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Penetration of boundary-driven flows into a rotating spherical thermally stratified fluid

Published online by Cambridge University Press:  11 February 2019

Grace A. Cox Open the ORCID record for Grace A. Cox [Opens in a new window] ,
Christopher J. Davies ,
Philip W. Livermore  and
James Singleton
Grace A. Cox*
Affiliation:
School of Environmental Sciences, University of Liverpool, LiverpoolL69 3GP, UK Department of Applied Mathematics, University of Leeds, LeedsLS2 9JT, UK Dublin Institute for Advanced Studies, Geophysics Section, Dublin 2, Ireland
Christopher J. Davies
Affiliation:
School of Earth and Environment, University of Leeds, LeedsLS2 9JT, UK
Philip W. Livermore
Affiliation:
School of Earth and Environment, University of Leeds, LeedsLS2 9JT, UK
James Singleton
Affiliation:
School of Earth and Environment, University of Leeds, LeedsLS2 9JT, UK
*
†Email address for correspondence: [email protected]
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Abstract

Motivated by the dynamics within terrestrial bodies, we consider a rotating, strongly thermally stratified fluid within a spherical shell subject to a prescribed laterally inhomogeneous heat-flux condition at the outer boundary. Using a numerical model, we explore a broad range of three key dimensionless numbers: a thermal stratification parameter (the relative size of boundary temperature gradients to imposed vertical temperature gradients), $10^{-3}\leqslant S\leqslant 10^{4}$, a buoyancy parameter (the strength of applied boundary heat-flux anomalies), $10^{-2}\leqslant B\leqslant 10^{6}$, and the Ekman number (ratio of viscous to Coriolis forces), $10^{-6}\leqslant E\leqslant 10^{-4}$. We find both steady and time-dependent solutions and delineate the regime boundaries. We focus on steady-state solutions, for which a clear transition is found between a low $S$ regime, in which buoyancy dominates the dynamics, and a high $S$ regime, in which stratification dominates. For the low-$S$ regime, we find that the characteristic flow speed scales as $B^{2/3}$, whereas for high-$S$, the radial and horizontal velocities scale respectively as $u_{r}\sim S^{-1}$, $u_{h}\sim S^{-3/4}B^{1/4}$ and are confined within a thin layer of depth $(SB)^{-1/4}$ at the outer edge of the domain. For the Earth, if lower mantle heterogeneous structure is due principally to chemical anomalies, we estimate that the core is in the high-$S$ regime and steady flows arising from strong outer boundary thermal anomalies cannot penetrate the stable layer. However, if the mantle heterogeneities are due to thermal anomalies and the heat-flux variation is large, the core will be in a low-$S$ regime in which the stable layer is likely penetrated by boundary-driven flows.

JFM classification

Convection: Buoyancy-driven instability Geophysical and Geological Flows: Rotating flows Geophysical and Geological Flows: Stratified flows
Type
JFM Papers
Information
Journal of Fluid Mechanics , Volume 864 , 10 April 2019 , pp. 519 - 553
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Copyright
© 2019 Cambridge University Press 

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