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Avoidance of disruptions at high /3n in ASDEX Upgrade with off-axis ECRH

机译:避免使用离轴ECRH的ASDEX升级中高/ 3n的中断

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摘要

Experiments on disruption avoidance have been carried out in H-mode ASDEX Upgrade plasmas: the localized perpendicular injection of ECRH (1.5 MW ~ 0.2P_(tot)) onto the q =2 resonant surface has led to the delay and/or complete avoidance of disruptions in a high β_N scenario (I_p =1 MA, B_t =2.1 T, q_(95) ~ 3.6, with NBI ~7.5 MW). In these discharges (at low q_(95) and low density) neoclassical tearing modes (NTMs) are excited: the growth and locking of the m =2/1 mode leads to the disruption. The scheme of the experiment is successfully applied in the same way as in previous disruption avoidance experiments in FTU and ASDEX Upgrade. As soon as the disruption precursor signal (the locked mode detector and/or the loop voltage) reaches the preset threshold, the ECRH power is triggered by real-time control. A poloidal scan in deposition location (P_(dep)) has been carried out by setting the poloidal launching mirrors at different angles in each discharge. The results depend on p_(dep): complete disruption avoidance can be achieved when the power is injected close to or onto the 2/1 island. When ECRH is injected outside the island (either at radii inside or outside the q — 2 surface), the discharge is disrupted as in the reference case.
机译:在H型ASDEX升级等离子体中进行了避免干扰的实验:将ECRH(1.5 MW〜0.2P_(tot))局部垂直注入q = 2共振表面导致了延迟和/或完全避免了干扰。在高β_N情景中发生的破坏(I_p = 1 MA,B_t = 2.1 T,q_(95)〜3.6,NBI〜7.5 MW)。在这些放电中(在低q_(95)和低密度下),新古典撕裂模式(NTM)被激发:m / n = 2/1模式的增长和锁定导致破坏。该实验方案已成功应用于FTU和ASDEX升级中先前避免干扰的实验中。一旦破坏前兆信号(锁定模式检测器和/或环路电压)达到预设阈值,ECRH功率就会由实时控制触发。通过在每次放电中将倍体发射镜设置在不同的角度,可以进行沉积位置的倍体扫描(P_(dep))。结果取决于p_(dep):当在2/1岛附近或上面注入电源时,可以完全避免干扰。当ECRH注入岛外(在q-2表面的内部或外部的半径处)时,放电会像参考例中那样受到干扰。

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  • 来源
    《Nuclear fusion》 |2011年第8期|p.504-512|共9页
  • 作者单位

    Associazione EURATOM-ENEA sulla Fusione, C.R. Frascati, Via E. Fermi 45, 00044 Frascati (Roma), Italy;

    Associazione EURATOM-ENEA sulla Fusione, IFP-CNR, Via R. Cozzi 53, 20125 Milano, Italy;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Associazione EURATOM-ENEA sulla Fusione, IFP-CNR, Via R. Cozzi 53, 20125 Milano, Italy;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Associazione EURATOM-ENEA sulla Fusione, IFP-CNR, Via R. Cozzi 53, 20125 Milano, Italy;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany<英作者单位十一>=Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

    Associazione EURATOM-ENEA sulla Fusione, IFP-CNR, Via R. Cozzi 53, 20125 Milano, Italy;

    Max-Planck-Institut fur Plasmaphysik, EURATOM Association, Boltzmannstr. 2, 85748 Garching bei Miinchen, Germany;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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