2005
DOI: 10.1016/j.molliq.2004.07.065
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Manifestation of polarization effects in dusty plasma

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Cited by 1 publication
(2 citation statements)
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“…In the model of statistical electroneutral cells for a rarefied plasmosol (a system of emitting macroparticles, buffer gas, and electrons [5][6][7][8][9][10]), the distribution of a self-consistent electrostatic potential πœ™(π‘Ÿ) in the free cell volume, 𝐢 β€² πœ‰ = 𝐢 𝑧 πœ‰ βˆ’ 𝑉 𝑝 , is described by the Poisson-Boltzmann equation, and the solution of the latter is expressed by the formula…”
Section: Local Electrostatic Field Of Plasmosolmentioning
confidence: 99%
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“…In the model of statistical electroneutral cells for a rarefied plasmosol (a system of emitting macroparticles, buffer gas, and electrons [5][6][7][8][9][10]), the distribution of a self-consistent electrostatic potential πœ™(π‘Ÿ) in the free cell volume, 𝐢 β€² πœ‰ = 𝐢 𝑧 πœ‰ βˆ’ 𝑉 𝑝 , is described by the Poisson-Boltzmann equation, and the solution of the latter is expressed by the formula…”
Section: Local Electrostatic Field Of Plasmosolmentioning
confidence: 99%
“…The electron subsystem quickly "traces" changes in the local selfconsistent electrostatic field in the LTE regions of a plasma system. The consideration of electron-ion processes in HPFs based on the model of quasi-neutral plasma cells and carried out in the framework of the "adiabatic approximation analog" opens new capabilities for the research and description of braking radiation emission in the LTE regions of nonequilibrium plasma systems [6][7][8][9][10]. In particular, monitoring the evolution of braking radiation and the intensity of its "particle" component in the signal emitted by heterogeneous plasma with a condensed dispersed phase (CDP), it is possible to study the parameters of the relevant heavy subsystem, i.e.…”
Section: Introductionmentioning
confidence: 99%