電気学会論文誌B(電力・エネルギー部門誌)
Online ISSN : 1348-8147
Print ISSN : 0385-4213
ISSN-L : 0385-4213
論文
FDTD法によるインパルス電圧測定系のステップ応答解析
岡 宏樹玉野 哲弘馬場 吉弘石井 勝長岡 直人雨谷 昭弘
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2012 年 132 巻 5 号 p. 507-514

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Unit step responses (USRs) of a USR-measuring system recommended by the International Electro-technical Commission (IEC) have been calculated, using the finite-difference time-domain (FDTD) method, for various conditions of grounding and shield ring. The USR measuring system subject to analysis has a resistor divider of height 3.3m and resistance 9kΩ. The conductivity and relative permittivity of the laboratory floor, on which the USR measuring system is placed, are set to a range from σ = 0.001mS/m to ∞ and a range from εr = 1 to 10, respectively. It turns out that USR parameters are not much influenced by either σ or εr if σ is higher than or equal to 10mS/m, and they are close to the USR parameters for σ = ∞. When σ is lower than about 0.1mS/m, USR parameters are more influenced by σ and εr. Variations in the partial response time Tα, the experimental response time Tn, the settling time Ts, and the overshoot β, due to the differences of σ and εr, are 8ns, 14ns, 150ns, and 50%, respectively. Even if the width of horizontal ground metal sheet is extended from wg = 2 to 3m, these variations are not much reduced. The extension of the width of vertical metal sheet from wv = 1 to 2m does not much influence the USR parameters, either. Both the installing height of shield ring h and its diameter d influence the USR parameters: Tα decreases with decreasing h and/or d. Note that the FDTD-calculated USR for σ = 0.1mS/m and εr = 10 agrees reasonably well with the corresponding measured USR: Tα = 19ns, Tn = 6ns, Ts = 310ns, and β = 53% vs. Tα = 16ns, Tn = 10ns, Ts = 280ns, and β = 44%.

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