Abstract
It is proposed that the multiple eigenvalue nature of the steady state flame equation corresponds to a flame problem in which flammability limits arise as a fundamental aspect of a one-dimensional adiabatic flame. This is in contrast to previous descriptions of flammability limits which ascribe the failure of flames to propagate under certain circumstances to natural convection or to heat losses. It is shown how it is possible for flame velocities to fall to zero for finite adiabatic flame temperatures by a variation of kinetic parameters in the ABC flame.
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