Boundary Zonal Flow in Rotating Turbulent Rayleigh-Bénard Convection

For rapidly rotating turbulent Rayleigh--Bénard convection in a slender cylindrical cell, experiments and direct numerical simulations reveal a boundary zonal flow (BZF) that replaces the classical large-scale circulation. The BZF is located near the vertical side wall and enables enhanced heat tran...

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Bibliographic Details
Published inarXiv.org
Main Authors Zhang, Xuan, Dennis P M van Gils, Horn, Susanne, Wedi, Marcel, Zwirner, Lukas, Ahlers, Guenter, Ecke, Robert E, Weiss, Stephan, Bodenschatz, Eberhard, Shishkina, Olga
Format Paper
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 21.11.2019
Subjects
Atmospheric pressure
Computational fluid dynamics
Computer simulation
Rayleigh-Benard convection
Rotation
Temperature distribution
Traveling waves
Turbulent flow
Zonal flow (meteorology)
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Summary:For rapidly rotating turbulent Rayleigh--Bénard convection in a slender cylindrical cell, experiments and direct numerical simulations reveal a boundary zonal flow (BZF) that replaces the classical large-scale circulation. The BZF is located near the vertical side wall and enables enhanced heat transport there. Although the azimuthal velocity of the BZF is cyclonic (in the rotating frame), the temperature is an anticyclonic traveling wave of mode one whose signature is a bimodal temperature distribution near the radial boundary. The BZF width is found to scale like \(Ra^{1/4}Ek^{2/3}\) where the Ekman number \(Ek\) decreases with increasing rotation rate.
ISSN:2331-8422
DOI:10.48550/arxiv.1911.09584