Electron velocity distribution in a fully ionized plasma under the action of crossed electric and magnetic fields
Article
Received:
- 27 Downloads
Abstract
A fully ionized spatially homogeneous plasma is subjected to weak constant crossed electric and magnetic fields, and the velocity distribution function for the electrons is studied. The Fokker-Planck type expression for the Lorentz gas is employed for the collision term in the Boltzmann equation. This equation is solved by direct expansion and some conditions of convergence of this expansion are obtained.
Keywords
Magnetic Field Distribution Function Velocity Distribution Boltzmann Equation Electron Velocity
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
Preview
Unable to display preview. Download preview PDF.
References
- [1]Bernstein I. B., Trehan S. K.: Nucl. Fusion1 (1960), 3.Google Scholar
- [2]Kruskal M. D., Bernstein I. B.: Phys. Fluids7 (1964), 407.Google Scholar
- [3]Niu K.: J. Phys. Soc. Japan23 (1967), 608.Google Scholar
- [4]Dreicer H.: Phys. Rev.115 (1959), 238.Google Scholar
- [5]Gurevich A. V.: Zh. Exp. Teor. Fyz.39 (1960), 1296.Google Scholar
Copyright information
© Czechoslovak Academy of Sciences 1970