[go: up one dir, main page]

CN109856057B - Liquid composition detection device and method using tapered optical fiber as medium - Google Patents

Liquid composition detection device and method using tapered optical fiber as medium Download PDF

Info

Publication number
CN109856057B
CN109856057B CN201910147830.XA CN201910147830A CN109856057B CN 109856057 B CN109856057 B CN 109856057B CN 201910147830 A CN201910147830 A CN 201910147830A CN 109856057 B CN109856057 B CN 109856057B
Authority
CN
China
Prior art keywords
fiber
light
tapered
erbium
laser
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
Application number
CN201910147830.XA
Other languages
Chinese (zh)
Other versions
CN109856057A (en
Inventor
巴德欣
董永康
闫嘉亮
张晓沛
李惠
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Harbin Institute of Technology Shenzhen
Original Assignee
Harbin Institute of Technology Shenzhen
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Harbin Institute of Technology Shenzhen filed Critical Harbin Institute of Technology Shenzhen
Priority to CN201910147830.XA priority Critical patent/CN109856057B/en
Publication of CN109856057A publication Critical patent/CN109856057A/en
Application granted granted Critical
Publication of CN109856057B publication Critical patent/CN109856057B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Optical Modulation, Optical Deflection, Nonlinear Optics, Optical Demodulation, Optical Logic Elements (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

以拉锥光纤为介质的液体成分检测装置及方法,涉及光检测技术领域。本发明解决了现有液体成分检测方法存在分辨率低和检测灵敏度低的问题。本发明的波形发生器发射的波形信号经微波放大器放大后发送至强度调制器,强度调制器利用波形信号对激光器发射的激光进行编码调节,调制后的激光信号一路作为探测光发送至单边带电光调制器;另一路作为泵浦光发送至第二掺铒光纤放大器;拉锥光纤设置在待测液体中;泵浦光与探测光经由受激布里渊散射效应在拉锥光纤中发生相互作用,相互作用后的探测光入射至探测器的感光面,经探测器光电转换后发送至示波器进行采集。本发明适合于检测液体成分。

Figure 201910147830

A liquid component detection device and method using a tapered optical fiber as a medium relate to the technical field of light detection. The invention solves the problems of low resolution and low detection sensitivity in the existing liquid component detection methods. The waveform signal emitted by the waveform generator of the present invention is amplified by the microwave amplifier and then sent to the intensity modulator. The intensity modulator uses the waveform signal to encode and adjust the laser light emitted by the laser, and the modulated laser signal is sent to the single-side charged signal as probe light all the way. Optical modulator; the other channel is sent to the second erbium-doped fiber amplifier as pump light; the taper fiber is set in the liquid to be tested; the pump light and the probe light interact in the taper fiber through the stimulated Brillouin scattering effect After the interaction, the probe light is incident on the photosensitive surface of the detector, and is sent to the oscilloscope for acquisition after photoelectric conversion by the detector. The present invention is suitable for detecting liquid components.

Figure 201910147830

Description

Liquid component detection device and method with tapered optical fiber as medium
Technical Field
The invention relates to the technical field of optical detection.
Background
The distributed optical fiber sensing technology has the advantages of high sensitivity, long sensing distance, electromagnetic interference resistance, corrosion resistance, convenience in arrangement and the like which are not possessed by a plurality of traditional sensors. The technology generally uses a single mode fiber as a sensing fiber, utilizes the modulation effect of the external physical quantity of the fiber on the transmitted light in the fiber, and realizes the measurement of the external physical quantity of the fiber by detecting the characteristic parameters (such as light intensity and polarization) of the light passing through the sensing fiber. The existing distributed optical fiber sensing technology is difficult to realize the detection of liquid components because the light is limited inside the sensing optical fiber.
The tapered optical fiber is a novel optical fiber sensing medium. The fiber diameter of the tapered optical fiber is several micrometers or even hundreds of nanometers, so that an evanescent field transmitted in the optical fiber is enhanced, and light can break through the limit of a cladding and enter the surrounding environment for transmission. Direct contact of the light with the external environment provides a viable way to achieve detection of the surrounding liquid components.
The existing distributed Brillouin liquid component detection technology taking a tapered optical fiber as a medium is based on the Brillouin optical time domain analysis principle. The technology belongs to the field of Brillouin optical fiber sensing technology. Different liquids to be tested have different brillouin frequency shifts. The detection of the liquid component to be detected can be realized by measuring the Brillouin frequency shift. The spatial resolution of the Brillouin optical time domain analysis technology is low and is generally in the meter level. The length of the tapered optical fiber is required to be at least meter level, and under the existing process conditions, the effective sensing area of the tapered optical fiber is generally centimeter level, the tapered optical fiber with meter level length is difficult to realize, the yield is extremely low, and the practical application capability of the technology is obviously limited. Moreover, this requires that the span of the space occupied by the liquid to be measured also be on the order of meters, which limits the detection sensitivity of the technique.
Disclosure of Invention
The invention provides a liquid component detection device and method with a tapered optical fiber as a medium, aiming at solving the problems of low spatial resolution and poor detection sensitivity of the existing liquid component detection method.
The invention relates to a liquid component detection device with a tapered optical fiber as a medium, which comprises a laser 1, an intensity modulator 2, a single-side charged optical modulator 3, a microwave source 4, a first erbium-doped optical fiber amplifier 5, a delay optical fiber 6, a tapered optical fiber 7, a circulator 9, a detector 10, an oscilloscope 11, a second erbium-doped optical fiber amplifier 12, a microwave amplifier 13 and a waveform generator 14;
a waveform signal emitted by the waveform generator 14 is amplified by the microwave amplifier 13 and then is sent to the intensity modulator 2, the intensity modulator 2 performs coding modulation on laser emitted by the laser 1 by using the waveform signal, and one path of the modulated laser signal is used as probe light and sent to the unilateral charged optical modulator 3; the other path of the light is used as pump light and sent to a second erbium-doped fiber amplifier 12;
the unilateral charged optical modulator 3 performs single-side band modulation on the optical signal by using a microwave signal sent by a microwave source 4 to form detection light with a downward frequency shift, the detection light with the downward frequency shift is transmitted to a delay optical fiber 6 for time delay after passing through a first erbium-doped optical fiber amplifier 5, the detection light delayed by the delay optical fiber 6 is transmitted to a tapered optical fiber 7, and the tapered optical fiber 7 is arranged in liquid to be detected;
the second erbium-doped fiber amplifier 12 amplifies the pump light, and then the pump light is emitted through the port 1 of the circulator 9 and is emitted to the tapered fiber 7 through the port 2; the amplified pump light and the delayed probe light interact in the tapered optical fiber 7 to form a correlation peak, stimulated Brillouin scattering occurs at the correlation peak, the probe light emitted from the tapered optical fiber 7 enters through the No. 2 port of the circulator 9, is emitted to the photosensitive surface of the detector 10 through the No. 3 port of the circulator 9, and is transmitted to the oscilloscope 11 after being subjected to photoelectric conversion by the detector 10.
Further, both the microwave source 4 and the waveform generator 14 are replaced with function generators.
Further, a pulse modulator is arranged between the second erbium-doped fiber amplifier 12 and the intensity modulator 2, and the pulse modulator receives the pump light output by the intensity modulator 2 to perform pulse modulation, and transmits the laser after pulse modulation to the second erbium-doped fiber amplifier 12.
The liquid component detection method with the tapered optical fiber as a medium comprises the following specific processes:
firstly, coding and modulating a laser signal by using a waveform signal, dividing the coded and modulated laser signal into two paths, wherein an upper path light is used as a detection light, and a lower path light is used as a pumping light;
step two, performing single-sideband modulation on the upper path optical signal by using microwaves to obtain detection light with a lower frequency shift, wherein the detection light with the lower frequency shift is amplified by a first erbium-doped fiber amplifier 5 and then enters a delay optical fiber 6, and the detection light is delayed by the delay optical fiber 6 and then enters a tapered optical fiber 7;
the down-path optical signal is injected into the No. 1 port of the circulator 9 after being amplified by the second erbium-doped optical fiber amplifier 12, is emitted out of the No. 2 port of the circulator 9 and then is incident to the tapered optical fiber 7;
and step three, the amplified pump light and the delayed detection light with the down-shift frequency interact in the tapered optical fiber 7 to form a correlation peak, stimulated Brillouin scattering occurs at the correlation peak, the detection light emitted from the tapered optical fiber 7 is emitted from the No. 2 port of the circulator 9 to the photosensitive surface of the detector 10 after being emitted from the No. 3 port of the circulator 9, and the detection light is subjected to photoelectric conversion by the detector 10 and then is sent to the oscilloscope 11. And fourthly, denoising and demodulating the received electric signal by using the oscilloscope 11 to obtain Brillouin frequency shift of a relevant peak in the tapered optical fiber, and obtaining the component of the liquid in which the tapered optical fiber is located according to the relation between the Brillouin frequency shift and the component of the liquid.
The present invention uses the brillouin frequency shift of a stimulated brillouin scattering signal in an optical fibre to detect the refractive index of a liquid. The optical field and the acoustic wave field of the non-tapered optical fiber are bound in the fiber core, and the optical field and the acoustic wave field of the tapered optical fiber can act with the outside, so that the outside influence is sensed, and the influence can be reflected through the change of Brillouin frequency shift, so that the refractive index of liquid can be detected. However, the length of the tapered optical fiber is generally short, the brillouin action region of the conventional brillouin sensing means is relatively long, signals with high signal-to-noise ratio at the tapered optical fiber are difficult to obtain, and brillouin action can only occur at the tapered optical fiber by using a brillouin correlation domain analysis (BOCDA) technology, so that signals with high signal-to-noise ratio are obtained, the distributed sensing effect is achieved, and the sensing sensitivity is remarkably improved.
Drawings
FIG. 1 is a schematic block diagram of a device for detecting a liquid component using a tapered optical fiber as a medium according to the present invention.
Detailed Description
The following detailed description of the embodiments of the present invention will be provided with reference to the accompanying drawings and examples, so that how to apply the technical means to solve the technical problems and achieve the corresponding technical effects can be fully understood and implemented. The embodiments and the features of the embodiments can be combined without conflict, and the technical solutions formed are all within the scope of the present invention.
The first embodiment is as follows: the following describes the present embodiment with reference to FIG. 1, in which the tapered optical fiber is used as a medium in the liquid component detection apparatus of the present embodiment,
the device comprises a laser 1, an intensity modulator 2, a single-side charged optical modulator 3, a microwave source 4, a first erbium-doped fiber amplifier 5, a delay fiber 6, a tapered fiber 7, a circulator 9, a detector 10, an oscilloscope 11, a second erbium-doped fiber amplifier 12, a microwave amplifier 13 and a waveform generator 14;
a waveform signal emitted by the waveform generator 14 is amplified by the microwave amplifier 13 and then is sent to the intensity modulator 2, the intensity modulator 2 performs coding modulation on laser emitted by the laser 1 by using the waveform signal, and one path of the modulated laser signal is used as probe light and sent to the unilateral charged optical modulator 3; the other path of the light is used as pump light and sent to a second erbium-doped fiber amplifier 12;
the unilateral charged optical modulator 3 performs single-side band modulation on the optical signal by using a microwave signal sent by a microwave source 4 to form detection light with a downward frequency shift, the detection light with the downward frequency shift is transmitted to a delay optical fiber 6 for time delay after passing through a first erbium-doped optical fiber amplifier 5, the detection light delayed by the delay optical fiber 6 is transmitted to a tapered optical fiber 7, and the tapered optical fiber 7 is arranged in liquid to be detected;
the second erbium-doped fiber amplifier 12 amplifies the pump light, and then the pump light is emitted through the port 1 of the circulator 9 and is emitted to the tapered fiber 7 through the port 2; the amplified pump light and the delayed probe light interact in the tapered optical fiber 7 to form a correlation peak, stimulated Brillouin scattering occurs at the correlation peak, the probe light emitted from the tapered optical fiber 7 enters through the No. 2 port of the circulator 9, is emitted to the photosensitive surface of the detector 10 through the No. 3 port of the circulator 9, and is transmitted to the oscilloscope 11 after being subjected to photoelectric conversion by the detector 10.
The second embodiment is as follows: in this embodiment, the liquid component detection apparatus using a tapered optical fiber as a medium according to the first embodiment is further described, in which the wavelength of the laser light output from the laser 1 is a distributed feedback type optical fiber laser having an output wavelength of 1550 nm.
The third concrete implementation mode: in this embodiment, the liquid component detection apparatus using a tapered optical fiber as a medium according to the first or second embodiment will be further described, in which both the microwave source 4 and the waveform generator 14 are replaced with function generators.
The fourth concrete implementation mode: in this embodiment, the liquid component detection apparatus using a tapered fiber as a medium according to the first or second embodiment is further described, in which a pulse modulator is provided between the second erbium-doped fiber amplifier 12 and the intensity modulator 2, the pulse modulator receives the pump light, performs pulse modulation, and transmits the pulse-modulated laser light to the second erbium-doped fiber amplifier 12.
The embodiment performs pulse modulation on the pump light, so that the acting peak power of the pump light can be improved, and the signal-to-noise ratio is enhanced. The tapered fiber has small effective gain length and high power requirement of pump light, and if continuous light is adopted, the optical fiber is easy to damage, and a pulse modulator is used for pulse modulation and then amplification, so that high peak power can be easily obtained, and a high signal-to-noise ratio can be obtained.
The fifth concrete implementation mode: in this embodiment, a pulse modulator is disposed between the second erbium-doped fiber amplifier 12 and the intensity modulator 2, and receives the pump light output by the intensity modulator 2, performs pulse modulation, and emits the pulse-modulated laser light to the second erbium-doped fiber amplifier 12. The sixth specific implementation mode: the method for detecting liquid components by taking the tapered optical fiber as a medium comprises the following specific processes:
firstly, coding and modulating a laser signal by using a waveform signal, dividing the coded and modulated laser signal into two paths, wherein an upper path light is used as a detection light, and a lower path light is used as a pumping light;
step two, performing single-sideband modulation on the upper path optical signal by using microwaves to obtain detection light with a lower frequency shift, wherein the detection light with the lower frequency shift is amplified by a first erbium-doped fiber amplifier 5 and then enters a delay optical fiber 6, and the detection light is delayed by the delay optical fiber 6 and then enters a tapered optical fiber 7;
the down-path optical signal is injected into the No. 1 port of the circulator 9 after being amplified by the second erbium-doped optical fiber amplifier 12, is emitted out of the No. 2 port of the circulator 9 and then is incident to the tapered optical fiber 7;
and step three, the amplified pump light and the delayed detection light with the down-shift frequency interact in the tapered optical fiber 7 to form a correlation peak, stimulated Brillouin scattering occurs at the correlation peak, the detection light emitted from the tapered optical fiber 7 is emitted from the No. 2 port of the circulator 9 to the photosensitive surface of the detector 10 after being emitted from the No. 3 port of the circulator 9, and the detection light is subjected to photoelectric conversion by the detector 10 and then is sent to the oscilloscope 11.
And fourthly, denoising and demodulating the received electric signal by using the oscilloscope 11 to obtain Brillouin frequency shift of a relevant peak in the tapered optical fiber, and obtaining the component of the liquid in which the tapered optical fiber is located according to the relation between the Brillouin frequency shift and the component of the liquid.
The invention adopts the Brillouin optical correlation domain analysis technology based on intensity modulation. The highest spatial resolution of the technology can reach 2 mm. The effective sensing length of the tapered optical fiber required by the technology is not less than 2mm, so that the drawing process of the tapered optical fiber is greatly reduced, and the practical level of the technology is obviously improved. On the other hand, the method of the invention can detect the liquid with a space span of millimeter level, which remarkably improves the sensing sensitivity. The relationship between the Brillouin frequency shift and the liquid composition is established by experimental determination of a liquid with known composition.
Although the embodiments of the present invention have been described above, the above descriptions are only for the convenience of understanding the present invention, and are not intended to limit the present invention. It will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention as defined by the appended claims.

Claims (4)

1.以拉锥光纤为介质的液体成分检测装置,其特征在于,该装置包括激光器(1)、强度调制器(2)、单边带电光调制器(3)、微波源(4)、第一掺铒光纤放大器(5)、延时光纤(6)、拉锥光纤(7)、环行器(9)、探测器(10)、示波器(11)、第二掺铒光纤放大器(12)、微波放大器(13)和波形发生器(14);1. a liquid composition detection device using a tapered optical fiber as a medium, characterized in that the device comprises a laser (1), an intensity modulator (2), a single-sideband electro-optical modulator (3), a microwave source (4), a an erbium-doped fiber amplifier (5), a time delay fiber (6), a tapered fiber (7), a circulator (9), a detector (10), an oscilloscope (11), a second erbium-doped fiber amplifier (12), a microwave amplifier (13) and a waveform generator (14); 波形发生器(14)发射的波形信号经微波放大器(13)放大后发送至强度调制器(2),强度调制器(2)利用波形信号对激光器(1)发射的激光进行编码调制,调制后的激光信号一路作为探测光发送至单边带电光调制器(3);另一路作为泵浦光发送至第二掺铒光纤放大器(12);The waveform signal emitted by the waveform generator (14) is amplified by the microwave amplifier (13) and then sent to the intensity modulator (2), and the intensity modulator (2) uses the waveform signal to encode and modulate the laser light emitted by the laser (1). One way of the laser signal is sent to the single-sideband electro-optical modulator (3) as probe light; the other way is sent to the second erbium-doped fiber amplifier (12) as pump light; 单边带电光调制器(3)利用微波源(4)发送的微波信号对该路光信号进行单边带调制,形成具有下移频的探测光,具有下移频的探测光经第一掺铒光纤放大器(5)后入射至延时光纤(6)进行延时,经延时光纤(6)延时后的探测光再入射至拉锥光纤(7),拉锥光纤(7)设置在待测液体中;The single-sideband electro-optical modulator (3) uses the microwave signal sent by the microwave source (4) to perform single-sideband modulation on the optical signal to form a probe light with a downshift, and the probe light with a downshift is subjected to a first doping The erbium fiber amplifier (5) is incident on the time delay fiber (6) for delaying, and the probe light after being delayed by the time delay fiber (6) is then incident on the tapered fiber (7), and the tapered fiber (7) is arranged in the tapered fiber (7). in the liquid to be tested; 第二掺铒光纤放大器(12)对泵浦光进行放大后通过环行器(9)的1端口射入经2号口射出至拉锥光纤(7);经过放大后的泵浦光与延时后的探测光在拉锥光纤(7)内相互作用,形成一个相关峰,在相关峰处发生受激布里渊散射,从拉锥光纤(7)射出的探测光经环行器(9)的2号口入,经环行器(9)的3号口射出至探测器(10)的感光面,经探测器(10)的光电转换后发送至示波器(11);The second erbium-doped fiber amplifier (12) amplifies the pump light and then enters through the 1 port of the circulator (9) and exits to the taper fiber (7) through the 2 port; the amplified pump light and the time delay The latter probe light interacts in the tapered fiber (7) to form a correlation peak, and stimulated Brillouin scattering occurs at the correlation peak, and the probe light emitted from the tapered fiber (7) passes through the circulator (9). It enters through the No. 2 port, and is emitted to the photosensitive surface of the detector (10) through the No. 3 port of the circulator (9), and is sent to the oscilloscope (11) after the photoelectric conversion of the detector (10); 第二掺铒光纤放大器(12)与强度调制器(2)之间设置有脉冲调制器,所述脉冲调制器接收强度调制器(2)输出的泵浦光进行脉冲调制,将脉冲调制后的激光发射至第二掺铒光纤放大器(12)。A pulse modulator is arranged between the second erbium-doped fiber amplifier (12) and the intensity modulator (2), and the pulse modulator receives the pump light output by the intensity modulator (2) to perform pulse modulation, and modulates the pulsed The laser is emitted to a second erbium-doped fiber amplifier (12). 2.根据权利要求1所述的以拉锥光纤为介质的液体成分检测装置,其特征在于,激光器(1)采用输出波长为1550nm的分布反馈式光纤激光器。2 . The liquid component detection device using a tapered fiber as a medium according to claim 1 , wherein the laser ( 1 ) adopts a distributed feedback fiber laser with an output wavelength of 1550 nm. 3 . 3.根据权利要求1或2所述的以拉锥光纤为介质的液体成分检测装置,其特征在于,微波源(4)和波形发生器(14)均替换为函数发生器。3 . The liquid component detection device using tapered optical fiber as a medium according to claim 1 or 2 , wherein the microwave source ( 4 ) and the waveform generator ( 14 ) are both replaced with function generators. 4 . 4.以拉锥光纤为介质的液体成分检测方法,其特征在于,该方法的具体过程为:4. The liquid composition detection method using tapered optical fiber as a medium is characterized in that, the specific process of the method is: 步骤一、利用波形信号对激光信号进行编码调制,将编码调制后的激光信号分为两路,上路光作为探测光,下路光作为泵浦光;Step 1, using the waveform signal to code-modulate the laser signal, dividing the code-modulated laser signal into two paths, the upper path light is used as the probe light, and the lower path light is used as the pump light; 步骤二、利用微波对上路光信号进行单边带调制,获得具有下移频的探测光,具有下移频的探测光经第一掺铒光纤放大器(5)放大后入射至延时光纤(6),经延时光纤(6)延时后入射至拉锥光纤(7);Step 2: Using microwaves to perform single-sideband modulation on the optical signal on the upper path to obtain a probe light with a downshift frequency, and the probe light with a downshift frequency is amplified by the first erbium-doped fiber amplifier (5) and then incident on the delay fiber (6). ), which is incident on the tapered fiber (7) after being delayed by the time delay fiber (6); 下路光信号通过第二掺铒光纤放大器(12)放大后的注入环行器(9)的1号口,经环行器(9)的2号口射出后入射至拉锥光纤(7);The drop optical signal is injected into the No. 1 port of the circulator (9) after being amplified by the second erbium-doped fiber amplifier (12), and is emitted through the No. 2 port of the circulator (9) and then incident on the tapered fiber (7); 步骤三、放大后的泵浦光和延时后的具有下移频的探测光在拉锥光纤(7)内相互作用,形成一个相关峰,在相关峰处发生受激布里渊散射,从拉锥光纤(7)射出的探测光由环行器(9)的2号口入射后,从环行器(9)的3号口射出至探测器(10)的感光面,经探测器(10)光电转换后发送至示波器(11);Step 3: The amplified pump light and the delayed probe light with the downshifted frequency interact in the taper fiber (7) to form a correlation peak, and stimulated Brillouin scattering occurs at the correlation peak. After the probe light emitted by the tapered fiber (7) is incident through the No. 2 port of the circulator (9), it is emitted from the No. 3 port of the circulator (9) to the photosensitive surface of the detector (10), and passes through the detector (10) After photoelectric conversion, it is sent to the oscilloscope (11); 步骤四、对示波器(11)对接收的的电信号进行去噪声和解调后获得拉锥光纤中相关峰处的布里渊频移,根据布里渊频移与液体成分的关系,获得拉锥光纤所处液体的成分。Step 4: De-noise and demodulate the received electrical signal with the oscilloscope (11) to obtain the Brillouin frequency shift at the correlation peak in the tapered fiber, and obtain the Brillouin frequency shift according to the relationship between the Brillouin frequency shift and the liquid composition. The composition of the liquid in which the tapered fiber is located.
CN201910147830.XA 2019-02-27 2019-02-27 Liquid composition detection device and method using tapered optical fiber as medium Expired - Fee Related CN109856057B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201910147830.XA CN109856057B (en) 2019-02-27 2019-02-27 Liquid composition detection device and method using tapered optical fiber as medium

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201910147830.XA CN109856057B (en) 2019-02-27 2019-02-27 Liquid composition detection device and method using tapered optical fiber as medium

Publications (2)

Publication Number Publication Date
CN109856057A CN109856057A (en) 2019-06-07
CN109856057B true CN109856057B (en) 2021-10-29

Family

ID=66899328

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201910147830.XA Expired - Fee Related CN109856057B (en) 2019-02-27 2019-02-27 Liquid composition detection device and method using tapered optical fiber as medium

Country Status (1)

Country Link
CN (1) CN109856057B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113390441B (en) * 2021-06-01 2023-07-21 重庆邮电大学 Device and measurement method for sensing changes in refractive index

Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101627294A (en) * 2007-03-06 2010-01-13 住友电气工业株式会社 Method for measuring polarization characteristics of optical fiber, drawing method, method for identifying abnormal point, and method for configuring optical fiber transmission line
CN102538985A (en) * 2011-12-27 2012-07-04 中国计量学院 Sensing signal detecting device and method based on fiber Brillouin ring laser
CN103123285A (en) * 2013-02-05 2013-05-29 太原理工大学 Distributed optical fiber sensing device based on chaotic laser coherence method, and measurement method of distributed optical fiber sensing device
CN103323399A (en) * 2013-05-31 2013-09-25 哈尔滨理工大学 Micro-nano fiber biosensor
WO2014034638A1 (en) * 2012-08-27 2014-03-06 国立大学法人東京大学 Optical fiber property measuring device and optical fiber property measuring method
CN103884703A (en) * 2014-03-10 2014-06-25 北京理工大学 Light-splitting pupil laser differential motion confocal Brillouin-Raman spectrum measurement method and device
KR101447090B1 (en) * 2013-04-29 2014-11-03 한국과학기술연구원 Distributed optical fiber sensor and sensing method using the same
CN105136177A (en) * 2015-08-27 2015-12-09 太原理工大学 Sub-millimeter spatial resolution distributed optical fiber sensing device and method
CN107543567A (en) * 2017-08-11 2018-01-05 太原理工大学 BOCDA distribution type optical fiber sensing equipments and method based on the modulation of physical accidental code
CN108917804A (en) * 2018-09-03 2018-11-30 哈尔滨工业大学 Quick long-distance distributed Brillouin light fiber sensing equipment based on chirp chain

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20090304551A1 (en) * 2006-01-31 2009-12-10 Drexel University Ultra Sensitive Tapered Fiber Optic Biosensor For Pathogens, Proteins, and DNA

Patent Citations (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101627294A (en) * 2007-03-06 2010-01-13 住友电气工业株式会社 Method for measuring polarization characteristics of optical fiber, drawing method, method for identifying abnormal point, and method for configuring optical fiber transmission line
CN102538985A (en) * 2011-12-27 2012-07-04 中国计量学院 Sensing signal detecting device and method based on fiber Brillouin ring laser
WO2014034638A1 (en) * 2012-08-27 2014-03-06 国立大学法人東京大学 Optical fiber property measuring device and optical fiber property measuring method
CN103123285A (en) * 2013-02-05 2013-05-29 太原理工大学 Distributed optical fiber sensing device based on chaotic laser coherence method, and measurement method of distributed optical fiber sensing device
KR101447090B1 (en) * 2013-04-29 2014-11-03 한국과학기술연구원 Distributed optical fiber sensor and sensing method using the same
CN103323399A (en) * 2013-05-31 2013-09-25 哈尔滨理工大学 Micro-nano fiber biosensor
CN103884703A (en) * 2014-03-10 2014-06-25 北京理工大学 Light-splitting pupil laser differential motion confocal Brillouin-Raman spectrum measurement method and device
CN105136177A (en) * 2015-08-27 2015-12-09 太原理工大学 Sub-millimeter spatial resolution distributed optical fiber sensing device and method
CN107543567A (en) * 2017-08-11 2018-01-05 太原理工大学 BOCDA distribution type optical fiber sensing equipments and method based on the modulation of physical accidental code
CN108917804A (en) * 2018-09-03 2018-11-30 哈尔滨工业大学 Quick long-distance distributed Brillouin light fiber sensing equipment based on chirp chain

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
Fiber distributed Brillouin sensing with optical correlation domain techniques;Kazuo Hotate;《Optical Fiber Technology》;20130916;全文 *
基于布里渊散射的分布式光纤传感技术;张博;《应用技术》;20150430;全文 *

Also Published As

Publication number Publication date
CN109856057A (en) 2019-06-07

Similar Documents

Publication Publication Date Title
CN101764646B (en) Wavelength-encoding optical time domain reflection test device and measurement method thereof
CN103115632B (en) Multi-wavelength Brillouin optical time-domain analyzer
CN105758433B (en) A kind of distribution type optical fiber sensing equipment based on Brillouin optical fiber laser
CN104677396A (en) Dynamic distributed Brillouin optical fiber sensing device and method
CN103364106B (en) A kind of Brillouin optical time domain analysis sensor-based system based on the pumping of overlength loop laser
CN107764297B (en) Dynamic Brillouin optical time domain analysis system based on pump pulse frequency sweep
CN101762290A (en) Distributed Raman amplification-based Brillouin optical time domain analysis system
CN102997949A (en) Method used for measuring temperature and strain simultaneously and based on brillouin scattering
WO2009097736A1 (en) Chaotic optical time domain reflectometer and measuring method thereof
CN101975626A (en) Brillouin scattering based distributive fiber sensing system
KR101889351B1 (en) Spatially-selective brillouin distributed optical fiber sensor with increased effective sensing points and sensing method using brillouin scattering
CN103763022B (en) A high spatial resolution optical frequency domain reflectometer system based on high-order sideband swept frequency modulation
CN104792343A (en) Single-ended structure dynamic measuring Brillouin optical fiber sensing system and sensing method
CN109297425A (en) A Brillouin Optical Time Domain Reflectometer Modulated by Physical Random Numbers
CN109186736A (en) It is a kind of can fixing frequency displacement structure slope auxiliary Brillouin fiber optic sensing vibration measurement device and measurement method
CN204439100U (en) Dynamic distributed Brillouin light fiber sensing equipment
CN115326186A (en) Ф-OTDR system based on phase-shifted double-pulse detection technology and its demodulation method
CN103616090B (en) A kind of brillouin distributed optical fiber sensing temp measuring system eliminating optical fiber attenuation
CN107764461B (en) Distributed hydraulic sensor system based on Brillouin dynamic grating
CN109856057B (en) Liquid composition detection device and method using tapered optical fiber as medium
CN108801305A (en) Method and device based on the Brillouin optical time-domain reflectometer that step pulse amplifies certainly
CN102607631A (en) Method for precisely estimating signal to noise ratio of EOM (Electro-Optic Modulator) pulse modulated BOTDR (Brillouin Optical Time Domain Reflectometer)
CN109781156B (en) BOTDA system based on Brillouin gain spectrum modulation and its sensing method
Liu et al. Monitoring distance enhancement with chaotic laser for OTDR system
CN109781154B (en) A Brillouin Correlation Domain Analysis System with High Spatial Resolution Based on Intensity Modulation

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
CB03 Change of inventor or designer information

Inventor after: Ba Dexin

Inventor after: Dong Yongkang

Inventor after: Yan Jialiang

Inventor after: Zhang Xiaopei

Inventor after: Li Hui

Inventor before: Dong Yongkang

Inventor before: Ba Dexin

Inventor before: Yan Jialiang

Inventor before: Zhang Xiaopei

Inventor before: Li Hui

CB03 Change of inventor or designer information
GR01 Patent grant
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20211029

CF01 Termination of patent right due to non-payment of annual fee