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光滑壁和粗糙壁限制对密集硬球悬浮液中粒子动力学的影响。

Influence of confinement by smooth and rough walls on particle dynamics in dense hard-sphere suspensions.

作者信息

Eral H B, van den Ende D, Mugele F, Duits M H G

机构信息

Physics of Complex Fluids, IMPACT Institute, University of Twente, PO Box 217, 7500 AE Enschede, The Netherlands.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2009 Dec;80(6 Pt 1):061403. doi: 10.1103/PhysRevE.80.061403. Epub 2009 Dec 14.

Abstract

We used video microscopy and particle tracking to study the dynamics of confined hard-sphere suspensions. Our fluids consisted of 1.1-microm-diameter silica spheres suspended at volume fractions of 0.33-0.42 in water-dimethyl sulfoxide. Suspensions were confined in a quasiparallel geometry between two glass surfaces: a millimeter-sized rough sphere and a smooth flat wall. First, as the separation distance (H) is decreased from 18 to 1 particle diameter, a transition takes place from a subdiffusive behavior (as in bulk) at large H, to completely caged particle dynamics at small H. These changes are accompanied by a strong decrease in the amplitude of the mean-square displacement (MSD) in the horizontal plane parallel to the confining surfaces. In contrast, the global volume fraction essentially remains constant when H is decreased. Second, measuring the MSD as a function of distance from the confining walls, we found that the MSD is not spatially uniform but smaller close to the walls. This effect is the strongest near the smooth wall where layering takes place. Although confinement also induces local variations in volume fraction, the spatial variations in MSD can be attributed only partially to this effect. The changes in MSD are predominantly a direct effect of the confining surfaces. Hence, both the wall roughness and the separation distance (H) influence the dynamics in confined geometries.

摘要

我们使用视频显微镜和粒子追踪技术来研究受限硬球悬浮液的动力学。我们的流体由直径为1.1微米的二氧化硅球体组成,这些球体以0.33 - 0.42的体积分数悬浮在水 - 二甲基亚砜中。悬浮液被限制在两个玻璃表面之间的准平行几何结构中:一个毫米大小的粗糙球体和一个光滑的平板壁。首先,当分离距离(H)从18个粒子直径减小到1个粒子直径时,会发生从大H时的亚扩散行为(如在本体中)到小H时完全受限的粒子动力学的转变。这些变化伴随着平行于限制表面的水平面内均方位移(MSD)振幅的强烈下降。相比之下,当H减小时,总体积分数基本保持不变。其次,测量MSD作为距限制壁距离的函数,我们发现MSD在空间上并不均匀,靠近壁处较小。这种效应在发生分层的光滑壁附近最强。尽管限制也会引起体积分数的局部变化,但MSD的空间变化只能部分归因于这种效应。MSD的变化主要是限制表面的直接影响。因此,壁的粗糙度和分离距离(H)都会影响受限几何结构中的动力学。

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