首页> 外文OA文献 >Measurement of high-k density fluctuation wavenumber spectrum in MAST and Doppler backscattering for spherical tokamaks
【2h】

Measurement of high-k density fluctuation wavenumber spectrum in MAST and Doppler backscattering for spherical tokamaks

机译:masT中高k密度波动波数谱的测量   球形托卡马克的多普勒反向散射

摘要

The high-k ($7 \lesssim k_{\bot} \rho_i \lesssim 11$) wavenumber spectrum ofdensity fluctuations has been measured for the first time in MAST [B. Lloyd etal, Nucl. Fusion 43, 1665 (2003)]. This was accomplished with the firstimplementation of Doppler backscattering (DBS) for core measurements in aspherical tokamak. DBS has become a well-established and versatile diagnostictechnique for the measurement of intermediate-k ($k_{\bot} \rho_i \sim 1$, andhigher) density fluctuations and flows in magnetically confined fusionexperiments. A novel implementation with 2D steering was necessary to enableDBS measurements in MAST, where the large magnetic field pitch angle presents achallenge. We report on the scattering considerations and ray tracingcalculations used to optimize the design and present data demonstratingmeasurement capabilities. Initial results confirm the applicability of thedesign and implementation approaches, showing the strong dependence ofscattering alignment on toroidal launch angle. We also present comparisons ofDBS plasma velocity measurements with charge exchange recombination and beamemission spectroscopy measurements, which show reasonable agreement over mostof the minor radius, but imply large poloidal flows approaching the magneticaxis in a discharge with an internal transport barrier. The 2D steering isshown to enable high-k measurements with DBS, at $k_{\bot}>20\\mathrm{cm}^{-1}$ ($k_{\bot} \rho_i>10$) for launch frequencies less than 75GHz; this capability is used to measure the wavenumber spectrum of turbulenceand we find $|n(k_{\bot})|^2 \propto k_{\bot}^{- 4.7 \pm 0.2}$ for $k_{\bot}\rho_i \approx 7-11$, which is similar to the expectation for the turbulentkinetic cascade of $|n(k_{\bot})|^2 \propto k_{\bot}^{- 13/3}$.
机译:在MAST中首次测量了高k($ 7 \ lesssim k _ {\ bot} \ rho_i \ lesssim 11 $)波数频谱密度波动。 Lloyd etal,Nucl。 [Fusion 43,1665(2003)]。这是通过在非球面托卡马克中首次实现多普勒反向散射(DBS)进行岩心测量而实现的。 DBS已成为一种成熟的通用诊断技术,用于测量磁约束聚变实验中的中间k($ k _ {\ bot} \ rho_i \ sim 1 $和更高)密度波动和流动。要在MAST中进行DBS测量,必须采用一种新颖的2D操纵实施方案,在该方案中,大的磁场俯仰角会带来挑战。我们报告了用于优化设计的散射注意事项和光线追踪计算,并展示了证明测量能力的数据。初步结果证实了该设计和实施方法的适用性,表明散射对准与环形发射角的强烈依赖性。我们还介绍了DBS等离子体速度测量与电荷交换重组和beamemission光谱学测量的比较,这些结果显示在大部分较小半径上都具有合理的一致性,但意味着在具有内部传输屏障的放电中接近磁轴的大的胶体流。图中显示了2D导向功能,可以使用DBS在发射频率$ k _ {\ bot}> 20 \\ mathrm {cm} ^ {-1} $($ k _ {\ bot} \ rho_i> 10 $)下进行高k测量小于75GHz;此功能用于测量湍流的波数谱,我们发现$ | n(k _ {\ bot})| ^ 2 \ propto k _ {\ bot} ^ {-4.7 \ pm 0.2} $对于$ k _ {\ bot} \ rho_i \ approx 7-11 $,类似于对$ | n(k _ {\ bot})| ^ 2 \ propto k _ {\ bot} ^ {-13/3} $的湍流级联的期望。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号