Capacitor with a Dielectric — Question 3

Section 25-5 · Physics pages 4096–4097

Question 3 Dielectric layers across the gap divide voltage inversely with permittivity Two dielectric layers each occupy half the gap d of a plate capacitor of area A. Their relative permittivities are 2 and 6. There is no free charge at their interface; thus ϵ1E1 = ϵ2E2. Fringing is negligible. A B d κ1 κ2 Ideal plate cross-section; fringing is neglected unless stated. (a) Find C in terms of C0 = ϵ0A/d. (b) At applied voltage V, find both fields and layer voltage drops.
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Question 3 - Solution Dielectric layers across the gap divide voltage inversely with permittivity A B d κ1 κ2 (a) Method and calculation V = Q A (d/2 2ϵ0 + d/2 6ϵ0 ) = Qd 3ϵ0A. C = 3C0. (b) Interpretation and further calculation E1 = Q 2ϵ0A = 3V 2d , E2 = Q 6ϵ0A = V 2d. V1 = 3V/4, V2 = V/4. Physical check The lower-permittivity layer sustains the larger electric field and voltage drop.

Question 3

Dielectric layers across the gap divide voltage inversely with permittivity

Two dielectric layers each occupy half the gap d of a plate capacitor of area A. Their relative permittivities are 2 and 6. There is no free charge at their interface; thus ϵ1E1=ϵ2E2\epsilon_1E_1=\epsilon_2E_2. Fringing is negligible.

Diagram shown in the original SVG worksheet.

  1. Find C in terms of C0=ϵ0A/dC_0=\epsilon_0A/d.

  2. At applied voltage V, find both fields and layer voltage drops.

Question 3 - Solution

Dielectric layers across the gap divide voltage inversely with permittivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V=QA(d/22ϵ0+d/26ϵ0)=Qd3ϵ0A.V=\frac QA\left(\frac{d/2}{2\epsilon_0}+\frac{d/2}{6\epsilon_0}\right)=\frac{Qd}{3\epsilon_0A}.C=3C0.C=3C_0.

(b) Interpretation and further calculation

E1=Q2ϵ0A=3V2d,E2=Q6ϵ0A=V2d.E_1=\frac{Q}{2\epsilon_0A}=\frac{3V}{2d},\quad E_2=\frac{Q}{6\epsilon_0A}=\frac{V}{2d}.V1=3V/4,V2=V/4.V_1=3V/4,\quad V_2=V/4.

Physical check

The lower-permittivity layer sustains the larger electric field and voltage drop.