2011
DOI: 10.4028/www.scientific.net/ddf.312-315.477
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Numerical Investigation of Impingement Heat Transfer Enhancement on a Flat Plate with an Attached Porous Medium

Abstract: The enhancement of impingement heat transfer on a flat plate covered with a thick layer of porous medium with or without a center hole was numerically investigated. The renormalization group turbulence model is selected for the fluid region while Forchheimer extended Darcy’s model is used for porous region. The numerical models were justified by comparisons with available experimental data. Computational results show that an attached porous medium with a center hole can effectively enhance jet impingement heat… Show more

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Cited by 1 publication
(7 citation statements)
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“…4. This conclusion agrees with that of [3,4]. It should be mentioned that in the present study, a center through hole is always made whenever the target plate is covered with porous material.…”
Section: Resultssupporting
confidence: 92%
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“…4. This conclusion agrees with that of [3,4]. It should be mentioned that in the present study, a center through hole is always made whenever the target plate is covered with porous material.…”
Section: Resultssupporting
confidence: 92%
“…The through hole is designed to trap the jet fluid so that it can reach the target plate and exchange heat which it more easily than the cases without a hole or with a shallower hole. It was shown in [3,4] that an attached porous medium with a center hole can effectively enhance jet impingement heat transfer on a flat plate when the cavity is deep enough, while an attached thick porous layer without a center hole has detrimental effect on heat transfer. When a comparison of the present results with that of a flat plate [4] (not shown for clarity of the figure) is made, it is found that for a target covered with thick porous material having a center trapping hole, the semi-spherical concave surface has about 20% -45% increase at the Defect and Diffusion Forum Vol.…”
Section: Resultsmentioning
confidence: 99%
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