Transmission electron microscopy characterization of Fuel Cladding Chemical Interaction (FCCI) in ATR-irradiated HT9 clad U-10M (10M = 5Mo-4.3Ti-0.7Zr wt%) metallic fuel

IF 2.8 2区 工程技术 Q3 MATERIALS SCIENCE, MULTIDISCIPLINARY Journal of Nuclear Materials Pub Date : 2024-06-05 DOI:10.1016/j.jnucmat.2024.155209
Yachun Wang, Jatuporn Burns, Tiankai Yao, Luca Capriotti
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Abstract

The pseudo-binary metallic fuel alloy, U-10M (wt%, M is the optimal combination of Mo, Ti, and Zr), has the potential to increase fuel solidus temperature, reduce the onset temperature of body-centered cubic phase, and increase the fuel's chemical stability compared with the conventional U-10Zr (wt%) metallic fuel. Post Irradiation Examination (PIE) confirmed excellent fuel performance for the U-10M (10M=5Mo-4.3Ti-0.7Zr wt%) fuel irradiated in the Advanced Test Reactor (ATR) to 2.2 at% burnup at Peak Inner Cladding Temperature (PICT) of 650 °C, an upper bound temperature for metallic fuel. But previous PIE study also observed Fuel Cladding Chemical Interaction (FCCI) on the cladding side, which is known as a fuel performance limiting issue but has not been fully understood yet. As an effort to improve the understanding of FCCI phenomenon, this study performed Scanning Electron Microscopy (SEM) and in-depth Transmission Electron Microscopy (TEM) characterization on a FCCI region. The examined FCCI region is dominated by (U, Zr)(Fe, Cr)2, suggesting that U-Fe interdiffusion reaction played a key role in inducing FCCI. Additionally, the FCCI boundary into the cladding consists of four distinctive phases, (U, Zr)(Fe, Cr)2, fcc-Cr, tetragonal UCr0.1Fe9.9Si2, intermetallic σ-FeCr, and lanthanide fission products at concentration up to ∼5.5 at%. Another goal of this study is to verify the involvement of Ti and Mo in FCCI formation on the cladding side. Observable Ti is found halfway of the thickness in the examined FCCI region, while 0.3–5 at% Mo is detected across the entire thickness of the examined FCCI region. Neither Ti nor Mo reacted with HT9 cladding constituents despite their diffusion footmark. Therefore, alloying Ti and Mo into the U-Zr fuel should not complicate the interdiffusion reaction on the HT9 cladding side.

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ATR 辐照 HT9 包层 U-10M(10M = 5Mo-4.3Ti-0.7Zr wt%)金属燃料中燃料包层化学相互作用 (FCCI) 的透射电子显微镜特性分析
与传统的U-10Zr(重量百分比)金属燃料相比,U-10M(重量百分比,M为Mo、Ti和Zr的最佳组合)假二元金属燃料合金具有提高燃料固相温度、降低体心立方相的起始温度和提高燃料化学稳定性的潜力。辐照后检查(PIE)证实,U-10M(10M=5Mo-4.3Ti-0.7Zr wt%)燃料在先进试验反应堆(ATR)中辐照至 2.2 at% 烧损度(内包层峰值温度(PICT)为 650 ℃,这是金属燃料的上限温度)时,具有优异的燃料性能。但之前的 PIE 研究也观察到了包层侧的燃料包层化学相互作用 (FCCI),这是众所周知的限制燃料性能的问题,但尚未得到充分理解。为了加深对 FCCI 现象的理解,本研究对 FCCI 区域进行了扫描电子显微镜(SEM)和深入的透射电子显微镜(TEM)表征。所观察到的 FCCI 区域以 (U,Zr)(Fe,Cr)2 为主,这表明 U-Fe 间扩散反应在诱导 FCCI 方面发挥了关键作用。此外,进入包层的 FCCI 边界由四种不同的相组成,即 (U,Zr)(Fe,Cr)2、ccc-Cr、四方 UCr0.1Fe9.9Si2、金属间 σ-FeCr 和镧系裂变产物(浓度高达 ∼ 5.5 at%)。本研究的另一个目标是验证钛和钼参与包层侧 FCCI 形成的情况。在检查的 FCCI 区域中,可观察到一半厚度的钛,而在检查的 FCCI 区域的整个厚度上检测到 0.3-5 at% 的钼。尽管有扩散脚印,但钛和钼都没有与 HT9 包层成分发生反应。因此,在 U-Zr 燃料中加入钛和钼合金应该不会使 HT9 包层侧的相互扩散反应复杂化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Journal of Nuclear Materials
Journal of Nuclear Materials 工程技术-材料科学:综合
CiteScore
5.70
自引率
25.80%
发文量
601
审稿时长
63 days
期刊介绍: The Journal of Nuclear Materials publishes high quality papers in materials research for nuclear applications, primarily fission reactors, fusion reactors, and similar environments including radiation areas of charged particle accelerators. Both original research and critical review papers covering experimental, theoretical, and computational aspects of either fundamental or applied nature are welcome. The breadth of the field is such that a wide range of processes and properties in the field of materials science and engineering is of interest to the readership, spanning atom-scale processes, microstructures, thermodynamics, mechanical properties, physical properties, and corrosion, for example. Topics covered by JNM Fission reactor materials, including fuels, cladding, core structures, pressure vessels, coolant interactions with materials, moderator and control components, fission product behavior. Materials aspects of the entire fuel cycle. Materials aspects of the actinides and their compounds. Performance of nuclear waste materials; materials aspects of the immobilization of wastes. Fusion reactor materials, including first walls, blankets, insulators and magnets. Neutron and charged particle radiation effects in materials, including defects, transmutations, microstructures, phase changes and macroscopic properties. Interaction of plasmas, ion beams, electron beams and electromagnetic radiation with materials relevant to nuclear systems.
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