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Dependence of the Chopping Current Level of a Vacuum Interrupter on Parallel Capacitance

机译:真空断路器的斩波电流水平对并联电容的依赖性

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The distribution of chopping currents of a vacuum circuit breaker using CuCr25 contact material was measured in a laboratory circuit consisting of a three-phase 20-kV cable system and a dry-type distribution transformer rated 900 kVA. The cable length between the upstream feeding transformer and the circuit breaker was several hundreds of meters. An inductive load connected to the distribution transformer provided a 50-Hz current of 10 A rms. Under these conditions, the mean chopping current level was between 3.2 and 3.5 A and showed no significant dependence on the arcing time, which was varied between 2 and 8 ms. After addition of a surge capacitor of 130 nF between the transformer terminals and ground, which very much reduces the overvoltage during switching, the chopping current level increased to 5.6 to 7.7 A in dependence of the arcing time. In order to explain this, the interaction of the arc with the electric circuit in particular with the cables on both sides of the breaker has to be evaluated. If the cables are long, travelling waves need to be considered as well as all return current paths in a three-phase circuit. The coincidence of excited network oscillations with random arc instabilities may result in either momentary amplification or damping of such oscillations. An additionally installed capacitor serves as a source sustaining a momentary current reduction after an arc instability and allows the excitation of a subsequent arc instability leading to an increase of the chopping current with longer arcing times. With low capacitance on the load side, there is no interaction and therefore no influence from the arcing time.
机译:使用CuCr25接触材料的真空断路器的斩波电流分布在实验室电路中进行了测量,该电路由三相20 kV电缆系统和额定功率为900 kVA的干式配电变压器组成。上游馈电变压器和断路器之间的电缆长度为数百米。连接到配电变压器的电感负载可提供10 A rms的50 Hz电流。在这些条件下,平均斩波电流水平在3.2至3.5 A之间,并且对电弧放电时间没有显着依赖性,电弧放电时间在2至8 ms之间变化。在变压器端子和地面之间增加了一个130 nF的电涌电容器后,该电容器在开关过程中大大降低了过电压,斩波电流水平根据电弧放电时间增加至5.6至7.7A。为了对此进行解释,必须评估电弧与电路的相互作用,尤其是与断路器两侧的电缆的相互作用。如果电缆较长,则需要考虑行波以及三相电路中的所有返回电流路径。激发网络振荡与随机电弧不稳定性的同时发生可能会导致这种振荡的瞬时放大或衰减。额外安装的电容器用作在电弧不稳定后维持瞬时电流减小的源,并允许激发随后的电弧不稳定,从而导致斩波电流随着电弧时间的延长而增加。负载侧的电容较低,因此不会产生相互作用,因此不会受到电弧放电时间的影响。

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