Energy Stored in an Electric Field — Question 7

Section 25-4 · Physics pages 4084–4085

Question 7 A nonlinear capacitor stores the integral of voltage against charge A reversible device obeys q(v) = C0v + βv3 for v nonnegative, with positive C0 and beta. It begins at q=v=0. V qA Axes and labels specify the model; the sketch is schematic. (a) Derive its stored energy at voltage V. (b) Compare with one half qV and find the ratio when βV 2 = C0.
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Question 7 - Solution A nonlinear capacitor stores the integral of voltage against charge V qA (a) Method and calculation dq = (C0 + 3βv2)dv, U = ∫V 0 v dq dvdv. U = 1 2C0V 2 + 3 4βV 4. (b) Interpretation and further calculation 1 2qV = 1 2C0V 2 + 1 2βV 4, U −1 2qV = 1 4βV 4. βV 2 = C0 : U/(qV/2) = 5/4. Physical check The familiar half-qV formula requires a linear charge-voltage law; the differential charging integral is the general relation here.

Question 7

A nonlinear capacitor stores the integral of voltage against charge

A reversible device obeys q(v)=C0v+βv3q(v)=C_0v+\beta v^3 for v nonnegative, with positive C0 and beta. It begins at q=v=0.

Diagram shown in the original SVG worksheet.

  1. Derive its stored energy at voltage V.

  2. Compare with one half qV and find the ratio when βV2=C0\beta V^2=C_0.

Question 7 - Solution

A nonlinear capacitor stores the integral of voltage against charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dq=(C0+3βv2)dv,U=∫0Vvdqdvdv.dq=(C_0+3\beta v^2)dv,\quad U=\int_0^Vv\frac{dq}{dv}dv.U=12C0V2+34βV4.U=\frac12C_0V^2+\frac34\beta V^4.

(b) Interpretation and further calculation

12qV=12C0V2+12βV4,U−12qV=14βV4.\tfrac12qV=\frac12C_0V^2+\frac12\beta V^4,\quad U-\tfrac12qV=\frac14\beta V^4.βV2=C0:U/(qV/2)=5/4.\beta V^2=C_0:\quad U/(qV/2)=5/4.

Physical check

The familiar half-qV formula requires a linear charge-voltage law; the differential charging integral is the general relation here.