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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.
Yu.M. Ado, A.G. Ufimtsev, V.V. Artisyuk, A. Yu. Konobeyev, Yu.A. Korovin, V.M. Murogov
Fusion Science and Technology | Volume 20 | Number 4 | December 1991 | Pages 683-688
Accelerator/Reactor Waste Transmutation | doi.org/10.13182/FST91-A11946919
Articles are hosted by Taylor and Francis Online.
A sharp increase in the efficiency of neutron generation is caused by cyclic deuteron accumulator with internal deuteron or beryllium target. In this accumulator, beam of deuterons of constant energy pass through the target many times with ionization energy loss compensated by high frequency electric field. Advantages of deuteron accelerator of 30-100 MeV is due to two factors: On the one hand, the desire to decrease the charged particle energy 10-30 times compared with a traditional electronuclear process plants and, on the other hand, the prospect of producing neutrons within a range of energies of greater interest for fusion studies and for efficiently burning high level nuclear wastes from nuclear power plants.