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使用孔隙尺度格子玻尔兹曼模拟预测二维 Berea 砂岩中的不混溶两相流特性。

Prediction of immiscible two-phase flow properties in a two-dimensional Berea sandstone using the pore-scale lattice Boltzmann simulation.

作者信息

Xu Meng, Liu Haihu

机构信息

School of Energy and Power Engineering, Xi'an Jiaotong University, 28 West Xianning Road, 710049, Xi'an, China.

出版信息

Eur Phys J E Soft Matter. 2018 Oct 18;41(10):124. doi: 10.1140/epje/i2018-11735-3.

Abstract

Immiscible two-phase flow in porous media is commonly encountered in industrial processes and environmental issues, such as enhanced oil recovery and the migration of fluids in an unsaturated zone. To deepen the current understanding of its underlying mechanism, this work focuses on the factors that influence the relative permeability and specific interfacial length of a two-phase flow in porous media, i.e., fluid saturation, viscosity ratio and contact angle. The lattice Boltzmann color-gradient model is adopted for pore-scale investigations, and the main findings are obtained as follows. Firstly, the relative permeability of each fluid increases as its saturation increases. The specific interfacial length first increases and then decreases as the saturation of the wetting fluid increases, and reaches a maximum when the permeabilities of both fluids are equal. Secondly, as the viscosity ratio of wetting to non-wetting fluids increases, the relative permeability of the wetting fluid will increase while that of the non-wetting fluid will decrease. The specific interfacial length will increase with increasing the viscosity difference between fluids. Finally, as the contact angle (measured from the wetting fluid) increases, the relative permeability of the wetting fluid overall increases while that of the non-wetting fluid decreases. Increasing contact angle always leads to a decrease in the specific interfacial length.

摘要

多孔介质中的不混溶两相流在工业过程和环境问题中普遍存在,例如强化采油和非饱和带中流体的运移。为了深化目前对其潜在机制的理解,本研究聚焦于影响多孔介质中两相流相对渗透率和比界面长度的因素,即流体饱和度、粘度比和接触角。采用格子玻尔兹曼颜色梯度模型进行孔隙尺度研究,主要研究结果如下。首先,每种流体的相对渗透率随其饱和度的增加而增加。比界面长度随润湿流体饱和度的增加先增加后减小,当两种流体的渗透率相等时达到最大值。其次,随着润湿流体与非润湿流体粘度比的增加,润湿流体的相对渗透率将增加,而非润湿流体的相对渗透率将降低。比界面长度将随着流体间粘度差的增加而增加。最后,随着接触角(从润湿流体测量)的增加,润湿流体的相对渗透率总体上增加,而非润湿流体的相对渗透率降低。接触角增大总是导致比界面长度减小。

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