Page 585 - Bird R.B. Transport phenomena
P. 585

§18.7  Diffusion  and Chemical Reaction Inside a Porous Catalyst  565

                    We  now  define an  "effective  diffusivity"  for  species  A  in the porous medium  by
                                                         dc,
                                                дг . = -Q)  -                        (18.7-4)
                                                 Л;     A
                 in  which  c A  is  the concentration  of  the  gas  A  contained  within  the pores.  The  effective
                 diffusivity  %b  must be  measured  experimentally.  It depends  generally  on pressure  and
                             A
                 temperature and  also  on the catalyst  pore structure. The actual mechanism  for  diffusion
                 in pores  is  complex,  since  the pore dimensions  may  be  smaller  than  the mean  free  path
                 of  the  diffusing  molecules.  We  do  not belabor  the question  of  mechanism  here but  as-
                 sume only that Eq. 18.7-4  can adequately  represent the diffusion  process  (see §24.6).
                    When  the  preceding  expression  is  inserted  into  Eq.  18.7-3,  we  get,  for  constant
                 diffusivity

                                                                                     (18.7-5)
                                                      dr
                 We  now  consider  the  situation  where  species  A  disappears  according  to  a  first-order
                 chemical  reaction  on  the  catalytic  surfaces  that  form  all  or  part  of  the  "walls"  of  the
                 winding  passages.  Let a be  the available  catalytic  surface  per  unit  volume  (of  solids  +
                 voids). Then R  =  -k"ac ,  and  Eq. 18.7-5 becomes  (see Eq. C.l-6)
                             A       A
                                               1  d  (ДЛСА                           (18.7-6)
                                                      dr
                 This  equation  is  to be  solved  with  the boundary  conditions that c A  =  c AR  at  r  =  R, and
                 that c  is  finite  at r  = 0.
                     A
                                                            2
                                                     2
                    Equations containing the operator  (l/r )(d/dr)[r (d/dr)]  can frequently  be  solved  by
                 using  a  "standard  trick"—namely,  a change  of  variable  c /c  =  (l/r)/(r). The equation
                                                                 A  AR
                 for/(r)  is  then
                                                                                     (18.7-7)
                 This is a standard second-order differential  equation, which  can be solved  in terms  of  ex-
                 ponentials or hyperbolic  functions.  When  it is  solved  and  the result  divided  by  r we  get
                 the following  solution  of  Eq. 18.7-6 in terms  of hyperbolic  functions  (see §C5):

                                                                 I*-                 (18.7-8)

                 Application  of the boundary conditions gives  finally

                                                                                     (18.7-9)


                     In studies  on chemical kinetics and catalysis  one is frequently  interested  in the molar
                 flux  N AR  or the molar flow  W AR  at the surface  r  —  R:

                                                2
                                       W fiR  = 4irR N AR  =  -                     (18.7-10)
                 When  Eq. 18.7-9 is used  in this expression,  we  get
                                                                                    (18.7-11)


                 This result gives the rate of conversion  (in moles/sec)  of Л to В in a single  catalyst  particle
                 of radius R in terms  of the parameters describing  the diffusion  and reaction  processes.
   580   581   582   583   584   585   586   587   588   589   590