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首页> 外文期刊>The Journal of Chemical Physics >THE EFFECTS OF COVALENT BONDS ON THE LOCALIZED RELAXATIONS IN THE GLASSY STATES OF LINEAR CHAIN AND NETWORK MACROMOLECULES
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THE EFFECTS OF COVALENT BONDS ON THE LOCALIZED RELAXATIONS IN THE GLASSY STATES OF LINEAR CHAIN AND NETWORK MACROMOLECULES

机译:共价键对线性链和网络大分子在玻璃态的局部弛豫的影响

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摘要

Dipolar relaxations in the glassy states of five molecular liquids and of their partially and completely polymerized structures, both linear chain and network types, were studied by dielectric measurements for a fixed ac frequency of 1 kHz. Calorimetric measurements were made to determine the number of covalent bonds formed at different instants of polymerization, and the results were combined with the dielectric data to investigate how the height of the relaxation peak indicating localized dipole diffusion changed as the number of covalent bonds in the spontaneously polymerizing material increased. The height, or strength, of the peak due to the localized relaxation process in the molecular liquid gradually decreased and the process approached extinction as the number of covalent bonds approached its limiting value. Concurrently, a new localized glassy state relaxation process evolved at a temperature with a peak 70-90 K above that of the one observed for the molecular state and its height increased and approached a constant value as the number of covalent bonds formed approached its limiting value. These changes were quantitatively similar for the five materials, irrespective of the structure of the macromolecular product. The extinction of the sub-T-g relaxation peak observed originally for the unreacted state has features in common with structural relaxation effects. (C) 1996 American Institute of Physics. [References: 30]
机译:通过介电测量固定频率为1 kHz的交流电,研究了五种分子液体及其部分和完全聚合的结构(线性链和网络类型)在玻璃态下的偶极弛豫。进行了量热测量,以确定在聚合的不同瞬间形成的共价键的数量,并将结果与​​介电数据相结合,研究表明局部偶极扩散的弛豫峰的高度如何随自发中的共价键数量的变化而变化聚合材料增加。由于分子液体中的局部弛豫过程而导致的峰高或强度逐渐降低,并且随着共价键数接近其极限值,该过程逐渐消失。同时,一种新的局部玻璃态弛豫过程发生在一个峰值,该峰值的峰值比分子态观测到的峰值高70-90 K,并且其高度增加,并且随着形成的共价键数趋近其极限值而接近恒定值。 。不管大分子产物的结构如何,对于五种材料,这些变化在数量上都是相似的。最初在未反应状态下观察到的sub-T-g弛豫峰的消失具有与结构弛豫效应相同的特征。 (C)1996年美国物理研究所。 [参考:30]

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