Thermal energy mitigation and toroidal peaking effects in JET disruptions

Thermal energy mitigation is critical to prevent damage to the tokamak in plasma disruptions. Previous investigations on JET suggest thermal stored energy (W_th) is poorly mitigated by either Massive Gas Injection (MGI) or Shattered Pellet Injection (SPI) Disruption Mitigation Systems (DMS). A contrasting investigation on ASDEX-Upgrade found that W_th is well mitigated with MGI. We investigate whether the apparent poor thermal mitigation on JET is explained by radiation peaking near the injected impurity plume, combined with the limited toroidal resolution of bolometry. High toroidal peaking in the pre-thermal quench (pre-TQ) is found in Ar/D2 MGI on JET, with >3x higher radiation near the plume than elsewhere throughout the pre-TQ. A previously unexplained toroidal peaking measurement in neon SPI is also successfully reproduced with similar peaking. These observations agree with literature from Alcator C-Mod, ASDEX-Upgrade, and KSTAR. This peaking is not captured in previous JET studies that found poor thermal mitigation. A set of 10% Ar, 90% D2 mix MGIs is analyzed using the Emis3D radiation modeling code. With injector peaking, almost two thirds of W_th is radiated, where estimates that do not account for injector peaking would indicate less than half. The toroidal spread of the injector peaking feature is poorly constrained, and up to 85% of W_th may be radiated using the largest possible spread. Similar radiated fractions are seen in a second set of MGI discharges and in a set of neon SPI discharges. The improved W_th mitigation suggests a reduced divertor melt risk in mitigated disruptions on ITER and SPARC. Higher peaking near DMS injectors could increase flash melting risk on nearby plasma facing components. Only single-injector cases are studied; simultaneous injection is not addressed.