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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.
H. Huang, S. A. Eddinger, R. B. Stephens, A. Nikroo
Fusion Science and Technology | Volume 55 | Number 4 | May 2009 | Pages 380-388
Technical Paper | Eighteenth Target Fabrication Specialists' Meeting | doi.org/10.13182/FST55-380
Articles are hosted by Taylor and Francis Online.
Rayleigh-Taylor instabilities are caused by features that affect shock velocity. These features can be statistically measured by radiography. We designed a precision radiography (PR) system that measures X-ray opacity variations in National Ignition Facility (NIF) ablator capsules to 10-4. Quantitative interpretation of the PR data is challenging and is the subject of this paper. The PR opacity power spectrum (PS) must be related to the NIF surface PS requirements (commonly known as the "NIF curves"). This relationship must be calculated for each specific shell. The compounding factors include X-ray spectra and spot size, detector resolution, shell diameter, coating thickness, dopant and impurity levels, and the coherency status of interface roughness between different layers. In this work, we developed a useful tool to quickly compute the NIF opacity curve (more precisely referred to as NIF "OD [optical depth] PS reference curve" in this paper) for any partially coated NIF shells or nonstandard developmental shells. This allows more rapid feedback on the quality of shells using only partially coated shells and enables benchmarking between the opacity (measured by a radiographic instrument) and surface roughness (measured by an atomic force microscope).