Physics:Wiedemann–Franz law

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Short description: Law of physics
Plot of the Wiedemann–Franz law for copper. Left axis: specific electric resistance ρ in 10-10 Ω m, red line and specific thermal conductivity λ in W/(K m), green line. Right axis: ρ times λ in 100 U2/K, blue line and Lorenz number ρ λ / K in U2/K2, pink line. Lorenz number is more or less constant.

In physics, the Wiedemann–Franz law states that the ratio of the electronic contribution of the thermal conductivity (κ) to the electrical conductivity (σ) of a metal is proportional to the temperature (T).[1]

[math]\displaystyle{ \frac \kappa \sigma = LT }[/math]

Theoretically, the proportionality constant L, known as the Lorenz number, is equal to

[math]\displaystyle{ L = \frac \kappa {\sigma T} = \frac{\pi^2} 3 \left(\frac{k_{\rm B}} e \right)^2 = 2.44\times 10^{-8}\;\mathrm{V}^2\mathrm{K}^{-2}, }[/math]

where kB is Boltzmann's constant and e is the elementary charge.

This empirical law is named after Gustav Wiedemann and Rudolph Franz, who in 1853 reported that κ/σ has approximately the same value for different metals at the same temperature.[2] The proportionality of κ/σ with temperature was discovered by Ludvig Lorenz in 1872.[3]

Derivation

Electric circuit with metal and a battery U. The arrows indicate the direction of the electric field E and the electric current density j.

Qualitatively, this relationship is based upon the fact that the heat and electrical transport both involve the free electrons in the metal.

The mathematical expression of the law can be derived as following. Electrical conduction of metals is a well-known phenomenon and is attributed to the free conduction electrons, which can be measured as sketched in the figure. The current density j is observed to be proportional to the applied electric field and follows Ohm's law where the prefactor is the specific electrical conductivity. Since the electric field and the current density are vectors Ohm's law is expressed here in bold face. The conductivity can in general be expressed as a tensor of the second rank (3×3 matrix). Here we restrict the discussion to isotropic, i.e. scalar conductivity. The specific resistivity is the inverse of the conductivity. Both parameters will be used in the following.

Drude model derivation

Paul Drude (c. 1900) realized that the phenomenological description of conductivity can be formulated quite generally (electron-, ion-, heat- etc. conductivity). Although the phenomenological description is incorrect for conduction electrons, it can serve as a preliminary treatment.[4]

The assumption is that the electrons move freely in the solid like in an ideal gas. The force applied to the electron by the electric field leads to an acceleration according to

[math]\displaystyle{ \mathbf{F} = - e \mathbf{E} = m \frac{\;d\mathbf{v}}{dt} }[/math]
[math]\displaystyle{ \;d\mathbf{v}= - \frac{e \mathbf{E}} m dt }[/math]

This would lead, however, to a constant acceleration and, ultimately, to an infinite velocity. The further assumption therefore is that the electrons bump into obstacles (like defects or phonons) once in a while which limits their free flight. This establishes an average or drift velocity Vd. The drift velocity is related to the average scattering time as becomes evident from the following relations.

[math]\displaystyle{ \frac{d\mathbf{v}}{dt}= - \frac{e \mathbf{E}} m - \frac{1}{\tau} \mathbf{v} }[/math]

From kinetic theory of gases, [math]\displaystyle{ \kappa = \frac{1}{3}c n\,\ell \,\langle v\rangle }[/math], where [math]\displaystyle{ c = \frac 32 k_{\rm B} }[/math] is the heat capacity per electron, [math]\displaystyle{ \ell }[/math] is the mean free path of electron, and

[math]\displaystyle{ \langle v\rangle = \sqrt{\frac{8k_{\rm B} T}{\pi m}}=\sqrt{\frac{8}{3\pi}}v_{\rm rms} }[/math],

is the average speed of the particles in the gas.

From Drude model,

[math]\displaystyle{ \sigma = \frac{ne^2\tau}{m} = \frac{ne^2\ell}{m\langle v\rangle} }[/math].

Therefore,

[math]\displaystyle{ \frac \kappa \sigma = \frac{c m \, \langle {v} \rangle^2}{3e^2} = \frac{4}{\pi} \frac{k_{\rm B}^2T}{e^2} = 0.94\times 10^{-8}\;\mathrm{V}^2\mathrm{K}^{-2} }[/math],

which is the Wiedemann–Franz law with an erroneous proportionality constant [math]\displaystyle{ \frac{4}{\pi}\approx 1.27 }[/math].

In Drude's original paper he used [math]\displaystyle{ \langle v^2\rangle }[/math] instead of [math]\displaystyle{ \langle v\rangle^2 }[/math], and also accidentally used a factor of 2. This meant his result is [math]\displaystyle{ L = 3 \left(\frac{k_{\rm B}} e \right)^2 = 2.22\times 10^{-8}\;\mathrm{V}^2\mathrm{K}^{-2}, }[/math]which is very close to experimental values. This is in fact due to 3 mistakes that conspired to make his result more accurate than warranted: the factor of 2 mistake; the specific heat per electron is in fact about 100 times less than [math]\displaystyle{ \frac 32 k_{\rm B} }[/math]; the mean squared velocity of electron is in fact about 100 times larger.[5]

Free electron model

After taking into account the quantum effects, as in the free electron model, the heat capacity, mean free path and average speed of electrons are modified and the proportionality constant is then corrected to [math]\displaystyle{ \frac{\pi^2} 3\approx3.29 }[/math], which agrees with experimental values.

Temperature dependence

The value L0 = 2.44×10−8 V2K−2 results from the fact that at low temperatures ([math]\displaystyle{ T\rightarrow 0 }[/math] K) the heat and charge currents are carried by the same quasi-particles: electrons or holes. At finite temperatures two mechanisms produce a deviation of the ratio [math]\displaystyle{ L = \kappa/(\sigma T) }[/math] from the theoretical Lorenz value L0: (i) other thermal carriers such as phonon or magnons, (ii) Inelastic scattering. As the temperature tends to 0K, inelastic scattering becomes weak and promotes large q scattering values (trajectory a in the figure). For each electron transported a thermal excitation is also carried and the Lorenz number is reached L = L0. Note that in a perfect metal, inelastic scattering would be completely absent in the limit [math]\displaystyle{ T\rightarrow 0 }[/math] K and the thermal conductivity would vanish [math]\displaystyle{ \kappa\rightarrow 0; L\rightarrow 0 }[/math]. At finite temperature small q scattering values are possible (trajectory b in the figure) and electron can be transported without the transport of a thermal excitation L(T) < L0. At higher temperatures, the contribution of phonon to thermal transport in a system becomes important. This can lead to L(T) > L0. Above the Debye temperature the phonon contribution to thermal transport is constant and the ratio L(T) is again found constant.

Sketch of the various scattering process important for the Wiedemann–Franz law.

[6][7]

Limitations of the theory

Experiments have shown that the value of L, while roughly constant, is not exactly the same for all materials. Kittel[8] gives some values of L ranging from L = 2.23×10−8V2K−2 for copper at 0 °C to L = 3.2×10−8V2K−2 for tungsten at 100 °C. Rosenberg[9] notes that the Wiedemann–Franz law is generally valid for high temperatures and for low (i.e., a few Kelvins) temperatures, but may not hold at intermediate temperatures.

In many high purity metals both the electrical and thermal conductivities rise as temperature is decreased. In certain materials (such as silver or aluminum) however, the value of L also may decrease with temperature. In the purest samples of silver and at very low temperatures, L can drop by as much as a factor of 10.[10]

In degenerate semiconductors, the Lorenz number L has a strong dependency on certain system parameters: dimensionality, strength of interatomic interactions and Fermi level. This law is not valid or the value of the Lorenz number can be reduced at least in the following cases: manipulating electronic density of states, varying doping density and layer thickness in superlattices and materials with correlated carriers. In thermoelectric materials there are also corrections due to boundary conditions, specifically open circuit vs. closed circuit. [11][12] [13]

Violations

In 2011, N. Wakeham et al. found that the ratio of the thermal and electrical Hall conductivities in the metallic phase of quasi-one-dimensional lithium molybdenum purple bronze Li0.9Mo6O17 diverges with decreasing temperature, reaching a value five orders of magnitude larger than that found in conventional metals obeying the Wiedemann–Franz law.[14][15] This due to spin-charge separation and it behaving as a Luttinger liquid.[14]

A Berkeley-led study in 2016 by S. Lee et al. also found a large violation of the Wiedemann–Franz law near the insulator-metal transition in VO2 nanobeams. In the metallic phase, the electronic contribution to thermal conductivity was much smaller than what would be expected from the Wiedemann–Franz law. The results can be explained in terms of independent propagation of charge and heat in a strongly correlated system.[16][17]

Molecular systems

In 2020, Galen Craven and Abraham Nitzan derived a Wiedemann-Franz law for molecular systems in which electronic conduction is dominated not by free electron motion as in metals, but instead by electron transfer between molecular sites.[18] The molecular Wiedemann-Franz law is given by

[math]\displaystyle{ \frac{\kappa}{\sigma} = L_\text{M}\frac{\lambda}{k_{\rm B}} }[/math]

where

[math]\displaystyle{ L_\text{M} = \frac{1} 2 \left(\frac{k_{\rm B}} e \right)^2 }[/math]

is the Lorenz number for molecules and [math]\displaystyle{ \lambda }[/math] is the reorganization energy for electron transfer.

See also

References

  1. ↑ Jones, William; March, Norman H. (1985). Theoretical Solid State Physics. Courier Dover Publications. ISBN 978-0-486-65016-6. https://archive.org/details/theoreticalsolid0001jone. 
  2. ↑ Franz, R.; Wiedemann, G. (1853). "Ueber die Wärme-Leitungsfähigkeit der Metalle" (in German). Annalen der Physik 165 (8): 497–531. doi:10.1002/andp.18531650802. Bibcode: 1853AnP...165..497F. https://zenodo.org/record/1423632. 
  3. ↑ Lorenz, L. (1872). "Bestimmung der Wärmegrade in absolutem Maasse" (in de). Annalen der Physik und Chemie 223 (11): 429–452. doi:10.1002/andp.18722231107. https://onlinelibrary.wiley.com/doi/10.1002/andp.18722231107. 
  4. ↑ Simon, Steven H. (2013). "3: Electrons in Metals: Drude Theory". The Oxford solid state basics. Oxford: Oxford university press. ISBN 978-0-19-968077-1. 
  5. ↑ Ashcroft, Neil W.; Mermin, N. David (2012). Solid state physics (Repr ed.). South Melbourne: Brooks/Cole Thomson Learning. pp. 23. ISBN 978-0-03-083993-1. 
  6. ↑ Mizutani, Uichiro (2003). Introduction to the Electron Theory of Metals. CAMBRIDGE UNIVERSITY PRESS. ISBN 9780511612626. 
  7. ↑ Thermal conductivity: theory, properties, and applications, edited by Terry Tritt, Kluwer Academic / Plenum Publishers, New York (2004), ISBN:978-0-387-26017-4
  8. ↑ Kittel, C., 2005. Introduction to Solid State Physics. John Wiley and Sons
  9. ↑ Rosenberg, H. 2004. The Solid State. Oxford University Press
  10. ↑ K. Gloos, C. Mitschka, F. Pobell and P. Smeibidl. Cryogenics, 30 (1990), p. 14, doi:10.1016/0011-2275(90)90107-N
  11. ↑ A. J. Minnich, M. S. Dresselhaus, Z. F. Ren and G. Chen. Bulk nanostructured thermoelectric materials: current research and future prospects, Energy & Environmental Science, 2009, 2, 466–479, doi:10.1039/b822664b
  12. ↑ A. Putatunda and D.J. Singh. Lorenz number in relation to estimates based on the Seebeck coefficient, Materials Today Physics, 2019, 8, 49-55, doi:10.1016/j.mtphys.2019.01.001
  13. ↑ Paothep Pichanusakorn, Prabhakar Bandaru. Nanostructured thermoelectrics, Materials Science and Engineering: R: Reports, Volume 67, Issues 2–4, 29 January 2010, pages 19–63, ISSN 0927-796X, doi:10.1016/j.mser.2009.10.001.
  14. ↑ 14.0 14.1 Wakeham, Nicholas; Bangura, Alimamy F.; Xu, Xiaofeng; Mercure, Jean-Francois; Greenblatt, Martha; Hussey, Nigel E. (2011-07-19). "Gross violation of the Wiedemann–Franz law in a quasi-one-dimensional conductor" (in en). Nature Communications 2: 396. doi:10.1038/ncomms1406. ISSN 2041-1723. PMID 21772267. Bibcode: 2011NatCo...2..396W. 
  15. ↑ "Bristol physicists break 150-year-old law". https://phys.org/news/2011-07-bristol-physicists-year-old-law.html. 
  16. ↑ Lee, Sangwook; Hippalgaonkar, Kedar; Yang, Fan; Hong, Jiawang; Ko, Changhyun; Suh, Joonki; Liu, Kai; Wang, Kevin et al. (2017-01-27). "Anomalously low electronic thermal conductivity in metallic vanadium dioxide" (in en). Science 355 (6323): 371–374. doi:10.1126/science.aag0410. ISSN 0036-8075. PMID 28126811. Bibcode: 2017Sci...355..371L. https://cloudfront.escholarship.org/dist/prd/content/qt4rk9v6jt/qt4rk9v6jt.pdf. 
  17. ↑ Yang, Sarah (2017-01-26). "For This Metal, Electricity Flows, But Not the Heat | Berkeley Lab". http://newscenter.lbl.gov/2017/01/26/electricity-not-heat-flows-in-vanadium-dioxide/. 
  18. ↑ Craven, Galen T.; Nitzan, Abraham (2020-02-12). "Wiedemann–Franz Law for Molecular Hopping Transport". Nano Letters 20 (2): 989–993. doi:10.1021/acs.nanolett.9b04070. ISSN 1530-6984. PMID 31951422. https://doi.org/10.1021/acs.nanolett.9b04070. 



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