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Human Factors, Instrumentation & Controls
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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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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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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A look inside NIST’s work to optimize cancer treatment and radiation dosimetry
In an article just published by the Taking Measure blog of the National Institute of Standards and Technology, Stephen Russek—who leads the Imaging Physics Project in the Magnetic Imaging Group at NIST and codirects the MRI Biomarker Measurement Service—describes his team’s work using phantom stand-ins for human tissue.
R. J. M. Konings, J. L. Kloosterman, J. A. Hendriks, H. Gruppelaar
Nuclear Science and Engineering | Volume 128 | Number 1 | January 1998 | Pages 70-75
Technical Paper | doi.org/10.13182/NSE98-A1946
Articles are hosted by Taylor and Francis Online.
Within the frame of the EFTTRA (Experimental Feasibility of Targets for TRAnsmutation) cooperation, rods of 99Tc metal are irradiated in the Petten High Flux Reactor for 193 effective full power days, during which ~6% of the 99Tc is transmuted to the stable 100Ru. The radial and axial ruthenium distributions in one of the rods are measured by electron probe microanalysis. In the radial direction, the ruthenium concentration strongly increases in the outer rim of the sample, while the axial distribution shows little variation. The average ruthenium concentration, as measured by isotope dilution mass spectrometry, is (6.4 ± 0.2)% at 5 mm from the bottom of the rod and (6.1 ± 0.2)% at 5 mm from the top. The ruthenium concentrations calculated by the KENO three-dimensional Monte Carlo code, 6.1% at 5 mm from the bottom of the rod and 5.7% at 5 mm from the top, are in reasonable agreement with the measured ones. However, the calculated radial distribution of the ruthenium concentration does not agree with the measurements. The radial profile calculated by the MCNP Monte Carlo code, which uses a pointwise cross-section library, agrees much better with the measurements.