By energy stored in a charged conductor Suppose, a conductor of capacity C is charged to a potential V and Q the charge on conductor at a instant.
The potential of the conductor V=CQ
Now, work done in bringing a small charge dQ at this potential is, dW=VdQ=CQdQ ∴ Total work done in charging it from 0 to Q is, W=0∫QdW=0∫QCQdQ =21CQ2
This work is stored as the potential energy, U=21CQ2(∵Q=VC) U=21CV2=21QV