Modeling of ion cyclotron resonance frequency heating of proton-boron plasmas in EHL-2 spherical tokamak

Pub Date : 2024-10-01 DOI:10.1088/2058-6272/ad68ae
Xianshu WU, Jingchun LI, Jiaqi DONG, Yuejiang SHI, Guoqing LIU, Yong LIU, Zhiqiang LONG, Buqing ZHANG, Baoshan YUAN (袁宝山), Y. K. Martin PENG, Minsheng LIU (刘敏胜)
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Abstract

Ion cyclotron resonance heating (ICRH) stands out as a widely utilized and cost-effective auxiliary method for plasma heating, bearing significant importance in achieving high-performance discharges in p-11B plasmas. In light of the specific context of p-11B plasma in the EHL-2 device, we conducted a comprehensive scan of the fundamental physical parameters of the antenna using the full-wave simulation program TORIC. Our preliminary result indicated that for p-11B plasma, optimal ion heating parameters include a frequency of 40 MHz, with a high toroidal mode number like to heat the majority H ions. In addition, we discussed the impact of concentration of minority ion species on ion cyclotron resonance heating when 11B serves as the heavy minority species. The significant difference in charge-to-mass ratio between boron and hydrogen ions results in a considerable distance between the hybrid resonance layer and the tow inverted cyclotron resonance layer, necessitating a quite low boron ion concentration to achieve effective minority heating. We also considered another method of direct heating of hydrogen ions in the presence of boron ion minority. It is found that at appropriate boron ion concentrations ( ), the position of the hybrid resonance layer approaches that of the hydrogen ion cyclotron resonance layer, thereby altering the polarization at this position and significantly enhancing hydrogen ion fundamental absorption.
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EHL-2 球形托卡马克中质子-硼等离子体的离子回旋共振频率加热建模
离子回旋共振加热(ICRH)是等离子体加热的一种广泛应用且经济有效的辅助方法,对于在 p-11B 等离子体中实现高性能放电具有重要意义。针对 EHL-2 装置中 p-11B 等离子体的具体情况,我们使用全波仿真程序 TORIC 对天线的基本物理参数进行了全面扫描。初步结果表明,对于 p-11B 等离子体,最佳离子加热参数包括频率为 40 MHz 的高环模数,以加热大部分 H 离子。此外,我们还讨论了当 11B 作为重少数离子时,少数离子的浓度对离子回旋共振加热的影响。硼离子和氢离子之间的电荷质量比差异很大,导致混合共振层和拖曳反向回旋共振层之间有相当大的距离,因此需要相当低的硼离子浓度才能实现有效的少数离子加热。我们还考虑了另一种在硼离子少数的存在下直接加热氢离子的方法。我们发现,在适当的硼离子浓度()下,混合共振层的位置接近氢离子回旋共振层的位置,从而改变了该位置的极化,显著增强了氢离子的基波吸收。
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