表面活性剂胶束对浓乳胶悬浮液的耗竭絮凝作用

M.K. Packman, Th.F. Tadros
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引用次数: 7

摘要

研究了加入高浓度非离子表面活性剂对体积分数φp = 0.4的聚苯乙烯乳液悬浮液流变性能的影响。使用了四种不同的表面活性剂,它们含有相同的疏水性基团(C9H19C6H5(CH2CH(CH3)O)13)和越来越大的亲水链(聚环氧乙烷),分别含有27、48、79和174个环氧乙烷(EO)单元)。采用稳态剪切应力(τ) -剪切速率(γ)测量以及振荡测量来研究流变学。由τ -γ曲线可以推断出屈服应力τβ和塑性粘度ηpl随表面活性剂浓度的变化规律。通过振荡测量,得到了不同表面活性剂浓度下复合模量G*、存储模量G '和损耗模量G″随频率的变化规律。所有结果表明,当表面活性剂浓度达到临界浓度时,随表面活性剂浓度的增加,流变性参数迅速增加。这种快速增长(非牛顿流)被认为是由于耗竭絮凝。后者被认为是在表面活性剂浓度超过表面活性剂胶束最大随机堆积所需的浓度时发生的,表面活性剂胶束被假设为球形。一个简单的计算(随机填充时使用0.63的值)利用胶束中表面活性剂分子的聚集数(从表面张力或光散射测量中获得)预测了絮凝开始时表面活性剂的浓度。用外推的屈服值计算了絮凝体中接触点之间的分离能量。将Esep与使用Asakura和Oosawa理论计算的耗尽吸引gdeep的理论自由能进行了比较。gdeep计算值与Esep实验值吻合较好。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Depletion flocculation of concentrated latex suspensions by surfactant micelles

The influence of addition of a high concentration of non-ionic surfactants on the rheology of a concentrated (volume fraction φp = 0.4) polystyrene latex suspension was investigated. Four different surfactants containing the same hydrophobic group (C9H19C6H5(CH2CH(CH3)O)13) and increasingly large hydrophilic chains (poly(ethylene oxide) with 27, 48, 79 and 174 ethylene oxide (EO) units) were used. The rheology was studied using steady-state shear stress (τ)—shear rate (γ) measurements as well as oscillatory measurements. From the τ—γ curves, the extrapolated yield stress τβ and plastic viscosity ηpl were obtained as a function of surfactant concentration. From oscillatory measurements, the complex modulus G*, the storage modulus G′ and loss modulus G″ were obtained as a function of frequency at different surfactant concentrations. All results showed a rapid increase in the rheological parameters with increase of surfactant concentration, once the latter reached a critical concentration. This rapid increase (non-Newtonian flow) was considered to be due to depletion flocculation. The latter was thought to occur at a surfactant concentration in excess of that required for maximum random packing of surfactant micelles, which were assumed to be spherical. A simple calculation (using a value of 0.63 for random packing) predicted the surfactant concentration at the onset of depletion flocculation, using the aggregation number of surfactant molecules in the micelle (obtained from surface-tension or light-scattering measurements).

The extrapolated yield value was used to calculate the energy of separation Esep between contact points in a floc. Esep was compared with the theoretical free energy of depletion attraction Gdep that was calculated using the Asakura and Oosawa theory. Agreement between the calculated Gdep and experimental Esep values was fair.

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