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Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure

Conjugate natural convection-conduction heat transfer in a square enclosure with a finite wall thickness is studied numerically in the present paper. The governing parameters considered are the Rayleigh number (5 × 10(3) ≤ Ra ≤ 10(6)), the wall-to-fluid thermal conductivity ratio (0.5 ≤ Kr ≤ 10), an...

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Autores principales: Saleh, Habibis, Hashim, Ishak
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Hindawi Publishing Corporation 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4058157/
https://www.ncbi.nlm.nih.gov/pubmed/24971390
http://dx.doi.org/10.1155/2014/786102
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author Saleh, Habibis
Hashim, Ishak
author_facet Saleh, Habibis
Hashim, Ishak
author_sort Saleh, Habibis
collection PubMed
description Conjugate natural convection-conduction heat transfer in a square enclosure with a finite wall thickness is studied numerically in the present paper. The governing parameters considered are the Rayleigh number (5 × 10(3) ≤ Ra ≤ 10(6)), the wall-to-fluid thermal conductivity ratio (0.5 ≤ Kr ≤ 10), and the ratio of wall thickness to its height (0.2 ≤ D ≤ 0.4). The staggered grid arrangement together with MAC method was employed to solve the governing equations. It is found that the fluid flow and the heat transfer can be controlled by the thickness of the bottom wall, the thermal conductivity ratio, and the Rayleigh number.
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spelling pubmed-40581572014-06-26 Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure Saleh, Habibis Hashim, Ishak ScientificWorldJournal Research Article Conjugate natural convection-conduction heat transfer in a square enclosure with a finite wall thickness is studied numerically in the present paper. The governing parameters considered are the Rayleigh number (5 × 10(3) ≤ Ra ≤ 10(6)), the wall-to-fluid thermal conductivity ratio (0.5 ≤ Kr ≤ 10), and the ratio of wall thickness to its height (0.2 ≤ D ≤ 0.4). The staggered grid arrangement together with MAC method was employed to solve the governing equations. It is found that the fluid flow and the heat transfer can be controlled by the thickness of the bottom wall, the thermal conductivity ratio, and the Rayleigh number. Hindawi Publishing Corporation 2014 2014-05-28 /pmc/articles/PMC4058157/ /pubmed/24971390 http://dx.doi.org/10.1155/2014/786102 Text en Copyright © 2014 H. Saleh and I. Hashim. https://creativecommons.org/licenses/by/3.0/ This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Research Article
Saleh, Habibis
Hashim, Ishak
Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure
title Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure
title_full Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure
title_fullStr Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure
title_full_unstemmed Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure
title_short Conjugate Heat Transfer in Rayleigh-Bénard Convection in a Square Enclosure
title_sort conjugate heat transfer in rayleigh-bénard convection in a square enclosure
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4058157/
https://www.ncbi.nlm.nih.gov/pubmed/24971390
http://dx.doi.org/10.1155/2014/786102
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