Page 540 - Bird R.B. Transport phenomena
P. 540

520  Chapter 17  Diffusivity  and the Mechanisms of Mass Transport

                           We may now calculate the flux  of helium from  Eq. 17.1-1 as
                                                                          2.04  X 1Q-
                                              j  = (2.6 g/cm )(2.0  X 1(T  cm /s)
                                                                      2
                                                         3
                                                                   8
                                              Ay                              3
                                                                           10~ cm
                                                                 2
                                                =  1.05  X 10" 11  g/cm s                      (17.1-13)
                               Next, the velocity  of the helium can be obtained from  Eq. 17.1-4:
                                                              _  ]Лу
                                                                                               (17.1-14)
                           At the lower  surface  of the plate (y = 0) this velocity  has the value
                                               1.05  X  10" g/cm s
                                                        n
                                                              2
                                                                    =  1-98  x                 (17.1-15)
                                                        7
                                                5.3  X 10~  g/cm 3
                           The  corresponding value  v  of the mass average  velocity  of the glass-helium  system  at у  = 0
                                                yQ
                           is then obtained from  Eq. 17.1-3
                                                   7
                                                              5
                                                                                      7
                                      v  = (2.04 X 10" )(1.98  X 10~  cm/s  + v )  + (1 -  2.04  X 10" )  (0)  (17.1-16)
                                       y0                             y0
                                                    7
                                                              5
                                           (2.04 X 1Q- )(1.98 X 10~  cm/s)
                                         =
                                      Vy0        1 -  (2.04  X  10~ )
                                                             7
                                                    12
                                         =  4.04X  10~ cm/s
                           Thus  it is  safe  to neglect v  in Eq. 17.1-14, and the analysis  of  the experiment in Fig. 17.1-1 at
                                                y
                           steady state is accurate.
       EXAMPLE   17.1-2    Show  that only  one diffusivity  is  needed  to describe  the diffusional  behavior  of  a  binary
                           mixture.
      The  Equivalence  of
                           SOLUTION
                           We begin by writing  Eq. 17.1-6 as  follows:
                                                         -
                                                     ]  = <3) V(D  =  + <$ Va)                 (17.1-17)
                                                     B   P  BA  B   P  BA  A
                           The  second form  of this equation follows  from the fact that io  + o)  = 1. We  next use the vec-
                                                                            A   B
                           tor  equivalents  of Eqs. 17.1-3 and 4 to write
                                                     )  = pa> {v  -  o) v  -  o) v )
                                                      A     A  A   A A   B B
                                                       =  pa) ((l  -  <x) )v  ~ o) v )
                                                            A      A  A   B B
                                                                 -  v )                        (17.1-18)
                                                                    e
                           Interchanging A  and  В in this expression  shows  that \ =  —] . Combining this with  the sec-
                                                                       A     B
                           ond  form  of  Eq. 17.1-17 then gives
                                                          )  A                                 (17.1-19)

                           Comparing this with  Eq. 17.1-5 gives  %b BA  = ЯЬ .  We  find  that the order of subscripts  is unim-
                                                                 АВ
                           portant  for  a  binary  system  and  that only  one  diffusivity  is  required  to describe  the  diffu-
                           sional behavior.
                               However, it may well  be that the diffusivity  for  a dilute solution  of Л in В and that for a
                           dilute solution  of  В in A  are numerically different.  The reason  for  this is that the diffusivity  is
                           concentration-dependent, so that the two  limiting values  mentioned above  are the values  of
                           the  diffusivity  %b  = 4b  at two different concentrations.
                                        BA    AB
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