Damage monitoring of engine fan blades based on EWT-entropy method
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摘要:
为了从发动机性能数据中寻找风扇叶片外来物损伤航班特征,从而将风扇叶片受外来物损伤的航班区分出来,在机载快速存储记录器(quick access recorder, QAR)数据检测中提出将经验小波分解和信息熵结合的方法。通过对各航班原始振动数据的拟合平滑处理和经验小波分解,提取了分解后各模态的能量熵和,分析了添加汉明(Hanmming)窗函数的多尺度熵,结果表明:拟合后数据的熵值变化更明显,且风扇叶片受外来物损伤航班的能量熵和有10%以上的降低趋势,改进后的多尺度熵有40%以上的增长趋势,均明显异于其他正常航班。证明采用EWT-熵值方法可以较好地对发动机风扇叶片外来物损伤情况进行监控。
Abstract:In order to find the characteristics of the flight damaged by foreign objects on the fan blades from the engine performance data, so as to distinguish the flights damaged by the foreign objects on the fan blades, a method combining empirical wavelet transform and information entropy was proposed in the airborne quick access recorder (QAR)data detection. Through the fitted and smoothed process and empirical wavelet transform of the original vibration data of each flight, the sum of the energy entropy of each intrinsic mode function after decomposition was extracted, and the multi-scale entropy of the added window function was analyzed. The result showed the entropy value of the fitted data changed more obviously, and the sum of the energy entropy of the flight with fan blades damaged by foreign objects had a decreasing trend of more than 10%, and the improved multi-scale entropy had an increasing trend of more than 40%, which was obviously different from other normal flights. It is proved that the EWT-entropy method can better monitor the damage by foreign objects of the engine fan blades.
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表 1 部分FOD损伤描述
Table 1. Part of FOD damage description
飞机编号 损伤发现日期 故障描述 A 2019年
12月18日左发4号叶片距叶尖3 mm位置有一豁口,长度约为4.14 mm,深度为不到1 mm,做记录 B 2020年
1月8日右发3号叶片前缘距叶尖27.4 cm位置有一长度为3 mm、深度为不到1 mm缺口,航后拆下叶片交金工已完成打磨和探伤 C 2019年
8月16日航后检查发现右发12号叶片叶尖有一处缺口,深度为0.79 mm,长度为4.7 mm,手册标准深度不超过1 mm,按手册检查不超标,留作记录 表 2 损伤航班能量熵和变化比例统计
Table 2. Statistics of the sum of energy entropies of damage flight and change ratio
飞机 能量熵和均值/nat 损伤航班能量熵和/nat 降低比例/% A 0.67464 0.581654 13.78 0.235134 65.15 B 0.612414 0.541216 11.63 0.553173 9.67 0.523676 14.49 C 0.235001 0.14828 36.90 0.177419 24.50 0.144154 38.66 0.162222 30.97 表 3 A飞机部分模态MSE与HMSE标准差
Table 3. Standard deviation of A aircraft partial modal MSE and HMSE
内涵模态 标准差/nat MSE HMSE IMF1 0.02936 0.02034 IMF2 0.044658 0.04717 $\vdots $ $\vdots $ $\vdots $ IMF17 0.1491 0.126287 IMF18 0.128497 0.111078 IMF19 0.138515 0.116193 表 4 A飞机20个内涵模态28个航班决定系数均值
Table 4. Average value of determination coefficient of 28 flights for 20 intrinsic mode functions of A aircraft
内涵模态 $ {R^2} $均值/nat 内涵模态 $ {R^2} $均值/nat IMF1 0.8962262 IMF11 0.2035216 IMF2 0.7579664 IMF12 0.3174590 IMF3 0.8224329 IMF13 0.2056715 IMF4 0.8420283 IMF14 0.0511563 IMF5 0.6808552 IMF15 −0.2335838 IMF6 0.5581359 IMF16 −0.13266203 IMF7 0.6555249 IMF17 −0.86031928 IMF8 0.3090201 IMF18 −0.46340345 IMF9 0.3602505 IMF19 −0.59026271 IMF10 0.3678542 IMF20 0.7740957 表 5 B和C飞机部分内涵模态决定系数均值
Table 5. Average value of determination coefficient for the partial intrinsic mode functions of B and C aircraft
飞机 保留模态 $ {R^2} $均值/nat B IMF22 0.6539462 C IMF8 0.7409416 表 6 异常航班的样本熵增长比例
Table 6. Sample entropy growth ratio of abnormal flight
飞机 异常
保留模态异常
尺度因子样本
熵均值/nat异常航班
样本熵/nat增长
比例/%A IMF2 1 0.0271 0.0872 221.74 2 0.0035 0.0056 58.58 3 0.0348 0.1065 206.44 4 0.0518 0.1695 227.38 5 0.0696 0.2405 245.55 6 0.0879 0.3079 250.28 7 0.1070 0.3729 248.50 8 0.1258 0.4125 227.90 9 0.1452 0.4463 207.37 10 0.1648 0.4694 184.83 11 0.1849 0.4850 162.30 12 0.2055 0.5149 150.56 13 0.2261 0.5425 139.94 14 0.2441 0.5417 121.92 15 0.2599 0.5355 106.04 16 0.2762 0.5147 86.35 17 0.2901 0.5558 91.58 18 0.3005 0.4907 63.29 19 0.3085 0.4658 50.98 20 0.3210 0.5173 61.15 B IMF22 3 0.5036 0.8405 66.89 4 0.5021 0.8904 77.33 5 0.5084 0.8096 59.24 6 0.5305 0.8015 51.08 7 0.5667 0.8080 42.57 8 0.5569 0.8057 44.69 9 0.5133 0.8118 58.16 10 0.4368 0.7703 76.35 11 0.3806 0.6728 76.77 12 0.3353 0.7218 115.26 13 0.2858 0.7047 146.57 14 0.2342 0.6081 159.64 15 0.1922 0.5027 161.55 16 0.1472 0.4507 206.18 17 0.1222 0.4596 276.10 18 0.0949 0.3546 273.65 19 0.0655 0.2145 227.48 20 0.0588 0.1959 233.16 C IMF8 13 0.2583 0.3757 45.45 14 0.2347 0.4420 88.32 15 0.2184 0.3697 69.27 16 0.2152 0.4321 100.78 17 0.2069 0.4966 140.01 18 0.2137 0.5028 135.33 19 0.2192 0.5288 141.21 20 0.2323 0.4648 100.06 -
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