Question #133842

given that fuel grade uranium contains 4% fissile material (235U) that the fissile material is completely utilised that 200MeV (1eV=1.6× 10^-19 J) of thermal energy is released during fission of a single 235U nucleus and that the thermal to electrical conversion of efficiency is 33% the annual requirement of fuel grade uranium for round the clock operation of a 1000MW nuclear power plant would be

Expert's answer

Let's denote MM as fuel grade uranium.

We know the mass of 235U is 0.04M0.04M. We need to calculate how many U-235 nucleus are inside of this mass.

N=0.04M235NA=0.04M235⋅6.02⋅1023=1.025⋅1020MN = \frac{0.04M}{235} N_A = \frac{0.04M}{235}\cdot 6.02 \cdot 10^{23}= 1.025\cdot 10^{20} M

These nucleus will produce

E=1.025⋅1020M⋅200  MeV=1.025⋅1020⋅200⋅106⋅1.6⋅10−19⋅M    J=E= 1.025 \cdot 10^{20} M \cdot 200 \; MeV = 1.025 \cdot 10^{20} \cdot 200 \cdot 10^{6} \cdot 1.6 \cdot 10^{-19} \cdot M \; \;J =

=328⋅107M    J= 328 \cdot 10^7 M \; \; J

This energy should be equal to ϵEt=0.33⋅1000  MW⋅1  year=330⋅106⋅31  556  926  J≈1.043⋅1016  J\epsilon \mathcal{E} t = 0.33 \cdot1000\; MW \cdot 1 \; year= 330 \cdot 10^6 \cdot 31\; 556\; 926 \; J \approx 1.043 \cdot 10^{16} \; J

So,

327⋅107M=1.043⋅1016327 \cdot 10^7 M = 1.043 \cdot 10^{16}

M=3.2⋅106  g=3.2⋅103  kg.M = 3.2 \cdot 10^{6} \; g = 3.2 \cdot 10^{3} \; kg.


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