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dc.contributor.authorTasso, H.en
dc.contributor.authorThroumoulopoulos, G. N.en
dc.date.accessioned2015-11-24T18:42:05Z-
dc.date.available2015-11-24T18:42:05Z-
dc.identifier.issn1070-664X-
dc.identifier.urihttps://olympias.lib.uoi.gr/jspui/handle/123456789/17725-
dc.rightsDefault Licence-
dc.subjecthydromagnetic stabilityen
dc.subjectinstabilityen
dc.subjectstabilizationen
dc.subjectrotationen
dc.subjectmodeen
dc.subjecttokamaksen
dc.subjectsystemsen
dc.subjecttheoremen
dc.titleLyapunov stability of flowing magnetohydrodynamic plasmas surrounded by resistive wallsen
heal.typejournalArticle-
heal.type.enJournal articleen
heal.type.elΆρθρο Περιοδικούel
heal.identifier.primaryDoi 10.1063/1.3606470-
heal.identifier.secondary<Go to ISI>://000293474500003-
heal.identifier.secondaryhttp://link.aip.org/getpdf/servlet/GetPDFServlet?filetype=pdf&id=PHPAEN000018000007070702000001-
heal.languageen-
heal.accesscampus-
heal.recordProviderΠανεπιστήμιο Ιωαννίνων. Σχολή Επιστημών και Τεχνολογιών. Τμήμα Βιολογικών Εφαρμογών και Τεχνολογιώνel
heal.publicationDate2011-
heal.abstractA general stability condition for plasma-vacuum systems with resistive walls is derived by using the Frieman Rotenberg Lagrangian stability formulation [Rev. Mod. Phys. 32, 898 ( 1960)]. It is shown that the Lyapunov stability limit for external modes does not depend upon the gyroscopic term but upon the sign of the perturbed potential energy only. In the absence of dissipation in the plasma such as viscosity, it is expected that the flow cannot stabilize the system. (C) 2011 American Institute of Physics. [doi:10.1063/1.3606470]en
heal.journalNamePhysics of Plasmasen
heal.journalTypepeer reviewed-
heal.fullTextAvailabilityTRUE-
Appears in Collections:Άρθρα σε επιστημονικά περιοδικά ( Ανοικτά) - ΦΥΣ

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