Dielectrics and Gauss' Law — Question 3

Section 25-7 · Physics pages 4136–4137

Question 3 A free charge sheet makes displacement different on the two sides of a layered gap Two dielectric layers of thicknesses t1, t2 and permittivities ϵ1, ϵ2 fill a plate gap. A fixed free interface sheet has density σs. Let z run from the lower electrode to the upper, and define V as lower minus upper potential. Fringing is negligible. A B d σs 1 2 Ideal plate cross-section; fringing is neglected unless stated. (a) Find D1 and D2 using the voltage and the interface jump. (b) Find the two electrode free charge densities and verify charge neutrality including the interface sheet.
Show solutionHide solution
Question 3 - Solution A free charge sheet makes displacement different on the two sides of a layered gap A B d σs 1 2 (a) Method and calculation D2 −D1 = σs, V = D1t1/ϵ1 + D2t2/ϵ2. D1 = V −σst2/ϵ2 t1/ϵ1 + t2/ϵ2 , D2 = D1 + σs. (b) Interpretation and further calculation σf,lower = D1, σf,upper = −D2. σf,lower + σs + σf,upper = D1 + σs −D2 = 0. Physical check Opposite electrode charges need not have equal magnitudes when free charge is trapped inside the gap.

Question 3

A free charge sheet makes displacement different on the two sides of a layered gap

Two dielectric layers of thicknesses t1,t2t_1,t_2 and permittivities ϵ1,ϵ2\epsilon_1,\epsilon_2 fill a plate gap. A fixed free interface sheet has density σs\sigma_s. Let z run from the lower electrode to the upper, and define V as lower minus upper potential. Fringing is negligible.

Diagram shown in the original SVG worksheet.

  1. Find D1 and D2 using the voltage and the interface jump.

  2. Find the two electrode free charge densities and verify charge neutrality including the interface sheet.

Question 3 - Solution

A free charge sheet makes displacement different on the two sides of a layered gap

Diagram shown in the original SVG worksheet.

(a) Method and calculation

D2−D1=σs,V=D1t1/ϵ1+D2t2/ϵ2.D_2-D_1=\sigma_s,\quad V=D_1t_1/\epsilon_1+D_2t_2/\epsilon_2.D1=V−σst2/ϵ2t1/ϵ1+t2/ϵ2,D2=D1+σs.D_1=\frac{V-\sigma_st_2/\epsilon_2}{t_1/\epsilon_1+t_2/\epsilon_2},\quad D_2=D_1+\sigma_s.

(b) Interpretation and further calculation

σf,lower=D1,σf,upper=−D2.\sigma_{f,\mathrm{lower}}=D_1,\quad\sigma_{f,\mathrm{upper}}=-D_2.σf,lower+σs+σf,upper=D1+σs−D2=0.\sigma_{f,\mathrm{lower}}+\sigma_s+\sigma_{f,\mathrm{upper}}=D_1+\sigma_s-D_2=0.

Physical check

Opposite electrode charges need not have equal magnitudes when free charge is trapped inside the gap.