We intend to close the gap between the numerical description of hydrocarbon flames using a large number of elementary reactions and the asymptotic description using very few reaction steps. To proceed in this direction we first reduce the hydrocarbon chemistry to the smallest number of steps that still provides a realistic flame structure. For the example of methane oxidation these are the four reaction steps
$$CH_4 + 2H + H_2 O = CO + 4H_2$$
(I)
$$CO + H_2 O = CO_2 + H_2$$
(II)
$$2H + M = H_2 + M$$
(III)
$$O_2 + 3H_2 = 2H + 2H_2 O$$
(IV)
Their rates are algebraicly complicated expressions that contain kinetic data from 9 elementary reactions. If standard values for these data are used, the flame velocity of a stoichiometric methane-air flame is calculated as 45.6 cm/sec . The reaction rates maybe simplified to include only data from the five most important reactions
$$\begin{gathered}CH_4 + H \to CH_3 + H_2 \hfill \\CH_4 + OH \to CH_3 + H_2 O \hfill \\CO + OH \rightleftarrows CO_2 + H \hfill \\O_2 + H + M \to HO_2 + M \hfill \\O_2 + H \rightleftarrows OH + O \hfill \\\end{gathered}$$
where the rate expression of the fourth of these reactions is modified. This model is proposed for the asymptotic analysis of the flame structure.
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