Fig. 11

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Perturbation energy E(t) for the radiating modes created by incoming inertial waves with various wavenumber sets (kxR0, kzR0; panel a). The energy is normalized by the initial inertial-wave energy Eiw(t = 0) for comparison among different cases. Panel b displays the time rates for perturbation energy ∂E/∂t (solid), base shear contribution Pb (dashed), viscous dissipation Dv (dotted), and power injected by the incoming inertial wave–vortex interaction Pf (dash-dot) for the case with (kxR0, kzR0) = (1, 1). The energy rates are normalized by fEiw(0) for nondimensionalization.
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