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314    CHAPTER 14 CHEMICAL KINETICS





                But
                                        k f1 ½NŠ ½NOŠ ¼ k b1 ½N 2 Š ½OŠ ¼ R 1 ;
                                                              e
                                             e
                                                 e
                                                           e
             so the net rate for Eqn (14.19) becomes  abR 1 þ R 1 .
                Using a similar procedure for Eqns (14.20), (14.21) and (14.24) involving NO gives the following
             expression, which allows for the change in volume over a time step,
                     1 d
                         ð½NOŠVÞ ¼ aðbR 1 þ R 2 þ R 3 þ 2aR 6 Þ þ R 1 þ bðR 2 þ R 3 Þ þ 2gR 6 :  (14.26)
                     V dt
             where V is the volume of the products zone.

             14.4.1.2 Expression for Atomic Nitrogen, N
             Equations (14.19)–(14.21), which all involve N, give
                               1 d
                                   ð½NŠVÞ¼ bðaR 1 þ R 2 þ R 3 Þþ R 1 þ aðR 2 þ R 3 Þ:    (14.27)
                               V dt


             14.4.1.3 Expression for Nitrous Oxide N 2 O
             Equations (14.22)–(14.25) all involve N 2 O and can be combined to give
                          1 d                                             2
                              ð½N 2 OŠVÞ¼  gðR 4 þ R 5 þ R 6 þ R 7 Þþ R 4 þ R 5 þ a R 6 þ R 7 :  (14.28)
                          V dt
                A finite time is required for the reactions to reach their equilibrium values; this is called the
             relaxation time. It has been found (Lavoie et al. (1970)) that the relaxation times of reactions (14.27)
             and (14.28) are several orders of magnitude shorter than those of reaction (14.26), and hence it can be
             assumed that the [N] and [N 2 O] values are at steady state, which means that the right-hand sides of
             Eqns (14.27) and (14.28) are zero. Then, from Eqn (14.27)

                                                R 1 þ aðR 2 þ R 3 Þ
                                            b ¼                ;                         (14.29)
                                                ðaR 1 þ R 2 þ R 3 Þ
             and, from Eqn (14.28)

                                                         2
                                              R 4 þ R 5 þ a R 6 þ R 7
                                           g ¼                   :                       (14.30)
                                               ðR 4 þ R 5 þ R 6 þ R 7 Þ
                These values can be substituted into Eqn (14.26) to give
                   1 d                 2         R 1                   R 6
                       ð½NOŠVÞ¼ 2 1   a                    þ                             (14.31)
                   V dt                   1 þ a½R 1 =ðR 2 þ R 3 ފ  1 þ½R 6 =ðR 4 þ R 5 þ R 7 ފ
                This is the rate equation for NO that is solved in computer programs to evaluate the level of NO in
             the products of combustion. It should be noted that the variation in the molar concentration is a first-
             order differential equation in time and relates the rate of change of [NO] to the instantaneous ratio of
             the actual concentration of NO to the equilibrium value (i.e. a). When the actual level of [NO] is at the
             equilibrium level then a ¼ 1 and the rate of change of [NO] ¼ 0.
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