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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.
Jean-Georges Wégrowe
Fusion Science and Technology | Volume 7 | Number 2 | March 1985 | Pages 250-274
Technical Paper | doi.org/10.13182/FST85-A24542
Articles are hosted by Taylor and Francis Online.
Experimental data from a number of lower hybrid experiments are compared with theoretical predictions in different domains of interest for reactor applications. While some points still remain undecided (enhancement of the number of resonant electrons in the current drive regime, for which a number of theoretical explanations are proposed) or not yet understood (occasional quenching of the wave penetration in the ion heating regime), a good general agreement of the experimental results with the conventional theories is found in many respects (wave coupling, wave propagation, boundaries of the high-frequency and plasma parameter domains for different types of interactions, ion heating in the majority of cases, parametric dependence of current drive, and power deposition on the electrons).