ScienceDirect® Home Skip Main Navigation Links
You have guest access to ScienceDirect. Find out more.
 
Home
Browse
My Settings
Alerts
Help
 Quick Search
 Search tips (Opens new window)
    Clear all fields    
advertisementadvertisement
International Journal of Heat and Mass Transfer
Volume 43, Issue 13, 1 July 2000, Pages 2245-2256
 
Font Size: Decrease Font Size  Increase Font Size
 Abstract - selected
Article
Purchase PDF (382 K)

 
 
 
Related Articles in ScienceDirect
View More Related Articles
 
View Record in Scopus
 
doi:10.1016/S0017-9310(99)00318-X    How to Cite or Link Using DOI (Opens New Window)
Copyright © 2000 Elsevier Science Ltd. All rights reserved.

Thermal management of high power electronics with phase change cooling

T. J. LuE-mail The Corresponding Author

Department of Engineering, Cambridge University, Cambridge CB2 1PZ, UK

Received 24 June 1999;
revised 18 October 1999.
Available online 8 March 2000.

Purchase the full-text article



References and further reading may be available for this article. To view references and further reading you must purchase this article.

Abstract

A study on the prospect of designing high power electronic packages with phase change cooling is presented, with special emphasis on minimising the rising of junction temperatures due to thermal transient effects. The one-dimensional thermal model consists of a finite slab suddenly exposed to a uniform heat flux at the top surface and cooled by convective air at the bottom. The phase change problem is divided into sub-problems and solved progressively. Before the slab starts to melt, both exact and approximate solutions are presented for the distribution of temperature in the slab as functions of time and Biot number Bi. The necessity of partitioning the time domain into two regimes, separated by the time t0 needed for the thermal front to traverse across the whole slab, is emphasised. After the slab melts, quasi-steady state solutions are obtained both for the melt depth and the evolution of surface temperature as functions of time and Biot number when tm>t0, with tm denoting the time needed for melting to commence at the top surface of the slab. The quasi-steady state solutions are compared with those obtained by using the method of finite elements. Approximate but simple analytical solutions are also constructed for the tm<t0 case which, again, are compared with the finite element results. Finally, these solutions are analysed to guide the design of advanced packages with optimised phase change cooling strategies.

Author Keywords: Phase change cooling; Power electronics; Thermal management; Finite elements; Materials selection

Nomenclature

Bi
Biot number
cs, cl
solid and melt specific heat
h
local heat transfer coefficient
H
phase change layer thickness
I1, I2
material indices
ks, kl
Solid and melt thermal conductivities
L
latent heat
Q
heat flux
t
time
tc
time for complete melting
t0
thermal penetration time
tm
melting time
T0
initial and environmental temperature
Tm, Tv
melting and boiling temperatures
Ts, Tl
solid and melt temperatures
x
coordinate
X
melt front position
ΔT
TmT0
κs, κl
solid and melt thermal diffusivities
ρ
density
l
liquid
s
solid

Article Outline

Nomenclature
1. Introduction
2. Specifications of the problem
3. Solutions before melting
3.1. Temperature profiles
3.2. Temperature regimes I and II
4. Solutions for low power densities (tm>t0)
4.1. Quasi-steady state solutions
4.2. Range of validity
5. Solutions for high power densities (tm<t0)
5.1. Approximate solutions
5.2. Finite element solutions
6. Design implications
Acknowledgements
Appendix. Effective coefficient of heat transfer
References








 
Home
Browse
My Settings
Alerts
Help
Elsevier.com (Opens new window)
About ScienceDirect  |  Contact Us  |  Information for Advertisers  |  Terms & Conditions  |  Privacy Policy
Copyright © 2008 Elsevier B.V. All rights reserved. ScienceDirect® is a registered trademark of Elsevier B.V.