Gauss' Law and Coulomb's Law — Question 9

Section 23-4 · Physics pages 3708–3709

Question 9 Coulomb superposition yields the enclosed-charge sum for an arbitrary surface Point charges qi lie away from a closed oriented surface S. Let Ωi = H S ˆri · ˆn dA/r2 i be its signed solid angle seen from source i. Use Ωi = 4π for an interior source and zero for an exterior source. +2q −q +7q Schematic; labels, not drawing lengths, specify the data. (a) Apply linear superposition to derive Gauss law from the Coulomb fields of all sources. (b) For interior charges +2q and −q plus exterior charge +7q, find the flux. Explain why moving the exterior charge can alter surface field values without changing this result.
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Question 9 - Solution Coulomb superposition yields the enclosed-charge sum for an arbitrary surface +2q −q +7q (a) Method and calculation E = X i qi 4πϵ0r2 i ˆri, Φ = X i qiΩi 4πϵ0 . Φ = 1 ϵ0 X i inside qi. (b) Interpretation and further calculation Φ = 2q −q ϵ0 + 7q 4πϵ0 (0) = q/ϵ0. Ωoutside = 0 while the source remains outside. Its local Coulomb contributions change under displacement, but their signed integral stays zero. Physical check Closed-surface flux adds linearly because both Coulomb superposition and the surface integral are linear.

Question 9

Coulomb superposition yields the enclosed-charge sum for an arbitrary surface

Point charges qiq_i lie away from a closed oriented surface S. Let Ωi=∮S𝒓̂i⋅𝒏̂dA/ri2\Omega_i=\oint_S\hat{\mathbf r}_i\cdot\hat{\mathbf n}\,dA/r_i^2 be its signed solid angle seen from source i. Use Ωi=4π\Omega_i=4\pi for an interior source and zero for an exterior source.

Diagram shown in the original SVG worksheet.

  1. Apply linear superposition to derive Gauss law from the Coulomb fields of all sources.

  2. For interior charges +2q+2q and −q-q plus exterior charge +7q+7q, find the flux. Explain why moving the exterior charge can alter surface field values without changing this result.

Question 9 - Solution

Coulomb superposition yields the enclosed-charge sum for an arbitrary surface

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬=∑iqi4πϵ0ri2𝒓̂i,Φ=∑iqiΩi4πϵ0.\mathbf E=\sum_i\frac{q_i}{4\pi\epsilon_0r_i^2}\hat{\mathbf r}_i,\quad\Phi=\sum_i\frac{q_i\Omega_i}{4\pi\epsilon_0}.Φ=1ϵ0∑iinsideqi.\Phi=\frac1{\epsilon_0}\sum_{i\ {\mathrm{inside}}}q_i.

(b) Interpretation and further calculation

Φ=2q−qϵ0+7q4πϵ0(0)=q/ϵ0.\Phi=\frac{2q-q}{\epsilon_0}+\frac{7q}{4\pi\epsilon_0}(0)=q/\epsilon_0.Ωoutside=0while the source remains outside.\Omega_{\mathrm{outside}}=0\quad\text{while the source remains outside}.Its local Coulomb contributions change under displacement, but their signed integral stays zero.

Physical check

Closed-surface flux adds linearly because both Coulomb superposition and the surface integral are linear.