The dependence of confinement on the isotope mass in the core and the edge of AUG and JET-ILW H-mode plasmas

被引:13
|
作者
Schneider, P. A. [1 ]
Angioni, C. [1 ]
Frassinetti, L. [2 ]
Horvath, L. [3 ]
Maslov, M. [3 ]
Auriemma, F. [4 ,5 ]
Cavedon, M. [1 ,6 ]
Challis, C. D. [3 ]
Delabie, E. [7 ]
Dunne, M. G. [1 ]
Climent, J. M. Fontdecaba [3 ]
Hobirk, J. [1 ]
Kappatou, A. [1 ]
Keeling, D. L. [3 ]
Kurzan, B. [1 ]
Lennholm, M. [3 ]
Lomanowski, B. [7 ]
Maggi, C. F. [3 ]
McDermott, R. M. [1 ]
Puetterich, T. [1 ]
Thorman, A. [3 ]
Willensdorfer, M. [1 ]
机构
[1] Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany
[2] KTH Royal Inst Technol, Tekn Ringen 31, Stockholm, Sweden
[3] United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England
[4] Univ Padua, Consorzio RFX CNR, Acciaierie Veneto SpA, Ist Nazl Fis Nucl,ENENA, Padua, Italy
[5] CNR, ISTP, Corso Stati Uniti 4, I-35127 Padua, Italy
[6] Univ Milano Bicocca, Dipartimento Fisica G Occhialini, Milan, Italy
[7] Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA
基金
英国工程与自然科学研究理事会;
关键词
tokamak; heat transport; isotope effect; pedestal stability; quasilinear modelling; INSTABILITIES; TRANSPORT;
D O I
10.1088/1741-4326/ac3e82
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
Experiments in ASDEX Upgrade (AUG) and JET with the ITER-like wall (JET-ILW) are performed to separate the pedestal and core contributions to confinement in H-modes with different main ion masses. A strong isotope mass dependence in the pedestal is found which is enhanced at high gas puffing. This is because the ELM type changes when going from D to H for matched engineering parameters, which is likely due to differences in the inter ELM transport with isotope mass. The pedestal can be matched in H and D plasmas by varying only the triangularity and keeping the engineering parameters relevant for core transport the same. With matched pedestals Astra/TGLF (Sat1geo) core transport simulations predict the experimental profiles equally well for H and D. These core transport simulations show a negligible mass dependence and no gyro-Bohm scaling is observed. However, to match the experimental observations at medium beta it is required to take the fast-ion dilution and rotation into account. This is not enough for high beta plasmas where for the first time a profile match between H and D plasmas was achieved experimentally. Under these conditions quasilinear modelling with TGLF over predicts the transport in the core of H and D plasmas alike.
引用
收藏
页数:11
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