Movable CISKSource: Journal of the Atmospheric Sciences:;1973:;Volume( 030 ):;issue: 001::page 50Author:Charney, J.
DOI: 10.1175/1520-0469(1973)030<0050:MC>2.0.CO;2Publisher: American Meteorological Society
Abstract: The analysis of Conditional Instability of the Second Kind (CISK) for a resting atmosphere leads to a maximum growth rate at zero width of the rain area. However, if the process takes place in a uniform current moving relative to the ground with a velocity ?, and the width of the rain area is 2a, an Ekman boundary layer cannot be established in the rain area when 2a/f, where f is the Coriolis parameter. It is shown that the incomplete development of the frictional boundary layer in this area leads to a maximum growth rate at a ≈300 km, and this seems to be a reasonable value for the half-width of a cloud cluster in a tropical depression or of the Intertropical Convergence Zone itself. The efolding time is of the order of half the spin- up time f?1E?½ where E is the Ekman number, i.e., about 2 days at 10°.
|
Collections
Show full item record
contributor author | Charney, J. | |
date accessioned | 2017-06-09T14:16:44Z | |
date available | 2017-06-09T14:16:44Z | |
date copyright | 1973/01/01 | |
date issued | 1973 | |
identifier issn | 0022-4928 | |
identifier other | ams-16294.pdf | |
identifier uri | http://onlinelibrary.yabesh.ir/handle/yetl/4152061 | |
description abstract | The analysis of Conditional Instability of the Second Kind (CISK) for a resting atmosphere leads to a maximum growth rate at zero width of the rain area. However, if the process takes place in a uniform current moving relative to the ground with a velocity ?, and the width of the rain area is 2a, an Ekman boundary layer cannot be established in the rain area when 2a/f, where f is the Coriolis parameter. It is shown that the incomplete development of the frictional boundary layer in this area leads to a maximum growth rate at a ≈300 km, and this seems to be a reasonable value for the half-width of a cloud cluster in a tropical depression or of the Intertropical Convergence Zone itself. The efolding time is of the order of half the spin- up time f?1E?½ where E is the Ekman number, i.e., about 2 days at 10°. | |
publisher | American Meteorological Society | |
title | Movable CISK | |
type | Journal Paper | |
journal volume | 30 | |
journal issue | 1 | |
journal title | Journal of the Atmospheric Sciences | |
identifier doi | 10.1175/1520-0469(1973)030<0050:MC>2.0.CO;2 | |
journal fristpage | 50 | |
journal lastpage | 52 | |
tree | Journal of the Atmospheric Sciences:;1973:;Volume( 030 ):;issue: 001 | |
contenttype | Fulltext |