密集聚合物体系中链式扩散及其互锁的蒙特卡罗晶格模型与分子动力学模拟

K.R. Haire, T.J. Carver, A.H. Windle
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引用次数: 39

摘要

本文报道了聚合物链的蒙特卡罗晶格模型(立方F)的发展,该模型能够访问链的质心扩散是主要过程的时间,即使链的长度远远超过纠缠的长度。与单个分子的旋转体积相比,模型的体积较大。该模型结合了一种算法,该算法允许在链的各个部分上进行合作运动的可能性,并提高了仿真的时间效率。模型和修正算法都已针对已知的标度定律进行了测试。对于较短的链,该模型被“反向映射”为聚乙烯的完整原子细节,并使用分子动力学(MD)模拟了较短的时间过程。在相同的分子量和温度条件下,将MD模型与聚乙烯的实验扩散数据进行了对比,并对晶格模型进行了时间校准。因此,细粒度MD模型和粗粒度MC模型相互关联,以覆盖从MD的单个原子运动到微秒数量级的时间范围,即六个数量级的范围。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
A Monte Carlo lattice model for chain diffusion in dense polymer systems and its interlocking with molecular dynamics simulation

The paper reports the development of a Monte Carlo lattice model (cubic F) of polymer chains which is able to access times where the diffusion of the centre-of-mass of the chains is the dominant process, even though the chain lengths are well above that for entanglement. The volume of the model is large when compared with the volume of gyration of the individual molecules. The model incorporates an algorithm, which allows for the possibility of co-operative motions over sections of the chains and increases the time efficiency of the simulation. Both the model and the modifying algorithm have been tested against the known scaling laws.

The model, for shorter chains, is ‘reverse mapped’ into full atomic detail as polyethylene and the shorter time processes simulated using molecular dynamics (MD). The MD model is tested against experimental diffusion data for polyethylene, of the same molecular weight and at the same temperature, and then used to time-calibrate the lattice model.

Both the fine grained MD model and the coarse grained MC model are thus interlocked to cover a time range from the individual atomic motions of MD up to the order of a microsecond, a range of six orders of magnitude.

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