Two parallel plate capacitors of capacitances C and 2C are connected in parallel and charged to a potential difference V0. The battery is then disconnected and the region between the plates of the capacitor C is completely filled with a material of dielectric constant 2. The potential difference across the capacitors now becomes:
∵ Capacitors are in parallel
∴Q1C=Q22C
⇒Q2=2Q1……(i)
V0=Q22C
After disconnecting the battery and inserting the dielectric in C.
V′1=Q′1CK=Q′12C
V′2=Q′22C
Charge will flow from 2 to 1 till Q′22C=Q′12C; i.e., till the two potentials are equal
Q′1=Q′2
Earlier potentials V0=Q1C
Now it is Q′12C
Q1+Q2=3Q1=Q′1+Q′2
Q′22C=Q′12C or Q′2=Q′1=3Q12
∴ New potential =3Q14Cor3V04