The long-time behavior of a reaction-diffusion front between one static (e.
g. porous solid) reactant A and one initially separated diffusing reactant
B is analyzed for the mean-field reaction-rate density R(rho (A), rho (B))
= k rho (m)(A)rho (n)(B). A uniformly valid asymptotic approximation is con
structed from matched self-similar solutions in a "reaction front" (of widt
h w similar to t(alpha), where R similar to t(beta) enters the dominant bal
ance) and a "diffusion layer" (of width W similar to t(1/2), where R is neg
ligible). The limiting solution exists if and only if m, n greater than or
equal to 1, in which case the scaling exponents are uniquely given by alpha
= (m - 1)/2(m + 1) and beta = m/(m + 1). In the diffusion layer, the commo
n ad hoc approximation of neglecting reactions is given mathematical justif
ication, and the exact transient decay of the reaction rate is derived. The
physical effects of higher-order kinetics (m, n > 1), such as the broadeni
ng of the reaction front and the slowing of transients, are also discussed.
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