Both nuclear fission and nuclear fusion are considered for large-scale energy generation

PHYSICS · Multi-part · A Level · Physics · Nuclear physics · Nuclear physics

Problem

Both nuclear fission and nuclear fusion are considered for large-scale energy generation. The fusion reaction 12H+13H→24He+n^2_1\text{H}+^3_1\text{H}\rightarrow {}^4_2\text{He}+n releases 17.6 MeV17.6\,\text{MeV} of energy per event. Assume molar masses M2 ⁣H=2 g mol−1M_{^2\!H}=2\,\text{g\,mol}^{-1}, M3 ⁣H=3 g mol−1M_{^3\!H}=3\,\text{g\,mol}^{-1} and M235 ⁣U=235 g mol−1M_{^{235}\!U}=235\,\text{g\,mol}^{-1}. Use NA=6.022×1023 mol−1N_A = 6.022\times10^{23}\,\text{mol}^{-1} and 1 eV=1.6×10−19 J1\,\text{eV}=1.6\times10^{-19}\,\text{J}. (i) A mixture contains equal numbers of deuterium and tritium nuclei. Calculate the energy obtainable when a total mass of 1.0 g1.0\,\text{g} of this mixture undergoes complete fusion. (ii) Determine the energy released when 1.0 g1.0\,\text{g} of 235U^{235}\text{U} undergoes complete fission, each fission event releasing 200 MeV200\,\text{MeV}. (iii) Find the ratio of the energies obtained per gram from the fusion fuel and from 235U^{235}\text{U}, respectively. Comment briefly on the result.

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