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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.
M. Reich, A. Bock, M. Maraschek, ASDEX Upgrade Team
Fusion Science and Technology | Volume 61 | Number 4 | May 2012 | Pages 309-313
Technical Paper | doi.org/10.13182/FST11-392
Articles are hosted by Taylor and Francis Online.
For electron cyclotron current drive-based stabilization of neoclassical tearing modes (NTMs), it is crucial that the current deposition occurs as close to the island as possible; hence, its location needs to be accurately known. An NTM, rotating in the laboratory frame, causes fluctuations of magnetic flux measurable by Mirnov coils (dB/dt). Temperature perturbations in the vicinity of an NTM are caused by displaced flux surfaces and thus have the same frequency as the Mirnov signal but show a constant phase difference, which depends on the mode topology (poloidal and toroidal periodicity), on the toroidal displacement of the Mirnov coil with respect to the temperature measurement, and on the sign of the temperature change between the X-point profile and the O-point profile, which inverts somewhere inside the island. The sign flip of ΔTe is equivalent to a change of the phase difference between Te and magnetic reference by and therefore can be localized using the presented correlation method. Using the suggested algorithm, we can determine the rational surface that coincides with the radial island location with low latency and good reliability in real time from electron cyclotron emission temperature profiles when correlated with the appropriate magnetic fluctuations on a modern workstation computer.