Natural Convection in Trapezoidal Enclosure Heated Partially from Below

Natural convection in a trapezoidal enclosure with partial heating from below and symmetrical cooling from the sides has been investigated numerically. The heating is simulated by a centrally located heat source on the bottom wall, and four different values of the dimensionless heat source length,...

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Main Authors: Ahmed W. Mustafa, Ihsan Ali Ghani
Format: Article
Language:English
Published: Al-Khwarizmi College of Engineering – University of Baghdad 2012-02-01
Series:Al-Khawarizmi Engineering Journal
Subjects:
Online Access:http://alkej.uobaghdad.edu.iq/index.php/alkej/article/view/107
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spelling doaj-fb57d0d41fc44a988e3020588aa224382020-11-25T02:22:58Zeng Al-Khwarizmi College of Engineering – University of BaghdadAl-Khawarizmi Engineering Journal1818-11712312-07892012-02-0181Natural Convection in Trapezoidal Enclosure Heated Partially from BelowAhmed W. Mustafa0Ihsan Ali Ghani1Department of Mechanical Engineering/College of Engineering/University of TikritDepartment of Mechanical Engineering/College of Engineering/University of Al-Mustansiriya Natural convection in a trapezoidal enclosure with partial heating from below and symmetrical cooling from the sides has been investigated numerically. The heating is simulated by a centrally located heat source on the bottom wall, and four different values of the dimensionless heat source length, 1/5, 2/5, 3/5, 4/5 are considered. The laminar flow field is analyzed numerically by solving the steady, two-dimensional incompressible Navier-Stokes and energy equations. The Cartesian velocity components and pressure on a collocated (non-staggered) grid are used as dependent variables in the momentum equations  discretized by finite volume method; body fitted coordinates are used to represent the trapezoidal enclosure, and grid generation technique based on elliptic partial differential equations is employed. SIMPLE algorithm is used to adjust the velocity field to satisfy the conservation of mass. The range of Rayleigh number is (103≤ Ra ≤105) and Prandtl number is 0.7. The results show that the average Nusselt number increases with the increases of the source length. http://alkej.uobaghdad.edu.iq/index.php/alkej/article/view/107Natural ConvectionTrapezoidal EnclosureFinite Volume
collection DOAJ
language English
format Article
sources DOAJ
author Ahmed W. Mustafa
Ihsan Ali Ghani
spellingShingle Ahmed W. Mustafa
Ihsan Ali Ghani
Natural Convection in Trapezoidal Enclosure Heated Partially from Below
Al-Khawarizmi Engineering Journal
Natural Convection
Trapezoidal Enclosure
Finite Volume
author_facet Ahmed W. Mustafa
Ihsan Ali Ghani
author_sort Ahmed W. Mustafa
title Natural Convection in Trapezoidal Enclosure Heated Partially from Below
title_short Natural Convection in Trapezoidal Enclosure Heated Partially from Below
title_full Natural Convection in Trapezoidal Enclosure Heated Partially from Below
title_fullStr Natural Convection in Trapezoidal Enclosure Heated Partially from Below
title_full_unstemmed Natural Convection in Trapezoidal Enclosure Heated Partially from Below
title_sort natural convection in trapezoidal enclosure heated partially from below
publisher Al-Khwarizmi College of Engineering – University of Baghdad
series Al-Khawarizmi Engineering Journal
issn 1818-1171
2312-0789
publishDate 2012-02-01
description Natural convection in a trapezoidal enclosure with partial heating from below and symmetrical cooling from the sides has been investigated numerically. The heating is simulated by a centrally located heat source on the bottom wall, and four different values of the dimensionless heat source length, 1/5, 2/5, 3/5, 4/5 are considered. The laminar flow field is analyzed numerically by solving the steady, two-dimensional incompressible Navier-Stokes and energy equations. The Cartesian velocity components and pressure on a collocated (non-staggered) grid are used as dependent variables in the momentum equations  discretized by finite volume method; body fitted coordinates are used to represent the trapezoidal enclosure, and grid generation technique based on elliptic partial differential equations is employed. SIMPLE algorithm is used to adjust the velocity field to satisfy the conservation of mass. The range of Rayleigh number is (103≤ Ra ≤105) and Prandtl number is 0.7. The results show that the average Nusselt number increases with the increases of the source length.
topic Natural Convection
Trapezoidal Enclosure
Finite Volume
url http://alkej.uobaghdad.edu.iq/index.php/alkej/article/view/107
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