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THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet
The basic properties of the near‐Earth current sheet from 8 R(E) to 12 R(E) were determined based on Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2013. Ampere's law was used to estimate the current density when the locations of two space...
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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John Wiley and Sons Inc.
2015
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5046188/ https://www.ncbi.nlm.nih.gov/pubmed/27722039 http://dx.doi.org/10.1002/2015JA021142 |
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author | Saito, Miho |
author_facet | Saito, Miho |
author_sort | Saito, Miho |
collection | PubMed |
description | The basic properties of the near‐Earth current sheet from 8 R(E) to 12 R(E) were determined based on Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2013. Ampere's law was used to estimate the current density when the locations of two spacecraft were suitable for the calculation. A total of 3838 current density observations were obtained to study the vertical profile. For typical solar wind conditions, the current density near (off) the central plane of the current sheet ranged from 1 to 2 nA/m(2) (1 to 8 nA/m(2)). All the high current densities appeared off the central plane of the current sheet, indicating the formation of a bifurcated current sheet structure when the current density increased above 2 nA/m(2). The median profile also showed a bifurcated structure, in which the half thickness was about 3 R(E). The distance between the peak of the current density and the central plane of the current sheet was 0.5 to 1 R(E). High current densities above 4 nA/m(2) were observed in some cases that occurred preferentially during substorms, but they also occurred in quiet times. In contrast to the commonly accepted picture, these high current densities can form without a high solar wind dynamic pressure. In addition, these high current densities can appear in two magnetic configurations: tail‐like and dipolar structures. At least two mechanisms, magnetic flux depletion and new current system formation during the expansion phase, other than plasma sheet compression are responsible for the formation of the bifurcated current sheets. |
format | Online Article Text |
id | pubmed-5046188 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-50461882016-10-06 THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet Saito, Miho J Geophys Res Space Phys Research Articles The basic properties of the near‐Earth current sheet from 8 R(E) to 12 R(E) were determined based on Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2013. Ampere's law was used to estimate the current density when the locations of two spacecraft were suitable for the calculation. A total of 3838 current density observations were obtained to study the vertical profile. For typical solar wind conditions, the current density near (off) the central plane of the current sheet ranged from 1 to 2 nA/m(2) (1 to 8 nA/m(2)). All the high current densities appeared off the central plane of the current sheet, indicating the formation of a bifurcated current sheet structure when the current density increased above 2 nA/m(2). The median profile also showed a bifurcated structure, in which the half thickness was about 3 R(E). The distance between the peak of the current density and the central plane of the current sheet was 0.5 to 1 R(E). High current densities above 4 nA/m(2) were observed in some cases that occurred preferentially during substorms, but they also occurred in quiet times. In contrast to the commonly accepted picture, these high current densities can form without a high solar wind dynamic pressure. In addition, these high current densities can appear in two magnetic configurations: tail‐like and dipolar structures. At least two mechanisms, magnetic flux depletion and new current system formation during the expansion phase, other than plasma sheet compression are responsible for the formation of the bifurcated current sheets. John Wiley and Sons Inc. 2015-08 2015-08-15 /pmc/articles/PMC5046188/ /pubmed/27722039 http://dx.doi.org/10.1002/2015JA021142 Text en ©2015. The Authors. This is an open access article under the terms of the Creative Commons Attribution‐NonCommercial‐NoDerivs (http://creativecommons.org/licenses/by-nc-nd/4.0/) License, which permits use and distribution in any medium, provided the original work is properly cited, the use is non‐commercial and no modifications or adaptations are made. |
spellingShingle | Research Articles Saito, Miho THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet |
title | THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet |
title_full | THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet |
title_fullStr | THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet |
title_full_unstemmed | THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet |
title_short | THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet |
title_sort | themis two‐point measurements of the cross‐tail current density: a thick bifurcated current sheet in the near‐earth plasma sheet |
topic | Research Articles |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5046188/ https://www.ncbi.nlm.nih.gov/pubmed/27722039 http://dx.doi.org/10.1002/2015JA021142 |
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