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Distinguishing between pulsed and continuous reconnection at the dayside magnetopause

Magnetic reconnection has been established as the dominant mechanism by which magnetic fields in different regions change topology to create open magnetic field lines that allow energy and momentum to flow into the magnetosphere. One of the persistent problems of magnetic reconnection is the questio...

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Autores principales: Trattner, K. J., Onsager, T. G., Petrinec, S. M., Fuselier, S. A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5014232/
https://www.ncbi.nlm.nih.gov/pubmed/27656333
http://dx.doi.org/10.1002/2014JA020713
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author Trattner, K. J.
Onsager, T. G.
Petrinec, S. M.
Fuselier, S. A.
author_facet Trattner, K. J.
Onsager, T. G.
Petrinec, S. M.
Fuselier, S. A.
author_sort Trattner, K. J.
collection PubMed
description Magnetic reconnection has been established as the dominant mechanism by which magnetic fields in different regions change topology to create open magnetic field lines that allow energy and momentum to flow into the magnetosphere. One of the persistent problems of magnetic reconnection is the question of whether the process is continuous or intermittent and what input condition(s) might favor one type of reconnection over the other. Observations from imagers that record FUV emissions caused by precipitating cusp ions demonstrate the global nature of magnetic reconnection. Those images show continuous ionospheric emissions even during changing interplanetary magnetic field conditions. On the other hand, in situ observations from polar‐orbiting satellites show distinctive cusp structures in flux distributions of precipitating ions, which are interpreted as the telltale signature of intermittent reconnection. This study uses a modification of the low‐velocity cutoff method, which was previously successfully used to determine the location of the reconnection site, to calculate for the cusp ion distributions the “time since reconnection occurred.” The “time since reconnection” is used to determine the “reconnection time” for the cusp magnetic field lines where these distributions have been observed. The profile of the reconnection time, either continuous or stepped, is a direct measurement of the nature of magnetic reconnection at the reconnection site. This paper will discuss a continuous and pulsed reconnection event from the Polar spacecraft to illustrate the methodology.
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spelling pubmed-50142322016-09-19 Distinguishing between pulsed and continuous reconnection at the dayside magnetopause Trattner, K. J. Onsager, T. G. Petrinec, S. M. Fuselier, S. A. J Geophys Res Space Phys Research Articles Magnetic reconnection has been established as the dominant mechanism by which magnetic fields in different regions change topology to create open magnetic field lines that allow energy and momentum to flow into the magnetosphere. One of the persistent problems of magnetic reconnection is the question of whether the process is continuous or intermittent and what input condition(s) might favor one type of reconnection over the other. Observations from imagers that record FUV emissions caused by precipitating cusp ions demonstrate the global nature of magnetic reconnection. Those images show continuous ionospheric emissions even during changing interplanetary magnetic field conditions. On the other hand, in situ observations from polar‐orbiting satellites show distinctive cusp structures in flux distributions of precipitating ions, which are interpreted as the telltale signature of intermittent reconnection. This study uses a modification of the low‐velocity cutoff method, which was previously successfully used to determine the location of the reconnection site, to calculate for the cusp ion distributions the “time since reconnection occurred.” The “time since reconnection” is used to determine the “reconnection time” for the cusp magnetic field lines where these distributions have been observed. The profile of the reconnection time, either continuous or stepped, is a direct measurement of the nature of magnetic reconnection at the reconnection site. This paper will discuss a continuous and pulsed reconnection event from the Polar spacecraft to illustrate the methodology. John Wiley and Sons Inc. 2015-03 2015-03-11 /pmc/articles/PMC5014232/ /pubmed/27656333 http://dx.doi.org/10.1002/2014JA020713 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
Trattner, K. J.
Onsager, T. G.
Petrinec, S. M.
Fuselier, S. A.
Distinguishing between pulsed and continuous reconnection at the dayside magnetopause
title Distinguishing between pulsed and continuous reconnection at the dayside magnetopause
title_full Distinguishing between pulsed and continuous reconnection at the dayside magnetopause
title_fullStr Distinguishing between pulsed and continuous reconnection at the dayside magnetopause
title_full_unstemmed Distinguishing between pulsed and continuous reconnection at the dayside magnetopause
title_short Distinguishing between pulsed and continuous reconnection at the dayside magnetopause
title_sort distinguishing between pulsed and continuous reconnection at the dayside magnetopause
topic Research Articles
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5014232/
https://www.ncbi.nlm.nih.gov/pubmed/27656333
http://dx.doi.org/10.1002/2014JA020713
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