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3.3 Chemical Kinetics and Chemical Equilibrium                  79

              This approximation allows us to determine the concentration of A*

                                            k f 1 A½Š M½Š

                                      A ½  Š ¼                           ð3:43Þ
                                           k b1 M½Š   k 2
                          *
              Substituting [A ] into Eq. (3.39) leads to

                                     dA½Š  k f 1 k 2 A½Š M½Š
                                         ¼                               ð3:44Þ
                                      dt   k b1 M½Š   k 2
                                                                     k
              Now, the rate of reaction constant k for the overall reaction A ! B þ C is
            determined by


                                       dA½Š
                                            ¼ k½AŠ
                                        dt
              And it gives the overall reaction rate constant as,

                                           k f 1 k 2 M½Š
                                      k ¼                                ð3:45Þ
                                          k 2   k b1 M
                                                 ½Š


            3.4 Thermodynamics of Combustion System

            Temperatures are assumed known in the preceding analyses. In case the tempera-
            ture of the combustion product mixture is unknown yet, it has to be determined
            from the combination of chemical equilibrium and thermodynamics. Related topics
            are briefly reviewed as follows for the readers without related training background.



            3.4.1 First Law of Thermodynamics


            The first law of thermodynamics is about the conservation of energy; the total
            energy of the thermodynamic system and its surrounding environment is conserved.
            Physically, the first law states that, for a closed system, the change in the internal
            energy is equal to the sum of the amount of heat energy supplied to the system and
            the work done by the system on the surroundings. The first law of a combustion
            system is mathematically described as

                                       DU ¼ Q   W                        ð3:46Þ
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