Page 32 - Introduction to Colloid and Surface Chemistry
P. 32

Kinetic properties  23


        Factional ratios

        The  frictional  coefficient  of  an  asymmetric particle  depends  on  its
        orientation.  At  low velocities such particles are  in a state of random
        orientation through accidental disturbances,  and the resistance  of the
        liquid  to  their  motion  can  be  expressed  in  terms  of  a  frictionai
        coefficient  averaged  over  all  possible  orientations.  For  particles  of
        equal  volume  the  frictional  coefficient  increases  with  increasing
        asymmetry.  This  is because,  although  the  resistance  of  the  liquid is
        reduced  when the  asymmetric particle  is end-on  to  the  direction  of
        flow, it  is increased  to  a greater  extent  with  side-on  orientations,  so
        that  on  average  there  is  an  increase  in  resistance.  The  frictional
        coefficient  is also  increased  by particle  solvation.
          A  particle containing a  given volume of dry  material  will have  its
        smallest  possible  frictional coefficient, / 0, in a particular liquid when
        it is in the  form  of an  unsolvated sphere. The frictional  ratio, f/f Q  (i.e.
        the ratio of the actual frictional  coefficient  to the frictional  coefficient
        of  the  equivalent  unsolvated  sphere)  is,  therefore,  a  measure  of  a
        combination  of asymmetry  and  solvation.
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          With  application  to  dissolved  proteins  in  mind,  Oncley  has
        computed  frictional  ratios  for  ellipsoids  of  revolution  of  varying
        degrees  of asymmetry and hydration. The  resulting contour diagram
        (Figure  2.1)  shows  the  combinations  of  axial  ratio  and hydration
        which  are  compatible  with  given  frictional  ratios.  The  separate
        contributions  of  asymmetry and  hydration  cannot  be  determined
        unless other  relevant information  is available.



        Brownian motion and translational diffusion

        Brownian  motion

        A  fundamental consequence  of  the  kinetic  theory  is  that,  in  the
        absence of external forces,  all suspended  particles, regardless  of their
        size, have the same average translational kinetic energy. The  average
                                                 3
        translational  kinetic energy for any particle is MT,  or  VikT  along a
                      l           l
        given axis -  i.e. /2m(dxldtf  = /ikT, etc.; in other words, the average
        particle  velocity increases  with  decreasing  particle  mass.
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