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Breaking ground on a new approach to construction
The drive to Kairos Power’s reactor demonstration site in Oak Ridge, Tenn., is not only scenic—it’s historic. Nearly 85 years ago, roughly 30,000 construction workers transformed orchards and farmland into a key Manhattan Project site. Depending on your route, you may pass by one of the three gatehouses that were once military checkpoints controlling access to Atomic Energy Commission production facilities.
Kanji Tasaka
Nuclear Science and Engineering | Volume 62 | Number 1 | January 1977 | Pages 167-174
Technical Note | doi.org/10.13182/NSE77-A26948
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Neutron capture effects on the decay power of fission products have been examined by varying the fissile nuclide, neutron spectrum, neutron flux, and irradiation and cooling times. Neutron capture transformations of fission products usually increase the decay power. However, at short cooling times, i.e., <C104 s, the capture effects are small, especially in a thermal reactor, where the negative contribution of135Xe offsets the positive contributions of other nuclides. The capture effect exhibits peaks at cooling times of 106 and 108 s and becomes negligible at 109 s. The former peak results mainly from the increases in the activities of103Ru, 134Cs, 136 Cs, 148Pm, 148Pm, and 156Eu, and the latter by activities of 134 Cs and 154Eu. The capture effect increases with increase of the flux level or irradiation time, and it is approximately proportional to the integrated flux at long cooling times. There is only a slight difference between the capture effect of two thermal reactors with epithermal indices of 0.1 and 0.2. In fast reactors, the effect is smaller than in thermal reactors at cooling times over 105 s, and depends only a little on the fissile nuclide. The decay power in fast reactors depends on the cross-section library selected to less than ∼ 1%.