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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.
K. Tomlinson, D. G. Schroen
Fusion Science and Technology | Volume 63 | Number 2 | March-April 2013 | Pages 288-295
Technical Paper | Selected papers from 20th Target Fabrication Meeting, May 20-24, 2012, Santa Fe, NM, Guest Editor: Robert C. Cook | doi.org/10.13182/FST13-A16352
Articles are hosted by Taylor and Francis Online.
Preshot characterization of the thickness and form of material samples in targets for dynamic materials properties experiments presents unique challenges. Because of design limitations, the measurement tools currently used introduce increasing error as samples deviate from perfect flatness or thickness uniformity. Contact measurements such as height gages and micrometers, for example, are insensitive to thickness variations occurring over spatial scales smaller than the contact probes. In addition, they measure thickness but not form and often damage samples. Standard confocal microscopes overcome some of these problems but can only measure form on the side of the sample that they see. Also, by design, they consistently overestimate thickness because form errors on the side of the sample against the reference surface always prevent perfect contact with it. We are developing a technique that may prove to be superior to both of these methods at characterizing both thickness and form of samples with both imperfect flatness and nonuniform thickness using only an interferometric optical profiler, an inexpensive fixture, a gage block, and a commercial three-dimensional modeling software. The end result is a computer model of the actual sample.