Insulators — Question 5

Section 41-3 · Physics pages 6840–6841

Question 5 Conduction loss and displacement current have different frequency dependence A dielectric slab has Jc = σE and Jd = ε dE/dt. Apply E = E0 cos ωt. Define loss tangent as the amplitude ratio tan δ = |Jc|/|Jd|. t J solid: Jc; dashed: Jd Schematic; labels, not drawing lengths, specify the data. (a) Derive the loss tangent and mean heating per volume. (b) Find the angular frequency where both current amplitudes are equal for σ = 10−6 S/m and ε = 5.00 × 10−11 F/m.
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Question 5 - Solution Conduction loss and displacement current have different frequency dependence t J solid: Jc; dashed: Jd (a) Method and calculation Jc = σE0 cos ωt, Jd = −ωεE0 sin ωt. tan δ = σ/(ωε), ⟨pv⟩= σE2 0/2 . (b) Interpretation and further calculation tan δ = 1 ⇒ω = σ/ε. ω = 2.00 × 104 s−1, f = ω/(2π) = 3.183 kHz . Physical check The displacement current is in quadrature with the field and contributes no mean Joule heating in this ideal model. Polarization relaxation can add loss beyond the stated conductivity term.

Question 5

Conduction loss and displacement current have different frequency dependence

A dielectric slab has Jc=σEJ_c=\sigma E and Jd=εdE/dtJ_d=\varepsilon\,dE/dt. Apply E=E0cos⁡ωtE=E_0\cos\omega t. Define loss tangent as the amplitude ratio tan⁡δ=|Jc|/|Jd|\tan\delta=|J_c|/|J_d|.

Diagram shown in the original SVG worksheet.

  1. Derive the loss tangent and mean heating per volume.

  2. Find the angular frequency where both current amplitudes are equal for σ=10−6S/m\sigma=10^{-6}\,\mathrm{S/m} and ε=5.00×10−11F/m\varepsilon=5.00\times10^{-11}\,\mathrm{F/m}.

Question 5 - Solution

Conduction loss and displacement current have different frequency dependence

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Jc=σE0cos⁡ωt,Jd=−ωεE0sin⁡ωt.J_c=\sigma E_0\cos\omega t,\quad J_d=-\omega\varepsilon E_0\sin\omega t.tan⁡δ=σ/(ωε),⟨pv⟩=σE02/2.\boxed{\tan\delta=\sigma/(\omega\varepsilon),\quad\langle p_v\rangle=\sigma E_0^2/2}.

(b) Interpretation and further calculation

tan⁡δ=1⇒ω=σ/ε.\tan\delta=1\Rightarrow\omega=\sigma/\varepsilon.ω=2.00×104s−1,f=ω/(2π)=3.183kHz.\boxed{\omega=2.00\times10^4\,\mathrm{s^{-1}},\quad f=\omega/(2\pi)=3.183\,\mathrm{kHz}}.

Physical check

The displacement current is in quadrature with the field and contributes no mean Joule heating in this ideal model. Polarization relaxation can add loss beyond the stated conductivity term.