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Thermal Spreading and Contact Resistance: Fundamentals and ApplicationsAvailable to Purchase
By
Yuri S. Muzychka,
Yuri S. Muzychka
Department of Mechanical and Mechatronics Engineering, Faculty of Engineering and Applied Science, Memorial University of Newfoundland, St. John’s, NL, Canada
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M. Michael Yovanovich
M. Michael Yovanovich
University of Waterloo, Department of Mechanical and Mechatronics Engineering, Faculty of Engineering, University of Waterloo, Waterloo, Ontario, Canada
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ISBN:
9781394187522
No. of Pages:
464
Publisher:
ASME
Publication date:
2023
eBook Chapter
2. Thermal Spreading in Isotropic Half-Space Regions Available to Purchase
By
Yuri S. Muzychka
,
Yuri S. Muzychka
Department of Mechanical and Mechatronics Engineering, Faculty of Engineering and Applied Science, Memorial University of Newfoundland, St. John’s, NL, Canada
Search for other works by this author on:
M. Michael Yovanovich
M. Michael Yovanovich
University of Waterloo, Department of Mechanical and Mechatronics Engineering, Faculty of Engineering, University of Waterloo, Waterloo, Ontario, Canada
Search for other works by this author on:
Page Count:
56
-
Published:2023
Citation
Muzychka, YS, & Yovanovich, MM. "Thermal Spreading in Isotropic Half-Space Regions." Thermal Spreading and Contact Resistance: Fundamentals and Applications. Ed. Muzychka, YS, & Yovanovich, MM. ASME, 2023.
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Steady or transient heat transfer occurs in a semi-infinite region or half-space z > 0, which may be isotropic or it may consist of one or more thin isotropic layers bonded to the isotropic half-space. The heat source is some planar singly or doubly connected area such as a circular annulus located in the “free” surface z = 0 of the half-space. The dimensions of the half-space are much larger than the largest dimension of the source area. The “free” surface z = 0 of the half-space outside the source area is traditionally assumed to be adiabatic.
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