Modelling the interaction of Alfvénic fluctuations with coronal mass ejections in the low solar corona

dc.contributor.authorSishtla Chaitanya Prasad
dc.contributor.authorPomoell Jens
dc.contributor.authorVainio Rami
dc.contributor.authorKilpua Emilia
dc.contributor.authorGood Simon
dc.contributor.organizationfi=avaruustutkimuslaboratorio|en=Space Research Laboratory|
dc.contributor.organization-code1.2.246.10.2458963.20.47833719389
dc.converis.publication-id380657710
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/380657710
dc.date.accessioned2025-08-27T23:33:17Z
dc.date.available2025-08-27T23:33:17Z
dc.description.abstract<p><em>Context.</em> Alfvénic fluctuations of various scales are ubiquitous in the corona; their non-linear interactions and eventual turbulent cascade result in an important heating mechanism that accelerates the solar wind. These fluctuations may be processed by large-scale, transient, and coherent heliospheric structures such as coronal mass ejections (CMEs). In this study we investigate the interactions between Alfvénic solar wind fluctuations and CMEs using magnetohydrodynamic (MHD) simulations.</p><p><em>Aims.</em> We study the transmission of upstream solar wind fluctuations into the CME leading to the formation of CME sheath fluctuations. Additionally, we investigate the influence of the fluctuation frequencies on the extent of the CME sheath.</p><p><em>Methods.</em> We used an ideal MHD model with an adiabatic equation of state. An Alfvén pump wave is injected into the quiet solar wind by perturbing the transverse magnetic field and velocity components, and a CME is injected by inserting a flux-rope modelled as a magnetic island into the quasi-steady solar wind.</p><p><em>Results.</em> The upstream Alfvén waves experience a decrease in wavelength and change in the wave vector direction due to the non-radial topology of the CME shock front. The CME sheath inhibits the transmission of long-wavelength fluctuations due to the presence of non-radial flows in this region. The frequency of the solar wind fluctuations also affects the steepening of MHD fast waves causing the CME shock propagation speed to vary with the solar wind fluctuation frequencies.</p>
dc.identifier.eissn1432-0746
dc.identifier.jour-issn0004-6361
dc.identifier.olddbid204179
dc.identifier.oldhandle10024/187206
dc.identifier.urihttps://www.utupub.fi/handle/11111/52353
dc.identifier.urlhttps://doi.org/10.1051/0004-6361/202347250
dc.identifier.urnURN:NBN:fi-fe2025082786344
dc.language.isoen
dc.okm.affiliatedauthorVainio, Rami
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationnot an international co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherEDP Sciences
dc.publisher.countryFranceen_GB
dc.publisher.countryRanskafi_FI
dc.publisher.country-codeFR
dc.relation.articlenumberA54
dc.relation.doi10.1051/0004-6361/202347250
dc.relation.ispartofjournalAstronomy and Astrophysics
dc.relation.volume679
dc.source.identifierhttps://www.utupub.fi/handle/10024/187206
dc.titleModelling the interaction of Alfvénic fluctuations with coronal mass ejections in the low solar corona
dc.year.issued2023

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