Linear stability of two-dimensional flows in a frame rotating with ang
ular velocity vector Omega=Omega e(z) perpendicular to their plane is
considered. Sufficient conditions for instability have been derived fo
r simple inviscid flows, namely parallel shear flows (characterized by
the ''Pedley'' or ''Bradshaw-Richardson'' number), circular vortices
(by the ''generalized Rayleigh'' discriminant) and unbounded flows hav
ing a quadratic streamfunction (with elliptical, rectilinear or hyperb
olic streamlines). These exact criteria are reviewed and contrasted us
ing stability analysis for both three-dimensional disturbances and ove
rsimplified ''pressureless'' versions of the linear theory. These sugg
est that one defines a general inviscid criterion for rotation and cur
vature, based on the sign of the second invariant of the ''inertial te
nsor,'' and stating that, in a Cartesian coordinate frame: a sufficien
t condition for instability is that Phi(x,y)=-1/2S:S+1/4W(t).W-t<0 som
ewhere in the flow domain. It involves the ''tilting vorticity'' W-t=W
+4 Ohm[Cambon et al., J. Fluid Mech. 278, 175 (1994)] and the symmetri
c part S of the velocity gradient of the basic flow. (C) 1997 American
Institute of Physics.