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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.
T. Saito, Y. Tatematsu, K. Kajiwara, H. Abe, M. Ishikawa, Y. Kiwamoto, Y. Imaizumi, K. Nishida, E. Yokoyama, M. Ichimura, K. Ishii, I. Katanuma, K. Yatsu
Fusion Science and Technology | Volume 39 | Number 1 | January 2001 | Pages 143-146
Topical Lectures | doi.org/10.13182/FST01-A11963427
Articles are hosted by Taylor and Francis Online.
This paper describes response of currents circulating in an end region of the GAMMA 10 tandem mirror to variation of an end plate resistance REP. By changing its value from less than 1 Ω to over 1 MΩ, are examined the variation of the plasma potentials and the current balance at the end plate during fundamental ECRH. Main results are as follows. First, for REP ≥ 3 kΩ, the end plate potential as measured from the vacuum vessel is nearly constant and for REP ≤ 0.5 kΩ, on the contrary, the current flowing through the resistance is nearly constant. Second, the plasma potentials other than the end plate weakly depends on REP. In particular, the plasma potential at the central cell hardly varies with REP. Third, with decreasing REP, a step-like increase in the net current flowing through the end plate is observed at REP ≈ Zeff. Ion currents are observed on ring electrodes installed in the mirror cell in which ECRH is applied. A part of the ion current is to be connected to the end plate current.