AMethod Combining Fractal Analysis and Single Channel ICA for Vibration Noise Reduction

Aiming at the problem that real engineering vibration signals are interfered by strong noise, this paper proposes a method combining single channel-independent component analysis (SCICA) and fractal analysis (FD) to reduce the effect of noise on the time-frequency analysis of vibration signals. First, phase space reconstruction is performed on the vibration signal to make the proper input for ICA algorithm. &e original is then decomposed into several component signals. &e fractal dimension of each component signals is calculated to determine whether the signal should be considered noise. Noisy component signals are then processed by wavelet denoising. Finally, the output signal after noise reduction is reconstructed using the filtered “right” component signals. &is paper uses the method to analyze real noisy vibration signal. Experimental results show the effectiveness of the proposed method.


Introduction
e measured vibration signals contain many high-frequency and low-frequency noises because of the test environment. us, the spectral components of the signal are complex. In addition, extracting the envelope of the signal is difficult for the reason of noise interference. Noise causes the inaccurate decomposition of the signal envelope, particularly, when using time-frequency analysis technology. An effective noise reduction method for time-frequency analysis would improve time-frequency resolution and algorithm performance, which are required both for practical applications and theoretical analysis. Wavelet denoising is a vibration signal, Qin et al. used the wavelet denoising method to improving the detection performance of distributed vibration sensor [1], and Xie et al. proposed an improved wavelet denoise method for vibration signal processing [2]. Other methods proposed an improved EMD method for time-frequency feature extraction of telemetry vibration [3]. Li et al. proposed a novel noise reduction technique for underwater acoustic signals based on complete ensemble empirical mode decomposition with adaptive noise, minimum mean square variance criterion, and least mean square adaptive filter [4]. For warship radio noise, Li et al. proposed a novel linear spectrum frequency feature extraction technique for warship radio noise based on complete ensemble empirical mode decomposition with adaptive noise, duffing chaotic oscillator, and weighted-permutation entropy [5]. Wang et al. proposed a new fault diagnosis method based on adaptive spectrum mode extraction [6]. For the data-driven fault diagnosis, Wang et al. proposed a novel technique based on AlexNet Convolutional neural network [7].
ICA is a common blind source separation method but generally requires at least two input signals [8]. In 2001, James and Lowe proposed an algorithm based on a dynamic embedded framework to apply an ICA algorithm to extract multidimensional brain activity signals from single brain electromagnetic signals [9]. Davies and James suggested that SCICA can sometimes be used to separate important components from a time series [10]. And, in [11], the author reviewed the concept and current practice of BSS based on second-order statistics and on higher-order statistics, which is known as ICA [12], and applied ensemble empirical mode decomposition to make use of ICA on single-channel neuromuscular signals [13]. Guerrero has proposed an adaptive noise reduction method that combines ICA and recursive least square (RLS) for processing EEG signals [14]. However, this method filters all source signals after ICA decomposition. In other words, part of the useful signal will be likely filtered out as noise, which is unacceptable for vibration signal processing. If useful information is lost because of filtering, the analysis and identification of vibration signals will be ambiguous.
To solve this problem, this paper proposes a vibration signal noise reduction method based on SCICA and FD. First, the Newton iteration ICA method is performed using real vibration signal based on kurtosis maximization of the vibration signal for blind source separation. Second, the component signal required for filtering is selected using fractal dimensions, different denoising methods are performed on the selected component signals, and finally, the signals are reconstructed. e results show that the proposed algorithm not only greatly suppresses noise but also effectively avoids the loss of useful information.

Methods
Abnormal signal filtering is especially problematic because noise greatly reduces the vibration signals. If the method filters the entire source signal, some information will be lost. To address this problem, this paper uses the signals fractal dimension to constrain the ICA filtering process, avoiding the loss of useful information. As shown in Figure 1, the algorithm is described below: (1) e collected vibration signal is preprocessed using zero drift correction and term trend elimination. Phase space reconstruction of the signal is then performed. (2) Blind source separation is performed on the signal using kurtosis maximization via the Newton iterative ICA algorithm [15]. e source signal component S � [S 1 , S 2 , . . . , S M ] and separating matrix W are then calculated. (3) e grid dimension D i , i � 1, 2, . . . , M, and M of each source signal are calculated. e source signal is screen filtered using the grid dimension. According to the preliminary analysis of many experiments, the grid dimension of source signals containing an abnormal signal is greater than 1.5. As a conservative screening condition, this paper sets the maximum step point of the grid dimension curve close to 1.5. Specific operational procedures: sequence grid dimension D i is in ascending order. e most significant step point of the arrangement curve is the screening conditions. e source signal component S can be divided into one part S f to be filtered and the other part S b to be retained.
(4) Next, wavelet denoising is performed on the filtering source signal S ff .
(5) e filtered source signal S f and S b are combined to produce a recombinant source signal S ′ . e same relative position is maintained during the combination. e separating matrix W is used to reconstruct the phase space signal X � WS ′ . e noise reduction vibration signal is obtained from X. A description of the phase space reduction method may be found elsewhere.

Phase Space Reconstruction.
e phase space reconstruction method is required when using ICA blind source separation for processing the single-channel vector data. In this paper, the chaotic phase space reconstruction method is performed on the signal to extend to multidimensional phase space. us, each aliasing source signal is reopened in a multidimensional space, and the ICA method is used to separate the source signals. In the 1980s, Packard et al. proposed the use of chaotic time series to reconstruct the phase space to reveal the dynamics of the system [16]. e basic idea is that the evolution of any component in the system is related to the change of all interacting components. By the Takens embedding theory for one dimension signal, a phase space equivalent to the original dynamic system can be constructed by determining its embedding dimension and adding time delay. e phase space contains the required information and characteristics of the original signal to obtain enough hidden information in the observation signal. As the dynamic embedding principle, the phase space reconstruction method construct delay vectors by delaying one-dimensional observation signal, and combining these vectors to build a multidimensional phase space can reveal the dynamic system in the chaotic attractor and chaotic time series. In order to obtain enough information content, the reconstructed phase space embedding dimension m should be at least greater than system freedom D, i.e., m ≥ 2 D + 1.
First, determine the embedding dimension m and the time delay τ; for a complex signal x(t), the time delay τ is added to obtain the delay vector at a time t: where t � 1, 2, . . . , N − (m − 1)τ and N is the length of the observed signal. ese delay vectors are combined to form an embedding matrix, which is a multidimensional delay signal: x � (

2)
Without prior information about vibration signals, selecting an embedding dimension is difficult. Instead, a delay time is selected before determining the embedding dimension according to the delay time. Many algorithms may be used to calculate the delay time, including the C-C algorithm [17], G-P algorithm, and mutual information method [18]. e algorithm processes are detailed elsewhere.
is paper compared the performance and computational efficiency and used the mutual information method to obtain the delay time. Finally, using the method proposed by Takens [19], the Cao algorithm [20] was implemented to calculate the embedding dimension.

Newton Iteration ICA Algorithm Based on Kurtosis
Maximization. e phase space reconstruction expended the single-channel signal into multiple channels. us, ICA can be applied. e ICA algorithm is a blind source separation method that uses the assumption of statistical independence of alias components. A separating matrix W can be constructed, and blind source separation can be realized as follows: where X � [x 1 , x 2 , . . . , x N ] T is the aliasing signal vector, A is the mixing matrix, S � [S 1 , S 2 , . . . , S M ] T is the source signal vector, and S � [S 1 , S 2 , . . . , S M ] T is the estimated value of S. e traditional method, which is based on ICA kurtosis and uses the fixed point iterative method to calculate the separating matrix, has many shortcomings, such as low computational efficiency, the possibility that the separating matrix fails to converge, and poor separation effects. Li et al.
proposed an alternative method based on the Newton iteration to calculate the separating matrix [21]. However, the results of the algorithm are unstable when the mean of the source signal is zero. To address these problems, this paper uses Newton iteration ICA by maximizing the kurtosis. e constraint matrix separation operation using Newton iterative algorithm is based on the kurtosis formula. e source signals may be obtained by reducing the Gaussian of the separation results. Simulation results show that this method improves the computational efficiency and separation effects. First, the kurtosis of the signal is defined as follows [22]: Let s � w T x, where x and w is a component of the separating matrix W. e gradient kurt(s) of w is (5) To maximize the kurtosis, the extreme solution is calculated under the constraints E(w T x 2 ) � ‖w‖ � 1 using the Lagrange algorithm as shown below: e iterative formula for w is calculated using the Newton iterative method: After each iteration, the decorrelation extraction and normalization are performed on the linear combination of independent components to prevent these components from converging to the same extreme point, which leads to the instability of the algorithm because of the zero-mean of the source signal. e formulas for this method are shown as follows: . (8) e separating matrix W is calculated by estimating all the components w with the method described above.

Fractal Dimension.
Fractal theory, an active area of signal processing research, is a mathematical tool that quantitatively describes various complex signals in nature. e fractal dimension of the vibration signal may be calculated to measure the complexity and irregularity of the signal. In fractal theory, larger fractal dimensions indicate that the signal is complex. For vibration signal processing, noise often causes the vibration signal components to be complicated, nonlinear, and nonstationary. us, the fractal dimension of the vibration signal is large. Many experimental results show the fractal dimension (grid dimension) of abnormal signals is greater than 1.5. Hence, the source signals with a larger fractal dimension may be filtered out avoiding meaningful information loss. e noise may be suppressed using a wavelet filter on the source signal, which has smaller fractal dimension. e fractal dimension contains the box dimension, correlation dimension, Hausdorff dimension, and grid dimension. For one-dimensional signals, the box dimension is equivalent to the grid dimension, which simplifies the computer processing. For an signal Shock and Vibration channel signal x|x i , i � 1, 2, . . . , N , the grid dimension is defined as where Δt is the sampling interval, M j � [x i+1− x i /Δt], and [x] represents the closest integer that is greater than x. First, the space of discrete signals is divided into a multidimensional grid, and the grid dimension is calculated by counting the grid points. e Euclidean space of discrete signals R N is divided as small as possible into grids with the area of Δ.
Points' count N ΔK of grid space of the signal x|x i , i � 1, 2, . . . , N is calculated. Different areas N ΔK are used to calculate the N ΔK point, yielding a point set x k , y k : e slope of the line formed by the set of points x k , y k is the grid dimension of the signal. e line is not straight, so the least-squares method is often used to fit a line for practical applications. Finally, the grid dimension D may be obtained.

Experiments and Results
is section contains 3 groups of experiments. e first uses general sin wave to show the effectiveness of the SCICA with phase space reconstruction. Two cases are given respective correspondence to the condition with or without noise. e section and third experiments apply the SCICA with FD (SCICA-FD) in noise reduction. Experiment 2 combines SCICA-FD with wavelet denoising, the basic knowledge of wavelet is given, and the experiment result is discussed. Similar to experiment 2, experiment 3 applies smoothing filtering to SCICA-FD to show the proposed method can be applied to different denoising methods.

Validation of SCICA Based on Phase Space Reconstruction
Case 1. Using general sine waves and performing phase space reconstruction-based SCICA to verify the effect, in the absence of noise, signal 1 and signal 2 and their mixed-signal are shown in Figure 2(a). SCICA firstly separates the mixedsignal with time delay calculated as 3 and the embedding dimension 7, which means 7 ICA components are obtained. Because too many signals are obtained by SCICA, principal component analysis (PCA) is applied to reduce the dimension to avoid choosing the signal from the 7 ICA output signals. It can be seen in Figure 2(b) that the three principal components with the largest contribution is added to more than 95%, so PCA is used to reduce the 7 dimension signal matrix to three dimensions. From the result shown in Figure 2(c), it can be seen that the phase space reconstruction-based SCICA can effectively separate the two sine signals from the combined signal. Case 2. Similar to Case 1, signal 1, signal 2, a random noise, and their mix signal are shown in Figure 3(a). e mixed signal is separated by SCICA with time delay which equals to 2 and embedding dimension which equals to 9 which means there is 9 ICA components. Again, PCA is used to reduce the dimension of the ICA output signal matrix. From Figure 3(b), the matrix should be reduced to 4 dimensions. e result is shown in Figure 3(c). It can be seen that compare to that of Case 1 (without noise), the output waveform has some fluctuation, but the signal obtained is still close enough to the original one.

Application to Wavelet
Denoising. From a signal perspective, wavelet denoising is a signal filtering method. Although wavelet denoising can be viewed as a low pass filter, the signal features can be preserved successfully after denoising, so it is better than the traditional low-pass filter.

Necessary Knowledge of Wavelet Denoising.
e model of a nonstationary, noisy, and one-dimensional signal is represented as follows: where f i is the true signal, e i is the noise, the noise property is unknown, and s i is the noisy signal series. To improve the signal-to-noise ratio (SNR) of the signal, it is necessary to reduce the noise. Taking the simplest noise model as an example, e i is considered as Gauss white noise N(0, 1). In the actual acquisition of vibration signal, the useful signal is usually low or some relatively stable signal and noise signal is normally high-frequency signal, and the noise reduction process can be processed according to the following methods. First, decompose the noise signal by wavelet transform, such as the three layers' decomposition, and the decomposition process is shown in Figure 4; the decomposed signals include two parts: approximate signal (CA3) and the detail signal (CD3, CD2, and CD1). e approximate signal represents the decomposed lowfrequency signal. Detail signals stand for high-frequency part. Because the noise belongs to high frequency signals, it is usually included in each detail signal level. In the process, the approximate signal of wavelet transform is reserved, and the detail signal is processed in the form of a threshold value. After the above process, the signal is reconstructed by wavelet transform, thus obtains the denoised signal in which the useful part is well preserved. e noise reduction process of the vibration signal s can be divided into three steps: Step 1 (vibration signal wavelet decomposition): select a wavelet, determine the wavelet decomposition layers N, and then take N layer wavelet decomposition to signal s. Also, the appropriate choice of wavelet base has a significant impact on the noise reduction effect. A suitable wavelet basis can make the signal energy be distributed on a small number of substrates.
Step 2: after the wavelet decomposition, the high frequency coefficient's threshold value is quantized. e high-frequency coefficient of each layer of the first layer to the N layer is selected, and a threshold value is selected to process the soft threshold quantization.
Step 3 (one-dimensional wavelet reconstruction): according to the low-frequency coefficients of the fourth layer of wavelet decomposition and the high-frequency coefficients of the first layer to the N layer, the wavelet reconstruction of the vibration signal is carried out. In the process of noise reduction, the threshold value of the highfrequency coefficient is selected, and the threshold and the soft threshold are given in two forms of Donoho [23]. Usually, the hard threshold denoising will cause the loss of available information, so the engineering signal analysis is mostly based on the soft threshold denoising technique. e method described in this paper is also a soft thresholding.

SCICA-FD with Wavelet Denoising. Using Case
Western Reserve University's bearing data, Figure 5(a) shows the vibration signal in time domain and its spectrum is shown in Figure 5(b). As shown in Figure 5(b), the vibration signal time domain contains large background noise, and the fault information is submerged in the noise.
Using the proposed method, the vibration data is separated by SCICA. e fractal dimension of each separated signal is shown in Figure 6. As mentioned before, this paper chooses signals with fractal dimension close to 1.5, which is number 4 to 13 in Figure 6. en, the same wavelet threshold is applied to the selected signal. e spectrum of the restored signal is shown in Figure 7(b). Performing only the wavelet denoising, the result is shown in Figure 7(a). Comparing to Figure 7(a), Figure 7(a) can tell that the proposed method reduces the noise and reserves the high-frequency part. Some of the high-frequency parts are a little weak.

Application to Smooth
Filtering. Wavelet denoising is applied in experiment 2; as mentioned, wavelet denoising can be considered a lowpass filter but retains more useful frequencies.
e smoothing filter used here is called Savitzky-Golay filter which is proposed in 1964 [24]. Savitzky-Golay filter is a low-pass filter based on polynomial fitting, compared to wavelet denoising, which is a simpler and more straightforward way. is paper shows in this part that our proposed SCICA-FD can be applied with even simpler methods.
e polynomial is used to fit the data. Due to the existence of fitting errors, the sum of squares of the total error is To minimize E, the derivative of E to each coefficient is set to 0, (z E /z a r ) � 0, r � 0, 1, 2, . . . , p, that is, and then, equation (15) can be written as Given the number of point M needed to fit, polynomial order P, and the data x(i), i � M, . . . , 0, . . . , M, to be fitted, the coefficients a 0 , a 1 , . . . , a p can be calculated by equation (17) and thus get the polynomial f i .
In the actual calculation, the best fitting polynomial to center point x(0) can be obtained as long as the coefficient a 0 is obtained, and assume M � 2 and P � 2, and applying equation (17), we obtain and consider a 0 as a filter factor or template: Moving the template on data x(n), central point f 0 can be calculated according to equation (19) and thus achieve fitting of x(n). h(n) is a symmetric FIR filter, which is n � O symmetry, so it has the characteristics of zero phase, and its coefficients sum equals 1, and its frequency characteristic is as follows: e smooth filter used in this paper set is M � 5 and p � 3.

SCICA-FD with Smooth
Filtering. Using the same data, recall that the time domain signal is plotted in Figure 5(a) and its spectrum is plotted in Figure 5(b). Apart from the denoising method, nothing changes, and compare d to experiment 2. at is, the SCICA-FD output is the same, and the fractal dimension of each separated signal is the same as that in Figure 6. e spectrum of the restored signal is shown in Figure 8(b). Applying only smooth filtering on the vibration signal, the filtering result is shown in Figure 8(a). After smooth filtering, the spectrum is similar to that of wavelet denoising as both algorithms have the characteristic of lowpass filter. First, carry out the proposed SCICA-FD than filtering only part of the component signals, and the result is shown in Figure 8(b). Again, both the 1000 Hz and 2000 Hz high frequency are retained and frequency elsewhere is depressed. From Figure 8(b), it is clear that the spectrum of vibration signal using SCICA-FD with smooth filtering has obvious fault shock characteristics at 1000 Hz and 2000 Hz.

Conclusion
e experimental results demonstrate that vibration signal components are complex. e signals exhibit both nonlinear and nonstationary characteristics. e proposed vibration noise reduction method combines the advantages of fractal analysis, blind source separation, and different denoising algorithms. Using the fractal dimension constraint with the SCICA, the denoising process avoids filtering useful information. us, the proposed method can reduce noise while ensuring that useful information is retained. e signal after noise reduction is smoother, and the burr is reduced. Although the amplitude of the noise was significantly attenuated because of the ICA algorithm, this change does not affect the analysis of the frequency domain components because changes in amplitude do not affect the time-frequency distribution. e proposed method effectively reduces noise and may have many theoretical and practical applications. Future work may show that the proposed method may be extended to other areas of research in which noise reduction is required.

Data Availability
e data used to support the findings of this study are available from the corresponding author upon request.

Conflicts of Interest
e authors declare that they have no conflicts of interest.