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Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone
Meso‐scale plasma convection and particle precipitation could be significant momentum and energy sources for the ionosphere‐thermosphere (I‐T) system. Following our previous work on the I‐T response to a typical midnight flow burst, flow bursts with different characteristics (lifetime, size, and spe...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
John Wiley and Sons Inc.
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9285067/ https://www.ncbi.nlm.nih.gov/pubmed/35845984 http://dx.doi.org/10.1029/2021JA029253 |
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author | Sheng, Cheng Deng, Yue Gabrielse, Christine Lyons, Larry R. Nishimura, Yukitoshi Heelis, Roderick A. Chen, Yun‐Ju |
author_facet | Sheng, Cheng Deng, Yue Gabrielse, Christine Lyons, Larry R. Nishimura, Yukitoshi Heelis, Roderick A. Chen, Yun‐Ju |
author_sort | Sheng, Cheng |
collection | PubMed |
description | Meso‐scale plasma convection and particle precipitation could be significant momentum and energy sources for the ionosphere‐thermosphere (I‐T) system. Following our previous work on the I‐T response to a typical midnight flow burst, flow bursts with different characteristics (lifetime, size, and speed) have been examined systematically with Global Ionosphere‐Thermosphere Model (GITM) simulations in this study. Differences between simulations with and without additional flow bursts are used to illustrate the impact of flow bursts on the I‐T system. The neutral density perturbation due to a flow burst increases with the lifetime, size, and flow speed of the flow burst. It was found that the neutral density perturbation is most sensitive to the size of a flow burst, increasing from ∼0.3% to ∼1.3% when the size changes from 80 to 200 km. A westward‐eastward asymmetry has been identified in neutral density, wind, and temperature perturbations, which may be due to the changing of the forcing location in geographic coordinates and the asymmetrical background state of the I‐T system. In addition to midnight flow bursts, simulations with flow bursts centered at noon, dawn, and dusk have also been carried out. A flow burst centered at noon (12.0 Local Time [LT], 73°N) produces the weakest perturbation, and a flow burst centered at dusk (18.0 LT, 71°N) produces the strongest. Single‐cell and two‐cell flow bursts induce very similar neutral density perturbation patterns. |
format | Online Article Text |
id | pubmed-9285067 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | John Wiley and Sons Inc. |
record_format | MEDLINE/PubMed |
spelling | pubmed-92850672022-07-15 Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone Sheng, Cheng Deng, Yue Gabrielse, Christine Lyons, Larry R. Nishimura, Yukitoshi Heelis, Roderick A. Chen, Yun‐Ju J Geophys Res Space Phys Research Article Meso‐scale plasma convection and particle precipitation could be significant momentum and energy sources for the ionosphere‐thermosphere (I‐T) system. Following our previous work on the I‐T response to a typical midnight flow burst, flow bursts with different characteristics (lifetime, size, and speed) have been examined systematically with Global Ionosphere‐Thermosphere Model (GITM) simulations in this study. Differences between simulations with and without additional flow bursts are used to illustrate the impact of flow bursts on the I‐T system. The neutral density perturbation due to a flow burst increases with the lifetime, size, and flow speed of the flow burst. It was found that the neutral density perturbation is most sensitive to the size of a flow burst, increasing from ∼0.3% to ∼1.3% when the size changes from 80 to 200 km. A westward‐eastward asymmetry has been identified in neutral density, wind, and temperature perturbations, which may be due to the changing of the forcing location in geographic coordinates and the asymmetrical background state of the I‐T system. In addition to midnight flow bursts, simulations with flow bursts centered at noon, dawn, and dusk have also been carried out. A flow burst centered at noon (12.0 Local Time [LT], 73°N) produces the weakest perturbation, and a flow burst centered at dusk (18.0 LT, 71°N) produces the strongest. Single‐cell and two‐cell flow bursts induce very similar neutral density perturbation patterns. John Wiley and Sons Inc. 2021-10-12 2021-10 /pmc/articles/PMC9285067/ /pubmed/35845984 http://dx.doi.org/10.1029/2021JA029253 Text en © 2021. The Authors. https://creativecommons.org/licenses/by-nc-nd/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by-nc-nd/4.0/ (https://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 Article Sheng, Cheng Deng, Yue Gabrielse, Christine Lyons, Larry R. Nishimura, Yukitoshi Heelis, Roderick A. Chen, Yun‐Ju Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone |
title | Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone |
title_full | Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone |
title_fullStr | Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone |
title_full_unstemmed | Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone |
title_short | Sensitivity of Upper Atmosphere to Different Characteristics of Flow Bursts in the Auroral Zone |
title_sort | sensitivity of upper atmosphere to different characteristics of flow bursts in the auroral zone |
topic | Research Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9285067/ https://www.ncbi.nlm.nih.gov/pubmed/35845984 http://dx.doi.org/10.1029/2021JA029253 |
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