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首页> 外文期刊>The Journal of Chemical Physics >Monte Carlo simulations of stress relaxation of entanglement-free Fraenkel chains. II. Nonlinear polymer viscoelasticity
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Monte Carlo simulations of stress relaxation of entanglement-free Fraenkel chains. II. Nonlinear polymer viscoelasticity

机译:无缠结的Fraenkel链应力松弛的蒙特卡洛模拟。二。非线性聚合物粘弹性

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The nonlinear viscoelastic behavior of the Fraenkel-chain model is studied with respect to the constitutive equation of the Rouse model. Distinctly different from the results of the Rouse model, the Fraenkel-chain model gives the following characteristic nonlinear behavior: (a) The two distinct dynamic modes in the relaxation modulus G(S)(t,lambda)-as observed in the linear region reported in Paper I [Y.-H. Lin and A. K. Das, J. Chem. Phys. 126, 074902 (2007), preceding paper]-or in the first normal-stress difference function G(Psi 1)(t,lambda) are shown to have different strain dependences: strain hardening for the fast mode and strain softening for the slow mode. (b) The Lodge-Meissner relation G(S)(t,lambda)=G(Psi 1)(t,lambda) holds over the whole time range, which has been shown both analytically and by simulation. (c) The second normal-stress difference is nonzero, being positive in the fast-mode region and negative in the slow-mode region. The comparisons between orientation and stress for all tensor components consistently confirm the strong correlation of the slow mode as well as its entropic nature with the segmental-orientation anisotropy as shown in the linear region studied in Paper I. A consequence of this correlation is the applicability of the stress-optical rule in the slow-mode region. This also leads to the expectation that the damping function h(lambda)=G(S)(t,lambda)/G(S)(t,lambda -> 0) and the ratio between the first and second normal-stress differences, N-2(t,lambda)/N-1(t,lambda), are described by the orientation tensor which has the same form as that given by Doi and Edwards [J. Chem. Soc. Faraday Trans. 2 74, 1789 (1978); 74, 1802 (1978)] with independent-alignment approximation for an entangled system. The similarity between the slow mode of an entanglement-free Fraenkel-chain system and the terminal mode of an entangled polymer system as observed in the comparison of theory, simulation, and experiment suggests that the close correlation of the entropic nature of the mode with the orientation anisotropy-as of the Fraenkel segment or the primitive step in the Doi-Edwards theory-is a generally valid physical concept in polymer viscoelasticity. (c) 2007 American Institute of Physics.
机译:针对Rouse模型的本构方程,研究了Fraenkel链模型的非线性粘弹性行为。与Rouse模型的结果截然不同,Fraenkel链模型具有以下特征非线性行为:(a)在线性区域中观察到的弛豫模量G(S)(t,lambda)中的两个不同的动态模式载于论文I [Y.-H. Lin和A.K. Das,J.Chem。物理126,074902(2007),先前的论文]-或在第一法向应力差函数G(Psi 1)(t,lambda)中显示出不同的应变依赖性:快速模式的应变硬化和慢速模式的应变软化模式。 (b)在整个时间范围内都保持了Lodge-Meissner关系G(S)(t,lambda)= G(Psi 1)(t,lambda),这已通过分析和仿真得到了证明。 (c)第二法向应力差不为零,在快速模式区域为正,在慢模式区域为负。所有张量分量的取向和应力之间的比较一致地证实了慢模及其熵性质与分段取向各向异性的强相关性,如论文I研究的线性区域所示。这种相关性的结果是适用性慢模区域中的应力-光学规则。这还导致期望阻尼函数h(lambda)= G(S)(t,lambda)/ G(S)(t,lambda-> 0)以及第一和第二法向应力差之间的比率, N-2(t,λ)/ N-1(t,λ)由取向张量描述,其取向与Doi和Edwards给出的形式相同。化学Soc。法拉第反式2 74,1789(1978); 74,1802(1978)]中描述了纠缠系统的独立对准近似。在理论,仿真和实验的比较中观察到,无缠结的Fraenkel链系统的慢模与缠结的聚合物系统的终模之间的相似性表明,该模的熵性质与聚合物的紧密关系密切相关。取向各向异性(例如弗兰克尔链段或Doi-Edwards理论中的原始步骤)是聚合物粘弹性中通常有效的物理概念。 (c)2007年美国物理研究所。

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