1. Advanced probes for edge plasma diagnostics on the CASTOR tokamak 探针在托卡马克边界等离子体诊断中的应用 组员 : 顾翔 陶军 金钊 吴铭钐 胡文慧 等离子体所 报告人 胡文慧 2014.10.15 J Stöckel,et al, Advanced probes for edge plasma diagnostics on the CASTOR tokamak, Journal of Physics, Conference Series, 63 (2007), 012001

2. Fig.1 CASTOR -Czech Academy of Sciences TORus Major radius0.4 m Minor radius0.1 m Toroidal magnetic field( 环向磁场 )<1.3 T Plasma current<15 kA Pulse length50 ms Plasma temperature0.20 keV Plasma density~ 1×10 19 m -3 Confinement time< 1 ms Edge density ~2×10 18 m -3 Edge temperature10-40 eV Built in Kurchatov Inst. Moscow 1958 Operational in IPP Prague since 1977 Reconstructed (new vessel) 1985 Associated to EURATOM 1999 Last shot 26 Oct 2007 CASTOR tokamak

3. It is evident that understanding of underlying physics in the edge plasma requires simultaneous measurement: - Plasma parameters like density, temperature, potential with a good spatial and temporal resolution (turbulence) ( 等离子体温度, 密度, 电势测量需要高的空间和时间分辨率 ) - Plasma flows in poloidal (and toroidal) direction ( 等离子体在换向和极向两个方向上都有流通量 ) A practical solution for small scale experiments => electric (Langmuir) probes ( 朗缪探针 ) Alternatively in large experiments (more sophisticated diagnostics): Fast cameras are used to visualize the density fluctuations ( ~100 k USD) ( 足够快的可视化测量 等离子体密度波动变化 ) Beam emission spectroscopy Microwave scattering …… What diagnostics are required ?

4. Single Langmuir probe 简单的工作原理示意图 Floating potential Ion saturation current

5. Rake probe on CASTOR-----Langmuir Probe Array ( 朗缪探针阵列 ) 时间分辨率 1~2 ms 16 small tips (diameter=2 mm) Distance of tips 2.5 mm Total extension 35 mm Fig.2 Picutre of single (left) and the double (right) rake probes The individual tips can operate in a sweeping mode and the current – voltage characteristic can be measured to determine the radial profile of electron density and temperature Fig.3 Radial profile of the electron temperature at the edge of CASTOR

6. Fig. 4 Electric circuit for measurement of the floating potential and the ion saturation current for probe arrays used on CASTOR. The switch is used to change the mode of operation between shots of operation. Fig. 5 Radial profile of the floating potential V fl (red circles) and the ion saturation current density J sat (blue triangles). 红：离子饱和流测量环路 蓝：悬浮电位测量环路

7. 2D Array of Langmuir Probes （二维探针矩阵） 2D matrix of 64 tips 空间分辨率 Poloidal resolution  6 mm Radial resolution  4.5 mm limite r separatrix A snapshot of potential structures poloidally: 42 mm radial position [mm] 2D matrix of 64 Langmuir probes 2D Structure of Edge Turbulence on the CASTOR Tokamak

8. Poloidal ring of electric and magnetic probes ( 极向探针环 ) Fig. 6 Picture of the full poloidal ring of 96 Langmuir probes. Probes are located at the radius r = 85 mm and their mutual poloidal distance is 5.5 mm Fig. 7 Poloidal structure of edge turbulence 例如悬浮电位, 等离子体密度

9. Segmented tunnel probe (STP) ( 隧 道探针 ) Fig. 8 Schematic drawing of the tunnel probe Fig. 9 the temporal evolution of the electron density and temperature 实现瞬态测量，在数据采集频率的限制下，时 间分辨率为 1μs

10. Fig. 10 Schematic drawing of the probe head of the STP. Two segmented tunnels are mounted back-to-back Mach probe ( 马赫探 针 ) black plate segments Fig. 11 隧道探针和阵列探针测量的电子温度比较 为了为消除等离子体流动 (plasma flows) 带来的误差

11. Ball pen probe --- 直接测量等离子体电位 把探头伸进或审处探针壳壳，改变 R 值，当探头 位于 h=0 时， R=1 ， 优点是能够承受高的等离子体能量负荷，可以 用在大型 tokamak 里面得到足够高的时间和空 间分辨率的测量结果

12. Gunderstrup probe --- 测量等离子体粒 子通量 Top View Polar diagram of Ion saturation current 离子饱和流的极向分布图 Several (eight) segments with a different orientation with respect to magnetic field lines The Gundestrup cauldron Parallel & perpendicular Mach numbes M || and M ⊥ derived with a high temporal resolution from the shape of the polar diagram 探针之间的间隙和角度偏差导致只有垂直和平行马赫数较为准确 Bt, Ip 环向和径向不对称说明既有 环向通量又有径向通量

13. Tools for edge plasma diagnostic and fluctuation measurements on CASTOR (Summary) Classical Langmuir probes – IV characteristics, local T e, n e, V fl at the plasma edge, routine measurements Radial & Poloidal arrays of Langmuir probes for spatially-temporally resolved measurements of plasma fluctuations Advanced probes – Segmented tunnel probe - a quite novel concept for fast T e and T i measurements Ball pen probe & Emissive probe – Direct measurement of plasma potential Oriented probes - Gundestrup and Mach probe for flow measurements during biasing experiments