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A SPHERICAL TOKAMAK EMPLOYING MAGNETICALLY DRIVEN PLASMA GUNS

机译:磁驱动等离子体枪的球形托卡马克

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In this study, the concept of a spherical tokamak with non-inductive current drive to be realized by an alternative method is presented. The analytical model of this conceptual design is a combination of peculiarities based on current drive by helicity injection as developed by Taylor and a spherical torus plasma with small aspect ratio (A between 1.2 and 2), and naturally large elongation (k in the range of 1.25 and 3) with an edge safety factor q_a between 1.5 and 4. The numerical scheme used in this computational experiment is constituted by the analytical expressions given by Peng and Wilson. In addition, the bootstrap current drive mechanism is also taken into consideration. These models are interactive. In the proposed system, a simulated single turn, very high current, toroidal field coil is controlled by a magnetically driven C-gun. The main part of the toroidal field coil consists of a shock heated, time varying, non-linear plasma belt in the flux conserver and a complementary back strap outside. The poloidal current loop is completed by a spark gap switch and a capacitor bank. The complete spherical torus plasma is formed by a multisegmented 24 C-guns system around the flux conserver. Because of the temperature and density gradients of these belts, pushed towards the centre of the flux conserver by the Lorentz forces, either toroidal or poloidal bootstrap currents are generated. On the other hand, helicity injection of the C-guns creates a second current drive mechanism. Consequently, a low aspect ratio, large elongated and strong paramagnetic spherical tokamak plasma is produced.
机译:在这项研究中,提出了一种通过替代方法实现的具有非感应电流驱动的球形托卡马克的概念。此概念设计的分析模型是基于泰勒(Taylor)开发的基于螺旋注入电流驱动的特性和具有较小长宽比(A在1.2和2之间)和自然地大的伸长率(k范围为k的球形圆环等离子体)的组合。 1.25和3)的边沿安全系数q_a在1.5和4之间。此计算实验中使用的数值方案由Peng和Wilson给出的解析表达式构成。另外,还考虑了自举电流驱动机制。这些模型是交互式的。在提出的系统中,模拟的单匝高电流环形磁场线圈由磁驱动的C型喷枪控制。环形场线圈的主要部分由位于通量存储器中的冲击加热,时变的非线性等离子带和外部的互补背带组成。极向电流环路由火花隙开关和电容器组完成。完整的球形环面等离子体由围绕助焊剂储存器的多段式24 C喷枪系统形成。由于这些带的温度和密度梯度被洛伦兹力推向通量保持器的中心,因此会产生环形或极向自举电流。另一方面,C枪的螺旋注入会产生第二种电流驱动机制。因此,产生了低纵横比,大的细长且强顺磁性的球形托卡马克等离子体。

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