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Electrophoretic mobility of colloidal particles in salt-free media

机译:胶体颗粒在无盐介质中的电泳迁移率

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It is shown that the electrophoretic mobility μ of dilute spherical colloidal particles of radius a, carrying charge Q in a salt-free medium (containing only counteri-ons) is expressed generally as μ = Q_(eff)/D_H, irrespective of the particle type, where Q_(eff) is the effective particle charge and D_H is the drag coefficient of the particle. There is a certain critical value of Q separating two cases: the low-charge case and the high-charge case. In the low-charge case, Q_(eff) equals the real particle charge Q, while in the high-charge case, Q_(eff) becomes constant independent of Q. In the high-charge case, in which case counter-ion condensation occurs in the vicinity of the particle surface, there are two kinds of counterions: bound and free counterions. Bound counterions condensed at the particle surface do not contribute to the electrophoretic mobility so Q_(eff) and μ become constant independent of Q.
机译:结果表明,半径为a的稀球形胶体粒子在无盐介质(仅包含对数)中携带电荷Q的电泳迁移率μ通常表示为μ= Q_(eff)/ D_H,与粒子无关类型,其中Q_(eff)是有效粒子电荷,D_H是粒子的阻力系数。 Q的某个临界值将两种情况分开:低电量情况和高电量情况。在低电荷情况下,Q_(eff)等于实际粒子电荷Q,而在高电荷情况下,Q_(eff)变得独立于Q不变。在高电荷情况下,抗衡离子凝结发生在粒子表面附近的抗衡离子有两种:结合的和自由的抗衡离子。凝聚在粒子表面的抗衡离子对电泳迁移率没有贡献,因此Q_(eff)和μ变得独立于Q不变。

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