Light power (μW) Wavelenght (nm) Strain and Temperature Measurement with Optical Fiber Bragg Grating Sensor What is a fiber Bragg grating ? • linear measurement, relative signal (no calibration) • high temperature and strain sensitivity • multiplexing capabilities • long term stability • immune to electromagnetic interference • flexibility and small diameter => embedding in structure possible • independent of the intensity of the light (spectral measurement) Principle of the sensors Experimental validation Experimental measurement device Contact: Laurent Robert ([email protected]) - Jean-José Orteu ([email protected]) Intensity Intensity Incident spectrum reflective spectrum Optical cladding Core FBG n°1 FBG n°2 FBG n°3 transmitted spectrum Intensity Refraction index Photosensitivity of silica: a UV pattern is printed into the fiber core as index variation • Periodical structure of pitch Λ formed by refractive index (n) variation of the core • Characteristic wavelength of the grating: λ b =2 n Λ • Variation of the Bragg wavelength (hypothesis: isotropic optical fiber under uniaxial longitudinal strain ε): , a, b and c constant • In detail, thermal variation: • In detail, longitudinal strain: P c b T a b b Δ + ε + Δ = λ λ Δ Δλ bT λ b = aΔT = ( α + ξ )ΔT Δλ b λ b = 1 − n 2 2 ρ 12 − νρ 11 + ρ 12 ( ) [ ] ε = 1 − p e ( ) ε = bε Grating inscription Tunable light source Powermeter Coupleur Y com2 RS232 com1 RS232 PC labview T and/or strain solicitation FBG embedded in a media Peak extraction: minimization (Levenberg-marquardt) of ( ) 2 2 B W 2 0 Ie I ) f( λ − λ − + = λ Maximum resolution : 1pm <=> 0,1°C or 1µε Bare FBG submitted to temperature Bare FBG submitted to tension FBG stuck on the surface of a specimen - comparison with strains measured by mechanical extensometer and full field strain measure (stereocorrelation) FBG embedded with epoxy resin in a groove - comparison with strains measured by mechanical extensometer and strain gauge Temperature variation of the Bragg wavelength for stuck and embedded FBGs: sensibility depends on the material Advantages n and Λ depend on temperature, strain, pressure => can be used as a sensor • holographic method: the fiber is positioned under classical interferometric fringes • phase mask method: the fiber is positioned under the interferometric fringes obtained by the one order diffraction produced by the mask • need temperature and strain discrimination • birefringence phenomena induced by radial strains • FBG embedded in complex media needs numerical simulation Metrological performances (1550 nm): • -100 < T < 500 °C • 0.1 < P < 100 MPa range • 10 -4 % < ε < 2 % • Thermal: 12 pm / °C • Strain: 1,2 pm / µε • Hydrostatic pres.: -4,5 pm / MPa sensitivity References: techniques de l’ingénieur (P. Ferdinand, R6 735, R2 802, M. Lequime R 460), S. Vacher (PhD Thesis, ENSMSE, St-Etienne, 2004) Applications: structural health monitoring of civil construction, intelligent sensing for innovative structures, composite (aeronautic) structure, seismology, medical and chemistry, measures and controls during industrial process, … :

Strain and Temperature Measurement with Optical Fiber ...jeanjose/CROMeP/posters/poster_FB… · fiber core as index variation • Periodical structure of pitch Λ formed by refractive

Download PDF Report

Upload
others
View
2
Download
0

Embed Size (px)

Citation preview

$Page 1: Strain and Temperature Measurement with Optical Fiber ...jeanjose/CROMeP/posters/poster_FB… · fiber core as index variation • Periodical structure of pitch Λ formed by refractive$

Ligh

t pow

er (µ

Wavelenght (nm)

Strain and Temperature Measurement withOptical Fiber Bragg Grating Sensor

What is a fiber Bragg grating ?

• linear measurement, relative signal(no calibration)

• high temperature and strain sensitivity

• multiplexing capabilities

• long term stability

• immune to electromagneticinterference

• flexibility and small diameter =>embedding in structure possible

• independent of the intensity of thelight (spectral measurement)

Principle of the sensors

Experimental validation

Experimental measurement device

Contact: Laurent Robert ([email protected]) - Jean-José Orteu ([email protected])

Intensity

Incidentspectrum

reflectivespectrum

Optical cladding Core

FBG n°1

FBG n°2

FBG n°3

transmittedspectrum

Intensity

Ref

ract

ion

inde

Photosensitivity of silica: a UV pattern is printed into thefiber core as index variation

• Periodical structure of pitch Λ formed by refractive index (n) variation of the core

• Characteristic wavelength of the grating: λb=2 n Λ

• Variation of the Bragg wavelength (hypothesis: isotropic optical fiber under uniaxial

longitudinal strain ε): , a, b and c constant

• In detail, thermal variation:

• In detail, longitudinal strain:

PcbTab

b Δ+ε+Δ=λ

λΔ

€

ΔλbTλb

= aΔT = (α + ξ)ΔT

€

Δλbλb

= 1 − n2

2ρ12 − ν ρ11 + ρ12( )[ ]

ε = 1 − pe( )ε = bε

Grating inscription

Tunable light source

Powermeter Coupleur Ycom2

RS232

com1

RS232

PC labview

T and/or strainsolicitation

FBGembeddedin a media

Peak extraction: minimization(Levenberg-marquardt) of

( )2

W20 IeI)f(

λ−λ−

+=λ

Maximum resolution : 1pm <=> 0,1°C or 1µε

Bare FBG submitted to temperature

Bare FBG submitted to tension FBG stuck on the surfaceof a specimen -comparison with strainsmeasured by mechanicalextensometer and fullfield strain measure(stereocorrelation)

FBG embedded withepoxy resin in a groove -comparison with strainsmeasured by mechanicalextensometer and straingauge

Temperature variation of the Bragg wavelengthfor stuck and embedded FBGs: sensibilitydepends on the material

Advantages

n and Λ depend on temperature, strain,pressure => can be used as a sensor

• holographic method: thefiber is positioned underclassical interferometricfringes

• phase mask method: thefiber is positioned underthe interferometric fringesobtained by the one orderdiffraction produced bythe mask

• need temperature and strain discrimination

• birefringence phenomena induced by radial strains

• FBG embedded in complex media needsnumerical simulation

Metrological performances (1550 nm):• -100 < T < 500 °C• 0.1 < P < 100 MPa range

• 10-4 % < ε < 2 %

• Thermal: 12 pm / °C• Strain: 1,2 pm / µε• Hydrostatic pres.: -4,5 pm / MPa

sensitivity

References: techniques de l’ingénieur (P. Ferdinand, R6 735, R2 802, M. Lequime R 460), S. Vacher (PhD Thesis, ENSMSE, St-Etienne, 2004)

Applications: structural health monitoring of civil construction, intelligent sensing forinnovative structures, composite (aeronautic) structure, seismology, medical andchemistry, measures and controls during industrial process, …