Insulators — Question 6

Section 41-3 · Physics pages 6842–6843

Question 6 Breakdown field imposes a maximum dielectric energy density A linear dielectric has permittivity ε = 4.00 × 10−11 F/m and idealized breakdown field Eb = 2.00 × 107 V/m. A slab thickness is d = .200 mm. E d A Schematic; labels, not drawing lengths, specify the data. (a) Find the breakdown voltage and maximum electrostatic energy density. (b) Find the maximum energy for dielectric volume Vd = 1.00 cm3.
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Question 6 - Solution Breakdown field imposes a maximum dielectric energy density E d A (a) Method and calculation Vb = Ebd = 4.00 × 103 V . umax = 1 2εE2 b = 8.00 × 103 J/m3 . (b) Interpretation and further calculation Umax = umaxVd, 1 cm3 = 10−6 m3. Umax = 8.00 × 10−3 J . Physical check This ideal bulk-field limit omits defects and edge enhancement. It illustrates that thickness sets voltage capacity while energy per volume depends on permittivity and field.

Question 6

Breakdown field imposes a maximum dielectric energy density

A linear dielectric has permittivity ε=4.00×10−11F/m\varepsilon=4.00\times10^{-11}\,\mathrm{F/m} and idealized breakdown field Eb=2.00×107V/mE_b=2.00\times10^7\,\mathrm{V/m}. A slab thickness is d=.200mmd=.200\,\mathrm{mm}.

Diagram shown in the original SVG worksheet.

  1. Find the breakdown voltage and maximum electrostatic energy density.

  2. Find the maximum energy for dielectric volume Vd=1.00cm3V_d=1.00\,\mathrm{cm^3}.

Question 6 - Solution

Breakdown field imposes a maximum dielectric energy density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Vb=Ebd=4.00×103V.\boxed{V_b=E_bd=4.00\times10^3\,\mathrm V}.umax=12εEb2=8.00×103J/m3.\boxed{u_{\max}=\tfrac12\varepsilon E_b^2=8.00\times10^3\,\mathrm{J/m^3}}.

(b) Interpretation and further calculation

Umax=umaxVd,1cm3=10−6m3.U_{\max}=u_{\max}V_d,\quad1\,\mathrm{cm^3}=10^{-6}\,\mathrm{m^3}.Umax=8.00×10−3J.\boxed{U_{\max}=8.00\times10^{-3}\,\mathrm J}.

Physical check

This ideal bulk-field limit omits defects and edge enhancement. It illustrates that thickness sets voltage capacity while energy per volume depends on permittivity and field.