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10.3 HEATS OF FORMATION AND HEATS OF REACTION             213




               10.2.3 COMBUSTION WITH RICH MIXTURES
               A rich mixture occurs when the quantity of air available is less than the stoichiometric quantity;
               this means that there is not sufficient air to burn the fuel. In this simplified approach it is assumed
               that the hydrogen combines preferentially with the oxygen and the carbon does not have sufficient
               oxygen to be completely burned to carbon dioxide: this results in partial oxidation of part of the
               carbon to carbon monoxide. It will be shown in Chapter 12 that the equilibrium equations, which
               control the way in which the hydrocarbon fuel oxidizes, govern the proportions of oxygen taken by
               the carbon and hydrogen of the fuel and that the approximation of preferential combination of
               oxygen and hydrogen is a reasonable one. In this case, to define a rich mixture, f is greater than
               unity. Then

                            2                 4   3f              4ðf   1Þ     7:52
                              O 2 þ 3:76N 2 /                                      N 2 :    (10.7)
                     CH 4 þ                          CO 2 þ 2H 2 O þ      CO
                            f                   f                    f          f
                  If the equivalence ratio is 1.2, then Eqn (10.7) is
                          CH 4 þ 1:667ðO 2 þ 3:76N 2 Þ/0:333CO 2 þ 2H 2 O þ 0:667CO   6:267N 2 :  (10.8)

                  It is quite obvious that operating the combustion on rich mixtures results in the production of
               carbon monoxide (CO), an extremely toxic gas. For this reason it is now not acceptable to operate
               combustion systems with rich mixtures. Note that Eqn (10.7) cannot be used with values of f > 4/3,
               otherwise the amount of CO 2 becomes negative. At this stage it must be assumed that the carbon is
               converted to carbon monoxide and carbon. The resulting equation is

                                2                        4               4      7:52
                                                                                    N 2 :   (10.9)
                          CH 4 þ  O 2 þ 3:76N 2 /2H 2 O þ    2 CO þ 3       C þ
                                f                        f               f       f
                  Equation (10.9) is a very hypothetical one because during combustion extensive dissociation oc-
               curs and this liberates oxygen by breaking down the water molecules: this oxygen is then available to
               create carbon monoxide and carbon dioxide rather than carbon molecules.
                  In reality it is also possible to produce pollutants even when the mixture is weaker than stoi-
               chiometric simply due to poor mixing of fuel and air, quenching of flames on cold cylinder or boiler
               walls, trapping of mixture in crevices (fluid mechanics effects) and also due to thermodynamic lim-
               itations in the process.

               10.3 HEATS OF FORMATION AND HEATS OF REACTION
               Combustion of fuels takes place either in a closed system or an open system. The relevant property of
               the fuel to be considered is the internal energy or enthalpy, respectively, of formation or reaction. In a
               naive manner it is often considered that combustion is a process of energy addition to the system. This
               is not true because the energy released during a combustion process is already contained in the re-
               actants, in the form of the chemical energy of the fuel (see Chapter 11). Hence it is possible to talk of
               adiabatic combustion as a process in which no energy (heat) is transferred to, or from, the system – the
               temperature of the system increases because of a rearrangement of the chemical bonds in the fuel and
               oxidant.
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