An improved higherorder analytical energy operator with adaptive local iterative filtering for early fault diagnosis of bearings
Jinbao Zhang^{1} , Yongqiang Zhao^{2} , Ming Liu^{3} , Lingxian Kong^{4}
^{1, 2, 3, 4}School of Mechatronics Engineering, Harbin Institute of Technology, Harbin, 150001, China
^{2}Corresponding author
Journal of Vibroengineering, Vol. 22, Issue 1, 2020, p. 6782.
https://doi.org/10.21595/jve.2019.20794
Received 12 May 2019; received in revised form 14 August 2019; accepted 16 September 2019; published 15 February 2020
Early fault diagnosis in rolling bearings is crucial to maintenance and safety in industry. To highlight the weak fault features from complex signals combined with multiple interferences and heavy background noise, a novel approach for bearing fault diagnosis based on higherorder analytic energy operator (HOAEO) and adaptive local iterative filtering (ALIF) is put forward. HOAEO has better effect in dealing with heavy noise. However, it is subjected to the limitation of monocomponents. To solve this limitation, ALIF is adopted firstly to decompose the nonlinear, nonstationary signals into multiple monocomponents adaptively. In the next, the resonance frequency band as the optimal intrinsic mode function (IMF) is selected according to the maximum kurtosis. In the following, HOAEO is utilized to highlight weak fault characteristics of the selected IMF. Finally, the early bearing fault is diagnosed by the energy operator spectrum based on fast Fourier transform (FFT). Comparisons in the simulation indicate that the fourth order HOAEO shows the best performance in fault diagnosis compared with Teager energy operator (TEO), analytic energy operator (AEO), the second and the third order HOAEO. The simulated test and experimental results demonstrate that the proposed approach could effectively extract weak fault characteristics from contaminated vibration signals.
 Adaptive local iterative filtering could decompose the nonstationary signals into several monocomponents without mode mixing
 Highorder analytical energy operator could reduce the noise and enhance the transient impacts in signals
 The monocomponent could relieve the limitation of highorder analytical energy operator in envelop demodulation
Keywords: early fault diagnosis, rolling bearing, higherorder analytic energy operator, adaptive local iterative filtering.
1. Introduction
Rolling element bearings are always playing critical roles in rotating machines and often work in harsh environment. Unexpected failures of them may be catastrophic and result in huge economic losses. Hence, it will be significant to accurately detect the existence of faults and diagnose at an early stage. With analysis of the bearing failure mechanism, transients of a defected bearing can be identified according to the interval between two adjacent impulses occurring at a characteristic frequency [13]. Based on the known characteristic frequency by theoretical formulas, fault types of bearings can be identified. But in practice, due to the complex correlation of the internal parts of the mechanical system, as well as the impacts and noise interference in the signal transmission process, the fault signals of the rolling bearing acquired are nonstationary and nonlinear. So a bandpass filter is required firstly for band selection and denoising [4, 5]. Qiu et al. [6] adopted wavelet filter for denoising to detect the weak signature in defected bearings. Nevertheless, the basis function in wavelet transform needs to be prespecified and the parameters of the basis function should be optimized in further. Wang et al. [7] employed binary wavelet packet transform (WPT) to decompose the signals into subbands and select the optimal band by local tangent space alignment combined with the minimum permutation entropy. Lei et al. [8] proposed an improved spectral kurtosis approach based on WPT with the bandpass filter selected in terms of the maximum kurtosis. As well, the basis function in WPT should be set in advance. Hence, the wavelet transform and WPT are not adaptive in signals decomposition.
In the following, adaptive mode decomposition methods are proposed to realize this adaption [9], and the representative is empirical mode decomposition (EMD) proposed by Huang et al. [10]. Then Cheng et al. [11] employed EMD to decompose an amplitude modulationfrequency modulation (AMFM) signal with multicomponents into a sum of IMFs to satisfy the requirement of TEO for the bearing fault diagnosis. However, the noise considerably affects the envelop process of the EMD algorithm, and serious mode mixing will arise. Moreover, EMD should be modified on the stop criterion, end effects as well as intermittency [12]. Aim at these problems, some algorithms are improved referring to EMD such as ensemble EMD [13], empirical wavelet transforms [14], variational mode decomposition (VMD) [15], ALIF [16] and so on. For example, Feng et al. [13] adopted ensemble EMD to decompose signals into monocomponent parts for bearing fault diagnosis based on Teager energy spectrum, and gave an improved energy separation with iterative generalized demodulation [17]. Wei et al. [18] realized signal decomposition via VMD with parameters optimized by the whale optimization algorithm, and performed the envelop demodulation through TEO. In particular, adaptive local iterative filtering method achieves the decomposition with iterative filters generated by the FokkerPlanck (FP) equation and an adaptive filter length selection by data driven. It could inhibit problems existed in EMD to some extent such as mode mixing [19], and has been applied in some fields, like oscillation mode analysis on power grids [20]. An et al. [21] have applied ALIF for envelope spectrum in bearing fault diagnosis, yet the result is not distinct with the envelop spectrum through the Hilbert transform.
As mentioned above in the application of TEO on bearing fault diagnosis [11, 13, 17, 18], TEO proposed by Kaiser [22] could efficiently enhance the transient characteristics of transient fault signals. It is a nonlinear differential energy operator, which is simple to compute and efficient in implementation. Potamianos et al. [23] proposed a smoothed TEO and showed smaller computational complexity and faster adaptation than the Hilbert transform. Fundamental theories concerning TEO are investigated by Maragos et al. [24, 25] with applications on speech analysis. Feng et al. [13] indicated that the Teager energy operator enhanced the spectrum compared with the squared envelope spectrum due to the difference of the constant frequency. Nevertheless, TEO and its modifications are subjected to the limitation of monocomponent and narrow frequency band, and sometimes may be negative. Otherwise, modifications of TEO are also investigated for bearing fault diagnosis, such as the calculus enhanced energy operator [26], the normalized complex Teager energy operator [27], the frequencyweighted energy operator [28], the analytic energy operator [29], and the higher order differential energy operator [2931], etc. Among the modifications, AEO improves the demodulation precision because it gives an analytic formula, but TEO omits two terms and it is just an approximation. In further, the higher order AEO performs better than AEO and TEO on denoising. However, the AEO is limited to the monocomponent as well. Hence, ALIF needs to be employed to decompose the faulty signals into monocomponents for better performance of the HOAEO.
From the above analysis, an approach based on ALIF and HOAEO for early bearing diagnosis is proposed and the paper is organized as follows. ALIF and HOAEO are respectively described in Section 2 and Section 3. Then in Section 4, procedure of the proposed method is illustrated by a simulation signal with heavy noise and interference harmonics. In addition, comparisons among TEO, AEO and HOAEO based on ALIF and EMD are performed. Section 5 presents two practical cases with the proposed method for further verification and the conclusions are finally drawn in Section 6.
2. Adaptive local iterative filtering
Given a nonlinear, nonstationary signal $x\left(t\right)$, the signal can be reconstructed with the sum of several IMFs and the residue:
where ${c}_{i}\left(t\right)$ represents the sifted IMF, $N$ is the number of the IMFs, and $r\left(t\right)$ is the residual. The IMF should satisfy two conditions: (1) the number of extrema and the number of zero crossings should either be equal or differ at most by one; (2) the mean of the upper envelope connecting all the local maxima and the lower envelope connecting all the local minima of the function must be zero at any point. The EMD process of the nonstationary signal consists of an inner loop and an outer loop. The inner loop is utilized to extract IMF components, while the outer loop is employed to determine the number of IMF components and the residual.
In EMD algorithm, the cubic spline interpolation is employed for the upper and the lower envelope functions, which will be susceptible to singularities. Consequently, iterative filtering computes the moving average $\mathrm{\Theta}\left(x\left(t\right)\right)$ of the signal $x\left(t\right)$ by the convolution:
in lieu of the envelop functions. In Eq. (2), ∗ represents the convolution operator, $f\left(t\right)$ constrained with ${\int}_{l}^{l}f\left(\tau \right)d\tau =1$ is a low pass filter and $l$ is the mask length. Afterwards by the sifting process, the first IMF is generated:
where $n$ is the iterative number, ${x}_{n}\left(t\right)={\mathrm{\Theta}}_{1,n1}\left({x}_{n1}\left(t\right)\right)$ and ${x}_{1}\left(t\right)=x\left(t\right)$. Since the number $n$ is impossible to achieve infinite in Eq. (3), so Eq. (4) is adopted as a stop criterion for iterations:
where $\epsilon $ is a prespecified parameter. If $\epsilon $ is large, rough decomposed results may be obtained. However, if $\epsilon $ is too small, the computation will be expensive and noise will be introduced. Finally, $\epsilon $ is determined to set as 0.001 after trials. By repeating the previous iterative process to the residual signal $r\left(t\right)=x\left(t\right){c}_{1}\left(t\right)$, the second IMF is obtained in the following. With the same procedure, all the subsequent IMFs could be produced by:
Finally, if $r\left(t\right)$ does not satisfy the two properties of IMF defined above, then treat it as the residual and stop the iteration.
The ALIF method is improved from the iterative filtering technique, which could adaptively adjust the filter with the FP equation, and adaptively compute the filter length. Consequently, the above Eq. (2) can be rewritten as:
which is subjected to:
where $f\left(t,\tau \right),\tau \in \left[l\left(t\right),l\left(t\right)\right]$ is the filter at time $t$, and $l\left(t\right)$ is the mask length varying with $t$.
3. Highorder analytical energy operator
3.1. Teager energy operator
For continuous time signal $x\left(t\right)$, the TEO could be expressed as:
where $x\text{'}\left(t\right)$ and $x\text{'}\text{'}\left(t\right)$ are the first and the second derivatives of $x\left(t\right)$ with respect to time $t$, respectively. The subscript $T$ represents Teager, and $c$ indicates continuous.
The general expression of the AMFM signal is:
where $a\left(t\right)$ and $\varphi \left(t\right)$ are timevarying amplitude and phase, respectively. Substitute Eq. (9) into Eq. (8), the Teager energy operator is rewritten as:
Set ${\mathrm{\Psi}}_{Tc}\left[a\left(t\right)\right]\approx 0$ and $\varphi \text{'}\text{'}\left(t\right)\approx 0$ based on the assumption that the AMFM signal varies slowly, then the conventional Teager energy operator is obtained [24]:
in which $w\left(t\right)$ is the instantaneous frequency.
For the discretetime signal, the time derivative can be approximately expressed by time difference as:
where subscript $d$ represents discrete. From the difference expression, it is found that only three sequential data points are considered to calculate TEO at each time point, which make TEO easy to carry out and suitable to capture the instantaneous energy of $x\left(t\right)$. However, it is noted that TEO gets good effects only when the instantaneous frequency and the instantaneous amplitude of the monocomponent signal are nearly constant or vary slowly.
3.2. Analytic energy operator
The analytic version of the signal $x\left(t\right)$ is:
where $\widehat{x}\left(t\right)$ is the Hilbert transform of the signal $x\left(t\right)$ and defined as:
Then the analytic energy operator is defined as:
By the comparison between Eq. (11) and Eq. (15), the difference lies in the instantaneous frequency $w\left(t\right)$, which is treated as a constant and has less effect on the enhancement of the energy. In addition, error exists in the demodulation of the TEO because of omitting two approximate terms. Hence, the result by AEO will be more precise than TEO for the demodulation of the monocomponent signal.
3.3. Higherorder analytic energy operator
Higher orders of the AEO are considered to further improve the signaltonoise ratio (SNR) in the presence of strong vibration interferences and its $M$th order continuous AEO is generally expressed as:
with the corresponding discrete expression [29]:
$\left.\frac{{\left(1\right)}^{\left(m1\right)}M!}{\left(Mm+1\right)!}\widehat{x}\left[n+\left(Mm+1\right)\right]x\left(n\right)\right\}.$
The first to the fourth order of the AEO with continuous and discrete types are listed respectively as follows:
${AEO}_{d1}\left[x\left(n\right)\right]=x\left(n+1\right)\widehat{x}\left(n\right)\widehat{x}\left(n+1\right)x\left(n\right),$
${AEO}_{c2}\left[x\left(t\right)\right]={x}^{\left(2\right)}\left(t\right)\widehat{x}\left(t\right){\widehat{x}}^{\left(2\right)}\left(t\right)x\left(t\right),$
${AEO}_{d2}\left[x\left(n\right)\right]=x\left(n+2\right)\widehat{x}\left(n\right)\widehat{x}\left(n+2\right)x\left(n\right)2{AEO}_{d1}\left[x\left(n\right)\right],$
${AEO}_{c3}\left[x\left(t\right)\right]={x}^{\left(3\right)}\left(t\right)\widehat{x}\left(t\right){\widehat{x}}^{\left(3\right)}\left(t\right)x\left(t\right),$
${AEO}_{d3}\left[x\left(n\right)\right]=x\left(n+3\right)\widehat{x}\left(n\right)\widehat{x}\left(n+3\right)x\left(n\right)3{AEO}_{d1}\left[x\left(n\right)\right]3{AEO}_{d2}\left[x\left(n\right)\right],$
${AEO}_{c4}\left[x\left(t\right)\right]={x}^{\left(4\right)}\left(t\right)\widehat{x}\left(t\right){\widehat{x}}^{\left(4\right)}\left(t\right)x\left(t\right),$
${AEO}_{d4}\left[x\left(n\right)\right]=x\left(n+4\right)\widehat{x}\left(n\right)\widehat{x}\left(n+4\right)x\left(n\right)4{AEO}_{d1}\left[x\left(n\right)\right]$
$6{AEO}_{d2}\left[x\left(n\right)\right]4{AEO}_{d3}\left[x\left(n\right)\right].$
As the AEO is based on differentiation, the derivation operators in higher orders will decrease the effect of vibration interferences but increase noise level meanwhile. Therefore, multiple HOAEOs are employed jointly as Eq. (19):
to deal with the noise problem such that an offset between the positive and negative noise values could be achieved to a certain degree. For example, when $J=4$, the combined HOAEO is expressed as:
$=\frac{1}{4}\left\{{AEO}_{d4}\left[x\left(n\right)\right]+5{AEO}_{d3}\left[x\left(n\right)\right]+10{AEO}_{d2}\left[x\left(n\right)\right]+10{AEO}_{d1}\left[x\left(n\right)\right]\right\}.$
In addition, the AEO in every order should be normalized with Eq. (21) for balance:
4. The proposed method with a simulation illustration
4.1. The proposed method
A framework based on ALIF and HOAEO has been established for the early fault diagnosis of rolling bearings, and the steps are as follows:
(1) The faulty signals are collected and adaptive local iterative filtering is employed to decompose the faulty signals into a sum of IMFs.
(2) The optimal IMF is selected based on the maximum kurtosis with Eq. (22):
Fig. 1. Flowchart of bearing early fault diagnosis with HOAEO improved by ALIF
(3) Analytic energy operators from order 1 to $J$ are performed on the optimal IMF to enhance transient impulses, and in the following the multiple HOAEO is computed with Eq. (19) and normalized with Eq. (21).
(4) Fast Fourier transform is utilized to the HOAEO of the optimal IMF to obtain the higherorder analytical energy spectrum.
(5) The bearing fault is finally identified by the comparison between the prominent frequency in the higherorder analytical energy spectrum and the theoretic fault characteristic frequency of the faulty bearing.
The flowchart of the proposed approach is demonstrated in Fig. 1.
4.2. Simulation illustration
To verify the proposed approach in extracting the transient characteristics of the signal, a simulation test is performed. Because periodical impulses in the vibration signal of a defected bearing decay in the exponential type, the simulation signal with interference harmonics can be expressed by the following formula:
$+\sum _{k=1}^{K}{L}_{k}\mathrm{sin}\left[{\omega}_{k}\frac{\left(nr{f}_{s}/{f}_{m}\right)}{{f}_{s}}\right],$
where $A$ is the amplitude of the impulseinduced vibration, $\xi $ is the damping characteristic factor, ${\omega}_{r}$ is the excited resonance angular frequency, ${f}_{m}$ is the fault characteristic frequency, ${f}_{s}$ is the sampling frequency, and $\delta \left(\bullet \right)$ is the Dirac function. In this simulation, parameters are set as: $A=$ 1.5, $\xi =$ 0.1, ${f}_{m}=$ 125 Hz, ${f}_{s}=$ 20000 Hz, ${\omega}_{r}=$ 4000$\pi $ rad/s. The interference harmonics are added with ${L}_{1}=$ 0.2, ${\omega}_{1}=$ 426$\pi $ rad/s and ${L}_{2}=$ 0.1, ${\omega}_{2}=$ 1230$\pi $ rad/s, respectively. The noisecontaminated signal is obtained by adding a Gaussian white noise with the SNR of –13 dB. A total of 20,000 samples are considered for the impulsive signal simulation as shown in Fig. 2 with the corresponding frequency spectrum by FFT.
Fig. 2. The stimulated fault signals with periodic impulses and the corresponding frequency spectrum
TEO, AEO and the corresponding 2, 3, 4HOAEO of the simulation signal are respectively shown in Fig. 3, as well as energy operator spectra of TEO, AEO and the 2, 3, 4HOAEO. From the comparison from Fig. 3(a) to Fig. 3(j), it can be seen that the operators are gradually away from the zero, namely, the negative limitation. In addition, fault characteristic frequency are submerged in the spectrum of the TEO in Fig. 3(b), hence it fails to diagnosis the fault. From the comparison of AEO and the corresponding 2, 3, 4HOAEO in Fig. 3(c) to Fig. 3(j), the fault characteristic frequency and its multiples are gradually distinct from AEO to the 4HOAEO. In addition, interference harmonics with 213 Hz and 615 Hz are removed. From the simulation analysis in [29], the fourth order AEO will be a better, hence the 4HOAEO is adopted in this paper for investigation of early bearing fault diagnosis. Nevertheless, the result of 4HOAEO is still not explicit due to the heavy noise. Hence, a preprocess with ALIF is introduced for lowpass filtering, and a comparison with EMD is performed. The convergence threshold $\epsilon $ in ALIF is set as 0.001, and the convergence criterion of EMD is referred to [32].
The first ten IMFs respectively with ALIF and EMD, with the corresponding frequency spectrum are shown in Fig. 4 and Fig. 5. Obviously, ALIF could get narrower frequency bands than EMD, which alleviate the mode mixing and will be more suitable for the 4HOAEO. The optimal IMF is obtained with the maximum kurtosis in Fig. 6. Based on the criteria, the fourth IMF in ALIF and the third IMF in EMD are selected. The optimal IMF by ALIF extracts more harmonic features in frequency domain than the one by EMD as shown in Fig. 7, meanwhile interference harmonics with 213 Hz and 615 Hz are efficiently separated by both ALIF and EMD, then type of the fault can be correctly identified.
Fig. 3. Energy operators of the simulation signals and the corresponding frequency spectra
a) TEO of the simulation signal
b) Frequency spectrum of TEO
c) AEO of the simulation signal
d) Frequency spectrum of AEO
e) 2HOAEO of the simulation signal
f) Frequency spectrum of 2HOAEO
g) 3HOAEO of the simulation signal
h) Frequency spectrum of 3HOAEO
i) 4HOAEO of the simulation signal
j) Frequency spectrum of 4HOAEO
5. Experimental verification
To further investigate effectiveness and feasibility of the proposed approach for weak fault transient extraction, two experimental cases respectively with artificially seeded damage and runtofailure are considered in this section.
Fig. 4. IMFs by ALIF and the corresponding frequency spectra
Fig. 5. IMFs by EMD and the corresponding frequency spectra
Fig. 6. Kurtosis of IMFs with ALIF and EMD
Fig. 7. 4HOAEO with the optimal IMFs and the fault characteristic frequency spectra with ALIF and EMD
a) 4HOAEO of the fourth IMF in ALIF
b) Frequency spectrum of the 4HOAEO with ALIF
c) 4HOAEO of the third IMF in EMD
d) Frequency spectrum of the 4HOAEO with EMD
5.1. Artificially seeded damage bearing with an inner race fault
The bearing data are downloaded from Bearing Data Centre of the Case Western Reserve University [33]. In this part, the drive end bearing with an inner race fault is investigated at speed of 1797 rpm. Since diameter of the fault in the inner race is 0.007 inch, this case can be treated as a slight fault. The fault characteristic frequency in theory can be calculated by Eq. (24) and Eq. (25).
Ball pass frequency on inner race (BPFI):
Ball pass frequency on outer race (BPFO):
where $d$ is the diameter of the rolling element, $D$ is the pitch diameter, $\alpha $ is the contact angle, $z$ is the number of rolling elements and ${f}_{r}$ the shaft speed.
Table 1. Structural parameters of the drive end bearing and the characteristic frequency
$d$  $D$  $z$  $\alpha $  ${f}_{r}$  ${f}_{I}$ 
7.94 mm  39.04 mm  9  0  29.95 Hz  162.19 Hz 
The bearing type is 62052RS JEM SKF and its structural parameters with the corresponding characteristic frequency by Eq. (24) are listed in Table 1. The signal with 20000 points is shown in Fig. 8 with the sampling rate 12 kHz. Obviously, there is no fault characteristic frequency band in the spectrum. The third IMF in ALIF and the second one in EMD are respectively selected as the optimal IMFs according to the maximum kurtosis in Fig. 9. The selected IMF and the corresponding frequency spectra are shown in Fig. 10. Compared with the band in Fig. 10(d), a narrower frequency band with less noise interference is obtained in Fig. 10(b), and the interval frequency between two impulses are obvious. Hence the frequency band containing fault information can be extracted efficiently by ALIF compared with EMD. In the following, based on the 4HOAEO combined with the selected IMF by ALIF, the fault characteristic frequency with its multiples can be identified evidently in Fig. 11(b), but EMD in Fig. 11(d) fails to clearly show the fault characteristic frequencies due to the interference with heavy noise and harmonic waves.
Fig. 8. The stimulated fault signals and the corresponding frequency spectrum
Fig. 9. Kurtosis of IMFs with ALIF and EMD
Fig. 10. The optimal IMFs and the corresponding frequency spectra with ALIF and EMD
a) The third IMF in ALIF
b) Frequency spectrum of the third IMF in ALIF
c) The second IMF in EMD
d) Frequency spectrum of the second IMF in EMD
Fig. 11. 4HOAEO of the optimal IMFs and the fault characteristic frequency spectra with ALIF and EMD
a) 4HOAEO of the third IMF in ALIF
b) Frequency spectrum of the 4HOAEO with ALIF
c) 4HOAEO of the second IMF in EMD
d) Frequency spectrum of the 4HOAEO with EMDs
5.2. Runtofailure bearing with an outer race fault
The data are from Intelligent Maintenance System in University of Cincinnati. As shown in Fig. 12, bearing test rig comprises four bearings that are installed on one shaft. The rotation speed of shaft is controlled at 2000 rpm and a radial load of 6000 lb is placed on the shaft by a spring mechanism. The data length in the save file is 20,480 points with sampling rate 20 kHz. Rexnord ZA115 double row bearings are used in the test with geometry parameters listed in Table 2. The fault characteristic frequency of the outer race is computed with Eq. (25). Details of the experiment could refer to [6].
Table 2. Structural parameters of bearing Rexnord ZA2115 and the characteristic frequency
$d$  $D$  $z$  $\alpha $  ${f}_{r}$  ${f}_{O}$ 
8.4 mm  71.5 mm  16  15.17°  33.3 Hz  236.4 Hz 
The bearing with outer race fault in the second group is selected for investigation. KolmogorovSmirnov (KS) test statistic [34] is employed for monitoring the degradation path of the bearing in Fig. 13. Based on the degradation path, the faulty signal at an early time point 5400 min is selected for study. The original signal at 5400 min with its corresponding frequency spectrum are shown in Fig. 14. The first IMF in ALIF as well as in EMD is selected according to the maximum kurtosis in Fig. 15. Though the third IMF in the EMD kurtosis is larger than the first one, it fails to diagnosis the fault. The reason may be that it is a false IMF produced by EMD. The selected IMFs and the corresponding frequency spectra are shown in Fig. 16. The interference harmonic with frequency 985.2 Hz has been separated. Both fault characteristic frequency bands are obvious, but the noise in the low frequency domain of the band with ALIF is nearly removed compared with EMD, which means the influence of the noise will be slight for the fault characteristic frequency that are in the low frequency domain as well. The comparison between Fig. 17(b) and Fig. 17(d) shows the better capability of ALIF in enhancement of the fault characteristic frequency.
Fig. 12. Illustration of bearing test rig with sensor placement
Fig. 13. Bearing degradation path with KS test statistic
Fig. 14. The stimulated fault signals and the corresponding frequency spectrum
Fig. 15. Kurtosis of IMFs with ALIF and EMD
Fig. 16. The optimal IMFs and the corresponding frequency spectra with ALIF and EMD
a) The first IMF in ALIF
b) Frequency spectrum of the first IMF in ALIF
c) The first IMF in EMD
d) Frequency spectrum of the first IMF in EMD
Fig. 17. 4HOAEO of the optimal IMFs and the fault characteristic frequency spectra with ALIF and EMD
a) 4HOAEO of the first IMF in ALIF
b) Frequency spectrum of the 4HOAEO with ALIF
c) 4HOAEO of the first IMF in EMD
d) Frequency spectrum of the 4HOAEO with EMD
6. Conclusions
In this paper, an improved HOAEO based on ALIF is proposed for the early fault diagnosis in rolling element bearings. The approach could deal with nonstationary signals mixed with heavy noise in the operation of the fault bearing. The Teager energy operator could highlight the transient impulses in vibration signals of the faulty bearing. To more accurately extract the fault information, analytical energy operator with its high orders are developed. According to the comparison among TEO, AEO and 2, 3 4HOAEO in the simulation, the 4HOAEO is superior to the others in dealing with interferences and heavy noise.
To overcome the limitation of monocomponent in energy operators and improve the diagnosis result, ALIF is utilized to decompose the nonlinear, nonstationary signals into multiple monocomponents, and the resonance frequency band as the optimal IMF is selected with the maximum kurtosis. Then 4HOAEO is employed to enhance the transient impulses in the optimal IMF and the corresponding spectrum is obtained with FFT. The effectiveness of the proposed approach in the early fault diagnosis has been verified with the simulation study and two practical applications. Besides, ALIF outperforms EMD in terms of denoising and elimination of mode mixing.
Since the proposed approach could perform well in experimental study considering heavy noise, then further studies could be extended to other mechanical parts like gears and practical applications. In addition, the bandfilter is selected with the criteria of the maximum kurtosis, hence the other bands which contains fault information may be overlooked. Therefore, reconstruction of signals should be considered.
Acknowledgements
This work was supported by the National Natural Science Foundation of China (Grant No. 51505100). The authors would like to thank the editors and the anonymous reviewers for their valuable suggestions which have greatly improved the paper.
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