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Experimental characterization of multiscale and multifield turbulence as a critical gradient threshold is surpassed in the DIII-D tokamak

机译:在DIII-D托卡马克中超过临界梯度阈值的多尺度和多场湍流的实验表征

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摘要

A critical gradient for long wavelength (k_θ ρ s ? 0.4) electron temperature fluctuations has been observed in an experiment in the DIII-D tokamak [J. L. Luxon, Nucl. Fusion 42, 614 (2002)], where below a threshold value of L_(Te) ~(-1) = | δ L_(Te)| / L_(Te)electron temperature fluctuations are constant and above they steadily increase. Above the critical gradient, the electron heat flux inferred by power balance also increases rapidly. Critical gradients are a predicted attribute of turbulence arising from linear instabilities and are thought to be related to transport stiffness. The presented results are the first direct, systematic demonstration of critical gradient behavior in turbulence measurements in a tokamak. The experiment was performed by changing the deposition location of electron cyclotron heating shot-to-shot to locally scan L_(Te) ~(-1) at r/a = 0.6 in L-mode plasmas; rotation was also varied by changing the momentum input from neutral beam injection. Temperature fluctuations were measured with a correlation electron cyclotron emission (CECE) radiometry system. In addition to the CECE measurements, an array of turbulence measurements were acquired to characterize fluctuations in multiple fields and at multiple scales as L_(Te) ~(-1) and rotation were modified: long wavelength (k_θ ρ s ? 0.5) density fluctuations were acquired with beam emission spectroscopy, the phase angle between electron temperature and density fluctuations was measured by coupling the CECE system and a reflectometer, intermediate scale (k_θ ρ s ~ 0.8) density fluctuations were measured with a Doppler backscattering (DBS) system, and low frequency flows were also measured with DBS. The accumulated measurements and trends constrain identification of the instability responsible for the observed critical gradient to the δ T e-driven trapped electron mode.
机译:在DIII-D托卡马克实验中,观察到了长波长(k_​​θρs≤0.4)电子温度波动的临界梯度[J. L.Luxon,Nucl。 [Fusion 42,614(2002)],其中低于阈值L_(Te)〜(-1)= | δL_(Te)| / L_(Te)电子温度波动是恒定的,并且在此之上稳定增加。在临界梯度之上,通过功率平衡推断出的电子热通量也迅速增加。临界梯度是线性不稳定性引起的湍流的预测属性,被认为与运输刚度有关。提出的结果是托卡马克湍流测量中临界梯度行为的首次直接,系统的演示。实验是通过改变电子回旋加速器的逐次沉积的沉积位置,以在L型等离子体中以r / a = 0.6局部扫描L_(Te)〜(-1)来进行的;旋转也通过改变来自中性束注入的动量输入而改变。用相关电子回旋加速器发射(CECE)辐射测量系统测量温度波动。除了CECE测量值外,还获得了一系列湍流测量值,以表征多个场的波动,并在L_(Te)〜(-1)和旋转被修改的多个尺度上进行了描述:长波长(k_​​θρs?0.5)密度波动用电子束发射光谱法获得,通过耦合CECE系统和反射计测量电子温度和密度波动之间的相角,通过多普勒背散射(DBS)系统测量中间尺度(k_θρs〜0.8)的密度波动,并且DBS还测量了低频流量。累积的测量值和趋势限制了对所观察到的δT e驱动的俘获电子模式的临界梯度的不稳定性的识别。

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