Page 66 - Chemical equilibria Volume 4
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42     Chemical Equilibria
                             The  number  of independent components is the  difference between the
                           number  of components in the system and the  number  of independent
                           transformations – i.e. the dimension of the vector space of the balance equations.
                           This number must be decreased by 1 in the case of the presence of ions, due to
                           the electrical neutrality condition, and decreased by 1 in the case of the species
                           belonging to a solid  phase if the condition  of conservation  of the
                           crystallographic sites is imposed.

                             Remember that the variance is the number of free variables in the system,
                           among the p external intensive physical variables and the molar fractions.
                           This number gives us the  maximum number of degrees of freedom of the
                           system; that maximum number of degrees of freedoms may be reduced by
                           the imposition of specific constraints. Gibbs’ phase rule applies equally to
                           open systems and closed systems, and pertains solely to the intensive
                           variables.



                           2.3.2. Duhem’s phase rule in closed systems

                             Duhem’s phase rule enables us to define a Duhem variance, which
                           applies only to closed  systems and pertains to the external intensive
                           variables, the composition variables and the quantities of matter. The goal is
                           always to determine the number of free variables.

                           2.3.2.1. Closure conditions
                             As before, we suppose that the system contains N components in φ phases
                           and is home to  R  independent transformations. The variation, over an
                           arbitrary length of time, of the quantity  n  of one of the components k in a
                                                                k
                           phase in the system will be given as a function of the reactional extents  ξ ρ

                           of the different transformations by:

                                   k ∑
                                 dn =  R  ν  dξ ρ                                        [2.40]
                                      ρ= 1  k ρ
                             By  integrating between the initial time, when  n = n , and  ξ =  0, we
                                                                              0
                                                                                      ρ
                                                                          k
                                                                              k
                           find:
                                      k ∑
                                 n =  n +  R  νξ ρ                                       [2.41]
                                      0
                                  k
                                         ρ= 1  k ρ
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