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  Steady state advanced scenarios at ASDEX Upgrade

Sips, A. C. C., Arslanbekov, R., Atanasiu, C., Becker, W., Becker, G., Behler, K., et al. (2002). Steady state advanced scenarios at ASDEX Upgrade. Plasma Physics and Controlled Fusion, 44(Suppl. 12B), B69-B83.

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Sips, A. C. C.1, Author           
Arslanbekov, R.2, Author           
Atanasiu, C.3, Author
Becker, W.4, Author           
Becker, G.5, Author           
Behler, K.6, Author                 
Behringer, K.7, Author           
Bergmann, A.5, Author           
Bilato, R.5, Author           
Bolshukhin, D.8, Author
Borrass, K.9, Author           
Braams, B.3, Author
Brambilla, M.5, Author           
Braun, F.4, Author           
Buhler, A.1, Author           
Conway, G.1, Author           
Coster, D.5, Author           
Drube, R.6, Author           
Dux, R.7, Author           
Egorov, S.8, Author
more..
Affiliations:
1Experimental Plasma Physics 1 (E1), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856295              
2External Organizations, ou_persistent22              
3Princeton Univ, Princeton, NJ 08544 USA; Tech Univ St Petersburg, CIS, St Petersburg, Russia; Univ Augsburg, D-8900 Augsburg, Germany; Natl Univ Ireland Univ Coll Cork, Cork, Ireland; Lawrence Livermore Natl Lab, Livermore, CA USA; Univ Stuttgart, IPF, D-7000 Stuttgart, Germany; EURATOM, IST, Lisbon, Portugal; IAP, Vienna, Austria; VTT Tekes, HUT Tekes, Helsinki, Finland, ou_persistent22              
4Technology (TE), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856318              
5Tokamak Theory (TOK), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856309              
6Experimental Plasma Physics 2 (E2), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856292              
7Experimental Plasma Physics 4 (E4), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856293              
8Max Planck Society, ou_persistent13              
9Tokamak Theory (TOK), Max Planck Institute for Plasma Physics, Max Planck Society, ou_persistent22              
10Experimental Plasma Physics 3 (E3), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856291              
11Tokamak: Edge and Divertor Physics (E2), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856308              
12Material Research (MF), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856328              
13Plasma Diagnostics Group (HUB), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856324              
14W7-X: Physics (PH), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856305              
15Tokamak Edge and Divertor Physics (E2), Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856308              
16Relativistic Plasmas, Max Planck Institute for Plasma Physics, Max Planck Society, ou_1856330              

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 Abstract: Recent experiments at ASDEX Upgrade have achieved advanced scenarios with high beta(N) (> 3) and confinement enhancement over ITER98(y, 2) scaling, H-H98y2 = 1.1-1.5, in steady state. These discharges have been obtained in a modified divertor configuration for ASDEX Upgrade, allowing operation at higher triangularity, and with a changed neutral beam injection (NBI) system, for a more tangential, off-axis beam deposition. The figure of merit, beta(N)H(ITER89-P) reaches up to 7.5 for several seconds in plasmas approaching stationary conditions. These advanced tokamak discharges have low magnetic shear in the centre, with q on-axis near 1, and edge safety factor, q(95) in the range 3.3-4.5. This q-profile is sustained by the bootstrap current, NBI-driven current and fishbone activity in the core. The off-axis heating leads to a strong peaking of the density profile and impurity accumulation in the core. This can be avoided by adding some central heating from ion cyclotron resonance heating or electron cyclotron resonance heating, since the temperature profiles are stiff in this advanced scenario (no internal transport barrier). Using a combination of NBI and gas fuelling line, average densities up to 80-90% of the Greenwald density are achieved, maintaining good confinement. The best integrated results in terms of confinement, stability and ability to operate at high density are obtained in highly shaped configurations, near double null, with delta = 0.43. At the highest densities, a strong reduction of the edge localized mode activity similar to type 11 activity is observed, providing a steady power load on the divertor, in the range of 6 MW m(-2), despite the high input power used (> 10 MW).

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Language(s): eng - English
 Dates: 2002
 Publication Status: Issued
 Pages: -
 Publishing info: -
 Table of Contents: -
 Rev. Type: Peer
 Identifiers: eDoc: 21225
ISI: 000180907400009
 Degree: -

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Title: Plasma Physics and Controlled Fusion
  Alternative Title : Plasma Phys. Control. Fusion
Source Genre: Journal
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Pages: - Volume / Issue: 44 (Suppl. 12B) Sequence Number: - Start / End Page: B69 - B83 Identifier: ISSN: 0741-3335