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Reduction of RF-sheaths potentials by compensation or suppression of parallel RF currents on ICRF antennas

机译:通过补偿或抑制ICRF天线上的并行RF电流来降低RF鞘电势

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Radio frequency (RF) sheaths are suspected of limiting the performance of present-day ion cyclotron range of frequencies (ICRFs) antennas over long pulses and should be minimized in future fusion devices. Within the simplest models, RF-sheath effects are quantified by the integral V_(RF) = ∫ E_(‖) · d/ where the parallel RF field E_(‖) is linked with the slow wave. On 'long open field lines' with large toroidal extension on both sides of the antenna it was shown that V_(RF) is excited by parallel RF currents j_(‖) flowing on the antenna structure.rnIn this paper, the validity of this simple sheath theory is tested experimentally on the Tore Supra (TS) ITER-like antenna prototype (ILP), together with antenna simulation and post-processing codes developed to compute V_(RF). The predicted poloidal localization of high-| V_(RF) | zones is confronted to that inferred from experimental data analysis. Surface temperature distribution on ILP front face, as well as ILP-induced modifications of RF coupling and hot spots on a magnetically connected lower hybrid current drive antenna, indicates local maxima of dc plasma potential in both the upper and lower parts of the ILP. This result, qualitatively conforming to V_(RF) simulations, is interpreted in terms of j_(‖) flowing on ILP frame.rnOnce the validation is done, such reliable theoretical models and numerical codes are then employed to provide predictive results. Indeed, we propose two ways to reduce | V_(RF) | by acting on j_(‖) on the antenna front face. The first method, more adapted for protruding antennas, consists of avoiding the j‖ circulation on the antenna structure, by slotting the antenna frame on its horizontal edges and by partially cutting the Faraday screen rods.rnThe second method, well suited for recessed antennas, consists of compensating j_(‖) of opposite signs along long flux tubes, with parallelepiped antennas aligned with (tilted) flux tubes.rnThe different concepts are assessed numerically on a two-strap TS antenna phased [0, n] using near RF fields from the antenna code TOPICA. Simulations stress the need to suppress all current paths for j_(‖) to substantially reduce | V_(RF) | over the whole antenna height.
机译:怀疑射频(RF)护套会限制长脉冲下当今离子回旋加速器频率范围(ICRF)天线的性能,因此在未来的融合设备中应将其最小化。在最简单的模型中,RF鞘效应通过积分V_(RF)=∫E_(‖)·d /来量化,其中并行RF场E_(‖)与慢波相关。在天线两侧具有较大环形延伸的“长开放磁场线”上,表明V_(RF)被流过天线结构的并行RF电流j_(‖)激发。rn本文证明了这种简单方法的有效性护套理论是在类似Tore Supra(TS)ITER的天线原型(ILP)上进行实验测试的,同时还开发了天线仿真和开发用于计算V_(RF)的后处理代码。高||的预测的倍性局部化V_(RF)|从实验数据分析得出的结论是这些区域面临的挑战。 ILP正面的表面温度分布,以及ILP感应的射频耦合和磁连接的下部混合电流驱动天线上的热点的变化,表明ILP上部和下部均存在直流等离子体电势的局部最大值。该结果在质量上符合V_(RF)模拟,将根据在ILP框架上流动的j_(‖)进行解释。一旦完成验证,然后将使用这种可靠的理论模型和数字代码来提供预测结果。实际上,我们提出了两种方法来减少| V_(RF)|通过作用在天线正面的j_(‖)上。第一种方法更适合于凸出天线,方法是通过在水平方向上开槽天线框架并部分切割法拉第屏蔽杆来避免天线结构上的j'循环。rn第二种方法非常适用于嵌入式天线,由沿长通量管补偿相反符号的j_(′)组成,平行六面体天线与(倾斜)通量管对齐。rn在相距[0,n]的两带TS天线上,使用来自天线代码TOPICA。模拟强调有必要抑制j_(‖)的所有电流路径,以大幅降低| V_(RF)|在整个天线高度上

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