...
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
【24h】

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:短时扩散率和长时间旋转扩散之间的关系

获取原文
获取原文并翻译 | 示例
           

摘要

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 (LDR0)-D-2/D-T0, where D-R0 is the rotational diffusivity at infinite dilution, D-T0 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(3)approximate to 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 (LDR0)-D-2/D-T0=9, which corresponds to a slender-body model of the individual fibers, the rotational diffusivity (D-R) scales as D-R/D(R0)similar to(nL(3))(-1.9) in the concentration regime of 70 <= nL(3)<= 150. Similarly with a parameter of (LDR0)-D-2/D-T0=4, corresponding to a rigid-dumbbell model, the rotational diffusivity scales as D-R/D(R0)similar to(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 (LDR0)-D-2/D(T0)less than or similar to 8, with higher values of this ratio exhibiting essentially the same scaling. Additional values of the ratio (LDR0)-D-2/D-T0 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. (C) 2005 American Institute of Physics.
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(LDR0)-D-2 / D-的敏感函数。 T0,其中D-R0是无限稀释时的旋转扩散率,D-T0是无限稀释时的平均质心扩散率,L是纤维长度。现有的硬质纤维在半稀释和集中状态下长期旋转扩散系数的理论无法准确地说明与用于模拟纤维的各种物理模型的旋转扩散和平移扩散系数的稀释值之间的关系。在这项工作中研究的浓度范围从nL(3)的数密度到0-150,这低于从各向同性向列相态的转变。通过对长径比(纤维长度对直径)为25、50和500的棒进行模拟,并对无限细的纤维进行投影,研究了纤维厚度的影响。棒的排除体积是通过使用短距离电势来实现的。对于长宽比为50且参数为(LDR0)-D-2 / D-T0 = 9的棒(对应于单个纤维的细长体模型),旋转扩散率(DR)随DR / D(R0)在(70 <= nL(3)<= 150)的浓度范围内类似于(nL(3))(-1.9)。与(LDR0)-D-2 / D-T0 = 4相似对应于刚性哑铃模型,在相同的浓度范围内,旋转扩散率的缩放比例类似于(nL(3))(-1.1)的DR / D(R0)。对于长宽比为25的棒,可以观察到(LDR0)-D-2 / D(T0)的缩放比例差异小于或类似于8,该比例的较高值显示出基本相同的缩放比例。研究了比率(LDR0)-D-2 / D-T0的其他值,以确定相对于该参数的悬架动力学的整体行为。这些发现解决了先前研究人员报告的旋转扩散率模拟结果之间的差异,并为悬浮在溶液中的刚性棒扩散率的精确理论的发展提供了新见解。 (C)2005美国物理研究所。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号