CN102937416B - A kind of fully distributed fiber switched based on orthogonal polarisation state strains and vibration sensing method and device - Google Patents

A kind of fully distributed fiber switched based on orthogonal polarisation state strains and vibration sensing method and device Download PDF

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CN102937416B
CN102937416B CN201210472921.9A CN201210472921A CN102937416B CN 102937416 B CN102937416 B CN 102937416B CN 201210472921 A CN201210472921 A CN 201210472921A CN 102937416 B CN102937416 B CN 102937416B
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王峰
张旭苹
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Nanjing University
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Abstract

一种基于正交偏振态倒换的全分布式光纤应变与振动传感装置,包括激光器(1),保偏耦合器(2)、保偏光纤、脉冲调制模块(3)、光放大器(4)、环形器(5)、传感光纤(6)、偏振态倒换装置(7)、耦合器(8)、平衡光电探测器(9)、微波源(10)、混频器(11)、带通滤波器(12)、信号采集与处理单元(13);激光器的输出的连续光经保偏耦合器(2)后分为两路:其中保偏耦合器(2)输出的第一路中所有的连接光纤均为保偏光纤,经偏振态倒换装置后,再输入到耦合器(8)的第一输入端;偏振态倒换装置具有两种状态,分别使输出的线偏振光的偏振方向对应于保偏光纤的快轴和慢轴;带通滤波器输出端连接到信号采集与处理单元。

A fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization switching, including a laser (1), a polarization maintaining coupler (2), a polarization maintaining fiber, a pulse modulation module (3), and an optical amplifier (4) , circulator (5), sensing fiber (6), polarization switching device (7), coupler (8), balanced photodetector (9), microwave source (10), mixer (11), band Pass filter (12), signal acquisition and processing unit (13); the continuous light output by the laser is divided into two paths after passing through the polarization maintaining coupler (2): the first path output by the polarization maintaining coupler (2) All connecting fibers are polarization-maintaining fibers, which are input to the first input end of the coupler (8) after passing through the polarization state switching device; the polarization state switching device has two states, which respectively make the polarization direction of the output linearly polarized light Corresponding to the fast axis and the slow axis of the polarization maintaining fiber; the output end of the bandpass filter is connected to the signal acquisition and processing unit.

Description

一种基于正交偏振态倒换的全分布式光纤应变与振动传感方法和装置A fully distributed optical fiber strain and vibration sensing method and device based on orthogonal polarization state switching

技术领域technical field

本发明涉及一种对应变和振动进行全分布式监测的光纤传感设备,尤其是一种结合布里渊光时域反射(BOTDR)技术及偏振光时域反射(POTDR)技术,并采用偏振态倒换装置和相干外差检测的全分布式光纤应变及振动传感技术。The invention relates to an optical fiber sensing device for fully distributed monitoring of strain and vibration, especially a combination of Brillouin Optical Time Domain Reflectometry (BOTDR) technology and Polarized Optical Time Domain Reflectometry (POTDR) technology, and adopts polarization Fully distributed optical fiber strain and vibration sensing technology with state switching device and coherent heterodyne detection.

背景技术Background technique

由于当光纤受到外界环境(如温度,压力,振动等)影响时,光纤中传输光的强度,相位,频率,偏振态等参量将会相应的发生变化,通过测量传输光的这些参量便可以获得相应物理量,这种技术称为光纤传感技术。When the optical fiber is affected by the external environment (such as temperature, pressure, vibration, etc.), the parameters such as the intensity, phase, frequency, and polarization state of the transmitted light in the optical fiber will change accordingly. By measuring these parameters of the transmitted light, it can be obtained Corresponding physical quantity, this technology is called fiber optic sensing technology.

相对于传统的电量型传感器,光纤传感器具有灵敏度高,抗电磁干扰,体积小,价格便宜,可进行远距离分布式测量的优点,因此自20世纪70年代末以来,光纤传感技术得到了广泛的发展,出现了基于瑞利散射,布里渊散射,拉曼散射等的全分布式光纤传感技术。这些光纤传感技术利用光纤中光波的不同物理参量进行传感,可测量光纤上与物理量相对应的不同的传感参量。Compared with traditional electrical sensors, optical fiber sensors have the advantages of high sensitivity, anti-electromagnetic interference, small size, low price, and long-distance distributed measurement. Therefore, since the late 1970s, optical fiber sensing technology has been widely used The development of fully distributed optical fiber sensing technology based on Rayleigh scattering, Brillouin scattering, Raman scattering, etc. has emerged. These optical fiber sensing technologies use different physical parameters of light waves in optical fibers for sensing, and can measure different sensing parameters corresponding to physical quantities on optical fibers.

1)光纤受应变影响时,光波在其中产生的布里渊散射光的频率会发生偏移,称为布里渊频移。布里渊频移量的大小与光纤所受应变的大小成正比。布里渊光时域反射(BOTDR)技术通过向光纤中注入脉冲光,并测量脉冲光在光纤中传播过程中连续产生的布里渊散射光的布里渊频移,进而确定出光纤沿线各个位置的应变信息。BOTDR技术是目前为止最主要的一种可准确测量光纤中应变大小的全分布式光纤传感技术。但BOTDR技术对振动事件的测量能力较弱。因为尽管理论上光纤在受到外界振动影响时会同时产生应变变化。但是,一方面由于微小振动引起的微弱应变对布里渊频移产生的影响较小,另一方面BOTDR技术对应变的测量速度较慢,通常需要十几秒以上。因此,BOTDR技术难以用于测量振动。1) When the optical fiber is affected by the strain, the frequency of the Brillouin scattered light generated by the light wave in it will shift, which is called the Brillouin frequency shift. The magnitude of the Brillouin frequency shift is proportional to the magnitude of the strain on the fiber. The Brillouin Optical Time Domain Reflectometry (BOTDR) technology injects pulsed light into the optical fiber and measures the Brillouin frequency shift of the Brillouin scattered light continuously generated during the propagation of the pulsed light in the optical fiber, so as to determine the The strain information for the location. BOTDR technology is by far the most important fully distributed optical fiber sensing technology that can accurately measure the strain in optical fiber. However, BOTDR technology is weak in measuring vibration events. Because although theoretically the optical fiber will produce strain changes at the same time when it is affected by external vibrations. However, on the one hand, the weak strain caused by tiny vibrations has little effect on the Brillouin frequency shift, and on the other hand, the BOTDR technology measures the strain at a slow speed, which usually takes more than ten seconds. Therefore, the BOTDR technique is difficult to use to measure vibration.

2)偏振光时域反射(POTDR)技术同样是向光纤中注入脉冲光。但它通过测量脉冲光在光纤沿线返回的散射光的偏振态的变化来确定光纤沿线各个位置的外部事件,从而进行全分布式测量。由于光纤中光波偏振态的变化对外部事件的响应非常灵敏,因此可以用来测量微弱的外部事件。同时由于POTDR技术通过光强信号来判断散射光偏振态的变化,响应时间短,故可以用来测量快速的扰动或振动。对于1km的传感距离,POTDR可测量的最大振动频率在100KHz以内。但由于普通单模光纤中光波的偏振态在长时间内难以保持恒定,且光纤受到的应变与偏振态的变化并非一一对应,因此POTDR技术难以对准静态的应变及较大的应变进行检测。2) The Polarized Optical Time Domain Reflectometry (POTDR) technology also injects pulsed light into the optical fiber. However, it determines the external events at various positions along the fiber by measuring the change of the polarization state of the scattered light returned by the pulsed light along the fiber, so as to perform a fully distributed measurement. Since changes in the polarization state of light waves in the fiber are very sensitive to external events, they can be used to measure weak external events. At the same time, because the POTDR technology judges the change of the polarization state of scattered light through the light intensity signal, and has a short response time, it can be used to measure fast disturbances or vibrations. For a sensing distance of 1km, the maximum vibration frequency that POTDR can measure is within 100KHz. However, since the polarization state of light waves in ordinary single-mode optical fibers is difficult to keep constant for a long time, and the strain on the optical fiber is not in one-to-one correspondence with the change of polarization state, it is difficult for POTDR technology to detect quasi-static strain and large strain .

发明内容Contents of the invention

本发明的目的是,提供一种既可以测量应变又可以测量快速振动变化的全分布式光纤传感器。尤其是基于正交偏振态倒换的全分布式光纤应变与振动传感方法和装置。既可以测量应变事件,又可以测量振动事件,大大提高了全分布式光纤传感器的测量功能和应用范围,并保证测量精度。The purpose of the present invention is to provide a fully distributed optical fiber sensor that can measure both strain and rapid vibration changes. In particular, a fully distributed optical fiber strain and vibration sensing method and device based on orthogonal polarization state switching. Both strain events and vibration events can be measured, which greatly improves the measurement function and application range of the fully distributed optical fiber sensor, and ensures measurement accuracy.

本发明的技术方案是,一种基于正交偏振态倒换的全分布式光纤应变与振动传感装置,其特征是包括激光器(1),保偏耦合器(2)、保偏光纤、脉冲调制模块(3)、光放大器(4)、环形器(5)、传感光纤(6)、偏振态倒换装置(7)、耦合器(8)、平衡光电探测器(9)、微波源(10)、混频器(11)、带通滤波器(12)、信号采集与处理单元(13);激光器(1)的输出的连续光经保偏耦合器(2)后分为两路:其中保偏耦合器输出的第一路中所有的连接光纤均为保偏光纤,其中的光波作为参考光,经偏振态倒换装置(7)后,再输入到耦合器(8)的第一输入端;偏振态倒换装置(7)具有两种状态,分别使输出的线偏振光的偏振方向对应于保偏光纤的快轴和慢轴;The technical solution of the present invention is a fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization switching, which is characterized in that it includes a laser (1), a polarization maintaining coupler (2), a polarization maintaining optical fiber, and a pulse modulation Module (3), optical amplifier (4), circulator (5), sensing fiber (6), polarization switching device (7), coupler (8), balanced photodetector (9), microwave source (10 ), a mixer (11), a bandpass filter (12), a signal acquisition and processing unit (13); the output continuous light of the laser (1) is divided into two paths after passing through the polarization maintaining coupler (2): All the connecting fibers in the first path output by the polarization-maintaining coupler are polarization-maintaining fibers, and the light waves in it are used as reference light, and then input to the first input end of the coupler (8) after passing through the polarization state switching device (7) ; The polarization state switching device (7) has two states, respectively making the polarization direction of the output linearly polarized light correspond to the fast axis and the slow axis of the polarization-maintaining fiber;

保偏耦合器输出的第二路经脉冲调制模块(3)、光放大器(4)后作为探测脉冲光经环形器(5)注入传感光纤(6);传感光纤中的布里渊散射光经环形器(5)返回后进入耦合器(8)的第二输入端;布里渊散射光与参考光在耦合器(8)中形成的混合信号经耦合器(8)的两个输出端输入到平衡光电探测器(9)中被转换为电信号;The second path output by the polarization-maintaining coupler passes through the pulse modulation module (3) and the optical amplifier (4), and then injects the detection pulse light into the sensing fiber (6) through the circulator (5); the Brillouin scattering in the sensing fiber The light returns through the circulator (5) and enters the second input end of the coupler (8); the mixed signal formed by the Brillouin scattered light and the reference light in the coupler (8) passes through the two outputs of the coupler (8) input to the balanced photodetector (9) to be converted into an electrical signal;

平衡光电探测器(9)的输出端与混频器(11)的第一输入端相连,微波源(10)与混频器(11)的第二输入端相连,混频器(11)的输出端连接到带通滤波器(12),带通滤波器(12)的输出端连接到信号采集与处理单元(13)。The output end of the balanced photodetector (9) is connected to the first input end of the mixer (11), the microwave source (10) is connected to the second input end of the mixer (11), and the mixer (11) The output end is connected to the band-pass filter (12), and the output end of the band-pass filter (12) is connected to the signal acquisition and processing unit (13).

偏振态倒换装置(7)在任一单一状态时,由布里渊散射光与参考光进行相干外差检测,获取散射光偏振态的变化信息,以此确定外部振动事件信息。When the polarization state switching device (7) is in any single state, coherent heterodyne detection is performed by the Brillouin scattered light and the reference light to obtain the change information of the polarization state of the scattered light, so as to determine the external vibration event information.

偏振态倒换装置(7)可以是偏振开关、偏振控制器或偏振分析仪等任何可使线偏振光的偏振态在相互正交的两个偏振方向切换的器件或仪器,线偏振光在这两个正交方向的偏振分别对应于偏振态倒换装置(7)的第一和第二两种工作状态。The polarization state switching device (7) can be any device or instrument that can switch the polarization state of linearly polarized light in two orthogonal polarization directions, such as a polarization switch, a polarization controller, or a polarization analyzer. The polarizations in the two orthogonal directions respectively correspond to the first and second working states of the polarization state switching device (7).

按照本发明所提供的一种既可以测量应变又可以测量快速振动变化的全分布式光纤传感器进行测量光纤传感方法,当偏振态倒换装置(7)处于任一种工作状态时,传感光纤所得到的信号为传感光纤中的散射光信号与偏振方向沿保偏光纤快轴或慢轴的线偏振光经耦合器(8)和平衡光电探测器(9)相干外差检测之后的结果;当传感光纤(6)某个位置受到应变影响时,该位置处产生的布里渊散射光的布里渊频移的大小发生改变;受到振动影响时,该位置处探测脉冲光的偏振态发生变化,则在传感光纤(6)中的布里渊散射光的偏振态发生变化;因此通过测量布里渊散射光的中心频率,对传感光纤(6)的应变进行传感,通过测量布里渊散射光的偏振态变化,对传感光纤(6)的振动进行传感。According to a fully distributed optical fiber sensor that can measure both strain and rapid vibration changes provided by the present invention for measuring optical fiber sensing method, when the polarization state switching device (7) is in any working state, the sensing optical fiber The obtained signal is the result of the coherent heterodyne detection of the scattered light signal in the sensing fiber and the linearly polarized light whose polarization direction is along the fast axis or slow axis of the polarization maintaining fiber through the coupler (8) and the balanced photodetector (9). ; When a certain position of the sensing fiber (6) is affected by strain, the magnitude of the Brillouin frequency shift of the Brillouin scattered light generated at this position changes; when affected by vibration, the polarization of the detected pulsed light at this position When the state changes, the polarization state of the Brillouin scattered light in the sensing fiber (6) changes; therefore, by measuring the center frequency of the Brillouin scattered light, the strain of the sensing fiber (6) is sensed, The vibration of the sensing fiber (6) is sensed by measuring the polarization state change of the Brillouin scattered light.

进一步的,传感光纤(6)得到的信号包含有布里渊散射光偏振态变化的信息,利用偏振光时域反射(POTDR)原理进行测量,利用散射光偏振态的变化信息对振动进行传感。Further, the signal obtained by the sensing fiber (6) contains the information of the polarization state change of the Brillouin scattered light, which is measured by the principle of polarized light time-domain reflectometry (POTDR), and the vibration is transmitted by using the information of the change of the polarization state of the scattered light. feel.

进一步的,当偏振态倒换装置(7)在第一和第二两种工作状态下分别工作等长时间,然后将在此两种工作状态下得到的外差信号功率累加,则可消除传感光纤中光波偏振态变化的影响。此时可利用布里渊光时域反射(BOTDR)原理进行测量,利用布里渊散射光的频率信息对光纤中的应变进行传感。Furthermore, when the polarization state switching device (7) works for equal time in the first and second working states respectively, and then accumulates the heterodyne signal power obtained in these two working states, the sensing can be eliminated Effects of changes in the polarization state of light waves in an optical fiber. At this time, the principle of Brillouin Optical Time Domain Reflectometry (BOTDR) can be used for measurement, and the frequency information of Brillouin scattered light can be used to sense the strain in the optical fiber.

当偏振态倒换装置(7)处于任一种工作状态时,由于脉冲光在光纤中不同位置的偏振态各不相同,由平衡光电探测器(9)相干外差检测之后得到的脉冲光在光纤沿线产生的布里渊信号有相应的波动起伏。在不同的时间多次测量光纤中的布里渊信号后,通过比较它们之间波动起伏的不同或利用时频变换的方法分析光纤各位置处波动起伏变化的频谱,可得到光纤中脉冲光在某位置处的偏振态的变化情况。When the polarization state switching device (7) is in any working state, since the polarization states of the pulsed light at different positions in the fiber are different, the pulsed light obtained after coherent heterodyne detection by the balanced photodetector (9) is in the fiber The Brillouin signal generated along the line has corresponding fluctuations. After measuring the Brillouin signal in the optical fiber several times at different times, by comparing the fluctuations between them or analyzing the frequency spectrum of the fluctuations at each position of the optical fiber by using the method of time-frequency transformation, the pulsed light in the optical fiber can be obtained. The change in polarization state at a location.

脉冲光在传感光纤中传输时会不断在光纤沿线产生布里渊散射光,其中心频率相对于探测光的中心频率有一定的偏移,此偏移被称为布里渊频移vB;将微波源(10)的频率设置为vM(vM与vB较为接近),则该高频信号经混频器(11)后,其中心频率会被转换到|vB-vM|;通过扫描微波源(10)的频率来调整混频器(11)的输出信号的频率,当通过带通滤波器(12)的信号功率达到最大时,即可得到布里渊散射光的布里渊频移,其大小为vB=vM-fBPF,其中fBPF为带通滤波器(12)的中心频率。传感装置在测量振动和应变时利用的散射光均为布里渊散射光。When the pulsed light is transmitted in the sensing fiber, it will continuously generate Brillouin scattered light along the fiber, and its center frequency has a certain offset from the center frequency of the detection light. This offset is called the Brillouin frequency shift v B ;Set the frequency of the microwave source (10) to v M (v M is relatively close to v B ), then after the high-frequency signal passes through the mixer (11), its center frequency will be converted to |v B -v M |; By scanning the frequency of the microwave source (10) to adjust the frequency of the output signal of the mixer (11), when the signal power through the band-pass filter (12) reaches the maximum, the Brillouin scattered light can be obtained Brillouin frequency shift, whose magnitude is v B =v M -f BPF , where f BPF is the center frequency of the band-pass filter (12). The scattered light used by the sensing device when measuring vibration and strain is Brillouin scattered light.

本发明有益效果:本发明结合了BOTDR技术和POTDR技术,既可以测量应变事件,又可以测量振动事件,大大提高了全分布式光纤传感器的测量功能和应用范围,同时可大幅降低系统的漏报率。本发明仅利用布里渊散射光信号进行应变和振动的传感,系统装置简单,整体成本及器件数量比两个系统的单独叠加小很多。在利用POTDR技术进行振动测量的同时,通过切换偏振态倒换装置的工作状态,实现利用BOTDR技术对应变的测量,因此对振动和应变的测量可同时进行,在测量时间上比分别利用BOTDR技术和POTDR技术对应变和振动的测量时间缩短很多,且可实现应变和振动的不间断测量。Beneficial effects of the present invention: the present invention combines BOTDR technology and POTDR technology, which can measure both strain events and vibration events, which greatly improves the measurement function and application range of fully distributed optical fiber sensors, and can greatly reduce system omissions Rate. The invention only uses the Brillouin scattered light signal to sense the strain and the vibration, the system device is simple, the overall cost and the number of devices are much smaller than the separate superposition of the two systems. While using POTDR technology for vibration measurement, by switching the working state of the polarization state switching device, the measurement of strain using BOTDR technology can be realized, so the measurement of vibration and strain can be carried out at the same time, and the measurement time is shorter than that of using BOTDR technology and respectively. POTDR technology greatly shortens the measurement time of strain and vibration, and can realize uninterrupted measurement of strain and vibration.

附图说明Description of drawings

图1为本发明提供的一种基于偏振态倒换的全分布式光纤应变与振动传感装置结构图。FIG. 1 is a structural diagram of a fully distributed optical fiber strain and vibration sensing device based on polarization switching provided by the present invention.

具体实施方式Detailed ways

如图1所示,一种基于正交偏振态倒换的全分布式光纤应变与振动传感装置的结构,包括激光器(1),保偏耦合器(2),保偏光纤(2-1),脉冲调制模块(3),光放大器(4),环形器(5),传感光纤(6),偏振态倒换装置(7),耦合器(8),平衡光电探测器(9),微波源(10),混频器(11),带通滤波器(12),信号采集与处理单元(13)。激光器(1)的输出的连续光经保偏耦合器(2)后分为两路:其中保偏耦合器输出的第一路中所有的连接光纤均为保偏光纤,其中的光波作为参考光,经偏振态倒换装置(7)后,再输入到耦合器(8)的第一输入端;偏振态倒换装置(7)具有两种状态,分别使输出的线偏振光的偏振方向对应于保偏光纤的快轴和慢轴;保偏耦合器输出的第二路经脉冲调制模块(3)、光放大器(4)后作为探测脉冲光经环形器(5)注入传感光纤(6);传感光纤中的布里渊散射光经环形器(5)返回后进入耦合器(8)的第二输入端;布里渊散射光与参考光在耦合器(8)中形成的混合信号经耦合器(8)的两个输出端输入到平衡光电探测器(9)中被转换为电信号。As shown in Figure 1, the structure of a fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization switching, including a laser (1), a polarization maintaining coupler (2), and a polarization maintaining fiber (2-1) , pulse modulation module (3), optical amplifier (4), circulator (5), sensing fiber (6), polarization switching device (7), coupler (8), balanced photodetector (9), microwave source (10), mixer (11), band-pass filter (12), signal acquisition and processing unit (13). The continuous light output by the laser (1) is divided into two paths after passing through the polarization maintaining coupler (2): all the connecting fibers in the first path output by the polarization maintaining coupler are polarization maintaining fibers, and the light waves in it are used as reference light , after passing through the polarization state switching device (7), it is input to the first input end of the coupler (8); the polarization state switching device (7) has two states, respectively making the polarization direction of the output linearly polarized light correspond to The fast axis and the slow axis of the polarizing fiber; the second path output by the polarization maintaining coupler passes through the pulse modulation module (3) and the optical amplifier (4), and then injects the detection pulse light into the sensing fiber (6) through the circulator (5); The Brillouin scattered light in the sensing fiber returns through the circulator (5) and then enters the second input end of the coupler (8); the mixed signal formed by the Brillouin scattered light and the reference light in the coupler (8) passes through The two output terminals of the coupler (8) are input into the balanced photodetector (9) and converted into electrical signals.

平衡光电探测器(9)的输出端与混频器(11)的第一输入端相连,微波源(10)与混频器(11)的第二输入端相连,混频器(11)的输出端连接到带通滤波器(12),带通滤波器(12)的输出端连接到信号采集与处理单元(13)。The output end of the balanced photodetector (9) is connected to the first input end of the mixer (11), the microwave source (10) is connected to the second input end of the mixer (11), and the mixer (11) The output end is connected to the band-pass filter (12), and the output end of the band-pass filter (12) is connected to the signal acquisition and processing unit (13).

参考光路的连接光纤均为保偏光纤,探测光路的光纤可以为单模光纤,也可为保偏光纤,保偏光纤的效果更好。The connecting optical fiber of the reference optical path is a polarization maintaining optical fiber, and the optical fiber of the detection optical path can be a single-mode optical fiber or a polarization maintaining optical fiber, and the effect of the polarization maintaining optical fiber is better.

偏振态倒换装置(7)可以是偏振开关、偏振控制器或偏振分析仪等任何可使线偏振光的偏振态在相互正交的两个偏振方向切换的器件或仪器,线偏振光在这两个正交方向的偏振分别对应于偏振态倒换装置(7)的第一和第二两种工作状态。The polarization state switching device (7) can be any device or instrument that can switch the polarization state of linearly polarized light in two orthogonal polarization directions, such as a polarization switch, a polarization controller, or a polarization analyzer. The polarizations in the two orthogonal directions respectively correspond to the first and second working states of the polarization state switching device (7).

脉冲调制模块(3)位于探测光路,偏振态倒换装置(7)位于参考光路。脉冲调制模块用于将光波调制成脉冲光。脉冲光的宽度由测量时所需的空间分辨率决定,一般为10ns~10μs之间。The pulse modulation module (3) is located in the detection optical path, and the polarization state switching device (7) is located in the reference optical path. The pulse modulation module is used to modulate light waves into pulsed light. The width of the pulsed light is determined by the spatial resolution required for measurement, generally between 10 ns and 10 μs.

传感装置在测量振动和应变时利用的散射光均为布里渊散射光。The scattered light used by the sensing device when measuring vibration and strain is Brillouin scattered light.

作为一个具体对应变和振动进行测量的例子,其具体实施步骤如下:As an example of measuring strain and vibration, the specific implementation steps are as follows:

激光器(1)发出的连续光为线偏振光,其中心波长为1550nm,线宽为2MHz,功率为10dBm。此光波经保偏耦合器(2)后分为两路,其中第一路作为参考光,经过偏振态倒换装置(7)(这里使用的是美国安捷伦公司的光器件分析仪N7788B)后,进入耦合比为50:50的耦合器(8)的第一输入端。第二路光经脉冲调制模块(3)(电光调制器)调制成脉宽为20ns的脉冲光,再经光放大器(4)(掺铒光纤放大器)放大后,作为探测脉冲光经环形器(5)进入传感光纤(6)。传感光纤(6)为普通的单模光纤,其折射率n=1.46,光纤中的声速va=5945m/s。脉冲光在传感光纤中传输时会不断在光纤沿线产生布里渊散射光,其中心频率相对于探测光的中心频率有一定的偏移,此偏移被称为布里渊频移vB,其大小vB=2nva/λ=11.2GHz。当传感光纤某个位置受到应变影响时,会使该位置处产生的布里渊散射光的布里渊频移的大小发生改变,受到振动影响时,会使该位置处探测脉冲光的偏振态发生变化,进而导致其在光纤中产生的布里渊散射光的偏振态发生变化。因此通过测量布里渊散射光的中心频率,可对光纤的应变进行传感,通过测量布里渊散射光的偏振态变化,可对光纤的振动进行传感。The continuous light emitted by the laser (1) is linearly polarized light with a central wavelength of 1550nm, a line width of 2MHz, and a power of 10dBm. The light wave is divided into two paths after passing through the polarization maintaining coupler (2), and the first path is used as a reference light. The first input of a coupler (8) with a coupling ratio of 50:50. The second light is modulated by the pulse modulation module (3) (electro-optic modulator) into pulsed light with a pulse width of 20 ns, and then amplified by the optical amplifier (4) (erbium-doped fiber amplifier), and then passed through the circulator ( 5) Enter the sensing fiber (6). The sensing fiber (6) is an ordinary single-mode fiber, its refractive index n=1.46, and the sound velocity v a in the fiber is 5945m/s. When the pulsed light is transmitted in the sensing fiber, it will continuously generate Brillouin scattered light along the fiber, and its center frequency has a certain offset from the center frequency of the detection light. This offset is called the Brillouin frequency shift v B , and its size v B =2nv a /λ=11.2GHz. When a certain position of the sensing fiber is affected by strain, the magnitude of the Brillouin frequency shift of the Brillouin scattered light generated at this position will change, and when it is affected by vibration, the polarization of the detected pulse light at this position will be changed. The state changes, which in turn causes the polarization state of the Brillouin scattered light generated in the fiber to change. Therefore, by measuring the center frequency of the Brillouin scattered light, the strain of the optical fiber can be sensed, and by measuring the polarization state change of the Brillouin scattered light, the vibration of the optical fiber can be sensed.

直到布里渊散射光沿光纤返回后,与第一路中的参考光一起进入耦合器(8)。它们的混合信号经响应频率能够覆盖到11.2GHz左右的平衡光电探测器(9)接收后转换为电信号。此电信号的频率即为布里渊散射光与参考光的频率差,其中心频率即为vB。将微波源(10)的频率设置为vB(vM与vB较为接近),则该高频信号经混频器(11)后,其中心频率会被转换到|vB-vM|。通过扫描微波源(10)的频率来调整混频器(11)的输出信号的频率,当通过带通滤波器(12)的信号功率达到最大时,即可得到布里渊散射光的布里渊频移,其大小为vB=vM-fBPF,其中fBPF为带通滤波器(12)的中心频率。After the Brillouin scattered light returns along the optical fiber, it enters the coupler (8) together with the reference light in the first path. Their mixed signals are converted into electrical signals after being received by a balanced photodetector (9) whose response frequency can cover about 11.2 GHz. The frequency of this electrical signal is the frequency difference between the Brillouin scattered light and the reference light, and its center frequency is v B . Set the frequency of the microwave source (10) to v B (v M is closer to v B ), then the high-frequency signal will be converted to |v B -v M | . By scanning the frequency of the microwave source (10) to adjust the frequency of the output signal of the mixer (11), when the signal power passing through the band-pass filter (12) reaches the maximum, the Brillouin scattered light can be obtained Deep frequency shift, its magnitude is v B =v M -f BPF , where f BPF is the center frequency of the band-pass filter (12).

探测脉冲光在传感光纤(6)中传输时会不断产生后向的布里渊散射光,为避免不同的探测脉冲光在传感光纤(6)中产生的布里渊散射光相互干扰,在对信号进行采集时只能允许在传感光纤(6)中同时存在一个探测脉冲光。因此将脉冲调制模块(3)与信号采集与处理单元(13)同步。在接收布里渊散射光时从探测脉冲光刚入射到传感光纤(6)中时开始计时,直到接收到探测脉冲光在传感光纤(6)末端产生的布里渊散射光后才能使脉冲调制模块(3)产生下一个探测脉冲光。在传感光纤(6)中产生布里渊散射光的位置l可通过光纤中的光速与时间差得到,即l=cΔt/2n,其中c≈3×108m/s为真空中的光速,Δt为从计时开始到接收到所需定位的布里渊散射光所经过的时间。对于长度为L传感光纤(6),两个探测脉冲光的时间间隔ΔT应大于2nL/c,即脉冲光在光纤中往返一次需要的时间,若传感光纤(6)长度为10km,则2nL/c ≈100μs。When the detection pulse light is transmitted in the sensing fiber (6), it will continuously generate backward Brillouin scattered light. In order to avoid the mutual interference of the Brillouin scattered light generated by different detection pulse lights in the sensing fiber (6), When collecting signals, only one detection pulse light is allowed to exist in the sensing optical fiber (6) at the same time. The pulse modulation module (3) is thus synchronized with the signal acquisition and processing unit (13). When receiving the Brillouin scattered light, start timing from the moment when the detection pulse light is incident on the sensing fiber (6) until the Brillouin scattered light generated by the detection pulse light at the end of the sensing fiber (6) is received. The pulse modulation module (3) generates the next detection pulse light. The position l where Brillouin scattered light is generated in the sensing fiber (6) can be obtained from the speed of light in the fiber and the time difference, that is, l=cΔt/2n, where c≈3×10 8 m/s is the speed of light in vacuum, Δt is the elapsed time from the start of timing to receiving the Brillouin scattered light at the desired location. For the sensing fiber (6) with a length of L, the time interval ΔT between two detection pulsed lights should be greater than 2nL/c, which is the time required for the pulsed light to go back and forth in the fiber once. If the length of the sensing fiber (6) is 10km, then 2nL/c ≈100μs.

在每次微波源改变到新的频率时,偏振态倒换装置(7)首先工作在第一种工作状态,使参考光的偏振方向沿第一路中保偏光纤的慢轴。由于从光纤不同位置产生的布里渊散射光的偏振态各不相同,所以从光纤不同位置产生的布里渊散射光与参考光混合经平衡光电探测器(9)相干外差检测后得到的信号会产生相应的波动起伏,这会影响对布里渊频移测量的准确性,但这同时包含了光纤沿线光波偏振态的信息。由于布里渊散射光的能量非常小,为获得较高的信噪比,在每次微波源改变到新的频率时,均需要对获得的信号进行N次累加平均。当偏振态倒换装置(7)处于第一种工作状态时,对信号反复测量N/2次,因此需要的时间为NΔT/2。如果传感光纤(6)长度为10km、两个脉冲光之间的时间间隔ΔT=120μs、平均次数N=16384次,则偏振态倒换装置(7)在这一工作状态下需要的时间NΔT/2≈1s。然后通过对比这N/2次测量得到的信号在光纤不同位置处的变化或利用时频变换的方法分析这些信号在光纤不同位置处的频谱可得到光纤沿线光波偏振态的变化情况,进而实现对光纤沿线振动的传感。然后使偏振态倒换装置(7)工作在第二种工作状态,使参考光的偏振方向沿第一路中保偏光纤的快轴。此时得到的信号同样包含有光纤沿线光波偏振态的信息。在这一状态下对信号反复测量N/2次,通过分析同样可得到光纤沿线光波偏振态的变化情况,进而可保证对光纤沿线的振动情况进行不间断的传感测量。将偏振态倒换装置(7)在两种工作状态下分别测量了N/2次的信号进行累加平均,可消除由于布里渊散射光的偏振态在光纤沿线变化造成的相干外差信号的波动起伏,也同时相当于对布里渊信号进行了N次平均,从而提高了对布里渊信号功率测量的准确性。然后再次改变微波源的频率,再重复上述测量步骤,可最终得到布里渊频移,进而实现对光纤中应变的测量。Every time the microwave source changes to a new frequency, the polarization state switching device (7) first works in the first working state, so that the polarization direction of the reference light is along the slow axis of the polarization-maintaining fiber in the first path. Since the polarization states of the Brillouin scattered light generated from different positions of the optical fiber are different, the Brillouin scattered light generated from different positions of the optical fiber is mixed with the reference light and obtained after coherent heterodyne detection by the balanced photodetector (9) The signal will produce corresponding fluctuations, which will affect the accuracy of the Brillouin frequency shift measurement, but it also contains information about the polarization state of the light wave along the fiber. Since the energy of Brillouin scattered light is very small, in order to obtain a higher signal-to-noise ratio, each time the microwave source changes to a new frequency, it is necessary to accumulate and average the obtained signal N times. When the polarization state switching device (7) is in the first working state, the signal is repeatedly measured N/2 times, so the required time is NΔT/2. If the length of the sensing fiber (6) is 10km, the time interval between two pulsed lights ΔT=120μs, and the average number of times N=16384 times, the time NΔT/ 2≈1s. Then, by comparing the changes of the signals obtained by these N/2 measurements at different positions of the optical fiber or analyzing the frequency spectrum of these signals at different positions of the optical fiber by using the method of time-frequency transformation, the change of the polarization state of the light wave along the optical fiber can be obtained, and then it can be realized. Sensing of vibrations along optical fibers. Then make the polarization state switching device (7) work in the second working state, so that the polarization direction of the reference light is along the fast axis of the polarization-maintaining fiber in the first path. The signal obtained at this time also contains information about the polarization state of the light wave along the fiber. In this state, the signal is repeatedly measured N/2 times, and the change of the polarization state of the light wave along the fiber can also be obtained through analysis, thereby ensuring uninterrupted sensing and measurement of the vibration along the fiber. Accumulate and average the signals measured N/2 times by the polarization state switching device (7) in two working states, which can eliminate the fluctuation of the coherent heterodyne signal caused by the polarization state of the Brillouin scattered light along the optical fiber. The ups and downs are also equivalent to averaging the Brillouin signal N times, thereby improving the accuracy of the power measurement of the Brillouin signal. Then change the frequency of the microwave source again, and repeat the above-mentioned measurement steps to finally obtain the Brillouin frequency shift, and then realize the measurement of the strain in the optical fiber.

Claims (5)

1. 一种基于正交偏振态倒换的全分布式光纤应变与振动传感装置,其特征是包括激光器(1),保偏耦合器(2)、保偏光纤(2-1)、脉冲调制模块(3)、光放大器(4)、环形器(5)、传感光纤(6)、偏振态倒换装置(7)、耦合器(8)、平衡光电探测器(9)、微波源(10)、混频器(11)、带通滤波器(12)、信号采集与处理单元(13);激光器(1)的输出的连续光经保偏耦合器(2)后分为两路:其中保偏耦合器(2)输出的第一路中所有的连接光纤均为保偏光纤,其中的光波作为参考光,经偏振态倒换装置(7)后,再输入到耦合器(8)的第一输入端;偏振态倒换装置(7)具有两种状态,分别使输出的线偏振光的偏振方向对应于保偏光纤的快轴和慢轴; 1. A fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization switching, which is characterized by including a laser (1), a polarization maintaining coupler (2), a polarization maintaining fiber (2-1), a pulse modulation Module (3), optical amplifier (4), circulator (5), sensing fiber (6), polarization switching device (7), coupler (8), balanced photodetector (9), microwave source (10 ), a mixer (11), a bandpass filter (12), a signal acquisition and processing unit (13); the output continuous light of the laser (1) is divided into two paths after passing through the polarization maintaining coupler (2): All the connecting fibers in the first path output by the polarization-maintaining coupler (2) are polarization-maintaining fibers, and the light wave in it is used as a reference light. An input end; the polarization state switching device (7) has two states, respectively making the polarization direction of the output linearly polarized light correspond to the fast axis and the slow axis of the polarization-maintaining fiber; 保偏耦合器(2)输出的第二路经脉冲调制模块(3)、光放大器(4)后作为探测脉冲光经环形器(5)注入传感光纤(6);传感光纤(6)中的布里渊散射光经环形器(5)返回后进入耦合器(8)的第二输入端;布里渊散射光与参考光在耦合器(8)中形成的混合信号经耦合器(8)的两个输出端输入到平衡光电探测器(9)中被转换为电信号; The second path output by the polarization-maintaining coupler (2) passes through the pulse modulation module (3) and the optical amplifier (4), and then injects the detection pulse light into the sensing fiber (6) through the circulator (5); the sensing fiber (6) The Brillouin scattered light in the circulator (5) returns to the second input end of the coupler (8); the mixed signal formed by the Brillouin scattered light and the reference light in the coupler (8) passes through the coupler ( The two output terminals of 8) are input into the balanced photodetector (9) and converted into electrical signals; 平衡光电探测器(9)的输出端与混频器(11)的第一输入端相连,微波源(10)与混频器(11)的第二输入端相连,混频器(11)的输出端连接到带通滤波器(12),带通滤波器(12)的输出端连接到信号采集与处理单元(13);使线偏振光的偏振态在相互正交的两个偏振方向切换的偏振态倒换装置(7)是偏振开关、偏振控制器或偏振分析仪,线偏振光在相互正交的两个正交方向的偏振分别对应于偏振态倒换装置(7)的第一和第二两种工作状态;脉冲调制模块位于探测光路,偏振态倒换装置位于参考光路。 The output end of the balanced photodetector (9) is connected to the first input end of the mixer (11), the microwave source (10) is connected to the second input end of the mixer (11), and the mixer (11) The output end is connected to the band-pass filter (12), and the output end of the band-pass filter (12) is connected to the signal acquisition and processing unit (13); the polarization state of the linearly polarized light is switched in two orthogonal polarization directions The polarization state switching device (7) is a polarization switch, a polarization controller or a polarization analyzer, and the polarizations of linearly polarized light in two orthogonal directions that are mutually orthogonal correspond to the first and second polarization state switching devices (7) respectively. Two working states; the pulse modulation module is located in the detection optical path, and the polarization state switching device is located in the reference optical path. 2.  根据权利要求1所述的基于正交偏振态倒换的全分布式光纤应变与振动传感装置,其特征在于当偏振态倒换装置(7)处于任一种工作状态时,传感光纤(6)所得到的信号为传感光纤(6)中的散射光信号与偏振方向沿保偏光纤快轴或慢轴的线偏振光经耦合器(8)和平衡光电探测器(9)相干外差检测之后的结果;当传感光纤(6)某个位置受到应变影响时,该位置处产生的布里渊散射光的布里渊频移的大小发生改变;受到振动影响时,该位置处探测脉冲光的偏振态发生变化,进而使在传感光纤(6)中的布里渊散射光的偏振态发生变化;因此通过测量布里渊散射光的中心频率,对传感光纤(6)的应变进行传感,通过测量布里渊散射光的偏振态变化,对传感光纤(6)的振动进行传感; 2. The fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization state switching according to claim 1, characterized in that when the polarization state switching device (7) is in any working state, the sensing fiber ( 6) The obtained signal is the scattered light signal in the sensing fiber (6) and the linearly polarized light whose polarization direction is along the fast axis or slow axis of the polarization-maintaining fiber, through the coupler (8) and the balanced photodetector (9). The result after differential detection; when a certain position of the sensing fiber (6) is affected by strain, the magnitude of the Brillouin frequency shift of the Brillouin scattered light generated at this position changes; when affected by vibration, the The polarization state of the detection pulse light changes, and then the polarization state of the Brillouin scattered light in the sensing fiber (6) changes; therefore, by measuring the center frequency of the Brillouin scattered light, the sensing fiber (6) The strain is sensed, and the vibration of the sensing fiber (6) is sensed by measuring the polarization state change of the Brillouin scattered light; 传感光纤(6)得到的信号包含有布里渊散射光偏振态变化的信息,利用偏振光时域反射方法进行测量,利用散射光偏振态的变化信息对振动进行传感。 The signal obtained by the sensing fiber (6) contains the information on the change of the polarization state of the Brillouin scattered light, which is measured by the polarized light time domain reflection method, and the vibration is sensed by using the information on the change of the polarization state of the scattered light. 3.根据权利要求2所述的基于正交偏振态倒换的全分布式光纤应变与振动传感装置,其特征是当偏振态倒换装置(7)在第一和第二两种工作状态下分别工作等长时间,将在此两种工作状态下得到的外差信号功率累加,则能消除传感光纤中光波偏振态变化的影响;此时可利用布里渊光时域反射方法进行测量,利用布里渊散射光的频率信息对光纤中的应变进行传感。 3. The fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization switching according to claim 2, characterized in that when the polarization switching device (7) is in the first and second working states respectively Working for a long time, adding the heterodyne signal power obtained under these two working conditions can eliminate the influence of the change of the polarization state of the light wave in the sensing fiber; at this time, the Brillouin optical time domain reflection method can be used for measurement. The strain in the optical fiber is sensed by using the frequency information of Brillouin scattered light. 4.根据权利要求3所述的基于正交偏振态倒换的全分布式光纤应变与振动传感装置,其特征是当偏振态倒换装置(7)处于任一种工作状态时,由于脉冲光在光纤中不同位置的偏振态各不相同,由平衡光电探测器(9)相干外差检测之后得到的脉冲光在光纤沿线产生的布里渊信号有相应的波动起伏;在不同的时间多次测量光纤中的布里渊信号后,通过比较它们之间波动起伏的不同或利用时频变换的方法分析光纤各位置处波动起伏变化的频谱,可得到光纤中脉冲光在某位置处的偏振态的变化情况。 4. The fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization state switching according to claim 3, characterized in that when the polarization state switching device (7) is in any working state, due to the pulsed light in The polarization states at different positions in the optical fiber are different, and the Brillouin signal generated by the pulsed light obtained after coherent heterodyne detection by the balanced photodetector (9) along the optical fiber has corresponding fluctuations; multiple measurements at different times After the Brillouin signal in the optical fiber, the polarization state of the pulsed light in the optical fiber at a certain position can be obtained by comparing the fluctuations between them or analyzing the frequency spectrum of the fluctuations at various positions in the optical fiber by using the time-frequency transformation method. Changes. 5.根据权利要求3所述的基于正交偏振态倒换的全分布式光纤应变与振动传感装置,其特征是脉冲光在传感光纤中传输时会不断在光纤沿线产生布里渊散射光,其中心频率相对于探测光的中心频率有一定的偏移,此偏移被称为布里渊频移ν B ;将微波源(10)的频率设置为ν M ν M ν B 接近,则该高频信号经混频器(11)后,其中心频率会被转换到∣ν B M ∣;通过扫描微波源(10)的频率来调整混频器(11)的输出信号的频率,当通过带通滤波器(12)的信号功率达到最大时,即可得到布里渊散射光的布里渊频移, 其大小为ν B =ν M -f BPF ,其中f BPF 为带通滤波器(12)的中心频率。 5. The fully distributed optical fiber strain and vibration sensing device based on orthogonal polarization switching according to claim 3, characterized in that when the pulsed light is transmitted in the sensing optical fiber, Brillouin scattered light will be continuously generated along the optical fiber , its center frequency has a certain offset relative to the center frequency of the probe light, this offset is called the Brillouin frequency shift ν B ; the frequency of the microwave source (10) is set to ν M , and ν M is close to ν B , the center frequency of the high-frequency signal will be converted to ∣ ν B M ∣ after passing through the mixer (11); the output signal of the mixer (11) is adjusted by scanning the frequency of the microwave source (10) When the signal power of the bandpass filter (12) reaches the maximum, the Brillouin frequency shift of the Brillouin scattered light can be obtained, and its magnitude is ν B = ν M -f BPF , where f BPF is Center frequency of the bandpass filter (12).
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