2012
DOI: 10.1063/1.3676628
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Modeling of asymmetric pulsed phenomena in dielectric-barrier atmospheric-pressure glow discharges

Abstract: Asymmetric current pulses in dielectric-barrier atmospheric-pressure glow discharges are investigated by a self-consistent, one-dimensional fluid model. It is found that the glow mode and Townsend mode can coexist in the asymmetric discharge even though the gas gap is rather large. The reason for this phenomenon is that the residual space charge plays the role of anode and reduces the gap width, resulting in the formation of a Townsend discharge.

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Cited by 28 publications
(15 citation statements)
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“…Our group has also made some effort on this aspect. According to our previous works, the SP1-AP1 transition in shorter gaps might be attributed to the discordance of the evolutionary paces between electrons and ions [16], while, in longer gaps, the rise in seed electron level induced by the electron backflow is the main reason for the generation of AP1 discharge [17], and the traditional explanations such as "residual positive column" [7] or "instantaneous anode" [18] in essence are special forms of the "electron backflow region". Furthermore, we also proposed a preliminary state-controlling method which can adjust the discharge mode from AP1 to SP1 by applying a first-peak-leveled driving voltage from the beginning of the discharge [19].…”
Section: Introductionmentioning
confidence: 99%
“…Our group has also made some effort on this aspect. According to our previous works, the SP1-AP1 transition in shorter gaps might be attributed to the discordance of the evolutionary paces between electrons and ions [16], while, in longer gaps, the rise in seed electron level induced by the electron backflow is the main reason for the generation of AP1 discharge [17], and the traditional explanations such as "residual positive column" [7] or "instantaneous anode" [18] in essence are special forms of the "electron backflow region". Furthermore, we also proposed a preliminary state-controlling method which can adjust the discharge mode from AP1 to SP1 by applying a first-peak-leveled driving voltage from the beginning of the discharge [19].…”
Section: Introductionmentioning
confidence: 99%
“…模式的转变, 常见的情形是汤森模式与辉光放电模式 之间的转换 [27,[30][31][32][33][34] . 2012年, Ha等人 [30] [33][34][35][36][37][38][39] 条件下实现的, 例如: 脉冲调制的射频 电压 [33] 、亚微秒脉冲型电压 [34][35][36] 、锯齿电压 [37] 、光滑 梯形电压 [38] 和射频脉冲与梯形脉冲结合电压 [39] 等, 这 些研究结果都表明了它们的放电特性完全不同于正 弦电压激发放电的特性. 在利用锯齿型电压 [37] 激发大 气压DBD放电中, 模拟研究发现每半个外加电压周期 中出现一个阶梯型放电, 并分析了占空比对放电的影 响.…”
Section: 射的作用 与此同时 大气压Dbd中也经常出现放电unclassified
“…[6][7][8][9] Occasionally, under certain conditions, the single period discharge may display an asymmetric discharge mode with different positive and negative current pulses. [10][11][12] Recently, more complex temporal nonlinear behaviors of APGD, such as period-doubling bifurcation and chaos, have been frequently observed in both experiments and numerical simulations. [13][14][15][16][17][18][19] Different from the single period discharge, the current pulses in period-doubling and chaos discharges repeat at multiple applied voltage cycles or fluctuate stochastically.…”
Section: Introductionmentioning
confidence: 99%