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材料研究学报  2025, Vol. 39 Issue (3): 172-184    DOI: 10.11901/1005.3093.2024.165
  研究论文 本期目录 | 过刊浏览 |
热等静压态镍基高温合金的高温氧化
钟伟杰1, 焦东玲1, 刘仲武1(), 刘娜2, 许文勇2, 李周2, 张国庆2
1.华南理工大学材料科学与工程学院 广州 510640
2.中国航发北京航空材料研究院 先进高温结构材料重点实验室 北京 100095
High Temperature Oxidation of a HIPed Nickel-based Superalloy
ZHONG Weijie1, JIAO Dongling1, LIU Zhongwu1(), LIU Na2, XU Wenyong2, LI Zhou2, ZHANG Guoqing2
1.School of Materials Science and Engineering, South China University of Technology, Guangzhou 510640, China
2.Science and Technology on Advanced High-Temperature Structural Materials Laboratory, AECC Beijing Institute of Aeronautical Materials, Beijing 100095, China
引用本文:

钟伟杰, 焦东玲, 刘仲武, 刘娜, 许文勇, 李周, 张国庆. 热等静压态镍基高温合金的高温氧化[J]. 材料研究学报, 2025, 39(3): 172-184.
Weijie ZHONG, Dongling JIAO, Zhongwu LIU, Na LIU, Wenyong XU, Zhou LI, Guoqing ZHANG. High Temperature Oxidation of a HIPed Nickel-based Superalloy[J]. Chinese Journal of Materials Research, 2025, 39(3): 172-184.

全文: PDF(8441 KB)   HTML
摘要: 

研究了热等静压态镍基高温合金的高温氧化动力学、氧影响区的特征、相组成、微观形貌和元素分布,总结了高温氧化特征和内氧化物的生成过程。结果表明,这种热等静压态高温合金在950 ℃的氧化属于完全抗氧化级别,其氧化动力学曲线和氧影响区深度的变化曲线都符合抛物线变化规律。在氧化初期,合金基体中的Ti、Al离子沿原始颗粒边界(PPB)向表面快速扩散并生成连续的Cr2O3、TiO2和Al2O3混合氧化层,而氧原子沿PPB向内扩散与第二相发生原位氧化反应生成颗粒状内氧化物Al2O3。氧化24h后合金表面的氧化层由最外部的TiO2、Al2O3混合氧化层和底部的Cr2O3氧化层组成,在贫铬区出现连续的内氧化物TiO2和Al2O3。在氧化后期(氧化时间超过100 h)合金表面氧化层中最外部的TiO2氧化层脱落,贫铬区中的内氧化物TiO2和Al2O3呈连续树根状分布。

关键词 金属材料高温氧化热等静压镍基高温合金微观形貌    
Abstract

A Ni-based alloy Ni-(12~18) Cr, (10~14) Co, (2~6) W, (2~6) Mo, (2~6) Ti, (2~6) Al was prepared via hot isostatic pressing by 150 MPa at 1150 oC with its argon gas atomization powders as raw material. Then its oxidation behavior in air at 950 oC was studied by intermittent weighing method in terms of the oxidation kinetics, phase composition, microstructure and elemental distribution of oxide scale and characteristics of oxygen-affected zone etc. The results show that the oxidation resistance of the as-HIPed superalloy at 950 oC has reached the full oxidation resistance grade in accord with the national standards. Both the oxidation kinetics curve and the depth variation curve of oxygen-affected zone follow a parabolic law. In the early stage of oxidation, Ti and Al atoms in the matrix diffuse rapidly along the prior particle boundaries (PPB) towards the alloy surface and form a continuous mixed oxide layer of Cr2O3, TiO2 and Al2O3. However, oxygen atoms diffuse inward along the PPB and undergoes in-situ oxidation reaction with secondary phases to form granular internal oxide Al2O3. After 24 hours oxidation, the surface oxide scale consists of the outmost layer of mixed oxides TiO2 and Al2O3, and the inner layer of Cr2O3 oxide. The continuous internal oxides TiO2 and Al2O3 appear in Cr-depleted zone. In the later stage of oxidation (> 100 h), the outmost TiO2 oxide layer peels off from the alloy surface, and the internal oxides TiO2 and Al2O3 distributed in Cr-depleted zone in a continuous root-like manner. Finally, the high temperature oxidation mechanism and formation process of internal oxides in as-HIPed nickel-based superalloy was also discussed.

Key wordsmetallic materials    high temperature oxidation    hot isostatic pressing    nickel-based superalloy    microstructure
收稿日期: 2024-04-07     
ZTFLH:  TG132.32  
基金资助:国家重点基础研究发展计划(2021YFB3704000)
通讯作者: 刘仲武,教授,zwliu@scut.edu.cn,研究方向为磁性功能材料、粉末冶金和高温合金
Corresponding author: LIU Zhongwu, Tel: (020)22236906, E-mail: zwliu@scut.edu.cn
作者简介: 钟伟杰,男,1992年生,博士
图1  热等静压态高温合金在950 ℃的等温氧化动力学曲线、平均氧化速率以及单位面积质量增量与时间的关系
图2  热等静压态高温合金在950 ℃氧化不同时间的氧影响区金相组织
图3  热等静压态高温合金在950 ℃等温氧化不同时间后氧影响区的厚度
图4  热等静压态高温合金在950 ℃氧化不同时间后的掠入射XRD谱
图5  热等静压态高温合金在950 ℃氧化不同时间后的表面微观形貌
图6  热等静压态高温合金在950 ℃氧化不同时间后表面氧化层的特征
图7  热等静压态高温合金在950 ℃氧化不同时间后表面氧化层元素的分布(a) 0.5 h (b) 24 h (c) 500 h
图8  热等静压态高温合金在950 ℃氧化前期(0~100 h)截面的微观形貌和元素分布
图9  热等静压态高温合金在950 ℃氧化前期(> 100 h)的截面微观形貌和元素分布
图10  高温合金中Cr、Ti和Al发生氧化反应的吉布斯自由能与温度的关系
图11  高温合金的DSC曲线和未氧化的热等静压态高温合金腐蚀形貌
图12  热等静压态高温合金在950 ℃氧化400 h后内氧化物的微观形貌和元素分布
图13  热等静压态高温合金在950 ℃氧化的相转变和内氧化过程
图14  热等静压态高温合金在950 ℃氧化的截面示意图
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