Bearability of cross-excitation modes of aero-engine dual-rotor system and its experimental verification
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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。
Abstract:To elucidate the contradictory phenomenon of the cross-excitation mode that the displacement or deformation of the excitation source rotor is very small while that of the excited rotor is absolutely dominant, the orthogonality between the force and the vibration mode is analyzed based on rotor modal analysis method and a dual-rotor model with inter-shaft bearing. A dual-rotor experimental setup was built, and modal experiment, response experiment and long-term resonance experiment were carried out. The experimental results showed that the critical speed error between the experimental results and the calculation results of the dual-rotor experimental setup was up to 3.7%, and the modal shape error was up to 9.5%. The unbalanced response during the acceleration and deceleration process had no peak at the cross-excitation mode. A long-time resonance exceeding 62 minutes was performed under the cross-excitation mode. Even if the maximum amount of applied imbalance was 145% of the coupling mode, the peak response was still less than 25% of the coupling mode. The research results fully prove that the cross-excitation mode is a mode with high acceptability, presenting vey low risk of severe vibration.
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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 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-84 0~ 10000 2 电涡流传感器 IN-085 0~ 10000 8 mV/μm 12 速度传感器 VS-080 15~2000 75 mV/(mm/s) 4 加速度传感器 AS-020 1.5~ 15000 100 mV/g 12 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 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 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 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 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 886 2056 第2阶(“交叉激励”) 1466 3680 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 -
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