(N/A) Total electric power target, $P = 2 \times 10^{5} \; MW = 2 \times 10^{11} \; W$.
Nuclear power required, $P_{n} = 10\% \text{ of } P = 0.1 \times 2 \times 10^{11} = 2 \times 10^{10} \; J/s$.
Total energy required per year, $E_{total} = P_{n} \times (365 \times 24 \times 3600) \; s = 2 \times 10^{10} \times 3.1536 \times 10^{7} = 6.3072 \times 10^{17} \; J$.
Energy per fission, $E_{f} = 200 \; MeV = 200 \times 10^{6} \times 1.6 \times 10^{-19} \; J = 3.2 \times 10^{-11} \; J$.
Efficiency of reactor, $\eta = 25\% = 0.25$.
Useful energy per fission, $E_{u} = \eta \times E_{f} = 0.25 \times 3.2 \times 10^{-11} = 8 \times 10^{-12} \; J$.
Number of fissions required per year, $N = \frac{E_{total}}{E_{u}} = \frac{6.3072 \times 10^{17}}{8 \times 10^{-12}} = 7.884 \times 10^{28} \; \text{atoms}$.
Mass of $1 \; \text{mole}$ of $^{235}U = 235 \; g = 0.235 \; kg$.
Number of atoms in $1 \; \text{mole} = 6.023 \times 10^{23}$.
Mass of uranium required, $M = \frac{N}{N_{A}} \times 0.235 = \frac{7.884 \times 10^{28}}{6.023 \times 10^{23}} \times 0.235 \approx 3.076 \times 10^{4} \; kg$.