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67 ICRTEDC -2014
Vol. 1, Spl. Issue 2 (May, 2014) e-ISSN: 1694-2310 | p-ISSN: 1694-2426
GV/ICRTEDC/16
SIMULATION OF MEMS
MICROHOTPLATE FOR METAL OXIDE
GAS SENSORS: REVIEW
1
Manju Ahuja, 2
Rajneesh Talwar, 3
B. Prasad
1
ECE Department ,RIMT-IET, Mandi Gobindgarh, Punjab, India
2
Principal, Chandigarh college of Engineering, Landran India
3
Professor, Electronics Science Department, Kurukshetra University, Kurukshetra, Haryana, India
1
manjugulati2007@gmail.com, 2
rtphdguidance@gmail.com, 3
bprasad2005@gmail.com
Abstract: Simulation of gas sensor with integrated micro
hotplate (MHP) of ultra low power consumption is
reviewed. Various parameters of gas sensor and MHP as
power, temperature ,heat insulation ,stress analysis and
deflection is studied using various Multiphysics
simulation tools like ANSYS and Conventorware.
Microheaters have been widely investigated because of
their extensive applications in gas sensors, flow rate
sensors and other microsystems. The microheaters are
designed to ensure low power consumption, low thermal
mass and better temperature uniformity. Thus optimization
of micromachined heater for sensing applications is
designed to withstand high-temperature.
Keywords : Microhotplate, Gas sensor, Micromachine
1. INTRODUCTION
We are gifted by nature with five senses. We are able to
feel and experience the surroundings through our sense of
touch, smell, taste etc. As we have progressed we have
started to understand the limitations of these senses which
we were once very proud of and realized sometimes the
sense organs can give unreliable information. Temperature
sensing is a classic example. Humans have developed very
reliable sensors for temperature, pressure, humidity etc.
measurements. Increase in the industrialization, an
offshoot of human evolution brought in the need to detect
the presence of certain chemical species especially gases.
Such sensors are not only required for the qualitative
estimates but very often quantitative estimate is
necessary for the production. Many of the gases used in
the industries could be fatal to humans. So it may be of
paramount importance to detect and monitor them outside
the work area. So a lot of efforts have gone into the
detection and monitoring of gases used in the industry.
Air pollution from various offensive gases has
been a serious problem in modern life. Gas detection is
important because it is necessary in many different fields,
for example, industrial emission control, household
security, vehicle emission control and environmental
monitoring etc. For example, Methane gas (CH ) affects
global warming 20 times more severely than carbon
dioxide gas (CO ). It is explosive, due to its high volatility
and flammability in air and in closed areas, methane gas
may cause suffocation. Controlling and monitoring of CO
is of great importance in environmental and industrial
fields. Similarly Ammonia gas (NH ) is produced and
utilized extensively in many chemical industries, fertilizer
factories, refrigeration systems, food processing, medical
diagnosis, fire power plants etc. A leak in the system can
results in the health hazards. Ammonia is toxic to human
at higher concentration. The exposure of ammonia causes
chronic lung disease, irritating and even burning the
respiratory track etc. Environmental pollution is a burning
global issue. So in many aspects of today's life, the use of
gas sensors becomes increasingly important.
For evaluating the performance of gas sensors, several
indicators should be considered: sensitivity: the minimum
value of target gases volume concentration when they
could be detected , selectivity: the ability of gas sensors to
identify a specific gas among a gas mixture , response
time: the period from the time when gas concentration
reaches a specific value to that when sensor generates a
warning signal , energy consumption ,reversibility:
whether the sensing materials could return to its original
state after detection ,adsorptive capacity (also affects
sensitivity and selectivity) ,fabrication cost [1].
2. METAL OXIDE GAS SENSING
Gas detection can be carried out by a wide range of
physical, chemical, electrochemical and optical principles.
Broadly, for gas monitoring, different kinds of sensor
systems can be used: Spectroscopic, Optical and Solid
State are the three main families of gas sensors.
Spectroscopic systems are those based on the direct
analysis of fundamental gas properties, such as molecular
mass or vibrational spectrum. Optical sensor systems are
based on the measurement of the absorption spectra after
light stimulation and metal oxides are based on the
change of physical and/or chemical properties of a sensing
material after gas exposure [2].
Metal oxide semiconductor gas sensors are utilised in a
variety of different roles and industries. They are relatively
inexpensive compared to other sensing technologies,
robust, lightweight, long lasting and benefit from high
material sensitivity and quick response times. They have
been used extensively to measure and monitor trace
amounts of environmentally important gases such as
carbon monoxide and nitrogen dioxide. Many metal
oxides are suitable for detecting combustible, reducing, or
oxidizing gases by conductive measurements. The
following oxides show a gas response in their
ICRTEDC-2014 68
conductivity: Cr2O3, Mn2O3, Co3O4, NiO, CuO, SrO,
In2O3, WO3, TiO2, V2O3, Fe2O3, GeO2, Nb2O5,
MoO3, Ta2O5, La2O3, CeO2, Nd2O3 . Metal oxides
selected for gas sensors can be determined from their
electronic structure. The range of electronic structures of
oxides is so wide that metal oxides were divided into two
the following categories :
(1) Transition-metal oxides (Fe2O3, NiO, Cr2O3, etc.)
(2) Non-transition-metal oxides, which include (a) pre-
transition-metal oxides (Al2O3, etc.)
(b) post-
transition-metal oxides (ZnO, SnO2 etc.)
Pre-transition-metal oxides (MgO, etc.) are expected to be
quite inert, because they have large band gaps. Neither
electrons nor holes can easily be formed. They are seldom
selected as gas sensor materials due to their difficulties in
electrical conductivity measurements .Post transition metal
oxides are widely used[3].
3. SIMULATION USING MEMS DESIGN TOOL
Any scientific research method involves a mutual
interdependence between experimental work and
theoretical work. An important bridge between the
experimental work and theoretical studies of a specific
research is the computer experiment or simulations. The
basic idea in computer simulations is to design and
simulate the actual physical system and to analyze the
simulation results. The main advantage is, complicated
physical systems can be easily studied, helping us
understand and predict the system by saving time & cost.
Therefore, modeling and simulations are required to adjust
and optimize the sensor for any specific application, prior
to fabrication of the device. Today a broad spectrum of
options for simulation is available; researchers use
everything from basic programming languages to various
high-level packages implementing advanced methods.
How much simplification takes place in the translation
process helps to determine the accuracy of the resulting
model. Much of the physics requires a three dimensional
simulations for a more accurate result. The finite element
analysis (FEA) tools Conventorware, ANSYS ,COMSOL,
ABAQUS can be employed to optimize sensor design
[4].
3.1 Microheater/Microhotplate simulation :Metal oxide
gas sensor require a device which can produce elevated
temperature (250 C -500 C) with small power
consumption. Microhotplate is used to produce the
elevated temperature for gas sensing films. Design of
heater, analysis of temperature distribution on the
sensitive layer and sensitivity, which is temperature
dependent, good mechanical stability at higher
temperature are main issues of heater for metal oxide gas
sensing applications . For these objectives, the thermal
characteristics of the microhotplate are optimized by
controlling the heat losses, dielectric materials and heater
configuration.
Many of existing gas sensors may not be suitable to make
high precision measurements of gas concentrations but
they can give only qualitative estimate such as presence of
given gas. At present, general gas sensors have some
common limitations like bulky, low consistency and high
power consumption. So there is an urgent need for the
development of small, low cost, high sensitivity, good
selectivity reliable sensors for control and measuring
gases, for automation of services with an excellent
performance, reliability and low price. The novel gas
sensor based on ‘‘micro-electro-mechanical systems
(MEMS)’’ adopts the traditional semiconductor
technology, and has many advantages in consistency,
homogeneity and microminiaturization, which make it
easy to achieve integration and low power consumption.
Thus the development of miniaturized gas sensors is an
increasingly active area of research. Such devices,
particularly when they feature low mass and low power
budgets, can impact a broad range of applications
including industrial process monitoring, building security
and extra terrestrial exploration [5].
Platinum based micro hotplates offer the advantages of
reliability, stable temperature coefficient of resistance
(TCR) and reproducibility. In literature [6], for
microheater design ,on Silicon substrate there are SiO2
and Si N dielectric layers.
Table 1: Temperature (K) distribution of different hotplate
membranes with different applied voltages
Membran
e Material
Heater
Temperature
at
Applied
voltage=1V
with 7.8mW
Power
Consumptio
n
Heater
Temperature
at
Applied
voltage=2V
with
31.3mW
Power
Consumptio
n
Heater
Temperature
at
Applied
voltage=3V
with
70.5mW
Power
Consumptio
n
SiO 395 689 1177
Si N 369 585 945
Si N
SiO2 346 491 733
The dimensions of the microhotplate membrane are
220×220 μm .The design consists of a square opening of
200×200 μm in back side of the Si substrate which is
500 μm thick. SiO and Si N layers are 1 μm and 0.35μm
thick respectively and platinum heater is laid over it. The
gap between the heating elements and width is 20 m with
thickness .3 m. The summary of the temperature (K)
distribution of platinum-based microhotplate with different
dielectric membranes are shown in Table 1 .
69 ICRTEDC -2014
Fig 1 : Temperature Vs Applied voltage
SiO2 membrane-based microhotplate has the higher
temperature in comparison to
Si N and both combination of SiO2 and
membranes Si N at same power consumption as shown
in fig 1. It is because that the thermal diffusivity of SiO2 is
smaller than the thermal diffusivity of Si N and
combination of SiO2 and Si N films .
Similarly the effects of various thicknesses of the heater
layer on the power consumption of the MHP are
evaluated, which is shown in Table 2.
Table 2 :Variation of power consumption with different voltages
for various heater layer thicknesses
Heater
Thickness
' m'
Power
consumption
'mW' at 1V
Power
consumption
'mW' at 2V
Power
consumption
'mW' at 3V
.3 7.84 31.3 70.5
.5 13.07 52.28 117.64
1 26.14 104.57 235.29
Variation of power consumption with thickness of heater
layer with voltage in fig 2.
Fig 2 : Power consumption Vs Applied voltage with different
heater layer thicknesses
Similarly for modeling and simulation of a micromachined
microhotplate (MHP) using (Si3N4) and silicon carbide
(SiC) membrane is designed to achieve low power
dissipation and uniform temperature distribution on the
sensing area at operating temperatures of up to 700°C
.Temperature gradient on the MHP decreases as the
thickness of the SiC is increased and is a minimum with a
value of 0.005°C/µm for SiC thickness of 2 μm and above.
A comparison between simulation and mathematically
modeled results for power dissipation and current density
of the MHP showed close agreement. An optimized
simulated device exhibited low power dissipation of 9.25
mW and minimum mechanical deflection of 1.2 μm at the
elevated temperature of 700°C [7].
In another paper, a design and analysis of an array of
100nm thin film MEMS based microheater on SOI wafer
is presented. The microheater is constructed on a SOI
wafer where temperature rise of 200°C is achieved with
minimum power consumption of 20mW.Also there is
minimum heat loss through the substrate. The temperature
rise is concentrated in only the microheater region and
there is excellent uniformity in the temperature
distribution in both the microheaters. Maximum stress
developed in oxide layer is 326 MPa which is within the
range of their breaking stress [8].
3.2 Simulation of gas sensing structure :
In literature novel design of metal-oxide NO2 gas sensor
integrated with micro heaters is presented in which
thermal simulation of heat insulation between sensing
diaphragm and substrate is carried which conclude that
heat loss can be neglected when the gap between substrate
and sensing membrane is larger than 15 µm. Also
Electro-thermo analysis of the micro heater is carried and
found when 2V applied voltage temp. is achieved at
215°C with uniform temp. distribution ,time response of
the heater is less than 0.1s , maximum displacement due
to thermal stress is less than 0.26 um. In stress analysis it
was found Maximum Von Mises stress is 127 kPa [9].
4. CONCLUSION
In the study of simulation of gas sensors and microhotplate
various parameters power, temperature distribution,
stress, displacement with variation of substrate thickness
, using different substrate materials ,different heater
material ,heater layer thickness are optimized.
5. FUTURE SCOPE
Keeping in the view of the objectives of miniaturization ,
portability, maximum sensitivity and compatible with
existing silicon planer technology Further different heater
geometries with different materials can be analysed. As
gas detection sensitivity is function of temperature an
attempt will be made to make temperature zones in the
sensor arrays which could enable us to use the same
sensors for different gases using COMSOL Multiphysics
especially for toxic gases such as NH , CH & CO .
REFERENCES
1. Xiao Liu , Sitian Cheng “A Survey on Gas Sensing
Technology '' Sensors vol.12 , pp. 9635- 9665, 2012.
2. Tanusree Majhi, MS Thesis ''Elctrothermal design and
fabrication of MEMS based microheater using a novel nickel
alloy for methane gas sensor based on nanocrystalline ZnO
thin film'' Jadavpur University,2006.
3. Chengxiang et al. “Metal Oxide Gas Sensors: Sensitivity and
Influencing Factors'' Sensors, Vol 10, pp 2088-2106, 2010.
1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.6 2.8 3
300
400
500
600
700
800
900
1000
1100
1200
Voltage (V)
Temperature(K) SiO2
Si3N4
SiO2+Si3N4
1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.6 2.8 3
0
50
100
150
200
250
Voltage(V)
PowerConsumption(mW)
.3 micron
.5 micron
1 micron
ICRTEDC-2014 70
4. Chenxu Zhao ,Ph.D Thesis ''Automated synthesis of Mixed
technology Mixed system with electronic system''
University of Southampton,2010.
5. Bijoy Kantha''Design and simulation of MEMS Microhotplate
for gas sensor applications'' Jadavpur University ,2010.
6. Mahanth Prasad “FEM simulation of platinum-based
microhotplate using different dielectric membranes for gas
sensing applications’’ published in “sensors & transducers
“in 2010.
7. John Ojur Dennis, Abdelaziz Yousif, Mohamad Naufal
Mohamad “Design, simulation and modelling of a high
temperature microhotplate for application in trace gas
detection” published in “International Journal of Engineering
& Technology'' 2010.
8. Avigyan Datta Gupta et al “Design and Analysis of MEMS
Based Microheater Array on SOI Wafer for Low Power Gas
Sensor Applications’’ published in “International Journal of
Scientific & Engineering Research '' 2010.
9. Ling-Han Li et al. “Design and Simulation of an Integrated
Metal Oxide Based Micro NO2 Gas Sensor ” presented in
“International symposium on Micro-Nano Mechatronics and
Human Science’’2006.

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SIMULATION OF MEMS MICROHOTPLATE FOR METAL OXIDE GAS SENSORS: REVIEW

  • 1. 67 ICRTEDC -2014 Vol. 1, Spl. Issue 2 (May, 2014) e-ISSN: 1694-2310 | p-ISSN: 1694-2426 GV/ICRTEDC/16 SIMULATION OF MEMS MICROHOTPLATE FOR METAL OXIDE GAS SENSORS: REVIEW 1 Manju Ahuja, 2 Rajneesh Talwar, 3 B. Prasad 1 ECE Department ,RIMT-IET, Mandi Gobindgarh, Punjab, India 2 Principal, Chandigarh college of Engineering, Landran India 3 Professor, Electronics Science Department, Kurukshetra University, Kurukshetra, Haryana, India 1 manjugulati2007@gmail.com, 2 rtphdguidance@gmail.com, 3 bprasad2005@gmail.com Abstract: Simulation of gas sensor with integrated micro hotplate (MHP) of ultra low power consumption is reviewed. Various parameters of gas sensor and MHP as power, temperature ,heat insulation ,stress analysis and deflection is studied using various Multiphysics simulation tools like ANSYS and Conventorware. Microheaters have been widely investigated because of their extensive applications in gas sensors, flow rate sensors and other microsystems. The microheaters are designed to ensure low power consumption, low thermal mass and better temperature uniformity. Thus optimization of micromachined heater for sensing applications is designed to withstand high-temperature. Keywords : Microhotplate, Gas sensor, Micromachine 1. INTRODUCTION We are gifted by nature with five senses. We are able to feel and experience the surroundings through our sense of touch, smell, taste etc. As we have progressed we have started to understand the limitations of these senses which we were once very proud of and realized sometimes the sense organs can give unreliable information. Temperature sensing is a classic example. Humans have developed very reliable sensors for temperature, pressure, humidity etc. measurements. Increase in the industrialization, an offshoot of human evolution brought in the need to detect the presence of certain chemical species especially gases. Such sensors are not only required for the qualitative estimates but very often quantitative estimate is necessary for the production. Many of the gases used in the industries could be fatal to humans. So it may be of paramount importance to detect and monitor them outside the work area. So a lot of efforts have gone into the detection and monitoring of gases used in the industry. Air pollution from various offensive gases has been a serious problem in modern life. Gas detection is important because it is necessary in many different fields, for example, industrial emission control, household security, vehicle emission control and environmental monitoring etc. For example, Methane gas (CH ) affects global warming 20 times more severely than carbon dioxide gas (CO ). It is explosive, due to its high volatility and flammability in air and in closed areas, methane gas may cause suffocation. Controlling and monitoring of CO is of great importance in environmental and industrial fields. Similarly Ammonia gas (NH ) is produced and utilized extensively in many chemical industries, fertilizer factories, refrigeration systems, food processing, medical diagnosis, fire power plants etc. A leak in the system can results in the health hazards. Ammonia is toxic to human at higher concentration. The exposure of ammonia causes chronic lung disease, irritating and even burning the respiratory track etc. Environmental pollution is a burning global issue. So in many aspects of today's life, the use of gas sensors becomes increasingly important. For evaluating the performance of gas sensors, several indicators should be considered: sensitivity: the minimum value of target gases volume concentration when they could be detected , selectivity: the ability of gas sensors to identify a specific gas among a gas mixture , response time: the period from the time when gas concentration reaches a specific value to that when sensor generates a warning signal , energy consumption ,reversibility: whether the sensing materials could return to its original state after detection ,adsorptive capacity (also affects sensitivity and selectivity) ,fabrication cost [1]. 2. METAL OXIDE GAS SENSING Gas detection can be carried out by a wide range of physical, chemical, electrochemical and optical principles. Broadly, for gas monitoring, different kinds of sensor systems can be used: Spectroscopic, Optical and Solid State are the three main families of gas sensors. Spectroscopic systems are those based on the direct analysis of fundamental gas properties, such as molecular mass or vibrational spectrum. Optical sensor systems are based on the measurement of the absorption spectra after light stimulation and metal oxides are based on the change of physical and/or chemical properties of a sensing material after gas exposure [2]. Metal oxide semiconductor gas sensors are utilised in a variety of different roles and industries. They are relatively inexpensive compared to other sensing technologies, robust, lightweight, long lasting and benefit from high material sensitivity and quick response times. They have been used extensively to measure and monitor trace amounts of environmentally important gases such as carbon monoxide and nitrogen dioxide. Many metal oxides are suitable for detecting combustible, reducing, or oxidizing gases by conductive measurements. The following oxides show a gas response in their
  • 2. ICRTEDC-2014 68 conductivity: Cr2O3, Mn2O3, Co3O4, NiO, CuO, SrO, In2O3, WO3, TiO2, V2O3, Fe2O3, GeO2, Nb2O5, MoO3, Ta2O5, La2O3, CeO2, Nd2O3 . Metal oxides selected for gas sensors can be determined from their electronic structure. The range of electronic structures of oxides is so wide that metal oxides were divided into two the following categories : (1) Transition-metal oxides (Fe2O3, NiO, Cr2O3, etc.) (2) Non-transition-metal oxides, which include (a) pre- transition-metal oxides (Al2O3, etc.) (b) post- transition-metal oxides (ZnO, SnO2 etc.) Pre-transition-metal oxides (MgO, etc.) are expected to be quite inert, because they have large band gaps. Neither electrons nor holes can easily be formed. They are seldom selected as gas sensor materials due to their difficulties in electrical conductivity measurements .Post transition metal oxides are widely used[3]. 3. SIMULATION USING MEMS DESIGN TOOL Any scientific research method involves a mutual interdependence between experimental work and theoretical work. An important bridge between the experimental work and theoretical studies of a specific research is the computer experiment or simulations. The basic idea in computer simulations is to design and simulate the actual physical system and to analyze the simulation results. The main advantage is, complicated physical systems can be easily studied, helping us understand and predict the system by saving time & cost. Therefore, modeling and simulations are required to adjust and optimize the sensor for any specific application, prior to fabrication of the device. Today a broad spectrum of options for simulation is available; researchers use everything from basic programming languages to various high-level packages implementing advanced methods. How much simplification takes place in the translation process helps to determine the accuracy of the resulting model. Much of the physics requires a three dimensional simulations for a more accurate result. The finite element analysis (FEA) tools Conventorware, ANSYS ,COMSOL, ABAQUS can be employed to optimize sensor design [4]. 3.1 Microheater/Microhotplate simulation :Metal oxide gas sensor require a device which can produce elevated temperature (250 C -500 C) with small power consumption. Microhotplate is used to produce the elevated temperature for gas sensing films. Design of heater, analysis of temperature distribution on the sensitive layer and sensitivity, which is temperature dependent, good mechanical stability at higher temperature are main issues of heater for metal oxide gas sensing applications . For these objectives, the thermal characteristics of the microhotplate are optimized by controlling the heat losses, dielectric materials and heater configuration. Many of existing gas sensors may not be suitable to make high precision measurements of gas concentrations but they can give only qualitative estimate such as presence of given gas. At present, general gas sensors have some common limitations like bulky, low consistency and high power consumption. So there is an urgent need for the development of small, low cost, high sensitivity, good selectivity reliable sensors for control and measuring gases, for automation of services with an excellent performance, reliability and low price. The novel gas sensor based on ‘‘micro-electro-mechanical systems (MEMS)’’ adopts the traditional semiconductor technology, and has many advantages in consistency, homogeneity and microminiaturization, which make it easy to achieve integration and low power consumption. Thus the development of miniaturized gas sensors is an increasingly active area of research. Such devices, particularly when they feature low mass and low power budgets, can impact a broad range of applications including industrial process monitoring, building security and extra terrestrial exploration [5]. Platinum based micro hotplates offer the advantages of reliability, stable temperature coefficient of resistance (TCR) and reproducibility. In literature [6], for microheater design ,on Silicon substrate there are SiO2 and Si N dielectric layers. Table 1: Temperature (K) distribution of different hotplate membranes with different applied voltages Membran e Material Heater Temperature at Applied voltage=1V with 7.8mW Power Consumptio n Heater Temperature at Applied voltage=2V with 31.3mW Power Consumptio n Heater Temperature at Applied voltage=3V with 70.5mW Power Consumptio n SiO 395 689 1177 Si N 369 585 945 Si N SiO2 346 491 733 The dimensions of the microhotplate membrane are 220×220 μm .The design consists of a square opening of 200×200 μm in back side of the Si substrate which is 500 μm thick. SiO and Si N layers are 1 μm and 0.35μm thick respectively and platinum heater is laid over it. The gap between the heating elements and width is 20 m with thickness .3 m. The summary of the temperature (K) distribution of platinum-based microhotplate with different dielectric membranes are shown in Table 1 .
  • 3. 69 ICRTEDC -2014 Fig 1 : Temperature Vs Applied voltage SiO2 membrane-based microhotplate has the higher temperature in comparison to Si N and both combination of SiO2 and membranes Si N at same power consumption as shown in fig 1. It is because that the thermal diffusivity of SiO2 is smaller than the thermal diffusivity of Si N and combination of SiO2 and Si N films . Similarly the effects of various thicknesses of the heater layer on the power consumption of the MHP are evaluated, which is shown in Table 2. Table 2 :Variation of power consumption with different voltages for various heater layer thicknesses Heater Thickness ' m' Power consumption 'mW' at 1V Power consumption 'mW' at 2V Power consumption 'mW' at 3V .3 7.84 31.3 70.5 .5 13.07 52.28 117.64 1 26.14 104.57 235.29 Variation of power consumption with thickness of heater layer with voltage in fig 2. Fig 2 : Power consumption Vs Applied voltage with different heater layer thicknesses Similarly for modeling and simulation of a micromachined microhotplate (MHP) using (Si3N4) and silicon carbide (SiC) membrane is designed to achieve low power dissipation and uniform temperature distribution on the sensing area at operating temperatures of up to 700°C .Temperature gradient on the MHP decreases as the thickness of the SiC is increased and is a minimum with a value of 0.005°C/µm for SiC thickness of 2 μm and above. A comparison between simulation and mathematically modeled results for power dissipation and current density of the MHP showed close agreement. An optimized simulated device exhibited low power dissipation of 9.25 mW and minimum mechanical deflection of 1.2 μm at the elevated temperature of 700°C [7]. In another paper, a design and analysis of an array of 100nm thin film MEMS based microheater on SOI wafer is presented. The microheater is constructed on a SOI wafer where temperature rise of 200°C is achieved with minimum power consumption of 20mW.Also there is minimum heat loss through the substrate. The temperature rise is concentrated in only the microheater region and there is excellent uniformity in the temperature distribution in both the microheaters. Maximum stress developed in oxide layer is 326 MPa which is within the range of their breaking stress [8]. 3.2 Simulation of gas sensing structure : In literature novel design of metal-oxide NO2 gas sensor integrated with micro heaters is presented in which thermal simulation of heat insulation between sensing diaphragm and substrate is carried which conclude that heat loss can be neglected when the gap between substrate and sensing membrane is larger than 15 µm. Also Electro-thermo analysis of the micro heater is carried and found when 2V applied voltage temp. is achieved at 215°C with uniform temp. distribution ,time response of the heater is less than 0.1s , maximum displacement due to thermal stress is less than 0.26 um. In stress analysis it was found Maximum Von Mises stress is 127 kPa [9]. 4. CONCLUSION In the study of simulation of gas sensors and microhotplate various parameters power, temperature distribution, stress, displacement with variation of substrate thickness , using different substrate materials ,different heater material ,heater layer thickness are optimized. 5. FUTURE SCOPE Keeping in the view of the objectives of miniaturization , portability, maximum sensitivity and compatible with existing silicon planer technology Further different heater geometries with different materials can be analysed. As gas detection sensitivity is function of temperature an attempt will be made to make temperature zones in the sensor arrays which could enable us to use the same sensors for different gases using COMSOL Multiphysics especially for toxic gases such as NH , CH & CO . REFERENCES 1. Xiao Liu , Sitian Cheng “A Survey on Gas Sensing Technology '' Sensors vol.12 , pp. 9635- 9665, 2012. 2. Tanusree Majhi, MS Thesis ''Elctrothermal design and fabrication of MEMS based microheater using a novel nickel alloy for methane gas sensor based on nanocrystalline ZnO thin film'' Jadavpur University,2006. 3. Chengxiang et al. “Metal Oxide Gas Sensors: Sensitivity and Influencing Factors'' Sensors, Vol 10, pp 2088-2106, 2010. 1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.6 2.8 3 300 400 500 600 700 800 900 1000 1100 1200 Voltage (V) Temperature(K) SiO2 Si3N4 SiO2+Si3N4 1 1.2 1.4 1.6 1.8 2 2.2 2.4 2.6 2.8 3 0 50 100 150 200 250 Voltage(V) PowerConsumption(mW) .3 micron .5 micron 1 micron
  • 4. ICRTEDC-2014 70 4. Chenxu Zhao ,Ph.D Thesis ''Automated synthesis of Mixed technology Mixed system with electronic system'' University of Southampton,2010. 5. Bijoy Kantha''Design and simulation of MEMS Microhotplate for gas sensor applications'' Jadavpur University ,2010. 6. Mahanth Prasad “FEM simulation of platinum-based microhotplate using different dielectric membranes for gas sensing applications’’ published in “sensors & transducers “in 2010. 7. John Ojur Dennis, Abdelaziz Yousif, Mohamad Naufal Mohamad “Design, simulation and modelling of a high temperature microhotplate for application in trace gas detection” published in “International Journal of Engineering & Technology'' 2010. 8. Avigyan Datta Gupta et al “Design and Analysis of MEMS Based Microheater Array on SOI Wafer for Low Power Gas Sensor Applications’’ published in “International Journal of Scientific & Engineering Research '' 2010. 9. Ling-Han Li et al. “Design and Simulation of an Integrated Metal Oxide Based Micro NO2 Gas Sensor ” presented in “International symposium on Micro-Nano Mechatronics and Human Science’’2006.