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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.
E. Alves, L.C. Alves, M.F da Silva, A.A. Melo, J.C. Soares, F. Scaffidi-Argentina
Fusion Science and Technology | Volume 38 | Number 3 | November 2000 | Pages 320-325
Technical Paper | Special Issue on Beryllium Technology for Fusion | doi.org/10.13182/FST00-A36145
Articles are hosted by Taylor and Francis Online.
The electrical resistivity behaviour of a beryllium pebble bed has been studied as a function of the temperature and pressure. At room temperature the resistivity of a single size 2 mm pebble bed decreases drastically from 2·10−2 Ωm to 10−4Ωm by applying an external pressure. After this first drop, the resistivity shows an almost linear decrease with the applied pressure. The same trend appears for a single size 0.1–0.2 mm pebble bed, but the resistivity values are about one order of magnitude higher than in the case of the 2 mm pebbles. At room temperature, the lowest resistivity values were found for the case of a binary pebble bed. After a mechanical cycling the electrical resistivity of the bed never reaches its initial value for zero pressure but it remains about one order of magnitude below the original value. After the first loading cycle the following loading/unloading resistivity curves do not show any significant change. The temperature dependence of the mixed pebble bed was investigated in air at 300 °C, 450 °C and 550 °C. The resistivity behaviour of the pebble bed with the applied pressure is, at high temperature, qualitatively the same as that observed at room temperature. For the same applied load the pebble bed electrical resistivity increases almost linearly with the temperature. Measurements of the oxyde content of the pebbles before and after the heating show a higher beryllium oxide content for the heated pebbles than for the not heated ones.