Abstract

The full dynamics of a multi-edge-localized-mode (ELM) cycle is modeled for the first time in realistic tokamak X-point geometry with the nonlinear reduced MHD code jorek. The diamagnetic rotation is found to be instrumental to stabilize the plasma after an ELM crash and to model the cyclic reconstruction and collapse of the plasma pressure profile. ELM relaxations are cyclically initiated each time the pedestal gradient crosses a triggering threshold. Diamagnetic drifts are also found to yield a near-symmetric ELM power deposition on the inner and outer divertor target plates, consistent with experimental measurements.

Highlights

  • HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not

  • The full dynamics of a multi-edge-localized-mode (ELM) cycle is modeled for the first time in realistic tokamak X-point geometry with the nonlinear reduced MHD code JOREK

  • The diamagnetic rotation is found to be instrumental to stabilize the plasma after an ELM crash and to model the cyclic reconstruction and collapse of the plasma pressure profile

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Summary

Introduction

HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. An example is given for a single n 1⁄4 8 ELM (only the n 1⁄4 0 and n 1⁄4 8 modes are included in the simulation) modeled without taking into account the diamagnetic effects (Fig. 1): during the ELM crash, characterized by a large peak of kinetic and magnetic energy of the n 1⁄4 8 mode (Fig. 1), the plasma edge is stochastized in a large extent: the region for normalized flux ψnorm > 0.85 is fully reconnected [Figs.

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