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PatternSelectionForConvectiveFlowInALiquidBridgeSubjectedToRemoteThermalAction.pdf (4.203Mb)
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Title
Pattern selection for convective flow in a liquid bridge subjected to remote thermal action
Author
Shevtsova, Valentina
Author (from another institution)
Gaponenko, Yuri
Yano, Takeru
Nishino, Kazuyoshi
Matsumoto, Shuji
Research Group
Mecánica de fluidos
Other institutions
Ikerbasque
Yokohama National University
Kanagawa University
Version
Postprint
Rights
© 2022 AIP Publishing
Access
Open access
URI
https://hdl.handle.net/20.500.11984/5885
Publisher’s version
https://doi.org/10.1063/5.0101901
Published at
Physics of Fluids  Vol. 34, Nº. 9 34. Article 092102. September,
Publisher
AIP Publishing
Abstract
The stability of thermocapillary/buoyant flows is affected by a remote thermal source. We present a nonlinear two-phase computational study of convection in a liquid bridge that develops under the act ... [+]
The stability of thermocapillary/buoyant flows is affected by a remote thermal source. We present a nonlinear two-phase computational study of convection in a liquid bridge that develops under the action of Marangoni and buoyancy forces as well as under the influence of distant thermal disturbances. The gas phase (air) occupies a typical annular container holding a liquid bridge (n-decane, Pr = 14), and the disturbances are locally imposed in the form of hot/cold spots on the outer wall of the container. The hydrothermal wave instability and pattern selection have been explored for two temperature differences Δ𝑇���� by varying the intensity of thermal source Hf over a wide range. Not far from the critical point, in all the cases, the instability emerges in the form of a standing wave, but the azimuthal wavenumber depends on whether the external perturbation is caused by cooling (m = 2) or by heating (m = 1). Further into supercritical area, 45% above the threshold, in the region with thermal perturbations ⎯200<𝐻����𝑓����<50, the flow pattern comprises, but is not limited to, a hydrothermal traveling wave with the azimuthal wavenumber m = 2. For hotter perturbations, the instability develops either in the form of traveling or standing waves, depending on Hf, with the prevailing mode m = 1, but with a strong presence of other modes. [-]
xmlui.dri2xhtml.METS-1.0.item-sponsorship
Gobierno de Bélgica
xmlui.dri2xhtml.METS-1.0.item-projectID
info:eu-repo/grantAgreement/GV/Elkartek 2022/KK-2022-00047/CAPV/Materiales Magnetoactivos Avanzados para Nuevos Sistemas Inteligentes/MMASINT
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