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.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.