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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.
Owen N. Jarvis, Pieter Van Belle, Malcolm A. Hone, Guy J. Sadler, G. A. H. Whitfield, F. Edward Cecil, Douglass S. Darrow, Basilio Esposito
Fusion Science and Technology | Volume 39 | Number 1 | January 2001 | Pages 84-95
Technical Paper | doi.org/10.13182/FST01-A154
Articles are hosted by Taylor and Francis Online.
Two screened, thin-foil charge collectors were mounted just beyond the plasma edge at an outboard position (below midplane) in the Joint European Torus to detect lost alpha particles during the 1997 high fusion power D-T experiments. No convincing observations of alpha-particle collection were obtained, possibly because of the low level of alpha-particle losses but more probably because the positioning of the detector was not ideal for the high fusion power discharges that were run at high plasma current and toroidal field. Under such conditions, alpha particles on escaping orbits leading toward the detector are highly likely to be intercepted by the nearby poloidal limiter. Moreover, a small alpha-particle signal would have been obscured by interference from a large and unexpected signal attributed here to fast neutrals, leaving the plasma and ionizing in the low density scrape-off region outside the plasma boundary. The interpretation of this unexpected signal is discussed. In all probability, it will also be encountered in any future attempts to detect lost alpha particles in a current measuring detector unless suitable precautions are taken, e.g., provision of a thin first foil to remove light charged particles with energies below ~0.5 MeV.