CN114812852A - Multi-sensor fusion optical fiber measuring system and method for complex flow - Google Patents
Multi-sensor fusion optical fiber measuring system and method for complex flow Download PDFInfo
- Publication number
- CN114812852A CN114812852A CN202210534381.6A CN202210534381A CN114812852A CN 114812852 A CN114812852 A CN 114812852A CN 202210534381 A CN202210534381 A CN 202210534381A CN 114812852 A CN114812852 A CN 114812852A
- Authority
- CN
- China
- Prior art keywords
- optical
- optical fiber
- fiber
- coupler
- signal
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 239000013307 optical fiber Substances 0.000 title claims abstract description 119
- 230000004927 fusion Effects 0.000 title claims abstract description 20
- 238000000034 method Methods 0.000 title description 16
- 239000000835 fiber Substances 0.000 claims abstract description 243
- 230000003287 optical effect Effects 0.000 claims abstract description 162
- 230000005540 biological transmission Effects 0.000 claims abstract description 96
- 239000000523 sample Substances 0.000 claims abstract description 40
- 229910001220 stainless steel Inorganic materials 0.000 claims abstract description 11
- 239000010935 stainless steel Substances 0.000 claims abstract description 11
- 230000008859 change Effects 0.000 claims description 26
- 238000005259 measurement Methods 0.000 claims description 26
- 239000007788 liquid Substances 0.000 claims description 23
- 238000001228 spectrum Methods 0.000 claims description 23
- 238000009826 distribution Methods 0.000 claims description 14
- 239000012530 fluid Substances 0.000 claims description 8
- 230000000694 effects Effects 0.000 claims description 7
- 238000000691 measurement method Methods 0.000 claims description 5
- 238000010408 sweeping Methods 0.000 claims description 3
- 230000001131 transforming effect Effects 0.000 claims description 3
- 230000010287 polarization Effects 0.000 claims description 2
- 230000035945 sensitivity Effects 0.000 claims 1
- 238000012360 testing method Methods 0.000 description 10
- 238000001514 detection method Methods 0.000 description 8
- 238000005516 engineering process Methods 0.000 description 8
- 238000011160 research Methods 0.000 description 3
- 230000005514 two-phase flow Effects 0.000 description 3
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 238000011161 development Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000007246 mechanism Effects 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000004458 analytical method Methods 0.000 description 1
- 238000010291 electrical method Methods 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 239000000284 extract Substances 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000009776 industrial production Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 230000005693 optoelectronics Effects 0.000 description 1
- 239000003208 petroleum Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000005057 refrigeration Methods 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01K—MEASURING TEMPERATURE; MEASURING QUANTITY OF HEAT; THERMALLY-SENSITIVE ELEMENTS NOT OTHERWISE PROVIDED FOR
- G01K11/00—Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00
- G01K11/32—Measuring temperature based upon physical or chemical changes not covered by groups G01K3/00, G01K5/00, G01K7/00 or G01K9/00 using changes in transmittance, scattering or luminescence in optical fibres
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B15/00—Measuring arrangements characterised by the use of electromagnetic waves or particle radiation, e.g. by the use of microwaves, X-rays, gamma rays or electrons
- G01B15/02—Measuring arrangements characterised by the use of electromagnetic waves or particle radiation, e.g. by the use of microwaves, X-rays, gamma rays or electrons for measuring thickness
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01L—MEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
- G01L11/00—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00
- G01L11/02—Measuring steady or quasi-steady pressure of a fluid or a fluent solid material by means not provided for in group G01L7/00 or G01L9/00 by optical means
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Arrangements For Transmission Of Measured Signals (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
Description
技术领域technical field
本发明属于复杂流动测试领域,具体为面向复杂流动的多传感器融合光纤测量系统及方法。The invention belongs to the field of complex flow testing, in particular to a multi-sensor fusion optical fiber measurement system and method for complex flow.
背景技术Background technique
两相及多相流等复杂流动广泛存在于核能、制冷、石油、化工等工业过程中,实现对复杂流动特征参数的检测对促进这些工业的发展具有重要意义。随着工业的快速发展及其自动化水平的不断提高,对复杂流动多种参数同时且准确测量的需求也在不断增加,其不仅能用于复杂流动特征的分析与预测,也可为科学研究和工程应用中深入认识复杂流动特性和机理提供新的研究手段。因此,对两相及多相流等复杂流动流动机理以及测量的研究在工业生产和科学研究领域都有非常重要的作用Complex flows such as two-phase and multi-phase flows widely exist in industrial processes such as nuclear energy, refrigeration, petroleum, and chemical industry. The detection of complex flow characteristic parameters is of great significance to promote the development of these industries. With the rapid development of industry and the continuous improvement of automation level, the demand for simultaneous and accurate measurement of multiple parameters of complex flow is also increasing. It can not only be used for the analysis and prediction of complex flow characteristics, but also for scientific research and In-depth understanding of complex flow characteristics and mechanisms in engineering applications provides new research methods. Therefore, the study of complex flow mechanism and measurement such as two-phase and multi-phase flow plays a very important role in industrial production and scientific research.
目前,国内外研究人员研究了多种针对复杂流动的检测方法,包括电学法,通过电极探针测量两相流及多相流的电导率变化来实现测量;射线法,利用射线在穿过流体时的吸收和散射效应来实现检测;差压法,通过流体流经节流装置产生的压差与流体流量之间存在对应关系进行测定;超声波法,利用超声波在两相及多相流中的传播时间以及其散射信号的强度来进行测量;高速摄影法,利用高速摄像机透过透明管段或窗口直接拍摄流体的图像,然后通过图像处理技术提取图像特征,再根据图像特征求取气液两相流的各种参数;光纤探针法,利用光纤探头与流体折射率的不同,通过检测返回的光强信息来研究气液两相流场某处的变化信息;光纤布拉格光栅法,当光纤布拉格光栅所处环境温度、应变等外部条件发生变化时,光纤布拉格光栅的布拉格波长会随之发生漂移,通过对布拉格波长的测量,即可实现对相应特征参量的测量。At present, researchers at home and abroad have studied a variety of detection methods for complex flows, including electrical methods, which measure the conductivity changes of two-phase and multi-phase flows through electrode probes; ray methods, which use rays to pass through the fluid. The detection is realized by the absorption and scattering effects during the time; the differential pressure method is measured by the correspondence between the pressure difference generated by the fluid flowing through the throttling device and the fluid flow; the ultrasonic method is used to detect the ultrasonic wave in two-phase and multi-phase flow. The propagation time and the intensity of its scattered signal are measured; the high-speed photography method uses a high-speed camera to directly take the image of the fluid through the transparent pipe section or window, and then extracts the image features through image processing technology, and then obtains the gas-liquid two-phase according to the image features. Various parameters of the flow; fiber probe method, which uses the difference in refractive index between the fiber probe and the fluid to study the change information of the gas-liquid two-phase flow field by detecting the returned light intensity information; the fiber Bragg grating method, when the fiber Bragg When the external conditions such as the ambient temperature and strain of the grating change, the Bragg wavelength of the fiber Bragg grating will drift accordingly. By measuring the Bragg wavelength, the corresponding characteristic parameters can be measured.
然而上述检测技术存在可测量特征参数单一、易受外界环境因素影响、使用条件苛刻、安全性低、无法实现长距离的空间连续分布式测量等问题。但在实际工程应用中往往需同时对多个复杂流动特征参量的时空分布信息进行高精度测量,以获得更为全面的流场信息。而现有的两相及多相流等复杂流动检测技术主要是点式和准分布式的单一物理量测量传感器,其获取物理量能解调出的两相及多相流特征参量较为有限,无法实现对复杂流动流场信息较为全面的检测,这些都严重制约了其在两相及多相流等复杂流动检测领域的实际应用。为此需要一种适用于两相及多相流等复杂流动测试领域的多传感器融合测量技术,以实现对流场不同特征参量时空信息的高精度同时测量。However, the above detection technologies have problems such as single measurable characteristic parameters, easy to be affected by external environmental factors, harsh use conditions, low security, and inability to achieve long-distance spatial continuous distributed measurement. However, in practical engineering applications, it is often necessary to measure the spatiotemporal distribution information of multiple complex flow characteristic parameters with high precision to obtain more comprehensive flow field information. However, the existing complex flow detection technologies such as two-phase and multi-phase flow are mainly point-type and quasi-distributed single physical quantity measurement sensors, and the characteristic parameters of two-phase and multi-phase flow that can be demodulated by acquiring physical quantities are relatively limited, which cannot be realized. The comprehensive detection of complex flow field information seriously restricts its practical application in the field of complex flow detection such as two-phase and multi-phase flow. Therefore, a multi-sensor fusion measurement technology suitable for complex flow testing fields such as two-phase and multi-phase flow is required to achieve high-precision simultaneous measurement of spatiotemporal information of different characteristic parameters of the flow field.
发明内容SUMMARY OF THE INVENTION
本发明为克服上述现有技术的缺点,提出了面向复杂流动的多传感器融合光纤测量系统及方法,该系统及方法能够实现对两相及多相流等复杂流动的压力、温度、液膜厚度等流动信息的同时测量。In order to overcome the above-mentioned shortcomings of the prior art, the present invention proposes a multi-sensor fusion optical fiber measurement system and method for complex flow, which can realize the pressure, temperature and liquid film thickness of complex flows such as two-phase and multi-phase flows. Measure while waiting for the flow of information.
本发明是采用如下技术方案实现的:The present invention adopts following technical scheme to realize:
一种面向复杂流动的多传感器融合光纤测量系统:包括保偏输出宽带光源、电光调制器、矢量网络分析仪、第一射频放大器、掺铒光纤放大器、光环行器、第一1×2光纤耦合器、第二1×2光纤耦合器、第三1×2光纤耦合器,第一传输光纤、分布式传感光纤、第二传输光纤、温度探头、第三传输光纤、光准直器、光耦合器、第四传输光纤、2×1光纤耦合器、光电探测器、第二射频放大器、计算机。其中温度探头由传感光纤、反射器、毛细不锈钢管构成。A multi-sensor fusion optical fiber measurement system for complex flow: including polarization-maintaining output broadband light source, electro-optic modulator, vector network analyzer, first radio frequency amplifier, erbium-doped fiber amplifier, optical circulator, first 1×2 fiber coupling device, second 1×2 fiber optic coupler, third 1×2 fiber optic coupler, first transmission fiber, distributed sensing fiber, second transmission fiber, temperature probe, third transmission fiber, optical collimator, optical Coupler, fourth transmission fiber, 2×1 fiber coupler, photodetector, second RF amplifier, computer. The temperature probe is composed of a sensing fiber, a reflector, and a capillary stainless steel tube.
保偏输出宽带光源的信号输出端通过保偏光纤跳线与电光调制器的输入端连接;矢量网络分析仪的信号输出端通过高频电缆与第一射频放大器的信号输入端连接;第一射频放大器的信号输出端通过高频电缆与电光调制器的信号输入端连接;电光调制器的输出端通过光纤跳线与掺铒光纤放大器的输入端连接;掺铒光纤放大器的输出端通过光纤跳线与光环行器的信号入射端连接;光环行器的反射端与第一1×2光纤耦合器的入射端连接;光环行器的信号输出端与2×1光纤耦合器的第一入射端连接;第一1×2光纤耦合器的第一出射端与第二1×2光纤耦合器的入射端连接,第一1×2光纤耦合器的第二出射端与第三1×2光纤耦合器的入射端连接;第二1×2光纤耦合器的第一出射端与第一传输光纤连接,第一传输光纤与分布式传感光纤连接;第二1×2光纤耦合器的第二出射端与第二传输光纤连接,第二传输光纤与温度探头连接;第三1×2光纤耦合器的第一出射端与第三传输光纤连接;第三1×2光纤耦合器的第二出射端与光准直器连接;光耦合器与第四传输光纤连接;第四传输光纤与2×1光纤耦合器的第二入射端连接;第四光纤耦合器的出射端通过光纤跳线与高速光电探测器的入射端连接;高速光电探测器的出射端通过高频电缆与第二射频放大器的信号输入端连接;第二射频放大器的信号输出端通过高频电缆与矢量网络分析仪的信号输入端连接,矢量网络分析仪通过高频电缆与计算机连接。The signal output end of the polarization-maintaining output broadband light source is connected to the input end of the electro-optical modulator through a polarization-maintaining fiber jumper; the signal output end of the vector network analyzer is connected to the signal input end of the first radio frequency amplifier through a high-frequency cable; the first radio frequency The signal output end of the amplifier is connected with the signal input end of the electro-optical modulator through a high-frequency cable; the output end of the electro-optical modulator is connected with the input end of the erbium-doped fiber amplifier through a fiber jumper; the output end of the erbium-doped fiber amplifier is connected by a fiber jumper Connect with the signal incident end of the optical circulator; connect the reflection end of the optical circulator with the incident end of the first 1×2 fiber coupler; connect the signal output end of the optical circulator with the first incident end of the 2×1 fiber coupler ; The first outgoing end of the first 1×2 fiber coupler is connected to the incoming end of the second 1×2 fiber coupler, and the second outgoing end of the first 1×2 fiber coupler is connected to the third 1×2 fiber coupler The incident end of the second 1×2 fiber optic coupler is connected to the first transmission fiber, and the first transmission fiber is connected to the distributed sensing fiber; the second output end of the second 1×2 fiber optic coupler is connected It is connected with the second transmission fiber, and the second transmission fiber is connected with the temperature probe; the first output end of the third 1×2 fiber coupler is connected with the third transmission fiber; the second output end of the third 1×2 fiber coupler is connected with The optical collimator is connected; the optical coupler is connected with the fourth transmission fiber; the fourth transmission fiber is connected with the second incident end of the 2×1 fiber coupler; the output end of the fourth fiber coupler is connected to the high-speed photoelectric detection through the fiber jumper The incident end of the high-speed photodetector is connected to the signal input end of the second RF amplifier through a high-frequency cable; the signal output end of the second RF amplifier is connected to the signal input end of the vector network analyzer through a high-frequency cable. , the vector network analyzer is connected to the computer through a high-frequency cable.
分布式传感光纤的纤芯中采用飞秒激光加工有连续的反射器。其中相邻反射器的间距对应的光程差大于保偏输出宽带光源的相干长度,且小于矢量网络分析仪产生的微波信号的相干长度。分布式传感光纤沿被测管道25轴向布置在管道内侧。The core of the distributed sensing fiber is fabricated with a continuous reflector using a femtosecond laser. The optical path difference corresponding to the spacing between adjacent reflectors is greater than the coherence length of the polarization-maintaining output broadband light source, and less than the coherence length of the microwave signal generated by the vector network analyzer. The distributed sensing optical fiber is axially arranged inside the pipeline along the
温度探头的传感光纤置于毛细不锈钢管内,传感光纤的纤芯中采用飞秒激光加工有一个反射器,且传感光纤末端与毛细不锈钢管末端齐平。其中反射器与传感光纤末端端面间距对应的光程差大于保偏输出宽带光源的相干长度,且小于矢量网络分析仪产生的微波信号的相干长度。温度探头嵌于被测管道内壁中,且探头端面与管道内壁齐平。The sensing fiber of the temperature probe is placed in a capillary stainless steel tube, a reflector is processed in the core of the sensing fiber by femtosecond laser, and the end of the sensing fiber is flush with the end of the capillary stainless steel tube. The optical path difference corresponding to the distance between the reflector and the end face of the sensing fiber is greater than the coherence length of the polarization-maintaining output broadband light source, and less than the coherence length of the microwave signal generated by the vector network analyzer. The temperature probe is embedded in the inner wall of the pipe under test, and the end face of the probe is flush with the inner wall of the pipe.
从第三1×2光纤耦合器的第一出射端开始,至第三传输光纤末端,再返回经第三传输光纤、第三1×2光纤耦合器、第一1×2光纤耦合器、光环行器至2×1光纤耦合器第一入射端的距离与从第三1×2光纤耦合器的第二出射端经光准直器、被测两相/多相流管道、光耦合器、第四传输光纤至2×1光纤耦合器第二入射端的距离对应的光程差大于保偏输出宽带光源的相干长度,而小于矢量网络分析仪产生的微波信号的相干长度。From the first output end of the third 1×2 fiber coupler, to the end of the third transmission fiber, and then back through the third transmission fiber, the third 1×2 fiber coupler, the first 1×2 fiber coupler, and the optical ring The distance from the runner to the first incident end of the 2×1 fiber coupler and from the second output end of the third 1×2 fiber coupler through the optical collimator, the two-phase/multi-phase flow pipeline under test, the optical coupler, the first The optical path difference corresponding to the distance from the four transmission fibers to the second incident end of the 2×1 fiber coupler is greater than the coherence length of the polarization-maintaining output broadband light source, but less than the coherence length of the microwave signal generated by the vector network analyzer.
第一传输光纤的长度大于第二传输光纤与温度探头的传感光纤的长度和;第二传输光纤的长度大于第三传输光纤的长度;第二传输光纤的长度大于从第三1×2光纤耦合器的第二出射端开始,经光准直器、被测管道、光耦合器、第四传输光纤至2×1光纤耦合器第二入射端的距离。The length of the first transmission fiber is greater than the sum of the lengths of the second transmission fiber and the sensing fiber of the temperature probe; the length of the second transmission fiber is greater than the length of the third transmission fiber; the length of the second transmission fiber is greater than that from the third 1×2 fiber The distance from the second outgoing end of the coupler to the second incoming end of the 2×1 fiber coupler through the optical collimator, the pipe under test, the optical coupler, and the fourth transmission fiber.
面向复杂流动的多传感器融合光纤测量方法,该方法在本发明所述的面向复杂流动的多传感器融合光纤测量系统中实现,该方法是采用如下步骤实现的:A complex flow-oriented multi-sensor fusion optical fiber measurement method is implemented in the complex flow-oriented multi-sensor fusion optical fiber measurement system of the present invention, and the method is implemented by the following steps:
保偏输出宽带光源输出的光信号进入电光调制器;矢量网络分析仪输出的微波信号经第一射频放大器放大后进入电光调制器;微波信号经电光调制器调制后加载到光信号上;经微波信号调制后的光信号从电光调制器输出后进入掺铒光纤放大器,经掺铒光纤放大器放大后输入到光环行器;光信号经光环行器的反射端输出后进入第一1×2光纤耦合器,经第一1×2光纤耦合器后分成两路;由第一出射端输出的光信号进入第二1×2光纤耦合器,由第二出射端输出的光信号进入第三1×2光纤耦合器;第二1×2光纤耦合器第一出射端输出的光信号通过第一传输光纤进入分布式传感光纤,并在传感光纤内的反射器处发生反射,反射的光信号的微波包络在相遇处发生干涉,干涉信号依次经第一传输光纤、第二1×2光纤耦合器、第一1×2光纤耦合器后返回光环行器,并从光环行器的出射端输出后进入2×1光纤耦合器;第二1×2光纤耦合器第二出射端输出的光信号通过第二传输光纤进入温度探头,并在传感光纤中的反射器及其末端端面处发生反射,反射的光信号的微波包络在相遇处发生干涉,干涉信号依次经第二传输光纤、第二1×2光纤耦合器、第一1×2光纤耦合器后返回光环行器,并从光环行器的出射端输出后进入2×1光纤耦合器;第三1×2光纤耦合器第一出射端输出的光信号进入第三传输光纤并在其末端端面处发生反射,反射信号依次经第三传输光纤、第三1×2光纤耦合器、第一1×2光纤耦合器后返回光环行器,并从光环行器的出射端输出后进入2×1光纤耦合器;第三1×2光纤耦合器第二出射端输出的光信号进入光准直器,经光准直器后进入被测管道,光信号穿过被测管道后进入光耦合器,并经传感光纤进入2×1光纤耦合器,并与经第三传输光纤末端端面反射回的光信号的微波包络发生干涉;微波干涉信号从2×1光纤耦合器出射端输出后进入高速光电探测器;经高速光电探测器转换为电信号后进入第二射频放大器;经第二射频放大器放大后被矢量网络分析仪采集,矢量网络分析仪将采集到的干涉信息输入到计算机。通过对矢量网络分析仪输出的微波信号进行扫频,即可得到微波信号的干涉谱。The optical signal output by the polarization-maintaining output broadband light source enters the electro-optic modulator; the microwave signal output by the vector network analyzer is amplified by the first RF amplifier and then enters the electro-optic modulator; the microwave signal is modulated by the electro-optic modulator and then loaded onto the optical signal; The modulated optical signal is output from the electro-optic modulator and then enters the erbium-doped fiber amplifier, which is amplified by the erbium-doped fiber amplifier and then input to the optical circulator; the optical signal is output through the reflection end of the optical circulator and then enters the first 1×2 fiber coupling It is divided into two paths after passing through the first 1×2 fiber coupler; the optical signal output from the first output end enters the second 1×2 fiber coupler, and the optical signal output from the second output end enters the third 1×2 fiber optic coupler. Optical fiber coupler; the optical signal output from the first output end of the second 1×2 optical fiber coupler enters the distributed sensing fiber through the first transmission fiber, and is reflected at the reflector in the sensing fiber. The microwave envelope interferes at the meeting point, and the interference signal returns to the optical circulator through the first transmission fiber, the second 1×2 fiber coupler, and the first 1×2 fiber coupler in turn, and is output from the output end of the optical circulator Then enter the 2×1 fiber coupler; the optical signal output from the second output end of the second 1×2 fiber coupler enters the temperature probe through the second transmission fiber, and is reflected at the reflector in the sensing fiber and its end face , the microwave envelope of the reflected optical signal interferes at the meeting point, and the interference signal returns to the optical circulator through the second transmission fiber, the second 1×2 fiber coupler, and the first 1×2 fiber coupler in turn, and is transmitted from the optical ring. The optical signal output from the output end of the traveler enters the 2×1 fiber coupler; the optical signal output from the first output end of the third 1×2 fiber coupler enters the third transmission fiber and is reflected at its end face, and the reflected signal passes through the third transmission fiber in turn. The three transmission fibers, the third 1×2 fiber coupler, and the first 1×2 fiber coupler return to the optical circulator, and are output from the output end of the optical circulator and then enter the 2×1 fiber coupler; the third 1×2 fiber coupler The optical signal output from the second output end of the optical fiber coupler enters the optical collimator, and then enters the measured pipeline after passing through the optical collimator. The optical signal enters the optical coupler after passing through the measured pipeline, and enters the 2×1 through the sensing fiber The optical fiber coupler interferes with the microwave envelope of the optical signal reflected by the end face of the third transmission fiber; the microwave interference signal is output from the output end of the 2×1 fiber coupler and then enters the high-speed photodetector; after the high-speed photodetector After being converted into an electrical signal, it enters the second radio frequency amplifier; after being amplified by the second radio frequency amplifier, it is collected by a vector network analyzer, and the vector network analyzer inputs the collected interference information to the computer. By sweeping the microwave signal output by the vector network analyzer, the interference spectrum of the microwave signal can be obtained.
分布式传感光纤受到两相/多相流复杂流型流态的影响,其相应位置处光纤的长度会随流体压力的变化而发生改变,从而导致反射器反射的光信号的光程发生变化,进而微波包络信号的干涉谱会发生频移;由于热光效应和热膨胀效应,温度变化会导致温度探头的传感光纤的长度和折射率发生改变,从而使传感光纤末端端面和反射器构成的法布里-珀罗腔的腔长发生变化,故其反射的光信号对应的光程差发生改变,使其对应的微波干涉谱发生频移;被测管道内液膜厚度的变化导致由该路光信号的光程发生变化,从而使该路光信号与经第三传输光纤末端端面反射回的光信号的微波包络发生干涉产生的微波干涉谱发生频移。两相/多相流等复杂流动的压力、温度、液膜厚度等流场变化信息与光程变化量存在对应关系,光程变化量与微波干涉谱频移量存在对应关系,故根据微波干涉谱频移量可通过分布式传感光纤测得压力分布信息,通过温度探头测得温度信息,以及通过第三1×2光纤耦合器的两输出光路构成的干涉系统测得液膜厚度信息。The distributed sensing fiber is affected by the complex flow regime of two-phase/multi-phase flow, and the length of the fiber at the corresponding position will change with the change of the fluid pressure, which will lead to the change of the optical path of the optical signal reflected by the reflector. , and then the interference spectrum of the microwave envelope signal will shift in frequency; due to the thermo-optic effect and thermal expansion effect, the temperature change will cause the length and refractive index of the sensing fiber of the temperature probe to change, so that the end face of the sensing fiber and the reflector will change. The cavity length of the formed Fabry-Perot cavity changes, so the optical path difference corresponding to the reflected optical signal changes, causing the corresponding microwave interference spectrum to shift in frequency; the change in the thickness of the liquid film in the measured pipeline causes The optical path of the optical signal of this path changes, so that the microwave interference spectrum generated by the interference of the optical signal of this path and the microwave envelope of the optical signal reflected back by the end face of the third transmission fiber is frequency shifted. There is a corresponding relationship between the pressure, temperature, liquid film thickness and other flow field change information of complex flows such as two-phase/multiphase flow and the optical path change. There is a corresponding relationship between the optical path change and the frequency shift of the microwave interference spectrum. Therefore, according to the microwave interference The spectral frequency shift can measure the pressure distribution information through the distributed sensing fiber, measure the temperature information through the temperature probe, and measure the liquid film thickness information through the interference system formed by the two output optical paths of the third 1×2 optical fiber coupler.
通过将采集到的微波干涉谱从频域变换到时域得到反射信号的空间分布信息,再根据各光路的实际光程区分出各传感器对应的反射信号;利用矩形窗函数对各传感器对应的微波干涉谱进行重构,进而可解调出待测的两相及多相流等复杂流动的压力分布、温度、液膜厚度等流场流动信息。The spatial distribution information of the reflected signal is obtained by transforming the collected microwave interference spectrum from the frequency domain to the time domain, and then the reflected signal corresponding to each sensor is distinguished according to the actual optical path of each optical path; the rectangular window function is used to analyze the microwave corresponding to each sensor. The interference spectrum can be reconstructed, and then the flow field flow information such as the pressure distribution, temperature, liquid film thickness and other complex flows of the two-phase and multi-phase flows to be measured can be demodulated.
通过温度探头测得的温度信息对分布式传感光纤测量中压力和温度交叉敏感问题进行温度补偿。The temperature information measured by the temperature probe is used to perform temperature compensation for the cross-sensitivity problem of pressure and temperature in the distributed sensing optical fiber measurement.
该系统及方法用于包括气液、液液在内的两相流以及包括油气水三相流在内的多相流等复杂流动下不同流型流态的压力分布、温度、液膜厚度等流场流动信息的同时测量。The system and method are used for the pressure distribution, temperature, liquid film thickness, etc. of different flow patterns under complex flows such as two-phase flow including gas-liquid and liquid-liquid and multiphase flow including oil-gas-water three-phase flow Simultaneous measurement of flow field flow information.
与现有的两相及多相流等复杂流动测试技术相比,本发明所述的面向复杂流动的多传感器融合光纤测量系统及方法,基于微波光子技术的优势,将光纤传感技术与微波干涉技术相结合,具有高信噪比、高测量分辨率、低波导依赖性以及强适应性等特点。可只采用一套信号发生和接收装置,将多种光纤传感器集于单一系统,实现对等复杂流动的压力分布、温度、液膜厚度等流动参数的同时测量。Compared with the existing complex flow measurement technologies such as two-phase and multi-phase flow, the multi-sensor fusion optical fiber measurement system and method for complex flow described in the present invention is based on the advantages of microwave photonic technology, and combines optical fiber sensing technology with microwave. The combination of interferometric technology has the characteristics of high signal-to-noise ratio, high measurement resolution, low waveguide dependence and strong adaptability. Only one set of signal generating and receiving devices can be used to integrate a variety of optical fiber sensors into a single system to achieve simultaneous measurement of flow parameters such as pressure distribution, temperature, and liquid film thickness in an equivalent complex flow.
附图说明Description of drawings
图1是本发明所述的面向复杂流动的多传感器融合光纤测量系统结构示意图。FIG. 1 is a schematic structural diagram of the complex flow-oriented multi-sensor fusion optical fiber measurement system according to the present invention.
图2为本发明所述系统中温度探头的结构示意图。FIG. 2 is a schematic structural diagram of a temperature probe in the system according to the present invention.
图中:1-保偏输出宽带光源;2-电光调制器;3-矢量网络分析仪;4-第一射频放大器;5-掺铒光纤放大器;6-光环行器;7-第一1×2光纤耦合器;8-第二1×2光纤耦合器;9-第三1×2光纤耦合器;10-第一传输光纤;11-分布式传感光纤;12-第二传输光纤;13-温度探头;14-第三传输光纤;15-光准直器;16-光耦合器;17-第四传输光纤;18-2×1光纤耦合器;19-光电探测器;20-第二射频放大器;21-计算机;22-传感光纤;23-反射器;24-毛细不锈钢管;25-被测管道。In the figure: 1- polarization maintaining output broadband light source; 2- electro-optic modulator; 3- vector network analyzer; 4- first RF amplifier; 5- erbium-doped fiber amplifier; 6- optical circulator; 7- first 1× 2 fiber coupler; 8-second 1×2 fiber coupler; 9-third 1×2 fiber coupler; 10-first transmission fiber; 11-distributed sensing fiber; 12-second transmission fiber; 13 -Temperature probe; 14-third transmission fiber; 15-optical collimator; 16-optical coupler; 17-fourth transmission fiber; 18-2×1 fiber coupler; 19-photodetector; 20-second RF amplifier; 21-computer; 22-sensing fiber; 23-reflector; 24-capillary stainless steel tube; 25-tested pipe.
具体实施方式Detailed ways
面向复杂流动的多传感器融合光纤测量系统,包括保偏输出宽带光源1、电光调制器2、矢量网络分析仪3、第一射频放大器4、掺铒光纤放大器5、光环行器6、第一1×2光纤耦合器7、第二1×2光纤耦合器8、第三1×2光纤耦合器9,第一传输光纤10、分布式传感光纤11、第二传输光纤12、温度探头13、第三传输光纤14、光准直器15、光耦合器16、第四传输光纤17、2×1光纤耦合器18、光电探测器19、第二射频放大器20、计算机21。其中温度探头由传感光纤22、反射器23、毛细不锈钢管24构成。Multi-sensor fusion optical fiber measurement system for complex flow, including polarization-maintaining output broadband light source 1, electro-
保偏输出宽带光源1的信号输出端通过保偏光纤跳线与电光调制器2的输入端连接;矢量网络分析仪3的信号输出端通过高频电缆与第一射频放大器4的信号输入端连接;第一射频放大器4的信号输出端通过高频电缆与电光调制器2的信号输入端连接;电光调制器2的输出端通过光纤跳线与掺铒光纤放大器5的输入端连接;掺铒光纤放大器5输出端通过光纤跳线与光环行器6的信号入射端连接;光环行器6的反射端与第一1×2光纤耦合器7的入射端连接;光环行器6的信号输出端与2×1光纤耦合器18的第一入射端连接;第一1×2光纤耦合器7的第一出射端与第二1×2光纤耦合器8的入射端连接,第一1×2光纤耦合器7的第二出射端与第三1×2光纤耦合器9的入射端连接;第二1×2光纤耦合器8的第一出射端与第一传输光纤10连接,第一传输光纤10与分布式传感光纤11连接;第二1×2光纤耦合器8的第二出射端与第二传输光纤12连接,第二传输光纤12与温度探头13连接;第三1×2光纤耦合器9的第一出射端与第三传输光纤14连接;第三1×2光纤耦合器9的第二出射端与光准直器15连接;光耦合器16与第四传输光纤17连接;第四传输光纤17与2×1光纤耦合器18的第二入射端连接;2×1光纤耦合器18的出射端通过光纤跳线与高速光电探测器19的入射端连接;高速光电探测器19的出射端通过高频电缆与第二射频放大器20的信号输入端连接;第二射频放大器20的信号输出端通过高频电缆与矢量网络分析仪3的信号输入端连接,矢量网络分析仪3通过高频电缆与计算机12连接。The signal output end of the polarization-maintaining output broadband light source 1 is connected to the input end of the electro-
具体实施时,分布式传感光纤9的纤芯中采用飞秒激光加工有连续的反射器。其中相邻反射器的间距对应的光程差大于保偏输出宽带光源的相干长度,且小于矢量网络分析仪3产生的微波信号的相干长度。分布式传感9光纤沿被测管道25轴向布置在管道内侧。In specific implementation, the core of the distributed sensing fiber 9 is processed with a continuous reflector by using a femtosecond laser. The optical path difference corresponding to the spacing between adjacent reflectors is greater than the coherence length of the polarization-maintaining output broadband light source, and less than the coherence length of the microwave signal generated by the
具体实施时,温度探头13的传感光纤22置于毛细不锈钢管24内,传感光纤22的纤芯中采用飞秒激光加工有一个反射器23,且传感光纤22末端与毛细不锈钢管24末端齐平。其中反射器23与传感光纤22末端端面间距对应的光程差大于保偏输出宽带光源的相干长度,且小于矢量网络分析仪3产生的微波信号的相干长度。温度探头13嵌于被测管道25内壁中,且探头端面与管道内壁齐平。In specific implementation, the
具体实施时,从第三1×2光纤耦合器9的第一出射端开始,至第三传输光纤14末端,再返回经第三传输光纤14、第三1×2光纤耦合器9、第一1×2光纤耦合器7、光环行器6至2×1光纤耦合器18第一入射端的距离与从第三1×2光纤耦合器9的第二出射端经光准直器15、被测两相/多相流管道25、光耦合器16、第四传输光纤17至2×1光纤耦合器18第二入射端的距离对应的光程差大于保偏输出宽带光源1的相干长度,而小于矢量网络分析仪3产生的微波信号的相干长度。In the specific implementation, from the first output end of the third 1×2 fiber coupler 9 to the end of the
具体实施时,第一传输光纤10的长度大于第二传输光纤12与温度探头的传感光纤22的长度和;第二传输光纤12的长度大于第三传输光纤14的长度;第二传输光纤12的长度大于第三1×2光纤耦合器9的第二出射端经光准直器15、被测管道25、光耦合器16、第四传输光纤17至2×1光纤耦合器18第二入射端的距离。In specific implementation, the length of the first transmission fiber 10 is greater than the length sum of the
本发明同时提供一种面向复杂流动的多传感器融合光纤测量方法,该方法在本发明所述的面向复杂流动的多传感器融合光纤测量系统中实现,该方法是采用如下步骤实现的:The present invention also provides a complex flow-oriented multi-sensor fusion optical fiber measurement method, which is implemented in the complex flow-oriented multi-sensor fusion optical fiber measurement system of the present invention, and the method is implemented by the following steps:
保偏输出宽带光源1输出的光信号进入电光调制器2;矢量网络分析仪3输出的微波信号经第一射频放大器4放大后进入电光调制器2;微波信号经电光调制器2调制后加载到光信号上;经微波信号调制后的光信号从电光调制器2输出后进入掺铒光纤放大器5,经掺铒光纤放大器5放大后输入到光环行器6;光信号经光环行器6的反射端输出后进入第一1×2光纤耦合器7,经第一1×2光纤耦合器7后分成两路;由第一出射端输出的光信号进入第二1×2光纤耦合器8,由第二出射端输出的光信号进入第三1×2光纤耦合器9;第二1×2光纤耦合器8第一出射端输出的光信号通过第一传输光纤10进入分布式传感光纤11,并在传感光纤11内的反射器处发生反射,反射的光信号的微波包络在相遇处发生干涉,干涉信号依次经第一传输光纤10、第二1×2光纤耦合器8、第一1×2光纤耦合器7后返回光环行器6,并从光环行器6的出射端输出后进入2×1光纤耦合器18;第二1×2光纤耦合器8第二出射端输出的光信号通过第二传输光纤12进入温度探头13,并在传感光纤22中的反射器及其末端端面处发生反射,反射的光信号的微波包络在相遇处发生干涉,干涉信号依次经第二传输光纤12、第二1×2光纤耦合器8、第一1×2光纤耦合器7后返回光环行器6,并从光环行器6的出射端输出后进入2×1光纤耦合器18;第三1×2光纤耦合器9第一出射端输出的光信号进入第三传输光纤14并在其末端端面处发生反射,反射信号依次经第三传输光纤14、第三1×2光纤耦合器9、第一1×2光纤耦合器7后返回光环行器6,并从光环行器6的出射端输出后进入2×1光纤耦合器18;第三1×2光纤耦合器9第二出射端输出的光信号进入光准直器15,经光准直器后进入被测两相/多相流管道25,光信号穿过被测管道25后进入光耦合器16,并经传感光纤17进入2×1光纤耦合器18,并与经第三传输光纤14末端端面反射回的光信号的微波包络发生干涉;微波干涉信号从2×1光纤耦合器18出射端输出后进入高速光电探测器19;经高速光电探测器19转换为电信号后进入第二射频放大器20;经第二射频放大器20放大后被矢量网络分析仪3采集,矢量网络分析仪3将采集到的干涉信息输入到计算机21。通过对矢量网络分析仪3输出的微波信号进行扫频,即可得到微波信号的干涉谱。The optical signal output by the polarization-maintaining output broadband light source 1 enters the electro-
具体实施时,分布式传感光纤11受到两相/多相流复杂流型流态影响,其相应位置处光纤的长度会随流体压力的变化而发生改变,从而导致反射器反射的光信号的光程发生变化,进而微波包络信号的干涉谱会发生频移;由于热光效应和热膨胀效应,温度变化会导致温度探头13的传感光纤22的长度和折射率发生改变,从而使传感光纤22末端端面和反射器23构成的法布里-珀罗腔的腔长发生变化,故其反射的光信号对应的光程差发生改变,使其对应的微波干涉谱发生频移;被测管道25内液膜厚度的变化导致由该路光信号的光程发生变化,从而使该路光信号与经第三传输光纤14末端端面反射回的光信号的微波包络发生干涉产生的微波干涉谱发生频移。两相/多相流等复杂流动压力、温度、液膜厚度等流场变化信息与光程变化量存在对应关系,光程变化量与微波干涉谱频移量存在对应关系,故根据微波干涉谱频移量可通过分布式传感光纤11测得压力分布信息,通过温度探头13测得温度信息,以及通过第三1×2光纤耦合器9的两输出光路构成的干涉系统测得液膜厚度信息。During the specific implementation, the distributed
具体实施时,通过将采集到的微波干涉谱从频域变换到时域得到反射信号的空间分布信息,再根据各光路的实际光程区分出各传感器对应的反射信号;利用矩形窗函数对各传感器对应的微波干涉谱进行重构,进而可解调出待测的两相及多相流等复杂流动的压力分布、温度、液膜厚度等流场流动信息。In the specific implementation, the spatial distribution information of the reflected signal is obtained by transforming the collected microwave interference spectrum from the frequency domain to the time domain, and then the reflected signal corresponding to each sensor is distinguished according to the actual optical path of each optical path; The microwave interference spectrum corresponding to the sensor is reconstructed, and then the pressure distribution, temperature, liquid film thickness and other flow field flow information of complex flows such as two-phase and multi-phase flows to be measured can be demodulated.
具体实施时,通过温度探头13测得的温度信息对分布式传感光纤11测量中压力和温度交叉敏感问题进行温度补偿。In a specific implementation, temperature compensation is performed for the cross-sensitivity problem of pressure and temperature in the measurement of the distributed
具体实施时,该系统及方法用于包括气液、液液在内的两相流以及包括油气水三相流在内的多相流等复杂流动的不同流型流态的压力分布、温度、液膜厚度等流动参数的同时测量。In specific implementation, the system and method are used for the pressure distribution, temperature, pressure, temperature, pressure, etc. of different flow patterns and flow states of complex flows such as two-phase flows including gas-liquid and liquid-liquid and multi-phase flows including oil-gas-water three-phase flow. Simultaneous measurement of flow parameters such as liquid film thickness.
Claims (6)
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202210534381.6A CN114812852B (en) | 2022-05-17 | 2022-05-17 | Multi-sensor fusion optical fiber measurement system and method for complex flow |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN202210534381.6A CN114812852B (en) | 2022-05-17 | 2022-05-17 | Multi-sensor fusion optical fiber measurement system and method for complex flow |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN114812852A true CN114812852A (en) | 2022-07-29 |
| CN114812852B CN114812852B (en) | 2025-04-22 |
Family
ID=82515458
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN202210534381.6A Active CN114812852B (en) | 2022-05-17 | 2022-05-17 | Multi-sensor fusion optical fiber measurement system and method for complex flow |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN114812852B (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN116481670A (en) * | 2023-04-24 | 2023-07-25 | 重庆大学 | Sapphire fiber F-P temperature sensing system and demodulation method based on microwave photon interference fiber loop and virtual reflection surface |
| CN118706161A (en) * | 2024-06-19 | 2024-09-27 | 天津大学 | A fiber grating distributed measurement device and method based on microwave domain and optical domain demodulation |
| CN118999642A (en) * | 2024-06-19 | 2024-11-22 | 天津大学 | Pressure and temperature distributed simultaneous measurement device and method based on microwave domain and optical domain demodulation |
| CN119845318A (en) * | 2025-03-19 | 2025-04-18 | 武汉理工大学 | Optical fiber synchronous composite sensing device and method for fluid temperature-pressure-flow |
Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20140340671A1 (en) * | 2013-05-20 | 2014-11-20 | Habsonic LLC | Optical carrier based microwave interferometric system and method |
| CN109631963A (en) * | 2019-01-21 | 2019-04-16 | 杭州光预科技有限公司 | Polynary parameter measurement system and method based on microstructured optical fibers interference microwave photon method for sensing |
| 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 |
| CN112014352A (en) * | 2020-08-25 | 2020-12-01 | 天津大学 | Multiphase flow parameter distributed optical fiber measuring system based on light-carried microwave interference |
| CN112284430A (en) * | 2020-10-23 | 2021-01-29 | 天津大学 | A multi-phase flow multi-parameter optical fiber detection device based on light-borne microwave interference |
| CN112747682A (en) * | 2020-12-22 | 2021-05-04 | 天津大学 | Liquid film thickness measurement system based on light carries microwave interference |
| WO2021093181A1 (en) * | 2019-11-13 | 2021-05-20 | 天津大学 | Differential cotdr distributed acoustic sensing device and method based on heterogeneous double-sideband chirped pulse |
-
2022
- 2022-05-17 CN CN202210534381.6A patent/CN114812852B/en active Active
Patent Citations (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20140340671A1 (en) * | 2013-05-20 | 2014-11-20 | Habsonic LLC | Optical carrier based microwave interferometric system and method |
| CN109631963A (en) * | 2019-01-21 | 2019-04-16 | 杭州光预科技有限公司 | Polynary parameter measurement system and method based on microstructured optical fibers interference microwave photon method for sensing |
| 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 |
| WO2021093181A1 (en) * | 2019-11-13 | 2021-05-20 | 天津大学 | Differential cotdr distributed acoustic sensing device and method based on heterogeneous double-sideband chirped pulse |
| CN112014352A (en) * | 2020-08-25 | 2020-12-01 | 天津大学 | Multiphase flow parameter distributed optical fiber measuring system based on light-carried microwave interference |
| CN112284430A (en) * | 2020-10-23 | 2021-01-29 | 天津大学 | A multi-phase flow multi-parameter optical fiber detection device based on light-borne microwave interference |
| CN112747682A (en) * | 2020-12-22 | 2021-05-04 | 天津大学 | Liquid film thickness measurement system based on light carries microwave interference |
Non-Patent Citations (1)
| Title |
|---|
| 鲁辉;张立军;郑占旗;张一恒;冷永清;廖先华;: "基于光纤的新型矢量和微波光子移相器", 强激光与粒子束, no. 12, 15 December 2011 (2011-12-15) * |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN116481670A (en) * | 2023-04-24 | 2023-07-25 | 重庆大学 | Sapphire fiber F-P temperature sensing system and demodulation method based on microwave photon interference fiber loop and virtual reflection surface |
| CN118706161A (en) * | 2024-06-19 | 2024-09-27 | 天津大学 | A fiber grating distributed measurement device and method based on microwave domain and optical domain demodulation |
| CN118999642A (en) * | 2024-06-19 | 2024-11-22 | 天津大学 | Pressure and temperature distributed simultaneous measurement device and method based on microwave domain and optical domain demodulation |
| CN119845318A (en) * | 2025-03-19 | 2025-04-18 | 武汉理工大学 | Optical fiber synchronous composite sensing device and method for fluid temperature-pressure-flow |
Also Published As
| Publication number | Publication date |
|---|---|
| CN114812852B (en) | 2025-04-22 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN114812852B (en) | Multi-sensor fusion optical fiber measurement system and method for complex flow | |
| CN112284430B (en) | A multi-phase flow multi-parameter optical fiber detection device based on light-borne microwave interference | |
| CN112014352A (en) | Multiphase flow parameter distributed optical fiber measuring system based on light-carried microwave interference | |
| CN100432658C (en) | A Mach-Zehnder Interferometer Sensor Based on Asymmetric Interference Arm | |
| WO2017219569A1 (en) | Optical fiber fabry-perot type flow measurement device and method with local bending for flow guiding | |
| Ding et al. | A low-flow fiber-optic flowmeter based on bending measuring using a cladding fiber Bragg grating | |
| CN101319878A (en) | A method and device for measuring optical fiber length with high precision and large range | |
| CN109959403A (en) | A multi-parameter large-capacity sensing system | |
| CN107036733A (en) | The many reference amounts Distributed Measurement System and measuring method of twin-core dim light grid array based on dark pulse light source | |
| CN104089682A (en) | Liquid level measurement device and method | |
| CN102322894A (en) | Allfiber type long period fiber grating solution multi-parameter sensing system | |
| CN114137273A (en) | Temperature sensitive current eliminating sensing device of FBG (fiber Bragg Grating) cascade optical fiber composite structure | |
| CN112747682B (en) | Liquid film thickness measurement system based on light carries microwave interference | |
| CN107782696B (en) | Sensing system and method for measuring the refractive index of distributed liquid using a taper fiber | |
| CN108007603B (en) | Multi-parameter distribution measuring system based on asymmetric double-core optical fiber | |
| Zhao et al. | Integrated hybrid optical fiber Mach-Zehnder interferometers for simultaneous measurement of seawater temperature and salinity | |
| Wu et al. | Temperature-compensated highly sensitive reflective SPR fiber sensor based on tapered seven-core fiber | |
| CN114812851A (en) | Microwave domain demodulation-based complex flow multi-path distributed measuring device and method | |
| Zhou et al. | Dual-channel SPR sensor based on an MMF-DHSMF-NCF reflective structure | |
| Li et al. | Multipoint displacement measurement based on low intracavity-loss FLRD method | |
| CN107631814B (en) | Optical self-coherent sensing optical path structure, frequency shift change detection method and sensing device | |
| Fu et al. | Experimental study of high sensitive surface plasmon resonance refractive index sensor based on coreless fiber coated Au film | |
| Li et al. | High sensitivity fiber optic ultraviolet light and temperature sensor based on Fabry-Perot cavity fabricated by MA-POSS material | |
| CN100451609C (en) | Interference evanescent wave chemical and biological sensor and system with fibre-optical Michelson | |
| CN109142244B (en) | Multi-ring-down interference type all-fiber gas sensor |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PB01 | Publication | ||
| PB01 | Publication | ||
| SE01 | Entry into force of request for substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant |