We consider a flame in a stoichiometric combustible mixture of two rea
ctants, A and B, having different diffusivities. We employ a thin reac
tion zone approximation and assume that the reaction ceases when the c
oncentrations and temperature approach their thermodynamic equilibrium
values. Thus, our analysis accounts for the possibility of a reversib
le stage in the combustion reactions. We find uniform flames and analy
ze both their cellular and pulsating instabilities. We compare our res
ults with those for a one reactant flame as well as with previously ob
tained results for a stoichiometric mixture of two reactants. Studies
of the latter assumed complete consumption of one of the reactants in
the reaction front and that both Lewis numbers, L(A) and L(B), are clo
se to 1. They showed that the cellular stability boundary for bimolecu
lar reactions is determined by an effective Lewis number which is the
arithmetic mean of L(A) and L(B), i.e., 1/2(L(A) + L(B)). By consideri
ng the limiting case of a negligibly small equilibrium constant, so th
at the final concentrations of the reactants approach zero, we show th
at for general Lewis numbers, not limited to being close to 1, the cel
lular stability boundary is determined by an effective Lewis number wh
ich, for equimolecular, e.g., bimolecular reactions, is the harmonic m
ean of the Lewis numbers of the two reactants, i.e., L(eff) = 2(L(A)(-
1) + L(B)(-1))(-1). The leading term of an asymptotic expansion of our
effective Lewis number, for both L(A) and L(B) close to 1, is the sim
ple arithmetic mean, previously obtained. For significantly different
Lewis numbers, a case not covered by previous results, our solution sh
ows that stability is determined by diffusion of the lighter reactant,
in accord with experimental observations. Thus, we provide a theoreti
cal basis for the effect of preferential diffusion. We also find that
dissociation of the product is stabilizing.