Experimental investigation of the return flow instability in magnetized spherical Couette flows

We conduct magnetized spherical Couette (MSC) flow experiments in the return flow instability regime with GaInSn as the working fluid, the ratio of the inner to the outer sphere radii ri/ro = 0.5, the Reynolds number Re = 1000, and the Hartmann number Ha ¿ [27.5, 40]. Rotating waves with different a...

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Detalles Bibliográficos
Autores: Ogbonna, Jude, García González, Fernando|||0000-0003-4507-0486, Gundrum, Thomas, Seilmayer, Martin, Stefani, Frank
Tipo de recurso: artículo
Fecha de publicación:2020
País:España
Institución:Universitat Politècnica de Catalunya (UPC)
Repositorio:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglés
OAI Identifier:oai:upcommons.upc.edu:2117/357104
Acceso en línea:https://hdl.handle.net/2117/357104
https://dx.doi.org/10.1063/5.0029570
Access Level:acceso abierto
Palabra clave:Fluid dynamics
Dinàmica de fluids
Àrees temàtiques de la UPC::Física::Física de fluids
Descripción
Sumario:We conduct magnetized spherical Couette (MSC) flow experiments in the return flow instability regime with GaInSn as the working fluid, the ratio of the inner to the outer sphere radii ri/ro = 0.5, the Reynolds number Re = 1000, and the Hartmann number Ha ¿ [27.5, 40]. Rotating waves with different azimuthal wavenumbers m ¿ {2, 3, 4} manifest in certain ranges of Ha in the experiments, depending on whether the values of Ha were fixed or varied from different initial values. These observations demonstrate the multistability of rotating waves, which we attribute to the dynamical system representing the state of the MSC flow tending to move along the same solution branch of the bifurcation diagram when Ha is varied. In experiments with both fixed and varying Ha, the rotation frequencies of the rotating waves are consistent with the results of nonlinear stability analysis. A brief numerical investigation shows that differences in the azimuthal wavenumbers of the rotating waves that develop in the flow also depend on the azimuthal modes that are initially excited.