For thermal neutrons calculate \overline{η} as a function of uranium enrichment and plot your results. Use the uranium data from the following table:
\nu | \sigma_{f}\ ({\mathrm{barns}}) | \sigma_{\alpha}\ ({\mathrm{barns}}) | |
Uranium-235 | 2.43 | 505 | 591 |
Plutonium-239 | 2.90 | 698 | 973 |
Uranium-238 | — | 0 | 2.42 |
We have \overline{{{\eta}}}=\frac{(\nu N\sigma_{f})^{25}}{(N\sigma_{a})^{25}+(N\sigma_{a})^{28}} =\frac{\nu^{25}\sigma_{f}^{\ 25}}{\sigma_{a}^{\ 25}}\frac{1}{1+(N^{28}/N^{25})\sigma_{a}^{28}/\sigma_{a}^{\ 25}}
Since the enrichment is \tilde{e}=N^{25}/(N^{25}+N^{28}) we have
\overline{{{\eta}}}=\frac{\nu^{25}{\sigma_{f}}^{ 25}}{{\sigma_{a}}^{ 25}}\frac{1}{{{1+(\hat{e}^{-1}-1){\sigma_{\!a}^{ 28}}\,/\,{\sigma_{\!a}^{\ 25}}}}}\, = 2.08{\frac{1}{1+0.00409\cdot({\hat{e}}^{-1}-1)}}