11–15 Oct 2021
Virtual in Consorzio RFX
Europe/Rome timezone

3D non-linear MHD simulations of deuterium shattered pellet injection into H-mode JET plasma

13 Oct 2021, 12:10
20m
Virtual in Consorzio RFX

Virtual in Consorzio RFX

Oral 2. Macro-instabilities, operational limits and disruptions ORAL SESSION

Speaker

Mengdi Kong (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK)

Description

Shattered pellet injection (SPI) is the current concept for the ITER disruption mitigation system (DMS) to prevent disruption-related damage from thermal loads, electromagnetic forces or runaway electron (RE) beams. Compared with impurity or mixed deuterium-impurity pellets that contain large quantity of impurities like neon, pure deuterium (D2) SPI is expected to strongly dilute the plasma without immediately triggering a thermal quench and could be instrumental for RE avoidance in ITER. Detailed simulations of D2-SPI-induced disruptions, especially the (pre-)thermal quench phase in a JET discharge (#96874) with the JOREK code will be presented. In this discharge, a pure D2 pellet with a diameter of 12.5mm (barrel A) was shattered before entering the 3MA/2.9T H-mode plasma, exhibiting a much longer cooling time (~9ms between the arrival of the first shards at the plasma edge and the onset of thermal quench) than that with impurity pellets (typically 1~2ms). 3D non-linear MHD simulations show that the plasma is not fully cooled during the penetration and ablation of the D2 shards, allowing the current density (j) to evolve on a much slower time scale than the penetration of the shards and no evident global contraction of j has been observed. Detailed comparison between simulations and experimental measurements will be presented to validate the model as well as clarify the underlying physics. In particular, the role of background impurities, pointed out as a concern in the predictions for ITER, will be examined in detail. Possible effects of plasma rotation on (pre-)thermal quench dynamics will also be discussed.

Primary author

Mengdi Kong (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK)

Co-authors

Eric Nardon (CEA, IRFM, F-13108 Saint-Paul-lez-Durance, France) Matthias Hoelzl (Max Planck Institute for Plasma Physics, Boltzmannstr. 2, 85748 Garching b. M., Germany) Daniele Bonfiglio (Consorzio RFX, Corso Stati Uniti 4, 35127 Padova, Italy) Di Hu (School of Physics, Beihang University, Beijing, 100191, China) Alexandru Boboc (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK) Pedro Carvalho (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK) Tim Hender (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK) Stefan Jachmich (ITER Organization, Route de Vinon sur Verdon, CS 90 046, 13067 Saint Paul-lez-Durance, Cedex, France) Kerry Lawson (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK) Umar Sheikh (École Polytechnique Fédérale de Lausanne (EPFL), Swiss Plasma Center (SPC), CH-1015 Lausanne, Switzerland) Scott Silburn (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK) Ryan Sweeney (Massachusetts Institute of Technology, Cambridge, MA 02139, USA) Gabor Szepesi (UKAEA-CCFE, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK)

Presentation materials