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Accelerator Applications
The division was organized to promote the advancement of knowledge of the use of particle accelerator technologies for nuclear and other applications. It focuses on production of neutrons and other particles, utilization of these particles for scientific or industrial purposes, such as the production or destruction of radionuclides significant to energy, medicine, defense or other endeavors, as well as imaging and diagnostics.
Meeting Spotlight
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
Standards Program
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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Argonne’s METL gears up to test more sodium fast reactor components
Argonne National Laboratory has successfully swapped out an aging cold trap in the sodium test loop called METL (Mechanisms Engineering Test Loop), the Department of Energy announced April 23. The upgrade is the first of its kind in the United States in more than 30 years, according to the DOE, and will help test components and operations for the sodium-cooled fast reactors being developed now.
K. L. Nash, S. Fried, A. M. Friedman, N. Susak, P. Rickert, J. C. Sullivan
Nuclear Technology | Volume 60 | Number 2 | February 1983 | Pages 257-266
Technical Paper | Radiation Effects and Their Relationship to Geological Repository / Radioactive Waste Management | doi.org/10.13182/NT83-A33081
Articles are hosted by Taylor and Francis Online.
The rates at which 241Am and 239Pu are leached by triply distilled water from a candidate borosilicate glass 76-101 can be adequately correlated by the exponential, An = An0l−kt, where An is the concentration of the actinide in molar mass per square centimetre. The values for the parameters An0 and k are 2.45 × 10−9 M/cm2 and 0.024 ± 0.001 h−1, respectively, over the period of 1 to 24 h. When the glass samples are irradiated with gamma rays from a 60Co source of 1 Mrad/h, values of the parameters (1-to 24-h irradiation time) are A0 = 5.6 × 10−9M/cm2, k = 0.103 ± 0.004 h−1 for 239Pu and A0 = 2.2 × 10−11 M/cm2, k = 0.104 ± 0.003 h−1 for 241 Am.