The momentum transfer collision cross sections, qₘ, of nitrogen molecules for slow electrons and the mean fractional electron energy loss, λ, in these collisions have been determined by the method of microwave interaction in gaseous discharge plasmas. The mean energy of the electron was varied from 0.04 to 0.46 ev. The cross section, qₘ, was found to be {~}17×{}10^-16 cm² at 0.04 ev. It decreases to {~}8×{}10^-16 cm² at 0.46 ev. The mean fractional energy loss of the electron, λ, in the energy range investigated, was found to be {~}5.5 in units of 2m/M. These results lend strong support to the theory of rotational excitation of N₂ by slow electrons.
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Anderson et al. (1956) studied this question.
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