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Oral presentation

Oral presentation

Simulations of toroidal rotation due to the neoclassical toroidal viscosity in tokamaks

Honda, Mitsuru; Satake, Shinsuke*; Suzuki, Yasuhiro*; Matsunaga, Go; Ide, Shunsuke; Yoshida, Maiko; Hayashi, Nobuhiko

no journal, , 

Oral presentation

Simulation of runaway electron confinement in presence of macroscopic MHD modes

Yagi, Masatoshi; Matsuyama, Akinobu; Wakasa, Arimitsu*; Nuga, Hideo

no journal, , 

Oral presentation

ITER remote experiments and simulations

Ozeki, Takahisa; Clement, L. S.*; Nakajima, Noriyoshi*

no journal, , 

Oral presentation

Oral presentation

Gyrokinetic Vlasov simulations of ITG-TEM driven turbulent transport on realistic tokamak equilibrium

Nakata, Motoki; Honda, Mitsuru; Yoshida, Maiko; Urano, Hajime; Maeyama, Shinya; Nunami, Masanori*; Watanabe, Tomohiko*

no journal, , 

First-principle based gyrokinetic simulation is a promising approach for investigating turbulent transport in future burning plasmas such as ITER an DEMO. In this study, ITG-TEM driven turbulent transport simulations on the realistic JT-60U tokamak equilibrium are realized by using a local gyrokinetic turbulence code GKV-J. Linear micro-stability analyses on several radial locations revealed that ITG, ITG-TEM, and TEM modes are dominant for inner, middle, and outer core regions, respectively. The nonlinear turbulence simulation results successfully reproduce the experimental results on ion and electron heat diffusivity in the core region, where the conventional fluid-type reduced transport model shows some deviations. Also, different nonlinear dependences of the turbulence/zonal-flow energy on the ion/electron heat and particle transport levels are newly identified, i.e., weaker impact on the electron heat and particle transport compared to the ion heat one.

Oral presentation

Excitation of flow-stabilized resistive wall mode in rotating tokamak plasmas

Aiba, Nobuyuki; Hirota, Makoto*; Shiraishi, Junya

no journal, , 

A mechanism exciting magnetohydrodynamic (MHD) instabilities in rotating tokamak plasmas is found numerically for the first time. This mechanism is the interplay between a resistive wall mode (RWM) and a stable MHD mode. When the plasma has a stable discrete eigenmode, a reversed shear Alfv$'e$n eigenmode (RSAE) for example, a MHD mode is destabilized when plasma equilibrium rotation frequency is similar to the frequency of this stable eigenmode in a static equilibrium. This destabilization is also observed even when the eigenmode couples with Alfv$'e$n continua. This result suggests that for steady state high beta tokamaks, like DEMO, it is necessary to shape the safety factor profile in such a way that no stable eigenmode exists in the band of rotation frequency.

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