CN108318060B - 2-micron-waveband three-parameter optical fiber sensor based on inclined optical fiber Bragg grating - Google Patents
2-micron-waveband three-parameter optical fiber sensor based on inclined optical fiber Bragg grating Download PDFInfo
- Publication number
- CN108318060B CN108318060B CN201711497662.4A CN201711497662A CN108318060B CN 108318060 B CN108318060 B CN 108318060B CN 201711497662 A CN201711497662 A CN 201711497662A CN 108318060 B CN108318060 B CN 108318060B
- Authority
- CN
- China
- Prior art keywords
- bragg grating
- fiber bragg
- fiber
- transmission peak
- peak wavelength
- 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.)
- Active
Links
- 239000013307 optical fiber Substances 0.000 title claims abstract description 19
- 239000000835 fiber Substances 0.000 claims abstract description 140
- 238000000034 method Methods 0.000 claims abstract description 21
- 230000007613 environmental effect Effects 0.000 claims abstract description 16
- 238000011897 real-time detection Methods 0.000 claims abstract description 4
- 230000005540 biological transmission Effects 0.000 claims description 60
- 238000005253 cladding Methods 0.000 claims description 57
- 238000001228 spectrum Methods 0.000 claims description 16
- 230000035945 sensitivity Effects 0.000 claims description 15
- 238000000411 transmission spectrum Methods 0.000 claims description 15
- 230000004927 fusion Effects 0.000 claims description 10
- 239000007788 liquid Substances 0.000 claims description 10
- 238000005259 measurement Methods 0.000 claims description 10
- 238000012545 processing Methods 0.000 claims description 5
- 238000000295 emission spectrum Methods 0.000 claims description 2
- 230000009286 beneficial effect Effects 0.000 abstract description 2
- 230000000694 effects Effects 0.000 abstract 1
- 230000007547 defect Effects 0.000 description 2
- 239000011159 matrix material Substances 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000010364 biochemical engineering Methods 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000003814 drug Substances 0.000 description 1
- 239000011152 fibreglass Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 239000000523 sample Substances 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
Images
Classifications
-
- 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
- G01D5/268—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 using optical fibres
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optical Transform (AREA)
- Length Measuring Devices By Optical Means (AREA)
Abstract
本发明提供了一种基于倾斜光纤Bragg光栅的2μm波段三参量光纤传感器及其使用方法，该光纤传感器包括宽谱光源(101)、第一单模光纤(102)、倾斜光纤Bragg光栅(103)、第二单模光纤(104)以及光谱仪(105)。本发明设计的光纤传感器，可以同时对温度、轴向应变与环境折射率进行传感，实现待测温度、轴向应变与环境折射率的实时检测；具有体积小、响应快、精度高、可操作性强等优点，具有有益的技术效果。
The invention provides a 2-μm-band three-parameter optical fiber sensor based on a tilted fiber Bragg grating and a method for using the same. The fiber sensor includes a broad-spectrum light source (101), a first single-mode fiber (102), and a tilted fiber Bragg grating (103) , a second single-mode fiber (104), and a spectrometer (105). The optical fiber sensor designed by the invention can sense temperature, axial strain and environmental refractive index at the same time, so as to realize real-time detection of the temperature to be measured, axial strain and environmental refractive index; It has the advantages of strong operability, etc., and has beneficial technical effects.
Description
Technical Field
The invention relates to the field of optical fiber sensors, in particular to a 2-micron-waveband three-parameter optical fiber sensor based on a tilted fiber Bragg grating, which can sense temperature, axial strain and environmental refractive index simultaneously.
Background
Theoretical and experimental studies on the 2 μm band are currently in a rapidly growing stage. Tm3+, Ho3+ ion doped fiberglass materials have a wide gain bandwidth range from 1.7 μm to 2.1 μm with good overlap with atmospheric gas absorption lines, such as H2O and CO2, making them well suited for CO2 gas detection and other sensing measurements. Moreover, the working bandwidth also provides a wide operating range for the laser in the safe band of human eyes. Due to these advantages, devices operating in the 2 μm band can be widely used in the fields of medicine, biology, lidar, remote sensing, military technology, etc.
Measurement of temperature, axial strain and ambient refractive index (SRI) is an important process in biochemical engineering, environmental monitoring and medical science. The optical fiber sensor has gained wide attention due to its advantages of small volume, fast response, strong operability, etc. In the field of optical fiber sensing, the application and research of fiber gratings have also become very popular and practical. The optical fiber Bragg grating sensor is mainly used for measuring stress strain, temperature and humidity, but the Bragg wavelength is sensitive to changes of stress and temperature, so that the problem of cross talk is difficult to eliminate. Although Long Period Fiber Gratings (LPFGs) have excellent performance for measurement of the ambient refractive index, their high cross-sensitivity to perturbations of the ambient environment is not negligible.
Tilted fiber Bragg gratings, because of their unique physical structure, which include the advantages of fiber Bragg gratings and long-period fiber Bragg gratings, can successfully overcome these disadvantages and show great potential in the simultaneous measurement of various parameters. However, in the manufacturing design of the existing inclined fiber Bragg grating, the inclined angle is too large, the wave band range is wide, and only the temperature and the refractive index can be measured simultaneously, so that the defects of slow response of a sensor, low measurement precision and insufficient environmental adaptability exist.
Disclosure of Invention
Aiming at the defects, the invention provides a 2-micron-waveband three-parameter optical fiber sensor based on a tilted fiber Bragg grating, which can sense the temperature, the axial strain and the ambient refractive index simultaneously.
The purpose of the invention is realized by the following technical scheme:
a2 mu m waveband three-parameter fiber sensor based on a tilted fiber Bragg grating comprises a wide spectrum light source (101), a first single-mode fiber (102), a tilted fiber Bragg grating (103), a second single-mode fiber (104) and a spectrometer (105), and is characterized in that:
the wide-spectrum light source (101) is connected with one end of the first single-mode fiber (102) through a fiber connector, the other end of the first single-mode fiber (102) is connected with one end of the inclined fiber Bragg grating (103), the other end of the inclined fiber Bragg grating (103) is connected with one end of the second single-mode fiber (104), and the other end of the second single-mode fiber (104) is connected with the spectrometer (105) through a fiber connector.
Preferably, the first single-mode fiber (102) and the tilted fiber Bragg grating (103) are connected by a fiber connector or fusion spliced by a fiber fusion splicer.
Preferably, the tilted fiber Bragg grating (103) and the second single-mode fiber (104) are connected by a fiber connector or fusion spliced by a fiber fusion splicer.
Preferably, the tilted fiber Bragg grating (103) is fabricated using a phase mask method of ultraviolet exposure.
Preferably, the phase mask needs to be inclined by 2 degrees when the inclined fiber Bragg grating (103) is manufactured.
Preferably, the core mode transmission peak wavelength, the 25 th order cladding mode transmission peak wavelength and the 28 th order cladding mode transmission peak wavelength of the tilted fiber Bragg grating (103) are taken as characteristic wavelengths of the optical fiber sensor.
Preferably, the optical fiber sensor senses the temperature, the axial strain and the environmental refractive index simultaneously, and realizes real-time detection of the temperature to be detected, the axial strain and the environmental refractive index.
A method for measuring a 2 μm band three-parameter fiber sensor using a tilted fiber Bragg grating is characterized by: the method comprises the following steps:
step one, a temperature calibration process: light emitted by a wide-spectrum light source (101) is incident on the inclined fiber Bragg grating, when the temperature changes, the transmission spectrum of the inclined fiber Bragg grating (103) can drift, and a spectrometer (105) is used for detecting the changes of the core mode transmission peak wavelength, the 25 th-order cladding mode transmission peak wavelength and the 28 th-order cladding mode transmission peak wavelength of the inclined fiber Bragg grating (103) to obtain a sensitivity coefficient related to the temperature;
step two, an axial strain calibration process: fixing two ends of the tilted fiber Bragg grating (103) on a stress adjusting frame, and stretching the tilted fiber Bragg grating (103) to generate strain; when the strain occurs, the transmission spectrum of the tilted fiber Bragg grating (103) can shift, and the spectrometer (105) is used for detecting the changes of the core mode transmission peak wavelength, the 25 th-order cladding mode transmission peak wavelength and the 28 th-order cladding mode transmission peak wavelength of the tilted fiber Bragg grating (103) to obtain the sensitivity coefficient related to the axial strain;
step three, the environmental refractive index calibration process: when the refractive index of liquid around the tilted fiber Bragg grating (103) changes, the transmission spectrum of the tilted fiber Bragg grating can drift, and the spectrometer (105) is used for detecting the changes of the core mode transmission peak wavelength, the 25 th order cladding mode transmission peak wavelength and the 28 th order cladding mode transmission peak wavelength of the tilted fiber Bragg grating (103) to obtain the sensitivity coefficient related to the environmental refractive index.
And step four, combining the temperature, the axial strain and the ambient refractive index sensitivity coefficient, and the core mold transmission peak wavelength, the 25 th order cladding mold transmission peak wavelength and the 28 th order cladding mold transmission peak wavelength variation to realize sensing measurement.
The invention has the beneficial effects that:
1. the optical fiber sensor designed by the invention can simultaneously sense the temperature, the axial strain and the environmental refractive index, and realize the real-time detection of the temperature to be detected, the axial strain and the environmental refractive index;
2. the sensor probe has the advantages of small volume, quick response, high precision, strong operability and the like.
Drawings
FIG. 1 is a schematic diagram of a 2 μm waveband three-parameter fiber sensor based on a tilted fiber Bragg grating according to the present invention;
FIG. 2 is a transmission spectrum of a tilted fiber Bragg grating (103) according to the present invention.
Detailed Description
Reference will now be made in detail to embodiments of the present invention, examples of which are illustrated in the accompanying drawings, wherein like reference numerals refer to the same or similar elements or elements having the same or similar function throughout. The embodiments described below with reference to the accompanying drawings are illustrative only for the purpose of explaining the present invention, and are not to be construed as limiting the present invention.
It will be understood by those skilled in the art that, unless otherwise defined, all terms (including technical and scientific terms) used herein have the same meaning as commonly understood by one of ordinary skill in the art to which this invention belongs. It will be further understood that terms, such as those defined in commonly used dictionaries, should be interpreted as having a meaning that is consistent with their meaning in the context of the prior art and will not be interpreted in an idealized or overly formal sense unless expressly so defined herein.
Example 1:
as shown in fig. 1, a 2 μm waveband three-parameter fiber sensor based on a tilted fiber Bragg grating comprises a wide spectrum light source (101), a first single mode fiber (102), a tilted fiber Bragg grating (103), a second single mode fiber (104), and a spectrometer (105); the wide-spectrum light source (101) is connected with one end of the first single-mode fiber (102) through a fiber connector, the other end of the first single-mode fiber (102) is connected with one end of the inclined fiber Bragg grating (103) through a fiber connector or through a fusion splicer, the other end of the inclined fiber Bragg grating (103) is connected with one end of the second single-mode fiber (104) through a fiber connector or through a fusion splicer, and the other end of the second single-mode fiber (104) is connected with the spectrometer (105) through a fiber connector.
The inclined fiber Bragg grating (103) is manufactured by using an ultraviolet exposure phase mask method, the length of the inclined fiber Bragg grating is 2cm, the phase mask needs to be inclined when the inclined fiber Bragg grating is manufactured, and the inclination angle is 2 degrees.
As shown in fig. 2, the tilted fiber Bragg grating (103) Mandrel transmission peak wavelength lambdacore1944.5nm, and the wavelength of the transmission peak of the cladding mode ranges from 1905nm to 1942.7nm, and the transmission peak of the cladding mode contains 38-step transmission peak of the cladding mode; the core-mode transmission peak wavelength lambda of the tilted fiber Bragg grating (103) is selectedcore25 th order cladding mode transmission peak wavelength lambdacladding,25And a 28 th order cladding mode transmission peak wavelength lambdacladding,28As the characteristic wavelength of the three-parameter sensing of the present invention.
The emission spectrum range of the wide-spectrum light source (101) is 1200-2050nm, and the whole transmission peak range of the inclined fiber Bragg grating (103) is covered;
example 2:
the 2-micron-waveband three-parameter optical fiber sensor based on the inclined optical fiber Bragg grating needs to be subjected to parameter calibration before sensing measurement, and the calibration process is as follows:
1. temperature T calibration process: placing the inclined fiber Bragg grating (103) into a temperature control box, and placing the rest part out of the temperature control box; light emitted by the wide-spectrum light source (101) is incident on the inclined fiber Bragg grating, when the temperature is not changed, the transmission spectrum of the inclined fiber Bragg grating (103) cannot shift, and when the temperature is changed, the transmission spectrum of the inclined fiber Bragg grating (103) can shift; the temperature of the temperature control box is gradually increased from 30 ℃ to 80 ℃, and the wavelength lambda of the mandrel transmission peak of the inclined fiber Bragg grating (103) is detected by the spectrometer (105)core25 th order cladding mode transmission peak wavelength lambdacladding,25And a 28 th order cladding mode transmission peak wavelength lambdacladding,28The variation and the sensitivity coefficient K of the three resonance peak wavelengths with respect to the temperature are obtained through data processingcore,T、Kcladding,25,T、Kcladding,28,T。
2. And (3) an axial strain epsilon calibration process: fixing two ends of the tilted fiber Bragg grating (103) on a stress adjusting frame, and stretching the tilted fiber Bragg grating (103) to generate strain; the light emitted by the wide-spectrum light source (101) is incident on the inclined fiber Bragg grating (103), and when no response occurs on the inclined fiber Bragg grating (103)When changed, the transmission spectrum of the tilted fiber Bragg grating (103) can not shift, and when the tilted fiber Bragg grating is strained, the transmission spectrum of the tilted fiber Bragg grating can shift; axial strain gradually increases from 0 to 3500 mu epsilon, and the core mode transmission peak wavelength lambda of the tilted fiber Bragg grating (103) is detected by the spectrometer (105)core25 th order cladding mode transmission peak wavelength lambdacladding,25And a 28 th order cladding mode transmission peak wavelength lambdacladding,28Changing and obtaining sensitivity coefficient K of three resonance peak wavelengths related to axial strain of the tilted fiber Bragg grating (103) through data processingcore,ε、Kcladding,25,ε、Kcladding,28,ε。
3. Ambient refractive index nextA calibration process: placing the tilted fiber Bragg grating (103) in a container filled with a liquid with a known refractive index, and placing the rest of the container outside, wherein the refractive index of the liquid in the container can be accurately adjusted and changed; light emitted by the wide-spectrum light source (101) is incident on the inclined fiber Bragg grating (103), and when the refractive index of liquid around the inclined fiber Bragg grating (103) is changed, the transmission spectrum of the inclined fiber Bragg grating can shift; the refractive index of the liquid gradually increases from 1.35749 to 1.47399, and the wavelength λ of the mandrel transmission peak of the tilted fiber Bragg grating (103) is detected by the spectrometer (105)core25 th order cladding mode transmission peak wavelength lambdacladding,25And a 28 th order cladding mode transmission peak wavelength lambdacladding,28The sensitivity coefficients of the three resonance peak wavelengths with respect to the environmental refractive index of the tilted fiber Bragg grating (103) are changed and obtained through data processing, namely 0,
4. Combining temperature, axial strain and ambient refractive index variations DeltaT,. DELTA.. epsilon,. DELTA.nextAnd sensitivity coefficient and wavelength lambda of transmission peak of the core model core25 th order cladding mode transmission peak wavelength lambdacladding,25And a 28 th order cladding mode transmission peak wavelength lambdacladding,28Variation quantity Delta lambdacore、△λcladding,25、△λcladding,28Obtaining the sensitivity momentThe matrix is as follows:
the variation quantity delta T, delta epsilon and delta n of the temperature, the axial strain and the ambient refractive index can be obtained through a reverse-push matrixextThe variation quantity delta lambda of the transmission peak wavelength of the core mold, the transmission peak wavelength of the 25 th order cladding mold and the transmission peak wavelength of the 28 th order cladding moldcore、△λcladding,25、△λcladding,28For implementing a sensing measurement:
the above description is only for the preferred embodiment of the present invention, but the scope of the present invention is not limited thereto, and any changes or substitutions that can be easily conceived by those skilled in the art within the technical scope of the present invention are included in the scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the claims.
Claims (1)
1. A method of 2 μm band three-parameter fiber sensor measurement using tilted fiber Bragg gratings, the fiber sensor comprising: the device comprises a wide-spectrum light source, a first single-mode fiber, an inclined fiber Bragg grating, a second single-mode fiber and a spectrometer, wherein the wide-spectrum light source is connected with one end of the first single-mode fiber through a fiber connector, the other end of the first single-mode fiber is connected with one end of the inclined fiber Bragg grating, the other end of the inclined fiber Bragg grating is connected with one end of the second single-mode fiber, and the other end of the second single-mode fiber is connected with the spectrometer through the fiber connector; the first single-mode fiber is connected with the inclined fiber Bragg grating through a fiber connector or in fusion connection through a fiber fusion splicer; the inclined fiber Bragg grating is connected with the second single-mode fiber through a fiber connector or in fusion connection through a fiber fusion splicer; the inclined fiber Bragg grating is manufactured to have an inclination angle of 2 degrees by using an ultraviolet exposure phase mask method; the core mode transmission peak wavelength, the 25 th-order cladding mode transmission peak wavelength and the 28 th-order cladding mode transmission peak wavelength of the inclined fiber Bragg grating are taken as characteristic wavelengths of the optical fiber sensor; the optical fiber sensor simultaneously senses temperature, axial strain and environmental refractive index, real-time detection of the temperature to be detected, the axial strain and the environmental refractive index is realized, and the axial strain is gradually increased from 0 to 3500 mu epsilon; the emission spectrum range of the wide-spectrum light source is 1200-2050nm, and the wide-spectrum light source covers the whole transmission peak range of the inclined fiber Bragg grating, and is characterized in that: the method comprises the following steps:
step one, a temperature calibration process: light emitted by a wide-spectrum light source is incident on the inclined fiber Bragg grating, when the temperature changes, the transmission spectrum of the inclined fiber Bragg grating can drift, and a spectrometer is used for detecting the changes of the core mode transmission peak wavelength, the 25 th-order cladding mode transmission peak wavelength and the 28 th-order cladding mode transmission peak wavelength of the inclined fiber Bragg grating to obtain a sensitivity coefficient related to the temperature; the temperature calibration process specifically comprises the following steps: placing the inclined fiber Bragg grating into a temperature control box, and placing the rest part out of the temperature control box; the light emitted by the wide-spectrum light source is incident on the inclined fiber Bragg grating, when the temperature is not changed, the transmission spectrum of the inclined fiber Bragg grating cannot drift, and when the temperature is changed, the transmission spectrum of the inclined fiber Bragg grating can drift; the temperature of the temperature control box is gradually increased from 30 ℃ to 80 ℃, the spectrometer is utilized to detect the core mold transmission peak wavelength, the 25 th order cladding mold transmission peak wavelength and the 28 th order cladding mold transmission peak wavelength variation of the inclined fiber Bragg grating, and the sensitivity coefficients of the three resonance peak wavelengths with respect to the temperature are obtained through data processing; step two, an axial strain calibration process: fixing two ends of the inclined fiber Bragg grating on a stress adjusting frame, and stretching the inclined fiber Bragg grating to generate strain; when the strain occurs, the transmission spectrum of the tilted fiber Bragg grating can drift, and the spectrometer is utilized to detect the changes of the core mode transmission peak wavelength, the 25 th-order cladding mode transmission peak wavelength and the 28 th-order cladding mode transmission peak wavelength of the tilted fiber Bragg grating, so as to obtain the sensitivity coefficient related to the axial strain; step three, the environmental refractive index calibration process: when the refractive index of liquid around the tilted fiber Bragg grating changes, the transmission spectrum of the tilted fiber Bragg grating can drift, and the spectrometer is used for detecting the changes of the wavelength of a core mode transmission peak, the wavelength of a 25 th-order cladding mode transmission peak and the wavelength of a 28 th-order cladding mode transmission peak of the tilted fiber Bragg grating to obtain a sensitivity coefficient related to the environmental refractive index; the environment refractive index calibration process specifically comprises the following steps: placing the tilted fiber Bragg grating in a container filled with liquid with known refractive index, and placing the rest part of the tilted fiber Bragg grating outside the container, wherein the refractive index of the liquid in the container is accurately adjusted and changed; light emitted by the wide-spectrum light source is incident on the inclined fiber Bragg grating, and when the refractive index of liquid around the inclined fiber Bragg grating is changed, the transmission spectrum of the inclined fiber Bragg grating can drift; the liquid refractive index is gradually increased from 1.35749 to 1.47399, the spectrometer is used for detecting the core mode transmission peak wavelength, the 25 th order cladding mode transmission peak wavelength and the 28 th order cladding mode transmission peak wavelength of the tilted fiber Bragg grating, and sensitivity coefficients of three resonance peak wavelengths relative to the ambient refractive index of the tilted fiber Bragg grating are obtained through data processing; and step four, combining the temperature, the axial strain and the ambient refractive index sensitivity coefficient, and the core mold transmission peak wavelength, the 25 th order cladding mold transmission peak wavelength and the 28 th order cladding mold transmission peak wavelength variation to realize sensing measurement.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201711497662.4A CN108318060B (en) | 2017-12-29 | 2017-12-29 | 2-micron-waveband three-parameter optical fiber sensor based on inclined optical fiber Bragg grating |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201711497662.4A CN108318060B (en) | 2017-12-29 | 2017-12-29 | 2-micron-waveband three-parameter optical fiber sensor based on inclined optical fiber Bragg grating |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN108318060A CN108318060A (en) | 2018-07-24 |
| CN108318060B true CN108318060B (en) | 2021-05-18 |
Family
ID=62893769
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201711497662.4A Active CN108318060B (en) | 2017-12-29 | 2017-12-29 | 2-micron-waveband three-parameter optical fiber sensor based on inclined optical fiber Bragg grating |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN108318060B (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN109855662B (en) * | 2019-02-28 | 2021-10-15 | 武汉理工大学 | Method and device for quasi-distributed multi-parameter measurement of fiber grating F-P cavity array |
| CN110702148B (en) * | 2019-08-07 | 2022-04-15 | 西安石油大学 | Preparation method and application of optical fiber sensing device capable of simultaneously distinguishing and measuring three parameters |
| CN112146799B (en) * | 2020-09-07 | 2022-09-06 | 桂林电子科技大学 | Optical fiber sensing device for integrated measurement of torsion and humidity |
| CN112146690A (en) * | 2020-09-07 | 2020-12-29 | 桂林电子科技大学 | Multi-parameter measuring device based on double-clad optical fiber |
Family Cites Families (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB201117355D0 (en) * | 2011-10-07 | 2011-11-23 | Isis Innovation | High harmonic optical generator |
| JP2014235007A (en) * | 2013-05-31 | 2014-12-15 | 国立大学法人 宮崎大学 | Device and method for detecting temperature and refractive index of medium |
| CN104764418B (en) * | 2014-01-07 | 2017-09-26 | 中国计量学院 | A kind of distortion measurement sensor based on gold-plated inclined optical fiber grating |
| CN105758827A (en) * | 2016-05-04 | 2016-07-13 | 中国计量大学 | Protein detection fiber optic sensor based on TFBG-SPR |
-
2017
- 2017-12-29 CN CN201711497662.4A patent/CN108318060B/en active Active
Non-Patent Citations (5)
| Title |
|---|
| 2μm掺Tm3+光纤激光器;林佶翔;《中国优秀硕士学位论文全文数据可 信息科技辑》;20090215(第02期);正文的第1-71页 * |
| 倾斜长周期光纤光栅薄膜传感器特性研究;陈海云等;《红外与激光工程》;20131130;第42卷(第11期);第3116-3121页 * |
| 倾角对倾斜光纤光栅光谱特性的影响;高宇飞等;《光学仪器》;20150831;第37卷(第4期);第339-343页 * |
| 李卓.基于45°光栅与可饱和吸收体的2μm锁模光纤激光器.《中国优秀硕士学位论文全文数据库 信息科技辑》.2017,(第02期), * |
| 用单一倾斜光纤光栅实现曲率和温度的同时测量;苗银萍等;《中国激光》;20090930;第36卷(第9期);第2388-2392页 * |
Also Published As
| Publication number | Publication date |
|---|---|
| CN108318060A (en) | 2018-07-24 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Ma et al. | Optical fiber sensors for high-temperature monitoring: a review | |
| Zhao et al. | Relative humidity sensor based on hollow core fiber filled with GQDs-PVA | |
| CN108318060B (en) | 2-micron-waveband three-parameter optical fiber sensor based on inclined optical fiber Bragg grating | |
| Rajan et al. | A fast response intrinsic humidity sensor based on an etched singlemode polymer fiber Bragg grating | |
| Yuan et al. | Tunable polymer fiber Bragg grating (FBG) inscription: fabrication of dual-FBG temperature compensated polymer optical fiber strain sensors | |
| CN107270949B (en) | Temperature and strain dual-parameter sensing system and its measurement method | |
| CN106706030A (en) | Method for realizing simultaneous sensing of temperature, strain and refractive index through single fiber bragg grating | |
| Pan et al. | Parallel-structured Fabry-Perot interferometers gas pressure sensor with ultraviolet glue sensitization based on dual Vernier effect | |
| Mądry et al. | Simultaneous measurement of temperature and relative humidity using a dual-wavelength erbium-doped fiber ring laser sensor | |
| CN205861241U (en) | A kind of based on spherical structure with the fibre optic temperature sensor of hollow optic fibre | |
| Arrizabalaga et al. | Miniature interferometric humidity sensor based on an off-center polymer cap onto optical fiber facet | |
| Liu et al. | Integrated fiber-optic sensor based on inscription of FBG in seven-core fiber for curvature and temperature measurements | |
| CN104132756B (en) | A kind of pressure sensing method utilizing the photonic crystal fiber grating of the bimodal reflectance spectrum of orthogonal polarization modes | |
| Zhu et al. | Ultrasensitive gas pressure sensor based on two parallel Fabry-Perot interferometers and enhanced Vernier effect | |
| CN105675545A (en) | High-sensitivity intensity detection method based on self-interference type micro resonator cavity light sensor | |
| JP5856307B2 (en) | Broadband fiber sensor array | |
| Zhang et al. | Long-period fiber grating humidity sensor based on spider silks | |
| CN209946004U (en) | A Fiber Optic Sensor Based on a Tunable Mach-Zehnder Interferometer | |
| Wahl et al. | Temperature and humidity measurements | |
| Shu et al. | Ultra-sensitive air pressure sensor based on gelatin diaphragm-based Fabry-Peroy interferometers and Vernier effect | |
| CN104777132A (en) | Surrounding refractive index measurement method based on thin cladding long period fiber bragg grating polarization property | |
| CN114486766A (en) | Optical fiber humidity sensor with temperature calibration function | |
| Woyessa et al. | Simultaneous measurement of temperature and humidity with microstructured polymer optical fiber Bragg gratings | |
| Zhu et al. | The measurement of sucrose concentration by two-tapered all-fiber Mach–Zehnder interferometer employing different coupling structures and manufacture processes | |
| CN215678090U (en) | Relative humidity sensor based on polyvinyl alcohol film and annular micro-nano optical fiber |
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 |