THE RESONANT FREQUENCIES OF CAVITIES IN A MAGNETOIONIC MEDIUM
The resonant frequencies for a hollow cylindrical or spherical cavity in a magnetoionic medium are derived using a simple model in which the boundary of the cavity is sharp and the medium outside it is homogeneous and loss free, but anisotropic. The effects of electron temperature and of nonlinearity are ignored. The problem is complementary to a similar problem treated by Herlofsen (1951), who discussed the resonant frequencies of a uniform cylindrical or spherical mass of isotropic plasma surrounded by a vacuum. It is found that the resonant frequencies are not equal to the characteristic frequencies of the plasma as usually described by the formulae X = 1, X = 1 ± Y, but are more complicated functions of the plasma frequency and the electron gyrofrequency. It is concluded that, for a plasma sheath or cavity of any structure, with a sharp or gradual boundary region, the resonant frequencies will in general differ from the characteristic frequencies of the undisturbed plasma. For a cylindrical cavity the resonant frequencies depend upon the angle between the axis of the cavity and the constant magnetic field. The results may have applications to the interpretation of plasma "spikes" observed with space vehicles, and to the theory of the radar cross section of a space vehicle within the ionosphere.