球形约束下的形状诱导偏析和异常粒子输运

Abhinendra Singh, J. Hernandez-Ortiz, H. Jaeger, J. D. de Pablo
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引用次数: 4

摘要

胶体或纳米颗粒在约束下的迁移对广泛的物理和生物过程至关重要。在这里,我们引入了流体力学连续体中粒子的最小模型来研究粒子形状和浓度如何影响粒子在球形约束下的输运。具体而言,采用浸入式边界一般几何类ewald方法,在适当的围壁防滑条件下,模拟了球体和圆柱体在短、长时间波动水动力相互作用影响下的动力学。采用了一种高效的$\it{O(N)}$并行有限元算法,从而允许在高浓度下进行模拟,同时实现了切比雪夫多项式近似,以满足波动耗散定理。观察到悬浮粒子的浓度依赖性异常扩散。研究发现,在球体背景(即具有简单各向异性程度的粒子)中引入圆柱体对粒子的结构和动力学有显著的影响。首先,增加圆柱体的比例会引起粒子偏析效应,其中球体被推向壁面而圆柱体保持在腔的中心附近。这种分离导致相对于在相同体积分数下的纯球系统中遇到的球的低迁移率。其次,扩散到异常的转变和异常的程度——通过均方位移与时间关系的幂律指数来量化——都随着圆柱体的比例变得更大而增加。这些发现与细胞质中扩散的研究相关,在细胞质中,蛋白质表现出大小和形状的分布,这可能导致在这里报告的模拟中确定的一些效应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Shape induced segregation and anomalous particle transport under spherical confinement
Colloid or nanoparticle mobility under confinement is of central importance to a wide range of physical and biological processes. Here, we introduce a minimal model of particles in a hydrodynamic continuum to examine how particle shape and concentration affect the transport of particles in spherical confinement. Specifically, an immersed boundary-General geometry Ewald-like approach is adopted to simulate the dynamics of spheres and cylinders under the influence of short-and long-range fluctuating hydrodynamic interactions with appropriate non-slip conditions at the confining walls. An efficient $\it{O(N)}$ parallel finite element algorithm is used, thereby allowing simulations at high concentrations, while a Chebyshev polynomial approximation is implemented in order to satisfy the fluctuation-dissipation theorem. A concentration-dependent anomalous diffusion is observed for suspended particles. It is found that introducing cylinders in a background of spheres, i.e. particles with a simple degree of anisotropy, has a pronounced influence on the structure and dynamics of the particles. First, increasing the fraction of cylinders induces a particle segregation effect, where spheres are pushed towards the wall and cylinders remain near the center of the cavity. This segregation leads to lower mobility for the spheres relative to that encountered in a system of pure spheres at the same volume fraction. Second, the diffusive-to-anomalous transition and the degree of anomaly--quantified by the power-law exponent in the mean square displacement vs. time relation-both increase as the fraction of cylinders becomes larger. These findings are of relevance for studies of diffusion in the cytoplasm, where proteins exhibit a distribution of size and shapes that could lead to some of the effects identified in the simulations reported here.
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