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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.
M. L. Walker, D. A. Humphreys
Fusion Science and Technology | Volume 50 | Number 4 | November 2006 | Pages 473-489
Technical Paper | doi.org/10.13182/FST06-A1271
Articles are hosted by Taylor and Francis Online.
We examine the issue of definition of coordinates used for plasma shape control simulations and real-time implementations and their relation to the validity of linearized plasma shape response models. By doing a careful analysis of these simple concepts, some subtle issues are exposed. Some of the implications are not obvious and, at first, counterintuitive.It is shown that the dynamics and output equations for plasma shape and current evolution, derived using a common method for linearizing around a plasma equilibrium, are each valid in different coordinates, and therefore additional work is needed to redefine both in a common coordinate system. In particular, it is demonstrated that the set of poloidal field (PF) coil currents that defines the equilibrium about which a model is linearized often does not define a valid origin for the linearized model equations. Requirements for a valid coordinate system are determined, and procedures for constructing such a system are described. We extend this analysis to also cover both cases where the transformed coordinate system is defined relative to a constant origin and where the coordinate origin is a function of time, i.e., to the definition of time-dependent feed-forward nominal trajectories.We also explore the issue of the small signal requirement for maintaining accuracy of the linearized models. It is shown that this requirement does not apply to either coil currents or voltages, but only to certain characteristics of the plasma. In particular, use of a "perturbed" coordinate system is not actually necessary.The primary motivation for this study is to properly account for relatively large changes in PF coil currents needed to maintain plasma shape and plasma current during long pulse discharges when using "small-signal" linearized plasma models. A related objective is to determine conditions under which plasma shape and current controllers must be updated during the discharge to account for the changing plasma response.