Displacement Current — Question 10

Section 32-3 · Physics pages 5230–5231

Question 10 Changing capacitor spacing adds a geometric term to displacement current A vacuum parallel-plate capacitor has fixed area A but slowly varying gap d(t) and voltage V(t). Neglect fringe fields and use instantaneous uniform E = V/d. E(t) d I Schematic; labels, not drawing lengths, specify the data. (a) Find plate charging current and gap displacement current. (b) For constant plate charge Q, find the required voltage law and the displacement current despite moving plates.
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Question 10 - Solution Changing capacitor spacing adds a geometric term to displacement current E(t) d I (a) Method and calculation Q = ϵ0AV/d ⇒I = ˙Q = ϵ0A ( ˙V d −V ˙d d2 ) . Id = ϵ0A ˙E = I . (b) Interpretation and further calculation Q fixed : V = Qd/(ϵ0A), E = Q/(ϵ0A). ˙V /V = ˙d/d, Id = 0 . Physical check A changing voltage alone does not guarantee changing electric field when the geometry also changes.

Question 10

Changing capacitor spacing adds a geometric term to displacement current

A vacuum parallel-plate capacitor has fixed area A but slowly varying gap d(t) and voltage V(t). Neglect fringe fields and use instantaneous uniform E=V/dE=V/d.

Diagram shown in the original SVG worksheet.

  1. Find plate charging current and gap displacement current.

  2. For constant plate charge Q, find the required voltage law and the displacement current despite moving plates.

Question 10 - Solution

Changing capacitor spacing adds a geometric term to displacement current

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q=ϵ0AV/d⇒I=Q̇=ϵ0A(V̇d−Vḋd2).Q=\epsilon_0AV/d\Rightarrow I=\dot Q=\epsilon_0A\left(\frac{\dot V}{d}-\frac{V\dot d}{d^2}\right).Id=ϵ0AĖ=I.\boxed{I_d=\epsilon_0A\dot E=I}.

(b) Interpretation and further calculation

Qfixed:V=Qd/(ϵ0A),E=Q/(ϵ0A).Q\ \text{fixed}:\quad V=Qd/(\epsilon_0A),\quad E=Q/(\epsilon_0A).V̇/V=ḋ/d,Id=0.\boxed{\dot V/V=\dot d/d,\quad I_d=0}.

Physical check

A changing voltage alone does not guarantee changing electric field when the geometry also changes.