CN113269082A - Partial discharge threshold denoising method based on improved variational modal decomposition - Google Patents

Partial discharge threshold denoising method based on improved variational modal decomposition Download PDF

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CN113269082A
CN113269082A CN202110556432.0A CN202110556432A CN113269082A CN 113269082 A CN113269082 A CN 113269082A CN 202110556432 A CN202110556432 A CN 202110556432A CN 113269082 A CN113269082 A CN 113269082A
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陈波
肖洒
沈道贤
刘冬梅
储昭碧
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Hefei University of Technology
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Abstract

The invention relates to a partial discharge threshold denoising method based on improved variational modal decomposition, which comprises the following steps: determining the decomposition layer number K of the variational modal decomposition; optimizing punishment factors corresponding to each layer of mode of variational mode decomposition; after the decomposition parameters are determined, decomposing the local discharge signal by using an optimized variational modal decomposition algorithm to obtain K intrinsic modal components with limited bandwidth, and calculating kurtosis values of the modal components; defining a significant component and a non-significant component of the kurtosis value; and reconstructing the effective component to obtain a reconstructed signal, and removing low-frequency white noise remained in the reconstructed signal to obtain a final denoised partial discharge signal. The invention effectively inhibits periodic narrow-band interference and white noise, reduces the distortion of the local discharge waveform, and completely retains the characteristic information of the local discharge signal.

Description

Partial discharge threshold denoising method based on improved variational modal decomposition
Technical Field
The invention relates to the field of partial discharge detection of high-voltage electrical equipment, in particular to a partial discharge threshold denoising method based on improved variational modal decomposition.
Background
With the increasing demand of electricity in China, the voltage level required by the power grid in China is higher and higher, and therefore, the high-voltage electrical equipment in the power grid needs to be guaranteed to operate stably and reliably. High voltage electrical equipment in electrical power systems, such as: gas insulated metal enclosed switchgear (GIS), power cable, etc., are in the live operating state for a long time, the inevitable insulating fault phenomenon that can appear. Partial Discharge (PD) is an early expression form of an insulation fault of high-voltage electrical equipment, so that the insulation state of the high-voltage electrical equipment can be effectively evaluated by partial discharge detection, potential faults of the equipment can be found in time, and the occurrence of operation faults is reduced. However, in the partial discharge detection, since the partial discharge signal is very weak and there is a serious noise interference in the detection site, the detected partial discharge signal is often submerged in the noise, which is not favorable for the partial discharge detection. Therefore, an effective noise suppression method is crucial to partial discharge detection of high-voltage electrical equipment.
Disclosure of Invention
The invention aims to provide a partial discharge threshold denoising method based on improved variational modal decomposition, and the algorithm process is clear and intuitive, has a good denoising effect and is high in solving speed.
In order to achieve the purpose, the invention adopts the following technical scheme:
a partial discharge threshold denoising method based on improved variational modal decomposition comprises the following steps:
step S1: determining the decomposition layer number K of the variational modal decomposition by utilizing the number of wave crests of the partial discharge signal spectrogram;
step S2: optimization of penalty factor alpha corresponding to each layer mode of variational modal decomposition by utilizing longicorn beard search algorithmK(k=1,2,...,K);
Step S3: after the decomposition parameters are determined, decomposing the local discharge signal by using an optimized variational modal decomposition algorithm to obtain K intrinsic modal components with limited bandwidth, and calculating kurtosis values of the modal components;
step S4: defining components with kurtosis values larger than 10 in the step S3 as valid components, and defining the rest as invalid components;
step S5: and reconstructing the effective components to obtain a reconstructed signal, and removing residual low-frequency white noise in the reconstructed signal by using a lifting wavelet threshold method to obtain a final denoised partial discharge signal.
In order to optimize the technical scheme, the specific measures adopted further comprise:
step S2 specifically includes:
s21: after the number of decomposition layers is determined, defining the search dimension of the longicorn whisker algorithm as K and the position of the longicorn as K
Figure RE-GDA0003146913760000021
Wherein N is the iteration number of the search;
s22: kurtosis is an index for evaluating impact property, and the expression is as follows:
Figure RE-GDA0003146913760000022
wherein: μ represents the mean value of the signal, and x represents the time series value of the signal;
defining an objective function f (x) of the longicorn algorithm as the sum of kurtosis of each modal component of the variational modal decomposition under each group of parameters, wherein the expression is as follows:
Figure RE-GDA0003146913760000023
wherein: k is the number of decomposition layers, Ku, obtained in step S1kIs the kurtosis value of the kth component, K ═ 1, 2.
S23: the longicorn whisker algorithm updating formula is as follows:
xn=xn-1nDsign[f(xr)-f(xl)]
wherein: d is a unitized random vector, xrIs the position of the right beard of the longicorn, xlIs the position of the left beard of the longicorn, deltanFor step size of each iteration, f (x)r) Is the target function value of the right beard of the longicorn, f (x)l) The target function value of the longicorn left tassel is shown, sign is a sign function, and the function of sign is as follows: when x is>0, sign (x) is 1; when x is 0, sign (x) is 0; when x is<At 0, sign (x) is-1.
Further, step S3 is specifically:
s31: the variable modal decomposition is to adaptively decompose the input signal x (t) into a plurality of modal component signals ukContinuously iterating and solving the optimal solution with the minimum sum of the estimation bandwidths of the modal components, wherein the expression is as follows:
Figure RE-GDA0003146913760000031
wherein: u. ofkIs the k-th modal component, ωkK is 1,2, for the respective center frequency, K, δ (t) is a dirac function,
Figure RE-GDA0003146913760000034
for gradient operations, x (t) represents the input signal;
s32: introducing a secondary penalty factor and a Lagrange multiplication operator to convert the secondary penalty factor and the Lagrange multiplication operator into an unconstrained variational problem, solving the problem by an alternating direction multiplier method, converting the quadratic penalty factor and the Lagrange multiplication operator into a frequency domain by utilizing Fourier equidistant transformation, and iteratively updating uk,ωkThe expression is:
Figure RE-GDA0003146913760000032
Figure RE-GDA0003146913760000033
wherein: the power factor represents Fourier transform;
s33: and outputting K modal components through inverse Fourier transform until the iteration stop condition is met.
Further, step S5 is specifically:
s51: reconstructing the effective component in the step S4 to obtain a reconstructed signal;
s52: selecting an optimal lifting wavelet basis function and an optimal decomposition scale;
s53: performing lifting wavelet decomposition on the reconstructed signal to obtain wavelet high-frequency coefficients and wavelet low-frequency coefficients of each layer;
s54: and carrying out soft threshold processing on the wavelet high-frequency coefficient obtained by decomposition, wherein the soft threshold function expression is as follows:
Figure RE-GDA0003146913760000041
wherein: djThe method is a wavelet decomposition coefficient, T is a threshold value, sign is a sign function, and the function of the method is as follows: when x is>0, sign (x) is 1; when x is 0, sign (x) is 0; when x is<0, sign (x) is-1;
s55: and performing lifting wavelet inverse transformation on the low-frequency wavelet coefficient and the high-frequency coefficient subjected to soft threshold processing to obtain a final denoised partial discharge signal.
According to the technical scheme, the partial discharge threshold denoising method based on the improved variational modal decomposition, which is disclosed by the invention, aims at the problem that the variational modal decomposition is difficult to adaptively select decomposition parameters in practical application, and provides that the number of decomposition layers is determined by the number of wave crests of a spectrogram, a punishment factor corresponding to each mode is optimized by adopting a Tianniu whisker search algorithm, and a kurtosis index is introduced to accurately select an effective component for reconstruction. The method effectively inhibits periodic narrow-band interference and white noise, reduces distortion of local discharge waveform, and completely retains characteristic information of the local discharge signal.
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FIG. 1 is a flowchart of a partial discharge threshold denoising method based on improved variational modal decomposition according to an embodiment of the present invention;
FIG. 2 is a time-domain sampling signal diagram of the original partial discharge signal in the present example;
FIG. 3 is a time-domain sampling signal diagram of the noise-contaminated partial discharge signal in the present example;
FIG. 4 is a graph of the spectrum of the noise-contaminated partial discharge signal in this example;
FIG. 5 is an iteration diagram of a Tianniu whisker search in this example;
FIG. 6 is a time domain diagram of modal components decomposed using a variational modal decomposition algorithm according to the present embodiment;
FIG. 7 is a spectrum of modal components decomposed using a variational modal decomposition algorithm according to the present embodiment;
FIG. 8 is a graph of denoising results using lifting db4 wavelet threshold in an example;
FIG. 9 is a graph of denoising results using ensemble empirical mode decomposition in an example;
FIG. 10 is a graph showing the results of the denoising method according to the present invention.
Detailed Description
The invention is further described below with reference to the accompanying drawings:
as shown in fig. 1, the present invention provides a partial discharge threshold denoising method based on improved variational modal decomposition, including the following steps:
step S1: determining the decomposition layer number K of the variational modal decomposition by utilizing the number of wave crests of the partial discharge signal spectrogram;
step S2: optimization of penalty factor alpha corresponding to each layer mode of variational modal decomposition by utilizing longicorn beard search algorithmk(k=1,2,...,K);
S21: after the number of decomposition layers is determined, defining the search dimension of the longicorn whisker algorithm as K and the position of the longicorn as K
Figure RE-GDA0003146913760000051
Wherein N is the iteration number of the search;
s22: kurtosis is an index for evaluating impact property, and the expression is as follows:
Figure RE-GDA0003146913760000052
wherein: μ represents the mean value of the signal, and x represents the time series value of the signal;
defining an objective function f (x) of the longicorn algorithm as the sum of kurtosis of each modal component of the variational modal decomposition under each group of parameters, wherein the expression is as follows:
Figure RE-GDA0003146913760000053
wherein: k is the number of decomposition layers, Ku, obtained in step S1kIs the kurtosis value of the kth component, K ═ 1, 2., K;
s23: the longicorn whisker algorithm updating formula is as follows:
xn=xn-1nDsign[f(xr)-f(xl)]
wherein: d is a unitized random vector, xrIs the position of the right beard of the longicorn, xlIs the position of the left beard of the longicorn, deltanFor step size of each iteration, f (x)r) Is the target function value of the right beard of the longicorn, f (x)l) The target function value of the longicorn left tassel is shown, sign is a sign function, and the function of sign is as follows: when x is>0, sign (x) is 1; when x is 0, sign (x) is 0; when x is<At 0, sign (x) is-1.
Step S3: after the decomposition parameters are determined, decomposing the local discharge signal by using an optimized variational modal decomposition algorithm to obtain K intrinsic modal components with limited bandwidth, and calculating kurtosis values of the modal components;
s31: the variable modal decomposition is to adaptively decompose the input signal x (t) into a plurality of modal component signals ukContinuously iterating and solving the optimal solution with the minimum sum of the estimation bandwidths of the modal components, wherein the expression is as follows:
Figure RE-GDA0003146913760000061
wherein: u. ofkIs the k-th modal component, ωkK is 1,2, for the respective center frequency, K, δ (t) is a dirac function,
Figure RE-GDA0003146913760000064
for gradient operations, x (t) represents the input signal;
s32: introducing a secondary penalty factor and a Lagrange multiplication operator to convert the secondary penalty factor and the Lagrange multiplication operator into an unconstrained variational problem, solving the problem by an alternating direction multiplier method, and then utilizing Fourier equidistant variationConversion to frequency domain, iterative update uk,ωkThe expression is:
Figure RE-GDA0003146913760000062
Figure RE-GDA0003146913760000063
wherein: the power factor represents Fourier transform;
s33: outputting K modal components through inverse Fourier transform until an iteration stop condition is met;
step S4: defining components with kurtosis values larger than 10 in the step S3 as valid components, and defining the rest as invalid components;
step S5: reconstructing the effective components to obtain a reconstructed signal, removing residual low-frequency white noise in the reconstructed signal by using a lifting wavelet threshold method to obtain a final denoised partial discharge signal;
s51: reconstructing the effective component in the step S4 to obtain a reconstructed signal;
s52: selecting an optimal lifting wavelet basis function and an optimal decomposition scale;
the optimal wavelet basis function selection process is as follows:
and selecting different wavelet functions as lifting wavelet bases, and performing noise reduction processing comparison on the same signal under the same decomposition scale. White noise is added into the single exponential oscillation attenuation function to serve as a noise-contaminated signal, the signal-to-noise ratio of the noise-contaminated signal is-18.96, and the selected lifting wavelet basis function is as follows: haar, db2, db4, db5, db6, sym4, all with a decomposition scale of 4. The snr after denoising using different lifting wavelet basis functions was calculated, and the results are shown in the following table, where it was found that denoising using wavelet db4 basis function was the best.
Under the same decomposition scale, adopting signal-to-noise ratio after noise reduction processing of different lifting wavelet basis functions
Wavelet basis function haar db2 db4 db5 db6 sym4
Signal to noise ratio 10.96 13.34 17.85 16.67 14.37 17.00
The optimal decomposition scale selection process comprises the following steps:
and decomposing the signal in different scales on the basis of determining the optimal wavelet basis function to determine the optimal decomposition scale. White noise is added into the single exponential oscillation attenuation function to serve as a noise-contaminated signal, the signal-to-noise ratio of the noise-contaminated signal is-18.96, and different decomposition scales J are set to be 3, 4, 5 and 6 respectively. The signal-to-noise ratio after noise reduction processing under different decomposition scales is calculated, and the result is shown in the following table, and the noise reduction processing result is found to be optimal when the decomposition scale is 3.
Under the optimal wavelet basis function, the signal-to-noise ratio after noise reduction processing is carried out by adopting different decomposition scales
Decomposition scale 3 4 5 6
Signal to noise ratio 18.23 16.46 13.24 14.67
S53: performing lifting wavelet decomposition on the reconstructed signal to obtain wavelet high-frequency coefficients and wavelet low-frequency coefficients of each layer;
s54: and carrying out soft threshold processing on the wavelet high-frequency coefficient obtained by decomposition, wherein the soft threshold function expression is as follows:
Figure RE-GDA0003146913760000081
wherein: djThe method is a wavelet decomposition coefficient, T is a threshold value, sign is a sign function, and the function of the method is as follows: when x is>0, sign (x) is 1; when x is 0, sign (x) is 0; when x is<0, sign (x) is-1;
s55: and performing lifting wavelet inverse transformation on the low-frequency wavelet coefficient and the high-frequency coefficient subjected to soft threshold processing to obtain a final denoised partial discharge signal.
The invention discloses a method based on improved variation modal decompositionThe partial discharge threshold denoising method comprises the steps of firstly, using the number of wave crests of a partial discharge signal spectrogram as the decomposition layer number K of variable modal decomposition, and optimizing a penalty factor alpha corresponding to each layer modal of the variable modal decomposition through a Tianniu whisker search algorithmk(K ═ 1, 2.., K). And then, processing the partial discharge signals by using the optimized variation mode decomposition to obtain K finite-bandwidth eigenmode components, and distinguishing effective components and ineffective components by adopting kurtosis index values. And finally reconstructing effective components, and removing residual white noise in the reconstructed signal by using a lifting wavelet threshold method to obtain a final denoised partial discharge signal. The invention can adaptively determine the decomposition parameters of the variational modal decomposition, simultaneously introduces the problem of lifting wavelet algorithm to process the incomplete filtering of low-frequency white noise, effectively filters periodic narrow-band interference and white noise, and better retains the integrity of the local discharge signal.
Examples of the design
Firstly, an ideal partial discharge signal model is established, a single-exponential oscillation attenuation model and a double-exponential oscillation attenuation model can be selected for simulation, periodic narrow-band interference signals and white noise are added into the ideal partial discharge model to simulate noise-polluted signals, and fig. 2 and 3 are graphs of the established ideal partial discharge signals and the noise-polluted partial discharge signals. And performing FFT analysis on the noise-contaminated signals, wherein FIG. 4 shows the frequency spectrum of the noise-contaminated partial discharge signals, and the number of decomposition layers for determining the variational modal decomposition is 5. FIG. 5 is a diagram of a search iteration process of a longicorn whisker, and each layer of penalty factors of variational modal decomposition is determined. And (3) processing the noise-contaminated partial discharge signal by using the optimized variation modal decomposition, wherein fig. 6 is a time domain diagram of each obtained modal component, and fig. 7 is a frequency spectrum corresponding to each modal component.
And calculating kurtosis values of the modal components, namely 18.34, 1.60, 1.56, 17.21 and 1.60 respectively, automatically identifying that the BIMF1 and the BIMF4 are effective components, reconstructing the effective components, and removing narrow-band interference signals and high-frequency white noise.
As can be seen from fig. 7, part of white noise with smaller amplitude still remains in BIMF1 and BIMF4, the white noise remaining in the reconstructed signal is further removed by using the lifting db4 wavelet threshold method, and finally the obtained denoised waveform is shown in fig. 10. Compared with other two traditional denoising methods, fig. 8 is a graph of denoising results by using lifting db4 wavelet threshold, and fig. 9 is a graph of denoising results by using ensemble empirical mode decomposition. As can be seen from the figure, the traditional method has a common denoising effect, the signal has serious waveform distortion and the partial discharge characteristic is lost, and the method provided by the invention has a good denoising effect, completely inhibits the noise and has a small signal distortion degree.
The above-mentioned embodiments are merely illustrative of the preferred embodiments of the present invention, and do not limit the scope of the present invention, and various modifications and improvements of the technical solution of the present invention by those skilled in the art should fall within the protection scope defined by the claims of the present invention without departing from the spirit of the present invention.

Claims (8)

1. A partial discharge threshold denoising method based on improved variational modal decomposition is characterized by comprising the following steps: the method comprises the following steps:
(1) determining the decomposition layer number K of the variational modal decomposition;
(2) optimizing punishment factors corresponding to each layer of mode of variational mode decomposition;
(3) after the decomposition parameters are determined, decomposing the local discharge signal by using an optimized variational modal decomposition algorithm to obtain K intrinsic modal components with limited bandwidth, and calculating kurtosis values of the modal components;
(4) defining a significant component and a non-significant component of the kurtosis value;
(5) and reconstructing the effective component to obtain a reconstructed signal, and removing low-frequency white noise remained in the reconstructed signal to obtain a final denoised partial discharge signal.
2. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 1, wherein: in the step (1), the number of decomposition layers K for determining the variational modal decomposition is determined by the number of peaks of the partial discharge signal spectrogram.
3. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 1, wherein: in the step (2), a longicorn whisker search algorithm is used for optimizing penalty factors corresponding to each layer of modal of variational modal decomposition.
4. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 1, wherein: in the step (4), the components with the kurtosis value larger than 10 are effective components, and the rest are ineffective components.
5. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 1, wherein: in the step (5), the removing of the low-frequency white noise remaining in the reconstructed signal is performed by a lifting wavelet threshold method.
6. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 3, wherein: in step 2, the longicorn stigma search formula is as follows:
xn=xn-1nDsign[f(xr)-f(xl)]
wherein: d is a unitized random vector, xrIs the position of the right beard of the longicorn, xlIs the position of the left beard of the longicorn, deltanFor step size of each iteration, f (x)r) Is the target function value of the right beard of the longicorn, f (x)l) The target function value of the longicorn left tassel is shown, sign is a sign function, and the function of sign is as follows: when x is>0, sign (x) is 1; when x is 0, sign (x) is 0; when x is<At 0, sign (x) is-1.
7. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 1, wherein: the step (3) specifically comprises the following steps:
(31) solving the optimal solution with the minimum sum of the modal component estimation bandwidths, wherein the expression is as follows:
Figure FDA0003077326130000021
wherein: u. ofkIs the k-th modal component, ωkK is 1,2, for the respective center frequency, K, δ (t) is a dirac function,
Figure FDA0003077326130000024
for gradient operations, x (t) represents the input signal;
(32) introducing a secondary penalty factor a and a Lagrange multiplication operator lambda to convert the secondary penalty factor a and the Lagrange multiplication operator lambda into an unconstrained variational problem, solving the problem by an alternating direction multiplier method, converting the problem into a frequency domain by utilizing Fourier equidistant transformation, and iteratively updating uk,ωkThe expression is as follows:
Figure FDA0003077326130000022
Figure FDA0003077326130000023
wherein: the power factor represents Fourier transform;
(33) and outputting K modal components through inverse Fourier transform until the iteration stop condition is met.
8. The partial discharge threshold denoising method based on improved variational modal decomposition according to claim 1, wherein: the step (5) specifically comprises the following steps:
(51) reconstructing the effective component in the step (4) to obtain a reconstructed signal;
(52) selecting an optimal lifting wavelet basis function and an optimal decomposition scale;
(53) performing lifting wavelet decomposition on the reconstructed signal to obtain wavelet high-frequency coefficients and wavelet low-frequency coefficients of each layer;
(54) and carrying out soft threshold processing on the wavelet high-frequency coefficient obtained by decomposition, wherein the soft threshold function expression is as follows:
Figure FDA0003077326130000031
wherein: djThe method is a wavelet decomposition coefficient, T is a threshold value, sign is a sign function, and the function of the method is as follows: when x is>0, sign (x) is 1; when x is 0, sign (x) is 0; when x is<0, sign (x) is-1;
(55) and performing lifting wavelet inverse transformation on the low-frequency wavelet coefficient and the high-frequency coefficient subjected to soft threshold processing to obtain a final denoised partial discharge signal.
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* Cited by examiner, † Cited by third party
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CN114492538A (en) * 2022-02-16 2022-05-13 国网江苏省电力有限公司宿迁供电分公司 Local discharge signal denoising method for urban medium-voltage distribution cable
CN114757233A (en) * 2022-04-24 2022-07-15 珠海市伊特高科技有限公司 ICEEMDAN partial discharge denoising method based on Pearson correlation coefficient
CN117332221A (en) * 2023-09-26 2024-01-02 国网江苏省电力有限公司南通供电分公司 Noise reduction method and system for oil leakage ultrasonic signals of hydraulic mechanism
CN117878973A (en) * 2024-03-13 2024-04-12 西安热工研究院有限公司 Frequency modulation method and system for fused salt coupling thermal power generating unit

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103630808A (en) * 2013-11-11 2014-03-12 华南理工大学 Partial discharge signal denoising method based on lifting wavelet transform
CN103675617A (en) * 2013-11-20 2014-03-26 西安交通大学 Anti-interference method for high-frequency partial discharge signal detection
CN105717422A (en) * 2015-12-04 2016-06-29 国家电网公司 High-voltage power equipment partial discharge feature extraction method and apparatus
CN106353649A (en) * 2016-09-18 2017-01-25 广东电网有限责任公司珠海供电局 Method for denoising partial discharge signals on basis of lifting wavelet transformation
CN107179486A (en) * 2017-05-24 2017-09-19 长沙理工大学 A kind of GIS device monitors ultrahigh-frequency signal noise-reduction method on-line
CN108804832A (en) * 2018-06-14 2018-11-13 东南大学 A kind of interval threshold Denoising of Partial Discharge based on VMD
CN108983058A (en) * 2018-08-29 2018-12-11 三峡大学 Partial discharge of transformer ultrahigh-frequency signal denoising method based on improved variation mode and singular value decomposition
CN111665424A (en) * 2020-06-15 2020-09-15 国网山东省电力公司潍坊供电公司 Electrical equipment partial discharge signal denoising method and system
CN111965499A (en) * 2020-07-27 2020-11-20 广东电网有限责任公司广州供电局 Partial discharge data denoising method and system based on empirical mode decomposition
CN112307963A (en) * 2020-10-30 2021-02-02 中国南方电网有限责任公司超高压输电公司检修试验中心 Converter transformer running state identification method based on vibration signals

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103630808A (en) * 2013-11-11 2014-03-12 华南理工大学 Partial discharge signal denoising method based on lifting wavelet transform
CN103675617A (en) * 2013-11-20 2014-03-26 西安交通大学 Anti-interference method for high-frequency partial discharge signal detection
CN105717422A (en) * 2015-12-04 2016-06-29 国家电网公司 High-voltage power equipment partial discharge feature extraction method and apparatus
CN106353649A (en) * 2016-09-18 2017-01-25 广东电网有限责任公司珠海供电局 Method for denoising partial discharge signals on basis of lifting wavelet transformation
CN107179486A (en) * 2017-05-24 2017-09-19 长沙理工大学 A kind of GIS device monitors ultrahigh-frequency signal noise-reduction method on-line
CN108804832A (en) * 2018-06-14 2018-11-13 东南大学 A kind of interval threshold Denoising of Partial Discharge based on VMD
CN108983058A (en) * 2018-08-29 2018-12-11 三峡大学 Partial discharge of transformer ultrahigh-frequency signal denoising method based on improved variation mode and singular value decomposition
CN111665424A (en) * 2020-06-15 2020-09-15 国网山东省电力公司潍坊供电公司 Electrical equipment partial discharge signal denoising method and system
CN111965499A (en) * 2020-07-27 2020-11-20 广东电网有限责任公司广州供电局 Partial discharge data denoising method and system based on empirical mode decomposition
CN112307963A (en) * 2020-10-30 2021-02-02 中国南方电网有限责任公司超高压输电公司检修试验中心 Converter transformer running state identification method based on vibration signals

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
吴炬卓 等: "基于提升小波分解的小波熵在抑制局部放电白噪声干扰中的应用", 《高压电器》 *
黄沁元 等: "基于变分模态分解和天牛须搜索的磁瓦内部缺陷声振检测", 《振动与冲击》 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113962266A (en) * 2021-10-25 2022-01-21 东北石油大学 Pipeline leakage signal denoising method based on improved BAS-VMD
CN114089138A (en) * 2021-11-26 2022-02-25 平顶山天安煤业股份有限公司 High-voltage cable partial discharge online monitoring method and system
CN114492538A (en) * 2022-02-16 2022-05-13 国网江苏省电力有限公司宿迁供电分公司 Local discharge signal denoising method for urban medium-voltage distribution cable
CN114492538B (en) * 2022-02-16 2023-09-05 国网江苏省电力有限公司宿迁供电分公司 Urban medium-voltage distribution cable partial discharge signal denoising method
CN114757233A (en) * 2022-04-24 2022-07-15 珠海市伊特高科技有限公司 ICEEMDAN partial discharge denoising method based on Pearson correlation coefficient
CN114757233B (en) * 2022-04-24 2023-07-11 珠海市伊特高科技有限公司 ICEEMDAN partial discharge denoising method based on pearson correlation coefficient
CN117332221A (en) * 2023-09-26 2024-01-02 国网江苏省电力有限公司南通供电分公司 Noise reduction method and system for oil leakage ultrasonic signals of hydraulic mechanism
CN117878973A (en) * 2024-03-13 2024-04-12 西安热工研究院有限公司 Frequency modulation method and system for fused salt coupling thermal power generating unit
CN117878973B (en) * 2024-03-13 2024-06-11 西安热工研究院有限公司 Frequency modulation method and system for fused salt coupling thermal power generating unit

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