Nonlinear wave-activity conservation laws and Hamiltonian structure for the two-dimensional anelastic equations

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Abstract

Exact, finite-amplitude, local wave-activity conservation laws are derived for disturbances to steady flows in the context of the two-dimensional anelastic equations. The conservation laws are expressed entirely in terms of Eulerian quantities, and have the property that, in the limit of a small-amplitude, slowly varying, monochromatic wave train, the wave-activity density A and flux F, averaged over phase, satify F=cgA cg is the group velocity of the waves. For nonparallel steady flows, the only conserved wave activity is a form of disturbance pseudoenergy; when the steady flow is parallel, there is in addition a conservation law for the disturbance pseudomomentum. -from Authors

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Scinocca, J. F., & Shepherd, T. G. (1992). Nonlinear wave-activity conservation laws and Hamiltonian structure for the two-dimensional anelastic equations. Journal of the Atmospheric Sciences, 49(1), 5–27. https://doi.org/10.1175/1520-0469(1992)049<0005:nwacla>2.0.co;2

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