It has been thought that asymmetric vertical displacement event (AVDE) disruptions in ITER might produce large electro-mechanical forces on the walls and other conducting structures surrounding the plasma. It is shown that ITER AVDE disruptions should produce a small asymmetric wall force, comparable to JET. This is demonstrated in simulations r1, 2s with the M3D 3D MHD code r3s and confirmed in JET experiments r4s in which the current was quenched with massive gas injection (MGI). In ITER the current quench (CQ) time, ?CQ, is less than or equal to the resistive wall penetration time, ?wall. JET is in a different parameter regime, with ?CQ ? ?wall. JET simulations were validated by comparison r1s to JET shot 71985 data and were in good agreement. The wall time was then artificially increased, keeping ?CQ fixed, and it was found that the wall force decreased. The reduction of the asymmetric wall force was also found in experimental data r4s of JET MGI mitigated disruption shots. Further simulations r2s were carried out of ITER AVDEs. The asymmetric wall force was calculated for a wide range of CQ times. For ?CQ ? ?wall, the force was not much larger than in JET. A fast CQ may cause production of runaway electrons (REs). The effect of replacing part of of the current with REs on MHD behaviour will be discussed. Simulations using a modified version of M3D with a fluid RE model r5s will be presented.

Asymmetric Wall Force Reduction in ITER and JET Disruptions

Paccagnella R;
2018

Abstract

It has been thought that asymmetric vertical displacement event (AVDE) disruptions in ITER might produce large electro-mechanical forces on the walls and other conducting structures surrounding the plasma. It is shown that ITER AVDE disruptions should produce a small asymmetric wall force, comparable to JET. This is demonstrated in simulations r1, 2s with the M3D 3D MHD code r3s and confirmed in JET experiments r4s in which the current was quenched with massive gas injection (MGI). In ITER the current quench (CQ) time, ?CQ, is less than or equal to the resistive wall penetration time, ?wall. JET is in a different parameter regime, with ?CQ ? ?wall. JET simulations were validated by comparison r1s to JET shot 71985 data and were in good agreement. The wall time was then artificially increased, keeping ?CQ fixed, and it was found that the wall force decreased. The reduction of the asymmetric wall force was also found in experimental data r4s of JET MGI mitigated disruption shots. Further simulations r2s were carried out of ITER AVDEs. The asymmetric wall force was calculated for a wide range of CQ times. For ?CQ ? ?wall, the force was not much larger than in JET. A fast CQ may cause production of runaway electrons (REs). The effect of replacing part of of the current with REs on MHD behaviour will be discussed. Simulations using a modified version of M3D with a fluid RE model r5s will be presented.
2018
Istituto gas ionizzati - IGI - Sede Padova
ITER
Asymmetric Wall Force Reduction
JET Disruptions
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/351788
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