The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements

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During the Condor campaign a number of instruments were set up in Peru to support the rocket experiments. In this series of papers we report on the results of the experiments designed to study the equatorial F region. In this overview paper we summarize the main results as well as report upon the ma...

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Detalles Bibliográficos
Autores: Kelley, M.C., LaBelle, J., Kudeki, E., Fejer, B.G., Basu, Sa., Basu, Su, Baker, K.D., Hanuise, C., Argo, P., Woodman Pollitt, Ronald Francisco, Swartz, W.E., Farley, D.T., Meriwether, J.W.
Formato: artículo
Fecha de Publicación:1986
Institución:Instituto Geofísico del Perú
Repositorio:IGP-Institucional
Lenguaje:inglés
OAI Identifier:oai:repositorio.igp.gob.pe:20.500.12816/1721
Enlace del recurso:http://hdl.handle.net/20.500.12816/1721
https://doi.org/10.1029/JA091iA05p05487
Nivel de acceso:acceso abierto
Materia:Region F
Ionosphere
Plasma
Radar
http://purl.org/pe-repo/ocde/ford#1.05.01
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dc.title.none.fl_str_mv The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
title The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
spellingShingle The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
Kelley, M.C.
Region F
Ionosphere
Plasma
Radar
http://purl.org/pe-repo/ocde/ford#1.05.01
title_short The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
title_full The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
title_fullStr The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
title_full_unstemmed The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
title_sort The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements
author Kelley, M.C.
author_facet Kelley, M.C.
LaBelle, J.
Kudeki, E.
Fejer, B.G.
Basu, Sa.
Basu, Su
Baker, K.D.
Hanuise, C.
Argo, P.
Woodman Pollitt, Ronald Francisco
Swartz, W.E.
Farley, D.T.
Meriwether, J.W.
author_role author
author2 LaBelle, J.
Kudeki, E.
Fejer, B.G.
Basu, Sa.
Basu, Su
Baker, K.D.
Hanuise, C.
Argo, P.
Woodman Pollitt, Ronald Francisco
Swartz, W.E.
Farley, D.T.
Meriwether, J.W.
author2_role author
author
author
author
author
author
author
author
author
author
author
author
dc.contributor.author.fl_str_mv Kelley, M.C.
LaBelle, J.
Kudeki, E.
Fejer, B.G.
Basu, Sa.
Basu, Su
Baker, K.D.
Hanuise, C.
Argo, P.
Woodman Pollitt, Ronald Francisco
Swartz, W.E.
Farley, D.T.
Meriwether, J.W.
dc.subject.none.fl_str_mv Region F
Ionosphere
Plasma
Radar
topic Region F
Ionosphere
Plasma
Radar
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 During the Condor campaign a number of instruments were set up in Peru to support the rocket experiments. In this series of papers we report on the results of the experiments designed to study the equatorial F region. In this overview paper we summarize the main results as well as report upon the macroscopic developments of spread F as evidenced by data from backscatter radars, from scintillation observations, and from digital ionosonde meaurements. In this latter regard, we argue here that at least two factors other than the classical gravitational Rayleigh-Taylor plasma instability process must operate to yield the longest-scale horizontal organization of spread F structures. The horizontal scale typical of plume separation distances can be explained by invoking the effect of a shear in the plasma flow, although detailed comparison with theory seems to require shear frequencies a bit higher than observations indicate. On the other hand, the largest-scale organization or modulation of the scattering layer cannot be explained by the shear theory and must be due to local time variations in the ionospheric drift or to gravity wave induced vertical motions. Using simultaneous rocket and radar data, we were also able to confirm the oft quoted hypothesis that rapid overhead height variations in the scattering region over Jicamarca are primarily spatial structures advecting overhead. The detailed rocket-radar comparison verified several other earlier results and speculations, particularly those made in the PLUMEX experiments. In particular, companion papers discuss and extend some of the PLUMEX results to include the role of anomalous diffusion (LaBelle et al., this issue) in the theory of equatorial spread F and to shed light upon the shallow spectral form often observed in the intermediate-scale regime (LaBelle and Kelley, this issue).
publishDate 1986
dc.date.accessioned.none.fl_str_mv 2018-07-05T15:48:27Z
dc.date.available.none.fl_str_mv 2018-07-05T15:48:27Z
dc.date.issued.fl_str_mv 1986-05
dc.type.none.fl_str_mv info:eu-repo/semantics/article
format article
dc.identifier.citation.none.fl_str_mv Kelley, M. C., LaBelle, J., Kudeki, E., Fejer, B. G., Basu, S., Basu, S., ... Meriwether, J. W. (1986). The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements.==$Journal of Geophysical Research: Space Physics, 91$==(A5), 5487-5503. https://doi.org/10.1029/JA091iA05p05487
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/20.500.12816/1721
dc.identifier.journal.none.fl_str_mv Journal of Geophysical Research: Space Physics
dc.identifier.doi.none.fl_str_mv https://doi.org/10.1029/JA091iA05p05487
identifier_str_mv Kelley, M. C., LaBelle, J., Kudeki, E., Fejer, B. G., Basu, S., Basu, S., ... Meriwether, J. W. (1986). The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements.==$Journal of Geophysical Research: Space Physics, 91$==(A5), 5487-5503. https://doi.org/10.1029/JA091iA05p05487
Journal of Geophysical Research: Space Physics
url http://hdl.handle.net/20.500.12816/1721
https://doi.org/10.1029/JA091iA05p05487
dc.language.iso.none.fl_str_mv eng
language eng
dc.relation.ispartof.none.fl_str_mv urn:issn:2169-9380
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dc.publisher.none.fl_str_mv American Geophysical Union
publisher.none.fl_str_mv American Geophysical Union
dc.source.none.fl_str_mv reponame:IGP-Institucional
instname:Instituto Geofísico del Perú
instacron:IGP
instname_str Instituto Geofísico del Perú
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collection IGP-Institucional
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spelling Kelley, M.C.LaBelle, J.Kudeki, E.Fejer, B.G.Basu, Sa.Basu, SuBaker, K.D.Hanuise, C.Argo, P.Woodman Pollitt, Ronald FranciscoSwartz, W.E.Farley, D.T.Meriwether, J.W.2018-07-05T15:48:27Z2018-07-05T15:48:27Z1986-05Kelley, M. C., LaBelle, J., Kudeki, E., Fejer, B. G., Basu, S., Basu, S., ... Meriwether, J. W. (1986). The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurements.==$Journal of Geophysical Research: Space Physics, 91$==(A5), 5487-5503. https://doi.org/10.1029/JA091iA05p05487http://hdl.handle.net/20.500.12816/1721Journal of Geophysical Research: Space Physicshttps://doi.org/10.1029/JA091iA05p05487During the Condor campaign a number of instruments were set up in Peru to support the rocket experiments. In this series of papers we report on the results of the experiments designed to study the equatorial F region. In this overview paper we summarize the main results as well as report upon the macroscopic developments of spread F as evidenced by data from backscatter radars, from scintillation observations, and from digital ionosonde meaurements. In this latter regard, we argue here that at least two factors other than the classical gravitational Rayleigh-Taylor plasma instability process must operate to yield the longest-scale horizontal organization of spread F structures. The horizontal scale typical of plume separation distances can be explained by invoking the effect of a shear in the plasma flow, although detailed comparison with theory seems to require shear frequencies a bit higher than observations indicate. On the other hand, the largest-scale organization or modulation of the scattering layer cannot be explained by the shear theory and must be due to local time variations in the ionospheric drift or to gravity wave induced vertical motions. Using simultaneous rocket and radar data, we were also able to confirm the oft quoted hypothesis that rapid overhead height variations in the scattering region over Jicamarca are primarily spatial structures advecting overhead. The detailed rocket-radar comparison verified several other earlier results and speculations, particularly those made in the PLUMEX experiments. In particular, companion papers discuss and extend some of the PLUMEX results to include the role of anomalous diffusion (LaBelle et al., this issue) in the theory of equatorial spread F and to shed light upon the shallow spectral form often observed in the intermediate-scale regime (LaBelle and Kelley, this issue).Por paresapplication/pdfengAmerican Geophysical Unionurn:issn:2169-9380info:eu-repo/semantics/openAccesshttps://creativecommons.org/licences/by/4.0/Region FIonospherePlasmaRadarhttp://purl.org/pe-repo/ocde/ford#1.05.01The Condor Equatorial Spread F campaign:Overview and results of the large-scale measurementsinfo:eu-repo/semantics/articlereponame:IGP-Institucionalinstname:Instituto Geofísico del Perúinstacron:IGPORIGINALCondor Project- Equatorial F Region Results.pdfCondor Project- Equatorial F Region Results.pdfapplication/pdf33104932https://repositorio.igp.gob.pe/bitstreams/e193628a-4903-4252-a0f8-36e5bdff08b4/download3ea103905279a3b8d1b85b8243111e84MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://repositorio.igp.gob.pe/bitstreams/74e68831-92ee-4940-b710-099addb4709b/download8a4605be74aa9ea9d79846c1fba20a33MD52THUMBNAILCondor Project- Equatorial F Region Results.pdf.jpgCondor Project- Equatorial F Region Results.pdf.jpgIM Thumbnailimage/jpeg36196https://repositorio.igp.gob.pe/bitstreams/67ff3d57-1aa8-4282-b025-e0f984ce4995/downloadf834601874a7e47c2ab6e3ecaaac2ff1MD53TEXTCondor Project- Equatorial F Region Results.pdf.txtCondor Project- Equatorial F Region Results.pdf.txtExtracted texttext/plain79https://repositorio.igp.gob.pe/bitstreams/77e31764-76e8-44ff-9b08-1a18d03463eb/downloadd8332a0f6bcb32827dae5005f9550191MD5420.500.12816/1721oai:repositorio.igp.gob.pe:20.500.12816/17212024-10-12 22:18:07.167https://creativecommons.org/licences/by/4.0/info:eu-repo/semantics/openAccessrestrictedhttps://repositorio.igp.gob.peRepositorio Geofísico Nacionalbiblio@igp.gob.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