Metals — Question 5

Section 41-4 · Physics pages 6860–6861

Question 5 Fermi motion determines the mean free path A metal has vF = 1.50 × 106 m/s and τ = 2.00 × 10−14 s. In a weak field its drift speed is only vd = 2.00 × 10−4 m/s. vd scattering path, speed ∼vF Schematic; labels, not drawing lengths, specify the data. (a) Find the mean free path and compare it with the drift displacement during one relaxation time. (b) For lattice spacing a = .300 nm, find the number of spacings in the mean free path and explain the distinct velocity scales.
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Question 5 - Solution Fermi motion determines the mean free path vd scattering path, speed ∼vF (a) Method and calculation ℓ= vF τ = 3.00 × 10−8 m = 30.0 nm . ∆xd = vdτ = 4.00 × 10−18 m, ℓ/∆xd = 7.50 × 109 . (b) Interpretation and further calculation ℓ/a = 30.0/.300 = 100 . ⟨v⟩= vd, |v| ∼vF ≫|⟨v⟩|. Physical check The large microscopic velocities nearly cancel in equilibrium. Current measures the small directional imbalance, whereas scattering paths involve the microscopic speed.

Question 5

Fermi motion determines the mean free path

A metal has vF=1.50×106m/sv_F=1.50\times10^6\,\mathrm{m/s} and τ=2.00×10−14s\tau=2.00\times10^{-14}\,\mathrm s. In a weak field its drift speed is only vd=2.00×10−4m/sv_d=2.00\times10^{-4}\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find the mean free path and compare it with the drift displacement during one relaxation time.

  2. For lattice spacing a=.300nma=.300\,\mathrm{nm}, find the number of spacings in the mean free path and explain the distinct velocity scales.

Question 5 - Solution

Fermi motion determines the mean free path

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ℓ=vFτ=3.00×10−8m=30.0nm.\boxed{\ell=v_F\tau=3.00\times10^{-8}\,\mathrm m=30.0\,\mathrm{nm}}.Δxd=vdτ=4.00×10−18m,ℓ/Δxd=7.50×109.\boxed{\Delta x_d=v_d\tau=4.00\times10^{-18}\,\mathrm m,\quad\ell/\Delta x_d=7.50\times10^9}.

(b) Interpretation and further calculation

ℓ/a=30.0/.300=100.\boxed{\ell/a=30.0/.300=100}.⟨𝒗⟩=𝒗d,|𝒗|∼vF≫|⟨𝒗⟩|.\langle\mathbf v\rangle=\mathbf v_d,\qquad |\mathbf v|\sim v_F\gg|\langle\mathbf v\rangle|.

Physical check

The large microscopic velocities nearly cancel in equilibrium. Current measures the small directional imbalance, whereas scattering paths involve the microscopic speed.