Pulling Apart Isolated Capacitor Plates

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Electrostatics Intermediate Capacitor

Source: High school physics (Chinese)

Problem

A parallel-plate capacitor has plate area $S$, separation $d$, and carries charge $Q$. The capacitor is isolated (disconnected from any source), and the plate separation is then doubled.

  1. By how much does the electrostatic energy change?
  2. How much work do external forces do against the electric force on the plates?

(1) Energy increases by $\Delta W = \dfrac{Q^2 d}{2 \varepsilon_0 S}$. (2) $W_{\text{ext}} = \dfrac{Q^2 d}{2 \varepsilon_0 S}$.

Charge is fixed at $Q$. The capacitance changes from $C = \dfrac{\varepsilon_0 S}{d}$ to $C' = \dfrac{\varepsilon_0 S}{2d} = \dfrac{C}{2}$.

Energies (using $W = Q^2/(2C)$):

$$W_1 = \dfrac{Q^2}{2C} = \dfrac{Q^2 d}{2 \varepsilon_0 S}, \qquad W_2 = \dfrac{Q^2}{2 C'} = \dfrac{Q^2 d}{\varepsilon_0 S}.$$

(1) Change in electrostatic energy:

$$\Delta W = W_2 - W_1 = \dfrac{Q^2 d}{2 \varepsilon_0 S}.$$

(2) Since the system is isolated, no source supplies energy; the increase in stored electrostatic energy comes entirely from external work done against the attractive force between the oppositely charged plates:

$$W_{\text{ext}} = \Delta W = \dfrac{Q^2 d}{2 \varepsilon_0 S}.$$