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平面上的纠缠动力学:使用多链分子动力学和单链滑链模型的研究。

Entanglement dynamics at flat surfaces: Investigations using multi-chain molecular dynamics and a single-chain slip-spring model.

机构信息

School of Mathematical, Physical and Computational Sciences, University of Reading, Reading RG6 6AX, United Kingdom.

出版信息

J Chem Phys. 2019 Mar 7;150(9):094906. doi: 10.1063/1.5045301.

Abstract

The dynamics of an entangled polymer melt confined in a channel by parallel plates is investigated by Molecular Dynamics (MD) simulations of a detailed, multi-chain model. A primitive path analysis predicts that the density of entanglements remains approximately constant throughout the gap and drops to lower values only in the immediate vicinity of the surface. Based on these observations, we propose a coarse-grained, single-chain slip-spring model with a uniform density of slip-spring anchors and slip-links. The slip-spring model is compared to the Kremer-Grest MD bead-spring model via equilibrium correlation functions of chain orientations. Reasonably good agreement between the single-chain model and the detailed multi-chain model is obtained for chain relaxation dynamics, both away from the surface and for chains whose center of mass positions are at a distance from the surface that is less than the bulk chain radius of gyration, without introducing any additional model parameters. Our results suggest that there is no considerable drop in topological interactions for chains in the vicinity of a single flat surface. We infer from the slip-spring model that the experimental plateau modulus of a confined polymer melt may be different to a corresponding unconfined system even if there is no drop in topological interactions for the confined case.

摘要

通过对详细的多链模型进行分子动力学 (MD) 模拟,研究了平行板约束下的纠缠聚合物熔体的动力学。原始路径分析预测,缠结密度在整个间隙中基本保持不变,仅在靠近表面的附近区域才会下降到较低的值。基于这些观察,我们提出了一种粗粒化的单链滑链模型,该模型具有均匀密度的滑链锚和滑链。通过链取向的平衡相关函数,将滑链模型与 Kremer-Grest MD 珠链模型进行了比较。对于远离表面的链以及质心位置与表面距离小于链旋转半径的链的链松弛动力学,单链模型与详细的多链模型之间得到了相当好的一致性,而无需引入任何额外的模型参数。我们的结果表明,对于单个平面附近的链,拓扑相互作用没有明显下降。我们从滑链模型推断,即使对于受限情况,拓扑相互作用没有下降,受限聚合物熔体的实验平台模量也可能与相应的无约束系统不同。

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