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PatternSelectionForConvectiveFlowInALiquidBridgeSubjectedToRemoteThermalAction.pdf (4.203Mb)
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Izenburua
Pattern selection for convective flow in a liquid bridge subjected to remote thermal action
Egilea
Shevtsova, ValentinaORCID
Egilea (beste erakunde batekoa)
Gaponenko, Yuri
Yano, Takeru
Nishino, Kazuyoshi
Matsumoto, Shuji
Ikerketa taldea
Mecánica de fluidos
Beste erakundeak
https://ror.org/01cc3fy72
https://ror.org/03zyp6p76
https://ror.org/02j6c0d67
Bertsioa
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Artikulua
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Ingelesa
Eskubideak
© 2022 AIP Publishing
Sarbidea
Sarbide irekia
URI
https://hdl.handle.net/20.500.11984/5885
Argitaratzailearen bertsioa
https://doi.org/10.1063/5.0101901
Non argitaratua
Physics of Fluids  Vol. 34, Nº. 9 34. Article 092102. September,
Argitaratzailea
AIP Publishing
Laburpena
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. [-]
Sponsorship
Gobierno de Bélgica
Projectu ID
info:eu-repo/grantAgreement/GV/Elkartek 2022/KK-2022-00047/CAPV/Materiales Magnetoactivos Avanzados para Nuevos Sistemas Inteligentes/MMASINT
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