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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.
James P. Blanchard, Qiyang Hu, Nasr Ghoniem
Fusion Science and Technology | Volume 56 | Number 1 | July 2009 | Pages 341-345
High Average Power Laser and Other IFE R&D | Eighteenth Topical Meeting on the Technology of Fusion Energy (Part 1) | doi.org/10.13182/FST09-A8925
Articles are hosted by Taylor and Francis Online.
Dry wall laser IFE chambers will experience large, transient heat and particle fluxes as the target yield products reach the wall. These threats, consisting of x-rays, ions, and neutrons, can lead to wall failure caused by transient stresses or as a result of deposited ions in the near-surface layer. We have developed a unified model for the calculation of temperatures, stresses, strains, and fracture behavior in a solid IFE chamber wall. The model is also coupled with ion transport sub-models that assess the effects of ions on the morphology of the wall materials. This paper describes the models incorporated into the new unified simulation and, in particular, presents new fracture models that permit fracture calculations without the need for an advanced finite element calculation. This fracture model assumes that an array of surface cracks is present in the wall surface and uses superposition to calculate the stress intensity factor via a numerical integration of the stress profile computed for an un-cracked geometry. We also describe approaches for computing the stresses due to inertial effects resulting from the rapid heating associated with the IFE threats. In some cases, these inertial effects lead to stress waves that can lead to premature wall damage and must be accounted for in the analysis. This model is based on semi-analytical solutions for stress waves due to shallow heating in a relatively thick solid. The combined thermomechanical model gives us detailed understanding of the fundamental mechanics of rapidly heated surfaces.