Parameter Optimization Process
In order to comprehensively compare the decomposition effects of the four optimized VMD methods and the traditional empirical parameter VMD, this paper compares and analyzes the three dimensions of fitness curve, time–frequency decomposition effect and eight performance indicators. The eight performance indicators are as follows: the optimal mode number, optimized penalty factor, false mode number, over-decomposition score, under-decomposition score, under-decomposition proportion, residual energy proportion, and computation time. Among them, over-decomposition and under-decomposition are quantitatively evaluated by an independent deduction system. All modal rationality judgments are carried out after eliminating false modes, so as to avoid the interference of meaningless components on the evaluation results.
Taking the number of iterations as the abscissa and the global optimal fitness value of the population as the ordinate, the fitness curves of each optimization algorithm are drawn. The faster the curve decreases, the higher the optimization efficiency of the algorithm is. The lower the fitness value after convergence, the better the decomposition quality corresponding to the parameter combination searched by the algorithm.
- 2.
Residual energy ratio
After VMD decomposition, the residual signal that is not captured by each mode is
The residual energy ratio is defined as
The smaller the ηr is, the more complete the acquisition of the original signal energy by the modal component is, and the higher the decomposition fidelity is.
- 3.
The number of optimal modes and the number of false modes
The optimal mode number Kopt is the final decomposition order of each method. Combined with the physical composition of the bucket runner signal, it can be preliminarily judged whether the mode division is reasonable.
Among the IMF components obtained by decomposition, some low-energy components have no clear physical meaning, and most of them are redundant components or noise generated by over-decomposition. In this paper, the proportion of component energy is used as the main criterion of false mode, supplemented by a frequency-domain spectrum peak test. The specific rules are as follows.
The energy ratio of the
kth IMF component is defined as
Main criterion: If
ηk < 0.3%, it is preliminarily judged as a false modal candidate. The selection of the threshold is based on the energy distribution of each redundant component after multiple sets of VMD over-decomposition experiments on the bucket runner signal. The upper-bound empirical value of the redundant component energy is 0.3%, and the components below this threshold have no identifiable physical characteristics in the time domain and frequency domain. The empirical validation of this threshold using the constructed signal with the known ground truth is presented in
Section 3.1.5.
Auxiliary criterion: Further check the spectrum of the candidate components that meet the main criterion. If there is no obvious narrowband spectral peak in the frequency domain, it is confirmed as a false mode.
The total number of false modes is
Kspurious, and the number of effective modes after removal is
- 4.
Evaluation of over-decomposition degree
Over-decomposition refers to the phenomenon where the number of modes is too large, and the same physical component is divided into multiple spectral adjacent modes. In this paper, the over-decomposition is determined by the modal separation index, which combines the center frequency difference of adjacent modes with the respective 3 dB bandwidth to quantify the spectral overlap.
- 5.
Calculation of 3 dB bandwidth
For each IMF component, the spectral peak
Amax and its corresponding frequency
fp are located in the frequency domain, and the difference between the left and right frequency points at the peak drop of 3 dB (i.e., the amplitude drop to
Amax/√2) is used as the 3 dB bandwidth:
where
fright and
fleft are the frequencies at which the left and right sides of the spectrum peak are lower than the half-power point for the first time, respectively, and are accurately calculated by linear interpolation.
- 6.
Modal separation calculation
Firstly, the spectrum analysis of the original signal is performed, and the dominant frequency fpeak corresponding to the maximum amplitude of the spectrum is extracted to set the percentage threshold λ1. λ1 times the dominant frequency is used as the critical interval for the over-decomposition determination. According to the pre-processing experimental results, this paper takes λ1 = 0.25 (i.e., 25% of the dominant frequency).
The effective IMFs after eliminating the spurious modes are sorted according to the center frequency from small to large, and the relative frequency separation degree of any
ith and
jth modes is calculated only within the effective mode, which does not involve the comparison with the residual or out-of-band components:
where
fi and
fj are the central frequencies of the two modes, respectively.
If sepij ≥ λ1∙fpeak, it shows that the frequency interval between the two modes is sufficient, and there is no over-decomposition; if sepij ≤ λ1∙fpeak, the two modal frequencies are close to each other, which is determined to be an over-decomposition event.
- 7.
Over-decomposition quantitative score
The deduction system is adopted: the initial score is
Rover, 1 point is deducted for each over-decomposition event, and the final score is recorded as
Sover:
where
Nover is the number of modal pairs satisfying sep
ij ≤
λ1∙
fpeak,
Rover is a positive integer, and 10 is taken in this paper. The higher
Sover is, the lighter the degree of over-decomposition is.
- 8.
Evaluation of under-decomposition degree
Under-decomposition refers to the phenomenon where the number of modes is too small and multiple independent physical components are mixed in the same mode. In this paper, the forced quadratic decomposition method is used to determine the under-decomposition. The method is as follows.
For each valid IMF component, the second VMD decomposition is enforced, and the number of sub-modes
K2 = 2 is fixed. The penalty factor
α2 of the second decomposition is 1.2 times the optimal value
αopt of the first decomposition. The sensitivity analysis and empirical justification for this multiplier are provided in
Section 3.1.6.
The remaining control parameters follow the setting of one decomposition to ensure the consistency of the decomposition bandwidth constraint and the reproducibility of the experiment.
The percentage threshold λ2 is set, and λ2 times the maximum amplitude value A’max of the original IMF spectrum is taken as the amplitude determination threshold. According to the results of preprocessing experiments, this paper takes λ2 = 0.35 (i.e., 35% of the spectral peak), which can effectively distinguish the real physical components from the decomposed noise. If the maximum amplitude of the two sub-mode spectra of the secondary decomposition is greater than λ2∙A’max, it indicates that the original mode still contains two separable independent components, and it is determined that the mode has under-decomposition.
The deduction system is adopted: the initial score is
Runder, 1 point is deducted for each under-decomposition event, and the final score is recorded as
Sunder:
where
Nunder is the number of under-decomposed modes,
Runder is a positive integer, and 10 is taken in this paper. The higher the
Sunder, the lighter the degree of under-decomposition.
At the same time, the proportion of under-decomposition is defined as
This index quantifies the proportion of under-decomposition under each method.
Sover and
Sunder are independent of each other, and the rationality of modal division is evaluated from the two opposite dimensions of ‘excessive separation’ and ‘insufficient separation’, respectively, which jointly reflect the matching degree between parameter selection and signal characteristics. The empirical validation of this scoring system using the constructed signal is presented in
Section 3.1.7.