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中国物理学会期刊

湍流和带状流在托卡马克等离子体中的非线性能量传递与能量耗散

Nonlinear energy transfers and dissipation in zonal flows and turbulence in tokamak edge plasmas

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  • 带状流和湍流阻尼是等离子体流(flow)演化中常见的物理现象, 湍流中的非线性能量传递是驱动流发展的基本机制. 本文基于HL-2A托卡马克边缘等离子体湍流与带状流实验, 利用双谱分析方法分析两点法测量的浮动电势数据, 从非线性能量函数分析的角度, 揭示了托卡马克边缘等离子体中, 带状流与湍流间以及湍流内部的非线性能量传递和湍流能量耗散共存的物理图景和机理. 研究结果表明, 湍流可在耗散的背景等离子体中存在和发展. 一方面观测到显著的带状流阻尼, 同时揭示了从测地声模(GAM)带状流向高频湍流的能量级联过程. 其中, GAM驱动的对流导致内部的波能量从低频向高频传递. 在另一类放电中, 发现了湍流阻尼与能量级联共存的现象. 能量级联导致大涡旋转变为小涡旋, 最终线性耗散. 在上述两种情况下, 仅有部分(约30%-40%)能量参与能量传递, 而大部分能量则因带状流和湍流的非线性阻尼作用而耗散. 注意上述比率估计值随具体放电参数的不同而有所变化. 湍流可因黏性与碰撞阻尼作用而自然衰减. 在HL-2A边缘等离子体湍流分析中也观察到了能量逆级联, 同时伴随着显著的湍流阻尼现象. 当湍流中参与逆级联的能量占比有限时, 湍流中的能量逆级联可以增强低频湍流, 但还不足以驱动带状流等大尺度结构.

     

    Zonal flow and turbulence damping are two common physical phenomena in the evolution of plasma flows, and nonlinear energy transfer in turbulence is the fundamental mechanism of flow driving. Based on HL-2A tokamak edge plasma turbulence and zonal flow experiments, this study employs the two-point method to measure floating potential signal data and utilizes bispectral analysis for data processing. From the perspective of nonlinear energy function analysis, it revealed the physical picture and mechanisms of coexisting nonlinear dissipation and nonlinear energy transfer in zonal flows and turbulence in tokamak edge plasmas. The findings indicate that turbulence can evolve and develop within fluid systems featuring background dissipation. Notably, a significant damping of zonal flows is observed. The research uncovers an energy cascade process from geodesic acoustic mode (GAM) zonal flows to high-frequency turbulence, where GAM-induced turbulent fluctuations cause internal wave energy to transfer from low- to high-frequency regions. In another discharge type, the coexisting phenomena of turbulence damping and energy cascade are observed, as shown in figure A. Energy cascade transforms large vortices into small ones, ultimately dissipating linearly. In both cases, only a portion (approximately 30%-40%) of nonlinear energy participates in energy transfer, while the majority dissipates due to nonlinear damping effects of zonal flows and turbulence. Note that the estimated ratio values mentioned above may vary depending on the specific discharge parameters. This demonstrates that turbulence can naturally decay through viscous and collisional damping. Collisional and other damping effects can trigger nonlinear energy dissipation. Additionally, the inverse energy cascade phenomena are observed in HL-2A edge plasma turbulence, accompanied by a pronounced turbulence damping. When the energy fraction involved in inverse energy cascade is limited, the inverse energy cascade in turbulence becomes insufficient to drive large-scale structures like zonal flows. The study reveals that the energy dissipation of zonal flow and turbulence includes two forms. The energy cascade in turbulence can convert a portion of large eddies into small eddies, which then dissipate linearly. Meanwhile, due to collisional damping and other damping effects, most low-frequency energy directly dissipates nonlinearly.

     

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