Physics

Physics

Problem

A parallel plate capacitor of capacity CC is connected to a battery of emf VV. The force between the plates is F0F_0. Now a dielectric slab of dielectric constant KK is inserted between the plates. The new force between the plates becomes FF. The relation between FF and F0F_0 is (A) F=K2F0F = K^2 F_0 (B) F=KF0F = K F_0 (C) F=F0K2F = \frac{F_0}{K^2} (D) F=F0F = F_0 (A) F=K2F0F = K^2 F_0 (B) F=KF0F = K F_0 (C) F=F0K2F = \frac{F_0}{K^2} (D) F=F0F = F_0
Intuitive explanation

The key insight is that the battery stays connected, so the voltage across the plates remains constant at VV. When you insert a dielectric, the capacitance increases by a factor of KK, which means more charge flows onto the plates from the battery. Since the attractive force between plates depends on the square of the charge (or equivalently, the square of the electric field), and the field strength increases by factor KK while voltage stays fixed, the force scales as K2K^2.

Intuitive explanation

The key insight is that the battery stays connected, so the voltage across the plates remains constant at VV. When you insert a dielectric, the capacitance increases by a factor of KK, which means more charge flows onto the plates from the battery. Since the attractive force between plates depends on the square of the charge (or equivalently, the square of the electric field), and the field strength increases by factor KK while voltage stays fixed, the force scales as K2K^2.

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