Assessing the Power Requirements for Sawtooth Control in ITER through Modelling and Joint Experiments
Creators
- 1. CCFE, Abingdon (United Kingdom)
- 2. CRPP, Lausanne (Switzerland)
- 3. MPI fuer Plasmaphysik, Garching (Germany)
- 4. General Atomics, San Diego (United States)
- 5. Aalto University, Aalto (Finland)
- 6. IRFM, CEA, St Paul-Lez-Durance (France)
- 7. Euratom/VR Association, EES, KTH, Stockholm (Sweden)
- 8. JET-EFDA, Culham Science Centre, Abingdon (United Kingdom)
Description
Full text: Recent advances in theoretical understanding and numerical modelling of sawtooth oscillations have allowed the invention and application of experimental control techniques. This enhanced understanding, coupled with demonstration of control techniques in ITER-relevant plasmas and using real-time feedback, has facilitated prediction of control actuator requirements for ITER. The control of sawteeth is important for baseline scenario operation of burning plasmas, since plasmas with long sawtooth periods are empirically more susceptible to neoclassical tearing modes, which result in substantial confinement degradation. The stabilising effects of alpha particles are likely to exacerbate this, so recent experiments have identified methods for amelioration. Sawtooth control using electron cyclotron current drive has been demonstrated in ITER-like plasmas with a large fast ion fraction, wide q = 1 radius and long uncontrolled sawtooth period in DIII-D and ASDEX Upgrade. Operation at βN = 3 without NTMs has been achieved in ITER demonstration plasmas in DIII-D using only modest ECCD power for sawtooth control. Further, real-time ECCD control techniques have been developed in TCV and Tore Supra. Numerical modelling suggests that the achieved driven current changes the local magnetic shear sufficiently to compensate for the stabilising influence of the fast particles. Extrapolating this to ITER, transport modelling coupled to ray-tracing predictions and using the linear stability thresholds for sawtooth onset suggests that 13 MW of ECCD could be sufficient to reduce the sawtooth period by 30%, and this being the case, dropping it below the NTM triggering threshold. However, since the ECCD control scheme is solely predicated upon changing the local magnetic shear, it is prudent to plan for 10 MW off-axis ICRH using 3He minority as a complementary scheme which directly damps the internal kink potential energy drive responsible for trapped fast ion stabilisation. Experimental evidence from JET plasmas heated with toroidally propagating ICRH using a 3He minority exhibited sawtooth control avoiding NTMs in H-mode, as predicted by drift-kinetic modelling. Such modelling suggests that 10 MW of ICRH in ITER will negate the stabilising effect of alphas. JET EFDA Contributors: See the Appendix of F. Romanelli et al., Proceedings of the 23rd IAEA Fusion Energy Conference 2010, Daejeon, Republic of Korea. (author)
Additional details
Publishing Information
- Imprint Title
- 24. IAEA Fusion Energy Conference. Programme and Book of Abstracts
- Imprint Pagination
- 789 p.
- Journal Page Range
- p. 588
- Report number
- IAEA-CN--197
Conference
- Title
- 24. IAEA Fusion Energy Conference
- Acronym
- FEC 2012
- Dates
- 8-13 Oct 2012
- Place
- San Diego, CA (United States)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 45034007
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference
- Descriptors DEI
- ALPHA PARTICLES; ASDEX TOKAMAK; CONTROL; CURRENTS; DOUBLET-3 DEVICE; ECR CURRENT DRIVE; HELIUM 3; H-MODE PLASMA CONFINEMENT; ICR HEATING; IONS; ITER TOKAMAK; NEOCLASSICAL TRANSPORT THEORY; PLASMA; POTENTIAL ENERGY; SAWTOOTH OSCILLATIONS; TCV TOKAMAK; TEARING INSTABILITY; TORE SUPRA TOKAMAK
- Descriptors DEC
- CHARGED PARTICLES; CHARGED-PARTICLE TRANSPORT THEORY; CLOSED PLASMA DEVICES; CONFINEMENT; ENERGY; EVEN-ODD NUCLEI; HEATING; HELIUM ISOTOPES; HIGH-FREQUENCY HEATING; INSTABILITY; IONIZING RADIATIONS; ISOTOPES; LIGHT NUCLEI; MAGNETIC CONFINEMENT; NON-INDUCTIVE CURRENT DRIVE; NUCLEI; OSCILLATIONS; PLASMA CONFINEMENT; PLASMA HEATING; PLASMA INSTABILITY; PLASMA MACROINSTABILITIES; RADIATIONS; STABLE ISOTOPES; THERMONUCLEAR DEVICES; THERMONUCLEAR REACTORS; TOKAMAK DEVICES; TOKAMAK TYPE REACTORS; TRANSPORT THEORY