Using the combined limits of a large activation energy and a ratio of
specific heats close to unity, a dispersion relation has recently been
derived which governs the stability of a steady Chapman-Jouguet deton
ation wave to two-dimensional linear disturbances. The analysis consid
ers instability evolution time scales that are long on the time scale
of fluid particle passage through the main reaction layer. In the foll
owing, a simplified polynomial form of the dispersion relation is deri
ved under an appropriate choice of a distinguished limit between an in
stability evolution time scale that is long on the time scale of parti
cle passage through the induction zone and a transverse disturbance wa
velength that is long compared to the hydrodynamic thickness of the in
duction zone. A third order in time, sixth order in space, parabolic l
inear evolution equation is derived which governs the initial dynamics
of cellular detonation formation. The linear dispersion relation is s
hown to have the properties of a most unstable wavenumber, leading to
a theoretical prediction of the initial detonation cell spacing and a
wavenumber above which all disturbances decay, eliminating the growth
of small-wavelength perturbations. The role played by the curvature of
the detonation front in the dynamics of the cellular instability is a
lso highlighted.