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首页> 外文期刊>Colloids and Surfaces, A. Physicochemical and Engineering Aspects >The determination of hydrodynamic size and zeta potential from electrophoretic mobility and light scattering measurements
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The determination of hydrodynamic size and zeta potential from electrophoretic mobility and light scattering measurements

机译:通过电泳迁移率和光散射测量确定流体力学尺寸和Zeta电位

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摘要

Colloidal particle diffusivities are usually measured by light scattering and zeta-potentials determined from electrophoretic mobilities. A hydrodynamic size can be calculated from the diffusivity by use of the Stokes-Einstein equation, although this ignores the influence of the surface charge and the ion cloud surrounding each particle. Similarly, zeta-potentials are often calculated from a radius determined by transmission electron microscopy or light scattering. In either case, a false picture emerges since the zeta-potential is defined as the potential at the electrokinetic shear surface. Here we show that a self-consistent picture emerges upon combining diffusivity and electrophoretic mobility measurements so as to include the effects of the diffuse layer in the hydrodynamic/electrokinetic particle size determination. The diffusivity and electrophoretic mobility of an anionic polystyrene latex were measured over a range of salt strengths. When diffuse layer effects were ignored, the particle diameter decreased monotonically from 180 nm to 158 mm as the salt concentration increased from (approximately) 10 mu M to 10 mM. When diffuse layer effects were incorporated into the analysis by simultaneously calculating the particle size and charge, the ionic strength dependence weakened. Above an ionic strength of 10(-4) M, the size varied by less than 1% and exceeded the dry size (from transmission electron microscopy) by about 4%. Although making use of the two experimental parameters has a significant impact on the calculated size, the effect on zeta-potentials is small. Some evidence of a fuzzy layer was present at ionic strengths below 10(-4) M since the particle size increased with diminishing ionic strength. (C) 1998 Elsevier Science B.V. [References: 8]
机译:胶体粒子的扩散率通常通过光散射和由电泳迁移率确定的ζ电位来测量。虽然可以忽略表面电荷和围绕每个粒子的离子云的影响,但可以使用Stokes-Einstein方程从扩散率计算出流体力学尺寸。类似地,ζ电势通常由透射电子显微镜或光散射确定的半径来计算。在这两种情况下,由于zeta电位都被定义为电动剪切表面的电位,因此出现了错误的图像。在这里,我们显示了在结合扩散率和电泳迁移率测量结果时出现了一个自洽的图像,以便在流体动力学/电动粒度确定中包括扩散层的影响。在一定盐浓度范围内测量了阴离子型聚苯乙烯胶乳的扩散率和电泳迁移率。当忽略扩散层效应时,随着盐浓度从(大约)10μM增加到10 mM,粒径从180 nm单调减小到158 mm。当通过同时计算粒径和电荷将扩散层效应纳入分析时,离子强度依赖性减弱。离子强度超过10(-4)M时,尺寸变化小于1%,超过干尺寸(根据透射电子显微镜)约4%。尽管使用这两个实验参数对计算的大小有显着影响,但对ζ电势的影响很小。在离子强度低于10(-4)M时,存在一些模糊层的证据,因为随着离子强度的减小,粒径增大。 (C)1998 Elsevier Science B.V. [参考:8]

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