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RIC panel discusses pathway to fusion commercialization
Fusion leaders at the Nuclear Regulatory Commission’s annual Regulatory Information Conference discussed the path forward for regulating the burgeoning fusion industry. The speakers discussed government and private industry initiatives in the United States and United Kingdom, with a focus on efforts shaping the near-term deployment of commercial fusion machines.
A recurring theme was the need to explain the difference between fission and fusion. Representatives from the Department of Energy and Type One Energy highlighted this as an important distinction for regulators, as it will allow fusion to undergo its own independent maturation process for developing standards and regulations in the same way that fission has. Lea Perlas, Fusion Program director at the Virginia Department of Health, said that confusion between fission and fusion has been a common cause for misplaced concerns among community members surrounding Commonwealth Fusion Systems’ proposed fusion plant site near Richmond, Va.
Cheol Ho Pyeon, Masao Yamanaka, Tadafumi Sano, Koichi Takamiya
Nuclear Science and Engineering | Volume 193 | Number 9 | September 2019 | Pages 1023-1032
Technical Paper | doi.org/10.1080/00295639.2019.1603014
Articles are hosted by Taylor and Francis Online.
At the Kyoto University Critical Assembly (KUCA), critical irradiation experiments on 237Np and 241Am foils are carried out in the neutron hard spectrum core. For nuclear transmutation of minor actinides, special attention is paid to determining 237Np and 241Am fission reaction rates and to 237Np capture reaction rates in the KUCA hard spectrum core. In the back-to-back (BTB) fission chamber, two nuclide foils (test: 237Np or 241Am; reference: 235U) are set closely to each other to measure the aforementioned fission reaction rates. Interestingly, the experimental 237Np and 241Am fission and capture reaction rates are attained by critical irradiation at low W reactor power for 1 h in the core and are successfully deduced through signals from the BTB fission chamber (fission) and the gamma-ray detection (capture) after the irradiation, respectively, together with MCNP calculations.