The ITER full size plasma source device design

被引:185
作者
Sonato, P. [1 ]
Agostinetti, P. [1 ]
Anaclerio, G. [1 ]
Antoni, V. [1 ]
Barana, O. [1 ]
Bigi, M. [1 ]
Boldrin, M. [1 ]
Cavenago, M. [2 ]
Dal Bello, S. [1 ]
Dalla Palma, M. [1 ]
Daniele, A. [3 ]
D'Arienzo, M. [1 ]
De Lorenzi, A. [1 ]
Ferro, A. [1 ]
Fiorentin, A. [1 ]
Gaio, E. [1 ]
Gazza, E. [1 ]
Grando, L. [1 ]
Fantini, F. [1 ]
Fellin, F. [1 ]
Luchetta, A. [1 ]
Manduchi, G. [1 ]
Milani, F. [1 ]
Marcuzzi, D. [1 ]
Novello, L. [1 ]
Pasqualotto, R. [1 ]
Pavei, M. [1 ]
Pengo, R. [2 ]
Peruzzo, S. [1 ]
Pesce, A. [1 ]
Pilan, N. [1 ]
Piovan, R. [1 ]
Pomaro, N. [1 ]
Recchia, M. [1 ]
Rigato, W. [1 ]
Rizzolo, A. [1 ]
Serianni, G. [1 ]
Spolaore, M. [1 ]
Spolaore, P. [2 ]
Sandri, S. [3 ]
Taliercio, C. [1 ]
Toigo, V. [1 ]
Valisa, M. [1 ]
Veltri, P. [1 ]
Zaccaria, R. [1 ]
Zamengo, A. [1 ]
Zanotto, L. [1 ]
机构
[1] EURATOM ENEA Assoc, Consorzio RFX, I-35127 Padua, Italy
[2] Ist Nazl Fis Nucl, Padua, Italy
[3] ENEA, Rome, Italy
关键词
ITER; Neutral beam; RF source; NEGATIVE-ION SOURCE; RF SOURCE; NBI;
D O I
10.1016/j.fusengdes.2008.11.095
中图分类号
TL [原子能技术]; O571 [原子核物理学];
学科分类号
0827 ; 082701 ;
摘要
In the framework of the strategy for the development and the procurement of the NB systems for ITER, it has been decided to build in Padova a test facility, including two experimental devices: a full size plasma source with low voltage extraction and a full size NB injector at full beam power (1 MV). These two different devices will separately address the main scientific and technological issues of the 17 MW NB injector for ITER. In particular the full size plasma source of negative ions will address the ITER performance requirements in terms of current density and uniformity, limitation of the electron/ion ratio and stationary operation at full current with high reliability and constant performances for the whole operating time up to 1 h. The required negative ion current density to be extracted from the plasma source ranges from 290 A/m(2) in D-2 (D-) and 350 A/m(2) in H-2 (H-) and these values should be obtained at the lowest admissible neutral pressure in the plasma source volume, nominally at 0.3 Pa. The electron to inn ratio should be limited to less than and the admissible ion inhomogeneity extracted from the grids should be better than 10% on the whole plasma cross-section having a surface exposed to the extraction grid of the order of 1 m(2). The main design choices will be presented in the paper as well as an overview of the design of the main components and systems. (C) 2009 P. Sonato. Published by Elsevier B.V. All rights reserved.
引用
收藏
页码:269 / 274
页数:6
相关论文
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