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Self-organized criticality and the dynamics of near-marginal turbulent transport in magnetically confined fusion plasmas

机译:磁约束聚变等离子体中的自组织临界和近边湍流动力学

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The high plasma temperatures expected at reactor conditions in magnetic confinement fusion toroidal devices suggest that near-marginal operation could be a reality in future devices and reactors. By near-marginal it is meant that the plasma profiles might wander around the local critical thresholds for the onset of instabilities. Self-organized criticality (SOC) was suggested in the mid 1990s as a more proper paradigm to describe the dynamics of tokamak plasma transport in near-marginal conditions. It advocated that, near marginality, the evolution of mean profiles and fluctuations should be considered simultaneously, in contrast to the more common view of a large separation of scales existing between them. Otherwise, intrinsic features of near-marginal transport would be missed, that are of importance to understand the properties of energy confinement. In the intervening 20 years, the relevance of the idea of SOC for near-marginal transport in fusion plasmas has transitioned from an initial excessive hype to the much more realistic standing of today, which we will attempt to examine critically in this review paper. First, the main theoretical ideas behind SOC will be described. Secondly, how they might relate to the dynamics of near-marginal transport in real magnetically confined plasmas will be discussed. Next, we will review what has been learnt about SOC from various numerical studies and what it has meant for the way in which we do numerical simulation of fusion plasmas today. Then, we will discuss the experimental evidence available from the several experiments that have looked for SOC dynamics in fusion plasmas. Finally, we will conclude by identifying the various problems that still remain open to investigation in this area. Special attention will be given to the discussion of frequent misconceptions and ongoing controversies. The review also contains a description of ongoing efforts that seek effective transport models better suited than traditional equations to capture SOC dynamics. Most of these models, based on the use of fractional transport equations and related concepts, could prove useful both in reactor operation and experiment control and design.
机译:磁约束聚变环形装置在反应堆条件下预期的高等离子体温度表明,在未来的装置和反应堆中,接近极限的运行可能成为现实。接近极限是指血浆分布可能会在不稳定的局部临界阈值附近徘徊。 1990年代中期,提出了自组织临界度(SOC)作为描述近边缘条件下托卡马克等离子体输运动力学的更合适范例。它主张,在接近边缘时,应同时考虑均值剖面和波动的演变,这与更为普遍的观点是,两者之间存在较大的尺度分离。否则,将忽略近边际运输的内在特征,这对于理解能量约束的性质非常重要。在过去的20年中,SOC在聚变等离子体中近边缘传输的想法已经从最初的过度炒作转变为今天更为现实的地位,我们将在这篇综述文件中尝试对其进行批判性研究。首先,将描述SOC背后的主要理论思想。其次,将讨论它们如何与真实的磁约束等离子体中的近边缘传输动力学相关。接下来,我们将回顾从各种数值研究中学到的关于SOC的知识,以及它对我们今天进行熔融等离子体数值模拟的方式的意义。然后,我们将讨论从几个寻找聚变等离子体中SOC动态的实验中获得的实验证据。最后,我们将通过确定仍然需要在该领域进行调查的各种问题来得出结论。将特别注意对常见误解和持续争议的讨论。审查还描述了正在进行的工作,这些工作正在寻求比传统公式更适合捕获SOC动态的有效传输模型。这些模型中的大多数基于分数输运方程式及相关概念的使用,可证明对反应堆运行以及实验控制和设计均有用。

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