Answer:
[tex]\frac{Q}{Q_0}=1[/tex]
Explanation:
Capacitance is defined as the charge divided in voltage.
[tex]C=\frac{Q}{V}(1)[/tex]
Introducing a dielectric into a parallel plate capacitor decreases its electric field. Therefore, the voltage decreases, as follows:
[tex]V=\frac{V_0}{k}[/tex]
Where k is the dielectric constant and [tex]V_0[/tex] the voltage of the capacitor without a dielectric
The capacitance with a dielectric between the capacitor plates is given by:
[tex]C=kC_0[/tex]
Where k is the dielectric constant and [tex]C_0[/tex] the capacitance of the capacitor without a dielectric. So, we have:
[tex]Q=CV\\Q=kC_0\frac{V_0}{k}\\Q=C_0V_0\\Q_0=C_0V_0\\Q=Q_0\\\frac{Q}{Q_0}=1[/tex]
Therefore, a capacitor with a dielectric stores the same charge as one without a dielectric.