CN109443405A - A kind of optic fiber grating wavelength demodulating system - Google Patents

A kind of optic fiber grating wavelength demodulating system Download PDF

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Publication number
CN109443405A
CN109443405A CN201811529281.4A CN201811529281A CN109443405A CN 109443405 A CN109443405 A CN 109443405A CN 201811529281 A CN201811529281 A CN 201811529281A CN 109443405 A CN109443405 A CN 109443405A
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China
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wavelength
fiber grating
interference
photoelectric detector
etalon
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CN201811529281.4A
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Inventor
彭庆军
钱国超
古洪瑞
陈伟根
万福
马仪
程志万
周仿荣
邹德旭
黄星
洪志湖
刘光祺
颜冰
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Electric Power Research Institute of Yunnan Power System Ltd
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Electric Power Research Institute of Yunnan Power System Ltd
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/353Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
    • G01D5/35306Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement
    • G01D5/35309Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement using multiple waves interferometer
    • G01D5/35312Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement using multiple waves interferometer using a Fabry Perot
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D21/00Measuring or testing not otherwise provided for
    • G01D21/02Measuring two or more variables by means not covered by a single other subclass

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Communication System (AREA)
  • Spectrometry And Color Measurement (AREA)
  • Semiconductor Lasers (AREA)

Abstract

This application discloses a kind of optic fiber grating wavelength demodulating systems, including light source, light source is the C-band Wavelength-swept laser of interior period triangle wave voltage driving, and light source, coupler, circulator and fiber grating are sequentially connected, and circulator is also sequentially connected with the first photoelectric detector, data collecting card;Coupler is also sequentially connected electrically with interference subsystem, the second photoelectric detector, data collecting card, computer;Interfering subsystem includes interference ontology and temperature control equipment, temperature control equipment includes semiconductor chilling plate, control circuit and cooling fan, F-P etalon, semiconductor chilling plate and control circuit are provided in interference ontology, semiconductor chilling plate, control circuit and power supply are sequentially connected, and are interfered and are provided with cooling fan on the outside of ontology.F-P etalon can dynamic nominal light fibre grating wavelength, and temperature control equipment can guarantee F-P etalon temperature tend to be constant, make its wavelength constant, effectively improve the precision and stability of demodulating system.

Description

A kind of optic fiber grating wavelength demodulating system
Technical field
This application involves technical field of optical fiber sensing more particularly to a kind of optic fiber grating wavelength demodulation based on linear interpolation System.
Background technique
Fiber grating sensing technology is a research hotspot in recent years, and compared with traditional sensor, fiber grating is passed Sensor has many advantages, such as electromagnetism interference, high sensitivity, small in size.For specific fiber-optic grating sensor, wavelength change There are corresponding relationships with pressure with environment temperature.It therefore, is accurate measurement temperature and pressure, the wavelength interrogation technique of fiber grating It is particularly significant.
The demodulating system of existing optic fiber grating wavelength is tunable TEA CO2 laser demodulating system.Existing tunable F-P Filter demodulating system mainly includes the devices such as wideband light source, F-P filter, coupler, photoelectric detector.This demodulating system Working principle be to be pasted onto the piezoelectric ceramics of F-P cavity side using triangle wave voltage driving, bring it about miniature deformation, cause F-P cavity change of cavity length, and then change the central wavelength penetrated.
But existing this demodulating system is easy to influence since the driving voltage and wavelength of its F-P filter are non-linear The precision of Wavelength demodulation, so that its stability is poor.In order to improve the precision of Wavelength demodulation, enhances its stability, propose one Kind optic fiber grating wavelength demodulating system.
Summary of the invention
This application provides a kind of optic fiber grating wavelength demodulating systems, low to solve existing system medium wavelength demodulation accuracy Technical problem.
To solve the above-mentioned problems, the application provides technical solution below:
A kind of optic fiber grating wavelength demodulating system, including light source, light source are the C-band wave of interior period triangle wave voltage driving Long scan laser, in which: light source is electrically connected with the first end of coupler, the second end of coupler and the first end electricity of circulator Connection, the second end of circulator are electrically connected with fiber grating, the third end of circulator and the first end electricity of the first photoelectric detector Connection, the second end of the first photoelectric detector are electrically connected with the first end of data collecting card;The third end of coupler and interference The first end of system is electrically connected, and interferes the second end of subsystem and the first end of the second photoelectric detector to be electrically connected, the second photoelectricity The second end of detector is electrically connected with the second end of data collecting card, the third end of data collecting card and calculating mechatronics;It is dry Relating to subsystem includes interference ontology and temperature control equipment, and temperature control equipment includes semiconductor chilling plate, control circuit and cold But fan interferes in ontology and is provided with F-P etalon, semiconductor chilling plate and control circuit, F-P etalon and semiconductor refrigerating Piece is not connected to, and semiconductor chilling plate is electrically connected with the first end of control circuit, and the second end of control circuit is electrically connected to a power source, and is done It relates to and is provided with cooling fan on the outside of ontology.
Optionally, the shell for interfering ontology is metal-back.
Optionally, the splitting ratio of coupler is 85:15.
A kind of test method of optic fiber grating wavelength demodulating system, which is characterized in that test method includes:
Coupler will be divided into two parts by received light from light source, and this two parts of light are transferred to interference subsystem and ring respectively Shape device;
For 15% light by interfering subsystem to be transferred to the second photoelectric detector, 85% light is transferred to light by circulator Fine grating;
The reflected light pass of fiber grating is transferred to the first photoelectric detector to circulator, and by circulator;
The light received is converted to electric signal respectively by the first photoelectric detector and the second photoelectric detector;
Electric signal is transferred to computer by data collecting card;
Computer calculates the wavelength of fiber grating according to linear interpolation algorithm.
Optionally, computer calculates the wavelength of fiber grating according to linear interpolation algorithm, comprising:
According to the wavelength of standard queries F-P etalon, when computer calculates the detection of fiber grating and etalon spectral peak Between;
Computer carries out linear interpolation calculating and can count as shown in formula (1) to fiber grating and two adjacent modular tool spectral peaks Calculate the wavelength of fiber grating;
λ in formulaFBGFor the wavelength of fiber grating, λLAnd λRThe respectively wave of left standard tool spectral peak and right standard tool spectral peak It is long, tFBG、tRAnd tLRespectively fiber grating spectral peak, the detection time of left standard tool spectral peak and right standard tool spectral peak.
The utility model has the advantages that the demodulating system includes light source, light source this application provides a kind of optic fiber grating wavelength demodulating system For the C-band Wavelength-swept laser of interior period triangle wave voltage driving.F-P filter inside laser is driven voltage tune System, length cyclically-varying with the variation of driving voltage of F-P cavity, so that the wavelength of output laser is with driving voltage Change and periodically scans for C-band.The light that laser issues arrives Measurement channel and reference channel by coupler difference is defeated, Specially light source is electrically connected with the first end of coupler, and the second end of coupler is connect with Measurement channel, the third end of coupler It is connect with reference channel.Connection in Measurement channel is as follows: the second end of coupler is electrically connected with the first end of circulator, annular The second end of device is electrically connected with fiber grating, and the third end of circulator is electrically connected with the first end of the first photoelectric detector, and first The second end of photoelectric detector is electrically connected with the first end of data collecting card.Connection in reference channel is as follows: the of coupler Three ends are electrically connected with the first end of interference subsystem, and the second end of subsystem and the first end of the second photoelectric detector is interfered to be electrically connected It connects, the second end of the second photoelectric detector is electrically connected with the second end of data collecting card, the third end of data collecting card and calculating Mechatronics.Use process: the light issued from Wavelength-swept laser is divided into two by the coupler that splitting ratio is 85:15 Point, 15% light enters the second photoelectric detector by reference to the F-P etalon in channel, and 85% light enters Measurement channel, Enter fiber grating by circulator, the reflected light of fiber grating is again introduced into circulator and propagates and enter the first Photoelectric Detection Device.Received light is converted to electric signal by the first photoelectric detector and the second photoelectric detector, and is passed through data collecting card and transmitted It is handled to computer.Due to characteristics such as F-P cavity hysteresis, creep properties and temperature changes, leads to Output of laser wavelength and drive Dynamic voltage is in non-critical linear.Therefore, F-P etalon being introduced in interference subsystem, dynamic mark is carried out to optic fiber grating wavelength It is fixed.Light source light spectrum is divided into multiple pectination intervals by F-P etalon, and Output of laser wavelength and driving voltage can be regarded as in each interval Linear relationship.Interfering subsystem includes interference ontology and temperature control equipment, and temperature control equipment includes semiconductor chilling plate, control Circuit processed and cooling fan interfere in ontology and are provided with F-P etalon, semiconductor chilling plate and control circuit, F-P etalon with Semiconductor chilling plate is not connected to, and semiconductor chilling plate is electrically connected with the first end of control circuit, the second end and electricity of control circuit Source electrical connection, interferes and is provided with cooling fan on the outside of ontology.In use process, control circuit is according to interference subsystem internal Temperature controls semiconductor chilling plate effect, so that the temperature in interference subsystem tends towards stability.Cooling fan is mounted on interference originally In vitro, heat can be taken away when the temperature rises, further such that the temperature of F-P etalon tends to be constant, make the wave of F-P etalon A length of constant.In the application, Wavelength-swept laser is capable of providing higher output power;F-P etalon can dynamic nominal light Fine grating wavelength calculates the wavelength of fiber grating using linear interpolation;Control circuit, semiconductor chilling plate in interference subsystem It can guarantee that the temperature of F-P etalon tends to be constant with temperature control equipments such as cooling fans, make its wavelength constant, thus effectively Improve the precision and stability of demodulating system.In the application, interfere the F-P etalon in subsystem can dynamic nominal light fibre grating Wavelength, and temperature control equipment can guarantee that the temperature of F-P etalon tends to be constant, make its wavelength constant, to effectively improve The precision and stability of demodulating system.
Detailed description of the invention
In order to illustrate more clearly of the technical solution of the application, letter will be made to attached drawing needed in the embodiment below Singly introduce, it should be apparent that, for those of ordinary skills, without any creative labor, It is also possible to obtain other drawings based on these drawings.
Fig. 1 is a kind of structural schematic diagram for optic fiber grating wavelength demodulating system that application provides;
Fig. 2 is a kind of structural schematic diagram for interference subsystem that application provides;
Fig. 3 is the test result figure for the F-P etalon temperature data that application provides;
Fig. 4 is the test result figure of optic fiber grating wavelength demodulating system provided by the present application;
Detailed description of the invention: 1- light source, 2- coupler, 3- circulator, 4- fiber grating, the first photoelectric detector of 5-, 6- data Capture card, 7- interference subsystem, the second photoelectric detector of 8-, 9- computer, 71- interference ontology, 72- temperature control equipment, 711-F-P etalon, 721- semiconductor chilling plate, 722- control circuit, 723- cooling fan.
Specific embodiment
Fig. 1 is a kind of structural schematic diagram of optic fiber grating wavelength demodulating system provided by the present application, and Fig. 2 provides for the application A kind of interference subsystem structural schematic diagram, referring to Fig. 1 and Fig. 2 it is found that this application provides a kind of optic fiber grating wavelength solutions Adjusting system, the demodulating system include light source 1, and light source 1 is the C-band Wavelength-swept laser of interior period triangle wave voltage driving. F-P filter inside laser is driven voltage modulated, length cyclically-varying with the variation of driving voltage of F-P cavity, So that the wavelength of output laser periodically scans for C-band with the variation of driving voltage.The light warp that laser issues Overcoupling device 2 is distinguished defeated to Measurement channel and reference channel, and specially light source 1 is electrically connected with the first end of coupler 2, coupler 2 second end is connect with Measurement channel, and the third end of coupler 2 is connect with reference channel.Connection in Measurement channel is as follows: coupling The second end of clutch 2 is electrically connected with the first end of circulator 3, and the second end of circulator 3 is electrically connected with fiber grating 4, circulator 3 Third end be electrically connected with the first end of the first photoelectric detector 5, the second end of the first photoelectric detector 5 and data collecting card 6 First end electrical connection.Connection in reference channel is as follows: the third end of coupler 2 and the first end of interference subsystem 7 are electrically connected It connects, the second end of interference subsystem 7 is electrically connected with the first end of the second photoelectric detector 8, the second end of the second photoelectric detector 8 It is electrically connected with the second end of data collecting card 6, the third end of data collecting card 6 is connect with electromechanics 9 is calculated.Use process: from wave It is two parts that the coupler 2 that the light that long scan laser issues is 85:15 by splitting ratio, which divides, and 15% light is by reference to channel In F-P etalon 711 enter the second photoelectric detector 8,85% light enters Measurement channel, enters optical fiber by circulator 3 Grating 4, the reflected light of fiber grating 4 are again introduced into circulator 3 and propagate and enter the first photoelectric detector 5.First Photoelectric Detection Received light is converted to electric signal by device 5 and the second photoelectric detector 8, and is transmitted to the progress of computer 9 by data collecting card 6 Processing.Due to characteristics such as F-P cavity hysteresis, creep properties and temperature changes, cause Output of laser wavelength and driving voltage in non-tight Ruling.Therefore, F-P etalon 711 being introduced in interference subsystem 7, dynamic calibration is carried out to 4 wavelength of fiber grating.F-P mark Light source light spectrum is divided into multiple pectination intervals by quasi- tool 711, and Output of laser wavelength and driving voltage can be regarded as linearly in each interval Relationship.Interfering subsystem 7 includes interference ontology 71 and temperature control equipment 72, and temperature control equipment 72 includes semiconductor chilling plate 721, control circuit 722 and cooling fan 723 interfere in ontology 71 and are provided with F-P etalon 711,721 and of semiconductor chilling plate Control circuit 722, F-P etalon 711 are not connected to semiconductor chilling plate 721, semiconductor chilling plate 721 and control circuit 722 First end electrical connection, the second end of control circuit 722 is electrically connected to a power source, and the outside of interference ontology 71 is provided with cooling fan 723.In use process, control circuit 722 is acted on according to the temperature control semiconductor chilling plate 721 inside interference subsystem 71, So that the temperature in interference subsystem 7 tends towards stability.Cooling fan 723 is mounted on outside interference ontology 41, can be when the temperature rises Heat is taken away, further such that the temperature of F-P etalon 711 tends to be constant, makes the wavelength constant of F-P etalon 711.This Shen Please in, Wavelength-swept laser is capable of providing higher output power;F-P etalon 711 can 4 wave of dynamic nominal light fibre grating It is long, the wavelength of fiber grating 4 is calculated using linear interpolation;Control circuit 722, semiconductor chilling plate 721 in interference subsystem 7 It can guarantee that the temperature of F-P etalon 711 tends to be constant with the equal temperature control equipments 72 of cooling fan 723, make its wavelength constant, To effectively improve the precision and stability of demodulating system.In the application, interfere the F-P etalon 711 in subsystem 7 can dynamic 4 wavelength of fiber grating is demarcated, and temperature control equipment 72 can guarantee that the temperature of F-P etalon 711 tends to be constant, make its wavelength Constant, to effectively improve the precision and stability of demodulating system.
In order to facilitate the temperature of control interference ontology 71, in the present embodiment, the shell of interference ontology 71 is metal-back.Metal It is good with thermal conductivity, and the advantages of be hardly damaged, the shell of interference ontology 71 is metal-back, not only facilitates control interference ontology 71 Temperature, make its stability enhance;The F-P etalon in interference ontology 71 can also be protected, its service life is improved.
In the application, other than providing a kind of optic fiber grating wavelength demodulating system, a kind of fiber grating wave is additionally provided The test method of long demodulating system, test method include:
S01: coupler will receive from light source is divided into two parts, and this two parts of light are transferred to interference subsystem and ring respectively Shape device;
Interference subsystem belongs to reference channel, and circulator belongs to Measurement channel.
By interfering subsystem to be transferred to the second photoelectric detector, 85% light is transmitted the light of S02:15% by circulator To fiber grating;
S03: the reflected light pass of fiber grating is transferred to the first photoelectric detector to circulator, and by circulator;
The light received is converted to electric signal respectively by the S04: the first photoelectric detector and the second photoelectric detector;
S05: electric signal is transferred to computer by data collecting card;
S06: computer calculates the wavelength of fiber grating according to linear interpolation algorithm.
According to the wavelength of standard queries F-P etalon, when computer calculates the detection of fiber grating and etalon spectral peak Between;
Computer carries out linear interpolation calculating and can count as shown in formula (1) to fiber grating and two adjacent modular tool spectral peaks Calculate the wavelength of fiber grating;
λ in formulaFBGFor the wavelength of fiber grating, λLAnd λRThe respectively wave of left standard tool spectral peak and right standard tool spectral peak It is long, tFBG、tRAnd tLRespectively fiber grating spectral peak, the detection time of left standard tool spectral peak and right standard tool spectral peak.
The effect realized in order to better illustrate the present invention illustrates optic fiber grating wavelength demodulating system below with reference to example Experiment effect.First verify that the temperature stability of the F-P etalon with temperature control equipment, the temperature control of established standards tool exists 23 DEG C, continuance test 24 hours or more, the temperature data of etalon is exported by temperature control equipment, is the application referring to Fig. 3 The test result figure of the F-P etalon temperature data of offer.
It can be seen that the temperature of etalon controls within ± 0.01 DEG C, therefore can guarantee that the wavelength of etalon is constant, Improve the stability of optic fiber grating wavelength demodulating system.
Optic fiber grating wavelength demodulating system proposed by the present invention is connect with fiber grating single channel.To verify fiber grating Fiber grating is placed in the water-bath that temperature fluctuation amplitude is ± 0.01 DEG C/1h, holds by the stability of Wavelength demodulation system, experiment Continuous test 24 hours or more, be the test result figure of optic fiber grating wavelength demodulating system provided by the present application referring to fig. 4.
It can be seen that the wavelength of fiber grating in for 24 hours in 0.3pm in the range of fluctuate, and wavelength is near fixed value Fluctuation, rather than only change in one direction, therefore in the performance steady in a long-term of optic fiber grating wavelength demodulating system interior for 24 hours For ± 0.15pm, stability with higher.
Those skilled in the art will readily occur to its of the application after considering the embodiment of specification and practice here Its embodiment.This application is intended to cover any variations, uses, or adaptations of the application, these modifications, purposes or Person's adaptive change follows the general principle of the application and including the not used common knowledge in the art of the application Or conventional techniques.The description and examples are only to be considered as illustrative, and the true scope and spirit of the application are by following Claim is pointed out.
It should be understood that the application is not limited to the precise structure that has been described above and shown in the drawings, and And various modifications and changes may be made without departing from the scope thereof.Scope of the present application is only limited by the accompanying claims.

Claims (5)

1. a kind of optic fiber grating wavelength demodulating system, which is characterized in that including light source (1), the light source (1) is interior periodic trigonometric The C-band Wavelength-swept laser of wave voltage driving, in which:
The light source (1) is electrically connected with the first end of coupler (2), and the of the second end of the coupler (2) and circulator (3) One end electrical connection, the second end of the circulator (3) is electrically connected with fiber grating (4), the third end of the circulator (3) and the The first end of one photoelectric detector (5) is electrically connected, second end and data collecting card (6) of first photoelectric detector (5) First end electrical connection;
The third end of the coupler (2) be electrically connected with the first end of interference subsystem (7), it is described interfere subsystem (7) the Two ends are electrically connected with the first end of the second photoelectric detector (8), the second end and the data of second photoelectric detector (8) The second end of capture card (6) is electrically connected, and the third end of the data collecting card (6) is electrically connected with computer (9);
The interference subsystem (7) includes interference ontology (71) and temperature control equipment (72), the temperature control equipment (72) Including semiconductor chilling plate (721), control circuit (722) and cooling fan (723), F- is provided in the interference ontology (71) P etalon (711), semiconductor chilling plate (721) and control circuit (722), the F-P etalon (711) and the semiconductor Cooling piece (721) is not connected to, and the semiconductor chilling plate (721) is electrically connected with the first end of control circuit (722), the control The second end of circuit (722) is electrically connected to a power source, and is provided with cooling fan (723) on the outside of the interference ontology (71).
2. demodulating system according to claim 1, which is characterized in that the shell of interference ontology (71) is metal-back.
3. demodulating system according to claim 1, which is characterized in that the splitting ratio of the coupler (2) is 85:15.
4. a kind of test method of optic fiber grating wavelength demodulating system, which is characterized in that the test method includes:
Coupler will be divided into two parts by received light from light source, and this two parts of light are transferred to interference subsystem and annular respectively Device;
For 15% light by interfering subsystem to be transferred to the second photoelectric detector, 85% light is transferred to optical fiber light by circulator Grid;
The reflected light pass of fiber grating is transferred to the first photoelectric detector to circulator, and by circulator;
The light received is converted to electric signal respectively by the first photoelectric detector and the second photoelectric detector;
Electric signal is transferred to computer by data collecting card;
Computer calculates the wavelength of fiber grating according to linear interpolation algorithm.
5. test method according to claim 4, which is characterized in that the computer calculates light according to linear interpolation algorithm The wavelength of fine grating, comprising:
According to the wavelength of standard queries F-P etalon, computer calculates the detection time of fiber grating and etalon spectral peak;
Computer carries out linear interpolation calculating and can calculate as shown in formula (1) to fiber grating and two adjacent modular tool spectral peaks The wavelength of fiber grating;
λ in formulaFBGFor the wavelength of fiber grating, λLAnd λRThe respectively wavelength of left standard tool spectral peak and right standard tool spectral peak, tFBG、tRAnd tLRespectively fiber grating spectral peak, the detection time of left standard tool spectral peak and right standard tool spectral peak.
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Citations (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050269489A1 (en) * 2004-06-04 2005-12-08 Domino Taverner Optical wavelength determination using multiple measurable features
CN101762557A (en) * 2009-10-28 2010-06-30 天津大学 Gas category classification method and classification device based on active inner cavity absorption spectrum
CN202267882U (en) * 2011-09-20 2012-06-06 华北电力大学(保定) Reference grating and F-P etalon temperature controlling apparatus
CN102879022A (en) * 2012-09-25 2013-01-16 杭州联光电子有限公司 Method and device for demodulating fiber bragg grating (FBG) sensor
CN103411686A (en) * 2013-08-27 2013-11-27 天津大学 Device and method for calibrating optical fiber scanning light source wavelength based on gas absorption spectral lines
CN103528607A (en) * 2013-10-24 2014-01-22 宁波振东光电有限公司 FBG (fiber bragg grating) interrogator
CN203422098U (en) * 2013-09-18 2014-02-05 哈尔滨理工大学 DFB laser-based FBG wavelength demodulator
US8731018B2 (en) * 2011-01-27 2014-05-20 Mitsubishi Electric Corporation Semiconductor laser
CN104180921A (en) * 2014-07-29 2014-12-03 天津大学 Temperature and stress measuring device based on orthogonal dual-polarization fiber laser
CN104457803A (en) * 2014-11-28 2015-03-25 中南大学 Wave length demodulating system and method based on F-P etalon and reference gratings
CN104931081A (en) * 2015-06-10 2015-09-23 天津大学 Composite wavelength reference-based fiber bragg grating sensing demodulation device and method
CN205957991U (en) * 2016-07-14 2017-02-15 青岛派科森光电技术股份有限公司 Fiber grating demodulation instrument
CN106940220A (en) * 2016-01-04 2017-07-11 中国计量学院 A kind of wavelength real-time measurement apparatus of Simple low-cost
CN107065619A (en) * 2017-05-15 2017-08-18 武汉光迅科技股份有限公司 The wavelength control electrode parameter establishing method and device of a kind of tunable laser
CN107843744A (en) * 2017-10-27 2018-03-27 中南大学 The Wavelength demodulation system and Wavelength demodulation method of optical fibre grating acceleration sensor
CN108507697A (en) * 2018-02-28 2018-09-07 华北电力大学(保定) A kind of sea water temperature depth profile sampling towed system based on Fibre Optical Sensor

Patent Citations (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20050269489A1 (en) * 2004-06-04 2005-12-08 Domino Taverner Optical wavelength determination using multiple measurable features
CN101762557A (en) * 2009-10-28 2010-06-30 天津大学 Gas category classification method and classification device based on active inner cavity absorption spectrum
US8731018B2 (en) * 2011-01-27 2014-05-20 Mitsubishi Electric Corporation Semiconductor laser
CN202267882U (en) * 2011-09-20 2012-06-06 华北电力大学(保定) Reference grating and F-P etalon temperature controlling apparatus
CN102879022A (en) * 2012-09-25 2013-01-16 杭州联光电子有限公司 Method and device for demodulating fiber bragg grating (FBG) sensor
CN103411686A (en) * 2013-08-27 2013-11-27 天津大学 Device and method for calibrating optical fiber scanning light source wavelength based on gas absorption spectral lines
CN203422098U (en) * 2013-09-18 2014-02-05 哈尔滨理工大学 DFB laser-based FBG wavelength demodulator
CN103528607A (en) * 2013-10-24 2014-01-22 宁波振东光电有限公司 FBG (fiber bragg grating) interrogator
CN104180921A (en) * 2014-07-29 2014-12-03 天津大学 Temperature and stress measuring device based on orthogonal dual-polarization fiber laser
CN104457803A (en) * 2014-11-28 2015-03-25 中南大学 Wave length demodulating system and method based on F-P etalon and reference gratings
CN104931081A (en) * 2015-06-10 2015-09-23 天津大学 Composite wavelength reference-based fiber bragg grating sensing demodulation device and method
CN106940220A (en) * 2016-01-04 2017-07-11 中国计量学院 A kind of wavelength real-time measurement apparatus of Simple low-cost
CN205957991U (en) * 2016-07-14 2017-02-15 青岛派科森光电技术股份有限公司 Fiber grating demodulation instrument
CN107065619A (en) * 2017-05-15 2017-08-18 武汉光迅科技股份有限公司 The wavelength control electrode parameter establishing method and device of a kind of tunable laser
CN107843744A (en) * 2017-10-27 2018-03-27 中南大学 The Wavelength demodulation system and Wavelength demodulation method of optical fibre grating acceleration sensor
CN108507697A (en) * 2018-02-28 2018-09-07 华北电力大学(保定) A kind of sea water temperature depth profile sampling towed system based on Fibre Optical Sensor

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