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Improving task performance, system reliability, system and personnel safety, efficiency, and effectiveness are the division's main objectives. Its major areas of interest include task design, procedures, training, instrument and control layout and placement, stress control, anthropometrics, psychological input, and motivation.
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ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
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Candidates for leadership provide statements: ANS Board of Directors
With the annual ANS election right around the corner, American Nuclear Society members will be going to the polls to vote for a vice president/president-elect, treasurer, and members-at-large for the Board of Directors. In January, Nuclear News published statements from candidates for vice president/president-elect and treasurer. This month, we are featuring statements from each nominee for the Board of Directors.
J W Rogers, D. A. Millsap, Y. D. Harker
Nuclear Technology | Volume 25 | Number 2 | February 1975 | Pages 330-348
Technical Paper | Material Dosimetry | doi.org/10.13182/NT75-A24372
Articles are hosted by Taylor and Francis Online.
The Coupled Fast Reactivity Measurements Facility (CFRMF) is a zoned-core critical assembly with a fast-neutron spectrum zone in the center of an enriched 235 U, water-moderated thermal “driver” zone. The neutron spectrum of the fast zone has a mean energy of ∼0.72 MeV with an energy distribution of interest in fast breeder reactor dosimetry and reaction rate studies. The CFRMF neutron field has become one of the standard spectra for testing fast-neutron reactions in fissile and nonfissile materials in an interlaboratory experimental effort. The CFRMF has found much use as a fast-neutron field for the activation of materials of interest in the fast breeder reactor programs because of its well -studied energy spectrum and spatial gradients, intensity [up to 1011 n/(cm2 sec)], the precise control and reproducibility of intensity and experimental amenabilities. The neutron energy spectrum at the core center has been measured by proton-recoil spectrometry between ∼3.0 keV and ∼2.5 MeV and calculated by resonance absorption, transport theory, and Monte Carlo multigroup techniques from 10 MeV down. Neutron flux distributions in the fast zone have been examined by activation and fission rate measurements which show that gradients do not exceed ∼0.3% in the region where the experiments are located.