Capacitor with a Dielectric — Question 1

Section 25-5 · Physics pages 4092–4093

Question 1 Inserting dielectric into an isolated capacitor lowers voltage and stored energy An isolated plate capacitor initially has capacitance C0, voltage V0 and energy U0. A linear lossless dielectric with relative permittivity 3 fills the gap quasistatically. The terminals remain disconnected. A B d κ Ideal plate cross-section; fringing is neglected unless stated. (a) Find final capacitance, charge and voltage. (b) Find final energy and external insertion work, neglecting friction and material deformation.
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Question 1 - Solution Inserting dielectric into an isolated capacitor lowers voltage and stored energy A B d κ (a) Method and calculation Cf = 3C0, Qf = Q0 = C0V0. Vf = Q0/Cf = V0/3. (b) Interpretation and further calculation Uf = Q2 0/(2Cf) = U0/3. Wext = ∆U = −2U0/3. Physical check The field pulls the dielectric inward, so an agent maintaining quasistatic motion extracts energy.

Question 1

Inserting dielectric into an isolated capacitor lowers voltage and stored energy

An isolated plate capacitor initially has capacitance C0, voltage V0 and energy U0. A linear lossless dielectric with relative permittivity 3 fills the gap quasistatically. The terminals remain disconnected.

Diagram shown in the original SVG worksheet.

  1. Find final capacitance, charge and voltage.

  2. Find final energy and external insertion work, neglecting friction and material deformation.

Question 1 - Solution

Inserting dielectric into an isolated capacitor lowers voltage and stored energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Cf=3C0,Qf=Q0=C0V0.C_f=3C_0,\quad Q_f=Q_0=C_0V_0.Vf=Q0/Cf=V0/3.V_f=Q_0/C_f=V_0/3.

(b) Interpretation and further calculation

Uf=Q02/(2Cf)=U0/3.U_f=Q_0^2/(2C_f)=U_0/3.Wext=ΔU=−2U0/3.W_{\mathrm{ext}}=\Delta U=-2U_0/3.

Physical check

The field pulls the dielectric inward, so an agent maintaining quasistatic motion extracts energy.