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Education and training to support Canadian nuclear workforce development
Along with several other nations, Canada has committed to net-zero emissions by 2050. Part of this plan is tripling nuclear generating capacity. As of 2025, the country has four operating nuclear generating stations with a total of 17 reactors, 16 of which are in the province of Ontario. The Independent Electricity System Operator has recommended that an additional 17,800 MWe of nuclear power be added to Ontario’s grid.
Constantinos Syros,* Claudio Ronchi, Cinzia Spanó
Nuclear Technology | Volume 94 | Number 2 | May 1991 | Pages 213-227
Technical Paper | Advances in Reactor Accident Consequence Assessment / Nuclear Reactor Safety | doi.org/10.13182/NT91-A34543
Articles are hosted by Taylor and Francis Online.
A semianalytical nonlinear model is described for the calculation of the burst release and release rate of volatile fission product (VFP) from a fuel pellet under steady-state and transient reactor conditions as well as the radial density distribution in the open porosity. The density of the VFP in the porosity channels is assumed to be c(r, t) = φ(r)exp[—LT(r)ω(t)] + Λ-1(t), where L is an analytical function of parameters characterizing the physics and the geometry of the pellet; φ(r) rigorously satisfies the required boundary conditions; and ω(t), the solution of a highly nonlinear differential equation, is a time function (“kinetic time”) that represents the evolution of the density profile. The constant Λ is suitably calculated with the zeroes of the Bessel function Jo(x). The density c(r, t) of the VFP in the open porosity of the pellet is used to find the pressure p(r, t) in the open pores. The integration procedure of the transport equation for different initial and boundary conditions is described. Calculation experiments are presented and discussed.