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玻璃态聚合物中银纹的生长、微观结构及破坏

Growth, microstructure, and failure of crazes in glassy polymers.

作者信息

Rottler Jörg, Robbins Mark O

机构信息

Department of Physics and Astronomy, The Johns Hopkins University, 3400 N. Charles Street, Baltimore, Maryland 21218, USA. Joerg@

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2003 Jul;68(1 Pt 1):011801. doi: 10.1103/PhysRevE.68.011801. Epub 2003 Jul 3.

Abstract

We report on an extensive study of craze formation in glassy polymers. Molecular dynamics simulations of a coarse-grained bead-spring model were employed to investigate the molecular level processes during craze nucleation, widening, and breakdown for a wide range of temperature, polymer chain length N, entanglement length N(e), and strength of adhesive interactions between polymer chains. Craze widening proceeds via a fibril-drawing process at constant drawing stress. The extension ratio is determined by the entanglement length, and the characteristic length of stretched chain segments in the polymer craze is N(e)/3. In the craze, tension is mostly carried by the covalent backbone bonds, and the force distribution develops an exponential tail at large tensile forces. The failure mode of crazes changes from disentanglement to scission for N/N(e) approximately 10, and breakdown through scission is governed by large stress fluctuations. The simulations also reveal inconsistencies with previous theoretical models of craze widening, which were based on continuum level hydrodynamics.

摘要

我们报告了一项关于玻璃态聚合物中银纹形成的广泛研究。采用粗粒化珠簧模型的分子动力学模拟,研究了在广泛的温度、聚合物链长N、缠结长度N(e)以及聚合物链间粘附相互作用强度范围内,银纹成核、扩展和破裂过程中的分子水平过程。银纹扩展通过在恒定拉伸应力下的原纤拉伸过程进行。伸长比由缠结长度决定,聚合物银纹中拉伸链段的特征长度为N(e)/3。在银纹中,张力主要由共价主链键承担,并且在大拉伸力下力分布呈现指数尾部。当N/N(e)约为10时,银纹的失效模式从解缠结转变为断裂,并且通过断裂的破裂由大应力波动控制。模拟还揭示了与先前基于连续介质水平流体动力学的银纹扩展理论模型不一致之处。

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