The capacitance \( C \) of a parallel plate capacitor without any dielectric between its plates is given by:
\[
C_0 = \frac{\epsilon_0 A}{d}
\]
where \( \epsilon_0 \) is the permittivity of free space, \( A \) is the area of one plate, and \( d \) is the separation between the plates.
When a dielectric medium with dielectric constant \( K \) is introduced between the plates, the capacitance increases by a factor of \( K \), because the dielectric reduces the effective electric field within the capacitor while maintaining the same charge. Thus, the new capacitance \( C \) is given by:
\[
C = KC_0 = K \frac{\epsilon_0 A}{d}
\]
This expression shows that the capacitance of a parallel plate capacitor is directly proportional to the dielectric constant of the medium between the plates, the permittivity of free space, and the area of the plates, and inversely proportional to the distance between the plates.