Step 1: Recall the formula for the capacitance of a parallel-plate capacitor.
The capacitance \(C_0\) of a parallel-plate capacitor with plate area \(A\) and separation \(d\), filled with vacuum, is:
\[ C_0 = \frac{\epsilon_0 A}{d} \]
where \(\epsilon_0\) is the permittivity of free space.
Step 2: Recall the effect of inserting a dielectric material.
When a dielectric material with dielectric constant \(K\) is inserted to completely fill the space between the plates, the permittivity of the space becomes \(\epsilon = K \epsilon_0\).
Step 3: Write the formula for the new capacitance.
The new capacitance \(C\) with the dielectric slab is:
\[ C = \frac{K \epsilon_0 A}{d} \]
Step 4: Compare the new capacitance with the original capacitance.
\[ C = K \left( \frac{\epsilon_0 A}{d} \right) = K C_0 \]
Thus, the capacitance increases by a factor of K. Since the dielectric constant \(K\) is always greater than 1 for materials, the capacitance always increases.