2017
DOI: 10.1134/s1990793117010183
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Diffusion-path approximation in nonlocal electron kinetics

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Cited by 7 publications
(6 citation statements)
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“…The formation of distribution function is caused by relatively slow acceleration of electrons in the longitudinal field and the fast electron transits in radial potential. Under these conditions, the coefficients of the kinetic equation can be averaged over the radial transits, due to the feasibility of the diffusion approximation [26]. When the radial potential varies weakly along the radial axies and rises substantially in the near-wall region, the averaged coefficients differ little from their values on the axis of the tube.…”
Section: Dust Particle Charging In the Stratified Glow Dischargementioning
confidence: 99%
“…The formation of distribution function is caused by relatively slow acceleration of electrons in the longitudinal field and the fast electron transits in radial potential. Under these conditions, the coefficients of the kinetic equation can be averaged over the radial transits, due to the feasibility of the diffusion approximation [26]. When the radial potential varies weakly along the radial axies and rises substantially in the near-wall region, the averaged coefficients differ little from their values on the axis of the tube.…”
Section: Dust Particle Charging In the Stratified Glow Dischargementioning
confidence: 99%
“…However, in [22], equation (14) was obtained for a local approximation, as terms with spatial gradients were not considered when deriving equation (14). Conversely, numerous studies [15,[23][24][25][26][27][28][29][30][31] have revealed that at low pressures, for electrons with energies below the wall potential e , w j the EDF depends only on the total energy ε, even in the inelastic energy range. Thus, equation (14) cannot remain in a nonlocal mode with a non-uniform profile of N m .…”
Section: Resultsmentioning
confidence: 99%
“…) is strongly compressed to the axis and declines as it approaches the periphery. A peaked profile of reaction rate constants for an electron-induced process with a large energy threshold is characteristic of a nonlocal EDF [23][24][25][26][27].…”
Section: Resultsmentioning
confidence: 99%
“…where n ea ex and n ea i are excitation and ionization collision frequencies; U ex and U i are excitation and ionization threshold energy, and which are set as 11.72 eV and 15.6 eV, respectively, for argon plasma. The electron-neutral cross sections are from [34].…”
Section: Electron Collisions Terms For the Kinetic Equationmentioning
confidence: 99%