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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.
Mikio Enoeda, Yoshinori Kawamura, Kenji Okuno, Ken-ichi Tanaka, Mitsuru Uetake, Masabumi Nishikawa
Fusion Science and Technology | Volume 28 | Number 3 | October 1995 | Pages 591-596
Tritium Processing | Proceedings of the Fifth Topical Meeting on Tritium Technology in Fission, Fusion, and Isotopic Applications Belgirate, Italy May 28-June 3, 1995 | doi.org/10.13182/FST95-A30467
Articles are hosted by Taylor and Francis Online.
Experimental results showed that Q2 gas was adsorbed effectively by CMSB on an early stage of breakthrough even though CH4 exists in the inlet gas. Particularly, in the case of Q2 with low concentration of CH4, the break through curve of Q2 showed almost the same curve as in the case of pure Q2 adsorption. However, CH4 gas spilled over adsorbed Q2 in the course of CH4 break-through. This means that the CMSB will eventually lose the ability to adsorb Q2 in the final stage of adsorption. The critical time when the CMSB loses the adsorption ability depends on the inlet CH4 concentration. Analysis of the results showed that the adsorption of Q2 and CH4 mixture can be roughly described by assuming the multi-component adsorption equations for Q2 and CH4 using Langmuir's equations. It was certified that the analysis model described and predicted the experimental observations very well.
