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Fusion Science and Technology
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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.”
T. J. Dolan*
Fusion Science and Technology | Volume 16 | Number 2 | September 1989 | Pages 149-156
Technical Paper | Plasma Engineering | doi.org/10.13182/FST89-A29144
Articles are hosted by Taylor and Francis Online.
The one-dimensional equilibrium code BPROF is used to calculate the plasma inductance as a function of beta and pinch parameter θ, and the results are represented by an algorithm. The attainable poloidal flux is calculated for a variety of cases, using the CCOIL code, to derive simple algorithms representing the ohmic heating (OH) and equilibrium field (EF) fluxes in terms of dimensionless parameters. Assuming a temperature scaling relationship with plasma current and size, the loop voltage equation is integrated to find the flux consumed versus the pulse length. This plasma equation is combined with the flux and inductance algorithms to estimate the attainable plasma pulse length, in terms of the peak magnetic field at the coil and the plasma and coil dimensions. The attainable pulse length depends mainly on the major radius. With R = 4 m, a/R = 0.12, and I = 10 MA, a pulse length of ∼15 s is predicted. The voltage drop due to helicity edge loss is a major uncertainty. The main value of this work is the derivation of simple equations for calculating plasma inductance, OH and EF coil fluxes, and plasma pulse length, without having to run BPROF, CCOIL, and plasma transport codes.
