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326    CHAPTER 15 COMBUSTION AND FLAMES




             15.2.2 PROCESSES OCCURRING IN COMBUSTION
             The thermodynamics of combustion generally relate to the gas in isolation from its surroundings.
             However, the surroundings, and the interaction of the gas with the walls of a container, etc. can have a
             major effect on the combustion process. The mechanisms by which the combusting gas interacts with
             its container are

             1. transport of gaseous reactant to the surface – diffusion;
             2. adsorption of gas molecules on surface;
             3. reaction of adsorbed molecules with the surface;
             4. desorption of gas molecules from the surface;
             5. transport of products from the surface back into the gas stream – diffusion.
                These effects might occur in a simple container, say an engine cylinder, or in a catalytic converter.
             In the first case the interaction might stop the reaction, while in the second one it might enhance the
             reactions.

             15.3 EXPLOSION LIMITS
             The kinetics of reactions was introduced previously, and it was stated that reactions would, in general,
             only occur when the atoms or ions of two constituents collided. The reaction rates were derived from
             this approach, and the Arrhenius equations (see Section 14.3) were introduced. The tendency for a
             mixture to spontaneously explode is affected by the conditions in which it is stored. A mixture of

             hydrogen and oxygen at 1 bar, and 500 C will remain in a metastable state, and will only explode if
             ignited. However, if the pressure of that mixture is reduced to around 10 mm Hg (about 0.01 bar) there
             will be a spontaneous explosion. Likewise, if the pressure was increased to about 2 bar there would
             also be an explosion. It is interesting to examine the mechanisms which make the mixture become
             hypergolic. The variation of explosion limits with state for the hydrogen–oxygen mixture is shown in
             Fig. 15.2.

                            10000


                                            Third limit
                             1000
                           Pressure / (mm Hg)  100  Second limit  No explosion





                              10
                                                          Explosion
                                                 First limit

                              1
                               390  410  430  450  470  490  510  530  550  570  590
                                                   Temperature / ( C)
             FIGURE 15.2
             Explosion limits for a mixture of hydrogen and oxygen (from Lewis and von Elbe (1961)).
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