Modeling of non-uniform thermoelement devices subject to lateral heat convection

In this paper, we draw attention to the importance of the lateral convection heat transfer effect on the operation of thermoelements with variable cross-sectional area. The significance of lateral heat convection arises from a new application, in which thermoelements form the walls of a MEMS-based...

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Main Authors: Kafafy, Raed, Hameed, Ammar
Format: Article
Language:English
Published: Scitec Publications Ltd. 2011
Subjects:
Online Access:http://irep.iium.edu.my/4270/
http://irep.iium.edu.my/4270/
http://irep.iium.edu.my/4270/
http://irep.iium.edu.my/4270/1/DDF.312-315.782.pdf
id iium-4270
recordtype eprints
spelling iium-42702013-07-03T04:45:33Z http://irep.iium.edu.my/4270/ Modeling of non-uniform thermoelement devices subject to lateral heat convection Kafafy, Raed Hameed, Ammar TJ Mechanical engineering and machinery TL Motor vehicles. Aeronautics. Astronautics In this paper, we draw attention to the importance of the lateral convection heat transfer effect on the operation of thermoelements with variable cross-sectional area. The significance of lateral heat convection arises from a new application, in which thermoelements form the walls of a MEMS-based convergent-divergent micronozzle in order to pump heat from the divergent part of the micronozzle to the convergent part to enhance overall performance. To assess the effect of thermoelement, we develop a quasi-one-dimensional model for thermoelements, in which, the physical phenomena of Peltier effect, Joule heating, Seebeck effect, longitudinal heat conduction, and lateral heat convection are considered. The general energy equation of the thermoelement with variable material properties is formulated with heat convection modeled as a lateral heat source. We used the model to study thermoelements with rectangular cross section and uniform thickness, but variable width. The width of the element is maximum at the location forming the micronozzle throat. Several geometries have been investigated; a piece-wise linear, parabolic and piece-wise sine wave. Two parameters which play important role in the thermal performance of thermoelement are identified. These are the thermal resistance ratio; ratio of longitudinal conduction resistance to lateral convection resistance, and heating ratio; ratio of Joule heating to Fourier conducted heat. The effects of varying these two parameters as well as thermoelement geometry have been investigated thoroughly and the results are presented in the form of charts to assist the design and material selection of the thermoelement. Scitec Publications Ltd. 2011-04 Article PeerReviewed application/pdf en http://irep.iium.edu.my/4270/1/DDF.312-315.782.pdf Kafafy, Raed and Hameed, Ammar (2011) Modeling of non-uniform thermoelement devices subject to lateral heat convection. Defect and Diffusion Forum, 312. pp. 782-787. ISSN 1012-0386 http://www.ttp.net/1012-0386.html doi:10.4028/www.scientific.net/DDF.312-315.782
repository_type Digital Repository
institution_category Local University
institution International Islamic University Malaysia
building IIUM Repository
collection Online Access
language English
topic TJ Mechanical engineering and machinery
TL Motor vehicles. Aeronautics. Astronautics
spellingShingle TJ Mechanical engineering and machinery
TL Motor vehicles. Aeronautics. Astronautics
Kafafy, Raed
Hameed, Ammar
Modeling of non-uniform thermoelement devices subject to lateral heat convection
description In this paper, we draw attention to the importance of the lateral convection heat transfer effect on the operation of thermoelements with variable cross-sectional area. The significance of lateral heat convection arises from a new application, in which thermoelements form the walls of a MEMS-based convergent-divergent micronozzle in order to pump heat from the divergent part of the micronozzle to the convergent part to enhance overall performance. To assess the effect of thermoelement, we develop a quasi-one-dimensional model for thermoelements, in which, the physical phenomena of Peltier effect, Joule heating, Seebeck effect, longitudinal heat conduction, and lateral heat convection are considered. The general energy equation of the thermoelement with variable material properties is formulated with heat convection modeled as a lateral heat source. We used the model to study thermoelements with rectangular cross section and uniform thickness, but variable width. The width of the element is maximum at the location forming the micronozzle throat. Several geometries have been investigated; a piece-wise linear, parabolic and piece-wise sine wave. Two parameters which play important role in the thermal performance of thermoelement are identified. These are the thermal resistance ratio; ratio of longitudinal conduction resistance to lateral convection resistance, and heating ratio; ratio of Joule heating to Fourier conducted heat. The effects of varying these two parameters as well as thermoelement geometry have been investigated thoroughly and the results are presented in the form of charts to assist the design and material selection of the thermoelement.
format Article
author Kafafy, Raed
Hameed, Ammar
author_facet Kafafy, Raed
Hameed, Ammar
author_sort Kafafy, Raed
title Modeling of non-uniform thermoelement devices subject to lateral heat convection
title_short Modeling of non-uniform thermoelement devices subject to lateral heat convection
title_full Modeling of non-uniform thermoelement devices subject to lateral heat convection
title_fullStr Modeling of non-uniform thermoelement devices subject to lateral heat convection
title_full_unstemmed Modeling of non-uniform thermoelement devices subject to lateral heat convection
title_sort modeling of non-uniform thermoelement devices subject to lateral heat convection
publisher Scitec Publications Ltd.
publishDate 2011
url http://irep.iium.edu.my/4270/
http://irep.iium.edu.my/4270/
http://irep.iium.edu.my/4270/
http://irep.iium.edu.my/4270/1/DDF.312-315.782.pdf
first_indexed 2023-09-18T20:12:26Z
last_indexed 2023-09-18T20:12:26Z
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