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North American construction is back—smaller and faster—at OPG’s Darlington
“The nuclear renaissance is real here,” said Ontario Power Generation’s Subo Sinnathamby on May 8, one year to the day after OPG secured a final investment decision to build the first of four planned BWRX-300 reactors at its Darlington nuclear power plant, and shortly after the new reactor’s foundation was lifted into place. “We got our license to construct in April and our [final investment decision] in May, and we’ve been off to the races since.”
Sin Kim, Goon Cherl Park
Nuclear Technology | Volume 122 | Number 3 | June 1998 | Pages 284-294
Technical Paper | Thermal Hydraulics | doi.org/10.13182/NT98-A2870
Articles are hosted by Taylor and Francis Online.
A thermal-hydraulic field analysis code using the finite element method is developed to analyze the effects of anisotropic turbulent diffusion and secondary flow on turbulent mixing, which is essential to the nuclear fuel performance analysis.In this study a new model of anisotropic eddy viscosity is developed. The representative value of the anisotropic factor is determined from the scale relation that is derived on the basis of the flow pulsation phenomenon. The spatial distribution is deduced qualitatively from well-known experiments. The flow fields calculated by this code are compared with experimental data and show good agreements, and the predicted turbulent mixing rates are successfully compared with the scale relation derived in the authors' previous work.The results show that the isotropic eddy viscosity model underestimates the mixing rate and gives the reverse trend as the gap size reduces, and the secondary flow has a minor effect compared with the anisotropic eddy viscosity in the turbulent mixing process. Although the mixing phenomenon of the flow pulsation is a convective process, it can be simulated only by the anisotropic model.