Non-axisymmetric Radiation Modeling of JET SPI Discharges Using Emis3D

ORAL

Abstract

Precise radiated power values in tokamak disruptions are required to ensure stored energy in net energy tokamaks like ITER and SPARC is well mitigated. In mitigated disruptions, 3D MHD modes and localized impurity sources break toroidal symmetry. To incorporate asymmetric radiation structures, the Emis3D code adopts a physics motivated guess-and-check approach. Virtual radiation structures are observed with the Cherab modeling framework [M. Carr EPS 2017] and a best fit chosen using a reduced χ2 statistic. 2D axisymmetric inversions, helical structures, and 3D MHD simulated distributions from JOREK [Huysmans NF 2007] are tested. Two JET discharges terminated by shattered neon pellets are analyzed. 2D inversions are the best fit to the current quench, but helical structures are within uncertainty. Helicals fit the pre-thermal quench (pre-TQ) best and exhibit a parallel flow towards the high-field side. JOREK agreement to experiment in the pre-TQ is improved by increasing fidelity of the impurity source. Radiated fractions of 0.95 +0.05/-0.31 and 0.98 +0.02/-0.26 are found, suggesting that the stored energy may have been fully mitigated.

*US DOE DE-SC0014264, DE-FC02-04ER54698, DE-AC05-00OR22725, DE-FG02-07ER54917, DEAC52-07NA27344, IO TA C18TD38FU, and Euratom grant 633053

Presenters

  • Benjamin Stein-Lubrano

    • MIT PSFC

Authors

  • Benjamin Stein-Lubrano

    • MIT PSFC
  • Ryan M Sweeney

    • MIT PSFC
    • Massachusetts Institute of Technology
    • MIT Plasma Science and Fusion Center
  • Daniele Bonfiglio

    • Consorzio RFX
  • Pedro Carvalho

    • Culham Centre for Fusion Energy (CCFE), Culham Science Centre, Abingdon, UK
  • Jack Lovell

    • Oak Ridge National Laboratory
  • Larry R BAYLOR

    • ORNL
    • Oak Ridge National Laboratory
  • Robert S Granetz

    • Massachusetts Institute of Technology (MIT)
    • Massachusetts Institute of Technology MI
    • Massachusetts Institute of Technology
    • MIT Plasma Science and Fusion Center
    • MIT
  • Stefan Jachmich

    • ITER Organization, Route de Vinon sur Verdon, 13115 St Paul Lez Durance, France
    • ITER Organization
  • Emmanuel Joffrin

    • CEA, IRFM, F-13108 Saint-Paul-lez-Durance, France
  • Michael LEHNEN

    • ITER Organization, Route de Vinon sur Verdon, 13115 St Paul Lez Durance, France
    • ITER Organization
    • ITER Organization, France
  • 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
  • Earl S Marmar

    • Massachusetts Institute of Technology MIT
  • Eric Nardon

    • CEA, IRFM, F-13108 Saint-Paul-lez-Durance, France
  • Umar A Sheikh

    • École Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC), Lausanne CH-1015, Switzerland
    • Ecole Polytechnique Federal de Lausanne
  • Daisuke Shiraki

    • Oak Ridge National Lab
    • Oak Ridge National Laboratory
  • Scott Silburn

    • Culham Centre for Fusion Energy (CCFE), Culham Science Centre, Abingdon, UK
    • UKAEA, CCFE, Culham Science Centre, Abingdon, United Kingdom