Since 18 of December 2019 conferences.iaea.org uses Nucleus credentials. Visit our help pages for information on how to Register and Sign-in using Nucleus.

17–22 Oct 2016
Kyoto International Conference Center
Japan timezone

Nonlocal Plasma Response to Edge Perturbation in Tokamak

19 Oct 2016, 08:30
4h
Kyoto International Conference Center

Kyoto International Conference Center

Takaragaike, Sakyo-ku, Kyoto 606-0001 Japan
Poster THC - Magnetic Confinement Theory and Modelling: Confinement Poster 3

Speaker

Dr Masatoshi Yagi (National Institutes for Quantum and Radiological Science and Technology, Rokkasho Fusion Institute)

Description

The transient transport events are observed in toroidally magnetic confinement devices. For example, the cold pulse experiment shows a rapid transient increase of electron temperature in the plasma core in response to an abrupt cooling at the edge. Understanding the nonlocal transport is important to control plasma core and/or fuel supply in ITER and DEMO. The nonlocal particle transport has been investigated based on 4-field reduced MHD model applying edge density source. It is shown that 0/0 and 1/0 modes play an important role for nonlocal transport. The edge cooling is also investigated based on 3-field gyro-fluid model, however, the nonlocal transport is found to be limited in the peripheral region [1]. To identify the effects of density source and temperature sink in the edge region, we have extended 4-field model[2] to 5-field model which consists of the vorticity equation, Ohm’s law, parallel ion momentum equation, electron density equation and electron temperature equation. Simulation study on nonlocal plasma response in tokamak is performed using global fluid code based on the 5-field model. A nonlocal plasma response to edge perturbation is found. The simulation result shows that (i) the mean central electron temperature increases according to the edge cooling (it is shown for the first time), (ii) the magnetic island located at q=2 rational surface plays an important role (acting as internal transport barrier) as well as non-resonant modes such as 0/0 and 1/0 (here m/n implies Fourier mode with poloidal mode number m and toroidal mode number n), (iii) re-distribution of electron temperature occurs after switching off source and sink where meso-scale mode plays a major role. Reference [1] N. Miyato, et al., IAEA FEC2014, TH/P2-12 (2014). [2] M. Yagi, et al., Nucl. Fusion 45 900 (2005).
Country or International Organization Japan
Paper Number TH/P3-21

Primary author

Dr Masatoshi Yagi (National Institutes for Quantum and Radiological Science and Technology, Rokkasho Fusion Institute)

Co-authors

Dr Akinobu Matsuyama (Japan Atomic Energy Agency) Dr Naoaki Miyato (Japan Atomic Energy Agency) Dr Tomonori Takizuka (Graduate School of Engineering, Osaka University)

Presentation materials