Copyright © 2004 Elsevier Ltd. All rights reserved.
Thermal radiation in ultralight metal foams with open cells
Received 13 June 2003;
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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
eff- total emissivity
λ,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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