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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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發(fā)表于 2025-3-25 03:58:10 | 只看該作者
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發(fā)表于 2025-3-25 11:04:12 | 只看該作者
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發(fā)表于 2025-3-25 17:38:37 | 只看該作者
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發(fā)表于 2025-3-25 20:01:45 | 只看該作者
Fusarium Head Blight in Latin Americamore 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.
26#
發(fā)表于 2025-3-26 02:14:32 | 只看該作者
https://doi.org/10.1007/978-94-007-7091-1 of the atmospheric gas is a complicated process that depends on the physical and chemical conditions of the atmosphere. Minor constituents like ozone or the ionospheric plasma play important roles in transferring solar energy into heat and momentum. Strictly speaking, one must solve a set of compli
27#
發(fā)表于 2025-3-26 08:19:46 | 只看該作者
Martha Díaz de Ackermann,Man Mohan Kohlie 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
28#
發(fā)表于 2025-3-26 11:31:28 | 只看該作者
29#
發(fā)表于 2025-3-26 13:23:24 | 只看該作者
Erlei M. Reis,Marcelo A. Carmona this, we have to solve the system of Equations (5.8). In the presence of a realistic background temperature with height dependent scale height and variable Brunt-V?is?l? frequency, this system can only be treated numerically. However, for an isothermal background atmosphere and constant dissipation
30#
發(fā)表于 2025-3-26 17:42:16 | 只看該作者
Erlei M. Reis,Marcelo A. Carmonanonlinear 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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