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H-MODE REGIMES AND OBSERVATIONS OF CENTRAL TOROIDAL ROTATION IN ALCATOR C-MOD

机译:振动器C-MOD的H型模式和中心环向旋转的观察

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The Enhanced Da or EDA H-mode regime in Alcator C-Mod has been investigated andrncompared in detail to ELM-free plasmas. (In this paper, ELM-free will refer to discharges with norntype I ELMs and with no sign of EDA, though technically, most EDA plasmas are ELM-free as well.)rnEDA discharges have only slightly lower energy confinement than comparable ELM-free ones, butrnshow markedly reduced impurity confinement. Thus EDA discharges do not accumulate impuritiesrnand typically have a lower fraction of radiated power. EDA plasmas are seen to be more likely at lowrnplasma current (q > 3.7 - 4), for moderate plasma shaping, (0.35 - 0.55), and for high neutral pressures.rnNo obvious trends were observed with input power or pressure (b). In both H-mode regimes, and inrnICRF heated L-modes, central impurity toroidal rotation has been deduced, from the Doppler shifts ofrnargon x-ray lines. Rotation velocities up to 1.3 x 10~5 m/s in the co-current direction have beenrnobserved in H-mode discharges that had no direct momentum input. There is a strong correlationrnbetween the increase in the central impurity rotation velocity and the increase in the plasma storedrnenergy, induced by ICRF heating. In otherwise similar discharges with the same stored energyrnincrease, plasmas with lower current rotate faster. The ion pressure gradient is an unimportantrncontributor to the central impurity rotation and the presence of a substantial core radial electric field isrninferred during the ICRF pulse. An inward shift of ions induced by ICRF waves could give rise to arnnon-ambipolar electric field in the plasma core. Comparisons with a neo-classical ion orbit shift modelrnshow good agreement with the observations, both in magnitude, and in the scaling with plasmarncurrent.
机译:已经研究了Alcator C-Mod中增强的Da或EDA H模式方案,并将其与不含ELM的血浆进行了详细比较。 (在本文中,无ELM指的是标准I型ELM且无EDA迹象的放电,尽管从技术上讲,大多数EDA等离子体也不含ELM。)rnEDA放电的能量限制仅比无ELM的低。 ,butrnshow显着降低了杂质限制。因此,EDA放电不会积聚杂质,通常具有较低的辐射功率。在低等离子电流(q> 3.7-4),中等等离子整形(0.35-0.55)和高中性压力下,EDA等离子体更有可能出现.rn在输入功率或压力下未观察到明显趋势(b)。在H模式和innICRF加热的L模式中,已经从菱形X射线线的多普勒频移推导了中心杂质环面旋转。在没有直接动量输入的H模式放电中,顺流方向的旋转速度高达1.3 x 10〜5 m / s。 ICRF加热引起的中心杂质旋转速度的增加与等离子体储能的增加之间有很强的相关性。在其他情况下,具有相同存储能量的类似放电会增加,具有较低电流的等离子体旋转得更快。离子压力梯度对中心杂质旋转不重要,并且在ICRF脉冲期间推断出存在明显的核心径向电场。由ICRF波感应的离子向内移动可能会在等离子体核心中产生arnnon-双极电场。与新古典离子轨道迁移模型的比较在大小和等离子电流的缩放方面均与观测结果吻合良好。

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