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dc.contributor.authorDudorov, A. E.en
dc.contributor.authorKhaibrakhmanov, S. A.en
dc.contributor.authorSobolev, A. M.en
dc.date.accessioned2021-08-31T14:59:23Z-
dc.date.available2021-08-31T14:59:23Z-
dc.date.issued2019-
dc.identifier.citationDudorov A. E. Dynamics of magnetic flux tubes in accretion discs of T Tauri stars / A. E. Dudorov, S. A. Khaibrakhmanov, A. M. Sobolev. — DOI 10.1093/mnras/stz1654 // Monthly Notices of the Royal Astronomical Society. — 2019. — Vol. 487. — Iss. 4. — P. 5388-5404.en
dc.identifier.issn358711-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85070070693&doi=10.1093%2fmnras%2fstz1654&partnerID=40&md5=727d2f6e4711d2235d73e89a91d7f073
dc.identifier.otherhttp://arxiv.org/pdf/1906.05133m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/101723-
dc.description.abstractDynamics of slender magnetic flux tubes (MFTs) in the accretion discs of T Tauri stars is investigated. We perform simulations taking into account buoyant, aerodynamic, and turbulent drag forces, radiative heat exchange between MFT and ambient gas, and magnetic field of the disc. The equations of MFT dynamics are solved using Runge-Kutta method of the fourth order. The simulations show that there are two regimes of MFT motion in absence of external magnetic field. In the region r < 0.2 au, the MFTs of radii 0.05 ≤ a0 ≤ 0.16, H (H is the scale height of the disc) with initial plasma beta of 1 experience thermal oscillations above the disc. The oscillations decay over some time, and MFTs continue upward motion afterwards. Thinner or thicker MFTs do not oscillate. MFT velocity increases with initial radius and magnetic field strength. MFTs rise periodically with velocities up to 5-15 km s-1 and periods of 0.5-10 yr determined by the toroidal magnetic field generation time. Approximately 20 per cent of disc mass and magnetic flux can escape to disc atmosphere via the magnetic buoyancy over characteristic time of disc evolution. MFTs dispersal forms expanding magnetized corona of the disc. External magnetic field causes MFT oscillations near the disc surface. These magnetic oscillations have periods from several days to 1-3 months at r < 0.6 au. The magnetic oscillations decay over few periods. We simulate MFT dynamics in accretion discs in the Chameleon I cluster. The simulations demonstrate that MFT oscillations can produce observed IR-variability of T Tauri stars. © 2019 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherOxford University Pressen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceMon. Not. R. Astron. Soc.2
dc.sourceMonthly Notices of the Royal Astronomical Societyen
dc.subjectACCRETION, ACCRETION DISCSen
dc.subjectDIFFUSIONen
dc.subjectISM: JETS AND OUTFLOWSen
dc.subjectISM: MAGNETIC FIELDSen
dc.subjectMHDen
dc.subjectSTARS: VARIABLES: T TAURI, HERBIG AE/BEen
dc.titleDynamics of magnetic flux tubes in accretion discs of T Tauri starsen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1093/mnras/stz1654-
dc.identifier.scopus85070070693-
local.contributor.employeeDudorov, A.E., Chelyabinsk State University, 129 Br. Kashirinykh str, Chelyabinsk, 454001, Russian Federation
local.contributor.employeeKhaibrakhmanov, S.A., Chelyabinsk State University, 129 Br. Kashirinykh str, Chelyabinsk, 454001, Russian Federation, Ural Federal University, 51 Lenin str, Ekaterinburg, 620000, Russian Federation
local.contributor.employeeSobolev, A.M., Ural Federal University, 51 Lenin str, Ekaterinburg, 620000, Russian Federation
local.description.firstpage5388-
local.description.lastpage5404-
local.issue4-
local.volume487-
local.contributor.departmentChelyabinsk State University, 129 Br. Kashirinykh str, Chelyabinsk, 454001, Russian Federation
local.contributor.departmentUral Federal University, 51 Lenin str, Ekaterinburg, 620000, Russian Federation
local.identifier.pure10287498-
local.identifier.pureb9b86628-2d51-445c-8b7f-bad21ccb1386uuid
local.identifier.eid2-s2.0-85070070693-
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