Investigation on the Characteristics of Dielectric Barrier Surface Discharge Driven by Repetitive Nanosecond Pulses in Airflows

2016 ◽  
Vol 44 (11) ◽  
pp. 2812-2818 ◽  
Author(s):  
Pang Lei ◽  
He Kun ◽  
Zhang Qiaogen ◽  
Di Dongxu ◽  
Long Tianjun
Author(s):  
Tomas Hurtig ◽  
Mattias Elfsberg ◽  
Zhongshan Li ◽  
Zhiwei Sun ◽  
Andreas Ehn ◽  
...  

2007 ◽  
Vol 16 (10) ◽  
pp. 3016-3021 ◽  
Author(s):  
Li Xue-Chen ◽  
Liu Zhi-Hui ◽  
Jia Peng-Ying ◽  
Li Li-Chun ◽  
Yin Zeng-Qian ◽  
...  

2020 ◽  
Vol 11 (11) ◽  
pp. 17-27
Author(s):  
Vadim V. VOEVODIN ◽  
◽  
Marina V. SOKOLOVA ◽  
Viktor R. SOLOV’YEV ◽  
Nikolay Yu. LYSOV ◽  
...  

The results from an experimental study of impulse surface discharge occurring in an electrode system containing a dielectric plate are presented. On one of its sides, the plate had a corona-producing electrode made of 50 mm thick copper foil grounded through a current shunt for measuring the discharge current. On its other side, the plate had a high-voltage electrode, to which the voltage from a pulse generator was applied. The article presents the results from measurements of the initial voltage and the sizes of the surface discharge area in air when applying single voltage pulses with different pulse front steepness in the range 0,1–3,4 kV/ms and amplitude in the range 7–15 kV. The measurements were carried out for different dielectric barrier materials with the e values from 2 to 35. The dielectric barrier thickness was 0,9–1,8 mm. The study results have shown that the initial surface discharge ignition voltage depends essentially on the voltage pulse parameters, whereas the barrier characteristics have a weaker effect on this voltage. It has been determined that the discharge has different discharge zone length and different structure depending on the dielectric barrier properties and applied voltage parameters. The streamer zone sizes decrease with increasing the barrier material e value at the same voltage pulse steepness and increase with increasing the steepness for each barrier material. The data obtained for a wide range of external conditions can be used in numerical modeling of discharge.


2018 ◽  
Vol 25 (10) ◽  
pp. 103503
Author(s):  
Jiayu Huang ◽  
Yuyang Pan ◽  
Fucheng Liu ◽  
Rong Han ◽  
Haoyang Sun ◽  
...  

2010 ◽  
Vol 22 (3) ◽  
pp. 539-544 ◽  
Author(s):  
章程 Zhang Cheng ◽  
邵涛 Shao Tao ◽  
于洋 Yu Yang ◽  
龙凯华 Long Kaihua ◽  
王珏 Wang Jue ◽  
...  

Nanomaterials ◽  
2019 ◽  
Vol 9 (10) ◽  
pp. 1381 ◽  
Author(s):  
Zhang ◽  
Yang ◽  
Wang ◽  
Jia ◽  
Yuan ◽  
...  

Discharge regime transition in a single pulse can present the breakdown mechanism of nanosecond pulsed dielectric barrier discharge. In this paper, regime transitions between streamer, diffuse, and surface discharges in nanosecond pulsed dielectric barrier discharge are studied experimentally using high resolution temporal–spatial spectra and instantaneous exposure images. After the triggering time of 2–10 ns, discharge was initiated with a stable initial streamer channel propagation. Then, transition of streamer-diffuse modes could be presented at the time of 10–34 ns, and a surface discharge can be formed sequentially on the dielectric plate. In order to analyze the possible reason for the varying discharge regimes in a single discharge pulse, the temporal–spatial distribution of vibrational population of molecular nitrogen N2 (C3Πu, v = 0,1,2) and reduced electric field were calculated by the temporal–spatial emission spectra. It is found that at the initial time, a distorted high reduced electric field was formed near the needle electrode, which excited the initial streamer. With the initial streamer propagating to the dielectric plate, the electric field was rebuilt, which drives the transition from streamer to diffuse, and also the propagation of surface discharge.


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