Boundary zonal flows in rapidly rotating turbulent thermal convection
arXiv:2009.03401 · doi:10.1017/jfm.2021.74
Abstract
Recently, in Zhang et al. (2020), it was found that in rapidly rotating turbulent Rayleigh-Bénard convection (RBC) in slender cylindrical containers (with diameter-to-height aspect ratio ) filled with a small-Prandtl-number fluid (), the Large Scale Circulation (LSC) is suppressed and a Boundary Zonal Flow (BZF) develops near the sidewall, characterized by a bimodal PDF of the temperature, cyclonic fluid motion, and anticyclonic drift of the flow pattern (with respect to the rotating frame). This BZF carries a disproportionate amount () of the total heat transport for but decreases rather abruptly for larger to about . In this work, we show that the BZF is robust and appears in rapidly rotating turbulent RBC in containers of different and in a broad range of and . Direct numerical simulations for , , and = 1/3, 1/2, 3/4, 1 and 2 show that the BZF width scales with the Rayleigh number and Ekman number as () and the drift frequency as , where is the cell height and the angular rotation rate. The mode number of the BZF is 1 for and for = {1,2} independent of and . The BZF is quite reminiscent of wall mode states in rotating convection.
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- Rapidly Rotating Wall-Mode Convection
- Data-driven identification of the spatio-temporal structure of turbulent flows by streaming Dynamic Mode Decomposition
- Scale-by-scale kinetic energy flux calculations in simulations of rotating convection