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3.2  Diffusion Coefficients  77


         The Stokes-Einstein  and Wilke-Chang  equations predict
       an inverse dependence of  liquid diffusivity with viscosity.
       The Hayduk-Minhas  equations predict a somewhat smaller
       dependence on viscosity. From data covering several orders
       of magnitude variation of viscosity, the liquid diffusivity is
       found to vary inversely with the viscosity raised to an expo-
       nent  closer  to  0.5  than  to  1.0. The  Stokes-Einstein  and
       Wilke-Chang  equations  also  predict  that  DABpB/T is  a
                                                            Use the Vignes equations to estimate diffusion coefficients over
       constant over a narrow temperature range. Because p~ de-
                                                          the entire composition range.
       creases exponentially with temperature, DAB is predicted to
       increase exponentially with temperature. For example, for a
       dilute solution of water in ethanol, the diffusivity of  water   SOLUTION
       increases by a factor of almost 20 when the absolute temper-
                                                          Using  a  spreadsheet  to  compute  the  derivatives  in  (3-45)  and
       ature is increased 50%. Over a wide temperature range, it is   (3-46), which are found to be essentially equal at any composition,
       preferable to express the effect of temperature on DAB by an   and the diffusivities from the same equations, the following results
       Arrhenius-type expression,                         are obtained with DAB = DBA at each composition. The calcula-
                                                          tions  show  a  minimum  diffusivity  at  a  methanol  mole  fraction
                                                          of 0.30.



       where, typically the activation energy for liquid diffusion, E,
       is no greater than 6,000 callmol.
         Equations (3-39), (3-40), and (3-42) for estimating diffu-
       sivity in binary liquid mixtures only apply to the solute, A, in
       a dilute solution of the solvent, B. Unlike binary gas mix-
      tures in which the diffusivity is almost independent of com-
      position, the effect of  composition on liquid diffusivity is
       complex, sometimes showing  strong positive  or  negative   If the diffusivity is assumed linear with mole fraction, the value at
      deviations from linearity with mole fraction.       XA  = 0.50 is  1.625 x  lop5, which is almost 40% higher than the
         Based on a nonideal form of Fick's law, Vignes  [9] has   predicted value of 1.18 x  lop5.
       shown that, except for strongly associated binary mixtures
       such as chloroform/acetone, which exhibit a rare negative de-
      viation from Raoult's law, infinite-dilution binary diffusivi-   Diffusivities of Electrolytes
      ties, (D),,  can be combined with mixture activity-coefficient   In an electrolyte solute, the diffusion coefficient of the dis-
      data or correlations thereof to predict liquid binary diffusion   solved salt, acid, or base depends on the ions, since they are
      coefficients DAB and DBA over the entire composition range.   the diffusing entities. However, in the absence of an electric
      The Vignes equations are:                           potential,  only  the  molecular  diffusion  of  the  electrolyte
                                                          molecule is of interest. The infinite-dilution diffusivity of a
                                                          single salt in an aqueous solution in cm2/s can be estimated
                                                          from the Nernst-Haskell  equation:




                                                          where
       EXAMPLE 3.7                                          n+ and n-  = valences of the cation and anion,
                                                                       respectively
      At  298  K  and  1 atm,  infinite-dilution  diffusion  coefficients  for
      the  methanol  (A)/water  (B)  system  are  1.5 x lop5  cm2/s  and   A+  and A-  = limiting ionic conductances in (A,/cm2)
       1.75 x   cm2/s for AB and BA, respectively.                     (~/cm)(g-equiv/cm3),  where A = amps and
         Activity-coefficient data for the same conditions as estimated   V = volts
      from the UNIFAC method are as follows:
                                                                   F = Faraday's constant
                                                                     = 96,500 coulombs/g-equiv
                                                                   T = temperature, K
                                                                   R = gas constant = 8.3 14 Jlmol-K

                                                          Values of A+  and A-  at 25'C  are listed in Table 3.7. At other
                                                          temperatures,  these  values  are  multiplied  by  T/334pB,
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