Large radiation losses in the electron energy balance equation due to electron impact excitation can cause the parallel scale length to become small enough that a short mean-free path expansion becomes questionable for the high-speed tail electrons. It then becomes necessary to limit the parallel electron heat flux so that it remains below its free-streaming value nT3/2/m, where n, T, and m are the electron density, temperature, and mass. A Boltzmann inelastic scattering col- lision operator is adopted to investigate whether electron impact excitation can lead to a self-consistent flux limit by depleting the electron tail.
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Catto et al. (1996) studied this question.
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