2016
DOI: 10.1063/1.4959172
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Fluid modeling of a high-voltage nanosecond pulsed xenon microdischarge

Abstract: A computational modeling study of high-voltage nanosecond pulsed microdischarge in xenon gas at 10 atm is presented. The discharge is observed to develop as two streamers originating from the cathode and the anode, and propagating toward each other until they merge to form a single continuous discharge channel. The peak plasma density obtained in the simulations is ∼1024 m−3, i.e., the ionization degree of plasma does not exceed 1%. The influence of the initial gas pre-ionization is established. It is seen tha… Show more

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Cited by 18 publications
(6 citation statements)
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“…The high energy tail region can be attributed to runaway [32,33] secondary electrons that gain significant energy while traveling across the sheath and these electrons extend well into the quasi-neutral region in the microplasmas simulated in this work. Also, the PIC-MCC EEPFs could possibly be described by a bi-Maxwellian distribution with two characteristic temperatures and formulating multi-temperature models could be an important direction in improving the accuracy of continuum simulations of DC microplasma devices that are expected to have significant secondary electron emission.…”
Section: Effect Of Pd At Constant Gap Sizementioning
confidence: 68%
“…The high energy tail region can be attributed to runaway [32,33] secondary electrons that gain significant energy while traveling across the sheath and these electrons extend well into the quasi-neutral region in the microplasmas simulated in this work. Also, the PIC-MCC EEPFs could possibly be described by a bi-Maxwellian distribution with two characteristic temperatures and formulating multi-temperature models could be an important direction in improving the accuracy of continuum simulations of DC microplasma devices that are expected to have significant secondary electron emission.…”
Section: Effect Of Pd At Constant Gap Sizementioning
confidence: 68%
“…13,14 Levko and Raja conducted a fluid modeling of nanosecond pulsed xenon micro-discharge with sphericalprotrusion electrodes. 15 It was previously realized that the discharge behavior depends strongly not only on the cathode dimension, the working gas, or the incident power like in the low-pressure cathodes but also on the electrode material, surface roughness, and protrusions. 16,17 As for the steady-state microdischarges at atmospheric pressure, the sheath thickness plays a significant role in the discharge properties, which would be largely affected by the electric field enhancement due to the presence of the surface protrusion.…”
Section: Introductionmentioning
confidence: 99%
“…The field emission is ignored since the maximum effective electric field is much smaller than the field emission threshold (10 9 V/m). 37,38 The discharge is sustained by the ion-impact secondary electron emission from the cathode. The normal flux of electrons emitted by the cathode is related to the flux of incident ions by an effective secondary emission coefficient c eff , which is fixed at 0.1.…”
mentioning
confidence: 99%