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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.
Y. Yasaka, N. Takano, H. Takeno
Fusion Science and Technology | Volume 39 | Number 1 | January 2001 | Pages 350-353
Poster Presentations | doi.org/10.13182/FST01-A11963478
Articles are hosted by Taylor and Francis Online.
A magnetic divertor is introduced to the HIEI tandem mirror to enhance the MHD stability in axisymmetric magnetic configuration. It is confirmed that the MHD flute modes can be stabilized by the divertor located at the midplane or off-midplane in the central cell. As the position of the magnetic nulls of the divertor is located at smaller radii, the plasma can be sustained with less fueling rates. The magnetic divertor provides a method to greatly enhance the stability of the flute modes for plasmas weakly stabilized by the RF ponderomotive force.