Capacitance of a Parallel Plate Capacitor with Partial Dielectric Slab:
Consider a parallel plate capacitor with plate area \( A \) and separation \( d \) between the plates. Let the capacitor be partially filled with a dielectric material of dielectric constant \( \varepsilon_r \) and thickness \( t \). The remaining gap is filled with air.
The total capacitance can be considered as the combination of two capacitors in series:
1. The capacitor with dielectric slab: Capacitance \( C_1 \),
2. The capacitor with air gap: Capacitance \( C_2 \).
1. Capacitance with dielectric slab:
The capacitance of the part filled with the dielectric is given by:
\[
C_1 = \frac{\varepsilon_r \varepsilon_0 A}{t}.
\]
2. Capacitance with air gap:
The capacitance of the part filled with air is given by:
\[
C_2 = \frac{\varepsilon_0 A}{d - t}.
\]
3. Total Capacitance (Series Combination):
Since the two capacitors are in series, the total capacitance \( C \) is given by:
\[
\frac{1}{C} = \frac{1}{C_1} + \frac{1}{C_2}.
\]
Substituting the expressions for \( C_1 \) and \( C_2 \):
\[
\frac{1}{C} = \frac{t}{\varepsilon_r \varepsilon_0 A} + \frac{d - t}{\varepsilon_0 A}.
\]
Simplifying the expression:
\[
\frac{1}{C} = \frac{d}{\varepsilon_0 A}.
\]
Thus, the total capacitance is:
\[
C = \frac{\varepsilon_0 A}{d}.
\]
So, the capacitance of a parallel plate capacitor with a partial dielectric filling is the same as that of an empty capacitor, but with the dielectric slab affecting the effective area.