Inertial Stability and Tropical Cyclone DevelopmentSource: Journal of the Atmospheric Sciences:;1982:;Volume( 039 ):;issue: 008::page 1687DOI: 10.1175/1520-0469(1982)039<1687:ISATCD>2.0.CO;2Publisher: American Meteorological Society
Abstract: We consider the frictionless, axisymmetric, balanced flow occurring in a thermally forced vortex on an f-plane. Following Eliassen (1952) we derive the diagnostic equation for the forced secondary circulation. This equation contains the spatially varying coefficients A (static stability), B (baroclinity), C (inertial stability), and the thermal forcing Q. Assuming that A is a constant, B = 0, and that C and Q are piecewise constant functions of radius, we obtain analytical solutions for the forced secondary circulation. The solutions illustrate the following points. 1) For a given Q an increase in inertial stability leads to a decrease in the forced secondary circulation and a change in the radial distribution of local temperature change, with enhanced ??/?t; in the region of high inertial stability. 2) Lower tropospheric tangential wind accelerations are larger inside the radius of maximum wind, which leads to a collapse of the radius of maximum wind. 3) The fraction of Q which ends up as ??/?t; increases during the tropical cyclone development, particularly if the horizontal extent of Q is small and close to the region of high inertial stability. 4) One can regard the formation of an eye as a process which tends to stabilize the vortex since it removes Q from the protected, highly stable inner region.
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| contributor author | Schubert, Wayne H. | |
| contributor author | Hack, James J. | |
| date accessioned | 2017-06-09T14:23:17Z | |
| date available | 2017-06-09T14:23:17Z | |
| date copyright | 1982/08/01 | |
| date issued | 1982 | |
| identifier issn | 0022-4928 | |
| identifier other | ams-18402.pdf | |
| identifier uri | http://onlinelibrary.yabesh.ir/handle/yetl/4154404 | |
| description abstract | We consider the frictionless, axisymmetric, balanced flow occurring in a thermally forced vortex on an f-plane. Following Eliassen (1952) we derive the diagnostic equation for the forced secondary circulation. This equation contains the spatially varying coefficients A (static stability), B (baroclinity), C (inertial stability), and the thermal forcing Q. Assuming that A is a constant, B = 0, and that C and Q are piecewise constant functions of radius, we obtain analytical solutions for the forced secondary circulation. The solutions illustrate the following points. 1) For a given Q an increase in inertial stability leads to a decrease in the forced secondary circulation and a change in the radial distribution of local temperature change, with enhanced ??/?t; in the region of high inertial stability. 2) Lower tropospheric tangential wind accelerations are larger inside the radius of maximum wind, which leads to a collapse of the radius of maximum wind. 3) The fraction of Q which ends up as ??/?t; increases during the tropical cyclone development, particularly if the horizontal extent of Q is small and close to the region of high inertial stability. 4) One can regard the formation of an eye as a process which tends to stabilize the vortex since it removes Q from the protected, highly stable inner region. | |
| publisher | American Meteorological Society | |
| title | Inertial Stability and Tropical Cyclone Development | |
| type | Journal Paper | |
| journal volume | 39 | |
| journal issue | 8 | |
| journal title | Journal of the Atmospheric Sciences | |
| identifier doi | 10.1175/1520-0469(1982)039<1687:ISATCD>2.0.CO;2 | |
| journal fristpage | 1687 | |
| journal lastpage | 1697 | |
| tree | Journal of the Atmospheric Sciences:;1982:;Volume( 039 ):;issue: 008 | |
| contenttype | Fulltext |