Conductors and Insulators — Question 10

Section 21-2 · Physics pages 3410–3411

Question 10 A surface density model distinguishes redistribution from net charging A spherical conductor of radius R has a supplied equilibrium surface-charge model σ(θ) = σ0 + σ1 cos θ, produced by a net charge and an external influence. The angle θ is measured from the north axis. Use dA = 2πR2 sin θ dθ, σ0 = 2.0 nC/m2, σ1 = 6.0 nC/m2, and R = .50 m. north θ + − Schematic; labels, not drawing lengths, specify the data. (a) Integrate to find the total surface charge and show why the cos θ term contributes no net charge. (b) Find the northern and southern hemisphere charges. Determine whether opposite signs on the two hemispheres are compatible with a positive total charge.
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Question 10 - Solution A surface density model distinguishes redistribution from net charging north θ + − (a) Method and calculation Q = 2πR2 ∫π 0 (σ0 + σ1 cos θ) sin θ dθ = 4πR2σ0. ∫π 0 cos θ sin θ dθ = 0, Q = 2π nC. (b) Interpretation and further calculation QN = 2πR2(σ0 + σ1/2) = 2.5π nC. QS = 2πR2(σ0 −σ1/2) = −.5π nC, QN + QS = 2π nC. The antisymmetric term moves charge between hemispheres without changing the total. Physical check The prescribed density requires an external influence; an isolated spherical conductor without one has a uniform equilibrium density.

Question 10

A surface density model distinguishes redistribution from net charging

A spherical conductor of radius RR has a supplied equilibrium surface-charge model σ(θ)=σ0+σ1cos⁡θ\sigma(\theta)=\sigma_0+\sigma_1\cos\theta, produced by a net charge and an external influence. The angle θ\theta is measured from the north axis. Use dA=2πR2sin⁡θdθdA=2\pi R^2\sin\theta\,d\theta, σ0=2.0\sigma_0=2.0 nC/m2^2, σ1=6.0\sigma_1=6.0 nC/m2^2, and R=.50R=.50 m.

Diagram shown in the original SVG worksheet.

  1. Integrate to find the total surface charge and show why the cos⁡θ\cos\theta term contributes no net charge.

  2. Find the northern and southern hemisphere charges. Determine whether opposite signs on the two hemispheres are compatible with a positive total charge.

Question 10 - Solution

A surface density model distinguishes redistribution from net charging

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q=2πR2∫0π(σ0+σ1cos⁡θ)sin⁡θdθ=4πR2σ0.Q=2\pi R^2\int_0^\pi(\sigma_0+\sigma_1\cos\theta)\sin\theta\,d\theta=4\pi R^2\sigma_0.∫0πcos⁡θsin⁡θdθ=0,Q=2πnC.\int_0^\pi\cos\theta\sin\theta\,d\theta=0,\quad Q=2\pi\,\mathrm{nC}.

(b) Interpretation and further calculation

QN=2πR2(σ0+σ1/2)=2.5πnC.Q_N=2\pi R^2(\sigma_0+\sigma_1/2)=2.5\pi\,\mathrm{nC}.QS=2πR2(σ0−σ1/2)=−.5πnC,QN+QS=2πnC.Q_S=2\pi R^2(\sigma_0-\sigma_1/2)=-.5\pi\,\mathrm{nC},\quad Q_N+Q_S=2\pi\,\mathrm{nC}.The antisymmetric term moves charge between hemispheres without changing the total.

Physical check

The prescribed density requires an external influence; an isolated spherical conductor without one has a uniform equilibrium density.