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206  Chapter 8: Catalysis and Catalytic Reactions

                           concentration gradient Cc, and for  77  are summarized in Table 8.1 in terms of a Thiele
                           modulus appropriate to each shape, as dictated by the form of the diffusion equation
                           in each case. Table 8.1 includes the case of a flat plate with two faces permeable.
                             The results for spherical and cylindrical shapes are approximately in accordance with
                           those shown in Figure 8.11, and in the limit of 4 +  large, become the same, if the Thiele
                           modulus is normalized in terms of a common effective diffusion-path-length parameter,
                           L,, defined by


                                                          volume of particle
                                               L,  =                                         (8.516)
                                                     exterior permeable surface area


                           Then the Thiele modulus normalized for shape is, for first-order kinetics:



                                                   4’  = L,(k/JD,)‘”  (n = 1)3               (8.517)


                             The consequences of this normalization are summarized for the various shapes in
                           Table 8.2. In Table 8.2, subscripts  FPl  and FP2 refer to a flat plate with 1 and 2 faces
                           permeable, respectively, and subscripts s  and c refer to sphere and cylinder, respec-
                           tively, all as given in Table 8.1. The main consequence is that, if  4’  replaces  4  in Figure
                           8.11,7  for all shapes lies approximately on the one line shown. The results become ex-
                           actly the same for large values of  $‘(q + l/+‘, independent of shape). In the transition
                           region between points G and H, the results differ slightly (about 17% at the most).

                                 Table 8.1  Effectiveness factor  (7)  for various particle shapes (assumptions in
                                 Example 8-4)
                                  Shape          4                 9                    rl

                                 flat  platea  L( k*ID,)‘”  cosh[4(  1 - z)]/cosh  4  (tanh  4114
                                 flat  plateb  L( kAID,)1’2  cosh[+(  $ - z)]/cosh(+/2)  tanh(@2)/(+/2)
                                                               R sinh(@/R)
                                  sphereC    R( kA/D,)‘/2      -
                                                               r   sinh  C#J       g&&J
                                 cylinder’   R(kA/D,)“2      (in terms of Bessel   3  (ratio of BF)
                                                              functions  (BF))
                                 a  One face permeable as in Example 8-4; see Figure  8.10(a).
                                 b  Two faces permeable.
                                 c  R  is particle radius; r  is radial coordinate (r  =  0 at center of particle).


                                        Table 8.2  Thiele modulus  (4’)  normalized with respect to shape
                                        and asymptotic value of  v

                                                                        Asymptotic value of  77
                                          Shape        -L
                                        flat plate (1)  L
                                        flat plate (2)  Ll2
                                          sphere      RI3
                                         cylinder     RI2



                           3See  footnote 2
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