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跨声速离心压气机激波与叶顶泄漏流相互作用数值研究

陈彦龙 张超炜 李广勇

陈彦龙, 张超炜, 李广勇. 跨声速离心压气机激波与叶顶泄漏流相互作用数值研究[J]. 航空动力学报, 2026, 41(X):20240788 doi: 10.13224/j.cnki.jasp.20240788
引用本文: 陈彦龙, 张超炜, 李广勇. 跨声速离心压气机激波与叶顶泄漏流相互作用数值研究[J]. 航空动力学报, 2026, 41(X):20240788 doi: 10.13224/j.cnki.jasp.20240788
Chen Yanlong, Zhang Chaowei, Li Guangyong. Numerical investigation of interaction between shock wave and tip leakage flow in transonic centrifugal compressors[J]. Journal of Aerospace Power, 2026, 41(X):20240788 doi: 10.13224/j.cnki.jasp.20240788
Citation: Chen Yanlong, Zhang Chaowei, Li Guangyong. Numerical investigation of interaction between shock wave and tip leakage flow in transonic centrifugal compressors[J]. Journal of Aerospace Power, 2026, 41(X):20240788 doi: 10.13224/j.cnki.jasp.20240788

跨声速离心压气机激波与叶顶泄漏流相互作用数值研究

doi: 10.13224/j.cnki.jasp.20240788
详细信息
    作者简介:

    陈彦龙(2000-),男,硕士生,主要从事离心压气机气动设计研究

    通讯作者:

    张超炜(1992-),男,讲师、硕士生导师,博士,主要从事叶轮机械气动热力学研究,E-mail:zhangchaowei@usst.edu.cn

  • 中图分类号: V231.1

Numerical investigation of interaction between shock wave and tip leakage flow in transonic centrifugal compressors

  • 摘要:

    对于跨声速离心压气机,激波与泄漏流的相互作用对失速具有重要影响。以级压比为6.1的Krain叶轮作为研究对象,数值研究在不同流量和叶顶间隙下,激波与叶顶泄漏流的相互作用,包括激波结构、叶顶泄漏涡轨迹和主流/泄漏流交界面位置的变化规律。结果表明,激波与泄漏涡相互作用形成一个低速区,激波被推向上游,呈现凹状,且随着流量减小,凹状幅度增大。叶顶泄漏涡轨迹和主流/叶顶泄漏流交界面(ITLMF)经过激波后发生偏转,随着流量减小,叶顶泄漏涡轨迹逐渐向压力面偏移,且受激波作用的偏转角度减小。ITLMF逐渐向叶片上游移动,在近失速点到达相邻叶片前缘。随着叶顶间隙增大,叶顶泄漏涡轨迹向相邻叶片压力面偏移,且受激波作用的偏转角度减小,ITLMF逐渐向相邻叶片上游移动。ITLMF受激波偏转会导致交界面提前在相邻叶片前缘溢出,对失速预测有重要影响。在原始模型基础上,考虑无量纲子午速度以及无量纲叶顶间隙对进口相对马赫数的影响,建立改进的ITLMF受激波作用偏转角度预测模型,并进行数值验证。结果表明:改进模型预测精度更高,在不同流量下平均误差由46.59%降至5.83%,不同叶顶间隙下平均误差由27.21%降至4.69%。

     

  • 图 1  Krain6叶轮子午流道

    Figure 1.  Meridional flow passage of Krain6 impeller

    图 2  Krain6叶轮计算域网格

    Figure 2.  Computational domain grid Krain6 impeller

    图 3  网格无关性验证

    Figure 3.  Verification of grid independence

    图 4  叶轮性能CFD模拟值和实验值结果对比

    Figure 4.  Comparison of impeller performance between CFD and experimental results

    图 5  Krain6叶轮测量平面划分

    Figure 5.  Measurement plane division of Krain6 impeller

    图 6  相对马赫数分布实验值与计算值对比(plane8截面)

    Figure 6.  Comparison of relative Mach number distribution between experimental and numerical results(plane8 cross-section)

    图 7  相对马赫数分布实验值与计算值对比(plane10截面)

    Figure 7.  Comparison of relative Mach number distribution between experimental and numerical results(plane10 cross-section)

    图 8  叶轮进口叶顶泄漏流相对速度流线分布

    Figure 8.  Relative velocity streamline distribution of tip leakage flow at impeller inlet

    图 9  近失速点处不同叶高相对马赫数分布

    Figure 9.  Relative Mach number contours at different span at near-stall point

    图 10  最高效率点处不同叶高相对马赫数分布

    Figure 10.  Relative Mach number contours at different span at peak efficiency point

    图 11  98%叶高静压分布及截面位置

    Figure 11.  Distribution of static pressure and cross sections at98% span

    图 12  98%叶高不同流量不同截面静压沿周向变化趋势

    Figure 12.  Circumferential variation trend of static pressure with different flows and sections at 98% span

    图 13  不同流量叶顶静压分布及泄漏涡轨迹变化情况

    Figure 13.  Static pressure distribution and TLV trajectory variation near tip with mass flow rate

    图 14  叶尖静压载荷沿流向分布随流量变化情况

    Figure 14.  Static pressure load distribution of the blade tip along the streamwise direction with mass flow rate

    图 15  不同流量叶顶附近静压分布及泄漏涡起始点分布

    Figure 15.  Static pressure distribution and initial point of TLV distribution near tip with mass flow rate

    图 16  进口叶尖相对马赫数随流量变化情况

    Figure 16.  Relative Mach number at inlet blade tip with mass flow rate

    图 17  不同流量叶顶附近熵分布及ITLMF位置变化情况

    Figure 17.  Entropy distribution and ITLMF variation near tip with mass flow rate

    图 18  近失速点叶尖旋转面流速矢量分布(按叶尖速度无量纲化)

    Figure 18.  Vectors distribution of flow velocity at blade tip revolution surface at near-stall point(normalized by rotor tip speed)

    图 19  近失速点进口叶顶区域熵分布

    Figure 19.  Entropy contours of inlet tip area at near-stall point

    图 20  不同间隙叶顶附近静压分布及泄漏涡轨迹变化情况(近失速流量)

    Figure 20.  Static pressure distribution and TLV trajectory variation near the blade tip with tip clearance size (near stall mass flow)

    图 21  不同间隙叶顶附近静压分布及泄漏涡轨迹变化情况($\dot m $=2.8 kg/s)

    Figure 21.  Static pressure distribution and TLV trajectory variation near the blade tip with tip clearance size ($\dot m $=2.8 kg/s)

    图 22  叶尖静压载荷沿流向分布随叶顶间隙变化情况(近失速流量)

    Figure 22.  Static pressure load distribution of the blade tip along the streamwise direction with tip clearance size (near stall mass flow)

    图 23  叶尖静压载荷沿流向分布随叶顶间隙变化情况($\dot m $=2.8 kg/s)

    Figure 23.  Static pressure load distribution of the blade tip along the streamwise direction with tip clearance size ($\dot m $=2.8 kg/s)

    图 24  不同间隙叶顶附近熵分布及ITLMF位置变化情况(近失速流量)

    Figure 24.  Entropy distribution and ITLMF variation near the blade tip with tip clearance size (near stall mass flow)

    图 25  不同间隙叶顶附近熵分布及ITLMF位置变化情况($\dot m $=2.8 kg/s)

    Figure 25.  Entropy distribution and ITLMF variation near the blade tip with tip clearance size ($\dot m $=2.8 kg/s)

    图 26  不同叶顶间隙下级等熵效率性能对比

    Figure 26.  Comparison of stage isentropic efficiency with tip clearance size

    图 27  不同叶顶间隙下级总压比性能对比

    Figure 27.  Comparison of stage pressure ratio with tip clearance size

    图 28  Krain6叶轮不同流量下原始模型结果与数值结果ITLMF偏转角度对比

    Figure 28.  Comparison of ITLMF deflection angle from original model predicted results and Numerical results with mass flow rate of Krain6 impeller

    图 29  近失速点98%叶高截面相对马赫数分布

    Figure 29.  98% span relative Mach number contours at near-stall point

    图 30  不同叶顶间隙近失速点进口叶尖相对马赫数沿周向变化趋势

    Figure 30.  Relative Mach number with circumferential position near inlet blade tip at near-stall point with tip clearance size

    图 31  Krain6叶轮不同流量下修正系数CM的数值结果

    Figure 31.  Correction factor Numerical results with mass flow rate of Krain6 impeller

    图 32  Krain6叶轮不同叶顶间隙下修正系数CM的数值结果($\dot m $=2.8 kg/s)

    Figure 32.  Correction factor Numerical results with tip clearance size of Krain6 impeller ($\dot m $=2.8 kg/s)

    图 33  Krain6叶轮不同流量下原始模型、改进模型结果与数值结果ITLMF偏转角度对比

    Figure 33.  Comparison of ITLMF deflection angle between model predicted and Numerical results with mass flow rate of Krain6 impeller

    图 34  PR9叶轮不同流量下原始模型、改进模型结果与数值结果ITLMF偏转角度对比

    Figure 34.  Comparison of ITLMF deflection angle from original model, modified model and Numerical results with mass flow rate of impeller PR9

    表  1  Krain6叶轮设计参数

    Table  1.   Design parameters of the Krain6 impeller

    设计参数数值
    转速/(r/min)50000
    流量/(kg/s)2.55
    级压比6.1
    叶片数Zf+Zs13+13
    叶顶间隙/mm0.5(LE)-0.3(TE)
    进口叶顶相对马赫数1.3
    等熵效率0.84
    前缘轮毂半径/mm30
    前缘叶尖半径/mm78
    下载: 导出CSV

    表  2  Krain6叶轮近失速流量不同叶顶间隙下原始模型结果与数值结果ITLMF偏转角度对比

    Table  2.   Comparison of ITLMF deflection angle between original model predicted results and CFD results with tip clearance size at near-stall mass flow rate of Krain6 impeller

    叶顶间隙
    c/mm
    原始模型
    δmodel/(°)
    数值模拟
    δCFD/(°)
    0.3 6.46 8.65
    0.5 5.27 7.58
    0.7 4.74 6.39
    下载: 导出CSV

    表  3  Krain6叶轮近失速流量不同叶顶间隙下原始模型、改进模型结果与数值结果ITLMF偏转角度对比

    Table  3.   Comparison of ITLMF deflection angle between model predicted and Numerical results with tip clearance size near stall mass flow rate of Krain6 impeller

    叶顶间隙
    c/mm
    原始模型
    δmodel/(°)
    改进模型
    δ*model/(°)
    数值模拟
    δCFD/(°)
    0.3 6.46 8.77 8.65
    0.5 5.27 7.78 7.58
    0.7 4.74 5.75 6.39
    下载: 导出CSV

    表  4  PR9叶轮设计参数

    Table  4.   Design parameters of impeller PR9

    设计参数 数值
    转速/(r/min) 56000
    设计流量/(kg/s) 2.0
    级压比 9.2
    叶顶间隙/mm 0.3(LE)-0.3(TE)
    前缘轮毂半径/mm 25
    前缘叶尖半径/mm 42
    等熵效率 0.79
    进口叶顶相对马赫数 0.98
    下载: 导出CSV
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  • 收稿日期:  2024-11-20
  • 网络出版日期:  2026-06-01

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