Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure

The plasma number density in the near-Earth plasma sheet depends on the solar wind number density and the north-south component of interplanetary magnetic field (IMF <I>B<sub>z</sub></I>) with time lag and duration of several hours. We examined the three-dimensional struct...

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Main Authors: D. Nagata, S. Machida, S. Ohtani, Y. Saito, T. Mukai
Format: Article
Language:English
Published: Copernicus Publications 2008-12-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/26/4031/2008/angeo-26-4031-2008.pdf
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spelling doaj-b1a0d6bb3239471bb8497c6e71a97b4d2020-11-25T00:37:19ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762008-12-01264031404910.5194/angeo-26-4031-2008Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structureD. Nagata0S. Machida1S. Ohtani2Y. Saito3T. Mukai4Department of Geophysics, Kyoto University, Kyoto 606-8502, JapanDepartment of Geophysics, Kyoto University, Kyoto 606-8502, JapanApplied Physics Laboratory, Johns Hopkins University, Laurel, MD 20723, USAInstitute of Space and Astronautical Science, Japan Aerospace Exploration Agency, Sagamihara, Kanagawa 229-8510, JapanInstitute of Space and Astronautical Science, Japan Aerospace Exploration Agency, Sagamihara, Kanagawa 229-8510, JapanThe plasma number density in the near-Earth plasma sheet depends on the solar wind number density and the north-south component of interplanetary magnetic field (IMF <I>B<sub>z</sub></I>) with time lag and duration of several hours. We examined the three-dimensional structure of such dependences by fitting observations of plasma sheet and solar wind to an empirical model equation. Analyses were conducted separately for northward and southward IMF conditions. Effects of solar wind speed and IMF orientation were also examined by further subdivision of the dataset. Based on obtained results, we discuss (i) the relative contribution of the ionosphere and solar wind to plasma sheet mass supply, (ii) the entry mechanisms for magnetosheath particles, and (iii) the plasma transport in the plasma sheet. We found that solar wind number density dependence is weaker and IMF <I>B<sub>z</sub></I> dependence is stronger for faster solar wind with southward IMF, which suggests the contribution of ionospheric particles. Further from the Earth, different interplanetary conditions result in different structures of solar wind dependence, which indicate different solar wind entry mechanisms: (1) southward IMF results in a strong dependence on solar wind number density in the flank high-latitude region, (2) slow solar wind with northward IMF leads to lower-latitude peaks of solar wind number density dependence in the flank region, (3) fast solar wind with northward IMF results in a strong dependence on solar wind number density at the down-tail dusk flank equator, and (4) solar wind number density dependence is stronger in the downstream of quasi-parallel bow shock. These features are attributable to (1) low-latitude dayside reconnection entry, (2) high-latitude dayside reconnection entry, (3) entry due to decay of Kelvin-Helmholtz vortices, and (4) diffusive entry mediated by kinetic Alfven waves, respectively. Effect of IMF <I>B<sub>z</sub></I> and its time lags show plasma sheet reconfiguration associated with enhanced convective transport under southward IMF. Duration of IMF <I>B<sub>z</sub></I> effect under northward IMF is interpreted in terms of turbulent diffusive transport.https://www.ann-geophys.net/26/4031/2008/angeo-26-4031-2008.pdf
collection DOAJ
language English
format Article
sources DOAJ
author D. Nagata
S. Machida
S. Ohtani
Y. Saito
T. Mukai
spellingShingle D. Nagata
S. Machida
S. Ohtani
Y. Saito
T. Mukai
Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure
Annales Geophysicae
author_facet D. Nagata
S. Machida
S. Ohtani
Y. Saito
T. Mukai
author_sort D. Nagata
title Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure
title_short Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure
title_full Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure
title_fullStr Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure
title_full_unstemmed Solar wind control of plasma number density in the near-Earth plasma sheet: three-dimensional structure
title_sort solar wind control of plasma number density in the near-earth plasma sheet: three-dimensional structure
publisher Copernicus Publications
series Annales Geophysicae
issn 0992-7689
1432-0576
publishDate 2008-12-01
description The plasma number density in the near-Earth plasma sheet depends on the solar wind number density and the north-south component of interplanetary magnetic field (IMF <I>B<sub>z</sub></I>) with time lag and duration of several hours. We examined the three-dimensional structure of such dependences by fitting observations of plasma sheet and solar wind to an empirical model equation. Analyses were conducted separately for northward and southward IMF conditions. Effects of solar wind speed and IMF orientation were also examined by further subdivision of the dataset. Based on obtained results, we discuss (i) the relative contribution of the ionosphere and solar wind to plasma sheet mass supply, (ii) the entry mechanisms for magnetosheath particles, and (iii) the plasma transport in the plasma sheet. We found that solar wind number density dependence is weaker and IMF <I>B<sub>z</sub></I> dependence is stronger for faster solar wind with southward IMF, which suggests the contribution of ionospheric particles. Further from the Earth, different interplanetary conditions result in different structures of solar wind dependence, which indicate different solar wind entry mechanisms: (1) southward IMF results in a strong dependence on solar wind number density in the flank high-latitude region, (2) slow solar wind with northward IMF leads to lower-latitude peaks of solar wind number density dependence in the flank region, (3) fast solar wind with northward IMF results in a strong dependence on solar wind number density at the down-tail dusk flank equator, and (4) solar wind number density dependence is stronger in the downstream of quasi-parallel bow shock. These features are attributable to (1) low-latitude dayside reconnection entry, (2) high-latitude dayside reconnection entry, (3) entry due to decay of Kelvin-Helmholtz vortices, and (4) diffusive entry mediated by kinetic Alfven waves, respectively. Effect of IMF <I>B<sub>z</sub></I> and its time lags show plasma sheet reconfiguration associated with enhanced convective transport under southward IMF. Duration of IMF <I>B<sub>z</sub></I> effect under northward IMF is interpreted in terms of turbulent diffusive transport.
url https://www.ann-geophys.net/26/4031/2008/angeo-26-4031-2008.pdf
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