Gauss' Law — Question 6

Section 23-3 · Physics pages 3682–3683

Question 6 Zero divergence away from a point does not exclude a concentrated source For every r > 0, a radial electric field is E = Cˆr/r2, with C > 0. You may use ∇· E = r−2d(r2Er)/dr wherever the field is smooth. R source Cross-section of concentric spherical surfaces; labels specify radii. (a) Find the ordinary volume charge density for r > 0 and the charge enclosed by any sphere centered at the origin. (b) Explain how these results coexist, and determine the net charge in any spherical annulus that excludes the origin.
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Question 6 - Solution Zero divergence away from a point does not exclude a concentrated source R source (a) Method and calculation r > 0 : ∇· E = 1 r2 dC dr = 0 ⇒ρ = 0. Φ(R) = 4πR2 C R2 = 4πC ⇒Qenc = 4πϵ0C. (b) Interpretation and further calculation Qa<r<b = ϵ0[Φ(b) −Φ(a)] = 0. Qr=0 = 4πϵ0C. The source is concentrated at the singular origin. The smooth-field divergence expression cannot be applied through that singular point as if the field were regular. Physical check Every centered sphere encloses the same concentrated charge, regardless of its nonzero radius.

Question 6

Zero divergence away from a point does not exclude a concentrated source

For every r>0r>0, a radial electric field is 𝑬=C𝒓̂/r2\mathbf E=C\hat{\mathbf r}/r^2, with C>0C>0. You may use 𝜵⋅𝑬=r−2d(r2Er)/dr\boldsymbol\nabla\cdot\mathbf E=r^{-2}d(r^2E_r)/dr wherever the field is smooth.

Diagram shown in the original SVG worksheet.

  1. Find the ordinary volume charge density for r>0r>0 and the charge enclosed by any sphere centered at the origin.

  2. Explain how these results coexist, and determine the net charge in any spherical annulus that excludes the origin.

Question 6 - Solution

Zero divergence away from a point does not exclude a concentrated source

Diagram shown in the original SVG worksheet.

(a) Method and calculation

r>0:𝜵⋅𝑬=1r2dCdr=0⇒ρ=0.r>0:\quad\boldsymbol\nabla\cdot\mathbf E=\frac1{r^2}\frac{dC}{dr}=0\Rightarrow\rho=0.Φ(R)=4πR2CR2=4πC⇒Qenc=4πϵ0C.\Phi(R)=4\pi R^2\frac C{R^2}=4\pi C\Rightarrow Q_{\mathrm{enc}}=4\pi\epsilon_0C.

(b) Interpretation and further calculation

Qa<r<b=ϵ0[Φ(b)−Φ(a)]=0.Q_{a<r<b}=\epsilon_0[\Phi(b)-\Phi(a)]=0.Qr=0=4πϵ0C.Q_{r=0}=4\pi\epsilon_0C.The source is concentrated at the singular origin. The smooth-field divergence expression cannot be applied through that singular point as if the field were regular.

Physical check

Every centered sphere encloses the same concentrated charge, regardless of its nonzero radius.