Resistance and Resistivity — Question 2

Section 26-3 · Physics pages 4194–4195

Question 2 A linearly tapered radius requires integrating local resistance A long slender conductor has resistivity ρ, length L and radius r(x) = a + (b −a)x/L, where a, b > 0. Treat slices as equipotential disks and neglect end corrections. a b L Schematic; labels, not drawing lengths, specify the data. (a) Derive its end-to-end resistance. (b) Compare it with a uniform wire whose radius is the arithmetic mean (a + b)/2.
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Question 2 - Solution A linearly tapered radius requires integrating local resistance a b L (a) Method and calculation dR = ρ dx πr(x)2 , R = ρL π(b −a) (1 a −1 b ) . R = ρL πab also by continuity when a = b. (b) Interpretation and further calculation Rmean = 4ρL π(a + b)2 . R Rmean = (a + b)2 4ab = 1 + (a −b)2 4ab ≥1. Physical check The narrow portion raises resistance more than the wide portion lowers it.

Question 2

A linearly tapered radius requires integrating local resistance

A long slender conductor has resistivity ρ\rho, length L and radius r(x)=a+(b−a)x/Lr(x)=a+(b-a)x/L, where a,b>0a,b>0. Treat slices as equipotential disks and neglect end corrections.

Diagram shown in the original SVG worksheet.

  1. Derive its end-to-end resistance.

  2. Compare it with a uniform wire whose radius is the arithmetic mean (a+b)/2(a+b)/2.

Question 2 - Solution

A linearly tapered radius requires integrating local resistance

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dR=ρdxπr(x)2,R=ρLπ(b−a)(1a−1b).dR=\frac{\rho\,dx}{\pi r(x)^2},\quad R=\frac{\rho L}{\pi(b-a)}\left(\frac1a-\frac1b\right).R=ρLπabalso by continuity when a=b.R=\frac{\rho L}{\pi ab}\quad\text{also by continuity when }a=b.

(b) Interpretation and further calculation

Rmean=4ρLπ(a+b)2.R_{\mathrm{mean}}=\frac{4\rho L}{\pi(a+b)^2}.RRmean=(a+b)24ab=1+(a−b)24ab≥1.\frac{R}{R_{\mathrm{mean}}}=\frac{(a+b)^2}{4ab}=1+\frac{(a-b)^2}{4ab}\ge1.

Physical check

The narrow portion raises resistance more than the wide portion lowers it.