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金属学报  2025, Vol. 61 Issue (11): 1689-1702    DOI: 10.11900/0412.1961.2024.00047
  研究论文 本期目录 | 过刊浏览 |
Zr-0.75Sn-0.35Fe-0.15Cr-xNb合金在高温空气/蒸汽混合气氛中的氧化行为
俞强, 徐诗彤(), 张佳楠, 姚美意(), 胡丽娟, 谢耀平, 周邦新
上海大学 材料研究所 上海 200072
Oxidation Behaviors of Zr-0.75Sn-0.35Fe-0.15Cr- xNb Alloys in High-Temperature Steam with Air
YU Qiang, XU Shitong(), ZHANG Jianan, YAO Meiyi(), HU Lijuan, XIE Yaoping, ZHOU Bangxin
Institute of Materials, Shanghai University, Shanghai 200072, China
引用本文:

俞强, 徐诗彤, 张佳楠, 姚美意, 胡丽娟, 谢耀平, 周邦新. Zr-0.75Sn-0.35Fe-0.15Cr-xNb合金在高温空气/蒸汽混合气氛中的氧化行为[J]. 金属学报, 2025, 61(11): 1689-1702.
Qiang YU, Shitong XU, Jianan ZHANG, Meiyi YAO, Lijuan HU, Yaoping XIE, Bangxin ZHOU. Oxidation Behaviors of Zr-0.75Sn-0.35Fe-0.15Cr- xNb Alloys in High-Temperature Steam with Air[J]. Acta Metall Sin, 2025, 61(11): 1689-1702.

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摘要: 

在发生失水事故(LOCA)过程中,锆合金包壳可能会暴露于空气和蒸汽的混合气氛中发生高温氧化,进而失去其结构完整性,威胁到核反应堆的安全,因此锆合金在高温空气/蒸汽混合气氛中的氧化行为是一个值得深入研究的问题。本工作熔炼并制备了Zr-0.75Sn-0.35Fe-0.15Cr-xNb (x = 0、0.15、0.30、0.50、1.0,质量分数,%)合金板状样品。采用同步热分析仪研究了5种锆合金在模拟LOCA工况下800~1200 ℃的20%空气+ 80%蒸汽混合气氛中的氧化行为,利用OM、SEM和配置波谱仪的电子探针显微分析仪分析了氧化样品横截面的显微组织和N、O元素分布。结果表明,Nb含量对锆合金高温氧化行为的影响非常复杂,锆合金抗高温氧化性能并不随Nb含量的变化呈单一变化规律,总体上添加Nb会使Zr-0.75Sn-0.35Fe-0.15Cr合金的抗高温氧化性能降低。5种锆合金的氧化动力学曲线大多遵循抛物线-直线或直线规律,随氧化温度升高和Nb含量增加而发生改变,并且在1000和1200 ℃发生氧化转折。在高温蒸汽中含有空气时会由于O2和N2的存在明显加速锆合金的氧化,其中N对锆合金的氧化起到类似“催化”作用;ZrN的形成和再氧化促进了疏松多孔氧化物的生成,导致氧化膜的保护作用减弱。在氧化过程中,Nb含量变化会影响锆合金基体的αβ和氧化膜单斜(m)↔四方(t)的复杂相变过程。此外,Nb有增大O在α-Zr中固溶的趋势,并且Nb的氧化促进氧化膜的开裂,对锆合金抗氧化性能产生不利影响;另一方面,Nb含量的增加又会降低阴离子空位浓度,Nb与O结合也会阻碍O的扩散,对锆合金的抗氧化性能起到改善作用。

关键词 锆合金失水事故高温氧化显微组织    
Abstract

Zirconium alloys are extensively utilized as fuel element materials in water-cooled nuclear reactors owing to their small thermal neutron absorption cross-section, exceptional resistance to high-temperature and high-pressure water corrosion, favorable compatibility with UO2, and moderate mechanical properties. Loss of coolant accidents (LOCAs) pose a critical risk during the operation of nuclear reactors. During such accidents, the zirconium alloy cladding may be exposed to a mixed atmosphere of air and steam, undergoing high-temperature oxidation that could compromise its structural integrity and threaten nuclear reactor safety. Therefore, understanding the oxidation behaviors of zirconium alloys in high-temperature air-steam environments is essential. This study focused on Zr-0.75Sn-0.35Fe-0.15Cr-xNb alloys (x = 0, 0.15, 0.30, 0.50, and 1.0; mass fraction, %), which were smelted and formed into plate samples. The oxidation behaviors of these alloys in a mixed atmosphere comprising 20% air and 80% steam at temperatures ranging from 800 oC to 1200 oC were investigated using a synchronous thermal analyzer under simulated LOCA conditions. The microstructure and distribution of N and O in the cross-section of the oxidized samples were examined via OM, SEM, and electron probe microanalysis coupled with wave-dispersive spectroscopy. Results indicate that the effect of Nb content on the high-temperature oxidation behavior of the zirconium alloys is complex and does not directly correlate with changes in Nb content. In general, adding Nb may reduce the high-temperature oxidation resistance of Zr-0.75Sn-0.35Fe-0.15Cr-xNb alloys. The oxidation kinetics curves of the five alloys predominantly follow parabolic-linear or linear laws and display variations with changes in oxidation temperature and Nb content. In particular, oxidation transitions occur at 1000 and 1200 oC. In high-temperature steam containing air, the oxidation of zirconium alloys is considerably accelerated by the presence of N2 and O2 in air, with N serving as a “catalytic-like” agent, providing new oxidation pathways. The formation and subsequent reoxidation of ZrN contribute to the creation of porous oxide layers, undermining the protective capability of the oxide film. The changing content of Nb during the oxidation process influences the αβ phase transformation in the zirconium alloy matrix and the monoclinic (m)↔tetragonal (t) phase transformation in the oxide film. Furthermore, Nb tends to increase the O solid solubility in α-Zr, and Nb oxidation promotes cracking of the oxide film, which detrimentally affects the oxidation resistance of the zirconium alloys. Conversely, an increase in Nb content reduces anion vacancy concentration and impedes O diffusion when Nb combines with O, thereby enhancing the oxidation resistance of the zirconium alloys.

Key wordszirconium alloy    loss of coolant accident (LOCA)    high-temperature oxidation    microstructure
收稿日期: 2024-02-08     
ZTFLH:  TL341  
基金资助:国家自然科学基金项目(51871141)
通讯作者: 姚美意,yaomeiyi@shu.edu.cn,主要从事核燃料包壳材料锆合金和容错燃料包壳材料的研究;
徐诗彤,xushitong@i.shu.edu.cn,主要从事核燃料包壳锆合金腐蚀研究
作者简介: 俞 强,男,1998年生,硕士生
AlloySnFeCrNbZr
0Nb0.730.320.14-Bal.
0.15Nb0.710.310.170.12Bal.
0.30Nb0.710.310.140.28Bal.
0.50Nb0.700.310.140.48Bal.
1.0Nb0.720.310.140.97Bal.
表1  实验用Zr-0.75Sn-0.35Fe-0.15Cr-xNb合金的成分分析结果 (mass fraction / %)
图1  Zr-0.75Sn-0.35Fe-0.15Cr-xNb合金在空气/蒸汽混合气氛中高温氧化的氧化增重曲线
T / oCAlloyTransitionTransition point / slnKnn
8000Nb--3.310.62
0.15Nb--3.290.66
0.30Nb--3.170.74
0.50Nb--2.730.94
1.0Nb--2.770.95
10000Nb--4.501.11
0.15NbBefore transition-4.021.00
First transition6661.761.92
Second transition19684.951.03
0.30NbBefore transition-4.421.11
First transition5943.511.54
Second transition13204.881.12
0.50NbBefore transition-4.531.17
First transition6963.031.79
Second transition15726.530.72
1.0NbBefore transition-4.201.09
First transition12541.821.91
Second transition21843.581.44
12000NbBefore transition-5.830.97
After transition3546.130.80
0.15NbBefore transition-6.090.98
After transition3546.460.77
0.30NbBefore transition-6.520.96
After transition3127.090.64
0.50NbBefore transition-6.080.98
After transition3126.530.72
1.0NbBefore transition-6.000.98
After transition2826.290.80
表2  Zr-0.75Sn-0.35Fe-0.15Cr-xNb合金在800~1200 ℃的空气/蒸汽混合气氛中的氧化动力学参数拟合结果
T / oCOxide time / sF0.15NbF0.30NbF0.50NbF1.0Nb
80018003.310.622.730.6
1080039.893.8265.1303.6
10001800-2.741.391.4-1.2
360024.969.791.768.6
1200180027.744.918.012.7
表3  与0Nb合金相比,0.15Nb、0.30Nb、0.50Nb和1.0Nb合金在800~1200 ℃空气/蒸汽混合气氛中氧化的氧化增重变化百分数 (%)
图2  5种合金在800~1200 ℃的空气/蒸汽混合气氛中氧化后横截面显微组织的OM像
图3  5种合金在800~1200 ℃的空气/蒸汽混合气氛中氧化后横截面显微组织的SEM像
图4  0.15Nb合金在800~1200 ℃的空气/蒸汽混合气氛中氧化后样品横截面的EPMA像和WDS元素面分布图
图5  1000和1200 ℃下0Nb、0.15Nb、0.50Nb和1.0Nb合金在空气/蒸汽混合气氛中的氧化增重与在N2/蒸汽混合气氛[21]和纯水蒸气气氛[19]中的氧化增重对比
AlloyΔw(N2/steam)[21] / Δw(steam)[19]Δw(Air/steam) / Δw(steam)[19]
1000 oC, 3600 s1200 oC, 1800 s1000 oC, 3600 s1200 oC, 1800 s
0Nb10.23.915.13.5
0.15Nb15.33.322.33.3
0.50Nb8.43.124.13.1
1.0Nb15.93.932.13.8
表4  1000和1200 ℃下0Nb、0.15Nb、0.50Nb和1.0Nb合金在空气/蒸汽混合气氛和N2/蒸汽混合气氛[21]中的氧化增重与纯水蒸气气氛[19]中的氧化增重比值
Reaction800 oC1000 oC1200 oCAverage
(4)-871.16-832.30-793.44-832.30
(5)-475.41-452.41-429.41-452.41
(6)-261.89-242.62-223.35-242.62
(7)-609.75-590.28-570.81-590.28
(8)-221.52-219.80-218.09-219.80
(9)-55.96-36.35-16.75-36.35
(10)-815.20-801.66-776.69-797.85
(11)-419.45-416.06-412.66-416.06
表5  800~1200 ℃氧化时反应(4)~(11)的Gibbs自由能(ΔG) (kJ·mol-1)
图6  锆合金在空气/蒸汽混合气氛中高温氧化的示意图
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