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Effective temperatures, sawtooth mixing, and stochastic diffusion ripple loss of fast H+ minority ions driven by ion cyclotron heating in the Tokamak Fusion Test Reactor

机译:托卡马克聚变测试反应堆中离子回旋加速器加热驱动的快速H +少数离子的有效温度,锯齿波混合和随机扩散波纹损失

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This paper presents studies of the H+ minority ions driven by Ion Cyclotron Radio Frequency (ICRF) heating in the Tokamak Fusion Test Reactor (TFTR) [R.J. Hawryluk et al., Phys. Plasmas 5, 1577 (1998)] deuterium plasmas using primarily passive H degrees flux detection in the energy range of 0.2-1.0 MeV. The measured passive H+ energy spectra are compared with active (Li pellet charge exchange) results. It is shown that in the passive mode the main donors for the neutralization of H+ ions in this energy range are C5+ ions. The measured effective H+ tail temperatures range from 0.15 MeV at an ICRF power of 2 MW to 0.35 MeV at 6 MW. Radial redistribution of ICRF-driven H+ ions was detected when giant sawtooth crashes occurred during the ICRF heating. The redistribution affected ions with energy below 0.7-0.8 MeV. The sawtooth crashes displaces H+ ions outward along the plasma major radius into the stochastic ripple diffusion domain where those ions are lost in similar to 10 msec. These observations are consistent with the model of the redistribution of energetic particles developed previously to explain the results of deuterium-tritium (DT) alpha-particle redistribution due to sawtooth oscillations observed in TFTR. The experimental data are also consistent with numerical simulations of H+ stochastic ripple diffusion losses. (C) 1999 American Institute of Physics. [References: 25]
机译:本文介绍了在托卡马克聚变测试反应堆(TFTR)中由离子回旋加速器射频(ICRF)加热驱动的H +少数离子的研究。 Hawryluk et al。,Phys。 Plasmas 5,1577(1998)]使用主要在0.2-1.0 MeV能量范围内进行无源H度通量检测的氘等离子体。将测得的被动H +能谱与主动(Li粒料交换)结果进行比较。结果表明,在被动模式下,用于中和H +离子的主要供体是C5 +离子。测得的有效H +尾部温度范围从ICRF功率2 MW的0.15 MeV到6 MW的0.35 MeV。当在ICRF加热过程中发生巨大的锯齿形碰撞时,检测到了ICRF驱动的H +离子的径向重新分布。重新分布会影响能量低于0.7-0.8 MeV的离子。锯齿形碰撞使H +离子沿着等离子长半径向外移位到随机波纹扩散域中,这些离子在此处损失了大约10毫秒。这些观察结果与先前开发的高能粒子重新分布模型一致,该模型用于解释由于TFTR中观察到的锯齿状振荡而导致的-((DT)α粒子重新分布的结果。实验数据也与H +随机波纹扩散损失的数值模拟一致。 (C)1999美国物理研究所。 [参考:25]

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