A theory of ignition is presented to analyse the effect of porosity on the
time to ignition of a semi-infinite porous energetic solid subjected to a c
onstant energy flux. An asymptotic perturbation analysis, based on the smal
lness of the gas-to-solid density ratio and the largeness of the activation
energy, is utilized to describe the inert and transition stages leading to
thermal runaway. As in the classical study of a nonporous solid, the trans
ition stage consists of three spatial regions in the limit of large activat
ion energy: a thin reactive-diffusive layer adjacent to the exposed surface
of the material where chemical effects are first felt, a somewhat thicker
transient-diffusive zone and, finally, an inert region where the temperatur
e field is still governed solely by conductive heat transfer. Solutions in
each region are constructed at each order with respect to the density-ratio
parameter and matched to one another using asymptotic matching principles.
It is found that the effects of porosity provide a leading-order reduction
in the time to ignition relative to that for the nonporous problem, arisin
g from the reduced amount of solid material that must be heated and the dif
ference in thermal conductivities of the solid and gaseous phases. A positi
ve correction to the leading-order ignition-delay time, however, is provide
d by the convective flow of gas out of the solid, which stems from the effe
cts of thermal expansion and removes energy from the system. The latter phe
nomenon is absent from the corresponding calculation for the nonporous prob
lem and produces a number of modifications at the next order in the analysi
s arising from the relative transport effects associated with the gas flow.