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Nuclear Installations Safety
Devoted specifically to the safety of nuclear installations and the health and safety of the public, this division seeks a better understanding of the role of safety in the design, construction and operation of nuclear installation facilities. The division also promotes engineering and scientific technology advancement associated with the safety of such facilities.
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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Fusion Science and Technology
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Latest News
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.
T.L. Grimm, K.E. Kreischer, W.C. Guss, R.J. Temkin
Fusion Science and Technology | Volume 21 | Number 3 | May 1992 | Pages 1648-1653
Plasma Engineering | doi.org/10.13182/FST92-A29957
Articles are hosted by Taylor and Francis Online.
A 200–300 GHz high power pulsed gyrotron oscillator has recently been operated in a 14 T Bitter magnet. The design of this pulsed gyrotron is based on continuous wave (CW) constraints. A single cylindrical waveguide cavity with linear tapers on each end was tested using two magnetron injection guns (MIG). The first produces a large electron beam which excites whispering gallery modes and the second produces a smaller beam that will couple to volume modes. The highest output power of 970 kW was generated at 229 GHz in the TE34,6 using the large MIG with a 59 A, 92 kV electron beam. This corresponds to an efficiency of 18% which was the highest produced in this mode. Similar efficiencies were obtained at 202 and 213 GHz using the same MIG and at 290 GHz using both the large and small MIG. The experimental power and efficiency is about a factor of two below the single mode theoretical predictions, even at low current. A detailed parameterization of the TE34,6 mode's operating range, measurements of the beam's velocity ratio (α), and comparison to previous high frequency work at MIT imply that mode competition is one important cause of the low experimental power and efficiency.