• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to a Brillouin scattering distributed optoelectronic measuring device, said device comprising a continuous light source (1), a coupler (2), an acousto-optical modulator (3), an optical fiber (5) to be tested for that it emits back a spontaneous Brillouin backscattering signal at a frequency νF equal to νp + νBz, where νBz is the Brillouin frequency to be measured at every z-point of said optical fiber (5), a local oscillator (16) emitting a another light signal intended to be mixed with said feedback signal emitted by Brillouin backscattering by said optical fiber (5) to be tested, a detection module (9) capable of detecting said Brillouin offset frequency νBz at any point z of said optical fiber and a processing module for connecting this Brillouin offset frequency νBz at any point z of said optical fiber to a temperature value and a deformation value. According to the invention, the local oscillator (16) comprises a reference optical fiber (18) having a Brillouin frequency identical to or close to that of the optical fiber (5) to be tested, said reference optical fiber (18) emitting a spontaneous Brillouin backscattering signal, in response to said continuous light signal emitted in said second arm by said light source (1), said Brillouin backscattering signal being emitted at a frequency νOL = ν0 - vBRef, where vBRef is the Brillouin frequency of the reference fiber without deformation and at a reference temperature.
    公开号:FR3043457A1
    申请号:FR1560681
    申请日:2015-11-06
    公开日:2017-05-12
    发明作者:Vincent Lanticq
    申请人:Febus Optics；
    IPC主号:
    专利说明:

    OPTOELECTRONIC MEASUREMENT DEVICE DISTRIBUTED BY DIFFUSION
    BRILLOUIN
    FIELD OF THE INVENTION The invention relates to an optoelectronic Brillouin scattering measurement device in an optical fiber using a single laser frequency to generate a light pulse. This type of device is still referred to as a Brillouin backscattered fiber optic sensor.
    [002] Such devices are used for the permanent control of the integrity and safety of systems and structures in civil engineering or the oil industry. They are used in particular for the monitoring of linear structures such as bridges, dams, hydraulic earth dikes or fluid transport networks (water, hydrocarbons, gas) in order to control the ground movements (slippage, settlement) or deformations of buried or non-buried pipes. An optical fiber is arranged along a structure to be monitored and a light signal is injected into said fiber. The light signal backscattered by the optical fiber then makes it possible to deduce the structural state of the structure.
    [Prior Art] [003] These optoelectronic Brillouin scattering measurement devices are more particularly used to measure, in real time, the temperature or deformations of large infrastructures in order to monitor their structural health and to ensure their maintenance. They provide, for each measurement, the temperature and deformation information at any point of the optical fiber connected to them. Measurements are generally made with a range of a few meters to several tens of kilometers and a metric or even centimeter resolution. Thus, for example, a measurement can be made every meter on a structure of a length of 20 kilometers.
    [004] Such devices exploiting the Brillouin backscattering phenomenon are already known and used for applications of temperature measurement and deformation in civil engineering.
    [005] The Brillouin frequency vb, linearly depends on the temperature and the deformation in the material. The frequency difference Avb between the incident wave and the backscattered wave therefore varies with the temperature variations ΔΤ and the strain ε according to the equation: Avb = ΟτΔΤ + CE £, where Oret CE are respectively the temperature and temperature sensitivity coefficients. deformation specific to the optical fiber used. At the wavelength λ 0 = 1550 nm and for a standard fiber as defined by the ITU-G652 standard (for example Coring® fibers - SMF-28 ™), the coefficients are of the order of Ct ~ 1MHz / ° C and Οε ~ 0.05ΜΗζ / με.
    [006] In order to be able to analyze intensity variations over tens of kilometers with metrical spatial resolution, measurement systems generally use OTDR (Optical Time Domain Reflectometry). The OTDR consists in propagating a light pulse in the optical fiber to be analyzed and measuring the return intensity as a function of time. The time that the backscattered light has to be detected makes it possible to locate the event to be measured (coordinate of a point z along the optical fiber). The spatial resolution is then a function of the width of the light pulse: a pulse of width 10 ns resulting for example a resolution of about 1 m.
    [007] Thanks to the Brillouin backscattering phenomenon combined with the OTDR technique, measurements of temperature and deformation are carried out all along the fiber over several tens of kilometers, with a metric or even centimeter resolution.
    [008] The measurements along the fiber are performed with a device as schematized in FIG. 1. Light from a light source 1, such as a laser, is distributed in two arms. One of the arms, called "pump", sends the light signal, in pulse form through an acousto-optic modulator 3, in the optical fiber 5 to be tested. A signal is backscattered by the fiber 5, according to the Brillouin phenomenon. According to the Brillouin phenomenon, the spectral components of backscattering of light by the material constituting the optical fiber, in general of silica, have a frequency vBz offset from that vO of the incident light wave. The Brillouin frequency offset is generally of the order of 11 GHz for an incident wave of wavelength λ 0 = 1550 nm. Such a frequency is very high. In order to be able to perform the processing on the backscattered signal, the frequency can be transposed at a lower frequency to reduce the bandwidth of the detector to be used and thus eliminate a large part of the noise. For this, a heterodyne detection is carried out as described, for example, in US Pat. No. 7,283,216. Heterodyne detection consists in recombining the backscattered signal to be analyzed with a wave coming from the other arm, called a "local oscillator" 6. For example, local oscillator 6 may be in the form of a Brillouin ring laser. In this case, the continuous light signal of frequency vo is directed to a circulator 7 which in turn directs it to a reference fiber. This reference fiber emits by spontaneous amplified diffusion a radiation in the opposite direction of frequency vo + VBref that the circulator sends to a coupler 13. The latter sends a part of the energy to the output signal, while it redirects the another portion to the reference fiber where the radiation is amplified by a gain factor G by stimulated Brillouin scattering before being redirected to the circulator 7 which returns the amplified radiation to the coupler 13 and the output. The local oscillator 6 then forms a stimulated Brillouin scattering amplification ring. A photo detector 9 makes it possible to recover the beat of the two signals. The recovered beat is then amplified and then transmitted to an electric spectrum analyzer.
    Such an optoelectronic measuring device distributed by Brillouin scattering in an optical fiber, using a single laser frequency to generate a light pulse, is more particularly described in the document US Pat. No. 7,283,216. The device according to this document makes it possible to perform, in real time, simultaneous measurements of temperature and constraints. A heterodyne detector makes it possible to recover the beat, between the signal coming from the local oscillator and the signal backscattered by the fiber to be analyzed, which lies in a frequency band exploitable by an analog receiver. The local oscillator used in this document is formed by a Brillouin ring laser and imposes that the circuit is coherent, that is to say that the return wave is in phase with the incident wave. The length of the reference fiber and the laser frequency must therefore be controlled and adjusted so that the cavity of the local oscillator provides the right frequency v0 to enable the frequency of the signal backscattered by the fiber to be tested to be transposed. at a lower frequency. The device described in this document is therefore complex to implement because it requires prior checks not to create disturbances on the return signal. In addition, the detection is an analog heterodyne detection, requiring the use of relatively bulky and energy consuming analog electronic components.
    Document CA 2 274 505 describes a device and a method for accurately and simultaneously measuring temperature variations and stresses along an optical fiber, itself arranged along a structure whose structure is to watch. The device described is however complex to implement. Indeed, the analysis of the detected signal is complex because it takes into account not only the Brillouin backscattering phenomenon but also another Rayleigh backscattering phenomenon. An optical detector comprising a scanning optical filter resolves Rayleigh peaks and Brillouin peaks and converts the optical signals into electrical signals, which are then processed by analog processing means. The measurement of the temperature and the stress at any point along the fiber, is to determine the scanning speed of the optical filter, slower than the optical pulse repetition rate, to measure the amplitude and the frequency of the lines. Brillouin versus Rayleigh lines as a function of time, then compare against a reference fiber. In addition, the device described in this document performs a direct optical detection and not a heterodyne detection. In addition, such a device provides a low frequency resolution induced by the use of a scanning optical filter.
    It often happens that the civil engineering works, whose structure is to be analyzed, are isolated from any human activity and therefore from any electrical network. In this case, in order to monitor all or part of the structure, an autonomous energy measurement system is necessary. Existing Brillouin scattering measurement devices do not allow autonomous operation and low energy consumption. They must therefore be located near technical premises often distant from each other several hundred kilometers. Since this distance is greater than the maximum range of these devices, part of the civil engineering works can not be continuously monitored by the existing Brillouin scattering measurement devices.
    In addition, another disadvantage of the existing systems is the duration of the measurements because this duration is long. Indeed, typically, the measurement time is greater than 1 minute for a 10Km fiber.
    [Technical problem] [0013] The object of the invention is therefore to remedy the disadvantages of the prior art. The object of the invention is in particular to provide a simple and compact space-saving optoelectronic Brillouin scattering measurement device whose optoelectronic configuration allows a significant reduction in the electrical energy consumption compared with existing devices, so that it can be supplied with low voltage, typically 12 or 24 volts, from a battery for example.
    The device proposed according to the invention has fewer elements than the existing systems described above and it is autonomous in energy which allows to have a portable device adapted to interventions by an operator on foot or at occasional measures. In addition, the device implements a digital signal processing from the output of the photodetector. The following signal processing is done digitally at the spectral level and not directly on the signal. Thus, the duration of a measurement is short relative to the measurement time of the systems of the prior art. Typically the duration of a measurement is from 1 to a few seconds for a fiber of 10Km.
    Another object of the invention is to provide a digital processing method of a signal from said optoelectronic measurement device distributed by Brillouin scattering.
    [Brief description of the invention! For this purpose, the invention relates to an optoelectronic measuring device distributed by Brillouin scattering, said device comprising a continuous light source emitting a continuous light signal at a first frequency vo, a coupler capable of dividing said light signal. continuous signal in two identical signals distributed in two arms, the first arm comprising a frequency-shifted pulse generator device comprising at least one acousto-optical modulator capable of transforming said continuous signal into a pulsed signal of frequency vp intended to be injected in an optical fiber to be tested to emit back a spontaneous Brillouin backscattering signal at a frequency vF equal to vp + vBz, where vBz is the Brillouin frequency to be measured at any point z of said optical fiber, and the second arm forming a local oscillator emitting another light signal to be mixed with said feedback signal set by Brillouin backscattering by said optical fiber to be tested to allow a lowering of the frequency of said return signal, so that a detection module can detect said Brillouin offset frequency vBz at any point z of said optical fiber and that a processing module can connect this Brillouin offset frequency vBz at any point z of said optical fiber to a temperature value and a deformation value, said device being mainly characterized in that the local oscillator comprises a reference optical fiber having a Brillouin frequency identical to or close to that of the optical fiber to be tested, said reference optical fiber emitting a spontaneous Brillouin backscattering signal, in response to said continuous light signal emitted into said second arm by said light source, said Brillouin backscattering signal being sent at a frequency vol = vo - vBRet, where vBRef is the Brillouin frequency of the reference fiber without deformation and at a reference temperature.
    Thus, the device according to the invention eliminates all the necessary prior checks when using a local oscillator having a Brillouin ring laser configuration. Indeed, in the configuration according to the invention, the return signal emitted by the reference fiber is an amplified spontaneous diffusion signal, and not the product of a resonance in a laser-like cavity (which would depend greatly on the exact length of the cavity, difficult to control according to influence parameters such as temperature).
    According to other optional features of the device: the reference optical fiber has an identical Brillouin frequency or a frequency close to that of the optical fiber to be tested, namely having a frequency difference of less than 50 MHz and so preferred a difference of less than 20MHz. the device according to the invention furthermore comprises: a coupler with at least two inputs for receiving the backscattered signal at the output of the circulator and the signal coming from the local oscillator and performing their mixing; a polarization jammer arranged upstream coupler inputs, the detection module comprises on the one hand a photodetector limiting the bandwidth to less than 1 GHz, preferably less than 500 MHz, and preferably in a band centered around 200 MHz, capable of detecting a beat between the backscattered signal from the optical fiber to be tested and the backscattered signal from the reference optical fiber, and a 5-digital analog converter capable of digitizing said beat detected by said photodetector. - The device also comprises a low frequency electric filter disposed between the coupler and the photodetector. This filter makes it possible to reduce the low frequency noise and thus improve the signal-to-noise ratio, the acousto-optical modulator with frequency offset greater than 0 100 MHz and preferably an offset of 200 MHz at 300 MHz. the processing module is a digital processing module able to use a Fast Fourier Transform (FFT) algorithm to calculate the Brillouin frequency at any point z of said optical fiber to be tested, and then to average the spectra obtained in the domain frequency for each z-point of said fiber 5 to determine the distributed measurement of the frequency variation along said fiber. Advantageously, the device is embedded and supplied with low voltage, typically 12 or 24 volts, from a battery. The device is thus easily portable and can be used for operations performed by foot operators or occasional measurements.
    The invention also relates to a method for the digital processing of a signal from an optoelectronic Brillouin scattering distributed measurement device described above, said method comprising the following steps: - digitizing a signal corresponding to the beat between a backscattered signal from an optical fiber (5) to be tested and a backscattered signal from a reference optical fiber (18), and detected by a photodetector (9), - cutting said digitized signal into a plurality of sections (T1 ... TL.TN) by application of a sliding window of the rectangular window or Hamming type, or of Hann or Blackman-Harris, each section presenting 0 a width equal to the temporal width of a half pulse of the pulse signal injected into the optical fiber to be tested, the width of each section
    Ref: 0453-FEBUS being furthermore centered around a date t corresponding to a coordinate point z of said optical fiber to be tested, - calculating, by using a FFT fast fourier transform algorithm, the frequency spectrum of each section (T1 ... TL.TN) of said digitized signal; repeating steps a, b and c and averaging the spectra obtained for each z-point of said optical fiber to be tested; - using the results obtained in the previous step, plot a graph of the measured distributed frequency variation as a function of the back-scatter time back and forth, - apply a coefficient of sensitivity to temperature on the one hand and a coefficient of sensitivity to the deformation on the other hand, on said obtained graph of measured distributed frequency variation, in order respectively to obtain a result in terms of measurement distributed in temperature or a result in terms of distributed measurement in deformation. Advantageously, the digital processing is performed by a graphics processor GPU type (Graphicai Processing Unit), because this algorithm is highly parallelizable namely that the same calculation is performed many times on different portions of the signal.
    Other advantages and features of the invention will become apparent on reading the following description given by way of illustrative and nonlimiting example, with reference to the appended figures which show: • Figure 1, already described, a diagram of a Brillouin backscattered distributed optoelectronic measurement device according to the prior art, FIG. 2, a diagram of a Brillouin backscattered distributed optoelectronic measurement device according to the invention, FIGS. 3A to 3E, temporal traces or spectral obtained at each stage of the digitized signal digital processing method, obtained after recombination of the backscattered signals by the optical fiber under test and by the reference optical fiber. FIGS. 4A to 4C show actual measurements made from the device of the invention; FIG. 5 shows the set of Brillouin scattering spectra on a fiber approximately 250m long. • Figure 6 shows the distributed measurement result, i.e. the set of maxima of the spectra of Figure 5.
    DETAILED DESCRIPTION OF THE INVENTION The term fiber to be tested (or under test) in the following, the optical fiber arranged along a structure to monitor and allows for a distributed measurement.
    By reference fiber is meant a fiber having a Brillouin frequency identical or close to the Brillouin frequency of the test fiber. The term close Brillouin frequency fiber refers to a fiber whose Brillouin frequency has a frequency difference with the Brillouin frequency of the test fiber, less than 50 MHz and preferably a difference of less than 20 MHz.
    The term "duration of a measurement" means the time required for the system to display a measurement at the nominal accuracy (in terms of deformation or temperature). This duration includes both: • the acquisition time, • the system calculation time (Fourier transforms, averages, etc.). The present invention relates generally to distributed measurement optoelectronic devices. by Brillouin scattering in an optical fiber. The invention relates more precisely to an optoelectronic configuration of the device making it possible to reduce its electrical consumption and to reduce its bulk.
    The use of the measures returned by this device is devoted to the optimization of the maintenance of civil engineering works. The continuity of the measurements along the optical fiber guarantees the detection of an event that would not have been by another method using point and localized measurements. Early detection of structural disorders in civil engineering works allows intervention before further degradation. Conversely, the lack of detection can delay routine maintenance operations if they are not necessary. In both cases, such an optoelectronic measurement device distributed by backscattering Brillouin allows an operator to achieve significant savings on the maintenance of civil engineering works.
    Figure 2 schematizes more particularly the configuration of such an optoelectronic measuring device distributed by Brillouin scattering in an optical fiber, according to the invention. The same references as in Figure 1 are used to designate the same elements. The device according to the invention also comprises a light source 1 emitting a continuous light signal. This light source 1 is advantageously embodied by a laser, preferably a DFB laser (from the acronym "Distributed Feedback"), using a Bragg grating. The emission wavelength k 0 is preferably equal to 155 nm, at the corresponding frequency v 1. The line of the emitted light wave is centered on the emission wavelength λο and its width is at most 1 MHz. The laser 1 emits a moderately strong continuous light signal, typically of the order of 20mW, in an optical fiber connecting it to the coupler 2. The coupler 2 makes it possible to divide the incident light signal emitted by the laser 1 into two identical signals distributed in two arms of the device.
    The first arm, also called "pump", comprises a frequency-shifted pulse generator device 30. This device 30 comprises at least one acousto-optical modulator 3. It may also include one or more amplifiers if necessary to give of the gain. The acousto-optical modulator 3 converts the continuous signal of frequency vo into a pulse signal of frequency vP = vo + va, where va is the frequency specific to modulator 3, and is generally greater than or equal to 100 and less than or equal to 500 MHz preferably of the order of 200 MHz. The temporal width of the pulse thus generated is between 10 ns and 50 ns, preferably 20 ns. The pulse signal is then directed to a circulator 4 which then injects it into the optical fiber 5 to be tested, on which the distributed measurement must be carried out. At the passage of the pulse signal, the optical fiber 5 transmits in the opposite direction a spontaneous Brillouin backscattering signal at the frequency vf = vo + va + vbz; where vbz is the Brillouin frequency to be measured at any coordinate point z along the optical fiber 5. This backscattered signal is directed by the circulator 4 to the coupler 8 where it is recombined with a signal from the local oscillator forming the second arm of the device.
    The local oscillator 16 advantageously comprises a circulator 17 which directs the incident continuous light signal, at the frequency vo, from the laser 1, in an optical fiber 18 of reference. This reference optical fiber 18 is advantageously identical to the optical fiber 5 under test. The reference fiber 18 is not subject to any deformation. It is placed at a reference temperature, generally between 18 and 25 ° C, preferably at a temperature of the order of 20 ° C. This reference fiber 18 also makes it possible to emit a Brillouin backscattering signal in response to the continuous signal emanating from the light source 1, so that the local oscillator 16 makes it possible to transform the incident frequency vo into a frequency vol = vo + VBret, where VBref represents the Brillouin frequency of the optical fiber 18 of reference, and which is in the same frequency range as the frequency vbz from the signal backscattered by the optical fiber 5 under test. The Brillouin frequency of the reference optical fiber is therefore in a frequency range around 11 GHz, generally between 10.5 and 11.5 GHz. The circulator 17 of the local oscillator 16 then sends the backscattered signal to the coupler 8 to mix with the backscattered signal from the optical fiber 5 under test.
    The signals from the optical fiber 5 under test and the reference optical fiber 18 are recombined in the coupler 8. At the output of the coupler 8, a signal is obtained which contains a beat between the signal from the optical fiber 5 under test and the reference optical fiber 18 of the local oscillator 16. This beat, of lower frequency, is electronically detectable through the use of a photodetector 9, bandwidth less than 1GHz preferably 500MHz. At the output of the photodetector 9, an electrical signal corresponding to the beat detected at the frequency of VBatt = va + (vbz - VBref) is thus obtained. The beat has a lower frequency than the incident signals because the frequency vo from the light source 1 is eliminated. Typically, the beat has a frequency below 500 MHz, and preferably around 200 MHz, corresponding to the order of magnitude of the frequency specific to the acousto-optic modulator 3.
    The beat signal obtained is then digitized, by means of an analog-digital converter module 11. Then it is processed by a digital processing module 12.
    The advantageous configuration of the local oscillator 16 according to the invention makes it possible to dispense with all the necessary preliminary checks when using a Brillouin ring laser in order to avoid disturbances on the signal (by instability of laser cavity). It also makes it possible to reduce the frequency to be detected by the photodetector to less than 500 MHz, and more particularly in a frequency band centered around 200 MHz. The optical configuration therefore makes it possible to increase the efficiency of the photodetector 9 by limiting the bandwidth to less than 1 GHz instead of 11 GHz, preferably 500 MHz.
    The digital processing module 12, for its part, advantageously uses a FFT fast fourier transform algorithm, for example by means of a logic integrated circuit known as FPGA (for "Field Programmable gate array"). ). It thus makes it possible to directly calculate the Brillouin frequency at any coordinate point z of the optical fiber under test. The digital processing module 12 also makes it possible to average the spectra obtained in the frequency domain, for each z-point of said fiber, after the application of the FFT fast fourier transform algorithm, in order to determine the frequency. distributed measurement of the frequency variation along said optical fiber under test.
    The various steps of the digital processing carried out on the digitized signal are more particularly illustrated by the experimental and explanatory FIGS. 3A to 3E which represent temporal or spectral traces obtained at each stage of the digitized signal digital processing method, obtained after recombination of the backscattered signals by the optical fiber under test and by the reference optical fiber.
    FIG. 3A represents the digitized signal at the output of the analog-digital converter 11.
    A first step of the digital processing performed by the digital processing module 12 is to cut the digitized signal into sections. The cutting in section is performed by applying a sliding time window on the signal. Preferably the windowing is done by a rectangular window or
    Hamming or Hann or Blackman-Harris. The cutting of the digitized signal is shown in FIG. 3B, a first section to be processed being identified by the reference T1 and the section N, in which the area of the event to be measured is located, being identified by the reference TN. Each section has a width equal to the time width of a half-pulse of the pulse signal injected into the optical fiber to be tested. Each section T1 ... TL. TN is further centered around a date ti ... ti .., în corresponding to a coordinate point z of said optical fiber to be tested. Thus, for a coordinate position z on the optical fiber 5, z = v. tz, where v = c / (2.n), where n is the refractive index of the optical fiber, c is the speed of light, v is the frequency of the optical wave, and the time tz then corresponds to the round-trip time (z) of a pulse, counted from the start point of the pulse to the z-point of measurement.
    The difference between two measurement points can be as small as 1 sampling unit (slip of an interval). However the difference between 2 independent measurements (spatial resolution) is considered equal to the half-width of the pulse. Thus, the difference between two independent measuring points z (t1), z (t2) is equal to the width of a half pulse.
    A second step of the digital processing then consists of calculating, by using a FFT fast fourier transform algorithm, the spectrum of each section T1 ... TL. TN of said digitized signal. Thus, for each section T1 ... TL. TN of the digitized signal a frequency spectrum is obtained. Such frequency spectra are illustrated in FIG. 3C for the T1 and TN sections of the cut signal of FIG. 3B. These frequency spectra make it possible to obtain the frequency of the beat VBatt = va + (vbz-VBref) and to determine the maximum frequency of the beat corresponding to each section T1 ... TL, TN. A third step consists of repeating the first two steps of cutting and using the fast fourier transform algorithm, and averaging the results in order to obtain an interpretable spectrum, that is to say the maximum one of which can be determined. . It is about averaging the FFT curves to determine the maximum as precisely as possible. For example, a Gaussian or Lorentz adjustment algorithm is used. This step can be seen as optional but the processed signals being noisy, it is, in practice, necessary.
    The fourth step of the digital processing then consists in determining the frequency positions of the maximas corresponding to the results of the adjustment algorithms, as a function of the z coordinates of the different points of the optical fiber 5, and to plot a graph of the distributed measurement. of frequency variation all along the optical fiber 5. Such a graph is shown in FIG. 3D, on which a variation of frequency with the duration t = 500ns, corresponding to the event zone of the TN section of the Figure 3B.
    Finally, a last step of the digital processing consists in applying the sensitivity coefficients, respectively of temperature Ct and of deformation Ce, specific to the optical fiber 5, to obtain a result respectively in terms of distributed measurement of temperature and deformation. FIG. 3E represents a graph obtained after application of the coefficient of resistance to deformation and making it possible to obtain the distributed measurement of deformation ε all along the optical fiber. Thus, on this graph, it can be seen that the optical fiber analyzed is deformed by 680 μm / m at the point z corresponding to the duration t of 500 ns. The strain sensitivity coefficient C est is typically 0.05MHz / (μm / m)) and the temperature sensitivity coefficient Ct is typically 1MHz / ° C.
    Figures 4A to 4C show actual measurements made from the invention.
    Figure 4A shows a temporal trace acquired directly at the output of the photodetector. This has a random modulation (in contrast to Figure 3A, explanatory), but contains, as shown in Figure 4B, a quasi-sinusoidal component corresponding to Brillouin scattering. FIG. 4C shows that the average spectrum born of the temporal portion, presented at 4B, is as described in the explanatory figure 2C. Figure 5 shows the set of Brillouin scattering spectra on a fiber length of about 250m. Figure 6 shows the distributed measurement result, that is, the set of maxima of the spectra of Figure 5.
    The fibers used are monomode fibers typically G652 type Coring® - SMF-28 ™ fibers, typically of index 1.45, 9pm core diameter, 125pm optical sheath, mechanical sheath 250pm. The length can be less than 1km, up to more than 50km.
    The invention allows a deletion of all analog electronic components, except the photodetector 9 and allows their replacement by a digitizer 11 and a digital processing module 12. Thus, it eliminates noise levels brought by analog active components such as amplifiers or oscillators for example. In addition, since the signal processing is entirely digital, the processes are less energy consuming and the device has a small footprint, so that it can be embedded. It can therefore advantageously be supplied with low voltage, typically 12 or 24 volts, from a battery. This battery can also be rechargeable, for example by an insulated solar panel, whose power requirement is of the order of 100 Watt continuous.
    In addition the device allows to use a digital calculation module 12 to perform parallel processing for each section which reduces the measurement time to the acquisition time, for example for 10km of fiber we can have 10000 acquisitions per second with a clock frequency of 10KHz processor and thus get 10000 averages. The numerical calculation module advantageously comprises graphical processing unit GPU (Graphical Processing Unit) in order to shift the highly parallelizable calculation thereon. Thus, the calculation is performed in parallel with the acquisition and the duration of a measurement corresponds to the acquisition time. This acquisition time is low compared to the acquisition time of the devices of the prior art. For example, for a fiber of 10km, with a clock frequency of the processor of 10Khz, one makes 10000 acquisitions in one second which makes it possible to have 10000 averages whereas in the state of the art the duration of 'a measurement is greater than one minute for 10km.
    权利要求:
    Claims (10)
    [1" id="c-fr-0001]
    1. Brillouin scattering distributed optoelectronic measuring device, said device comprising a continuous light source (1) emitting a continuous light signal at a first frequency vo, a coupler (2) capable of dividing said continuous light signal into two identical distributed signals in two arms, the first arm comprising a frequency-shifted pulse generating device (30) comprising at least one acousto-optical modulator (3) adapted to transform said continuous signal into a pulse signal, of frequency vp, intended to be injected in an optical fiber (5) to be tested to output a spontaneous Brillouin backscattering signal at a frequency vF equal to vp + vBz, where vBz is the Brillouin frequency to be measured at any point z of said optical fiber (5 ), and the second arm forming a local oscillator (16) transmitting another light signal to be mixed with said return signal emitted by retrod firing Brillouin by said optical fiber (5) to be tested to allow a lowering of the frequency of said feedback signal, so that a detection module (9) can detect said Brillouin offset frequency vBz at any point z of said fiber optical and a processing module (12) can connect this Brillouin offset frequency vBz at any point z of said optical fiber to a temperature value and a deformation value, said device being characterized in that the local oscillator ( 16) comprises a reference optical fiber (18) having a Brillouin frequency identical to or close to that of the optical fiber (5) to be tested, said reference optical fiber (18) emitting a spontaneous Brillouin backscattering signal, in response to said a continuous light signal emitted in said second arm by said light source (1), said Brillouin backscattering signal being emitted at a frequency vol = vO - vBRef, where vBRef is the Brillouin frequency of the reference fiber without deformation and at a reference temperature.
    [2" id="c-fr-0002]
    2. Device according to claim 1, characterized in that the reference optical fiber (18) has an identical Brillouin frequency or a frequency close to that of the optical fiber (5) to be tested ie having a frequency difference, lower at 50MHz and preferably a difference of less than 20MHz.
    [3" id="c-fr-0003]
    3. Device according to claims 1 or 2, characterized in that it comprises: - a coupler (8) with at least two inputs for receiving the backscattered signal output of the circulator (4) and the signal from the local oscillator (18) and perform their mixing, - a polarization jammer (19) disposed upstream of the inputs of the coupler (8).
    [4" id="c-fr-0004]
    4. Device according to claim 1, characterized in that the detection module comprises on the one hand a photodetector (9) limiting the bandwidth to less than 1GHz, preferably less than 500 MHz, and preferably in a a band centered around 200 MHz, capable of detecting a beat between the backscattered signal coming from the optical fiber (5) to be tested and the backscattered signal coming from the optical fiber (18) of reference, and an analog-to-digital converter (11) capable of digitizing said beat detected by said photodetector (9).
    [5" id="c-fr-0005]
    5. Device according to claims 3 and 4, characterized in that it further comprises a low frequency electric filter disposed between the coupler (8) and the photodetector (9) to eliminate the noise of optical intensity brought by the Brillouin scattering in the reference fiber.
    [6" id="c-fr-0006]
    6. Device according to claim 1, characterized in that the acousto-optic modulator (3) with frequency offset greater than 100MHz and preferably an offset of 200MHz to 3ÛÛMHz.
    [7" id="c-fr-0007]
    7. Device according to claim 1, characterized in that the processing module (12) is a digital processing module capable of using a Fast Fourier Transform (FFT) algorithm to calculate the Brillouin frequency at any point z of said optical fiber to be tested, then averaging the spectra obtained in the frequency domain for each z-point of said fiber in order to determine the distributed measurement of the frequency variation along said fiber.
    [8" id="c-fr-0008]
    8. Device according to one of claims 1 to 7, characterized in that it is embedded and supplied with low voltage, typically 12 or 24 volts, from a battery.
    [9" id="c-fr-0009]
    9. A method of digitally processing a signal from a Brillouin scattering distributed optoelectronic measurement device according to one of claims 1 to 8, said method comprising the following steps: a) digitizing a signal corresponding to the beat between a signal backscattered from an optical fiber (5) to be tested and a backscattered signal from a reference optical fiber (18), and detected by a photodetector (9), b) cutting said digitized signal into a plurality of sections (T1 ... TN ... TN) by applying a sliding window of rectangular window type or Hamming, or Hann or Blackman-Harris, each section having a width equal to the temporal width of a half impulse of the pulse signal injected into the optical fiber (5) to be tested, the width of each section being furthermore centered around a date t corresponding to a coordinate point z of said optical fiber (5) to test, c) calculating, by using a FFT fast fourier transform algorithm, the frequency spectrum of each section (T1 ... TL.TN) of said digitized signal; d) repeating steps a), b) and c) and averaging the spectra obtained for each z-point of said optical fiber to be tested; e) using the results obtained in the previous step, plot a graph of the measured distributed frequency variation as a function of the back-scattered back-trip time t, f) apply a coefficient of sensitivity to temperature on the one hand and a coefficient of sensitivity to the deformation on the other hand, on said obtained graph of measured distributed frequency variation, in order respectively to obtain a result in terms of measurement distributed in temperature or a result in terms of distributed measurement in deformation.
    [10" id="c-fr-0010]
    10. Digital processing method according to claim 9, characterized in that said digital processing is performed by a graphical processing unit GPU (Graphical Processing Unit) in parallel with the acquisition.
    类似技术:
    公开号 | 公开日 | 专利标题
    EP3371554B1|2020-01-01|Optoelectronic device for distributed measurement by means of brillouin scattering
    EP3635354B1|2021-06-30|Optoelectronic device for distributed measurement by means of optical fibre
    CA2502275C|2008-08-05|System and method for resolution enhancement of a distributed sensor
    EP3353502B1|2019-10-30|Measurement system and temperature and/or shape change sensor using brillouin back-reflection analysis
    US10539476B2|2020-01-21|Temperature or strain distribution sensor comprising a coherent receiver to determine a temperature or a strain associated with a device under test
    CN109210385B|2020-10-20|Phase-OTDR | -based distributed optical fiber sensing system and method
    CN110470376B|2021-08-24|Interference distributed optical fiber acoustic sensing device and sensing method thereof
    EP2405287B1|2013-03-20|Device for remote laser detection and interferometry method
    WO2013001242A1|2013-01-03|Device for managing pulses in pump-probe spectroscopy
    RU2444001C1|2012-02-27|Brillouin reflectometer
    FR3034190B1|2019-10-25|OPTICAL FIBER SENSOR DISTRIBUTED FROM STRAIN STATE
    Liu et al.2014|A novel optical fiber reflectometry technique with high spatial resolution and long distance
    FR2710150A1|1995-03-24|Method for measuring the Brillouin scattering in an optical fibre and device for implementing this method
    FR3099245A1|2021-01-29|METHOD AND DEVICE FOR RECONSTRUCTING A RETRODUCED VECTOR ELECTROMAGNETIC WAVE
    FR2514959A1|1983-04-22|HETERODYNE DETECTION TRANSMITTER-RECEIVER LASER DEVICE
    Zhou et al.2012|High-spatial-resolution distributed vibration measurement using time-resolved optical frequency-domain reflectometry
    Cordes et al.2010|High axial resolution swept source for optical coherence tomography
    FR2622006A1|1989-04-21|Method and device for processing a beam emitted by a single-frequency semiconductor laser source
    Kaczmarek et al.2004|Optical frequency domain reflectometer for diagnostics of short distance networks
    同族专利:
    公开号 | 公开日
    US20190063963A1|2019-02-28|
    EP3371554B1|2020-01-01|
    WO2017077257A1|2017-05-11|
    EA034423B1|2020-02-06|
    CN108603773B|2020-05-29|
    CA3004394A1|2017-05-11|
    FR3043457B1|2020-02-07|
    CN108603773A|2018-09-28|
    EP3371554A1|2018-09-12|
    US10274345B2|2019-04-30|
    EA201800304A1|2018-10-31|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    JP2010217029A|2009-03-17|2010-09-30|Nippon Telegr & Teleph Corp <Ntt>|Method and apparatus for measuring brillouin backward scattering light|CN111051832A|2017-05-11|2020-04-21|费布斯光学公司|Photoelectric device for optical fiber distributed measurement|GB9626099D0|1996-12-16|1997-02-05|King S College London|Distributed strain and temperature measuring system|
    US7283216B1|2004-06-22|2007-10-16|Np Photonics, Inc.|Distributed fiber sensor based on spontaneous brilluoin scattering|
    GB2440952B|2006-08-16|2009-04-08|Schlumberger Holdings|Measuring brillouin backscatter from an optical fibre using digitisation|
    CN100504309C|2007-09-30|2009-06-24|南京大学|Brillouin optical time domain reflection measuring method based on quick fourier transform|
    US9120286B2|2011-03-31|2015-09-01|Fos Llc|Fiber optic sensor thermally matched support tubes for distributed fiber optic sensing|
    GB201020827D0|2010-12-08|2011-01-19|Fotech Solutions Ltd|Distrubuted optical fibre sensor|
    CN203310428U|2013-06-26|2013-11-27|武汉华之洋光电系统有限责任公司|Distributed Brillouin optical fiber sensing system based on coherent detection|
    CN103674110B|2013-11-26|2016-06-01|北京航天时代光电科技有限公司|A kind of distribution type fiber-optic temperature strain sensor based on Brillouin's light amplification detection|CN108896274B|2018-06-14|2019-12-27|大连理工大学|Distributed optical fiber strain demodulation method based on subset window length optimization algorithm|
    EP3757522B1|2019-06-28|2021-07-21|Alcatel Submarine Networks|Method and apparatus for suppression of noise due to local oscillator instability in a coherent fiber optical sensor|
    CN110361037B|2019-07-01|2021-11-23|武汉理工大学|Distributed sensing preprocessing system based on weak grating array and peak searching method|
    CN111486881A|2020-04-23|2020-08-04|全球能源互联网研究院有限公司|Distributed optical fiber multi-parameter sensing device|
    法律状态:
    2016-10-20| PLFP| Fee payment|Year of fee payment: 2 |
    2017-05-12| PLSC| Publication of the preliminary search report|Effective date: 20170512 |
    2017-10-20| PLFP| Fee payment|Year of fee payment: 3 |
    2019-10-22| PLFP| Fee payment|Year of fee payment: 5 |
    2020-11-19| PLFP| Fee payment|Year of fee payment: 6 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1560681|2015-11-06|
    FR1560681A|FR3043457B1|2015-11-06|2015-11-06|OPTOELECTRONIC DEVICE FOR MEASUREMENT DISTRIBUTED BY BRILLOUIN DIFFUSION.|FR1560681A| FR3043457B1|2015-11-06|2015-11-06|OPTOELECTRONIC DEVICE FOR MEASUREMENT DISTRIBUTED BY BRILLOUIN DIFFUSION.|
    CN201680078220.3A| CN108603773B|2015-11-06|2016-11-04|Photoelectric distributed measuring device based on Brillouin scattering|
    CA3004394A| CA3004394A1|2015-11-06|2016-11-04|Optoelectronic distributed measuring device based on brillouin scattering|
    EA201800304A| EA034423B1|2015-11-06|2016-11-04|Method for digitally processing a signal generated by an optoelectronic distributed measuring device based on brillouin scattering|
    US15/773,626| US10274345B2|2015-11-06|2016-11-04|Optoelectronic distributed measuring device based on brillouin scattering|
    EP16806253.7A| EP3371554B1|2015-11-06|2016-11-04|Optoelectronic device for distributed measurement by means of brillouin scattering|
    PCT/FR2016/052870| WO2017077257A1|2015-11-06|2016-11-04|Optoelectronic distributed measuring device based on brillouin scattering|
    [返回顶部]