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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Deep Space: The new frontier of radiation controls
In commercial nuclear power, there has always been a deliberate tension between the regulator and the utility owner. The regulator fundamentally exists to protect the worker, and the utility, to make a profit. It is a win-win balance.
From the U.S. nuclear industry has emerged a brilliantly successful occupational nuclear safety record—largely the result of an ALARA (as low as reasonably achievable) process that has driven exposure rates down to what only a decade ago would have been considered unthinkable. In the U.S. nuclear industry, the system has accomplished an excellent, nearly seamless process that succeeds to the benefit of both employee and utility owner.
R. J. Price
Nuclear Technology | Volume 16 | Number 3 | December 1972 | Pages 536-542
Technical Paper | Material | doi.org/10.13182/NT72-A31222
Articles are hosted by Taylor and Francis Online.
Hot-pressed α-silicon carbide temperature monitors were irradiated at 525 and 772°C to 4.8 × 1021 n/cm2 (E > 0.18 MeV). Postirradiation isochronal annealing was carried out for 1-h periods at either 25 or 50°C intervals between 300°C and 1200 to 1500°C. Above the irradiation temperature the sample length decreased linearly with annealing temperature, while the electrical resistivity increased exponentially with temperature. Straight lines were fitted through the length-versus-temperature and log (resistivity)-versus-temperature data points and the temperature, T1 at which the line intersected the as-irradiated base line was measured. For both length change and resistivity, mean values of T1 agreed with the measured irradiation temperature within experimental accuracy. The precision of a single determination of T1 was obtained from curve-fitting statistics and was about ±20°C for irradiation at 525°C and ±30 at 772°C (90% confidence limits) for both length and resistivity measurements. The sample-to-sample reproducibility of T1 was estimated from the standard deviation of four repeated measurements and was similar to the precision of a single determination.