Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux

Magnetic flux ropes (MFRs) constitute the core structure of coronal mass ejections (CMEs), but hot debates remain on whether the MFR forms before or during solar eruptions. Furthermore, how flare reconnection shapes the erupting MFR is still elusive in three dimensions. Here we studied a new MHD sim...

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Main Authors: Chaowei Jiang, Jun Chen, Aiying Duan, Xinkai Bian, Xinyi Wang, Jiaying Li, Peng Zou, Xueshang Feng
Format: Article
Language:English
Published: Frontiers Media S.A. 2021-10-01
Series:Frontiers in Physics
Subjects:
Online Access:https://www.frontiersin.org/articles/10.3389/fphy.2021.746576/full
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spelling doaj-b316c79ce09246d090cde5da9d11a5a92021-10-01T09:42:19ZengFrontiers Media S.A.Frontiers in Physics2296-424X2021-10-01910.3389/fphy.2021.746576746576Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection FluxChaowei Jiang0Jun Chen1Jun Chen2Aiying Duan3Xinkai Bian4Xinyi Wang5Jiaying Li6Peng Zou7Xueshang Feng8Xueshang Feng9Institute of Space Science and Applied Technology, Harbin Institute of Technology, Shenzhen, ChinaSchool of Astronomy and Space Science, Nanjing University, Nanjing, ChinaCAS Key Laboratory of Geospace Environment, School of Earth and Space Sciences, University of Science and Technology of China, Hefei, ChinaSchool of Atmospheric Sciences, Sun Yat-sen University, Zhuhai, ChinaInstitute of Space Science and Applied Technology, Harbin Institute of Technology, Shenzhen, ChinaState Key Laboratory for Space Weather, Center for Space Science and Applied Research, Chinese Academy of Sciences, Beijing, ChinaInstitute of Space Science and Applied Technology, Harbin Institute of Technology, Shenzhen, ChinaInstitute of Space Science and Applied Technology, Harbin Institute of Technology, Shenzhen, ChinaInstitute of Space Science and Applied Technology, Harbin Institute of Technology, Shenzhen, ChinaState Key Laboratory for Space Weather, Center for Space Science and Applied Research, Chinese Academy of Sciences, Beijing, ChinaMagnetic flux ropes (MFRs) constitute the core structure of coronal mass ejections (CMEs), but hot debates remain on whether the MFR forms before or during solar eruptions. Furthermore, how flare reconnection shapes the erupting MFR is still elusive in three dimensions. Here we studied a new MHD simulation of CME initiation by tether-cutting magnetic reconnection in a single magnetic arcade. The simulation follows the whole life, including the birth and subsequent evolution, of an MFR during eruption. In the early phase, the MFR is partially separated from its ambient field by a magnetic quasi-separatrix layer (QSL) that has a double-J shaped footprint on the bottom surface. With the ongoing of the reconnection, the arms of the two J-shaped footprints continually separate from each other, and the hooks of the J shaped footprints expand and eventually become closed almost at the eruption peak time, and thereafter the MFR is fully separated from the un-reconnected field by the QSL. We further studied the evolution of the toroidal flux in the MFR and compared it with that of the reconnected flux. Our simulation reproduced an evolution pattern of increase-to-decrease of the toroidal flux, which is reported recently in observations of variations in flare ribbons and transient coronal dimming. The increase of toroidal flux is owing to the flare reconnection in the early phase that transforms the sheared arcade to twisted field lines, while its decrease is a result of reconnection between field lines in the interior of the MFR in the later phase.https://www.frontiersin.org/articles/10.3389/fphy.2021.746576/fullmagnetic fieldsmagnetohydrodynamics (MHD)methods: numericalsun: coronasun: flares
collection DOAJ
language English
format Article
sources DOAJ
author Chaowei Jiang
Jun Chen
Jun Chen
Aiying Duan
Xinkai Bian
Xinyi Wang
Jiaying Li
Peng Zou
Xueshang Feng
Xueshang Feng
spellingShingle Chaowei Jiang
Jun Chen
Jun Chen
Aiying Duan
Xinkai Bian
Xinyi Wang
Jiaying Li
Peng Zou
Xueshang Feng
Xueshang Feng
Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux
Frontiers in Physics
magnetic fields
magnetohydrodynamics (MHD)
methods: numerical
sun: corona
sun: flares
author_facet Chaowei Jiang
Jun Chen
Jun Chen
Aiying Duan
Xinkai Bian
Xinyi Wang
Jiaying Li
Peng Zou
Xueshang Feng
Xueshang Feng
author_sort Chaowei Jiang
title Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux
title_short Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux
title_full Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux
title_fullStr Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux
title_full_unstemmed Formation of Magnetic Flux Rope During Solar Eruption. I. Evolution of Toroidal Flux and Reconnection Flux
title_sort formation of magnetic flux rope during solar eruption. i. evolution of toroidal flux and reconnection flux
publisher Frontiers Media S.A.
series Frontiers in Physics
issn 2296-424X
publishDate 2021-10-01
description Magnetic flux ropes (MFRs) constitute the core structure of coronal mass ejections (CMEs), but hot debates remain on whether the MFR forms before or during solar eruptions. Furthermore, how flare reconnection shapes the erupting MFR is still elusive in three dimensions. Here we studied a new MHD simulation of CME initiation by tether-cutting magnetic reconnection in a single magnetic arcade. The simulation follows the whole life, including the birth and subsequent evolution, of an MFR during eruption. In the early phase, the MFR is partially separated from its ambient field by a magnetic quasi-separatrix layer (QSL) that has a double-J shaped footprint on the bottom surface. With the ongoing of the reconnection, the arms of the two J-shaped footprints continually separate from each other, and the hooks of the J shaped footprints expand and eventually become closed almost at the eruption peak time, and thereafter the MFR is fully separated from the un-reconnected field by the QSL. We further studied the evolution of the toroidal flux in the MFR and compared it with that of the reconnected flux. Our simulation reproduced an evolution pattern of increase-to-decrease of the toroidal flux, which is reported recently in observations of variations in flare ribbons and transient coronal dimming. The increase of toroidal flux is owing to the flare reconnection in the early phase that transforms the sheared arcade to twisted field lines, while its decrease is a result of reconnection between field lines in the interior of the MFR in the later phase.
topic magnetic fields
magnetohydrodynamics (MHD)
methods: numerical
sun: corona
sun: flares
url https://www.frontiersin.org/articles/10.3389/fphy.2021.746576/full
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