Abstract
Macroscopic parameters, such as drift velocity, diffusion, ionization, and attachment coefficients, used to describe the development of a discharge are normally measured in a swarm-type experiment (Huxley and Crompton, 1974). To analyze these experiments, we must assume that the electrons have reached an equilibrium hydrodynamic state so that their behavior after a sufficiently long time is such that the distribution function f(r,v,t,) (r, v and t are the position and velocity vectors and the time, respectively) can be considered a function of the density n(r,t). The transport parameters are then time and position independent (Kumar et al., 1980). In a great number of cases, the equilibrium regime effectively exists, and the preceding hypothesis is perfectly valid. Nevertheless, even if sufficient time has elapsed for the swarm to reach
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Segur, P., Yousfi, M., Boeuf, J.P., Marode, E., Davies, A.J., Evans, J.G. (1983). The Microscopic Treatment of Nonequilibrium Regions in a Weakly Ionized Gas. In: Kunhardt, E.E., Luessen, L.H. (eds) Electrical Breakdown and Discharges in Gases. NATO Advanced Science Institutes Series, vol 89a. Springer, Boston, MA. https://doi.org/10.1007/978-1-4684-4409-4_12
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DOI: https://doi.org/10.1007/978-1-4684-4409-4_12
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