An Improved Wavelet Threshold Denoising Method for Health Monitoring Data: A Case Study of the Hong Kong-Zhuhai-Macao Bridge Immersed Tunnel
Abstract
:Featured Application
Abstract
1. Introduction
2. Improved Wavelet Threshold Denoising Method
2.1. Classical Wavelet Transform Methods
2.2. Basic Wavelet Threshold Denoising Method
2.3. Commonly Used Wavelet Basis for Denoising
- (1)
- Orthogonality: It can make the analysis simple and facilitate the accurate reconstruction of the signal.
- (2)
- Symmetry: The symmetrical wavelet basis makes the signal undistorted, and the running speed of the algorithm can also be improved.
- (3)
- Regularity: It determines the smoothness of the reconstructed signal, which affects the resolution in the frequency domain.
- (4)
- Vanishing moment: The higher the vanishing moment of the wavelet basis, the faster the attenuation at high frequencies. Therefore, the more concentrated the energy of the transformed signal, and the better the frequency domain locality can be maintained.
2.4. Method Improvement via Optimizing Wavelet Parameters
2.4.1. Optimal Wavelet Basis
2.4.2. Threshold Selection Rules
2.4.3. Optimal Decomposition Layers
- (1)
- Calculate the index value of each layer
- (2)
- Normalization of all indexes
- (3)
- Calculate the weight of each index
- (4)
- Calculate the score
3. Health Monitoring Data of the HZMB Immersed Tunnel
3.1. Background of the HZMB Immersed Tunnel
3.2. Monitoring Items
3.3. Description of Sensors and Health Monitoring Data
- (1)
- Ground motion
- (2)
- Strain of elements
- (3)
- Joint deformation
- (4)
- Temperature and humidity
4. Illustrative Example of Proposed Method
4.1. Noise in Health Monitoring Data of the HZMB Immersed Tunnel
4.2. Determination of the Optimal Wavelet Basis
4.3. Determination of the Optimal Wavelet Decomposition Layers
4.4. Denoising Results
5. Conclusions
- (1)
- The quantitative evaluation factor, the Sparse Index (SI), is effective for choosing the optimal wavelet basis for a given separation task, which is validated by the approximate coefficient of the original signal and reconstructed signal after denoising.
- (2)
- The variation coefficient method is suitable for comprehensive evaluation of the denoising results by integrating three indexes, namely the root mean square error (RMSE), signal-to-noise ratio (SNR) and smoothness (SMOT), which avoid the unstable and unreliable evaluation by a single index.
- (3)
- The concrete strain health monitoring data of the HZMB immersed tunnel has obvious noise phenomenon, which may cause problems if it is directly used to analyze the structural state. The application of the proposed wavelet threshold denoising method demonstrates good effect, which proves that the proposed method is reliable and can be applied in the denoising of health monitoring data of critical infrastructure.
Author Contributions
Funding
Institutional Review Board Statement
Informed Consent Statement
Data Availability Statement
Acknowledgments
Conflicts of Interest
References
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Index | Formula | Core Concern | Correlation with the Number of Layers | Correlation with Denoising Effect |
---|---|---|---|---|
RMSE | high frequency detail | positively correlated | negatively correlated | |
SNR | high frequency detail | negatively correlated | positively correlated | |
SMOT | low frequency approximation | negatively correlated | negatively correlated |
Monitoring item | Data | Sensors | Installation Location |
---|---|---|---|
Structural responses | ground motion | 3D accelerometer | |
strain of element | FBG strain sensor | | |
joint deformation | displacement meter | | |
Environmental loads | temperature humidity | thermometer hygrometer | |
Wavelet Basis | June | August | October | December | Average Ranking |
---|---|---|---|---|---|
db4 * | 8001.23 | 8602.58 | 9591.84 | 8503.50 | 15.25 |
db5 | 7999.58 | 8589.13 | 9599.54 | 8495.31 | 14.25 |
db6 | 8018.02 | 8613.19 | 9594.12 | 8466.70 | 16 |
db7 | 8018.29 | 8612.75 | 9578.43 | 8458.29 | 13 |
db8 | 7991.01 | 8588.05 | 9602.97 | 8471.25 | 11.5 |
db9 | 7996.80 | 8603.29 | 9590.40 | 8467.05 | 12 |
sym4 ** | 8005.19 | 8643.32 | 9589.52 | 8512.81 | 17.75 |
sym5 | 8006.20 | 8604.73 | 9608.01 | 8477.20 | 16.75 |
sym6 | 7985.82 | 8617.04 | 9567.02 | 8471.13 | 10.5 |
sym7 | 7989.02 | 8582.14 | 9590.40 | 8496.14 | 10.5 |
sym8 | 7984.43 | 8610.07 | 9569.49 | 8453.37 | 6.75 |
sym9 | 7986.99 | 8597.47 | 9588.57 | 8442.58 | 6 |
sym10 | 7985.72 | 8605.50 | 9567.13 | 8444.88 | 6.25 |
sym11 | 7989.75 | 8573.70 | 9597.81 | 8460.48 | 8.25 |
sym12 | 7984.51 | 8600.23 | 9573.49 | 8453.88 | 5.25 |
sym13 | 7981.59 | 8584.90 | 9609.61 | 8436.08 | 6.25 |
coif3 *** | 7996.46 | 8611.83 | 9586.39 | 8471.45 | 13.25 |
coif4 | 7985.78 | 8607.17 | 9592.58 | 8461.40 | 10.75 |
coif5 | 7982.60 | 8597.93 | 9599.51 | 8464.90 | 8.25 |
coif6 | 7985.44 | 8601.74 | 9605.49 | 8479.89 | 12.25 |
coif7 | 7991.55 | 8601.05 | 9617.08 | 8486.84 | 15 |
coif8 | 7993.86 | 8606.54 | 9627.60 | 8491.81 | 17.25 |
bior1.1 **** | 8312.55 | 8962.69 | 9860.08 | 8920.30 | 24 |
bior1.3 | 8550.51 | 9184.83 | 10,100.92 | 9148.77 | 26.25 |
bior2.2 | 8825.44 | 9446.93 | 10,489.33 | 9285.45 | 29 |
bior2.4 | 8587.86 | 9216.15 | 10,269.83 | 9060.60 | 27 |
bior3.1 | 14,081.81 | 14,898.99 | 16,232.34 | 14,702.62 | 33.75 |
bior3.3 | 11,079.45 | 11,797.47 | 13,029.48 | 11,624.38 | 32 |
rbio1.1 ***** | 8312.55 | 8962.69 | 9860.08 | 8920.30 | 24 |
rbio1.3 | 8167.93 | 8777.54 | 9805.52 | 8679.98 | 23 |
rbio2.2 | 8986.85 | 9700.68 | 10,704.76 | 9607.84 | 30 |
rbio2.4 | 8641.32 | 9304.25 | 10,266.36 | 9186.08 | 27.75 |
rbio3.1 | 13,956.77 | 14,854.77 | 15,890.53 | 14,853.39 | 33.25 |
rbio3.3 | 11,034.62 | 11,733.42 | 12,886.81 | 11,584.53 | 31 |
Decomposition Layers | June | August | October | December |
---|---|---|---|---|
1 layer | 0.5835 | 0.653 | 0.6664 | 0.6664 |
2 layers | 0.2909 | 0.3429 | 0.3544 | 0.3544 |
3 layers | 0.184 | 0.231 | 0.2386 | 0.2386 |
4 layers | 0.152 | 0.1983 | 0.2056 | 0.2056 |
5 layers | 0.1464 | 0.1945 | 0.1999 | 0.1999 |
6 layers | 0.1505 | 0.2032 | 0.2043 | 0.2043 |
7 layers | 0.1795 | 0.2549 | 0.2366 | 0.2366 |
8 layers | 0.2063 | 0.287 | 0.2636 | 0.2636 |
9 layers | 0.2626 | 0.3039 | 0.311 | 0.311 |
10 layers | 0.4165 | 0.347 | 0.3336 | 0.3336 |
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Jiang, X.; Lang, Q.; Jing, Q.; Wang, H.; Chen, J.; Ai, Q. An Improved Wavelet Threshold Denoising Method for Health Monitoring Data: A Case Study of the Hong Kong-Zhuhai-Macao Bridge Immersed Tunnel. Appl. Sci. 2022, 12, 6743. https://doi.org/10.3390/app12136743
Jiang X, Lang Q, Jing Q, Wang H, Chen J, Ai Q. An Improved Wavelet Threshold Denoising Method for Health Monitoring Data: A Case Study of the Hong Kong-Zhuhai-Macao Bridge Immersed Tunnel. Applied Sciences. 2022; 12(13):6743. https://doi.org/10.3390/app12136743
Chicago/Turabian StyleJiang, Xinghong, Qing Lang, Qiang Jing, Hui Wang, Juntao Chen, and Qing Ai. 2022. "An Improved Wavelet Threshold Denoising Method for Health Monitoring Data: A Case Study of the Hong Kong-Zhuhai-Macao Bridge Immersed Tunnel" Applied Sciences 12, no. 13: 6743. https://doi.org/10.3390/app12136743
APA StyleJiang, X., Lang, Q., Jing, Q., Wang, H., Chen, J., & Ai, Q. (2022). An Improved Wavelet Threshold Denoising Method for Health Monitoring Data: A Case Study of the Hong Kong-Zhuhai-Macao Bridge Immersed Tunnel. Applied Sciences, 12(13), 6743. https://doi.org/10.3390/app12136743