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contributor authorSasamori, Takashi
contributor authorYoungblut, Carl E.
date accessioned2017-06-09T14:22:02Z
date available2017-06-09T14:22:02Z
date copyright1981/01/01
date issued1981
identifier issn0022-4928
identifier otherams-18063.pdf
identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4154027
description abstractA linear stability analysis was made for forced stationary planetary waves to supplement the theoretical interpretation on the large dissipative role of the transient motions, using simple quasi-geostrophic models on the midlatitude ?-plane. For the simplest model in which the nonlinear effect is truncated by a triad interaction, the stability criteria are given by a pair of inequalities, the first of which specifies the critical amplitude of the basic state wave and the second the difference between the longitudinal and latitudinal wavenumber which are required for the perturbation to be unstable. The analysis for the two-layer baroclinic atmosphere suggests that the perturbations superimposed on the basic state with wavenumber three are likely to be unstable. The growth rate calculated from the model is compared favorably to the dissipation rate of the stationary wave due to the transient motions analysed in Part I.
publisherAmerican Meteorological Society
titleThe Nonlinear Effects of Transient and Stationary Eddies on the Winter Mean Circulation. Part II: The Stability of Stationary Waves
typeJournal Paper
journal volume38
journal issue1
journal titleJournal of the Atmospheric Sciences
identifier doi10.1175/1520-0469(1981)038<0087:TNEOTA>2.0.CO;2
journal fristpage87
journal lastpage96
treeJournal of the Atmospheric Sciences:;1981:;Volume( 038 ):;issue: 001
contenttypeFulltext


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