Applying Gauss' Law: Planar Symmetry — Question 8

Section 23-7 · Physics pages 3766–3767

Question 8 Forces between charged sheets use only the field of the other sheet Two infinite thin insulating sheets with fixed densities σ1 and σ2 lie at x = 0 and x = d > 0. Ignore their mechanical supports. To compute force on a sheet, exclude its own field. x σ1 σ2 Opposite-sign case in part (b): arrows show attraction between the two infinite sheets. (a) Derive the signed force per area on each sheet and check their sum. (b) For σ1 = σ and σ2 = −2σ, find the attraction pressure. Explain why multiplying the second sheet density by the total gap field gives an incorrect result.
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Question 8 - Solution Forces between charged sheets use only the field of the other sheet x σ1 σ2 (a) Method and calculation E1→2 = σ1/(2ϵ0), E2→1 = −σ2/(2ϵ0). f2x = σ1σ2 2ϵ0 , f1x = −σ1σ2 2ϵ0 , f1x + f2x = 0. (b) Interpretation and further calculation σ1 = σ, σ2 = −2σ : f2x = −σ2/ϵ0, P = σ2/ϵ0. σ2Egap = (−2σ) 3σ 2ϵ0 = −3σ2/ϵ0̸ = f2x. The gap field includes the second sheet self-field, which must not be used as an external force on that same sheet. Physical check The force magnitude is independent of d in the ideal infinite-plane approximation; opposite signs attract.

Question 8

Forces between charged sheets use only the field of the other sheet

Two infinite thin insulating sheets with fixed densities σ1\sigma_1 and σ2\sigma_2 lie at x=0x=0 and x=d>0x=d>0. Ignore their mechanical supports. To compute force on a sheet, exclude its own field.

Diagram shown in the original SVG worksheet.

  1. Derive the signed force per area on each sheet and check their sum.

  2. For σ1=σ\sigma_1=\sigma and σ2=−2σ\sigma_2=-2\sigma, find the attraction pressure. Explain why multiplying the second sheet density by the total gap field gives an incorrect result.

Question 8 - Solution

Forces between charged sheets use only the field of the other sheet

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E1→2=σ1/(2ϵ0),E2→1=−σ2/(2ϵ0).E_{1\to2}=\sigma_1/(2\epsilon_0),\quad E_{2\to1}=-\sigma_2/(2\epsilon_0).f2x=σ1σ22ϵ0,f1x=−σ1σ22ϵ0,f1x+f2x=0.f_{2x}=\frac{\sigma_1\sigma_2}{2\epsilon_0},\quad f_{1x}=-\frac{\sigma_1\sigma_2}{2\epsilon_0},\quad f_{1x}+f_{2x}=0.

(b) Interpretation and further calculation

σ1=σ,σ2=−2σ:f2x=−σ2/ϵ0,P=σ2/ϵ0.\sigma_1=\sigma,\ \sigma_2=-2\sigma:\quad f_{2x}=-\sigma^2/\epsilon_0,\quad P=\sigma^2/\epsilon_0.σ2Egap=(−2σ)3σ2ϵ0=−3σ2/ϵ0≠f2x.\sigma_2E_{\mathrm{gap}}=(-2\sigma)\frac{3\sigma}{2\epsilon_0}=-3\sigma^2/\epsilon_0\ne f_{2x}.The gap field includes the second sheet self-field, which must not be used as an external force on that same sheet.

Physical check

The force magnitude is independent of d in the ideal infinite-plane approximation; opposite signs attract.