Toroidal and poloidal energy in rotating Rayleigh–Bénard convection

Susanne Horn, Olga Shishkina

Research output: Contribution to journalArticle

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Abstract

We consider rotating Rayleigh–Bénard convection of a fluid with a Prandtl number of in a cylindrical cell with an aspect ratio . Direct numerical simulations (DNS) were performed for the Rayleigh number range and the inverse Rossby number range . We propose a method to capture regime transitions based on the decomposition of the velocity field into toroidal and poloidal parts. We identify four different regimes. First, a buoyancy-dominated regime occurring while the toroidal energy is not affected by rotation and remains equal to that in the non-rotating case, . Second, a rotation-influenced regime, starting at rotation rates where and ending at a critical inverse Rossby number that is determined by the balance of the toroidal and poloidal energy, . Third, a rotation-dominated regime, where the toroidal energy is larger than both and . Fourth, a geostrophic regime for high rotation rates where the toroidal energy drops below the value for non-rotating convection.
Original languageEnglish
Pages (from-to)232-255
Number of pages24
JournalJournal of Fluid Mechanics
Volume762
Early online date2 Dec 2014
DOIs
Publication statusPublished - 10 Jan 2015
Externally publishedYes

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convection
energy
Prandtl number
Direct numerical simulation
Buoyancy
Rayleigh number
Aspect ratio
direct numerical simulation
buoyancy
Convection
aspect ratio
Decomposition
velocity distribution
Fluids
decomposition
fluids
cells

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Toroidal and poloidal energy in rotating Rayleigh–Bénard convection. / Horn, Susanne; Shishkina, Olga.

In: Journal of Fluid Mechanics, Vol. 762, 10.01.2015, p. 232-255.

Research output: Contribution to journalArticle

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