2011
DOI: 10.1134/s1063784211010051
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Transition to the obstructed discharge and a sharp change in the voltage-current characteristic as a result of gas heating in a short (positive-column-free) high-pressure glow discharge

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Cited by 14 publications
(3 citation statements)
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“…Therefore, the breakdown can be triggered at an earlier moment, indicating a lower ϕ b with the rise of the air content in stage II. From equation (10), it also explains why V gb decreases as the air content increases in stage II, as shown in Fig. 6.…”
Section: ) Stage I: 50 Ppm-500 Ppmmentioning
confidence: 83%
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“…Therefore, the breakdown can be triggered at an earlier moment, indicating a lower ϕ b with the rise of the air content in stage II. From equation (10), it also explains why V gb decreases as the air content increases in stage II, as shown in Fig. 6.…”
Section: ) Stage I: 50 Ppm-500 Ppmmentioning
confidence: 83%
“…where ϕ b represents the phase corresponding to the moment of the first breakdown and ε r is the permittivity of the dielectric layer. From equation (10), we know that the increase of V gb implies the time delay of initial ignition. Thus, as the air content increases from 50 ppm to 500 ppm, the first breakdown is gradually delayed in stage I.…”
Section: ) Stage I: 50 Ppm-500 Ppmmentioning
confidence: 99%
“…This regime is unstable [32]. But at the same time, modeling based on the fluid approximation of plasma (as well as the analytical model of Engel and Steenbeck [61]) in one-dimensional and two-dimensional approximation gives an incident branch on the CVC in the region of low currents. It should be noted that in experiments both at low and high pressures, as well as in the framework of numerical calculations for discharges at low and medium pressures, oscillating modes of transition from the Townsend mode to the normal glow mode were reproduced [17,[63][64][65][66][67][68][69].…”
Section: Verification Model For Normal Glow Dischargementioning
confidence: 99%