Relaxation in the glass transition regime interpreted in terms of the aggregate model

M. Köpf, H.G. Kilian
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引用次数: 7

Abstract

The retardation time spectra in the glass transition range are discussed on hand of multidimensional deuteron NMR experiments, measurements of the dielectric loss and the T1-relaxation of proton spins in liquids at different temperatures and different frequencies. The data can be described by applying the model of reversible aggregation. Every liquid is here characterized by a broad aggregate size distribution. Relaxation is interpreted as collective response of intra-aggregate Debye processes running off while the aggregate ensemble fluctuates. The relaxation time increases with the volume of the aggregate so that every relaxation time distribution is strictly related to the aggregate size distribution. The shape of relaxation mode distributions is similar, the width depends on how the molecular mechanisms couple to the stationary dynamics. The coupling changes on heating so that the width of the relaxation mode distribution decreases. A full description of the α-process needs to account for aggregate ensemble fluctuations, a bimodal relaxation mode spectrum and a heterogeneous kinetics.

用聚集体模型解释的玻璃化转变体系中的松弛
通过多维氘核磁共振实验、不同温度和不同频率下液体中介电损耗和质子自旋t1弛豫的测量,讨论了玻璃跃迁范围内的延迟时间谱。数据可以用可逆聚合模型来描述。这里的每一种液体的特点都是具有广泛的粒径分布。弛豫被解释为聚集体内部的德拜过程在聚集体整体波动时的集体响应。松弛时间随骨料体积的增大而增大,使得每一个松弛时间分布都与骨料粒度分布严格相关。弛豫模式分布的形状是相似的,其宽度取决于分子机制如何与静止动力学耦合。在加热过程中,耦合发生变化,使得弛豫模分布的宽度减小。α-过程的完整描述需要考虑总体综涨落、双峰弛豫模式谱和非均相动力学。
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