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The division provides a forum for focused technical dialogue on thermal hydraulic technology in the nuclear industry. Specifically, this will include heat transfer and fluid mechanics involved in the utilization of nuclear energy. It is intended to attract the highest quality of theoretical and experimental work to ANS, including research on basic phenomena and application to nuclear system design.
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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.
R. W. Moir
Fusion Science and Technology | Volume 61 | Number 1 | January 2012 | Pages 243-249
Fusion-Fission Hybrids and Transmutation | Proceedings of the Fifteenth International Conference on Emerging Nuclear Energy Systems | doi.org/10.13182/FST12-A13427
Articles are hosted by Taylor and Francis Online.
Fusion reactors can be designed to breed fissile material for startup and makeup fuel for fission reactors while suppressing fissioning, thereby enhancing safety. Each fusion reaction can release about 2.1 times the 14 MeV neutron's energy in the blanket in this fission-suppressed design while producing 0.6 fissile atoms, which is 2660 kg/1000 MW of fusion power for a full power year. The revenues would be doubled from such a plant by selling both fuel at a price of $60/g and electricity at $0.05/kWh for Q=Pfusion/Pinput=4. Fusion reactors could also be designed to destroy fission wastes by fissioning, but this is not a natural use of fusion whereas it is a designed use of fission reactors. Fusion could supply makeup fuel to fission reactors dedicated to fissioning wastes with some of their neutrons. The design for safety and heat removal is already accomplished with fission reactors; however, fusion reactors have geometry that compromises safety with a complex and thin wall separating the fusion zone from the fission blanket zone. Fusion is unique compared to fission in that its high-energy 14 MeV neutron can generate up to 0.05 232Uatoms for each 233U atom produced from thorium, about twice the IAEA standards of “reduced protection” or “self protection.”