CN103940905A - Beam structural damage detection method based on stable wavelet transform and fractal analysis - Google Patents
Beam structural damage detection method based on stable wavelet transform and fractal analysis Download PDFInfo
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Abstract
The invention relates to a beam structural damage detection method based on stable wavelet transform and fractal analysis, and the method is particularly applicable to situation that weak damage to a beam structure is detected based on a modal vibration shape or a working vibration shape of the beam in a noise environment (on-site engineering environment). The method comprises the following steps: measuring the modal vibration shape or the working vibration shape of the beam, enabling the number of sampling points of the testing vibration shape to meet the requirements on the stable wavelet transform, performing stable wavelet transform hierarchy decomposition on the testing vibration shape so as to obtain detail transform coefficients of different scales after the decomposition, performing Katz fractal analysis on each detail transform coefficient under a set window so as to obtain fractal dimensional trace of different scales, respectively calculating the information entropy of the fractal dimensional trace of different scales so as to obtain an information entropy-spectrum, and judging according to the scale fractal dimensional trace of a layer (scale) enabling the values in the information entropy-spectrum to be suddenly reduced, wherein high jumping of the scale fractal dimensional trace indicates happening of damage, and the position of the damage is pointed out.
Description
Technical field
The present invention relates to a kind of girder construction damage detecting method based on Stationary Wavelet Transform and fractals.
Background technology
Works is carried out to health monitoring, to structure earlier damage is keeped in repair, not only can significantly reduce maintenance cost, and can ensure structural behaviour, the extending structure life-span.Beam structure, as the typical members of works, damages identification to it, particularly does structure Non-Destructive Testing and has obtained domestic and international broad research.
Structural damage detection method based on theory of oscillation is at present domestic and international broad research and large class methods that obtained Preliminary Applications.But these method ubiquities: insensitive to small and weak damage, noise immunity is low, rely on the deficiencies such as harmless benchmark architecture.To the damage check of works, often under noise circumstance (engineering site environment), to the detection of the small and weak damage of structure, and generally lack the original mechanics parameter information of works.Research shows that structure microlesion only has remarkable response on some or several power yardsticks of total, and insensitive to other yardstick.Based on Stationary Wavelet Transform, the vibration shape is carried out to multiple dimensioned layering decomposition, and the research that combination utilizes the advantage of Fractal Dimension Analysis technology in announcement Signal Singularity to carry out the small and weak damage check of girder construction under noise circumstance have not been reported.
Summary of the invention
For overcoming the problems referred to above, the invention provides a kind of girder construction damage detecting method based on Stationary Wavelet Transform and fractals.Be specially adapted to the detection to the small and weak damage of girder construction under noise circumstance.
The method is carried out multiple dimensioned layering decomposition based on Stationary Wavelet Transform to the vibration shape, and in conjunction with utilizing Fractal Dimension Analysis technology to carry out structural damage detection in the advantage disclosing in Signal Singularity.Than existing method, that the present invention has is responsive to small and weak damage, anti-noise ability by force, does not rely on the advantages such as harmless benchmark architecture.Can be used for the small and weak damage of girder construction under noise circumstance to detect.The invention solves in addition in multi-scale Wavelet Analysis and select which (a bit) yardstick to carry out a difficult problem for damage check, the Structure Damage Identification to other based on multiscale analysis has inspiration and reference function.
For reaching above object, the technical solution adopted in the present invention is:
A girder construction damage detecting method based on Stationary Wavelet Transform and fractals, comprises the following steps: A, based on modern measurement equipment, as laser scanning vialog, obtains Mode Shape or the work vibration shape shape signal W of girder construction;
B, vibration shape multiscale analysis;
If vibration shape shape signal W data length does not meet the needs of Stationary Wavelet Transform (stationary wavelet transform, SWT), Data of Mode is carried out to linear interpolation, obtaining number is 2
nthe new signal W of multiple
*, to meet the needs that the vibration shape carried out to Stationary Wavelet Transform; N is the number of plies of the vibration shape being carried out to Stationary Wavelet Transform predecomposition, gets 4 or 5; If W data length meets the needs of SWT, W is carried out to Stationary Wavelet Transform, obtain yardstick mode factor.
To W or W
*carry out Stationary Wavelet Transform, obtain vibration shape Scale Decomposition coefficient as the formula (1):
W (or W
*)=A
n+ D
n+ D
n-1+ ... D
i+ ... + D
2+ D
1(1)
In formula, A
nand D
ifor vibration shape Scale Decomposition coefficient, i=1,2 ..., N; N is the number of plies of predecomposition, and N gets 4 or 5.Wherein A
nfor yardstick 2
non approximation coefficient, D
ifor yardstick 2
ion detail coefficients; In operation, can utilize ' swt ' order in MATLAB software to realize the multiscale analysis of formula (1) to the vibration shape;
C, obtain the scale fractal dimension trace (scale fractal dimension trajectory, SFDT) of each detail coefficients: given one comprises the moving window that number of samples is n, and n=4,6 or 8, makes sliding window along detail coefficients D
isquiggle constantly move forward, each mobile sliding window all calculates Katz fractal dimension (the Katz's fractal dimension of contained segment of curve in window, KFD) and as the fractal dimension of this sliding window central sample point, along with sliding window traversal whole piece squiggle, just obtain corresponding to D
iscale fractal dimension trace (SFDT-D
i); Wherein KFD is calculated as follows:
In formula: d is the maximal value of the air line distance of any two sampled points on the interior squiggle of window; L is squiggle total length in window;
D, calculating SFDT-D
iinformation entropy (information entropy, IE), composition information entropy-spectrum: calculate each SFDT-D by formula (3)
iinformation entropy,
In formula: N
isFDT-D
isample points, Probability p
ikcalculated by formula (4),
C ' in formula
ikthe SFDT-D through threshold value correction
icoefficient, the coefficient settings that is not more than threshold value is zero, and the coefficient that is greater than threshold value remains unchanged; Threshold value is defined as average and the standard deviation sum of SFDT-Di original coefficient; Min represents to get minimum value.
By each SFDT-D
iinformation entropy composition information entropy-spectrum
in information entropy-spectrum, diminish the suddenly layer at place of numerical value is defined as structural damage detection yardstick used.Damage identification by the SFDT under this yardstick: in SFDT, high takeofing indicating the generation of damage, and indicated the position of damage.
Beneficial effect of the present invention shows:
1. whether the present invention can be used for the various damages of beam structure, as the detection of crackle, hole, layering, corrosion etc., can disclose damage to occur, and can determine the exact position of damage.
2. the present invention is by decomposing (formula (1)) and further Fractal Dimension Analysis (formula (2)) to the layering of the vibration shape, make this law possess the ability of identifying small and weak damage under noise circumstance, be particularly suitable for the detection of the small and weak damage of beam structure under engineering site environment.
3. the present invention utilizes the vibration shape scale fractal dimension trace information entropy (formula (3)) of definition to determine that damage information accounts for the layer at leading vibration shape scale coefficient place, has solved a difficult problem for How to choose yardstick in the girder construction damage check based on multi-scale Wavelet Analysis.
Brief description of the drawings
In order to be illustrated more clearly in the embodiment of the present application or technical scheme of the prior art, to the accompanying drawing of required use in embodiment or description of the Prior Art be briefly described below, apparently, the accompanying drawing the following describes is only some embodiment that record in the application, for those of ordinary skill in the art, do not paying under the prerequisite of creative work, can also obtain according to these accompanying drawings other accompanying drawing;
Fig. 1 method schematic diagram;
The actual measurement vibration shape of Fig. 2 girder construction under 3950Hz frequency excitation;
In Fig. 2, testing sampling number is 297.
Fig. 3 girder construction is the vibration shape after data expansion under 3950Hz frequency excitation;
Fig. 3 explanation: by linear interpolation, sampling number is expanded to 320, to meet the needs of Stationary Wavelet Transform.This example is decomposed number of plies N=4, and 320 is 2
420 times.
The each detail coefficients figure of Fig. 4 vibration shape Stationary Wavelet Transform;
Fig. 4 has shown the multiscale analysis effect to the vibration shape.
Scale fractal dimension trace diagram in Fig. 5 vibration shape SWT detail coefficients.
Fig. 5 explanation: at SFDT-D
3on can detect the generation of damage, and can accurately determine its position.
Embodiment
The correlation technique content of not addressing below all can adopt or use for reference prior art.
In order to make those skilled in the art person understand better the technical scheme in the application, below in conjunction with the accompanying drawing in the embodiment of the present application, technical scheme in the embodiment of the present application is clearly and completely described, obviously, described embodiment is only some embodiments of the present application, instead of whole embodiment.Based on the embodiment in the application, those of ordinary skill in the art are not making the every other embodiment obtaining under creative work prerequisite, all should belong to the scope of the application's protection.
Embodiment
The semi-girder that the present embodiment selects one 6061 aluminium alloys to make, beam length 543mm, wide 30mm, high 8mm, at the beam back side apart from stiff end 293mm place, opens a wide 1mm, and deeply 1mm runs through the crack of beam width direction.
With modality vibration exciter as power driver at the beam back side, near applying sinusoidal excitation with natural frequency near free end, measure the vibration in beam front as sensor with laser vibration measurer simultaneously, obtain the vibration shape signal of beam under excitation frequency; The vibration shape of the present embodiment is drawn by 297 sampled points that are spacedly distributed on beam.
In the present embodiment, laser sensor is the PSV-400 laser scanning vialog that German Polytec company produces; Power driver is 4890 modality vibration exciters that B & K company of Denmark produces.Multiscale analysis to the vibration shape in analysis and obtaining of scale fractal dimension trace all utilize MATLAB software programming to realize.
Taking girder construction, the test result under 3950Hz frequency excitation is carried out the detailed description of this method as example below, can certainly select the test result under other excitation frequencies to carry out damage check.
A. obtain the vibration shape of girder construction under 3950Hz frequency excitation by actual measurement, as shown in Figure 2.
B. by linear interpolation, by Data of Mode continuation to 320 point, (this example is decomposed number of plies N=4, and 320 is 2
420 times), obtain the vibration shape after data expansions, as shown in Figure 3.The vibration shape after data expansion is carried out to Stationary Wavelet Transform layering decomposition, and decomposing the number of plies is 4, and N=4 in formula (1), obtains each detail coefficients D thus
1, D
2, D
3, D
4, as shown in Figure 4.In operation, can utilize ' swt ' order in MATLAB software to realize the Stationary Wavelet Transform layering decomposition to the expansion vibration shape.
C. given one to comprise number of samples be 6 moving window, sliding window is constantly moved forward along the squiggle of each detail coefficients, each mobile sliding window all calculates the Katz fractal dimension of contained segment of curve in window the fractal dimension as this sliding window central sample point by formula (2), along with sliding window traversal whole piece squiggle, just obtain corresponding scale fractal dimension trace.Each scale fractal dimension trace SFDT-D
1, SFDT-D
2, SFDT-D
3, SFDT-D
4as shown in Figure 5.
D. the information entropy of calculating each scale fractal dimension trace by formula (3), the information entropy obtaining under each yardstick is
Visible yardstick information entropy-spectrum, the 3rd layer of sudden change that existence diminishes, represents that this layer (yardstick) can be used as the yardstick of damage check.
As seen from Figure 5, diminish suddenly in the information entropy-spectrum SFDT-D of place layer correspondence
3(the 3rd layer of scale fractal that detail coefficients is corresponding dimension trace of the vibration shape) has unique high takeofing, and the transverse axis position (about 290mm) that this peak value is corresponding is the damage position detecting, (circled positions in figure) conforms to actual damage position.Confirm thus the validity of the present invention to girder construction damage check; Meanwhile, this test contains neighbourhood noise and degree of injury is less, and the adaptability of this method to the small and weak structural damage detection of girder construction under noise circumstance has been described.
The above is only the application's preferred implementation, makes those skilled in the art can understand or realize the application.To be apparent to one skilled in the art to the multiple amendment of these embodiment, General Principle as defined herein can, in the case of not departing from the application's spirit or scope, realize in other embodiments.Therefore, the application will can not be restricted to these embodiment shown in this article, but will meet the widest scope consistent with principle disclosed herein and features of novelty.
Claims (1)
1. the girder construction damage detecting method based on Stationary Wavelet Transform and fractals, is characterized in that comprising the following steps:
A, the Mode Shape of obtaining girder construction or work vibration shape shape signal W;
B, vibration shape multiscale analysis;
If vibration shape shape signal W data length does not meet the needs of Stationary Wavelet Transform SWT, Data of Mode is carried out to linear interpolation, obtaining number is 2
nthe new signal W of multiple
*, to meet the needs that the vibration shape carried out to Stationary Wavelet Transform; N is the number of plies of the vibration shape being carried out to Stationary Wavelet Transform predecomposition, gets 4 or 5; If W data length meets the needs of SWT, W is carried out to Stationary Wavelet Transform, obtain yardstick mode factor;
To W or W
*carry out Stationary Wavelet Transform, obtain vibration shape Scale Decomposition coefficient as the formula (1):
W(W
*)=A
N+D
N+D
N-1+…D
i+…+D
2+D
1 (1)
In formula, A
nand D
ifor vibration shape Scale Decomposition coefficient, wherein A
nfor yardstick 2
non approximation coefficient, D
ifor yardstick 2
ion detail coefficients; In operation, utilize ' swt ' order in MATLAB software to realize the multiscale analysis of formula (1) to the vibration shape;
C, obtain the scale fractal dimension trace SFDT of each detail coefficients: given one comprises the moving window that number of samples is n, and n=4,6 or 8, makes sliding window along detail coefficients D
isquiggle constantly move forward, each mobile sliding window all calculates the Katz fractal dimension KFD of contained segment of curve in window the fractal dimension as this sliding window central sample point, along with sliding window travels through whole piece squiggle, just obtains corresponding to D
iscale fractal dimension trace (SFDT-D
i); Wherein KFD is calculated as follows:
In formula: d is the maximal value of the air line distance of any two sampled points on the interior squiggle of window; L is squiggle total length in window;
D, calculating SFDT-D
iinformation entropy IE, composition information entropy-spectrum: calculate each SFDT-D by formula (3)
iinformation entropy,
In formula: N
isFDT-D
isample points, Probability p
ikcalculated by formula (4),
C ' in formula
ikthe SFDT-D through threshold value correction
icoefficient, is not more than the SFDT-D of threshold value
icoefficient settings is zero, and is greater than the SFDT-D of threshold value
icoefficient remains unchanged; Threshold value is defined as SFDT-D
ithe average of original coefficient and standard deviation sum; Min represents to get minimum value;
By each SFDT-D
iinformation entropy composition information entropy-spectrum
in information entropy-spectrum, diminish the suddenly layer at place of numerical value is defined as structural damage detection yardstick used; Damage identification by the SFDT under this yardstick: in SFDT, high takeofing indicating the generation of damage, and indicated the position of damage;
Described i=1,2 ..., N, described N is the number of plies of predecomposition, gets 4 or 5.
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Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP3822802B2 (en) * | 2001-03-30 | 2006-09-20 | 財団法人鉄道総合技術研究所 | Concrete evaluation method and concrete evaluation equipment using impact sound |
CN101451338A (en) * | 2008-07-31 | 2009-06-10 | 重庆大学 | Separation method of bridge structural state historical information |
CN103575807A (en) * | 2013-10-24 | 2014-02-12 | 河海大学 | Method for detecting structural damage of beam based on Teager energy operator-wavelet transformation curvature mode |
-
2014
- 2014-04-16 CN CN201410153570.4A patent/CN103940905A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP3822802B2 (en) * | 2001-03-30 | 2006-09-20 | 財団法人鉄道総合技術研究所 | Concrete evaluation method and concrete evaluation equipment using impact sound |
CN101451338A (en) * | 2008-07-31 | 2009-06-10 | 重庆大学 | Separation method of bridge structural state historical information |
CN103575807A (en) * | 2013-10-24 | 2014-02-12 | 河海大学 | Method for detecting structural damage of beam based on Teager energy operator-wavelet transformation curvature mode |
Non-Patent Citations (2)
Title |
---|
楼铁峰,等: "小波理论及在结构损伤识别中的应用", 《中国水运》 * |
赵建英: "小波奇异性检测在梁结构损伤识别中的研究", 《工学硕士学位论文》 * |
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Application publication date: 20140723 |