2009
DOI: 10.1016/j.elstat.2008.12.001
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Electrical characterization of dielectric barrier discharge driven by repetitive nanosecond pulses in atmospheric air

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Cited by 58 publications
(24 citation statements)
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“…It can be found that the negative peak of the discharge current was much smaller than the positive peak, which was different from the results of using semiconductor opening switch and different electrical parameters of the power supply [39,40]. …”
Section: Voltage and Current Waveformcontrasting
confidence: 60%
“…It can be found that the negative peak of the discharge current was much smaller than the positive peak, which was different from the results of using semiconductor opening switch and different electrical parameters of the power supply [39,40]. …”
Section: Voltage and Current Waveformcontrasting
confidence: 60%
“…Many experimental and theoretical studies or simulations have been presented. Some these include electrical characteristics, the transition between filamentary and homogeneous discharge modes, comparison of high-voltage ac and pulsed discharge and so on [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33]. Pulsed power generators, however, vary widely in performance according to load requirements, different results may be obtained from using various pulsed power generators and kinds of discharge configurations [4-6, 13, 14, 17, 19, 21, 29, 31].…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, it was observed that the secondary discharge at the falling edge depended on surface properties of the dielectric barrier [25]. The driving power supply and discharge configuration are the key factors determining discharge characteristic [26][27][28][29][30][31][32][33][34][35]. APGD or glow-like homogeneous discharge can be produced by various pulsed power source, such as inductive energy storage pulsed power applied to a needlearray electrode in nitrogen [26], sphere-to-plane discharge configuration excitated by a decay pulse source using double spark gaps [27], time-variable negative pulses used in two-planar electrodes [28].…”
Section: Introductionmentioning
confidence: 99%
“…Commonly used materials are glass and alumina ceramic. Due to the thickness, they exhibit high dielectric breakdown voltages [25], [26]. Theoretically, the initiation voltage, i.e., the voltage that initiates the ozone generation, is close to its breakdown voltage; for a typical chamber using glass as dielectric with discharge gap of 1 mm, the initiation voltage is about 10-20 kV [4], [27].…”
mentioning
confidence: 99%