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Radiative Thermal Conductivity in Planetary Interiors

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Abstract

IT is customary to invoke radiative thermal conductivity as a mechanism for efficiently removing heat from the Earth's interior1. Clark2 derived the formula for radiative thermal conductivity in planetary conditions, where n is the refractive index, B is the blackbody function, γ is the radiation wavelength, α is the absorption coefficient and s is the backscattering coefficient. He used this relationship to estimate the radiative conductivity for a number of minerals by measuring α at room temperature and neglecting s (ref. 3).

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References

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  2. Clark, jun., S. P., Trans. Amer. Geophys. Un., 38, 931 (1957).

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  3. Clark, jun., S. P., Amer. Mineral., 42, 732 (1957).

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  4. McConnell, jun., R. K., McClaine, L. A., Lee, D. W., Aronson, J. R., and Allen, R. V., Rev. Geophys., 5, 121 (1967).

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  5. Aronson, J. R., Emslie, A. G., McConnell, jun., R. K., Eckroad, S. W., and von Thüna, P. C., Trans. Amer. Geophys. Un., 48, 211 (1967).

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  6. Aronson, J. R., Emslie, A. G., McConnell, jun., R. K., Eckroad, S. W., and von Thüna, P. C., Rep. NASA Manned Spacecraft Center (Contract NAS9–5840) (1967).

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ARONSON, J., ECKROAD, S., EMSLIE, A. et al. Radiative Thermal Conductivity in Planetary Interiors. Nature 216, 1096–1097 (1967). https://doi.org/10.1038/2161096a0

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