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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.
X. Albets-Chico, H. Radhakrishnan, S. C. Kassinos
Fusion Science and Technology | Volume 61 | Number 1 | January 2012 | Pages 1-10
Technical Paper | doi.org/10.13182/FST12-A13335
Articles are hosted by Taylor and Francis Online.
This paper addresses liquid-metal flow under a strong, fringing, decreasing magnetic field in an insulating circular pipe by a full resolution of the magnetohydrodynamic (MHD) equations. The aims of the paper are first to provide a detailed description of the flow and second to perform a study of the restrictions related to the approximate numerical techniques commonly used in the nuclear fusion field, namely, the so-called core flow approximation based on asymptotic methods. Finally, a comparison between full MHD solutions obtained under conducting and insulating circular pipe walls, at similar MHD conditions, is provided. The current results show that the role of inertia is clearly more important under electrically insulating ducts because no net braking MHD forces are present in such configurations. This fact adversely affects the accuracy of asymptotic method results. From a phenomenological point of view, the effects of wall conductivity are found to be very important. For instance, when insulating walls are present, the intensity of the generated near-wall jets is three times larger than that found in conducting configurations. As a result, the shear effects and the triggering of turbulence in the downstream area are clearly enhanced.