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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.
Osamu Mitarai, Sigeru Sudo
Fusion Science and Technology | Volume 27 | Number 4 | July 1995 | Pages 377-388
Technical Paper | Plasma Engineering | doi.org/10.13182/FST95-A30358
Articles are hosted by Taylor and Francis Online.
Ignition characteristics in deuterium-tritium helical (stellarator) reactors of various sizes are studied with the operation path method on the plane and the POPCON method. Based on empirical large helical device scaling, confinement must be improved by a factor > 1.5 for reaching ignition and a factor >γH = 2 for optimum fusion power in a helical reactor with R > 8 m, ā = 2 m, and B0 > 6 T. The density limit and the confinement time saturation effect with respect to the density degrade the favorable density scaling of the confinement time (τE ∝ n0.69) and are found to be important limiting factors for ignition characteristics. For a reactor with R = 10 m, ā = 2 m, γH = 2, and B0 = 7 T and with an excess heating power Pex = 100 MW, the minimum auxiliary heating power is ∼55 MW at an operating density 40% below the density limit, and ignition can be reached in a finite time. The ignition characteristics for larger size reactors (R = 15 and 20 m) and gyro-reduced Bohm scaling are also studied.