2007
DOI: 10.1088/0022-3727/40/3/015
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Dynamics of multichannel and quasi-homogeneous sliding discharge formation in rare gases

Abstract: Results of experiments with Ne, Ar and Xe as well as computer simulations are presented, aimed at testing an earlier proposed model of temporal dynamics of multichannel structure development in a pulsed high-current sliding gas discharge. The obtained and discussed experimental data include the values of an averaged channel radius, the pulsed near-surface breakdown voltage, the saturated spark resistance, the spatial structure of spark channels registered photographically under different discharge voltages and… Show more

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Cited by 15 publications
(29 citation statements)
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“…The experimental value of electron mobility in argon ͑ e p = 0.23ϫ 10 6 cm 2 Torr/ V s⇒ e = 0.03 m 2 / V s͒ is obtained from Ref. 15. Using Eq.…”
Section: ͑1͒mentioning
confidence: 99%
“…The experimental value of electron mobility in argon ͑ e p = 0.23ϫ 10 6 cm 2 Torr/ V s⇒ e = 0.03 m 2 / V s͒ is obtained from Ref. 15. Using Eq.…”
Section: ͑1͒mentioning
confidence: 99%
“…Figure 2 shows the applied voltage and discharge current waveforms obtained in APPJ with electrode distance 80 mm, applied voltage 4:5 kV, and resistance 10 kΩ. Electron density can be estimated from the measured value of current density according to the relation [17].…”
Section: Resultsmentioning
confidence: 99%
“…Herein, we follow Sarani et al and use for current density the formula J=nefalse(eμEfalse) so that ne=J/false(eμEfalse) where, e is the elementary charge. For the electron mobility we use the value μ=3×102m2/false(Vsfalse); the strength of the electric field E=ΔV/del is calculated by taking ΔV=5 kV and del=20 mm while the current density is calculated using J = I/A. Herein, we take for the current I = 3 mA while A=1/4πD2 with D = 0.2 mm.…”
Section: Resultsmentioning
confidence: 99%