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46     Chapter 3  Chemical Equilibrium  in Aqueous  Solutions


                                       This differentiation yields
                                                                     N,SO         N,,"
                                                          A,S"(iso)  =   riA,SP - R   rilnri          (3.5- 16)
                                                                    i=  1         i=  1
                                       The same form of equation can be used to calculate the standard molar entropy
                                       S:(iso)   of the isomer group. The entropy of formation of the isomer group is equal
                                       to the mole-fraction-weighted entropy of formation plus the entropy of mixing the
                                       isomers.
                                           The equation for the standard molar heat capacity of formation of an isomer
                                       group can be obtained  by  using

                                                                           i3Af H"(iso)
                                                              A,C;(iso)  = -                          (3.5- 17)

                                       This differentiation yields

                                                         N,\O
                                               C;,(iso)   = 1 riC;,(i)  + RT~ (T rL(AfIQ2 - (AfHo(iso))')  (3.5-18)
                                                                           i=l
                                                                      ~
                                                         i=  1
                                       Equation (3.5-18) has been written in terms of molar heat capacities C&i),  rather
                                       than heat capacities of formation, because  the heat capacities of  the elements are
                                       on  both  sides  and  cancel.  The  second  term  of  this  equation  is  always  posi-
                                       tive  because  the  weighted  average  of  the  squares  is  always  greater  than  the
                                       square of  the average. Equation  3.5-18 is in accord  with  LeChatelier's principle:
                                       As  the  temperature  is  raised,  the  equilibrium  shifts  in  the  direction  that
                                       causes  the  absorption  of  heat.  Equation  3.5-18  can  also  be  derived  using
                                        C,  = - T(d2G/dT2), (equation  2.5-25).
                                           Equations  3.5-14  and  3.5-16  can  be  substituted  in  A,G"(iso)  =
                                       A,H"(iso)  - TA,S"(iso) to obtain another form for the standard Gibbs energy of
                                       formation  of  an isomer group.

                                                                    NiSO           N,,,
                                                          A,G"(iso) = c riAfGP + RT   rilnri          (3.5-1 9)
                                                                    i=  1          i=  1
                                        In other words,  the standard  Gibbs energy of  formation  of  an isomer  group at
                                        equilibrium  is  equal  to  the  mole  fraction-weighted  average  of  standard  Gibbs
                                        energies of formation  of  the isomers plus the Gibbs energy of  mixing.
                                           The fundamental equation for G of a system made up of isomer groups is
                                                                             Niso
                                                        dG = -SdT  + VdP + c pi(iso)dni(iso)           (3.5-20)
                                                                             i= 1
                                        where Niso is the number of isomer groups. In this equation an isomer group may
                                        consist  of  a  single species. This equation  can be  used  to derive  the  equilibrium
                                        expressions for reactions written  in terms  of  isomer  groups. Since isomer groups
                                        can be treated like species in chemical thermodynamics, they can be referred to a
                                        pseudospecies.  Equation 3.5-20 is based  on the assumption that the species in an
                                        isomer group are in equilibrium with each other. The number of  natural variables
                                        for a one-phase system consisting  of  Niso isomer groups is D  = Niso + 2 prior  to
                                        application  of  the constraints  due to reactions between  the isomer groups. If  the
                                        reactions  between  the isomer  groups  are at equilibrium,  the  number  of  compo-
                                        nents replaces the number  of  isomer groups and D  = C + 2.


                                           3.6  EFFECT OF IONIC STRENGTH ON EQUILIBRIA
                                                IN SOLUTION REACTIONS


                                        The activity  coefficient yi  of  an ion  depends  on the ionic  strength  (I = ($z:ci,
                                        where zi is the charge number) according to the Debye-Huckel theory in the limit
                                        of  low ionic strengths. As  discussed in Section  1.2, this equation can be extended
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