Title: Fiber Optic Grating Sensors and Applications
1 Fiber Optic Grating Sensors and Applications
Blue Road Research
2Criteria for a Successful Fiber Optic Sensor
Application
- Meets and important application need
- Is unique, superior solution
- Is economically compelling
3Fiber Grating Sensors
- Key parameters - strain and temperature
- Competitive technology - electrical resistive
strain gauges and thermocouples/low cost (20) -
well known, difficult to embed and successfully
operate - Today - fiber gratings are high cost items (200
each) being used to measure strain and
temperature in embedded materials - The future - cost competitive with electrical
strain gauges with options for 3 axis strain
measurement, environmentally superior performance
4Fiber Grating Sensor Prospects
- Fiber gratings are likely to drop into the 25 to
40 range for small quantity buys in two to three
years enabling direct competitiveness with
electrical strain gauges.
5Fiber Grating - Holographic Method
6Fiber Grating - Phase Mask Method
7Means to Write Fiber Gratings
- Long exposure side imaged interference pattern
- United technology / operates to approximately 500
deg C - Good spectral characteristics /reflectance
- Short pulse side imaged interference pattern
- Naval Research Lab / operates to 800 deg C
- Demonstrated manufacture during draw
- First gratings low of quality
8Means to Write Fiber Gratings(continued)
- Phase masks
- Moderate temperature
- Good performance
- Canadian Communication Research Center
- Line by line
- Higher temperature to 800 deg C
- Canadian Communication Research Center
- Phase masks / bending fiber
- Brown University / Bragg Technology
- Wider bandwidth, good performance
9Major Historical Milestones
- K.O. Hill, CRC 1978, discovery of
photosensitivity. - Lam and Garside, McMaster U. 1981, observed
photosensitivity as a two photon effect. - Meltz, Morey, and Glenn, UTRC 1989, side writing
technique with UV laser. - Hill and Snitzer, CRC and Rutgers 1993, mask
technique for writing fiber gratings. - LeMaire, ATT 1993, Hydrogen loading.
- Archambault, Reekie, Russell, Southampton U.
1993, single pulse, type 2 grating, and draw
tower exposure.
(Source - 3M Bragg Grating Technologies)
10Bragg Grating Exposure
(Source - 3M Bragg Grating Technologies)
11Photoinduced Index Change
120.1 Chirp, Peaks at 0.25 and 0.75L
13Grating Reflection with 1nm Bandwidth and Reduced
Sidelobes
14Coupling to Cladding Modes with 4o Blaze
15Wavelength-Selective Light Coupling from Fibers
with Bragg Gratings
16Bandpass Filter with Fiber Gratings in Michelson
Arrangement
17Transmission of Fiber Bragg Grating Pair as
Fabry-Perot Interferometer
18External Cavity Laser Diode
(Source - 3M Bragg Grating Technologies)
19External Cavity Laser Diode
(Source - 3M Bragg Grating Technologies)
20Temperature Relation for Grating Sensors
- ?? / ? ( ? ? ) ?T
- ? expansion coefficient
- 0.55x10-6 oC-1 for silica
- ? thermooptic coefficient for fiber core
material - 8.31x10-6 oC-1 estimated for GeO2
doping - ?? / ? 8.86x10-6 ?T
- ?? 0.0073 nm/oC at 820 nm
- From S. Tahahashi and S. Shibata,
- Journal of Non-Crystalline Solids 30(1979)
359-370
21Strain Relation for Grating Sensors
- ?? / ? (1 - pe) ?
- pe photoelastic constant
- (n2 / 2)p12 - ?(p11 p12) 0.22
for silica - ?? / ? 0.78 ?
- ?? 6.4 nm / 1 at 820 nm
22Fiber Grating Wavelength Shift
(Source - 3M Bragg Grating Technologies)
23Reflectivity Over Test Period at 650 oC
24Bandwidth Over Test Period at 650 oC
25Transmission Plots Before and After High
Temperature Exposure
(Source - 3M Bragg Grating Technologies)
26Temperature and Strain Cycling
- Use preannealed FBG
- 4 hour cycles, 21 oC to 427oC
- 512 cycles over 2048 hr..
- No change measured in FBG spectrum
- Apply dynamic strain in tension load
- Maximum strain 2500 microstrain
- 1.4 million cycles
- No change measured in FBG spectrum
27Fiber Grating Demodulators
- Open loop versus closed loop
- Open loop single grating approach requires
broadband grating - Brown University is working on broadband chirped
gratings - PZT stacks and designs for adequate modulation
exist at modest voltages
28Low Cost Approaches
- Overcoupled coupler
- Miniature Mach-Zehnder
- Fiber grating spectral filter
29Overcoupled Beamsplitter Layout
30Overcoupled Coupler Issues
- Thermal drift more severe with higher sensitivity
- Polarization mixing issues
- Packaging of sensitive devices
- very long overcoupled couplers are fragile
31Miniature Mach-Zehnder
- More rugged than overcoupled coupler approach
with comparable sensitivity - Superior thermal and polarization properties to
overcoupled coupler - Smooth spectral profile
- Needs further thermal and polarization
improvements - close to ready
32Grating Sensor with Fiber-Interferometric
Wavelength Discriminator
33Fiber Grating Spectral Filter
- Can be tailored to match desired dynamic range
and sensitivity - Athermal package for operation over -40 to 80 oC
(less than 0.1 nm drift) - Relatively polarization independent
- Suitable for a demodulator with approximately 100
microstrain sensitivity and /- 5000 microstrain
range
34Fiber Grating Spectral Filter Demodulator
35Chirped Fiber Grating Spectral Filter
361550 nm Grating Demodulation Kit
- 1550 nm ELED light source
- (2) 3 dB beamsplitters
- Chirped fiber grating filter
- (2) receivers
- Patch cords
- FC connector cleaner
- 1 single axis grating sensor
- Data CD with manual
- Optional DAQ card software
- Optional Carrying case
37High Speed Grating Demodulators
- Stand-alone configuration
- Three bandwidth options
- 1kHz, 10 kHz, 2 MHz
- Flexible design for varied applications
- Integrated light source and spectral filters
38Fiber Grating System
39Fiber Fabry-Perot Tunable Filters
40Fabry-Perot Detector/Fiber
41Fiber Bragg Grating Sensor Array with Fiber
Fabry-Perot Demodulator
42Shift in FFP Control Voltage and Bragg Wavelength
with Applied Strain to FBG Sensor Element
43Bragg Grating Axial Strain and Temperature Sensor
- Measures ?T and ?1 for surface mounted
applications - Overlaid Bragg gratings at two wavelengths
- 850 and 1300 nm
- Output spectrum contains two peaks
- ?b1 f1(?1,?T) and ?b2 f2(?1,?T)
44Multi-Parameter Bragg Grating
- Two overlaid Bragg gratings created in
birefringent fiber - ?1, ?2
- Birefringent fiber can transmit two orthogonal
polarization modes - p,q
- Reflected spectrum will contain four peaks
- ?p1, ?q2, ?p2, ?q2
- Four peaks can be used to determine three axis of
strain and temperature - ?1, ?2, ?3, ?T
45Bragg Grating in Birefringent Fiber
- Two polarization modes with different values of n
(np, nq) - Two distinct Bragg peaks
46Response of Birefringent Fiber to Applied Strain
and Temperature
- When the fiber is subjected to ? or ?T, ? will
shift due to change in d (elongation) and n
(stress-optic effect)
47Response of Birefringent Fiber to Applied Strain
and Temperature
- If we assume ?230, the equations are linear in ?
and ?T
483 Axis Strain and Temperature
49Two Overlaid Gratings in Birefringent Fiber
- If we add a second grating to the fiber at a
different wavelength, we will obtain two
additional peaks in the reflected spectrum - The response of these new peaks will be different
due to the wavelength dependence of fiber
properties (pij, etc.) - The response of the four peaks to strain and
temperature can be expressed as
50Determining Three Axes of Strain and Temperature
- Provided K is well conditioned, we can determine
the strains (?1, ?2, ?3) and temperature (?T)
from the change in wavelength of the four peaks
using
51Experimental Setup to Test the Three Axis Strain
and Temperature Sensor
52Experimental Setup to Test the Three Axis Strain
and Temperature Sensor
53Axial Loading of 3 Axis Fiber Grating Sensor
54Transverse Loading of 3 Axis Fiber Grating Sensor
55Transverse Loading of 3 Axis Fiber Grating Sensor
56Transverse Loading of 3 Axis Fiber Grating Sensor
573 Axis Demodulation Kit
58Possible Applications of 3 Axis Sensor
- Aerospace
- Biomedical
- Geotechnical
- Civil structures
59Civil Structure Applications for 3 Axis Sensor
60Civil Structure Applications for 3 Axis Sensor
(continued)
61Civil Structure Applications for 3 Axis Sensor
(continued)
62Long Period Fiber Gratings
- Temperature dependence 0.04 to 0.05 nm/ oC (short
period grating is about 0.01nm/oC) - Strain dependence very fiber specific, examples
Grating A - 0.7 nm/m?, Grating B - 1.5 nm/m?
(short period gratings are 1.0 to 1.8 nm/m? for
the 1.3 to 1.5 micron range) - Extremely sensitive to bending which can override
the grating - Reference Vengsarker et al, JLT, p.53, Jan 96