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首页> 外文期刊>The Journal of Chemical Physics >Simulations of concentrated suspensions of rigid fibers:Relationship between short-time diffusivities and the long-time rotational diffusion
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Simulations of concentrated suspensions of rigid fibers:Relationship between short-time diffusivities and the long-time rotational diffusion

机译:刚性纤维集中悬浮液的模拟:短时扩散率与长时间旋转扩散之间的关系

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Brownian dynamics simulations of the behavior of suspensions of fibers demonstrate that the scaling of the rotational diffusivity with respect to the number density(nL~3)is a sensitive function of the thickness and the parameter L~2D_R /D_(T_0),where D_R is the rotational diffusivity at infinite dilution,D_(T_0)is the average center-of-mass diffusivity at infinite dilution,and L is the fiber length.Existing theories for the long-time rotational diffusivities of rigid fibers in the semidilute and concentrated regimes fail to accurately account for the relationship with the dilute values of the rotational and translational diffusivities of the various physical models used to simulate the fibers.The concentration regime studied in this work ranges from a number density of nL~3approx= 0-150,which is below the transition from an isotropic to nematic state.The effect of the fiber thickness was studied by performing simulations of rods with aspect ratios(fiber length over diameter)of 25,50,and 500,as well as performing projections for infinitely thin fibers.The excluded volume of the rods was enforced through the use of short-range potentials.For a rod with an aspect ratio of 50 with a parameter of L~2D_R_0 /D_T_0 = 9,which corresponds to a slender-body model of the individual fibers,the rotational diffusivity(D_R)scales as D_R/D_R_0 ~(nL~3)~(-1.9)in the concentration regime of 70 <=nL~3 <= 150.Similarly with a parameter of L2D_R /D_T_0 =4,corresponding to a rigid-dumbbell model,the rotational diffusivity scales as D_RID~_R_0 ~(nL~3)~(-1.1)over the same range of concentrations.For rods with aspect ratios of 25,it is observed that a difference in the scaling is seen for L~2D_R_0/D_T_0<= 8,with higher values of this ratio exhibiting essentially the same scaling.Additional values of the ratio L~2D_R_0/D_T_0 were investigated to determine the overall behavior of the suspension dynamics with respect to this parameter.These findings resolve discrepancies between simulation results for rotational diffusivities reported by previous investigators and provide new insights for the development of an accurate theory for the diffusivity of rigid rods suspended in solution.
机译:纤维悬浮液行为的布朗动力学模拟表明,旋转扩散率相对于数密度(nL〜3)的缩放是厚度和参数L〜2D_R / D_(T_0)的敏感函数,其中D_R是无限稀释时的旋转扩散系数,D_(T_0)是无限稀释时的平均质心扩散系数,L是纤维长度。半稀释和集中状态下刚性纤维的长期旋转扩散的现有理论未能准确说明与用于模拟纤维的各种物理模型的旋转和平移扩散率的稀释值之间的关系。在这项工作中研究的浓度范围为nL〜3approx = 0-150的数密度。通过对长径比(纤维长度对直径)为25,50的棒进行模拟,研究了纤维厚度的影响。 d 500,以及对无限细的纤维进行投影。通过使用短距离电势来增强棒的排除体积。对于长宽比为50且参数为L〜2D_R_0 / D_T_0 = 9的棒对应于单个纤维的细长体模型,在70 <= nL〜3 <= 150的浓度范围内,旋转扩散系数(D_R)缩放为D_R / D_R_0〜(nL〜3)〜(-1.9)类似地,在参数L2D_R / D_T_0 = 4的情况下,对应于刚性哑铃模型,在相同的浓度范围内旋转扩散系数的范围为D_RID〜_R_0〜(nL〜3)〜(-1.1)。比率为25,观察到L〜2D_R_0 / D_T_0 <= 8的缩放比例存在差异,该比率的较高值基本上表现出相同的缩放比例。对比率L〜2D_R_0 / D_T_0的其他值进行了研究确定相对于该参数的悬架动力学的整体行为。这些发现解决了模拟结果之间的差异。这是先前研究者报道的旋转扩散系数的研究,为悬浮在溶液中的刚性棒的扩散系数的精确理论的发展提供了新的见解。

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