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流体和脂质膜模拟中的扩散系数差异

Divergent Diffusion Coefficients in Simulations of Fluids and Lipid Membranes.

作者信息

Vögele Martin, Hummer Gerhard

机构信息

Department of Theoretical Biophysics, Max Planck Institute of Biophysics , Max-von-Laue-Straße 3, 60438 Frankfurt am Main, Germany.

出版信息

J Phys Chem B. 2016 Aug 25;120(33):8722-32. doi: 10.1021/acs.jpcb.6b05102. Epub 2016 Jul 22.

Abstract

We investigate the dependence of single-particle diffusion coefficients on the size and shape of the simulation box in molecular dynamics simulations of fluids and lipid membranes. We find that the diffusion coefficients of lipids and a carbon nanotube embedded in a lipid membrane diverge with the logarithm of the box width. For a neat Lennard-Jones fluid in flat rectangular boxes, diffusion becomes anisotropic, diverging logarithmically in all three directions with increasing box width. In elongated boxes, the diffusion coefficients normal to the long axis diverge linearly with the height-to-width ratio. For both lipid membranes and neat fluids, this behavior is predicted quantitatively by hydrodynamic theory. Mean-square displacements in the neat fluid exhibit intermediate regimes of anomalous diffusion, with t ln t and t(3/2) components in flat and elongated boxes, respectively. For membranes, the large finite-size effects, and the apparent inability to determine a well-defined lipid diffusion coefficient from simulation, rationalize difficulties in comparing simulation results to each other and to those from experiments.

摘要

在流体和脂质膜的分子动力学模拟中,我们研究了单粒子扩散系数对模拟盒大小和形状的依赖性。我们发现,嵌入脂质膜中的脂质和碳纳米管的扩散系数随盒宽度的对数而发散。对于扁平矩形盒中的纯 Lennard-Jones 流体,扩散变得各向异性,随着盒宽度增加,在所有三个方向上对数发散。在细长盒中,垂直于长轴的扩散系数随高宽比线性发散。对于脂质膜和纯流体,这种行为都由流体动力学理论定量预测。纯流体中的均方位移表现出反常扩散的中间区域,在扁平盒和细长盒中分别具有 t ln t 和 t(3/2) 分量。对于膜来说,巨大的有限尺寸效应以及从模拟中明显无法确定明确的脂质扩散系数,使得将模拟结果相互比较以及与实验结果进行比较变得困难。

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