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捏合在阿迪亚-U托卡马克欧姆放电中氩杂质输运中的作用

Role of pinch in Argon impurity transport in ohmic discharges of Aditya-U Tokamak.

作者信息

Shah K, Ghosh J, Patel S, Chowdhuri M B, Jadeja K A, Shukla G, Macwan T, Kumar A, Dolui S, Singh K, Tanna R L, Patel K M, Dey R, Manchanda R, Ramaiya N, Kumar R, Aich S, Yadava N, Purohit S, Gupta M K, Nagora U C, Pathak S K, Atrey P K, Mayya K B K

机构信息

Department of Physics, Pandit Deendayal Energy University, Raisan, Gandhinagar, 382 007, India.

Institute for Plasma Research, Bhat, Gandhinagar, 382 428, India.

出版信息

Sci Rep. 2023 Sep 26;13(1):16087. doi: 10.1038/s41598-023-42746-2.

Abstract

We present experimental results of the trace argon impurity puffing in the ohmic plasmas of Aditya-U tokamak performed to study the argon transport behaviour. Argon line emissions in visible and Vacuum Ultra Violet (VUV) spectral ranges arising from the plasma edge and core respectively are measured simultaneously. During the experiments, space resolved brightness profile of Ar line emissions at 472.69 nm (3p4s P-3p4p D), 473.59 nm (3p4s P-3p4p P), 476.49 nm (3p4s P-3p4p P), 480.60 nm (3p4s P-3p4p P) are recorded using a high resolution visible spectrometer. Also, a VUV spectrometer has been used to simultaneously observe Ar line emission at 18.79 nm (2s2p P-2s2p P) and Ar line emission at 22.11 nm (2s S-2s2p P). The diffusivity and convective velocity of Ar are obtained by comparing the measured radial emissivity profile of Ar emission and the line intensity ratio of Ar and Ar ions, with those simulated using the impurity transport code, STRAHL. Argon diffusivities ~ 12 m/s and ~ 0.3 m/s have been observed in the edge (ρ > 0.85) and core region of the Aditya-U, respectively. The diffusivity values both in the edge and core region are found to be higher than the neo-classical values suggesting that the argon impurity transport is mainly anomalous in the Aditya-U tokamak. Also, an inward pinch of ~ 10 m/s mainly driven by Ware pinch is required to match the measured and simulated data. The measured peaked profile of Ar density suggests impurity accumulation in these discharges.

摘要

我们展示了在Aditya - U托卡马克的欧姆等离子体中进行微量氩杂质吹气实验的结果,以研究氩的输运行为。分别来自等离子体边缘和核心的可见光和真空紫外(VUV)光谱范围内的氩线发射被同时测量。在实验过程中,使用高分辨率可见光谱仪记录了472.69 nm(3p4s P - 3p4p D)、473.59 nm(3p4s P - 3p4p P)、476.49 nm(3p4s P - 3p4p P)、480.60 nm(3p4s P - 3p4p P)处氩线发射的空间分辨亮度分布。此外,一台VUV光谱仪被用于同时观测18.79 nm(2s2p P - 2s2p P)处的氩线发射和22.11 nm(2s S - 2s2p P)处的氩线发射。通过将测量的氩发射径向发射率分布以及氩与氩离子的线强度比与使用杂质输运代码STRAHL模拟的结果进行比较,获得了氩的扩散率和对流速度。在Aditya - U的边缘(ρ>0.85)和核心区域分别观测到氩的扩散率约为12 m/s和约0.3 m/s。边缘和核心区域的扩散率值均高于新经典值,这表明在Aditya - U托卡马克中氩杂质输运主要是反常的。此外,需要一个主要由Ware箍缩驱动的约10 m/s的向内箍缩来使测量数据和模拟数据相匹配。测量的氩密度峰值分布表明在这些放电中存在杂质积累。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7d5d/10522584/738766200a9e/41598_2023_42746_Fig1_HTML.jpg

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