弛豫时间的分布作为一种方法的分离和识别的复杂过程测量阻抗谱

J. Bartoszek, Yixin Liu, J. Karczewski, Sea-Fue Wang, A. Mroziński, P. Jasiński
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引用次数: 9

摘要

阻抗谱是表征电子和电化学系统最常用的测量方法之一。阻抗谱的分辨率有限,许多不同的过程可能重叠,这可能是在其适当的后续分析中阻碍的原因。目前解决这一问题的方法有三种:阻抗谱本身的检验、等效电路的拟合和弛豫时间(DRT)的计算。后一种方法不需要任何模型或关于系统的进一步知识。通过DRT计算,得到了一个与被测系统松弛过程相关的相对窄峰图。即峰的位置与过程的时间常数有关,而峰下的面积与松弛阻力有关。这项工作的目的是测试可用的拟合函数来计算包含不同等效电路元件的先前准备的模型的峰值下面积。用精确的公式描述了上述元件的松弛时间分布,验证了所得结果。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Distribution of relaxation times as a method of separation and identification of complex processes measured by impedance spectroscopy
Impedance spectroscopy is one of the most commonly performed measurements to characterize electronic and electrochemical systems. Impedance spectra have limited resolution and many different processes may overlap what could be the reason of obstructions in its proper later analysis. Up to date, there are three approaches to solve this problem: examining impedance spectra itself, fitting spectra with equivalent circuits, and calculating the distribution of relaxation times (DRT). The latter method does not require any model or further knowledge about the system. As a result of DRT calculation, a plot containing relatively narrow peaks related to relaxation process of measured system is obtained. Namely, the position of the peak is related to time constant of the process, while the area under the peak to relaxation resistance. The aim of this work is to test available fitting functions to calculate area under a peak for previously prepared model containing different equivalent circuit elements. Obtained results are validated using exact formulas describing distribution of relaxation times for mentioned elements.
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