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Depletion interactions produced by nonadsorbing charged and uncharged spheroids

机译:由不吸附的带电和不带电球体产生的耗尽相互作用

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The effect of macromolecule shape on the depletion attraction between two hard spherical particles in a solution with nonadsorbing hard spheroidal macromolecules of arbitrary size and aspect ratio was investigated using a modified form of the force-balance model of J. Y. Walz and A. Sharma (1994, J. Colloid Interface Sci. 168, 495). The macromolecules were represented as general spheroids, which could be either charged or uncharged. For the uncharged case, a set of analytical expressions describing the depletion attraction, valid for particles much larger than the characteristic macromolecule size, was developed. Comparisons with the case of spherical macromolecules were made under the condition of either constant macromolecule number density, rho (b), Or constant volume fraction, phi. It was found that increasing the spheroidal macromolecule aspect ratio (major axis length/minor axis length) decreases the depletion attraction at constant rho (b), but increases the interaction at constant phi. In the latter case, the interaction produced by prolate macromolecules is greater than that produced by oblate macromolecules of equal axis lengths, while the opposite is true at constant rho (b) A simple scaling analysis is used to explain these trends. Surface charge is found to increase both the range and the magnitude of the depletion attraction; however, the general trends are the same as those found in the uncharged systems. Finally, the effect of the depletion attraction produced by spherical and spheroidal macromolecules on the stability of a dispersion of charged particles was examined. It was found that charged spheroids at concentrations of order 1% volume can produce secondary energy wells of sufficient magnitude to induce flocculation in a dispersion of charged spherical particles. (C) 2000 Academic Press. [References: 62]
机译:使用JY Walz和A.Sharma(1994, J.Colloid Interface Sci.168,495)。大分子表示为一般球体,可以带电或不带电。对于不带电的情况,开发了一组描述耗尽吸引力的解析表达式,适用于远大于特征高分子尺寸的颗粒。在恒定的大分子数密度rho(b)或恒定的体积分数phi的条件下,与球形大分子进行了比较。已发现,增加球形大分子的长径比(长轴长度/短轴长度)会减小在常数rh(b)下的耗尽吸引,但会增加在常数phi下的相互作用。在后一种情况下,扁长形大分子所产生的相互作用大于等轴长的扁长形大分子所产生的相互作用,而在常数rho下则相反。(b)使用简单的比例分析来解释这些趋势。发现表面电荷会增加耗尽引力的范围和大小。但是,总体趋势与未收费系统中的趋势相同。最后,研究了球形和球形大分子产生的耗尽吸引对带电粒子分散体稳定性的影响。已经发现,带电球状体的浓度约为1%(体积),可以产生足够数量的次级能量阱,从而在带电球形颗粒的分散体中引起絮凝。 (C)2000学术出版社。 [参考:62]

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