CN106052730B - A kind of signal demodulating method and device for distributed fiber-optic sensor system - Google Patents

A kind of signal demodulating method and device for distributed fiber-optic sensor system Download PDF

Info

Publication number
CN106052730B
CN106052730B CN201610607797.0A CN201610607797A CN106052730B CN 106052730 B CN106052730 B CN 106052730B CN 201610607797 A CN201610607797 A CN 201610607797A CN 106052730 B CN106052730 B CN 106052730B
Authority
CN
China
Prior art keywords
optical pulse
pulse code
code sequence
signal
impulse response
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.)
Active
Application number
CN201610607797.0A
Other languages
Chinese (zh)
Other versions
CN106052730A (en
Inventor
洪小斌
王晟
杨智生
吴晓晓
林文桥
伍剑
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.)
Beijing University of Posts and Telecommunications
Original Assignee
Beijing University of Posts and Telecommunications
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 Beijing University of Posts and Telecommunications filed Critical Beijing University of Posts and Telecommunications
Priority to CN201610607797.0A priority Critical patent/CN106052730B/en
Publication of CN106052730A publication Critical patent/CN106052730A/en
Application granted granted Critical
Publication of CN106052730B publication Critical patent/CN106052730B/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
    • G01D5/3537Optical fibre sensor using a particular arrangement of the optical fibre itself
    • G01D5/35377Means for amplifying or modifying the measured quantity
    • 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

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Testing Of Optical Devices Or Fibers (AREA)
  • Optical Communication System (AREA)

Abstract

The invention discloses a kind of signal demodulating method and device for distributed fiber-optic sensor system, obtains the signal after an optical pulse code sequence and optical pulse code sequence and the impulse response convolution of testing fiber;By the signal after the optical pulse code sequence and convolution of acquisition, respectively by Fourier transform to frequency domain, according to the signal after the optical pulse code sequence and convolution after conversion, the impulse response of the testing fiber under frequency domain is calculated;The obtained impulse response of testing fiber under frequency domain is converted into by time domain by inverse fourier transform, obtains the impulse response of testing fiber.The present invention is used for the signal demodulating method and device of distributed fiber-optic sensor system, is inputted using pulsatile once, and it is this condition of impulse response no at all to consider the sum of complementary Gray code auto-correlation, therefore reduces demodulating error.

Description

A kind of signal demodulating method and device for distributed fiber-optic sensor system
Technical field
The invention belongs to signal demodulation techniques field, and in particular to a kind of signal solution for distributed fiber-optic sensor system Adjust method and device.
Background technology
Distributed fiber-optic sensor system is using light wave as transducing signal, using optical fiber as transmission medium, can perceive and demodulate and is outer Boundary's measurand is with time and the continuously distributed information in space, since optical fiber itself is not charged, small, light weight, pliable Song, electromagnetism interference, radiation resistance are good, can particularly be adapted under the adverse circumstances such as inflammable, explosive and strong electromagnetic Use so that it has extensive in key areas such as following intelligent grid, Oilfield Pipelines security monitoring, communication line attack early warnings Application demand.Distributed fiber-optic sensor technology is divided into based on Rayleigh scattering, based on Raman scattering, the biography based on Brillouin scattering Sense technology.
The spatial resolution both direction of distributed fiber-optic sensor technology towards farther distance sensing and higher develops. Optical pulse code is then an important way of lifting system distance sensing.The core concept of optical pulse code technology, is to use The length that the symbol " 1 " by intensity modulated of specific rule and " 0 " form (is commonly divided into for L optical pulse code sequences Simplex is encoded and complementary Gray code), to replace the single pumping pulse in sensing solutions, then the response song that solution is transferred to Line is decoded using corresponding decoding process, the lifting system signal-to-noise ratio on the premise of time of measuring is not changed, and then is extended Distance sensing.Optical pulse code technology is widely used in various optical fiber sensing systems, such as optical time domain reflection (OTDR), Raman Optical time domain reflection (ROTDR), Brillouin light Time Domain Reflectometry (BOTDR), Brillouin optical time domain analysis (BOTDA).
By taking bipolarity Gray code as an example, cataloged procedure is as follows:By specific two code lengths of law generation be L and The complementary Gray code light pulse sequence A being made of symbol " 1 " and " -1 "kAnd Bk.Due to light arteries and veins in OTDR, ROTDR, BOTDR Punching cannot be negative, so AkA by being made of accordingly symbol " 1 " and symbol " 0 " againk1,Ak2Make the difference to obtain, BkAgain by corresponding The B being made of symbol " 1 " and symbol " 0 "k1,Bk2Make the difference to obtain.Can be by gain-type pulse and attenuation type pulse in BOTDA Form " 1 " and " -1 " code.AkAnd BkRelation should meet:
Ak*Ak+Bk*Bk=2L δk (1)
Wherein * represents related operator, as shown in Figure 1.And δkRepresent discrete impulse function, expression formula is:
By designed complementary Gray code light pulse sequence AkAnd BkIncident optical respectively, the impulse response h with optical fiberk After carrying out convolution, two groups of different responses are respectively obtained, i.e.,With
The optical fiber impulse response h of corresponding above-mentioned cataloged procedurekDemodulating process it is as follows:By above-mentioned two groups of different responses point Not with corresponding original, complementary gray-code sequence AkAnd BkRelevant operation is carried out, and two groups of responses after relevant operation are summed, The optical fiber impulse response of signal-to-noise ratio lifting is can obtain, expression formula is:
According to the characteristic of Complementary Golay sequences, the main peak of the auto-correlation function of the two is identical, and secondary lobe is complementary.Auto-correlation letter After number summation obtains sensing function, the amplitude of main peak doubles, and secondary lobe is cancelled out each other.
But in actual application system, as shown in Fig. 2, the laser that laser is sent, by by waveform generator (AWG) electrooptic modulator (EOM) of control, forms the pulse after coding.After amplifying by erbium-doped fiber amplifier (EDFA), Enter by circulator in testing fiber.
EDFA cannot be guaranteed that identical gain is amplified when to Optical pulse amplification, for continuous light pulse, therefore pass through After crossing EDFA, relatively after light pulse amplitude can be relatively low, it is inconsistent the symbol power of diverse location occur, as shown in Figure 3.It is difficult at this time To ensure formula (1), as shown in figure 4, so as to which in demodulation, the sum of complementary Gray code auto-correlation is not impulse response but is rushing Swash the secondary lobe that response side occurs, cause measurement error.Simulated using the impulse response of 20km optical fiber as Fig. 5.It is demodulated Afterwards, the response obtained is Fig. 6.It can be found that there is very big shake after demodulation, demodulating error can be bigger.
The content of the invention
The purpose of the embodiment of the present invention be to provide a kind of signal demodulating method for distributed fiber-optic sensor system and Device, to reduce the demodulating error to optical fiber impulse response.
To reach above-mentioned purpose, the embodiment of the invention discloses a kind of signal solution for distributed fiber-optic sensor system Tune method, comprises the following steps:
Obtain the letter after an optical pulse code sequence and optical pulse code sequence and the impulse response convolution of testing fiber Number;
By the signal after the optical pulse code sequence and convolution of acquisition, respectively by Fourier transform to frequency domain, according to change The signal after optical pulse code sequence and convolution after changing, is calculated the impulse response of the testing fiber under frequency domain;
The obtained impulse response of testing fiber under frequency domain is converted into by time domain by inverse fourier transform, is obtained to be measured The impulse response of optical fiber.
Preferably, the impulse response that the testing fiber under frequency domain is calculated, calculation formula are:Its In, H represents the impulse response of the testing fiber under frequency domain, and Y represents the optical pulse code sequence after passing through Fourier transform to frequency domain Row and the signal after the impulse response convolution of testing fiber, AfRepresent the optical pulse code sequence after passing through Fourier transform to frequency domain Row.
Preferably, it is described to be converted into the obtained impulse response of testing fiber under frequency domain by inverse fourier transform Time domain, calculation formula are:Wherein, h represents the impulse response of the testing fiber under time domain, and Y, which is represented, passes through Fourier Optical pulse code sequence after leaf transformation to frequency domain and the signal after the impulse response convolution of testing fiber, AfRepresentative passes through Fourier Optical pulse code sequence after leaf transformation to frequency domain.
Preferably, the optical pulse code sequence of the testing fiber is:Original optical pulse coded sequence is by mixing bait light Fiber amplifier is amplified the optical pulse code sequence after processing.
Preferably, the original optical pulse coded sequence is:Two light pulses obtained using complementary Gray code are compiled Code sequence in any one.
The embodiment of the invention also discloses, a kind of signal demodulating equipment for distributed fiber-optic sensor system, including,
Signal obtains module, obtains an optical pulse code sequence and the impulse of optical pulse code sequence and testing fiber Respond the signal after convolution;
Signal conversion module, by the signal after the optical pulse code sequence and convolution of acquisition, passes through Fourier transform respectively To frequency domain, according to the signal after the optical pulse code sequence and convolution after conversion, rushing under frequency domain testing fiber is calculated Swash response;
Signal inverse transform module, is converted the obtained impulse response of testing fiber under frequency domain by inverse fourier transform To time domain, the impulse response of testing fiber is obtained.
Preferably, the impulse response that the testing fiber under frequency domain is calculated, calculation formula are:Its In, H represents the impulse response of the testing fiber under frequency domain, and Y represents the optical pulse code sequence after passing through Fourier transform to frequency domain Row and the signal after the impulse response convolution of testing fiber, AfRepresent the optical pulse code sequence after passing through Fourier transform to frequency domain Row.
Preferably, it is described to be converted into the obtained impulse response of testing fiber under frequency domain by inverse fourier transform Time domain, calculation formula are:Wherein, h represents the impulse response of the testing fiber under time domain, and Y, which is represented, passes through Fourier Optical pulse code sequence after leaf transformation to frequency domain and the signal after the impulse response convolution of testing fiber, AfRepresentative passes through Fourier Optical pulse code sequence after leaf transformation to frequency domain.
Preferably, the optical pulse code sequence of the testing fiber is:By original optical pulse coded sequence by mixing bait Fiber amplifier is amplified the optical pulse code sequence after processing.
Preferably, the original optical pulse coded sequence is:Two light pulses obtained using complementary Gray code are compiled Code sequence in any one.
As seen from the above technical solutions, the embodiment of the present invention is by obtaining an optical pulse code sequence and light pulse Signal after the impulse response convolution of coded sequence and testing fiber;By the letter after the optical pulse code sequence and convolution of acquisition Number, respectively by Fourier transform to frequency domain, according to the signal after the optical pulse code sequence and convolution after conversion, it is calculated The impulse response of testing fiber under frequency domain;The impulse response of testing fiber under frequency domain that will be obtained by inverse fourier transform Time domain is converted into, obtains the impulse response of testing fiber.Since the present invention is using pulsatile once input, no at all consider complementary The sum of Gray code auto-correlation is this condition of optical fiber impulse response, therefore reduces demodulating error.
Certainly, implement any of the products of the present invention or method must be not necessarily required to reach all the above excellent at the same time Point.
Brief description of the drawings
In order to illustrate more clearly about the embodiment of the present invention or technical scheme of the prior art, below will be to embodiment or existing There is attached drawing needed in technology description to be briefly described, it should be apparent that, drawings in the following description are only this Some embodiments of invention, for those of ordinary skill in the art, without creative efforts, can be with Other attached drawings are obtained according to these attached drawings.
Fig. 1 is using complementary Gray code schematic diagram in background technology;
Fig. 2 is the application system figure that signal demodulates in background technology;
Fig. 3 is to amplify the inconsistent coded light pulses of afterpulse power by EDFA in the application system;
Fig. 4 is the Gray code light pulse auto-correlation summation after EDFA in the application system;
The original transfer function that Fig. 5 is used when being and being simulated in background technology;
Fig. 6 is the transmission function after being demodulated to original transfer function described in Fig. 5 by Gray;
Fig. 7 is the flow chart of the embodiment of the present invention one;
Fig. 8 is optical pulse code and the signal graph after optical fiber impulse response convolution in the embodiment of the present invention one;
The original transfer function that Fig. 9 is used when being using the simulation of one method of the embodiment of the present invention;
Figure 10 is to the transmission function after original transfer function demodulation described in Fig. 9;
Figure 11 is the structure diagram of the embodiment of the present invention two.
Embodiment
Below in conjunction with the attached drawing in the embodiment of the present invention, the technical solution in the embodiment of the present invention is carried out clear, complete Site preparation describes, it is clear that described embodiment is only part of the embodiment of the present invention, instead of all the embodiments.It is based on Embodiment in the present invention, those of ordinary skill in the art are obtained every other without making creative work Embodiment, belongs to the scope of protection of the invention.
Embodiment one
The present invention is used for a kind of embodiment of the signal demodulating method of distributed fiber-optic sensor system, can be applied to Fig. 2 institutes In the scene shown, step is as shown in fig. 7, comprises following steps:
Step 701:Obtain an optical pulse code sequence and the impulse response of optical pulse code sequence and testing fiber volume Signal after product;
It should be noted that the optical pulse code sequence, can be any one of any one coding mode generation A optical pulse code sequence.
Preferably, the optical pulse code sequence, for the two optical pulse code sequences obtained using complementary Gray code Any one in row.
Preferably, the method for obtaining optical pulse code sequence, for the method for generally use in the prior art, is specially:One The laser that laser is sent, by the electrooptic modulator controlled by arbitrary waveform generator, forms the pulse after coding.After coding Pulse received after erbium-doped fiber amplifier amplification by photodetector, photodetector is by the pulse after coding It is changed into electric signal, electric signal is passed in oscillograph and shown, then obtains optical pulse code sequence by computer.
Preferably, the method for obtaining the signal after optical pulse code sequence and the impulse response convolution of testing fiber, is existing There is the method for generally use in technology, be specially:By the amplified optical pulse code sequence of erbium-doped fiber amplifier, by ring Row device enters in testing fiber, and the signal after the impulse response convolution of optical pulse code sequence and testing fiber is by photodetector Received, the signal after the convolution is changed into electric signal by photodetector, and electric signal is passed in oscillograph and shown Show, then the signal after convolution is obtained by computer, as shown in Figure 8.
Step 702:By the signal after the optical pulse code sequence of the acquisition and the convolution, by Fourier transform extremely Frequency domain, is calculated the impulse response of the testing fiber under frequency domain;
The impulse response that the testing fiber under frequency domain is calculated, calculation formula are:Wherein, H is represented The impulse response of testing fiber under frequency domain, Y represent the optical pulse code sequence after passing through Fourier transform to frequency domain and light to be measured Signal after fine impulse response convolution, AfRepresent the optical pulse code sequence after passing through Fourier transform to frequency domain.
It should be noted that the Fourier transform process is completed in a computer.Fourier transform is ability General knowledge known to field technique personnel, therefore detailed description will be omitted.
Step 703:The impulse response of the testing fiber under frequency domain is converted into by time domain by inverse fourier transform, is obtained To the impulse response of testing fiber.
It is described that the impulse response of the testing fiber under frequency domain is converted into by time domain by inverse fourier transform, calculate public Formula is:Wherein, h represents the impulse response of the testing fiber under time domain, and Y is represented by Fourier transform to frequency Optical pulse code sequence behind domain and the signal after the impulse response convolution of testing fiber, AfRepresent by Fourier transform to frequency Optical pulse code sequence behind domain.
It should be noted that the inverse fourier transform process is completed in a computer.Inverse fourier transform is Well known to a person skilled in the art general knowledge, therefore detailed description will be omitted.
Simulated using the transmission function of 20km optical fiber as Fig. 9, carry out what signal demodulated using the present embodiment method Transmission function is as shown in Figure 10, it can be seen that error very little.
Using above-described embodiment, following beneficial effect can be reached:Coded format is not required, available for various codings Demodulation, only need to determine a coded sequence;Pass through the condition of EDFA Erbium-Doped Fiber Amplifier amplification in optical pulse code sequence Under, the present embodiment is inputted using pulsatile once, and no at all considering the sum of complementary Gray code auto-correlation, whether optical fiber impulse is rung This condition is answered, therefore reduces demodulating error.
Embodiment two
The present invention is used for a kind of embodiment of the signal demodulating equipment of distributed fiber-optic sensor system, as shown in figure 11, bag Include,
Signal obtains module 111, obtains an optical pulse code sequence and the optical pulse code sequence and testing fiber Impulse response convolution after signal;
It should be noted that the optical pulse code sequence, can be any one of any one coding mode generation A optical pulse code sequence.
Preferably, the optical pulse code sequence, for the two optical pulse code sequences obtained using complementary Gray code Any one in row.
Preferably, the method for obtaining optical pulse code sequence, for the method for generally use in the prior art, is specially:One The laser that laser is sent, by the electrooptic modulator controlled by arbitrary waveform generator, forms the pulse after coding.After coding Pulse by erbium-doped fiber amplifier amplification after, obtained by computer.
Preferably, the method for obtaining the signal after optical pulse code sequence and the impulse response convolution of testing fiber, is existing There is the method for generally use in technology, be specially:By the amplified optical pulse code sequence of erbium-doped fiber amplifier, by ring Row device enters in testing fiber, and the signal after the impulse response convolution of optical pulse code sequence and testing fiber is by photodetector Received, the signal after the convolution is changed into electric signal by photodetector, and electric signal is passed in oscillograph and shown Show, then the signal after convolution is obtained by computer.
Signal conversion module 112, by the signal after the optical pulse code sequence of the acquisition and the convolution, passes through Fourier The impulse response of the testing fiber under frequency domain is calculated to frequency domain in leaf transformation;
The impulse response that the testing fiber under frequency domain is calculated, calculation formula are:Wherein, H is represented The impulse response of testing fiber under frequency domain, Y represent the optical pulse code sequence after passing through Fourier transform to frequency domain and light to be measured Signal after fine impulse response convolution, AfRepresent the optical pulse code sequence after passing through Fourier transform to frequency domain.
It should be noted that the Fourier transform process is completed in a computer.Fourier transform is ability General knowledge known to field technique personnel, therefore detailed description will be omitted.
Signal inverse transform module 113, is become the impulse response of the testing fiber under frequency domain by inverse fourier transform Time domain is shifted to, obtains the impulse response of testing fiber.
It is described that the impulse response of the testing fiber under frequency domain is converted into by time domain by inverse fourier transform, calculate public Formula is:Wherein, h represents the impulse response of the testing fiber under time domain, and Y is represented by Fourier transform to frequency Optical pulse code sequence behind domain and the signal after the impulse response convolution of testing fiber, AfRepresent by Fourier transform to frequency Optical pulse code sequence behind domain.
It should be noted that the inverse fourier transform process is completed in a computer.Inverse fourier transform is Well known to a person skilled in the art general knowledge, therefore detailed description will be omitted.
It should be noted that herein, relational terms such as first and second and the like are used merely to a reality Body or operation are distinguished with another entity or operation, are deposited without necessarily requiring or implying between these entities or operation In any this actual relation or order.Moreover, term " comprising ", "comprising" or its any other variant are intended to Non-exclusive inclusion, so that process, method, article or equipment including a series of elements not only will including those Element, but also including other elements that are not explicitly listed, or further include as this process, method, article or equipment Intrinsic key element.In the absence of more restrictions, the key element limited by sentence "including a ...", it is not excluded that Also there are other identical element in process, method, article or equipment including the key element.
Each embodiment in this specification is described using relevant mode, identical similar portion between each embodiment Divide mutually referring to what each embodiment stressed is the difference with other embodiment.It is real especially for system For applying example, since it is substantially similar to embodiment of the method, so description is fairly simple, related part is referring to embodiment of the method Part explanation.
The foregoing is merely illustrative of the preferred embodiments of the present invention, is not intended to limit the scope of the present invention.It is all Any modification, equivalent replacement, improvement and so within the spirit and principles in the present invention, are all contained in protection scope of the present invention It is interior.

Claims (10)

1. a kind of signal demodulating method for distributed fiber-optic sensor system, it is characterised in that comprise the following steps:
Obtain the signal after an optical pulse code sequence and optical pulse code sequence and the impulse response convolution of testing fiber;
By the signal after the optical pulse code sequence and convolution of acquisition, respectively by Fourier transform to frequency domain, after conversion Optical pulse code sequence and convolution after signal, the impulse response of the testing fiber under frequency domain is calculated;
The obtained impulse response of testing fiber under frequency domain is converted into by time domain by inverse fourier transform, obtains testing fiber Impulse response.
2. the signal demodulating method according to claim 1 for distributed fiber-optic sensor system, it is characterised in that described The impulse response that the testing fiber under frequency domain is calculated, calculation formula is:Wherein, H is represented and treated under frequency domain The impulse response of optical fiber is surveyed, Y represents the impulse of optical pulse code sequence and testing fiber after passing through Fourier transform to frequency domain Respond the signal after convolution, AfRepresent the optical pulse code sequence after passing through Fourier transform to frequency domain.
3. the signal demodulating method according to claim 2 for distributed fiber-optic sensor system, it is characterised in that described The obtained impulse response of testing fiber under frequency domain is converted into by time domain by inverse fourier transform, calculation formula is:Wherein, h represents the impulse response of the testing fiber under time domain, and Y is represented by after Fourier transform to frequency domain Signal after optical pulse code sequence and the impulse response convolution of testing fiber, AfRepresent by after Fourier transform to frequency domain Optical pulse code sequence.
4. the signal demodulating method for distributed fiber-optic sensor system according to claim 1-3 any one, it is special Sign is that the optical pulse code sequence of the testing fiber is:The optical pulse code sequence of acquisition is amplified by erbium-doped fiber Device is amplified the optical pulse code sequence after processing.
5. the signal demodulating method according to claim 4 for distributed fiber-optic sensor system, it is characterised in that described The optical pulse code sequence of acquisition be:It is any one in the two optical pulse code sequences obtained using complementary Gray code It is a.
A kind of 6. signal demodulating equipment for distributed fiber-optic sensor system, it is characterised in that including,
Signal obtains module, obtains an optical pulse code sequence and the impulse response of optical pulse code sequence and testing fiber Signal after convolution;
Signal conversion module, by the signal after the optical pulse code sequence and convolution of acquisition, passes through Fourier transform to frequency respectively Domain, according to the signal after the optical pulse code sequence and convolution after conversion, the impulse that the testing fiber under frequency domain is calculated is rung Should;
Signal inverse transform module, will be obtained when the impulse response of testing fiber is converted under frequency domain by inverse fourier transform Domain, obtains the impulse response of testing fiber.
7. the signal demodulating equipment according to claim 6 for distributed fiber-optic sensor system, it is characterised in that described The impulse response that the testing fiber under frequency domain is calculated, calculation formula is:Wherein, H is represented and treated under frequency domain The impulse response of optical fiber is surveyed, Y represents the impulse of optical pulse code sequence and testing fiber after passing through Fourier transform to frequency domain Respond the signal after convolution, AfRepresent the optical pulse code sequence after passing through Fourier transform to frequency domain.
8. the signal demodulating equipment according to claim 7 for distributed fiber-optic sensor system, it is characterised in that described The obtained impulse response of testing fiber under frequency domain is converted into by time domain by inverse fourier transform, calculation formula is:Wherein, h represents the impulse response of the testing fiber under time domain, and Y is represented by after Fourier transform to frequency domain Signal after optical pulse code sequence and the impulse response convolution of testing fiber, AfRepresent by after Fourier transform to frequency domain Optical pulse code sequence.
9. the signal demodulating equipment for distributed fiber-optic sensor system according to claim 6-8 any one, it is special Sign is that the optical pulse code sequence of the testing fiber is:The optical pulse code sequence of acquisition is put by erbium-doped fiber Big device is amplified the optical pulse code sequence after processing.
10. the signal demodulating equipment according to claim 9 for distributed fiber-optic sensor system, it is characterised in that institute The optical pulse code sequence for the acquisition stated is:It is any one in the two optical pulse code sequences obtained using complementary Gray code It is a.
CN201610607797.0A 2016-07-28 2016-07-28 A kind of signal demodulating method and device for distributed fiber-optic sensor system Active CN106052730B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610607797.0A CN106052730B (en) 2016-07-28 2016-07-28 A kind of signal demodulating method and device for distributed fiber-optic sensor system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610607797.0A CN106052730B (en) 2016-07-28 2016-07-28 A kind of signal demodulating method and device for distributed fiber-optic sensor system

Publications (2)

Publication Number Publication Date
CN106052730A CN106052730A (en) 2016-10-26
CN106052730B true CN106052730B (en) 2018-05-08

Family

ID=57196429

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610607797.0A Active CN106052730B (en) 2016-07-28 2016-07-28 A kind of signal demodulating method and device for distributed fiber-optic sensor system

Country Status (1)

Country Link
CN (1) CN106052730B (en)

Families Citing this family (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107390276B (en) * 2017-07-21 2019-01-22 太原理工大学 A kind of underground utilities positioning device and method based on complementary Gray code
CN107782346B (en) * 2017-10-27 2019-08-27 武汉理工大学 Large-scale optical fiber grating sensing network demodulation system and method based on Gray code
CN109506686B (en) * 2018-12-19 2021-03-23 武汉理工光科股份有限公司 Method for improving detection performance of isotactic fiber bragg grating
US10727937B1 (en) * 2019-03-01 2020-07-28 Huawei Technologies Co., Ltd. Multi-layer encoding of optical signals
CN110568439B (en) * 2019-09-25 2023-08-22 中南大学 Deconvolution-based impulse type through-wall radar antenna ringing suppression method
CN112444959B (en) * 2020-11-20 2023-01-17 中电科思仪科技(安徽)有限公司 Device and method for processing optical fiber image ghost
CN114061736B (en) * 2021-11-18 2022-11-25 北京邮电大学 Rayleigh distributed phase demodulation optical fiber sensing method and system based on frequency and intensity encoding and decoding

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101893455A (en) * 2010-07-09 2010-11-24 哈尔滨工程大学 Optical fiber composite chamber laser feedback effect sensor and special demodulating method thereof
CN102322884A (en) * 2011-08-09 2012-01-18 中国计量学院 Merge the very-long-range pulse code distribution type fiber-optic Brillouin sensing device of optical fiber Brillouin frequency shifter
CN102374873A (en) * 2011-09-19 2012-03-14 武汉邮电科学研究院 Sensing system based on optical OFDM (Orthogonal Frequency Division Multiplexing) and FBG (Fiber Bragg Grating) monitoring method thereof
CN104155619A (en) * 2014-08-20 2014-11-19 天津大学 Distributed optical frequency domain reflection magnetic field sensing device based on magnetostriction and demodulation method

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7339678B2 (en) * 2005-11-09 2008-03-04 Northrop Grumman Corporation Method and system of using odd harmonics for phase generated carrier homodyne
JP4826747B2 (en) * 2006-02-24 2011-11-30 横河電機株式会社 Method for measuring frequency shift of Brillouin scattered light and apparatus using the same

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101893455A (en) * 2010-07-09 2010-11-24 哈尔滨工程大学 Optical fiber composite chamber laser feedback effect sensor and special demodulating method thereof
CN102322884A (en) * 2011-08-09 2012-01-18 中国计量学院 Merge the very-long-range pulse code distribution type fiber-optic Brillouin sensing device of optical fiber Brillouin frequency shifter
CN102374873A (en) * 2011-09-19 2012-03-14 武汉邮电科学研究院 Sensing system based on optical OFDM (Orthogonal Frequency Division Multiplexing) and FBG (Fiber Bragg Grating) monitoring method thereof
CN104155619A (en) * 2014-08-20 2014-11-19 天津大学 Distributed optical frequency domain reflection magnetic field sensing device based on magnetostriction and demodulation method

Also Published As

Publication number Publication date
CN106052730A (en) 2016-10-26

Similar Documents

Publication Publication Date Title
CN106052730B (en) A kind of signal demodulating method and device for distributed fiber-optic sensor system
Martins et al. Real time dynamic strain monitoring of optical links using the backreflection of live PSK data
Elooz et al. High-resolution long-reach distributed Brillouin sensing based on combined time-domain and correlation-domain analysis
Chen et al. Fiber-optic distributed acoustic sensor based on a chirped pulse and a non-matched filter
CN102636251B (en) Phase sensitivity light time domain reflection system and method for improving SNR (signal to noise ratio) thereof
CN104819770B (en) Phase optical time domain reflecting device and method with phase demodulating is detected based on heterodyne
CN104467984B (en) A kind of distribution type fiber-optic sound wave communication method and device
CN101852627B (en) Coding technique for improving detection performance of distributed fiber sensor and application thereof
CN106574852A (en) Method and apparatus for measuring a distributed physical value of an optical device under test
Wu et al. Quasi-distributed fiber-optic acoustic sensing system based on pulse compression technique and phase-noise compensation
CN107063433B (en) Phase-sensitive optical time domain reflectometer and its implementation based on Golay complementary series
CN106595776B (en) A kind of more physical quantity sensor-based systems of distribution type fiber-optic and method
CN107607135A (en) A kind of chaos Brillouin light time domain/coherent field convergence analysis device and method
CN102761363A (en) Method and device for detecting optical time domain reflectometer signals
London et al. High-resolution long-range distributed Brillouin analysis using dual-layer phase and amplitude coding
CN102865914A (en) Distributed optic fiber vibrating sensor
CN107036734A (en) A kind of fully distributed fiber temperature or the method for sensing and sensor of strain
CN109579887A (en) A kind of time division multiplex optical fiber grating sensing system and method based on composite coding
Jiang et al. Quasi-distributed fiber-optic acoustic sensing with MIMO technology
CN108288999A (en) The application that noise reduction distribution type fiber-optic water based on Rayleigh scattering is listened
Luo et al. Optical chaos and hybrid WDM/TDM based large capacity quasi-distributed sensing network with real-time fiber fault monitoring
Shiloh et al. Highly-sensitive distributed dynamic strain sensing via perfect periodic coherent codes
de Miguel Soto et al. Spectral shadowing suppression technique in phase-OTDR sensing based on weak fiber Bragg grating array
CN102564481A (en) Method and device for improving signal-to-noise ratio of distributed optical fiber Brillouin sensor
CN106949954B (en) A kind of fiber-optic vibration signal supervisory instrument and method

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