Assume a parallel-plate capacitor, of plate area A and plate separation d is filled with a dielectric of relative permittivity (dielectric constant) k. Its capacitance is C = \(\frac{k \varepsilon_{0} A}{d}\) ......... (1)
If it is charged to a voltage (potential) V, the charge on its plates is Q = CV.
Since the battery is disconnected after it is charged, the charge Q on its plates, and consequently the product CV, remain unchanged.
On removing the dielectric completely, its capacitance becomes from Eq. (1),
C' = \(\frac{\varepsilon_{0} A}{d}=\frac{1}{k} C\) ............. (2)
that is, its capacitance decreases by the factor k. Since C'V' = CV, its new voltage is
V' = \(\frac{C}{C^{\prime}}\) V = kV ........(3)
so that its voltage increases by the factor k. The stored potential energy, U = \(\frac{1}{2}\) QV, so that Q remaining constant, U increases by the factor k. The electric field, E = V/ d, so that E also increases by a factor k.