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  4. Convective instability in superposed fluid and anisotropic porous layers
 
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Convective instability in superposed fluid and anisotropic porous layers

Journal
Physics of Fluids A
Journal Volume
3
Journal Issue
4
Pages
556-565
Date Issued
1991
Author(s)
Chen, F.
Chen, C.F.
CHIEN-FU CHEN  
FALIN CHEN  
DOI
10.1063/1.858117
URI
https://scholars.lib.ntu.edu.tw/handle/123456789/486095
URL
https://www.scopus.com/inward/record.uri?eid=2-s2.0-0007648759&doi=10.1063%2f1.858117&partnerID=40&md5=11357e184ff7d6e0908918841a3ca330
Abstract
The onset of thermal convection due to heating from below in a system consisting of a fluid layer overlying a porous layer with anisotropic permeability and thermal diffusivity is studied. Flow in the porous medium is assumed to be governed by Darcy’s law; the Beavers–Joseph condition is applied at the interface between the two layers. The linear perturbation equations are solved numerically. It is found that the effects of anisotropy on the onset of thermal convection are most profound for small values of the depth ratio ζ (ratio of fluid layer thickness to porous layer thickness), since in that case, the onset of convection corresponds to significant motion in both layers. For fixed values of the vertical permeability in the porous medium, decreasing the value of ξ (ratio of horizontal to vertical permeability) leads to stabilization of the superposed layer configuration because of increased resistance to motion in the porous medium. For larger values of ζ, the onset of motion is increasingly confined to the fluid layer, with the transport of heat through the porous layer occurring primarily by conduction. Accordingly, the influence of ξ on the stability characteristics for larger ζ is less significant than the effects of an anisotropic thermal conductivity.
Type
journal article

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