Insulators — Question 10

Section 41-3 · Physics pages 6850–6851

Question 10 A displacement pulse distinguishes polarization charging from steady leakage A dielectric of area A and thickness d is driven by a linear voltage ramp V (t) = V0t/tr for 0 < t < tr, then held at V0. Use I = A[σE + ε ˙E] and E = V/d. t I tr Schematic; labels, not drawing lengths, specify the data. (a) Derive current during the ramp and immediately after it. (b) Find the integrated displacement charge and compare it with the final capacitor charge.
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Question 10 - Solution A displacement pulse distinguishes polarization charging from steady leakage t I tr (a) Method and calculation 0 < t < tr : I(t) = AV0 d (σt/tr + ε/tr) . t > tr : I = σAV0/d . (b) Interpretation and further calculation Qd = ∫tr 0 εAV0 dtr dt = εAV0/d. C = εA/d ⇒Qd = CV0 . Physical check The displacement charge is independent of ramp duration. The additional conduction charge grows with time and is not stored as ideal capacitor charge.

Question 10

A displacement pulse distinguishes polarization charging from steady leakage

A dielectric of area A and thickness d is driven by a linear voltage ramp V(t)=V0t/trV(t)=V_0t/t_r for 0<t<tr0<t<t_r, then held at V0V_0. Use I=A[σE+εĖ]I=A[\sigma E+\varepsilon\dot E] and E=V/dE=V/d.

Diagram shown in the original SVG worksheet.

  1. Derive current during the ramp and immediately after it.

  2. Find the integrated displacement charge and compare it with the final capacitor charge.

Question 10 - Solution

A displacement pulse distinguishes polarization charging from steady leakage

Diagram shown in the original SVG worksheet.

(a) Method and calculation

0<t<tr:I(t)=AV0d(σt/tr+ε/tr).0<t<t_r:\quad\boxed{I(t)=\frac{A V_0}{d}\left(\sigma t/t_r+\varepsilon/t_r\right)}.t>tr:I=σAV0/d.t>t_r:\quad\boxed{I=\sigma A V_0/d}.

(b) Interpretation and further calculation

Qd=∫0trεAV0dtrdt=εAV0/d.Q_d=\int_0^{t_r}\frac{\varepsilon A V_0}{dt_r}\,dt=\varepsilon A V_0/d.C=εA/d⇒Qd=CV0.C=\varepsilon A/d\Rightarrow\boxed{Q_d=CV_0}.

Physical check

The displacement charge is independent of ramp duration. The additional conduction charge grows with time and is not stored as ideal capacitor charge.