Metals — Question 9

Section 41-4 · Physics pages 6868–6869

Question 9 Electrical resistance estimates electronic heat conduction Assume the Wiedemann–Franz relation κeρ = L0T, with L0 = 2.44 × 10−8 W Ω/K2. A metal at 300 K has ρ = 2.00 × 10−8 Ωm. ˙Q L A Schematic; labels, not drawing lengths, specify the data. (a) Find its electronic thermal conductivity. (b) A rod has area 2.00 mm2, length .100 m, and a small temperature difference 5.00 K near 300 K. Find heat flow and the product of electrical resistance and thermal conductance.
Show solutionHide solution
Question 9 - Solution Electrical resistance estimates electronic heat conduction ˙Q L A (a) Method and calculation κe = L0T/ρ = 366 W/(m K) . κe ∝T/ρ within the supplied transport model. (b) Interpretation and further calculation ˙Q = κeA∆T/L = .0366 W . R = ρL/A, Gth = κeA/L ⇒RGth = L0T = 7.32 × 10−6 W Ω/K . Physical check The geometry cancels in the product. Lattice heat transport and departures from the assumed Lorenz number can change the total measured thermal conductivity.

Question 9

Electrical resistance estimates electronic heat conduction

Assume the Wiedemann–Franz relation κeρ=L0T\kappa_e\rho=L_0T, with L0=2.44×10−8WΩ/K2L_0=2.44\times10^{-8}\,\mathrm{W\,\Omega/K^2}. A metal at 300 K has ρ=2.00×10−8Ωm\rho=2.00\times10^{-8}\,\Omega\,\mathrm m.

Diagram shown in the original SVG worksheet.

  1. Find its electronic thermal conductivity.

  2. A rod has area 2.00mm22.00\,\mathrm{mm^2}, length .100 m, and a small temperature difference 5.00 K near 300 K. Find heat flow and the product of electrical resistance and thermal conductance.

Question 9 - Solution

Electrical resistance estimates electronic heat conduction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

κe=L0T/ρ=366W/(mK).\boxed{\kappa_e=L_0T/\rho=366\,\mathrm{W/(m\,K)}}.κe∝T/ρwithin the supplied transport model.\kappa_e\propto T/\rho\quad\text{within the supplied transport model}.

(b) Interpretation and further calculation

Q̇=κeAΔT/L=.0366W.\boxed{\dot Q=\kappa_e A\Delta T/L=.0366\,\mathrm W}.R=ρL/A,Gth=κeA/L⇒RGth=L0T=7.32×10−6WΩ/K.R=\rho L/A,\quad G_{\mathrm{th}}=\kappa_e A/L\Rightarrow\boxed{RG_{\mathrm{th}}=L_0T=7.32\times10^{-6}\,\mathrm{W\,\Omega/K}}.

Physical check

The geometry cancels in the product. Lattice heat transport and departures from the assumed Lorenz number can change the total measured thermal conductivity.