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General Kenneth Nichols and the Manhattan Project
Nichols
The Oak Ridger has published the latest in a series of articles about General Kenneth D. Nichols, the Manhattan Project, and the 1954 Atomic Energy Act. The series has been produced by Nichols’ grandniece Barbara Rogers Scollin and Oak Ridge (Tenn.) city historian David Ray Smith. Gen. Nichols (1907–2000) was the district engineer for the Manhattan Engineer District during the Manhattan Project.
As Smith and Scollin explain, Nichols “had supervision of the research and development connected with, and the design, construction, and operation of, all plants required to produce plutonium-239 and uranium-235, including the construction of the towns of Oak Ridge, Tennessee, and Richland, Washington. The responsibility of his position was massive as he oversaw a workforce of both military and civilian personnel of approximately 125,000; his Oak Ridge office became the center of the wartime atomic energy’s activities.”
A. Radkowsky, A. Galperin, T. Elperin
Nuclear Science and Engineering | Volume 79 | Number 1 | September 1981 | Pages 85-98
Technical Paper | doi.org/10.13182/NSE81-A19044
Articles are hosted by Taylor and Francis Online.
A careful study has been made of the effect of depletion of the fissile component of reactor fuel on the resonance component of the Doppler reactivity coefficient (DRC) for a lattice typical of a boiling water reactor (BWR). A parallel investigation has been carried out for both uranium- and thorium-based fuels. It is found that there are three principal effects, as follows, the first two of which tend to decrease the magnitude of the resonance component of the DRC and the third to increase it: direct competition of fission product absorption with that of the fertile isotopes overlapping of the fission product resonances with those of the fertile isotopes in uranium only, the formation of a large saturating resonance in 240Pu. As a result, in uranium-based fuels the resonance component of the DRC changes very little with depletion of the fissile isotope, while in thorium-based fuels there is a significant decrease in magnitude. Our results cannot be applied directly to a BWR since this would require consideration of the depletion history and void distribution over the entire core. The burnup selected for the uranium fuel was 35 000 MWd/ton, in line with current practice. In this material, effect 3 above is close to its maximum value while effects 1 and 2 increase with further burnup. Thus, it is also true that for extended burnup of uranium fuels, as are now being considered by the U.S. Department of Energy, the resonance component of the DRC is expected to decrease in magnitude.