CN107121095A - A kind of method and device of accurate measurement super-large curvature radius - Google Patents

A kind of method and device of accurate measurement super-large curvature radius Download PDF

Info

Publication number
CN107121095A
CN107121095A CN201710427891.2A CN201710427891A CN107121095A CN 107121095 A CN107121095 A CN 107121095A CN 201710427891 A CN201710427891 A CN 201710427891A CN 107121095 A CN107121095 A CN 107121095A
Authority
CN
China
Prior art keywords
mrow
grating
mfrac
moire fringe
high precision
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
CN201710427891.2A
Other languages
Chinese (zh)
Other versions
CN107121095B (en
Inventor
侯昌伦
辛青
藏月
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.)
Hangzhou Dianzi University
Hangzhou Electronic Science and Technology University
Original Assignee
Hangzhou Electronic Science and Technology 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 Hangzhou Electronic Science and Technology University filed Critical Hangzhou Electronic Science and Technology University
Priority to CN201710427891.2A priority Critical patent/CN107121095B/en
Publication of CN107121095A publication Critical patent/CN107121095A/en
Application granted granted Critical
Publication of CN107121095B publication Critical patent/CN107121095B/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
    • G01B11/24Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures
    • G01B11/255Measuring arrangements characterised by the use of optical techniques for measuring contours or curvatures for measuring radius of curvature

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)

Abstract

The invention discloses a kind of device and method of accurate measurement super-large curvature radius, the device includes:Detected element, light source;Spectroscope, inclination is placed between detected element and light source, and the illumination for light source to be sent is mapped to detected element surface, on the reflected light back that detected element is reflected to the first grating and the second grating;First grating and the second grating;For the Taibo picture and the second grating formation Moire fringe that under the irradiation of reflected parallel light, the first grating is produced at the second grating;Imaging system;For gathering Moire fringe image, and transmit it to computer;Computer;The angle of Moire fringe is determined for handling Moire fringe image, and then calculates the radius of curvature for obtaining detected element.The apparatus structure is simple, and can realize the accurate measurement to optical element super-large curvature radius.

Description

A kind of method and device of accurate measurement super-large curvature radius
Technical field
The invention belongs to optical element radius of curvature measurement field, more particularly to a kind of accurate measurement super-large curvature radius Method and device.
Background technology
Optical elements of large caliber system is large-scale high power laser system, such as domestic IC F laser drivers, American National point The thousands of all kinds of optics that must be used in fiery device (NIF) and French megajoule laser engineering (Mega-Joule Project) Element.Only more than 400 × 500 all kinds of bore optical elements just have 8000, wherein for space filtering and the focal length focused on Just there are 1000 or so away from lens combination, therefore effective parameter inspection must be carried out for these large-aperture long-focus optical systems Survey.Also it is big in U.S. LIGO (laser interferometer Gravitational Wave Observatory) system Amount uses bigbore optical element.
Optical elements of large caliber is dry due to bore big (more than 250mm), radius of curvature big (being more than 10 meters), air agitation etc. The factor of disturbing has a strong impact on the precision of test.The spherometer of existing curvature radius measurement method such as contact, from imaging curvature half Cable diameter gauge and use principle of interference radius of curvature measurement instrument can be realized high-precision to small radius of curvature (being less than 10 meters) Measurement.But be difficult to obtain high-precision using traditional radius measurement means for super-large curvature radius (being more than 5000m) How measurement, realize that the high-precision measurement to this kind of a large amount of use elements has great importance to these major projects.
Accordingly, it would be desirable to develop a kind of detecting instrument for being capable of accurate super-large curvature radius, there is provided to laser fusion, gravitation The accurate measurement instrument device of optical element in the country such as wave measurement large project, as lens from processing each operation to final The detection foundation and standard of qualified examination, to meet the requirement to these optical element quality.
The content of the invention
The problem of in order to solve to be difficult to measurement optical element super-large curvature radius in the prior art, the present invention is proposed A kind of method and device of accurate measurement super-large curvature radius.The apparatus structure is simple, and can realize bent to optical element super large The accurate measurement of rate radius.
First aspect present invention proposes a kind of device of accurate measurement super-large curvature radius, including;
Detected element, light source;
Spectroscope, inclination is placed between detected element and light source, and the illumination for light source to be sent is mapped to detected element table On face, the reflected light back that detected element is reflected to the first grating and the second grating;
First grating and the second grating;For under the irradiation of reflected parallel light, the first grating to be produced at the second grating Taibo picture and the second grating formation Moire fringe;
Imaging system;For gathering Moire fringe image, and transmit it to computer;
Computer;The angle of Moire fringe is determined for handling Moire fringe image, and then calculating obtains detected element Radius of curvature.
Preferably, the device that first aspect present invention is provided also includes:Between spectroscope and light source and for inciting somebody to action The transmitting light that light source is sent becomes the collimation lens of directional light.When light source is nearer from detected element, collimation lens is arranged at Between light source and spectroscope, diverging light can be become directional light.
Preferably, the device that first aspect present invention is provided also includes:For adjusting the pin hole in light emission direction, using The first high precision displacement platform in fixed laser and pin hole, the second high accuracy for fixing the second grating and imaging system Displacement platform and the high precision displacement drive for driving the first high precision displacement platform and the movement of the second high precision displacement platform Dynamic device.
The laser and pin hole being fixed on the first high precision displacement platform, under the driving of high precision displacement driver, Different positions can be accurately moved to, by repeatedly measuring the combination power value under different light source positions, and then are solved The radius of curvature of detected element is calculated, the influence of the collimation of illuminating bundle so can be effectively eliminated.
To prevent influence of the air draught to measurement, preferably, whole device is sealed with cover.
Second aspect of the present invention provides a kind of accurate measurement super-large curvature radius of application first aspect offer system Method, is specifically included:
(1) accurate measurement super-large curvature radius system is demarcated due to tested focal length value for from first block of grating to The distance of focus, by accurately moving measured lens along optical axis, can obtain the accurate standard mirror of multigroup focal length, realize multisystem Accurate Calibration;
(2) the first high precision displacement platform is driven to be moved to corresponding position using high precision displacement driver, it is to avoid to shine The influence of the collimation of Mingguang City's beam;
(3) the second high precision displacement platform is driven to be moved to corresponding position using high precision displacement driver, record the The distance between one grating and the second grating z, the first grating and the second grating grid line angle theta;
(4) Moire fringe image is gathered using imaging system, and Moire fringe image is transmitted to computer;
(5) computer is handled receiving moiré topography picture, determines the angle [alpha] of Moire fringe, and calculating is obtained The radius of curvature Δ r of detected element;
Wherein, s is the distance between the first grating and detected element optical axis, and r is the radius of detected element, and its value is:
For the cycle P of the first grating1With the cycle P of the second grating2Ratio;
The calculation formula of the angle [alpha] of Moire fringe is:
P′1For the cycle of Taibo picture, according to the enlargement ratio relation of Taibo pictureObtain;
Δ z is z uncertainty, and Δ s is s uncertainty, and Δ θ is θ uncertainty, and Δ α is α uncertainty, Δ β is β uncertainty.
Preferably, uncertainty Δ z is obtained with uncertainty Δ s by high-precision optical grating ruler measurement, its value is respectively reached 0.1mm and 0.01mm.
Preferably, uncertainty Δ α acquisition methods are:Due to the angle that α is the Moire fringe that computer is calculated, Using the black and white strip pattern with the angle accurately determined of a precise Printing, adopted by the image of multiple measuring system Collecting system obtains the image of pattern and calculated with the method for Moire fringe angle calculation, obtains α uncertainty Δ α, its Value reaches 0.003 °.
Uncertainty Δ θ acquisition methods are:When tested reflecting surface is plane, while the grid line angle of two blocks of gratings is At 0 degree, the cycle of Morie fringe is infinitely great (image collected is uniform gray-scale map) in theory, with this as the starting point, is led to The turntable for crossing precision controls the angle of grid line between two blocks of gratings, and the uncertainty of grid line angle is determined by precision rotation platform, It is possible thereby to obtain θ uncertainty Δ θ, its value reaches 0.003 °.
Preferably, uncertainty Δ β acquisition methods are:Due to ratios of the β for the cycle of two gratings, pass through scanning The accurate measurement of Electronic Speculum, can accurately obtain β uncertainty Δ β, and its value is 0.00001.
The device of accurate measurement super-large curvature radius of the invention, is combined with most basic optical gauge, simple in construction, Cost is low, and simple to operate during measurement, can realize the accurate measurement to optical element super-large curvature radius.
Brief description of the drawings
Fig. 1 is first structural representation of the device for the accurate measurement super-large curvature radius applied in embodiment 1;
Fig. 2 is second structural representation of the device for the accurate measurement super-large curvature radius applied in embodiment 1;
Fig. 3 is that device in embodiment 2 shown in application drawing 1 enters and repeatedly measures the tested radius of resolving by the mobile light source of precision Schematic diagram;
Fig. 4 is that device in embodiment 2 shown in application drawing 2 enters and repeatedly measures the tested radius of resolving by the mobile light source of precision Schematic diagram.
Embodiment
In order to more specifically describe the present invention, below in conjunction with the accompanying drawings and embodiment is to technical scheme It is described in detail.
Embodiment 1
As shown in figure 1, the device of the accurate measurement super-large curvature radius of the present embodiment application includes:Radius is 5000m Detected element, infrared laser, the microcobjective for playing collimating effect, imaging len, pin hole, the cycle ratio of a light splitting are 1.004018 grating 1 and grating 2, CCD, frosted glass plate, computer and the high precision displacement driver for supporting grating 2, it is red Outer laser is fixed on high precision displacement platform one with pin hole, and grating 2, frosted glass plate and CCD are fixed on high precision displacement On platform two.
After terminating to accurate measurement super-large curvature radius system calibrating;
First, the first high precision displacement platform is driven to be moved to corresponding position using high precision displacement driver, it is to avoid The influence of the collimation of illuminating bundle;
Then, drive the second high precision displacement platform to be moved to corresponding position using high precision displacement driver, record The grid line angle theta that the distance between first grating and the second grating z are 10m, the first grating and the second grating is 0.3 °;
Next, gathering Moire fringe image using imaging system, and Moire fringe image is transmitted to computer;
Finally, computer is handled receiving moiré topography picture, and the angle [alpha] for determining Moire fringe is 37.4813 °, and calculate and obtain the radius of curvature of detected element and be:
Δ r=2*0.1mm (Δ z)+2*0.01mm (Δ s)+24.89m (Δ z)+3.11m (Δ β)+20.67m (Δ θ)+ 0.135m (Δ α)=48.80522m
Relative measurement error is:
It can be seen that Δ z, Δ θ, Δ β influence very big to measurement accuracy from above-mentioned analysis.If can reduce Δ z (makes 10 meters of measurement distance uncertainty is less than 0.1mm, strictly controlled environment factor such as temperature humidity, using Reneshaw grating scales Precision can further be improved).According to the radius of specific measuring cell, further optimization initial parameter is set, such as grating grid Angle, the parameter such as screen periods ratio, can also further improve measurement accuracy.
The present embodiment can be carried out with the structure shown in application drawing 2 in the measurement of detected element radius, Fig. 2, do not collimated Lens, and serve light splitting for spectroscope.
Embodiment 2
Using the system described in Fig. 1, by the position of accurate movement light source, take multiple measurements under the light source position of difference Combination power value, principle schematic is as shown in Figure 3.
Because the light that laser is sent is constantly present certain focal power after colimated light system, it is impossible to accomplish preferably Directional light.Assuming that this focal power isThe focal length for the tested surface that tested radius is R is R/2, then combines focal powerFor:
Wherein d is the distance between colimated light system equivalent lens and measured lens.
Test system initial position is debugged, and light source is placed near collimation lens focal length.Measured lens are put Put in measurement position, gather Moire fringe, measure the angle of Moire fringe and calculate measured value R now1;Accurately to reach Dynamic light source δ1, Moire fringe image is gathered, measured value R now is calculated2;Continue accurate forward movement light source δ2, identical behaviour Make, gather Moire fringe image, measured value R3 now is calculated by computer.
According to set imaging formula, Wo Menyou:
U expression things are away from v1、v2、v3The image distance under three kinds of states is represented, by above-mentioned various calculating, measured lens are obtained Radius R.
The present embodiment can be taken multiple measurements not with position of the structure shown in application drawing 2 by accurate movement light source With the combination power value under spot light position, principle schematic is as shown in Figure 4.
Technical scheme and beneficial effect are described in detail above-described embodiment, Ying Li Solution is to the foregoing is only presently most preferred embodiment of the invention, is not intended to limit the invention, all principle models in the present invention Interior done any modification, supplement and equivalent substitution etc. are enclosed, be should be included in the scope of the protection.

Claims (4)

1. a kind of device of accurate measurement super-large curvature radius, it is characterised in that including;
Detected element, light source;
Spectroscope, inclination is placed between detected element and light source, and the illumination for light source to be sent is mapped to detected element surface, will The reflected light back of detected element reflection is on the first grating and the second grating;
First grating and the second grating;For under the irradiation of reflected parallel light, the Thailand that the first grating is produced at the second grating Uncle with the second grating as forming Moire fringe;
Imaging system;For gathering Moire fringe image, and transmit it to computer;
Computer;The angle of Moire fringe is determined for handling Moire fringe image, and then calculates the curvature for obtaining detected element Radius.
2. the device of accurate measurement super-large curvature radius as claimed in claim 1, it is characterised in that described device is also wrapped Include:Transmitting light between spectroscope and light source and for light source to be sent becomes the collimation lens of directional light.
3. the device of accurate measurement super-large curvature radius as claimed in claim 1, it is characterised in that described device is also wrapped Include:For adjusting the pin hole in light emission direction, the first high precision displacement platform for fixed laser and pin hole, for solid Second high precision displacement platform of fixed second grating and imaging system and for driving the first high precision displacement platform and second The high precision displacement driver of high precision displacement platform movement.
4. a kind of method of the accurate measurement super-large curvature radius of system described in application claim 1 or 3, is specifically included:
(1) accurate measurement super-large curvature radius system is demarcated, because tested focal length value is from first block of grating to Jiao The distance of point, by accurately moving measured lens along optical axis, can obtain the accurate standard mirror of multigroup focal length, realize multisystem Accurate Calibration;
(2) the first high precision displacement platform is driven to be moved to corresponding position using high precision displacement driver, it is to avoid illumination light The influence of the collimation of beam;
(3) drive the second high precision displacement platform to be moved to corresponding position using high precision displacement driver, record the first light The distance between grid and the second grating z, the first grating and the second grating grid line angle theta;
(4) Moire fringe image is gathered using imaging system, and Moire fringe image is transmitted to computer;
(5) computer is handled receiving moiré topography picture, determines the angle [alpha] of Moire fringe, and calculating is tested The radius of curvature Δ r of element;
<mrow> <mi>&amp;Delta;</mi> <mi>r</mi> <mo>=</mo> <msqrt> <mrow> <msup> <mrow> <mo>(</mo> <mfrac> <mrow> <mo>&amp;part;</mo> <mi>r</mi> </mrow> <mrow> <mo>&amp;part;</mo> <mi>z</mi> </mrow> </mfrac> <mo>&amp;CenterDot;</mo> <mi>&amp;Delta;</mi> <mi>z</mi> <mo>)</mo> </mrow> <mn>2</mn> </msup> <mo>+</mo> <msup> <mrow> <mo>(</mo> <mfrac> <mrow> <mo>&amp;part;</mo> <mi>r</mi> </mrow> <mrow> <mo>&amp;part;</mo> <mi>&amp;beta;</mi> </mrow> </mfrac> <mo>&amp;CenterDot;</mo> <mi>&amp;Delta;</mi> <mi>&amp;beta;</mi> <mo>)</mo> </mrow> <mn>2</mn> </msup> <mo>+</mo> <msup> <mrow> <mo>(</mo> <mfrac> <mrow> <mo>&amp;part;</mo> <mi>r</mi> </mrow> <mrow> <mo>&amp;part;</mo> <mi>&amp;alpha;</mi> </mrow> </mfrac> <mo>&amp;CenterDot;</mo> <mi>&amp;Delta;</mi> <mi>&amp;alpha;</mi> <mo>)</mo> </mrow> <mn>2</mn> </msup> <mo>+</mo> <msup> <mrow> <mo>(</mo> <mfrac> <mrow> <mo>&amp;part;</mo> <mi>r</mi> </mrow> <mrow> <mo>&amp;part;</mo> <mi>&amp;theta;</mi> </mrow> </mfrac> <mo>&amp;CenterDot;</mo> <mi>&amp;Delta;</mi> <mi>&amp;theta;</mi> <mo>)</mo> </mrow> <mn>2</mn> </msup> <mo>+</mo> <msup> <mrow> <mo>(</mo> <mfrac> <mrow> <mo>&amp;part;</mo> <mi>r</mi> </mrow> <mrow> <mo>&amp;part;</mo> <mi>s</mi> </mrow> </mfrac> <mo>&amp;CenterDot;</mo> <mi>&amp;Delta;</mi> <mi>s</mi> <mo>)</mo> </mrow> <mn>2</mn> </msup> </mrow> </msqrt> </mrow>
Wherein, s is the distance between the first grating and detected element optical axis, and r is the radius of detected element, and its value is:
<mrow> <mi>r</mi> <mo>=</mo> <mfrac> <mrow> <mn>2</mn> <mi>z</mi> </mrow> <mrow> <mi>&amp;beta;</mi> <mi>t</mi> <mi>a</mi> <mi>n</mi> <mi>&amp;alpha;</mi> <mo>&amp;CenterDot;</mo> <mi>s</mi> <mi>i</mi> <mi>n</mi> <mi>&amp;theta;</mi> <mo>+</mo> <mi>&amp;beta;</mi> <mi>c</mi> <mi>o</mi> <mi>s</mi> <mi>&amp;theta;</mi> <mo>-</mo> <mn>1</mn> </mrow> </mfrac> <mo>+</mo> <mn>2</mn> <mi>s</mi> <mo>+</mo> <mn>2</mn> <mi>z</mi> </mrow>
For the cycle P of the first grating1With the cycle P of the second grating2Ratio;
The calculation formula of the angle [alpha] of Moire fringe is:
<mrow> <mi>t</mi> <mi>a</mi> <mi>n</mi> <mi>&amp;alpha;</mi> <mo>=</mo> <mfrac> <mrow> <mfrac> <msub> <mi>P</mi> <mn>2</mn> </msub> <msubsup> <mi>P</mi> <mn>1</mn> <mo>&amp;prime;</mo> </msubsup> </mfrac> <mo>-</mo> <mi>c</mi> <mi>o</mi> <mi>s</mi> <mi>&amp;theta;</mi> </mrow> <mrow> <mi>s</mi> <mi>i</mi> <mi>n</mi> <mi>&amp;theta;</mi> </mrow> </mfrac> </mrow> 1
P′1For the cycle of Taibo picture, according to the enlargement ratio relation of Taibo pictureObtain;
Δ z is z uncertainty, and Δ s is s uncertainty, and Δ θ is θ uncertainty, and Δ α is α uncertainty, and Δ β is β uncertainty.
CN201710427891.2A 2017-06-08 2017-06-08 A kind of method and device of precise measurement super-large curvature radius Active CN107121095B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710427891.2A CN107121095B (en) 2017-06-08 2017-06-08 A kind of method and device of precise measurement super-large curvature radius

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710427891.2A CN107121095B (en) 2017-06-08 2017-06-08 A kind of method and device of precise measurement super-large curvature radius

Publications (2)

Publication Number Publication Date
CN107121095A true CN107121095A (en) 2017-09-01
CN107121095B CN107121095B (en) 2019-10-18

Family

ID=59729745

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710427891.2A Active CN107121095B (en) 2017-06-08 2017-06-08 A kind of method and device of precise measurement super-large curvature radius

Country Status (1)

Country Link
CN (1) CN107121095B (en)

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108106560A (en) * 2018-01-30 2018-06-01 青岛海泰光电技术有限公司 The comparative method for measuring method and its measuring device of optical element larger radius of curvature
CN108317988A (en) * 2018-04-19 2018-07-24 南京腾元软磁有限公司 Sample thickness in-situ measurement method based on transmission electron microscope surface imaging
CN109883357A (en) * 2019-04-19 2019-06-14 北京理工大学 Laterally subtract each other differential confocal parabola vertex curvature radius measurement method
CN109883356A (en) * 2019-04-19 2019-06-14 北京理工大学 Bilateral dislocation differential confocal parabola vertex curvature radius measurement method
CN109945804A (en) * 2019-04-19 2019-06-28 北京理工大学 Laterally subtract each other differential confocal super-large curvature radius measuring method
CN109945803A (en) * 2019-04-19 2019-06-28 北京理工大学 Laterally subtract each other laser differential confocal cylindrical curvature radius measurement method
CN109990732A (en) * 2019-04-19 2019-07-09 北京理工大学 Laterally subtract each other differential confocal curvature radius measurement method
CN110631509A (en) * 2019-10-10 2019-12-31 南京理工大学 Object surface curvature detection system and method based on grating Talbot image
CN110793467A (en) * 2018-08-02 2020-02-14 昆明勋凯瑞光学仪器有限公司 Optical lens piece curvature radius precision detection device
WO2021128517A1 (en) * 2019-12-23 2021-07-01 深圳市速普仪器有限公司 Radius of curvature measurement apparatus and radius of curvature measurement method
CN117804349A (en) * 2024-03-01 2024-04-02 中国科学技术大学 Grating displacement sensor debugging method based on moire fringe correlation calculation

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11821755B1 (en) * 2023-07-19 2023-11-21 Mloptic Corp. Moiré-based distance measurement method

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TW200944749A (en) * 2008-04-21 2009-11-01 Jing-Heng Chen Vertical reflective type moire measurement structure for measuring the surface curvature of an object
JP4512822B2 (en) * 2004-10-20 2010-07-28 国立大学法人 筑波大学 Line condensing type Fourier domain interference shape measuring device
CN101957182A (en) * 2010-08-04 2011-01-26 中国科学院光电技术研究所 Large-caliber high-gradient optical mirror surface online measurement system
CN101995230A (en) * 2010-10-29 2011-03-30 浙江大学 Talbot effect-based aspheric surface detection system
CN102252824A (en) * 2011-04-12 2011-11-23 浙江大学 Compound differential type long-focus measuring device based on Talbot effect
CN102313642A (en) * 2011-08-30 2012-01-11 浙江大学 High-precision focus detection device for long-focus lens
CN102331336A (en) * 2011-06-15 2012-01-25 浙江大学 Method and device for measuring focal distance of long-focal-length and large-aperture lens
CN103063413A (en) * 2012-12-24 2013-04-24 南京理工大学 Integrated long-focus measuring device based on Talbot-moire technology

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4512822B2 (en) * 2004-10-20 2010-07-28 国立大学法人 筑波大学 Line condensing type Fourier domain interference shape measuring device
TW200944749A (en) * 2008-04-21 2009-11-01 Jing-Heng Chen Vertical reflective type moire measurement structure for measuring the surface curvature of an object
CN101957182A (en) * 2010-08-04 2011-01-26 中国科学院光电技术研究所 Large-caliber high-gradient optical mirror surface online measurement system
CN101995230A (en) * 2010-10-29 2011-03-30 浙江大学 Talbot effect-based aspheric surface detection system
CN102252824A (en) * 2011-04-12 2011-11-23 浙江大学 Compound differential type long-focus measuring device based on Talbot effect
CN102331336A (en) * 2011-06-15 2012-01-25 浙江大学 Method and device for measuring focal distance of long-focal-length and large-aperture lens
CN102313642A (en) * 2011-08-30 2012-01-11 浙江大学 High-precision focus detection device for long-focus lens
CN103063413A (en) * 2012-12-24 2013-04-24 南京理工大学 Integrated long-focus measuring device based on Talbot-moire technology

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
侯昌伦等: "大口径长焦距镜面和透镜的扫描法焦距测量技术", 《计量学报》 *
赵琦等: "基于泰伯-莫尔干涉技术的焦距测量系统校准技术研究", 《激光与光电子学进展》 *

Cited By (18)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108106560A (en) * 2018-01-30 2018-06-01 青岛海泰光电技术有限公司 The comparative method for measuring method and its measuring device of optical element larger radius of curvature
CN108106560B (en) * 2018-01-30 2024-01-26 青岛海泰光电技术有限公司 Method and device for measuring large radius of curvature of optical element by comparison method
CN108317988A (en) * 2018-04-19 2018-07-24 南京腾元软磁有限公司 Sample thickness in-situ measurement method based on transmission electron microscope surface imaging
CN110793467A (en) * 2018-08-02 2020-02-14 昆明勋凯瑞光学仪器有限公司 Optical lens piece curvature radius precision detection device
CN109945804A (en) * 2019-04-19 2019-06-28 北京理工大学 Laterally subtract each other differential confocal super-large curvature radius measuring method
CN109945804B (en) * 2019-04-19 2020-12-15 北京理工大学 Transverse subtraction differential confocal measuring method for super-large curvature radius
CN109990732A (en) * 2019-04-19 2019-07-09 北京理工大学 Laterally subtract each other differential confocal curvature radius measurement method
CN109883357A (en) * 2019-04-19 2019-06-14 北京理工大学 Laterally subtract each other differential confocal parabola vertex curvature radius measurement method
CN109883356A (en) * 2019-04-19 2019-06-14 北京理工大学 Bilateral dislocation differential confocal parabola vertex curvature radius measurement method
CN109883357B (en) * 2019-04-19 2020-08-11 北京理工大学 Transverse subtraction differential confocal paraboloid vertex curvature radius measuring method
CN109883356B (en) * 2019-04-19 2020-12-11 北京理工大学 Bilateral dislocation differential confocal paraboloid vertex curvature radius measuring method
CN109945803A (en) * 2019-04-19 2019-06-28 北京理工大学 Laterally subtract each other laser differential confocal cylindrical curvature radius measurement method
CN109945803B (en) * 2019-04-19 2021-03-09 北京理工大学 Transverse subtraction laser differential confocal cylindrical surface curvature radius measuring method
CN110631509B (en) * 2019-10-10 2021-10-08 南京理工大学 Object surface curvature detection system and method based on grating Talbot image
CN110631509A (en) * 2019-10-10 2019-12-31 南京理工大学 Object surface curvature detection system and method based on grating Talbot image
WO2021128517A1 (en) * 2019-12-23 2021-07-01 深圳市速普仪器有限公司 Radius of curvature measurement apparatus and radius of curvature measurement method
CN117804349A (en) * 2024-03-01 2024-04-02 中国科学技术大学 Grating displacement sensor debugging method based on moire fringe correlation calculation
CN117804349B (en) * 2024-03-01 2024-04-30 中国科学技术大学 Grating displacement sensor debugging method based on moire fringe correlation calculation

Also Published As

Publication number Publication date
CN107121095B (en) 2019-10-18

Similar Documents

Publication Publication Date Title
CN107121095A (en) A kind of method and device of accurate measurement super-large curvature radius
CN101476880B (en) Surface shape detection apparatus and method for large-bore plane optical element
CN103954589B (en) The precision measurement apparatus of a kind of optical material specific refractory power and method
CN101153914B (en) Remote sensing mechanism testing device and method thereof
CN204831220U (en) Calcirm -fluoride optical flat two sides depth of parallelism high accuracy testing arrangement
CN103542813B (en) One kind is based on border differential and the self-alignment laser diameter measuring instrument of ambient light
CN104833486B (en) Multiple reflections formula laser differential confocal Long focal length measurement method and apparatus
CN106052585A (en) Surface shape detection device and detection method
CN106500843A (en) A kind of imaging spectrometer optimum image plane calibration method and device
CN112432766B (en) Laser scanning galvanometer performance detection method
JPH10311779A (en) Equipment for measuring characteristics of lens
CN106247989A (en) A kind of guide rail rolling angle field calibration and measurement apparatus and method
CN111238408A (en) Device and method for rapidly measuring parallelism of parallel flat plate
CN105783743B (en) Sheet metal print based on infrared reflection method applies wet-film thickness on-line detecting system
CN101469975A (en) Optical detecting instrument and method thereof
CN112284984B (en) Solid surface energy measuring device and method based on light reflection
CN103245488B (en) A kind of broadband large scale plane raster diffraction efficiency measurer
CN109799078B (en) Collimator focal length measuring device and method using moire fringe amplification effect
CN105091797B (en) A kind of single CCD intensity correlation autocollimator
CN106403829B (en) Coating thickness detector based on double light path infrared reflection method
CN108362210A (en) Simple lens laser displacement gauge head with linear structure
CN104155085B (en) Large-diameter sampling split plate sampling rate testing device and testing method
CN208547571U (en) Water body optical attenuation coefficient measuring device
CN106017441A (en) Portable high-precision laser long-working distance auto-collimation apparatus and method thereof
CN105180820B (en) A kind of transparent capillary inner surface face type test system and method for testing

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
CB03 Change of inventor or designer information

Inventor after: Hou Changlun

Inventor after: Xin Qing

Inventor after: Cang Yue

Inventor before: Hou Changlun

Inventor before: Xin Qing

Inventor before: Cang Yue

CB03 Change of inventor or designer information