Dielectrics and Gauss' Law — Question 2

Section 25-7 · Physics pages 4134–4135

Question 2 An oblique dielectric interface preserves tangential field and normal displacement Two homogeneous linear dielectrics meet at a flat interface with no free surface charge. Let n point from medium 1 to 2 and t be tangent. Relative permittivities are 2 and 5; E1 = (3ˆn + 4ˆt) V/m. n 1 2 Schematic; labels, not drawing lengths, specify the data. (a) Find E2 using D2n = D1n and E2t = E1t. (b) Find the net bound interface charge density using σb = (P1 −P2) · ˆn.
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Question 2 - Solution An oblique dielectric interface preserves tangential field and normal displacement n 1 2 (a) Method and calculation 2ϵ0(3) = 5ϵ0E2n ⇒E2n = 1.20 V/m. E2 = (1.20ˆn + 4.00ˆt) V/m. (b) Interpretation and further calculation P1n = ϵ0(2 −1)(3) = 3ϵ0 V/m, P2n = ϵ0(5 −1)(1.20) = 4.80ϵ0 V/m. σb = −1.80ϵ0 V/m, E2n −E1n = σb/ϵ0. Physical check A jump in normal E is allowed even without free interface charge because bound interface charge is generally present.

Question 2

An oblique dielectric interface preserves tangential field and normal displacement

Two homogeneous linear dielectrics meet at a flat interface with no free surface charge. Let n point from medium 1 to 2 and t be tangent. Relative permittivities are 2 and 5; 𝑬1=(3𝒏̂+4𝒕̂)\mathbf E_1=(3\hat{\mathbf n}+4\hat{\mathbf t}) V/m.

Diagram shown in the original SVG worksheet.

  1. Find E2 using D2n=D1nD_{2n}=D_{1n} and E2t=E1tE_{2t}=E_{1t}.

  2. Find the net bound interface charge density using σb=(𝑷1−𝑷2)⋅𝒏̂\sigma_b=(\mathbf P_1-\mathbf P_2)\cdot\hat{\mathbf n}.

Question 2 - Solution

An oblique dielectric interface preserves tangential field and normal displacement

Diagram shown in the original SVG worksheet.

(a) Method and calculation

2ϵ0(3)=5ϵ0E2n⇒E2n=1.20V/m.2\epsilon_0(3)=5\epsilon_0E_{2n}\Rightarrow E_{2n}=1.20\,\mathrm{V/m}.𝑬2=(1.20𝒏̂+4.00𝒕̂)V/m.\mathbf E_2=(1.20\hat{\mathbf n}+4.00\hat{\mathbf t})\,\mathrm{V/m}.

(b) Interpretation and further calculation

P1n=ϵ0(2−1)(3)=3ϵ0V/m,P2n=ϵ0(5−1)(1.20)=4.80ϵ0V/m.P_{1n}=\epsilon_0(2-1)(3)=3\epsilon_0\,\mathrm{V/m},\quad P_{2n}=\epsilon_0(5-1)(1.20)=4.80\epsilon_0\,\mathrm{V/m}.σb=−1.80ϵ0V/m,E2n−E1n=σb/ϵ0.\sigma_b=-1.80\epsilon_0\,\mathrm{V/m},\quad E_{2n}-E_{1n}=\sigma_b/\epsilon_0.

Physical check

A jump in normal E is allowed even without free interface charge because bound interface charge is generally present.