CN106097430A - A kind of laser stripe center line extraction method of many gaussian signals matching - Google Patents
A kind of laser stripe center line extraction method of many gaussian signals matching Download PDFInfo
- Publication number
- CN106097430A CN106097430A CN201610487738.4A CN201610487738A CN106097430A CN 106097430 A CN106097430 A CN 106097430A CN 201610487738 A CN201610487738 A CN 201610487738A CN 106097430 A CN106097430 A CN 106097430A
- Authority
- CN
- China
- Prior art keywords
- signal
- gaussian
- substrate
- max
- dilatability
- 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
Links
Classifications
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T15/00—3D [Three Dimensional] image rendering
- G06T15/50—Lighting effects
- G06T15/503—Blending, e.g. for anti-aliasing
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T15/00—3D [Three Dimensional] image rendering
- G06T15/005—General purpose rendering architectures
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T7/00—Image analysis
- G06T7/0002—Inspection of images, e.g. flaw detection
- G06T7/0004—Industrial image inspection
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T7/00—Image analysis
- G06T7/0002—Inspection of images, e.g. flaw detection
- G06T7/0012—Biomedical image inspection
-
- G—PHYSICS
- G06—COMPUTING; CALCULATING OR COUNTING
- G06T—IMAGE DATA PROCESSING OR GENERATION, IN GENERAL
- G06T2211/00—Image generation
- G06T2211/40—Computed tomography
- G06T2211/416—Exact reconstruction
Abstract
The present invention is to provide the laser stripe center line extraction method of a kind of many gaussian signals matching.The inventive method has different expectation and the gaussian signal of method by using one group, get up with different positions and weighed combination, the farthest distribution of matching laser line image a line pixel value, when finding optimal matching combination, when combining according to each gaussian signal, location can make the optimal estimation to laser lines center.The inventive method can effectively solve, in the case of the pixel value of laser line image is distributed and cannot meet symmetry and homogeneity, to estimate the center of laser lines exactly, improve the precision of 3D scan rebuilding.
Description
Technical field
The present invention relates to the processing method of a kind of low cost 3D scanning system based on laser lines, be specifically related to one
Plant laser lines center extraction method based on gaussian signal matching.
Background technology
Three-dimension object recognition technology is at numerous areas such as robot workpiece grabbing, self-navigations, automatically detection, medical analysis
Have a wide range of applications.And 3D scanning system is as topmost data acquisition means, its acquisition precision will directly affect identification
Success or not.
It is currently based on the contactless 3D scanning system precision height of structure light, applied range, but the cost of its costliness limits
Having made the universal of it, therefore measuring system with the low cost of laser in place structure light has the most wide market and research sky
Between.
In a 3D scanning system based on laser, owing to there is camera collection precision, laser stripe has necessarily
Width and testee surface irregularity cause the problems such as reflective scattering, extracting laser stripe center the most exactly will be straight
Connect the acquisition precision of decision systems.
At present conventional lines center extraction algorithm has: extremum method, threshold method, geometrical center method, image thinning method, based on
The method of least square of Gauss distribution, Hessian matrix method etc..
Summary of the invention
It is an object of the invention to provide a kind of centrage that can accurately extract laser stripe image, make based on laser
3D scanning system there is the laser stripe center line extraction method of many gaussian signals matching of higher acquisition precision.
The object of the present invention is achieved like this:
Step one: obtained the image I comprising laser lines by image capture device, the resolution of image I is Ymax×
Xmax;
Step 2: set N (the N ∈ [1, X of image Imax]) row pixel value constitute sequence be initial data MN(j),(j
∈[1,Ymax]), obtain input signal m by a cube interpolation algorithmN(t), wherein t=nTs, TsIt is spaced for interpolation, N ∈ [1,
Xmax], j ∈ [1, Ymax];
Step 3: for the data after the laser lines pixel value normalization of the Nth row of image I, a scope is set and exists
Threshold value between 0.2 to 0.5, when pixel value data are more than described threshold value, is labeled as 1 by this pixel, less than described threshold value
Time, then it is labeled as 0;Calculate the average of row sequence number belonging to all pixels being labeled as 1, using this average as initial center point
u0, calculate the difference of the pixel point range sequence number maxima and minima being labeled as 1, using this difference as initial width of fringe simultaneously
w0;
Step 4: build one group of M and there is different expectation and the substrate gaussian signal set G for matching of variance, collection
The length of all substrate gaussian signals in conjunction and input signal mNT () is identical, and set zi=2 σi 2, σiHigh for i-stage substrate
The standard deviation of this signal, and by ziThe dilatability of named i-stage substrate gaussian signal, order expectation ui=u0+si, and by ui
The symmetrical centre of named i-stage substrate gaussian signal, wherein, u0For initial center point, siFor side-play amount;
Initial center point u that will obtain in step 30Symmetrical centre u as first order substrate gaussian signal0, i.e. u1=
u0, initial width of fringe w0For determining the dilatability of first order substrate gaussian signalWherein q is constant,
Thus obtain one group of M the substrate gaussian signal set G with different dilatability.
In above formula, gzi,uiX () is i-stage substrate gaussian signal, and its dilatability is zi, symmetrical centre is ui。
Step 5: by calculating maximum cross-correlation coefficient, tries to achieve the similarity of each substrate gaussian signal and input signal:
Wherein, rzi(τi) it is the maximum cross-correlation value of input signal and i-stage substrate gaussian signal, τiIt is that two signals are mutual
When pass value takes maximum, the relative alternate position spike of two signals;
Step 6: define artificial signal gfX () is m the substrate Gaussian function with different dilatability and symmetrical centre,
According to the signal after one group of fixing matching weights superposition, and setting initial m=2, matching weights are one group of fixing constant,
Choosing of it should follow dilatability ziThe biggest, matching weights this principle the biggest;
Step 7: according to following formula, calculate by substrate gaussian signal by one group of fixing matching weights be formed by stacking artificial
Signal gf(t),
Wherein φi(i ∈ [1, M]) is matching weights, is one group of fixed constant,
Afterbody that is i-th (i=m) the level substrate gaussian signal of this artificial signal of change composition is inclined within the specific limits
Shifting amount si, recalculate artificial signal, be further continued for cross correlation measure r calculating artificial signal with input signalf(τm):
rf(τm)=max (cov < mN(t),gf(t) >)=max (∑ mN(τ)gf(t+τ))
Find and make cross correlation measure rf(τm) maximum time side-play amount si, now adding this side-play amount is siSubstrate Gauss letter
Number time, artificial signal is the most similar to input signal, τmPoor for artificial signal during cross correlation measure maximum and position input signal;
Step 8: make m=m+1, repeats step 7, until m=M, has i.e. added afterbody substrate Gaussian function;
Step 9: when the symmetrical centre side-play amount of each substrate gaussian signal is respectively s1,s2,s3,…smTime, by these
The artificial signal that substrate gaussian signal combines and input signal have the highest similarity, make rf(τ) τ taking maximum is
Integral position is poor, the calculating optimal estimation p to central point:
Wherein λi(i ∈ [1, M]) is the Combining weights of the symmetrical centre of i-stage substrate gaussian signal, and this Combining weights is
One group of fixing constant, choosing of it should follow dilatability ziThe biggest, Combining weights this principle the biggest, uiFor each substrate Gauss
The symmetrical centre of signal, rziThe substrate gaussian signal of the variant dilatability obtained for step 5 and input signal maximum mutually
Pass is worth, rziThe highest, then comprising more dilatability in explanation input signal is ziThe composition of substrate gaussian signal, ηiFor revising
Proportionality constant, for reacting the significance level of the symmetrical centre of the Gaussian function of different dilatability;
Step 10: repetition step 2 is to step 9, until having calculated all XmaxThe central point of row, obtains laser lines
The optimal estimation of picture centre line.
The method of the present invention mainly uses one group of gaussian signal approximating method to former laser line image cross section.Pass through
Using the Gaussian function with different average and variance is basis function, by certain rule combination superposition, comes farthest
The distribution of the laser stripe image cross section that matching collects.When finding optimal fitting result, according to each gaussian signal
Symmetrical centre, extrapolates the optimal estimation to laser stripe center by certain rule.
Present invention advantage compared with prior art is: existing method major part assumes the cross section of laser line image
The distribution of pixel there is the character such as symmetry and homogeneity, and during actual acquisition, due to incident angle, object being measured
The problems such as refraction scattering that surface irregularity causes, image capture device noise, the pixel of the cross section of laser line image
Distribution is difficult to meet general symmetry and homogeneity.The distribution that the method for the present invention does not relies on the pixel of cross section is the fullest
Foot the two characteristic, is distributed by the pixel value using multiple gaussian signals of difference expectation and variance to carry out matching cross section, looks for
To when making cross correlation maximum, the relative position of each different gaussian signals, so that it is determined that the center of laser lines.Carry greatly
The computational accuracy of high centrage.
Accompanying drawing explanation
Fig. 1 is the inventive method flow chart.
Fig. 2 is the object being measured for test.
Fig. 3 is laser stripe image instance 1.
Fig. 4 is that certain a line pixel value of example 1 is distributed and to the input signal scattergram after its interpolation, gives simultaneously
Use the calculated initial center point of threshold method.
Fig. 5 be to this row pixel value of example 1 use two-stage gaussian signal matching time, the side-play amount of second level gaussian signal with
The graph of a relation of maximum cross-correlation coefficient.
Fig. 6 is the optimal result schematic diagram that this row pixel value of example 1 uses two-stage gaussian signal matching.
When Fig. 7 is that this row pixel value of example 1 is added third level gaussian signal matching, the side-play amount of third level gaussian signal
Graph of a relation with maximum cross-correlation coefficient.
Fig. 8 is the optimal result schematic diagram that this row pixel value of example 1 uses three grades of gaussian signal matchings.
Fig. 9 is the central line pick-up result figure to example 1.
Figure 10 is the difference of centrage result and the ideal situation using the inventive method to extract.
Figure 11 is to use the geometrical center method central line pick-up result figure to example 1.
Figure 12 is the difference of centrage result and the ideal situation using geometrical center method to extract.
Figure 13 is to use the inventive method to extract centrage testee carries out the top view of 3D reconstruction.
Figure 14 is to use geometrical center method to extract centrage testee carries out the top view of 3D reconstruction.
Detailed description of the invention
The present invention is described in detail in citing below in conjunction with the accompanying drawings.
The inventive method does not relies on the distribution of laser line image pixel value and has the requirement of higher-symmetry, by using
Multiple gaussian signals of different expectations and variance carry out the pixel value distribution of matching laser lines single file, find and make cross correlation maximum
Time, the relative position of each different gaussian signals, so that it is determined that the center of these row laser lines.Calculate laser line image institute
Having capable laser rays sliver transvers section central point, can try to achieve the centrage of laser line image, detailed process comprises the following steps:
(1) use 3D based on laser to measure systematic survey testee as shown in Figure 2, obtain laser line image sequence
In a certain image instance 1, as shown in Figure 3.
(2) in treating excess syndrome example 1, nth row of pixels value sequence, as initial data, for the ease of calculating, is first normalized place
Reason, as shown in circular hollow point in Fig. 4.Owing to initial data is the most sparse, in order to improve, step (7) calculates cross correlation measure
Accuracy, carries out interpolation operation to initial data, obtains the most intensive input signal, shown in as shown in lines in Fig. 4.
(3) use threshold method i.e. to the initial data after normalization, scope threshold value between 0.2 to 0.5 be set,
The pixel value that will be greater than this threshold value is labeled as 1, is labeled as 0 less than the pixel value of this threshold value, calculates pixel value and is labeled as the pixel of 1
The row coordinate average at some place, i.e. initial center point u0, as shown in Fig. 4 stellate point, and maximum column coordinate is sat with minimum row
Target difference, i.e. width w0。
(4) central point obtained according to step (3) and width, determine one group of M substrate gaussian signal for matching altogether,
It is shown below.
uiFor the symmetrical centre of i-stage gaussian signal, siFor the symmetrical centre of i-stage gaussian signal relative to initial center point
Side-play amount.σiFor the standard deviation of i-stage gaussian signal, definitionFor the dilatability of i-stage gaussian signal, and the first order
The dilatability of gaussian signal is determined by the width in step (3), and q is constant.
(5) the maximum cross-correlation coefficient of this group substrate gaussian signal and input signal is calculated:
(6) definition m have the Gaussian function of different dilatability and symmetrical centre according to one group fix matching weights
Signal after superposition is artificial signal gfX (), matching weights are one group of fixing constant, and it is chosen and should follow dilatability ziIt is the biggest,
Matching weights this principle the biggest.And set initial m=2, first order gaussian signal side-play amount s1=0.
(7) according to following formula, the artificial signal being formed by stacking by substrate gaussian signal is calculated by one group of fixing matching weights
gf(t)。
Wherein φi(i ∈ [1, M]) is matching weights, is one group of fixed constant.
With 0.1 pixel wide as step-length in certain limit (being 8 pixel unit width in this example), composition is altered in steps
Side-play amount s of the afterbody of this artificial signal that is i-th (i=m) level gaussian signali, calculate after often changing a side-play amount
Artificial signal and the cross correlation measure of input signal:
rf(τm)=max (cov < mN(t),gf(t) >)=max (∑ mN(τ)gf(t+τ)) (4)
Find and make cross correlation measure rf(τm) maximum time side-play amount si, now adding this side-play amount is siGaussian signal time,
Artificial signal is the most similar to input signal, and now τmPoor for artificial signal during cross correlation measure maximum and position input signal.
(8) make m=m+1, repeat step 7.Until m=M, i.e. add afterbody substrate Gaussian function.
When example 1 carrying out centrage and calculating, three grades of (i.e. M=3) different gaussian signals are used to carry out matching example 1 the
The pixel value distribution of N row, when Fig. 5 is m=2, changes side-play amount s of second level gaussian signal symmetrical centre2The artificial letter obtained
Number with the relation of the cross-correlation coefficient of input signal, this example is worked as s2When=-1.8, artificial signal and input signal have higher
Similarity.Fig. 6 is the optimal fitting result using first order gaussian signal to superpose with second level gaussian signal, and thick line is artificial
Signal, black thin is the input signal treating matching.When Fig. 7 is m=M=3, change the inclined of third level gaussian signal symmetrical centre
Shifting amount s3The artificial signal obtained and the relation of the cross-correlation coefficient of input signal, work as s in this example3When=1.1, artificial signal with
Input signal has higher similarity.Fig. 8 is the optimal fitting result making three grades of gaussian signal superpositions, and thick line is artificial letter
Number, black thin is the input signal treating matching.
From figure 8, it is seen that artificial signal and input signal have higher similarity.
(9) optimal estimation to central point is calculated:
Believe to input signal each Gauss time the most similar according to the artificial signal that makes that step (7) obtains to step (8)
Number symmetrical centre side-play amount si, calculate symmetrical centre u of each gaussian signali=u0+si.Calculate artificial signal and input again
The maximum cross-correlation coefficient r of signalf(τ) take displacement τ during maximum, calculate the optimum to central point finally according to formula (5)
Estimation p:
Wherein λiFor the weights of variant center of energy, this Combining weights is one group of fixing constant, and choosing of it should be abided by
Follow dilatability ziThe biggest, Combining weights this principle the biggest, riGaussian function for variant dilatability is similar to input signal
Degree, riThe highest, then comprising more dilatability in explanation input signal is ziThe composition of gaussian signal, ηiNormal for revising ratio
Number, for reacting the significance level of the center of energy of the Gaussian function of different dilatability.
In this example to the central point result of example 1 Nth row laser line image as shown in black * shape point in Fig. 8.
(10) repetition step (2) is to step (9), has calculated all XmaxThe central point of row, i.e. can obtain laser stripe figure
As the calculating of the centrage of example 1, result is as shown in Figure 9.Give the difference with ideal situation, as shown in Figure 10 simultaneously.
In order to contrast the effectiveness of the inventive method further, we use traditional geometrical center method to carry out example 1
Centrage calculates.Laser lines centrage result is as shown in figure 11.With ideal situation difference as shown in figure 12.Finally, we are right
All laser line image carry out central line pick-up, according to the parameter demarcated, testee as shown in Figure 2 are carried out three
Dimension is rebuild, and Figure 13 is that the inventive method calculates centrage the result rebuild.Figure 14 calculates centrage for using geometrical center method
And the result rebuild, in terms of reconstructed results, reconstructed results details based on the inventive method is clear, performance is abundant, has higher
Reduction degree.
Claims (1)
1. a laser stripe center line extraction method for the matching of gaussian signal more than, is characterized in that:
Step one: obtained the image I comprising laser lines by image capture device, the resolution of image I is Ymax×Xmax;
Step 2: set N (the N ∈ [1, X of image Imax]) row pixel value constitute sequence be initial data MN(j),(j∈[1,
Ymax]), obtain input signal m by a cube interpolation algorithmN(t), wherein t=nTs, TsIt is spaced for interpolation, N ∈ [1, Xmax],j∈
[1, Ymax];
Step 3: for the data after the laser lines pixel value normalization of the Nth row of image I, a scope is set and arrives 0.2
Threshold value between 0.5, when pixel value data are more than described threshold value, is labeled as 1 by this pixel, during less than described threshold value, then
It is labeled as 0;Calculate the average of row sequence number belonging to all pixels being labeled as 1, using this average as initial center point u0, simultaneously
Calculate the difference of pixel point range sequence number maxima and minima being labeled as 1, using this difference as initial width of fringe w0;
Step 4: build one group of M and there is different expectation and the substrate gaussian signal set G for matching of variance, in set
Length and input signal m of all substrate gaussian signalsNT () is identical, and set zi=2 σi 2, σiBelieve for i-stage substrate Gauss
Number standard deviation, and by ziThe dilatability of named i-stage substrate gaussian signal, order expectation ui=u0+si, and by uiName
For the symmetrical centre of i-stage substrate gaussian signal, wherein, u0For initial center point, siFor side-play amount;
Initial center point u that will obtain in step 30Symmetrical centre u as first order substrate gaussian signal0, i.e. u1=u0, just
Beginning width of fringe w0For determining the dilatability of first order substrate gaussian signalWherein q is constant, thus
To one group of M substrate gaussian signal set G with different dilatability,
In above formula, gzi,uiX () is i-stage substrate gaussian signal, and its dilatability is zi, symmetrical centre is ui;
Step 5: by calculating maximum cross-correlation coefficient, tries to achieve the similarity of each substrate gaussian signal and input signal:
Wherein, rzi(τi) it is the maximum cross-correlation value of input signal and i-stage substrate gaussian signal, τiIt is two signal cross correlation values
When taking maximum, the relative alternate position spike of two signals;
Step 6: define artificial signal gfX () is m the substrate Gaussian function with different dilatability and symmetrical centre, according to one
Signal after the matching weights superposition that group is fixing, and set initial m=2, matching weights are one group of fixing constant, its choosing
Take and should follow dilatability ziThe biggest, matching weights this principle the biggest;
Step 7: according to following formula, calculate the artificial signal g being formed by stacking by substrate gaussian signal by one group of fixing matching weightsf
(t),
Wherein φi(i ∈ [1, M]) is matching weights, is one group of fixed constant,
Change side-play amount s of afterbody that is i-th (i=m) the level substrate gaussian signal forming this artificial signali, recalculate people
Make signal, be further continued for cross correlation measure r calculating artificial signal with input signalf(τm):
rf(τm)=max (cov < mN(t), gf(t) >)=max (∑ mN(τ)gf(t+τ))
Find and make cross correlation measure rf(τm) maximum time side-play amount si, now adding this side-play amount is siSubstrate gaussian signal time,
Artificial signal is the most similar to input signal, τmPoor for artificial signal during cross correlation measure maximum and position input signal;
Step 8: make m=m+1, repeats step 7, until m=M, has i.e. added afterbody substrate Gaussian function;
Step 9: when the symmetrical centre side-play amount of each substrate gaussian signal is respectively s1, s2, s3... smTime, high by these substrates
The artificial signal that this signal combines and input signal have the highest similarity, make rf(τ) τ taking maximum is overall position
Put difference, the calculating optimal estimation p to central point:
Wherein λi(i ∈ [1, M]) is the Combining weights of the symmetrical centre of i-stage substrate gaussian signal, and this Combining weights is one group and consolidates
Fixed constant, choosing of it should follow dilatability ziThe biggest, Combining weights this principle the biggest, uiFor each substrate gaussian signal
Symmetrical centre, rziThe substrate gaussian signal of the variant dilatability obtained for step 5 and the maximum cross-correlation value of input signal,
rziThe highest, then comprising more dilatability in explanation input signal is ziThe composition of substrate gaussian signal, ηiFor revising ratio
Constant, for reacting the significance level of the symmetrical centre of the Gaussian function of different dilatability;
Step 10: repetition step 2 is to step 9, until having calculated all XmaxThe central point of row, obtains laser line image
The optimal estimation of centrage.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610487738.4A CN106097430B (en) | 2016-06-28 | 2016-06-28 | A kind of laser stripe center line extraction method of more gaussian signal fittings |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201610487738.4A CN106097430B (en) | 2016-06-28 | 2016-06-28 | A kind of laser stripe center line extraction method of more gaussian signal fittings |
Publications (2)
Publication Number | Publication Date |
---|---|
CN106097430A true CN106097430A (en) | 2016-11-09 |
CN106097430B CN106097430B (en) | 2018-10-26 |
Family
ID=57215004
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201610487738.4A Active CN106097430B (en) | 2016-06-28 | 2016-06-28 | A kind of laser stripe center line extraction method of more gaussian signal fittings |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN106097430B (en) |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107133565A (en) * | 2017-03-31 | 2017-09-05 | 大连理工大学 | Laser incising molded line feature extracting method based on line laser |
CN108564621A (en) * | 2018-04-28 | 2018-09-21 | 中国科学院电子学研究所 | Structured light strip center extraction method and device for rut detection |
CN108921936A (en) * | 2018-06-08 | 2018-11-30 | 上海大学 | A kind of underwater laser grating matching and stereo reconstruction method based on ligh field model |
CN110866924A (en) * | 2019-09-24 | 2020-03-06 | 重庆邮电大学 | Line structured light center line extraction method and storage medium |
CN112116619A (en) * | 2020-09-16 | 2020-12-22 | 昆明理工大学 | Multi-line structured light system stripe center line extraction method based on structural constraint |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101504770A (en) * | 2009-03-19 | 2009-08-12 | 北京航空航天大学 | Structural light strip center extraction method |
CN101986322A (en) * | 2010-11-22 | 2011-03-16 | 南京大学 | Structured light stripe central point reliability evaluation method |
CN104616325A (en) * | 2015-01-21 | 2015-05-13 | 大连理工大学 | Rapid and high-precision method for extracting light strip center on large surface |
CN104657587A (en) * | 2015-01-08 | 2015-05-27 | 华中科技大学 | Method for extracting center line of laser stripe |
-
2016
- 2016-06-28 CN CN201610487738.4A patent/CN106097430B/en active Active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101504770A (en) * | 2009-03-19 | 2009-08-12 | 北京航空航天大学 | Structural light strip center extraction method |
CN101986322A (en) * | 2010-11-22 | 2011-03-16 | 南京大学 | Structured light stripe central point reliability evaluation method |
CN104657587A (en) * | 2015-01-08 | 2015-05-27 | 华中科技大学 | Method for extracting center line of laser stripe |
CN104616325A (en) * | 2015-01-21 | 2015-05-13 | 大连理工大学 | Rapid and high-precision method for extracting light strip center on large surface |
Non-Patent Citations (3)
Title |
---|
田庆国等: "利用轮廓线多边形表示实时提取光带中心线", 《光学精密工程》 * |
陈瑞改等: "干涉条纹中心线提取与细化的新方法", 《激光杂志》 * |
高世一等: "变边限高斯拟合提取激光条纹中心线方法的研究", 《仪器仪表学报》 * |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107133565A (en) * | 2017-03-31 | 2017-09-05 | 大连理工大学 | Laser incising molded line feature extracting method based on line laser |
CN107133565B (en) * | 2017-03-31 | 2020-04-07 | 大连理工大学 | Line laser-based laser engraving line feature extraction method |
CN108564621A (en) * | 2018-04-28 | 2018-09-21 | 中国科学院电子学研究所 | Structured light strip center extraction method and device for rut detection |
CN108564621B (en) * | 2018-04-28 | 2021-09-24 | 中国科学院电子学研究所 | Structured light strip center extraction method and device for track detection |
CN108921936A (en) * | 2018-06-08 | 2018-11-30 | 上海大学 | A kind of underwater laser grating matching and stereo reconstruction method based on ligh field model |
CN110866924A (en) * | 2019-09-24 | 2020-03-06 | 重庆邮电大学 | Line structured light center line extraction method and storage medium |
CN110866924B (en) * | 2019-09-24 | 2023-04-07 | 重庆邮电大学 | Line structured light center line extraction method and storage medium |
CN112116619A (en) * | 2020-09-16 | 2020-12-22 | 昆明理工大学 | Multi-line structured light system stripe center line extraction method based on structural constraint |
Also Published As
Publication number | Publication date |
---|---|
CN106097430B (en) | 2018-10-26 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN106097430A (en) | A kind of laser stripe center line extraction method of many gaussian signals matching | |
CN103295239B (en) | A kind of autoegistration method of the laser point cloud data based on datum plane image | |
CN104101331B (en) | Based on the noncooperative target pose measurement of all-optical field camera | |
CN105354841B (en) | A kind of rapid remote sensing image matching method and system | |
CN103604417B (en) | The multi-view images bi-directional matching strategy that object space is information constrained | |
CN106595702B (en) | A kind of multisensor spatial registration method based on astronomy calibration | |
CN103778626B (en) | A kind of fast image registration method of view-based access control model marking area | |
CN101315698A (en) | Characteristic matching method based on straight line characteristic image registration | |
CN102446354A (en) | Integral registration method of high-precision multisource ground laser point clouds | |
CN103198475B (en) | Based on the total focus synthetic aperture perspective imaging method that multilevel iteration visualization is optimized | |
CN104834931A (en) | Improved SIFT algorithm based on wavelet transformation | |
CN105678757A (en) | Object displacement measurement method | |
CN112017248B (en) | 2D laser radar camera multi-frame single-step calibration method based on dotted line characteristics | |
CN103679701B (en) | Crystal pattern based on Support vector regression is as outline of straight line detection method | |
CN108765476A (en) | A kind of polarization image method for registering | |
CN109870106A (en) | A kind of building volume measurement method based on unmanned plane picture | |
CN109978957B (en) | Binocular system calibration method based on quantum behavior particle swarm | |
CN102789644B (en) | Novel camera calibration method based on two crossed straight lines | |
He et al. | IGICP: Intensity and Geometry Enhanced LiDAR Odometry | |
CN103605980B (en) | ISAR (inverse synthetic aperture radar) target component detection method based on local feature matching | |
CN107728196A (en) | Obtain the method and system of Angle Domain Common Image Gather | |
CN102999896B (en) | Method for linearly solving intrinsic parameters of camera by aid of three tangent circles | |
Yoshisada et al. | Indoor map generation from multiple LiDAR point clouds | |
CN104484647A (en) | High-resolution remote sensing image cloud height detection method | |
CN105066905B (en) | Wavelet transform profilometry noise restraint 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 |