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Colin Judge: Testing structural materials in Idaho’s newest hot cell facility
Idaho National Laboratory’s newest facility—the Sample Preparation Laboratory (SPL)—sits across the road from the Hot Fuel Examination Facility (HFEF), which started operating in 1975. SPL will host the first new hot cells at INL’s Materials and Fuels Complex (MFC) in 50 years, giving INL researchers and partners new flexibility to test the structural properties of irradiated materials fresh from the Advanced Test Reactor (ATR) or from a partner’s facility.
Materials meant to withstand extreme conditions in fission or fusion power plants must be tested under similar conditions and pushed past their breaking points so performance and limitations can be understood and improved. Once irradiated, materials samples can be cut down to size in SPL and packaged for testing in other facilities at INL or other national laboratories, commercial labs, or universities. But they can also be subjected to extreme thermal or corrosive conditions and mechanical testing right in SPL, explains Colin Judge, who, as INL’s division director for nuclear materials performance, oversees SPL and other facilities at the MFC.
SPL won’t go “hot” until January 2026, but Judge spoke with NN staff writer Susan Gallier about its capabilities as his team was moving instruments into the new facility.
Timothy J. Drzewiecki, Brian L. Mount, Martin Lopez de Bertodano
Nuclear Technology | Volume 165 | Number 1 | January 2009 | Pages 18-31
Technical Paper | Thermal Hydraulics | doi.org/10.13182/NT09-A4059
Articles are hosted by Taylor and Francis Online.
The fast boron shutdown injection system in the CNA II pressurized heavy water reactor consists of a set of jets flowing through a very large moderator tank that contains an array of cylindrical coolant channels. The prediction of the turbulent jet mixing is required to determine an accurate distribution of boron inside the moderator tank. The boron distribution is used to calculate the multidimensional insertion of negative reactivity into the reactor during fast shutdown in a PARCS/RELAP5 model of CNA II.A computational fluid dynamics (CFD) code is used to determine the distribution of boron in the moderator tank. The flow is analyzed with a porous-medium model based on volume-averaged momentum, turbulent kinetic energy, and turbulence dissipation equations. The additional source terms that arise due to the averaging must be constituted. The constitutive relations for the additional source terms that are implemented in the present model are (a) the drag force on an array of cylinders for the momentum equations and (b) the additional mixing effect of the cylinders, which results in the sources of turbulent kinetic energy and turbulence dissipation transport equations.The CFD analysis is performed on a porous, axisymmetric domain. The CFD results are compared with data for the boron concentration distribution obtained in a scaled geometrically similar experiment, demonstrating the validity of the approach. Finally, based on the similarity of turbulent jets, the validated model is scaled up to prototypic conditions and inserted into the PARCS/RELAP5 model.