Step 1: Key Formula:
The capacitance (C) of a parallel plate capacitor with plate area A, distance between plates d, and vacuum (or air) between the plates is given by the formula:
\[ C = \frac{\epsilon_0 A}{d} \]
where \(\epsilon_0\) is the permittivity of free space. We will use this formula as the baseline for all three cases.
Step 2: Analysis of each case:
(i) Distance between the plates is doubled.
The initial capacitance is \( C = \frac{\epsilon_0 A}{d} \).
The new distance is \( d' = 2d \).
The new capacitance, \( C' \), will be:
\[ C' = \frac{\epsilon_0 A}{d'} = \frac{\epsilon_0 A}{2d} = \frac{1}{2} \left( \frac{\epsilon_0 A}{d} \right) = \frac{1}{2} C \]
Effect: The capacitance is halved.
(ii) Area of the plates is halved.
The initial capacitance is \( C = \frac{\epsilon_0 A}{d} \).
The new area is \( A' = A/2 \).
The new capacitance, \( C' \), will be:
\[ C' = \frac{\epsilon_0 A'}{d} = \frac{\epsilon_0 (A/2)}{d} = \frac{1}{2} \left( \frac{\epsilon_0 A}{d} \right) = \frac{1}{2} C \]
Effect: The capacitance is halved.
(iii) A dielectric medium is filled between the plates.
When a dielectric medium of dielectric constant K is completely filled between the plates, the capacitance formula becomes:
\[ C' = \frac{K \epsilon_0 A}{d} \]
Since the original capacitance was \( C = \frac{\epsilon_0 A}{d} \), we can write:
\[ C' = K . C \]
For any dielectric medium, the dielectric constant K is always greater than 1 (\(K>1\)).
Effect: The capacitance increases by a factor of K.