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Nuclear Energy Strategy announced at CNA2026
At the Canadian Nuclear Association Conference (CNA2026) in Ottawa, Ontario, on April 29, Minister of Energy and Natural Resources Tim Hodgson announced that Natural Resources Canada (NRCan) is developing a new Nuclear Energy Strategy for the country. The strategy, which is slated to be released by the end of this year, will be based on four objectives: 1) enabling new nuclear builds across Canada, 2) being a global supplier and exporter of nuclear technology and services, 3) expanding uranium production and nuclear fuel opportunities, and 4) developing new Canadian nuclear innovations, including in both fission and fusion technologies.
Steve Kahn, Randall Harman, Vernon Forgue
Nuclear Science and Engineering | Volume 23 | Number 1 | September 1965 | Pages 8-20
Technical Paper | doi.org/10.13182/NSE65-A19254
Articles are hosted by Taylor and Francis Online.
Energy spectra were obtained experimentally for fission fragments escaping from backed films of enriched uranium dioxide that were less than 11 µm thick. The data were reduced to give values for the relative average escape energies (R), escape fractions (S) and energy deposition efficiencies (D). A mathematical model was developed to synthesize these results using a Monte-Carlo-type computer code. This code included the fission-fragment masses, yields, and initial energies, the experimental source-detector geometry, a range-energy relationship, an energy-loss relationship and a function for the pulse-height defect in surface-barrier detectors. Various functions for these last three parameters were used in combination to obtain results that duplicated the experimental spectra and R, S and D values. The agreement was obtained with range proportional to (energy)1/2, the square energy-loss function, and pulse-height defect = A (E) (M-B), where A and B are constants and E and M are energy and mass, respectively. The experimental detection functions were removed from the code, and the spectra and R, S and D values were calculated for a 2π geometry. These values agreed well with those calculated using weighted averages for range and initial energy.