EPJ Web of Conferences
Volume 87, 2015EC18 - 18th Joint Workshop on Electron Cyclotron Emission and Electron Cyclotron Resonance Heating
|Number of page(s)||6|
|Published online||12 March 2015|
Assessment of the ITER EC Upper Launcher Performance
1 Istituto di Fisica del Plasma CNR, 20125, Milano, Italy
2 Max-Planck-Institut för Plasmaphysik, D-85748 Garching, Germany
3 EPFL-CRPP, CH-1015 Lausanne, Switzerland
4 Fusion for Energy, C/ Josep Pla no 2, 08019 Barcelona, Spain
5 ITER Organization, Route de Vinon sur Verdon, 13115 Saint Paul Lez Durance, France
a e-mail: email@example.com
Published online: 12 March 2015
The 24 MW ITER Electron Cyclotron (EC) Heating and Current Drive (H&CD) system, operating at 170 GHz, consists of one Equatorial (EL) and four Upper Launchers (UL). The main task of the UL will be the control of Magneto-Hydrodynamic (MHD) activity such as Neoclassical Tearing Modes (NTMs) at the q=3/2 and q=2 surfaces, but it will also be needed for current profile tailoring in advanced scenarios and to assist plasma break-down and L- to H-mode transition. Moreover, it is required to be e.ective both when ITER will operate at nominal and reduced magnetic field magnitude. Here the performance of the UL is assessed through the study of the full temporal evolution of di.erent scenarios, including the reference ITER 15MA H-mode plasma, a half-field case at 2.65T, and a steady state scenario.
The ECCD efficiency has been evaluated for a wide range of injection angles, deriving the optimal angles and the power required for NTMs stabilization, as well as the steering range necessary to reach the rational surfaces during all the phases of the discharge. The steering sensitivity to shifts of the target or aiming errors has been estimated too. The result is an assessment of the UL design requirements to achieve the desired functionalities, which, together with the engineering limits, will be used to drive the optimization and finalization of the UL design.
© Owned by the authors, published by EDP Sciences, 2015
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