CN107402054B - Optical fiber water level sensing device and method based on Mach-Zehnder interference - Google Patents
Optical fiber water level sensing device and method based on Mach-Zehnder interference Download PDFInfo
- Publication number
- CN107402054B CN107402054B CN201710613811.2A CN201710613811A CN107402054B CN 107402054 B CN107402054 B CN 107402054B CN 201710613811 A CN201710613811 A CN 201710613811A CN 107402054 B CN107402054 B CN 107402054B
- Authority
- CN
- China
- Prior art keywords
- collimator
- coupler
- water level
- arm
- reference arm
- 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.)
- Expired - Fee Related
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
- G01F23/284—Electromagnetic waves
- G01F23/292—Light, e.g. infrared or ultraviolet
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/32—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
- G01D5/34—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
- G01D5/353—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre
- G01D5/35306—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement
- G01D5/35329—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells influencing the transmission properties of an optical fibre using an interferometer arrangement using interferometer with two arms in transmission, e.g. Mach-Zender interferometer
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02A—TECHNOLOGIES FOR ADAPTATION TO CLIMATE CHANGE
- Y02A90/00—Technologies having an indirect contribution to adaptation to climate change
- Y02A90/30—Assessment of water resources
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Thermal Sciences (AREA)
- Fluid Mechanics (AREA)
- Length Measuring Devices By Optical Means (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Abstract
Description
技术领域technical field
本发明属于光纤传感的技术领域,尤其涉及一种基于马赫-增德尔干涉的光纤水位传感装置及方法。The invention belongs to the technical field of optical fiber sensing, in particular to an optical fiber water level sensing device and method based on Mach-Zehnder interference.
背景技术Background technique
在某些复杂的环境中,对水位的实时监测必不可少。例如地下水资源复杂难测,且地下水的污染和地下水超采引起的地面沉降是缓变型的,一旦积累到一定程度,将造成不可逆的破坏;海底情况复杂,当海啸发生时,会给周边的人们带来巨大的经济财产损失,甚至威胁生命安全,因此实时有效的监测水位变化非常重要。为了提高测量精度并实现非接触绝对测量,采用光学干涉技术,为了简化光路结构和提高光路稳定性,结合了光纤传感技术,提出了一种光纤干涉水位传感器。In some complex environments, real-time monitoring of water levels is essential. For example, groundwater resources are complex and unpredictable, and groundwater pollution and land subsidence caused by overexploitation of groundwater are slow-changing. Once accumulated to a certain extent, irreversible damage will be caused; the seabed is complicated. It will bring huge economic and property losses, and even threaten life safety, so it is very important to monitor water level changes in real time and effectively. In order to improve the measurement accuracy and realize the non-contact absolute measurement, the optical interference technology is adopted. In order to simplify the optical path structure and improve the stability of the optical path, combined with the optical fiber sensing technology, a fiber optic interference water level sensor is proposed.
水位传感器有很多不同的类型,在公开的专利号为CN205049204U的中国专利中,提出了一种压阻式水位计,该水位计采用电流型压阻传感器,通过恒流源电流的作用,输出变化的电压信号,再经过放大、模数转换、信号处理后发送至数据采集装置,该水位计的缺点是电路结构复杂,受电磁干扰影响严重;在公开的专利号为CN205898251U的中国专利中,提出了一种超声波水位计,该水位计包括发射模块、接收模块等,利用超声波发射接收的原理来测量液位,但超声波的发射接收对环境要求比较高,不能应用于复杂恶劣的水环境下;在公开的专利号为CN204461547U的中国专利中,提出了一种光纤干涉水位传感器,利用光纤传感技术,构造迈克尔逊干涉结构,通过相位解调实现水位测量,但是该结构将光纤缠绕在硅胶柱体上,当水位变化时光纤被拉伸,当光纤达到拉伸极限时,橡胶柱体还可以进行弹性变化,因此光纤拉伸量较大时不能准确反应水位的变化。There are many different types of water level sensors. In the published Chinese patent No. CN205049204U, a piezoresistive water level gauge is proposed. The water level gauge uses a current-type piezoresistive sensor. Through the action of a constant current source current, the output changes The voltage signal of the water level gauge is sent to the data acquisition device after amplification, analog-to-digital conversion, and signal processing. The disadvantage of the water level gauge is that the circuit structure is complex and is seriously affected by electromagnetic interference; An ultrasonic water level gauge is developed. The water level gauge includes a transmitting module, a receiving module, etc., and uses the principle of ultrasonic transmitting and receiving to measure the liquid level. However, the ultrasonic transmitting and receiving has relatively high environmental requirements and cannot be applied in complex and harsh water environments; In the published Chinese patent No. CN204461547U, an optical fiber interference water level sensor is proposed, using optical fiber sensing technology, constructing a Michelson interference structure, and realizing water level measurement through phase demodulation, but this structure winds the optical fiber on a silica gel column In general, when the water level changes, the optical fiber is stretched. When the optical fiber reaches the stretching limit, the rubber cylinder can also undergo elastic changes. Therefore, when the optical fiber is stretched a lot, it cannot accurately reflect the change of the water level.
综上所述,如何解决现有技术中存在的水位传感器测量精度低、范围小的问题,尚缺乏有效的解决方案。To sum up, there is still no effective solution on how to solve the problems of low measurement accuracy and small range of the water level sensor in the prior art.
发明内容Contents of the invention
本发明为了解决上述问题,克服现有技术中存在的水位传感器测量精度低、范围小的问题,本发明的第一目的是提供一种基于马赫-增德尔干涉的光纤水位传感装置。In order to solve the above problems, the present invention overcomes the problems of low measurement accuracy and small range of water level sensors in the prior art. The first purpose of the present invention is to provide a fiber optic water level sensor device based on Mach-Zehnder interference.
为了实现上述目的,本发明采用如下一种技术方案:In order to achieve the above object, the present invention adopts the following technical scheme:
一种基于马赫-增德尔干涉的光纤水位传感装置,该装置包括:A fiber optic water level sensing device based on Mach-Zehnder interference, the device comprising:
激光器(1)、第一耦合器(2)、第一准直器(3)、第二准直器(4)、敏感结构(5)、第二耦合器(6)、光电探测器(7)和上位机解调系统(8);Laser (1), first coupler (2), first collimator (3), second collimator (4), sensitive structure (5), second coupler (6), photodetector (7 ) and host computer demodulation system (8);
所述激光器(1)的输出与所述第一耦合器(2)的输入端相连;The output of the laser (1) is connected to the input of the first coupler (2);
所述第一耦合器(2)的输出端分为两路,一路连接所述第一准直器(3)和所述第二准直器(4)后连接所述第二耦合器(6)的输入端,构成探测臂,所述敏感结构(5)用于固定所述第一准直器(3)和所述第二准直器(4)并感受水位变化,另一路连接所述第二耦合器(6)的另一个输入端,构成参考臂;The output end of the first coupler (2) is divided into two paths, one path is connected to the first collimator (3) and the second collimator (4) and then connected to the second coupler (6 ) to form the detection arm, the sensitive structure (5) is used to fix the first collimator (3) and the second collimator (4) and sense the water level change, the other way is connected to the The other input end of the second coupler (6) constitutes a reference arm;
所述第二耦合器(6)的输出端依次连接所述光电探测器(7)和上位机解调系统(8),从所述第一耦合器(2)分别经探测臂和参考臂到达所述第二耦合器(6)的结构构成马赫-增德尔干涉。The output end of the second coupler (6) is connected to the photodetector (7) and the host computer demodulation system (8) in sequence, and reaches from the first coupler (2) through the detection arm and the reference arm respectively. The structure of the second coupler (6) constitutes Mach-Zehnder interference.
进一步的,所述敏感结构(5)包括架框(10)、外接头(9)、压紧块(11)、两个焊接细管(12)、连接固定片(13)、锁紧螺钉(14)、水带(15)、夹紧片(16)、两个过渡焊片(17),所述外接头(9)通过所述架框(10)固定;Further, the sensitive structure (5) includes a frame (10), an external joint (9), a pressing block (11), two welded thin tubes (12), a connection fixing piece (13), a locking screw ( 14), hose (15), clamping piece (16), two transition welding pieces (17), the external joint (9) is fixed by the frame (10);
所述压紧块(11)压紧所述水带(15),两个过渡焊片(17)安装于所述压紧块(11)上,两个焊接细管(12)分别连接所述第一准直器(3)、所述第二准直器(4)和两个过渡焊片(17),所述连接固定片(13)的一端通过锁紧螺钉(14)固定于所述架框(10)上,另一端与所述压紧块(11)焊在一起,所述夹紧片(16)夹紧所述水带(15),实现密封。The compression block (11) compresses the water belt (15), two transition welding pieces (17) are installed on the compression block (11), and two welding thin tubes (12) are respectively connected to the The first collimator (3), the second collimator (4) and two transition welding pieces (17), one end of the connecting fixed piece (13) is fixed to the described On the frame (10), the other end is welded together with the pressing block (11), and the clamping piece (16) clamps the hose (15) to realize sealing.
进一步的,所述外接头(9)与所述水带(15)连接,水位发生变化时,水通过所述外接头(9)进入所述水带(15)。Further, the external joint (9) is connected to the water belt (15), and when the water level changes, water enters the water belt (15) through the external joint (9).
进一步的,所述压紧块(11)包括第一压紧块与第二压紧块,所述第一压紧块与所述第二压紧块分别位于所述水带两侧。Further, the pressing block (11) includes a first pressing block and a second pressing block, and the first pressing block and the second pressing block are respectively located on both sides of the hose.
进一步的,所述第一压紧块与所述第二压紧块之间的间隙可变,且根据所述水带(15)内的水量变化。Further, the gap between the first compaction block and the second compaction block is variable, and changes according to the water volume in the water belt (15).
进一步的,两个过渡焊片(17)组成第一过渡焊片组,所述敏感结构还包括第二过渡焊片组,所述第二过渡焊片组安装于所述压紧块(11)上所述第一过渡焊片组的对称侧。Further, two transition soldering pieces (17) form a first transitional welding piece group, and the sensitive structure further includes a second transitional welding piece group, and the second transitional welding piece group is installed on the pressing block (11) The symmetrical side of the above-mentioned first transition pad group.
进一步的,两个焊接细管(12)组成第一焊接细管组,所述敏感结构还包括第二焊接细管组,所述第二焊接细管组分别连接所述第一准直器(3)、所述第二准直器(4)和第二过渡焊片组中的两个过渡焊片。Further, two welded thin tubes (12) form a first welded thin tube group, and the sensitive structure also includes a second welded thin tube group, and the second welded thin tube group is respectively connected to the first collimator ( 3), the second collimator (4) and two transition pads in the second transition pad group.
进一步的,所述夹紧片(16)包括第一夹紧片和第二夹紧片,所述第一夹紧片与所述第二夹紧片分别位于所述水带两侧,所述第一夹紧片和第二夹紧片均与架框(10)连接。Further, the clamping piece (16) includes a first clamping piece and a second clamping piece, the first clamping piece and the second clamping piece are respectively located on both sides of the hose, the Both the first clamping piece and the second clamping piece are connected with the frame (10).
进一步的,所述激光器(1)采用扫频激光器。Further, the laser (1) is a frequency-swept laser.
进一步的,所述第一耦合器(2)到所述第一准直器(3)间的距离与所述第二准直器(4)到所述第二耦合器(6)的距离之和为所述第一耦合器(2)经过光纤直接到所述第二耦合器(6)的距离。Further, the distance between the first coupler (2) to the first collimator (3) and the distance from the second collimator (4) to the second coupler (6) and are the distances from the first coupler (2) directly to the second coupler (6) through the optical fiber.
该装置的工作原理为:The working principle of the device is:
所述敏感结构(5)的所述外接头(9)直接与水接触,当水位发生变化时,水通过所述外接头(9)进入所述水带(15),所述水带(15)中水变多,使所述压紧块(11)的间隙增大,所述第一准直器(3)和所述第二准直器(4)间的距离也增大,导致干涉结构中探测臂的长度发生变化,继而导致干涉信号的相位发生变化。The external joint (9) of the sensitive structure (5) is directly in contact with water, and when the water level changes, water enters the water belt (15) through the external joint (9), and the water belt (15) ) becomes more water, the gap between the pressing blocks (11) increases, and the distance between the first collimator (3) and the second collimator (4) also increases, resulting in interference The length of the probe arm changes in the structure, which in turn causes the phase of the interference signal to change.
在本发明中,采用两个准直器结构,当水位变化时,使两准直器间距改变,不受光纤拉伸量的限制,可以同时提高水位的测量精度和测量范围。有效避免了传统水位计将光纤缠绕在顺变柱体上,当水位变化时光纤被拉伸,当光纤达到拉伸极限时,橡胶柱体还可以进行弹性变化,影响水位测量精度的问题。In the present invention, two collimator structures are adopted, and when the water level changes, the distance between the two collimators is changed without being limited by the stretching amount of the optical fiber, and the measurement accuracy and measurement range of the water level can be improved at the same time. It effectively avoids the problem that the traditional water level gauge winds the optical fiber on the variable cylinder. When the water level changes, the optical fiber is stretched. When the optical fiber reaches the stretching limit, the rubber cylinder can also undergo elastic changes, which affects the accuracy of water level measurement.
在本发明中,敏感结构的外接头直接与水接触,当水位发生变化时,水通过外接头进入水带,水带中水变多,使压紧块的间隙增大,两个准直器间的距离也增大,导致干涉结构中探测臂的长度发生变化,继而导致干涉信号的相位发生变化。实现了基于马赫-增德尔干涉的光纤水位测量,提高了水位测量精度。In the present invention, the outer joint of the sensitive structure is directly in contact with the water. When the water level changes, the water enters the hose through the outer joint, and the water in the hose becomes more, which increases the gap between the pressing blocks. The two collimators The distance between them also increases, resulting in a change in the length of the detection arm in the interferometric structure, which in turn causes a change in the phase of the interferometric signal. The optical fiber water level measurement based on Mach-Zehnder interference is realized, and the accuracy of water level measurement is improved.
本发明的第二目的是提供一种基于马赫-增德尔干涉的光纤水位传感方法。The second object of the present invention is to provide an optical fiber water level sensing method based on Mach-Zehnder interference.
为了实现上述目的,本发明采用如下一种技术方案:In order to achieve the above object, the present invention adopts the following technical scheme:
一种基于马赫-增德尔干涉的光纤水位传感方法,该方法基于上述一种基于马赫-增德尔干涉的光纤水位传感装置,该方法包括以下步骤:An optical fiber water level sensing method based on Mach-Zender interference, the method is based on the above-mentioned optical fiber water level sensing device based on Mach-Zender interference, the method comprises the following steps:
(1)获取激光器(1)的起始频率、扫描步进频率与工作时间,计算扫描频率,分别计算所述第一耦合器(2)输出两路光信号经过探测臂和参考臂的输出场强;(1) Obtain the initial frequency, scanning step frequency and working time of the laser (1), calculate the scanning frequency, and calculate the output fields of the first coupler (2) outputting two optical signals through the detection arm and the reference arm respectively powerful;
(2)根据探测臂的输出场强和参考臂的输出场强分别计算探测臂的输出光强和参考臂的输出光强,根据探测臂的输出光强和参考臂的输出光强计算探测臂和参考臂的干涉光强,由此计算出所述第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差;将相位差对时间微分,计算得到第一准直器(3)和第二准直器(4)间的距离;(2) Calculate the output light intensity of the detection arm and the output light intensity of the reference arm according to the output field strength of the detection arm and the output field strength of the reference arm, and calculate the detection arm according to the output light intensity of the detection arm and the output light intensity of the reference arm and the interference light intensity of the reference arm, thereby calculating the phase difference of the two optical signals output by the first coupler (2) after passing through the detection arm and the reference arm; the phase difference is differentiated to time, and the first collimation is calculated The distance between the device (3) and the second collimator (4);
(3)根据第一准直器(3)和第二准直器(4)间的距离,结合水位的压强公式和水位的压强与第一准直器(3)和第二准直器(4)间的距离的关系,最终计算出当前的水位值。(3) according to the distance between the first collimator (3) and the second collimator (4), combine the pressure formula of the water level and the pressure of the water level with the first collimator (3) and the second collimator ( 4) The relationship between the distance between them, and finally calculate the current water level value.
进一步的,所述步骤(1)中探测臂的输出场强E1为:Further, the output field strength E of the detection arm in the step (1) is:
其中,E0为常量,f0为激光器(1)的起始频率,k为激光器(1)的扫描步进频率,t为激光器(1)的扫频时间,n为折射率,C为光速,为第一耦合器(2)输出光信号的初始相位,L1为第一耦合器到第一准直器间的距离,L2为第二准直器到第二耦合器的距离,ΔL为两个准直器间的距离,ΔL为待计算的变量。Among them, E 0 is a constant, f 0 is the initial frequency of the laser (1), k is the scanning step frequency of the laser (1), t is the sweep time of the laser (1), n is the refractive index, and C is the speed of light , is the initial phase of the output optical signal of the first coupler (2), L 1 is the distance between the first coupler and the first collimator, L 2 is the distance from the second collimator to the second coupler, ΔL is The distance between the two collimators, ΔL is the variable to be calculated.
进一步的,所述步骤(1)中参考臂的输出场强E2为:Further, the output field strength E of the reference arm in the step (1) is:
其中,E0为常量,f0为激光器(1)的起始频率,k为激光器(1)的扫描步进频率,t为激光器(1)的扫频时间,n为折射率,C为光速,为第一耦合器(2)输出光信号的初始相位,L3为第一耦合器(2)经过光纤直接到第二耦合器(6)的距离。Among them, E 0 is a constant, f 0 is the initial frequency of the laser (1), k is the scanning step frequency of the laser (1), t is the sweep time of the laser (1), n is the refractive index, and C is the speed of light , is the initial phase of the optical signal output by the first coupler (2), and L3 is the distance from the first coupler (2) directly to the second coupler (6) through the optical fiber.
进一步的,所述步骤(2)中计算出所述第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差的具体步骤为:Further, in the step (2), the specific steps for calculating the phase difference of the two optical signals output by the first coupler (2) after passing through the detection arm and the reference arm are as follows:
探测臂和参考臂的干涉光强I为:The interference light intensity I of the detection arm and the reference arm is:
其中,I1为探测臂的输出光强,I2为参考臂的输出光强,为第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差;Among them, I 1 is the output light intensity of the detection arm, I 2 is the output light intensity of the reference arm, Outputting the phase difference between the two optical signals passing through the detection arm and the reference arm for the first coupler (2);
根据探测臂和参考臂的干涉光强I得到探测臂和参考臂的干涉光强I的交流项信号I′为:According to the interference light intensity I of the detection arm and the reference arm, the AC term signal I′ of the interference light intensity I of the detection arm and the reference arm is obtained as:
对离散化的探测臂和参考臂的干涉光强I的交流项信号I′做希尔伯特变换,得到第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差为:Hilbert transform is performed on the AC term signal I′ of the interference light intensity I of the discretized detection arm and the reference arm, and the phase difference between the two optical signals output by the first coupler (2) after passing through the detection arm and the reference arm is obtained. for:
进一步的,所述步骤(2)中第一准直器(3)和第二准直器(4)间的距离为ΔL:Further, the distance between the first collimator (3) and the second collimator (4) in the step (2) is ΔL:
其中,为第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差/>对扫频时间t的微分。in, The first coupler (2) outputs the phase difference of the two optical signals after passing through the detection arm and the reference arm /> Differentiation with respect to sweep time t.
进一步的,所述步骤(2)中第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差对扫频时间t的微分/>的计算方法为:Further, in the step (2), the first coupler (2) outputs the phase difference of the two optical signals after passing through the detection arm and the reference arm Differentiation with respect to sweep time t /> The calculation method is:
根据第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差做相位解缠绕,并计算出相位差/>与扫频时间t的关系;According to the phase difference of the two optical signals output by the first coupler (2) after passing through the detection arm and the reference arm Do phase unwrapping and calculate the phase difference /> The relationship with the sweep time t;
对相位差与扫频时间t做曲线拟合,根据拟合出的曲线得到拟合曲线的斜率,即为/> phase difference Do curve fitting with the frequency sweep time t, and get the slope of the fitting curve according to the fitted curve, which is />
进一步的,所述步骤(3)中的具体步骤为:Further, the specific steps in the step (3) are:
水位的压强公式为:The formula for water level pressure is:
P=ρghP = ρgh
其中,ρ为水的密度,g为重力加速度,h为当前水位值;Among them, ρ is the density of water, g is the acceleration of gravity, and h is the current water level;
水位的压强与第一准直器(3)和第二准直器(4)间的距离的关系为:The relationship between the pressure of the water level and the distance between the first collimator (3) and the second collimator (4) is:
P=C1×ΔLP=C 1 ×ΔL
其中,C1为机械结构决定的常量;Among them, C 1 is a constant determined by the mechanical structure;
结合水位的压强公式和水位的压强与第一准直器(3)和第二准直器(4)间的距离的关系,最终计算出当前的水位值h为:Combining the pressure formula of the water level and the relationship between the pressure of the water level and the distance between the first collimator (3) and the second collimator (4), the current water level value h is finally calculated as:
进一步的,当前的水位值h的测量范围由相位差与扫频时间t做曲线拟合后的拟合曲线斜率/>和扫描步进频率k来决定:Further, the measurement range of the current water level value h is determined by the phase difference The slope of the fitting curve after curve fitting with the sweep time t and scan step frequency k to determine:
单位时间内最大改变量为2π,则第一准直器(3)和第二准直器(4)间的距离ΔL最大值为/>单位时间内最小改变量为2π/N,其中N为扫描步进次数,则第一准直器(3)和第二准直器(4)间的距离ΔL最小值为/>因此水位h的测量范围为/> The maximum amount of change per unit time is 2π, then the maximum distance ΔL between the first collimator (3) and the second collimator (4) is /> The minimum amount of change per unit time is 2π/N, where N is the number of scanning steps, then the minimum distance ΔL between the first collimator (3) and the second collimator (4) is /> Therefore the measurement range of the water level h is />
理论上,频率步进次数N取值可以无穷大,激光器(1)的扫描步进频率k的取值可以无穷小,因此,本发明可以进一步提高水位的测量范围。Theoretically, the number of frequency steps N can be infinitely large, and the value of the scanning step frequency k of the laser (1) can be infinitely small. Therefore, the present invention can further increase the measurement range of the water level.
进一步的,当前的水位值h的测量精度由激光器(1)的扫描步进次数N决定:Further, the measurement accuracy of the current water level value h Determined by the number of scanning steps N of the laser (1):
本发明的有益效果:Beneficial effects of the present invention:
(1)本发明的一种基于马赫-增德尔干涉的光纤水位传感装置,采用两个准直器结构,当水位变化时,使两准直器间距改变,不受光纤拉伸量的限制,可以同时提高水位的测量精度和测量范围。本发明有效避免了传统水位计将光纤缠绕在顺变柱体上,当水位变化时光纤被拉伸,但是当光纤达到拉伸极限时,橡胶柱体还可以进行弹性变化,影响水位测量精度的问题。(1) A fiber optic water level sensing device based on Mach-Zehnder interference of the present invention adopts two collimator structures, and when the water level changes, the distance between the two collimators is changed without being limited by the stretching amount of the optical fiber , can simultaneously improve the measurement accuracy and measurement range of the water level. The invention effectively avoids the problem that the traditional water level gauge winds the optical fiber on the variable cylinder. When the water level changes, the optical fiber is stretched. However, when the optical fiber reaches the stretching limit, the rubber cylinder can also undergo elastic changes, which affects the accuracy of water level measurement. .
(2)本发明的一种基于马赫-增德尔干涉的光纤水位传感装置,敏感结构的外接头直接与水接触,当水位发生变化时,水通过外接头进入水带,水带中水变多,使压紧块的间隙增大,两个准直器间的距离也增大,导致干涉结构中探测臂的长度发生变化,继而导致干涉信号的相位发生变化。实现了基于马赫-增德尔干涉的光纤水位测量,提高了水位测量精度。(2) A kind of optical fiber water level sensing device based on Mach-Zehnder interference of the present invention, the external joint of sensitive structure directly contacts with water, when water level changes, water enters water belt through external joint, and the water in the water belt changes If there are too many, the gap between the pressing blocks will increase, and the distance between the two collimators will also increase, resulting in a change in the length of the detection arm in the interference structure, which in turn leads to a change in the phase of the interference signal. The optical fiber water level measurement based on Mach-Zehnder interference is realized, and the accuracy of water level measurement is improved.
(3)本发明的一种基于马赫-增德尔干涉的光纤水位传感方法,根据一种基于马赫-增德尔干涉的光纤水位传感装置计算出的当前的水位值的测量范围由相位拟合后的斜率和扫描步进频率k决定;/>单位时间内最大改变量为2π,则ΔL的最大值为/>单位时间内最小改变量为2π/N,则ΔL最小值为/>理论上,频率步进次数N取值可以无穷大,扫描步进频率k的取值可以无穷小,本发明可以进一步提高水位的测量范围。(3) A kind of optical fiber water level sensing method based on Mach-Zender interference of the present invention, according to a kind of measuring range of the current water level value calculated by the optical fiber water level sensing device based on Mach-Zender interference by phase fitting slope after and scan step frequency k decision; /> The maximum change in unit time is 2π, then the maximum value of ΔL is /> The minimum change in unit time is 2π/N, then the minimum value of ΔL is /> Theoretically, the value of the frequency step frequency N can be infinite, and the value of the scanning step frequency k can be infinitely small, and the present invention can further increase the measurement range of the water level.
附图说明Description of drawings
图1为本发明的一种基于马赫-增德尔干涉的光纤水位传感装置的结构图;Fig. 1 is the structural diagram of a kind of optical fiber water level sensing device based on Mach-Zehnder interference of the present invention;
图2为本发明的一种基于马赫-增德尔干涉的光纤水位传感装置的系统框图;Fig. 2 is a system block diagram of an optical fiber water level sensing device based on Mach-Zender interference of the present invention;
图3为本发明的一种基于马赫-增德尔干涉的光纤水位传感装置中敏感结构的结构图;Fig. 3 is a structural diagram of a sensitive structure in an optical fiber water level sensing device based on Mach-Zehnder interference of the present invention;
图4为本发明的一种基于马赫-增德尔干涉的光纤水位传感装置中敏感结构的剖面图;Fig. 4 is a sectional view of a sensitive structure in an optical fiber water level sensing device based on Mach-Zehnder interference of the present invention;
图5为本发明的一种基于马赫-增德尔干涉的光纤水位传感方法的流程图。Fig. 5 is a flow chart of an optical fiber water level sensing method based on Mach-Zehnder interference of the present invention.
其中,1.激光器,2.第一耦合器,3.第一准直器,4.第二准直器,5.敏感结构,6.第二耦合器,7.光电探测器,8.上位机解调系统,9.外接头,10.架框,11.压紧块,12.焊接细管,13.连接固定片,14.锁紧螺钉,15.水带,16.夹紧片,17.过渡焊片。Among them, 1. Laser, 2. First coupler, 3. First collimator, 4. Second collimator, 5. Sensitive structure, 6. Second coupler, 7. Photodetector, 8. Upper Machine demodulation system, 9. Outer joint, 10. Frame, 11. Compression block, 12. Welded thin tube, 13. Connection fixing piece, 14. Locking screw, 15. Water belt, 16. Clamping piece, 17. Transition solder tabs.
具体实施方式:Detailed ways:
应该指出,以下详细说明都是例示性的,旨在对本申请提供进一步的说明。除非另有指明,本文使用的所有技术和科学术语具有与本申请所属技术领域的普通技术人员通常理解的相同含义。It should be pointed out that the following detailed description is exemplary and intended to provide further explanation to the present application. Unless defined otherwise, all technical and scientific terms used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this application belongs.
需要注意的是,这里所使用的术语仅是为了描述具体实施方式,而非意图限制根据本申请的示例性实施方式。如在这里所使用的,除非上下文另外明确指出,否则单数形式也意图包括复数形式,此外,还应当理解的是,当在本说明书中使用术语“包含”和/或“包括”时,其指明存在特征、步骤、操作、器件、组件和/或它们的组合。It should be noted that the terminology used here is only for describing specific implementations, and is not intended to limit the exemplary implementations according to the present application. As used herein, unless the context clearly dictates otherwise, the singular is intended to include the plural, and it should also be understood that when the terms "comprising" and/or "comprising" are used in this specification, they mean There are features, steps, operations, means, components and/or combinations thereof.
在不冲突的情况下,本申请中的实施例及实施例中的特征可以相互组合。下面结合附图与实施例对本发明作进一步说明。In the case of no conflict, the embodiments in the present application and the features in the embodiments can be combined with each other. The present invention will be further described below in conjunction with the accompanying drawings and embodiments.
实施例1:Example 1:
正如背景技术所介绍的,本发明为了解决上述问题,克服现有技术中存在的水位传感器测量精度低、范围小的问题,本发明的第一目的是提供一种基于马赫-增德尔干涉的光纤水位传感装置。As introduced in the background technology, in order to solve the above problems, the present invention overcomes the problems of low measurement accuracy and small range of water level sensors in the prior art. The first purpose of the present invention is to provide an optical fiber based on Mach-Zehnder interference Water level sensing device.
为了实现上述目的,本发明采用如下一种技术方案:In order to achieve the above object, the present invention adopts the following technical scheme:
如图1所示,As shown in Figure 1,
一种基于马赫-增德尔干涉的光纤水位传感装置,该装置包括:A fiber optic water level sensing device based on Mach-Zehnder interference, the device comprising:
激光器(1)、第一耦合器(2)、第一准直器(3)、第二准直器(4)、敏感结构(5)、第二耦合器(6)、光电探测器(7)、上位机解调系统(8)。Laser (1), first coupler (2), first collimator (3), second collimator (4), sensitive structure (5), second coupler (6), photodetector (7 ), PC demodulation system (8).
其中,敏感结构(5)用于固定两个准直器,如图3和图4所示,包括外接头(9)、架框(10)、压紧块(11)、两个焊接细管(12)、连接固定片(13)、锁紧螺钉(14)、水带(15)、夹紧片(16)、两个过渡焊片(17)。外接头(9)与其他部分通过架框(10)连接,压紧块(11)压紧水带(15),两个焊接细管(12)分别连接两个准直器和两个过渡焊片(17),连接固定片(13)的一端通过锁紧螺钉(14)固定,另一端与压紧块(11)焊在一起,夹紧片(16)夹紧水带(15),实现密封,过渡焊片(17)安装在压紧块(11)上。Among them, the sensitive structure (5) is used to fix the two collimators, as shown in Figure 3 and Figure 4, including the external joint (9), the frame (10), the pressing block (11), two welded thin tubes (12), connecting the fixed piece (13), the locking screw (14), the hose (15), the clamping piece (16), and two transition welding pieces (17). The outer joint (9) is connected with other parts through the frame (10), the compression block (11) compresses the hose (15), and the two welding thin tubes (12) are respectively connected to two collimators and two transition welding piece (17), one end connected to the fixed piece (13) is fixed by a locking screw (14), the other end is welded together with the pressing block (11), and the clamping piece (16) clamps the hose (15) to realize For sealing, the transition welding piece (17) is installed on the compression block (11).
所述外接头(9)与所述水带(15)连接,水位发生变化时,水通过所述外接头(9)进入所述水带(15)。The external joint (9) is connected to the water belt (15), and when the water level changes, water enters the water belt (15) through the external joint (9).
所述压紧块(11)包括第一压紧块与第二压紧块,所述第一压紧块与所述第二压紧块分别位于所述水带两侧。The pressing block (11) includes a first pressing block and a second pressing block, and the first pressing block and the second pressing block are respectively located on two sides of the hose.
所述第一压紧块与所述第二压紧块之间的间隙可变,且根据所述水带(15)内的水量变化。The gap between the first compacting block and the second compacting block is variable and varies according to the water volume in the hose (15).
两个过渡焊片(17)组成第一过渡焊片组,所述敏感结构还包括第二过渡焊片组,所述第二过渡焊片组安装于所述压紧块(11)上所述第一过渡焊片组的对称侧。Two transition soldering pieces (17) form a first transitional welding piece group, and the sensitive structure also includes a second transitional welding piece group, and the second transitional welding piece group is installed on the pressing block (11). The symmetrical side of the first transition pad set.
两个焊接细管(12)组成第一焊接细管组,所述敏感结构还包括第二焊接细管组,所述第二焊接细管组分别连接所述第一准直器(3)、所述第二准直器(4)和第二过渡焊片组中的两个过渡焊片。Two welded thin tubes (12) form a first welded thin tube group, and the sensitive structure also includes a second welded thin tube group, and the second welded thin tube group is respectively connected to the first collimator (3), The second collimator (4) and the two transition pads in the second transition pad set.
所述夹紧片(16)包括第一夹紧片和第二夹紧片,所述第一夹紧片与所述第二夹紧片分别位于所述水带两侧,所述第一夹紧片和第二夹紧片均与架框(10)连接。The clamping piece (16) includes a first clamping piece and a second clamping piece, the first clamping piece and the second clamping piece are respectively located on both sides of the hose, and the first clamping piece Both the tight piece and the second clamping piece are connected with the frame (10).
敏感结构(5)的外接头(9)直接与水接触,当水位发生变化时,水通过外接头(9)进入水带(15),水带(15)中水变多,使压紧块(11)的间隙增大,两个准直器间的距离也增大,导致干涉结构中探测臂的长度发生变化,继而导致干涉信号的相位发生变化。The outer joint (9) of the sensitive structure (5) is directly in contact with the water, and when the water level changes, the water enters the hose (15) through the outer joint (9), and the water in the hose (15) becomes more, causing the pressing block to As the gap of (11) increases, the distance between the two collimators also increases, resulting in a change in the length of the detection arm in the interference structure, which in turn leads to a change in the phase of the interference signal.
如图1和图2所示,激光器(1)的输出与第一耦合器(2)的输入端相连,第一耦合器(2)的输出端分为两路,一路连接第一准直器(3)和第二准直器(4)后接第二耦合器(6)的输入端,构成探测臂,敏感结构(5)用来固定两个准直器并可以感受水位变化,另一路直接连接第二耦合器(6)的另一个输入端,构成参考臂,第二耦合器(6)的输出端接光电探测器(7),从第一耦合器分别经探测臂和参考臂到达第二耦合器的结构构成马赫-增德尔干涉,光电探测器(7)再连接到上位机解调系统(8)。As shown in Figures 1 and 2, the output of the laser (1) is connected to the input of the first coupler (2), and the output of the first coupler (2) is divided into two paths, one of which is connected to the first collimator (3) and the second collimator (4) are connected to the input end of the second coupler (6) to form a detection arm. The sensitive structure (5) is used to fix the two collimators and can feel the water level change. The other input end of the second coupler (6) is directly connected to form a reference arm, and the output end of the second coupler (6) is connected to the photodetector (7), and the first coupler reaches through the detection arm and the reference arm respectively. The structure of the second coupler constitutes Mach-Zehnder interference, and the photodetector (7) is connected to the host computer demodulation system (8).
实施例2:Example 2:
本发明的第二目的是提供一种基于马赫-增德尔干涉的光纤水位传感方法。The second object of the present invention is to provide an optical fiber water level sensing method based on Mach-Zehnder interference.
为了实现上述目的,本发明采用如下一种技术方案:In order to achieve the above object, the present invention adopts the following technical scheme:
如图5所示,As shown in Figure 5,
一种基于马赫-增德尔干涉的光纤水位传感方法,该方法基于上述一种基于马赫-增德尔干涉的光纤水位传感装置,该方法包括以下步骤:An optical fiber water level sensing method based on Mach-Zender interference, the method is based on the above-mentioned optical fiber water level sensing device based on Mach-Zender interference, the method comprises the following steps:
(1)获取激光器(1)的起始频率、扫描步进频率与工作时间,计算扫描频率,分别计算所述第一耦合器(2)输出两路光信号经过探测臂和参考臂的输出场强;(1) Obtain the initial frequency, scanning step frequency and working time of the laser (1), calculate the scanning frequency, and calculate the output fields of the first coupler (2) outputting two optical signals through the detection arm and the reference arm respectively powerful;
(2)根据探测臂的输出场强和参考臂的输出场强分别计算探测臂的输出光强和参考臂的输出光强,根据探测臂的输出光强和参考臂的输出光强计算探测臂和参考臂的干涉光强,由此计算出所述第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差;将相位差对时间微分,计算得到第一准直器(3)和第二准直器(4)间的距离;(2) Calculate the output light intensity of the detection arm and the output light intensity of the reference arm according to the output field strength of the detection arm and the output field strength of the reference arm, and calculate the detection arm according to the output light intensity of the detection arm and the output light intensity of the reference arm and the interference light intensity of the reference arm, thereby calculating the phase difference of the two optical signals output by the first coupler (2) after passing through the detection arm and the reference arm; the phase difference is differentiated to time, and the first collimation is calculated The distance between the device (3) and the second collimator (4);
(3)根据第一准直器(3)和第二准直器(4)间的距离,结合水位的压强公式和水位的压强与第一准直器(3)和第二准直器(4)间的距离的关系,最终计算出当前的水位值。(3) according to the distance between the first collimator (3) and the second collimator (4), combine the pressure formula of the water level and the pressure of the water level with the first collimator (3) and the second collimator ( 4) The relationship between the distance between them, and finally calculate the current water level value.
在本实施例中,具体的方法步骤为:In this embodiment, the specific method steps are:
一种基于马赫-增德尔干涉的光纤水位传感装置中的激光器(1)采用扫频激光器,激光器(1)的起始频率记为f0,激光器(1)的扫描频率记为f,且:The laser (1) in an optical fiber water level sensing device based on Mach-Zehnder interference adopts a frequency-sweeping laser, the starting frequency of the laser (1) is denoted as f 0 , the scanning frequency of the laser (1) is denoted as f, and :
f=f0+ktf=f 0 +kt
其中k为激光器(1)的扫描步进频率,t为激光器(1)的扫频时间。Where k is the scanning step frequency of the laser (1), and t is the frequency scanning time of the laser (1).
在本实施例中,激光器(1)的起始频率f0为191200GHz,激光器(1)的扫描步进频率k为1GHz,激光器(1)的扫描频率f为:In the present embodiment, the starting frequency f of the laser (1) is 191200GHz , the scanning step frequency k of the laser (1) is 1GHz, and the scanning frequency f of the laser (1) is:
f=191200GHz+1GHz×tf=191200GHz+1GHz×t
第一耦合器(2)到第一准直器(3)间的距离为L1,两个准直器间的距离即第一准直器(3)和第二准直器(4)间的距离为ΔL,第二准直器(4)到第二耦合器(6)的距离为L2,从第一耦合器(2)经过光纤直接到第二耦合器(6)的距离为L3,且L1+L2=L3。The distance between the first coupler (2) and the first collimator (3) is L 1 , the distance between the two collimators is the distance between the first collimator (3) and the second collimator (4) The distance is ΔL, the distance from the second collimator (4) to the second coupler (6) is L 2 , and the distance from the first coupler (2) directly to the second coupler (6) through the optical fiber is L 3 , and L 1 +L 2 =L 3 .
第一耦合器(2)输出两路光信号,分别经过探测臂和参考臂,其场强表达式分别为:The first coupler (2) outputs two optical signals, which pass through the detection arm and the reference arm respectively, and their field strength expressions are respectively:
其中E1为探测臂的输出场强,E2为参考臂的输出场强,E0为常量,n为折射率,C为光速,为第一耦合器(2)输出光信号的初始相。where E1 is the output field strength of the detection arm, E2 is the output field strength of the reference arm, E0 is a constant, n is the refractive index, C is the speed of light, The initial phase of the output optical signal for the first coupler (2).
在本实施例中,将激光器(1)的起始频率f0为191200GHz,激光器(1)的扫描步进频率k为1GHz代入探测臂的输出场强E1和参考臂的输出场强E2的计算公式:In the present embodiment, the starting frequency f0 of the laser (1) is 191200GHz, and the scanning step frequency k of the laser (1) is 1GHz and substituted into the output field strength E1 of the detection arm and the output field strength E2 of the reference arm The formula for calculating:
探测臂和参考臂的干涉光强为:The interference light intensity of the detection arm and the reference arm is:
其中I1为探测臂的输出光强,I2为参考臂的输出光强,为第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差。Where I 1 is the output light intensity of the detection arm, I 2 is the output light intensity of the reference arm, The first coupler (2) outputs the phase difference of the two optical signals after passing through the detection arm and the reference arm.
干涉光强的交流项信号为:The AC term signal of interference light intensity is:
对离散化的探测臂和参考臂的干涉光强I的交流项信号I′做希尔伯特变换,得到第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差为:Hilbert transform is performed on the AC term signal I′ of the interference light intensity I of the discretized detection arm and the reference arm, and the phase difference between the two optical signals output by the first coupler (2) after passing through the detection arm and the reference arm is obtained. for:
在本实施例中,将激光器(1)的起始频率f0为191200GHz,激光器(1)的扫描步进频率k为1GHz代入上述公式:In the present embodiment, the starting frequency f of the laser (1) is 191200GHz, and the scanning step frequency k of the laser (1) is 1GHz and is substituted into the above formula:
第一耦合器(2)输出两路光信号经过探测臂和参考臂后的相位差随扫频时间t改变,对扫频时间t做微分可得:The first coupler (2) outputs the phase difference of the two optical signals after passing through the detection arm and the reference arm As the sweep time t changes, we can differentiate the sweep time t to get:
在本实施例中,In this example,
因此两准直器间的距离为:So the distance between the two collimators is:
在本实施例中,In this example,
其中,的计算方法如下:in, The calculation method is as follows:
首先对离散化的I′做希尔伯特变换,并得到相位值由于相位在π处发生跳边,为了得到真实的相位变化,做相位解缠绕并计算出相位与扫频时间的关系,再对相位值和扫频时间做曲线拟合,得到拟合曲线的斜率,即为/> First, do a Hilbert transform on the discretized I′, and get the phase value Since the phase jumps at π, in order to obtain the real phase change, do phase unwrapping and calculate the relationship between phase and sweep time, and then do curve fitting on the phase value and sweep time to get the slope of the fitting curve , which is />
水位的压强公式为:The formula for water level pressure is:
P=ρghP = ρgh
其中ρ为水的密度,g为重力加速度,h为当前水位值。Where ρ is the density of water, g is the acceleration of gravity, and h is the current water level.
水位的压强与两准直器间距ΔL的关系为:The relationship between the pressure of the water level and the distance ΔL between the two collimators is:
P=C1×ΔLP=C 1 ×ΔL
其中C1为机械结构决定的常量。Among them, C 1 is a constant determined by the mechanical structure.
则当前水位值h为:Then the current water level value h is:
水位的测量范围由相位拟合后的斜率和扫描步进频率k来决定:The measurement range of water level is determined by the slope after phase fitting and scan step frequency k to determine:
单位时间内最大改变量为2π,则ΔL最大值为/>单位时间内最小改变量为2π/N,其中N=5000为频率步进次数,则ΔL最小值为/>因此水位h的测量范围为/> The maximum change in unit time is 2π, then the maximum value of ΔL is /> The minimum amount of change per unit time is 2π/N, where N=5000 is the number of frequency steps, then the minimum value of ΔL is /> Therefore the measurement range of the water level h is />
水位的测量精度由扫描步进次数决定:Water level measurement accuracy Determined by the number of scan steps:
以上所述仅为本申请的优选实施例而已,并不用于限制本申请,对于本领域的技术人员来说,本申请可以有各种更改和变化。凡在本申请的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本申请的保护范围之内。The above descriptions are only preferred embodiments of the present application, and are not intended to limit the present application. For those skilled in the art, there may be various modifications and changes in the present application. Any modifications, equivalent replacements, improvements, etc. made within the spirit and principles of this application shall be included within the protection scope of this application.
Claims (8)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710613811.2A CN107402054B (en) | 2017-07-25 | 2017-07-25 | Optical fiber water level sensing device and method based on Mach-Zehnder interference |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710613811.2A CN107402054B (en) | 2017-07-25 | 2017-07-25 | Optical fiber water level sensing device and method based on Mach-Zehnder interference |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107402054A CN107402054A (en) | 2017-11-28 |
CN107402054B true CN107402054B (en) | 2023-08-15 |
Family
ID=60402449
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201710613811.2A Expired - Fee Related CN107402054B (en) | 2017-07-25 | 2017-07-25 | Optical fiber water level sensing device and method based on Mach-Zehnder interference |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107402054B (en) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109211356B (en) * | 2018-11-09 | 2023-10-10 | 珠海任驰光电科技有限公司 | Optical fiber interference water level sensor and sensing method based on frequency shift technology |
CN110646020B (en) * | 2019-10-30 | 2023-01-24 | 电子科技大学中山学院 | Optical fiber interference device and method |
CN111561910B (en) * | 2020-05-27 | 2022-03-11 | 珠海任驰光电科技有限公司 | Optical fiber interferometric sedimentation instrument, system and measurement method with adjustable pressure difference range |
Citations (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0188393A1 (en) * | 1985-01-09 | 1986-07-23 | Kabushiki Kaisha TOPCON | Liquid level height-measuring apparatus |
US4678909A (en) * | 1984-03-31 | 1987-07-07 | Kent Scientific And Industrial Projects Limited | Optical pressure sensing apparatus |
US5721615A (en) * | 1993-07-12 | 1998-02-24 | The Secretary Of State For Defense In Her Britannic Majesty's Government Of The United Kingdom Of Great Britain And Northern Ireland | Sensor system for measurement of temperature or strain |
CN101614607A (en) * | 2009-07-31 | 2009-12-30 | 武汉光子科技有限公司 | Optical fiber F-P pressure sensor and pressure liquid level sensing device thereof |
CN102069252A (en) * | 2010-11-25 | 2011-05-25 | 天津市天发重型水电设备制造有限公司 | Method for manufacturing pole coil |
CN103697954A (en) * | 2013-12-27 | 2014-04-02 | 电子科技大学 | Micro-cavity interference flow velocity differential-pressure-sensitive structure and flow velocity and quantity sensor with micro-cavity interference fiber |
CN104697609A (en) * | 2015-03-24 | 2015-06-10 | 吉林大学 | Optical fiber interference water level sensor |
CN205138602U (en) * | 2015-11-20 | 2016-04-06 | 武汉新烽光电股份有限公司 | Optic fibre liquid level measurement device of light path is received to two bills |
CN105758567A (en) * | 2016-04-21 | 2016-07-13 | 吉林大学 | Fiber interference type pressure sensor based on 3*3 coupler |
CN205655954U (en) * | 2016-05-16 | 2016-10-19 | 珠海任驰光电科技有限公司 | Optic fibre hydraulic pressure sensor based on mach - increase dare to interfere |
CN106841680A (en) * | 2017-03-30 | 2017-06-13 | 吉林大学 | A kind of optical fiber interference type detector device with collimater |
CN206930335U (en) * | 2017-07-25 | 2018-01-26 | 吉林大学 | A kind of optical fiber level sensing device for increasing Dare interference based on Mach |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US20040093939A1 (en) * | 2002-11-14 | 2004-05-20 | Arias Herman Diaz | Non-contact level detector for fluids in a container |
-
2017
- 2017-07-25 CN CN201710613811.2A patent/CN107402054B/en not_active Expired - Fee Related
Patent Citations (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4678909A (en) * | 1984-03-31 | 1987-07-07 | Kent Scientific And Industrial Projects Limited | Optical pressure sensing apparatus |
EP0188393A1 (en) * | 1985-01-09 | 1986-07-23 | Kabushiki Kaisha TOPCON | Liquid level height-measuring apparatus |
US5721615A (en) * | 1993-07-12 | 1998-02-24 | The Secretary Of State For Defense In Her Britannic Majesty's Government Of The United Kingdom Of Great Britain And Northern Ireland | Sensor system for measurement of temperature or strain |
CN101614607A (en) * | 2009-07-31 | 2009-12-30 | 武汉光子科技有限公司 | Optical fiber F-P pressure sensor and pressure liquid level sensing device thereof |
CN102069252A (en) * | 2010-11-25 | 2011-05-25 | 天津市天发重型水电设备制造有限公司 | Method for manufacturing pole coil |
CN103697954A (en) * | 2013-12-27 | 2014-04-02 | 电子科技大学 | Micro-cavity interference flow velocity differential-pressure-sensitive structure and flow velocity and quantity sensor with micro-cavity interference fiber |
CN104697609A (en) * | 2015-03-24 | 2015-06-10 | 吉林大学 | Optical fiber interference water level sensor |
CN205138602U (en) * | 2015-11-20 | 2016-04-06 | 武汉新烽光电股份有限公司 | Optic fibre liquid level measurement device of light path is received to two bills |
CN105758567A (en) * | 2016-04-21 | 2016-07-13 | 吉林大学 | Fiber interference type pressure sensor based on 3*3 coupler |
CN205655954U (en) * | 2016-05-16 | 2016-10-19 | 珠海任驰光电科技有限公司 | Optic fibre hydraulic pressure sensor based on mach - increase dare to interfere |
CN106841680A (en) * | 2017-03-30 | 2017-06-13 | 吉林大学 | A kind of optical fiber interference type detector device with collimater |
CN206930335U (en) * | 2017-07-25 | 2018-01-26 | 吉林大学 | A kind of optical fiber level sensing device for increasing Dare interference based on Mach |
Non-Patent Citations (1)
Title |
---|
Fiber-Optic Michelson Interferometric Acoustic Sensor Based on a PP/PET Diaphragm;Li Liu;IEEE;第16卷(第9期);第3054-3058页 * |
Also Published As
Publication number | Publication date |
---|---|
CN107402054A (en) | 2017-11-28 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN201155991Y (en) | A New Fiber Bragg Grating Acceleration Sensor | |
CN201892569U (en) | High-sensitivity and low-frequency vibrating sensor based on MMF-TFBG optical fiber structure | |
CN101949685B (en) | Fiber laser self-mixing interferometer and measurement method thereof | |
CN103697954B (en) | A kind of microcavity interference flow velocity pressure reduction sensitive structure and microcavity interference flow velocity of optical flow transducer | |
CN106153978B (en) | Measuring Method of Flow Velocity Based on Optical Fiber MEMS Faber Microcavity | |
CN104390694B (en) | Cladded-fiber grating vibration senses instrument | |
CN107402054B (en) | Optical fiber water level sensing device and method based on Mach-Zehnder interference | |
CN109141491A (en) | Pressure-type optical fiber is slightly variable sensor | |
CN101625258A (en) | Optical fiber vibration sensing system based on Mach-Zehnder interferometer and sensing method | |
CN111854923B (en) | Acoustic wave measurement system, cantilever beam type optical fiber acoustic wave sensor demodulation system and method | |
CN105890679A (en) | Optical fiber Fabry-Perot type flow measuring device with local bending for flow guiding and measuring method | |
CN104833314B (en) | A kind of fiber optic high-resolution strain transducer and measuring method | |
CN103454034B (en) | Optical fiber micrometric displacement air pressure measuring apparatus | |
CN206930335U (en) | A kind of optical fiber level sensing device for increasing Dare interference based on Mach | |
CN107314888B (en) | Polarization performance measurement method of multifunctional lithium niobate integrated device | |
CN111579816A (en) | Acceleration Measuring Instrument Based on Photoelectric Oscillator | |
CN108896837B (en) | Integrated optical waveguide three-dimensional electric field sensor system | |
Bock et al. | Highly sensitive fiber-optic sensor for dynamic pressure measurements | |
CN1587946A (en) | Optical fiber vibrative sensor based on optical fiber raster | |
CN205607417U (en) | Disturbance signal measurement device of distributed optical fiber M -Z interferometer | |
CN201688838U (en) | Temperature insensitive type fiber grating tilt sensor | |
CN104614093B (en) | Bending-insensitive distributed Brillouin optical fiber temperature and strain sensor | |
CN107631814B (en) | Optical self-coherent sensing optical path structure, frequency shift change detection method and sensing device | |
CN202075306U (en) | FBG (fiber bragg grating) acceleration transducer based on tapered structure | |
CN101825435A (en) | All-fiber-optic displacement measuring method and device thereof |
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 | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20230815 |