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8.5 Heterogeneous Catalysis: Kinetics in Porous Catalyst Particles 203

                             That is, on applying equation 8.5-4 to both faces of the strip, we have


                                         -D,Ac%  = -D,A,   [$$  +  & &)dx]    + (-rA)A,dx       (8.5-6)


                             for any surface kinetics, where A, is the cross-sectional area perpendicular to the direction
                             of diffusion of A  (A,  is constant here and cancels). The rate law for (-   rA)  is not specified,
                             but the units of (-I*)  are mol A rnd3 (particle) s-l. If we introduce first-order kinetics
                             ((-rA)  = kAcA), equation 8.5-6 becomes

                                                       d2c,ldx2  -  k,c,lD,  = 0                (8.5-7)

                             To obtain a nondimensional form of this equation, we define dimensionless concentration,
                             I/J,  and length, z, respectively, as
                                                            t+b = c,/c,                         (8.5-8)
                                                              z  = XlL                          (8.5-9)

                             Equation 8.5-7 in nondimensional form is then

                                                      d2$ldz2   - (kAL2/D,>+  =  0             (8.5-10)

                             The coefficient of  $  in equation 8.5-10 is used to define a dimensionless group called the
                             Thiele modulus,2  4:


                                                     C#I  = L(k,lD,)“2  (n = 1)               (8.5-11)  1


                             so that equation 8.5-10 becomes

                                                         d2+ldz2   -  42$ = 0                  (8.512)

                               The importance of  4  is that its magnitude is a measure of the ratio of intrinsic reaction
                             rate (through kA)   to diffusion rate (through 0,).   Thus, for a given value of kA,   a large value
                             of  4  corresponds to a relatively low value of  D,,  and hence to relatively high diffusional
                             resistance (referred to as “strong pore-diffusion” resistance). Conversely, a small value of
                             $J  corresponds to “negligible pore-diffusion” resistance.
                               The solution of equation 8.5-12 provides the concentration profile for  I,!J  as a function of
                             z,  +(z).  On integrating the equation twice, we obtain

                                                         t/t  = Cle4z  + C2e-4z               (8.5-12a)

                             where  Ct  and  C2  are integration constants to be obtained from the boundary conditions:

                                                         at z = 0,   $=l                      (8.512b)
                                                       atz = 1,    dr+Wdz  =  0               (SS-lk)



                             *Equation 8.5-11 applies to a first-order surface reaction for a particle of flat-plate geometry with one face
                             permeable. In the next two sections, the effects of shape and reaction order on I$  are described. A general form
                             independent of kinetics and of shape is given in Section 8.5.4.5. The units of kA   are such that 4  is dimensionless.
                             For catalytic reactions, the rate constant may be expressed per unit mass of catalyst (k&,,.   To convert to kA   for
                             use in equation 8.5-11 or other equations for C#J,  (k,&,   is multiplied by pP,   the particle density.
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