垂直通道中马克斯韦尔-卡塔尼奥流体的索雷特驱动对流

IF 2.5 3区 工程技术 Q2 MECHANICS
Yanjun Sun , Beinan Jia , Long Chang , Yongjun Jian
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引用次数: 0

摘要

索雷特效应(又称热扩散)在液体双扩散对流现象中起着至关重要的作用。本研究探讨了在 Maxwell-Cattaneo (M-C) 流体的垂直双扩散层内的索雷特驱动对流,在该双扩散层中,边界保持恒定的温度和溶质浓度,且彼此不同。Maxwell-Cattaneo 流体的传热方程受双曲热传导规律支配,而不是典型的傅立叶抛物线规律。采用切比雪夫配位法求解相应的稳定性特征值问题。由于 M-C 效应,中性稳定曲线显示出明显的波动响应。当 Cattaneo 数(C)达到 0.02 时,临界 Grashof 数(Gr)出现多个局部极小值。在 Maxwell-Cattaneo 和 Soret 以及 Grashof 数的共同作用下,热对流的不稳定性被放大,而双重扩散效应似乎抑制了对流系统的不稳定性。当 Gr 数升至 8200 以上时,索雷特效应对对流不稳定性的影响将显著减弱。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Soret-driven convection of Maxwell-Cattaneo fluids in a vertical channel

The Soret effect, also known as thermal diffusion, plays a crucial role in the phenomenon of double diffusion convection in liquids. This study investigates Soret-driven convection within a vertical double-diffusive layer of Maxwell-Cattaneo (M-C) fluids, where the boundaries maintain constant temperatures and solute concentrations that are distinct from each other. The heat transfer equation for Maxwell-Cattaneo fluids is governed by a hyperbolic rule of heat conduction, rather than the typical Fourier parabolic one. The Chebyshev collocation method is employed to solve the corresponding stability eigenvalue problem. The neutral stability curve shows significant fluctuation responses due to the M-C effect. When the Cattaneo number (C) reaches 0.02, multiple local minima appear in the critical Grashof number (Gr). The instability the thermal convection is found to be amplified by the combined effects of Maxwell-Cattaneo and Soret, along with the Grashof number, while the double diffusion effect appears to suppress the instability of convective system. The influence of Soret effect on convective instability will diminish dramatically as the Gr number rises above 8200.

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来源期刊
CiteScore
5.90
自引率
3.80%
发文量
127
审稿时长
58 days
期刊介绍: The European Journal of Mechanics - B/Fluids publishes papers in all fields of fluid mechanics. Although investigations in well-established areas are within the scope of the journal, recent developments and innovative ideas are particularly welcome. Theoretical, computational and experimental papers are equally welcome. Mathematical methods, be they deterministic or stochastic, analytical or numerical, will be accepted provided they serve to clarify some identifiable problems in fluid mechanics, and provided the significance of results is explained. Similarly, experimental papers must add physical insight in to the understanding of fluid mechanics.
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