The propagation of internal gravity waves in a shear flow in a rotating fluid is examined for the case when the rotation vector is inclined to the vertical. It is shown that internal gravity waves approaching a critical level, where ω*, the Doppler-shifted frequency, equals 2Ω V , the vertical component of the Coriolis parameter, will be either transmitted or absorbed according as \[ W_gω*2Ω_V\{m(U_z + 2Ω_H)-lV_z\} 0; \] here W g is the vertical group velocity, 2Ω H is the horizontal component of the Coriolis parameter, l and m are the easterly and northerly wavenumber components, and U z and V z are the shear rates of the easterly and northerly components of the mean flow. Between critical levels, wave action flux is conserved. However, for a wave absorbed at a critical level, the wave action flux is attenuated by a factor exp { − 2π| m ( U z + 2Ω H ) − lV z ]/( lU z + mV z )|}. The phenomenon is also analysed using a WKBJ approximation.
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Roger Grimshaw (1975) studied this question.
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