Capacitor with a Dielectric — Question 5

Section 25-5 · Physics pages 4100–4101

Question 5 A partial-thickness insertion can identify an unknown permittivity A dielectric slab of thickness t=.600d fills the plate area but leaves vacuum in the rest of the gap. The measured capacitance doubles relative to the empty capacitor C0. Neglect fringing. A B d t Ideal plate cross-section; fringing is neglected unless stated. (a) Derive the effective-gap expression for capacitance. (b) Infer the dielectric relative permittivity and check that it is physically consistent with the measured ratio.
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Question 5 - Solution A partial-thickness insertion can identify an unknown permittivity A B d t (a) Method and calculation V = Q ϵ0A ( d −t + t κ ) . C C0 = d d −t + t/κ = 1 1 −f + f/κ, f = t/d. (b) Interpretation and further calculation 1 2 = .400 + .600 κ ⇒κ = 6.00. 1 < C/C0 < 1/(1 −f) = 2.50, so the observed ratio 2 lies in the finite-positive-permittivity range for κ > 1. Physical check A slab with arbitrarily high permittivity cannot remove the voltage drop across the remaining vacuum.

Question 5

A partial-thickness insertion can identify an unknown permittivity

A dielectric slab of thickness t=.600d fills the plate area but leaves vacuum in the rest of the gap. The measured capacitance doubles relative to the empty capacitor C0. Neglect fringing.

Diagram shown in the original SVG worksheet.

  1. Derive the effective-gap expression for capacitance.

  2. Infer the dielectric relative permittivity and check that it is physically consistent with the measured ratio.

Question 5 - Solution

A partial-thickness insertion can identify an unknown permittivity

Diagram shown in the original SVG worksheet.

(a) Method and calculation

V=Qϵ0A(d−t+tκ).V=\frac{Q}{\epsilon_0A}\left(d-t+\frac t\kappa\right).CC0=dd−t+t/κ=11−f+f/κ,f=t/d.\frac C{C_0}=\frac d{d-t+t/\kappa}=\frac1{1-f+f/\kappa},\quad f=t/d.

(b) Interpretation and further calculation

12=.400+.600κ⇒κ=6.00.\frac12=.400+\frac{.600}{\kappa}\Rightarrow\kappa=6.00.1<C/C0<1/(1−f)=2.50,1<C/C_0<1/(1-f)=2.50,so the observed ratio 2 lies in the finite-positive-permittivity range for κ>1\kappa>1.

Physical check

A slab with arbitrarily high permittivity cannot remove the voltage drop across the remaining vacuum.