Pulling Apart Capacitor Plates at Constant Voltage

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Electrostatics Intermediate Capacitor

Source: High school physics (Chinese)

Problem

A parallel-plate capacitor with plate area $S$ and separation $d$ is connected to a constant-voltage source of voltage $U$. With the source remaining connected, the plate separation is doubled.

  1. By how much does the electrostatic energy stored in the capacitor change?
  2. How much energy is returned to the source during this process?
  3. How much work do external forces do against the electric force on the plates?

(1) $\Delta W = -\dfrac{\varepsilon_0 S U^2}{4d}$ (capacitor energy decreases). (2) $W_{\text{returned}} = \dfrac{\varepsilon_0 S U^2}{2d}$. (3) $W_{\text{ext}} = \dfrac{\varepsilon_0 S U^2}{4d}$.

The voltage is fixed at $U$. The capacitance halves ($C \to C/2$), so the charge halves and the energy halves.

Initial: $C = \dfrac{\varepsilon_0 S}{d}$, $W_1 = \tfrac{1}{2} C U^2 = \dfrac{\varepsilon_0 S U^2}{2d}$, $Q_1 = CU = \dfrac{\varepsilon_0 S U}{d}$.

Final: $C' = \dfrac{C}{2}$, $W_2 = \tfrac{1}{2} C' U^2 = \dfrac{\varepsilon_0 S U^2}{4d}$, $Q_2 = C' U = \dfrac{Q_1}{2}$.

(1) Change in capacitor energy:

$$\Delta W = W_2 - W_1 = -\dfrac{\varepsilon_0 S U^2}{4d} \quad (\text{decreases}).$$

(2) Charge $|\Delta Q| = Q_1 - Q_2 = \dfrac{\varepsilon_0 S U}{2d}$ flows back to the source. The energy returned is:

$$W_{\text{returned}} = U |\Delta Q| = \dfrac{\varepsilon_0 S U^2}{2d}.$$

(3) Energy balance (no dissipation): $W_{\text{ext}} + W_{\text{source}\to\text{cap}} = \Delta W$, with $W_{\text{source}\to\text{cap}} = -W_{\text{returned}} = -\dfrac{\varepsilon_0 S U^2}{2d}$. Hence:

$$W_{\text{ext}} = \Delta W - W_{\text{source}\to\text{cap}} = -\dfrac{\varepsilon_0 S U^2}{4d} + \dfrac{\varepsilon_0 S U^2}{2d} = \dfrac{\varepsilon_0 S U^2}{4d}.$$