The linear stability of steady frontal zones is considered using the p
rimitive equations. The frontal zones chosen have uniform potential vo
rticity and form a sequence of ''snapshots'' of the deformation-induce
d front as it evolves toward frontal collapse. The stability for a giv
en along front wavelength is determined by integrating a numerical mod
el forward from an initial condition of the basic-state front plus whi
te noise. Two classes of instabilities emerge. In one class, the modes
are modified versions of familiar, synoptic-scale baroclinic waves. T
he other class consists of Kelvin-Helmholtz (KH) instabilities. These
modes have wavelengths of order 1 km and exist only when the cross-fro
ntal scale is of order 10 km or smaller. With e-folding times of a few
minutes, the growth of IM waves may limit the cross-frontal scale of
active, time-dependent frontal flows, although boundary layer processe
s are probably important, at least for surface fronts, before KH modes
appear. No other instabilities are found, contrary to the calculation
s of Moore and Peltier.