Experiment on intermittent rotating instability based on wavelet transform analysis
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摘要:
以一亚声速轴流压气机孤立转子实验台为研究对象,对其叶顶动态压力展开了测量,以探究旋转不稳定性(RI)的时频特征及物理本质。通过功率谱估计,对RI的空间分布和频率特征进行了研究,发现RI的频率特征和空间分布不随叶顶间隙、转速和流量而变化。使用小波变换对RI的时频特征进行了研究,发现RI在时间上并不连续。叶顶间隙的增大会提高RI的发生频率。使用人工模拟信号对RI的时频特征做了模拟,验证了RI只会出现在特定叶片上的假设。叶顶压力分布测量结果显示RI的物理本质是泄漏涡破碎后形成的载荷高低交错的两通道流动结构。
Abstract:A subsonic axial compressor isolated rotor test rig was taken as the research object to explore the time-frequency characteristics and physical nature of rotational instability (RI) through measurement of unsteady pressure at the blade tip region. Using the power spectrum estimation, the spatial distribution and frequency characteristics of RI were studied, indicating that the frequency characteristics and spatial distribution of RI did not change with the blade tip clearance size, rotating speed and mass flow rate. Using wavelet transform to study the time-frequency characteristics of RI, it was found that RI was not continuous in time. The increase of blade tip clearance would increase the occurrence frequency of RI. The time-frequency characteristics of RI were simulated by artificial signals, and the hypothesis that RI would only appear on specific blades was verified. The pressure field on the tip of the blade showed that the physical nature of RI was represented by a two-channel flow structure with alternating high and low loading formed by the tip leakage vortex breakdown.
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表 1 转子叶片主要设计参数
Table 1. Main design specifications of the rotor blade
参数 叶根 叶中 叶顶 半径/mm 91 120 149 弦长/mm 30 30 30 弯角/(°) 53.1 41.2 30.7 安装角/(°) 59.8 48.5 37.2 几何进口角/(°) 29.8 25.1 21.1 几何出口角/(°) 82.9 66.3 51.9 表 2 实验中转速与叶顶间隙设置
Table 2. Rotating speed and clearance size in experiment
序号 叶顶间隙/mm 转速/(r/min) 1 0.3 8130 2 0.3 10765 3 0.5 8130 4 0.5 10765 5 0.7 8130 6 0.7 10765 7 0.9 8130 8 0.9 10765 表 3 人工信号No.3中各叶片通道RI激活率
Table 3. RI activation rate of each blade passage in artificial signal No.3
序号 B 序号 B 序号 B 1 0.7859 11 0.2257 21 0 2 0 12 0 22 0 3 0 13 0.4812 23 0 4 0 14 0 24 0 5 0 15 0.4012 25 0 6 0 16 0.9754 26 0 7 0 17 0 27 0 8 0.5757 18 0 28 0.5417 9 0.6955 19 0 29 0 10 0 20 0 30 0 -
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