Potential Due to a Continuous Charge Distribution — Question 4

Section 24-8 · Physics pages 3938–3939

Question 4 A finite rod approaches an infinite-line voltage difference without a finite absolute voltage A uniform rod extends from x=-L to L with line density λ > 0. Points lie a perpendicular distance b>0 from its midpoint. For finite L set zero potential at infinity. −L L P Schematic; labels, not drawing lengths, specify the data. (a) Derive V(b). (b) Find the limit of V(b2)-V(b1) as L tends to infinity and explain why the individual voltages diverge.
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Question 4 - Solution A finite rod approaches an infinite-line voltage difference without a finite absolute voltage −L L P (a) Method and calculation V (b) = 2kλ ∫L 0 dx √ x2 + b2 = 2kλ arsinh(L/b). V (b) = 2kλ ln ( L + √ L2 + b2 b ) . (b) Interpretation and further calculation L ≫b : V (b) ≃2kλ ln(2L/b). lim L→∞[V (b2) −V (b1)] = 2kλ ln(b1/b2). Physical check The divergent term depends on L alone and cancels from the difference; the infinite-line model needs a finite-radius reference.

Question 4

A finite rod approaches an infinite-line voltage difference without a finite absolute voltage

A uniform rod extends from x=-L to L with line density λ>0\lambda>0. Points lie a perpendicular distance b>0 from its midpoint. For finite L set zero potential at infinity.

Diagram shown in the original SVG worksheet.

  1. Derive V(b).

  2. Find the limit of V(b2)-V(b1) as L tends to infinity and explain why the individual voltages diverge.

Question 4 - Solution

A finite rod approaches an infinite-line voltage difference without a finite absolute voltage

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(b)=2kλ∫0Ldxx2+b2=2kλarsinh⁡(L/b).V(b)=2k\lambda\int_0^L\frac{dx}{\sqrt{x^2+b^2}}=2k\lambda\operatorname{arsinh}(L/b).V(b)=2kλln⁡(L+L2+b2b).V(b)=2k\lambda\ln\left(\frac{L+\sqrt{L^2+b^2}}b\right).

(b) Interpretation and further calculation

L≫b:V(b)≃2kλln⁡(2L/b).L\gg b:\quad V(b)\simeq2k\lambda\ln(2L/b).limL→∞[V(b2)−V(b1)]=2kλln⁡(b1/b2).\lim_{L\to\infty}[V(b_2)-V(b_1)]=2k\lambda\ln(b_1/b_2).

Physical check

The divergent term depends on L alone and cancels from the difference; the infinite-line model needs a finite-radius reference.