Page 38 - Introduction to Colloid and Surface Chemistry
P. 38

Kinetic properties  29

        reciprocal of the  ffictional  ratio /// 0. Charge  effects  are discussed  on
        page  37.

        Measurement of diffusion coefficients 27

        Free boundary  methods

        To  study  free  diffusion,  a  sharp  boundary  must  first  be  formed
        between the solution and the solvent (or solution of lower concentra-
        tion)  in  a  suitable  diffusion  cell.  One  of  the  most  satisfactory
        techniques for  achieving this end  is the  sliding method illustrated in
        Figure  2.3.  The  boundary can  be  displaced  away  from  the ground-
        glass flanges to  facilitate  optical observation,  and  can  be  sharpened
        even  further  by  gently  sucking  away  any  mixed  layers  with  an
        extremely fine capillary tube inserted  from  above.











         Figure 2.3  Formation  of an initially sharp boundary between two miscible liquids

          As  diffusion  proceeds,  concentration  and  concentration gradient
        changes will take place as illustrated in Figure 2.4. To ensure that the
        broadening  of  the  boundary is due  to  diffusion  only, very  accurate
        temperature control (to avoid convection currents) and freedom  from
        mechanical vibration must be maintained. The  avoidance of convec-
        tion  is  a  problem  common  to  all  kinetic  methods  of  investigating
        colloidal  systems.
          Concentration  changes  are  observed  optically  from  time  to  time
        either  by  light  absorption  (e.g.  ultraviolet  absorption  for  protein
        solutions)  or,  more  usually, by  schlieren  or  interference  methods.
        These optical  methods for examining concentration changes in liquid
        columns (especially  the  schlieren technique in its various forms)  are
        also  employed  in  the  ultracentrifuge  and  for  studying moving-
        boundary electrophoresis. The schlieren method is based on the  fact
        that,  at  a  boundary  between  two  transparent  liquids  of  different
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