Assessment of the ITER electron cyclotron upper launcher capabilities in view of an optimized design

The 24 MW ITER electron cyclotron (EC) heating and current drive (H and CD) system, operating at 170 GHz, consists of one equatorial and four upper launchers (UL). The main task of the UL will be the control of magneto-hydrodynamic activity such as neoclassical tearing modes (NTMs) at the q = 3/2 and q = 2 surfaces and sawteeth at q = 1, 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 effective both when ITER will operate at nominal and reduced magnetic field magnitude.Here the performance of the UL has been assessed through the study of the full temporal evolution of different scenarios, including the reference ITER 15 MA H-mode plasma, a half-field case at 2.65 T 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 with simplified criteria. An injected power ranging from 3 MW to 9 MW should be sufficient to control NTMs in the flat-top phase of the scenarios considered here. The result of the analysis shows that the EC system maintains a good performance level even at intermediate values of the magnetic field, between the nominal and the half-field value. The analysis has also allowed to evaluate the adequateness of the available steering range for reaching the rational surfaces during all the phases of the discharge and to quantify the steering sensitivity to shifts of the target or aiming errors. The result is an assessment of the UL design requirements to achieve the desired functionalities, which will be used to drive the optimization and finalization of the UL design.

[1]  Daniela Farina,et al.  A Quasi-Optical Beam-Tracing Code for Electron Cyclotron Absorption and Current Drive: GRAY , 2007 .

[2]  T. Goodman,et al.  Guidelines for internal optics optimization of the ITER EC H&CD upper launcher , 2014 .

[3]  Timothy Goodman,et al.  On recent results in the modelling of neoclassical-tearing-mode stabilization via electron cyclotron current drive and their impact on the design of the upper EC launcher for ITER , 2015 .

[4]  G. V. Pereverzev,et al.  Beam tracing in inhomogeneous anisotropic plasmas , 1998 .

[5]  Omar Maj,et al.  The wave energy flux of high frequency diffracting beams in complex geometrical optics , 2013 .

[6]  Olivier Sauter,et al.  Physics analysis of the ITER ECW system for optimized performance , 2008 .

[7]  V. Erckmann,et al.  Ray Tracing Simulations of ECR Heating and ECE Diagnostic at W7-X Stellarator , 2007 .

[8]  Lorenzo Figini,et al.  Potential of the ITER electron cyclotron equatorial launcher for heating and current drive at nominal and reduced fields , 2012 .

[9]  Paul H. Rutherford,et al.  Nonlinear growth of the tearing mode , 1973 .

[10]  Olivier Sauter,et al.  On the requirements to control neoclassical tearing modes in burning plasmas , 2010 .

[11]  Daniela Farina,et al.  Benchmarking of electron cyclotron heating and current drive codes on ITER scenarios within the European Integrated Tokamak Modelling framework , 2012 .

[12]  G. Gantenbein,et al.  Control of NTMs by ECCD on ASDEX Upgrade in view of ITER application , 2007 .

[13]  Harvey,et al.  Power dependence of electron-cyclotron current drive for low- and high-field absorption in tokamaks. , 1989, Physical review letters.

[14]  Lorenzo Figini,et al.  The targeted heating and current drive applications for the ITER electron cyclotron system , 2015 .

[15]  M. A. Henderson,et al.  ITER ECRH-ECCD System Capabilities for Extended Physics Applications , 2007 .

[16]  L Garzotti,et al.  Self-consistent simulation of plasma scenarios for ITER using a combination of 1.5D transport codes and free-boundary equilibrium codes , 2013 .

[17]  Lorenzo Figini,et al.  Optimization of the ITER electron cyclotron equatorial launcher for improved heating and current drive functional capabilities , 2014 .

[18]  L. L. Lao,et al.  Beta limits in long-pulse tokamak discharges , 1997 .

[19]  R. W. Harvey,et al.  Benchmarking of codes for electron cyclotron heating and electron cyclotron current drive under ITER conditions , 2008 .

[20]  Nicola Bertelli,et al.  Requirements on localized current drive for the suppression of neoclassical tearing modes , 2011 .

[21]  Giovanni Ramponi,et al.  Overview of the ITER EC upper launcher , 2008 .