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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.
W. M. Stacey, Jr.
Fusion Science and Technology | Volume 23 | Number 2 | March 1993 | Pages 157-166
Technical Paper | Plasma Engineering | doi.org/10.13182/FST93-A30145
Articles are hosted by Taylor and Francis Online.
A new “rotational” energy flux is derived for highly collisional impurity ions in tokamaks with strong unbalanced neutral beam injection (NBI). The derivation is based on a consistent ordering of kinetic theory. The rotational flux, which is of a collisional origin and vanishes when the rotation vanishes, is ∼ε2δ−1 times larger than the conventional neoclassical energy flux. This rotational energy flux and a previously derived momentum flux of a similar nature reproduce the experimentally observed relation between momentum and ion energy transport, τφ/τi ∼ O(1), χφ/χi ∼ O(1). The magnitude of χi resulting from this rotational energy flux is the same as is observed in many tokamaks with strong unbalanced NBI. This suggests the control of energy confinement via the control of impurity content in strongly rotating tokamak plasmas.
