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Individual Molecular Dynamics of an Entangled Polyethylene Melt Undergoing Steady Shear Flow: Steady-State and Transient Dynamics

机译:稳态剪切流下纠缠聚乙烯熔体的单个分子动力学:稳态和瞬态动力学

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摘要

The startup and steady shear flow properties of an entangled, monodisperse polyethylene liquid (C1000H2002) were investigated via virtual experimentation using nonequilibrium molecular dynamics. The simulations revealed a multifaceted dynamical response of the liquid to the imposed flow field in which entanglement loss leading to individual molecular rotation plays a dominant role in dictating the bulk rheological response at intermediate and high shear rates. Under steady shear conditions, four regimes of flow behavior were evident. In the linear viscoelastic regime (γ˙<τd1), orientation of the reptation tube network dictates the rheological response. Within the second regime (τd1<γ˙<τR1), the tube segments begin to stretch mildly and the molecular entanglement network begins to relax as flow strength increases; however, the dominant relaxation mechanism in this region remains the orientation of the tube segments. In the third regime (τR1<γ˙<τe1), molecular disentangling accelerates and tube stretching dominates the response. Additionally, the rotation of molecules become a significant source of the overall dynamic response. In the fourth regime (γ˙>τe1), the entanglement network deteriorates such that some molecules become almost completely unraveled, and molecular tumbling becomes the dominant relaxation mechanism. The comparison of transient shear viscosity, η+, with the dynamic responses of key variables of the tube model, including the tube segmental orientation, S, and tube stretch, λ, revealed that the stress overshoot and undershoot in steady shear flow of entangled liquids are essentially originated and dynamically controlled by the Sxy component of the tube orientation tensor, rather than the tube stretch, over a wide range of flow strengths.
机译:通过使用非平衡分子动力学的虚拟实验,研究了纠缠的单分散聚乙烯液体(C1000H2002)的启动和稳态剪切流动特性。模拟揭示了液体对施加流场的多方面动力学响应,其中导致单个分子旋转的缠结损失在决定中等和高剪切速率下的总体流变响应中起着主导作用。在稳定剪切条件下,明显表现出四种流动特性。在线性粘弹性状态下(<数学xmlns:mml =“ http://www.w3.org/1998/Math/MathML” id =“ mm1”溢出=“ scroll”> γ ˙ / mo> τ d 1 ),the管网络的方向决定了流变反应。在第二种机制内( τ d 1 / mo> < mover accent =“ true”> γ ˙ / mo> τ R 1 ),管段开始温和拉伸,随着流动强度的增加,分子缠结网络开始松弛。但是,该区域的主要松弛机制仍然是管段的方向。在第三种情况下( τ R 1 / mo> < mover accent =“ true”> γ ˙ / mo> τ e 1 ),分子解缠加速并加速伸展主导着反应。另外,分子的旋转成为整个动态响应的重要来源。在第四种情况下( γ ˙ τ e 1 ),纠缠网络恶化,使得某些分子变成几乎完全解开,分子翻滚成为主要的松弛机制。瞬时剪切粘度的比较 η + ,具有管模型关键变量的动态响应,包括管分段方向, S 和管拉伸, λ 揭示,纠缠液体的稳定剪切流中的应力上冲和下冲本质上是由 S x 在广泛的流动强度范围内,管取向张量的y 分量而不是管拉伸量。

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