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首页> 外文期刊>Nuclear Materials and Energy >Deposition of carbon inside gaps of castellated tungsten blocks with intrinsic misalignment
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Deposition of carbon inside gaps of castellated tungsten blocks with intrinsic misalignment

机译:具有固有失准的齿形钨块间隙内的碳沉积

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Highlight ? The castellated blocks are manufactured and installed at central divertor in KSTAR. ? The surface density of inside the toroidal and poloidal gap of castellated blocks is in a range from 0.5×10 15 up to 6.7×10 15 atom/cm 2 . ? Compare the carbon deposition on the toroidal and poloidal gaps, contribution of each species can be separated. ? The contribution of neutrals is common for both gaps. ? The carbon density on chamfered shape is the lowest in to the four shapes. ? At the Raman spectra, decrease of I(D)/I(G) as a function of distance from the gap entrance indicates the increase of hydrogen contents. Abstract When PFCs have castellated structure, co-deposition of fuel inside gaps between castellated blocks is an important issue. Four different shapes of castellated tungsten blocks were fabricated to study corresponding issues in KSTAR: Conventional “basic” rectangular shape, single chamfer leading edge, double-chamfer and rounded edge, with two different poloidal gap distances of 0.5mm and 1.0mm. These tungsten blocks were exposed plasma of L- and H-mode discharges during a whole campaign in 2014. The blocks were taken out from the vacuum vessel after the campaign. Gap deposition was analyzed by Electron Probe X-ray Micro Analyzer (EPMA) to obtain carbon surface density (atoms/cm 2 ), and by Raman spectroscopy to identify chemical bonding structure of carbon deposits in gaps. The carbon surface density in toroidal and poloidal gaps was in a range from 0.5 × 10 15 atom/cm 2 up to 6.7 × 10 15 atom/cm 2 . At the gap entrance, contribution of ions is 6.0–6.7 × 10 15 atom/cm 2 , decreased down to 1.0 × 10 15 atom/cm 2 at a depth of 0.5mm, and remains constant afterwards. The contribution of charge exchange neutral is about 3.0 × 10 15 atom/cm 2 at the gap entrance, and then gradually decreases as a function of distance from the entrance. Deposition in 1.0mm wide gaps show much larger deposition patterns and that particles have reached much deeper inside the gap. Raman spectra show that the intensity ratio I(D)/I(G) decreases from top to the depth of 5mm indicating the increase of hydrogen contents.
机译:突出显示? cast形块在KSTAR的中央分流器上制造和安装。 ? cast形块的环状和多倍间隙内部的表面密度在0.5×10 15至6.7×10 15原子/ cm 2的范围内。 ?比较碳沉积在环形和极向间隙上,每种物质的贡献可以分开。 ?对于这两个差距,中性因素的贡献是共同的。 ?在四个形状中,倒角形状的碳密度最低。 ?在拉曼光谱中,I(D)/ I(G)的减少是距间隙入口的距离的函数,表明氢含量增加。摘要当全氟化碳具有have堡结构时,在cast堡块之间的间隙内燃料的共沉积是一个重要问题。制作了四种不同形状的齿形钨块以研究KSTAR中的相应问题:常规的“基本”矩形形状,单倒角前缘,双倒角和倒圆角,两种不同的倍体间隙距离分别为0.5mm和1.0mm。这些钨块在2014年的整个战役中均暴露于L型和H型放电的等离子体中。战役结束后,将这些钨块从真空容器中取出。通过电子探针X射线微分析仪(EPMA)分析间隙沉积,以获得碳表面密度(atoms / cm 2),并通过拉曼光谱法鉴定间隙中碳沉积物的化学键结构。环状和多倍间隙中的碳表面密度在0.5×10 15原子/ cm 2至6.7×10 15原子/ cm 2的范围内。在间隙入口处,离子的贡献为6.0–6.7×10 15原子/ cm 2,在0.5mm的深度处下降至1.0×10 15原子/ cm 2,此后保持恒定。电荷交换中性在间隙入口处的贡献约为3.0×10 15原子/ cm 2,然后随着距入口的距离而逐渐减小。在1.0毫米宽的间隙中进行的沉积显示出更大的沉积图案,并且颗粒在间隙内部的深度更深。拉曼光谱显示强度比I(D)/ I(G)从顶部到5mm深度减小,表明氢含量增加。

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