(c) On sharing of charges loss in electrical energy,
$\Delta U = \frac{C_{1}C_{2}}{2\left( C_{1}{+ C}_{2} \right)}\left( V_{1} - V_{2} \right).$ In present case $C_{1} = C_{2} = C_{\ }$
$\therefore\ \Delta U = \frac{C^{2}}{2(2C)}\ \left( V_{1} - V_{2} \right)^{2} = \frac{1}{4}C\left( V_{1} - V_{2} \right)^{2}$