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首页> 外文期刊>Physical chemistry chemical physics: PCCP >Main and secondary relaxations of non-polymeric high-T-g glass formers as revealed by dielectric spectroscopy
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Main and secondary relaxations of non-polymeric high-T-g glass formers as revealed by dielectric spectroscopy

机译:由介电光谱透露的非聚合物高T-G玻璃造型器的主要和二次松弛

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摘要

A series of high-T-g glass formers with T-g values varying between 347 and 390 K and molar masses in the range of 341 and 504 g mol(-1) are investigated by dielectric spectroscopy. They are compared to paradigmatic reference systems. Differently polar side groups are attached to a rigid non-polar core unit at different positions. Thereby, the dielectric relaxation strength varies over more than two decades. All the relaxation features typical of molecular glass formers are rediscovered, i.e. stretching of the main (alpha-) relaxation, a more or less pronounced secondary (beta-) process, and a fragility index quite similar to that of other molecular systems. The position of the polar nitrile side group influences the manifestation of the beta-relaxation. The alpha-relaxation stretching displays the trend to become less with higher relaxation strength Delta epsilon(alpha), confirming recent reports. Typical for a generic beta-process is the increase of its amplitude above T-g, which is found to follow a power-law behaviour as a function of the ratio tau(alpha)/tau(beta) with a universal exponent; yet, its relative amplitude to that of the alpha-relaxation varies as does the temporal separation of both processes. The mean activation energy of the beta-process as well as the width of the energy distribution g(beta)(E) increases more or less systematically with T-g. The latter is determined from the dielectric spectra subjected to a scaling procedure assuming a thermally activated process. Plotting g(beta)(E) as a function of the reduced energy scale E/T-g, the distributions are centred between 19-35 and their widths differ by a factor 2-3.
机译:通过介电光谱研究了一系列具有在347和390k和341和504g mol(-1)范围内的T-G值的高T-G玻璃造形剂,其在347和390k和摩尔质量范围内。它们与范式参考系统进行比较。不同的极性侧组在不同位置附接到刚性非极性芯单元。因此,介电松弛强度在二十多年超过二十年中变化。典型的分子玻璃造型器的所有弛豫特征是重新发现的,即延伸主要(α-)弛豫,或多或少明显的二次(β-)工艺,以及与其他分子系统相似的脆性指数。极性丁腈侧组的位置影响β松弛的表现。 alpha-leastation伸展显示较高的休闲强度δε(alpha)变得更少的趋势,确认最近的报告。通用β-过程的典型是其幅度高于T-g的增加,这被发现遵循幂律行为,作为具有普遍指数的TAU(alpha)/ Tau(Beta)的比率;然而,其与α松弛的相对幅度变化,两种过程的时间分离都变化。 β-过程的平均活化能量以及能量分布G(β)(e)的宽度以T-g系统地增加或多或少地增加。假设具有热敏处理的缩放过程的介电光谱从经受缩放过程的介电光谱确定后者。绘制G(β)(e)作为降低能量尺度E / T-g的函数,分布在19-35之间以19-35之间的中心,其宽度不同为2-3。

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