Thermal conductivity and Lorenz number of the Ce1−xLaxNiAl4 Kondo alloys

2014 ◽  
Vol 193 ◽  
pp. 26-29 ◽  
Author(s):  
A. Kowalczyk ◽  
M. Falkowski ◽  
T. Toliński
1966 ◽  
Vol 44 (9) ◽  
pp. 2035-2039 ◽  
Author(s):  
T. M. Dauphinee ◽  
L. D. Armstrong ◽  
S. B. Woods

Results of two previously unreported determinations of the thermal conductivity of very pure lead are given. The first set of measurements covered the temperature range −40 to +310 °C, while the second set covered the range 25 to 170 °C to check a small irregularity of the first set. The resistance ratio R/R0 of the first sample was measured from 0 °C to 160 °C. The results may be expressed within 1% by the linear equation K = 0.3555 – 1.36t/104 watt cm−1 °C−1. The Lorenz number drops linearly by about 0.5% between 0 and 150 °C.


1987 ◽  
Vol 120 (5) ◽  
pp. 241-245 ◽  
Author(s):  
Atsunobu Nakamura ◽  
Norio Kawakami ◽  
Ayao Okiji

ACS Nano ◽  
2018 ◽  
Vol 12 (2) ◽  
pp. 1120-1127 ◽  
Author(s):  
Zhe Luo ◽  
Jifa Tian ◽  
Shouyuan Huang ◽  
Mithun Srinivasan ◽  
Jesse Maassen ◽  
...  

1974 ◽  
Vol 35 (C4) ◽  
pp. C4-313-C4-316 ◽  
Author(s):  
G. BUSCH ◽  
H.-J. GÜNTHERODT ◽  
W. HALLER ◽  
P. WYSSMANN

RSC Advances ◽  
2018 ◽  
Vol 8 (44) ◽  
pp. 24893-24899 ◽  
Author(s):  
Gui-Cang He ◽  
Heng Lu ◽  
Xian-Zi Dong ◽  
Yong-Liang Zhang ◽  
Jie Liu ◽  
...  

Investigation of temperature dependence of electrical resistivity, thermal conductivity and Lorenz number of silver nanowire, and design of a thermometer.


1972 ◽  
Vol 41 (1) ◽  
pp. 29-30 ◽  
Author(s):  
G. Busch ◽  
H.-J. Güntherodt ◽  
W. Haller ◽  
P. Wyssmann

2020 ◽  
Vol 80 (8) ◽  
Author(s):  
Shubhalaxmi Rath ◽  
Binoy Krishna Patra

Abstract We have studied the effect of strong magnetic field on the charge and thermal transport properties of hot QCD matter at finite chemical potential. For this purpose, we have calculated the electrical conductivity ($$\sigma _\mathrm{el}$$σel) and the thermal conductivity ($$\kappa $$κ) using kinetic theory in the relaxation time approximation, where the interactions are subsumed through the distribution functions within the quasiparticle model at finite temperature, strong magnetic field and finite chemical potential. This study helps to understand the impacts of strong magnetic field and chemical potential on the local equilibrium by the Knudsen number ($$\Omega $$Ω) through $$\kappa $$κ and on the relative behavior between thermal conductivity and electrical conductivity through the Lorenz number (L) in the Wiedemann–Franz law. We have observed that, both $$\sigma _\mathrm{el}$$σel and $$\kappa $$κ get increased in the presence of strong magnetic field, and the additional presence of chemical potential further increases their magnitudes, where $$\sigma _\mathrm{el}$$σel shows decreasing trend with the temperature, opposite to its increasing behavior in the isotropic medium, whereas $$\kappa $$κ increases slowly with the temperature, contrary to its fast increase in the isotropic medium. The variation in $$\kappa $$κ explains the decrease of the Knudsen number with the increase of the temperature. However, in the presence of strong magnetic field and finite chemical potential, $$\Omega $$Ω gets enhanced and approaches unity, thus, the system may move slightly away from the equilibrium state. The Lorenz number ($$\kappa /(\sigma _\mathrm{el} T))$$κ/(σelT)) in the abovementioned regime of strong magnetic field and finite chemical potential shows linear enhancement with the temperature and has smaller magnitude than the isotropic one, thus, it describes the violation of the Wiedemann–Franz law for the hot and dense QCD matter in the presence of a strong magnetic field.


1989 ◽  
Vol 116 (1) ◽  
pp. 377-382 ◽  
Author(s):  
M. S. R. Chari ◽  
R. G. Sharma

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