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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.
André L. Rogister
Fusion Science and Technology | Volume 37 | Number 2 | March 2000 | Pages 239-248
Instabilities and Transport | doi.org/10.13182/FST00-A11963219
Articles are hosted by Taylor and Francis Online.
Most experts consider that the causes of anomalous energy and particle transport in fusion devices are low frequency “drift” waves, themselves driven unstable by the equilibrium gradients and the associated drifts across the confining magnetic field (hence the terminology). We first introduce the dimensionless parameters which characterize drift waves (drift ordering). We then accordingly simplify the conventional two fluids description and obtain the general eigenvalue equations for drift eigenmodes. We finally search for solutions with angular frequency ω~ω* (the diamagnetic drift frequency), ω~λω*, etc … assuming λ≡LN(T)/qR ≪ 1 [LN(T) is the density (temperature) gradient length and qR is the connection length]. We recover in this way both the electron and the ion drift branches. The poloidal variation of the magnetic field has two opposite effects on the growth (damping) rate according to whether the width of the modes is larger or smaller than the distance between the rational surfaces q(r)=m/ℓ and q(r+Δ)=(m+l)/ℓ. Kinetic effects and the role of trapped particles are not described by the two fluid description but could be readily included.