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Overview of first Wendelstein 7-X high-performance operation

机译:第一个Wendelstein 7-X高性能操作概述

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The optimized superconducting stellarator device Wendelstein 7-X (with major radius R = 5.5 m, minor radius a = 0.5 m, and 30 m(3) plasma volume) restarted operation after the assembly of a graphite heat shield and 10 inertially cooled island divertor modules. This paper reports on the results from the first high-performance plasma operation. Glow discharge conditioning and ECRH conditioning discharges in helium turned out to be important for density and edge radiation control. Plasma densities of 1-4.5 x 10(19) m(-3) with central electron temperatures 5-10 keV were routinely achieved with hydrogen gas fueling, frequently terminated by a radiative collapse. In a first stage, plasma densities up to 1.4 x 10(20) m(-3) were reached with hydrogen pellet injection and helium gas fueling. Here, the ions are indirectly heated, and at a central density of 8 . 10(19) m(-3) a temperature of 3.4 keV with T-e/T-i = 1 was transiently accomplished, which corresponds to nT(i)(0)tau(E) = 6.4 x 10(19) keV s m(-3) with a peak diamagnetic energy of 1.1 MJ and volume-averaged normalized plasma pressure = 1.2%. The routine access to high plasma densities was opened with boronization of the first wall. After boronization, the oxygen impurity content was reduced by a factor of 10, the carbon impurity content by a factor of 5. The reduced (edge) plasma radiation level gives routinely access to higher densities without radiation collapse, e.g. well above 1 x 10(20) m(-2) line integrated density and T-e = T-i = 2 keV central temperatures at moderate ECRH power. Both X2 and O2 mode ECRH schemes were successfully applied. Core turbulence was measured with a phase contrast imaging diagnostic and suppression of turbulence during pellet injection was observed.
机译:石墨隔热罩和10个惯性冷却的岛状偏滤器组装完成后,优化的超导星化装置Wendelstein 7-X(长半径R = 5.5 m,短半径a = 0.5 m,等离子体积为30 m(3))重新开始运行。模块。本文报告了首次高性能等离子操作的结果。事实证明,氦气中的辉光放电调节和ECRH调节放电对于控制密度和边缘辐射非常重要。氢气燃料通常可达到1-4.5 x 10(19)m(-3)的等离子体密度,中心电子温度为5-10 keV,通常会因辐射塌陷而终止。在第一阶段中,通过氢颗粒注入和氦气供气,血浆密度达到1.4 x 10(20)m(-3)。在此,离子以8的中心密度间接加热。 10(19)m(-3)瞬间达到3.4 keV,Te / Ti = 1的温度,相当于nT(i)(0)tau(E)= 6.4 x 10(19)keV sm(-3) )具有1.1 MJ的峰值抗磁能,体积平均归一化等离子体压力β= 1.2%。随着第一壁的硼化,打开了获得高等离子体密度的常规通道。硼化后,氧杂质含量降低了10倍,碳杂质含量降低了5倍。降低的(边缘)等离子体辐射水平使常规方法可以获得更高的密度,而没有辐射塌陷,例如在中等ECRH功率下,远高于1 x 10(20)m(-2)的线积分密度和T-e = T-i = 2 keV中心温度。 X2和O2模式ECRH方案都已成功应用。用相衬成像诊断仪测量核心湍流,并观察到颗粒注入过程中的湍流抑制。

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