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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.
Abhijit Sen
Fusion Science and Technology | Volume 59 | Number 3 | April 2011 | Pages 526-538
Lecture | Fourth ITER International Summer School (IISS2010) | doi.org/10.13182/FST11-A11694
Articles are hosted by Taylor and Francis Online.
The creation of large-sized magnetic islands through excitation of neoclassical tearing modes (NTMs) and the concommitant degradation of energy confinement is a major concern for ITER. The basic physical mechanisms governing the dynamics of this instability are introduced, and important experimental observations and techniques of controlling or suppressing these modes are briefly reviewed. The effects of plasma rotation on the excitation threshold and saturated island sizes of NTMs, as observed in many recent experiments, and their present understanding as obtained from model analytical and numerical simulations are discussed.