Dielectrics and Gauss' Law — Question 6

Section 25-7 · Physics pages 4142–4143

Question 6 A uniformly distributed free charge induces compensating bulk and surface bound charges Use D = ϵ0E + P, ∇· D = ρf, ρb = −∇· P and σb = P · ˆn, where n points out of the dielectric. A nonconducting sphere of radius R and uniform relative permittivity kappa contains fixed uniform free volume density rho0. Outside is vacuum; no free surface charge is present. R ρ0 Cross-section of concentric spherical surfaces; labels specify radii. (a) Find the interior D, E and bound volume density. (b) Find the bound surface density and show that the net bound charge is zero.
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Question 6 - Solution A uniformly distributed free charge induces compensating bulk and surface bound charges R ρ0 (a) Method and calculation 4πr2Dr = 4πr3 3 ρ0 ⇒Dr = ρ0r/3, Er = ρ0r/(3κϵ0). Pr = (1 −1/κ)ρ0r/3 ⇒ρb = −(1 −1/κ)ρ0. (b) Interpretation and further calculation σb(R) = Pr(R) = (1 −1/κ)ρ0R/3. Qb,volume = −4πR3 3 (1 −1/κ)ρ0 = −Qb,surface. Physical check The bound charges redistribute a neutral dielectric; they do not change its total charge.

Question 6

A uniformly distributed free charge induces compensating bulk and surface bound charges

Use 𝑫=ϵ0𝑬+𝑷\mathbf D=\epsilon_0\mathbf E+\mathbf P, ∇⋅𝑫=ρf\nabla\cdot\mathbf D=\rho_f, ρb=−∇⋅𝑷\rho_b=-\nabla\cdot\mathbf P and σb=𝑷⋅𝒏̂\sigma_b=\mathbf P\cdot\hat{\mathbf n}, where n points out of the dielectric. A nonconducting sphere of radius R and uniform relative permittivity kappa contains fixed uniform free volume density rho0. Outside is vacuum; no free surface charge is present.

Diagram shown in the original SVG worksheet.

  1. Find the interior D, E and bound volume density.

  2. Find the bound surface density and show that the net bound charge is zero.

Question 6 - Solution

A uniformly distributed free charge induces compensating bulk and surface bound charges

Diagram shown in the original SVG worksheet.

(a) Method and calculation

4πr2Dr=4πr33ρ0⇒Dr=ρ0r/3,Er=ρ0r/(3κϵ0).4\pi r^2D_r=\frac{4\pi r^3}{3}\rho_0\Rightarrow D_r=\rho_0r/3,\quad E_r=\rho_0r/(3\kappa\epsilon_0).Pr=(1−1/κ)ρ0r/3⇒ρb=−(1−1/κ)ρ0.P_r=(1-1/\kappa)\rho_0r/3\Rightarrow\rho_b=-(1-1/\kappa)\rho_0.

(b) Interpretation and further calculation

σb(R)=Pr(R)=(1−1/κ)ρ0R/3.\sigma_b(R)=P_r(R)=(1-1/\kappa)\rho_0R/3.Qb,volume=−4πR33(1−1/κ)ρ0=−Qb,surface.Q_{b,\mathrm{volume}}=-\frac{4\pi R^3}{3}(1-1/\kappa)\rho_0=-Q_{b,\mathrm{surface}}.

Physical check

The bound charges redistribute a neutral dielectric; they do not change its total charge.