In this paper, we extend the study of instabilities in flows driven by the
radiation pressure of an ionizing continuum to flows that are not plane par
allel. It is well known that the plane-parallel instability leads eventuall
y to the formation of continuum-driven shocks backed by a sonic transition.
If these structures are thin, we find that they are unstable to a corrugat
ion mode, and evolve to form sharp-peaked triangular profiles. Once this ha
s occurred, the thin-shock approximation is no longer valid.
We study the further development of the shocks by numerical hydrodynamic si
mulations. The flow tends to break up into numerous discrete bow-shaped com
ponents. The speed of these components through the upstream material is alm
ost constant. As a result, the maximal velocity of radiatively driven shock
s through the upstream gas may be determined by instabilities rather than b
y other physical effects. Interactions between gas in the wings of neighbou
ring bowshocks can, however, form subsequent generations of bowshocks that
are faster and more acute than their predecessors.
One likely location where continuum-driven shocks may occur is in the broad
-line regions of active nuclei. We discuss the application of our results t
o such flows.