Insulators — Question 3

Section 41-3 · Physics pages 6836–6837

Question 3 A leaky dielectric gives a geometry-independent discharge time A parallel-plate capacitor is filled by a uniform dielectric of permittivity ε and finite conductivity σ. Plate area is A, separation d, and edge effects are negligible. The source is disconnected after charging. ε, σ d Schematic; labels, not drawing lengths, specify the data. (a) Find capacitance and leakage resistance. (b) Derive the voltage-decay time constant and explain why changing A or d does not change it.
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Question 3 - Solution A leaky dielectric gives a geometry-independent discharge time ε, σ d (a) Method and calculation C = εA/d, Rℓ= d/(σA) . Iℓ= V/Rℓ, C ˙V = −Iℓ⇒˙V = −V/(RℓC). (b) Interpretation and further calculation V (t) = V0e−t/τ, τ = RℓC = ε/σ . ∂τ/∂A = ∂τ/∂d = 0 (ε, σ fixed). Physical check The cancellation applies to bulk leakage through the same homogeneous dielectric that sets capacitance. Surface leakage or an external resistor need not share it.

Question 3

A leaky dielectric gives a geometry-independent discharge time

A parallel-plate capacitor is filled by a uniform dielectric of permittivity ε\varepsilon and finite conductivity σ\sigma. Plate area is A, separation d, and edge effects are negligible. The source is disconnected after charging.

Diagram shown in the original SVG worksheet.

  1. Find capacitance and leakage resistance.

  2. Derive the voltage-decay time constant and explain why changing A or d does not change it.

Question 3 - Solution

A leaky dielectric gives a geometry-independent discharge time

Diagram shown in the original SVG worksheet.

(a) Method and calculation

C=εA/d,Rℓ=d/(σA).\boxed{C=\varepsilon A/d,\quad R_\ell=d/(\sigma A)}.Iℓ=V/Rℓ,CV̇=−Iℓ⇒V̇=−V/(RℓC).I_\ell=V/R_\ell,\quad C\dot V=-I_\ell\Rightarrow\dot V=-V/(R_\ell C).

(b) Interpretation and further calculation

V(t)=V0e−t/τ,τ=RℓC=ε/σ.\boxed{V(t)=V_0e^{-t/\tau},\quad\tau=R_\ell C=\varepsilon/\sigma}.∂τ/∂A=∂τ/∂d=0(ε,σ fixed).\boxed{\partial\tau/\partial A=\partial\tau/\partial d=0}\quad(\varepsilon,\sigma\text{ fixed}).

Physical check

The cancellation applies to bulk leakage through the same homogeneous dielectric that sets capacitance. Surface leakage or an external resistor need not share it.