Page 257 - Introduction to chemical reaction engineering and kinetics
P. 257

238 Chapter 9: Multiphase Reacting Systems

                            and (- RA)  and (-   Rn)  are related by
                                                         c-w = M-R,)                          (9.1-8a)

                            we  eliminate  (-RA),  (  -RB)  and  cAs  (Concentration    at the surface) from these four equa-
                            tions to obtain a differential equation involving  dR/dt,  which, on integration, provides the
                            desired relation. The equation resulting for  dR/dt  is








                            which leads to






                                                                                              (9.1-40)



                            from equation 9.1-34. For simplicity, we consider results for the two limiting cases of
                            equation 9.1-34 (ignoring  K21R’12   or  K,IR),   as described in Section 9.1.2.3.3.
                              For  small   particles, integration of 9.1-40 without the term  K21R’j2  results in


                                                                                    ,         (9.1-41)


                            or, since, for a spherical particle

                                                         fE  = 1 -  (R/RJ3                    (9.1-42)

                                                                                         II  (9.1-43)





                            The time tl  for complete reaction (fn  = 1) is


                                                      G=*(g+&)                                (9.1-44)


                              For  large  particles, the corresponding results (with the term  K,IR  in equation 9.1-40
                            dropped)  are:


                                                                                               (9.1-45)



                                                                     1  [
                                                        1 - (1 - fn)l’2 +  &-  1  - (1  - fs)“3  (9.1-46)
   252   253   254   255   256   257   258   259   260   261   262