Work, Energy, and Emf — Question 9

Section 27-2 · Physics pages 4348–4349

Question 9 Constant-voltage and reversible capacitor charging demand different source work An initially uncharged capacitor C is charged to V0. Method A uses a constant ideal source V0 with a resistor. Method B raises the source voltage quasistatically to track the capacitor voltage, with arbitrarily small losses. + − Vs R C Circuit connections and marked polarities define the model; wire lengths are schematic. (a) Find source work, stored energy and loss for method A. (b) Integrate source work for method B and compare the two methods.
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Question 9 - Solution Constant-voltage and reversible capacitor charging demand different source work + − Vs R C (a) Method and calculation Qf = CV0, WA = V0Qf = CV 2 0 . Uf = 1 2CV 2 0 , Wloss,A = WA −Uf = 1 2CV 2 0 . (b) Interpretation and further calculation WB = ∫Qf 0 q C dq = Q2 f/(2C) = 1 2CV 2 0 . WB/WA = 1/2, Wloss,B →0. Physical check The work depends on the source voltage at each transferred charge, not just the final capacitor state.

Question 9

Constant-voltage and reversible capacitor charging demand different source work

An initially uncharged capacitor C is charged to V0. Method A uses a constant ideal source V0 with a resistor. Method B raises the source voltage quasistatically to track the capacitor voltage, with arbitrarily small losses.

Diagram shown in the original SVG worksheet.

  1. Find source work, stored energy and loss for method A.

  2. Integrate source work for method B and compare the two methods.

Question 9 - Solution

Constant-voltage and reversible capacitor charging demand different source work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qf=CV0,WA=V0Qf=CV02.Q_f=CV_0,\quad W_A=V_0Q_f=CV_0^2.Uf=12CV02,Wloss,A=WA−Uf=12CV02.U_f=\tfrac12CV_0^2,\quad W_{{\mathrm{loss}},A}=W_A-U_f=\tfrac12CV_0^2.

(b) Interpretation and further calculation

WB=∫0QfqCdq=Qf2/(2C)=12CV02.W_B=\int_0^{Q_f}\frac qC\,dq=Q_f^2/(2C)=\tfrac12CV_0^2.WB/WA=1/2,Wloss,B→0.W_B/W_A=1/2,\quad W_{{\mathrm{loss}},B}\to0.

Physical check

The work depends on the source voltage at each transferred charge, not just the final capacitor state.