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Scaling behaviour in Rayleigh–Bénard convection with and without rotation

Published online by Cambridge University Press:  01 February 2013

E. M. King*
Affiliation:
Department of Earth and Planetary Science, University of California, Berkeley, CA 94720-4767, USA Department of Physics, University of California, Berkeley, CA 94720-7300, USA
S. Stellmach
Affiliation:
Institut für Geophysik, WWU Münster, Corrensstrasse 24, 48149 Münster, Germany
B. Buffett
Affiliation:
Department of Earth and Planetary Science, University of California, Berkeley, CA 94720-4767, USA
*
Email address for correspondence: [email protected]

Abstract

Rotating Rayleigh–Bénard convection provides a simplified dynamical analogue for many planetary and stellar fluid systems. Here, we use numerical simulations of rotating Rayleigh–Bénard convection to investigate the scaling behaviour of five quantities over a range of Rayleigh ($1{0}^{3} \lesssim \mathit{Ra}\lesssim 1{0}^{9} $), Prandtl ($1\leq \mathit{Pr}\leq 100$) and Ekman ($1{0}^{- 6} \leq E\leq \infty $) numbers. The five quantities of interest are the viscous and thermal boundary layer thicknesses, ${\delta }_{v} $ and ${\delta }_{T} $, mean temperature gradients, $\beta $, characteristic horizontal length scales, $\ell $, and flow speeds, $\mathit{Pe}$. Three parameter regimes in which different scalings apply are quantified: non-rotating, weakly rotating and rotationally constrained. In the rotationally constrained regime, all five quantities are affected by rotation. In the weakly rotating regime, ${\delta }_{T} $, $\beta $ and $\mathit{Pe}$, roughly conform to their non-rotating behaviour, but ${\delta }_{v} $ and $\ell $ are still strongly affected by the Coriolis force. A summary of scaling results is given in table 2.

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Papers
Copyright
©2013 Cambridge University Press

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