Abstract
The equations governing the quasi-one-dimensional unsteady motion of an ideal, inviscid, perfectly conducting compressible fluid, subjected to an oblique magnetic field, are linearized in the neighborhood of a known simple wave flow and weakly nonisentropic perturbations are considered. The perturbations superposed on simple wave flow in non-uniform ducts may then be determined by quadratures. Because of the arbitrary orientation of the magnetic field, both slow and fast simple waves may be considered. The author's previous work on the case of a transverse magnetic field and the nonmagnetic case is contained as a special case of the analysis.
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