The generation of shear flow driven by a large amplitude drift wave, r
epresented by the Hasegawa-Mima-Charney (HMC) equation, has been inves
tigated. It is shown that, besides a finite amplitude threshold for th
e shear flow instability to occur, there is also a necessary condition
on the aspect ratio of the large amplitude drift wave, due to conserv
ation of the average potential vorticity, that needs to be satisfied.
A comprehensive comparison of the shear-flow instability criterion for
the HMC equation and the incompressible, invisicid, hydrodynamic equa
tion has been undertaken. (C) 1995 American Institute of Physics.