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Electrohydrodynamic instability of dielectric fluid layer between two semi-infinite identical conducting fluids in porous medium

机译:多孔介质中两种半无限相同导电流体之间介电层的电流体动力学不稳定性

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The electrohydrodynamic instability of a plane layer of dielectric fluid which is in hydrostatic equilibrium between two semi-infinite conducting fluids with surface charges in porous media is investigated. The dispersion relation is derived for the general case of Brinkman model for both high medium viscosity and permeability, and by considering the fluid layer is very thin. The limiting case of Darcy model in which the viscous convective term is absent is also investigated. The dispersion relations for both antisymmetrical and symmetrical disturbance cases are derived, respectively. For non-porous medium and absence of the electric field, we found that all waves, in both models, are damped, while for porous medium and sufficiently large electric field values, there will be stability (in Brinkman model), and instability (in Darcy model). It is found (in Brinkman model) that each of the electric fields, porosity of the porous medium, surface tension, and the fluid layer depth have a stabilizing effect, while the fluid viscosity has a destabilizing influence, and the medium permeability has a dual role (stabilizing and then destabilizing) separated by a critical wavenumber value that increases with increasing medium permeability values. It is found (in Darcy model) that the electric field has a destabilizing effect, and both the surface tension and the liquid depth have stabilizing effects, while the fluid viscosity has a dual role (stabilizing and then destabilizing), whereas both the porosity of porous medium and the medium permeability have dual roles (destabilizing and then stabilizing) separated by a constant critical wavenumber value. The effects of these parameters hold, for the symmetrical disturbance case, in both models, more faster than their effects in the corresponding antisymmetrical disturbance ones. Finally, consideration is given to the relevance of the results in explaining the mechanism by which the presence of an electric field in porous medium promotes more readily the coalescence of water droplets on a water surface. (c) 2005 Elsevier B.V. All rights reserved.
机译:研究了在多孔介质中具有表面电荷的两种半无限导电流体之间处于静水平衡的介电液平面层的电流体动力学不稳定性。对于Brinkman模型的一般情况,对于高介质粘度和渗透率,并通过考虑流体层非常薄,得出了色散关系。还研究了不存在粘性对流项的Darcy模型的极限情况。分别推导了非对称和对称扰动情况下的色散关系。对于无孔介质和没有电场,我们发现两个模型中的所有波都被阻尼,而对于多孔介质和足够大的电场值,将存在稳定性(在Brinkman模型中)和不稳定性(在Brinkman模型中)。达西模型)。 (在布林克曼模型中)发现,电场,多孔介质的孔隙率,表面张力和流体层深度均具有稳定作用,而流体粘度具有不稳定影响,并且介质渗透率具有双重效应。作用(稳定,然后不稳定)被临界波数值所分隔,该临界波数值随介质渗透率值的增加而增加。发现(在达西模型中)电场具有去稳定作用,表面张力和液体深度都具有去稳定作用,而流体粘度具有双重作用(先稳定然后去稳定),而孔隙度则具有双重作用。多孔介质和介质渗透性具有双重作用(去稳定,然后稳定),它们被恒定的临界波数值隔开。对于两个模型,在对称干扰情况下,这些参数的影响要比在相应的非对称干扰模型中的影响更快。最后,在解释多孔介质中电场的存在可促进水表面上的水滴聚结的机理时,应考虑结果的相关性。 (c)2005 Elsevier B.V.保留所有权利。

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