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Study of nonlinear electrophoresis

机译:非线性电泳研究

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We distinguish two kinds of nonlinear electrophoresis that can be observed in strong electric fields. The first is due to the interaction of the applied field E with the field-induced ionic charges, under conditions when the field-induced variation of the electrolyte concentration remains small compared to its equilibrium value. The second one ("superfast electrophoresis") is related to the interaction of a strong applied field with a secondary diffuse layer of counterions ("space charge") which is induced by the external field outside the primary diffuse electrical double layer because of the concentration polarization. In the first case, with increasing field strength, the processes that are nonlinear with respect to E start playing a more important role that can be characterized by the third power term in the expansion of the electrophoretic velocity in powers of E. An expression is derived for "cubic electrophoresis" of spherical particles with a thin double layer, using the procedure of successive approximation in powers of small- parameter E. In line with the theory at E = 100 V/cm and higher substantial nonlinear effects in the electrophoretic velocity of polystyrene latex and aluminum oxide particles as well as yeast cells were observed. In the second case, the interaction of the "space charge" that is formed near the surface of electron-type conducting particles like magnesium or semiconductors like pyrite and molybdenite with a strong electric field (100-500 V/cm) produces electrophoretic velocities that are 1-2 orders of magnitude higher compared with those typical for nonconducting particles. It has been shown that the mobility of particles increases linearly with E and the particle size, in contrast to classical electrophoresis. This can be explained by the Dukhin-Mishchuk theory of superfast electrophoresis. A new method for measuring electrophoresis in strong electric fields has been developed.
机译:我们区分了两种在强电场中可以观察到的非线性电泳。首先是由于在电场引起的电解质浓度变化与其平衡值相比仍较小的情况下,施加的电场E与电场感应的离子电荷的相互作用。第二个(“超快电泳”)与强外加电场与抗衡离子的次级扩散层(“空间电荷”)的相互作用有关,该次级扩散层由初级扩散双电层外部的外场由于浓度而引起偏振。在第一种情况下,随着场强的增加,相对于E而言非线性的过程开始扮演更重要的角色,其特征可以是E的电泳速度的扩展中的第三幂项。对于具有薄双层的球形颗粒的“立方电泳”,使用小参数E的幂的逐次逼近过程。符合E = 100 V / cm时的理论和较高的电泳速度非线性效应观察到聚苯乙烯胶乳和氧化铝颗粒以及酵母细胞。在第二种情况下,在具有强电场(100-500 V / cm)的电子型导电颗粒(如镁)或半导体(如黄铁矿和辉钼矿)的表面附近形成的“空间电荷”的相互作用产生了电泳速度,与非导电粒子的典型值相比,高出1-2个数量级。已经证明,与经典电泳相反,粒子的迁移率随E和粒子尺寸线性增加。这可以通过Dukhin-Mishchuk超快速电泳理论来解释。已经开发出一种在强电场中测量电泳的新方法。

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