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Double-diffusive convection for a heated cylinder submerged in a salt-stratified fluid layer
Author(s) -
YiHsin Chen,
C.-K. Liu
Publication year - 1997
Publication title -
heat and mass transfer
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.551
H-Index - 68
eISSN - 1432-1181
pISSN - 0947-7411
DOI - 10.1007/s002310050157
Subject(s) - plume , natural convection , rayleigh number , double diffusive convection , convection , buoyancy , mechanics , nusselt number , cylinder , temperature gradient , materials science , physics , thermodynamics , meteorology , geometry , reynolds number , turbulence , mathematics
Double-diffusive convection due to a cylindrical source submerged in a salt-stratified solution is numerically investigated in this study. For proper simulation of the vortex generated around the cylinder, a computational domain with irregular shape is employed. Flow conditions depend strongly on the thermal Rayleigh number, Ra T , and the buoyancy ratio, R ρ. There are two types of onset of instability existing in the flow field. Both types are due to either the interaction of the upward temperature gradient and downward salinity gradient or the interaction of the lateral temperature gradient and downward salinity gradient. The onset of layer instability due to plume convection is due to the former, whereas, the onset of layer instability of layers around the cylinder is due to the latter. Both types can be found in the flow field. The transport mechanism of layers at the top of the basic plume belongs to former while that due to basic plume and layer around the cylinder are the latter. The increase in Ra T reinforces the plume convection and reduces the layer numbers generated around the cylinder for the same buoyancy ratio. For the same Ra T , the increase of R ρ suppresses the plume convection but reinforces the layers generated around the cylinder. The profiles of local Nusselt number reflects the heat transfer characteristics of plume convection and layered structure. The profiles of averaged Nusselt number are between the pure conduction and natural convection modes and the variation is due to the evolution of layers.

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