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dc.contributor.authorThroumoulopoulos, G. N.en
dc.contributor.authorPoulipoulis, G.en
dc.contributor.authorPantis, G.en
dc.contributor.authorTasso, H.en
dc.date.accessioned2015-11-24T18:28:52Z-
dc.date.available2015-11-24T18:28:52Z-
dc.identifier.issn0375-9601-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/16197-
dc.rightsDefault Licence-
dc.subjectmagnetohydrodynamicsen
dc.subjectequilibriumen
dc.subjectplasma flowsen
dc.subjectmagnetic confinementen
dc.subjectastrophysicsen
dc.subjectincompressible flowsen
dc.subjectastrophysical jetsen
dc.subjectplasmaen
dc.subjectsuppressionen
dc.titleExact magnetohydrodynamic equilibria with flow and effects on the Shafranov shiften
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.primaryDOI 10.1016/j.physleta.2003.09.005-
heal.identifier.secondary<Go to ISI>://000186248100017-
heal.identifier.secondaryhttp://ac.els-cdn.com/S0375960103013471/1-s2.0-S0375960103013471-main.pdf?_tid=279d8d41cd8919bf0706c11562ad2353&acdnat=1334232525_0d9668ce4d5bb518d76c6e58fffbb79e-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.publicationDate2003-
heal.abstractExact solutions of the equation governing the equilibrium magnetohydrodynamic states of an axisymmetric plasma with incompressible flows of arbitrary direction [Phys. Pasmas 5 (1998) 2378] are constructed for toroidal current density profiles peaked on the magnetic axis in connection with the ansatz S = -ku, where S = d/du[rho(dPhi/du)(2)] (k is a parameter, u labels the magnetic surfaces; rho(u) and Phi(u) are the density and the electrostatic potential, respectively). They pertain to either unbounded plasmas of astrophysical concern or bounded plasmas of arbitrary aspect ratio. For k = 0, a case which includes flows parallel to the magnetic field, the solutions are expressed in terms of Kummer functions while for k not equal 0 in terms of Airy functions. On the basis of a tokamak solution with k not equal 0 describing a plasma surrounded by a perfectly conducted boundary of rectangular cross-section it turns out that the Shafranov shift is a decreasing function which can vanish for a positive value of k. This value is larger the smaller the aspect ratio of the configuration. (C) 2003 Published by Elsevier B.V.en
heal.journalNamePhysics Letters Aen
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά) - ΦΥΣ

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