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13.8 CONCLUDING REMARKS          305




               of about 0.13, and this is equivalent to about 13,000 ppm (parts per million [by mass]): this level is
               typical of that which would be achieved at equilibrium conditions in an engine.
                  Before considering the effect of the rate of reactions on the actual levels of NO achieved, it is
               worthwhile seeing the effect of fuel on the level of exhaust constituents. The additional reactions do
               not have a major effect on the exhaust composition with octane as a fuel, and the CO 2 level is still
               significantly higher than with methane, as would be expected. However, the general level of NO is
               higher with octane than methane because of the slightly higher temperatures achieved with this fuel,
               and the larger proportion of CO 2 which can be ‘robbed’ for oxygen. The maximum levels of NO again
               occur around f ¼ 0.7 to 0.8, and result in about 14,000 ppm.
                  The levels of NO in the exhaust gas of an engine are significantly lower than those calculated above
               for a number of reasons. First, the reactions occurring in the cylinder are not instantaneous, but are
               restricted by the rate at which reacting molecules meet: this is known as chemical kinetics or rate
               kinetics, and is the subject of Chapter 14. The effect of these kinetics is that the instantaneous level of
               NO in the cylinder does not achieve the equilibrium level, and lags it when it is increasing as shown in
               Fig. 14.1. When the equilibrium concentration is decreasing the actual level of NO still cannot
               maintain pace with it, and again lags the level while it decreases down the expansion stroke of the
               engine, as shown qualitatively in Fig. 14.1; in fact these reactions tend to ‘freeze’ at around 2000 K,
               and this level then dominates the exhaust value. Second, the combustion process does not take place
               instantaneously at tdc as shown here, but is spread over a significant period of the cycle and the
               pressures and temperatures are lower than those attained in the ‘Otto’ cycle: this will reduce the peak
               equilibrium level of NO.
                  It is shown on Figs 13.10 and 13.11 that the peak level of NO at equilibrium occurs at around
               f ¼ 0.7–0.8, but experience shows that the maximum values of NO in engine exhaust systems (around
               2000–5000 ppm) occur at about f ¼ 0.9. This can be explained by considering the effect of rate
               kinetics. It will be shown in Chapter 14 that the rate at which a reaction occurs is exponentially related
               to temperature. Hence, while the equilibrium level of NO is maximum at f ¼ 0.7–0.8 the lower
               temperature at this equivalence ratio limits the amount of NO produced by the reaction. The peak value
               of NO occurs at f ¼ 0.9 because the driving force (the equilibrium concentration) and the rate of
               reaction combine at this equivalence ratio to maximise production of this pollutant.

               13.8 CONCLUDING REMARKS
               This chapter has laid the foundation for considering the production of emissions from combustion
               systems. It delivers essential information for the evaluation of rate kinetics, which is considered in
               Chapter 14.
                  The chapter has shown that the composition of typical gas mixtures found in engines at tdc is very
               dependent on the fuel, equivalence ratio, the temperature and pressure achieved during the process.
               The early sections, which neglect NO x , show how the proportions of CO, CO 2 ,H 2 O and H 2 vary with
               equivalence ratio, and the particular carbon/hydrogen ratio of the fuel used. The effect of dissociation
               on the peak temperatures and pressures achieved is also discussed.
                  The final section considered the dissociation processes that produced NO, and showed that the
               maximum equilibrium concentration of NO was found at relatively weak mixtures, when there was an
               abundance of ‘free’ oxygen.
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