Displacement Current — Question 1

Section 32-3 · Physics pages 5212–5213

Question 1 A capacitor gap carries the same generalized current as its charging wire A parallel-plate vacuum capacitor has fixed area A and gap d, with negligible fringing. Its plate charge is Q(t). Define Id = ϵ0 dΦE/dt. E(t) d I Schematic; labels, not drawing lengths, specify the data. (a) Prove that gap displacement current equals the charging-wire current. (b) For C=30.0 pF and voltage rising at 2.00 × 108 V/s, find both currents.
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Question 1 - Solution A capacitor gap carries the same generalized current as its charging wire E(t) d I (a) Method and calculation E = Q/(ϵ0A), ΦE = EA = Q/ϵ0. Id = ϵ0 ˙ΦE = ˙Q = Iwire . (b) Interpretation and further calculation Q = CV ⇒I = C ˙V = (30.0 × 10−12)(2.00 × 108). Id = Iwire = 6.00 mA . Physical check The equality concerns magnetic circulation; it does not mean free charges cross the vacuum gap.

Question 1

A capacitor gap carries the same generalized current as its charging wire

A parallel-plate vacuum capacitor has fixed area A and gap d, with negligible fringing. Its plate charge is Q(t). Define Id=ϵ0dΦE/dtI_d=\epsilon_0\,d\Phi_E/dt.

Diagram shown in the original SVG worksheet.

  1. Prove that gap displacement current equals the charging-wire current.

  2. For C=30.0 pF and voltage rising at 2.00×1082.00\times10^8 V/s, find both currents.

Question 1 - Solution

A capacitor gap carries the same generalized current as its charging wire

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E=Q/(ϵ0A),ΦE=EA=Q/ϵ0.E=Q/(\epsilon_0A),\quad\Phi_E=EA=Q/\epsilon_0.Id=ϵ0Φ̇E=Q̇=Iwire.\boxed{I_d=\epsilon_0\dot\Phi_E=\dot Q=I_{\mathrm{wire}}}.

(b) Interpretation and further calculation

Q=CV⇒I=CV̇=(30.0×10−12)(2.00×108).Q=CV\Rightarrow I=C\dot V=(30.0\times10^{-12})(2.00\times10^8).Id=Iwire=6.00mA.\boxed{I_d=I_{\mathrm{wire}}=6.00\,mA}.

Physical check

The equality concerns magnetic circulation; it does not mean free charges cross the vacuum gap.