  to  obtain  a  reliable  potentiometer  of  standard,  not 
unique,  design  and  to  use  the  system  illustrated  on  page  295. 
In  the  first  instance  accurate  temperature  control  is  unnecessary. 
In  the  second  instance  it  is  advisable  if  for  no  other  purpose  than 
the  avoidance  of  vexatious  uncertainties. 


CHAPTER  XI 
ON  CHANGES  OF  FREE-ENERGY 

.  ...  in  our  measurements  of  nature  the  rules  of  operation  are 
in  our  control  to  modify  as  we  see  fit,  and  we  would  certainly  be 
foolish  if  we  did  not  modify  them  to  our  advantage  according  to 
the  particular  kind  of  physical  system  or  problem  with  which 
we  are  dealing. — BRIDGMAN. 

From  two  points  of  view  it  is  advisable  for  those  who  undertake 
the  determination  of  hydrions  to  review  those  aspects  of  thermo- 
dynamics which  are  of  more  immediate  importance  to  the  subject. 
In  the  first  place,  the  equations  which  are  used  are  fundamentally 
of  thermodynamic  origin;  and,  if  they  are  to  be  applied  intelli- 
gently, their  meaning  should  be  appreciated.  In  the  second  place 
it  will  be  of  interest  to  see  how  a  consideration  of  energy  changes 
and  means  of  their  measurement  may  illuminate  a  rather  gloomy 
aspect  of  our  previous  treatment  of  equilibria.  At  the  very  origin 
of  the  derivation  of  the  equilibrium  equation  which  we  have  been 
using,  the  statement  was  made  that  the  equilibrium  constant 
could  remain  a  constant  only  while  the  environment  remained 
constant.  Strictly  this  is,  of  course,  an  impractical  condition. 
Every  change  in  the  concentration  of  the  reacting  species,  as  well 
as  every  change  in  the  amount  of  extraneous  matter  present,  is 
a  change  of  the  environment.  We  were  content  to  ignore  this 
while  surveying  the  larger  features  of  the  subject.  We  were 
content  to  ignore  it  because  a  judicious  selection  of  cases  made  it 
appear  that  our  neglect  is  of  secondary  importance.  But  even 
then  we  soon  encountered  aggravating  discrepancies.  The  equi- 
librium constant  for  acetate  solutions  of  only  moderately  varying 
composition  appeared  to  vary  appreciably.  The  equilibrium  of 
an  indicator  system  seemed  to  change  with  addition  of  neutral 
salts.  We  may  well  believe  that  part  of  each  discrepancy  is 
attributable  to  forces  which  we  shall  not  be  able  to  evaluate  even 
with  the  aid  of  the  more  complete  equations.  However,  a  con- 
siderable part  of  the  discrepancies  encountered  will  be  shown  to 

230 


xi  LAWS  OF  "IDEAL"  GAS  231 

arise  from  the  attempt  to  apply  approximate  equations  to  data 
the  precision  of  which  warrants  more  elegant  formulation. 

The  approximate  equation  is  based  upon  the  conduct  of  the 
"ideal"  gas.  Since  this  equation  not  only  is  extensively  used  but 
also  serves  as  a  model,  its  derivation  will  be  given  first.  There 
will  then  follow  a  presentation  of  equations  which  are  more  strictly 
applicable  to  the  actual  systems  which  we  know  do  not  behave  in 
a  manner  comparable  with  that  of  an  ideal  gas,  or  ideal  solute. 

APPLICATION    OF   THE   LAWS    OF   AN    "iDEAL"    GAS 

For  the  sake  of  simplicity  imagine  two  aqueous  solutions,  one 
containing  sugar  at  the  molar  concentration  [S]i  and  the  other 
containing  sugar  at  the  molar  concentration  [S]2.  Let  these 
solutions  be  under  the  same  external  pressure  and  be  separated 
by  a  semipermeable  membrane,  permeable  to  the  water  but  not 
to  the  sugar.  Let  the  membrane  be  movable.  The  sugar  in  solu- 
tion at  the  higher  concentration  will  drive  the  membrane  before 
it,  there  will  be  a  tendency  toward  the  equalization  of  sugar  con- 
centrations and,  if  the  membrane  be  under  restraint,  work  will 
be  expended  in  overcoming  force.1  By  this  trivial  presentation 
there  is  suggested  a  crude  analogy  with  the  tendency  toward 
equalization  of. concentrations  when  two  vessels  of  gas  at  different 
pressures  are  connected  and  with  the  mechanical  work  which  the 
process  of  equalization  can  do.  In  this  analogy  originates  one 
manner  in  which  energy  changes  are  related  to  the  accompanying 
material  changes.  The  comparatively  simple  gas  laws  are  rather 
directly  applied  to  solutes. 

There  may  first  be  considered  the  simple  fact  that  a  gas  can 
absorb  energy  as  heat  and,  by  the  resulting  expansion,  expend 
energy  as  mechanically  measurable  work.  Imagine  the  gas, 
initially  at  volume  Vi,  to  be  held  under  the  constant  pressure,  P, 
of  a  frictionless  piston  of  cross-sectional  area  A.  Let  the  gas  be 
heated  until  it  shall  have  expanded  to  volume  V2.  The  piston 
will  then  have  been  pushed  through  a  distance  determined  by  the 

value  of  — or  — .     Now  the  product  of  area,  A,  and  pres- 

A  A 

1  The  reader  should  not  interpret  this  as  a  description  of  the  mechanism. 


232  THE    DETERMINATION    OF    HYDROGEN    IONS 

sure,  P,  gives  the  magnitude  of  the  force  which  the  expanding  gas 
has  to  overcome.  Also 

force  X  distance  =  work 

Hence; 

AV 

work  =  (PA)  —  or  W  =  PAV  (1) 

A 

If  the  heat  added  is  more  than  equivalent  to  the  work  done,  the 
difference  is  attributed  to  an  increase  of  internal  energy,  U.  If 
Q  is  heat  added  and  W  is  work  done  by  the  system  we  write 

AU  =  Q  -  W  (2) 

We  shall  find  that  differences  of  energy  so  defined  have  perfectly 
definite  values  for  definite  changes  of  state. 

Now  let  it  be  assumed  that  the  gas  is  an  "ideal"  gas,  one 
specification  for  which  is  that  its  internal  energy  per  mole  is 
determined  by  the  temperature  alone.  Then  AU  may  be  made 
zero  by  maintaining  this  gas  at  constant  temperature. 

But  although  W  will  now  equal  Q  its  magnitude  may  range 
widely.  If,  for  instance,  the  opposing  pressure  of  the  piston  be 
always  maintained  during  the  expansion  at  a  value  much  less 
than  the  pressure  of  the  gas,  it  is  obvious  that  not  all  the  work 
possible  to  obtain  will  be  gotten.  The  maximum  work  will  be 
obtained  when  the  opposing,  outside  pressure  differs  from  the 
internal  pressure  by  an  infinitesimal. 

Under  these  conditions  of  maximum  work  let  the  second 
specification  in  the  definition  of  an  "ideal"  gas  be  applied,  namely 
rigid  conformity  to  relation  (3)  which,  it  will  be  recalled,  is  an 
expression  of  the  laws  of  Boyle  and  Gay-Lussac. 

PV  =  nRT  (3) 

P  is  the  pressure  in  atmospheres,  V  is  the  volume  in  liters,  n  is 
the  number  of  moles  of  the  gas,  R  is  the  gas  constant,  and  T  is 
the  absolute  temperature.2 
For  one  mole  of  gas 

PV  =  RT  (3a) 

2  See  page  245. 


XI 


WORK   OF   GAS   EXPANSION 


233 


At  constant  temperature,  the  pressure-volume  relation  will  be 
described  by  some  isotherm  on  a  P:V  diagram  such  as  the 
isotherm  of  figure  38.  Starting  at  PiVi  (A  of  the  figure)  the  gas, 
expanding  against  the  external  pressure  Pi  —  dP  (dP  being  an 
infinitesimal)  increases  in  volume  to  the  extent  of  the  infinitesimal 
dV.  The  work  done  is  (Pi  —  dP)  dV.  •  But  since  the  product  of 
the  infinitesimals,  namely  (dP)  (dV),  is  negligible  compared  with 
P**V, 

dW  =  PidV  (4) 

At  the  new  pressure  PI  —  dP  let  the  process  be  repeated  and  finally 
let   the   infinitesimal  steps   be  repeated  an  infinite  number  of 


Fia.  38.  ISOTHERMAL  PV-CuRVE  FOR  A  "PERFECT  GAS" 

times  (as  suggested  crudely  by  the  steps  of  the  figure)  until  the 
gas  has  been  brought  to  V2  and  P2  at  B.  Then  the  work  which 
will  have  been  performed  will  equal  the  area  ABC.  To  formulate 
this  the  method  of  the  integral  calculus  must  be  used. 

At  each  step  dW  =  PdV.  Find  the  sum  of  all  steps  between 
Vi  and  V2;  that  is,  integrate  (5)  as  indicated,  between  the  limits 
Vi  and  V8. 


v« 


W 


PdV 


(5) 


Since  P  is  variable  it  must  be  found  in  terms  of  V  from  the  rela- 
tion PV  =  nRT. 

vz  v» 

dV 


W 


nRT 


(6) 


234  THE    DETERMINATION    OF   HYDROGEN   IONS 

The  integral  is 

W  =  nRT  In  ^ 

Or,  since  for  an  ideal  gas  PiVi  =  P2V2, 

W  =  nRT  In  ^  (7) 

Pz 

In  these  equations  In  (logariihmus  naturalis)  symbolizes  (natural) 
logarithm  to  the  base  e. 

Equation  (7)  states  by  symbols  and  tacit  implications  that  the 
maximum  work  capable  of  being  performed  by  a  perfect  gas,  ab- 
sorbing heat  from  its  surroundings  but  kept  at  constant  tem- 
perature, is  equal  to  the  product  of  the  number  of  moles  of  gas  n, 
the  gas  constant  R,  the  absolute  temperature  of  the  gas  T,  and 
the  natural  logarithm  of  the  ratio  of  the  initial  and  final  pressures. 

Next  imagine  a  dilute  solution  of  some  substance,  for  which  the 
osmotic  pressure  can  be  calculated  from  the  ideal  gas  equation, 
PV  =  nRT. 

Without  having  to  repeat  the  reasoning  applied  in  the  case  of 
the  gas  and  without  necessarily  having  to  bring  forth  a  specific 
device  which  will  perform  work  while  the  substance  is  being 
brought  from  one  solution  to  another,  we  may  at  once  apply 
equation  (7)  specifying  that  in  this  application  the  pressures  are 
the  osmotic  pressures  of  the  dissolved  substance  in  question. 
In  general,  wherever  we  have  a  substance  which  we  assume  is 
conducting  itself  as  an  ideal  gas  or  ideal  solute  and  this  substance 
is  transferred  between  two  pressures  PI  and  P2,  we  may  write: 

W  =  RT  In  ^  (8) 

"2 

for  the  reversible  work  of  isothermal  transfer  of  one  mole  of 
substance.  If  concentrations  of  the  substance  A  are  proportional 
to  the  respective  pressures 

W  =  RT  In  [^  (9) 

[A]2 

'r 

The  work,  W,  if  expressed  in  electrical  terms,  is  nFE.  E  is 
the  faraday,  n  is  number  of  f aradays  required  to  effect  the  trans- 


XI  ELECTRICAL   WORK  235 

fer  of  one  mole  and  E  is  the  electrical  potential.     Hence  equa- 
tion (9)  may  be  written 


Thermodynamics  presents  this  proximate  equation  to  the  ex- 
perimentalist and  leaves  it  to  his  ingenuity  first  to  devise  an  ex- 
perimental means  of  applying  it  and  next  to  determine  whether 
the  assumptions  regarding  the  chemical  transformations,  which 
take  place  in  this  particular  device,  are  met.  In  Chapter 
XII  a  device  is  described  and  conditions  specified  whereby  it  is 
believed  that  equation  (10)  is  applicable  to  the  determination  of 
the  ratio  between  two  hydrogen  ion  concentrations.  The  specific 
equation  is 


where  the  electrical  work  term  EF  is  used  since  the  device  is  sup- 
posed to  furnish  this  work  by  flow  of  electricity. 

It  is  now  our  duty  to  note  that  the  most  fundamental  and  most 
dangerous  assumption  which  led  to  equation  (11)  was  that  the 
hydrogen  ions  obey  the  laws  of  the  ideal  solute.  It  should  be 
evident  in  the  rather  fair  harmony  of  the  subject  matter  presented 
up  to  this  point  that  data  based  ultimately  upon  the  conduct  of 
the  hydrogen  electrode  and  interpreted  through  the  simple  equa- 
tion (11)  have  not  distorted  the  picture  very  severely.  Indeed 
there  is  a  rough  analogy  between  the  picture  we  have  drawn  and 
a  map  of  an  area  drawn  with  the  assumption  that  the  needle  of 
the  compass  points  true  north.  There  are,  as  it  were,  local 
perturbations  with  every  solution.  True  and  apparent  concen- 
trations become  as  far  apart  as  north  pole  and  magnetic  pole  in 
certain  cases;  but  local  navigation  remains  possible. 

The  laws  of  an  ideal  gas  may  be  considered  as  limiting  laws  to 
which  the  conduct  of  the  actual  substance  approaches  under 
simple  conditions.  What  then  prevents  their  general  application? 
It  appears  that,  to  make  these  laws  applicable,  the  size  of  the 
molecules  would  have  to  approach  the  mathematical  point  and 
there  would  have  to  be  no  cohesive  or  other  forces  of  inter-action. 
In  the  case  of  ions  the  electrostatic  forces  of  interaction  appear 


236        THE  DETERMINATION  OF  HYDROGEN  IONS 

to  far  outweigh  other  matters  in  their  interference  with  the 
applicability  of  the  gas  laws.  We,  therefore,  face  an  extremely 
complex  problem. 

Not  only  should  account  be  taken  of  deviations  from  the  gas 
laws  due  to  the  inherent  nature  of  the  solute,  but  the  solvent 
surely  cannot  be  considered  merely  as  an  invariant  environment. 

But  let  us  take  under  consideration  two  solutions  of  the  sub- 
stance A  at  concentrations  [A]i  and  [A]2.  At  extremely  high  dilu- 
tions variations  of  the  solvent's  properties  with  variation  of  the 
concentration  of  the  solute  tend  to  vanish  and  the  solute  is 
highly  dispersed.  Then  equation  (10)  holds  for  transfer  of  A  from 
one  low  concentration  to  another  in  a  medium  of  nearly  constant 
properties.  If  conditions  are  not  simple,  equations  (9)  to  (11) 
will  not  hold.  We  may  than  introduce  corrections.  For  con- 
centration [A]i  let  the  deviation  in  energy  be  coi  and  for  [A]2, 
co2  etc.  Equation  (12)  describes  the  experimental  data. 

W  =  RT  In  ^  +  coi  -  co2  (12) 

LAj2 

The  w  terms  are  merely  the  correction  terms  expressed  in  the 
dimensions  of  energy.  If  we  wish  to  express  the  corrections  in 
terms  of  factors  to  be  applied  to  the  concentrations,  substitute 
i  for  «i  and  "RTlny^  for  co2.  Then  we  have  (13)  or  (14) 

W  =  RT  In  [£r  +  RT  In  -  (13) 

[Ah  72 

(14) 


IAJ2  72 

A  term  such  as  [A]i7i  may  now  be  considered  as  a  "corrected 
concentration,"  and  may  be  called  the  active  concentration  or 
the  activity,  7  is  the  activity  coefficient. 

The  symbol  a  is  usually  used  for  activity.  We  shall  paren- 
thesize a  chemical  symbol  when  we  signify  the  activity  of  the  sub- 
stance whose  symbol  is  inclosed  in  the  parentheses,  just  as  we 
use  brackets  to  signify  the  concentration  of  the  substance  whose 
symbol  is  enclosed  in  brackets.  Then 

W  =  RT-ln  (^  (15) 

(A)  2 


XI  FREE   ENERGY  237 

Now  we  have  an  equation  of  the  form  of  that  derived  from  the 
ideal  gas  laws  and  can  proceed  to  all  the  mathematical  develop- 
ments which  have  already  been  made  with  the  gas  laws. 

This  legitimate  juggling  does  scant  justice  to  the  subject,  for 
by  following  the  route  to  the  same  final  equation  (15)  which  was 
followed  by  Lewis  (See  Lewis  and  Randall,  Thermodynamics  and 
references  therein  to  early  papers  by  Lewis),  we  shall  encounter 
some  useful  ideas. 

THE  FREE  ENERGY  EQUATION 

It  is  a  principle  of  thermodynamics  that  the  total  energy,  E,  of 
a  system  in  a  given  state  will  return  to  the  same  value  if  the 
system  be  put  through  a  cyclic  process  and  be  returned  to  the 
first  state.  Likewise  if  a  system  be  known  in  two  states  and  if 
we  designate  the  total  energy  in  the  one  case  by  EI  and  in  the 
other  case  by  E2,  we  may  speak  of  the  increment  of  total  energy 
AE  =  E2  —  EI  or  of  an  infinitesimal  increment  dE.  This  will 
be  measurable  in  the  sense  that  we  can  speak  of  dE>  as  being 
determined  by  the  heat  added,  dq,  and  by  the  work,  dw,  done  by 
the  system  according  to  the  equation : 

dE  =  dq  -  dW  (16) 

The  negative  sign  is  given  to  dW,  as  it  occurs  in  (16),  to  signify 
energy  lost  from  the  system  because  of  the  work  done  by  the 
system. 

Temporarily  we  shall  use  another  quantity  called  the  entropy,  S. 
In  theory  any  system  can,  by  means  of  reversible  processes  be 
put  through  any  desired  changes  and  then  be  returned  to  its 
first  state.  It  will  then  have  the  original  value  of  the  entropy, 
all  changes  in  the  entropy  of  the  system  being  measured  by  the 
equation 

dS  =  f  (17) 

Equations  (16)  and  (17)  give  (18) 

dE  =  TdS  -  dW  (18) 


238  THE    DETERMINATION    OF   HYDROGEN    IONS 

In  the  measurement  of  energy  changes  there  is  occasion  to  dis- 
tinguish certain  quantities  which  it  is  a  convenience  to  name. 
The  quantities  are: 

E  +  PV  =  H,  called  "the  heat  content" 

E  -  TS  =  A,  called  "the  free  energy"  by  Helmholtz 

E  -  TS  +  PV  =  F,  called  "the  free  energy"  by  Lewis. 

Distinction  between  H,  A  and  F  should  be  kept  clear.  We  shall 
use  only  F  and  shall  refer  to  it  without  qualification  as  the  free 
energy 

F  =  E  -  TS  +  PV  (19) 

By  differentiation 

dF  =  dE  -  TdS  -  SdT  +  PdV  +  VdP  (20) 

Combine  (20)  and  (18). 

dF  =  -  SdT  +  VdP  -  dW  +  PdV  (21) 

At  constant  temperature  and  pressure  dT  =  0  and  dP  =  0. 
Hence 

-dF  =  dW  -  PdV  (22) 

In  (22)  PdV  is  what  may  be  called  the  hydrostatic  work  done  by 
any  change  of  volume  at  pressure  P.  Hence  the  decrease  in 
free  energy,  —  dF,  attending  a  reversible  change  of  state,  measured 
at  constant  temperature  and  pressure,  may  be  described  as  the 
maximal  non-hydrostatic  work,  dW  —  PdV.  The  following 
treatment  will  be  limited  throughout  by  the  understanding  that 
temperature  and  pressure  are  to  remain  constant.  Hence  we 
shall  speak  only  of  changes  of  free-energy,  and  can  eliminate 
from  consideration  A,  and  H. 

Consider  a  system  made  up  of  several  components.  If  to  this 
system  there  be  added  an  infinitesimal  mass,  dma,  of  component 
A,  all  other  conditions  remaining  the  same,  we  may  say  that  the 
energy  of  the  system  is  increased  by  the  addition  of  chemical 
energy.  The  increase  of  the  energy  of  the  system  per  unit 
(any  unit)  increase  of  the  mass  of  the  given  component  will  be 
defined  by 

dE  _ 

dm  ~  M 


XI  CHEMICAL   POTENTIAL  239 

where  ju  is  called  the  chemical  potential  of  the  given  substance  in 
the  system  considered.  If  we  choose  the  molecular  weight  as 
the  unit  of  mass  of  component  A,  and  indicate  by  Na  the  number 
of  moles 


Gibbs  shows  that  if  the  temperature  and  pressure  of  the  system 
be  kept  constant  and  the  masses  of  all  other  components  be  kept 
constant 

/J|W  ;        (23) 

a' T,  P,  Njj,  Nc 

dF  being  the  increase  of  free  energy.     The  subscripts  T  and  P 
are  reminders  of  constancy  of   temperature  and  pressure  and  the 
subscripts  Nb,  Nc  .    .    .    .   indicate  constancy  of  the  masses  of 
other  components. 
But 


,  P,  Nb,  Nc 


is  what  Lewis  calls  the  partial  molal  free  energy,  Fa,  of  component 
A.  Hence 

}  (23a) 

a/T,  P,  Nb,  Nc 

As  a  solution  is  diluted  its  solute  tends  to  conform  closer  to  the 
conduct  of  an  ideal  solute.  As  a  limiting  law  we  can  state  for 
solute  A 

Ma  =  ra  =  RT/n  [A]  +  B  (24) 

Here  B  is  a  function  of  temperature  and  is  a  constant  at  a  fixed 
temperature.  But  being  a  limiting  law  (24)  cannot  be  applied  in 
general.  However,  the  convenient  form  of  this  equation  can  be 
preserved  by  substituting  for  the  concentration  [A]  a  defined 
quantity  as  will  presently  be  done. 

We  are  quite  accustomed  to  think  of  the  flow  of  heat  as  deter- 
mined by  the  relative  temperatures  of  the  bodies  between  which 


240  THE    DETERMINATION    OF   HYDROGEN    IONS 

heat-exchange  takes  place.  "  .  .  .  .we  may  imagine  every- 
thing to  have  a  certain  tendency  to  lose  heat,  or  we  may  say  that 
heat  has  a  tendency  to  escape  from  every  system.  Temperature 
is  then  a  measure  of  this  escaping  tendency  of  heat."  (Lewis 
and  Randall,  Thermodynamics)  .  In  the  same  way  we  may  think 
of  the  escaping  tendency  of  a  real  substance,  for  example  water. 
If  the  escaping  tendency  of  water  is  the  same  for  the  water  in  a 
solution  as  it  is  for  the  water  in  the  vapor  phase  above  the  solu- 
tion, water  will  not  of  itself  pass  from  the  one  phase  to  the  other. 
If  the  escaping  tendency  of  the  water  is  greater  in  one  phase 
than  in  a  second,  water  will  pass  from  the  first  phase  to  the  second. 
So  it  is  in  general  for  any  substance. 

Gibbs  (1878)  had  shown  that  the  chemical  potential,  /z,  has 
these  properties. 

As  a  concrete  measure  of  escaping  tendency  there  is  liberty  to 
choose  any  measure  which  is  convenient.  Vapor  tension  might  be 
chosen;  but  true  partial  vapor  pressures  are  not  generally  meas- 
ured. The  so-called  fugacity  (symbol  /)  is  used  as  a  suitable 
measure.  For  solute  A  we  may  define  its  fugacity  by  the  equation 

Ma  =  Fa  =  RTZrc/a  +  B  (25) 

At  extreme  dilution 

Ata  =  Fa  =  RTZn  [A]  +  B  =  RTZn/a  +  B  (26) 


But  (25)  holds  at  any  concentration.  For  two  states  of  a  sub- 
stance at  constant  temperature,  the  states  being  indicated  by 
subscripts  0  and  1,  we  have 

+  B  (27) 

+  B  (28) 


or  Mi  ~  Mo  =         rc  (29) 

Jo 

Now  choose  one  state  of  the  substance  as  standard  and  let  its 
fugacity   be  /0.    The  relative  fugacity,   y  will  be  called  the 

Jo 

activity  -,  aA.    Then 

aA  (30) 


XI  EQUILIBRIUM   EQUATION  241 

We  shall  now  represent  the  activity  of  any  substance  by  a  paren- 
thesis placed  about  the  symbol  for  the  substance.  For  example 
(A)  is  the  activity  of  substance  A,  e.g., 

Mi  -  MO  =  RTZn  (A) 

If  then  two  states  of  a  solute  A  are  being  compared  and  both  differ 
from  the  standard  state  chosen, 


-  M2  =  RT  In  (31) 


Mi 


Comparison  with  (14)  and  (15)  shows  that  activity  is  related  to 
concentration  by  introducing  the  coefficient  y  called  the  activity 
coefficient.  From  the  above  we  have: 

AF  =  F!  -  F2  =  MI  -  M2  =  RT  In  j^-1  =  RTfn  ^f1   (32) 

[A]2  72  (A)8 

THE   EQUATION   FOR    CHEMICAL   EQUILIBRIUM 

Equation  (23)  is 

dF 


or 

Ma  dNa  =  dF 

with  the  understanding  that  temperature  and  pressure  are  con- 
stant and  that  all  other  components  are  constant  while  an  in- 
finitesimal change  is  made  in  component  A.  Even  though  all 
other  components  are  subject  to  change,  the  initial  or  the  final 
state  of  a  system  of  components  a,  b,  c  .  .  .  .  n  may  be  described  by 

F  =  NaMa  +  NbMb  +  NcMc-  .  .  .Nnjun  (33) 


Suppose  we  have  a  chemical  reaction  in  which  Na  moles  of  con- 
stituent a  and  Nb  moles  of  constituent  b  are  transformed  to  Nr 
moles  of  constituent  r  and  Ns  moles  of  constituent  s. 

Naa  +  Nbb  -»  Nrr  +  N8s 


242  THE    DETERMINATION    OF   HYDROGEN   IONS 

Before  the  reaction 


Fi  =  N.MS  +  NbMb  (34) 

After  the  reaction 

(35) 


That  we  may  have  a  definite  basis  of  reference,  let  F0  represent 
the  free  energy  of  a  system  in  which  the  components  are  in  a 
selected  standard  state  indicated  by  subscript  0. 


+  NbMbo  (36) 

+  NrMro  (37) 

Fl  -  Fol  =  Na(/*a  -  Mao)  +  NbGub  -  /ibo)  (38) 

Ft    -    FOZ    =    Nr(Mr    "    Mro)    +   Ns(Ma    -    Mso)  (39) 

But  by  (30) 

Ma  —  Mao  =  RT/n  (a) 
Mb  -  Mbo  =  RT/n  (b) 
etc. 

Hence 

Fl  -  Fol  =  RTln  (a)Na(b)Nb  (40) 

Fz  -  F02  =  RTln  (r)Nr(s)Ns  (41) 

frNNr/g)N. 
-  AFi,,  -  (-  AFo)  =  Fx  -  F2  -  (F01  -  Fo2)  =  -  RT  Z»i  (a)Na  b)Nb     <42) 

But  Foi  —  ^02,  the  difference  of  free  energy  of  the  systems  with 
components  in  the  standard  states,  is  a  constant,  K/.  For  con- 
venience put  K'  =  RTln  K. 

(r)Nr(s)N' 
-  AF1(2  =  RT  In  K  --  RT  In  (43) 


At  the  state  of  equilibrium  we  have  such  values  of  (r)Nr,   (s)N% 
etc.  in  (43)  that  no  change  occurs  and  —  A/^2  =  0.     Hence, 


RT  In  K  =  RT  In 


(a)Na(b)Nb 


XI  ACTIVITY   COEFFICIENTS  243 

or 

(r)N'(s)N» 

=  K  (44) 


In  (44)  j£  is  the  ordinary  mass  action  constant  for  the  equilib- 
rium equation  in  which  activities  have  been  substituted  for 
concentrations. 

Likewise  for  the  equilibrium  of  the  reversible  reaction 

HA  ?±  H+  +  A- 
we  may  write 

=  .. 


instead  of  the  approximate  equation 

[J^yJ  =  KL  (46) 

By  introducing  activity  coefficients  as  described  on  page  236,  we 
also  have 

[H+]  7H*  [A-]  7A- 


[HA]  THA 


=  Ka  (47) 


To  illustrate  the  applications  of  these  equations,  cases  will  be 
introduced  at  appropriate  places  in  the  subsequent  development. 
To  relieve  the  subject  of  the  rather  artificial  aspect  it  has  now 
attained,  there  will  be  given  in  outline  in  Chapter  XXV  the 
theory  which  Debye  and  Hiickel  have  proposed  as  a  partial  ex- 
planation of  those  deviations  from  the  laws  of  an  ideal  solute 
which  are  observed  with  solutions  of  ions. 

It  has  become  evident  in  the  derivation  of  the  equilibrium  equa- 
tion by  means  of  free  energy  changes  that  we  have  abandoned  the 
use  of  concentrations  except  as  they  may  be  introduced  by  the 
device  of  the  relation 

[Ah.  =  (A) 

This  is  a  great  convenience  because  custom  has  established  the 
use  of  the  balance  and  volumetric  flask  as  a  means  of  defining  the 
composition  of  solutions.  However,  we  should  not  lose  sight  of 


244  THE    DETERMINATION    OF   HYDROGEN   IONS 

the  fact  that  there  is  a  certain  degree  of  artificiality  involved  in 
this  manner  of  relating  states  to  concentration.  Were  the  measure 
of  free  energy  changes  as  easy  as  weighing,  the  sprinkling  of  a 
substance  into  a  solution  until  the  partial  free  energy  balances 
some  standard  might  prove  as  useful  in  many  instances  as  the 
current  practice  of  weighing  and  measuring.  Indeed  this  is  what 
has  actually  happened  in  very  many  applications  of  the  hydrogen 
electrode  to  problems  of  biochemistry  and  industry.  A  phenomenon 
unrelated  in  any  known  way  to  anything  measurable  by  balance 
or  volumetric  flask  is  related  to  the  so-called  pH  value  of  the  solu- 
tion. When  the  method  of  measuring  the  pH  value  is  analyzed 
it  is  found  to  be  a  measurement  of  a  free  energy  change.  The 
"hydrion  concentration,"  which  pH  is  supposed  to  represent, 
and  the  not  very  successful  attempt  to  standardize  by  reference 
to  a  "normal  potential"  are  introductions  which  are  not  essential 
but  which  are  used  to  satisfy  our  constant  desire  to  relate  degree 
of  action  to  mass.3 

In  other  words  the  free  energy  equation  has  its  own  intrinsic 
value  capable  of  standardization  and  use  without  reference  to 
mass  and  capable  of  describing  systems  in  terms  of  the  direction 
and  extent  of  the  flow  of  energy  when  these  systems  are  allowed  to 
react  upon  one  another. 

Of  course,  this  not  satisfying.  Trie  aim  of  science  is  to  relate 
all  properties  and  all  phenomena.  The  convenience  of  laboratory- 
practice  demands  the  use  of  the  balance,  and  molecular  theory 
urges  us  to  take  account  of  particle  number.  Nevertheless  it  is 
well  to  overemphasize  the  above  aspect  for  a  moment  lest  too 
slavish  attention  to  the  more  customary  formula  introduce  terms 
which  are  often  unnecessary. 


NUMERICAL  VALUES  FOR   2.3026    - 

F 

In  the  practical  application  of  electromotive  force  measurements 
and  in  numerical  calculations  for  theoretical  purposes  there  are 

3  It  might  be  said  at  this  point  that  it  is  easy  to  imagine  a  process  con- 
trolled by  automatic  potentiometric  methods  and  that  it  would  be  only 
adding  unnecessary  complexities  to  translate  the  electromotive  force  into 
artificial  terms. 


XI  NUMERICAL   FACTOR  245 


occasions  to  use  the  numerical  value  of  -  -  at  a  given  value  of 

the   absolute   temperature,   T.     Furthermore   equations   of   the 
form 

T»rn  /TT_L\ 

(48) 

are  more  frequently  used  with  Briggsian  instead  of  Naperian 
logarithms  as: 


E  =  2.3026         log,,  (49) 


2 
-prn 

We,  therefore,  desire  values  of  2.3026   —  .    R  is  the  gas  con- 

F 

stant,  T  is  the  absolute  temperature  (273°.  1  +  t°C),  and  F  is 
the  f  araday. 

In  making  numerical  solutions  of  this  equation  it  is  essential 
to  use  a  set  of  consistent  units  for  the  quantities  concerned. 
Before  these  are  discussed  it  may  be  noted  that  the  values  in 
current  use  for  x  in  the  relation 


ln(     )  =  xT  loglo(     ) 

j} 

differ  from  one  another  by  an  amount  too  small  for  the  difference 
to  be  of  much  significance  in  physical  applications.  On  the  other 
hand  the  differences  between  some  of  the  extreme  values  are  such 
that  discrepancies  as  large  as  0.6  millivolt4  appear  in  certain 
common  calculations.  Since  it  is  irritating  to  have  to  take 
account  of  such  unnecessary  discrepancies  in  calculations  which 
form  the  basis  for  the  comparison  of  experimental  data,  it  is 
desirable  to  adhere  to  a  well  standardized  value  which  incident- 
ally shall  have  more  digits  than  may  be  necessary  to  develop  the 
actual  significance  of  measurements.  International  Critical  Tables 

4  Comparison  of  six  well-known  texts  shows,  as  extremes  of  the  value 
of  x,  0.0001983  and  0.0001985.  For  t  =  25°C.,  (T  =  298.1°),  xT  is  0.059113 
in  the  first  instance  and  0.059173  in  the  second.  The  calculated  differ- 
ence of  potential  between  a  hydrogen  electrode  in  a  solution  of  pH  =  0 
and  a  hydrogen  electrode  in  a  solution  of  pH  =  10  would  be  0.59113  volts 
by  the  use  of  the  first  factor  and  0.59173  volts  by  the  use  of  the  second,  a 
discrepancy  of  0.6  millivolt. 


246  THE    DETEKMINATION    OF   HYDROGEN    IONS 

now  provides  accepted  values  with  which  the  desired  value  may 
be  reached. 

P  V 

In  equation  (48)  the  gas  constant,  R,  is          °    with  n   =    1 

273.1 

understood. 

V0,  the  volume  of  one  mole  of  a  perfect  gas  at  0°C.,  is  22412 
milliliters  when  the  pressure  is  one  atmosphere,  45°  latitude. 
In  distinction  from  this  pressure,  the  normal  atmosphere  (An)  is 
defined  as  the  pressure  exerted  by  a  vertical  column  of  liquid  76  cm. 
long,  density  13.5951  grams  per  cubic  centimeter,  acceleration  of 
gravity  being  980.665  centimeters  per  second  per  second.  The 
atmosphere  at  45°  latitude  (A45)  is  assumed  to  be  related  to 
the  normal  atmosphere  (An)  as 

Iog10^  =  0.000,021,4 

A45 

Also  one  milliliter  =  1.000,027  cubic  centimeters.  Hence  V0 
at  0°C.  and  one  normal  atmosphere  is  22411.5  cubic  centimeters. 
P0,  to  be  consistent  with  the  above,  is  to  be  regarded  as  one 
normal  atmosphere  and  it  may  here  be  remarked  that,  when  the 
value  we  are  now  developing  is  to  be  applied  to  the  barometric 
correction  for  the  hydrogen  electrode,  the  pressure  should  be. 
strictly  speaking,  in  terms  of  the  normal  atmosphere. 
Po  =  980.665  X  76  X  13.5951  =  1,013,250  dynes  per  square  cm. 
Then 

^       1,013,250  X  22,411.5 

R  = •  =  83, 150,684  ergs  per  degree  per  mole. 

273.] 

International  Critical  Tables  rounds  the  value  off  to  8.315  X  107 
since  it  is  not  more  accurately  known,  but,  since  the  stated 
logarithm  (which  will  probably  be  used  in  calculations)  corre- 
sponds to  8.31507  X  107  we  shall  continue  with  the  latter  value. 

One  joule  absolute  =  107  ergs. 

One  joule  absolute  =  one  volt-coulomb  (abs). 

Hence  R  =  8.31507  volt-coulombs  (abs). 

International  Critical  Tables  accepts  as  a  basic  constant  one 
faraday  =  96500  coulombs  (abs).  Hence  equation  (48),  with  E 
to  be  stated  in  absolute  volts,  is 

_  8.31507          (H+). 
96500  (H+), 


XI  INTERNATIONAL  UNITS  247 

Transposing  to  common  logarithms   (base   10)   by  multiplying 
with  the  modulus  2.302585,  we  have : 

E  =  0.000198406  T  log  ^^  (50) 

(ti+)2 

The  units  employed  up  to  this  point  have  been  those  of  the 
absolute  system  for  which  the  fundamental  constants  are  the 
centimeter,  the  gram  and  the  second  (cgs-system) .  Most  actual 
measurements  of  potential  difference  (E)  are  not  made  in  terms 
of  absolute  volts  but  are  usually  supposed  to  be  made  in  terms  of 
the  so-called  international  volt.  This  is  a  quantity  derived  by 
means  of  Ohm's  law  [E  (in  volts)  =  current  (in  amperes)  X 
resistance  (in  ohms)]  from  the  following  definitions  of  the  inter- 
national ohm  and  of  the  international  ampere. 

The  international  ohm  is  the  resistance  offered  to  an  unvarying 
electric  current  by  a  column  of  mercury  at  the  temperature  of 
melting  ice,  14.4521  grams  in  mass,  of  a  constant  cross-sectional 
area  and  of  a  length  of  106.300  cm. 

The  international  ampere  is  the  unvarying  electric  current 
which,  when  passed  through  a  solution  of  nitrate  of  silver  in 
water  in  accordance  with  specification  II  (of  the  1908  London 
conference),  deposits  silver  at  the  rate  of  0.00111800  gram  per 
second. 

Consequently  the  international  volt  (by  Ohms'  law)  is  the  elec- 
trical pressure  (electromotive  force)  which,  when  steadily  applied 
to  a  conductor  the  resistance  of  which  is  one  international  ohm, 
will  produce  a  current  of  one  international  ampere. 

Notwithstanding  this  definition  the  socalled  international  volt 
in  actual  use  is  derived  from  sets  of  Weston  standard  cells  main- 
tained by  national  standards  laboratories.  In  agreement  with 
the  London  conference  of  1908  the  "saturated"  Weston  cell 
(see  page  342)  is  considered  to  have  an  electromotive  force  of 
1.01830  international  volts  at  20°C.  This  is  virtually  the  defini- 
tion of  a  new  unit  and  according  to  International  Critical  Tables 
it  "furnishes  a  subsidiary  definition  which  is  slightly  discordant 
with  the  primary  one."  Therefore  International  Critical  Tables 
distinguishes  between  conversion  factors  which  are  based  on  the 
defined  value  of  the  Weston  cell  and  which  are  designated  by  (v) 


248  THE    DETERMINATION    OF   HYDROGEN   IONS 

and  conversion  factors  based  on  the  defintions  arising  from  the 
performance  of  the  silver  coulometer  and  designated  by  (a). 

One  international  volt  (v)  =  1.00042  absolute  volt. 
One  international  volt  (a)  =  1.00045  absolute  volt. 

Before  making  a  transformation  of  equation  (50)  by  the  use  of 
one  of  these  conversion  factors  we  shall  discuss  two  questions 
concerning  which  there  may  be  some  curiosity. 

The  first  concerns  the  faraday.  It  might  appear  that,  when 
the  international  ampere  is  once  defined,  the  introduction  of  the 
accepted  value  107.880  as  the  atomic  weight  of  silver  would 

107  880 

furnish  '• =  96493.7   international    coulombs    as    the 

0.00111800 

derived  value  of  what  might  tentatively  be  called  the  "inter- 
national faraday."  But  in  the  definition  of  the  international 
ampere  it  is  well  understood  that  the  word  "silver"  refers  to  the 
gross  deposit.  (For  the  inadequacy  of  the  specifications  see 
Bureau  of  Standards  circular  60,  pp.  34  to  36  and  Bureau  of  Stand- 
ards Bulletin  13,  499.)  Hence,  if  care  be  taken  to  distinguish 
between  the  use  of  the  above  derivation  as  one  of  several  experi- 
mental evaluations  of  the  faraday  and  its  use  as  a  definition  of 
a  new  quantity  (tentatively  called  "international  faraday")  it 
will  be  appreciated  that  the  latter  use  is  inconsistent  with  the 
concept  of  the  faraday  as  a  quantity  not  subject  to  legislative 
definition.  This  is  the  attitude  of  International  Critical  Tables.5 
Accordingly  International  Critical  Tables,  expressing  the  mag- 
nitude of  the  faraday  (the  only  unit  of  that  name  which  is  recog- 
nized) in  terms  of  the  various  units,  states  first  its  accepted  basic 
constant; 

one  faraday  =  96500  absolute  coulombs 
and  then  the  conversion  factors 

one  faraday  =  96510  international  coulombs  (v) 
one  faraday  =  96507  international  coulombs  (a) 

5  According  to  personal  correspondence  with  Dr.  N.  Ernest  Dorsey, 
Associate  Editor,  International  Critical  Tables  whom  I  thank  for  several 
very  helpful  comments  on  this  section. 


XI  NUMERICAL   FACTOR  249 

The  second  question  concerns  the  choice  between  the  con- 
version factor  for  absolute  to  international  volts  (v)  and  the  con- 
version factor  for  absolute  to  international  volts  (a).  Were 
there  a  definite  prospect  of  an  immediate  revision  of  the  defined 
value  of  the  Weston  cell,  reestablishing  the  true  international 
volt  as  that  to  be  in  actual  use,  it  would  be  wise  to  employ  the 
(a)  conversion  factor.  However  certified  values  for  the  Weston 
cells  in  use  are  in  terms  of  the  international  volt  (v)  and  while  the 
matter  is  one  of  very  minor  physical  significance  it  seems  more 
consistent  with  practice  to  use  the  factor  1.00042. 

Hence 

E  =  0.000,198,322  T  log  —  ^  (51) 

(H+J2 

in  international  volts  (v). 

A  table  of  values  for  0.000,198,322  T  will  be  found  in  the 
Appendix,  page  674. 

Since  electromotive  force  measurements  furnish  data  for  the 
calculation  of  free  energy  changes  it  is  desirable  to  have  equation 
(49)  in  the  form 


A  numerical  form  of  this,  consistent  with  the  derivations  given 
above,  is; 

Joules  (abs)  =  96500  E  (abs)  =  19.1462  T  log  ^IT     (52) 


Gram  calories  (15°)  =  4.575  T  log          i  (52a) 

(Jti+)2 

96500  E  (abs.  volts)  =  joules  'absolute 

96510  E  (international  volts  (v))  =  international  joules  (v) 

23058.5  E  (abs.  volts)  =  gram  calorie  (15°C.) 

The  last  is  derived  by  use  of  the  conversion  factor  one  gram 
calorie  (15°C.)   =  4.185  absolute  joules. 

In  the  above  discussion  no  attention  was  paid  to  the  uncer- 
tainties of  the  basic  constants  because  such  questions  do  not  enter 


250  THE    DETERMINATION    OF   HYDROGEN   IONS 

the  use  of  a  factor  in  preserving  uniformity  in  calculations.  How- 
ever, if  there  are  introduced  the  estimated  uncertainties  tabulated 
in  International  Critical  Tables,  we  find  that  F  is  uncertain  by 
about  one  part  in  10,000  and  R  by  about  0.9  part  in  10,000  (from 
the  uncertainty  of  V0). 

Hence  the  factor  in  equation  (51)  is 

0.000,198,3221 
±0.000,000,038] 

To  is  uncertain  by  not  over  0°.15,  or  5.5  parts  in  10,000. 
Hence,  in  Appendix  C,  A  at  0°C.  is  uncertain  by  about  5.5  +  1.9 
=  7.4  parts  in  10,000;  or  at  0°C. 

/     0.054162"!  I        (  18.4631"! 

=  \  ±0.000040]  A      \  ±0.0014] 

Likewise,  at  30°C,  A  is  uncertain  by  about  4.9  +  1.9  =  6.8  parts 
per  107000  or 

0.0601111          !_      f  16.6357"! 
±0.000041]         A      \±0.0011] 

On  the  other  hand  if  we  are  concerned  with  precision  of  poten- 
tial measurements  only,  a  precision  to  within  ±0.0001  volt 
in  an  observation  requires  the  use  of  the  fifth  decimal  place  in  A 
(appendix  C)  to  maintain  uniformity  of  statement  consistent 
with  such  observational  precision. 


CHAPTER  XII 

THEORY  OF  THE  HYDROGEN  ELECTRODE 

One  of  the  oldest  unsolved  problems  in  physical  chemistry  is  the 
source  of  E.M.F.  in  the  simple  galvanic  cell  and  the  mechanism 
of  its  production. — RIDEAL. 

There  are  two  aspects  of  the  theory  of  the  hydrogen  electrode 
which  may  well  be  kept  distinct.  One  is  the  problem  of  its 
mechanism.  The  other  is  its  application  to  the  measurement  of 
the  free  energy  change  in  the  transfer  of  hydrions  from  one  con- 
centration to  another.  A  complete  solution  to  the  first  is  not 
attained.  The  second  is  a  matter  of  thermodynamics  and,  to  the 
extent  that  we  can  detect  the  actual  factors  that  must  be  taken 
into  account,  our  formulations  are  safe  if  made  by  the  all  too 
general  methods  of  thermodynamics. 

We  shall  studiously  avoid  any  attempt  to  discuss  the  mechanistic 
aspect,  and  shall  refer  only  to  those  few  of  many  papers  on  the 
subject  which  are  found  in  Transactions  of  the  Faraday  Society, 
Vol.  19  (1924).  On  the  other  hand  it  will  be  necessary  to  intro- 
duce one  or  another  concept  of  the  gross  aspect  of  the  electrode 
mechanism  in  order  to  meet  the  elementary  requirements  of 
thermodynamics.  The  reason  for  this  is  simple.  Thermo- 
dynamics provides  the  formulation  of  a  cell  reaction:  but,  before 
this  rather  ethereal  generalization  can  be  applied,  the  data  of  the 
analyst,  of  inorganic  or  organic  chemistry  and  the  deductions  of 
the  physical  chemist  regarding  the  states  of  substances  in  solution 
must  be  assembled  to  provide  some  knowledge  of  the  concrete 
components  of  a  system  that  are  to  be  dignified  by  a  place  in  the 
equation.  Such  data  need  only  inform  us  of  the  initial  and 
final  products  of  the  cell  reaction;  and  because  we  are  then  con- 
cerned in  no  essential  way  with  the  true  path  of  the  reaction  or 
with  intermediate  products  we  cannot  be  said  to  be  dealing  funda- 
mentally with  the  mechanism.  By  the  same  token  we  are  at 
liberty  to  employ  artificial  hypotheses  of  intermediate  stages  if  it 
adds  anything  to  the  convenience  of  our  formulation;  for  we 

251 


252        THE  DETERMINATION  OF  HYDROGEN  IONS 

realize  at  the  introduction  of  these  hypotheses  that  they  are 
matters  of  convenience  only  and  are  destined  from  the  first  to  be 
eliminated  from  the  final  equations. 

We  shall  first  consider  Nernst's  (1889)  concept  of  electrolytic 
solution  tension  as  a  useful  way  of  remembering  certain  important 
relations. 

If  a  metal  be  placed  in  a  solution  of  its  salt  there  will  be  a  differ- 
ence of  electrical  potential  between  metal  and  solution  which  will 
vary  in  an  orderly  manner  with  the  concentration  of  the  metal 
ions.  To  account  for  the  difference  of  potential  Nernst  assumed 
that  a  metal  possesses  a  characteristic  solution  tension  comparable 
with  the  vapor  pressure  of  a  liquid,  or  better,  with  the  solution 
pressure  of  a  crystal  of  sugar — but  with  the  important  qualifica- 
tion that  it  is  the  metal  ions  which  pass  into  solution.  Imagine 
first  that  the  metal  is  in  contact  with  pure  water.  The  metal 
ions  passing  into  solution  carry  their  positive  charges  and  leave 
the  metal  negative.  Thus  there  is  established  a  so-called  double 
layer  of  electrical  charges  at  the  interface  between  metal  and  solu- 
tion, the  solution  being  positively  and  the  metal  negatively 
charged  relative  to  one  another.  This  potential  difference 
forcibly  opposes  further  dissolution  of  metallic  ions,  for  the 
relative  positive  electrical  field  in  the  solution  and  the  relative 
negative  field  in  the  metal  restrain  any  further  migration  of 
positively  charged  ions  from  the  metal  to  the  solution.  Equilib- 
rium is  established  when  the  electrostatic  control  equalizes  the 
solution  pressure. 

If  now  there  are  already  in  the  solution  ions  of  the  metal, 
fewer  ions  will  escape  from  the  metal  and  the  metal  is  left  more 
positive. 

Therefore  the  higher  the  concentration  of  the  positive  metallic 
ions  in  the  solution  the  more  positive  will  be  the  charge  on  the 
metal  and,  conversely,  the  lower  the  concentration  of  the  metallic 
ions  in  the  solution  the  more  negative  will  be  the  charge  on  the 
metal. 

Not  only  metals  but  various  gases  are  found  to  act  in  a  similar 
way  when  means  are  devised  to  bring  them  into  a  situation  as 
easily  handled  as  are  metal  electrodes.  Hydrogen  is  one  of  these 
gases  and  the  means  of  handling  it  as  an  electromotively  active 
gas  is  to  take  it  up  in  one  of  those  metals  such  as  platinum,  pal- 


XII 


HYDROGEN   CELL 


253 


ladium  or  iridium  which  in  a  finely  divided  condition  hold  large 
quantities  of  hydrogen.  Platinum  black  deposited  upon  plati- 
num and  laden  with  hydrogen  forms  a  hydrogen  electrode.  It 
can  be  brought  into  equilibrium  with  hydrogen  ions  as  silver  is 
brought  into  equilibrium  with  silver  ions ;  and  the  more  positive 
it  becomes  the  higher  must  be  the  concentration  of  the  positively 
charged  hydrogen  ions  in  the  surrounding  solution. 

The  metal-metal  ion  system  is  only  a  special  case  of  a  system 
the  components  of  which  differ  by  one  or  more  electrons.  Such 
systems  are  called  oxidation-reduction  systems.  The  system 
H2  :  H+  is  one  of  these.  If  we  assume  an  electron  escaping 
tendency  for  this  system,  we  can  formulate  the  relation  between 


p, 


FIG.  39.  DIAGRAM  OF  Two  HYDROGEN  HALF-CELLS  IN  LIQUID 

JUNCTION  AT  L 

I,  current  indicating  instrument  when  cell  is  allowed  to  run  or  poten- 
tiometer when  E.  M.  F.  is  to  be  balanced. 

the  cell's  electromotive  force  and  the  material  changes  by  the 
method  developed  in  Chapter  XVIII. 

Let  us  now  operate  with  the  cell  depicted  in  figure  39,  where 
one  solution  of  hydrion  concentration  [H+]i  is  under  the  hydrogen 
pressure  PI  and  the  other  solution  of  hydrion  concentration 
[H+]2  is  under  the  hydrogen  pressure  P2.  As  is  usual  in  the 
application  of  the  thermo dynamic  formulation  we  have  to  assume 
that  we  know  enough  about  the  mechanism  of  the  cell  to  describe 
its  main  function.  The  end  result,  which  is  all  we  need  to  know, 
is  the  lowering  of  hydrogen  pressure  and  the  raising  of  hydrion 
concentration  on  one  side,  the  raising  of  hydrogen  pressure  and 
the  lowering  of  hydrion  concentration  on  the  other  side,  and  the 


254  THE    DETERMINATION    OF   HYDROGEN   IONS 

accompanying  flow  of  a  definite  electric  current.  We  will 
assume  in  this  instance  that  hydrogen  will  pass  from  the  gaseous 
phase  on  one  side  to  yield  electrons  to  the  metal  and  to  pro- 
duce new  hydrions;  that  the  electrons  flow  through  the  exterior 
metal  connections  to  the  electrode  in  the  other  solution  and  that 
there  they  add  to  hydrions  and  form  new  hydrogen  molecules. 

Instead  of  allowing  the  cell  to  run  down  (with,  the  expenditure 
of  electrical  energy  and  the  approach  to  equalization  of  hydrogen 
pressure  and  hydrogen  ion  concentrations)  we  balance  the  electro- 
motive force  of  the  cell  potentiometrically.  We  then  assume 
that  any  compensating  adjustments  in  the  distribution  of  the 
other  ions  which  would  have  to  accompany  the  changes  in  hydrion 
concentration  play  no  direct  part  in  the  electrode  conduct  and 
that  events  at  the  liquid  junction  (L,  fig.  39)  are  to  be  handled 
by  the  method  of  Chapter  XIII. 

From  the  theory  presented  in  Chapter  XI  we  know  that  if  we 
have  hydrions  in  two  solutions  at  concentrations  [H+]i  and 
[H+J2  and  if  we  assume  that  the  ideal  gas  laws,  relating  tem- 
perature, pressure  and  concentration,  are  obeyed,  the  free  energy 
change  AF  for  the  transfer  of  one  gram  mole  of  hydrogen  ions  from 
the  higher  concentration,  [H+]i,  to  the  lower  concentration,  [H+]2, 
is  formulated  by  the  relation: 

-AF  =  RTZwj|5-1  (1) 

Lii"t"j2 

A  similar  relation  holds  for  the  transfer  of  one  gram  mole  of 
hydrogen  gas  from  pressure  PI  to  pressure  P2,  or,  for  one  equiva- 
lent of  hydrogen, 


-  AF  =  RT  In  —  (2) 


The  energy  lost  from  the  system  is  equal  to  the  work  done  by 
the  changing  system  under  the  conditions  of  maximum  work.  If 
the  work  which  would  be  done  by  the  current,  were  the  cell 
allowed  to  run,  is  expressed  in  electrical  terms  we  have 

-AF  =  EnF  (3) 

where  E  is  the  electrical  pressure  or  electromotive  force  that  we 
measure  in  volts  by  the  potentiomefcric  method  (see  Chapter  XVI) 


XII  HYDROGEN   CELL   EQUATION  255 

F  is  the  faraday,  the  quantity  of  electricity  associated  with  one 
electrochemical  equivalent  and  n  is  the  number  of  electrochemical 
equivalents. 

Then  equation  (1)  gives  that  part  of  the  free  energy  change 
associated  with  the  virtual  transfer  of  hydrions;  or  by  using  equa- 
tion (3)  with  (1)  and  assuming  n  =  1, 


A  second  portion  of  the  work  is  concerned  with  the  changing 
hydrogen  pressure,  and  for  one  equivalent  of  hydrogen 


E'F  =  RT  In  ~r=  (5) 

VP2 

But  on  any  one  side  the  hydrogen  pressure  tends  to  decline  and 
the  hydrion  concentration  to  rise  when  electrons  flow  from  this 
side  ;  on  the  other  side  the  hydrogen  pressure  tends  to  rise  and  the 
hydrion  concentration  to  decline  as  electrons  flow  in.  Hence  on 
any  one  side  the  effect  of  a  change  in  hydrogen  pressure  is  oppo- 
site to  that  of  a  change  in  the  same  direction  on  the  part  of  hydro- 
gen ion  concentration,  The  total  work  is  the  difference  : 

EF  -  E'F  =  RT  In  [H+]l     ^  (6) 

[H+]2  V  Px 

If  the  hydrogen  pressure  is  the  same  on  both  sides,  and  is  main- 
tained so,  we  have: 


As  explained  in  Chapter  XI,  and  as  noted  above,  the  measure- 
ment must  be  made  under  conditions  of  maximum  work.  This  is 
fulfilled  when  the  cell  is  not  allowed  to  run  but  is  held  with  its 
electromotive  force  nicely  balanced  by  a  potentiometer  (see 
Chapter  XVI).  It  is  the  electromotive  force  (E.  M.  F.)  of  the  cell 
as  if  on  open  circuit  that  is  measured  and  called  E  of  the  above 
equations.  Separating  E  we  have  from  (7) 

RT      [H+],  ,, 

E  =         iW 


256        THE  DETERMINATION  OF  HYDROGEN  IONS 

We  have  continued  up  to  this  point  with  the  assumption  that 
the  hydrions  obey  the  laws  of  an  ideal  gas.  Actually  they  do  not 
do  so  strictly  and  therefore,  if  we  are  to  be  strict  in  the  applica- 
tion of  the  equation,  we  should  substitute  for  concentrations  the 
corresponding  activities  of  the  hydrions.  The  FORM  of  the 
equation  then  remains  the  same.  See  the  previous  chapter.  Thus 
at  constant  hydrogen  pressure 

RT      (H+), 
In 


Here  it  will  be  recalled  that  we  use  parentheses  to  indicate  activity 
just  as  we  use  brackets  to  indicate  concentrations. 

It  will  also  be  recalled  that  in  Chapter  XI  attention  was 
directed  to  the  simple  proposition  of  using  the  hydrogen  electrode 
potentials  themselves  as  the  data  characteristic  of  solutions. 
With  only  a  formal  modification,  this  is  what  is  done  in  a  com- 
parative way  when  some  solution  is  given  an  arbitrary  hydrion 
activity  of  unity,  other  solutions  are  compared  with  it  and  the 
data  are  thrown  into  the  form  which  at  25°,  for  example,  will  be 

E  1 

0.05912          B  (H+) 
Compare  with 


The  significance  of  the  equation  for  the  "concentration"  chain 
is  that,  if  T  is  known,  and  if  the  activity  of  the  ions  in  the  other 
solution  is  known,  then  the  activity  of  the  ions  in  one  solution  can 
be  determined  from  the  E.  M.  F.  of  the  chain.  Fundamentally 
there  is  no  other  way  of  applying  electromotive  force  determina- 
tions to  the  estimation  of  ion  activities,  unless  there  can  be  brought 
to  bear  mass  action  relations.  This  makes  it  necessary  to  start 
somewhere  in  the  system  with  a  solution  whose  hydrogen  ion 
activity  has  been  determined  by  an  independent  method. 

But  let  us  assume  the  concentration  formulation  and  let  us 
assume  for  the  moment  that  the  conductivity  method  will  give 
us  correct  information  upon  the  hydrogen  ion  concentration  of 
some  simple  solution  such  as  that  of  HC1. 


XII  NORMAL  HYDROGEN    ELECTRODE  257 

It  will  be  remembered  that  hydrogen  ion  concentrations  are 
expressed  in  terms  of  normality,  a  solution  normal  with  respect 
to  hydrogen  ions  being  one  which  contains  in  one  liter  of  solution 
1  gram1  of  hydrogen  ions. 

If,  then,  the  normality  of  the  hydrogen  ion  concentration  in 
any  unknown  solution  is  to  be  determined  it  would  seem  that  the 
most  convenient  solution  with  which  to  compare  the  unknown 
would  be  a  solution  of  normal  hydrogen  ion  concentration.  Be- 
tween a  hydrogen  electrode  in  this  standard  and  a  hydrogen  elec- 
trode in  the  unknown  solution  of  hydrogen  ion  normality  [H+]x 
there  would  be  a  difference  of  potential,  E  given  by  the  equation  : 

E  =  0.000,198,322  T  logz^rr  (10) 


A  measurement  of  E  and  T  would  give  [H+]x.  Now  E  in  the 
above  equation  is  the  difference  between  the  potential  difference  at 
the  one  hydrogen  electrode  and  the  potential  difference  at  the  other 
hydrogen  electrode.  Nothing  need  be  known  about  the  value  of 
either  single  potential  difference  and  very  little  is  known.  If  the 
electrode  in  the  normal  solution  is  made  the  standard  it  is  ob- 
viously convenient  for  present  purposes  to  call  the  potential 
difference  between  this  electrode  and  the  solution  zero.  Thus 
arose  the  definition: 

The  potential  at  a  hydrogen  electrode  under  one  atmosphere 
pressure  of  hydrogen  in  a  hypothetical  solution  normal  with 
respect  to  the  hydrogen  ion  shall  be  considered  to  be  zero  at  all 
temperatures.2 

To  conform  to  the  use  of  "activity"  this  may  be  modified  to: 

The  potential  at  a  hydrogen  electrode  under  one  atmosphere  pres- 
sure of  hydrogen  in  a  solution  of  unit  hydrion  activity  shall  be  con- 
sidered to  be  zero  at  all  temperatures. 

The  term  "normal  hydrogen  electrode"  is  now  associated  with 
the  latter  definition. 

1  It  makes  little  difference  whether  we  regard  the  atomic  weight  of 
hydrogen  as  1.0  or  as  1.008  for  the  purpose  at  hand. 

2  In  various  places,  notably  in  the  report  of  the  Potential  Commission 
of  the  Bunsen-Gesellschaft  (Abegg,  Auerbach  and  Luther,  1910)  it  is  not 
specifically  stated  that  this  difference  of  potential  shall  be  zero  at  all  tem- 
peratures, but  it  seems  to  have  been  so  understood  and  is  specifically  so 
stated  by  Lewis  (1913). 


258  THE    DETERMINATION    OF   HYDROGEN   IONS 

Having  established  by  definition  the  value  of  the  potential 
difference  at  the  ' 'normal  hydrogen  electrode"  it  becomes  con- 
venient to  speak  of  the  potential  difference  at  any  other  hydrogen 
electrode  as  the  hydrogen  electrode  potential,  thus  abbreviating 
the  term  ' 'potential  difference."  It  is,  of  course,  implied  that 
such  a  "potential"  is  referred  to  the  potential  difference  at  the 
normal  hydrogen  electrode.  To  indicate  this  the  symbol  Eh  is 
used. 

Unfortunately  the  standard  solution  would  have  to  be  pre- 
pared by  means  of  "strong"  acids  and  the  estimation  of  the 
hydrogen  ion  activity  would  fall  under  those  uncertainties 
which  we  shall  leave  to  Chapter  XXIII  for  discussion.  In  the 
meantime  we  shall  assume  that  a  well  established  standard  is 
available  and  that  this  conforms  to  the  demand  of  the  rigid 
equation  for  which  the  standard  should  be  unit  activity  instead 
of  the  unit  concentration.  With  this  we  could  proceed  to  the 
comparison  of  all  solutions  applying  directly  the  formula  which 
relates  the  E.  M.  F.  of  a  "concentration  cell"  to  the  ratio  of 
activities  (or  for  approximate  purposes  to  concentrations).  But 
it  is  more  convenient  to  substitute  for  the  standard  a  "working 
standard"  known  as  the  calomel  half-cell.  (See  Chapter  XV.) 
When  this  is  joined  to  a  hydrogen  half-cell  we  need  to  know 
the  potential  difference  between  the  calomel  half-cell  and  the 
ultimate  hydrogen  standard.  Then  we  can  correct  the  observed 
E.  M.  F.  by  this  difference  and  can  consider  the  corrected  E.  M.  F. 
to  be  as  if  it  were  that  between  two  hydrogen  half-cells  for  which 
we  have  the  above  formula. 

We  have  continued  with  the  assumption  that  there  is  no  dif- 
ference of  potential  in  a  cell  other  than  those  at  the  electrode- 
solution  interfaces.  As  a  matter  of  fact  a  potential  difference 
arises  wherever  too  unlike  solutions  are  put  in  liquid  junction. 
The  importance  of  this  and  the  attendant  difficulties  are  the 
occasion  for  a  separate  chapter  on  the  subject.  See  Chapter 
XIII. 

ON   THE    SIGN    OF   ELECTRODE   POTENTIALS 

Convention  in  regard  to  signs  will  be  discussed  again  in  Chapter 
XVIII.  Here  it  may  be  said  that  we  shall  use  the  convention  to 
be  used  by  International  Critical  Tables.  The  metal  of  the 


-.7 


+.6 


+.5 


+.3 
+.2 

4.1 


O.I  N.  CAL.  AT  20° 


0.1  N.  CAL.  AT  40* 


^SAT.  CAL.  AT  20' 


SAT.  CAL.  AT  40' 


FIG.  40.  RELATION  BETWEEN  pH  AND  CHANGE  OF  POTENTIAL  OF  THE 
METAL  OF  A  HYDROGEN  ELECTRODE  (AT  20°C.  AND  40°C.)  RELATIVE 

TO  ZERO  POTENTIAL  OF  THE  NORMAL  HYDROGEN  ELECTRODE 
Also  the  change  of  potential  of  the  quinhydrone  electrode  with  change 
of  pH  (see  Chapter  XIX).     Also  positions  of  arbitrarily  assigned  poten- 
tials of  0.1  N  and  saturated  calomel  half -cells   (see  Chapter  XXIII). 
Compare  this  figure  with  table  A,  Appendix. 

259 


260         THE  DETERMINATION  OF  HYDROGEN  IONS 

hydrogen  electrode  then  appears  to  become  more  negative  as  the 
pH  value  of  the  solution  increases.  Figure  40  shows  this  rela- 
tion and  also  the  orientation  of  the  potential  of  the  metal  of  a 
hydrogen  electrode  in  a  solution  of  any  pH  relative  to  the  poten- 
tial of  the  mercury  of  calomel  half-cells. 

BAROMETRIC    CORRECTIONS 

While  we  included  at  one  point  the  effect  of  varying  hydrogen 
pressure  we  continued  the  later  discussion  under  the  assumption 
that  the  hydrogen  electrode  is  operating  with  one  atmosphere 
pressure  of  hydrogen.  If  the  hydrogen  pressure  varies  from  this, 
the  above  equation  is  incomplete.  Instead  of  reincorporating 
the  hydrogen  pressure  in  the  working  equation  it  is  more  con- 
venient to  deal  with  a  variation  of  hydrogen  pressure  as  a  cor- 
rection. 

The  potential  difference  between  a  metal  and  solution  will  vary 
somewhat  with  the  condition  of  the  metal.  A  hammered,  twisted 
or  scratched  electrode  may  show  a  different  potential  against  a 
given  concentration  of  its  ions  than  will  an  electrolytically  de- 
posited metal.  In  the  case  of  the  hydrogen  electrode  it  seems 
to  make  little  difference  whether  the  hydrogen  be  held  in  platinum, 
palladium  or  iridium  but  it  does  make  a  considerable  difference 
if.  the  surrounding  pressure  of  hydrogen  varies.  If  we  have  two 
hydrogen  electrodes  immersed  in  the  same  solution  at  the  same 
temperature  but  under  different  pressures  of  gaseous  hydrogen, 
we  may  assume  that  the  concentration  of  the  hydrogen  in  one 
electrode  is  different  from  that  in  the  other  electrode,  and  that 
the  potential  difference  may  be  expressed  as 

(11) 


in  which  equation  R,  T,  n,  and  F  have  their  customary  signifi- 
cances and  [H]i  and  [H]2  are  concentrations  of  atomic  hydrogen  in 
the  electrodes  (platinum  black).  Since  n  is  1,  it  may  be  omitted. 
We  may  now  assume  that  there  is  an  equilibrium  between  the 
molecular  hydrogen  about  the  electrode  and  the  atomic  or  ionic 
hydrogen  in,  or  issuing  from,  the  electrode.  This  equilibrium 
may  be  expressed  in  accordance  with  the  mass  law  as  follows: 


XII  BAROMETEIC    CORRECTION  261 

[HI  X  TH1 

-  —  J        —  -  =  K  where  [H]  =  concentration  of  atomic  hydrogen 
1H2] 

and  [H2]  =  concentration  of  molecular  hydrogen 
Whence, 

[H]  =  \/K[ij  (12) 

Substituting  (12)  in  (11),  we  have 


E     .  RT  K  RT 


F         VK[H2]2         2F       [H2]2 

It  should  be  noted  that  the  factor  2  in  this  equation  does  not 
come  from  giving  hydrogen  an  effective  valence  of  2,  as  has  often 
been  stated,  but  from  the  introduction  of  equation  (12). 

If  the  ratio  of  pressures  is  equal  to  the  ratio  of  gas  concen- 
trations 


2F       PH2 
If  P'H2  be  one  atmosphere  and  PH2  be  expressed  in  atmospheres 


This  is  the  equation  for  the  difference  of  potential  between  a 
hydrogen  electrode  under  one  atmosphere  pressure  of  hydrogen 
(e.g.,  the  normal  hydrogen  electrode)  and  a  hydrogen  electrode 
under  pressure  Pn2. 

Experimental  justification  of  this  equation  is  found  in  the  ex- 
periments of  Wulf,  Czepinski,  Lewis  and  Rupert,  Lewis  and 
Randall,  Lewis  and  Sargent,  Ellis,  Loomis  and  Acree  and  others. 

Hainsworth,  Rowley  and  Maclnnes  (1922,  1924)  have  studied 
the  effect  of  pressures  up  to  1000  atmospheres  and  taking  account 
of  the  volume  changes  of  Hg,  calomel,  etc.  which  are  negligible 
for  smaller  differences  in  pressure,  they  find  a  linear  relation 
up  to  100  atmospheres. 

Several  writers  have  felt  constrained  to  emphasize  the  fact  that 
in  determining  the  hydrogen  pressure  from  barometer  readings 
they  have  subtracted  the  vapor  pressure  of  the  solution.  The 


262  THE    DETERMINATION    OF   HYDROGEN   IONS 

emphasis  is  still  advisable,  for  a  considerable  number  of  precise 
hydrogen  electrode  data  are  published  with  corrections  for  baro- 
metric pressure  on  the  basis  that  the  normal  hydrogen  electrode 
pressure  is  one  atmosphere  including  the  vapor  pressure  of  the 
solution.  Corrections  should  be  made  to  one  atmosphere  pres- 
sure of  hydrogen,  or  else  the  standardised  should  be  distinctly 
specified. 

Clark  and  Lubs  (1916)  used  the  commonly  accepted  "standard 
condition"  of  a  gas  which  is  the  concentration  at  0°C.  and  760 
mm.  pressure.  Their  final  values  were  not  thereby  rendered 
incomparable  with  other's  values  since  the  correction  was  applied 
to  the  standard  as  well. 

In  applying  the  correction, 


bar. 


2F        PHt  ' 


it  will  be  remembered  that  a  decrease  of  the  hydrogen  pressure 
may  be  considered  as  a  decrease  of  the  electrolytic  solution 
tension  of  the  hydrogen.     Hence  under  decreased  hydrogen  pres- 
sure the  electrode  is  left  more  positive.     See  figure  77,  page  387. 
In  the  cell 

-  PtlH,|H+lKCl,HgCl|Hg+ 

if  the  hydrogen  is  under  diminished  pressure  the  E.  M.  F.  of  the 
cell  is  too  low.  Hence  the  correction  must  be  applied  to  make 
the  E.  M.  F.  larger  than  observed.  The  working  equation  is 
then: 

E.M.F.  +E(bar.)   —  E  (calomel)    __      TT  /-j^X 

0.000198322  T 

To  aid  in  the  calculation  of  pressure  corrections  it  is  convenient 
to  plot  a  curve  giving  the  millivolts  to  be  added  to  the  observed 
E.  M.  F.  for  various  corrected  partial  pressures.  Tables  of  correc- 
tions from  which  a  chart  may  be  plotted  are  given  in  the  Appen- 
dix. In  these  tables  the  barometer  pressures  given  are  the  cor- 
rected pressures.  If  hydrogen  escapes  from  about  the  hydrogen 


XII  BAROMETRIC    CORRECTION  263 

electrode  through  a  trap3  or  other  device  which  exerts  back  pres- 
sure, this  pressure  must  be  taken  into  consideration.  Otherwise 
it  is  assumed  that  the  pressure  of  the  hydrogen  is  that  of  the 
barometer  less  the  vapor  pressure  of  the  solution. 

For  all  ordinary  cases  it  may  be  assumed  that  the  vapor  pres- 
sure is  that  of  pure  water  at  the  temperature  indicated. 

If  the  unit  pressure  is  one  atmosphere,  the  partial  pressure 
must  be  reduced  to  atmospheres. 

As  inspection  of  the  table  in  the  Appendix  will  indicate,  the 
barometric  correction  may  be  neglected  in  rough  measurements. 
.But  in  very  exact  measurements  it  is  necessary  to  make  the  usual 
corrections  for  the  barometer  reading. 

3  It  is  good  practice  to  prevent  back  diffusion  of  oxygen  by  letting  the 
hydrogen  escape  through  a  long  but  not  too  narrow  tube  instead  of  through 
a  trap. 


CHAPTER  XIII 

POTENTIAL  DIFFERENCES  AT  LIQUID  JUNCTIONS 

Until  a  problem  has  been  logically  defined  it  cannot  be  experimentally 
solved. — LEWIS  AND  RANDALL. 

INTRODUCTION 

By  far  the  most  unsatisfactory  aspect  of  electric  cells  is  the 
interference  of  the  liquid  junction  with  simple  and  certain  formu- 
lation of  the  electromotive  force  of  the  cell.  Whenever  two  solu- 
tions of  different  composition  are  brought  in  contact  with  one 
another  there  develops  at  the  junction  a  potential  difference. 
Since  the  structure  of  the  junction  is  not  a  permanent  affair,  the 
ordinary  principles  of  equilibria  are  difficult  to  apply.  Prac- 
tically the  junction  is  difficult  to  reproduce  in  a  manner  which 
will  furnish  a  reproducible  potential  with  solutions  of  different 
electrolytes. 

So  troublesome  has  this  matter  proved  to  be  that  the  tendency 
in  theoretical  work  is  definitely  toward  the  selection  of  those  cells, 
which,  from  a  practical  point  of  view,  have  no  liquid  junction  and, 
from  a  theoretical  point  of  view,  can  be  formulated  as  if  they  had 
none.  An  example  of  such  a  cell  is  that  described  by: 

-  Pt,  H2  (1  atmos.)  1  HC1  (0.1M),  HgCl  (s)  |  Hg  +, 

namely,  a  cell  composed  of  a  hydrogen  electrode  under  one  atmos- 
phere of  hydrogen  and  a  mercury  electrode  covered  by  mercurous 
chloride  (solid  phase  in  excess),  both  in  the  "same"  solution  of 
tenth  molar  hydrochloric  acid. 

If,  in  considering  this  cell,  we  were  to  keep  uppermost  in  mind 
the  principles  of  oxidation-reduction  equilibria  (see  Chapter 
XVIII),  we  might  doubt  the  practicability  of  the  cell,  because  the 
difference  between  the  potentials  at  the  two  electrodes  is  so  large 
that  we  would  conclude  at  once  that  the  mercurous  chloride 
should  be  reduced  by  the  H2:H+  system  (at  the  platinum  elec- 
trode, at  least,  if  not  in  the  solution  itself).  As  a  matter  of  fact 

264 


XIII  LIQUID   JUNCTION   POTENTIAL  265 

this  difficulty  has  arisen1  and  the  higher,  more  reproducible  po- 
tentials of  the  cell  are  obtained  by  a  degree  of  isolation  of  the 
solutions  about  the  two  electrodes.  Then  these  solutions  are 
made  different,  the  one  being  saturated  with  mercurous  chloride 
and  the  other  not.  Theoretically  a  liquid  junction  potential 
might  be  present;  but,  because  of  their  very  low  concentration, 
the  mercury-  and  chloride  ions  in  excess  upon  the  one  side  have 
no  practically  significant  effect  in  the  liquid  junction. 

Such  cells  are  sometimes  called  "cells  without  liquid  junction" 
or  "cells  without  transference."  Those  cells  in  which  there  occurs 
a  liquid  junction  which  has  to  be  considered  are  sometimes  called 
"cells  with  transference." 

By  ingenious  combinations  of  the  data  for  cells  without  trans- 
ference it  has  been  possible  in  recent  years  to  build  a  considera- 
ble body  of  important  data.  But  unfortunately  the  solutions 
met  in  the  wider  applications  of  cell  measurements  are  so  varied 
that  the  introduction  of  liquid  junctions  is  a  necessity  in  the 
majority  of  cases.  We  shall  find  that  such  junctions  introduce  a 
serious  uncertainty  into  what  would  otherwise  be  a  most  precise 
account  of  acid-base  equilibria. 

In  writing  the  structure  of  a  cell,  it  is  customary  to  designate 
the  position  of  a  potential  difference  by  a  vertical  line.  When 
such  a  potential  difference  is  to  be  considered  as  eliminated  a 
double  line  is  used.  Thus 

Pt,  H2 1  N/10  HC1 1  N/10  KC1,  HgCl  |  Hg 

indicates  that  there  are  potential  differences  at  the  positions 
shown  by  the  lines;  while  if  the  above  chain  is  written  as 

Pt,  H2 1  N/10  HC1 1|  N/10  KC1,  HgCl  |  Hg 

the  double  line  indicates  that  the  liquid  junction  potential  dif- 
ference is  to  be  left  out  of   consideration  in  formulating  the 
E.M.F.,  it  having  been  allowed  for  by  some  separate  treatment. 
Scatchard  (1925)  has  departed  from  this  convention  by  using 

1  Nonhebel  (1926)  has  not  found  this  difficulty  with  the  silver-silver 
chloride  half -cell. 


266 


THE    DETERMINATION    OF   HYDROGEN   IONS 


the  double  line  to  indicate  a  flowing  junction.     We  shall  signify 
a  flowing  junction  by  a  waved  line,  for  instance, 

N/lOHCljN/lOKCl 
The  flowing  junction  is  described  on  page  274. 

THE  CAUSE 

The  principal  cause  of  the  potential  difference  was  attributed 
by  Nernst  (1889)  to  unequal  rates  of  diffusion  of  ions  across  the 
junction. 

It  has  been  found  in  the  study  of  electrolytic  conduction  that, 
under  uniform  potential  gradient,  different  ions  move  through  a 
solution  with  different  velocities.  The  following  table  taken  from 
Lewis'  A  System  of  Physical  Chemistry  shows  the  velocites  of 
several  ions  in  aqueous  solution  under  a  potential  gradient  of  one 
volt  per  centimeter. 

TABLE  50 

Ionic  velocities 


ION 

ABSOLUTE 
VELOCITY  IN 
CENTIMETEE8 
PER  SECOND, 
18°C. 

ION 

ABSOLUTE 
VELOCITY  IN 
CENTIMETERS 
PER  SECOND, 
18°C. 

H+               

32  50  10  ~4 

OH~ 

17.80  10  ~4 

K+ 

6  70  10  ~4 

cr~ 

6.78  10~4 

Na+            .       ... 

4  51  10  ~4 

N03~         

6.40  10~4 

Li+  

3.47  10~4 

CHsCOCr  

3.20  10~4 

Ag+ 

5  70  10  ~4 

Since,  in  each  case,  the  potential  gradient  is  the  same  and  the 
ionic  charge  the  same,  it  may  be  inferred  that  the  order  in 
which  the  velocities  stand  in  the  table  is  the  order  in  which  the 
velocities  of  free  movement  will  stand. 

Let  it  now  be  assumed  that  a  solution  of  hydrochloric  acid  is 
placed  in  contact  with  pure  water  of  negligible  ion  content  at  an 
imaginary  plane  surface.  Independently  of  one  another  the 
chloride  and  the  hydrogen  ions  will  tend  to  migrate  across  the 
interface  and  into  the  water.  As  shown  in  the  above  table  the 
velocity  of  the  hydrogen  ion  under  the  influence  of  a  potential 
gradient  is  much  greater  than  the  velocity  of  the  chloride  ion 


XIII  FORMULATION  267 

under  the  same  gradient,  and  the  relative  velocities  of  free  move- 
ment must,  therefore,  be  in  the  same  proportion.  Consequently 
there  will  be  established  on  the  water  side  of  the  plane  an  excess 
positive  charge.  This  charge  will  increase  until,  by  the  electro- 
static attraction  the  slower  moving  chloride  ions  are  brought  to 
the  velocity  of  the  hydrogen  ions.  When  this  state  is  reached, 
as  it  is  almost  instantaneously,  there  is  established  a  potential 
difference  at  the  liquid  junction.  If  the  water  is  replaced  by  a 
solution  of  an  electrolyte,  we  have  not  only  the  chloride  and  the 
hydrogen  ions  migrating  across  the  boundary  into  this  new  solu- 
tion, but  the  ions  of  this  solution  migrating  into  the  hydrochloric 
acid  solution. 

FORMULATIONS 

Before  modern  requirements  led  to  a  reexamination  of  all  the 
assumptions  entering  attempts  to  formulate  liquid  junction 
potentials  it  was  considered  legitimate  to  operate  with  free  energy 
equations  expressed  with  concentrations  and  with  transport  num- 
bers considered  to  be  independent  of  the  environment.  Merely 
as  an  illustration  consider  the  comparatively  simple  case  where 
two  solutions  of  different  concentrations  of  the  same  binary 
electrolyte  are  placed  in  contact. 

Let  the  concentration  of  the  ions  on  one  side  of  the  interface 
be  C  and  on  the  other  side  be  a  lesser  concentration  C', 

When  migration  has  established  the  steady  potential  EL  let 
it  be  over  an  interface  of  such  extent  that  EL  is  due  to  the  separa- 
tion of  one  faraday.  If  that  fraction2  of  the  separated  charge 
which  is  carried  by  the  anion  is  n,  the  work  involved  in  the  trans- 

C 

port  of  n  equivalents  from  C  to  C'  is  n  RT  In  ™*     Likewise,  if 

L» 

that  fraction  of  the  charge  carried  by  the  cations  is  1  — n,  the 
work  involved  in  the  transport  of  1— n  equivalents  from  C  to  C' 

C 

is  (1  — n)  RT  In  p-/     The  work  involved  in  the  separation  of  the 

ions  as  they  migrate  from  the  high  to  the  low  concentration  is 

ELF  =  nRT  In  %  -  (1  -  n)  RT  In  ^ 
O  O 

2n  =  transport  number. 


268         THE  DETERMINATION  OF  HYDROGEN  IONS 

Whence 

r>rp  /-i 

EL  =  (2n-l)^Z«g  (1) 

Equation  (1)  was  derived  on  the  assumption  that,  in  the  formu- 
lation of  energy  changes,  concentration  ratios  can  be  substituted 
for  activity  ratios  and  on  the  assumption  that  the  activities  of 
the  ions  of  opposite  charge  are  equal  to  the  corresponding  con- 
centration. Omitting  these  assumptions  we  would  find  the  equa- 
tion to  be  as  follows  for  two  solutions  of  hydrochloric  acid 


Here,  as  elsewhere  in  this  book,  ()  indicates  activity.  nc  and  na 
are  the  transport  numbers  of  cations  and  anions  respectively  at 
the  states  found.  Equation  (2)  makes  it  evident  that  a  com- 
plete solution  for  EL  would  require  knowledge  of  the  individual 
ion  activities  in  the  two  solutions.  In  this  connection  we  may 
quote  Harned  (see  page  782  Taylor's  A  Treatise  on  Physical 
Chemistry).  "Thermodynamics  offers  valuable  aid  in  the  study 
of  liquid  junction  potentials,  but  it  is  not  possible  by  thermo- 
dynamic  methods  alone  to  evaluate  liquid  junction  potentials, 
since  a  knowledge  of  individual  ion  activities  would  be  required. 
We  are  thus  confronted  with  the  interesting  perplexity  that  it  is 
not  possible  to  compute  liquid  junction  potentials  without  a 
knowledge  of  individual  ion  activities,  and  it  is  not  possible  to 
determine  individual  ion  activities  without  an  exact  knowledge 
of  liquid  junction  potentials.  For  the  solution  of  this  difficult 
problem,  it  is  necessary  to  go  outside  the  domain  of  exact  thermo- 
dynamics." 

Lewis  and  Sargent  (1909)  have  treated  the  special  case  of  two 
equally  concentrated  solutions  of  two  different  uni-univalent  salts 
having  one  ion  in  common.  Substituting  equivalent  conduc- 
tivities as  proportional  to  mobilities  they  obtain 


(3) 


XIII 


LIQUID   JUNCTION   POTENTIALS 


269 


where  Xi  and  X2  are  the  equivalent  conductivities  of  two  solutions. 
In  their  experimental  study  of  cells  of  the  type 

Ag  |  AgCl,  HCl(c)  |  KC1,  (c),  AgCl  |  Ag. 
ABC 

Maclnnes  and  Yeh  (1921)  assume,  for  purposes  of  calculation, 
that  the  activities  of  the  chloride  ions  in  the  two  solutions,  of 
KC1  and  HC1,  are  the  same  when  these  two  solutions  have  the 
same  concentration,  c.  Then  the  potential  difference  ascribed 
to  A  should  be  the  same  as  that  ascribed  to  C  and  the  electro- 
motive force  of  the  cell  should  be  the  liquid  junction  potential  at  B. 

TABLE  51 

Potentials  at  junctions  of  solutions  of  univalent  chlorides 
25°C. 


O.lN  SOLUTION 

O.OlN  SOLUTIONS 

ELECTROLYTES  AT 
JUNCTION 

"Observed" 
Maclnnes  and 
Yeh 

Calculated 
Lewis 
and  Sargent's 
formula 

"Observed" 
Maclnnes  and 
Yeh 

Calculated 
Lewis 
and  Sargent's 
formula 

volts 

volts 

volts 

volts 

HC1;  KC1 

0.02578 

0.02840 

0.02572 

0.02740 

HC1;  NaCl 

0.03309 

0.03330 

0.03116 

0.03190 

HC1;  NH4C1 

0.02840 

0.02860 

0.02702 

0.02740 

KC1;  NaCl 

0.00642 

0.00490 

0.00565 

0.00450 

NaCl;  NH4C1 

-0.00424 

-0.00460 

-0.00426 

-0.00450 

With  this  assumption  the  observed  potentials  can  be  compared 
directly  with  those  calculated  by  Lewis  and  Sargent's  formula  as 
in  table  51. 

Scat  chard  (1925)  has  calculated  the  junction  potential  at  A, 
below,  to  be  0.0027  volt  and  at  B  to  be  0.0047  volt. 

KC1  (0.1M)  $  KC1  (sat.) 

+A- 
HC1  (0.1M)  $  KC1  (sat.) 

-B+ 

These  estimates  are  of  considerable  importance  to  the  stand- 
ardization of  pH  values  as  will  appear  in  Chapter  XXIII. 


270         THE  DETERMINATION  OF  HYDROGEN  IONS 

Earned  (1926)  has  considered  in  detail  a  calculation  of  the 
liquid  junction  potentials  at 

HCl(O.l),  KC1(M)  |  KC1  (sat.) 
when  M  is  varied  from  0  to  3.     He  gives  the  following  results. 


M 

JUNCTION  POTENTIAL 

volts 

0.0 

0.00158 

0.3 

0.00105 

0.5 

0.00089 

1.0 

0.00082 

2.0 

0.00085 

3.0 

0.00082 

The  potentials  of  liquid  junctions  between  solutions  of  the  same 
electrolyte  at  different  concentrations  are  independent  of  the 
manner  in  which  the  junction  is  formed  provided  no  membrane 
is  interposed.  In  contrast  to  this  the  potentials  at  the  junctions 
of  solutions  of  different  electrolytes  vary  with  the  manner  in 
which  the  junction  is  formed.  If,  in  addition,  the  solutions  are 
complex  the  problem  of  formulation  becomes  extremely  difficult 
or  impossible  of  numerical  solution. 

Among  the  more  important  formulations  there  should  be 
mentioned  the  following.  Planck  (1890)  assumed  the  junction 
to  be  initially  sharp  and  mixing  to  take  place  by  diffusion.  Pro- 
ceeding from  Nernst's  formulation  he  reached  an  equation  which 
has  served  as  a  valuable  guide.  Johnson  (1904)  extended  the 
formula  to  the  case  where  the  valences  of  the  ions  are  not  the  same. 
P.  Henderson  (1907,  1908)  treated  the  case  of  a  "mixture  bound- 
ary," one  in  which  the  intervening  layer  is  made  up  of  a  series  of 
mixtures  of  the  two  solutions  in  graded  proportions.  Gumming 
(1912)  modified  the  equation  by  introducing  the  mobilities  of 
the  ions  at  the  different  concentrations  used.  These  and  nu- 
merous other  treatments  have  been  appreciably  modified  by  the 
realization  that  it  is  more  consistent  with  the  use  of  free-energy 
equations  to  employ  activities  in  place  of  concentrations  and  also 
by  the  realization  that  ion  mobilities  vary  with  the  nature  and 
concentration  of  the  solution. 


XIII  METHODS    OF   FORMING   JUNCTIONS  271 

What  appears  to  be  a  comprehensively  general  treatment  has 
recently  been  published  by  Taylor  (1927).  Of  particular  im- 
portance to  our  subject  is  Taylor's  development  of  the  idea  that, 
if  the  electromotive  force  of  a  cell  with  transference  is  to  be 
formulated  rigidly,  the  cell  should  be  treated  as  a  whole,  and  that 
separate  treatment  of  liquid  junction  potentials  must  be  regarded 
as  a  convenient  grouping  of  terms  and  without  physical  sig- 
nificance. He  pertinently  remarks  that  the  electromotive  forces 
of  cells  commonly  used  for  the  determination  of  pH  numbers 
depend  not  only  upon  the  activity  of  the  acid  but  also  on  the 
activity  of  every  molecular  species  and  on  the  mobility  of  every 
ion.  "If  these  are  sufficiently  well  known  to  be  allowed  for,  the 
acid  activity  is  likely  to  be  sufficiently  well  known  not  to  need 
measurement." 

To  meet  the  demands  of  rigid  treatment  there  is  very  little 
that  can  be  done  with  ordinary  measurements,  but  we  shall  see 
in  a  subsequent  section  that  the  elementary  theory  predicts 
moderate  success  in  the  approach  to  what  may  be  considered  for 
practical  purposes  a  relatively  low,  constant  liquid  junction  po- 
tential against  a  solution  saturated  with  KC1.  Before  this  is 
discussed  let  us  consider  certain  experimental  matters  of  im- 
portance. 

METHODS   OF   FORMING   LIQUID    JUNCTIONS 

For  a  reason  to  be  discussed  in  the  next  section,  liquid  junc- 
tions between  solutions  of  different  electrolytes  are  usually  formed 
by  interposing  a  solution  of  potassium  chloride.  Usually  this  is 
a  saturated  solution.  Since  this  saturated  solution  is  frequently 
the  more  dense  of  the  two  solutions  placed  in  contact  it  is  led 
to  the  junction  from  below. 

Experience  has  suggested  the  advisability  of  avoiding  junction 
in  capillary  spaces  (Gumming  and  Gilchrist,  1923).  If  a 
capillary  is  desired  (to  delay  change  of  structure  at  the  junction 
during  treatment  of  a  solution)  the  arrangement  indicated  in 
figure  49,  page  301,  is  useful.  There  a  wide  liquid  junction  is 
found  in  the  bulb.  It  is  protected  from  the  titrated  solution 
by  the  capillary  goose-neck.  For  bridging  between  open  vessels 
there  is  a  wide  variety  of  devices  of  which  only  a  few  are  shown 
in  figure  41. 


272 


THE  DETERMINATION  OF  HYDROGEN  IONS 


Agar  saturated  with  KC1  is  sometimes  very  convenient. 
Michaelis  and  Fujita  (1923)  prepare  this  as  follows.  Agar  (3 
grams)  is  thoroughly  melted  in  100  grams  water.  Avoid  direct 
flame.  Heat  in  steam  sterilizer  or  water  bath.  Add  40  grams 
KC1  and  stir  gently  till  dissolved.  Pour  the  mixture  while  hot 
into  the  tube  and  then  cool.  Gelfan  (1926)  described  an  agar- 
KC1  junction  made  in  a  quartz  capillary  1-2  microns  in  diameter. 

Wicks  have  sometimes  been  used.  See,  for  instance,  Michaelis 
(1914)  and  Walpole  (1914). 

Very  frequently  a  membrane,  such  as  parchment  or  collodion, 
(cf.  Fales  and  Stammelman,  1923)  is  used  at  the  junction.  There 
are  instances  of  routine  measurements  in  which  this  practice  is 
desirable.  On  the  other  hand  it  may  seriously  complicate  the 


FIG.  41.  "SIPHONS"  FOR  BRIDGES 
Upper  siphons  contain  agar-KCl 

situation  and  render  more  difficult  the  interpretation  of  the  cell's 
electromotive  force.  (Cf.  Prideaux  and  Crooks,  1924.)  For  the 
introduction  of  a  membrane  is  virtually  the  introduction  of  a  new 
phase  and  one  junction  is  replaced  by  two.  Usually  the  junction 
potential  is  increased.  This  has  been  accounted  for  on  the 
assumption  of  a  disproportionate  change  in  the  transport  num- 
bers of  the  ions  as  they  enter  the  membrane  phase.  In  the  dis- 
cussion of  non-aqueous  solutions  there  will  be  a  brief  sketch  of 
phase  boundary  potentials  and  the  subject  could  appropriately 
be  discussed  here.  However,  it  is  a  very  large  subject  with  an 
extensive  and  highly  technical  literature.  To  discuss  this  for 
the  sake  of  an  adequate  presentation  of  devices  which  so  far 
have  found  comparatively  little  use  in  the  exact  application  of 


XIII  DRIFT   OF  JUNCTION   POTENTIAL  273 

the  hydrogen  electrode  would  hardly  be  profitable.  It  may 
simply  be  said  that,  while  the  interposition  of  a  membrane  is 
sometimes  useful  in  comparative,  routine  measurements;  it  is 
usually  avoided  in  fundamental  studies  except  of  the  membrane 
potential  itself.  See  Michaelis  (1926). 

Aqueous  gels  do  not  have  such  a  serious  effect  upon  relative 
migration  velocities  as  do  membranes  such  as  parchment ;  but  that 
agar  bridges  are  not  in  good  repute  for  exact  work  is  well  known. 
For  instance  Lamb  and  Larson  (1920)  in  speaking  of  their  own 
use  of  an  agar-KCl  bridge  remark  "Under  ordinary  circumstances 
this  type  of  junction  would  not  have  been  adopted  for  it  does 
not  give  the  utmost  accuracy."  But  see  Michaelis  and  Fujita 
(1923)  who  are  of  the  opposite  opinion  for  a  particular  arrangement. 
See  page  279. 

In  their  study  of  transference  numbers  Maclnnes  and  his  co- 
workers  (see  Maclnnes,  Cowperthwaite  and  Huang  (1927),  use 
devices  by  which  a  boundary  is  formed  with  a  shearing  motion. 

There  is  good  evidence  that  the  potential  at  a  boundary  formed 
by  mixture  may  differ  from  that  at  a  boundary  formed  by 
diffusion.  A  change  in  the  structure  frequently  appears  in  a 
change  of  potential  with  time.  For  instance,  Chanoz  (1906)  con- 
structed the  symmetrical  arrangement : 

Electrode  MR  |  M'R'  |  MR  Electrode, 
A         B 

and  then,  by  maintaining  a  more  or  less  sharp  boundary  at  A  by 
renewal  of  the  contact,  and  allowing  diffusion  to  occur  at  B, 
he  obtained  very  definite  E.M.F.'s  instead  of  the  zero  E.M.F. 
which  the  symmetrical  arrangement  demanded.  This  time  effect 
had  been  noted  by  Weyl  (1905)  and  has  since  been  frequently  re- 
ported, for  instance,  by  Bjerrum  (1911),  Lewis  and  Rupert 
(1911),  Gumming  and  Gilchrist  (1913),  Walpole  (1914)  and 
Fales  and  Vosburgh  (1918). 

Since  the  change  of  potential  has  been  ascribed  to  the  diffusion 
or  mixing  which  alters  the  distribution  of  the  contending,  migrat- 
ing ions,  it  has  seemed  to  many  that  the  effect  could  be  made  more 
uniform  and  conditions  more  reproducible  if  sand  or  other  ma- 
terial were  used  to  delay  mixing  and  diffusion. 


274  THE    DETERMINATION    OF   HYDROGEN   IONS 

Lewis,  Brighton  and  Sebastian  (1917)  using  Bjerrum's  (1911) 
suggestion  of  a  layer  of  sand  in  which  to  establish  the  liquid 
contact  found  that  "at  no  time  were  reproducible  results  obtained 
nor  results  which  remained  constant  to  0.0001  volt  for  more  than 
a  minute  or  two.  The  potential  of  the  liquid  junction  first  es- 
tablished was  surprisingly  high  (0.030  volt)  and  fell  rapidly 
without  reaching  any  definite  limiting  value."  The  liquids 
placed  in  contact  in  this  experiment  were  0.1  M  HC1  and  0.1  M 
KC1.  These  authors  abandoned  the  sand  method. 

On  the  other  hand  Myers  and  Acree  (1913)  report  satisfaction 
with  Bjerrum's  "Sandfiillung." 

Fales  and  Mudge  (1920)  recommend  "small  cones  of  cotton 
wool  fitted  snugly,  but  not  tightly,  into  the  siphon  tubes/' 

According  to  Fricke  (1924)  foreign  porous  material  at  the  junc- 
tion may  be  a  cause  of  error. 

Other  devices  such  as  the  use  of  a  wick  have  been  resorted  to, 
but,  on  the  whole,  direct  liquid  contact  is  considered  the  best. 
There  may,  however,  be  occasion  when  the  employment  of  some 
restraint  is  advantageous  for  rough  comparative  measurements. 

In  the  description  of  the  system  shown  by  figure  47,  page  295, 
it  is  stated  that  liquid  junction  is  formed  by  first  pinching  the 
connecting  rubber  tube  to  displace  KC1  solution,  turning  the  key 
of  the  cock  and  then,  by  slow  release  of  the  pressure  on  the 
rubber  tube,  drawing  the  solution  back  into  a  wide  part  of  the 
tube.  As  judged  by  the  reproducibility  of  cell  potentials  this 
gives  a  satisfactory  way  of  forming  a  liquid  junction. 

In  1920  Lamb  and  Larson  described  the  "flowing  junction" 
which  they  find  to  be  much  more  reproducible  than  the  junctions 
usually  made.  They  conclude  "that  a  'flowing'  junction,  obtained 
simply  by  having  an  upward  current  of  the  heavier  electrolyte 
meet  a  downward  current  of  the  lighter  electrolyte  in  a  vertical 
tube  at  its  point  of  union  with  a  horizontal  outflow  tube,  or  by 
allowing  the  lighter  electrolyte  to  flow  constantly  into  a  large 
volume  of  the  heavier  electrolyte,  even  with  N  solution,  gives 
potentials  constant  and  reproducible  to  0.01  of  a  millivolt." 

Maclnnes  and  Yeh  (1921)  improved  the  system  of  Lamb  and 
Larson  and  confirmed  the  principle  that  reproducible  liquid  junc- 
tion potentials  may  be  thus  obtained,  but  they  find  most  interest- 
ing effects  with  different  rates  of  flow.  Of  particular  importance 


XIII 


FLOWING    JUNCTION 


275 


is  the  observation  that  the  reproducible  potentials  are  not  the 
highest  that  can  be  obtained. 

The  arrangement  used  by  Maclnnes  and  Yeh  is  shown  in 
figure  42.  A  and  B  are  reservoirs  which  supply  the  two  solutions 
to  the  junction  at  J.  The  rate  of  flow  is  adjusted  by  a  screw 
pinchcock  on  a  rubber  tube  attached  at  P.  In  starting  the 
operation  the  rubber  tip  E  of  a  glass  rod  is  pushed  into  its  seat 
and  separates  the  two  parts  of  the  apparatus.  The  pinchcock  at 
P  is  closed.  The  two  halves  are  then  filled  with  their  respective 
solutions  and  adjusted  to  the  same  hydrostatic  pressures.  P 
and  E  are  opened  and  a  flowing  boundary  with  sharp  definition 


FIG.  42.  CELL  WITH  "FLOWING  JUNCTION" 
(After  Maclnnes  and  Yeh) 

forms  at  J  and  proceeds  along  the  waste  to  P.  If  initial  mixing 
is  allowed  to  take  place  no  amount  of  flowing  will  produce  con- 
stant potentials. 

Roberts  and  Fenwick  (1927)  use  an  ingenious  device  for  a 
flowing  junction.  It  is  illustrated  in  figure  43.  "A  hole  about 
1  mm.  in  diameter  is  drilled  in  a  thin  strip  of  mica  (about  1.5 
X  7  cm.)  by  means  of  a  glass-rod  drill,  working  from  both  sides 
of  the  plate  so  that  the  edges  are  as  smooth  as  possible;  it  is 
placed  about  5  mm.  below  the  exit  tubes  of  the  electrodes.  The 
lower  edge  of  the  plate  is  notched  and  the  faces  are  painted  with 
hot  paraffin,  except  for  a  narrow  channel  (indicated  by  dotted 
line)  past  the  hole."  A  channel  leads  to  one  point  of  the  plate 
on  the  one  side  and  to  the  other  point  of  the  plate  on  the  other 
side.  "This  insures  that  the  only  liquid  junction  is  at  the  aperture 
in  the  plate." 


276 


THE    DETERMINATION   OF   HYDROGEN   IONS 


The  flowing  junction  has  been  applied  also  by  Aten  and  van 
Dalfsen  (1926),  S0rensen  and  Linderstr0m-Lang  (1924)  and 
others.  Aten  and  van  Dalfsen  allow  the  intermediate  solution 
to  flow  through  plates  of  porous  alundum. 

As  Scatchard  says,  the  flowing  junction  is  usually  not  practical 
with  the  hydrogen-half  cell  "since  the  change  in  pressure  due  to 
the  changing  level  affects  the  potential  of  the  hydrogen  electrode, 
and  since  the  junction  is  disturbed  by  the  rocking  or  gas  bubbling 
at  the  hydrogen  electrode."  Scatchard  (1925)  says  "The  flow- 
ing junction  presumably  gives  a  'mixture  boundary/ — one  in 
which  the  composition  of  each  infinitesimal  layer  is  the  same  as 
though  it  had  been  prepared  by  stirring  together  the  two  solu- 
tions in  the  proper  proportions,  and  one  which  is  extremely  thin. 


lose*) 


a    b 


r 


I    P    I  P 

FIG.  43.  ROBERTS  AND  FENWICK'S  DEVICE  FOR  A  "FLOWING  JUNCTION" 

When  the  flow  is  stopped  the  junction  changes  to  a  'diffusion 
boundary,' — one  whose  composition  is  determined  by  the  rates 
of  diffusion  of  the  various  ions,  which  gradually  increases  in 
thickness.  Any  change  in  the  total  electromotive  force  of  the 
cell  when  the  flow  is  stopped  must  be  due  to  the  difference  between 
the  potentials  of  these  two  types  of  liquid  junction.  Then  the 
effect  on  the  electromotive  force  of  stopping  the  flow  should  give 
some  insight  into  the  absolute  magnitude  of  the  liquid-junction 
potential."  Scatchard  then  shows  that,  with  the  junction  of  satu- 
rated potassium  chloride  solution  with  hydrochloric  acid  solu- 
tions, stopping  the  flow  resulted  in  a  slow  increase  of  the  cell 
potential,  the  maximum  increase  being  of  the  same  order  of 
magnitude  for  1.0  M,  0.1  M  or  0.01  M  HC1.  "Since  this  differ- 
ence is  almost  independent  of  the  acid  concentration,  it  appears 
that  at  least  the  order  of  magnitude  of  the  potential  must  be  the 
same  in  dilute  as  in  concentrated  solutions."  The  difference 


xiii  BJERRUM'S  EXTRAPOLATION  277 

was  about  0.35  millivolts  between  the  potentials  at  the  "mixture 
boundary"  and  the  "diffusion  boundary."  "Both  cannot  be 
zero,"  says  Scatchard,  "and  it  is  probable  that  neither  is." 

POTASSIUM  CHLORIDE  AS  A  REDUCER  OF  JUNCTION  POTENTIAL 

A  very  excellent  illustration  of  the  proposition  that  "a  problem 
cannot  be  experimentally  solved  until  it  is  logically  defined"  arose 
from  the  theory  of  Nernst  that  the  junction  potential  is  due  to 
the  unequal  tendencies  in  the  migration  of  ions.  The  table  of 
velocities  given  on  page  266  will  show  that  if  KC1  is  concerned, 
no  large  potential  can  arise  from  the  participation  of  its  ions, 
because  they  move  with  approximately  the  same  velocity.  If  such 
a  salt  be  present  in  high  concentration  upon  both  or  even  one 
side  of  the  interface,  its  ions  will  dominate  the  situation,  and, 
migrating  at  nearly  equal  velocities,  will  tend  to  maintain  a  con- 
stant junction-potential  difference  which  undoubtedly  is  not  zero 
but  approaches  it  within  a  few  millivolts. 

Bjerrum  (1911)  studied  the  potential  differences  developed  when 
concentrated  solutions  of  potassium  chloride  were  employed  and 
estimated  the  theoretical  values  with  the  aid  of  Planck's  formula 
and  with  the  aid  of  Henderson's  formula.  He  came  to  the  con- 
clusion that  the  use  of  a  3.5  M  KC1  solution  would  not  com- 
pletely eliminate  the  potential  against  hydrochloric  acid  solu- 
tions; but  he  suggested  a  more  or  less  empirical  extrapolation 
which  would,  he  thought,  give  the  proper  correction.  The  cor- 
rection is  the  difference  in  the  E.M.F.'s  of  a  chain  found  when 
first  3.5  M  KC1  is  used  and  then  when  1.75  M  KC1  is  used  to  con- 
nect two  electrodes. 

An  instance  of  the  application  of  this  extrapolation  is  taken 
from  a  paper  by  S0rensen  and  Linderstr0m-Lang  (1924).  The 
cells  used  were 

I  -  Pt,  H2  (1  atmos.)  |  0.01  N  HC1  +  0.09  N  KC1 1  1.75  N  KC1 1 

0.1  N  KC1,  HgCl  |  Hg+ 

II  -  Pt,  H2  (1  atmos.)  |  0.01  N  HC1  +  0.09  N  KC1 1  3.5  N  KC1 1 

0.1  N  KC1,  HgCl  |  Hg+ 

The  average  potential  of  cell  I  at  18°  was  0.45688  volt 
The  average  potential  of  cell  II  at  18°  was  0.45624  volt 
The  difference  was  0.00064  volt 


278  THE    DETERMINATION    OF   HYDROGEN    IONS 

This  difference  subtracted  from  the  potential  of  cell  II  gives  E  = 
0.4556.     E  is  regarded  as  the  potential  of  the  cell 

-Pt,H2(latmos.)|0.01NHCl+0.09NKCl||0.1NKCl,HgCl|Hg+ 

Fales  and  Vosburgh  (1918)  made  an  extensive  comparison  of 
various  chains,  and  with  the  aid  of  Planck's  formula  to  give  the 
order  of  magnitude  of  various  contact  potentials,  and  the  assump- 
tion of  equal  activities  of  H+  and  Cl~  ions,  they  have  attempted 
to  assign  values  which  will  lead  to  a  general  consistency.  They 
concur  with  others  in  finding  Planck's  formula  invalid  in  the 
assignment  of  accurate  values  to  liquid  junctions,  such  as: 

"xM  KC1|  1.0  M  HC1  and  *M  KCl|  0.1  M  HC1  where  x  ranges 
from  0.1  to  4.1  and  the  temperature  is  25°C." 

They  conclude  that  "there  is  no  contact  potential  difference 
at  25°  between  a  saturated  solution  of  potassium  chloride  (4.1  M) 
and  hydrochloric  acid  solutions  ranging  in  concentrations  from 
0.1  molar  to  1.0  molar/'  agreeing  with  the  suggestion  of  Loomis 
and  Acree  (1911). 

Because  of  the  great  detail  concerned  in  the  reasoning  of  Fales 
and  Vosburgh  it  is  impossible  to  briefly  summarize  their  work, 
but  before  their  conclusion  can  be  considered  valid  it  must  be 
noted  that  they  themselves  point  out  that  "in  an  electromotive 
force  combination  having  a  contact  potential  difference  as  one  of 
its  component  electromotive  forces,  the  diffusion  across  the  liquid 
junction  of  the  one  liquid  into  the  other  brings  about  a  decrease 
in  the  magnitude  of  the  contact  potential  difference,  and  this 
decrease  may  amount  to  as  much  as  one-tenth  of  the  initial 
magnitude  of  the  contact  potential  difference."  This  experi- 
mental uncertainty  undoubtedly  renders  questionable  the  com- 
parability, if  not  the  precision  of  measurements  by  different  ex- 
perimenters. If  so  there  may  lurk  in  the  data  used  by  Fales 
and  Vosburgh,  in  their  argument  of  adjustment  to  consistency, 
an  indefinite  degree  of  incomparability.  The  conclusion  quoted 
above  is  not  accepted  by  all.  Consult  Aten  and  van  Dalfsen. 
Scatchard  (1925),  for  instance,  follows  a  method  of  estimation 
which  leads  to  the  value  0.0047  volt  for  the  potential  at  the 
junction 

HC1  (0.1M)  $  KC1  (sat.) 


XIII  USE   OF  SATURATED    KC1  279 

This  matter  will  be  discussed  at  the  point  where  it  is  shown 
to  affect  the  standardization  of  all  pH  values.  See  Chapter  XXIII. 

It  has  been  stated  by  S0rensen  and  Linderstr0m-Lang  (1924) 
that  in  the  study  of  practically  all  solutions  used  for  biological 
investigations,  with  exception  of  markedly  acid  or  alkaline  solu- 
tions, the  Bjerrum  extrapolation  gives  the  same  results  as  the 
interposition  of  saturated  potassium  chloride  solution.  This  is, 
of  course,  their  direct  conclusion  from  actual  measurements  and 
is  based  on  no  assumptions.  It  does  not  necessarily  follow  that 
the  liquid  junction  potential  has  been  eliminated  but  the  ap- 
proximate identity  in  the  results  of  the  two  methods  suggests  that, 
even  if  elimination  is  not  successful,  a  fairly  constant  value  is 
involved. 

One  very  pertinent  reason  for  believing  that  the  junction  po- 
tential between  a  saturated  potassium  chloride  solution  and  a 
buffer  solution  which  is  neither  very  acid  or  very  alkaline  is  low, 
is  that  the  concentrations  of  the  excessively  mobile  hydrogen 
and  hydroxyl  ions  are  negligible.  Other  things  being  equal,  the 
junction  potential  should  then  be  determined  largely  by  such  in- 
equality as  may  exist  between  the  velocities  of  the  potassium  and 
chloride  ions.  The  tendency  is  then  toward  some  small,  constant, 
liquid-junction  potential  rather  than  toward  the  complete  elimina- 
tion sometimes  assumed. 

In  some  of  the  earlier  investigations  of  liquid  junction  potentials 
studies  were  made  with  ammonium  nitrate.  See  for  instance 
Abegg  and  Cumming  (1907),  Bjerrum  (1911),  Poma  (1914). 
Drucker  (1927)  has  recently  investigated  several  other  salts  in 
bridging  solutions.  The  subject  is  important  to  those  cases  in 
which  a  chloride  is  incompatible  with  a  component  of  the  ad- 
jacent solution.  See  also  Aten  and  Van  Dalfsen  (1926). 

Michaelis  and  Kakinuma  (1923)  and  Michaelis  and  Fujita  (1923) 
prefer  the  employment  of  potassium  chloride  in  the  way  indicated 
below  by  a  type  case. 

N 


Pt,H 


100 


HC1 


100 


HC1  +  KC1  (sat.) 


KC1  (sat.),  HgCl 


Hg 


A  B  C  D 

The  argument  is  that  since  the  activities  of  the  hydrochloric 
acid  on  the  two  sides  of  junction  B  are  nearly  the  same  their 


280         THE  DETERMINATION  OF  HYDROGEN  IONS 

contribution  to  the  junction  potential  will  be  low.  The  junction 
potential  at  B  will  certainly  be  lower  than  at 

KCl  (sat.) 

Likewise  the  high  excess  of  KCl  on  both  sides  of  junction  C  tends 
to  dominate  the  situation  there.  Michaelis  and  Fujita  give 
examples  showing  that  their  method  yields  substantially  the  same 
results  as  the  Bjerrum  extrapolation. 

The  argument  is  not  rigid  enough  for  the  purposes  of  Chapter 
XXIII. 

While  the  Bjerrum  extrapolation  is  still  frequently  used,  its 
theoretical  basis  is  insecure  and  its  results  are  unsatisfactory. 
Therefore,  it  seems  preferable  to  ignore  it.  The  use  of  a  saturated 
solution  of  KCl  is  preferable  since  it  provides  a  reduction  of  contact 
potential  sufficient  for  many  purposes  and  a  simple  and  widely 
used  procedure,  adherence  to  which  makes  possible  the  comparison 
of  "pH  numbers"  as  obtained  by  a  uniform  procedure.  Data 
obtained  with  3.5N  KCl  are  often  not  comparable  with  those 
obtained  with  saturated  KCl  as  bridging  solution. 

As  indicated  by  the  quotation  from  Harned  (see  page  268)  no 
precise  solution  of  the  problem  can  be  obtained  until  some  means 
is  found  for  definitely  determining  the  individual  ion  activities 
and  transport  numbers  without  involvement  of  cells  having  liquid 
junction  potentials.  Until  a  precise  solution  is  found  we  must  be 
sceptical  not  only  of  absolute  values  sometimes  assigned  to  the 
potentials  at  junctions  of  even  simple  solutions  but  guardful  of 
our  acceptance  of  statements  regarding  the  potentials  at  the 
junction  of  complex  solutions  when  the  basis  of  estimation  is  not 
precisely  given. 


CHAPTER  XIV 

HYDROGEN  HALF-CELLS 

We  can  only  explore  the  world  with  apparatus,  which  is  itself  part  of 
the  world. — EDDINGTON. 

THE    BASE    OF   THE    HYDROGEN   ELECTRODE 

Usually  the  base  of  a  hydrogen  electrode  is  simply  a  piece  of 
platinum  foil  or  wire.  If  wire  is  used  an  end  is  fused  into  a  glass 
tube  and  the  latter  is  filled  with  mercury  to  form  a  convenient 
means  of  making  contact  with  the  lead  from  the  potentiometer 
circuit.  The  free  end  of  the  platinum  wire  may  then  be  wound 
upon  a  machine  screw.  On  withdrawing  the  screw  the  wire  is 
left  in  a  neat  coil.  If  foil  is  used  it  may  be  cut  to  a  very  short 
T  and  the  stem  fused  into  the  glass  tube  as  was  the  wire ;  but  this 
is  not  advisable  except  when  very  thin  foil  is  used.  Usually  the 
stem  is  made  by  welding  to  the  foil  a  short  piece  of  platinum 
wire.  The  welding  as  follows.  Over  a  piece  of  polished  steel, 
heat  the  two  pieces  of  platinum  to  a  white  heat  with  a  blast  lamp. 
Suddenly  strike  the  hot  pieces  against  the  steel  with  a  flat  punch. 
Next,  draw  off  a  soft,  lead-free  glass  tube  to  a  thin  and  blunt 
point.  Break  the  capillary  tip  to  permit  the  wire  to  enter.  Slip 
the  wire  in  until  the  foil  touches  the  glass.  Then,  with  foil  upper- 
most, rotate  the  tube  with  the  junction  in  the  tip  of  a  fine,  hot 
flame.  Let  the  glass  fuse  until  a  perfect  seal  is  made  and  a  little 
of  the  glass  fuses  to  the  edge  of  the  foil.  The  steps  are  illustrated 
in  figure  44. 


FIG.  44.  CONSTRUCTION  OF  SIMPLE  ELECTRODE 
281 


282        THE  DETERMINATION  OF  HYDROGEN  IONS 

It  is  important  to  avoid  a  seal  with  too  thin  a  glass  junction, 
for  such  a  seal  may  easily  be  broken.  It  is  likewise  important 
to  avoid  too  heavy  a  seal  for  then  proper  annealing  becomes 
difficult.  A  little  experience  enables  one  to  make  seals  requiring 
no  special  annealing.  If  a  light  but  substantial  junction  with  the 
edge  of  the  foil  is  made  the  electrode  will  be  rugged. 

For  highly  refined  investigations  it  may  be  an  advantage  to 
make  the  seal  with  an  alcohol  flame  and  thus  avoid  the  injurious 
effects  upon  platinum  of  the  sulfur  in  ordinary  gas.  Under  no 
circumstances  should  there  be  used  a  glass  (e.g.,  "Pyrex")  having 
a  coefficient  of  expansion  very  different  from  that  of  platinum, 
for  imperfections  of  the  seal  are  sure  to  develop.  In  this  connec- 
tion it  may  be  said  that  the  most  frequent  mistake  in  making 
electrodes  is  the  use  of  too  large  a  sealing  wire.  Large  wire  is 
resorted  to  in  order  that  the  pendant  foil  may  be  held  in  place. 
The  inevitable  result  of  the  use  of  so  large  a  wire  is  that  the  glass 
seal  becomes  subject  to  imperfections  which,  while  not  detected 
at  first,  may  permit  fatal  creepage  of  mercury  from  the  interior 
junction  to  the  exposed  exterior.  Some  prefer  to  do  away  with 
the  mercury  within  the  glass  tube.  They  solder  a  copper  lead  to 
the  end  of  the  platinum  wire  which  is  destined  to  be  within  the 
glass  tube.  This,  of  course,  is  quite  permissible  and  sometimes 
advisable  if  done  properly  and  with  design,  but  the  good  tech- 
nician will  not  humble  himself  by  doing  it  to  avoid  creepage  of 
mercury  through  cracks.  Fear  of  mercury  creepage  under  the 
very  best  of  conditions,  while  never  disturbing  the  author,  has 
led  some  investigators  to  prefer  the  all-wire  connection. 

By  the  trick  of  catching  the  edge  of  the  foil  with  the  softened 
glass  the  electrode  is  stiffened  and  then  the  wire  leading  through 
the  glass  seal  may  be  made  so  small  that  a  good  seal  is  very  easily 
made.  Foil  0.08  mm.  thick,  1  centimeter  square  welded  to  wire 
0.08  mm.  in  diameter  does  very  well. 

In  place  of  platinum  foil,  gauze  is  sometimes  used.  Thus 
Schmidt  and  Finger  (1908)  refer  to  the  "Cottrell-electrode"  which 
consists  of  two  cylinders  of  platinum  gauze  separated  from  one 
another  by  fusing  their  rims  to  rings  of  glass.  A  platinum  lead 
welded  to  each  cylinder  connects  with  a  separate  mercury  cup. 
There  are  thus  formed  two  electrodes.  The  advantage  of  gauze 
is  a  large  catalytic  surface.  The  disadvantage  is  that  the  diffi- 


XIV  FILM   ELECTKODES  283 

culty  of  cleaning  the  crevices  will  make  a  careful  technician 
nervous. 

It  is  sometimes  assumed  that  complete  equilibrium  can  be 
attained  only  when  the  hydrogen  in  the  interior  of  the  metal 
supporting  the  platinum  black  is  in  equilibrium  with  that  on  the 
surface.  To  reduce  the  time  factor  of  this  soaking-in  process  it 
is  considered  advantageous  to  use  as  the  supporting  metal  a  very 
thin  film  of  platinum  or  iridium  deposited  upon  glass.  Doubtless 
the  finest  of  such  films  could  be  deposited  by  holding  the  glass 
tangent  to  the  Crookes'  dark  space  of  a  vacuum  discharge  and 
spattering  the  metal  on  from  electrodes  under  5000  volts  difference 
of  potential.  The  method  practiced  is  to  burn  the  metal  on  from 
a  volatile  solvent.  The  receipt  given  by  Westhaver  (1905)  is 
as  follows:  0.3  gram  iridium  chloride  moistened  with  concentrated 
HC1  is  dissolved  in  1  cc.  absolute  alcohol  saturated  with  boric 
acid.  To  this  is  added  a  mixture  of  1  cc.  Venetian  turpentine  and 
2  cc.  lavender  oil.  The  glass,  after  being  dipped  in  this  solution, 
is  "whipped"  with  a  stroke  of  the  arm  to  throw  off  excess  liquid 
and  then  rotated  while  drying  above  an  alcohol  flame.  It  is 
then  gradually  lowered  into  the  alcohol  flame  and  there  heated 
until  the  film  is  first  reduced  to  the  mirroring  metal  and  this 
metal  then  adheres  to  the  gently  softened  glass.  The  process 
should  be  repeated  until  a  good  conducting  film  is  obtained. 

Gooch  and  Burdick  (1912)  have  better  success  with  a  viscous 
mixture  of  pure  chloroplatinic  acid  and  glycerine.  This  is  applied 
with  an  asbestos  swab  to  the  glass  which  has  previously  been 
heated  to  a  temperature  which  will  instantly  volatilize  the 
glycerine.  The  resulting  film  is  heated  until  it  adheres  well  to 
the  glass. 

Meillere  (1920)  gives  the  following  recipe.  Five-tenths  gram 
dry  platinum  chloride  is  triturated  with  10  or  15  grams  of  essence 
of  camomile.  The  mixture  is  thinned  with  about  an  equal 
volume  of  methyl  alcohol. 

Rheinberg  (1923)  has  a  patented  process  of  platinizing  glass 
which  is  used  in  producing  mirrors.  (See  Glazebrook,  vol.  40 

Mozolowski  and  Parnas  (1926)  use  gilded  glass  in  their  quin- 
hydrone  electrode  vessel.  They  dissolve  about  0.1  gram  gold 
chloride  in  a  drop  of  absolute  alcohol  and  while  the  solution  is 
cooled  they  add  a  drop  of  lavender  oil.  A  drop  of  the  mixture 


284  THE    DETERMINATION   OF   HYDROGEN   IONS 

is  placed  on  the  glass  and  carefully  heated.  (See  also  Eilert 
(1922).) 

If  after  some  practice  it  is  found  that  even  deposits  can  be 
formed  by  one  or  another  of  the  methods,  the  next  difficulty  met 
is  in  obtaining  good  adherence  of  the  film  to  the  glass.  This  must 
be  done  by  heating  sufficiently  but  at  the  same  time  there  must 
be  avoided  a  fusion  of  such  extent  that  the  continuity  of  the 
metallic  film  will  be  destroyed.  If  the  glass  support  is  made  of 
a  "hard"  glass  such  a  fusion  will  be  more  easily  avoided  and  at 
the  same  time  volatilization  of  impurities  in  the  film  will  be  made 
easier  because  of  the  higher  temperature  permitted.  However, 
in  the  selection  of  such  a  glass  one  with  a  temperature  coefficient 
of  expansion  approximately  equal  to  the  platinum  should  be 
selected, — chiefly  as  a  provision  for  the  next  step  which  will  now 
be  described. 

The  chief  technical  difficulty  in  the  preparation  of  electrodes 
with  the  films  described  is  in  establishing  the  necessary  electrical 
connection.  An  exposed  platinum  wire  contact  destroys  the 
object  in  using  the  film.  Ordinarily  the  electrode  is  made  by  first 
coating  a  bar  of  glass  in  the  end  of  which  there  is  sealed  a  plati- 
num wire  and  then  fusing  this  bar  into  the  end  of  a  glass  tube  so 
that  the  platinum  contact  is  exposed  within  the  tube  where 
mercury  contact  may  be  made.  Connection  with  the  film  is  made 
by  the  film  of  metal  that  runs  through  the  glass  seal.  It  is  less 
clumsy  to  seal  the  wire  into  the  end  of  a  glass  tube,  break  off 
the  wire  flush  with  the  glass,  coat  the  tube  with  the  film  and 
then  cover  the  exposed  wire  with  a  drop  of  molten  glass. 

In  place  of  capping  the  exposed  butt  of  the  wire  with  glass  it 
might  be  well  to  try  some  of  the  newer  synthetic  lacquers. 

There  is  so  little  advantage  in  these  film-electrodes  that  they 
are  seldom  used. 

A  scheme  which  is  said  to  partially  accomplish  the  purpose 
of  a  thin  film  of  supporting  metal  is  to  cover  a  platinum  support 
with  a  gold-plate,  gold  being  relatively  impervious  to  hydrogen. 
It  is  doubtful  whether  this  reason  has  much  practical  weight. 
Hammett  (1922)  thinks  it  has  none.  However  a  gold-plate  is  of 
great  advantage.  It  offers  a  surface  upon  which  deposits  of 
"black"  adhere  well.  It  forms  a  support  easily  dissolved  by 
electrolysis  in  hydrochloric  acid,  thus  providing  an  easy  means  of 


XIV  DEPOSITION   OF   "BLACK"  285 

removing  old  deposits.  And  the  character  of  the  gold  deposit 
gives  an  additional  means  of  testing  the  cleanliness  of  the  elec- 
trode prior  to  blackening. 

For  the  gold  plating  of  electrodes  the  following  recipe  may  be 
used.  Dissolve  0.7  gram  gold  chloride  in  50  cc.  water  and  pre- 
cipitate the  gold  with  ammonia  water,  taking  care  to  avoid  an 
excess.  Filter,  wash  and  dissolve  immediately  in  a  KCN  solution 
consisting  of  1.25  grams  KCN  in  100  cc.  water.  Boil  till  the 
solution  is  free  from  ammonia. 

PREPARATION   FOR   DEPOSITING   BLACK 

One  of  the  essentials  for  making  good  deposits  is  a  very  high 
degree  of  cleanliness  of  the  electrode.  In  addition  to  the  ordinary 
methods  of  cleaning  it  may  be  necessary  to  resort  to  the  use  of 
very  fine  emery  paper  to  remove  those  spots  which  sometimes 
resist  solvents.  Alcoholic  alkali  should  be  used  if  the  fingers  or 
other  source  of  grease  touch  the  foil.  Hammett  (1922)  uses  a 
water  scrubber  for  the  final  cleaning.  A  good  test  of  cleanli- 
ness is  the  evenness  with  which  bubbles  of  hydrogen  escape  from 
the  surface  during  electrolysis  in  dilute  sulfuric  acid. 

A  prerequisite  for  the  good  deposition  of  black  is  adequate 
distribution  of  current.  A  large  electrode  may  require  more  than 
one  electrical  lead. 

In  the  author's  practice  no  electrode  is  ever  subjected  to  the 
blast  lamp  treatment  which  others  recommend.  In  the  first 
place  this  is  done  at  great  risk  to  the  glass  seal  which  may  resist 
for  a  few  times  but  which  may  develop  invisible  cracks.  In  the 
second  place  blast  lamp  treatment  does  not  improve  the  surface 
of  the  platinum  and  may  obviously  injure  it.  If  redeposition  of 
"black"  under  favorable  conditions  fails  to  yield  a  good  elec- 
trode, experience  has  shown  that  it  is  best  to  retire  the  electrode 
from  service  without  hesitation.  It  is  therefore  not  good  prac- 
tice to  so  tie  up  a  particular  electrode  by  sealing  it  into  an  ex- 
pensive ground  glass  stopper  or  into  the  vessel  itself  that  there 
will  be  fatal  hesitation  in  rejecting  it.  On  the  other  hand  when 
such  practice  becomes  advisable  for  certain  research  purposes 
the  seal  should  be  made  in  such  a  way  that  it  may  be  broken  and 
the  electrode  replaced. 


286  THE    DETERMINATION    OF   HYDROGEN   IONS 


According  to  the  work  of  earlier  investigators  and  the  con- 
sensus of  opinion  among  more  recent  investigators  there  seems  to 
be  no  difference  under  equilibrium  conditions  between  coatings  of 
platinum-,  iridium-  or  palladium-black.  Of  the  three,  iridium  is 
recommended  by  Lewis,  Brighton  and  Sebastian  because  of  its 
higher  catalytic  activity,  and  palladium  by  Clark  and  Lubs  (1916) 
for  use  in  the  study  of  physiological  solutions  because  of  the 
relative  ease  with  which  one  deposit  may  be  removed  before  the 
deposition  of  the  next  in  the  frequent  renewals  which  are  often 
necessary.  Palladium  black  is  easily  removed  by  electrolysis  in 
HC1.  Deposits  of  platinum  or  iridium  may  be  removed  by 
electrolysis  in  HC1  solution,  if  they  are  deposited  upon  a  gold 
plate.  They  are  difficult  to  remove  if  deposited  on  platinum. 

Earned  (1926),  who  says  that  a  thin  coating  of  black  is  essen- 
tial, gives  the  following  directions:  "Good  results  were  obtained 
by  electrolyzing  a  solution  of  chloroplatinic  acid  containing  0.5 
gram  of  platinum  in  100  cc.  of  solution  for  one  minute  with  a 
current  density  of  0.3  ampere  per  square  centimeter  of  cathode 
surface." 

The  author  has  used  deposits  of  platinum,  iridium  and  pal- 
ladium upon  platinum,  upon  gold-plated  platinum  'and  upon 
"rhotanium"  alloy.  Acidified  (HC1)  3  per  cent  solutions  of  the 
chlorides  of  each  metal  are  used  without  much  attention  to  the 
exact  strength.  The  current  from  a  four- volt  storage  battery  is 
allowed  to  produce  a  vigorous  evolution  of  gas.  The  electrode, 
after  the  deposition,  is  connected  to  the  negative  pole  of  the  bat- 
tery, placed  in  a  dilute  sulfuric  acid  solution  and  charged  with 
hydrogen.  It  is  required  that  the  bubbles  of  hydrogen  then 
escaping  come  off  evenly,  that  the  electrode  shall  have  been 
evenly  covered  with  the  deposit  in  thickness  sufficient  to  cover 
the  glint  of  polished  metal,  and  that  the  deposit  shall  adhere 
under  a  vigorous  stream  of  water. 

The  system  used  by  the  author  for  deposition  of  "black"  is 
as  follows.  A  row  of  small  vessels,  such  as  weighing  bottles 
about  2  cm.  diameter  and  5  cm.  deep  are  fitted  with  electrodes. 
These  electrodes  are  all  attached  through  binding  posts  mounted 
on  a  wooden  rail.  These  in  turn  are  connected  to  one  pole  of 
a  double-pole,  double-throw  switch.  The  opposite  pole  is  con- 


XIV  DEPOSITION   OF    "BLACK"  287 

nected  with  a  flexible  lead  tipped  with  platinum.  This  lead  is 
used  to  connect  with  the  electrodes  to  be  treated.  The  middle 
connections  of  the  double-throw  switch  are  connected  with  a  4- volt 
storage  battery.  The  other  connections  are  cross-wired.  One  of 
the  vessels  is  filled  with  hydrochloric  acid  made  by  a  one-to-one 
dilution  of  ordinary  37  per  cent  acid.  This  is  used  to  dissolve 
previous  deposits  with  the  aid  of  electrolysis  (switch  reversed, 
treated  electrode  +).  Another  vessel  is  filled  with  10  per  cent 
sulfuric  acid  for  preliminary  direct  and  counter-electrolysis  to 
test  the  cleanliness  of  the  electrode.  Another  vessel  is  filled  with 
the  platinum,  palladium  or  iridium  chloride  solution.  When  using 
palladium  so-called  reagent  palladium  is  used  as  +  electrode 
and  this  is  removed  from  the  solution  when  not  in  use.  After 
deposition  of  the  black  the  electrode  under  treatment  is  quickly 
placed  under  a  vigorous  stream  of  water  and  then  electrolyzed 
in  a  another  vessel  of  freshly  prepared  ten  per  cent  sulfuric  acid 
until  thoroughly  charged  with  hydrogen. 

When  used  with  inorganic  solutions  which  undergo  no  decom- 
position electrodes  may  often  be  used  repeatedly,  provided  they 
are  kept  clean  and  not  allowed  to  dry.  When  there  is  any  sign 
or  suspicion  of  an  electrode  becoming  clogged,  poisoned,  worn, 
dry  or  in  any  way  injured,  there  should  be  not  the  slightest  hesi- 
tation in  reblackening  or  even  rejecting  it. 

For  the  deposition  of  platinum  black  Ellis  (1916)  uses  a  solu- 
tion of  pure  chloroplatinic  acid  containing  1  per  cent  Pt.  He 
cautions  against  the  use  of  the  lead  acetate  which  has  come  down 
to  us  in  recipes  for  the  deposition  of  platinum  black  upon  elec- 
trodes for  conductivity  measurements.  For  the  deposition  Ellis 
uses  a  small  auxiliary  electrode  and  a  current  large  enough  to 
liberate  gas  freely  at  both  electrodes.  He  continues  the  deposi- 
tion with  five-minute  reversals  of  current  for  two  hours  and  ob- 
tains a  very  thick  coating. 

Beans  and  Hammett  (1925),  compare  Hammett  (1922),  see  no 
reason  for  the  objection  to  traces  of  lead  which  Ellis  emphasizes. 
Britton  (1925)  believes  lead  increases  the  efficiency.  The  author 
sees  no  occasion  for  its  introduction.  Hammett  (1922)  finds  that 
pure  chloroplatinic  acid  prepared  by  the  method  of  Wichers 
(1921)  tends  to  yield  bright  deposits  in  place  of  the  usual  black. 
The  inference  is  that  the  usual  black  owes  its  nature  to  the 


288  THE    DETERMINATION    OF    HYDROGEN    IONS 

presence   of  impurities  in   commercial   preparations  of   chloro- 
platinic  acid. 
Hammett  (1922)  says: 

"For  the  deposition  of  platinum  black  from  a  solution  of  chlorplatinic 
acid  containing  a  trace  of  lead  ion,  current  density  and  concentration  of 
chlorplatinic  acid  are  of  minor  importance,  except  that  with  very  dilute 
solutions  stirring  becomes  necessary.  Reversing  the  direction  of  the  cur- 
rent at  intervals  seems  to  have  little  effect,  but  the  current  should  always 
pass  in  the  direction  of  cathodic  polarization  for  some  time  at  the  end  of  the 
process  if  commutation  is  used.  If  the  final  treatment  is  anodic  the  reduc- 
tion of  the  oxidation  products  formed  requires  so  much  time  that  the  elec- 
trode is  slow  in  coming  to  equilibrium." 

The  above  statement  reflects  the  usual  opinion  that  current 
density  is  of  minor  importance. 

For  the  deposition  of  iridium  Lewis,  Brighton  and  Sebastian 
(1917)  make  the  gold  or  gold-plated  electrode  the  cathode  in  a 
5  per  cent  solution  of  iridium  chloride.  "The  best  results  were 
obtained  with  a  very  small  current  running  for  from  twelve  to 
twenty-four  hours.  Too  large  a  current  gives  a  deposit  which 
appears  more  like  platinum  black  and  which  is  easily  rubbed  off." 

Preferences  in  regard  to  the  thickness  of  the  "black"  deposit 
vary  widely.  For  instance  Earned  (1926),  Prideaux  (1924)  and 
the  writer  (see  earlier  editions)  concur  in  preferring  compara- 
tively light  coats;  while  Ellis  (1916)  Blackadder  (1925)  and 
others  either  state  specifically  that  they  prefer  heavy  coats  or 
describe  an  electrolysis  of  such  duration  and  current  density  that 
very  heavy  deposits  are  sure  to  occur.  In  the  writer's  opinion 
it  is  only  the  nature  of  the  directly  exposed  surface  that  counts 
in  the  ideal  electrode  and  very  heavy  deposits  are  potentially 
dangerous  on  account  of  occlusions,  if  for  no  other  reason.  Of 
course  there  must  be  some  "body"  in  reserve  for  as  Beans  and 
Hammett  (1925)  have  shown  the  catalytically  active  smooth 
deposits  which  they  have  been  able  to  prepare  may  soon  lose 
activity.  These  same  investigators  point  out  that  occlusions  of 
acid  from  the  electrolytic  bath  may  seriously  affect  the  apparent 
pH  value  of  very  poorly  buffered  solutions  when  heavily  coated 
electrodes  are  used.  For  such  solutions  they  recommend  a  plating 
of  gold  covered  by  the  active  deposit  of  smooth  platinum  which 
they  obtain  by  using  very  pure  chloro  platinic  acid.  For  the 
preparation  of  pure  Pt,  see  Wichers  (1921). 


xiv  PT  AND  PD  " BLACK"  289 

I  use  deposits  barely  sufficient  in  thickness  to  obscure  the  glint 
of  polished  metal  beneath.  Compared  with  one  another  in  the 
same  solution  they  will  agree  within  0.02  millivolt.  Andrews 
reports  "sluggish"  electrodes  or  even  "the  complete  failure  of 
electrodes  due  to  too  heavy  deposits"  (of  Pd). 

According  to  Hofmann  (1922)  prolonged  charging  with  hydro- 
gen will  lower  the  ability  of  an  electrode  to  catalyze  the  reduction 
of  oxygen.  This  catalysis  proceeds  better  in  acid  solution  than 
in  alkaline  solution  and  it  is  enhanced  by  pretreatment  of  the 
electrode  with  alternate  cathode  and  anode  polarization.  It  is 
difficult  to  discuss  this  proposition  adequately  for  there  is  a  very 
extensive  and  highly  puzzling  literature  on  the  effect  of  oxygen 
upon  platinum  catalysts. 

Hammett  (1922)  says: 

"In  general  the  time  required  for  attainment  of  equilibrium  depends 
upon  the  efficiency  of  removal  of  oxygen;  and  is  more  a  function  of  the  de- 
sign of  the  cell  and  the  rate  of  hydrogen  flow  than  of  the  properties  of  the 
electrode.  Electrodes  deteriorate  under  the  influence  of  hydrogen,  becom- 
ing much  more  sensitive  to  traces  of  oxygen  and  finally  unusable;  but  the 
process  is  partially  reversed  by  exposure  to  oxygen.  Lack  of  attention  to 
the  complete  exclusion  of  oxygen  and  the  use  of  aged  electrodes  may  pro- 
duce no  ill  results  on  measurements  in  acid  or  neutral  range,  but  every  care 
must  be  taken  when  the  solution  is  strongly  alkaline." 

Andrews  (1924)  reports  a  detailed  study  of  electrodes  coated 
with  palladium  black,  noting  in  particular  some  of  the  factors 
which  lead  to  poor  deposits  such  as  solutions  too  concentrated  or 
too  dilute.  Andrews'  general  conclusion  was  that  palladium 
electrodes  are  less  reliable  than  platinum  and  his  difficulties  are 
certainly  worthy  of  being  regarded  as  a  reason  for  advocating 
platinum  black  in  place  of  palladium  black.  However,  it  is  im- 
portant to  note  that  Andrews  did  not  use  a  cell  well  suited  to  the 
demonstration  of  single-potential  stabilities,  and  it  is  also  in- 
teresting to  note  the  following.  Dr.  Barnett  Cohen  has  made 
most  of  the  innumerable  hydrogen  electrode  measurements  for 
the  Hygienic  Laboratory  during  the  last  six  years  and  usually 
with  palladium  black  electrodes.  In  running  through  his  records 
I  find  among  quadruplicate  measurements  with  four  vessels  run 
in  parallel  that  there  are  occasional  discrepancies  which  are  crossed 
out  and  made  the  occasion  for  repetitions  of  measurements. 


290  THE    DETERMINATION    OF   HYDROGEN   IONS 

His  tendency  in  routine  measurements  is  to  accept  only  measure- 
ments agreeing  within  0.2  millivolt.  He  evidently  considers  as 
satisfactory  quadruplicates  those  which  agree  within  0.1  milli- 
volt. Very  many  of  his  results  are  such.  And  this  with  pal- 
ladium electrodes  used  as  Andrews  uses  them — apparently. 

Palladium  black  is  said  to  be  attacked  by  hydrochloric  acid 
and  is  not  recommended  for  the  study  of  such  solutions. 

HYDROGEN   ELECTRODE   VESSELS 

So  many  types  of  vessel  have  been  published  that  it  is  diffi- 
cult to  do  justice  to  the  advantages  of  each.  The  selection  must 
depend  in,  some  instances  upon  the  material  to  be  handled,  but 
in  any  case  there  are  a  few  principles  which  it  is  hoped  will  be 
made  clear  by  a  discussion  of  a  few  of  the  more  widely  used 
vessels. 

The  usual  method  of  operation  is  to  partially  or  wholly  im- 
merse the  electrode  in  the  solution  to  be  measured  and  then  to 
bubble  hydrogen  through  the  vessel  till  constant  potential  is 
attained.  The  vessel  described  by  Lewis,  Brighton  and  Sebastian 
(1917)  and  illustrated  in  figure  45  is  representative  of  the  general 
type  of  vessel  used  for  what  may  be  called  the  classic  mode  of 
operation.  The  following  is  the  quoted  description  of  this  vessel: 

Hydrogen  from  the  generator  enters  at  A,  and  is  washed  in  the  bubbler 
B  with  the  same  solution  that  is  contained  in  the  electrode  vessel.  This 
efficient  bubbling  apparatus  saturates  the  gas  with  water  vapor,  so  that 
the  current  of  hydrogen  may  run  for  a  long  period  of  time  without  changing 
the  composition  of  the  solution  in  the  main  vessel.  The  gas  rises  from  the 
tip  C,  saturating  and  stirring  the  whole  liquid  from  G  to  F,  and  leaves  the 
apparatus  through  the  small  trap  E,  which  also  contains  a  small  amount 
of  the  same  solution.  The  platinum  wire  attached  to  the  electrode  D  is 
sealed  by  lead  glass  into  the  ground  glass  stopper  M.  L  is  a  joint  made  by 
fusing  together  the  end  of  the  platinum  wire  and  the  connecting  wire  of 
copper.  The  surface  of  the  solution  stands  at  the  height  F  so  that  the 
iridium  electrode  is  about  one-half  immersed.  The  apparatus  from  F 
through  G,  H,  I  to  J  is  filled  with  the  solution.  With  the  form  of  construc- 
tion shown  it  is  an  easy  matter  to  fill  the  tube  without  leaving  any  bubbles 
of  air.  The  reservoir  K  filled  with  the  same  solution  serves  to  rinse  out 
the  tube  I,  J  from  time  to  time.  The  whole  apparatus  may  be  mounted 
upon  a  transite  board,  or  for  the  sake  of  greater  mobility,  may  be  held  in  a 
clamp,  the  several  parts  being  rigidly  attached  to  one  another  to  avoid 


XIV 


VESSELS 


291 


accidental  breakage.    The  whole  is  immersed  in  the  thermostat  about  to 
the  point  L. 

The  tube  J  dips  into  an  open  tube  through  which  communication  is  made 
to  other  electrode  vessels.  This  connecting  tube  may  be  filled  with  the 
same  solution  as  is  contained  in  the  hydrogen  electrode  vessel  or  with  any 
other  solution  whic^  is  desired.  All  measurements  with  acids  are  made 
with  one  of  the  stopcocks  H,  I,  closed.  These  stopcocks  are  not  greased 
and  there  is  a  film  of  acid  in  the  closed  stopcock  which  suffices  to  carry  the 
current  during  measurement.  In  order  to  make  sure  that  no  liquid  poten- 
tial is  accidentally  established,  the  second  stopcock  may  be  closed  up  and 


FIG.  45.  HYDROGEN  ELECTRODE  VESSEL  OF  LEWIS,   BRIGHTON  AND 

SEBASTIAN 


the  first  opened.  No  difference  of  potential  in  acid  solution  has  ever  been 
observed  during  this  procedure  (but  this  is  not  true  for  solutions  of  salt 
and  alkalies).  If  it  is  desired  that  both  stopcocks  be  open,  the  same  liquid 
that  is  in  the  electrode  vessel  is  placed  in  the  connecting  tube  at  J  and 
the  stopcocks  H  and  I  are  opened  after  the  current  of  hydrogen  has  been 
cut  off  by  the  stopcock  A,  and  the  opening  of  the  trap  E  has  been  closed. 

If  hydrogen  enters  the  cell  at  the  rate  of  one  or  two  bubbles  per  minute 
several  hours  are  required  for  the  saturation  of  the  solution  and  for  the 
removal  of  air.  After  this  time  the  potential  is  absolutely  independent  of 
the  rate  of  flow  of  hydrogen  and  the  generator  may  be  entirely  cut  off  for 
many  hours  without  any  change. 


292  THE    DETERMINATION    OF   HYDROGEN   IONS 

Gerke  and  Geddes  (1927)  describe  a  vessel  especially  designed 
for  the  study  of  cells  such  as  Pt,  H2  |  HC1,  HgCl  |  Hg  when  the 
electrolyte  is  very  dilute.  There  are  numerous  other  designs 
for  the  special  purposes  of  investigations  on  the  electrochemistry 
of  special  cells. 

For  some  biochemical  studies  such  vessels  are  unsuitable.  It 
is  sometimes  absolutely  essential  that  equilibrium  potentials  be 
established  rapidly.  The  necessity  is  perfectly  apparent  when  one 
is  dealing  with  an  actively  fermenting  culture.  It  is  not  always 
so  apparent  when  dealing  with  other  solutions,  but  it  is  suspected 
that  absolutely  complete  equilibrium  is  never  attained  in  some 
complex  biochemical  solutions  and  that  we  have  to  depend  upon 
speeding  the  approach  to  equilibrium  between  hydrogen  and 
hydrogen  ions  till  a  virtual  equilibrium  point  is  attained  (see 
Chapter  XVIII). 

It  was  shown  by  Michaelis  and  B,onaf  ( 1909)  that  a  fairly  con- 
stant E.  M.  F.  is  quickly  attained,  even  in  blood,  if  the  platinized 
electrode,  previously  saturated  with  hydrogen,  is  allowed  to 
merely  touch  the  surface  of  the  solution.  This  is  probably  due, 
as  suggested  by  Hasselbalch  (1913)  and  again  by  Konikoff  (1913), 
to  a  rather  sharply  localized  equilibrium  at  the  point  of  contact. 
Reductions  and  gas  interchanges  having  taken  place  within  the 
small  volume  at  the  point  of  contact,  diffusion  from  the  remain- 
ing body  of  the  solution  is  hindered  by  the  density  of  the  surface 
layer  with  which  alone  the  electrode  comes  in  contact. 

In  exploring  new  fluids  it  appeared  hazardous  to  the  writer  to 
rely  upon  such  a  device,  which  appears  to  take  advantage  of 
only  a  localized  and  hence  a  pseudo-equilibrium,  and  which  makes 
no  allowance  for  a  possible  difference  between  the  solution  and 
surface  film  in  the  activity  of  the  hydrogen  ions.  Hasselbalch 's 
(1911)  principle  seemed  therefore  to  be  more  suitable. 

Hasselbalch  found  that  a  very  rapid  attainment  of  a  constant 
potential  can  be  obtained  by  shaking  the  electrode  vessel.  Under 
these  conditions  there  should  be  not  only  a  more  rapid  inter- 
change of  gas  between  the  solution,  the  gaseous  hydrogen,  and 
the  electrode,  an  interchange  whose  rapidity  Dolezalek  (1899) 
and  Bose  (1900)  consider  necessary,  but  the  combined  or  molec- 
ular oxygen,  or  its  equivalent,  in  the  whole  solution  should  be 
more  rapidly  brought  into  contact  with  the  electrode  and  there 


xrv 


VESSELS 


293 


reduced.  Furthermore,  by  periodically  exposing  the  electrode  the 
hydrogen  is  required  to  penetrate  only  a  thin  film  of  liquid  before 
it  is  absorbed  by  the  platinum  black.  The  electrode  should 
therefore  act  more  rapidly  as  a  hydrogen  carrier.  For  these 
reasons  a  true  equilibrium  embracing  the  whole  solution  should 


12  MM 
FOR  NS  0  STOPPER 


BORE  2  MM. 
WALLS    2  MM 


•WALLS  I  MM 
-OUTSIDE    DIAM.  9  MM. 


75  HI 


FIG.  46.  A  HYDROGEN  ELECTRODE  VESSEL 
(Clark  (1915).     Drawing  by  courtesy  A.  H.  Thomas  Company) 

Notes.  In  submitting  this  working  drawing  to  a  glass  blower  it  shall  be 
specified  that:  (1)  Cocks  shall  be  joined  to  chamber  with  a  neat  and  wide 
flare  that  shall  not  trap  liquid.  (2)  Cocks  shall  be  ground  to  hold  high 
vacuum.  (3)  Bores  of  cock  keys  shall  meet  outlets  with  precision.  (4) 
The  handles  of  keys  shall  be  marked  with  colored  glass  to  show  positions  of 
bores.  (5)  The  handles  of  both  keys  shall  be  on  the  same  side  (front  of 
drawing).  (6)  Vessel  shall  be  carefully  annealed.  (7)  Opening  for  no.  0 
rubber  stopper  shall  be  smooth  and  shall  have  standard  taper  of  the  stand- 
ard no.  0  stopper.  (8)  Dimensions  as  given  shall  be  followed  as  closely  as 
possible.  (9)  No  chipped  keys  or  violation  of  the  above  specifications 
shall  be  accepted. 

be  rapidly  obtained  with  the  shaking  electrode;  and  indeed  a 
constant  potential  is  soon  reached. 

Eggert  (1914-1915)  in  Nernst's  laboratory  made  a  study  of  the 
rapidity  of  reduction  by  hydrogen  electrodes  in  which  he  com- 
pared the  effect  of  alternate  immersion  and  exposure  to  the  hydro- 
gen atmosphere  with  the  effect  of  continued  immersion.  In  the 


294  THE    DETERMINATION   OF   HYDROGEN   IONS 

reduction  of  metal  salt  solutions  such  as  ferric  salts  he  obtained 
a  much  greater  velocity  of  reduction  when  the  electrode  was 
periodically  removed  from  the  liquid  carrying  a  thin  film  of 
solution  to  be  exposed  to  the  hydrogen.  The  maximum  velocity 
was  proportional  to  the  platinum  surface  and  the  time  of  contact 
with  the  gas.  It  was  independent  of  the  number  of  times  per 
minute  the  electrode  was  raised  and  lowered.  As  the  reaction 
neared  completion  the  decrease  in  velocity  of  reaction  became 
exponential. 

Making  use  of  the  principles  brought  out  in  the  preceding  dis- 
cussion and  also  certain  suggestions  noted  in  the  chapter  on  liquid 
junction  potentials  Clark  (1915)  designed  a  vessel  which  appears 
to  have  found  favor  for  general  use.  A  working  drawing  of  this 
vessel  is  shown  in  figure  46.  This  drawing  shows  the  type  of 
three-way  cock  employed  by  Cullen.  Cullen  (1922)  also  has 
added  a  small  thermometer  for  use  when  the  vessel  is  operated 
without  thermostat  control.  If  solutions  more  viscous  than 
fresh  milk  are  to  be  used,  the  bores  of  the  inlet  and  outlet  tubes 
should  be  made  larger.  If  only  very  small  quantities  of  the 
solution  to  be  tested  are  available,  the  dimensions  of  the  vessel 
may  be  reduced.  In  figure  47  is  a  diagrammatic  sketch  of  the 
complete  system  now  in  use  by  the  author  for  ordinary  work. 

The  electrode  vessel  is  mounted  in  a  clamp  pivoted  behind  the 
rubber  connection  between  J  and  H.  This  clamp  runs  in  a 
groove  of  the  eccentric  I,  the  rotation  of  which  rocks  the  vessel.1 
In  the  manipulation  of  the  vessel,  the  purpose  is,  first,  to  bring 
every  portion  of  the  solution  into  intimate  contact  with  the 
electrode  F  and  the  hydrogen  atmosphere,  to  make  use  of  the 
principle  of  alternate  exposure  and  immersion  of  electrode  and 
then,  when  equilibrium  is  attained,  to  draw  the  solution  into 
contact  with  concentrated  KC1  solution  and  form  a  wide  contact 
at  H  in  a  reproducible  manner.  The  E.M.F.  is  measured  directly 
after  the  formation  of  this  liquid  junction. 

The  vessel  is  first  flooded  with  an  abundance  of  hydrogen  by 
filling  the  vessel  as  full  as  possible  with  water,  displacing  this 
with  the  hydrogen,  and  then  flushing  with  successive  charges  of 
hydrogen  from  the  backed-up  generator.  Water  or  solution  is 

1  Dr.  A.  B.  Hastings  rocks  the  vessel  with  the  aid  of  an  automobile  wind 
shield  wiper  operating  with  compressed  air. 


XIV 


VESSELS 


295 


296  THE    DETERMINATION    OF   HYDROGEN   IONS 

run  into  the  vessel  from  the  reservoir  D  which  can  be  emptied 
through  the  drain  B  by  the  proper  turning  of  the  cock  C.  Solu- 
tion or  hydrogen  displaced  from  the  vessel  is  drained  off  at  B'. 
These  drains  when  they  emerge  from  the  electrical  shielding  (see 
p.  357)  should  hang  free  of  any  laboratory  drain. 

With  the  vessel  rocked  back  to  its  lowest  position  the  solution 
to  be  tested  is  run  in  from  D  (after  a  preliminary  and  thorough 
rinsing  of  the  vessel  with  the  solution)  until  the  chamber  E  is 
about  half  full.  Cock  G  is  closed  and  cock  C  is  turned  so  as  to 
permit  a  constant  pressure  of  hydrogen  from  A  to  bear  upon  the 
solution.  For  very  careful  work  it  is  well  to  displace  dissolved 
oxygen  by  first  bubbling  hydrogen  through  the  solution,  provided 
carbonate  solutions  are  not  concerned.  The  rocking  is  then  com- 
menced and  is  continued  until  experience  shows  that  equilibrium 
is  attained  with  the  solution  of  the  type  under  examination.  The 
eccentric  I  should  give  the  vessel  an  excursion  which  will  alter- 
nately completely  immerse  the  electrode  F  and  expose  it  all  to  the 
hydrogen  atmosphere.  The  rate  of  rocking  may  be  adjusted  to 
obtain  the  maximum  mixing  effect  without  churning. 

To  establish  the  liquid  junction  the  rubber  tube  between  J  and 
H  is  pinched  while  G  is  turned  to  allow  KC1  solution  to  escape  at 
B'.  Then  a  turn  of  G  and  the  release  of  the  pinch  draws  the 
solution  down  through  the  cock  to  form  a  broad  mixed  junction 
at  H.  For  a  new  junction  the  old  is  flushed  away  with  fresh 
KC1  from  the  reservoir  N  by  properly  setting  cock  L. 

With  the  closed  form  of  calomel  electrode,  M,  shown  in  the 
figure,  no  closed  stopcocks  need  be  interposed  between  the  terminals 
of  the  cell.  With  the  customary  calomel  electrode  vessel  it  is 
necessary  to  use  a  closed  cock  somewhere  and  since  this  must  be 
left  ungreased  it  is  well  to  have  it  a  special  cock2  at  J. 

If  a  tube  be  led  out  from  J  and  branched,  several  hydrogen 
electrode  vessels  may  be  joined  into  the  system.  In  any  event 
it  is  well  to  work  with  two  vessels  in  parallel  so  that  one  may  be 
flushing  with  hydrogen  while  the  other  is  shaking. 

2  To  make  an  easily  turning  cock  out  of  which  KC1  will  not  creep,  grease 
the  narrow  part  of  the  socket  and  the  wide  part  of  the  key.  When  the  key 
is  replaced  there  will  be  two  bands  of  lubricant  on  which  the  key  will  ride 
with  an  uncontaminated  zone  between  for  the  film  of  KC1  solution. 

See  Shepherd  and  Ledig  (1927)  on  the  preparation  of  stopcock  lu- 
bricant. 


XIV  VESSELS  297 

The  electrode  F  is  supported  in  a  sulfur-free  rubber  stopper. 
A  glass  stopper  may  be  ground  into  place  but  is  seldom  of  any 
advantage  and  may  prove  to  be  a  mistake.  In  the  first  place  it 
is  advisable  to  be  free  with  electrodes  and  to  instantly  reject  any 
which  fail  to  receive  a  proper  coating  of  metal.  The  inclination  to 
do  this  is  less  if  it  entails  the  rejection  of  a  carefully  ground  stop- 
per. Unless  the  stopper  is  accurately  ground  into  place  it  is 
worthless.  Furthermore  it  is  very  difficult  to  so  grind  a  glass 
stopper  that  there  will  be  left  no  capillary  space  to  trap  liquid. 
A  rubber  stopper  can  be  forced  into  place  without  leaving  such  a 
space.  The  rapidity  with  which  measurements  are  usually  taken 
makes  it  improbable  that  a  rubber  stopper,  if  made  sulfur  free, 
can  have  any  appreciable  effect.  If  the  rubber  must  be  pro- 
tected a  coating  of  paraffin  will  do. 

The  calomel  electrode  M  is  of  the  saturated  type  so  that  no 
particular  care  need  be  taken  to  protect  it  from  the  saturated 
KC1  used  in  making  junctions.  This  is  the  working  standard 
for  the  accurate  standardization  of  which  there  is  held  in  reserve 
the  battery  of  accurately  made,  tenth-normal,  calomel  electrodes 
P.  This  battery  may  be  connected  with  the  system  at  any  time 
by  making  liquid  connection  at  O  and  opening  K. 

After  a  measurement  the  liquid  junction  is  eliminated,  the  space 
rinsed  with  the  tenth  normal  KC1,  and  liquid  .contact  left  broken. 

The  design  of  this  system  is  obviously  for  an  air  bath.  The 
necessity  of  raising  cocks  out  of  an  oil  bath  would  not  permit 
such  direct  connections  as  are  here  shown. 

In  figure  48  are  shown  several  other  designs  of  electrode  ves- 
sels. A  is  one  of  the  original  Hasselbalch  vessels  which  has  since 
been  modified  for  the  use  of  replaceable  electrodes.  B  (S0rensen), 
(Ellis)  and  C  (Walpole),  are  operated  in  a  manner  similar  to  the 
vessel  shown  in  figure  45.  Walpole  7s  vessel  was  made  of  silica 
and  the  electrode  was  of  platinum  film  as  described  on  page  283. 
D  (McClendon  and  Magoon)  was  designed  for  determinations 
with  small  quantities  of  blood.  E  (Michaelis),  employs  a  sta- 
tionary hydrogen  atmosphere  and  a  wick  connection  for  the 
liquid  junction.  See  also  Farkas  (1903)  for  use  of  the  stationary 
hydrogen  atmosphere.  G  (Long)  is  a  simple  device  which  the 
designer  thought  applied  the  essential  principles  of  Clark's 
vessel.  Barendrecht's  vessel,  H,  is  designed  for  immersion  in  an 


298  THE    DETERMINATION    OF   HYDROGEN   IONS 


FIG.  48.  TYPES  OF  HYDROGEN  ELECTRODE  VESSELS 


XIV  VESSELS  299 

open  beaker  for  estimations  during  titrations.  It  is  similar  to  a 
design  of  Walpole's  (1914),  but  is  provided  with  a  plunger  the 
working  of  which  permits  the  rinsing  of  the  bulb  and  the  precise 
adjustment  of  the  level  of  the  liquid.  Another  immersion  elec- 
trode is  Hildebrand's,  F,  the  successful  operation  of  which  de- 
pends upon  a  vigorous  stream  of  hydrogen,  which,  on  escaping 
from  the  bell  surges  the  solution  about  the  electrode.  It  is 
similar  to  several  simple  designs  used  for  a  long  time  in  electro- 
metric  titrations.  A  modification  which  provides  better  protec- 
tion of  the  electrode  from  oxygen  is  Bunker's  design,  I. 

Monier-Williams  (1924)  describes  a  vessel  which  is  useful  for 
the  study  of  pastes.  A  straight  tube  is  provided  with  side  tubes 
for  the  hydrogen  inlet  and  outlet.  The  tube  is  packed  with  the 
paste  up  to  the  side  tubes.  At  this  surface  of  the  paste  a  wire 
electrode  touches.  The  other  surface  of  the  paste  is  thrust  into 
a  KC1  solution. 

Vies  and  Vellinger  (1925)  mention  the  development  of  the 
vessel  of  Vies,  Reiss  and  Vellinger  (1924)  for  use  with  plastic 
materials. 

Simms  (1923)  describes  a  water- jacketed  electrode  vessel  the 
water  jacket  being  a  local  thermostat.  See  also  Rawlings  (1926). 

In  some  cases  a  preliminary  reduction  of  a  solution  may  be 
accomplished  by  making  the  solution,  in  the  presence  of  hydrogen, 
travel  down  a  long  spiral  of  platinized  wire.  The  spiral  is  made 
by  winding  no.  24  copper  wire  closely  upon  a  rod.  It  is  mounted 
with  a  spread  of  the  turns  just  sufficient  to  hold  together  descend- 
ing drops.  It  is  plated  with  gold  and  then  platinized.  Liquid  de- 
livered slowly  at  the  top  of  the  spiral  will  be  broken  into  drops 
which  in  the  descent  of  the  spiral  are  thoroughly  stirred.  The 
reduced  solution  is  brought  into  contact  with  an  electrode  in  a 
constricted  part  of  the  enclosing  tube  and  is  then  delivered  to  a 
continuous-flow  liquid  junction  such  as  that  described  by  Lamb 
and  Larson  or  Maclnnes  (see  page  274).  The  hydrogen  by  suit- 
able devices  may  be  given  the  carbon-dioxid  partial  pressure  of 
the  tested  solution.  Such  a  scheme  is  useful  only  in  dealing  with 
continuous  treatment  processes  where  abundance  of  material  is 
available. 

Aten  and  Van  Ginneken  (1925)  in  their  study  of  sugar  saps  of 
varying  pH  value  used  flowing  solutions  presaturated  with  hydro- 


300  THE   DETERMINATION    OF   HYDROGEN   IONS 

gen  before  arrival  at  the  electrode.  Their  apparatus  is  described 
as  useful  for  continuous  measurements  of  flowing  solutions. 

Keller  (1922)  has  described  a  hydrogen  electrode  with  a  re- 
placeable disk  of  platinum  gauze.  This  is  held  by  a  cap  to  a  hard 
rubber  support  which  contains  a  portable  calomel  electrode.  The 
system  is  rugged  and  may  be  used  as  an  immersion  cell  for 
determining  the  pH  values  of  liquids  in  commercial  processes. 

At  this  point  it  may  be  of  interest  to  note  that  Wilke  (1913) 
attempted  to  make  a  hydrogen  electrode  by  using  a  thin  tube  of 
palladium  on  the  interior  of  which  hydrogen  was  maintained 
under  pressure.  One  of  the  difficulties  with  such  an  electrode  is 
the  estimation  of  the  hydrogen  pressure  at  the  solution-electrode 
interface.  Wilke's  idea  has  never  been  developed  to  a  practical 
point  so  far  as  I  know,  but  it  is  worthy  of  study  as  an  im- 
mersion electrode  for  industrial  use.  See  citation  to  Drucker. 

Knobel  (1923)  describes  an  electrode  which  is  superficially  like 
Wilke's  in  that  the  hydrogen  passes  from  a  central  core  outward 
to  the  solution.  However  Knobel  uses  a  graphite  cylinder  and 
it  is  through  the  pores  of  this  that  the  hydrogen  makes  its  way. 
The  outer  particles  of  the  graphite  are  platinized  and  as  the 
hydrogen  passes  these  it  is  as  if  the  graphite  cylinder  were  a  dis- 
tributor for  the  hydrogen  which  escapes  at  normal  pressure. 
Schrnid  (1924)  has  described  some  interesting  experiments  with 
a  similar  electrode.  Some  of  Schmid's  publications  are  difficult 
to  obtain  but  his  studies  should  be  watched.  They  are  of  con- 
siderable interest.  For  other  electrodes  see  Sannie  (1924), 
Swyngedauw  (1927)  and  particularly  the  "Birnenelektrode"  of 
Michaelis. 

For  purposes  of  titration  many  of  the  vessels  described  for 
exact  measurements,  or  for  special  purposes  are  inconvenient. 
Therefore  there  are  to  be  found  a  number  of  vessels  especially 
designed  for  titrations.  Hastings'  (1921)  is  one  of  these.  Bovie's 
(1922)  is  another. 

For  titrations  and  for  general  utility  as  well  as  for  potentio- 
metric  studies  of  oxidation-reduction  equilibria  the  vessel  with 
attached  calomel  half-cell  shown  in  figure  49  has  proved  useful 
(See  Clark  and  Cohen,  1923;  Studies  on  oxidation-reduction,  III.) 
The  mechanical  stirrer  shown  in  their  figure  is  usually  not  neces- 
sary. The  holder  has  been  simplified  in  the  design  shown  by 


XIV 


TITRATION   VESSELS 


301 


figure  50.  A  is  a  standard  "1J  inch  pipe  lock-nut"  the  interior 
threads  of  which  hold  a  No.  10  rubber  stopper.  The  interior 
diameter  of  this  lock-nut  is  approximately  4.6  cm.  while  the 
greatest  diameter  of  a  No.  10  rubber  stopper  is  about  5  cm. 
Therefore  the  stopper  may  be  ground  down  at  its  widest  part  to 
a  cylindrical  shape  of  about  4.7  cm.  diameter.  It  is  squeezed 
into  place  with  the  smaller,  tapered  end  projecting  and  ready  to 
receive  the  mouth  of  a  glass  cylinder.  B  is  a  bar  [for  support. 
It  is  tightly  screwed  into  place.  A  smaller  bar,  D,  carries  the 
movable  platform  E  which,  when  turned  into  place,  supports  the 
glass  cylinder.  The  calomel  half-cell  vessel  is  attached  to  the 


4 


FIG.  49 


Spring 


FIG.  50 


FIG.  49.  ELECTRODE  VESSEL  WITH  ATTACHED  CALOMEL  HALF-CELL 
FIG.  50.  HOLDER  FOR  TITRATION  VESSEL  AND  CALOMEL  HALF-CELL 

brass  plate  C  by  a  lead  cleat  with  the  bolts^shown  and  a  soft  copper 
wire  running  through  the  holes. 

The  calomel  half-cell  vessel  is  shown  in  figure  49.    Cf.  page  305. 

There  have  recently  been  several  designs  of  electrode  vessel 
adapted  to  operating  with  very  small  quantities  of  fluid.  Bodine 
and  Fink  (1925)  for  instance  have  cut  down  dimensions  till  they 
operate  with  0.015  to  0.020  cc.  of  fluid;  Bodine  (1927)  uses  0.01 
cc.  Their  vessel  has  been  employed  in  studying  the  blood  of  . 
insects  and  the  interior  of  Fundulus  egg  cells.  Winterstein 
(1927),  also  describes  a  micro  vessel. 

Lehmann  (1923)  raises  a  drop  of  liquid  on  a  little  table  in  a 


302  THE    DETERMINATION    OF   HYDROGEN   IONS 

tube  filled  with  hydrogen  till  it  makes  contact  with  a  platinum 
point  and  a  capillary  liquid  junction.  The  general  design  has 
been  modified  in  a  number  of  instances.  Solowiew  (1926)  adapts 
it  to  multiple  measurements  and  Radsimowska  (1924)  to  measure- 
ments with  gels.  Wladimiroff  and  Galwialo  (1925)  describe  diffi- 
culties in  using  the  principle  with  liquids  containing  C02. 

Taylor  (1925)  mentions  fine-drawn  electrode  points  designed 
for  micro-injection  work.  Compare  Gelfan  (1926). 

McClendon  (1915)  describes  a  hydrogen-calomel  cell  of  such 
dimensions  that  it  may  be  swallowed  for  measurements  of  pH  in 
the  stomach. 

Schaede,  Neukirch  and  Halpert  (1921)  have  an  electrode  vessel 
for  subcutaneous  injection. 

In  conclusion  it  may  be  said  that  with  ordinary  care  almost  any 
simple  combination  of  electrode  and  electrode  vessel  will  give 
fairly  good  results.  On  the  other  hand  it  is  often  necessary  not 
only  to  provide  against  continuous  loss  of  C02  from  biological 
solutions  but  also  to  arrange  for  rapid  attainment  of  equilibrium. 
Since  electrode  measurements  are  often  the  last  resort,  since  one 
can  easily  be  misled  by  pseudo-equilibria  and  since  attention  to  a 
few  simple  details  of  construction  and  operation  frequently  in- 
creases very  greatly  the  speed  of  experimentation,  the  "simplicity" 
of  certain  designs  is  sometimes  more  apparent  than  real. 

One  of  the  most  astonishing  aspects  of  many  of  the  various 
designs  is  the  frequency  with  which  there  appears  no  care  for  the 
elimination  of  "dead  spaces."  There  is  also  an  apparent  lack  of 
interest  in  the  fact  that  an  equilibrium  involving  three  phases 
has  to  be  established.  As  Beans  and  Hammett  (1925)  have  well 
said  the  design  of  a  vessel  is  as  important  as  the  nature  of  the 
electrode  itself  in  attaining  rapidity  of  measurement.  Thus  Rice 
and  Rider  (1923)  describe  cases  in  which  as  much  as  30  minutes 
were  required  for  the  attainment  of  equilibrium  with  an  ordinary 
immersion  type  electrode.  This  time  was  very  considerably 
decreased  by  alternately  raising  and  lowering  the  electrode,  an 
operation  provided  for  in  the  use  of  Clark's  vessel. 

However  it  would  be  invidious  to  select  any  particular  design 
for  criticism,  the  more  so  because  none  yet  published  is  perfectly 
adapted  to  all  purposes.  Those  described  are  therefore  to  be 
considered  as  illustrations  from  which  the  reader  may  select 
items  or  suggestions  to  incorporate  in  his  own  design. 


CHAPTER  XV 

"CALOMEL"  AND  OTHER  STANDARD  J[ALF-CELLS 


Unless  otherwise  specified  the  calomel  half-cell  is  one  in  which 
mercury  and  calomel  are  overlaid  with  a  definite  concentration  of 
potassium  chloride.  It  is  commonly  called  a  calomel  electrode. 
For  particular  purposes  some  other  chloride  or  hydrochloric  acid 
is  used. 

The  general  type  of  construction  is  shown  by  A,  figure  51.  A 
layer  of  very  pure  mercury  is  covered  with  a  layer  of  very  pure 
calomel  and  over  all  is  a  solution  having  a  definite  concentration 
of  KC1  and  saturated  with  calomel.  Calomel,  mercurous  chloride, 
is  Hg2Cl2.  For  convenience  its  formula  will  be  written  HgCl.1 

The  difference  of  potential  attributed  to  the  interface  between 
mercury  and  solution  is  determined  primarily  by  the  concentra- 
tion of  the  mercurous  ions  supplied  from  the  calomel.  But, 
since  there  is  equilibrium  between  the  calomel,  the  mercurous  ions 
and  the  chloride  ions,  the  concentration  of  the  mercurous  ions  is 
determined  by  the  chloride  ion  activity.  This  is  determined 
chiefly  by  the  concentration  of  the  KC1.  One  of  three  concentra- 
tions of  KC1  is  usually  employed — either  0.1  molecular,  1.0  molec- 
ular or  saturated  KC1.  Half-cells  with  these  concentrations  of 
KC1  are  ordinarily  referred  to  as  the  "tenth  normal-,"  "normal-" 
or  "saturated  calomel  electrodes."  These  should  be  distinguished 
from  cells  in  which  the  potassium  chloride  solution  is  made  on  the 
molality  basis — number  of  moles  of  potassium  chloride  per  1000 
grams  of  water.  0.1  N  KC1  is  0.1006  molal  and  the  mercury  of  the 
0.1  N  half-cell  is  0.00015  volt  negative  to  that  of  the  0.1  M  half- 
cell. 

In  figure  51  are  shown  several  calomel  electrode  vessels  each 

1  Although  Ogg  (Z.  physik.  Chem.,  1898,  27,  285)  showed  that  the  mer- 
curous ion  is  Hg2++  and  accordingly  mercurous  cjiloride  is  often  written 
Hg2Cl2,  practice  has  tended  to  the  use  of  HgCl  in  describing  the  calomel 
half-cell  since  for  usual  purposes  we  are  not  concerned  with  this  detail. 

303 


304  THE    DETERMINATION    OF   HYDROGEN   IONS 


V 


FIG.  51.  TYPES  OF  CALOMEL  ELECTRODE  VESSELS 


XV  CALOMEL   VESSELS  305 

with  a  feature  that  may  be  adapted  to  a  particular  requirement. 
Walpole's  (1914)  vessel,  A,  is  provided  with  a  contact  that  leads 
out  of  the  thermostat  liquid  and  with  a  three-way  cock  for  flushing 
away  contaminated  KC1.  A  more  elaborate  provision  for  the 
protection  of  the  KC1  of  the  electrode  is  shown  in  the  vessel  of 
Lewis,  Brighton  and  Sebastian  (1917),  B.  A  form  useful  as  a 
saturated  calomel  electrode  in  titrations  is  shown  at  C.  Fresh 
KC1  passes  through  the  U-tube  to  take  the  temperature  of  the 
bath  and  to  become  saturated  with  calomel  shown  at  the  bottom 
of  this  U-tube.  D  is  Ellis'  (1916)  vessel,  which  in  the  particular 
form  shown  was  designed  to  be  seated  directly  to  the  remainder  of 
the  apparatus  used.  A  valuable  feature  is  the  manner  of  making 
electrical  contact.  Instead  of  the  customary  sealed-in  platinum 
wire  Ellis  uses  a  mercury  column.  On  closing  the  cocks  the  ves- 
sel may  be  shaken  thoroughly  to  establish  equilibrium.  This 
feature  has  not  been  generally  practiced.  Vessel  E  is  a  simple 
form  useful  for  the  occasional  comparison  electrode.  It  may  be 
made  by  sealing  the  cock  of  an  ordinary  absorption  tube  to  a 
test  tube  and  adding  the  side  arm.  F  is  the  vessel  of  Fales  and 
Vosburgh  (1918)  with  electric  contact  made  as  in  the  familiar 
Ostwald  vessel  (G). 

In  adding  new  KC1  solution  to  a  vessel  it  must  be  borne  in  mind 
that  the  solution  should  be  saturated  with  calomel  before  equilib- 
rium can  be  expected.  It  is  well  therefore  to  have  in  reserve  a 
quantity  of  carefully  prepared  solution  saturated  with  calomel. 

In  figure  49  is  shown  a  serviceable  calomel  half-cell  which  has 
been  used  with  the  attached  titration- vessel  described  on  page  301. 
It  is  made  of  Pyrex  and  therefore  the  parts  are  easily  joined.  The 
three-way  cock  B  and  the  two-way  cock  A  are  placed  as  shown  for 
avoidance  of  breakage.  Since  the  platinum  contact  is  made 
through  Pyrex  glass  the  wire  should  be  very  fine  and  the  surround- 
ing glass  thick.  Wire  about  0.06  mm.  diameter  is  used.  The 
inevitable  slight  defect  of  a  platinum-Pyrex  glass  seal  is  of  no  con- 
sequence in  this  instance  since  pure  mercury  is  placed  on  both 
sides.  The  vessel  is  filled  with  cock  A  open.  Thereafter  this 
cock  is  kept  closed.  Indeed  it  is  feasible  to  do  away  with  this 
cock  and  to  draw  the  tube  off  to  a  capillary  which  is  sealed  after 
the  filling.  When  measurements  are  being  made  cock  B  is  turned 
as  shown  in  the  figure.  When  not  in  use  the  cell  is  opened  to  the 


306  THE   DETEEMINATION   OF   HYDROGEN   IONS 

reservoir  R  to  accommodate  temperature  changes.  When  the 
liquid  junction  at  G  is  to  be  renewed  G  is  flushed  from  reservoir  R. 
Liquid  junction  is  made  at  G  as  follows.  The  old  junction  is 
flushed  away  by  KC1  solution  from  R.  Cock  B  is  closed.  G  is 
lowered  into  a  portion  of  the  solution  to  be  examined.  Through 
a  rubber  tube  attached  to  R  gentle  suction  is  applied  while  cock  B 
is  cautiously  opened.  The  solution  flows  gently  into  G  making  a 
sharp  junction  with  the  heavy  KC1  solution.  When  the  junction 
is  at  the  widest  part  of  G  the  cock  is  turned  as  shown  in  the  figure. 
It  is  then  assumed  that  there  will  be  inappreciable  diffusion  from 
G  through  the  capillary  into  the  solution  to  be  tested. 

This  calomel  half-cell  vessel  is  attached  to  the  holder  of  figure  50 
by  a  lead  cleat  placed  at  D  of  figure  49. 

In  assembling  this  vessel  according  to  the  plan  of  figure  49  the 
tube  leading  from  G  is  broken,  run  through  the  rubber  stopper 
and  resealed  in  place. 

Usually  a  calomel  half-cell  is  attached  to  a  reserve  of  KC1  which 
is  not  to  pass  through  the  half-cell  proper  but  is  used  to  flush  liquid 
junctions. 

Some  years  ago  there  were  demonstrated  in  exhibits  outfits  in 
which  this  KC1  solution  for  flushing  was  colored  for  the  con- 
venience of  observing  liquid  junctions.  The  coloring  matter  was 
not  revealed.  Simms  (1923)  uses  azurine  G  for  this  purpose. 

PREPARATION   OF  MATERIALS  FOR   CALOMEL  HALF-CELLS 

Mercury 

The  mercury  used  in  the  preparation  of  these  "electrodes"  or 
half-cells  should  be  the  purest  obtainable.  In  Chapter  XVII 
methods  of  purification  are  described.  Sufficient  mercury  should 
be  used  to  cover  the  platinum  contact  deeply  enough  to  prevent 
solution  reaching  this  contact  on  accidental  shaking. 

More  portable  half-cells  are  made  by  amalgamating  a  plati- 
num wire  or  foil.  This  is  done  by  electrolyzing  a  solution  of 
mercurous  nitrate,  the  wire  being  the  negative  pole.  Provision 
is  then  made  for  keeping  a  paste  of  calomel  about  this  wire. 

Sometimes  the  platinum  wire  is  amalgamated  even  when  massive 
mercury  is  used  about  it. 


XV  PREPARATION  OF  CALOMEL  307 

Calomel 

Some  success  has  been  attained  with  the  use  of  the  better 
grades  of  calomel  supplied  on  the  market  but  the  risk  is  so  great 
that  it  is  best  to  prepare  this  material  in  the  laboratory.  A 
chemical  and  an  electrolytic  method  will  be  described. 

The  chemical  preparation  of  calomel.  Carefully  redistill  the  best 
obtainable  grade  of  nitric  acid.  Dilute  this  slightly  and  with  it 
dissolve  some  of  the  mercury  prepared  as  described  in  Chapter 
XVII,  always  maintaining  a  large  excess  of  mercury.  Pour  the 
solution  into  a  large  amount  of  distilled  water  making  sure  that 
the  resulting  solution  is  distinctly  acid.  Now,  having  distilled 
pure  hydrochloric  acid  from  a  20  per  cent  solution  and  taken  the 
middle  portion  of  the  distillate,  dilute  and  add  it  slowly  to  the 
mercurous  nitrate  solution  with  constant  stirring.  When  the  pre- 
cipitate has  collected,  decant  and  treat  with  repeated  quantities 
of  pure  distilled  water  (preferably  conductivity  water).  The 
calomel  is  sometimes  washed  with  suction  upon  a  Buchner  funnel, 
but,  if  due  regard  be  taken  for  the  inefficiency  of  washing  by  de- 
cantation,  it  is  preferable  to  wash  repeatedly  by  decantation.  There 
is  thereby  obtained  a  more  even-grained  calomel.  Throughout 
the  process  there  should  be  present  some  free  mercury. 

Electrolytic  preparation  of  calomel.  Doubtless  the  better  prepa- 
ration of  calomel  is  formed  by  electrolysis  according  to  the  method 
of  Lipscomb  and  Hulett  (1916).  This  is  carried  out  in  the  same 
way  that  the  mercurous  sulfate  for  Weston  cells  is  formed.  For 
the  preparation  of  mercurous  sulfate  Wolff  and  Waters  (1907) 
employ  the  apparatus  shown  in  figure  52.  An  improvised  appa- 
ratus may  be  made  of  a  glass  tube  with  paddles,  platinum  wire 
electrode  and  mercury  contact  and  with  two  spools  for  bearing 
and  pulley.  In  place  of  the  sulfuric  acid  there  is  used  normal 
hydrochloric  acid.  Ewing  (1925)  uses  KC1.  A  direct  current 
(from  a  four-volt  storage  battery)  must  be  used.  The  alternating 
current  sometimes  used  in  the  preparation  of  mercurous  sulfate 
does  not  seem  to  work  in  the  preparation  of  calomel  according  to 
some  preliminary  experiments  which  Mr.  McKelvy  and  Mr. 
Shoemaker  of  the  Bureau  of  Standards  kindly  made  for  the  writer. 
During  the  electrolysis  the  calomel  formed  at  the  mercury  surface 
should  be  scraped  off  by  the  paddles  c  and  c  (fig.  52).  The  calomel 
formed  by  this  process  is  heavily  laden  with  finely  divided  mer- 


308 


THE  DETERMINATION  OF  HYDROGEN  IONS 


cury.  Indeed  it  is  possible  to  obtain  a  finely  divided  material 
which  consists  so  largely  of  mercury  itself  that,  when  used  in 
cells  subjected  to  repeated  flushing  with  new  potassium  chloride 
solution,  the  calomel  finally  becomes  washed  out.  Very  good  cells 
are  made  by  combining  calomel  made  by  the  chemical^  process 


FIG.  52.  WOLFF  AND  WATERS'  APPARATUS  FOR  THE  ELECTROLYTIC 

PREPARATION  OF  MERCUROUS  SULFATE  AS  USED  FOR  THE 

PREPARATION  OF  CALOMEL 

and  that  made  by  the  electrolytic  process.  The  first  provides  the 
abundance  of  calomel;  the  second  the  intimate  contact  with 
mercury. 

Calomel  formed  by  either  the  chemical  or  the  electrolytic  proc- 
ess should  be  shaken  with  repeated  changes  of  the  KC1  solution 
to  be  used  in  the  half-cell  before  the  calomel  is  placed  in  such  a  cell. 


XV  VARIATION    OF    POTENTIAL  309 

Potassium  chloride 

Lewis,  Brighton  and  Sebastian  (1917)  state  that  certain  grades 
of  commercial  KC1  are  pure  enough  to  be  used  in  the  preparation 
of  KC1  solutions  for  the  calomel  electrode  while  other  samples 
"contain  an  unknown  impurity  which  has  a  surprisingly  large 
effect  upon  the  E.M.F.  and  which  can  only  be  eliminated  by 
several  recrystallizations."  Gjaldbaek  (1924)  tells  of  various 
so-called. "high-grade"  commercial  preparations  which  contained 
various  impurities  such  as  ferric  salts,  ultramarine,  etc.,  evidently 
from  unclean  containers.  The  author  has  had  similar  experiences. 
On  one  occasion  a  selenium  compound  was  found!  It  is  there- 
fore obvious  that  the  only  safe  procedure,  in  lieu  of  careful  testing 
by  the  actual  construction  of  electrodes  from  different  material, 
is  to  put  the  best  available  KC1  through  several  recrystallizations. 

VARIATIONS    OF   POTENTIAL 

The  variations  in  the  potentials  of  calomel  electrodes  have  been 
the  subject  of  numerous  investigations.  Richards  (1897)  ascribed 
it  partly  to  the  formation  of  mercuric  chloride.  Compare  Rich- 
ards and  Archibald  (1902).  Sauer  (1904)  on  the  other  hand  con- 
cluded that  this  had  little  to  do  with  the  inconstancy.  Arguing 
upon  the  well  known  fact  that  the  solubility  of  slightly  soluble 
material  is  influenced  by  the  size  of  the  grains  in  the  solid  phase, 
Sauer  thought  to  try  the  effect  of  varying  the  grain  size  of  the 
calomel  as  well  as  the  effect  of  the  presence  of  finely  divided 
mercury.  With  cells  made  up  with  various  combinations  he 
found  the  following  comparisons : 

—  Hg    calomel    against  calomel         Hg+      =  0.00287  volt 
(fine)      (coarse)  (fine)       (coarse) 

-Hg    calomel   against  calomel  Hg+      =  0.00037  volt 

(fine)      (coarse)  (coarse)  (coarse) 

—  Hg    calomel   against  calomel  Hg+      =  0.0025  volt 
(coarse)  (coarse)                  (fine)  (coarse) 

Lewis  and  Sargent  (1909)  state  that  they  do  not  confirm  Sauer 
in  regard  to  the  effect  of  the  finely  divided  mercury  but  that  they 
do  confirm  him  in  regard  to  the  state  of  the  calomel.  These 
authors  and  others  recommend  that  grinding  the  calomel  with 
mercury  to  form  a  paste  be  avoided  as  this  tends  to  make  an  un- 


310         THE  DETERMINATION  OF  HYDROGEN  IONS 

even  grain.  It  is  better  to  shake  the  mercury  and  the  calomel 
together  but  this  is  unnecessary  if  electrolytic  calomel  is  used. 

In  some  of  the  older  papers  it  was  suggested  that  oxygen  should 
be  eliminated  from  the  cell.  This  has  been  more  or  less  neglected 
but  recent,  highly  refined  investigations2  are  conducted  with  the 
cells  deaerated  by  a  stream  of  pure  nitrogen. 

By  the  use  of  carefully  prepared  materials  and  the  selection  of 
the  better  agreeing  members  of  a  series,  calomel  electrodes  may  be 
reproduced  to  agree  within  0.1  millivolt  or  better;  but  it  has  not 
yet  been  established  whether  or  not  this  represents  the  order  of 
agreement  among  electrodes  made  in  different  laboratories. 
Furthermore  there  still  remains  the  question  of  the  effect  of  minor 
disturbances.  There  is  no  question  that  "true"  values  are  not  to 
be  expected  until  all  parts  of  the  system  are  in  equilibrium  and 
that  a  preliminary  shaking  such  as  Ellis  uses  will  hasten  the 
attainment  of  equilibrium.  On  the  other  hand  a  disturbance  which 
will  alter  the  surface  structure  of  the  mercury  exposed  may  pro- 
duce a  slight  temporary  shift  in  the  potential-difference.  The 
subject  remains  for  systematic  investigation. 

An  extensive  investigation  of  unsaturated  calomel  electrodes 
was  made  by  Acree  and  his  students  (Myers  and  Acree,  Loomis 
and  Acree),  but  how  far  the  reproducibility,  which  they  attained 
by  short  circuiting  the  differences  of  potential,  is  representative  of 
the  general  reproducibility  of  such  electrodes  is  not  yet  established. 

Acree  has  called  attention  to  the  possible  concentration  of  the 
KC1  solution  by  the  evaporation  of  water  and  its  condensation  on 
the  walls  of  vessels  unequally  heated  in  thermostats. 

THE  "SATURATED"  CALOMEL  HALF-CELL 

This  differs  in  no  way  from  other  calomel  half-cells  except  that 
the  solution  is  saturated  with  KC1  in  the  presence  of  solid  KC1  at 
all  temperatures  used. 

As  a  working  standard  the  saturated  calomel  half-cell  is  un- 
doubtedly the  best  as  pointed  out  by  Michaelis  and  Davidoff 
(1912).  It  does  not  require  careful  protection  from  the  saturated 
KC1  solution  usually  employedjis'a  liquid  junction  and  it  has  a 

2  See  Guntelberg  (1926)  and  Randall  and  Young  (1928)  on  the  action  of 
oxygen  on  calomel  and  similar  electrodes. 


XV 


CALOMEL   ELECTRODE   POTENTIALS 


311 


high  conductivity  permitting  full  use  of  the  sensitivity  of  a  low- 
resistance  galvanometer. 

There  is  not  very  good  agreement  between  the  values  assigned 
to  the  saturated3  calomel  half-cell  by  different  laboratories  and  it 
had  therefore  best  be  regarded  for  the  time  being  as  a  good  work- 
ing-standard to  be  checked  from  time  to  time  against  carefully 
made  normal  or  tenth  normal  calomel  electrodes  or  against  a 
hydrogen  electrode  in  a  standard  solution.  For  ordinary  meas- 
urements however  the  values  given  in  table  A  of  the  Appendix 
are  adequate. 

VALUES   ASSIGNED   TO   CALOMEL   HALF-CELLS 

An  adequate  discussion  of  the  values  assigned  to  calomel  half -cells  must 
await  the  consideration  of  several  matters  to  be  taken  up  in  Chapter  XXIII. 
To  clear  the  way  for  the  difficult  presentation  of  standardization,  which  is 
the  subject  of  Chapter  XXIII,  and  to  provide  a  brief  review,' which  may  be 
useful  in  itself,  we  may  recount  here  some  of  the  more  frequently  used 
values.  These  values  are  presented  without  critical  comment.  However, 
the  reader  should  be  warned  that,  quite  aside  from  differences  in  the  ulti- 
mate bases  of  standardization,  there  is  frequently  lacking  clear  definition 
of  what  a  stated  potential  refers  to.  For  instance  consider  the  half -cell 

Hg  |  HgCl,  KC1  (0.1M)  |  KC1  (sat.)  || 
A  B  C 

A  difference  of  potential  can  be  allocated  to  each  of  the  interfaces  A  and 
B.  At  C  there  is  a  liquid-junction  potential  when  this  half-cell  is  put  in 
liquid-junction  with  another  half-cell.  By  means  of  the  symbol  ||  it  is  in- 

3  Solubility  of  KC1  in  water  (The  Chemist's  Year  Book  Interpolation  of 
Berkeley's  data): 


TEMPERATURE 

GRAMS  KC1 
PER  100  GRAMS 
WATER 

MOLALITY 

TEMPERATURE 

GRAMS  KC1 
PER  100 
GRAMS  WATER 

MOLALITY 

0 

28.13 

3.77 

40 

40.32 

5.41    - 

15 

32.90 

4.41 

60 

45.88 

6.15 

20 

34.51 

4.63 

80 

50.95 

6.83 

25 

36.00 

4.83 

100 

56.08 

7.52 

30 

37.49 

5.03 

Specific  gravity  of  solution  saturated  at  0°  =  1.15  (Seidell's  Solubility 
Tables).  Hence  solution  is  about  3.39  N. 

Specific  gravity  of  solution  saturated  at  15°  =  1.172.  Hence  solution 
is  about  3.89  N. 

Specific  gravity  of  solution  saturated  at  25°  =  1.1785.  Hence  solution 
is  about  4.18  N. 


312         THE  DETERMINATION  OF  HYDROGEN  IONS 

dicated  that  this  junction-potential  is  to  be  treated  separately  and  that  con- 
sideration of  it  is  to  be  neglected  in  evaluating  the  potential  of  the  half-cell. 
Then  there  remains  the  potential  differences  at  A  and  C.  When  a  value  for 
the  calomel  cell  is  stated  it  sometimes  means  definitely  the  potential  at  A,  it 
sometimes  means  definitely  the  algebraic  sum  of  the  potentials  at  A  and  B. 
Frequently  the  distinction  is  not  preserved.  Put  more  frequently  the 
potential  at  C,  stated  to  have  been  taken  care  of  separately,  enters  the 
final  evaluation  of  what  is  really  the  sum  of  the  potentials  at  A  and  B 
although  stated  to  be  the  value  at  A.  We  shall  not  attempt  to  preserve  the 
important  distinction  until  the  matter  is  again  discussed  in  Chapter  XXIII. 
Largely  upon  the  basis  of  Palmaer's  (1907)  work  the  value  0.560  volt  has 
been  used  as  the  "absolute"  difference  of  potential  between  mercury  and 
N/l  KC1  saturated  with  calomel  in  the  presence  of  solid  calomel  at  18°C. 
(The  mercury  being  positive  to  the  solution.)  There  is  some  skepticism4 
regarding  the  reliability  of  this  value,  but  for  the  particular  purpose  with 
which  we  are  now  concerned  it  makes  little  difference  what  the  value  is  if 
proper  relative  relations  are  maintained. 

Because  of  this  it  has  been  agreed  that  some  one  half -cell  shall  be  made 
the  standard  of  reference.  The  hypothetical  normal  hydrogen  electrode 
has  been  agreed  upon  as  a  standard  of  reference  and  potentials  of  calomel 
half-cells  are  usually  referred  to  that  standard  as  having  zero  potential 
difference. 

In  the  report  of  the  "Potential  Commission"  of  the  Bunsen-Gesellschaft 
(Abegg,  Auerbach  and  Luther,  1911)  the  normal  hydrogen  electrode  stand- 
ard of  difference  of  potential  was  adopted.  The  differences  of  potential 
between  the  normal  hydrogen  electrode  and  the  tenth-normal  and  normal 
KC1  calomel  electrodes  were  given  as  0.337  and  0.284-0.283  respectively. 
Auerbach  (1912)  in  a  review  of  this  report  called  attention  to  the  smaller 
temperature  coefficient  of  the  potential  difference  at  the  tenth-normal 
calomel  electrode  when  referred  to  the  normal  hydrogen  electrode  (as  hav- 
ing zero  potential  difference  at  all  temperatures)  and  suggested  that  the 
tenth-normal  electrode  be  taken  as  the  working  standard  with  the  value 
0.3370  between  20 °C.  and  30 °C. 

Loomis  and  Acree  (1911)  present  a  choice  of  values  for  the  tenth-normal 
calomel  electrode  at  25°C.  referred  to  the  normal  hydrogen  electrode. 
The  choice  depends  upon  the  ionization  ascribed  to  the  hydrochloric  acid 
solutions  used  in  their  hydrogen  electrodes  and  upon  the  values  of  the  con- 
tact differences  of  potential  which  were  involved.  Loomis  (1915)  is  in- 
clined to  accept  the  value  0.3360. 

Clark  and  Lubs  (1916)  give  a  compilation  of  Bjerrum's  values  and 
those  of  S0rensen  and  Koefoed  published  by  Sprensen  (1912).  See  table  52. 

In  1914  Lewis  and  Randall  applied  "corrected  degrees  of  dissociation" 
to  the  hydrochloric  acid  solutions  used  in  arriving  at  the  difference  of 

4  Whether  this  is  just  or  unjust  is  a  question  concerning  which  we  are  in 
doubt.  No  critical  review  in  the  light  of  modern  researches  is  known  to  the 
author. 


XV 


CALOMEL    ELECTRODE    POTENTIALS 


313 


potential  at  25°  between  calomel  electrodes  and  the  theoretical  normal 
hydrogen  electrode.  Denning  the  normal  calomel  electrode  as  the  com- 
bination Hg,  Hg2Cl2,  KC1  (1M),  KC1  (0.1M)  they  reach  the  value  0.2776. 
The  difference  of  potential  between  this  electrode  and  the  tenth  normal 
they  give  as  0.0530.  Whence  the  value  for  the  tenth  normal  electrode  is 
0.3306.  These  values  were  revised  by  Lewis,  Brighton  and  Sebastian  (1917) 
to  0.2828  for  the  difference  of  potential  between  the  normal  calomel  and  the 
normal  hydro  gen  electrodes,  and  0.0529  for  the  difference  between  the  normal 
and  the  tenth  normal.  They  were  revised  again  by  Lewis  and  Randall 
(1923)  to  0.2822  for  the  normal  cell. 

Eeattie   (1920)  calculated  for  the  potential    difference  at  the  normal 
calomel  electrode  0.2826  and  compares  this  value  with  0.2824  which  is  Lewis, 

TABLE  52 

Potentials  of  "0.1  N  calomel  half -cell" 


POTENTIAL  DIFFERENCE  BE- 

TWEEN   NORMAL  HYDROGEN 

ELECTRODE    AND  N/10  CALOM  Et 

ELECTRODE  WHEN  HYDROGEN' 

AUTHOR 

TEMPERATURE 

PRESSURE  IS 

Oneatmosphere 

One 

less  vapor 
pressure 

atmosphere 

°C. 

volts 

volts 

Bjerrum  

o 

0.3366 

0.3367 

S0rensen  and  Koefoed  \ 

18 

20 

0.3377 
0.3375 

0.3380 
0.3378 

B  j  errum  

25 

0.3367 

0.3371 

30 

0.3364 

0.3370 

40 

0.3349 

0.3359 

S0rensen  and  Koefoed  • 

50 

0.3326 

0.3344 

60 

0.3290 

0.3321 

75 

0.3243 

0.3315 

Brighton  and  Sebastian's  result  (see  above)  when  corrected  by  Beattie  for 
the  liquid  junction  potential  difference  between  0.1  N  and  1  N  KC1.  For 
later  values  see  Chapter  XXIII  and  appendix  table  A. 

Michaelis  (1914)  gives  in  table  53  several  values  for  the  potential  dif- 
ferences referred  to  the  normal  hydrogen  electrode  for  the  tenth  normal 
and  the  saturated  calomel  electrodes.  See  table  53. 

Fales  and  Mudge  seem  not  to  have  made  any  independent  measurements 
which  furnish  more  reliable  values  for  the  difference  of  potential  between  a 
saturated  calomel  half-cell  and  the  "normal  hydrogen  electrode."  These 
authors  have  however  extended  the  work  of  Michaelis  and  have  found 


314 


THE    DETERMINATION    OF   HYDROGEN   IONS 


evidence  that  the  saturated  calomel  half -cell  is  reliable  within  the  tempera- 
ture interval  5°-60°C. 

S0rensen  and  Linderstr0m-Lang  (1924)  are  of  the  opinion  that  the  satu- 
rated potassium  chloride  calomel  half -cell,  "which  offers  certain  advantages 
as  a  working  electrode  is  hardly  suitable  as  a  standard."  In  their  study  of 
calomel  half -cells  with  solutions  of  potassium  chloride  more  concentrated 
than  no rmal  they  used  3.5  NKC1.  They  cite  a  number  of  investigations, 
chiefly  in  Danish  laboratories,  of  the  difference  of  potential  between  this 
half -cell  and  the  tenth  normal  half -cell  at  18°  and  give  0.0831  as  the  best 
value .  This  is  the  value  of  Gj  aldbaek  (1924) . 

TABLE  53 

Potentials  of  tenth  normal  and  saturated  calomel  half -cells 
(After  Michaelis  (1914)) 


TEMPERATURE 

TENTH  NORMAL 

SATURATED 

15 

0.2525 

16 

0.2517 

17 

0.2509 

18 

0.3377 

0.2503 

19 

0.2495 

20 

0.3375 

0.2488 

21 

0.2482 

22 

0.2475 

23 

0.2468 

24 

0.2463 

25 

0.2458 

30 

0.3364 

37 

0.2355 

38 

0.3355 

0.2350 

40 

0.3349 

50 

0.3326 

60 

0.3290 

TEMPERATURE    COEFFICIENTS 

We  have  no  concern  for  the  temperature  coefficient  of  the  ab- 
solute potential  difference  at  the  calomel  electrode.  By  agreement 
the  potential  assigned  is  that  of  the  cell 


Hg 


HgCl,  KC1 


H+ 

a  =  1 


Pt,  H2  (1  atmos.) 


when  the  potential  difference  at  the  normal  hydrogen  electrode  is 
assumed  to  be  zero  at  all  temperatures. 


XV  SILVER   CHLORIDE   ELECTRODE  315 

Thus  it  comes  about  that  the  absolute  temperature  coefficient 
for  the  saturated  calomel  half-cell  (as  measured  directly  in  ab- 
sence of  thermal  equilibrium)  is  low  and  positive  while  by  the 
standard  of  reference  it  is  high  and  negative. 

There  exists  in  the  literature  considerable  confusion  in  regard  to 
this  matter.  Its  further  discussion  will  be  postponed  to  .Chapters 
XXII  and  XXIII,  since  the  question  of  temperature  coefficients  is 
of  importance  to  the  subject  as  a  whole. 

THE   SILVER   CHLORIDE   ELECTRODE 

Comparable  in  principle  to  the  so-called  calomel  electrode  is 
the  half-cell:  Ag|AgCl,  definite  chloride  solution.  This  is  fre- 
quently called  the  silver  chloride  electrode.  It  may  be  used  as  a 
standard  half-cell  just  as  the  mercury-calomel-KCl  half-cell  is 
used;  but  it  has  been  put  to  use  chiefly  in  theoretical  studies  on 
the  activities  of  chlorides  in  solution. 

Linhart  (1919)  prepared  his  silver  as  follows:  "the  silver  was  deposited 
by  a  current  of  5  to  7  amperes  in  a  cell  consisting  of  an  anode  of  silver  and  a 
cathode  of  fine  platinum  wire,  dipping  into  a  solution  of  silver  nitrate. 
Under  the  influence  of  this  large  current  the  silver  gathered  about  the 
platinum  wire  in  loose,  spongy  clots  easily  loosened  by  a  slight  tapping 
of  the  wire.  The  silver  so  obtained  was  then  washed  and  kept  under  pure 
water  until  needed." 

Giintelberg  (1926)  confirms  American  workers  in  finding  that 
silver  formed  from  cyanide  solutions  gives  a  more  negative  poten- 
tial than  those  samples  which  are  deposited  from  silver  nitrate 
solutions,  from  the  reduction  of  silver  nitrate  with  ferrous  sulfate 
(Br0nsted)  or  by  heating  Ag20  (Lewis).  He  used  a  spiral  of 
platinum  covered  with  Ag2O,  converted  the  latter  to  silver  at 
500°  and  then  deposited  AgCl  by  electrolysis.  He  keeps  oxygen 
out  by  use  of  pure  nitrogen  and  surrounds  the  electrode  with 
AgCl  crystals  made  by  the  slow  removal  of  ammonia  (over 
sulfuric  acid)  from  ammoniacal  silver  solutions. 

Maclnnes  and  Beattie  (1920)  find  it  advisable  to  deposit  the 
silver  chloride  from  a  solution  of  the  same  composition  and  con- 
centration as  that  to  be  used  as  electrolyte. 

They  formed  a  thick  deposit  of  silver  on  1.5  cm.  sq.  platinum 
gauze  by  electrolysis  (3  milliamperes,  24  hours)  in  potassium  silver 
cyanide.  After  washing  the  electrode  they  deposited  a  coating  of 


316  THE    DETERMINATION    OF    HYDROGEN    IONS 

silver  chloride  by  20  minutes  electrolysis  with  5  to  7  milliamperes 
in  lithium  chloride  solution. 

Scatchard  (1925)  gives  0.0453  at  25°C  for  the  potential  of  the 
cell 

-  Hg  |  HgCl,  KC1  (sat.)  $KC1  (0.1  Molal),  AgCl  |  Ag  +  and. 
0.0466  at  25°C.  for  the  potential  of  the  cell 
-  Ag  |  AgCi,  KC1  (0.1  Molal)    KC1  (0.1  Molal),  HgCl  |  Hg  + 

For  details  concerning  this  half-cell  see :  Br0nsted  (1920),  Gerke 
(1922),  Giintelberg  (1926),  Jahn  (1900),  Lewis  (1906),  Linhart 
(1919),  Maclnnes  and  Beattie  (1920),  Maclnnes  and  Parker 
(1915),  Noyes  and  Ellis  (1917),  Scatchard  (1925),  Sheppard  and 
Elliott  (1920),  and  Randall  and  Young  (1928). 

THE    MERCURY-MERCURIC   OXIDE    ELECTRODE 

This  has  played  its  part  in  the  examination  of  alkaline  solutions. 
See  Chapter  XX. 

MISCELLANEOUS   STANDARD    HALF-CELLS 

As  described  in  Chapter  X  a  hydrogen  electrode  half-cell  with 
a  solution  of  known  hydrogen  ion  concentration  is  useful.  Such 
half -cells  require  no  further  mention  here.  However  it  may  be 
noted  that  Pinkhof  (1919)  suggested  special  half-cells  with  single 
potentials  equal  to  those  of  a  hydrogen  electrode  at  selected  end- 
points  of  tit  rations.  Sharp  and  MacDougall  (1922)  describe  lead 
and  cadmium  electrodes  having  such  potentials  for  the  range  pH 
4  to  pH  10.  Such  devices  are  of  little  use  except  for  standardized 
procedures  of  extensive  routine.  Then  they  may  be  very  useful. 

In  addition  there  are  the  innumerable  electrodes  of  general 
electro-chemistry.  References  to  the  older  literature  will  be  found 
assembled  by  Abegg,  Auerbach  and  Luther  (1911-1915).  Lewis 
and  Randall  in  Thermodynamics  have  discussed  several  standard 
half-cells  which  may  be  adapted  to  special  purposes  in  the  con- 
struction of  cells  one  half-cell  of  which  is  to  be  the  hydrogen  half- 
cell. 

Of  very  great  usefulness  is  the  quinhydrone  electrode  in  stand- 
ardized solution.  See  Chapter  XIX. 


CHAPTER  XVI 

THE  POTENTIOMETER,  NULL-POINT  INSTRUMENTS  AND  ACCESSORY 

EQUIPMENT 

An  excellent  example  of  an  actual  process  which  is  very  nearly  rever- 
sible is  furnished  when  the  electromotive  force  of  a  galvanic  bat- 
tery is  measured  by  means  of  a  sensitive  potentiometer. — LEWIS 
AND  RANDALL. 

With  the  newest  galvanometers  you  can  very  well  observe  currents    • 
which  would  require  to  last  a  century  before  decomposing  one 
milligram  of  water.— HELMHOLTZ  (in  1881). 

We  ordinarily  speak  of  measuring  the  electromotive  force  of  a 
cell  in  a  casual  manner  as  if  it  were  merely  the  measurement  of  a 
potential  difference.  However,  it  is  perfectly  well  known  that 
if  the  cell  is  allowed  to  furnish  current  it  will  "run  down"  and 
ultimately  will  furnish  no  electromotive  force.  To  allow  the  cell 
to  furnish  current  during  the  measurement  is  obviously  to  take 
the  measurement  with  declining  potential.  Likewise  the  cell, 
if  reversible,  will  act  as  an  accumulator  when  current  is  fed  to  it. 
To  put  the  matter  more  elegantly  we  may  say  that  the  measure- 
ment must  be  made  under  conditions  of  reversibility  and  maximum 
work  (see  Chapter  XI).  Therefore,  instead  of  applying  directly 
some  instrument  such  as  a  volt-meter,  which  draws  current,  we 
nicely  balance  the  electromotive  force  of  the  cell  by  an  opposing, 
external  electromotive  force.  No  current  passes  through  the 
cell  at  such  a  balance.  This  lack  of  current  is  made  evident  by 
absence  of  effect  in  an  indicating  instrument,  the  null-point  in- 
strument. 

This  is  the  Poggendorf  compensation  method,  the  poten- 
tiometer method.  In  a  sense  the  null-point  instrument,  for 
example,  a  galvanometer,  serves  two  purposes;  that  of  an  indi- 
cator in  the  potentiometric  method  itself,  and  that  of  an  indi- 
cator of  the  fact  that  so  far  as  the  electrical  phenomena  themselves 
are  concerned  the  cell  is  operating  close  to  that  infinitesimal  rate 
which  is  one  condition  of  maximum  work. 

317 


318 


THE    DETEEMINATION    OF   HYDROGEN   IONS 


THE   POTENTIOMETER 

The  principle  of  the  potentiometer  may  be  illustrated  by  the 
arrangement  shown  in  figure  53  which  is  suitable  for  very  rough 
measurements. 

According  to  elementary  modern  theory  the  flow  of  electricity 
in  metals  is  the  flow  of  electrons,  the  electron  being  the  unit 
electrical  charge.  By  an  unfortunate  chance  the  two  kinds  of 
electricity,  which  were  recognized  when  a  glass  rod  was  rubbed 
with  silk,  were  given  signs  (+  for  the  glass  and  —  for  the  silk) 
which  now  leave  us  in  the  predicament  of  habitually  speaking  of 
the  flow  of  positive  electricity  when  the  evidence  is  for  the  flow 


FIG.  53.  ELEMENTARY  POTENTIOMETER 

of  negative  charges,  the  electrons.  But  so  far  as  the  illustration 
of  principles  is  concerned  it  makes  little  difference  and  we  shall 
depart  from  custom  and  shall  deal  with  the  negative  charges  in 
order  to  make  free  use  of  a  helpful  but  very  incomplete  analogy. 
We  may  imagine  the  electrons,  already  free  in  the  metal  of  our 
electrical  conductors,  to  be  comparable  with  the  molecules  of  a 
gas  which  if  left  to  themselves  will  distribute  themselves  uni- 
formly throughout  their  container  (the  connected  metallic  parts 
of  our  circuits).  We  may  now  imagine  the  battery  S  (fig.  53) 
as  a  pump  maintaining  a  flow  of  gas  (electrons)  through  pipes 
(wires)  to  R  to  A  to  B  and  back  to  S.  The  pipe  (wire)  AB 


XVI  POTENTIOMETER  319 

offers  a  uniform  resistance  to  the  flow  so  that  there  is  a  uniform 
fall  of  pressure  (potential)  from  A  to  B  while  the  pump  (battery) 
S  maintains  a  uniform  flow  of  gas  (electrons).  If  we  lead  in  at 
C  and  D  the  ends  of  the  pipes  (wires)  from  another  pump  (battery) 
X,  taking  care  that  the  high  pressure  pipe  (wire)  from  X  leads 
in  on  the  high  pressure  side  of  AB,  we  can  move  C,  D  or  both 
C  and  D  until  they  span  a  length  of  AB  such  that  the  difference 
of  pressure  (difference  of  potential)  between  C  and  D  on  AB  is 
equal  and  opposite  to  the  difference  of  pressure  (difference  of 
potential)  exerted  between  C  and  D  by  X.  Then  no  current 
can  flow  from  X  through  the  current-indicating  instrument  G 
and  we  thereby  know  that  balance  is  attained. 

If  we  know  the  fall  of  electrical  potential  per  unit  length  along 
AB  the  difference  of  potential  exerted  by  X  will  be  known  from 
the  length  of  wire  between  C  and  D.  We  now  come  to  the  man- 
ner in  which  this  fall  of  potential  per  unit  length  is  determined. 

Choosing  for  units  of  electrical  difference  of  potential,  electrical 
resistance  and  electrical  current,  the  volt,  the  ohm,  and  the  am- 
pere respectively,  we  find  that  they  are  related  by  Ohm's  law: 

,  f.  s      Difference  in  potential  (in  volts) 

Current  (in  amperes)  = 

Resistance  (in  ohms) 

or 

ci  (1) 

With  this  relation  we  could  establish  the  fall  of  potential  along 
AB  by  measuring  the  resistance  of  AB  and  the  current  flowing. 
But  this  is  unnecessary,  for  we  have  in  the  Weston  cell  a  standard 
of  electromotive  force  (E.M.F.)  which  may  be  directly  applied 
in  the  following  manner.  The  unknown  X  (figure  53)  is  switched 
out  of  circuit  and  in  its  place  is  put  a  Weston  cell  of  known  E.M.F. 
Adjustment  of  C  and  D  is  made  until  the  "null-point"  is  attained, 
when  the  potential  difference  between  the  new  positions  of  C  and 
D  is  equal  to  the  E.M.F.  of  the  Weston  cell.  From  such  a 
setting  the  potential  fall  per  unit  length  of  AB  is  calculated.  It 
must  be  especially  noted  however  that  for  such  a  procedure  to 
be  valid  the  current  in  the  potentiometer  circuit  must  be  kept 
constant  between  the  operations  of  standardization  and  of  measure- 


320 


THE  DETEKMINATION  OF  HYDROGEN  IONS 


ment  for  the  fundamental  relationship  upon  which  reliance   is 
placed  is  that  of  Ohm's  law,  C  =  — . 

It  will  be  noted  that  the  establishment  of  the  difference  of  po- 
tential between  any  two  points  on  AB  by  the  action  of  S  and  the 
resistance  of  AB  is  strictly  dependent  upon  the  relation  given  by 
Ohm's  law;  but,  since  we  draw  no  current  from  X  when  balance 
is  attained,  the  resistance  of  its  circuit  is  of  no  fundamental  im- 
portance. It  only  affects  the  current  which  can  flow  through  the 


+  0 


FIG.  54.  WIRING  OF  THE  LEEDS  AND  NORTHRUP  POTENTIOMETER  (TYPE  K) 
(Courtesy  of  Leeds  and  Northrup  Company) 

indicating  instrument  G  when  the  potential  differences  are  out 
of  balance.  It  is  therefore  concerned  only  in  the  sensitivity  of  G. 

The  simple  potentiometer  system  described  above  is  susceptible 
to  refinement  both  in  precision  and  in  convenience  of  operation. 

With  the  inevitable  variations  in  the  potentiometer  current 
which  occur  as  the  battery  runs  down  it  would  be  necessary  to 
recalculate  from  moment  to  moment  the  difference  of  potential 
per  unit  length  of  the  wire  AB  if  the  procedure  so  far  described 
were  used.  This  trouble  is  at  once  eliminated  if  the  contacts  of 
the  Weston  cell  can  be  thrown  in  at  fixed  points  and  the  current 
be  then  adjusted  by  means  of  the  rheostat  R  so  that  there  is 


XVI 


POTENTIOMETER 


321 


always  the  same  uniform  current  producing,  through  the  re- 
sistance between  the  Weston  cell  contacts,  the  potential  dif- 
ference of  this  standard  cell.  Having  thus  arranged  for  the 
adjustment  of  a  uniform  current  at  all  times  and  having  the  re- 
sistance of  AB  already  fixed  it  is  now  permissible  to  calibrate  the 
wire  AB  in  terms  of  volts. 

In  the  Leeds  and  Northrup  potentiometer  (fig.  54),  the  resist- 
ance AB  of  the  elementary  instrument  (fig.  53)  is  divided  into  two 
sections  one  of  which  A-D  (fig.  54)  is  made  up  of  a  series  of 
resistance  coils  between  which  M  makes  contact  and  the  other 
portion  of  which  is  a  resistance  wire  along  which  M'  can  slide. 


FIG.  55.  THE  LEEDS  AND  NORTHRUP  POTENTIOMETER 
(Courtesy  of  Leeds  and  Northrup  Company) 

When  the  potentiometer  current  has  been  given  the  proper  value, 
in  the  manner  which  will  be  described,  the  fall  of  potential  across 
any  one  of  the  coils  is  0.1  volt  so  that  as  M  is  shifted  from  the 
zero  point  0  the  potential  difference  between  M  and  D  is  in- 
creased 0.1  volt  at  each  step.  Likewise,  when  the  current  is  in 
adjustment,  the  shifting  of  M'  away  from  D  increases  by  in- 
finitesimal1 fractions  of  a  volt  the  difference  of  potential  between 
M  and  M'. 

To  adjust  the  potentiometer  current  so  that  the  several  re- 

1  There  is,  of  course,  a  limit,  an  indefinite  limit,  to  the  divisions  readable. 
There  is  also  a  limit  below  which  a  reading  would  have  no  meaning  if  the 
errors  of  calibration  were  neglected. 


322 


THE    DETERMINATION    OF   HYDROGEN   IONS 


sistances  in  the  potentiometer  circuit  will  produce  the  differences 
of  potential  in  terms  of  which  the  instrument  is  calibrated,  use 
is  made  of  the  Weston  cell  in  the  following  manner.  By  means 
of  a  switch,  U,  the  unknown  is  thrown  out  and  the  Weston  cell 
is  thrown  into  circuit.  One  pole  of  the  Weston  cell  circuit  is 
fixed  permanently.  The  other  can  be  moved  along  a  resistance 
at  T,  constructed  so  that  the  dial  indicates  the  value  of  the 
particular  cell  in  use.  When  so  placed  as  to  correspond  with  the 
value  of  the  Weston  cell  in  use  this  contact  at  T  is  left  in  its 
position.  Now  the  current  flowing  from  the  battery  W  is  ad- 
justed by  means  of  the  rheostat  R  until  the  difference  of  poten- 


FIG.  56.  ARRANGEMENT  OF  "RESISTANCE  BOXES"   FOR  POTENTIOMETER 

tial  between  T  and  0.5  balances  the  potential  difference  of  the 
Weston  cell  as  indicated  by  the  cessation  of  current  in  the  galva- 
nometer GA.  The  resistance  T  to  0.5  is  such  that  the  E.M.F. 
of  the  battery  acting  across  this  resistance  will  produce  the 
desired  potentiometer  current.  This  current  now  acting  across 
the  several  resistances  furnishes  the  indicated  potentials,  i.e.,  a 
potential  difference  of  0.1  volt  across  each  coil. 

Another  arrangement  which  employs  the  ordinary  sets  of  re- 
sistances in  common  use  is  illustrated  in  figure  56. 

A  and  B  are  duplicate  sets  of  resistances  placed  in  series  with 
the  battery  Ba  and  adjusting  rheostats  RI  and  R2.  If  the  cur- 


XVI  RESISTANCE-BOX   POTENTIOMETER  323 

rent  be  kept  uniform  throughout  this  system  the  potential  dif- 
ference across  the  terminals  of  B  can  be  varied  in  accordance 
with  Ohm's  law  by  plugging  in  or  out  resistance  in  B.  But  to 
keep  the  current  constant,  while  the  resistance  in  B  is  changed, 
a  like  resistance  is  added  to  the  circuit  at  A  when  it  is  removed 
from  B,  and  removed  from  A  when  it  is  added  to  B. 

As  mentioned  before,  the  potential  difference  could  be  deter- 
mined from  the  resistance  in  B  and  a  measurement  of  the  current ; 
but  this  is  avoided  by  the  direct  application  of  a  Weston  cell  of 
known  potential.  Assuming  constant  current,  a  Weston  cell,  W, 
replaces  X  by  adjustment  of  switch  S.  Adjustment  to  the  null- 
point  is  made  by  altering  the  resistance  in  B  with  compensation 
in  A.  The  unknown  is  then  thrown  into  circuit  and  adjustment 
of  resistance  made  to  the  null-point  by  changing  A  and  B.  If 
Ew  is  the  known  E.M.F.  of  the  Weston  cell,  Ex  the  potential 
of  the  measured  cell,  rw  the  resistance  in  circuit  when  the 
Weston  cell  is  in  balance  and  rc  the  resistance  in  circuit  when 
the  measured  cell  is  in  balance  we  have 

C  (constant)  =  -  -  =  - 
rc        rw 

Whence 

Trt       _   TP       c  ff)\ 

ILX  =  ±LW—  (2) 

The  system  is  improved  by  providing  rheostats  RI  and  R2  to 
regulate  the  potentiometer  current  till  constant  difference  of 
potential  is  attained  between  terminals.  Then  the  resistances 
may  be  calibrated  in  volts. 

It  is  further  improved  by  introducing  resistance  Rw,  placed  as 
is  the  exterior  resistance  T  of  figure  54,  and  Weston  cell  at  W. 

It  will  be  noted  that  in  this  arrangement  every  one  of  the  plug 
contacts  is  in  the  potentiometer  circuit.  A  bad  contact,  such  as 
may  be  produced  by  failure  to  seat  a  plug  firmly  during  the 
plugging  in  and  out  of  resistance,  or  by  corrosion  of  a  plug  or 
dial  contact,  will  therefore  seriously  affect  the  accuracy  of  this 
potentiometer  system.  It  requires  constant  care. 

Lewis,  Brighton  and  Sebastian  (1917)  used  two  decade  resist- 


324         THE  DETERMINATION  OF  HYDROGEN  IONS 

ance  boxes  of  9999  ohms  each.  With  an  external  resistance  the 
current  was  adjusted  to  exactly  0.0001  ampere.  Thus  each  ohm 
indicated  by  the  resistance  boxes  when  balance  was  attained  cor- 
responded to  0.0001  volt.  Their  standard  cell  which  gave  at 
25°  1.0181  volts  was  spanned  across  B  (fig.  56)  and  182  ohms  of 
the  external  resistance,  Rw. 

Another  mode  of  using  the  simple  system  illustrated  in  figure 
53  is  a  device  frequently  used  by  physicists,  and  introduced  into 
hydrogen  electrode  work  by  Sand  (1911)  and  again  by  Hilde- 
brand  (1913).  Instead  of  calibrating  unit  lengths  along  AD 
by  means  of  the  Weston  cell,  or  otherwise  applying  the  Weston 
cell  directly  in  the  system,  the  contacts  C  and  D  carry  the  termi- 
nals of  a  voltmeter.  When  balance  is  attained  this  voltmeter 
shows  directly  the  difference  of  potential  between  C  and  D,  and 
therefore  the  E.M.F.  of  X.2 

A  diagram  of  such  an  arrangement  is  shown  in  figure  57. 
There  is  an  apparent  advantage  in  the  fact  that  the  Weston  cell 
may  be  dispensed  with  and  resistance  values  need  not  be  known. 
There  are  however  serious  limitations  to  the  precision  of  a  volt- 
meter and,  in  two  cases  which  the  author  knows,  accuracy  within 
the  limited  precision  of  the  instruments  was  attained  only  after 
recalibration. 

A  voltmeter  is  generally  calibrated  for  potential  differences 
imposed  at  the  terminals  of  leads  supplied  with  the  instrument. 

Turning  again  to  figure  53  we  recall  that  when  any  given  fall 
of  potential  occurs  between  A  and  B,  a  definite  current  flows  in 
the  circuit  SRAB.  If  the  resistance  of  AB  is  known,  a  measure 
of  the  current  flowing  permits  one  to  calculate  the  fall  of  poten- 
tial between  A  and  B,  Thus  a  current-measuring  instrument 
(ammeter)  placed  in  series  with  the  fixed  resistance  AB  may  be 

2  It  is  sometimes  assumed  that  because  the  circuit  of  the  system  under 
measurement  is  placed  in  the  position  of  a  shunt  on  the  potentiometer  cir- 
cuit that  its  resistance  must  be  high  in  order  that  CD  (fig.  53)  may  indicate 
correctly  the  potential  difference.  The  fact  that  no  current  flows  in  this 
branch  when  balance  obtains  shows  clearly  that  its  resistance  can  have  no 
effect  on  the  accuracy  of  the  indication.  It  has  also  been  assumed  that  if 
CD  is  spanned  by  a  voltmeter,  the  resistance  of  the  voltmeter  should  be 
taken  into  consideration.  But  a  voltmeter  is  calibrated  to  always  indicate 
the  potential  difference  between  its  terminals,  which  should  be  considered 
part  of  the  instrument  itself. 


XVI 


VOLT-METER    SYSTEM 


325 


calibrated  to  indicate  differences  of  potential  between  A  and  B. 
To  use  this  system  the  terminals  of  the  cell  C  and  D  (fig.  53) 
are  moved  to  A  and  B  and  there  permanently  fixed.  An  am- 
meter is  placed  between  R  and  S  and  adjustment  of  R  is  made 
until  no  current  flows  in  G.  The  difference  of  potential  between 
A  and  B,  as  indicated  by  the  calibrated  and  renamed  reading  of 
the  ammeter,  is  then  equal  to  the  E.M.F.  of  the  gas  chain. 

Much  the  same  limitations  noted  in  the  voltmeter  system  apply 
to  the  ammeter  system. 


FIG.  57.  VOLTMETER  POTENTIOMETER  SYSTEM 


A  modification  of  the  system  briefly  described  above  is  found 
in  the  "Pyrovolter."  The  essential  modification  is  a  device  of 
wiring  whereby  the  same  indicating  instrument  is  used  to  measure 
current  (indicated  in  volts)  and  to  indicate  the  null-point. 

Of  potentiometer  characteristics  little  need  be  said  for  the 
choice  in  the  first  instance  will  lie  between  instruments  sold  by 
reliable  makers.  In  the  second  instance  the  choice  will  lie  be- 
tween instruments  of  different  range  and  many  of  the  unique 


326  THE    DETERMINATION    OF   HYDROGEN   IONS 

instruments  may  be  at  once  eliminated  by  a  calculation  which 
shows  that  the  reputed  accuracy  involves  too  close  a  scale  read- 
ing to  be  reliable.  Certain  difficulties  which  enter  into  the 
construction  of  potentiometers  for  accurate  thermo-couple  work 
are  hardly  significant  for  the  order  of  accuracy  required  of  hydro- 
gen electrode  work.  The  range  from  zero  to  1.2  volts  and  the 
subdivisions  0.0001  volt  do  for  measurements  of  ordinary  range 
and  accuracy.  There  should  be  a  variable  resistance  to  accom- 
modate the  variations  in  individual  Weston  cells  of  from  1.0.175 
to  1.0194  volts,  and  provision  for  quickly  and  easily  interchanging 
Weston  cells  with  measured  E.M.F. 

Several  of  the  features  of  standard  potentiometers  may  be 
eliminated  to  reduce  their  cost  without  injury  to  their  use  for 
hydrogen  electrode  measurements.  Steps  in  this  direction  have 
been  taken  by  at  least  one  manufacturer. 

Having  described  the  fundamental  principles  of  the  potentiom- 
eter it  seems  hardly  worth  while  to  discuss  the  numerous  modi- 
fications found  among  manufactured  instruments  or  used  in  the 
construction  of  home-made  designs.  With  the  advent  into  every 
town  of  the  numerous  and  varied  parts  of  radio  apparatus  cer- 
tain accessory  parts  of  a  potentiometer  may  be  readily  purchased 
and  the  amateur  can  concentrate  his  attention  upon  the  essential 
resistances.  But,  unless  he  is  equipped  to  make  these  with 
accuracy  and  to  mount  them  with  care,  he  may  waste  the  cost  of 
a  satisfactory  instrument. 

With  regard  to  the  more  special  or  unique  designs  found  on 
the  market  it  may  simply  be  said  that  they  were  developed  for 
special  purposes  and  that  unless  these  special  purposes  are  to  be 
accommodated,  the  purchaser  will  do  well  to  depend  only  upon 
an  instrument  of  universal  applicability. 

When  rubber  is  used  as  the  insulating  material  of  instruments 
employed  as  potentiometers  the  rubber  should  not  be  left  exposed 
to  the  light  unduly.  The  action  of  the  light  not  only  injures 
the  appearance  of  the  rubber  but  also  may  cause  the  formation 
of  conducting  surface  layers. 

If  the  potentiometer  system  contains  a  sliding  contact  and 
this  contact  is  not  involved  in  the  resistance  of  the  primary  poten- 
tiometer circuit  proper,  the  contact  should  be  kept  heavily  coated 
with  pure  vaseline.  If  there  be  any  doubt  whatever  about  the 


XVI 


BALLISTIC    GALVANOMETER 


327 


quality  of  this  vaseline  it  should  be  boiled  with  several  changes 
of  distilled  water,  skimmed  off  when  cool  and  then  thoroughly 
dried.  If  this  is  done  there  will  seldom  be  any  need  to  resort  to 
the  heroic  and  dangerous  procedure  of  polishing. 

It  cannot  be  too  strongly  emphasized  that  while  a  low  order 
of  precision  is  often  adequate  for  a  certain  purpose  the  employ- 
ment of  crude  measuring  instruments  often  obscures  the  data  of 
greatest  significance.  This  statement  should  not  be  interpreted 
as  a  discouragement  to  those  who  are  about  to  undertake  measure- 
ments with  some  such  system  as  that  illustrated  in  figure  57 


FIG. 


58.  DIAGRAM   OP   CONNECTIONS   FOR   CONDENSER   METHOD   OF 

MEASURING  POTENTIAL  DIFFERENCES 
(Courtesy  of  Leeds  and  Northrup  Company) 


for  important  data  have  been  obtained  with  just  such  instruments. 
The  statement  is  intended  rather  as  an  encouragement  to  the 
beginner  who  will  find  the  handling  of  more  precise  instruments 
easy  and  the  rewards  rich. 

BALLISTIC   GALVANOMETER   SYSTEM 

In  a  few  instances  there  has  been  employed  a  system  of  meas- 
urement, the  principle  of  which  is  illustrated  in  the  wiring  diagram 
of  figure  58.  See  Beans  and  Oakes  (1920).  The  E.M.F.  of  a 
cell  is  allowed  to  charge  a  fixed  condenser.  By  throwing 


328  THE   DETERMINATION    OF   HYDROGEN   IONS 

the  discharge  key  to  the  right  the  charge  accumulated  by  the 
condenser  is  allowed  to  discharge  through  a  ballistic  galvanometer, 
the  deflection  in  which  may  be  made  a  measure  of  the  accumu- 
lated charge  and  hence  of  the  E.M.F.  of  the  cell. 

The  ballistic  galvanometer  is  one  designed  to  indicate  by  the 
angular  deflection  of  its  coil  the  quantity  of  electricity  passing 
through  the  coil  as  a  sudden  discharge.  The  quantity  of  elec- 
tricity stored  in  the  condenser  is  a  function  of  its  dimensions 
and  material  and  of  the  difference  of  potential  imposed  at  its 
terminals.  The  dimensions  and  material  being  fixed,  the  charge 
becomes  proportional  to  the  difference  of  potential.  A  definite 
difference  of  potential  may  be  imposed  by  means  of  the  Weston 
cell.  The  resulting  charge  in  the  condenser  is  discharged  through 
the  ballistic  galvanometer  giving  the  coil  a  definite  deflection. 
This  serves  to  calibrate  a  given  set-up  if  the  galvanometer  is  so 
designed  that  the  deflection  at  each  section  of  the  scale  is  propor- 
tional to  the  quantity  of  electricity  discharged  through  the  coil 
and  if  the  wiring  be  such  that  no  serious  changes  of  capacity  and 
inductance  occur  in  manipulation. 

The  advantage  of  this  condenser  method  is  that  the  condenser 
may  be  conveniently  made  of  such  capacity  that  insignificant 
current  is  drawn  from  the  cell  under  measurement.  If,  then,  the 
technique  used  at  the  electrodes  is  refined,  it  should  be  possible 
to  measure  equilibrium  potentials  which  would  be  easily  dis- 
placed by  current  withdrawal.  However,  until  there  are  pub- 
lished more  definite  data  relating  the  conditions  of  electrode 
measurements  to  the  theory  of  the  condenser  method,  this 
system  is  not  to  be  recommended  for  ordinary  use. 

USES   OF   THE   ELECTRON   TUBE 

The  3-electrode  thermionic  vaccum  tube  has  been  used-  in 
several  arrangements  for  following  changes  in  the  electromotive 
forces  of  cells. 

The  tube  referred  to  is  one  or  another  of  the  several  tubes  used 
as  detectors  or  amplifiers  in  radio  communication.  A  glass  tube 
(figure  59  (1)),  exhausted  to  a  very  low  gas  pressure  is  supplied 
with  an  atmosphere  of  electrons  by  their  emission  from  the  hot 
iilament  F.  These  electrons  produce  what  may  be  called  a  space 
^charge  in  the  tube.  Surrounding  the  filament  is  a  metallic  sheath 


XVI 


ELECTRON   VALVE 


329 


called  the  plate,  P.  If  this  is  maintained  by  the  battery  B  at  a 
potential  positive  to  the  filament,  the  electrons  will  migrate  to 
the  plate  and  there  is  established  a  unidirectional  current  known 
as  the  plate  current.  Interposed  between  filament  and  plate  is 
a  grid,  G,  of  wire  or  perforated  sheet  metal,  through  which  the 
electrons  must  pass  in  their  migration  from  filament  to  plate. 


FIG.   59.  WIRING  DIAGRAMS  FOR  ELECTRON  VALVE  "POTENTIOMETERS" 

If  this  grid  be  charged  positively  with  relation  to  the  filament 
it  will  aid  in  the  withdrawal  of  electrons  from  the  filament;  but 
if  this  grid  be  charged  negatively  with  relation  to  the  filament  it 
will  oppose  the  electron  emission.  In  figure  60  there  is  shown 
by  the  curve  marked  0  the  plate  current  at  different  plate 
voltages  when  the  grid  is  not  charged.  For  such  a  relation  the 
filament  must  be  maintained  with  constant  current.  If  a  posi- 


330 


THE  DETERMINATION  OF  HYDROGEN  IONS 


tive  potential  of  4.5  volts  is  placed  on  the  grid,  the  plate  current, 
with  change  of  plate  potential,  follows  the  indicated  curve  of  figure 
60.  Now  choose  constant  plate  voltage,  e.g.,  40  volts  and  see  the 
second  chart  of  figure  60.  The  plate  current  is  now  revealed  as 
a  function  of  grid  potential.  If  the  filament  current  were  now 
increased  the  curve  would  be  shifted.  If  the  plate  current  is  to 
be  nearly  a  linear  function  of  grid  potential,  the  plate  potential, 
filament  current  and  the  grid  potential  itself  must  be  adjusted 
till  the  operation  is  within  the  straighter  portion  of  such  a  curve. 
Goode  in  his  first  article  gives  the  relation  between  grid  potential 
and  grid  current  shown  in  figure  60  for  the  particular  tube  and 


*)IO 

U 


111 

$' 


20     40     60    80     100   120 
PLATE    POTENTIAL 


GRID     POTENTIAL 


100 


9550 

o 


-1.0      -,5  0         +.5       4-1.0 

GRID.   VOLTS  TO  -  END  OF  FILAMENT 

FlG.    60 


working  condition  he  used.  He  notes  that,  unless  the  grid  be 
given  a  negative  potential,  enough  current  may  be  drawn  to 
discharge  a  hydrogen  electrode.  He,  therefore,  connected  the 
hydrogen  electrode  terminal  to  the  grid  and  the  calomel  electrode 
terminal  to  the  negative  end  of  the  filament.  Others  use  a  "C" 
battery  to  make  the  grid  more  negative.  This  should  not  be 
overdone,  for  slight  currents  in  the  opposite  direction  may  be 
produced  in  the  grid  circuit  as  the  grid  is  made  more  negative. 

Goode  (1922)  applies  the  principle  in  the  device  shown  by  figure 
59  (2).  The  cell  was  placed  at  X.  A  galvanometer,  I,  was  used 
as  the  plate  current  indicating  instrument.  Since  the  sensitivity 
of  the  galvanometer  was  too  high  its  terminals  were  shunted  by 


XVI  ELECTRON   VALVE  331 

resistances,  R.  A  calibration  curve  was  then  plotted  from  gal- 
vanometer deflections  at  known  potentials  of  X.  Goode  obtained 
good  titration  curves  with  this  device.  He  emphasized  the  ad- 
vantages of  the  principle  to  be :  first,  continuous  reading  without 
the  balancing  for  each  potential  required  in  the  potentiometer 
system;  second,  the  possibility  of  such  a  design  that  no,  or  at 
most  very  little,  current  is  drawn  from  the  cell. 

Goode  called  attention  to  the  fact  that  steady  operation  re- 
quires steady  filament  current.  Williams  and  Whitenach  (1927) 
introduce  a  rheostat  R  and  ammeter  M  (see  figure  59  (3)),  to 
aid  in  this  control.  By  reference  to  figure  60  it  will  be  observed 
that  the  plate  current  declines  as  the  grid  potential  becomes  more 
negative.  By  use  of  a  "C"  battery  (Figure  59  (3))  Williams  and 
Whitenach  were  able  to  operate  with  the  galvanometer  un- 
shunted.  Bienfait  (1926)  (see  figure  59  (4))  introduces  as  a 
current  indicating  instrument  a  millivolt  meter,  I,  of  300  ohms 
and  scale  range  of  17  millivolts.  The  compensation  current  and 
value  per  scale  division  on  this  reading  instrument  are  regulated 
by  rheostats. 

Goode  (1925)  elaborated  upon  his  original  design  by  that 
shown  in  figure  59  (5).  However,  he  has  recently  replaced  this 
(personal  communication)  with  a  two  valve  system,  which  he  has 
so  wired  that  the  indicating  current  shown  by  a  milliammeter 
of  15  milliampere  range  is  very  closely  proportional  to  the  po- 
tential difference  between  filament  and  grid  produced  by  the  cell 
under  measurement. 

It  is  sometimes  stated  that  the  use  of  the  electron  valve  in- 
volves no  withdrawal  of  current  from  the  cell  under  measure- 
ment. Whether  this  is  true  or  not  in  the  specific  case  depends 
upon  the  characteristics  of  the  particular  tube  in  use  and  how 
they  are  utilized  but  particularly  upon  the  negativity  of  the  grid 
with  relation  to  the  filament.  Goode  in  a  private  communica- 
tion cites  evidence  that  he  can  produce  conditions  under  which 
no  appreciable  current  is  drawn. 

Since  the  operation  of  a  tube  depends  upon  its  characteristics 
which  may  change,  upon  filament  current,  which  may  change, 
upon  "B"  battery  potential,  which  may  change,  calibration  of 
the  relations  between  indicating  current  and  grid-filament  poten- 
tial difference  is  necessary  not  only  in  the  first  instance  but  at 


332         THE  DETERMINATION  OF  HYDROGEN  IONS 

intervals  thereafter.  For  descriptions  of  the  detail  in  the  man- 
agement of  tubes  see  Van  der  Bijl  (1920). 

For  other  wiring  diagrams  and  applications  of  the  electron 
valve  to  cell  measurements  see:  Calhane  and  Gushing  (1923), 
King  (1924),  Treadwell  (1925),  Wendt  (1927),  Pope  and  Gowlett 
(1927),  Buytendyk,  Brinkman  and  Mook  (1927),  Buytendyk  and 
Brinkman  (1927),  and  Voegtlin  and  De  Eds  (1928). 

There  are  various  possible  extensions  of  the  electron  valve  to 
the  purposes  of  hydrion  control  as  in  the  control  of  mechanical 
devices,  etc. 

NULL-POINT   INSTRUMENTS 

Referring  to  figure  53  and  the  accompanying  text  the  reader 
will  see  that  in  the  balancing  of  potential  differences  by  the  Pog- 
gendorf  compensation  method  there  is  required  a  current  indicat- 
ing instrument  to  determine  the  null-point.  Such  instruments 
will  be  briefly  described,  and  some  of  their  characteristics  dis- 
cussed. 

In  the  selection  of  instruments  for  the  measurement  of  the 
electromotive  force  of  cells  it  is  desirable  that  there  should  be  a 
balancing  of  instrumental  characteristics  and  the  selection  of 
those  best  adapted  to  the  order  of  accuracy  required.  A  null- 
point  instrument  of  low  sensitivity  may  annul  the  value  of  a 
well-designed,  expensive  and  accurate  potentiometer;  and  a 
galvanometer  of  excessive  sensitivity  may  be  very  disconcerting 
to  use.  The  potentiometer  system  and  the  null-point  instrument 
should  be  adapted  one  to  the  other  and  to  their  relation  to  the 
system  to  be  measured. 

The  several  corrections  which  have  to  be  found  and  applied  to 
accurate  measurements  of  hydrogen  electrode  potentials  are 
matters  of  a  millivolt  or  two  and  fractions  thereof.  Collectively 
they  may  amount  to  a  value  of  the  order  of  5  millivolts.  Whether 
or  not  such  corrections  are  to  be  taken  into  account  is  a  question 
the  answer  to  which  may  be  considered  to  determine  whether  a 
rough  measuring  system  or  an  accurate  one  is  to  be  used.  For  all 
"rough"  measurements  the  capillary  electrometer  is  a  good  null- 
point  instrument.  It  has  a  sufficiently  high  resistance  to  hinder 
the  displacement  of  electrode  equilibria  at  unbalance  of  a  crude 
potentiometer  system.  It  is  easily  constructed  by  anyone  with 


XVI  GALVANOMETER  333 

a  knowledge  of  the  elements  of  glass  blowing,  and  without  par- 
ticular care  may  be  made  sensitive  to  0.001  volt. 

For  "accurate"  measurements  there  is  little  use  in  making  an 
elaborate  capillary  electrometer  or  in  temporizing  with  poor 
galvanometers. 

The  apportionment  of  galvanometer  characteristics  is  a  compli- 
cated affair  which  must  be  left  in  the  hands  of  instrument  makers, 
but  there  are  certain  relations  which  should  be  fulfilled  by  an  in- 
strument to  be  used  for  the  purpose  at  hand,  and  general  knowl- 
edge of  these  is  quite  necessary  in  selecting  instruments  from  the 
wide  and  often  confusing  variety  on  the  market. 

THE    GALVANOMETER 

The  galvanometer  is  a  current-indicating  instrument,  which, 
in  the  form  useful  for  the  purpose  at  hand,  consists  of  a  coil  of 
wire  suspended  in  the  magnetic  field  of  a  strong  permanent 
magnet.  The  leads  to  the  terminals  of  this  coil  are  the  upper  and 
lower  "suspensions."  They  are  connected  to  the  circuit  in  which 
the  presence  of  current  is  to  be  detected.  If  current  flow  through 
the  coil,  it  will  produce  a  magnetic  field.  This,  interacting  with 
the  field  of  the  permanent  magnet,  causes  the  coil  to  turn  till  it 
tends  to  embrace  the  maximum  number  of  lines  of  force.  Ob- 
viously the  approach  to  the  maximum  is  determined  largely  by 
the  torsion  of  the  suspensions. 

Provision  should  be  made  for  mounting  a  galvanometer  where 
it  will  receive  the  least  vibration.  If  the  building  is  subjected 
to  troublesome  vibrations  some  sort  of  rubber  support  may  be 
interposed  between  the  galvanometer  mounting  and  the  wall 
bracket  or  suspension.  Three  tennis  balls  held  in  place  by  de- 
pressions in  a  block  of  wood  on  which  the  galvanometer  is  placed 
may  help.  In  some  instances  the  more  elaborate  Julius  sus- 
pension, such  as  those  advertised,  may  be  necessary.  It  is  cer- 
tainly a  great  help  and,  for  extensive  work,  quite  worth  the 
trouble  and  expense  of  installation. 

Complete  formulation  of  galvanometer  conduct  is  an  extremely 
complicated  problem,  including  as  it  does  the  properties  of 
materials.  We  shall  pass  a  discussion  of  this  and  come  at  once  to 
the  end  result, — the  description  of  a  galvanometer  in  terms  of  its 
sensitivity,  as  determined  experimentally. 


334 


THE    DETERMINATION    OF   HYDROGEN   IONS 


GALVANOMETER    SENSITIVITY 

Galvanometer  sensitivities  are  expressed  in  various  ways. 
Since  one's  attention  is  centered  upon  detecting  potential  dif- 
ferences the  temptation  is  to  ask  for  the  galvanometer  sensitivity 
in  terms  of  microvolt  sensitivity.  There  are  two  ways  of  ex- 
pressing this  which  lead  to  different  values.  One  is  the  deflection 
caused  by  a  microvolt  acting  at  the  terminals  of  the  galvanometer. 


FIG.  61.  A  GALVANOMETER 
(Courtesy  of  Leeds  and  Northrup  Company) 

The  more  useful  value  is  the  deflection  caused  by  a  microvolt 
acting  through  the  external  critical  damping  resistance.  But  in 
the  last  analysis  the  instrument  is  to  be  used  for  the  detection 
of  very  small  currents  and  these  currents  when  allowed  to  flow 
through  the  galvanometer  by  the  unbalancing  of  the  circuit  at 
a  slight  potential  difference  are  determined  by  the  total  resistance 
of  the  circuit.  The  instrument  might  be  such  that  a  microvolt 
at  the  terminals  would  cause  a  wide  deflection,  while,  if  forced 


XVI  DAMPING  335 

to  act  through  a  large  external  resistance,  this  microvolt  would 
leave  the  galvanometer  "dead."  For  this  reason  it  is  best  to 
know  the  sensitivity  in  terms  of  the  resistance  through  which  a 
unit  voltage  will  cause  a  given  deflection.  This  is  the  megohm 
sensitivity  and  is  defined  as  "the  number  of  megohms  (million 
ohms)  of  resistance  which  must  be  placed  in  the  galvanometer 
circuit  in  order  that  from  an  impressed  E.M.F.  of  one  volt  there 
shall  result  a  deflection  of  one  millimeter"  upon  a  scale  one  meter 
from  the  reflecting  mirror  (Leeds  and  Northrup  catalogue  20, 
1918).  The  numerical  value  of  this  megohm  sensitivity  also 
represents  the  microampere  sensitivity  if  this  is  defined  as  the 
number  of  millimeters  deflection  caused  by  one  microampere. 

In  hydrogen  electrode  measurements  the  resistance  of  the  cells 
varies  greatly  with  design  (length  and  width  of  liquid  conductors) 
and  with  the  composition  of  the  solutions  used  (e.g.  saturated  or 
M/10  KC1).  Constricted,  long  tubes  may  raise  the  resistance  of 
a  chain  so  high  as  to  annul  the  sensitivity  of  a  galvanometer  unless 
this  has  a  high  megohm  sensitivity. 

In  the  practical  attainment  of  a  given  sensitivity  we  enter 
complexities,  since  the  arrangements  by  which  high  megohm 
sensitivity  is  attained  affect  other  galvanometer  characteristics. 
One  of  these,  which  is  not  essential  but  is  desirable,  is  a  short 
period.  A  short  period  facilitates  the  setting  of  a  potentiometer. 
If  the  circuits  are  out  of  balance,  as  they  generally  are  at  the 
beginning  of  a  measurement,  the  direction  for  readjustment  may 
be  inferred  from  the  direction  of  galvanometer  deflection  without 
bringing  the  coil  back  each  time  to  zero  setting,  but  there  comes 
a  time  when  prompt  return  to  zero  setting  is  essential  to  make 
sure  that  slight  resettings  of  the  potentiometer  are  being  made 
in  the  proper  direction. 

DAMPING 

For  a  return  of  the  coil  to  zero  without  oscillation  it  is  neces- 
sary to  have  some  sort  of  damping.  This  is  generally  a  shunt 
across  the  galvanometer  terminals,  the  so-called  critical  damping 
resistance.  This  shunt  permits  a  flow  of  current  (when  the  main 
galvanometer  circuit  is  opened)  which  is  generated  by  the  turning 
of  the  coil  in  the  magnetic  field.  The  magnetic  field  produced  in 
the  coil  by  this  current  interacting  with  the  field  of  the  perma- 


336  THE    DETERMINATION    OF   HYDROGEN    IONS 

nent  magnet  tends  to  oppose  the  further  swing  of  the  coil.  When 
the  resistance  of  the  shunt  is  so  adjusted  to  the  galvanometer 
characteristics  that  the  swing  progresses  without  undue  delay  to 
zero  setting  and  there  stops  without  oscillation,  the  galvanometer 
is  said  to  be  critically  damped.  Critical  damping  as  applied  to 
deflection  on  a  closed  circuit  need  not  be  considered  when  the 
galvanometer  is  used  as  a  null-point  instrument.  Since  some  of 
the  best  galvanometers  are  not  supplied  with  a  damping  resist- 
ance the  purchaser  of  an  outfit  for  hydrogen  electrode  work  should 
take  care  to  see  that  he  includes  the  proper  unit.  Underdamped 
and  overdamped  instruments  will  prove  very  troublesome  or 
useless. 

If  there  is  no  damping,  the  coil  will  oscillate  like  a  free,  torsion 
pendulum.  If  infinitely  damped,  the  coil  would  never  return  to 
zero  setting.  If  underdamped,  the  coil  will  oscillate  but  will 
come  to  rest  rapidly.  If  overdamped,  the  coil  will  not  oscillate 
but  will  come  to  rest  too  slowly. 

These  very  brief  considerations  are  presented  merely  as  an  aid 
in  the  selection  of  instruments.  The  manner  in  which  desirable 
qualities  are  combined  is  a  matter  of  considerable  complexity  but 
fortunately  makers  are  coming  to  appreciate  the  very  simple  but 
important  requirements  for  hydrogen  electrode  work  and  are 
prepared  to  furnish  them.  A  galvanometer  used  by  the  author 
had  the  following  characteristics;  coil  resistance  530  ohms,  critical 
damping  resistance  9,000  ohms,  period  6  seconds,  sensitivity  2245 
megohms.  It  was  not  the  ideal  instrument  for  the  hydrogen 
electrode  system  in  use  but  was  very  satisfactory.  A  shorter 
period  is  desirable  and  a  higher  coil  resistance  to  correspond 
better  with  the  average  resistance  of  the  order  of  one  to  two 
thousand  ohms  in  some  gas  chains,  would  be  desirable;  but  im- 
provement in  both  of  these  directions  at  the  same  time  may  in- 
crease the  expense  of  the  instrument  beyond  the  practical  worth. 
Indeed  certain  instruments  now  on  the  market  are  satisfactory 
for  almost  any  type  of  hydrogen  electrode  measurements. 

In  using  a  galvanometer  it  is  important  to  remember  that  while 
the  E.M.F.  of  a  cell  is  unbalanced  its  circuit  should  be  left  closed 
only  long  enough  to  show  the  direction  of  the  galvanometer  deflec- 
tion. Otherwise  current  will  flow  in  one  direction  or  the  other 
through  the  chain  and  tend  to  upset  the  electrode  equilibrium. 


XVI 


CAPILLARY   ELECTROMETER 


337 


A  mere  tap  on  the  key  which  closes  the  galvanometer  circuit  is 
sufficient  till  balance  is  obtained. 


CAPILLARY   ELECTROMETER 

The  capillary  electrometer  depends  for  its  action  upon  the  altera- 
tion of  surface  tension  between  mercury  and  sulfuric  acid  with 
alteration  of  the  potential  difference  at  the  interface.  A  simple 
form  suitable  for  that  degree  of  precision  which  does  not  call  for 
the  advantages  of  a  galvanometer  is  illustrated  in  figure  62. 

Platinum  contacts  are  sealed  into  two  test  tubes  and  the  tubes 
are  joined  as  illustrated  by  means  of  a  capillary  K  of  about  0.5  mm. 


FIG.  62.  DIAGRAM  OF  CAPILLARY  ELECTROMETER  AND  KEY 

diameter.  In  making  the  seals  between  capillary  and, tubes  the 
capillary  is  first  blown  out  at  each  end  and  can  then  be  treated  as 
a  tube  of  ordinary  dimensions  in  making  a  T  joint.  After  a  thor- 
ough cleaning  the  instrument  is  filled  as  illustrated  with  clean, 
distilled  mercury,  sufficient  mercury  being  poured  into  the  left 
tube  to  bring  the  meniscus  in  the  capillary  near  a  convenient 
point.  In  the  other  tube  is  now  placed  a  solution  of  sulfuric  acid 
made  by  adding  5.8  cc.  water  to  10  cc.  sulfuric  acid  of  1.84  specific 
gravity.  The  air  is  forced  out  of  the  capillary  with  mercury 
until  a  sharp  contact  between  mercury  and  acid  occurs  in  the 
capillary.  The  instrument  is  now  mounted  before  a  microscope 


338  THE    DETERMINATION    OF   HYDROGEN   IONS 

using  as  high  power  lenses  as  the  radius  of  the  glass  capillary  will 
permit.  The  definition  of  the  mercury  meniscus  is  brought  out 
by  cementing  to  the  capillary  with  Canada  balsam  a  cover  glass 
as  illustrated. 

Mislowitzer  (1928)  projects  the  image  of  the  mercury  meniscus 
upon  a  screen  and  thereby  obtains  high  magnification. 

Among  the  numerous  other  forms  of  capillary  electrometer 
there  might  be  mentioned  that  of  Miiller  (1926).  He  uses  the 
double  capillary  effect,  that  is  the  rise  at  the  one  end  and  the 
fall  at  the  other  end  of  a  thread  of  mercury.  He  claims  that  the 
double  effect  can  be  satisfactorily  followed  with  a  reading  glass. 

Bennett  (1925)  uses,  in  his  two-capillary  instrument,  tubes  of 
0.012  mm.  diameter.  He  finds  that  smaller  tubes  are  apt  to 
exhibit  a  "sticking  effect"  while  of  course  larger  tubes  decrease 
the  sensitivity.  The  1925  edition  of  "Ostwald-Luther"  states 
that  tubes  at  least  0.3  mm.  wide  should  be  employed. 

Menzel  and  Kriiger  (1926)  use  a  tube  0.8  mm.  diameter.  They 
use  2N  H2S04  (not  the  concentration  of  highest  conductivity) 
and  recommend  capillaries  of  uniform  round  bore. 

An  important  feature  in  the  use  of  the  capillary  electrometer 
is  its  short  circuiting  between  measurements.  This  is  done  by  the 
key  shown  in  figure  62.  Tapping  down  on  the  key  breaks  the 
short-circuit  and  brings  the  terminals  of  the  electrometer  into 
the  circuit  to  be  balanced.  If  the  E.M.F.  is  out  of  balance  the 
potential  difference  at  the  mercury-acid  interface  causes  the 
mercury  to  rise  or  fall  in  the  capillary.  Releasing  the  key  short- 
circuits  the  terminals  and  allows  the  mercury  to  return  to  its 
normal  position.  Adjustment  of  the  potentiometer  is  continued 
till  no  movement  of  the  mercury  can  be  detected.  To  establish 
a  point  of  reference  from  which  to  judge  the  movement  of  the 
mercury  meniscus  the  microscope  should  contain  the  familiar 
micrometer  disk  at  the  diaphragm  of  the  eye  piece.  In  lieu  of 
this  an  extremely  fine  drawn  thread  of  glass  or  a  spider  web  may 
be  held  at  the  diaphragm  of  the  eye  piece  by  touches  of  Canada 
balsam. 

THE    QUADRANT    ELECTROMETER 

The  quadrant  electrometer  has  not  been  very  frequently  used 
as  a  null-point  instrument  in  potentiometric  measurements  but 


XVI  QUADRANT    ELECTROMETER  339 

it  will  come  into  more  frequent  use  with  the  development  of  the 
"glass  electrode"  and  the  study  of  non-aqueous  solutions  of  low 
conductivity  (see  Hall  and  Conant,  1928).  Bovie  uses  it  in 
general. 

In  a  form  useful  for  the  purpose  at  hand  a  very  light  vane  of 
aluminium  is  suspended  by  an  extremely  fine  thread,  preferably 
of  quartz,  which  is  metallized  on  the  surface  in  order  to  conduct 
charges  to  the  vane.  The  vane  or  "needle"  is  surrounded  by  a 
flat,  cylindrical  metal  box  cut  into  quadrants  each  highly  insulated. 
Two  opposite  quadrants  are  connected  to  one  terminal  and  the 
remaining  quadrants  to  another  terminal.  If  now  the  vane  or 
needle  be  charged  from  one  terminal  of  a  high-voltage  battery 
the  other  terminal  of  which  is  grounded,  and  a  difference  of  po- 
tential be  established  between  the  two  sets  of  quadrants,  the 
needle  will  be  deflected  by  the  electrostatic  forces  imposed  and 
induced. 

Since  the  current  drawn  for  its  operation  is  only  the  amount 
necessary  to  charge  a  system  of  very  low  capacity  to  the  low 
potential  difference  when  the  potentiometer  is  slightly  out  of 
balance  with  the  measured  E.M.F.  (and  to  zero  potential 
difference  at  balance)  the  quadrant  electrometer  might  be  of 
special  value  in  the  study  of  easily  displaced,  electrode  equilibria. 
However,  the  attainment  of  the  desired  sensitivity  with  some  of 
these  instruments  is  a  task  requiring  skill  and  patience.  Further- 
more the  rated  sensitivity  is  sometimes  attained  by  adjusting  the 
so-called  electrostatic  control  to  such  a  value  that  the  zero  posi- 
tion of  the  needle  is  rendered  highly  unstable.  This,  combined 
with  the  very  long  period  at  high  sensitivity,  renders  the  instru- 
ment unsatisfactory  for  common  use.  Against  these  objections 
are:  first,  the  point  mentioned  above,  and  second  the  advantage 
that  the  instrument  may  ordinarily  be  left  in  circuit  during  the 
adjustment  of  the  potentiometer  as  is  not  the  case  with  the  gal- 
vanometer. 

For  discussions  of  "electrostatic  control"  see  for  instance 
Beattie  (1910-1912)  and  Compton  and  Compton  (1919). 

The  quadrant  electrometer  is  especially  useful  in  the  study  of 
"glass  electrodes"  (see  page  432).  In  the  circuit  of  the  glass 
electrode  the  resistance  may  be  of  the  order  of  "over  fifty 
megohms."  Therefore  the  ordinary  current-indicating  instru- 


340  THE    DETEEMINATION    OF   HYDROGEN   IONS 

ments,  such  as  the  galvanometer,  suffer  great  impairments  of 
sensitivity.     A  static  instrument  must  replace  them. 

A  wiring  diagram  for  a  quadrant  electrometer  is  shown  in  figure 
63.  HI  is  a  resistance  of  about  2  megohms,  interposed  merely 
to  prevent  high  discharge  currents  on  accidental  short-circuit  of 
the  high  potential  battery  B.  The  double-throw  switch  Si  pro- 
vides for  grounding  the  electrometer  needle  during  adjustments. 
By  means  of  switch  82  the  quadrants  may  be  grounded  during 
adjustments,  or  the  one  pair  of  quadrants  may  be  connected  to 
one  pole  of  the  cell  X  which  is  under  measurement.  The  other 
pole  of  X  is  connected  to  the  other  pair  of  quadrants  and  the 
potentiometer  grounded  at  O.  Kerridge  (1926)  prefers  to  lead 
the  connections  from  each  pair  of  quadrants  to  a  switch  that 
permits  the  position  of  the  quadrant  pairs  in  the  wiring  to  be 


FIG.  63.  WIRING  DIAGRAM  OF  POTENTIOMETER  SYSTEM  IN  WHICH  A  QUAD- 
RANT ELECTROMETER  Is  USED  AS  NULL-POINT  INSTRUMENT 

reversed.  The  potentiometer  circuit  is  shown  in  elementary 
outline  with  the  potentiometer  battery  A,  regulating  rheostat  R2 
and  grounding,  G,  at  the  zero  end,  0.  For  a  discussion  of  shield- 
ing and  insulation  see  Chapter  XVII,  and  Brown  (1924). 

Kerridge  (1926)  also  describes  the  use  of  the  "Lindemann 
electrometer."  See  Lindemann  and  Keeley  (1924). 

TELEPHONE   RECEIVER 

The  modern  high  resistance  telephone  receiver  of  the  type  used 
in  radio  reception  may  serve  in  an  emergency  [Kiplinger  (1921)]. 
Lack  of  balance  between  potentiometer  adjustment  and  measured 
E.M.F.  is  indicated  by  a  click  in  the  receiver  when  the  poten- 
tiometer key  is  tapped;  but  there  is  of  course  nothing  but  the 
loudness  of  the  click  to  show  how  far  from  balance  the  adjustment 


XVI 


RECORDING   POTENTIOMETER 


341 


is,  and  only  the  decrement  of  the  sound  to  indicate  that  adjust- 
ment in  the  proper  direction  is  being  made. 


PORTABLE    SETS 


There  are  those  who  prefer  potentiometer,  null-point  instrument 
and  electrode  vessel  mounted  together.  In  consequence  there  are 
on  the  market  a  wide  variety  of  so-called  portable  sets.  Several 
of  these  are  described  in  the  literature.  The  author  prefers  to 
give  each  part  of  a  set  its  appropriate  mounting  according  to  the 
needs  of  the  ^investigation. 


FIG.  64.  LEEDS  AND  NOKTHRUP  RECORDING  POTENTIOMETER 
(Courtesy  of  Leeds  and  Northrup  Company) 


RECORDING   POTENTIOMETERS 

For  recording  potential  changes  within  the  range  of  the  extended 
wire  of  the  Leeds  and  Northrup  potentiometer,  Gesell  and  Hertz- 
mann  (1926)  attach  a  spindle  to  the  drum,  wind  a  thread  about 
this  and  run  the  end  of  this  thread  to  the  writing  point  of  a 
kymograph. 

An  automatic  recording  potentiometer  is  manufactured  by  the 
Leeds  and  Northrup  Co.  The  shaft  which  rotates  the  poten- 
tiometer wire  also  holds  an  adjustable  disk  with  knobs  for  con- 
tact with  a  relay  circuit.  At  a  determined  potential  a  relay  can 


342 


THE  DETERMINATION  OF  HYDROGEN  IONS 


be  actuated   and  through  this   control  various  mechanical  ap- 
paratus can  be  operated. 

Numerous  photographic  devices  are  available  for  recording 
galvanometer  deflections.  Buytendyk,  Brinkman  and  Mook 
(1927)  used  photographic  records  with  the  electron  valve  system. 

THE    WESTON    STANDARD    CELL 

Among  several  cells  which  give  fairly  constant,  determined 
electromotive  forces,  the  Weston  cell  is  the  one  most  frequently 
used.  Indeed  it  has  become  an  international  standard  for  the 
practical  maintenance  of  the  value  of  the  international  volt. 

The  elementary  construction  of  the  Weston  cell  is  illustrated 
in  figure  65.  Pure  mercury  forms  one  electrode  and  a  cadmium 


Hg-Cd 


FIG.  65.  DIAGRAM  OF  THE  WESTON  STANDARD  CELL 

amalgam  the  other.  The  mercury  electrode  is  overlaid  with 
mercurous  sulfate.  The  electrolyte  solution  is  a  solution  of  cad- 
mium sulf  ate.  Two  chief  forrns  of  the  cell  are  in  use.  In  one  the 
cadmium  sulfate  solution  is  maintained  at  the  saturation  point 
by  the  presence  of  solid  cadmium  sulfate  not  shown  in  the  diagram 
but  present  on  each  side.  In  the  other  cell,  referred  to  as  the 
"unsaturated"  cell,  in  contradistinction  to  the  "saturated"  cell, 
the  concentration  of  cadmium  sulfate  in  solution  is  that  of  a 
solution  saturated  at  4°C.  This  results  in  a  solution  which  is 
unsaturated  at  ordinary  temperature. 

It  is  the  saturated  cell,  sometimes  called  the  normal  cell,  that 
is  used  to  maintain  the  value  of  the  volt,  since  it  is  regarded  as 
the  more  reproducible  and  constant.  On  the  other  hand  the  un- 
saturated cell  is  often  preferred  for  routine  use  because  it  is  easily 


XVI  WESTON   CELLS  343 

made  portable  and  because  it  has  a  temperature  coefficient  so 
small  as  to  be  negligible  for  many  purposes. 

Electrode  potential  measurements,  made  by  the  ordinary 
potentiometric  method,  are  referred  to  the  electromotive  force 
of  a  particular  West  on  cell  or  set  of  West  on  cells.  Reliability  in 
this  basic  device  is  therefore  fundamental.  Since  preparation  of 
reliable  cells  has  been  made  a  subject  of  conscientious  scientific 
study  by  certain  of  the  commercial  firms  which  make  these  cells, 
and  since  the  cells  are  now  available  in  rugged  form,  it  is  hardly 
worth  the  while  of  an  investigator,  who  is  not  interested  in  the 
cell  itself,  to  undertake  the  preparation.  However  a  brief  de- 
scription of  the  preparation  may  be  instructive. 

The  mercury  in  the  left  arm  should  be  carefully  purified  (page 
364)  and  the  same  material  should  be  used  for  the  preparation 
of  the  cadmium  amalgam.  This  amalgam  consists  of  12.53  per 
cent  by  weight  of  electrolytic  cadmium.  The  amalgam  is  formed 
by  heating  mercury  over  a  steam  bath  and  stirring  in  the  cad- 
mium. Any  oxid  formed  may  be  strained  off  by  pouring  the 
molten  amalgam  through  a  test  tube  drawn  out  to  a  long  capillary. 
An  electrolytic  method  of  preparing  the  amalgam  is  described 
by  Hulett  (1911).  Such  a  method  is  now  used  by  the  Bureau  of 
Standards. 

Cadmium  sulfate  may  be  recrystallized  as  described  by  Wolff 
and  Waters  (1907).  Dissolve  in  excess  of  water  at  70°C.,  filter, 
add  excess  of  basic  cadmium  sulfate  and  a  few  cubic  centimeters 
of  hydrogen  peroxid  to  oxidize  ferrous  iron,  and  heat  several 
hours.  Then  filter,  acidify  slightly  and  evaporate  to  a  small 
volume.  Filter  while  hot  and  wash  the  crystals  with  cold  water. 
Recrystallize  slowly  from  an  initially  unsaturated  solution.  The 
cadmium  sulfate  solution  of  a  "normal"  West  on  cell  is  a  solution 
saturated  at  whatever  temperature  the  cell  is  used,  and  therefore 
the  cell  should  contain  crystals  of  the  sulfate.  The  ordinary 
unsaturated  cell  has  a  cadmium  sulfate  solution  that  is  saturated 
at  4°C.  \ 

In  the  study  of  Weston  cells  considerable  attention  has  been 
paid  to  the  quality  of  the  mercurous  sulfate.  Perhaps  the  best 
and  at  the  same  time  the  most  conveniently  prepared  material  is 

3  A  10  per  cent  amalgam  is  commonly  used  in  England  because  it  is  better 
adapted  to  low  temperature  conditions. 


344         THE  DETERMINATION  OF  HYDROGEN  IONS 

that  made  electrolytically.  Where  the  alternating  current  is 
available  it  is  preferable  to  use  it.  A  good  average  set  of  condi- 
tions is  a  sixty  cycle  alternating  current  sent  through  a  25  per 
cent  sulfuric  acid  solution  with  a  current  density  at  the  electrodes 
of  5  to  10  amperes  per  square  decimeter.  With  either  the  alter- 
nating or  direct  current  the  apparatus  described  by  fig.  52  is 
convenient. 

In  the  Weston  cell  the  lead-in  wires  of  platinum  should  be 
amalgamated  electrolytically  by  making  a  wire  the  cathode  in  a 
solution  of  pure  mercurous  nitrate  in  dilute  nitric  acid. 

After  filling  the  cell  it  may  be  sealed  off  in  the  blast  flame  or 
corked  and  sealed  with  wax. 

In  some  portable  Weston  cells  of  commerce  the  mercury  is 
introduced  as  amalgamated  electrodes.  For  a  description  of 
commercial  cells  see  Vosburgh  and  Eppley  (1924). 

The  unsaturated  cell  is  often  described  as  having  no  tem- 
perature coefficient.  This  is  not  strictly  true.  Vosburgh  and 
Eppley  (1923)  find  that  the  temperature  coefficient  varies  with 
the  electromotive  force,  being  a  linear  function  thereof.  For 
cells  with  an  E.M.F.  of  1.01827  it  was  0.000,0028  volt  per 
degree.  This  temperature  coefficient  declined  to  —0.000,013  per 
degree  for  cells  with  an  E.M.F.  of  1.0210.  Of  more  practical 
importance  than  the  temperature  coefficient  for  the  whole  cell 
is  the  fact  that  it  is  comparatively  small  because  of  the  approxi- 
mate balancing  of  much  larger  temperature  coefficients  for  the 
two  half-cells.  Hence  unequal  heating  of  the  two  limbs  may 
have  a  serious  effect.  In  addition  there  may  be  some  hysteresis 
during  temperature  changes.  See,  for  instance,  Vosburgh  and 
Eppley  (1924).  The  hysteresis  effect  is  more  likely  to  produce 
abnormal  electromotive  forces  when  the  temperature  is  suddenly 
lowered  than  when  the  temperature  is  suddenly  raised.  Because 
of  the  abnormalities  produced  by  temperature  changes  it  is  ad- 
visable to  protect  unsaturated  cells  against  these  changes  of 
temperature  by  some  sort  of  thermal  insulation. 

As  the  result  of  cooperative  measurements  by  the  national 
standards  laboratories  of  England,  France,  Germany  and  the 
United  States,  and  upon  agreement  as  to  convention,  the  normal 
Weston  cell  was  defined  as  having  the  value  1.01830  inter- 
national volts  at  20 °C.  Since  the  value  of  the  international  volt 


XVI  WESTON   CELLS  345 

(see  page  247)  is  practically  maintained  by  use  of  groups  of 
Weston  cells  maintained  at  each  national  standards  laboratory, 
the  above  definition  amounts  to  a  secondary  definition  of  the 
international  volt. 

It  is  important  to  note  that  the  international  agreement  came 
into  force  January  1,  1911  and  that  prior  to  that  time  the  values 
in  force  in  different  countries  varied  to  an  extent  that  makes 
necessary  various  corrections  in  the  comparison  of  the  older 
potential  measurements. 

TABLE  53a 

Increments  in  the  electromotive  force  of  saturated  Weston  cells  when  the  tem- 
perature has  been  changed  and  made  constant  at  temperatures  other 
than  the  standard  of  reference,  i.e.,  20° C . 


TEMPERATURE 

INCREMENT 

°<7. 

volts 

5 

+  0.000,362 

10 

-fO.  000,301 

15 

+0.000,179 

20 

0.000,000 

25 

-0.000,226 

30 

-0.000,491 

35 

-0.000,789 

40 

-0.001,112 

The  temperature  coefficient  of  the  normal  Weston  cell  was 
given  by  Wolff  (1908).  The  formula  which  has  received  inter- 
national adoption  is  based  on"WohTs  formula  but  has  been  changed 
slightly  to  :4 

Et  =  E20  -  0.000,040,6  (t  -  20)  -  0.000,000,95  (t  -  20)2 
+  0.000,000,01  (t  -  20)3 

By  this  formula  the  differences  in  volts  from  the  value  at  20 °C. 
are  those  found  in  table  53a. 

Again  it  may  be  emphasized  that  this  formula  applies  to  the 
saturated  Weston  cell  and  that  ordinarily  the  comparatively 
slight  temperature  coefficient  of  the  unsaturated  cell  is  neglected. 

For  example,  a  Weston  cell  (saturated  type)  is  certified  as 

4  Personal  communication  from  Dr.  G.  W.  Vinal,  U.  S.  Bureau  of  Stand- 
ards. 


346         THE  DETERMINATION  OF  HYDROGEN  IONS 

having  a  value  of  1.01832  volt  at  25 °C.  Assuming  that  this 
particular  cell  behaves  normally  its  value  at  20°  should  be  1.01855. 

While  the  commercial  cells  used  in  the  United  States  are 
usually  of  the  unsaturated  type,  those  employed  in  England  are 
said  to  be  usually  of  the  saturated  type.  Since  the  question  of 
temperature  control  has  to  be  given  serious  consideration  in  the 
use  of  the  saturated  type  and  may  ordinarily  be  neglected  (except 
protection  from  sudden  changes)  in  the  use  of  the  unsaturated  cell, 
the  purchaser  should  always  be  informed  of  the  type. 

In  certifying  cells  of  the  unsaturated  type  the  Bureau  of 
Standards  advises  the  following  precautions. 

"Precautions  in  using  standard  cells;  (1)  The  cell  should  not  be 
exposed  to  temperatures  below  4°C.  nor  above  40°C.,  (2)  abrupt 
changes  in  temperature  should  be  avoided,  (3)  all  parts  of  the 
cell  should  be  at  the  same  temperature,  (4)  current  in  excess  of 
0.0001  ampere  should  never  pass  through  the  cell,  (5)  the  elec- 
tromotive force  of  the  cell  should  be  redetermined  at  intervals  of 
a  year  or  two." 

STORAGE   BATTERIES 

The  storage  battery  or  accumulator  is  a  convenient  and  reli- 
able source  of  current  for  the  potentiometer.  Standard  poten- 
tiometers are  generally  designed  for  use  with  a  single  cell  which 
gives  an  E.M.F.  of  about  two  volts. 

The  more  familiar  cell  consists  of  two  groups  of  lead  plates  im- 
mersed in  a  sulfuric  acid  solution. of  definite  specific  gravity. 
The  plates  of  one  group  are  connected  to  one  pole  of  the  cell  and 
the  plates  of  the  other  group  are  connected  to  the  other  pole. 
When  a  current  is  passed  through  the  cell  it  will  produce  lead 
peroxide  upon  the  plates  by  which  the  positive  current  enters 
and  spongy  lead  upon  the  other  plates.  Therefore,  on  charging, 
the  plates  in  connection  with  the  positive  pole  assume  the  brown 
color  of  the  oxide  while  the  plates  in  connection  with  the  negative 
pole  assume  the  slate  color  of  the  spongy  metal.  The  poles  should 
be  distinctly  marked  so  that  one  need  not  inspect  the  plates  to 
distinguish  the  polarity;  but,  should  the  marks  become  obscured 
and  the  cell  be  a  closed  cell,  the  polarity  should  be  carefully 
tested  with  a  voltmeter  before  attaching  the  charging  current. 
In  lieu  of  a  voltmeter  the  polarity  may  be  tested  with  a  paper 


XVI  STORAGE    BATTERIES  347 

moistened  with  KI  solution.  On  applying  the  terminals  to  the 
paper  a  brown  stain  is  produced  at  the  positive  pole.  "Positive 
reaction  at  positive  pole." 

In  charging  a  cell  the  positive  pole  of  the  charging  circuit  should 
be  connected  to  the  positive  terminal  of  the  cell,  else  the  cell  will 
be  ruined.  If  a  direct  current  lighting  circuit  is  available,  it  may 
be  used  to  charge  a  cell,  or  battery  of  cells,  provided  sufficient 
resistance  be  placed  in  series. 

Resistances  are  conveniently  formed  from  filament  lamps 
arranged  in  parallel  so  that  when  the  bank  of  lamps  is  placed  in 
series  with  the  battery  and  the  charging  source  the  introduction 
of  more  or  fewer  lamps  will  allow  more  or  less  current  to  flow. 
Much  energy  is  wasted  in  the  resistance  which  it  is  necessary  to 
employ  when  a  cell  or  small  battery  of  cells  is  charged  with  a  high 
potential  line,  and  therefore  it  is  more  economical  to  employ  low 
voltage  circuits.  However  these  are  seldom  available. 

When  only  an  alternating  current  is  available  it  is  necessary  to 
use  some  means  of  changing  this  to  a  direct  current.  The  motor- 
generator  may  be  used;  but,  with  the  development  of  amateur 
radio  and  the  widespread  demand  for  simple  means  of  charging 
"A"  batteries,  several  inexpensive  rectifiers  have  become  available. 
These  are  chiefly  of  two  types.  In  the  one  rectification  is  accom- 
plished with  the  aid  of  the  electron- valve  principle  (see  page  329). 
In  the  other,  use  is  made  of  the  property  of  the  interface  between 
certain  metals  and  an  electrolyte  solution  whereby  current  will 
pass  chiefly  in  one  direction.  These  rectifiers  are  designed  for 
two  purposes.  Those  of  larger  capacity  are  designed  for  the 
charging  of  batteries  from  the  condition  of  discharge  to  full 
capacity.  Others,  of  smaller  capacity,  are  designed  for  that 
slight  recharging  at  frequent  intervals  which  is  sufficient  to 
maintain  the  battery  near  complete  capacity.  The  latter  type 
are  often  referred  to  as  "trickle"  chargers. 

The  electrolyte  of  the  lead  cell  is  pure  sulfuric  acid  solution, 
the  density  of  which  varies  with  the  type  and  purpose  of  the  cell. 
The  specific  gravity  of  the  fully  charged  cell  may  vary  from  1.210 
for  stationary  batteries  to  1.300  for  aviation  batteries.  On  dis- 
charge the  sulfuric  acid  combines  with  the  active  material  of  the 
plates  and  is  deposited  with  a  resulting  lowering  of  the  specific 
gravity  of  the  electrolyte.  Thus  the  specific  gravity  of  the  elec- 


348  THE    DETERMINATION    OF   HYDROGEN    IONS 

trolyte  is  highest  when  the  battery  is  fully  charged  and  lowers 
during  discharge.  If  there  be  reason  to  suspect  that  the  density 
proper  for  the  type  of  battery  in  use  is  not  being  maintained,  it 
should  be  tested  with  a  hydrometer  and,  in  case  fresh  acid  is  to 
be  added,  only  the  purest  and  properly  diluted  acid  should  be 
added.  The  occasion  for  this  is  so  rare  that  ordinarily  only 
pure,  distilled  water  should  be  added  to  restore  loss  by  evapora- 
tion and  gassing.  Impurities  of  the  acid  or  water  may  have  very 
serious  effects  upon  the  conduct  and  capacity  of  a  cell.  None  of 
the  substances  suggested  to  improve  the  electrolyte  is  necessary 
and  few,  if  any,  have  merit. 

Among  sources  of  trouble  are  the  following.  Overcharging  may 
loosen  the  active  material  of  the  plates.  Habitual  undercharging 
may  cause  excessive  accumulation  of  lead  sulfate  which,  having 
a  larger  volume  than  the  original  material  of  the  plates,  causes 
mechanical  strain  and  buckling.  Corroded  terminals  may  be 
cleaned  with  a  cloth  moistened  with  ammonia  water.  The 
terminals  should  be  covered  with  vaseline.  Defective  plates  or 
separators,  while  sometimes  defects  of  manufacture,  may  be 
caused  by  a  variety  of  mistreatments  and  usually  can  be  repaired 
only  by  opening  the  cell.  If  they  cause  internal  short  circuits 
this  will  be  evident  by  low  open  circuit  voltage.  If  they  cause  the 
elimination  of  one  or  more  plates  from  use,  the  capacity  of  the 
cell  will  be  lowered.  Excess  sulphation  may  result  from  neglect. 
A  remedy  is  to  remove  the  electrolyte,  fill  the  cell  with  water, 
place  the  battery  on  charge  for  a  long  time  and  finally  adjust  the 
specific  gravity  of  the  electrolyte  to  the  proper  value. 

In  discharging  a  cell  its  voltage  should  not  be  allowed  to  fall 
below  1.8  volts.  When  or  before  the  cell  has  reached  this  value 
it  should  be  recharged. 

In  using  a  storage  cell  to  supply  potentiometer  current  it  is  es- 
sential that  the  highest  stability  in  the  current  should  be  attained 
since  the  fundamental  principle  of  the  potentiometer  involves  the 
maintenance  of  constant  current  between  the  moment  at  which 
the  Weston  cell  is  balanced  and  the  moment  at  which  the  measured 
E.M.F.  is  balanced.  Steadiness  of  current  is  attained  first  by 
having  a  storage  cell  of  sufficient  capacity,  and  second  by  using  it 
at  the  most  favorable  voltage.  Capacity  is  attained  by  the  num- 
ber and  size  of  the  plates.  A  cell  of  60  ampere-hour  capacity  is 


XVI  STOEAGE   BATTERIES  349 

sufficient  for  ordinary  work.  The  current  from  a  storage  cell  is 
steadiest  when  the  voltage  has  fallen  to  2  volts.  When  a  potenti- 
ometer system  of  sufficient  resistance  is  used  it  is  good  practice  to 
leave  the  cell  in  circuit,  replacing  it  or  recharging  it  of  course  when 
the  voltage  has  fallen  to  1.8  or  1.9  volts,  and  thus  insure  the 
attainment  of  a  steady  current  when  measurements  are  to  be 
made. 

In  no  case  should  a  cell  used  for  supplying  potentiometer  cur- 
rent be  wired  so  that  a  throw  of  a  switch  will  replace  the  dis- 
charging with  the  charging  circuit.  The  danger  of  leakage  from 
the  high  potential  'circuit  is  too  great  a  risk  for  the  slight  con- 
venience. 

Eppley  and  Gray  (1922)  replaced  the  storage  battery  by  a  large 
Weston  cell  in  a  special  potentiometer  circuit  but  they  state  that 
even  two  of  these  large  cells  would  not  operate  a  Leeds  and 
Northrup  type  K  potentiometer  satisfactorily. 

Some  of  the  newer  potentiometers  are  designed  to  operate 
with  dry-cells. 

The  alkaline  storage  cell,  sometimes  called  the  nickel-iron  cell 
and  known  in  America  as  the  Edison  cell  has  been  used  for 
potentiometer  circuits,  for  example  by  Gerke  and  Geddes  (1927). 

The  electrolyte  of  the  Edison  cell  is  usually  a  solution  of 
potassium  hydroxide  (plus  a  small  amount  of  LiOH).  The 
specific  gravity  does  not  vary  during  charge  and  discharge  as  it 
does  in  the  lead  cell.  Three  densities  of  electrolyte  are  employed. 
The  "first  fill"  electrolyte  has  a  specific  gravity  of  1.228.  Spil- 
lage is  replaced  with  electrolyte  of  specific  gravity  1.210.  After 
long  use  and  when  the  specific  gravity  has  fallen  to  1.160,  there 
is  used  a  "renewal  electrolyte"  of  specific  gravity  1.248. 

See  also: 

Storage  Batteries,  Vinal  (1925).  A  summary  of  characteristics  operation, 
etc.,  prepared  for  the  use  of  laboratory  technicians.  Contains  a  brief 
bibliography. 


CHAPTER  XVII 

HYDROGEN  GENERATORS,  WIRING,  INSULATION,  SHIELDING, 
TEMPERATURE  CONTROL,  PURIFICATION  OF  MERCURY 

Don't  descend  into  the  well  with  a  rotten  rope. — TURKISH  PROVERB. 
HYDROGEN   GENERATORS 

When  there  is  no  particular  reason  for  attaining  equilibrium 
rapidly  at  the  electrode  a  moderate  supply  of  hydrogen  will  do. 
When,  however,  speed  is  essential,  or  when  there  are  used  those 
immersion  electrodes  which  are  not  well  guarded  against  access 
of  atmospheric  oxygen  an  abundant  supply  of  hydrogen  is  essen- 
tial. Indeed  it  may  be  said  that  one  of  the  most  frequent  faults 
of  the  cruder  equipments  is  the  failure  to  provide  an  adequate 
supply  of  pure  hydrogen  or  the  failure  to  use  generously  the 
available  supply. 

Hydrogen  generated  from  zinc  and  sulfuric  acid  has  been  used 
in  a  number  of  investigations.  If  this  method  be  employed, 
particular  care  should  be  taken  to  eliminate  from  the  generator 
those  dead  spaces  which  are  frequently  made  the  more  obvious 
evidence  of  bad  design,  to  have  an  abundant  capacity  with  which 
to  sweep  out  the  gas  spaces  of  cumbersome  absorption  vessels 
and  to  properly  purify  the  hydrogen.  To  purify  hydrogen  made 
from  zinc  and  sulphuric  acid  pass  it  in  succession  through  KOH 
solution,  HgCl2  solution,  P2O5,  and  platinized  asbestos  at  about 
500°C.  (See  Franzen,  Ber.,  39,  906)  (Heinrich,  Ber.,  48,  1915, 
p.  2006). 

A  very  convenient  supply  of  hydrogen  is  the  commercial,  com- 
pressed gas  in  tanks.  According  to  Moser  (1920)  the  industrial 
preparation  varies  but  the  chief  methods  are  the  electrolytic  and 
the  Linde-Caro-Franck  processes.  Of  these  the  first  yields  the 
better  product.  Hydrogen  by  the  second  process  contains,  among 
other  impurities,  iron  carbonyl  which  may  be  detected  by  the 
yellow  flame  and  the  deposit  of  iron  oxid  formed  when  the  hydro- 
gen flame  impinges  upon  cold  porcelain.  Moser  found  that  it 

350 


XVII 


HYDROGEN  GENERATORS 


351 


was  impractical  to  remove  this  iron  carbonyl  and  he  states  that 
hydrogen  containing  it  is  unfit  for  laboratory  purposes.  On  the 
other  hand,  electrolytic  hydrogen  ordinarily  contains  only  traces 


H 


FIG.  66.  AN  ELECTROLYTIC  HYDROGEN  GENERATOR 

of  air  and  C02  and  is  free  from  arsenic  and  CO.  To  purify  it  pass 
the  gas  over  KOH  and  then  through  a  tube  of  hot,  platinized 
asbestos.  If  it  is  desired  to  dry  the  hydrogen,  use  soda  lime  or 


352  THE   DETERMINATION   OF   HYDROGEN   IONS 

P2O5,  but  not  H2S04.  If  P2O5  is  used  it  should  be  free  from  P203, 
i.e.,  distilled  in  a  current  of  hot  dry  air. 

In  purchasing  tank  hydrogen  it  is  well  to  be  on  guard  against 
tanks  which  have  been  used  for  other  gases. 

For  controlling  the  flow  of  gas  from  a  high  pressure  tank  the 
valve  on  the  tank  itself  is  seldom  sufficiently  delicate.  There 
should  be  coupled  to  it  a  delicate  needle  valve.  If  this  cannot 
be  obtained  use  a  diaphragm  valve  for  the  reduction  of  the  pres- 
sure. Even  then  there  should  be  placed  between  the  tank  and 
the  electrode  vessel  a  T  tube,  one  branch  of  which  dips  under 
mercury  and  forms  a  safety  valve. 

On  the  whole  electrolytic  generators  are  satisfactory  if  a  direct 
current  is  available.  In  figure  66  is  shown  a  generator  the  body  of 
which  is  an  ordinary  museum  jar.  The  glass  cover  may  be 
perforated  by  drilling  with  a  brass  tube  fed  with  a  mixture  of 
carborundum  and  glycerine.  If  this  mixture  is  kept  in  place  by 
a  ring  paraffined  in  position,  and  the  brass  tube  is  turned  on  a 
drill  press  with  intermittent  contact  of  the  drill  with  the  glass, 
the  perforation  may  be  made  within  a  few  minutes.  The  elec- 
trolyte used  is  10  per  cent  sodium  hydroxid.  The  electrodes  are 
nickel.  To  remove  the  spatter  of  electrolyte  and  to  protect  the 
material  in  the  heater,  the  hydrogen  passes  over  a  layer  of  con- 
centrated KOH  solution,  H;  and  to  remove  traces  of  residual 
oxygen  the  hydrogen  is  passed  through  a  heater.  In  the  design 
shown  the  gas  passes  through  a  tungsten  filament  lamp.  Lewis, 
Brighton  and  Sebastian  use  a  heated  platinum  wire.  More  com- 
monly there  is  used  a  gas-heated  or  electrically  heated  tube 
containing  platinized  asbestos.1 

In  the  author's  design  shown  in  figure  66  the  wiring  is  so  ar- 
ranged that,  when  there  is  no  demand  for  hydrogen,  the  heater 
may  be  turned  off  at  S2  and  a  lamp  thrown  into  series  with  the 
generating  circuit  by  switch  Si.  The  generator  then  continues 
to  operate  on  a  low  current  and  sufficient  hydrogen  is  liberated 
to  keep  the  system  free  from  air.  Such  a  generator  can  be  run 
continuously  for  months  at  a  time.  When  in  use  the  generator 
carries  about  4.5  amperes.  If  this  current  be  taken  from  a  high 
voltage  lighting  system  there  must  be  placed  in  series  a  proper 

1  Biilmann's  interesting  remarks  on  this  are  cited  on  page  354. 


XVII 


HYDROGEN  GENERATORS 


353 


resistance  which  can  be  either  built  up  by  a  bank  of  lamps  or 
constructed  from  nichrome  wire. 

While  it  is  usually  considered  good  practice  to  eliminate  the 
residual  oxygen  from  electrolytic  hydrogen  by  the  use  of  some 
such  device  as  a  tube  of  heated  platinized  asbestos  (see  below), 
there  may  be  occasions  when  a  supply  of  pure  hydrogen  direct 
from  the  generator  is  desired.  Oxygen  may  accumulate  on  the 
hydrogen  side  of  the  generator  by  diffusion  from  the  oxygen  side. 
This  has  long  been  recognized.  Biilmann  and  Jensen  (1927) 
report  0.13  per  cent  02.  Gaede  (1913)  introduced  a  simple  means 
of  prevention.  His  principle  is  illustrated  in  figure  67.  A  sup- 
plementary electrode  at  C  is  supplied  a  small  current  through 
resistance  R.  From  this  electrode  ascend  fine  bubbles  of  hydro- 


FIG.  67.  ILLUSTRATING  THE  PRINCIPLE  OF  THE  GAEDE-NIESE  HYDROGEN 

GENERATOR 

gen  which,  starting  with  zero  partial  pressure  of  oxygen,  "clean 
up"  the  residual  oxygen  diffusing  from  the  oxygen  layer  above. 
Niese  (1923)  describes  a  more  practical  generator  embodying 
Gaede's  principle.  He  describes  the  hydrogen  thus  obtained  as 
having  exceptional  purity.  Consult  citation  to  Elveden. 

Usually  investigators  have  passed  the  hydrogen  through  tubes 
containing  platinum  in  some  form  which,  when  heated  to  about 
400°C.  very  effectively  removes  residual  oxygen.  On  comparing 
hydrogen  that  had  passed  through  platinized  asbestos  with 
hydrogen  that  had  passed  through  platinum  gauze  Biilmann  and 
Jensen  (1927)  found  that  the  potential  of  the  cell 

-  Pt,  H2 1  HC1  (0.1N),  quinhydrone  |  Pt  + 


354  THE    DETERMINATION   OF   HYDROGEN   IONS 

was  about  half  a  millivolt  higher  in  the  first  case  than  in  the  second. 
This  they  ascribed  to  a  component  in  the  hydrogen  from  the 
platinized  asbestos  that  was  more  active  than  the  hydrogen. 
They  believe  it  to  be  silicon  hydride.  See  also  their  references, 
and  compare  with  Bach  (1925). 

Guntelberg  (1926)  removes  residual  oxygen  from  electrolytic 
hydrogen  (he  prefers  KOH  solution)  by  passing  it  over  copper  at 
450°C.  The  copper  is  pretreated  with  several  oxidations  and 
reductions. 

For  the  conduction  of  hydrogen  over  long  distances,  soft-drawn, 
seamless,  copper  tubing  is  best.  That  with  about  3.2  mm.  ex- 
ternal diameter  is  satisfactory.  Where  this  is  to  be  joined  to  a 
metal  connection,  silver  solder2  applied  with  borax  flux  is  prefera- 
ble to  tin-lead  solder,  since  the  latter  type  of  junction  is  apt  to 


HH  BRASS  SLEEVE  ^H  GLASS  TUBE 
Hi  COPPER  TUBE   d]  SILVER  SOLDER 
ODE  KHOTINSKY  CEMENT 

FIG.  68.  JUNCTION  OF  COPPER  AND  GLASS  TUBES 

contain  "pin-holes."  Where  the  copper  tube  is  to  be  joined  to 
glass  tubing  use  a  piece  of  brass  like  that  of  figure  68.  This  is 
quickly  turned  on  the  lathe.  The  copper  tube  is  first  silver- 
soldered  to  the  brass  sleeve.  The  copper  tube  should  not  fit  too 
loosely.  If  the  metal  is  very  hot  when  the  solder  flows,  silver 
solder  will  run  into  the  junction  nicely.  To  join  with  the  glass 
tube,  warm  both  brass  tube  and  glass  tube,  smear  each  with  hot 
deKhotinsky  cement  and  slip  the  two  together.  The  interior 
diameter  of  the  sleeve  should  be  little  larger  than  the  glass  tube. 
Extra  cement  is  then  moulded,  while  warm,  about  the  whole 
joint  in  order  to  strengthen  it  mechanically. 

2  Silver  solder:  composed  of  6.5  parts  copper,  2.0  parts  zinc  and  11.0 
parts  silver.  This  solder  is  described  as  fusing  at  about  983°C.  A  nickel 
wire  is  useful  in  spreading  the  flux  and  solder.  The  flux  is  prefused  borax. 
The  heat  of  a  blast  lamp  is  required.  Hardware  stores  carry  the  solder. 


XVII 


WIRING 


355 


For  tne  more  elaborate  trains  there  may  be  used  standard 
"f  inch,"  bronze  cocks  of  the  type  with  ground  keys  under  spring 
tension.  These  are  furnished  with  all  sorts  of  ends  for  use  with 
standard  "f  inch"  pipe  fittings  and  with  attachments  for  either 
the  so-called  "compression"  or  the  "soldered  connection"  with 
copper  tubing.  See  for  instance  the  catalogue  of  the  Lunken- 
heimer  Company,  Cincinnati. 

WIRING 

Whenever  a  set-up  is  to  be  made  more  than  an  improvisation 
it  pays  to  make  a  good  job  of  the  wiring.  A  poor  connection  may 


FIG.  69.  SWITCHES  FOR  CONNECTING  HALF-CELLS  WITH  POTENTIOMETER 

be  a  source  of  endless  trouble  and  unsystematized  wiring  may 
lead  to  confusion  in  the  comparison  of  calomel  electrodes  and  the 
application  of  corrections  of  wrong  sign. 

Soldered  connections  or  stout  binding  posts  that  permit  strong 
pressure  without  cutting  of  the  wire  are  preferable  to  any  other 
form  of  contact.  If  for  any  reason  mercury  contacts  are  used 
they  had  best  be  through  platinum  soldered  to  the  copper  lead. 
Copper  wires  led  into  mercury  should  not  take  the  form  of  a 
siphon  else  some  months  after  installation  it  may  be  found  that 
the  mercury  has  been  siphoned  off. 

Thermo-electromotive  forces  are  seldom  large  enough  to  affect 


356  THE   DETEKMINATION    OF   HYDROGEN   IONS 

measurements  of  the  order  of  accuracy  with  which  we  are  now 
concerned  if  care  be  taken  to  make  contacts  so  far  as  possible 
between  copper  and  copper  at  points  subject  to  fluctuations  in 
temperature. 

A  generous  use  of  copper  knife  switches  can  be  made  to  con- 
tribute to  the  ease  and  certainty  of  check  measurements.  For 
instance  if  there  be  a  battery  of  hydrogen  electrodes  and  a  set  of 
calomel  electrodes,  wires  may  be  led  from  each  to  a  centre  con- 
nection of  single-pole,  double-throw  switches  as  shown  in  figure  69. 
All  the  upper  connections  of  these  switches  are  connected  to  the 
+  pole  of  the  potentiometer's  E.  M.  F.  circuit,  and  all  the  lower 
connections  to  the  —  pole.  By  observing  the  rule  that  no  two 
switches  shall  be  closed  in  the  same  direction,  short-circuiting  of 
combinations  is  avoided.  The  position  of  a  switch  shows  at  once 
the  sign  of  the  metal  of  the  attached  half-cell  in  relation  to  any 
other  that  may  be  put  into  liquid  junction.  This  is  a  great  con- 
venience in  comparing  calomel  electrodes  where  one  half-cell  may 
be  positive  to  another  and  negative  to  a  third.  Such  a  bank  of 
single  pole  switches  permits  the  comparison  of  any  electrode  with 
any  other  when  liquid  junction  is  established;  and,  if  a  leak  occur 
in  the  electrical  system,  the  ability  to  connect  one  wire  at  a  time 
with  the  potentiometer  and  galvanometer  often  helps  in  the  tracing 
of  the  leak. 

INSULATION 

For  wires  perhaps  the  most  satisfactory  insulation  for  general 
use  is  pliable  rubber.  The  textiles  are  unsatisfactory  in  damp 
weather  and  although  paper  is  used  very  successfully  in  telephone 
cables  where  close  packing  is  desired  it  must  be  protected  ab- 
solutely from  dampness.  Even  the  terminals  of  the  lead  covered 
cables  must  be  boxed.  Enameled  wire,  the  enamel  of  which  can 
be  tested  for  leaks  by  obvious  connections  made  while  the  wire 
is  run  through  a  mercury  bath,  makes  very  pretty  wiring. 

In  ordinary  potentiometric  measurements,  but  especially  in 
the  operation  of  an  electrometer,  the  high  intrinsic  insulating 
qualities  of  materials  which  are  of  supreme  importance  in  high 
tension  work,  may  become  of  secondary  importance  compared 
with  surface  leakages.  Cleanliness  of  supports  is  therefore  a  part 
of  good  technique,  for  accumulation  of  dirt  may  enhance  the  con- 


xvii  INSULATION;  SHIELDING  357 

ductivity  of  surface  films  of  moisture.  As  far  as  moisture  films 
are  concerned  paraffin,  if  kept  clean,  is  an  excellent  preventive 
of  excess  trouble  for  moisture  does  not  "film  out"  very  well  on 
its  surface.  Of  the  same  properties,  but  preferred  for  its  mechan- 
ical strength,  is  mineral  paraffin  known  as  ozokerite.  When 
such  surfaces  become  dirty  they  should  first  be  wiped  and  then 
flamed  wherever  this  is  practicable. 

The  insulating  material  frequently  used  for  the  machined  parts 
of  instruments,  e.g.,  the  plate  of  a  potentiometer,  is  hard  rubber. 
The  qualities  of  such  rubber  vary  widely.  While  it  usually  has 
a  high  insulating  value  this  may  become  impaired  and  the  surface 
may  become  unsightly  by  the  oxidation  of  its  sulfur  under  the 
action  of  light.  I  know  of  no  satisfactory  remedy.  A  pre- 
ventive is  the  protection  from  light. 

Bakelite  is  replacing  rubber  for  many  purposes  and  since  the 
advent  of  amateur  radio  it  is  readily  available  in  sheets  which  can 
be  cut  to  good  purpose  in  the  installation  and  wiring  of  a  poten- 
tiometer equipment. 

For  some  of  the  extreme  measures  necessary  in  the  operation 
of  the  glass  electrode  with  an  electrometer  as  null-point  instru- 
ment, see  Kerridge  (1926)  and  Brown  (1924). 

SHIELDING 

Electrical  leaks  from  surrounding  high  potential  circuits  are 
sometimes  strangely  absent  from  the  most  crude  systems  and 
sometimes  persistently  disconcerting  if  there  is  not  efficient 
shielding.  The  principle  of  shielding  is  based  on  the  following 
considerations.  If  between  two  supposedly  well-insulated  points 
on  a  light  or  heating  circuit,  or  between  one  point  of  such  a  circuit 
and  a  grounding  such  as  a  water  or  drain  pipe,  there  is  a  slight 
flow  of  current,  the  electrical  charges  will  distribute  themselves 
over  the  surface  films  of  moisture  on  wood  and  glass-ware.  At 
two  points  between  which  there  is  a  difference  of  potential  the 
wires  of  the  measured  or  measuring  system  may  pick  up  the 
difference  of  potential  to  the  detriment  of  the  measurement.  If 
however  all  supports  of  the  measured  and  measuring  systems  lie 
on  a  good  conductor  such  as  a  sheet  of  metal,  the  electrical  leak- 
age from  without  will  distribute  itself  over  an  equipotential 
surface  and  no  differences  of  potential  can  be  picked  up.  To  shield 


358         THE  DETERMINATION  OF  HYDROGEN  IONS 

efficiently,  then,  it  is  necessary  that  all  parts  of  the  system  be 
mounted  upon  metal  that  can  be  brought  into  good  conducting 
contact.  In  many  instances  the  complications  of  hydrogen  elec- 
trode apparatus  and  especially  the  separation  of  potentiometer 
from  temperature  bath  make  a  simple  shielding  impracticable. 
Care  must  then  be  taken  that  all  of  the  separate  parts  are  well 
connected.  Tinfoil  winding  of  insulated  wire  in  contact  with  un- 
shielded points  can  be  soldered  to  stout  wires  for  connection  to 
other  parts  by  dropping  hot  solder  on  the  well-cleaned  juncture. 

Flexible,  rubber-covered  wire  with  a  spirally  wound  armor  is 
especially  valuable  for  shielded  connections.  It  is  sold  for 
automobile  connections. 

Shielding  should  not  be  considered  as  in  any  way  taking  the 
place  of  good  insulation  of  the  constituent  parts  of  the  measured 
or  measuring  systems. 

For  further  details  in  regard  to  shielding  see  W.  P.  White 
(1914). 

TEMPERATURE    CONTROL 

Baths 

Temperature  control  is  a  matter  where  individual  preference 
holds  sway.  There  are  almost  as  many  modifications  of  various 
types  of  regulators  as  there  are  workers.  Even  in  the  case  of 
electrical  measurements  where  orthodoxy  interdicts  the  use  of  a 
water  bath  it  has  been  said  (Fales  and  Vosburgh  and  others)  that 
it  can  be  made  to  give  satisfaction. 

Yet  there  are  a  few  who  may  actually  make  use  of  a  few  words 
of  suggestion  regarding  temperature  control  for  hydrogen  electrode 
work. 

As  a  rule  the  water  bath  is  not  used  because  of  the  difficulty  of 
preventing  electrical  leakage.  Some  special  grades  of  kerosene 
are  sold  to  replace  the  water  of  an  ordinary  liquid  bath  but  for 
most  purposes  ordinary  kerosene  does  very  well.  The  free  acid 
sometimes  found  in  ordinary  kerosene  may  injure  fine  metallic 
instruments.  To  avoid  this,  use  the  grade  sold  as  "acid-free, 
medium,  government  oil." 

A  liquid  bath  has  the  advantage  that  the  relatively  high  spe- 
cific heat  of  the  liquid  facilitates  heat  exchange  and  within  a  half 
hour  or  so  brings  material  to  the  controlled  temperature,  but 


XVII 


AIR    BATH 


359 


compared  with  an  air  bath  it  has  the  disadvantage  that  stopcocks 
must  be  brought  up  out  of  the  liquid  to  prevent  the  seepage  of  the 
oil.  The  advantage  of  the  high  specific  heat  of  a  liquid  is  falsely 
applied  when  the  constancy  of  a  liquid  bath  is  considered  to  be  a 
great  advantage  over  the  -more  inconstant  air  bath.  The  lower 
the  specific  heat  of  the  fluid  the  less  effect  will  variation  in  the 
temperature  of  that  fluid  have  upon  material  which  has  already 
been  brought  to  and  is  to  be  kept  at  constant  temperature.  For 


FIG.  70.  CROSS-SECTION  OF  AN  AIR  BATH 

this  reason  a  well-stirred  air  bath  whose  temperature  may  oscillate 
about  a  well-controlled  mean  may  actually  maintain  a  steadier 
temperature  in  the  material  under  observation  than  does  a  liquid 
bath  which  itself  is  more  constant.  It  is  the  temperature  of  the 
material  under  observation  and  not  the  temperature  of  the  bath 
which  is  of  prime  interest  when  the  temperature  is  once  attained. 
An  air  bath  can  be  made  to  give  very  good  temperature  control 
and  since  it  is  more  cleanly  than  an  oil  bath  and  permits  direct- 


360         THE  DETERMINATION  OF  HYDROGEN  IONS 

ness  and  simplicity  in  the  design  of  apparatus  a  brief  description 
of  one  form  used  by  the  writer  for  some  years  may  be  of  interest. 
A  schematic  longitudinal  section  illustrating  the  main  features 
is  shown  in  figure  70. 

The  walls  of  the  box  are  lined  with  cork  board  finished  off 
on  the  interior  with  "transite."  The  front  is  a  hinged  door 
constructed  like  the  rest  of  the  box  but  provided  with  a  double 
glass  window  and  three  4-inch  hand  holes  through  which  appara- 
tus can  be  reached.  On  the  interior  are  mounted  the  two  shelves 
A  and  B  extending  from  the  front  to  the  back  wall  and  providing 
two  flues  for  the  air  currents  generated  by  the  fan  F. 

The  writer  at  one  time  used  a  no.  0  Sirocco  fan  manufactured 
by  the  American  Blower  Company,  demounted  from  its  casing 
and  mounted  in  the  bearing  illustrated.  He  now  uses  a  four- 
blade  fan  taken  from  a  desk-fan  and  mounted  so  that  it  turns 
in  the  hole  F  of  the  partition  and  blows  toward  E.  The  baffle 
plates  at  E,  made  of  strips  of  tin  arranged  as  in  an  egg-box,  and 
intended  to  establish  parallel  lines  of  flow  when  the  centrifugal 
fan  was  used,  are  now  eliminated. 

In  the  illustration  the  oil  cup  is  shown  as  if  it  delivers  into  an 
annular  space  cut  out  of  the  Babbit-metal  bearing.  In  reality 
this  annular  space  is  provided  by  cutting  away  a  portion  of  the 
steel  shaft. 

The  heating  of  the  air  is  done  electrically  with  the  use  of  bare, 
nichrome  wire  of  no.  30  B.  and  S.  gauge.  When  using  the 
centrifugal  fan  the  wire  is  strung  between  rings  of  asbestos  board 
(the  hard  variety  known  as  "transite"  or  "asbestos  wood")  which 
fit  over  the  fan  at  H.  With  the  blade-fan  the  partition  at  F  is 
made  of  asbestos  board  and  the  wire  is  strung  over  the  opening. 
The  air  is  thus  heated  at  its  position  of  highest  velocity.  The 
electrical  current  in  this  heating  coil  can  be  adjusted  with  the 
weather  so  that  the  time  during  which  the  regulator  leaves  the 
heat  on  is  about  as  long  as  the  time  during  which  the  regulator 
leaves  the  heat  off.  In  other  words  adjustment  is  made  so  that 
the  heating  and  cooling  curves  have  about  the  same  slope. 

When  the  room  temperature  is  not  low  enough  to  provide  the 
necessary  cooling  the  box  I  is  filled  with  ice  water.  Surrounding 
this  is  an  air  chamber  into  which  air  is  forced  from  the  high  pres- 
sure side  of  the  fan.  J  should  be  provided  with  a  damper  which 


XVII  REGULATORS  361 

can  easily  be  reached  and  adjusted.  A  loop  of  copper  tubing 
carrying  cold  water  near  the  heating  wires  would  probably  do  as 
well. 

To  lessen  danger  of  electrical  leakage  over  damp  surfaces  the 
air  is  kept  dry  by  a  pan  of  calcium  chlorid  placed  under  B. 

A  double  window  at  W  over  which  is  hung  an  electric  light  pro- 
vides illumination  of  the  interior.  A  solution  of  a  nickel  salt  is 
placed  at  this  window  to  absorb  the  heat  from  the  lamp. 

The  double  window  in  the  door  (not  shown)  should  be  beveled 
toward  the  interior  to  widen  the  range  of  vision. 

Such  a  box  has  been  held  for  a  period  of  eight  hours  with  no 
change  which  could  be  detected  by  means  of  a  tapped  Beckmann 
thermometer  and  with  momentary  fluctuations  of  0.003°  as  de- 
termined with  a  thermo-element.  The  average  operation  is  a 
temperature  control  within  ±0.03°  with  occasional  unexplained 
variations  which  may  reach  0.1°.  Because  of  the  slowness  with 
which  air  brings  material  to  its  temperature,  the  air  bath  is  con- 
tinuously kept  in  operation,  and  if  a  measurement  is  to  be  made 
quickly  the  solution  is  preheated  to  the  desired  temperature. 

Regulators 

Given  efficient  stirring  and  a  considerate  regulation  of  the 
current  used  in  heating,  accurate  temperature  control  reduces  to 
the  careful  construction  of  the  regulator.  The  ideal  regulator 
should  respond  instantaneously.  This  implies  rapid  heat  con- 
duction. Regulators  which  provide  this  by  having  a  metal  con- 
tainer have  been  described  but  glass  will  ordinarily  be  used. 
At  all  events  there  are  two  simple  principles  of  regulator  construc- 
tion the  neglect  of  which  may  cause  trouble  or  decrease  sensitivity 
and  attention  to  which  improves  greatly  almost  any  type.  The 
first  is  the  protection  of  the  mercury  contact  from  the  corroding 
effect  of  oxygen.  The  second  is  the  elimination  of  platinum 
contacts  which  mercury  will  soon  or  later  "wet,"  and  the  sub- 
stitution of  an  iron,  nickel  or  nichrome  wire  contact. 

After  trials  of  various  designs  the  author  has  adopted  the  form 
of  regulator  head  shown  in  figure  71.  (See  Clark,  1913.) 

Pyrex  glass  is  used  in  its  construction.  To  seal  the  platinum 
lead  at  P  a  very  fine  wire  is  used  and  the  seal  is  made  mechanically 
strong  by  a  sufficient  thickness  of  glass.  Although  such  a  seal 


362 


THE   DETERMINATION    OF   HYDROGEN   IONS 


will  usually  not  be  vacuum-tight  it  can  be  made  so  by  having  the 
mercury  in  the  exterior  arm  during  the  evacuation  presently  to 
be  mentioned.  Preparatory  to  rilling  the  bulb  the  glass  side  arm 
is  constricted  at  D  as  a  preliminary  to  sealing;  beyond  this  con- 
striction it  is  drawn  off  to  a  fine  capillary  E.  The  head  is  then 
attached  to  a  pump  and  the  apparatus  exhausted.  Then  the 
capillary  side  arm  is  broken  under  a  reservoir  of  carefully  purified 
mercury.  If  the  exhaustion  has  been  well 
done,  mercury  will  fill  the  vessel  with  practically 
no  gas  bubbles  left.  The  vessel  is  then  detached 
from  the  pump  and  a  stream  of  pure  hydrogen 
is  swept  through  the  head  entering  at  E. 
There  has  previously  been  prepared  the  contact 
wire  of  "Chromel"  alloy.  This  should  be  large 
enough  to  fill  the  capillary  at  A  nearly 
completely.  However,  its  tip,  to  make  contact 
at  B,  is  etched  with  aqua  regia  until  it  gives 
ample  space  for  the  mercury  column.  If  it  takes 
too  much  space  in  the  capillary  at  B,  mercury 
will  be  squeezed  off  as  drops  when  it  rises  with 
overheating.  With  the  wire  in  place,  deKhotinsky 
cement  is  melted  at  K,  with  care  to  prevent  it 
creeping  to  the  bulb  below.  Meanwhile  the  hy- 
drogen pressure  is  kept  from  building  up  by  es- 
caping through  a  trap.  The  side  arm  is  now 
sealed  at  D.  Ample  excess  mercury  has  been 
left  and  this  is  now  thrown  into  the  side  arm  as 
(1913).  Drawing  shown.  Rough  adjustment  is  made  by  throwing 
by  Courtesy  A.  mercury  m  or  out  of  this  reservoir.  Fine  adjust- 
ments are  made  by  warming  the  cement  at  K  and 
raising  or  lowering  the  wire.  When  adjusted  the 
wire  is  clamped  in  the  chuck  C,  designed  by  A.  H.  Thomas  Com- 
pany, or  simply  held  by  the  cement.  The  capillary  at  B  and  the 
size  of  the  mercury  bulb  can  be  adjusted  to  requirements. 

For  discussion  of  other  regulators  and  principles  of  thermostat 
control  see  numerous  references  in  Chemical  Abstracts  and,  for 
example,  Tian  (1923). 


FIG.  71.  A 
TEMPERATURE 
REGULATOR 
(After    Clark 


H.Thomas  Com- 
pany) 


XVII 


HEAT   CONTROL 


363 


HEAT   CONTROL 

For  electrical  heating,  the  control  system  shown  in  figure  72  is 
simple  and  effective.  The  current  from  the  main,  M,  passes 
through  a  bank  of  lamps  L  to  the  heater  by  way  of  H.  Lamps 
are  used  since  they  provide  a  convenient  variety  of  resistance 
adjustable  to  the  current  desired.  The  current  is  thrown  on  or 
off  by  the  relay,  R,  controlled  by  current  from  the  regulator 
connected  to  T.  To  lower  sparking  the  gap  at  the  relay  is  shunted 
by  lamp  B.  If  direct  current  is  available  it  may  be  used  for  the 
operation  of  the  relay  by  drawing  a  low  potential  circuit  from  the 
resistance  O.  In  case  only  alternating  current  is  available  a  storage 
battery  is  placed  in  series  with  the  relay  and  thermoregulater  T. 
Too  strong  a  current  is  to  be  avoided.  A  sharp,  positive  action  of 


FIG.  72.  WIRING  FOR  HEAT-CONTROL  BY  RELAY 

the  relay  should  be  provided  against  the  day  when  the  relay 
contact  may  become  clogged  with  dust.  To  reduce  sparking  at 
the  regulator  and  at  the  relay  contacts,  inductive  coils  in  the 
wiring  should  be  avoided.  Spanning  the  spark  gaps  with  properly 
adjusted  condensers  made  of  alternate  layers  of  tin  foil  and 
paraffin  paper  may  eliminate  most  of  the  sparking,  if  the  proper 
capacity  be  used. 

For  relay  contacts  the  tungsten  contacts  used  in  gas  engines 
are  very  good. 

For  heaters  to  be  used  in  water  baths  electric  filament  lamps 
are  frequently  used.  With  oil  baths,  base  "Chromel"  alloy  may 
be  used.  This  should  be  kept  immersed  and  the  leads  made 
heavy.  For  good  regulation  it  is  essential  to  adjust  the  current 
until  the  heating  rate  is  about  the  same  as  the  cooling  rate.  This 


364  THE   DETERMINATION    OF   HYDROGEN   IONS 

is  easily  determined  by  noting  the  number  of  lamps  used  in  series 
with  the  heater  when  the  current  is  on  about  the  same  length  of 
time  it  is  off. 

PURIFICATION   OF  MERCURY 

Pure  mercury  is  essential  for  many  purposes  in  hydrogen  elec- 
trode work, — for  the  calomel  and  the  mercury  of  calomel  elec- 
trodes, for  Weston  cells  should  these  be  "home  made/'  for  thermo- 
regulators  and  for  the  capillary  electrometer. 

The  more  commonly  practiced  methods  of  purification  make 
use  of  the  wide  difference  between  mercury  and  its  more  trouble- 
some impurities  in  what  may  be  descriptively  put  as  the  "electro- 
lytic solution  tension."  Exposed  to  any  solution  which  tends  to 
dissolve  base  metals,  the  mercury  will  give  up  its  basic  impurities 
before  it  goes  into  solution  itself,  provided  of  course  the  reaction 
is  not  too  violent  for  the  approach  to  equilibrium  conditions. 

The  most  commonly  used  solvent  for  this  purpose  is  slightly 
diluted  nitric  acid  although  a  variety  of  other  solutions  such  as 
ferric  chloride  may  be  used. 

To  make  such  operations  efficient  it  is  necessary  to  expose  as 
large  a  surface  as  possible  to  the  solution.  Therefore  the  mercury 
is  sometimes  sprayed  into  a  long  column  of  solution  which  is  sup- 
ported by  a  narrow  U-tube  of  mercury.  The  mercury  as  it  col- 
lects in  this  U-tube  separates  from  the  solution  and  runs  out  into 
a  receiver.  To  insure  good  separation  the  collecting  tube  should 
be  widened  where  the  mercury  collects  but  this  widening  should 
not  be  so  large  as  to  prevent  circulation  of  all  the  mercury.  A 
piece  of  very  fine-meshed  silk  tied  over  the  widened  tip  of  a  funnel 
makes  a  fine  spray  if  the  silk  be  kept  under  the  liquid.  This  sim- 
ple device  can  be  made  free  from  dead  spaces  so  that  all  the  mer- 
cury will  pass  through  successive  treatments.  It  is  more  difficult 
to  eliminate  these  dead  spaces  in  elaborate  apparatus;  but  such 
apparatus,  in  which  use  is  made  of  an  air  lift  for  circulating  the 
mercury,  makes  practicable  a  large  number  of  treatments.  A 
combination  of  the  air  lift  with  other  processes  and  a  review  of 
similar  methods  has  been  described  by  Patten  and  Mains  (1917). 

Hulett's  (1905,  1911)  method  for  the  purification  of  mercury 
consists  in  distilling  the  mercury  under  diminished  pressure  in  a 
current  of  air,  the  air  oxidizing  the  base  metals.  Any  of  these 


XVII  PURIFICATION   OF  MERCURY  365 

oxids  which  are  carried  over  are  filtered  from  the  mercury  by  pass- 
ing it  through  a  series  of  perforated  filter  papers  or  long  fine  cap- 
illaries. A  convenient  still  for  the  purpose  is  made  as  follows. 
Fuse  to  the  neck  of  a  Pyrex  Kjeldahl  flask  a  tube  about  30  cm. 
long  which  raises  out  of  the  heat  of  the  furnace  the  stopper  that 
carries  the  capillary  air-feed.  Into  the  neck  of  the  flask  fuse  by 
a  T-joint  seal  a  1.5  cm.  tube  and  bend  this  slightly  upward  for  a 
length  of  15  cm.  so  that  spattered  mercury  may  run  back.  To  the 
end  of  this  15  cm.  length  join  the  condensing  tube,  which  is  simply 
an  air  condenser  made  of  a  meter  length  of  tubing  bent  zigzag. 
Pass  the  end  of  this  through  the  stopper  of  a  suction  flask  and 
attach  suction  to  the  side  tube  of  this  flask.  The  mercury  in  the 
Kjeldahl  flask  may  be  heated  by  a  gas  flame  or  an  electric  furnace. 
For  a  220  volt  D.  C.  circuit  12  meters  of  no.  26  nichrome  (Chromel) 
wire  wound  around  a  thin  asbestos  covering  of  a  tin  can  makes 
a  good  improvised  heating  unit  if  well  insulated  with  asbestos  or 
alundum  cement.  A  little  of  this  cement  applied  between  the 
turns  of  wire  after  winding  will  keep  the  wire  in  place  after  the 
expansion  by  the  heat. 

In  the  construction  of  such  stills  it  is  best  to  avoid  soft  glass 
because  of  the  danger  of  collapse  on  accidental  over-heating. 
Hostetter  and  Sosman  describe  a  quartz  still. 

Both  the  air  current,  that  is  delivered  under  the  surface  of  the 
mercury  by  means  of  a  capillary  tube,  and  the  heating  should  be 
regulated  so  that  distillation  takes  place  smoothly. 

Since  it  is  very  difficult  to  remove  the  last  traces  of  oxid  from 
mercury  prepared  by  Hulett's  distillation  the  author  always  makes 
a  final  distillation  in  vacuo  at  low  temperature.  An  old  but  good 
form  of  vacuum  still  is  easily  constructed  by  dropping  from  the 
ends  of  an  inclined  tube  two  capillary  tubes  somewhat  over  baro- 
metric length.  One  of  these  is  turned  up  to  join  a  mercury  res- 
ervoir, the  other,  the  condenser  and  delivery  tube,  is  turned  up 
about  10  cm.  to  prevent  loss  of  the  mercury  column  with  changes 
in  external  pressure.  The  apparatus  is  filled  with  mercury  by  suc- 
tion while  it  is  inclined  to  the  vertical.  Releasing  the  suction 
and  bringing  the  still  to  the  vertical  leaves  the  mercury  in  the 
still  chamber  supported  by  a  column  of  mercury  resting  on  atmos- 
pheric pressure  and  protected  by  the  column  in  the  capillary 
condenser.  The  heating  unit  is  wire  wound  over  asbestos.  The 


366         THE  DETERMINATION  OF  HYDROGEN  IONS 

heat  should  be  regulated  by  a  rheostat  till  the  mercury  distills 
very  slowly.  By  having  the  mercury  condense  in  a  capillary  the 
still  becomes  self-pumping. 

CAUTION 

Perhaps  few  of  us  who  work  with  mercury  have  a  proper  regard 
for  the  real  sources  of  danger  to  health.  The  vapor  pressure  of 
mercury  at  laboratory  temperatures  is  not  to  be  feared,  but 
emulsification  with  the  dust  of  the  floor  may  subdivide  the  mercury 
until  it  can  float  in  the  air  as  a  distinct  menace.  Its  handling 
with  fingers  greasy  with  stop  cock  lubricant  is  also  to  be  avoided 
on  account  of  possible  penetration  of  the  skin  but  more  particu- 
larly because  of  the  demonstrated  ease  with  which  material  on 
the  hands  reaches  the  mouth. 


CHAPTER  XVIII 
OXIDATION-REDUCTION  POTENTIALS 

We  must  remember  that  we  cannot  get  more  out  of  the  mathematical 
mill  than  we  put  into  it,  though  we  may  get  it  in  a  form  infinitely 
more  useful  for  our  purpose.  —  JOHN  HOPKINSON. 

THE  RELATION  OF  HYDROGEN  ELECTRODE  POTENTIALS  TO 
REDUCTION  POTENTIALS 

The  hydrogen  electrode  is  constructed  of  a  noble  metal  laden 
with  hydrogen,  and  it  may  be  asked  what  relation  it  bears  to 
those  electrodes  which  consist  of  the  noble  metal  alone  and 
which  are  used  to  determine  the  so-called  oxidation-reduction 
potentials  of  solutions  of  mixtures  such  as  ferrous  and  ferric  iron. 

If  a  platinum  or  gold  electrode  be  placed  in  an  acid  solution  of 
ferrous  and  ferric  chlorides  there  will  almost  immediately  be 
assumed  a  stable  potential  which  is  determined  by  the  ratio  of 
the  ferrous  to  the  ferric  ions.  The  relation  which  is  found  to 
hold  is  given  by  the  equation: 

RT  . 


where  Eh  is  the  observed  potential  difference  between  the  elec- 
trode and  the  standard  normal  hydrogen  electrode,  E0  is  a  con- 
stant characteristic  of  this  'particular  oxidation-reduction  equilib- 
rium and  equal  to  Eh  when  the  ratio  L,  +++  is  unity,  R,  T,  n 

and  F  have  their  customary  significances,  and  [Fe++]  and  [Fe+++] 
represent  concentrations  of  the  ferrous  and  the  ferric  ions  re- 
spectively. This  equation  will  be  referred  to  later  as  Peters' 
(1898)  equation.  Its  general  form  is: 


nF       [Ox] 

where  [Red]  represents  the  concentration  of  the  reductant  and 
[Ox]  represents  the  concentration  of  the  oxidant. 

367 


Titrations, 
Reduced  Indiao  Sul|>honatcs 

at  f)H  3.11 
=  ynono-     3=tri- 


2=  di- 


4=Tetra- 


0        20         40         60        80      100 

FIG.  73.  RELATION  OF  ELECTRODE  POTENTIAL,  Eh,  TO  PERCENTAGE 
OXIDATION  AT  CONSTANT  pH 

368 


XVIII  OXIDATION-REDUCTION  369 

• 

If  we  plot  Eh  on  one  coordinate  and  the  percentage  reduction 
on  the  other  coordinate,  we  obtain  a  set  of  curves  identical  in 
form  for  a  given  value  of  n.  The  position  of  each  curve  along 
the  Eh  axis  is  determined  by  the  value  of  E0'  which  fixes  the 
middle  point  and  thereby  places  the  curve  of  a  specific  system. 

Such  curves  for  four  different  systems  are  shown  in  figure  73. 
In  these  cases  the  hydrion  concentration  was  held  constant  for 
reasons  which  will  appear  later.  Each  of  these  particular  curves 
has  the  slope  characteristic  of  an  oxidation-reduction  system  in 
which  the  transformation  of  oxidant  to  reductant  involves  at  one 
and  the  same  step  two  electrochemical  equivalents.  That  is,  n, 
in  equation  (2),  has  the  value  2.  With  the  noteworthy  excep- 
tion that  these  titration  curves  reveal  no  stepwise  oxidation, 
they  are  analogous  to  the  curves  for  acid-base  equilibria  described 
in  Chapter  I. 

It  will  be  clearly  understood  that  in  using  the  term  "oxidation" 
or  the  term  "oxidant"  we  do  not  imply  that  oxygen  is  neces- 
sarily concerned.  Oxidation  is  one  of  those  terms  established 
under  an  old  order  of  thought  and  carried  into  a  new  order  with 
its  meaning  broadened.  As  COg  is  a  "higher"  oxide  of  carbon 
than  CO  it  is  natural  to  regard  the  process  represented  by  2CO 
-{-  O2  — »  2C02  as  an  oxidation.  The  reverse  process,  which  leads 
to  reduction  in  the  degree  of  oxidation,  is  naturally  called  reduc- 
tion. At  one  time  it  was  seen  fit  to  classify  certain  types  of 
chemical  change  in  terms  of  the  participation  of  oxygen.  A 
schematicized  representation  of  the  transformation  of  ferrous  to 
ferric  iron  may  be  based  upon  this  practice. 

<—  reduction 

oxidation  — > 
2FeO   +   0  ^=±  Fe203 

solution          -f  -f  solution 

4HC1  6HC1 

I  I 

2FeCl2  2FeCl3 

ionization  |  I  ionization 

2Fe++  ±^2e  +  2Fe+++ 
<—  reduction 
oxidation  — > 


370  THE   DETERMINATION   OF   HYDROGEN   IONS 

• 

Neglecting  the  by-products  in  the  above  reactions  and  con- 
centrating attention  upon  the  states  of  the  iron,  we  see  that  Fe+++ 
may  be  related  to  the  higher  oxide  and  Fe++  may  be  related  to 
the  lower  oxide.  Hence  Fe+++  may  be  called  the  oxidant  and 
Fe++  the  reductant  of  the  system  Fe+++:  Fe++.  Through  a 
variety  of  such  schemes  a  number  of  transformations  which  are 
now  conveniently  pictured  as  mere  gain  or  loss  of  electrons  are 
described  as  reductions  and  oxidations  respectively.  For  some- 
what more  detail  see  Clark  (1923). 

The  term  ' 'reduction"  does  not,  in  itself,  imply  any  relation  to 
the  participation  of  hydrogen;  but  it  is  often  assumed  that  hydro- 
gen is  concerned  in  reduction  in  much  the  same  way  that  oxygen 
was  thought  to  be  concerned  in  every  "oxidation." 

Before  coming  to  a  more  generalized  presentation  we  shall 
describe  the  relation  between  the  hydrogen  electrode  and  the 
oxidation-reduction  electrode  in  terms  of  hydrogen  and  hydrogen 
ions. 

It  is  known  that  certain  reducing  agents  are  so  active  that 
they  evolve  hydrogen  from  aqueous  solutions.  In  such  a  solu- 
tion an  electrode  would  become  charged  with  hydrogen  and 
would  conduct  itself  much  like  a  hydrogen  electrode.  The  rela- 
tions then  obtaining  can  be  extended  and,  if  we  wish  to  represent 
the  interaction  of  the  reducing  agent  with  the  hydrogen  ions,  we 
have: 

H+  +  reducing  agent  ^±  H  +  oxidation  product 
If  equilibrium  is  established  for  the  above  reaction 

[H+]  [Red]  _ 
[H]  [Ox] 

T,  [H]       [Red] 
^  [H+]  "   [Ox] 

Substituting  K  =L.Lfor  the  ratio  „  in  Peters'  equation, 
(2),  and  placing  n  =  1  for  the  case  at  hand  we  have 

,       RT  [H] 

Eh  =  E0-— Z«K  — 


XVIII         FORMULATION  IN  TERMS  OF  HYDROGEN  ELECTRODE        371 

Since  the  atomic  hydrogen  bears  a  definite  relation  to  the  partial 
pressure  of  molecular  hydrogen,  P,  through  the  equilibrium  ex- 
pressed by; 

[H?  =  KhP, 

we  may  substitute,  collect  constants  under  another  constant  K', 
combine  E0'  and  In  K'  as  E0  and  obtain 


\/p  , 

Eh=  E0-        Jn 


Compare  this  with  the  general  relation  for  the  hydrogen  elec- 
trode 


(4) 

EH  in  (4)  is  zero  by  definition  when  there  is  used  the  "normal 
hydrogen  electrode"  system  of  reference.  When  (3)  is  placed 
on  the  same  basis  E0  is  also  zero,  since  each  of  the  other  terms  in 
(3)  is  identical  with  the  corresponding  term  in  (4). 

In  other  words  we  have  substituted  for  the  oxidation-reduction 
equilibrium  the  corresponding  point  of  equilibrium  between 
hydrogen  and  hydrogen  ions,  and  have  considered  the  potential 
difference  at  the  electrode  as  if  it  were  that  of  a  hydrogen  elec- 
trode. An  inference  is  that  wherever  we  have  an  oxidation- 
reduction  equilibrium  the  components  will  have  interacted  with 
hydrogen  ions  (or  water)  liberating  free  hydrogen  and  building 
up  at  the  electrode  a  definite  pressure  of  hydrogen.  Conversely, 
if  hydrogen  is  already  present  at  the  electrode  with  a  pressure 
too  high  for  the  oxidation-reduction  equilibrium  in  question, 
hydrogen  will  be  withdrawn  until  its  pressure  is  in  harmony 
with  the  oxidation-reduction  equilibrium  (the  position  of  the 
latter  having  been  shifted  more  or  less  by  reduction).  When 
a  constant  pressure  of  hydrogen  is  maintained  at  the  electrode, 
as  it  is  in  the  customary  use  of  the  hydrogen  electrode,  no  true 
equilibrium  can  be  attained  until  this  hydrogen  has  so  far  re- 
duced all  the  substances  in  the  solution  that  they  can  support 
one  atmosphere  pressure  of  hydrogen. 

Incidentally  it  may  be  mentioned  that  it  is  a  matter  of  indiffer- 


372  THE    DETERMINATION    OF   HYDROGEN   IONS 

ence  whether  we  regard  the  re  duct  ant  to  interact  with  the  hydro- 
gen ions  or  the  oxidant  with  the  hydroxyl  ions  or  each  with  water. 
By  use  of  the  equilibrium  equations  which  are  involved  we  reach 
the  same  end-result  whatever  the  path. 

Furthermore  by  the  use  of  certain  theoretical  relations  between 
the  hydrogen  electrode  and  the  oxygen  electrode  we  could  define 
a  potential  in  terms  of  that  of  an  oxygen  electrode. 

This  method  of  relating  oxidation-reduction  equilibria  to  elec- 
trode potentials  is  convenient  for  showing  the  condition  which 
must  obtain  for  a  true  hydrogen  electrode  potential;  but  when  we 
attempt  to  follow  some  of  the  logical  consequences  of  this,  the 
customary  exposition,  we  not  only  meet  some  serious  difficulties 
but  obscure  some  very  important  relations. 

Let  us  calculate  the  hydrogen  pressure  in  equilibrium  with  an 
equimolecular  mixture  of  ferrous  and  ferric  chlorid  in  a  solution 
held  at  pH  1.  A  platinum  electrode  in  such  a  solution  will  have 
a  potential  about  0.75  volt  more  positive  than  the  "normal  hy- 
drogen electrode."  Let  us  consider  this  to  be  the  difference  of 
potential  between  a  hydrogen  electrode  at  pH  1  and  a  normal 
hydrogen  electrode.  Let  us  calculate,  then,  the  hydrogen  pressure 
at  25°C.  from  the  equation: 


0.75  =  -  0.059  log  —  -  (5) 

We  find  the  hydrogen  pressure  to  be  about  10~27  atmospheres. 
At  one  atmosphere  pressure  a  mole  of  hydrogen  occupies  about 
22  liters  and  contains  about  6  X  1023  molecules.  If  the  pressure 
is  reduced  to  6  X  10~23  atmospheres  there  would  be  but  one 
molecule  of  hydrogen  in  22  liters.  If  reduced  to  10~27  atmos- 
pheres there  would  be  but  one  molecule  in  about  37,000  liters. 
To  assume  any  physical  significance  in  such  values  is,  of  course, 
ridiculous.  It  is  only  by  courtesy  then  that  an  electrode  in  a 
mixture  of  ferrous  and  ferric  iron  at  pH  1  can  be  considered  as  a 
hydrogen  electrode. 

FORMULATION  BY  USE  OF  ELECTRON  TRANSFER 

The  problem  of  mechanism  suggested  above  will  not  be  solved 
by  the  following  formal  treatment;  but  this  treatment  may  aid 
the  student  to  retain  an  orderly  view  of  important  relations,  and 


XVIII  ELECTRON   TRANSFER  373 

it  will  provide  a  basis  on  which  to  discuss  the  interrelations  of 
electrodes  of  different  type.  When  this  interrelation  is  under- 
stood a  more  generalized  point  of  view  is  easier  to  attain. 

It  is  generally  agreed  that  one  of  the  fundamental  parts  of  an 
oxidation-reduction  process  is  an  exchange  of  electrons.  Al- 
though too  great  an  emphasis  on  this  as  a  reality  may  be  objec- 
tionable, the  objection  is  not  relevant  to  our  present  purpose,— 
the  organization  of  relations. 

We  shall  use  the  concept  as  a  means  of  developing  several 
different  equations  by  a  common  route.  On  entirely  different 
grounds  we  shall  return  to  the  discussion  of  actuality  later. 

An  example  of  a  process  involving  electron  exchange  is: 

Ferric  ion  +  electron  ^±  ferrous  ion 

+          e       ^±      Fe++ 


Since  such  a  reversible  reaction  is  not  dependent  upon  the 
presence  of  an  electrode  (acting  as  a  catalyst)  it  is  probable  that 
an  exchange  of  electrons  is  going  on  continuously.  There  must 
then  be  some  condition  virtually  equivalent  to  a  free-electron 
pressure.  If  we  desire  a  mechanistic  picture  we  may  imagine  a 
moment  in  the  exchange  during  which  the  electron  is  balanced 
between  the  forces  of  each  ion.  At  this  moment  the  electron 
may  be  considered  to  belong  to  neither  ion  and  to  be  a  property 
of  the  environment.  Undoubtedly  the  situation  is  not  so  simple 
as  this  picture  suggests;  and,  although  the  presence  of  free  elec- 
trons has  been  demonstrated  in  liquid  ammonia  and  methylamine 
solutions,  the  experimental  evidence  is  not  sufficient  to  justify 
our  assuming  the  presence  of  free  electrons  in  aqueous  solutions 
to  be  a  fact.  However,  it  may  be  said  at  once  that  we  are  not 
now  concerned  with  the  objective  actuality  of  a  "freedom."  A 
pressure  of  free  electrons  may  be  postulated  as  the  virtual  equiva- 
lent of  a  condition  not  yet  clearly  formulated;  it  may  be  used  in 
much  the  same  way  that  Nernst  used  "solution  tension,"  — 
destined  from  the  first  to  be  eliminated  from  those  equations 
which  are  employed  to  formulate  experimental  data. 

An  electron  escaping  tendency  may  be  postulated  without 
necessarily  implying  appreciable  numbers  of  free  electrons  and 
without  immediate  investigation  of  the  source  of  the  electrons 
which  are  transferred  from  one  system  to  another  when  the  oxi- 


374  THE    DETERMINATION    OF   HYDROGEN   IONS 

dant  and  reductant  of  one  system  interact  with  the  oxidant  and 
reductant  of  another  system. 

Imagine  an  aqueous  solution  of  ferrous-  and  ferric  chlorides  in 
which  there  is,  initially,  an  exact  equivalence  between  the  positive 
charges  carried  by  all  cations  and  the  negative  charges  carried  by 
all  anions.  If  an  electron  should  leave  a  ferrous  ion  without 
passing  over  to  a  ferric  ion  (thereby  creating  a  new  ferrous  ion 
to  take  the  place  of  the  first)  no  disturbance  of  the  solution's 
electroneutrality  would  occur.  There  would  still  be  equivalence 
of  positive  and  negative  charges.  The  same  would  be  true  if 
the  ferrous  and  ferric  ions  reacted  with  components  of  the  solu- 
tion as 

Fe++  +  H+  ^  Fe+++  +  H 
Fe++  +  Cl  ^±  Fe+++  -f  Cl~ 

We  are  evidently  not  concerned  with  ordinary,  electrostatic 
affairs. 

There  might  be  expected  some  degree  of  action  between  the 
iron  ions  and  components  of  the  solution  in  the  sense  written 
above.  However,  it  has  already  been  indicated  (page  372)  that 
the  action  of  ferrous  ions  on  hydrions  to  form  hydrogen  and 
ferric  ions  cannot  be  appreciable.  Indeed  we  shall  anticipate  a 
conclusion  to  be  drawn  when  the  formulation  is  complete  and  the 
data  are  at  hand.  We  shall  state  that  no  appreciable  chlorine 
would  be  formed  from  the  second  of  the  above  reactions.  In 
general  none  of  the  oxidation-reduction  systems  to  be  considered 
in  this  section  acts  appreciably  on  other  components  of  the  solu- 
tions to  be  considered. 

Therefore,  in  an  acid1  solution  of  ferric  and  ferrous  chlorides, 
we  shall  consider  the  oxidation-reduction  system  to  be  exclusively 
that  represented  by 


electron 

*Acid  to  prevent  hydrolysis  and  the  formation  of  Fe(OH)2  and  Fe(OH)3. 
The  participation  of  these  and  other  complexes  is  considered  in  a  separate 
section. 


XVIII  DERIVATION    OF   EQUATION  375 

This  we  shall  call  the  "iron  system."     The  equilibrium  state 
we  shall  describe  by 

fFo-H-n   (^ 

-  -  KFe  (6) 


Where  (  )  represents  activity  and  (e)  Fe  is  the  electron  activity2  in 
the  iron  solution. 

Next  imagine  another  oxidation-reduction  system  described  by 


;  -  *  H2 
hydrion     electron     hydrogen 

This  we  shall  call  the  hydrogen  system. 

Knowing  that  hydrogen  by  itself  acts  slowly,  we  may  assume, 
in  the  following  discussion,  the  presence  of  a  catalyst  that  will 
always  insure  the  attainment  of  the  equilibrium  states  to  be  con- 
sidered. For  convenience  we  shall  use  hydrogen  pressure,  P, 
(in  atmospheres)  in  defining  the  equilibrium  equation. 


For  the  transfer  of  F  (one  faraday)  electrons  from   activity 
(c)H  to  activity  (e)Fe 

-  A*1  =  E  F  =  RT  In  7%  (9) 

WFe 

Where  E  is  the  electromotive  force  in  volts. 

Substitute  in  (9)  the  equivalents  of  (e)n  and  (e)pe  from  equa- 
tions (6)  and  (7) 


Rewrite  (10)  as  (13)  where 

(11) 


2  The  electron  activity  need  not  be  defined.  It  is  a  tentative  expedient 
destined  from  the  first  to  be  eliminated  from  the  final  equations.  But 
see  page  376. 


RT.      1 
'  =  "F"  ln  *T 

J^-Fe 

RT7    \/P 

RT      (Fe~+) 

(12) 
(13) 

F  ln  (H+)  H 

F        (Fe++) 

376  THE    DETERMINATION    OF   HYDROGEN    IONS 

and 


E  =  EH  +  EFe 

We  shall  now  make  the  definition  that  when  P  =  1  and  when  (H+) 
=  i,  (e)H  =  1.  Then  by  (7)  KH  =  1  and  by  (11)  EH  =  0.  Equa- 
tion (13)  may  then  be  written 

T>rp  /TT< U4-N 

(14)3 


3If  the  solution  containing  the  iron  system  and  that  containing  the 
hydrogen  system  were  mixed  the  two  systems  would  react  either  toward 
the  right  or  the  left  as  expressed  below. 

H  +  Fe+++^  Fe++  +  H  + 


We  can  anticipate  and  say  that  it  would  he  largely  toward  the  right  as 
written.  That  is,  hydrogen  (represented  for  brevity  as  atomic)  gives  up 
electrons  to  Fe+++.  Fe++  and  H  +  are  formed.  At  equilibrium  in  the 
mixture  (e)Fe  =  («)H.  Hence  by  (6)  and  (7) 

CFe")  (H+)        KH 

-  —  r  =    —  —  (fl) 

V  P       KFe 


If  relative  values  of  KH  and  Kpe  could  be  found,  the  state  of  the  equilibrium 
would  be  denned.  Such  relative  values  will  appear  in  due  course  of  the 
development. 

By  mixing  the  two  solutions  we  obtain  no  external  work  of  definite 
magnitude. 

Next  suppose  the  solution  containing  the  iron  system  were  separated 
from  the  solution  containing  the  hydrogen  system  by  an  intervening  solu- 
tion of  KC1  (saturated).  We  shall  assume  that  this  solution  eliminates 
liquid  junction  potential  of  the  kind  caused  by  unequal  rates  of  diffusion 
of  ions.  We  have  already  anticipated  the  conclusion  that  the  electron 
escaping  tendency  or  activity  is  greater  for  the  electrons  in  the  hydrogen 
system  than  for  those  in  the  iron  system.  Presumably  then  electrons 
could  escape  into  the  potassium  chloride  solution  from  the  side  of  the 
hydrogen  system  more  easily  than  from  the  side  of  the  iron  system.  But 
if  we  permit  free  diffusion  of  ions  this  should  cause  no  potential  difference 
since  the  electrons  can  be  accompanied  by  positive  ions,  and  since  we 
have  postulated  for  the  sake  of  simplicity  that  the  KCl-solution  eliminates 
diffusion  potentials  of  the  ordinary  kind.  Indeed  there  is  no  occasion  to 


xvin  "FUNDAMENTAL"  EQUATION  377 

E  of  (13)  is  here  written  Eh  to  signify  reference  to  the  standard 
hydrogen  system.     When  (Fe++)   =   (Fe+++),  Eh  =  EFe. 

In  general  when  (e)H  is  unity  and  the  hydrogen  system  is  con- 
nected as  specified  with  any  oxidation-reduction  system  the 
electron  activity  of  which  is  (e),  equation  (9)  may  be  written 
as  (15) 


(«)  (15) 

f 

This  will  be  our  "fundamental"  equation.     See  footnotes  3  and  4. 

believe  that  there  occurs  appreciable  transfer  of  free  electrons  across  the 
the  boundary.  Of  course,  in  time,  the  components  of  the  iron  and  hydro- 
gen systems  will  diffuse,  meet  and  interact.  But  we  shall  assume  that  this 
does  not  occur  within  the  time  of  an  ordinary  experiment.  For  ordinary 
purposes  we  can  assume  that  the  interposed  solution  of  KC1  is  itself 
"unattacked"  and  keeps  the  two  oxidation-reduction  systems  from  inter- 
acting. 

But  suppose  that  the  intervening  KCl-solution  contained  some  oxida- 
tion-reduction system  which  could  be  acted  upon  by  the  iron  system  on 
the  one  hand,  or  by  the  hydrogen  system  on  the  other  hand,  or  by  both. 
If  we  permit  diffusion  of  the  components  of  this  new  system  within  the 
intervening  solution,  or  assume  transfer  of  electrons  in  the  tendency  of 
the  intermediate  system  to  maintain  equilibrium  between  contiguous 
layers,  it  is  obvious  that  the  new  system  will  transmit  to  the  iron  system 
the  reducing  action  of  the  hydrogen  system  or  that  it  will  transmit  to  the 
hydrogen  system  the  oxidizing  action  of  the  iron  system.  Then,  in  the  iron 
solution,  the  concentration  of  Fe+++  will  be  lowered  and  that  of  Fe++ 
raised;  while,  in  the  hydrogen  system  under  constant  hydrogen  pressure, 
the  concentration  of  H+  will  be  raised.  To  compensate  for  these  effects 
negative  ions  must  migrate  from  the  iron  side  to  the  hydrogen  side  and  in 
quantity  equivalent  to  the  virtual  flow  of  electrons  in  the  opposite  direc- 
tion. Consequently  no  unidirectional  electric  current  has  been  produced. 
No  external  work  of  definite  magnitude  is  produced. 

In  passing  it  may  be  emphasized  that  we  are  assuming  both  free  move- 
ment of  ions  and  simultaneity  of  events.  In  the  absence  of  either  of  these 
conditions  interesting  phenomena  might  occur. 

Return  to  the  case  in  which  the  iron-  and  the  hydrogen  systems  are 
separated  by  the  pure  solution  of  potassium  chloride.  But  now  provide 
any  new  path  by  which  electrons  unaccompanied  by  ions  can  pass  from  the 
side  where  their  escaping  tendency  is  the  higher  to  the  side  where  their 
escaping  tendency  is  the  lower.  Filter  the  ions,  as  it  were.  Continuing 
with  our  anticipation  which  is  to  be  fulfilled  when  the  formulation  is 
complete  and  the  data  are  at  hand,  we  state  that  the  electron  escaping 
tendency  is  the  greater  at  the  hydrogen  side.  Therefore,  through  the  path 


378  THE    DETERMINATION    OF   HYDROGEN    IONS 

In  general  an  oxidation-reduction  system  can  be  defined  by 
Ox  +  ne  ^±  Redn~ 

by 

Oxn++  ne  =  Red 

or  by  any  intermediate  case.  To  avoid  complexity  of  symbols 
consider  the  first  of  the  above  cases  to  be  the  type  and  write 
the  equilibrium  equation 


Substitute  the  equivalent  of  (c)  by  equation  (16)  in  equation  (15) 
and  separate  the  constant  as  E0. 

This  is  the  type  equation  for  the  electromotive  force  between  any 
oxidation-reduction  system  (involving  n  equivalents  in  a  non- 
stepwise  oxidation  or  reduction)  and  the  standard  hydrogen 
system  connected  in  the  manner  indicated. 

The  procedure  provides  a  uniform  method  of  deriving  the 
electromotive  force  equation  for  any  oxidation-reduction  system 
referred  to  the  hydrogen  standard. 

In  the  development  given  above  we  have  not  specified  the 


provided,  electrons  will  pass  from  the  hydrogen  side  leaving  an  excess  of 
H+  on  that  side.  They  will  enter  the  iron  system  and  transform  Fe+++ 
to  Fe++.  Excess  chloride  ions  are  left  on  the  iron  side.  These  migrate  to 
the  excess  H+  on  the  hydrogen  side.  A  unidirectional  electric  current  is 
generated.  Simultaneity  of  the  steps,  separated  for  purposes  of  descrip- 
tion, is,  of  course,  assumed. 

Were  these  processes  allowed  to  take  place  without  restraint  there 
would  be  waste  of  energy  by  resistance,  heating,  etc.  But  now  let  the 
electron  path  be  supplied  with  any  device  whereby  the  pressure  of  the 
electron  stream  can  be  exactly  counterbalanced.  Presumably,  if  the 
whole  system  is  under  constant  external  pressure  and  constant  tempera- 
ture, and  if  the  pressure  of  the  electrons  is  balanced,  we  have  the  condi- 
tions for  the  measurement  of  the  free  energy  change  of  a  reversible  process. 


"FUNDAMENTAL"  EQUATION  379 

nature  of  the  path4  whereby  electrons  without  accompanying  ions 
may  pass  from  one  oxidation-reduction  system  to  another. 

The  path  usually  provided,  although  not  necessarily  the  only 
path  that  could  be  provided,  is  a  metallic  path.  In  providing 
such  a  path  we  feel  fairly  sure  that  appreciable  transfer  of  ions 
does  not  occur  and  that  movement  of  electrons,  or  the  equivalent 
thereof,  does  occur  in  that  path. 

However,  if  our  formulation  is  to  hold  there  should  be  no  appre- 
ciable attack  upon  the  metal  immersed  in  either  solution.  Were 
that  to  occur  there  would  be  a  local  effect  comparable  with  the 
local  effect  in  the  case  of  direct  contact  between  the  iron  and 

4  That  the  Volta-effect  does  not  enter  is  indicated  as  follows:  Let  dF 
be  the  increase  in  total  free  energy  of  a  system  when  dn  equivalents  of 

dF 

electrons  are  added.    Then  — -  is  the  partial  molar  free  energy  of  electrons 

dn 

in  that  system. 

When  an  electron  is  removed  from  a  material  system  an  unmatched 
positive  charge  is  left.  There  is  then  an  electrostatic  attraction  which 

must  be  overcome.     This  electrostatic  effect  is  part  of  — •     Therefore, 

dn 

dF 

— -  will  be  considered  to  be  made  up  of  two  terms.  One  of  these,  F.  corre- 
dn 

sponds  to  the  free  energy  of  neutral  molecules.  The  other  is  the  electro- 
static energy,  N0€V  where  V  is  the  electrostatic  potential,  N0  is  the  Avo- 
gadro  number  ande  the  electron  charge  (negative). 

|^  =  F  -  N0eV  (a) 

Assume  two  metals  indicated  in  the  following  equations  by  subscripts  mi 
and  m2  and  two  solutions  indicated  by  subscripts  Si  and  s2. 

Let  metal  mi  be  contiguous  to  solution  si  and  metal  m2  be  contiguous 
to  solution  s2.  At  these  contiguous  faces  interchanges  of  electrons  or 
material  permit  establishment  of  equilibrium  between  the  contiguous 
phases. 

Hence 

— J  =  — J  =  Fm  -  NoeVmi  =  p.  -  N0eV.  (b) 

dn          dn 

Also 

dn          dn 


380  THE    DETERMINATION    OF    HYDROGEN    IONS 

hydrogen  systems  discussed  in  footnote  3.  To  avoid  the  latter  we 
separated  the  two  solutions  by  "unattackable"  KCl-solution.  To 
avoid  the  similar  effect  at  the  electrode  we  provide  an  "unattack- 
able"  metal. 

A  base  metal  in  contact  with  a  solution  of  its  ions  is  a  very 
special  and  a  comparatively  rare  case,  although  it  is  the  case 
which,  until  recently,  has  received  the  most  attention.  Certain 
aspects  of  this  case  can  be  discussed  to  better  advantage  later. 
For  the  moment  we  may  assume  that  the  massive  metal  maintains 
the  activity  of  the  metal  molecules  or  atoms  in  the  given  solution 
at  a  constant  value.  Therefore,  the  equilibrium  equation  (18) 
of  the  system 

Mn+  +  ne  ^±  M 


may  be  written 

~K 


(19) 


In  accordance  with  the  scheme  discussed  above,  solutions  Si  and  83  are 
to  be  separated  by  an  "unattackable"  solution  to  prevent  transfers  which 
will  establish  a  mixing.  But  for  present  purposes  we  can  neglect  the 
intermediate  solution  and  retain  the  conditions  it  was  supposed  to  es- 
tablish. One  of  these  was  elimination  of  junction  potential  due  to  unequal 
migration  of  ions.  Another  was  such  an  unrestrained  migration  of  ions 
as  to  prevent  the  production  of  any  excess  electric  charge  of  any  kind  in 
either  solution.  In  short,  it  is  supposed  that  no  electrostatic  difference 
of  potential  exists  between  the  two  solutions.  Therefore, 

V.,  -  V82  =  0  (d) 

By  (b)  (c)  and  (d) 


dn          dn 

But  it  is  the  difference  in  free  energy  per  equivalent  of  electrons  which 
is  measured  by  the  potentiometric  method,  and  it  is  the  difference  FS 
—  FS2  that  was  used  in  our  formal  equations. 

For  references  on  the  Volta-effect  see  Rodebush  (1927),  Langmuir 
(1916),  Lodge  (1885)  and  Corbino  (1927). 


XVIII  SUMMARY    OF    EQUATIONS  381 

By  the  usual  procedure  we  substitute  the  equivalent  of  (e)  by 
(19)  in  the  "fundamental  equation,"  (15).  We  also  separate  the 
constant  as  usual  and  obtain: 


Eh  =  Eo  +  ^-  In  (M«+)  (20) 

nr 

For  convenience  we  shall  now  assemble  a  few  equations  of  part  icu- 
lar  importance  to  our  subject. 

The  "hydrogen  system": 

Eh=  -    ^fc(g|  (21) 

The  " oxygen  system": 

02  +  2H20  +  4e  ^±  40H- 
Let  (H20)  be  constant.     p0  =  pressure  of  02. 

RT7    (OH-) 

Eh  =  E°-T^VpT  (22) 

Metal-metal  ion  system : 

Mn+  +  ne  ^±  M 
See  above 


Eh  =  E0  +    -  In  (M»+)  (23) 

nr 


Any  oxidation-reduction  system  of  the  type 
Ox  +  ne  ^  Red*- 


*•*!!  **O  — -       l/*v  /  s~~         \ 

nF          (Ox) 
Special  oxidation-reduction  system 

Ox  +  2e  ^  Red— 

RT  ^  (Red~) 


(24) 


382        THE  DETERMINATION  OF  HYDROGEN  IONS 

The  development  given  above  may  not  be  comprehensive 
enough  to  meet  all  requirements  as  to  detail  but  it  is  general 
enough  and  sufficiently  rigid  to  have  some  advantage.  Its  chief 
advantages  are:  first  an  easily  remembered  device  for  the  formula- 
tion of  the  orienting  equation  of  any  cell,  second  the  emphasis  of 
the  family  relationship  of  cells  which  all  too  often  are  considered 
unique.  Both  of  these  advantages  will  be  utilized  in  the  dis- 
cussion of  important  matters  to  follow. 

THE   PARTICIPATION   OP  HYDRIONS 

Of  importance  to  the  subject  of  this  book  is  the  fact  that  the 
reductant  appearing  in  equation  (25)  is  an  anion.  There  are 
various  cases  analogous  with  this  but  different  in  type.  For  in- 
stance, a  positive  charge  in  an  oxidant's  cation  may  be  neutralized 
by  one  electron  and  an  anion  may  be  created  by  a  second  electron. 

Ox+  +  2e  ^±  Red- 

It  will  not  alter  the  principle  if  we  continue  with  the  very  simple 
case  described  by 

Ox  +  2C  =  Red— 
The  orienting  electrode  equation  is 


And  now  to  avoid  complexities,  the  consideration  of  which 
would  not  seriously  alter  the  conclusions,  we  shall  assume  that 
activities  may  be  replaced  by  concentrations.  Equation  (26) 
then  becomes:5 


Assume  that  the  oxidant  has  neither  acidic  nor  basic  groups  and 
that  its  concentration  during  shifts  in  hydrion  concentration  can 
always  be  identified  as  that  of  the  total  oxidant,  [SJ.  If  we  wish 
to  reconstruct  (27)  to  include  the  total  reductant,  [SR],  as  is 

6  In  this  book  ()  signifies  activity  and  [  ]  concentration. 


XVIII  PARTICIPATION   OF   HYDRIONS  383 

necessary  when  we  know  nothing  about  the  concentration  of  the 
anion,  Red  ,  and  are  forced  to  measure  the  total  reductant,  it 
is  necessary  to  use  the  equilibrium  equations: 

[H+]  [HRed-]  _ 
[H2Red] 

[H+][Red-~]  _ 

[HRed-] 
and  the  summation 

[SK]  =  [Red—]  +  [H  Red-]  +  [H2Red]  (30) 

Substitute  (28)  and  (29)  in  (30)  and  solve  for  [Red—] 

[SR]  Ki  K2 


Substitute  (31)  in  (27),  collect  constants  under  E0  and  replace 
[Ox]  by  [SJ. 


ra  I 
Eh  =  Eo  "    F  ln  [sj  +  W  ln  [Kl  K2  +  Kl  IH+1  +  [H+]2]  (32) 

If  [H+]  is  kept  constant,  as  by  means  of  a  strong  buffer  solu- 
tion, the  last  term  of  (32)  is  constant  and  (32)  may  be  written  : 


It  was  this  equation  that  was  used  in  constructing  the  curves  of 
figure  73. 

When  the  acidic  or  basic  nature  of  the  system  is  changed,  the 
form  of  the  last  term  in  equation  (32)  is  altered.     For  the  system 

Ox  +  2e  ^±  Red- 


RT      [SR]       RT 
Eh==E°-W^[sJ  +  WZn 

where  Kr  is  defined  by 

•       [Red-]  [H+] 
[HRed] 


384         THE  DETERMINATION  OF  HYDROGEN  IONS 

and  Ko  is  defined  by 

[Oi]  Kw 


[OxOH]  [H+] 

Thus  it  is  evident  that  the  peculiarities  of  a  given  system  are 
(with  some  exceptions)  expressed  by  the  last  term  of  such  equa- 
tions as  (32)  and  (34). 

Obviously  if  [H+]  is  constant,  (34)  like  (32)  may  be  written  as 

(33). 

To  study  the  last  term  of  (32)  set  ^1  =  -t     Then  (32)  be- 

[S0]       1 

comes  (35) 


Eh  =  Eo  +  ^-  In  [KiK*  +  K!  [H+]  +  [H+]2]  (35) 

Zr 

The  geometry  of  (35)  is  illustrated  in  figure  74.  Vary  [H+]  but 
let  [H+]  be  determined  in  each  instance  by  the  independently 
measured  pH  value  of  a  buffer  solution.  When  [H+]  is  large  in 


relation  to  KI  and  K2,  Eh  varies  as  —  In  [H+],  or,  at  30°,  -0.06 

F 

pH.  When  [H+]  is  small  in  relation  to  KI  and  K2  the  last  term 
in  (35)  is  practically  constant  and  the  potential  is  no  longer 
affected  by  alteration  of  pH.  Between  these  extremes  the  curve 
passes  through  points  of  inflexion  centered  at  values  of  pH  equal 
to  pKi  and  pK2. 

In  figure  74  the  geometry  of  (33)  is  illustrated  by  the  curves 
for  certain  fixed  values  of  [H+].  Left  of  figure. 

To  obtain  the  picture  representative  of  the  complete  equation 
(32),  a  figure  in  three  dimensions  is  necessary.  It  will  be  similar 
to  that  represented  by  the  isometric  drawing  of  figure  75.  This 
shows  a  surface  descriptive  of  the  system  of  which  2-6  dibromo 
benzenone  indophenol  is  the  oxidant.  (See  Cohen,  Gibbs  and 
Clark  (1924).) 

In  many  cases  which  have  proved  amenable  to  measurement, 
other  than  the  two  acidic  groups  assumed  above  for  purposes  of 
simplicity  must  be  taken  into  consideration.  Even  a  group  not 
directly  concerned  in  the  oxidation-reduction  process  may  have  its 
dissociation  constant  altered  when  the  substance  is  transformed 


XVIII 


PARTICIPATION    OF   HYDRIONS 


385 


from  an  oxidant  to  a  reductant.  The  resulting  energy-change  then 
becomes  evident;  and  the  equation  required  to  account  for  the 
actual  measurements  may  be  more  complicated. 

The  more  varied  examples  of  the  several  effects  are  to  be  found 
in  a  series  of  papers  entitled  Studies  on  Oxidation-Reduction  by 


h 

^ 

\ 

\ 

s. 

\ 

\l 

-*E 

A 

V 

\ 

I  apH 

\ 

^-- 

^^ 

^J 

\ 

\ 

\ 

\ 

\                   P«1 

9 

\ 

V           -AE  _  .. 

HK^-" 

\.   \              oK                -AE 

1* 

3 

I    H5  ^ 

=^_ 

00             5 

0               ( 

i 

>                  8                 10                   214 

OXIDATION 

FIG.  74.  (Le/0  RELATION  OF  ELECTRODE  POTENTIAL  TO  PERCENTAGE 
OXIDATION  AT  CONSTANT  pH  AT  VARIOUS  LEVELS  OF  pH;  (Right) 
RELATION  OF  ELECTRODE  POTENTIAL  TO  pH  AT  CONSTANT  PERCENTAGE 
(50  per  cent)  OXIDATION 

SYSTEM:  Anthraquinone,2,7-disulfonic  acid  and  its  reductant  at  25°. 
Drawn  from  data  of  Conant,  Kahn,   Fieser  and  Kurtz   (1922). 


0.05912  expressed  as  0.06. 


ApH 


Clark,  Cohen,  Gibbs,  Sullivan,  Cannan  et  al.  reviewed  up  to  1925 
by  Clark  in  Chemical  Reviews,  2,  127,  (1925).  See  also  the  ref- 
erences there  given  to  papers  by  Biilmann,  by  LaMer,  by  Conant 
and  their  coworkers. 


386 


THE    DETERMINATION    OF   HYDROGEN   IONS 


Since,  in  the  majority  of  cases,  equation  (33)  applies  when  [H+] 
is  constant,  this  equation  may  be  considered  applicable  at  any 
fixed  level  of  [H+]  and  attention  may  be  centered  upon  the  rela- 


ro    I 

tion  of  potential  to  pH  when  L-I*I  =  1. 

[S0J 


With  this  understood  a 


FIG.  75.  ISOMETRIC  DRAWING  OF  THE  SURFACE  DESCRIPTIVE  OF  THE  SYSTEM 
COMPOSED  OF  2-6  DIBROMO  PHENOL  INDOPHENOL  AND  ITS  REDUCTANT 
(After  Cohen,  Gibbs  and  Clark  (1924).    See  Clark  et  al.    Studies  on 
Oxidation-Reduction,  VI.) 

system  may  be  described  graphically  by  the  so-called  E'0:  pH 
curve.     Figure  76  illustrates  a  few  of  the  many  cases  in  which 

[•Q       I 


[S0J 


has  been  maintained  at  a  ratio  of  unity  and  the  potential 


measured  as  pH  is  varied.  On  curves  3  and  4  (fig.  76)  the  points 
at  pH  =  3.91  correspond  to  the  mid-points  of  the  corresponding 
curves  in  figure  73. 


+1.2 

+  .8 
+.6 
+  .4 
+  .2 
0 
-.2 


-.4 

Eh 
-.6 

-.8 


PH 


0 


>  p 
H/0, 

-   10° 


.- 


icr4 
10° 

4 


FIG.  77 
FIG.  76 

1.  Relation  of  potential  of  hydrogen  electrode  (1  atmosphere^Hz)  to  pH. 
12.  Theoretical  relation  of  potential  of  oxygen  electrode  (1  atmosphere 

O2)  to  pH. 

2-11.  Systems  at  50  per  cent  reduction,  named  below  by  one  component. 

2.  Anthraquinone-/3-sulfonic  acid  (oxidant). 

3.  Indigo  disulfonate  (oxidant). 

4.  Indigo  tetra  sulf onate  (oxidant) . 

5.  Methylene  blue  (oxidant). 

Br  S08Na 


6.  Oxidant:  HO 


Br 

Cl 


7.  Oxidant:  HO 


-  N 


-  N 


=  0. 


=  0. 


Cl 


8.  Benzo-quinone  (oxidant). 

9.  K,Fe(CN)6:K4Fe(CN)6. 

11.  o-Tolidine  (reductant). 

FIG.  77.  THEORETICAL  RELATIONS  BETWEEN  ELECTRODE  POTENTIAL,  Eh,  pH 
AND  PARTIAL  PRESSURES  OF  HYDROGEN  AND  OXYGEN 

Each  decrement  of  the  partial  pressure  of  hydrogen  by  10~4  shifts  the 
potential  of  a  hydrogen  electrode  at  30°  +  0.03  X  4  =  0.12  volt. 

Each  decrement  of  the  partial  pressure  of  oxygen  by  10~4  shifts  the  theo- 
retical potential  of  an  oxygen  electrode  —  0.015  X  4  =  —0.06  volt. 

Since  the  position  of  any  one  of  the  diagonals  of  figure  77  is  determined  by  log 
hydrogen  pressure'  Clark  Pr°P°sed  the  term  "rH"  *°r  this  quantity,  believing  that  it  would  be 
a  convenience  for  the  general  discussion  of,' the  general  position  of  an  oxidation-reduction  sys- 
tem.    Unfortunately  the  term  rH  has  been  frequently  used  where  potential  would  be  far  pref- 
erable.   Because  of  this  indiscriminant  use,  further  employment  of  rH  is  to  be  discouraged. 

387 


388  THE    DETERMINATION    OF   HYDROGEN    IONS 

THE  RELATION  OF  HYDROGEN  POTENTIALS  TO  GENERAL  RELATIONS 
DESCRIBED   GRAPHICALLY 

To  show  graphically  the  possibilities  of  interpreting  the  poten- 
tials of  one  system  in  terms  of  the  potentials  of  another  consider 
figure  77.  At  pH  =  0  a  properly  prepared  electrode  under  one 
atmosphere  of  hydrogen  is  given  the  arbitrary  reference  poten- 
tial of  0.  As  pH  increases,  the  potential  of  such  an  electrode 
becomes  more  negative,  and,  at  the  temperature  chosen  for 
purposes  of  the  drawing,  it  becomes  more  negative  by  0.06  volt 
per  unit  increase  of  pH.  In  short  the  line  thus  defined,  and 
readily  identified  on  the  chart,  is  the  line  of  the  potential  of  a 
hydrogen  electrode  under  one  atmosphere  of  hydrogen.  Above 
this  line  and  distant  about  1.23  volts  at  all  values  of  pH  is  the 
line  of  the  hypothetical  oxygen  electrode  under  one  atmosphere 
of  oxygen.  The  region  above  this  line  of  the  oxygen  electrode 
may  be  considered  for  present  purposes  as  the  region  of  oxygen 
"overvoltage"  and  the  region  below  the  line  of  the  hydrogen 
electrode  may  be  considered  the  region  of  hydrogen  "  over  volt  age." 
In  other  words  they  are  regions  in  which  the  potentials  would 
be  such  that,  at  the  given  pH  value  of  the  solution,  hydrogen 
or  oxygen,  as  the  case  might  be,  would  be  liberated  from  water 
at  an  equilibrium  pressure  of  over  one  atmosphere.  Between  these 
arbitrary  limits  lie  the  oxidation-reduction  systems  which  are 
stable  enough  in  the  presence  of  water  not  to  decompose  this 
solvent  extensively. 

If  the  hydrogen  electrode  be  under  a  partial  pressure  of  hydro- 
gen less  than  one  atmosphere,  but  constant,  the  line  will  be  shifted 
upward  (calculation  by  equation  (21)).  The  successive  positions 
of  the  shifted  lines  in  the  figure  are  determined  by  hydrogen 
pressures. each  of  which  is  1/10,000  that  of  the  preceding. 

In  a  similar  manner  there  is  illustrated  the  shift  in  the  position 
of  the  line  of  the  oxygen  electrode  as  the  oxygen  pressure  declines 
in  steps  of  1/10,000  the  pressure  of  the  preceding  case.  (Calcula- 
tion by  equation  (22).) 

By  superimposing  figure  76  on  figure  77  it  is  possible  to  make  a 
formalistic  interpretation  of  the  potentials  of  the  various  systems 
in  terms  of  the  potential  of  either  an  oxygen  or  a  hydrogen 
electrode. 


XVIII  INTERRELATIONS  389 

It  has  already  been  indicated  that  such  an  interpretation  may 
be  highly  artificial. 

Now  each  curve  in  figure  76  is  for  the  half-reduced  state  of  the 
actual  system.  If  the  potential  becomes  more  negative,  the  per- 
centage reduction  of  a  given  system  increases  as  shown,  for  in- 
stance, by  figure  73.  To  attain  true  equilibrium  at  the  hydrogen 
electrode  the  methylene  blue  system,  for  instance,  would  first  have 
to  be  "completely"  reduced.  To  attain  true  equilibrium  at  a 
definite  one  to  one  ratio  of  methylene  blue  and  methylene  white 
both  hydrogen  and  oxygen  would  have  to  be  practically  elim- 
inated. 

The  reader  himself  can  carry  forward  the  further  interrelation- 
ships and  might  profitably  consider  the  interpretation  of  any 
electrode  potential  in  terms  of  any  one  of  the  systems.  He  might 
assume,  for  instance,  the  universal  presence  of  iron  (E0  =  0.75) 
and  interpret  all  potentials  in  terms  of  the  system  Fe+++  +  e 
^±  Fe++. 

The  practical  aspect  of  the  matter  is  this.  We  cannot  avoid 
the  possibility  of  other  systems  participating  when  we  set  up  an 
experiment  on  one.  Thus  with  a  platinum  electrode  immersed 
in  a  mixture  of  ferric  and  ferrous  ions  in  aqueous  solution,  we 
must,  strictly  speaking,  consider  the  following  oxidation-reduction 
systems:  Fe+++:Fe++;  H+:H2;  O2:OH-;  and  Pt++++:Pt.  How- 
ever, when  we  come  to  know  the  quantitative  values  of  the 
equilibrium  potentials  for  different  systems,  or  even  their  orders 
of  magnitude,  we  come  to  realize  that  the  ferric-ferrous  system 
by  interaction  with  water  or  water  constituents  or  with  chloride 
ions  in  a  ferrous-ferric  chloride  mixture  cannot  liberate  appre- 
ciable quantities  of  hydrogen,  oxygen  or  chlorine  and  that  the 
potential  of  the  system  is  incompatible  with  appreciable  amounts 
of  platinum  ions.  No  appreciable  energy  flows  into  the  transfor- 
mation of  these  systems  and  we  rest  content  that  we  are  con- 
cerned practically  with  only  the  energy  changes  of  the  system 
Fe++:Fe+++. 

In  general,  characteristic  data  for  one  system  should  be  ob- 
tained under  conditions  which  preclude  interference  by  another 
system. 

This  is  the  conclusion  we  anticipated  during  the  formulation 
in  the  first  instance.  The  quantitative  data  of  accuracy  suffi- 


390  THE   DETERMINATION   OF   HYDROGEN   IONS 

cient  for  the  purpose  may  be  found  in  the  compilation  by  Abegg, 
Auerbach  and  Luther  (1911-1915).     Cf.  Gerke  (1925). 

USE  OF  THE  GENERAL  RELATIONS  IN  DETERMINING  pH  VALUES 

Suppose  the  potential  of  an  electrode  were  stabilized  by  some 
definite  oxidation-reduction  system  which  involved  the  hydrion. 
As  one  instance  consider  a  system  to  which  there  applies  the 
equation 


Eh  =  E0  -         ln         +     j    in  [KlK2  +  Ei  [H+]  +  [H+?]  (36) 

If  there  were  no  interaction  of  oxidant  or  reductant  with  constitu- 
ents of  the  solution,  the  addition  of  the  oxidant  and  reductant  in 
a  one  to  one  ratio  would  leave 


Eh  -  Eo  +      -  In  [EiE.  +  E,  [H+]  +  [H+?]          (37) 
«v 

If  KI  and  K£  were  very  small  in  relation  to  [H+]  it  would  mean 
that,  while  this  relation  held,  the  acidic  nature  of  the  reductant 
would  not  be  brought  into  play  to  affect  the  acid-base  equilibrium 
of  the  solution.  Also  the  above  equation  would  then  reduce  to 


Eh  =  Eo  +    -  In  [H+]  (38) 

Jb 

If  we  may  assume  that  E0  has  been  evaluated  by  a  set  of  stand- 
ardizing measurements  with  known  values  of  [H+],  then  in  any 
other  case  a  determination  of  Eh  yields  the  value  of  [H+]. 

Chapter  XIX  will  be  devoted  to  such  cases. 

There  remains  a  possibility  not  yet  given  the  attention  it 
deserves. 

It  was  specified  above  that  the  oxidant  or  reductant  should  not 
react  with  other  reductants  or  oxidants  in  the  solution  and  thus 
suffer  a  change  in  ratio.  This  is  a  severe  limitation,  which,  as 
we  shall  see  in  a  later  chapter,  appears  less  prominently  in  prac- 
tice than  might  be  expected  because  of  the  slowness  of  certain 
oxidation-reduction  processes.  If  the  potential-controlling  system 
were  to  suffer  oxidation  or  reduction,  there  would  be  a  change  of 


XVIII  NEW   SYSTEMS   FOR   pH   MEASUREMENT  391 

potential  independent  of  a  change  in  pH.  In  many  cases  this 
means  that  protection  from  the  oxidizing  action  of  the  air  would 
have  to  be  provided.  In  all  cases  it  means  avoidance  of  the 
presence  of  any  oxidizing  or  reducing  agent  sufficiently  active 
to  appreciably  attack,  within  the  time  of  the  experiment,  either 
the  reductant  or  the  oxidant  employed.  This  does  not  mean 
that  any  oxidizing  or  any  reducing  agent  is  an  incompatible. 
Quite  the  contrary  will  reveal  the  still  unutilized  possibilities  in 
determining  the  dissociation  constants  of  very  active  oxidants  and 
reductants. 

Assume  for  instance  that  the  system  designated  by  Oxa:Reda 
is  to  be  employed  in  equimolecular  mixture.  Suppose  that  the 
potential  of  this  system  varies  linearly  with  pH.  Now  let  it  be 
applied  to  the  measurement  of  the  pH  values  of  solutions  con- 
taining the  reductant  of  a  system  designated  by  Redb:0xb. 

Were  the  characteristic  potential  of  the  "b"  system  negative 
to  that  of  the  "a"  system,  there  would  be  extensive  interaction 
between  the  "a"  and  "b"  systems.  The  reductant  of  the  "b" 
system  would  reduce  some  of  the  oxidant  of  the  "a"  system. 
The  extent  is  determined  by  the  relative  concentrations  and  also 
by  the  "spread"  between  the  "characteristic"  potentials  of  the 
two  systems. 

But  were  the  potential  of  the  "b"  system  positive  to  that  of  the 
"a"  system  the  reductant  of  the  "b"  system  could  not  act  ex- 
tensively upon  the  oxidant  of  the  "a"  system.  Therefore,  if  the 
"b"  system  were  used  in  an  extensively  reduced  condition  (prac- 
tically the  reductant  alone),  the  ratio  of  oxidant  to  reductant  in 
the  "a"  system  should  not  be  seriously  affected. 

How  seriously  remains  to  be  calculated  by  specific  assumptions. 

At  constant  pH  the  potentials  of  the  systems  separately  are 
defined  by 

Eha  =  Ea  -  0.03  log  (39) 


Ehb  =  E;-  0.03  log  (40) 

[bObJ 

The  systems  react  to  a  common  potential,  Eha  =  Ehb.  Hence: 

TT'  TT'  ^  no  1^  [Sra]  [Sob]  x.v 

E.  -  Eb  =  0.03  to  (41) 


392         THE  DETERMINATION  OF  HYDROGEN  IONS 

Let  Ea  =  0.15  volt  and  Eb  =  0.60  volt. 

Then 

[Sr>]  [Sob]  ,v 

[Soa][Srb]" 

Let  the  initial  concentrations  of  the  measuring  system  be  as 
low  as  [Sra]  =  [SoJ  =  10  ~4  while  of  the  measured  system  let 
[Srb]  be  as  high  as  1  normal,  initially.  In  changing  from  the 
initial  state  to  that  defined  by  (42)  x  moles  of  reductant  "b"  have 
reacted  with  x  moles  of  oxidant  "a"  to  increase  by  x  moles  the 
concentration  of  reductant  "a"  and  form  x  moles  of  oxidant  "b."6 

+  X]  [X] 


[10~4  -  x]  [1  -  x] 

An  approximate  solution  of  this  yields  a  value  of  x  very  nearly 
zero.  In  other  words  the  measuring  system,  "a,"  nas  n°t  been 
appreciably  affected. 

This  principle  is  tacitly  assumed  in  the  application  of  the 
hydrogen:  hydrion  system  to  the  measurement  of  pH  values  in 
solution  containing  a  reductant  of  another  oxidation-reduction 
system;  but  the  principle  should  be  applicable  generally,  and  not 
only  to  measurements  in  the  presence  of  reductants,  but  also  to 
measurements  in  the  presence  of  oxidants.  In  the  latter  case  the 
measuring  system  should  be  one  as  positive  as  can  be  selected. 

It  is  to  be  hoped  that  when  a  sufficient  variety  of  well  defined 
systems  are  available  the  principle  here  described  will  be  applied 
and  will  leave  no  excuse  for  an  ionization  constant  of  any  oxidant 
or  reductant  remaining  undetermined  when  its  value  is  of  appreci- 
able magnitude. 

For  an  example  see  Cannan  and  Knight  (1928). 


On  page  375  the  electromotive  force  of  a  cell  is  formulated  by 
use  of  the  postulate  that  the  escaping  tendencies  or  activities  of 
the  electrons  are  different  in  two  oxidation-reduction  systems. 
In  the  cell  these  two  oxidation-reduction  systems  are  placed  in 

6  For  simplicity  there  are  assumed  equivalent  valences. 


XVIII  SIGN   OF  ELECTRODE   POTENTIAL  393 

liquid  junction  with  an  intermediate  solution  which  can  be 
attacked  chemically  by  neither  oxidation-reduction  system  but 
which  will  permit  migration  of  ions.  We  assume,  for  sim- 
plicity, equality  of  ionic  migrations  and,  therefore,  no  potential 
difference  at  the  junction.  The  metallic  circuit  provides  a  path 
which  permits  electrons  but  not  ions  to  migrate  from  one  system 
to  the  other. 

The  introduction  of  a  path  through  which  electrons  alone  pass 
from  the  one  system  to  the  other  establishes  a  unidirectional 
electric  current.  If  the  current  is  not  entirely  restrained  it  will 
appear  that  this  path  (usually  a  metal)  has  the  more  negative 
potential  in  the  section  nearest  the  system  of  higher  electron 
escaping  tendency. 

With  this  scheme  it  becomes  a  convenience  to  give  to  the 
potential  of  an  electrode  the  sign  of  the  metal  as  found  in  a  cell 
made  up  of  the  given  electrode  and  the  standard  of  reference,  the 
normal  hydrogen  electrode. 

This  is,  I  am  told,  in  harmony  with  the  convention  to  be  used 
in  International  Critical  Tables. 

In  relating  a  cell  reaction  to  the  signs  of  the  cell  terminals  it  is 
convenient  to  argue  as  follows. 

The  system  Cl2:Cl~  has  a  much  greater  tendency  to  absorb 
electrons  (oxidize)  than  has  the  system  H2:H+  (which  is  the  re- 
ducing system  par  excellence.  An  indifferent  electrode  may  be 
thought  of  as  an  indicator  of  the  relative  ability  of  the  solution 
system  to  give  or  take  electrons.  It  is  charged  positively  by  an 
oxidizing  system  such  as  C12 :  Gh,  relative  to  the  charge  produced 
by  a  reducing  system  such  as  H2 :  H+.  The  extension  of  the  con- 
cept is  simple.  It  must,  of  course,  be  combined  with  some  con- 
vention regarding  the  way  of  writing  the  cell  reaction  in  cases 
which  are  not  obvious. 

When  a  cell  description  is  written  in  this  book,  it  will  be  written 
not  only  with  the  relatively  negative  metal  phase  at  the  left,  but, 
to  avoid  any  ambiguity,  each  sign  will  be  given  as  that  of  the 
exterior  lead  on  open  circuit,  the  open  circuit  being  the  ideal 
potentiometric  balance  as  if  against  a  condenser.  Thus 

-  Pt,  H2 1  HC1,  HgCl  |  Hg  + 

means  that  the  mercury  is  positive  relative  to  the  platinum  as  it 
would  be  found  to  be  at  potentiometric  balance.  The  reductant 


394  THE   DETERMINATION    OF   HYDROGEN   IONS 

(H2)  of  the  system  having  the  higher  electron  escaping  tendency 
releases  electrons  to  the  nearest  metal.  These  electrons  flow  in 
the  exterior  circuit  to  attack  the  oxidant  and  set  free  the  reductant 
(Hg)  of  the  system  with  the  lesser  electron  escaping  tendency. 

Lewis  and  Randall  in  Thermodynamics  adopt  "the  convention 
that  the  electromotive  force  given  shall  represent  the  tendency 
of  the  negative  current  to  pass  spontaneously  through  the  cell 
from  right  to  left."  (Thermodynamics,  p.  390.) 

They  write 

H2(g),  HC1  (0.1  M),  Cl2(g);  E  =  1.4885 
or 

Cla(g),  HC1  (0.1  M),  H2(g):  E  =  -1.4885 

When  they  represent  a  half-cell  such  as 

Hg  |  HgCl,  KC1  (0.1  N)  || 

they  state  the  order  electrode  |  electrolyte.  "We  then  say  that 
the  single  potential  measures  the  tendency  for  negative  elec- 
tricity to  pass  from  right  to  left."  When  they  write 

"D.E.;E  =  -0.3351" 

they  refer  the  potential  of  the  "decinormal  electrode"  to  the 
normal  hydrogen  electrode  by 

Hg  |  HgCl,  KC1  (0.1  N)  ||  H+  (activity  1)  |  H2  (1  atmos.)  Pt 

and,  since  the  negative  current  goes  from  left  to  right  through 
the  cell  as  written,  the  negative  sign  is  given,  as  above. 

As  a  consequence  it  is  found  that  the  signs  given  to  single 
electrode  potentials  by  Lewis  and  Randall,  and  by  many  who 
adopt  their  convention,  are  opposite  to  those  used  in  this  book. 

We  could  use  the  system  of  Lewis  and  Randall  by  writing,  for 
instance, 

||  KC1  (0.1  N),  HgCl  |  Hg;  E  =  0.3351 
instead  of  their 

Hg  |  HgCl,  KC1  (0.1  N)  ||  ;  E  =  -0.3351 

Although  this  will  frequently  be  done  we  here  ignore  the  order 
and  use  the  following  convention.  The  sign  of  an  electrode 


XVIII  FINITE  EATIOS  395 

potential  of  a  given  half-cell  shall  be  the  sign  of  the  potential  of 
its  metal  relative  to  that  of  the  metal  of  the  normal  hydrogen 
half-cell. 

For  interesting  discussions  of  the  sign  of  electrode  potentials 
see:  Lewis  and  Randall  (1923),  Porter  (1924)  and  Transactions 
American  Electrochemical  Society  31,  249;  33,  85;  34,  196. 

ON   FINITE   RATIOS 

In  any  case  where  a  definite  potential  difference  is  to  be  established  at 
the  electrode  there  must  be  in  the  system  two  species,  one  of  which  is  the 
direct  or  indirect  reduction  product  of  the  other,  and  the  ratio  of  their 
concentrations  or  activities  must  be  of  finite  magnitude.  Neglect  of  this 
principle  is  not  infrequent,  and  is  doubtless  due  to  the  emphasis  which  has 
been  placed  upon  the  final,  working-form  of  the  equation  for  the  differ- 
ence of  potential  between  a  metal  and  a  solution  of  its  ions.  See  equation 
(20)  page  381 .  In  obtaining  the  final  form  of  this  equation  certain  assump- 
tions have  been  made  and  the  potential-difference  at  the  electrode  is  made 
to  appear  as  if  it  were  dependent  only  upon  the  concentration  of  one 
species,  namely  the  metal  ions.  Whether  this  be  the  explanation  or  not, 
there  are  not  infrequently  encountered  in  the  literature  attempts  to 
measure  electrode  potential  differences  with  a  single  oxidant  or  reductant. 
It  should  be  plain  from  a  study  of  figure  73  that,  when  the  oxidant  or  re- 
ductant alone  is  present,  the  electrode  potential-difference  becomes 
asymptotic  to  the  Eh  axis.  Were  it  possible  to  eliminate  absolutely  every 
trace  of  the  oxidant,  the  potential-difference  obtained  with  the  reductant 
alone  would  tend  to  become  infinite. 

When  we  meet  such  a  prediction  in  an  equation  we  should  be  suspicious. 
Perhaps  for  the  potential  produced  by  a  pure  reductant  or  by  a  pure 
oxidant  there  is  an  inherent  limitation  of  a  kind  not  implied  by  the  equation 
which  rests  upon  the  assumption  of  a  reversible  system.  On  the  other 
hand  the  general  treatment  implies  the  following. 

The  potential  could  not  become  infinite  for  two  reasons.  In  solution  an 
infinitesimal  reaction  with  the  solvent  would  prevent  it.  Second  the 
production  of  a  pure  reductant  could  not  be  attained  in  a  world  which  has 
suffered  extensive  interactions  of  its  components  unless  there  were  created 
de  novo  another  reducing  reagent  belonging  to  a  system  of  infinite  nega- 
tive potential  or  unless  there  were  created  de  novo  an  absolutely  pure  re- 
ducing agent  which  could  be  the  reductant  of  a  low  potential  system  if  it 
were  employed  in  infinite  mass. 

Wherever  stable  potentials  are  reported  as  having  been  found  with  re- 
ductant alone  it  is  doubtless  due  to  the  presence  of  the  oxidant  as  an 
impurity. 

While  there  may  be  no  rigid  proof  of  the  statements  made  above  they 
are  implicit  in  the  equations.  Whatever  their  limitations,  they  have 
several  practical  implications. 


396  THE    DETERMINATION    OF    HYDROGEN    IONS 

So  far  as  mere  formulation  is  concerned  it  should  be  possible  to  attain 
the  electrode  potential  of  the  system  metal-metal  ion  by  means  of  an  un- 
attackable  metal  immersed  in  a  solution  of  the  metal  ions,  provided  the 
saturation  value  of  the  metal  were  maintained  by  a  piece  of  the  metal 
placed  elsewhere.  The  system  metal-metal  ion  is  a  special  -case  of  an 
oxidation-reduction  system  which  should  be  measurable  in  the  ordinary 
way.  The  difficulty  would  be  in  maintaining  between  the  metal  serving 
merely  as  electrode  and  the  metal  serving  merely  as  saturator  a  sufficiently 
fast  diffusion  of  the  almost  insoluble  metal  molecules  to  maintain  a  finite 
ratio  of  oxidant  to  reductant  at  the  electrode.  For  this  reason  the  only 
practical  way  is  to  make  the  electrode  of  the  metal  itself  or  to  have  it 
present  at  the  electrode  in  appreciable  quantities,  as  in  the  case  of  an 
amalgam  electrode.  Otherwise  the  inevitable  impurities,  such  as  hydrogen 
or  oxygen,  of  the  "unattackable"  electrode  would  make  it  behave  as  a 
more  or  less  indefinite  hydrogen,  oxygen  or  other  kind  of  electrode. 

By  the  same  token  a  system  which  does  not  reversibly  maintain  a  finite 
ratio  of  oxidant  and  reductant,  leaves  the  electrode  functioning  in  an 
almost  uninterpretable  manner.  Irrespective  of  what  can  be  done  under 
such  circumstances,  the  recognition  of  this  fact  leads  to  skepticism  re- 
garding all  measurements  which  cannot  satisfy  the  requirements  of  the 
equations  on  introduction  of  known  components.  There  is  ample  room 
and  frequent  occasion  for  bold  adventure  in  the  use  of  electrode  measure- 
ments, especially  in  the  study  of  so-called  irreversible,  organic  oxidation- 
reduction  systems;  but,  unless  the  equations  can  be  satisfied  by  the  intro- 
duction of  known  components,  one  should  warn  his  reader  that  he  is  ad- 
venturing and  that  he  is  not  citing  definitive  data. 

FREE   ENERGY   CHANGES 

Since  the  validity  of  Faraday's  law  is  assumed  and  measurements  of 
cells  are  measurements  of  electromotive  force,  it  has  been  convenient  to 
separate  Eh  and  to  place  nF  on  the  other  side  of  the  equation.  However, 
nFE  is  the  free-energy  change  in  volt-coulombs.  Therefore,  all  the  electro- 
motive force  equations  permit  the  calculation  of  the  free  energy-change, 
—  AF,  from 

-AF  =  nFE  (43) 

It  is  unnecessary  to  repeat  all  the  equations  in  the  new  form;  but  one  case 
will  be  instructive.  Consider  equation  (32)  page  383  and  rewrite  it  as: 

r«      -1 

-  AF  =  2FEh  =  2FE0  -  RT  In  ^  +  RT  In  [KiK,  +  Ki  [H+]  +  [H+]2]    (44) 

|koj 

The  employment  of  Eh  signifies  (by  subscript  h)  reference  to  the  "normal 
hydrogen  electrode."  For  simplicity  we  shall  consider  this  to  be  a  hydro- 
gen electrode  in  a  solution  of  unit  hydrion  concentration  under  one  atmo- 
sphere pressure  of  H2.  Therefore,  the  processes  to  be  discussed  involve 
reference  to  this  standard  hydrogen  system. 


XVIII  FREE   ENERGY   CHANGES  397 

We  shall  assume  that  KI  and  K2  have  such  values  that  [H+]  can  be  made 
either  large  or  small  with  relation  to  either. 

Let  it  be  assumed  in  all  cases  that  [SR]  =  [S0]  =  1.  Then  equation  (44) 
can  be  written 

-AF  =  2FE0  +  RT  In  [KiK,  +  Kj  [H+]  +  [H+]»]  (45) 

First  make  [H+]  large  in  relation  to  KI  and  K2.  Then  we  have  prac- 
tically 

-A*1!  =  2FE0  +  2RT  In  [H+]  (46) 

When  [H+]   =    1  we  have 

-AF2  =  2  FE0  (47) 

There  is  implied  the  suppression  of  the  dissociation  of  the  reductant. 
Hence  (47)  gives  the  free  energy  of  the  process 

(1  atmos.) 
S0  +  H2  ;=±  SR  (hydrogenated)l 

(48) 
Ox  +  H2  ^±  H2Red  J 

For  any  value  of  [H+]  other  than  1,  equation  (46)  gives  not  only  the 
free  energy  of  the  process  (48)  but  the  free  energy  of  transport  of  hydrions 
from  the  standard  solution  to  any  value  of  [H+J.  See  (49) 

-AFi  +  AF2  =  2RT  In  [H+]  (49) 

Second,  make  [H+]  small  in  relation  to  KI  and  K2.  Then  (45)  is  prac- 
tically 

-AF3  =  2FE0  +  RT  In  KiK2  (50) 

Subtract  (47)  from  (50) 

-AF3  +  AF2  =  RT  In  KiK2  (51) 

tH+P  [Red"] 

[H2Red] 
Hence 

' 


Equation  (52)  gives  the  free  energy  of  the  process 

H2Red  -»  2H+  +  Red"  -  (53) 

This  is  the  free  energy  of  ionization  which,  by  the  use  of  [H+]  =  1  in 
the  derivation,  is  the  energy  which  would  have  to  be  expended  to  accom- 
plish ionization  against  a  normal  concentration  of  hydrions.  Likewise  the 
free  energy  of  the  separate  ionizations  can  be  formulated. 


398         THE  DETERMINATION  OF  HYDROGEN  IONS 

When  the  hydrion  concentration  is  lowered  ionization  takes  place 
spontaneously.  This  condition  is  met  when  the  free  energy  of  hydrion 
transport,  between  IN  and  the  normality  permitting  practically  complete 
ionization,  compensates  the  energy  which  would  have  to  be  expended  on 
the  system  to  cause  ionization  at  1  N  H+. 

In  short,  our  equations  contain  implicitly  the  free  energies  of  ioniza- 
tion and  what  may  be  called  rather  inexactly  the  free  energy  of  hydrion 
dilution. 

SOME   REMARKS   ON   MECHANISM 

It  was  stated  early  in  this  chapter  that  the  use  of  the  electron-transfer 
concept  was  to  be  a  formality  and  a  convenience;  and,  although  it  may 
have  been  stressed  here  and  there  in  a  manner  which  betrayed  the  author's 
preference  for  the  concept  as  a  picture  of  actuality,  it  remains  a  formality. 
The  satisfaction  of  the  resulting  equations  is  no  proof  of  the  validity  of 
the  postulate,  for  it  was  made  clear  that  there  are  several  other  ways  in 
which  the  equations  could  be  derived.  Also  the  equations  are  of  thermo- 
dynamic  origin,  and,,  although  mechanistic  ideas  were  introduced  both 
to  clarify  the  subject,  and  to  make  general  equations  specific,  the  fulfill- 
ment of  a  thermodynamic  relation  cannot  per  se  throw  any  light  on  mech- 
anism. 

It  has  been  repeatedly  stated  that  the  strength  of  thermodynamics  is 
its  independence  of  mechanistic  concept.  This  is  because  the  energy 
change,  which  a  thermodynamic  equation  may  formulate,  is  independent 
of  the  path.  The  thermodynamic  method  per  se  has  nothing  to  say  about 
conditions  which  might  make  the  change  take  one  path  rather  than  another. 
Yet  in  this  chapter  we  have  made  rather  free  use  of  certain  mechanistic 
concepts.  This  is  because  we  have  to  face  the  following  situation.  If  free 
energy  change  is  to  be  formulated,  all  that  thermodynamics  offers  is  an 
equation  for  a  process.  The  methods  of  general  chemistry  must  be  used 
to  give  some  idea  of  specific  components  to  be  used  in  the  practical  solution; 
otherwise  the  experimentalist  is  not  equipped  to  handle  the  process.  The 
innumerable  methods  of  formulating  cell  reactions  thermodynamically 
have  been  advanced  after  the  cells  have  been  devised. 

In  all  cases  some  molecular  theory  is  introduced.  So  it  was  that  we 
found  ourselves  specifying,  for  instance,  that  a  reductant  can  take  the 
form  H2Red,  HRed"  or  Red"  ~.  Were  the  theory  of  electrolytic  dissocia- 
tion in  disrepute  this  would  be  considered  horribly  mechanistic. 

In  general  we  find  ourselves  dealing  with  relations  which  take  the  form 
of  the  thermodynamic  equation  but  in  which  we  have  introduced  molecular 
theory.  This  introduction  carries  with  it  not  only  the  truth  of  our  molecu- 
lar theory  but  its  assumptions.  When  we  put  the  true  and  the  assumed 
into  the  mathematical  mill  the  mill  grinds  out  in  new  and  often  startling 
form  only  what  is  put  in.  Many  of  the  consequences  are  very  alluring  and 
it  behooves  us  to  be  on  guard. 


XVIII  MECHANISM  399 

It  has  been  shown  above  that  whether  we  start  with  the  orienting 
reaction 

Ox  +  2e  ^  Red-  ~ 
or  Ox  +  H2  ^  H2Red 

we  attain  the  same  final  working  equation  which  in  this  case  is: 
Eh  =  E0  -  H  In  !jg  +  g  In  [K,K2  +  K,  [Hi  +  pi*].] 

Let  us  disregard  implied  electrode  mechanism  and  consider  this  last  equa- 
tion as  an  empirical  one  which  correctly  formulates  experimental  facts. 
We  then  still  imply  solution  processes  such  as 


i  H+  +  HRed- 
and  HRed- ;=±H+  + Red- - 

In  the  preceding  section  it  was  shown  that  the  equation  involves  the 
free  energies  of  ionization  and  of  hydrion  "dilution."  It,  therefore, 
appears  that  a  choice  between  the  orienting  reactions 

Ox  +  2€;=±  Red~~ 
and  Ox  +  2e  +  2H+  ^±  H2Red 

(the  latter  being  formally  equivalent  to 
Ox    +  H2  =  H2Red 

is  somewhat  like  the  choice  permissible  in  measuring  the  height  of  a  ladder. 
We  may  measure  from  the  bottom  up  or  from  the  top  down.  We  may 
measure  the  total  free  energy  change  by  counting  in  the  free  energy  of 
ionization  from  one  direction  or  the  other.7 

But  suppose  there  is  under  consideration  an  oxidation-reduction  system 
the  reductant  of  which  can  take  either  the  form  HRed  or  Red".  While  we 
may  have  properly  formulated  the  free  energy  change  for  the  formation  of 
one  or  the  other  or  both,  it  might  well  be  that  the  species  Red"  is  effective 
in  the  electrode  phenomena  and  that  the  species  HRed  is  not  effective  or 
that  HRed  is  effective  and  Red"  not.  Now  let  the  dissociation  constant, 
Ka,  of 

[H+][Red-] 
[H  Red]          Ka 


7  Dixon  (1927)  chooses  his  position  at  the  top  of  the  ladder  and  leaves 
the  impression  that  this  has  something  to  do  with  the  argument  of  Cohen, 
Gibbs  and  Clark  (1924),  which,  of  course,  it  has  not.  See  pages  402, 
521  and  Studies  on  oxidation-reduction,  V.  (Clark  et  al.). 


400        THE  DETERMINATION  OF  HYDROGEN  IONS 

have  the  value  10~13.    The  ratio  — —  —  would  be  1  at  pH  =  13  while  at 

[Hrveclj 

pH  =  0  the  ratio  would  be  10~13.  A  thousandth  normal  solution  would 
contain  the  species  Red"  at  only  about  10"16  normality.  If  we  choose  to 
say  that  this  species  is  the  exclusively  active  reductant  we  have  to  account 
for  physical  effectiveness  at  10~16  N.  The  discussion  now  joins  with  the 
remarks  on  page  372  concerning  the  assumed  functioning  of  the  electrode 
as  a  hydrogen  electrode  in  a  ferric-ferrous  ion  solution.  We  found  there 
but  one  of  many  instances  of  the  physically  absurd  values  encountered 
when  restricted  points  of  view  and  restricted  methods  of  expressing  relations 
are  applied  to  electrode  potential  differences.  One  or  two  other  instances 
will  be  given. 

Lehfeldt  (1899)  says  of  the  so-called  solution  pressures  postulated  by 
Nernst  and  briefly  discussed  in  Chapter  XII: 

" we  have  Zinc 9.9  X  1018 

Nickel 1.3  X  10° 

Palladium 1.5  X  10~36 

The  first  of  them  is  startlingly  large.    The  third  is  so  small  as  to  involve 

the  rejection  of  the  entire  molecular  theory  of  fluids." 

Lehfeldt  then  shows  that,  in  order  to  permit  at  the  electrode  the  pres- 
sure indicated  above  for  palladium,  the  solution  would  have  to  be  so 
dilute  as  to  contain  but  one  or  two  ions  of  palladium  in  a  space  the  size  of 
the  earth.  No  stable  potential  could  be  measured  under  such  a  circum- 
stance. On  the  other  hand  Lehfeldt  calculates  that  to  produce  the  high 
pressure  indicated  for  zinc  ''1.27  grams  of  the  metal  would  have  to  pass 
into  the  ionic  form  per  square  centimeter,  which  is  obviously  not  the  case." 

Another  aspect  of  the  matter  was  emphasized  in  a  lively  discussion  be- 
tween Haber,  Danneel,  Bodlander  and  Abegg  in  Zeitscrift  fur  Elektro- 
chemie,  1904.  Haber  points  out  that,  if  the  well  established  relation 
between  a  silver  electrode  and  a  solution  containing  silver  ions  be  extra- 
polated to  include  the  conditions  found  in  a  silver  cyanide  solution,  the 
indicated  concentration  of  the  silver  ion  will  be  so  low  as  to  have  no  phys- 
ical significance.  Haber  mentions  the  experiment  oi  Bodlander  and  Eber- 
lein  where  the  potential  and  the  quantity  of  solution  were  such  that  there 
was  present  at  any  moment  less  than  one  discrete  silver  ion.  The  greater 
part  of  the  discussion  centred  upon  the  resolution  of  the  equilibrium 
constant  into  a  ratio  of  rates  of  reaction,  and  upon  the  conclusion  that, 
if  the  silver  ion  in  the  cyanide  solution  has  a  concentration  of  the  order 
of  magnitude  calculated,  it  must  react  with  movements  of  a  speed  greater 
than  that  of  light  or  else  that  the  known  reactions  of  silver  in  silver  cyanide 
must  take  place  directly  from  the  position  in  the  complex.  Previous  ioniza- 
tion  is  then  unnecessary.  Were  the  latter  assumption  not  true,  how  could 
the  stability  of  the  electrode  potential  be  supported? 

A  similar  question  was  raised  but  not  answered  in  a  discussion  between 
Langmuir  and  Patten  printed  in  Trans.  Am.  Electrochem.  Soc.  29,  (1916) 


XVIII  MECHANISM  401 

pp.  293  and  296.  It  concerned  the  hydrogen  electrode  operating  in  a  solu- 
tion of  hydrion  concentration  of  10~10  normal.  Whatever  the  validity  of 
the  conclusion  that  so  and  so  much  free  energy-change  is  involved  in  the 
transfer  of  hydrions  from  one  normal  to  10~l°  normal,  is  such  a  low  con- 
centration physically  effective? 

These  matters  may  be  somewhat  clarified  if  we  return  to  a  consideration 
of  the  oxidation-reduction  systems  noted  above. 

Here  are  systems  in  the  description  of  which  there  are  included  the 
free  energies  of  complex  formations,  i.e.,  the  formation  of  the  undissociated 
acids  or  bases  from  their  ionization  products.  By  analogy,  there  should 
be  included  in  the  description  of  the  silver  system  the  free  energy  of 
formation  of  the  silver  cyanide  complex.  By  the  neglect  of  this  aspect, 
the  chosen,  orienting  reaction 

Ag+  +  e  ^  Ag 

has  been  raised  to  an  importance  to  which  it  is  not  entitled.     It  is  because 

of  emphasis  upon  this  orienting  reaction  that  there  has  been  created  the 

puzzle  mentioned  above. 

But  there  still  remains  a  real,  mechanistic  problem.    The  only  answer 

that  appears  plausible  is,  as  mentioned  above,  that  the  silver  cyanide 

acts  directly. 

Thus  Br0nsted  (1926),  in  discussing  a  similar  situation,  remarks: 
"Nernst's  formula  often  leads  to  absurd  ion  concentrations — for  instance 

in  the  case  of  a  copper  electrode  in  a  potassium  cyanide  solution — and  it 

seems  unreasonable  to  assume 

metal  ;=±  metal  ion  +  electron 

In  such  circumstances,  and  in  general,  the  potential  between  electrode 
and  solution  might  be  denned  by  means  of  more  direct  reactions.  For  the 
copper-copper  cyanide  system  we  might  have: 

Cu  +  Cn~  ^  CuCn  +  « 
or  Cu  +  2Cn~  ^±  Cu(Cn)2  +  2e." 

In  the  case  of  the  oxidation-reduction  systems  which  we  have  discussed 
there  are  cases  in  which  the  reductant  has  high  dissociation  constants 
and  cases  in  which  it  has  low  dissociation  constants.  If,  in  either  case, 
the  effectiveness  of  the  reductant  were  dependent  on  but  one  form,  rapidity 
in  the  attainment  of  electrode  potential  would  not  be  expected  over  the 
entire  range  of  the  enormous  variation  in  hydrion  concentration  used 
experimentally.  Thermodynamics  has  nothing  to  say  on  this  matter  of 
rapid  attainment  of  equilibrium.  The  fact  is  that  no  significant  variation 
from  a  nearly  instantaneous  adjustment  is  observed. 

In  these  same  cases,  analysis  suggests  that  two  equivalents  are  con- 
cerned in  the  oxidation-reduction  process.  So  far  as  thermodynamics  is 
concerned  it  is  ready  to  provide  equations  for  the  transfer  of  the  equiva- 


402        THE  DETERMINATION  OF  HYDROGEN  IONS 

lents  either  together  or  separately  and  step-wise.  Experiment  (in  the 
cases  under  consideration)  reveals  no  trace  of  step-wise  reduction! 

Not  all  oxidation-reduction  processes  are  amenable  to  study  by  the 
electrode  method.  So  far  as  thermodynamics  is  concerned  it  is  able  to 
provide  a  formulation  of  the  free  energy  of  reduction  in  terms  of  volt- 
coulombs  or  of  calories.  It  is  incapable  of  predicting  what  systems  are 
and  what  systems  are  not  amenable  to  study  by  the  electrode  method. 
The  fact  that  in  the  cases  under  consideration  there  can  be  generated 
an  electric  current  and  that  presumably  electrons  are  sent  into  the  measur- 
ing system,  must  have  a  significance  to  mechanism.  Cohen,  Gibbs  and 
Clark8  (1924)  argued  from  these  non-thermodynamic  aspects  that  the  essen- 
tial or  determinative  factor  is  the  pairing  of  electrons  in  the  molecule  and 
the  impossibility  of  passing  from  reductant  to  oxidant  without  breaking 
the  original  structure  with  the  transfer  of  an  electron  pair  (in  the  specific 
cases  they  discuss). 

In  emphasizing  this  aspect  they  stated  that  the  question  of  hydrogen- 
ation  was  an  incidental  matter  depending  on  the  hydrion  concentration  of 
the  solution  and  the  dissociation  constant  of  the  reductant.  There  might 
have  been  an  inference  of  a  division  in  time  between  transfer  of  electrons 
and  transfer  of  protons.  This  and  a  misunderstanding  of  the  nature  of 
the  argument  evidently  threw  Dixon  (1927)  completely  off  the  theme  and 
led  to  his  placing  undue  emphasis  upon  one  special  formulation  the  particu- 
lar nature  of  which  was  pointed  out  in  the  previous  edition  of  this  book 
and  by  Clark  (1923).  The  inference  of  separate  steps  divided  in  time  is 
not  essential  to  the  conclusion  which  has  to  do  with  the  determinative 
as  distinct  from  the  incidental  processes  convenient  to  use  in  formulations. 

It  will  readily  be  perceived  that  the  non-thermodynamic  dimensions  of 
molecular  theory  have  been  used  in  the  argument  on  mechanism.  loniza- 
tion,  pairing  of  equivalents,  an  electrical  phenomenon,  statistical  num- 
bers, etc.,  are  the  subjects  discussed. 

The  resulting  picture  is  laden  with  assumptions  and  some  of  these  are 
important  to  the  main  subject  of  this  book. 

The  greater  part  of  the  troubles  mentioned  arise  from  trying  to  get 
more  out  of  the  mathematical  mill  than  we  put  into  it.  When  we  put  into 
the  mill  an  assumed  mechanistic  relation  (as  we  eventually  must  to  bring 
thermodynamics  from  its  ethereal  heights  to  deal  with  material  problems) 
we  shall  get  out  so  much  of  the  truth  and  so  much  of  the  limitations  as  are 
inherent  in  the  assumption.  Since  mechanistic  concepts  are  based  not 
on  rigid  arguments  but  are  attempts  to  harmonize  a  picture  drawn  with 
imperfect  knowledge,  there  should  be  on  the  one  hand  no  hesitancy  in 
artistic  efforts  toward  harmony,  and,  on  the  other  hand  no  disposition  to 
impose  the  artistry  where  it  serves  no  good  purpose. 

We  suggest  the  direct  action  of  undissociated  molecules  in  phenomena 
usually  attributed  to  ions  only.  It  should  not  be  forgotten  that  this  does 
not  place  the  two  kinds  of  species  on  a  parity.  Thermodynamically  they 

8  Clark  et  al. 


XVIII  MECHANISM  403 

differ  by  the  energy  of  formation  of  the  one  from  the  others.  There  is  no 
inherent  reason  for  undue  emphasis  upon  the  transcendent  importance  of 
ions  as  participants  in  chemical  reaction.  There  is  every  reason  for 
utilizing  the  distinction,  noted  above,  in  the  free  energy-changes. 

From  the  foregoing  discussions  it  should  be  evident  that  the  designation 
of  a  particular  electrode-solution  system  depends  so  far  as  convenience  is 
concerned  upon  relations  which  we  seek,  it  being  more  convenient  in  some 
instances  to  formulate  all  data  in  terms  of  hydrogen  electrode  potentials 
and  in  other  instances  in  terms  of  reduction  potentials.  So  far  as  the 
actual  physical  maintenance  of  electrode  conditions  is  concerned  the 
designation  of  an  electrode  as  of  one  or  the  other  type  will  certainly  depend 
upon  a  finite  ratio  of  two  products,  one  of  which  is  the  reduction  product  of 
the  other;  but  the  discovery  of  what  these  species  are  is  often  a  most  diffi- 
cult problem  for  the  solution  of  which  the  electrode  equations  by  them- 
selves and  thermodynamics  by  itself  are  not  sufficient.  Here  the  methods 
of  general  chemistry  must  be  employed.  Here  also  are  pitfalls.  Never- 
theless, in  the  end,  the  strength  of  the  accumulating  information  will 
doubtless  be  found  to  be  not  in  the  purely  thermodynamic  contributions 
alone  nor  in  the  purely  statistical  contributions  alone  but  in  harmonious 
union. 


CHAPTER  XIX 

THE    QUINHYDRONE   AND    SIMILAR   HALF-CELLS 

A  half-cell  which  has  won  favor  as  a  convenient  device  with 
which  to  determine  hydrion  activity  is  the  so-called  quinhydrone 
electrode.  Its  development  has  been  due  largely  to  the  work  of 
Biilmann  and  his  collaborators.  See  the  re'sume'  by  Biilmann 
(1927). 

A 


PH  " 
FIG.  78.  RELATION  OF  ELECTRODE  POTENTIAL,  Eh,  TO  pH 

QQ,  Quino -quinhydrone  electrode;  Q,  quinhydrone  electrode;  C,  chlor- 
anil  electrode;  HQ,  hydro -quinhydrone  electrode.  Potential  of  saturated 
KC1  calomel  electrode  shown  by  S. 

Structurally  the  half -cell  is  very  simple.  An  "unattackable" 
metal,  such  as  gold  or  platinum,  serves  as  electrode  proper.  The 
solution  to  be  examined  is  saturated  with  quinhydrone.  To 
complete  a  cell,  the  quinhydrone  half-cell  may  be  put  in  liquid 
junction  with  a  calomel  half-cell,  with  a  standard  hydrogen  half- 
cell,  or  with  another  quinhydrone  half-cell  in  which  the  solution 
is  a  standard  buffer. 

See  page  259  and  figure  78  for  graphs  showing  the  relation  of 
the  potential  to  pH. 

404 


XIX 


THEORY   OF   QUINHYDRONE   ELECTRODE 


405 


THEORY 

Quinhydrone  is  a  peculiar  complex  formed  of  equimolecular 
proportions  of  quinone  and  hydro quinone.1  The  first  is  the 
"oxidation  product"  of  the  second.  We  shall  first  regard  the 
quinhydrone  as  furnishing  equimolecular  concentrations  of  an 
oxidant  and  reductant. 

Whatever  may  be  the  actual  mechanism  by  which  the  one  is 
transformed  into  the  other,  we  may,  for  present  purposes,  assume 
two,  reversible,  main  steps,  of  which  the  second  and  not  the  first 
is,  in  turn,  stepwise. 

O  0- 


quinone  +  2  electrons 


anion  of  hydroquinone 


anion  of  hydroquinone  -f  2  H+  ^±  hydroquinone 
(stepwise) 

The  approximate  equation  for  such  a  system  was  developed  in 
Chapter  XVIII.  Its  development  need  not  be  repeated;  but  it 
may  be  noted  that  in  writing  the  sum  of  all  forms  of  reductant 
and  oxidant  we  should  include  the  dissolved,  undissociated 
quinhydrone,  Q.  Then  the  equation  is: 


1  Strictly  speaking  we  should  speak  of  benzoquinone  and  benzohydro- 
quinone,  since  the  terms  "quinone"  and  "hydroquinone"  have  generic 
as  well  as  specific  meanings. 


406  THE   DETERMINATION    OF   HYDROGEN    IONS 

Here  Eh  is  the  observed  potential  referred  to  the  normal  hydrogen 
electrode,  E0  is  the  characteristic  constant  of  the  system,  [SR] 
and  [S0]  are,  respectively,  the  concentrations  of  total  reductant 
and  total  oxidant,  [Q]  is  the  concentration  of  dissolved,  undis- 
sociated  quinhydrone  and  KI  and  K2  are  the  dissociation  constants 
of  the  reductant.  The  first  dissociation  constant  of  hydro- 
quinone  is  of  the  order  of  10~10  and  the  second  is  somewhat  lower. 
Consequently  at  pH  8  the  compound  is  only  about  1  per  cent 
dissociated,  at  pH  7  about  0.1  per  cent  dissociated  and  from  then 
on  through  the  lower  values  of  pH  it  can  be  considered  for  certain 
purposes  as  completely  in  the  undissociated  form.  By  referring 
directly  to  equation  (1)  we  see  that,  when  [H+]  is  large  (over  10~8 
for  approximate  limit)  compared  to  KI  and  K2  the  sum  in  the 
last  term  reduces  practically  to  the  value  of  [H+]2.  Hence,  with 
an  approximation  that  the  better  approaches  the  truth  the  higher 
the  value  of  [H+],  we  may  write  the  last  term: 


Assuming  [SR]  —  [Q]  =  [S0]  —  [Q],  we  have 

RT 

Eh  =  Eo  +  -^  In  [H+]  (2) 

r 

At  25°C.,  for  instance,  (2)  would  be: 

Eh  =  Eo  -  0.05912  pH  (3) 

The  above  was  stated  in  terms  of  concentrations  for  the  sake 
of  deriving  the  approximate  equation  and  showing  why  alkaline 
solutions  should  be  avoided  if  (2)  is  to  be  applied.  The  ap- 
proximation also  serves  another  purpose.  It  indicates  that 
if  we  are  content  to  operate  in  acid  solutions  we  may  simplify  the 
development  of  the  more  exact  equation  which  is  to  be  in  terms 
of  activities. 

For  the  reaction 

Quinone  +  2  H+  +  2  e^±  Hydroquinone 

(quinone)  (H+)2  (e)2  _  R 
(hydroquinone) 


XIX  QUINO-   AND    HYDROQUINHYDRONE    ELECTRODE  407 

Solve  for  (e)  and  introduce  in  equation  15  of  Chapter  XVIII. 


Eh  _  Eo  _         ln  (hydroquinone)  fa 

2F  (qumone) 

[Note:  In  this  book  activities  are  denoted  by  ()  while  concentra- 
tions are  denoted  by  [].] 
For  the  equilibrium  in  the  reaction 

quinone  +  hydroquinone  ^±  quinhydrone 
we  may  write: 

(qumone)  (hydroquinone)       ,r  /rN 

—f  —  .  ,     ,  --  ^—   —  =  Kq  (5; 

(quinhydrone) 

But,  since  (quinhydrone)  is  a  constant  when  the  solid  phase  is 
present, 

(quinone)  (hydroquinone)  =  Kqa  (6) 

Now  consider  the  case  when  there  is  added  to  the  quinhydrone 
in  solid  phase  either  quinone  or  hydroquinone  to  keep  the  solu- 
tion saturated  with  two  of  the  three  substances.  Then,  in  addi- 
tion to  constancy  in  the  activity  of  quinhydrone  which  establishes 
(6),  one  of  the  variables  in  (6)  is  made  constant  and  hence  the 
other  must  be. 

We  need  not  know  the  values  of  (quinone)  or  (hydroquinone) 
to  know  that  equation  (4)  will  be  reduced  to  : 


Eh  =  EQq  +        In  (H+)  (7) 

JB 

when  quinone  and  quinhydrone  are  the  solid  phases.  This  then 
is  the  equation  for  the  system  which  Biilmann  and  Lund  (1921) 
call  the  quino-quinhydrone  electrode. 

Likewise  when  hydroquinone  and  quinhydrone  are  the  solid 
phases  equation  (4)  reduces  to: 


Eh  =  Ehq  +        In  (H+)  (8) 

Jj 

This  is  the  equation  for  the  so-called  hydro-quinhydrone  electrode. 
The  values  of  Eqq  and  Ehq  may  be  established  independently 


408  THE    DETERMINATION    OF   HYDROGEN    IONS 

by  a  procedure  similar  to  that  noted  in  determining  the  charac- 
teristic constant  of  the  quinhydrone  electrode. 

It  is  to  be  particularly  noted  that  the  only  variable  remaining 
at  the  right  of  equations  (7)  and  (8)  is  (H+).  Therefore,  in  the 
sense  that  nothing  that  can  effect  the  activities  of  the  quinone, 
hydroquinone  or  quinhydrone  will  affect  the  potential,  these 
electrodes  are  said  to  be  "  without  salt  effect."  There  will  be  less 
chance  of  misunderstanding  if  we  say  that,  if  these  electrodes 
and  the  hydrogen  electrode  at  constant  pressure  respond  only  to 
changes  of  (H+)  their  potentials  should  run  parallel.  Within  the 
limits  of  experimental  error  it  seems  to  have  been  demonstrated 
that  they  do. 

When  quinhydrone  is  the  only  component  of  the  solid  phase 
the  situation  is  not  so  easily  simplified.  We  cannot  assume 
equality  of  the  activities  :  (hydroquinone)  and  (quinone)  ;  but  we 
may  assume  equality  of  the  concentrations  [S0]  and  [Sr],  the  total 
oxidant  and  the  total  reductant  in  solution.  But,  in  acid  solution, 

1       (hydroquinone) 
[SJ  -  [Q]  =  [hydroquinone]  =  —  — 

7r 

and 

[SJ  -  [Q]  =  [quiBone] 


To 

where  [Q]  is  the  concentration  of  quinhydrone  and  7,.  and  j0  are 

the  activity  coefficients  of  the  hydroquinone  and  quinone,  re- 

spectively. 

Using  the  above  relations  and 

[8J  =  [S0] 
we  reach: 

(hydroquinone)  _  7, 
(quinone)  y0 

Consequently  equation  (4)  becomes: 


iCH+J  (9) 

Zb         70          * 

This  equation  for  the  true  quinhydrone  electrode  now  contains 
the  activity  coefficients  of  the  hydroquinone  and  quinone  and, 


XIX 


SALT-EFFECT;  QUINHYDRONE  ELECTRODE 


409 


since  the  ratio  does  not  remain  the  same  while  the  constitution 
of  the  solution  is  changed,  the  electrode  exhibits  what  is  called 
a  "salt-effect,"  which  is  a  special  "salt-effect." 

S0rensen,  S0rensen  and  Linderstr0m-Lang  (1921)  confirmed 
equation  (9)  by  determining  yT  and  y0  through  solubility  measure- 
ments with  hydroquinone  and  quinone.  They  also  traced  the 
details  contributing  to  the  conclusions  of  equations  (7)  and  (8). 

Equation  (9)  in  its  numerical  form  for  18°C.  may  be  recast 
to  the  form: 


0.05773 


0.5  log  - 
To 

Tr 


(10) 


Linderstr0m-Lang  replaces  —0.5  log  —  nby  Q,  the  magnitude  of 

To 

TABLE  54 

"Salt  correction,"  Qg,  for  quinhydrone  electrode  at  18° 

Add  value  to     q  to  obtain  corrected  value  of  pH. 

0.0577o 


SOLUTION 

Qs 

SOLUTION 

QS 

0  01  N  HC1           

-0  001 

0.5  M  (NH4)2SO4  

+0  019 

0  02  N  HC1 

-0  002 

1  0  M  (NH4)2SO4 

0  038 

0  05  N  HC1  

-0.003 

1.5M  (NH4)2SO4  

0.057 

0  10  N  HC1             .       .    . 

-0  005 

2  0  M  (NH4)2SO4  

0  078 

0  01  N  HC1  +  0  09  N  KC1 

-0  009 

2.5M  (NH4)oSO4 

0  097 

0  04MNaCl  

-0.005 

3.0M  (NH4)2S04  

0.116 

0  09  M  NaCl  

-0.008 

3.5M  (NH4)2S04  

0.135 

0  49  M  NaCl 

-0  021 

4  0  M  (NH4)2SO4    .  . 

0  156 

0  99  M  NaCl  

-0.045 

4  5  M  (NH4)2SO4 

0.175 

1  99  M  NaCl 

-0  094 

5  0  M  (NH4)2SO4 

0  194 

2  99  M  NaCl  

-0.145 

3  99  M  NaCl    . 

-0  200 

which  must  be  added  to  the  observed  value  of 


Eq  -  Eh 


to  obtain 


0.05773 

the  true  value  of  pH.  Since  this  correction  term,  Q,  will  vary 
it  is  feasible  to  list  only  a  few  cases.  Linderstr0m-Lang  (1924) 
gives  the  values  shown  in  tables  54  and  55.  His  estimates  of 
the  corrections  applicable  to  milk  and  blood  serum  are  not  in 
very  good  agreement  with  those  of  Lester  (1924)  on  the  one  hand 


410 


THE   DETERMINATION    OF   HYDROGEN   IONS 


or  of  Kolthoff  (1925)  on  the  other  hand;  but  his  data  are  the 
more  carefully  rationalized.  They  may  serve  to  indicate  the 
order  of  magnitude  of  the  corrections  to  be  expected  and  for 
approximate  purposes  may  be  considered  additive  for  limited 
ranges  of  concentrations.  For  rough  work  the  salt  effect  may  be 
ignored  as  negligible  compared  with  errors  of  technique. 

PREPARATION    OF   QUINHYDRONE 

Biilmann  (1927)  after  some  years  experience  recommends  the 
following  method  of  preparing  quinhydrone,  the  method  used  by 
Biilmann  and  Lund  (1921). 

TABLE  55 

Protein  correction  Qp  for  quinhydrone  electrode  at  18°  at  indicated  pH  value 

of  solution 


EGG  ALBUMIN 

pH 

QP 

SEBUM 
ALBUMIN 

pH 

QP 

0.3Cn* 

4.0 

+0.003 

0.3  Cn* 

4.0 

+0.048 

O.SCn 

4.5 

-0.017 

0.3Cn 

4.5 

+0.033 

0.3Cn 

5.0 

-0.028 

0.3Cn 

5.0 

+0.028 

0.3  Cn 

5.5 

-0.031 

0.3  Cn 

5.5 

+0.029 

8EBDM 
ALBUMIN 

pH 

QP 

SERUM 
ALBUMIN 

pH 

QP 

0.1  Cn* 

4.7 

+0.009 

0.6Cn* 

4.7 

0.045 

0.2  Cn 

4.7 

+0.017 

0.8  Cn 

4.7 

0.055 

0.4Cn 

4.7 

0.033 

1.0  Cn 

4.7 

0.064 

*  Cn  =  gram  equivalents  of  protein  nitrogen. 

A  solution  of  one  hundred  grams  of  iron  alum  in  300  cc.  of 
water  at  65°C.  is  poured  into  100  cc.  of  a  warm  solution  contain- 
ing 25  grams  commercial  hydroquinone.  The  mixture  is  cooled, 
the  quinhydrone  is  filtered  with  suction  and  washed  three  or  four 
times  with  cold  water.  Dry  between  filter  paper  at  room  tem- 
perature and  store  in  dark  bottles.  Yield:  15  to  16  grams. 

This  preparation  may  contain  traces  of  iron  which  Biilmann 
believes  to  have  no  appreciable  effect  on  the  potential.  High 
temperature  drying  should  be  avoided  since  quinone  may  vol- 
atilize sufficiently  to  alter  the  desired  ratio  of  reductant  to  oxidant. 


XIX  QUINHYDRONE    ELECTRODES  411 

Schreiner  (1925)  prefers  a  purer  product.  He  crystallizes 
hydroquinone  from  50  per  cent  aqueous  acetic  acid  and  quinone 
from  water  acidified  with  acetic  acid.  For  the  preparation  of 
quinhy drone  from  these  pure  products  an  acetic  acid  solution  of 
the  hydroquinone  is  added  in  excess  to  an  acetic  acid  solution  of 
the  quinone. 

Arnd  and  Siemers  (1926)  find  that  occluded  acidic  impurities 
may  appreciably  affect  the  potential  in  poorly  buffered  solutions 
and  therefore  they  recrystallize  the  quinhydrone  from  water  at 
70°C.  Kolthoff  (1927)  thinks  crystallization  from  water  has  an 
unfavorable  effect.  He  extracts  the  preparation  with  water 
before  use. 

It  is  not  improbable  that  attempts  to  prepare  quinhydrone  of 
high  purity  by  repeated  crystallization  have  sometimes  failed 
to  yield  a  reliable  product  because  no  attention  was  given  to  the 
tendency  of  the  product  to  oxidize,  or  otherwise  change,  in  neutral 
as  well  as  in  alkaline  solution.  While  I  have  had  little  experience, 
I  would  suggest  that  recrystallization  be  done  in  acid  solution. 
As  the  preparation  becomes  purer  the  amount  of  acid  necessary 
becomes  small.  Recrystallization  in  acid  solution  followed  by 
washing  in  the  absence  of  air  would  seem  a  priori  to  be  the  better 
procedure. 

ELECTRODES  AND  ELECTRODE  VESSELS 

Since  the  possible  effects  of  atmospheric  oxygen  in  changing  the 
ratio  of  oxidant  to  reductant  are  usually  neglected,  the  common 
forms  of  electrode  vessel  make  no  allowance  for  the  management 
of  a  gas  phase  as  does  any  well  designed  vessel  for  the  hydrogen 
electrode.  This  simplifies  the  design.  Indeed  there  is  not  very 
much  to  say  about  the  vessel,  unless  one  describes  all  the  unim- 
portant details  which  have  been  made  the  occasion  for  papers 
on  the  subject.2 

Biilmann  and  Lund's  vessels  are  shown  by  1  and  2  of  figure  79. 
Biilmann  recommends  that  at  least  two  electrodes  be  used. 
Among  several  vessels  designed  to  handle  small  quantities  of  solu- 
tion may  be  mentioned  that  of  Cullen  and  Biilmann  (1925), 
No.  3.  The  gold  plated  wire  is  moistened  and  dipped  into  crystals 

2  Apparently  we  have  here  a  case  where  multiplicity  of  design  is  in 
direct  proportion  to  the  simplicity  permissible. 


412         THE  DETERMINATION  OF  HYDROGEN  IONS 


I 


-Q 
-Au 


FIG.  79.  VESSELS  FOR  QUINHYDRONE  HALF-CELLS 


XIX  ERRORS   WITH   QUINHYDRONE   ELECTRODE  413 

of  quinhy drone.  These  adhere.  The  electrode  is  then  placed  in 
the  capillary  and  solution  is  drawn  in.  The  tip  of  the  vessel  is 
then  placed  in  the  KC1  bridge. 

No.  4  is  a  simple  quinhy  drone  cell,  one  half -cell  of  which 
contains  a  standard  buffer  solution,  e.g.,  "standard  acetate." 
The  junction  is  made  with  a  bridge  of  KCl-agar.  This  was  used 
by  Viebel. 

No.  5  represents  the  vessel  of  Mozolowski  and  iParnas  (1926). 
A  small  platinum  wire  is  fused  to  a  copper  lead.  The  platinum 
wire  runs  through  the  bottom  of  the  vessel  and  makes  contact 
with  a  gold  film.  No.  6  represents  one  of  the  vessels  of  Mis- 
lowitzer  (1925).  One  of  the  compartments  carries  a  reference 
solution  the  other  the  tested  solution.  Junction  is  made  with 
KC1  solution  in  the  joint.  Smolik  (1926)  uses  a  similar  device. 

No.  7  is  a  micro-electrode  vessel  designed  by  Ettisch  (1925). 

Regarding  the  electrode  itself  it  may  be  said  that  there  apply 
the  precautions  discussed  in  Chapter  XIV  during  the  description 
of  the  preparation  of  the  base  of  the  hydrogen  electrode.  No 
"black"  is  to  be  deposited  but  Biilmann  emphasizes  the  necessity 
for  a  good  and  clean  surface.  There  are  those  who  prefer  plati- 
num and  those  who  prefer  gold  surfaces.  Biilmann  is  a  bit  in- 
definite regarding  his  preference;  but  Corran  and  Lewis  (1924) 
prefer  gold  while  Mislowitzer  (1926)  and  Grossmann  (1927)  prefer 
platinum. 

SOURCES   OF   ERROR 

In  alkaline  solutions  two  effects  must  be  taken  into  account. 
In  the  first  place  the  ionization  of  hydroquinone  becomes  appreci- 
able above  about  pH  8.5  and  renders  inapplicable  the  simplified 
equation.  If  the  dissociation  constants  of  hydroquinone  were 
accurately  known  this  could  be  corrected  for;  but  it  would  not 
obviate  a  serious  difficulty, — the  decomposition  and  oxidation 
which  takes  place  readily  in  the  system  when  subjected  to  alkaline 
solutions.  See,  for  example,  LaMer  and  Parsons  (1923),  LaMer 
and  Rideal  (1924),  and  Conant,  Kahn,  Fieser  and  Kurtz  (1922). 
In  a  more  or  less  arbitrary  way  Biilmann  (1927)  sets  pH  8.5  as 
the  limit  of  measurements  of  the  accuracy  of  0.01  unit  pH  but  it 
must  be  noted  that  his  basis  is  the  effect  of  dissociation. 

A  second  fundamental  consideration  is  the  avoidance  of  oxidiz- 


414  THE    DETERMINATION    OF   HYDROGEN   IONS 

ing  or  reducing  solutions  which  can  change  the  ratio  of  oxidant 
to  reductant  the  mainteinance  of  which  is  essential.  It  is  by  no 
means  a  simple  matter  to  treat  this  aspect  with  complete  assur- 
ance. As  indicated  on  page  371  the  complete  avoidance  of  solu- 
tions which  are  potentially  capable  of  exercising  a  reducing  or 
oxidizing  action  would  seriously  limit  the  application  of  any 
device  for  the  determination  of  pH  by  electrode  methods.  It 
would  eliminate  the  quinhydrone  electrode  from  one  of  its  spheres 
of  greatest  value.  For  it  was  shown  by  Biilmann  (1921)  in  one 
of  his  first  papers  on  the  subject  that  the  quinhydrone  electrode 
may  be  used  to  determie  the  pH  values  of  dilute  nitric  acid  solu- 
tions and  of  solutions  of  unsaturated  organic  acids  which  cannot 
be  well  handled  with  the  aid  of  the  hydrogen  electrode.  The  more 
obvious  explanation  of  this  success  is  that  the  oxidizing  or  the 
reducing  agent  acts  so  slowly  that  the  ratio  of  quinone  to  hydro- 
quinone  is  not  appreciably  changed  within  the  time  required  for 
the  attainment  of  the  equilibrium  in  the  system  quinhydrone- 
quinone-hydroquinone-electrode.  And  here  it  may  be  remarked 
that  the  absence  of  a  gas  phase,  the  absence  of  a  complicated 
solid  phase  (platinum  black)  and  the  absence  of  the  catalytic 
effect  of  the  platinum  black  probably  contribute  to  the  rapidity 
of  the  attainment  of  equilibrium.  Indeed  those  who  are  accus- 
tomed to  the  hydrogen  electrode  and  to  the  necessity  of  establish- 
ing by  long  waits  the  fair  permanence  of  potential  and  the  ab- 
sence of  significant  drift  of  potential  will  be  inclined  to  use  poor 
judgment  in  the  application  of  the  quinhydrone  electrode.  Of 
course  some  time  must  be  allowed  for  the  attainment  of  equi- 
librium. We  may  reasonably  assume  that  the  equilibrum  poten- 
tial is  approached  asymptotically;  but  if  we  do  not  seek  the  utmost 
refinement  we  may  rely  on  the  experience  (with  stable  buffer 
solutions)  that  the  equilibrium  potential  is  very  closely  ap- 
proached within  a  very  few  minutes.3  Subsequent  drifts  of 
potential  in  complicated  and  unstable  solutions  may  then  be  due 
to  secondary  reactions  causing  a  fundamentally  true  error  in  the 
measurement.  A  clear  separation  of  the  two  effects,  asymptotic 

8  The  photographic  record  of  potential  change  made  by  Buytendijk 
and  Brinkman  (1926)  indicates  that,  in  the  absence  of  carbonate,  the 
equilibrium  potential  is  reached,  or  closely  approached  within  a  few  seconds 
after  a  change  is  made  in  a  previously  equilibrated  system. 


XIX  ERRORS    OF    QUINHYDRONE    ELECTRODE  415 

approach  to  equilibrium  potential  on  the  one  hand  and  reaction 
of  the  oxidation-reduction  system  internally  or  with  constituents 
of  the  solution  on  the  other  hand,  is  probably  the  greatest  puzzle 
in  the  practical  application  of  the  quinhydrone  electrode  or  of 
any  similar  system. 

Among  the  problems  which  have  not  yet  been  adequately 
solved  is  that  of  the  conduct  of  the  quinhydrone  system  in  protein 
solutions.  In  the  first  place  there  occur  in  the  literature  scattered 
references  to  the  combination  of  quinone  with  protein.  See  for 
example  Cooper  and  Nicholas  (1927)  and  the  subject  of  quinone 
tanning  dealt  with  in  treatises  on  tanning.  Yet  the  application 
of  the  system  to  the  study  of  milk,  beer,  blood  serum  etc.  has 
been  fairly  successful.  A  summary  with  references  pertaining  to 
these  applications  is  given  in  Biilmann's  review,  (Biilmann,  1927). 

True  errors  caused  by  reaction  of  the  system  with  the  con- 
stituents of  the  solution  must  be  carefully  distinguished  from 
apparent  error  resulting  from  the  attempt  to  apply  to  all  sorts  of 
solution  the  simple  equation  cast  in  terms  of  concentrations  or  the 
data  standardized  with  the  aid  of  simplifying  assumptions. 

There  remain  a  number  of  sources  of  error  due  to  faulty  tech- 
nique. Quinhydrone  is  not  always  easy  to  wet.  Compare  Cor- 
ran  and  Lewis  (1924).  Loss  of  quinone  by  drying  quinhydrone 
at  too  high  temperature,  the  occlusion  of  oxidation  products  etc., 
alter  the  ratio  of  oxidant  to  reductant.  In  buffer-poor  solutions 
the  occlusion  of  acid  or  of  impurities  having  a  direct  effect  on  the 
acid-base  equilibrium  of  the  solution  with  which  the  quinhydrone 
is  mixed  have  been  detected  as  sources  of  error.  Biilmann  (1927) 
presents  an  elaborate  discussion  of  the  errors  of  temperature 
fluctuation.  Biilmann  cautions  against  the  use  of  electrodes 
which  have  developed  minute  cracks  in  the  glass  seal.  It  would 
seem  from  his  discussion  that  a  good  part  of  the  false  potentials 
thereby  attained  is  due  to  the  mercury.  Let  it  be  noted  however 
that  mercury  electrodes  have  been  used  successfully  in  similar 
cases.  In  the  cases  cited  by  Clark  and  Cohen  (1923)  the  mercury 
was  of  very  high  purity.  Compare  also  Butler,  Hugh  and  Hey 
(1926). 

APPLICATIONS 

The  quinhydrone  and  similar  self-cells  have  found  many  ap- 
plications. In  some  instances  they  have  been  applied  simply  as 


416         THE  DETERMINATION  OF  HYDROGEN  IONS 

substitutes  for  the  hydrogen  half -cell.  However,  they  have 
unique  uses.  The  absence  of  a  catalytically  active  metal  and  of 
an  intense  reducing  system  has  permitted  the  quinhydrone  elec- 
trode to  be  applied  to  solutions  of  dilute  nitric  acid,  unsaturated 
organic  acids  and  a  variety  of  oxidizing  systems  which  either  are 
too  slow  in  their  action  to  appreciably  disturb  the  equilibrium  of 
the  electrode  or  are  oxidants  of  low  oxidizing  intensity.  (See 
page  391.)  Furthermore  there  is  no  gas  phase  and  consequently 
no  complexity  such  as  is  encountered  when  the  hydrogen  half- 
cell  is  used  with  carbonate  solutions.  This  is  of  particular  im- 
portance to  the  study  of  biological  systems. 

Because  the  quinhydrone  electrode  is  much  more  simple  to 
operate  than  the  hydrogen  electrode  and  yet  can  be  used  with 
the  potentiometer  system  and  other  equipment  provided  for  the 
hydrogen  electrode,  it  has  been  put  into  practice  by  very  many 
of  those  who  are  already  equipped  for  hydrogen  electrode  measure- 
ments and  by  those  entering  the  general  field  for  the  first  time. 
Because  of  this  it  is  practically  impossible  without  diligent  and 
detailed  examination  of  the  world's  literature  to  assemble  a  com- 
plete list  of  applications.  And  yet  it  is  in  special  applications 
that  there  have  appeared  special  sources  of  error,  better  knowledge 
of  limitations  and  the  occasions  for  special  technique.  These 
minutiae  cannot  be  covered  adequately  in  a  general  text.  Hence 
there  are  assembled  below  an  incomplete  list  of  references  to 
applications  by  subject, — a  list  which  it  is  hoped  will  be  of  use  to 
those  who  are  in  search  of  the  records  of  applicability  in  their 
several  specialties. 

Alkaloids,  medicinals,  etc.:  Baggesgaard-Rasmussen  and  Shou 
(1925),  Brunius  and  Karsmark  (1927),  Wagener  and  McGill 
(1925);  Aluminum  solutions:  Felling  (1925);  Blood,  plasma, 
serum,  etc.:  Corran  and  Lewis  (1924),  Cullen  and  Biilmann 
(1925),  Cullen  and  Earle  (1928),  Grossman  (1927),  Runge  and 
Schmidt  (1926),  Liu  (1927),  Meeker  and  Oser  (1926),  Mis- 
lowitzer  (1925,  1926),  Schaefer  (1926),  Schaefer  and  Schmidt 
(1925),  Vellinger  and  Roche  (1925);  Copper  solutions:  O'Sullivan 
(1925);  Dairy  products:  Lester  (1924),  Knudsen  (1925),  Linder- 
str0m-Lang  and  Kodama  (1925),  Watson  (1927) ;  Feces:  Robinson 
(1925);  Gastric  juice:  Schaefer  and  Schmidt  (1925),  Va"na  (1926); 
Nickel  solutions:  Parker  and  Greer  (1926);  Plant-juices:  Dom- 


XIX  CHLORANIL   ELECTRODE  417 

ontvich  (1925);  Protein  solutions:  Freundlich  and  Neukircher 
(1926),  Linderstr0m-Lang  and  Kodama  (1925);  Soils:  Arnd  and 
Siemers  (1926),  Baver  (1926),  Biilmann  (1924),  Biilmann  and  Tov- 
borg-Jensen  (1927),  Brioux  and  Pien  (1925),  Hissink  and  van 
der  Spek  (1926),  Itano,  Arakawa  and  Hosoda  (1926-1927),  Kappen 
and  Beling  (1925),  Olsen  and  Linderstr0m-Lang  (1927),  Schmidt 
(1925),  Snyder  (1927);  Sugar  solutions;  Balch  (1925),  Biilmann 
and  Katagiri  (1927),  Paine  and  Balch  (1927);  Tanning:  Hugonin 
(1925) ;  Water  (natural) :  Parker  and  Baylis  (1926) ;  Wine:  Dietzel 
and  Rosenbaum  (1927);  Titrations,  measurements  of  dissociation 
constants,  theoretical  work,  non-aqueous  solutions,  etc.:  Auerbach  and 
Smolczyk  (1924),  Bodforss  (1922),  Biilmann  and  Henriques  (1924), 
Buytendijk,  Brinkman  and  Mook  (1927),  Conant  et  al.  (1922- 
1927),  Cray  and  Westrip  (1925),  Daniel  (1927),  Darmois  (1924), 
Darmois  and  Honnelaitre  (1924),  Ebert  (1925),  Harris  (1923)  ,Itano 
and  Hosoda  (1926),  Klit  (1927),  Kolthoff  (1923,  1927),  KolthofT 
and  Bosch  (1927),  LaMer  and  Baker  (1922),  LaMer  and  Parsons 
(1923),  LaMer  and  Rideal  (1924),  Larsson  (1922),  Pring  (1923, 
1924),  Rabinowitsch  and  Kargin  (1927),  Schreiner  (1922,  1925), 
S0rensen  and  Linderstr0m-Lang  (1924),  Wagener  and  McGill 
(1925). 

THE   CHLORANIL   ELECTRODE 

Among  the  several  quinone-hydroquinone  systems  studied  by 
Conant  and  Fieser  (1923)  and  by  others,  that  of  tetrachloroquinone 
and  its  hydroquinone  promises  to  rival  the  benzoquinone-benzo- 
hydroquinone  system  in  usefulness.  With  tetrachloroquinone 
(Chloranil)  and  the  corresponding  hydroquinone 


Cl 


Chloranil          Hydroquinone  of  chloranil 


418  THE    DETERMINATION    OF   HYDROGEN   IONS 

it  is  possible  to  saturate  solutions  simultaneously  with  both 
oxidant  and  reductant  as  is  not  the  case  with  hydroquinone  and 
quinone. 

If  then  a  cell  be  formed  as  follows 


Pt 


C6C14O2  (sat.) 


Solution  A 


Bridge 


(sat.) 


Solution  B 


C6C14O2H2  (sat.) 


Pt 


and  if  the  bridge  can  be  assumed  to  eliminate  junction  potential 
the  electrode  process  is 

C6C1402  (solid)  +  2H+  +  2e  ^±  C6C1402H2  (solid) 

Here  the  end  products  are  solid  phases  which  at  a  given  tempera- 
ture and  crystal  form  may  be  regarded  as  having  fixed  activities. 
The  free  energy  change  attending  the  passage  of  one  mole  of 
hydrion  from  one  solution  to  the  other  is  given  at  once  by  FE 
and  E  is  the  electromotive  force  of  the  cell.  Obviously  the  solu- 
tion must  be  acid  enough  to  permit  the  retention  of  the  solid  phase 
of  the  reductant.  The  cell  potential  is  then  a  measure  of  the 
relative  activities  of  the  hydrion  in  the  two  solutions 

RT      (H+)A 


Accordingly  Conant,  Small  and  Taylor  (1925),  Hall  and  Conant 
(1927)  and  Conant  and  Hall  (1927)  find  the  chloranil  electrode 
eminently  suited  to  the  comparison  of  solutions  with  different 
solvents.  See  Chapter  XXIX. 

One  difficulty  arises  in  the  very  small  solubility  of  chloranil 
and  its  reductant.  Because  of  this  the  solution  rates  become  im- 
portant to  the  approach  of  an  equilibrium  potential.  Hall  and 
Conant  determine  by  preliminary  measurements  how  much  of 
each  substance  is  necessary  to  give  a  quick  crystallization  when 
heated  to  50°  and  cooled  to  the  working  temperature. 

SUMMARY   OF   EQUATIONS 

Quinhydrone  electrode 

•prp 

Eh  =  Eq  +  —  -  In  (H+)  +  (a  correction  term  specific  for  each  solution) 
F 

For  values  of  the  correction  term  see  pages  409-410.     Omitting 


XIX 


EQUATIONS,    QUINHYDRONE   CELL 


419 


consideration  of  the  correction  term  we  have  the  numerical 
form  at  25°C. 

Eh  =  Eq  -  0.05912  pH 

For  the  numerical  factor  at  various  temperatures  see  Appendix. 
For  the  cell 

-  Pt,  H2  (1  atmos.)  |  HC1  (0.1N),  quinhydrone  |  Pt  +        I 

at  18°C.  Biilmann  and  Jensen  (1926)  obtain  0.70439  d=  0.00004 
volt.  Since  the  difference  of  potential  between  the  hydrogen 
and  quinhydrone  electrodes  should  be  the  same  at  all  values  of 
pH  in  the  acid  region  under  ideal  conditions,  we  may  regard 
+0.7044  to  be  the  value  of  Eq  at  18°C.  Biilmann  and  Krarup 
(1924)  obtained  the  following  expression  for  the  temperature 
coefficient  of  cell  (I) 

Eht  =  0.7175  -  0.00074  t 

To  conform  to  Biilman  and  Jensen's  value  at  18°  we  shall  use 
Eht  =  0.7177  -  0.00074  t 

Accordingly  there  can  be  found  the  values  of  Eq  given  in  table  56. 

Veibel  (1923)  recommended  the  quinhydrone  half-cell  as  one 
which,  if  prepared  from  day  to  day  with  a  standard  solution 
could  serve  in  the  standardization  of  hydrogen-  or  calomel  half- 
cells. 

When,  however,  the  quinhydrone  half-cell  is  put  in  junction 
with  saturated  KC1  solution,  as  it  is  in  standardizing  the  saturated 
calomel  half-cell,  there  is  introduced  an  uncertain  liquid  junction 
potential.  It  then  becomes  a  matter  of  considerable  importance 
to  distinguish  the  manner  in  which  the  two  type  cells  below  are 
to  be  handled. 


Hg 


HgCl,  KC1  (sat.) 


Hg 


HgCl,  KC1  (sat.) 


HC1  (0.1N) 

quinhydrone 

Phosphate  buffer 

quinhydrone 


Pt 


Pt 


II 


III 


In  cell  II  the  liquid  junction  potential  is  doubtless  much  larger 
than  in  cell  III. 


420 


THE    DETERMINATION   OF   HYDROGEN   IONS 


The  practice  is  either  to  neglect  the  change  or  to  estimate  it  by 
the  Bjerrum  extrapolation.  Partly  because  of  diversity  in  this 
practice,  and  partly  because  of  the  discrepancies  in  primary 
experimental  data  involving  no  calculations,  we  have  been  unable 
reconcile  various  estimates  of  numbers  used  in  the  practical  appli- 
cation of  the  quinhy drone  electrode. 

Most  of  the  data  assembled  by  Biilmann  (1927)  proceed  from 
standardizations  with  0.01N  HC1  +  0.09N  KC1  but  with  2.029 
as  the  assumed  pH  value. 

We  shall  make  the  following  tentative  estimates. 

Assume  1.078  for  the  pH  number  of  0.1N  HC1  and  calculate 
therefrom  the'hydrogen  potentials  at  various  temperatures.  See 
table  A  page  672.  From  these  estimates  compile  with  the  aid  of 
table  A  the  numbers  found  in  table  56  below. 

TABLE  56 

Tentative  values  for  cells  containing  the  quinhydrone  half-cells 


Cell  A 


Half-Cell  B 


CeU  C      Hg 


CellD 


Ft,  H2(l  atmos.) 


KC1 

(sat.) 


HgCl,  KC1  (0.1N) 


(H+)  =  1 
quinhydrone 


HC1  (0.1) 


Pt 


quinhydrone 


Pt 


KC1  (sat.) 


[HC1  (0.1N) 
quinhydrone 


Pt 


Hg 


HgCl,  KC1  (sat.) 


HC1  (0.1N) 
quinhydrone 


Pt 


CELL  OE  HALF-CELL 

A 

B 

C 

D 

•c. 

volts 

volts 

volts 

volts  (approx.) 

18 

0.7044 

0.6423 

0.3043 

0.391 

20 

0.7029 

0.6404 

0.3025 

0.390 

25 

0.6992 

0.6356 

0.2980 

0.3898 

30 

0.6955 

0.6308 

0.2937 

0.389 

35 

0.6918 

0.6261 

0.2896 

0.388 

38 

0.6896 

0.6232 

0.2871 

0.387 

40 

0.6881 

,0.6213 

0.2855 

0.387 

XIX 


EQUATIONS 


421 


See  pages  259  and  404  for  the  position  of  the  line  of  the  quin- 
hydrone  electrode  on  the  E:pH  diagram. 

Quino-quinhydrone  electrode 


or  at  25' 


For  the  cell 


-  Pt,  H2(l  atmos,) 


Eh  =  Eqq  -  0.05912  pH 

quinone  (s) 


HC1  (0.1N) 


quinhydrone  (s) 


Biilman  and  Lund  (1921)  found  at  18°  0.7564.     Schreiner' 
(1925)  data  give 

Eh  =  0.7759  -  0.000842  t 
for  the  range  5°  to  18°.     We  then  have 


t 

EQQ 

t 

Eqq 

°c. 

•c. 

0 

0.7716 

18 

0.7664 

5 

0.7674 

20 

0.7548 

10 

0.7632 

25 

0.7505 

15 

0.7590 

Conant  and  Fieser  (1923)  find  0.7488  at  25°  and  0.7699  at  Oc 
Hydro-quinhy drone  electrode 
Eh  =  Ehq  +  —  In  (H+) 

or  at  25° 

Eh  =  Ehq  -  0.05912  pH. 


For  the  cell 


-  Pt,  H2(l  atmos.; 


HC1  (0.1N) 


quinhydrone  (s) 
hydroquinone  (s) 


Pt 


422 


THE    DETERMINATION    OF   HYDROGEN   IONS 


Biilmann  and  Lund  (1921)  found  at  18°  0.6177.  Schreiner  (1925) 
finds  a  temperature  coefficient  of  —0.000651  volt  per  degree 
between  12°  and  22°  and  -0.000641  volt  per  degree  between  22° 
and  32°.  Hence  we  have: 


t 

_Ehq 

t 

Ehq 

•c. 

°C7. 

0 

0.6294 

20 

0.6164 

10 

0.6242 

25 

0.6132 

15 

0.6197 

30 

0.6100 

18 

0.6177 

Conant  and  Fieser  (1923)  find  0.6126  at  25°  and  0.6272  at  0°. 

Chloranil  electrode 
Eh  =  Ee  +  ^  In  (H+) 

P 

Conant  and  Fieser  (1923)  found  that  when  chloranil  and  hydro- 
chloranil  are  present  in  the  solid  phase  Ec  =  0.664  at  25° C.  and 
0.683  at  0°C. 

Note  that  this  not  the  potential  of  a  homogeneous  system 
(solution)  at  50  per  cent  reduction. 

SUMMARY 
See  Appendix,  table  A  for  a  table  of  standardized  values. 


CHAPTER  XX 

METAL  OXIDE  ELECTRODES;  THE  GLASS  ELECTRODE;  THE 
OXYGEN  ELECTRODE 

METAL   OXIDE    ELECTRODES 

Equations 

The  reversible  exchange  of  electrons  between  a  metal  and  its 
ions  may  be  regarded  as  an  oxidation-reduction  process.  For  the 
system  : 

Mn+  +  ne  ^±  M, 

we  may  write  the  electrode  potential  equation  (1)  directly  from 
equation  (15)  of  Chapter  XVIII  (page  377). 


Were  the  metal-metal  ion  system  the  only  one  present,  the 
saturation  of  the  solution  with  respect  to  the  metal  should  be 
accomplished  by  the  presence  of  a  mass  of  the  metal  in  a  solid 
phase  other  than  that  of  the  electrode  itself.  E  should  then  be 
determinable  by  an  unattackable  electrode.  Of  course  this  is 
quite  impracticable  because  M,  specified  formally  as  a  com- 
ponent of  the  solution,  has  an  activity  (M)  of  such  an  insig- 
nificant magnitude  that  the  slightest  disturbance  of  the  electrode 
itself,  by  the  presence  of  the  slightest  trace  of  another  oxidation- 
reduction  system,  would  vitiate  the  measurement.  Consequently 
in  the  study  of  the  metal-metal  ion  system  the  electrode  itself  is 
made  of  the  metal  in  question  in  order  that  this  metal  may 
dominate  the  situation  in  the  immediate  interface  between  elec- 
trode and  solution. 

We  develop  this  point  of  view  in  order  that  we  may  avoid  the 
confusion  arising  from  the  consideration  of  the  electrode  as  highly 
specialized.  We  shall  regard  it  as  fundamentally  an  oxidation- 
reduction  electrode  the  potential  of  which  may  be  determined  by 
the  system  Mn+:M  or  by  the  system  Ma+:Mb+. 

423 


424  THE    DETERMINATION    OF   HYDROGEN   IONS 

In  the  first  case  we  assume  the  activity  of  the  metal  in  solution 
to  be  constant  and  equation  (1)  reduces  to 


E  =  Eo  +  =    In  (M»+)  (2) 

nJb 

Now  suppose  the  alkalinity  of  the  solution  is  sufficient  to  form 
the  metal  hydroxide.    For  the  reaction 

M*+  +  n  OH-  ^±  M  OHn 
write  the  equilibrium  equation 

(M»+)  (OH-)* 
(MOHn) 

Let  the  activity  of  the  metal  hydroxide  in  solution  be  constant 
by  reason  of  the  presence  of  the  solid  phase.    Then 

(Mn+)  (OH-)n  =  KB  (3) 

Hence  by  (2)  and  (3) 


or 

B-Ei+5£zn(H+)  (5) 

r 

If,  in  place  of  the  hydroxide,  there  is  present  the  oxide  it  is 
necessary  for  purposes  of  formal  treatment  to  assume  that  the 
oxide  will  attain  equilibrium  with  its  hydrate  d  product  namely 
the  hydroxide  in  question,  and  that  this  in  turn  will  attain  con- 
stancy of  activity  in  the  solution  by  reason  of  the  presence  of  the 
solid  phase.  Hence  equation  (5)  should  still  hold,  if  the  condi- 
tions are  met. 

The  above  theoretical  discussion  assumed  but  one  oxide.  In 
the  presence  of  two  oxides  there  could  be  only  a  pseudo-equilib- 
rium; but  that  the  main  result  should  not  be  affected  were  there 
two  oxides  in  the  presence  of  the  metal,  is  revealed  by  the  follow- 
ing. Consider  a  metal  in  two  states  of  oxidation,  Ma+  and  Mb+. 

Ma+  +  ne  ^  Mb+ 


XX  THEORY    OF   OXIDE   ELECTRODES  425 

By  equation  (15)  page  377 


Using  the  two  solubility  products 

(Mb+)  =  Kb  (H+)b 

(Ma+)  =  Ka  (H+> 
we  have 


RT      (H+)»  , 

E°  +         lH 


But  b  —  a  =  n.    Hence: 

T?T 

E  =  E;  +  ^-MH+)  (8) 

r 

Equation  (8)  is  equation  (5)  again.  The  reason  the  same  equa- 
tion is  reached  may  be  put  in  general  terms  as  follows.  In  addi- 
tion to  those  energy  changes  associated  with  electron  exchange 
and  which  are  not  directly  associated  with  the  hydrogen  ions  or 
hydroxyl  ions,  there  are  involved  the  energies  of  ionization  of  the 
metal  hydroxides  and  the  energy  of  hydrion  dilution.  We  have 
assumed  that  one  determinant  of  the  ionization  is  fixed  by  the 
constant  activity  of  the  hydroxide  or  hydroxides.  There  remains 
the  effect  of  varying  hydroxyl  or  hydrion  concentration.  This 
effect  takes  the  form,  in  the  energy  equation,  of  the  free  energy  of 
dilution  of  the  hydrions,  or  hydroxyl  ions,  according  to  the  choice 
in  formulation.  Separating  from  the  free  energy  cnange  the  po- 
tential, or  intensity  factor,  we  have  a  relation  parallel  to  the 
case  of  the  hydrogen  electrode.  Compare  equation  (5)  or  (8) 
with  equation  (38)  page  390. 

The  situation  would  be  very  different  were  the  hydroxide,  or 
one  of  two  or  more  hydroxides  which  might  be  involved  in  a 
pseudo-equilibrium  to  not  saturate  the  solution.  Any  one  of  such 
instances  would  then  become  a  very  special  case  and  no  common 
equation  would  be  applicable. 

There  will  be  detected  in  this  development  several  aspects, 
expressed  or  implied,  which  impose  difficult  experimental  restric- 


426  THE    DETERMINATION    OF    HYDROGEN    IONS 

tions.  In  addition  to  the  difficulty  of  attaining  complete  equilib- 
rium with  materials  so  susceptible  to  acquiring  different  forms 
(see  for  example  Maddison,  1926)  or  degrees  of  dispersion  as  are 
the  metal  hydroxides  and  oxides,  there  is  implied  the  difficulty 
of  controlling  the  activity  of  any  one  form  by  control  of  the  con- 
stitution of  the  solution.  Furthermore  it  would  appear  that  the 
water  activity  must  be  involved  for  the  ionic  product  entered  the 
equation  in  step  (4)~(5).  This  is  probably  of  secondary  con- 
sequence in  most  instances. 

With  the  exception  of  one  or  two  of  the  simpler  cases  which 
have  been  worked  upon,  for  example  the  mercury-mercury  oxide 
system,  little  of  a  systematic  nature  has  been  done  to  illuminate 
those  "oxide  electrodes." 

THE   MERCURY-MERCURIC   OXIDE    ELECTRODE 

Br0nsted  (1909)  finds  that  the  cell 

-  Pt,  H2 1  KOH,  HgO  |  Hg  + 

gives  the  same  electromotive  force  when  the  concentration  of 
KOH  is  changed.  There  are  small  differences  due  to  the  chang- 
ing activity  of  the  water.  On  the  assumption  of  complete  disso- 
ciation of  KOH  these  findings  satisfy  equation  (5)  and  the  tacit 
implication  spoken  of  above. 

A  few  references.  Br0nsted  (1909),  Donnan  and  Allmand 
(1911),  Fried  (1926),  Kolthoff  (1916),  Lamb  and  Larson  (1920), 
Chow  (1920),  Knobel  (1923),  Fricke  and  Rohmann  (1924),  Aten 
and  Van  Dalfsen  (1926). 

THE  "ANTIMONY  ELECTRODE" 

Uhl  and  Kestranek  (1923)  used  the  combination  antimony- 
antimony  oxide  with  promising  results.  Although  they  believed 
that  ordinary  commercial  antimony  contains  enough  oxide  to 
fulfill  the  requirements,  Kolthoff  and  Hartong  (1925)  recommend 
the  addition  of  the  oxide.  This  they  prepare  by  treating  antimony 
with  nitric  acid,  evaporating  to  dryness  and  igniting. 

In  studying  the  potentials  of  their  electrodes  in  buffer  solutions 
of  known  pH-values  Kolthoff  and  Hartong  did  not  obtain  the 
coefficient  0.057  demanded  by  equation  (5)  and  the  temperature 


XX  ANTIMONY    ELECTRODE  427 

of  operation.  They  found  it  to  be  about  0.0485  between  pH  1 
and  pH  5  and  approximately  0.0536  above  pH  9.  Between  5  and 
9  their  results  were  erratic. 

Buytendijk  and  Woerdeman  (1927)  have  used  this  electrode  in 
micro  form. 

Vies  and  Vies  and  Vellinger  (1927)  in  a  study  of  the  antimony 
electrode  find  that  the  empirical  equation 

pH  ==  0.0175  E  +  a 

holds  at  24°  over  a  considerable  range  of  pH.  In  this  equation  a 
is  a  constant  which  must  be  determined  for  each  particular 
electrode  by  measurements  with  buffer  solutions.  E  is  ex- 
pressed in  millivolts.  Consequently  if  E  is  expressed  in  volts 
we  have 

E  =  0.05714  pH  -  0.05714  a 

At  24°  the  coefficient  should  be  0.05892. 

Dr.  Fenwick1  kindly  permits  me  to  quote  as  follows  from  the 
manuscript  of  a  paper  entitled  The  antimony-antimony  trioxide 
electrode  and  its  use  as  a  measure  of  acidity  by  E.  J.  Roberts  and  F. 
Fenwick.  ".  .  .  The  potential  of  the  antimony-antimony 
trioxide  electrode  attains  its  maximum  accuracy  only  provided 
that  the  presence  of  any  unstable  solid  phase  in  the  system, 
notably  orthorhombic  antimony  trioxide,  is  carefully  avoided, 
dissolved  oxygen  is  eliminated  from  the  solution,  and  the  equi- 
librium is  approached  from  the  alkaline  side.  Under  these  condi- 
tions the  potential  of  the  electrode  is  a  linear  function  of  the 
logarithm  of  the  activity  of  hydrogen  ion,  with  the  theoretical 
slope,  from  pH  1  to  10."  Their  paper  when  published  should 
be  consulted  as  the  best  treatment  available.  See  also  Schuhmann 
(1924). 

THE   MANGANESE   DIOXIDE   ELECTRODE 

Gesell  and  Hertzman  (1926)  prepare  the  manganese  dioxide 
electrode  as  follows.  A  platinum  wire  about  0.5  mm.  diameter 
is  sealed  into  the  end  of  a  glass  tube  leaving  a  1  mm.  length  pro- 
truding. This  is  rounded  with  a  fine  stone  "to  avoid  point 
effects,"  plated  with  platinum  black,  and  fired  in  an  alcohol 

1  Personal  communication  from  Dr.  Fenwick. 


428  THE   DETERMINATION    OF   HYDKOGEN   IONS 

flame.  It  is  then  coated  during  1.5  minutes  by  connecting  it  to 
the  positive  lead  of  a  6  volt  battery  while  it  is  immersed  in  a 
solution  of  manganese  sulfate  ("0.4  N")>  acidified  with  sulfuric 
acid.  The  negative  electrode  was  placed  2  cm.  from  the  positive 
and  650  ohms  were  placed  in  the  external  circuit.  According  to 
these  authors  the  above  procedure  accomplished  a  compromise 
between  the  production  of  an  electrode  which  adjusts  rapidly  but 
which  has  a  coating  too  thin  and  too  easily  dissolved  and  an  elec- 
trode which  is  substantial  but  sluggish. 

That  the  potential  tends  to  be  a  linear  function  of  the  pH- value 
of  the  solution  is  roughly  confirmed;  but  Gesell,  for  instance, 
found  with  different  solutions  at  pH  7.4  that  the  potential  might 
vary  as  much  as  0.22  volts  corresponding  to  3  units  pH  by  the 
formula  deduced  above  and  to  2.3  units  pH  by  GeselFs  formula. 

Gesell's  interest  in  the  manganese  dioxide  electrode  is  chiefly  as 
a  convenient  means  of  following  changes  for  instance  in  the 
circulating  blood  or  in  the  expired  air. 

Parker  (1927)  has  used  the  manganese  dioxide  electrode  in 
control  of  industrial  processes. 

References.  Tower  (1895),  Smith  (1896),  Roaf  (1914),  Gesell 
and  Hertzman  (1926),  Gesell  andMcGinty  (1926),  Parker  (1927). 

OTHER   OXIDE   ELECTRODES 

Several  other  oxide  electrodes  including  those  with  Pb02, 
Ag203,  and  T1203  were  studied  by  Tower  (1895)  and  occasionally 
one  has  been  subjected  to  further  study.  See  for  example  Kolt- 
hoff  (1921)  and  especially  Fried  (1926).  Baylis  (1923)  found, 
empirically,  promising  results  with  the  tungsten  filament  of  an 
electric  light  bulb.  While  the  response  to  pH-changes  might  be 
ascribed  to  a  tungsten  oxide  electrode  the  relation  of  pH  to  poten- 
tial does  not  follow  that  formulated  above.  Parker  and  Baylis 
(1926)  made  some  further  studies  of  its  empirical  use. 

THE    OXYGEN  ELECTRODE 

Theoretically  an  unattackable  electrode  under  a  definite  partial 
pressure  of  oxygen  should  give  a  potential  which  is  a  linear  func- 
tion of  the  pH  value  of  the  solution.  See  equation  22  page  381. 


XX  OXYGEN  AND    GLASS   ELECTRODES  429 

Practically  the  calculated  potential  (see  figure  77,  page  387)  is 
not  attained  with  platinum,  gold  and  other  "unattackable" 
metals,  nor  is  the  linear  relation  always  found.  Empirically  this 
electrode  has  been  put  to  use  occasionally. 

See:  Arthur  and  Keeler  (1922),  Furman  (1922-1923),  Goard  and 
Rideal  (1924),  Malaprade  (1926),  Montillon  and  Cassel  (1924), 
Naray-Syabo  (1927),  Popoff  and  McHenry  (1925),  Smith  and  Giesy 
(1923),  Tilley  and  Ralston  (1923),  Van  der  Meulen  and  Wilcoxon 
(1923). 

Numerous  combinations  of  electrode  metals  differing  in  po- 
larization ability  have  been  put  to  use  in  end-point  titration.  See 
references  in  Kolthoff  and  Furman  Potentiometric  Titrations  (1926). 

THE 
Imagine  a  cell  of  the  following  type. 

Hg  |  HgCl,  KC1  (sat.)  |  solution  1  |  solution  2  |  KC1  (sat.),  HgCl  |  Hg     I 
A  BOB'  A' 

Potentials  at  A  and  A'  balance  one  another.  Assume  that 
potentials  at  B  and  B'  balance  one  another.  Instead  of  an 
ordinary,  liquid  junction  at  C  imagine  some  material  which  permits 
the  passage  of  a  particular  kind  of  ion  between  solutions  1  and  2. 
If  this  ion,  i,  were  alone  able  to  pass,  it  would  tend  to  go  from  the 
solution  in  which  its  chemical  potential  were  the  higher  to  the 
solution  in  which  its  chemical  potential  were  the  lower  and  would 
carry  nF  per  mole.  At  potentiometric  balance  the  potential  of 
the  cell  would  be 

"-¥"8; 

Suppose  solutions  1  and  2  were  solutions  of  silver  nitrate  with 
silver  ion  activities  (Ag+)i  and  (Ag+)2,  and  suppose  the  partition 
at  C  were  metallic  silver.  Instead  of  formulating  the  equation 
by  means  of  single  electrode  potentials,  we  may  consider  the 
metallic  silver  partition  to  be  one  permeable  only  to  silver  ions. 
Then  by  equation  (10)  we  have 


430  THE    DETERMINATION    OF   HYDROGEN    IONS 

Now  Haber  and  Klemenziewicz  (1909)  found  that,  with  such  an 
arrangement  as  that  stated  by  schema  I,  the  electromotive  force 
of  the  cell  conformed  to  the  equation 


when  a  very  thin  partition  of  glass  was  placed  at  C. 

They  regarded  the  glass  as  a  phase  containing  water  and 
hydrions  and  hydroxyl  ions  at  constant  concentration.  If  water 
penetrates  and  not  the  other  electrolytes  of  solution  1  and  2, 
equation  (12)  should  apply.  Michaelis2  pointed  out  the  analogy 
between  this  case  and  the  silver  cell  mentioned  above. 

However,  Horovitz  (1923)  showed  that  equation  (12)  would 
express  experimental  results  only  under  particular  conditions  and 
that  the  nature  of  the  glass  and  the  kind  of  ions  in  solution  are  of 
great  importance.  Accordingly  he  formulated  in  terms  of  ionic 
exchange  between  glass  and  solution,  thereby  taking  into  con- 
sideration the  specific  properties  of  the  glass.  Another  method  of 
approach  is  suggested  by  Michaelis'  study  of  membrane  per- 
meabilities. See  Michaelis  (1926).  Should  it  happen  that  the 
ionic  mobility  of  the  hydrion  in  a  particular  membrane  is  much 
larger  than  that  of  any  other  ion  there  would  be  a  virtual  approach 
to  the  condition  leading  to  equation  (12). 

See  Hurd,  Engel  and  Vernon  (1927)  on  ion  replacement  in  glass. 

Horovitz  presented  a  paper  on  the  theoretical  aspects  at  the 
Richmond  Meeting  of  the  American  Chemical  Society  in  April, 
1927,  but  I  have  not  noted  its  publication. 

In  all  events  the  matter  reduces  very  largely  to  a  selection  of 
glass  which  will  give  the  desired  effect.  Considerable  information 
on  this  aspect  was  furnished  by  Horovitz  (1923),  Horovitz,  Horn, 
Zimmermann  and  Schneider  (1925)  and  Horovitz  and  Zimmer- 
mann  (1925)  who  showed  that  certain  glasses  could  function  ap- 
parently as  "sodium  electrodes,"  "potassium  electrodes,"  "zinc 
electrodes,"  "silver  electrodes,"  etc.,  according  to  their  compo- 
sition and  the  solutions  in  contact.  In  a  solution  containing 
sodium  ions  the  well  known  thermometer  glass  59  III  and  glass 
397  III  (a  soda  glass)  behaved  as  "sodium  electrodes."  Gerate- 

2  See  Perlzweig's  translation  (1926). 


XX  GLASS   ELECTRODES  431 

glas  16  III  and  glass  1447  III,  which  contain  zinc,  behaved  as 
"zinc  electrodes."  A  number  of  glasses  were  also  found  to  func- 
tion as  "silver  electrodes"  in  solutions  of  silver  nitrate.  Mis- 
cellaneous lead  glasses  functioned  fairly  well  as  "hydrogen  elec- 
trodes." 

For  the  purposes  of  ordinary  measurements  with  buffer  solu- 
tions it  is  difficult  to  judge  the  conduct  of  particular  glasses  from 
Horovitz's  papers.  He  employed  none  of  the  common  buffer 
solutions  and  the  hydrogen  electrode  function  was  judged  by  acid- 
alkali  cells. 

Kerridge  (1925)  obtained  poor  results  with  "Durosil"  glass  and 
fused  silica  and  reported  glasses  which  acted  as  mixed  "sodium-" 
and  "hydrogen  electrodes"  in  sodium  phosphate  buffers  and  as 
"hydrogen  electrodes"  in  potassium  phosphate  buffers.  Among 
the  glasses  acting  as  mixed  electrodes  were  borosilicate  glasses. 
She  reports  success  with  "an  ordinary  soft  soda  laboratory 


Hughes  (1928)  concludes  that  a  glass  should  be  as  free  as 
possible  from  potash,  alumina  and  borates.  He  suggests  a  glass 
made  of  72  per  cent  Si02,  8  per  cent  CaO  and  20  per  cent  Na2O. 
The  bulb  should  be  blown  as  rapidly  as  possible  to  avoid 
devitrification. 

APPARATUS 

Wolf  (1927)  gives  references  to  some  earlier  uses  of  glass 
membranes. 

Helmholtz  (1881)  in  his  picture  of  what  was  one  of  the  first 
"glass  electrodes,"  used  a  bulb  as  did  Haber  and  Klemensiewicz. 
Others  have  continued  the  use  of  a  bulb  of  extremely  thin  glass 
blown  from  the  end  of  a  piece  of  relatively  thick  glass  tube. 
Korridge  (1925)  introduced  more  convenient  and  more  rugged 
designs  one  of  which  is  shown  in  figure  80.  The  chief  feature  is 
to  give  to  the  glass  membrane  the  form  of  a  deep  spoon  which  is 
"0.025  to  0.030  mm.  thick  in  its  thinnest  part."  This  is  filled 
with  the  unknown.  On  the  other  side  of  the  membrane  is  placed 
a  buffer  solution  of  known  pH- value. 

Kerridge  states  that  newly  blown  vessels  require  careful  clean- 
ing with  hydrochloric  acid,  steaming  for  two  hours  and  soaking 


432 


THE  DETERMINATION  OF  HYDROGEN  IONS 


with  distilled  water  for  24  hours  before  use.    The  cell  used  is 
according  to  the  following  scheme. 

Hg  |  HgCl,  KC1  (sat.)  |  Solution  1  |  JJ  Solution  2  |  KC1  (sat.),  HgCl  [  Hg 

glass 
membrane 

In  the  figure  the  vessel  is  shown  mounted  with  two  calomel 
half-cells. 


Insulator 


'SA — 7"  Insulator 


FIG.  80.  THE  CELL 

Hg  |  HgOl,  KC1  (sat.)  |  Unknown  |  Glass  |  Buffer  1  KC1  (sat.),  HgCl  |  Hg 
Kerridge's  Mounting  of  "Glass  Electrode,"  showing  spoon  form. 

The  "insulator"  indicated  in  the  figure  is  "amberite"  or  "orca." 
Blocks  of  such  material  support  the  calomel  half-cells  from  the 
stand  through  rack-and-pinion  adjusters.  For  further  details  of 
insulation,  etc.,  see  Brown  (1924)  and  for  description  of  quadrant 
electrometer  see  page  338. 

"Diffusion  of  potassium  chloride  into  the  solution  in  the  glass 


XX  GLASS    ELECTRODES  433 

electrode  is  prevented  by  small  ground  caps  fitted  over  the  tips 
of  the  calomel  electrodes  and  the  two  taps,  ungreased  in  the  middle 
race,  are  turned  off  while  the  measurements  are  being  made." 
The  caps  are  rinsed  and  wiped  before  immersion. 

If,  for  instance,  a;cid  potassium  phthalate  is  used  as  the  buffer 
within  the  vessel  and  its  pH  value  be  regarded  as  3.97,  the  formula 
should  be  according  the  Kerridge  (1926)  : 


where  Es  is  the  potential  found  with  the  phthalate  and  Ex  is 
that  found  with  the  solution  under  test. 

Kerridge  (1926)  claims  an  accuracy  characterized  by  a  probable 
error  of  0.01  pH  unit.  This  requires  of  the  quadrant  electrometer 
alone  a  sensitivity  capable  of  detecting  ±0.6  millivolt. 

Reliability  of  results  are  suggested  by  the  following  comparisons: 

Blood  by  glass  electrode  method  .........  ..................  7  .  75 

Blood  by  Dale-Evans  method  ..............................  7.73 

Phosphate  solution  by  glass  electrode  method  ...............  7.37 

Phosphate  solution  by  H-electrode  method  .................  7.  39 

Sycamore  leaves,  extract,  by  glass  electrode  method  ........  4.88 

Sycamore  leaves,  extract,  by  H-electrode  method  ...........  4.91 

For  further  details  of  theory  and  practice  see:  Bayliss,  Ker- 
ridge and  Verney  (1926),  Borelius  (1914),  Brown  (1924),  Cremer 
(1906),  Freundlich  (1921),  Freundlich  and  Ettisch  (1925), 
Freundlich  and  Rona  (1920),  Gross  and  Halpern  (1925),  Haber 
and  Klemensiewicz  (1909),  Hoet  and  Marks  (1926),  Hoet  and 
Kerridge  (1926),  Horovitz  (1923)  (1925),  Horovitz  and  Zimmer- 
man (1925),  Horovitz,  Horn,  Zimmerman  and  Schneider  (1925), 
Hughes  (1926-1928),  Katz,  Kerridge  and  Long  (1925),  Kerridge 
(1925),  Kerridge  (1926),  Schiller  (1924),  and  v.  Steiger  (1924). 


CHAPTER  XXI 

SOURCES  OF  ERROR  IN  POTENTIOMETRIC  MEASUREMENTS  OF  pH 

The  way  to  be  safe  is  never  to  feel  secure. — BURKE. 
ERRORS   OF  TECHNIQUE 

Sources  of  error  are  legion.  Some  of  them  are  specific  to  the 
hydrogen  electrode;  some  of  them  are  specific  to  the  quinhydrone 
electrode;  some  of  them  may  arise  in  the  use  of  any  cell;  occa- 
sionally one  evinces  the  stupidity  of  the  operator. 

During  a  series  of  measurements  it  became  necessary  to  empty 
and  refill  a  horizontal  tube  having  a  stopcock.  Potentials  became 
erratic.  This  was  traced  to  a  bubble  of  gas  which  had  clung  to 
the  bore  of  the  stopcock  key.  To  avoid  this  the  "horizontal" 
had  been  given  a  pitch  but  the  flow  had  not  been  adequate  that 
time.  One  day  after  a  year  or  so  of  smooth  operation  potentials 
became  erratic.  Tne  drain  tube  from  the  electrode  vessel  emptied 
through  a  six  inch  air  gap  to  the  laboratory  drain.  The  tube  was 
hidden  for  aesthetic  reasons,  and  it  had  not  been  observed  that  a 
stalagmite  and  a  stalactite  of  KC1  were  forming.  On  the  day  in 
question  they  met!  Not  only  was  faith  in  the  shielding  shattered 
and  the  shielding  redone;  but  the  hiding  of  the  drain  tube  and 
even  remote  connection  with  the  piping  became  taboo. 

These  little  incidents  from  the  writer's  experience  are  cited 
merely  to  suggest  the  constant  watchfulness  both  in  the  design 
of  apparatus  and  in  its  operation  which  is  necessary.  How  often 
has  it  been  suggested  that  the  high  tension  charging  line  and  the 
delivery  line  of  the  potentiometer's  storage  battery  be  placed  on  a 
double  throw,  double  pole  switch!  This  neat  scheme  pleases  till 
some  damp  day  at  the  end  of  which  a  day  is  counted  lost. 

The  reader,  if  he  counts  himself  an  experimenter,  knows  full 
well  the  impossibility  of  attempting  to  caution  on  every  point  of 
technique.  Something  must  be  left  to  common  sense  and  if  this 
is  not  possessed,  how  hopeless  is  the  task  of  going  over  in  absentia 

434 


XXI  ERRORS  435 

the  details  of  a  measurement  in  an  attempt  to  trace  a  suspected 
fault.  The  hoarding  of  solutions  which  should  be  used  to  wash 
away  the  buffer  action  of  solutions  previously  occupying  the 
electrode  vessel,  miserly  supplies  of  hydrogen,  contamination  of 
standard  half-cells  by  the  solutions  of  liquid  junctions,  electric 
leakage,  poor  reproduction  of  liquid  junctions,  dirty  electrodes, 
forgetfulness  of  hysteresis  in  cells  subjected  to  temperature 
changes,  neglect  of  corrections  for  particular  half-cells,  barometer 
changes  etc.,  plain  carelessness  and  ordinary  stupidity  all  usually 
disappear  at  the  hands  of  anyone  who  understands  the  ele- 
mentary theory  of  his  device  and  sets  about  it  to  meet  the  require- 
ments of  that  theory.  Then  day  after  day  as  the  eye  is  taken 
from  the  galvanometer  at  balance  the  readings  of  the  poten- 
tiometer dial  are  found  to  hit  the  mark  within  ±0.1  millivolt  for 
the  same  solution  and  confidence  that  something  definite  is  being 
measured  becomes  conviction.  And  at  last,  when  cells  and  condi- 
tions are  changed  and  small,  distinct  discrepancies  appear,  the 
experimenter  learns  to  his  sorrow  that  he  has  yet  to  master  many 
a  detail  of  technique. 

ERRORS   ARISING    FROM    THE    INHERENT   LIMITATIONS    OF    THE 
HYDROGEN   ELECTRODE 

Presence  of  oxidizable  material 

We  have  already  discussed  in  Chapter  XVIII  the  relation  be- 
tween the  hydrogen  electrode  and  the  "reduction  electrode,"  and 
have  shown  that  no  true  hydrogen  electrode  potential  can  be 
attained  until  the  solution  is  so  far  reduced  that  it  can  support  one 
atmosphere  of  hydrogen.  It  is  thus  made  perfectly  obvious  that 
a  measurement  of  pH  must  be  preceded  by  a  very  thorough  reduc- 
tion of  the  solution.1 

The  hydrogen  electrode  if  properly  treated  gives  such  a  pre- 
cisely defined  potential  in  well  buffered  solution,  reaches  this 
potential  so  rapidly,  returns  when  polarized,  and  adjusts  itself  to 
temperature  and  pressure  changes  so  well  that  there  is  little  doubt 

1  In  some  instances  it  is  important  to  remember  that  reduction  of  the 
constituents  of  a  solution  may  so  change  the  acidic  or  basic  properties  of 
these  constituents  that  serious  shifts  in  pH  may  occur. 


436  THE    DETERMINATION    OF   HYDROGEN   IONS 

of  its  being  a  reversible,  accommodating,  fairly  quick-acting  elec- 
trode. It  is  perhaps  because  of  this  that  it  shows  a  hydrogen 
electrode  potential  in  solutions  which  could  be  slowly  reduced 
by  hydrogen.  For  instance  there  are  many  organic  and  inor- 
ganic substances  which  theoretically  may  be  reduced  by  any 
system  having  the  reduction  potential  of  the  hydrogen  elec- 
trode, but  which,  nevertheless,  give  stable  and  reproducible 
potentials  as  of  the  acid-base  equilibria  of  their  solutions  and 
without  being  appreciably  reduced.  It  is  simply  that  advan- 
tage is  taken  of  the  rapidity  in  the  adjustment  of  the  acid- 
base  equilibria  and  the  comparatively  great  slowness  in  the 
adjustment  of  the  oxidation-reduction  equilibria.  One  is  almost 
afraid  to  estimate  the  limitations  which  would  be  placed  upon 
the  hydrogen  electrode  were  this  not  so.  Not  only  would 
there  be  left  hardly  a  biological  solution  suitable  for  the  measure- 
ment but  many  an  inorganic  solution  which  the  physical  chemist 
has  studied  with  the  utmost  care  and  with  supreme  confidence  in 
the  measurements  would  be  thrown  out  of  court. 

In  a  sense  we  face  a  paradox.  We  prepare  the  electrode  to 
catalyze  reduction  and  yet  must  avoid  that  "thorough"  reduction 
which  almost  inadvertently  was  specified  in  one  of  the  paragraphs 
above. 

It  is  impracticable  to  list  all  the  systems  which  are  incompatible 
with  a  hydrogen  electrode  potential.  The  practical  way  to  deal 
with  the  problem  is  to  assume  that  a  rapid  attainment  of  electrode 
equilibrium  and  its  maintenance  after  attainment  is  evidence 
that  the  small  amounts  of  oxidants  such  as  oxygen,  ferric  iron 
etc.  which  are  frequently  present,  have  been  reduced  and  that  no 
important  constituent  of  the  solution  is  "depolarizing"  the 
electrode.  :  .  •£;.§ '•$$'$ 

Evans  (1921)  has  maintained  that  in  the  electrometric  measure- 
ment of  carbonate  solutions  the  carbonate  is  reduced  to  formate 
and  that  for  this  reason  previous  measurements  of  the  pH  of 
blood  have  been  in  error.  There  are  various  reasons  for  doubting 
the  validity  of  Evans'  last  conclusion;  but,  since  the  question  is 
one  of  fact,  Cullen  and  Hastings  (1922)  have  investigated  the 
matter  and  have  failed  to  confirm  Evans.  Martin  and  Lepper 
(1926)  concur  with  others  in  believing  that  Evans  criticism  has 


XXI  ERRORS  437 

little  significance  in  measurements  of  bicarbonate  solutions  of 
ordinary  strength  but  they  believe  they  have  detected  the  forma- 
tion of  formic  acid  in  solutions  of  bicarbonate  so  dilute  (0.0002  M) 
that  the  minute  amount  of  the  stronger  acid  formed  makes  an 
appreciable  difference  in  pH.  Since  these  investigators  employed 
phenol  red  and  neutral  red  to  show  the  pH-change  and  did  not 
recognize,  or  at  least  did  not  discuss,  the  changes  which  may  take 
place  in  these  indicators  on  reduction,  their  observations  must  be 
repeated  and  their  conclusion  regarded  with  caution.  See  also 
comments  on  Evans'  objection  by  Conway-Verney  and  Bayliss 
(1923). 

Oakes  and  Salisbury  (1922)  threw  doubt  on  the  reliability  of 
the  phthalate  solution  which  Clark  and  Lubs  (1916)  recommended 
as  a  convenient  working  standard  for  checking  hydrogen  elec- 
trode measurements.  Clark  (1922)  repeated  some  experiments 
which  might  haVe  revealed  the  instability  of  the  phthalate  solu- 
tion at  the  hydrogen  electrode  but  found  no  sign  of  electrode 
drift.  See  also  Wood  and  Murdick  (1922).  Draves  and  Tartar 
(1925)  believed  they  had  shown  the  nature  of  the  discrepancy 
when  they  found  that,  under  ordinary  conditions,  the  phthalate 
solution  is  stable  but  that  with  heavy  coatings  of  platinum  black 
appreciable  reduction  of  phthalate  occurs.  Yet  Blackadder 
(1925)  refers  to  his  preference  for  very  heavy  coatings  of  platinum 
black  on  his  electrodes  and  at  another  part  of  his  paper  remarks 
that  his  measurements  "have  invariably  checked  with  the  pub- 
lished pH  figures  of  an  M/20  potassium  acid  phthalate  solution, 
namely  3.97"  (Clark  and  Lubs'  value).  Evidently  the  last  word 
on  this  subject  has  not  been  said.  However,  Clark  and  his  co- 
workers  continue  to  use  phthalate  as  a  working  standard,  having 
never  observed  discrepancies  with  highly  purified  preparations. 

The  depolarizing  action  of  such  solutions  as  those  of  ferric 
iron  is  rapid.  However,  it  is  interesting  to  note  that  the  hydrogen- 
hydrogen  ion  equilibrium  also  adjusts  rapidly,  and  that,  if  it  be 
given  its  opportunity,  it  can  compete  fairly  well.  I  once  had 
occasion  to  attempt  the  measurement  of  the  pH  value  of  a  ferric 
chlorid  solution  with  the  hydrogen  electrode!  A  reasonable 
magnitude  was  obtained  by  use  of  initial  potentials  as  the  elec- 
trode in  a  shaking  vessel  descended  into  the  solution.  Of  course 


438  THE    DETERMINATION    OF   HYDROGEN   IONS 

the  values  were  quite  unreliable  and  are  not  to  be  compared  with 
initial  potentials  taken  with  the  much  more  rapidly  adjusting 
oxidation-reduction  electrode  such  as  the  quinhydrone  electrode. 
I  would  never  have  had  the  courage  to  mention  these  very  crude 
experiments  had  Browne  (1923)  not  had  reasonable  success  with 
ferric  oxide  hydrosols  containing  small  quantities  of  ferric  chloride. 
He  presaturates  the  electrode  with  hydrogen  and  thrusts  it  into 
the  liquid,  taking  the  first  potentiometric  reading,  which  he  says 
remained  fairly  constant  for  a  few  seconds.  He  used  three  or 
four  electrodes  to  fix  the  approximate  value  for  the  setting  of  the 
potentiometer  and  then  operated  with  several  other  electrodes. 
The  effect  of  an  intense  and  active  oxidizing  agent  will  be  at 
once  recognized.  At  the  other  extreme  are  the  cases  where  no 
drift  of  the  E.M.F.  in  the  direction  of  an  oxidizing  action  at  the 
hydrogen  electrode  will  be  detected.  Between  these  extremes  lie 
the  subtle  uncertainties  which  make  it  advisable  to  check  electro- 
metric  measurements  with  indicator  measurements  and  to  apply 
tests  of  reproducibility,  of  the  effect  of  polarization,  of  the  effect 
of  time  on  drift  of  potential  and  all  other  means  available  to 
establish  the  reliability  of  an  electrometric  measurement  in  every 
doubtful  case. 

POISONS 

There  are  effects  of  unknown  cause  which  are  included  under 
the  term  "poisoned  electrodes."  An  electrode  may  be  "poisoned" 
by  a  well  defined  cause  such  as  one  of  those  to  be  mentioned 
presently;  but  occasionally  an  electrode  will  begin  to  fail  for 
reasons  which  cannot  be  traced.  There  is  hardly  any  way  of 
putting  an  observer  on  his  guard  against  this  except  to  call  his 
attention  to  the  fact  that  if  he  is  familiar  with  his  galvanometer 
he  will  notice  a  peculiar  drift  when  balancing  E.M.F.'s. 

Adsorption  of  material  by  the  platinum  black  (with  such  avidity 
sometimes  that  redeposition  of  the  black  is  necessary),  the  deposit 
of  films  of  protein,  have  been  detected  as  definite  causes  of  elec- 
trode "poisoning."  Kubelka  and  Wagner  (1926)  call  attention 
to  the  coating  of  the  electrode  by  deposits  of  colloidal  material 
in  the  solutions  they  studied.  For  rough  measurements  they 
believe  it  permissible  to  avoid  the  effects  of  such  coatings  by 
pushing  the  wire  of  the  Hildebrand  type  electrode  deeper  into  the 


XXI  ELECTRODE    POISONS  439 

solution  to  expose  new  surface.  In  measuring  a  series  of  protein 
solutions  or  other  solutions  from  which  gummy  precipitates  may 
form,  it  is  good  practice  to  make  the  measurements  in  the  order  of 
increasing  solubility.  This  will  tend  to  protect  the  electrode  from 
becoming  clogged. 

Michaelis  (1914)  places  free  ammonia  and  hydrogen  sulfid 
among  the  poisons.  However,  there  is  no  special  difficulty  in 
obtaining  hydrogen  electrode  potentials  agreeing  with  colorimetric 
measurements  in  bacterial  cultures  containing  distinct  traces  of 
ammonia  or  hydrogen  sulfid.  My  recollection  is  that  S0rensen 
has  not  expressed  worry  over  the  reliability  of  measurements  with 
protein  solutions  containing  ammonium  salts.  (See,  for  instance, 
S0rensen,  Linderstr0m-Lang  and  Lund  (1926.))  Aten  and  Van 
Ginneken  (1925)  record  consistent  values  for  the  basic  dissocia- 
tion constant  of  ammonia  as  measured  with  solutions  0.2  M  with 
respect  to  ammonia  in  ammonium  chloride  solutions.  Yet 
Prideaux  and  Gilbert  (1927)  quote  Bottger  as  saying  that  the 
hydrogen  electrode  is  untrustworthy  with  ammonia  and  some 
amines. 

Alkaloids  have  been  listed  as  electrode  "poisons."  (Isgarischev 
and  Koldaewa  (1924).)  Yet  alkaloids  have  been  titrated  fre- 
quently with  the  hydrogen  electrode  as  end  point  indicator  and 
their  dissociation  constants  have  been  measured  by  hydrogen 
electrode  equilibrium  studies  by  Prideaux  and  Gilbert  (1927). 

Britton  (1925)  finds  the  electrode  to  function  poorly  in  the 
presence  of  sulfur  and  sulphites. 

The  mercury  ions  which  may  diffuse  into  the  hydrogen  electrode 
vessel  from  the  calomel  electrode  have  been  the  cause  of  a  caution 
by  Earned  (1926)  and  by  Bovie  and  Hughes  (1923).  The  latter 
used  a  rather  drastic  means  of  prevention.  They  introduced  a 
very  thin  glass  partition  between  the  calomel  electrode  vessel  and 
the  bridge  of  pure  KC1  solution.  They  could  still  get  current 
enough  for  they  used  the  quadrant  electrometer  as  null-point 
instrument.  With  proper  design  of  the  flushing  arrangements, 
this  drastic  precaution  seems  quite  unnecessary. 

Koehler  (1920)  uses  several  cocks  and  flushing  side-tubes  for 
protection. 

Aten,  Bruin  and  Lange  (1927)  have  studied  the  poisoning  action 
of  As2O3.  They  distinguish  two  phases,  acute  and  permanent, 


440         THE  DETERMINATION  OF  HYDROGEN  IONS 

and  say  that  although  there  may  be  complete  or  partial  recovery 
from  the  first  the  permanent  effect  may  increase.  They  also  say 
that  HgCl2  behaves  like  As20a,  that  H2S  and  KCN  have  but 
slight  poisoning  effects  and  that  the  hydrolysis  of  KCN  in  solu- 
tion may  be  studied  with  the  hydrogen  electrode. 

Of  the  antiseptics  used  in  biological  solutions  Michaelis  (1914) 
states  that  neither  chloroform  nor  toluol  interfere  if  dissolved. 
Chloroform  may  hydrolyze  to  hydrochloric  acid.  Drops  of  toluol, 
however,  affect  the  electrode.  Phenol  is  permissible  but  of 
course  in  alkaline  solutions  participates  in  the  acid-base  equilibria. 
While  he  gives  no  details  Schmidt  (1916)  apparently  finds  the 
presence  of  octyl  alcohol  permissible.  This  he  uses  to  prevent 
frothing  of  protein  solutions.  Without  study  of  details  I  have 
used  octyl  alcohol  for  the  same  purpose  and  find  no  reason  to 
doubt  Schmidt's  conclusion. 

There  is  an  extensive  literature  upon  the  so-called  "poisons" 
which  interfere  with  the  catalytic  activity  of  the  finely  divided 
noble  metals  used  on  the  hydrogen  electrode.  This  literature  is 
most  suggestive,  but  there  is  still  need  for  more  direct  studies  of 
the  conditions  surrounding  the  catalytic  activity  of  the  hydrogen 
electrode. 

Simply  for  the  sake  of  clearness  we  may  distinguish  two  func- 
tions of  the  electrode.  The  electrode  is  first  of  all  a  convenient 
third  body  by  which  there  is  established  electrical  connection  with 
the  system,  hydrogen-hydrogen  ions.  That  the  equilibrium  of 
this  system  should  not  be  disturbed  by  the  presence  of  a  sub- 
stance "poisoning"  the  catalytic  activity  of  the  platinum  black 
has  been  tacitly  assumed  in  the  derivation  of  the  thermodynamic 
equation  for  electrode  potentials.  If  the  reduction  of  the  solu- 
tion could  be  accomplished  without  dependence  upon  the  catalytic 
activity  of  the  electrode,  it  should  be  theoretically  possible  to 
attain  a  true  hydrogen  electrode  potential  even  in  the  presence  of 
a  substance  acting  as  a  poison  of  catalysis. 

Aten,  Bruin  and  Lange  (1927)  say:  "In  order  to  test  whether  a 
hydrogen  electrode  is  poisoned,  a  small  quantity  of  oxygen,  for 
example  0.05  per  cent,  may  be  added  to  the  hydrogen  and  the 
effect  of  stopping  the  hydrogen  current  may  be  observed.  If  there 
is  no  rise  of  potential  in  the  first  case,  and  no  decrease  in  the 
second,  one  can  be  fairly  sure  that  there  is  no  poisoning  effect. 


XXI  EFFECT   OF   OXYGEN  441 

If  there  is  a  rjoisoning  substance  present,  the  best  way  of  working 
is  to  use  an  electrode  of  large  area,  covered  with  finely  divided 
platinum  black,  to  have  the  hydrogen  as  free  of  oxygen  as  possible 
and  to  stop  the  hydrogen  current  before  taking  a  reading." 

Hammett  (1923)  has  made  an  interesting  study  of  the  poten- 
tials of  hydrogen  electrodes  when  oxygen  in  definite  proportions 
is  added  to  the  hydrogen.  He  finds  that  the  change  of  potential 
for  any  given  percentage  of  oxygen  varies  with  the  condition  of 
the  platinum,  a  fact  which  may  be  attributed  to  variation  of  the 
catalytic  activity.  On  long  exposure  to  hydrogen  the  electrode 
becomes  so  sensitive  to  oxygen  "that  no  reasonable  precautions 
can  give  correct  results."  For  instance  in  a  phosphate  buffer 
after  an  hour  or  so  the  addition  of  0.009  per  cent  02  gave  only 
0.02  millivolt  change  and  0.43  per  cent  O2  4.0  millivolts  change. 
But  twenty  hours  later  0.048  per  cent  O2  caused  8  millivolts 
change.  The  sensitiveness  becomes  greater  in  alkaline  solution. 
Thus  the  addition  of  0.046  per  cent  02  to  the  hydrogen  gave: 

with  0.1  M  HC1  0.00  mv.  change 

with  phosphate  buffer        0.38  mv.  change 
with  0.1  N  KOH  20 .00  mv.  change 

This  is  doubtless  one  of  the  chief  reasons  for  the  difficulty  in 
making  precise  measurements  of  alkaline  solutions. 

It  is,  therefore,  appropriate  to  note  the  following  relative  rates 
of  diffusion  of  gases  through  rubber 


GAS 

KATE 

Nitrogen  

1  00 

Air  

1  15 

Oxygen  

2  56 

Hydrogen  

5  50 

Carbon  dioxide  

13  57 

In  refined  measurements  the  use  of  rubber  tubing  is  avoided 
whenever  possible.  Regarding  the  effects  of  oxygen  which  diffuses 
through  rubber  see  Biilmann  and  Jensen  (1927).  With  an 
electrode  in  0.1  N  HC1  50  cm.  of  rubber  tubing  made  a  difference 
of  0.13  millivolt.  But  see  above  for  alkaline  solutions. 

That  the  catalytic  action  of  the  "black"  need  not  be  present 


442  THE    DETERMINATION    OF   HYDROGEN   IONS 

at  the  electrode  itself  has  been  shown  by  Biilmann  and  Klit 
(1927).  They  obtain  good  hydrogen  potentials  with  blank 
platinum  when  colloidial  palladium  is  used  in  the  solution. 

In  ordinary  practice  an  electrode  is  used  not  only  as  an 
electrode  per  se  but  also  as  a  hydrogenation  catalyst.  As  such  it 
is  very  sensitive  to  "poisons."  "Poisons"  are  then  to  be  regarded 
as  the  cause  of  sluggish  electrodes.  Among  these  we  find  all 
degrees.  Hydrogenation  to  a  point  compatible  with  a  true  hydro- 
gen electrode  potential  may  be  delayed  but  slightly  and  we  may 
say  that  the  electrode  is  a  bit  slow  in  attaining  a  stable  potential 
without  our  ever  suspecting  a  "poison,"  or  the  "black"  may  be 
so  seriously  injured  that  it  becomes  entirely  impractical  to  await 
equilibrium. 

And  just  as  "poisons"  may  render  an  electrode  useless  for  prac- 
tical measurements,  so  the  employment  of  accelerators  of  catalysis 
may  promote  efficiency.  With  the  exception  of  a  brief,  unpub- 
lished note  by  Bovie  little  work  has  been  done  in  this  direction. 

The  attempt  by  Centnerszwer  and  Straumanis  (1925)  to  affect 
the  potential  of  a  hydrogen  electrode  by  radium  emanation  gave 
negative  results. 

UNBUFFERED    SOLUTIONS 

Not  infrequently  the  attempt  is  made  to  measure  potentio- 
metrically  the  pH  value  of  an  unbuffered  solution  such  as  that  of 
KC1.  It  is  not  entirely  the  fault  of  the  method  but  rather  of  the 
nature  of  the  solution  that  this  is  a  task  requiring  the  very  highest 
refinements  known  to  experimental  art.  If  for  the  sake  of  the 
argument  we  assume  that  the  solution  under  examination  is  that 
of  a  perfectly  neutral  salt  having  under  ideal  conditions  a  hydro- 
gen ion  concentration  of  0.000,000,1  N,  a  simple  calculation  will 
show  what  an  enormous  displacement  in  pH  will  be  caused  by 
the  admittance  of  the  slightest  trace  of  C02  from  the  atmosphere, 
of  alkali  from  a  glass  container,  of  impurities  occluded  in  the 
electrode  or  of  impurities  carried  into  the  solution  with  the  sol- 
vent or  solute.  Conversely,  even  if  the  measurement  were  such 
as  to  give  the  true  value  under  ideal  conditions  it  would  have 
little  practical  significance  because  of  the  difficulty  in  holding  the 
conditions  ideal. 

By  the  same  reasoning  it  appears  probable  that  it  would  be 


XXI  EFFECT  OF    C02  443 

difficult  to  obtain  true  electrode  potentials  even  with  a  potentio- 
metric  system  drawing  no  current  during  its  adjustment.  When 
no  buffer  is  present  there  is  a  negligible  reserve  of  hydrogen  ions. 
But  the  introduction  of  the  electrode  with  its  enormous  surface 
must  displace  the  equilibrium.  How  much  the  displacement 
will  be  depends  both  on  relative  proportions  of  electrode  and 
solution  and  on  the  technique  used. 

The  writer  can  see  little  practical  use  in  attempting  electrode 
measurements  with  unbuffered  solutions  and  would  prefer  in- 
direction in  the  treatment  of  certain  theoretical  matters  which 
might  be  illuminated  were  reliable  measurements  available. 

There  are  however  instances  in  which  it  is  very  desirable  to 
obtain  measurements  of  slightly  buffered  solutions.  Various  ex- 
tracts and  washings  reveal  the  condition  of  their  source  if  care- 
fully measured.  If  the  retention  of  the  acid  of  the  electrolyzing 
bath  by  the  black  of  the  electrode  can  be  avoided  and  if  the  ab- 
sorptive nature  of  the  black  can  be  reduced,  there  seems  to  be 
inherent  in  the  electrode  method  greater  delicacy  than  in  the  use 
of  very  dilute  indicator  solutions  which  are  often  the  preferred 
means  of  studying  slightly  buffered  solutions.  Beans  and  Ham- 
mett  (1925)  seem  to  have  accomplished  this  by  preparing  catalyti- 
cally  active,  smooth  deposits  of  platinum.  They  obtain  such 
deposits  by  using  pure  chloroplatinic  acid. 

PARTICIPATION   OF   C02 

From  what  has  already  been  said,  the  effect  of  the  presence  of 
oxygen  is  obvious.  Indifferent  gases  such  as  nitrogen  may  be 
considered  merely  as  diluents  of  the  hydrogen  and  as  such  must 
be  taken  into  consideration  in  accurate  estimations  of  the  partial 
pressure  of  hydrogen.  Gases  like  carbon  dioxid  on  the  other  hand 
act  not  only  as  diluents  but  also  become  components  of  any  acid- 
base  equilibrium  established  in  their  presence. 

In  very  many  instances  biological  fluids  contain  carbonate  and 
the  double  effect  of  the  carbon  dioxid  upon  the  partial  pressure 
of  the  hydrogen  and  upon  the  hydrogen  ion  equilibria  render 
accurate  measurements  difficult  unless  both  effects  are  taken  into 
consideration  and  put  under  control. 

At  high  acidities  in  the  neighborhood  of  pH  5  carbon  dioxide 
will  have  relatively  little  effect  upon  a  solution  buffered  by  other 


444  THE    DETERMINATION    OF   HYDROGEN    IONS 

than  carbonates.2  As  the  pH  of  solutions  increases,  the  participa- 
tion of  CO2  in  the  acid-base  equilibria  becomes  of  more  and  more 
importance.  The  C02  partial  pressure  in  equilibrium  with  the 
carbonates  of  a  solution  is  a  function  of  both  the  pH  and  the 
total  carbonate.  If,  however,  we  consider  for  the  sake  of  the 
argument  that  the  total  carbonate  remains  fairly  low  and  constant, 
the  C02  partial  pressure  becomes  less  with  increase  in  pH  while 
its  effect  upon  the  hydrogen  ion  equilibria  increases  with  increase 
in  pH.  Therefore  it  may  be  said  that  it  is  of  more  importance 
under  ordinary  conditions  to  maintain  the  original  C02  content 
of  the  solution  than  it  is  to  be  concerned  about  the  effect  of  CO2 
upon  the  partial  pressure  of  the  hydrogen.  Furthermore  the  effect 
of  diminishing  the  partial  pressure  of  the  hydrogen  is  of  relatively 
small  importance. 

For  these  reasons  the  bubbling  of  hydrogen  through  the  solu- 
tion is  to  be  avoided  unless  one  cares  to  determine  the  partial 
pressure  of  C02  which  must  be  introduced  into  the  hydrogen  to 
maintain  the  carbonate  equilibria  and  then  provides  the  proper 
mixture  (Hober  1903).  Cf .  Schaede,  Neukirch  and  Halpert  (1921). 
The  method  usually  employed  is  to  use  a  vessel  such  as  that  of 
Hasselbalch,  of  McClendon  or  of  Clark  in  which  a  preliminary 
sample  of  the  solution  can  be  shaken  to  provide  the  solution's 
own  partial  pressure  of  CO2,  and  in  which  there  is  provision  for 
the  introduction  of  a  fresh  sample  with  its  full  C02  pressure. 
The  hydrogen  supply  is  then  kept  at  atmospheric  pressure  and 
the  partial  pressure  of  hydrogen  in  the  electrode  vessel  is  either 
considered  to  be  unaffected  by  the  C02  pressure  or  corrected  from 
the  known  CO2  pressure  of  the  solution  under  examination. 

Another  method  is  to  employ  such  a  ratio  of  solution  volume 
to  gas  volume  that  the  loss  of  C02  from  the  solution  into  the  gas 
space  is  insignificant.  [Compare  Michaelis  (1914),  Swyngedauw 
(1927),  Etienne,  Verain  and  Bourgeaud  (1925).] 

Of  course,  in  cases  where  the  total  carbonate  in  solution  rises  to 
considerable  concentrations,  the  partial  CO2  pressure  may  become 

2  Like  so  many  problems  of  this  kind  it  can  be  adequately  solved  only 
by  use  of  quantitative  data.  No  definite  limit,  such  as  pH  =  5,  can  be 
given.  The  relative  effectiveness  of  a  given  partial  pressure  of  CO2  de- 
pends upon  the  total  carbonate  and  the  pH  region.  See  page  561.  By 
"carbonate"  is  meant  either  carbonate  or  bicarbonate. 


XXI  CRITERIA    OF   RELIABILITY  445 

of  very  significant  magnitude  and  its  effect  in  lowering  the  hydro- 
gen pressure  must  be  carefully  considered. 

With  the  demand  for  ever  higher  accuracy  in  the  study  of  solu- 
tions containing  carbonates  a  return  is  being  made  to  Hober's 
(1903)  practice  of  supplying  in  the  hydrogen  stream  or  atmos- 
phere the  desired  partial  pressure  of  C02.  See  for  instance  War- 
burg (1922)  and  Walker,  Bray  and  Johnston  (1927). 

CRITERIA   OF  RELIABILITY 

The  criteria  of  reliability  of  hydrogen  electrode  measurements 
are  difficult  to  place  upon  a  rigid  basis  but  certain  practical  tests 
are  easy  to  apply.  Reproducibility  of  an  E.  M.  F.  with  different 
electrodes  and  different  vessels  is  the  foremost  test  of  reliability, 
but  not  a  final  test.  Second  is  the  stability  of  this  E.  M.  F.  when 
attained.  In  case  flowing  hydrogen  is  used  the  potential  should 
be  the  same  with  different  rates  of  flow.  It  is  not  always  prac- 
ticable to  distinguish  between  a  drift  due  to  alteration  in  the 
difference  of  potential  at  liquid  junctions  and  a  drift  at  the  elec- 
trode but  in  most  cases  the  drift  at  the  liquid  junction  is  less  rapid 
and  less  extensive  than  a  drift  at  the  electrode  when  the  latter 
is  due  to  a  failure  to  establish  a  true  hydrogen-hydrogen  ion 
equilibrium.  A  test  which  is  sometimes  applied  is  to  polarize 
the  hydrogen  electrode  slightly  and  then  see  if  the  original 
E.  M.  F.  is  reestablished.  This  may  be  done  sufficiently  well  by 
displacing  the  E.  M.  F.  balance  in  the  potentiometer  system. 
Where  salt  and  protein  errors  do  not  interfere,  the  gross  reliability 
of  a  hydrogen  electrode  measurement  may  be  tested  colorimetri- 
cally.  This  checking  of  one  system  with  the  other  is  of  inestimable 
value  in  some  instances  as  it  has  proved  to  be  in  the  study  of  soil 
extracts.  There  the  possibilities  of  various  factors  interfering 
with  any  accurate  measurement  of  hydrogen  ion  concentration 
dimmed  the  courage  of  investigators  until  Gillespie  (1916) 
demonstrated  substantial  agreement  between  the  two  methods. 
Subsequent  correlation  of  various  phenomena  with  soil  acidity  so 
determined  has  now  established  the  usefulness  of  the  methods. 

In  addition  to  the  tests  so  far  mentioned  there  remains  the  test 
of  orderly  series.  Certain  of  the  general  relations  of  electrolytes 
are  so  well  established  that,  if  a  solution  be  titrated  with  acid  or 
alkali  and  the  resulting  pH  values  measured,  it  will  be  known 


4:46  THE    DETERMINATION    OF   HYDROGEN   IONS 

from  the  position  and  the  shape  of  the  "titration  curve"  whether 
the  pH  measurements  are  reasonable  or  not.  This  of  course  is  a 
poor  satisfaction  if  there  is  any  reason  to  doubt  the  measurements 
in  the  first  place  but  it  is  a  procedure  not  to  be  scorned. 

TEMPERATURE    VARIATIONS 

The  effect  of  temperature  variations  upon  the  accuracy  of 
electrometric  measurements  is  a  question  upon  which  it  is  difficult 
to  pass  judgment.  Of  course,  if  measurements  are  not  intended 
to  be  refined,  one  may  assume  the  temperature  of  the  room  to  be 
the  temperature  of  the  system  at  the  moment  of  the  electrical 
measurement.  It  is  then  a  simple  matter  to  select  from  tables 
the  values  and  factors  applicable  at  the  selected  temperature. 
Since  such  a  procedure  introduces  errors  which  are  not  serious 
for  many  purposes,  insistence  upon  temperature  regulation  may 
be  open  to  criticism  as  an  unnecessary  luxury.  Those  who  take 
this  position  are  doubtless  able  to  escape  the  psychological  effects 
of  uncertainty,  but  they  can  hardly  escape  the  inconvenience  of 
having  to  deal  with  new  values  and  new  factors  with  every  shift 
in  temperature.  Temperature  control  so  simplifies  rough  measure- 
ments that  much  time  is  saved,  and  for  this  reason  is  recommended 
even  when  it  is  unnecessary.  But  before  the  practice  of  neglecting 
temperature  control  can  have  scientific  standing  it  needs  more 
experimental  investigation  than  it  has  been  accorded.  Calcula- 
tions are  quite  insufficient  for  we  have  little  data  upon  the  hys- 
teresis in  the  adaptation  of  different  systems  to  temperature 
variation.  Thus  Hammett  (1922)  notes  that  although  the  cell 

Hg  |  HgCl,  KC1  (sat.)  |  HC1  (0.1  M)  |  Pt,  H2 

has  a  comparatively  small  temperature  coefficient,  it  is  very 
sensitive  to  sudden  changes  of  temperature. 

Cullen  (1922),  finding  that  the  temperature  in  an  electrode 
vessel  is  seldom  that  of  the  surrounding  air  in  a  room  subject  to 
temperature  variation,  has  devised  a  modification  of  the  Clark 
electrode  vessel  whereby  the  temperature  of  the  solution  can  be 
measured.  The  same  modification  can  easily  be  made  in  a  calomel 
electrode  vessel. 

Of  course  no  data  for  which  accuracy  is  claimed  should  ever  be 


XXI  TEMPERATURE  EFFECTS  447 

reported  without  there  having  been  temperature  control  of  appro- 
priate accuracy.  In  view  of  the  hysteresis  that  may  occur  a  mere 
record  of  the  temperature  at  a  given  moment  is  of  no  use,  nor 
is  it  worth  while  to  attempt  calculations  of  ''temperature 
corrections." 

ERRORS   WITH   THE    QUINHYDRONE    ELECTRODE 

See  Chapter  XIX,  page  414. 


CHAPTER  XXII 
TEMPERATURE  COEFFICIENTS 

An  isolated  system  obviously  cannot  be  said  to  have  reached  equilib- 
rium until  the  temperature  is  the  same  in  all  its  parts. — EASTMAN. 


In  deriving  the  type  equation 

(H+)  (A) 
(HA) 


Ka 


we  assumed  constancy  of  temperature  as  one  of  the  fundamental 
conditions.  If  this  equation  can  be  satisfied  at  one  fixed  tem- 
perature, it  is  to  be  presumed  that  it  can  be  satisfied  at  another 
fixed  temperature;  but  it  is  also  to  be  presumed  that  each  change 
in  the  temperature  to  some  new  value  will  result  in  a  new  value 
for  Ka.  Therefore  it  would  be  necessary  to  determine  the  values 
of  Ka  for  a  series  of  fixed  temperatures  if  the  temperature  coeffi- 
cient of  Ka  is  to  be  determined.  At  each  temperature  the  value 
of  Ka  would  be  determined  by  the  specific  properties  of  the  com- 
ponents of  the  system  at  that  temperature  and  the  temperature 
coefficients  of  Ka  would  not  be  predicted  from  any  universal  rule 
of  conduct  with  an  accuracy  sufficient  for  our  purposes. 

The  same  would  be  true  of  the  activities  of  the  hydrions  in  a 
solution  of  some  specific,  completely  ionized  acid. 

Most  of  the  data  of  our  subject  rest  ultimately  upon  measure- 
ments of  hydrogen  cells.  In  the  treatment  of  these  cells  it  is 
agreed  that  the  standard  of  reference  shall  be  the  so-called  normal 
hydrogen  electrode,  and  that  the  potential  of  this  electrode  shall 
be  called  zero.1  Since  this  is  our  ultimate  standard  and  since  it 

1  The  Gibbs-Helmholtz  equation  is 

T  dE       E  +  AH 
TdT=        HS 

where  E,  T,  n  and  F  have  their  customary  meanings  and  AH  is  the  increase 
in  heat  content  (see  page  238).  If,  instead  of  applying  this  to  the  whole 

448 


XXII  TEMPERATURE    COEFFICIENTS  449 

is  not  permitted  to  employ  any  of  the  ordinary  equations  except 
at  constant  temperature,  we  must  add  the  specification  that  the 
potential  of  this  electrode  is  to  be  zero  at  all  temperatures. 
However,  we  must  operate  with  some  material  system  the 
hydrion  activities  of  which  are  known  at  different  temperatures 
or  are  assumed  to  be  the  same  within  moderate  variation  of  tem- 
perature. 

It  will  be  made  plain  in  Chapter  XXIII  that  it  is  a  very  difficult 
matter  to  determine  the  hydrion  activity  of  any  actual  solution 
which  is  to  be  used  as  an  original  standard.  Nevertheless,  this 
must  be  done  if  there  is  to  be  maintained  a  consistent  use  of  the 
equation 

RT7 

-  Eh  =  — -  In 


F        (H+) 

Imagine,  for  the  sake  of  the  argument,  that  tenth  molar  hydro- 
chloric acid  solution  is  to  be  the  original  standard  and  that 
(H+)25  is  determined  for  one  temperature,  25°C.  Strictly  (H+)30, 
the  hydrion  activity  of  this  particular  solution  at  30°C.  might  be 
different.  Then  it  would  be  necessary  to  repeat  at  30°  the  method 
used  in  reaching  the  value  at  20°. 

However,  there  are  three  justifications  for  regarding  the  hydrion 
activity  in  a  dilute  hydrochloric  acid  solution  to  be  fairly  con- 
stant within  moderate  ranges  of  temperature.  The  Debye- 
Hiickel  theory  indicates  that  at  high  dilution  the  activity  coeffi- 
cient should  not  change  greatly  with  change  of  temperature. 
(See  page  500.)  •  Experimental  values  of  the  heat  of  dilution  are 
very  small  up  to  0.1  M.  Various  measurements  of  the  colligative 
properties  indicate  that  the  change  is  small.  For  these  reasons 
the  assumption  of  constant  hydrion  activity  of  a  dilute  hydro- 
chloric acid  solution  has  entered  estimates  of  various  tempera- 
ture coefficients,  notably  that  of  the  potential  of  the  tenth  normal 
calomel  half-cell. 

Before  discussing  specific  cases  it  may  be  emphasized  that  we 
are  not  at  all  concerned  with  the  absolute  temperature  coefficient 

cell,  we  write  it  for  the  normal  hydrogen  half-cell  and  define  E  =  0  and  — 

dT 

=  0,  it  follows  that  AH  =  0.     That  is,  the  change  in  heat  content  of  the 
normal  hydrogen  half-cell  is  zero  by  definition. 


450  THE    DETERMINATION    OF   HYDROGEN   IONS 

of  any  single  electrode  potential.  Since  there  is  no  way  of  measur- 
ing a  single  electrode  potential,  it  has  been  convenient  to  introduce 
the  definition  that  the  standard  selected  shall  be  zero.  Since 
none  of  the  ordinary  equations  applies  to  systems  which  are  not 
in  thermal  equilibrium  we  have  no  fundamental  interest  in 
measuring  the  difference  of  potential  between  two  half-cells  of 
the  same  composition,  each  at  a  different  temperature.  There- 
fore, there  is  added  the  specification  that  the  standard  potential 
shall  be  zero  at  all  temperatures.  There  is  a  still  more  pertinent 
reason  for  lack  of  interest  in  this  latter  type  of  experiment.  We 
have  difficulties  enough  with  liquid  junctions  without  introducing 
the  large  potentials  at  liquid  junctions  in  a  temperature  gradient. 

The  confusion  in  the  subject  should  be  apparent  if  we  now  state  that 
measurements  with  cells  not  at  thermal  equilibrium  frequently  have  been 
introduced  in  discussions  of  temperature  coefficients  of  quantities  apply- 
ing to  our  subject.  Furthermore,  in  several  of  these  discussions  the 
"normal  hydrogen  electrode"  itself  has  been  given  a  temperature  coeffi- 
cient. Thus  S0rensen  and  Linderstr0m-Lang  (1924)  say  ....  the 
hydrogen  electrode,  with  an  electrode  liquid  1  N  with  regard  to  hydrogen 
ions,  has  a  temperature  coefficient  of  almost  the  same  magnitude  as  the 
0.1  normal  calomel  electrode  .  .  .  .  "  also  they  say  "  ....  it  seems  to 
us  hardly  practical,  in  the  definition  of  TTO  (potential  of  normal  hydrogen 
electrode)  to  introduce  as  Clark2  has  done  the  supposition  that  the  poten- 
tial between  hydrogen  platinum  electrode  and  the  IN  hydrogen  ion  solu- 
tion should  be  taken  as  nil  at  all  temperatures,  since  the  whole  tempera- 
ture coefficient  of  the  cell3  would  thus  fall  upon  the  calomel  electrode,  the 
true  temperature  coefficient  of  which  is  as  mentioned  above,  quite  differ- 
ent from  that  of  the  cell." 

Also  Kolthoff  and  Tekelenburg  (1926)  say  "  .  .  :  .  the  potential  of 
the  N  hydrogen  electrode  increases  with  the  temperature."  Compare 
also  Kolthoff  and  Furman  (1926)  and  Mislowitzer  (1928). 

Since  the  problem  necessitates  the  definition  of  some  standard  of  refer- 
ence, there  seems  to  be  no  fundamental  reason  why  various  schemes  can- 
not be  devised  for  dealing  with  the  temperature  coefficients  of  cells.  How- 
ever, I  have  failed  to  find,  either  in  the  treatment  by  S0rensen  (1912), 
S0rensen  and  Linderstr0m-Lang  (1924)  or  in  the  treatment  by  Kolthoff  and 
Tekelenburg  (1927),  a  precise  definition  of  the  problem.  I  shall,  there- 
fore, refrain  from  joining  them  in  this  matter  and  shall  use  Lewis'  (1914) 
definition.  This  is,  I  believe,  the  custom  in  the  treatment  of  cells  not 

2  It  was  Lewis  (1914)  who  specified  that  the  "normal  hydrogen  electrode" 
shall  be  considered  as  having  zero  potential  at  all  temperatures. 

3  Referring  to  the  cell  Ft,  H2  j  H+  (1M)  j  KC1,  HgCl  |  Hg. 


XXII 


CALOMEL  HALF-CELL 


451 


concerned  in  pH  measurements.  Furthermore,  I  must  confess  inability 
to  trace  the  manner  in  which  either  S0rensen  and  Linderstr0m-Lang  or 
Kolthoff  and  Tekelenburg  have  utilized  their  measurements  of  cells  not 
in  thermal  equilibrium.  It  appears  to  me  that  in  the  end  the  determinative 
measurements  they  made  were  of  cells  in  thermal  equilibrium  and  that 
the  hydrion  activity  of  some  definitive  material  solution  was  either  calcu- 
lated or  assumed  to  be  the  same  at  different  temperatures.  The  poten- 
tial of  a  hydrogen  electrode  in  any  material  solution  other  than  that 
which  maintains  unit  activity  will  of  course  have  a  temperature  coefficient 
within  the  meaning  of  the  definition  adopted. 


TEMPERATURE   COEFFICIENT  FOR   THE   CALOMEL   HALF-CELL 

Lewis  and  Randall  (1914)  give  the  following  method  of  deter- 
mining the  temperature  coefficient  for  the  tenth-normal  KC1 
calomel  half-cell. 


FIG.  81.  ELECTKOMOTIVE  FORCES,  E,  AT  TEMPERATURES  t°C.  FOR  THE  CELL 
-Pt,  H2  (1  atmos.)  |  HC1  (0.1  M),  HgCl  |  Hg+ 

Figure  81  depicts  the  change  of  potential  of  the  celt 

-Pt,  H2 1  HC1  (0.1  M),  HgCl  |  Hg+  I 

when,  in  each  case  at  constant  temperature,  the  potentials  of  the 
cell  are  measured  at  different  temperatures. 

The  data  led  Lewis  and  Randall  (1914)  to  the  empirical  equation 

Ej  =  0.0964  +  0.001881  T  -  0.000,002,90  T2  (1) 

Differentiation  of  (1)  gives 


dT 


=  0.001,881  -  0.000,005,80  T 


(2) 


452        THE  DETERMINATION  OF  HYDROGEN  IONS 

As  was  stated  before,  the  temperature  coefficient  of  the  poten- 
tial of  the  half-cell 

Pt,  H2 1  HC1  (0.1  M) 

should,  in  strictness,  be  determined  experimentally  (by  some 
procedure  such  as  is  outlined  in  Chapter  XXIII) .  However,  in  the 
absence  of  adequate  data,  Lewis  and  Randall  assume  that  for 
moderate  changes  of  temperature  the  hydrion  activity  in  0.1  M 
HC1  will  remain  a  constant,  C.  The  potential  of  this  half-cell 
is  given  by 

Eh  =  0.000,198,322  T  log  C  (3) 

Lewis  and  Randall  used  for  Eh  the  value  —0.0684  at  25°.  In- 
troduce Eh  =  -0.0684  and  T  -  273.1  +  25  into  (3)  and  solve 
for  log  C.  This  gives:  log  C  =  -1.15696.  Introduce  this 
value  in  (3)  and  differentiate  to  obtain : 

AEh 

~^-=  ~  0.000229  (4) 

This  is  the  temperature  coefficient  of  the  potential  at  the  plati- 
num electrode  of  cell  I,  the  over-all  temperature  coefficient  of 
which  is  given  by  equation  (2).  Consequently  0.000229  must 
be  subtracted  from  the  right  of  equation  (2)  to  yield  in  (5)  the 
temperature  coefficient  of  the  calomel  half -cell  with  0.1  M  HCL 
We  shall  round  off  the  numbers  and  use : 

dE 

—  =  0.00165  -  0.000,005,80  T  (5) 

a! 

Lewis  and  Randall  assume  that  (2)  will  apply  also  to  the  cell 
-  Pt,  H2 1  HC1  (0.1  M)  ||  KC1  (0.1  M),  HgCl    Hg+       III 

Consequently  (5)  gives  the  temperature  coefficient  of  the  half- 
cell 

||KC1  (0.1  M),  HgCl|Hg  IV 

Equation  (5)  is  the  differential  of  (6) 

Ec  =  Eoc  +  0.00165  T  -  0.000,002,90  T2  (6) 


XXII 


CALOMEL   HALF-CELL 


453 


Eoc  can  be  found  by  taking  either  S0rensen's  value  Ec  =  0.3380 
for  18°C.  or  the  value  0.3353  at  25°  from  table  61  (see  page  472). 
Then  the  values  of  Ec  at  different  temperatures  may  be  calcu- 
lated. 

In  Chapter  XXIII  are  presented  arguments  leading  to  the  use 
of  a  standardized  value  for  the  standard  half-cell  :- 

||  KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg  V 

Assuming  that  the  temperature  coefficient  of  half-cell  IV  applies 
to  the  standard  half-cell  V  and  adopting  S0rensen's  value  for 

TABLE  57 

Values  of  calomel  half-cells  at  different  temperatures 
Half-cell  IV  ||  KC1  (0.1  M),  HgCl  |  Hg 
Half-cell    V  ||  KC1  (sat.)      |  KC1  (0.1  N),  HgCl  |  Hg 
Half-cell  VI  ||  KC1  (0.1  N)  |  KC1  (1.0  N),  HgCl  J  Hg 


' 

HALF-CELL  IV 
USING  0.3353 
AT  25° 

HALF-CELL  V 
(S0RENSEN) 
CALCULATED 

HALF-CELL  V 

(S0RENSEN) 
FOUND 

HALF-CELL  VI 

(S0REN8EN  BASIS) 

18 

0.3357 

0.3380 

0.3380 

0.2865 

20 

0.3356 

0.3379 

0.3378 

0.2860 

25 

0.3353 

0.3376 

0.2848 

30 

0.3348 

0.3371 

0.3370 

0.2835 

35 

0.3365 

38 

0.3361 

40 

0.3335 

0.3358 

0.3359 

50 

(0.3315) 

(0.3338) 

0.3344 

18°  as  a  point  of  reference,  we  obtain  the  values  for  the  standard 
half-cell  V  shown  in  table  57. 
For  the  cell 

-  Hg  |  HgCl,  KC1  (l.ON)  |  KC1  (0.1N),  HgCl  |  Hg  + 

the  author  finds  at  20°  0.0519,  and  at  30°  0.0536.  Interpolation 
between  these  values  on  the  assumption  that  the  E.  M.  F.  is  a 
linear  function  of  the  temperature  gives  an  E.  M.  F.  at  25° 
which  is  within  0.15  millivolts  of  that  found  by  Lewis,  Brighton 
and  Sebastian  for  a  similar  cell  with  molal  and  0.1  molal  KC1 
and  a  linear  temperature  coefficient  of  0.000,17.  Sauer's  value 


454         THE  DETERMINATION  OF  HYDROGEN  IONS 

at  18°  is  0.0514  and  that  of  Fales  and  Vosburgh  at  25°  is  0.0524. 
Neither  of  these  values  falls  in  with  those  mentioned  above  but 
when  taken  by  themselves  and  with  the  15°  value,  0.0509,  given 
in  the  footnote  of  the  paper  by  Fales  and  Vosburgh  (1918)  they 
furnish  a  temperature  coefficient  of  the  same  order. 

With  these  data  we  can  calculate  the  value  of  the  half  -cell 

||  KC1  (0.1  N)  |  KC1  (1.0  N),  HgCl  |  Hg  VI 

from  the  standardized  value  of  the  "  tenth  normal"  calomel 
half-cell. 

For  the  potential  of  the  saturated  KC1  calomel  half-cell  Michaelis 
(1914)  gives  values  at  different  temperatures  which  are  not  quite 
a  linear  function  of  temperature.  Vellinger  (1926)  finds  a  linear 
relation.  Neither  author  gives  all  the  details  of  the  method  of 
reference.  Fales  and  Mudge  (1920)  report  potentials  at  different 
temperatures  for  the  cell 

•-  Pt,  H2  1  HC1  (0.1  M)  |  KC1  (sat.),  HgCl  |  Hg  + 

The  temperature  coefficient  of  this  cell  was  almost  linear.  If,  as 
was  done  in  calculating  the  temperature  coefficient  for  the 
0.1  N  KC1  calomel  half  -cell,  we  assume  that  the  potential  of  the 
hydrogen  electrode  in  0.1  M  HC1  becomes  more  negative  by 
0.00023  volts  per  degree  increase  of  temperature  we  calculate 
from  the  data  of  Fales  and  Mudge  the  following  approximate 
temperature  coefficients. 


-  =  -0.000,788  between  25°  and  40° 
dt 

—  =  -0.000,695  between  40°  and  60° 
dt 

—  =  -0.000,75    between  25°  and  60°  by  best  curve 
dt 

A  best  straight  line  through  Michaelis'  data  gives  —0.000,761. 
Vellinger  gives  -0.000,66. 

Fales  and  Mudge  (1920)  give  only  their  value  at  25°  as  re- 
liable4 for  the  potential  between  the  0.1M  calomel  half-cell  and 

4  They  did  not  adequately  protect  their  half-cells  from  interdiffusion. 


XXII 


SATURATED    CALOMEL   HALF-CELL 


455 


the  saturated  calomel  half-cell.     They  report  as  the  average  of 
36  cells  0.0918±0.0002.     If  we  use  0.3376  for  the  half-cell 

||  KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 
we  obtain  0.2458  =t  0.0002  for  the  half-cell1 
||KCl(sat.),HgCl|Hg 

This  is  practically  the  same  as  the  value  0.2457  for  25°  re- 
ported by  Vellinger,  0.2458  (0.2460  corrected  to  our  value  for 
the  tenth  normal)  reported  by  Michaelis  and  0.2454  Scatchard 
(see  page  470).  We  shall  use  0.2458  at  25°  as  an  orienting  value. 

The  several  temperature  coefficients  are  not  in  adequate  agree- 
ment for  the  satisfactory  calculation  of  values  for  other  tempera- 


tures.    If,  however,  we  use  - 

dt 


-0.000,76  (the  average  of 


Michaelis'  and  Fales  and  Mudge's  values  for  the  lower  tempera- 
tures) we  obtain  the  values  of  the  following  table. 

TABLE  58 

Tentative  values  for  the  cell 
IIKC1  (sat.),  HgCl  !  Hg 


t 

E 

t 

E 

18 

0.2511 

30 

0.2420 

20 

0.2496 

35 

0.2382 

25 

0.2458 

38 

0.2359 

40 

0.2344 

At  38°  the  value  in  the  table  is  0.0013  volt  lower  than  that  of 
Vellinger  and  0.0009  volt  higher  than  that  of  Michaelis. 

Tentatively  it  will  be  wise  to  use  the  above  values  as  approxi- 
mations and  to  standardize  each  saturated  half-cell  as  used. 

It  is  interesting  to  note  that  the  saturated  calomel  half-cell 
has  a  large  temperature  coefficient  and,  by  reason  of  its  nature, 
is  especially  subject  to  hysteresis.  Temperature  fluctuations 
therefore  jeopardize  accurate  measurements.  On  the  other  hand 
the  potential  of  a  cell  composed  of  a  hydrogen  or  quinhydrone 
half-cell  and  a  saturated  KC1  calomel  half-cell  has  a  small  tem- 
perature coefficient  so  that,  if  constant  temperature  prevail,  the 


456         THE  DETERMINATION  OF  HYDROGEN  IONS 

temperature  value  may  be  in  considerable  error  without  causing 
great  error  in  the  potential.  The  error  then  incident  to  the 
mistaken  temperature  lies  in  the  use  of  the  wrong  temperature 
factor. 

TEMPERATURE    COEFFICIENTS   FOR    BUFFER    SOLUTIONS 

In  the  standardization  of  buffer  solutions,  cells  of  the  type 
given  below  were  used  directly  or  indirectly  by  S0rensen  (1909), 
Clark  and  Lubs  (1916),  Walbum  (1920)  and  others. 


-  Pt,  H2  (1  atmos.) 


Buffer 
Solution 


KC1 

(sat.) 


KC1 
(0.1  N) 


,HgCl 


B  C  D 


If,  at  a  given  temperature,  the  electromotive  force  of  the  cell 
is  measured,  the  potential  at  A  is  readily  calculated  when  the 
potential  of  the  half-cell 

||  KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 

at  the  given  temperature  is  known  and  the  potential  of  B  is  zero. 

In  Chapter  XXIII  it  will  be  recommended  that  variation  of  the 
potential  at  B  be  neglected  and  that  the  algebraic  sum  of  the 
potentials  at  B,  C  and  D  be  regarded  as  the  potential  of  the  so- 
called  tenth  normal  calomel  electrode  as  it  has  been  applied  in 
these  instances.  The  previous  section  gives  the  standardized 
values  of  this  half-cell  at  various  temperatures. 

This  procedure  standardizes  an  arbitrary  method  of  computing 
the  potential  at  A. 

The  so-called  pH-values  of  buffer  solutions  are  calculated  from 
the  relation 

—  potential  at  A 


pH  = 


0.000,198,322  T 


This  gives  a  definite  methodical  meaning  to  pH  values.  The 
pH  values  of  any  given  buffer  solution  at  stated'  temperatures 
must  then  be  determined  experimentally  by  the  standardized 
procedure.  Such  essentially  is  the  procedure  followed  by  Wal- 
bum. His  values  are  found  in  Chapter  IX. 

Kolthoff   and   Tekelenburg   (1927)    have  stated  an  extensive 


XXII 


BUFFERS 


457 


TABLE  59 

Kolthoff  and  Tekelenburg's  data  for  pH  values  of  buffers  at  different 

temperatures 


BUFFER 

TEMPERATURE 

pH 

(HYDROGEN  ELECTRODE 
SERIES) 

•c. 

0.  1  M  acetic  acid 

25 

4.60 

0.1  M  sodium  acetate 

40 

4.61 

50 

4.63 

Mono  sodium  citrate  0.1  M 

18 

3.66 

30 

3.65 

40 

3.65 

50 

3.66 

60 

3.65 

Di  sodium  citrate  0.1  M 

20 

4.96* 

30 

4.96 

40 

4.96 

50 

4.97 

Acid  potassium  phthalate  0.05  M 

18 

3.92 

30 

3.92 

* 

40 

3.93 

50 

3.94 

60 

3.94 

Sprensen's  "citrate  4.45" 

18 

4.45 

30 

4.43 

40 

4.41 

50 

4.40 

« 

60 

4.40 

S0rensen's  "Glycine—  HC1  2.28" 

18 

2.26 

30 

2.25 

40 

2.25 

50 

2.25 

0.15M  Na2HPO4 

25 

11.29 

0.1    MNaOH 

40 

11.08 

*  Compare  Walbum.     See  page  211, 


458         THE  DETERMINATION  OF  HYDROGEN  IONS 

series  of  pH  values  for  various  buffer  mixtures  at  different  tem- 
peratures. They  state  that  they  "have  made  a  thorough  in- 
vestigation" of  the  temperature  coefficients  of  "the  hydro  gen- 
and  quinhydrone  electrodes"  but  the  details  are  contained  in 
Tekelenburg's  dissertation  (1926)  and  have  not  been  available 
to  me.  It  appears  that  although  they  give  an  extensive  dis- 
cussion of  the  absolute  temperature  coefficients  of  various  half- 
cells,  measured  without  thermal  equilibrium  of  the  cell  as  a 
whole,  Kolthoff  and  Tekelenburg  assumed  pH  2.038  as  the  value 
of  0.01  N  HC1  +  0.09  N  KC1  at  all  temperatures  (?). 

As  already  indicated  a  similar  assumption  of  the  constancy  of 
the  hydrion  activity  of  a  hydrochloric  acid  solution  entered 
Lewis'  derivation.  It  is,  therefore,  not  improbable  that  the  data 
of  Kolthoff  and  Tekelenburg  finally  are  in  terms  of  the  system 
here  recommended  so  far  as  temperature  coefficients  are  con- 
cerned. 

Representative  data  from  their  paper  are  given  in  table  59. 

By  reason  of  a  departure  from  usual  methods  of  standardization 
Kolthoff  and  Tekelenburg's  pH  values  are  somewhat  lower  than 
usual.  This  should  not  affect  the  temperature  coefficients. 

Hastings  and  Sendroy  (1924)  have  obtained  the  data  for 
phosphate  solutions  at  20°  and  38°  which  are  tabulated  on 
page  212. 

TEMPERATURE   COEFFICIENTS   OF  INDICATOR   CONSTANTS 

•  In  the  older  literature  very  little  was  said  of  the  effect  of  tem- 
perature variation. 

Kolthoff  (1921)  has  extended  the  theory  of  Schoorl  in  which 
account  is  taken  of  the  acidic  or  basic  nature  of  an  indicator, 
but  there  often  remains  some  question  as  to  how  a  given  indicator 
is  to  be  classified.  Kolthoff,  using  the  values  of  Kohlrausch  and 
Heydweiller  for  the  dissociation  constant  of  water  at  various 
temperatures,  has  reduced  his  observations  to  the  following 
table.  In  this  table  the  displacement  of  —0.4  for  the  thymol 
blue  means  that  if  thymol  blue  in  a  solution  at  70° C.  shows  the 
same  color  as  the  same  concentration  of  this  indicator  in  a  buffer 
of  pH  9.4  at  ordinary  temperature  then  the  pH  of  the  solution 
at  70°C.  is  9.0.  Corrections  for  temperatures  between  room 


XXII 


INDICATORS 


459 


temperature  and  70°C.  may  be  interpolated  from  the  data  in  the 
table. 

In  determining  their  temperature  coefficients  for  indicator 
constants  Michaelis  and  Gyemant  (1920)  (see  page  129)  assumed 
constancy  in  the  pH  of  acetate  buffers  used  with  p-nitrophenol 
In  the  study  of  m-nitrophenol  they  used  phosphate  buffers  to  the 
pH  values  of  which  they  ascribed  a  temperature  coefficient  based 
on  the  work  of  Michaelis  and  Garmendia.  They  also  used  a 

TABLE  60 
Displacement  of  indicator  exponent  between  18°C.  and  70°C.  after  Kolthoff 


INDICATOR 

pH 

DISPLACEMENT 

pOH 

DISPLACEMENT 

KATIO  OF 
DISSOCIATION 
CONSTANT  AT 
70°C.  TO  THAT 
AT  ORDINARY 
TEMPERATURE 

Nitramine 

—  1  45 

0  0 

1  0 

Phenol  phthalein  

-0  9  to  0  4 

—0  55tol  05 

About  5 

Thymol  blue,  alkaline  range  .  .  . 
a-naphthol  phthalein  

-0.4 
-0  4 

-1.05 
-1  05 

2.5 

2  5 

Curcumine  

-0.4 

-1.05 

2  5 

Phenol  red 

—0  3 

—  1  15 

2  0 

Neutral  red  

-0  7 

-0  75 

Brom  cresol  purple 

0  0 

-1  45 

1  0 

Azolitmin 

0  0 

—  1  45 

1  0 

Methyl  red  

—0  2 

-1  25 

Lacmoid 

—0  4 

—  1  05 

2  5 

p-nitro  phenol  

-0  5 

—0  95 

3  2 

Methyl  orange  .  . 

-0  3 

—  1  15 

14  0 

Butter  yellow  

-0.18 

-1  17 

15  0 

Bromphenol  blue  

0  0 

—  1  45 

1  0 

Tropaeolin  OO 

-0  45 

-1  0 

10  0 

Thymol  blue,  acid  range  

0.0 

-1.45 

1.0 

temperature  coefficient  for  borate  buffers  in  determining,  for 
instance,  the  temperature  coefficients  for  salicyl  yellow.  The 
original  articles  must  be  consulted  for  the  somewhat  involved 
detail. 

Hastings  and  Sendroy  (1924)  and  Hastings,  Sendroy  and  Rob- 
son  (1925)  have  systematized  the  Gillespie  method  as  applied  by 
Cullen  (1922),  see  also  Austin,  Stadie  and  Robinson  (1925). 
They  determined  anew  the  pH  values  of  phosphate  buffers  (see 


460 


THE  DETERMINATION  OF  HYDROGEN  IONS 


page  212)  at  20°  and  38°  and  of  acetate  buffers  at  20°.  In  the 
latter  case  they  assumed  no  change  of  pH  with  change  of  tem- 
perature to  38°C.  In  these  standardizations  0.1  N  HC1  with 
assigned  value  of  pH  1.08  was  employed.  They  obtain  the 
pK'  values  of  the  following  table: 

Indicator  exponents  at  different  temperatures 


INDICATOR 

*< 

P< 

Phenol  red. 

7  78 

7  65 

Brorn  cresol  purple 

6  19 

6  09 

Chlor  phenol  red 

6  02 

5  93 

Brom  cresol  green  

4.72 

4.72 

Compare  these  with  values  of  table  11,  page  94.  See  figure 
18,  page  103. 

TEMPERATURE   COEFFICIENTS   OF  OTHER   EQUILIBRIUM    CONSTANTS 

In  the  older  literature  are  to  be  found  numerous  measurements 
of  the  temperature  coefficients  of  acid  and  base  dissociation  con- 
stants. These  were  based  upon  conductivity,  for  the  most  part. 
Extensive  data  are  assembled  by  Scudder  (1914)  and  in  Landolt- 
Bornstein's  Tabellen  (1923). 

See  page  45  for  estimates  of  Kw  at  different  temperatures. 

TEMPERATURE    COEFFICIENTS    OF    QUINHYDRONE    ELECTRODE 

POTENTIALS 


See  page  419. 


CONCLUSION 


At  the  present  time  the  lack  of  sufficiently  extensive  systematic 
data  has  made  necessary  various  and  divers  assumptions  by 
different  authors  who  have  dealt  with  the  temperature  coeffi- 
cients of  the  quantities  briefly  treated  in  this  chapter.  By  reason 
of  the  variety  of  these  assumptions  and,  in  many  cases,  the  lack 
of  sufficiently  specific  detail,  it  is  impracticable  to  systematize  the 
existing  data.  The  operator  must  choose  his  system  and  should 
state  in  detail  the  assumptions  he  makes. 


CHAPTER  XXIII 

STANDARDIZATION  OF  pH  MEASUREMENTS 

//  there  is  a  service  which  philosophy  can  render  with  more  advan- 
tage to  science  than  any  other,  it  is  probably  to  keep  reminding 
men  of  science  never  to  forget  to  criticise  their  categories  before 
employing  them.  —  VISCOUNT  HALDANE. 

In  the  development  of  the  theory  of  electrolytic  dissociation 
the  hydrogen  electrode  came  upon  the  scene  comparatively  late 
and  after  many  of  the  quantitative  relations  had  been  outlined 
by  conductance  data.  It  was,  therefore,  natural  that  these  data 
should  have  been  accepted  in  the  standardization  of  poten- 
tiometric  measurements.  It  now  appears  that  the  interpretation 
of  conductance  data  is  more  complicated  than  at  first  supposed 
and  that  certain  of  the  values  that  have  been  used  in  the  stand- 
ardization of  potentiometric  measurements  are  in  doubt.  Also, 
it  is  now  recognized  that  the  hydrogen  cell  does  not  directly  give 
information  upon  relative  hydrion  concentrations.  The  result- 
ing confusion  demands  careful  consideration. 

Let  us  review  briefly  the  way  in  which  conductance  data  entered 
the  standardization  of  potentiometric  measurements. 

Assume,  first,  the  validity  of  the  ideal  gas  laws.  Then  the 
following  equation  relates  the  electromotive  force  of  a  hydrogen 
cell  to  the  concentrations  of  hydrions  in  solutions  1  and  2,  pro- 
vided the  hydrogen  partial  pressure  is  the  same  at  each  electrode. 


By  use  of  this  relation  one  can  determine  in  the  first  instance  only 
the  ratio  of  two  hydrogen  ion  concentrations.  If  the  value  of 
either  [H+]i  or  [H+]2  is  to  be  found,  the  value  of  the  other  must 
be  known.  Conductance  data  have  been  relied  upon  to  furnish 
one  known. 

Likewise,  when  there  is  used  a  cell  composed  of  a  calomel  half- 
cell  and  a  hydrogen  half-cell,  the  value  assigned  to  the  calomel 

461 


462  THE    DETERMINATION    OF   HYDROGEN    IONS 

half-cell  is  such  that,  when  it  is  subtracted  from  the  total  E.M.F. 
of  the  cell,  the  resulting  E.M.F.  is  as  if  between  a  normal  hydro- 
gen electrode  and  the  hydrogen  electrode  under  measurement. 
This  implies  the  experimental  determination  of  the  difference  of 
potential  between  a  normal  hydrogen  electrode  and  the  calomel 
electrode  or  else  between  the  calomel  electrode  and  a  hydrogen 
electrode  in  some  solution  of  known  hydrogen  ion  concentration. 
To  determine  this  known  hydrogen  ion  concentration  conduct- 
ance data  upon  hydrochloric  acid  solutions  have  been  relied 
upon. 

Only  when  some  standard  of  reference  is  agreed  upon,  can  [H+]i, 
of  equation  (1),  be  set  at  unity  and  the  equation  written: 

E.  M.  F.  X  F  _J_ 

2.3026  RT          °g  [H+j 

or 

E.  M.  F. 

=  pH  (2a) 


0.000,198,322  T 

The  principle  which  was  assumed  in  the  use  of  the  conductivity 
method  may  be  described  briefly  as  follows. 

With  a  given  potential  gradient  between  two  fixed  electrodes, 
the  current  carried  by  the  ions  in  the  solution  should  be  a  direct 
function  of  the  number  of  equivalents  of  ions  and  of  the  speeds  of 
their  ionic  migrations.  If,  independent  of  the  dilution,  each  of 
the  several  kinds  of  ions  has  its  fixed  migratory  speed  under  the 
given  potential  gradient,  the  current  becomes  a  measure  of  the 
number  of  equivalents  of  carrying  ions.  Suppose  then  that  the 
solution  has  been  diluted  until  its  solute,  an  ionogen  acid,  has 
attained  complete  dissociation.  Further  dilution  does  not  in- 
crease the  proportion  of  ions  to  total  acid  and  the  current,  per 
equivalent  of  acid,  per  unit  volume,  under  the  given  conditions, 
becomes  constant.  While  complete  dissociation  was  not  sup- 
posed to  occur  until  infinite  dilution  was  reached,  we  shall  assume 
that  the  means  of  extrapolating  to  this  condition  were  adequate. 
Then  for  a  simple  acid,  of  type  HA,  the  ratio  of  equivalent 
conductance  at  a  given  concentration,  to  the  equivalent  conduct- 
ance at  infinite  dilution  should  give  a,  the  degree  of  dissociation. 


XXIII  STANDARDIZATION  463 

It  is  then  a  simple  matter  to  calculate  the  hydrogen  ion  concen- 
tration. 

We  have  already  noted  that  attempts  to  apply  this  idea  of 
progressive  ionization  to  strong  acids  in  solution  rested  upon  a 
misconception  of  the  nature  of  strong  acids.  But  in  addition 
there  is  the  view,  outlined  in  Chapter  XXV,  that,  although  ions 
in  solution  may  be  regarded  as  free  and  separate  entities  in  the 
sense  that  they  have  departed  from  fixed  combinations  in  their 
ionogens,  they  are  still  subject  to  an  interionic  force.  On  dilu- 
tion the  effect  of  this  becomes  less.  Under  the  stress  of  an  elec- 
tric field  the  ion  groups  become  distorted  and  the  fields  between 
them  and  the  solvent  molecules  change  from  point  to  point  of  the 
migration.  The  energy  involved  varies  with  the  density  of  the 
ion  atmosphere  (i.e.,  with  dilution)  and  enters  the  formulation 
of  conductance  in  a  complicated  manner.  It  appears  as  if  the 
ions  of  a  given  kind  have  migratory  speeds  which  vary  with  the 
composition  (e.g.,  dilution)  of  the  solution.  Therefore,  one  of 
the  important  postulates  of  the  classical  theory  fails.  Jahn 
(1900)  and  Lewis  (1912)  long  ago  noted  the  discrepancies  and  ex- 
pressed them  as  the  failure  of  the  postulate  of  constant  migratory 
speed.  For  a  discussion  of  the  matter  in  terms  of  Debye's 
treatment  see  Debye  (1927)  and  Onsager  (1927)  (see  references 
under  Faraday  Society). 

The  remodeling  of  the  theory  of  conduction  in  solution  has  left 
open  to  serious  doubt  the  older  values  for  hydrogen  ion  concen- 
trations in  specific  solutions. 

But  let  us  suppose  that  adequate  methods  are  available  for 
determining  the  hydrogen  ion  concentration  of  some  solution  to 
be  used  as  a  standard  for  hydrogen  electrode  comparisons.  Is 
the  problem  solved?  It  is  not.  It  will  be  recalled  that  the 
potentiometric  method,  employed  in  the  use  of  the  hydrogen 
electrode,  measures  the  free  energy  of  transport  of  hydrogen  ions 
between  two  solutions.  There  is  no  simple,  general  relation  be- 
tween this  free  energy  change  and  the  corresponding  change  in 
concentration.  As  explained  in  Chapter  XI,  solutions  of  differ- 
ent composition  have  different  constraints  upon  the  ease  with 
which  hydrogen  ions  may  be  removed.  This  necessitates  the 
inclusion  of  a  correction  term  specific  for  each  member  of  a  pair 
of  solutions  when  the  energy  equation  for  a  "concentration"  cell 
is  formulated  in  the  classical  manner. 


464         THE  DETERMINATION  OF  HYDROGEN  IONS 

The  more  extensive  and  accurate  data  which  bear  upon  our 
subject  are  those  obtained  with  solutions  of  hydrochloric  acid. 
But  both  experiment  and  the  Debye-Hiickel  equation  show  that 
the  correction  cannot  be  eliminated  in  the  range  of  concentration 
of  hydrochloric  acid  solutions  within  which  it  is  practicable  to  op- 
erate. In  other  words  it  is  impossible  in  the  first  instance  to 
calculate  a  definite  electrode  potential  by  reference  alone  to  a 
unit  concentration  of  HCL  We  have  to  console  ourselves  with 
the  remembrance  that  the  correction  disappears  only  at  infinite 
dilution.  The  problem  then  is  to  establish  a  substantial  basic 
datum  with  that  somewhat  unsubstantial  hydrochloric  acid  solu- 
tion of  zero  concentration  !  Obviously  the  only  way  this  can  be 
done  is  to  extrapolate  some  function  to  the  condition  of  zero 
concentration.  How  this  is  done  and  what  function  is  used  will 
appear  presently. 

By  way  of  illustration  one  of  many  routes  will  now  be  followed 
to  specifications  which  could  serve  in  the  standardization  of  pH 
measurements. 

Consider  the  cell: 

-  Pt,  H2  1  HC1,  AgCl  |  Ag  +, 

namely  a  hydrogen  electrode  and  a  silver-silver  chloride  electrode 
both  in  contact  with  the  same  solution  of  hydrochloric  acid.  Since 
no  appreciable  liquid-junction  potential  is  concerned  and  since 
the  silver-silver  chloride  electrode  is  probably  better  than  the 
calomel  electrode  for  use  with  the  hydrogen  electrode  in  acid 
solution,  there  is  a  distinct  advantage  in  considering  this  cell  first. 
At  the  hydrogen  electrode  the  single  potential  difference  may  be 
formulated  by  equation  (3)  where  a  constant,  E'H,  is  included 
because  no  standard  of  potential-difference  has  yet  been  defined. 

VH  (3) 


VH  is  a  variable  correction  introduced  to  allow  for  the  failure  of 
the  classical  equation. 

At  the  silver  electrode  the  potential  difference  may  be  formu- 
lated in  its  lowest  terms  by: 

•' 

Cl-l-VA.  (4) 


XXIII  STANDARDIZATION  465 

Here  again  a  variable  correction,  VAg,  is  introduced  to  allow  for 
the  failure  of  the  classical  equation  which  is  based  on  the  ideal 
gas  laws. 

At  unit  hydrogen  pressure,  when  P  =  1,  we  have  for  the  cell 
as  a  whole  (silver  positive  to  platinum): 


EA.  -  EH  =  Ei,  -  EH  -    ~  In  [H+]  [C1-]  -  VAe  -  VH  (5) 

X1 

In  accord  with  a  rather  widely  accepted  conclusion  we  shall 
now  assume  that  hydrochloric  acid  is  completely  dissociated 
within  the  range  of  concentration  to  be  considered.  Then 

[H+]  [C1-]  -  [HClp 

where  [HC1]  represents  simply  the  analytical  concentration  of 
hydrochloric  acid  without  specification  of  its  state. 

Introducing  this  assumption  and  using  the  numerical  form  of 
the  equation  for  25°C.,  we  have 

EAg  -  EH  =  E'AS  -  E'H  -  0.11824  log  [HC1]  -  VAe  -  VH     (6) 
or 
-  EH  =  E'Ag  -  E'H  -  0.05912  log  [H+]  -  0.05912  log  [Cl]  -  VAg  -  VH     (6a) 

In  figure  82  experimental  values  for  EAg  —  EH,  as  assembled  by 
Scatchard  (1925),  are  charted  as  the  curve  labeled  A.  To 
harmonize  with  a  subsequent  figure,  the  abscissa  is  made  the 
square  root  of  the  molality  of  the  hydrochloric  acid  solution. 

If  the  classical  equations  were  followed  VAg  and  VH  of  equation 
(6a)  would  each  be  zero.  Then,  if  complete  dissociation  of  hydro- 
chloric acid  were  assumed,  the  values  of  [H+]  and  [Cl~]  could  be 
calculated  from  the  known  molality  of  the  hydrochloric  acid 
solution.  Then,  since  EAg  —  EH  has  been  determined  in  each 
instance,  the  equation  can  be  solved  for  E'Ag  —  E'H.  This  con- 
stant value  should  determine  the  level  of  a  line  such  as  that  shown 
in  figure  82  at  0.2226  volts.  Line  B.  It  is  evident  that  E'Ag  -  E'H, 
when  so  calculated  ^y  neglect  of  VAg  and  VH,  furnishes  data  which 
do  not  conform  to  this  reference  line  at  0.2226. 

Since  the  corrections  disappear  at  infinite  dilution,  a  curve 
drawn  through  the  blackened  cycles  should  meet  the  desired 


466 


THE   DETERMINATION    OF   HYDROGEN   IONS 


base  line  at  M  =  0.     The  problem  is  thus  resolved  into  the  diffi- 
cult task  of  extrapolating  this  to  M  =  0  or  V£  =  0. 

To  this  problem  we  shall  revert  presently.  For  the  moment 
assume  that  the  extrapolation  has  been  carried  out  correctly  and 
that  the  intersection  has  been  found  to  be  at  0.2226  volt.  This  is 
value  of  E'AE  —  E'H  in  equation  (6).  Now  introduce  the  defini- 


.5 


.4 


.2226 
.2 


1COT  .1 

FIG.  82.  CURVE  A:  ELECTROMOTIVE  FORCE  E  AT  VARIOUS  VALUES  OF 

VM  FOR  THE  CELL 

Ft,  H2  (1  atmos.)  |  HC1  (X),  AgCJ  |  Ag 
V/*  =  Vmolality  of  HC1.    Curve  B:  EAS'  -  EH'. 

tion  of  the  normal  hydrogen  electrode  given  on  page  257;  but, 
for  the  convenience  of  the  present  purpose,  recast  the  definition 
to  the  following.  The  normal  hydrogen  electrode  shall  have  a 
single  potential  difference  of  zero  when  the  hydrogen  pressure  is 
one  atmosphere  and  the  concentration  of  hydrogen  ions  is  such 
that 

In  [H+]  +  VH  =  0 


XXIII 


STANDARDIZATION 


467 


As  a  result  of  this  definition  it  will  be  seen  from  equation  (3) 
that  E'H  is  zero  by  definition.  Consequently  the  value  of  E'Ag 
—  E'H  in  (6)  is  the  value  of  E'Ag,  namely  the  constant  of  the  silver- 
silver  chloride  electrode,  referred  to  the  defined  hydrogen  stand- 
ard of  potential. 

Now  let  us  return  to  the  extrapolation  of  the  curve  through  the 
points  shown  in  figure  82  by  blackened  circles.  For  this  purpose 
the  curve  will  have  to  be  made  on  larger  scale.  See  figure  83. 
Extrapolations  to  M  =  0  have  been  made  with  the  aid  of  em- 
pirical curve-fitting  or  empirical  equations.  Thus  Linhart  (1917), 


.236 


.234 


£32 


LJ 


.228 
.226 


.22il^ 


ff 


j          ^ 
v/r 

FIG.  83.  CORRECTIONS  AT  VARIOUS  VALUES  OF  Vi«  FOR  THE  CONSTANT  OF 

THE  CELL 

-Ft,  H2  (1  atmos)  |  HC1,  AgCl  \  Ag+ 

whose  admirable  data  are  those  falling  closest  to  M  =  0,  ex- 
trapolated to  0.2234.  Scatchard  (1925),  however,  gives  to  Lin- 
hart's  last  point  more  weight  than  Linhart  allows.  He  also  uses 
as  guides  to  his  own  extrapolation  the  Debye-Hiickel  equa- 
tion1 both  in  its  simplest  reduced  form  to  give  the  tangent  shown, 
and,  in  a  more  extended  form,  to  pick  up  the  departure  from  this 
tangent  at  the  points  for  the  higher  concentrations.  By  these 


Chapter  XXV. 


468  THE    DETERMINATION   OF   HYDROGEN   IONS 

means  Scatchard  finds  the  intersection  with  the  ordinate  M  =  0, 
to  be  at  0.2226  volt.2 

For  present  purposes  we  shall  use  Scatchard's  -value  0.2226 
volt  for  the  electromotive  force  of  the  cell : 

Pt,  H2 1  HC1,  AgCl  |  Ag 

which  would  obtain  were  [HC1]  =  1  and  were  there  no  correction 
terms.  In  other  words  it  is  the  electromotive  force  when  the 
activity  is  unity,  i.e.,  (HC1)  =  I.3 

Returning  now  to  the  experimental  data  for  the  real  cell  with 
0.1  M  HC1,  we  might  assume  that  the  correction,  (  —  VAK  —  VH)  = 
0.0114  (see  fig.  83)  could  be  equally  divided  between  VAK  and  VH. 
This  would  be  equivalent  to  assuming  the  activity  coefficients  of 
the  hydrion  and  chloride  ion  to  be  equal  to  one  another.  On  this 
basis  we  obtain 

0.2226  +  0.05912  +  0.00570  =  -f  0.2874 
for  the  silver  chloride  half-cell  with  0.1  M  HC1  and 
0  -  0.05912  -  0.00570  =  -0.06484 

for  the  hydrogen  half-cell  with  0.1M  HC1.  Although  the  above 
assumption  will  later  be  rejected,  we  might  use  the  value  —0.0648 
for  the  hydrogen  half-cell  with  0.1  M  HC1  and  consider  this  our 
standard.  However,  if  we  were  to  join  this  half-cell  with  other 
miscellaneous  half-cells,  we  would  encounter  the  difficulty  of 
varying  liquid  junction  potential.  As  explained  in  Chapter  XIII 
the  magnitude  of  the  liquid  junction  potential  is  greatly  reduced 
when  one  side  is  a  saturated  solution  of  potassium  chloride.  For 
this  reason  it  is  usual,  in  miscellaneous  measurements,  to  form  a 
cell  in  which  saturated  KC1  solution  forms  a  bridge.  Were  the 

2  LaMer  (1927)  has  criticized  Scatchard's  employment  of  the  Debye- 
Hiickel  equation  in  this  extrapolation.    However,  it  will  presently  be- 
come clear  that  there  is  no  occasion  for  our  attempting  here  to  resolve  this 
difference  of  opinion  or  to  enter  a  detailed  discussion  of  the  comparison 
between  Scatchard's  data  and  those  of  Nonhebel  and  of  Randall  and 
Vanselow  to  which  LaMer  refers.     There  has  just  come  to  hand  Randall 
and  Young's  paper  in  which  the  value  is  lowered  to  0.2221. 

3  The  reader  is  again  reminded  that  ()  is  used  to  indicate  activity  while 
[]  is  used  to  indicate  concentration. 

4  This  corresponds  to  pH  =  1.096. 


XXIII  STANDARDIZATION  469 

calomel  half-cell  with  saturated  KC1  considered  by  all  to  be  a 
safe,  permanent  standard  of  reproducible  qualities,  we  might 
consider  alone*  the  comparisons  of  this  half-cell  with  the  hydrogen 
half-cell  discussed  above.  It  is  preferable  to  seek  the  value  of  the 
more  reproducible  "tenth  normal"  calomel  half-cell.  Scatchard 
proceeds  as  follows. 
He  used  the  arrangement 

Hg  |  HgCl,  KC1  (sat.)  $HC1  (X),  AgCl  |  Ag 
A 

and  varied  X.  A  flowing  junction  was  used  at  A.  The  equation 
may  be  written: 

Eoba  =  E'0  -  E'Ag  -  0.05912  log  [Q-]  -  VAg  -  VL.     (7) 

where  E'c  is  the  constant  potential  at  the  mercury,  E'Ag  is  the 
constant,  0.2226  volt  (see  above),  characteristic  of  the  silver- 
silver  chloride  electrode  discussed  previously,  VAg  is  the  correc- 
tion for  the  silver-silver  chloride  electrode  and  VL  is  the  variable 
potential  at  junction  A. 

The  data  can  be  treated  graphically  in  a  manner  quite  com- 
parable with  that  used  in  the  former  case.  Scatchard  made  the 
extrapolation  with  the  aid  of  the  simplified  Debye-Htickel  equa- 
tion. However,  in  the  present  instance  there  is  a  rather  delicate 
point  to  watch.  If  the  extrapolation  were  made  purely  em- 
pirically there  might  be  obtained  the  value  of  E'c  —  E'Ag  +  VL. 
Here  VL  is  included  since  the  loci  of  the  points  are  certainly  deter- 
mined by  VL  in  part  and  its  value  might  well  be  changing.  In- 
herent in  such  an  extrapolation  would  be  the  conclusion  that  the 
part  contributed  to  the  value  of  E'c  —  E'Ag  +  VL  by  VL  at 
the  limit  would  then  be  the  potential  of  the  junction  saturated 
KC1  \  Water.  However,  if,  within  the  range  of  the  last  points 
nearest  the  tangent  drawn  by  means  of  the  Debye-Hiickel  relation, 
the  liquid-junction  potential  does  not  vary  much,  the  fact  that  the 
Debye-Hiickel  relation  was  used  and  that  this  has  nothing  to  do 
with  liquid  junctions,  would  lead  to  the  conclusion  that  the  con- 
tribution of  VL  is  as  if  it  were  of  the  liquid  junction  potential  of 
saturated  KCl^HCl  in  the  lower  experimental  ranges  of  [HC1]. 
Apparently  this  is  Scatchard's  interpretation.  He  finds  E'0  — 
E'Ag  =  0.0228  volt.  E'Ag,  as  noted,  is  0.2226.  Hence  E'c  +  VL 


470 


THE    DETERMINATION   OF   HYDROGEN   IONS 


=  0.2454  volt.  This  is  the  potential  at  Scatchard's  saturated 
KC1  calomel  electrode  including  a  liquid  junction  potential  as  if 
against  0.1  (or  less)  M  HC1  and  made  with  flowing  junction. 

Instead  of  attempting  to  go  to  the  decinormal  calomel  half-cell 
by  direct  comparison,  Scatchard  takes  a  route  summarized  as 
follows  with  the  aid  of  figure  84. 

We  have  already  discussed  the  cell  composed  of  the  half-cells 
(3)  and  (8)  of  figure  84  (potential  x).  We  have  noted  how  a 
study  of  cells  of  this  type  may  be  made  to  yield  the  value  of 


.3373--.- HdlHdCf.KO  (O.IMH    (I) 

..    !..     -.    .... 


Pt,  H,|  H+Mctiwty/)  (0) 


1___L_L  pttHt  |  HCI  (0.1  M) 


(8) 


FIG.  84 

Note:  First  steps  do  not  require  activity  of  Cl-  but  of  HCI 

half-cell  (7)  with  potential  (a)  standardized  with  reference  to 
half-cell  (0)  the  potential  at  which  is  defined  as  zero.  In  a 
comparable  way  the  cell  composed  of  half-cells  (2)  and  (8) 
(potential  y)  and  of  variations  of  this  cell  with  different  con- 
centrations of  HCI  are  made  to  yield  the  value  of  half-cell  (5) 
(potential  b).  For  this  purpose  Scatchard  uses  the  data  of  others 
for4"cell  (2)-(8)  and  applies  his  own  value  for  the  correction  term 
that  yields  the  value  of  (5). 


XXIII  STANDARDIZATION  471 

Next  cell  (6)-(8)  with  potential  z,  was  treated  as  outlined  above 
to  reach  the  standardized  value  of  (6),  potential  c.  Experi- 
mental cell  (6)-(8)  possesses  a  junction  potential,  namely  that  of 
KC1  (sat.)jHCl  (0.1  M),  which  will  be  called  VLI.  In  reach- 
ing a  value  for  half-cell  (4)  by  observation  of  potential  d  this 
junction  potential,  VLI,  is  carried  along  in  the  standardization. 
Also  the  potential  of  the  new  junction  KC1  (sat.)fKCl  (0.1  M) 
is  introduced  experimentally. 

The  difference  between  b  and  a,  that  is  the  difference  of  poten- 
tential  between  the  calomel  and  the  silver  chloride  electrodes  in  a 
solution  of  the  same  chloride  ion  activity,  is  e.  This  same  dif- 
ference should  apply  to  the  cell  (l)-(4).  Thus  the  value  0.3373 
for  the  calomel  electrode  with  0.1  molal  KC1  is  reached.  A 
correction  for  change  from  0.1  molal  to  0.1  normal  brings  the 
value  to  0.3372  for  the  decinormal  calomel  electrode.  There 
has  been  carried  along,  in  the  standardization,  the  potential  of 
the  customary  junction  KC1  (sat.)jKCl  (0.1  N),  which  should 
be  included  for  practical  purposes,  and  also  a  junction  potential 
as  of  KC1  (sat.)iHCl  (0.1  M,  or  less). 

If  the  value  for  the  tenth  normal  calomel  half-cell  is  to  be  ob- 
tained without  those  liquid-junction  potentials  which  were  car- 
ried along  in  the  above  calculations,  we  may  take  a  new  start 
with  half-cell  5  (fig.  84).  Introduce  the  estimated  activity  of 
chloride  ions  in  0.1  M  KCl-solution.  Scatchard  uses  0.0762  for 
this  activity.  Whence  0.3353  is  the  estimated  potential  of  the 
decinormal  cell  without  liquid-junction. 

In  summary  we  have : 

HC1  \  KC1  (sat.),  HgCl  |  Hg  ;  Eh  =  +0.2454  at  25° 

||  KC1  (0.1  M),  HgCl  |  Hg  ;  Eh  =  +0.3353  at  25° 

HCljKCl  (sat.)  |  KC1  (0.1  N),HgCl  |  Hg      ;Eh  =  +0.3372  at  25° 

Now  let  us  return  to  the  problem  mentioned  on  page  468  namely 
the  partition  of  the  correction  between  the  silver  chloride  and 
hydrogen  half-cells.  It  is  a  bold  assumption,  and  one  which  is 
not  in  good  repute,  to  make  the  even  partition  there  used.  Scat- 
chard  employs  his  measurements  with  the  cell 

Hg  |  HgCl,  KC1  (sat.)  $HC1,  AgCl  |  Ag 
A 


472 


THE    DETERMINATION   OF   HYDROGEN    IONS 


He  employs  the  aforementioned  assumptions  regarding  liquid 
junction  potentials  and  the  Debye-Hiickel  equation  for  extra- 
polation to  zero  concentration  of  HCL  Thereby  he  is  able  to 
calculate  the  corrections  for  the  chloride  half-cell  at  the  several 
concentrations  of  hydrochloric  acid.  Having  already  obtained 
the  sum  of  th§  corrections  for  the  chloride  and  hydrogen  half-cell, 
he  obtains  the  corrections  for  the  hydrogen  half-cell. 

Using  activity  coefficients  in  place  of  potential  corrections  and 
the  relation 


THCI  = 


X  TCI" 


Scatchard   finds,   for   instance    in   the    case    of    0.1    M   HC1: 
7ci  =0.762;  TH+  =  0.841  and  V7H~  x  7cT  =  THCI  =  0.801. 

We  have  rounded  off  the  value  of  7H+  to  0.84  and  employ  this 
to  calculate  the  pH  values  of  HC1:KC1  solutions  given  on  page  201. 
We  also  employ  it  to  obtain  those  calculated  potentials  of  the 
hydrogen  half-cell  with  0.1  N  HC1  which  are  given  in  table  A, 
page  672. 

TABLE  61 

Some  values  assigned  to  calomel  half-cells  at  %5°C. 

Parenthesized  values  are  calculated  from  unparenthesized  values. 
Bracketed  values  are  calculated  from  measurements  at  other  tempera- 
tures. 


HALF 

-CELL 

AUTHORITY 

||  KC1  (0.1M), 

HgCl  |  Hg 

II  KC1  (0.1M)  1 
KC1  (l.OM),  HgCl| 
Hg 

Beattie  (1920)  

(0  3353) 

0  2826 

Lewis  and  Randall  (1921) 

0  3351 

(0  2822) 

S0rensen  and  Linderstr0m-Lang  (1924)  .  .  . 
Scatchard  (1925)  

[0.3354] 
0.3353 

(0.2825) 
(0.2826) 

Average.  .  .  . 

0  3353* 

*  There  has  just  come  to  hand  Randall  and  Young's  paper  in  which  they 
give  0.3341  for  the  potential  of  the  half-cell  in  vacuum  but  state  that  the 
value  of  the  half-cell  in  air  will  be  about  0.3354  by  reason  of  an  error  of 
one  to  three  millivolts  caused  by  the  presence  of  air. 

It  seems  hardly  necessary  to  outline  other  routes.  That  men- 
tioned shows  not  only  the  nature  of  the  argument  but  two  aspects 


XXIII  STANDARDIZATION  473 

of  special  interest  to  the  purpose  of  this  chapter.  In  the  first 
place  it  is  evident  that  methods  of  reaching  standard  values  are 
becoming  more  rationalized.  In  the  second  place  there  remain  a 
number  of  small  discrepancies  and  fundamental  difficulties 
(especially  with  liquid-junction  potentials)  sufficient  to  cause 
appreciable  variation  in  the  values  used  by  different  authors  in 
arriving  at  the  value  of  any  specified  half-cell.  The  latter  fact  is 
obscured  by  the  uncritical  comparison  in  table  61.  The  apparent 
agreement  obtains  because  of  a  remarkable  cancellation  of  small 
differences.  But  even  if  it  be  granted  that  the  average  in  table 
61  is  final,  its  acceptance  settles  only  part  of  our  problem.  Con- 
sider the  cell : 

Pt,  H2  (1  atmos.)  |  solution  X  |  KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 
ABC  D 

As  solution  X  is  changed  there  is  not  only  a  change  of  potential 
difference  at  A,  but  there  is  also  a  change  of  liquid  junction  poten- 
tial at  B.  Knowledge  of  the  potential  of  C  +  D  and  a  measure- 
ment of  the  whole  cell  is,  therefore,  not  sufficient  to  give  the 
potential  at  A.  Strictly,  each  change  of  solution  X  will  produce 
a  change  of  potential  at  B.  Since  there  is  no  universal  rule  by 
which  the  potential  at  B  can  be  calculated  in  each  and  every 
case,  it  is  necessary  in  practice  to  introduce  an  assumption.  Two 
assumptions  have  been  the  more  customary.  One  is  that  the 
junction  potential  at  B  shall  be  neglected.  The  other  is  that  it 
shall  be  estimated  by  the  Bjerrum  extrapolation  (see  page  277), 
using  3.5  M  and  1.75  M  KC1  in  place  of  saturated  KC1  solution 
as  bridge. 

The  latter  assumption  was  used  by  S0rensen  (1909)  in  deriving 
the  value  of  the  "tenth  normal  calomel  electrode"  from  measure- 
ments of  the  cell 

3.5N 
Pt,  H2  (1  atmos.)!  HC1  (0.1N)  |  KC1     or    |  KC1  (0.1N),  HgCl  |  Hg 

1.75N 

It  has  usually  been  assumed  that  because  S0rensen  used  con- 
ductivity data  to  obtain  the  hydrion  concentration  of  0.1  N  HC1 
and  thence  calculated  0.3380  (18°)  for  the  potential  of  the  "tenth 
normal  calomel  half-cell"  that  this  value  must  necessarily  be 


474  THE   DETERMINATION    OF   HYDROGEN    IONS 

erroneous.  As  a  matter  of  fact  the  Bjerrum  extrapolation5 
which  he  used  was  large  (74  mv.)  and  it  appears  that,  by  chance, 
he  obtained  a  value  which  can  still  be  justified.  If  we  compare 
the  S0rensen  value  at  25°  (see  page  453)  with  Scatchard's  es- 
timate for  the  half-cell, 


HC1  $  KC1  (sat.) 


KC1  (0.1  N),  HgCl 


Hg 


B  C  D 

we  have: 

0.3376  (S0rensen) 
0.3372  (Scatchard) 

According  to  Scatchard's  estimate  the  potential  at  C  is  0.0027 
volt  with  the  orientation  shown  above  and,  at  B,  0.0047  with 
the  orientation  shown  when  the  solution  in  the  hydrogen  half- 
cell  is  0.1  M  HC1.  (Earned  (1926)  calculated  0.0016.) 

Since  the  S0rensen  value,  for  the  so  called  "0.1  N  calomel  electrode"  is 
now  frequently  used  as  if  of  the  above  half-cell  and  happens  to  be  so  near 
to  a  significant  value  under  particular  circumstances,  it  may  be  con- 
sidered. It  is  especially  important  to  consider  the  Sprensen  value  because 
it  has  been  used  extensively  in  the  standardization  of  buffer  solutions, 
ionization  constants  and  a  host  of  miscellaneous  data.  The  value  was  in 
substantial  agreement  with  that  recommended  by  Auerbach  (1912)  and 
adopted  by  the  "Potential  Commission,"  whence  arose  substantial  agree- 
ment with  other  types  of  investigation.  It  would  be  quite  impracticable 
to  cite  all  of  even  the  types  of  data  that  conform  substantially  to  the  basis 
established  by  S0rensen.  Much  of  it  is  data  of  high  accuracy  and  com- 
plexity. See,  for  example,  the  researches  on  blood  and  the  involved  car- 
bonate equilibria. 

6  S0rensen's  average  value  for  the  cell 

Pt,  H2  |  HC1  (0.1  N)  |  KC1  (3.5  N)  |  KC1  (0.1  N),  HgCl  [  Hg 

was  0.4025  volt.  His  use  of  the  Bjerrum  extrapolation  reduced  this  to 
0.3975  volt.  If  we  neglect  the  extrapolation  and  use  0.3380  volt  for  the 
potential  of  the  tenth  normal  calomel  half-cell,  we  obtain 

0  4025  0  3380 

-  =  1.12,  as  the  pH  number  of  0.1  N  HC1  at  18°C.  in 


place  of  S0rensen's  assumed  value  1.04;  but  this  calculation  is  made  with 
the  use  of  a  potential  obtained  with  3.5  N  KC1  solution,  instead  of 
saturated  KCl_solution,  as  bridge. 


XXIII  STANDARDIZATION  475 

For  purposes  of  discussion  we  shall  use  the  S0rensen  value  0.3376  (25°) 
for  the  half-cell 

HC1  |  KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 
and  0.3353  (25°)  for  the  half-cell 

||KC1  (0.1  N),  HgCl  |  Hg 

Since  there  are  only  a  few  who  retain  confidence  in  the  Bjerrum  extra- 
polation we  shall  neglect  it  and  shall  continue  with  the  assumption  that 
saturated  KC1  solution  is  to  be  used.  In  discussing  the  cell 

Ft,  H2  (1  atmos.)  |  solution  X  |  KC1  (sat.)  |  KC1  (0.1  M),  HgCl  |  Hg 

B  C 

the  junction  potential  at  B  is  to  be  neglected  in  calculations. 

Undoubtedly  when  solution  X  is  a  phosphate  solution  this  junction 
potential  is  much  less  than  when  solution  X  is  a  dilute  hydrochloric  acid 
solution.  How  much  less,  there  is  no  certain  way  of  telling.  As  an  ex- 
treme we  can  consider  it  to  compensate  that  at  G.  If  so  the  value 
0.3353  should  be  used  for  the  "calomel  half-cell"  instead  of  the  customary 
0.3376.  But  if,  on  the  dangerous  assumption  made  above,  we  adopted 
0.3353  for  universal  use,  we  would  certainly  be  in  error  when  operating  with 
very  acid  solutions. 

Attempts  to  proceed  with  the  adoption  of  any  fixed  single  value  for  a 
half -cell  involving  a  liquid  junction,  the  potential  of  which  is  susceptible 
to  appreciable  change  as  the  solution  under  study  is  changed,  is,  of  course, 
not  strictly  logical;  but  we  are  now  considering  arbitrary  assumptions 
necessary  to  ordinary  operation.  In  the  study  of  phosphate  buffers  will 
the  use  of  0.3376  in  place  of  0.3353  be  serious?  So  far  as  pH  numbers  are 
concerned 

0.3376  -  0.3353 

=  0.0389^0.04 


0.05912 

gives  the  correction  that  should  be  added  to  a  pH  number  at  25°  were 
0.3353  used  in  place  of  0.3376. 

But  such  an  error  is  of  no  practical  consequence  in  the  comparison  of 
acid-salt  systems  in  which  the  acid  is  very  weak.  When  [H+]  is  of  the 
order  of  10~5  or  less  it  may  be  neglected  in  calculating  the  undissociated 
residue  from  [HA]  —  [H+]  =  [A],  except  at  impracticably  high  dilutions. 
As  discussed  in  Chapter  XXVII  any  standard  of  reference  will  do  and  our 
chief  concern  is  then  with  agreement  upon  the  standard  selected. 

A  more  or  less  uncertain  but  reasonable  compromise  may  be  made  by 
allowing  the  error  for  the  extreme  case  of  the  phosphate  buffer  where  the 
error  is  of  no  practical  importance  and  adopting  0.3376  which  leads  to 
substantially  reasonable  values  in  very  acid  solutions  where  [H+]  is  of 
importance  not  only  as  an  index  but  of  itself. 


476  THE   DETERMINATION   OF   HYDROGEN   IONS 

Possibly  a  sliding  scale  of  values  could  be  devised  but  in  the  present 
state  of  affairs  this  would  be  dangerous. 

The  adoption  of  a  fixed  value,  which  is  roughly  adapted  to  the  more 
acid  solutions  and  which  allows  an  error  for  the  extreme  case  where  the 
error  is  of  no  practical  importance,  will  doubtless  lead  to  appreciable  error 
in  the  study  of  intermediate  cases. 

Cohn,  Heyroth  and  Menkin  (1928)  believe  they  detect  this  in  their  treat- 
ment of  acid,  acetate  solutions,  a  discrepancy  in  the  drift  of  —  log  7  being 
removed  by  the  employment  of  0.3357  instead  of  0.3380  for  measurements 
at  18°.  They  also  note  that,  if  electromotive  force  measurements  are  to 
be  brought  into  harmony  with  recent  corrected  conductivity  measurements 
of  the  dissociation  constant  of  acetic  acid,  the  value  of  the  half-cell 

||  KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 

with  neglect  of  liquid  junction  potential  "should  be  between  0.3364  and 
0.3370." 

To  what  extent  such  adjustments  will  have  to  be  made  as  the  case  is 
changed  is  a  question  on  which  I  shall  not  even  venture  an  opinion;  but 
that,  strictly,  each  individual  case  is  a  new  case,  in  which  allowance  for  a 
different  junction  potential  must  be  made,  can  hardly  be  gainsaid,  es- 
pecially when  the  cases  are  those  in  which  [H+]  is  high. 

The  use  of  a  stated  pH  value  for  0.1  N  HC1  and  the  use  of  the  cell 


Pt,  H2  (1  atmos.) 


HC1 
0.1  N 


KC1  (sat.),  HgCl 


Hg 


in  standardizing  the  saturated  calomel  half-cell  has  the  appearance  of 
being  direct,  simple  and  clear.  However,  it  is  not  always  certain  that 
liquid  junctions  are  established  in  a  uniform  manner  by  different  workers 
and,  as  emphasized  by  Clark  and  Lubs  (1916),  the  variability  of  potential 
at  the  junction  HC1  |  KC1  (sat.)  with  different  methods  of  forming  the 
junction  makes  the  use  of  HC1  dangerous  for  routine  standardization 
purposes. 

To  illustrate  the  variation  of  present  practice  there  may  be  cited  a  few 
of  many  bases  of  standardization. 

Cullen,  Keeler  and  Robinson  (1925),  Hastings  and  Sendroy  (1924)  and  a 
group  of  American  students  of  blood  equilibria  have  been  using  pH  1.08 
for  0.1  N  HC1  as  a  standardizing  value  with  which  to  establish  the  value  of 
a  "working,"  saturated  calomel  half -cell.  Neglecting  liquid  junction 
potentials,  they  obtain,  for  M/15  phosphate  buffers,  pH  values  about  0.01 
unit  pH  greater  than  S0rensen's  values.  Hence  pH  1.09,  as  used  by  Simms 
(1926),  would  leave  another  0.02  pH  unit  to  be  added  were  the  0.04 
correction  mentioned  above  to  be  followed.  Levene,  Simms  and  Bass 
(1926)  use  1.075  for  0.1  M  HC1. 

S0rensen  and  Linderstr0m-Lang  (1924)  in  no.  10  of  their  recommenda- 


XXIII 


STANDARDIZATION 


477 


tions  advocate  the  use  of  0.4556  volts  as  the  extrapolated  (Bjerrum)  value 
of  the  following  cell  (presumably  at  18°) : 


Pt,  H2  (1  atmos.) 


0.01  N  HC1 


0.09  N  KC1 


3.5  N  KC1 

and 
1.5  N  KC1 


KC1  (0.1  N),  HgCl  |  Hg 


If  we  tentatively  assume  that  this  is  also  the  potential  of  the  cell 


Pt,  H2  (1  atmos.  ) 


0.01  N  HC1 
0.09  N  KC1 


KC1  (sat.)  |  KC1  (0.1  N)  HgCl  |  Hg 


and  assume  0.3380  for  the  half-cell 


KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 

we  obtain  pH  =  2.037.  This  is  substantially  the  number,  2.04  suggested 
by  Cullen,  Keeler  and  Robinson  (1925)  for  use  with  sat.  KC1  and  neglect 
of  liquid  junction,  and  2.038  by  Kolthoff  and  Tekelenburg  (1927)  for  use 
with  the  Bjerrum  extrapolation.  Biilmann  (1927)  accepts  2.029  on  the  basis 
of  a  personal  communication  from  Bjerrum,  and  uses  it  with  the  Bjerrum 
extrapolation  in  his  discussion  of  the  quinhy drone  electrode. 

Other  values  for  0.01  N  HC1  +  0.09  N  KC1  are  included  in  the  following 
list  of  contrasts. 

2.029  Biilmann  (1927) 

2.038  Kolthoff  and  Tekelenberg  (1927) 

2.063  Gjaldbaek  (1925) 

2.078  Table  35a,  page  201 

2.093  Larsson  (1922) 

S0rensen  and  Linderstr0m-Lang  (1927)  have  recently  abandoned  the 
0.3380  value  for  the  "tenth  normal"  calomel  half -cell  and  are  using  0.3357 
(18°)  as  a  basis,  with  intervening  solution  of  saturated  KC1  and  neglect 
of  liquid  junction.  Their  former  (1924)  general  recommendations  permit 
the  Bjerrum  extrapolation  and  their  specification  no.  10  provides  for  it 
in  "specially  accurate  measurements." 

Many  other  cases  could  be  cited  to  show  appreciable  differences  in 
standards. 

American  practice  has  tended  toward  the  use  of  saturated  potassium 
chloride  solution  as  a  bridge  or  the  use  of  the  saturated  KCl-calomel  half- 
cell  as  a  working  standard  and  the  stated  tentative  assumption  that  the 
liquid  junction  potential  shall  be  neglected.  Many  European  workers 
still  operate  with  the  old  method  of  extrapolation  introduced  by  Bjerrum 
and  with  the  3.5  N  KC1  calomel  half-cell.  Although  S0rensen  and  Linder- 
str0m-Lang  state  that  the  two  methods  give  practically  the  same  result  in 
ordinary  buffers,  it  is  by  no  means  certain  that  the  two  methods  will  lead 
to  the  same  set  of  values  when  hydrochloric  acid  solutions  of  one  kind  or 
another  are  used  as  ultimate  standards.  Direct  comparison  of  the  results 


478  THE   DETERMINATION    OF   HYDROGEN   IONS 

of  the  two  kinds  of  practice  is  beset  with  danger  when  the  practical  stand- 
ard of  reference  is  a  hydrochloric  acid  solution. 

In  the  absence  of  any  thoroughly  developed  fundamental  basis  we  may 
well  expect  in  the  near  future  as  many  slight  but  distinct  differences  in 
methods  of  standardization  as  have  appeared  in  the  recent  past.  Indeed 
it  may  be  questioned  whether  any  recommendation  is  worth  while.  A 
decision  would  not  permit  a  recalculation  of  all  important  data,  because 
these  data  in  very  many  instances  have  been  published  without  the  detail 
necessary  to  that  purpose.  A  decision  might  have  no  weight  unless  it 
either  formulate  custom  or  presage  the  value  of  the  final  standard.  Custom 
is  now  less  easily  formulated  than  when  the  second  edition  was  written 
and,  insofar  as  we  may  judge  by  past  experience  in  this  matter,  the  accept- 
ance of  the  " latest  value"  is  a  dangerous  procedure.  However,  it  is  quite 
impracticable  to  review  all  the  various  standards  in  detail  and  some 
decision  must  be  made  for  the  purposes  of  this  book.  I  dislike  to  be 
merely  conservative  but  am  constrained  to  adhere  to  the  principle  stated 
in  the  second  edition,  where  it  was  said:  "  ....  it  will  be  wise  during 
the  present  period  of  transition  to  adopt  a  provisional  standard  and  in 
lieu  of  agreement  reached  in  convention  to  let  that  standard  be  in  har- 
mony with  that  tacitly  implied  in  the  greater  body  of  data."  In  one 
respect  the  future  can  be  safely  predicted.  The  Bjerrum  extrapolation 
will  be  abandoned  as  contributing  nothing  definite.  If  so  the  saturated 
KC1  calomel  half-cell  will  doubtless  become  the  "working  standard"  and 
the  3.5  N  KC1  calomel  half -cell  will  -become  an  "extra"  in  the  scheme. 
However,  while  there  remains  doubt  concerning  the  reproducibility  of  the 
saturated  KC1  calomel  half-cell  (a  doubt  which  may  not  be  well  founded) 
either  the  redefined  tenth  normal  calomel  half-cell,  oi  the  hydrogen  half- 
cell  with  0.1  N  HC1,  will  be  preferred  as  the  ultimate,  practical  standard. 
Of  these  two  half-cells  the  last  has  a  dangerously  high  liquid  junction 
potential  at  the  junction  HC1  |  KC1  (sat.).  Undoubtedly  the  individual 
operator  will  be  able  to  reproduce  his  data;  but  the  practice  has  shown 
such  a  variety  in  the  manner  of  forming  the  liquid  junction  that  the 
specification  of  this  half-cell  would  have  to  involve  very  careful  specifica- 
tion of  the  manner  of  forming  the  liquid  junction.  Therefore  the  first 
half-cell  is,  for  the  present,  to  be  preferred. 

As  already  noted,  it  is  impracticable  to  attempt  correction  of  all6  im- 
portant data  to  strict  conformity  with  the  specifications  to  follow  and 
a  certain  speciousness  results  if  it  be  thought  that  these  specifications 
lead  to  strict  harmony  between  measurements  made  accordingly  and  the 

6  The  data  for  the  buffer  mixtures  of  Clark  and  Lubs  (1916)  [see  page  200] 
were  obtained  with  the  use  of  a  saturated  KCl-calomel  half-cell  which  was 
standardized  against  a  group  of  tenth  normal  KC1  calomel  half-cells. 
There  were  also  used  Bjerrum  extrapolations  which  were  very  large  in 
the  case  of  the  HC1-KC1  mixtures.  To  conform  to  the  specifications  of 
this  chapter  the  original  data  have  been  used  in  recalculations  which  are 
embodied  in  table  35,  page  200. 


XXIII  STANDARDIZATION  479 

measurements  of  the  past  which  were  "based  on  the  S0rensen  value  for 
the  tenth  normal  calomel  half-cell."  Nevertheless  the  agreement  should 
be  substantial.  That  is  the  best  that  can  be  made  of  the  situation. 

That  a  considerable  part  of  the  discrepancies  appearing  in  the  literature 
is  due  to  disagreement  of  primary  experimental  data  rather  than  to  the 
selection  of  different  bases  of  reference  appears  in  the  footnote  to  table  A, 
page  672.  In  that  footnote  are  a  few  data  which,  for  the  most  part,  rep- 
resent direct  measurements.  They  are  compared  with  the  numbers 
derived  from  the  table.  In  some  instances,  such  as  Walpole's  use  of  a 
seasoned,  saturated,  calomel  half-cell,  and  the  author's  measurement  of 
cell  III:  VI,  the  experiments  cited  are  of  intermediate  measurements  and 
as  such  are  not  fundamental.  In  other  instances  a  careful  scrutiny  of 
conditions  might  reveal  reasons  for  rejecting  one  or  another  of  the  numbers 
given.  However,  a  comparison  of  numerous  other  data,  which  are  less 
easily  compared  and  tabulated,  supports  the  impression  made  by  this  set 
of  comparisons.  The  problem  appears  to  be  quite  as  much  one  of  technique 
as  of  formulation.  For  this  reason  recurring  shifts  of  standard  and  the 
absence  of  data  revealing  the  reproducibility  of  measurements,  both  of 
which  characterize  a  considerable  part  of  the  modern  literature,  have  made 
the  second  decimal  of  pH  numbers  as  uncertain  as  they  were  in  a  less  so- 
phisticated period. 

The  following  specifications  are  substantially  those  recom- 
mended in  the  second  edition,  accepted  by  S0rensen  and  Linder- 
str0m-Lang  and  then,  by  a  curious  fate,7  abandoned  by  the  latter. 

7  Originally  pH  was  denned  by  pH  =  log Actually,  the  numerical 

values  called  pH  have  been  determined  by  dividing   the  potential  of  a 

O  QftO f\   ~R  T 

hydrogen  cell  by    J ..     In  the  comparison  of  one  solution  with  a 

F 

standard  solution  of  hydrion  activity  of  unity,  the  rigid  relation  may  be 
written 

1  -EF 

°g  (H+)    "  2.3026  RT 

where  (H+)  represents  the  hydrogen  ion  activity  of  the  solution  under 
investigation.  Consequently  the  measured  values  called  pH  are  log 

and  not,  as  defined,  log  p^~pj* 

Recognizing  this  Sprensen  and  Linderstr0m-Lang  (1924)  proposed  that 
pH  retain  its  original  defined  meaning  and  that  a  new  symbol  pafl  be 

used  for  log  •—  • 


480         THE  DETERMINATION  OF  HYDROGEN  IONS 

1.  The  following  half-cell  shall  be  used  as  a  standard  of  reference 

KC1  (saturated)  |  KC1  (0.1  N),  HgCl(s)  |  Hg 

2.  It  shall  be  assumed,  arbitrarily,  that  in  the  cell 

Pt,  H2  (1  atmos.)  |  H+  (activity,  X)  |  KC1  (sat.)  |  KC1  (0.1N),  HgCl(s)  1 
ABC  D 

the  potential  difference  at  B  remains  constant  as  X  varies  and 
that  the  sum  of  the  potential  differences  at  B,  C  and  D  is  as 
follows  "at  each  indicated  temperature. 

Temper- 
ature, 
°C 18°  20°  25°  30°  35°  38°  40° 

Potential 
Differ- 
ence...  0 . 3380  0 . 3379  0 . 3376  0 . 3371  0 . 3365  0 . 3361  0 . 3358 

3.  The  standard  experimental  meaning  of  pH  shall  be  the 
potential  of  the  above  cell  considered  as  of  positive  numerical 

This  proposal  is  in  itself  quite  consistent  and  elegant.  It  provides  con- 
sistent symbols  to  be  used  whenever  there  is  occasion  to  abbreviate  log 

— —  and  log  — —  in  the  writing  of  equations. 

But  Sprensen  and  Linderstr0m-Lang  went  beyond  questions  of  defini- 
tion and  coupled  their  symbols  with  two  proposed  values  of  the  0.1  N 
calomel  half-cell.  One,  e.g.,  0.3380  at  18°,  was  to  be  used  in  estimating 
values  of  pH,  and  the  other,  0.3357,  was  to  be  used  in  calculating  values 
of  paH.  Such  coupling  of  the  proposals  is  a  source  of  confusion.  Spren- 
sen  and  Linderstrpm-Lang  should  have  warned  their  readers  that  there  is 
no  constant  difference  between  hydrogen  ion  concentration  and  hydrogen 
ion  activity  as  implied  on  page  37  of  their  article.  They  appeared  to  be  in 
agreement  with  the  proposals  of  the  second  edition  of  this  book  but  ig- 
nored its  proposal  of  an  experimental  meaning  for  a  pH  number. 

In  their  later  articles  (see,  for  instance,  Sprensen  and  Linderstr0m-Lang 
(1927))  they  use  0.3357  instead  of  the  older  value,  0.3380,  for  the  "0.1  N 
calomel  half-cell." 

In  this  book  pan  is  not  used.  It  must  be  assumed  that  the  reader  appre- 
ciates the  qualifications  stated  or  implied  in  the  use  of  the  laws  of  an 
ideal  solution.  These  idealized  relations  are  useful  within  limits  to  outline 
the  subject.  Then  "pH"  can  retain  its  original  meaning.  With  regard 
to  meticulous  uses  the  following  may  be  said.  Any  numerical  value 
given  to  (H+)  implies  customary  usage.  Unless  liquid  junction  potentials 
are  accurately  estimated  when  the  potential  of  the  customary  cell  is  used 


XXIII  STANDARDIZATION  481 

value,  less  the  above  value  for  the  calomel  half-cell  pertaining  to 
the  temperature  used,  the  difference  being  divided  by  the  nu- 
merical quantity  0.000,198,322  T,  where  T  is  the  absolute  tem- 
perature. 

4.  When  a  value  of  pH  is  modified  by  attempts  to  correct  for 
the  potentials  at  B  and  C,  or  by  the  use  of  some  estimated  value 
of  the  potential  at  D  alone,  or  by  any  other  modification  of  the 
above  procedure,  a  statement  of  all  essential  modifications  shall 
be  made. 

5.  If  there  be  used  any  secondary  standard,  such  as  the  poten- 

to  calculate  log  ,  it  is  not  strictly  proper  to  name  the  calculated 

value  log  ,  or  pan-     However,  it  is  legitimate  to   proceed  with  the 

recognition  that  the  measurement  is  of  an  energy  relation  which  if  it 
could  be  carefully  analyzed  would  give  a  measure  of  activity,  and  to 
assume  for  purposes  of  approximation  that  numbers  called  "pH"  can  be 

used  where  log  would  occur  in  the  energy  equation.    That  the  ideal 

equation  in  terms  of  concentrations  could  not  be  applied  strictly  has  long 
been  recognized,  although  not  emphasized  in  the  past.  The  modern 
developments  have  served  to  make  the  emphasis  strong  but  have  created 
no  essentially  new  situation.  Since  almost  all  of  the  values  entering  our 
subject  are  based  on  the  conduct  of  hydrogen  cells  they  might  be  renamed 
pag,  were  the  uncertainties  of  liquid  junction  potentials  adequately 
taken  care  of.  But,  in  the  absence  of  %iality  both  in  regard  to  liquid 
junction  potentials  and  the  hydrion  activity  of  any  given  standard  solution, 
it  seems  preferable  to  give  an  arbitrary  but  definite  meaning  to  numbers 
called  pH. 

That  the  introduction  of  pan  may  accomplish  no  good  purpose  appears 
in  such  comparisons  as  the  following.  Hastings,  Murray  and  Sendroy 
(1927),  in  using  pan,  with  stated  assumptions  in  regard  to  the  calculation 
of  numerical  values,  find  occasion  to  note  that  their  values  differ  from 
similarly  named  values  given  by  Sprensen  and  Linderstrpm-Lang.  The 
latter  authors  in  the  same  year  were  using  0.3357  for  the  calomel  half- 
cell  while  Hastings,  Murray  and  Sendroy  were  using  as  a  basis  of  reference 
pan  =  1.08  for  0.1  N  HC1.  Both  were  neglecting  the  liquid  junction 
between  saturated  KC1  solution  and  the  several  solutions  placed  on  the 
other  side  of  the  junction.  In  the  absence  of  finality  in  regard  to  several 
of  the  questions  concerned  it  is  probable  that  each  set  of  workers  could 
establish  a  reasonable  justification  for  the  usage  they  adopted.  In  that 
case,  and  others  of  like  nature,  we  have  different  meanings  for  paH  so 
far  as  its  quantitative  aspect  is  concerned. 


482  THE    DETERMINATION    OF   HYDROGEN   IONS 

tial,  of  a  hydrogen  electrode  or  of  a  quinhydrone  electrode  in  a 
standard  buffer  solution,  the  attempt  shall  be  made  to  use  this 
standard  in  accordance  with  the  specifications  made  above. 

It  may  be  emphasized  that  section  5  provides  for  the  use  of 
any  secondary  standard  if  there  is  no  desire  to  actually  use  the 
tenth  normal  calomel  half-cell;  but  that,  if  the  other  specifications 
are  adopted,  the  secondary  standard  should  not  be  evaluated 
de  novo. 

In  case  the  above  system  is  not  accepted,  it  is  recommended  that 
every  assumption  and  every  detail  of  the  system  adopted  be 
carefully  stated.  In  particular  it  may  be  said  that  a  statement 
regarding  the  potential  of  a  half-cell  without  statement  of  as- 
sumptions regarding  the  liquid  junctions  used  in  actual  cells  is 
misleading. 

In  the  next  chapter  there  will  be  stated  secondary  standards 
which  conform  more  or  less  closely  to  the  above  specifications. 
Lest  the  values  there  stated  appear  too  neglectful  of  values  given 
elsewhere  in  the  literature  let  it  be  said  here  that  the  matter  has 
now  come  to  such  a  pass  that  it  would  be  impracticable  to  review 
and  reconcile  all  the  schemes  in  use. 

Experimental  and  theoretical  difficulties  with  liquid  junction 
potentials  are  largely  responsible  for  discrepancies  in  primary  ex- 
perimental data  and  for  diversity  of  treatment.  The  cells  with 
which  we  are  chiefly  concerned  are  distinctly  different  from  cells 
without  liquid  junction.  While  the  treatment  of  the  latter  has 
been  acquiring  elegance,  demands  upon  the  practical  application 
of  the  former  have  left  several  matters  undecided.  Indeed  it  ap- 
pears as  if  progress  with  cells  having  no  liquid  junction  has 
created  the  erroneous  impression  that  our  main  problem  is  near- 
ing  complete  solution.  Yet,  for  the  purpose  at  hand,  there  is 
neither  adequate  knowledge  of  liquid  junction  potentials  nor  ade- 
quate information  upon  the  reproducibility  and  the  temperature 
coefficients  of  standard  half-cells.  Therefore  that  otherwise  de- 
testable practice  of  arbitrary  standardization  seems  necessary  for 
the  purposes  of  routine  reports. 


CHAPTER  XXIV 

STANDARD  SOLUTIONS  FOR  THE  ROUTINE  CHECKING  OF  HYDROGEN 
ELECTRODE  MEASUREMENTS 

Thou  shall  not  have  in  thy  bag  divers  weights,  a  great  and  a  small. 
Thou  shalt  not  have  in  thy  house  divers  measures,  a  great  and  a 

small. 
But  thou  shalt  have  a  perfect  and  just  weight,  a  perfect  and  just 

measure  shalt  thou  have. — Deuteronomy,  XXV:  13-15. 

In  the  routine  measurement  of  hydrogen  ion  concentrations  it 
is  desirable  to  frequently  check  the  system.  To  do  so  in  detail 
is  a  matter  of  considerable  trouble ;  but  if  a  measurement  be  taken 
upon  some  solution  of  well  defined  pH,  and  it  is  found  that  the 
potential  of  the  cell  agrees  with  that  which  someone  has  deter- 
mined by  careful  and  detailed  measurements  upon  all  parts,  it 
is  reasonably  certain  that  the  several  souices  of  E.M.F.  are 
correct. 

Any  one  of  the  buffer  mixtures  whose  pH  value  has  been  es- 
tablished may  be  used  for  this  purpose,  but  there  are  sometimes 
good  reasons  for  making  a  particular  choice. 

In  view  of  the  fact  that  different  authors  have  recently  been 
selecting  several  reference  values  which  do  not  agree,  there  is 
need  that  each  author  state  definitely  the  value  selected  and  the 
mode  of  its  application.  The  following  discussion  concerns  values 
in  substantial  harmony  with  the  recommendations  of  the  pre- 
vious chapter, — a  restriction  made  necessary  by  the  fact  that 
discussion  of  all  standards  would  be  impracticable. 

STANDARD   ACETATE 

Michaelis  (1914)  recommends  what  has  come  to  be  known  as 
"standard  acetate."  This  is  a  solution  tenth  molecular  with 
respect  to  both  sodium  acetate  and  acetic  acid.  Its  preparation 
and  hydrogen  electrode  potential  at  18°C.  have  been  carefully 

483 


484  THE   DETERMINATION   OF   HYDROGEN   IONS 

studied  by  Walpole  (1914).    Walpole  proposes  two  methods  for 
its  preparation: 

(1)  From  N-sodium  hydroxid  solution  free  from  carbon  dioxid  and 
N-acetic  acid  adjusted  by  suitable  titration  (using  phenolphthalein),  so  as 
to  be  exactly  equivalent  to  it. 

(2)  From  N-sodium  acetate  and  N-acetic  acid  adjusted  by  titration  of 
a  baryta  solution,  the  strength  of  which  is  known  exactly  in  terms  of  the 
N-hydrochloric  acid  solution  used  to  standardize  electrometrically  the 
normal  solution  of  sodium  acetate. 

Walpole  defines  N-sodium  acetate  as  a  "solution  of  pure  sodium 
acetate  of  such  concentration  that  when  20  cc.  are  taken,  mixed 
with  20  cc.  of  N-hydrochloric  acid,  and  diluted  to  100  cc.,  the 
potential  of  a  hydrogen  electrode  in  equilibrium  with  it  is  the 
same  as  that  of  a  hydrogen  electrode  in  equilibrium  with  a  solu- 
tion 0.2  normal  with  respect  to  both  acetic  acid  and  sodium 
chloride."  By  mixing  the  N-acetate  with  the  N-HC1  in  accord- 
ance with  this  definition  and  then  determining  the  potential  of  a 
hydrogen  electrode  in  equilibrium  with  it,  Walpole  shows  that  the 
N-sodium  acetate  solution  may  be  accurately  standardized.  In 
table  62  are  given  Walpole 's  values  showing  the  relation  of  the 
E.M.F.  of  the  chain: 

-  Pt,  H2 1  Acetate  |  KC1  (sat.)  |  KC1  (0.1  M)  Hg2Cl2 1  Hg  + 

at  18°,  to  the  cubic  centimeters  of  N-HC1  added  to  20  cc.  N- 
sodium  acetate  and  diluted  to  100  cc.     If,  for  instance,  the  poten- 

x-  i  f       j  •    n  xo™      M     ^        j.-      Concentration   of   HC1    . 

tial  found  is  0.4800  volts,  the  ratio    is 

Concentration  of  NaAc 

20  2 

— '—    Hence  the  sodium  acetate  is  0.9901N. 

20.0 

TABLE  62 


CUBIC  CENTIMETERS  OF  N/l  HC1  TO  20  CUBIC 
CENTIMETERS  N/l  NaAc  DILUTED 
TO  100  CUBIC  CENTIMETERS 

E.  M.  F. 

19.00 

0.5270 

19.40 

0.5155 

19.50 

0.5125 

19.90 

0.4945 

20.00 

0.4898 

20.39 

0.4712 

20.89 

0.4549 

21.00 

0.4525 

XXIV  CHECK   SOLUTIONS  485 

These  values  are  more  convenient  to  use  if  plotted  as  Walpole 
has  done. 

Walpole  found  the  above  cell  with  "standard  acetate"  at  18°C. 
to  be  0.6046.  The  contact  potential  still  to  be  eliminated  was 
estimated  by  the  Bjerrum  extrapolation  to  be  0.0001  volt.  This 
is  negligible. 

The  value  0.6046  seems  to  be  the  value  of  the  chain  corrected 
to  one  atmosphere  hydrogen  plus  vapor  pressure. 
M 

ACID   POTASSIUM  PHTHALATE 

20 

It  will  be  noted  that  both  S0rensen's  standard  glycocoll  (see 
page  486)  and  the  standard  acetate  solutions  must  be  constructed 
by  adjustment  of  the  ratio  of  the  components.  While  there  is 
no  great  difficulty  in  this  there  remain  the  labor  and  the  chance  of 
error  that  are  involved.  Clark  and  Lubs  (1916)  have  shown 
that  acid  potassium  phthalate  possesses  a  unique  combination 
of  qualities  desirable  for  the  standard  under  discussion.  The  first 
and  second  dissociation  constants  of  phthalic  acid  are  so  close  to 
one  another  that  the  second  hydrogen  comes  into  play  before  the 
first  is  completely  neutralized  (see  fig.  5  page  28).  As  a  con- 
sequence the  half-neutralized  phthalic  acid  (KH  Phthalate) 
exhibits  a  good  buffer  action.  The  salt  of  this  composition  crystal- 
lizes beautifully  without  water  of  crystallization,  and,  as  was 
shown  by  Dodge  (1915)  and  confirmed  by  Hendrixson  (1915)  it 
is  an  excellent  substance  for  the  standardization  of  alkali  solutions. 
As  such  it  is  used  to  standardize  the  alkali  entering  into  the  buffer 
mixtures  of  Clark  and  Lubs  (see  page  197).  The  outstanding 
feature  is  that  the  ratio  of  acid  to  base  is  fixed  by  the  composi- 
tion of  the  crystals  and  not  by  adjustment  as  in  other  standards. 
The  salt  may  be  dried  at  105CC.  and  a  solution  of  accurate  con- 
centration constructed. 

The  original  data  of  Clark  and  Lubs  (1916)  for  the  cell      • 

Pt,  H2  (1  atmos.)   |  KH  Phthalate  (0.05  Molar)  |  KC1  (sat.) 

B 
|  KC1  (0.1  N),  HgCl  |  Hg 

was  0.5689  volts  at  20°C.  Using  0.3379  for  the  half-cell  to  the 
right  of  B  and  neglecting  liquid  junction  potential  at  B,  we  ob- 
tain pH  =  3.974. 


486 


THE  DETERMINATION  OF  HYDROGEN  IONS 


If  we  assume  inappreciable  change  in  this  value  between  18° 
and  40°  [see  Kolthoff  and  Tekelenburg  (1927)]  we  obtain  the 
following  tentative  values. 


Half  Cell  I:    Pt,  H2  (1  atmos.) 


KC1  (sat.) 


Cell    II: 
Cell  III: 


Half  cell  I 
Half  cell  I 


KH  Phthalate 

0.05  M 

KC1  (sat.)  |  KC1  (0.1  N),  HgCl 
KC1  (sat.),  HgCl  |  Hg 


Hg 


TABLE  63 


POTENTIAL  IN  VOLTS  OF  CELL  OR  HALF-CELL 


TEMPERATURE 

I 

II 

III 

°c. 

volts 

volts 

volts  (approx.) 

18 

-0.2292 

0.5672 

0.480 

20 

-0.2310 

0.5689 

0.481 

25 

-0.2347 

0.5723 

0.481 

30 

-0.2386 

0.5757 

0.481 

35 

-0.2426 

0.5791 

0.481 

38 

-0.2449 

0.5810 

0.481 

40 

-0.2465 

0.5823 

0.481 

There  have  been  objections  to  the  use  of  phthalate  solutions 
as  standards,  based  upon  the  reduction  of  phthalate  at  the  hydro- 
gen electrode.  A  discussion  of  this  is  found  on  page  437.  See 
also  Kolthoff  and  Tekelenburg  (1927). 

OTHER   STANDARD   BUFFERS 

Any  one  of  the  buffer  mixtures  having  a  well  defined  pH-value 
may  be  used.  There  then  is  implied  the  acceptance  of  the 
standard  conditions  under  which  the  pH  value  was  determined 
in  the  first  instance.  S0rensen  (1909),  having  established  his 
basis  by  the  method  indicated  in  the  previous  chapter,  used  that 
mixture  of  eight  volumes  of  his  standard  glycocoll  to  two  volumes 
of  his  standard  hydrochloric  acid  which  is  described  in  Chapter  IX. 

HYDROCHLORIC   ACID    SOLUTIONS 

S0rensen  and  Linderstr0m-Lang  (1924),  Cullen,  Keeler  and 
Robinson  (1925),  Michaelis,  Kolthoff  and  others  advocate 


xxrv 


CHECK   SOLUTIONS 


487 


0.01  N  HC1  +  0.09  N  KC1,  or  other  mixtures  of  low  acid  con- 
centration. See  Michaelis  and  Kakinuma  (1923),  Michaelis  and 
Fujita  (1923)  and  Michaelis  and  Mizutani  (1924),  Biilmann 
(1927)  and  page  472.  Michaelis  and  Kruger  (1921)  use  0.0025  N 
HC1  +  0.0975  N  KC1.  Because  of  the  difficulty  of  calculating 
(H+)  in  such  mixtures  0.1  N  HC1  is  preferred  by  some. 

In  the  use  of  0.1  M  HC1  solution  as  a  working  standard 
the  inclination  has  been  to  make  it  the  ultimate  standard.  How- 
ever, attention  has  been  called  to  the  fact  that  the  liquid  junction 
potential  is  a  difficult  matter  to  handle  both  experimentally  and 
theoretically.  It  is  doubtful  whether  these  standards  are  well 
adapted  to  routine  standardization. 

With  this  caution  we  may  call  attention  to  the  pH  values 
stated  in  table  35a,  page  201,  and  to  the  corresponding  hydrogen 
electrode  potentials  given  in  table  A,  page  672. 


For  convenience  we  shall  repeat  here  the  arbitrarily  assigned 
values  of  the  practical  half -cell 

|  KC1  (sat.)  |  KC1  (0.1  N)  HgCl  |  Hg 
This  is  not  the  half-cell 

||KCl(0.1N),HgCl|Hg 

which  is  the  true  tenth  normal  calomel  half-cell  without  liquid 
junction. 

TABLE  64 
Arbitrary  values  of  practical  tenth  normal  calomel  half-cell 


t 

POTENTIAL 

t 

POTENTIAL 

18 

0.3380 

35 

0.3365 

20 

0.3379 

38 

0.3361 

25 

0.3376 

40 

0.3358 

30 

0.3371 

488  THE    DETERMINATION    OF   HYDROGEN   IONS 

SATURATED   KC1   CALOMEL   HALF-CELL 

As  stated  in  Chapter  XXII  the  temperature  coefficient  is  un- 
certain. The  values  given  in  Chapter  XXII  are  as  shown  in 
table  65. 

TABLE  65 


t 

POTENTIAL 

t 

POTENTIAL 

18 

0.251 

35 

0.238 

20 

0.250 

38 

0.236 

25 

0.2458 

40 

0.234 

30 

0.242 

QUINHYDRONE   HALF-CELLS 

See  Chapter  XIX. 

CAUTION 

The  investigator  who  has  been  following  a  particular  system 
of  standardization  may  find  in  table  A,  page  672,  one  or  another 
value  which  he  is  prepared  to  dispute.  The  author's  own  data 
for  the  "saturated  calomel  half-cell"  at  30°C.  is  appreciably 
higher  than  that  given  in  the  table.  Attention  has  been  called 
to  the  unsatisfactory  temperature  coefficient  in  this  case.  See 
page  455.  At  several  points  in  this  book  attention  is  being  called 
to  several  matters  which  need  investigation.  Emphasis  of  this 
aspect  seems  wiser  than  partiality  in  the  selection  of  values.  The 
emphasis  seems  particularly  important  at  the  present  time  be- 
cause in  some  instances  the  elegancies  of  formulation  have  ob- 
scured discrepancies  in  experimental  data. 

In  addition  the  assumption  on  which  table  A  is  based  introduces 
a  source  of  discrepancy. 


CHAPTER  XXV 

THE  THEORY  OF  DEBYE  AND  HUCKEL 

I  am  not  satisfied  with  the  view  so  often  expressed  that  the  sole  aim 
of  scientific  theory  is  "economy  of  thought"  I  cannot  reject 
the  hope  that  theory  is  by  slow  stages  leading  us  nearer  to  the  truth 
of  things. — A.  S.  EDDINGTON. 

INTRODUCTION 

The  chemist  who  is  untrained  in  the  methods  of  mathematical 
physics  will  regard  the  papers  of  Debye  and  Huckel  as  of  "f rightful 
mien;"  but  he  is  becoming  familiar  with  the  simple,  final  equations 
as  they  occur  with  ever  increasing  frequency  in  current  journal 
articles,  and  as  they  are  applied  to  a  wide  variety  of  important 
problems.  The  theory  attains  its  momentum  at  the  time  our 
respected  and  beloved  Arrhenius  passes  from  the  world.  It  will 
doubtless  come  to  be  regarded  as  the  greatest  of  the  justifications 
of  Arrhenius'  brilliant  theory.  This  is  not  alone  because  it  deals 
vigorously  with  those  anomalies  which  have  constituted  the  weak 
point  in  the  theory  of  electrolytes;  it  is  largely  because  Debye 
and  Huckel,  going  in  the  direction  indicated  by  Milner,  have  es- 
tablished connection  between  the  more  purely  thermodynamic 
trend  of  the  recent  period  and  statistical  mechanics.  This 
achievement,  and  the  fact  that  it  is  stimulating  new  types  of  in- 
vestigation, mark  the  beginning  of  a  new  period  in  the  develop- 
ment of  Arrhenius'  theory.  The  achievement  is  injured  but  little 
by  the  several  stated  and  implied  limitations  imposed  by  the 
introduction  of  simplifying  assumptions  in  the  first  struggle  with 
the  difficulties. 

Because  of  the  difficult  mathematical  argument  used  by  Debye 
and  Huckel,  I  cannot  discuss  the  details.  Only  the  outline  will 
be  given.  No  doubt  this  will  not  be  considered  satisfactory  by 
those  who  are  well  acquainted  with  the  subject.  However,  the 
importance  of  the  theory  is  my  justification  for  an  attempt  to 
sketch  the  argument.  If  a  reader  will  not  make  the  mistake  of 
using  such  an  outline  when  he  should  consult  the  original  papers 

489 


490  THE   DETERMINATION    OF   HYDROGEN    IONS 

he  may  find  it  to  be  of  some  aid  to  his  understanding  of  what  the 
simple  final  equations  are  about. 

The  central  idea  in  the  theory  of  Debye  and  Hiickel  (1923)  is 
this :  Although  ions  in  solution  may  not  obey  strictly  the  ideal  gas 
laws  because  of  the  same  sort  of  interferences  which  obtain  in  the 
case  of  neutral  molecules,  there  is,  in  the  case  of  ions,  the  added 
interference  of  the  mutual  interaction  of  the  electrically  charged 
particles.  Account  of  this  must  be  taken  when  there  is  formu- 
lated the  free  energy  of  transfer  of  a  particular  kind  of  ion  from 
one  concentration  to  another,  because  the  free  energies  of  separa- 
tion at  two  different  ion  concentrations  differ.  Dilution  of  a 
solution  increases  the  dispersion  with  consequent  closer  approach 
of  the  conduct  of  the  ions  to  the  laws  of  the  ideal  gas.  Were  this 
interionic  action  alone  responsible  for  deviations  from  the  gas  laws, 
its  effect  should  fully  account  for  those  correction  terms  which  we 
have  previously  described  as  the  activity  coefficients.  (See  Chap- 
ter XI,  page  236.)  Debye  and  Hiickel  show  that  on  this  basis 
the  correction  terms  for  very  dilute  solutions  can  be  calculated. 

One  of  the  most  important  of  the  main  results  is  the  following 
simple  equation,  applicable  to  very  dilute  aqueous  solutions  at 
25°C. 

-  log  7,  =  0.5  zj 

where  71  is  the  activity  coefficient  of  an  ion  of  the  ith  kind  with 
valence  zi?  and  where  /*  is  the  "ionic  strength"  of  the  solution. 
The  ionic  strength  of  the  solution  is  obtained  by  multiplying  the 
concentration  of  each  ion  by  the  square  of  that  ion's  valence 
number,  summing  all  these  products  and  dividing  the  result 
by  two. 

The  equation  written  above  is  a  limiting  equation  applicable 
only  at  very  high  dilution.  For  moderately  dilute  solutions  the 
average  diameter  of  the  ions  is  taken  into  account  and  the  equa- 
tion then  is 

0.5  z? 
-  log  71 


1+3.3X 
where  a  is  the  average  ionic  diameter. 


XXV  DEBYE-HUCKEL   THEORY  491 

DERIVATIONS 

Fix  attention  upon  a  positive  ion  (see  figure  85).  Let  it  have 
an  effective  radius  a,  by  which  will  be  understood  a  limit  within 
which  other  ions  cannot  penetrate.  This  radius,  a,  will  enter  the 
argument  later.  Concentric  with  the  ion  considered,  imagine 
there  to  be  shell  of  radius  r,  in  which  we  find  an  element  of  space 
of  infinitesimal  thickness  dr  and  infinitesimal  volume  dv,  situated 
as  shown  in  figure  85. 

The  first  problem  is  to  find  some  expression  for  the  relative 
numbers  of  positive  and  negative  ions  which  will  enter  dv,  which 
is  in  the  electric  field  of  the  central  ion. 

For  this  purpose  there  is  used  the  Boltzmann  principle.  We 
shall  employ  it  somewhat  loosely. 


FIG.  85 

When  a  positive  ion  enters  dv  it  gains  potential  energy  of  posi- 
tion by  reason  of  its  approach  to  the  repelling  central  ion.  Like- 
wise when  a  negative  ion  enters  dv  it  loses  potential  energy.  When 
an  ion  enters  dv  let  AF  be  the  gain  in  energy  per  mole  of  a 
positive  ion  of  valence  za.  Let  N0  represent  the  Avagadro 
number.  Let  [a]!  be  the  concentration  of  positive  ions  of  the  ath 
kind  expressed  in  moles  per  cubic  centimeter.1  Let  e  be  the 
elementary  electric  charge  and  \j/  the  potential. 


(I)2 
Were  there  no  interionic  force,  the  positive  ions  of  the  ath 

1  This  space  relationship  will  later  be  translated  to  moles  per  liter. 

2  N0[ali  dv  gives  the  number  of  particles  and  N0[a]i  dv  zae  the  number  of 
charges.     The  number  of  unit  charges  multiplied  by  the  potential  at  the 
place  found  is  the  energy  required  to  bring  the  ions  from  a  place  of  zero 
potential. 


492  THE   DETERMINATION   OF   HYDROGEN   IONS 

kind  would  be  evenly  distributed  and  their  concentration  would 
be,  stoichiometrically,  [a]2.  Except  for  the  work  included  in  AF 
we  will  assume  that  the  ions  behave  as  an  ideal  solute.  Then 
the  free  energy  of  transfer  between  an  imagined  homogenous 
solution  in  which  the  concentration  is  [a]2  and  the  place  where  the 
concentration  is  [a]i  is  given  by  (2). 

-  AF  =  RT  In  [^~  (2) 

LaJ2 

Apply  (2)  to  account  for  the  energy-change  locally  between  the 
condensed  state  and  that  of  complete  dispersion.  A  combina- 
tion of  equations  (1)  and  (2)  gives  (3)3  where  e  is  the  base  of 
Naperian  logarithms. 

r  i        r  i  (        No  za  e  $\  ( 

[aji-[a]tle—        RT      1 

This  is  a  special  application  of  the  Boltzmann  principle.4  Equa- 
tion (3)  states  that  the  concentration  of  the  ions  in  dv,  namely 
[a]i  is  a  function  first  of  the  concentration,  [a]2,  which  would  be 
found  there  were  there  no  interionic  force  and  second  an  ex- 
ponential function  of  the  ratio  of  the  potential  energy  to  the 
thermal  energy.  The  parenthesized  term  of  (3)  can  be  expanded 
by  the  formula 

•\r  -y-2  V-3 

«-1  +  ii  +  fi  +  fi    etc- 

(See  Mellor,  Higher  Mathematics.)    An   approximation5  is  here 


-  i        — 

8  x  =  y  In  w  may  be  written  w  =  ey.    Hence  7-7-  =  eRT. 

[a]  2 

4  See  p.  1025  of  article  by  Dushman  in  Taylor's  Treatise  on  Physical 
Chemistry. 

6  Instead  of  the  approximation  being  presented  in  this  way,  it  is  some- 
times found  that  the  equations  are  kept  in  exponential  form  till  the  equa- 
tion for  the  density  5,  appearing  in  our  equation  (6),  is  in  exponential  form. 
Then  there  appears  the  term 


which  is    —2   sin  hyp  jr™.    Here  "sin  hyp,"  sometimes  written  "sinh," 
signifies  hyperbolic  sine  (see  Mellor-Higher  Mathematics).    It  is  at  this 

point  that  the  approximation  is  introduced  since  —2  sin  hyp  -j^-p  is   ap- 

fj, 
proximately  —2;. 


XXV  DEBYE-HUCKEL   THEORY  493 

considered  permissible  and  all  terms  after  the  second  are  ignored. 
Then  (3)  becomes: 

r  i          r  i          r  -,    No  za  e  i/'  ,  N 

[a]i  =  [a]2  -  [a]2  —      -  (4) 


Likewise  for  a  negative  ion  of  the  bth  kind  and  valence  Zbi 

<5> 


Confine  attention  for  the  moment  to  a  solution  which  contains 
only  ions  of  the  kinds  a  and  b.  The  density  of  electrostatic 
charge  in  any  element  of  volume  dv  is  determined  by  the  dif- 
ference between  the  numbers  of  positive  and  negative  charges 
brought  there  by  these  ions.  If  this  density  be  denoted  by  5, 

5  =  No  [a]i  za  e  -  N0  [b]i  zb  fe  (6) 

Combination  of  (4),  (5)  and  (6)  yields  (7). 

5  =  (N0  [a],  za  e  -  No  [b],  zb  €)  -  ^         [[a],  z*  +  [b],  zj]     (7) 


Since  the  subscripts  "2"  refer  the  concentrations  to  the 
stoichiometrical,  the  rule  of  electroneutrality  of  the  solution  as  a 
whole  demands  that  the  first  parenthesized  two  terms  to  the  right 
of  (7)  reduce  to  zero.  Were  more  than  two  kinds  of  ions  con- 
cerned, there  would  appear  a  similar  but  more  extended  set  of 
these  terms,  but  the  differences  between  them  would  be  zero.  To 
express  the  more  general  equation  the  bracketed  part  of  the  last 
term  in  (7)  may  be  replaced  by  2  (cz2)  which  indicates  that  the 
concentration  per  cubic  centimeter  of  each  ion  is  to  be  multiplied 
by  the  square  of  that  ion's  valence  and  all  such  products  added 
together.  Equation  (7)  may  then  be  written  in  the  more  general 
form  of  (8) 

(8) 

There  is  now  to  be  found  a  relation  between  the  density  of 
electrostatic  charge,  6,  the  potential  ^  and  the  radial  distance,  r, 


494  THE    DETERMINATION    OF   HYDROGEN    IONS 

of  the  element  of  volume  dv  from  the  central,  positive  ion.     Here 
there  is  applied  Poisson's6  equation,  which  is  : 


dr  D 

Here  D  is  the  dielectric  constant  of  the  medium  and  TT  has  its 
ordinary  mathematical  significance. 
Substitute  (8)  in  (9)  to  obtain  (10). 


DRT 

On  examination  of  the  coefficient  of  \J/  in  (10),  it  is  found  to  have 
the  dimensions7  of  the  square  of  a  reciprocal  length.     Designate 

this  length  by  -.     Then 

1  47rN*62:S(cz2) 

=  K  -- 


6  It  has  been  said  that  the  introduction  of  the  Poisson  equation  in  the 
treatment  of  this  subject  was  a  stroke  of  genius.  By  its  use  Debye  and 
Hiickel  avoided  the  chief  difficulty  encountered  by  Milner  (1912-13)  who 
had  mastered  the  principles  of  the  subject  but  who  failed  to  develop  equa- 
tions which  da  not  require  elaborate  trial  calculations. 

This  equation  of  Poisson  (Simeon  Denis  Poisson,  1781-1840)  is 

-  47r5 
v"V  =  —  =—  Vector  Analysis 


5V       dV       5V  4?rS 

--  1  ---  1  --  =  --  Rectangular  coordinates 

dx2       dy2        Oz2  D 

' 


dr          dr>         sin  6  50  50  sin2  6 

=  --  Polar  (spherical)  coordinates 

The  last  equation  becomes  (9)  on  the  assumption  of  spherical  symmetry. 
In  the  equation  written  in  the  terms  of  Vector  analysis  VV  represents  the 
operation  of  the  next  equation.  V  is  called  "nabla,"  "alted"  or  "del." 

For  the  development  of  Poisson's  equation  see  Gibbs  and  Wilson  (1925), 
Vector  Analysis,  pp.  206  and  230. 

7  For  brief  discussions  of  dimensions  see  Smithsonian  Physical  Tables 
or  International  Critical  Tables. 

[N3  [e2]  fc]  _  [m-2]  U2]  [ml-3]  _  1 

[D]  [R]  [T]  =  [e2  f-1  I-2]  [flm-1  T-1]  IT]  =  F2 


XXV  DEBYE-HUCKEL   THEORY  495 

On  examining  the  equations  leading  to  (11)  Debye  and  Hiickel 
find  that  the  length  -  is  (approximately)  that  radial  distance  at 
which  the  density  of  the  ion-atmosphere  about  the  central  ion 

declines  an  -  th  part.8    As  shown  by  (11)  this  length  is  determined 
e 

by  the  concentrations  of  the  ions,  the  ion  valencies,  the  dielectric 
constant  of  the  medium  and  the  temperature.  If,  for  instance, 
the  temperature  T  increases,  the  length  increases, — an  expression 
of  the  tendency  of  increased  thermal  agitation  to  make  the  ion- 
distribution  more  nearly  uniform.  If  z,  any  ion  valence,  increases, 
the  length  decreases, — an  expression  of  the  local  clustering  effect 
of  ions  with  high  valence. 

Now  substitute  (11)  in  (10)  and  obtain  (12),  or  (12a)  (the  latter 
by  the  notation  of  footnote  6). 

;r)  =  *2  *  (12) 

ar/ 

V2  \f/  =  «2  \l/  (12a) 

Equation  (12),  or  (12a),  is  a  linear  differential  equation  of  the 
second  order  when  all  terms  involving  powers  of  ^  greater  than 
one  are  suppressed  in  accordance  with  the  first  approximation 
noted  on  page  492.  Then  the  solution  of  (12)  becomes: 

(13)9 

8  The  conception  involved  is  of  importance  to  the  treatment  of  the  so- 
called  Helmholtz  double-layer.     Consider  a  particle  or  an  electrode  sur- 
face which,  for  any  reason,  has  a  potential  different  from  the  solution  with 
which  it  is  in  contact.    There  will  be  near  the  interface  a  greater  density 
of  positive  or  negative  ions  according  to  the  sign  of  the  relative  potential 

of  the  particle  or  electrode.    The  distance  —  represents  the  distance  at 

which  the  potential  difference  has  declined  to  -  th  of  its  value  at  the  inter- 

e 

face  considered  as  a  mathematical  surface. 

For  a  discussion  of  the  applicability  of  this  concept  to  the  study  of  the 
precipitation  of  colloids  by  neutral  salts  see  Burton  (1926)  and  forth- 
coming article  by  Mueller. 

9  The  general  solution  of  (12)  has  been  given  by  Gronwall  (1927).     A 
more  complete  treatment  is  to  appear  in  Physik.  Zeit.  in  a  joint  paper 
with  LaMer  and  Sandred. — Personal  correspondence  with  Dr.  V.  K.  LaMer. 


496  THE    DETERMINATION    OF   HYDROGEN    IONS 

In  equation  (13)  A  and  A'  are  integration  constants.  Of  these 
A'  must  be  zero;  otherwise  \l/  would  approach  infinity  instead  of 
zero  as  r  approaches  infinity.  Hence 

I  =  A (14) 


The  linear  approximation  can  be  obtained  as  follows.     Perform  the 
indicated  operations  to  obtain  the  identities: 


1   d  (     dA  _  dty       2  <ty  _ 

I    j.2    \   =  _l_ = 

r2  dr  \     drj  ~  <fr*        r  <fr 


Hence  by  (e),  (f)  and  (d) 


(12) 


Multiply  by  r  and  transpose  to  obtain: 

d2<f/  d\f/ 

dr2  dr 

or 

— — K2  (rtfO  =  0  (b) 

dr2 

We  now  have  r  ^  as  variable  instead  of  \f/. 
Let 

r^  =  y  (c) 

Then 


-*>y=0  (d) 

Now  try  the  solution 

Then 


Xr  f    ^ 

y  =  e  (e) 


X'  eXr  -   *2  e^  =  0  =  eXr  (X2  -  /c2) 
or 

X  =  ±  K  (g) 

Now  combine  (g)  and  (e) 

y  =  e*  "  (h) 

Substitute  (h)  in  (c) 

iV  =  e±lcr 
or  in  general 


where  A  and  A'  are  integration  constants. 

Equation  (i)  is  identical  with  (13)  of  the  text.  The  result  may  be 
verified  by  performing  the  operations  indicated  by  the  operator  V2^  of 
equation  (12a).  See  footnote  6. 


XXV  DEBYE-HUCKEL  THEORY  497 

The  potential  \f/i  at  any  point  in  the  interior  of  the  central  ion 
(see  figure  85)  of  valence  Zi  is: 


where  —  is  the  part  contributed  by  the  ionic  charge  of  the  central 
Dr 

ion  and  B  is  the  part  contributed  by  the  surrounding  ion-atmos- 
phere. In  the  description  of  figure  85  it  was  specified  that  a 
is  the  limit  of  approach  of  other  ions  to  the  central  ion.  At  this 
limit  the  potential  of  the  surrounding  ion-atmosphere,  given  by 
(14),  must  equal  \f/i  given  by  (15).  Also  at  this  limit  r  =  a. 
Then 

Ae-n=^  +  B  (16) 

a         Da 

Furthermore  the  field  strengths  —  must  become  equal.     Hence 

da. 

differentiate  (14)  and  (15)  and  equate  by  —  =  —  letting  r  =  a. 

dr        dr 


Solve  for  A,  substitute  in  (16)  and  find  B. 

_  ZiC*  /.ox 

" 


These  steps  have  not  only  yielded  the  integration  constant,  A, 
of  (14)  but  have  led  directly  to  B,  the  desired  quantity,  which  is 
the  potential  of  the  central  ion  due  to  the  surrounding  ion- 
atmosphere,  assuming  that  there  is  a  definite  limit,  a,  to  the 
approach  of  the  ion-atmosphere.  If  the  central  ion,  instead  of 
being  the  positive  ion  considered  so  far,  has  a  valence  ±zj,  the 
work  of  removal  will  be: 

,M(=FB)  =       .       4*'* 
2  r  2  D(l  +  «  a) 

10  This  may  be  derived  from  Poisson's  equation  by  making  5  =  0. 


498         THE  DETERMINATION  OF  HYDROGEN  IONS 

For  No  ions  the  work,  w,  of  removal  will  be: 

No  z?  c2  K 
W  =  2D(l+Ka) 


(20) 


In  (20)  w  is  the  free  energy11  involved  in  the  removal  of  one 
mole  of  ions  of  the  i  th  kind  from  the  electrical  field  of  their  ion- 
atmospheres  to  an  infinitely  dilute  solution  of  the  same  medium 
at  the  same  temperature. 

If  two  solutions  of  these  ions  of  concentrations  Ci  and  Co  were 
ideal,  the  free-energy  of  transfer  would  be 

-  A  F  =  RT  In  *£  (21) 

Co 

If  the  solution  of  concentration  Ci  were  not  ideal  but  that  of 
the  infinitely  dilute  solution  of  concentration  C0  were  ideal,  the 
observed  free  energy  increase  would  be 

-  A  F  =  RT  In  *£  +  RT  In  Tl  (22) 

Co 

where  71  is  the  activity  coefficient  described  on  page  236.  On  the 
assumption  that  the  interionic  electrostatic  forces  are  alone 
responsible  for  deviation  from  the  ideal  (or  limiting)  law  of  solu- 
tions it  is  obvious  that  the  term  RT  In  71  of  (22)  is  —  w  of  (20), 
and  that,  when  solutions  are  being  described  by  the  ideal  laws, 
this  term  must  be  applied  as  a  correction.  Hence 

No  zf  e2  K 


The  equivalent  of  K  by  equation  (11)  will  now  be  recalled;  but 
instead  of  retaining  c,  moles  per  cubic  centimeter,  we  shall  use  C, 
moles  per  1000  cubic  centimeters  (approximately  moles  per 
liter).  Then  equation  (11)  becomes  (24). 


-/: 


1000  DRT 


(24) 


11  "Free  energy"  (Lewis)  by  reason  of  the  nature  of  the  method  of 
measurement  of  the  electrical  quantities  involved.  See  Debye  (1925), 
Bjerrum  (1926),  Br0nsted  (1927)  and  particularly  E.  Q.  Adams  (1926). 


XXV  DEBYE-HUCKEL   THEORY  499 

In  combining  equations  (23)  and  (24)  we  may  segregate  the 
universal  constants,  N0,  e,  R,  and  IT  and  may  substitute  their 
numerical  values. 

No  =  6.061  X  1023;     5  =  4.774  X  1Q-10; 
R    =  8.315  X  107;      TT  =  3.1416. 

Equation  (23)  will  also  be  transformed  to  the  use  of  logarithms 
to  the  base  10. 12  There  will  then  remain  two  quantities  D,  the 
dielectric  constant,  and  T,  the  absolute  temperature,  which  may 
be  given  numerical  values  only  under  special  conditions.  To 
note  how  variations  of  D  and  T  affect  the  calculated  numerical 
form  of  the  equation  it  will  be  convenient  to  write  the  combined 
equations  (23)  and  (24)  as  follows: 


-log  7,--  •=£  (25) 

1  +  li  a  Vs  (Cz') 


where 

1.2833  X  106 
(DT)1-5 

and 


(26) 


3.557  X  10'  ,     , 

(DD» 

In  place  of  S  (Cz2),  used  in  the  above,  there  is  usually  employed 
Lewis'  p.,  which  is  called  the  ionic  strength  and  defined  by: 

fj.  =  -  (miZi  +  m2Z2  +  msZg  +,       etc.)  (28) 

2 

Here  mi,  m2,  m3  etc.,  are  the  molalities  (moles  per  1000  grams 
of  solvent)  of  the  ions.  Since  the  Debye-Hiickel  theory  was 
derived  with  the  aid  of  space  relations,  concentrations  should  be 
expressed  in  moles  per  1000  cc.  However,  assuming  the  dis- 
tinction between  moles  per  1000  cc.,  moles  per  liter  and  moles 
per  1000  grams  water  to  be  negligible,  we  may  write 

2M  =  2  (Cz2) 
12  By  use  of:  Inx  =  log  ex  =  2.3026  logio  x  =  2.3026  log  x. 


500 


THE   DETERMINATION    OF   HYDROGEN   IONS 


Then  equation  (25)  becomes: 
-  log  71  = 


V2  z2  VI 


V2 


For  values  of  8,  &V2,  P  and  PV2  see  table  66. 

TABLE  66 

Coefficients  for  the  Debye-Huckel  equation 
1.2833  X  106  ™        3.557  X  109 


(29) 


(DT) 


(DT) 


0-6 


t°  (CENTI- 
GRADE) 

T 

D* 

a 

9 

8V2 

WV2 

0 

273.1 

88.0 

0.344 

2.29  X  107 

0.487 

3.24  X  107 

15 

288.1 

82.5 

0.350 

2.31  X  107 

0.495 

3.26  X  107 

18 

291.1 

81.0 

0.354 

2.32  X  107 

0.501 

3.28  X  107 

20 

293.1 

80.5 

0.354 

2.32  X  107 

0.501 

3.28  X  107 

25 

298.1 

78.8 

0.356 

2.32  X  107 

0.504 

3.28  X  107 

30 

303.1 

77.0 

0.360 

2.33  X  107 

0.509 

3.29  X  107 

*  The  values  for  the  dielectric  constant  of  water  as  given  in  the  litera- 
ture vary  to  an  extent  important  to  the  present  purpose.  Since  this  situa- 
tion is  stimulating  reinvestigation  of  the  subject,  the  reader  will  look  for 
new  values  in  the  literature  subsequent  to  the  publication  of  this  book 
and  will  realize  that  the  values  given  above  are  purposely  rounded. 

Table  66  shows  that  temperature  has  little  effect  upon  the 
magnitude  of  the  coefficients.  Therefore  the  final  equation  (29) 
may  be  simplified  to : 


-  log  71  = 


0.5  zf  VM 


1  +3.3  X  ]07  a  VM 


(29a) 


The  constant,  a,  was  specified  to  be  the  radial  distance  within 
which  other  ions  could  not  approach  the  central  ion  of  figure  85; 
but,  in  the  course  of  the  development  of  the  final  equations,  a 
should  be  reinterpreted  as  the  average  effective  diameter  of  all 
the  ions.  In  the  absence  of  experimental,  specific  values  for  this 
average  effective  diameter  of  the  possibly  hydrated  ions,  the 
constant,  a,  becomes  more  or  less  an  arbitrary  constant.  To  a 
ascribe  the  value  1  X  10~8,  which  is  merely  the  order  of  magni- 
tude of  ion  diameters.  It  is  then  readily  calculated,  by  equation 


XXV 


DEBYE-HUCKEL  THEOKY 


501 


(28)  and  the  values  of  JB-v/2  in  table  66,  that,  when  VM  is  less 
than  the  order  of  magnitude  0.1,  equation  (29a)  reduces^prac- 
tically  to: 

-  log  71  =  0.5  zf  VM  (29b) 

There  are  several  experimental  verifications  of  this  last  simple 
equation  (29b)  at  the  high  dilution  called  for  by  the  above  condi- 
tion that  VM  <  0.1.  Furthermore  the  introduction  of  an  average 
diameter,  a,  of  a  reasonable  order  of  magnitude  tends  to  extend 
the  verification  of  the  Debye-Hiickel  theory  by  making  (29a) 
appear  applicable  to  somewhat  more  concentrated  solutions. 

The  above  equations  relate  to  the  activity  coefficient  of  an 
ion  of  the  ith  kind.  If  a  salt  dissociate  so  that  each  molecule 
furnishes  za  ions  of  the  bth  kind  and  zb  ions  of  the  a,th  kind,  za 
being  the  valence  of  the  "a"  ion  and  zb  the  valence  of  the  "b" 
ion,  the  mean  activity  coefficient  of  the  ions,  7B,  may  be  de- 
fined by 

Zb  log  7a  +  za  log  7b 


log  7s  = 


Zb 


Application  of  (29b)  then  yields  (31) 

—  log  78  =  0.5  zazb  V/i 


(30) 


(31) 


If  a  salt  like  MgS(>4  dissociate  to  two  ions  of  the  same  valence 
number,  equation  (31)  is  obtained  again  for  this  case. 

For  salts  of  different  valence-type  the  coefficient  0.5  zaZb  for 
25°C.  has  the  values  shown  below. 


EXAMPLE 

VALENCE-TYPE 

COEFFICIENT 

KC1 

1-1 

0  5 

K2S04  

1-2 

1.0 

A1(N03)3  

3-1 

1  5 

MgS04 

2-2 

2  0 

Ca3(P04)2  

2-3 

3.0 

(Co(NH3)6(Co(CN)6) 

3-3 

4  5 

DISCUSSION 


There  have  been  numerous  experiments  designed  to  test  th*e 
simple  equation  applicable   at  high  dilution  where  the  average 


502  THE    DETERMINATION    OF    HYDROGEN    IONS 

ionic  diameter  is  negligible  and  also  to  test  the  equation  contain- 
ing a,  the  average  ionic  diameter.  These  experiments  cover 
variation  of  dielectric  constant  by  the  use  of  solvents  of  various 
dielectric  constant;  they  cover  variation  of  the  ionic  strength  in 
which  the  ionic  strength  is  obtained  with  salts  of  very  different 
valence-type;  they  cover  measurements  of  the  activity  coeffi- 
cients of  solutes  of  very  different  valence-types. 

See  Noyes  et  al.  on  various  tests  of  the  Debye-Hiickel  equation. 

Substantially,  the  theory  in  the  quantitative  form  given  by  the 
equations  is  confirmed  as  a  limiting  law;  but  obviously  the  theory 
makes  no  pretense  to  deal  with  effects  other  than  the  electro- 
static and  there  are  two  approximations  introduced.  One  is  the 
use  of  the  dielectric  constant  of  the  solvent  in  place  of  the  di- 
electric constant  of  the  solution.  Htickel  (1925)  attempts  to 
correct  for  this.  He  introduces  a  reasonably  deduced  additional 
term.  The  other  approximation  is  in  the  mathematical  develop- 
ment. It  is  in  the  step  taken  to  reach  equation  (4).  After 
expanding  the  series  term  only  the  first  two  terms  of  the  ex- 
pansion were  considered.  LaMer  (1927)  claims  that  a  considera- 
tion of  the  higher  terms  is  sufficient  to  account  for  the  major  por- 
tion of  those  discrepancies  between  theory  and  experiment  which 
have  been  particularly  noticeable  with  salts  of  high  valence,  since 

z2 

a  factor  —  enters  at  successively  higher  powers  for  each  succes- 
a 

z2 

sive  approximation  in  the  solution  of  equation  (12).     When  - 

a 

is  greater  than  0.5  (i.e.  when  a  is  less  than  two  Angstrom  units 
for  a  uni-univalent  salt,  or  less  than  eight  Angstrom  units  for  a  bi- 
bivalent  salt)  a  consideration  of  the  Debye  approximation  alone 
gives  distorted  calculated  results  and  quite  misleading  values  of 

z2 

"a"  according  to  LaMer.     When  —  approaches  unity,   the  in- 

a 

fluence  of  the  higher  terms  is  sufficient  to  make  it  appear  as  if 
the  limiting  slope  were  larger  than  its  value  of  0.5  at  concentra- 
tions as  low  as  those  corresponding  to  O.OOlju.  For  further  details 
of  this  aspect  see  a  forthcoming  paper  by  LaMer,  Gronwall  and 
Sandred.13 

is  private  correspondence  with  Dr.  LaMer. 


XXV  DISCUSSION  503 

There  has  also  been  considered  the  inherent  difficulty  resulting 
from  the  assumption  that  the  ions  have  spherical  fields.  This 
is  to  neglect,  not  only  the  spatial  configurations  demanded  es- 
pecially of  organic  molecules,  but  also  the  polarities  of  large  ions. 

Pending  the  highly  refined  investigations,  experimental  and 
theoretical,  which  are  expected  to  throw  light  upon  the  manner 
in  which  these  and  other  details  of  the  theory  are  to  be  handled, 
we  may  consider  the  Debye-Hiickel  theory  from  the  following 
two  points  of  view. 

In  the  first  place  the  theory  has  been  so  well  substantiated  in 
its  main  outline  that  we  may  have  considerable  confidence  in 
using  the  reduced  equation  to  calculate  corrections  of  the  first 
order  for  very  dilute  solutions  (e.g.  v>  <  0-1)-  For  solutions  of 
slightly  higher  ionic  strength  it  will  be  recalled  that  the  apparent 
ionic  diameter  enters  as  of  numerical  significance.  That  the  use 
of  values  of  a  reasonable  order  of  magnitude  leads  to  corrections 
in  the  right  direction  is  of  general  theoretical  interest. 

In  the  second  place  it  will  be  well  to  remember  that  there  are 
some  conflicting  views  regarding  several  aspects  of  the  theory. 
Mention  was  made  of  LaMer's  objection  to  the  approximation  in 
the  expansion  of  the  series  (see  page  492).  Others  believe  this 
objection  to  be  not  serious.  By  adjusting  the  value  of  a  in 
equation  (29)  there  is  extended  the  range  of  concentrations  within 
which  experimental  data  conform  to  the  calculated  curves.  Such 
adjustment  will  be  considered  empirical  curve-fitting  by  some. 
Others  will  regard  it  as  entirely  justified  by  the  demands  of  the 
theory. 

It  is  not  the  function  of  this  outline  to  discuss  these  and  several 
other  matters  which  are  now  under  discussion.  The  point  to  be 
emphasized  is  this.  In  the  immediate  future  we  may  expect  an 
orderly  presentation  of  correction  terms  stated  by  means  of  the 
equations  given  above. 

In  addition  to  the  terms  stated  there  is  frequently  employed  an 
additional  term  KP/i  placed  as  follows 

0.5  z? 


K8/x  has  been  called  the  "salting  out  term"  and  is  supposed  to 
operate  at  high  salt  concentration. 


504 


THE  DETERMINATION  OF  HYDROGEN  IONS 


SOME  APPLICATIONS 

A  few  examples  of  the  application  of  the  theory  follow. 

Consider  a  salt  which  will  not  react  chemically  with  the  solvent 
or  with  other  salts  present  in  the  solution.  Let  the  salt  chosen 
have  a  very  low  solubility  and  let  it  be  present  in  the  solid  phase 
so  that  its  activity  in  solution  will  be  maintained  constant  while 
the  ionic  strength  of  the  solution  is  changed. 

(salt)  in  solution    =    (salt)  8Olid  phase 

[salt]i7i  =  [salt]2T2  =  [salt]373  etc. 


or 


.08 
.07 
.06 
.05 
.04 
.03 
.02 
.0  I 

.00 


MA 


oNaCI 


K2SO4 


.01       .02      .03      .04     .05      .06      .07      .08      .09        JO        Jl 

V7T 

FIG.  86 


Here  subscripts  indicate  solutions  1,  2,  3  etc.,  brackets  indicate 
concentration  and  parentheses  indicate  activity.  Hence  by 
introduction  of  equation  (31) 


i      [salt]i 

[salt!  =  loS  ^2  -  log  71  =  zazb  0 .5 


(32) 


If  a  pure,  aqueous  solution  of  the  salt  alone  is  used,  only  its  ions 
(and  those  of  water)  contribute  to  M;  but  /*  may  be  varied  by 


XXV 


APPLICATIONS 


505 


adding  extraneous  salts  in  various  concentrations  and  various 
valence-types.  These  should  have  effect  on  the  ratio  of  solu- 
bilities   ^  only  as.  they  affect  p..  On  the  other  hand  a  change 

[salt]2 

in  the  valence-type  of  the  salt  under  study,  while  still  affecting  /*, 
will  make  itself  felt  chiefly  through  new  values  of  zazb.  For  a 
salt  of  fixed  valence-type  the  logarithm  of  the  ratio  of  two  solu- 
bilities is  in  linear  relation  to  the  increment  in  the  square  root 
of  the  ionic  strength  of  the  solution.  At  infinite  dilution,  /*  =  0 
(neglecting  the  ions  of  water)  and,  since  there  is  no  correction  to 
the  gas  law,  log  7  =  0.  Hence  the  data  on  solubilities  should 
give  a  straight  line  when  charted  as  in  figure  86,  and  this  line, 
extrapolated,  should  pass  through  the  origin. 

In  figure  86,  reproduced  from  LaMer's  (1927)  paper,  the  curves 
are  for  the  valence-types  tabulated  below. 


CURVE 

SALT 

VALENCE- 
TYPE 

SOLUBILITY  IN 
WATER 

I 

[Co(NH3)4(N02)  (CNS)]' 
[Co(NH3)2(N02)2(C204)]' 

1-1 

0.  000335  M 

II 

[Co(NH,)4(C,04)]'i  [S206]" 

1-2 
or  2-1 

0.00015  M 

III 

[Co(NH3)6]^[Co(NH,)2(N02)J(C204)]/3 

3-1 
or  1-3 

0.0000504  M 

IV 

fCo(NH3)6'"  [Fe(CN.)]"' 

3-3 

0.000030  M 

In  the  figure  the  salts  used  to  produce  variation  of  /x  are  indicated. 

The  extrapolation  should  lead  to  the  origin  VM  —  0  and  —  log  7 
=  0,  i.e.,  to  no  correction  to  the  gas  laws  at  infinite  dilution. 

Thes^e  data  verify  the  theory.  At  high  dilutions  the  slope  of  a 
curve  is  that  predicted  from  the  numerical  form  of  the  equation 
which  takes  account  of  the  electrical  environment.  The  valence 
factor  (zazb)  is  correct,  since  the  slopes  of  the  several  curves  have 
the  corresponding  ratios  1:2:3:9. 

While  such  results  are  eminently  satisfactory,  difficulties  begin 
with  salts  of  higher  solubilities  for  the  reasons  mentioned  in  the 
foregoing  text.  It  will  be  found  that  a  large  number  of  the  charts 


506 


THE    DETERMINATION    OF    HYDROGEN    IONS 


in  the  literature  take  the  form  of  one  of  the  curves  of  figure  87. 
The  linear  relation  of  the  reduced  equation  (31)  is  seen  as  a 
limiting  relation  obtaining  when  the  ionic  diameter  approaches 
zero.  The  introduction  of  an  assumed  ionic  diameter  (un- 
doubtedly of  the  right  order  of  magnitude)  will  give  a  curve  of 
the  form  shown  in  figure  88. 

We  may  now  pass  to  some  examples  of  particular  importance 
to  our  main  subject  matter. 

Cohn  (1927)  has  gone  over  the  subject  of  phosphate  buffer 
solutions  with  the  aid  of  previous  data  and  new  data  of  his  own 


MOLAR 


O  .3 
O 


.2 


1.0 


a=OA 


.4        .6        .8 

V7T 

FIG.  87 


1.0       1.2       \A 


and  has  attempted  to  account  for  deviations  from  the  simple 
equilibrium  equations  by  means  of  the  Debye-Hiickel  equation. 
Let  us  write  the  relation: 


(33) 


Here  activities  are  indicated  by  use  of  parentheses.     Equation 
(33)  can  be  rewritten  as 


(34) 


XXV 


APPLICATIONS 


507 


Here  brackets  represent  concentrations. 

72  is  the  activity  coefficient  of  the  ion  HP04~~  ~ 
71  is  the  activity  coefficient  of  the  ion  H2P04~ 

pH  is  used  in  (34)  in  its  physical  meaning  of  log  — — ,  since  its 

values  are  obtained  by  the  method  of  the  hydrogen  electrode. 

Assume    complete    dissociation    of    salts   and   therefore    that 
[HPO4 — ]  and  [H2PO4~]  are  determined  from  the  known  concen- 


4.71 
4.72 
4.73 

/ 

^ 

^ 

6.56 
6.66    K 
6.76     | 

6.96    CL 
7.06 
Tl« 

/ 

^ 

/ 

°s 

x 

// 

/ 

/ 

1 

/ 

/ 

/ 

/ 

"* 

hr 

&       A        .6       .8       1.0      1.2      1.4      1.6 

Q. 


FIG.  88.  CORRECTION  CURVES  FOR  pK2'  OF  PHOSPHATE  (o)  AND  pK'  OF 

ACETATE  (•) 


trations  of  the  alkali  salts.     Now  let 
duce  equation  (29a)  in  numerical  form. 

pK  =  PH  -  °'5 


[HPO, 


[H2P04-] 


1  +  3.3  X  107  a 


=  1,  and  intro- 


(35) 


Where  za  is  the  valence  of  the  ion  H2P04~,  namely  1  ;  and  ZB  is 
the  valence  of  the  ion  HP04~  ",  namely  2.     Then  (35)  is 


pK  =  PH  + 


1.5 


1  +  3.3  X  107  a 


(36) 


If  a  in  (36)  were  very  small  the  equation  would  reduce  prac- 
tically to 

pK  =  pH-h  1.5V/I  (37) 


508  THE    DETERMINATION    OF   HYDROGEN   IONS 

In  Chapter  I  it  was  shown  that  under  ideal  conditions  pK  =  pH 


when  the  ratio  of  concentrations 


—  1 

=  1.    The  term  1.5  V/x 


[H2P04- 

'  1. 


of  the  approximate  equation  (37),  or  the  term  — 

1  +  3.3  X  107aVM 

of  (36)  is  then  a  correction  term  for  the  interaction  of  all  the  ions 
present.  If  the  observed  values  of  pH  are  plotted  against  the 
square  root  of  the  ionic  strength  there  should  be  obtained  with 
equation  (37)  a  straight  line;  and  with  (36)  a  set  of  curves  any  one 
of  which  is  dependent  on  the  value  of  a.  In  figure  88  the  linear 
relation  is  shown  and  also  a  curve  which  passes  very  nicely  through 
or  near  the  observed  values.  The  latter  curve  is  drawn  with 
(36)  and  Cohn's  assumption  that  the  mean  ionic  diameter,  a, 
has  the  value  5  X  10 ~8  cm.  Although  this  is  a  reasonable  assump- 
tion in  so  far  as  it  is  a  possible  order  of  magnitude,  it  remains 
an  assumption.  Yet  its  use,  which  in  (36)  yields  (38), 

pK  =  pH  +       L5  ^  r  (38) 

1  +  1.65  VM 

gives  a  mathematical  formulation  of  the  observed  values  which  is 
satisfactory.  Another  way  of  showing  this  is  to  use  (38)  as  is 
done  in  table  67  to  calculate  pK.  It  is  seen  that,  whereas  the  pH 
values  (which  should  be  the  constant  pK  according  to  the  simpli- 
fied theory  of  Chapter  I)  differ  in  the  extreme  by  0.568  unit,  the 
corrected  values  differ  in  the  extreme  by  only  0.040  unit. 

Of  course  when  the  ratio  of  primary  to  secondary  phosphate 
changes,  as  it  does  in  ordinary  buffer  solutions,  the  value  of  the 
ionic  strength,  /z,  changes. 

Cohn  has  also  made  use  of  the  extended  equation: 


1+3.3X  107a\/M 

where  K8ju  is  the  so-called  "salting-out  term."  K8  varies  with 
the  composition  of  the  [mixture  and  is  determined  empirically. 
Cohn  regards  the  above] formula  as  an  "empirical  interpolation 
formula."  With  its  aid  he  has  prepared  a  series  of  charts  and 
tables  with  which  to  ''facilitate  the  preparation  of  buffer  solutions 


XXV 


BUFFERS 


509 


of  the  same  ionic  strength  and  varying  pH  or  the  same  pH 
and  varying  ionic  strength."     See  page  216. 

Cohn,  Heyroth  and  Menkin  (1928)  have  applied  the  same 
principles  to  acetate  systems.  This  is  of  particular  interest  in 
connection  with  the  discussion  of  Chapter  I  where,  with  due 
warning  of  the  consequences,  we  found  that  the  application  of 
the  more  extended  classical  equations  failed  to  yield  a  constant 

TABLE  67 

Corrected  constants  for  phosphate  system  (after  Cohn,  1927} 


EXPERIMENTERS 

%x 

:i 

a. 
M 

1 

H 

^ 

1 

gg 

P 

* 

a 

•* 

i 

w 
A 

0.00133 

0.00267 

0.052 

7.088 

0.071 

7.159 

0.00266 

0.00532 

0.073 

7.068 

0.098 

7.166 

Michaelis  and  Kriiger  < 

0.00334 

0.00667 

0.082 

7.069 

0.108 

7.177 

0.01333 

0.02667 

0.163 

6.990 

0.193 

7.183 

Clark  and  Lubs          

0.03334 
0.05000 
0.06667 
0.06667 
0.06667 

0.06667 
0.10000 
0.13333 
0.13333 
0.13333 

0.258 
0.316 
0.365 
0.365 
0.365 

6.904 
6.843 
6.813 
6.813 
6.817 

0.272 
0.312 
0.342 
0.342 
0.342 

7.176 
7.155 
7.155 
7.155 
7.160 

Michaelis  and  Kriiger      .   . 

S0rensen    

0.12000 

0.2400 

0.490 

6.737 

0.406 

7.143 

0.16667 

0.3333 

0.577 

6.721 

0.433 

7.154 

Cohn  < 

0.33334 
0.50000 
0.60000 

0.6668 
1.0000 
1.2000 

0.817 

i.ooo 

1.095 

6.638 
6.599 
6.570 

0.522 
0.566 
0.585 

7.160 
7.165 
7.155 

0.66667 

1.33333 

1.154 

6.573 

0.596 

7.169 

1.20000 

2.4000 

1.549 

6.520 

0.653 

7.173 

Average  

7.163 

pK  =  pH  + 


1.5 


1  +  1.65 


which  is  satisfactory  for  other  than  purposes  of  approximate 
treatment.  Cohn,  Heyroth  and  Menkin  find  that  in  this  case 
an  apparent  error  is  introduced  by  use  of  the  value  0.3380  for 
the  tenth  normal  calomel  half-cell  at  18°C.  This  is  because  [H+] 
enters  equation  (19)  of  Chapter  I  in  a  sum  and  the  higher  the 
value  of  the  calomel  half-cell  the  higher  the  apparent  value  of 
[H+].  By  reducing  [H+]  by  use  of  a  smaller  value  (0.3355)  for 


510 


THE    DETERMINATION   OF   HYDROGEN   IONS 


the  calomel  half-cell  they  find  a  good  correspondence  between 
calculated  and  observed  corrections.  They  then  find  that  the 
acetate  system  can  be  described  by 


-  log 


[CH3  COO-] 


0.5 


, 

=  pK 


The  graphically  interpolated  values  for  the  correction  term  are 
given  on  page  219.  Figure  88  shows  the  correction  for  various 
dilutions  of  an  equimolecular  mixture  of  acetic  acid  and  sodium 
acetate. 


C2J        030       035        040       045      050 


005       010        015 


02i 
1? 


030        035        040       045        050 


FIG.  89.  APPARENT  DISSOCIATION  EXPONENTS,  pK/  AND  pK2r,  OF  CARBONIC 

ACIDS  AT  DIFFERENT  IONIC  STRENGTHS 

Left:  Points  marked  o  and  ®  determined  by  Hastings  and  Sendroy; 
points  marked  El  calculated  from  Warburg's  data.  Line  determined  by 
pKV  =  6.33  -  0.5  V?.  Right:  pK2'  =  10.22  -  1.1  VM.  (After  Hastings 
Sendroy  (1925).) 

With  the  phosphate  and  acetate  systems  so  described  it  is  now 
possible  to  prepare  buffer  solutions  of  known  ionic  strength  be- 
tween pH  3.6  and  7.6. 

Figure  89  shows  the  effect  of  ionic  strength  (plotted  as  square 
root)  upon  the  apparent  dissociation  constants  (in  terms  of  pK7) 
of  carbonic  acid  as  determined  by  Hastings  and  Sendroy  (1925). 

We  owe  to  Br0nsted  (1921)  a  first  sketch  of  a  possible  syste- 
matic description  of  the  "salt  effects"  found  in  the  use  of  indi- 
cators in  solutions  of  different  salts.  He  emphasized  the  necessity 
of  introducing  the  more  rigid  equations  and  of  considering  the 
"salt  effect"  as  an  expression  of  the  alteration  of  activity  under 


XXV 


INDICATORS 


511 


specific  changes  of  condition,  v.  Halban  and  Ebert  (1924)  give 
an  extensive  treatment  of  picric  acid  which  will  repay  careful 
study.  In  this  they  make  use  of  the  Debye-Hiickel  equation. 

I  am  indebted  to  Dr.  A.  B.  Hastings  and  Dr.  Julius  Sendroy, 
Jr.,  for  their  permission  to  publish  figure  90  in  which  they  show 
the  apparent  variation  of  the  pK  values  of  indicators  as  the  ionic 
strength  of  the  buffer  solution  is  changed  by  means  of  different 


•».0 

4.6 
4.7 
4.8 
4.9 

CL  6.3 
6.4 

7.7 
7.8 
7.9 
8.0 

B.C.G. 

x 

e 

^^° 

—  ^" 

—  * 

. 

/ 

^^ 

^^ 

^.  ._ 
r-^^ 

^ 

/ 

^ 

^ 

^^ 

0  MgCI2 
A  NaCI 

^ 

5 

acp. 

s' 

x'', 

,^- 

*-  ' 

.  —  »- 

—  •£ 

x-'' 

^ 

rr^ 

.-^0— 

*-^ 

X 

^ 

^ 

A  NaCI 
O  MgSO4 

> 

2 

RR. 

/ 

'' 

.  —  * 

.  >• 

xx 

^*- 

.  —  <" 

,-^<*^ 

^^ 

> 

^ 

^^ 

^*- 

U  MgCS04 

^^ 

.1             .2            .3            .4            .£ 

V/7 

FIG.  90.  "SALT  EFFECT"  WITH  INDICATORS 

B.C.G.   =  brom  cresol  green;  B.C. P.   =  brom  cresol  purple;  P.R.  = 
phenol  red.     (Courtesy  of  Hastings  and  Sendroy.) 

buffers  and  added  salts  of  various  types.  Although  the  limiting 
equation  is  inapplicable  these  investigators  have  systematized  the 
experimental  data  in  a  way  which  is  of  far  greater  value  than 
the  loosely  constructed  tables  of  the  past,  and  by  use  of  the 
coordinates  -  -  log  7  and  VM-  There  remains  distinct  evidence 
of  "specific  salt  errors."  This  shows  that,  in  the  use  of  indicators 
with  specific  solutions,  experimental  calibration  must  still  be  used 
whenever  precise  values  are  to  be  stated. 


512  THE   DETERMINATION   OF   HYDROGEN   IONS 

REVIEWS 

The  Theory  of  Strong  Electrolytes.    A  general  discussion  held  by  The 

Faraday  Society,  Trans.  Faraday  Soc.,  April,  1927. 
LaMer.    Recent  Advances  in  the  lonization  Theory  as  Applied  to  Strong 

Electrolytes.    Trans.  Am.  Electrochem.  Soc.,  April,  1927. 
Scatchard.    The    Interaction    of    Electrolytes    with    Non-electrolytes. 

Chem.  Rev.,  3,  383  (1927). 
Annual  Reports  on  the  Progress  of  Chemistry  issued  by  The  Chemical 

Society  (London)  1926  and  1927. 
Also  Hiickel  (1924)  and  Noyes  (1924). 


CHAPTER  XXVI 

SUPPLEMENTARY  METHODS 
But  yet  I'll  make  assurance  double-sure. — MACBETH,  IV:  1 

When  the  control  of  any  process  has  been  found  to  be  indexed  by  the 
activity  or  concentration  of  the  hydrogen  or  hydroxyl  ions,  when  the 
quantitative  relations  have  been  established  and  contributory  factors  are 
controllable,  there  is  established  a  possible  means  of  estimating  the  activity 
or  concentration  of  the  hydroxyl  or  hydrogen  ions.  Many  such  instances 
are  known.  From  among  them  a  few  may  be  chosen  for  their  convenience. 
They  are  spoken  of  here  as  supplementary  methods  because  they  are  super- 
seded in  general  practice  by  indicators,  the  hydrogen  electrode  and  the 
quinhydrone  electrode.  Several  have  historical  value  because  they  were 
used  in  establishing  the  laws  of  electrolytic  dissociation.  Others  have 
intrinsic  value  because  they  are  available  either  for  checking  the  customary 
procedures  or  for  determinations  in  cases  where  there  is  reason  to  doubt 
the  reliability  of  the  usual  methods.  Those  which  are  kinetic  methods 
will  in  the  end  make  their  distinctive  contributions  by  showing  what  they 
can  of  the  correlation  of  certain  kinetic  affairs  with  equilibrium  states. 
Generally  they  are  rather  useful  to  "make  assurance  double  sure." 

An  instance  of  the  last  procedure  is  the  following.  Clibbens  and  Francis 
(1912)  found  that  the  decomposition  of  nitrosotriacetonamine  (see  Heintz, 
1877)  into  nitrogen  and  phorone  is  a  function  of  the  catalytic  activity  of 
hydroxyl  ions.  Francis  and  Geake  (1913)  then  applied  the  relation  to  the 
determination  of  hydroxyl  ion  concentrations,  Francis,  Geake  and  Roche 
(1915)  improved  the  technique,  and  then  McBain  and  Bolam  (1918)  used 
the  method  to  check  their  electrometric  measurements  of  the  hydrolysis 
of  soap  solutions. 

It  is  just  in  such  checking  that  the  value  of  these  so  called  supple- 
mentary methods  will  be  appreciated.  But,  since  they  will  find  only  occa- 
sional use  and  under  circumstances  which  will  require  a  detailed  considera- 
tion of  their  particular  applicability,  there  seems  to  be  no  reason  to  do 
more  than  indicate  a  few  of  the  methods  in  brief  outline. 

Among  the  reactions  which  have  historical  interest  there  are,  besides 
the  most  frequently  studied  inversion  of  cane  sugar,  the  following. 

Bredig  and  Fraenkel  (1905)  used  diazoacetic  ester 

N2CH-CO2  C2H5  +  H2O  =  N2  +  (OH)CH2CO2C2H5 

The  nitrogen  evolved  from  time  to  time  was  measured  and  the  values 

k 
used  in  the  equation  for  a  monomolecular  reaction.    At  25°C.,  —-  =  32.5. 

513 


514  THE    DETEKMINATION    OF   HYDROGEN    IONS 

The  method  was  applied  with  only  partial  success  by  Hober  (1900)  to 
blood.  Van  Dam  (1908)  used  it  in  the  examination  of  rennet  coagulation 
of  milk. 

The  decomposition  of  nitrosotriacetonamine  is  represented  in  outline 
by  the  following  equation: 

/CH2  •  C(CH3)2\  /CH  :  C(CH3)2 

C0<;  >N  -  NO  ->  C0<(  +  N2  +  H20 

XCH2  -  C(CH3)/  NCH  :  C(CH3)2 

The  original  quantity  of  nitrosotriacetonamine  is  known  and  the  extent 
of  the  decomposition  at  the  end  of  measured  intervals  of  time  is  measured 
by  the  volume  of  nitrogen  evolved. 

Francis,  Geake  and  Roche  (I.e.)  found  the  relation  between  the  velocity 

k 

constant  and  [OH~]  to  be  -    "—  ;  =  1.92  at  30°.     See  Colvin  (1926). 
(OH    J 

Br0nsted  (1926)  finds  that  the  rate  of  ad,dition  of  water  to  nitratoaquo- 
tetramine  cobalt  ion  is  very  sensitive  to  the  hydrion  activity  of  the  solu- 
tion and  suggests  the  use  of  the  rate  in  determining  hydrion  activities. 

Numerous  other  methods  are  mentioned  in  the  texts  of  physical  chem- 
istry and,  now  that  interest  in  the  theory  is  reviving,  are  detailed  in  current 
journal  articles. 

For  the  most  part  these  supplementary  methods  are  catalytic  and 
involve  what  are  called  pseudo-unimolecular  reactions.  Consider  the 
reaction 


A  +  H+-^  H+  +  products 

If  [H+j  is  maintained  constant,  as  by  a  buffer  solution,  the  decline  of  [A] 
with  increase  of  time  may  be  described  by 

-  d[A]  =  k'  [A]  [H+] 


dt 

-  d(A] 
[A] 


=  k7  [H+]  dt 


Treat  [H+]  as  constant  and  integrate  between  [A]i  at  time  ti  and  [A]2 
at  time  t2 

_  in  j^ji  =  k'  [H+]  (ti  -  t2) 
If  2.303  k'  =  k 

log  ^  =  k  [H+]  (t,  -  ti)  =  tk  [H+] 


XXVI  INVEKSTON   OF   SUGAR  515 

Many  methods  have  been  used  to  follow  reaction  velocities.  Among 
these  may  be  mentioned  measurement  of  the  gas  evolved,  as,  for  instance, 
i»  the  decomposition  of  nitrosotriacetoneamine  and  the  change  in  optical 
rotation  during  the  hydrolysis  of  cane  sugar  to  invert  sugar. 

Brpnsted  and  King  (1925)  describe  an  apparatus  suitable  for  following 
either  the  decomposition  of  nitrosotriacetonamine  or  any  reaction  of  a 
similar  nature  wherein  nitrogen  is  evolved.  Their  paper  should  be  con- 
sulted for  a  discussion  of  the  manner  in  which  the  salt  concentration  of  a 
buffer  solution  affects  the  velocity  constant. 

The  polarimetric  method  is  described  as  follows  by  Lamble  and  Lewis 
(1915)  (see  Rice  in  Taylor's  Treatise}. 

Polarimeter  tubes  4-dcm.  in  length  were  used,  surrounded  by  jackets, 
through  which  water  at  25°  ±  0.1  was  circulated.  25  cc.  of  standard  hydro- 
chloric acid  solution  was  added  to  25  cc.  of  a  20  per  cent  solution  of  sucrose, 
both  solutions  being  at  25°C.,  and  immediately  the  mixture  was  placed  in 
the  observation  tube;  the  rotation  at  is  noted  at  convenient  time  intervals 
and  the  final  rotation  ««,  is  measured  after  at  least  48  hours  from  the  start 
of  the  reaction.  We  can  assume  that  the  velocity  of  the  reaction  will  be 
proportional  to  the  concentration  of  the  cane  sugar  and  to  the  concentration 
of  the  hydrochloric  acid,  if  the  reaction  takes  place  in  dilute  solution. 
The  velocity  equation  will  be,  therefore, 

[H+]  kt  =  log  jgl 

[A]  2 

where  [H+]  is  the  initial  concentration  of  the  hydrochloric  acid  which  re- 
mains constant  during  the  experiment,  [A]i  is  the  initial  concentration  of 
the  cane  sugar  and  [A]2  is  its  concentration  after  time  t.  The  ratio  is 
independent  of  the  particular  unit  of  concentration  used  so  that  if  the 

rotations  are  additive  we  can  replace  -r~  by  — ~»  where  a0is  the  initial 

IA]2        at  —  « oo 

rotation  and  aro  is  the  final  rotation.  Rosanoff,  Clarke  and  Sibley  showed 
that  the  specific  rotation  of  the  solution  is  an  additive  function  of  its  com- 
position and  also  gave  a  method  for  calculating  a0;  a  slight  error  in  the 
value  of  «0  will  be  greatly  magnified  in  the  value  of  k  calculated  for  the 
earlier  stages  of  the  reaction,  so  instead  of  trying  to  obtain  a0  by  direct 
observation  they  extrapolated  to  t  =  0  the  straight  line  obtained  by 
plotting  values  of  t  against  corresponding  values  of  log  (at  —  «<») ;  this  gives 
far  more  reliable  values  of  log  («0  —  «„)  than  can  be  obtained  by  direct 
measurement. 

For  other  methods  consult  texts  of  physical  chemistry,  for  example  the 
article  by  Rice  in  A  Treatise  on  Physical  Chemistry,  edited  by  Taylor. 

A  large  proportion  of  reactions  proceeding  in  homogeneous  solutions 
are  catalyzed  by  hydrion  or  hydro xyl  ions.  For  this  reason  emphasis  was 
first  placed  upon  these  ions.  However,  it  was  soon  found  that  neutral 
salts  when  added  to  solutions  of  strong  acids  markedly  increase  the  rates 


516        THE  DETEKMINATION  OF  HYDROGEN  IONS 

of  such  reactions  as  the  inversion  of  cane  sugar.  Several  theories  have 
been  advanced  to  account  for  this.  Considerable  systematic  advance  has 
been  made  by  the  use  of  activities  in  place  of  concentrations  in  the  equa- 
tions for  reaction  kinetics  and  by  the  use  of  the  hypothesis  that,  in  the 
formation  of  an  unstable  critical  complex  between  reacting  molecules  and 
ions,  the  charged  complex  is  subject  to  those  interionic  forces  which 
markedly  affect  the  activity  coefficients.  Also  catalytic  functions  are  now 
admitted  for  ions  other  than  hydrogen  and  hydroxyl. 

In  many  instances  these  catalytic  methods  of  determining  hydrogen  or 
hydroxyl  ion  concentrations  may  be  applied  with  neglect  of  the  salt- 
effect  if  only  the  order  of  magnitude  be  desired;  but  if  they  are  applied  for 
accurate  data  the  current  literature  should  be  consulted  for  important 
treatments  of  what  is  often  called  the  salt  effect.  See  especially  Br0nsted 
(1923-1927),  Dawson  (1926-1927),  Scatchard  (1926),  Kilpatrick  (1926), 
Pedersen  (1927)  and  references  to  other  modern  work  in  Annual  Reports 
on  the  Progress  of  Chemistry  for  1927,  London  Chemical  Society  (1928), 
pp.  33  and  331. 

CONDUCTIVITY 

The  conductivity  of  a  solution  is  dependent  upon  the  concentrations  ot 
all  the  ions  and  upon  the  mobilities  of  each.  It  is  therefore  obvious  that 
a  somewhat  detailed  knowledge  of  the  constituents  of  a  solution  and  of 
the  properties  of  the  constituents  is  necessary  before  conductivity  measure- 
ments can  reveal  any  accurate  information  of  the  hydrogen  or  hydroxyl 
ion  concentration.  Even  when  the  constituents  are  known  it  is  a  matter 
of  considerable  difficulty  to  resolve  the  part  played  by  the  hydrogen 
ions  if  the  solution  is  complex.  However,  the  mobilities  of  the  hydrogen 
and  hydroxyl  ions  are  so  much  greater  than  those  of  other  ions  (see  page 
279)  that  methods  of  approximation  may  be  based  thereon.  If,  for  in- 
stance, a  solution  can  be  neutralized  without  too  great  a  change  in  its 
composition  it  may  happen  that  with  the  disappearance  of  the  greater 
part  of  the  hydrogen  ions  there  will  appear  a  great  lowering  in  conductance. 
Then,  with  the  appearance  of  greater  hydroxyl  ion  concentration,  the 
conductance  will  rise.  The  minimum  or  a  kink  in  the  curve  is  a  rough 
indication  of  neutrality.  Thus  the  conductivity  method  is  sometimes 
useful  in  titrations.  See  Kolthoff  for  details  and  references  on  titration 
by  the  conductivity  method. 

The  elementary  principles  of  conductivity  measurements  will  be  found 
in  any  standard  text  of  physical  chemistry  but  the  more  refined  theoretical 
and  instrumental  aspects  are  only  to  be  found  by  following  the  more 
recent  journal  literature.  See  Jones  and  Josephs  (1928). 

Of  course,  the  major  field  of  usefulness  of  the  conductivity  method  has 
been  in  the  determination  of  dissociation  constants  of  weak  acids. 

As  mentioned  in  Chapter  XXV,  change  in  the  ionic  strength  of  a  solu- 
tion changes  the  inter-ionic  forces  which  affect  the  mobilities  of  ions. 
Therefore,  the  original  basis  for  calculating  the  degree  of  ionization  from 
the  ratio  of  conductance  at  one  concentration  to  the  conductance  at  in- 


XXVI  MISCELLANEOUS  METHODS  517 

finite  dilution  must  be  altered.  However,  Maclnnes  (1926)  proposes 
dividing  the  equivalent  conductance  of  an  acid  at  a  given  concentration  by 
the  equivalent  conductance  of  completely  dissociated  acid  at  the  same  ion 
concentration.  He  thereby  obtains  for  acetic  acid,  for  instance,  Ka  = 
1.743  X  10~5  to  1.784  X  10~6.  (A  discrepancy  of  only  0.01  pH  unit  in  the 
range  of  concentration  0.07  to  0.002.) 

MISCELLANEOUS   METHODS 

Were  it  worth  while  there  could  be  detailed  under  this  heading  a  wide 
variety  of  phenomena  which  have  actually  been  used  to  determine  approxi- 
mately the  hydrogen  ion  concentration  of  a  solution.  We  may  instance 
the  precipitation  of  casein  from  milk  by  the  acid  fermentation  of  bacteria. 
This  has  not  been  clearly  distinguished  in  all  cases  from  coagulation 
produced  by  rennet-like  enzymes;  but,  when  it  has  been,  the  precipitation 
or  non-precipitation  of  casein  from  milk  cultures  has  served  a  useful 
purpose  in  the  rough  classification  of  different  degrees  of  acid  fermentation. 
In  like  manner  the  precipitation  of  uric  acid  or  of  xanthine  has  been  used 
(Wood,  1903).  See  also  pages  575  and  582. 

Many  of  the  physical  methods  are  of  considerable  interest.  For  in- 
stance the  determination  of  distribution  ratios  of  a  given  substance  be- 
tween different  solvents  enters  very  frequently  into  the  determination  of 
activities  and  into  the  determination  of  hydrion  activities.  The  fact  that 
water  completely  extracts  certain  salts  from  benzene  solution  has  been 
used  as  an  argument  for  complete  dissociation  in  the  aqueous  phase  (see 
for  example  Hill  ('21)).  Distribution  between  liquid  and  liquid  is  only 
a  special  case  of  heterogeneous  equilibria  and  if  we  attempted  to  discuss 
even  the  main  principles  a  chapter  of  considerable  magnitude  would  soon 
develop.  An  exposition  of  the  matter  is  given  in  such  treatises  as  that  of 
A.  E.  Hill  in  Taylors  Treatise  on  Physical  Chemistry  page  343.  Of  peculiar 
interest  to  biochemistry  is  the  manner  in  which  the  distribution  of  carbon 
dioxide  between  the  gaseous  and  the  liquid  phases  enters  an  equilibrium 
equation  whereby,  with  the  measurement  of  CO2  partial  pressure  and  one 
other  quantity  such  as  "total  carbonate,"  the  pH  value  of  a  bicarbonate 
solution  may  be  determined.  See  Chapter  XXX  under  "Blood."  Thus 
the  bicarbonate  system  is  made  an  indicator  as  truly  as  phenol  red  is  an 
indicator. 

An  interesting  application  of  equilibria  involving  a  gas  phase  is  the 
"electric  nose"  developed  by  Hickman  and  Hyndman  (1928).  A  small 
amount  of  ammonium  salt  is  placed  in  the  acid  solution  which  is  to  be  mixed 
with  an  alkaline  solution.  On  admixture,  ammonia  is  set  free  at  a  partial 
pressure  depending  largely  upon  the  pH  value  of  the  mixture.  This 
ammonja  can  be  aspirated  to  a  separate  aqueous  solution  the  conductivity 
or  reaction  of  which  now  becomes  a  function  of  the  adjustment  in  the  main 
mixture.  A  device  operating  upon  the  response  of  this  "nose"  controls 
the  main  mixing. 

See  also  Osterhout  (1918)  on  the  use  of  partial  pressures  of  CO2  for 
following  respiration. 


518  THE   DETERMINATION   OF   HYDROGEN   IONS 

In  the  literature  are  found  many  and  divers  interesting,  suggestive  or 
obviously  cumbersome  physical  methods.  The  heat  of  neutralization  of 
acids  and  bases  and  the  cessation  of  heat  evolution  when,  in  a  titration, 
neutralization  is  complete  has  been  put  to  use  by  Dutoit  and  Grobet 
(1921).  Cornec  (1913)  attempted  to  estimate  the  end-point  in  titrations 
by  changes  in  refractive  indices.  His  following  of  the  changes  in  freezing 
points  yielded  some  interesting  curves,  for  instance  that  of  chromate- 
bichromate.  Windisch  and  Dietrich  (1919-1921)  put  alteration  of  surface 
tensions  to  use.  In  this  connection  we  may  remark  that  Harkins  and 
Clark  (1925)  find  that  the  surface  tensions  of  solutions  of  sodium  nonylate 
are  especially  sensitive  to  changes  in  pH. 

Correlation  between  changes  in  optical  rotation  and  pH  are  discussed 
briefly  in  Chapter  XXX.  In  Chapter  VII  fluorimetry  is  mentioned. 

Taste  has  its  very  restricted  place. 


CHAPTER  XXVII 

AN  ALTERNATE  METHOD  OF  FORMULATING  ACID-BASE  EQUILIBRIA 

A  particular  statistical  law  can  have  various  origins. — GUYE 

"//  there's  no  meaning  in  it,"  said  the  King,  "that  saves  a  world 
of  trouble,  you  know,  as  we  needn't  try  to  find  any." — LEWIS 
CARROLL,  in  Alice  in  Wonderland. 

The  usual  formulation  of  acid-base  equilibria  starts  with  the  con- 
sideration of  the  ionization  of  the  acid  or  the  base.  If  there  is  used  Br0n- 
sted's  generalization,  namely 

Acid  ^±  Base  +  H  + 

e.g.  HA     ?±  A-    +  H+ 

or  NHt  ^  NH3  +  H+, 

and  the  equilibrium  equation 

(Base)  (H+)  = 
(Acid)  ' 

the  hydrion  appears  of  importance  coordinate  with  the  acid  and  the  base, 
the  acid  and  the  anion  or  the  base  and  the  cation. 

Likewise  the  usual  formulation  of  the  equilibrium  established  at  the 
hydrogen  electrode  involves  the  assumption  that  hydrogen  ionizes  in  the 
sense  of 


and  that  equilibrium  between  the  free  hydrions  in  the  electrode  and  those 
in  the  solution  is  of  primary  importance.  Accordingly  the  activity  of 
free  hydrions  appears  to  be  of  paramount  importance  to  the  operation  of 
a  hydrogen  electrode,  even  in  alkaline  solution.  But  the  activity  of 
hydrions  may  be  as  low  as  10~~14,  or  less,  in  alkaline  solutions  and  the 
concentration  of  hydrions,  calculated  in  the  usual  manner, l  is  of  that  order 
of  magnitude.  The  opinion  has  been  expressed  that  the  support  of  stable 
potentials  by  hydrions  acting  at  concentrations  less  than  10~~10  is  not  to 
be  expected  on  grounds  of  kinetic  theory.  (See  Chapter  XVIII.) 

Now  that  No,  the  number  of  molecules  of  solute  present  per  liter  in  a 
molar  solution,  is  accurately  known,  it  is  certain  that  in  a  solution  having 

1  The  discussion  is  not  seriously  altered  by  maintaining  a  meticulous 
distinction  between  "activity"  and  concentration. 

519 


520  THE    DETEKMINATION   OF   HYDROGEN   IONS 

a  hydrogen  ion  normality  as  low  as  10~13  there  are  about  1010  hydrogen  ions 
per  liter.  This  estimate,  when  taken  in  conjunction  with  the  electrical 
charge  associated  with  each  ion,  may  indicate  how  it  is  that  a  normality 
of  ID"13  H+  may  be  detected. 

But  there  still  remains  the  fact  that  this  normality  is  very  low  in  com- 
parison with  the  other  material  present  even  in  distilled  water.  In  solu- 
tions heavily  buffered  at  pH  13  we  find  the  hydrogen  electrode  or  an  acid 
indicator  rigidly  stabilized  in  its  conduct  and  it  is  questioned  whether  this 
can  be  brought  about  by  such  extreme  relative  dilutions  of  the  hydrogen 
ions  alone.  Keller  (1921)  has  expressed  doubt  of  another  sort.  He  calls 
attention  to  the  diminutive  size  of  the  hydrogen  ion  (allowing  for  hydra- 
tion)  compared  with  a  giant  protein  molecule,  and,  picturesquely  pro- 
portioning the  one  to  the  other  as  a  bacterium  to  a  Mont  Blanc,  he 
questions  the  influence  upon  the  protein  which  is  attributed  to  the 
hydrogen  ion. 

All  these  are  "sharp-hooked  questions"  which,  were  they  "baited  with 
more  skill,  needs  must  catch  the  answer."  In  many  of  the  answers  given 
there  lies  an  easily  detected  fallacy.  It  is  that  our  present  convenient 
modes  of  formulating  relations  are  regarded  as  complete  pictures  of  the 
physical  facts  and  as  such  are  followed  to  the  bitter  end  with  disastrous 
results.  In  a  previous  chapter  we  have  attempted  to  broaden  the  outlook 
just  a  little,  and  have  suggested  that  in  many  cases  a  more  complete 
formulation  of  relations  would  show  that  as  the  physical  effectiveness  of 
one  ion  fades  out  at  extreme  dilution  other  components  of  the  solution 
maintain  the  continuity.  From  this  point  of  view  even  the  more  extreme 
"calculation  values"  retain  a  definite  significance. 

We  shall  show  that  an  extremely  low  hydrogen  ion  concentration  is  sig- 
nificant as  an  index  of  the  state  of  an  equilibrium  in  which  the  hydrogen 
ion  itself  has  little  actual  physical  significance.  Its  introduction  as  a 
component  of  the  equilibrium  is  a  convenient  and  at  the  same  time  a 
stoichiometrically  true  and  mathematically  correct  mode  of  expression 
containing  no  implications  regarding  the  actual  physical  effectiveness  of  a 
low  hydrogen  ion  concentration  as  an  individual  quantity  separable  from 
the  other  components  of  a  solution.  At  higher  concentrations  there  can 
be  little  doubt  of  the  physical  effectiveness  of  the  hydrogen  ions  whatever 
their  size,  or  energy  relative  to  other  bodies.  The  energy  placed  on  the 
grid  of  an  electron  tube  may  be  small,  but  the  potential  of  the  grid  may 
determine  a  large  flow  of  energy  between  filament  and  plate.  The  hydro- 
gen ions  in  a  solution  may  be  small  in  relative  size  or  relative  numbers,  but 
they  may  control  the  mobilization  of  a  large  reserve. 

These  remarks  need  not  be  left  in  the  above  form.  They  may  be  stated 
mathematically. 

To  emphasize  one  important  aspect  we  shall  deal  first  with  acids  any 
one  of  which  is  so  "weak"  that  the  hydrions  which  it  liberates,  when 
the  salt  is  present  in  solution,  are  too  few  for  their  concentration  to  ap- 
proach the  order  of  magnitude  of  the  concentration  of  either  the  acid  or 
of  the  salt  of  that  acid.  Indeed  we  shall  assume  that  the  hydrion  con- 


XXVII  ALTERNATE  FORMULATION  521 

centration  is  so  low  in  comparison  with  that  of  any  of  the  chief  components 
of  the  solution  that  it  may  be  entirely  neglected  in  approximate  equations. 
We  shall  then  proceed  to  develop  the  ordinary  equilibrium  equations,  and 
shall  deal  later  with  the  hydrogen  electrode, — in  each  case  dispensing  with 
the  use  of  concentrations  of  free  hydrions. 

Experiment  makes  us  familiar  with  the  fact  that  a  weak  acid  may  be 
displaced  partially  or  completely  from  its  salt  by  certain  other  weak  acids. 
For  instance,  consider  the  reversible  reaction  between  sodium  phenolate 
and  acetic  acid.  Assuming  complete  dissociation  of  the  salts,  we  may  write 
the  reversible  reaction 

P-        +        HAc       ^±    HP     +     Ac- 
phenolate        acetic  acid       phenol        acetate 

and  the  equilibrium  equation 

-  K  (1) 

"   K 


[HP]  [Ac-]  ~ 

Evaluation  of  the  constant  KAB  of  equation  (1)  would  be  of  great  value 
in  calculating  both  the  direction  and  the  extent  of  the  interaction  be- 
tween the  system  acetate -acetic  acid  and  the  system  phenolate-phenol.  To 
make  the  matter  simple  assume  first  that  the  acetate-acetic  acid  system 

is  to  be  used  with  the  initial  ratio  *•  j  at  unity  and  in  such  relatively 
large  concentrations  that  the  addition  of  small  quantities  of  phenol  or 
phenolate  will  not  appreciably  change  the  ratio  *•  ^ .  Were  KAB  greater 

than  unity,  it  would  signify  that  the  acetate-acetic  acid  system  would 
convert  phenol  to  phenolate.  We  know  that  the  conversion  is  in  the 
opposite  direction.  KAB  is  less  than  unity,  indicating  the  tendency  for 
the  conversion  of  phenolate  to  phenol.  Furthermore,  KAB  is  much  less 
than  unity,  indicating  the  tendency  toward  extensive  conversion.  Now 

consider  the  converse  case  in  which  the  phenolate-phenol  system  is  pre- 

rp-i 
dominant  and  the  ratio         J    is  unity.    The  fact  that  KAB  is  not  only 

[HP] 

less  than  unity  but  much  less,  indicates  that  the  phenolate-phenol  sys- 
tem will  convert  the  acetate-acetic  acid  system  extensively  in  the  direc- 
tion of  acetate  and  not  in  the  direction  of  acetic  acid. 

In  general  the  extent  of  conversion  at  the  attainment  of  an  equilibrium 
state  may  be  calculated  as  follows.  Introduce  the  initial  values  in  place 
of  [HAc],  [Ac-],  [HP]  and  [P~].  Use  the  value*  1(T«-4  for  KAB  and  solve 
the  following  equation  for  x,  the  change  between  initial  and  final  con- 
centration. 

([P-]  -  x)  ([HAc]  -  x) 

([HP]  +  x)  ([Ac-]  +  x)  W 

2  Approximate  value. 


522         THE  DETERMINATION  OF  HYDROGEN  IONS 

In  the  special  case  where,  initially,  [P~]  =  [HAc]  =  [HP]  =  [Ac~],  equation 
(2)  reduces  practically  to  x  =  [P~]  =  [HAc].  Whence  the  conversion  to 
phenol  and  acetate  is  practically  complete. 

Obviously  it  would  be  a  great  advantage  to  have  a  constant  comparable 
with  KAB  for  each  system  composed  of  one  weak  acid  and  its  salt  in  ad- 
mixture with  another  weak  acid  and  its  salt.  Of  course  we  have  data  for 
these;  but  derived  in  a  way  different  from  that  to  be  discussed.  A  system- 
atic study  of  this  problem  could  have  been  made  as  follows. 

Let  us  choose  as  a  standard  of  reference  any  system  of  a  weak  acid  and 
its  salt.  To  be  specific  let  us  choose  as  the  standard  a  solution  made  with 
0.1  mole  acetic  acid  and  0.1  mole  sodium  acetate  per  liter  of  solution. 

Add  to  this  standard  solution  so  small  a  quantity  of  brom  cresol  green 
that  it  may  be  assumed  not  to  change  appreciably  the  ratio  of  acetic  acid 
to  acetate.  Experiment  shows  that  this  indicator  is  partially  transformed 
by  the  mixture;  while  in  a  solution  of  sodium  acetate  it  is  "blue"  and  in 
a  solution  of  acetic  acid  it  is  "yellow."  Assume  that  the  "yellow"  is 
proportional  to  the  concentration  of  the  acid,  HI,  and  the  "blue"  is  pro- 
portional to  the  concentration  of  the  anion,  I~.  Write  the  equilibrium 
equation 

IHAc]  H-] 

KAI 


It  will  be  convenient  to  rewrite  (3)  in  the  following  logarithmic  form: 


When  we  have  the  selected  standard  condition,  namely  - 

[HAc] 

III 
[HI] 


log  KAI  =  log  r^  (5) 


Now  the  ratio  }~-.  can  be  determined  colorimetrically  by  the  Gillespie 
[HI] 

method  (See  Chapter  VI).     This  experimental  datum  being  determined, 
KAI  is  made  known. 

[Ac~] 

Next  proceed  to  vary  the  ratio  and  in  each  instance  to  determine 

[HAcJ 

colorimetrically  the  ratio  ~^- .    With  the  aid  of  (4)  chart  the  results  as 
[HI] 

[Ac~] 

shown  in  figure  91.    There  the  ordinates  are  log  rLTT  .    .  and  the  abscissas 

[HAc] 

are  percentage  salt  formation — in  this  first  instance  that  of  brom  cresol 
green. 

Next  proceed  with  brom  cresol  purple  in  the  acetic  acid-acetate  mix- 
tures. In  this  instance  we  encounter  some  experimental  difficulty  be- 
cause it  is  impossible  to  produce  a  high  percentage  of  salt  formation  with 


XXVII 


ALTERNATE  FORMULATION 


523 


brom  cresol  purple  without  using  such  high  values  of  the  ratio 


that 


[HAc] 

exact  knowledge  of  the  values  of  this  ratio  are  subject  to  considerable 
uncertainty  because  of  experimental  errors.  Nevertheless  a  considerable 
portion  of  the  complete  data  may  be  obtained  experimentally  and  written 
into  the  equation 


log 


[Ac~] 
[HAc] 


log 


K 


+  log 


AI' 


[r-1 

[HI'] 


(6) 


-3 

-4 


B.CG. 


PHENOL 


25 


\ 


50        75 100 


PERCENT  NEUTRALIZATION 


I 
OL 


FIG.  91.  APPROXIMATE  DESCRIPTION  OF  ACID-BASE  EQUILIBRIA  BY 
REFERENCE  TO  0.1  M  ACETIC  ACID  +  0.1  M  SODIUM  ACETATE  AS 

STANDARD  OF  REFERENCE 
Subsequent  alignment  with  usual  pH  scale 


Here  HI'  and  I~~'  refer  to  brom  cresol  purple  and  its  anion  respectively, 
and  KAI'  is  the  equilibrium  constant  for  the  reaction 

HAc  +  I7"  5=±  HF  +  Ac~ 

The  results  are  charted  in  figure  91. 

Although  there  was  difficulty  in  using  the  acetic  acid-acetate  mixtures 
to  produce  a  wide  range  of  transformation  in  brom  cresol  purple,  it  is  found 


524  THE   DETERMINATION    OF   HYDEOGEN   IONS 

experimentally  that  no  such  difficulty  arises  when  mixtures  of  KH2PO4  and 
Na2HPO4  are  used.    We  shall  then  have  the  equilibrium  equation 


[I'-l 
log  L—         T  =  log  KPT,  +  log  l—  (7) 


Combine  equations  (6)  and  (7) 


When  kP°^  =  1,  we  have: 


log  7777-;  =  loS  77—  +  log  77—  =  log  77-  0) 

lllAcJ  -^AI'  ^PI'  ^AP 

In  (9)  the  constant  KAP  has  been  substituted  for  the  product  KAI'  Kpi'. 
The  significance  is  made  clear  in  figure  91. 

It  is  unnecessary  to  proceed  further  with  the  detail  of  such  a  develop- 
ment. What  has  been  given  briefly  is  sufficient.  By  selecting  some 
solution  of  a  weak  acid  and  its  salt  as  a  standard  of  reference,  and  by 
comparing  other  systems  of  weak  acids  and  their  salts  with  this  standard 
(either  directly  or  indirectly)  it  is  possible  to  systematize  equilibria  in 
terms  of  the  standard  of  reference. 

We  find  in  figure  91  that  the  system  phenol-phenolate  is  charted  with 

ordinate  log  *         •     There  should  be  no  difficulty  in  appreciating  how, 

[Jri  A.CJ 

by  the  use  of  intermediate  systems,  the  placement  of  this  system  could 
be  found  and  there  should  be  no  doubt  of  the  real  value  of  such  data. 

Yet  someone  might  note  the  very  large  value  of  log  •'          when  phenol  is 

90  per  cent  neutralized  and  might  object  that  such  a  value  can  have  no 
physical  significance.  Such  an  objection  would  be  quite  comparable  with 
one  objection  to  the  use  of  large  values  of  pH.  But,  should  the  occasion 
arise,  the  objector  would  not  hesitate  to  use  the  equilibrium  constants 
indicated  in  figure  91  to  calculate  the  extent  of  a  change  in  a  given  phenol- 
phenolate  system  produced  by  the  addition  of  a  given  mixture  of  primary 
and  secondary  phosphates. 

However,  the  objection  to  employing  these  "calculation  values,"  ex- 
pressed in  terms  of  a  particular  system,  can  be  removed.  Our  present 
interest  is  only  in  the  relation  of  one  system  of  a  weak  acid  and  its  salt  to 
another  system  of  a  weak  acid  and  its  salt.  The  relative  position  of  each  of 
the  systems  shown  in  the  figure  (or  of  any  other  system  we  may  wish  to 
include)  is  our  only  concern.  This  relative  position  will  not  be  changed 
if  we  preserve  the  same  numerical  scale  for  the  ordinate  but  change  the 


XXVII  ALTERNATE  FORMULATION  525 

origin.  One  might  add  the  constant  777  and  call  the  ordinate  the  axis  of 
pQ.  A  distance  between  the  centre  points  of  any  two  curves  would  remain 
the  same  and  would  be  the  negative  logarithm  of  the  equilibrium  constant 
for  the  reaction  between  the  two  systems  described  by  those  curves. 

By  considering  the  brom  cresol  green  system  to  be  the  temporary 
working  standard  we  would  be  able  to  work  out  the  curve  for  the  acetic 
acid-acetate  system.  To  avoid  confusion  this  has  not  been  included  in 

the  figure,  the  ordinate  of  which  is  log  f-       *• 

[rlAcj 

If,  for  purposes  of  illustration,  we  continue  to  use  approximate  equa- 
tions, we  can  easily  introduce  into  this  scheme  of  presentation  the  case 
of  any  acid  which  directly  furnishes  appreciable  concentrations  of  hydrogen 
ions. 

Consider  the  equilibrium  between  hydrochloric  acid  and  the  acetate- 
acetic  acid  system. 

The  equilibrium  for  the  reaction 

Na+  +  Ac-  +  H+  +  Cl-  ^  Na+  +  01  -  +  HAc 

is  expressed  by 

[Ac-]  [H+] 


[HAc] 
or 


iog-o          ao) 

[Ac"] 

When  we  choose  the  standard  state,  namely  r  -  -  =  1,  we  find 

[HAc] 

los  it  (11) 

We  need  not  pause  to  outline  direct,  or  intermediate,  means  whereby 
equation  (10)  can  be  experimentally  studied,  or  how  the  value  4.63  for 
—log  KAC  is  reached.  Assuming  that  this  relation  is  determined,  apply 
(10)  to  the  case  of  0.1  N  hydrochloric  acid  during  titration  with  sodium 
hydroxide.  Assume  that  at  each  stage  of  this  titration  the  concentration 
of  residual  hydrochloric  acid  equals  [H+].  The  "titration  curve"  is 
plotted  in  figure  91  with  the  aid  of  (10).  For  example,  at  half-neutraliza- 
tion [H+]  =  0.05  or 


With  any  given  value  of  [H+]  established,  it  is  now  possible  to  recon- 
struct the  scale  of  the  ordinate  in  terms  of  pH.  See  this  scale  at  the 
right  of  figure  91. 


526  THE    DETERMINATION   OF   HYDROGEN   IONS 

The  development  given  above  is  so  obvious  in  its  outline  that  perhaps 
some  of  the  detail  was  unnecessary.  From  the  main  theme  we  may  draw 
these  conclusions.  No  physical  effectiveness  of  extremely  small  hydrion 
concentrations  need  be  sought  and  no  particular  virtue  need  be  attached 
to  a  standard  of  reference  so  long  as  we  are  concerned  only  with  the  ap- 
proximate equations  expressing  equilibria  in  mixtures  of  weak  acids  and 
their  salts. 

When  exact  formulation  is  undertaken  there  apply  to  the  equations 
given  above  the  same  type  of  correction  for  departure  from  the  laws  of  the 
ideal  gas  that  have  been  discussed  in  previous  chapters;  but  in  some  in- 
stances different  standards  of  reference  would  be  used. 

There  remains  a  matter  of  some  physical  significance.  The  scheme  out- 
lined in  this  chapter  implies  that  ionization  of  a  weak  acid  is  not  a  neces- 
sary preliminary  to  reaction  but  that  a  reaction  can  proceed  in  the  sense: — 

HA  +  R-  ^  HR  +  A- 

i.e.,  by  direct  transfer  of  a  hydrion  from  the  molecule  of  one  species  to  the 
anion  of  another  species.  There  is  no  reason  to  suppose  that  this  is  the 
exclusive  process  any  more  than  there  is  reason  to  believe  that  preliminary 
ionization  is  necessary.  There  is  reason  to  believe  free  hydrions  to  be 
present  in  solutions  of  acids  as  "weak"  as  acetic.  Historically  such  cases 
became  prototypes  the  conduct  of  which  has  been  extrapolated  to  cases 
in  which  there  is  no  direct  evidence  of  free  hydrions.  So  far  as  the  author 
knows  there  is  no  way  to  call  forth  the  characteristic  "acid"  properties 
of  extremely  weak  acids  except  to  attack  them  with  bases.  Then  the 
formulation  can  legitimately  follow  that  outlined,  not  necessarily  in  ex- 
perimental procedure,  but  rather  in  the  interpretation  which  does  away 
with  the  necessity  of  thinking  in  terms  of  hydrion  concentrations. 

However  the  customary  formulation  with  the  use  of  pH  values  is  by 
far  the  more  convenient. 

Now  consider  the  hydrogen  electrode,  which  is  usually  regarded  as  a 
means  of  measuring  the  activities  of  free  hydrions. 

As  usual,  assume  that  at  the  electrode  hydrogen  ionizes  to  protons  and 
electrons.  In  a  solution  of  a  strong  acid  containing  only  the  ions  of  the 
acid  and  no  undissociated  acid  molecules,  we  very  naturally  assume  that 
the  equilibrium  potential  is  determined  by  the  distribution  of  hydrions 
between  solution  and  electrode.  The  assumed  scheme  is  successfully 
extrapolated  to  apply  to  the  conduct  of  an  electrode  in  a  solution  contain- 
ing a  weak  acid  and  its  salt,  the  calculated  hydrion  activity  being  in 
some  cases  as  low  as  10~n,  or  less. 

We  may  equally  well  assume  that  the  electrons  arising  from  the  ioniza- 
tion of  the  hydrogen  attack  the  peripheral  protons  of  the  weak  acid  directly. 
Idealizing  the  reaction  as 

2HA  +  2e  ^  H2  +  2  A-, 


XXVII  ALTERNATE  FORMULATION  527 

and  proceeding  to  the  formulation  of  the  potential  at  a  single  electrode  by 
the  method  of  Chapter  XVIII  we  have  equation  (12) 


In  (12)  P  is  the  pressure  of  hydrogen  in  atmospheres.  Hereafter  we  shall 
maintain  this  pressure  at  one  atmosphere  and  so  eliminate  P  from  the 
equations. 

If  one  hydrogen  electrode  is  immersed  in  a  solution  of  acetic  acid  and 
sodium  acetate  and  another  hydrogen  electrode  is  immersed  in  a  solution 
of  primary  and  secondary  alkali  phosphates,  if  the  solutions  are  joined  and 
liquid  junction  potential  is  supposed  to  be  eliminated,  we  have: 


RT       (HAc)  (HP04 
F      '    (Ac-)  (H2P07) 


E.M.F.  =  EA  -  Ep  +  —  In    „._:  V/TT_V  (13) 


Now  choose  the  solution  which  is  0.1  M  with  respect  to  acetic  acid  and 
0.1  M  with  respect  to  sodium  acetate  as  a  standard  of  reference.  Also 
assign  to  EA  (which  is  the  single  potential  for  the  equimolecular  mixture) 
the  arbitrary  value  0.  Also  when  the  potential  of  the  cell  under  considera- 
tion, or  any  other  cell,  is  referred  to  this  standard  let  the  reference  be 
shown  by  the  subscript  "a"  in  Ea,  the  electromotive  force  of  the  cell. 

Then  equation  (13)  becomes: 


When  =  '•  we  have 


Without  being  shown  the  detail,  the  reader  will  at  once  perceive  that 
by  constructing  cells  one  half  of  which  contains  the  standard  acetate  solu- 
tion and  the  other  half  of  which  contains  in  succession  mixtures  of  weak 
acids  and  their  respective  salts  we  can  construct  a  systematic  chart  of 
equilibrium  relations  comparable  with  figure  91. 

It  is  also  evident  that  any  standard  of  reference  can  be  chosen,  for  in- 
stance the  calomel  half-cell.  Such  changes  of  reference  are  similar  to  the 
addition  of  a  constant  quantity  to  each  value  on  the  ordinate  of  figure  91 
discussed  previously. 

But  of  more  importance  is  it  to  note  that  we  need  not  specify  the  elec- 
trode process.  We  may  simply  specify  that  we  are  dealing  with  some 
process  by  which  the  weak  acid  is  converted  to  its  anion.  Consider  any 
half-cell  as  the  standard  of  potential  reference.  The  process  at  this  half- 


528  THE    DETEEMINATION   OF   HYDROGEN    IONS 

cell  need  not  be  known.  Use  the  subscript  "a"  to  show  reference  to  this 
standard.  It  was  suggested  above  that  the  reference  can  have  any  value. 
We  shall  then  still  have  the  relation 

E8  F  =  E  F  -  RT  In  -  (15) 


This  formulates  the  free  energy  change  in  the  transformation  of  a  mole 
of  an  acid  to  a  mole  of  the  corresponding  anion  by  some  process,  standard, 
but  of  unknown  nature.  Evaluations  have  a  most  obvious  use  for  they 
enable  one  to  calculate  the  direction  and  extent  of  the  conversion  of  one 
acid  into  its  salt  by  another  system  of  an  acid  and  its  salt. 

We  have  already  stated  that  a  hydrogen  electrode  in  a  solution  of  hydro- 
chloric acid  can  be  considered  most  reasonably  as  functioning  in  response 
to  free  hydrions.  If  such  a  solution  of  hydrion  activity  of  unity  is  made 
the  standard  of  reference  and  if  the  process  at  the  other  electrode  is  con- 
sidered to  be 

2HA  +  2€  ^  H2  +  2A- 

we  can  formulate  the  potential  of  the  cell,  as  mentioned  previously,  by  the 
method  of  Chapter  XVIII  and  so  obtain  (when  the  hydrogen  pressure 
on  both  sides  is  unity): 


or  in  numerical  form  for  25°C. 

Eh          E 


. 

'  los 


It  will  now  be  remembered  that  a  value  of  pH  as  actually  determined  is 

E  E 

none  other  than  —    ~*V  .  The  constant  —       "would,  by  any  other  name  be 
0.059  0.059 

a  constant  still.     Call  it  pK.    Then  equation  (17)  may  be  written  as  (18) 
pH  =  PK  +  log  -  (18) 


This  is,  of  course,  the  familiar  Henderson-Hasselbalch  equation  in 
terms  of  activity.  It  was  derived  by  using  the  customary  standard  of 
reference  which  implies  the  participation  of  free  hydrions  in  that  half 
of  the  cell  which  is  the  standard  half-cell;  but  it  is  now  implied  that  in 
that  half-cell  which  is  of  particular  interest  no  appreciable  quantities  of 
free  hydrions  need  be  present. 

The  above  outline  should  not  be  interpreted  as  meaning  that  no  hydrions 
are  present  in  solutions  buffered  by  very  weak  acids  and  their  salts.  In- 


XXVII  ALTERNATE  FORMULATION  529 

deed  the  complete  equations  would  take  into  consideration  both  hydrions 
and  hydroxyl  ions.  These  components  would  then  be  of  particular  im- 
portance in  very  acid  or  very  alkaline  solutions,  of  relatively  negligible 
importance  in  "neutral"  solutions  and  in  the  intermediate  zones  they 
would  rise  or  fall  in  their  importance  according  to  the  concentrations  and 
states  of  equilibria  of  the  components  of  a  solution.  Here  we  are  probably 
dealing  with  a  class  of  cases  in  which  the  physical  effectiveness  of  one  or 
another  species  dwindles  gradually  as  conditions  change  and  while  the 
dwindling  occurs  other  species  take  up  and  maintain  the  continuity  of 
effects. 

The  above  outline  has  no  advantage  over  the  usual  presentation.  In- 
deed it  is  clumsy  because  no  advantage  has  been  taken  of  the  common 
component  of  acid-base  equilibria,  namely  the  hydrion.  Use  of  the  hydrion 
concentration  or  activity  makes  the  ordinary  presentation  direct  and 
elegant.  The  purpose  of  the  alternate  presentation  is  to  convince  the 
elementary  student  that  the  extremely  small  "calculation"  values  he  is 
asked  to  use  are  truly  indices  of  positions  of  equilibria  among  relatively 
large  quantities  of  material.  It  then  appears  that  he  is  dealing  with  a 
problem  in  the  organization  of  his  experimental  facts.  Furthermore  the 
alternate  method,  in  spite  of  its  formality,  may  help  to  dispel  illusions 
which  some  writers  have  introduced  into  a  comparatively  simple  set  of 
formulations.  For  instance  Dixon  (1927)  uses,  as  the  keynote  of  an  argu- 
ment on  mechanism,  the  assumption  that  the  hydrogen  electrode  actually 
functions  in  the  way  ordinarily  described.  He  does  not  tell  his  reader 
that  the  ordinary  description,  although  an  invaluable  convenience,  is  not 
necessary  even  to  the  formulation  of  acid-base  equilibria. 

One  suggestion  of  possible  value  comes  from  the  use  of  the  alternate 
formulation.  Suppose  an  event  involving  kinetics  is  apparently  under  the 
control  of  the  hydrion  concentration  as  ordinarily  described.  If  the  ap- 
parent critical  range  is  say  5-6  on  the  pH  scale,  may  it  not  obscure  insight 
to  say  that  the  event  "is  controlled  by  the  hydrogen  ion  concentration?" 


CHAPTER  XXVIII 

ELEMENTARY  THEORY  OF  TITRA.TION 

In  figure  92  are  shown  titration  curves  of  hydrochloric  acid  at 
two  concentrations  and  titration  curves  of  acetic  and  boric  acids. 
In  each  case  the  curve  has  been  extended  to  reveal  its  course  when 
excess  alkali  is  added.  The  abscissa  of  the  figure  is  made  per- 
centage neutralization  for  a  purpose  which  will  appear  presently. 
In  the  construction  of  the  curves  volume  changes  are  neglected 
for  purposes  of  simplicity. 

Neglect  for  the  moment  the  curve  for  the  more  dilute  solution 
of  hydrochloric  acid.  Consider  the  nature  of  the  end-points  in 
the  other  three  cases. 

When  all  but  a  very  small  part  of  the  hydrochloric  acid  has  been 
neutralized  there  comes  an  approach  to  what  appears,  in  prac- 
ticable operations,  to  be  a  sharp  "break"  in  the  titration  curve. 
On  the  addition  of  the  last  trace  of  base  required  for  complete 
neutralization  the  pH  value  of  the  solution  plunges  to  the  alkaline 
region.  Much  the  same  sort  of  phenomenon  occurs  in  the  titra- 
tion of  acetic  acid;  but  it  is  important  to  note  that  the  range  of  pH 
values,  compatible  with  a  negligible  error  in  the  estimation  of  the 
true  end-point,  is  now  much  narrower.  As  shown  by  the  figure 
no  significant  error  would  be  made  were  the  hydrochloric  acid 
solution  which  is  under  consideration  to  be  titrated  to  pH  =  6.0; 
while  a  very  considerable  error  would  be  made  were  the  acetic 
acid  solution  to  be  titrated  to  this  value.  In  the  case  of  boric 
acid  there  is  no  precipitous  change  of  pH  at  the  end-point.  Con- 
sequently a  high,  and  almost  impracticable,  accuracy  would  be 
required  in  titrating  to  an  exactly  determined  pH  value. 

In  the  titration  of  the  more  dilute  solution  of  hydrochloric  acid 
the  latitude  allowable  has  constricted  and  again  a  very  high 
accuracy  in  the  attainment  of  an  end-point  pH-value  is  required. 

Theoretically  any  method  which  reveals  the  pH  value  of  the 
correct  end-point  and  which  does  not  seriously  interfere  with  the 
equilibria  involved  can  be  adapted  to  the  purposes  of  titration. 

530 


XXVIII 


THEORY    OF   TITRATION 


531 


However  the  hydrogen  electrode  and  indicator  methods  are  most 
widely  used.  Of  these  the  indicator  method  is  best  adapted  to 
the  ordinary  work  of  the  analytical  laboratory. 

It  is  obvious  that,  having  selected  the  stoichiometric  per- 
centage neutralization  as  the  abscissa  of  figure  92,  we  may  place  in 
this  figure  the  independent  titration  curve  for  a  very  dilute  solu- 
tion of  an  indicator  just  as  we  placed  in  the  same  figure  the 


14 


53fe^ 


20      40/     6.0      60 
Bsrcent.  Neutralization 


100     120     140      160      180     200 

FIG.  92.  TITRATION  CURVES 


titration  curve  for  a  very  dilute  solution  of  hydrochloric  acid. 
Moreover  such  a  curve  for  the  high  dilutions  usually  employed  is 
practically  the  same  as  the  curve  relating  the  percentage  apparent 
dissociation  (and  consequently  percentage  color  transformation) 
to  pH.  Furthermore  no  large  error  is  made  if  it  be  assumed  that 
the  indicator  when  present  in  a  solution  of  the  acid  being  titrated 
does  not  displace  the  titration  curve  of  that  acid.  Then  the 


532  THE    DETERMINATION    OF    HYDROGEN    IONS 

buffer  system  (titrated  acid  +  salt  of  the  acid),  by  determining 
the  value  of  pH,  determines  the  degree  of  color  developed  in  the 
indicator.  (See  Chapters  I  and  V). 

As  shown  by  figure  92,  either  brorn  cresol  green  or  phenol- 
phthalein  could  be  used  as  end-point  indicator  in  the  titration  of 
tenth  normal  hydrochloric  acid,  because  at,  or  extremely  close 
to,  the  completion  of  neutralization  the  value  of  pH  sweeps  through 
the  whole  range  of  brom  cresol  green  and  well  into  the  range  of 
phenolphthalein.  On  the  other  hand  the  dissociation  constant 
of  acetic  acid  is  so  low  that  the  flat  portion  of  the  curve  for  acetic 
acid  lies  in  the  region  of  partial  color-transformation  of  brom 
cresol  green  and  only  gradual  color  transformation  is  observed 
with  no  satisfactory  large  change  at  the  end-point.  The  use  of 
phenolphthalein  is  indicated  in  this  case. 

As  already  noted  the  requirement  in  the  case  of  boric  acid  is 
so  strict  that  boric  acid  is  considered  to  be  an  untitratable  acid 
until  by  a  curious  combination  with  glycerine  it  is  made  a  stronger 
acid.  It  is  not  so  generally  realized  that  at  high  dilutions  a 
similar  restriction  is  placed  on  the  titration  of  an  acid  even  so 
strong  as  hydrochloric. 

The  principles  thus  briefly  outlined  •  apply  to  the  titration  of 
bases  with  strong  acids,  but,  of  course,  with  the  direction  of  pH 
change  reversed  and  with  the  end-points  tending  to  lie  on  the 
acid  side  of  pH  7.0.  A  hydrogen  ion  concentration  of  10~7  N  or 
pH  7.0  is  called  the  neutral  point  because  it  is  the  concentration 
of  both  the  hydrogen  and  the  hydroxyl  ions  in  pure  water;  but 
evidently  it  is  seldom  the  practical  or  the  theoretical  point  of 
neutrality  for  titrations. 

The  problem  of  titration  with  weak  acids  or  bases  as  reagents 
is  complicated  and  by  reason  of  the  ever  shifting  end-points  re- 
quired in  passing  from  case  to  case  and  the  very  narrow  limits, 
the  practice  is  to  be  avoided. 

With  this  brief  outline  in  mind  the  reader  will  do  well  to  .study 
the  classic  paper  of  A.  A.  Noyes,  Quantitative  Application  of  the 
Theory  of  Indicators  to  Volumetric  Analysis  (J.  Am.  Chem.  Soc. 
32,  p.  815,  1910)  and  the  monograph  by  Niels  Bjerrum,  Die 
Theorie  der  alkalimetrischen  und  azidimetrischen  Titrierungen 
(Sammlung  chem.  chem.-tech.  Vortrdge,  31,  p.  1,  1914).  Much 
less  elegant  than  the  treatments  there  found,  but  more  condensed, 
is  the  following. 


XXVIII  THEORY   OF  TITRATION  533 

In  Chapter  I  there  was  developed  an  equation  relating  all  the 
components  of  a  solution  containing  a  univalent  acid  and  a  uni- 
valent  strong  base.  That  equation  is 


[Sa]  -  [B+]  -  [H+]  +  £ 


This  was  derived  by  means  of  the  classic  equations  which  do 
not  hold  accurately.  Tentatively  we  shall  neglect  this  aspect 
and  shall  return  to  it  later. 

It  will  be  in  accord  with  modern  tendencies  to  consider  [s], 
the  concentration  of  undissociated  'salt,  negligible  under  most 
but  not  all  circumstances. 

Consider  first  the  situation  obtaining  under  ideal  conditions 
when  at  the  true  end-point  of  a  titration  exactly  equivalent 
amounts  of  acid  [Sa]  and  total  base  (equal  to  [B+])  are  present. 
Then  the  equation  reduces  to 

[H+P  +  [Sa]  [H+]2  -  Kw  [H+]  _ 


Kw  -  [H+p 

Although  it  is  impracticable  to  solve  this  equation  for  [H+], 
it  is  practicable  to  proceed  by  either  of  two  methods.  In  the 
first,  there  are  introduced  assumed  values  of  [Sa]  and  [H+]  and 
the  equation  is  solved  for  Ka.  With  a  sufficient  number  of  such 
numerical  solutions  of  the  equation  there  can  be  drawn  up  a 
table  (or  chart)  showing  the  ideal  values  of  [H+]  (or  pH)  for 
various  values  of  [Sa]  and  Ka.  By  the  second  procedure  use  is 
made  of  the  fact  that  in  numerical  solutions  of  the  equation  with 
values  ordinarily  encountered  the  terms  [H+]3  and  Kw  [H+] 
usually  can  be  neglected  without  serious  error.  As  a  consequence 
there  may  be  used  within  proper  limitations  the  expression; 

pH  (of  ideal  end-point)  =  J  [log  ([SJ  +  K.)  -  log  KaKw] 

Either  procedure  leads  to  data  for  figure  93. 

Figure  93  may  be  used  in  the  following  manner.  Given  the 
value  of  Ka  of  the  acid  to  be  titrated,  note  the  corresponding 
diagonal  in  the  figure  and  follow  it  to  its  intersection  with  the 


534  THE    DETERMINATION    OF   HYDROGEN   IONS 

line  indicating  the  concentration  of  the  salt  at  the  final  volume. 
Then  read  upon  the  abscissa  the  ideal  value  of  pH  for  the  end- 
point. 

In  the  figure  the  diagonals  have  been  continued  only  to  the 
heavy,  interrupted  line  signifying  the  limit  for  0.1  per  cent  error 
of  excess  base.  The  position  of  this  line  is  roughly  determined 
as  follows. 

Suppose  a  solution  normal  with  respect  to  the  final  concentra- 
tion of  the  salt  formed  is  over-titrated  so  that  there  is  present 
0.1  per  cent  excess  base.  Assume  that  this  excess  base  produces  a 
solution  of  the  same  pH  value  as  that  of  a  pure  water  solution 
containing  this  same  amount  of  completely  dissociated  base  alone. 
Obviously  the  solution  then  will  be  1  X  10 ~3  normal  with  respect 
to  hydroxyl  ions  or,  if  pKw  =  14,  the  pH  value  will  be  11.0. 
Repeat  this  calculation  with  other  cases.  There  is  thus  deter- 
mined the  position  of  the  line  in  question. 

For  instance,  assume  that  there  is  to  be  titrated  a  solution  of 
an  acid  with  Ka  value  1  X  10 ~4  and  that  the  concentration  of 
the  salt  at  the  end- volume  is  to  be  0.1  normal.  The  ideal  value 
of  pH  at  the  end-point  is  shown  by  the  chart  to  be  8.5  but  if  an 
error  of  0.1  per  cent  excess  base  is  to  be  allowed  the  pH  value 
can  be  10.  Likewise  for  a  final  solution  of  0.01  normal  salt  an 
acid  of  Ka  =  1  X  10~5  should  be  titrated  ideally  to  pH  =  8.5 
with  a  limit  at  pH  =  9.0. 

The  figure  does  not  show  directly  the  limiting  values  of  pELfor 
errors  due  to  insufficient  base.  However,  as  suggested  by  figure  92 
the  full  curve  is  so  nearly  symmetrical  with  respect  to  the  end- 
point  that  the  "acid  limit"  is  about  as  far  displaced  in  one  direc- 
tion from  the  true  end-point  as  the  excess  base  limit  is  displaced 
in  the  other  direction. 

For  example  if  Ka  =  10~4  and  [S]  =  0.01  N  the  ideal  end- 
point  is  pH  =  8.0  and  the  limits  for  0.1  per  cent  error  excess  base 
or  insufficient  base  are  respectively  pH  =  9.0  and  pH  =  7.0. 

The  error  of  the  approximate  treatment  increases  with  the 
dilution  of  the  solution  and  the  pKa  value  of  the  acid  being  ti- 
trated. It  becomes  obvious  in  the  extreme  cases  where  the  op- 
timal end-point  is  shown  as  identical  with  the  limit  for  0.1  per 
cent  error.  However,  the  chart  can  still  be  interpreted  to  mean 
that  in  these  extreme  cases  an  impracticable  accuracy  would  be 
required,  for  instance  with  0.01  N  and  Ka  =  10~6  or  with  O.I  N 
and  Ka  =  10~7. 


^ 

1.0  Nj  1 

V 

t 

^ 

V* 

V' 

t 

4 

j» 

^ 

4 

? 

V 

t 

E: 

/ 

-r- 

/ 

/: 

/ 

J— 

/ 

T*  — 

/ 

/ 

/ 

/ 

/ 

/ 

2 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

2 

/ 

/ 

/ 

/ 
/ 

/ 

1  / 

/ 

/ 

7 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

/ 

f' 

o.owM 

/ 

/ 

// 

1  / 

\l 

/  : 

\  —  A 

at 
.an 
(d 
(o 

Chart  tor  Selecting 

Ideal  value  of  pHkbcissa) 
e-rvd-poiivt  irv  the  titration  of 



•  / 

1 

/ 

1  / 

/ 

/ 

/ 

^x 

— 

/ 

/ 

/ 

/ 

• 

/ 

/ 

/x 

,  acid  of  given  Ka-value 
agon-al)  when  normality 
rdinate)  of  resulting  salt 
tlv  strorvg  base  is  given. 
zLimit  for  0.1%  excess  foas 

1  / 

/ 

/ 

Wl 

e. 

1  / 

/ 

,r 

— 

/ 

/, 

' 

nnnnsjL-l 

' 

PH 


10 


11 


FIG.  93 


O.OlN  


Chart  for   Selecting 

Ideal  value  of 
at  end- point  in  the  titration  of  a 
base  of  given Kf  value  (diagonal) 
wXen normality  (ordinate)  of 
resulting  salt  with  strong 
acid  is  give-TV. 

—  'Limit  of  0.1V.  excess  acid. 


0.001N  = 


0.0001N 


PH 


536  THE    DETERMINATION   OF   HYDROGEN   IONS 

In  an  analogous  manner  there  can  be  developed  the  chart  show- 
ing the  ideal  end-points  for  the  titration  of  bases  of  various  values 
of  Kb,  and  showing  the  limits  for  0.1  per  cent  excess  acid.  This 
chart  is  shown  in  figure  94. 

In  the  titration  of  multi-acidic  acids  it  usually  occurs  that  the 
first  and  secohd  dissociatiofo.  constants  are  sufficiently  different 
in  magnitude  to  make  the  end-point  at  the  completion  of  the 
last  stage  of  the  titration  that  which  it  would  be  were  there  being 
titrated  a  univalent  acid  having  the  dissociation  constant  of  the 
last  step  in  the  titration  of  the  multivalent  acid-  Consequently 
the  principles  already  developed  can  be  extended  and  extended 
not  only  to  the  complete  titration  of  multivalent  acids  but  also 
to  the  titration  of  multivalent  bases.  However,  it  is  well  to  bear 
in  mind  an  item  often  overlooked.  In  searching  tables  of  disso- 
ciation constants  one  will  frequently  find  that  the  constants  for 
the  distinctively  strong  groups  of  a  given  acid  or  base  are  the 
only  constants  given.  It  may  be  that  nothing  is  said  about  the 
weaker  groups;  yet  it  may  well  be  that  one  or  another  of  these 
weak  groups  begin  to  function  at  the  higher  alkalinities  to  which 
it  is  often  necessary  to  titrate  the  stronger  groups. 

Since  the  error  in  the  titration  of  small  amounts  of  acid  or  base 
becomes  larger  the  higher  the  dilution,  Rehberg  (1925)  advises  the 
use  of  low  dilutions.  The  resulting  small  volume  will  then  throw 
the  error  upon  the  volumetric  apparatus  and  to  meet  this  Rehberg 
advocates  micro  volumetric  methods.  This  is  a  deduction  from 
the  theory  which  is  of  great  practical  importance. 

Modification  of  the  theory  must  be  introduced  if  account  is 
to  be  taken  of  the  effects  of  neutral  salts.  In  the  first  place 
the  presence  of  neutral  salts  will  shift  the  equilibria  in  such  a  way 
that  the  stoichiometric  end-point  is  at  a  value  of  [H+]  or  at  a 
value  of  the  hydrion  activity  somewhat  different  than  that  calcu- 
lated by  means  of  the  classic  equations.  In  the  second  place  the 
color  of  an  indicator  used  to  detect  a  given  end-point  will  be 
somewhat  different  than  that  calculated  by  means  of  the  classic 
equations  with  the  aid  of  constants  determined  for  one  environ- 
ment (e.g.,  standard  buffer  solutions).  However,  we  have  al- 
ready noted  the  considerable  latitude  usually  allowed  and  we 
have  seen  that  this  latitude  becomes  narrow  only  for  extremely 
weak  acids  and  bases  or  for  very  dilute  solutions.  Therefore,  if 


XXVIII  THEORY   OF   TITRATION  537 

the  tendency  of  the  operator  is  to  keep  his  end-points  near  the 
ideal  values  he  need  worry  little  about  the  effects  of  neutral 
salts  except  in  the  extreme  cases  or  for  the  very  highest  precision. 
When  he  does  meet  the  cases  requiring  exceptional  care  he  is  pre- 
sented with  a  situation  which  may  be  one  of  such  a  variable  class 
that  a  general  formulation  is  hardly  practicable.  Indeed  it 
would  not  be  permissible  to  use  dissociation  constants  determined 
for  only  one  set  of  conditions. 

There  is  one  set  of  cases  where  the  matter  becomes  of  some 
importance  to  common  practice.  Frequently  the  occasion  arises 
in  which  it  is  desired  to  titrate  a  multivalent  acid  to  some  inter- 
mediate salt,  for  instance  phosphoric  acid  to  NaH2P04.  It  could 
be  assumed  with  very  good  approximation  that  the  classical 
equations  apply.  Then  there  is  easily  calculated  the  desired  pH 
value  when  pKi  and  pK2  are  known.  But  for  high  accuracy  the 
complete  equations  are  necessary. 

With  this  very  brief  outline  of  the  main  features  we  may  turn 
again  to  the  selection  of  indicators.  In  a  more  elegant  presenta- 
tion of  the  theory  of  titration,  consideration  should  be  given  to 
such  matters  as  the  more  favorable  degree  of  transformation  of 
an  indicator  which  is  to  be  used  as  end-point  indicator.  However, 
it  seems  to  me  to  be  adequate  for  most  purposes  to  let  the  ideal 
and  limiting  end-points  graphically  exhibited  in  figures  93  and 
94  be  the  guides  and  in  specific  applications  to  select  the  proper 
indicator  either  by  the  aid  of  the  color  chart  (page  65),  or,  under 
more  exacting  conditions,  to  set  up  a  standard  color  to  which  to 
titrate  by  means  of  the  selected  indicator  and  standard  buffer 
solutions. 

From  the  general  form  of  a  titration  curve  it  is  evident  that 
the  difference  of  potential  between  similar  electrodes  in  solutions 
which  differ  always  by  a  fixed  amount  in  the  degree  of  neutraliza- 
tion varies  with  the  degree  of  neutralization  and  attains  a  maxi- 
mum at  the  end-point.  Cox  (1925)  put  this  principle  to  instru- 
mental use  in  the  following  way.  He  divided  the  solution  to  be 
titrated,  placed  one  aliquot  in  one  beaker  and  another  in  a  second 
beaker,  connected  the  two  solutions  with  a  wet  filter  paper  and 
proceeded  to  titrate  with  two  burettes  keeping  the  interval  of  the 
amounts  added  from  each  burette  0.2  cc.  At  the  end-point  the 
difference  of  potential  between  the  two  electrodes  reaches  a 


538 


THE  DETERMINATION  OF  HYDROGEN  IONS 


maximum.  Maclnnes  and  Jones  (1926,  1927)  simplified  the  pro- 
cedure by  an  ingenious  device  so  that  only  one  burette  is  necessary. 
They  shelter  one  electrode  of  figure  95.  It  will  not  immediately 
attain  the  potential  of  the  other  as  reagent  is  added.  At  the 
end-point  the  difference  of  potential  between  the  two  will  rise 


0.6  0.6  1.0 

RATIO:   BASC  /  ACID 

FIG.  95.  MAC!NNES  AND  JONES'  SHELTERED  ELECTRODE  FOR  TITRATION 

AND  TYPICAL  COURSE  OF  THE  CHANGE  OF  POTENTIAL  BETWEEN  THE 

SHELTERED  AND  UNSHELTERED  ELECTRODES  DURING  A  TITRATION 

to  a  sharp  maximum.  Maclnnes  analyzes  the  theoretical  error 
due  to  this  arrangement  and  concludes  that,  with  the  dimen- 
sions of  the  shelter  he  employs,  "the  method  is  capable  of  high 
accuracy  and  is  applicable  in  every  case  in  which  a  potentiometer 
technique  is  possible." 

For  discussion  of  potentiometric  methods  applied  to  titration 
in  general  see:  M  tiller  (1926),  Kolthoff  and  Furman  (1926), 
Popoff  (1927). 


CHAPTER  XXIX 
NON-AQUEOUS  SOLUTIONS 

Indeed  water  is  not  our  sole  reliance;  hundreds  of  solvents  stand  us  in 
good  stead  to  effect  electrolysis,  and  among  these  are  solvents  which 
bring  about  the  ionization  of  salts  as  extensively  as  water — or  even 
more  extensively. — FREE  TRANSLATION  OF  P.  WALDEN. 

The  main  principles  discussed  in  the  preceding  chapters  should 
apply  to  non-aqueous  solutions,  except  in  so  far  as  quantities 
peculiar  to  water,  for  example,  Kw,  and  numerical  values  applic- 
able to  water  solutions  are  concerned.  On  the  other  hand  we 
do  not  have  the  extensive  data  which  permit  so  comprehensive 
a  treatment  as  that  accorded  aqueous  solutions. 

From  one  point  of  view  each  solvent  is  worthy  of  a  separate 
treatment  comparable  with  that  accorded  water  solutions.  If 
so,  individual  standardization  of  activities  might  be  undertaken 
without  reference  to  intercomparisons.  As  one  of  several  exam- 
ples of  such  independent  studies  there  may  be  cited  Banner's 
(1922)  investigation  of  the  cell: 

Pt,  H2 1  HC1,  HgCl  |  Hg 

with  ethanol  as  solvent,  and  Scatchard's  (1925)  treatment  of 
this  and  other  studies. 

However,  when  we  pass  from  consideration  of  the  solvent, 
water,  which  has  attracted  most  attention,  to  a  consideration  of 
"miscellaneous"  solvents,  intercomparison  becomes  the  more 
interesting.  If  the  point  of  view  of  intercomparison  is  taken,  a 
most  important  caution  needs  statement  at  the  very  beginning. 
Let  us  put  it  in  the  following  manner. 

We  have  seen  that  the  greater  part  of  our  data  for  aqueous 
systems  rests  upon  use  of  "concentration  cells"  which,  granting 
certain  assumptions  in  regard  to  liquid  junctions,  determines  the 
free  energy  of  transport  of  hydrions  between  two  solutions.  As 
a  reference  there  is  used  a  theoretical  standard  of  activity  or, 
practically,  a  solution  of  hydrochloric  acid  which  for  simplicity 
we  shall  now  say  has  a  hydrion  activity  of  unity.  But  it  was  more 

539 


540  THE    DETERMINATION    OF   HYDROGEN   IONS 

or  less  immaterial  to  the  purposes  of  the  preceding  chapters  to 
specify  the  state  of  the  hydrion.  It  was  even  said  that  we  would 
agree  to  ignore  the  hydration.  It  is  highly  probably  that  in 
aqueous  solutions  there  are  few  anhydrous  hydrions,  H+,and 
that  the  hydrions  are  largely  hydrated,1  e.g.,  H3+0  (see  Br0nsted, 
1927  and  Schreiner,  1922-1924).  If  then  we  have  a  cell  of  the 
following  type 


Pt,H2 


Aqueous  solution        II  Non-aqueous  solution 
hydrion  activity  =  1  ||     of  an  acid 


Pt,H2 


the  transport  of  ' 'hydrions"  might  well  involve  a  large  quantity 
of  free  energy  in  the  exchange  of  the  solvents  of  solvation. 

We  can  avoid  this  mechanistic  conception  and  can  still  choose 
the  aqueous  system  as  a  standard  and  say  that  the  activity  of 
the  hydrion  is  unity  in  the  non-aqueous  solution  when  the  poten- 
tial of  the  above  cell  is  zero. 

Nevertheless,  in  practice,  we  still  have  the  liquid  junction  poten- 
tial which  was  eliminated  from  consideration  in  the  above  dis- 
cussion. Suppose  two  solvents  are  in  junction.  Suppose  these 
solvents  are  miscible  to  only  a  slight  extent  so  that  two  contiguous 
phases  may  be  established  in  equilibrium.  It  is  convenient  to 
regard  the  ions  in  solution  to  have  individual  distribution  coeffi- 
cients and  in  general  to  be  distributed  between  the  two  solvents 
in  such  proportions  that  there  will  be  a  potential  difference  at 
the  interface.  This  potential  difference  is  now  a  constraint  which 
has  its  part  in  determining  the  escaping  tendencies  of  the  ions. 
When  the  potential  of  the  above  cell  (with  actual  liquid  junction) 
is  zero,  it  does  not  mean  that  the  two  electrode  potentials  are  the 
same.  Hence  the  application  of  the  above  definition  of  unit 
activity  for  the  non-aqueous  phase  would  imply  some  means  of 
eliminating  the  phase  boundary  potential. 

The  so-called  phase  boundary  potential  at  equilibrium  is  not 
to  be  confused  with  the  potential  arising  from  unequal  rates  of 
migration  of  ions  between  contiguous  but  miscible  solvents  as 
discussed  in  Chapter  XIII.  Phase  boundary  potentials  may  be 
very  large.2 

As  set  forth  in  Chapter  XXVII,  the  approximate  equations  of 

1  An  extensive  review  of  the  literature  on  ion  hydration  up  to  1922  is 
given  by  Fricke  (1922). 

2  For  discussion  see  Michaelis  and  Perlzweig  (1926). 


XXIX  NON-AQUEOUS   SOLUTIONS  541 

acid-base  equilibria  are  valid  when  there  is  chosen  any  arbitrary 
reference  and  for  many  purposes  the  study  of  non-aqueous  solu- 
tions by  the  potentiometric  method  may  well  proceed  with  the 
use  of  any  standard  of  potential.  One  further  caution  is  then 
necessary.  As  D,  the  dielectric  constant  of  the  solution,  de- 
creases, the  correction  term  or,  —  log  71,  increases  as  shown  by 
inspection  of  equation  25,  Chapter  XXV.*  Consequently  the 
apparent  dissociation  constants  of  acids  in  non-aqueous  solution 
should  change  more  rapidly  than  in  aqueous  solutions  with 
change  in  the  ionic  strength  of  the  solution.  With  few  excep- 
tions the  dielectric  constants  of  non-aqueous  solvents  are  much 
smaller  than  that  of  water.  The  following  values  are  approximate. 


SOLVENT  (LIQUIDS) 

DIELECTRIC 
CONSTANT 

HCN  

95 

Water  

81 

Glycerol.  

56 

Ethanol  

21 

Acetone  

21 

Ammonia  

21  (-34°) 

Glacial  acetic  acid  

10 

Benzene  

2 

Hexane  

1.9 

(Air)  

1  0006 

(Vacuum).  .  .  . 

1  0 

Before  proceeding  it  will  be  well  to  mention  the  advantage,  in 
this  field,  of  a  formulation  of  acid-base  equilibria  developed  by 
Adams  (1916),  Michaelis  (1914),  Bjerrum  and  particularly 
Br0nsted  (1923). 

Let  there  be  a  substance  S  which  can  liberate  a  hydrion 

S  ^±  B  +  H+  (A) 

Examples  are 

CH3COOH  ^±  CH3COO-  +  H+ 
acetic  acid  acetate 

NH4+       ^      NH3      +H+ 
ammonium        ammonia 

COOHCOO-      ^±  COO-COO-  +  H+ 
1st  oxalate  anion         2nd  oxalate  anion 

NH2C6H4C6H4NH3+  ;=±  NH2C6H4-C6H4NH2  +  H+ 
1st  benzidine  cation  benzidine 

*For  an  extreme  see  Schreiner  and  Frivold  (1926). 


542         THE  DETERMINATION  OF  HYDROGEN  IONS 

By  this  scheme  one  avoids  the  formal  inclusion  of  the  solvent  as, 
for  instance,  in  the  formulation  of  ammonium:  ammonia  equi- 
libria. See  page  48.  One  may  then  write  in  general  for  a 
reaction  of  type  A,  above : 

(BHH+) 

(S) 
or 

(S) 


(B)  (H+)  " 

where  Ka  is  called  the  dissociation  constant  of  an  acid  and  Kb 
the  association  constant  of  a  base. 

It  is  confusing  to  name  cations,  anions  and  undissociated 
molecules  in  the  way  Br0nsted  does  below. 

NH+  ^±  NH3  +  H+ 
acid       base 

CHsCOOH  ^  CH3COO-  +  H+ 

acid  base 

The  formal  scheme  he  proposes  is  convenient  and  illuminating 
and  can  be  used  without  the  new  names. 

While  thermodynamic  methods  are  not  concerned  with  mech- 
anism, it  is  profitable  to  reconsider  the  formulation  of  acid-base 
equilibria  with  regard  to  the  solvent  concerned. 

In  formulating  the  equilibrium  state  for  the  ionization  of  an 
acid 

HA  ^  H+  +  A- 
we  wrote 

(H+)  (A-) 

(HA) 
We  could  have  assumed  interaction  with  water 

HA  +  H2O  ^±  HjO  +  A- 
and  could  have  written 

(HfO)  (A-) 


(HA)  (H20) 


=  K 


XXIX  NON-AQUEOUS   SOLUTIONS  543 

or  if  (H20)  is  considered  constant 
(HJ-Q)  (A-) 


(HA) 


tinguish  this  hydrion  from  H+,  the  proton.  Likewise  for  an 
acid  in  any  solvent,  the  activity  of  which  is  considered  constant, 
we  may  write: 


(HA) 

Here  Hsol  represents  the  solvated  proton. 
Now  suppose  a  base  B  to  be  added  to  the  acid  solution  and  to 
react  according  to 

B  +  Hsol  ^  BH+  +  Sol. 
Considering  (Sol)  a  constant  we  have 
(B)  (Hs+ol) 


, 
Kbs 


(BH+) 

Combination  of  (1)  and  (2)  gives 

(BH+)  (A-)          «  , 

(B)  (HA)      *  Kb. 

which  is  the  equilibrium  equation  for 

B  +  H  A  ^  BH+  +  A- 

At  equilibrium  the  extent  to  which  this  reaction  will  have  pro- 
ceeded from  left  to  right,  as  written,  may  now  be  described  by 

K  TC 

the  ratio  -=r*>     That  is,  the  magnitude  of  ^  determines  whether 

J^bs  Kb3 

or  not  a  given  acid  and  a  given  base  will  react  extensively  in  the 
given  solvent  to  furnish  a  stable  salt  without  what  corresponds 
to  hydrolysis  in  aqueous  solution. 

Kas  is  a  measure  of  the  extent  to  which  the  solvent  tends  to 
appropriate  the  proton  of  HA;  while  Kbs  is  a  measure  of  the  ex- 
tent to  which  the  solvent  tends  to  appropriate  the  proton  of 
BH+.  If  Kas  is  much  larger  than  Kbs,  the  cation,feH+  can  form. 


544 


THE  DETERMINATION  OF  HYDROGEN  IONS 


Thus  Hall  and  Conant  (1928)  (see  figure  96)  show  that  urea 
and  other  bases,  which  are  too  "weak"  to  form  stable  salts  in 
water  solution,  can  be  titrated  and  form  stable  salts  with  sulfuric 
acid  or  perchloric  acid  in  glacial  acetic  acid  solution. 


HAc 


.0 


FIG.  96/TiTRATioN  OF  0.05  N  BASES  IN  GLACIAL  ACETIC  ACID  WITH  X 

EQUIVALENTS  OP  PERCHLORIC  ACID 
(Advance  data  furnished  by  courtesy  of  Dr.  Norris  F.  Hall) 

In  liquid  ammonia  we  have  a  solvent  with  a  great  "affinity" 
for  hydrions.  In  this  case  the  solvated  hydrion  is  the  ammonium 
ion  NH4+.  Franklin  (1924)  shows  that  phenolphthalein  in  liquid 
ammonia  is  colorless  but  on  addition  of  potassium  amid  the  red 
color  develops. 


KNH2  +  HP  ~+  KNH3+ 


P~ 

colored  anion 


XXJX 


NON-AQUEOUS   SOLUTIONS 


545 


On  "back-titration"  with  the  acid,  (NC)2NH,  we  may  regard 
this  acid  to  furnish  hydrions  which  are  solvated  to  NH4+.  H+ 
+  NH3  =  NH4+.  This  ammonium  ion,  solvated  proton,  reacts 
as  follows 

NH4+  +  P-  =  NH3  +  HP 

Thus  the  discharge  of  color  in  a  liquid  ammonia  solution  of 
phenolphthalein  salt  may  be  attributed  to  the  acidifying  effect 
of  the  ammonium  ion! 

In  their  study  of  glacial  acetic  acid  solutions  Hall  and  Conant 
(1927)  and  Conant  and  Hall  (1927)  use  the  cell 


Pt 


C6C1402  (sat.) 
C6C1402H2  (sat.) 

HX  in  glacial 
acetic  acid 


Bridge 


.KC1,  (sat.) 
HgCl 

aqueous 


Hg 


For  a  note  on  the  chloranil  electrode  see  page  417. 

The  bridge  was  a  supersaturated  solution  of  lithium  chloride 
in  acetic  acid,  crystallization  being  inhibited  by  a  small  amount 
of  gelatin.  This  solution  was  enclosed  in  a  glass-stoppered  U- 
tube.  Because  of  the  high  resistance  of  the  cell,  a  quadrant 
electrometer  was  used  as  null-point  instrument. 

Figure  96  shows  the  results  with  several  bases  titrated  with 
perchloric  acid  in  glacial  acetic  acid.  The  ordinates  are:  on  the 
left  the  potentials  of  the  cell  and  on  the  right  the  "pH  numbers"3 
calculated  with  an  arbitrary  reference  point  which  is  defined  by 


0.566  -  E 
0.0591 


at  25' 


3  It  will  be  noted  that  the  description  of  the  data  shown  in  figure  96 
can  be  accomplished  by  use  of  the  potentials  without  the  so-called  pH 
values.  In  either  case  an  assumption  regarding  the  phase-boundary 
potential  has  been  used.  According  to  the  temperament  of  the  reader 
he  will  be  pleased  or  offended  by  the  use  of  "pH"  in  this  instance.  No 
fundamental  objection  can  be  raised  since  Conant  and  Hall  state  their 
assumptions  and  use  pH  in  the  activity  sense.  However,  their  values  are 
such  as  to  make  correction  factors  several  thousand  times  the  quantity 
corrected  if  the  connotation  of  a  "corrected  concentration"  be  retained 
for  "the  activity."  If  this  connotation  be  retained,  the  use  of  "pH"  in 
these  cases  is  inartistic.  Conant  and  Hall  speak  of  super-acid  solutions 
in  these  cases.  Compare  page  38. 


546 


THE    DETERMINATION    OF   HYDROGEN   IONS 


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XXIX  NON-AQUEOUS   SOLUTIONS  547 

On  this  scale  the  zero  for  pH  is  the  value  of  a  urea  solution  44 
per  cent  neutralized. 

In  table  68  are  shown  buffer  solutions  in  glacial  acetic  acid 
prepared  from  sulfuric  acid  (nos.  1  and  2)  from  acetanilid  and 
sulfuric  acid  (no.  3)  from  benzamid  and  sulfuric  acid  (no.  4), 
from  acetanilid  and  sulfuric  acid  (no.  5)  and  from  urea  and 
sulfuric  acid  (nos.  6,  7  and  8).  The  potentials  of  the  above  cell 
are  shown  in  the  upper  row  of  the  table  and  the  "pH"  value  in 
the  lowest  row.  The  color  changes  of  several  indicators  in  these 
buffer  solutions  are  indicated  in  the  table. 

Bishop,  Kittredge  and  Hildebrand  (1922)  used  the  following 
cell  for  titrations  in  ethanol. 


H2  (1  atmos.),  Pt 


Solution  in 
Ethanol 


NaBr  (0.1  N) 
Ethanol          ' HgBr 


Hg 


They  titrated  various  acids  with  a  solution  of  sodium  ethylate 
and  various  bases  with  anhydrous  HC1  dissolved  in  ethanol. 

Bishop,  Kittredge  and  Hildebrand  determined  roughly  the 
positions  of  color-change  of  various  indicators  on  an  arbitrary 
scale. 

Michaelis  and  Mizutani  (1925)  report  upon  the  changes  of 
apparent  dissociation  constants  (expressed  as  pK')  of  several 
acids,  of  ammonia  and  of  several  ampholytes  as  the  solvent  is 
gradually  changed  from  aqueous  to  alcoholic  through  inter- 
mediate mixtures.  While  a  rough  parallelism  is  to  be  noticed  in 
the  changes  of  pK  for  certain  acids,  there  remain  notable  ex- 
ceptions. Michaelis  and  Mizutani  (1924)  give  the  changes  in 
apparent  pK'  of  nitrophenol  indicators  and  phenolphthalein 
with  change  in  the  alcohol  content  of  the  solution.  See  also 
Kolthoff  (1923),  Thiel,  Wulfken  and  Dassler  (1924). 

Cray  and  Westrip  (1925)  have  calibrated  a  series  of  buffer 
solutions  and  worked  out  the  "pH-ranges"  of  various  indicators 
for  acetone  containing  10  volumes  of  water  in  100  volumes  of 
acetone-water. 

Linderstr0m-Lang  (1927)  discusses  the  advantages  of  titrating 
amino  acids  in  acetone  solution. 

For  an  example  of  a  study  of  equilibria  in  two  phase  systems 
see  Murray  (1923). 


548  THE    DETERMINATION    OF   HYDROGEN   IONS 

The  quinhydrone  electrode  has  been  used  in  the  study  of  non- 
aqueous  solutions  by  Schreiner  (1924),  Larrson  (1924),  Ebert 
(1925),  Millet  (1927),  Pring  (1925),  Cray  and  Westrip  (1925), 
Lund  (1926). 

A  review  of  the  electrochemistry  of  non-aqueous  solutions  is 
given  by  Walden  (1924)  and  Miiller  (1924).  See  also  Germann 
(1925). 


CHAPTER  XXX 

APPLICATIONS 

Finally,  acidity  and  alkalinity  surpass  all  other  conditions,  even 
temperature  and  concentration  of  reacting  substances,  in  the  in- 
fluence which  they  exert  upon  many  chemical  processes. — L.  J. 
HENDERSON. 

GENERAL  REMARKS 

It  is  because  of  the  great  variety  of  applications  in  research, 
routine  and  industry  that  the  theories  and  devices  outlined  in  the 
previous  chapters  have  been  developed.  The  physical  chemist 
sees  in  them  the  instruments  of  approximation  or  of  precision 
with  which  there  have  been  discovered  orderly  relations  of  ines- 
timable service  to  the  chemist  and  with  which  there  have  been 
established  quantitative  values  for  free  energy  changes.  The  bio- 
chemist might  almost  claim  some  of  these  methods  as  his  own,  not 
only  because  necessity  has  driven  him  to  take  a  leading  part  in 
their  development,  but  also  because  their  application  has  become 
part  of  his  daily  routine  in  very  many  instances. 

As  a  comprehensive  generalization  it  may  be  said  that  the 
hydrogen  ion  concentration  of  a  solution  influences  in  some 
degree  every  substance  with  acidic  or  basic  properties.  When  we 
have  said  this  we  have  said  that  the  hydrogen  ion  concentration 
influences  the  great  majority  of  compounds,  especially  those  of 
biochemical  interest.  Such  a  generalization,  however,  would  be 
misleading  if  not  tempered  by  a  proper  appreciation  of  propor- 
tion. Rarely  is  it  necessary  to  consider  the  ionization  of  the 
sugars  since  their  dissociation  constants  are  of  the  order  of  10~18 
and  their  ionization  may  usually  be  neglected  in  the  pH  region 
encountered  in  physiological  studies.  Likewise  there  are  zones  of 
pH  within  which  any  given  acidic  or  basic  group  will  be  found  in 
dilute  solution  to  be  in  a  practically  undissociated  or  fully  dis- 
sociated state.  Perhaps  there  is  no  more  vivid  way  of  illustrat- 
ing this  than  by  a  contemplation  of  the  conduct  of  indicators. 
Above  a  certain  zone  of  hydrogen  ion  concentration  phenol- 

549 


550  THE    DETERMINATION    OF   HYDROGEN    IONS 

phthalein  solutions  are  colorless.  Below  this  zone  (until  intense 
alkalinity  is  reached)  only  the  colored  form  exists.  Within  the 
zone  the  color  of  a  phenolphthalein  solution  is  intimately  related 
to  the  hydrogen  ion  concentration.  The  conduct  of  phenol- 
phthalein, which  happens  to  be  visible  because  of  tautomeric 
changes  which  accompany  dissociation,  is  a  prototype  of  the  con- 
duct of  all  acids.  Just  as  we  may  suppress  the  dissociation  of 
phenolphthalein  by  raising  the  hydrogen  ion  concentration  of  the 
solution  so  may  we  suppress  the  dissociation  of  any  acid  if  we  can 
find  a  more  intensely  ionizing  acid  with  which  to  increase  the 
hydrogen  ion  concentration  of  the  solution.  Similar  relations 
hold  for  bases,  and,  if  we  regard  methyl  red  as  a  base,  we  may 
illustrate  with  it  the  conduct  of  a  base  as  we  illustrated  the  con- 
duct of  an  acid  by  means  of  phenolphthalein. 

Such  illustrations  may  serve  to  emphasize  the  reason  underly- 
ing the  following  conclusion.  Whenever,  in  the  study  of  a  physi- 
ological process,  of  a  step  in  analysis  requiring  pH  adjustments  or 
of  any  case  involving  equilibria  comparable  with  those  mentioned 
above,  there  is  sought  the  effect  of  the  pH  of  the  solution,  it  may 
be  expected  that  no  particularly  profound  effect  will  be  observed 
beyond  a  certain  zone  of  pH.  Within  or  at  the  borders  of  such  a 
zone  the  larger  effects  will  be  observed.  From  this  we  may  con- 
clude that  the  methods  of  determining  hydrogen  ion  concentra- 
tions should  meet  two  classes  of  requirements.  In  the  first 
place,  when  the  phenomenon  under  investigation  or  control  in- 
volves an  equilibrium  which  is  seriously  affected  by  the  pH  of 
the  solution,  the  method  of  determining  pH  values  should  be  the 
most  accurate  available.  In  the  second  place,  when  the  equi- 
librium is  held  practically  constant  over  a  wide  range  of  pH,  an 
approximate  determination  of  pH  is  sufficient  and  refinement 
may  be  only  a  waste  of  time. 

Neglecting  certain  considerations  which  often  have  to  enter 
into  a  choice  of  methods  it  may  be  said  that  the  electrometric 
method  had  best  be  applied  in  the  first  case  and  the  indicator 
method  in  the  second.  When  the  nature  of  the  process  is  not 
known,  and  it  therefore  becomes  impossible  to  tell  a  priori  which 
method  is  to  be  chosen,  the  colorimetric  method  becomes  a  means 
of  exploration  and  the  electrometric  method  a  means  of  con- 
firmation. 


XXX  GENERAL  REMARKS  551 

Exception  will  be  taken  to  this  statement  as  comprehensive 
for  there  are  cases  where  one  or  another  method  has  to  be  dis- 
carded because  of  the  nature  of  the  solution  under  examination. 
Nevertheless,  in  general,  the  utility  of  the  colorimetric  method 
lies  in  its  availability  where  approximations  are  needed  and 
exact  determinations  are  useless  and  also  in  its  value  for  recon- 
naissance; while  the  value  of  the  electrometric  method  lies  in  its 
relative  precision. 

In  some  instances  the  qualitative  and  quantitative  relations  of 
a  phenomenon  to  pH  should  be  carefully  distinguished.  Note,  for 
instance,  the  significance  of  an  optimum  or  characterizing  point. 
Consider  the  conduct  of  phenol  red  and  of  cresol  red.  These  two 
indicators  appear  to  a  casual  observer  to  be  very  much  alike 
in  color  and  each  exhibits  a  similar  color  in  buffer  solutions  of  pH 
7.6,  7.8,  etc.  Careful  study,  however,  shows  that  each  point  on 
the  dissociation  curve  of  phenol  red  lies  at  a  lower  pH  than  the 
corresponding  point  on  the  dissociation  curve  of  cresol  red.  If 
the  half  transformation  point  be  taken  as  characteristic  it  may  be 
used  to  identify  these  two  indicators.  Likewise  it  is  the  dissocia- 
tion constant  of  an  acid  or  a  base,  the  isoelectric  point  of  a  protein, 
the  optimum  pH  for  acid  agglutination  of  bacteria,  or  an  optimum 
for  a  process  such  as  enzyme  activity  that  furnishes  characteristic 
data. 

When  there  is  observed  a  correlation  between  pH  and  some 
effect,  the  mere  determination  of  pH  alone  will  of  course  throw 
but  little  light  upon  the  real  nature  of  the  phenomenon  except 
in  rare  instances.  Determination  of  the  hydrogen  ion  concentra- 
tion will  not  even  distinguish  whether  a  given  effect  is  influenced 
by  the  hydrogen  or  the  hydroxyl  ions,  nor  will  it  always  reveal 
whether  the  influence  observed  is  direct  or  indirect.  The  so- 
called  hydrion  concentration  or  pH  number  of  a  solution  may  be 
only  an  index  of  the  position  of  an  equilibrium  state  in  which  the 
hydrion  is  an  entity  of  no  great  importance  from  a  physical  point 
of  view.  See  Chapter  XXVII.  However,  if  only  as  an  index, 
its  importance  remains.  Therefore  advantage  should  be  taken 
of  the  comparative  ease  with  which  the  concentration  of  hydrogen 
ions  may  be  determined  or  controlled  and  its  influence  known  or 
made  a  constant  during  the  study  of  any  other  factor  which  may 
influence  a  process.  From  this  point  of  view  methods  of  deter- 


552  THE    DETERMINATION    OF   HYDROGEN   IONS 

mining  hydrogen  ion  concentration  take  their  place  beside  ther- 
mometers, buffer  mixtures  beside  thermostats  and  automatic 
control  devices  beside  thermoregulators. 

Indeed  it  may  be  said  that  the  failure  to  take  advantage  of 
these  devices  is  still  a  prolific  source  of  error  in  the  experimental 
work  of  every  branch  of  science  having  to  do  with  solutions.  In 
one  case  the  neglect  may  be  gross;  in  another  case  it  may  be  a 
perfectly  excusable  mis  judgment.  A  complete  understanding  of 
the  effects  of  the  hydrogen  or  hydroxyl  ion,  or  of  the  effects  of 
those  equilibrium  states  of  which  pH  is  an  index,  is  very  far  from 
attainment  and  those  who  faithfully  control  their  solutions  are 
often  rewarded  by  the  most  surprising  results.  To  emphasize 
this  aspect  we  may  call  attention  to  the  fact  that  while  the  disso- 
ciation of  glucose  is  negligible  in  the  region  of  pH  7  so  far  as  any 
great  effect  upon  the  displacement  of  other  acid-base  equilibria 
is  concerned,  a  converse  effect,  which  does  not  belong  to  the 
category  of  equilibria,  is  decidedly  not  negligible.  A  shift  in  pH 
from  7.0  to  7.4  has  a  very  marked  influence  upon  the  conduct  of 
glucose  in  heated  solutions  as  every  one  who  has  made  culture 
media  knows. 

Nor  is  it  adequately  realized  that  the  formulations  of  the 
measurements  we  make  are  so  fundamentally  thermo dynamic 
that  they  may  ignore  intermediate  stages  in  chemical  trans- 
formations or  may  lead  to  false  impressions  regarding  the  entities 
which  convenience  forces  us  to  symbolize  in  some  particular  way. 
Reference  was  made  on  page  540  to  the  fact  that  for  the  purposes 
of  a  limited  thermodynamic  treatment  it  is  a  matter  of  indif- 
ference whether  we  regard  the  hydrion  in  aqueous  solution  to  be 
hydrated  or  not.  Yet  this  item  may  leap  into  importance  when 
we  attempt  to  compare  events  in  different  solvents.  So,  also,  the 
ignoring  of  groups  which,  as  measured  by  ordinary  methods, 
appear  to  have  in  aqueous  solution  little  tendency  to  dissociate, 
may  obscure  their  parts  in  kinetic  events. 

Our  methods  of  formulation  tend  to  emphasize  either  one 
particular  function  or  some  refinement  of  this  function  that  re- 
quires a  new  symbolism.  We  may  then  fall  victim  to  that 
restraint  upon  outlook  which  led  Comte  to  remark:  "every 
attempt  to  employ  mathematical  methods  in  the  study  of  chem- 
ical questions  must  be  considered  profoundly  irrational  and  con- 


XXX  ON   THE   BIBLIOGRAPHY  553 

trary  to  the  spirit  of  chemistry "     Mellor,  who  gives  this 

translation  of  Comte,  believes  that  the  key  to  these  remarks  is 
Comte's  statement  that  "our  feeble  minds  can  no  longer  trace 
the  logical  consequences  of  the  laws  of  natural  phenomena  when- 
ever we  attempt  to  simultaneously  include  more  than  two  or 
three  essential  factors."  Nevertheless  the  requirements  of  bio- 
chemistry impose  the  task  of  simultaneously  including  many 
factors.  If  this  task  is  to  be  met,  the  physical  chemist  must 
develop  methods  of  formulation  of  such  fundamental  directness, 
simplicity  and  generality  that  the  biochemist  will  not  mistake 
the  formalities  of  convenience  which  lead  to  "vanishing  par- 
ticulars" for  those  other  and  still  necessarily  artificial  devices  of 
the  intellect  which  lead  to  a  comprehension  of  togetherness. 

ON  THE  BIBLIOGRAPHY 

As  mentioned  in  the  first  edition  of  this  book,  the  applications 
had,  by  1920,  become  so  numerous,  and  in  many  instances  so 
detailed,  that  the  time  had  come  for  a  redispersion  among  the 
several  sciences  of  the  material  that  had  from  time  to  time  been 
assembled  by  authors  who  were  intent  upon  emphasizing  the 
importance  of  hydrion  concentration.  The  crude  statistics  noted 
in  the  preface  to  this,  the  third  edition,  indicate  the  appalling 
task  that  awaits  any  one  who  attempts  to  assemble  a  complete 
bibliography.  Even  the  limited  comprehensiveness  of  the  bib- 
liography of  the  second  edition  is  no  longer  practicable.  Con- 
sequently, while  this  chapter  retains  its  old  form,  there  has  had 
to  enter  the  element  of  selection.  This  has  been  distressing  to 
the  author,  ostensibly  because  of  the  injustices  that  may  be  done 
to  subject  matter  and  to  leading  authors,  but  probably  because 
selection  reveals  the  ignorance  of  the  selector.  However,  for 
those  students  who  desire  "leads"  in  their  first  attack  upon  the 
literature  there  may  remain  some  value  in  the  following  sketches. 

These  sketches  and  various  assemblies  of  references  in  the  text 
serve  as  crude  indices  to  the  bibliography.  In  this  are  to  be 
found  only  some  six  hundred  of  the  references  in  the  second  edition. 
Consequently  the  older  edition  should  be  consulted  for  many  of 
the  earlier  references.  The  following  selection  of  over  1600  refer- 
ences is  not  to  be  considered  in  any  other  way  than  as  an 
introduction  to  a  vast  literature. 


554        THE  DETERMINATION  OF  HYDROGEN  IONS 
GENERAL  TREATISES 

What  may  be  called  the  fundamental  classic  is  the  paper  pub- 
lished by  S.  Arrhenius  in  1887.  The  subsequent  evolution  of  the 
theory  of  electrolytic  dissociation  to  1914  is  reviewed  by  Arrhenius 
(1914)  and  in  Faraday  Society  Symposium  (1927). 

Among  several  papers  of  historical  interest  is  that  of  Bugarzsky 
and  Liebermann  (1898)  who  first  applied  the  hydrogen  electrode 
to  a  biochemical  problem,  and  Bottger's  paper  on  titration. 

Two  classics  of  biochemistry  are  S0rensen's  (19C9)  Etudes 
enzymatiques  II  in  which  are  organized  the  subjects  of  buffer 
solutions  and  indicators  and  Henderson's  (1909)  Das  Gleichge- 
wicht  zwischen  Basen  and  Sauren  im  tierischen  Organismus  in 
which  is  outlined  the  acid-base  equilibria  of  the  blood. 

The  papers  of  Noyes  (1910)  and  of  Bjerrum  (1914)  on  the 
theory  of  titration  have  needed  but  slight  elaboration  since  their 
publication. 

No  one  has  contributed  so  widely  to  the  applications  of  indi- 
cator and  electrode  methods  as  has  Michaelis.  Indeed  an  ex- 
cellent cross-sectional  view  of  the  variety  of  these  applications 
can  be  obtained  by  reading  Michaelis'  numerous  papers.  These 
are  "easily  traced  in  abstract  journals  and  will  not  be  cited  in 
detail.  The  first  edition  (1914)  of  Michaelis'  Die  Wasserstoffio- 
nenkonz'entration  contained  brief  reviews  of  applications.  The 
second  edition  (1922),  now  in  an  English  translation  by  Perlz- 
weig  (1926),  elaborated  the  theoretical  sections  of  the  first. 

As  the  subject  has  gained  prominence  in  special  fields  the 
journals  and  compilations  covering  these  fields  have  published 
reviews.  These  reviews  are  too  numerous  to  mention.  Books 
by  the  following  authors  may  be  cited: 

Kolthoff  (1923).  Der  Gebrauch  von  Farbenindicatoren.  Springer,  Berlin. 
French  edition  translated  by  Vellinger,  1927.  English  edition  trans- 
lated by  Furman  (1926).  John  Wiley. 

Kopacewski  (1926) .  Les  ions  d'hydrogene.  Signification,  mesure,  appli- 
cations, donnees  numeriques.  Gauthier-Villars,  Paris. 

Michaelis  (1914-1923).  Die  Wasserstoffionenkonzentration.  Springer,  Ber- 
lin. The  second  edition  (1923)  enlarged  upon  only  the  theoretical 
part  of  the  first.  Second  edition  translated  into  English  by  Perlz- 
weig,  1926.  Williams  and  Wilkins,  Baltimore. 

Mislowitzer  (1928).  Die  Bestimmung  der  Wasserstoffionenkonzentration 
von  Fliissigkeiten.  Springer,  Berlin. 


f  *  *  .     • 


XXX  SPECIAL   APPLICATIONS,    A-B  555 

Mizutani    (1925).     The   determination   of  hydrogen   ions.     (In    Japanese) 

Tokyo. 

Prideaux  (1917).     The  theory  and  use  of  indicators.     Van  Nostrand,  N.  Y. 
Vincent  (1924).    La  concentration  en  ions  hydrogene  et  sa  mesure  par  la 

methode  electrometrique.    Hermann,  Paris. 
See  also  Rona  (1926). 

SPECIAL  APPLICATIONS 

Analyses.  Hydrion  methods  have  manifold  applications  through  the 
theory  of  titration.  See  Chapter  XXVIII.  Intimately  related  are 
methods  of  oxidation-reduction  titration,  one  aspect  of  which  was  discussed 
in  Chapter  XVIII.  For  particulars  in  regard  to  potentiometric  Nitrations 
in  analysis  see  Miiller  (1926),  Kolthoff  and  Furman  (1926)  and  Popoff 
(1927).  The  empiricism  that  characterized  the  older  developments  in 
analytical  chemistry  often  left  specifications  for  the  use  of  mixtures  of 
acids  and  their  salts.  These  we  now  know  control  the  ratios  of  the  con- 
centrations of  ions  and  undissociated  molecules,  and  a  useful  index  to  such 
a  ratio  is  the  proper  combination  of  the  pH  number  of  the  solution  and  the 
pKa  or  pKb  number  of  a  given  system.  The  older  specifications  also 
left  directions  for  delicate  proportionment  of  reagents  which  often  can 
be  conveniently  expressed  in  terms  of  pH.  These  conveniences  are  coming 
into  wide  use  without  that  systematic  record  which  permits  adequate 
references.  As  examples  in  the  field  of  inorganic  analysis  there  may  be 
cited  the  papers  by  Blum  (1913,  1914  and  1916),  Fales  and  Ware  (1919), 
Hildebrand  and  cowofkers  (1913-1916),  Robinson  (1923).  Among  several 
methods  of  biochemistry  there  may  be  mentioned  the  benzidine  sulfate 
method  for  the  determination  of  sulfate  (see  any  text).  General  princi- 
ples of  the  application  are  to  be  found  in  modern  texts  of  inorganic  anal- 
ysis, e.g.,  Kolthoff  and  Menzel's  Massanalyse  (1928),  Fales  (1925),  and  the 
older  text  of  Stieglitz  (1917).  Separations  of  proteins,  amino  acids  etc. 
involve  constant  attention  to  pH.  See,  for  example,  Abel  et  al.  (1927), 
Vickery  and  Leavenworth  (1927),  Foster  and  Schmidt  (1923). 

Bacteriology.  The  applications  in  bacteriology  up  to  1917  are  reviewed 
by  Clark  and  Lubs  (1917).  For  a  bibliography  on  the  role  of  ions  in 
general  in  bacterial  physiology  see  I.  S.  Falk  (1923).  For  various  modern 
applications  see  Jordan  and  Falk  (1928),  Buchanan  and  Fulmer  (1928). 

Acid  agglutination  of  bacteria,  first  definitely  recognized  by  Michaelis 
(1911)  in  its  relation  to  hydrion  concentration  has  been  found  to  be  of 
some  diagnostic  use.  For  example,  Gillespie  (1914).  Eisenberg  gives  an 
extensive  bibliography  up  to  1919.  See  especially  Northrop  and  DeKruif 
(1922)  and  De  Kruif  (1922). 

Adjustment  of  the  reaction  of  media  by  the  old  titrimetric  procedure  was 
criticized  by  Clark  (1915),  and,  on  the  introduction  of  suitable  indicators 
and  the  evidence  for  the  advantage  of  adjusting  on  the  pH  basis,  the 
titrimetric  method  has  been  abandoned  for  more  significant  and  easier 
modern  methods.  Studies  on  growth  optima  (which  see  below)  have  shown 


556         THE  DETERMINATION  OF  HYDROGEN  IONS 

that  for  the  cultivation  of  most  saprophytes  approximate  indicator  control 
is  sufficient.  For  particular  purposes  and  especially  for  the  study  of 
certain  important  pathogens,  it  is  well  to  adjust  with  the  precision  at- 
tained with  standards.  Seldom  is  electrometric  control  necessary.  Data 
for  special  media  and  special  organisms  now  usually  accompany  all  de- 
scriptions. See,  for  example,  Standard  Methods  of  Water  Analysis,  H.  N. 
Cohn  (1919),  Medical  Research  Committee  (1919). 

Antigenic  action.  For  example  see  Falk  and  Powdermaker  (1925). 
See  Immunology. 

Bacterial  products,  purification.  For  example,  see  Michaelis  and 
Davidsohn  (1924). 

Bacteriophage.  For  examples  see,  Davison  (1922),  Arloing  and  Chavanne 
(1925),  and  Todd  (1927). 

Bacteriostatic  action  of  dyes.  For  examples  see,  Churchman  (1922), 
Smith  (1922),  and  Stearn  and  Stearn  (1924,  1926). 

Disinfectant  action  of  acids  and  bases  is  certainly  in  large  measure  a 
function  of  hydrogen  and  hydroxyl  ion  activity;  but  specific  effects  of 
certain  acids  and  bases  which  were  suspected  before,  have  now  been  more 
clearly  demonstrated  by  the  use  of  hydrogen  ion  methods.  By  the  con- 
ductivity method,  Winslow  and  Lochridge  (1906)  were  able  to  show  the 
effect  of  the  hydrogen  ion  in  simple  solutions  and  predicted  relations 
which  more  powerful  methods  have  extended  to  complex  media.  Cohen 
(1922)  has  reviewed  certain  of  the  fundamental  relations  between  pH  and 
viability  of  bacteria  under  sublethal  conditions.  The  more  direct  action 
of  hydrion  concentration  upon  cells  must  be  distinguished  from  its  control 
upon  the  effective  state  of  a  toxic  compound.  Knowledge  of  pH  effects  is 
therefore  essential  to  the  assay  of  disinfectants  and  to  the  advancement 
of  chemotherapy. 

See  review  by  Bonacorsi  (1923),  and  references  by  Jarisch  (1926).  Ex- 
amples: Michaelis  and  Dernby  (1922),  Dernby  and  Davide  (1922),  Eggerth 
(1926),  Fleischer  and  Amster  (1923),  Kuroda  (1926),  Levine,  Toulouse  and 
Buchanan  (1928). 

Electrophoresis .  Winslow,  Falk  and  Caulfield  (1923),  and  papers  by 
Falk  in  Journal  of  Infectious  Diseases,  1925-1927. 

Gram  reaction.    See  "Staining." 

Influence  of  pH  on  bacterial  metabolism.  The  reaction  of  the  medium, 
even  within  the  zone  of  optimal  bacterial  growth,  is  found  to  influence 
either  the  absolute  rate,  or  the  relative  rate  of  specific  types  of  metab- 
olism. Not  only  the  activity  but  also  the  production  of  enzymes  is 
influenced;  and  the  production  of  special  products  such  as  toxins  is  par- 
tially controlled  by  the  pH  of  the  medium. 

Examples:  Virtanen  and  Barlund  (1926),  Arzberger,  Peterson  and  Fred 
(1920),  Clark  (1920),  Avery  and  Cullen  (1920),  Merrill  and  Clark  (1928). 

Morphology.    Example:  Reed  and  Orr  (1923). 

Motility.    Example:  Reed  and  MacLeod  (1924). 

Optimal  Zones  and  the  limits  of  growth  and  general  metabolism  have 
naturally  been  the  chief  interest  in  the  first  surveys  of  the  influence  of  hy- 


XXX 


BACTERIOLOGY 


557 


TABLE  69 

Optimum  and  limiting  reactions  for  the  activities  of  microorganisms 
(After  Waksman,  1927) 


ORGANISMS 

ACID 
MAXI- 
MUM 

OPTIMUM 

ALKALI 

MAXIMUM 

AUTHOR 

Nitrosomonas  

pH 

3  9 

PH 

7  7-7  9 

pH 

9  7 

Gaarder  and  Hagen 

Nitrobacter    .  .  . 

3  9 

6  8-7  3 

13  0 

IVIeek  and  Lipman 

Nitrification  in  soils  

3  5 

65-75 

11  9 

Gerretsen  Waksman 

Thiobacillus  denitrificans 
Th   thiooxidans 

5.0 
1  0 

7.0-9.0 
2  0-4  0 

10.75 

6  or?) 

Trautwein 
Waksman  and  Starkey 

Bac   pycnoticus 

5  2 

6  8-8  7 

Q  2 

Ruhland 

Bac.  amylobacter  . 

5  7 

69-73 

Dorner 

Azotobacter    .... 

5  6-6  0 

6  5-7  8 

8  8-9  2 

Gainey     Johnson    and 

Bad.  radicicola  of: 
Medicago  and  Melilo- 
tus  

5  O] 

Lipman,      Yamagato 
Itano,  Stapp 

Pisum  and  Vicia 

4  8 

Trifolium  and  Phase- 
olus  

4  3[ 

11.0 

Fred    and    Davenport, 
Fred     and     Loomis, 

Soja  

3  4 

Bryan 

Lupinus  

3  2 

Bact   coli 

4  4 

6  5 

7  3 

Dernby 

Bact.  vulgare  

4  4 

6  5 

8  4 

Dernby 

Bact.  pyocyaneum  
Bact   stutzeri 

5.6 
6  1 

6.8 

7  0-8  2 

8.0 
9  6-9  8 

Dernby 
Zacharowa 

Bac   subtilis  

4  2 

75-85 

9  4 

Itano 

Bac.  putrificus 

5  8 

5  8 

8  5 

Dernby 

Act  scabies 

4  8-5  0 

6  5-7  5 

8  7 

Gillespie  ^Waksman 

Mucor  glomerula  

32-34 

87-92 

Asp   terricola 

1  6-1  8 

90-93 

Pen.  italicum  

16-18 

91-93 

Johnson 

Fus.  oxysporum. 

1  8-2  0 

9  2-11  1 

Asp  niger 

1  2 

1  7-7  7 

Terroine  and  Wurmser 

Gibberella  saubinetii  
Spore    germination    of 
fungi 

3.0 

1  5-2  5 

4.8-9.4 
3  0-4  0 

11.7 

Maclnnes 
Webb 

For  other  data  on  the  culture  of  microorganisms  other  than  bacteria 
see  Sakamura  (1924),  A.  Saunders  (1924),  Sartory,  Sartory  and  Meyer  (1927), 
Scott  (1924),  Waksman  (1927),  Webb  and  Fellows  (1926). 


558         THE  DETERMINATION  OF  HYDROGEN  IONS 

drion  concentration  upon  bacterial  activity.  It  is  now  clear  that  more 
exact  studies  will  have  to  differentiate  between  optimal  pH  to  initiate 
growth,  optimal  zones  of  growth,  optimal  zones  for  general  or  special 
metabolism,  optimal  zones  for  preservation,  etc.  The  self-limitation  first 
clearly  defined  by  Michaelis  and  Marcora  (1912)  has  been  applied  to  cer- 
tain practical  tests,  for  example  see  Clark  (1915),  Avery  and  Cullen  (1919). 
pH  limits  for  special  organisms  of  commercial  significance  are  exemplified 
by  control  of  "rope"  in  bread  (Cohn,  Wolbach,  Henderson  and  Cathcart, 
1918)  and  potato  scab  (Gillespie  and  Hurst,  1918).  Growth  optima  and 
limits  usually  accompany  modern  descriptions  and  are  best  sought  in  the 
special  literature.  As  illustrations  there  may  be  quoted  table  69. 
Several  of  the  pH  numbers  are  first  approximations. 

Sporulation.    Example :  Itano  and  Neill  (1919) . 

Testing  fermentation.  See,  for  examples:  Chesney  (1922),  Clark  and 
Lubs  (1917),  Nichols  and  Wood  (1922). 

Toxin  production.  Examples:  Abt  and  Loiseau  (1922),  Davide  and 
Dernby  (1921),  Dernby  and  Allander  (1921),  Dernby  and  Walbum  (1923), 
Jonesco-Mihaesti  and  Popesco  (1922),  Walbum  (1922-1923),  Cook  et  al. 
(1921).  See  also  Immunology. 

Vaccine  virus.    Defries  and  McKinnon  (1926) . 

Virulence.    Felton  and  Dougherty  (1924),  Defries  and  McKinnon  (1926) . 

Viscosity  of  bacterial  suspensions.    Falk  and  Harrison  (1926). 

Blood.  The  hydrion  concentration,  or  the  ratio  between  acid  residues 
and  their  anions,  is,  with  the  exception  of  temporary  fluctuations  (exercise, 
etc.),  regulated  with  remarkable  constancy  in  the  blood  of  any  normal 
individual.  It-  very  seldom  varies  far  from  pH  7.4.  Van  Slyke  (1921) 
places  the  normal  variation  between  7.3  and  7.5  and  the  limits  usually 
compatible  with  life  at  about  7.0  and  7.8,  although  he  takes  these  as  data 
convenient  to  a  general  description. 

The  bicarbonate-carbonic  acid  equilibrium  is  important  because  one  of 
the  chief  functions  of  the  blood  is  to  carry  C02.  The  bicarbonate  system 
is  also  used  as  an  indicator. 

See  carbonate  equilibria  for  the  derivation  of 

[HCOj] 

PH  -  PK^  10g  [fr^ck] 
and 

[free  CO2]  =  K0P 

Inspection  of  relations  involving  the  carbonate  ion,  CO3~~  (see  page  561), 
will  show  that,  at  pH  7.4,  [CO3~~]  may  be  neglected  and  that  the  fixed 
carbon  dioxide  may  be  regarded  for  present  purposes  as  almost  entirely  in 
the  form  of  bicarbonate.  Therefore  the  above  equations  suffice.  They 
can  be  combined  to 

[HCOj] 
PH  =  pK;  +  log  -r- 


XXX 


BLOOD 


559 


If  equations  in  terms  of  activities  are  to  be  used,  it  is  convenient  to  know 
that  Van  Slyke,  Hastings,  Murray  and  Sendroy  (1925)  have  estimated  the 
ionic  strength  of  blood  to  be  n  =  0.16. 

In  using  the  ideal  equation  with  whole  blood,  serum  or  solutions  such 
as  hemoglobin,  the  constants  must  be  evaluated  for  the  specific  conditions. 
Van  Slyke,  Cullen  and  Hastings  (1922)  use  the  values  shown  below 


SOLUTION 

KO 

WHEN  FOR- 
MULA 18  USED 
FOR  MILLIMOLS 

KO 

WHEN  FOR- 
MULA IS  USED 
FOR  VOLUME  — 
PER  CENT 

pK 

Water  

0  0326 

0.0730 

Serum  or  plasma 

0  0318 

0  0712 

6  14 

Whole  blood 

0  0300 

0  0672 

6  18 

12  per  cent  Hemoglobin  in  30  mM 
NaHCO3  

0.0312 

0.0699 

6.18 

Since  [HCO3-J  =  [Total  CO2]  -  [free  CO2],  the  above  equation  mav  be 
used  in  the  form 


PH  =  pKj  +  log 


[Total  C02]  -  KpP 
K0P 


This  shows  that,  for  the  definition  of  the  equilibrium  state,  two  measure- 
ments are  necessary:  pH  and  [Total  CO2];  pH  and  P;  or  [Total  CO2]  and  P. 

Fifty  volumes  per  cent  total  CO2  and  pH  7.4  may  be  regarded  as  an 
orienting  norm. 

Investigative  methods  utilize  pairs  of  these  quantities  in  determining, 
among  other  constituents  of  the  blood,  ratios  of  acid  residues  to  anions, 

on  the  principle  that,  at  a  common  pH  value,  the  determination  of 


[tree  C/L^J 

measures  all  such  ratios  of  any  anion  concentration  to  the  concentration 
of  the  dissociation  residue. 

A  tentative  hypothesis  which  is  useful  for  a  gross  description  of  the 
manner  in  which  these  ratios  is  kept  constant  is  that  the  "respiratory 
center"  is  sensitive  to  changes  of  pH,  stimulating  lung-  ventilation  as  pH 
decreases,  and  checking  lung-  ventilation  as  pH  increases.  This  hy- 
pothesis is  disputed.  (See  for  example  Y.  Henderson,  1922.)  It  remains 
a  hint  the  value  of  which  is  lost  when  it  is  forgotten  that  hydrion  concen- 
tration of  itself,  when  unrelated  to  definite  equilibria,  means  little 
chemically. 

When  "combustion"  in  the  tissues  is  incomplete  and  acid  products  of 
combustion  replace  the  CO2  which  the  lungs  can  eliminate,  and  when  these 
non-volatile  or  "fixed"  acids  cannot  be  eliminated  by  the  kidneys  as  fast 
as  produced,  the  fixed  acid  anions  will  replace  bicarbonate  ions.  Hence 
[Total  CO2]  in  the  last  equation  has  a  significance  of  its  own. 


560         THE  DETERMINATION  OF  HYDROGEN  IONS 

While  the  bicarbonate  system  is  important  in  itself,  it  is  not  the  chief 
buffer  system  of  the  blood.  The  protein  systems  are  the  more  powerful 
buffers  and  of  these  the  systems  involving  hemoglobin  and  oxyhemoglobin 
are  the  most  important.  Here  are  met  two  distinct  aspects.  In  the  first 
place  oxyhemoglobin  behaves  in  a  way  conveniently  described  as  if  it  were 
a  stronger  acid  than  hemoglobin.  Consequently  oxidation  in  the  lungs 
results  in  the  virtual  transfer  of  base  from  bicarbonate  to  oxyhemoglobin 
tending  to  displacement  of  C02.  In  the  tissues  the  reverse  effect,  attend- 
ing reduction  of  the  blood  pigment,  provides  base  to  combine  isohydrically 
with  CO2.  In  addition,  both  hemoglobin  oxyhemoglobin,  and  the  other 
proteins  exercise  ordinary  buffer  action.  In  these  two  senses  the  blood 
pigment  is  the  most  important  carrier  of  C02  as  well  as  the  chief  carrier 
of  oxygen. 

The  buffers  of  the  blood  are  distributed  between  the  cells  and  plasma. 
Not  all  the  constituents  of  the  buffer  systems  diffuse  freely  between  the 
cells  and  plasma.  Of  those  constituents  of  the  cell,  which  are  of  chief 
importance  and  which  do  not  diffuse  out,  are  the  several  forms  of  hemo- 
globin and  oxyhemoglobin  and  the  base  K+.  Likewise  the  plasma  pro- 
teins and  Na+  do  not  diffuse  inward.  There  is  established  a  complex 
Donnan  equilibrium  (see  page  568)  in  the  maintenance  of  which,  during 
CO 2  exchanges,  the  anions  HC03~  and  Cl~~  migrate  in  and  out  to  adjust 
electroneutrality,  and  water  migrates  in  and  out  to  maintain  osmotic 
equilibrium. 

Intimately  connected  with  the  regulation  of  the  hydrogen  ion  concen- 
tration of  the  blood  are  the  functions  of  the  kidneys.  [See  Cushny  (1926), 
and  Marshall  (1926).]  By  their  action  there  are  eliminated  the  non- 
volatile products  of  metabolism,  several  of  which  are  of  great  importance 
for  the  acid-base  equilibria  of  the  blood.  The  colorimetric  determination 
of  the  pH  of  the  urine  is  a  comparatively  simple  procedure  which  furnishes 
valuable  data  when  properly  connected  with  other  data.  (See  for  in- 
stance Blatherwick,  and  the  works  of  Henderson,  of  Palmer,  of  Van  Slyke, 
of  Cullen,  of  Hastings,  of  Austin,  etc.) 

While  the  greatest  interest  has  centered  in  the  subjects  briefly  men- 
tioned above,  there  remain  innumerable  other  problems  of  importance. 
Of  these  there  may  be  mentioned  the  relation  of  the  pH  of  the  blood  to 
the  calcium-carrying  power,  to  the  activity  of  various  enzymes,  to  the 
permeabilities  of  tissue  membranes,  to  the  activity  of  leucocytes,  and  to 
various  reactions  used  in  the  serum  diagnosis  of  disease. 

There  have  been  numerous  studies  of  the  blood  of  lower  animals.  See 
for  example,  Bodine  (1926),  Duval  (1924),  Glazer  (1925),  Gellhorn  (1927), 
Hawkins  (1924),  and  references  in  Porter  (1927). 

Gasometric,  colorimetric  and  potentiometric  methods  of  determining 
pH  numbers  of  blood,  serum  etc.  are  so  highly  specialized  that  the  special 
literature  of  the  technique  and  of  the  principles  of  the  equilibria  con- 
cerned should  be  consulted. 

The  following  references  are  selected  from  a  huge  literature  as  being 
especially  helpful. 


XXX  CARBONATES  561 

Historical.    Henderson  (1908-1909). 

Reviews  and  theoretical  discussions.  Austin  and  Cullen  (1926),  Hen- 
derson (1926),  Murray  and  Hastings  (1925),  Van  Slyke  and  Van  Slyke 
et  al.  (1921-1927),  Warburg  (1922). 

Methods.  Austin,  Stadie  and  Robinson  (1925),  Cullen  (1922),  Cullen 
and  Hastings  (1922),  Cullen,  Keeler  and  Robinson  (1925),  Dale  and  Evans 
(1920),  Eisenman  (1927),  Hastings  and  Sendroy  (1924r-1925). 

Physiological  data.  Cullen  and  Robinson  (1923),  Drury,  Beattie  and 
Rous  (1927),  Gamble  (1922). 

Respiration.    Haldane  (1922),  Barcroft  (1925). 

Carbonate  equilibria.  Because  of  their  general  importance  to  bio- 
chemistry and  general  chemistry,  equilibria  in  carbonate  and  bicarbonate 
solutions  deserve  special  mention.  The  following  treatment  is  necessarily 
brief. 

When  carbon  dioxide  dissolves  in  water  it  presumably  is  present  both 
as  anhydrous  C02  and  as  the  hydrate  H2C03,  carbonic  acid.  For  a  dis- 
cussion of  the  rate  of  hydration  and  proportions  of  the  forms,  see  experi- 
ments and  references  by  Buytendijk,  Brinkman  and  Mook  (1927).*  Ana- 
lytical methods  do  not  ordinarily  distinguish  the  two  forms,  and,  since  the 
sum  of  the  two  is  generally  the  more  important  quantity,  we  may  write  the 
equilibrium  equation  for  the  relation  between  a  partial  pressure,  P  (atmos- 
pheres) of  gaseous  carbon  dioxid  and  the  dissolved  carbon  dioxid  as  follows  : 


[CO,]  +  [H2C03]  =  [free  CO2]  =  Ko'P  (a) 

In  the  presence  of  bases  we  still  have  the  above  relation  holding  between 
the  partial  pressure  and  that  portion  of  the  total  CO2  which  remains  un- 
combined.  However,  variation  in  the  composition  of  the  solution  will 
vary  the  magnitude  of  KQ.  Dissolved  CO2  reacts  with  water  and  since 
[H2O]  may  be  regarded  as  constant  we  have  the  equilibrium  equation 


[OCM  =^+l  (b) 


[H2C03]  [H2C03] 

The  H2CO3  dissociates  in  steps  and  for  the  first  step  the  equilibrium 
condition  is: 

[HC031 


Combining  equations  (b)  and  (c)  and  collecting  constants  we  have 

[H 


[COJ  +  [H2C03] 

or  using  the  convention  mentioned  above 

[H+]  [HC031 
[free  CO  j     ~ 


(d) 


Cf.  Faurholt  (1924). 


562  THE    DETERMINATION    OF    HYDROGEN    IONS 

The  constant  K/  is  sometimes  called  the  first  dissociation  constant  of 
carbonic  acid.  It  is  not  strictly  so  but  is  rather  of  the  nature  of  an  "ap- 
parent dissociation  constant."  Ki'  is  more  useful  than  the  true  dissocia- 
tion constant  but  is  probably  much  smaller. 

For  the  second  stage  of  dissociation  the  equilibrium  condition  is: 

[H 


For  simplicity  the  above  equations  were  stated  in  terms  of  concentra- 
tions, as  is  permissible  for  ideal  conditions,  for  a  limited  range  of  con- 
ditions or  for  limiting  equations.  Equations  (a),  (d)  and  (e)  may  now  be 
restated  with  correction  terms  or  with  activities. 

[free  C02]To  =  (free  C02)  =  K0P  (f) 

(H+)  [HCO^]  71        (H+)  (HCOp 


Ki  (g) 

K2  (h) 


(free  C02)  (free  CO2) 

(H+)  [C03— ]  72  _  (H+)  'CO,"") 
(HC03)  (HCO~) 

The  relation 

[free  CO2]  =  —  P 

7o 

may  be  assumed  to  be  subject  to  use  with  solutions  containing  no  free 
base  which  would  form  appreciable  amounts  of  bicarbonate  and  carbonate 

T£- 

ions.    Values  of — -for  solutions  of  sodium  chloride  are  given  by  Johnston 

7o 

(1915)  from  the  data  of  Bohr. 
Concentration  of 

NaCl,  molar...  0.0         0.1          0.2         0.3         0.5          1.0 
jr 

— at25° 0.0338    0.0329    0.0321    0.0314    0.0300    0.0270 

7o 

See  also  Walker,  Bray  and  Johnston  (1927). 

Randall' and  Failey  (1927)  tabulate  values  of  y0  at  15°  and  25°  for 
various  ionic  strengths,  using,  however,  molality  as  the  basis  of  calcula- 
tion. Their  equation  is 

KP 

Molality  of  CO2  =  — 
7 


XXX 


CAKBONATES 


563 


In  water  the  solubility  of  C02  is  0.0478  molal  at  15°  and  0.0370  molal  at 
25°.    Representative  values  of  7  at  25°  are: 


SALT 

M 

7 

KC1  1 

0.508 

1.072 

HC1  1 

1.031 
0.505 

1.143 
1.015 

2.080 

0.998 

See  also  section  on  "Blood,"  and  papers  by  Van  Slyke  and  Neill  (1924) 
and  Van  Slyke  and  Sendroy  (1927)  for  details  of  manometric  measurement 
of  CO 2  extracted  from  solutions. 

TABLE  70 

Values  of  log  <f>  interpolated  at  a  series  of  ionic  strengths 
(After  Walker,  Bray  and  Johnston,  1927) 


A« 

25° 

BASE 

37° 

BASE 

<p25/<p37 

K 

Na 

Li 

K 

Na 

Li 

0.00 

2.491 

2.491 

2.491 

2.296 

2.292 

2.296 

1.57 

0.01 

2.403 

2.400 

2.396 

2.205 

2.204 

2.200 

1.57 

0.02 

2.376 

2.371 

2.362 

2.177 

2.174 

2.165 

1.58 

0.04 

2.342 

2.334 

2.318 

2.142 

2.135 

2.118 

1.59 

0.06 

2.319 

2.308 

2.286 

2.118 

2.106 

2.084 

1.59 

0.08 

2.300 

2.286 

2.260 

2.096 

2.082 

2.055 

1.60 

0.10 

2.286 

2.267 

2.238 

2.079 

2.060 

2.031 

1.61 

0.20 

2.236 

2.194 

2.160 

2.015 

1.980 

1.952 

1.64 

0.40 

2.186 

2.100 

1.871 

0.60 

2.158 

2.034 

1.828 

0.80 

2.139 

1.982 

1.0 

2.122 

1.939 

1.5 

2.098 

1.860 

2.0 

2.085 

1.802 

2.5 

2.074 

1.753 

Combination  of  equations  (f)  and  (g)  gives 

pH  -  log  [HC03-]  +  log  KoP  =  pKi  +  log  71  (i) 

The  quantities  on  the  left  are  determinable  if  [HCO3~]  is  regarded  equal, 
for  instance,  to  [NaHCO3]. 

Hastings  and  Sendroy  (1925)  find  that  pK,  at  38°  is  6.33  and  log  71  = 
Hence,  if  we  let  pKi'  =  pKi  +  log  71 


6.33  - 


564 


THE    DETERMINATION    OF   HYDROGEN   IONS 


Likewise  they  find  at  38  °C. 

pKY  =  pK2  +  log  72  =  10.22  -  1.1  V~ 

By  combining  several  activity  coefficients  and  the  first  and  second  dis- 
sociation constants,  Walker,  Bray  and  Johnston  (1927)  derive: 


[C03-]P 

They  tabulate  the  values  of  log  <p  at  a  series  of  ionic  strengths  and  at  25° 
and  37°C.  See  table  70. 

"This  table  enables  one  to  calculate  the  concentration  of  bicarbonate 
and  of  carbonate  in  any  solution  in  equilibrium  with  the  partial  pressure 
P  (atm.)  of  carbon  dioxide,  provided  the  total  alkali  associated  with  both 
carbonate  and  bicarbonate  is  known;  or  conversely,  to  compute  the  equi- 
librium pressure." 


FIG.  97.  RELATION  OF  PAKTIAL  PRESSURE  OF  CO2  IN  (ATMOSPHERES)  TO 
PER  CENT  Na2CO3  IN  CARBONATE-BICARBONATE  MIXTURE 

As  an  illustration  there  are  given  in  figure  97  the  pressures  of  CO2  over 
a  solution  in  one  case  0.1  molal  with  respect  to  [Na2CO3]  +  [NaHCO3], 
and  in  the  other  case  0.01  molal  with  respect  to  the  same  sum,  when  the 
per  cent  of  [Na2CO3]  is  changed.  The  CO2  partial  pressure  of  our  atmos- 
phere is  about  0.0003  atmosphere.  The  figure  shows  that  the  0.01  M 
solution  will  absorb  CO2  when  [Na2C03l  is  over  10  per  cent  while  the  0.1  M 
solution  will  absorb  CO2  when  [Na2C03]  is  over  50  per  cent. 

Equations  (f),   (g)  and  (h)  give 


K, 


Kg  P 


(H+)« 

The  equilibrium  for  the  dissociation  of  calcium  carbonate  is : 

(CO")  (Ca++) 
(CaC03) 


XXX  SPECIAL   APPLICATIONS,    C  565 

If  (CaCO3)  is  maintained  constant  by  the  presence  of  the  solid  phase 

(CO,-)  (Ca++)  =  K. 
where  K8  is  the  solubility  product,  or 

K8  (H+)2 

=  • 

-T7-       T7"       -rr      T) 

JtVo  IVl   -IA.2  -t 

Thus  the  activity  (or  concentration)  of  calcium  in  a  solution  in  contact 
with  CaCO3  is  a  function  of  the  hydrion  activity  and  CO2  partial  pressure. 
This  relation  is  of  importance  in  geology  as  well  as  in  biochemistry.  See 
Hastings  et  al.  (1927),  and  an  application  by  Atkins  (1922). 

An  interesting  discussion  of  the  importance  of  carbonate  equilibria  to 
life  is  given  by  Henderson  in  The  Fitness  of  the  Environment. 

Catalysis.    See  Chapter  XXVI. 

Colloid  chemistry.  S0rensen,  in  the  introduction  to  his  1917  paper, 
Studies  on  Proteins,  discusses  the  significance  to  colloid  chemistry  of 
careful  studies  of  acid-base  equilibria  in  protein  solutions.  Michaelis,  in 
The  Effects  of  Ions  in  Colloid  Systems,  discusses  several  aspects,  especially 
adsorption.  Rideal  (1926)  gives  brief  treatments  of  many  of  the  funda- 
mental principles  concerned. 

There  exists,  in  one  school,  a  rather  strange  prejudice  against  attempts 
to  make  the  methods  of  acid-base  equilibrium  studies  yield  what  they  are 
capable  of  yielding.  This  has  doubtless  been  due  in  some  measure  to  the 
disposition  of  another  school  to  push  the  signal  triumphs  beyond  clear 
accomplishment.  The  resulting  confusion  makes  it  impossible  to  give  a 
fair  statement  even  of  the  chief  topics.  The  student  will  do  well  to  culti- 
vate ability  to  detect  extremes  of  statement.  He  should  know  that  in- 
numerable investigators  are  proceeding,  oblivious  to  controversies,  to 
make  the  methods  of  hydrion  control  and  measurement  yield  results  of 
immediate  practical  and  theoretical  interest. 

Reference  to  the  role  of  hydrion  concentration  will  be  found  in  such 
general  texts  as  those  of:  Freundlich  (1922-1927),  Bogue  (1924),  Colloid 
Symposium  Monographs  (1922-date). 

Crystallization.  In  the  crystallization  of  ampholytes,  acids  and  bases, 
it  is  common  practice  to  adjust  the  hydrion  concentration  of  the  solution 
to  the  point  of  incipient  precipitation.  See  for  instance  the  crystalliza- 
tion of  egg  albumin  (S0rensen  (1917)  and  of  insulin  (Abel,  et  al.  (1927)). 

Dr.  Edgar  T.  Wherry  calls  my  attention  to  the  fact  that  it  has  long  been 
known  that  the  acidity  of  a  solution  may  have  some  bearing  on  the  habit 
of  the  crystals  separating  from  it.  Alum  crystals  are  octahedral  when 
deposited  from  strongly  acid  solutions,  cubic  when  the  acidity  is  reduced  ; 
sodium  chloride  is  reported  to  show  the  reverse.  (See  Tertsch,  1926.) 
Thus  far,  however,  only  qualitative  information  is  available,  and  the  pH 
values  at  which  habit-changes  become  significant  remain  to  be  determined. 
This  may  have  technical  bearings.  See  Saylor  (1928). 


566  THE    DETERMINATION   OF  HYDKOGEN   IONS 

Digestive  system.  The  digestive  tract  is  primarily  the  channel  for  the 
intense  activity  of  hydrolytic  enzymes  and  as  such  is  provided  with  mech- 
anisms for  the  establishment  of  hydrogen  ion  concentrations  favorable  to 
these  enzymes.  Hydrogen  electrode  methods  have  correlated  the  regional 
activity  of  particular  enzymes  with  the  reactions  there  found,  have  clarified 
some  of  the  differences  between  the  digestive  processes  of  infancy  and 
adult  life,  aided  in  attempts  to  explain  the  formation  of  acid  and  alkali 
and  have  been  of  service  in  the  improvement  of  clinical  methods  for  the 
assay  of  pepsin  activity  and  the  diagnosis  of  abnormal  secretion  of  hydro- 
chloric acid  in  the  stomach.  The  control  of  specific  physiological  func- 
tions such  as  secretion  of  conditioning  agents,  permeabilities,  and  activities 
of  the  varied  musculature,  as  well  as  investigations  upon  the  condition  in 
the  digestive  tract  of  substances  such  as  calcium  and  phosphate  are  sub- 
jects which  have  been  discussed.  Shohl  and  King  (1920)  and  Kahn  and 
Stokes  (1926)  have  reviewed  and  improved  methods  of  studying  gastric 
acidity.  Some  of  the  problems  of  gastric  acidity  have  been  reviewed  by 
Michaelis  (1927).  Schwarz  et  al.  (1924)  and  McClendon  et  al.  have  re- 
viewed several  aspects  of  digestion.  For  references  on  saliva  see  G. 
Clark  and  Carter  (1927).  As  two  of  many  examples  of  studies  on  lower 
animals  see  Yonge  (1925),  Redman  et  al.  (1927). 

Distribution  coefficients.  Imagine  two  phases  in  contact,  e.g.,  water 
and  benzene,  and  neglect  the  complexities  due  to  the  solubility  of  the 
substance  of  one  phase  in  the  other.  Dissolve  in  either  phase  a  substance 
A,  and  let  it  distribute  itself  between  the  two  phases.  Actually,  or  in 
imagination,  let  the  substance  A  enter  a  vapor  phase  and  assume  Henry's 
law  for  the  distribution  between  each  of  the  solvents  and  the  vapor  phase 
where  the  partial  pressure  of  A  is  P. 

[A]w  =  kzP  (a) 

[A]b  =  k2P  (b) 

By  (a)  and  (b) 

[AIw       k: 

FTP  =  r-  =  -K-d  (c) 

[A]b       k2 

The  ratio  r—r^  should  then  be  constant  and  independent  of  that  concentra- 


tion  in  either  phase  which  is  proportional  to  P.    Kd  is  the  so-called  distri- 
bution coefficient. 

Now  let  A  be  an  acid,  HA,  and  assume 

1)  lonization  in  the  water-phase 

HA  ^  H+  +  A 

2)  The  equilibrium 

[H+]w  [A]w 


XXX  SPECIAL   APPLICATIONS,    D  567 

3)  The  summation  for  the  aqueous  phase 

[S]w  =  [AJW  +  [HAJW  (e) 

4)  The  distribution  of  molecules. 

[HA1W 
[lA]T    Kd 

Equations  (d),  (e)  and  (f)  yield  (g) 

[S]w  [H+]w 
[HA]b  =  (g) 


If  Ka  be  so  small  as  to  be  negligible  in  the  sum  (Ka  +  [H+]w),  we  have  (h) 

[HAJb  =  ^  (h) 

If  [H+]w  =  Ka  we  have  (i) 

[HAJb  =  ~  (0 

If  [H+]w  be  so  small  as  to  be  negligible  in  the  sum  (Ka  +  [H+]w),  we 
have  (j) 

rcn      rcr+i 

(J) 

When[H+]w  is  very  small  relative  to  KdKa,  [HA]b  is  very  small  relative 
to  [Slw. 

These  approximate  relations  formulate  one  of  the  most  common  of 
laboratory  practices;  namely,  the  extraction  of  organic  acids  from  water 
solutions  by  means  of  organic  solvents.  Acidification  of  the  aqueous 
phase  to  form  the  undissociated  molecules  from  the  salts  may  bring  about 
an  enormous  increase  in  the  concentration  of  the  substance  in  the  non- 
aqueous  phase.  Change  of  [H+]  from  [H+]  =  Ka  to  practically  complete 
suppression  of  ionization  doubles  the  relative  concentration. 

In  case  the  dissociation  constants  of  two  acids  are  of  very  different 
orders  of  magnitude,  a  fractional  separation  can  be  accomplished  by 
adjusting  the  hydrion  concentration  to  a  value  between  those  of  the  two 
dissociation  constants. 

The  strict  application  of  the  principle  briefly  outlined  is  frequently 
complicated  by  association  of  molecules  in  one  phase,  by  considerable 
departures  from  Henry's  law,  etc.  See  further  detail  by  Hill,  p.  343 
Taylor's  Treatise  on  Physical  Chemistry,  and  Murray  (1923). 

Donnan  equilibria.  An  elementary  example  only  will  be  given  to  il- 
lustrate a  principle  implicit  in  Gibbs'  treatment  of  equilibria  but  brought 


568 


THE    DETERMINATION    OF    HYDROGEN    IONS 


into  prominence  by  the  important  work  of  Donnan  (1911)  and  Donnan 
and  Harris  (1911). 

Imagine  a  membrane,  M,  on  one  side  of  which  there  is  an  aqueous  solu- 
tion of  hydrochloric  acid  and  on  the  other  side  of  which  there  is  not  only 
hydrochloric  acid  but  an  acid  HR  neither  the  undissociated  molecule  nor 
the  anion  of  which  can  penetrate  the  membrane. 


inside" 

[H+] 

[C1-] 

[HR] 
[R-] 


M 


"outside" 
[H+]0 


The  presence  of  R~~  upon  one  side  only  will  tend  to  produce  asym- 
metry of  electric  charge  on  opposite  sides  of  the  membrane,  and  there  will 
be  a  tendency  toward  the  compensation  of  this  both  by  redistribution  of 
the  diffusible  ions  and  readjustment  of  the  ionization  of  the  HR:  R~ 
system.  Also  the  presence  of  HR  and  R~~  upon  one  side  only  tends  to 
diminish  the  partial  molal  free  energy  of  the  solvent.  This  will  tend  to 
be  compensated  by  a  movement  of  water  which  may  occur  until,  at  equilib- 
brium,  the  counter  hydrostatic  pressure  has  contributed  its  part  to  the 
balancing. 

To  simplify  the  elementary  discussion,  assume  that  the  species  HR 
and  R~  have  so  little  effect  on  "osmotic  pressure"  that  their  contribution 
to  this  effect  may  be  neglected.  Also  assume  that  the  solutions  are  suffi- 
ciently near  "ideal"  to  permit  the  use  of  concentrations  rather  than 
activities.1 

Imagine  in  each  solution  a  hydrogen  electrode  under  one  atmosphere 
pressure  of  hydrogen.  The  E.  M.  F.  of  this  gas-cell  will  be  determined  in 
part  by  the  ratio  of  the  hydrion  concentrations  on  the  two  sides  and  in 
part  by  the  potential  difference  EM  across  the  membrane. 


We  may  also  imagine  two  chloride  electrodes. 

•prp  r/->n_i 

Kl   ,     IL/1  Jo    . 


For  this  cell 


"M 


1  An  entanglement  might  occur  in  the  use  of  activities  were  the  electro- 
static constraint  neglected  in  applying  the  definition  that  the  activities 
of  a  substance  in  two  phases  are  the  same  when  the  substance  will  not  of 
itself  pass  from  one  phase  to  the  other. 


XXX 


BONN  AN   EQUILIBRIA 


569 


But  if  the  system  as  a  whole  has  attained  equilibrium,  no  work  can  be 
obtained  by  transfer  of  either  hydrions  or  chloride  ions  and  E.  M.  F.  =0 
in  each  case.  Then,  since  EM  is  the  same, 

[H+h        [Cl-]o 


[H+]o       [Cl-]i 

In  general  the  ratio  of  the  concentration  of  an  anion  in  the  "outside" 
solution  to  the  concentration  of  that  anion  in  the  "inside"  solution  is  the 
same  as  the  ratio  of  the  concentrations  of  any  other  anion  "outside"  and 
"inside"  and  is  inversely  proportional  to  the  ratio  of  "outside"  and 
"inside"  concentrations  of  any  cation. 

Although  asymmetry  in  the  distribution  of  ions  was  supposed  to  be 
the  origin  of  the  membrane  potential-difference,  a  considerable  potential 
difference  may  be  caused  by  such  a  small  inequality  of  material  that  we 
may  still  assume  the  ordinary  rule  of  electroneutrality  in  each  solution. 
Then  on  one  side  (inside) 


Also  outside 


=  [H+Ji 


[Cl-]o 


(b) 

(c) 


Substitute  the  equivalents  of  [Cl  Ji  and  [Cl  J0  from  (b)  and  (c)  in  equation 
(a)  and  obtain 

1H+]2  -  [H+]i  [R-Ji    =  [H+]J  (d) 

If,  then,  the  "outside"  and  "inside"  solutions  before  the  attainment 
of  equilibrium  were  of  the  same  hydrion  concentration,  hydrions  would 
diffuse  inward  for  the  hydrion  concentration  of  the  inside  solution  will  be 
greater  than  that  of  the  outside  solution  at  equilibrium.  (A  quantity 
must  be  subtracted  from  [H+]?  in  (d)  to  equal  [H*]2.) 

If  the  non-diffusible  substance  were  an  ampholyte,  forming  R+  on  the 
acid  side  of  the  isoelectric  point,  the  above  relations  regarding  [H+]j  and 
[H+]0  would  be  reversed  on  the  acid  side  of  the  isoelectric  point. 

To  indicate  the  magnitude  of  migrations  with  no  chloride  inside  initially, 
assume  that  the  membrane  is  placed  so  that  the  two  solutions  are  of  equal 
volume.  Between  the  initial  and  final  states  of  the  system  chloride  ions 
have  diffused  from  right  to  left  (see  scheme  below)  till  the  concentration 
[C1-],  is  x. 


Initial  state 


Equilibrium  state  [HR]3 
[R-]3 
[H+]3 


M 


M 


[C1-], 
[H+]2 


570 

Then 


THE  DETERMINATION  OF  HYDROGEN  IONS 


[H+]8  =  [H+]i  +  x  and  [H+]4  =  [H+]2  -  x 
or,  since  at  equilibrium 

[H+]3    =    [Cl-]4 

[H+]4       [01-],' 


[H+h  +  x  =  [H+]2  -  x 
[H+]2  -  x  "  x 


Whence 


x  = 


21H- 


The  following  table  will  give  an  idea  of  the  magnitude  of  the  effects  due 
to  the  conditions  assumed. 

As  we  have  already  indicated,  the  difference  of  potential  between  two 
hydrogen  electrodes  placed  on  opposite  sides  of  the  membrane  must,  at 
the  equilibrium  state  of  the  system,  be  equal  and  opposite  to  the  potential 
difference  at  the  membrane.  Hence  the  membrane  potential  difference 
may  be  expressed  in  terms  of  a  hydrogen  electrode  gas  chain : 

RT.    |H+la 

F  in[H+i; 

By  using  this  relation  we  calculate  the  membrane  potential  difference 
given  in  millivolts  in  the  last  column  of  the  following  table. 


«.„,, 

n 

INITIAL  RATIO 

PER  CENT  HC1 
DIFFUSED  TO 
ESTABLISH 
EQUILIBRIUM 

EQUILIBRIUM 
DISTRIBUTION 

RATIO  |  —  ^|* 

MEMBRANE 
POTENTIAL  IN 
MILLIVOLTS 

0.01 

1.0 

0.01 

49.8 

1.01 

-    0.3 

1.0 

1.0 

1.0 

33.3 

2.0 

-  18.0 

1.0 

0.01 

100.0 

0.98 

101.0 

-120.0 

Of  course  the  conditions  assumed  for  purposes  of  illustration  are  ex- 
tremely simple  but  they  suffice  to  indicate  the  nature  of  relations  of  very 
great  importance  in  the  physiology  of  the  living  cell. 

The  equations  should  be  used  with  activities  if  strictly  applied. 

For  one  of  many  illustrations  of  the  application,  see  Van  Slyke  (1926). 

Ecology.  Cells  living  in  intimate  contact  with  an  aqueous  solution  are 
found  to  be  dependent  in  various  degree  and  various  manner  upon  the 
hydrion  concentration  of  the  solution.  See  the  manifold  aspects  il- 
lustrated by  the  texts  of  references  under  Bacteriology. 


XXX  ELECTROPHORESIS  571 

Likewise  organisms  drawing  sustenance  from  the  soil  are  found  to  be 
dependent  upon  the  "soil  reaction"  as  determined  by  measurements  of 
aqueous  extracts.  See  Soils.  The  more  complex  multicellular  organisms 
may  in  some  instances  respond  directly  to  the  hydrion  concentration  of 
the  environment  but  more  often  they  are  indirectly  affected  through  the 
effects  upon  organized  and  unorganized  foodstuffs.  Through  this  complex 
chain,  the  distribution  of  the  higher  forms  of  life  exhibits  a  considerable 
degree  of  correlation  with  the  pH  values  of  the  natural  waters  or  soils 
with  which  they  are  associated. 

The  literature  on  reaction  as  an  ecological  factor  has  now  reached  con- 
siderable bulk,  and  only  a  few  typical  articles  can  be  noted  here:  Fungi, 
Waksman  (1924);  Marine  Algae,  Legendre  (1925);  Fresh  Water  Algae, 
Wehrle  (1927) ;  Liverworts,  Dop  and  Chalaud  (1926) ;  Ferns,  Wherry  (1920- 
1921);  Coniferous  trees,  Hesselman  (1926);  Higher  plants,  O.  Arrhenius 
(1920),  Atkins  (1922),  Wherry  (1920),  Olsen  (1923),  Chodat  (1924),  Christo- 
phersen  (1925);  Earthworms,  O,  Arrhenius  (1921);  Snails,  Atkins  and 
Lebour  (1923) ;  and  Fish,  Coker  (1925) .  See  especially  the  book  by  Mevius 
(1927). 

Electrophoresis  (cataphoresis)  and  electro-osmosis.  An  electrically 
charged  body  placed  between  an  anode  and  a  cathode  will  tend  to  move 
toward  the  pole  having  a  charge  opposite  in  sign  to  the  charge  on  the 
body.  If  the  body  is  a  simple  ion,  the  movement  is  called  ionic  migration. 
If  the  body  is  a  particle  suspended  in  a  medium  such  as  water,  the  move- 
ment is  called  electrophoresis.  More  generally  it  is  known  as  cataphoresis. 
The  distinction  between  ionic  migration  and  electrophoresis  is  not  always 
clear  in  the  case  of  material  in  the  colloidal  state. 

We  shall  not  discuss  the  various  theories  advanced  to  account  for  the 
experimental  facts  but  shall  treat  briefly  only  that  point  of  view  which 
it  will  be  profitable  to  investigate  further  with  the  aid  of  methods  for 
determining  pH. 

Since  acidic  or  basic  ionization  may  determine  the  sign  of  the  charge 
upon  a  body  of  amphoteric  nature  the  sign  may  be  a  function  of  the  pH 
of  the  medium.  The  direction  of  electrophoresis  is  then  a  function  of  pH. 
At  the  isoelectric  point  electrophoresis  is  a  minimum.  The  method  of 
electrophoresis  is  useful  in  determining  isoelectric  points. 

There  can  be  no  movement  such  as  that  noted  above  without  a  recip- 
rocal interaction  between  suspended  or  dissolved  material  and  the  dis- 
persing medium.  If  then  the  charged  particles  are  fixed  in  position,  as 
in  the  form  of  a  porous  diaphragm,  are  placed  in  water  and  the  whole 
subjected  to  a  potential  gradient,  the  water  will  tend  to  move  (electro- 
osmosis).  The  same  relative  relations  indicated  above  then  hold.  If  the 
diaphragm  is  of  an  amphoteric  nature  the  direction  of  water  flow  will 
depend  upon  the  acidic  and  basic  properties  of  the  diaphragm  and  upon 
pH  of  the  aqueous  phase. 

In  either  one  of  the  two  cases  (particles  fixed  or  free  to  move)  the  same 
end  result  will  be  obtained  if  the  particles  adsorb  hydrogen  and  hydroxyl 
ions  according  to  their  adsorption  isotherms.  Equality  of  adsorption 


572 


THE    DETERMINATION    OF   HYDROGEN   IONS 


TABLE  71 

Optimal  reactions  for  the  activity  of  various  enzymes 
(After  Waksman  and  Davison,  1926) 


ENZYME 

SOURCE 

OPTIMAL  pH 

Amylase  (diastase)  —  < 
Arginase 

Asp.  niger 
Duodenal     contents 
(infants) 
Malt 
Pancreas 
Potato  juice 
Saliva 

Liver 

3.5-5.5 
6.0-8.0  (viscosity) 

4.4-4.5 
7.0 
6.0-7.0 
5.6  (acetate  buffer) 
6.6  (phosphate  buffer) 
10  0 

Carboxylase  

Yeast 

53-62 

Catalase  < 
Emulsin 

Blood 
Liver 

Vegetables 

7.5  (10  minutes) 
7.0 
7.0-10.0 
4  4 

Erepsin  \ 

Intestine  (pig) 
Intestine  (pig) 

7.9  (glycyl-glycin) 
8.6  (conductivity 
method) 

Invertase.  . 

Intestine  (dog) 
Ox  spleen 
Yeast 
Asp.  niger 
Potato  juice 
Yeast 

7.7  (albumose) 
7.5-8.5 
7.8 
2.5-3.5 
4.0-5.0 
4  4-4  6  (52  1°C  ) 

Lipase  \ 

Yeast 
Fresh  yeast  cells 
Blood 
Duodenal  juice 
Duodenal  juice 

4.2  (22.3°C.) 
4.2-5.2 

7.8-8.6 
5.0 
8.5 

Maltase 

Gastric  juice 
Gastric  juice  of  dog 
Serum 
Asp.  oryzae 

4.0-5.0 
4.9  (2.5  to  8.0) 
7.0-8.6 
3.0  (35.5°C.)-7.2  (47°C.) 
4  0 

Oxidase 

Beer  yeast 
Vegetables 

6.6 
7  0-10  0 

Pancreatin    (trypsin- 
erepsin)  

Ox  pancreas 
Ox  pancreas 

9.7        (gelatin       liquef. 
37°C.) 
7  7_g  o      (peptone      de- 

Pectase  

Fruit 

comp.) 
4  3 

XXX 


ENZYMES 


573 


TABLE  71- Concluded 


ENZYME 

SOURCE 

OPTIMAL  pH 

Pepsin  J 
Peroxidase 

Animal  tissues 
Stomach 
Stomach 
Yeast 
Vegetables 

3.0-3.5  (gelatin) 
1.2-1.6  (acid  albumin) 
1.4  (edestin) 
4.0-4.5 
7  0-10  0 

Protease                          < 

Asp.  oryzae 
Autolyzing      animal 
tissue 

5.1 
4.5 

6n  7  n 

Rennet  (lab)  / 

Malt 
Malignant       human 
and  rat  tumors 
Papain 
Stomach 

.  u—  /  .  u 
3.7-4.2 
7.0 

5.0-7.0 
5.0 

Trypsin                            < 

Stomach 
Animal  tissues 
Pancreas 
Pancreas 

6.0-6.4 
7.8  (peptone) 
9.5 
8.3  (casein) 

Urease  

Pancreas 
Yeast 
Yeast 
Soy  bean 

7.5-8.3  (fibrin) 
7.0  (peptone) 
8.0 
About  7  0 

Zymase  J 

Living  yeast 

4.5-5.5  (28°C.,  no  nitro- 
gen) 

Living  yeast 

4.5-6.5       (28°C.,      plus 
yeast  water) 

and  consequently  equality  of  electrical  charge  is  attained  at  a  definite 
pH  value.  The  position  of  such  an  "isoelectric"  point  is  a  function  of 
the  properties  of  the  material  and  may  lie  anywhere  along  the  pH  scale 
(according  to  the  nature  of  the  material)  with  a  narrow  or  broad  isoelectric 
zone . 

See,  for  examples,  Gyemant  (1921),  Michaelis  and  Perlzweig  (1926), 
Northrop  and  De  Kruif  (1921-1922),  Winslow,  and  Falk,  and  Caulfield 
(1923),  Porter  (1921). 

Enzymes.  The  influence  of  hydrogen  ion  concentration,  or  activity, 
upon  the  properties  of  enzymes  has  been  the  subject  of  an  enormous  num- 
ber of  investigations  since  the  classic  paper  of  S0rensen  (1909).  Data 
pertaining  to  specific  enzymes  may  be  traced  through  the  comprehensive 
treatise,  Die  Fermente  edited  by  Oppenheimer.  This  is  now  (1928)  appear- 
ing in  sections.  A  discussion  of  enzymes  as  electrolytes  and  as  colloids 
is  found  in  Chemie  der  Enzyme  I,  3  aufl.  by  v.  Euler  (1925)  see  also  Fodor 


574         THE  DETERMINATION  OF  HYDROGEN  IONS 

(1926),  Rona  (1926),  and  in  Waksman  and  Davison's  Enzymes  (1926). 
See  also  K.  G.  Falk  (1924).  Table  71  is  part  of  that  compiled  by 
Waksman  and  Davison,  whose  book  should  be  consulted  for  references. 

Foods.  Considerable  variation  in  pH  values  of  food  extracts,  juices, 
etc.,  is  of  importance  to  canning  (see  Canning),2  to  thermal  destruction  of 
vitamines  [See  LaMer  (1921),  Sherman  and  Burton  (1926)  and  Zilva  (1923)] 
and  to  numerous  industrial  treatments  of  food-stuffs. 

pH -values  of  various  foods  are  given  by  Bigelow  and  Cathcart  (1921), 
E.  H.  Harvey  (1924). 

The  relative  quantities  of  inorganic  anions  and  cations  and  of  acids 
or  bases  which  can  be  "burned"  to  products  which  can  be  eliminated  by 
the  lungs  or  must  be  eliminated  by  the  kidney  are  important  to  the  study 
of  acid-base  metabolism  and  "neutrality "-regulation.  See  Blatherwick 
(1914). 

Filtration.  Hydrogen  ion  concentration,  through  its  influence  upon  the 
dispersion  of  certain  colloids  and  upon  the  conditioning  of  filter  material, 
may  control  the  filterability  of  a  substance.  Holderer's  thesis  from 
Perrin's  laboratory  presents  in  admirable  form  many  of  the  theoretical 
aspects  of  the  subject.  The  subject  is  not  only  of  considerable  theoretical 
interest  but  also  of  great  practical  importance.  Buffer  control  with  indi- 
cator tests  may  in  many  instances  facilitate  nitrations  upon  an  industrial 
as  well  as  a  laboratory  scale.  See  Electrophoresis. 

Glass,  effect  of,  on  reaction  of  solutions.  Many  glasses  contain  so 
much  "free-alkali"  that  they  can  seriously  affect  the  pH  value  of  poorly 
buffered  solutions,  especially  when  used  as  containers  during  heating. 
See,  as  examples,  Esty  and  Cathcart  (1921),  Fabian  (1921),  fiwe  (19?0). 

Hydrolysis  of  salts.  Inspection  of  several  titration  curves  discussed 
in  previous  chapters  will  show  that,  when  equivalents  of  a  univalent  acid 
and  a  univalent  base  are  mixed,  the  solution  has  a  pH -value  which  is  seldom 
that  of  "neutrality"  and  varies  with  the  salt.  Instead  of  estimating  such 
values  in  the  manner  described  in  Chapter  XXVIII,  it  is  now  desired  to 
treat  the  subject  from  the  following  point  of  view.  The  preformed  salt 
is  used  to  construct  the  solution.  Now  the  reaction  between  an  acid  and 
a  base  is  reversible 

HA  +  BOH  ^±  BA  +  H20 

Consequently,  if  the  preformed  salt,  BA,  be  used,  it  will  react  with  water 
to  some  extent  and  will  form  some  acid,  HA,  and  base,  BOH.  The  conse- 
quent splitting  of  water  is  the  occasion  for  speaking  of  a  hydrolysis. 

The  resulting  acid,  HA,  and  base,  BOH,  ionize.  The  ionization  of  the 
acid  tends  to  increase  the  hydrogen  ion  concentration,  and  the  ionization 
of  the  base  tends  to  increase  the  hydroxyl  ion  concentration.  If  these 
tendencies  are  equal,  the  pH  value  of  the  original  water  will  not  be  altered 
except  through  the  effect  of  the  salt  upon  Kw  (see  page  46).  If  the  acid 
is  "stronger"  than  the  base,  pH  will  be  lessened  and  if  the  base  is  "stronger" 

2  See  page  576. 


XXX 


SPECIAL  APPLICATIONS,    F~H 


575 


than  the  acid,  pH  will  be  increased.     For  detail  return  to  the  method  oi 
Chapter  XXVIII. 

Hydroxides  of  the  metals,  precipitation  of.  See  solubility  product  and 
precipitations.  Were  the  precipitates  formed  from  solutions  of  metal  salts 
by  the  addition  of  strong  alkalies,  true  hydroxides  of  the  type  M(OH)n, 
the  treatment  would  be  simple  and  could  be  illustrated  in  outline  by 
graphs  such  as  that  of  figure  100,  page  582.  There  would  then  be  a  fairly 
narrow  zone  of  pH  within  which  a  metal  hydroxide  having  a  characteristic 
solubility  product  would  be  precipitated.  Undoubtedly  the  simple  rela- 


0       10      20      30      40      50      60      70      80      90      100     110 
CCs  N/IO-NaOH. 

FIG.  98.  BRITTON'S  CURVES  SHOWING  ZONES  OF  PRECIPITATION  OF  METAL 

HYDROXIDES 


tions  then  obtaining  may  be  used  to  outline  one  of  the  chief  aspects  of  the 
problem.  However,  many  of  the  precipitates  carry  down  the  anion,  are 
not  true  hydroxides  and  must  be  regarded  either  as  solid  solutions  or 
treated  by  the  methods  of  colloid  chemistry.  In  a  few  instances  only 
are  there  evidences  of  a  definite  chemical  compound  of  constant  composi- 
tion within  the  zone  of  precipitation  and  before  the  true  hydroxide  is 
formed.  Hence  much  of  the  literature  regarding  definite  "basic  salts" 
must  be  revised.  Britton  (1925)  has  assembled  highly  interesting  pre- 
liminary data  on  the  zones  of  pH  within  which  the  precipitates  are  formed. 
While  it  is  impossible  to  tabulate  extensive  data  here,  there  may  be  repro- 


576  THE   DETERMINATION    OF   HYDROGEN    IONS 

duced  Britton's  set  of  curves  (fig.  98)  showing  the  approximate  location  of 
zones  of  precipitation.  Trace  the  more  specialized  literature  through 
Britton's  references  and  texts  of  analytical  methods. 

Immunity.  Since  substances  concerned  in  immunological  reactions  are 
the  protein  antigens,  are  protein-like  or  are  found  in  solutions  containing 
proteins  on  which  they  are  believed  to  be  adsorbed  or  with  which  they 
are  believed  to  be  in  combination,  pH  control  and  measurement  find  fre- 
quent application  But  the  literature  is  vast  and  the  references  therein 
to  our  subject  are  too  frequent  for  review  A  few  references  will  be  cited 
by  way  of  illustration:  Brooks  (1920),  Coulter  (1920-1922),  Defries  and 
McKinnon  (1926),  DeKruif  and  Northrop  (1922),  A.  Evans  (1922),  Falk  and 
Caulfield  (1923),  Falk  and  Powdermaker  (1925),  Felton  and  Dougherty 
(1924),  Hirsch  (1922-1924),  Homer  (1917),  Mason  (1922),  Michaelis  and 
Davidsohn  (1912),  Mond  (1927),  Shaffer  (1924),  Sobotka  and  Friedlander 
(1928),  Watson  and  Wallace  (1924).  See  also  Wells  (1925). 

Industrial  uses.  The  most  direct  applications  are  in  the  manufacture 
of  salts  such  as  KH2PO4,  titration  of  acids  or  bases  for  yields,  extractions 
as  of  alkaloids  (see  distribution  coefficients)  and  the  control  of  reaction 
rates  and  equilibria.  Processes  in  which  complex  equilibria  are  involved 
are  exemplified  by  the  treatment  of  boiler  water,  see  Greer  and  Parker 
(1926)  and  the  coagulation  processes  of  water  purification,  see  Buswell 
(1927).  Pickling  solutions  are  frequently  put  under  automatic  control. 

The  leather  industry  furnishes  an  example  of  the  application  of  the 
physical  chemistry  of  proteins,  in  the  development  of  which  pH -measure- 
ments have  had  a  leading  part.  See  book  by  Wilson  (1928).  In  the  bread 
industry  pH -control  has  played  an  important  part.  Glutin  is  conditioned 
and  the  activity  of  yeast  and  the  evolution  of  CO2  from  baking  powders 
are  conditioned  by  the  hydrion  concentration  of  the  dough.  Adequate 
pH  control  may  hold  in  check  the  "rope"  organism  (Henderson,  1918) 
and  Cohn  et  al.  See  review  by  S0rensen  (1924).  Cf.,  for  examples,  Green 
and  Bailey  (1927)  and  mill  control  by  Weaver  (1925) . 

As  originally  outlined  in  older  terms  by  Pasteur,  the  "reaction"  of 
wort  and  of  must  have  much  to  do  with  the  brewing  of  beer  and  wine 
fermentation.  The  control  of  "diseases"  of  beer  and  wine  and  the  con- 
ditioning of  the  proteins  held  in  solution  are  controllable  by  pH  methods. 
See  innumerable  journal  articles  on  brewing,  for  example,  Emslander  (1915 
-1919),  Hulton  (1924),  R.  H.  Hopkins  (1925),  N.  Parsons  (1924),  Wind- 
ish,  Dietrich  and  Kolbach  (1922),  and  Ventre's  (1925)  book  on  wine. 

The  gelation  optimum  of  pectin  is  pH  3.0  and  the  optimum  of  pectase 
is  4.3.  For  these  reasons  pH  control  is  important  in  the  manufacture  of 
jellies.  See  for  examples  Tarr  (1923)  and  Luers  and  Lochmuller  (1927). 

Heat-penetration,  temperature,  holding-time  and  the  hydrion  concen- 
tration of  the  food  have  been  so  correlated  with  the  death-rates  of  various 
bacteria  that  economy  and  certainty  in  commercial  canning  of  foods  can 
be  assured.  See  Bigelow  et  al.,  Rogers,  Deysher  and  Evans  (1921). 

The  fermentation  industries  have  continuous  use  for  pH  measurements. 
See  "Bacteriology"  and  "Enzymes." 


XXX  SPECIAL   APPLICATIONS,    I~M  577 

In  the  sizing  of  paper  and  other  processes  of  the  paper  industry  pH 
measurements  are  used.  See  Shaw  (1925),  Atsuki  and  Nakamura  (1927). 

Some  processes  incidental  to  the  textile  industry  in  which  pH  measure- 
ments are  useful  have  been  cited  by  Trotman  (1926),  Sacks  (1927)  and 
Strachan  (1926),  King  (1927). 

Wilson,  Copeland  and  Heisig  (1923)  and  Cobrum  (1927)  give  examples 
of  application  in  sewage  treatment.  See  Buswell  (1927). 

Lyon,  Fron  and  Fournier  (1927)  describe  pH  measurements  as  a  means 
of  judging  wood. 

A  very  active  field  of  application  is  in  the  sugar  industry  where  pH  con- 
trol of  several  steps  has  become  an  established  practice.  Among  in- 
numerable papers  see  Paine  and  Balch  (1927),  Perkins  (1923),  Aten,  van- 
Ginneken  and  Engelhard  (1926),  Blowski  and  Holven  (1925) .  The  methods 
have  been  extended  to  uses  of  sugar  such  as  candy  manufacture,  Sjostrom 
(1922). 

The  potential  at  which  hydrogen  is  deposited  freely  upon  an  electrode 
is  a  function  of  the  hydrogen  ion  concentration  of  the  solution.  Therefore, 
pH  is  important  in  controlling  gassy  deposits  in  electroplating.  In  addi- 
tion it  is  found  that  buffer  solutions,  maintaining  the  pH  within  definite 
limits,  aid  in  the  production  of  desirable  qualities  of  deposits,  especially 
of  nickel.  See  Thompson  (1922),  book  by  Blum  and  Hogaboom  (1924), 
Montillon  and  Cassel  (1924)  and  Britton's  sketch  (1927). 

On  dry  cells  see  Holler  and  Ritchie  (1920). 

In  corrosion  the  activity  of  hydrions  plays  an  important  part.  See 
review  by  Bancroft  (1924)  and  Corrosion  Symposium  (1925). 

To  a  greater  or  lesser  degree  pH  methods  have  been  employed  in  the 
study  of  cements  (Lerch  and  Bogue  (1927);  exchange  silicates,  see  Jenny 
(1927)  and  Sweeney  and  Riley  (1926) ;  commercial  carbons,  see  Hauge  and 
Willaman  (1927),  Miller  (1928);  the  catalytic  decomposition  of  explosives, 
Farmer  (1920),  Angeli  and  Errani  (1920);  rubber  latex,  Freundlich  and 
Hausen  (1925),  Bishop  (1927);  clay,  Fessler  and  Kraner  (1927),  Randolph 
and  Donnenwirth  (1926)  and  Oakley  (1927)  and  innumerable  other  subjects. 

Additional  references  on  several  of  the  subjects  mentioned  above  are  to 
be  found  in  W.  A.  taylor's  (1928)  brochure.  Parker  (1927)  has  noted 
several  instances  where  potentiometric  control  is  used. 

In  innumerable  cases  the  methods  are  applied  to  very  incidental  steps 
of  important  processes.  In  other  cases  acid-base  equilibria  are  funda- 
mental to  a  process.  So  varied  are  the  examples  of  each  type  that  the 
above  sketch  has  little  value  other  than  to  call  attention  to  an  enormous 
field. 

Milk.  A  case  exhibiting  the  tendency  of  physiological  fluids  to  maintain 
constant  ratio  of  dissociated  to  undissociated  forms  of  acids  and  bases. 
Cow's  milk  is  usually  near  pH  =  6.5.  Its  variation  is  used  as  an  index  to 
diseased  condition  of  udder,  or,  in  market  milk,  to  indicate  spoilage. 
Complete  description  of  acid-base  equilibria  of  milk  is  lacking;  cf.  Clark 
(1927).  For  review  of  manifold  applications  of  hydrion-methods  in  dairy 
science,  see  Rogers  (1928). 


578 


THE  DETERMINATION   OF  HYDROGEN   IONS 


Inorganic  chemistry.  Studies  of  inorganic  equilibria  involving  hydrions 
are  too  numerous  to  mention. 

Optical  rotation.  The  specific  rotation  of  an  optically  active  acid, 
base  or  ampholyte  may  be  distinct  from  that  of  its  salt.  Consequently 
the  apparent  specific  rotation  will  vary  as  the  solution  passes  through  a 
zone  of  pH  centered  at  the  pK  value.  See  figure  99.  As  examples  of  many 
studies  which  have  been  made,  see  Liquier  (1925),  Vies  et  al.  (1926),  Levine 
et  al.  (1927). 

Mutarotation,  especially  of  sugar  solutions,  has  long  been  known  to  be 
a  function  of  the  hydrion  concentration  of  the  solution.  See  treatment 
in  modern  terms  by  Br0nsted  and  Guggenheim  (1927),  Lowry  (1927),  Kuhn 
and  Jacob  (1924). 


1 

2 

3 

I 
0-4 

5 
6 

^ 

\ 

V 

^> 

O^JV 

N 

\, 

0.2     Q3      0.4-      0.5      0.6     Q7 

ROTATION.  DEGREES   PER  CM. 

PER  MOLE 

FIG.  99.  ROTATION  OF  POLARIZED  LIGHT  BY  TARTARIC  ACID-TARTARATE 
SOLUTIONS  AS  A  FUNCTION  OF  pH 

(After  Vies  and  Vellinger  (1925)) 

Organic  chemistry.  One  of  the  common  practices  of  organic  chemistry 
is  to  modify  the  properties  of  a  compound  by  substituting  groups  of  acidic 
or  basic  nature  and  of  different  strength  or  by  modifying  the  strength  of 
such  acidic  or  basic  groups  by  the  introduction  of  other  groups  wlr'ch 
themselves  are  not  acidic  or  basic.  And  yet  one  can  search  hundreds  of 
articles  or  their  abstracts  before  coming  upon  mention  of  the  quantitative 
aspect  which  is  susceptible  to  elaboration  by  the  methods  here  described. 
Much  of  the  material  is  assembled  in  texts  on  physical  chemistry.  The 
methods  of  measurement  and  control  are  frequently  practiced  uncon- 
sciously and  as  often  practiced  so  much  as  a  matter  of  course  as  to  seem 
unworthy  of  special  mention. 


XXX  SPECIAL  APPLICATIONS,    I~P  579 

Permeability  of  membranes.  In  some  instances  the  material  of  a  mem- 
brane may  be  conditioned  by  the  hydrion  concentration  of  the  solution 
with  which  it  is  in  contact.  Thereby  its  permeability  in  general  may  be 
altered.  The  question  whether  the  ionized  form  or  the  undissociated  resi- 
due of  a  particular  substance  is  the  form  penetrating  a  given  membrane  is 
now  receiving  considerable  attention.  See,  for  example,  Osterhout 
(1922).  The  participation  of  electrostatic  forces  in  the  distribution  of 
ions  between  solution  phase  and  membrane  phase  is  discussed  in  a  review 
by  Michaelis  (1926).  Weber  (1926)  gives  a  bibliography  1922-1926.  See 
also  book  by  Stiles  (1924). 

Pharmacology,  pharmaceutics,  etc.  Innumerable  applications.  Exam- 
ples : 

1.  The  active  form  of  a  drug  may  be  the  unionized  form.    See  Michaelis 
and  Dernby  (1922),  Dernby  and  Davide  (1922),  Trevan  and  Boock  (1927). 

2.  The  stability  in  solution  may  be  a  function  of  pH.    See  Levy  and 
Cullen  (1920),  Stasiak  (1926),  Tainter  (1926),  Macht  and  Shohl  (1920), 
Plant  Research  Lab.  (1925). 

3.  The  hydrolysis  in  situ  may  be  a  function  of  pH.    See  Shohl  and 
Deming  (1920). 

4.  The  extraction  from  crudes  may  depend  upon  the  partition  coeffi- 
cient of  the  ionized  and   non-ionized  forms.    See  "Distribution  Coeffi- 
cients" and  Fabre  and  Parinaud  (1925),Evers  (1922). 

5.  The  preparation  of  a  drug  for  injection  may  depend  upon  proper 
titration.    See  Elvove  and  Clark  (1924). 

6.  The  control  of  an  organ  used  for  test  is  dependent  on  the  pH  of  the 
fluid.    See  "Physiology"  and,  for  example,  Gruber  (1926). 

See  review  by  Jarisch  (1926)  and  Brunius  and  Karsmark  (1927). 

Photographic  processes.  The  most  general  material  for.  suspending  the 
silver  halides  is  gelatine.  In  the  manufacture  of  gelatine,  pH  control  is 
advantageous.  In  the  preparation  of  the  emulsion,  in  determining  the 
grain-growth  of  the  suspended  silver  halide,  in  affecting  that  decompo- 
sition of  thiourea  derivatives  which  has  to  do  with  sensitizing,  and  in 
preventing  hydrolysis  of  gelatine  and  reduction  of  silver  salts,  pH  control 
is  used.  Swelling  of  gelatine  is  controlled  by  neutral  salts  as  well  as 
bypH. 

Many  of  the  dyes  used  as  optical  sensitizers  are  typical  indicators  and 
only  the  colored  forms  are  effective.  Control  of  pH  on  the  one  hand  and 
adjustment  of  dissociation  constants  on  the  other  hand  have  obvious  uses. 

The  usual  organic  developers  operate  in  alkaline  solution.  The  re- 
duction potentials  of  the  systems  are  functions  of  [H+j.  Reaction  velocity 
and  "fog"  are,  in  part,  controlled  by  preventing  excess  alkalinity. 

If  the  fixing  bath  of  "hypo"  (sodium  thiosulfate)  has  a  pH  value  less 
than  about  4.0,  the  thiosulfate  will  decompose  with  liberation  of  sulfur. 
If  the  pH  value  is  greater  than  6.0,  stains  may  result  from  fixation  of  iron 
compounds  and  reduction  of  silver  by  traces  of  developer.  The  fixing 
bath  is,  therefore,  buffered  in  various  ways. 

"Temporary"  hardening  is  controlled  by  salts  and  the  acidity  of  the 


580         THE  DETERMINATION  OF  HYDROGEN  IONS 

solution.     ''Permanent"  hardening  by  alums  is  similar  to  certain  processes 
of  tanning.     The  hardening  effect  of  alum  is  a  function  of  pH. 

Indicators  for  photographic  processes  must  in  many  cases  show  a  useful 
color  change  in  red  or  yellow  light. 

pH  control  is  used  in  "after  processes,"  e.g.,  intensification  and  reduc- 
tion by  increasing  or  diminishing  the  density  of  the  deposit,  in  the  bleach- 
ing of  the  reversal  process,  in  toning  and  dyeing,  and  in  transfer  processes. 
References:  Rawlings  (1926),  Sheppard  (1925-1926),  Sheppard  and 
Elliott  (1923),  Sheppard,  Elliott  and  Sweet  (1923),  Wightman,  Trivelli 
and  Sheppard  (1923). 

Physiology,  general.  The  classic  examples  of  applications  in  this  field 
are  the  description  of  the  acid-base  equilibria  of  the  blood  (see  "Blood") 
and  the  control  of  enzyme  activities  (see  "Enzymes").  But  it  is  imprac- 
ticable to  enumerate  all  the  other  applications. 

One  of  the  most  important  applications  of  the  principles  discussed  in 
this  book  is  in  the  adjustment  of  physiological  salt  solutions,  perfusion 
solutions,  etc.  Michaelis  (1914)  and  others  have  called  attention  to  the 
fact  that  some  of  the  older  solutions  were  not  adequately  buffered  or 
adjusted.  Improvement  has  been  accomplished  by  the  introduction  of 
phosphate  buffers  or  by  making  use  of  the  equilibria  of  bicarbonate  solu- 
tions under  definite  tensions  of  CO2. 

Among  numerous  papers  on  the  subject  may  be  mentioned  those  by 
A.  C.  Evans  (1922),  Fleisch  (1922),  Barkan,  Broemser  and  Hahn  (1922), 
Chopra  and  Sudhamoy  (1925),  Mason  and  Sanford  (1924),  and  such 
discussions  as  are  found  in  texts,  e.g.,  Bayliss  (1927). 

In  Recent  Advances  in  Physiology  (1926)  Evans  discusses  the  chemistry 
and  physiology  of  muscle  contraction  and  refers  to  the  effect  of  pH  on  the 
recovery  of  muscle.  See  also  McSwiney  and  Newton  (1927)  and  Meyer- 
hof  (1923).  Andrus  and  Carter  (1927)  conclude  that  cardiac  tissue  is 
peculiarly  sensitive  to  alterations  of  hydrion  concentration  and  that  per- 
haps a  difference  of  pH  within  and  without  the  cell  is  a  factor  in  excitation . 
Katz,  Kerridge  and  Long  (1925)  find  the  buffering  capacity  of  cardiac 
muscle  is  lower  than  that  of  skeletal  muscle  and  that  the  critical  level  of 
pH  is  higher  for  the  former.  Evans  (1926)  reviews  the  evidence  relating 
contraction  to  pH  within  and  without  the  cell.  On  the  zones  of  pH  favor- 
able to  the  several  phases  of  heart  action  see  Dale  and  Thacher  (1914). 

Gray  (1922)  finds  that  ciliary  movement  declines  rapidly  as  the  pH  of 
the  solution  is  lowered  from  about  7.2  to  6.0.  Organic  acids  are  more 
effective  because  of  penetration.  See  Jacobs  (1920).  Pantin  (1923)  re- 
views amoeboid  movement.  See  also  Hopkins  (1926)  on  locomotion  of 
protozoa  and  Fenn  (1922),  Feringa  (1923),  and  Jochims  (1927)  on  phago- 
cytosis. Clowes  and  Smith  (1923)  deal  with  the  activity  of  spermatozoa 
in  relation  to  the  hydrion  concentration  of  the  medium.  See  also  Gel- 
horn  (1927),  Kalwaryjski  (1926),  Anderson  (1922),  Healy  (1922)  and  Vies 
(1924) . 

Lillie  and  Shepard  (1923)  find  that  heliotropism  of  arenicola  larvae  is 
controlled  by  changes  in  the  reaction  of  balanced  isotonic  solutions.  See 
also  Rose  (1924). 


XXX  PHYSIOLOGY  581 

Two  important  methods  of  attack  on  various  problems  of  cell  physiol- 
ogy are  provided  by  the  development  on  the  one  hand  of  Harrison's  tissue 
culture  and  on  the  other  hand  of  Barber's  micro  manipulation  methods. 
Lewis  and  Felton  (1922)  and  Fischer  (1921)  describe  the  uses  of  pH  measure- 
ments in  tissue  culture  while  Chambers  (1926-1927)  describes  the  revela- 
tion of  the  pH  of  the  cell  interior  which  has  come  from  the  use  of  his  im- 
proved methods  of  micro-injection.  In  a  recent  paper  Chambers  shows 
that  the  normal  cytoplasmic  pH  of  star  fish  eggs  is  6.7  while  that  of 
the  nucleus  is  7.5.  For  comments  on  the  relation  of  pH  and  reduction 
potentials  of  cell  interior  see  Cohen,  Chambers  and  Reznikoff  (1928) .  The 
influence  of  pH  on  rates  of  reduction  of  methylene  blue  by  tissues  is  dis- 
cussed by  Ahlgren  (1925).  The  metabolism  of  the  developing  egg  with 
reference  to  pH  is  discussed  by  Needham  (1925).  For  notes  on  hen's 
eggs  see  Sharp  and  Whitaker  (1927).  For  references  on  tumor  cells  see 
Warburg  (1926). 

Rous  (1925^1927)  (see  Drury  et  al.  1927)  has  carried  out  an  extensive 
study  of  the  ' 'relative  reaction"  of  living  mammalian  tissues.  But  see 
Chambers.  Mudd  (1925)  reports  the  effect  of  hydrion  concentration  upon 
electroendosmosis  through  mammalian  serous  membranes.  For  a  review 
of  plasmolysis  see  Prdt  (1926),  and  hemolysis,  Mond  (1927),  Rockwood 
(1925). 

The  hydrion  concentration  of  the  medium  is  a  controlling  factor  in  the 
culture  (Morea,  1927,  Saunders,  1924),  growth  and  locomotion  (Hopkins, 
1926)  reproduction  and  encystment  (Beers,  1927,  Koffman,  1924)  of  pro- 
tozoa. Pruthi  (1927)  shows  the  relation  to  protozoan  sequence  in  hay 
infusions.  Shapiro  (1927),  by  feeding  selected  indicators  to  protozoa  was 
able  to  assign  definite  values  to  the  acidity  of  food  vacuoles.  See  Stoll 
(1923)  on  hookworms  and  Jewell  (1920)  on  tadpoles. 

Bodine  (1926)  used  a  micro  electrode  in  studying  the  blood  of  insects. 
See  ' 'Blood"  for  other  references  to  the  blood  of  lower  animals. 

On  body  fluids  see  brief  mention  in  such  texts  as  those  of  Hober  (1927) 
and  Kopacewski  (1926),  comments  on  general  principles  of  exchange  by  Van 
Slyke  (1926) ;  McQuarrie  and  Shohl  (1925)  on  cerebrospinal  fluid;  Talbert 
(1922)  on  sweat,  etc. 

Brief  reviews  of  the  role  of  hydrion  concentration  in  several  other 
phenomena  must  be  sought  in  such  general  texts  as  that  of  Rogers  (1927), 
Hober  (1927),  Bayliss  (1927),  but  more  particularly  in  the  special  literature. 

In  the  field  of  Plant  Physiology  the  applications  have  been  numerous. 
Although  it  is  dufficult  to  separate  subjects  in  this  field  from  those  re- 
ferred to  in  the  sections  "Soils"  and  "Ecology,"  there  may  be  mentioned, 
merely  by  way  of  illustration,  the  following  subjects  and  references: 
Absorption  by  plants :  Robbins  (1926) ;  pH  numbers  of  plant  cells ;  Pfeiffer 
(1927),  Haas  (1917),  Atkins  (1922-1924),  Small  (1926),  Rea  and  Small 
(1927);  pH  gradient:  Gustafsen  (1924);  Photoperiodism :  Garner,  Bacon 
and  Allard  (1924);  Turgor:  Pfeiffer  (1927);  Staining:  Naylor  (1926); 
Chlorosis :  McCall  and  Haag  (1921 ) .  An  excellent  review  of  several  aspects 
of  plant  physiology  in  which  pH  measurements  have  been  used  is  given 


582 


THE  DETERMINATION   OF  HYDROGEN  IONS 


by  Pfeiffer  (1927).  Numerous  investigations  have  been  made  of  the  role 
of  reaction  in  the  defense  against  parasites.  Examples  are:  'Gillespie  and 
Hurst  (1918),  Scott  (1922-1924),  Mclnnes,  J.  (1922),  Berridge  (1924)  and 
Kurd  (1924),  Atkins  (1922). 

Precipitations.  Usually  an  acidic  ionogen  is  less  soluble  than  its  alkali 
salt  and  a  basic  ionogen  is  less  soluble  than  its  chloride.  Figure  100 
illustrates  in  elementary  outline  phenomena  that  may  occur  in  titrating 
the  hydrochloride  of  a  base.  The  abscissa  represents  percentage  neu- 
tralization of  the  hydrochloric  acid  combined  with  the  base.  The  equilib- 
rium is  given  approximately  by: 


(a) 


I 
CL 


20      40       60      80       100 

PERCENT   NEUTRALIZATION 
FIG.  100.  TITRATION  OF  100  cc.  OP  N/100  HYDROCHLORIDE  OF  A  BASE 

(14-Kb  =  4)  WITH  NaOH 
Solubility  of  free  base  2  X  10~3  in  one  case  and  2.2  X  10~2  in  the  other  case 

Accordingly  the  type  curve  is  plotted  with  center  at  pH  =  4.0. 

Suppose  the  solubility  of  the  free  base,  [B],  is  2  X  10~3.     Then  when  the 
solid  form  has  precipitated 


pH  =  4.0  -  2.7  -  log  [BH+]  =  1.3  -  log  [BH+] 


(b) 


If  0.1  M  hydrochloride  of  the  base  has  been  titrated  to  incipient  pre- 
cipitation, [BH+]  =  0.1  -  0.002  =  0.098  (neglecting  dilution).  Hence 
pH  =  2.3  which  is  point  a  of  figure  100.  It  may  be  that  precipitation  will 
not  occur  at  once  and  that  the  solution  will  remain  supersaturated  to 
point  b.  Then,  with  the  formation  of  a  precipitate,  the  pH  value  jumps 
back  to  c.  From  then  on  the  curve  is  determined  by  equation  (b)  ap- 
proximately. 

If  the  solubility  of  the  free  base  is  2.2  X  10~2  precipitation  will  determine 
the  following  equation 


pH  =  4.0  -  1.66  -  log  [BH+]  =  2.34  -  log  [BH 


(c) 


XXX 


SPECIAL  APPLICATIONS,    P 


583 


Then  at  incipient  precipitation  [BH+]  =0.1  -  0.02  =  0.078.  Hence  pH 
=  3.54  approximately.  The  titration  curve  may  continue  to  c  instead  of 
"breaking"  at  d;  but,  with  precipitation,  the  pH  value  will  drop  back  to  f . 

The  above  description  is  approximate,  not  only  because  of  the  neglect 
of  dilution  and  the  use  of  the  first  approximation  equation,  but  particu- 
larly because  the  activities  were  not  used  and  no  consideration  was  given 
to  the  effect  of  ionic  strength  of  the  solution  upon  solubility.  Nevertheless 
the  example  illustrates  how  the  "titration  curve"  is  displaced  to  a  greater 
or  lesser  extent  depending  upon  the  magnitude  of  the  solubility  of  the 
precipitable  component.  It  illustrates  the  flattening  of  the  curve  or  in- 
creased buffer  index  in  a  narrowed  zone.  It  also  illustrates  a  method  of 
determining  solubility. 

Recently  Naegeli  (1926)  has  given  an  extensive  review  of  instances, 
chiefly  from  the  field  of  colloid  chemistry.  He  proposed  to  elevate  to 
the  rank  of  a  new  principle  of  acidimetry  the  employment  of  substances 
which  precipitate  at  low  concentrations  and  at  definite  zones  of  pH.  He 
suggests  in  particular  isonitrosoacetyl-p-amino  azo  benzene  (indicator  a) 
and  isonitrosoacetyl-p-toluoazo-p-toluidine  (indicator  b).  For  these 
Naegeli  finds  the  following  ranges: 


RAl 

?GE 

BUFFER  SOLUTION 

Indicator  a 

Indicator  b 

Borax-NaOH  
Phosphate- 
NaOH 

turbid 
turbid 

10.95-11.01 
10  80-10  90 

clear 
clear 

turbid 
turbid 

11.30-11.36 
11.55-11.63 

clear 
clear 

Glycocol- 
NaOH  .      .     . 

turbid 

10.91-10.98 

clear 

turbid 

11.68-11.74 

clear 

Note  the  extremely  narrow  range.  Since  the  zone  lies  near  those  values 
of  pH  which  are  required  for  the  titration  of  certain  weak  acids  by  strong 
bases  (see  page  535)  Naegeli  had  some  success  in  this  application. 

Proteins.  From  what  is  known  of  their  chemical  structure,  proteins  are 
believed  to  be  amphoteric.  As  such  their  conduct  should  be  subject  to 
the  state  of  the  acid-base  equilibria  of  the  solution  in  which  they  are  dis- 
persed. Because  of  the  high  molecular  weights  of  proteins  and  the  ap- 
parently numerous  groups  which  can  function  as  acids  or  bases,  it  is  im- 
practicable to  formulate  equations  comparable  to  those  of  simple  systems 
and  to  subject  these  to  experimental  test.  For  the  same  reason  experi- 
mental progress  in  developing  analogies  with  the  equilibria  of  simple 
systems  has  required  the  most  painstaking  work.  Such  work  is  well 
exemplified  in  the  classic  papers  of  S0rensen  and  his  coworkers  which  are 
to  be  found  chiefly  in  Compt.  rend.  trav.  lab.  Carlsberg,  1917  to  date. 
Beginning  with  the  work  of  Hardy  (1899-1905),  Loeb  (1909),  Michaelis 
(1909),  Chick  (1913),  Pauli  (1903-date)  and  continuing  through  the  later 


584         THE  DETERMINATION  OF  HYDROGEN  IONS 

work  of  these  same  authors,  and  of  Cohn,  S0rensen  and  numerous  others,  a 
large  body  of  excellent  working  hypotheses  and  fundamental  data  has  been 
accumulated.  See  such  reviews  as  that  of  Cohn  (1925)  and  Lloyd's  book. 
Loeb  reentered  the  field  about  1918.  His  book  (1922)  contains  interesting 
material  more  precisely  formulated  elsewhere. 

As  an  example  of  the  application  of  the  Debye-Htickel  equation  to  pro- 
tein solutions  see  Cohn  and  Prentiss  (1927)  and  S0rensen  and  Linderstr0m- 
Lang  (1927). 

Solubility,  solubility  product.  The  true  solubility  of  a  compound  may 
be  regarded  as  independent  of  the  hydrogen  ion  concentration  of  the  solu- 
tion; but  if  the  compound  is  an  acid,  a  base  or  an  ampholyte,  some  of  the 
material  present  in  solution  may  be  ionized  and  the  apparent  solubility 
will  include  both  the  ionized  and  unionized  forms.  Therefore,  the  total 
or  apparent  solubility  is  a  function  of  pH. 

Since  the  presence  of  extraneous  material  often  has  a  great  influence 
upon  the  true  solubility  of  a  substance  there  is  some  advantage  in  starting 
the  elementary  formulation  with  the  use  of  the  activity-concept. 

When  the  activities  of  a  substance  in  two  phases  are  the  same  the  sub- 
stance will  not  of  itself  pass  from  one  phase  to  the  other.  Let  the  acid 
HA  be  present  in  a  solid  phase  where  the  activity  is  (HA)8. 

(HA)S  =  a  constant  (a) 

The  activity  in  the  liquid  phase  will  be  the  same  at  equilibrium. 

(HA)i  =  (HA).  (b) 

In  the  liquid  phase 

(H+),  (A-), 

(HA),  K" 

or  by  (a),  (b)  and  (c): 

(H+)i  (A)i  =  a  constant  =  Ka  (d) 

The  constant  Ks  is  called  the  solubility  product. 
Introducing  activity  coefficients,  we  have : 

[H+]  [A~]  =  ^—  (e) 

TH+  ?A- 
or 

(H+)  =  ~—,  (e-2) 

TA-  [A-] 

Chapter  XXV  deals  with  the  calculation  of  activity  coefficients  and 
indicates  that  a  first  order  approximation  of  their  evaluation  for  very 
dilute  solutions  has  been  accomplished.  See  figure  86,  page  504.  This 
accounts  for  the  influence  of  neutral  salts  of  various  valence-types  at  high 


XXX  SPECIAL   APPLICATIONS,    S  585 

dilution;  but  in  the  presence  of  high  concentrations  of  salts  and  other 
material  the  distribution  of  water  is  seriously  affected  and  a  "salting  out" 
process  may  be  superimposed.  Inexplicable  effects  such  as  are  observed 
when  an  organic  solvent  is  but  slightly  altered  by  addition  or  withdrawal 
of  a  minute  quantity  of  some  solute  are  often  encountered. 

Soils.  A  water  extract  of  a  soil  will  have  taken  up  acids,  bases  and 
salts  in  ratios  conveniently  described  in  terms  of  pH.  A  narrow  range  of 
pH  values  may  be  determined  by  the  mineral  constituents  of  the  soil 
[see,  for  example,  Kappen  (1916)]  by  the  products  of  leaf  and  wood  de- 
composition [see,  for  example,  Od6n  (1916)],  by  material  excreted  by  plant 
roots  [see,  for  example,  Duggar  (1920),  Davidson  and  Wherry  (1924)],  by 
bacterial  metabolism  [see,  for  example,  Waksman  (1927)]  or  by  artificial 
additions.  In  the  absence  of  artificial  additions  there  may  be  reached  a 
natural  balance  in  the  contribution  of  each  factor.  This  may  permit 
a  correlation  between  pH  and  soil-type  [see,  for  example,  Gillespie  and 
Hurst  (1918)]  or  between  pH  and  plant-type  [see  references  under  Ecology]. 

The  causal  relation  between  the  frequency  of  occurrence  of  a  given 
plant  species  in  soils  of  a  narrow  range  of  pH  and  the  pH  may  be  direct  in 
some  instances.  More  often  it  is  probably  indirect  and  is  concerned  with 
the  influence  of  soil-reaction  upon  the  micro-organisms  concerned  in 
supplying  plant  nutrition  [see  Waksman  (1927)]  or  upon  parasites  [see, 
for  example,  Gillespie  (1918)].  However,  the  end  result  is  a  zone  of  pH 
favorable  for  each  given  species  of  plant. 

The  importance  of  controlling  the  soil  pH  in  agriculture  is  now 
widely  recognized.  Lime  is  frequently  used  to  increase  pH  [see,  for 
example,  discussion  by  Hoagland  and  Christie  (1918)]  and  sulfur  (which 
oxidizes  to  H2S04)  to  decrease  pH  [see  discussion  by  Lipman,  Waksman 
and  Joffe,  1921]. 

Some  data  have  been  obtained  in  recent  years  on  the  optimum  pH  values 
for  the  production  of  individual  crops.  The  most  extensive  of  these 
studies  is  that  of  O.  Arrhenius  (1926).  The  pH  values  of  70,000  samples 
from  15,000  fields  in  which  sugar  beets  were  growing  were  determined. 
Both  the  highest  yields  and  the  maximum  sugar  contents  were  found 
uniformly  in  the  range  pH  7.0  to  7.5.  A  list  of  several  hundred  plants  of 
agricultural  and  horticultural  interest,  arranged  according  to  their  op- 
timum pH  values,  has  been  published  by  Wherry  (1926). 

There  is  now  an  enormous  literature  on  the  manifold  aspects  of  the 
subject.  The  following  reviews  may  be  consulted.  Fisher  (1921),  Knick- 
mann  (1925),  Olsen  (1923),  Wherry  (1922),  Wiegner  and  Gessner  (1926), 
Trenel  (1927). 

Staining  and  dyeing.  Most  dyestuffs  are  of  basic  or  acidic  nature. 
Many  have  ionization  constants  the  values  of  which  fall  within  the  range 
of  ordinary  hydrogen  ion  concentrations.  Systematic  evaluations  remain 
to  be  conducted.  Many  of  the  substances  which  "take"  dyes  are  them- 
selves basic  or  acidic.  Consequently  there  are  good  grounds  for  believing 
that  dyeing  is  in  some  measure  salt  formation.  However,  the  ordinary 
equilibrium  laws  are  inapplicable  for  account  must  be  taken  of  the  fact  that 


586         THE  DETERMINATION  OF  HYDROGEN  IONS 

many  dyes  in  the  aqueous  phase  are  dispersed  in  colloidial  degree,  of  the 
fact  that  the  material  dyed  is  often  surface-active  and  of  the  fact  that 
dye-substrate  "compounds"  exhibit  specific  properties.  There  is  here 
another  instance  where  progress  requires  the  close  cooperation  of  various 
theoretical  and  experimental  methods  of  approach. 

Empirically,  the  control  of  hydrion  concentrations  and  the  study  of 
the  acidic  or  basic  nature  of  the  substrate  have  yielded  information  of 
considerable  value,  which  should  not  be  regarded  as  determinative  of 
theory  nor  neglected  by  the  theorist. 

Examples:  Agulhon  and  L6obardy  (1921),  Boissevain  (1927),  Collier 
(1924),  Elod  (1925-1926),  Gellhorn  (1927),  Haden  (1923),  Marker  and 
Gordon  (1924),  Mommsen  (1926),  Naylor  (1926),  Pfeiffer  (1927),  Rohde 
(1920),  Ruhland  (1923),  Sheppe  and  Constable  (1923),  Speakman  (1924), 
Smith  (1922),  Steam  and  Steam  (1924),  Weiser  and  Porter  (1927),  Zirkle 
(1927),  Balint  (1926). 

Surface  tension.  See  investigation  and  references  by  Hartridge  and 
Peters  (1922),  Egn6r  and  Hagg  (1927)  and  general  treatment  by  Rideal 
(1926). 

Taste.  One  of  the  original  means  of  distinguishing  acids.  See  page 
1.  There  has  been  considerable  discussion  of  the  function  of  [H+j. 
See  review  by  Dietzel  (1926). 

Water,  distilled  and  "conductivity."  Review  by  Bencowitz  and  Hotch- 
kiss  (1925);  cf.  Bordas  and  Touplain  (1926),  Kolthoff  (1926),  and  Bjerrum 
(1927). 

Waters,  inland.  The  pH  value  of  an  inland  water  may  be  influenced  by 
the  deposits  with  which  it  comes  in  contact.  For  an  extreme  see  Wells 
(1921).  For  the  effect  of  stratification  in  lakes  see  Juday,  Fred  and  Wilson 
(1924).  For  the  effect  of  industrial  wastes  and  sewage  see  Buswell  (1927). 
See  also  "Ecology,"  Shelford  (1925),  Cowles  and  Schwitalla  (1923),  Saunders 
(1921). 

Water,  sea.  The  carbonate  equilibrium  tends  to  maintain  sea  water  at 
a  constant  pH.  This  has  doubtless  varied  with  the  CO2-tension  of  the 
atmosphere  in  geological  time.  Locally  it  varies  with  temperature,  the 
photosynthetic  action  of  the  flora,  accretions  from  rivers,  and  contact 
with  geologic  deposits.  The  wider  aspects  have  been  described  in  Hen- 
derson's Fitness  of  the  Environment,  The  charting  of  the  pH  values  of 
different  regions  of  the  seas  has  been  of  aid  in  oceanographic  surveys  and 
of  value  to  the  study  of  plant  and  animal  distribution.  See  treatises  by 
Palitzsch  (1922),  Gaarder  (1916-1917),  Legendre  (1926),  Mayer  (1922), 
Bresslau  (1926),  Atkins  et  al.  (1924). 


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600  THE  DETERMINATION   OF  HYDROGEN   IONS 

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602  THE   DETERMINATION    OF   HYDROGEN    IONS 

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628         THE  DETERMINATION  OF  HYDROGEN  IONS 

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634  THE  DETERMINATION   OF  HYDROGEN   IONS 

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WINDISH,  W.,  AND  DIETRICH,  W.  1919  Neue  Wege  zur  Bestimmung  der 
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WINDISCH,  W.,  AND  DIETRICH,  W.  1920  tlber  das  Puffersystem  primares 
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WINSLOW,  C.-E.  A.,  AND  LOCHRIDGE,  E.  E.  1906  The  toxic  effect  of  cer- 
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APPENDIX 

TABLE  A 

ARBITRARILY  STANDARDIZED  VALUES  FOR  HALF-CELLS 
See  Chapter  XXIII  and  especially  page  488. 


||  (H+)  =  1  |  H8(l  atmos.),  Pt. 

KC1  (sat.)  |  KC1  (0.1  N),  HgCl  |  Hg 

KC1  (sat.),  HgCl  |  Hg 

KC1  (sat.)  I  HC1  (0.1  N)  |  H2(l  atmos.),  Pt. 

KC1  (sat.)  I  KHPhthalate  (0.05  M)  j  H2(l  atmos.),  Pt. 

fa«+  i  I  Acetic  acid  (0.1  N)  I  H  /,  nfm  q  N    Pf 
(sat.)  |  Na  Acetate  (0  !  M)  I  Ha(l  atmos.),  Pt. 

(H+)  =  1,  quinhydrone  I  Pt. 


Half -Cell  I 
Half -Cell  II 
Half -Cell  III 
Half -Cell  IV 
Half -Cell  V 

Half -Cell  VI 

Half-Cell  VII 

Half-Cell  VIII  KC1  (sat.)  |  HC1  (0.1  N),  quinhydrone  |  Pt. 


L  H 

HALF-CELL 

gl 

I 

II 

III 

Iva 

V 

VI 

VII 

VIII 

°C. 

volts 

volts 

volts 

volts 

volts 

volts 

volts 

volt* 

18 

0.0000 

0.3380 

0.251 

-0.0621 

(-0.229) 

-0.2668 

0.7044 

0.6423 

20 

0.0000 

0.3379 

0.250 

-0.0625 

-0.2310 

-0.2686 

0.7029 

0.6404 

25 

0.0000 

0.3376 

0.2458 

-0.0636 

(-0.235) 

-0.2732 

0.6992 

0.6356 

30 

0.0000 

0.3371 

0.242 

-0.0647 

(-0.239) 

0.6955 

0.6308 

35 

0.0000 

0.3365 

0.238 

-0.0657 

0.6918 

0.6261 

38 

0.0000 

0.3361 

0.236 

-0.0664 

0.6896 

0.6232 

40 

0.0000 

0.3358 

0.234 

-0.0668 

0.6881 

0.6213 

Examples  of  experimental  values  (see  page  479) 


CELL 

P 

E 

CITATION 

CELL 

TEMPER- 
ATURE 

E 

CITATION 

II  -III 

18 

0.087 

Table 

III:  IV 

25 

0.3094 

Table 

0.0885 

Walpole,  1914 

0.3103 

Fales  and  Mudge,  1920 

0.0874 

Michaelis,  1914 

0.3102S 

Harned,  1926 

25 

0.0918 
0.0918 
0.0916b 

Table 
Fales  and  Mudge,  1920 
Ewing,  1925 

38 

0.3024 
0.3024 

Table 
Stadie  and  Hawes,  1928, 
maximum 

0  3010 

Stadie  and  Hawes  1928 

II:  IV 

18 

0.4001 

Table 

minimum 

0.4011° 

S0rensen   and    Linder- 
str0m-Lang,  1924 

40 

0.3008 
0.3016 

Table 
Fales  and  Mudge,  1920 

25 

0.4012d 
0.4010 
0.4000 

Table 
Myers  and  Acree,  1913 
Loomis  and  Acree,  1911 

III:V 

30 

0.481 
0.482 

Table 
Author 

0.4004 
0.3995 

Harned,  1915 
Fales    and    Vosburgh, 
1918 

III:  VI 

18 

0.5178 
0.5175 

Table 
Michaelis,  1914 

O'.3985e 

Cohn    and     Berggren, 
1925 

25 

0.5190 
0.5195 

Table 
Michaelis,  1914 

II:  VI 

18 

0.6048 

Table 

VI:  IV 

18 

0.2047 

Table 

0.6046f 

Walpole,  1914 

0.2095h 

Michaelis     and    Kaki- 

numa,  1923 

0.2085h 

Michaelis   and    Fujita, 

1923 

a  Calculated  with  assumption  that  yH+  =  0.84  and  neglect  of  junction  potential.  ^  Calcu- 
lated from  data  for  Hg  |  HgCl,  KC1  (sat.)  |  KC1  (1.  N),  HgCl  |  Hg.  c  With  3.5  N  KC1  as 
bridge.  d  0.4009^  calculated  from  Scatchard's  data.  e  Calculated.  *  Unconnected  for 
barometer?  Add  0.3  m.v.?  *  Unconnected  for  change  from  molal  to  molar.  ^  Special 
liquid  junction. 

672 


APPENDIX 


673 


TABLE  B 

SHOWING  RELATION  OF  [H+]  TO  pH  (ON  THE  ASSUMPTION  THAT 


See  Chapter  XXIII 


pH 

[H+] 

pH 

[H+] 

pH 

[H+] 

x.OO 

1.000    X  10~x 

x.35 

0.447    X  10~x 

x.70 

0.200    X  10~x 

x.Ol 

0.977    X  10~x 

x.36 

0.437    X  10~x 

x.71 

0.195    X  10~x 

x.02 

0.955    X  10~x 

x.37 

0.427    X  10~x 

x.72 

0.191    X  10~x 

x.03 

0.933    X  10~x 

.38 

0.417    X  10~x 

x.73 

0.186    X  10~x 

x.04 

0.912    X  10~x 

.39 

0.407    X  10~x 

x.74 

0.182    X  10~x 

x.05 

0.891    X  10~x 

.40 

0.398    X  10~x 

x.75 

0.178    X  10~x 

x.06 

0.871    X  10~x 

.41 

0.389    X  10~x 

x.76 

0.174    X  10~x 

x.07 

0.851    X  10~x 

.42 

0.380    X  10~x 

x.77 

0.  170    X  10~x 

x.08 

0.832    X  10~x 

.43 

0.372    X  10~x 

x.78 

0.166    X  10~x 

x.09 

0.813    X  10~x 

.44 

0.363    X  10"~x 

x.79 

0.162    X  10~x 

x.10 

0.794    X  10~x 

.45 

0.355    X  10~x 

x.80 

0.158    X  10~x 

x.ll 

0.776    X  10~x 

.46 

0.347    X  10~x 

x.81 

0.155    X  10~x 

x.12 

0.759    X  10~x 

.47 

0.339    X  10~x 

x.82 

0.151    X  10~x 

x.13 

0.741    X  10~x 

.48 

0.331    X  10~x 

x.83 

0.148    X  10~x 

x.14 

0.725    X  10~x 

.49 

0.324    X  10~x 

x.84 

0.144    X  10~x 

x.15 

0.708    X  10~x 

.50 

0.316    X  10~x 

x.85 

0.141    X  10~x 

x.16 

0.692    X  10~x 

.51 

,  0.309    X  10~x 

x.86 

0.138    X  10~x 

x.17 

0.676    X  10~x 

.52 

0.302    X  10~x 

x.87 

0.135    X  10~x 

x.18 

0.661    X  10~x 

.53 

0.295    X  10~x 

x.88 

0.132    X  10~x 

x.19 

0.646    X  10~x 

54 

0.288    X  10~x 

x.89 

0.129    X  10~x 

x.20 

0.631    X  10~x 

55 

0.282    X  10~x 

x.90 

0.126    X  10~x 

x.21 

0.617    X  10~x 

56 

0.275    X  10~x 

x.91 

0.123    X  10~x 

x.22 

0.603    X  10~x 

57 

0.269    X  10~x 

x.92 

0.120    X  10~x 

x.23 

0.589    X  10~x 

58 

0.263    X  10~x 

x.93 

0.  117    X  10~x 

x.24 

0.575    X  10~x 

59 

0.257    X  10~x 

x.94 

0.115    X  10~x 

x.25 

0.562    X  10~x 

60 

0.251    X  10~x 

x.95 

0.112    X  10~x 

x.26 

0.549    X  10~x 

61 

0.245    X  10~x 

x.96 

0.110    X  10~x 

x.27 

0.537    X  10~x 

62 

0.240    X  10~x 

x.97 

0.107    X  10~x 

x.28 

0.525    X  10~x 

63 

0.234    X  10~x 

x.98 

0.105    X  10~x 

x.29 

0.513    X  10~x 

64 

0.229    X  10~x 

x.99 

0.102    X  10~x 

x.30 

0.501    X  10~x 

65 

0.224    X  10~x 

1  +  x.OO 

0.100    X  10"x 

x.31 

0.490    X  10~x 

66 

0.219    X  10~x 

1  +  x.Ol 

0.0977  X  10~x 

x.32 

0.479    X  10~x 

67 

0.214    X  10~x 

1  +X.02 

0.0955  X  10~x 

x.33 

0.468    X  10~x 

68 

0.209    X  10~x 

x.34 

0.457    X  10~x 

69 

0.204    X  10~x 

Examples:  pll  =  7.00;[H+]  =  1.000  X  10~7 
pH  =  6.63;  [H+]  =  0.234  X  10~6 
[H+]  =  1.23  X  10~8;  pH  =  7.91 


2.34  X  10" 


See  Klopsteg  (1921). 


TABLE  C 

FACTORS  FOR  CONCENTRATION  CELLS  0°C  TO  70°C. 


E  =  0.000,198,322  T  log     !  (when  valence  =  1).     A 

V^2 

See  discussion  page  250  for  uncertainties. 


0.000,198,322  T. 


1  * 

t  (CENTIGRADE) 

T  (ABSOLUTE) 

A 

A 

LOG  A 

0 

273.1 

0.054162 

18.463 

2.7336935 

1 

274.1 

0.054360 

18.396 

2.7352808 

2 

275.1 

0.054558 

18.329 

2.7368624 

3 

276.1 

0.054757 

18.263 

2.7384382 

4 

277.1 

0.054955 

18.197 

2.7400083 

5 

278.1 

0.055153 

18.131 

2.7415728 

6 

279.1 

0.055352 

18.066 

2.7431316 

7 

280.1 

0.055550 

18.002 

2.7446849 

8 

281.1 

0.055748 

17.938 

2.7462326 

9 

282.1 

0.055947 

17.874 

2.7477749 

10 

283.1 

0.056145 

17.811 

2.7493117 

11 

284.1 

0.056343 

17.748 

2.7508430 

12 

285.1 

0.056542 

17.686 

2.7523690 

13 

286.1 

0.056740 

17.624 

2.7538897 

14 

287.1 

0.056938 

17.563 

2.7554050 

15 

288.1 

0.057137 

17.502 

2.7569151 

16 

289.1 

0.057335 

17.441 

2.7584199 

17 

290.1 

0.057533 

17.381 

2.7599195 

18 

291.1 

0.057732 

17.321 

2.7614140 

19 

292.1 

0.057930 

17.262 

2.7629034 

20 

293.1 

0.058128 

17.203 

2.7643876 

21 

294.1 

0.058327 

17.145 

2.7658668 

22 

295.1 

0.058525 

17.087 

2.7673410 

23 

296.1 

0.058723 

17.029 

2.7688102 

24 

297.1 

0.058921 

16.972 

2.7702745 

25 

298.1 

0.059120 

16.915 

2.7717338 

26 

299.1 

0.059318 

16.858 

2.7731882 

27 

300.1 

0.059516 

16.802 

2.7746378 

28 

301.1 

0.059715 

16.746 

2.7760826 

29 

302.1 

0.059913 

16.691 

2.7775225 

30 

303.1 

0.060111 

16.636 

2.7789577 

31 

304.1 

0.060310 

16.581 

2.7803882 

32 

305.1 

0.060508 

16.527 

2.7818140 

33 

306.1 

0.060706 

16.473 

2.7832351 

34 

307.1 

0.060905 

16.419 

2.7846516 

35 

308.1 

0.061103 

16.366 

2.7860635 

36 

309.1 

0.0613C1 

16.313 

2.7874708 

37 

310.1 

0.061500 

16.260 

2.7888736 

38 

311.1 

0.061698 

16.208 

2.7902718 

39 

312.1 

0.061896 

16.156 

2.7916656 

40 

313.1 

0.062095 

16.104 

2.7930549 

45 

318.1 

0.063086 

15.851 

2.7999355 

50 

323.1 

0.064078 

15.606 

2.8067088 

55 

328.1 

0.065069 

15.368 

2.8133780 

60 

333.1 

0.066061 

15.137 

2.8199464 

65 

338.1 

0.067053 

14.914 

2.8264170 

70 

343.1 

0.068044 

14.696 

2.8327925 

*  Useful  in  machine  calculations. 

674 


APPENDIX 


675 


TABLE  D 

CORRECTION  OF  BAROMETER  READING  FOR  TEMPERATURE 

When  the  mercury  in  the  barometer  is  at  the  temperature  t  subtract  the 
following  millimeters  to  obtain  the  barometic  height  in  terms  of  mercury 
at  zero  degrees  centigrade. 


t 

BAROMETER   READINGS  IN  MILLIMETERS 

720 

730 

740 

750 

760 

770 

780 

17 

2.0 

2.0 

2.1 

2.1 

2.1 

2.1 

2.2 

18 

2.1 

2.1 

2.2 

2.2 

2.2 

2.3 

2.3 

19 

2.2 

2.3 

2.3 

2.3 

2.4 

2.4 

2.4 

20 

2.3 

2.4 

2.4 

2.4 

2.5 

2.5 

2.5 

21 

2.5 

2.5 

2.5 

2.6 

2.6 

2.6 

2.7 

22 

2.6 

2.6 

2.7 

2.7 

2.7 

2.8 

2.8 

23 

2.7 

2.7 

2.8 

2.8 

2.8 

2.9 

2.9 

24 

2.8 

2.9 

2.9 

2.9 

3.0 

3.0 

3.1 

25 

2.9 

3.0 

3.0 

3.1 

3.1 

3.1 

3.2 

26 

3.0 

3.1 

3.1 

3.2 

3.2 

3.3 

3.3 

27 

3.2 

3.2 

3.3 

3.3 

3.3 

34 

3.4 

28 

3.3 

3.3 

3.4 

3.4 

3.5 

3.5 

3.6 

29 

3.4 

3.4 

3.5 

3.5 

3.6 

3.6 

3.7 

30 

3.5 

3.6 

3.6 

3.7 

3.7 

3.8 

3.8 

31 

36 

3.7 

3.7 

3.8 

3.8 

3.9 

39 

For  various  refined  corrections  of  barometric  readings  see  article  on 
Barometry  and  Manometry  by  Kimball  in  International  Critical  Tables, 
Vol.  1,  p.  68. 


676 


THE  DETERMINATION   OF  HYDROGEN   IONS 


TABLE  E 

BAROMETRIC  CORRECTIONS  FOR  H-ELECTRODE  POTENTIALS 
(Data  for  use  in  plotting  correction  curves) 


Ebar. 


0.000,198322  T  ]o    760 


TEMPER- 
ATURE 

CORRECTED 

PRESSURE 

VAPOR 

PRESSURE 

X 

760 
LOO  — 

X 

Ebar. 

•c. 

mm. 

WOT. 

millivolts 

f 

780 

769.5 

-0.00537 

-0.15 

12 

760 

10.5 

749.5 

+0.00604 

+0.17 

I 

740 

729.5 

0.01779 

0.50 

f 

780 

15.5 

764.5 

-0.00256 

-0.07 

18 

760 

744.5 

+0.00895 

+0.26 

I 

740 

724.5 

0.02078 

0.60 

f 

780 

17.5 

762.5 

-0.00143 

-0.04 

20 

760 

742.5 

+0.01012 

+0.29 

I 

740 

722.5 

0.02198 

0.64 

( 

780 

23.8 

756.2 

0.00218 

0.06 

25 

760 

736.2 

0.01382 

0.41 

I 

740 

716.2 

0.02578 

0.76 

f 

780 

31.8 

748.2 

0.00680 

0.20 

30 

760 

728.2 

0.01856 

0.56 

I 

740 

708.2 

0.03066 

0.92 

f 

780 

42.2 

737.8 

0.01288 

0.39 

35 

760 

717.8 

0.02481 

0.76 

I 

740 

697.8 

0.03708 

1.13 

f 

780 

55.3 

724.8 

0.02060 

0.64 

40 

760 

704.8 

0.03275 

1.02 

I 

740 

684.7 

0.04525 

1.41 

E.  M.  F.  +  Ebar.  -  Ecal. 
0.000,198322  T 


APPENDIX 


677 


VALUES  OF  Loo 


AND  OF  Loo 


TABLE  F 
a 


MULTIPLIED  BY  THE  TEMPERA- 


TURE FACTORS  FOR  CONCENTRATION  CELLS  AT  20°,  25°,  30°  AND  37.5°C. 


a 

a 

/v 
•  +*.**                    .» 

Cn/TIPLIED  BY 

1  —a 

1  —  a 

0.058128 

(20) 

0.059120 

(25) 

0.060111 
(30) 

0.061599 
(37.5) 

0.001 

-2.9996 

-0.1744 

-0.1773 

-0.1803 

-0.1848 

0.005 

-2.2989 

-0.1336 

-0.1359 

-0.1382 

-0.1416 

0.01 

-  .9956 

-0.1160 

-0.1180 

-0.1200 

-0.  1229 

0.02 

-  .6902 

-0.0982 

-0.0999 

-0.1016 

-0.1041 

0.03 

-  .5096 

-0.0878 

-0.0892 

-0.0907 

-0.0930 

0.04 

-  .3802 

-0.0802 

-0.0816 

-0.0830 

-0.0850 

0.05 

-  .2788 

-0.0743 

-0.0758 

-0.0769 

-0.0788 

0.06 

-  .1950 

-0.0695 

-0.0706 

-0.0718 

-0.0736 

0.07 

-  .1234 

-0.0653 

-0.0664 

-0.0675 

-0.0692 

0.08 

-  .0607 

-0.0617 

-0.0627 

-0.0638 

-0.0653 

0.09 

-  .0048 

-0.0584 

-0.0594 

-0.0604 

-0.0619 

0.10 

-0.9542 

-0.0555 

-0.0564 

-0.0574 

-0.0588 

0.11 

-0.9080 

-0.0528 

-0.0537 

-0.0546 

-0.0559 

0.12 

-0.8653 

-0.0503 

-0.0512 

-0.0520 

-0.0533 

0.13 

—0.8256 

-0.0480 

-0.0488 

-0.0496 

-0.0509 

0.14 

-0.7884 

-0.0458 

-0.0466 

-0.0474 

-0.0486 

0.15 

-0.7533 

-0.0438 

-0.0445 

-0.0453 

-0.0464 

0.16 

-0.7202 

-0.0419 

-0.0426 

-0.0433 

-0.0444 

0.17 

-0.6886 

-0.0400 

-0.0407 

-0.0414 

-0.0424 

0.18 

-0.6585 

-0.0383 

-0.0389 

-0.0396 

-0.0406 

0.19 

-0.6297 

-0.0366 

-0.0372 

-0.0379 

-0.0388 

0.20 

-0.6021 

-0.0350 

-0.0356 

-0.0362 

-0.0371 

0.21 

-0.5754 

-0.0334 

-0.0340 

-0.0346 

-0.0354 

0.22 

-0.5497 

-0.0320 

-0.0325 

-0.0330 

-0.0339 

0.23 

-0.5248 

-0.0305 

-0.0310 

-0.0315 

-0.0323 

0.24 

-0.5006 

-0.0291 

-0.0296 

-0.0301 

-0.0308 

0.25 

-0.4771 

-0.0277 

-0.0282 

-0.0287 

-0.0294 

0.28 

-0.4543 

-0.0264 

-0.0269 

-0.0273 

-0.0280 

0.27 

-0.4320 

-0.0251 

-0.0255 

-0.0260 

-0.0266 

0.28 

-0.4102 

-0.0238 

-0.0243 

-0.0247 

-0.0253 

0.29 

-0.3888 

-0.0226 

-0.0230 

-0.0234 

-0.0239 

0.30 

-0.3680 

-0.0214 

-0.0218 

-0.0221 

-0.0227 

0.31 

-0.3475 

-0.0202 

-0.0205 

-0.0209 

-0.0214 

0.32 

-0.3274 

-0.0190 

-0.0194 

-0.0197 

-0.0202 

0.33 

-0.3076 

-0.0179 

-0.0182 

-0.0185 

-0.0189 

0.34 

-0.2880 

-0.0167 

-0.0170 

-0.0173 

-0.0177 

0.35 

-0.2688 

-0.0156 

-0.0159 

-0.0162 

-0.0166 

0.36 

-0.2499 

-0.0145 

-0.0148 

-0.0150 

-0.0154 

0.37 

-0.2311 

-0.0134 

-0.0137 

-0.0139 

-0.0142 

0.38 

-0.2126 

-0.0124 

-0.0126 

-0.0128 

-0.0131 

0.39 

-0.1943 

-0.0113 

-0.0115 

-0.0117 

-0.0120 

0.40 

-0.1761 

-0.0102 

-0.0104 

-0.0106 

-0.0108 

0.41 

-0.1581 

-0.0092 

-0.0093 

-0.0095 

-0.0097 

0.42 

-0.1402 

-0.0081 

-0.0083 

-0.0084 

-0.0086 

0.43 

-0.1224 

-0.0071 

-0.0072 

-0.0074 

-0.0075 

0.44 

-0.1047 

-0.0061 

-0.0062 

-0.0063 

-0.0064 

0.45 

-0.0871 

-0.0051 

-0.0051 

-0.0052 

-0.0054 

0.46 

-0.0696 

-0.0040 

-0.0041 

-0.0042 

-0.0043 

0.47 

-0.0522 

-0.0030 

-0.0031 

-0.0031 

-0.0032 

0.48 

-0.0347 

-0.0020 

-0.0021 

-0.0021 

-0.0021 

0.49 

-0.0174 

-0.0010 

-0.0010 

-0.0010 

-0.0011 

0.50 

±0.0000 

±0.0000 

±0.0000 

±0.0000 

±0.0000 

0.51 

+0.0174 

+0.0010 

+0.0010 

+0.0010 

+0.0011 

0.52 

+0.0347 

+0.0020 

+0.0021 

+0.0021 

+0.0021 

For  values  beyond  a  =  0.50  the  table  progresses  inversely  as  above  but  with  sign  +.    Exam- 
ple: a  =  0.53,  (1  -  a  =  0.47),  read  row  for  a  =  0,47,  i.e.,  log  ,—^—  =  +  0.0522,  etc.    If  a  =  0.80, 

1  —  a 

(1  -  a  =  0.20),  read  row  for  a  -  0.20,  i.e.,  log  ^—^ —  =*  +  0.6021,  etc. 


678 


THE   DETERMINATION    OF  HYDROGEN   IONS 


TABLE  G 

DISSOCIATION  EXPONENTS  OF  ACIDS 

Important:  Values  are  to  be  regarded  as  approximate.    It  is  impracticable 
to  state  conditions  in  every  case.    Note  distinction  between  pK  and  pK' . 


ACID 

pK' 

AUTHOR- 
ITY 

ACID 

pK' 

AUTHOR- 
ITY 

Acetic                               pK 

4  73* 

(4) 

Malonic 

2  80 

d) 

Alloxan 

6  6 

(3) 

Malonic  2d 

5  68 

(1) 

Arsenic 

2  3 

(3) 

Mucic  .    . 

3  2 

(6) 

Arsenic  2d 

4  4 

(3) 

Nitrous 

3  4 

(3)  18° 

Arsenic  3d 

9  2 

(3) 

Oxalic 

1  42 

CD 

9  2 

(3) 

Oxalic  2d 

4  39 

(6) 

Azelaic 

4  6 

(1) 

Phenol 

10  0 

(3) 

Azelaic  2d 

5  6 

(6)  18° 

Phosphoric                    pKi 

2  11* 

(10) 

Barbituric 

4  0 

(3) 

Phosphoric                    pK.2 

7  16* 

(9) 

Benzoic 

4  2 

(3) 

Phosphoric                    pKs 

12  66* 

(10) 

Boric                                  .    . 

9  2 

(3) 

o-phthalic 

2  92 

(1) 

Butyric 

4  8 

(3) 

o-phthalic  2d 

5  41 

(1) 

Carbonic                         pKi 

6  33* 

(5) 

m-phthalic 

3  54 

(1) 

Carbonic                    .  .  pK2 

10  22* 

(5) 

m-phthalic  2d 

4  62 

(i) 

Citric 

3  08 

(8) 

Pinaelic 

2  92 

(1) 

Citric  2d 

4  39 

(8) 

Pimelic  2d 

5  41 

(1) 

Citric  3d 

5  49 

(8) 

4  8 

(3) 

Formic 

3  7 

(3) 

4  1 

(6) 

Fumaric 

3  03 

(1) 

5  63 

(2) 

Fumaric  2d 

4  49 

(1) 

3  0 

(3) 

Glucose 

12  3 

(3)     ' 

4  62 

(D 

Glutaric 

4  32 

(1) 

Sebacic  2d 

5  60 

(D 

Glutaric2d  .~7r... 

5.54 

(1) 

Succinic 

4  18 

(i) 

Hippuric 

3  7 

(3) 

5  57 

CD 

Hydrocyanic  

9.1 

(3) 

Sulfanilic 

3  2 

(3) 

Hydrogen  sulphide  

7  2 

(3)  18° 

Sulfurous 

1  8 

(3) 

Hydrogen  sulphide  2d  

14.7 

(7)    0° 

Sulfurous  2d  .  .. 

5.3 

(3) 

Itaconic         . 

3  8 

(6) 

2  56 

(1) 

Itaconic  2d 

5  7 

(6) 

4  41 

(1) 

Lactic  

3.85 

(6) 

d-Tartaric 

3  0 

(6) 

Maleic  

1  93 

(1) 

d-Tartaric  2d 

4  39 

(2) 

Maleic  2d 

6  58 

(I) 

Thiodiglycollic 

3  31 

(R) 

1-malic 

3  48 

(6) 

Thiodiglycollic  2d 

4  46 

(2) 

1-malic  2d  

5  11 

(2) 

Uric 

5  8 

(6^  18° 

*  pK  value. 


Authorities 


(1)  Chandler  (1908)  25°. 

(2)  Larsson  (1922)  18°. 

(3)  Landolt-Bornstein  (1923)  25°. 

(4)  Cohn,  Heyroth  and  Menkin  (1928)  see  page  509. 

(5)  Hastings  and  Sendroy  (1925).    pKi'  =  6.33  -  0.5 

at  38°. 

(6)  Scudder  (1914)  25°. 

(7)  Jellinek  and  Czerwinski  (1922). 

(8)  Hastings  and  Van  Slyke  (1922). 

* 


at  38°.    pK'2  =  10.22  -  1. 


(9)  Cohn  (1927).    pKs'  =  7.16 

1  +  1.5 

(10)  Sendroy  and  Hastings  (1927).    pKi' 
at  38°. 


+  KSM  (see  page  506). 
/x 

2.11  -0.5  VM  at  18°.    pK»' 


12.60  -  2.25 


APPENDIX 


679 


TABLE  H 

DISSOCIATION  CONSTANTS  AND  ASSOCIATION  EXPONENTS  OF  BASES 


[B+l  [OH-] 
[BOH] 


=  Kb 


[B]  [H 


Kab 


pKab   =   log 


[BH] 
Assumptions : 

=  Kw  —  pKb 
Values  of  Kw  taken  from  table  6,  page  45 
Values  of  Kb  taken  from  Kolthof?  and  Furman  (1926) 


'       BASE 

Kb  TEMPERATURE  °C. 

PKab 

Ammonia  

1  75  X  10*5    18° 

9  37 

Aniline           

4  6    X  lO"10  25° 

4  56 

Ethylamine 

5  6    X  10~4    25° 

10  64 

Diethylamine  

1  26  X  10~3    25° 

11  00 

Triethylamine 

6  4    X  10~4    25° 

10  70 

Methylamine  

SOX  10~4    25° 

10  59 

Dime  thy  lamine  ....       .    . 

7  4    X  10~4    25° 

10  76 

Trimethylamine 

7  4    X  10~B    25° 

9  76 

Pyridine  

2  3    X  10~9    25° 

5  26 

Urea    

about  (1  5    X  10~14     ?) 

(0  1) 

680 


THE  DETEKMINATION   OF  HYDROGEN   IONS 


TABLE  I 
DISSOCIATION  EXPONENTS  AND  ASSOCIATION  EXPONENTS  OF  AMINO 

ACIDS  AT  25° 
(After  Bjerrum  (1923)) 

pKw 


pK  =  log  — 


kb 


[NH2RCOQ-] 

[NH2RCOOH] 
[NH+RCOOH]  [OH-] 
[NH2RCOOHJ 


K, 


KT 


13.90 

[NH+RCOO-]  [H+] 
[NH+RCOOH] 

[NH+RCOO-]  [OH] 
[NH2RCOO-] 


P*a 

PKW- 
PKb 

PKA 

PKW- 
PKB 

Aliphatic: 
Glycine                .       ... 

9  75 

2  33 

2  33 

Q  75 

IVlethyl  glycine 

9  89 

2  15 

2  15 

9  on 

Dimethyl  glycine 

9  85 

1  93 

1  93 

Q  85 

Betaine  

ca!4 

1  34 

1  34 

ca!4 

Alanine 

9  72 

2  61 

2  61 

972 

L/eucine  

9  75 

2  26 

2  26 

9  75 

Phenylalanin  

8  60 

2  01 

2  01 

C    Af) 

Tyrosine  

8  40 

2  51 

2  51 

8  40 

Glycyl  glycine  . 

7  74 

3  20 

3  20 

7  74 

Alanyl  glycine  

7  74 

3  20 

3  20 

7  74 

Leucyl  glycine  .    . 

7  82 

3  38 

3  38 

7  82 

Taurine  

8  8 

caO 

cctO 

8  8 

Asparagine  

8  87 

2  08 

2  08 

c  07 

[First  step  .  . 

12 

<6  94 

1  94 

12 

Lysine  <  0          ,    * 
I  feecond  step 

1  94 

fi  Q4 

[First  step 

>13  96 

6  9 

2  24 

ca!4 

Argmme  \Second  step  

2  24 

7  0 

Histidine  (*irst  •te?  
(Second  step 

8.66 

5.66 
1  60 

1.60 

8.66 
.5  fifi 

.  ,  [First  sten 

3  82 

1  Q8 

1  Q8 

10    1 

Aspartic  acid  <  0 
[becond  step  

12  1 

3  82 

Aromatic  : 
o-amino  benzoic  

4  98 

2  04 

2  04 

4  98 

m-amino  benzoic  

4  92 

3  27 

3  27 

4  92 

p-amino  benzoic  

4  80 

1  Q8 

1   Q8 

4  80 

o-benzbetaine  

>14 

1  35 

1  35 

—0  1 

m-benzbetaine  

>14 

3  43 

3  43 

—0  1 

p-benzbetaine  

ca!4 

3  41 

3  41 

ca—  0  1 

o-amino  benzene  sulfonic  acid, 
m-amino  benzene  sulfonic  acid.  . 
p-amino  benzene  sulfonic  acid.  .  . 

2.48 
3.73 
3.24 

2.48 
3.73 
3.24 

APPENDIX 


681 


TABLE  J 

ALKALOIDS— HALF  TRANSFORMATION  POINTS  AT  15°C.  AS  DETERMINED 
ROUGHLY  BY  KOLTHOFF  (1925) 

pK  =  14.2  -  log 


ALKALOID 

pK' 

ALKALOID 

PK 

PK 

Aconitine 

8  32 

Brucine 

8  16 

2  50 

Atropine  

9  85 

Cinchonine  

8  35 

4  28 

Cocaine  

8  61 

Emetine      

8  43 

7  56 

Codeine 

8  15 

Nicotine 

8  04 

3  24 

Coniine  

11  10 

Novocaine  

9  05 

2  47 

Morphine  . 

8  07 

Quinine 

8  23 

4  50 

Thebaine 

8  15 

Strychnine 

8  20 

2  50 

682 


THE   DETERMINATION   OF  HYDROGEN   IONS 


TABLE  K 

RELATION  OF  PERCENTAGE  REDUCTION  TO  POTENTIAL  AT  CONSTANT  pH 

[Sr] 


DETERMINED  BY  Eh  =  E'0  -  0.03006  LOG 


[So] 


AT  30°C. 


(Values  rounded  to  nearest  millivolt) 


EBDXJCTION 

-0.03006  LOG  ||4 

[CO] 

REDUCTION 

-  0.03006  LOG  |^j 

per  cent 

volts 

per  cent 

volts 

1 

+0.060 

55 

-0.003 

2 

0.051 

60 

0.005 

5 

0.038 

65 

0.008 

10 

0.029 

70 

0.011 

15 

0.023 

75 

0.014 

20 

0.018 

80 

0.018 

25 

0.014 

85 

0.023 

30 

0.011 

90 

0.029 

35 

0.008 

95 

0.038 

40 

0.005 

98 

0.051 

45 

+0.003 

99 

-0.060 

50 

±0.000 

APPENDIX 


683 


TABLE  L 

Eo'  VALUES  FOR  SEVERAL  OXIDATION-REDUCTION  INDICATORS,  30°C. 
(Values  rounded  to  nearest  millivolt) 


B 

H 

g 

o 
a 

i 

o 

1 

DLPHONA1 

H 
p 

H 

!i 

JULPHONJ 

HENOL  IN 

fc 

o 
§ 

B 

8  GREEN 

OL  INDO- 

o 

pH 

£ 

| 

00 

« 

w 

eji  3 

^o 

O 

K 

o 

« 

X 

1 

i 

« 

H 

H 

• 

B 

Ss 

S* 

ifc 

«S 

*3  O 

H 

g 

W 

ft  J 

s 

§ 

E 

i 
s 

8 

H 

i 

H 

•LTJYLE 

III 

Si 

6-DICH 
0-CRE8 

6-DICH 
PHENO 

NDSCH: 

CHLORi 
PHENO 

•BROMC 

PHENO: 

K 

& 

2 

g 

TH 

TH 

« 

<N~ 

3 

6 

S 

5.0 

-0.010 

0.032 

0.065 

0.101 

0.221 

0.262 

0.335 

0.366 

0.335 

5.2 

0.022 

0.020 

0.053 

0.088 

0.208 

0.249 

0.322 

0.352 

0.320 

5.4 

0.034 

+0.008 

0.041 

0.077 

0.196 

0.236 

* 

0.307 

0.339 

0.307 

* 

• 

5.6 

0.045 

-0.004 

0.029 

0.066 

0.184 

0.223 

0.292 

0.325 

0.293 

5.8 

0.057 

0.016 

0.017 

0.056 

0.173 

0.210 

0.277 

0.310 

0.281 

6.0 

0.069 

0.028 

+0.006 

0.047 

0.162 

0.196 

0.183 

0.261 

0.295 

0.270 

0.301 

6.2 

0.081 

0.039 

-0.006 

0.039 

0.151 

0.181 

0.171 

0.245 

0.279 

0.259 

0.288 

6.4 

0.092 

0.051 

0.017 

0.031 

0.141 

0.166 

0.159 

0.228 

0.263 

0.249 

0.275 

* 

6.6 

0.104 

0.061 

0.027 

0.024 

0.132 

0.150 

0.147 

0.212 

0.247 

0.240 

0.262 

6.8 

0.114 

0.072 

0.037 

0.017 

0.123 

0.134 

0.135 

0.196 

0.232 

0.232 

0.248 

7.0 

0.125 

0.081 

0.046 

0.011 

0.115 

0.119 

0.123 

0.181 

0.217 

0.224 

0.233 

0.248 

7.2 

0.134 

0.091 

0.055 

+0.004 

0.108 

0.103 

0.111 

0.166 

0.203 

0.217 

0.218 

0.235 

7.4 

0.143 

0.099 

0.062 

-0.002 

0.101 

0.088 

0.099 

0.152 

0.189 

0.210 

0.203 

0.221 

7.6 

0.152 

0.107 

0.070 

0.008 

0.094 

0.073 

0.087 

0.138 

0.175 

0.204 

0.187 

0.208 

7.8 

0.160 

0.114 

0.077 

0.014 

0.088 

0.060 

0.074 

0.125 

0.162 

0.197 

0.170 

0.193 

8.0 

0.167 

0.121 

0.083 

0.020 

0.082 

0.046 

0.062 

0.112 

0.150 

0.155 

0.178 

8.2 

0.174 

0.127 

0.090 

0.026 

0.075 

0.034 

0.049 

0.099 

0.137 

0.139 

0.163 

8.4 

0.180 

0.134 

0.096 

0.032 

0.069 

0.021 

0.026 

0.087 

0.125 

0.124 

0.148 

8.6 

0.187 

0.140 

0.102 

0.038 

0.063 

+0.010 

0.023 

0.075 

0.113 

t 

0.109 

0.133 

8.8 

0.193 

0.146 

0.108 

0.044 

0.057 

-0.002 

+0.010 

0.063 

0.101 

0.095 

0.117 

9.0 

-0.199 

-0.152 

-0.114 

-0.050 

0.051 

-0.012 

-0.003 

0.051 

0.089 

0.082 

0.103 

*  Unstable  in  this  region  of  pH. 
t  Decomposes  in  this  region  of  pH. 


684  THE   DETERMINATION   OF  HYDROGEN   IONS 

TABLE  M 
SYMBOLS  AND  CONVENIENT  FORMULAS 

For  notation  see  definitions  in  text  as  a  notation  is  introduced 
(A)    Read:  The  activity  of  A. 
[A]    Read:  The  concentration  of  A  in  moles  per  liter,  unless  otherwise 

specified. 

=    Read:  Is  approximately  or  essentially  equal  to. 
=     Read:  Is  equal  to. 
=     Read:  Is  identical  with. 
>     Read:  Is  greater  than. 
<     Read:  Is  less  than. 
f    Symbol  of  integration. 
S    Read:  The  sum  of  all  terms  following. 
A    Read:  The  increment  of. 
II    Read:  Liquid  junction  potential  is  here  considered  to  be  eliminated 

or  otherwise  allowed  for. 
|    Read:  There  is  a  potential  difference  here. 

J    Read:  There  is  a  junction  potential  here  and  the  junction  is  a  flow- 
ing junction. 

In    Read:  Logarithm  to  the  base  e. 
log    Read:  Logarithm  to  the  base  10. 
log  x  =  0.43429  In  x 
In  x  =  2.3026  log  x 
d    Read:  The  infinitesimal  increment  of  or  differential  of. 

d(a^)  d  v 

-^— '  =  arln  a  — 

dx  d  x 

pH  s  log  ; — —     (formally).    For  the  experimental  meaning  see  Chapter 

XXIII. 

pK  s  log  —  (formally).     For  experimental  meaning  compare  with  pH. 

JEV 

See  also  subject  index. 

TABLE  N 

DEFINITIONS  (OP  LESS  COMMON  TERMS)  WHICH  ARE  USED  AND  NOT 
INCLUDED  IN  THE  TEXT 

Definitions  are  the  most  accursed  of  all  things  on  the  face  of  the 
earth. — R.  HUNTER. 

I.  C.  T.  refers  to  International  Critical  Tables. 
Dimensions  are  enclosed  in  [  ]. 

Ampere. — Unit  of  electric  current.  Abs.  ampere  =  0.1  cgs.  unit.  Int. 
ampere  is  that  unvarying  electric  current  which,  when  passed 
through  a  solution  of  silver  nitrate  in  water,  in  accordance  with 
certain  specifications,  deposits  silver  at  the  rate  of  0.00111800  gram 
per  second.  /.  C.  T. 


APPENDIX  685 

Angstrom  unit. — (A).  [1].  10~10  meters.  International  Angstrom  de- 
fined as  such  a  length  that  wave-length  of  red  cadmium  line  in  air 
at  15°C.,  An,  is  exactly  6438.4696  Int.  A;  it  =  10"10  m  within  ex- 
perimental error.  7.  C.  T. 

Anion. — An  ion  with  net  excess  negative  charge  causing  it  to  travel  toward 
the  anode  (+)  in  electrolysis. 

Anode.— See  electrode. 

Atmosphere. — [force  area"1],  [m/lt2].  1.  Normal  atmosphere  (An)  de- 
fined as  pressure  exerted  by  vertical  column  of  liquid  76  cm.  long, 
density  13.5951  grams  per  cm.3,  acceleration  of  gravity  being  980.665 
cm.  sec."2.  2.  Atmosphere  at  45°  (A45)  differs  from  An  only  in  use 
of  acceleration  of  gravity  at  sea  level  and  lat.  45°  instead  of  980.655 
cm.  see."2.  3.  British  atmosphere  is  based  on  30  inches  instead  of 
76  cm.  I.  C.  T. 

Avogadro's  number. — (N0),  [m"1].  Number  of  molecules  in  a  mole. 
7.  C.  T. 

Calorie.— [Heat],  [m!2/t2].  1.  Heat  per  unit  of  mass,  per  °C.  of  rise,  re- 
quired to  produce  small  rise  in  temperature  of  water  under  pressure 
An;  varies  with  temperature,  which  must  be  stated.  If  unit  of 
mass  is  gram,  it  is  called  small  calorie,  gram  calorie,  or  calorie; 
symbol  is  cal.  If  unit  of  mass  is  kilogram,  it  is  called  large  calorie, 
kilogram  calorie,  or  Calorie;  symbol,  Cal.  (2)  Mean  calorie  = 
1/100  of  heat  required  to  raise  unit  mass  of  water  from  0°  to  100°C., 
pressure  An.  /.  C.  T. 

Cation. — An  ion  with  net  excess  positive  charge  causing  it  to  travel 
toward  the  cathode  (— )  in  electrolysis. 

Cathode.— See  electrode. 

Colligative  properties. — "The  properties  of  solutions  are  determined, 
not  by  the  relative  weights  of  the  substances  present,  but  rather 
by  the  relative  number  of  molecules  of  the  constituents  present  in 
the  solution.  Such  properties  of  solutions  have  been  designated  by 
Ostwald  as  colligative  properties."  Frazer,  p.  235,  Taylor's  Treatise. 

Conductance.— Reciprocal  of  resistance.    7.  C.  T. 

Conductivity,  Electrical. — Reciprocal  of  electrical  resistivity  (q.v.).  1. 
(K)  Volume  conductivity  =  reciprocal  of  volume  resistivity; 
specific  conductance.  2.  Mass  conductivity  =  K/d;  d  =  density. 
3.  Equivalent  conductivity  (A)  is  K/C;  c  =  equivalents  of  solute 
per  unit  volume  of  solution.  4.  Molecular  conductivity  (/*)  is 
K/m;  m  =  moles  of  solute  per  unit  volume  of  solution.  7.  C.  T. 

Coulomb. — The  quantity  of  electricity  transferred  in  one  second  by  a 
current  of  one  ampere.  7.  C.  T. 

Dielectric  constant.— («)  (or  D)  [t2//tl2],  [«].  The  force  (/)  of  repulsion 
between  two  point  charges  (e,  e')  of  electricity  at  a  distance  (r)  apart 
in  a  uniform  medium  of  great  extent  is  /  =  ee'/cr2;  c  depends  upon 
the  nature  of  the  medium,  and  is  called  its  dielectric  constant. 
7.  C.  T. 


686         THE  DETERMINATION  OF  HYDEOGEN  IONS 

Dichromatism. — From  Si-(two)  and  XP&/-K*  (color). 

Dyne.' — [ml/t2].  The  cgs.  unit  of  force.  The  force  which,  when  acting 
continuously  upon  a  mass  of  one  gram  and  not  opposed  by  another, 
will  impart  to  the  mass  a  uniform  acceleration  of  one  cm.  per  sec.2. 
7.  C.  T. 

Electromotive  force.— (E),  (E.  M.  F.).     See  Potential. 

Electron. — Negative  electrons  are  very  small  negatively  charged  parti- 
cles observed  under  many,  very  diverse  conditions.  All  appear  to 
be  alike  in  every  way,  including  amount  of  charge  carried.  They 
appear  to  be  one  of  the  basic  elements  of  which  atoms  are  made. 
7.  C.  T. 

Applied  by  G.  J.  Stoney  (1891)  to  the  electric  charge  associated 
with  each  "bond"  in  one  chemical  atom. 

Electrolytes. — "Many  bodies  are  decomposed  directly  by  the  electric 
current,  their  elements  being  set  free;  these  I  propose  to  call  elec- 
trolytes." Faraday  in  1834. 

Electrode. — "In  place  of  the  term  pole,  I  propose  using  that  of  elec- 
trode, and  I  mean  thereby  that  substance,  or  rather  surface, 
whether  of  air,  water,  metal  or  any  other  body,  which  bounds  the 
extent  of  the  decomposing  matter  in  the  direction  of  the  electric 
current.  If  a  system  is  so  oriented  with  respect  to  the  points  of  the 
compass  that  what  is  called  the  positive  current  enters  at  the  east 
and  departs  at  the  west  (the  direction  of  the  sun's  apparent  motion) 
the  anode  (up  way)  is  that  surface  at  which  the  electric  current 
according  to  our  present  expression  enters.  The  cathode  (down  way) 
is  that  surface  at  which  the  current  leaves  the  decomposing  body." 
Faraday  in  1834. 

Equivalent.— (equiv.).  Electrochemical  equivalent  (briefly  equivalent) 
of  an  ion- — actual  or  potential — is  its  formula  weight  divided  by 
its  valence.  7.  C.  T. 

Erg.— [force  .  distance],  [m!2/t2].  Work  done  by  a  force  of  one  dyne 
while  acting  through  a  distance  of  one  centimeter  in  its  own  direc- 
tion. 7.  C.  T. 

Faraday. — (F).  The  electrical  charge  carried  in  electrolysis  by  one 
gram-equivalent. 

Field. — The  field  of  a  physical  quantity  is  the  region  of  space  within  which 
phenomena  characteristic  of  the  quantity  exist.  The  strength,  or 
intensity,  of  the  field  at  any  point  is  measured  by  the  magnitude  at 
that  point  of  some  chosen,  characteristic  phenomenon,  and  the 
complete  designation  of  the  field  includes  an  indication  of  this 
phenomenon;  e.g.,  electrical  field  of  force.  As  force  is  the  phe- 
nomenon most  frequently  chosen,  and  in  other  cases  the  context 
indicates  what  is  intended,  the  explicit  designation  of  the  chosen 
phenomenon  is  quite  frequently  omitted.  7.  C.  T. 

Force.— [ml/t2].  That  which  imparts  acceleration  to  material  bodies. 
7.  C.  T. 


APPENDIX  687 

Gas,  Ideal.— One  which  strictly  satisfies  the  equation  (pv  =  RTm)  and 
other  relations  deduced  from  the  classical  kinetic  theory  of  gases 
on  the  assumption  that  the  molecules  are  infinitely  small  and  devoid 
of  mutual  attraction.  7.  C.  T. 

Gravity,  Acceleration  of.— (g),  (ga),  [1/t2].  Unless  the  contrary  is  in- 
dicated, this  expression  refers  specifically  to  the  earth,  and  de- 
notes the  resultant  acceleration  downward  experienced  by  a  freely 
falling  body  placed  at  the  point  considered.  It  includes  centrifugal 
effects  arising  from  the  rotation  of  the  earth,  as  well  as  the  effects 
of  gravitational  attraction  (cf.  Gravity,  standard).  /.  C.  T. 

Hydrion.— Proposed  by  Walker  (1901)  to  replace  the  name  ' 'hydrogen 
ion,"  for  H+. 

International  electrical  units.— A  system  of  electrical  and  magnetic  units 
based  upon  the  ohm,  the  ampere,  and  secondarily  upon  the  volt, 
all  as  realized  by  certain  concrete  standards  which  have  been  in- 
ternationally agreed  upon,  and  upon  the  cgs.  units  for  such  other 
quantities  as  may  be  involved.  The  concrete  standards  have  been 
so  chosen  as  to  make  the  international  system  nearly  identical  with 
the  practical  system;  as  now  defined,  the  outstanding  discrepancy 
in  no  case  exceeds  52  parts  in  100,000.  In  distinguishing  between  the 
two  systems,  the  units  of  the  practical  system  are  described  as 
absolute,  those  of  the  other,  as  international.  The  introduction 
of  the  volt  as  a  secondary  unit  defined  by  a  concrete  standard 
(Weston  normal  cell  =  1.018300  Int.  volts  at  20°C.)  introduces  con- 
fusion when  measurements  of  high  precision  are  to  be  recorded. 
In  these  Tables,  values  based  upon  the  Int.  ohm  and  the  Int.  am- 
pere (as  defined  by  the  silver  voltameter)  are  denoted  by  (a).  Those 
based  on  the  Int.  ohm  and  the  Int.  volt  (as  defined  by  the  standard 
cell)  are  denoted  by  (v).  /.  C.  T. 

Ion. — From  luv,  "a  traveller,"  is  the  general  term  for  a  substance  which, 
by  reason  of  a  net  excess  positive  or  negative  charge  or  charges, 
travels  in  an  electric  field. 

lonogen. — A  term  proposed  by  Alexander  Smith  (1901)  for  a  material  which 
is  capable  of  forming  ions. 

Isobestic  point. — A  point  of  equal  "quenching,"  or,  as  applied  in  spec- 
trophotometry,  of  equal  extinction. 

Isohydric  solutions. — Solutions  of  the  same  hydrion  concentration,  or 
activity  (according  to  use). 

Joule.— [miyt2].  1.  Absolute  joule  =  107  ergs.  2.  International  joule 
=  work  expended  per  second  by  an  Int.  ampere  in  an  Int.  ohm. 
7.  C.  T. 

Kilo-.— Prefix  denoting  1,000.    7.  C.  T. 

Mega-.— Prefix  =  1,000,000.    7.  C.  T. 

Micro-.— Prefix  denoting  1/106.    7.  C.  T. 

Micron.— (M).     Unit  of  length  =  1/10.  m6  =  0.001  mm.    7.  C.  T. 

Milli-.— Prefix  =  0.001.    7.  C.  T. 


688  THE  DETERMINATION   OF  HYDROGEN  IONS 

Mobility  (of  ions  in  solution). — At  infinite  dilution  the  equivalent  con- 
ductance, Aoo,  was  stated  by  Kohlrausch  to  be  the  sum  of  two 
effects,  one  due  to  the  anions,  the  other  to  the  cations.  Kohlrausch 
called  these  the  mobilities  and  defined  the  mobilities  of  the  anions 
and  cations,  V  and  U,  respectively,  by  the  relation  Aoo  =  V  +  U. 

Molality. — The  number  of  moles  of  a  solute  in  1000  grams  of  solvent. 

Molarity. — The  number  of  moles  of  a  solute  in  1  liter  of  solution. 

Mole. — A  variable,  derived  unit  of  mass;  its  mass  is  numerically  equal  to 
the  molecular  weight  of  the  substance  measured.  The  expressions 
gram -mole,  kilogram -mole,  etc.  are  used  to  designate  the  basic  unit 
of  mass  employed.  Similarly  derived  units  based  upon  the  atomic 
weight,  the  formula  weight,  or  the  equivalent  are  called  the  gram- 
atom,  gram-formula  weight  or  gram-equivalent  when  the  gram  is 
the  basic  unit,  and  correspondingly  in  other  cases.  7.  C.  T. 

Molecular  weight. — (M).  The  sum  of  atomic  weights  of  all  the  atoms 
contained  in  a  molecule.  7.  C.  T. 

Normal.— A  concentration  of  one  gram-equivalent  per  liter.    7.  C.  T. 

Ohm. — (ft).  A  unit  of  electrical  resistance.  1.  Absolute  ohm  =  109 
cgsm.  units.  2.  International  ohm  is  the  resistance,  at  the  tem- 
perature of  melting  ice,  offered  to  an  unvarying  electric  current 
by  a  column  of  mercury,  of  constant  sectional  area,  having  a  mass 
of  14.4521  grams  and  a  length,  at  the  temperature  mentioned,  of 
106.300  cm.  7.  C.  T. 

Percent.— (%).  The  number  of  units  of  the  constituent  in  100  units  of 
the  mixture  containing  it.  If  units  of  volume  are  used,  the  ratio  is 
called  volume  per  cent;  if  units  of  mass,  it  is  called  mass  per  cent, 
weight  per  cent,  or  simply  per  cent.  (%  must  be  distinguished 
from  %0  which  is  frequently  used  to  denote  per  thousand.) — I.  C.  T. 

Phase. — "A  phase  is  any  part  of  a  system,  which  is  homogeneous  through- 
out; it  is  bounded  by  a  surface  and  is  mechanically  separable  from 
the  other  parts  of  the  system."  Hill  in  Taylor's  Treatise,  p.  370. 

Potential. — The  excess  of  the  potential  at  the  point  A  over  that  at  B, 
with  reference  to  any  quantity  ra,  is  the  mechanical  work  per  unit 
of  m  which  must  be  done  in  carrying  a  very  small  positive  amount 
of  m  from  B  to  A.  The  difference  in  electrical  potential  is  called 
electromotive  force,  emf,  E.  M.  F.,  potential  difference;  in 
magnetic  potential,  is  called  magnetomotive  force,  mmf .  7.  C.  T. 

Potential  gradient.— The  space  rate  of  increase  in  the  potential.  If  the 
direction  in  which  the  rate  to  be  measured  is  not  stated,  that  cor- 
responding to  the  maximum  gradient  is  to  be  understood.  7.  C.  T. 

Power. — The  time  rate  of  doing  work. 

Pressure.— (p),  (P).  [m/lt2].  Normal  force  per  unit  of  area.  A  hydro- 
static pressure  is  a  pressure  which  is  the  same  in  all  directions. 
7.  C.  T. 

Quadrant.— 1.  Unit  of  angle  =  90°.    7.  C.  T. 


APPENDIX  689 

Resistance. — 1.  The  electrical  resistance  of  a  body  between  two  specified 
equipotential  surfaces  is  E/I,  where  E  is  the  unchanging  difference 
in  the  potentials  of  the  surfaces  and  I  is  the  resulting  current  across 
any  transverse  section  between  them.  2.  Specific  resistance.  7. 
C.T. 

Solute. — A  component  of  a  solution  present  in  amount  smaller  than  that 
of  the  solvent. 

Solvent. — The  component  of  a  solution  present  in  the  largest  amount. 

Spectrum. — "The  spectrum  is  a  graphic  arrangement  or  setting  in  order 
of  radiant  energy  with  respect  to  wave-length  or  frequency."  Kept. 
Optical  Soc. 

Stoichiometric. — Pertaining  to  the  ratio  of  the  masses  of  the  several  ele- 
ments contained  in  a  pure  chemical  compound.  I.  C.  T. 

A  term  introduced  by  Richter  to  denote  the  determination  of  the 
relative  amounts  in  which  acids  and  bases  neutralize  one  another. 

Transport  number  (of  ions  in  solution). — "If  in  electrolysis  one  equiva- 
lent of  kation  is  deposited,  a  fraction  n  is  taken  from  the  immediate 
vicinity  of  the  electrode,  and  the  fraction  (1  —  n)  migrates  into 
the  kathode  space  from  the  bulk  of  the  solution.  Thus  n  equiva- 
lents of  anion  must  migrate  out  of  the  kathode  space  to  make  up 
the  total  charge  F  crossing  any  section  of  the  electrolyte.  The 

current  is  carried  by  anions  and  kations  in  the  ratio •    The 

1  —  n 

fraction  n  was  called  by  Hittorf  the  transport  number  of  the  anion. 
The  transport  number  of  the  kation  is  1  —  n."  See  Partington 
in  Taylor's  Treatise,  p.  543. 

Volt. — The  electrical  potential  difference  which,  when  steadily  applied 
to  a  conductor  having  a  resistance  of  one  ohm,  will  produce  in  it  a 
current  of  one  ampere  (cf.  absolute  and  international  units).  The 
Int.  Committee  authorized  by  the  London  Conference,  1908,  agreed 
to  regard  the  emf  of  the  Weston  normal  cell  at  20°C.  as  exactly  1.0183 
Int.  volts.  This  furnishes  a  subsidiary  definition  which  is  slightly 
discordant  with  the  primary  one.  These  tables  distinguish  be- 
tween the  two,  and  between  units  derived  from  them,  by  using  (a) 
to  denote  those  based  on  ampere  and  ohm,  and  (v)  to  denote  those 
based  on  volt  as  defined  by  the  Weston  cell.  7.  C.  T. 

Wave-length. — (A).  Distance  between  consecutive  corresponding  points 
in  a  monofrequent  wave  train.  Occasionally  applied  to  complex 
waves.  7.  C.  T. 

Weight. — The  force  with  which  a  body,  left  to  itself,  is  urged  towards  the 
earth.  In  the  absolute  systems  of  units  it  is  numerically  equal  to 
the  mass  of  the  body  multiplied  by  the  acceleration  of  gravity  (g) 
at  the  position  considered;  hence  varied  with  position.  Such  ex- 
pressions as  gram  weight  [pound  weight]  are  to  be  interpreted  as 
meaning  the  weight  of  a  gram  [a  pound]  at  a  place  where  g  has  the 
standard  value,  980.665  cm. /sec.2  7.  C.  T. 


LOGARITHMS  OF  NUMBERS 


^8 

PKOPOBTIONAL  PARTS 

•<  w 

K  « 

t>  a 

0 

1 

2 

3 

4 

5 

6 

7 

8 

9 

11 

1 

2 

3 

4 

5 

6 

7 

8 

9 

10 

0000 

0043 

0086 

0128 

0170 

0212 

0253 

0294 

0334 

0374 

4 

8 

12 

17 

21 

25 

29 

33 

37 

11 

0414 

0453 

0492 

0531 

0569 

0607 

0645 

0682 

0719 

0755 

4 

8 

11 

15 

19 

23 

26 

30 

34 

12 

0792 

0828 

0864 

0899 

0934 

0969 

1004 

1038 

1072 

1106 

3 

7 

10 

14 

17 

21 

24 

28 

31 

13 

1139 

1173 

1206 

1239 

1271 

1303 

1335 

1367 

1399 

1430 

3 

6 

10 

13 

16 

19 

23 

26 

29 

14 

1461 

1492 

1523 

1553 

1584 

1614 

1644 

1673 

1703 

1732 

3 

6 

9 

12 

15 

18 

21 

24 

27 

15 

1761 

1790 

1818 

1847 

1875 

1903 

1931 

1959 

1987 

2014 

3 

6 

8 

11 

14 

17 

20 

22 

25 

16 

2041 

2068 

2095 

2122 

2148 

2175 

2201 

2227 

2253 

2279 

3 

5 

8 

11 

13 

16 

18 

21 

24 

17 

2304 

2330 

2355 

2380 

2405 

2430 

2455 

2480 

2504 

2529 

2 

5 

7 

10 

12 

15 

17 

20 

22 

18 

2553 

2577 

2601 

2625 

2648 

2672 

2695 

2718 

2742 

2765 

2 

5 

7 

9 

12 

14 

16 

19 

21 

19 

2788 

2810 

2833 

2856 

2878 

2900 

2923 

2945 

2967 

2989 

2 

4 

7 

9 

11 

13 

16 

18 

20 

20 

3010 

3032 

3054 

3075 

3096 

3118 

3139 

3160 

3181 

3201 

2 

4 

6 

8 

11 

13 

15 

17 

19 

21 

3222 

3243 

3263 

3284 

3304 

3324 

3345 

3365 

3385 

3404 

2 

4 

6 

8 

10 

12 

14 

16 

18 

22 

3424 

3444 

3464 

3483 

3502 

3522 

3541 

3560 

3579 

3598 

2 

4 

6 

8 

10 

12 

14 

15 

17 

23 

3617 

3636 

3655 

3674 

3692 

3711 

3729 

3747 

3766 

3784 

2 

4 

6 

7 

9 

11 

13 

15 

17 

24 

3802 

3820 

3838 

3856 

3874 

3892 

3909 

3927 

3945 

3962 

2 

4 

5 

7 

9 

11 

12 

14 

16 

25 

3979 

3997 

4014 

4031 

4048 

4065 

4082 

4099 

4116 

4133 

2 

3 

5 

7 

9 

10 

12 

14 

15 

26 

4150 

4166 

4183 

4200 

4216 

4232 

4249 

4265 

4281 

4298 

2 

3 

5 

i 

8 

10 

11 

13 

15 

27 

4314 

4330 

4346 

4362 

4378 

4393 

4409 

4425 

4440 

4456 

2 

3 

5 

6 

8 

9 

11 

13 

14 

28 

4472 

4487 

4502 

4518 

4533 

4548 

4564 

4579 

4594 

4609 

2 

3 

5 

6 

8 

9 

11 

12 

14 

29 

4624 

4639 

4654 

4669 

4683 

4698 

4713 

4728 

4742 

4757 

1 

3 

4 

6 

7 

9 

10 

12 

13 

30 

4771 

4786 

4800 

4814 

4829 

4843 

4857 

4871 

4886 

49CO 

1 

3 

4 

6 

7 

9 

10 

11 

13 

31 

4914 

4928 

4942 

4955 

4969 

4983 

4997 

5011 

5024 

5038 

1 

4 

6 

7 

8 

10 

11 

12 

32 

5052 

5065 

5079 

5092 

5105 

5119 

5132 

5145 

5159 

5172 

1 

4 

7 

8 

9 

11 

12 

33 

5185 

5198 

5211 

5224 

5237 

5250 

5263 

5276 

5289 

5302 

1 

4 

6 

8 

9 

10 

12 

34 

5315 

5328 

5340 

5353 

5366 

5378 

5391 

5403 

5416 

5428 

1 

4 

6 

8 

9 

10 

11 

35 

5441 

5453 

5465 

5478 

5490 

5502 

5514 

5527 

5539 

5551 

1 

4 

6 

7 

9 

10 

11 

36 

5563 

5575 

5587 

5599 

5611 

5623 

5635 

5647 

5658 

5670 

1 

4 

6 

7 

8 

10 

11 

37 

5682 

5694 

5705 

5717 

5729 

5740 

5752 

5763 

5775 

5786 

1 

3 

6 

7 

8 

9 

10 

38 

5798 

5809 

5821 

5832 

5843 

5855 

5866 

5877 

5888 

5899 

1 

3 

6 

7 

8 

9 

10 

39 

5911 

5922 

5933 

5944 

5955 

5966 

5977 

5988 

5999 

6010 

1 

3 

4 

5 

7 

8 

9 

10 

40 

6021 

6031 

6042 

6053 

6064 

6075 

6085 

6096 

6107 

6117 

1 

4 

6 

8 

9 

10 

41 

8128 

6138 

6149 

6160 

6170 

6180 

6191 

6201 

6212 

6222 

1 

4 

6 

7 

8 

9 

42 

6232 

6243 

6253 

6263 

6274 

6284 

6294 

6304 

6314 

6325 

1 

4 

6 

7 

8 

9 

43 

6335 

6345 

6355 

6365 

6375 

6385 

6395 

6405 

6415 

6425 

1 

4 

6 

7 

8 

9 

44 

6435 

6444 

6454 

6464 

6474 

6484 

6493 

6503 

6513 

6522 

1 

4 

6 

7 

8 

9 

45 

6532 

6542 

6551 

6561 

6571 

6580 

6590 

6599 

6609 

6618 

4 

6 

7 

8 

9 

46 

6628 

6637 

6646 

6656 

6665 

6675 

6684 

6693 

6702 

6712 

4 

6 

7 

7 

8 

47 

6721 

6730 

6739 

6749 

6758 

6767 

6776 

6785 

6794 

6803 

4 

5 

6 

7 

8 

48 

6812 

6821 

6830 

6839 

6848 

6857 

6866 

6875 

6884 

6893 

4 

4 

C 

«J 

6 

7 

8 

49 

6902 

6911 

6920 

6928 

6937 

6946 

6955 

6964 

6972 

6981 

4 

4 

5 

6 

7 

8 

50 

6990 

6998 

7007 

7016 

7024 

7033 

7042 

7050 

7059 

7067 

1 

c 

4 

r 

«j 

6 

*T 
i 

8 

51 

7076 

7084 

7093 

7101 

7110 

7118 

7126 

7135 

7143 

7152 

1 

c 

4 

e 
O 

6 

7 

8 

52 

7160 

7168 

7177 

7185 

7193 

7202 

7210 

7218 

7226 

7235 

1 

c 

4 

Pj 

6 

7 

7 

53 

7243 

7251 

7259 

7267 

7275 

7284 

7292 

7300 

7308 

7316 

1 

o 

^ 

/j 

c 

6 

6 

7 

54 

7324 

7332 

7340 

7348 

7356 

7364 

7372 

7380 

7388 

7396 

1 

9 

3 

4 

K 
O 

6 

6 

7 

690 


LOGARITHMS  OP  NUMBERS — Continued 


a  8 

PROPORTIONAL  PARTS 

«  B 

0  3 
11 

1 

2 

3 

4 

5 

6 

_ 

1 

2 

3 

4 

5 

6 

7 

8 

9 

55 

7404 

7412 

7419 

7427 

7435 

7443 

7451 

7459 

7466 

7474 

1 

2 

2 

3 

4 

5 

5 

6 

7 

56 

7482 

7490 

7497 

7505 

7513 

7520 

7528 

7536 

7543 

7551 

1 

2 

2 

3 

4 

5 

5 

0 

7 

57 

7559 

7566 

7574 

7582 

7589 

7597 

7604 

7612 

7619 

7627 

1 

2 

2 

3 

4 

5 

5 

6 

7 

58 

7634 

7642 

7649 

7657 

7664 

7672 

7679 

7686 

7694 

7701 

1 

1 

2 

3 

4 

4 

5 

6 

7 

59 

7709 

7716 

7723 

7731 

7738 

7745 

7752 

7760 

7767 

7774 

1 

1 

2 

3 

4 

4 

5 

6 

7 

60 

7782 

7789 

7796 

7803 

7810 

7818 

7825 

7832 

7839 

7846 

1 

1 

2 

3 

4 

4 

5 

6 

6 

61 

7853 

7860 

7868 

7875 

7882 

7889 

7896 

7903 

7910 

7917 

1 

1 

2 

3 

4 

4 

5 

6 

6 

62 

7924 

7931 

7938 

7945 

7952 

7959 

7966 

7973 

7980 

7987 

1 

1 

2 

3 

3 

4 

5 

G 

6 

63 

7993 

8000 

8007 

8014 

8021 

8028 

8035 

8041 

8048 

8055 

1 

1 

2 

3 

3 

4 

5 

5 

6 

64 

8062 

8069 

8075 

8082 

8089 

8096 

8102 

8109 

8116 

8122 

1 

1 

2 

3 

3 

4 

5 

5 

6 

65 

8129 

8136 

8142 

8149 

8156 

8162 

8169 

8176 

8182 

8189 

1 

1 

2 

3 

3 

4 

5 

5 

6 

66 

8195 

8202 

8209 

8215 

8222 

8228 

8235 

8241 

8248 

8254 

1 

1 

2 

3 

3 

4 

5 

5 

6 

67 

8261 

8267 

8274 

8280 

8287 

8293 

8299 

8306 

8312 

8319 

1 

1 

2 

3 

3 

4 

5 

5 

6 

68 

8325 

8331 

8338 

8344 

8351 

8357 

8363 

8370 

8376 

8382 

1 

1 

2 

3 

3 

4 

4 

5 

6 

69 

8388 

8395 

8401 

8407 

8414 

8420 

8426 

8432 

8439 

8445 

1 

1 

2 

2 

3 

4 

4 

5 

6 

70 

8451 

8457 

8463 

8470 

8476 

8482 

8488 

8494 

8500 

8506 

1 

2 

2 

3 

4 

4 

5 

6 

71 

8513 

8519 

8525 

8531 

8537 

8543 

8549 

8555 

8561 

8567 

1 

2 

2 

3 

4 

4 

5 

5 

72 

8573 

8579 

8585 

8591 

8597 

8603 

8609 

8615 

8621 

8627 

1 

2 

2 

3 

4 

4 

5 

5 

73 

8633 

8639 

8645 

8651 

8657 

8663 

8669 

8675 

8681 

8686 

1 

2 

2 

3 

4 

4 

5 

5 

74 

8692 

8698 

8704 

8710 

8716 

8722 

8727 

8733 

8739 

8745 

1 

2 

2 

3 

4 

4 

5 

5 

75 

8751 

8756 

8762 

8768 

8774 

8779 

8785 

8791 

8797 

8802 

1 

1 

2 

2 

3 

3 

4 

5 

5 

76 

8808 

8814 

8820 

8825 

8831 

8837 

8842 

8848 

8854 

8859 

1 

1 

2 

2 

3 

3 

4 

5 

5 

77 

8865 

8871 

8876 

8882 

8887 

8893 

8899 

8904 

8910 

8915 

1 

1 

2 

2 

3 

3 

4 

4 

5 

78 

8921 

8927 

8932 

8938 

8943 

8949 

8954 

8960 

8965 

8971 

1 

1 

2 

2 

3 

3 

4 

4 

5 

79 

8976 

8982 

8987 

8993 

8998 

9004 

9009 

9015 

9020 

9025 

1 

1 

2 

2 

3 

3 

4 

4 

5 

80 

9031 

9036 

9042 

9047 

9053 

9058 

9063 

9069 

9074 

9079 

1 

2 

2 

3 

3 

4 

4 

5 

81 

9085 

9090 

9096 

9101 

9106 

9112 

9117 

9122 

9128 

9133 

1 

2 

2 

3 

3 

4 

4 

5 

82 

9138 

9143 

9149 

9154 

9159 

9165 

9170 

9175 

9180 

9186 

1 

2 

2 

3 

3 

4 

4 

5 

83 

9191 

9196 

9201 

9206 

9212 

9217 

9222 

9227 

9232 

9238 

1 

2 

2 

3 

3 

4 

4 

5 

84 

9243 

9248 

9253 

9258 

9263 

9269 

9274 

9279 

9284 

9289 

1 

2 

2 

3 

3 

4 

4 

5 

85 

9294 

9299 

9304 

9309 

9315 

9320 

9325 

9330 

9335 

9340 

1 

1 

2 

o 

£ 

3 

3 

4 

4 

5 

86 

9345 

9350 

9355 

9360 

9365 

9370 

9375 

9380 

9385 

9390 

1 

1 

2 

2 

3 

3 

4 

4 

5 

87 

9395 

9400 

9405 

9410 

9415 

9420 

9425 

9430 

9435 

9440 

0 

1 

1 

2 

2 

3 

3 

4 

4 

88 

9445 

9450 

9455 

9460 

9465 

9469 

9474 

9479 

9484 

9489 

0 

1 

1 

2 

2 

3 

3 

4 

4 

89 

9494 

9499 

9504 

9509 

9513 

9518 

9523 

9528 

9533 

9538 

0 

1 

1 

2 

2 

3 

3 

4 

4 

90 

9542 

9547 

9552 

9557 

9562 

9566 

9571 

9576 

9581 

9586 

0 

1 

1 

2 

2 

3 

3 

4 

4 

91 

9590 

9595 

9600 

9605 

9609 

9614 

9619 

9624 

9628 

9633 

0 

1 

1 

2 

2 

3 

3 

4 

4 

92 

9638 

9643 

9647 

9652 

9657 

9661 

9666 

9671 

9675 

9680 

0 

1 

1 

2 

2 

3 

3 

4 

4 

93 

9685 

9689 

9694 

9699 

9703 

9708 

9713 

9717 

9722 

9727 

0 

1 

1 

2 

2 

3 

3 

4 

4 

94 

9731 

9736 

9741 

9745 

9750 

9754 

9759 

9763 

9768 

9773 

0 

1 

1 

2 

2 

3 

3 

4 

4 

95 

9777 

9782 

9786 

9791 

9795 

9800 

9805 

9809 

9814 

9818 

0 

1 

1 

2 

2 

3 

3 

4 

4 

96 

9823 

9827 

9832 

9836 

9841 

9845 

9850 

9854 

9859 

9863 

0 

1 

1 

2 

2 

3 

3 

4 

4 

97 

9868 

9872 

9877 

9881 

9886 

9890 

9894 

9899 

9903 

9908 

0 

1 

1 

2 

2 

3 

3 

4 

4 

98 

9912 

9917 

9921 

9926 

9930 

9934 

9939 

9943 

9948 

9952 

0 

1 

1 

2 

2 

3 

3 

4 

4 

99 

9956 

9961 

9965 

9969 

9974 

9978 

9983 

9987 

9991 

9996 

0 

1 

1 

2 

2 

3 

3 

3 

4 

691 


INDEX  OF  AUTHORS 


(Exclusive  of  those  referred  to  in  pages  555  to  586  and  page  87) 


Abegg,  257,  279,  312,  316,  390,  400 
Acree,  70,  95,  111,  112,  116,  159,  215, 

216,  261,  274,  278,  310,  312,  672 
Adams,  38,  110,  159,  498,  541 
Allmand,  426 
Andrews,  289,  290 
Arakawa,  417 
Archibald,  309 
Arnd,  411,  417 
Arndt,  188 
Arrhenius,  489,  554 
Arthur,  429 

Aten,  276,  278,  299,  426,  439,  440 
Atkins,  215 

Auerbach,  257,  312,  316,  390,  417,  474 
Austin,  459 
Avery,  138,  216 

Bach,  354 

Baeyer,  70 

Baggesgaard-Rasmussen,  416 

Baker,  159,  417 

Balch,  417 

Barendrecht,  297 

Barnett,  122,  123,  170 

Bass,  476 

Bausch  and  Lomb,  170 

Baver,  417 

Baylis,  417,  428 

Bayliss,  433,  437 

Beans,  287,  288,  302,  327,  443 

Beattie,  J.  A.,  313,  315,  316,  472 

Beattie,  R.,  339 

Beilstein,  75 

Beinfait,  331 

Beling,  417 

Bennett,  338 

Berggren,  672 


Biilmann,  352,  353,  385,  404,  410,  411, 
413,  414,  415,  416,  417,  418,  420,  441, 
442,  487 

Birge,  159 

Bischoff,  173 

Bishop,  547 

Bjerrum,  15,  33,  68,  170,  180,  273, 
274,  277,  279,  280,  312,  473,  474, 
475,  477,  478,  485,  532,  541,  554, 
680 

Blackadder,  288,  437 

Blackwood,  176 

Bodforss,  417 

Bodine,  300 

Bodlander,  400 

Bogen,  97 

Bogert,  69 

Bohi,  44 

Bolam,  513 

Boltger,  439 

Borelius,  433 

Bosch,  417 

Bose,  292 

Bottger,  554 

Bourgeaud,  444 

Bovie,  53,  300,  339,  439,  442 

Bray,  445 

Bredig,  513 

Brightman,  159 

Brighton,  44,  95,  274,  286,  288,  290, 
305,  309,  313,  323,  352,  453 

Bridges,  271 

Brinkman,  332,  342,  414,  417 

Brioux,  417 

Britton,  287,  439 

Erode,  151,  152,  157,  176 

Brodel,  174 

Bronfenbrenner,  117 


694 


INDEX    OF   AUTHORS 


Br0nsted,  49,  187,  315,  316,  401,  426, 
498,  510,  514, 515,  516,  519,  540,  541, 
542 

Breslau,  174 

Brown,  95,  140,  340,  357,  432,  433 

Browne,  438 

Bru6re,  159,  174 

Bruin,  439,  440 

Brunius,  416 

Buch,  159 

Buckmaster,  173 

Bugarzsky,  554 

Bunker,  299 

Burdick,  283 

Burton,  495 

Butler,  415 

Buytendyk,  332,  342,  414,  417,  427 

Calhane,  332 

Campbell,  176 

Cannan,  385,  392 

Carr,  97 

Cassel,  429 

Centners  zwer,  442 

Chandler,  678 

Chanoz,  273 

Chapman,  122,  123 

Chow,  426 

Clark,  38,  70,  71,  76,  91,  94,  95,  120, 
138,  185,  189,  192,  194,  202,  204, 
262,  286,  294,  297,  300,  302,  312, 
362,  370,  384,  385,  386,  387,  399, 
402,  415,  437,  444,  446,  450,  456, 
476,  478,  485,  509 

Clark,  G.  L.,  518 

Clarke,  515 

Clibbens,  513 

Cohen,  A.,  98 

Cohen,  B.,  70,  71,  91,  94,  119,  157, 
183,  184,  186,  289,  300,  384,  385, 
386,  399,  402,  415 

Cohn,  75 

Cohn,  E.  J.,  42,  192,  204,  215,  216, 
218, 219,  476,  506,  508,  509,  672,  678 

Compte,  552 

Compton,  339 


Conant,  285,  339,  413,  417,  418,  544, 

545 

Conn,  123 
Conover,  194 
Conway-Verney,  437 
Cooledge,  172 
Cooper,  415 
Coran,  415,  416 
Cornec,  518 
Cornog,  197 
Corran,  413 
Cottrell,  282 
Cowperthwaite,  273 
Cox,  537 

Cray,  417,  547,  548 
Cremer,  433 
Crooks,  272 
Cullen,  138,  294,  411,  416,  436,  446, 

459,  476,  477,  486 
Gumming,  270,  271,  273,  279 
Gushing,  332 
Czepinski,  261 
Czerwinski,  678 

Daniel,  98,  417 

Danneel,  400 

Banner,  539 

Darmois,  417 

Dassler,  152,  153,  547 

Davidoff,  310 

Davidson,  159 

Dawson,  191,  516 

Debye,  60,  463,  464,  467,  489,  490, 

494,  495,  498 
De  Eds,  332 
Derrien,  38 
Desha,  173 
Diehl,  81,  144 
Dietrich,  518 
Dietzel,  417 
Dixon,  399,  402,  529 
Dodge,  193,  194,  197,  485 
Dolezalek,  292 
Domontvich,  416 
Donnan,  426 
Dorsey,  248 


INDEX   OF  AUTHORS 


695 


Douglas,  182,  184 
Draves,  437 
Drucker,  279 
Dubois,  190 
Durgin,  195 
Dushman,  492 
Dutoit,  518 

Earle,  416 

Eberlein,  400 

Ebert,  158,  178,  417,  511,  548 

Eggert,  293 

Eilert,  284 

Elliott,  316 

Ellis,  H.  A.,  139 

Ellis,  J.  H.,  261,  287,  288,  297,  310, 

316 

Elvove,  71 
Elveden,  353 
Engel,  430 
Eppley,  344,  349 
Etienne,  444 
Ettisch,  413,  433 
Evans,  436 
Evers,  97,  139 
Ewing,  307,  672 

Tales,  272,  273,  274,  278,  305,  313, 

358,  454,  455,  672 
Farkas,  297 
Fels,  68 
Felton,  97,  139 
Fenwick,  275,  276,  427 
Fernbach,  50 
Fieser,  385,  413,  417 
Finger,  282 
Fink,  301 
Fontes,  38 
Forbes,  69,  96 
Foster,  32 
Foulk,  198 
Fraenkel,  513,  514 
Franklin,  544 
Franzen,  350 
Freude,  70 
Freundlich,  417,  433 
Fricke,  274,  426,  540 


Fried,  426,  428 
Friedenthal,  38,  68 
Frivold,  541 
Fromageot,  159 

Fujita,  272,  273,  279,  280,  487,  672 
Furman,  32,  44,  135,  429,  450,  538, 
554,  679 

Gaede,  353 

Galwialo,  302 

Gardiner,  176 

Garmendia,  459 

Geake,  513,  515 

Geddes,  292,  349 

Geidel,  175 

Gelfan,  272,  302 

Gerke,  292,  316,  349 

Germann,  548 

Gerretsen,  170 

Gesell,  341,  427,  428 

Gibbs,  194,  239,  240,  384,  385,  386, 

399,  402,  494 
Gibson,  160 
Giesy,  429 
Gilbert,  439 
Gil  christ,  271,  273 
Gillespie,  121,  122,  133,  168,  170,  445 
Giribaldo,  38 
Gjaldbaek,  309,  314,  477 
Goard,  429 
Gooch,  283 
Goode,  330,  331,  332 
Gowlett,  332 
Grabowski,  69 
Gray,  349 
Green,  75 
Greer,  416 
Grieg-Smith,  174 
Grobet,  518 
Gronwall,  495,  502 
Gross,  433 
Grossman,  413,  416 
Grunberg,  98 
Guild,  159 
Guillaumin,  38 

Giintelberg,  310,  315,  316,  354 
Guyemant,  96,  131,  133,  459 


696 


INDEX    OF   AUTHORS 


Haber,  400,  430,  431,  433 

Hainsworth,  261 

Halban,  158,  176,  178,  511 

Hall,  339,  418,  544,  545. 

Halpern,  433 

Halpert,  302,  444 

Hammett,  284, 285, 287,  288, 289,  302, 

441,  443,  446 
Hantzsch,  118 
Harkins,  518 
Harned,  268,  270,  280,  286,  288,  439, 

474,  672 
Harris,  417 
Harrison,  173 
Hartong,  426 
Haskins,  174 
Hasselbalch,  292,  444 
Hastings,  103,  125,  126,  127,  128,  170, 

187,  212,  294,  300,  436,  458,  459, 

476,  481,  510,  511,  678 
Hawes,  672 
Hay,  190 
Heinrich,  350 
Heintz,  515 
Helmholtz,  238,  431 
Henderson,  51,  53,  69,  96,  554 
Henderson,  P.,  270 
Henri,  159 
Henriques,  417 
Hendrixson,  485 
Hertzman,  341,  427,  428 
Hey,  415 

Heydweiller,  43,  44,  458 
Heyroth,  192,  215,  216,  219,  476,  509, 

678 

Hickman,  175,  517 
Hildebrand,  159,  299,  324,  547 
Hill,  517 
Hirsch,  159 
Hissink,  417 
Hittorf,  689 
Hjort,  176 
Hober,  444,  445 
Hock,  97 
Hoet,  433 
Hofmann,  289 
Hollingsworth,  198 


Holmes,  94,  155,  156,  157,  158,  159 

Honnelaitre,  417 

Hopfield,  95 

Horn,  430,  433 

Horovitz,  430,  431,  433 

Hosoda,  417 

Hostetter,  365 

Hottinger,  69 

Houben,  98 

Huang,  273 

Hubert,  50 

Hubbard,  95 

Hlickel,  60,  464,  467,  489,  490,  494, 

495,  502 
Hugh,  514 

Hughes,  430,  431,  433 
Hugonin,  417 
Hulett,  307,  343,  364 
Kurd,  430 
Hurwitz,  172 
Hutchinson,  159 
Hyndman,  517 

Isgarischev,  439 
Itano,  417 

Jahn,  316,  463 
Janke,  174 
Jellinek,  678 
Jensen,  353,  418,  441 
Johnson,  270 
Johnston,  445 
Jones,  159,  195,  538 
J0rgensen,  174 
Joule,  246,  687 
Julius,  74 

Kahn,  385,  413 

Kakinuma,  279,  487,  672 

Kappen,  417 

Kargin,  417 

Karsmark,  416 

Katagiri,  417 

Katz,  433 

Keeler,  429,  476,  477,  486 

Keeley,  340 

Keller,  300,  520 


INDEX    OF   AUTHORS 


697 


Kerridge,  340,  357,  431,  432,  433 

Ketranek,  426 

Keuffel,  145 

Kilpatrick,  516 

Kimball,  672 

King,  332,  515 

Kilpinger,  340 

Kittridge,  547 

Klemenziewicz,  430,  431,  433 

Klit,  417,  442 

Knobel,  300,  426 

Knudsen,  416 

Kodama,  416,  417 

Koefoed,  312 

Koehler,  439 

Kohlrausch,  43,  44,  458 

Koldaewa,  439 

Kolthoff,  32,  38,  44,  69,  98,  134,  135, 
139,  170,  174,  181,  183,  188,  215, 
216,  409,  411,  417,  426,  428,  429, 
450,  456,  457,  458,  459,  477,  486, 
516,  538,  547,  554,  679 

Konikoff,  292 

Kopacewski,  554 

Koppel,  54,  57 

Kropacsy,  174 

Kriiger,  338,  487,  509 

Kubelka,  438 

Kurtz,  385,  413 

Laar,  106 

Lamb,  273,  274,  426 

Lamble,  515 

Lambling,  38 

LaMer,  385,  413,  417,  468,  495,  502, 

503,  515 

LaMotte  Co.,  140 
Lange,  439,  440 
Langmuir,  380,  400 
Larrson,  417,  548 
Larson,  273,  274,  426 
Larsson,  477,  678 
Lavoisier,  1 

Leeds  and  Northrup,  341 
Ledig,  296 
Lehfeldt,  400 
Lehmann,  54,  301 


Lepper,  436 

Lester,  409,  416 

Levene,  31 

Levine,  476 

Levy,  69,  70 

Lewis,  G.  N.,  44,  49,  237,  238,  257, 
261,  268,  269,  273,  274,  286,  288, 
290,  305,  309,  312,  313,  315,  316, 
323,  352,  394,  395,  450,  451,  452, 
458,  463,  472,  499 

Lewis,  W.  McC.,  266,  413,  415,  416, 
515 

Liebermann,  554 

Liu,  416 

Lindemann,  340 

Linderstr0m-Lang,  31,  39,  276,  277, 
279,  314,  409,  416,  417,  439,  450, 
472,  476,  479,  480,  481,  486,  547,  672 

Lindhard,  139 

Linhart,  316,  467 

Linstead,  175 

Lipscomb,  307 

Lizius,  97 

Lodge,  380 

Long,  297,  433 

Loomis,  261,  278,  310,  312,  672 

Loose,  69 

Lorenz,  44 

Lowey,  176 

Lowry,  49 

Lubs,  70,  91,  94,  95,  111,  112,  120, 
138, 185, 189, 192, 194, 202, 204,  262, 
286,  312,  437,  456,  476,  478,  485,  509 

Lucretius,  8 

Lund,  69,  159,  410,  411,  439,  548 

Luther,  257,  312,  316,  390 

McBain,  190,  513 
McClendon,  182,  297,  302,  444 
McCrae,  170 
MacDougall,  316 
McGill,  416,  417 
McGinty,  428 
McHenry,  429 
Mclnerney,  136 

Maclnnes,  261,  269,  273,  274,  275, 
315,  316,  517,  538 


INDEX   OF  AUTHORS 


Mcllvaine,  214 

McKelvy,  307 

Maddison,  426 

Magoon,  297 

Mains,  364 

Malaprade,  429 

Mallock,  8 

Marks,  433 

Marriott,  69,  70 

Martin,  436 

Meacham,  95 

Meeker,  95,  416 

Meillere,  283 

Mellet,  173 

Mellon,  216 

Mellor,  553 

Menkin,  193,  215,  216,  219,  476,  509, 
678 

Menzel,  338 

Meyer,  172 

Meyers,  274 

Michaelis,  44,  45,  46,  54,  96,  127,  131, 
133,  172,  183,  188,  202,  272,  273, 
279,  280,  292,  297,  300,  310,  313, 
430,  439,  444,  454,  455,  459,  483, 
486,  487,  509,  540,  541,  547,  554,  672 

Miller,  182,  184 

Millet,  548 

Mills,  1 

Milner,  60,  489,  494 

Mines,  170 

Mislowitzer,  338,  413,  416,  450,  554 

Mizutani,  487,  547,  555 

Moir,  97,  159 

Monier-Williams,  299 

Montillon,  429 

Mook,  332,  342,  417 

Moore,  50 

Morse,  67 

Morton,  159 

Moser,  350 

Mozolowski,  283,  413 

Mudge,  274,  313,  454,  455,  672 

Mueller,  495 

Miiller,  176,  338,  538,  548 

Murdick,  437 

Murray,  481,  547 

Myers,  170,  310,  672 


Nachtwey,  188 

Naegeli,  140,  204,  583 

Naray-Syabo,  429 

Needham,  139 

Nernst,  68,  252,  266,  270,  373 

Neukrich,  302,  444 

Neukircher,  417 

Nicholas,  415 

Niese,  353 

Niklas,  97 

Nonhebel,  265,  468 

Noyes,  114,  316,  502,  532,  554 

Oakes,  327,  437 
Ogg,  303 
Olsen,  417 
Onsager,  463 
Orndorff,  95 
Oser,  416 
Ostenberg,  172 
Osterhout,  517 
Ostwald,  100,  305 
O'Sullivan,  416 

Paine,  417 

Palitzsch,  69,  70,  179,  180,  182,  205, 

213 

Palmaer,  313 
Pantin,  215 
Paracelsus,  1 
Parker,  316,  417,  428,  466 
Parnas,  283,  413 
Parsons,  182,  184,  413,  417 
Partridge,  176 
Patten,  364,  400 
Paulus,  159 
Peard,  184 
Pedersen,  516 
Felling,  416 

Perlzweig,  32,  54,  540,  554 
Pfeiffer,  139 
Pien,  417 
Pinkof,  316 
Planck,  270 
Poggendorf,  317,  332 
Poma,  279 
Pope,  332 
Popoff,  429,  538 


INDEX   OF  AUTHORS 


Porter,  395 

Prideaux,  75,  96,  153,  159,  182,  215, 

272,  288,  439,  555 
Pring,  417,  548 
Pringsheim,  173 

Rabinowitsch,  417 

Radsimowska,  302 

Ralston,  429 

Ramage,  182,  184 

Randall,  237,  261,  310,  312,  313,  316, 

394,  395,  451,  452,  468,  472 
Rapkine,  139 
Rawlings,  299 
Rebello,  135 
Rehberg,  536 
Reimann,  176 
Reinhard,  159 
Reiss,  189,  299 
Remsen,  69 
Rheinberg,  283 
Rice,  302,  515 
Richards,  309 
Richter,  38,  689 
Rideal,  251,  413,  417,  429 
Rider,  302 
Risch,  174 
Roaf,  50,  428 
Roberts,  275,  276,  427 
Robinson,  459,  476,  477,  486 
Robl,  173 

Robson,  103,  125,  126,  127,  128,  459 
Roche,  416,  513,  514 
Rodebush,  380 
Rona,  292,  433,  555 
Rosanoff,  515 
Rosenbaum,  417 
Rosenstein,  110,  159 
Ross,  195 
Rowley,  261 
Rowe,  76 
Rowntree,  69,  70 
Runge,  416 
Rupert,  261,  273 
Rupp,  E.,  69 
Rupp,  P.,  68 


St.  Johnston,  184 

Salessky,  68 

Salisbury,  437 

Salm,  68,  75,  101 

Sand,  324 

Sandred,  495,  502 

Sannie",  300 

Sargent,  261,  268,  269,  309 

Sauer,  309,  453 

Saunders,  95,  164 

Scatchard,  69, 265, 269,  276, 278,  316, 

455,  465,  467,  468,  469,  470,  471, 

472,  474,  512,  516,  539 
Schaede,  302,  444 
Schaefer,  416 
Scheitz,  67 
Schielding,  434 
Schiller,  433 
Schmid,  300 

Schmidt,  C.  L.  A.,  32,  282,  440 
Schmidt,  O.,  416 
Schmidt,  F.,  416,  417 
Schneider,  430,  433 
Schoorl,  458 

Schreiner,  411,  417,  540,  541,  548 
Schuhmann,  427 
Schultz,  74,  76 
Scudder,  460,  678 
Sebastian,  44,  274,  286,  288,  290,  305, 

309,  323,  352,  453 
Sendroy,  103,  125,  126,  127,  128,  187, 

212,  458,  459,  476,  481,  510,  511,  678 
Sharp,  136,  316 
Shepherd,  M.,  296 
Sheppard,  S.  E.,  316 
Sherrill,  173 
Shoemaker,  307 
Shou,  416 
Sibley,  515 
Siedentorff,  176 
Siegler-Soru,  159 
Siemers,  411,  417 
Simms,  31,  299,  306,  476 
Slagle,  111 
Small,  418 
Smith,  428,  429,  687 
Smolczyk,  417 


700 


INDEX   OF  AUTHORS 


Smolik,  413 

Snyder,  94,  159,  417 

Sohon,  70 

Solowiew,  302 

Sonden,  174 

S0rensen,  31,  36,  37,  39,  42,  68,  69, 
75,  90,  133,  170,  172,  179,  180,  185, 
188,  192,  202,  203,  204,  205,  211, 
276,  277,  279,  297,  312,  314,  409, 
417,  439,  450,  453,  456,  472,  473, 
474,  475,  476,  477,  479,  480,  481, 
485,  486,  509,  554,  672 

Sosman,  365 

Spiro,  54,  57 

Stadie,  459,  672 

Stammelman,  272 

v.  Steiger,  433 

Stenstrom,  159 

Stieglitz,  113,  116 

Stoney,  686 

Straumanis,  442 

Sullivan,  385 

Swyngedauw,  300,  444 

Tartar,  437 

Taub,  174 

Taufel,  57 

Taylor,  271,  302,  418 

Tekelenburg,  450,  457,  458,  477,  486 

Thiel,  69,  81,  144,  152,  153,  547 

Tian,  362 

Tilley,  429 

Tipping,  159 

Tovborg-Jensen,  417 

Tower,  428 

Treadwell,  332 

Troland,  161 

Uhl,  426 
Ulrich,  139 

Vana,  416 

Van  Alstine,  125 

Van  Dalfsen,  276,  278,  426 

Van  der  Meulen,  429 

Van  der  Bijl,  332 

Van  der  Spek,  417 


Van  Ginneken,  299,  439 
Vanselow,  468 

Van  Slyke,  54,  56,  57,  215,  678 
Van't  Hoff,  8 

Vellinger,  299,  416,  427,  454,  455,  554 
Verain,  444 
Verney,  433 
Vernon,  430 
Viebel,  419 
Vinal,  345,  349 
Vincent,  555 
Vleeschhouwer,  215,  216 
Vies,  139,  156,  159,  299,  427 
Voegtlin,  332 

Vosburgh,  273,  278,  305,  344,  358, 
354,  672 

Wagener,  416,  417 

Wagner,  57,  438 

Walbum,  67,  206,  211,  456 

Walden,  539,  548 

Walker,  445,  687 

Walpole,  20,  21,  24,  42,  67,  69,  134, 
135,  137,  171,  172,  192,  205,  215, 
272,  273,  297,  299,  305,  479,  484, 
485,  672 

Walther,  139 

Walsh,  150,  176 

Warburg,  445 

Ward,  96,  215 

Washburn,  51 

Waters,  307,  343 

Wegscheider,  116 

Wells,  184 

Wendt,  332 

Westhaver,  283 

Westrip,  417,  547,  548 

Weyl,  273 

Wherry,  38,  136,  170 

White,  70,  111,  358 

Whitenack,  331 

Whitley,  50 

Wickers,  287,  288 

Wijs,  43 

Wilcoxon,  429 

Wilke,  300 

Williams,  331 


INDEX   OF  AUTHORS  70 1 

Williamson,  188  Wulf,  261 

Wilson,  494  Wulff,  135 

Windish,  518  Wtilfken,  152,  153,  547 

Winterstein,  301 

Wladimiroff,  302  Yeh,  269,  274,  275 

Woerdeman,  426  Young,  310,  316,  468,  472 

Wolf,  431 

Wolff,  307,  343,  345  Zimmermann,  430,  433 

Wood,  173,  437,  517  Zoller,  188 

Wu,  170  Zsigmondy,  117 


INDEX  OF  SUBJECTS 


(Exclusive  of  material  in  table'8) 


A  (free  energy,  Helmholtz),  238 

a,  see  ionic  diameter 

a,  see  activity 

a,  see  degree  of  dissociation;  table 


of  log 


-,77 


Absolute,  potential,  275,  ,312;  tem- 
perature, 245;  versus  international 
units,  247, 249 

Absorption  (light),  100,  141;  curves, 
144,  151,  152,  175;  formula,  143; 
index,  145;  salt-effect,  158,  178; 
by  solvent,  143 

Acetate,  20,  24,  42;  arbitrary  stand- 
ard, 522;  activity  coefficient,  476, 
507,  508;  buffer  index,  57;  buffer 
tables,  219;  temperature  coeffi- 
cient, 457,  459;  standard,  42,  223, 
483-485,  672 

Acetic  acid,  20,  24,  42;  dissociation 
constant,  517;  pK,  678;  solutions, 
544 

"Acid,"  1 

Acid,  agglutination,  555;  classifica- 
tion, 1,  7;  concentrated,  41;  color, 
63;  defined,  3,  49,  519,  541-542; 
dissociation    constants,    15,    678; 
multivalent,    26,    111;    pure,    12, 
40;  strength  of,  11,  578;  strong,  11, 
33,  53;  weak,  11,  526 
"Active  acidity,"  38 
Activity,  39,  60,  178,  236,  256,  268, 
568;  defined,  236,  240;  coefficient, 
178,  217,  236,  241,  243,  408,  476, 
490,  498-511,  516,  541,  562,  584; 
coefficient  defined,  236,  241;  elec- 
tron, 376;  of  solid  phases,  426 
Adsorption,  53,  135,  565,  571;  buffer 

effect  and,  53 
Agar-KCl,  272;  bridge,  273 


Agglutination,  31,  104 
Air  bath,  297 
Alanine,  32 
Alcohol  solutions,  547 
Alizarin,   74,    188;   green,   73;   sul- 
fonate,  183;  Yellow  GG,  96,  127, 
128,  129;  Yellow  R,  93 
"Alkali,"  1 

Alkali,  standard,  195-198 
Alkaline,  2;  color,  63;  solutions  and 
H-potential,   289;   solutions   and 
difficulty  of   pH   measurements, 
441 

Alkalinity,  2,  17 

Alkaloids,    dissociation   constants, 
681;  electrode  poisons,  439;  indi- 
cator error,  188 
Alternate   method   of   formulating 

acid  base  equilibria,  519 
Alternating  current  for  calomel,  307; 

for  mercurous  sulfate,  344 
Aluminum  and  alizarin,  188 
Amalgam,  Cd,  343;  Na  for  alkali, 

197;  electrodes,  396 
Amalgamation  of  Ft,  306,  344 
Amino  acids,  dissociation  constants, 

680;  curves,  32;  separation,  555 
Amino  benzoic  acid,  29 
Ammeter  potentiometer,  325 
Ammonia,  47;  buffers,  180;  electrode 
poison,   439;  equilibria,   48,   545; 
indicators  in,  517 
Ammonium  ion,  545 
Ammonium  nitrate  in  liquid  junc- 
tion, 279 

Amoeboid  movement,  580 
Ampere,  247,  319,  684 
Ampholytes,  26,  27,  32,  583;  disso- 
ciation exponents,  680 
Amplitude  of  vibration,  148-149 


703 


704 


INDEX   OF   SUBJECTS 


Analyses,  pH  in,  555 

Angstrom  unit,  142,  685 

Anion,  685 

Anode,  685 

Anthraquinone  indicators,  74,  86; 
2-7,  sulfonic  acid,  385 

Antigens,  576 

Antigenic  action,  556 

Antimony  electrode,  426 

Apparent  dissociation  constant, 
121,  562 

Approximate  equation,  16,  22 

Approximations  with  indicators, 
119 

Arginine,  32 

Armored  wire,  358  r 

Arrhenius,  picture,  facing  489 

Arsenic,  electrode  poison,  439 

Artificial  color  standards,  174 

Asparagine,  41 

Association,  constant,  11,  542;  ex- 
ponents, 679,  680;  of  ions,  58 

Atmosphere,  246,  685 

Automatic  control,  176,  244,  577 

Avagadro  number,  491,  519,  685 

Azine  indicators,  73,  77,  85 

Azo,  indicators,  70,  72;  Yellow  3G, 
181 

Azolitmin,  67,  183,  459 

Azurine  G,  306 

0,  see  buffer  index 

Bacteria,  agglutination  of,  104,  dif- 
ferentiation of,  138;  growth  of,  104 

Bacteriology,  pH  in,  136,  555 

Bacteriophage,  556 

Bacteriostatic  action,  556 

Bakelite,  357 

Balanced  neutrality,  50 

Ballistic  galvanometer,  327 

Barometer  and  barometric  correc- 
tions, 246,  260,  443,  675,  676 

Base,  2;  defined,  3, 519,  541,  542;  dis- 
sociation constants,  679;  formula- 
tion of  equilibria,  17,  47;  strong, 
33,  49;  weak,  49 

Baths,  358,  359 


Batteries,  330,  346 

Beer,  576 

Beer's  law,  144,  167 

Benzene-azo-,  a-naphthylamine,  92, 
185;  -benzylaniline,  92,  185;  -di- 
methylaniline,  92;  -diphenyla- 
mine,  92,  185 

Benzene  sulfonic  acid  azo-,  benzyl- 
aniline,  185;  -a-naphthol,  183; 
-a-naphthylamine,  93,  185;  -naph- 
thylamine,  183;  -m-chlorodiethyl 
aniline,  92,  185 

Benzoquinone,  see  quinone 

Benzidine  sulfate,  555 

Bibliography,  comments  on,  x,  553 

Bicarbonate,  see  carbonate 

Bicolor  standards,  122,  125,  126,  127, 
128 

Binding  posts,  355 

Bjerrum's  extrapolation,  94,  171, 
193,  202,  212,  277,  279,  280,  420, 
473,  478,  485 

"Black"  see  platinum 

Blood,  104,  558,  581;  electrode  ves- 
sel for  297,  433;  insect,  301 

Blue  glass,  172 

Body  fluids,  581 

Boltzmann  principle,  491,  492 

Borate  buffers,  193,  201,  208,  209, 
213,  215,  459,  478;  curves,  199,  205 

Boric  acid,  195,  532;  molecular 
weight,  195,  213 

Boundary  potentials,  see  liquid 
junction  potential 

Boyle's  law,  232 

Bread,  558,  576 

Brewing,  xiii,  576 

Briggs  logarithms,  245,  684,  690 

Brom  chlor  phenol  blue,  157, 183, 186 

Brom  cresol  green,  94,  103,  125,  126, 
157,  159,  182,  183,  186,  460,  511 

Brom  cresol  purple,  94,  95,  102,  103, 
104,  122,  126,  127,  138,  142,  151, 
157,  161,  164,  165,  181,  182,  185, 
186,  189,  459,  460,  511 

Brom  phenol  blue,  94,  102,  104,  122, 
151,  157,  181,  182,  184-186,  459 


INDEX    OF   SUBJECTS 


705 


Brom  phenol  red,  94,  157,  183,  186 

Brom  thymol  blue,  94,  102,  105,  122, 
142,  151,  157,  175,  182,  185,  186 

Buffer,  Acree's,  215;  acetone,  547; 
action,  50, 582;  AtHns',  215;  Clark 
and  Lubs',  192;  corrections,  202, 
478,  507;  Cohn's  system,  216; 
glacial  acetic  acid,  547;  Hastings 
and  Sendroy's,  212;  index,  55; 
Mcllvaine's,  214;  Kolthoff  and 
Vleeschhouwer's,  215;  Palitzsch's, 
213;  Prideaux  and  Ward's,  215; 
S0rensen's,  203;  standards,  192; 
tablets,  216;  temperature  coeffi- 
cients, 190,  206,  208-212,  456; 
uses,  50,  63,  486,  580;  Walbum's, 
211  ;Walpole's,  215;  weak,  190,  415 

Bunsen  flame,  lines  in,  142 

Butter  yellow,  181,  459 

Cabbage  extract  indicator,  67 

Cadmium,  amalgam,  343;  sulfate, 
343 

Calcium  in  blood,  560;  carbonate, 
564 

Calculation,  numbers,  61,  400,  519, 
524,  529;  uniformity  of,  225 

Calomel,  formula  of,  303;  grain  of, 
309;  preparation,  307;  reduction 
of,  261 

Calomel  electrode,  224,  303,  311-314, 
467,  472,  478,  480,  482,  487;  abso- 
lute potential  of,  312;  with  0.1  N 
KC1,  259,  453,  461,  469,  471-475, 
487,  509,  672;  with  1.0  N  KC1, 
453;  with  3.5  N  KC1,  314,  478; 
with  saturated  KC1,  297,  310,  453, 
454,  469-471,  488,  672;  with  HC1, 
303,  451,  464;  vessels,  296,  301,  303 

Calorie,  249,  685 

Candy,  577 

Canning,  574,  576 

Capillary,  action  of  paper,  135;  elec- 
trometer, 332,  337;  glass  seals,  337; 
1  quid  junctions,  271,  272 

Carbon  dioxide,  see  carbonic  acid; 
in  electrode  measurements,  444 


Carbonate,  buffers,  215;  equilibria, 
114,  558,  561,  586;  reduction  of, 
436;  in  standard  all- ali,  195-198; 
solutions,  414,  444,  445 

Carbonic  acid,  electrode  effect,  443; 
dissociation  constants,  510,  678; 
as  indicator,  517,  559 

Carbon  electrode,  300 

Carbons,  577 

Carvacrol  sulfon  phthalein,  102 

Casein  precipitation,  519 

Catalysis,  373,  440,  442,  515 

Cataphoresis,  see  electrophoresis 

Cathode,  6,  685 

Cation,  6,  685 

Cerebrospinal  fluid,  581 

Cell  (electric),  discharge  of,  227; 
dry,  577;  liquid  junction,  265,  271; 
measurements,  226,  479;  open 
circuit,  255;  reaction,  235;  special, 
316;  potential,  255,  672;  with 
transference,  265 

Cell  (living),  culture,  555,  581;  in- 
terior, 581 

Cements,  577 

cgs-system,  247 

Characteristic  data,  551 

Charcoal  as  buffer,  53 

Charging  of  batteries,  347 

Charge,  electric,  4 

Chemical  potential,  239 

Chemotherapy,  556 

China  blue,  117 

Chloranil,  417;  electrode,  417,  422, 
445 

Chlor  cresol  green,  157 

Chlor  phenol  red,  94,  103,  126,  157, 
183,  460 

Chloride  ion,  activity,  471 ;  velocity, 
226 

Chloride :  Chlorine  potential,  393 

Chloroform,  errors  due  to,  91,  92, 
440 

Chromate,  518 

Chromel  alloy  heater,  363,  365; 
wire,  362 

Chromophore,  106 


706 


INDEX   OF  SUBJECTS 


Chlorosis,  581 

Ciliary  movement,  580 

Citrate  buffers,  203,  205,  209,  211, 
214;  temperature  coefficients,  457 

Citrate-phosphate  buffers,  214 

Citric  acid  titration,  29 

Clark  and  Lubs',  buffers,  199,  200; 
indicators,  94 

Classics,  554 

Clay,  577 

Cleanliness,  356 

Cleaning  electrodes,  285 

Cobalt-blue  glass,  131 

Cochineal,  67,  99 

Cocks,  bronze,  355 

Cohn's  system  of  buffers,  216 

Colligative  properties,  6,  685 

Collodion  at  junction,  272 

Colloidal,  indicators,  117,  189;  solu- 
tions, 42,  495,  565,  571,  586 

Color  chart,  between  64  and  65; 
comments  on,  64-65,  120,  174 

Color,  62,  166;  artificial,  174;  blind- 
ness, 164;  comparison,  131;  for 
KC1  solution,  306,  indicator,  92, 
94,  100,  106, 107,  141, 152,  162,  166; 
memory,  120;  natural,  133,  159; 
standards,  174;  wedge,  170 

Colored  glass,  131,  174 

Colorimeter,  see  comparator 

Colorimet^,  141 

Comparator,  123,  124,  131,  133,  136, 
141,  166,  167,  169,  171 

Conditions,  constant,  see  environ- 
ment 

Concentration  units,  11 

Concentration  versus  activity,  178 

Conductivity,  228,  269,  461,  463, 
476,  516,  556,  685 

Concentration  cells,  see  cells 

Condensers,  potential  measurement 
with,  327;  at  spark  gap,  363 

Congo  red,  72,  117,  183,  188,  189 

Contacts,  potentiometer,  323;  relay, 
363;  regulator,  361 

Contact  potential,  see  liquid  junc- 
tions and  Volta-effect 


Control,  heat,  363;  potentiometric, 

244,  341 
Copper,   cyanide,   400;  removal  of 

O2,  354;  switches,  355;  tubing,  354 
Corrosion,  323,  577 
Cotton  at  junctions,  274 
Coulomb,  685 

Cresol  phthalein,  94,  70, 102, 104, 185 
Cresol  red,  94,  102,  104,  122,  141, 

142,  151,  157,  182,  184-186 
Criteria  of  reliability,  445 
Croceme,  74 

Crystal  violet,  107,  110,  117 
Crystal-structure,  58 
Crystallization,  565 
Culture  of  cells,  555,  581 
Culture  media,  52,  136,  555 
Curcumine,  459 

Damping,  335 

Dead  spaces,  302 

Debye-Hiickel  equations,  490,  500, 
503;  applications,  467-469,  504; 
buffers  and,  216;  coefficients  of, 
500;  derivation,  491;  discussion, 
60,  243,  489,  501;  indicators  and, 
187;  proteins  and,  586;  tempera- 
ture coefficients  and,  449 

Definitions,  6,  684 

Degree  of  dissociation  (a),  14,  15, 

.  23,  27,  30,  53,  63,  100,  129,  165 

Deposition,  of  frlack,  286;  of  metals, 
see  electroplating. 

Detector  tube,  328 

Developers,  579 

Diaphragms,  571 

Diaphragm  valve,  352 

Diazoacetic  ester,  513 

Dichromatic  indicators,  162-164 

Dichromatism,  161,  686 

Dielectric  constant,  499,  500,  541, 
685 

Diffusion  boundary,  see  liquid  junc- 
tion 

Digestive  system,  566 

Dilution,  13,  24,  40,  135,  187 

Dimensions,  494 


INDEX   OF   SUBJECT^ 


Dinitrobenzoylene  urea,  69 
Dinitrohydroquinone,  69,  96 
Dinitro  indicators,  see  nitro 
Disazo  indicators,  72,  80 
Disinfection,  556 

Dispersion,  59;  of  indicators,  117 
Dissociation,  complete,  11,  59;  con- 
stant, 11,  154,  178,  392,  476,  542, 
562;  constants  of  acids,  11,  517, 
678;  constants  of  alkaloids,  681; 
constants    of    ampholytes,    680; 
constants  of  bases,  679;  constants 
and  ionic  strength,  510;  constants 
and  temperature  coefficients,  460; 
constants     and     titration,     536; 
curves,  16, 25,  30,  47;  exponent,  15, 
559;  residue,  29, 47;  stepwise,  25, 96 
Distillation,  of  HC1,  198;  of  mer- 
cury, 365;  of  water  in  cell,  310 
Distilled  water,  193,  203,  520 
Distribution  coefficients,  517,  540, 

566,  579 

Donnan  equilibria,  560,  567 
Drift  of  potential,  414,  438,  445 
Drop  ratios,  122 
Drugs,  139,  579 
Duboscq  colorimeter,  167 

E,  see  energy 

E,  see  potential 

Eh,  223,  258,  377 

Earthworms,  571 

Ecology,  570,  571 

Edison  cell,  349 

Eggs,  301,  581 

Electric  current,  unidirectional, 
329,  377 

Electric  light,  character  of,  164 

Electric,  contacts,  326;  leaks,  357, 
358;  nose,  517 

Electrical,  nature  of  matter,  3; 
potential,  see  potential;  units,  see 
International  units 

Electricity,  sign  of,  318 

Electrode,  aging,  289;  alternate  im- 
mersion and  exposure,  293-296, 
302;  antimony,  426;  base  of,  281; 


707 

calomel,  see  calomel;  cleaning, 
285,286;  construction,  281;  Cot- 
trell  282;  defined,  686;  deposition 
on,  't  87;  deterioration  of,  287;  dis- 
turbance of,  276,  310;  function, 
379,  [440;  film,  283;  gauze,  282,  300; 
glast,  429;  graphite,  300;  im- 
mersion, 290,  293-296,  299,  302; 
injury,  285;  mechanism,  373; 
metal,  281,  380,  396,  400,  401,  404, 
411,  413;  method  in  outline,  221; 
micro,  581 ;  normal  hydrogen,  257, 
312;  occulsions,  443;  oxide,  see 
oxide;  potentials,  see  potentials; 
quinhydrone,  see  quinhy drone ; 
rejection  of,  297;  reversible,  435; 
sensitivity  to  O2,  289;  sheltered, 
538;  sluggish,  289,  414,  428,  442; 
state  of  metal  in,  260;  tempera- 
ture of,  294;  touch-,  292;  tube, 
300;  unattackable,  379,  380;  ves- 
sels, see  vessels 

Electrolytes,  686 

Electrolytic,  production  of  alkali, 
198;  solution  tension,  252 

Electrometer,  capillary,  337;  insula- 
tion, 356;  Lindemann's,  340;  quad- 
rant, 338 

Electromotive  force,  253,  686,  see 
also  potential 

Electron,  3,  4.  8,  318,  526,  686; 
activity,  375,  376;  chemistry,  99; 
emmission,  328;  escaping  tend- 
.  ency,  253;  free,  373;  path,  377, 
379,  393;  pressure,  373;  reduction 
and,  402;  shifts,  107;  transfer,  372; 
tube,  328,  342,  347 

Electronic  structures,  58,  109 

Electroneutrality,  4;  of  solutions, 
20,  374,  380 

Electro-osmosis,  571,  581 

Electrophoresis,  556,  571 

Electroplating,  of  black,  286;  of 
gold,  285;  of  nickel,  etc.,  557;  of 
smooth  platinum,  288 

Electrostatic  force,  6,  34,  59,  60, 
235,  252,  267,  374,  379,  490,  568,  579 


708 


INDEX   OF  SUBJECTS 


Elements,  structure  of,  4 

E.  M.  F.  (electromotive  force)  see 
potential 

Enamel  insulation,  356 

End-point  in  titration,  530,  534 

Energy,  equilibria  and,  10,  36,  60, 
108,  109,  116,  230,  237,  244,  396; 
free,  238;  ionization,  109,  116; 
partial  molal,  239;  tautomerism, 
108,  109,  115;  waste,  378 

Enol,  106 

Entropy,  237 

Environment,  9,  18,  44,  61,  230, 
236,  267 

Enzymes,  37,  556,  566,  572-573 

Equations:  absorption  of  radiant 
energy,  144;  acid  catalysis,  515; 
acid  equilibrium,  10;  acid  (multi- 
valent),  27;  activity,  236,  243; 
activity  of  buffers,  500,  508,  510; 
activity  coefficient,  501 ;  alternate 
formulation,  522-525;  ampholytes, 
31;  approximation,  22;  antimony 
electrode,  427;  barometer,  261, 
262;  base  equilibrium,  17,  48; 
Beer's,  144;  Boltzmann's,  492; 
Boyle  and  Gay-Lussac,  232;  buf- 
fer, 56;  calcium  equilibria,  565; 
carbonate  equilibria,  561;  chem- 
ical potential,  239;  chloranil 
electrode,  418,  422;  comparator, 
167;  conversion  of  logarithms,  684; 
Debye-Huckel,  490,  500,  503;  dis- 
tribution coefficient,  567;  Donnan 
equilibria,  569;  electrode,  235; 
electron  equilibria,  375;  equilib- 
rium, 243;  equilibria  including 
solvent,  542;  extinction  coeffi- 
cient, 144;  free-energy,  238,  396; 
"fundamental,"  377;  gas,  232, 234; 
Gibbs-Helmholtz,  448;  glass-elec- 
trode, 430,  433;  Henderson-Has- 
selbalch,  15,  22,  528;  hydrogen 
electrode,  225,  235,  255,  256,  257, 
371,  381,  527;  hydrion  in  oxida- 
tion-reduction, 383,  390;  hydro- 
quinhydrone,  421;  indicator,  102, 


121,  178,  187;  ionic  strength,  499; 
isoelectric,  31;  Lambert's,  144; 
liquid  junction,  268;  metal  elec- 
trode, 380;  metal-oxide  electrode. 
425;  monomolecular  reaction,  514; 
numerical  form,  249;  Ohm's  law, 
319;  oxidation-reduction,  378,  381; 
oxygen  electrode,  381;  Peter's, 
367;  photometer,  150;  Poisson's, 
494;  potentiometer,  323;  quin- 
hy drone  electrode,  405,  408,  418; 
quino-quinhydrone,  421;  spectro- 
photometer  and  pH,  153,  155,  156; 
solubility  product,  584;  tauto- 
meric  equilibria,  115;  tempera- 
ture coefficients  of  calomel  cells, 
452,  454;  temperature  coefficients 
of  Weston  cells,  345;  transmit- 
tance,  144;  water  equilibria,  18; 
work,  234 

Equilibria,  8,  9;  acid,  521;  Donnan, 
567;  dynamic,  106;  local,  292; 
liquid  junction  and,  265;  pseudo, 
292 

Equilibrium  constants,  11,  61,  230 
(see  also  dissociation) 

Equipotential  surface,  357 

Equivalent,  686 

Errors  with  hydrogen  electrode, 
434-447,  see  also  potentiometer, 
calomel  oxidation  reduction  po- 
tentials electrode,  standardiza- 
tion, etc. 

Errors  with  indicators,  177-191,  see 
also  spectrophotometer,  stand- 
ardization, etc. 

Errors  with  quinhy drone,  413;  see 
also  oxidation-reduction  poten- 
tials 

Erythrolein,  67 

Erythrolitmin,  67 

Escaping  tendency,  240;  of  elec- 
trons, 373,  377 

Ethanol,  see  alcohol 

Ethyl  red,  102 

Exhibition  of  indicators.^  120 

Explosives,  577 


INDEX    OF   SUBJECTS 


709 


Exponent,  dissociation,  15;  hydrion, 

37 
Extinction,     coefficient,     145,     156; 

setting,  148 

Extractions,  567,  576,  579 
Eye,    differentiation   by,    131,    167; 

visibility  range,  160 

Fj  see  free  energy 

F,  see  faraday 

f,  see  fugacity 

F,  see  partial  molal  energy 

Fading  of  indicators,  92,  189 

Faraday,  248,  686 

Fate,  9 

Fermentation,  136,  137,  558,  576 

Ferric  salts,  and  H  electrode,  437 

Ferro-ferricyanide  potential,  387 

Field,  electric,  497 

Field-kit,  170 

Film  electrode,  283,  297,  413 

Films  of  indicator  solution,  173 

Filter,  light,  175 

"Filtering  ions,"  377 

Filtration,  574 

Finite  ratios,  395 

Fish,  571 

Flowing  junctions,  266,  274-276,  469 

Fluorescein,  173 

Fluorescence,  173 

Foods,  574 

Force,  232,  686 

Formulas,  684 

Fraunhofer  lines,  142 

Free  energy,  60,  230,  238,  239,  254, 

267,  396,  397,  463 
Free    energy    equation    numerical 

form,  249 

Freezing  points,  6,  518 
Fugacity,  240 
"Fundamental  equation,"  377 

7  (gamma),  see  activity  coefficient 

Galvanometer,    332-336;    ballistic, 

327;  damping  of,  335;  mounting, 

333;  record,  342;  sensitivity,  320, 

332-336 


Gas,  ideal,  231,  232,  235,  687;  con- 
stant, 246;  diffusion,  441;  equa- 
tion, 231 

Gastric  acidity,  104,  566 

Gauze  electrodes,  300 

Gay-Lussac  law,  232 

Gels  in  junction,  273 

Generator,  Hydrogen,  352 

Gibbs-Helmholtz  equation,  448 

Gillespie,  comparator,  168;  method, 
121,  459 

Glacial  acetic  acid,  equilibria  in,  544 

Glass,  colored,  131,  174;  composi- 
tion for  electrode,  431 ;  drilling  of, 
352;  electrode,  339,  357,  429; 
opal,  139;  seals,  281,  285,  305,  337, 
361;  dissolving  of,  574 

Glucose  conduct  and  pH,  552 

Glycocoll,  41,  203;  buffers,  206,  210, 
457;  curve,  205;  standard,  486 

Gold,  electrodes,  284,  286,  411,  413; 
electrodeposition,  285;  deposit  on 
glass,  283 

Grain  size  of  calomel,  309 

Gram  reaction,  556 

Graphite  electrode,  300 

Grid  potential,  330 

H  (heat  content),  238,  448 

[H+],  relation  to  pH,  37,  673 

Haemolysis,  581 

Heart,  580 

Heat,  content,  238,  448;  of  neutrali- 
zation, 518 

Heating,  of  baths,  360,  363;  of 
mercury  still,  365 

Helianthin,  75 

Heliotrophism,  580 

Hellige  comparator  (see  Anonymous 
author  in  bibliography) 

Helmholtz  double  layer,  495 

Hemoglobin,  560 

Henderson-Hasselbalch  equation, 
15,  22,  528 

Henry's  law,  566 

Hermaphroditic  ion,  32 

Hildebrand  electrode,  438 


710 


INDEX   OF  SUBJECTS 


Histidine,  32 

Hookworm,  581 

Hybrid  ion,  32 

Hydration  of  ions,  6,  48,  114,  500, 
540,  543,  561 

Hydrion,  6,  529,  687;  activity,  480; 
alkaline  solution,  42;  catalysis, 
514;  transport,  253,  254,  397;  im- 
portance of,  520-526,  529,  549;  in 
oxidation-reduction  equilibria, 
382;  negative,  6;  solvated,  540, 
543,  552  (see  hydration) ;  velocity, 
266 

Hydrochloric  acid,  activity,  449, 
458;  activity  coefficient,  193; 
buffers,  193,  201;  complete  disso- 
ciation, 11,  33,  449,  465,  472;  junc- 
tion potential,  269,  276-279,  478, 
566;  pH  values  of,  201,  420,  458, 
468,  474,  476,  477;  standard,  198; 
standards,  201,  458,  460,  476,  487; 
titration  of,  33,  530 

Hydrogen,  electrode,  221,  251,  387, 
435,  440,  444,  519,  527;  generators, 
350;  ion,  seehydrion;  ion  cataly- 
sis, 375;  potential,  see  potential ; 
pressure,  see  barometric;  purifica- 
tion, 350,  351;  rate  of  bubbling, 
"  291;  reduction  by,  370,  389; 
supply,  350;  tanked,  350 

Hydrogenation,  397,  399,  402 

Hydrogen  sulfid  as  poison,  439,  440 

Hydrolysis,  44,  574,  579 

Hydro-quinhydrone  electrode,  404, 
407,  421,  422 

Hydroquinone,  405 

Hydroxids,  metal,  424,  575 

Hydroxyl  ion,  3, 17,  42;  velocity,  266 

"Hypo,"  579 

Hysteresis,  344,  446,  455 

Ideal,  conditions,  9,  42;  equations, 
235;  gas,  see  gas;  solute,  490 

Illuminants,  163 

Impurities,  detection  by  pH,  138 

Indicators,  absorption,  94-101,  142; 
absorption  maxima,  94,  142,  151, 


157;  activity,  178,  187,  511;  alco- 
holic solutions,  91,  547;  ampho- 
teric,  116;  approximations  with, 
119;  cellulose  vehicle  for,  135; 
choice  of,  67,  164;  colloidal,  117, 
189;  color,  141, 152, 164;  constants, 
101-103,  126-129,  132-134,  157, 
460;  curves,  103-104;  dissociation, 
53,  101;  errors,  see  errors;  fading 
of,  91,  120,  189;  field-kit  of,  136, 
170;  films  of,  173;  fluorescent,  173; 
glacial  acetic  acid  solutions  of, 
546;  history,  68,  99;  impure,  95; 
inorganic,  98;  ionic  strength  and, 
187,  511;  labeling,  71-75;  lability 
of  99;  lists  of,  76;  mixed,  96,  140, 
175;  molecular  weights,  94;  multi- 
valent,  111,  116,  123;  natural,  67, 
86;  one-color,  96,  126;  oxidation- 
reduction,  189,  387,  683;  paper, 
134;  partial  neutralization  of,  91, 
190;  precipitation,  140,  181,  188, 
583;  preparation  of,  91-94,  126; 
protein  effects  with,  91 ;  ranges  of, 
65,  76-86,  92-98,  103,  120,  165, 
166,  176;  reduction,  see  oxidation- 
reduction;  salt  effects  with,  70, 
91,  92,  132,  133,  136,  158,  178,  511; 
selections  of,  92,  94,  96;  specific 
errors  with,  188;  stability,  92,  120, 
125, 189;  structures,  71 ;  synonyms, 
87;  tautomerism,  105-116,  154; 
temperature  coefficients,  125-129, 
189,  458,  460;  theory,  99;  thread, 
135;  time  changes,  117,  135,  189; 
titration  with,  68,  175,  176,  531- 
536 
Indigo,  carmine,  74,  368;  sulfonates, 

74,  368,  387,  683 
Indophenol,  73,  84,  386,  387,  683 
Industrial  applications,  576 
Infinite  dilution,  59,  462,  464 
Inorganic,    color    standards,    174; 

indicators,  98 
Insects,  581 
Insulation,  356,  432 
Integration,  233 


INDEX   OF   SUBJECTS 


711 


Integrating  sphere,  145 

Internal  energy,  232 

International  units,  247,  342,  687 

Ion,  6,  687;  atmosphere,  497;  ex- 
change, 430;  fields  of,  503;  migra- 
tion, 266,  376,  378,  569,  571; 
mobility,  270,  688 

Ionic  diameter,  491,  497,  500,  503, 
506;  strength  GO,  187, 201, 216,  490, 
493,  504,  508,  510,  559 

lonization,  5,  8;  color  and,  107; 
complete,  11;  electric  charge  and, 
571;  free  energy  of,  108,  397;  step- 
wise,  110;  tautomerism  and,  116 

lonogen,  687 

Iridium,  260;  on  glass,  283;  elec- 
trodes, 286 

Iron  carbonyl,  350 

Iron  system,  potentials  of,  367,  387 

Isatin,  105 

Isobathmen,  152 

Isobestic  point,  153,  687 

Isoelectric  point,  30,  31,  187,  569, 
573 

Isohydric,  absorption  curves,  152; 
solutions,  191,  687 

Isonitrosoacetyl-p-aminobenzene, 
583 

Isonitrosoacetyl-p-toluazo-p-tolu- 
idine,  583 

Isotherm,  233 

Jelly,  576 

Julius  suspension,  333 
Junctions,  see  liquid  junctions;  of 
copper  and  glass,  354 

K,  versus  K',  11,  116;  Ka,  11;  Kb, 
17;  Kt,  153;  KX,  144;  KB,  584;  Ku, 
153;  Kw,  18,  42-46,  49;  K  (kappa), 
see  kappa  K0/z,  503 

Kappa,  494,  495 

KC1,  see  potassium  chloride 

Kerosine  for  baths,  358 

Keto,  106 

Keuffel  and  Esser  color  analyser, 
145,  146 


Key  for  electrometer,  338 
deKhotinsky  cement,  354 
Kidneys,  559,  560,  574 
Kinetics,  10,  513,  516,  529,  576 
Konig-Martins  photometer,  147 

Labeling,  71-75,  138,  204 

Lability,  100,  106 

Lacmoid,  69,  459 

Lacmosol,  69 

Lactam,  lactim,  lactone,  106,  111 

Lambert's  law,  144 

X  (lambda)  as  wave  length,  142,  689 

Lead  storage  battery,  346 

Leaks,  electrical,  356,  357 

Leather,  576 

Leeds  and  Northrop  potentiom- 
eters, 321,  341 

Light,  161 

Light-filter,  175 

Life,  9 

Limiting  laws,  239,  502 

Linde-Caro-Frank  process,  350 

Lindemann  electrometer,  340 

Liquid  junctions,  221,  271,  296,  302, 
306,  545;  capillary,  302;  diffusion, 
376;  flowing,  274;  membranes,  etc. 
at,  272;  wick,  297;  with  salts  other 
than  KC1,  279 

Liquid  junction  potentials,  221,  228, 
264,  311,  473-^78,  540;  arbitrary 
treatment,  221,  456;  drifts  of,  445; 
formulation  of,  376;  hydrochloric 
acid,  269-278,  471-478;  potassium 
chloride,  221,  269-280,  380,  418, 
419,  456,  468-478;  uncertainty  of, 
476;  in  temperature  gradient,  450 

Litmus,  2,  67;  milk,  138,  189 

In,  143,  684 

Logarithms,  Briggs,  table  of,  690; 
natural,  234,  684 

Lovibond  tintometer,  175 

Luminosity,  161;  curves,  162 

Lysine,  32 

Manganese  dioxide  electrode,  427 
Mauve,  92,  185 


712 


INDEX   OF   SUBJECTS 


Maximum  work,  232,  255,  317 
Mechanism,  251,  253,  398,  520,  542 
Mechanical  control,  332 
Megohm  sensitivity,  335 
Membranes,  272,  571,  579,  581 
Membrane  potential,  272,  568 
Mercurous,   chloride,   see   calomel; 

sulfate,  307,  343 

Mercury  (see  also  amalgam),  arc, 
142,    164;    danger   of,    366;   elec- 
trodes, 415;  electrode  poison,  282, 
439;  purification  of,  364;  siphoned 
by  Cu,  355;  still,  365;  subdivision 
and  potential,  309 
Mercuric  oxide  electrode,  316,  426 
Metabolism,  556,  581 
Meta  cresol  purple,  94,  157,  183,  186 
Metal  electrode,  see  electrode 
Metal  hydroxides,  575 
Metal  oxide  electrodes,  422 
Metanil  yellow,  92,  184 
Methylene  blue,  387,  581,  683 
Methyl  orange,  72,  92,  93,  112,  117, 

175,  181-185,  459 

Methyl  red,  68-72,  93,  95,  102-104, 
120-123,  138,  151,  175,  181-185, 
459 

Methyl  red  test,  138 
Methyl-thymol  blue,  98 
Methyl  violet,  72,  92,  185 
Michaelis,  picture,  554;  method,  126 
Microampere  sensitivity,  335 
Micro,     antimony    electrode,    427; 
burette,    125,     536;    colorimetric 
methods,  139;  electrodes,  299-301, 
412-413,  427;  junctions,  272;  volu- 
metric methods,  536;  vessels,  301 
Migration,  ionic,  462,  569,  571 
Milk,  104,  136,  577,  687 
Miscellaneous  indicators,  86 
Mixed  indicators,  96,  140,  175 
Mixture  boundary,  270,  273,  276 
Mobility,  688 
Moderator,  50 

Molar  transmissive  index,  145 
Molecular,    solution,    688;    theory, 
398,  402 


Monomolecular  reaction,  513-515 

ju  (mu),  as  chemical  potential,  see 
chemical  potential;  as  ionic 
strength,  see  ionic  strength;  as 
micron,  see  m/j. 

m/x  (millimicron),  142 

Multivalent  ions,  116,  536 

Muscle,  566,  580 

Mutarotation,  578 

n  (number  of  moles),  232 

n  (number  of  faradays),  234 

n  (transport  number),  267 

NO  (Avagadro  number),  491,  519 

N  (normality),  35 

Naperian  logarithms,  245 

Naphthol,    phthalein,    69,   93,    102, 

180,  213;  sulfon  phthalein,   102; 

sulfonic  acid,  173 
Natural,  color,  159,  170;  indicators, 

67,  86 

Neutrality,  31,  39,  42,  43,  532,  574 
Neutral  red,  73,  93,  180,  183,  185, 

186,  459 

Neutralization,  1,  16 
Nichrome,  see  Chromel 
Nickel  electrode,  352 
Nickel-iron  cell,  349 
Nickel  plating,  577 
Nickel  salts  for  absorption  of  heat, 

361 

Nicol  prism,  148 
Nitramine,  72,  183,  459 
Nitratoaquotetramine  cobalt,  514 
Nitrogen,  for  cells,  310,  315 
Nitro  indicators,  72,  76,  96 
Nitrophenol,  72,  76,  93,  96,  128-133, 

180-188 

Nitrosotriacetonamine,  513,  514 
Normal  atmosphere,  246,  685 
Normal    hydrogen    electrode,    222, 

257,  259,  312,  448,  450,  466,  672 
Normal  solution,  35 
Normal  Weston  cell,  342 
Non-aqueous  solutions,  339,  539 
Null-point,   317,  319;   instruments, 

332 


INDEX    OF   SUBJECTS 


713 


Ohm,  319,  247,  688 

Ohm's  law,  247,  319 

Oil  baths,  358 

One-color  indicators,  see  indicators 

Opal  glass,  130 

Optical  rotation,  148,  578;  sensitiz- 
ers,  579 

Optimal  growth,  556,  557 

Orange  II,  75 

Orange  4,  181 

Orange  IV,  188 

Orderly  series  test,  445 

Organic  chemistry,  remarks  on,  578 

Ortho,  see  several  compounds  with 
this  prefix 

Ostwald's  theory,  100,  113 

Overvoltage,  388 

Oxazine  indicators,  73,  85 

Oxidation,  264,  369,  371,  381,  414 

Oxidation-reduction,  indicators,  see 
indicators;  potentials,  367,  416, 
682,  683 

Oxonium  ion,  543 

Oxygen,  diffusion,  353,  441;  calomel 
electrode  and,  310;  electrode,  372, 
381,  387,  388,  428;  hydrogen  elec- 
trode and,  289,  296,  353,  440; 
removal,  354 

Ozokerite,  357 

P  (pressure),  see  hydrogen 

paH,  39,  479 

pH,  15,  20,  36,  41,  48,  225,  256,  271, 
479;  in  activity  sense,  545;  calcu- 
lation number,  39,  256,  280,  456, 
480,  545;  calculation  of,  225,  271; 
defined,  36.  479,  480;  meaning, 
20,  61,  528;  relation  to  [H+],  672; 
scale,  35;  substitutes  for,  38 

pK,  15,  40,  62,  678 

pOH,  18 

Palladium,  black,  260;  electrodes, 
286,  289;  solution  in  HC1,  287,  290; 
tube  electrode,  300 

Paper,  577;  indicator,  134 

Paraffin,  357;  bottle,  196 

Para  (prefix),  see  several  com- 
pounds 


Parasites  and  pH,  582,  585 

Partial,  molar  free  energy,  239; 
pressure,  262 

Partition,  see  distribution  coeffi- 
cient 

Pastes,  electrode  for,  299 

Pectin,  576 

Period  of  galvanometer,  335 

Permeability,  560,  579,  580 

Peters'  equation,  367 

Phagocytosis,  580 

Pharmacology,  579 

Phase,  688;  boundary,  272,  540 

Phenolphthalein,  68,  73,  93,  95,  96, 
101,  102,  110,  116,  123,  127-129, 
151,  165,  180-185,  213,  459,  544 

Phenol  red,  73,  94,  101-104,  111,  112, 
122,  126,  128,  151,  157,  164,  181- 
189,  459,  460,  511 

Phenol  thymol  phthalein,  98 

Phenol  violet,  98 

Phenyl  acetic  acid  buffer,  215 

Phosphate,  acid  potassium,  194, 
203,  204;  buffers,  193,  214-216,  457, 
459,  478,  506,  509;  buffer  tables, 
200,  210,  216,  217,  218;  citrate 
mixtures,  214;  curves,  28,  199,  205; 
dissociation  constants,  678;  purifi- 
cation, 195;  secondary  sodium,  204 

Photoelectric  cells,  176 

Photographic  methods,  145,  342 

Photography,  pH  in,  579 

Photometer,  146-147 

Photoperiodism,  581 

Phthalate,  buffers,  193,  457,  458; 
buffer  table,  200;  curves,  28,  199; 
indicator  error,  188;  preparation 
of,  193,  194;  reduction  of,  437,  486; 
standards,  485,  486,  672 

Phthaleins,  73,  81,  102 

Physiology,  pH  in,  580 

Pickling,  576 

Picric  acid,  96,  511 

Pipe  fittings,  355 

Pipettes,  broken  tips,  202 

Plant,  distribution,  571,  585;  physi- 
ology, 581,  585 

Plasmolysis,  581 


714 


INDEX   OF   SUBJECTS 


Platinum,  asbestos,  353;  black,  260, 
285-288;  bright,  287,  288,  443; 
electrodes,  281-286,  413;  glass 
seals,  305,  361;  on  glass,  283;  pure, 
288;  removal  of  02  by,  353;  wet 
by  mercury,  361 

Poisons,  438 

Poisson's  equation,  494 

Polarity  test,  347 

Polarization,  445;  of  radiant  energy, 
147;  of  sugar  solutions,  515 

Pole,  see  electrode 

Portable  apparatus,  341 

Potassium  chloride,  309;  coloring 
for,  306;  creeping  of,  296;  impur- 
ities in,  309;  junction  potentials, 
see  liquid  junction;  solubility,  311 

Potassium  hydroxide,  titration  of, 
33 

Potassium  phosphate,  see  phos- 
phate 

Potassium  phthalate,  see  phthalate 

Potato  scab,  355 

Potential,  258,  495,  688;  absolute, 
312;  arbitrary  values,  672;  Com- 
mission, 257,  312,  474;  equations, 
see  equations;  gradient,  688; 
interrelations,  389;  ion,  491,  493; 
liquid  junction,  see  liquid  junc- 
tion; measurement,  319;  mem- 
brane, 570;  oxidation-reduction, 
367;  rapidity  of  adjustment,  414; 
reproducibility,  289,  310;  single, 
222,  257 

Potentiometer,  227,  317;  balance, 
254;  range,  326 

Precipitation,  54,  117,  188,  517,  575, 
582;  indicators,  98,  140,  583 

Pressure,  see  barometric 

Propyl  red,  70,  102,  189 

Proteins,  555,  565,  576,  583;  and 
electrode  conduct,  439 

Protein  effects,  133,  179,  188 

Proton,  4,  6,  100 

Protozoa,  581 

Pseudo  equilibria,  see  equilibria 

Puffer,  50 


Pyridine  and  indicators,  188 
Pyrovolter,  325 

Quadrant  electrometer,  338,  433,  545 
Quinhy drone,    405;   electrode,    404; 

potentials,  259,  387,  420,  672 
Quinoline  blue,  73;  indicators,  73,  83 
Quinone,  405 
Quinone  group,  107 
Quinone-phenolate  theory,  111 
Quino-quinhydrone   electrode,   404, 

407,  418;  equation,  421;  potential, 

421 

R  (gas  constant),  232,  246 

Radiant  energy,  141,  143 

Radio  parts,  326 

Radium  emanation  and  electrode, 
442 

Range  of  indicators,  see  indicators 

Ratio,  importance  of  finite,  395 

Reaction,  8;  number,  37 

Recording  potentiometer,  341 

Kectifiers,  347 

Reductant,  pure,  395 

Reduction,  99,  264,  292,  294,  299, 
369,  370,  581;  potentials,  367,  682 

Refraction,  147 

Refractive  index,  518 

Reflection  and  indicators,  173 

Reflection  spectrum,  58 

Regulator,  361;  mixtures,  50 

Relay,  341,  363 

Resistance,  and  galvanometer  sensi- 
tivity, 320,  324,  335;  of  cells,  335, 
545 

Resistance  box  potentiometer,  322 

Respiratory  center,  559 

Reversibility,  8,  317 

rH,  387 

Rhotanium  alloy,  286 

Rocker,  294,  296 

Ropy  bread,  558,  576 

Rosolic  acid,  93,  183,  185 

Rubber,  care  of,  326;  insulation, 
356,  357;  latex,  577;  sulfur-free, 
297 


INDEX   OF  SUBJECTS 


715 


Salicyl  yellow,  96 

Saliva,  566 

Salm's  method,  101 

Salts,  basic,  575;  complete  dissocia- 
tion of,  12-14,  19,  24,  33,  59,  517; 
crystal  structure,  58;  effect,  34, 
45,  46,  92,  132-136,  179,  187,  213, 
409,  510,  515,  584;  solutions 
(physiological),  580;  undisso- 
ciated,  23 

Salting-out,  585;  term,  503,  508 

Sand  in  junction,  274 

Saturated  KC1,  see  potassium 
chloride 

Saturated  Weston  cell,  342 

Screen,  light,  163 

Sea  water,  see  water 

Sector  in  photometry,  146 

Sensitivity  (galvanometer),  311, 
333-339 

Sewage,  577 

Sheltered  electrode,  538 

Shielding,  296,  357 

Sign,  of  charge,  318;  of  potential, 
223,  258,  392 

Silica  vessel,  297 

Silicates,  577 

Silicon  hydride  in  H2,  354 

Silver,  315;  chloride  electrode,  265, 
315,  464,  471;  complexes,  400; 
plating,  315;  solder,  354 

Siphons,  272 

Snails,  571 

Sodium  salts,  see  respective  salts 

Soils,  445,  571,  585 

Solder,  connections,  355;  pinholes 
in,  354;  silver,  354 

Solubility,  30,  31,  262,  504,  582,  584 

Solubility  product,  565,  584 

Solution  tension,  252,  373,  400 

Solvation,  540,  543 

S0rensen,  picture,  frontispiece 

S0rensen- value,  37 

S0rensen's  value  of  calomel  elec- 
trode, 474 

Spaniolitmin,  67 

Sparking  at  contacts,  363 


Specific  errors,  188 

Spectrometer,  146,  150 

Spectrophotometers,  145 

Spectrophotometry,  141 

Spectrum,  141,  689 

Spectroscopy,  109 

Spermatozoa,  580 

Spider  web,  338 

Sporulation,  558 

Spot  plate,  140 

Stability,  of  indicators,  125;  of 
potentials,  445;  of  solutions,  579; 
of  thiosulfate,  579 

Staining,  581,  585 

Standard  acetate,  see  acetate; 
arbitrary,  524,  528,  672;  buffers, 
192;  color,  63,  64,  130;  half-cells, 
419;  potential,  224,  453,  480; 
secondary,  34,  482;  solution,  483 

Statistical  treatment,  9 

Step-wise  dissociation,  26;  reduc- 
tion, 378,  402 

Still,  mercury,  365 

Stopcock,  lubricant,  296;  bronze, 
355 

Storage  battery,  346 

Strength  of  acid,  11 

Strong  electrolytes,  57 

Structure,  electronic,  4;  indicator, 
72,  105 

Sublimation  of  phthalic  anhydrid, 
194 

Sugar,  hydrolysis,  513,  515;  manu- 
facture, 577;  conduct  in  alkaline 
solution,  552;  dissociation  con- 
stant of,  11,  678 

Sulfite  as  poison,  439 

Sulfonphthaleins,  69,  94,  102,  157 

Sulfur  as  poison,  439 

Superacid,  38,  545 

Supersaturation,  582 

Supplementary  methods,  513 

Surface  structure  and  potential,  310 

Surface  tension,  518,  586 

Suspensions,  galvanometer,  333, 
Julius,  333 

Sweat,  581 


716 


INDEX   OF   SUBJECTS 


Swelling,  31,  579 
Switches,  355,  356 
Symbols,  684 
Synonyms,  87 

T  (absolute  temperature),  245; 
(transmittance),  144 

Tadpoles,  581 
Tampon,  50 

Tanks  of  H2,  350 

Tanning,  576,  580 

Taste,  1,  518,  586 

Tautomer,  106,  110,  113 

Tautomeric  equilibria,  115 

Tautomerism,  105 

Telephone  receiver,  340 

Temperature,  240;  absolute,  245; 
bath,  358,  361;  control,  229,  358; 
thermoj  unctions,  358 

Temperature  coefficients,  259,  448; 
of  calomel  cell,  312,  314;  of  buffer 
values,  206-212;  of  indicator  con- 
stants, 103,  129,  189,  459;  of  Kw, 
44,  45;  of  normal  hydrogen  elec- 
trode, 257,  312;  of  quinhydrone 
potential,  419,  421,  422;  of  Weston 
cell  potentials,  344,  345 

Temperature  factors  for  concentra- 
tion cells,  674 

Textiles,  577 

Thermal  equilibrium,  450 

Thermionic  tube,  328 

Thermodynamics,  61,  230,  235,  237, 
251,  268,  398,  401,  403,  552 

Thermoelectric,  forces,  326,  355; 
methods,  145 

Thermoregulators,  361,  552 

Thermostats,  see  baths 

Thymol  blue,  94,  102,  104,  122,  151, 
157,  159,  164,  181-186,  459 

Thymol  phthalein,  93,  185 

Thymol  violet,  98 

Time-changes,  117,  273 

Tissue,  culture,  139,  581;  reaction, 
581 


Titration,  518;  in  acetic  acid,  544;  in 
acetone,  547;  in  alcohol,  547;  by 
conductivity,  516;  of  culture 
media,  137;  curves,  23,  25,  28,  29, 
32,  33,  51,  52,  54,  199,  205,  544,  582; 
methods,  555;  theory  of,  530; 
vessels,  300 

Tolidine,  387 

Topfer's  indicator,  185 

Touch-electrode,  392 

Toxins,  556,  558 

Transmission,  see  absorption 

Transmissive  index,  145 

Transmittance,  144 

Transport,  in  membranes,  272; 
numbers,  267,  689 

Trap  for  H2,  263 

Trickle  charger,  347 

Triphenyl  methanes,  69,  72,  80,  118, 
189 

Tropaeolins,  75,  92,  93,  181-185, 
459 

Tumor  cells,  581 

Tungsten,  contacts,  363;  electrode, 
428 

Turbidity,  136,  159,  162,  172 

Tugor,  581 

Unbuffered  solutions,  190,  442 
Urine,  560,  574 

Vacine  virus,  558 

Valence,  5,  109 

Valve,  electron,  328;  diaphragm,  352 

Van  Slyke's  buffer  index,  55 

Vapor  pressure  and  H-potential,  261 

Velocities,  10 

Vessels,  calomel,  305;  glass  elec- 
trode, 432;  hydrogen,  290;  quin- 
hydrone, 411 

Virage,  90 

Virulence,  558 

Viscosity,  31,  558 

Visibility,  160 

Vitamines,  574 

Volt,  247,  319,  342,  689 


INDEX    OF   SUBJECTS 


717 


Volta-effect,  379 
Volt-coulomb,  246,  396 
Volt-meter,  324 

W  (work),  232 

Wallaston  prism,  147 

Walpole's  comparator,  168,  171 

Water,  activity,  426;  boiler,  576; 
conductivity,  193,  586;  distilled, 
193,  203,  586;  equilibria,  18;  fresh, 
586;  measurements  with,  131; 
pure,  43;  purification  of,  193,  203, 
576;  sea,  104,  182,  184,  213,  586 

Wave  length,  142,  689 

Weak  acids,  see  acids 

Weston  cells,  227,  247,  319,  342,  349, 
687 


White  light,  161 
Wick-junction,  272 
Wind-shield  wiper,  294 
Wines,  104,  576 
Wiring,  355,  363 
Witte  peptone  titration,  51 
Wood,  577 
Work,  231,  254 

X-ray  analysis,  58 
Xylene  cyanole  F  F,  175 

Yeast,  104 

Zero  potential,  371 
Zwitter  lonen,  32 


Sans  Tache 


Sans  Tache 


IN  THE  "elder  days  of  art"  each  artist  or  craftsman 
enjoyed   the    privilege    of    independent    creation.     He 
carried  through  a  process  of   manufacture  from  be- 
ginning to  end.     The  scribe  of  the  days  before  the  printing 
press  was  such  a  craftsman.     So  was  the  printer  in  the 
days  before  the  machine  process.     He  stood  or  fell,  as  a 
craftsman,  by  the  merit  or  demerit  of  his  finished  product. 

Modern  machine  production  has  added  much  to  the  work- 
er's productivity  and  to  his  material  welfare.;  but  it  has 
deprived  him  of  the  old  creative  distinctiveness.  His  work 
is  merged  in  the  work  of  the  team,  and  lost  sight  of  as  some- 
thing representing  him  and  his  personality. 

Many  hands  and  minds  contribute  to  the  manufacture  of  a 
book,  in  this  day  of  specialization.  There  are  seven  dis- 
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The  printing  craftsman  of  today  is  quite  as  much  a  crafts- 
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Raymond  Gallagher. 

Cutter:  WTilliam  Armiger. 

Folders:  Laurence  Krug,  Shipley  Bellinger. 


MICHAELIS' 
Hydrogen  Ion  Concentration 

Its  Significance  in  the  Biological  Sciences 
and  Methods  for  its  Determinations- 
Principles  of  the  Theory 

By  LEONOR  MICHAELIS 

For  a  better  understanding  of  the  whole  theory  of 
hydrogen  ion  determination,  one  needs  MICHAELIS 
along  with  Clark. 

This  translation,  by  WILLIAM  A.  PERLZWEIG,  in- 
cludes addenda,  prepared  by  Dr.  Michaelis,  which 
makes  it  in  effect  a  new  edition,  after  the  Second 
German  Revised  Edition.  In  particular  reference  is 
made  to  the  recent  contributions  to  the  activity  theory 
of  ionization  by  G.  N.  Lewis,  Bjerrum  and  Debye; 
the  modification  of  the  theory  concerning  the  dissocia- 
tion of  the  amphyolytes  by  Bjerrum;  and  the  theory  of 
oxidation-reduction  potentials.  Says  Dr.  Michaelis 
"The  latter  is  sufficiently  developed  in  the  new  text  to 
give  the  reader  a  basis  for  understanding  the  application 
of  this  theory  to  the  use  of  the  quinhydrone  electrode, 
and  to  prepare  him  for  the  more  recent  studies  in  this 
field,  particularly  those  of  W.  M.  Clark." 

"A  useful  and  a  comprehensive  summary  of  the 
principles  of  a  very  important  field  of  physical  chemistry" 
says  the  Journal  of  the  Franklin  Institute. 

Cloth,    6x9,    Illustrated,    Bibliography. 
Price  $5.00 

THE  WILLIAMS  &  WILKINS  COMPANY 
BALTIMORE,  U.  S  .  A. 


GENERAL  LIBRARY 
UNIVERSITY  OF  CALIFORNIA—BERKELEY 

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