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Sökning: WFRF:(Rigamonti D) > (2023) > Experiments in high...

Experiments in high-performance JET plasmas in preparation of second harmonic ICRF heating of tritium in ITER

Mantsinen, M. J. (författare)
Barcelona Supercomp Ctr, Barcelona, Spain.;ICREA, Barcelona, Spain.
Jacquet, P. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Lerche, E. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.;ERM KMS, Plasma Phys Lab, B-1000 Brussels, Belgium.
visa fler...
Gallart, D. (författare)
Barcelona Supercomp Ctr, Barcelona, Spain.
Kirov, K. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Mantica, P. (författare)
CNR, Inst Plasma Sci & Technol, I-20125 Bari, Italy.
Taylor, D. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Van Eester, D. (författare)
ERM KMS, Plasma Phys Lab, B-1000 Brussels, Belgium.
Baruzzo, M. (författare)
ENEA, Fus & Nucl Safety Dept, CR Frascati, I-00044 Frascati, Italy.
Carvalho, I. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Challis, C. D. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Dal Molin, A. (författare)
CNR, Inst Plasma Sci & Technol, I-20125 Bari, Italy.
Delabie, E. (författare)
Oak Ridge Natl Lab, Oak Ridge, TN 37830 USA.
de la Luna, E. (författare)
CIEMAT, Lab Nacl Fus, Madrid 28040, Spain.
Dumont, R. (författare)
CEA, IRFM, F-13108 St Paul Les Durance, France.
Dumortier, P. (författare)
ERM KMS, Plasma Phys Lab, B-1000 Brussels, Belgium.
Eriksson, Jacob, Dr, 1985- (författare)
Uppsala universitet,Tillämpad kärnfysik
Frigione, D. (författare)
Univ Tor Vergata, Rome, Italy.
Garcia, J. (författare)
CEA, IRFM, F-13108 St Paul Les Durance, France.
Garzotti, L. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Giroud, C. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Henriques, R. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Hobirk, J. (författare)
Max Planck Inst Plasma Phys, Boltzmannstr 2, D- 85748 Garching, Germany.
Kappatou, A. (författare)
Max Planck Inst Plasma Phys, Boltzmannstr 2, D- 85748 Garching, Germany.
Kazakov, Y. (författare)
ERM KMS, Plasma Phys Lab, B-1000 Brussels, Belgium.
Keeling, D. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
King, D. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Kiptily, V. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Lennholm, M. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Lomas, P. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Lowry, C. (författare)
European Commiss, B-1049 Geel, Belgium.
Maggi, C. F. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Mailloux, J. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Maslov, M. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Menmuir, S. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Monakhov, I. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Morales, R. B. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Noble, C. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Nocente, M. (författare)
CNR, Inst Plasma Sci & Technol, I-20125 Bari, Italy.;Univ Milano Bicocca, Dipartimento Fis G Occhialini, Milan, Italy.
Patel, A. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Pucella, G. (författare)
ENEA, Fus & Nucl Safety Dept, CR Frascati, I-00044 Frascati, Italy.
Reux, C. (författare)
CEA, IRFM, F-13108 St Paul Les Durance, France.
Rigamonti, D. (författare)
CNR, Inst Plasma Sci & Technol, I-20125 Bari, Italy.
Rimini, F. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Sheikh, A. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Silburn, S. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Siren, P. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.
Solano, E. R. (författare)
CIEMAT, Lab Nacl Fus, Madrid 28040, Spain.
Stancar, Z. (författare)
United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England.;Slovenian Fus Assoc SFA, Jozef Stefan Inst, SI-1000 Ljubljana, Slovenia.
Tardocchi, M. (författare)
CNR, Inst Plasma Sci & Technol, I-20125 Bari, Italy.
visa färre...
Barcelona Supercomp Ctr, Barcelona, Spain;ICREA, Barcelona, Spain. United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England. (creator_code:org_t)
Institute of Physics (IOP), 2023
2023
Engelska.
Ingår i: Nuclear Fusion. - : Institute of Physics (IOP). - 0029-5515 .- 1741-4326. ; 63:11
  • Tidskriftsartikel (refereegranskat)
Abstract Ämnesord
Stäng  
  • The reference ion cyclotron resonance frequency (ICRF) heating schemes for ITER deuterium-tritium (D-T) plasmas at the full magnetic field of 5.3 T are second harmonic heating of T and 3He minority heating. The wave-particle resonance location for these schemes coincide and are central at a wave frequency of 53 MHz at 5.3 T. Experiments have been carried out in the second major D-T campaign (DTE2) at JET, and in its prior D campaigns, to integrate these ICRF scenarios in JET high-performance plasmas and to compare their performance with the commonly used hydrogen (H) minority heating. In 50:50 D:T plasmas, up to 35% and 5% larger fusion power and diamagnetic energy content, respectively, were obtained with second harmonic heating of T as compared to H minority heating at comparable total input powers and gas injection rates. The core ion temperature was up to 30% and 20% higher with second harmonic T and 3He minority heating, respectively, with respect to H minority heating. These are favourable results for the use of these scenarios in ITER and future fusion reactors. According to modelling, adding ICRF heating to neutral beam injection using D and T beams resulted in a 10%-20% increase of on-axis bulk ion heating in the D-T plasmas due to its localisation in the plasma core. Central power deposition was confirmed with the break-in-slope and fast Fourier transform analysis of ion and electron temperature in response to ICRF modulation. The tail temperature of fast ICRF-accelerated tritons, their enhancement of the fusion yield and time behaviour as measured by an upgraded magnetic proton recoil spectrometer and neutral particle analyser were found in agreement with theoretical predictions. No losses of ICRF-accelerated ions were observed by fast ion detectors, which was as expected given the high plasma density of n e approximate to 7-8 x 1019 m-3 in the main heating phase that limited the formation of ICRF-accelerated fast ion tails. 3He was introduced in the machine by 3He gas injection, and the 3He concentration was measured by a high-resolution optical penning gauge in the sub-divertor region. The DTE2 experiments with 3He minority heating were carried with a low 3He concentration in the range of 2%-4% given the fact that the highest neutron rates with 3He minority heating in D plasmas were obtained at low 3He concentrations of similar to 2%, which also coincided with the highest plasma diamagnetic energy content. In addition to 3He introduced by 3He gas injection, an intrinsic concentration of 3He of the order of 0.2%-0.4% was measured in D-T plasmas before 3He was introduced in the device, which is attributed to the radioactive decay of tritium to 3He. According to modelling, even such low intrinsic concentrations of 3He lead to significant changes in ICRF power partitioning during second harmonic heating of T due to absorption of up to 30% of the wave power by 3He.

Ämnesord

NATURVETENSKAP  -- Fysik -- Fusion, plasma och rymdfysik (hsv//swe)
NATURAL SCIENCES  -- Physical Sciences -- Fusion, Plasma and Space Physics (hsv//eng)

Nyckelord

ICRF heating
fast ions
computational modelling
JET tokamak
H-mode hybrid plasma scenario
deuterium-tritium fuel mixture

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