CN202195825U - Extra-long distance pulse-coding distributed optical fiber Raman and Brillouin photon sensor - Google Patents
Extra-long distance pulse-coding distributed optical fiber Raman and Brillouin photon sensor Download PDFInfo
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- CN202195825U CN202195825U CN2011202864433U CN201120286443U CN202195825U CN 202195825 U CN202195825 U CN 202195825U CN 2011202864433 U CN2011202864433 U CN 2011202864433U CN 201120286443 U CN201120286443 U CN 201120286443U CN 202195825 U CN202195825 U CN 202195825U
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Abstract
The utility model discloses an extra-long distance pulse-coding distributed optical fiber Raman and Brillouin photon sensor which is used for measuring temperature and strain and is formed by utilizing a pulse coding principle, an optical fiber stimulated Raman scattering effect, a spontaneous Raman scattering temperature effect, a spontaneous Brillouin scattering strain effect and an optical time domain reflecting principle. In the sensor, the amplified pulse-coding reverse anti-Stokes Raman scattered light and the amplified pulse-coding reverse Stokes Raman scattered light can be respectively input to a direct detection system by two optoelectronic receiving modules to be decoded and demodulated, and the strength ratio of the amplified pulse-coding reverse anti-Stokes Raman scattered light and the amplified pulse-coding reverse Stokes Raman scattered light can be measured, so as to obtain the temperature information of all the segments of an optical fiber. Beating frequency is carried out on the amplified pulse-coding reverse optical fiber Brillouin scattered light and the local light of an outer cavity narrow-band optical fiber laser for coherent detection, and the strain information of all the segments of the optical fiber can be obtained by decoding and demodulating frequency shift. The sensor adopts time series coding laser pulse, thereby effectively increasing the number of photons of the incident sensing optical fiber and improving the signal to noise ratio, so as to increase the measuring length and improve the measuring accuracy and the space resolution.
Description
Technical field
The utility model relates to very-long-range pulse code distributed fiber Raman and Brillouin's photon sensor of integrated optical fiber Raman amplifier, belongs to the fiber optic sensor technology field.
Background technology
In the distributed fiberoptic sensor field; There is distributed fiber Raman scattered photon temperature sensor to detect field temperature both at home and abroad; There is distribution type fiber-optic Brillouin scattering photon sensor to detect on-the-spot strain and temperature abroad, owing to there is cross effect, the strain and the temperature of measuring optical fiber simultaneously; Newson research team of Southampton, Britain university proposes to adopt the laser of narrowband light source to utilize the spontaneous dorsad anti-Stokes Raman scattering thermometric of optical fiber and measure strain with spontaneous optical fiber Brillouin scattering effect; But, therefore, measure the low (M.N.Allahbabi of precision of temperature and strain because the spectral bandwidth of optical fiber Brillouin scattering is very narrow; Y.T.Cho and T.P.Newson
Simulataneous Distributed Measurements of Temperature and Strain using Spontaneous Raman and Brillouin Scattering, Optics Letters,2005,1 June, p.1276-1278).Zhang Zaixuan research team of the China Measures Institute proposes to adopt the LASER Light Source of two different spectral bandwidths; Adopt the temperature of the fiber raman scattering strength ratio measuring optical fiber of wideband light source; The strain of the deviation ratio measuring optical fiber of the optical fiber Brillouin scattered ray of employing narrow-band light source; Tentatively solved strain and temperature simultaneously measuring problem (Zhang Zaixuan etc. " very-long-range distributed fiber Raman and Brillouin's photon sensor ", ZL200710156868.0); The China Measures Institute is eastwards surplus; It is (eastwards surplus that propositions such as Zhang Zaixuan are applied to the fully distributed fiber sensor with the pulse code technology; Zhang Zaixuan etc. " adopting the distributed optical fiber Raman temperature sensor of train pulse coding and decoding " CN101819073A) adopt the pulse code technology to improve the photon number that transmits in optical fiber sensing system, make Raman scattering light intensity dorsad improve; Improve the signal to noise ratio (S/N ratio) of system, thereby improved the signal to noise ratio (S/N ratio) of system greatly.Merge the pulse code technology; Fiber raman scattering, Brillouin scattering technology; The excited Raman amplifying technique can improve measuring distance and measuring accuracy effectively; Satisfy the safety and Health monitoring of petroleum pipe line, transferring electric power cable in recent years, to the active demand of the strain of very-long-range 100km fully distributed fiber, TEMP net.
Summary of the invention
The purpose of the utility model is to propose a kind of very-long-range pulse code distributed fiber Raman and Brillouin's photon sensor, to realize the measurement length of increase system, improves the precision of measuring temperature and strain simultaneously.
The very-long-range pulse code distributed fiber Raman of the utility model and Brillouin's photon sensor pack are drawn together waveform generator, semiconductor exocoel narrow-band impulse fiber laser, semiconductor FP chamber band optical fiber laser instrument; The optical fiber channel-splitting filter, pulse code photomodulator, optical fiber wave multiplexer; Isolator, fibre optic Raman laser, pumping-signal optical fibre coupling mechanism; Bidirectional coupler, very-long-range single-mode fiber, fiber grating narrow band reflective filter; Wavelength division multiplexer; Two photoelectricity receiver modules, direct detection system, two narrow band fiber grating filters; Pass through circulator; Coherent Detection system and industrial computer, the output terminal of industrial computer links to each other with the input end of waveform generator, and an output terminal of waveform generator links to each other with the input end of semiconductor FP chamber band optical fiber laser instrument; Another output terminal of waveform generator links to each other with an input end of pulse code photomodulator; The output terminal of semiconductor FP chamber band optical fiber laser instrument links to each other with an input end of optical fiber wave multiplexer, and the output terminal of semiconductor exocoel narrow-band impulse fiber laser links to each other with the input end of optical fiber channel-splitting filter, and an output terminal of optical fiber channel-splitting filter links to each other with another input end of pulse code photomodulator; Another output terminal warp second narrow band fiber grating filter of optical fiber channel-splitting filter links to each other with an input end through circulator; The output terminal of pulse code photomodulator links to each other with another input end of optical fiber wave multiplexer, and the output terminal of optical fiber wave multiplexer links to each other with the input end of isolator, and the output terminal of isolator links to each other with an input end of pumping-signal optical fibre coupling mechanism; Another input end of pumping-signal optical fibre coupling mechanism links to each other with fibre optic Raman laser; Pumping-the output terminal of signal optical fibre coupling mechanism links to each other with the input end of bidirectional coupler, and an output terminal of bidirectional coupler connects the very-long-range single-mode fiber, and another output terminal of bidirectional coupler links to each other with the input end of wavelength division multiplexer through the fiber grating narrow band reflective filter; An output terminal of wavelength division multiplexer links to each other with an input end of direct detection system through the first photoelectricity receiver module; Another output terminal of wavelength division multiplexer links to each other with another input end of direct detection system through the second photoelectricity receiver module, and the 3rd output terminal of wavelength division multiplexer links to each other with the input end of the first narrow band fiber grating filter, and directly the output terminal of detection system links to each other with an input end of industrial computer; The output terminal of the first narrow band fiber grating filter links to each other with another input end through circulator, and the output terminal through circulator links to each other with another input end of industrial computer through the Coherent Detection system.
In the utility model, described semiconductor FP chamber band optical fiber laser instrument is made up of the F-P semiconductor laser, and its centre wavelength is 1550nm, and spectral width is 3nm, the unit pulse width < 6ns of laser.
In the utility model, described semiconductor exocoel narrow-band impulse fiber laser is that centre wavelength is 1555nm, and spectral bandwidth is the fiber laser that the 20mW of 200kHz moves continuously.
In the utility model, described encoded light modulator is lithium niobate Mach-Ze Deer modulator (Mach – Zehnder modulator (MZM)).
In the utility model, described fibre optic Raman laser is that wavelength is the adjustable power fibre optic Raman laser of 1465nm.It and pumping-signal optical fibre coupling mechanism and very-long-range 100km single-mode fiber are combined into the pumped distributed fiber Raman amplifier of forward direction of a Gain Adjustable.
In the utility model, described fiber grating narrowband reflection wave filter is high reflectance, high-isolation (greater than 35dB), and wavelength is spaced apart the fiber grating reflective filter of 0.3nm for the 1465nm narrow-band spectrum.
In the utility model, described wavelength division multiplexer has four ports, an input port; Three output ports, first output port are the 1450nm ports, are optical fiber anti-Stokes Raman diffused light delivery outlet; Second output port is the 1660nm port; Be optical fiber Stokes Raman diffused light delivery outlet, the 3rd output port is the 1550nm port, is fiber Rayleigh and Brillouin scattering delivery outlet.
In the utility model, the described first narrow band fiber grating filter is that centre wavelength is 1555.08nm, and spectral bandwidth is 0.1nm, the fiber grating of loss < 0.3dB, isolation>35dB.The second narrow band fiber grating filter is that centre wavelength is 1555.0nm, and spectral bandwidth is 0.1nm, the fiber grating of loss < 0.3dB, isolation>35dB.
In the utility model, described Coherent Detection system is the spectrum analyzer of spectral range 9kHz-26.5GHz.
Very-long-range pulse code distributed fiber Raman and Brillouin's photon sensor are based on the nonlinear fiber optical scattering and merge principle, wavelength-division multiplex principle and pulse code principle; Utilize optical fiber stimulated Raman scattering effect, the measurement temperature that the temperature effect of spontaneous Raman scattering and spontaneous brillouin scattering strain effect and optical time domain reflection principle are processed and the sensor of strain.
The coding and decoding principle of pulse code distributed Raman, Brillouin scattering Fibre Optical Sensor:
The train pulse coding of this sensor realizes that through s-matrix conversion the s-matrix conversion is a kind of variant that the standard hadamard gets (Hadamard) conversion, and also can be described as hadamard must change.The element of s-matrix is formed by " 0 " and " 1 ", and these characteristics are applicable to laser train pulse coding very much, and on behalf of laser instrument, available in practical application " O " close, and represents laser instrument to open with " 1 ".The coded system of this employing " 0 ", " 1 " can be described as simple code again.And the process of decoding is corresponding contrary s-matrix conversion.
Learn by the coding principle derivation, adopt the obtainable signal to noise ratio (S/N ratio) of train pulse coding and decoding of N position to be improved as:
Can know that by (1) formula signal to noise ratio (S/N ratio) is improved along with the raising of coding figure place and improved.
When N gets 255:
The space orientation resolution of Fibre Optical Sensor is by the narrow pulse width decision of unit; Owing to adopt the multiple-pulse emission; When improving the ballistic phonon number, can improve spatial resolution through pressing narrow laser pulse width again, and needn't improve single peak-power of laser pulse from and prevented that effectively fiber nonlinear effect from causing the distortion of anti-Stokes Raman light Time Domain Reflectometry (OTDR) curve dorsad.
Excited Raman amplifier principle:
When frequency is ν
0Incident laser and optical fiber molecule produce the nonlinear interaction scattering, emit a phonon and be called Stokes Raman scattering photon ν=ν
0-Δ ν absorbs a phonon and is called anti-Stokes Raman scattering photon ν
0+ Δ ν, the phonon frequency of optical fiber molecule is Δ ν, numerical value is 13.2THz.Can be expressed as
ν=ν
0±Δν （2）
The turn off gain of amplifier does
Wherein
Be the pump light power input of amplifier,
I 0 Be light intensity,
Be the free area of optical fiber,
Be Raman gain coefficienct,,
Be the effective interaction length (having considered the absorption loss of optical fiber to pumping) of optical fiber, its expression formula is following:
（4）
Wherein
Be the fibre loss at pump frequency place,
LBe fiber lengths, for fiber Raman amplifier, pump power has only when surpassing a certain threshold value, just might produce excited Raman to signal and amplify the stokes wave in optical fiber
ν=ν 0 -Δ νIn fiber medium, increase fast, the power of most of pump light can convert stokes light to, and Raman amplification is arranged, and gain can suppress the loss of optical fiber, improves the operating distance of fully distributed fiber strain, temperature sensor.
The temperature-measurement principle of fiber raman scattering: the strength ratio of anti-Stokes Raman diffused light and Stokes Raman diffused light
I (T):
Wherein
Be the level value after opto-electronic conversion,
ν a ,
ν s Be respectively the frequency of anti-Stokes Raman scattering photon and Stokes Raman scattering photon, h is Bo Langke (Planck) constant, h=6.626 068 76.52 x10
-34J.s (physics constant data in 1998), Δ ν are that the phonon frequency of an optical fiber molecule is 13.2THz, and k is a Boltzmann constant, k=1.380 650324x10
-23JK
-1, T is Kai Erwen (Kelvin) absolute temperature.By both strength ratios, obtain the temperature information of each section of optical fiber.
The measurement strain of optical fiber Brillouin scattering, temperature principle:
In optical fiber; The nonlinear interaction of sound wave in the laser of incident optical and the optical fiber, light wave produces sound wave through electrostriction, causes the periodic modulation (refractive-index grating) of optical fibre refractivity; Produce the Brillouin scattering that frequency moves down, the frequency displacement of the Brillouin scattering dorsad that in optical fiber, produces
ν B For:
ν B =2nv/λ （6）
Wherein n is the refractive index at lambda1-wavelength λ place, and v is the velocity of sound in the optical fiber, to silica fibre, and near λ=1550nm,
ν B Be about 11GHz.
（7）
The frequency displacement of Brillouin scattering
The coefficient of strain C of frequency displacement wherein
ν εWith temperature coefficient C
ν ΤFor
Through measuring optical fiber dorsad the frequency displacement of brillouin line obtain the dependent variable of each section on the optical fiber.
The beneficial effect of the utility model is:
The utility model merges principle, excited Raman amplification principle based on the nonlinear fiber optical scattering; Wavelength-division multiplex principle and pulse code principle adopt time series coding laser pulse, when improving the ballistic phonon number, can improve spatial resolution through pressing narrow laser pulse width again; Improved the signal to noise ratio (S/N ratio) of sensor-based system; The excited Raman gain can suppress the loss of optical fiber, improves the operating distance of fully distributed fiber strain, temperature sensor, has improved the measuring accuracy of sensor-based system.When online temperature and strain are realized in the space, measure and improved measuring accuracy.
Description of drawings
Fig. 1 is the very-long-range pulse code distributed fiber Raman of the utility model and the synoptic diagram of Brillouin's photon sensor.
Embodiment
With reference to Fig. 1, the very-long-range pulse code distributed fiber Raman of invention and Brillouin's photon sensor comprise waveform generator 9; Semiconductor exocoel narrow-band impulse fiber laser 10, semiconductor FP chamber band optical fiber laser instrument 11, optical fiber channel-splitting filter 12; Pulse code photomodulator 13, optical fiber wave multiplexer 14, isolator 15; Fibre optic Raman laser 16, pumping-signal optical fibre coupling mechanism 17, bidirectional coupler 18; Very-long-range single-mode fiber 19, fiber grating narrow band reflective filter 20, wavelength division multiplexer 21; Two photoelectricity receiver modules 22,23; Direct 24, two narrow band fiber grating filters of detection system 25,26 are through circulator 27; Coherent Detection system 28 and industrial computer 29; The output terminal of industrial computer 29 links to each other with the input end of waveform generator 9, and an output terminal of waveform generator 9 links to each other with the input end of semiconductor FP chamber band optical fiber laser instrument 11, and another output terminal of waveform generator 9 links to each other with an input end of pulse code photomodulator 13; The output terminal of semiconductor FP chamber band optical fiber laser instrument 11 links to each other with an input end of optical fiber wave multiplexer 14; The output terminal of semiconductor exocoel narrow-band impulse fiber laser 10 links to each other with the input end of optical fiber channel-splitting filter 12, and an output terminal of optical fiber channel-splitting filter 12 links to each other with another input end of pulse code photomodulator 13, and another output terminal warp second narrow band fiber grating filter 26 of optical fiber channel-splitting filter 12 links to each other with an input end through circulator 27; The output terminal of pulse code photomodulator 13 links to each other with another input end of optical fiber wave multiplexer 14; The output terminal of optical fiber wave multiplexer 14 links to each other with the input end of isolator 15, and the output terminal of isolator 15 links to each other with an input end of pumping-signal optical fibre coupling mechanism 17, and another input end of pumping-signal optical fibre coupling mechanism 17 links to each other with fibre optic Raman laser 16; The output terminal of pumping-signal optical fibre coupling mechanism 17 links to each other with the input end of bidirectional coupler 18; An output terminal of bidirectional coupler 18 connects very-long-range single-mode fiber 19, and another output terminal of bidirectional coupler 18 links to each other through the input end of fiber grating narrow band reflective filter 20 with wavelength division multiplexer 21, and the 1450nm port of wavelength division multiplexer 21 links to each other with an input end of direct detection system 24 through the first photoelectricity receiver module 22; The 1660nm port of wavelength division multiplexer 21 links to each other with another input end of direct detection system 24 through the second photoelectricity receiver module 23, and the 1550nm port of wavelength division multiplexer 21 links to each other with the input end of the first narrow band fiber grating filter 25.Directly the output terminal of detection system 24 links to each other with an input end of industrial computer 29; The output terminal of the first narrow band fiber grating filter 25 links to each other with another input end through circulator 27, and the output terminal through circulator 27 links to each other with another input end of industrial computer 29 through Coherent Detection system 28.
During work, waveform generator 9 is under industrial computer 29 controls, and output is pressed
255 coded pulses of the sequence that the s-matrix transformation rule is arranged drive semiconductor FP chamber band optical fiber laser instrument 11, produce the time series coding laser pulse in broadband, through the optical fiber wave multiplexer
, Bidirectional coupler 18 Rayleigh scattering, Brillouin scattering and the Raman diffused light that optical fiber is reverse reflects away through the Rayleigh scattering of fiber grating narrow band reflective filter 20 with harmful fiber Raman amplifier pump light; Anti-Stokes that will amplify through fiber Raman amplifier through the scattered light that filters two ports through wavelength division multiplexer 21 and Stokes Raman diffused light pass through the first photoelectricity receiver module 22, the second photoelectricity receiver module 23 respectively; Get into direct detection system 24; Measure both strength ratios; Obtain the temperature information of each section of optical fiber; Coded pulse decoding demodulation through direct detection system 24 and industrial computer 29 will be gathered, add up obtains 100km sensor fibre place field temperature information.
Semiconductor exocoel narrow-band impulse fiber laser 10 connects the pulse code photomodulator 13 by waveform generator 10 controls of industrial computer 29 generations successively through an output terminal of optical fiber channel-splitting filter 12, produces the time series coding laser pulse of arrowband.The reverse optical fiber Brillouin scattering that wavelength division multiplexer 21 will amplify through fiber Raman amplifier; Through narrow band fiber grating filter 25; Through circulator 27 this flash of light preceding an earthquake with the exocoel narrow band fiber laser instrument of process narrow band fiber grating filter 26; Carry out Coherent Detection through Coherent Detection system 28 beat frequencies, through the coded pulse decoding demodulation that Coherent Detection system 28 and industrial computer 29 will be gathered, add up, measure frequency displacement acquisition 100km sensor fibre strain information at the scene.Adopt the coded light pulses sequence of pulse code principle on time domain, increased the photon number of incident optical effectively, improved the signal to noise ratio (S/N ratio) of sensing system, increased the measurement length of sensor, improved the reliability and the spatial resolution of sensor.Send the temperature on the sensor fibre, strain information to the remote monitoring net through internet or wireless network by industrial computer.
In the utility model; Described direct detection system is to detect 1450nm by the optical fiber anti-Stokes Raman scattering of fiber Raman amplifier amplification and the strength ratio of 1660nm Stokes Raman scattering; Coded pulse decoding demodulation through digital signal processor and industrial computer will be gathered, add up obtains 100km sensor fibre place field temperature information and sends the remote monitoring net to.
In the utility model; Described Coherent Detection system detects the heterodyne signal of local signal of excited Brillouin echoed signal and arrowband single frequency optical fiber laser of the relevant amplification of sensor fibre; The coded pulse decoding demodulation that to gather, add up by Coherent Detection system and industrial computer, obtain the 100km sensor fibre at the scene strain, temperature information and send the remote monitoring net to.
Claims (9)
1. a very-long-range pulse code distributed fiber Raman and Brillouin's photon sensor is characterized in that comprising that waveform sends out
Give birth to device (9), semiconductor exocoel narrow-band impulse fiber laser (10), semiconductor FP chamber band optical fiber laser instrument (11); Optical fiber channel-splitting filter (12), pulse code photomodulator (13), optical fiber wave multiplexer (14); Isolator (15); Fibre optic Raman laser (16), pumping-signal optical fibre coupling mechanism (17), bidirectional coupler (18); Very-long-range single-mode fiber (19); Fiber grating narrow band reflective filter (20), wavelength division multiplexer (21), two photoelectricity receiver modules (22,23); Direct detection system (24); Two narrow band fiber grating filters (25,26), through circulator (27), Coherent Detection system (28) and industrial computer (29); The output terminal of industrial computer (29) links to each other with the input end of waveform generator (9); An output terminal of waveform generator (9) links to each other with the input end of semiconductor FP chamber band optical fiber laser instrument (11), and another output terminal of waveform generator (9) links to each other with an input end of pulse code photomodulator (13), and the output terminal of semiconductor FP chamber band optical fiber laser instrument (11) links to each other with an input end of optical fiber wave multiplexer (14); The output terminal of semiconductor exocoel narrow-band impulse fiber laser (10) links to each other with the input end of optical fiber channel-splitting filter (12); An output terminal of optical fiber channel-splitting filter (12) links to each other with another input end of pulse code photomodulator (13), and another output terminal warp second narrow band fiber grating filter (26) of optical fiber channel-splitting filter (12) links to each other with an input end through circulator (27), and the output terminal of pulse code photomodulator (13) links to each other with another input end of optical fiber wave multiplexer (14); The output terminal of optical fiber wave multiplexer (14) links to each other with the input end of isolator (15); The output terminal of isolator (15) links to each other with an input end of pumping-signal optical fibre coupling mechanism (17), and another input end of pumping-signal optical fibre coupling mechanism (17) links to each other with fibre optic Raman laser (16), and the output terminal of pumping-signal optical fibre coupling mechanism (17) links to each other with the input end of bidirectional coupler (18); An output terminal of bidirectional coupler (18) connects very-long-range single-mode fiber (19); Another output terminal of bidirectional coupler (18) links to each other through the input end of fiber grating narrow band reflective filter (20) with wavelength division multiplexer (21), and an output terminal of wavelength division multiplexer (21) links to each other through the input end of the first photoelectricity receiver module (22) with direct detection system (24), and another output terminal of wavelength division multiplexer (21) links to each other through second photoelectricity receiver module (23) another input end with direct detection system (24); The 3rd output terminal of wavelength division multiplexer (21) links to each other with the input end of the first narrow band fiber grating filter (25); Directly the output terminal of detection system (24) links to each other with an input end of industrial computer (29), and the output terminal of the first narrow band fiber grating filter (25) links to each other with another input end through circulator (27), and the output terminal through circulator (27) links to each other with another input end of industrial computer (29) through Coherent Detection system (28).
2. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor; The centre wavelength that it is characterized in that semiconductor FP chamber band optical fiber laser instrument (11) is 1550nm; Spectral width is 3nm, the unit pulse width < 6ns of laser.
3. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor; The centre wavelength that it is characterized in that semiconductor exocoel narrow-band impulse fiber laser (10) is 1555nm, and spectral bandwidth is the fiber laser that the 20mW of 200kHz moves continuously.
4. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor is characterized in that pulse code photomodulator (13) is lithium niobate Mach-Ze Deer modulator.
5. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor is characterized in that fibre optic Raman laser (16) is that wavelength is the adjustable power fibre optic Raman laser of 1465nm.
6. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor is characterized in that fiber grating narrowband reflection wave filter (20) is wavelength is spaced apart 0.3nm for the 1465nm narrow-band spectrum a fiber grating reflective filter.
7. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor; It is characterized in that wavelength division multiplexer (21) has four ports, an input port, three output ports; First output port is the 1450nm port; Be optical fiber anti-Stokes Raman diffused light delivery outlet, second output port is the 1660nm port, is optical fiber Stokes Raman diffused light delivery outlet; The 3rd output port is the 1550nm port, is fiber Rayleigh and Brillouin scattering delivery outlet.
8. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor; It is characterized in that the first narrow band fiber grating filter (25) is that centre wavelength is 1555.08nm; Spectral bandwidth is 0.1nm, the fiber grating of loss < 0.3dB, isolation>35dB; The second narrow band fiber grating filter (26) is that centre wavelength is 1555.0nm, and spectral bandwidth is 0.1nm, the fiber grating of loss < 0.3dB, isolation>35dB.
9. very-long-range pulse code distributed fiber Raman according to claim 1 and Brillouin's photon sensor is characterized in that Coherent Detection system (28) is the spectrum analyzer of spectral range 9kHz-26.5GHz.
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Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102322808A (en) * | 2011-08-09 | 2012-01-18 | 中国计量学院 | Very long range pulse coding distribution type Fiber Raman and Brillouin photon sensor |
| CN105806510A (en) * | 2016-04-20 | 2016-07-27 | 青岛派科森光电技术股份有限公司 | Embedded single-mode distributed optical fiber sensing system based on light source encoding |
| CN107817012A (en) * | 2016-09-14 | 2018-03-20 | 通用汽车环球科技运作有限责任公司 | Sensor and production and preparation method thereof |
| CN108534910A (en) * | 2018-03-19 | 2018-09-14 | 浙江师范大学 | A kind of distributed dual sampling method based on Asymmetric Twin-Core Fiber |
| CN110715929A (en) * | 2019-10-14 | 2020-01-21 | 长安大学 | Distributed strain micro crack detection system and method based on stacking self-encoder |
| CN111006701A (en) * | 2019-12-30 | 2020-04-14 | 暨南大学 | Bipolar differential phase coding Brillouin optical time domain reflectometer with ultrahigh spatial resolution |
-
2011
- 2011-08-09 CN CN2011202864433U patent/CN202195825U/en not_active Expired - Lifetime
Cited By (9)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN102322808A (en) * | 2011-08-09 | 2012-01-18 | 中国计量学院 | Very long range pulse coding distribution type Fiber Raman and Brillouin photon sensor |
| CN102322808B (en) * | 2011-08-09 | 2013-03-27 | 中国计量学院 | Very long range pulse coding distribution type Fiber Raman and Brillouin photon sensor |
| CN105806510A (en) * | 2016-04-20 | 2016-07-27 | 青岛派科森光电技术股份有限公司 | Embedded single-mode distributed optical fiber sensing system based on light source encoding |
| CN107817012A (en) * | 2016-09-14 | 2018-03-20 | 通用汽车环球科技运作有限责任公司 | Sensor and production and preparation method thereof |
| US10591549B2 (en) | 2016-09-14 | 2020-03-17 | GM Global Technology Operations LLC | Sensor and method of making and using the same |
| CN108534910A (en) * | 2018-03-19 | 2018-09-14 | 浙江师范大学 | A kind of distributed dual sampling method based on Asymmetric Twin-Core Fiber |
| CN110715929A (en) * | 2019-10-14 | 2020-01-21 | 长安大学 | Distributed strain micro crack detection system and method based on stacking self-encoder |
| CN111006701A (en) * | 2019-12-30 | 2020-04-14 | 暨南大学 | Bipolar differential phase coding Brillouin optical time domain reflectometer with ultrahigh spatial resolution |
| CN111006701B (en) * | 2019-12-30 | 2021-05-07 | 暨南大学 | Bipolar differential phase coding Brillouin optical time domain reflectometer with ultrahigh spatial resolution |
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