Applying Gauss' Law: Planar Symmetry — Question 1

Section 23-7 · Physics pages 3752–3753

Question 1 An isolated insulating sheet splits its flux equally between two sides An infinite nonconducting sheet in x = 0 carries uniform density σ > 0. There are no other sources. Choose a symmetric pillbox with each end face area A. σ Schematic; labels, not drawing lengths, specify the data. (a) Derive the field magnitude and direction on each side. (b) Compare this result with the field immediately outside a conductor surface having the same local density. Explain the factor of two by counting the nonzero pillbox faces.
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Question 1 - Solution An isolated insulating sheet splits its flux equally between two sides σ (a) Method and calculation Φ = EA + EA = 2EA, Qenc = σA. E(x) = σ 2ϵ0 sgn(x)ˆx (x̸ = 0). (b) Interpretation and further calculation Conductor: Emetal = 0, EvacuumA = σA/ϵ0. Evacuum = σ/ϵ0 = 2Eisolated sheet. The single-sheet result relies on reflection symmetry; the conductor boundary instead has zero field on its metal side. Physical check The factor of two is not a contradiction: the field on the second side differs in the two physical systems.

Question 1

An isolated insulating sheet splits its flux equally between two sides

An infinite nonconducting sheet in x=0x=0 carries uniform density σ>0\sigma>0. There are no other sources. Choose a symmetric pillbox with each end face area A.

Diagram shown in the original SVG worksheet.

  1. Derive the field magnitude and direction on each side.

  2. Compare this result with the field immediately outside a conductor surface having the same local density. Explain the factor of two by counting the nonzero pillbox faces.

Question 1 - Solution

An isolated insulating sheet splits its flux equally between two sides

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Φ=EA+EA=2EA,Qenc=σA.\Phi=EA+EA=2EA,\quad Q_{\mathrm{enc}}=\sigma A.𝑬(x)=σ2ϵ0sgn⁡(x)𝒙̂(x≠0).\mathbf E(x)=\frac\sigma{2\epsilon_0}\operatorname{sgn}(x)\hat{\mathbf x}\quad(x\ne0).

(b) Interpretation and further calculation

Conductor:Emetal=0,EvacuumA=σA/ϵ0.\text{Conductor:}\quad E_{\mathrm{metal}}=0,\quad E_{\mathrm{vacuum}}A=\sigma A/\epsilon_0.Evacuum=σ/ϵ0=2Eisolatedsheet.E_{\mathrm{vacuum}}=\sigma/\epsilon_0=2E_{\mathrm{isolated\ sheet}}.The single-sheet result relies on reflection symmetry; the conductor boundary instead has zero field on its metal side.

Physical check

The factor of two is not a contradiction: the field on the second side differs in the two physical systems.