Lifetimes of metastable windy states in two-dimensional Rayleigh-Benard convection with stress-free boundaries

被引:4
作者
Wang, Qi [1 ]
Goluskin, David [2 ]
Lohse, Detlef [3 ,4 ,5 ]
机构
[1] Southern Univ Sci & Technol, Dept Mech & Aerosp Engn, Shenzhen 518055, Peoples R China
[2] Univ Victoria, Dept Math & Stat, Victoria, BC V8P 5C2, Canada
[3] Univ Twente, Phys Fluids Grp, POB 217, NL-7500AE Enschede, Netherlands
[4] Univ Twente, Max Planck Ctr Complex Fluid Dynam, J M Burgers Ctr Fluid Dynam, POB 217, NL-7500AE Enschede, Netherlands
[5] Max Planck Inst Dynam & Selforg, D-37077 Gottingen, Germany
基金
加拿大自然科学与工程研究理事会;
关键词
Benard convection; TURBULENCE; CIRCULATION; TRANSITION; FLOWS;
D O I
10.1017/jfm.2023.875
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
Two-dimensional horizontally periodic Rayleigh-Benard convection between stress-free boundaries displays two distinct types of states, depending on the initial conditions. Roll states are composed of pairs of counter-rotating convection rolls. Windy states are dominated by strong horizontal wind (also called zonal flow) that is vertically sheared, precludes convection rolls and suppresses heat transport. Windy states occur only when the Rayleigh number Ra is sufficiently above the onset of convection. At intermediate Ra values, windy states can be induced by suitable initial conditions, but they undergo a transition to roll states after finite lifetimes. At larger Ra values, where windy states have been observed for the full duration of simulations, it is unknown whether they represent chaotic attractors or only metastable states that would eventually undergo a transition to roll states. We study this question using direct numerical simulations of a fluid with a Prandtl number of 10 in a layer whose horizontal period is eight times its height. At each of seven Ra values between 9 x 10(6) and 2.25 x 10(7) we have carried out 200 or more simulations, all from initial conditions leading to windy convection with finite lifetimes. The lifetime statistics at each Ra indicate a memoryless process with survival probability decreasing exponentially in time. The mean lifetimes grow with Ra approximately as Ra-4. This analysis provides no Ra value at which windy convection becomes stable; it might remain metastable at larger Ra with extremely long lifetimes.
引用
收藏
页数:11
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