TY - JOUR
T1 - Simulation of co-existence of ballooning and kink instabilities in PLATO tokamak plasma
AU - Tomimatsu, Shuhei
AU - Kasuya, Naohiro
AU - Sato, Masahiko
AU - Fukuyama, Atsushi
AU - Yagi, Masatoshi
AU - Nagashima, Yoshihiko
AU - Fujisawa, Akihide
N1 - Funding Information:
This study is partially supported by the Grant-in-Aid for Scientific Research (JP16K06938, JP17H06089, JP20K03905) of JSPS, the collaboration program of NIFS (NIFS19KNST144, NIFS18KNXN373) and of RIAM of Kyushu University. JFRS-1 supercomputer in IFERC-CSC is used for the nonlinear calculations.
Publisher Copyright:
© 2020 The Japan Society of Plasma Science and Nuclear Fusion Research.
PY - 2020
Y1 - 2020
N2 - Magneto-hydro-dynamics (MHD) simulations are carried out for the first time with PLATO tokamak parameters to represent competition of plasma instabilities. The plasma equilibrium is evaluated with the vertical coil configuration in PLATO by using free boundary equilibrium code. The equilibrium is introduced from TASK/EQ to MHD simulations by MIPS code to calculate nonlinear saturation dynamics. In the simulation, a ballooning mode and kink mode both become unstable. We present the dependencies on plasma parameters to identify the instabilities. The ballooning and kink modes become unstable in the steep gradient region and at the safety factor q = 1 surface near the center of the plasma, respectively, so the nonlinear flattening of the pressure profile near the center is stronger in the kink case. The interaction between the modes affects the evolution of instabilities.
AB - Magneto-hydro-dynamics (MHD) simulations are carried out for the first time with PLATO tokamak parameters to represent competition of plasma instabilities. The plasma equilibrium is evaluated with the vertical coil configuration in PLATO by using free boundary equilibrium code. The equilibrium is introduced from TASK/EQ to MHD simulations by MIPS code to calculate nonlinear saturation dynamics. In the simulation, a ballooning mode and kink mode both become unstable. We present the dependencies on plasma parameters to identify the instabilities. The ballooning and kink modes become unstable in the steep gradient region and at the safety factor q = 1 surface near the center of the plasma, respectively, so the nonlinear flattening of the pressure profile near the center is stronger in the kink case. The interaction between the modes affects the evolution of instabilities.
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U2 - 10.1585/PFR.15.1403052
DO - 10.1585/PFR.15.1403052
M3 - Article
AN - SCOPUS:85089504594
SN - 1880-6821
VL - 15
JO - Plasma and Fusion Research
JF - Plasma and Fusion Research
M1 - 1403052
ER -