Resistance and Resistivity — Question 4

Section 26-3 · Physics pages 4198–4199

Question 4 Radial leakage through a cylindrical insulator has logarithmic resistance A material of uniform resistivity ρ fills the gap between coaxial electrodes of radii a and b and length L. End effects are negligible; leakage flows radially. a b I Schematic; labels, not drawing lengths, specify the data. (a) Find the leakage resistance. (b) For a thin gap d = b −a ≪a, obtain the leading approximation and identify its effective area.
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Question 4 - Solution Radial leakage through a cylindrical insulator has logarithmic resistance a b I (a) Method and calculation dR = ρ dr 2πrL. R = ρ 2πL ln(b/a). (b) Interpretation and further calculation ln(b/a) = ln(1 + d/a) = d/a + O((d/a)2). R ≃ρd/(2πaL) = ρd/Ainner. Physical check Here the current path is radial, so the conducting area grows with radius.

Question 4

Radial leakage through a cylindrical insulator has logarithmic resistance

A material of uniform resistivity ρ\rho fills the gap between coaxial electrodes of radii a and b and length L. End effects are negligible; leakage flows radially.

Diagram shown in the original SVG worksheet.

  1. Find the leakage resistance.

  2. For a thin gap d=b−a≪ad=b-a\ll a, obtain the leading approximation and identify its effective area.

Question 4 - Solution

Radial leakage through a cylindrical insulator has logarithmic resistance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dR=ρdr2πrL.dR=\frac{\rho\,dr}{2\pi rL}.R=ρ2πLln⁡(b/a).R=\frac{\rho}{2\pi L}\ln(b/a).

(b) Interpretation and further calculation

ln⁡(b/a)=ln⁡(1+d/a)=d/a+O((d/a)2).\ln(b/a)=\ln(1+d/a)=d/a+O((d/a)^2).R≃ρd/(2πaL)=ρd/Ainner.R\simeq\rho d/(2\pi aL)=\rho d/A_{\mathrm{inner}}.

Physical check

Here the current path is radial, so the conducting area grows with radius.