Applying Gauss' Law: Planar Symmetry — Question 2

Section 23-7 · Physics pages 3754–3755

Question 2 Unequal opposing sheets leave a residual exterior field Two infinite nonconducting sheets lie at x = 0 and x = d > 0, with fixed densities +σ and −2σ, respectively, where σ > 0. No external uniform field is added. x +σ −2σ 0 d Edge-on view of infinite planes; their lateral extent is not shown. (a) Use superposition to find Ex in all three regions. (b) Find the difference between the far-right and far-left fields and compare it with total sheet charge per area divided by ϵ0.
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Question 2 - Solution Unequal opposing sheets leave a residual exterior field x +σ −2σ 0 d (a) Method and calculation Ex = σ 2ϵ0 sgn(x) −2σ 2ϵ0 sgn(x −d). Ex =        σ/(2ϵ0), x < 0, 3σ/(2ϵ0), 0 < x < d, −σ/(2ϵ0), x > d. (b) Interpretation and further calculation Ex(+∞) −Ex(−∞) = −σ/ϵ0. Σ = σ −2σ = −σ ⇒∆Ex = Σ/ϵ0. The fields add in the gap; the unequal charges prevent cancellation in the exterior. Physical check Each field jump is fixed by its own sheet: +σ/ϵ0 at 0 and −2σ/ϵ0 at d.

Question 2

Unequal opposing sheets leave a residual exterior field

Two infinite nonconducting sheets lie at x=0x=0 and x=d>0x=d>0, with fixed densities +σ+\sigma and −2σ-2\sigma, respectively, where σ>0\sigma>0. No external uniform field is added.

Diagram shown in the original SVG worksheet.

  1. Use superposition to find ExE_x in all three regions.

  2. Find the difference between the far-right and far-left fields and compare it with total sheet charge per area divided by ϵ0\epsilon_0.

Question 2 - Solution

Unequal opposing sheets leave a residual exterior field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex=σ2ϵ0sgn⁡(x)−2σ2ϵ0sgn⁡(x−d).E_x=\frac\sigma{2\epsilon_0}\operatorname{sgn}(x)-\frac{2\sigma}{2\epsilon_0}\operatorname{sgn}(x-d).Ex={σ/(2ϵ0),x<0,3σ/(2ϵ0),0<x<d,−σ/(2ϵ0),x>d.E_x=\begin{cases}\sigma/(2\epsilon_0),&x<0,\\3\sigma/(2\epsilon_0),&0<x<d,\\-\sigma/(2\epsilon_0),&x>d.\end{cases}

(b) Interpretation and further calculation

Ex(+∞)−Ex(−∞)=−σ/ϵ0.E_x(+\infty)-E_x(-\infty)=-\sigma/\epsilon_0.Σ=σ−2σ=−σ⇒ΔEx=Σ/ϵ0.\Sigma=\sigma-2\sigma=-\sigma\Rightarrow\Delta E_x=\Sigma/\epsilon_0.The fields add in the gap; the unequal charges prevent cancellation in the exterior.

Physical check

Each field jump is fixed by its own sheet: +σ/ϵ0+\sigma/\epsilon_0 at 0 and −2σ/ϵ0-2\sigma/\epsilon_0 at d.