Page 480 - Modelling in Transport Phenomena A Conceptual Approach
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460     CHAPTER 10.  UNSTEADY MICROSCOPIC BAL. WITHOUT GEN.

             The physical significance and the order of  magnitude of  the terms in &.  (10.3-7)
             are given in Table 10.6.


             Table 10.6  The physical significance and the order of  magnitude of  the terms in
             Eq. (10.3-7).
                Term       Physical Significance   Order of  Magnitude

                             Rate of  diffusion

                 -         Rate of  accumulation     cAl  - CA,
                 aCA
                  at            of  mass A               t

             Therefore, the ratio of the rate of  diffusion to the rate of  accumulation of  mass A
             is given by

                       Rate of diffusion    -  DAB (CA~ - CA,)/L~ DAB t
                                            -
                                                                -
                 Rate of  mass A accumulation    (CAI  - cAo        L2      (10.3-10)
             which is completely analogous to the Fourier number, Fo .
                Introduction of  the dimensionless quantities

                                          e=   CAI  - CA                    (10.3-11)
                                              CAI - CA,
                                                  z
                                              E=,                           (10.3-12)

                                                'DAB t
                                            7-z-                            (10.3-13)
                                                 L2
             reduces Eqs.  (10.3-7) and (10.3-8)  to
                                            ae   =-
                                                  a2e
                                            -
                                            87-  at2                        (10.3-14)
                                       at  r=O       e=i
                                       at  E=l       e=o                    (10.3-15)
                                       at  E=-1      e=O
             Note the  Eqs.  (10.3-14)  and (10.3-15)  are identical waUh Eqs.  (10.2-14,  and (10.2-
             15).  Therefore, the solution given by  Eq. (10.2-32)  is also valid  for  this  case,
             i.e.,
                              00
                              00
                                                          +
                                                                            (10.3-16)
                                                            ;)
                                                      s [(n + ;)   74       (10.3-16)
                                                       [(n
                                                      s
                                                               74
                             n=O
                             n=O
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