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Deep Space: The new frontier of radiation controls
In commercial nuclear power, there has always been a deliberate tension between the regulator and the utility owner. The regulator fundamentally exists to protect the worker, and the utility, to make a profit. It is a win-win balance.
From the U.S. nuclear industry has emerged a brilliantly successful occupational nuclear safety record—largely the result of an ALARA (as low as reasonably achievable) process that has driven exposure rates down to what only a decade ago would have been considered unthinkable. In the U.S. nuclear industry, the system has accomplished an excellent, nearly seamless process that succeeds to the benefit of both employee and utility owner.
A. V. Melnikov, A. Alonso, E. Ascasíbar, R. Balbin, A. A. Chmyga, Yu. N. Dnestrovskij, L. G. Eliseev, T. Estrada, J. M. Fontdecaba, C. Fuentes, J. Guasp, J. Herranz, C. Hidalgo, A. D. Komarov, A. S. Kozachek, L. I. Krupnik, M. Liniers, S. E. Lysenko, K. J. McCarthy, M. A. Ochando, I. Pastor, J. L. De Pablos, M. A. Pedrosa, S. V. Perfilov, S. Ya. Petrov, V. I. Tereshin, TJ-II Team
Fusion Science and Technology | Volume 51 | Number 1 | January 2007 | Pages 31-37
Technical Paper | Stellarators | doi.org/10.13182/FST07-A1284
Articles are hosted by Taylor and Francis Online.
The heavy ion beam probe diagnostic is used in the TJ-II stellarator to study directly the plasma electric potential with good spatial (up to 1 cm) and temporal (up to 2 s) resolution. Singly charged heavy ions, Cs+, with energies of up to 125 keV are used to probe the plasma column from the edge to the core. Both electron cyclotron resonance heating (ECRH) and neutral beam injection (NBI)-heated plasmas (PECRH = 200 to 400 kW, PNBI = 200 to 400 kW, ENBI = 28 keV) have been studied.Low-density ECRH [[over bar]n = (0.5 to 1.1) × 1019 m-3] plasmas in TJ-II are characterized by positive plasma potential on the order of 1000 to 400 V. A negative electric potential appears at the edge when the line-averaged density exceeds 0.5 × 1019 m-3. Further density rises are accompanied by a decrease in the core plasma potential, which becomes fully negative for plasma densities [over bar]n 1.5 × 1019 m-3. The NBI plasmas are characterized by a negative electric potential across the whole plasma cross section from the core to the edge. In this case, the absolute value of the central potential is on the order of -500 V. These results show a clear link between plasma potential and density in the TJ-II stellarator.
