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Hey, David
I think I'm missing the point as well. Are you implying that the firs=
t charges arriving at the uncharged capacitor have CV^2 of energy? Si=
nce there is no potential difference across the capacitor at that tim=
e, it requires essentially zero work (in the absence of dissipative c=
oncerns) to put them on the plates. As time goes on the capacitor's p=
otential difference rises to some final value V determined by the cha=
racteristics of the device (C) and the amount of charge stored on its=
plates. Since the charge of the "full" capacitor will equal CV, and =
the average potential difference across it will be (V+0)/2, the store=
d energy, equal to the work done in charging, it will be CV*V/2, or 1=
/2CV^2. Where's the missing energy?