Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session UO5: Research in Support of ITER
2:00 PM–5:00 PM,
Thursday, November 8, 2018
OCC
Room: B113-114
Chair: Francesca Turco, Columbia University
Abstract ID: BAPS.2018.DPP.UO5.15
Abstract: UO5.00015 : The Development of First Plasma Operations on ITER
4:48 PM–5:00 PM
Presenter:
Joseph Snipes
(ITER Organization)
Authors:
Joseph Snipes
(ITER Organization)
Himank Anand
(ITER Organization)
Ken Blackler
(ITER Organization)
Peter C de Vries
(ITER Organization)
Juan Luis Fernandez-Hernando
(ITER Organization)
Yuri Gribov
(ITER Organization)
Mark Andrew Henderson
(ITER Organization)
Jean-Yves Journeaux
(ITER Organization)
Tim Luce
(ITER Organization)
Ignacio Prieto-diaz
(ITER Organization)
Anders Wallander
(ITER Organization)
Luca Zabeo
(ITER Organization)
Isabel Nunes
(IST Lisbon Portugal)
ITER construction is well underway and first plasma operations are planned at the end of 2025. Plant system commissioning has begun and will proceed up to the closure of the cryostat in late 2024, which defines the start of integrated commissioning, including that of the Central Interlock System (CIS), the Plasma Control System (PCS), and associated diagnostics to ensure investment protection and central control functions can be carried out. An independent system will also be commissioned for superconducting magnet protection to avoid approaching force, field, and temperature limits. First plasma scenarios in hydrogen with BT = 2.65 T will first attempt Ohmic breakdown within a neutral pressure range of 0.3 mPa < p < 0.7 mPa, limited by runaways at the low end and by inability to ensure Ip ≥ 100 kA for ≥ 100 ms at the high end. If Ohmic breakdown is unsuccessful, electron cyclotron heating will be added in 0.83 MW steps for short pulses (< 300 ms), possibly up to 6.7 MW injected at 2nd harmonic. The PCS must ensure that Ip < 1 MA to stay within structural limits of the vacuum vessel supports to the temporary poloidal stainless steel limiters. A backup option to improve breakdown is to operate at full toroidal field of 5.3 T with 1st harmonic ECH after magnet commissioning.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.UO5.15
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