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具有不同分子结构的柔性聚电解质周围的抗衡离子分布。

Counter-ion distribution around flexible polyelectrolytes having different molecular architecture.

作者信息

Chremos Alexandros, Douglas Jack F

机构信息

Materials Science and Engineering Division, National Institute of Standards and Technology, Gaithersburg, MD 20899, USA.

出版信息

Soft Matter. 2016 Mar 21;12(11):2932-41. doi: 10.1039/c5sm02873f.

Abstract

We explore the monovalent counter-ion distribution around flexible highly-charged polyelectrolytes with different molecular architectures (linear chains, stars, and unknotted and trefoil rings) using molecular dynamics simulations that include an explicit solvent that interacts with the polyelectrolyte. In particular, we find that the molecular topology influences the fraction of counter-ions transiently associating with the polyelectrolyte on a scale of the order of the chain segments, forming a "condensed" counter-ion interfacial layer. As with the hydrogen bonding of water to proteins and other polymers, the persistence time of these interfacial "bound" counter-ions is relatively short, O(1 ps), and we characterize the fluctuations in the number of the counter-ions populating the interfacial layer. We also find that the counter-ions are distributed in a non-uniform fashion on the polyelectrolyte backbone, forming dynamical clusters whose form and average size is sensitive to molecular architecture. In addition, we find that the residual bound counter-ions, not located in either the interfacial layer or the bulk solution, form a diffuse ionic cloud around the polyelectrolyte due to the uncompensated polyelectrolyte charge along the backbone. Generally charge valence strongly influences the extent of the diffuse counter-ion cloud, but in the case of monovalent counter-ions, we find that the size of the diffuse counter-ion cloud nearly coincides with the polyelectrolyte radius of gyration, independent of molecular topology.

摘要

我们使用分子动力学模拟来探索具有不同分子结构(线性链、星形以及无纽结和三叶结环)的柔性高电荷聚电解质周围的单价抗衡离子分布,该模拟包括与聚电解质相互作用的明确溶剂。特别地,我们发现分子拓扑结构在链段尺度上影响与聚电解质瞬时缔合的抗衡离子分数,形成一个“凝聚”的抗衡离子界面层。与水与蛋白质及其他聚合物的氢键作用类似,这些界面“结合”抗衡离子的持续时间相对较短,为O(1皮秒),并且我们对填充在界面层中的抗衡离子数量的波动进行了表征。我们还发现抗衡离子以非均匀方式分布在聚电解质主链上,形成动态簇,其形式和平均大小对分子结构敏感。此外,我们发现,由于沿主链未被补偿的聚电解质电荷,未位于界面层或本体溶液中的残余结合抗衡离子在聚电解质周围形成一个扩散离子云。一般来说,电荷价态强烈影响扩散抗衡离子云的范围,但对于单价抗衡离子,我们发现扩散抗衡离子云的大小几乎与聚电解质的回转半径一致,与分子拓扑结构无关。

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