Determination of Non-Inductive Residual Voltage for Steep (0.5 Microsecond Front Time) Impulse Currents on Station Class Surge Arrester Blocks

J. P, C. Prabhakar, N. Vasudev, M. Kanyakumari
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Abstract

Metal Oxide Surge Arrester (MOSA) has been an essential part of power system since years. It safeguards the substation/distribution line equipment by limiting the surge voltage to an acceptable value. This is realized by the nonlinear property of the Zinc Oxide blocks used inside the MOSA. Protection Margin (PM) of the power system is defined as the difference between the BIL of the power system equipment to be protected and the residual voltage of the MOSA. The residual voltage of the MOSA depends on the peak and rate of rise of the surge current, therefore faster the surge, higher the residual voltage across MOSA. Power system is subjected to fast transients caused due to current chopping, bushing flashovers inside the valve hall, restrike in circuit breaker contacts, etc. MOSA when subjected to steeper current surges observe higher residual voltage, which shrinks the PM and may even damage the equipment to be protected. Steep impulse residual voltage of MOSA comprises of a non-inductive part, which is the property of the MOSA block and an inductive component which is determined by the length of the MOSA. IS 15086–4, 2017 [1] defines steep current of virtual front time of 1 microsecond and virtual time to half of not more than 20 microseconds. The standard also defines the procedure to measure the noninductive component of the residual voltage of MOSA when subjected to steep current impulse. But, even steeper currents can occur in the power systems due to reasons mentioned earlier; therefore, it is important to know the non-inductive residual voltage of the MOSA when subjected to such steeper current impulses. Hence in this paper, a steeper current impulse of 0.5 microsecond virtual front time is generated and the non-inductive residual voltage drop across the MOSA block is estimated for various classifications of station class surge arrester blocks. Comparison of steep (0.5 microsecond front time) current impulse residual voltage and lightning current impulse residual voltage is also performed which will be useful in conducting proper insulation co-ordination study of critical installations.
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车站级浪涌避雷器块上陡峭(0.5微秒前时间)冲击电流的无感残余电压测定
多年来,金属氧化物避雷器(MOSA)一直是电力系统的重要组成部分。它通过将浪涌电压限制在可接受的值来保护变电站/配电线路设备。这是由MOSA内部使用的氧化锌块的非线性特性实现的。电力系统的保护余量(Protection Margin, PM)是指被保护的电力系统设备的BIL值与MOSA的残余电压的差值。MOSA的剩余电压取决于浪涌电流的峰值和上升速率,因此浪涌越快,MOSA上的剩余电压越高。电力系统遭受由电流斩波、阀厅内套管闪络、断路器触点重击等引起的快速瞬变。当受到更陡的电流浪涌时,MOSA观察到更高的残余电压,这会缩小PM,甚至可能损坏要保护的设备。MOSA的陡脉冲残余电压由MOSA块的非感应部分和由MOSA长度决定的感应部分组成。IS 15086-4, 2017[1]定义了陡电流的虚拟前端时间为1微秒,虚拟前端时间为不超过20微秒的一半。本标准还规定了在受到大电流冲击时测量MOSA剩余电压的非感分量的方法。但是,由于前面提到的原因,电力系统中可能会出现更陡的电流;因此,了解MOSA在受到这种更陡的电流脉冲时的非感剩余电压是很重要的。因此,在本文中,产生了0.5微秒虚拟前时间的更陡的电流脉冲,并估计了不同类别的站级避雷器块在MOSA块上的无感剩余电压降。本文还比较了陡电流(0.5微秒前时间)冲击残余电压和雷电电流冲击残余电压,这将有助于对关键装置进行适当的绝缘协调研究。
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