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首页> 外文期刊>Journal of Colloid and Interface Science >Transient phoretic migration of a permselective colloidal particle
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Transient phoretic migration of a permselective colloidal particle

机译:选择性胶体粒子的瞬态电泳迁移

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摘要

We quantify the phoretic migration of a spherical cation-permselective colloidal particle immersed in a binary electrolyte under a time-dependent electric field. We invoke the thin-Debye-layer approximation, where the size of ionic Debye layer enveloping the particle is much smaller than the particle radius. The imposed electric field generates ion concentration gradients, or concentration polarization, in the bulk (electroneutral) electrolyte outside the Debye layer. The bulk ion concentration polarization-and consequently the particle's phoretic velocity-evolves on the time scale for ion diffusion around the particle, which can be on the order of milliseconds for typical colloidal dimensions. Notably, concentration polarization arises here solely due to the permselectivity of the particle; it does not require non-uniform ionic transport in the Debye layer (i.e., surface conduction). Thus, the phoretic transport of a permselective particle is significantly different to that of a inert, dielectric particle, since surface conduction is necessary to achieve bulk concentration polarization in the (more commonly studied) latter case. Calculations are presented for a permselective particle under oscillatory (ac) and suddenly applied electric fields. In the former case, the particle velocity possesses frequency-dependent components in phase and out of phase with the driving field; in the latter case, the particle approaches its terminal velocity with a long-time (algebraic) tail.
机译:我们量化了在时变电场下浸没在二元电解质中的球形阳离子选择性渗透胶体粒子的电泳迁移。我们调用薄Debye层近似,其中包围粒子的离子Debye层的大小比粒子半径小得多。施加的电场在德拜层外的整体(电中性)电解质中产生离子浓度梯度或浓度极化。整体离子浓度极化-因此粒子的电泳速度-随离子在粒子周围扩散的时间尺度而变化,对于典型的胶体尺寸,该时间尺度可以为毫秒量级。值得注意的是,此处的浓度极化仅是由于粒子的渗透选择性而产生的;它不需要在德拜层中进行不均匀的离子传输(即表面传导)。因此,选择性渗透粒子的电泳传输与惰性介电粒子的电泳传输明显不同,因为在后一种情况下(更普遍研究),表面传导对于实现体积浓度极化是必需的。给出了在振荡(ac)和突然施加的电场下的选择性渗透粒子的计算结果。在前一种情况下,质点速度具有与驱动场同相和异相的频率相关分量。在后一种情况下,粒子具有较长的(代数)尾巴接近其最终速度。

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