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ANS Student Conference 2025
April 3–5, 2025
Albuquerque, NM|The University of New Mexico
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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.
Suresh V. Garimella, Richard N. Christensen
Nuclear Technology | Volume 89 | Number 3 | March 1990 | Pages 388-398
Technical Paper | Heat Transfer and Fluid Flow | doi.org/10.13182/NT90-A34377
Articles are hosted by Taylor and Francis Online.
An experimental investigation was undertaken in which transient condensation of steam-air mixtures occurred on one face of a large aluminum block of which all the other faces were insulated. Tests were conducted in a pressure vessel at pressures of up to 650 kPa. The transients were provided by a sudden increase in the vessel pressure from a given value to a much higher value by the introduction of additional steam. Temperature measurements within the block agreed well with results from a finite difference analysis of the condensing surface and block. Visual observation of the condensing surface indicated that the mode of condensation was predominantly dropwise. The dependence of the heat transfer coefficient on time, pressure, severity of the transient, percentage of noncondensables, and the driving temperature difference was studied. The results at the much higher pressures and transient conditions used in this study agreed with observations in the literature of such trends at lower pressures. There was evidence of the occurrence of a buildup of noncondensables at the condensing surface with time.