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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.
A. Kumar, Y. Ikeda, C. Konno
Fusion Science and Technology | Volume 19 | Number 3 | May 1991 | Pages 1979-1988
Neutronic | Proceedings of the Ninth Topical Meeting on the Technology of Fusion Energy (Oak Brook, Illinois, October 7-11, 1990) | doi.org/10.13182/FST91-A29632
Articles are hosted by Taylor and Francis Online.
The experimental measurement of nuclear heat deposition rates in a simulated D-T fusion neutron environment has assumed importance due to untested nature of large body of kerma factor libraries. An experimental effort was recently initiated to develop and apply calorimetric technique to measure heat deposition in various materials subjected to D-T neutron fields, in the framework of JAERI/USDOE collaborative program on fusion neutronics. Thermistors and platinum RTD's were employed as thermal sensors within calorimeters made of single materials (or probes). The first experiments were conducted during June 1989 and the tested materials included: Fe, Al, C, Cu. Each of these calorimeters was placed inside a vacuum chamber and the mean distance from the target was ∼8 cm. The calorimeters were subjected to spaced neutron pulses of 3 to 10 min duration. The measured heat deposition rates ranged from 7 to 30 µW/g for a normalized source strength of 1012 n/s-iron and graphite providing the lowest and the highest rates respectively. These single probe experiments were analyzed using 3D code MCNP. The single probe experiments were carried out again in december 1989. This allowed to verify the reproducibility. This time, the average target-probe distance was shortened to ∼5 cm which led to 2 to 3 times higher rates. Tungsten was also included. Ratio of computed (C) to measured (E) rates varied from 0.79 to 1.77 for RMCCS evaluation of MCNP. Four evaluations, available with MCNP, throw up large deviations; For example, C/E for iron for an experiment ranges from 0.40 to 0.94. In addition to single probe experiments, two novel experiments were conducted with multiple probes in separate host media of iron and graphite. C/E varied from 0.51 to 2.36.