Thus when a dielectric is inserted in a charged capacitor (not connected to a power supply), the electric field would be decreased and so would the voltage (=Ed). Since C=QV, this means that C must be bigger when a dielectric is inserted.
For a parallel-plate capacitor containing a dielectric, the capacitance is:
C=kϵ0Ad
Where k is the dielectric constant.
In general, adding a dielectric to a capacitor increases the capacitance by a factor of k.