佛罗里达州肯尼迪航天中心39B发射场防雷系统下导线接地电阻的计算

C. Mata, A. G. Mata
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引用次数: 3

摘要

在佛罗里达州肯尼迪航天中心(KSC)的39B发射场(LC39B)设计和建造了一种新的防雷系统(LPS),该系统由一个悬链线系统(在地面以上约181米的高度)组成,由安装在三个三角形塔顶的三个绝缘体支撑。九个下导线(每个约250米长)连接到悬链线系统。每个下导线连接到一个半径为7.62米的圆形平衡导线,该平衡导线由六个等间距、6米长的垂直接地棒连接。在LC39B的接地要求,所有地下和地上的金属管道,外壳,滚道和电缆托盘,在7.62米的平衡,连接到平衡,这导致一个复杂的互连接地系统,考虑到许多金属管道,滚道和电缆托盘在多个方向上运行在LC39B周围。这种接地系统的复杂性使得使用多根金属棒或木桩的电位降法不适用于测量下行导线的接地阻抗。为了计算下导线的接地阻抗,使用了接地钳(EGC),一种测量接地阻抗的无接地装置,以及LPS的备选瞬态程序(ATP)模型。EGC用于测量各下导电路的回路阻抗加上接地阻抗,ATP模型用于计算各下导电路的回路阻抗。然后通过从EGC测量中减去atp计算的回路阻抗来计算下行导体的接地电阻。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Calculating the Lightning Protection System downconductors' grounding resistance at Launch Complex 39B, Kennedy Space Center, Florida
A new Lightning Protection System (LPS) was designed and built at Launch Complex 39B (LC39B), at the Kennedy Space Center (KSC), Florida, which consists of a catenary wire system (at a height of about 181 meters above ground level) supported by three insulators installed atop three towers in a triangular configuration. Nine downconductors (each about 250 meters long) are connected to the catenary wire system. Each downconductor is connected to a 7.62-meter-radius circular counterpoise conductor with six equally spaced, 6-meter-long vertical grounding rods. Grounding requirements at LC39B call for all underground and aboveground metallic piping, enclosures, raceways, and cable trays, within 7.62 meters of the counterpoise, to be bonded to the counterpoise, which results in a complex interconnected grounding system, given the many metallic piping, raceways, and cable trays that run in multiple directions around LC39B. The complexity of this grounding system makes the fall-of-potential method, which uses multiple metallic rods or stakes, unsuitable for measuring the grounding impedances of the downconductors. To calculate the grounding impedance of the downconductors, an Earth Ground Clamp (EGC), a stakeless device for measuring grounding impedance, and an Alternative Transient Program (ATP) model of the LPS are used. The EGC is used to measure the loop impedance plus the grounding impedance of each downconductor, and the ATP model is used to calculate the loop impedance of each downconductor circuit. The grounding resistance of the downconductors is then calculated by subtracting the ATP-calculated loop impedances from the EGC measurements.
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