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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.
T. Kammash
Nuclear Science and Engineering | Volume 7 | Number 5 | May 1960 | Pages 425-434
Technical Paper | doi.org/10.13182/NSE60-A25740
Articles are hosted by Taylor and Francis Online.
The elastic-plastic deformation of a tube subjected to radially uniform heat generation is considered using Tresca's yield function, its associated flow rule, and a linear work-hardening law. The tube is assumed to be in the state of plane strain and all the elastic and thermal parameters are taken to be temperature independent. For a uniform heat source Q, which increases monotonically with time and which has an insulated inner surface, yielding commences at the inner boundary and propagates outward upon further thermal loading. Immediately after initiation of yield, a plastic region (inner) and an elastic region (outer) are formed with the tangential stress as the intermediate principal stress in both regions. The maximum strength of a heat source, QM, to which a tube may be subjected is taken to correspond to that value of Q which makes the tube almost entirely plastic. This value of Q is computed for several graphite tubes of different thicknesses and then compared with an experimentally obtained QF which corresponds to total failure (fracture) of these tubes. A value of approximately 2.5 is obtained for QF/QM for tubes of moderate thicknesses. Furthermore, the ratio QF/QM remains practically constant as tube thickness increases. Agreement between theory and experiment especially in depicting the dependence of failure load on tube thickness and temperature gradient is considered excellent in light of the many assumptions made. The application of this theory to the design of nuclear reactor fuel elements is also pointed out.