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NRC looks to leverage previous approvals for large LWRs
During this time of resurging interest in nuclear power, many conversations have centered on one fundamental problem: Electricity is needed now, but nuclear projects (in recent decades) have taken many years to get permitted and built.
In the past few years, a bevy of new strategies have been pursued to fix this problem. Workforce programs that seek to laterally transition skilled people from other industries, plans to reuse the transmission infrastructure at shuttered coal sites, efforts to restart plants like Palisades or Duane Arnold, new reactor designs that build on the legacy of research done in the early days of atomic power—all of these plans share a common throughline: leveraging work already done instead of starting over from square one to get new plants designed and built.
Ch. Lagrange, O. Bersillon, D. G. Madland
Nuclear Science and Engineering | Volume 83 | Number 3 | March 1983 | Pages 396-401
Technical Note | doi.org/10.13182/NSE83-A17575
Articles are hosted by Taylor and Francis Online.
As coupled-channel calculations are very time consuming when applied to odd-mass target nuclei using the actual level schemes, the adequacy of the following approximation is studied. Calculations are performed for a fictitious even-even nucleus with the same mass number as the odd-mass target of interest. Deformation parameters are obtained from a systematic available in this mass region, and the optical model parameters used are extrapolated from those determined for the neighboring even-even nuclei. Direct elastic and inelastic scattering cross sections resulting from such calculations are distributed among the true ground-state band levels of the odd-mass nucleus. Comparisons of calculations made with a fixed set of optical parameters, but using either the actual or the fictitious level scheme, are presented for ground-state bands of K = 1/2 and K = 5/2. The approximation proposed can be applied with great confidence over the energy range 10 keV to 20 MeV in case of K = 1/2. In case of K = 5/2, the approximation gives satisfactory results in the limited energy range 4 to 20 MeV.