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Radiation Protection & Shielding
The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
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International Conference on Mathematics and Computational Methods Applied to Nuclear Science and Engineering (M&C 2025)
April 27–30, 2025
Denver, CO|The Westin Denver Downtown
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The Standards Committee is responsible for the development and maintenance of voluntary consensus standards that address the design, analysis, and operation of components, systems, and facilities related to the application of nuclear science and technology. Find out What’s New, check out the Standards Store, or Get Involved today!
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ANS designates Armour Research Foundation Reactor as Nuclear Historic Landmark
The American Nuclear Society presented the Illinois Institute of Technology with a plaque last week to officially designate the Armour Research Foundation Reactor a Nuclear Historic Landmark, following the Society’s decision to confer the status onto the reactor in September 2024.
H. Zimmermann
Nuclear Technology | Volume 28 | Number 1 | January 1976 | Pages 127-133
Technical Paper | Fuels for Pulsed Reactor / Fuel | doi.org/10.13182/NT76-A31546
Articles are hosted by Taylor and Francis Online.
The fission gas behavior in oxide fuel elements irradiated within the irradiation program of the Fast Breeder Project was determined. The amount of fission gas was measured in three steps as released fission gas, fission gas retained in bubbles and pores, and fission gas retained in the fuel matrix. This was done by the puncturing of the fuel rods, by the grinding of the fuel, and by the chemical solution of the powdered fuel, respectively. Under the conditions prevailing in fast breeder reactors, the fractional fission gas release is ∼90% or more after medium and high burnups. The release rate is not constant, but there are periods with particularly high release rates (breakaway release). The retained fission gas reaches concentrations of ∼1.5 × 10−2 gas atoms per uranium and plutonium atoms in fuel regions with temperatures below 1100°C. The concentration decreases with increasing temperatures. At temperatures above 1500°C the concentration of the retained gas is ∼2 × 10−4 gas atoms per initial metal atom. Up to five times more fission gas is retained in bubbles and pores than in the matrix. There is a relation between plastic deformation of the cladding by mechanical interaction with the fuel and the concentration of fission gas in bubbles.