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基于阵列式陶瓷基复合材料铠甲的涡轮叶片冷却方案

吕东 戴小钦 刘英实 孔星傲 李泳凡

吕东, 戴小钦, 刘英实, 等. 基于阵列式陶瓷基复合材料铠甲的涡轮叶片冷却方案[J]. 航空动力学报, 2025, 40(4):20240525 doi: 10.13224/j.cnki.jasp.20240525
引用本文: 吕东, 戴小钦, 刘英实, 等. 基于阵列式陶瓷基复合材料铠甲的涡轮叶片冷却方案[J]. 航空动力学报, 2025, 40(4):20240525 doi: 10.13224/j.cnki.jasp.20240525
LYU Dong, DAI Xiaoqin, LIU Yingshi, et al. Turbine blade cooling scheme based on arrayed ceramic matrix composite armors[J]. Journal of Aerospace Power, 2025, 40(4):20240525 doi: 10.13224/j.cnki.jasp.20240525
Citation: LYU Dong, DAI Xiaoqin, LIU Yingshi, et al. Turbine blade cooling scheme based on arrayed ceramic matrix composite armors[J]. Journal of Aerospace Power, 2025, 40(4):20240525 doi: 10.13224/j.cnki.jasp.20240525

基于阵列式陶瓷基复合材料铠甲的涡轮叶片冷却方案

doi: 10.13224/j.cnki.jasp.20240525
基金项目: HY行动项目(KZ38230132)
详细信息
    作者简介:

    吕东(1979-),男,教授、博士生导师,博士,主要从事涡轮叶片冷却方面的研究。E-mail:ld@dlut.edu.cn

  • 中图分类号: V232

Turbine blade cooling scheme based on arrayed ceramic matrix composite armors

  • 摘要:

    基于金属与非金属材料组合式结构的设计思想,设计了一种采用阵列式陶瓷基复合材料(CMC)铠甲的涡轮叶片冷却方案。通过在叶片前部高热负荷区覆盖铠甲并代替原有叶型,以及在其间隙中通少量冷却气的方式,来加强对叶片金属基体的热防护。采用了三维流热耦合数值仿真方法,以及与典型气膜冷却对比的方式,对方案的强化冷却机理和可达到的效果开展了研究,并对部分设计方法进行了总结。方案在冷气用量降低了24.2%的同时,还可将金属区域冷却效果大幅度提高69.2%,达到了0.95,热防护效果显著。而此时CMC铠甲仍有不低于130 K的温度裕度,表明燃气温度在2000 K基础上还可以进一步提高。在设计方法和原则上,为避免出现前缘燃气入侵,应保证冷气压比不低于1.03。可通过使铠甲间缝隙交错和倾斜的优化方式来加强冷却效果。

     

  • 图 1  基于阵列式CMC铠甲的冷却方案

    Figure 1.  Cooling scheme based on arrayed CMC armors

    图 2  冷气流动路径示意图

    Figure 2.  Diagram of coolant flow path

    图 3  气膜冷却仿真模型

    Figure 3.  Simulation model of film cooling

    图 4  网格及局部加密

    Figure 4.  Mesh and local refinements

    图 5  θπ变化

    Figure 5.  Variation of θ with π

    图 6  冷气三维流线图(π=1.03)

    Figure 6.  3D streamlines of coolant (π=1.03)

    图 7  CMC铠甲方案燃气流线及β云图(π=1.03)

    Figure 7.  Gas streamlines and β contours of CMC armors scheme (π=1.03)

    图 8  两种方案金属区域Tw云图(π=1.03)

    Figure 8.  Metal region Tw contours of both schemes (π=1.03)

    图 9  ηθ的变化

    Figure 9.  Variation of η with θ

    图 10  CMC铠甲Tw云图(π=1.03)

    Figure 10.  Tw contours of CMC armors (π=1.03)

    图 11  前缘铠甲Tw云图和各π工况下的φ

    Figure 11.  Tw contours of leading edge armors and φ of each π condition

    表  1  边界条件及工质物性

    Table  1.   Boundary conditions & material characteristics

    位置 参数 数值
    燃气
    进口
    总压$p_{\mathrm{g}}^* $/kPa 2026.5
    总温$T_{\mathrm{g}}^* $/K 2000
    湍流度Ig/% 10.0
    冷气
    进口
    总压$p_{\mathrm{c}}^* $/kPa (1.01~1.05)$p_{\mathrm{g}}^* $
    静温Tc/K 700
    湍流度Ic/% 5.0
    出口 静压pout/kPa 1114.6
    主要
    物性
    金属导热系数λm/(W/(m·K)) 20.0
    CMC导热系数λcmc/(W/(m·K)) 8.0
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  • 收稿日期:  2024-07-30
  • 网络出版日期:  2024-11-19

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