The dynamics of time-dependent, planar propagation of gaseous detonations i
s addressed on the basis of a three-step chemistry model that describes bra
nched-chain processes. Relevant nondimensional parameters are the ratio of
the heat release to the thermal enthalpy at the Neumann state, the nondimen
sional activation energies for the initiation and branching steps, the rati
o of the branching time to the initiation time and the ratio of the branchi
ng time to the recombination time. The limit of strong overdrive is conside
red, in which pressure remains constant downstream from the leading shock i
n the first approximation, and the ratio of specific heats gamma is taken t
o be near unity. A two-term expansion in the strong overdrive factor is int
roduced, and an integral equation is derived describing the nonlinear dynam
ics and exhibiting a bifurcation parameter, the reciprocal of the product o
f (gamma -1), the nondimensional heat release and the nondimensional branch
ing activation energy, with an acoustic correction. A stability analysis sh
ows that, depending on values of the parameters, either the mode of lowest
frequency or a mode of higher frequency may be most unstable. Numerical int
egrations exhibit different conditions under which oscillations die, low-fr
equency oscillations prevail, high-frequency oscillations prevail, highly n
onlinear oscillations persist, or detonation failure occurs. This type of p
arametric analysis is feasible because of the relative simplicity of the mo
del, which still is more realistic than a one-step, Arrhenius chemical appr
oximation. In particular, by addressing the limit of slow radical recombina
tion compared with branching, explicit results are derived for the critical
value of the bifurcation parameter, involving the ratio of the recombinati
on time to the induction time. The results help to clarify the general natu
re of one-dimensional detonation instability and provide simplifications th
at can be employed in efficiently relating gaseous detonation behavior to t
he true underlying chemistry. (C) 2001 American Institute of Physics.