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有限元方法在热障涂层研究领域中的发展与应用

刘延宽 王源生 王璐璐

刘延宽, 王源生, 王璐璐. 有限元方法在热障涂层研究领域中的发展与应用[J]. 航空动力学报, 2024, 39(10):20220762 doi: 10.13224/j.cnki.jasp.20220762
引用本文: 刘延宽, 王源生, 王璐璐. 有限元方法在热障涂层研究领域中的发展与应用[J]. 航空动力学报, 2024, 39(10):20220762 doi: 10.13224/j.cnki.jasp.20220762
LIU Yankuan, WANG Yuansheng, WANG Lulu. Development and application of finite element methods in research field of thermal barrier coatings[J]. Journal of Aerospace Power, 2024, 39(10):20220762 doi: 10.13224/j.cnki.jasp.20220762
Citation: LIU Yankuan, WANG Yuansheng, WANG Lulu. Development and application of finite element methods in research field of thermal barrier coatings[J]. Journal of Aerospace Power, 2024, 39(10):20220762 doi: 10.13224/j.cnki.jasp.20220762

有限元方法在热障涂层研究领域中的发展与应用

doi: 10.13224/j.cnki.jasp.20220762
基金项目: 天津市教委科研计划项目(2020KJ016)
详细信息
    作者简介:

    刘延宽(1988-),男,副教授,博士,主要从事热障涂层方向的研究。E-mail:yk-liu@cauc.edu.cn

  • 中图分类号: V231.1

Development and application of finite element methods in research field of thermal barrier coatings

  • 摘要:

    分别从热生成氧化物(TGO)生长行为及应力应变、热障涂层(TBC)整体热力学性能、热障涂层结构优化及寿命预测三大方面进行概述,分析近些年来有限元方法在该研究领域中的发展与应用,总结目前研究中存在的问题和局限性。目前研究的发展方向主要是将失效理论、多物理场耦合以及Python子程序等与复杂的物理模型相结合,以获取更为准确的有限元分析结果。然而受限于真实TGO形貌毫无规律、高温条件下材料物性参数不充足、陶瓷层内微观孔隙随机分布等诸多问题,所得计算结果相比实际仍存在一定差距。今后可以从物理模型精细度、层间边界条件、动态生长模拟等方面进行更深入的研究。

     

  • 图 1  TGO不规则形貌及生长模型[19]

    Figure 1.  Model of TGO irregular morphology and growth [19]

    图 2  TBC模型示意图[37]

    Figure 2.  Schematic of TBC model [37]

    图 3  冷却至25 ℃后,不同TGO厚度下界面等效塑性应变(ε)的分布 [37]

    Figure 3.  Distribution of equivalent plastic strain (ε) for different TGO thicknesses when TBC is cooled down to 25 ℃[37]

    图 4  在63次热循环后TBC热应力分布[41]

    Figure 4.  Thermal stress distribution of TBC after 63 thermal cycles [41]

    图 5  不同孔隙率下,热导率和弹性模量随孔径的变化[49]

    Figure 5.  Evolution of thermal conductivity and elastic modulus with pore size at different porosities [49]

    图 6  热流路径及温度分布[49]

    Figure 6.  Heat flow path and temperature distribution [49]

    图 7  孔隙横纵比和倾斜角对有效热导率的影响[50]

    Figure 7.  Effect of pore aspect ratio and pore tilt angle on thermal conductivity of coating [50]

    图 8  涡轮叶片温度分布 [62]

    Figure 8.  Temperature distribution of turbine blade[62]

    图 9  涡轮叶片应力分布[62]

    Figure 9.  Stress distribution of turbine blade[62]

    图 10  波长λ随陶瓷层和黏结层厚度的变化[83]

    Figure 10.  Wavelength λ variation with TC and BC thickness [83]

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  • 收稿日期:  2022-10-03
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