Applying Gauss' Law: Spherical Symmetry — Question 6

Section 23-8 · Physics pages 3782–3783

Question 6 A neutral core-and-coating sphere can confine a nonzero field to its interior A sphere has density ρ1 > 0 for r < a and uniform density ρ2 in a < r < b. Choose ρ2 so the total charge is zero. There are no separate surface sheets or external sources. ρ1 ρ2 a b Cross-section of concentric regions with opposite signed fixed volume charge. (a) Find ρ2 and the field in the core and exterior. (b) Derive the coating-region field, determine its sign and show where the largest field occurs.
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Question 6 - Solution A neutral core-and-coating sphere can confine a nonzero field to its interior ρ1 ρ2 a b (a) Method and calculation 4π 3 [ρ1a3 + ρ2(b3 −a3)] = 0 ⇒ρ2 = −ρ1a3 b3 −a3 . Er = ρ1r 3ϵ0 (r < a), Er = 0 (r > b). (b) Interpretation and further calculation Er = ρ1a3 3ϵ0(b3 −a3) ( b3 r2 −r ) > 0 (a < r < b). dEr dr = ρ1a3 3ϵ0(b3 −a3) ( −2b3 r3 −1 ) < 0. The core field rises to Emax = ρ1a/(3ϵ0) at a, then decreases to zero through the coating. Physical check Total neutrality determines the exterior field here only because the entire distribution is spherically symmetric.

Question 6

A neutral core-and-coating sphere can confine a nonzero field to its interior

A sphere has density ρ1>0\rho_1>0 for r<ar<a and uniform density ρ2\rho_2 in a<r<ba<r<b. Choose ρ2\rho_2 so the total charge is zero. There are no separate surface sheets or external sources.

Diagram shown in the original SVG worksheet.

  1. Find ρ2\rho_2 and the field in the core and exterior.

  2. Derive the coating-region field, determine its sign and show where the largest field occurs.

Question 6 - Solution

A neutral core-and-coating sphere can confine a nonzero field to its interior

Diagram shown in the original SVG worksheet.

(a) Method and calculation

4π3[ρ1a3+ρ2(b3−a3)]=0⇒ρ2=−ρ1a3b3−a3.\frac{4\pi}{3}[\rho_1a^3+\rho_2(b^3-a^3)]=0\Rightarrow\rho_2=-\frac{\rho_1a^3}{b^3-a^3}.Er=ρ1r3ϵ0(r<a),Er=0(r>b).E_r=\frac{\rho_1r}{3\epsilon_0}\quad(r<a),\qquad E_r=0\quad(r>b).

(b) Interpretation and further calculation

Er=ρ1a33ϵ0(b3−a3)(b3r2−r)>0(a<r<b).E_r=\frac{\rho_1a^3}{3\epsilon_0(b^3-a^3)}\left(\frac{b^3}{r^2}-r\right)>0\quad(a<r<b).dErdr=ρ1a33ϵ0(b3−a3)(−2b3r3−1)<0.\frac{dE_r}{dr}=\frac{\rho_1a^3}{3\epsilon_0(b^3-a^3)}\left(-\frac{2b^3}{r^3}-1\right)<0.The core field rises to Emax=ρ1a/(3ϵ0)E_{\max}=\rho_1a/(3\epsilon_0) at a, then decreases to zero through the coating.

Physical check

Total neutrality determines the exterior field here only because the entire distribution is spherically symmetric.