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RESEARCH PAPERS

Onset of Finger Convection in a Horizontal Porous Layer Underlying a Fluid Layer

[+] Author and Article Information
F. Chen, C. F. Chen

Department of Aerospace and Mechanical Engineering, University of Arizona, Tucson, AZ 85721

J. Heat Transfer 110(2), 403-409 (May 01, 1988) (7 pages) doi:10.1115/1.3250499 History: Received December 22, 1986; Online October 20, 2009

Abstract

In the directional solidification of concentrated alloys, the frozen solid region is separated from the melt region by a mushy zone consisting of dendrites immersed in the melt. Simultaneous occurrence of temperature and solute gradients through the melt and mushy zones may be conducive to the occurrence of salt-finger convection, which may in turn cause adverse effects such as channel segregation. We have considered the problem of the onset of finger convection in a porous layer underlying a fluid layer using linear stability analysis. The eigenvalue problem is solved by a shooting method. As a check on the method of solution and the associated computer program, we first consider the thermal convection problem. In this process, it is discovered that at low depth ratios d̂ (the ratio of the fluid layer depth to the porous layer depth), the marginal stability curve is bimodal. At small d̂, the long-wave branch is the most unstable and the convection is dominated by the porous layer. At large d̂, the short-wave branch is the most unstable and the convection is dominated by the fluid layer, with a convection pattern consisting of square cells in the fluid layer. In the salt-finger case with a given thermal Rayleigh number Ram = 50, as the depth ratio d̂ is increased from zero, the critical salt Rayleigh number Rasm first decreases, reaches a minimum, and then increases. The system is more stable at d̂ > 0.2 than at d̂ = 0. This rather unusual behavior is again due to the fact that at small d̂, convection is dominated by the porous layer and, at large d̂, convection is dominated by the fluid layer. However, in the latter case, the convection pattern in the fluid layer consists of a number of high aspect ratio cells.

Copyright © 1988 by ASME
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