The Electric Field Due to a Line of Charge — Question 9

Section 22-5 · Physics pages 3568–3569

Question 9 A nonuniform ring has a center field controlled by its first angular harmonic A circular ring of radius R has density λ(ϕ) = λ0(1 + β cos ϕ), with λ0 > 0 and |β| ≤1. Angle is measured from +x. x Heavier right semicircle illustrates positive beta; actual density varies smoothly. (a) Find its total charge and center-field vector. (b) Find its dipole moment about the center and explain how the same total charge can coexist with different center fields.
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Question 9 - Solution A nonuniform ring has a center field controlled by its first angular harmonic x (a) Method and calculation Q = R ∫2π 0 λ(ϕ) dϕ = 2πRλ0. Ex = −kλ0 R ∫2π 0 (1 + β cos ϕ) cos ϕ dϕ = −πkλ0β R , Ey = 0. (b) Interpretation and further calculation px = R2 ∫2π 0 λ(ϕ) cos ϕ dϕ = πλ0βR2, py = 0. E(0) = −kp/R3. Varying β redistributes charge without changing Q; the stronger positive-charge side pushes the center field toward the opposite side. Physical check The bound on beta keeps the density nonnegative everywhere, including the least populated side.

Question 9

A nonuniform ring has a center field controlled by its first angular harmonic

A circular ring of radius R has density λ(ϕ)=λ0(1+βcos⁡ϕ)\lambda(\phi)=\lambda_0(1+\beta\cos\phi), with λ0>0\lambda_0>0 and |β|≤1|\beta|\le1. Angle is measured from +x+x.

Diagram shown in the original SVG worksheet.

  1. Find its total charge and center-field vector.

  2. Find its dipole moment about the center and explain how the same total charge can coexist with different center fields.

Question 9 - Solution

A nonuniform ring has a center field controlled by its first angular harmonic

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q=R∫02πλ(ϕ)dϕ=2πRλ0.Q=R\int_0^{2\pi}\lambda(\phi)\,d\phi=2\pi R\lambda_0.Ex=−kλ0R∫02π(1+βcos⁡ϕ)cos⁡ϕdϕ=−πkλ0βR,Ey=0.E_x=-\frac{k\lambda_0}{R}\int_0^{2\pi}(1+\beta\cos\phi)\cos\phi\,d\phi=-\frac{\pi k\lambda_0\beta}{R},\quad E_y=0.

(b) Interpretation and further calculation

px=R2∫02πλ(ϕ)cos⁡ϕdϕ=πλ0βR2,py=0.p_x=R^2\int_0^{2\pi}\lambda(\phi)\cos\phi\,d\phi=\pi\lambda_0\beta R^2,\quad p_y=0.𝑬(0)=−k𝒑/R3.\mathbf E(0)=-k\mathbf p/R^3.Varying β\beta redistributes charge without changing Q; the stronger positive-charge side pushes the center field toward the opposite side.

Physical check

The bound on beta keeps the density nonnegative everywhere, including the least populated side.