Page 670 - Bird R.B. Transport phenomena
P. 670

650  Chapter  20  Concentration  Distributions  with  More Than One Independent Variable

                           with  a constant, provided  that  H o  = H (p, T) and C pA  = C fl8  = constant.  It is further  assumed
                                                          a
                           that  c, k, and p are essentially  constant.  Here  the dissipation  term  (T:VV)  and the work  term
                           2 (ja  * ga)  a r e  appropriately  neglected.  {Hint: Use the species  equation  of  continuity  of Eq.
                            a
                           19.1-10.)
                           (b)  Show  that the solution  of Eq. 20B.2-1, with  the initial  condition  that  T = T.  at t  = 0, and
                                                                                          A
                           the boundary  conditions  that T = T  at z  = 0 and T = Т.  at z =  <*, is
                                                       o
                                                                       л
                                                                             f )              (20B.2-2)
                                                 T,-T o
                           with
                                                              and  <p  = v*  Г-               (20В.2-3)
                                                                     T

                           (c)  Show  that the interfacial  mass and energy  fluxes are related  to T  and Т.  by
                                                                                       л
                                                                                 o
                                                N
                                              — _ A0  +  Nb0 —  = V^r(l  + erf <р )<р  ехр ^   (20В.2-4)
                                                                            т
                                                                         (
                                               [q /C (T  -  TJ]
                                                o  p  o
                           so  that N /q 0  and  N /q 0  are  constant  for  f  >  0.  This  nifty  result  arises  because  there  is  no
                                  A0
                                            B0
                           characteristic length or time in the mathematical model  of  the  system.
                    20B.3.  Stoichiometric  boundary  condition  for  rapid  irreversible  reaction.  The  reactant  fluxes  in
                           Example 20.1-2 must satisfy  the stoichiometric relation
                                              at z -  z (t),  c {v  -  v )  -  ~  c (v  -  v )  (20B.3-1)
                                                    R      A  lA  R       P  zB  K
                           in which  v R  = dz /dt.  Show  that this  relation  leads  to  Eq. 20.1-31  when  use  is  made  of  Fick's
                                        R
                           first  law, with  the assumptions  of constant с and instantaneous irreversible  reaction.
                    20B.4.  Taylor dispersion in  slit flow (Fig. 2B.3).  Show  that, for  laminar  flow  in a plane slit  of  width
                           IB  and length  L, the Taylor  dispersion  coefficient  is




                    20B.5.  Diffusion  from  an  instantaneous point source.  At  time  t  = 0, a mass  m A  of  species  Л  is  in-
                           jected  into a large body  of  fluid  B. Take the point  of  injection  to be  the origin  of  coordinates.
                           The material  A  diffuses  radially  in all  directions. The solution  may  be  found  in Carslaw  and
                           Jaeger:  2

                                                                            О                 (20В.5-1)
                                                                          л н
                           (a)  Verify  that Eq. 20B.5-1 satisfies Fick's second law.
                           (b)  Verify  that Eq. 20B.5-1 satisfies the boundary  conditions at r = <».
                           (c)  Show  that  Eq. 20B.5-1, when  integrated over all space, gives m , as required.
                                                                               A
                           (d)  What  happens  to Eq. 20B.5-1 when  t -> 0?
                    20B.6.  Unsteady diffusion  with  first-order  chemical reaction.  Use Eq. 20.1-43 to obtain the concen-
                           tration profile  for  the following  situations:
                           (a)  The stationary  semi-infinite  system  of  Problem 20C.3.



                              2
                                H. S. Carslaw  and  J. C. Jaeger,  Conduction of Heat  in Solids, 2nd  edition, Oxford  University  Press
                           (1959), p. 257.
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