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Long-term strategy calls for up to 10 new reactors in Canada
Canada has launched a Nuclear Energy Strategy, a long-term vision of its nuclear power potential that includes plans to deploy up to 10 new large-scale reactors in the country by 2040.
The June 22 announcement, along with ongoing projects at Darlington and Bruce Power, further confirm Canada's ambitions to expand its nuclear power presence not just domestically but also abroad. Four pillars stand at the heart of the country’s Nuclear Energy Strategy: new nuclear builds in Canada, maintaining its status as a top nuclear supplier and exporter, expanding uranium production, and continuing nuclear fission and fusion innovations.
George I. Bell
Nuclear Science and Engineering | Volume 21 | Number 3 | March 1965 | Pages 390-401
Technical Paper | doi.org/10.13182/NSE65-1
Articles are hosted by Taylor and Francis Online.
We consider the probability, pn(R,t∫; ,,t), that in a multiplying system, a neutron with position velocity , at time t leads to exactly n neutrons in region R of , space at time t∫. By formulating pn in terms of first collision probabilities we derive a non-linear (Boltzmann-like) integro-differential equation for the probability generating function, G. The linearized equation for = 1 - G is shown to be adjoint to the usual Boltzmann equation for the average neutron flux. The behavior of for subcritical and supercritical systems is analyzed. For large t∫-t, it is shown that for subcritical systems approaches zero exponentially, while for supercritical systems → which is a solution of the time-independent non-linear equation for and equals the probability of getting a divergent chain reaction from the initial neutron. In section B, one-velocity theory with isotropic scattering is described in some detail while in section C are outlined the extensions to 1) energy-dependent problems with anisotropic scattering 2) multiple final states, 3) random sources, 4) counting problems, and 5) delayed neutron precursors. In section D methods for solution of equations for G are briefly discussed, and it is shown that the asymptotic behavior may be found from solutions of linear time-independent ‘adjoint α’ and ‘adjoint k’ calculations. Derivation of a point model independent of space and velocity is carried out by an expansion in adjoint α eigenfunctions and the model parameters are shown to differ from those usually assumed in point models.