The nonlinear interaction equations describing vortex-Rayleigh wave in
teractions in highly curved boundary layers are derived. These equatio
ns describe a strongly nonlinear interaction between an inviscid wave
system and a streamwise vortex. The coupling between the two structure
s is quite different from that found by Hall and Smith [13] in the abs
ence of wall curvature. Here the vortex is forced over a finite region
of the flow rather than in the critical layer associated with the wav
e system. When the interaction takes place the wave system remains loc
ally neutral as it moves downstream and its self interaction drives a
vortex field of the same magnitude as that driven by the wall curvatur
e. This modification of the mean state then alters the wave properties
and forces the wave amplitude to adjust itself in order that the wave
frequency is constant. Solutions of the interaction equations are fou
nd for the initial stages of the interaction in the case when the wave
amplitude is initially small. Our analysis suggests that finite ampli
tude disturbances can only exist when the vortex field is nonzero at t
he initial position where the interaction is stimulated.