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Individual chain dynamics of a polyethylene melt undergoing steady shear flow

机译:经历稳定剪切流的聚乙烯熔体的单个链动力学

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Individual molecule dynamics have been shown to influence significantly the bulk rheological and microstructural properties of short-chain, unentangled, linear polyethylene liquids undergoing high strain-rate flows. The objective of this work was to extend this analysis to a linear polyethylene composed of macromolecules of a much greater length and entanglement density; i.e., a liquid consisting of C400H802 molecules, with approximately ten kinks per chain at equilibrium, as calculated by the Z1 code of Kroger [Comput. Phys. Commun. 168, 209-232 (2005)]. To achieve this, we performed nonequilibrium molecular dynamics (NEMD) simulations of a model system using the well-established potential model of Siepmann et al. [Nature 365, 330-332 (1993)] for a wide range of Weissenberg numbers (Wi) under steady shear flow. A recent study by Baig et al. [Macromolecules 43, 6886-6902 (2010)] examined this same system using NEMD simulations, but focused on the bulk rheological and microstructural properties as calculated from ensemble averages of the chains comprising the macromolecular liquids. In so doing, some key features of the system dynamics were not fully elucidated, which this article aims to highlight. Specifically, it was found that this polyethylene liquid displays multiple timescales associated with not only the decorrelation of the end-to-end vector (commonly related to the Rouse time or disengagement time, depending on the entanglement density of the liquid), but also ones associated with the retraction and rotation cycles of the individual molecules. Furthermore, when accounting for these individual chain dynamics, the "longest" relaxation time of the system was higher by a factor of 1.7, independent of shear rate, when calculated self-consistently due to the coupling of relaxation modes. Brownian dynamics (BD) simulations were also performed on an analogous free-draining bead-rod chain model to compare the rotation and retraction dynamics of a single chain in dilute solution with individual molecular motions in the melt. These BD simulations revealed that the dynamics of the free-draining chain are qualitatively and quantitatively similar to those of the individual chains comprising the polyethylene melt at strain rates in excess of Wi approximate to 50, implying a possible breakdown of reptation theory in the high shear limit. An examination of the bulk-average properties revealed the effects of the chain rotation and retraction cycles upon commonly modeled microstructural properties, such as the distribution function of the chain end-to-end vector and the entanglement number density. (C) 2015 The Society of Rheology.
机译:单个分子动力学已显示出显着影响经历高应变速率流动的短链,无缠结,线性聚乙烯液体的整体流变学和微观结构性质。这项工作的目的是将这种分析扩展到由更大长度和缠结密度的大分子组成的线性聚乙烯。即一种由C400H802分子组成的液体,平衡时每条链大约十个扭结,如Kroger的Z1代码所计算。物理公社168,209-232(2005)]。为了实现这一目标,我们使用Siepmann等人已建立的潜在模型对模型系统进行了非平衡分子动力学(NEMD)模拟。 [Nature 365,330-332(1993)]中的Weissenberg数(Wi)范围很广,在稳定剪切流作用下。 Baig等人的最新研究。 [Macromolecules 43,6886-6902(2010)]使用NEMD模拟检查了相同的系统,但重点研究了由组成高分子液体的链的总体平均值计算得到的整体流变学和微观结构性质。这样做时,系统动力学的一些关键功能尚未完全阐明,本文旨在强调这些功能。具体而言,发现该聚乙烯液体显示出多个时间尺度,不仅与端到端向量的去相关(通常与Rouse时间或脱离时间有关,取决于液体的缠结密度),而且还与时间相关。与单个分子的缩回和旋转周期有关。此外,当考虑到这些单独的链动力学时,由于松弛模式的耦合而进行自洽计算时,系统的“最长”松弛时间将增加1.7倍,与剪切速率无关。还对类似的自由排水珠-杆链模型进行了布朗动力学(BD)模拟,以比较稀溶液中单链的旋转和回缩动力学与熔体中的单个分子运动。这些BD模拟表明,在超过Wi约50的应变速率下,自由排水链的动力学在质量和数量上与包含聚乙烯熔体的单个链的动力学在质量和数量上相似,这意味着在高剪切力下蠕变理论可能会崩溃。限制。体积平均性质的检查揭示了链旋转和回缩循环对通常建模的微观结构性质的影响,例如链端对端向量的分布函数和缠结数密度。 (C)2015流变学学会。

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