Stability of Rossby waves in the β-plane approximation

Abstract

Floquet theory is used to describe the unstable spectrum at large scales of the β-plane equation linearized about Rossby waves. Base flows consisting of one to three Rossby waves are considered analytically using continued fractions and the method of multiple scales, while base flows with more than three Rossby waves are studied numerically. It is demonstrated that the mechanism for instability changes from inflectional to triad resonance at an O(1) transition Rhines number, Rh= U/( βL 2), independent of the Reynolds number. For a single Rossby wave base flow, the critical Reynolds number Re c for instability is found in various limits. In the limits Rh→∞ and k→0, the classical value Re c = 2 is recovered. For Rh→0 and all orientations of the Rossby wave except zonal and meridional, the base flow is unstable for all Reynolds numbers; a zonal Rossby wave is stable, while a meridional Rossby wave has critical Reynolds number Re c = 2 . For more isotropic base flows consisting of many Rossby waves (up to 40), the most unstable mode is purely zonal for 2≤ Rh<∞ and is nearly zonal for Rh=1/2, where the transition Rhines number is again O(1), independent of the Reynolds number and consistent with a change in the mechanism for instability from inflectional to triad resonance.