Energy Stored in an Electric Field — Question 1

Section 25-4 · Physics pages 4072–4073

Question 1 Integrating the charging voltage avoids double-counting stored energy An initially uncharged linear capacitor C=8.00 nF is charged quasistatically to 50.0 V. V qA Axes and labels specify the model; the sketch is schematic. (a) Derive its stored energy by integrating the incremental work. (b) Find its final charge and compare the stored energy with Q times the final voltage.
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Question 1 - Solution Integrating the charging voltage avoids double-counting stored energy V qA (a) Method and calculation dU = v(q) dq = q C dq, U = ∫Q 0 q C dq = Q2 2C = 1 2CV 2. U = 1 2(8.00 × 10−9)(50.0)2 = 10.0 µJ. (b) Interpretation and further calculation Q = CV = 400 nC. QV = 20.0 µJ = 2U, v = V/2. Physical check The instantaneous charging voltage rises from zero; using the final voltage for every charge increment overestimates the work.

Question 1

Integrating the charging voltage avoids double-counting stored energy

An initially uncharged linear capacitor C=8.00 nF is charged quasistatically to 50.0 V.

Diagram shown in the original SVG worksheet.

  1. Derive its stored energy by integrating the incremental work.

  2. Find its final charge and compare the stored energy with Q times the final voltage.

Question 1 - Solution

Integrating the charging voltage avoids double-counting stored energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dU=v(q)dq=qCdq,U=∫0QqCdq=Q22C=12CV2.dU=v(q)\,dq=\frac qC\,dq,\quad U=\int_0^Q\frac qC\,dq=\frac{Q^2}{2C}=\frac12CV^2.U=12(8.00×10−9)(50.0)2=10.0μJ.U=\tfrac12(8.00\times10^{-9})(50.0)^2=10.0\,\mu\mathrm J.

(b) Interpretation and further calculation

Q=CV=400nC.Q=CV=400\,\mathrm{nC}.QV=20.0μJ=2U,v¯=V/2.QV=20.0\,\mu\mathrm J=2U,\quad\overline v=V/2.

Physical check

The instantaneous charging voltage rises from zero; using the final voltage for every charge increment overestimates the work.