The modeling of the Edge-localized-mode (ELM) should be rigorously pursued for reliable and robust ELM control for steady-state long-pulse H-mode operation in ITER as well as DEMO. In the KSTAR discharge {\#}7328, a linear stability of the ELMs is investigated using M3D-C1 and BOUT++ codes. This is achieved by linear simulation for the n= 8 mode structure of the ELM observed by the KSTAR electron cyclotron emission imaging (ECEI) systems. In the process of analysis, variations due to the plasma equilibrium profiles and transport coefficients on the ELM growth rate are investigated and simulation results with the two codes are compared. The numerical simulations are extended to nonlinear phase of the ELM dynamics, which includes saturation a...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
A control of the ELM-crash is required for a stable plasma operation in a fusion reactor if the H-mo...
Full understanding of ELM physics is one of the most important issues to achieve stable plasma opera...
Time-dependent nonlinear simulation using the BOUT++ 3-field model is performed for a study of edge ...
KSTAR electron cyclotron emission imaging (ECEI) systems have contributed to understanding the funda...
Time-dependent nonlinear simulation using the BOUT++ 3-field model is performed for a study of edge ...
The verification between the three different MHD simulation codes is an important process to cross-c...
Following the first operation of H-mode in KSTAR in 2009, study of the edge localized modes (ELM) ha...
A detailed study of edge-localized mode (ELM) dynamics in the KSTAR tokamak is performed using a two...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
A control of the ELM-crash is required for a stable plasma operation in a fusion reactor if the H-mo...
Full understanding of ELM physics is one of the most important issues to achieve stable plasma opera...
Time-dependent nonlinear simulation using the BOUT++ 3-field model is performed for a study of edge ...
KSTAR electron cyclotron emission imaging (ECEI) systems have contributed to understanding the funda...
Time-dependent nonlinear simulation using the BOUT++ 3-field model is performed for a study of edge ...
The verification between the three different MHD simulation codes is an important process to cross-c...
Following the first operation of H-mode in KSTAR in 2009, study of the edge localized modes (ELM) ha...
A detailed study of edge-localized mode (ELM) dynamics in the KSTAR tokamak is performed using a two...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...
The explanation of the existence of the rotating MHD modes in the pedestal region before Type I edge...