The Electric Field Due to a Line of Charge — Question 4

Section 22-5 · Physics pages 3558–3559

Question 4 An off-center observation point retains both rod-field components A uniform positive line density λ occupies 0 ≤x ≤L. Observe at P= (0, y), y > 0. Use k for the Coulomb constant. P Schematic; labels, not drawing lengths, specify the data. (a) Integrate both field components. (b) For L = y, find the angle of the field left of the upward vertical and the component ratio.
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Question 4 - Solution An off-center observation point retains both rod-field components P (a) Method and calculation Ex = −kλ ∫L 0 x dx (x2 + y2)3/2 = −kλ ( 1 y − 1 √ L2 + y2 ) . Ey = kλy ∫L 0 dx (x2 + y2)3/2 = kλL y √ L2 + y2 . (b) Interpretation and further calculation L = y : |Ex| Ey = √ 2 −1. α = tan−1( √ 2 −1) = 22.5◦. Every element pushes P upward and leftward, so neither component cancels. Physical check Using the midpoint formula here would incorrectly impose a symmetry the source does not possess.

Question 4

An off-center observation point retains both rod-field components

A uniform positive line density λ\lambda occupies 0≤x≤L0\le x\le L. Observe at P=(0,y)=(0,y), y>0y>0. Use k for the Coulomb constant.

Diagram shown in the original SVG worksheet.

  1. Integrate both field components.

  2. For L=yL=y, find the angle of the field left of the upward vertical and the component ratio.

Question 4 - Solution

An off-center observation point retains both rod-field components

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex=−kλ∫0Lxdx(x2+y2)3/2=−kλ(1y−1L2+y2).E_x=-k\lambda\int_0^L\frac{x\,dx}{(x^2+y^2)^{3/2}}=-k\lambda\left(\frac1y-\frac1{\sqrt{L^2+y^2}}\right).Ey=kλy∫0Ldx(x2+y2)3/2=kλLyL2+y2.E_y=k\lambda y\int_0^L\frac{dx}{(x^2+y^2)^{3/2}}=\frac{k\lambda L}{y\sqrt{L^2+y^2}}.

(b) Interpretation and further calculation

L=y:|Ex|Ey=2−1.L=y:\quad\frac{|E_x|}{E_y}=\sqrt2-1.α=tan⁡−1(2−1)=22.5∘.\alpha=\tan^{-1}(\sqrt2-1)=22.5^\circ.Every element pushes P upward and leftward, so neither component cancels.

Physical check

Using the midpoint formula here would incorrectly impose a symmetry the source does not possess.