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脉冲爆震驱动下涡轮流场的非定常特征研究

刘俊余 王治武 李俊林 张子旭

刘俊余, 王治武, 李俊林, 等. 脉冲爆震驱动下涡轮流场的非定常特征研究[J]. 航空动力学报, 2025, 40(5):20230490 doi: 10.13224/j.cnki.jasp.20230490
引用本文: 刘俊余, 王治武, 李俊林, 等. 脉冲爆震驱动下涡轮流场的非定常特征研究[J]. 航空动力学报, 2025, 40(5):20230490 doi: 10.13224/j.cnki.jasp.20230490
LIU Junyu, WANG Zhiwu, LI Junlin, et al. Unsteady characteristics of turbine flow field driven by pulse detonation[J]. Journal of Aerospace Power, 2025, 40(5):20230490 doi: 10.13224/j.cnki.jasp.20230490
Citation: LIU Junyu, WANG Zhiwu, LI Junlin, et al. Unsteady characteristics of turbine flow field driven by pulse detonation[J]. Journal of Aerospace Power, 2025, 40(5):20230490 doi: 10.13224/j.cnki.jasp.20230490

脉冲爆震驱动下涡轮流场的非定常特征研究

doi: 10.13224/j.cnki.jasp.20230490
基金项目: 国家自然科学基金(12372338,U2241272); 陕西省自然科学基金(2023-JCYB-352,2022JZ-20); 广东省基础与应用基础研究基金(2023A1515011663)
详细信息
    作者简介:

    刘俊余(1997-),男,硕士,主要从事脉冲爆震燃烧室与轴流涡轮的匹配研究。E-mail:ljynwpu@163.com

    通讯作者:

    王治武(1981-),男,教授,博士,研究领域为燃烧与流动、爆震推进等。E-mail:malsoo@mail.nwpu.edu.cn

  • 中图分类号: V231.2

Unsteady characteristics of turbine flow field driven by pulse detonation

  • 摘要:

    为了揭示脉冲爆震的非定常性对涡轮流场的影响,建立了GE-E3两级高压涡轮的三维数值模型,以研究爆震驱动下涡轮的流场特征。对50%叶高处的基元级流动进行分析,对动叶表面的分离流动以及叶顶间隙的泄漏流动进行了研究。结果表明:前导激波驱动燃气以超声速流过涡轮流道,导致燃气在叶栅斜切口出现了明显的超声速斜切口膨胀以及叶栅外的自由膨胀。前导激波与叶片相互作用会造成气流攻角的大幅变化,并产生多处局部逆压梯度,导致叶片表面出现严重的流动分离。此外,前导激波作用于动叶会增大叶顶间隙两侧的压差,使得间隙泄漏流量急剧增大,这增强了泄漏流与主流的剪切和掺混,导致主流区出现明显的熵增。

     

  • 图 1  GE-E3两级高压涡轮几何模型及网格划分

    Figure 1.  GE-E3 two-stage high pressure turbine geometry model and meshing

    图 2  爆震驱动下涡轮入口参数随时间的变化

    Figure 2.  Variation of turbine inlet parameters with time under detonation driving

    图 3  不同网格尺寸划分下第一级动叶叶顶间隙泄漏流线

    Figure 3.  Rotor 1 tip clearance leakage streamline under different mesh sizes

    图 4  数值模拟与试验参数的对比

    Figure 4.  Comparison of simulation and experimental results

    图 5  50%叶高处的基元级温度分布随时间的变化

    Figure 5.  Temperature of elementary stage with 50% blade height changes with time

    图 6  50%叶高处的基元级相对马赫数分布随时间的变化

    Figure 6.  Relative Mach number of elementary stage with 50% blade height changes with time

    图 7  动叶入口气流角和速度三角形示意图

    Figure 7.  Inlet flow angle and velocity triangle of rotor blade

    图 8  两级动叶的入口平均相对气流角和相对速度

    Figure 8.  Average inlet relative flow angle and relative velocity of two-stage rotor blades

    图 9  前导激波与作用于第一级动叶的相对速度和流线分布

    Figure 9.  Relative velocity and streamline distribution under the interaction between leading shock wave and Rotor 1

    图 10  第一级动叶压力面和吸力面处的极限流线

    Figure 10.  Limiting streamlines at the pressure and suction surfaces of Rotor 1

    图 11  前导激波作用下第一级动叶叶顶间隙中部的流线和压力分布

    Figure 11.  Streamline and pressure distribution in the middle of Rotor 1 tip clearance under the action of leading shock wave

    图 12  两级动叶的泄漏流量随时间的变化

    Figure 12.  Variation of leakage flow rate of two-stage rotor with time

    图 13  前导激波作用下第一级动叶50%弦长处的熵与流线

    Figure 13.  Entropy and streamline at 50% chord of Rotor 1 under leading shock

    图 14  前导激波作用下第一级动叶机匣端区的轴向涡量

    Figure 14.  Axial vorticity in the end region of Rotor 1 casing under the action of leading shock wave

    表  1  试验工况下涡轮性能参数的对比

    Table  1.   Comparison of turbine performance parameters under test conditions

    参数试验结果数值结果
    涡轮效率/%92.5393.33
    落压比5.0144.969
    流量/(kg/s)11.8012.54
    功率/kW29733066
    下载: 导出CSV

    表  2  两级动叶的总压恢复系数

    Table  2.   Total pressure recovery coefficient of two-stage rotor

    工况条件总压恢复系数
    第一级动叶处第二级动叶处
    爆震驱动0.810.87
    NASA试验0.940.96
    下载: 导出CSV
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  • 收稿日期:  2023-07-28
  • 网络出版日期:  2024-06-23

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