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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.
Masahiro Kinoshita
Fusion Science and Technology | Volume 6 | Number 3 | November 1984 | Pages 574-583
Technical Paper | Tritium System | doi.org/10.13182/FST84-A23139
Articles are hosted by Taylor and Francis Online.
The simulation procedure used in the code, CRYDIS-2, is greatly improved. The previous procedure used the Newton-Raphson method choosing a set of temperatures and liquid flow rates for the independent variables. Considering the property that the convergence characteristics of the liquid flow rates are much less sensitive to the type of the iterative method than those of the temperatures, the iterative loop is divided into two loops — the inner loop of the quasi-Newton method for temperature corrections and the outer loop of the successive iteration for flow rate corrections. The corrections of the deviation coefficients are also made in the outer loop, together with the flow rate corrections, when the nonideality of the hydrogen isotope solution is incorporated in the model. Since the order of the Jacobian matrix is halved, and the numerical evaluation of the Jacobian matrix and its inversion are needed only once, both the computer storage requirements and computation time are remarkably reduced. Thus, a new computer code, CRYDIS-N, which uses an efficient simulation procedure, is developed. Also, a simple but powerful method for estimating the initial set of temperatures is proposed, and it assures rapid achievement of convergence. The simulation procedure is a verison particularly developed for simulating hydrogen isotope distillation columns.