A Microscopic View of Ohm's Law — Question 6

Section 26-5 · Physics pages 4242–4243

Question 6 A sinusoidal field exposes the finite response time of drift The current satisfies τ dJ/dt + J = σ0E0 cos ωt. Consider only its long-time periodic response, with ω > 0. t solid: E; dashed: J Schematic; labels, not drawing lengths, specify the data. (a) Use J = A cos ωt + B sin ωt to solve for A and B. (b) Find the amplitude and phase lag, and the frequency at which the amplitude is reduced to 1/ √ 2 of its low-frequency value.
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Question 6 - Solution A sinusoidal field exposes the finite response time of drift t solid: E; dashed: J (a) Method and calculation A + ωτB = σ0E0, B −ωτA = 0. A = σ0E0 1 + (ωτ)2 , B = σ0E0ωτ 1 + (ωτ)2 . (b) Interpretation and further calculation J = σ0E0 √ 1 + (ωτ)2 cos(ωt −ϕ), ϕ = tan−1(ωτ). ωτ = 1 ⇒ω = 1/τ, ϕ = π/4. Physical check The algebra is a supplied relaxation equation, so no AC circuit theory is required.

Question 6

A sinusoidal field exposes the finite response time of drift

The current satisfies τdJ/dt+J=σ0E0cos⁡ωt\tau\,dJ/dt+J=\sigma_0E_0\cos\omega t. Consider only its long-time periodic response, with ω>0\omega>0.

Diagram shown in the original SVG worksheet.

  1. Use J=Acos⁡ωt+Bsin⁡ωtJ=A\cos\omega t+B\sin\omega t to solve for A and B.

  2. Find the amplitude and phase lag, and the frequency at which the amplitude is reduced to 1/21/\sqrt2 of its low-frequency value.

Question 6 - Solution

A sinusoidal field exposes the finite response time of drift

Diagram shown in the original SVG worksheet.

(a) Method and calculation

A+ωτB=σ0E0,B−ωτA=0.A+\omega\tau B=\sigma_0E_0,\quad B-\omega\tau A=0.A=σ0E01+(ωτ)2,B=σ0E0ωτ1+(ωτ)2.A=\frac{\sigma_0E_0}{1+(\omega\tau)^2},\quad B=\frac{\sigma_0E_0\omega\tau}{1+(\omega\tau)^2}.

(b) Interpretation and further calculation

J=σ0E01+(ωτ)2cos⁡(ωt−ϕ),ϕ=tan⁡−1(ωτ).J=\frac{\sigma_0E_0}{\sqrt{1+(\omega\tau)^2}}\cos(\omega t-\phi),\quad\phi=\tan^{-1}(\omega\tau).ωτ=1⇒ω=1/τ,ϕ=π/4.\omega\tau=1\Rightarrow\omega=1/\tau,\quad\phi=\pi/4.

Physical check

The algebra is a supplied relaxation equation, so no AC circuit theory is required.