The thermal boundary layer induced within a horizontal semi-infinite layer
of Boussinesq fluid by a sinusoidally heated bounding plate is known to be
susceptible to vortex instability. The structure of shea wavelength convect
ion is considered here and the analysis taken from linear, through weakly n
onlinear and onto the fully nonlinear stage. At this point the activity is
sufficiently strong that it induces large changes in the underlying thermal
profile and the overall how characteristics are determined by the solution
of a free boundary-value problem. This solution demonstrates that the high
ly nonlinear vortices tend to settle into a periodic form in which interval
s of intense activity alternate with times of relative quiescence.