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Numerical simulation of runaway electrons generation in sulfur hexafluoride
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10.1063/1.3676256
/content/aip/journal/jap/111/1/10.1063/1.3676256
http://aip.metastore.ingenta.com/content/aip/journal/jap/111/1/10.1063/1.3676256
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(Color online) Distributions of potential (a), of negative ions SF6 (b), and of difference between negative and positive charge densities (c, d) in the CA gap at different times; ϕ 0 = 120 kV, T = 1 ns, P = 105 Pa.

Image of FIG. 2.
FIG. 2.

(Color online) (a) Time dependence of the emitted dNem /dt and total number of the electrons Ne in the CA gap; (b) time dependence of the numbers of ionizations and attachments per time step; ϕ 0 = 120 kV, T = 1 ns, P = 105 Pa.

Image of FIG. 3.
FIG. 3.

(Color online) (a) Time dependence of the quantity of the RAE with ɛe  ≥ 1 and ɛe ≥20 keV inside the CA gap; (b) space distribution of electrons with ɛe ≥ 20 keV at different times; ϕ 0 = 120 kV, T = 1 ns, P = 105 Pa.

Image of FIG. 4.
FIG. 4.

(Color online) Time dependence of RAE number for different amplitudes of cathode potential: (a) NRAE with ɛe ≥ 1 keV, and (b) NRAE with ɛe ≥20 keV; (c) EEDF at the anode at t = 0.5 ns for different amplitudes of cathode potential; T = 1 ns; P = 105 Pa.

Image of FIG. 5.
FIG. 5.

(Color online) Time dependence of the RAE number with ɛe ≥20 keV at different SF6 pressures (a) and different HV pulse rise times (c) for T = 1 ns and ϕ 0 = 120 kV; EEDF at the anode at different SF6 pressures (b) and different HV rise times (d) for P = 105 Pa and ϕ 0 = 120 kV.

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/content/aip/journal/jap/111/1/10.1063/1.3676256
2012-01-12
2014-04-25
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Numerical simulation of runaway electrons generation in sulfur hexafluoride
http://aip.metastore.ingenta.com/content/aip/journal/jap/111/1/10.1063/1.3676256
10.1063/1.3676256
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