Page 320 - Advanced Thermodynamics for Engineers, Second Edition
P. 320

310    CHAPTER 14 CHEMICAL KINETICS




             where
                                 q ¼ 4
                                 n ij ¼ stoichiometric coefficient of i in reaction j
                                             0
                                                    00
                                  A 1 ¼ CO 2  n ¼ 1  n ¼ 0
                                             1      1
                                                    00
                                             0
                                  A 2 ¼ H 2  n ¼ 1  n ¼ 0
                                             2
                                                    2
                                             0
                                                    00
                                  A 3 ¼ H 2 O  n ¼ 0  n ¼ 1
                                             3
                                                    3
                                                    00
                                             0
                                  A 4 ¼ CO  n ¼ 0  n ¼ 1
                                                    4
                                             4
                The law of mass action, which is derived from the kinetic theory of gases, states that the rate of
             formation, or depletion, of a species is proportional to the product of molar concentrations of the
             reactants, each raised to the power of its stoichiometric coefficient. Hence the rate of formation of
             species j, for an elementary reaction, is
                                             n 1j  n 2j      n nj
                                       R j f½A 1 Š  ½A 2 Š  ..::½A n Š
             or
                                           n                                              (14.6)
                                           Y
                                       R j f  ½A i Š n ij  for ð j ¼ 1; ...sÞ:
                                           i¼1
             and s ¼ total number of simultaneous reactions.
                Equation (14.6) may be written as
                                             n
                                            Y
                                                  n ij
                                      R j ¼ k j  ½A i Š  for ð j ¼ 1; ...sÞ;              (14.7)
                                            i¼1
             where k j is the rate constant for the reaction. In Eqns (14.1)–(14.5) the reaction was described as
             having a forward and backward direction, with rates k f and k b . The reaction shown in Eqn (14.7) can be
             described in this way as
                                             n
                                                  n 0
                                            Y
                                     R fj ¼ k fj  ½A i Š  ij  for ð j ¼ 1; ...sÞ;         (14.8)
                                            i¼1
             and
                                              n
                                                  n
                                             Y     00
                                     R bj ¼ k bj  ½A i Š  ij  for ð j ¼ 1; ...sÞ:         (14.9)
                                             i¼1
                The rate of change with time of species i is proportional to the change of the stoichiometric co-
             efficients of A i in the reaction equation (the system is effectively a first-order one attempting to achieve
             the equilibrium state). Thus, for the forward direction

                                                     n              n
                                 d½A i Š            Y      0        Y     0
                                        ¼ n   n ij  k fj  ½A i Š ¼ Dn ij k fj  ½A i Š  ij  (14.10)
                                                           ij
                                     j      0   00        n              n
                                            ij
                                   dt
                                      f             i¼1             i¼1
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