NATURAL CONVECTIVE HEAT-TRANSFER FROM A CYLINDER IN AN ENCLOSURE PARTLY FILLED WITH A POROUS-MEDIUM

Citation
Ph. Oosthuizen et D. Naylor, NATURAL CONVECTIVE HEAT-TRANSFER FROM A CYLINDER IN AN ENCLOSURE PARTLY FILLED WITH A POROUS-MEDIUM, INTERNATIONAL JOURNAL OF NUMERICAL METHODS FOR HEAT & FLUID FLOW, 6(6), 1996, pp. 51-63
Citations number
12
Categorie Soggetti
Mathematical Method, Physical Science",Mechanics,Mathematics
ISSN journal
09615539
Volume
6
Issue
6
Year of publication
1996
Pages
51 - 63
Database
ISI
SICI code
0961-5539(1996)6:6<51:NCHFAC>2.0.ZU;2-9
Abstract
Heat transfer from a cylinder placed on the vertical centre-line of a square enclosure partly filled with a porous medium that is saturated with a fluid has been numerically studied. The cylinder is buried in t he porous medium. The horizontal upper surface of the porous medium is separated from the rest of the enclosure by a horizontal impermeable barrier that is assumed to offer negligible resistance to heat transfe r. The gap between the barrier and the top of the enclosure is filled with the same fluid as that with which the porous medium is saturated. The surface of the cylinder is at a uniform high temperature. The bot tom and sides of the enclosure are assumed to be adiabatic while the h orizontal upper surface of the enclosure is assumed to be kept at a un iform low temperature. The natural convective flows that occur in the porous medium and in the fluid layer above the barrier have been assum ed to be steady, laminar, two-dimensional and symmetrical about the ve rtical centre-line of the enclosure. Fluid properties have been assume d constant except for the density change with temperature which gives rise to the buoyancy forces. The governing equations have been express ed in dimensionless form and solved using a finite element procedure. Results have been obtained for a Prandtl number of 0.7 for a wide rang e of the governing parameters. The main aim of the study was to determ ine how the mean heat transfer rate from the cylinder is affected by t he size of the fluid gap at the top of the enclosure. The effect of th is gap size has been related to changes in the flow pattern in the por ous and fluid regions.