Dielectrics and Gauss' Law — Question 1

Section 25-7 · Physics pages 4132–4133

Question 1 Gauss law separates electrode charge from the bound charge that screens it Use D = ϵ0E + P, ∇· D = ρf, ρb = −∇· P and σb = P · ˆn, where n points out of the dielectric. A linear dielectric of relative permittivity kappa fills a plate gap from z=0 to d. The electrode at zero has free charge density +σf and the one at d has −σf, with σf > 0. Neglect fringing. A B d z, D Ideal plate cross-section; fringing is neglected unless stated. (a) Find D, E and P in the gap. (b) Find the bound charge on each dielectric face and verify the field using total charge.
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Question 1 - Solution Gauss law separates electrode charge from the bound charge that screens it A B d z, D (a) Method and calculation D = σfˆz, E = σf κϵ0 ˆz. P = ϵ0(κ −1)E = σf(1 −1/κ)ˆz. (b) Interpretation and further calculation σb(0) = −σf(1 −1/κ), σb(d) = +σf(1 −1/κ), ρb = 0. E = σf + σb(0) ϵ0 = σf κϵ0 . Physical check Gauss law for D counts free charge; Gauss law for E counts free plus bound charge.

Question 1

Gauss law separates electrode charge from the bound charge that screens it

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 linear dielectric of relative permittivity kappa fills a plate gap from z=0 to d. The electrode at zero has free charge density +σf+\sigma_f and the one at d has −σf-\sigma_f, with σf>0\sigma_f>0. Neglect fringing.

Diagram shown in the original SVG worksheet.

  1. Find D, E and P in the gap.

  2. Find the bound charge on each dielectric face and verify the field using total charge.

Question 1 - Solution

Gauss law separates electrode charge from the bound charge that screens it

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑫=σf𝒛̂,𝑬=σfκϵ0𝒛̂.\mathbf D=\sigma_f\hat{\mathbf z},\quad\mathbf E=\frac{\sigma_f}{\kappa\epsilon_0}\hat{\mathbf z}.𝑷=ϵ0(κ−1)𝑬=σf(1−1/κ)𝒛̂.\mathbf P=\epsilon_0(\kappa-1)\mathbf E=\sigma_f(1-1/\kappa)\hat{\mathbf z}.

(b) Interpretation and further calculation

σb(0)=−σf(1−1/κ),σb(d)=+σf(1−1/κ),ρb=0.\sigma_b(0)=-\sigma_f(1-1/\kappa),\quad\sigma_b(d)=+\sigma_f(1-1/\kappa),\quad\rho_b=0.E=σf+σb(0)ϵ0=σfκϵ0.E=\frac{\sigma_f+\sigma_b(0)}{\epsilon_0}=\frac{\sigma_f}{\kappa\epsilon_0}.

Physical check

Gauss law for D counts free charge; Gauss law for E counts free plus bound charge.