轴向压缩聚合物棒在玻璃和橡胶过渡中的后屈曲平衡状态

Ksenia Alekseevna Tikhomirova, Nikolay Aleksandrovich Trufanov
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引用次数: 4

摘要

聚合物材料在冷却和加热下的玻璃化和橡胶化转变是一种形状记忆效应的基础,即材料在外部影响下暂时保存变形形状并恢复原始形状的能力。本工作旨在模拟轴向压缩聚合物棒在屈曲后平衡状态下的形状记忆效应,这是欧拉弹性理论在玻璃材料情况下的推广。为了建模,我们使用了一种新型的本构关系来描述非晶聚合物在宽温度范围内的热力学行为。为了确定轻链环氧树脂的模型参数,利用动态力学分析仪进行了一系列实验。通过数值模拟发现了温度变化过程中环氧棒的后屈曲状态。所得结果说明了轴向压缩杆屈曲时的形状记忆效应。热-机械形状记忆循环包括变形发展和保存阶段以及随后初始形状的恢复阶段。根据得到的结果,最大挠度对应于橡胶材料状态下的第一个加载步骤,因为弹性模量很低。在恒定负荷下的冷却过程中,变形保持恒定。在玻璃态卸载后,由于玻璃弹性模量明显大于橡胶弹性模量,挠度减小幅度较小。在随后的加热过程中,棒恢复其初始未变形的形状。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

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Post-buckled equilibrium state of axially compressed polymeric rod in glass and rubbery transitions

Glass and rubbery transitions under cooling and heating of polymeric materials underlie a shape memory effect, that is a material ability to save temporarily the deformed shape and restore the original one under the external influence. The present work aims to model the shape memory effect for an axially compressed polymeric rod in its post-buckled equilibrium state, which is the generalization of Euler’s elastica for a glassy material case.

For modeling, we use a new type of constitutive relations describing the thermomechanical behavior of amorphous polymers over a wide temperature range. To define the model parameters for lightly-linked epoxy resin a series of experiments was conducted using the Dynamic Mechanical Analyzer.

Post-buckled states of an epoxy rod equilibrium during the temperature change have been found from numerical simulation. The obtained results illustrate the shape memory effect in case of axially compressed rod buckling.

The thermomechanical shape-memory cycle includes the stages of deformation development and preservation and the subsequent recovery of the initial shape. According to the obtained results, maximum deflection corresponds to the first loading step at the rubbery material state, because the elastic modulus is very low. During cooling under a constant load the deformation remains constant. After unloading in glassy state the deflection decreases by a small value, because the glassy elastic modulus significantly exceeds the rubbery one. During subsequent heating the rod recovers its initial undeformed shape.

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