2012
DOI: 10.1002/eej.21253
|View full text |Cite
|
Sign up to set email alerts
|

Generation of uniform discharge by dielectric barrier discharge device in atmospheric‐pressure air

Abstract: We found that the generation of a uniform discharge in atmospheric-pressure air was possible in the frequency range from 32 Hz to 1.1 kHz using alumina as a barrier material of the DBD (Dielectric Barrier Discharge) device. We also found that there is a voltage domain for the generation of the uniform discharge. The domain becomes wider with the increase of the frequency. If the applied voltage is slightly higher than the upper limit voltage of stable generation of a uniform discharge, the uniform discharge ch… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
3
0

Year Published

2014
2014
2023
2023

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 8 publications
(4 citation statements)
references
References 10 publications
1
3
0
Order By: Relevance
“…The slope of (2) increases during the discharge and has a slight bulge compared to slope (4), as seen in figure 5(b). Differences between halfcycles in asymmetric DBD configurations have been observed previously by Osawa et al and Stollenwerk et al; the former observing alternating Townsend and filamentary discharges by using alumina and soda-glass on opposing electrodes, the latter observing offsets in the charge accumulation between half-cycles on a BSO crystal acting as the barrier on one electrode and ITO on the other [27][28][29]. Similar effects may be at play here and only the more constant slope of ( 4) is used to determine the effective dielectric capacitance.…”
Section: Capacitances From the Q-v Parallelogramssupporting
confidence: 60%
“…The slope of (2) increases during the discharge and has a slight bulge compared to slope (4), as seen in figure 5(b). Differences between halfcycles in asymmetric DBD configurations have been observed previously by Osawa et al and Stollenwerk et al; the former observing alternating Townsend and filamentary discharges by using alumina and soda-glass on opposing electrodes, the latter observing offsets in the charge accumulation between half-cycles on a BSO crystal acting as the barrier on one electrode and ITO on the other [27][28][29]. Similar effects may be at play here and only the more constant slope of ( 4) is used to determine the effective dielectric capacitance.…”
Section: Capacitances From the Q-v Parallelogramssupporting
confidence: 60%
“…Looking at the figure more precisely, it can be seen that the inception of the discharges became faster with the increase of O 2 content. Gap voltage during discharge can be calculated from the difference of voltages applied to the DBD device and to the barrier plates [14]. The gap voltages thus calculated are also shown in Figure 2a.…”
Section: Methodsmentioning
confidence: 99%
“…This explains the intensive effort of the plasma community to invent novel DBD configurations and perform experimental and theoretical research on DBD plasma regimes. The numerous original papers and comprehensive reviews relevant to these topics [29][30][31][32][33][34][35][36][37][38][39][40] can serve as an evidence for this statement.…”
Section: Introductionmentioning
confidence: 93%