A Charged Isolated Conductor — Question 4

Section 23-5 · Physics pages 3718–3719

Question 4 A centered cavity source produces three distinct radial field regions A spherical conducting shell has inner radius a and outer radius b. A point charge q is fixed at the common center, and the shell has net charge Qc. There are no external sources; the system is in electrostatic equilibrium. q a b Cross-section of a conducting shell in electrostatic equilibrium; shaded material is metal. (a) Find the field for 0 < r < a, a < r < b and r > b. (b) Find both surface densities and verify the field jump at each interface using normals directed from metal into vacuum.
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Question 4 - Solution A centered cavity source produces three distinct radial field regions q a b (a) Method and calculation Er(r) = q 4πϵ0r2 (0 < r < a), Er = 0 (a < r < b). Er(r) = q + Qc 4πϵ0r2 (r > b). (b) Interpretation and further calculation σa = − q 4πa2 , σb = q + Qc 4πb2 . En,a = E(a−) · (−ˆr) = σa/ϵ0, En,b = Er(b+) = σb/ϵ0. At the cavity wall, the outward normal from the metal points inward toward the center. Physical check The cavity contains a source, so zero field in the metal does not imply zero field in the cavity.

Question 4

A centered cavity source produces three distinct radial field regions

A spherical conducting shell has inner radius a and outer radius b. A point charge q is fixed at the common center, and the shell has net charge QcQ_c. There are no external sources; the system is in electrostatic equilibrium.

Diagram shown in the original SVG worksheet.

  1. Find the field for 0<r<a0<r<a, a<r<ba<r<b and r>br>b.

  2. Find both surface densities and verify the field jump at each interface using normals directed from metal into vacuum.

Question 4 - Solution

A centered cavity source produces three distinct radial field regions

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Er(r)=q4πϵ0r2(0<r<a),Er=0(a<r<b).E_r(r)=\frac{q}{4\pi\epsilon_0r^2}\quad(0<r<a),\qquad E_r=0\quad(a<r<b).Er(r)=q+Qc4πϵ0r2(r>b).E_r(r)=\frac{q+Q_c}{4\pi\epsilon_0r^2}\quad(r>b).

(b) Interpretation and further calculation

σa=−q4πa2,σb=q+Qc4πb2.\sigma_a=-\frac{q}{4\pi a^2},\quad\sigma_b=\frac{q+Q_c}{4\pi b^2}.En,a=𝑬(a−)⋅(−𝒓̂)=σa/ϵ0,En,b=Er(b+)=σb/ϵ0.E_{n,a}=\mathbf E(a^-)\cdot(-\hat{\mathbf r})=\sigma_a/\epsilon_0,\quad E_{n,b}=E_r(b^+)=\sigma_b/\epsilon_0.At the cavity wall, the outward normal from the metal points inward toward the center.

Physical check

The cavity contains a source, so zero field in the metal does not imply zero field in the cavity.