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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.
S. A. Cherenshchykov
Fusion Science and Technology | Volume 66 | Number 2 | October 2014 | Pages 358-367
Technical Note | doi.org/10.13182/FST13-720
Articles are hosted by Taylor and Francis Online.
The injection of a nonrelativistic electron beam into a toroidal solenoid is considered. A secondary emission magnetron injection gun is proposed as a source of the electron beam. Using the drift approximation, a step value after the first turn of the beam around the solenoid is calculated. For multiturn injection, the beam must not return to the electron gun. Thus, the step value must be large enough by comparison with the gun dimension. Using this condition and the Hull cutoff magnetic field equation, the maximum electrode diameters of the magnetron injection gun are calculated. The maximum gun perveance is calculated using scale theory and experimental data from other authors. Because of the small dimensions of the gun, a concept for a multibeam gun is proposed. As an example, the total current and total power are calculated for two values of the electron beam energy and three operational facilities. In comparison with existing sources for auxiliary plasma heating, a novel approach can provide higher power. The calculated levels of the electric field strength in the gun are several times lower than those achieved in experiments. Prospects for the novel concept for plasma heating and current drive and the problem of gun cooling are discussed. Other possible applications are discussed too.