Abstract
Electron-ion bremsstrahlung in a weakly ionized uniform non-stationary plasma (in the absence of external fields) is investigated. The momentum transfer frequencyν 1 is assumed to be velocity independent (H2 and He plasmas). The respective Fokker-Planck equation is applied for two initial electron distributions: maxwellian with the temperatureT 0, and delta distribution (C δ(ν−ν 0)). The results are expressed analytically. In the case of initial delta distribution a different behaviour of intensity is found forq (ratio of final and initial temperatures) more or less than 3/2. From the calculations one may deduce that fors=(2mν1 t/M)≳5 the difference between equilibrium and non-equilibrium intensities becomes insignificant.
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Kvasnica, J. Electron-ion bremsstrahlung of a non-equilibrium plasma. Czech J Phys 26, 646–650 (1976). https://doi.org/10.1007/BF01589594
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DOI: https://doi.org/10.1007/BF01589594