Energy Stored in an Electric Field — Question 6

Section 25-4 · Physics pages 4082–4083

Question 6 The exterior energy of a charged sphere has a long radial tail An isolated conducting sphere of radius R carries charge Q in vacuum. Its exterior field is E = Q/(4πϵ0r2) and its interior field is zero. R Cross-section of concentric spherical surfaces; labels specify radii. (a) Integrate the field energy from R to infinity. (b) Find the fraction of energy outside radius nR, n>1, and the radius containing 90 percent of the field energy.
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Question 6 - Solution The exterior energy of a charged sphere has a long radial tail R (a) Method and calculation U = ∫∞ R ϵ0E2 2 4πr2dr = Q2 8πϵ0 ∫∞ R dr r2 . U = Q2 8πϵ0R. (b) Interpretation and further calculation Ur>nR/U = 1/n. UR<r<r90/U = 1 −R/r90 = .900 ⇒r90 = 10R. Physical check The energy density falls as inverse fourth power, but the growing spherical shell volume makes the energy tail fall only as inverse radius.

Question 6

The exterior energy of a charged sphere has a long radial tail

An isolated conducting sphere of radius R carries charge Q in vacuum. Its exterior field is E=Q/(4πϵ0r2)E=Q/(4\pi\epsilon_0r^2) and its interior field is zero.

Diagram shown in the original SVG worksheet.

  1. Integrate the field energy from R to infinity.

  2. Find the fraction of energy outside radius nR, n>1, and the radius containing 90 percent of the field energy.

Question 6 - Solution

The exterior energy of a charged sphere has a long radial tail

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=∫R∞ϵ0E224πr2dr=Q28πϵ0∫R∞drr2.U=\int_R^\infty\frac{\epsilon_0E^2}{2}4\pi r^2dr=\frac{Q^2}{8\pi\epsilon_0}\int_R^\infty\frac{dr}{r^2}.U=Q28πϵ0R.U=\frac{Q^2}{8\pi\epsilon_0R}.

(b) Interpretation and further calculation

Ur>nR/U=1/n.U_{r>nR}/U=1/n.UR<r<r90/U=1−R/r90=.900⇒r90=10R.U_{R<r<r_{90}}/U=1-R/r_{90}=.900\Rightarrow r_{90}=10R.

Physical check

The energy density falls as inverse fourth power, but the growing spherical shell volume makes the energy tail fall only as inverse radius.