Mean zonal flows induced by weak mechanical forcings in rotating spheroids
David C\'ebron, J\'er\'emie Vidal, Nathana\"el Schaeffer, Antonin, Borderies, Alban Sauret

TL;DR
This paper develops a boundary-layer theory to predict mean zonal flows induced by weak mechanical forcings in rotating spheroids, validated by numerical simulations, with implications for planetary fluid dynamics.
Contribution
It extends existing theories to include spheroidal geometries and combined spatial-temporal perturbations, providing new insights into planetary-scale flow generation.
Findings
Analytical predictions match numerical simulations well.
Mean zonal flows are significantly affected by spheroidal geometry.
Critical latitude effects influence flow structures and shear layers.
Abstract
The generation of mean flows is a long-standing issue in rotating fluids. Motivated by planetary objects, we consider here a rapidly rotating fluid-filled spheroid, which is subject to weak perturbations of either the boundary (e.g. tides) or the rotation vector (e.g. in direction by precession, or in magnitude by longitudinal librations). Using boundary-layer theory, we determine the mean zonal flows generated by nonlinear interactions within the viscous Ekman layer. These flows are of interest because they survive in the relevant planetary regime of both vanishing forcings and viscous effects. We extend the theory to take into account (i) the combination of spatial and temporal perturbations, providing new mechanically driven zonal flows (e.g. driven by latitudinal librations), and (ii) the spheroidal geometry relevant for planetary bodies. Wherever possible, our analytical…
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