
%0 Journal Article
%A Klemens, PG 
%T The Contribution of Phonons to the Thomson Coefficient
%J Australian Journal of Physics
%D 1954/09/01
%V 7
%N 3
%P 520-522
%K 
%R https://doi.org/10.1071/PH540520
%U https://www.publish.csiro.au/paper/PH540520 
%X An electric current of density j flowing in a temperature gradient \1T gives up heat in a reversible way; the amount of heat thus liberated per unit volume and unit time is given by -p.j\1T, (1) p. being the Thomson coefficient, which can be shown to be T d r l(Kl )' p.=-e dT(P Ko -~ 5' (2) where ~ is the Fermi energy, and the K's are the usual transport coefficients as defined by Mott and Jones (1936, p. 306, equation (99)), or more generally by Wilson (1953, p. 305). 
