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Second round of Launch Pad selections includes eight newcomers
The National Reactor Innovation Center at Idaho National Laboratory has announced 13 project selections across 12 companies for the Nuclear Energy Launch Pad, a Department of Energy–led program that integrates reactor and fuel facility authorization, testing, and deployment support for private nuclear developers.
The Launch Pad emerged from the Reactor Pilot Program and Fuel Line Pilot Program.
According to INL, projects selected include reactor development and nuclear fuel cycle advancements, including fabrication, enrichment, and conversion technologies.
A. V. Melnikov, C. Hidalgo, A. A. Chmyga, N. B. Dreval, L. G. Eliseev, S. M. Khrebtov, A. D. Komarov, A. S. Kozachok, L. I. Krupnik, I. Pastor, M. A. Pedrosa, S. V. Perfilov, K. McCarthy, M. A. Ochando, G. Van Oost, C. Silva, B. Goncalves, Yu. N. Dnestrovskij, S. E. Lysenko, M. V. Ufimtsev, V. I. Tereshin
Fusion Science and Technology | Volume 46 | Number 2 | September 2004 | Pages 299-311
Technical Papers | Stellarators | doi.org/10.13182/FST04-A568
Articles are hosted by Taylor and Francis Online.
The effect of edge biasing on plasma potential was investigated in the TJ-II stellarator and the T-10 tokamak. The Heavy Ion Beam Probe (HIBP) diagnostic, a unique tool for studying the core potential directly, was used in both machines. Experiments in TJ-II show that it is possible to modify the global confinement and edge plasma parameters with limiter biasing, illustrating the direct impact of radial electric fields on TJ-II confinement properties. For the first time it was shown that the plasma column in a stellarator can be charged as a whole for a hot, near-reactor-relevant plasma. The plasma potential and electric fields evolve on two different characteristic time scales. Although the experimental conditions in the two machines have many important differences, the basic features of plasma potential behavior have some similarities: The potential response has the same polarity and scale as the biasing voltage, and the fluctuations are suppressed near the electrode/limiter region. However, whereas both edge and core plasma potential are affected by biasing in TJ-II, the potential changes mainly near the biased electrode in T-10.