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Dynamics of edge limit cycle oscillation in the JFT-2M Tokamak

T. Kobayashi, K. Itoh, T. Ido, K. Kamiya, S.-I. Itoh, Y. Miura, Y. Nagashima, A. Fujisawa, S. Inagaki, K. Ida2014年被引用 30Nuclear FusionIF 3出版社

In the JFT-2M tokamak (JFT standing for JAERI Fusion Torus), the limit cycle oscillation (LCO), together with several variables, i.e., the electrostatic potential, radial electric field, electron density, turbulence intensity, and Dα emission from the divertor region, is observed before the L-to-H transition. The spatiotemporal dynamics of the LCO is analysed in detail. Zonal flows are not seen, while modulation is observed in the edge-localized poloidal flow and density gradient. Modulation is also seen in the Reynolds stress, caused by that in the turbulence intensity and turbulence wavenumber. However, flow acceleration cannot be explained by the modulation in the Reynolds stress. Rapid inward propagation is also observed for the density gradient and turbulence packet. The characteristics of the propagation are verified by means of turbulence spreading theory and diffusion theory.

日本語訳

JFT-2Mトカマク(JFTはJAERI Fusion Torusの略)において、極限周期振動(LCO)が、いくつかの変数、すなわち静電ポテンシャル、径方向電場、電子密度、乱流、およびダイバータ領域からのDα発光とともに、L-H遷移の前に観測された。LCOの時空間ダイナミクスが詳細に解析された。帯状流は観測されない一方で、エッジ局在ポロイダル流と密度勾配における変調が観測された。レイノルズ応力における変調も観測され、これは乱流強度と乱流波数における変調によって引き起こされた。しかしながら、流れの加速はレイノルズ応力の変調によって説明することはできなかった。密度勾配と乱流パケットについても急速な内向き伝播が観測された。この伝播の特性は、乱流拡散理論と拡散理論を用いて検証された。

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