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首页> 外文期刊>Macromolecules >Hierarchical multiscale modeling of polymer-solid interfaces: Atomistic to coarse-grained description and structural and conformational properties of polystyrene-gold systems
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Hierarchical multiscale modeling of polymer-solid interfaces: Atomistic to coarse-grained description and structural and conformational properties of polystyrene-gold systems

机译:聚合物-固体界面的分层多尺度建模:原子到粗粒度描述以及聚苯乙烯-金系统的结构和构象性质

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摘要

A hierarchical simulation approach was developed in order to study polystyrene films sandwiched between two parallel Au(111) surfaces. The coarse-grained potentials describing the interaction of polystyrene with the gold surface were developed systematically using constrained all-atom molecular simulations of a styrene trimer on the Au(111) surface. The model was validated by studying a 5 nm film of short (10-mer) atactic polystyrene chains using all-atom and coarse-grained molecular dynamics simulations. The density, structure, and conformational properties of coarse-grained films were found to be in excellent agreement with all-atom ones. The coarse-grained model was then used to study the structural and conformational properties of roughly 10 and 20 nm thick films with 10-, 50-, 100-, and 200-mer chains. The width of the interphase region of the polymer films is property specific. The density profiles reached the bulk value around 1.5 nm from the interface, for all chain lengths. An estimate of the width of the interphase region based on the conformation tensor profile indicates that the interphase width is around 2-3 times the radius of gyration, which is proportional to the square root of the chain length (number of monomers), and for 200-mer chains is approximately 6-10 nm.
机译:为了研究夹在两个平行Au(111)表面之间的聚苯乙烯薄膜,开发了一种分层模拟方法。使用Au(111)表面上的苯乙烯三聚体的受限​​全原子分子模拟,系统地开发了描述聚苯乙烯与金表面相互作用的粗粒度电势。通过使用全原子和粗粒度的分子动力学模拟研究短(10-mer)无规聚苯乙烯链的5 nm薄膜来验证该模型。发现粗颗粒薄膜的密度,结构和构象性质与全原子薄膜具有极好的一致性。然后,使用粗颗粒模型研究具有10个,50个,100个和200个单体链的约10和20 nm厚膜的结构和构象性质。聚合物膜的相间区域的宽度是特性特定的。对于所有链长,密度分布均在距界面约1.5 nm处达到体积值。根据构象张量分布对相间区域的宽度进行估算,表明相间宽度约为回转半径的2-3倍,该半径与链长的平方根(单体数)成正比,对于200-mer链约为6-10 nm。

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