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具有温度调制的瑞利-贝纳德磁对流

Rayleigh-Bénard magnetoconvection with temperature modulation.

作者信息

Hazra Suparna, Kumar Krishna, Mitra Saheli

机构信息

Department of Physics, Indian Institute of Technology Kharagpur, Kharagpur 721302, West Bengal, India.

Laboratoire de Physique des Solides, Université Paris-Saclay, CNRS, 91405 Orsay, France.

出版信息

Proc Math Phys Eng Sci. 2020 Oct;476(2242):20200289. doi: 10.1098/rspa.2020.0289. Epub 2020 Oct 14.

DOI:10.1098/rspa.2020.0289
PMID:33223933
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7655742/
Abstract

Floquet analysis of modulated magnetoconvection in Rayleigh-Bénard geometry is performed. A sinusoidally varying temperature is imposed on the lower plate. As Rayleigh number Ra is increased above a critical value Ra, the oscillatory magnetoconvection begins. The flow at the onset of magnetoconvection may oscillate either subhar- monically or harmonically with the external modulation. The critical Rayleigh number Ra varies non-monotonically with the modulation frequency for appreciable value of the modulation amplitude . The temperature modulation may either postpone or prepone the appearance of magnetoconvection. The magnetoconvective flow always oscillates harmonically at larger values of . The threshold Ra and the corresponding wavenumber approach to their values for the stationary magnetoconvection in the absence of modulation ( = 0), as  → ∞. Two different zones of harmonic instability merge to form a single instability zone with two local minima for higher values of Chandrasekhar's number , which is qualitatively new. We have also observed a new type of bicritical point, which involves two different sets of harmonic oscillations. The effects of variation of and Pr on the threshold Ra and critical wavenumber are also investigated.

摘要

对瑞利 - 贝纳德几何结构中调制磁对流进行了弗洛凯分析。在下板施加正弦变化的温度。当瑞利数(Ra)增加到高于临界值(Ra_c)时,振荡磁对流开始。磁对流开始时的流动可能与外部调制以次谐波或谐波形式振荡。对于可观的调制幅度值,临界瑞利数(Ra_c)随调制频率非单调变化。温度调制可能会推迟或提前磁对流的出现。在较大的(\omega)值时,磁对流流动总是以谐波形式振荡。当(\omega\to\infty)时,阈值(Ra_c)和相应的波数(k)趋近于无调制((\omega = 0))时稳态磁对流的数值。对于更高的钱德拉塞卡数(Q)值,两个不同的谐波不稳定区域合并形成一个具有两个局部最小值的单一不稳定区域,这在性质上是新的。我们还观察到一种新型的双临界点,它涉及两组不同的谐波振荡。还研究了(Q)和普朗特数(Pr)的变化对阈值(Ra_c)和临界波数(k)的影响。