Bhaumik Materials Science Division, CSIR-National Aerospace tories, Bangalore, IndiaLabora-Dhananjay Bodas Centre of Nanobioscience, Agharkar Research Institute, Pune,India Jeevanjyoti C
Trang 1Springer Tracts in Mechanical Engineering
Tai Lieu Chat Luong
Trang 2Springer Tracts in Mechanical Engineering
For further volumes:
http://www.springer.com/series/11693
Trang 4K J Vinoy
Electrical Communication Engineering
Indian Institute of Science
BangaloreKarnatakaIndia
S B KrupanidhiMaterials Research CentreIndian Institute of ScienceBangalore
KarnatakaIndia
ISSN 2195-9862 ISSN 2195-9870 (electronic)
ISBN 978-81-322-1912-5 ISBN 978-81-322-1913-2 (eBook)
DOI 10.1007/978-81-322-1913-2
Springer New Delhi Heidelberg New York Dordrecht London
Library of Congress Control Number: 2014938988
Springer India 2014
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Trang 5Dedicated to
Prof Vasudev K Aatre
for his inspiring vision, unwavering
conviction, and tireless effort that have resulted in creating and nurturing a vibrant multidisciplinary research field of micro and smart systems in India
Trang 6Prof Vasudev Kalkunte Aatre was born in 1939 in Bangalore where he alsospent most of his childhood and formative years He obtained his B.E from UVCE(then under Mysore University) in 1961, M.E from the Indian Institute of Science(IISc), Bangalore in 1963, and Ph.D from the University of Waterloo, Canada, in
1967, all in Electrical Engineering He worked as Professor of Electrical neering at Technical University of Nova Scotia, Canada, from 1968 to 1980 Hewas also a Visiting Professor at IISc in 1977 In 1980 he joined the DefenceResearch and Development Organisation (DRDO) of India
Engi-Prof Aatre worked in India’s Ministry of Defence in various capacities for
24 years He started his career in DRDO as a Principal Scientific Officer(1980–1984) Subsequently, he became the Director of the Naval PhysicalOceanographic Laboratory (1984–1991), the Chief Controller (1991–1999), andfinally, led the organization as the Director General and Scientific Advisor toDefence Minister (1999–2004) During this long period of dedicated service, hedesigned and developed sonar suites for surface ships, submarines, and the air arm
of the Indian Navy He was also instrumental in the development of integratedelectronic warfare systems for the Indian Army, Navy, and Air Force, and heestablished GaAs MMIC fabrication facility and VLSI design centers for theMinistry of Defence Prof Aatre is also the founding president of the Institute ofSmart Structures and Systems (ISSS) and has led the national programs on smartmaterials and micro and smart systems
He has published over 60 papers in the fields of active filters, digital signalprocessing, and defense electronics, and has two books entitled Network Theoryand Filter Design and Micro and Smart Systems, both published by John Wiley &Sons He is a Fellow of the IEEE (USA) and the National Academy of Engineering(India), a Distinguished Fellow of IETE (India) and several other societies
Dr Aatre is the recipient of the prestigious Padma Bhushan Award of theGovernment of India
Trang 7Since the dawn of civilization, Nature has been man’s greatest teacher We havelearned by observing and mimicking Nature and natural phenomena with theultimate goal of building systems as complex, efficient, and optimal as biologicalsystems created by Nature Such systems, if they have to mimic biological sys-tems, need to continuously sense the environment and respond, to a degree,optimally to achieve certain objectives or perform certain tasks Although over thecenturies, especially for the last century and a half, man has developed materials,devices, and systems, which have found application in myriad fields, competingwith natural systems is a dream yet to be fulfilled The recent advances in smart,micro, and nano systems have opened up a possibility of achieving this goal.Institute of Smart Structures and Systems (ISSS) was started by a group ofscientists, technologists, and engineers in India from academic institutions, spaceand defense departments in 1998 to trigger research and development in poten-tially highly application-oriented areas of micro and smart systems ISSS activelyparticipated in formulating two National Programs—National Program on SmartMaterials (NPSM) followed by the National Program on Micro and Smart Systems(NPMASS), both sponsored by the five Scientific Departments of the Government
of India and funded by the Department of Defence, India
While setting up infrastructural facilities such as MEMS foundries, LTCCpackaging facility, and developing sensors, actuators and subsystems for aero-nautical, automobile, and biomedical applications were the principal goals ofNPSM and NPMASS, supporting research projects in materials, sensors, andactuators and developing human resources in this area were equally importantgoals of the two programs Towards this, the two national programs sponsoredseveral R&D projects to academic institutions and national laboratories besidesestablishing 65 National MEMS Design Centers (NMDCs) in institutions acrossthe country These institutions and centers have conducted research, trainedundergraduate and postgraduate students, thus creating a large body of humanresources capable of pursuing developments in the general area of micro and nanosystems This special edition gives a glimpse of the R&D work carried out in theseinstitutions and centers
The contents of this special edition clearly bring out two facts The first andforemost is the large number of institutions involved in such R&D work and their
vii
Trang 8geographical spread in India This augurs well for the future development of thisfield and for the development of the required human resources thereof The second
is that the R&D activities cover the entire spectrum of the field from materials tosystems and applications
The founding members of ISSS were guided by one conviction that ‘‘India hadmissed the microelectronic revolution but should not miss the micro-machine andnano revolution.’’ The happenings of the last decade and a half give great hope Iwish special editions like this were brought out once in three years to coincidewith the triennial International Conference organized by ISSS
Trang 9This book covers multiple facets of micro and smart systems technologies iaturization of sensors and actuators through effective use of smart materials formsthe core of the book Related aspects of material processing and characterization;modeling and simulation; and applications are also given due importance Twentynine chapters written by competent research teams from academia and governmentresearch labs comprise a valuable resource that gives a bird’s-eye view of the state
Min-of the art Min-of the field in India While the technological details Min-of the workdescribed in this book are self-explanatory, it is pertinent to introspect on how it allhappened in India not too long after the miniaturization revolution transpiredelsewhere in the world
Generous financial support and guidance from the government, vision anddriving force of a leader, and a professional society that can enthuse an ableworkforce are perhaps three necessary factors to initiate and establish a newresearch area in a country India has had all of these in the last 15 years to lay afirm foundation for micro and smart systems technologies First, the DefenceResearch and Development Organisation (DRDO) and four other science andtechnology departments of the Government of India, initiated and ran two largeresearch programs, namely, National Programme on Smart Materials (NPSM,2000–2006) and National Programme on Micro and Smart Materials and Systems(NPMASS, 2007–2014), with a combined budget of nearly Rs 270 crores ($45 Mtoday) Second, Prof V K Aatre, gave unstinted leadership and support tonumerous researchers and research administrators whom he inspired and nurtured.Third, a professional society, ambitiously christened, the Institute of SmartStructures and Systems (ISSS) was founded in 1998 to bring together experts frommultiple disciplines to create a research community in micro and smart systems inIndia As a result of these efforts, India today is proud to claim its presence in thefield This edited monograph, with the exception of one chapter, is a record of thework done in India and thus it stands as a testimony to the success of a well-conceived and ably executed endeavor
Many researchers from the academia and government research laboratoriescontributed to NPSM and NPMASS, which were admirably administered by theAeronautical Development Agency (ADA) under the guidance of the Board forSmart materials Research and Technology (B-SMART) Constant support from thepast and present Heads of DRDO and its higher management has helped run these
ix
Trang 10programs well Program offices of NPSM and NPMASS, which operated out ofADA, Bangalore, since 2000, did exemplary work in liaising with various arms ofthe programs and grantees, bringing synergy and effective program management.The chairs and members of Programme Assessment and Recommendation Com-mittees (PARCs) looked after the technical details of the funded projects Theresult of the untiring efforts of all these and many more individuals—too many tomention here—is widespread awareness of micro and smart systems technologiesand engagement into research and development activities in almost all parts ofIndia NPSM and NPMASS have paid particular attention to human resourcedevelopment by establishing more than 65 National MEMS Design Centres(NMDCs) in many states of India covering the length and breadth of the country.Hundreds of researchers have been involved in more than 150 projects funded byNPSM and NPMASS.
The most significant outcome of this concerted effort is that the spirit of tidisciplinary research in micro and smart technologies now pervades all parts ofIndia Most researchers began with modeling and design Not too long ago inIndia, possessing a license of a microsystems simulation software meant beingengaged in research in this area But today it has changed; with the establishment
mul-of state-mul-of-the-art well-equipped cleanrooms and characterization facilities,researchers in India are able to fabricate and even package devices and systems.All aspects of the field, development of microsensors and microactuators; materialprocessing and characterization; fabrication; advanced modeling, design, andsimulation; and systems design have all begun Packaging and transfer of tech-nology have also commenced The chapters in this book are indeed organizedaccordingly
The final link in this chain of events is commercialization of the developedtechnology This step needs conscious effort and copious resources, perhaps anorder of magnitude more than what went into creating the able research com-munity The time is now ripe to involve the established industries and to nurtureentrepreneurship One hopes that the same level of commitment and financialsupport will be given to incubating companies in micro and smart technologies inorder to create a thriving industry in these areas in India
G K AnanthasureshRudra Pratap
S B Krupanidhi
Trang 11K J Vinoy
G K AnanthasureshRudra Pratap
S B KrupanidhiBangalore, April 2014
xi
Trang 12Part I Microsensors
Design, Development, Fabrication, Packaging, and Testing
of MEMS Pressure Sensors for Aerospace Applications 3
K N Bhat, M M Nayak, Vijay Kumar, Linet Thomas,
S Manish, Vijay Thyagarajan, Pandian, Jeyabal,
Shyam Gaurav, Gurudat, Navakanta Bhat and Rudra Pratap
MEMS Piezoresistive Accelerometers 19Tarun Kanti Bhattacharyya and Anindya Lal Roy
A Handheld Explosives Detector Based on Amplifying
Fluorescent Polymer 35Anil Kumar, Jasmine Sinha, Ashok K Majji, J Raviprakash,
Sathyadeep Viswanathan, Justin K Paul, S Vijay Mohan,
Shilpa K Sanjeeva, Swathi Korrapati and Chandrashekhar B Nair
Development of a Surface Plasmon Resonance-Based
Biosensing System 49
S Mukherji, Munshi Imran Hossain, T Kundu and Deepali Chandratre
Design and Development of Ion-Sensitive Field-Effect Transistor
and Extended-Gate Field-Effect Transistor Platforms
for Chemical and Biological Sensors 73
V K Khanna, R Mukhiya, R Sharma, P K Khanna, S Kumar,
D K Kharbanda, P C Panchariya and A H Kiranmayee
Part II Microactuators
RF MEMS Single-Pole-Multi-Throw Switching Circuits 91Shiban K Koul and Sukomal Dey
xiii
Trang 13Piezoelectric Actuators in Helicopter Active Vibration Control 111
R Ganguli and S R Viswamurthy
Design and Development of a Piezoelectrically Actuated
Micropump for Drug Delivery Application 127Paul Braineard Eladi, Dhiman Chatterjee and Amitava DasGupta
Development and Characterization of PZT Multilayered Stacks
for Vibration Control 143
P K Panda and B Sahoo
Development of Piezoelectric and Electrostatic RF MEMS Devices 155Abhay Joshi, Abhijeet Kshirsagar, S DattaGupta, K Natarajan
and S A Gangal
Part III Materials and Processes
Nickel–Titanium Shape Memory Alloy Wires for Thermal
Actuators 181
S K Bhaumik, K V Ramaiah and C N Saikrishna
Processing and Characterization of Shape Memory Films
for Microactuators 199
S Mohan and Sudhir Kumar Sharma
Piezoceramic Coatings for MEMS and Structural
Health Monitoring 213Soma Dutta
Cost-Effective Processing of Polymers and Application to Devices 229Bhoopesh Mahale, Abhay Joshi, Abhijeet Kshirsagar,
S DattaGupta, Dhananjay Bodas and S A Gangal
Chemical Synthesis of Nanomaterials and Structures,
Including Nanostructured Thin Films, for Different Applications 249
S A Shivashankar
A Study on Hydrophobicity of Silicon and a Few
Dielectric Materials 265Vijay Kumar and N N Sharma
Trang 14Materials for Embedded Capacitors, Inductors,
Nonreciprocal Devices, and Solid Oxide Fuel Cells
in Low Temperature Co-fired Ceramic 285Vivek Rane, Varsha Chaware, Shrikant Kulkarni,
Siddharth Duttagupta and Girish Phatak
Smart Materials for Energy Harvesting, Energy Storage,
and Energy Efficient Solid-State Electronic Refrigeration 303Jayanta Parui, D Saranya and S B Krupanidhi
Part IV Modeling and Simulation
Vibratory MEMS and Squeeze Film Effects 319Rudra Pratap and Anish Roychowdhury
Streaming Potential in Microflows and Nanoflows 339Jeevanjyoti Chakraborty and Suman Chakraborty
A Simulation Module for Microsystems using Hybrid Finite
Elements: An Overview 355Kunal D Patil, Sreenath Balakrishnan, C S Jog
and G K Ananthasuresh
Structural Health Monitoring: Nonlinear Effects
in the Prognostic Analysis of Crack Growth in Structural Joints 375
B Dattaguru
Part V Systems and Applications
Smart e-Textile-Based Nanosensors for Cardiac Monitoring
with Smart Phone and Wireless Mobile Platform 387Prashanth Kumar, Pratyush Rai, Sechang Oh, Robert E Harbaugh
and Vijay K Varadan
Polymer-Based Micro/Nano Cantilever Electro-Mechanical
Sensor Systems for Bio/Chemical Sensing Applications 403Rajul S Patkar, Manoj Kandpal, Neena Gilda, Prasenjit Ray
and V Ramgopal Rao
Smart Materials Technology for Aerospace Applications 423
S Gopalakrishnan
Trang 15Electronic Circuits for Piezoelectric Resonant Sensors 439
M Umapathy, G Uma and K Suresh
A Universal Energy Harvesting Scheme for Operating
Low-Power Wireless Sensor Nodes Using Multiple Energy
Resources 453
K J Vinoy and T V Prabhakar
RF MEMS True-Time-Delay Phase Shifter 467Shiban K Koul and Sukomal Dey
MEMS Sensors for Underwater Applications 487
V Natarajan, M Kathiresan, K A Thomas, Rajeev R Ashokan,
G Suresh, E Varadarajan and Shiny Nair
Author Index 503Subject Index 505
Trang 16Com-S K Bhaumik Materials Science Division, CSIR-National Aerospace tories, Bangalore, India
Labora-Dhananjay Bodas Centre of Nanobioscience, Agharkar Research Institute, Pune,India
Jeevanjyoti Chakraborty Advanced Technology Development Centre, IndianInstitute of Technology Kharagpur, Kharagpur, West Bengal, India; MathematicalInstitute, University of Oxford, Oxford, UK
Suman Chakraborty Advanced Technology Development Centre, Indian tute of Technology Kharagpur, Kharagpur, West Bengal, India; MechanicalEngineering Department, Indian Institute of Technology Kharagpur, Kharagpur,West Bengal, India
Insti-Deepali Chandratre IIT Bombay, Mumbai, India
Dhiman Chatterjee Department of Mechanical Engineering, Indian Institute ofTechnology Madras, Chennai, India
xvii
Trang 17Varsha Chaware Centre for Materials for Electronics Technology (C-MET),Panchawati, Pune, India
Amitava DasGupta Department of Electrical Engineering, Indian Institute ofTechnology Madras, Chennai, India
S DattaGupta Department of Electrical Engineering, Indian Institute of nology, Mumbai, India
Tech-B Dattaguru Institute of Aerospace Engineering and Management, Jain versity, Bangalore, India; TechMahindra, Bangalore, India
Uni-Sukomal Dey Centre for Applied Research in Electronics, Indian Institute ofTechnology Delhi, Hauz Khas, New Delhi, India
Soma Dutta Materials Science Division, CSIR-National Aerospace Laboratories,Bangalore, India
Paul Braineard Eladi Department of Electrical Engineering, Indian Institute ofTechnology Madras, Chennai, India
S A Gangal Department of Electronic Science, University of Pune, hind Road, Pune, India
Ganeshk-R Ganguli Department of Aerospace Engineering, Indian Institute of Science,Bangalore, India
Shyam Gaurav Centre for Nano Science and Engineering, Indian Institute ofScience, Bangalore, India
Neena Gilda Department of Electrical Engineering, Indian Institute of nology Bombay, Mumbai, India
Tech-S Gopalakrishnan Department of Aerospace Engineering, Indian Institute ofScience, Bangalore, India
Gurudat Centre for Nano Science and Engineering, Indian Institute of Science,Bangalore, India
Robert E Harbaugh Department of Neurosurgery, Penn State UniversityMedical School, Hershey, PA, USA
Munshi Imran Hossain IIT Bombay, Mumbai, India
Jeyabal Centre for Nano Science and Engineering, Indian Institute of Science,Bangalore, India
C S Jog Computational Nanoengineering (CoNe) group and Mechanical neering, Indian Institute of Science, Bangalore, India
Engi-Abhay Joshi Department of Electronic Science, University of Pune, GaneshkhindRoad, Pune, India
Trang 18Manoj Kandpal Department of Electrical Engineering, Indian Institute ofTechnology Bombay, Mumbai, India
M Kathiresan Naval Physical and Oceanographic Laboratory, Thrikkakara,Kochi, India
P K Khanna CSIR-Central Electronics Engineering Research Institute, Pilani,Rajasthan, India; Academy of Scientific and Innovative Research (AcSIR), NewDelhi, India
V K Khanna CSIR-Central Electronics Engineering Research Institute, Pilani,Rajasthan, India; Academy of Scientific and Innovative Research (AcSIR), NewDelhi, India
D K Kharbanda CSIR-Central Electronics Engineering Research Institute, lani, Rajasthan, India; Academy of Scientific and Innovative Research (AcSIR),New Delhi, India
Pi-A H Kiranmayee CSIR-Central Electronics Engineering Research Institute,Pilani, Rajasthan, India
Swathi Korrapati Bigtec Private Limited, Bengaluru, India
Shiban K Koul Centre for Applied Research in Electronics, Indian Institute ofTechnology Delhi, Hauz Khas, New Delhi, India
S B Krupanidhi Materials Research Centre, Indian Institute of Science, galore, India
Ban-Abhijeet Kshirsagar Department of Electronic Science, University of Pune,Ganeshkhind Road, Pune 411007, India; Department of Electrical Engineering,Indian Institute of Technology, Mumbai, India
Shrikant Kulkarni Centre for Materials for Electronics Technology (C-MET),Panchawati, Pune, India
Anil Kumar Indian Institute of Technology Bombay, Mumbai, India
Prashanth Kumar Department of Electrical Engineering, University ofArkansas, Fayetteville, AR, USA
S Kumar CSIR-Central Electronics Engineering Research Institute, Pilani,Rajasthan, India
Vijay Kumar Department of Mechanical Engineering, Nanomaterials andNational MEMS Design Centre, Birla Institute of Technology and Science, Pilani,India
T Kundu IIT Bombay, Mumbai, India
Bhoopesh Mahale Department of Electronic Science, University of Pune,Ganeshkhind Road, Pune, India
Trang 19Ashok K Majji Indian Institute of Technology Bombay, Mumbai, India
S Manish Centre for Nano Science and Engineering, Indian Institute of Science,Bangalore, India
S Mohan Indian Institute of Science, Bengaluru, India
S Mukherji IIT Bombay, Mumbai, India
R Mukhiya CSIR-Central Electronics Engineering Research Institute, Pilani,Rajasthan, India; Academy of Scientific and Innovative Research (AcSIR), NewDelhi, India
Chandrashekhar B Nair Bigtec Private Limited, Bengaluru, India
Shiny Nair Naval Physical and Oceanographic Laboratory, Thrikkakara, Kochi,India
K Natarajan Department of Telecommunication Engineering, MS RamaiahInstitute of Technology, Bangalore, India
V Natarajan Naval Physical and Oceanographic Laboratory, Thrikkakara,Kochi, India
M M Nayak Centre for Nano Science and Engineering, Indian Institute ofScience, Bangalore, India
Sechang Oh Department of Electrical Engineering, University of Arkansas,Fayetteville, AR, USA
P C Panchariya CSIR-Central Electronics Engineering Research Institute, lani, Rajasthan, India; Academy of Scientific and Innovative Research (AcSIR),New Delhi, India
Pi-P K Panda Materials Science Division, CSIR-National Aerospace Laboratories,Kodihalli, Bangalore, India
Pandian Centre for Nano Science and Engineering, Indian Institute of Science,Bangalore, India
Jayanta Parui Materials Research Centre, Indian Institute of Science, Bangalore,India
Kunal D Patil Computational Nanoengineering (CoNe) group and MechanicalEngineering, Indian Institute of Science, Bangalore, India
Rajul S Patkar Department of Electrical Engineering, Indian Institute ofTechnology Bombay, Mumbai, India
Justin K Paul Bigtec Private Limited, Bengaluru, India
Girish Phatak Centre for Materials for Electronics Technology (C-MET),Panchawati, Pune, India
Trang 20T V Prabhakar Department of Electronic Systems Engineering, Indian Institute
of Science, Bangalore, India
Rudra Pratap Center for Nano Science and Engineering and Department ofMechanical Engineering, Indian Institute of Science, Bangalore, India
Pratyush Rai Department of Electrical Engineering, University of Arkansas,Fayetteville, AR, USA
K V Ramaiah Materials Science Division, CSIR-National Aerospace tories, Bangalore, India
Labora-Vivek Rane G M Vedak College of Science, Raigad, Maharashtra, India
V Ramgopal Rao Department of Electrical Engineering, Indian Institute ofTechnology Bombay, Mumbai, India
J Raviprakash Bigtec Private Limited, Bengaluru, India
Prasenjit Ray Department of Electrical Engineering, Indian Institute of nology Bombay, Mumbai, India
Tech-Anindya Lal Roy Advanced Technology Development Centre, Indian Institute ofTechnology, Kharagpur, India
Anish Roychowdhury Center for Nano Science and Engineering and Department
of Mechanical Engineering, Indian Institute of Science, Bangalore, India
B Sahoo Materials Science Division, CSIR-National Aerospace Laboratories,Kodihalli, Bangalore, India
C N Saikrishna Materials Science Division, CSIR-National Aerospace ratories, Bangalore, India
Labo-Shilpa K Sanjeeva Bigtec Private Limited, Bengaluru, India
D Saranya Materials Research Centre, Indian Institute of Science, Bangalore,India
N N Sharma Department of Mechanical Engineering, Nanomaterials andNational MEMS Design Centre, Birla Institute of Technology and Science, Pilani,India
R Sharma CSIR-Central Electronics Engineering Research Institute, Pilani,Rajasthan, India; Academy of Scientific and Innovative Research (AcSIR), NewDelhi, India
Sudhir Kumar Sharma Indian Institute of Science, Bengaluru, India
S A Shivashankar Centre for Nano Science and Engineering, Indian Institute ofScience, Bangalore, India
Jasmine Sinha Johns Hopkins University, Baltimore, USA
Trang 21G Suresh Naval Physical and Oceanographic Laboratory, Thrikkakara, Kochi,India
K Suresh Department of Instrumentation and Control Engineering, NationalInstitute of Technology, Tiruchirappalli, India
K A Thomas Naval Physical and Oceanographic Laboratory, Thrikkakara,Kochi, India
Linet Thomas Centre for Nano Science and Engineering, Indian Institute ofScience, Bangalore, India
Vijay Thyagarajan Centre for Nano Science and Engineering, Indian Institute ofScience, Bangalore, India
G Uma Department of Instrumentation and Control Engineering, NationalInstitute of Technology, Tiruchirappalli, India
M Umapathy Department of Instrumentation and Control Engineering, NationalInstitute of Technology, Tiruchirappalli, India
Vijay K Varadan Department of Electrical Engineering, University of Arkansas,Fayetteville, AR, USA; Department of Biomedical Engineering, University ofArkansas, Fayetteville, AR, USA; Department of Neurosurgery, Penn State Uni-versity Medical School, Hershey, PA, USA; Global Institute of Nanotechnology inEngineering and Medicine, Fayetteville, AR, USA
E Varadarajan Naval Physical and Oceanographic Laboratory, Thrikkakara,Kochi, India
Vijay Kumar Centre for Nano Science and Engineering, Indian Institute ofScience, Bangalore, India
S Vijay Mohan Bigtec Private Limited, Bangalore, India
K J Vinoy Department of Electrical Communication Engineering, IndianInstitute of Science, Bangalore, India
S R Viswamurthy National Aerospace Laboratories, Council of Scientific andIndustrial Research, Bangalore, India
Sathyadeep Viswanathan Bigtec Private Limited, Bengaluru, India
Trang 22ADC Analog-to-digital converter
AFE Antiferroelectric
AFE-FE Antiferroelectric to ferroelectric switching
AFP Amplifying fluorescent polymer
A-IgG Anti-immunoglobulin G
APA Amplified piezo actuator
ASME American society for mechanical Engineers
ASSURED Affordable, sensitive, specific, user-friendly, rapid and robust,
equipment-free, and delivered to those who need it
ASTM American society for testing and materials
ATS Alkyltricholrosilane
CBP Cardiac biopotentials
CFRP Carbon fiber reinforced plastics
CMOS Complementary metal oxide semiconductor
CSIR Council of scientific and industrial research, India
CVD Cardiovascular diseases
CVI C for virtual instrumentation
DAC Digital-to-analog converter
DNA Deoxy-ribonucleic acid
DNT 2,4-Dinitrotoluene
DoS Department of Space, India
DRDO Defence Research and Development Organization, India
DRIE Deep reactive ion etching
DSC Differential scanning calorimeter
DST Department of Science and Technology, India
xxiii
Trang 23EDC N-(3-Dimethylaminopropyl)-N0Ethyl-carbodiimide HydrochlorideEESSs Electrical energy storage systems
EGFET Extended-gate field-effect transistor
EMI Electro magnetic interference
FEA Finite element analysis
FE-AFE Ferroelectric to antiferroelectric switching
FEM Finite element method
FITC Fluorescein Isothiocyanate
FSO Full scale output
FWHM Full width at half maxima
GFRP Glass fiber reinforced plastics
GPRS General packet radio service
HMX High melting explosive
(Octahydro-1,3,5,7-tetranitro-1,3,5,7-tetrazocine)
ICAF International Committee for Aeronautical Fatigue
ICCMS International Congress on Computational mechanics and SimulationIDE Inter Digited electrode
ISFET Ion-sensitive field-effect transistor
KMF Kotagiri Mission Fellowship Hospital
LCD Liquid crystal display
LED Light emitting diode
LPCVD Low-pressure chemical vapor deposition
LSCO Lanthanum strontium cobaltate
LTCC Low-temperature co-fired ceramic
LUMO Lowest unoccupied molecular orbital
MEMS Micro electro mechanical systems
MOSFET Metal-oxide semiconductor field-effect-transistor
MuA 11-Mercapto-undecanoic acid
MWCNT Multi-wall carbon nanotubes
NDE Non destructive evaluation
NPMASS National Programme on Micro and Smart Systems
NPSM National Programme on Smart Materials
Op-Amp Operational amplifier
OTS Octadecyltrichlorosilane
PANP Polyaniline nanoparticles
Trang 24PBS Phosphate buffer saline
PCB Printed circuit board
PDE Partial differential equation
PDMS Polydimethylsiloxane
PDMS Poly-dimethyl Siloxane
PECVD Plasma enhanced chemical vapor deposition
PEDOT PSS:poly (3,4-ethylenedioxythiophene) poly(styrenesulfonate)PETN Penta erythritol tetra nitrate
pHpzc pH at the point of zero charge
PLD Pulsed laser deposition
PLZT Lead lanthanum zirconate titanate
PMN Lead magnesium niobate
pMUTs Piezoelectric micromachined ultrasonic transducers
PZT Lead zirconate titanate
RC Resistance capacitance network
RCA Radio Corporation of America
RDX Research Department Explosive
(1,3,5-Trinitro-1,3,5-triazacyclohexane)
REFET Reference field-effect transistor
RIE Reactive ion etching
RIU Refractive index unit
SAMs Self assembled monolayers
SEM Scanning electron microscopy
SHM Structural health monitoring
SIF Stress intensity factor
SOI Silicon on insulator
SPR Surface plasmon resonance
SWCNT Single walled carbon nanotubes
TCAD Technology computer-aided design
TEM Transmission electron microscopy
TMAH Tetra-methyl ammonium hydroxide
TNT 2,4,6-Trinitrotoluene
T-NT Titanium-rich nickel titanium
UART Universal asynchronous receiver/transmitter
Trang 25UTM Universal testing machine
WCA Water contact angle
XRD X-ray diffraction
Trang 26Part I
Microsensors
Trang 27Design, Development, Fabrication,
Packaging, and Testing of MEMS
Pressure Sensors for Aerospace
Applications
K N Bhat, M M Nayak, Vijay Kumar, Linet Thomas, S Manish,
Vijay Thyagarajan, Pandian, Jeyabal, Shyam Gaurav, Gurudat,
Navakanta Bhat and Rudra Pratap
Abstract In this chapter we present the design, fabrication, packaging, and ibration of silicon micro machined piezo-resistive pressure sensors for operation inthe pressure range of 1.2–400 bar Based on the detailed Finite Element Analysis(FEA), the diaphragm dimensions and the optimized locations for the piezo-resistors are designed, to achieve the best performance parameters over a widerange of pressures, with minimum nonlinearity and adequate burst pressure Theprocess parameters are optimized and the pressure sensors fabricated in the Centrefor Nano Science and Engineering (CeNSE) at IISc The wafers are diced, thedevices mounted on headers, wire bonded and packaged suitably, tested, andcalibrated at the cell level to determine the adequacy of the performance param-eters of the sensors for different pressure ranges The results achieved on thepressure transducer assembly with Active Temperature Compensation and theoffset compensation using electronics and EMI filters in a single package arepresented Excellent linearity within 0.5 % in the output voltage versus pressure isdemonstrated, over the specified pressure ranges (i) 0-1.2 bar and (ii) 0-400 bar,and over the temperature range of -40C to +80C
cal-Keywords Pressure sensors Microfabrication Packaging Aerospace cations Finite element analysisPressure sensor calibration
appli-1 Introduction
Pressure sensors cater to about 60 % of the MEMS market Among the varioustypes of pressure sensors, piezo-resistive pressure sensors are easy to design to suit
a wide range of pressure ranges They are simple to fabricate with a suitably
K N Bhat ( &) M M Nayak V Kumar L Thomas S Manish V Thyagarajan Pandian Jeyabal S Gaurav Gurudat N Bhat R Pratap
Centre for Nano Science and Engineering, Indian Institute of Science, Bangalore, India e-mail: knbhat@gmail.com
K J Vinoy et al (eds.), Micro and Smart Devices and Systems,
Springer Tracts in Mechanical Engineering, DOI: 10.1007/978-81-322-1913-2_1,
Springer India 2014
3
Trang 28designed diaphragm acting as the sensing element and piezo-resistors serving astransducers Miniaturization and batch processing of this device is achieved withgreat precision using the silicon micromachining technique for realizing the dia-phragm [1 3] The piezo-resistors and the interconnections are achieved usingphotolithography, diffusion, ion implantation, and thin film deposition, which arewell established in the microelectronics technology All the finer aspects of design,fabrication, packaging, characterization, and calibration of silicon micro machinedpiezo-resistive pressure sensors ranging from 1.2 (0.12) to 400 bar (40 MPa)fabricated at the National Nano Fabrication Centre (NNFC) of the Centre for NanoScience and Engineering (CeNSE) at the Indian Institute of Science, Bangalore inIndia are presented in the following sections of this chapter The analysis and theexperimental results on the devices fabricated have shown that the best results interms of sensitivity and accuracy can be achieved by appropriately laying out theresistors either inside or outside the diaphragm, depending on the diaphragmdimensions and aspect ratios, which are decided by the maximum pressure range
of operation The chapter also brings out the various critical issues encounteredduring packaging and calibrating the pressure sensors
2 FEM Analysis and Diaphragm Design Considerations
Based on the theory of plates [4], which assumes that the diaphragm is anchoredall around its edges (as shown in Fig.1a), the location of the maximum stress isusually identified to be at the center of the edge of the diaphragm and hence thepiezo-resistors are conventionally embedded on the inner side of the diaphragmedge However, for the silicon micro machined diaphragms, realized either byDeep Reactive Ion Etching (DRIE) or wet chemical anisotropic etching, thephysical location of the anchor position is on the backside of the chip as shown inFig.1b and c Hence, the maximum stress position with respect to the diaphragmand the positions of piezoresitors on the chip need to be assessed
A rigorous 3D FEM-based COMSOL [5, 6] simulation of these bulk micromachined diaphragms has indeed shown that the position of the longitudinal peakstress component, estimated along the line XX’ (marked in Fig.1d) lies outside thediaphragm edge at a distance Xp (marked in Fig.1b and c), when the aspect ratio,length/height (L/h), of the diaphragm is low In Fig.2we show the typical resultobtained for the case of a DRIE etched diaphragm having thickness h = 200 lmand lateral dimension L = 750 lm, for different magnitudes of pressure applied onthis DRIE diaphragm as shown in the inset For this case, the L/h ratio is 3.75 andthe location of the peak stress lies outside the diaphragm edge at a distance
Xp= 75 lm It is also interesting to note that the position of the peak stressremains the same irrespective of the magnitude of the pressure applied
The effects of aspect ratio (L/h) on the position Xp of the peak longitudinalstress, for an applied pressure P = 100 bar is studied using the FEM simulationtool, considering L/h ratios ranging from 2.5 to 8.5 by varying L from 500 to
Trang 29Fig 1 Cross-section of the diaphragm a anchored on all sides (as in the theory of plates) b and
c anchored on the backside (as obtained in the DRIE and KOH etched silicon) d Top view of the chip showing the square diaphragm of side length L (= 2a) by dashed line The side length of the square chip is shown as 2A
Fig 2 FEM analysis results showing the stress distribution along XX’ for different magnitudes
of pressure P (in bars) = 10, 25, 50, 75, and 100 applied on a DRIE diaphragm having
h = 200 lm and L = 750 lm, and a square chip having the side length 2A = 2 mm,
t = 400 lm
Trang 301700 lm and keeping the DRIE etched diaphragm thickness fixed at h = 200 lm.The results are shown in Fig.3 The distance (Xp) between the edge of the dia-phragm and the position of peak as a function of L/h ratio determined for the caseshaving h = 200 lm and h = 20 lm are shown in Table1a and b.
We also determined the effect of the diaphragm lateral length L on the position
of the peak stress (Xp), with a fixed diaphragm thickness, h = 100 lm, consideringboth DRIE etched and KOH etched diaphragms with crosssection shown inFig.1b, c The results obtained from all the simulation studies involving variousthicknesses and L/h ratios are shown in Fig.4, where Xp is plotted versus L/h ratio
It can be seen that in general, Xp is positive when the aspect ratio is below eightindicating that the peak stress lies outside the diaphragm portion for these cases As
it can be seen from Fig.4, in the case of thick diaphragms with h = 200 lm thatare used for high-pressure applications, the location of peak stress lies at
Xp= +50 lm outside the diaphragm edge when L/h ratio is equal to 5, sponding to L = 1000 lm On the other hand when L/h [ 8, corresponding to thecases L [ 1600 lm, with h = 200 lm, Xp becomes negative showing that thelocation of the peak stress shifts onto the diaphragm surface In this situation as thediaphragm is too large the pressure range of operation decreases In the case of thindiaphragms of the order of 20 lm thickness, Xp = 0 or very small (Xp = +1 to+3 lm) Thus, in situations where the diaphragm is thin, the theory of plates holdsgood with the maximum stress occurring at the diaphragm edge
corre-Fig 3 FEM analysis results showing the variation of stress along XX’ for a 200 lm thick DRIE etched diaphragm, for different diaphragm side lengths (L) as running parameter, when a pressure
of 100 bar is applied
Trang 31Table 1 Variation of peak position relative to the diaphragm edge (Xp) and the maximum total stress as the L/h ratio is changed for a DRIE etched diaphragm of thickness a h = 200 lm.
P = 100 bar and b h = 20 lm, P = 1 bar
100, 200 lm, and for the KOH etched diaphragms with h = 100 lm
Trang 323 Pressure Sensor Design and Fabrication
3.1 Pressure Sensor for Operation up to 400 bar
The lateral dimension of chip was chosen to be 2 9 2 mm, and based on the FEMsimulations a reasonable diaphragm dimension of 750 9 750 lm and a diaphragmthickness of 210 lm was chosen to ensure that the maximum stress on chip is only0.3 GPa at 400 bar, so that the maximum stress is well below 1 Gpa even at1,000 bar Once again the maximum stress versus pressure was determined to belinear over the pressure range 0–400 bar The resistors of the Wheatstone bridge ofthe sensors were placed outside the diaphragm at a distance of 77 lm from thediaphragm edge Considering a sheet resistance of 200 ohm/square, individualresistor dimensions were decided to be L/W = 20 A mask layout for a five-maskprocess was designed and the mask plates were prepared at the NNFC of CeNSE atIISc Figure5shows the composite mask layout of the five-mask process.Each of the process steps are marked alongside the individual masks Thestarting wafer is an SOI (100) wafer with N-type device layer thickness 210 lm,
Fig 5 Composite mask layout for the 400 bar Pressure sensor
Trang 33BOX layer of 1 lm, and P type handle wafer thickness 400 lm This wafer isthermally oxidized and P+ diffusion window is opened using Mask#1 in the oxideand boron diffusion is carried out in this region at 1,100C for 30 min to achieve asheet resistance in the range 5-6 ohm/square This is followed by ion implanta-tion at 80 KeV with a dose of 3 9 1014Boron ions/cm2into the region opened inthe oxide using Mask#2 Thermal annealing is done at 1,000C in Nitrogenambient for 30 min to achieve a sheet resistance of 180-190 ohms/square Fol-lowing this step, backside alignment lithography is carried out aligned with respect
to the patterns already created, using the Mask#3 to open window in the backside.DRIE is carried out using Bosch process with etch rates of 10 lm/min initially and
4 lm/min during the last 10 min, using the photoresist as the masking layer Afterstripping of the PR in oxygen plasma aluminum metallization is carried out andpatterned using Mask#4 Next, the Forming Gas Anneal (FGA) is carried out for
30 min at 450C This is followed by deposition of silicon dioxide by PECVD at
350C to a thickness of 0.1 lm In the final step, lithography is carried out usingMask#5 and the pad oxide and scribe lines are etched The backside oxide isremoved protecting the front surface and borofloat glass is anodically bonded on tothe backside in an evacuated bonding system During the bonding process thetemperature is maintained at 390C and the glass is biased at a negative voltage of1,000 V for 30 min as shown in Fig.6
A photograph of the completed pressure sensor after the anodic bonding isshown in Fig.7 The wafer is next diced using a diamond saw and then diesmounted on a header and wire bonded A photograph of the diced sensor and the die
Fig 6 Screenshot taken during anodic bonding of silicon wafer to glass The high current pulse indicates the successful completion of bonding process
Trang 34mounted and wire bonded sensor is shown in Fig.8a and b respectively Figure9shows the packaged 400 bar pressure sensor with compensating electronics.
3.2 Pressure Sensor for Operation up to 1.2 bar
Based on the FEM analysis similar to that presented in Sect 2, a thin squarediaphragm of h = 25 lm and L =1 mm is chosen for this pressure range (0-1,
2 bar) The FEM-based COMSOL simulated stress distribution across the
Fig 7 Photograph of processed and anodic bonded 100 mm silicon wafer showing about 700 pressure sensors The devices occupy only the 75 mm diameter area
Fig 8 a Front side view and backside view of the pressure sensor die after dicing b Pressure sensor die mounted on the header and wire bonded
Trang 35diaphragm along the XX’ line (as in Fig.1d) is shown in Fig.10 It can be seen thatthe maximum stress occurs at the edge of the diaphragm For this situation of highL/h ratio = 40, the theory of plates is applicable as discussed inSect 2and hencethe maximum longitudinal stress is estimated to be equal to 48 MPa at the center ofthe diaphragm edge, for the applied pressure P = 0.12 MPa (1.2 bar) using the
Fig 9 Photograph of the packaged 400 bar pressure sensor along with electronics, a Without the connector and pressure port b With the connector and the welded pressure port
Fig 10 Stress distribution across the top surface of a square diaphragm with its thickness
h = 25 lm and side length L = 1 mm for pressure P = 0-1.2 bar
Trang 36analytical expression rL¼ P L=2hð Þ2 This value is very close to the value of
46 MPa determined using the FEM-based analysis with COMSOL (see Fig.10)
As in the case of 400 bar sensor, in this case also the starting wafer is SOI wafer,the only difference being in the SOI layer thickness, which in this case is h = 25 lm.The mask layout, the number of masks, and process parameters are exactly the same
as the 400 bar sensor However, as the aspect ratio is L/h = 40 in this case, theposition of the piezo-resistors is at the edge on the inner side of the diaphragm At theend of the five-mask process, anodic bonding of the wafer to glass is carried out andthe individual dies are separated by dicing and followed by die mounting wirebonding and other packaging steps The packaged devices are calibrated and elec-tronically compensated for temperature drift Figure11shows the photographs ofthe packaged 1.2 bar pressure sensors alongwith electronics and EMI filters
4 Testing, Calibration and Temperature Compensation
of the Pressure Sensors
4.1 Setup for Testing Packaged Sensors
The photograph of a Hydraulic Pressure Calibrator, procured from M/s DHB, UK.Model DHB 42 H-542, capable of operation in the range of 0-1,200 Bar is shown
in Fig.12 The transducer to be tested is mounted on the calibrator adapter andelectrical connections are made to stabilized power supply, digital voltmeter(DVM), and decade box This setup is used to calibrate the 0-400 bar MEMSsensor in five equal ascending and descending steps In addition, proof pressureapplication, burst pressure trials, and testing of glass to metal seals are also carriedout up to 800 Bars
Fig 11 Photographs of 1.2 bar pressure sensors packed and hermetically sealed with electronics
Trang 374.2 Testing and Temperature Compensation
of 1200 milli Bar Pressure Sensor
The 0-1,200 milli bar MEMS-based pressure transducers were wire bonded,encapsulated, and then tested through a wide range of temperatures (-40C, 0 C,+25C, +50 C, and +80 C) Figure 13 shows the raw milli volt output atvarious temperatures with respect to input pressure
From the above results, the drift in the range of 1-13910-3/FSO/C may benoted in the Zero Offset and Full Scale Output (FSO) with temperature In terms ofactual values, the drift in Zero Offset is as high as 50.34 mV between 25C and -
40C and the drift in the full scale output voltage is 56.95 mV at 1,200 milli bars.Similarly, the drift in Zero Offset and FSO between 25C and 80 C was found to
be 15.83 mV and 24.12 mV respectively To compensate for these drifts, weutilize active temperature compensation technique using advanced differentialsensor signal conditioning CMOS IC ZMD 31050 This IC contains programmablegain amplifier, multiplexer, built-in temperature sensor, ADC, DAC, PWM, ROM,EEPROM, analog output, I2C, digital interface and other blocks After program-ming the compensation circuit and retesting the overall drift is reduced to
1910-4-1910-5/FSO/C and thus the Zero Offset and FSO can be adjusted tosuit many requirements Figure14 shows the linear and repeatable output at
Packaged Pressure sensor Under test
Fig 12 Hydraulic calibration set-up to calibrate 0-400 bar pressure transducers at CeNSE, IISc
Trang 38+25C, -33.5 C and +65 C, randomly chosen temperatures for the validation
of active compensation The maximum nonlinearity and hysteresis was also found
to be within 0.5 % FSO To utilize these transducers for aerospace application,specific EMI filters and necessary protection diodes were also incorporated in thecircuit and tested from 16 to 36 V DC excitation
The transducer was subjected to proof pressure of 2.4 bar, twice the nominalpressure and random vibration tests for their survival under harsh environment.The drift after these tests is found to be within the allowable limits
4.3 Testing and Calibration of 400 Bar (Gauge) Pressure
Transducer Output at Different Temperatures
The 0-400 bar absolute MEMS pressure transducer was temperature sated Figure15 shows a linear output from -40 to +80C and the overalltemperature drift was found to be within 1910-4- 6910-5/FSO/oC The sensorwas also calibrated at +80C, +50 C, +25 C, -20 C, and -40 C for fiveascending and descending equal pressure intervals (80 bar) The inset shows thephotograph of a 0-400 bar Pressure sensor with built-in electronics having avoltage regulator and ZMD 31050 signal conditioning IC for active temperaturecompensation along with sensor protection filter at the pressure end The inputexcitation can be from 16 to 36 V DC The nominal excitation is 28 V DC TheMaximum nonlinearity and hysteresis of this transducer was found to be within0.855 % FSO, as calculated using least squares best fit straight line method.The pressure end connection has M1491.5 thread for 10 mm length with an ‘‘O’’
compen-Fig 13 Output voltage versus pressure at various temperatures with the 1.2 bar pressure sensor before compensation
Trang 39Fig 14 Temperature compensated output versus pressure at different temperatures for the 1.2 bar pressure (Gauge) sensor
Fig 15 Temperature compensated output voltage versus pressure from the 400 bar pressure transducer at different temperatures
Trang 40ring groove for arresting the leak during mechanical interfacing We employ laser
or electron beam welding, AISI 304L stainless steel assembly for corrosionresistance and robust mechanical integrity
The MEMS piezo-resistive sensor is mounted on a glass to metal seal (normallycalled as ‘‘Header’’) made out of Kovar metal with matching glass to withstand apressure of above 800 bars The insulation resistance between all the leads of thisglass to metal seal with the body of the transducer is above 100 mega ohms at
50 V DC for proper isolation as per aerospace requirements This assembly is alsohelium leak tested for a leak rate better than 10-8sccm/sec for long-term oper-ational stability This transducer is tested under random vibration conditions in Xand Y axes at 13.5 g rms, over a frequency range of 20 Hz-2 KHz for 3 minutes.After, all the calibration and testing, the drift was within allowable limits
4.4 Dynamic Testing on the Pressure Sensor
To experimentally verify the output response of 1,200 milli bar pressure ducer, a simple dynamic test setup was rigged up as shown in Fig.16consisting of
trans-a low pressure source, 3-wtrans-ay vtrans-alve, required tubing, cltrans-amp, power supply, digittrans-alvoltmeter, storage oscilloscope, and related accessories A balloon was pressurized
so that the considerable output can be recorded through the transducer under test
Fig 16 Dynamic pressure testing on 1,200 milli bar absolute MEMS-based pressure transducer