AOT/盐水/角鲨烷“海绵”L3相的特征长度和曲率

Q3 Materials Science
Giuseppe Tartaro, Luigi Gentile, Gerardo Palazzo
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引用次数: 3

摘要

在25℃条件下,测定了盐度(NaCl浓度)对双(2-乙基己基)琥珀酸磺基钠(AOT)与等体积角鲨烷和盐水组成的体系的影响。在所有的NaCl浓度下,样品都是三相的,上层由纯角鲨烷组成,而盐水存在于另外两相中。当NaCl浓度低于1.6% w/v时,层状相和海绵相(L3)共存。当NaCl浓度大于1.6% w/v时,L3与纯盐水共存。用热重法测定了AOT双分子层中AOT的溶解量。当盐水中NaCl浓度高于2% w/v时,AOT海绵相收缩,排出盐水,双分子层中存在的角鲨烷变得可以忽略不计。用SAXS和扩散核磁共振进一步表征了L3相。在不含角鲨烷的情况下,水和AOT的自扩散系数与相同盐度下的自扩散系数基本一致。海绵相的SAXS曲线已拟合到一个方程,该方程考虑了双层结构和大尺度相互作用的贡献,从而可以确定平均孔间分离D *和双层相关长度ξ。相关长度被解释为反映连接双层的静态随机性,而不是反映动态热波动。考虑相关长度为沿双层表面沿临界角度变化(θ∗)的位移,在该临界角度变化(θ∗)之下,表面看起来是平坦的,允许定义曲率(H)为|H| =θ∗ξ。相关长度与双层体积分数的平方呈线性关系,这是由先前的理论模型提出的,假设海绵相在热力学上被限制为等于自发曲率的曲率。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Characteristic length and curvature of the AOT/brine/squalane “sponge” L3 phases

Characteristic length and curvature of the AOT/brine/squalane “sponge” L3 phases

The effect of salinity (NaCl concentration) was determined at 25 ​°C for systems composed of sodium bis(2-ethylhexyl) sulfosuccinate (AOT) and equal volumes of squalane and brine. At all the NaCl concentrations the samples are triphasic with an upper phase made of pure squalane while brine is present in two other phases. At NaCl concentration (in brine) below 1.6 %w/v there is the coexistence of lamellar and sponge (L3) phases. Loading with NaCl above 1.6 %w/v one observes the coexistence of L3 and pure brine. The amount of AOT dissolved in the AOT bilayer has been quantified by thermogravimetric analysis. At salinity above 2 %w/v of NaCl in brine, the AOT sponge phase shrinks expelling brine and the squalane whose presence in the bilayer becomes negligible. The L3 phases have been further characterized by SAXS and diffusion-NMR. The measured self-diffusion coefficients of water and AOT are essentially coincident with those measured at the same salinity in the absence of squalane. The SAXS curves of sponge phases have been fitted to a single equation accounting for the contributions of the bilayer structure and of the large-scale interactions allowing the determination of the average interpore separation D∗ and the bilayer correlation length ξ. The correlation length has been interpreted as reflecting static randomness of connected bilayer instead of the dynamic thermal undulations. Considering the correlation length as the displacement along the bilayer surface subtending a critical angular change (θ∗) below which the surface appears as flat, permits to define the curvature (H) as |H| =θξ. The correlation length scales linearly with the square of the bilayer volume fraction as proposed by a previous theoretical model assuming the sponge phases are thermodynamically constrained to a curvature that equals the spontaneous curvature.

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来源期刊
JCIS open
JCIS open Physical and Theoretical Chemistry, Colloid and Surface Chemistry, Surfaces, Coatings and Films
CiteScore
4.10
自引率
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审稿时长
36 days
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