We present the final part of the laminar flame theory based on the not
ion of the minimum entropy production in weakly nonequilibrium systems
. A correction has been made to the Zel'dovich-Frank Kamenetskii-Landa
u formula for the laminar flame velocity at large Lewis numbers. If th
e flame velocity calculated in this work corresponds to the stable reg
ime of front propagation, the problem under consideration is analogous
to the Kolmogorov-Petrovskii-Piskunov problem. With sufficiently high
reaction orders, the width of a thermally diffusive boundary layer in
creases by a logarithmic law.