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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.
Vitaly T. Astrelin, Eugeny V. Bobukh
Fusion Science and Technology | Volume 35 | Number 1 | January 1999 | Pages 299-303
Poster Presentations | doi.org/10.13182/FST99-A11963871
Articles are hosted by Taylor and Francis Online.
A numerical simulation of decelerating, scattering, and trapping fast electrons by plasma in a magnetic trap is reported. Fast non-thermal electrons are generated via the interaction of the relativistic electron beam with the plasma. Their energy significantly exceeds the thermal energy of plasma particles. For real experimental conditions where the mean free path of electrons is larger than the length of a local magnetic pit, the kinetic equation for distribution function of electrons is numerically solved. The effect of electron scattering and trapping into the pit is calculated.