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dc.creatorIatridis, A. I.en
dc.creatorSarris, I. E.en
dc.creatorVlachos, N. S.en
dc.date.accessioned2015-11-23T10:30:13Z
dc.date.available2015-11-23T10:30:13Z
dc.date.issued2013
dc.identifier10.1209/0295-5075/101/44005
dc.identifier.issn0295-5075
dc.identifier.urihttp://hdl.handle.net/11615/28530
dc.description.abstractThe electromagnetically driven liquid metal flow in a toroidal duct of a square cross-section is studied numerically searching for the critical Reynolds (Re) and Hartmann (Ha) numbers where transition occurs. Results are reported for Ha up to 500, building a transition map of critical Reynolds and Hartmann numbers and showing two distinct regimes of transition signified by the destabilization of the secondary flow: The first, for Ha < 18, where the Lorentz force is balanced by fluid momentum diffusion and the second, for Ha >= 18, where it is balanced by fluid inertia. In both cases, the destabilization of the secondary flow occurs primarily near the concave sidewall. For Ha >= 18 the transition follows approximately the relationship Re = 16.803 Ha(1.43) for values of Re and Ha in the range 80 < Re/Ha < 224. Copyright (C) EPLA, 2013en
dc.sourceEplen
dc.source.uri<Go to ISI>://WOS:000315999100012
dc.subjectHARTMANN LAYERen
dc.subjectMAGNETOHYDRODYNAMIC FLOWen
dc.subjectINSTABILITYen
dc.subjectPhysics, Multidisciplinaryen
dc.titleTransition of an electromagnetically driven liquid metal flow from laminar to turbulent in a toroidal square ducten
dc.typejournalArticleen


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