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An analysis of conventional grounding impedance based on the impulsive current distribution of a horizontal electrode

机译:基于水平电极脉冲电流分布的常规接地阻抗分析

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摘要

The performance of a grounding system should be evaluated in terms of the grounding impedance for a lightning surge containing high frequency components. The ground resistance is regarded as grounding impedance measured in a low frequency. When designing the grounding system, the grounding impedance and effective length should be considered. In this study, the conventional grounding impedance was measured as functions of the front time of the impulse current and the length of the horizontal electrode used largely as the grounding electrode of the transmission tower. In order to find the relation between the conventional grounding impedance and current distribution, the magnitude of the dispersed impulse current at every 10 m interval of the horizontal electrode, which is 50 m long, was measured and simulated as a function of the front time of the injected impulse current. The conventional grounding impedance was also measured and simulated as functions of the front time of the impulse current. The current distribution and grounding impedance for the first and second strokes were also examined. As a result, the conventional grounding impedance of a long horizontal electrode was similar to that of a short horizontal electrode for fast front time. As the front time of the injected current became shorter, the current distribution increased near the current injection point. In addition, the simulated results in the multi-layered soil structure were very similar to the measured results. In case of the second stroke containing high frequency components, the simulated conventional grounding impedance of the horizontal electrode was almost the same regardless of the length of the horizontal electrode being longer than 10m since a large portion of the current was dispersed within 0-10 m section of the horizontal electrodes.
机译:应根据包含高频分量的雷电浪涌的接地阻抗来评估接地系统的性能。接地电阻被视为低频测量的接地阻抗。设计接地系统时,应考虑接地阻抗和有效长度。在这项研究中,测量传统的接地阻抗是脉冲电流的前置时间和水平电极长度的函数,水平电极的长度主要用作输电塔的接地电极。为了找到常规接地阻抗与电流分布之间的关系,测量并模拟了水​​平电极每10 m间隔(50 m长)上的分散脉冲电流的大小,并模拟了它的前沿时间。注入的脉冲电流。还测量了常规接地阻抗,并将其模拟为脉冲电流的前置时间的函数。还检查了第一冲程和第二冲程的电流分布和接地阻抗。结果,长的水平电极的常规接地阻抗与短的水平电极的常规接地阻抗相似,以实现快速的前置时间。随着注入电流的前置时间变短,电流分布在电流注入点附近增加。此外,在多层土壤结构中的模拟结果与实测结果非常相似。在第二冲程包含高频分量的情况下,水平电极的模拟常规接地阻抗几乎相同,而与水平电极的长度大于10m无关,因为大部分电流分散在0-10 m内水平电极的横截面。

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