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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.
Robert E. Woodley, Robert E. Einziger, H. Craig Buchanan
Nuclear Technology | Volume 85 | Number 1 | April 1989 | Pages 74-88
Technical Paper | Nuclear Fuel | doi.org/10.13182/NT89-A34229
Articles are hosted by Taylor and Francis Online.
A series of pressurized water reactor spent-fuel samples from Turkey Point Unit 3 have been oxidized at temperatures between 140 and 225°C in air atmospheres with dew points between 14.5 and -70°C, using a thermogravimetric analysis system. Tests lasted between 400 and 2100 h. At the conclusion of a test, the atmosphere was sampled to determine the release of fission gas during testing, and the fuel samples were analyzed for microstructural changes. It appears that the mechanisms for oxidation of spent fuel to U3O7 takes place in two steps that occur somewhat simultaneously. Oxygen migrates along the grain boundaries, which are oxidized and enlarged. The grains oxidize by the inward progression of a layer of U4O9 saturated with oxygen. A simplified model of the mechanism, which considers oxygen diffusion through the product layer as the rate-controlling step, yields an activation energy of 113 ± 17 kJ/mol. Moisture, between dew points of —70 to +14.5°C, i.e., water vapor partial pressures varying over four orders of magnitude, had no significant effect on the oxidation rate.