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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.
J. Reece Roth
Fusion Science and Technology | Volume 2 | Number 1 | January 1982 | Pages 29-42
Overview | doi.org/10.13182/FST82-A20732
Articles are hosted by Taylor and Francis Online.
The consequences are assessed of a common set of engineering constraints on the characteristics of fusion reactors that employ deuterium-tritium (D-T), advanced, and exotic fusion fuel cycles. A set of uniform assumptions is made regarding blanket costs, wall loading limits, fusion power density limits, radio-frequency technologies, etc. From these common constraints, the regimes of ion number density, ion kinetic temperature, and plasma stability index β, which lead to attractive fusion reactors, are found. It is demonstrated that if tokamaks are restricted to values of β < 0.05, no fuel cycle other than D-T is compatible with currently accepted engineering constraints. The catalyzed deuterium-deuterium and the D-3He reactions are attractive for values of β > ∼0.20. It is found that the charged particle or “neutron-free” reactions such as ρ-6Li, even if ignitible, are inconsistent with engineering constraints, even at β = 1.0, because of their low reactivity. As expected, the D-T reaction allows the widest range of operating parameters because of its high reactivity. However, it can be used only with difficulty at high values of β because of wall loading limitations. Finally, the limitations imposed by electron cyclotron resonance heating (ECRH) of the plasma are examined. It is found that the cutoff density implied by ECRH (above which radiation is reflected from the plasma) places a serious additional constraint on the accessible operating regime of some advanced fuel fusion reactors.