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T (°C)
                                  1400                               Molecular Chemical Equilibria     89


                                  1000


                                   600



                                   200

                                                                                   x CO
                                      0       0.2     0.4     0.6      0.8     1

                                 Figure 3.13. Boudouard diagram for a total pressure of 1 atmosphere


                             Figure 3.13 shows the binary diagram of that reaction for a total pressure of
                           1 bar. If the carbon is not of pure phase – e.g. if we have the same equilibrium in
                           the presence of steel (solution of carbon in iron) – then relation [3.68] is replaced
                           by:

                                      (I)
                                  2
                                 P CO  / aP CO  2  =  K P                                [3.69]
                                      C
                             This formula involves the carbon activity in convention (I). Therefore,
                           the diagram in Figure 3.13 will be plotted, with the total pressure and carbon
                           activity being constant.


                           3.5. Ternary diagrams of chemical equilibria

                             The purpose of the ternary diagram is to enable us to quickly read the
                           composition at equilibrium at a certain temperature and a certain pressure,
                           knowing the initial conditions, for reactions involving a single phase with
                           three components (mixture of three  gases or condensed solution with
                           components). As the reaction may also involve pure phases – e.g. solids –
                           we shall write it very generally  with its three components in the
                           polycomponent phase A 1, A 2 and A 3, in the form:

                                solids + β 1A 1 +   β 2A 2 = β 3A 3 + solids            [3R.26]
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