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采用动态更新速度剖面和电场相互作用并结合力偏置蒙特卡罗方法模拟胶体堵塞对膜过滤的影响。

Simulation of colloidal fouling by coupling a dynamically updating velocity profile and electric field interactions with Force Bias Monte Carlo methods for membrane filtration.

机构信息

Department of Mechanical Engineering & Materials Science, Rice University, Houston, TX 77005, United States.

出版信息

J Colloid Interface Sci. 2013 Jun 1;399:77-86. doi: 10.1016/j.jcis.2012.10.074. Epub 2012 Nov 29.

DOI:10.1016/j.jcis.2012.10.074
PMID:23540433
Abstract

Pressure-driven flow through a channel with membrane walls is modeled for high particulate volume fractions of 10%. Particle transport is influenced by Brownian diffusion, shear-induced diffusion, and convection due to the axial crossflow. The particles are also subject to electrostatic double layer repulsion and van der Waals attraction, from both particle-particle and particle-membrane interactions. Force Bias Monte Carlo (FBMC) simulations predict the deposition of the particles onto the membranes, where both hydrodynamics and the change in particle potentials determine the probability that a proposed move is accepted. The particle volume fraction is used to determine an apparent local viscosity observed by the continuum flow. As particles migrate, the crossflow velocity field evolves in quasi-steady fashion with each time instance appearing fully developed in the downstream direction. Particles subject to combined hydrodynamic and electric effects (electrostatic double layer repulsion and van der Waals attraction) reach a more stable steady-state as compared to systems with only hydrodynamic effects considered. As expected, at higher crossflow Reynolds numbers more particles remain in the crossflow free stream.

摘要

采用膜壁的通道内压力驱动流动模型,用于模拟高达 10%的高颗粒体积分数。颗粒输运受到布朗扩散、剪切诱导扩散和轴向横流引起的对流的影响。颗粒还受到静电双电层排斥和范德华吸引力的影响,这来自颗粒-颗粒和颗粒-膜相互作用。力偏置蒙特卡罗(FBMC)模拟预测了颗粒在膜上的沉积,其中流体动力学和颗粒势的变化决定了提议的迁移是否被接受的概率。颗粒体积分数用于确定连续流观察到的表观局部粘度。随着颗粒的迁移,横流速度场以准稳态方式演变,每个时间实例在下游方向上都呈现完全发展的状态。与仅考虑流体动力效应的系统相比,受到流体动力和电效应(静电双电层排斥和范德华吸引力)共同作用的颗粒达到更稳定的稳态。如预期的那样,在更高的横流雷诺数下,更多的颗粒留在横流自由流中。

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