Displacement Current — Question 4

Section 32-3 · Physics pages 5218–5219

Question 4 An RC charging current and gap displacement current decay together A vacuum capacitor C is charged from an ideal voltage V0 through resistance R, starting uncharged. Its voltage is VC = V0(1 −e−t/(RC)). E(t) d I Schematic; labels, not drawing lengths, specify the data. (a) Find the displacement current and total displacement charge integral. (b) Find the fraction of final capacitor charge accumulated by the time current has fallen to one-quarter its initial value.
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Question 4 - Solution An RC charging current and gap displacement current decay together E(t) d I (a) Method and calculation Id = C ˙VC = (V0/R)e−t/(RC). ∫∞ 0 Id dt = CV0 . (b) Interpretation and further calculation Id/Id(0) = 1/4 ⇒t = RC ln 4. Q(t)/(CV0) = 1 −e−ln 4 = 3/4 . Physical check The time integral of displacement current equals transferred plate charge, while the microscopic transport occurs in the leads.

Question 4

An RC charging current and gap displacement current decay together

A vacuum capacitor C is charged from an ideal voltage V0 through resistance R, starting uncharged. Its voltage is VC=V0(1−e−t/(RC))V_C=V_0(1-e^{-t/(RC)}).

Diagram shown in the original SVG worksheet.

  1. Find the displacement current and total displacement charge integral.

  2. Find the fraction of final capacitor charge accumulated by the time current has fallen to one-quarter its initial value.

Question 4 - Solution

An RC charging current and gap displacement current decay together

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Id=CV̇C=(V0/R)e−t/(RC).I_d=C\dot V_C=(V_0/R)e^{-t/(RC)}.∫0∞Iddt=CV0.\boxed{\int_0^\infty I_d\,dt=CV_0}.

(b) Interpretation and further calculation

Id/Id(0)=1/4⇒t=RCln⁡4.I_d/I_d(0)=1/4\Rightarrow t=RC\ln4.Q(t)/(CV0)=1−e−ln⁡4=3/4.\boxed{Q(t)/(CV_0)=1-e^{-\ln4}=3/4}.

Physical check

The time integral of displacement current equals transferred plate charge, while the microscopic transport occurs in the leads.