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各向异性层状微乳液的截断随机波分析

Clipped random wave analysis of anisometric lamellar microemulsions.

作者信息

Choy D, Chen S H

机构信息

Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2001 Feb;63(2 Pt 1):021401. doi: 10.1103/PhysRevE.63.021401. Epub 2001 Jan 10.

DOI:10.1103/PhysRevE.63.021401
PMID:11308486
Abstract

Small-angle neutron scattering experiments were performed on C10E4-D2O-octane (where C10E4 is tetraethylene glycol monodecyl ether) anisometric microemulsions in the lamellar phase at a constant surfactant volume fraction of 20% and at the hydrophile-lipophile balance temperature of 22.5 degrees C. The results were analyzed using a clipped random wave model with a specific spectral distribution function developed by us previously. This enabled us to generate three-dimensional morphologies of the microemulsions, which showed clearly that in sufficiently anisometric microemulsions the oil-water interface was no longer connected. At large anisometry isolated regions of oil or water were found, and the transition from a bicontinuous structure at isometry to these isolated micelles far from isometry goes through an intermediate cylindrical morphology when the oil-to-water or water-to-oil ratio is around 4 to 1. We further computed the joint distribution function of the mean curvature H and Gaussian curvature K of the entire oil-water interface for each anisometric microemulsion. In particular, we show the distribution of , , and

-(2) for different isolated regions within an oil-rich microemulsion at an oil-to-water ratio of 85% to 15%. These distributions allowed us to prove that the isolated regions formed in highly anisometric microemulsions were small and had spherical topology.

摘要

在层状相中,于20%的恒定表面活性剂体积分数以及22.5摄氏度的亲水亲油平衡温度下,对C10E4-D2O-辛烷(其中C10E4是四乙二醇单癸醚)各向异性微乳液进行了小角中子散射实验。使用我们之前开发的具有特定光谱分布函数的截断随机波模型对结果进行了分析。这使我们能够生成微乳液的三维形态,结果清楚地表明,在足够各向异性的微乳液中,油水界面不再相连。在大的各向异性情况下,发现了油或水的孤立区域,并且当油与水或水与油的比例约为4比1时,从等轴状态下的双连续结构到远离等轴状态的这些孤立胶束的转变会经历中间的圆柱形形态。我们进一步计算了每个各向异性微乳液整个油水界面的平均曲率H和高斯曲率K的联合分布函数。特别是,我们展示了在油与水比例为85%至15%的富油微乳液中不同孤立区域的、和

-(2)的分布。这些分布使我们能够证明在高度各向异性微乳液中形成的孤立区域很小且具有球形拓扑结构。

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