Potential Due to a Point Charge — Question 10

Section 24-5 · Physics pages 3890–3891

Question 10 A distant point source looks locally like a constant plus a uniform field A positive point charge Q is at x=-R. For |x| ≪R, observations lie near the origin on the x axis. Use V (x) = kQ/(R + x) with infinity reference. x Q 0 x Schematic; labels, not drawing lengths, specify the data. (a) Expand V through second order in x/R and identify the locally uniform field term. (b) Find the relative error of the linear approximation at x=.100R, using the exact potential as denominator.
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Question 10 - Solution A distant point source looks locally like a constant plus a uniform field x Q 0 x (a) Method and calculation V (x) = kQ R [ 1 −x R + x2 R2 + O((x/R)3) ] . Vlin = kQ R −kQ R2 x, Elocal = kQ/R2. (b) Interpretation and further calculation Vlin −Vexact Vexact = (1 −x/R)(1 + x/R) −1 = −x2/R2. x = .100R : relative error = −.0100 = −1.00%. Physical check The large constant voltage is reference-dependent; the linear term supplies the leading measurable local field.

Question 10

A distant point source looks locally like a constant plus a uniform field

A positive point charge Q is at x=-R. For |x|≪R|x|\ll R, observations lie near the origin on the x axis. Use V(x)=kQ/(R+x)V(x)=kQ/(R+x) with infinity reference.

Diagram shown in the original SVG worksheet.

  1. Expand V through second order in x/R and identify the locally uniform field term.

  2. Find the relative error of the linear approximation at x=.100R, using the exact potential as denominator.

Question 10 - Solution

A distant point source looks locally like a constant plus a uniform field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V(x)=kQR[1−xR+x2R2+O((x/R)3)].V(x)=\frac{kQ}{R}\left[1-\frac xR+\frac{x^2}{R^2}+O((x/R)^3)\right].Vlin=kQR−kQR2x,Elocal=kQ/R2.V_{\mathrm{lin}}=\frac{kQ}{R}-\frac{kQ}{R^2}x,\quad E_{\mathrm{local}}=kQ/R^2.

(b) Interpretation and further calculation

Vlin−VexactVexact=(1−x/R)(1+x/R)−1=−x2/R2.\frac{V_{\mathrm{lin}}-V_{\mathrm{exact}}}{V_{\mathrm{exact}}}=(1-x/R)(1+x/R)-1=-x^2/R^2.x=.100R:relative error=−.0100=−1.00%.x=.100R:\quad\text{relative error}=-.0100=-1.00\%.

Physical check

The large constant voltage is reference-dependent; the linear term supplies the leading measurable local field.