Let there be a capacitor with charge "Q" , potential difference across it "V" and it's capacitance "C."
We have "Q=CV"
Also work done "W=VQ"
If the source delivers a small amount of charge "dQ" at a constant potential "V" , the work done "dW=dQ\\times V =\\frac{Q}{C}dQ"
Now the total work to deliver a charge "Q" is given by
"W=\\displaystyle\\int_{0}^{Q} \\frac{Q}{C}dQ=\\frac{Q^2}{2C}"
Work done =energy stored in the capacitor.
Substituting "Q=CV" in above equation we have,
Energy stored in capacitor "= E=\\frac{Q^2}{2C}=\\frac{1}{2} CV^2"
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