Transition of MHD flows in confined geometries with helical boundary conditions

(b) Clear out of the corner in the case of slip (half full symbols) and no slip (full symbols) boundary conditions during the displacement of a microgel 2.2% by a microgel 1.6%

full symbols) and no slip (full symbols) boundary conditions during the displacement of a microgel 2.2% by a microgel 1.6% at various wall shear stress calculated when the

addition, we predict novel magnetically-induced insulator – metal and polar – non-polar transitions. More specifically, we find that both the multiferroic E-AFM order and the

For flows of blockage ratio b = 0.50, in relation to the results of the Floquet stability analysis of section 6.3, inspection of the flow for a range of Reynolds numbers with A =

Die Diagnose der Erkrankung basiert auf bildgebenden Verfahren und der An- zucht des Erregers aus Urin, Blut, Sputum oder durch Punktion gewonnen Materia- les. Zumeist

Durant leur séjour, les artistes créent une œuvre et reflètent dans leur travail leur perception des enjeux de leur région d’accueil.. ECHANGE, DIALOGUE

One may then understand that there exists some optimum in the choice of T in terms of the maximization of mean toroidal plasma speed and that a ‘moderate’ up-down temperature gradient

Toroidal velocities are computed for increasing Hartmann numbers using no-slip boundary conditions.. Typical JET parameters have been taken: the major radius is r 0 = 3m, the