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Christopher G. Kruse and Ronald B. Smith

.g., viscosity) and diabatic heating (for a complete description, see Andrews and Mcintyre 1978 ; Bühler 2009 ). The x pseudomomentum is a wave quantity that quantifies nondissipative wave forcing of the Lagrangian-mean flow. The last term in Eq. (5) is nonzero when waves are being generated or dissipated. In the present study, this term quantifies the dissipative forcing of the Lagrangian-mean flow. Equation (5) is valid for waves of finite amplitude. For small-amplitude, slowly-varying waves in an

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