Evolution of weakly nonlinear and slowly varying Rossby waves in planetary
atmospheres and oceans is considered within the quasi-geostrophic equation on
unbounded domains. When the mean flow profile has a jump in the ambient
potential vorticity, localized eigenmodes are trapped by the mean flow with a
non-resonant speed of propagation. We address amplitude equations for these
modes. Whereas the linear problem is suggestive of a two-dimensional
Zakharov-Kuznetsov equation, we found that the dynamics of Rossby waves is
effectively linear and moreover confined to zonal waveguides of the mean flow.
This eliminates even the ubiquitous Korteweg-de Vries equations as underlying
models for spatially localized coherent structures in these geophysical flows