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Wave Propagation in a Non-Maxwellian, Magnetoactive, Nonlinear Plasma
Robert J. Papa
Richard E. Haskell
出版
Air Force Cambridge Research Laboratories, Office of Aerospace Research, United States Air Force
, 1966
URL
http://books.google.com.hk/books?id=_aWmqzY0lOgC&hl=&source=gbs_api
EBook
FULL_PUBLIC_DOMAIN
註釋
Expressions for the components of a nonlinear ac conductivity tensor have been derived - corresponding to a temperate, weakly ionized, lossy magnetoplsma. The electrical conductivity tensor is nonlinear because its components are functions of the isotropic part of the electron velocity distribution function f, where f depends upon the amplitude and polarization of the local rf field By diagonalizing the conductivity tensor and referring Maxwell's field equations to the principal co-ordinate directions, it is shown that an elliptically polarized em wave normally incident upon an inhomogeneous magnetoplasma slab will launch only a right-hand and left-hand wave into the plasma if both the dc magnetic field and the electron density gradients are perpendicular to the interfaces. The net reflection transmission coefficients for left-hand and right-hand modes are computed using a Runge-Kutta numerical integration procedure. For low power levels, the right-hand and left-hand waves propagate independently of one another. For high field intensities, the propagation of the right-hand mode depends upon the amplitude of the left-hand mode, and vice versa. Reflection and transmission coefficients are presented as a function of normalized plasma parameters. (Author).