Dielectrics and Gauss' Law β€” Question 7

Section 25-7 Β· Physics pages 4144–4145

Question 7 A prescribed polarization profile changes voltage through its spatial average Use D = Ο΅0E + P, βˆ‡Β· D = ρf, ρb = βˆ’βˆ‡Β· P and Οƒb = P Β· Λ†n, where n points out of the dielectric. In a plate gap 0 < z < d, the prescribed polarization is P = P0(z/d)2Λ†z. The electrodes carry free densities +Οƒf at zero and βˆ’Οƒf at d. There is no free bulk charge. z Pz Axes and labels specify the model; the sketch is schematic. (a) Find the bound volume and surface charge densities and verify their net sum is zero. (b) Find E(z) and the voltage drop from the lower electrode to the upper.
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Question 7 - Solution A prescribed polarization profile changes voltage through its spatial average z Pz (a) Method and calculation ρb = βˆ’2P0z/d2, Οƒb(0) = 0, Οƒb(d) = P0. ∫d 0 ρb dz + Οƒb(0) + Οƒb(d) = βˆ’P0 + P0 = 0. (b) Interpretation and further calculation Dz = Οƒf β‡’Ez = Οƒf βˆ’P0(z/d)2 Ο΅0 . Vlower βˆ’Vupper = ∫d 0 Ezdz = d Ο΅0 (Οƒf βˆ’P0/3). Physical check This is a prescribed polarization model; it need not obey a constant-permittivity constitutive relation.

Question 7

A prescribed polarization profile changes voltage through its spatial average

Use 𝑫=Ο΅0𝑬+𝑷\mathbf D=\epsilon_0\mathbf E+\mathbf P, βˆ‡β‹…π‘«=ρf\nabla\cdot\mathbf D=\rho_f, ρb=βˆ’βˆ‡β‹…π‘·\rho_b=-\nabla\cdot\mathbf P and Οƒb=𝑷⋅𝒏̂\sigma_b=\mathbf P\cdot\hat{\mathbf n}, where n points out of the dielectric. In a plate gap 0<z<d0<z<d, the prescribed polarization is 𝑷=P0(z/d)2𝒛̂\mathbf P=P_0(z/d)^2\hat{\mathbf z}. The electrodes carry free densities +Οƒf+\sigma_f at zero and βˆ’Οƒf-\sigma_f at d. There is no free bulk charge.

Diagram shown in the original SVG worksheet.

  1. Find the bound volume and surface charge densities and verify their net sum is zero.

  2. Find E(z) and the voltage drop from the lower electrode to the upper.

Question 7 - Solution

A prescribed polarization profile changes voltage through its spatial average

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ρb=βˆ’2P0z/d2,Οƒb(0)=0,Οƒb(d)=P0.\rho_b=-2P_0z/d^2,\quad\sigma_b(0)=0,\quad\sigma_b(d)=P_0.∫0dρbdz+Οƒb(0)+Οƒb(d)=βˆ’P0+P0=0.\int_0^d\rho_b\,dz+\sigma_b(0)+\sigma_b(d)=-P_0+P_0=0.

(b) Interpretation and further calculation

Dz=Οƒfβ‡’Ez=Οƒfβˆ’P0(z/d)2Ο΅0.D_z=\sigma_f\Rightarrow E_z=\frac{\sigma_f-P_0(z/d)^2}{\epsilon_0}.Vlowerβˆ’Vupper=∫0dEzdz=dΟ΅0(Οƒfβˆ’P0/3).V_{\mathrm{lower}}-V_{\mathrm{upper}}=\int_0^dE_zdz=\frac d{\epsilon_0}(\sigma_f-P_0/3).

Physical check

This is a prescribed polarization model; it need not obey a constant-permittivity constitutive relation.