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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.
Eric Tucker, J. Gilligan
Fusion Science and Technology | Volume 33 | Number 2 | March 1998 | Pages 118-129
Technical Paper | doi.org/10.13182/FST98-A22
Articles are hosted by Taylor and Francis Online.
The vapor shield outward expansion rate can be shown to affect energy transport through the vapor shield, thereby influencing the vapor shield effectiveness. To more accurately determine the divertor plate erosion depth from a tokamak fusion reactor disruption or plasma gun sources, it is then necessary to include source plasma (beam) momentum transfer and beam mass deposition to the expanding vapor shield. Other factors such as incident heat flux and target Z value are shown to influence the vapor shield expansion rate as well. Code calculations show that increasing heat fluxes can increase the fraction of vapor shield kinetic energy and lower the fraction f of incident energy transported to the solid. Low-Z materials give higher kinetic energies as well but result in a higher f due to a lower specific heat. These results can also be applied to plasma gun technology to help increase its efficiency. In an electrothermal gun, the plasma expansion rate (rate at which vaporized material travels out of the gun) can cause differing plasma residence times and differing plasma temperatures as well. Determining the mechanisms that influence the vapor shield expansion rate and showing its sensitivity on f can give us a qualitative way of determining how changing parameters can influence plasma gun efficiency. Low-energy (<200 eV) disruption plasmas add much mass as well as momentum to a vapor shield. Mass addition can cause the vapor shield temperature and f to differ for a given incident heat flux and change the vapor shield expansion rate as well. Also, we find that deuterium's shielding effectiveness differs from carbon.