Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling
Abstract Thermospheric mass density values around the 400-km altitude in the cusp can be significantly enhanced as compared to regions around the cusp. To gain insights into the extent to which the magnitude of the cusp mass density enhancements can be explained by the static distributions of modera...
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oai:doaj.org-article:43041ad2325740509742b42a66cf02b12021-11-08T11:02:29ZTime-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling10.1186/s40623-021-01535-91880-5981https://doaj.org/article/43041ad2325740509742b42a66cf02b12021-11-01T00:00:00Zhttps://doi.org/10.1186/s40623-021-01535-9https://doaj.org/toc/1880-5981Abstract Thermospheric mass density values around the 400-km altitude in the cusp can be significantly enhanced as compared to regions around the cusp. To gain insights into the extent to which the magnitude of the cusp mass density enhancements can be explained by the static distributions of moderate electric field and electron precipitation typical for a period of large IMF B Y, we employed a high-resolution two-dimensional local model that can represent the plasma features that are characteristic of the cusp: azimuthal ion flow and low-energy electron precipitation. We also calculated the thermospheric dynamics with and without neutral–ion drag. We found that in the calculation with this drag the obtained mass density enhancement is 10% at most, indicating that the thermospheric dynamics imposing the moderate static electric field and electron precipitation can only explain about one-third of the typical magnitude of cusp thermospheric mass density, i.e., 33%. We also found that in the calculation without neutral–ion drag the magnitude of the mass density enhancement is slightly larger than the one with the neutral–ion drag. To explain the average magnitude of the cusp mass density enhancements completely, other energy inputs such as Alfvén waves, in addition to the static distributions of electric field and electron precipitation, are needed. Graphical AbstractTomokazu OigawaHiroyuki ShinagawaSatoshi TaguchiSpringerOpenarticleNeutral mass density anomalyNeutral upwellingCuspJoule heatingNeutral–ion dragGeography. Anthropology. RecreationGGeodesyQB275-343GeologyQE1-996.5ENEarth, Planets and Space, Vol 73, Iss 1, Pp 1-13 (2021) |
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Neutral mass density anomaly Neutral upwelling Cusp Joule heating Neutral–ion drag Geography. Anthropology. Recreation G Geodesy QB275-343 Geology QE1-996.5 |
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Neutral mass density anomaly Neutral upwelling Cusp Joule heating Neutral–ion drag Geography. Anthropology. Recreation G Geodesy QB275-343 Geology QE1-996.5 Tomokazu Oigawa Hiroyuki Shinagawa Satoshi Taguchi Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling |
description |
Abstract Thermospheric mass density values around the 400-km altitude in the cusp can be significantly enhanced as compared to regions around the cusp. To gain insights into the extent to which the magnitude of the cusp mass density enhancements can be explained by the static distributions of moderate electric field and electron precipitation typical for a period of large IMF B Y, we employed a high-resolution two-dimensional local model that can represent the plasma features that are characteristic of the cusp: azimuthal ion flow and low-energy electron precipitation. We also calculated the thermospheric dynamics with and without neutral–ion drag. We found that in the calculation with this drag the obtained mass density enhancement is 10% at most, indicating that the thermospheric dynamics imposing the moderate static electric field and electron precipitation can only explain about one-third of the typical magnitude of cusp thermospheric mass density, i.e., 33%. We also found that in the calculation without neutral–ion drag the magnitude of the mass density enhancement is slightly larger than the one with the neutral–ion drag. To explain the average magnitude of the cusp mass density enhancements completely, other energy inputs such as Alfvén waves, in addition to the static distributions of electric field and electron precipitation, are needed. Graphical Abstract |
format |
article |
author |
Tomokazu Oigawa Hiroyuki Shinagawa Satoshi Taguchi |
author_facet |
Tomokazu Oigawa Hiroyuki Shinagawa Satoshi Taguchi |
author_sort |
Tomokazu Oigawa |
title |
Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling |
title_short |
Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling |
title_full |
Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling |
title_fullStr |
Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling |
title_full_unstemmed |
Time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large IMF B Y: a high-resolution two-dimensional local modeling |
title_sort |
time-dependent responses of the neutral mass density to fixed magnetospheric energy inputs into the cusp region in the thermosphere during a period of large imf b y: a high-resolution two-dimensional local modeling |
publisher |
SpringerOpen |
publishDate |
2021 |
url |
https://doaj.org/article/43041ad2325740509742b42a66cf02b1 |
work_keys_str_mv |
AT tomokazuoigawa timedependentresponsesoftheneutralmassdensitytofixedmagnetosphericenergyinputsintothecuspregioninthethermosphereduringaperiodoflargeimfbyahighresolutiontwodimensionallocalmodeling AT hiroyukishinagawa timedependentresponsesoftheneutralmassdensitytofixedmagnetosphericenergyinputsintothecuspregioninthethermosphereduringaperiodoflargeimfbyahighresolutiontwodimensionallocalmodeling AT satoshitaguchi timedependentresponsesoftheneutralmassdensitytofixedmagnetosphericenergyinputsintothecuspregioninthethermosphereduringaperiodoflargeimfbyahighresolutiontwodimensionallocalmodeling |
_version_ |
1718442416447422464 |