EHD convection in an enclosed rectangular domain

P. Vázquez, Jian Wu, P. Traoré, A. Pérez
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Abstract

In this work, we present the results of numerical simulations of the EHD convection between parallel plates in a rectangular domain with no-slip boundary conditions at all the walls. The electroconvection between parallel plates in an infinite domain is a classic EHD problem. Experimental, theoretical and numeric studies show that when a high enough voltage is applied across the plates, the liquid is set into motion. The nature of the bifurcation is subcritical. A roll pattern is established where the maximum velocity of the liquid is higher than the drift velocity of the ions. As a consequence, regions voided of electric charge appears in the bulk. However, when the domain is enclosed by rigid walls, the nature of the bifurcation changes, becoming supercritical. Stable velocity rolls with a maximum velocity smaller than the drift velocity of the ions are possible. We present a numeric analysis of these new phenomena. The physical mechanism which leads to this situation is analyzed and discussed. The evolution of the bifurcation diagrams with the aspect ratio of the cavity is also provided and analyzed.
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封闭矩形域中的EHD对流
在此工作中,我们给出了在所有壁面无滑移边界条件下矩形区域内平行板间EHD对流的数值模拟结果。无限域中平行板间的电对流是一个经典的EHD问题。实验、理论和数值研究表明,当在平板上施加足够高的电压时,液体就会开始运动。分岔的性质是次临界的。当液体的最大速度高于离子的漂移速度时,建立了一种滚转模式。因此,在整体中出现了无电荷的区域。然而,当区域被刚性壁包围时,分岔的性质发生了变化,成为超临界的。最大速度小于离子漂移速度的稳定速度滚转是可能的。我们对这些新现象进行了数值分析。对导致这种情况的物理机理进行了分析和讨论。给出并分析了分岔图随空腔宽高比的演变规律。
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