Potential Due to a Continuous Charge Distribution — Question 3

Section 24-8 · Physics pages 3936–3937

Question 3 An axial rod potential contains a logarithm of two endpoint distances A uniform rod occupies 0 ≤x ≤L and has positive line density λ. Observe at x=-a with a>0. Use infinity reference. 0 L P −a Schematic; labels, not drawing lengths, specify the data. (a) Integrate the potential and express the logarithm using a dimensionless ratio. (b) Find its leading approximation for a much larger than L and the first relative correction to the point-charge result.
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Question 3 - Solution An axial rod potential contains a logarithm of two endpoint distances 0 L P −a (a) Method and calculation V (−a) = kλ ∫L 0 dx a + x = kλ[ln(a + x)]L 0 . V (−a) = kλ ln(1 + L/a). (b) Interpretation and further calculation V = kλL a [ 1 −L 2a + O(L2/a2) ] . Q = λL, V −kQ/a kQ/a ≃−L 2a. Physical check The expansion uses the near endpoint as origin; choosing the rod center would remove its first-order displacement correction.

Question 3

An axial rod potential contains a logarithm of two endpoint distances

A uniform rod occupies 0≤x≤L0\le x\le L and has positive line density λ\lambda. Observe at x=-a with a>0. Use infinity reference.

Diagram shown in the original SVG worksheet.

  1. Integrate the potential and express the logarithm using a dimensionless ratio.

  2. Find its leading approximation for a much larger than L and the first relative correction to the point-charge result.

Question 3 - Solution

An axial rod potential contains a logarithm of two endpoint distances

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(−a)=kλ∫0Ldxa+x=kλ[ln⁡(a+x)]0L.V(-a)=k\lambda\int_0^L\frac{dx}{a+x}=k\lambda[\ln(a+x)]_0^L.V(−a)=kλln⁡(1+L/a).V(-a)=k\lambda\ln(1+L/a).

(b) Interpretation and further calculation

V=kλLa[1−L2a+O(L2/a2)].V=\frac{k\lambda L}{a}\left[1-\frac{L}{2a}+O(L^2/a^2)\right].Q=λL,V−kQ/akQ/a≃−L2a.Q=\lambda L,\quad\frac{V-kQ/a}{kQ/a}\simeq-\frac L{2a}.

Physical check

The expansion uses the near endpoint as origin; choosing the rod center would remove its first-order displacement correction.