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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.
Lung Kwang Pan
Nuclear Technology | Volume 124 | Number 3 | December 1998 | Pages 276-283
Technical Paper | Radiation Measurements and Instrumentation | doi.org/10.13182/NT98-A2926
Articles are hosted by Taylor and Francis Online.
A feasibility study of gross alpha counting in real environmental samples using the superheated-liquid-droplet (SLD) technique has been carried out. To find an alternative technique as a fast screening for gross alpha counting in environmental samples, various samples acquired from real groundwater and soil were mixed with the SLD emulsion. The intersections of alpha particles with the superheated liquid Freon-12 droplets trigger the vaporization of the droplet and form bubbles. The acoustic wave accompanying the bubble formation can be recorded by a piezoelectric sensor. The number of bubbles recorded represents a measurement of the gross alpha counting. These results are reasonable when compared with those obtained using the conventional methods. However, for practical application, the SLD fabrication and correlated counting process still need to be further modified.
