INFLUENCE OF POLYANILINE DEPOSITED ON Mg TOWARDS SENSITIVITY TO LPG AND CO 2 NORHASSIMAH BINTI HASSIM

Similar documents
EFFECT OF GRAPHENE OXIDE (GO) IN IMPROVING THE PERFORMANCE OF HIGH VOLTAGE INSULATOR NUR FARAH AIN BINTI ISA UNIVERSITI TEKNOLOGI MALAYSIA

INDIRECT TENSION TEST OF HOT MIX ASPHALT AS RELATED TO TEMPERATURE CHANGES AND BINDER TYPES AKRIMA BINTI ABU BAKAR

THE DEVELOPMENT OF PORTABLE SENSOR TO DETERMINE THE FRESHNESS AND QUALITY OF FRUITS USING CAPACITIVE TECHNIQUE LAI KAI LING

OPTIMIZATION OF CHROMIUM, NICKEL AND VANADIUM ANALYSIS IN CRUDE OIL USING GRAPHITE FURNACE ATOMIC ABSORPTION SPECTROSCOPY NURUL HANIS KAMARUDIN

ANOLYTE SOLUTION GENERATED FROM ELECTROCHEMICAL ACTIVATION PROCESS FOR THE TREATMENT OF PHENOL

HYDROGEN RECOVERY FROM THE REFORMING GAS USING COMMERCIAL ACTIVATED CARBON MEHDI RAHMANIAN

COVRE OPTIMIZATION FOR IMAGE STEGANOGRAPHY BY USING IMAGE FEATURES ZAID NIDHAL KHUDHAIR

MODELING AND SIMULATION OF BILAYER GRAPHENE NANORIBBON FIELD EFFECT TRANSISTOR SEYED MAHDI MOUSAVI UNIVERSITI TEKNOLOGI MALAYSIA

RAINFALL SERIES LIM TOU HIN

MATHEMATICAL MODELLING OF UNSTEADY BIOMAGNETIC FLUID FLOW AND HEAT TRANSFER WITH GRAVITATIONAL ACCELERATION

MICROWAVE SYNTHESIS OF SODALITE FROM COAL FLY ASH AS SOLID BASE CATALYST FOR KNOEVENAGEL REACTION MOHD HILMI BIN MOHAMED

ELIMINATION OF RAINDROPS EFFECTS IN INFRARED SENSITIVE CAMERA AHMAD SHARMI BIN ABDULLAH

ARTIFICIAL NEURAL NETWORK AND KALMAN FILTER APPROACHES BASED ON ARIMA FOR DAILY WIND SPEED FORECASTING OSAMAH BASHEER SHUKUR

MONTE CARLO SIMULATION OF NEUTRON RADIOGRAPHY 2 (NUR-2) SYSTEM AT TRIGA MARK II RESEARCH REACTOR OF MALAYSIAN NUCLEAR AGENCY

COMPUTATIONAL STUDY OF PROTON TRANSFER IN RESTRICTED SULFONIC ACID FOR PROTON EXCHANGE MEMBRANE FUEL CELL SITI NADIAH BINTI MD AJEMAN

ADSORPTION OF ARSENATE BY HEXADECYLPYRIDINIUM BROMIDE MODIFIED NATURAL ZEOLITE MOHD AMMARUL AFFIQ BIN MD BUANG UNIVERSITI TEKNOLOGI MALAYSIA

Catalytic bead sensors are used primarily to detect

A COMPUTATIONAL FLUID DYNAMIC FRAMEWORK FOR MODELING AND SIMULATION OF PROTON EXCHANGE MEMBRANE FUEL CELL HAMID KAZEMI ESFEH

ADSORPTION AND STRIPPING OF ETHANOL FROM AQUEOUS SOLUTION USING SEPABEADS207 ADSORBENT

UNIVERSITI TEKNOLOGI MALAYSIA

UNIVERSITI PUTRA MALAYSIA

EFFECTS OF SURFACE ROUGHNESS USING DIFFERENT ELECTRODES ON ELECTRICAL DISCHARGE MACHINING (EDM) MOHD ABD LATIF BIN ABD GHANI

INDEX SELECTION ENGINE FOR SPATIAL DATABASE SYSTEM MARUTO MASSERIE SARDADI UNIVERSITI TEKNOLOGI MALAYSIA

DEMULSIFICATION OF CRUDE OIL EMULSIONS VIA MICROWAVE ASSISTED CHEMICALS (ENVIRONMENTAL FRIENDLY) NUR HAFIZAH BINTI HUSSIN

ALTERNATIVE STRIP METHOD FOR A LATERALLY DRIFTING SHIP IN WAVES MUHAMAD BIN RAMLI

COMPUTATIONAL STUDY OF TURBULENT UNCONFINED SWIRL FLAMES ANIS ATHIRAH BINTI MOHD AZLI

TABLE OF CONTENTS CHAPTER TITLE PAGE

ROOFTOP MAPPING AND INFORMATION SYSTEM FOR RAINWATER HARVESTING SURAYA BINTI SAMSUDIN UNIVERSITI TEKNOLOGI MALAYSIA

MULTISTAGE ARTIFICIAL NEURAL NETWORK IN STRUCTURAL DAMAGE DETECTION GOH LYN DEE

MECHANICAL PROPERTIES OF CALCIUM CARBONATE AND COCONUT SHELL FILLED POLYPROPYLENE COMPOSITES MEHDI HEIDARI UNIVERSITI TEKNOLOGI MALAYSIA

INFLUENCES OF GROUNDWATER, RAINFALL, AND TIDES ON BEACH PROFILES CHANGES AT DESARU BEACH FARIZUL NIZAM BIN ABDULLAH

SYNTHESIS AND CHARACTERIZATION OF POLYACRYLAMIDE BASED HYDROGEL CONTAINING MAGNESIUM OXIDE NANOPARTICLES FOR ANTIBACTERIAL APPLICATIONS

SYNTHESIS AND CHARACTERIZATION OF MESO-SUBSTITUTED PORPHYRIN MUHAMMAD TAHIR MUHAMMAD

PRODUCTION OF POLYHYDROXYALKANATE (PHA) FROM WASTE COOKING OIL USING PSEUDOMONAS OLEOVORANS FARZANEH SABBAGH MOJAVERYAZDI

EFFECTS OF Ni 3 Ti (DO 24 ) PRECIPITATES AND COMPOSITION ON Ni-BASED SUPERALLOYS USING MOLECULAR DYNAMICS METHOD

EFFECT OF NOZZLE ANGLE ON JET IMPINGEMENT COOLING SYSTEM KHAIDER BIN ABU BAKAR

EFFECT OF ROCK MASS PROPERTIES ON SKIN FRICTION OF ROCK SOCKET. YUSLIZA BINTI ALIAS UNIVERSITI TEKNOLOGI MALAYSIA

NUMERICAL INVESTIGATION OF TURBULENT NANOFLUID FLOW EFFECT ON ENHANCING HEAT TRANSFER IN STRAIGHT CHANNELS DHAFIR GIYATH JEHAD

ULTIMATE STRENGTH ANALYSIS OF SHIPS PLATE DUE TO CORROSION ZULFAQIH BIN LAZIM

POSITION CONTROL USING FUZZY-BASED CONTROLLER FOR PNEUMATIC-SERVO CYLINDER IN BALL AND BEAM APPLICATION MUHAMMAD ASYRAF BIN AZMAN

BOUNDARY INTEGRAL EQUATION WITH THE GENERALIZED NEUMANN KERNEL FOR COMPUTING GREEN S FUNCTION FOR MULTIPLY CONNECTED REGIONS

SYSTEM IDENTIFICATION MODEL AND PREDICTIVE FUNCTIONAL CONTROL OF AN ELECTRO-HYDRAULIC ACTUATOR SYSTEM NOOR HANIS IZZUDDIN BIN MAT LAZIM

FOURIER TRANSFORM TECHNIQUE FOR ANALYTICAL SOLUTION OF DIFFUSION EQUATION OF CONCENTRATION SPHERICAL DROPS IN ROTATING DISC CONTACTOR COLUMN

COMPUTATIONAL ANALYSIS OF HEAT TRANSFER RATE USING THERMAL RESPONSE FACTOR METHOD TENGKU FAKHRUZZAMAN BIN TENGKU YUSOFF

EMPIRICAL STRENQTH ENVELOPE FOR SHALE NUR 'AIN BINTI MAT YUSOF

SOLAR RADIATION EQUATION OF TIME PUNITHA A/P MARIMUTHOO

FRAGMENT REWEIGHTING IN LIGAND-BASED VIRTUAL SCREENING ALI AHMED ALFAKIABDALLA ABDELRAHIM

ENHANCED COPY-PASTE IMAGE FORGERY DETECTION BASED ON ARCHIMEDEAN SPIRAL AND COARSE-TO-FINE APPROACH MOHAMMAD AKBARPOUR SEKEH

FLOOD MAPPING OF NORTHERN PENINSULAR MALAYSIA USING SAR IMAGES HAFSAT SALEH DUTSENWAI

OPTICAL TWEEZER INDUCED BY MICRORING RESONATOR MUHAMMAD SAFWAN BIN ABD AZIZ

SOLUBILITY MODEL OF PALM OIL EXTRACTION FROM PALM FRUIT USING SUB-CRITICAL R134a NUR SYUHADA BINTI ABD RAHMAN

MODELING AND CONTROLLER DESIGN FOR AN INVERTED PENDULUM SYSTEM AHMAD NOR KASRUDDIN BIN NASIR UNIVERSITI TEKNOLOGI MALAYSIA

SHAPE-BASED TWO DIMENSIONAL DESCRIPTOR FOR SEARCHING MOLECULAR DATABASE

STABILITY AND SIMULATION OF A STANDING WAVE IN POROUS MEDIA LAU SIEW CHING UNIVERSTI TEKNOLOGI MALAYSIA

SEDIMENTATION RATE AT SETIU LAGOON USING NATURAL. RADIOTRACER 210 Pb TECHNIQUE

EFFECT OF SOIL TYPE ON SEISMIC PERFROMANCE OF REINFORCED CONCRETE SCHOOL BUILDING

CHARACTERISTICS OF SOLITARY WAVE IN FIBER BRAGG GRATING MARDIANA SHAHADATUL AINI BINTI ZAINUDIN UNIVERSITI TEKNOLOGI MALAYSIA

NUMERICAL SIMULATIONS ON THE EFFECTS OF USING VENTILATION FAN ON CONDITIONS OF AIR INSIDE A CAR PASSENGER COMPARTMENT INTAN SABARIAH BINTI SABRI

ONLINE LOCATION DETERMINATION OF SWITCHED CAPACITOR BANK IN DISTRIBUTION SYSTEM AHMED JAMAL NOORI AL-ANI

ROOT FINDING OF A SYSTEM OF NONLINEAR EQUATIONS USING THE COMBINATION OF NEWTON, CONJUGATE GRADIENT AND QUADRATURE METHODS

ISOLATION AND CHARACTERIZATION OF NANOCELLULOSE FROM EMPTY FRUIT BUNCH FIBER FOR NANOCOMPOSITE APPLICATION

DENSITY FUNCTIONAL THEORY SIMULATION OF MAGNETISM DUE TO ATOMIC VACANCIES IN GRAPHENE USING SIESTA

OPTIMAL CONTROL BASED ON NONLINEAR CONJUGATE GRADIENT METHOD IN CARDIAC ELECTROPHYSIOLOGY NG KIN WEI UNIVERSITI TEKNOLOGI MALAYSIA

Cork Institute of Technology. Summer 2005 Instrumental Analysis (Time: 3 Hours) Section A

EVALUATION OF FUSION SCORE FOR FACE VERIFICATION SYSTEM REZA ARFA

Figure 1. Contact mode AFM (A) and the corresponding scanning Kelvin probe image (B) of Pt-TiN surface.

DETECTION OF STRUCTURAL DEFORMATION FROM 3D POINT CLOUDS JONATHAN NYOKA CHIVATSI UNIVERSITI TEKNOLOGI MALAYSIA

CHARACTERIZATION OF IRRADIATION MODIFICATION OF ETHYLENE VINYL ACETATE/ EPOXIDIZED NATURAL RUBBER/ HALLOYSITE NANOTUBES NANOCOMPOSITES

UNCERTAINTY ANALYSIS OF TWO-SHAFT GAS TURBINE PARAMETER OF ARTIFICIAL NEURAL NETWORK (ANN) APPROXIMATED FUNCTION USING SEQUENTIAL PERTURBATION METHOD

A COMPARISO OF MODAL FLEXIBILITY METHOD A D MODAL CURVATURE METHOD I STRUCTURAL DAMAGE DETECTIO OOR SABRI A ZAHARUDI

STABILITY OF TRIAXIAL WEAVE FABRIC COMPOSITES EMPLOYING FINITE ELEMENT MODEL WITH HOMOGENIZED CONSTITUTIVE RELATION NORHIDAYAH RASIN

ENGINEERING PROPERTIES OF OLDER ALLUVIUM BADEE ABDULQAWI HAMOOD ALSHAMERI. Universiti Teknologi Malaysia

A STUDY ON THE CHARACTERISTICS OF RAINFALL DATA AND ITS PARAMETER ESTIMATES JAYANTI A/P ARUMUGAM UNIVERSITI TEKNOLOGI MALAYSIA

WIND TUNNEL TEST TO INVESTIGATE TRANSITION TO TURBULENCE ON WIND TURBINE AIRFOIL MAHDI HOZHABRI NAMIN UNIVERSITI TEKNOLOGI MALAYSIA

DYNAMIC SIMULATION OF COLUMNS CONSIDERING GEOMETRIC NONLINEARITY MOSTAFA MIRSHEKARI

ROCK SHAFT RESISTANCE OF BORED PILES SOCKETED INTO DECOMPOSED MALAYSIA GRANITE RAJA SHAHROM NIZAM SHAH BIN RAJA SHOIB UNIVERSITI TEKNOLOGI MALAYSIA

MATHEMATICAL MODELING FOR TSUNAMI WAVES USING LATTICE BOLTZMANN METHOD SARA ZERGANI. UNIVERSITI TEKNOLOGI MALAYSIAi

ELECTRODEPOSITION OF CARBOXYLATED MULTIWALL CARBON NANOTUBE ON GRAPHITE REINFORCEMENT CARBON FOR VOLTAMMETRY DETECTION OF CADMIUM

SYNTHESIS AND CHARACTERIZATION OF SUPRAMOLECULAR POLYMER BASED ON LINOLEIC ACID OF SUNFLOWER OIL MILI PURBAYA UNIVERSITI TEKNOLOGI MALAYSIA

White Paper. Overview: NDIR Definition:

EFFECTS OF TEMPERATURE IN REACTIVE DISTILLATION OF VAPOR FROM NON-CATALYTIC PENTAERYTHRITOL TETRADODECANOATE (PETD) REACTOR SHAHRULNIZAM JAMEN

A GENERALIZED POWER-LAW MODEL OF BLOOD FLOW THROUGH TAPERED ARTERIES WITH AN OVERLAPPING STENOSIS HUDA SALMI BINTI AHMAD

COMPUTATIONAL MODELLING AND SIMULATION OF BIOMAGNETIC FLUID FLOW IN A STENOTIC AND ANEURYSMAL ARTERY NURSALASAWATI BINTI RUSLI

DEVELOPMENT OF GEODETIC DEFORMATION ANALYSIS SOFTWARE BASED ON ITERATIVE WEIGHTED SIMILARITY TRANSFORMATION TECHNIQUE ABDALLATEF A. M.

MODELING AND CONTROL OF A CLASS OF AERIAL ROBOTIC SYSTEMS TAN ENG TECK UNIVERSITI TEKNOLOGY MALAYSIA

THE DEVELOPMENT OF A HYDRAULIC FLOW METER AZAM BIN AHMAD

Section B Bahagian B. [20 marks] [20 markah] Answer any one questions from this section. Jawab mana-mana satu soalan daripada bahagian ini.

PREDICTION OF FREE FATTY ACID IN CRUDE PALM OIL USING NEAR INFRARED SPECTROSCOPY SITI NURHIDAYAH NAQIAH BINTI ABDULL RANI

RS DYNAMICS ECOPROBE 5. Portable IR/PID Gas Analyzer PID. PID and IR Analyzers

UNIVERSITI PUTRA MALAYSIA GENERATING MUTUALLY UNBIASED BASES AND DISCRETE WIGNER FUNCTION FOR THREE-QUBIT SYSTEM


INTEGRATED MALAYSIAN METEOROLOGICAL DATA ATMOSPHERIC DISPERSION SOFTWARE FOR AIR POLLUTANT DISPERSION SIMULATION

SOLVING FRACTIONAL DIFFUSION EQUATION USING VARIATIONAL ITERATION METHOD AND ADOMIAN DECOMPOSITION METHOD

ADSORPTION OF ACID FUCHSIN AND FAST GREEN ON ACTIVATED CARBONS

AN APPROPRIATE LOT SIZING TECHNIQUE FOR INVENTORY POLICY PROBLEM WITH DECREASING DEMAND

MATERIAL SELECTION IN MECHANICAL DESIGN OF CAR BUMPER NURUL AZWAN BIN ADNAN BACHELOR OF ENGINEERING UNIVERSITI MALAYSIA PAHANG

Cracking. 191 minutes. 186 marks. Page 1 of 27

Questions, Myths and Misconceptions about Using Photoionization Detectors

SPRING GROVE AREA SCHOOL DISTRICT

UNSTEADY MAGNETOHYDRODYNAMICS FLOW OF A MICROPOLAR FLUID WITH HEAT AND MASS TRANSFER AURANGZAIB MANGI UNIVERSITI TEKNOLOGI MALAYSIA

Transcription:

ii INFLUENCE OF POLYANILINE DEPOSITED ON Mg TOWARDS SENSITIVITY TO LPG AND CO 2 NORHASSIMAH BINTI HASSIM A Thesis Submitted in Fulfillment of the Requirement for the Award of the Degree of Bachelor of Chemical Engineering (Gas Technology) Faculty of Chemical & Natural Resources Engineering Universiti Malaysia Pahang MAY, 2009

iii I declare that this thesis entitled Influence of Polyaniline Deposited on Mg towards Sensitivity to LPG and CO 2 is the result of my own research except as cited in the references. The thesis has not been accepted for any degree and is not concurrently submitted in candidature of any other degree. Signature :. Name : NORHASSIMAH BINTI HASSIM Date : 2 MAY 2009

iv Special Dedication of This Appreciative Feeling to My Beloved father and mother; Mr. Hassim Damawi and Mrs. Saniyah Mohd Noor Loving brothers and sister; Haffiza, Haffizan, Hazwan and Hamira Also some special who gave me encouragement For Their Love, Support and Best Wishes.

v ACKNOWLEGDEMENTS I wish to express my humble thanks to ALLAH S.W.T. for the strength, inspiration and encouragement given to me through out the completion of this project without any obstacle. A lot of experiences and knowledge were gained along the way. I wished to express my sincere appreciation to my supervisors, Mr. Azizan Bin Ramli as well as, Mr. Syamsul Bahari Abdullah for their critics, advices, motivation, friendship and input of ideas, unalloyed support, guidance and endless encouragement during the course of writing this project. I also like to express my heartfelt thanks to JP s for contributions one way or the other in order to make this project a successful one. Lastly to my parents for there moral support, I will always be grateful for their loving kindness and thanks to all friends for their advice and motivation. Without their endless support and interest, this project would not have been the same as presented here. Unfortunately, it is not possible for me to list all involved in this limited space. I am grateful to everybody that involved directly of indirectly in helping me completing this project.

vi ABSTRACT Gas sensors are primarily used in the gas and oil industry and have a very commercial value due to its higher sensitivity properties in detecting minor leakage. As the sensors heterojunction are composed of combination metal oxide and organic polymer, the use of sensor would expect upgrade in term of their sensitivity, selectivity and stability. Two methods used for heterojunction fabrication are chemical bath deposition and electrodeposition. The sensors sample are tested based on I-V characteristic would inevitably inflict low current values. In this experimental work, MgO was employed due to its high conductivity and lower operating cost while polyaniline was used due to its high mechanical strength. Two different gases were used, which are LPG and CO 2 respectively. Preliminary results showed that the sensor sample was successfully giving the conductivity effect. Further studies also revealed that the response time of sensor was mainly influenced by the different concentration of gases used. The higher gas response for LPG is 45% while for CO 2 is 55%. Low concentration of the gases can be improved in future study by carrying out the larger scale of sensing chamber.

vii ABSTRAK Penggunaan alat sensor gas pada dasarnya adalah lebih tertumpu kepada industri gas dan minyak kerana gas sensor mempunyai nilai komersial yang tinggi berikutan sifat sensitivitinya dalam mengesan kebocoran-kebocoran kecil. Sensor gas ini adalah terdiri daripada kombinasi oksida logam dan polimer organik di mana penggunaan kedua-dua bahan ini dijangka dapat meningkatkan tahap sensitiviti, pemilihan dan juga kestabilan. Dua kaedah yang telah digunakan dalam pembuatan sensor ini adalah pemendapan mandian kimia dan pengelektroendapan. Sensor gas ini telah diuji berdasarkan ciri-ciri I-V yang menghasilkan penurunan nilai arus. Di dalam kajian ini, MgO digunakan kerana ia mengkonduksi arus yang tinggi dan kos penggunaannya yang lebih rendah. Dua jenis gas digunakan ialah LPG dan CO 2. Keputusan kajian pada peringkat permulaan menunjukkan gas sensor ini dikenalpasti dapat mengkonduksi arus elektrik dengan baik. Kajian berikutnya membuktikan masa reaksi sensor dipengaruhi oleh kepekatan gas yang digunakan. Reaksi gas untuk LPG adalah 45% manakala untuk CO 2 adalah 55%. Kepekatan gas yang rendah dapat dipertingkatkan pada kajian akan datang dengan menggunakan unit pengesan berskala besar.

viii TABLE OF CONTENTS CHAPTER TITLE PAGE TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENTS ABSTRACT ABSTRAK TABLE OF CONTENTS LIST OF TABLES LIST OF FIGURES LIST OF SYMBOLS LIST OF ABBREVIATIONS LIST OF APPENDICES ii iii iv v vi vii viii xi xiii xv xvi xvii 1 INTRODUCTION 1 1.1 General 1 1.1.1 Electrochemical Sensors 2 1.1.2 Catalytic Bead Sensors 3 1.1.3 Solid-State Gas Sensors 4 1.1.4 Infrared Gas Sensors 5 1.1.5 Photoionization Sensors 7

ix 1.2 Problem Statements 9 1.3 Objectives 9 1.4 Scopes of the Study 10 1.5 Rationale and Significance 10 2 LITERATURE REVIEW 12 2.1 General 12 2.2 Development of Gas Sensor 12 2.3 Polyaniline (PANI) 15 2.3.1 Conductivity of Polyaniline 17 2.3.2 Application Using PANI Based Conductive Polymer 21 2.4 Magnesium Oxide (MgO) 21 2.4.1 Chemical and Physical Properties 23 2.4.2 Common Uses for MgO 24 2.4.2.1 Antacid 25 2.4.2.2 Drying Agent 25 2.4.2.3 Refractory 25 2.4.2.4 Insulator 26 2.4.2.5 Dietary Supplement 26 2.4.2.6 Other Uses 26 2.5 Liquefied Petroleum Gas (LPG) 27 2.5.1 LPG Properties and Characteristic 27 2.5.2 Advantages of LPG 30 2.6 Carbon Dioxide (CO 2 ) 30 2.6.1 Chemical and Physical Properties 33 2.7 Summary 35

x 3 METHODOLOGY 38 3.1 Introduction 38 3.2 Materials and Equipments 38 3.3 Overall Experimental Procedures 39 3.3.1 Preparation of MgO Thin Film 39 3.3.2 Fabrication of a p-polyaniline/n-mgo Heterojunction 40 3.3.3 Sensing Properties p-polyaniline/n-mgo Heterojunction 42 3.4 Summary of Methodology 45 4 RESULTS AND DISCUSSION 46 4.1 Qualitative Analysis 46 4.1.1 Analysis of p-polyaniline/n-mgo Heterojunction 46 4.2 Quantitative Analysis 48 4.2.1 Sensing Performance towards LPG 48 4.2.2 Sensing Performance towards CO 2 54 4.3 Comparison between sensing performance 59 5 CONCLUSIONS AND RECOMMENDATIONS 60 5.1 Conclusions 60 5.2 Recommendations 61 REFERENCES 63 Appendices A-E 67-73

xi LIST OF TABLES TABLE NO. TITLE PAGE 2.1 The properties of MgO 24 2.2 Approximate properties of LPG 29 2.3 The properties of CO 2 34 2.4 Summary of literature review 36 4.1 Electrical current values before LPG exposures 48 4.2 Exposures towards LPG for 10s 49 4.3 Exposures towards LPG for 20s 50 4.4 Exposures towards LPG for 30s 50 4.5 Exposures towards LPG for 40s 50 4.6 Exposures towards LPG for 50s 51 4.7 Electrical current values before CO 2 exposures 54 4.8 Pressure effect towards CO 2 for 30s 55 4.9 Pressure effect towards CO 2 for 40s 55

xii 4.10 Pressure effect towards CO 2 for 50s 55 4.11 Exposures towards CO 2 for 30s 56 4.12 Exposures towards CO 2 for 40s 57 4.13 Exposures towards CO 2 for 50s 57

xiii LIST OF FIGURES FIGURE NO. TITLE PAGE 1.1 Electrochemical sensors 2 1.2 A catalytic bead sensor 3 1.3 A solid state sensor 5 1.4 Infrared gas sensor with the gas cell assembly 6 1.5 A pocket photoionization monitor 7 2.1 A schematic representation of a p-polyaniline/n-tio 2 Heterojunction 16 2.2 Structure of conducting polymers 18 2.3 Main polyaniline structure 20 2.4 Lewis symbol for MgO 22 2.5 Structure of Butane and Propane 28 2.6 The mechanism of CO 2 detection 31 2.7 Apparatus for evaluation of sensor performance 32

xiv 2.8 A linear structure of CO 2 33 3.1 Preparation of MgO layer using CBD 40 3.2 The flow of electrolytic cell 41 3.3 Deposited polyaniline by DC supply 42 3.4 A schematic view of assembly unit 43 3.5 Home-made assembly unit 44 3.6 The methodology for fabrication heterojunction and gas testing 45 4.1 The heterojunction sensor 47 4.2 LPG response vs. response time for each exposure 52 4.3 LPG response vs. time at fixed voltage 53 4.4 Gas response vs. pressure at each exposure 56 4.5 CO 2 response vs. response time for each exposure 58 4.6 CO 2 response vs. time at fixed voltage 58

xv LIST OF SYMBOLS I - Electrical current A - Ampere V - Voltage R - Gas Law Constant % - Percentage g - Gravity = 9.81 m/s µ - Micron K - Kelvin atm - Atmosphere ml - Milliliter M - Molar V - Volume P - Pressure

xvi LIST OF ABBREVIATIONS CO 2 - Carbon Dioxide DC - Direct Current EB - Emeraldine Base IR - Infrared LPG - Liquefied Petroleum Gas MgO - Magnesium Oxide MOX - Metal Oxide PANI - Polyaniline PVA - Polyvinyl Alcohol PVC - Polyvinylchloride TiO2 - Titanium (II) Oxide ZnO - Zinc (II) Oxide

xvii LIST OF APPENDICES APPENDIX TITLE PAGE A LPG cylinder and regulator 67 B Heterojunction sensor within sensor 68 C Side view of home made assembly 69 D Reactivity series of metal 70 E Oxides sorted by oxidation state 71

1 CHAPTER 1 INTRODUCTION 1.1 GENERAL A gas sensor is a transducer that detects gas molecules and which produces an electrical signal with a magnitude proportional to the concentration of the gas. The transducer itself means a device that transforms one type of input energy into output energy of another. Unlike other types of measurement, that are relatively straightforward and deal with voltage, temperature, and humidity, the measurement of gases is much more complicated. There are literally hundreds of different gases and there is a wide array of diverse applications in which these gases are present, so that each application must implement a unique set of requirements. There are many different technologies currently available for the detection of gases, each with certain advantages and disadvantages. The five types most suitable and widely used as gas monitors for area air quality and safety applications are electrochemical, catalytic bead, solid state, infrared and photoionization which can be discuss below. All of these sensors are commonly used for detection of toxic and combustible gases in the work area for human and

2 property protection or for process control. One common characteristic of these sensors is that they are not specialized to detect any one specific gas. Each sensor is sensitive to a group or a family of gases. In other words, the sensor is nonspecific and is subject to interference by other gases. 1.1.1 ELECTROCHEMICAL SENSORS The oldest electrochemical sensors date back to the 1950s and were used for oxygen monitoring. The miniaturized electrochemical sensors became available for detection of many difference toxic gases in explosive limit ranges, with the sensors exhibiting good sensitivity and selectivity. A variety of electrochemical sensors are being used extensively in many stationary and portable applications currently. Figure 1.1 shows a small collection of such electrochemical sensors. Figure 1.1 Electrochemical Sensors

3 These sensors operate by reacting with the gas of interest and producing and electrical signal proportional to the gas concentration. They are minimally affected by pressure changes but still important to keep within the same pressure since the differential pressure within the sensor can cause sensor damage. In summary, different electrochemical sensors may appear very similar but they are constructed with different materials including such critical elements as sensing electrodes, electrolyte composition and porosity of hydrophobic barriers. 1.1.2 Catalytic Bead Sensors Catalytic bead sensors are used primarily to detect combustible gases. Initially, these sensors were used for monitoring gas in coal mines where they replaced canaries that had been used for a long period of time. It itself is quite simple in design and is easy to manufacture. In simplest form, it was comprised of a single platinum wire. A catalytic bead sensor is shown in Figure 1.2. Figure 1.2 A Catalytic Bead Sensor

4 Combustible gas mixtures will not burn until they reach an ignition temperature. However, in the presence of certain chemical media, the gas will start to burn or ignite at lower temperatures. The phenomenon is called a catalytic combustion. The platinum possesses excellent mechanical properties, thus it is physically strong and can be transformed into a fine bead wire which can be processed into small sensor beads. Furthermore, platinum has excellent chemical properties. It is corrosion resistant and can be operated at elevated temperatures for a long period of time without changing its physical properties. It is capable of producing a constant reliable signal over an extended period of time. For overall technology, the particularly true in selecting, preparing and processing all the chemicals needed to make the final sensor. 1.1.3 Solid-State Gas Sensors Today, solid-state sensors are available for the detection of more than 150 different gases including sensors for the gases which could otherwise only be detected using expensive analytical instruments. Each sensor has different characteristics and different manufacturers offer different levels of performance and quality. A solid-state sensor consists of one or more metal oxides from transition metals such as tin oxide, aluminium oxide, etc. Figure 1.3 below has shown the solid-state sensor.

5 Figure 1.3 A Solid-State Sensor In the presence of gas, the metal oxide causes the gas to dissociate into charged ions or complexes which results in the transfer of electrons. Meanwhile, pair of biased electrodes is imbedded into the metal oxide to measure its conductivity change. The changes in the conductivity of the sensor resulting from the interaction with the gas molecules are measured as a signal. Typically, a solidstate sensor produces a very strong signal especially at high gas concentrations. 1.1.4 Infrared Gas Sensors Infrared gas (IR) detection is a well-developed measurement technology. The gases to be detected are often corrosive and reactive. With most sensor types, the sensor itself is directly exposed to the gas, often causing the sensor to drift or die prematurely. The detector does not directly interact with the gas to be

6 detected. The gas molecules interact only with a light beam and only the sample cell are directly exposed to the gas stream. Figure 1.4 below has shown an example an infrared gas sensor with the gas cell assembly exposed. Figure 1.4 Infrared Gas Monitor with the Gas Cell Assembly The infrared detection principle incorporates only a small portion of the very wide electromagnetic spectrum. The portion used is that which we can feel as heat. A regular incandescent light bulb is a good infrared source. A heated wire filament radiates sufficient energy in the 1-5 µ, micron range for the detection of most hydrocarbons, carbon dioxide and carbon monoxide. Infrared detectors convert electromagnetic radiation energy or temperature changes into electrical signals. Normally, the size and mass of the device are important in determining its response time. The basic characteristics are including DC stability, no bias and responding to all wavelengths.

7 1.1.5 Photoionization Sensors The photoionization detector utilizes ultraviolet light to ionize gas molecules and is commonly employed in the detection of volatile organic compounds. The electronic that lamps were used today led to the design of small portable photoionization detectors as shown in Figure 1.5 that have proven to be both practical and reliable. It is which offer fast response and the ability to detect low gas concentrations. The ions produced by the ionization process are collected by electrodes and the current generated is a measure of the analyte concentration. If the energy of an incoming photon is high enough, photo-excitation can occur to such an extent that an electron is completely removed from its molecular orbital. The greater the concentration of the component, the more ions are produced and the greater the current. Figure 1.5 A Pocket Photoionization Monitor

8 The gases that we are going to test in this study are liquefied petroleum gas (LPG) and carbon dioxide (CO 2 ). LPG is defined as a petroleum product composed predominantly of any of the following hydrocarbons or mixtures including propane, propylene, butanes and butylenes. The most important is that LPG products are gases at atmospheric temperatures and pressures but they can be liquefied and maintained in their liquid state with relative ease. Meanwhile, CO 2 is known as a colorless, odorless gas and acidic oxide but it is non flammable at atmospheric temperature and pressure. It is an important greenhouse gas that helps to trap heat in our atmosphere through the greenhouse effect. However, a gradual increase in CO 2 concentrations in Earth's atmosphere is helping to drive global warming, threatening to disrupt our planet's climate. The certainty is these gases are potentially hazardous due to high possibility of explosion accidents caused by leakage or by human error. 1.2 Problem Statements Nowadays, the industry s demands for detecting and monitoring of toxic and inflammable gas sensors operating at lower temperature which are inexpensive have become more intense. Most of the industrial, domestic or residential needs the sensors in terms of ease of installation, economic and function well in any condition or surrounding. They are being set to invest the small cost but require the high efficiency of sensors. Semiconductor inorganic gas sensors like doped or undoped SnO2, ZnO or Fe2O3 have been well studied to detect most of reducing gases and they are considered interesting for their low cost and simple sensing methods. Nevertheless, there still exist some problems with them, for example high working temperature of 423 to 623 K for SnO2 and 673 to 723 K for ZnO. At