甲基和乙基纤维素溶液的微波介电弛豫

H. Farber, S. Petrucci
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引用次数: 0

摘要

报道了甲基纤维素溶液和乙基纤维素溶液在25℃和1 - 90ghz频率范围内的复介电常数。介电常数的实、虚系数显示出随频率变化的松弛曲线,可以用Cole-Davidson分布函数或两个离散德拜松弛过程的和来解释。对后一种描述的偏爱不是基于最优的数值拟合,而是基于两个德拜过程分别与氢键断裂(如醇)和烷氧基和/或分子翻滚有关的建议。通过报道甲基纤维素溶剂-二甲氧基乙烷混合物在整个组成范围内的复介电常数,给出了上述假设的证据。结果表明,松弛贡献ε0-ε∞1归因于低Debye弛豫过程(并归属于氢键断裂过程),与甲基纤维素溶液的摩尔浓度成正比。这表明,用甲氧基取代羟基后,与纯二甲氧基相比,当不存在-OH基团时,归因于(ε0-ε∞1)的效应减小并消失。此外,通过将贡献ε0-ε∞1视为在液体混合物中处理的立场,表观偶极矩μ ~ 3 Debyes由Böttcher理论计算。这个数字与用Onsager理论计算的醇的μ值相当。以上似乎表明,尽管Cole-Davidson分布函数可能在数值上符合弛豫曲线,但它(根据其本身的性质)逃避了介电弛豫过程的分子描述。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Microwave dielectric relaxation of methyl and ethylcellosolve

The complex dielectric permittivity of methyl and ethylcellosolve at 25°C and in the frequency range 1–90 GHz are reported. The real and imaginary coefficients of the permittivity show a relaxation profile with frequency that can be interpreted either by a Cole-Davidson distribution function or by the sum of two discrete Debye-relaxation processes. Preference for the latter description is given not on the basis of an optimum of a numerical fit, but rather on the proposal that the two Debye processes are related to H-bond breaking, as for the alcohols, and to alkoxy and/or molecular tumbling respectively. Evidence of the above hypothesis is given by reporting the complex permittivity of methylcellosolve-dimethoxyethane mixtures in the whole composition range. It is shown that the relaxation contribution ε0∞1, attributed to the lower Debye relaxation process (and assigned to the H-bond breaking process) is proportional to the molarity of methylcellosolve up to the pure liquid. This shows that by substituting the OH group by the methoxy group, the effect attributed to (ε0∞1) decreases and disappears when no -OH groups are present as for pure dimethoxyethane. Further, by taking the position that the contribution ε0∞1 is to be dealt with as in liquid mixtures, the apparent dipole moment μ∼3 Debyes is calculated by the Böttcher theory. This figure is comparable to the values of μ calculated by the Onsager theory for the alcohols. The above seems to suggest that although the Cole-Davidson distribution function may fit the relaxation profile numerically, it eludes (by its own nature) the molecular description of the dielectric relaxation processes.

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