Metals — Question 1

Section 41-4 · Physics pages 6852–6853

Question 1 Momentum relaxation sets the metallic dc conductivity A one-band metal has electron density n, effective mass m, and relaxation time τ. Its mean velocity obeys m˙v = −eE −mv/τ, where e > 0. I L A Schematic; labels, not drawing lengths, specify the data. (a) Derive the steady conductivity and mobility. (b) For n = 5.00 × 1028 m−3, m = 9.11 × 10−31 kg, τ = 2.00 × 10−14 s, and e = 1.60 × 10−19 C, evaluate both.
Show solutionHide solution
Question 1 - Solution Momentum relaxation sets the metallic dc conductivity I L A (a) Method and calculation ˙v = 0 ⇒vd = −eτE/m, J = −nevd. σ = ne2τ/m, µ = eτ/m . (b) Interpretation and further calculation σ = (5.00 × 1028)(1.60 × 10−19)2(2.00 × 10−14) 9.11 × 10−31 . σ = 2.81 × 107 S/m, µ = 3.51 × 10−3 m2/(V s) . Physical check Electron velocity opposes the field but conventional current follows it. The relaxation term transfers electronic momentum to the lattice and defects.

Question 1

Momentum relaxation sets the metallic dc conductivity

A one-band metal has electron density n, effective mass m, and relaxation time τ\tau. Its mean velocity obeys mv̇=−eE−mv/τm\dot v=-eE-mv/\tau, where e>0e>0.

Diagram shown in the original SVG worksheet.

  1. Derive the steady conductivity and mobility.

  2. For n=5.00×1028m−3n=5.00\times10^{28}\,\mathrm{m^{-3}}, m=9.11×10−31kgm=9.11\times10^{-31}\,\mathrm{kg}, τ=2.00×10−14s\tau=2.00\times10^{-14}\,\mathrm s, and e=1.60×10−19Ce=1.60\times10^{-19}\,\mathrm C, evaluate both.

Question 1 - Solution

Momentum relaxation sets the metallic dc conductivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

v̇=0⇒vd=−eτE/m,J=−nevd.\dot v=0\Rightarrow v_d=-e\tau E/m,\qquad J=-nev_d.σ=ne2τ/m,μ=eτ/m.\boxed{\sigma=ne^2\tau/m,\quad\mu=e\tau/m}.

(b) Interpretation and further calculation

σ=(5.00×1028)(1.60×10−19)2(2.00×10−14)9.11×10−31.\sigma=\frac{(5.00\times10^{28})(1.60\times10^{-19})^2(2.00\times10^{-14})}{9.11\times10^{-31}}.σ=2.81×107S/m,μ=3.51×10−3m2/(Vs).\boxed{\sigma=2.81\times10^7\,\mathrm{S/m},\quad\mu=3.51\times10^{-3}\,\mathrm{m^2/(V\,s)}}.

Physical check

Electron velocity opposes the field but conventional current follows it. The relaxation term transfers electronic momentum to the lattice and defects.