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258    CHAPTER 12 CHEMICAL EQUILIBRIUM AND DISSOCIATION




                        0
                Now DG is a function of T alone (having been defined at a standard pressure, p 0 ), therefore
                        T
                 ¼ fðTÞ.
             K p r
                                                              is related to the datum pressure used to
                Equation (12.56) shows that the numerical value of K p r
                    0
             define m . If the amounts of substance of reactants and products are the same then the value of K p is not
             affected by the datum pressure (because y a þ y b   y c   y d ¼ 0). However, if the amounts of substance
                                                                  1
             of products and reactants are not equal, as is the case for the CO þ O 2 /CO 2 reaction, then the value
                                                                  2
             of K p will be dependent on the units of pressure. Hence the value of equilibrium constant, K p , is the
             same for the water gas reaction ðCO þ H 2 O/CO 2 þ H 2 Þ in both SI and imperial units because K p is
             dimensionless in this case.
             12.5.1 K p DEFINED IN TERMS OF MOLE FRACTION
             The definition of partial pressure is
                                                  p a ¼ x a p                            (12.60)

                Hence replacing the terms for partial pressure in Eqn (12.57) by the definition in Eqn (12.60) gives:
                                       (     )      "        !           #
                                        p p y d         x x y d
                                                         y c
                                         y c
                                                         c
                                                           d
                                         c
                                            d
                                  <T ln        ¼<T ln         p ðy c þy d  y a  y b Þ    (12.61)
                                         y a y b
                                        p a p           x a x
                                                         y a y b
                                            b              b
             which results in the following expression for K p in terms of mole fraction
                                                     !
                                                 x x y d
                                                  y c
                                                  c
                                                    d
                                          K p ¼   y a y b  p ðy c þy d  y a  y b Þ       (12.62)
                                                 x a x
                                                    b
                The above expressions are known as the law of mass action.
             12.6 VARIATION OF GIBBS ENERGY WITH COMPOSITION
             Equations (12.57) and (12.62) show that the equilibrium composition of a mixture is defined by the
             equilibrium constant that can be defined in terms of the partial pressures or mole fractions of the
             constituents of the mixture: the equilibrium constant was evaluated by equating the change of Gibbs
                                                                 ¼ 0. It is instructive to examine how
             energy at constant pressure and temperature to zero, i.e. dGÞ p;T
             the Gibbs energy of a mixture varies with composition at constant temperature and pressure. Assume
             that two components of a mixture, A and B, can combine chemically to produce compound C. This is a
             slightly simplified form of Eqns (12.38) and (12.39). If the chemical equation is
                                                 A þ B/2C;                               (12.63)
             then at some point in the reaction, defined by the fraction of reaction, ε, the chemical composition is
                                           ð1   εÞA þð1   εÞB þ 2εC                      (12.64)

             and the Gibbs energy is
                                        G ¼ð1   εÞm þð1   εÞm þ 2εm c                    (12.65)
                                                             b
                                                   a
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