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首页> 外文期刊>Plasma physics and controlled fusion >High-power ECH and fully non-inductive operation with ECCD in the TCV tokamak
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High-power ECH and fully non-inductive operation with ECCD in the TCV tokamak

机译:大功率ECH和TCV托卡马克中的ECCD完全无感运行

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摘要

Experiments with high-power electron cyclotron heating (ECH) and current drive (ECCD) in the TCV tokamak are discussed. Power up to 2.7 MW from six gyrotrons is delivered to the tokamak at the second-harmonic frequency (82.7 GHz) in X-mode. The power is transmitted to the plasma by six independent launchers, each equipped with steerable mirrors that allow a wide variety of injection angles in both the poloidal and toroidal directions. Fully non-inductive operation of the tokamak has been achieved in steady state, for the full 2 s gyrotron pulse duration, by co-ECCD with a highest current to date of 210 kA at full power. The experimentally measured ECCD efficiency agrees well with predictions obtained from linear modelling. We have observed that the highest global efficiency attainable at a given power is limited by stability constraints. While the efficiency is maximum bn the magnetic axis, a disruptive MHD instability occurs when the width of the deposition profile is lower than a minimum value, which increases with total power. Many ECCD discharges display a high level of electron energy confinement, enhanced by up to a factor of two over the Rebut-Lallia-Watkins (RLW) scaling law, which by contrast is well satisfied in ohmic conditions. The longest confinement times (up to four times RLW) are observed with central counter-ECCD. Central electron heat diffusivities comparable to ohmic levels are obtained in these scenarios, with electron temperatures in excess of 10 keV. [References: 22]
机译:讨论了在TCV托卡马克中使用大功率电子回旋加速器(ECH)和电流驱动(ECCD)进行的实验。来自六个回旋管的高达2.7 MW的功率以X模式的第二谐波频率(82.7 GHz)被输送到托卡马克。功率通过六个独立的发射器传输到等离子体,每个发射器都配备了可操纵的反射镜,这些反射镜允许在极向和超环向两个方向上具有多种注入角。迄今为止,托卡马克在2 s的回旋加速器脉冲持续时间内一直处于稳定状态,在全功率下,其最大电流为210 kA,是迄今为止完全无感的操作。实验测量的ECCD效率与从线性建模获得的预测非常吻合。我们已经观察到,在给定功率下可获得的最高全局效率受到稳定性约束的限制。尽管效率在磁轴上最大,但当沉积轮廓的宽度小于最小值时,会破坏MHD,这会随总功率而增加。许多ECCD放电显示出高水平的电子能量约束,比Rebut-Lallia-Watkins(RLW)缩放定律提高了2倍,相比之下,在欧姆条件下可以很好地满足这一要求。使用中央计数器ECCD观察到最长的限制时间(最多为RLW的四倍)。在这些情况下,当电子温度超过10 keV时,可获得与欧姆级相当的中心电子热扩散率。 [参考:22]

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