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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.”
Glenn T. Sager, George H. Miley, Keith H. Burrell
Fusion Science and Technology | Volume 18 | Number 3 | November 1990 | Pages 389-396
Alpha Particles in Fusion Research | Technical Paper | doi.org/10.13182/FST90-A29272
Articles are hosted by Taylor and Francis Online.
Neoclassical transport of minority suprathernial alpha particles is investigated. This work departs from previous investigations in that (a) the banana-width ordering parameter ρθ/L is not formally restricted to be a small parameter and (b) a linearized collision operator that retains the effects of pitch-angle scattering, electron and ion drag, and speed diffusion is used. A step model approximation for the large-aspect-ratio, circular-cross-section tokamak magnetic field is adopted to simplify the orbit-averaging procedure. Assuming that the suprathermal alphas are in the banana regime, an asymptotic expansion in τB/τs ≪ 1 is carried out. The lowest order distribution is independent of poloidal angle on a drift surface and is completely determined by solving an orbit-averaged drift kinetic equation, A variational problem is derived that is equivalent to this three-dimensional, inhomogeneous differential equation. A similar procedure yields an expression for the first-order component f1. Knowledge of f1 is sufficient to obtain expressions for particle and heat fluxes directly from the definitions or from alternate expressions. Extension of this model to account for loss regions in phase space is outlined.