2002
DOI: 10.1088/0022-3727/35/8/306
|View full text |Cite
|
Sign up to set email alerts
|

Influence of interaction between charged particles and dielectric surface over a homogeneous barrier discharge in nitrogen

Abstract: A fluid model of the homogeneous barrier discharge is constructed for nitrogen at atmospheric pressure. The primary excitation and ionization processes specific for this discharge are pointed out. The calculations show that, in a wide range of external conditions, the homogeneous barrier discharge in nitrogen has a form of Townsend discharge which is easy to study. The influence of different mechanisms of electron emission from dielectric barriers and surface recombination over the electrical characteristics o… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

5
190
0
3

Year Published

2009
2009
2021
2021

Publication Types

Select...
7
3

Relationship

0
10

Authors

Journals

citations
Cited by 288 publications
(198 citation statements)
references
References 18 publications
5
190
0
3
Order By: Relevance
“…2): z 2 = 6, z 3 = 8, y 1 = −3, y 2 = −1, y e = 5, and y ∞ = 7 mm. The following physical parameters were used in calculations: the pressure and the temperature of air p = 2.6 · 10 4 Pa and T = 223 K, the amplitude and the frequency of the applied harmonic voltage ϕ 0 = 5 kV and f = 10 kHz, the dielectric con- stants of the insulation layers ε 1 = 2.1 (Te §on) and ε 2 = 3.5 (Kapton), the coe©cients of the secondary ion electron emission on dielectric and electrode surfaces equal 0.05, the frequency of electron desorption from dielectric surface equals 5 kHz [19], and the electron ion recombination coe©cient on dielectric surface equals 10 −7 cm 2 /s [19].…”
Section: 5mentioning
confidence: 99%
“…2): z 2 = 6, z 3 = 8, y 1 = −3, y 2 = −1, y e = 5, and y ∞ = 7 mm. The following physical parameters were used in calculations: the pressure and the temperature of air p = 2.6 · 10 4 Pa and T = 223 K, the amplitude and the frequency of the applied harmonic voltage ϕ 0 = 5 kV and f = 10 kHz, the dielectric con- stants of the insulation layers ε 1 = 2.1 (Te §on) and ε 2 = 3.5 (Kapton), the coe©cients of the secondary ion electron emission on dielectric and electrode surfaces equal 0.05, the frequency of electron desorption from dielectric surface equals 5 kHz [19], and the electron ion recombination coe©cient on dielectric surface equals 10 −7 cm 2 /s [19].…”
Section: 5mentioning
confidence: 99%
“…There have been several numerical studies to investigate the influence of applied voltage parameters, gap width, electrode parameters, materials, and width of the dielectric layer, on discharge performance and energy efficiency of the DBDs. [13][14][15][16] However, most of these studies have been performed on DBDs between parallel-plate electrodes, whereas diagnostics on DBDs with co-axial electrode configuration are comparatively less. [17][18][19] Most of the applications of nonthermal plasma used for decomposing gaseous pollutants are performed in co-axial DBD reactors.…”
Section: Introductionmentioning
confidence: 99%
“…suggested that many seed electrons necessary for a uniform/homogeneous discharge could be produced by 37 electrons trapped on the dielectric surface [3]. Recently, long lifetime of charge trapping on alumina used as 38 dielectric in DBD plasma has been evidenced by Thermally stimulated current [1] and Thermoluminescence 39 technique [4].…”
mentioning
confidence: 99%