Page 47 - Introduction to Colloid and Surface Chemistry
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38  Kinetic properties

        mass material to  which  the  membrane is permeable  can  virtually  be
        eliminated.
          The  usefulness of osmotic pressure measurements is, nevertheless,
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                                                         4
        limited  to  a relative molecular mass range of about  10 -10 .  Below
          4
        10 , permeability of the membrane to the molecules under considera-
                                                   6
        tion might prove to be troublesome; and above  10 , the osmotic  pres-
        sure  will  be  too  small to  permit  sufficiently  accurate  measurements.
          Osmosis  takes  place  when  a  solution  and  a  solvent  (or  two
        solutions of different  concentrations)  are separated  from  each  other
        by a semipermeable membrane -  i.e. a membrane which is permeable
        to  the  solvent  but  not  to  the  solute.  The  tendency  to  equalise
        chemical potentials (and, hence, concentrations)  on either  side of the
        membrane results in a net  diffusion  of solvent across  the  membrane.
        The counter-pressure necessary to balance this osmotic flow is termed
        the  osmotic pressure.
          Osmosis  can  also  take  place  in  gels and  constitutes  an  important
        swelling mechanism.
          The  osmotic  pressure  II of a solution is described  in general terms
        by  the  so-called  viral equation
                    (  1         2      }
             U  = cRT\  —  + B 7c + B*c  +  .  .  .            (2.21)
                    (M                  )
        where  c  is  the  concentration  of  the  solution  (expressed  as  mass of
        solute  divided  by  volume of  solution),  M  is  the  molar  mass  of  the
        solute,  and # 2, #3, etc.,  are constants.
          Therefore,

             M = /?7Vlimn/c                                    (2.22)
                      c-»0                                    X
          Deviations  from  ideal  behaviour  are  relatively  small for  solutions
        of  compact  macromolecules  such  as  proteins  but  can  be  quite
        appreciable  for  solutions  of  linear  polymers.  Such  deviations  have
                                      137 138
        been  treated  thermodynamically ' ,  mainly  in  terms  of  the
        entropy  change  on  mixing,  which  is considerably  greater  (especially
        for  linear polymers dissolved  in good solvents) than the ideal  entropy
        change  on  mixing for  a  system  obeying  Raoult's  law. This  leads  to
        solvent  activities  which  are  smaller  than  ideal  -  i.e.  an  apparent
        increase  in  the  concentration  and  an  actual  increase  in  the  osmotic
        pressure  of the  polymer  solution.
          The  resulting relative  molecular  mass refers  to the  composition of
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