The dependence of confinement on the isotope mass in the core and the edge of AUG and JET-ILW H-mode plasmasUnited Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Univ Padua, Consorzio RFX CNR, Acciaierie Veneto SpA, Ist Nazl Fis Nucl,ENENA, Padua, Italy.;CNR, ISTP, Corso Stati Uniti 4, I-35127 Padua, Italy..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany.;Univ Milano Bicocca, Dipartimento Fisica G Occhialini, Milan, Italy..
United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Oak Ridge Natl Lab, Oak Ridge, TN 37831 USA..
United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
United Kingdom Atom Energy Author, Culham Ctr Fus Energy, Culham Sci Ctr, Abingdon OX14 3DB, Oxon, England..
Max Planck Inst Plasma Phys, Boltzmannstr 2, D-85748 Garching, Germany..
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2022 (English)In: Nuclear Fusion, ISSN 0029-5515, E-ISSN 1741-4326, Vol. 62, no 2, article id 026014Article in journal (Refereed) Published
Abstract [en]
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.
Place, publisher, year, edition, pages
IOP Publishing , 2022. Vol. 62, no 2, article id 026014
Keywords [en]
tokamak, heat transport, isotope effect, pedestal stability, quasilinear modelling
National Category
Fusion, Plasma and Space Physics
Identifiers
URN: urn:nbn:se:kth:diva-306847DOI: 10.1088/1741-4326/ac3e82ISI: 000732436800001Scopus ID: 2-s2.0-85122621650OAI: oai:DiVA.org:kth-306847DiVA, id: diva2:1625823
Note
QC 20220110
2022-01-102022-01-102022-06-25Bibliographically approved