Toroidal and poloidal energy in rotating Rayleigh-Bénard convection
arXiv:1404.7755 · doi:10.1017/jfm.2014.652
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 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 as long as 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 turbulence regime for high rotation rates where the toroidal energy drops below the value of non-rotating convection.
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