Applying Gauss' Law: Cylindrical Symmetry — Question 6

Section 23-6 · Physics pages 3742–3743

Question 6 A coaxial conductor can shield the exterior while retaining a gap field An infinite inner conducting cylinder of radius a carries charge per length λ > 0. A coaxial outer conductor occupies b < r < c, with a < b < c, and has net charge per length Λ. Everything is in electrostatic equilibrium. a b c Cross-section perpendicular to an infinite cylinder axis; end effects are excluded. (a) Find the charge per length on the inner and outer surfaces of the outer conductor. (b) Derive the field in the vacuum gap and outside c, then choose Λ so the exterior field vanishes.
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Question 6 - Solution A coaxial conductor can shield the exterior while retaining a gap field a b c (a) Method and calculation Eb<r<c = 0 ⇒λ + λb = 0 ⇒λb = −λ. λc = Λ −λb = Λ + λ. (b) Interpretation and further calculation Er = λ 2πϵ0r (a < r < b), Er = λ + Λ 2πϵ0r (r > c). Λ = −λ ⇒Er>c = 0, Ea<r<b̸ = 0. The Gaussian surface in the metal determines the induced inner charge before symmetry is used in the vacuum regions. Physical check The induced surface densities are −λ/(2πb) and (Λ + λ)/(2πc), not equal merely because total charges may cancel.

Question 6

A coaxial conductor can shield the exterior while retaining a gap field

An infinite inner conducting cylinder of radius a carries charge per length λ>0\lambda>0. A coaxial outer conductor occupies b<r<cb<r<c, with a<b<ca<b<c, and has net charge per length Λ\Lambda. Everything is in electrostatic equilibrium.

Diagram shown in the original SVG worksheet.

  1. Find the charge per length on the inner and outer surfaces of the outer conductor.

  2. Derive the field in the vacuum gap and outside c, then choose Λ\Lambda so the exterior field vanishes.

Question 6 - Solution

A coaxial conductor can shield the exterior while retaining a gap field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Eb<r<c=0⇒λ+λb=0⇒λb=−λ.E_{b<r<c}=0\Rightarrow\lambda+\lambda_b=0\Rightarrow\lambda_b=-\lambda.λc=Λ−λb=Λ+λ.\lambda_c=\Lambda-\lambda_b=\Lambda+\lambda.

(b) Interpretation and further calculation

Er=λ2πϵ0r(a<r<b),Er=λ+Λ2πϵ0r(r>c).E_r=\frac{\lambda}{2\pi\epsilon_0r}\quad(a<r<b),\quad E_r=\frac{\lambda+\Lambda}{2\pi\epsilon_0r}\quad(r>c).Λ=−λ⇒Er>c=0,Ea<r<b≠0.\Lambda=-\lambda\Rightarrow E_{r>c}=0,\quad E_{a<r<b}\ne0.The Gaussian surface in the metal determines the induced inner charge before symmetry is used in the vacuum regions.

Physical check

The induced surface densities are −λ/(2πb)-\lambda/(2\pi b) and (Λ+λ)/(2πc)(\Lambda+\lambda)/(2\pi c), not equal merely because total charges may cancel.