ANS is committed to advancing, fostering, and promoting the development and application of nuclear sciences and technologies to benefit society.
Explore the many uses for nuclear science and its impact on energy, the environment, healthcare, food, and more.
Explore membership for yourself or for your organization.
Conference Spotlight
2026 Nuclear Energy Conference & Expo (NECX)
August 24–27, 2026
Dallas, TX|Hilton Anatole
Latest Magazine Issues
Jun 2026
Jan 2026
2026
Latest Journal Issues
Nuclear Science and Engineering
July 2026
Nuclear Technology
June 2026
Fusion Science and Technology
May 2026
Latest News
North American construction is back—smaller and faster—at OPG’s Darlington
“The nuclear renaissance is real here,” said Ontario Power Generation’s Subo Sinnathamby on May 8, one year to the day after OPG secured a final investment decision to build the first of four planned BWRX-300 reactors at its Darlington nuclear power plant, and shortly after the new reactor’s foundation was lifted into place. “We got our license to construct in April and our [final investment decision] in May, and we’ve been off to the races since.”
J. C. Rook, K. P. Weber, E. C. Corcoran
Nuclear Technology | Volume 206 | Number 12 | December 2020 | Pages 1861-1874
Technical Paper | doi.org/10.1080/00295450.2020.1720557
Articles are hosted by Taylor and Francis Online.
For irradiation experiments (e.g., of per- and polyfluoroalkyl substances), values of nuclear particle flux and absorbed dose rates were obtained for the Safe LOW-POwer Kritical Experiment-2 (SLOWPOKE-2) nuclear reactor at the Royal Military College of Canada using extensive simulations of the reactor core via the Monte Carlo N-Particle code, version 6 (MCNP6). Calculations from this work were compared to data from previously conducted experimental and simulation work to ensure simulation fidelity. In addition, reactor core burnup calculations were conducted using the fuel-depletion capability in MCNP6.1 to address the 30+ years of SLOWPOKE-2 reactor use. The combined absorbed dose rate in the inner irradiation sites was simulated to be 36 ± 1 kGy h−1 at a 10-kW(thermal) power setting, specifically, 20 ± 6 kGy h−1 from neutrons and 16 ± 5 kGy h−1 from photons.