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arXiv 0709.0769cond-mat.softcond-mat.mtrl-sci
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Polymer玻璃的应变硬化:缠结、能量学和塑性

Strain Hardening of Polymer Glasses: Entanglements, Energetics, and Plasticity

Robert S. Hoy, Mark O. Robbins

摘要:

模拟被用来研究聚合物玻璃中应变硬化的微观起源。虽然在很宽的温度范围内的应力-应变曲线可以拟合熵网络模型预测的函数形式,但许多其他结果与这些模型的物理图像根本不一致。应力太大而不能成为熵,并且与温度有错误的趋势。在大应变下,最引人注目的硬化反映了能量的增加,因为链在纠缠之间被拉紧,而不是熵的变化。当加热到玻璃化转变温度以上时,只有在变形样品的形状恢复过程中才观察到弱的熵应力。虽然短链不形成缠结网络,但它们表现出部分形状恢复、取向和应变硬化。所有链长的应力崩溃时,对链拉伸的微观措施,而不是宏观拉伸绘制。热对应力的贡献与通过链间键的断裂和重整测量的塑性速率成正比。这些观察结果表明,应变硬化的正确微观理论应该基于玻璃态物理学,而不是橡胶弹性。

英文摘要:

Simulations are used to examine the microscopic origins of strain hardening in polymer glasses. While stress-strain curves for a wide range of temperature can be fit to the functional form predicted by entropic network models, many other results are fundamentally inconsistent with the physical picture underlying these models. Stresses are too large to be entropic and have the wrong trend with temperature. The most dramatic hardening at large strains reflects increases in energy as chains are pulled taut between entanglements rather than a change in entropy. A weak entropic stress is only observed in shape recovery of deformed samples when heated above the glass transition. While short chains do not form an entangled network, they exhibit partial shape recovery, orientation, and strain hardening. Stresses for all chain lengths collapse when plotted against a microscopic measure of chain stretching rather than the macroscopic stretch. The thermal contribution to the stress is directly proportional to the rate of plasticity as measured by breaking and reforming of interchain bonds. These observations suggest that the correct microscopic theory of strain hardening should be based on glassy state physics rather than rubber elasticity.

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