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International Journal of Heat and Mass Transfer
Volume 47, Issues 14-16, July 2004, Pages 2927-2939
 
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doi:10.1016/j.ijheatmasstransfer.2004.03.006    How to Cite or Link Using DOI (Opens New Window)
Copyright © 2004 Elsevier Ltd. All rights reserved.

Thermal radiation in ultralight metal foams with open cells

C. Y. Zhao1, T. J. LuCorresponding Author Contact Information, E-mail The Corresponding Author and H. P. Hodson

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

Received 13 June 2003; 
Revised 16 March 2004. 
Available online 23 April 2004.

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Abstract

This paper presents results from experimental measurements on radiative transfer in FeCrAlY (a steel based high temperature alloy) foams having high porosity (95%) and different cell sizes, manufactured at low cost from the sintering route. The spectral transmittance and reflectance are measured at different infrared wavelengths ranging from 2.5 to 50 μm, which are subsequently used to determine the extinction coefficient and foam emissivity. The results show that the spectral quantities are strongly dependent on the wavelength, particularly in the short wavelength regime (<25 μm). Whilst the extinction coefficient decreases with increasing cell size, the effect of cell size on foam reflectance is not significant. When the temperature is increased, the total extinction coefficient increases but the total reflectance decreases. An analytical model based on geometric optics laws, diffraction theory and metal foam morphology is developed to predict the radiative transfer, with cell size (or cell ligament diameter) and porosity identified as the two key parameters that dictate the foam radiative properties. Close agreement between the predicted effective foam conductivity due to radiation alone and that measured is observed. At fixed porosity, the radiative conductivity of the metal foam increases with increasing cell size and temperature.

Author Keywords: Metal foams; Thermal radiation; Transmittance; Reflectance; Extinction coefficient; Emissivity; Experimental measurement; Modelling

Nomenclature

Nomenclature
C, C1, C2
constants
Cs
correction scan of source with sample
Ce
correction scan of source without sample
di
inner diameter of cell ligament, m
do
outer diameter of cell ligament, m
dp
cell size, m
D0
dark sample scan for zero offset
E
emissive power
f
influence function, Eq. (24)
I, Iλ
total intensity and spectral intensity of radiant energy
K, Kλ
total and spectral extinction coefficient, 1/m
KR
Rosseland mean extinction coefficient, 1/m
Kλ*
weighted spectral extinction coefficient, 1/m
kc
effective thermal conductivity due to conduction, W/mK
ke
effective thermal conductivity of metal foam, W/mK
kr
effective radiative thermal conductivity, W/mK
L
sample height, m
m
complex refractive index
n
constant
q
heat flux, W/m2
Rf
reference scan (hemisphere radiance)
S
sample scan (sample radiance)
T
temperature, K
α, αλ
absorption coefficient and spectral volume absorption coefficient
χ
non-dimensional size parameter
var epsiloneff
total emissivity
var epsilonλ,eff
spectral emissivity
λ
wavelength, m
ρeff
total reflectance
ρλ,eff
spectral reflectance
σ
Stefan–Boltzman constant
σs
scattering coefficient
τ, τλ
total transmittance and spectral transmittance
φ
porosity of foam
Φλ
spectral volumetric phase function of scattering

Article Outline

Nomenclature
1. Introduction
2. Metal foam samples
3. Experimental equipment and measurement procedures
4. Experimental results
4.1. Spectral transmittance, τλ
4.2. Extinction coefficient
4.3. Reflectance
4.4. Emissivity
4.5. Effective radiative conductivity kr
5. Modeling based on the effective medium approach
5.1. Rosseland diffusion
5.2. Spectral absorption and scattering coefficients
5.3. Phase function
5.4. Prediction versus measurement
6. Conclusions
Acknowledgements
References
















 
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