两亲性二嵌共聚物溶液中囊泡形态发生的能量和熵动因

Senyuan Liu, Radhakrishna Sureshkumar
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摘要

本文采用粗粒度分子动力学模拟,研究了随机分布的两亲性二嵌段共聚物 PB-PEO(聚丁二烯-b-聚氧化乙烯)在水中自组装形成的囊泡(聚合体)的时空演变过程。泡化途径包括几种中间结构,如球形/杆状聚集体、蠕虫状胶束、薄片和空腔。薄片到囊泡的转变发生在聚集数不变的情况下,同时伴随着溶剂可接触表面积的减少。模拟预测结果与囊泡形成机制基本一致,在囊泡形成机制中,水分子与聚合物片段之间不利的疏水相互作用沿着薄片边缘被消除,但代价是获得曲率能。然而,杆状薄片到囊泡的转变伴随着共聚物堆积密度的增加。因此,模拟预测的伴随囊泡形成的表面积变化大大低于理论估计值。信息熵的变化(用节段伸展参数 s 的概率分布函数(定义为最大节段伸展与瞬时节段伸展之间的差值)的对数期望值量化)在统计上沿泡化路径并不显著。对于棒状体、片状体和聚合体,s 遵循对数正态分布。这可以根据单个二嵌段链在水中的构型动力学来解释。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Energetic and Entropic Motifs in Vesicle Morphogenesis in Amphiphilic Diblock Copolymer Solutions
Coarse-grained molecular dynamic simulations are employed to investigate the spatiotemporal evolution of vesicles (polymersomes) via self-assembly of randomly distributed amphiphilic diblock copolymers PB-PEO (Poly(Butadiene)-b-Poly(Ethylene Oxide)) in water. The vesiculation pathway consists of several intermediate structures, such as spherical/rodlike aggregates, wormlike micelles, lamellae, and cavities. The lamella-to-vesicle transition occurs at a constant aggregation number and is accompanied by a reduction in the solvent-accessible surface area. Simulation predictions are in qualitative agreement with the mechanism of vesicle formation in which the unfavorable hydrophobic interactions between water molecules and polymer segments, along the edge of the lamella, are eliminated at the expense of gaining curvature energy. However, rod–lamella–vesicle transition is accompanied by an increase in copolymer packing density. Hence, the change in the surface area accompanying vesiculation predicted by the simulations is significantly lower than theoretical estimates. Changes in information entropy, quantified by the expectation of the logarithm of the probability distribution function of the segmental stretch parameter s, defined as the difference between the maximum and instantaneous segmental extension, are statistically insignificant along the vesiculation pathway. For rods, lamellae, and polymersomes, s follows a log normal distribution. This is explained based on the configurational dynamics of a single diblock chain in water.
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