Part of JES-02 — Electrostatic Potential, Capacitance & Energy

Dielectric Effects on Capacitors

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A dielectric is an insulating material that increases capacitance when placed between capacitor plates. Dielectric constant K = CwithCwithout\frac{C_with}{C_without} >= 1. Two scenarios must be distinguished:

Battery connected (V constant): Inserting dielectric increases C by K. Since V is fixed, Q = CV increases by K. E = Vd\frac{V}{d} stays the same. Energy U = \frac{1}{2}$$CV^2 increases by K. Extra energy comes from the battery.

Battery disconnected (Q constant): C increases by K. V = QC\frac{Q}{C} decreases by K. E = Vd\frac{V}{d} decreases by K. Energy U = Q^22C\frac{2}{2C} decreases by K. Lost energy goes into pulling the dielectric in (or is released as work).

The dielectric is pulled into the capacitor in both cases — this is because the system moves toward lower energy (battery off) or the battery supplies energy to increase the charge (battery on). Force on dielectric slab (partially inserted, battery on): F = 12\frac{1}{2}(K-1)epsilon0epsilon_0Ad\frac{A}{d}V2V^2 / L, where L is the plate length.

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