CN100419480C - Distributed cone optical-fiber grating sensor, its band width demodulator and detection method - Google Patents
Distributed cone optical-fiber grating sensor, its band width demodulator and detection method Download PDFInfo
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- CN100419480C CN100419480C CNB2006100105278A CN200610010527A CN100419480C CN 100419480 C CN100419480 C CN 100419480C CN B2006100105278 A CNB2006100105278 A CN B2006100105278A CN 200610010527 A CN200610010527 A CN 200610010527A CN 100419480 C CN100419480 C CN 100419480C
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Abstract
This invention relates to distribution tamper fiber grating sensor and its wide modulation device and its test method and to fiber brag grating sensor technique and its spectrum analysis technique field, wherein, the grating sensor is composed of several fiber sections with length as L shape grating and it provides one plane diffraction grating CCD array tamper reflection light band modulation device and can realize tamper fiber grating reflection wide band measurement and its change computation, record and simultaneous measurement.
Description
Technical field
The present invention relates to optical fiber Bragg grating sensing technology and field of spectral analysis technology.
Background technology
Fiber Bragg Grating FBG (FBG) has many outstanding advantages such as electromagnetic interference (EMI) in light weight, corrosion-resistant, anti-, highly sensitive, compact conformation as a kind of wavelength-modulated type sensor, dynamically and in the static measurement field have a wide range of applications at burn into vibration, temperature, stress/strain etc.Simultaneously,, make fiber grating can be used for distributed measurement, and be not subjected to factors such as coupling loss and light source output power fluctuation to accuracy of measurement system and the stable influence that brings to physical quantity because fiber grating has wavelength-modulated.But there is a great problem in fiber-optic grating sensor in practical engineering application, it is the drift that the variation of temperature and stress all can cause its foveal reflex wavelength, but we are difficult to only by the measurement of fiber grating reflection wavelength being distinguished their variations separately, the temperature-stress cross sensitivity problem of Here it is fiber grating.This problem is one of focus in the optical fiber grating sensing field all the time.At this problem, carried out a lot of researchs both at home and abroad, many solutions have also been proposed.But these solutions are used a plurality of fiber gratings or a plurality of light source mostly, the independent demodulation instruments of the many covers of have even needs, cause the raising of sensor-based system overall cost and the complicacy of realization, be unfavorable for the popularization of fiber grating sensing technology in actual engineering.In recent years, in time, has and adopts cone optical-fiber grating to realize that the measuring method of the stress/strain of temperature-insensitive is seen in report, these methods have solved " cross sensitivity problem " with simple structure, lower cost, but the reflected light that these methods all are based on cone optical-fiber grating carries out power measurement, obtain the stress/strain information of institute's sensing then by the variation of this power, they have deviated from the most remarkable characteristic of fiber grating as wavelength-modulated type sensor, make the taper grating can not be used further to realize distributed sensing mode.Simultaneously, the fluctuation of light source output power and the factors such as coupling loss in the light path system all can have influence on the precision and the stability of sensor-based system, if will overcome these influences, then will cause the increase of entire system cost.
Summary of the invention
Existingly carry out the stress/strain information that power measurement obtains institute's sensing in order to solve based on reflected light to cone optical-fiber grating, cause the taper grating can not be used further to realize distributed sensing mode, and senser element is added in the influence of fiber grating and thereby the independent demodulation instrument of many covers causes the baroque problem of sensor apparatus for the variation of difference temperature and stress, the invention provides a kind of distributed cone optical-fiber grating sensor and reflected light bandwidth demodulating equipment thereof, detection method.
Distributed cone optical-fiber grating sensor of the present invention is made of the fiber segment of multistage with diameter, and every section fiber segment contains the taper Bragg grating that length L is, head end, the end of multistage fiber segment are serially connected successively.The taper Bragg grating that every section fiber segment contained is the taper of corroding by along the optical fiber axial linear, and this taper Bragg grating is linear variation along the cross-sectional area of grating orientation.
The reflected light bandwidth demodulating equipment of above-mentioned distributed cone optical-fiber grating sensor, by the collimating optics device, plane diffraction grating, the collecting optics device, line array CCD, CCD controls and reads circuit, A/D change-over circuit and central processing unit are formed, the taper optical grating reflection light of distributed cone optical-fiber grating sensor output incides the light input end of collimating optics device, taper optical grating reflection light is by becoming parallel beam behind the collimating optics device collimation and shining on the plane diffraction grating, light beams of different wavelengths will be along different scattered through angles after the plane diffraction grating beam split, after assembling by the collecting optics device, the light beams of different wavelengths of this different angles scattering shines the sensitization side of line array CCD, at sensitization side acquisition light beams of different wavelengths formed a section or several sections area of illuminations of line array CCD; CCD control and read circuit control and each pixel that is used for line array CCD that link to each other with line array CCD and export reading of analog electrical signal, CCD controls and reads the input end of the output terminal connection A/D change-over circuit of circuit, and the output terminal of A/D change-over circuit connects the ccd signal input end of central processing unit.
Utilize above-mentioned distributed cone optical-fiber grating sensor and based on the detection method of the stress/temperature variation of above-mentioned reflected light bandwidth demodulating equipment, it carries out successively according to the following steps:
Step 1, the reflected light bandwidth demodulating equipment of above-mentioned distributed cone optical-fiber grating sensor is calibrated: 1. determine its stress sensitivity K separately by each taper grating sensor being applied specified stress and temperature respectively
εWith temperature control K
T2. distributed cone optical-fiber grating sensor is applied vertically specified STRESS VARIATION amount, utilize reflected light bandwidth demodulating equipment to know the width of formed a section or several sections area of illuminations of light beams of different wavelengths on the line array CCD then, set up the variation relation of the pairing area of illumination width of different wave length on the stress of distributed cone optical-fiber grating sensor induction and the line array CCD then;
Step 4, the line array CCD the preceding paragraph that obtains according to the analytical calculation of step 3 central processing unit or the width of several sections area of illuminations, the variation relation of the pairing area of illumination width of different wave length is determined each measurement point pairing stress value ε at this moment on the stress that utilizes distributed cone optical-fiber grating sensor that step 1 obtains induction and the line array CCD;
In the following formula, Δ λ
BIt is the drift value of the Bragg grating foveal reflex wavelength asked of step 5; K
εIt is the stress sensitivity coefficient of this taper grating of obtaining of step 1; ε is surveyed stress value by step 4; K
TTemperature control coefficient for this taper grating that step 1 obtained; Δ T is a temperature variation.
Principle of work: the present invention measures on the basis with the feasibility that obtains measured stress/strain information and puts forward taper grating reflection light being carried out spectral width (hereinafter referred to as " bandwidth ").
Known, along Bragg (Prague) reflected wavelength lambda of reflection type optical fiber optical grating axial
B(z) be
λ
B(z)＝2n
eff(z)Λ(z) (1)
In the formula, grating periods lambda and effective refractive index n
EffAll be the function of optical grating axial stress value ε:
Λ(ε)＝Λ
0(1+ε) (2)
n
eff(ε)＝n
eff0+κ
εε (3)
In the formula, κ
εThe factor of expression strain refractive index influence, Λ
0And n
Eff0Be respectively the grating cycle and the effective refractive index of ε=0 o'clock.The stress value ε of ordering at optical grating axial z can be expressed as
ε(z)＝F/EA(z)(4)
In the formula, F is the pulling force that is added in the grating two ends, and E is the optical fiber Young modulus, the cross-sectional area that A (z) is ordered for grating z.
Know that by formula (2) and (3) the Bragg wavelength that optical grating axial z is ordered under strain regime is
λ
B＝2n
eff(ε
z)Λ(ε
z)≈2n
eff0Λ
0+2(n
eff0Λ
0+k
εΛ
0)ε
z (5)
The bandwidth of hence one can see that grating is
Δλ＝λ
B(L)-λ
B(0)+Δλ(δn)(6)
In the formula, λ
B(0), λ
B(L) be the Bragg reflection wavelength at grating head and the tail two ends respectively, Δ λ (δ n) changes the grating bandwidth that causes by grating refractive index.After preparing grating was finished, δ n (z) no longer changed, and its bandwidth Delta lambda that causes (δ n) can not change yet.
When the Bragg grating along axially by after the linearity corrosion, be linear variation along the cross-sectional area of grating orientation, establishing the one end is A (0), the other end is A (L), and A (L)＜A (0).Can be derived by formula (4), (5), (6), when the pulling force at grating two ends was F, the bandwidth of grating was
As can be known by after the linearity corrosion, the bandwidth of grating is linear change with stress, shown in Fig. 3 and 4 by formula (7).For the high light grid, grating corrosion back tension masterpiece time spent, the broadened bandwidth of grating, but the reflective power of each point is constant on the grating, increase so the total reflective power P in the grating bandwidth is linear, total so in the grating bandwidth reflective power P also be linear change with stress, can be expressed as
P＝kF+B (8)
In the formula, k and B are proportionality constants.
When temperature change, the Bragg wavelength change of each point is on the grating
Δλ
B＝(ξ
s+α
s)ΔT (9)
Wherein, ξ
sAnd α
sIt is respectively fiber optic materials thermo-optical coeffecient (7 * 10
-6K
-1) and thermal expansivity.By formula (9) as can be known, temperature change can not influence the variation of optical grating reflection bandwidth or power, as illustrated in Figures 5 and 6
Based on the above-mentioned theory basis, the present invention adopts the bandwidth of measuring taper grating reflection light to determine the STRESS VARIATION amount, thereby the variation difference of temperature and stress is come, and has solved the cross sensitivity problem, measures when having realized temperature and stress; And this measuring method also kept the most remarkable characteristic of fiber grating as wavelength-modulated type sensor, can realize the distributed sensing mode.Because the bandwidth of grating is linear change with stress, the width of the light beams of different wavelengths that then obtains on line array CCD formed a section or several sections area of illuminations also is linear change with stress; So, 1. determine the width of area of illumination and the linear relationship between suffered stress, when actual measurement, can calibrate the result then and know stress value with reference to this by calibration in advance; 2. pass through above-mentioned one section or the several sections specific data processing methods of area of illuminations employing, the drift value of the centre wavelength of the different light beams that comprised in the acquisition cone optical-fiber grating reflected light, can know the stress of ad-hoc location and the common influence that temperature variation is caused, the stress value of being known in from this common influence, removing 1. then, get final product temperature variation.
Invention effect: the invention provides a kind of wide demodulating equipment of taper grating reflection light belt that adopts plane diffraction grating-CCD linear array, it can realize the measurement of cone optical-fiber grating reflectance spectrum bandwidth and calculating, the record of this bandwidth change, and then can realize following purpose on the basis of using the difference in functionality software module: measure in temperature-resistant stress/strain measurement, temperature and the stress, the distributed of distributed measurement, temperature and the stress of stress/strain measure etc. simultaneously.Make the sensing of taper grating pair stress no longer rely on measurement based on demodulating equipment of the present invention to taper optical grating reflection luminous power, the wavelength-modulated characteristics of fiber-optic grating sensor have been recovered, make cone optical-fiber grating can be used for distributed sensing, this sensing mode is influenced by light source fluctuation, coupling loss etc. no longer simultaneously, have demodulation mode simple, that easily realize, good application prospects is arranged.Demodulating equipment proposed by the invention is simple in structure, each function is clear, realizes easily; And can further develop and become an all purpose instrument that volume is less, its input end directly is connected with optical fiber, output terminal can directly be connected with computing machine and carries out further data processing (or divorced from computer and directly use dsp chip to solve the problem of signal Processing), and then output institute desire temperature or the stress/strain value measured.
Description of drawings
Fig. 1 is the structural representation of distributed cone optical-fiber grating sensor of the present invention.Fig. 2 is the structural representation of the reflected light bandwidth demodulating equipment of distributed cone optical-fiber grating sensor of the present invention.Fig. 3 is that stress inferior pyramidal grating reflection spectrum changes synoptic diagram, and horizontal ordinate is represented the central wavelength lambda (nm) of taper optical grating reflection light, and ordinate is represented the pulse amplitude R (dB) of taper optical grating reflection light.Fig. 4 is the wide and stress changing relation synoptic diagram of taper optical grating reflection bands of a spectrum, and horizontal ordinate is represented the centre wavelength (nm) of taper optical grating reflection light, and ordinate is represented the bandwidth change amount (nm) of taper optical grating reflection light ,-◆-expression stress point.Taper grating reflection spectrum changed synoptic diagram when Fig. 5 was temperature variation, and horizontal ordinate is represented the central wavelength lambda (nm) of taper optical grating reflection light, and ordinate is represented the pulse amplitude R (dB) of taper optical grating reflection light.To be that taper optical grating reflection bands of a spectrum are wide concern synoptic diagram with temperature variation to Fig. 6, and horizontal ordinate is represented the centre wavelength (nm) of taper optical grating reflection light, and ordinate is represented the bandwidth change amount (nm) of taper optical grating reflection light ,-zero-expression temperature variation measurement point.
Embodiment
Embodiment one: referring to Fig. 1, this embodiment distributed cone optical-fiber grating sensor, the mountain multistage constitutes with the fiber segment 1 of diameter, and every section fiber segment 1 contains the taper Bragg grating 2 that length is L, and head end, the end of multistage fiber segment 1 are serially connected successively.The taper Bragg grating 2 that every section fiber segment 1 is contained is the tapers of corroding by along the optical fiber axial linear, and this taper Bragg grating 2 is linear variation along the cross-sectional area of grating orientation.Fiber segment 1 adopts single-mode fiber.The preparation method of every section fiber segment 1 of this embodiment is: utilize the phase mask method to write uniform Prague (Bragg) fiber grating at the single-mode fiber upside of handling through high ballast hydrogen, the grating reflection rate all is higher than 99%; Behind the grating high annealing, the bandwidth of grating and reflectivity no longer change with temperature and time; Grating after will annealing then immerses in the HF acid solution, at the uniform velocity pulls out from HF acid.Because the speed of corrosion was directly proportional with the time, so the xsect of grating was linear change after grating was corroded.In this embodiment, we erode to D (L)=90 μ m with the diameter of fiber segment from D (0)=125 μ m, and L represents the length of Bragg grating.
Embodiment two: referring to Fig. 2, the reflected light bandwidth demodulating equipment of the described distributed cone optical-fiber grating sensor of embodiment one is by collimating optics device 4, plane diffraction grating 6, collecting optics device 5, line array CCD 7, CCD controls and reads circuit 8, A/D change-over circuit 9 and central processing unit 10 are formed, the taper optical grating reflection light of distributed cone optical-fiber grating sensor 3 outputs incides the light input end of collimating optics device 4, taper optical grating reflection light becomes parallel beam after by collimating optics device 4 collimation and shines on the plane diffraction grating 6, after plane diffraction grating 6 beam split, obtain light beams of different wavelengths along the different angles scattering, after assembling by collecting optics device 5, the light beams of different wavelengths of this different angles scattering incides the sensitization side of line array CCD 7, at sensitization side acquisition light beams of different wavelengths formed a section or several sections area of illuminations of line array CCD 7; CCD control and read circuit 8 control and each pixel that is used for line array CCD 7 that link to each other with line array CCD 7 and export reading of analog electrical signal, CCD controls and reads the input end of the output terminal connection A/D change-over circuit 9 of circuit 8, and the output terminal of A/D change-over circuit 9 connects the ccd signal input end of central processing unit 10.Described collimating optics device 4 adopts collimation lens set.Described collecting optics device 5 adopts convex lens.
Described plane diffraction grating 6 adopts the plane grating of 600 lines/mm, and generally speaking, the line number is high more, and precision is high more.Described line array CCD 7 can adopt the line array CCD device of 2048 pixels, as the TCD142D of Toshiba Corp's production; The resolution of the high more then demodulating equipment of the contained pixel number of line array CCD is high more; The spectral range of long more then its energy demodulation of the length of ccd array is big more, thereby reusable grating number is many more in the sensor-based system.CCD control and read circuit 8 and realize the driving of line array CCD 7 and reading of output signal, it provides work schedule and reads the opto-electronic conversion output signal of CCD by certain time sequence for CCD, adopts current techique.A/D change-over circuit 9 adopts 12 A/D transition cards, as the grand PCI-7422 that opens up the production of observing and controlling company in Beijing.Central processing unit 10 carries out the demodulating equipment data processing, and to obtain needed heat transfer agent, it can adopt computer programming or dsp chip (digital signal processor) to realize, as the TMS320 series of TI company.
Embodiment three: referring to Fig. 1 and 2, utilize embodiment one described distributed cone optical-fiber grating sensor and, carry out according to the following steps successively based on the detection method of the stress/temperature variation of the reflected light bandwidth demodulating equipment of embodiment two described distributed cone optical-fiber grating sensors:
Step 1, the reflected light bandwidth demodulating equipment of embodiment two described distributed cone optical-fiber grating sensors 3 is calibrated: 1. determine its stress sensitivity K separately by each taper grating sensor being applied specified stress and temperature respectively
εWith temperature control K
T2. distributed cone optical-fiber grating sensor 3 is applied vertically specified STRESS VARIATION amount, utilize reflected light bandwidth demodulating equipment to know the width of formed a section or several sections area of illuminations of light beams of different wavelengths on the line array CCD 7 then, set up the variation relation of the pairing area of illumination width of different wave length on the stress of distributed cone optical-fiber grating sensor 3 inductions and the line array CCD 7 then;
Step 4, line array CCD 7 the preceding paragraphs that obtain according to 10 analytical calculations of step 3 central processing unit or the width of several sections area of illuminations, the variation relation of the pairing area of illumination width of different wave length is determined each measurement point pairing stress value ε at this moment on the stress that utilizes distributed cone optical-fiber grating sensor that step 1 obtains 3 induction and the line array CCD 7;
In the following formula, Δ λ
BIt is the drift value of the Bragg grating foveal reflex wavelength asked of step 5; K
εIt is the stress sensitivity coefficient of this taper grating of obtaining of step 1; ε is surveyed stress value by step 4; K
TTemperature control coefficient for this taper grating that step 1 obtained; Δ T is a temperature variation.The inventive method is based on and designs on the basis of embodiment two, and is simple, practical.
Claims (7)
1. distributed cone optical-fiber grating sensor, it is characterized in that described distributed cone optical-fiber grating sensor is made of the fiber segment (1) of multistage with diameter, every section fiber segment (1) contains the taper Bragg grating (2) that length is L, and head end, the end of multistage fiber segment (1) are serially connected successively.
2. distributed cone optical-fiber grating sensor according to claim 1, it is characterized in that the taper Bragg grating (2) that every section fiber segment (1) is contained is the taper of corroding by along the optical fiber axial linear, this taper Bragg grating (2) is linear variation along the cross-sectional area of grating orientation.
3. distributed cone optical-fiber grating sensor according to claim 1 is characterized in that fiber segment (1) adopts single-mode fiber.
4. the reflected light bandwidth demodulating equipment that comprises the described a kind of distributed cone optical-fiber grating sensor of claim 1, it is characterized in that described reflected light bandwidth demodulating equipment is by collimating optics device (4), plane diffraction grating (6), collecting optics device (5), line array CCD (7), CCD controls and reads circuit (8), A/D change-over circuit (9) and central processing unit (10) are formed, the taper optical grating reflection light of distributed cone optical-fiber grating sensor (3) output incides the light input end of collimating optics device (4), taper optical grating reflection light is by becoming parallel beam behind collimating optics device (4) collimation and shining on the plane diffraction grating (6), after plane diffraction grating (6) beam split, obtain light beams of different wavelengths along the different angles scattering, after assembling by collecting optics device (5), the light beams of different wavelengths of this different angles scattering shines the sensitization side of line array CCD (7), at sensitization side acquisition light beams of different wavelengths formed a section or several sections area of illuminations of line array CCD (7); CCD control and read circuit (8) control and each pixel that is used for line array CCD (7) that link to each other with line array CCD (7) and export reading of analog electrical signal, CCD controls and reads the input end of the output terminal connection A/D change-over circuit (9) of circuit (8), and the output terminal of A/D change-over circuit (9) connects the ccd signal input end of central processing unit (10).
5. the reflected light bandwidth demodulating equipment of distributed cone optical-fiber grating sensor according to claim 4 is characterized in that described collimating optics device (4) adopts collimation lens set.
6. the reflected light bandwidth demodulating equipment of distributed cone optical-fiber grating sensor according to claim 4 is characterized in that described collecting optics device (5) adopts convex lens.
7. the reflected light bandwidth of a distributed cone optical-fiber grating sensor is reconciled the Device Testing method, uses the described device test right of claim 4 to require 1 the catoptrical method of sensor, it is characterized in that described method carries out successively according to the following steps:
Step 1, the reflected light bandwidth demodulating equipment of the described distributed cone optical-fiber grating sensor of claim 4 (3) is calibrated: 1. determine its stress sensitivity K separately by each taper grating sensor being applied specified stress and temperature respectively
εWith temperature control K
T2. distributed cone optical-fiber grating sensor (3) is applied specified STRESS VARIATION amount vertically, utilize reflected light bandwidth demodulating equipment to know that line array CCD (7) goes up the width of formed a section or several sections area of illuminations of light beams of different wavelengths then, set up the stress of distributed cone optical-fiber grating sensor (3) induction and the variation relation of the last pairing area of illumination width of different wave length of line array CCD (7) then;
Step 2, the described distributed cone optical-fiber grating sensor of claim 1 (3) is imbedded interior of articles that needs monitoring or the surface that sticks to member to be measured, a taper Bragg grating is positioned at the measurement point of a needs monitoring, the centre wavelength of a plurality of taper Bragg gratings is all different in the distributed cone optical-fiber grating sensor (3), and the distance between the foveal reflex wavelength of adjacent conical Bragg grating will guarantee that the reflected light of adjacent conical Bragg grating does not disturb mutually;
Step 3, make the taper optical grating reflection light of distributed cone optical-fiber grating sensor (3) output incide in the reflected light bandwidth demodulating equipment of above-mentioned distributed cone optical-fiber grating sensor (3) by collimating optics device (4), from distributed cone optical-fiber grating sensor (3) folded light beam that obtains is the light pulse that contains the different centre wavelengths with certain bandwidth of each measurement point temperature and STRESS VARIATION information, this light pulse is by collimating optics device (4), plane diffraction grating (6), collecting optics device (5) is at one section or several sections area of illuminations of the sensitization side formation of line array CCD (7), utilize CCD control and read circuit (8), A/D change-over circuit (9) is gathered the image information of line array CCD (7), utilizes the reflectance spectrum information of central processing unit (10) analytical calculation distributed cone optical-fiber grating sensor (3) and the width of line array CCD (7) the preceding paragraph or several sections area of illuminations;
Step 4, line array CCD (7) the preceding paragraph that obtains according to step 3 central processing unit (10) analytical calculation or the width of several sections area of illuminations, utilize the stress of distributed cone optical-fiber grating sensor that step 1 obtains (3) induction and the variation relation that line array CCD (7) is gone up the pairing area of illumination width of different wave length, determine each measurement point pairing stress value ε this moment;
Step 5, the reflectance spectrum information that obtains according to step 3 central processing unit (10) analytical calculation are determined the drift value of the Bragg grating foveal reflex wavelength of each point;
Step 6, for each measurement point, the stress sensitivity K that utilizes in the step 1 to be obtained
εWith temperature control K
T, the drift value of the Bragg grating foveal reflex wavelength asked of step 5 and the measurement point stress value ε that step 4 obtains, can obtain the variation of temperature amount by following formula, thereby temperature and stress difference are come:
In the following formula, Δ λ
BIt is the drift value of the Bragg grating foveal reflex wavelength asked of step 5; K
εIt is the stress sensitivity coefficient of this taper grating of obtaining of step 1; ε is surveyed stress value by step 4; K
TTemperature control coefficient for this taper grating that step 1 obtained; Δ T is a temperature variation.
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| CN102147362B (en) * | 2010-12-10 | 2012-11-14 | 中国计量学院 | Temperature self-compensation FBG (Fiber Bragg Grating) refractive index sensor based on conical corrosion |
| CN102445222A (en) * | 2011-09-23 | 2012-05-09 | 北京交通大学 | Conical fiber grating-based sensing demodulation system |
| CN108593119B (en) * | 2018-04-11 | 2020-10-30 | 南京大学 | Continuous distributed microstructure optical fiber biochemical sensor and signal processing method |
| CN111006600A (en) * | 2019-10-31 | 2020-04-14 | 中国空间技术研究院 | System for measuring satellite temperature and deformation quantity by using fiber bragg grating |
| CN112525328A (en) * | 2020-11-30 | 2021-03-19 | 北京遥测技术研究所 | PSD-based fiber bragg grating vibration sensor demodulation system and method |
| CN115756012A (en) * | 2022-11-30 | 2023-03-07 | 威海激光通信先进技术研究院 | Device and method for controlling temperature gradient of satellite laser communication terminal |
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| CN1329716A (en) * | 1998-12-04 | 2002-01-02 | 塞德拉公司 | Strain-isolated bragg grating temperature sensor |
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| US6490931B1 (en) * | 1998-12-04 | 2002-12-10 | Weatherford/Lamb, Inc. | Fused tension-based fiber grating pressure sensor |
| US20040182166A1 (en) * | 2003-03-21 | 2004-09-23 | Jones Richard Todd | Optical differential pressure transducer utilizing a bellows and flexure system |
| CN1563901A (en) * | 2004-03-12 | 2005-01-12 | 吉林大学 | Stress strain sensor based on temp insensitiveness of fiber glass raster |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1329716A (en) * | 1998-12-04 | 2002-01-02 | 塞德拉公司 | Strain-isolated bragg grating temperature sensor |
| CN1334920A (en) * | 1998-12-04 | 2002-02-06 | 塞德拉公司 | Bragg grating pressure sensor |
| US6490931B1 (en) * | 1998-12-04 | 2002-12-10 | Weatherford/Lamb, Inc. | Fused tension-based fiber grating pressure sensor |
| US20040182166A1 (en) * | 2003-03-21 | 2004-09-23 | Jones Richard Todd | Optical differential pressure transducer utilizing a bellows and flexure system |
| CN1563901A (en) * | 2004-03-12 | 2005-01-12 | 吉林大学 | Stress strain sensor based on temp insensitiveness of fiber glass raster |
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