Applying Gauss' Law: Planar Symmetry — Question 3

Section 23-7 · Physics pages 3756–3757

Question 3 Desired piecewise fields determine three sheet charges Three infinite insulating sheets lie at x = −d, 0 and +d. The desired field is zero outside the stack, +E0ˆx in −d < x < 0 and +2E0ˆx in 0 < x < d, with E0 > 0. −d 0 d E0 2E0 Schematic; labels, not drawing lengths, specify the data. (a) Find the three surface densities from the field jumps. (b) Check the total charge per area and verify one of the interior fields by adding individual sheet contributions.
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Question 3 - Solution Desired piecewise fields determine three sheet charges −d 0 d E0 2E0 (a) Method and calculation σi = ϵ0(Ex,right −Ex,left). σ−d = ϵ0E0, σ0 = ϵ0E0, σ+d = −2ϵ0E0. (b) Interpretation and further calculation Σ = σ−d + σ0 + σ+d = 0. −d < x < 0 : Ex = σ−d −σ0 −σ+d 2ϵ0 = E0. Zero net sheet charge allows zero exterior field, while distinct interior jumps create different gap fields. Physical check The field data also fix the otherwise possible added uniform field through the specified zero exterior values.

Question 3

Desired piecewise fields determine three sheet charges

Three infinite insulating sheets lie at x=−dx=-d, 0 and +d+d. The desired field is zero outside the stack, +E0𝒙̂+E_0\hat{\mathbf x} in −d<x<0-d<x<0 and +2E0𝒙̂+2E_0\hat{\mathbf x} in 0<x<d0<x<d, with E0>0E_0>0.

Diagram shown in the original SVG worksheet.

  1. Find the three surface densities from the field jumps.

  2. Check the total charge per area and verify one of the interior fields by adding individual sheet contributions.

Question 3 - Solution

Desired piecewise fields determine three sheet charges

Diagram shown in the original SVG worksheet.

(a) Method and calculation

σi=ϵ0(Ex,right−Ex,left).\sigma_i=\epsilon_0(E_{x,\mathrm{right}}-E_{x,\mathrm{left}}).σ−d=ϵ0E0,σ0=ϵ0E0,σ+d=−2ϵ0E0.\sigma_{-d}=\epsilon_0E_0,\quad\sigma_0=\epsilon_0E_0,\quad\sigma_{+d}=-2\epsilon_0E_0.

(b) Interpretation and further calculation

Σ=σ−d+σ0+σ+d=0.\Sigma=\sigma_{-d}+\sigma_0+\sigma_{+d}=0.−d<x<0:Ex=σ−d−σ0−σ+d2ϵ0=E0.-d<x<0:\quad E_x=\frac{\sigma_{-d}-\sigma_0-\sigma_{+d}}{2\epsilon_0}=E_0.Zero net sheet charge allows zero exterior field, while distinct interior jumps create different gap fields.

Physical check

The field data also fix the otherwise possible added uniform field through the specified zero exterior values.