Page 101 - Introduction to Colloid and Surface Chemistry
P. 101

Liquid-gas and liquid-liquid interfaces  9.1

           ions are  held  in the  Stern layer; even so,  the  zeta potential of an
           ionic  micelle  is usually high.
         3.  The  retarding  influence of  the  ionic  atmospheres  of  unattached
           counter-ions  on  the  migration of  the  surfactant  ions  is  greatly
           increased  on aggregation.

          The  last  two  factors,  which  cause  the  molar  conductivity  to
         decrease  with  concentration  beyond  the  c.m.c.,  normally outweigh
         the first factor, which has the  reverse  effect  (see  Figure 4.13). When
         conductance  measurements are made at very high field strengths the
         ionic atmospheres cannot  re-form quickly enough (Wien effect)  and
         some  of the  bound  counter-ions  are  set free.  It is interesting to note
        that  under  these  conditions  the  molar  conductivity increases  with
        concentration  beyond the  c.m.c.

        Sharpness of critical micelle concentrations

        There are  two current theories  relating to the abruptness with which
                                                               53 155
        micellisation  takes  place  above  a certain  critical concentration '  .
          The  first  of  these  theories  applies  the  law of  mass  action  to  the
        equilibrium  between  unassociated  molecules or ions and micelles, as
        illustrated by the following simplified  calculation for the micellisation
        of non-ionic surfactants. If c is the stoichiometric concentration of the
        solution, x  is the  fraction of monomer units aggregated  and m  is the
        number of monomer  units per  micelle,

              mX  =  (X) m
             c(l-x)  cx/m

        Therefore,  applying the  law of  mass action,
             _,    cx/m
                                                               (4.23)
                      jc)f
        For  moderately  large  values  of  m,  this  expression  requires  that  x
        should  remain  very  small  up  to  a  certain  value  of  c  and  increase
        rapidly thereafter.  The  sharpness  of the discontinuity will depend on
        the value of m  (m  =  <» gives a perfect  discontinuity). If this treatment
        is  modified  to  account  for  the  counter-ions  associated  with an  ionic
        micelle,  then  an  even  more  abrupt  discontinuity than  the  above  is
        predicted.
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