The Electric Field Due to a Line of Charge — Question 10

Section 22-5 · Physics pages 3570–3571

Question 10 The null between parallel line charges reflects inverse-distance rather than inverse-square decay Two infinite straight lines parallel to z cross the xy plane at x = −a and x = a. Their positive densities are λ and 2λ. On the x axis use the line-field magnitude 2kλ/r. x ⊙ ⊙ λ 2λ Schematic; labels, not drawing lengths, specify the data. (a) Find the field null between the lines. (b) Generalize the relation between a null location x0 and the ratio λR/λL. Explain why the point-charge cancellation formula cannot be substituted.
Show solutionHide solution
Question 10 - Solution The null between parallel line charges reflects inverse-distance rather than inverse-square decay x ⊙ ⊙ λ 2λ (a) Method and calculation Ex = 2kλ x + a −4kλ a −x = 0. a −x = 2(x + a) ⇒x = −a/3. (b) Interpretation and further calculation λL x0 + a = λR a −x0 ⇒λR λL = a −x0 a + x0 . Eline ∝r−1, Epoint ∝r−2. The null is closer to the weaker line, but the distance ratio follows a different power law. Physical check The circles show cross-sections of infinite lines normal to the page, not individual point charges.

Question 10

The null between parallel line charges reflects inverse-distance rather than inverse-square decay

Two infinite straight lines parallel to z cross the xy plane at x=−ax=-a and x=ax=a. Their positive densities are λ\lambda and 2λ2\lambda. On the x axis use the line-field magnitude 2kλ/r2k\lambda/r.

Diagram shown in the original SVG worksheet.

  1. Find the field null between the lines.

  2. Generalize the relation between a null location x0x_0 and the ratio λR/λL\lambda_R/\lambda_L. Explain why the point-charge cancellation formula cannot be substituted.

Question 10 - Solution

The null between parallel line charges reflects inverse-distance rather than inverse-square decay

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex=2kλx+a−4kλa−x=0.E_x=\frac{2k\lambda}{x+a}-\frac{4k\lambda}{a-x}=0.a−x=2(x+a)⇒x=−a/3.a-x=2(x+a)\Rightarrow x=-a/3.

(b) Interpretation and further calculation

λLx0+a=λRa−x0⇒λRλL=a−x0a+x0.\frac{\lambda_L}{x_0+a}=\frac{\lambda_R}{a-x_0}\Rightarrow\frac{\lambda_R}{\lambda_L}=\frac{a-x_0}{a+x_0}.Eline∝r−1,Epoint∝r−2.E_{\mathrm{line}}\propto r^{-1},\quad E_{\mathrm{point}}\propto r^{-2}.The null is closer to the weaker line, but the distance ratio follows a different power law.

Physical check

The circles show cross-sections of infinite lines normal to the page, not individual point charges.