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Titlebook: Atmospheric Tidal and Planetary Waves; Hans Volland Book 1988 Kluwer Academic Publishers 1988 Scale.Southern Oscillation.Storm.Tide.wind

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41#
發(fā)表于 2025-3-28 16:55:10 | 只看該作者
Basic Equations,more convenient, however, to separate the atmospheric wave motions from a hypothetical motionless or stationary background atmosphere. The wind can be divided into a source-free (no divergence) and a curl-free (no vorticity) component.
42#
發(fā)表于 2025-3-28 19:06:10 | 只看該作者
43#
發(fā)表于 2025-3-28 23:44:01 | 只看該作者
Internal Energy Sources and Sinks,e to be taken into account. These indirect sources and sinks are a consequence of our limited ability to deal with the full complex system Earth-Ocean-Atmosphere on all scales of motion and to account for all physical and chemical processes in the multi-component atmospheric gas. Instead, we try to
44#
發(fā)表于 2025-3-29 05:15:27 | 只看該作者
Horizontal Modal Structure,iction and Newtonian cooling as dissipation terms. In this approximation, which often simulates observed wave structure reasonably well, the waves can be considered as decoupled from each other. It is then possible to find general solutions of any time dependent disturbance by linearly superimposing
45#
發(fā)表于 2025-3-29 11:12:30 | 只看該作者
46#
發(fā)表于 2025-3-29 15:02:36 | 只看該作者
Nonlinear Wave Propagation,nonlinear loss processes such as turbulence and eddy heat conduction by Rayleigh friction and Newtonian cooling. However, even without these loss processes, the waves interfere with each other via the nonlinear advection terms in the equations of motion. This nonlinear coupling gives rise to new wav
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