Energy Stored in an Electric Field — Question 5

Section 25-4 · Physics pages 4080–4081

Question 5 Integrating coaxial field energy reproduces the terminal formula A long vacuum coaxial capacitor has radii a,b and length L, with opposite line charges ±λ. Use E(r) = λ/(2πϵ0r) and energy density u = ϵ0E2/2. a b Schematic; labels, not drawing lengths, specify the data. (a) Integrate the energy throughout the gap. (b) Express the result as Q squared over 2C and find what fraction lies between a and √ ab.
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Question 5 - Solution Integrating coaxial field energy reproduces the terminal formula a b (a) Method and calculation U = ∫b a ϵ0E2 2 (2πrL)dr = λ2L 4πϵ0 ∫b a dr r . U = λ2L 4πϵ0 ln(b/a). (b) Interpretation and further calculation Q = λL, C = 2πϵ0L ln(b/a) ⇒U = Q2/(2C). U(a < r < √ ab) U = ln( √ ab/a) ln(b/a) = 1 2. Physical check Equal logarithmic radial intervals contain equal energy in this geometry, despite their unequal physical volumes.

Question 5

Integrating coaxial field energy reproduces the terminal formula

A long vacuum coaxial capacitor has radii a,b and length L, with opposite line charges ±λ\pm\lambda. Use E(r)=λ/(2πϵ0r)E(r)=\lambda/(2\pi\epsilon_0r) and energy density u=ϵ0E2/2u=\epsilon_0E^2/2.

Diagram shown in the original SVG worksheet.

  1. Integrate the energy throughout the gap.

  2. Express the result as Q squared over 2C and find what fraction lies between a and ab\sqrt{ab}.

Question 5 - Solution

Integrating coaxial field energy reproduces the terminal formula

Diagram shown in the original SVG worksheet.

(a) Method and calculation

U=∫abϵ0E22(2πrL)dr=λ2L4πϵ0∫abdrr.U=\int_a^b\frac{\epsilon_0E^2}{2}(2\pi rL)dr=\frac{\lambda^2L}{4\pi\epsilon_0}\int_a^b\frac{dr}{r}.U=λ2L4πϵ0ln⁡(b/a).U=\frac{\lambda^2L}{4\pi\epsilon_0}\ln(b/a).

(b) Interpretation and further calculation

Q=λL,C=2πϵ0Lln⁡(b/a)⇒U=Q2/(2C).Q=\lambda L,\quad C=\frac{2\pi\epsilon_0L}{\ln(b/a)}\Rightarrow U=Q^2/(2C).U(a<r<ab)U=ln⁡(ab/a)ln⁡(b/a)=12.\frac{U(a<r<\sqrt{ab})}{U}=\frac{\ln(\sqrt{ab}/a)}{\ln(b/a)}=\frac12.

Physical check

Equal logarithmic radial intervals contain equal energy in this geometry, despite their unequal physical volumes.