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首页> 外文期刊>Journal of Colloid and Interface Science >RHEOLOGY OF COLLOIDAL PARTICLES IN A CONFINED CHANNEL UNDER SHEAR FLOW BY BROWNIAN DYNAMIC SIMULATIONS
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RHEOLOGY OF COLLOIDAL PARTICLES IN A CONFINED CHANNEL UNDER SHEAR FLOW BY BROWNIAN DYNAMIC SIMULATIONS

机译:布朗流动模拟下剪切流中受限通道中胶体颗粒的流变学

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摘要

A colloidal system of strongly charged particles, confined between two charged walls, is studied under static conditions and in the presence of shear flows. Brownian Dynamics simulations (ED) are used to determine the concentration profiles for several separations of charged walls. Results show good agreement with those obtained under static conditions using the Hypernetted Chain Approximation (HNC) and Monte Carlo simulations. Results obtained with ED and HNC for neutral walls show more similarities than those between ED and Monte Carlo simulations depending on the initial state of the colloidal particles. The presence of a shear flow field perturbs the equilibrium concentration profiles and the distribution function in the flow direction, generating a structureless system, as confirmed by the absence of peaks in the radial distribution function. The mobility of the particles in the transversal direction decreases rapidly and becomes practically frozen. The flow exhibits a non-Newtonian behavior with shear-thinning viscosity. Due to the interparticle interactions and particle-wall interactions, the viscosity is lower as the wall separation decreases, giving rise to an apparent slip in the colloidal suspension. The slip velocity for repulsive walls is higher than that obtained with neutral walls and increases with the shear stress according to a power law, as observed in polymer solutions. The shear viscosity and the normal stress differences depend strongly on the combined effect of confinement, concentration of particles, magnitudes of inter-particle interactions and wall-particle repulsion. (C) 1997 Academic Press. [References: 27]
机译:在静态条件下,在剪切流作用下,研究了两个带电壁之间的强带电粒子的胶体体系。布朗动力学模拟(ED)用于确定带电壁的几次分离的浓度曲线。结果表明,这些结果与在静态条件下使用超网链近似(HNC)和蒙特卡洛模拟获得的结果吻合良好。用ED和HNC获得的中性壁结果显示出比ED和Monte Carlo模拟之间更多的相似性,这取决于胶体颗粒的初始状态。剪切流场的存在扰动了平衡浓度分布和流向中的分布函数,从而生成了一个无结构的系统,这可以通过径向分布函数中不存在峰值来确认。颗粒在横向上的迁移率迅速降低并实际上被冻结。流动表现出具有剪切稀化粘度的非牛顿行为。由于颗粒间相互作用和颗粒-壁相互作用,随着壁间距的减小,粘度降低,从而在胶体悬浮液中产生明显的滑移。如在聚合物溶液中所观察到的,排斥壁的滑移速度高于中性壁所获得的滑移速度,并且根据幂定律随剪切应力而增加。剪切粘度和法向应力差在很大程度上取决于约束,颗粒浓度,颗粒间相互作用的大小和壁-颗粒排斥的综合作用。 (C)1997学术出版社。 [参考:27]

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