A non-linear MHD code, named JOREK, is under development with the aim of studying the non-linear evolution of the MHD instabilities thought to be responsible for edge localized modes (ELMs): external kink (peeling) and medium-n ballooning modes. The full toroidal X-point geometry is taken into account including the separatrix, open and closed field lines. Analysis of the influence of the separatrix shows a strong stabilization of the ideal and resistive MHD external kink/peeling modes. One instability remains unstable in the presence of the X-point, characterized by a combination of a tearing and a peeling mode. The so-called peeling-tearing mode shows a much weaker dependence on the edge q. Non-linearly the n = 1 peeling-tearing mode satur...
The full dynamics of a multi-edge-localized-mode (ELM) cycle is modeled for the first time in realis...
Nonlinear simulations with the 3D electromagnetic two-fluid BOUT code are employed to study the dyna...
A triggering mechanism responsible for the explosive onset of edge localised modes (ELMs) in fusion ...
International audienceNon-linear MHD simulations of edge localized modes (ELMs) show features in qua...
In non-linear MHD simulations of ELMs [1], a radially localised, toroidally symmetric, poloidal flow...
Abstract. The non-linear characteristics and consequences of ideal magnetohydrodynamic (MHD) instabi...
Using the nonlinear 3D MHD code JOREK with reduced MHD equations (visco-resistive MHD), we have succ...
Understanding the physics of the H-Mode pedestal and edge localized modes (ELMs) is very important t...
Abstract. In non-linear MHD simulations of ELMs [1], a radially localised, toroidally symmetric, pol...
The impact of n=2 resonant magnetic perturbation (RMP) on the pedestal and peeling-ballooning mode (...
The aim of nuclear fusion energy research is to demonstrate the feasibility of nuclear fusion reacto...
Using the nonlinear 3D MHD code JOREK with reduced MHD equations (visco-resistive MHD), we have succ...
Edge localized modes (ELMs) are repetitive instabilities driven by the large pressure gradients and ...
Macroscopic instabilities and their unfavourable effects on plasma confinement pose a central challe...
The full dynamics of a multi-edge-localized-mode (ELM) cycle is modeled for the first time in realis...
Nonlinear simulations with the 3D electromagnetic two-fluid BOUT code are employed to study the dyna...
A triggering mechanism responsible for the explosive onset of edge localised modes (ELMs) in fusion ...
International audienceNon-linear MHD simulations of edge localized modes (ELMs) show features in qua...
In non-linear MHD simulations of ELMs [1], a radially localised, toroidally symmetric, poloidal flow...
Abstract. The non-linear characteristics and consequences of ideal magnetohydrodynamic (MHD) instabi...
Using the nonlinear 3D MHD code JOREK with reduced MHD equations (visco-resistive MHD), we have succ...
Understanding the physics of the H-Mode pedestal and edge localized modes (ELMs) is very important t...
Abstract. In non-linear MHD simulations of ELMs [1], a radially localised, toroidally symmetric, pol...
The impact of n=2 resonant magnetic perturbation (RMP) on the pedestal and peeling-ballooning mode (...
The aim of nuclear fusion energy research is to demonstrate the feasibility of nuclear fusion reacto...
Using the nonlinear 3D MHD code JOREK with reduced MHD equations (visco-resistive MHD), we have succ...
Edge localized modes (ELMs) are repetitive instabilities driven by the large pressure gradients and ...
Macroscopic instabilities and their unfavourable effects on plasma confinement pose a central challe...
The full dynamics of a multi-edge-localized-mode (ELM) cycle is modeled for the first time in realis...
Nonlinear simulations with the 3D electromagnetic two-fluid BOUT code are employed to study the dyna...
A triggering mechanism responsible for the explosive onset of edge localised modes (ELMs) in fusion ...