CN105444793A - Fiber Bragg raster sensing device based on high-speed pulse laser - Google Patents

Fiber Bragg raster sensing device based on high-speed pulse laser Download PDF

Info

Publication number
CN105444793A
CN105444793A CN201510785578.7A CN201510785578A CN105444793A CN 105444793 A CN105444793 A CN 105444793A CN 201510785578 A CN201510785578 A CN 201510785578A CN 105444793 A CN105444793 A CN 105444793A
Authority
CN
China
Prior art keywords
fiber bragg
optical
high speed
pulsed laser
bragg grating
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
CN201510785578.7A
Other languages
Chinese (zh)
Other versions
CN105444793B (en
Inventor
邹卫文
雷萌
杨光
陈建平
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.)
Shanghai Jiaotong University
Original Assignee
Shanghai Jiaotong 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 Shanghai Jiaotong University filed Critical Shanghai Jiaotong University
Priority to CN201510785578.7A priority Critical patent/CN105444793B/en
Publication of CN105444793A publication Critical patent/CN105444793A/en
Application granted granted Critical
Publication of CN105444793B publication Critical patent/CN105444793B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • 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
    • G01D5/35338Mechanical 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 other arrangements than interferometer arrangements

Abstract

The invention relates to a fiber Bragg raster sensing device based on a high-speed pulse laser. The fiber Bragg raster sensing device includes the high-speed pulse laser, a dispersion module, a fiber Bragg raster array, a data acquisition module, and a data processing module. Based on the high-speed pulse laser, the narrow pulse being broad in band and high in repetition rate is provided, and the demodulation rate and the dynamic range of a fiber Bragg raster sensing demodulation system is greatly improved. Through the adoption of a photon time stretching method, the measurement of the wavelength shift of the optical fiber Bragg raster in the frequency domain is converted to the measurement of the time shift in the time domain, and the signal processing precision of the time domain is higher. Therefore, the demodulation precision of fiber Bragg sensing system can be significantly improved, and the requirement on the sampling rate of the data acquisition and processing modules is also reduced.

Description

Based on the optical fiber Bragg grating sensing device of high speed pulsed laser
Technical field
The present invention relates to a kind of method and apparatus of sensory field of optic fibre, specifically a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser.
Background technology
Optical fiber has sensing and transmission dual-use function and quality is light, electromagnetism interference, the advantage such as high temperature resistant, corrosion-resistant, fiber Bragg grating sensor except there is the advantage of general Fibre Optical Sensor, also have multiplexing capacity strong, can the advantage of distributed sensing.In recent years, fiber Bragg grating sensor has been a great concern and is rapidly developed, and is widely applied in the monitoring field such as strain, temperature of intelligent building, civil engineering work, medical engineering or other extreme environments.Optical fiber Bragg grating sensing mostly is wavelength-modulated, traditional demodulation mode can be roughly divided into two kinds due to the difference of detection method, the first is based on passive detection, namely frequency discriminator is used Bragg wavelength drift to be converted into the change of light intensity or the displacement in light intensity space, this method can use boundary filter, array waveguide grating, wavelength division multiplexer or realize based on the spectrum charge-coupled image sensor of holographic grating, its advantage is that system is simple, economical, but the signal that the interference of the shake of light source or environment may be taken as sensor is reflected back and causes the precision of demodulation not high, in addition, passive detection is also difficult to realize dynamic sensitive [A.Fender at a high speed, E.J.Rigg, R.R.J.Maier, W.N.MacPherson, J.S.Barton, A.J.Moore, J.D.C.Jones, D.Zhao, L.Zhang, I.Bennion, S.McCulloch, andB.J.S.Jones, " DynamictwoaxiscurvaturemeasurementusingmulticorefiberBra gggratingsinterrogatedbyarrayedwaveguidegrating, " Appl.Opt., vol.45, no.36, pp.9041-9048, Dec.2006].The second is active detection, it is the phase change of Received signal strength based on optical interferometry by the converts displacement of bragg wavelength, the structure of interfering can be that non-balanced Mach increases Dare interferometer, fabry perot interferometer, Michelson interferometer or long period fiber grating, active detection is owing to eliminating the shake of light source, its measuring accuracy is higher than passive detection a lot, but because active mode is based on optical interference, so to environmental perturbation, such as temperature variation or small vibrations, very sensitive, therefore impact can be brought on the stability of system, in addition, demodulation speed based on active detection method has been limited in a few KHz, dynamic range is less [H.Xia also, C.Zhang, H.Mu, andD.Sun, " Edgetechniquefordirectdetectionofstrainandtemperaturebas edonopticaltimedomainreflectometry, " Appl.Opt., vol.48, no.2, pp.189-197, Jan.2009].
But, Fiber Bragg Grating FBG demodulating system at a high speed has very big demand in a lot of research, in order to obtain the optical fiber Bragg grating sensing demodulating system of high speed, high precision, great dynamic range, high speed pulsed laser has been selected as suitable light source, re-use one section of dispersive medium and the ultrashort light pulse that laser instrument sends can be mapped to time domain from frequency domain, its main advantage is that the displacement of bragg wavelength can be mapped to the displacement of time in time domain linearly, so just can be recorded row relax of going forward side by side in real time.
Summary of the invention
The object of the invention is to for the deficiencies in the prior art, a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser is proposed, adopt the narrow pulse laser with high repetition frequency and large bandwidth as light source, improve sensing and demodulating speed and dynamic range.Utilize the principle that photon time stretches, the wavelength shift of frequency domain is mapped to the time shifting of time domain, thus effectively improves demodulation accuracy, and reduce the sampling rate requirement to Back end data acquisition module.
Technical scheme of the present invention is as follows:
A kind of optical fiber Bragg grating sensing device based on high speed pulsed laser, its feature is, comprises high speed pulsed laser, optical splitter, the first dispersion compensation module, optical directional coupler, Fiber Bragg Grating FBG array, the first photodetector, the second dispersion compensation module, the second photodetector, data acquisition module and data processing module;
Described optical splitter in the light pulse direction that described pulsed laser sends, the first via light signal exported from this optical splitter enters the first port of described optical directional coupler through the first described dispersion compensation module, and after the reflection of described Fiber Bragg Grating FBG array, return the second port entering optical directional coupler from the second port input of optical directional coupler, export from the 3rd port of optical directional coupler, described data acquisition module is conveyed into successively after the second described dispersion compensation module and the second photodetector, be converted to electric signal transmission from the second road light signal of described optical splitter output through the first described photodetector and enter described data acquisition module, this data acquisition module respectively with the first described photodetector, second photodetector is connected with data processing module.
Described high speed pulsed laser for generation of the burst pulse with wide range and high repetition frequency, can adopt but be not limited to passive mode-locking fiber laser, Active Mode-locked Fiber Laser is locked to derived reference signal and the method such as multi-laser synthesis realizes.
Described dispersion compensation module is used for light signal to stretch in time domain, can adopt but be not limited to the method realization that single-mode fiber, dispersion compensating fiber, linear chirp optical fiber grating etc. can produce dispersion.
Described photodetector can adopt PIN to manage or APD pipe.
Described optical splitter is optical branching device or photo-coupler.
Described optical directional coupler can be optical circulator also can be photo-coupler.
Described data acquisition module, for gathering time-domain signal, can adopt but be not limited to data collecting card or oscillograph.
The data that described data processing module is used for gathering process, and the deadline is displaced to the conversion of transducing signal, can adopt but be not limited to digital signal processor or computer software.
Based on above technical characterstic, the present invention has the following advantages:
1, the present invention is based on high speed pulsed laser, effectively improve demodulation rate and the dynamic range of current optical fiber Bragg grating sensing demodulating system.
2, the present invention has used the principle that photon time stretches, the wavelength shift of frequency domain is mapped to the time shifting of time domain, improve the demodulation accuracy of current optical fiber Bragg grating sensing demodulating system at double, and reduce the sampling rate requirement to Back end data Acquire and process module.
Accompanying drawing explanation
Fig. 1 is one embodiment of the present of invention figure.
Fig. 2 is the Fiber Bragg Grating FBG demodulation principle figure that the present invention uses photon time stretching principle.
Fig. 3 be the optical fiber Bragg grating sensing device that the present invention is based on high speed pulsed laser obtain time-stretching pulse waveform (a) with the embodiment in Fig. 1, pulse waveform that laser instrument directly exports; (b), pulse waveform after first dispersion compensation module; (c), pulse waveform after second dispersion compensation module.
Fig. 4 is the time domain waveform of Fiber Bragg Grating FBG reflected signal under the experimental result (a) obtained with the embodiment in Fig. 1 of the optical fiber Bragg grating sensing device that the present invention is based on high speed pulsed laser, different external influence; Time shifting-wavelength shift curve under (b), different external influence after photon time stretches.
Embodiment
A specific embodiment of the present invention is provided below in conjunction with accompanying drawing.The present embodiment is implemented premised on technical scheme of the present invention, gives detailed embodiment and process, but protection scope of the present invention should not be limited to following embodiment.
Fig. 1 is one embodiment of the present of invention figure.Its basic comprising comprises: high speed pulsed laser 1, optical splitter 2, first dispersion compensation module 3, optical directional coupler 4, Fiber Bragg Grating FBG array 5, first photodetector 6, second dispersion compensation module 7, second photodetector 8, data acquisition module 9 and data processing module 10.
The annexation of above-mentioned each parts is as follows: described high speed pulsed laser adopts passive mode-locking fiber laser 1, and its ultrashort light pulse produced carries out light splitting by described optical splitter 2; Light splitting Hou mono-road light signal is converted to the data acquisition module 9 described in electric signal access by the first described photodetector 6; Another road light signal is after the first described dispersion compensation module 3, and the chirped optical pulse of generation enters described optical directional coupler 4; The output of described optical directional coupler 4 enters described Fiber Bragg Grating FBG array 5, and the light pulse of returning through sensing back reflection enters described optical directional coupler 4; It exports through the second described dispersion compensation module 7, and the light pulse signal after the second described dispersion compensation module 7 carries out time domain stretching is converted to the data acquisition module 9 described in electric signal access through the second described photodetector 8; Described data processing module 10 processes the data that described data acquisition module 9 collects.
The principle of work of this embodiment as shown in Figure 2.For high speed pulsed laser, owing to having used dispersion and non-linear management, can ultrashort pulse be produced and can wide range be realized, its produce light pulse after the first dispersion compensation module due to GVD (Group Velocity Dispersion) effect, namely velocity of propagation is different in a fiber for the composition of different wave length, chirped optical pulse is drawn as in time domain, Fiber Bragg Grating FBG energy reflection wavelength equals the light of its bragg wavelength, when its effect of outer bound pair, its bragg wavelength can change, therefore sensing can be used for, pulse reflects through Fiber Bragg Grating FBG, the information of the bragg wavelength entrained by it also reflects, then after the second dispersion compensation module in time domain by further broadening, if the dispersion measure of two dispersion compensation module is respectively D 1and D 2, then dispersion drawing coefficient can be expressed as
Adding of these two dispersion compensation module, complete photon time to stretch, the advantage of this scheme is: first, be the displacement of transmission time in time domain by wavelength at the converts displacement of time domain, and the signal transacting precision of time domain is higher, therefore the demodulation accuracy of native system, also namely resolution can be significantly increased; Secondly, pulse stretches in time domain by time-stretching, and frequency domain bandwidth is compressed, and therefore by the lower analog bandwidth in rear end and the data acquisition and procession module quantifies process compared with low sampling rate, thus can reduce the requirement to Back end data Acquire and process module.
The direct acting factor of native system resolution is dispersion draw ratio, namely dispersion draw ratio is larger, resolution is higher, and dispersion drawing coefficient is determined jointly by following factor: the dispersion measure being first two dispersion compensation module, the dispersion measure of second dispersion compensation module is larger, and dispersion drawing coefficient is larger; Next is the repetition frequency of high speed pulsed laser, and repetition frequency is lower, then the recurrent interval is larger, and under the nonoverlapping prerequisite of adjacent pulse, the dispersion drawing coefficient that can realize is larger.
The Fiber Bragg Grating FBG number that native system can use is determined by the bandwidth of high speed pulsed laser, and bandwidth is larger, and the Fiber Bragg Grating FBG number that can use is more.
Native system can be widely used in petroleum industry by the present invention, and geophysics and ocean subject etc. need great dynamic range, fast and the field of high-precision sensing demodulation.

Claims (8)

1. the optical fiber Bragg grating sensing device based on high speed pulsed laser, it is characterized in that, comprise high speed pulsed laser (1), optical splitter (2), the first dispersion compensation module (3), optical directional coupler (4), Fiber Bragg Grating FBG array (5), the first photodetector (6), the second dispersion compensation module (7), the second photodetector (8), data acquisition module (9) and data processing module (10);
At the optical splitter (2) that the light pulse direction that described pulsed laser (1) sends is described, the first via light signal exported from this optical splitter (2) enters the first port of described optical directional coupler (4) through described the first dispersion compensation module (3), and after the reflection of described Fiber Bragg Grating FBG array (5), return the second port entering optical directional coupler (4) from the second port input of optical directional coupler (4), export from the 3rd port of optical directional coupler (4), described data acquisition module (9) is conveyed into successively after described the second dispersion compensation module (7) and the second photodetector (8), the the second road light signal exported from described optical splitter (2) is converted to electric signal transmission through described the first photodetector (6) and enters described data acquisition module (9), this data acquisition module (9) respectively with described the first photodetector (6), second photodetector (8) is connected with data processing module (10).
2. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, it is characterized in that, described high speed pulsed laser is for generation of the burst pulse with high repetition frequency, and for passive mode-locking fiber laser, Active Mode-locked Fiber Laser is locked to derived reference signal or multi-laser synthesizes.
3. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, it is characterized in that, described dispersion compensation module is used for light signal to stretch in time domain, is single-mode fiber, dispersion compensating fiber or linear chirp optical fiber grating.
4. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, is characterized in that, the first described photodetector and the second photodetector adopt PIN pipe or APD pipe.
5. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, it is characterized in that, described optical splitter is optical branching device or photo-coupler.
6. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, is characterized in that, described optical directional coupler (4) is optical circulator or photo-coupler.
7. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, is characterized in that, described data acquisition module, for gathering time-domain signal, is data collecting card or oscillograph.
8. a kind of optical fiber Bragg grating sensing device based on high speed pulsed laser according to claim 1, it is characterized in that, the data that described data processing module is used for gathering process, deadline is displaced to the conversion of transducing signal, is digital signal processor or computer software.
CN201510785578.7A 2015-11-16 2015-11-16 Optical fiber Bragg grating sensing device based on high speed pulsed laser Active CN105444793B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201510785578.7A CN105444793B (en) 2015-11-16 2015-11-16 Optical fiber Bragg grating sensing device based on high speed pulsed laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510785578.7A CN105444793B (en) 2015-11-16 2015-11-16 Optical fiber Bragg grating sensing device based on high speed pulsed laser

Publications (2)

Publication Number Publication Date
CN105444793A true CN105444793A (en) 2016-03-30
CN105444793B CN105444793B (en) 2018-09-14

Family

ID=55555260

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201510785578.7A Active CN105444793B (en) 2015-11-16 2015-11-16 Optical fiber Bragg grating sensing device based on high speed pulsed laser

Country Status (1)

Country Link
CN (1) CN105444793B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106017533A (en) * 2016-06-23 2016-10-12 山东省科学院激光研究所 Rapid tuning real-time calibration fiber grating demodulation device and work method
CN106840221A (en) * 2017-01-06 2017-06-13 武汉理工大学 Fiber grating demodulation device and method based on dispersion Mach Zehnder interferometry
CN107276681A (en) * 2017-05-09 2017-10-20 中国科学院半导体研究所 The incoherent optical signal processing system of nonlinear time-domain stretching is carried out to microwave signal
CN109884704A (en) * 2019-01-18 2019-06-14 潜能恒信能源技术股份有限公司 A kind of device and method for eliminating optical fiber detector system noise
CN114459514A (en) * 2021-12-20 2022-05-10 哈尔滨理工大学 High-speed fiber grating sensing system and method for chirp frequency coding
CN114660790A (en) * 2022-04-06 2022-06-24 中山大学 Optical pulse time stretching device and method and spectral measurement system

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030123771A1 (en) * 2001-11-11 2003-07-03 Yue Liu Optical signal modulation method and optical signal transmission system for high speed transmission system
CN102359763A (en) * 2011-08-09 2012-02-22 中国计量学院 Fully distributed optical fiber Raman and Rayleigh photon sensor of impulse coding fiber laser
CN102645761A (en) * 2012-04-26 2012-08-22 上海交通大学 High speed photoelectric real-time oscilloscope system
CN103018997A (en) * 2012-12-18 2013-04-03 上海交通大学 Continuous signal light analog-digital conversion system based on self-phase modulation effect
CN103808342A (en) * 2014-03-05 2014-05-21 武汉理工大学 High-speed demodulation method and device for high-capacity weak grating sensing network
CN203839695U (en) * 2014-03-24 2014-09-17 杭州电子科技大学 2-micrometer active mode-locking optical fiber laser based on polarization controller
CN104706322A (en) * 2015-03-12 2015-06-17 清华大学 Sweep frequency optical coherent imaging system based on optical calculation

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030123771A1 (en) * 2001-11-11 2003-07-03 Yue Liu Optical signal modulation method and optical signal transmission system for high speed transmission system
CN102359763A (en) * 2011-08-09 2012-02-22 中国计量学院 Fully distributed optical fiber Raman and Rayleigh photon sensor of impulse coding fiber laser
CN102645761A (en) * 2012-04-26 2012-08-22 上海交通大学 High speed photoelectric real-time oscilloscope system
CN103018997A (en) * 2012-12-18 2013-04-03 上海交通大学 Continuous signal light analog-digital conversion system based on self-phase modulation effect
CN103808342A (en) * 2014-03-05 2014-05-21 武汉理工大学 High-speed demodulation method and device for high-capacity weak grating sensing network
CN203839695U (en) * 2014-03-24 2014-09-17 杭州电子科技大学 2-micrometer active mode-locking optical fiber laser based on polarization controller
CN104706322A (en) * 2015-03-12 2015-06-17 清华大学 Sweep frequency optical coherent imaging system based on optical calculation

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
车雅良 等: "大啁啾光纤布拉格光栅的脉冲响应特性研究", 《光学学报》 *

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106017533A (en) * 2016-06-23 2016-10-12 山东省科学院激光研究所 Rapid tuning real-time calibration fiber grating demodulation device and work method
CN106840221A (en) * 2017-01-06 2017-06-13 武汉理工大学 Fiber grating demodulation device and method based on dispersion Mach Zehnder interferometry
CN106840221B (en) * 2017-01-06 2019-03-26 武汉理工大学 Fiber grating demodulation device and method based on dispersion Mach Zehnder interferometry
CN107276681A (en) * 2017-05-09 2017-10-20 中国科学院半导体研究所 The incoherent optical signal processing system of nonlinear time-domain stretching is carried out to microwave signal
CN107276681B (en) * 2017-05-09 2019-05-10 中国科学院半导体研究所 The incoherent optical signal processing system of nonlinear time-domain stretching is carried out to microwave signal
CN109884704A (en) * 2019-01-18 2019-06-14 潜能恒信能源技术股份有限公司 A kind of device and method for eliminating optical fiber detector system noise
CN114459514A (en) * 2021-12-20 2022-05-10 哈尔滨理工大学 High-speed fiber grating sensing system and method for chirp frequency coding
CN114459514B (en) * 2021-12-20 2024-01-30 哈尔滨理工大学 High-speed fiber bragg grating sensing system and method for chirp frequency coding
CN114660790A (en) * 2022-04-06 2022-06-24 中山大学 Optical pulse time stretching device and method and spectral measurement system

Also Published As

Publication number Publication date
CN105444793B (en) 2018-09-14

Similar Documents

Publication Publication Date Title
CN105444793B (en) Optical fiber Bragg grating sensing device based on high speed pulsed laser
CN101634571B (en) Optical pulse raster distributed fiber sensing device
CN102384799B (en) Frequency sweeping and data processing method based on Brillouin distributed fiber sensing system correlation detection scheme
CN102901525B (en) Ultra-large capacity time division and wavelength division fiber grating sensing system and query method thereof
CN102607621A (en) Distributed optical fiber Brillouin sensing device and method thereof for detecting temperature and strain synchronously
CN101650509B (en) Bragg grating high-speed demodulating system based on cascade-connection long period fiber grating
CN201876324U (en) Double-light source light path structure of distributed optical fiber Raman temperature sensor
CN106802160B (en) Fiber grating sensing demodulation system and method based on fork-shaped interference pattern
CN101298992A (en) Distributed type fiber optic sensor based on optical fiber cavity attenuation and vibration technique
CN101373145A (en) Embedded type multichannel high speed optical fiber grating sensor demodulation system
CN106643832A (en) Phase-sensitive optical time-domain reflectometer based on linear frequency-modulation pulse and measurement method of phase-sensitive optical time-domain reflectometer
CN204027726U (en) A kind of distributed optical fiber sensing system based on Brillouin scattering
CN101532850B (en) Method and device for sensing and demodulating Bragg fiber grating
CN109959403B (en) Multi-parameter large-capacity sensing system
CN1955640A (en) Fibre-optical grating sensor and its wavelength demodulation method and sensor
CN102269573A (en) Quasi-distributed composite structure strain and temperature detection system
CN103697922A (en) High-speed demodulation system of optical fiber F-P cavity sensor
CN110375781A (en) The self-adapting data acquisition system of variable measurement range in a kind of OFDR
CN103438915A (en) F-P sensor multiplexing method and system based on frequency shift interference
CN107356275A (en) A kind of method that spectral resolution is improved in optical frequency domain reflection-based optical fiber distributed sensing
CN102853936A (en) Remote distributed fiber Raman temperature sensor
CN203929276U (en) A kind of optical signal detecting disposal system based on resonance technique
CN104729750A (en) Distributed optical fiber temperature sensor based on Brillouin scattering
CN103175555A (en) Multi-parameter distributed fiber-optic sensor based on multi-mechanism fusion
CN110375779A (en) The device and method for improving OFDR frequency domain sample rate

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant