Insulators — Question 7

Section 41-3 · Physics pages 6844–6845

Question 7 Series dielectric layers concentrate the electric field in the lower permittivity Two planar insulating layers in series have thicknesses d1 = d2 = d and permittivities ε1 = 2ε0, ε2 = 6ε0. There is no free interface charge. Apply total voltage V normal to the layers. 2ε0 6ε0 Schematic; labels, not drawing lengths, specify the data. (a) Find both fields in terms of V and d. (b) If both materials have breakdown field Eb, find the total voltage at first breakdown and both voltage fractions.
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Question 7 - Solution Series dielectric layers concentrate the electric field in the lower permittivity 2ε0 6ε0 (a) Method and calculation D = ε1E1 = ε2E2 ⇒E1 = 3E2. V = d(E1 + E2) ⇒E1 = 3V/(4d), E2 = V/(4d) . (b) Interpretation and further calculation E1 = Eb ⇒Vmax = 4dEb/3 . V1/V = 3/4, V2/V = 1/4, E2 = Eb/3 at first breakdown . Physical check Continuity applies to normal displacement D in the absence of free interface charge, not to E. The lower-permittivity layer reaches the common breakdown field first.

Question 7

Series dielectric layers concentrate the electric field in the lower permittivity

Two planar insulating layers in series have thicknesses d1=d2=dd_1=d_2=d and permittivities ε1=2ε0\varepsilon_1=2\varepsilon_0, ε2=6ε0\varepsilon_2=6\varepsilon_0. There is no free interface charge. Apply total voltage V normal to the layers.

Diagram shown in the original SVG worksheet.

  1. Find both fields in terms of V and d.

  2. If both materials have breakdown field EbE_b, find the total voltage at first breakdown and both voltage fractions.

Question 7 - Solution

Series dielectric layers concentrate the electric field in the lower permittivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

D=ε1E1=ε2E2⇒E1=3E2.D=\varepsilon_1E_1=\varepsilon_2E_2\Rightarrow E_1=3E_2.V=d(E1+E2)⇒E1=3V/(4d),E2=V/(4d).V=d(E_1+E_2)\Rightarrow\boxed{E_1=3V/(4d),\quad E_2=V/(4d)}.

(b) Interpretation and further calculation

E1=Eb⇒Vmax=4dEb/3.E_1=E_b\Rightarrow\boxed{V_{\max}=4dE_b/3}.V1/V=3/4,V2/V=1/4,E2=Eb/3 at first breakdown.\boxed{V_1/V=3/4,\quad V_2/V=1/4,\quad E_2=E_b/3\text{ at first breakdown}}.

Physical check

Continuity applies to normal displacement D in the absence of free interface charge, not to E. The lower-permittivity layer reaches the common breakdown field first.