CN103808267A - Spectrograph-based optical displacement sensor signal demodulation method - Google Patents

Spectrograph-based optical displacement sensor signal demodulation method Download PDF

Info

Publication number
CN103808267A
CN103808267A CN201210451998.8A CN201210451998A CN103808267A CN 103808267 A CN103808267 A CN 103808267A CN 201210451998 A CN201210451998 A CN 201210451998A CN 103808267 A CN103808267 A CN 103808267A
Authority
CN
China
Prior art keywords
array data
displacement sensor
light intensity
central wavelength
spectrometer
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
CN201210451998.8A
Other languages
Chinese (zh)
Other versions
CN103808267B (en
Inventor
李秉实
张兵
王东辉
包艳
吴忠
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.)
No 618 Research Institute of China Aviation Industry
Original Assignee
No 618 Research Institute of China Aviation Industry
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 No 618 Research Institute of China Aviation Industry filed Critical No 618 Research Institute of China Aviation Industry
Priority to CN201210451998.8A priority Critical patent/CN103808267B/en
Publication of CN103808267A publication Critical patent/CN103808267A/en
Application granted granted Critical
Publication of CN103808267B publication Critical patent/CN103808267B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Abstract

The invention relates to a spectrograph-based optical displacement sensor signal demodulation method. According the scheme, a data processing process of a wavelength encoding type optical displacement sensor comprises (1) reading spectroscopic data of output diffraction light of the sensor through a spectrograph; (2) processing the data through a full width at half maximum peak searching algorithm to obtain central wavelength; (3) performing comprehensive regression interpolation on the central wavelength to obtain displacement information. The spectrograph-based optical displacement sensor signal demodulation method has the advantages of being rapid, not needing a gate code calculation process and shortening data processing time; being accurate, avoiding gate code equation fitting errors and improving the calculation accuracy; being independent, not being influenced by optical grating diffraction angle errors and eliminating machining and assembling errors due to the facts that a former process of obtaining the grate code through a diffraction formula is eliminated and the displacement is directly obtained through the central wavelength.

Description

A kind of optical displacement sensor signal demodulating method based on spectrometer
Technical field
The present invention relates to a kind of optical displacement sensor signal demodulating method based on spectrometer.
Background technology
Along with light passes the development that flies control techniques, the research of optical displacement sensor deepens continuously, optical displacement sensor output signal be treated as research emphasis, in the development of Wavelength-encoding formula optical displacement sensor, most crucial data processing is to be resolved the displacement information of sensor by wavelength, and treatment scheme is: the spectroscopic data of the output diffraction light of (1) spectrometer read sensor; (2) by algorithm, data are processed and obtained centre wavelength; (3) try to achieve grid by diffraction formula close; (4) calculate displacement by the close equation of grating grid.
Due to current preparing grating process technology limit, the close equation of grid, for approximate three distributions, calculates step (3) and solves difficulty increase, and the processing time increases; Error in processing simultaneously, assembling, makes incident light incident angle produce deviation, causes the result of calculation of diffraction formula not conform to the actual conditions, and calculates wrong displacement information.
Summary of the invention
The object of the invention is to propose a kind of optical displacement sensor signal demodulating method based on spectrometer.
The technical scheme that the present invention takes is that a kind of optical displacement sensor signal demodulating method based on spectrometer, comprises the following steps:
Step 1: optical displacement sensor output arrowband diffraction light signal is to spectrometer;
Step 2: spectrometer reads the spectral information of arrowband diffraction light;
Step 3: spectrometer, by the corresponding array data of the wavelength X in spectral information and light intensity I, is input to computing machine;
Step 4: computing machine utilizes halfwidth method to process the corresponding array data of wavelength X and light intensity I, obtains the central wavelength lambda of arrowband diffraction light 0;
Step 5: to central wavelength lambda 0carry out interpolation arithmetic, obtain displacement information, complete demodulation.
Preferably, the method for halfwidth described in step 4 is: first utilize point-to-point comparison method to obtain the maximal value I of light intensity I mAX, after the corresponding array data of light intensity I is deducted to the I of 0.1~0.9 multiple mAX, obtain the new array data of light intensity I, then by maximal value I mAXpoint to the left and right both direction point-by-point comparison obtains the absolute value minimum value I of the new array data of light intensity I mINL, I mINR, I mINL, I mINRtwo corresponding wavelength value λ mINLand λ mINRintermediate value λ mID, be central wavelength lambda 0.
Preferably, the interpolation arithmetic described in step 5 is: first pass through survey record one group switching centre wavelength X first markwith displacement X markcorresponding array data, then in test, try to achieve central wavelength lambda 0after, search central wavelength lambda 0at λ markinterval of living in corresponding array data, then obtains displacement in interval interpolate value.
The advantage that the present invention has and beneficial effect: a) rapidity, without the process of carrying out the close calculating of grid, has shortened data processing time; B) accuracy, has cast aside the error of the close equation models of grid, has improved computational accuracy; C) independence, is not subject to the impact of optical grating diffraction angular error, has eliminated processing and rigging error.
Accompanying drawing explanation
Fig. 1 is the treatment scheme of many information fusion fast resolution algorithm, the linear arrowband diffraction light of wavelength and displacement centered by sensor output signal, by spectrometer, spectral information is read in to computing machine, utilize halfwidth method to calculate centre wavelength, draw displacement by interpolation arithmetic, complete sensor displacement test.
Fig. 2 is the corresponding relation curve of typical light displacement transducer output light wavelength and light intensity.
Fig. 3 is the process example that halfwidth method solves centre wavelength.
Fig. 4 is the process example that method of interpolation solves displacement.
Embodiment
Below in conjunction with Figure of description, the present invention is elaborated, concrete operation step is as follows:
Step 1: optical displacement sensor output arrowband diffraction light signal is to spectrometer;
Step 2: spectrometer reads the spectral information of arrowband diffraction light;
Step 3: spectrometer, by the corresponding array data of the wavelength X in spectral information and light intensity I, is input to computing machine;
Step 4: computing machine utilizes halfwidth method to process the corresponding array data of wavelength X and light intensity I, obtains the central wavelength lambda of arrowband diffraction light 0.First utilize point-to-point comparison method to obtain the maximal value I of light intensity I mAX, after the corresponding array data of light intensity I is deducted to the I of 0.1~0.9 multiple mAX, obtain the new array data of light intensity I, then by maximal value I mAXpoint to the left and right both direction point-by-point comparison obtains the absolute value minimum value I of the new array data of light intensity I mINL, I mINR, I mINL, I mINRtwo corresponding wavelength value λ mINLand λ mINRintermediate value λ mID, be central wavelength lambda 0.;
Step 5: to central wavelength lambda 0carry out interpolation arithmetic, first pass through survey record one group switching centre wavelength X first markwith displacement X markcorresponding array data, then in test, try to achieve central wavelength lambda 0after, search central wavelength lambda 0at λ markinterval of living in corresponding array data, then obtains displacement in interval interpolate value, completes demodulation.
Embodiment
Step 1: optical displacement sensor output arrowband diffraction light signal is to spectrometer;
Step 2: spectrometer is chosen the HR4000 type of ocean company, reads the spectral information of arrowband diffraction light;
Step 3: spectrometer, by the corresponding array data of the wavelength X in spectral information and light intensity I, is input to computing machine, the corresponding array of wavelength X and light intensity I is two arrays that comprise 3648 numerical value, its typical corresponding relation is as shown in Figure 2;
Step 4: computing machine utilizes halfwidth method to process the corresponding array data of wavelength X and light intensity I, obtains the central wavelength lambda of arrowband diffraction light 0.First utilize point-to-point comparison method to obtain the maximal value I of light intensity I mAX, its light intensity value is 9144; After the corresponding array data of light intensity I is deducted to the I of 0.5 multiple mAX, obtaining the new array data of light intensity I, the new wavelength X of array and the corresponding relation of light intensity I are as shown in Figure 3; Again by maximal value I mAXpoint to the left and right both direction point-by-point comparison obtains the absolute value minimum value I of the new array data of light intensity I mINL, I mINR, be respectively 5.8 and 14.7; I mINL, I mINRtwo corresponding wavelength value λ mINLand λ mINRbe respectively 713.4nm and 735.6nm, its intermediate value 724.5nm is central wavelength lambda 0;
Step 5: to central wavelength lambda 0carry out interpolation arithmetic, first pass through survey record one group switching centre wavelength X first markwith displacement X markcorresponding array data, then in test, try to achieve central wavelength lambda 0after, search central wavelength lambda 0at λ markinterval of living in corresponding array data, then obtains displacement in interval interpolate value, and as shown in Figure 4,724.5nm is at λ for example markin corresponding array data at λ mark 1(722.2nm), λ mark 2(727.1nm), between, between point (722.2nm, 44mm) and (727.1nm, 46mm), carry out linear interpolation arithmetic and can obtain displacement X 0for 44.94mm, now complete demodulation.

Claims (3)

1. the optical displacement sensor signal demodulating method based on spectrometer, is characterized in that, comprises the following steps:
Step 1: optical displacement sensor output arrowband diffraction light signal is to spectrometer;
Step 2: spectrometer reads the spectral information of arrowband diffraction light;
Step 3: spectrometer, by the corresponding array data of the wavelength X in spectral information and light intensity I, is input to computing machine;
Step 4: computing machine utilizes halfwidth method to process the corresponding array data of wavelength X and light intensity I, obtains the central wavelength lambda of arrowband diffraction light 0;
Step 5: to central wavelength lambda 0carry out interpolation arithmetic, obtain displacement information, complete demodulation.
2. a kind of optical displacement sensor signal demodulating method based on spectrometer according to claim 1, is characterized in that, the method for halfwidth described in step 4 is: first utilize point-to-point comparison method to obtain the maximal value I of light intensity I mAX, after the corresponding array data of light intensity I is deducted to the I of 0.1~0.9 multiple mAX, obtain the new array data of light intensity I, then by maximal value I mAXpoint to the left and right both direction point-by-point comparison obtains the absolute value minimum value I of the new array data of light intensity I mINL, I mINR, I mINL, I mINRtwo corresponding wavelength value λ mINLand λ mINRintermediate value λ mID, be central wavelength lambda 0.
3. a kind of optical displacement sensor signal demodulating method based on spectrometer according to claim 1 and 2, is characterized in that, the interpolation arithmetic described in step 5 is: first pass through survey record one group switching centre wavelength X first markwith displacement X markcorresponding array data, then in test, try to achieve central wavelength lambda 0after, search central wavelength lambda 0at λ markinterval of living in corresponding array data, then obtains displacement in interval interpolate value.
CN201210451998.8A 2012-11-12 2012-11-12 A kind of optical displacement sensor signal demodulating method based on spectrogrph Active CN103808267B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201210451998.8A CN103808267B (en) 2012-11-12 2012-11-12 A kind of optical displacement sensor signal demodulating method based on spectrogrph

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201210451998.8A CN103808267B (en) 2012-11-12 2012-11-12 A kind of optical displacement sensor signal demodulating method based on spectrogrph

Publications (2)

Publication Number Publication Date
CN103808267A true CN103808267A (en) 2014-05-21
CN103808267B CN103808267B (en) 2016-12-21

Family

ID=50705386

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201210451998.8A Active CN103808267B (en) 2012-11-12 2012-11-12 A kind of optical displacement sensor signal demodulating method based on spectrogrph

Country Status (1)

Country Link
CN (1) CN103808267B (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105259667A (en) * 2015-11-09 2016-01-20 中国科学院上海光学精密机械研究所 An adjusting method for a cylindrical surface stretcher grating pair

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070019208A1 (en) * 2004-12-10 2007-01-25 Fuji Photo Film Co., Ltd. Optical tomography apparatus
CN101915593A (en) * 2010-07-16 2010-12-15 山东大学 Device for demodulating fiber bragg grating reflection wavelength by utilizing ASE light source light spectrum failing edge

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20070019208A1 (en) * 2004-12-10 2007-01-25 Fuji Photo Film Co., Ltd. Optical tomography apparatus
CN101915593A (en) * 2010-07-16 2010-12-15 山东大学 Device for demodulating fiber bragg grating reflection wavelength by utilizing ASE light source light spectrum failing edge

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
李秉实: "变栅距光栅衍射强度分布的一般公式及其应用", 《传感器世界》 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105259667A (en) * 2015-11-09 2016-01-20 中国科学院上海光学精密机械研究所 An adjusting method for a cylindrical surface stretcher grating pair

Also Published As

Publication number Publication date
CN103808267B (en) 2016-12-21

Similar Documents

Publication Publication Date Title
CN105424185B (en) A kind of computer assisted all band spectrometer wavelength calibration method
CN108362208B (en) Pseudo-random code channel grating ruler and reading method thereof
CN102706372B (en) Optical fiber wavelength demodulating light spectrum peak value positioning method
CN110207596B (en) Image coding method, grating ruler measuring device and measuring method
CN101797704A (en) Method for thermal deformation error compensation of digital control gear hobbing machine
JP5102395B2 (en) Method and circuit for automatically calibrating electromagnetic induction furnace power
WO2013174216A1 (en) Single-track absolute grating scale and image encoding method thereof
CN105222892A (en) A kind of wavelength scaling method of ultraviolet spectrometer (UVS)
WO2016058287A1 (en) Design method for spectrograph and spectrograph
CN102184542A (en) Stereo matching method for stereo binocular vision measurement
CN105068032B (en) A kind of calibration method of photovoltaic combiner box current acquisition channel temperature coefficient of deviation
CN115859080A (en) Optical fiber Bragg grating signal peak value detection algorithm based on asymmetric Gaussian model
CN104075669A (en) Fault-tolerant coding and decoding method for complicated surface coded light measurement
CN103808267A (en) Spectrograph-based optical displacement sensor signal demodulation method
CN102200581B (en) High-precision moisture Raman system and scaling method using monochromator
CN201034729Y (en) Quick-speed spectrometer
CN105486408A (en) Three-wavelength Stokes vector polarization measurement system and method bases on color CCD
CN104567743A (en) Angle displacement measurement device and measurement method thereof
CN110411485A (en) The transmission-type absolute rotary encoder and measurement method of light interference are filtered out based on exposure mask
CN105758521B (en) The optical fiber grating regulating system and method for spectral resolution are improved using fine motion grating
CN105890636B (en) The optical fiber grating regulating system for improving spectral resolution is translated using slit
CN102385216A (en) Fiber Bragg grating (FBG) demodulation method based on modular interference of polarization maintaining fiber (PMF)
CN209894695U (en) Double-detector time division multiplexing volume holographic material sensitivity real-time testing device
CN111121827B (en) TMR magnetic encoder system based on Kalman filtering
CN110296725B (en) Asymmetric spectrum demodulation method of fiber Bragg grating sensor based on distributed estimation algorithm

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant