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SU ZA IRI BIN DAUD

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SUZAIRI BIN DAUD

A thesis submitted in fulfillment o f the requirements for the award o f the degree of

Master o f Science (Physics)

Faculty o f Science Universiti Teknologi Malaysia

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A C K N O W LE D G E M E N T

Praised be to Allah s . w . t . Peace and Blessing be to Prophet Muhammad s.a.w...

In the preparation o f this thesis, I was in contact with numerous researchers and academicians. They have contributed towards my understanding and thoughts of the Physics o f sensors. In particular, I wish to express my sincere appreciation and gratitude to my main supervisor, Prof. Dr. Jalil Ali, for his encouragement, guidance, and friendship. I am also very thankful to my co-supervisor, Dr. Saktioto for his guidance and motivations. W ithout their continued support and interest, the completion o f thesis would definitely be impossible.

I wish to express my sincere thanks to the staff o f Photonics Research Laboratory, Fibre Optics Laboratory, Optoelectronics Laboratory, librians o f PSZ, and all staffs from Institute o f Advanced Photonics Science and Faculty o f Science, UTM, especially Mr. Ab. Rasid Isnin and Mr. Nasir Abu Bakar, for their help and cooperation. My sincere appreciation also extends to all my friends who have provided assistance and various occasions. Their views and suggestions have been useful indeed.

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A BSTRA CT

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A BSTR A K

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C H A P T E R T IT L E PA G E

D EC LA R A TIO N ii

D ED IC A TIO N iii

A C K N O W LE D G E M E N T iv

A B STR A C T v

A BSTRA K vi

TA BLE O F C O N TEN TS vii

L IST O F TABLES x

L IST O F F IG U R ES xi

L IST O F SYM BOLS xiii

L IST O F A PPEN D IC ES xvi

1 IN T R O D U C TIO N 1

1.1 Introduction 1

1.2 Background o f Study 2

1.3 Problem Statements 4

1.4 Objective 4

1.5 Scope o f Study 4

1.6 Significance o f Study 5

1.7 Organization o f Study 5

LIT E R A T U R E R E V IE W 2.1 Introduction

2.2 Historical Perspective of Fibre Bragg Grating

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2.3 Fibre Bragg Grating 8

2.4 Fibre Bragg Grating as a Sensor 10

2.5 Overview o f Fibre Bragg Grating for Temperature Sensing 11 2.6 Advantages o f Fibre Bragg Grating Sensor 13 2.7 Sun Radiation and Spectral Wavelength 15 2.7.1 Composition o f Solar Radiation 16

3 T H E O R Y 17

3.1 Introduction 17

3.2 Coupled-Mode Theory 17

3.2.1 Coupled-Mode Equations 19

3.2.2 Coupling Coefficient 20

3.3 Principle o f Fibre Bragg Grating 22

3.4 Properties o f Fibre Bragg Grating 22

3.4.1 Bragg W avelength 23

3.4.2 Bragg Grating Bandwidth 24

3.4.3 Bragg Grating Reflectivity 26

3.5 Optical Response o f Fibre Bragg Grating 28 3.5.1 Optical Response to Wavelength 29

3.5.2 Optical Response to Strain 29

3.5.3 Optical Response to Temperature 31 3.6 Characteristics o f Fibre Bragg Grating 32

3.6.1 Bragg Condition 33

3.6.2 Transmission and Reflection in Fibre Bragg Grating 34

3.6.3 Effective Refractive Index 35

3.6.4 Grating Period 36

4 EX PE R IM E N T A L SET-U P 37

4.1 Introduction 37

4.2 M easurement o f Fibre Loss 37

4.3 Design o f Fibre Bragg Grating Temperature Sensing 39

4.3.1 Tunable Laser Source 40

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4.3.3 Fibre Optic Coupler 42 4.4 M easurement o f Fibre Bragg Grating for Temperature

Sensing 43

4.4.1 M easurement o f Transmission Spectrum 43 4.4.2 M easurement o f Reflection Spectrum 44

5 R ESU L T AND D ISCU SSIO N 47

5.1 Introduction 47

5.2 Fibre Loss M easurement 47

5.2.1 Fibre Loss M easurement by Experiment 48 5.2.2 Fibre Loss M easurement by Calculation 48 5.3 FBG Reflection and Transmission Spectra at Room

Temperature 50

5.4 Result o f Fibre Bragg Grating for Temperature Sensing 52 5.4.1 Effect o f Different Placement Height on FBG

Sensitivity 56

5.4.2 Effect o f Focusing Element on FBG Sensitivity 58 5.4.2.1 Effect o f Convex Lens Focusing on FBG

Sensitivity 59

5.4.2.2 Effect o f Hand Lens Focusing on FBG

Sensitivity 60

5.4.2.3 Comparison o f Different Focusing Elements 62 5.4.3 Bandwidth o f Fibre Bragg Grating 65 5.4.6 Reflectivity o f Fibre Bragg Grating 66

5.5 Interpretation and Discussion 67

6 C O N C LU SIO N 70

6.1 Conclusion 70

6.2 Recommendation for Future W ork 71

R E FE R E N C E S Appendices A-I

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L IS T O F TABLES

TA BLE NO. T IT L E PA G E

Table 4.1 Details o f focusing elements 39

Table 5.1 Power meter reading o f fibre loss 48

Table 5.2 Sensitivity o f the FBG at different height 58 Table 5.3 Effect o f focusing convex lens on the sensitivity o f FBG at

different placement height from the rooftop floor 60 Table 5.4 Effect o f focusing convex lens on the sensitivity o f FBG at

different positions from the rooftop floor 62

Table 5.5 Sensitivities o f FBG for different focusing elements based on

transmission spectrum 65

Table 5.6 Sensitivities o f FBG for different focusing elements based on

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FIG U R E NO. T IT L E PA G E

Figure 2.1 Reflected and transmitted light in the FBG 9

Figure 2.2 The FBG system 10

Figure 3.1 Illustration o f contradirectional coupling 18

Figure 3.2 Schematic o f enlarge FBG 23

Figure 3.3 Calculation o f FWHM using reflection spectrum 24

Figure 3.4 The FBG system 32

Figure 3.5 Transmission and reflection in FBG 35

Figure 4.1 Experimental set-up for fibre loss measurement 38 Figure 4.2 Schematic o f the basic experimental set-up 39

Figure 4.3 Tunable Laser Source model MG9638A 40

Figure 4.4 Optical Spectrum Analyzer model MS9710B 41

Figure 4.5 3-dB fibre optic coupler 42

Figure 4.6 Schematic o f experimental set-up to measure transmission spectrum44 Figure 4.7 Schematic o f experimental set-up to measure reflection spectrum 45

Figure 4.8 Close-up o f the experimental set-up 46

Figure 4.9 Experimental set-up for FBG temperature sensing 46 Figure 5.1 Reflection spectrum provided by the manufacturer, QPS

Photonics Inc, Canada 50

Figure 5.2 Reflection spectrum at 23 °C 51

Figure 5.3 Transmission spectrum at 23 °C 51

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Figure 5.6 Shift o f Bragg wavelength in different temperature for transmission

spectrum 57

Figure 5.7 Shift o f Bragg wavelength in different temperature for reflection spectrum

Figure 5.8 Effect o f a focusing convex lens on the Bragg wavelength for

different temperature from the transmission spectrum 59 Figure 5.9 Effect o f focusing convex lens on the Bragg wavelength shift from

the reflection spectrum 59

Figure 5.10 Effect o f hand lens focusing on the Bragg wavelength shift at

different temperature obtained from the transmission spectrum 61 Figure 5.11 Effect o f hand lens focusing on the Bragg wavelength shift at

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a - Core radius

b - Wavelength position at 0 °C

CMT - Coupled-mode theory

d - Power dip

dB - Decibel

DNA - Acid deoksibonukleid

E - Electric field

EMI - Electromagnetic interference

FBG - Fibre Bragg grating

FBGs - Fibre Bragg gratings FOS - Fibre optic sensor

FW H M - Full width at half maximum

H - Magnetic field

HiBi - High birefringent

K - Grating momentum vector

k - Propagating constant vector

k - Propagating constant

k ! - Modal wavevector o f the forward-propagating wave k 2 - Modal wavevector o f the backward-propagating wave

L - Grating length

MHz - Mega Hertz

Mp - Fraction of fibre mode power

N - Number of grating plane

NA - Numerical aperture

nm - nanometer

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nco - Core average index neff - Effective refractive index

no - Average refractive index

ni - Refractive index of fibre core n2 - Refractive index of fibre cladding OSA - Optical Spectrum Analyzer pm/°C - pikometer per degree Celsius

R - Reflectivity

R(L,X) - Reflectivity in the function o f length and wavelength s - Fringe visibility of the index change

T - Temperature

TLS - Tunable Laser Source

UV - Ultraviolet

UVA - Ultraviolet A

UVB - Ultraviolet B

UVC - Ultraviolet C

z - Distance along the fibre longitudinal axis

e - Permittivity

U - Permeability

ez - Strain

a - Thermo-expansion coefficient

£ - Thermo-optic coefficient

Q - Coupling coefficient

A - Grating period

Ag - Grating spacing

Apm - Phase mask period

X - Wavelength

XB - Bragg wavelength

Xin - Incident light

XB,0 - Nominal Bragg wavelength

Xo - Initial wavelength

SL - Change o f length

dneff - Change o f refractive index

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An - Dept of index modulation

A T - Temperature change

AXb - Bragg wavelength shift

°C - Degree Celsius

°F - Degree Farenheigh

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L IS T O F A PPEN D IC ES

A PPEN D IX T IT L E PA G E

A Standard sheet o f MG9638A wavelength variable laser source 77 B Wavelength standard o f MS9710B Optical Spectrum Analyzer 78

C Details o f fibre optic coupler 79

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IN T R O D U C TIO N

1.1 In tro d u ctio n

Over the last five decades, fibre optic sensors (FOS) have emerged as modern device in sensing and telecommunication technologies. FOS can be classified as fluorescent/spectrally-based, intensity-based, or interferometric. Fluorescent-decay temperature sensor, blackbody radiation temperature sensor, Fabry-Perot temperature sensor, interferometric temperature sensor, polarimetric temperature sensor, and dual mode temperature sensor are examples of sensors used in fibre optic temperature sensing. Fibre Bragg grating (FBG) has the unique advantage as an fibre optic temperature sensor as compared with all other temperature sensors (Neil, 1990).

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The most important innovation o f the 1990’s in FOS is the development of FBG sensors. Fibre Bragg grating can used as a sensor because of its excellent unique properties. FBG emerges as an important technology in fibre optic sensing due to its smart structure, excellent linear characteristics, immune to electromagnetic interference (EMI), low fibre loss, and other outstanding advantages (Lai et al., 2002). Nowadays, decent and sophisticated techniques in temperature measurement become very important and necessary for safety precautions in industrial requirements (Bowei, 2004).

The FBG sensitivity measurements will be assessed for different FB G ’s position from the rooftop floor using different focusing elements at periods of the day. The research will examine the effect o f different focusing elements, FBG positions, and temperature variations on the sensor head of the FBG. Measurements made will be based on the transmission and reflection spectrum of the FBG.

1.2 B ackground of Study

A sensor is a device that measures a physical quantity and converts it into a signal which can be read by an instrument. For example, mercury in glass thermometer converts the measured temperature into expansion and contraction of the liquid which can be read on a calibrated glass tube. A thermocouple converts the temperature measurement to an output voltage which can be read by a voltmeter. For accuracy purposes, most sensors are calibrated against known standards.

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conventional temperature sensors are all point sensors. In other words, they are localized sensors, which can only provide temperature reading over a small area rather than providing an overall temperature profile (Udd, 1995). These sensors are also suitable for the passive multiplexing, but difficult in practice, due to size limitations (Xiaopei et al., 2004).

Optical fibre offers a number of distinguishing and excellent advantages over conventional sensors. Fibre Bragg grating (FBG) sensor is one of the most important and useful optical fibre sensors. The concept of FBG was discovered three decades ago by Hill and his co-workers (Hill, 1978). However, most o f the recognized pioneering work about FBG and its applications were only published a decade later after it’s discovery by a group o f researchers at United Technology Research Centre (Meltz et al., 1989).

FBG sensors are dielectric and virtually immune to electromagnetic interference (EMI). It can withstand against hostile environment, including in high and excessive temperature. It can be used to measure high temperature, until 1000 °C (Hirayama et al., 2000). It is also utilized as a distributed sensor. In principle, distributed sensors are different from point sensors. Here the parameter of interest is measured with certain spatial resolution at any points along a single optical fibre. They would permit the use of power sensors and represents more effective use of optical fibre that are used for both measurements and data transmission, which allows them to become more attractive.

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1.3 Problem Statem ent

The main motivation of this research is to design, construct, and develop temperature sensor using a commercial fibre Bragg grating (FBG) sensor under outdoor condition. To this end, a commercial germanium-doped silica fibre Bragg grating is used. This research will examine the effect of temperature variations on the characteristics of an outdoor FBG temperature sensor. How does the characteristics of FBG sensor respond to changes under different environment conditions and placement heights o f FBG? How does the focusing elements such as convex lens and hand lens affect the sensitivity o f FBG? These investigations can be used to determine the performance of FBG sensor for outdoor temperature measurement. Its performance will be evaluated based on the transmission and reflection spectrum.

1.4 O bjective

The objective o f this research is to design, construct, and develop an outdoor FBG temperature sensor system for different FBG placement heights from the rooftop floor. The effect of FBG at different heights from the rooftop floor will be evaluated. The research will also analyze the effect o f focusing elements on the FBG sensor head based on the transmission and reflection spectrum.

1.5 Scope of Study

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heights of FBG with different focusing elements used at the sensor head. The convex lens and hand lens were used as the focusing elements in this research. The performance or sensitivity o f the FBG will be analyzed in terms o f the Bragg wavelength shift.

1.6 Significance of Study

This research enables us to understand FBG temperature sensing performance by examining the characteristics and properties of the FBG. Initially studies shows that there are rapid fluctuations in outdoor temperature. The sudden change in outdoor conditions such as temperature variation, rain, and effect of wind blowing may affect the stability of the reading.

With the increasing needs for health monitoring in structures such as bridges, tunnels, highways, dams, aircraft wings, and spacecraft fuel tanks, it is imperative to design and develop an effective sensor system which can detect any sudden changes in strain, pressure, and temperature. The practical challenges here may include decoupling at different sensing parameters for long term thermal stability of the FBG under outdoor environment. This enables us to apply the FBG temperature sensor in a variety o f fields, such as medical, construction, manufacturing, industry, and many more.

1.7 O rganization of Study

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Archer, Cristina; Jacobson, Mark. "Evaluation o f Global W ind Power". Stanford. http://www.stanford.edu/group/efmh/winds/global_winds.html. Retrieved 2008-06-03.

Bowei, Z. (2004). “High Temperature Sensors based on Hydrogen L oaded Fiber B ragg Gratings ". M. Sc. Thesis. Concordia University, Canada.

Bowei, Z. and Mojtaba, K. (2005). “Characteristics o f F iber B ragg G rating Temperature Sensor at E levated Temperatures".

Proceedings o f the 2005 International Conference on MEMS, NANO and Smart Systems (ICM EN S’05).

Edmon, C., Chen-Chun Y., Stephen, E S., Stephen, J., and Ralph, P T. (2004).

“Characterization o f the response o ffib re B ragg gratings fa b rica ted in

stress and geom etrically induced high birefringence fib res to

temperature and transverse load". UK: Institute o f physics publishing. 13, 888, 894, 895.

Georges T., Delevaque E., Monerie M., Lamouler P., and Bayon J. F ,” Pair induced quenching in erbium doped silicate f ib e r s’, IEEE Optical Amplifiers and Their Applications, Technical Digest, 17, 71 (1992).

Grattan, K. T. V., and Meggit, B. T. (2000). “O ptical F iber Sensor: Advanced Applications- B ragg Gratings and D istributed Sensors ". Boston. Kluwer

(24)

Hill, K. O., Fujii, Y., Johnson, D.C., and Kawasaki, B. S. (1978). “Photosensitivity in O ptical Fiber Waveguides; Application to Reflection F ilter Fabrication ”.

Applied Physics Letter. 32 (10), 647-649.

Hill, K.O. (2002). “Fiber Optics Handbooks-Fiber, D eviced, and Systems f o r optical Comm unication”. America. McGraw-Hill.

Hilaire, St., Pierre; G. J. A. (2005). “ United States Patent 6904201 ”. Retrieved on July 6, 2005, from http://www.freepatentsonline.com/6904201.html.

Ho, S. P., Ali, J., Rahman, R. A., Saktioto (2008). “Growth Dynamics and Characteristics o f F abricated F iber B ragg Grating using Phase M ask

M eth od ”. Workshop on Recent Advances o f Low Dimensional Structures (WRA-LDSD). 7-9 April 2008. The University o f Nottingham, UK.

Ho, S. P., “Properties o f F abricated Fiber B ragg Grating f o r Temperature Sensing Using Phase M ask Technique” . Master Thesis, UTM, (2008).

Jeff, H. (2002). “ Understanding F iber Optics (Fourth E dition )”. London: Prentice Hall, 153-157.

Juergens, J. (2005). “Thermal Evaluation o f Fiber B ragg Gratings a t Extreme Tem peratures”. Canada Technology and Communication Research Center.

Jung, J. et al., 1999. “Fiber B ragg Grating Temperature Sensor with Controllable Sensitivity”, Appl. Opt, 38(13), Pg. 2752-2754.

Kashyap, R. (1999). “Fiber B ragg G ratings”. London: Academic Press Inc. 185 189.

(25)

Lai, Y. C., Qiu, G. F., Zhang, W., Zhang, L., Bennion, I., Granttan, K.T.V. (2002).

“Am plified Spontaneous Em ission-based Technique f o r Simultaneous.

M easurement o f Temperature and Strain by Combining Active Fiber with

F iber Gratings ". Review o f Instrument, American Institute o f Physics (AIP). 73 (9).

Lam, D.K.W. and Garside, B.K. (1981). “Characterization o f Single-mode O ptical Fiber Filters ". Applied Optics. 20, 440 - 445.

Malo, B., et al.,A podised in fib e r B ragg grating reflectors photoim printed using a p h a se m a sk ”, Electronic Letters, Vol. 31, 1995 pp. 223-225.

Meltz, G., Morey, W.W. and, Glen W.H. (1989). “Formation o f Bragg Gratings in O ptical F ibre by Transverse H olographic M eth o d ". Optics Letters. 14 (15), 823-825.

Morey, W. M., Ball, G. A. and Meltz, G. (Feb. 1994). “Photoinduced B ragg Gratings in O ptical Fibers ". Optics and Photocs News: 8-14.

Muhs, Jeff (2007). “D esign and Analysis o f H ybrid Solar Lighting and Full Spectrum Solar Energy System” Oak Ridge National Laboratory.

N. Hirayama, Y. Sano, ISA Transaction 39 (2000) 169-173. “Fiber B ragg Grating Temperature sensor fo r P ractical Use".

Neil, J. Guillermo (1999). “D evelopm ent o f Temperature Compensated Fiber Optic Strain Sensors based on Fiber B ragg Gratings ". University o f Toronto. Institute for Aerospace Studies.

Noyes, W M (1860-03-31). "The Law o f Light" (PDF). The N ew York Times.

(26)

Othonos, A. “Fiber B ragg gratings”, Review o f Scientific Instruments, Vol. 68, 1997, pp.4309-4341.

Othonos, A. and Kalli, K. (1999). “Fiber B ragg Gratings: Fundamentals and Applications in Telecommunication and Sensing”. Boston (USA): Artech House Inc.

Rahman, R. A., Ikhsan, S., Supian, H. M. (2000). “Fibre Optic B ragg Grating Sensors:A N ew Technology f o r Smart Structure M onitoring in M alaysia ”.

IEEE 0-7803-6355-8.

Ramesh, S. K.; Kuo, C. W, Righini, G. C., Najafi, S. I. (1999). “Design and fabrication o f a Fiber B ragg Grating tem perature sen so r”.

International Society for Optical Engineering proceedings series.

Ronald, S., 2003: “Seeing The Light" Feb 2003; Trade & Industry.

Shilton AN, Powell N, Mara DD, Craggs R (2008). ""Solar-powered aeration and disinfection, anaerobic co-digestion, biological CO(2) scrubbing and biofuel

production: the energy and carbon management opportunities o f waste

stabilisation p o n d s ”. Water Sci. Technol. 58 (1): 253-258.

Simpson, A. G. (2005). “O ptical Fibre Sensor and their Application” . Ph.D. Thesis, Aston University.

Strasser, T. A., J. R. Pedrazzai, and M. J. Andrejio, “Reflective mode conversion withUV-induced p h a se grating in two-m ode fib e r ’", Conference on Optical Fiber Communication OFC 1997, Dallas, TX, FRS 16-21, 1997, paper FB3. Snyder, A. W., and Love, J. D. (1983). “O ptical Waveguide Theory”. Chapman &

(27)

Tahir, B. A., Ali, J. and Rahman, R. A. (2005). “Strain Measurements Using Fibre B ragg Grating Sensor” . American Journal o f Applied Science (Special Issue).40-48.

Tanaka, T. et al, “100 Ghz-spacing 8-channel Light Source Integrated with Gratings and LDs on PL C Platform” . The Institude o f Electronics, Information and Communication Engineers, Technical Report o f IEICE, (2002).

Udd, E., Nelson, D., and Lawrence, C. (1997). “M ultiple axis strain sensing using fib r e gratings written onto birefrigent single m ode optical fib r e” .

Williamsburg: Proc. 12th Int. Conf. O ptical F ibre Sensors. 354-357.

Xiaopei, C., Yan, Z., Gang, P., Jiju, A. (2004). “Experimental design in F iber Optic D evelopm en t”. International Journal o f productivity and Performance, 53, 8.

Yonghang, S., Jinglei, H., Weizhong, Z., Tong, S., Kenneth, T. V. G., William, D.N.P.(2004). “Fiber-optic Sensor System f o r Heat-flux M easurem ent”.

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