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contributor authorHyun, Jae Min
contributor authorPeskin, Richard L.
date accessioned2017-06-09T14:19:12Z
date available2017-06-09T14:19:12Z
date copyright1976/11/01
date issued1976
identifier issn0022-4928
identifier otherams-17175.pdf
identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4153040
description abstractAn analytical study is made of the baroclinic instability problem for a zonal wind U (z), by modifying the Eady model through relaxation of the shallow-layer approximation. The linearized perturbation equation is derived, including the mass-divergence effect in the continuity equation and the non-hydrostatic effect in the vertical momentum equation. When U (z) = constant, the non-hydrostatic effect decreases the effective propagation speeds of wave having short horizontal wavelengths. Assuming that the zonal current velocity profile is linear, two limiting cases are treated (i.e., the geostrophic-type instability limit and the symmetric-type instability limit). For the case of the geostrophic-type instability limit, the mass-divergence effect seems to reduce primarily the wave propagation speeds, while the unstable wave growth rates are decreased by both the mass-divergence and the non-hydrostatic effects. However, for the case of the symmetric-type instability limit, the mass-divergence effect is quite mild, but the non-hydrostatic effect strongly affects the unstable wave growth rates.
publisherAmerican Meteorological Society
titleBaroclinic Instabilities of a Deep Fluid
typeJournal Paper
journal volume33
journal issue11
journal titleJournal of the Atmospheric Sciences
identifier doi10.1175/1520-0469(1976)033<2054:BIOADF>2.0.CO;2
journal fristpage2054
journal lastpage2065
treeJournal of the Atmospheric Sciences:;1976:;Volume( 033 ):;issue: 011
contenttypeFulltext


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