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CN111896095A - A Vibration Localization Method for Distributed Optical Fiber Double M-Z Interferometer Based on HHT Transform - Google Patents

A Vibration Localization Method for Distributed Optical Fiber Double M-Z Interferometer Based on HHT Transform Download PDF

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CN111896095A
CN111896095A CN202010516348.1A CN202010516348A CN111896095A CN 111896095 A CN111896095 A CN 111896095A CN 202010516348 A CN202010516348 A CN 202010516348A CN 111896095 A CN111896095 A CN 111896095A
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vibration
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optical fiber
imfs
hilbert
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秦增光
李钊
刘兆军
徐演平
丛振华
渠帅
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Shandong University
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    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H9/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
    • G01H9/004Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means using fibre optic sensors

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Abstract

本发明公开了一种基于HHT变换的分布式光纤双M‑Z干涉仪的振动定位方法,具体步骤为,S1.取一段振动光纤信号S(t)按分段三次Hermite差值多项式做经验模态分解EMD,得到本征模态函数IMFs;S2.对分解得到的IMFs做Hilbert变换得到原始信号S(t)的瞬时频率;S3.将所有本征模态函数IMFs做HT后的结果叠加,得到Hilbert谱;S4.根据Hilbert谱峰值位置提取包含振动信息的信号段Sp(t);S5.将提取出的信号段Sp(t)做互相关运算及定位运算得出振动位置信息。其优点在于,提取有振动的区域信号做互相关计算得到时间延迟,有利于提高定位精度,减少计算时间。

Figure 202010516348

The invention discloses a vibration positioning method of a distributed optical fiber double M-Z interferometer based on HHT transformation. The specific steps are as follows: S1. Take a section of vibrating optical fiber signal S(t) and use a piecewise cubic Hermite difference polynomial as an empirical model Decompose EMD to obtain the eigenmode function IMFs; S2. Perform Hilbert transform on the decomposed IMFs to obtain the instantaneous frequency of the original signal S(t); S3. Superimpose the results of all eigenmode functions IMFs after HT, Obtain the Hilbert spectrum; S4. Extract the signal segment Sp (t) containing the vibration information according to the peak position of the Hilbert spectrum; S5. Perform the cross-correlation operation and the positioning operation on the extracted signal segment Sp (t) to obtain the vibration location information. The advantage is that the time delay can be obtained by extracting the signals in the area with vibration and performing the cross-correlation calculation, which is beneficial to improve the positioning accuracy and reduce the calculation time.

Figure 202010516348

Description

一种基于HHT变换的分布式光纤双M-Z干涉仪的振动定位方法A Vibration Localization Method for Distributed Optical Fiber Double M-Z Interferometer Based on HHT Transform

技术领域technical field

本发明涉及一种双M-Z分布式光纤传感振动定位的方法,属于分布式光纤传感技术领域。The invention relates to a vibration positioning method for double M-Z distributed optical fiber sensing, belonging to the technical field of distributed optical fiber sensing.

背景技术Background technique

分布式光纤传感系统是一种利用光纤作为传感敏感元件和传输信号介质的传感系统,可以对光纤链路上发生的振动行为实时监测并且准确定位。Distributed optical fiber sensing system is a sensing system that uses optical fiber as a sensing sensitive element and a signal transmission medium, which can monitor and accurately locate the vibration behavior occurring on the optical fiber link in real time.

分布式光纤传感系统具有一系列优点,如无源安全、长距离、高分辨率、低成本,在建筑结构健康监测、油气管道安全预警、周界安防监控以及智能物联网应用等领域具有广泛的前景。Distributed optical fiber sensing systems have a series of advantages, such as passive safety, long distance, high resolution, and low cost, and are widely used in building structure health monitoring, oil and gas pipeline safety early warning, perimeter security monitoring, and intelligent IoT applications. Prospects.

基于双M-Z的分布式光纤传感系统是利用光的干涉原理,由于噪声等影响会使得振动定位精度下降,从信号中难以确定振动起始点也会对精度和处理时间带来不利的影响,因此需要寻找一种能精准定位的方法。The distributed optical fiber sensing system based on double M-Z uses the interference principle of light. Due to the influence of noise, the vibration positioning accuracy will be reduced, and it is difficult to determine the vibration starting point from the signal. Need to find a way to accurately locate.

发明内容SUMMARY OF THE INVENTION

针对以上提出的问题,本发明提供一种改善双M-Z分布式光纤传感系统振动定位的方法,该方法能提高定位精度且降低数据处理时间。其技术方案为,In view of the above-mentioned problems, the present invention provides a method for improving the vibration positioning of a dual M-Z distributed optical fiber sensing system, which can improve the positioning accuracy and reduce the data processing time. Its technical solution is,

一种基于HHT变换的分布式光纤双M-Z干涉仪的振动定位方法,具体步骤为,A vibration positioning method of a distributed optical fiber double M-Z interferometer based on HHT transformation, the specific steps are:

S1.取一段振动光纤信号S(t)按分段三次Hermite差值多项式做经验模态分解EMD,得到本征模态函数IMFs;S1. Take a section of vibrating optical fiber signal S(t) and perform empirical mode decomposition EMD according to the piecewise cubic Hermite difference polynomial to obtain the eigenmode function IMFs;

S2.对分解得到的IMFs做Hilbert变换得到原始信号S(t)的瞬时频率;S2. Hilbert transform the decomposed IMFs to obtain the instantaneous frequency of the original signal S(t);

S3.将所有本征模态函数IMFs做HT后的结果叠加,得到Hilbert谱;S3. Superimpose the results of all eigenmode functions IMFs after HT to obtain the Hilbert spectrum;

S4.根据Hilbert谱峰值位置提取包含振动信息的信号段Sp(t);S4. Extract the signal segment Sp (t) containing vibration information according to the peak position of the Hilbert spectrum;

S5.将提取出的信号段Sp(t)做互相关运算及定位运算得出振动位置信息。S5. Perform cross-correlation operation and positioning operation on the extracted signal segment Sp (t) to obtain vibration position information.

进一步的,经验模态分解EMD过程为,将一个原始信号S(t)的极大值点用三次Hermite差值方式拟合出上包络线,用同样的方式得出下包络线;上包络线、下包络线取均值,得到平均包络线ml;用原始信号S(t)减去平均包络线ml,得到一个新的信号f(t),即Further, the EMD process of empirical mode decomposition is to fit the maximum point of an original signal S(t) with the cubic Hermite difference method to fit the upper envelope, and obtain the lower envelope in the same way; Take the average of the envelope and the lower envelope to get the average envelope ml; subtract the average envelope ml from the original signal S(t) to get a new signal f(t), that is

S(t)-ml=f(t)S(t)-ml=f(t)

若新信号f(t)还存在负的局部极大值和正的局部极小值,则继续按上操作分解,由此得出多个本征模函数IMFs和余波。If the new signal f(t) still has negative local maxima and positive local minima, continue to decompose according to the above operation, thereby obtaining multiple eigenmode functions IMFs and aftermath.

进一步的,希尔伯特谱分析HSA将经验模态分解EMD分解出的多个本征模态函数IMFs分别各自做Hilbert变换,由此得到瞬时频率,并将所有本征模态函数IMFs做Hilbert变换后的结果组合得到Hilbert谱,获得原始信号S(t)的频率变化情况。Further, Hilbert spectrum analysis HSA performs Hilbert transform for multiple eigenmode functions IMFs decomposed by EMD, respectively, to obtain the instantaneous frequency, and converts all eigenmode functions IMFs to Hilbert The transformed results are combined to obtain the Hilbert spectrum, and the frequency variation of the original signal S(t) is obtained.

进一步的,根据Hilbert谱峰值位置提取包含振动信息的信号段Sp(t),其中沿顺时针方向的信号段为

Figure BDA0002530251000000021
沿逆时针方向的信号段为
Figure BDA0002530251000000022
取高峰值处附近0.01s的数据做互相关运算,得出延时时间,进而得出振动位置信息。Further, the signal segment Sp (t) containing vibration information is extracted according to the peak position of the Hilbert spectrum, wherein the signal segment along the clockwise direction is
Figure BDA0002530251000000021
The signal segment in the counterclockwise direction is
Figure BDA0002530251000000022
Take the data of 0.01s near the high peak for cross-correlation operation, obtain the delay time, and then obtain the vibration position information.

进一步的,沿顺时针方向的信号段为

Figure BDA0002530251000000023
和沿逆时针方向的信号段为
Figure BDA0002530251000000024
到达两个平衡探测器的时间存在一定延迟τ,Further, the signal segment in the clockwise direction is
Figure BDA0002530251000000023
and the signal segment in the counterclockwise direction is
Figure BDA0002530251000000024
There is a certain delay τ in the time to reach the two balanced detectors,

τ=tL-x+tL-txτ=t Lx +t L -t x ,

振动位置计算公式:Vibration position calculation formula:

Figure BDA0002530251000000025
Figure BDA0002530251000000025

L为传感光纤和传导光纤的长度,τ为顺逆两束光到达平衡探测器间的时间延迟,c为真空中的光速,n为光纤折射率,x为振动位置。L is the length of the sensing fiber and the conducting fiber, τ is the time delay between the forward and reverse beams reaching the equilibrium detector, c is the speed of light in vacuum, n is the refractive index of the fiber, and x is the vibration position.

有益效果beneficial effect

与传统的双M-Z定位方法不同,这里采用HHT确定包含振动的区域信号,可以清晰直观的提取有效信号,提取有振动的区域信号做互相关计算得到时间延迟,有利于提高定位精度,减少计算时间。Different from the traditional dual M-Z positioning method, the HHT is used here to determine the regional signal containing vibration, which can extract the effective signal clearly and intuitively, and extract the regional signal with vibration for cross-correlation calculation to obtain the time delay, which is beneficial to improve the positioning accuracy and reduce the calculation time. .

附图说明Description of drawings

图1为双M-Z分布式光纤传感系统示意图;Figure 1 is a schematic diagram of a dual M-Z distributed optical fiber sensing system;

图2为计算分布式光纤传感振动位置的方法流程图;Fig. 2 is the method flow chart of calculating the vibration position of distributed optical fiber sensing;

图3为一段原始信号图;Fig. 3 is a section of original signal diagram;

图4为原始信号的希尔伯特谱图。Figure 4 is a Hilbert spectrogram of the original signal.

其中1-光源;2-隔离器;3-耦合器一;4-耦合器二;5-耦合器三;6-耦合器四;7-传感光纤;8-传导光纤;9-第一平衡探测器;10-第二平衡探测器;11-采集处理系统。1-light source; 2-isolator; 3-coupler one; 4-coupler two; 5-coupler three; 6-coupler four; 7-sensing fiber; 8-conducting fiber; 9-first balance Detector; 10-Second Balance Detector; 11-Acquisition Processing System.

具体实施方式Detailed ways

下面结合附图1-4和具体实施例对技术作进一步说明,以助于理解本发明的内容。The technology will be further described below in conjunction with the accompanying drawings 1-4 and specific embodiments to help understand the content of the present invention.

一种基于HHT变换的分布式光纤双M-Z干涉仪的振动定位方法,具体步骤为,A vibration positioning method of a distributed optical fiber double M-Z interferometer based on HHT transformation, the specific steps are:

S1.取一段振动光纤信号S(t)按分段三次Hermite差值多项式做经验模态分解EMD,得到本征模态函数IMFs;S1. Take a section of vibrating optical fiber signal S(t) and perform empirical mode decomposition EMD according to the piecewise cubic Hermite difference polynomial to obtain the eigenmode function IMFs;

希尔伯特-黄变换HHT包括经验模态分解EMD和希尔伯特谱分析HAS,Hilbert-Huang transform HHT includes empirical mode decomposition EMD and Hilbert spectral analysis HAS,

EMD的基本思想是:把一个频率变化无规律的波转化成多个单一频率波+残余波的形式。The basic idea of EMD is to convert a wave with irregular frequency changes into multiple single frequency waves + residual waves.

其中经验模态分解EMD过程为,将一个原始信号S(t)的极大值点用三次Hermite差值方式拟合出上包络线,用同样的方式得出下包络线;上包络线、下包络线取均值,得到平均包络线ml;用原始信号S(t)减去平均包络线ml,得到一个新的信号f(t),即Among them, the EMD process of empirical mode decomposition is to fit the maximum point of an original signal S(t) with the cubic Hermite difference method to fit the upper envelope, and use the same method to obtain the lower envelope; Take the average of the line and the lower envelope to get the average envelope ml; subtract the average envelope ml from the original signal S(t) to get a new signal f(t), that is

S(t)-ml=f(t)S(t)-ml=f(t)

若新信号n(t)还存在负的局部极大值和正的局部极小值,则继续按上操作分解,由此得出多个本征模函数IMFs和余波。If the new signal n(t) still has negative local maxima and positive local minima, continue to decompose according to the above operation, thereby obtaining multiple eigenmode functions IMFs and aftermath.

S2.希尔伯特谱分析HSA将经验模态分解EMD分解出的多个本征模态函数IMFs分别各自做Hilbert变换,由此得到原始信号S(t)的瞬时频率;S2. Hilbert Spectrum Analysis HSA performs Hilbert transforms on multiple eigenmode functions IMFs decomposed by EMD, respectively, thereby obtaining the instantaneous frequency of the original signal S(t);

当有振动发生时,振动使传感光纤产生应力,在应力作用下信号的频率会变高,高频区域信号中包含了振动信号。When vibration occurs, the vibration will cause stress to the sensing fiber, and the frequency of the signal will become higher under the action of the stress, and the signal in the high frequency region contains the vibration signal.

S3.将所有本征模态函数IMFs做HT后的结果叠加,得到Hilbert谱,获得原始信号S(t)的频率变化情况。S3. Superimpose the results of all eigenmode functions IMFs after HT to obtain the Hilbert spectrum, and obtain the frequency change of the original signal S(t).

S4.根据Hilbert谱峰值位置提取包含振动信息的信号段Sp(t);将提取出的信号段Sp(t)做互相关运算及定位运算得出振动位置信息;S4. according to Hilbert spectrum peak position, extract the signal segment S p (t) that contains vibration information; The extracted signal segment Sp ( t ) is done cross-correlation operation and positioning operation to obtain vibration location information;

其中沿顺时针方向的信号段为

Figure BDA0002530251000000031
沿逆时针方向的信号段为
Figure BDA0002530251000000032
取高峰值处附近0.01s的数据做互相关运算,得出延时时间,进而得出振动位置信息。where the signal segment in the clockwise direction is
Figure BDA0002530251000000031
The signal segment in the counterclockwise direction is
Figure BDA0002530251000000032
Take the data of 0.01s near the high peak for cross-correlation operation, obtain the delay time, and then obtain the vibration position information.

取高峰值处附近0.01s的数据具体为解释为:取高峰值前后共0.01s的数据,比如高峰值在0.09s处,数据采集范围为0.085s-0.095s。Taking the data of 0.01s near the high peak value is specifically interpreted as: taking the data of 0.01s before and after the high peak value, for example, the high peak value is at 0.09s, and the data collection range is 0.085s-0.095s.

当有振动作用在M点时,沿顺时针方向的信号段为

Figure BDA0002530251000000041
和沿逆时针方向的信号段为
Figure BDA0002530251000000042
到达两个平衡探测器的时间存在一定延迟τ,When there is vibration acting on point M, the signal segment in the clockwise direction is
Figure BDA0002530251000000041
and the signal segment in the counterclockwise direction is
Figure BDA0002530251000000042
There is a certain delay τ in the time to reach the two balanced detectors,

τ=tL-x+tL-txτ=t Lx +t L -t x ,

振动位置计算公式:Vibration position calculation formula:

Figure BDA0002530251000000043
Figure BDA0002530251000000043

L为传感光纤和传导光纤的长度,τ为顺逆两束光到达平衡探测器间的时间延迟,c为真空中的光速,n为光纤折射率,x为振动位置,即M点到耦合器二的距离。L is the length of the sensing fiber and the conducting fiber, τ is the time delay between the forward and reverse light beams reaching the balanced detector, c is the speed of light in vacuum, n is the refractive index of the fiber, and x is the vibration position, that is, the point M to the coupling The distance of the second device.

系统参数如下:The system parameters are as follows:

如图1所示,光源1发出的光经隔离器2后到达耦合器一3被分为50:50的两束光,分别沿顺时针方向和逆时针方向传播,顺时针方向传播的光经耦合器二4分为两束后在传感光纤7的另一端耦合器三5处干涉,并经传导光纤8传输至耦合器四6到第二平衡探测器10处接收;逆时针方向传播的光经传导光纤8后在耦合器三5处按50:50分束,沿逆时针方向经过传感光纤7后在耦合器二4干涉,再由第一平衡探测器9接收。第一平衡探测器9和第二平衡探测器10把探测到的光信号转为电信号后进入采集处理系统11进行定位计算。As shown in Figure 1, the light emitted by the light source 1 passes through the isolator 2 and then reaches the coupler-3 and is divided into two beams of 50:50, which propagate in the clockwise and counterclockwise directions respectively. The light propagating in the clockwise direction passes through the The coupler 24 is divided into two bundles and interferes at the other end of the sensing fiber 7 at the coupler 35, and is transmitted to the coupler 46 through the conducting fiber 8 to receive at the second balanced detector 10; The light is split by 50:50 at the coupler 3 5 after passing through the conducting fiber 8 , passes through the sensing fiber 7 in the counterclockwise direction, interferes at the coupler 2 4 , and is then received by the first balanced detector 9 . The first balance detector 9 and the second balance detector 10 convert the detected optical signals into electrical signals and then enter the acquisition and processing system 11 for positioning calculation.

光源选用RIO窄线宽激光器,产生光波长为1550nm,线宽小于3kHz,功率10mW;The light source is a RIO narrow linewidth laser, the wavelength of light is 1550nm, the linewidth is less than 3kHz, and the power is 10mW;

传感光纤和传导光纤长度为2km;The length of sensing fiber and conducting fiber is 2km;

平衡探测器选用Thorlabs PDB450C-AC,选取档位为增益104V/A,带宽45MHz;The balanced detector uses Thorlabs PDB450C-AC, the selected gear is the gain of 10 4 V/A, and the bandwidth is 45 MHz;

耦合器一3、耦合器二4、耦合器三5、耦合器四6分光比均为50:50;The split ratio of coupler one 3, coupler two 4, coupler three 5, coupler four 6 is 50:50;

采集处理系统选用内置NI PCI-5114采集卡的计算机,电脑处理器采用

Figure BDA0002530251000000044
CoreTM i5-7200U CPU@2.50GHz 2.71GHz,内存8G;The acquisition and processing system uses a computer with a built-in NI PCI-5114 acquisition card, and the computer processor uses
Figure BDA0002530251000000044
Core TM i5-7200U CPU@2.50GHz 2.71GHz, memory 8G;

采样率选用10MHz/s,采样时间为0.1s,振动区域信号时间选取0.01s;The sampling rate is 10MHz/s, the sampling time is 0.1s, and the signal time in the vibration area is 0.01s;

传感光纤和传导光纤均采用双芯铠装光缆;Both the sensing fiber and the conducting fiber are double-core armored fiber optic cables;

振动位置在与耦合器二4相距1800m处,采用脚踩光缆的方式施加振动;The vibration position is 1800m away from the coupler 24, and the vibration is applied by stepping on the optical cable;

隔离器的作用是只允许光单向通过,防止后向散射光对光源造成损坏;The function of the isolator is to only allow light to pass in one direction, preventing backscattered light from causing damage to the light source;

对采集的信号做EMD分解,得到10层IMFs和余波,再对每层IMF分别做Hilbert变换,叠加后得到Hilbert谱,清晰直观的反映原始信号的频率变化情况;从图中可以看出,880000采样点处频率最高,选取830000~930000采样点处的区域信号作为振动的有效信号,对此做互相关运算计算得出两路信号的时间延迟,通过计算得出定位为1810m,误差为10m。The collected signal is decomposed by EMD to obtain 10 layers of IMFs and aftermath, and then Hilbert transform is performed on each layer of IMF. After superposition, the Hilbert spectrum is obtained, which clearly and intuitively reflects the frequency change of the original signal; The frequency at the sampling point is the highest, and the regional signal at the sampling point 830,000 to 930,000 is selected as the effective signal of vibration, and the cross-correlation operation is performed to calculate the time delay of the two signals.

为了说明该方法的有效性,分别取不同频率的区域信号做定位运算,比较其定位误差的大小,如下表所示。In order to illustrate the effectiveness of this method, the regional signals of different frequencies are respectively used for positioning operation, and the size of the positioning error is compared, as shown in the following table.

区域信号regional signal 0.05s~0.06s0.05s~0.06s 0.06s~0.07s0.06s~0.07s 0.07s~0.08s0.07s~0.08s 0.08s~0.09s0.08s~0.09s 0.09s~0.10s0.09s~0.10s 定位误差positioning error -80m-80m 40m40m 20m20m 10m10m -20m-20m

从表中可以看出,取高频段的信号定位误差比低频段信号定位误差小。It can be seen from the table that the positioning error of the high-frequency signal is smaller than that of the low-frequency signal.

从图4中可以看出高峰值在0.09s处,数据采集范围为0.08s-0.09s。It can be seen from Figure 4 that the high peak is at 0.09s, and the data acquisition range is 0.08s-0.09s.

当然,上述说明并非对本技术的限制,本技术也不仅限于上述举例,本技术Of course, the above description does not limit the present technology, and the present technology is not limited to the above examples.

领域的普通技术人员在本发明的实质范围内所做出的变化、改型、添加或替换,Changes, modifications, additions or substitutions made by a person of ordinary skill in the art within the essential scope of the present invention,

也属于本技术的保护范围。It also belongs to the protection scope of this technology.

Claims (5)

1. A vibration positioning method of a distributed optical fiber double M-Z interferometer based on HHT transformation is characterized by comprising the following specific steps,
s1, taking a section of vibration optical fiber signal S (t) to perform Empirical Mode Decomposition (EMD) according to a Hermite difference polynomial of three times in a segmented mode to obtain Intrinsic Mode Functions (IMFs);
s2, carrying out Hilbert transformation on the IMFs obtained by decomposition to obtain the instantaneous frequency of an original signal S (t);
s3, stacking results of all intrinsic mode functions IMFs after HT to obtain a Hilbert spectrum;
s4, extracting a signal segment S containing vibration information according to the peak position of the Hilbert spectrump(t);
S5, extracting the signal segment SpAnd (t) performing cross-correlation operation and positioning operation to obtain vibration position information.
2. The vibration localization method of a distributed fiber double M-Z interferometer based on HHT transformation as claimed in claim 1, wherein the EMD process is that fitting the maximum point of an original signal S (t) to the upper envelope line by using a three times Hermite difference mode, and obtaining the lower envelope line by using the same mode; taking the average value of the upper envelope line and the lower envelope line to obtain an average envelope line ml; subtracting the average envelope ml from the original signal S (t) to obtain a new signal f (t), i.e.
S(t)-ml=f(t)
If there are also negative local maxima and positive local minima of the new signal f (t), the decomposition continues as above, thus yielding a plurality of eigenmode functions IMFs and a residual wave.
3. The vibration localization method of a distributed fiber double M-Z interferometer based on HHT transformation as claimed in claim 2, wherein Hilbert spectrum analysis HSA performs Hilbert transformation on a plurality of intrinsic mode functions IMFs decomposed by empirical mode decomposition EMD, respectively, to obtain instantaneous frequencies, and combines results of all intrinsic mode functions IMFs after Hilbert transformation to obtain Hilbert spectra, so as to obtain frequency variation of original signal s (t).
4. The method of claim 1, wherein the signal segment S containing vibration information is extracted according to Hilbert spectrum peak positionp(t) wherein the signal segment in the clockwise direction is
Figure FDA0002530250990000011
The signal segment in the counterclockwise direction is
Figure FDA0002530250990000012
And taking data of 0.01s near the high peak value to perform cross-correlation operation to obtain delay time and further obtain vibration position information.
5. The method of claim 4, wherein the signal segment in the clockwise direction is
Figure FDA0002530250990000021
And a signal segment in the counterclockwise direction of
Figure FDA0002530250990000022
There is a certain delay tau in the time of arrival at the two balanced detectors,
τ=tL-x+tL-tx
vibration position calculation formula:
Figure FDA0002530250990000023
l is the length of the sensing optical fiber and the conducting optical fiber, tau is the time delay between the forward and backward beams of light reaching the balanced detector, c is the speed of light in vacuum, n is the refractive index of the optical fiber, and x is the vibration position.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114964457A (en) * 2021-02-23 2022-08-30 中国石油天然气股份有限公司 Data processing method and device for dual Mach-Zehnder vibration sensing system

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102322880A (en) * 2011-08-18 2012-01-18 天津大学 Polarization sensitive distributive optical frequency domain reflection disturbance sensor and demodulation method
CN102997946A (en) * 2011-09-16 2013-03-27 北京航空航天大学 Fiber-distributed disturbance sensor and disturbance positioning method thereof
CN103617684A (en) * 2013-12-12 2014-03-05 威海北洋电气集团股份有限公司 Interference type optical fiber perimeter vibration intrusion recognition algorithm
CN105632059A (en) * 2015-12-29 2016-06-01 天津大学 Distributed optical fiber perimeter security system
CN106248119A (en) * 2016-07-14 2016-12-21 南京大学 A kind of distributed ultrahigh speed disturbance quantitative detecting method and device
CN107885940A (en) * 2017-11-10 2018-04-06 吉林大学 A kind of signal characteristic extracting methods for distributed optical fiber vibration sensing system
CN107957276A (en) * 2018-01-05 2018-04-24 南京大学 Phase sensitive optical time domain reflectometer and its measuring method based on frequency-drift compensation
CN108981767A (en) * 2018-08-17 2018-12-11 山东省科学院激光研究所 Optical fiber distributed type monitors system and method
CN110132329A (en) * 2019-05-08 2019-08-16 汕头大学 Stress, temperature and vibration composite detection fiber optic sensor and signal processing method
CN111157098A (en) * 2019-12-31 2020-05-15 中国科学院长春光学精密机械与物理研究所 Demodulation device for simultaneously obtaining amplitude and phase of vibration signal

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102322880A (en) * 2011-08-18 2012-01-18 天津大学 Polarization sensitive distributive optical frequency domain reflection disturbance sensor and demodulation method
CN102997946A (en) * 2011-09-16 2013-03-27 北京航空航天大学 Fiber-distributed disturbance sensor and disturbance positioning method thereof
CN103617684A (en) * 2013-12-12 2014-03-05 威海北洋电气集团股份有限公司 Interference type optical fiber perimeter vibration intrusion recognition algorithm
CN105632059A (en) * 2015-12-29 2016-06-01 天津大学 Distributed optical fiber perimeter security system
CN106248119A (en) * 2016-07-14 2016-12-21 南京大学 A kind of distributed ultrahigh speed disturbance quantitative detecting method and device
CN107885940A (en) * 2017-11-10 2018-04-06 吉林大学 A kind of signal characteristic extracting methods for distributed optical fiber vibration sensing system
CN107957276A (en) * 2018-01-05 2018-04-24 南京大学 Phase sensitive optical time domain reflectometer and its measuring method based on frequency-drift compensation
CN108981767A (en) * 2018-08-17 2018-12-11 山东省科学院激光研究所 Optical fiber distributed type monitors system and method
CN110132329A (en) * 2019-05-08 2019-08-16 汕头大学 Stress, temperature and vibration composite detection fiber optic sensor and signal processing method
CN111157098A (en) * 2019-12-31 2020-05-15 中国科学院长春光学精密机械与物理研究所 Demodulation device for simultaneously obtaining amplitude and phase of vibration signal

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
QINGHUA ZHANG,ECT: "Hilber-Huang Transform based method for monitoring the crack of concrete arch by using FBG sensors", 《OPTIK》 *
吴娇: "Mach-Zehnder干涉仪在石油管道监控中的应用", 《中国优秀硕士学位论文全文数据库 信息科技辑》 *
王思远: "M-Z干涉仪型光纤分布式扰动传感系统模式识别方法研究", 《中国优秀硕士学位论文全文数据库 信息科技辑》 *
王艳歌,等: "《改进的HHT变换在光纤振动模式识别中的应用》", 《现代电子技术》 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN114964457A (en) * 2021-02-23 2022-08-30 中国石油天然气股份有限公司 Data processing method and device for dual Mach-Zehnder vibration sensing system

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