29 June 2026 to 3 July 2026
EICC, Edinburgh
Europe/London timezone

ICRF power coupling and absorption in full- and reduced-field scenarios for SPARC’s first campaign

Not scheduled
20m
EICC, Edinburgh

EICC, Edinburgh

150 Morrison St, Edinburgh EH3 8EE
Poster Presentation Scenario Development, Heating and Current Drive (MCF)

Description

SPARC, a medium-sized high-field tokamak, is under assembly and preparation for its first campaign, which aims to demonstrate net fusion energy. Operation at both the full 12.2 T field and a reduced ~8.5-8.9 T field is considered. The operational points are governed by the resonance conditions required for delivering power to plasma from the only auxiliary heating system in SPARC, Ion Cyclotron Range of Frequencies (ICRF) heating, which operates at 120±1 MHz. The corresponding heating schemes are ³He minority (plus harmonic T) for the ~12 T scenario and H minority (plus harmonic D and T) for the ~8 T scenario. 20 MW of ICRF power will be installed for the first campaign, with 10 antennas delivering power to the plasma. Both L- and H-mode plasmas are planned on the path to achieving Q>1. For H-mode operation, the ICRF heating must meet the requirements of the L-H transition power threshold, sustain the H-mode, deliver power robustly in the presence of ELMs, and steer the plasma into the Q>1 operational space.
In this contribution, we present an analysis of ICRF power coupling – through impedance match tuning and edge density tailoring – as well as core power absorption via parameter scans of resonance location, minority species concentration, antenna wave spectrum, and core plasma profiles. The effects of ICRF fast ions on heating efficiency, fusion gain enhancement, and sawtooth stabilisation are studied to obtain a self-consistent picture of ICRF interaction with the plasma. In the all-metal-wall device, tungsten sputtering and accumulation are concerns which might limit the operational range for both ICRF power level and plasma profiles. Prediction and minimisation of sputtering associated with ICRF physics processes are carried out using RF sheath modelling, near-field optimisation and extrapolation of sputtering rates from ASDEX Upgrade experimental data to SPARC.

Author

Maria Usoltseva (Commonwealth Fusion Systems)

Co-authors

Dr Anna A. Teplukhina (Commonwealth Fusion Systems) Dr Christina Migliore (Plasma Science and Fusion Center, MIT) Dr Erik Johnson (Commonwealth Fusion Systems) Dr Gregory M. Wallace (Plasma Science and Fusion Center, MIT) Dr John C. Wright (Plasma Science and Fusion Center, MIT) Dr Markus Weiland (Max-Planck-Institut für Plasmaphysik) Dr Michael Garrett (Commonwealth Fusion Systems) Mr Michael Sieben (Max-Planck-Institut für Plasmaphysik) N. Howard (MIT Plasma Science and Fusion Center) Dr Peter Matthews (Commonwealth Fusion Systems) Phil Snyder (Commonwealth Fusion Systems) Roberto Bilato (Max Planck Institute for Plasma Physics, Germany) Dr Volodymyr Bobkov (Max-Planck-Institut für Plasmaphysik)

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