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航空发动机双转子系统“交叉激励”模态的“可容度”及试验验证

程驰 廖明夫 雷新亮 石斌 王瑞 况钧耀

程驰, 廖明夫, 雷新亮, 等. 航空发动机双转子系统“交叉激励”模态的“可容度”及试验验证[J]. 航空动力学报, 2026, 41(8):20240782 doi: 10.13224/j.cnki.jasp.20240782
引用本文: 程驰, 廖明夫, 雷新亮, 等. 航空发动机双转子系统“交叉激励”模态的“可容度”及试验验证[J]. 航空动力学报, 2026, 41(8):20240782 doi: 10.13224/j.cnki.jasp.20240782
Cheng Chi, Liao Mingfu, Lei Xinliang, et al. Bearability of cross-excitation modes of aero-engine dual-rotor system and its experimental verification[J]. Journal of Aerospace Power, 2026, 41(8):20240782 doi: 10.13224/j.cnki.jasp.20240782
Citation: Cheng Chi, Liao Mingfu, Lei Xinliang, et al. Bearability of cross-excitation modes of aero-engine dual-rotor system and its experimental verification[J]. Journal of Aerospace Power, 2026, 41(8):20240782 doi: 10.13224/j.cnki.jasp.20240782

航空发动机双转子系统“交叉激励”模态的“可容度”及试验验证

doi: 10.13224/j.cnki.jasp.20240782
基金项目: 国家科技重大专项
详细信息
    作者简介:

    程驰(1999-),男,博士生,主要从事航空发动机转子动力学研究。E-mail:chengchi2023@mail.nwpu.edu.cn

    通讯作者:

    廖明夫(1960-),男,教授,博士,主要从事航空发动机转子动力学和风能工程研究。E-mail:mfliao@nwpu.edu.cn

  • 中图分类号: V235.13

Bearability of cross-excitation modes of aero-engine dual-rotor system and its experimental verification

  • 摘要:

    为剖析航空发动机双转子系统“交叉激励”模态的特性,并评估其“可容度”,以某型发动机带中介轴承双转子相似模型为对象,将高、低压转子分别取为独立的单元体,以作用力和反作用力来替代中介轴承的耦合作用;利用转子模态分析方法,分析作用力与振型的正交性,由此证明了“交叉激励”模态的高“可容度”特性。最后,利用与某型发动机动力学相似的双转子试验器进行了试验验证。开展了模态测试、响应测试,以及“长时间共振”试验。双转子试验器升降速过程中,不平衡响应在“交叉激励”模态处无峰值;在“交叉激励”模态下双转子经历了超过62 min的“长时间共振”,所施加的不平衡量最大为耦合模态的145%,而响应峰值小于耦合模态的25%。本文的理论分析和试验结果表明,“交叉激励”模态为“可容模态”,剧烈振动的风险很低。

     

  • 图 1  双转子模型

    Figure 1.  Dual-rotor model

    图 2  双转子临界转速图谱

    Figure 2.  Critical speed map of dual-rotor

    图 3  低压转子激励的模态振型

    Figure 3.  Mode shapes for low-pressure (LP) rotor excitation

    图 4  高压转子激励的模态振型

    Figure 4.  Mode shapes for high-pressure (HP) rotor excitation

    图 5  低压转子单元体和高压转子的作用力

    Figure 5.  Forces between the low-pressure rotor unit and the high-pressure rotor

    图 6  双转子模拟试验器及其振动测试系统的布置[14]

    Figure 6.  Arrangement of a dual-rotor experimental setup and its vibration testing system[14]

    图 7  振动数据采集系统

    Figure 7.  Vibration data acquisition system

    图 8  集成化测控平台

    Figure 8.  Integrated measurement and control platform

    图 9  双转子系统临界转速测试试验流程

    Figure 9.  Critical speed experiment procedure for dual-rotor system

    图 10  双转子临界转速的实测与设计结果的对比

    Figure 10.  Comparison of experimental and calculated results of critical speed diagram for dual-rotor system

    图 11  低压激励前3阶振型实测与设计结果的对比

    Figure 11.  Comparison of experimental results with calculated results for three order vibration patterns of LP rotor excitation

    图 12  高压激励前4阶振型的实测与设计结果的对比

    Figure 12.  Comparison of experimental results with calculated results for four order vibration patterns of HP rotor excitation

    图 13  双转子系统共同工作线

    Figure 13.  Common working line for dual-rotor system

    图 14  双转子系统的振动响应三维图谱

    Figure 14.  Three-dimensional mapping of the vibration response for dual-rotor system

    图 15  低压激励第1阶和第2阶模态振型

    Figure 15.  Mode shapes of the first and second order under low-pressure excitation

    图 16  在低压激励第1阶和第2阶模态下“长时间共振”试验的转速-时间图

    Figure 16.  Variation of rotor speeds with time during prolonged resonance experiments at the first and second order mode with low-pressure excitation

    图 17  低压激励第1阶和第2阶模态下“长时间共振”的振动幅值随时间的变化(低压转速基频)

    Figure 17.  Variation of measured vibration amplitude with time after prolonged resonance in the first and second order mode of low-pressure excitation (low-pressure rotational speed fundamental frequency)

    图 18  低压激励第1阶和第2阶模态下“长时间共振”的振动幅值随时间的变化(高压转速基频)

    Figure 18.  Variation of measured vibration amplitude with time after prolonged resonance in the first and second order mode of low-pressure excitation (high-pressure rotational speed fundamental frequency)

    图 19  高压激励第1阶和第2阶模态振型

    Figure 19.  Mode shapes of the first and second order under high-pressure excitation

    图 20  在高压激励第1阶和第2阶模态下“长时间共振”试验的转速-时间图

    Figure 20.  Variation of rotor speeds with time during prolonged resonance experiments at the first and second order mode with HP excitation

    图 21  高压激励第1阶和第2阶模态下“长时间共振”的振动幅值随时间的变化(高压转速基频)

    Figure 21.  Variation of measured vibration amplitude with time after prolonged resonance in the first and second order mode of high-pressure excitation (high-pressure rotational speed fundamental frequency)

    图 22  高压激励第1阶和第2阶模态下“长时间共振”的振动幅值随时间的变化(低压转速基频)

    Figure 22.  Variation of measured vibration amplitude with time after prolonged resonance in the first and second order mode of high-pressure excitation (low-pressure rotational speed fundamental frequency)

    表  1  各阶模态的模态可容度评价函数计算结果

    Table  1.   Calculation of the criterion function of mode acceptability for each order of modes

    模态阶次 评价参数
    弹支总应变能
    占比
    模态不平衡
    影响因子
    中介轴承应变能
    评价函数值
    模态可容度
    评价函数值
    低压转子激励第1阶 0.808 0.353 1 0.932
    低压转子激励第2阶
    (“交叉激励”)
    0.982 0.002 1 0.999
    低压转子激励第3阶 0.466 0.247 1 0.868
    高压转子激励第1阶 0.820 0.540 1 0.903
    高压转子激励第2阶
    (“交叉激励”)
    0.540 0.036 1 0.983
    高压转子激励第3阶 0.514 0.560 0 0
    高压转子激励第4阶 0.205 0.289 1 0.770
    下载: 导出CSV

    表  2  传感器参数

    Table  2.   Technical parameters of sensors

    类型型号频响范围/Hz灵敏度数量
    光电传感器P-840~100002
    电涡流传感器IN-0850~100008 mV/μm12
    速度传感器VS-08015~200075 mV/(mm/s)4
    加速度传感器AS-0201.5~15000100 mV/g12
    下载: 导出CSV

    表  3  不平衡试验时高、低压转子不平衡质量及其分布

    Table  3.   Imbalance and its distribution in high and low pressure rotors during unbalance experiment

    不平衡
    质量分布
    试验条件 计算条件
    大小/
    (g·cm )
    相位/
    (°)
    大小/
    (g·cm )
    相位/
    (°)
    风扇盘 4.3 180 5.0 180
    低压涡轮盘 25.7 0 25.0 0
    高压一级压气机盘 5.22 0 5.0 0
    高压涡轮盘 24.78 180 25.0 180
    下载: 导出CSV

    表  4  对转条件下要进行“长时间共振”试验的模态及其设计计算的模态“可容度”

    Table  4.   Modes to be subjected to long-time resonance experiments under counter-rotating conditions and their calculated acceptability

    模态设计的“可容度”
    低压激励第1阶0.932
    低压激励第2阶(“交叉激励”)0.999
    高压激励第1阶0.903
    高压激励第2阶(“交叉激励”)0.983
    下载: 导出CSV

    表  5  低压激励第1阶和第2阶模态对应的高压转速和低压转速

    Table  5.   High and low pressure rotational speed corresponding to first and second order mode for low- pressure excitation (r/min)

    低压激励模态 低压转速 高压转速
    第1阶 1 846 4074
    第2阶(“交叉激励”) 3043 4919
    下载: 导出CSV

    表  6  在低压激励第1阶和第2阶模态下“长时间共振”试验时,低压转子不平衡质量的分布

    Table  6.   Distribution of imbalance of low-pressure rotor during prolonged resonance experiment at first and second order mode of low-pressure excitation

    参数 低压激励模态
    第1阶 第2阶
    总不平衡量/(g·cm ) 52.5 76.2
    风扇盘 大小/(g·cm ) 7.5 12.5
    相位/(°) 0 0
    低压涡轮盘 大小/(g·cm ) 45 63.7
    相位/(°) 180 180
    下载: 导出CSV

    表  7  高压激励第1阶和第2阶模态对应的高压转速和低压转速

    Table  7.   High and low pressure rotational speed corresponding to first and second order mode for high- pressure excitation (r/min)

    低压激励模态低压转速高压转速
    第1阶8862056
    第2阶(“交叉激励”)14663680
    下载: 导出CSV

    表  8  在高压激励第1阶和第2阶模态下“长时间共振”试验时,高压转子不平衡质量的分布

    Table  8.   Distribution of imbalance of high-pressure rotor during prolonged resonance experiment at first and second order mode of high-pressure excitation

    参数 模态阶次
    第1阶 第2阶
    总不平衡量/(g·cm ) 84.4 156.1
    一级压气机盘 大小/(g·cm ) 13.2 49.2
    相位/(°) 0 0
    二级压气机盘 大小/(g·cm ) 17.1 47.0
    相位/(°) 0 0
    三级压气机盘 大小/(g·cm ) 20.6 28.6
    相位/(°) 0 0
    高压涡轮盘 大小/(g·cm ) 33.5 31.3
    相位/(°) 0 0
    下载: 导出CSV
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  • 收稿日期:  2024-11-18
  • 网络出版日期:  2026-05-29

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