CN108020179B - A kind of High-precision angle measuring device and method - Google Patents

A kind of High-precision angle measuring device and method Download PDF

Info

Publication number
CN108020179B
CN108020179B CN201711452067.9A CN201711452067A CN108020179B CN 108020179 B CN108020179 B CN 108020179B CN 201711452067 A CN201711452067 A CN 201711452067A CN 108020179 B CN108020179 B CN 108020179B
Authority
CN
China
Prior art keywords
beam splitter
measured
reflecting mirror
laser
angle
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.)
Active
Application number
CN201711452067.9A
Other languages
Chinese (zh)
Other versions
CN108020179A (en
Inventor
于东钰
黎高平
吴磊
桑鹏
阴万宏
李四维
吕春莉
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 institute of Applied Optics
Original Assignee
Xian institute of Applied Optics
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 institute of Applied Optics filed Critical Xian institute of Applied Optics
Priority to CN201711452067.9A priority Critical patent/CN108020179B/en
Publication of CN108020179A publication Critical patent/CN108020179A/en
Application granted granted Critical
Publication of CN108020179B publication Critical patent/CN108020179B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/26Measuring arrangements characterised by the use of optical techniques for measuring angles or tapers; for testing the alignment of axes

Abstract

The present invention proposes a kind of High-precision angle measuring device and method, and laser light source becomes after beam expanding lens and attenuator expands parallel laser;Parallel laser is expanded by the first beam splitter, reflecting mirror, third beam splitter, the 4th beam splitter, forms the first reference beam;Parallel laser is expanded by the first beam splitter, the second beam splitter, third beam splitter, the 4th beam splitter, forms the second reference beam;Parallel laser is expanded by the first beam splitter, the second beam splitter, reflecting mirror to be measured, the 4th beam splitter, forms light beam to be measured;First reference beam, the second reference beam, the light beam to be measured coherent superposition in CCD camera image planes generate interference pattern, and input picture processing system.Location information is carried out linear fit by measuring the location information of laser interference hot spot by the present invention, by calculating the variable quantity of linear distance, calculates the angle change of incident laser.Under identical measurement accuracy, this method avoid the rigors adjusted the distance, and provide a kind of method for the miniaturization of High-precision angle measuring device.

Description

A kind of High-precision angle measuring device and method
Technical field
The invention belongs to optical metrology fields, relate generally to the High-precision angle measuring device and method of small angle variation.
Background technique
With the development of technology, sub-micro arc angles measure, and it is in the urgent need to address to have become many high-quality precision and sophisticated technologies Major issue.Collimator method or four-quadrant method are now mostly used, it is high using collimator method measurement accuracy, but equipment is heavy, Environmental requirement is high, adjusts difficult.Such as measurement sub-micro arc angles objective focal length must reach 2m, need to occupy big quantity space.Four The high sensitivity of quadrant method position, it is assumed that reaching 4 quadrant detector distance from reflecting mirror is 2.5m, and the sensitivity of this method reaches To 1 μ rad.But since laser facula is not equally distributed rectangular light spot, the differential amplification output valve of four-quadrant and laser Facula position is in non-linear, and since non-gaussian stray light exists, four-quadrant method is not suitable for high-precision fixed measurement, and And the very difficult tune of initial position on laser reflection to 4 quadrant detector surface, it is inconvenient to use.
Foreign countries have delivered " Application of the Fourier in optical&Laser Technology in 2012 Analysis methods to the three beam interferometry " it proposes to utilize three interference of light of fourier analysis Method measures low-angle amount, is made of laser polarizing film beam splitter camera.Fu Li is carried out to the coherent image of formation Leaf analysis simultaneously is further calculated to obtain angle change to the result of analysis.Minimum 10um of camera pixel or so at this stage, Due to camera pixel can not accomplish it is infinitely small, so the space sampling frequency of image is relatively low to lead to the space that Fourier Tranform obtains Frequency accuracy is lower, so that the angular error calculated is big.
Summary of the invention
In order to solve the problems existing in the prior art, the present invention proposes a kind of High-precision angle measuring device and method, in reality The measurement accuracy for meeting sub-micro arc angles while miniaturization measuring device now, is suitable for on-the-spot test.
The technical solution of the present invention is as follows:
A kind of High-precision angle measuring device, it is characterised in that: including laser light source, beam expanding lens, attenuator, beam splitting Mirror, reflecting mirror, reflecting mirror to be measured, CCD camera and image processing system;
Laser light source becomes after beam expanding lens and attenuator expands parallel laser;
It expands parallel laser and passes through the first beam splitter 1, reflecting mirror, third beam splitter 3, the 4th beam splitter 4, the shape on camera At the first reference beam 1;
Parallel laser is expanded by the first beam splitter 1, the second beam splitter 2, third beam splitter 3, the 4th beam splitter 4, in phase The second reference beam 2 is formed on machine;
Parallel laser is expanded by the first beam splitter 1, the second beam splitter 2, reflecting mirror to be measured, the 4th beam splitter 4, in camera It is upper to form light beam to be measured;
First reference beam 1, the second reference beam 2, the light beam to be measured coherent superposition in CCD camera image planes generate interference Figure, and input picture processing system.
Further preferred embodiment, a kind of High-precision angle measuring device, it is characterised in that: each beam splitter with enter Irradiating light beam angle at 45 °, reflecting mirror and incident beam angle are not equal to 45 °, and reflecting mirror to be measured and incident beam institute are at folder Angle is not equal to 45 °.
Further preferred embodiment, a kind of High-precision angle measuring device, it is characterised in that: reflecting mirror and incident light Beam angle is not equal to 45 ° in 45 ° of ± 10 ' range;Reflecting mirror to be measured and incident beam angle are at 45 ° ± 10 ' In range, and it is not equal to 45 °.
First reference beam 1, the second reference beam 2, the light beam to be measured coherent superposition in CCD camera image planes generate interference pattern Shown in 2, the second reference beam 2 and light beam to be measured or the first reference beam 1 and light beam to be measured, the interference pattern formed on CCD is such as Shown in Fig. 3.The center-of-mass coordinate that all hot spots in interference pattern 2 are found out using centroid method is carried out linear by the stripe direction of interference pattern 3 Fitting calculates the vertical range between adjacent two straight lines, and then can accurately calculate the angle change of plane mirror to be measured.
Based on the above principles, using above-mentioned measuring device, the method for carrying out High-precision angle measurement, it is characterised in that: packet Include following steps:
Step 1: lighting laser light source, open CCD camera and image processing system;Fixed reflecting mirror to be measured, passes through adjusting First beam splitter 1, the second beam splitter 2, third beam splitter 3, the 4th beam splitter 4, reflecting mirror join the first reference beam 1, second It examines light beam 2, light beam to be measured and generates interference the first plaque-like interference pattern 1 of formation on CCD;
Step 2: low-angle offset occurs for reflecting mirror to be measured, and other elements are motionless, obtains the first reference beam 1, second ginseng It examines light beam 2, light beam to be measured and generates interference the second plaque-like interference pattern 2 of formation on CCD;
Step 3: covering reference beam all the way, the speckle pattern interferometry that another way reference beam and light beam to be measured are formed on CCD Fig. 3;
Step 4: the center-of-mass coordinate of all hot spots in the first plaque-like interference pattern 1 of step 1 generation is found out using centroid method (x1i、y1i) and step 2 generate the second plaque-like interference pattern 2 in all hot spots center-of-mass coordinate (x2i、y2i);
Step 5: according to the stripe direction for speckle pattern interferometry Fig. 3 that step 3 generates, to corresponding in the first plaque-like interference pattern 1 The center-of-mass coordinate of same striped carries out linear fit, obtains several straight lines, and calculates being averaged for distance between adjacent two straight lines Value Da;Linear fit is carried out to the center-of-mass coordinate for corresponding to same striped in the second plaque-like interference pattern 2, obtains several straight lines, and Calculate the average value D of distance between adjacent two straight linesb
Step 6: the angle change of reflecting mirror to be measured in step 2 is calculated as follows:
Step 6.1: calculate spatial frequency variation value:Wherein γ is pixel dimension;
Step 6.2: calculation value: Δ β=Δ f λ, wherein λ is optical maser wavelength used.
Beneficial effect
Location information is carried out linear fit by measuring the location information of laser interference hot spot by the present invention, passes through meter The variable quantity for calculating linear distance, cleverly calculates the angle change of incident laser.Under identical measurement accuracy, compared to using Light pipe method measurement angle, this method avoid the rigors adjusted the distance, and provide one for the miniaturization of High-precision angle measuring device Kind method.
Detailed description of the invention
A kind of measurement method schematic diagram of High-precision angle measurement of Fig. 1.
The three beams of laser interference pattern of Fig. 2 High-precision angle measurement.
Two beam laser interference figures in the measurement of Fig. 3 High-precision angle.
Specific embodiment
In order to further disclose the present invention, with reference to the accompanying drawing and preferred embodiment the invention will be further described.
As shown in Figure 1, the measurement method that the High-precision angle in the present embodiment measures includes laser light source, beam expanding lens, declines Subtract piece, beam splitter, reflecting mirror, reflecting mirror to be measured, CCD and image recording and processing system;Reflecting mirror to be measured is installed on angled In the equipment of variation;Three laser beams formed by each beam splitter and reflecting mirror are almost parallel, are ultimately incident upon CCD camera On.
As shown in Figure 1,632.8nm laser light source is placed in front of beam expanding lens, the position of beam expanding lens and laser is adjusted It is set to export approximate planar light.Attenuator is placed behind the light source at 10mm, each beam splitter and reflecting mirror riding position are such as Shown in Fig. 1, each mirror is almost parallel and is spaced apart from each other 50cm.Adjust laser, beam expanding lens, beam splitter, reflecting mirror CCD camera shooting Relative altitude between machine makes three's common optical axis.CCD camera is connected with image recording with processing system.
High-precision angle measuring process is carried out using above-mentioned apparatus are as follows:
Step 1: lighting laser light source, open CCD camera and image processing system;Fixed reflecting mirror to be measured, passes through adjusting First beam splitter 1, the second beam splitter 2, third beam splitter 3, the 4th beam splitter 4, reflecting mirror join the first reference beam 1, second It examines light beam 2, light beam to be measured and generates interference the first plaque-like interference pattern 1 of formation on CCD;
Step 2: low-angle offset occurs for reflecting mirror to be measured, and other elements are motionless, obtains the first reference beam 1, second ginseng It examines light beam 2, light beam to be measured and generates interference the second plaque-like interference pattern 2 of formation on CCD;
Step 3: covering reference beam all the way, the speckle pattern interferometry that another way reference beam and light beam to be measured are formed on CCD Fig. 3;
Step 4: the center-of-mass coordinate of all hot spots in the first plaque-like interference pattern 1 of step 1 generation is found out using centroid method (x1i、y1i) and step 2 generate the second plaque-like interference pattern 2 in all hot spots center-of-mass coordinate (x2i、y2i);
Step 5: according to the stripe direction for speckle pattern interferometry Fig. 3 that step 3 generates, to corresponding in the first plaque-like interference pattern 1 The center-of-mass coordinate of same striped carries out linear fit, obtains straight line la1:ya1=kxa1+ca1、la2:ya2=kxa2+ca2、la3:ya3= kxa3+ca3... .., and calculate the average value D of distance between adjacent two straight linesa;It is same to corresponding in the second plaque-like interference pattern 2 The center-of-mass coordinate of striped carries out linear fit, obtains straight line Lb1:yb1=Kxb1+cb1、Lb2:yb2=Kxb2+cb2、Lb3:yb3=Kxb3 +cb3... .., and calculate the average value D of distance between adjacent two straight linesb
Step 6: the angle change of reflecting mirror to be measured in step 2 is calculated as follows:
Step 6.1: calculate spatial frequency variation value:Wherein γ is pixel dimension;
Step 6.2: calculation value: Δ β=Δ f λ, wherein λ is optical maser wavelength 632.8nm used.
The present invention obtains variable quantity to low-angle using the method that three beams of laser is interfered and measures, and finds out interference by calculating Facula mass center carries out linear fit according to specific direction, calculates finally by the variation of the distance between adjacent two straight line to be measured The angle change of reflecting mirror.This method has the characteristics that occupy little space, method is simple, measurement accuracy is high, application prospect is wide.

Claims (4)

1. a kind of High-precision angle measuring device, it is characterised in that: including laser light source, beam expanding lens, attenuator, beam splitter, anti- Penetrate mirror, reflecting mirror to be measured, CCD camera and image processing system;
Laser light source becomes after beam expanding lens and attenuator expands parallel laser;
Parallel laser is expanded by the first beam splitter, reflecting mirror, third beam splitter, the 4th beam splitter, forms the first reference beam;
Parallel laser is expanded by the first beam splitter, the second beam splitter, third beam splitter, the 4th beam splitter, forms the second reference Light beam;
Parallel laser is expanded by the first beam splitter, the second beam splitter, reflecting mirror to be measured, the 4th beam splitter, forms light beam to be measured;
In a stage of measurement process, the first reference beam, the second reference beam, the light beam to be measured phase in CCD camera image planes Dry superposition generates interference pattern, and input picture processing system;In another stage of measurement process, the first reference beam or the second ginseng It examines light beam and the light beam to be measured coherent superposition in CCD camera image planes and generates interference pattern, and input picture processing system.
2. a kind of High-precision angle measuring device according to claim 1, it is characterised in that: each beam splitter and incident beam Angle at 45 °, reflecting mirror and incident beam angle are not equal to 45 °, and reflecting mirror to be measured and incident beam angle differ In 45 °.
3. a kind of High-precision angle measuring device according to claim 2, it is characterised in that: reflecting mirror and incident beam institute at Angle is not equal to 45 ° in 45 ° of ± 10 ' range;Reflecting mirror to be measured and incident beam angle are in 45 ° of ± 10 ' range It is interior, and it is not equal to 45 °.
4. using measuring device described in claim 1, the method for progress High-precision angle measurement, it is characterised in that: including following Step:
Step 1: lighting laser light source, open CCD camera and image processing system;Fixed reflecting mirror to be measured, by adjusting first Beam splitter, the second beam splitter, third beam splitter, the 4th beam splitter, reflecting mirror make the first reference beam, the second reference beam, to It surveys light beam and generates interference the first plaque-like interference pattern of formation on CCD;
Step 2: low-angle offset occurs for reflecting mirror to be measured, and other elements are motionless, obtain the first reference beam, the second reference light Beam, light beam to be measured generate interference on CCD and form the second plaque-like interference pattern;
Step 3: covering reference beam all the way, the interference fringe that another way reference beam and light beam to be measured are formed on CCD;
Step 4: the center-of-mass coordinate (x of all hot spots in the first plaque-like interference pattern of step 1 generation is found out using centroid method1i、y1i), And step 2 generate the second plaque-like interference pattern in all hot spots center-of-mass coordinate (x2i、y2i);
Step 5: according to step 3 generate interference fringe stripe direction, in the first plaque-like interference pattern correspond to same The center-of-mass coordinate of line carries out linear fit, obtains several straight lines, and calculate the average value D of distance between adjacent two straight linesa;It is right Linear fit is carried out corresponding to the center-of-mass coordinate of same striped in second plaque-like interference pattern, obtains several straight lines, and calculate adjacent The average value D of distance between two straight linesb
Step 6: the angle change of reflecting mirror to be measured in step 2 is calculated as follows:
Step 6.1: calculate spatial frequency variation value:Wherein γ is pixel dimension;
Step 6.2: calculation value: Δ β=Δ f λ, wherein λ is optical maser wavelength used.
CN201711452067.9A 2017-12-28 2017-12-28 A kind of High-precision angle measuring device and method Active CN108020179B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201711452067.9A CN108020179B (en) 2017-12-28 2017-12-28 A kind of High-precision angle measuring device and method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201711452067.9A CN108020179B (en) 2017-12-28 2017-12-28 A kind of High-precision angle measuring device and method

Publications (2)

Publication Number Publication Date
CN108020179A CN108020179A (en) 2018-05-11
CN108020179B true CN108020179B (en) 2019-11-05

Family

ID=62071935

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201711452067.9A Active CN108020179B (en) 2017-12-28 2017-12-28 A kind of High-precision angle measuring device and method

Country Status (1)

Country Link
CN (1) CN108020179B (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102018126544A1 (en) * 2018-10-24 2020-04-30 MAX-PLANCK-Gesellschaft zur Förderung der Wissenschaften e.V. Method and device for detecting changes in direction of a light beam
CN110631510B (en) * 2019-09-12 2020-07-31 中国科学院西安光学精密机械研究所 High-precision angle measuring device and method based on Michelson structure
CN110673334B (en) * 2019-09-29 2021-08-13 中国科学院空间应用工程与技术中心 Automatic light beam transmission stabilizing system and method
CN111006582B (en) * 2019-12-06 2021-09-07 中国科学院光电技术研究所 Interference phase shift sensitivity enhancing method based on moire fringes
CN112611340B (en) * 2020-11-19 2022-04-01 易思维(杭州)科技有限公司 Method for adjusting laser light plane in vision sensor
CN113654656B (en) * 2021-10-18 2022-02-11 之江实验室 Light beam drift detection device and method based on three-light-beam interference
CN114370935A (en) * 2022-01-10 2022-04-19 中国人民解放军63892部队 CCD target surface laser energy distribution measuring system and method based on image fusion

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN2099299U (en) * 1991-08-30 1992-03-18 华中理工大学 Non-contact type ultra-precise surface measuring equipment
US6525821B1 (en) * 1997-06-11 2003-02-25 Ut-Battelle, L.L.C. Acquisition and replay systems for direct-to-digital holography and holovision
US6563592B2 (en) * 2001-03-19 2003-05-13 The United States Of America As Represented By The Secretary Of The Army Interferometric alignment device
FR2978824B1 (en) * 2011-08-05 2014-03-21 Thales Sa INTERFEROMETER POSTURE DETECTION SYSTEM
CN102944989B (en) * 2012-10-23 2015-07-01 深圳大学 Phase-shift digital holographic high-speed imaging method and system
KR101948912B1 (en) * 2014-07-09 2019-02-15 에이에스엠엘 네델란즈 비.브이. Inspection apparatus, inspection method and device manufacturing method
CN105698710B (en) * 2016-01-28 2017-05-10 襄阳宏伟航空器有限责任公司 A dynamic angle measurement apparatus and application thereof

Also Published As

Publication number Publication date
CN108020179A (en) 2018-05-11

Similar Documents

Publication Publication Date Title
CN108020179B (en) A kind of High-precision angle measuring device and method
CN106840027B (en) The astigmatic compensation type interference checking device and detection method of freeform optics surface
Kemao Applications of windowed Fourier fringe analysis in optical measurement: a review
CN108061639B (en) A kind of Larger Dynamic range of combining adaptive optical technology, high-precision phase position difference method wavefront measurement instrument
CN104655051B (en) A kind of high-speed structures light 3 d shape vertical measurement method
CN101788263B (en) Coaxial Fizeau synchronous phase shifting interferometer capable of adjusting extended light illumination
CN104949630B (en) A kind of adjustable point-diffraction interference device of large-numerical aperture fringe contrast
CN105466359B (en) A kind of precision surface type measurement device
JP7082137B2 (en) Radius of curvature measurement by spectral control interferometry
JP6553967B2 (en) Instantaneous phase shift interferometer
CN110017794B (en) Dynamic phase deformation interference measurement device and method
CN114008405A (en) Apparatus and method for measuring interface of optical element
CN101324421A (en) Synchronous phase-shift fiso interferometer
CN104713494B (en) The dual wavelength tuning interference testing device and method of Fourier transformation phase shift calibration
CN105318847A (en) Aspheric non-zero digit circular subaperture stitching method based on system modeling
CN109668526B (en) High-precision inclination angle measuring method based on optical transfer function
WO2018000943A1 (en) Method and apparatus for detecting concave cylindrical surfaces and cylindrical diverging lenses
CN105890538A (en) Three-surface interference type high-accuracy curved surface profile measuring system and method
Nguyen et al. Real-time 3D measurement of freeform surfaces by dynamic deflectometry based on diagonal spatial carrier-frequency pattern projection
CN201251428Y (en) Synchronous phase-shifting fizeau interferometer
CN102589472A (en) Method for highly precisely eliminating adjustment error in spherical surface shape interference detection
Chatterjee et al. Measurement of residual wedge angle with a reversal shear interferometer
Disawal et al. Measurement of displacement using phase shifted wedge plate lateral shearing interferometry
CN111220971B (en) Method for measuring absolute distance with high precision without being influenced by inclination angle
CN106338261A (en) Angle deviation calibration method between two interferometer emergence plane wave light beams

Legal Events

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