A Two-dimensional Time-frequency Multi-scale Entropy Method for Rolling Bearing Fault Diagnosis
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摘要: 多尺度熵是一种有效表征一维振动信号复杂性和不规则程度的非线性动力学方法,但其只考虑了信号的时域复杂性,而忽略了频域信息。为了综合利用振动信号时频域信息和量度时频分布的复杂性特征,将二维多尺度熵引入到滚动轴承的故障诊断中,提出了一种基于二维时频多尺度熵和萤火虫算法优化支持向量机的滚动轴承故障诊断方法。首先,采用连续小波变换将一维时间序列转换为时频图像;其次,计算时频图像的二维多尺度熵值;再次,将得到的二维多尺度熵值输入到萤火虫优化的支持向量机中进行分类和预测;最后,通过滚动轴承试验数据分析验证所提方法的有效性。结果表明:论文所提方法能够准确地识别滚动轴承的故障类型和故障程度。
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关键词:
- 二维时频多尺度熵 /
- 时频分布 /
- 滚动轴承 /
- 萤火虫优化支持向量机 /
- 故障诊断
Abstract: Multi-scale entropy is an effective nonlinear dynamic method to characterize the complexity and irregularity of one-dimensional vibration signal, but it only considers the time-domain complexity of the signal and ignores the frequency-domain information. For comprehensive utilization of the vibration signal frequency domain information and measure of the complexity of the time-frequency distribution characteristics, the two-dimensional multi-scale entropy is introduced into the fault diagnosis of rolling bearings, and a new rolling bearing fault diagnosis method based on two-dimensional time-frequency multi-scale entropy (TFMSE2D) and firefly algorithm optimization support vector machine is proposed. Firstly, a one-dimensional time series is transformed into a time-frequency image by continuous wavelet transform. Secondly, the TFMSE2D of time-frequency image is calculated. Then, the TFMSE2D is input into the firefly optimized support vector machine for classification and prediction. Finally, through the rolling bearing experiment data verify the validity of the proposed method. The results show that the proposed method can accurately identify roller bearing fault type and fault degree. -
表 1 不同方法的参数及识别率
Table 1. Parameters and recognition rate of different methods
方法 参数设置 最优参数 识别率/% TFMSE2D m=2
r=0.25c=34.3589
g=0.9373100 MSE1D m=2
r=0.25c=74.1677
g=18.7573100 MPE1D m=2
λ=1c=29.0371
g=31.6586100 MFE1D m=2
r=0.15
n=2c=28.5010
g=6.9890100 表 2 不同方法的参数及识别率
Table 2. Parameters and recognition rates of different methods
方法 参数设置 最优参数 识别率/% TFMSE2D m=2
r=0.25c=26.3190
g=1.0245100 MSE1D m=2
r=0.25c=46.9301
g=10.575497.619 MPE1D m=2
λ=1c=11.2882
g=60.198395.2381 MFE1D m=2
r=0.15
n=2c=19.7435
g=2.566498.4172 -
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