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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.
Jakob Weitman
Nuclear Science and Engineering | Volume 18 | Number 2 | February 1964 | Pages 246-259
Technical Paper | doi.org/10.13182/NSE64-A18325
Articles are hosted by Taylor and Francis Online.
The effective resonance integral of thorium oxide rods has been determined as a function of their surface-to-mass ratio. The range of S/M values covered is 0.15 - 0.65 cm2/g. An experimental technique based on the comparison of activities obtained in thermal and slowing-down neutron fluxes was employed. The shape of the resonance neutron spectrum was determined from measurements with a fast chopper and from calculations, permitting deduction of a correction factor which relates the experimental values to the ideal 1/E case. The results are summarized by the following expression: The main contribution to the margin of error arises from the uncertainties in the 4% spectral correction applied, in the 1.5 b “l/v” part deducted and in the 1510 b infinite-dilution integral of gold, used as a standard. In order to compare the consistency of Dresner's first equivalence theorem and Nordheim's numerical calculations relative to our results, the resonance integral values for thorium metal rods obtained previously by Hellstrand and Weitman have been recalculated, using recent cross section and spectrum data. The new formula is It differs from the old one mainly because of the proved non-l/v behaviour of the thorium cross section below the first resonance.