Department of Materials Science and Department of Chemistry, University of Illinois, 1304 West Green Street, Urbana, Illinois 61801, USA.
Department of Physics, Syracuse University, Syracuse, New York 13244, USA.
J Chem Phys. 2016 Dec 7;145(21):214903. doi: 10.1063/1.4968516.
We employ a first-principles-based, force-level approach to construct the anharmonic tube confinement field for entangled fluids of rigid needles, and also for chains described at the primitive-path (PP) level in two limiting situations where chain stretch is assumed to either be completely equilibrated or unrelaxed. The influence of shear and extensional deformation and polymer orientation is determined in a nonlinear elastic limit where dissipative relaxation processes are intentionally neglected. For needles and PP-level chains, a self-consistent analysis of transverse polymer harmonic dynamical fluctuations predicts that deformation-induced orientation leads to tube weakening or widening. In contrast, for deformed polymers in which chain stretch does not relax, we find tube strengthening or compression. For all three systems, a finite maximum transverse entanglement force localizing the polymers in effective tubes is predicted. The conditions when this entanglement force can be overcome by an externally applied force associated with macroscopic deformation can be crisply defined in the nonlinear elastic limit, and the possibility of a "microscopic absolute yielding" event destroying the tube confinement can be analyzed. For needles and contour-relaxed PP chains, this force imbalance occurs at a stress of order the equilibrium shear modulus and a strain of order unity, corresponding to a mechanically fragile entanglement tube field. However, for unrelaxed stretched chains, tube compression stabilizes transverse polymer confinement, and there appears to be no force imbalance. These results collectively suggest that the crossover from elastic to irreversible viscous response requires chain retraction to initiate disentanglement. We qualitatively discuss comparisons with existing phenomenological models for nonlinear startup shear, step strain, and creep rheology experiments.
我们采用基于第一性原理的力场方法构建了刚性针状分子纠缠流体以及原始路径(PP)水平下链的非谐管限制场,在两种极限情况下对链拉伸进行了完全平衡或未松弛的假设。在有意忽略耗散松弛过程的非线性弹性极限下,确定了剪切和拉伸变形以及聚合物取向的影响。对于针状分子和 PP 水平的链,横向聚合物谐动态波动的自洽分析表明,变形诱导的取向导致管弱化或变宽。相比之下,对于链拉伸不松弛的变形聚合物,我们发现管增强或压缩。对于所有三种系统,都预测存在一个有限的最大横向缠结力,将聚合物限制在有效的管中。在非线性弹性极限下,可以清晰地定义克服与宏观变形相关的外部施加力的这种缠结力的条件,并且可以分析破坏管限制的“微观绝对屈服”事件的可能性。对于针状分子和轮廓松弛的 PP 链,这种力不平衡发生在平衡剪切模量量级的应力和量级为 1 的应变下,对应于机械脆弱的缠结管场。然而,对于未松弛的拉伸链,管压缩稳定了横向聚合物的限制,似乎没有力不平衡。这些结果共同表明,从弹性到不可逆粘性响应的转变需要链回缩来引发解缠。我们定性地讨论了与现有的非线性启动剪切、阶跃应变和蠕变流变实验的经验模型的比较。