2016
DOI: 10.1088/1009-0630/18/5/13
|View full text |Cite
|
Sign up to set email alerts
|

Volume Diffuse Dielectric Barrier Discharge Plasma Produced by Nanosecond High Voltage Pulse in Airflow

Abstract: Volume diffuse dielectric barrier discharge (DBD) plasma is produced in subsonic airflow by nanosecond high-voltage pulse power supply with a plate-to-plate discharge cell at 6 mm air gap length. The discharge images, optical emission spectra (OES), the applied voltage and current waveforms of the discharge at the changed airflow rates are obtained. When airflow rate is increased, the transition of the discharge mode and the variations of discharge intensity, breakdown characteristics and the temperature of th… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

1
15
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 19 publications
(16 citation statements)
references
References 30 publications
(23 reference statements)
1
15
0
Order By: Relevance
“…When the airflow is introduced between the electrodes, the charged particles are affected by the transport effect of airflow. These particles move along the direction of the incoming airflow or are even blown out the discharge area [2,3,15,44]. In this paper, the time between two pulses is about (0-3)×10 −4 s (PRF of 0-3800 Hz) and the characteristic time of the airflow through the electrodes is (0-8)×10 −4 s (electrode characteristic length/airflow velocity).…”
Section: Discussion Of the Nonlinearity Phenomena Of The Initiating A...mentioning
confidence: 81%
See 2 more Smart Citations
“…When the airflow is introduced between the electrodes, the charged particles are affected by the transport effect of airflow. These particles move along the direction of the incoming airflow or are even blown out the discharge area [2,3,15,44]. In this paper, the time between two pulses is about (0-3)×10 −4 s (PRF of 0-3800 Hz) and the characteristic time of the airflow through the electrodes is (0-8)×10 −4 s (electrode characteristic length/airflow velocity).…”
Section: Discussion Of the Nonlinearity Phenomena Of The Initiating A...mentioning
confidence: 81%
“…The influence of airflow on discharge working boundary has also received attention, mostly focusing on the study of the breakdown characteristics of discharge [6,7,[11][12][13][14][15][16][17][18][19][20]. The position of discharge breakdown moves along the airflow direction, because the airflow will transport the residual particles of the micro-discharge channels [7,11].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…As the discharge tends to reignite at the position where MD remnants accumulate, the redistribution of MD remnants can affect the space-time distribution of discharge filaments, [31] and even promote the transition from filamentary discharge to diffuse discharge at certain conditions. [32,33] It is, thus, worth exploring how to realize and maintain large-volume diffuse discharge in flowing air. Besides, the discharge uniformity at different cycles in flowing air has rarely been studied.…”
Section: Introductionmentioning
confidence: 99%
“…As the discharge tends to reignite at the position where MD remnants accumulate, the redistribution of MD remnants can affect the space–time distribution of discharge filaments, [ 31 ] and even promote the transition from filamentary discharge to diffuse discharge at certain conditions. [ 32,33 ]…”
Section: Introductionmentioning
confidence: 99%