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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.”
Diethelm Schroeder-Richter, Sabiha Yildiz
Fusion Science and Technology | Volume 29 | Number 4 | July 1996 | Pages 512-518
Technical Paper | Blanket Engineering | doi.org/10.13182/FST96-A30694
Articles are hosted by Taylor and Francis Online.
The critical heat flux (CHF) is studied experimentally in vertical tubes heated directly using power current (direct current 2500 A, 15 V) and cooled with water at a low mass flow rate (0 to 0 2 Mg/m2·s) and at low pressure (0.1 to 0.8 MPa). A smooth tube and a tube with a porous coating layer sintered onto the inner surface were used. The tube and the porous coating layer are both made from INCONEL-600. The results (so far at moderate heat fluxes) are compared with each other and with correlations by Katto and by Weber. Enhancement of heat transfer was determined as well as a negative effect of the porous coating below the expected value of CHF. It seems that a disadvantage of the coated tube corresponds to the apparently annular flow regime alone; whereas, the CHFs can be enhanced by the porous layer as long as the bubbly flow pattern is maintained up to the location of maximum heat flux. Obviously, the latter situation is established during high-heat-flux conditions, i.e., at high subcooling and high flow rate, which are the classical design characteristics of high-heat-flux components infusion reactors.
