A Denoising Method of Ship Radiated Noise Signal Based on Modified CEEMDAN, Dispersion Entropy, and Interval Thresholding
Abstract
:1. Introduction
2. Basic Theory
2.1. CEEMDAN
- Step 1.
- Generate , where is a zero mean unit variance white noise realization;
- Step 2.
- Decompose completely each by EMD getting their modes , where indicates the mode;
- Step 3.
- Assign as the kth mode of x, obtained by averaging the corresponding modes: .
- Step 1.
- For every decompose each by EMD, until its first mode and compute ;
- Step 2.
- At the first stage () compute the first residue ;
- Step 3.
- For every decompose each by EMD and define the second CEEMDAN mode as ;
- Step 4.
- For calculate the kth residue ;
- Step 5.
- For every decompose each by EMD and define the CEEMDAN mode as .
2.2. MCEEMDAN Method
2.2.1. NPE
2.2.2. Steps of MCEEMDAN Method
- Step 1.
- Set , and ;
- Step 2.
- Set , and generate signal group (). Determine the first IMF by EMD: ; then obtain the first residue . Calculate of and judge whether is greater than . If , go to step 5, otherwise do ;
- Step 3.
- Generate signal group (). Determine the kth IMF by EMD: ; then obtain the kth residue ;
- Step 4.
- Calculate the of . Is larger than ?
- Yes, go to step 5, and save 1st to k−1th IMFs as noise-assisted IMFs;
- No, do , go back to step 3 for next IMF;
- Step 5.
- Decompose by EMD to obtain the remaining IMFs.
2.3. DE
- Step 1.
- Mapping of the N elements in the input signal x into c classes. The first part of the mapping applies the normal cumulative distribution function (NCDF) to x in order to obtain a normalized vector y (with values from 0 to 1). Then, y is linearly mapped to a vector z with integers values from 1 to c using the formula , where the rounding can be an increasing or a decreasing to the next digit;
- Step 2.
- Creation of embedding vectors (namely ), where m is the number of embedding dimensions and d the time delay. Each element of the embedding vectors is defined choosing m elements from z at distance d starting from position i (that is, , with i and j ranging from 1 to and from 1 to m respectively). Each embedding vector is mapped to a dispersion pattern , where , ,…, ;
- Step 3.
- Calculation of the probabilities of each of the dispersion patterns (i.e., the number of occurrences of each dispersion pattern out of the number of embedding vectors);
- Step 4.
- Calculation of the normalized dispersion entropy .
2.4. Interval Thresholding
3. Steps of MCEEMDAN-DE-IT
3.1. The Proposed Method
- Step 1.
- The SR-N signal is decomposed into a series of IMFs by MCEEMDAN.
- Step 2.
- Calculate the DE of each IMF;
- Step 3.
- According to the DE value, IMFs are divided into three types: noise IMFs, noise-dominated IMFs, and pure IMFs. If DE is greater than 0.88, the corresponding IMF is determined to be a noise IMF. Then look for the last IMF with DE greater than 0.65, and determine the IMF and the previous IMFs as noise-dominated IMFs. In addition, the remaining IMFs are pure IMFs;
- Step 4.
- Interval threshold denoising is performed on all noise-dominated IMFs;
- Step 5.
- Finally, the noise IMFs are removed, and the pure IMFs and the processed noise-dominated IMFs are reconstructed to obtain the final denoised signal. Therefore, the denoised signal can be expressed as:
3.2. Evaluation Criteria for SR-N Signal Noise Reduction
3.2.1. NI
3.2.2. SdrSampEn
- Step 1.
- Given a time series and model parameters embedding dimension m, and spatial offset δ;
- Step 2.
- Use time series, m, to compute the RP by using the Chebyshev distance;
- Step 3.
- Use offset δ to construct the BLCM of the RP to obtain ;
- Step 4.
- Set , repeat steps 2–3 to obtain ;
- Step 5.
- Finally, .
4. Simulation Signal Analysis
4.1. Performance Analysis of MCEEMDAN
4.2. Comparison of SE, PE, and DE
5. Denoising of Chen’s Chaotic Signal
6. Denoising of Real Ship Radiated Noise Signal
7. Conclusions
- (1)
- MCEEMDAN, the modified signal decomposition method proposed in this paper, combines CEEMDAN and traditional EMD through NPE. It not only inherits the advantages of CEEMDAN, but also reduces the consuming time. MCEEMDAN is suitable for nonlinear and non-stationary signal processing, so we introduce it into the denoising of SR-N signal.
- (2)
- Simulation results show that, compared with SE and PE, DE is robust to noise and computationally fast. Therefore, we use DE to measure the complexity of IMF.
- (3)
- The Chen’s chaotic signals with different SNRs are denoised by four methods. The experimental results show that compared with EMD-DE-IT, EEMD-DE-IT and CEEMD-DE-IT, the proposed method has lower RMSE and higher SNR.
- (4)
- For the real SR-N signal, two kinds of evaluated criteria for denoised effect are introduced (NI, and SdrSampEn). The results show that the proposed method can reduce the high-frequency noise of SR-N signal and has advantages in chaotic attractor topological configuration reversion.
Author Contributions
Funding
Conflicts of Interest
References
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Parameter | EMD | EEMD 1 | CEEMD | CEEMDAN | MCEEMDAN |
---|---|---|---|---|---|
IO | 0.0588 | 0.0794 | 0.0833 | 0.0702 | 0.0048 |
CT/s | 0.3545 | 15.6348 | 13.1243 | 17.5604 | 14.2405 |
REOM 2 |
SE | PE | DE | |
---|---|---|---|
CT/s | 2.7910 | 0.5061 | 0.0683 |
IMF1 | IMF2 | IMF3 | IMF4 | IMF5 | IMF6 |
0.9490 | 0.9917 | 0.9696 | 0.6632 | 0.6518 | 0.6194 |
IMF7 | IMF8 | IMF9 | IMF10 | IMF11 | IMF12 |
0.5816 | 0.5493 | 0.5207 | 0.5019 | 0.4400 | 0.4639 |
EMD-DE-IT | EEMD-DE-IT | CEEMD-DE-IT | The Proposed Method | |
---|---|---|---|---|
SNR/dB | 15.4841 | 18.2918 | 18.5110 | 19.1971 |
RMSE | 1.5641 | 1.1321 | 1.1039 | 1.0201 |
SR-N Signal | Status | NI | SdrSampEn | DE |
---|---|---|---|---|
Ship-I | Before denoising | 0.3130 | 1.1493 | 0.7029 |
After denoising | 0.3065 | 0.6043 | 0.6579 | |
Ship-II | Before denoising | 0.2284 | 1.6801 | 0.7952 |
After denoising | 0.2044 | 0.7490 | 0.6962 | |
Ship-III | Before denoising | 0.3173 | 1.8320 | 0.7881 |
After denoising | 0.2860 | 0.7226 | 0.6753 |
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Li, G.; Yang, Z.; Yang, H. A Denoising Method of Ship Radiated Noise Signal Based on Modified CEEMDAN, Dispersion Entropy, and Interval Thresholding. Electronics 2019, 8, 597. https://doi.org/10.3390/electronics8060597
Li G, Yang Z, Yang H. A Denoising Method of Ship Radiated Noise Signal Based on Modified CEEMDAN, Dispersion Entropy, and Interval Thresholding. Electronics. 2019; 8(6):597. https://doi.org/10.3390/electronics8060597
Chicago/Turabian StyleLi, Guohui, Zhichao Yang, and Hong Yang. 2019. "A Denoising Method of Ship Radiated Noise Signal Based on Modified CEEMDAN, Dispersion Entropy, and Interval Thresholding" Electronics 8, no. 6: 597. https://doi.org/10.3390/electronics8060597
APA StyleLi, G., Yang, Z., & Yang, H. (2019). A Denoising Method of Ship Radiated Noise Signal Based on Modified CEEMDAN, Dispersion Entropy, and Interval Thresholding. Electronics, 8(6), 597. https://doi.org/10.3390/electronics8060597