Confinement in Mixed Isotope Plasmas with Constant ELM Frequency in JET-ILW

ORAL

Abstract

Over recent years a series of dedicated experiments have been performed on JET to study the effect of plasma isotope on plasma parameters in an ITER-like wall. These experiments have included plasmas with a single main isotope of H, D or T and mixtures such as HD, HT and ultimately DT. The effective mass of the plasma can have several different effects on plasma parameters e.g., confinement, L-H transition power and ELM frequency.



Variations of isotope mixture from H to D were performed in type I ELMy H-mode plasmas of the same magnetic field, plasma current and divertor configuration. These variations were performed with and without the use of ELM-control via the perturbation of the vertical magnetic field. This was included as an attempt to separate the effects of fELM from the isotope effect on pedestal confinement.



A clear increase in plasma stored energy was observed with increasing effective mass, in cases with and without external control of ELMs. This increase was driven by an increase in plasma density driven by the pedestal density. For plasmas that used vertical kicks the plasma thermal stored energy (Wth) varied as ~Meff0.7. Results in a HT mixture matched the results in a HD mixture with the same Meff. Further results in pure tritium proved more difficult to include in the dataset due to changes in the access to H-mode, impurity behaviour and density peaking. This scaling analysis, variation of Ti/Te, tritium behaviour and the results at constant bN will be presented.

*This work has been carried out within the framework of the EUROfusion Consortium, funded by the European Union via the Euratom Research and Training Programme (Grant Agreement No 101052200 — EUROfusion). Views and opinions expressed are however those of the author(s) only and do not necessarily reflect those of the European Union or the European Commission. Neither the European Union nor the European Commission can be held responsible for them.

Publication: Planned paper on special edition of JET DT results

Presenters

  • Damian B King

    • UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK
    • UKAEA, Culham Science Centre, Abingdon, OX143DB, United Kingdom
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom

Authors

  • Damian B King

    • UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK
    • UKAEA, Culham Science Centre, Abingdon, OX143DB, United Kingdom
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom
  • Eleonora Viezzer

    • University of Seville,Spain
    • Department of Atomic, Molecular and Nuclear Physics, University of Seville, Seville, Spain
  • Matteo Baruzzo

    • ENEA C. R. Frascati, via E. Fermi 45, 00044 Frascati (Roma), Italy
    • Consorzio RFX, Padova, Italy
  • Elena De La Luna

    • Laboratorio Nacional de Fusión, CIEMAT, Madrid, Spain
    • Laboratorio Nacional de Fusión, CIEMAT, Madrid, Spain,
    • Laboratorio Nacional de Fusion, CIEMAT, Madrid, Spain
    • Laboratorio Nacional de Fusión, CIEMAT, 28040 Madrid, Spain
    • Laboratorio Nacional de Fusión, CIEMAT
  • Jeronimo Garcia

    • CEA
    • CEA, IRFM, F-13108 Saint Paul Lez Durance, France
    • CEA, IRFM, Saint-Paul-lez-Durance, France
    • CEA, IRFM, F-13108 Saint-Paul-lez-Durance, France
    • CEA, Cadarache, France
    • CEA, IRFM, F-13108 Saint-Paul-lex-Durance, France
    • CEA, IRFM, Saint-Paul-Lez-Durance, France
    • CEA, IRFM, F-13108 St-Paul-Lez-Durance, France
  • Ephrem Delabie

    • Oak Ridge National Laboratory
  • Wojech Gromelski

    • Institute of Plasma Physics and Laser Microfusion, Warsaw, Poland
  • rafael henriques

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
  • Jon C Hillesheim

    • Culham Science Centre
  • Laszlo Horvath

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
    • UKAEA, CCFE, Culham Science Centre, Abingdon, UK; York Plasma Institute, Department of Physics, University of York, York, UK of Great Britain and Northern Ireland
  • Krassimir Kirov

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
    • UKAEA, Culham Science Centre, Abingdon, OX143DB, United Kingdom
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom
  • Morten Lennholm

    • UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
    • UKAEA
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom
  • Costanza F Maggi

    • Culham Centre for Fusion Energy (CCFE), Culham Science Centre, Abingdon, UK
    • UKAEA/CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
    • UKAEA, Culham Science Centre, Abingdon, OX143DB, United Kingdom
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom
  • Mikhail Maslov

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
    • UKAEA, Culham Science Centre, Abingdon, OX143DB, United Kingdom
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom
  • Ash Patel

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
  • Philip A Schneider

    • Max-Planck-Institut für Plasmaphysik, Garching b. München, Germany
  • Ridhima Sharma

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK
    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,
  • Tom Wilson

    • United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, UK,