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首页> 外文期刊>The Journal of Chemical Physics >New model for nearly constant dielectric loss in conductive systems: Temperature and concentration dependencies
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New model for nearly constant dielectric loss in conductive systems: Temperature and concentration dependencies

机译:导电系统中几乎恒定的介电损耗的新模型:温度和浓度依赖性

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By appropriate fitting of conductive-system frequency-response data for two different ionic materials over ranges of temperature and ionic concentration, it is shown how dispersion associated entirely with ionic motion and that leading to nearly constant dielectric loss (NCL) can be unambiguously distinguished and separated. The latter is clearly associated with polarization of the bulk material, and in the limit of zero mobile-ion concentration NCL appears to approach zero, yielding only a bulk dielectric constant, #epsilon#_D infinity 0, one that is frequency-independent over the usual immittance-spectroscopy experimental range. For nonzero ionic concentration, however, dielectric NCL appears and can be represented by a small-exponent constant phase element (CPE) complex power law in frequency. This part of the full response may be modeled either by a CPE that includes all bulk dielectric dispersion or, more plausibly, by #epsilon#_D infinity 0 and a CPE representing only incremental bulk dispersion associated with coupling between ionic motion and bulk polarization. In this case, interestingly, precise power-law dependencies of various dielectric parameters on ionic concentration are established but need theoretical explanation. Fitting of the ionic part of the total dispersion with three different Kohlrausch-Williams-Watts models leads to dependencies of their different #beta#-shape parameters and dielectric quantities on temperature and on ionic concentration and strongly suggests that the widely used original-modulus-formalism dispersion fitting model is incorrect and should be replaced by a corrected version.
机译:通过适当拟合两种不同离子材料在温度和离子浓度范围内的导电系统频率响应数据,可以显示出如何明确地区分与离子运动完全相关的色散以及导致几乎恒定的介电损耗(NCL)的色散,以及分开。后者显然与块状材料的极化有关,并且在零移动离子浓度的极限下,NCL似乎接近零,仅产生块状介电常数#epsilon#_D infinity 0,该常数在频率上与频率无关。常用的光谱法实验范围。但是,对于非零离子浓度,会出现电介质NCL,并且可以用小指数恒定相位元素(CPE)频率的复幂定律表示。可以通过包括所有体电介质色散的CPE或更合理地通过#epsilon_D infinity 0和仅表示与离子运动和体极化之间的耦合相关的增量体色散的CPE来建模全部响应的这一部分。在这种情况下,有趣的是,建立了各种介电参数对离子浓度的精确幂律依赖性,但需要进行理论解释。用三种不同的Kohlrausch-Williams-Watts模型拟合总分散体的离子部分会导致其不同的#beta#形状参数和介电常数对温度和离子浓度的依赖性,并强烈暗示了广泛使用的原始模量-形式主义散布拟合模型不正确,应使用更正的版本代替。

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