Applying Gauss' Law: Planar Symmetry — Question 7

Section 23-7 · Physics pages 3764–3765

Question 7 A neutral metal insert changes gap width while leaving fixed-sheet field unchanged Infinite insulating sheets at x = 0 and x = d carry fixed +σ and −σ, with σ > 0. A neutral conducting slab of thickness t is centered between them, with 0 < t < d. Assume equilibrium and zero exterior field. +σ −σ metal t Schematic; labels, not drawing lengths, specify the data. (a) Find the field in each vacuum gap and the induced density on each metal face. (b) A weak positive charge q starts from rest just to the right of the left sheet and travels across the left vacuum gap. Find its kinetic-energy gain immediately before reaching the metal, neglecting image-force disturbance.
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Question 7 - Solution A neutral metal insert changes gap width while leaving fixed-sheet field unchanged +σ −σ metal t (a) Method and calculation Egap = σ/ϵ0, Emetal = 0. σmetal,left = ϵ0(0 −Egap) = −σ, σmetal,right = +σ. (b) Interpretation and further calculation g = (d −t)/2, ∆K = q ∫g 0 Egap dx. ∆K = qσ(d −t) 2ϵ0 . The field magnitude is fixed by the sheet charge, while the metal shortens the available vacuum acceleration distance. Physical check The probe motion ends at the metal surface; no field-free transit through conducting material is assumed.

Question 7

A neutral metal insert changes gap width while leaving fixed-sheet field unchanged

Infinite insulating sheets at x=0x=0 and x=dx=d carry fixed +σ+\sigma and −σ-\sigma, with σ>0\sigma>0. A neutral conducting slab of thickness t is centered between them, with 0<t<d0<t<d. Assume equilibrium and zero exterior field.

Diagram shown in the original SVG worksheet.

  1. Find the field in each vacuum gap and the induced density on each metal face.

  2. A weak positive charge q starts from rest just to the right of the left sheet and travels across the left vacuum gap. Find its kinetic-energy gain immediately before reaching the metal, neglecting image-force disturbance.

Question 7 - Solution

A neutral metal insert changes gap width while leaving fixed-sheet field unchanged

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Egap=σ/ϵ0,Emetal=0.E_{\mathrm{gap}}=\sigma/\epsilon_0,\quad E_{\mathrm{metal}}=0.σmetal,left=ϵ0(0−Egap)=−σ,σmetal,right=+σ.\sigma_{\mathrm{metal,left}}=\epsilon_0(0-E_{\mathrm{gap}})=-\sigma,\quad\sigma_{\mathrm{metal,right}}=+\sigma.

(b) Interpretation and further calculation

g=(d−t)/2,ΔK=q∫0gEgapdx.g=(d-t)/2,\quad\Delta K=q\int_0^gE_{\mathrm{gap}}\,dx.ΔK=qσ(d−t)2ϵ0.\Delta K=\frac{q\sigma(d-t)}{2\epsilon_0}.The field magnitude is fixed by the sheet charge, while the metal shortens the available vacuum acceleration distance.

Physical check

The probe motion ends at the metal surface; no field-free transit through conducting material is assumed.