Isotope physics of heat and particle transport with tritium in JET-ILW type-I ELMy H-mode plasmas

被引:18
|
作者
Schneider, P. A. [1 ]
Angioni, C. [1 ]
Auriemma, F. [2 ,3 ]
Bonanomi, N. [1 ]
Goerler, T. [1 ]
Henriques, R. [4 ,5 ]
Horvath, L. [5 ,6 ]
King, D. [5 ]
Lorenzini, R. [2 ,3 ]
Nystrom, H. [7 ]
Maslov, M. [5 ]
Ruiz, J. [8 ]
Szepesi, G. [5 ]
Challis, C. D. [5 ]
Chomiczewska, A. [9 ]
Delabie, E. [10 ]
Fontdecaba, J. M. [11 ]
Frassinetti, L. [7 ]
Garcia, J. [12 ]
Giroud, C. [5 ]
Hillesheim, J. [5 ]
Hobirk, J. [1 ]
Kappatou, A. [1 ]
Keeling, D. L. [5 ]
Kowalska-Strzeciwilk, E. [9 ]
Lennholm, M. [5 ]
Lomanowski, B. [10 ]
Luda di Cortemiglia, T. [1 ]
Maggi, C. F. [5 ]
Menmuir, S. [5 ]
Pucella, G. [13 ]
Thorman, A. [5 ]
机构
[1] Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany
[2] Univ Padua, Consorzio RFX CNR, Acciaierie Venete SpA, ENEA,INFN, Padua, Italy
[3] CNR ISTP, Corso Stati Uniti 4, I-35127 Padua, Italy
[4] Univ Lisbon, Inst Super Tecn, Inst Plasmas & Fusao Nucl, P-1049001 Lisbon, Portugal
[5] United Kingdom Atom Energy Author, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England
[6] Princeton Plasma Phys Lab, Princeton, NJ 08540 USA
[7] KTH Royal Inst Technol, Teknikringen 31, Stockholm, Sweden
[8] Univ Oxford, Rudolf Peierls Ctr Theoret Phys, Oxford OX1 3PU, England
[9] Inst Plasma Phys & Laser Microfus, Warsaw, Poland
[10] Oak Ridge Natl Lab, Oak Ridge, TN USA
[11] Lab Nacl Fus Ciemat, E-28040 Madrid, Spain
[12] CEA, IRFM, F-13108 St Paul Les Durance, France
[13] ENEA CR Frascati, Dip Fus & Tecnol Sicurezza Nucl, Via E Fermi 45, I-00044 Frascati, Roma, Italy
基金
英国工程与自然科学研究理事会;
关键词
H-mode; tritium; heat transport; particle transport; stability; isotopes; ASDEX UPGRADE; CONFINEMENT; COLLISIONALITY; ELECTRON; PEAKING; IMPACT; SHEAR;
D O I
10.1088/1741-4326/acf560
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
As part the DTE2 campaign in the JET tokamak, we conducted a parameter scan in T and D-T complementing existing pulses in H and D. For the different main ion masses, type-I ELMy H-modes at fixed plasma current and magnetic field can have the pedestal pressure varying by a factor of 4 and the total pressure changing from beta(N) = 1.0 to 3.0. We investigated the pedestal and core isotope mass dependencies using this extensive data set. The pedestal shows a strong mass dependence on the density, which influences the core due to the strong coupling between both plasma regions. To better understand the causes for the observed isotope mass dependence in the pedestal, we analysed the interplay between heat and particle transport and the edge localised mode (ELM) stability. For this purpose, we developed a dynamic ELM cycle model with basic transport assumptions and a realistic neutral penetration. The temporal evolution and resulting ELM frequency introduce an additional experimental constraint that conventional quasi-stationary transport analysis cannot provide. Our model shows that a mass dependence in the ELM stability or in the transport alone cannot explain the observations. One requires a mass dependence in the ELM stability as well as one in the particle sources. The core confinement time increases with pedestal pressure for all isotope masses due to profile stiffness and electromagnetic turbulence stabilisation. Interestingly, T and D-T plasmas show an improved core confinement time compared to H and D plasmas even for matched pedestal pressures. For T, this improvement is largely due to the unique pedestal composition of higher densities and lower temperatures than H and D. With a reduced gyroBohm factor at lower temperatures, more turbulent drive in the form of steeper gradients is required to transport the same amount of heat. This picture is supported by quasilinear flux-driven modelling using TGLF-SAT2 within Astra. With the experimental boundary condition TGLF-SAT2 predicts the core profiles well for gyroBohm heat fluxes >15, however, overestimates the heat and particle transport closer to the turbulent threshold.
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收藏
页数:38
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