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    • 专利摘要:
    The invention relates to an optoelectronic measuring device distributed by optical fiber, said device comprising a continuous light source (1) emitting a continuous light signal at a first frequency v0, an acousto-optical modulator (6) able to transform said continuous signal a pulse signal for injection into an optical fiber (15) to be tested and a photo-detection module (10) adapted to detect a backscatter signal from a Rayleigh backscatter and spontaneous Brillouin backscattering from said optical fiber (15) to be tested, said device being characterized in that it further comprises a first coupler (3) and a second coupler (9), said second coupler (9) being able to mix the signal of the local oscillator with backscatter signal from said optical fiber (15) to be tested before transmitting it to the photo-detection module (10), the backscatter signal being modulated at the less at a frequency vrB equal to v0 - vbref + VA + VbAS, where VbAS is the anti-Stokes Brillouin (backscattering) frequency, and preferably also modulated at a frequency vrR equal to v0 + vA of Rayleigh backscattering which can be measured at any point z of said optical fiber (15), and said photo-detection module (10) being able to transmit the received backscattering signal, to a processing module (12) able to connect said anti-Stokes Brillouin frequency vbAS at a temperature value or a deformation value at any point z of said optical fiber (15) to be tested.
    公开号:FR3066280A1
    申请号:FR1754158
    申请日:2017-05-11
    公开日:2018-11-16
    发明作者:Vincent Lanticq；Pierre Clement；Etienne Almoric
    申请人:Febus Optics；
    IPC主号:
    专利说明:

    OPTOELECTRONIC FIBER DISTRIBUTED MEASUREMENT DEVICE
    [Field of the inventionl [001] The invention relates to an optoelectronic device for measuring distributed by optical fiber. The invention relates more specifically to an optoelectronic device capable of measuring the parameters of the Brillouin and Rayleigh backscatter spectra and which may include a means capable of separating the distributed measurement of temperature and the distributed measurement of deformation.
    Such devices can be used for the permanent control of the integrity and security of systems and structures in the civil engineering or the petroleum industry.
    [Prior Art] [003] Optoelectronic fiber optic measurement devices are generally used to measure, in real time, the temperature and deformations of large infrastructures in order to monitor their structural health and ensure their maintenance. They provide, at each measurement, the temperature and deformation information at any point of the optical fiber connected to them. The measurements are generally carried out with a range of a few meters to several tens of kilometers and a metric or even centimeter resolution. So, for example, a measurement can be made every meter on a structure with a length of 20 kilometers.
    Optoelectronic measurement devices distributed by optical fiber exploiting the Brillouin backscatter phenomenon are already known and used for applications of temperature and deformation measurements in civil engineering. These systems find in particular a privileged ground for the monitoring of linear structures such as bridges, dams, hydraulic earth dams or fluid transport networks (water, hydrocarbons, gas) in order to control ground movements (sliding, settlement ) or the deformations of the buried pipes or not.
    In order to be able to analyze variations in intensity over tens of kilometers with metric spatial resolution, the measurement systems generally use optical temporal reflectometry OTDR (from the English acronym "Optical Time Domain Reflectometry"). OTDR consists in propagating a light pulse in the optical fiber to analyze and to measure the return intensity as a function of time. The time it takes for the backscattered light 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, for example resulting in a resolution of about 1 m. Thanks to the Brillouin backscatter phenomenon combined with the OTDR technique, temperature and deformation measurements are made distributed along the fiber, over several tens of kilometers, with metric or even centimeter resolution.
    The measurements along the fiber are carried out with a device as shown schematically in Figure 1. The light from a light source 1, such as a laser, is distributed in two arms. One of the arms, called a “pump”, makes it possible to send the light signal, in impulse form thanks to an acousto-optical modulator 6, in the optical fiber 15 to be tested. A signal is backscattered by the optical fiber 15, according to the Brillouin phenomenon. According to the Brillouin phenomenon, the spectral components of backscattering of light by the material constituting the optical fiber, generally silica, have a frequency vBz offset from that vO of the incident light wave. The Brillouin frequency offset is generally around 11 GHz for an incident wave of wavelength λo = 1550 nm. Such a frequency is very high. To be able to carry out the processing on the backscattered signal, it is possible to transpose the frequency to 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 consisting in recombining the backscattered signal to be analyzed with a wave coming from the other arm, called “local oscillator” 50. This local oscillator 50 can for example be in the form of a laser in Brillouin ring. In this case, the continuous light signal of frequency vo is directed to a circulator 51 which in turn directs it to a reference fiber. This reference fiber emits by amplified spontaneous scattering radiation in the opposite direction of frequency vo - VBref which the circulator sends to a coupler 52. The latter sends part of the energy to the output signal, while it redirects the another part to the reference fiber where the radiation is amplified by a gain factor G by stimulated Brillouin scattering (amplified spontaneous) before being redirected to the circulator 51 which returns the amplified radiation to the coupler 52 and the output. The local oscillator 50 then forms an amplification ring by stimulated Brillouin scattering. A photo-detector 10 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 12. Such an optoelectronic measurement device distributed by Brillouin scattering in an optical fiber, using a single laser frequency to generate a light pulse, is more particularly described in document US 7,283,216. Document JP 2010 217029 describes another optoelectronic device. distributed measurement by Brillouin scattering using a single laser frequency to generate a pulse of light. The device aims, via heterodyne detection, to reduce the light reception bandwidth of the Brillouin backscattering light so as to reduce the costs and facilitate the processing of the backscattered light. For this, the device comprises a reference fiber similar to the test fiber so as to measure a frequency difference between the backscatter lights of the reference line and of the line to be tested. However, one of the drawbacks of these devices is that they have long measurement times. Indeed, typically, the measurement time is greater than 1 minute for a 10 km fiber.
    In addition, during the Brillouin backscattering measurement, the temperature and deformation parameters both create the same physical phenomenon in the optical fiber (variation of the Brillouin backscattering frequency vb). Thus, the Brillouin frequency vb, depends linearly on the temperature and the deformation in the material. The frequency shift Avb between the incident wave and the backscattered wave therefore varies with the temperature variations ΔΤ and deformation ε according to the equation: Avb = ΟτΔΤ + Οεε, where Ct and Ce are the temperature sensitivity coefficients and deformation specific to the optical fiber used. Thus, at the present time it is impossible to be able to differentiate the temperature parameter and that of deformation on the same Brillouin backscatter measurement.
    The only way to overcome this problem with this type of device is to fix one of the two constraints, either by mechanically fixing the optical fiber to be able to measure only the temperature, either by thermal insulation or by making the approximation that the temperature is stable around the optical fiber for the purpose of measuring only deformation. These methods are never 100% effective and there is always a residual uncertainty on the measurement because it is impossible to guarantee that a fiber is protected from all stresses (for example friction or crushing of the tube) especially when the cable which contains it is no longer accessible.
    Other solutions have been proposed such as carrying out distributed temperature measurements by Raman scattering (Alahbabi, Μ. N., et al. Optics Letters 30, no. 11 (June 1,2005): 1276-78 ) and use this measurement to subtract the effect of temperature on the Brillouin frequency to determine the deformation. But this often poses significant implementation difficulties because the two measurements are not carried out in the same fiber, and two separate instruments are used. Therefore, a perfect spatial alignment of the measurements of the two instruments is necessary. There is also a high level of complexity, a deterioration in accuracy, notably linked to the cumulative drifts of the two devices and also an additional cost associated with the purchase of two devices and the engineering of use of the two measurements to translate the results into measurement simultaneous temperature and deformation (for example alignment of measurement grids, estimation of uncertainties, correction of drifts). Finally, in general, systems based on two separate measures generate poor quality results because generally the errors linked to the two measures accumulate and there is a drift in the transfer functions of each measure which must be taken into account in the uncertainty about long-term measures.
    Thus, there is also a need for a device capable in a single measurement and from a single optical fiber to be tested of differentiating the temperature parameter and that of deformation.
    [Technical problem] The invention therefore aims to remedy the drawbacks of the prior art. The invention aims in particular to propose an optoelectronic measurement device distributed by optical fiber, simple and space-saving and capable of producing a more precise and rapid measurement comprising little or no interference at low frequencies. For this, the optoelectronic device has a new architecture allowing the generation of a local oscillator that does not induce little or no spurious signals. A reference fiber is included in the "pump" arm to generate an amplified spontaneous diffusion signal allowing to get rid of all the necessary prior checks.
    The invention also aims to propose an optoelectronic measurement device distributed by optical fiber, capable in a single measurement and from a single optical fiber to be tested, of differentiating the temperature parameter and that of deformation. For this, the optoelectronic device presents a new architecture allowing a simultaneous measurement of the anti-Stokes line of Brillouin backscattering and Rayleigh backscattering.
    In addition, the device proposed according to the invention makes it possible to carry out analyzes much faster than the devices of the prior art while comprising fewer energy consuming elements than the existing systems described in the prior art which makes it possible to have a portable device suitable for interventions by a foot operator or for occasional measurements.
    [Brief Description of the Inventionl To this end, the optoelectronic measurement device distributed by optical fiber according to the invention comprises a continuous light source emitting a continuous light signal at a first frequency vo, a modulator capable of imposing a frequency offset of at least 100 MHz to the continuous signal and to transform it into a pulse signal intended to be injected into an optical fiber to be tested and a photo-detection module capable of detecting a backscatter signal originating from the fiber optic 15 to be tested, resulting from an amplified spontaneous Brillouin backscattering and / or a Rayleigh backscattering coming from said optical fiber to be tested, said device being mainly characterized in that it further comprises a first coupler and a second coupler, said first coupler being capable of dividing said continuous light signal into two signals of identical frequency distributed in two b flush, - a first arm connecting the first coupler to a reference fiber block comprising a reference fiber, said reference fiber block being capable of emitting another light signal of frequency vo - vbref, where vbref is the Brillouin frequency of the fiber without distortion and at a reference temperature, - a second arm connecting the first coupler to the second coupler located upstream of the photo-detection module and capable of transmitting to the second coupler a continuous light signal at a frequency vo, thus constituting a local oscillator, said second coupler being able to couple the signal from the local oscillator to the backscatter signal from said optical fiber to be tested before transmitting it to the photo-detection module, the backscatter signal being modulated at an equal vrB frequency at vo - vbref + va + vbAs, where vbAs is the Brillouin anti-Stokes backscattering frequency that can be measured in any point z of said optical fiber, and said photo-detection module being able to transmit the received backscattering signal, to a processing module able to link the modulation of the backscattering signal to a temperature value and to a deformation value at any point z of said optical fiber to be tested.
    Thus, the device used makes it possible to dispense with all the prior checks necessary when using a local oscillator having a Brillouin ring laser configuration. In fact, in the configuration according to the invention, the return signal emitted by the reference fiber is an amplified spontaneous diffusion signal (by stimulated diffusion), and not the product of a resonance in a laser type cavity which consequently would strongly depend on the exact length of the cavity, difficult to control depending on influence parameters such as temperature.
    In addition, this new architecture including the presence of a reference block positioned on the pump line gives the user the possibility of measuring the Brillouin backscatter anti-Stokes line. Such a configuration makes it possible to improve the measurement quality by having a signal in the local oscillator without interference at low frequencies. It is therefore not necessary to use a low frequency electric filter at the output of the photo-detection module. Finally, such a configuration has a smaller footprint and reduced electrical consumption.
    According to another advantageous characteristic of the device, it can further comprise a third coupler and a fourth coupler, the third coupler being capable of dividing said continuous light signal coming from the light source into two signals of identical frequency distributed in two arms , - a first arm connecting the third coupler to the first coupler and capable of transmitting to the first coupler a continuous light signal at a frequency vo, - a second arm connecting the third coupler to the fourth coupler located upstream of the modulator and capable of transmitting to the fourth coupler an initial signal at a frequency vo, said fourth coupler being capable of coupling the initial signal vo to the light signal of frequency vo - vbref, coming from the reference block.
    This optional feature based in particular on the presence of a series of couplers gives the user the possibility of differentiating, in a single measurement and on a single fiber to be tested, the temperature parameter and that of deformation. It allows a simultaneous measurement of the anti-Stokes line of Brillouin backscattering and Rayleigh backscattering and this from a single measurement, the latter always being situated around the frequency vo + va (.va in the electrical field). is particularly advantageous compared to the devices of the prior art which require the implementation of two measurements, for example via the use of two measurement devices (for example Brillouin and Raman).
    The invention also relates to a method of digital processing of a signal for example from an optoelectronic measurement device distributed by optical fiber according to the invention, said method comprising the following steps: - digitizing a corresponding signal to the beating between a backscattered signal from an optical fiber to be tested and a reference signal, and detected by a photo-detection module, - cutting said digital signal into a plurality of sections (T1 ... Τί.,. ΤΝ ) by applying a sliding time window of the rectangular window or Hamming, or Hann or Blackman-Harris window type, each section having a width equal to the time width of a pulse of the pulse signal injected into the optical fiber to be tested , the width of each section being further centered around a date t corresponding to a point of coordinate z of said optical fiber to be tested, - calculate, pa r use of a discrete quarter transform algorithm, the frequency spectrum of each section (T1 ... Τί.,. ΤΝ) of said digitized signal; - repeating the first three steps and averaging the frequency spectra obtained for each point z of said optical fiber to be tested; - from the averaged frequency spectra, determine the variation of the frequency maxima of the Brillouin backscattering, and / or the variation of the total intensity of the Brillouin backscattering and / or the variation of the total intensity of the Rayleigh backscattering, by as a function of the back and forth time tz of backscattering, - apply a coefficient of sensitivity to temperature on the one hand and a coefficient of sensitivity to deformation on the other hand, on said determined variation (s), in order to obtain a result in term of measurement distributed in temperature and / or a result in term of measurement distributed in deformation.
    The method according to the invention relates to digital processing of the signals which can be applied as soon as the output of a photo-detection module. The following signal processing is done digitally at the spectral level and not directly on the signal. This processing includes in particular the cutting of the digitized signal into a plurality of sections whose width is equal to the temporal width of a pulse of the pulse signal injected into the optical fiber to be tested. Thus, the duration of a measurement is short relative to the duration of measurement of the systems of the prior art. Typically the duration of a measurement is 1 to a few seconds for a 10 km fiber.
    According to another advantageous characteristic of the method, it can comprise the determination, from the averaged frequency spectra, of the variation of the frequency maxima of the Brillouin Anti-Stokes backscattering and the variation of the total intensity of the Brillouin backscattering and the variation of the total intensity of the Rayleigh backscatter as a function of the time back and forth tz of the backscatter, as well as the determination of the ratio of total Rayleigh intensity and total Brillouin intensity at any point (z) of the fiber. This ratio corresponding to the Landau Placzek ratio.
    This optional feature allows the user to differentiate, in a single processed measurement, the temperature parameter and that of deformation. This is particularly advantageous compared to the prior art methods which require the processing of signals originating from at least two measurements.
    Other advantages and characteristics of the invention will appear on reading the following description given by way of illustrative and nonlimiting example, with reference to the appended figures which represent: • Figure 1, already described, a diagram of an optoelectronic measurement device distributed by Brillouin backscattering according to the prior art, • Figure 2, a diagram of an optoelectronic measurement device distributed by optical fiber according to the invention, the dotted elements being optional elements, • FIGS. 3A to 3C, time traces obtained in the first steps of the digital processing process of the digitized signal, and averaged, interpretable frequency spectra, obtained following the fourth step of the process according to the invention relating to the portion T1 (solid line ) TN (dotted line), • Figures 4A to 4B, the Brillouin frequency (4A) and the Landau Pla report czek (4B) at two different temperatures, obtained from a set of scattering spectra (Rayleigh and Brillouin) on a fiber of length about 150 m, • Figures 5A to 5B, distributed measurements of temperatures (5A ) and deformation (5B), obtained on a fiber of 150 meters with the device according to the invention, from a single measurement.
    [Detailed description of the invention] [0024] The term “optical fiber to be tested (or under test)” is used below to refer to the optical fiber placed along a structure to be monitored and which makes it possible to carry out a distributed measurement.
    By reference optical fiber is meant an optical fiber which may have a different Brillouin frequency, identical or substantially identical to the frequency
    Brillouin of the test fiber. This reference optical fiber is maintained throughout the measurement without deformation and at a reference temperature. The term optical fiber with different Brillouin frequency designates an optical fiber whose Brillouin frequency has a frequency difference with the Brillouin frequency of the optical fiber to be tested, of at least 200 MHz and preferably a difference of at least 300 MHz .
    "Single measurement" means a series of pulses making it possible to obtain an averaged frequency spectrum.
    The term “measurement duration” is understood to mean the time necessary for the system to display a measurement at nominal accuracy in terms of deformation or temperature. This duration includes both: • the acquisition time, • the system calculation time (Fourrier transforms, averages, etc.) By substantially or substantially identical, we mean in the sense of the invention a value varying by less than 30% relative to the compared value, preferably by less than 20%, even more preferably by less than 10%.
    By majority, we mean within the meaning of the invention at least 50%.
    The present invention relates generally to optoelectronic devices for distributed fiber optic measurement. The invention relates more precisely to an optoelectronic configuration of the device making it possible to increase its accuracy, to reduce its electrical consumption, to reduce its size, to reduce the duration of a measurement and to provide a distributed measurement separate from the temperature and the deformation.
    Figure 2 shows more particularly the configuration of an optoelectronic measuring device distributed by 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 materialized by a laser, preferably a DFB laser (from the English acronym "Distributed Feedback"), using a Bragg grating. The emission wavelength λ 0 is preferably equal to or substantially equal to 1550 nm, at the corresponding frequency vo.
    The beam of the emitted light wave is centered on the emission wavelength Ào and its width is at most 1 MHz.
    Advantageously, the light source 1 is frequency tunable and it is possible to vary its frequency continuously at a speed of at least 1 GHz / sec over an interval of at least 125 GHz. More preferably, the light source 1 is capable of emitting continuous laser radiation at an optical frequency vo which can be varied, over the duration of all the acquisitions, following a continuous ramp of at least 250 GHz. This frequency modulation must be continuous and not by frequency step and thus makes it possible to reduce the effects of intra-pulse interference and therefore the noise. This feature is particularly important when monitoring Rayleigh backscatter is desired.
    Light source 1, for example a laser, emits a moderately strong continuous light signal, typically of the order of 20 mW, in an optical fiber connecting it to a first coupler 3 or to the third coupler 2.
    The first coupler 3, receiving the light signal via light source 1 or via the first arm 21 of the third coupler 2, is capable of dividing said continuous light signal into two signals of identical frequency distributed in two arms.
    The first arm 31 connects the first coupler 3 to a reference fiber block 4 comprising a reference fiber 42, said reference fiber block 4 being capable of emitting another light signal of frequency vo - vbref, where vbref is the Brillouin frequency of the reference fiber 42, intended to be transmitted to the modulator 6 or to be mixed with said initial signal by a fourth coupler 5. Thus, the reference block 4 makes it possible to return the information in a lower frequency band improving thus the performance of the device. The reference optical fiber 42 is stored without deformation and at a reference temperature. The second arm 32 connects the first coupler 3 to a second coupler 9 located downstream from the modulator 6 and is capable of transmitting to the second coupler 9 a continuous light signal at a frequency vo, thus constituting a local oscillator. More particularly, the second arm 32 connects the first coupler 3 to a second coupler 9 located upstream of the photodetection module 10 and preferably it is positioned just before said photodetection module 10.
    The first coupler 3 is able to direct enough energy from the light signal to the first arm 31 so as to exceed the Stimulated Brillouin Scattering threshold and thus, in the reference fiber 42, l backscattered wave is shifted in frequency by -vbref relative to the optical wave. Advantageously, the first coupler 3 is capable of directing the majority of the energy of the light signal towards the first arm 31. Preferably, the first coupler 3 is capable of directing more than 70%, more preferably more than 80 %, even more preferably substantially 90% of the energy of the light signal towards the first arm 31.
    The reference block 4 advantageously comprises a circulator 41 which directs the incident continuous light signal, at the frequency vo, from the first coupler 3, in a reference optical fiber 42. This reference optical fiber 42 can be identical to the optical fiber 15 to be tested. Advantageously, the reference fiber 42 is not subjected 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 42 also makes it possible to emit a signal by Brillouin backscattering in response to the continuous signal emanating from the light source 1, so that the reference block 4 makes it possible to transform the incident frequency vo into a frequency Vbr = vo- VBref, where VBref represents the Brillouin frequency of the reference optical fiber 42, and which lies for example in the same frequency range as the frequency VbAs originating from the signal backscattered by the optical fiber 15 to be tested. In addition, advantageously, the reference optical fiber 42 of the reference fiber block 4 has a Brillouin frequency different from that of the optical fiber 15 to be tested. For example, the reference optical fiber 42 has a Brillouin frequency offset by at least 200 MHz, preferably by at least 300 MHz relative to the Brillouin response of the fiber to be measured. Preferably, the Brillouin frequency of the reference optical fiber 42 has a frequency difference with the Brillouin frequency of the optical fiber 15 to be tested, between 300 MHz and 1 GHz. This avoids any spectral overlap of the Rayleigh and Brillouin spectra while limiting the requirements for further signal processing. Indeed, the photo-detection module 10 located at the end of the optoelectronic assembly receives a signal from the Rayleigh backscatter which is modulated at the frequency of the acousto-optical modulator va (for example 200 MHz) and from the Brillouin backscatter frequency modulated (vbAs - vbref + va) without there being any overlap between the two spectra.
    Such architecture allows positioning the reference fiber 42 on the same optical arm as the optical fiber 15 to be tested. This has the advantage of improving the quality of measurement by having a signal in the local oscillator coming directly from the source and therefore without interference at low frequencies. It is therefore not necessary to use a low frequency electric filter at the output of the photodetection module. This configuration also makes it possible to measure the anti-Stokes line of the Brillouin backscattering and, unlike the devices of the prior art, to access measurements close to the DC (for example around 100 MHz) in the electrical field where there is no was previously not possible to make reliable measurements.
    The third coupler 2 allows the incident light signal emitted by the light source 1 to be divided into two signals of identical frequency distributed in two arms 21, 22 of the device.
    The first arm 21 connects the third coupler 2 to the first coupler 3 and the first arm 21 is able to transmit to the first coupler 3 a continuous light signal at a frequency vo. The second arm 22 connects the third coupler 2 to a fourth coupler 5 located upstream of the modulator 6 and this second arm 22 is capable of transmitting to the fourth coupler 5 an initial signal at a frequency vo.
    Advantageously, the third coupler 2 is capable of directing the majority of the energy of the light signal towards the first arm 21. Preferably, the third coupler 2 is capable of directing more than 70%, more preferably more than 80%, even more preferably substantially 90% of the energy of the light signal towards the first arm 21.
    As specified, the fourth coupler 5 is able to mix the initial signal vo from the second arm 22 of the third coupler 2 with the light signal of frequency vo - vbref from the reference fiber 42 and inject them into the modulator 6. The signals from the reference optical fiber 42 are therefore recombined with the initial signal vodans the fourth coupler 5. At the output of the fourth coupler 5, a signal is obtained which contains a signal at the frequency v - vbref coming from the reference optical fiber 42 and a signal at the same frequency as the initial signal vo.
    The modulator 6 is able to impose a frequency offset of at least 100 MHz on the continuous signal and to transform it into a pulse signal intended to be injected into an optical fiber 15 to be tested. Preferably, the modulator 6 is an acousto-optic modulator 6. The modulator 6 can be associated with one or more amplifiers if necessary to give gain. The signal coming from the modulator 6 comprises at least two components, - a continuous component of frequency vo - vbref, transformed into a pulse component of frequency vpi = vo - vbref + va, and - a continuous component of frequency vo, transformed into a component pulse frequency vP2 = vo + va.
    The modulator 6 is able to generate a pulse signal having a frequency offset from the frequency of the continuous light signal. The frequency offset will applied to said offset frequency may be greater than or equal to 100 MHz. The frequency va is the frequency specific to the modulator 6 and is generally greater than or equal to 100 MHz and less than or equal to 1 GHz, preferably substantially equal to 200 MHz. The temporal width of the pulse thus generated can for example be between 10 ns and 500 ns, preferably it is substantially equal to 20 ns. The pulse signal is then directed to a circulator 7 which then injects it into the optical fiber 15 to be tested, on which the distributed measurement must be carried out. When the pulse signal passes, the optical fiber 15 transmits in the opposite direction a signal by spontaneous Brillouin backscattering at the frequency vfi = vo - vbref + va + vbAS (z); and vo - vbref + va - VbS (z) in which vbAs is the anti-Stokes Brillouin frequency to be measured at any point of z coordinate along the optical fiber 15. VbS (z) is the Brillouin Stokes frequency. The optical fiber 15 also emits in the opposite direction a signal by Rayleigh backscattering at the frequency vf2 = vo + va.
    These backscattered signals are directed, by the circulator 7, to the second coupler 9 where they are recombined with a signal vo from the local oscillator. In addition, advantageously, the second arm 32 can comprise a polarization jammer 8 then disposed upstream of the inputs of a second coupler 9. This makes it possible to reduce the effects of interference due to the polarization between the arm of the local oscillator and the measurement arm 25, also called a “pump” arm, and located between the circulator 7 and a second coupler 9.
    The second coupler 9 is able to couple the signal from the local oscillator to the backscatter signal from the optical fiber 15 to be tested before transmitting it to the photo-detection module 10. The second coupler 9 can be associated with optional modules such as a polarization beam splitter or polarization hybridization. The backscatter signal can be modulated at least at a Brillouin frequency vrB equal to vo - vbref + va + vbAs, where vbAs is the Brillouin anti-Stokes backscatter frequency that can be measured at any point z of the optical fiber 15 to be tested. This gives the user the possibility of measuring the Brillouin backscatter anti-Stokes line while taking advantage of a local oscillator without interference at low frequencies and thus improves the quality of the measurement.
    The backscatter signal from the optical fiber 15 to be tested can also be modulated at a Rayleigh frequency vrR equal to vo + va. This is possible when the device according to the invention comprises the third coupler 2 and fourth coupler 5. This second coupler 9 then allows the Rayleigh backscatter created in the optical fiber 15 to be tested to couple with the frequency of the local oscillator. Thus, the device according to the invention also makes it possible to measure the Rayleigh backscatter spectrum. Preferably, the backscatter signal is modulated at a frequency vrR equal to vo + va and at a frequency vrB equal to vo - vbref + va + vbAs.
    This or these beats are electronically detectable through the use of a photo-detection module 10 positioned downstream of the second coupler 9 and it is able to transmit the backscatter signal received to a processing module 12. The photo-detection module 10 comprises at least one photo-detector. Advantageously, the photo-detection module 10 has a bandwidth of at least 800 MHz, preferably at least 1GHz. The photo-detection module 10 located at the end of the optoelectronic assembly is capable of receiving a signal from the Rayleigh backscatter modulated at the frequency of the acousto-optical modulator va and the Brillouin backscatter modulated at the frequency (vbAs - vbref + go). Under these conditions, at the output of the photo-detection module 10 the electrical signal obtained corresponding to the beats detected at the frequency of VBatti = va + (vbAs - VBref) corresponding to the Brillouin backscattering and at the frequency of VBatt2 = va corresponding to the Rayleigh backscatter. Thanks to the architecture of the device according to the invention, these beats were obtained from a single measurement and a single optical fiber 15 to be tested. In addition, these beats have a lower frequency than the incident signals because the frequency vo from the light source 1 is eliminated. Typically, a first beat corresponding to Batti = va + (vôas - VBref) has a frequency greater than 200 MHz, and preferably around 500 MHz, and a second beat corresponding to VBatt2 = va has a frequency for example substantially equal to 200 MHz, corresponding to the order of magnitude of the frequency specific to modulator 6. Indeed, va - (vbs + VBref) is around 20 GHZ and therefore out of band. The optical configuration therefore makes it possible to increase the efficiency of the photo-detection module 10 by limiting the bandwidth to less than 2 GHz instead of 11 GHz, preferably to less than 1 GHz, for example between 400 MHz and 1 GHz.
    Advantageously, the device according to the invention may not include a low frequency electric filter at the output of the photo-detection module 10. Indeed, as previously specified, the positioning of the reference fiber 42 on the same optical arm that the optical fiber 15 to be tested makes it possible to improve the quality of measurement by having a signal in the local oscillator without interference at low frequencies. By eliminating these parasites at low frequencies, this configuration also gives access to information which cannot be used with the configurations of the prior art (e.g. <100 MHz).
    The beat signal (s) obtained can then be digitized, by means of an analog-to-digital converter module 11. Then they are processed by a digital processing module 12. Advantageously, the analog-digital converter module 11 has a bandwidth of at least 800 MHz, preferably at least 1 GHz and a sampling speed of at least 1.6 Gech / s, preferably d '' at least 2 Gech / s.
    The processing module 12 is configured to connect said Brillouin anti-Stokes vbAs frequency to a temperature value and / or to a deformation value at any point z of said optical fiber 15 to be tested. Thus, it is able to separate the temperature measurement and the deformation measurement in order to obtain, from a single measurement, distinct values of temperature and deformation. The latter may include an acquisition card which makes it possible to acquire the signal generated by the photo detection module 10 and therefore have a bandwidth and a sampling frequency capable of analyzing a signal corresponding to: va + VbAs- vbref. Thus, advantageously, the processing module 12 is able to measure a signal having a bandwidth of at least 800 MHz, preferably of at least 1 GHz and a sampling speed of at least 1.6 Gech / s , preferably at least 2 Gech / s in order to detect the two spectra simultaneously (Brillouin spectrum and Rayleigh spectrum). In addition, advantageously, it is advisable to use an acquisition card with a high resolution such as for example a resolution greater than or equal to 10 bits. This allows, considering the small variations in intensity of the Brillouin backscattered spectrum as a function of temperature, to reach an accuracy of around 1 ° C. The analog-digital converter 11 and processing 12 modules are presented separately but can be integrated into one and the same assembly positioned directly after the photo-detection module 10.
    The processing module 12 is capable of cutting the digitized signal into a plurality of sections (T1 ... Τί.,. ΤΝ) by application of a sliding time window of the rectangular window or Hamming or Hann type. or Blackman-Harris, each section having a width equal to the time width of a pulse of the pulse signal injected into the optical fiber 15 to be tested, the width of each section being further centered around a date t corresponding to a z coordinate point of said optical fiber 15 to be tested.
    In addition, the digital processing module 12 advantageously uses a discrete quartermaster transform algorithm (preferably fast), for example by means of a logic integrated circuit known by the acronym FPGA (for “Field Programmable Spoiler”). Array ”). It thus makes it possible to directly calculate the Brillouin frequency, the total intensity of the Brillouin backscattering and / or the total intensity of the Rayleigh backscattering at any point of the z coordinate of the optical fiber 15 under test. The digital processing module 12 also makes it possible to average the spectra obtained in the frequency domain, for each point z of said fiber, at the end of the application of the discrete quartermaster transform algorithm (preferably fast), in order to determine the distributed measurement of the frequency variation all along said optical fiber 15 under test.
    According to another aspect, the invention relates to a method of digital processing of a signal which can be derived, preferably from, an optoelectronic measurement device distributed by optical fiber according to the invention. The various stages of digital processing carried out on the digitized signal are more particularly illustrated by experimental and explanatory Figures 3 to 5 which represent temporal or spectral traces obtained at each stage of the digital processing process of the digitized signal, obtained after recombination of the signals backscattered by the optical fiber under test and by the reference optical fiber.
    The processing method according to the invention comprises a first step of digitizing a signal corresponding to the beat between a backscattered signal from an optical fiber 15 to be tested and a reference signal, and detected by a photo module -detection 10. FIG. 3A represents the digitized signal at the output of the analog-digital converter 11. Preferably, the digitized signal comes from only one measurement and the processing method according to the invention relies on only one measurement carried out on an optical fiber 15 to be tested. Preferably, the signal comprises a va + beat (vüas - VBref) and a va beat.
    A second step in the digital processing performed by the digital processing module 12, consists of cutting the digitized signal into sections. The first step is to cut the digitized signal into sections around the date t corresponding to the z position on the fiber of width equal to the time width of the pulse. The segmentation is carried out for example by applying a sliding time window to the signal. Preferably, the windowing is produced by a rectangular window or by Hamming or by Hann or by Blackman-Harris. The division 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 being identified by the reference TN. Each section advantageously has a width equal to the time width of a pulse of the pulse signal injected into the optical fiber 5 to be tested. Each section T1 ... Ti ... TN is also centered around a date ti, ... ti..Tn corresponding to a point of coordinate z of said optical fiber to be tested. Thus, for a position of coordinate z on the optical fiber 15, z = 2nc * t, with c the speed of light and n the optical index of the fiber, and the time tz then corresponds to the round trip time (z ) of a pulse, counted down from the starting point of the pulse to the measurement point z. The difference between two measurement points can be as small as a sampling unit (slip of an interval). However, the difference between two independent measurements (spatial resolution) is considered to be equal to the width of the pulse. Thus, the distance between two independent measurement points z (t1), z (t2) is equal to the width of a pulse.
    Preferably, the digitized signal has portion by portion at least two spectra corresponding to the Brillouin spectrum va + (vb3s (z) - vBref) and to the Rayleigh spectrum va. A third step in digital processing then consists in calculating the frequency spectrum of each section T1 ... TÎ ... TN of said digitized signal, by the use of a Discrete Fourier Transform algorithm DFT and preferably an algorithm of FFT Fast Fourier transform. Thus, for each section T1 ... Ti ... TN of the digitized signal, a frequency spectrum is obtained.
    A fourth step consists in repeating the three stages of digitization, cutting and calculation of the frequency spectrum, and in averaging the results in order to obtain an averaged, interpretable frequency spectrum. Preferably, the fourth step makes it possible to generate an interpretable frequency spectrum comprising a Brillouin spectrum and a Rayleigh spectrum of which the maximum can be determined for the Brillouin frequency measurement, the energy for the Brillouin intensity measurement and the energy for the Rayleigh intensity measurement. It is a question of averaging the DFT curves (preferably FFT) to minimize the background noise. For example, we use a Gaussian or Lorentz adjustment algorithm. Two interpretable averaged frequency spectra are illustrated in Figure 3C corresponding to the section T1 (solid line) and to the section TN (dotted line) of the cut signal of Figure 3B. These interpretable averaged frequency spectra make it possible to obtain the frequency of the beats vA + (vbAS (z) - VBref) and va. And for example to determine, for the beat vA + (vbAS (z) - v &amp; ef), the frequency position of the maxima of the Brillouin spectrum.
    The fifth step of the digital processing then consists in determining the variation of the frequency positions of the maxima of the Brillouin spectrum and / or of the total intensity of the Rayleigh and Brillouin spectra, as a function of the z coordinates of the different points of the optical fiber 15 , and may include a step consisting in drawing one or more graphs of the distributed measurement of variation of maximum frequency or intensity along the optical fiber 15 to be tested. Preferably, the fifth step of the digital processing consists in determining the frequency positions of the maxima of the Brillouin spectrum and the total intensity of the Rayleigh and Brillouin spectra respectively, as a function of the z coordinates of the different points of the optical fiber 15. For example, FIG. 4A represents the frequency positions of the maxima of the Brillouin spectrum as a function of the z coordinates of the optical fiber 15 to be tested under two different conditions: in an environment at homogeneous temperature (solid line) and in an environment where the optical fiber 15 is exposed to a heat source (dotted line). This fifth step can also include a sub-step for determining the ratio of total Rayleigh intensity and total Brillouin intensity at any point (z) of the fiber in order to determine the Landau Placzek ratio depending on the temperature parameter. . Variations in temperature only created on an optical fiber cause the Brillouin backscattering intensity to increase or decrease. This intensity can be normalized by means of a Rayleigh backscattering measurement which makes it possible to give information on the linear losses of the fiber tested as well as the defects of the latter which can cause optical losses. This normalization involves the calculation of the Landau Placzek ratio. For example, FIG. 4B represents the Landau Placzek ratio as a function of the z coordinates of the optical fiber 15 to be tested under the two conditions above. The intensity of the Brillouin backscatter spectrum varies depending on the temperature parameter. However, in order to obtain a representative measurement of the Brillouin intensity, the Brillouin backscattering intensity should be normalized by the Rayleigh backscattering intensity (representative of the optical losses in a fiber). In this way only the intensity variations on the Brillouin backscattered spectrum due only to the temperature are measured. The variation can for example be measured with respect to values of frequency positions of the maxima, and / or of total intensity, obtained during a previous measurement. Said values being a function of the coordinates z of the different points of the optical fiber 15.
    Finally, a last step in digital processing consists in applying the sensitivity coefficient specific to the optical fiber 15 to be tested to variations in frequency positions and / or variations in total intensities of the Rayleigh and Brillouin spectra determined upstream. This can provide two results corresponding to a distributed measurement of deformation and a distributed measurement of temperature. This was not possible from a single measurement with the methods of the prior art since vBas (z) depends on these two parameters. In addition, in the prior art methods, these measurements could be obtained by an analysis of the Brillouin and Raman spectra, the acquisition of which requires two different devices and therefore necessarily two measurements.
    In particular, the last step of the digital processing consists in applying the coefficients of sensitivity, respectively of temperature Ct and of deformation CE, specific to the optical fiber 15, to obtain a result respectively in terms of distributed measurement of temperature and distributed measure of deformation. FIGS. 5A and 5B represent a graph obtained after application of the deformation sensitivity coefficients and making it possible respectively to obtain the distributed measurement of deformation ε all along the optical fiber and the distributed temperature measurement T all along the fiber optical. Thus, in the graph of FIG. 5A, it can be seen that the optical fiber analyzed is not deformed, whereas with regard to FIG. 5B there is a periodic variation of the temperature corresponding well to the presence of a source of heat near the coiled optical fiber 15. The coefficient Cvbs of sensitivity to deformation is typically 0.05 MHz / (pm / m)) and the coefficient of sensitivity to temperature CvbTest typically 1 MHz / ° C.
    More particularly, these measures can be determined by reversing the linear system (1).
    Linear system (1):
    With CPbs which can be considered zero compared to CPbT = 0.32% / ° C
    The invention allows a deletion of all analog electronic components, except the photo-detection module 10 and allows their replacement by a digitizer 11 and a digital processing module 12. Thus, it overcomes noise levels provided by active analog components such as amplifiers or oscillators for example. In addition, the signal processing being entirely digital, the treatments consume less energy and the
    device has a small footprint, so it can be carried. 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 is able to operate by accessing only one end of the optical fiber 15 to be tested and, as has been seen, it is capable of separately measuring the temperature and the deformations in the optical fiber 15 to be tested by a single measurement.
    In addition, the device makes it possible to use a digital calculation module making it possible to carry out treatments in parallel for each section, which reduces the measurement time to the acquisition time, for example for 10 km of fiber. have 10,000 acquisitions per second with a processor clock frequency of 10 kHz and thus obtain 10,000 averages. The digital calculation module advantageously includes a GPU type graphics processor (Graphical Processing Unit) in order to transfer the highly parallelizable calculation onto it. 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 10km fiber, with a processor clock frequency of 10 kHz, 10,000 acquisitions are made in one second, which gives 10,000 averages, whereas in the prior art the duration of a measurement is greater than one minute for 10 km.
    The use of the measurements returned by this device is devoted to optimizing the maintenance of works in the field of civil engineering or oil and gas for example. The continuity of the measurements along the optical fiber guarantees the detection of an event which would not have been by another process using punctual and localized measurements. The early detection of structural disorders in structures allows intervention before further deterioration. Conversely, the absence of detection can delay systematic maintenance operations if they are not necessary. In both cases, such an optoelectronic measurement device distributed by optical fiber allows an operator to make significant savings on the maintenance of civil engineering works.
    权利要求:
    Claims (10)
    [1" id="c-fr-0001]
    1. Optoelectronic measurement device distributed by optical fiber, said device comprising a continuous light source (1) emitting a continuous light signal at a first frequency vo, a modulator (6) capable of imposing a frequency offset of at least 100 Mhz to the continuous signal and to transform it into a pulse signal intended to be injected into an optical fiber (15) to be tested and a photo-detection module (10) capable of detecting a backscatter signal, coming from the optical fiber (15 ) to be tested, resulting from spontaneous Brillouin backscattering and / or Rayleigh backscattering coming from said optical fiber (15) to be tested, said device being characterized in that it further comprises a first coupler (3) and a second coupler (9), said first coupler (3) being capable of dividing said continuous light signal into two signals of identical frequency distributed in two arms, - a first arm (31) connecting the first coupler (3) to a reference fiber block (4) comprising a reference fiber (42), said reference fiber block (4) being capable of emitting another light signal of frequency vo - vbref, where vbref is the Brillouin frequency reference fiber (42) without deformation and at a reference temperature, - a second arm (32) connecting the first coupler (3) to the second coupler (9) located upstream of the photo-detection module (10) and capable of transmitting to the second coupler (9) a continuous light signal at a frequency vo, thus constituting a local oscillator, said second coupler (9) being capable of coupling the signal of the local oscillator to the backscatter signal from said optical fiber (15) to be tested before transmitting it to the photo-detection module (10), the backscatter signal being modulated at a frequency vrB equal to vo - vbref + va + vbAs, where vbAs is the Brillouin anti-Stokes backscatter frequency up be measured at any point z of said optical fiber (15), and said photo-detection module (10) being capable of transmitting the received backscatter signal, to a processing module (12) capable of connecting the modulation of the signal backscattering at a temperature value and at a deformation value at any point z of said optical fiber (15) to be tested.
    [2" id="c-fr-0002]
    2. Device according to claim 1, characterized in that it further comprises a third coupler (2) and a fourth coupler (5), the third coupler (2) being capable of dividing said continuous light signal coming from the light source (1) in two signals of identical frequency distributed in two arms, - a first arm (21) connecting the third coupler (2) to the first coupler (3) and capable of transmitting to the first coupler (3) a continuous light signal at a vo frequency, a second arm (22) connecting the third coupler (2) to the fourth coupler (5) located upstream of the modulator (6) and capable of transmitting to the fourth coupler (5) an initial signal at a vo frequency, said frequency fourth coupler (5) being able to couple the initial signal vo to the light signal of frequency v - vbref, coming from the reference block (4).
    [3" id="c-fr-0003]
    3. Device according to one of claims 1 or 2, characterized in that the reference optical fiber (42) has a Brillouin frequency offset by at least 200 MHz relative to the Brillouin response of the optical fiber (15) at test.
    [4" id="c-fr-0004]
    4. Device according to one of claims 2 or 3, characterized in that the backscatter signal contains the Rayleigh backscatter spectrum at a frequency vrR equal to vo + va and the Brillouin backscatter spectrum at a frequency vrB equal to vo - vbref + VA + VbAS.
    [5" id="c-fr-0005]
    5. Device according to any one of claims 1 to 4, characterized in that it comprises an analog-digital converter module 11 having a bandwidth of at least 800 MHz and a sampling frequency of at least 1, 6 Gech / s.
    [6" id="c-fr-0006]
    6. Optoelectronic measurement device distributed by optical fiber according to any one of claims 1 to 5, characterized in that it is able to operate by accessing only one end of the optical fiber (15) to be tested.
    [7" id="c-fr-0007]
    7. Optoelectronic distributed fiber optic measurement device according to any one of claims 1 to 6, characterized in that it is capable of separately measuring the temperature and the deformations in the optical fiber (15) to be tested in one one and only measure.
    [8" id="c-fr-0008]
    8. Optoelectronic measuring device distributed by optical fiber according to any one of claims 1 to 7, characterized in that the processing module 12 is capable of cutting the digital signal into a plurality of sections (T1 ... TÎ .. .TN) by application of a sliding time window of rectangular window type or of Hamming, or of Hann or of Blackman-Harris, each section having a width equal to the time width of a pulse of the pulse signal injected into the optical fiber. (15) to be tested, the width of each section being further centered around a date t corresponding to a point of coordinate z of said optical fiber (15) to be tested.
    [9" id="c-fr-0009]
    9. A method of digital processing of a signal from an optoelectronic measurement device distributed by optical fiber according to one of claims 1 to 8, said method comprising the following steps: - digitizing a signal corresponding to the beat between a backscattered signal from an optical fiber (15) to be tested and a reference signal, and detected by a photo-detection module (10); - cutting said digital signal into a plurality of sections (T1 ... TÎ ... TN) by applying a sliding time window of rectangular window or Hamming, Hann or Blackman-Harris type, each section having a width equal to the time width of a pulse of the pulse signal injected into the optical fiber (15) to be tested, the width of each section being further centered around a date t corresponding to a point of z coordinate of said optical fiber (15) to be tested; - calculate, by using a discrete quartermaster transform algorithm, the frequency spectrum of each section (T1 ... TÎ ... TN) of said digitized signal; - repeating the first three steps and averaging the frequency spectra obtained for each point z of said optical fiber (15) to be tested; - from the averaged frequency spectra, determine the variation of the frequency maxima of the Brillouin backscattering, and / or the variation of the total intensity of the Brillouin backscattering and / or the variation of the total intensity of the Rayleigh backscattering, by back and forth time function tz of backscatter; and - applying a coefficient of temperature sensitivity on the one hand and a coefficient of sensitivity to deformation on the other hand, on said determined variation (s), in order to obtain a result in terms of measurement distributed in temperature and / or a result in terms of measurement distributed in deformation.
    [10" id="c-fr-0010]
    10. A digital processing method according to claim 9, characterized in that it comprises the determination, from the averaged frequency spectra, of the variation of the frequency maxima of the Brillouin Anti-Stoke backscatter and the variation of the total intensity. of the Brillouin backscatter and the variation of the total intensity of the Rayleigh backscatter as a function of the round trip time tz of backscatter, as well as the determination of the ratio of Rayleigh intensity and Brillouin intensity at any point (z) of the fiber.
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    同族专利:
    公开号 | 公开日
    EP3635354A2|2020-04-15|
    ES2893548T3|2022-02-09|
    EP3635354B1|2021-06-30|
    US20200109971A1|2020-04-09|
    WO2018207163A2|2018-11-15|
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    2018-11-16| PLSC| Publication of the preliminary search report|Effective date: 20181116 |
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    优先权:
    申请号 | 申请日 | 专利标题
    FR1754158|2017-05-11|
    FR1754158A|FR3066280B1|2017-05-11|2017-05-11|OPTOELECTRONIC MEASURING DEVICE DISTRIBUTED BY OPTICAL FIBER|FR1754158A| FR3066280B1|2017-05-11|2017-05-11|OPTOELECTRONIC MEASURING DEVICE DISTRIBUTED BY OPTICAL FIBER|
    CA3063048A| CA3063048A1|2017-05-11|2018-05-14|Optoelectronic device for distributed measurement by means of optical fibre|
    PCT/IB2018/053353| WO2018207163A2|2017-05-11|2018-05-14|Optoelectronic device for distributed measurement by means of optical fibre|
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    EP18728981.4A| EP3635354B1|2017-05-11|2018-05-14|Optoelectronic device for distributed measurement by means of optical fibre|
    ES18728981T| ES2893548T3|2017-05-11|2018-05-14|Optoelectronic device for distributed measurement based on fiber optics|
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