Fluctuating Junctions of Physically Cross-Linked Networks in a Single-Chain Model. – Consistency Between the Relaxation Modulus for Small Deformations and Green-Kubo Predictions

T. Indei
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Abstract

In theoretical attempts of predicting the viscoelastic behavior of polymer networks, such as chemical gels of rubbers, physical gels of associating polymers, and entangled polymer melts, the affine assumption is often employed to describe the junction (or node) motion of the networks under flows or deformations. That is, the motion of the junctions is assumed to obey the same deformation tensor as that used for the macroscopic deformation applied to the network surface. While the affine assumption captures the essential feature of the node dynamics somehow on average, neglect of the spatial (and temporal) fluctuations of junctions around the affine motion gives rise to several fundamental problems. One example is an overestimation of the plateau modulus for a given network topology when the affine assumption is employed. Also the viscoelastic relaxation spectrum depends on the extent of junction fluctuations. One way to implement the junction fluctuation into the theoretical model is to introduce the virtual spring that connects a point of the chain, which is supposed to be a member of a network junction, and the background field that is assumed to deform affinely. However, in singlechain models of polymer networks, the inclusion of the virtual spring brings about several fundamental problems. There have been some arguments about whether to include explicitly the stress σv originating from the virtual springs into the expression of the total stress σ of the network. Likhtman neglected σv in his slip-spring model for entangled polymer melts and assumed that the total stress σ is given by the stress from the chain σc alone because otherwise the contribution from the virtual springs is double counted. On the other hand, as Ramírez et al. noticed, the neglect of σv leads to a disagreement between the dynamic modulus of the chain part Gc(t ) obtained by applying a small external deformation to the network and that obtained from the Green-Kubo (GK) formula of the linear response theory Fluctuating Junctions of Physically Cross-Linked Networks in a Single-Chain Model. – Consistency Between the Relaxation Modulus for Small Deformations and Green-Kubo Predictions
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单链模型中物理交联网络的波动结点。-小变形松弛模量与Green-Kubo预测之间的一致性
在预测聚合物网络的粘弹性行为的理论尝试中,如橡胶的化学凝胶、缔合聚合物的物理凝胶和纠缠的聚合物熔体,仿射假设经常被用来描述网络在流动或变形下的结(或节点)运动。也就是说,假设结点的运动遵循与施加于网络表面的宏观变形相同的变形张量。虽然仿射假设在某种程度上平均捕获了节点动力学的基本特征,但忽略了围绕仿射运动的节点的空间(和时间)波动,导致了几个基本问题。一个例子是当采用仿射假设时,对给定网络拓扑的平台模量的高估。粘弹性松弛谱也取决于结起伏的程度。在理论模型中实现节点波动的一种方法是引入虚拟弹簧,该弹簧连接链的一个点,假设它是网络节点的成员,并假设背景场是仿射变形的。然而,在聚合物网络的单链模型中,包含虚拟弹簧会带来几个基本问题。在网络总应力σ表达式中是否应显式地包含虚拟弹簧的应力σv,一直存在争议。Likhtman在他的缠结聚合物熔体的滑移弹簧模型中忽略了σv,并假设总应力σ仅由来自链σc的应力给出,否则虚拟弹簧的贡献将被重复计算。另一方面,如Ramírez等人注意到的,忽略σv会导致通过对网络施加小的外部变形得到的链部分的动态模量Gc(t)与单链模型中物理交联网络的线性响应理论波动结Green-Kubo (GK)公式得到的动态模量不一致。-小变形松弛模量与Green-Kubo预测之间的一致性
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