Page 240 - Introduction to Colloid and Surface Chemistry
P. 240

Colloid stability  229

          The  rate  at  which particles aggregate is given by
               dn
             _. _„, —•£••»•* 2
                  -
                  — , &2/I
               df
        where n  is the  number of  particles  per  unit  volume of sol at  time  t,
        and  k 2  is a second-order  rate constant,
           Integrating, and putting n -  n 0 at t = 0, gives




          During  the  course  of  coagulation  k 2  usually  decreases,  and
        sometimes  an equilibrium  state  is reached  with the  sol only partially
        coagulated. This may be a consequence  of the height of the repulsion
        energy  barrier  increasing with  increasing particle  size.  In  experimental
        tests  of  stability theories  it  is usual  to  restrict  measurements  to  the
        early stages of coagulation (where the aggregating mechanism is most
        straightforward),  using moderately  dilute  sols.
          The  particle  concentration  during early  stages  of coagulation  can
        be  determined  directly,  by  visual  particle  counting,  or  indirectly,
        from  turbidity  (spectrophotometric  or  light  scattering)  measure-.
              23 110 204
        ments '   '  .  If  necessary,  coagulation  in  an  aliquot of  sol  can  be
        halted  prior  to  examination by the  addition  of  a  small  amount  of  a
        stabilising agent, such as gelatin. The  rate constant k 2  is given as the
        slope of  a plot  of  l/n  against  t.
          In most colloid stability studies, coagulation  rates are measured, as
        far  as  possible,  under  perikinetic  (non-agitated)  conditions,  where
        particle-particle  encounters  are  solely  the  result  of  Brownian
        motion. Particle  aggregation  under orthokinetic (agitated)  conditions
        is  of  technological  importance.  Agitation increases  the  particle  flux
        by  a  factor  which  depends  on  the  third  power  of  the  collision
        diameter  of the  particles.  With large particles,  such  as in  emulsions,
                                                           4
        orthokinetic aggregation  can occur  at up to  as much as  10  times the
        perikinetic  rate; but, with  particles  at  the  lower end of the  colloidal
        size  range,  stirring  has  relatively  little  effect  on  their  rate  of
        aggregation.
          The potential energy barrier to coagulation  can be reduced  to zero
        by  the  addition  of  excess  electrolyte,  which creates  a  situation  in
        which  every  encounter  between  the  particles  leads  to  permanent
        contact.  The  theory  of  rapid  (diffusion-controlled) coagulation  was
                                 110
        developed  by Smoluchowski .  For  a monodispersed  sol containing
   235   236   237   238   239   240   241   242   243   244   245