Gauss' Law — Question 8

Section 23-3 · Physics pages 3686–3687

Question 8 Deforming a Gaussian surface changes flux only by swept charge A closed surface is expanded into a second surface without losing any previously enclosed region. The added region has volume ∆V and uniform volume charge density ρ. Arbitrary fixed charges may also lie inside the original surface and outside the final one. ρ Schematic; labels, not drawing lengths, specify the data. (a) Derive the change in outward flux and evaluate its sign for negative ρ. (b) Now form the boundary of just the added region, including the original inner surface. Explain the orientation of that inner boundary and recover the same flux difference.
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Question 8 - Solution Deforming a Gaussian surface changes flux only by swept charge ρ (a) Method and calculation Q2 = Q1 + ρ∆V, Φi = Qi/ϵ0. ∆Φ = Φ2 −Φ1 = ρ∆V/ϵ0 < 0 (ρ < 0). (b) Interpretation and further calculation ˆninner,layer = −ˆn1, Φlayer = Φ2 −Φ1. Φlayer = Qlayer/ϵ0 = ρ∆V/ϵ0. The inner boundary normal points into the removed central volume, outward from the layer itself. Physical check Surface shape is irrelevant to the difference once the added charge is specified; no field symmetry is required.

Question 8

Deforming a Gaussian surface changes flux only by swept charge

A closed surface is expanded into a second surface without losing any previously enclosed region. The added region has volume ΔV\Delta V and uniform volume charge density ρ\rho. Arbitrary fixed charges may also lie inside the original surface and outside the final one.

Diagram shown in the original SVG worksheet.

  1. Derive the change in outward flux and evaluate its sign for negative ρ\rho.

  2. Now form the boundary of just the added region, including the original inner surface. Explain the orientation of that inner boundary and recover the same flux difference.

Question 8 - Solution

Deforming a Gaussian surface changes flux only by swept charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q2=Q1+ρΔV,Φi=Qi/ϵ0.Q_2=Q_1+\rho\Delta V,\quad\Phi_i=Q_i/\epsilon_0.ΔΦ=Φ2−Φ1=ρΔV/ϵ0<0(ρ<0).\Delta\Phi=\Phi_2-\Phi_1=\rho\Delta V/\epsilon_0<0\quad(\rho<0).

(b) Interpretation and further calculation

𝒏̂inner,layer=−𝒏̂1,Φlayer=Φ2−Φ1.\hat{\mathbf n}_{\mathrm{inner,layer}}=-\hat{\mathbf n}_{1},\quad\Phi_{\mathrm{layer}}=\Phi_2-\Phi_1.Φlayer=Qlayer/ϵ0=ρΔV/ϵ0.\Phi_{\mathrm{layer}}=Q_{\mathrm{layer}}/\epsilon_0=\rho\Delta V/\epsilon_0.The inner boundary normal points into the removed central volume, outward from the layer itself.

Physical check

Surface shape is irrelevant to the difference once the added charge is specified; no field symmetry is required.