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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.
Fermín Cuevas, José Francisco Fernandáz, Carlos Sánchez*
Fusion Science and Technology | Volume 32 | Number 4 | December 1997 | Pages 644-654
Technical Paper | Special Section: Plasma Control Issues for Tokamaks / Nuclear Reactions in Solid | doi.org/10.13182/FST97-A19909
Articles are hosted by Taylor and Francis Online.
The possible occurrence of nuclear reactions in solids (NRS) is tested in a well-characterized iodide-titanium film after a high deuterium loading. This film proves to have a higher purity than common titanium samples used in NRS experiments. The titanium deuteration is accomplished in the same chamber where the film is grown to avoid any superficial contamination of the sample. A complete set of NRS experiments is performed, checking as triggering mechanisms of the NRS phenomena the imposition of different electric fields and the crossing of the δ-ϵ and β-δ boundary phases of the Ti-D system. Neutron measurements are monitored while doing these experiments, and no clear evidence of the nuclear fusion reaction D + D → 3He + n is detected; the detection limit for this reaction is Λ = 3 × 10−21 fusions per pair of deuterons per second. However, some anomalous neutron signals are monitored by one of the detectors, which makes further investigation desirable.