Using the equations presented previously and assuming that the nuclear fuel is Uranium-233 instead of Uranium-235, estimate the number of grams of U-233 that must be consumed per day to produce 1000 MWT of recoverable power.
From the equations presented previously, it can be seen that a 1000 MWT reactor will require a daily consumption rate of 1000 × 1.05(1 + α) = 1050(1 + α) g/day of whatever fissile material it uses. In the case of Uranium-233, the value for α (from Table 7.12) is 0.089, and therefore, 1050 (1 + 0.089) = 1143.45 g of Uranium-233 must be consumed to generate this amount of power for 1 day. This is equivalent to about 2.5 lbs of Uranium-233 consumed per day.
TABLE 7.12 | |||||
Fission Threshold Energy for the Most Common Heavy Elements in MeV | |||||
Isotope Name | Type of Nuclear Material |
Isotopic Rest Mass (AMU) |
Total Binding Energy of All Nucleons (MeV) |
Fission Threshold Energy (MeV) |
Binding Energy of Last Neutron (MeV) |
Th-232 | Fertile | 232.038051 | 5.9 | N/A^a | |
Th-233 | Fissionable | 6.5 | 5.1 | ||
U-233 | Fissile | 233.039628 | 1771.8 | 5.5 | N/A |
U-234 | Fissionable | 234.040947 | 1776.6 | 4.6 | 6.6 |
U-235 | Fissile | 235.043924 | 1783.9 | 5.75 | N/A |
U-236 | Fissionable | 236.045563 | 1790.4 | 5.3 | 6.4 |
U-238 | Fissionable | 236.050785 | 1801.7 | 5.85 | N/A |
U-239 | Fissionable | 239.05429 | 1806.5 | 5.5 | 4.9 |
Pu-239 | Fissile | 239.052158 | 1806.9 | 5.5 | N/A |
Pu-240 | Fissionable | 4.0 | 6.4 | ||
Source: L amarsh, J.R., Introduction to Nuclear Reactor Theory, second printing, Addison-Wesley Publishing Company, Inc., Reading, MA, 1972. |