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Thermal Interruption Performance of Ultrahigh-Pressure Free-Burning Nitrogen Arc

机译:超高压自由燃烧氮弧的热中断性能

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In this paper, an experimental investigation of the thermal interruption performance of free-burning nitrogen arcs at 1 bar, 20 bar, and 40 bar filling pressures is reported. This work contributes to the fundamental understanding of arc characteristics at very high gas filling pressures. A resonant circuit is used to generate an arc peak current of 130 A at a frequency of 190 Hz. An ignition copper wire initiates the arc between a 4 mm diameter pin electrode and a ring electrode. The arc burns freely at a fixed inter-electrode gap of 50 mm without any forced gas flow. A resistive-capacitive branch parallel to the arc controls the initial rate of rise of recovery voltage. By changing the parallel resistance, the rate of rise of recovery voltage is varied from 9.8 V/μs to 84.8 V/ μs. Time to re-ignition and the corresponding re-ignition voltages are considered as the primary parameters to characterize the thermal interruption performance. It is observed that the re-ignition time rises with the decrease of rate of rise of recovery voltage at all pressure levels, which is expected. However, in the absence of a forced gas flow, high gas filling pressure results in a reduction of the time to re-ignition and the re-ignition voltage in contrast to atmospheric pressure nitrogen arc.
机译:本文报道了在1巴,20巴和40巴填充压力下的自由燃烧氮弧的热中断性能的实验研究。这项工作有助于在非常高的气体灌装压力下对电弧特性的基本理解。谐振电路用于以190Hz的频率产生130a的电弧峰值电流。点火铜线在4mm直径销电极和环形电极之间启动电弧。电弧在50mm的固定电极间隙中自由燃烧,而没有任何强制气体流动。平行于电弧的电阻电容分支控制恢复电压的初始速率。通过改变并联电阻,恢复电压的上升速率从9.8 V /μs变化为84.8V /μs。重新点火的时间和相应的再点火电压被认为是表征热中断性能的主要参数。观察到,重新点火时间随着预期的所有压力水平的恢复电压升高率的降低而上升。然而,在没有强制气流的情况下,高气体填充压力导致减少重新点火的时间和与大气压氮弧相反的重新点火和再点火电压。

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