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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.
Boris Breizman
Fusion Science and Technology | Volume 59 | Number 3 | April 2011 | Pages 549-560
Lecture | Fourth ITER International Summer School (IISS2010) | doi.org/10.13182/FST11-A11696
Articles are hosted by Taylor and Francis Online.
The buildup of the energetic particle population in fusion plasmas is typically slow compared to the growth times of energetic-particle driven instabilities. This feature draws special attention to nonlinear studies of unstable waves in the near-threshold regimes. The goal is to characterize the long-time behavior of the weakly dissipative waves and resonant particles in the presence of particle sources and sinks. There are numerous experimental observations of energetic-particle driven instabilities. In some cases the unstable modes grow to a level at which they cause enhanced transport and anomalous losses of the fast particles. In other cases the losses are small but the modes exhibit an intricate nonlinear behavior: generation of sidebands, quasi-periodic bursts, change of the mode frequency in time, etc. This lecture, presented at the 4th ITER International Summer School in Austin, Texas, provides a first-principles physics basis for understanding these phenomena.