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首页> 外文期刊>The Journal of Chemical Physics >Electrophoretic properties of highly charged colloids: A hybrid molecular dynamics/lattice Boltzmann simulation study
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Electrophoretic properties of highly charged colloids: A hybrid molecular dynamics/lattice Boltzmann simulation study

机译:高电荷胶体的电泳性能:混合分子动力学/格子玻尔兹曼模拟研究

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Using computer simulations, the electrophoretic motion of a positively charged colloid (macroion) in an electrolyte solution is studied in the framework of the primitive model. In this model, the electrolyte is considered as a system of negatively and positively charged microions (counterions and coions, respectively) that are immersed into a structureless medium. Hydrodynamic interactions are fully taken into account by applying a hybrid simulation scheme, where the charged ions (i.e., macroion and electrolyte), propagated via molecular dynamics, are coupled to a lattice Boltzmann (LB) fluid. In a recent electrophoretic experiment by Martin-Molina et al. [J. Phys. Chem. B 106, 6881 (2002)], it was shown that, for multivalent salt ions, the mobility mu initially increases with charge density sigma, reaches a maximum, and then decreases with further increase of sigma. The aim of the present work is to elucidate the behavior of mu at high values of sigma. Even for the case of monovalent microions, a decrease of mu with sigma is found. A dynamic Stern layer is defined that includes all the counterions that move with the macroion while subjected to an external electrical field. The number of counterions in the Stern layer, q(0), is a crucial parameter for the behavior of mu at high values of sigma. In this case, the mobility mu depends primarily on the ratio q(0)/Q (with Q the valency of the macroion). The previous contention that the increase in the distortion of the electric double layer (EDL) with increasing sigma leads to the lowering of mu does not hold for high sigma. In fact, it is shown that the deformation of the EDL decreases with the increase of sigma. The role of hydrodynamic interactions is inferred from direct comparisons to Langevin simulations where the coupling to the LB fluid is switched off. Moreover, systems with divalent counterions are considered. In this case, at high values of sigma the phenomenon of charge inversion is found. (c) 2007 American Institute of Physics.
机译:使用计算机模拟,在原始模型的框架内研究了带正电的胶体(宏蛋白)在电解质溶液中的电泳运动。在此模型中,电解质被视为浸入无结构介质中的带负电和带正电的微离子(分别为抗衡离子和co离子)的系统。通过应用混合模拟方案充分考虑了流体动力学的相互作用,在该方案中,通过分子动力学传播的带电离子(即大分子离子和电解质)与晶格玻尔兹曼(LB)流体耦合。在Martin-Molina等人最近的电泳实验中。 [J.物理化学[B 106,6881(2002)]表明,对于多价盐离子,迁移率mu最初随电荷密度σ的增加而增加,达到最大值,然后随着σ的进一步增加而减小。本工作的目的是阐明在高sigma值下mu的行为。即使对于单价微米离子,也发现mu随sigma减小。定义了一个动态斯特恩层,其中包括在受到外部电场的作用下与大分子一起移动的所有抗衡离子。斯特恩层中抗衡离子的数量q(0)是mu在高sigma值下的行为的关键参数。在这种情况下,迁移率μ主要取决于比率q(0)/ Q(Q为大离子的化合价)。先前关于双电层(EDL)的畸变随sigma增大而增加导致mu降低的争论并不适用于高sigma。实际上,表明EDL的变形随着σ的增加而减小。从与LB流体的耦合断开的Langevin模拟的直接比较中可以推断出流体动力相互作用的作用。此外,考虑具有二价抗衡离子的系统。在这种情况下,在σ高的情况下,会发现电荷反转现象。 (c)2007年美国物理研究所。

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