Loading…
Unified Framework of Forced Magnetic Reconnection and Alfven Resonance
A unified linear theory that includes forced reconnection as a particular case of Alfvén resonance is presented. We consider a generalized Taylor problem in which a sheared magnetic field is subject to a time-dependent boundary perturbation oscillating at frequency \(\omega_0\). By analyzing the asy...
Saved in:
Published in: | arXiv.org 2024-06 |
---|---|
Main Authors: | , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | |
---|---|
cites | |
container_end_page | |
container_issue | |
container_start_page | |
container_title | arXiv.org |
container_volume | |
creator | Urbanski, D Tenerani, A Waelbroeck, F L |
description | A unified linear theory that includes forced reconnection as a particular case of Alfvén resonance is presented. We consider a generalized Taylor problem in which a sheared magnetic field is subject to a time-dependent boundary perturbation oscillating at frequency \(\omega_0\). By analyzing the asymptotic time response of the system, the theory demonstrates that the Alfvén resonance is due to the residues at the resonant poles, in the complex frequency plane, introduced by the boundary perturbation. Alfvén resonance transitions towards forced reconnection, described by the constant-psi regime for (normalized) times \(t\gg S^{1/3}\), when the forcing frequency of the boundary perturbation is \(\omega_0\ll S^{-1/3}\), allowing the coupling of the Alfvén resonances across the neutral line with the reconnecting mode, as originally suggested in [1]. Additionally, it is shown that even if forced reconnection develops for finite, albeit small, frequencies, the reconnection rate and reconnected flux are strongly reduced for frequencies \(\omega_0\gg S^{-3/5}\). |
doi_str_mv | 10.48550/arxiv.2404.19616 |
format | article |
fullrecord | <record><control><sourceid>proquest</sourceid><recordid>TN_cdi_proquest_journals_3049794286</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>3049794286</sourcerecordid><originalsourceid>FETCH-LOGICAL-a526-3866e41fddd43613efb1fd32a491105d91d509fdcb94a50d472d637fe09147643</originalsourceid><addsrcrecordid>eNotjcFKAzEURYMgWGo_wF3A9YxJ3ktmsizFUaEiSF2XNHmRqTXRzLT6-Q7Y1eGexT2M3UhRY6u1uHPltz_VCgXW0hppLthMAciqRaWu2GIY9kIIZRqlNcxY95b62FPgXXGf9JPLB8-Rd7n4yT2790Rj7_kr-ZwS-bHPibsU-PIQT5QmP-TkkqdrdhndYaDFmXO26e43q8dq_fLwtFquK6eVqaA1hlDGEAKCkUBxNw1QDq2UQgcrgxY2Br-z6LQI2KhgoIkkrMTGIMzZ7f_tV8nfRxrG7T4fS5qKWxBoG4uqNfAHKEJMJQ</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>3049794286</pqid></control><display><type>article</type><title>Unified Framework of Forced Magnetic Reconnection and Alfven Resonance</title><source>Publicly Available Content (ProQuest)</source><creator>Urbanski, D ; Tenerani, A ; Waelbroeck, F L</creator><creatorcontrib>Urbanski, D ; Tenerani, A ; Waelbroeck, F L</creatorcontrib><description>A unified linear theory that includes forced reconnection as a particular case of Alfvén resonance is presented. We consider a generalized Taylor problem in which a sheared magnetic field is subject to a time-dependent boundary perturbation oscillating at frequency \(\omega_0\). By analyzing the asymptotic time response of the system, the theory demonstrates that the Alfvén resonance is due to the residues at the resonant poles, in the complex frequency plane, introduced by the boundary perturbation. Alfvén resonance transitions towards forced reconnection, described by the constant-psi regime for (normalized) times \(t\gg S^{1/3}\), when the forcing frequency of the boundary perturbation is \(\omega_0\ll S^{-1/3}\), allowing the coupling of the Alfvén resonances across the neutral line with the reconnecting mode, as originally suggested in [1]. Additionally, it is shown that even if forced reconnection develops for finite, albeit small, frequencies, the reconnection rate and reconnected flux are strongly reduced for frequencies \(\omega_0\gg S^{-3/5}\).</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2404.19616</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Magnetic resonance ; Perturbation ; Resonance ; Time dependence ; Time response</subject><ispartof>arXiv.org, 2024-06</ispartof><rights>2024. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/3049794286?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>776,780,25731,27902,36989,44566</link.rule.ids></links><search><creatorcontrib>Urbanski, D</creatorcontrib><creatorcontrib>Tenerani, A</creatorcontrib><creatorcontrib>Waelbroeck, F L</creatorcontrib><title>Unified Framework of Forced Magnetic Reconnection and Alfven Resonance</title><title>arXiv.org</title><description>A unified linear theory that includes forced reconnection as a particular case of Alfvén resonance is presented. We consider a generalized Taylor problem in which a sheared magnetic field is subject to a time-dependent boundary perturbation oscillating at frequency \(\omega_0\). By analyzing the asymptotic time response of the system, the theory demonstrates that the Alfvén resonance is due to the residues at the resonant poles, in the complex frequency plane, introduced by the boundary perturbation. Alfvén resonance transitions towards forced reconnection, described by the constant-psi regime for (normalized) times \(t\gg S^{1/3}\), when the forcing frequency of the boundary perturbation is \(\omega_0\ll S^{-1/3}\), allowing the coupling of the Alfvén resonances across the neutral line with the reconnecting mode, as originally suggested in [1]. Additionally, it is shown that even if forced reconnection develops for finite, albeit small, frequencies, the reconnection rate and reconnected flux are strongly reduced for frequencies \(\omega_0\gg S^{-3/5}\).</description><subject>Magnetic resonance</subject><subject>Perturbation</subject><subject>Resonance</subject><subject>Time dependence</subject><subject>Time response</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNotjcFKAzEURYMgWGo_wF3A9YxJ3ktmsizFUaEiSF2XNHmRqTXRzLT6-Q7Y1eGexT2M3UhRY6u1uHPltz_VCgXW0hppLthMAciqRaWu2GIY9kIIZRqlNcxY95b62FPgXXGf9JPLB8-Rd7n4yT2790Rj7_kr-ZwS-bHPibsU-PIQT5QmP-TkkqdrdhndYaDFmXO26e43q8dq_fLwtFquK6eVqaA1hlDGEAKCkUBxNw1QDq2UQgcrgxY2Br-z6LQI2KhgoIkkrMTGIMzZ7f_tV8nfRxrG7T4fS5qKWxBoG4uqNfAHKEJMJQ</recordid><startdate>20240603</startdate><enddate>20240603</enddate><creator>Urbanski, D</creator><creator>Tenerani, A</creator><creator>Waelbroeck, F L</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20240603</creationdate><title>Unified Framework of Forced Magnetic Reconnection and Alfven Resonance</title><author>Urbanski, D ; Tenerani, A ; Waelbroeck, F L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a526-3866e41fddd43613efb1fd32a491105d91d509fdcb94a50d472d637fe09147643</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Magnetic resonance</topic><topic>Perturbation</topic><topic>Resonance</topic><topic>Time dependence</topic><topic>Time response</topic><toplevel>online_resources</toplevel><creatorcontrib>Urbanski, D</creatorcontrib><creatorcontrib>Tenerani, A</creatorcontrib><creatorcontrib>Waelbroeck, F L</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>AUTh Library subscriptions: ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>ProQuest Engineering Database</collection><collection>Publicly Available Content (ProQuest)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering collection</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Urbanski, D</au><au>Tenerani, A</au><au>Waelbroeck, F L</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Unified Framework of Forced Magnetic Reconnection and Alfven Resonance</atitle><jtitle>arXiv.org</jtitle><date>2024-06-03</date><risdate>2024</risdate><eissn>2331-8422</eissn><abstract>A unified linear theory that includes forced reconnection as a particular case of Alfvén resonance is presented. We consider a generalized Taylor problem in which a sheared magnetic field is subject to a time-dependent boundary perturbation oscillating at frequency \(\omega_0\). By analyzing the asymptotic time response of the system, the theory demonstrates that the Alfvén resonance is due to the residues at the resonant poles, in the complex frequency plane, introduced by the boundary perturbation. Alfvén resonance transitions towards forced reconnection, described by the constant-psi regime for (normalized) times \(t\gg S^{1/3}\), when the forcing frequency of the boundary perturbation is \(\omega_0\ll S^{-1/3}\), allowing the coupling of the Alfvén resonances across the neutral line with the reconnecting mode, as originally suggested in [1]. Additionally, it is shown that even if forced reconnection develops for finite, albeit small, frequencies, the reconnection rate and reconnected flux are strongly reduced for frequencies \(\omega_0\gg S^{-3/5}\).</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2404.19616</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
ispartof | arXiv.org, 2024-06 |
issn | 2331-8422 |
language | eng |
recordid | cdi_proquest_journals_3049794286 |
source | Publicly Available Content (ProQuest) |
subjects | Magnetic resonance Perturbation Resonance Time dependence Time response |
title | Unified Framework of Forced Magnetic Reconnection and Alfven Resonance |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-02-02T05%3A59%3A34IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Unified%20Framework%20of%20Forced%20Magnetic%20Reconnection%20and%20Alfven%20Resonance&rft.jtitle=arXiv.org&rft.au=Urbanski,%20D&rft.date=2024-06-03&rft.eissn=2331-8422&rft_id=info:doi/10.48550/arxiv.2404.19616&rft_dat=%3Cproquest%3E3049794286%3C/proquest%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a526-3866e41fddd43613efb1fd32a491105d91d509fdcb94a50d472d637fe09147643%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=3049794286&rft_id=info:pmid/&rfr_iscdi=true |