The Wiedemann-Franz Law Asaf Rozen, Alexander Palevski, Eli Raz
The Wiedemann-Franz Law β’ Heat and electrical transport involve free electrons 2 ππ = π 2 π = π π πΆ = 2.44 β 10 β8 ππ» πΏ 2 3 π π π
The Wiedemann-Franz Law β’ Discovered in 1853 by Gustav Wiedemann and Rudolph Franz β’ Broadly used in modern solid state physics Crossno, J., Shi, J. K., Wang, K., Liu, X., Harzheim, A., Lucas, A., ... & Ohki, T. A. (2016). Observation of the Dirac fluid and the breakdown of the Wiedemann- Franz law in graphene. Science , 351 (6277), 1058- 1061.
Parts Of The Experiment β’ Part A β Electric conductivity (π) of various metals. β’ Part B β Thermal conductivity (π) of Copper. β’ Part C β Measure heat capacity (π π ) and heat loss. β’ Part D β Measure the relative π of different metals. β’ Part E β Discover the Wiedemann-Franz law.
Equipment
Part A β Electrical conductivy (π) β’ Aluminum, Brass and Copper tubes Top View β’ Small magnet falls at a constant speed
Part B β Thermal conductivity (π) Temperature [C] β’ Power on one side, Reservoir on the other Heater Position [m] reservoir Heat
Part B β Thermal conductivity (π) Isolated Rod Readout Box Heat Reservoir
Part B β Thermal conductivity (π)
Part C β Measure Heat Capacity And Heat Loss To Correct π reservoir Heater Heat
Part C β Measure Heat Capacity And Heat Loss To Correct π reservoir Heater Heat
Part C β Measure Heat Capacity And Heat Loss To Correct π β’ The rod is not at steady state β’ There is heat loss to the environment
Part C β Measure Heat Capacity And Heat Loss To Correct π β’ The rod is not at steady state β’ There is heat loss to the environment β’ We use cooling- heating-cooling cycle
Part D β Measure The Relative π Of Different Metals β’ Using alternating material rod β’ Get accurate relative thermal conductivity β’ Using the knowledge from part C to correct results reservoir Heat reservoir Heat
Part E β Discover The Wiedemann-Franz Law Acknowledgments β Roy Beck- Barkai, Yoram Dagan
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