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The Radiation Protection and Shielding Division is developing and promoting radiation protection and shielding aspects of nuclear science and technology — including interaction of nuclear radiation with materials and biological systems, instruments and techniques for the measurement of nuclear radiation fields, and radiation shield design and evaluation.
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2024 ANS Winter Conference and Expo
November 17–21, 2024
Orlando, FL|Renaissance Orlando at SeaWorld
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New laws offer nuclear industry incentives for existing power plant uprates
This year, the U.S. nuclear industry received a much-needed economic boost that could help preserve operating nuclear power plants and incentivize upgrades that extend their lifespan and power output.
Signed into law in 2022, the Inflation Reduction Act offers production tax credits (PTCs) for existing nuclear power plants and either PTCs or investment tax credits (ITCs) for new carbon-free generation. These credits could make power uprates—increasing the maximum power level at which a commercial plant may operate—a much more appealing option for utilities.
N. Tsoulfanidis, B. W. Wehring, M. E. Wyman
Nuclear Science and Engineering | Volume 43 | Number 1 | January 1971 | Pages 42-53
Technical Paper | doi.org/10.13182/NSE71-A21244
Articles are hosted by Taylor and Francis Online.
Previously, absolute measurements were reported for the time-dependent beta energy spectra from fission fragments for electron energies >0.75 MeV. The fragments were produced in the thermal-neutron fission of 235U. To obtain results for electron energies below 0.75 MeV and to provide overlap with the previous results, absolute measurements were made of the time-dependent energy spectra using an experimental system specifically designed for the electron energy range of 0.1 to 1.0 MeV. In this system, a vacuum chamber housed a thin plastic scintillator for the detection of the low-energy electrons, a source foil which was fissioned in a thermal-neutron beam, and a surface-barrier detector for the monitoring of the fission rate. The source foil consisted of 10.4 mg/cm2 of 235U covered and sealed to form a localized source of fission fragments. A deposit of 138 µg/cm2 of 235U on the outside of this foil facing the surface-barrier detector provided the fission fragments for the monitor. Electron energy spectra were measured for the cases of (i) spectrum build-up after initiation of a constant fission rate in a clean foil, (ii) spectrum decay after termination of 8 h of a constant fission rate, and (iii) spectrum decay following a sudden burst of fission produced by a reactor power pulse. The resulting spectra were corrected for the effects of energy resolution and source thickness by unfolding them with the use of a measured system response function. The time-dependent energy measurements for the low-energy betas were combined with the previous measurements for the high-energy betas and the results are presented in tables and graphs. Also given are the total number of betas per fission and the total beta energy per fission for various times during the build-up or the decay of the spectra. Comparisons are made with previous experimental and theoretical work.