Abstract
In the ASDEX Upgrade tokamak, the growth of non-axisymmetric magnetic perturbation (NAMP) associated with the ELM crash events has been observed, and both the poloidal and toroidal phases of NAMPs, measured by a set of Mirnov coils, were highly random. By applying an n = 1 magnetic perturbation (MP) field, the phases of NAMPs were locked to the phase of the total n = 1 resonant MP (RMP) field, which takes the plasma response to the MP field into account. This observation can be explained by the resonant electromagnetic J × B torque applied by the RMP field on a magnetic island formed due to the magnetic reconnection, which is predicted to occur during the ELM crashes by several numerical modelling results.
Highlights
Magnetic reconnection [8], which is followed by the formation of magnetic islands at the rational flux surfaces, plays a vital role for understanding the collapse events in magnetized plasmas, such as sawtooth crashes [9], minor disruptions [10] in tokamaks and solar flares [11] in the solar atmosphere
Plasmas, the magnetic island structure was directly described by the radial distribution of the nonaxisymmetric magnetic perturbations (NAMPs) [ 17 ] measured by magnetic probes around the rational surface
We report the observations from the ASDEX Upgrade tokamak experiments on the NAMPs with low toroidal mode number growing associated with the edge-localized mode (ELM) crash events, which are similar to those observed in TCV [28]
Summary
Magnetic reconnection [8], which is followed by the formation of magnetic islands at the rational flux surfaces, plays a vital role for understanding the collapse events in magnetized plasmas, such as sawtooth crashes [9], minor disruptions [10] in tokamaks and solar flares [11] in the solar atmosphere. This observation can be explained by the resonant electromagnetic J×B torque, applied by the RMP field on a magnetic island due to the magnetic reconnection, which is predicted to occur during the ELM crashes by several numerical modelling results.
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