Instability of a shallow-water potential-vorticity front
David Gerard Dritschel, Jacques Vanneste
Abstract
David Gerard Dritschel, Jacques Vanneste
Abstract
A straight front separating two semi-infinite regions of uniform potential vorticity (PV) in a rotating shallow-water fluid gives rise to a localized fluid jet and a geostrophically balanced shelf in the free surface. The linear stability of this configuration, consisting of the simplest non-trivial PV distribution, has been studied previously, with ambiguous results. We revisit the problem and show that the flow is weakly unstable when the maximum Rossby number ${\textsfi R}\,{>}\,1$ . The instability is surprisingly weak, indeed exponentially so, scaling like $\exp[-4.3/({\textsfi R} - 1)]$ as ${\textsfi R}\,{\to}\,1$ . Even when ${\textsfi R}\,{=}\,\sqrt{2}$ (when the maximum Froude number ${\textsfi F}\,{=}\,1$ ), the maximum growth rate is only $7.76\,{\times}\,10^{-6}$ times the Coriolis frequency. Its existence nonetheless sheds light on the concept of ‘balance’ in geophysical flows, i.e. the degree to which the PV controls the dynamical evolution of these flows.
OpenAlex reports 27 citations for this work. Citation counts describe recorded attention and do not establish research quality.
A contribution statement is not available in the OpenAlex record.
Method details are not available in the OpenAlex metadata.
Findings are not separately available in the OpenAlex metadata.
Limitations are not available in the OpenAlex metadata.
Application details are not available in the OpenAlex metadata.
A straight front separating two semi-infinite regions of uniform potential vorticity (PV) in a rotating shallow-water fluid gives rise to a localized fluid jet and a geostrophically balanced shelf in the free surface. The linear stability of this configuration, consisting of the simplest non-trivial PV distribution, has been studied previously, with ambiguous results. We revisit the problem and show that the flow is weakly unstable when the maximum Rossby number ${\textsfi R}\,{>}\,1$ . The instability is surprisingly weak, indeed exponentially so, scaling like $\exp[-4.3/({\textsfi R} - 1)]$ as ${\textsfi R}\,{\to}\,1$ . Even when ${\textsfi R}\,{=}\,\sqrt{2}$ (when the maximum Froude number ${\textsfi F}\,{=}\,1$ ), the maximum growth rate is only $7.76\,{\times}\,10^{-6}$ times the Coriolis frequency. Its existence nonetheless sheds light on the concept of ‘balance’ in geophysical flows, i.e. the degree to which the PV controls the dynamical evolution of these flows.
Key concepts: Potential vorticity, Front (military), Instability, Vorticity, Positive vorticity advection, Mechanics, Waves and shallow water, Geology