On the Forcing of Time-Mean Flows by Transient, Small-Amplitude EddiesSource: Journal of the Atmospheric Sciences:;1989:;Volume( 047 ):;issue: 015::page 1837Author:Andrews, David G.
DOI: 10.1175/1520-0469(1990)047<1837:OTFOTM>2.0.CO;2Publisher: American Meteorological Society
Abstract: Small-amplitude, transient disturbances to a steady, zonally asymmetric basic state are considered, for barotropic (or baroclinic, quasi-geostrophic) flow on a beta-plane. An explicit expression is derived for the eddy vorticity (or potential vorticity) flux in terms of the basic velocity and basic vorticity (or potential vorticity), and transient and nonconservative eddy effects, plus an identically nondivergent term. The divergence of the time mean of this flux provides the forcing of the time-mean flow. The theory generalizes a ?nonacceleration? result due to Plumb. In the case of conservative flow, the relevant expressions can be obtained in Eulerian form; however, for nonconservative flow it appears to be necessary to introduce the Lagrangian fluid particle displacements. Possible applications of the theory to the interpretation of atmospheric and model data are mentioned.
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contributor author | Andrews, David G. | |
date accessioned | 2017-06-09T14:29:50Z | |
date available | 2017-06-09T14:29:50Z | |
date copyright | 1990/08/01 | |
date issued | 1989 | |
identifier issn | 0022-4928 | |
identifier other | ams-20361.pdf | |
identifier uri | http://onlinelibrary.yabesh.ir/handle/yetl/4156581 | |
description abstract | Small-amplitude, transient disturbances to a steady, zonally asymmetric basic state are considered, for barotropic (or baroclinic, quasi-geostrophic) flow on a beta-plane. An explicit expression is derived for the eddy vorticity (or potential vorticity) flux in terms of the basic velocity and basic vorticity (or potential vorticity), and transient and nonconservative eddy effects, plus an identically nondivergent term. The divergence of the time mean of this flux provides the forcing of the time-mean flow. The theory generalizes a ?nonacceleration? result due to Plumb. In the case of conservative flow, the relevant expressions can be obtained in Eulerian form; however, for nonconservative flow it appears to be necessary to introduce the Lagrangian fluid particle displacements. Possible applications of the theory to the interpretation of atmospheric and model data are mentioned. | |
publisher | American Meteorological Society | |
title | On the Forcing of Time-Mean Flows by Transient, Small-Amplitude Eddies | |
type | Journal Paper | |
journal volume | 47 | |
journal issue | 15 | |
journal title | Journal of the Atmospheric Sciences | |
identifier doi | 10.1175/1520-0469(1990)047<1837:OTFOTM>2.0.CO;2 | |
journal fristpage | 1837 | |
journal lastpage | 1844 | |
tree | Journal of the Atmospheric Sciences:;1989:;Volume( 047 ):;issue: 015 | |
contenttype | Fulltext |