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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.”
Peter Mioduszewski
Fusion Science and Technology | Volume 32 | Number 2 | September 1997 | Pages 277-286
Technical Paper | First-Wall Technology | doi.org/10.13182/FST97-A19897
Articles are hosted by Taylor and Francis Online.
The purpose of a volumetric neutron source is the development and testing of the nuclear components of a fusion reactor. The main issue in this case is very long pulse operation, such as 2 weeks at a time, to elicit the nuclear effects to be studied. Operation at this pulse length will cause extreme erosion if the edge plasma cannot be tailored appropriately. Typical erosion rates that can be expected at some of the plasma-facing components such as the divertor target or the divertor baffles, without specifying a particular type of device, are analyzed. Accurate predictions of erosion and redeposition require not only knowledge of the erosion mechanism but also detailed knowledge of the plasma parameters, plasma flows, and their spatial distributions, as well as temperature distributions of plasma-facing components and other parameters. It is, therefore, a very difficult task to predict erosion/redeposition rates and patterns for future machines. Nevertheless, some estimate is needed of expected erosion rates, crude as they may be, so future machines for long-pulse operation can be designed. For that purpose, physical sputtering is examined only as a basis for erosion estimates and does not take into account the important processes of chemical sputtering and radiation-enhanced sublimation or the complicated redeposition processes. Even with this simplified approach, one can grasp the order of magnitude of erosion rates that will be encountered when a plasma device is operated for long pulses and at high-duty cycles.