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Use of reconstructed 3D equilibria to determine onset conditions of helical cores in tokamaks for extrapolation to ITER

机译:使用重构的3D平衡确定托卡马克中螺旋形核的起始条件以外推至ITER

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摘要

Large, spontaneous m = 1/1 helical cores are shown to be expected in tokamaks such as ITER with extended regions of low- or reversed- magnetic shear profiles and q near 1 in the core. The threshold for this spontaneous symmetry breaking is determined using VMEC scans, beginning with reconstructed 3D equilibria from DIII-D and Alcator C-Mod based on observed internal 3D deformations. The helical core is a saturated internal kink mode (Wesson 1986 Plasma Phys. Control. Fusion 28 243); its onset threshold is shown to be proportional to (dρ/dρ)/B_t~2 around q = 1. Below the threshold, applied 3D fields can drive a helical core to finite size, as in DIII-D. The helical core size thereby depends on the magnitude of the applied perturbation. Above it, a small, random 3D kick causes a bifurcation from axisymmetry and excites a spontaneous helical core, which is independent of the kick size. Systematic scans of the q-profile show that the onset threshold is very sensitive to the q-shear in the core. Helical cores occur frequently in Alcator C-Mod during ramp-up when slow current penetration results in a reversed shear q-profile, which is favorable for helical core formation. Finally, a comparison of the helical core onset threshold for discharges from DIII-D, Alcator C-Mod and ITER confirms that while DIII-D is marginally stable, Alcator C-Mod and especially ITER are highly susceptible to helical core formation without being driven by an externally applied 3D magnetic field.
机译:预计在托卡马克(如ITER)中会出现大型的,自发的m / n = 1/1的螺旋形磁心,而ITER具有低或反向磁性剪切剖面的扩展区域,磁心中的q接近1。使用VMEC扫描确定此自发对称性断裂的阈值,首先根据观察到的内部3D变形从DIII-D和Alcator C-Mod重建3D平衡。螺旋芯是饱和的内部扭结模式(Wesson 1986 Plasma Phys。Control。Fusion 28 243);它的起始阈值在q = 1附近与(dρ/dρ)/ B_t〜2成正比。在阈值以下,施加的3D场可以将螺旋形磁芯驱动到有限的大小,如DIII-D中所示。因此,螺旋芯的大小取决于所施加扰动的大小。在其上方,小的,随机的3D踢动会导致轴对称分叉并激发自发的螺旋形核心,而螺旋形的核心与踢动大小无关。对q轮廓的系统扫描显示,起始阈值对核心中的q剪切非常敏感。螺旋形铁心在Alcator C-Mod的加速过程中经常出现,这时缓慢的电流穿透会导致反向的剪切q形轮廓,这有利于螺旋形铁心的形成。最后,通过比较DIII-D,Alcator C-Mod和ITER放电的螺旋铁心起始阈值,可以确认,虽然DIII-D略微稳定,但Alcator C-Mod尤其是ITER在不被驱动的情况下极易形成螺旋铁心通过外部施加的3D磁场。

著录项

  • 来源
    《Nuclear fusion》 |2018年第3期|036004.1-036004.12|共12页
  • 作者单位

    Oak Ridge National Laboratory, Oak Ridge, TN, United States of America;

    Oak Ridge National Laboratory, Oak Ridge, TN, United States of America;

    Oak Ridge National Laboratory, Oak Ridge, TN, United States of America;

    Oak Ridge National Laboratory, Oak Ridge, TN, United States of America;

    Oak Ridge National Laboratory, Oak Ridge, TN, United States of America;

    Princeton Plasma Physics Laboratory, Princeton, NJ, United States of America;

    Oak Ridge National Laboratory, Oak Ridge, TN, United States of America;

    General Atomics, PO Box 85608, San Diego, CA, United States of America;

  • 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);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    helical core; snake; tokamak; stability;

    机译:螺旋芯蛇;托卡马克稳定性;

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