Onset of unsteady horizontal convection in rectangle tank at $Pr=1$

dc.creatorSun, Liang
dc.creatorMA, Dong-Jun
dc.creatorZhang, Wei
dc.creatorSun, De-Jun
dc.date2007-02-05
dc.date2008-04-15
dc.date.accessioned2026-07-07T13:16:36Z
dc.date.available2026-07-07T13:16:36Z
dc.descriptionThe horizontal convection within a rectangle tank is numerically simulated. The flow is found to be unsteady at high Rayleigh numbers. There is a Hopf bifurcation of $Ra$ from steady solutions to periodic solutions, and the critical Rayleigh number $Ra_c$ is obtained as $Ra_c=5.5377\times 10^8$ for the middle plume forcing at $Pr=1$, which is much larger than the formerly obtained value. Besides, the unstable perturbations are always generated from the central jet, which implies that the onset of instability is due to velocity shear (shear instability) other than thermally dynamics (thermal instability). Finally, Paparella and Young's [J. Fluid Mech. 466 (2002) 205] first hypotheses about the destabilization of the flow is numerically proved, i.e. the middle plume forcing can lead to a destabilization of the flow.
dc.description4pages, 6 figures, extension of Chin. Phys. Lett. 2008, 25(6), in press
dc.identifierhttps://arxiv.org/abs/physics/0702037
dc.identifierhttp://arxiv.org/abs/physics/0702037
dc.identifierChin. Phys. Lett. 2008, 25(6), 2121-2124
dc.identifierdoi:10.1088/0256-307X/25/6/054
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/230842
dc.subjectFluid Dynamics
dc.subjectAtmospheric and Oceanic Physics
dc.titleOnset of unsteady horizontal convection in rectangle tank at $Pr=1$
dc.typetext

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