CN112099100A - Magnetic resonance sounding signal envelope extraction method based on adaptive local iterative filtering - Google Patents
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Abstract
The invention belongs to the field of magnetic resonance sounding signal processing, in particular to a magnetic resonance sounding signal envelope extraction method based on self-adaptive local iterative filtering, which directly converts an MRS signal into an envelope signal f (t) by utilizing Hilbert transform and spectrum shift; determining a decomposition order of the envelope signal and a mask coefficient selected when a filtering interval is calculated by adopting a traversal mode for the envelope signal, respectively adopting an ALIF algorithm to extract IMF components through an inner loop and extract an effective MRS signal envelope through an outer loop to finish an extraction process for a real part and an imaginary part of the envelope signal f (t) according to the decomposition order and the mask coefficient, and extracting the effective MRS signal envelope through a margin combination mode. The problem of modal aliasing existing in EMD can be effectively avoided.
Description
Technical Field
The invention belongs to the field of Magnetic Resonance Sounding (MRS) signal processing, and particularly relates to a Magnetic Resonance Sounding signal envelope extraction method based on adaptive local iterative filtering.
Background
The surface nuclear Magnetic Resonance (MRS) is an advanced method capable of quantitatively determining the storage state of groundwater in the world at present because it directly acts on hydrogen protons in groundwater. Compared with other geophysical exploration methods, the MRS method can provide hydrogeological information such as the content and position of underground water and the porosity of a water storage layer medium without drilling. Therefore, in recent years, the method is widely applied to the aspects of underground water detection, evaluation, monitoring and early warning of hidden danger of geological disasters and the like. The method excites hydrogen protons in underground water through an artificially generated alternating electromagnetic field, and the excited hydrogen protons generate energy level transition. When the artificial field is removed, the acquisition system receives MRS signals generated when the hydrogen protons release energy to return, and detection of underground water is achieved. The general expression for a full-wave nuclear magnetic resonance signal is:
the equation contains four key parameters of the MRS signal: e0、
fL、
Respectively, an initial amplitude of the signal related to the water content of the formation, a relaxation time related to the porosity of the aquifer (the relaxation time of free water ranges from 30ms to 1000ms), larmor frequencies with different values for different zones, and an initial phase related to the conductivity of the aquifer.
Although the MRS method has the above advantages, in practical application, because the method uses a natural geomagnetic field as a background excitation field, shielding measures cannot be taken, so random noise, power frequency harmonic interference and accidental spike noise in the environment all affect a nano-volt level weak MRS signal, and effective extraction of the MRS signal is difficult to achieve.
In view of the above problems, a great deal of research work has been conducted by experts and scholars at home and abroad. The classical process flow comprises the following: firstly, removing spike noise by adopting a nonlinear energy operator or a statistical means; secondly, removing power line harmonics by adopting a harmonic modeling method based on a least square method theory; then, overlapping the data acquired for many times to suppress random noise; and finally, extracting envelope and gate integral processing of the superposed data, and providing the processed data to inversion software to realize the explanation of the underground hydrogeological information. For corrupted MRS signals, even those completely swamped by noise, suppression or removal of the noise is inevitably required to extract the required information. At present, for filtering power frequency harmonic waves and random noise: legchenko and Valla, in Removal of power-line harmonics from magnetic resonance measures (Journal of Applied Geophysics, Vol. 53: 103-. In the article "Adaptive noise cancellation of multichannel magnetic resonance signals" (geophysics Journal International, vol.191: 88-100.) by Dalgaard et al, it is proposed to use an Adaptive noise cancellation algorithm to process a multichannel MRS probe signal, so as to cancel out the correlated noise in the main channel and the reference channel. Tianbaofeng et al, in a paper "magnetic resonance signal noise suppression method based on reference coil and variable step size adaptation" (in the Proc. geophysical sciences, vol. 55, No. 7: 2462-. Ghanati et al, in the article "Joint application of a static optimization process empirical mode decomposition to MRS noise cancellation" (Journal of Applied geomatics, vol 111, 5: 110 + 120), proposed the extraction of effective MRS signal attenuation trend based on EMD and CEEMD methods. Larsen et al, in the paper "Noise cancel harmonic signal combining model-based removal of powerline harmonics and multichannel Wiener filtering" (geographic Journal International 2014, volume 196, 2: 828. sup. 836 page.), realizes effective Noise suppression by combining power frequency harmonic modeling with multichannel Wiener filtering, and proposes a method adopting delay harmonic modeling for the special case of same frequency harmonic interference. Qi Wang et al, in An paper "An alternative adaptive approach to handling co-frequency harmonic in surface nuclear magnetic resonance data" (Geophanic Journal International, 2018, Vol. 215, 1962 and page 1973.) propose that power frequency harmonic modeling based on the least squares theory is used to remove power line harmonic noise interference. In addition, some scholars propose to perform noise suppression on MRS signals by statistical means such as Singular Spectral Analysis (SSA) and bisingular value decomposition (D-SVD). The data processing means adopts various strategies to remove and suppress noise, and finally adopts an envelope extraction algorithm to extract the MRS signal attenuation envelope. Although the above algorithms all obtain significant effects under certain conditions, due to the difference of geographic environmental conditions, and the irregularity, instability and specific spatial distribution of noise sources, the application of the algorithms is limited, and a more effective and good algorithm needs to be continuously searched for and applied to the aspects of MRS signal noise elimination, suppression and information extraction.
Disclosure of Invention
Aiming at the problems that the complexity of noise contained in MRS signals and the conventional EMD algorithm easily generates mode aliasing, the invention provides a magnetic resonance sounding signal envelope extraction method based on adaptive local iterative filtering, which can effectively avoid the mode aliasing problem of EMD.
The present invention is achieved in such a way that,
a magnetic resonance sounding signal envelope extraction method based on adaptive local iterative filtering comprises the following steps:
step 1: a group of MRS signals F (t) acquired by a nuclear magnetic resonance sounding water detector are directly converted into envelope signals f (t) by Hilbert transform and spectrum shifting;
step 2: determining the decomposition order of the envelope signal in the step 1 and the mask coefficient selected when calculating the filtering interval by adopting a traversal mode for the envelope signal, wherein the method comprises the following steps of firstly, using the mask coefficientIs determined as a certain value and then passes through the MRS signal initial amplitude E0And MRS signal mean decay time
Determining an optimal decomposition order; after the resolution order is determined, the initial amplitude E of MRS signal is determined by traversing the coefficients between 1.0-3.0 at intervals of 0.20And MRS signal mean decay time
To determine the optimal mask coefficients;
and step 3: and (3) extracting an IMF component from the real part and the imaginary part of the envelope signal f (t) by adopting an ALIF algorithm through an inner loop and extracting an effective MRS signal envelope by ending an extraction process through an outer loop respectively according to the decomposition order and the mask coefficient selected in the step (2) in a margin combination mode.
Further, the inner loop process in step 3 comprises: calculating the convolution of an envelope signal f (t) to be decomposed and a filter function omega (t) to obtain a sliding operator (f) (t), then extracting the solved sliding operator (f) (t) from the envelope signal f (t), calculating to obtain a fluctuation operator kappa (f) (t), if the fluctuation operator kappa (f) (t) meets an IMF condition, taking kappa (f) (t) as an extracted IMF component c (t), and if the fluctuation operator kappa (f) (t) does not meet the IMF condition, continuously and repeatedly screening to obtain the IMF component with fixed frequency components.
Further, in the step 3, the external circulation process includes removing the IMF components c (t) obtained in the internal circulation process from the envelope signals f (t) to be decomposed to obtain a margin γ (t), terminating iteration if the margin γ (t) presents a monotonous trend characteristic, otherwise, taking the γ (t) as an original signal, entering the internal circulation, continuing to repeat the above steps until the condition is met, terminating the circulation, and finally obtaining a plurality of IMF components.
Further, the inner circulation process in step 3 specifically includes:
step 3 a: selecting a value of an expected decomposition order M for a real part and an imaginary part and a value of a mask coefficient lambda for calculating a filtering interval;
and step 3 b: calculating a filtering interval l according to equation (1)n
In the formula, N represents the number of sampling points of envelope signal f (x), k represents the number of extreme points of signal to be decomposed, λ represents a scalar parameter, and λ ∈ [1, 3 ]]，
Represents rounding down;
and step 3 c: solving a filter function according to a Fokker-Planck equation of the formula (2)
Wherein p (x) and q (x) are both smoothly derivable functions and are in [ a, b ], wherein a < 0 < b, satisfying: q (a) q (b) 0, and q (x) > 0 for any x e (a, b);
P(a)＜0＜P(b)；
alpha and beta are called steady state coefficients, and the value range is (0, 1);
in the equation
Will produce a diffusion effect and drive the equation solution h (x) to move from the center point of the interval (a, b) to the end points a and b; at the same time, the user can select the desired position,
bringing h (x) from both ends of a and b toward the center of the interval (a, b), and when the two are balanced, the following are provided:
at this time, the equation has a non-zero solution h (x) and satisfies the condition:
for any x epsilon (a, b), h (x) is more than or equal to 0;
for any one
H (x) is 0;
representing that all equation solutions fall on the interval [ a, b ], solving the Fokker-Planck equation solution h (x) as a solved filter function omega (t), wherein the filter function omega (t) solves different analytic values along with the change of the interval [ a, b ], so that the self-adaptive solution of the ALIF algorithm to the filter function is realized;
and step 3 d: solving for the sliding operator (f) (x) using equation (4)
In the formula, ω (t) represents a filter function, lnRepresenting a filtering interval;
step 3 e: computing the fluctuation operator κ (f) (x) using equation (5)
κ(f)(x)＝f(x)-(f)(x) (5)
And step 3 f: judging whether the fluctuation operator kappa (f) (x) meets the condition of the IMF component by using the formula (6), and if so, obtaining a first IMF component c1(x) If not, taking kappa (f) (x) as the signal to be decomposed, and continuing to repeat the processes from the step 3b to the step 3e until the condition of IMF component is satisfied, stopping screening,
wherein, IMFs (x) represents the current IMF to be judged, and IMFc (x) represents the previous IMF component, which represents the defined threshold, and ranges from 0.001 to 0.2.
Further, the external circulation process in the step 3 comprises the following steps:
step 3 g: obtaining the margin by equation (7)
γ1(x)＝f(x)-c1(x) (7)
Will gamma1(x) Repeating the inner loop process as the original signal to obtain the 2 nd IMF component, and using the formula (8) as the judgment gamman(x) The criterion of showing a monotonic trend characteristic, when the value is greater than 20, indicates that gamma isn(x) If the trend characteristic is monotonous, the circulation is terminated to obtain a plurality of IMF components, gamman(x) Is the nth margin, c1(x) The first IMF component, where f (x) is represented by equation (9);
where f is the current original signal, γkThe currently obtained margin is normally a reasonable value of 20;
wherein, ci(x) Is the ith IMF component.
Compared with the prior art, the invention has the beneficial effects that:
the invention selects a self-adaptive local iterative filtering algorithm as an extraction method of signal envelopes, the method comprises the steps of solving by utilizing the obtained filtering function and filtering interval to obtain a sliding operator, then extracting the sliding operator from an original signal, calculating to obtain a fluctuation operator, checking whether the fluctuation operator meets the condition of IMF component, continuously updating the filtering function and the filtering interval to obtain the IMF component until all IMF components are extracted from the original signal and the remaining margin has obvious monotone trend characteristics, and finally obtaining a plurality of intrinsic mode function components to realize effective decomposition of the signal. In view of the fact that the adaptive local iterative filtering has a solid mathematical foundation and can solve the problem of mode aliasing existing in the traditional EMD, the invention provides the method for extracting the envelope of the MRS signal by adopting the ALIF algorithm directly, and by means of the characteristic of algorithm self-adaptation, the filtering function is selected in a self-adaptive mode, so that the filtering process has smoothness, and artificial oscillation cannot be generated in the IMF component generated subsequently. In addition, in order to capture non-stationary changes in signal frequency and amplitude, the length of the filter is adjusted accordingly. Therefore, according to local conditions in the whole signal processing process, all signals are not considered together, unnecessary influence factors are reduced, and the accuracy and the reliability of a processing result are greatly improved. Therefore, the effective application of the method has profound theoretical significance for improving the anti-interference capability of the magnetic resonance sounding technology, has new application value for directly extracting the envelope of the magnetic resonance sounding signal, and has instructive effect on the thought inspiration of the theoretical method research in the field of signal processing.
Drawings
Fig. 1 is a block flow diagram of magnetic resonance sounding signal envelope extraction based on adaptive local iterative filtering;
FIG. 2 is a block flow diagram of an adaptive local iterative filtering algorithm;
fig. 3 shows an ideal MRS signal and frequency spectrum, fig. 3A is a time-amplitude diagram, and fig. 3B is a frequency-power spectral density diagram;
fig. 4 illustrates a noisy MRS signal and its frequency spectrum, fig. 4A is a time-amplitude diagram, and fig. 4B is a frequency-power spectral density diagram;
fig. 5 illustrates a full-wave signal of noisy MRS full-wave signal converted into an envelope signal, fig. 5A illustrates a time-amplitude diagram of a full-wave signal and its envelope signal, and fig. 5B illustrates a time-amplitude diagram of a real part and an imaginary part of an envelope signal.
Fig. 6 is an IMF component graph obtained by decomposition processing of the ALIF algorithm, fig. 6A is an IMF component time-amplitude graph obtained by decomposition of the real part of the original envelope signal, and fig. 6B is an IMF component time-amplitude graph obtained by decomposition of the imaginary part thereof.
Fig. 7 is a graph of the residual time-amplitude remaining after extraction of the IMF components, fig. 7A, 7B being real and imaginary, respectively.
Fig. 8 shows the signal envelope resulting from the residual combination of the real and imaginary parts, fig. 8A is a time-amplitude diagram, and fig. 8B is a frequency-amplitude diagram.
Fig. 9 shows the measured MRS signal and its power spectrum, fig. 9A is a time-amplitude graph, and fig. 9B is a frequency-power spectral density graph.
Fig. 10 measures an envelope signal finally obtained by the MRS signal.
Detailed Description
In order to make the objects, technical solutions and advantages of the present invention more apparent, the present invention is further described in detail with reference to the following embodiments. It should be understood that the specific embodiments described herein are merely illustrative of the invention and are not intended to limit the invention.
As shown in fig. 1, the magnetic resonance sounding signal envelope extraction algorithm based on adaptive local iterative filtering includes the following steps:
step 1: a group of MRS signals F (t) acquired by a nuclear magnetic resonance sounding water detector are directly converted into envelope signals f (t) by Hilbert transform and spectrum shifting;
step 2: determining the order of decomposition and the mask coefficient selected during the calculation of the filtering interval in a traversal manner, i.e. determining the mask coefficient as a certain value, and then determining the initial amplitude E of the MRS signal0And MRS signal mean decay time
Determining an optimal decomposition order; after the resolution order is determined, the initial amplitude E of MRS signal is determined by traversing the coefficients between 1.0-3.0 at intervals of 0.20And MRS signal mean decay time
To determine the optimal mask coefficients;
and step 3: and (3) according to the key parameters selected in the step (2), including the decomposed order and the mask coefficient selected when the filtering interval is calculated, respectively processing the real part and the imaginary part by adopting an ALIF algorithm, and extracting a good and effective MRS signal envelope in a margin combination mode.
wherein the internal circulation process is as follows: calculating the convolution of an envelope signal f (t) to be decomposed and a filter function omega (t) to obtain a sliding operator (f) (t), then extracting the solved sliding operator (f) (t) from the envelope signal f (t), calculating to obtain a fluctuation operator kappa (f) (t), and if the fluctuation operator kappa (f) (t) meets the IMF condition, obtaining the component kappa (f) (t) which is the extracted IMF. Under the general condition, the fluctuation operators obtained by the first calculation do not meet the condition of the IMF component, and the IMF component of the fixed frequency component can be obtained by continuously and repeatedly screening in a circulating way. Therefore, the inner loop is stopped until the condition of the IMF component is satisfied.
The external circulation process is as follows: and (3) removing the IMF components c (t) obtained in the inner loop process from the signals f (t) to be decomposed to obtain the residual gamma (t), terminating iteration if the gamma (t) presents an obvious monotonous trend characteristic, otherwise, taking the gamma (t) as an original signal, entering the inner loop, continuously repeating the steps until the conditions are met, terminating the loop, and finally obtaining a plurality of IMF components.
As shown in fig. 2, the Adaptive Local Iterative Filtering (ALIF) algorithm provided by the present invention performs processing on a noisy MRS signal, that is, the specific steps of the inner loop process and the outer loop process are as follows:
step 3 a: selecting a value of an expected decomposition order M for a real part and an imaginary part and a value of a mask coefficient lambda for calculating a filtering interval;
and step 3 b: calculating a filtering interval l according to equation (1)n
In the formula, N represents the number of sampling points of envelope signal f (x), k represents the number of extreme points of signal to be decomposed, λ represents a scalar parameter, and λ ∈ [1, 3 ]]，
Indicating a rounding down.
And step 3 c: solving a filter function according to a Fokker-Planck equation of the formula (2)
Wherein p (x) and q (x) are both smoothly derivable functions and satisfy, at [ a, b ] (where a < 0 < b):
(1) q (a) q (b) 0, and q (x) > 0 for any x e (a, b);
(2)p(a)＜0＜p(b)。
alpha and beta are called steady state coefficients, and the value range is (0, 1).
In the equation
Will produce a diffusion effect and drive the equation solution h (x) to move from the center point of the interval (a, b) to the end points a and b; at the same time, the user can select the desired position,
h (x) from both ends of a and b to the center of the interval (a, b). When the two are in equilibrium, there are:
at this time, the equation has a non-zero solution h (x) and satisfies the condition:
(1) for any x epsilon (a, b), h (x) is more than or equal to 0;
(2) for any one
H (x) is 0;
this means that the equation solution set falls on the interval [ a, b ] completely, and the solution h (x) of the Fokker-Planck equation is the sought filter function ω (t). And omega (t) is solved to obtain different analytic values along with the change of the intervals (a, b), so that the adaptive solution of the ALIF algorithm to the filter function is realized.
And step 3 d: solving for the sliding operator (f) (x) using equation (4)
In the formula, ω (t) represents a filter function, lnRepresenting a filtering interval;
step 3 e: computing the fluctuation operator κ (f) (x) using equation (5)
κ(f)(x)＝f(x)-(f)(x) (5)
And step 3 f: judging whether the fluctuation operator kappa (f) (x) meets the condition of the IMF component by using the formula (6), and if so, obtaining a first IMF component c1(x) If not, taking kappa (f) (x) as a signal to be decomposed, and continuing to repeat the processes from the step 3b to the step 3e until the condition of IMF component is met, stopping screening.
In the formula, IMFs (x) represents the current IMF to be determined, and IMFc (x) represents the previous IMF component. Representing a defined threshold, ranging between 0.001 and 0.2.
Step 3 g: step 3 g: obtaining the margin by equation (7)
γ1(x)＝f(x)-c1(x) (7)
Will gamma1(x) Repeating the inner loop process as the original signal to obtain the 2 nd IMF component, and using the formula (8) as the judgment gamman(x) The criterion of showing a monotonic trend characteristic, when the value is greater than 20, indicates that gamma isn(x) If the trend characteristic is monotonous, the circulation is terminated to obtain a plurality of IMF components, gamman(x) Is the nth margin, c1(x) The first IMF component, where f (x) is represented by equation (9);
where f is the current original signal, γkThe currently obtained margin is normally a reasonable value of 20;
wherein, ci(x) Is the ith IMF component.
Example 1
This example is a simulation experiment of the method of the present invention conducted in the MATLAB 7.0 programming environment.
A magnetic resonance sounding signal envelope extraction algorithm simulation experiment based on adaptive local iterative filtering comprises the following steps:
step (1): by using
Constructing Larmor frequency of 2114Hz and amplitude E0180nV, relaxation time
The ideal MRS signal is 100ms, as shown in fig. 3, where fig. 3A is a time-amplitude graph and fig. 3B is a frequency-power spectral density graph. In addition, gaussian random white noise with the amplitude of 10nV is added, noise-containing MRS signals are generated by 80 power frequency harmonics with the amplitude of (0, 40) nV, the phase of (-pi, pi) is randomly generated, and the fundamental frequency of (49.9, 50.1), as shown in fig. 4, fig. 4A is a time-amplitude diagram, and fig. 4B is a frequency-power spectral density diagram;
step (2): first, the generated noise-containing MRS full-wave signal is converted into an envelope signal, as shown in fig. 5, fig. 5A is a time-amplitude diagram of the full-wave signal and its envelope signal, and fig. 5B is a time-amplitude diagram of the real part and imaginary part of the envelope signal. Then, the decomposition process of the ALIF algorithm is performed to obtain 7 IMF components, as shown in fig. 6, and fig. 6A, B shows an exploded view of the real part and the imaginary part of the full-wave signal after being converted into the envelope signal, respectively. Finally, after extracting the IMF component from the original signal, the remaining margin left is the target to be acquired, as shown in fig. 7, and fig. 7A and 7B are the margin of the real part and the margin of the imaginary part, respectively.
And (3): through the above process, further, the signal envelope can be directly obtained by combining the residuals of the real part and the imaginary part, as shown in fig. 8, where fig. 8A is a time-amplitude diagram and fig. 8B is a frequency-amplitude diagram.
In order to verify the practicability of the method, parameter extraction is carried out on the obtained MRS signal envelope, and the initial amplitude and the relaxation time of the obtained key parameters are respectively E0＝173.2983nV，T2 *The relative error is 3.7231% and 9.3126% respectively, which satisfy the application requirement 109.3 ms.
Example 2
In this embodiment, the MRS signal collected in the field of the cultural square in the vinpocetine city is used as the processing target of the method of the present invention.
The magnetic resonance sounding signal envelope extraction algorithm based on the adaptive local iterative filtering, referring to fig. 1, comprises the following steps:
step (1): a set of original noisy MRS signals acquired by a magnetic resonance depth sounding (MRS) water detector, the local larmor frequency is 2352Hz, as shown in fig. 9, fig. 9A is a time-amplitude graph, and fig. 9B is a frequency-power spectral density graph.
Step (2): and converting the acquired original full-wave MRS signal into an envelope signal, then carrying out decomposition processing of an ALIF algorithm, wherein the decomposition order is 7, and finally obtaining the remaining margin.
And (3): after the above processing procedure, the MRS signal envelope may be directly extracted, as shown in fig. 10.
The above description is only for the purpose of illustrating the preferred embodiments of the present invention and is not to be construed as limiting the invention, and any modifications, equivalents and improvements made within the spirit and principle of the present invention are intended to be included within the scope of the present invention.
Claims (5)
1. A magnetic resonance sounding signal envelope extraction method based on adaptive local iterative filtering is characterized by comprising the following steps:
step 1: a group of MRS signals F (t) acquired by a nuclear magnetic resonance sounding water detector are directly converted into envelope signals f (t) by Hilbert transform and spectrum shifting;
step 2: determining the decomposition order of the envelope signal in a traversal mode on the envelope signal in the step 1And calculating mask coefficient selected during filtering interval, including determining the mask coefficient as a certain value, and then using MRS signal initial amplitude E0And MRS signal mean decay time
Determining an optimal decomposition order; after the resolution order is determined, the initial amplitude E of MRS signal is determined by traversing the coefficients between 1.0-3.0 at intervals of 0.20And MRS signal mean decay time
To determine the optimal mask coefficients;
and step 3: and (3) extracting an IMF component from the real part and the imaginary part of the envelope signal f (t) by adopting an ALIF algorithm through an inner loop and extracting an effective MRS signal envelope by ending an extraction process through an outer loop respectively according to the decomposition order and the mask coefficient selected in the step (2) in a margin combination mode.
2. The method of claim 1, wherein said inner loop process of step 3 comprises: calculating the convolution of an envelope signal f (t) to be decomposed and a filter function omega (t) to obtain a sliding operator (f) (t), then extracting the solved sliding operator (f) (t) from the envelope signal f (t), calculating to obtain a fluctuation operator kappa (f) (t), if the fluctuation operator kappa (f) (t) meets an IMF condition, taking kappa (f) (t) as an extracted IMF component c (t), and if the fluctuation operator kappa (f) (t) does not meet the IMF condition, continuously and repeatedly screening to obtain the IMF component with fixed frequency components.
3. The method according to claim 2, wherein the outer loop process in step 3 comprises removing the IMF components c (t) obtained in the inner loop process from the envelope signal f (t) to be decomposed to obtain a margin γ (t), terminating the iteration if the margin γ (t) exhibits a monotonous trend characteristic, otherwise, taking γ (t) as an original signal, entering the inner loop, and continuing to repeat the above steps until a condition is met, terminating the loop, and finally obtaining a plurality of IMF components.
4. A method according to claim 3, wherein said inner loop process in step 3 specifically comprises:
step 3 a: selecting a value of an expected decomposition order M for a real part and an imaginary part and a value of a mask coefficient lambda for calculating a filtering interval;
and step 3 b: calculating a filtering interval l according to equation (1)n
In the formula, N represents the number of sampling points of envelope signal f (x), k represents the number of extreme points of signal to be decomposed, λ represents a scalar parameter, and λ ∈ [1, 3 ]]，
Represents rounding down;
and step 3 c: solving a filter function according to a Fokker-Planck equation of the formula (2)
Wherein p (x) and q (x) are both smoothly derivable functions and are in [ a, b ], wherein a < 0 < b, satisfying: q (a) q (b) 0, and q (x) > 0 for any x e (a, b);
p(a)＜0＜p(b)；
alpha and beta are called steady state coefficients, and the value range is (0, 1);
in the equation
Will produce a diffusion effect and drive the equation solution h (x) to move from the center point of the interval (a, b) to the end points a and b; at the same time, the user can select the desired position,
bringing h (x) from both ends of a and b toward the center of the interval (a, b), and when the two are balanced, the following are provided:
at this time, the equation has a non-zero solution h (x) and satisfies the condition:
for any x epsilon (a, b), h (x) is more than or equal to 0;
for any one
H (x) is 0;
representing that all equation solutions fall on the interval [ a, b ], solving the Fokker-Planck equation solution h (x) as a solved filter function omega (t), wherein the filter function omega (t) solves different analytic values along with the change of the interval [ a, b ], so that the self-adaptive solution of the ALIF algorithm to the filter function is realized;
and step 3 d: solving for the sliding operator (f) (x) using equation (4)
In the formula, ω (t) represents a filter function, lnRepresenting a filtering interval;
step 3 e: computing the fluctuation operator κ (f) (x) using equation (5)
κ(f)(x)＝f(x)-(f)(x) (5)
And step 3 f: judging whether the fluctuation operator kappa (f) (x) meets the condition of the IMF component by using the formula (6), and if so, obtaining a first IMF component c1(x) If not, taking kappa (f) (x) as the signal to be decomposed, and continuing to repeat the processes from the step 3b to the step 3e until the condition of IMF component is satisfied, stopping screening,
wherein, IMFs (x) represents the current IMF to be judged, and IMFc (x) represents the previous IMF component, which represents the defined threshold, and ranges from 0.001 to 0.2.
5. The method of claim 3, wherein the outer loop process in step 3 comprises:
step 3 g: obtaining the margin by equation (7)
γ1(x)＝f(x)-c1(x) (7)
Will gamma1(x) Repeating the inner loop process as the original signal to obtain the 2 nd IMF component, and using the formula (8) as the judgment gamman(x) The criterion of showing a monotonic trend characteristic, when the value is greater than 20, indicates that gamma isn(x) If the trend characteristic is monotonous, the circulation is terminated to obtain a plurality of IMF components, gamman(x) Is the nth margin, c1(x) The first IMF component, where f (x) is represented by equation (9);
where f is the current original signal, γkThe currently obtained margin is normally a reasonable value of 20;
wherein, ci(x) Is the ith IMF component.
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Citations (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102368095A (en) * | 2011-09-10 | 2012-03-07 | 吉林大学 | Extraction method for relaxation time spectrum of nuclear magnetic resonance detection signal for underground water by utilizing multi exponent fitting technology |
| WO2015114244A1 (en) * | 2014-01-29 | 2015-08-06 | Centre National De La Recherche Scientifique (Cnrs) | Device and method for ultrasonic inspection of bone quality |
| CN106198018A (en) * | 2016-06-29 | 2016-12-07 | 潍坊学院 | The EEMD of a kind of rotating machinery and smooth iteration envelope Analysis Method |
| CN106198013A (en) * | 2016-06-29 | 2016-12-07 | 潍坊学院 | A kind of envelope Analysis Method based on empirical mode decomposition filtering |
| CN107783200A (en) * | 2017-11-21 | 2018-03-09 | 吉林大学 | Joint EMD and TFPF algorithms a kind of all-wave magnetic resonance signal random noise method for reducing |
| CN108459353A (en) * | 2018-03-26 | 2018-08-28 | 吉林大学 | Faint magnetic resonance signal extracting method and device under a kind of electromagnetic noise background |
| CN109470135A (en) * | 2018-11-12 | 2019-03-15 | 吉林大学 | CSAMT data inactivity bearing calibration |
| CN109827697A (en) * | 2019-03-19 | 2019-05-31 | 东南大学 | Suspension cable time-varying Suo Li recognition methods based on local mean value mode decomposition |
| CN111239837A (en) * | 2020-02-20 | 2020-06-05 | 吉林大学 | Ground nuclear magnetic resonance signal parameter extraction method based on MCMC |
| CN111352163A (en) * | 2020-03-03 | 2020-06-30 | 吉林大学 | Magnetotelluric depth sounding-based static effect correction method and system |
-
2020
- 2020-08-25 CN CN202010860696.0A patent/CN112099100B/en active Active
Patent Citations (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102368095A (en) * | 2011-09-10 | 2012-03-07 | 吉林大学 | Extraction method for relaxation time spectrum of nuclear magnetic resonance detection signal for underground water by utilizing multi exponent fitting technology |
| WO2015114244A1 (en) * | 2014-01-29 | 2015-08-06 | Centre National De La Recherche Scientifique (Cnrs) | Device and method for ultrasonic inspection of bone quality |
| CN106198018A (en) * | 2016-06-29 | 2016-12-07 | 潍坊学院 | The EEMD of a kind of rotating machinery and smooth iteration envelope Analysis Method |
| CN106198013A (en) * | 2016-06-29 | 2016-12-07 | 潍坊学院 | A kind of envelope Analysis Method based on empirical mode decomposition filtering |
| CN107783200A (en) * | 2017-11-21 | 2018-03-09 | 吉林大学 | Joint EMD and TFPF algorithms a kind of all-wave magnetic resonance signal random noise method for reducing |
| CN108459353A (en) * | 2018-03-26 | 2018-08-28 | 吉林大学 | Faint magnetic resonance signal extracting method and device under a kind of electromagnetic noise background |
| CN109470135A (en) * | 2018-11-12 | 2019-03-15 | 吉林大学 | CSAMT data inactivity bearing calibration |
| CN109827697A (en) * | 2019-03-19 | 2019-05-31 | 东南大学 | Suspension cable time-varying Suo Li recognition methods based on local mean value mode decomposition |
| CN111239837A (en) * | 2020-02-20 | 2020-06-05 | 吉林大学 | Ground nuclear magnetic resonance signal parameter extraction method based on MCMC |
| CN111352163A (en) * | 2020-03-03 | 2020-06-30 | 吉林大学 | Magnetotelluric depth sounding-based static effect correction method and system |
Non-Patent Citations (1)
| Title |
|---|
| 陈保家等: "基于自适应局部迭代滤波和能量算子解调的滚动轴承故障特征提取", 《南京理工大学学报》 * |
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