The onset of zonal modes in two-dimensional Rayleigh-Bénard convection

We study the stability of steady convection rolls in two-dimensional Rayleigh-Bénard convection with free-slip boundaries and horizontal periodicity over 12 orders of magnitude in the Prandtl number (10-6 ≤ Pr ≤ 106) and 6 orders of magnitude in the Rayleigh number(8π4 < Ra ≤ 108). The analysis...

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Bibliographic Details
Main Authors: Dallas, V. (Author), Howell, P.D (Author), Winchester, P. (Author)
Format: Article
Language:English
Published: Cambridge University Press 2022
Subjects:
Online Access:View Fulltext in Publisher
LEADER 02444nam a2200361Ia 4500
001 10.1017-jfm.2022.185
008 220425s2022 CNT 000 0 und d
020 |a 00221120 (ISSN) 
245 1 0 |a The onset of zonal modes in two-dimensional Rayleigh-Bénard convection 
260 0 |b Cambridge University Press  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1017/jfm.2022.185 
520 3 |a We study the stability of steady convection rolls in two-dimensional Rayleigh-Bénard convection with free-slip boundaries and horizontal periodicity over 12 orders of magnitude in the Prandtl number (10-6 ≤ Pr ≤ 106) and 6 orders of magnitude in the Rayleigh number(8π4 < Ra ≤ 108). The analysis is facilitated by partitioning our modal expansion into so-called even and odd modes. With aspect ratio Γ =2, we observe that zonal modes (with horizontal wavenumber equal to zero) can emerge only once the steady convection roll state consisting of even modes only becomes unstable to odd perturbations. We determine the stability boundary in the (Pr, Ra) plane and observe remarkably intricate features corresponding to qualitative changes in the solution, as well as three regions where the steady convection rolls lose and subsequently regain stability as the Rayleigh number is increased. We study the asymptotic limit Pr → 0 and find that the steady convection rolls become unstable almost instantaneously, eventually leading to nonlinear relaxation osculations and bursts, which we can explain with a weakly nonlinear analysis. In the complementary large-Pr limit, we observe that the zonal modes at the instability switch off abruptly at a large, but finite, Prandtl number. © The Author(s), 2022. Published by Cambridge University Press. 
650 0 4 |a Aspect ratio 
650 0 4 |a Benard convection 
650 0 4 |a Bénard convection 
650 0 4 |a bifurcation 
650 0 4 |a Free-slip 
650 0 4 |a low-dimensional models 
650 0 4 |a Low-dimensional models 
650 0 4 |a Modal expansion 
650 0 4 |a Natural convection 
650 0 4 |a Nonlinear analysis 
650 0 4 |a Orders of magnitude 
650 0 4 |a Prandtl number 
650 0 4 |a Rayleigh number 
650 0 4 |a Slip boundary 
650 0 4 |a Steady convection 
650 0 4 |a Two-dimensional 
650 0 4 |a Zonal modes 
700 1 |a Dallas, V.  |e author 
700 1 |a Howell, P.D.  |e author 
700 1 |a Winchester, P.  |e author 
773 |t Journal of Fluid Mechanics