Applying Gauss' Law: Spherical Symmetry — Question 7

Section 23-8 · Physics pages 3784–3785

Question 7 A smoothed Coulomb field reveals an exponential radial charge distribution A spherically symmetric field is measured as Er(r) = Q[1 −e−(r/a)3]/(4πϵ0r2) for r > 0, with Q, a > 0. Assume no source singularity is hidden at the origin. r r1/2 Schematic spherical charge distribution with no sharp outer boundary. (a) Infer Qenc(r) and the volume density using dQenc/dr = 4πr2ρ(r). (b) Find the radius containing half the total charge and the leading field near the origin. Check regularity there.
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Question 7 - Solution A smoothed Coulomb field reveals an exponential radial charge distribution r r1/2 (a) Method and calculation Qenc(r) = 4πϵ0r2Er = Q[1 −e−(r/a)3]. ρ(r) = 1 4πr2 dQenc dr = 3Q 4πa3 e−(r/a)3. (b) Interpretation and further calculation Qenc(r1/2) = Q/2 ⇒r1/2 = a(ln 2)1/3 ≈.884997a. r ≪a : 1 −e−(r/a)3 ≃(r/a)3 ⇒Er ≃ Qr 4πϵ0a3 . The density is finite and the vector field tends continuously to zero at the center. Physical check The enclosed charge approaches Q at infinity and approaches zero as r3 at the origin, leaving no point-charge term.

Question 7

A smoothed Coulomb field reveals an exponential radial charge distribution

A spherically symmetric field is measured as Er(r)=Q[1−e−(r/a)3]/(4πϵ0r2)E_r(r)=Q[1-e^{-(r/a)^3}]/(4\pi\epsilon_0r^2) for r>0r>0, with Q,a>0Q,a>0. Assume no source singularity is hidden at the origin.

Diagram shown in the original SVG worksheet.

  1. Infer Qenc(r)Q_{\mathrm{enc}}(r) and the volume density using dQenc/dr=4πr2ρ(r)dQ_{\mathrm{enc}}/dr=4\pi r^2\rho(r).

  2. Find the radius containing half the total charge and the leading field near the origin. Check regularity there.

Question 7 - Solution

A smoothed Coulomb field reveals an exponential radial charge distribution

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qenc(r)=4πϵ0r2Er=Q[1−e−(r/a)3].Q_{\mathrm{enc}}(r)=4\pi\epsilon_0r^2E_r=Q[1-e^{-(r/a)^3}].ρ(r)=14πr2dQencdr=3Q4πa3e−(r/a)3.\rho(r)=\frac1{4\pi r^2}\frac{dQ_{\mathrm{enc}}}{dr}=\frac{3Q}{4\pi a^3}e^{-(r/a)^3}.

(b) Interpretation and further calculation

Qenc(r1/2)=Q/2⇒r1/2=a(ln⁡2)1/3≈.884997a.Q_{\mathrm{enc}}(r_{1/2})=Q/2\Rightarrow r_{1/2}=a(\ln2)^{1/3}\approx.884997a.r≪a:1−e−(r/a)3≃(r/a)3⇒Er≃Qr4πϵ0a3.r\ll a:\quad1-e^{-(r/a)^3}\simeq(r/a)^3\Rightarrow E_r\simeq\frac{Qr}{4\pi\epsilon_0a^3}.The density is finite and the vector field tends continuously to zero at the center.

Physical check

The enclosed charge approaches Q at infinity and approaches zero as r3r^3 at the origin, leaving no point-charge term.