Applying Gauss' Law: Spherical Symmetry — Question 3

Section 23-8 · Physics pages 3776–3777

Question 3 A quadratic radial density produces a cubic interior field A spherical insulator has density ρ(r) = ρ0r2/R2 for r < R, with ρ0 > 0, and no charge outside. Compare it with a uniformly charged sphere of the same R and same total charge. R ρ(r) Cross-section of concentric spherical surfaces; labels specify radii. (a) Derive its enclosed charge, interior field and total charge. (b) Find the density of the uniform comparison sphere and the ratio of interior fields at the same nonzero radius.
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Question 3 - Solution A quadratic radial density produces a cubic interior field R ρ(r) (a) Method and calculation Qenc = 4π ∫r 0 ρ0u2 R2 u2 du = 4πρ0r5 5R2 . Egraded = ρ0r3 5ϵ0R2 , Q = 4πρ0R3 5 . (b) Interpretation and further calculation ρuniform = Q 4πR3/3 = 3ρ0 5 , Euniform = ρ0r 5ϵ0 . Egraded/Euniform = (r/R)2. The stronger outward weighting reduces the enclosed fraction more severely at small r than a uniform sphere does. Physical check Both profiles have the same exterior field, so exterior measurements alone cannot distinguish their radial density distributions.

Question 3

A quadratic radial density produces a cubic interior field

A spherical insulator has density ρ(r)=ρ0r2/R2\rho(r)=\rho_0r^2/R^2 for r<Rr<R, with ρ0>0\rho_0>0, and no charge outside. Compare it with a uniformly charged sphere of the same R and same total charge.

Diagram shown in the original SVG worksheet.

  1. Derive its enclosed charge, interior field and total charge.

  2. Find the density of the uniform comparison sphere and the ratio of interior fields at the same nonzero radius.

Question 3 - Solution

A quadratic radial density produces a cubic interior field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qenc=4π∫0rρ0u2R2u2du=4πρ0r55R2.Q_{\mathrm{enc}}=4\pi\int_0^r\frac{\rho_0u^2}{R^2}u^2\,du=\frac{4\pi\rho_0r^5}{5R^2}.Egraded=ρ0r35ϵ0R2,Q=4πρ0R35.E_{\mathrm{graded}}=\frac{\rho_0r^3}{5\epsilon_0R^2},\quad Q=\frac{4\pi\rho_0R^3}{5}.

(b) Interpretation and further calculation

ρuniform=Q4πR3/3=3ρ05,Euniform=ρ0r5ϵ0.\rho_{\mathrm{uniform}}=\frac Q{4\pi R^3/3}=\frac{3\rho_0}{5},\quad E_{\mathrm{uniform}}=\frac{\rho_0r}{5\epsilon_0}.Egraded/Euniform=(r/R)2.E_{\mathrm{graded}}/E_{\mathrm{uniform}}=(r/R)^2.The stronger outward weighting reduces the enclosed fraction more severely at small r than a uniform sphere does.

Physical check

Both profiles have the same exterior field, so exterior measurements alone cannot distinguish their radial density distributions.