Page 230 - Introduction to Colloid and Surface Chemistry
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Colloid stability  219

        If the  two particles are of the same material, this expression becomes

                  =                                            (8,13)
               m
                                                         I9
        giving  values of A i3l  for hydrosols of up to  about  10"  J.
          A 132  will  be  positive  (interparticle attraction) where AH  and  A 22
        are  either both  greater  than  or  both  less than A 33.  However,  in the
        unusual situation where A 33 has a value intermediate between those
        of AH  and A 22, then A i32 is negative -  i.e. a repulsive van der Waals
        interaction  between the  particles  is predicted,
               for the  interaction  of particles of the same material is always
          A m
        positive -  i.e.  the van der Waals interaction  energy is always one of
        attraction. This interaction will be weakest when the particles and the
        dispersion  medium are  chemically similar, since AH  and A 33  will  be
        of  similar magnitude and the  value of A m  will  therefore, be low.

        Potential energy curves

        The  total  energy of interaction between  the  particles  in a lyophobic
        sol is obtained  by summation of the  electric double layer and van  der
        Waais energies,  as illustrated in Figure  8.2.
          The  general  character  of  the  resulting  potential  energy-distance
        curve  can  be  deduced  from  the  properties  of  the  two  components.
        For  the  interaction  between  particles  of  the  same  material,  the
        double-layer  repulsion  energy  (equation  (8.5))  is  an  approximately
        exponential  function  of  the  distance  between  the  particles  with  a
        range  of the order  of the  thickness of the double  layer (I/*), and  the
        van  der  Waals  attraction  energy  (equation  (8.10))  decreases  as  an
        inverse  power  of  the  distance  between  the  particles.  Consequently,
        van  der  Waals  attraction  will  predominate  at  small*  and  at  large
        interparticle distances.  At intermediate distances  double-layer  repul-
        sion  may  predominate,* depending  on  the  actual  values  of  the  two
        forces.  Figure  8.2  shows  the  two  general  types  of  potential  energy
        curve which are possible. The total potential energy curve V(l)  shows
        a repulsive  energy maximum, whereas in curve  V(2)  the  double-layer
        repulsion  does not predominate  over van der Waals attraction  at any
        interparticle  distance.
          'Repulsion due to overlapping of electron clouds (Born repulsion) predominates at
        very  small  distances  when  the  particles  come  into  contact,  and  so  there  is a  deep
        minimum  in the  potential energy curve which  is not shown  in Figures 8.2-8.4.
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