Energy Stored in an Electric Field — Question 2

Section 25-4 · Physics pages 4074–4075

Question 2 An isolated plate capacitor resists separation with a constant ideal force A vacuum parallel-plate capacitor has area A, gap d and fixed charges ±Q. Neglect fringing and allow the gap to increase quasistatically. A B d +d Ideal plate cross-section; fringing is neglected unless stated. (a) Express U(d) and find the electric force conjugate to increasing d. (b) Find external work to double d and compare the force with the field of the opposite plate acting on Q.
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Question 2 - Solution An isolated plate capacitor resists separation with a constant ideal force A B d +d (a) Method and calculation C = ϵ0A/d, U = Q2 2C = Q2d 2ϵ0A. Fd = − (∂U ∂d ) Q = −Q2 2ϵ0A. (b) Interpretation and further calculation Wext = U(2d) −U(d) = Q2d 2ϵ0A. Eother = Q 2ϵ0A ⇒|F| = QEother = Q2 2ϵ0A. Physical check A plate does not exert a net force on itself; using the full gap field in QE would double the correct force.

Question 2

An isolated plate capacitor resists separation with a constant ideal force

A vacuum parallel-plate capacitor has area A, gap d and fixed charges ±Q\pm Q. Neglect fringing and allow the gap to increase quasistatically.

Diagram shown in the original SVG worksheet.

  1. Express U(d) and find the electric force conjugate to increasing d.

  2. Find external work to double d and compare the force with the field of the opposite plate acting on Q.

Question 2 - Solution

An isolated plate capacitor resists separation with a constant ideal force

Diagram shown in the original SVG worksheet.

(a) Method and calculation

C=ϵ0A/d,U=Q22C=Q2d2ϵ0A.C=\epsilon_0A/d,\quad U=\frac{Q^2}{2C}=\frac{Q^2d}{2\epsilon_0A}.Fd=−(∂U∂d)Q=−Q22ϵ0A.F_d=-\left(\frac{\partial U}{\partial d}\right)_Q=-\frac{Q^2}{2\epsilon_0A}.

(b) Interpretation and further calculation

Wext=U(2d)−U(d)=Q2d2ϵ0A.W_{\mathrm{ext}}=U(2d)-U(d)=\frac{Q^2d}{2\epsilon_0A}.Eother=Q2ϵ0A⇒|F|=QEother=Q22ϵ0A.E_{\mathrm{other}}=\frac{Q}{2\epsilon_0A}\Rightarrow |F|=QE_{\mathrm{other}}=\frac{Q^2}{2\epsilon_0A}.

Physical check

A plate does not exert a net force on itself; using the full gap field in QE would double the correct force.