EEMD修正爆破加速度零漂信号中的最优白噪声系数

王志亮 陈贵豪 黄佑鹏

王志亮, 陈贵豪, 黄佑鹏. EEMD修正爆破加速度零漂信号中的最优白噪声系数[J]. 爆炸与冲击, 2019, 39(8): 084201. doi: 10.11883/bzycj-2019-0154
引用本文: 王志亮, 陈贵豪, 黄佑鹏. EEMD修正爆破加速度零漂信号中的最优白噪声系数[J]. 爆炸与冲击, 2019, 39(8): 084201. doi: 10.11883/bzycj-2019-0154
WANG Zhiliang, CHEN Guihao, HUANG Youpeng. Optimal white noise coefficient in EEMD corrected zero drift signal of blasting acceleration[J]. Explosion And Shock Waves, 2019, 39(8): 084201. doi: 10.11883/bzycj-2019-0154
Citation: WANG Zhiliang, CHEN Guihao, HUANG Youpeng. Optimal white noise coefficient in EEMD corrected zero drift signal of blasting acceleration[J]. Explosion And Shock Waves, 2019, 39(8): 084201. doi: 10.11883/bzycj-2019-0154

EEMD修正爆破加速度零漂信号中的最优白噪声系数

doi: 10.11883/bzycj-2019-0154
基金项目: 国家自然科学基金(51579062,51379147)
详细信息
    作者简介:

    王志亮(1969- ),男,博士,教授,cvewzL@hfut.edu.cn

  • 中图分类号: O384

Optimal white noise coefficient in EEMD corrected zero drift signal of blasting acceleration

  • 摘要: 为了有效降低振动信号误差以提高数据的可信度,先针对花岗岩爆破试验中的加速度零漂信号,使用集合经验模态分解(ensemble empirical mode decomposition,EEMD)与高低频处理相结合的方法进行修正;接着,根据信号冲击响应谱提出表征修正前后频域平均偏差幅度的修正指数;最后,基于频域和时域分别讨论了不同白噪声系数范围内信号的修正效果。分析表明:EEMD方法能够有效地消除爆破加速度信号的零漂现象,但对积分后速度信号的零漂趋势改善有限;随着白噪声系数增大,不同频段上修正指数均不同程度地增大,二者呈现幂指数关系;根据不同频段上的修正指数分析,可以确定不同零漂加速度信号对应的最优白噪声系数范围。本文提出的修正指数可为EEMD方法处理加速度零漂信号时白噪声系数的合理选取提供参考。
  • 图  1  EMD算法流程图

    Figure  1.  Flow chart of EMD algorithm

    图  2  试验与数据采集

    Figure  2.  Test and data collection

    图  3  爆破加速度信号A

    Figure  3.  Blast acceleration signal A

    图  4  EEMD分解信号(k=0.10)

    Figure  4.  Signals decomposed by EEMD method (k=0.10)

    图  5  部分IMF分量频谱图

    Figure  5.  Spectrograms of partial IMF components

    图  6  EEMD修正前后的信号

    Figure  6.  Signals before and after EEMD correction

    图  7  不同白噪声系数下EEMD修正信号的冲击响应谱

    Figure  7.  Shock response spectra of signals modified by EEMD under different white noise coefficients

    图  8  不同白系数噪声下不同频段上的冲击响应谱修正指数

    Figure  8.  Correction indices of shock response spectra on different frequency bands under different white noise coefficients

    图  9  不同白系数噪声下不同频段上的冲击响应谱修正指数

    Figure  9.  Correction indices of shock response spectrum on different frequency bands under different white noise coefficients

    图  10  爆破加速度信号B及其修正信号

    Figure  10.  Blast acceleration signal B and its corrected signal

    图  11  EEMD修正前后速度曲线

    Figure  11.  Velocity curves before and after correcting by EEMD

    图  12  滑动平均法修正后速度曲线

    Figure  12.  Velocity curve modified by sliding average method

    图  13  两种方法处理后信号与原始信号的冲击响应谱

    Figure  13.  Shock response spectra of original signals and processed signals by the two methods

    表  1  不同白噪声系数下IMF分量主频

    Table  1.   Dominant frequencies of IMF components under different white noise coefficients

    IMF分量主频/HzIMF分量主频/Hz
    k=0.05k=0.10k=0.15k=0.20k=0.05k=0.10k=0.15k=0.20
    IMF118 86018 74018 76018 760IMF8440540600640
    IMF218 88018 80018 840 1 800IMF9240280300320
    IMF3 7 500 8 420 8 480 8 500IMF10100200220220
    IMF4 5 100 7 520 7 520 7 520IMF11 40 40 40 40
    IMF5 2 280 3 180 5 160 5 160IMF12 20 20 20 20
    IMF6 1 240 1 360 1 560 2 340IMF13 20 20 20 20
    IMF7 660 740 800 840δ 20 20 20 20
    下载: 导出CSV

    表  2  不同频段修正指数范围

    Table  2.   Ranges of correction index on different frequency bands

    频段/Hz ${\bar D_{\min }}/{\text{%}} $ ${\bar D_{\max }}/{\text{%}} $ 频段/Hz ${\bar D_{\min }}/{\text{%}} $ ${\bar D_{\max }}/{\text{%}} $
    (0, 40] 8.86 86.72 (4 000, 19 000] 0.79 1.88
    (40, 30 000] 1.85 4.34 (19 000, 30 000] 0.37 0.85
    (40, 4 000] 9.99 23.34
    下载: 导出CSV
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出版历程
  • 收稿日期:  2019-04-23
  • 修回日期:  2019-06-03
  • 网络出版日期:  2019-07-25
  • 刊出日期:  2019-08-01

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