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偶极硬球胶体中的有序排列和短时间取向扩散

Ordering and short-time orientational diffusion in dipolar hard-spherical colloids.

作者信息

Alarcón-Waess O, Diaz-Herrera E

机构信息

Departamento de Física y Matemáticas, UDLA, Puebla, Santa Catarina Martir, Cholula 72820 Puebla, Mexico.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2002 Mar;65(3 Pt 1):031402. doi: 10.1103/PhysRevE.65.031402. Epub 2002 Feb 11.

DOI:10.1103/PhysRevE.65.031402
PMID:11909052
Abstract

Orientational hydrodynamic functions and short-time, self-orientational and collective orientational diffusion coefficients of dipolar hard-spherical colloids are performed on a homogeneous isotropic phase, as functions of the wave vector q, for various values of the volume fraction and the dipolar strength of the macroparticles. The calculation is based on the dynamic orientational structure factor, which is the time-dependent self-correlation of the orientation density. We assume that the time evolution of the orientation density is given by the Smoluchoswki's equation, taking into account the hydrodynamic interactions as well as the dipolar interaction. The former are considered assuming pairwise additivity. The importance of the dynamic orientational structure factor is that its initial slope can be measured in a depolarized light scattering experiment. The results predict a different behavior for dilute and for dense dipolar colloids. The ordering phenomena are studied via the ordering coefficients, which are the orientational hydrodynamic functions at q=0. The results show that as the dipolar colloid evolves to the instability line, the translational ordering velocity increases while the rotational one reduces. The short-time orientational diffusion coefficients at q=0 are also performed. They predict that near to the instability line, the dipolar colloid diffuses translationally more than rotationally. At very dilute concentration the dipolar colloid presents an unexpected dynamical behavior, which seems to indicate that the colloid could be evolving to a reentrant phase.

摘要

针对具有偶极作用的硬球胶体,在均匀各向同性相中,研究了其取向流体动力学函数以及短时间的自取向和集体取向扩散系数,这些都是波矢q的函数,同时考虑了不同的体积分数和大颗粒的偶极强度。计算基于动态取向结构因子,它是取向密度随时间变化的自相关函数。我们假设取向密度的时间演化由斯莫卢霍夫斯基方程给出,其中考虑了流体动力学相互作用以及偶极相互作用。前者通过成对加和性来考虑。动态取向结构因子的重要性在于其初始斜率可以在去偏振光散射实验中测量。结果预测了稀溶液和浓溶液中偶极胶体的不同行为。通过有序系数研究有序现象,有序系数是q = 0时的取向流体动力学函数。结果表明,随着偶极胶体向不稳定线演化,平移有序速度增加而旋转有序速度降低。还计算了q = 0时的短时间取向扩散系数。结果预测,在接近不稳定线时,偶极胶体的平移扩散比旋转扩散更显著。在非常稀溶液浓度下,偶极胶体呈现出意想不到的动力学行为,这似乎表明胶体可能正在演变为再入相。

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