Turbulence in the middle atmosphere: A review

Descripción del Articulo

The stratosphere is characterized for being highly statically stable. lt takes considerable energy to interchange parcels of air from different altitudes; thus, turbulence is normally inhibited, Wind shears of the order of 40 m/sec per kilometer are necessary to overcome the stabilizing effect of ne...

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Detalles Bibliográficos
Autor: Woodman Pollitt, Ronald Francisco
Formato: objeto de conferencia
Fecha de Publicación:1980
Institución:Instituto Geofísico del Perú
Repositorio:IGP-Institucional
Lenguaje:inglés
OAI Identifier:oai:repositorio.igp.gob.pe:20.500.12816/579
Enlace del recurso:http://hdl.handle.net/20.500.12816/579
Nivel de acceso:acceso abierto
Materia:Stratosphere
Turbulence
Stratospheric winds
http://purl.org/pe-repo/ocde/ford#1.05.01
Descripción
Sumario:The stratosphere is characterized for being highly statically stable. lt takes considerable energy to interchange parcels of air from different altitudes; thus, turbulence is normally inhibited, Wind shears of the order of 40 m/sec per kilometer are necessary to overcome the stabilizing effect of negative buoyancy if turbulence is to occur. Shears close to these values do exist in narrow but horizontally exten­sive layers as a consequence of internal gravity waves and the two­dimensional (horizontal) turbulent character of mesoscale stratospheric winds. Shorter wavelength waves, superimposed on these shears, make the local shear exceed the threshold (Richardson number < 0.25) for Kelvin­Helmholtz instabilities to occur and in turn, to break into turbulence. In addition, the shear of these waves may be enhanced by a nonlinear unstable amplification of those gravity waves whose phase velocity matches the local wind velocity. As a consequence, turbulence in the stratosphere occurs intermittently, in extensive layers from ten to a few hundred kilometers in extent, and only a few ten to a few hundred meters in thickness.
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