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气冷涡轮导叶流热耦合计算及机理

李心语 刘火星

李心语, 刘火星. 气冷涡轮导叶流热耦合计算及机理[J]. 北京航空航天大学学报, 2021, 47(11): 2378-2386. doi: 10.13700/j.bh.1001-5965.2020.0435
引用本文: 李心语, 刘火星. 气冷涡轮导叶流热耦合计算及机理[J]. 北京航空航天大学学报, 2021, 47(11): 2378-2386. doi: 10.13700/j.bh.1001-5965.2020.0435
LI Xinyu, LIU Huoxing. Conjugate heat transfer simulation and mechanism of air-cooled turbine guide vanes[J]. Journal of Beijing University of Aeronautics and Astronautics, 2021, 47(11): 2378-2386. doi: 10.13700/j.bh.1001-5965.2020.0435(in Chinese)
Citation: LI Xinyu, LIU Huoxing. Conjugate heat transfer simulation and mechanism of air-cooled turbine guide vanes[J]. Journal of Beijing University of Aeronautics and Astronautics, 2021, 47(11): 2378-2386. doi: 10.13700/j.bh.1001-5965.2020.0435(in Chinese)

气冷涡轮导叶流热耦合计算及机理

doi: 10.13700/j.bh.1001-5965.2020.0435
详细信息
    通讯作者:

    刘火星, E-mail: liuhuoxing@buaa.edu.cn

  • 中图分类号: V232.4;TK121

Conjugate heat transfer simulation and mechanism of air-cooled turbine guide vanes

More Information
  • 摘要:

    针对气冷涡轮叶片的多场耦合特性,利用流热耦合(CHT)方法,对采用不同气冷结构的高压涡轮导叶进行数值模拟。在内冷涡轮导叶算例中,对比实验数据选取精度较高的流热耦合计算方案,分析该内冷涡轮导叶的多场特性及耦合机理。在此基础上,以带有气膜冷却孔及内冷通道的气冷涡轮导叶为研究对象,重点围绕冷却射流与主流的相互作用,讨论近壁边界层中流热耦合关系及气冷效率影响因素等相关问题。结果表明:采用流热耦合计算方法及合适的湍流转捩模型有利于提高数值精度;气冷涡轮导叶的流场温度场密切耦合,流动换热特性互相影响;冷气射速低时,增加冷气流量可提高气膜冷却效率,冷气量达到一定值时,冷气流量增加将导致气膜冷却孔后上游冷却效果变差,下游冷却效果变好;冷气射速较高时,将与主流相互作用产生复杂流动结构(如肾形涡、马蹄涡等),对温度分布存在一定影响。

     

  • 图 1  MARK Ⅱ几何气动外形及内冷结构编号示意图

    Figure 1.  MARKⅡgeometry and schematic diagram of internal cooling structure numbering

    图 2  MARK Ⅱ叶片三维网格划分情况

    Figure 2.  Generation of 3D mesh of MarkⅡblade

    图 3  不同壁温条件下叶表温度分布曲线

    Figure 3.  Surface temperature distribution curves of blade under different wall temperature conditions

    图 4  不同计算模型求解的叶表温度分布曲线

    Figure 4.  Surface temperature distribution curves of blade solved by different calculation models

    图 5  不同PrT条件求解的叶表温度分布曲线

    Figure 5.  Surface temperature distribution curves of blade solved under different PrT conditions

    图 6  叶表压力分布曲线

    Figure 6.  Surface pressure distribution curve of blade

    图 7  MARKⅡ叶表马赫数云图

    Figure 7.  Contour of Mach number at surface of MARKⅡblade

    图 8  叶表温度分布曲线

    Figure 8.  Surface temperature distribution curve of blade

    图 9  叶表换热系数分布曲线

    图 10  流体域及叶片内部温度分布云图

    Figure 10.  Temperature distribution contour in fluid domain and blade interior

    图 11  叶片内部等效热应力分布

    Figure 11.  Distribution of equivalent thermal stress inside blade

    图 12  给定约束后叶片总变形量

    Figure 12.  Total variation quantity of blade with given constraints

    Figure 13.  Schematic diagram of outlet angle of film-cooling hole

    图 14  气冷叶片几何造型

    Figure 14.  Geometry model of air-cooled blade

    图 15  流体域网格划分

    Figure 15.  Mesh generation of fluid domain

    图 16  叶片网格组装示意图

    Figure 16.  Schematic diagram of assembled mesh of blade

    图 17  改型MARKⅡ叶表马赫数云图

    Figure 17.  Contour of Mach number at surface of retrofittedMARKⅡblade

    图 18  叶表温度云图

    Figure 18.  Contour of temperature at surface of blade

    图 19  不同吹风比下压力面温度分布

    Figure 19.  Temperature distribution of pressure surface under different blowing ratios

    图 20  不同冷气射速下气膜冷却孔下游流线放大图

    Figure 20.  Enlarged streamline distribution of downstream hole at different flow velocities of cold air

    图 21  高速射流条件下不同位置横向流线发展过程

    Figure 21.  Development of transverse streamlines at different positions under high-speed jet conditions

    图 22  高速射流条件下受剪切作用形成的二次涡对

    Figure 22.  Secondary vortex pair induced by shear under high-speed jet conditions

    图 23  高速射流条件下局部壁面极限流线

    Figure 23.  Local wall limit streamlines under high-speedjet conditions

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出版历程
  • 收稿日期:  2020-08-17
  • 录用日期:  2020-09-18
  • 网络出版日期:  2021-11-20

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