Page 117 - Chemical equilibria Volume 4
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Molecular Chemical Equilibria     93
                           A 2A 1, then the system evolves as the reaction progresses, in accordance with
                           very specific compositions set by the initial conditions and the
                           stoichiometric numbers β 1, β 2 and β 3. The curve, passing through a specific
                           point M and giving all the compositions of the system during the reaction, is
                           called the iso-composition curve.
                             At a given pressure and temperature, the iso-composition corresponding
                           to the chosen initial state intersects the iso-Q curve at point E representing
                           the state of thermodynamic equilibrium  at the chosen temperature and
                           pressure and for the chosen initial composition.

                             We shall quantify those data by  establishing the iso-Q and iso-
                           composition curves in the case of perfect solutions. First, though, we shall
                           demonstrate an important property of equilibria with perfect solutions.


                           3.5.2. Molar fractions at equilibrium and initial composition

                             We consider equilibria which involve a poly-component perfect phase,
                           and demonstrate the following theorem:

                           THEOREM 3.1– In such equilibria, the molar fraction of a formed component
                           is, at thermodynamic equilibrium,  maximal when that equilibrium is
                           achieved on the basis of the reagents taken in stoichiometric proportions.

                             This theorem is very general, as long as several components belong to the
                           same phase. We shall now demonstrate it in the case of the three-component
                           reactions given by balance equation [3R.26].

                             Hence, we consider the initial mixture of a mole and containing u moles
                           of A 1 and 1–u moles of A 2. Let z denote the number of moles of A 3 formed.
                           We can see that the quantities of the different components are given by:

                                 n =−   z                                                [3.81]
                                    u
                                 1
                                           β
                                    1 u −
                                 n =−       2  z                                         [3.82]
                                  2
                                           β 1
                                     β
                                 n =  3  z                                               [3.83]
                                     β 1
                                  3
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