ITER Neutral Beam Test Facility

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View of the Neutral Beam Test Facility View of the Neutral Beam Test Facility building.jpg
View of the Neutral Beam Test Facility

The ITER Neutral Beam Test Facility is a part of the International Thermonuclear Experimental Reactor (ITER) in Padova, Veneto, Italy. [1] The facility will host the full-scale prototype of the reactor's neutral beam injector, MITICA (Megavolt ITer Injector & Concept Advancement), and a smaller prototype of its ion source, SPIDER (Source for the Production of Ions of Deuterium Extracted from a Radio frequency plasma). [2] SPIDER started its operation in June 2018. SPIDER will be used to optimize the ion beam source, to optimize the use of caesium vapor, and to verify the uniformity of the extracted ion beam also during long pulses.

Contents

ITER heating neutral beams

To deliver power to the fusion plasma in ITER, two heating neutral beam injectors will be installed. They are designed to provide the power of 17 MW each, through the 23 m beamlines, up to the four-meter diameter container: in order to deposit sufficient heating power in the plasma core instead of the plasma edges, the beam particle energy shall be about 1 MeV, thus increasing the neutral beam system complexity to an unprecedented level. This will be the main auxiliary heating system of the reactor. Due to its low conversion efficiency, the neutral beam injector first needs to start a precursor negative ion beam of 40 A, and then neutralizes it by passing it through a gas cell (with an efficiency < 60%), and then by a residual ion dump (the remaining 40—20% negative, 20% positive). The neutralized beam is then dumped on a calorimeter during conditioning phases, or coupled with the plasma. Further reionization losses or interception with the mechanical components reduce its current to 17 A. [3]

Purposes

Inside view of the neutral beam test facility; picture taken from the top of MITICA bioshield, during the maintenance of SPIDER (reassembly of SPIDER ongoing in the working area at the center of the picture) Inside view of NBTF.jpg
Inside view of the neutral beam test facility; picture taken from the top of MITICA bioshield, during the maintenance of SPIDER (reassembly of SPIDER ongoing in the working area at the center of the picture)

The role of the test facility includes research and development on the following topics:

Prototypes at the NBTF

Negative ion extraction with reduced number of beamlets, in early volume operation of SPIDER (May/June 2019) SPIDER during negative ion extraction.png
Negative ion extraction with reduced number of beamlets, in early volume operation of SPIDER (May/June 2019)

SPIDER is the first large experimental devices to start the operation at the test facility (May 2018). The components of MITICA are currently under procurement, with its first operation expected in late 2023.

SPIDER

The design parameters of SPIDER are the following:

During 2018, the plasma discharge by eight ion source RF drivers were optimised. In 2019 the operation with hydrogen negative ion beam begun: for the first year, SPIDER will operate with a reduced number of beamlets (80 instead of 1280) due to limitations in the vacuum system. In 2021, the first operation with caesium was performed.

Capabilities

The capabilities of SPIDER and MITICA are listed in the following table in comparison with the objectives of the ITER Heating Neutral Beam and with other existing devices based on RF-driven sources. The obtained results reported in table refers to the operation at low filling pressure of 0.3 Pa; a marked improvement of performances is found for higher operating pressures, but a low pressure is required to minimise the heat loads due to stray particles, generated by interaction of the beam ions with the background gas along the multi-grid electrostatic accelerator of MITICA and ITER HNB sources.

ExperimentFirst operationBeam energy (achieved/ target)negative ion beam current (achieved/ target)negative ion beam current density (achieved/ target)Ion source typeAccelerator typeNeutraliser typeBeamline lengthNeutral beam equivalent currentTarget single beamlet divergence at 0.3 Pa (gaussian 1/e)Achieved single beamlet divergence at 0.3 Pa ±10% (gaussian 1/e)
BATMAN Upgrade [4] upgraded in 2018~60 kV ? (hydrogen)350 A/m2 [5] / 330 A/m2 (hydrogen)RF-driven caesiated surface-plasma sourceMulti-aperture electrostatic triode-~3 m--11 mrad (core divergence including ~75% beamlet current)
ELISE [6] Feb 2013~60 kV~27 A (hydrogen)~280 A/m2 [7] / 330 A/m2 (hydrogen)RF-driven caesiated surface-plasma sourceMulti-aperture electrostatic triode-~5 m---
SPIDERMay 201850 kV [8] / 110 kV~1 A [8] / 54 A (hydrogen)225 A/m2 [8] / 330 A/m2 (hydrogen)RF-driven caesiated surface-plasma sourceMulti-aperture electrostatic triode-~5 m-<7 mrad12 mrad [8]
MITICA2025 (expected)880 kV (hydrogen) / 1000 kV (deuterium)-/ 40 A (hydrogen)-/ 330 A/m2 (hydrogen)RF-driven caesiated surface-plasma sourceMulti-grid multi-aperture concept (7 electrodes)4 Gas cells~13 m16.7 A<7 mrad-
ITER HNBTBD880 kV (hydrogen) / 1000 kV (deuterium)40 A-/ 330 A/m2 (hydrogen)RF-driven caesiated surface-plasma sourceMulti-grid multi-aperture concept (7 electrodes)4 Gas cells~22.5 m16.7 A<7 mrad-

See also

References

  1. ↑ "ITER Neutral Beam Test Facility: Construction is progressing fast in Padova". EUROfusion. 15 July 2013. Archived from the original on 2016-01-27. Retrieved 2023-11-05.
  2. ↑ V. Toigo, D. Boilson, T. Bonicelli, R. Piovan, M. Hanada, et al. 2015 Nucl. Fusion 55:8 083025
  3. ↑ LR Grisham, P Agostinetti, G Barrera, P Blatchford, D Boilson, J Chareyre, et al., Recent improvements to the ITER neutral beam system design, Fusion Engineering and Design 87 (11), 1805-1815
  4. ↑ Fantz, U.; Bonomo, F.; Fröschle, M.; Heinemann, B.; Hurlbatt, A.; Kraus, W.; Schiesko, L.; Nocentini, R.; Riedl, R.; Wimmer, C. (2019). "Advanced NBI beam characterization capabilities at the recently improved test facility BATMAN Upgrade". Fusion Engineering and Design. 146: 212–215. Bibcode:2019FusED.146..212F. doi:10.1016/j.fusengdes.2018.12.020. hdl: 21.11116/0000-0004-8043-F .
  5. ↑ Heinemann, B.; Fantz, U.; Kraus, W.; Schiesko, L.; Wimmer, C.; Wünderlich, D.; Bonomo, F.; Fröschle, M.; Nocentini, R.; Riedl, R. (2017). "Towards large and powerful radio frequency driven negative ion sources for fusion". New Journal of Physics. 19 (1): 015001. Bibcode:2017NJPh...19a5001H. doi: 10.1088/1367-2630/aa520c .
  6. ↑ World's largest test facility for negative ion sources opens to develop heating for ITER – December 2012 Archived 2019-08-02 at the Wayback Machine . Retrieved on 2019-08-02.
  7. ↑ Fantz, U.; Briefi, S.; Heiler, A.; Wimmer, C.; Wünderlich, D. (2021). "Negative Hydrogen Ion Sources for Fusion: From Plasma Generation to Beam Properties". Frontiers in Physics. 9: 473. Bibcode:2021FrP.....9..473F. doi: 10.3389/fphy.2021.709651 .
  8. 1 2 3 4 Sartori, E.; Agostini, M.; Barbisan, M.; Bigi, M.; Boldrin, M.; Brombin, M.; Casagrande, R.; Dal Bello, S.; Dan, M.; Duteil, B.P.; Fadone, M.; Grando, L.; Maistrello, A.; Pavei, M.; Pimazzoni, A. (2022). "First operations with caesium of the negative ion source SPIDER". Nuclear Fusion. 62 (8): 086022. Bibcode:2022NucFu..62h6022S. doi:10.1088/1741-4326/ac715e. hdl: 11577/3448494 . ISSN   0029-5515.

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