Abstract

The collision frequencies for use in the continuum momentum equation are found for low energy electrons in N 2 and O 2 and for the polarization interaction between ions and neutral molecules; consideration is given to the case of low-frequency transport phenomena in a weakly ionized ionospheric plasma. For the electrons, the method of assuming a displaced Maxwellian velocity distribution function is compared with the method of obtaining transport coefficients from the linearized Boltzmann equation. It is found that the method of assuming a displaced Maxwellian distribution for the electrons is not a good approximation, and reasons why this is so are given.

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