Two-stage Crash Process in Resistive Drift Ballooning Mode Driven ELM Crash
Haruki Seto, Xueqiao Xu, Benjamin D. Dudson, Masatoshi Yagi

TL;DR
This study numerically simulates a two-stage crash process in edge localized modes driven by resistive drift-ballooning modes, revealing complex nonlinear interactions and their impact on ELM trigger dynamics in tokamak plasmas.
Contribution
It demonstrates the two-stage crash process driven by RDBMs in a full torus domain, highlighting the role of nonlinear couplings and turbulence in ELM dynamics.
Findings
First crash triggered by linearly unstable RDBMs and magnetic island excitation.
Middle-n turbulence develops and localizes around X-points, causing small energy loss.
Second crash occurs when turbulence covers the entire poloidal region.
Abstract
We report a two-stage crash process in edge localized mode (ELM) driven by resistive drift-ballooning modes (RDBMs) numerically simulated in a full annular torus domain. In the early nonlinear phase, the first crash is triggered by linearly unstable RDBMs and m/n = 2/1 magnetic islands are nonlinearly excited via nonlinear couplings of RDBMs. Simultaneously, middle-n RDBM turbulence develops but is poloidally localized around X-points of the magnetic islands, leading to the small energy loss. Here m is the poloidal mode number, n is the toroidal mode number, the q = 2 rational surface exists at the pressure gradient peak, and q is the safety factor, respectively. The second crash occurs in the late nonlinear phase. Low-n magnetic islands are also excited around the q = 2 surface via nonlinear couplings among the middle-n turbulence. Since the turbulence develops from the X-points of…
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Taxonomy
TopicsMagnetic confinement fusion research · Physics of Superconductivity and Magnetism · Ionosphere and magnetosphere dynamics
