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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.
Akira Endou
Nuclear Technology | Volume 114 | Number 3 | June 1996 | Pages 285-291
Technical Paper | Fission Reactor | doi.org/10.13182/NT96-A35233
Articles are hosted by Taylor and Francis Online.
In liquid-metal-cooled fast breeder reactors (LMFBRs), electromagnetic flowmeters (EMFs) have been extensively used to measure the coolant flow rate. Because the coolant flow rate is one of the most important parameters, a high accuracy and a fast response are required for the flow rate measurement. However, it was thought that the response might become slower when the pipe diameter of the EMF was increased. Therefore, a quantitative evaluation of the response was needed. To evaluate the response time of EMFs, an equation of the transient response was derived based on the realistic approximation that the EMF pipe is made of nonconductive material. The response is expressed as a function of the reciprocal of the square of the pipe radius a and of the length L of the external magnetic field along the pipe axis. However, when the aspect ratio L/2a is larger than two, the length of the external magnetic field has an almost insignificant effect on the response, and the response time increases with increasing a2. The transient response can be calculated with an uncertainty of less than a few percent. A first-order approximation of the derived equation is given by the first lag term with the time constant of µσa2/ 3.832 with permeability µ and conductivity a of the coolant. Even though the EMF has a diameter as large as 30 in., the response time is 45 ms and sufficiently fast compared with other sensors used in LMFBRs.