Page 262 - Introduction to Colloid and Surface Chemistry
P. 262

Rheology  251


        Electroviscous  effects

        When  dispersions  containing  charged  particles  are  sheared,  extra
        energy  is required  to  overcome  the  interaction  between  ions  in  the
        double  layers  around  the  particles  and  the  electrical  charge  on  the
        particle  surfaces,  thus leading  to  an  increased  viscosity.
          For charged flexible chains, in addition  to the  above  effect  (which
        is usually  small),  the  nature  of the  double  layer influences  the chain
        configuration.  At  low  ionic  strengths  the  double-layer  repulsions
        between  the  various parts  of the flexible chain have a relatively long
        range and  tend  to give the chain an extended  configuration, whereas
        at  high  ionic  strengths  the  range  of  the  double-layer  interactions is
        less,  which  permits  a  more  coiled  configuration.  Therefore,  the
        viscosity  decreases with  increasing ionic strength, often  in a marked
        fashion.



        Polymer relative molecular masses from  viscosity measurements

        Viscosity  measurements  cannot  be  used  to  distinguish  between
        particles  of  different  size  but  of  the  same  shape  and  degree  of
        solvation.  However,  if the  shape  and/or  solvation  factor  alters  with
        particle  size,  viscosity  measurements  can  be  used  for  determining
        particle  sizes.
          If  a  polymer  molecule  in  solution  behaves  as  a  random  coil,  its
        average  end-to-end  distance  is proportional  to  the  square  root of its
                                                             5
        extended  chain length (see  page 25) -  i.e.  proportional  to M? , where
            is the  relative  molecular  mass.  The  average  solvated  volume of
        M T
                                                          5
        the  polymer  molecule  is, therefore,  proportional  to  A/J  and,  since
        the  unsolvated  volume is proportional  to  Af r,  the  average  solvation
                                             5
                                 5
        factor  is proportional  to  A/J /A/ r (i.e.  M? ). The  intrinsic viscosity of
        a  polymer solution is, in turn, proportional  to  the  average solvation
        factor  of the polymer  coils -  i.e.
             foj  =  KM?- 5

        where  K  is a proportipnality  constant.
          For most  linear  high polymers  in solution  the chains are  somewhat
        more  extended  than  random,  and  the  relation  between  intrinsic
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