基于有限元的长轴杆件硬质涂层的热应力研究
Study on Thermal Stress of Hard Coating of Long Axis Bar Based on Finite Element
DOI: 10.12677/MS.2022.1211118, PDF,    科研立项经费支持
作者: 王靖文, 宋慧瑾*, 王自龙:成都大学机械工程学院,四川 成都
关键词: 有限元分析热应力ABAQUS软件热力耦合 Finite Element Analysis Thermal Stress ABAQUS Software Thermal Coupling
摘要: 长轴杆件零部件因其结构的特殊性在表面硬质涂层的制备过程中受到一定限制。本文利用有限元模拟计算了长轴杆件表面Ti系涂层在600℃环境温度范围内杆件的热应力变化及涂层厚度对基体和涂层的影响。结果表明:在涂层制备过程中,杆件热应力在两端会出现应力集中,且随着温度上升,应力逐渐向杆件中间部分扩散,温度稳定后,应力集中现象逐渐消失;基体两端表面随着温度上升,出现中心应力低于四周应力的现象,使用的四种Ti系涂层材料中TiAlN涂层的热应力最大,为74.02 MPa,Ti的热应力最小,为38.01 MPa。涂层厚度的增加,在5~9 μm范围内,TiAlN涂层的热应力变化不明显。
Abstract: Due to the particularity of its structure, long axis bar parts in the surface hard coating preparation process are limited. In this paper, the thermal stress variation of Ti-based coating on the surface of long axis bar in 600˚C ambient temperature is calculated and the influence of coating thickness on the substrate and coating is simulated by finite element method. The results show that during the coating preparation process, the thermal stress of the rod will be concentrated at both ends, and as the temperature rises, the stress gradually diffuses to the middle part of the rod. After the temperature is stable, the stress concentration phenomenon gradually disappears. With the increase of temperature at both ends of the substrate, the central stress is lower than the surrounding stress. Among the four Ti-based coating materials used, the thermal stress of TiAlN coating is the largest, 74.02 MPa, and the thermal stress of Ti is the smallest, 38.01 MPa. With the increase of coating thickness, the thermal stress of TiAlN coating does not change obviously in the range of 5~9 μm.
文章引用:王靖文, 宋慧瑾, 王自龙. 基于有限元的长轴杆件硬质涂层的热应力研究[J]. 材料科学, 2022, 12(11): 1064-1069. https://doi.org/10.12677/MS.2022.1211118

参考文献

[1] 宋慧瑾, 鄢强, 李玫, 董志红, 杨强. 梯度纳米硬质涂层内部应力的有限元分析[J]. 真空科学与技术学报, 2015, 35(6): 726-731. [Google Scholar] [CrossRef
[2] 邹微微, 王玉霞, 徐扬, 张秀. AlN薄膜的热应力模拟计算[J]. 光机电信息, 2011, 28(1): 10-14.
[3] 周溯源. 氮硼化钛基纳米复合涂层制备、表征及性能研究[D]: [博士学位论文]. 武汉: 武汉大学, 2016.
[4] Ali, R., Sebastiani, M. and Bemporad, E. (2015) Influence of Ti-TiN Multilayer PVD-Coatings Design on Residual Stresses and Adhesion. Materials & Design, 75, 47-56. [Google Scholar] [CrossRef
[5] Yan, J., Mi, C.W. and Liu, Z.X. (2019) A Semianalytical and Finite-Element Solution to the Unbonded Contact between a Frictionless Layer and an FGM-Coated Half-Plane. Mathe-matics and Mechanics of Solids, 24, 448-464. [Google Scholar] [CrossRef
[6] Sun, Z.N., Li, X.P. and Li, X.H. (2021) The Finite Element Analysis of Elastic-Plastic Contact of Single Asperity with Different Materials. 2021 7th International Conference on Condition Monitoring of Machinery in Non-Stationary Operations (CMMNO), Guangzhou, 11-13 June 2021, 108-114. [Google Scholar] [CrossRef
[7] Yilmaz, K.B., et al. (2019) Analytical and Finite Ele-ment Solution of the Sliding Frictional Contact Problem for a Homogeneous Orthotropic Coating-isotropic substrate sys-tem. Journal of Applied Mathematics and Mechanics, 99, e201800117. [Google Scholar] [CrossRef
[8] Maria, V. and Pelekasis, N. (2021) Numerical Study of the Interac-tion between a Pulsating Coated Microbubble and a Rigid Wall. I. Translational Motion. Physical Review Fluids, 6, Arti-cle ID: 013601. [Google Scholar] [CrossRef
[9] Bolot, R., Aussavy, D. and Montavon, G. (2017) Applica-tion of FEM to Estimate Thermo-Mechanical Properties of Plasma Sprayed Composite Coatings. Coatings, 7, 12 p. [Google Scholar] [CrossRef
[10] Hu, Z.C., Liu, B., Wang, L., et al. (2020) Research Progress of Failure Mechanism of Thermal Barrier Coatings at High Temperature via Finite Element Method. Coatings, 10, 25 p. [Google Scholar] [CrossRef