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demonstrate that the slope of line PP’ (which is necessarily negative) gives
                           the temperature of inversion of the reaction:   Molecular Chemical Equilibria     73
                                CO 2 + H 2 = CO + H 2O                                   [3R.5]

                             This is the temperature for which, at equilibrium, we have the relation:

                                 P CO  =  P H 2 O                                        [3.46]
                                 P     P
                                  CO 2  H  2
                             Similarly, let us now compare the pole diagrams of reduction of two
                           metal oxides, MO and M’O by hydrogen, as follows:

                                MO + H 2 = M + H 2O                                      [3R.6]

                                M’O + H 2 = M’ + H 2O                                    [3R.7]

                             The straight line joining the two poles P and P’ of those two reactions at
                           the same temperature gives the equilibrium temperature of the reaction
                           between solids:

                                MO + M’  = M + OM’                                       [3R.8]



                           3.3. Representation of the evolution of an equilibrium with the
                           temperature

                             As temperature is an important variable of chemical equilibrium, users
                           have attempted to represent the evolution of a chemical  equilibrium  with
                           changing temperature. Two methods are discussed below.



                           3.3.1. Diagram in van ’t Hoff coordinates

                             The first mode of representation is based on relation [3.28], applied in
                           convention (I). The method involves representing, in standard pressure
                           conditions (in practice at the pressure of 1  bar), the logarithm of the
                           equilibrium  constant as  a function of the inverse of temperature. This
                           representation gives us  practically a straight line, because the standard
                                       0
                           enthalpy  Δ h and standard entropy  Δ s of the reaction are practically
                                                                 0
                                                               r
                                     r
                           independent  of the temperature. Hence, the  slope of that line  may be
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