Abstract
The theoretical basis of the Wiedemann-Franz-Lorenz law is reviewed. The Lorenz ratio takes the Sommerfeld value Lo provided (a) the thermal conductivity is electronic (b) the electron gas is highly degenerate and (c) the effective relaxation time is the same for electrical and for thermal conduction. The conditions are discussed for high degeneracy, and for deviations from Lo at high temperatures. It is shown that the relaxation time is unique except for pure metals at low temperatures and cases when electron-electron scattering is important. Corrections for the lattice thermal conductivity are not discussed in detail.
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References
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© 1989 Purdue Research Foundation
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Klemens, P.G. (1989). Theory of Lorenz Ratio of Metals and Alloys. In: Hasselman, D.P.H., Thomas, J.R. (eds) Thermal Conductivity 20. Springer, Boston, MA. https://doi.org/10.1007/978-1-4613-0761-7_6
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DOI: https://doi.org/10.1007/978-1-4613-0761-7_6
Publisher Name: Springer, Boston, MA
Print ISBN: 978-1-4612-8069-9
Online ISBN: 978-1-4613-0761-7
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