In a nuclear reactor, energy is produced by the following process:
1H2+1H2→1H3+P1H3+1H2→2He4+n
The reactor produces a power of 1010 MW with 50% efficiency. The number of deutrons required to run the reactor for one year will be apporoximately: m(12H) = 2.014 u. m(p) = 1.007 u. m(n) = 1.008u. m(2He4) = 4.00 1u
5×1035
For each reaction involving both the processes, mass defect
=3×2.014−4.001−1.007=0.028u
Energy released per deutron =931.5×0.0283MeV
Let n be the number of deutrons required
Total energy −931.5×0.0263×nMeV−P×tη−1016×365×24×60×600.5
n=5×1035