Page 616 - Bird R.B. Transport phenomena
        P. 616
     596   Chapter 19  Equations of Change for  Multicomponent Systems
                           This is to be solved  with the boundary conditions
                           B.C.1:                      atz  = 0,  c  = c                      (19.4-21)
                                                                  A   A0
                           B.C. 2:                     at  r  =  R,  c A  =  0                (19.4-22)
                           B.C. 3:                     at  r = 0,  c A  = finite              (19.4-23)
                           For  short distances z into the reactor, the concentration c A  differs  from  c A0  only  near the wall,
                           where the velocity  profile  is practically  linear. Hence we  can introduce the variable  у  = R -  r,
                           neglect  curvature  terms, and  replace  B.C. 3 by  a fictitious  boundary  condition at у  =  oo (see
                           Example  12.2-2  for  a detailed  discussion  of  this method  of  treating the entrance region  of the
                           tube).
                              The  reformulated  problem statement is then
                                                                      д
                                                            У  дСА      С А
                                                       2v z ma x        2                     (19.4-24)
                                                         '  R  dz     ду
                           with the boundary conditions
                           B.C. 1:                     at  z  =  0,   С А0                    (19.4-25)
                           B.C. 2:                     at  у  =  0,  <м  = 0                  (19.4-26)
                           B.C. 3:                     at  у  =  oo,  С А  =  С А0            (19.4-27)
                           This problem can be solved  by the method of combination of independent variables  by  seeking
                                                                            2
                                                                                  1/3
                           a  solution  of the form c /c A0  = /(17), where  77 = (y/R)(2z; zmax R /92)^ z) . One thus obtains the
                                                                                s
                                             A
                           ordinary differential  equation/" + З77/' = 0, which can be integrated to give (see Eq. C.I-9)
                                                         2
                                                    f       —               —   —
                                                                            3
                                                    Jo  exp(-77       exp(-rj )drj             (19.4-28)
                                               C A0
                                                    Jo
                           This problem  is mathematically  analogous  to the Graetz problem  of Problem  12D.4, в  of that
                           problem being  analogous  to 1 -  (c /c )  here.
                                                        A0
                                                      A
                              Experiments  of the type  described  here  have  proved  useful  for obtaining  mass  transfer
                           data  at  high  Schmidt  numbers.  2  A  particularly  attractive  reaction  is  the reduction  of  ferri-
                           cyanide ions on metallic  surfaces  according to the reaction
                                                     Fe(CN)  2     > Fe(CN) " 4                (19.4-29)
                                                           6              6
                           in  which  ferricyanide  and ferrocyanide  take the place  of Л and В in the above  development.
                           This  electrochemical  reaction is quite  rapid  under  properly  chosen  conditions. Furthermore,
                           since  it involves  only  electron  transfer,  the physical  properties  of the solution  are almost en-
                           tirely  unaffected.  The forced  diffusion  effects  neglected  here may be suppressed  by the addi-
                           tion  of an indifferent  electrolyte in excess. ' 3 4
                           Figure  19.4-3 shows  schematically  how  oxygen  and carbon monoxide combine at a catalytic
      EXAMPLE   19.4-3
                           surface  (palladium)  to  make  carbon  dioxide,  according  to  the  technologically  important
     Catalytic Oxidation   reaction 5
     of Carbon Monoxide                                  O, + 2CO -> 2CO,                      (19.4-30)
                              2
                                D. W. Hubbard and  E. N. Lightfoot, bid.  Eng.  Chem. Fundam.,  5, 370-379  (1966).
                              3
                                J. S. Newman, Electrochemical Systems, 2nd edition, Prentice-Hall, Englewood  Cliffs,  N.J. (1991), §1.10.
                                J. R. Selman and C. W. Tobias, Advances  in Chemical Engineering, 10, Academic Press, New  York,
                              4
                           N.Y. (1978), pp. 212-318.
                               В. С  Gates, Catalytic Chemistry, Wiley, New York  (1992), pp. 356-362; C. N. Satterfield,
                              5
                           Heterogeneous Catalysis in Industrial  Practice, McGraw-Hill, New York, 2nd edition (1991), Chapter 8.
     	
