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...
Autor: | |
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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 |
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dc.title.none.fl_str_mv |
Turbulence in the middle atmosphere: A review |
title |
Turbulence in the middle atmosphere: A review |
spellingShingle |
Turbulence in the middle atmosphere: A review Woodman Pollitt, Ronald Francisco Stratosphere Turbulence Stratospheric winds http://purl.org/pe-repo/ocde/ford#1.05.01 |
title_short |
Turbulence in the middle atmosphere: A review |
title_full |
Turbulence in the middle atmosphere: A review |
title_fullStr |
Turbulence in the middle atmosphere: A review |
title_full_unstemmed |
Turbulence in the middle atmosphere: A review |
title_sort |
Turbulence in the middle atmosphere: A review |
author |
Woodman Pollitt, Ronald Francisco |
author_facet |
Woodman Pollitt, Ronald Francisco |
author_role |
author |
dc.contributor.author.fl_str_mv |
Woodman Pollitt, Ronald Francisco |
dc.subject.none.fl_str_mv |
Stratosphere Turbulence Stratospheric winds |
topic |
Stratosphere Turbulence Stratospheric winds http://purl.org/pe-repo/ocde/ford#1.05.01 |
dc.subject.ocde.none.fl_str_mv |
http://purl.org/pe-repo/ocde/ford#1.05.01 |
description |
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. |
publishDate |
1980 |
dc.date.accessioned.none.fl_str_mv |
2016-11-08T00:06:19Z 2017-12-21T19:41:47Z |
dc.date.available.none.fl_str_mv |
2016-11-08T00:06:19Z 2017-12-21T19:41:47Z |
dc.date.issued.fl_str_mv |
1980 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/conferenceObject |
format |
conferenceObject |
dc.identifier.citation.none.fl_str_mv |
Woodman, R. F. (1980). Turbulence in the middle atmosphere: A review. |
dc.identifier.uri.none.fl_str_mv |
http://hdl.handle.net/20.500.12816/579 |
identifier_str_mv |
Woodman, R. F. (1980). Turbulence in the middle atmosphere: A review. |
url |
http://hdl.handle.net/20.500.12816/579 |
dc.language.iso.none.fl_str_mv |
eng |
language |
eng |
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info:eu-repo/semantics/openAccess |
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https://creativecommons.org/licences/by/4.0/ |
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openAccess |
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https://creativecommons.org/licences/by/4.0/ |
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Woodman Pollitt, Ronald Francisco2016-11-08T00:06:19Z2017-12-21T19:41:47Z2016-11-08T00:06:19Z2017-12-21T19:41:47Z1980Woodman, R. F. (1980). Turbulence in the middle atmosphere: A review.http://hdl.handle.net/20.500.12816/579The 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.application/pdfengEditor no identificadoinfo:eu-repo/semantics/openAccesshttps://creativecommons.org/licences/by/4.0/StratosphereTurbulenceStratospheric windshttp://purl.org/pe-repo/ocde/ford#1.05.01Turbulence in the middle atmosphere: A reviewinfo:eu-repo/semantics/conferenceObjectreponame:IGP-Institucionalinstname:Instituto Geofísico del Perúinstacron:IGPORIGINALTurbulence in the middle atmosphere- a review.PDFapplication/pdf170428https://repositorio.igp.gob.pe/bitstreams/41098a3d-da12-410c-81e8-2c5c31ab9efe/download70ec3912b8d344cf36f124f95773cf24MD51LICENSElicense.txttext/plain1748https://repositorio.igp.gob.pe/bitstreams/4b04327e-0df7-40a0-aab9-27fff65f0f04/download8a4605be74aa9ea9d79846c1fba20a33MD52THUMBNAILTurbulence in the middle atmosphere- a review.PDF.jpgTurbulence in the middle atmosphere- a review.PDF.jpgIM Thumbnailimage/jpeg103449https://repositorio.igp.gob.pe/bitstreams/95dcfd27-66f4-48c6-9402-71e1a224d743/download963be3af8b95d3c27e4a54a95320c149MD53TEXTTurbulence in the middle atmosphere- a review.PDF.txtTurbulence in the middle atmosphere- a review.PDF.txtExtracted texttext/plain5https://repositorio.igp.gob.pe/bitstreams/e168fb09-d8e8-4965-a4bd-9e99a07a764d/downloadcc9067c2ee470dc248b14b194209a34eMD5420.500.12816/579oai:repositorio.igp.gob.pe:20.500.12816/5792024-10-12 22:18:21.087https://creativecommons.org/licences/by/4.0/info:eu-repo/semantics/openAccessopen.accesshttps://repositorio.igp.gob.peRepositorio Geofísico Nacionalbiblio@igp.gob.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 |
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