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Coal and biomass cofiring: CFD modeling                             95

              From modeling point of view, different approaches exist for char reactions, e.g., as
           follows:
           •  One-film model: There is no flame in the gas phase. Char is directly oxidized into CO 2 at the
              particle surface. As a result, both the temperature and CO 2 peak at the particle surface and
              decay when moving away from the particle surface.
           •  Two-film model: The principal product at the char particle surface is CO. CO diffuses always
              from the particle surface and reacts with inward-diffusing O 2 ,CO þ 0.5O 2 / CO 2 , forming
              a visible flame at a distance away from the surface.
           •  Continuous-film model: A flame zone is distributed within the boundary layer around the
              char particle, rather than occurring in one or two sheets.
              The one-film model is most widely used for char reactions in solid fuel combustion
           CFD, in which different char surface reaction regimes can be identified: kinetics-
           controlled (zone I), diffusion- and kinetics-controlled (zone II), and diffusion-
           controlled (zone III).




           4.3.5  Homogeneous reactions

           In coal and biomass cofiring, the combustion of the released volatiles plays a vital role
           in ignition, local stoichiometry, flame stability, and pollutant formation. Therefore,
           gas-phase reaction modeling is also important. The overwhelming majority of indus-
           trial combustion CFD relies on global combustion mechanisms. The commonly used
           global mechanisms include the two-step hydrocarbon oxidation mechanism by West-
           brook and Dryer (WD) (Westbrook and Dryer, 1981, 1984) and the four-step mecha-
           nism developed by Jones and Lindstedt (JL) (Jones and Lindstedt, 1988) for alkane
           hydrocarbons up to butane in mixtures with air in premixed and diffusion flames. Tak-
           ing CH 4 as an example, the WD two-step mechanism is

               CH 4 þ 1:5O 2 /CO þ 2H 2 O                                  (R5)

               CO þ 0:5O 2 4CO 2                                           (R6)

              And the JL four-step scheme reads

               CH 4 þ 0:5O 2 /CO þ 2H 2                                    (R7)

               CH 4 þ H 2 O/CO þ 3H 2                                      (R8)

               H 2 þ 0:5O 2 4H 2 O                                         (R9)

               CO þ H 2 O4CO 2 þ H 2                                      (R10)

           which includes two competing fuel breakdown reactions into CO and H 2 and two
           reversible reactions controlling the rate of reactions for CO and H 2 .
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