CN106096530A - A kind of Modal Parameters Identification under strong background noise environment - Google Patents

A kind of Modal Parameters Identification under strong background noise environment Download PDF

Info

Publication number
CN106096530A
CN106096530A CN201610397420.7A CN201610397420A CN106096530A CN 106096530 A CN106096530 A CN 106096530A CN 201610397420 A CN201610397420 A CN 201610397420A CN 106096530 A CN106096530 A CN 106096530A
Authority
CN
China
Prior art keywords
response signal
frame
spectrum
impulse response
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201610397420.7A
Other languages
Chinese (zh)
Other versions
CN106096530B (en
Inventor
王琇峰
和丹
曾志豪
林京
雷亚国
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Xian Jiaotong University
Original Assignee
Xian Jiaotong University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Xian Jiaotong University filed Critical Xian Jiaotong University
Priority to CN201610397420.7A priority Critical patent/CN106096530B/en
Publication of CN106096530A publication Critical patent/CN106096530A/en
Application granted granted Critical
Publication of CN106096530B publication Critical patent/CN106096530B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2218/00Aspects of pattern recognition specially adapted for signal processing
    • G06F2218/02Preprocessing
    • G06F2218/04Denoising
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2218/00Aspects of pattern recognition specially adapted for signal processing
    • G06F2218/08Feature extraction

Landscapes

  • Engineering & Computer Science (AREA)
  • Theoretical Computer Science (AREA)
  • Artificial Intelligence (AREA)
  • Computer Vision & Pattern Recognition (AREA)
  • Signal Processing (AREA)
  • Physics & Mathematics (AREA)
  • General Engineering & Computer Science (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Abstract

A kind of Modal Parameters Identification under strong background noise environment, first pass through power hammer tap test and record one-level impulse response signal, then by spectrum-subtraction, one-level impulse response signal is carried out preliminary noise reduction, obtain secondary vein punching response signal, re-use Minimum Mean Square Error short time spectrum method and secondary vein punching response signal is carried out secondary noise reduction, obtain preferable impulse response signal, finally use Modal Parameter Identification algorithm that preferable impulse response letter is carried out Modal Parameter Identification, the present invention has self adaptation, calculating speed is fast, the Modal Parameter Identification advantage such as accurately under strong noise environment.

Description

A kind of Modal Parameters Identification under strong background noise environment
Technical field
The present invention relates to mould measurement field, particularly to the Modal Parameter Identification side under a kind of strong background noise environment Method.
Background technology
Modal Parameter Identification technology plays important in fields such as fault diagnosis, dynamic response analysis and Modifying model Effect, identification parameter includes natural frequency, damping ratio and the vibration shape.Conventional Modal Parameters Identification is divided into frequency domain and time domain Two big classes.Frequency domain and Time domain identification method all based on the impulse response signal that obtains of test data carry out modal parameter knowledge Not, impulse response signal accurately and reliably is therefore obtained most important.Due to signal measuring, in transmitting procedure inevitably By sound pollution in various degree, particularly in the mould measurement of large scale structure, around the parts such as motor, pump, air-conditioning produce Raw very noisy is relatively big on impulse response signal impact, and the accuracy of Modal Parameter Identification is by extreme influence.
For the problems referred to above, currently mainly use the modes such as statistical average, wavelet de-noising and singular value decomposition to eliminate and make an uproar The sound interference to impulse response signal, improves Modal Parameter Identification accuracy.Wherein, statistical average must assure that in measurement process Middle parameter does not changes, and otherwise uses statistical average nonsensical.And wavelet de-noising and singularity value decomposition are required for root Arranging different threshold parameter according to noise power, no survey noise reduction is impacted.Meanwhile, show currently without result of study, When the periodic component in very noisy and natural frequency close to or overlapping time, existing method can accurately identify modal parameter.Cause This, there is limitation in current Modal Parameters Identification, also room for improvement.
Summary of the invention
In order to overcome the shortcoming of above-mentioned prior art, it is an object of the invention to provide under a kind of strong background noise environment Modal Parameters Identification, improves Precision of Estimating Modal Parameter, has self adaptation strong, calculates speed fast, solid under strong noise environment The advantage such as have frequency identification accurately.
In order to achieve the above object, the technical scheme that the present invention takes is:
Modal Parameters Identification under a kind of strong background noise environment, comprises the following steps:
Step one, hammers tap test into shape by power, records one-level impulse response signal y (t), the one-level impulse response letter recorded Number y (t) comprises preferable impulse response signalWith ambient noise signal n (t), t represents the time;
Step 2, uses Optimal Smoothing Algorithm, the noise Estimation Algorithm of minimum statistics, or minimum controlled recursive average method In any one obtain one-level impulse response signal y (t) background noise estimated value
Step 3, estimates the background noise of one-level impulse response signal y (t) recorded He one-level impulse response signal y (t) EvaluationCarry out framing, add Hanning window and FFT process, obtain y (t) amplitude spectrum Y (p, k) and phase spectrum φ (p, k), andAmplitude spectrum(p, k) represents the kth root spectral component amplitude of the pth frame signal of y (t) to Y, and (p k) represents y to φ The kth root spectral component phase place of the pth frame signal of (t),RepresentThe kth root spectral component amplitude of pth frame signal, During framing, every frame length is the sample frequency of 0.02 times, front and back uses the degree of overlapping of 50% between frame;
Step 4, by spectrum-subtraction, to the amplitude spectrum Y recording one-level impulse response signal y (t), (p, k) carries out noise reduction process, obtains Compose to preliminary noise reduction amplitudeComputing formula is: Wherein, spectrum subtracts factor alpha=9, β=0.05;
Step 5, the phase spectrum φ that step 3 is obtained (p, preliminary noise reduction amplitude spectrum k) and obtained in step 4In conjunction with, by inverse fourier transform and overlap-add, obtain secondary vein punching response signal y1(t);
Step 6, uses Optimal Smoothing Algorithm, the noise Estimation Algorithm of minimum statistics, or minimum controlled recursive average method In any one obtain secondary vein punching response signal y1The background noise estimated value of (t)
Step 7, to secondary vein punching response signal y1(t) and secondary vein punching response signal y1The background noise estimated value of (t)Carry out framing, add Hanning window and FFT process, obtain secondary vein punching response signal y1The amplitude spectrum Y of (t)1(p, k) and phase place Spectrum φ1(p, k), andAmplitude spectrumY1(p k) represents y1The kth root spectral component width of the pth frame signal of (t) Value, φ1(p k) represents y1The kth root spectral component phase place of the pth frame signal of (t),RepresentPth frame signal Kth root spectral component amplitude, during framing, every frame length is the sample frequency of 0.2 times, front and back uses the degree of overlapping of 50% between frame;
Step 8, calculates secondary vein punching response signal y1Each frame posteriori SNR estimated value of (t), computing formula is:Wherein,RepresentVariance,With Y1(p, k) in step It is calculated in rapid five;
Step 9, by Minimum Mean Square Error short time spectrum method to secondary vein punching response signal y1The amplitude spectrum Y of (t)1 (p, k) carries out secondary noise reduction process, obtains secondary noise reduction amplitude spectrumThis calculating process uses endless form to enter OK, circulation starts to last frame to terminate from the first frame, carries out successively 1.~5. walking calculating below, and step is as follows:
1. use classical DD algorithm, calculate secondary vein punching response signal y1The pth frame a priori SNR estimation value of (t), meter Calculation formula is:
Wherein, attenuation quotient β ' =0.98;It is calculated in step 8;Initial value be set to 0 vector, later each frame The is used 5. to walk result of calculation;The posteriori SNR of the kth root spectral component representing pth+1 frame signal is estimated Value, this value is calculated in step 8;
2. secondary vein punching response signal y is calculated1The noise suppression factor of the pth frame spectral component of (t), computing formula is:WhereinThe is used 1. to walk result of calculation;
3. use prior weight evaluation method, calculate secondary vein punching response signal y1T the pth frame prior weight of () is estimated Evaluation, computing formula is:
Wherein, decline Subtract factor beta '=0.98;Y1(p k) is calculated in step 7;It is calculated in step 8;GDD(p, K) the is used 2. to walk result of calculation;It is calculated in step 8;
4. secondary vein punching response signal y is calculated1The noise suppression factor of the pth frame spectral component of (t), computing formula is:WhereinThe is used 3. to walk result of calculation;
5. by Minimum Mean Square Error short time spectrum method to Y1(p, pth frame spectral component k) carries out secondary noise reduction process, Obtain secondary noise reduction amplitude spectrumComputing formula is:Wherein (p k) uses G 4. walk result of calculation;Y1(p k) is calculated in step 7;
Step 10, the phase spectrum φ that will obtain in step 71(p, k) and use after Minimum Mean Square Error short time spectrum method The secondary noise reduction amplitude spectrum obtainedIn conjunction with, by inverse fourier transform and overlap-add, obtain preferable pulse and ring Induction signal
Step 11, by Modal Parameters Identification to preferable impulse response signalCarry out modal parameter knowledge Not.
Beneficial effects of the present invention: research finds, the method can effectively eliminate the steady letter in test pulse response signal Continuous part in number part and non-stationary signal, retains the transient portion thereof in non-stationary signal, i.e. preferably impulse response letter Number, thus improve Precision of Estimating Modal Parameter.
Compared to existing method, it is strong that the method has self adaptation, calculates speed fast, natural frequency identification under strong noise environment The advantage such as accurately.Even if the method is strong at test noise, in test noise, cyclic component and structural natural frequencies extremely connect In the case of Jin, it is also possible to accurately identify structural natural frequencies.
Accompanying drawing explanation
Fig. 1 is the steam turbine generator body diagram for Modal Parameter Identification.
Fig. 2 is one-level impulse response signal y (t) time-domain diagram of vibration measuring point.
Fig. 3 is one-level impulse response signal y (t) frequency domain figure of vibration measuring point.
Fig. 4 be vibration measuring point one-level impulse response signal y (t) processed by the invention after time-domain diagram.
Fig. 5 be vibration measuring point one-level impulse response signal y (t) processed by the invention after frequency domain figure.
Detailed description of the invention
Describe the present invention with case study on implementation below in conjunction with the accompanying drawings.
There is generator housing mesomerism problem in the generating set of certain nuclear power plant in running, in order to solve resonance Problem, demand accurately identifies the structural natural frequencies of generator housing, owing to site environment noise is strong, and in test noise Cyclic component and generator housing natural frequency are very close to, and existing method can not accurately identify the intrinsic frequency of generator housing Rate.This problem is solved below by the present invention.
Modal Parameters Identification under a kind of strong background noise environment, comprises the following steps:
Step one, hammers Knock test into shape by power, records the one-level impulse response signal y vibrating measuring point on generator housing T (), sample frequency is 500Hz, is shown that steam turbine generator body diagram with reference to Fig. 1, Fig. 1, and the casing of electromotor 3 only depends on Being placed on installation foundation 4 by gravity, the rotor 5 of electromotor 3 is connected on generator's cover 2 by sliding bearing, electromotor 3 Casing top connect and have 2 hydrogen-cooled devices of electromotor 1, vibration point position is arranged on 1 hydrogen-cooled device of electromotor 1;Fig. 2 and Tu 3 is one-level impulse response signal time domain waveform and the frequency domain vibrating measuring point on the generator housing by obtaining after this step respectively Oscillogram, owing to the environment noise around steam turbine generator is relatively big, in Fig. 2, the one-level impulse response signal of display is by noise Signal contamination, in Fig. 3, a prominent frequency (49.82Hz) of display is periodic noise;
Step 2, uses Optimal Smoothing Algorithm to obtain the background noise estimated value of one-level impulse response signal y (t)
Step 3, estimates the background noise of one-level impulse response signal y (t) recorded He one-level impulse response signal y (t) EvaluationCarry out framing, add Hanning window and FFT process, obtain y (t) amplitude spectrum Y (p, k) and phase spectrum φ (p, k), andAmplitude spectrumDuring framing, every frame length is the sample frequency of 0.02 times, front and back uses the weight of 50% between frame Folded degree;
Step 4, by spectrum-subtraction, to the amplitude spectrum Y of one-level impulse response signal y (t), (p, k) carries out noise reduction process, obtains Compose to preliminary noise reduction amplitudeComputing formula is:
Wherein, spectrum subtracts factor alpha=9, β=0.05;
Step 5, the phase spectrum φ that step 3 is obtained (p, preliminary noise reduction amplitude spectrum k) and obtained in step 4In conjunction with, by inverse fourier transform and overlap-add, obtain secondary vein punching response signal y1(t);
Step 6, uses Optimal Smoothing Algorithm to obtain secondary vein punching response signal y1The background noise estimated value of (t)
Step 7, to secondary vein punching response signal y1(t) and secondary vein punching response signal y1The background noise estimated value of (t)Carry out framing, add Hanning window and FFT process, obtain secondary vein punching response signal y1The amplitude spectrum Y of (t)1(p, k) and phase place Spectrum φ1(p, k), andAmplitude spectrumDuring framing, every frame length is the sample frequency of 0.2 times, front and back frame it Between use 50% degree of overlapping;
Step 8, calculates secondary vein punching response signal y1Each frame posteriori SNR estimated value of (t), computing formula is:Wherein,RepresentVariance,With Y1(p, k) in step It is calculated in five;
Step 9, by Minimum Mean Square Error short time spectrum method to secondary vein punching response signal y1The amplitude spectrum Y of (t)1 (p, k) carries out secondary noise reduction process, obtains the amplitude spectrum after secondary noise reductionThis calculating process uses endless form to enter OK, circulation starts to last frame to terminate from the first frame, carries out successively 1.~5. walking calculating below, and step is as follows:
1. use classical DD algorithm, calculate secondary vein punching response signal y1The pth frame a priori SNR estimation value of (t), meter Calculation formula is:
Wherein, attenuation quotient β ' =0.98;It is calculated in step 8;Initial value be set to 0 vector, later each frame The is used 5. to walk result of calculation;The posteriori SNR of the kth root spectral component representing pth+1 frame signal is estimated Value, this value is calculated in step 8;
2. secondary vein punching response signal y is calculated1The noise suppression factor of the pth frame spectral component of (t), computing formula is:WhereinThe is used 1. to walk result of calculation;
3. use the prior weight evaluation method of improvement, calculate secondary vein punching response signal y1The pth frame priori letter of (t) Making an uproar compared estimate value, computing formula is:
Wherein, Attenuation quotient β '=0.98;Y1(p k) is calculated in step 7;It is calculated in step 8;GDD (p k) uses 2. to walk result of calculation;It is calculated in step 8;
4. secondary vein punching response signal y is calculated1The noise suppression factor of the pth frame spectral component of (t), computing formula is:WhereinThe is used 3. to walk result of calculation;
5. by Minimum Mean Square Error short time spectrum method to Y1(p, pth frame spectral component k) carries out secondary noise reduction process, Obtain secondary noise reduction amplitude spectrumComputing formula is:Wherein (p k) uses G 4. walk result of calculation;Y1(p k) is calculated in step 7;
Step 10, the phase spectrum φ that will obtain in step 71(p, k) and use after Minimum Mean Square Error short time spectrum method The secondary noise reduction amplitude spectrum obtainedIn conjunction with, by inverse fourier transform and overlap-add, obtain preferable pulse and ring Induction signalIt is preferable impulse response signal with reference to Fig. 4, Fig. 4Time domain beamformer;
Step 11, to preferable impulse response signalCarry out Fourier transform, identify from corresponding frequency domain figure Generator housing natural frequency, Fig. 4 shows that the environment noise in one-level impulse response signal y (t) is removed;Fig. 5 is preferable Impulse response signalFrequency domain figure, the intrinsic of 48.99Hz can be there is with generator housing visible in detail from Fig. 5 Frequency, and then can determine whether that generator housing mesomerism problem is the natural frequency (48.99Hz) due to generator housing and work Make to turn frequency (50Hz) and get too close to caused.
Above content is to combine concrete preferred implementation further description made for the present invention, it is impossible to assert The detailed description of the invention of the present invention is only limitted to this, for general technical staff of the technical field of the invention, is not taking off On the premise of present inventive concept, it is also possible to make some simple deduction or replace, all should be considered as belonging to the present invention by institute The claims submitted to determine scope of patent protection.

Claims (1)

1. the Modal Parameters Identification under a strong background noise environment, it is characterised in that comprise the following steps:
Step one, hammers tap test into shape by power, records one-level impulse response signal y (t), the one-level impulse response signal y recorded T () comprises preferable impulse response signalWith ambient noise signal n (t), t represents the time;
Step 2, uses in Optimal Smoothing Algorithm, the noise Estimation Algorithm of minimum statistics, or minimum controlled recursive average method and appoints Meaning one obtains the background noise estimated value of one-level impulse response signal y (t)
Step 3, the background noise estimated value to one-level impulse response signal y (t) recorded He one-level impulse response signal y (t)Carry out framing, add Hanning window and FFT process, obtain y (t) amplitude spectrum Y (p, k) and phase spectrum φ (p, k), and Amplitude spectrum(p, k) represents the kth root spectral component amplitude of the pth frame signal of y (t) to Y, and (p k) represents y's (t) to φ The kth root spectral component phase place of pth frame signal,RepresentThe kth root spectral component amplitude of pth frame signal, framing Time, every frame length is the sample frequency of 0.02 times, front and back uses the degree of overlapping of 50% between frame;
Step 4, by spectrum-subtraction, to the amplitude spectrum Y recording one-level impulse response signal y (t), (p, k) carries out noise reduction process, obtains Compose to preliminary noise reduction amplitudeComputing formula is:
Wherein, spectrum subtracts factor alpha=9, β=0.05;
Step 5, the phase spectrum φ that step 3 is obtained (p, preliminary noise reduction amplitude spectrum k) and obtained in step 4 In conjunction with, by inverse fourier transform and overlap-add, obtain secondary vein punching response signal y1(t);
Step 6, uses in Optimal Smoothing Algorithm, the noise Estimation Algorithm of minimum statistics, or minimum controlled recursive average method and appoints Meaning one obtains secondary vein punching response signal y1The background noise estimated value of (t)
Step 7, to secondary vein punching response signal y1(t) and secondary vein punching response signal y1The background noise estimated value of (t) Carry out framing, add Hanning window and FFT process, obtain secondary vein punching response signal y1The amplitude spectrum Y of (t)1(p, k) with phase spectrum φ1 (p, k), andAmplitude spectrumY1(p k) represents y1The kth root spectral component amplitude of the pth frame signal of (t), φ1(p k) represents y1The kth root spectral component phase place of the pth frame signal of (t),RepresentPth frame signal K root spectral component amplitude, during framing, every frame length is the sample frequency of 0.2 times, front and back uses the degree of overlapping of 50% between frame;
Step 8, calculates secondary vein punching response signal y1Each frame posteriori SNR estimated value of (t), computing formula is:Wherein,RepresentVariance,With Y1(p, k) in step It is calculated in five;
Step 9, by Minimum Mean Square Error short time spectrum method to secondary vein punching response signal y1The amplitude spectrum Y of (t)1(p,k) Carry out secondary noise reduction process, obtain secondary noise reduction amplitude spectrumThis calculating process uses endless form to carry out, and follows Ring starts to last frame to terminate from the first frame, carries out successively 1.~5. walking calculating below, and step is as follows:
1. use classical DD algorithm, calculate secondary vein punching response signal y1The pth frame a priori SNR estimation value of (t), computing formula For:
Wherein, attenuation quotient β '= 0.98;It is calculated in step 8;Initial value be set to 0 vector, later each frame makes 5. result of calculation is walked with;Represent the posteriori SNR estimated value of the kth root spectral component of pth+1 frame signal, This value is calculated in step 8;
2. secondary vein punching response signal y is calculated1The noise suppression factor of the pth frame spectral component of (t), computing formula is:WhereinThe is used 1. to walk result of calculation;
3. use prior weight evaluation method, calculate secondary vein punching response signal y1The pth frame a priori SNR estimation value of (t), Computing formula is:
Wherein, decay system Number β '=0.98;Y1(p k) is calculated in step 7;It is calculated in step 8;GDD(p k) makes 2. result of calculation is walked with;It is calculated in step 8;
4. secondary vein punching response signal y is calculated1The noise suppression factor of the pth frame spectral component of (t), computing formula is:WhereinThe is used 3. to walk result of calculation;
5. by Minimum Mean Square Error short time spectrum method to Y1(p, pth frame spectral component k) carries out secondary noise reduction process, obtains Secondary noise reduction amplitude is composedComputing formula is:Wherein (p k) uses to G 4. result of calculation is walked;Y1(p k) is calculated in step 7;
Step 10, the phase spectrum φ that will obtain in step 71(p k) and obtains after using Minimum Mean Square Error short time spectrum method Secondary noise reduction amplitude spectrumIn conjunction with, by inverse fourier transform and overlap-add, obtain preferable impulse response letter Number
Step 11, by Modal Parameters Identification to preferable impulse response signalCarry out Modal Parameter Identification.
CN201610397420.7A 2016-06-07 2016-06-07 A kind of Modal Parameters Identification under strong background noise environment Active CN106096530B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610397420.7A CN106096530B (en) 2016-06-07 2016-06-07 A kind of Modal Parameters Identification under strong background noise environment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610397420.7A CN106096530B (en) 2016-06-07 2016-06-07 A kind of Modal Parameters Identification under strong background noise environment

Publications (2)

Publication Number Publication Date
CN106096530A true CN106096530A (en) 2016-11-09
CN106096530B CN106096530B (en) 2019-04-16

Family

ID=57448569

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610397420.7A Active CN106096530B (en) 2016-06-07 2016-06-07 A kind of Modal Parameters Identification under strong background noise environment

Country Status (1)

Country Link
CN (1) CN106096530B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112067116A (en) * 2020-07-13 2020-12-11 东南大学 Method for testing and analyzing impact vibration of medium and small bridges with noise resistance

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103246890A (en) * 2013-05-15 2013-08-14 中国石油大学(华东) Modal parameter recognizing method based on multi-input multi-output signal noise reduction
CN105205461A (en) * 2015-09-18 2015-12-30 中国石油大学(华东) Signal noise reducing method for modal parameter identification

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103246890A (en) * 2013-05-15 2013-08-14 中国石油大学(华东) Modal parameter recognizing method based on multi-input multi-output signal noise reduction
CN105205461A (en) * 2015-09-18 2015-12-30 中国石油大学(华东) Signal noise reducing method for modal parameter identification

Non-Patent Citations (6)

* Cited by examiner, † Cited by third party
Title
B.CAUBERGHE ET AL: "Identification of modal parameters including unmeasured forces and transient effects", 《JOURNAL OF SOUND AND VIBRATION》 *
CYRIL PLAPOUS ET AL: "Improved Signal-to-Noise Ratio Estimation for Speech Enhancement", 《IEEE TRANSACTIONS ON AUDIO,SPEECH AND LANGUAGE PROCESSING》 *
SAU-LON JAMES HU ET AL: "Model order determination and noise removal for modal parameter estimation", 《MECHANICAL SYSTEMS AND SIGNAL PROCESSING》 *
WEN-HWA WU ET AL: "A Multiple Random Decrement Method for Modal Parameter Identification of Stay Cables Based on Ambient Vibration Signals", 《ADVANCES IN STRUCTURAL ENGINEERING》 *
YARIV EPHRAIM ET AL: "Speech Enhancement Using a Minimum Mean-Square Error Short-Time Spectral Amplitude Estimator", 《IEEE TRANSACTIONS ON ACOUSTICS,SPEECH,AND SIGNAL PROCESSING》 *
王树青等: "一种模态参数识别的虚假模态剔除技术", 《中国海洋大学学报》 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112067116A (en) * 2020-07-13 2020-12-11 东南大学 Method for testing and analyzing impact vibration of medium and small bridges with noise resistance

Also Published As

Publication number Publication date
CN106096530B (en) 2019-04-16

Similar Documents

Publication Publication Date Title
CN108168891B (en) Method and equipment for extracting weak fault signal characteristics of rolling bearing
Huang et al. Time-frequency squeezing and generalized demodulation combined for variable speed bearing fault diagnosis
Hu et al. An adaptive and tacholess order analysis method based on enhanced empirical wavelet transform for fault detection of bearings with varying speeds
Liu et al. Adaptive spectral kurtosis filtering based on Morlet wavelet and its application for signal transients detection
Yang et al. Vibration condition monitoring system for wind turbine bearings based on noise suppression with multi-point data fusion
CN111665051A (en) Bearing fault diagnosis method under strong noise variable-speed condition based on energy weight method
CN106546892A (en) The recognition methodss of shelf depreciation ultrasonic audio and system based on deep learning
CN112101174A (en) LOF-Kurtogram-based mechanical fault diagnosis method
CN108871742B (en) Improved key-phase-free fault feature order extraction method
Akin et al. Phase-sensitive detection of motor fault signatures in the presence of noise
Wang et al. Bearing fault diagnosis of direct-drive wind turbines using multiscale filtering spectrum
CN110987438A (en) Method for detecting periodical vibration impact signals of hydraulic generator in variable rotating speed process
CN104714075B (en) A kind of electric network voltage flicker envelope parameters extracting method
Sun et al. Fault detection of rolling bearing using sparse representation-based adjacent signal difference
CN107831013B (en) Utilize the Method for Bearing Fault Diagnosis of probability principal component analysis enhancing cyclic bispectrum
Pang et al. Rolling bearing fault diagnosis based on SVDP-based kurtogram and Iterative autocorrelation of Teager energy operator
CN108120597A (en) Seat type crane hoisting mechanism fault signature extracting method under variable speed
Sun et al. Cyclostationary analysis of irregular statistical cyclicity and extraction of rotating speed for bearing diagnostics with speed fluctuations
CN108398260B (en) Method for quickly evaluating instantaneous angular speed of gearbox based on mixed probability method
Guan et al. Adaptive linear chirplet transform for analyzing signals with crossing frequency trajectories
CN105180959A (en) Anti-interference step counting method for wrist type step counting devices
Sun et al. Modal identification from non-stationary responses of high-rise buildings by variational mode decomposition and direct interpolation techniques
CN106096530A (en) A kind of Modal Parameters Identification under strong background noise environment
Vercoutter et al. Tip timing spectral estimation method for aeroelastic vibrations of turbomachinery blades
CN113255482A (en) HHT pulse parameter identification-based far-field harmonic wave earthquake motion synthesis method

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant