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5.3 Reversible Reactions 95

                           In this form, the sets of exponents czi and a/ are related to each other by restrictions
                           imposed by thermodynamics, as shown in the next section.

      5.3.2  Thermodynamic Restrictions on Rate and on Rate Laws

                           Thermodynamics imposes restrictions on both the rate r and the form of the rate law
                           representing it. Thus, at given (T, P),  for a system reacting spontaneously (but not at
                           equilibrium),
                                                      AG,,,  <  0 and r >  0                   (5.3-5)

                           At equilibrium,

                                                     A%,   =  0 and  r = 0                     (5.3-6)

                           The third possibility of r < 0 cannot arise, since AG,,, cannot be positive for sponta-
                           neous change.
                             Equation 5.3-6 leads to a necessary relation between  (Y~  and  aj  in equation 5.3-4. From
                           this latter equation, at equilibrium,


                                                         kf(T)   fI4~
                                                                 i = l
                                                         -=-                                   (5.3-7)
                                                         k,(T)
                                                                 fi c;:,
                                                                 i = l
                            Also, at equilibrium, the equilibrium constant is


                                                                                               (5.3-8)


                            Since kf/k, and Kc,eq are both functions of  T only, they are functionally related (Den-
                            bigh, 1981, p. 444):
                                                         k, (0                                 (5.3-9)
                                                         - = w&q)
                                                         4 m


                            or



                                                                                              (5.3-10)


                                                       i=l
                            It follows necessarily (Blum and Luus, 1964; Aris, 1968) that  4  is such that



                                                                                             (5.3-11)

                                                  $$ =  (Kc,eJ  (n   ’  0)
                                                   r
                             where
                                                      II  = (a; - cqyvi;  i = 1,2,.  .  .    (5.3-12)
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