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Writhed Analytical Magnetic Flux Rope Model

Observations of magnetic clouds, within interplanetary coronal mass ejections (ICMEs), are often well described by flux rope models. Most of these assume either a cylindrical or toroidal geometry. In some cases, these models are also capable of accounting for non‐axisymmetric cross‐sections but they...

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Autores principales: Weiss, A. J., Nieves‐Chinchilla, T., Möstl, C., Reiss, M. A., Amerstorfer, T., Bailey, R. L.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10078358/
https://www.ncbi.nlm.nih.gov/pubmed/37032658
http://dx.doi.org/10.1029/2022JA030898
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author Weiss, A. J.
Nieves‐Chinchilla, T.
Möstl, C.
Reiss, M. A.
Amerstorfer, T.
Bailey, R. L.
author_facet Weiss, A. J.
Nieves‐Chinchilla, T.
Möstl, C.
Reiss, M. A.
Amerstorfer, T.
Bailey, R. L.
author_sort Weiss, A. J.
collection PubMed
description Observations of magnetic clouds, within interplanetary coronal mass ejections (ICMEs), are often well described by flux rope models. Most of these assume either a cylindrical or toroidal geometry. In some cases, these models are also capable of accounting for non‐axisymmetric cross‐sections but they generally all assume axial invariance. It can be expected that any ICME, and its flux rope, will be deformed along its axis due to influences such as the solar wind. In this work, we aim to develop a writhed analytical magnetic flux rope model which would allow us to analytically describe a flux rope structure with varying curvature and torsion so that we are no longer constrained to a cylindrical or toroidal geometry. In this first iteration of our model we will solely focus on a circular cross‐section of constant size. We describe our flux rope geometry in terms of a parametrized flux rope axis and a parallel transport frame. We derive expressions for the axial and poloidal magnetic field components under the assumption that the total axial magnetic flux is conserved. We find an entire class of possible solutions, which differ by the choice of integration constants, and present the results for a specific example. In general, we find that the twist of the magnetic field locally changes when the geometry deviates from a cylinder or torus. This new approach also allows us to generate completely new types of in situ magnetic field profiles which strongly deviate from those generated by cylindrical or toroidal models.
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spelling pubmed-100783582023-04-07 Writhed Analytical Magnetic Flux Rope Model Weiss, A. J. Nieves‐Chinchilla, T. Möstl, C. Reiss, M. A. Amerstorfer, T. Bailey, R. L. J Geophys Res Space Phys Research Article Observations of magnetic clouds, within interplanetary coronal mass ejections (ICMEs), are often well described by flux rope models. Most of these assume either a cylindrical or toroidal geometry. In some cases, these models are also capable of accounting for non‐axisymmetric cross‐sections but they generally all assume axial invariance. It can be expected that any ICME, and its flux rope, will be deformed along its axis due to influences such as the solar wind. In this work, we aim to develop a writhed analytical magnetic flux rope model which would allow us to analytically describe a flux rope structure with varying curvature and torsion so that we are no longer constrained to a cylindrical or toroidal geometry. In this first iteration of our model we will solely focus on a circular cross‐section of constant size. We describe our flux rope geometry in terms of a parametrized flux rope axis and a parallel transport frame. We derive expressions for the axial and poloidal magnetic field components under the assumption that the total axial magnetic flux is conserved. We find an entire class of possible solutions, which differ by the choice of integration constants, and present the results for a specific example. In general, we find that the twist of the magnetic field locally changes when the geometry deviates from a cylinder or torus. This new approach also allows us to generate completely new types of in situ magnetic field profiles which strongly deviate from those generated by cylindrical or toroidal models. John Wiley and Sons Inc. 2022-11-30 2022-12 /pmc/articles/PMC10078358/ /pubmed/37032658 http://dx.doi.org/10.1029/2022JA030898 Text en © 2022. The Authors. https://creativecommons.org/licenses/by/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.
spellingShingle Research Article
Weiss, A. J.
Nieves‐Chinchilla, T.
Möstl, C.
Reiss, M. A.
Amerstorfer, T.
Bailey, R. L.
Writhed Analytical Magnetic Flux Rope Model
title Writhed Analytical Magnetic Flux Rope Model
title_full Writhed Analytical Magnetic Flux Rope Model
title_fullStr Writhed Analytical Magnetic Flux Rope Model
title_full_unstemmed Writhed Analytical Magnetic Flux Rope Model
title_short Writhed Analytical Magnetic Flux Rope Model
title_sort writhed analytical magnetic flux rope model
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10078358/
https://www.ncbi.nlm.nih.gov/pubmed/37032658
http://dx.doi.org/10.1029/2022JA030898
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