The Electric Field Due to a Line of Charge — Question 6

Section 22-5 · Physics pages 3562–3563

Question 6 A charged semicircle gives a finite center field despite equal source distances A thin uniformly charged upper semicircle has radius R and total charge Q > 0. Parameterize its points by (R cos ϕ, R sin ϕ) with 0 ≤ϕ ≤π. R Schematic; labels, not drawing lengths, specify the data. (a) Integrate the center field using dq = λR dϕ. (b) Express the result in terms of Q and compare with the field of a complete uniformly charged circle carrying the same Q.
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Question 6 - Solution A charged semicircle gives a finite center field despite equal source distances R (a) Method and calculation λ = Q/(πR), dE = −kλ R (cos ϕ, sin ϕ) dϕ. Ex = 0, Ey = −kλ R ∫π 0 sin ϕ dϕ = −2kQ πR2 . (b) Interpretation and further calculation full circle : ∫2π 0 cos ϕ dϕ = ∫2π 0 sin ϕ dϕ = 0. Efull(0) = 0. Equal distances set equal weighting per charge element, but vector cancellation depends on the angular distribution. Physical check The semicircle field points downward, away from the positively charged upper arc.

Question 6

A charged semicircle gives a finite center field despite equal source distances

A thin uniformly charged upper semicircle has radius R and total charge Q>0Q>0. Parameterize its points by (Rcos⁡ϕ,Rsin⁡ϕ)(R\cos\phi,R\sin\phi) with 0≤ϕ≤π0\le\phi\le\pi.

Diagram shown in the original SVG worksheet.

  1. Integrate the center field using dq=λRdϕdq=\lambda R\,d\phi.

  2. Express the result in terms of Q and compare with the field of a complete uniformly charged circle carrying the same Q.

Question 6 - Solution

A charged semicircle gives a finite center field despite equal source distances

Diagram shown in the original SVG worksheet.

(a) Method and calculation

λ=Q/(πR),d𝑬=−kλR(cos⁡ϕ,sin⁡ϕ)dϕ.\lambda=Q/(\pi R),\quad d\mathbf E=-\frac{k\lambda}{R}(\cos\phi,\sin\phi)\,d\phi.Ex=0,Ey=−kλR∫0πsin⁡ϕdϕ=−2kQπR2.E_x=0,\quad E_y=-\frac{k\lambda}{R}\int_0^\pi\sin\phi\,d\phi=-\frac{2kQ}{\pi R^2}.

(b) Interpretation and further calculation

full circle:∫02πcos⁡ϕdϕ=∫02πsin⁡ϕdϕ=0.\text{full circle}:\quad\int_0^{2\pi}\cos\phi\,d\phi=\int_0^{2\pi}\sin\phi\,d\phi=0.𝑬full(0)=𝟎.\mathbf E_{\mathrm{full}}(0)=\mathbf0.Equal distances set equal weighting per charge element, but vector cancellation depends on the angular distribution.

Physical check

The semicircle field points downward, away from the positively charged upper arc.