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Nuclear Nonproliferation Policy
The mission of the Nuclear Nonproliferation Policy Division (NNPD) is to promote the peaceful use of nuclear technology while simultaneously preventing the diversion and misuse of nuclear material and technology through appropriate safeguards and security, and promotion of nuclear nonproliferation policies. To achieve this mission, the objectives of the NNPD are to: Promote policy that discourages the proliferation of nuclear technology and material to inappropriate entities. Provide information to ANS members, the technical community at large, opinion leaders, and decision makers to improve their understanding of nuclear nonproliferation issues. Become a recognized technical resource on nuclear nonproliferation, safeguards, and security issues. Serve as the integration and coordination body for nuclear nonproliferation activities for the ANS. Work cooperatively with other ANS divisions to achieve these objective nonproliferation policies.
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ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
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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. L. Kaplan
Nuclear Science and Engineering | Volume 27 | Number 2 | February 1967 | Pages 388-393
Technical Paper | doi.org/10.13182/NSE67-A18277
Articles are hosted by Taylor and Francis Online.
Attenuation by a floor barrier of fallout gamma radiation scattered into a basement has been studied experimentally with cylindrical steel structures. These structures were 2-ft high, 2-ft in diameter, with a 4-ft-deep basement. Wall thicknesses varied between 5 and 60 psf, with floor thicknesses of 0, 10, 20, and 40 psf. Detectors in the basement were located between 0.25 and 3 ft below ground. Cobalt-60 point sources were used to simulate the fallout field. Basement reduction factors predicted by structure shielding theory were lower than the experimental results by a factor of between 1.5 and 8. This discrepancy was attributed to the theoretical floor-barrier reduction factor. A new theoretical floor-barrier reduction factor, which is a function of both the floor thickness and the solid-angle fraction subtended at the detector by the floor, was constructed within the formalism of the existing structure shielding theory. This new function agreed quite well with both experimental results and Monte Carlo calculations, over the entire range of wall and floor thicknesses used in the experiment.