Page 191 - Modeling of Chemical Kinetics and Reactor Design
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Reaction Rate Expression  161

                                For any product C or D, the partial pressure is expressed as:


                                 p = C RT =  p   −  c  (π  − ) π                        (3-209)
                                  C
                                                   ∆ n  O
                                              CO
                                      C
                                For an ideal gas at both constant temperature and pressure, but with
                              changing number of moles during reaction, Levenspiel relates that

                                V = V (1 + ε X )                                        (3-210)
                                                A
                                             A
                                      O
                              where
                                     V          −  V           V     −  V
                                 ε =  all A reacted  no reaction  =  X A =1  X A =0
                                  A
                                            V no reaction          V X A =0             (3-211)

                                Levenspiel considers the cases where the relationship between
                              concentration and conversion of reacting specie is not obvious, but
                              depends on a number of factors.



                                        CASE 1: CONSTANT DENSITY SYSTEMS

                                This case includes most liquid reactions and also those gas reactions
                              that operate at both constant temperature and pressure with no change
                              in the number of moles during reaction.  The relationship between
                              concentration C  and fractional conversion X  is as follows:
                                             A
                                                                         A
                                 X =−    C A  and dX = −   dC A
                                     1
                                                      A
                                  A
                                        C                  C
                                          AO                 AO
                                 C A  =− X    and dC = −   C   dX
                                       1
                                 C AO      A          A     AO    A                     (3-212)

                              where ε  = 0. The changes in B and C to A are
                                     A

                                 C   − C     C   −  C  C C  − C CO
                                  AO    A  =  BO    B  =                                (3-213)
                                     a          b          c
                              or
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