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Progress of tungsten spectral modeling for ITER edge plasma diagnostics based on tungsten spectroscopy in LHD

机译:基于LHD钨光谱法的钨纤维型诊断钨光谱建模进展

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Strong radiative cooling by tungsten ions in the core plasma is one of issues in fusion reactors. Quantitative analysis of tungsten density in divertor plasma, scrape-off layer, and main plasma relies on accuracy of spectroscopic model of tungsten ions. We have developed a collisional-radiative (CR) model for tungsten ions to estimate line intensities of tungsten ions and also have measured tungsten spectra in wide wavelength region from extreme ultraviolet (EUV) to visible wavelengths simultaneously in the Large Helical Device (LHD) with tungsten pellet injection to validate the CR model for tungsten ions. So-called unresolved transition array (UTA) measured in EUV spectra at 4.5–7?nm are commonly seen in fusion plasmas with electron temperature of around 1?keV, which corresponds to edge temperature in ITER. The UTA is strong and largely contributes to the radiation power at this temperature, so the CR model calculation is required to reproduce the UTA to estimate the tungsten radiation power. We have developed the CR model to include recombination processes, which were not considered before for tungsten ions, as a hybrid model with fine-structure levels and configuration-averaged levels for W25+–W39+ions. The 6?nm-peak of UTA is not still reproduced well, but the recombination processes and cascade from higher levels can enhance spectral intensities. Contribution of dielectronic recombination from the excited states of W28+ions is examined but it is small for W27+ions. The spectral profiles of n?=?4–5 transition peaks at 2–4?nm do not change much with recombination processes. Analysis of measured EUV spectra in LHD plasma shows that tungsten is accumulated first into core plasma to produce hollow temperature distribution due to large radiation power of tungsten ions, and continuous NBI heating recovers central electron temperature and the UTA appears again in EUV spectra with weaker intensity than one at the earlier phase. Reduced intensity of UTA and electron temperature estimated from EUV spectra indicate that tungsten is transported outward and the amount of tungsten emitting EUV spectra is reduced to about 1/4.
机译:通过核心等离子体中的钨离子的强烈辐射冷却是融合反应器中的问题之一。钨极血浆,刮削层和主等离子体中钨密度的定量分析依赖于钨离子的光谱模型精度。我们已经开发了一种用于钨离子的碰撞 - 辐射(Cr)模型,以估计钨离子的线强度,并且在大螺旋装置(LHD)中同时从极端紫外(EUV)中的宽波长区域中的钨光谱测量到可见波长钨颗粒注射以验证钨离子的Cr模型。所谓的未解决的过渡阵列(UTA)在EUV光谱中测量为4.5-7Ω·nm,通常在融合等离子体中看到,电子温度约为1Ω·keV,其对应于迭代中的边缘温度。 UTA强大,主要有助于该温度的辐射功率,因此CR模型计算需要再现UTA来估计钨辐射功率。我们已经开发了Cr模型以包括重组过程,该方法在钨离子之前未考虑,作为具有细结构水平的杂种模型和W25 + -W39 +离子的配置平均水平。 uta的6?nm峰值仍然仍然良好,但重组过程和来自较高水平的级联可以增强光谱强度。研究了来自W28 +离子的激发态的硫代重组的贡献,但为W27 +离子小。 Nα=α= 4-5的光谱分布在2-4Ω·4-5的过渡峰不会随着重组过程而变化很大。 LHD等离子体中测量的EUV光谱分析表明,钨罐累积成核等离子体,以产生由于钨离子的大辐射功率而产生中空温度分布,而连续的NBI加热恢复中央电子温度,强度较弱的EUV光谱再次出现UURA比早期阶段的一个。从EUV光谱估计的UTA和电子温度的强度表明钨以外输送,发射EUV光谱的钨量减少到约1/4。

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