Shock wave in a long-air-gap leader discharge

We report the shock wave phenomenon in an air-gap leader discharge observed using an interferometer. The continuous temporal evolution of the shock wave and plasma channel is recorded and reproduced with a thermohydrodynamic model based on the measured current, providing a prediction of the pressure...

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Main Authors: Yingzhe Cui, Chijie Zhuang, Rong Zeng, Xuan Zhou
Format: Article
Language:English
Published: AIP Publishing LLC 2019-06-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5100519
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spelling doaj-f0a56aa69887485cb9aae481d1592e292020-11-25T01:48:29ZengAIP Publishing LLCAIP Advances2158-32262019-06-0196065011065011-710.1063/1.5100519037906ADVShock wave in a long-air-gap leader dischargeYingzhe Cui0Chijie Zhuang1Rong Zeng2Xuan Zhou3Department of Electrical Engineering, Tsinghua University, Beijing 100084, ChinaDepartment of Electrical Engineering, Tsinghua University, Beijing 100084, ChinaDepartment of Electrical Engineering, Tsinghua University, Beijing 100084, ChinaDepartment of Electrical Engineering, Tsinghua University, Beijing 100084, ChinaWe report the shock wave phenomenon in an air-gap leader discharge observed using an interferometer. The continuous temporal evolution of the shock wave and plasma channel is recorded and reproduced with a thermohydrodynamic model based on the measured current, providing a prediction of the pressure pulses of the shock wave. The weak shock wave propagates at nearly the speed of sound, and the simulation results for the shock wave front positions and the plasma channel radius are consistent with experimental measurements. Experimental observations and numerical comparisons show that continuous energy injection results in a temporary overpressure process in the plasma channel and generates the shock wave. The pressure at the shock front falls rapidly and decays with propagation of the wave. In the weak shock region, the pressure wave decays as P∝R−3/4. The wave propagation predicted using the thermohydrodynamic model is compared with propagations predicted using the Vlases and Jones models, and we find that a measurement of the shock wave propagation trajectory gives an estimate of the energy injected to the leader channel during a discharge.http://dx.doi.org/10.1063/1.5100519
collection DOAJ
language English
format Article
sources DOAJ
author Yingzhe Cui
Chijie Zhuang
Rong Zeng
Xuan Zhou
spellingShingle Yingzhe Cui
Chijie Zhuang
Rong Zeng
Xuan Zhou
Shock wave in a long-air-gap leader discharge
AIP Advances
author_facet Yingzhe Cui
Chijie Zhuang
Rong Zeng
Xuan Zhou
author_sort Yingzhe Cui
title Shock wave in a long-air-gap leader discharge
title_short Shock wave in a long-air-gap leader discharge
title_full Shock wave in a long-air-gap leader discharge
title_fullStr Shock wave in a long-air-gap leader discharge
title_full_unstemmed Shock wave in a long-air-gap leader discharge
title_sort shock wave in a long-air-gap leader discharge
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2019-06-01
description We report the shock wave phenomenon in an air-gap leader discharge observed using an interferometer. The continuous temporal evolution of the shock wave and plasma channel is recorded and reproduced with a thermohydrodynamic model based on the measured current, providing a prediction of the pressure pulses of the shock wave. The weak shock wave propagates at nearly the speed of sound, and the simulation results for the shock wave front positions and the plasma channel radius are consistent with experimental measurements. Experimental observations and numerical comparisons show that continuous energy injection results in a temporary overpressure process in the plasma channel and generates the shock wave. The pressure at the shock front falls rapidly and decays with propagation of the wave. In the weak shock region, the pressure wave decays as P∝R−3/4. The wave propagation predicted using the thermohydrodynamic model is compared with propagations predicted using the Vlases and Jones models, and we find that a measurement of the shock wave propagation trajectory gives an estimate of the energy injected to the leader channel during a discharge.
url http://dx.doi.org/10.1063/1.5100519
work_keys_str_mv AT yingzhecui shockwaveinalongairgapleaderdischarge
AT chijiezhuang shockwaveinalongairgapleaderdischarge
AT rongzeng shockwaveinalongairgapleaderdischarge
AT xuanzhou shockwaveinalongairgapleaderdischarge
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