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A phenomenological explanation for the anomalous ion heating observed in the JET alpha-heating experiment of 1997

机译:对1997年JET alpha加热实验中观察到的异常离子加热的现象学解释

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摘要

In the so-called 'alpha-heating' experiment performed on the JET tokamak during the deuterium-tritium campaign of 1997, the ion temperature was found to be far exceeding (both in absolute value and in its rise time) the level that could have been expected from direct collisional heating by the fusion-born alpha particles themselves and energy equipartition with the electrons. To date, no explanation has been put forward for this long standing puzzle, despite much work having been performed on this subject in the early 2000s. Two analysis methods that have recently become available have been employed to re-analyse these observations of an anomalous ion heating. First, an algorithm based on the sparse representation of signals has been used to analyse magnetic, reflectometry and electron-cyclotron emission measurements of the turbulence spectra in the drift-wave range of frequencies. This analysis has then been complemented with turbulence simulations performed with the GENE code. We find, both experimentally and in the simulations, that the presence of a minority, but sufficiently large, population of fusion-born alpha particles that have not yet fully thermalized stabilizes the turbulence in the ion-drift direction, but practically does not affect the turbulence in the electron-drift direction. We link such stabilization of the ion-drift-wave turbulence to the increase in the ion temperature above the level achieved in similar discharges that did not have (at all or enough) alpha particles. When the fusion-born alpha particles have fully thermalized, the turbulence spectrum in the ion-drift direction reappears at somewhat larger amplitudes, which we link to the ensuing reduction in the ion temperature. This phenomenological dynamics fully corresponds to the actual experimental observations. By taking into account an effect of the alpha particles that had not been previously considered, our new analysis finally presents a phenomenological explanation for the so-far-unexplained anomalous ion heating observed in the JET alpha-heating experiment of 1997. Through the formulation of an empirical criterion for ion-drift-wave turbulence stabilization by fusion-born alpha particles, we also show why similar observations were not made in the other deuterium-tritium experiments run so far in JET and TFTR. This allows assessing the operational domain for this stabilization mechanism for ion-drift-wave turbulence in future burning plasma experiments such as ITER, which may open a new path towards the sustainment of a high energy gain in such forthcoming devices.
机译:在1997年的氘-运动中对JET托卡马克进行的所谓的“α-加热”实验中,发现离子温度远远超过了(绝对值和上升时间)可以达到的水平。熔体诞生的α粒子本身以及与电子的能量均等分配是直接碰撞加热所期望的。迄今为止,尽管在2000年代初已经在这个问题上进行了许多工作,但对于这个长期存在的难题尚未提出任何解释。最近使用了两种分析方法来重新分析异常离子加热的这些观察结果。首先,基于信号稀疏表示的算法已被用于分析在频率漂移波范围内湍流频谱的磁,反射测量和电子回旋辐射测量。然后,用GENE代码进行的湍流模拟对这一分析进行了补充。我们在实验和模拟中都发现,少数但还足够大的尚未完全热化的融合生成的α粒子的存在稳定了离子漂移方向上的湍流,但实际上并没有影响电子漂移方向的湍流。我们将离子漂移波湍流的这种稳定与离子温度的升高联系在一起,离子温度的升高高于没有(完全或不足)α粒子的类似放电所达到的水平。当融合生成的α粒子完全热化时,离子漂移方向上的湍流谱会以更大的幅度出现,这与随后离子温度的降低有关。这种现象学动力学完全符合实际的实验观察。考虑到先前未曾考虑过的α粒子的影响,我们的新分析最终为现象学解释了1997年JETα加热实验中观察到的无法解释的异常离子加热。作为通过熔体产生的α粒子稳定离子漂移波湍流的经验标准,我们还表明了为什么到目前为止在JET和TFTR中进行的其他氘-实验中没有进行类似的观察。这允许在未来燃烧的等离子体实验(例如ITER)中为离子漂移波湍流的稳定机制评估操作域,这可能会为维持这种即将到来的装置中的高能量增益开辟一条新途径。

著录项

  • 来源
    《Nuclear fusion》 |2012年第8期|p.13.1-13.26|共26页
  • 作者

    D. Testa; M. Albergante;

  • 作者单位

    CRPP, Association EURATOM-Confederation Suisse, EPFL, Lausanne, Switzerland;

    CRPP, Association EURATOM-Confederation Suisse, EPFL, Lausanne, Switzerland;

  • 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

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