a review of gas sensors employed in electronic nose applications
DESCRIPTION
SensorsTRANSCRIPT
Research articleA review of gas sensorsemployed in electronicnose applications
K Arshak
E Moore
GM Lyons
J Harris and
S Clifford
The authors
K Arshak E Moore GM Lyons J Harris and S Clifford
are all based at the College of Informatics and Electronics
University of Limerick Limerick Ireland
Keywords
Sensors Gases
Abstract
This paper reviews the range of sensors used in electronic
nose (e-nose) systems to date It outlines the operating
principles and fabrication methods of each sensor type
as well as the applications in which the different sensors
have been utilised It also outlines the advantages and
disadvantages of each sensor for application in a
cost-effective low-power handheld e-nose system
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Introduction
The human nose has been used as an analytical
tool in many industries to measure the quality of
food drinks perfumes and also cosmetic and
chemical products It is commonly used for
assessing quality through odour and this is
carried out using sensory panels where a group
of people fills out questionnaires on the smells
associated with the substance being analysed
These sensory panels are extremely subjective as
human smell assessment is affected by many
factors Individual variations occur and may be
affected by physical and mental health as well as
fatigue (Pearce et al 2003) For this reason gas
chromatography and mass spectrometry have
been employed to aid human panels to assess
the quality of products through odour
evaluation and identification and also to obtain
more consistent results However these assistive
techniques are not portable they tend to be
expensive and their performance is relatively
slow (Nagle et al 1998)
The solution to the shortcomings of sensory
panels and the associated analytical techniques
is the electronic nose (e-nose) E-nose systems
utilize an array of sensors to give a fingerprint
response to a given odour and pattern
recognition software then performs odour
identification and discrimination The e-nose is
a cost-effective solution to the problems
associated with sensory panels and with
chromatographic and mass-spectrometric
techniques and can accommodate real time
performance in the field when implemented in
portable form
Principle of operation of e-nose systems
The e-nose attempts to emulate the mammalian
nose by using an array of sensors that can
simulate mammalian olfactory responses
to aromas The odour molecules are drawn
into the e-nose using sampling techniques
such as headspace sampling diffusion
methods bubblers or pre-concentrators
Sensor Review
Volume 24 middot Number 2 middot 2004 middot pp 181ndash198
q Emerald Group Publishing Limited middot ISSN 0260-2288
DOI 10110802602280410525977
This work was conducted as part of a collaborative
project between AMT Ireland University of
Limerick and University College Cork and is funded
by Enterprise Ireland under project ref no ATRP
2002427 (Intelli-SceNT)
181
(Pearce et al 2003) The odour sample is
drawn across the sensor array and induces a
reversible physical andor chemical change in
the sensing material which causes an associated
change in electrical properties such as
conductivity (Harsanyi 2000) Each ldquocellrdquo in
the array can behave like a receptor by
responding to different odours to varying
degrees (Shurmer and Gardner 1992) These
changes are transduced into electrical signals
which are preprocessed and conditioned before
identification by a pattern recognition system as
shown in Figure 1 The e-nose system is
designed so that the overall response pattern
from the array is unique for a given odour in a
family of odours to be considered by the system
E-nose sensor response to odorants
The response of e-nose sensors to odorants is
generally regarded as a first order time response
The first stage in odour analysis is to flush a
reference gas through the sensor to obtain a
baseline The sensor is exposed to the odorant
which causes changes in its output signal until
the sensor reaches steady-state The odorant is
finally flushed out of the sensor using the
reference gas and the sensor returns back to its
baseline as shown in Figure 2 The time during
which the sensor is exposed to the odorant is
referred to as the response time while the time
it takes the sensor to return to its baseline
resistance is called the recovery time
The next stage in analysing the odour is
sensor response manipulation with respect to
the baseline This process compensates for
noise drift and also for inherently large or
small signals (Pearce et al 2003) The three
most commonly used methods as defined by
Pearce et al (2003) are as follows
(1) Differential the baseline xs(0) is subtracted
from the sensor response xs(t) to remove
any noise or drift dA present The baseline
manipulated response ys(t) is determined
by
ysethtTHORN frac14 ethxsethtTHORN thorn dATHORN2 ethxseth0THORN thorn dATHORN
frac14 xsethtTHORN2 xseth0THORN eth1THORN
(2) Relative the sensor response is divided by
the baseline This process eliminates
multiplicative drift dM and a dimensionless
response ys(t) is obtained
ysethtTHORN frac14xsethtTHORNeth1thorn dMTHORN
xseth0THORNeth1thorn dMTHORNfrac14
xsethtTHORN
xseth0THORNeth2THORN
(3) Fractional the baseline is subtracted from
the response xs(t) and then divided by the
baseline xs(0) from the sensor response
which provides a dimensionless normalised
Figure 1 Comparison of the mammalian olfactory system and the e-nose system
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
182
response ys(t) that can compensate for
inherently large or small signals
ysethtTHORN frac14xsethtTHORN2 xseth0THORN
xseth0THORNeth3THORN
The choice of baseline manipulation depends
on the sensor type being used the sensor
applications and also the researchers preference
However certain manipulation techniques have
been shown to be more suitable to certain
sensor types and also variations in the
manipulation techniques can occur in the
literature which will be discussed later in this
paper
Sensitivity is the measure of the change in
output of a sensor for a change in the input This
is the standard definition given for the sensitivity
of a sensor in several texts on sensor related
topics (Fraden 1996 Gopel et al 1989
Johnson 1997) In the case of e-nose sensors
the sensitivity of the sensor (S ) to the odorant is
the change in the sensor output parameter ( y)
ie resistance for a change in the concentration
of the odorant (x) as shown in equation (4)
S frac14Dy
Dxeth4THORN
However in the literature several authors use
different values to measure sensitivity usually
calculated from baseline-manipulated data
Sensors employed in e-nose systems
Gas molecules interact with solid-state sensors
by absorption adsorption or chemical reactions
with thin or thick films of the sensor material
The sensor device detects the physical andor
chemical changes incurred by these processes
and these changes are measured as an electrical
signal The most common types of changes
utilised in e-nose sensor systems are shown in
Table I along with the classes of sensor devices
used to detect these changes
Some aspects of these classes of sensors
along with several examples from each class are
explored in the following sections of this review
Conductivity sensors
Conducting polymer composites intrinsically
conducting polymers and metal oxides are three
of the most commonly utilised classes of sensing
materials in conductivity sensors These
materials work on the principle that a change in
some property of the material resulting from
interaction with a gasodour leads to a change in
resistance in the sensor The mechanisms that
lead to these resistance changes are different
for each material type however the structure
and layout of conductivity sensors prepared
using these materials are essentially the same
A schematic of a typical conductivity sensor
design is shown in Figure 3
The sensing material is deposited over
interdigitated or two parallel electrodes which
form the electrical connections through which
the relative resistance change is measured
The heater is required when metal oxides are
used as the sensing material because very high
temperatures are required for effective
operation of metal oxide sensors
Conducting polymer composite sensors
Conducting polymer composites consist of
conducting particles such as polypyrrole and
carbon black interspersed in an insulating
polymer matrix (Albert and Lewis 2000)
Figure 2 E-nose sensor response to an odorant
Table I Physical changes in the sensor active film and the
sensor devices used to transduce them into electrical signals
Physical changes Sensor devices
Conductivity Conductivity sensors
Mass Piezoelectric sensors
Optical Optical sensors
Work function MOSFET sensors
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
183
On exposure to gases these materials change
resistance and this change is due to percolation
effects or more complex mechanisms in the case
of polypyrrole filled composites
When the polymer composite sensor is
exposed to a vapour some of the vapour
permeates into the polymer and causes the
polymer film to expand The vapour-induced
expansion of the polymer composite causes an
increase in the electrical resistance of the
polymer composite because the polymer
expansion reduces the number of conducting
pathways for charge carriers (Munoz et al
1999) This increase in resistance is consistent
with percolation theory Polypyrrole-based
composites have a more complex transduction
mechanism because the odour molecules can
cause expansion of both the insulating polymer
and the polypyrrole particles Changes in the
intrinsic conductivity of the polypyrrole
particles can also occur if the odour interacts
chemically with the conducting polymer
backbone Therefore resistance changes in the
polypyrrole-based composites are more difficult
to predict (Albert and Lewis 2000)
Carbon black based composites were
prepared by suspending the carbon black in a
solution of the insulating polymer in a suitable
solvent The overall composition of this solution
is usually 80 per cent insulating polymer-
20 per cent carbon black by weight Different
techniques have been used to apply the active
material onto the substrate which are shown in
Table II
The transducer device is usually a flat
substrate with either two parallel electrodes or
interdigitated electrodes deposited onto the
substrate surface as shown in Figure 3
However both bulk and surface
micromachining have also been used to produce
wells on silicon substrates using patterned
silicon nitrideoxide as insulation and gold
electrodes as the metal contacts The polymer is
dropped into the well using a syringe as shown
in Figure 4 (Zee and Judy 2001)
Examples of the types of substrates and
electrodes used are given in Table III along with
the electrode dimensions given in the literature
Polypyrrole-based composites are usually
prepared by chemically polymerizing pyrrole
using phosphomolybdic acid in a solution
containing the insulating polymer A thin film
coating (40-100 nm thick) is then applied across
interdigitated electrodes (typical electrode gaps
were 15mm) using dip coating (Freund and
Lewis 1995)
The fractional baseline manipulation
response is the most common method used to
record the sensor response from conducting gas
sensors (Pearce et al 2003) This fractional
baseline manipulation is referred to as the
maximum relative differential resistance
change DRRb DR is the maximum change in
the resistance of the sensor during exposure to
the odorant and Rb is the baseline resistance
before exposure
Response times may vary from seconds to
minutes as shown in Table IV and in some
cases milliseconds (Munoz et al 1999)
However typically a set of exposure cycles
is quoted for each analyte ie initial reference
gas analyte and final reference gas exposure
times The response time depends on the rate
of diffusion of the permeant into the polymer
The diffusion rate mainly depends on the nature
of the polymer permeant and the crosslinking
the concentration of the permeant and thickness
of the film and on the effects of fillers
plasticisers and temperature (George and
Thomas 2001) General response times for
conducting polymer composites are given in
Table IV
The transport properties depend on the
fractional free volume (FFV) in the polymer and
on the mobility of the segments of the polymer
chains The segmental mobility of the polymer
chains depends on the extent of unsaturation
Therefore segmental mobility is significantly
Figure 3 Typical structure of a conductivity sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
184
reduced with increased numbers of double and
triple bonds on the carbon-carbon backbone
The presence of crystalline domains can have
two different effects on the permeability of a
polymer Crystallites are generally impermeable
to vapours at room temperature and will reduce
the diffusion coefficient However crystallites
act as large crosslinking regions in terms of the
chains entering and leaving the areas around the
crystallite in which diffusion occurs (Comyn
1985) Increased defect formation and a
reduction in interlamellar links predominate
and overshadow the effect of geometric
impedance to such an extent that diffusivity
increases despite increasing crystallinity (Vieth
1991) For example in PE-grafted carbon black
chemiresistors heat treatment of the composite
improved the crystallinity of the matrix PE and
resulted in a five-fold increase in the response of
the sensor to cyclohexane vapour compared to
the untreated sensor (Chen et al 2002)
The size and shape of the penetrating
molecule affects the rate of uptake of the vapour
by the polymer where increased size of the
molecule decreases the diffusion coefficient
Flattened or elongated molecules diffuse faster
than spherical-shaped molecules (George and
Thomas 2001)
The partial pressure ie the concentration
of the penetrant gas at the gas polymer interface
affects the response of the sensor The response
is inversely related to the vapour pressure of the
analyte at the surface Low vapour pressure
compounds can be detected in the low ppb
range while high vapour pressure compounds
need to be in the high ppm range to be detected
This is due to the polymergas partition
coefficient where low vapour pressure gas
molecules have a higher tendency to inhabit the
polymer and thus can be detected at much lower
concentrations (Munoz et al 1999)
The equilibrium partition coefficient is
essentially the solubility coefficient of the
vapour in the polymer (Vieth 1991) Sensors
with constant thickness but with different
surface areas have the same response when
exposed to analytes with moderate partition
coefficients However analytes with higher
partition coefficients have higher affinity to
sensors with smaller area In this case reducing
the sensor area increases the sensitivity of the
sensor towards particular analytes Therefore
the relationship between the partition
co-efficient and the sensor geometry is an
important factor in optimising polymer
composite sensor response (Briglin et al 2002)
Table II Application techniques used to deposit carbon black based composites
Reference Polymer Coating thickness Coating application technique
Matthews et al (2002) Poly(alkylacrylate) Thin film 086mm Spray coating
Severin et al (1998) Poly(co-vinyl-acetate) Thin film 1mm Spin coating
Severin et al (2000) Poly(vinyl butyral) Thin film NA Dip coating
Figure 4 Bulk micromachined well as used by Zee and Judy (2001)
Table III Electrodes and substrates used in conducting polymer composite sensors
Substrate
Electrode
material
Electrode
dimensions
(mm)
Electrode gap
(mm)
Electrode
thickness
(nm) Reference
Glass microscope slides Gold NA 5 50-100 Lonergan et al (1996)
Glass microscope slides Gold 10 pound 10 5 50 Doleman et al (1998a)
Glass microscope slides Gold Chromium 20 pound 10 5 30 20 Doleman et al (1998a b)
Micromachined silicon wafer Gold 01 in width 05 NA Zee and Judy (2001)
Glass microscope slide Gold Chromium 18 in length 04 50 15-30 Briglin et al (2002)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
185
Generally composite polymers have operating
resistances of approximately 1 to 1000 kV with
sensitivities of up to 100 per cent DRRb per mg
l gas depending on the filler type particle
loading and vapour transport properties
(Partridge et al 2000) Sensitivity to
hydrophobic analytes for conducting polymer
composites were found to be one to two orders
of magnitude higher than those recorded for
intrinsically conducting polymers (Partridge
et al 2000) The polymer composites show
linear responses to concentration for various
analytes and also good repeatability after several
exposures (Severin 2000 Zee and Judy 2001)
From the above discussion it can be seen that
for high sensitivity fast response and short
recovery times it is essential that the sensor
geometry and all the associated properties of the
polymer sensing material be highly optimised
Conducting polymer composites offer many
advantages over other materials when utilised as
gas sensors High discrimination in array
sensors can be easily achieved using these
materials due to the wide range of polymeric
materials available on the market This is due to
the fact that different polymers give different
levels of response to a given odour Conducting
polymer composites are also relatively
inexpensive and easy to prepare Sensors
prepared from these materials can operate in
conditions of high relative humidity and also
show highly linear responses for a wide range of
gases (Munoz et al 1999) No heater is
required as sensors prepared from these
materials operate at room temperature This is
an important advantage with portable battery
powered e-nose systems as a heater would
significantly increase the power consumption of
the system The signal conditioning circuitry
required for these sensors is relatively simple as
only a resistance change is being measured
The main drawbacks of using conducting
polymer composites as e-nose sensors are aging
which leads to sensor drift and also these
materials are unsuitable for detecting certain
gases for example carbon-polymer composites
are not sensitive to trimethylamine (TMA) for
fish odour applications
Intrinsically conducting polymers
Intrinsically conducting polymers (ICP) have
linear backbones composed of unsaturated
monomers ie alternating double and single
bonds along the backbone that can be doped as
semiconductors or conductors (Heeger 2001)
Yasufuku (2001) describes them as p electron
conjugated polymers where the p symbol relates
to the unsaturated structure of the monomer
containing an unpaired carbon electron
These conducting polymers can be n-doped or
p-doped depending on the doping materials
used Conducting polymers such as polypyrrole
polythiophene and polyaniline as shown in
Figure 5 are typically used for e-nose sensing
The doping of these materials generates charge
carriers and also alters their band structure
which both induce increasedmobility of holes or
electrons in the polymer depending on the type
of doping used (Albert and Lewis 2000
Dickinson et al 1998)
The principle of operation for ICP e-nose
sensors is that the odorant is absorbed into the
polymer and alters the conductivity of the
polymer (Albert and Lewis 2000 Dickinson
et al 1998) Three types of conductivity are
affected in intrinsically conducting polymers
(1) The intrachain conductivity in which the
conductivity along the backbone is altered
(2) The intermolecular conductivity which is due
to electron hopping to different chains
because of analyte sorption (Charlesworth
et al 1997) and
(3) The ionic conductivity which is affected by
proton tunneling induced by hydrogen
bond interaction at the backbone and also
by ion migration through the polymer
(Albert and Lewis 2000) The physical
structure of the polymer also has a major
influence on the conductivity (Yasufuku
2001) Albert and Lewis (2000) described
how the conductivity of doped polyaniline
was greatly increased on interaction with
ethanol caused by the hydrogen bonds
Table IV General response times for conducting polymer
composites
Response time (s) Reference
lt2-4 Lonergan et al (1996)
60 Partridge (2000)
180-240 Corcoran (1993b)
20-200 Doleman et al (1998)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
186
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
hara
cter
istic
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com
mer
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e-no
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Man
ufacturer
Sensor
type
No
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Pattern
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
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Sensor
type
No
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Applications
Pattern
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
(Pearce et al 2003) The odour sample is
drawn across the sensor array and induces a
reversible physical andor chemical change in
the sensing material which causes an associated
change in electrical properties such as
conductivity (Harsanyi 2000) Each ldquocellrdquo in
the array can behave like a receptor by
responding to different odours to varying
degrees (Shurmer and Gardner 1992) These
changes are transduced into electrical signals
which are preprocessed and conditioned before
identification by a pattern recognition system as
shown in Figure 1 The e-nose system is
designed so that the overall response pattern
from the array is unique for a given odour in a
family of odours to be considered by the system
E-nose sensor response to odorants
The response of e-nose sensors to odorants is
generally regarded as a first order time response
The first stage in odour analysis is to flush a
reference gas through the sensor to obtain a
baseline The sensor is exposed to the odorant
which causes changes in its output signal until
the sensor reaches steady-state The odorant is
finally flushed out of the sensor using the
reference gas and the sensor returns back to its
baseline as shown in Figure 2 The time during
which the sensor is exposed to the odorant is
referred to as the response time while the time
it takes the sensor to return to its baseline
resistance is called the recovery time
The next stage in analysing the odour is
sensor response manipulation with respect to
the baseline This process compensates for
noise drift and also for inherently large or
small signals (Pearce et al 2003) The three
most commonly used methods as defined by
Pearce et al (2003) are as follows
(1) Differential the baseline xs(0) is subtracted
from the sensor response xs(t) to remove
any noise or drift dA present The baseline
manipulated response ys(t) is determined
by
ysethtTHORN frac14 ethxsethtTHORN thorn dATHORN2 ethxseth0THORN thorn dATHORN
frac14 xsethtTHORN2 xseth0THORN eth1THORN
(2) Relative the sensor response is divided by
the baseline This process eliminates
multiplicative drift dM and a dimensionless
response ys(t) is obtained
ysethtTHORN frac14xsethtTHORNeth1thorn dMTHORN
xseth0THORNeth1thorn dMTHORNfrac14
xsethtTHORN
xseth0THORNeth2THORN
(3) Fractional the baseline is subtracted from
the response xs(t) and then divided by the
baseline xs(0) from the sensor response
which provides a dimensionless normalised
Figure 1 Comparison of the mammalian olfactory system and the e-nose system
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
182
response ys(t) that can compensate for
inherently large or small signals
ysethtTHORN frac14xsethtTHORN2 xseth0THORN
xseth0THORNeth3THORN
The choice of baseline manipulation depends
on the sensor type being used the sensor
applications and also the researchers preference
However certain manipulation techniques have
been shown to be more suitable to certain
sensor types and also variations in the
manipulation techniques can occur in the
literature which will be discussed later in this
paper
Sensitivity is the measure of the change in
output of a sensor for a change in the input This
is the standard definition given for the sensitivity
of a sensor in several texts on sensor related
topics (Fraden 1996 Gopel et al 1989
Johnson 1997) In the case of e-nose sensors
the sensitivity of the sensor (S ) to the odorant is
the change in the sensor output parameter ( y)
ie resistance for a change in the concentration
of the odorant (x) as shown in equation (4)
S frac14Dy
Dxeth4THORN
However in the literature several authors use
different values to measure sensitivity usually
calculated from baseline-manipulated data
Sensors employed in e-nose systems
Gas molecules interact with solid-state sensors
by absorption adsorption or chemical reactions
with thin or thick films of the sensor material
The sensor device detects the physical andor
chemical changes incurred by these processes
and these changes are measured as an electrical
signal The most common types of changes
utilised in e-nose sensor systems are shown in
Table I along with the classes of sensor devices
used to detect these changes
Some aspects of these classes of sensors
along with several examples from each class are
explored in the following sections of this review
Conductivity sensors
Conducting polymer composites intrinsically
conducting polymers and metal oxides are three
of the most commonly utilised classes of sensing
materials in conductivity sensors These
materials work on the principle that a change in
some property of the material resulting from
interaction with a gasodour leads to a change in
resistance in the sensor The mechanisms that
lead to these resistance changes are different
for each material type however the structure
and layout of conductivity sensors prepared
using these materials are essentially the same
A schematic of a typical conductivity sensor
design is shown in Figure 3
The sensing material is deposited over
interdigitated or two parallel electrodes which
form the electrical connections through which
the relative resistance change is measured
The heater is required when metal oxides are
used as the sensing material because very high
temperatures are required for effective
operation of metal oxide sensors
Conducting polymer composite sensors
Conducting polymer composites consist of
conducting particles such as polypyrrole and
carbon black interspersed in an insulating
polymer matrix (Albert and Lewis 2000)
Figure 2 E-nose sensor response to an odorant
Table I Physical changes in the sensor active film and the
sensor devices used to transduce them into electrical signals
Physical changes Sensor devices
Conductivity Conductivity sensors
Mass Piezoelectric sensors
Optical Optical sensors
Work function MOSFET sensors
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
183
On exposure to gases these materials change
resistance and this change is due to percolation
effects or more complex mechanisms in the case
of polypyrrole filled composites
When the polymer composite sensor is
exposed to a vapour some of the vapour
permeates into the polymer and causes the
polymer film to expand The vapour-induced
expansion of the polymer composite causes an
increase in the electrical resistance of the
polymer composite because the polymer
expansion reduces the number of conducting
pathways for charge carriers (Munoz et al
1999) This increase in resistance is consistent
with percolation theory Polypyrrole-based
composites have a more complex transduction
mechanism because the odour molecules can
cause expansion of both the insulating polymer
and the polypyrrole particles Changes in the
intrinsic conductivity of the polypyrrole
particles can also occur if the odour interacts
chemically with the conducting polymer
backbone Therefore resistance changes in the
polypyrrole-based composites are more difficult
to predict (Albert and Lewis 2000)
Carbon black based composites were
prepared by suspending the carbon black in a
solution of the insulating polymer in a suitable
solvent The overall composition of this solution
is usually 80 per cent insulating polymer-
20 per cent carbon black by weight Different
techniques have been used to apply the active
material onto the substrate which are shown in
Table II
The transducer device is usually a flat
substrate with either two parallel electrodes or
interdigitated electrodes deposited onto the
substrate surface as shown in Figure 3
However both bulk and surface
micromachining have also been used to produce
wells on silicon substrates using patterned
silicon nitrideoxide as insulation and gold
electrodes as the metal contacts The polymer is
dropped into the well using a syringe as shown
in Figure 4 (Zee and Judy 2001)
Examples of the types of substrates and
electrodes used are given in Table III along with
the electrode dimensions given in the literature
Polypyrrole-based composites are usually
prepared by chemically polymerizing pyrrole
using phosphomolybdic acid in a solution
containing the insulating polymer A thin film
coating (40-100 nm thick) is then applied across
interdigitated electrodes (typical electrode gaps
were 15mm) using dip coating (Freund and
Lewis 1995)
The fractional baseline manipulation
response is the most common method used to
record the sensor response from conducting gas
sensors (Pearce et al 2003) This fractional
baseline manipulation is referred to as the
maximum relative differential resistance
change DRRb DR is the maximum change in
the resistance of the sensor during exposure to
the odorant and Rb is the baseline resistance
before exposure
Response times may vary from seconds to
minutes as shown in Table IV and in some
cases milliseconds (Munoz et al 1999)
However typically a set of exposure cycles
is quoted for each analyte ie initial reference
gas analyte and final reference gas exposure
times The response time depends on the rate
of diffusion of the permeant into the polymer
The diffusion rate mainly depends on the nature
of the polymer permeant and the crosslinking
the concentration of the permeant and thickness
of the film and on the effects of fillers
plasticisers and temperature (George and
Thomas 2001) General response times for
conducting polymer composites are given in
Table IV
The transport properties depend on the
fractional free volume (FFV) in the polymer and
on the mobility of the segments of the polymer
chains The segmental mobility of the polymer
chains depends on the extent of unsaturation
Therefore segmental mobility is significantly
Figure 3 Typical structure of a conductivity sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
184
reduced with increased numbers of double and
triple bonds on the carbon-carbon backbone
The presence of crystalline domains can have
two different effects on the permeability of a
polymer Crystallites are generally impermeable
to vapours at room temperature and will reduce
the diffusion coefficient However crystallites
act as large crosslinking regions in terms of the
chains entering and leaving the areas around the
crystallite in which diffusion occurs (Comyn
1985) Increased defect formation and a
reduction in interlamellar links predominate
and overshadow the effect of geometric
impedance to such an extent that diffusivity
increases despite increasing crystallinity (Vieth
1991) For example in PE-grafted carbon black
chemiresistors heat treatment of the composite
improved the crystallinity of the matrix PE and
resulted in a five-fold increase in the response of
the sensor to cyclohexane vapour compared to
the untreated sensor (Chen et al 2002)
The size and shape of the penetrating
molecule affects the rate of uptake of the vapour
by the polymer where increased size of the
molecule decreases the diffusion coefficient
Flattened or elongated molecules diffuse faster
than spherical-shaped molecules (George and
Thomas 2001)
The partial pressure ie the concentration
of the penetrant gas at the gas polymer interface
affects the response of the sensor The response
is inversely related to the vapour pressure of the
analyte at the surface Low vapour pressure
compounds can be detected in the low ppb
range while high vapour pressure compounds
need to be in the high ppm range to be detected
This is due to the polymergas partition
coefficient where low vapour pressure gas
molecules have a higher tendency to inhabit the
polymer and thus can be detected at much lower
concentrations (Munoz et al 1999)
The equilibrium partition coefficient is
essentially the solubility coefficient of the
vapour in the polymer (Vieth 1991) Sensors
with constant thickness but with different
surface areas have the same response when
exposed to analytes with moderate partition
coefficients However analytes with higher
partition coefficients have higher affinity to
sensors with smaller area In this case reducing
the sensor area increases the sensitivity of the
sensor towards particular analytes Therefore
the relationship between the partition
co-efficient and the sensor geometry is an
important factor in optimising polymer
composite sensor response (Briglin et al 2002)
Table II Application techniques used to deposit carbon black based composites
Reference Polymer Coating thickness Coating application technique
Matthews et al (2002) Poly(alkylacrylate) Thin film 086mm Spray coating
Severin et al (1998) Poly(co-vinyl-acetate) Thin film 1mm Spin coating
Severin et al (2000) Poly(vinyl butyral) Thin film NA Dip coating
Figure 4 Bulk micromachined well as used by Zee and Judy (2001)
Table III Electrodes and substrates used in conducting polymer composite sensors
Substrate
Electrode
material
Electrode
dimensions
(mm)
Electrode gap
(mm)
Electrode
thickness
(nm) Reference
Glass microscope slides Gold NA 5 50-100 Lonergan et al (1996)
Glass microscope slides Gold 10 pound 10 5 50 Doleman et al (1998a)
Glass microscope slides Gold Chromium 20 pound 10 5 30 20 Doleman et al (1998a b)
Micromachined silicon wafer Gold 01 in width 05 NA Zee and Judy (2001)
Glass microscope slide Gold Chromium 18 in length 04 50 15-30 Briglin et al (2002)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
185
Generally composite polymers have operating
resistances of approximately 1 to 1000 kV with
sensitivities of up to 100 per cent DRRb per mg
l gas depending on the filler type particle
loading and vapour transport properties
(Partridge et al 2000) Sensitivity to
hydrophobic analytes for conducting polymer
composites were found to be one to two orders
of magnitude higher than those recorded for
intrinsically conducting polymers (Partridge
et al 2000) The polymer composites show
linear responses to concentration for various
analytes and also good repeatability after several
exposures (Severin 2000 Zee and Judy 2001)
From the above discussion it can be seen that
for high sensitivity fast response and short
recovery times it is essential that the sensor
geometry and all the associated properties of the
polymer sensing material be highly optimised
Conducting polymer composites offer many
advantages over other materials when utilised as
gas sensors High discrimination in array
sensors can be easily achieved using these
materials due to the wide range of polymeric
materials available on the market This is due to
the fact that different polymers give different
levels of response to a given odour Conducting
polymer composites are also relatively
inexpensive and easy to prepare Sensors
prepared from these materials can operate in
conditions of high relative humidity and also
show highly linear responses for a wide range of
gases (Munoz et al 1999) No heater is
required as sensors prepared from these
materials operate at room temperature This is
an important advantage with portable battery
powered e-nose systems as a heater would
significantly increase the power consumption of
the system The signal conditioning circuitry
required for these sensors is relatively simple as
only a resistance change is being measured
The main drawbacks of using conducting
polymer composites as e-nose sensors are aging
which leads to sensor drift and also these
materials are unsuitable for detecting certain
gases for example carbon-polymer composites
are not sensitive to trimethylamine (TMA) for
fish odour applications
Intrinsically conducting polymers
Intrinsically conducting polymers (ICP) have
linear backbones composed of unsaturated
monomers ie alternating double and single
bonds along the backbone that can be doped as
semiconductors or conductors (Heeger 2001)
Yasufuku (2001) describes them as p electron
conjugated polymers where the p symbol relates
to the unsaturated structure of the monomer
containing an unpaired carbon electron
These conducting polymers can be n-doped or
p-doped depending on the doping materials
used Conducting polymers such as polypyrrole
polythiophene and polyaniline as shown in
Figure 5 are typically used for e-nose sensing
The doping of these materials generates charge
carriers and also alters their band structure
which both induce increasedmobility of holes or
electrons in the polymer depending on the type
of doping used (Albert and Lewis 2000
Dickinson et al 1998)
The principle of operation for ICP e-nose
sensors is that the odorant is absorbed into the
polymer and alters the conductivity of the
polymer (Albert and Lewis 2000 Dickinson
et al 1998) Three types of conductivity are
affected in intrinsically conducting polymers
(1) The intrachain conductivity in which the
conductivity along the backbone is altered
(2) The intermolecular conductivity which is due
to electron hopping to different chains
because of analyte sorption (Charlesworth
et al 1997) and
(3) The ionic conductivity which is affected by
proton tunneling induced by hydrogen
bond interaction at the backbone and also
by ion migration through the polymer
(Albert and Lewis 2000) The physical
structure of the polymer also has a major
influence on the conductivity (Yasufuku
2001) Albert and Lewis (2000) described
how the conductivity of doped polyaniline
was greatly increased on interaction with
ethanol caused by the hydrogen bonds
Table IV General response times for conducting polymer
composites
Response time (s) Reference
lt2-4 Lonergan et al (1996)
60 Partridge (2000)
180-240 Corcoran (1993b)
20-200 Doleman et al (1998)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
186
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
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we
stca
lcom
Forschungszen
trum
Karlsruhe
MO
SSA
W40
8
Envi
ronm
enta
lpr
otec
tion
indu
stria
lpr
oces
sco
ntro
lai
r
mon
itorin
gin
text
ilem
ills
fire
alar
ms
Qua
lity
cont
rol
info
od
prod
uctio
nA
utom
otiv
eap
plic
atio
ns
PCA
ww
wf
zkd
eFZ
K2
engl
ish
HKR-Sen
sorsystemeGmbH
QC
M6
Food
and
beve
rage
sco
smet
ics
and
perf
umes
or
gani
c
mat
eria
ls
phar
mac
eutic
alin
dust
ry
AN
N
CA
DFA
PC
A
Des
ktop
ww
wh
kr-s
enso
rde
Tech
nica
lU
nive
rsity
ofM
unic
h
Ger
man
y
Illumina
FOndash
Life
scie
nces
fo
odpr
oces
sing
ag
ricul
ture
ch
emic
alde
tect
ion
AN
Nw
ww
illu
min
aco
mTu
fts
Uni
vers
ity
USA
(Con
tinue
d)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
SQ
CM
16-4
0Fo
odan
dbe
vera
gepr
oces
sing
per
fum
eoi
lsa
gric
ultu
ralo
dour
s
and
chem
ical
anal
ysis
pr
oces
sco
ntro
l
AN
N
PCA
Des
ktop
ww
wle
nnar
tz-e
lect
roni
cde
PDF_
docu
men
ts
Uni
vers
ityof
Tubi
ngen
Marconitechnologies
MastiffElectronic
System
sLtd
CP
16Sn
iffs
palm
sfo
rpe
rson
alid
entifi
catio
nw
ww
mas
tiffc
ouk
MicrosensorSystem
sSA
W2
Che
mic
alag
ent
dete
ctio
nch
emic
alw
arfa
re(C
W)
agen
tsan
d
toxi
cin
dust
rial
chem
ical
s(T
ICs)
anal
ysis
Palm
top
ww
wm
icro
sens
orsy
stem
sco
mp
df
hazm
atca
d
OligoSe
nse
CO
ndashA
utom
otiv
eap
plic
atio
nsf
ood
eval
uatio
npa
ckag
ing
eval
uatio
nht
tp
ww
wo
ligos
ense
be
RST
Rostock
Rau
m-fah
rtund
UmweltschatzGmbH
MO
SQ
CM
SAW
6-10
Early
reco
gniti
onof
fires
w
arni
ngin
the
even
tof
esca
peof
haza
rdou
ssu
bsta
nces
le
akde
tect
ion
wor
kpla
cem
onito
ring
AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
response ys(t) that can compensate for
inherently large or small signals
ysethtTHORN frac14xsethtTHORN2 xseth0THORN
xseth0THORNeth3THORN
The choice of baseline manipulation depends
on the sensor type being used the sensor
applications and also the researchers preference
However certain manipulation techniques have
been shown to be more suitable to certain
sensor types and also variations in the
manipulation techniques can occur in the
literature which will be discussed later in this
paper
Sensitivity is the measure of the change in
output of a sensor for a change in the input This
is the standard definition given for the sensitivity
of a sensor in several texts on sensor related
topics (Fraden 1996 Gopel et al 1989
Johnson 1997) In the case of e-nose sensors
the sensitivity of the sensor (S ) to the odorant is
the change in the sensor output parameter ( y)
ie resistance for a change in the concentration
of the odorant (x) as shown in equation (4)
S frac14Dy
Dxeth4THORN
However in the literature several authors use
different values to measure sensitivity usually
calculated from baseline-manipulated data
Sensors employed in e-nose systems
Gas molecules interact with solid-state sensors
by absorption adsorption or chemical reactions
with thin or thick films of the sensor material
The sensor device detects the physical andor
chemical changes incurred by these processes
and these changes are measured as an electrical
signal The most common types of changes
utilised in e-nose sensor systems are shown in
Table I along with the classes of sensor devices
used to detect these changes
Some aspects of these classes of sensors
along with several examples from each class are
explored in the following sections of this review
Conductivity sensors
Conducting polymer composites intrinsically
conducting polymers and metal oxides are three
of the most commonly utilised classes of sensing
materials in conductivity sensors These
materials work on the principle that a change in
some property of the material resulting from
interaction with a gasodour leads to a change in
resistance in the sensor The mechanisms that
lead to these resistance changes are different
for each material type however the structure
and layout of conductivity sensors prepared
using these materials are essentially the same
A schematic of a typical conductivity sensor
design is shown in Figure 3
The sensing material is deposited over
interdigitated or two parallel electrodes which
form the electrical connections through which
the relative resistance change is measured
The heater is required when metal oxides are
used as the sensing material because very high
temperatures are required for effective
operation of metal oxide sensors
Conducting polymer composite sensors
Conducting polymer composites consist of
conducting particles such as polypyrrole and
carbon black interspersed in an insulating
polymer matrix (Albert and Lewis 2000)
Figure 2 E-nose sensor response to an odorant
Table I Physical changes in the sensor active film and the
sensor devices used to transduce them into electrical signals
Physical changes Sensor devices
Conductivity Conductivity sensors
Mass Piezoelectric sensors
Optical Optical sensors
Work function MOSFET sensors
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
183
On exposure to gases these materials change
resistance and this change is due to percolation
effects or more complex mechanisms in the case
of polypyrrole filled composites
When the polymer composite sensor is
exposed to a vapour some of the vapour
permeates into the polymer and causes the
polymer film to expand The vapour-induced
expansion of the polymer composite causes an
increase in the electrical resistance of the
polymer composite because the polymer
expansion reduces the number of conducting
pathways for charge carriers (Munoz et al
1999) This increase in resistance is consistent
with percolation theory Polypyrrole-based
composites have a more complex transduction
mechanism because the odour molecules can
cause expansion of both the insulating polymer
and the polypyrrole particles Changes in the
intrinsic conductivity of the polypyrrole
particles can also occur if the odour interacts
chemically with the conducting polymer
backbone Therefore resistance changes in the
polypyrrole-based composites are more difficult
to predict (Albert and Lewis 2000)
Carbon black based composites were
prepared by suspending the carbon black in a
solution of the insulating polymer in a suitable
solvent The overall composition of this solution
is usually 80 per cent insulating polymer-
20 per cent carbon black by weight Different
techniques have been used to apply the active
material onto the substrate which are shown in
Table II
The transducer device is usually a flat
substrate with either two parallel electrodes or
interdigitated electrodes deposited onto the
substrate surface as shown in Figure 3
However both bulk and surface
micromachining have also been used to produce
wells on silicon substrates using patterned
silicon nitrideoxide as insulation and gold
electrodes as the metal contacts The polymer is
dropped into the well using a syringe as shown
in Figure 4 (Zee and Judy 2001)
Examples of the types of substrates and
electrodes used are given in Table III along with
the electrode dimensions given in the literature
Polypyrrole-based composites are usually
prepared by chemically polymerizing pyrrole
using phosphomolybdic acid in a solution
containing the insulating polymer A thin film
coating (40-100 nm thick) is then applied across
interdigitated electrodes (typical electrode gaps
were 15mm) using dip coating (Freund and
Lewis 1995)
The fractional baseline manipulation
response is the most common method used to
record the sensor response from conducting gas
sensors (Pearce et al 2003) This fractional
baseline manipulation is referred to as the
maximum relative differential resistance
change DRRb DR is the maximum change in
the resistance of the sensor during exposure to
the odorant and Rb is the baseline resistance
before exposure
Response times may vary from seconds to
minutes as shown in Table IV and in some
cases milliseconds (Munoz et al 1999)
However typically a set of exposure cycles
is quoted for each analyte ie initial reference
gas analyte and final reference gas exposure
times The response time depends on the rate
of diffusion of the permeant into the polymer
The diffusion rate mainly depends on the nature
of the polymer permeant and the crosslinking
the concentration of the permeant and thickness
of the film and on the effects of fillers
plasticisers and temperature (George and
Thomas 2001) General response times for
conducting polymer composites are given in
Table IV
The transport properties depend on the
fractional free volume (FFV) in the polymer and
on the mobility of the segments of the polymer
chains The segmental mobility of the polymer
chains depends on the extent of unsaturation
Therefore segmental mobility is significantly
Figure 3 Typical structure of a conductivity sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
184
reduced with increased numbers of double and
triple bonds on the carbon-carbon backbone
The presence of crystalline domains can have
two different effects on the permeability of a
polymer Crystallites are generally impermeable
to vapours at room temperature and will reduce
the diffusion coefficient However crystallites
act as large crosslinking regions in terms of the
chains entering and leaving the areas around the
crystallite in which diffusion occurs (Comyn
1985) Increased defect formation and a
reduction in interlamellar links predominate
and overshadow the effect of geometric
impedance to such an extent that diffusivity
increases despite increasing crystallinity (Vieth
1991) For example in PE-grafted carbon black
chemiresistors heat treatment of the composite
improved the crystallinity of the matrix PE and
resulted in a five-fold increase in the response of
the sensor to cyclohexane vapour compared to
the untreated sensor (Chen et al 2002)
The size and shape of the penetrating
molecule affects the rate of uptake of the vapour
by the polymer where increased size of the
molecule decreases the diffusion coefficient
Flattened or elongated molecules diffuse faster
than spherical-shaped molecules (George and
Thomas 2001)
The partial pressure ie the concentration
of the penetrant gas at the gas polymer interface
affects the response of the sensor The response
is inversely related to the vapour pressure of the
analyte at the surface Low vapour pressure
compounds can be detected in the low ppb
range while high vapour pressure compounds
need to be in the high ppm range to be detected
This is due to the polymergas partition
coefficient where low vapour pressure gas
molecules have a higher tendency to inhabit the
polymer and thus can be detected at much lower
concentrations (Munoz et al 1999)
The equilibrium partition coefficient is
essentially the solubility coefficient of the
vapour in the polymer (Vieth 1991) Sensors
with constant thickness but with different
surface areas have the same response when
exposed to analytes with moderate partition
coefficients However analytes with higher
partition coefficients have higher affinity to
sensors with smaller area In this case reducing
the sensor area increases the sensitivity of the
sensor towards particular analytes Therefore
the relationship between the partition
co-efficient and the sensor geometry is an
important factor in optimising polymer
composite sensor response (Briglin et al 2002)
Table II Application techniques used to deposit carbon black based composites
Reference Polymer Coating thickness Coating application technique
Matthews et al (2002) Poly(alkylacrylate) Thin film 086mm Spray coating
Severin et al (1998) Poly(co-vinyl-acetate) Thin film 1mm Spin coating
Severin et al (2000) Poly(vinyl butyral) Thin film NA Dip coating
Figure 4 Bulk micromachined well as used by Zee and Judy (2001)
Table III Electrodes and substrates used in conducting polymer composite sensors
Substrate
Electrode
material
Electrode
dimensions
(mm)
Electrode gap
(mm)
Electrode
thickness
(nm) Reference
Glass microscope slides Gold NA 5 50-100 Lonergan et al (1996)
Glass microscope slides Gold 10 pound 10 5 50 Doleman et al (1998a)
Glass microscope slides Gold Chromium 20 pound 10 5 30 20 Doleman et al (1998a b)
Micromachined silicon wafer Gold 01 in width 05 NA Zee and Judy (2001)
Glass microscope slide Gold Chromium 18 in length 04 50 15-30 Briglin et al (2002)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
185
Generally composite polymers have operating
resistances of approximately 1 to 1000 kV with
sensitivities of up to 100 per cent DRRb per mg
l gas depending on the filler type particle
loading and vapour transport properties
(Partridge et al 2000) Sensitivity to
hydrophobic analytes for conducting polymer
composites were found to be one to two orders
of magnitude higher than those recorded for
intrinsically conducting polymers (Partridge
et al 2000) The polymer composites show
linear responses to concentration for various
analytes and also good repeatability after several
exposures (Severin 2000 Zee and Judy 2001)
From the above discussion it can be seen that
for high sensitivity fast response and short
recovery times it is essential that the sensor
geometry and all the associated properties of the
polymer sensing material be highly optimised
Conducting polymer composites offer many
advantages over other materials when utilised as
gas sensors High discrimination in array
sensors can be easily achieved using these
materials due to the wide range of polymeric
materials available on the market This is due to
the fact that different polymers give different
levels of response to a given odour Conducting
polymer composites are also relatively
inexpensive and easy to prepare Sensors
prepared from these materials can operate in
conditions of high relative humidity and also
show highly linear responses for a wide range of
gases (Munoz et al 1999) No heater is
required as sensors prepared from these
materials operate at room temperature This is
an important advantage with portable battery
powered e-nose systems as a heater would
significantly increase the power consumption of
the system The signal conditioning circuitry
required for these sensors is relatively simple as
only a resistance change is being measured
The main drawbacks of using conducting
polymer composites as e-nose sensors are aging
which leads to sensor drift and also these
materials are unsuitable for detecting certain
gases for example carbon-polymer composites
are not sensitive to trimethylamine (TMA) for
fish odour applications
Intrinsically conducting polymers
Intrinsically conducting polymers (ICP) have
linear backbones composed of unsaturated
monomers ie alternating double and single
bonds along the backbone that can be doped as
semiconductors or conductors (Heeger 2001)
Yasufuku (2001) describes them as p electron
conjugated polymers where the p symbol relates
to the unsaturated structure of the monomer
containing an unpaired carbon electron
These conducting polymers can be n-doped or
p-doped depending on the doping materials
used Conducting polymers such as polypyrrole
polythiophene and polyaniline as shown in
Figure 5 are typically used for e-nose sensing
The doping of these materials generates charge
carriers and also alters their band structure
which both induce increasedmobility of holes or
electrons in the polymer depending on the type
of doping used (Albert and Lewis 2000
Dickinson et al 1998)
The principle of operation for ICP e-nose
sensors is that the odorant is absorbed into the
polymer and alters the conductivity of the
polymer (Albert and Lewis 2000 Dickinson
et al 1998) Three types of conductivity are
affected in intrinsically conducting polymers
(1) The intrachain conductivity in which the
conductivity along the backbone is altered
(2) The intermolecular conductivity which is due
to electron hopping to different chains
because of analyte sorption (Charlesworth
et al 1997) and
(3) The ionic conductivity which is affected by
proton tunneling induced by hydrogen
bond interaction at the backbone and also
by ion migration through the polymer
(Albert and Lewis 2000) The physical
structure of the polymer also has a major
influence on the conductivity (Yasufuku
2001) Albert and Lewis (2000) described
how the conductivity of doped polyaniline
was greatly increased on interaction with
ethanol caused by the hydrogen bonds
Table IV General response times for conducting polymer
composites
Response time (s) Reference
lt2-4 Lonergan et al (1996)
60 Partridge (2000)
180-240 Corcoran (1993b)
20-200 Doleman et al (1998)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
186
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
hara
cter
istic
sof
com
mer
cial
e-no
ses
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Airsense
analysisGmbH
MO
S10
Food
eval
uatio
nfla
vour
and
frag
ranc
ete
stin
gA
NN
D
C
PCA
Lapt
op
ww
wa
irsen
sec
om
AlphaMOS-Multi
Organ
olepticSystem
s
CP
MO
S
QC
M
SAW
6-24
Ana
lysi
sof
food
type
squ
ality
cont
rolo
ffoo
dst
orag
efr
esh
fish
and
petr
oche
mic
alpr
oduc
ts
pack
agin
gev
alua
tion
anal
ysis
of
dairy
prod
ucts
al
coho
licbe
vera
ges
and
perf
umes
AN
N
DFA
PCA
Des
ktop
ww
wa
lpha
-mos
com
Applied
Sensor
IR
MO
S
MO
SFET
QC
M
22Id
entifi
catio
nof
purit
ypr
oces
san
dqu
ality
cont
rol
envi
ronm
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lan
alys
is
med
ical
diag
nosi
s
AN
N
PCA
Lapt
op
ww
wa
pplie
dsen
sorc
om
Uni
vers
ityof
Link
opin
gs
Swed
en
AromaS
canPLC
CP
32En
viro
nmen
tal
mon
itorin
gch
emic
alqu
ality
cont
rol
phar
mac
eutic
alpr
oduc
tev
alua
tion
AN
N
Des
ktop
Uni
vers
ityof
Man
ches
ter
Inst
itute
ofsc
ienc
ean
dte
chno
logy
UK
Array
Tech
QC
M8
Dia
gnos
ing
lung
canc
er
food
anal
ysis
Uni
vers
ityof
Rom
e
Bloodhoundsensors
CP
14Fo
odev
alua
tion
flavo
uran
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robi
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ronm
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lm
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ring
degr
adat
ion
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ctio
n
AN
N
CA
PC
A
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Lapt
op
Uni
vers
ityof
Leed
sU
K
Cyran
oScience
Inc
CP
32Fo
odqu
ality
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emic
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alys
is
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hnes
ssp
oila
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amin
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tect
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iste
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info
ods
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PCA
Palm
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Technologies
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nsorTechnology
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Food
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SPR
Des
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Envi
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Food
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
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CM
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Uni
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Marconitechnologies
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iffs
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mas
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MicrosensorSystem
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Che
mic
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rial
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ysis
Palm
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ood
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Des
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Ant
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wn
ose-
netw
ork
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Cra
nfiel
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nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
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ide
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icon
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Pndash
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uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
On exposure to gases these materials change
resistance and this change is due to percolation
effects or more complex mechanisms in the case
of polypyrrole filled composites
When the polymer composite sensor is
exposed to a vapour some of the vapour
permeates into the polymer and causes the
polymer film to expand The vapour-induced
expansion of the polymer composite causes an
increase in the electrical resistance of the
polymer composite because the polymer
expansion reduces the number of conducting
pathways for charge carriers (Munoz et al
1999) This increase in resistance is consistent
with percolation theory Polypyrrole-based
composites have a more complex transduction
mechanism because the odour molecules can
cause expansion of both the insulating polymer
and the polypyrrole particles Changes in the
intrinsic conductivity of the polypyrrole
particles can also occur if the odour interacts
chemically with the conducting polymer
backbone Therefore resistance changes in the
polypyrrole-based composites are more difficult
to predict (Albert and Lewis 2000)
Carbon black based composites were
prepared by suspending the carbon black in a
solution of the insulating polymer in a suitable
solvent The overall composition of this solution
is usually 80 per cent insulating polymer-
20 per cent carbon black by weight Different
techniques have been used to apply the active
material onto the substrate which are shown in
Table II
The transducer device is usually a flat
substrate with either two parallel electrodes or
interdigitated electrodes deposited onto the
substrate surface as shown in Figure 3
However both bulk and surface
micromachining have also been used to produce
wells on silicon substrates using patterned
silicon nitrideoxide as insulation and gold
electrodes as the metal contacts The polymer is
dropped into the well using a syringe as shown
in Figure 4 (Zee and Judy 2001)
Examples of the types of substrates and
electrodes used are given in Table III along with
the electrode dimensions given in the literature
Polypyrrole-based composites are usually
prepared by chemically polymerizing pyrrole
using phosphomolybdic acid in a solution
containing the insulating polymer A thin film
coating (40-100 nm thick) is then applied across
interdigitated electrodes (typical electrode gaps
were 15mm) using dip coating (Freund and
Lewis 1995)
The fractional baseline manipulation
response is the most common method used to
record the sensor response from conducting gas
sensors (Pearce et al 2003) This fractional
baseline manipulation is referred to as the
maximum relative differential resistance
change DRRb DR is the maximum change in
the resistance of the sensor during exposure to
the odorant and Rb is the baseline resistance
before exposure
Response times may vary from seconds to
minutes as shown in Table IV and in some
cases milliseconds (Munoz et al 1999)
However typically a set of exposure cycles
is quoted for each analyte ie initial reference
gas analyte and final reference gas exposure
times The response time depends on the rate
of diffusion of the permeant into the polymer
The diffusion rate mainly depends on the nature
of the polymer permeant and the crosslinking
the concentration of the permeant and thickness
of the film and on the effects of fillers
plasticisers and temperature (George and
Thomas 2001) General response times for
conducting polymer composites are given in
Table IV
The transport properties depend on the
fractional free volume (FFV) in the polymer and
on the mobility of the segments of the polymer
chains The segmental mobility of the polymer
chains depends on the extent of unsaturation
Therefore segmental mobility is significantly
Figure 3 Typical structure of a conductivity sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
184
reduced with increased numbers of double and
triple bonds on the carbon-carbon backbone
The presence of crystalline domains can have
two different effects on the permeability of a
polymer Crystallites are generally impermeable
to vapours at room temperature and will reduce
the diffusion coefficient However crystallites
act as large crosslinking regions in terms of the
chains entering and leaving the areas around the
crystallite in which diffusion occurs (Comyn
1985) Increased defect formation and a
reduction in interlamellar links predominate
and overshadow the effect of geometric
impedance to such an extent that diffusivity
increases despite increasing crystallinity (Vieth
1991) For example in PE-grafted carbon black
chemiresistors heat treatment of the composite
improved the crystallinity of the matrix PE and
resulted in a five-fold increase in the response of
the sensor to cyclohexane vapour compared to
the untreated sensor (Chen et al 2002)
The size and shape of the penetrating
molecule affects the rate of uptake of the vapour
by the polymer where increased size of the
molecule decreases the diffusion coefficient
Flattened or elongated molecules diffuse faster
than spherical-shaped molecules (George and
Thomas 2001)
The partial pressure ie the concentration
of the penetrant gas at the gas polymer interface
affects the response of the sensor The response
is inversely related to the vapour pressure of the
analyte at the surface Low vapour pressure
compounds can be detected in the low ppb
range while high vapour pressure compounds
need to be in the high ppm range to be detected
This is due to the polymergas partition
coefficient where low vapour pressure gas
molecules have a higher tendency to inhabit the
polymer and thus can be detected at much lower
concentrations (Munoz et al 1999)
The equilibrium partition coefficient is
essentially the solubility coefficient of the
vapour in the polymer (Vieth 1991) Sensors
with constant thickness but with different
surface areas have the same response when
exposed to analytes with moderate partition
coefficients However analytes with higher
partition coefficients have higher affinity to
sensors with smaller area In this case reducing
the sensor area increases the sensitivity of the
sensor towards particular analytes Therefore
the relationship between the partition
co-efficient and the sensor geometry is an
important factor in optimising polymer
composite sensor response (Briglin et al 2002)
Table II Application techniques used to deposit carbon black based composites
Reference Polymer Coating thickness Coating application technique
Matthews et al (2002) Poly(alkylacrylate) Thin film 086mm Spray coating
Severin et al (1998) Poly(co-vinyl-acetate) Thin film 1mm Spin coating
Severin et al (2000) Poly(vinyl butyral) Thin film NA Dip coating
Figure 4 Bulk micromachined well as used by Zee and Judy (2001)
Table III Electrodes and substrates used in conducting polymer composite sensors
Substrate
Electrode
material
Electrode
dimensions
(mm)
Electrode gap
(mm)
Electrode
thickness
(nm) Reference
Glass microscope slides Gold NA 5 50-100 Lonergan et al (1996)
Glass microscope slides Gold 10 pound 10 5 50 Doleman et al (1998a)
Glass microscope slides Gold Chromium 20 pound 10 5 30 20 Doleman et al (1998a b)
Micromachined silicon wafer Gold 01 in width 05 NA Zee and Judy (2001)
Glass microscope slide Gold Chromium 18 in length 04 50 15-30 Briglin et al (2002)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
185
Generally composite polymers have operating
resistances of approximately 1 to 1000 kV with
sensitivities of up to 100 per cent DRRb per mg
l gas depending on the filler type particle
loading and vapour transport properties
(Partridge et al 2000) Sensitivity to
hydrophobic analytes for conducting polymer
composites were found to be one to two orders
of magnitude higher than those recorded for
intrinsically conducting polymers (Partridge
et al 2000) The polymer composites show
linear responses to concentration for various
analytes and also good repeatability after several
exposures (Severin 2000 Zee and Judy 2001)
From the above discussion it can be seen that
for high sensitivity fast response and short
recovery times it is essential that the sensor
geometry and all the associated properties of the
polymer sensing material be highly optimised
Conducting polymer composites offer many
advantages over other materials when utilised as
gas sensors High discrimination in array
sensors can be easily achieved using these
materials due to the wide range of polymeric
materials available on the market This is due to
the fact that different polymers give different
levels of response to a given odour Conducting
polymer composites are also relatively
inexpensive and easy to prepare Sensors
prepared from these materials can operate in
conditions of high relative humidity and also
show highly linear responses for a wide range of
gases (Munoz et al 1999) No heater is
required as sensors prepared from these
materials operate at room temperature This is
an important advantage with portable battery
powered e-nose systems as a heater would
significantly increase the power consumption of
the system The signal conditioning circuitry
required for these sensors is relatively simple as
only a resistance change is being measured
The main drawbacks of using conducting
polymer composites as e-nose sensors are aging
which leads to sensor drift and also these
materials are unsuitable for detecting certain
gases for example carbon-polymer composites
are not sensitive to trimethylamine (TMA) for
fish odour applications
Intrinsically conducting polymers
Intrinsically conducting polymers (ICP) have
linear backbones composed of unsaturated
monomers ie alternating double and single
bonds along the backbone that can be doped as
semiconductors or conductors (Heeger 2001)
Yasufuku (2001) describes them as p electron
conjugated polymers where the p symbol relates
to the unsaturated structure of the monomer
containing an unpaired carbon electron
These conducting polymers can be n-doped or
p-doped depending on the doping materials
used Conducting polymers such as polypyrrole
polythiophene and polyaniline as shown in
Figure 5 are typically used for e-nose sensing
The doping of these materials generates charge
carriers and also alters their band structure
which both induce increasedmobility of holes or
electrons in the polymer depending on the type
of doping used (Albert and Lewis 2000
Dickinson et al 1998)
The principle of operation for ICP e-nose
sensors is that the odorant is absorbed into the
polymer and alters the conductivity of the
polymer (Albert and Lewis 2000 Dickinson
et al 1998) Three types of conductivity are
affected in intrinsically conducting polymers
(1) The intrachain conductivity in which the
conductivity along the backbone is altered
(2) The intermolecular conductivity which is due
to electron hopping to different chains
because of analyte sorption (Charlesworth
et al 1997) and
(3) The ionic conductivity which is affected by
proton tunneling induced by hydrogen
bond interaction at the backbone and also
by ion migration through the polymer
(Albert and Lewis 2000) The physical
structure of the polymer also has a major
influence on the conductivity (Yasufuku
2001) Albert and Lewis (2000) described
how the conductivity of doped polyaniline
was greatly increased on interaction with
ethanol caused by the hydrogen bonds
Table IV General response times for conducting polymer
composites
Response time (s) Reference
lt2-4 Lonergan et al (1996)
60 Partridge (2000)
180-240 Corcoran (1993b)
20-200 Doleman et al (1998)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
186
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
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Sensor
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Applications
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
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PGpp
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rLV
PG
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ntD
RR
bp
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DL
01-
5pp
m
Ope
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re
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vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
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spon
setim
es
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mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
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al
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orat
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mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
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cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
reduced with increased numbers of double and
triple bonds on the carbon-carbon backbone
The presence of crystalline domains can have
two different effects on the permeability of a
polymer Crystallites are generally impermeable
to vapours at room temperature and will reduce
the diffusion coefficient However crystallites
act as large crosslinking regions in terms of the
chains entering and leaving the areas around the
crystallite in which diffusion occurs (Comyn
1985) Increased defect formation and a
reduction in interlamellar links predominate
and overshadow the effect of geometric
impedance to such an extent that diffusivity
increases despite increasing crystallinity (Vieth
1991) For example in PE-grafted carbon black
chemiresistors heat treatment of the composite
improved the crystallinity of the matrix PE and
resulted in a five-fold increase in the response of
the sensor to cyclohexane vapour compared to
the untreated sensor (Chen et al 2002)
The size and shape of the penetrating
molecule affects the rate of uptake of the vapour
by the polymer where increased size of the
molecule decreases the diffusion coefficient
Flattened or elongated molecules diffuse faster
than spherical-shaped molecules (George and
Thomas 2001)
The partial pressure ie the concentration
of the penetrant gas at the gas polymer interface
affects the response of the sensor The response
is inversely related to the vapour pressure of the
analyte at the surface Low vapour pressure
compounds can be detected in the low ppb
range while high vapour pressure compounds
need to be in the high ppm range to be detected
This is due to the polymergas partition
coefficient where low vapour pressure gas
molecules have a higher tendency to inhabit the
polymer and thus can be detected at much lower
concentrations (Munoz et al 1999)
The equilibrium partition coefficient is
essentially the solubility coefficient of the
vapour in the polymer (Vieth 1991) Sensors
with constant thickness but with different
surface areas have the same response when
exposed to analytes with moderate partition
coefficients However analytes with higher
partition coefficients have higher affinity to
sensors with smaller area In this case reducing
the sensor area increases the sensitivity of the
sensor towards particular analytes Therefore
the relationship between the partition
co-efficient and the sensor geometry is an
important factor in optimising polymer
composite sensor response (Briglin et al 2002)
Table II Application techniques used to deposit carbon black based composites
Reference Polymer Coating thickness Coating application technique
Matthews et al (2002) Poly(alkylacrylate) Thin film 086mm Spray coating
Severin et al (1998) Poly(co-vinyl-acetate) Thin film 1mm Spin coating
Severin et al (2000) Poly(vinyl butyral) Thin film NA Dip coating
Figure 4 Bulk micromachined well as used by Zee and Judy (2001)
Table III Electrodes and substrates used in conducting polymer composite sensors
Substrate
Electrode
material
Electrode
dimensions
(mm)
Electrode gap
(mm)
Electrode
thickness
(nm) Reference
Glass microscope slides Gold NA 5 50-100 Lonergan et al (1996)
Glass microscope slides Gold 10 pound 10 5 50 Doleman et al (1998a)
Glass microscope slides Gold Chromium 20 pound 10 5 30 20 Doleman et al (1998a b)
Micromachined silicon wafer Gold 01 in width 05 NA Zee and Judy (2001)
Glass microscope slide Gold Chromium 18 in length 04 50 15-30 Briglin et al (2002)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
185
Generally composite polymers have operating
resistances of approximately 1 to 1000 kV with
sensitivities of up to 100 per cent DRRb per mg
l gas depending on the filler type particle
loading and vapour transport properties
(Partridge et al 2000) Sensitivity to
hydrophobic analytes for conducting polymer
composites were found to be one to two orders
of magnitude higher than those recorded for
intrinsically conducting polymers (Partridge
et al 2000) The polymer composites show
linear responses to concentration for various
analytes and also good repeatability after several
exposures (Severin 2000 Zee and Judy 2001)
From the above discussion it can be seen that
for high sensitivity fast response and short
recovery times it is essential that the sensor
geometry and all the associated properties of the
polymer sensing material be highly optimised
Conducting polymer composites offer many
advantages over other materials when utilised as
gas sensors High discrimination in array
sensors can be easily achieved using these
materials due to the wide range of polymeric
materials available on the market This is due to
the fact that different polymers give different
levels of response to a given odour Conducting
polymer composites are also relatively
inexpensive and easy to prepare Sensors
prepared from these materials can operate in
conditions of high relative humidity and also
show highly linear responses for a wide range of
gases (Munoz et al 1999) No heater is
required as sensors prepared from these
materials operate at room temperature This is
an important advantage with portable battery
powered e-nose systems as a heater would
significantly increase the power consumption of
the system The signal conditioning circuitry
required for these sensors is relatively simple as
only a resistance change is being measured
The main drawbacks of using conducting
polymer composites as e-nose sensors are aging
which leads to sensor drift and also these
materials are unsuitable for detecting certain
gases for example carbon-polymer composites
are not sensitive to trimethylamine (TMA) for
fish odour applications
Intrinsically conducting polymers
Intrinsically conducting polymers (ICP) have
linear backbones composed of unsaturated
monomers ie alternating double and single
bonds along the backbone that can be doped as
semiconductors or conductors (Heeger 2001)
Yasufuku (2001) describes them as p electron
conjugated polymers where the p symbol relates
to the unsaturated structure of the monomer
containing an unpaired carbon electron
These conducting polymers can be n-doped or
p-doped depending on the doping materials
used Conducting polymers such as polypyrrole
polythiophene and polyaniline as shown in
Figure 5 are typically used for e-nose sensing
The doping of these materials generates charge
carriers and also alters their band structure
which both induce increasedmobility of holes or
electrons in the polymer depending on the type
of doping used (Albert and Lewis 2000
Dickinson et al 1998)
The principle of operation for ICP e-nose
sensors is that the odorant is absorbed into the
polymer and alters the conductivity of the
polymer (Albert and Lewis 2000 Dickinson
et al 1998) Three types of conductivity are
affected in intrinsically conducting polymers
(1) The intrachain conductivity in which the
conductivity along the backbone is altered
(2) The intermolecular conductivity which is due
to electron hopping to different chains
because of analyte sorption (Charlesworth
et al 1997) and
(3) The ionic conductivity which is affected by
proton tunneling induced by hydrogen
bond interaction at the backbone and also
by ion migration through the polymer
(Albert and Lewis 2000) The physical
structure of the polymer also has a major
influence on the conductivity (Yasufuku
2001) Albert and Lewis (2000) described
how the conductivity of doped polyaniline
was greatly increased on interaction with
ethanol caused by the hydrogen bonds
Table IV General response times for conducting polymer
composites
Response time (s) Reference
lt2-4 Lonergan et al (1996)
60 Partridge (2000)
180-240 Corcoran (1993b)
20-200 Doleman et al (1998)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
186
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
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gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
Generally composite polymers have operating
resistances of approximately 1 to 1000 kV with
sensitivities of up to 100 per cent DRRb per mg
l gas depending on the filler type particle
loading and vapour transport properties
(Partridge et al 2000) Sensitivity to
hydrophobic analytes for conducting polymer
composites were found to be one to two orders
of magnitude higher than those recorded for
intrinsically conducting polymers (Partridge
et al 2000) The polymer composites show
linear responses to concentration for various
analytes and also good repeatability after several
exposures (Severin 2000 Zee and Judy 2001)
From the above discussion it can be seen that
for high sensitivity fast response and short
recovery times it is essential that the sensor
geometry and all the associated properties of the
polymer sensing material be highly optimised
Conducting polymer composites offer many
advantages over other materials when utilised as
gas sensors High discrimination in array
sensors can be easily achieved using these
materials due to the wide range of polymeric
materials available on the market This is due to
the fact that different polymers give different
levels of response to a given odour Conducting
polymer composites are also relatively
inexpensive and easy to prepare Sensors
prepared from these materials can operate in
conditions of high relative humidity and also
show highly linear responses for a wide range of
gases (Munoz et al 1999) No heater is
required as sensors prepared from these
materials operate at room temperature This is
an important advantage with portable battery
powered e-nose systems as a heater would
significantly increase the power consumption of
the system The signal conditioning circuitry
required for these sensors is relatively simple as
only a resistance change is being measured
The main drawbacks of using conducting
polymer composites as e-nose sensors are aging
which leads to sensor drift and also these
materials are unsuitable for detecting certain
gases for example carbon-polymer composites
are not sensitive to trimethylamine (TMA) for
fish odour applications
Intrinsically conducting polymers
Intrinsically conducting polymers (ICP) have
linear backbones composed of unsaturated
monomers ie alternating double and single
bonds along the backbone that can be doped as
semiconductors or conductors (Heeger 2001)
Yasufuku (2001) describes them as p electron
conjugated polymers where the p symbol relates
to the unsaturated structure of the monomer
containing an unpaired carbon electron
These conducting polymers can be n-doped or
p-doped depending on the doping materials
used Conducting polymers such as polypyrrole
polythiophene and polyaniline as shown in
Figure 5 are typically used for e-nose sensing
The doping of these materials generates charge
carriers and also alters their band structure
which both induce increasedmobility of holes or
electrons in the polymer depending on the type
of doping used (Albert and Lewis 2000
Dickinson et al 1998)
The principle of operation for ICP e-nose
sensors is that the odorant is absorbed into the
polymer and alters the conductivity of the
polymer (Albert and Lewis 2000 Dickinson
et al 1998) Three types of conductivity are
affected in intrinsically conducting polymers
(1) The intrachain conductivity in which the
conductivity along the backbone is altered
(2) The intermolecular conductivity which is due
to electron hopping to different chains
because of analyte sorption (Charlesworth
et al 1997) and
(3) The ionic conductivity which is affected by
proton tunneling induced by hydrogen
bond interaction at the backbone and also
by ion migration through the polymer
(Albert and Lewis 2000) The physical
structure of the polymer also has a major
influence on the conductivity (Yasufuku
2001) Albert and Lewis (2000) described
how the conductivity of doped polyaniline
was greatly increased on interaction with
ethanol caused by the hydrogen bonds
Table IV General response times for conducting polymer
composites
Response time (s) Reference
lt2-4 Lonergan et al (1996)
60 Partridge (2000)
180-240 Corcoran (1993b)
20-200 Doleman et al (1998)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
186
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
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df
hazm
atca
d
OligoSe
nse
CO
ndashA
utom
otiv
eap
plic
atio
nsf
ood
eval
uatio
npa
ckag
ing
eval
uatio
nht
tp
ww
wo
ligos
ense
be
RST
Rostock
Rau
m-fah
rtund
UmweltschatzGmbH
MO
SQ
CM
SAW
6-10
Early
reco
gniti
onof
fires
w
arni
ngin
the
even
tof
esca
peof
haza
rdou
ssu
bsta
nces
le
akde
tect
ion
wor
kpla
cem
onito
ring
AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
tightening or restructuring the polymer into
a more crystalline shape
Intrinsically conducting polymers are generally
deposited onto a substrate with interdigitated
electrodes using electrochemical techniques or
by chemical polymerisation (Freund and
Lewis 1995 Yasufuku 2001) Sensors with a
more simple structure can be prepared where
the polymer is deposited between two
conducting electrodes (Guadarrama et al
2000) Electrochemical polymerisation is
carried out using a three-electrode
electrochemical cell with the electrodes on
the substrate used as the working electrodes
(Gardner and Bartlett 1995) A potential is
applied across the electrode that initiates the
polymerisation of the polymer onto the
substrate The polymer is initially deposited
onto the electrodes and then grows between
them thus producing a complete thin film across
the electrode arrangement as the polymerisation
reactions progress Electrode thickness can
range from 1 to 10mm and the electrode gap
is typically 10-50mm (Albert and Lewis 2000
Guadarrama et al 2000) The total charge
applied during the polymerisation process
determines the thickness of the resultant film
while the final applied voltage determines the
doping concentration
Partridge et al (2000) described the sensor
characteristics of intrinsically conducting
polymers produced by pulsing the potential
during polymerisation and observed a
1-50 per cent relative differential resistance
change (DRRb) for saturated gas
The response of ICP sensors depends on
the sorption of the vapour into the sensing
material causing swelling and this affects
the electron density on the polymeric chains
(Albert and Lewis 2000) The sorption
properties of these materials essentially depend
on the diffusion rate of the permeant into the
polymer matrix as explained earlier for
composite conducting polymers Generally
the reported response times for ICPs vary
considerably from seconds to minutes eg 30 s
(Sotzing et al 2000) 60 s (Pearce et al
2003) and 180-240 s (Corcoran 1993a)
Polythiophene and poly(dodecylthiophene)
sensors have sensitivities from approximately
02 up to 18 (DRRb for 300 ppm gas for
10min) for gases such as CH4 CHCl3 and NH4
(Sakurai et al 2002) Polypyrrole gas sensors
were reported to have sensitivities (mVppm)
ranging from 026 to 501 depending on the
counter ions used in the polymers films
(Fang et al 2002) These response times and
sensitivities are reported for an extremely vast
variety of materials prepared by various
techniques sensor geometries and odour
molecules rendering direct comparisons
between sensors prepared by different
researchers difficult if not impractical
Intrinsically conducting polymers have a
number of advantages when used in e-nose
systems Increased discrimination when
developing sensor arrays can easily be achieved
with these materials as a wide range of
intrinsically conducting polymers are available
on the market (Albert and Lewis 2000) ICP
sensors operate at room temperature (Shurmer
and Gardner 1992) thereby simplifying the
required system electronics Conducting
polymers show a good response to a wide range
of analytes and have fast response and recovery
times especially for polar compounds
Problems related to intrinsically conducting
polymer sensors include poorly understood
signal transduction mechanisms difficulties in
Figure 5 Chemical structures of (a) polyaniline (b) polypyrrole and (c) polythiophene
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
187
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
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effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
resolving some types of analytes high sensitivity
to humidity (Albert and Lewis 2000) and
the sensor response can drift with time
The fabrication techniques for these sensors
can also be difficult and time-consuming
(Nagle et al 1998) and large variations in the
properties of the sensors can occur from batch
to batch (Nagle et al 1998) Finally the
lifetime of these sensors can be quite short
typically 9-18 months due to oxidation of the
polymer (Schaller et al 1998)
Metal oxide sensors
The principle of operation of metal oxide
sensors is based on the change in conductance
of the oxide on interaction with a gas and
the change is usually proportional to the
concentration of the gas There are two types of
metal oxide sensors n-type (zinc oxide tin
dioxide titanium dioxide or iron (III) oxide)
which respond to reducing gases and p-type
(nickel oxide cobalt oxide) which respond to
oxidising gases (Pearce et al 2003) The n-type
sensor operates as follows oxygen in the air
reacts with the surface of the sensor and traps
any free electrons on the surface or at the grain
boundaries of the oxide grains This produces
large resistance in these areas due to the lack of
carriers and the resulting potential barriers
produced between the grains inhibit the carrier
mobility However if the sensor is introduced to
a reducing gas like H2 CH4 CO C2H5 or H2S
the resistance drops because the gas reacts
with the oxygen and releases an electron
This lowers the potential barrier and allows
the electrons to flow thereby increasing the
conductivity P-type sensors respond to
oxidising gases like O2 NO2 and Cl2 as these
gases remove electrons and produce holes
ie producing charge carriers Equations (1)
and (2) describe the reactions occurring at
the surface
1
2O2 thorn e2 O2ethsTHORN eth5THORN
RethgTHORN thornO2ethsTHORN ROethgTHORN thorn e eth6THORN
Where e is an electron from the oxide R(g) is
the reducing gas and g and s are the surface and
gas respectively (Albert and Lewis 2000
Pearce et al 2003)
Thick and thin film fabrication methods have
been used to produce metal oxide gas sensors
The metal oxide films are deposited using
screenprinting (Schmid et al 2003)
spincoating (Hamakawa et al 2002) RF
sputtering (Tao and Tsai 2002) or chemical
vapour deposition (Dai 1998) onto a flat or
tube type substrate made of alumina glass
silicon or some other ceramic Gold platinum
silver or aluminium electrodes are deposited
onto the substrate using the same methods
There are various electrode designs but the
interdigitated structure appears to be the most
common approach A heating element is printed
onto the back of the substrate to provide the
high temperatures required for metal oxides to
operate as gas sensors typically 200-5008C
Film thickness ranges from 10 to 300mm for
thick film and 6-1000 nm for thin film
(Schaller et al 1998) Catalytic metals are
sometimes applied on top of the oxides to
improve sensitivity to certain gases The same
preparative methods are used to apply the
catalytic metal (Albert and Lewis 2000
Penza et al 2001b c)
The sensitivity of oxide gas sensors
ethDR=RbTHORN=cethgasTHORN is calculated with DR frac14 R2 Rb
for oxidising gases and as DR frac14 Rb 2 R for
reducing gases where Rb is the baseline
resistance and R is the resistance on exposure to
the odour and c(gas) is the concentration of
the gas (Steffes et al 2001) The sensitivity of
the metal oxide sensor depends on the film
thickness and the temperature at which the
sensor is operated with thinner films being
more sensitive to gases (Schaller et al 1998)
The sensitivity can be improved by adding a
catalytic metal to the oxide however excessive
doping can reduce sensitivity The effect of
doping SnO2 sensors with Cu for example
demonstrated significant increases in sensitivity
(Galdikas et al 1995) The grain size of the
oxide also affects the sensitivity and selectivity to
particular gases as the grain boundaries act as
scattering centres for the electrons (Schaller
et al 1998) The ratio of the grain size (D) to
the electron depletion layer thickness (L)
ranging below D=2L frac14 1 ie the depletion
region extends over the entire grain governs the
sensitivity of the sensor (Behr and Fliegel
1995) Thin film metal oxide sensors saturate
quickly which can reduce the sensitivity range
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
188
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
in which the sensor can operate The sensitivity
of metal oxide sensors is very dependent on the
operating temperature for example the
sensitivity DR=Rb (per 10 ppm NO2) for In2O3
gas sensors range from approximately 12 to 16
with the operating temperature varying from
350 to 4508C (Steffes et al 2001) For SnO2
gas sensors doped with Al2O3 the sensitivity per
500 ppm CH4 ranges from 02 to 07 between
250 and 4008C (Saha et al 2001)
The response times for tin oxides tend to be
very fast and can reach steady-state in less than
7 s (Doleman et al 1998a b) The general
response times for tin oxide sensors with gas
concentrations between 0 and 400 ppm and at
temperatures between 250 and 5008C are 5 to
35 s and the recovery times vary from 15 to 70 s
(Albert and Lewis 2000) Corcoran gave values
of 20 s for thick film metal oxide sensors and
12 s for thin filmmetal oxide sensors (Corcoran
1993b)
The main advantages of metal oxide sensors
are fast response and recovery times which
mainly depend on the temperature and the level
of interaction between the sensor and gas
(Penza et al 2001c) Thin film metal oxide
sensors are small and relatively inexpensive to
fabricate have lower power consumption than
thick film sensors and can be integrated directly
into the measurement circuitry (Dai 1998)
However they have many disadvantages due to
their high operating temperatures which results
in increased power consumption over sensors
fabricated from materials other than metal
oxides As a result no handheld e-nose system
has been fabricated utilising sensors prepared
from metal oxides (Pearce et al 2003)
They also suffer from sulphur poisoning due to
irreversible binding of compounds that contain
sulphur to the sensor oxide (Dickinson et al
1998) and ethanol can also blind the sensor
from other volatile organic compound (VOC)
gases (Schaller et al 1998)
Piezoelectric sensors used in e-nose arrays
There are two types of piezoelectric sensors
used in gas sensing the surface acoustic wave
(SAW) device and the quartz crystal
microbalance (QCM) The SAW device
produces a surface wave that travels along the
surface of the sensor while the QCM produces a
wave that travels through the bulk of the sensor
Both types of devices work on the principle that
a change in the mass of the piezoelectric sensor
coating due to gas absorption results in a change
in the resonant frequency on exposure to a
vapour (Albert and Lewis 2000)
Surface acoustic wave sensor
The SAW device is composed of a piezoelectric
substrate with an input (transmitting) and
output (receiving) interdigital transducer
deposited on top of the substrate
(Khlebarov et al 1992) The sensitive
membrane is placed between the transducers
Figure 6 and an ac signal is applied across the
input transducer creating an acoustic two-
dimensional wave that propagates along the
surface of the crystal at a depth of one
wavelength at operating frequencies between
100 and 400MHz (Pearce et al 2003) The
mass of the gas sensitive membrane of the SAW
device is changed on interaction with a
compatible analyte and causes the frequency of
the wave to be altered The change in frequency
with sorption of a vapour is given by
Df frac14 Df pcvKp=rp eth7THORN
where Dfp is the change in frequency caused
by the membrane cv is the vapour
concentration Kp is the partition coefficient
rp is the density of the polymer membrane
used (Albert and Lewis 2000 Nagle et al
1998 Pearce et al 2003)
The substrates are normally prepared from
ZnO lithium niobate or quartz which are
piezoelectric in nature (Pearce et al 2003)
The sensitive membrane is usually polymeric or
Figure 6 SAW sensor
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
189
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
hara
cter
istic
sof
com
mer
cial
e-no
ses
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Airsense
analysisGmbH
MO
S10
Food
eval
uatio
nfla
vour
and
frag
ranc
ete
stin
gA
NN
D
C
PCA
Lapt
op
ww
wa
irsen
sec
om
AlphaMOS-Multi
Organ
olepticSystem
s
CP
MO
S
QC
M
SAW
6-24
Ana
lysi
sof
food
type
squ
ality
cont
rolo
ffoo
dst
orag
efr
esh
fish
and
petr
oche
mic
alpr
oduc
ts
pack
agin
gev
alua
tion
anal
ysis
of
dairy
prod
ucts
al
coho
licbe
vera
ges
and
perf
umes
AN
N
DFA
PCA
Des
ktop
ww
wa
lpha
-mos
com
Applied
Sensor
IR
MO
S
MO
SFET
QC
M
22Id
entifi
catio
nof
purit
ypr
oces
san
dqu
ality
cont
rol
envi
ronm
enta
lan
alys
is
med
ical
diag
nosi
s
AN
N
PCA
Lapt
op
ww
wa
pplie
dsen
sorc
om
Uni
vers
ityof
Link
opin
gs
Swed
en
AromaS
canPLC
CP
32En
viro
nmen
tal
mon
itorin
gch
emic
alqu
ality
cont
rol
phar
mac
eutic
alpr
oduc
tev
alua
tion
AN
N
Des
ktop
Uni
vers
ityof
Man
ches
ter
Inst
itute
ofsc
ienc
ean
dte
chno
logy
UK
Array
Tech
QC
M8
Dia
gnos
ing
lung
canc
er
food
anal
ysis
Uni
vers
ityof
Rom
e
Bloodhoundsensors
CP
14Fo
odev
alua
tion
flavo
uran
dfr
agra
nce
test
ing
mic
robi
olog
y
envi
ronm
enta
lm
onito
ring
degr
adat
ion
dete
ctio
n
AN
N
CA
PC
A
DA
Lapt
op
Uni
vers
ityof
Leed
sU
K
Cyran
oScience
Inc
CP
32Fo
odqu
ality
ch
emic
alan
alys
is
fres
hnes
ssp
oila
ge
cont
amin
atio
nde
tect
ion
cons
iste
ncy
info
ods
and
beve
rage
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PCA
Palm
top
ww
wc
yran
osci
ence
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m
Cal
iforn
iain
stitu
teof
Tech
nolo
gy
USA
MarconiApplied
Technologies
QC
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CP
MO
SSA
W
8-28
AN
N
DA
PC
AU
nive
rsity
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arw
ick
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ElectronicSe
nsorTechnology
Inc
GC
SA
W1
Food
and
beve
rage
qual
ity
bact
eria
iden
tifica
tion
expl
osiv
es
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drug
dete
ctio
nen
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nmen
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SPR
Des
ktop
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lcom
Forschungszen
trum
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Envi
ronm
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ntro
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Qua
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ish
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sorsystemeGmbH
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Food
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rsity
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unic
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Illumina
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Life
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ture
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emic
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AN
Nw
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fts
Uni
vers
ity
USA
(Con
tinue
d)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
SQ
CM
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odan
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Des
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lect
roni
cde
PDF_
docu
men
ts
Uni
vers
ityof
Tubi
ngen
Marconitechnologies
MastiffElectronic
System
sLtd
CP
16Sn
iffs
palm
sfo
rpe
rson
alid
entifi
catio
nw
ww
mas
tiffc
ouk
MicrosensorSystem
sSA
W2
Che
mic
alag
ent
dete
ctio
nch
emic
alw
arfa
re(C
W)
agen
tsan
d
toxi
cin
dust
rial
chem
ical
s(T
ICs)
anal
ysis
Palm
top
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wm
icro
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orsy
stem
sco
mp
df
hazm
atca
d
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nse
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ndashA
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otiv
eap
plic
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nsf
ood
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ckag
ing
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uatio
nht
tp
ww
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ligos
ense
be
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Rostock
Rau
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rtund
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CM
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Early
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gniti
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arni
ngin
the
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tof
esca
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ssu
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akde
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kpla
cem
onito
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AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
liquid crystal however phospholipids and fatty
acids deposited using Langmuir-Blodgett
techniques have also been used (Albert and
Lewis 2000) Generally SAW devices are
produced commercially by photolithography
where airbrush techniques are often used to
deposit the thin films (Nagle et al 1998
Schaller et al 1998) approximately 20-30 nm
thick (Groves and Zellers 2001) SAW devices
have also been produced by utilising screen
printing techniques (White and Turner 1997)
dip coating and spin coating
The sensitivity of the SAW device to a
particular odour depends on the type sensitive
membrane and the uptake of vapours by
polymers are governed by the same factors as
those for composite conducting polymer sensors
as detailed earlier in this paper The sensitivity is
normally quoted as differential response
ie Dfpppm of odour (Hierlemann et al 1995
Pearce et al 2003) Polymer-coated SAW
devices have quite low detection limits for
example tetrachloroethylene trichloroethylene
and methoxyflurane have been detected at
concentrations as low as 07 06 and 4ppm
respectively (Albert and Lewis 2000)
Groves et al used an array of SAW devices
with polymer coatings 20-30 nm thick to
detect 16 different solvents using four
different polymers Sensitivities ranging
from 05 up to 12Hzmgm3 have been achieved
with these devices (Groves et al 2001)
Organophosphorous compounds have also been
detected using these types of devices at
concentrations from 10 to 100 ppm at
temperatures between 25 and 508C where
a sensitivity of 27Hzppm at 308C
(Dejous et al 1995)
As can be seen above SAW devices can detect
a broad spectrum of odours due to the wide
range of gas sensitive coatings available
(Carey et al 1986 Grate and Abraham 1991)
and they also offer high sensitivity and fast
response times and their fabrication is
compatible with current planar IC technologies
(Nagle et al 1998)
However SAW devices suffer from poor
signal to noise performance because of the high
frequencies at which they operate (Schaller
et al 1998) and the circuitry required to
operate them is complex and expensive (Pearce
et al 2003) Batch to batch reproducibility is
difficult to achieve and the replacement of
damaged sensors was also found to be
problematic (Schaller et al 1998)
Quartz crystal microbalance sensor
Quartz crystal microbalance (QCM) gas
sensors operate on the same principle as SAW
devices When an ac voltage is applied across
the piezoelectric quartz crystal the material
oscillates at its resonant frequency normally
between 10 and 30MHz (Schaller et al 1998)
The three-dimensional wave produced
travels through the entire bulk of the crystal
A membrane is deposited onto the surface of
the crystal and this layer adsorbs gas when
exposed to the vapour which results in an
increase in its mass This increase in mass
alters the resonant frequency of the quartz
crystal and this change in resonant frequency is
therefore used for the detection of the vapour
(Albert and Lewis 2000)
The sensor shown in Figure 7 is composed
of a quartz disc coated with the absorbing
polymer layer and a set of gold electrodes
evaporated onto either side of the polymer
quartz structure Micromachining is used to
fabricate the QCM devices which makes the
fabrication of small sensor structures possible
Coatings can be between 10 nm and 1mm and
are applied using spincoating airbrushing
inkjet printing or dip coating (Schaller et al
1998)
The sensitivity of QCMs is given by
Df
Dcfrac14
eth223 pound 1026THORNf 2
Aeth8THORN
Figure 7 Quartz crystal microbalance with polymer coating
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
190
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
hara
cter
istic
sof
com
mer
cial
e-no
ses
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Airsense
analysisGmbH
MO
S10
Food
eval
uatio
nfla
vour
and
frag
ranc
ete
stin
gA
NN
D
C
PCA
Lapt
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ww
wa
irsen
sec
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olepticSystem
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CP
MO
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M
SAW
6-24
Ana
lysi
sof
food
type
squ
ality
cont
rolo
ffoo
dst
orag
efr
esh
fish
and
petr
oche
mic
alpr
oduc
ts
pack
agin
gev
alua
tion
anal
ysis
of
dairy
prod
ucts
al
coho
licbe
vera
ges
and
perf
umes
AN
N
DFA
PCA
Des
ktop
ww
wa
lpha
-mos
com
Applied
Sensor
IR
MO
S
MO
SFET
QC
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22Id
entifi
catio
nof
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san
dqu
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cont
rol
envi
ronm
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lan
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med
ical
diag
nosi
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AN
N
PCA
Lapt
op
ww
wa
pplie
dsen
sorc
om
Uni
vers
ityof
Link
opin
gs
Swed
en
AromaS
canPLC
CP
32En
viro
nmen
tal
mon
itorin
gch
emic
alqu
ality
cont
rol
phar
mac
eutic
alpr
oduc
tev
alua
tion
AN
N
Des
ktop
Uni
vers
ityof
Man
ches
ter
Inst
itute
ofsc
ienc
ean
dte
chno
logy
UK
Array
Tech
QC
M8
Dia
gnos
ing
lung
canc
er
food
anal
ysis
Uni
vers
ityof
Rom
e
Bloodhoundsensors
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14Fo
odev
alua
tion
flavo
uran
dfr
agra
nce
test
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mic
robi
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envi
ronm
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lm
onito
ring
degr
adat
ion
dete
ctio
n
AN
N
CA
PC
A
DA
Lapt
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Uni
vers
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Leed
sU
K
Cyran
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Inc
CP
32Fo
odqu
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emic
alan
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fres
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amin
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Palm
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Cal
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GC
SA
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Food
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beve
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iden
tifica
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and
drug
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SPR
Des
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Envi
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A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
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MO
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Early
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edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
where f is the fundamental frequency c is the
concentration and A is the area of the sensitive
film (Carey and Kowalski 1986) Higher
frequencies and smaller surface areas of
sensitive coatings give rise to higher sensitivity
(Carey 1987)
A quartz crystal microbalance gas sensor was
developed and had a linear frequency shift on
interaction with ethanol n-heptane and acetone
and showed a 16Hz shift for 25 ppm of ethanol
and 15Hz shift for 1 ppm of n-heptane
(Kim 2002) demonstrating their high
sensitivity to organic vapours QCM devices are
sensitive to a diverse range of analytes and are
also very selective (Pearce et al 2003)
Polyvinylpyrrolidone modified QCMs have
been used to detect various organic vapours and
had sensitivities in the range of 75-482Hzmgl
(Mirmohseni and Oladegaragoze 2003)
The advantages of using QCMs are fast
response times typically 10 s (Haug et al
1993) however response times of 30 s to 1min
have been reported (Carey 1987) However
QCM gas sensors have many disadvantages
which include complex fabrication processes
and interface circuitry (Nagle et al 1998) and
poor signal to noise performance due to surface
interferences and the size of the crystal (Nagle
et al 1998) As with SAW devices batch-to-
batch reproducibility of QCM gas sensors and
the replacement of damaged sensors are difficult
(Dickinson et al 1998)
Optical sensors used in e-nose arrays
Optical fibre sensor arrays are yet another
approach to odour identification in e-nose
systems The sides or tips of the optic fibres
(thickness 2mm) are coated with a fluorescent
dye encapsulated in a polymer matrix as shown
in Figure 8 Polarity alterations in the
fluorescent dye on interaction with the vapour
changes the dyersquos optical properties such as
intensity change spectrum change lifetime
change or wavelength shift in fluorescence
(Nagle et al 1998 Pearce et al 2003)
These optical changes are used as the response
mechanism for odour detection (Grattan and
Sun 2000 Gopel 1992)
The sensitivity depends on the type of
fluorescent dye or mixture of dyes and the
type of polymer used to support the dye
(Nagle et al 1998) The nature of the polymer
controls the response and the most important
factors are polarity hydrophobicity porosity
and swelling tendency (Nagle et al 1998
Pearce et al 2003) Adsorbants such as
alumina can be added to the polymer to
improve the response by lowering the detection
limits of the sensor (Walt et al 1998)
Polyanaline-coated optical sensors have been
used to detect ammonia at concentrations as
low as 1 ppm and the linear dynamic range
was between 180 and 18000 ppm ( Jin 2001)
Optical gas sensors have very fast response
times less than 10 s for sampling and analysis
(Walt et al 1998)
These compact lightweight optical gas
sensors can be multiplexed on a single fibre
network immune to electromagnetic
interference (EMI) and can operate in high
radiation areas due to Bragg and other grating
based optical sensors (Gopel 1992 Walt et al
1998)
However there are several disadvantages
of these types of sensors The associated
electronics and software are very complex
leading to increased cost and the sensors have
quite a short lifetime due to photobleaching
(Nagle et al 1998) However this problem
was overcome by measuring the temporal
Figure 8 A gas optical fibre sensor The odorant interacts with the material and causes a shift in the wavelength of the
propagating light wave
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
191
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
hara
cter
istic
sof
com
mer
cial
e-no
ses
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Airsense
analysisGmbH
MO
S10
Food
eval
uatio
nfla
vour
and
frag
ranc
ete
stin
gA
NN
D
C
PCA
Lapt
op
ww
wa
irsen
sec
om
AlphaMOS-Multi
Organ
olepticSystem
s
CP
MO
S
QC
M
SAW
6-24
Ana
lysi
sof
food
type
squ
ality
cont
rolo
ffoo
dst
orag
efr
esh
fish
and
petr
oche
mic
alpr
oduc
ts
pack
agin
gev
alua
tion
anal
ysis
of
dairy
prod
ucts
al
coho
licbe
vera
ges
and
perf
umes
AN
N
DFA
PCA
Des
ktop
ww
wa
lpha
-mos
com
Applied
Sensor
IR
MO
S
MO
SFET
QC
M
22Id
entifi
catio
nof
purit
ypr
oces
san
dqu
ality
cont
rol
envi
ronm
enta
lan
alys
is
med
ical
diag
nosi
s
AN
N
PCA
Lapt
op
ww
wa
pplie
dsen
sorc
om
Uni
vers
ityof
Link
opin
gs
Swed
en
AromaS
canPLC
CP
32En
viro
nmen
tal
mon
itorin
gch
emic
alqu
ality
cont
rol
phar
mac
eutic
alpr
oduc
tev
alua
tion
AN
N
Des
ktop
Uni
vers
ityof
Man
ches
ter
Inst
itute
ofsc
ienc
ean
dte
chno
logy
UK
Array
Tech
QC
M8
Dia
gnos
ing
lung
canc
er
food
anal
ysis
Uni
vers
ityof
Rom
e
Bloodhoundsensors
CP
14Fo
odev
alua
tion
flavo
uran
dfr
agra
nce
test
ing
mic
robi
olog
y
envi
ronm
enta
lm
onito
ring
degr
adat
ion
dete
ctio
n
AN
N
CA
PC
A
DA
Lapt
op
Uni
vers
ityof
Leed
sU
K
Cyran
oScience
Inc
CP
32Fo
odqu
ality
ch
emic
alan
alys
is
fres
hnes
ssp
oila
ge
cont
amin
atio
nde
tect
ion
cons
iste
ncy
info
ods
and
beve
rage
s
PCA
Palm
top
ww
wc
yran
osci
ence
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m
Cal
iforn
iain
stitu
teof
Tech
nolo
gy
USA
MarconiApplied
Technologies
QC
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CP
MO
SSA
W
8-28
AN
N
DA
PC
AU
nive
rsity
ofW
arw
ick
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ElectronicSe
nsorTechnology
Inc
GC
SA
W1
Food
and
beve
rage
qual
ity
bact
eria
iden
tifica
tion
expl
osiv
es
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drug
dete
ctio
nen
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nmen
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SPR
Des
ktop
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lcom
Forschungszen
trum
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Envi
ronm
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ntro
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Qua
lity
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uctio
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otiv
eap
plic
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PCA
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K2
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ish
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sorsystemeGmbH
QC
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Food
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rage
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smet
ics
and
perf
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rsity
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man
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Illumina
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Life
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odpr
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ricul
ture
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emic
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AN
Nw
ww
illu
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fts
Uni
vers
ity
USA
(Con
tinue
d)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
SQ
CM
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odan
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gepr
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Des
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nnar
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lect
roni
cde
PDF_
docu
men
ts
Uni
vers
ityof
Tubi
ngen
Marconitechnologies
MastiffElectronic
System
sLtd
CP
16Sn
iffs
palm
sfo
rpe
rson
alid
entifi
catio
nw
ww
mas
tiffc
ouk
MicrosensorSystem
sSA
W2
Che
mic
alag
ent
dete
ctio
nch
emic
alw
arfa
re(C
W)
agen
tsan
d
toxi
cin
dust
rial
chem
ical
s(T
ICs)
anal
ysis
Palm
top
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wm
icro
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orsy
stem
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mp
df
hazm
atca
d
OligoSe
nse
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ndashA
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otiv
eap
plic
atio
nsf
ood
eval
uatio
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ckag
ing
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uatio
nht
tp
ww
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ligos
ense
be
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Rostock
Rau
m-fah
rtund
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MO
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CM
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gniti
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arni
ngin
the
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tof
esca
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ssu
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akde
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kpla
cem
onito
ring
AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
responses because these remain consistent
despite photobleaching (Walt et al 1998)
Metal-oxide-semiconductor field-effect
transistor sensor and its use in the e-nose
The metal-oxide-semiconductor field-effect
transistor (MOSFET) is a transducer device
used in e-nose to transform a physicalchemical
change into an electrical signal The MOSFET
sensor is a metal-insulator-semiconductor
(MIS) device and its structure is shown in
Figure 9 (Eisele et al 2001)
This particular sensor works on the principle
that the threshold voltage of the MOSFET
sensor changes on interaction of the gate
material usually a catalytic metal with certain
gases such as hydrogen due to corresponding
changes in the work functions of the metal
and the oxide layers (Pearce et al 2003)
The changes in the work functions occur due to
the polarization of the surface and interface
of the catalytic metal and oxide layer when the
gas interacts with the catalytically active surface
(Kalman et al 2000) In order for the physical
changes in the sensor to occur the metal-
insulator interface has to be accessible to the
gas Therefore a porous gas sensitive gate
material is used to facilitate diffusion of gas into
the material (Eisele et al 2001) It has been
observed that the change in the threshold
voltage is proportional to the concentration of
the analyte and is used as the response
mechanism for the gas Changes in the drain-
source current and the gate voltage have also
been used as the response mechanisms for the
MOSFET gas sensors as they are also affected
by changes in the work function (Albert and
Lewis 2000 Nagle et al 1998)
Gas sensing MOSFETs are produced by
standard microfabrication techniques which
incorporate the deposition of gas sensitive
catalytic metals onto the silicon dioxide gate
layer (Nagle et al 1998) In the case of catalytic
metals such as platinum (Pt) palladium (Pd)
and iridium (Ir) the gate material is thermally
evaporated onto the gate oxide surface through
a mask forming 100-400 nm thick films or
3-30 nm thin films depending on the application
(Albert and Lewis 2000) Thick films have
been used to detect hydrogen and hydrogen
sulphide while thin films are more porous and
can detect amines alcohols and aldehydes
(Kalman et al 2000)
Polymers have also been used as the
gate material for MOSFET gas sensors
(Hatfield et al 2000) Covington et al 2001
used three polymers (poly(ethylene-co-vinyl
acetate poly(styrene-co-butadiene)
poly(9-vinylcarbazole)) mixed with 20 per cent
carbon black which were deposited onto the
FETs using a spray system The polymer
thickness was between 19 and 37mm
respectively (Covington et al 2001) These
MOSFETs which use polymers as the sensitive
membrane are more commonly called PolFETs
and can operate at room temperature
Apart from the standard MOSFET gas
sensor architecture a hybrid suspended gate
FET (HSGFET) gas sensor can also be
fabricated by micromachining (Figure 10)
The HSGFET is a metal air-gap insulator
(MAIS) device The air-gap allows easy access
to both the gate material and the insulator so
diffusion is not necessary and therefore a wider
choice of gas sensitive materials can be used
(Eisele et al 2001 Pearce et al 2003)
The catalytic metal thickness and the
operating temperatures of the MOSFETs in
Figure 10 Hybrid suspended gate field effect transistor
Figure 9 MOSFET gas sensor with gas sensitive membrane
deposited on top of SiO2
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
192
Table
VC
hara
cter
istic
sof
com
mer
cial
e-no
ses
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Airsense
analysisGmbH
MO
S10
Food
eval
uatio
nfla
vour
and
frag
ranc
ete
stin
gA
NN
D
C
PCA
Lapt
op
ww
wa
irsen
sec
om
AlphaMOS-Multi
Organ
olepticSystem
s
CP
MO
S
QC
M
SAW
6-24
Ana
lysi
sof
food
type
squ
ality
cont
rolo
ffoo
dst
orag
efr
esh
fish
and
petr
oche
mic
alpr
oduc
ts
pack
agin
gev
alua
tion
anal
ysis
of
dairy
prod
ucts
al
coho
licbe
vera
ges
and
perf
umes
AN
N
DFA
PCA
Des
ktop
ww
wa
lpha
-mos
com
Applied
Sensor
IR
MO
S
MO
SFET
QC
M
22Id
entifi
catio
nof
purit
ypr
oces
san
dqu
ality
cont
rol
envi
ronm
enta
lan
alys
is
med
ical
diag
nosi
s
AN
N
PCA
Lapt
op
ww
wa
pplie
dsen
sorc
om
Uni
vers
ityof
Link
opin
gs
Swed
en
AromaS
canPLC
CP
32En
viro
nmen
tal
mon
itorin
gch
emic
alqu
ality
cont
rol
phar
mac
eutic
alpr
oduc
tev
alua
tion
AN
N
Des
ktop
Uni
vers
ityof
Man
ches
ter
Inst
itute
ofsc
ienc
ean
dte
chno
logy
UK
Array
Tech
QC
M8
Dia
gnos
ing
lung
canc
er
food
anal
ysis
Uni
vers
ityof
Rom
e
Bloodhoundsensors
CP
14Fo
odev
alua
tion
flavo
uran
dfr
agra
nce
test
ing
mic
robi
olog
y
envi
ronm
enta
lm
onito
ring
degr
adat
ion
dete
ctio
n
AN
N
CA
PC
A
DA
Lapt
op
Uni
vers
ityof
Leed
sU
K
Cyran
oScience
Inc
CP
32Fo
odqu
ality
ch
emic
alan
alys
is
fres
hnes
ssp
oila
ge
cont
amin
atio
nde
tect
ion
cons
iste
ncy
info
ods
and
beve
rage
s
PCA
Palm
top
ww
wc
yran
osci
ence
sco
m
Cal
iforn
iain
stitu
teof
Tech
nolo
gy
USA
MarconiApplied
Technologies
QC
M
CP
MO
SSA
W
8-28
AN
N
DA
PC
AU
nive
rsity
ofW
arw
ick
UK
ElectronicSe
nsorTechnology
Inc
GC
SA
W1
Food
and
beve
rage
qual
ity
bact
eria
iden
tifica
tion
expl
osiv
es
and
drug
dete
ctio
nen
viro
nmen
tal
mon
itorin
g
SPR
Des
ktop
ww
we
stca
lcom
Forschungszen
trum
Karlsruhe
MO
SSA
W40
8
Envi
ronm
enta
lpr
otec
tion
indu
stria
lpr
oces
sco
ntro
lai
r
mon
itorin
gin
text
ilem
ills
fire
alar
ms
Qua
lity
cont
rol
info
od
prod
uctio
nA
utom
otiv
eap
plic
atio
ns
PCA
ww
wf
zkd
eFZ
K2
engl
ish
HKR-Sen
sorsystemeGmbH
QC
M6
Food
and
beve
rage
sco
smet
ics
and
perf
umes
or
gani
c
mat
eria
ls
phar
mac
eutic
alin
dust
ry
AN
N
CA
DFA
PC
A
Des
ktop
ww
wh
kr-s
enso
rde
Tech
nica
lU
nive
rsity
ofM
unic
h
Ger
man
y
Illumina
FOndash
Life
scie
nces
fo
odpr
oces
sing
ag
ricul
ture
ch
emic
alde
tect
ion
AN
Nw
ww
illu
min
aco
mTu
fts
Uni
vers
ity
USA
(Con
tinue
d)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
SQ
CM
16-4
0Fo
odan
dbe
vera
gepr
oces
sing
per
fum
eoi
lsa
gric
ultu
ralo
dour
s
and
chem
ical
anal
ysis
pr
oces
sco
ntro
l
AN
N
PCA
Des
ktop
ww
wle
nnar
tz-e
lect
roni
cde
PDF_
docu
men
ts
Uni
vers
ityof
Tubi
ngen
Marconitechnologies
MastiffElectronic
System
sLtd
CP
16Sn
iffs
palm
sfo
rpe
rson
alid
entifi
catio
nw
ww
mas
tiffc
ouk
MicrosensorSystem
sSA
W2
Che
mic
alag
ent
dete
ctio
nch
emic
alw
arfa
re(C
W)
agen
tsan
d
toxi
cin
dust
rial
chem
ical
s(T
ICs)
anal
ysis
Palm
top
ww
wm
icro
sens
orsy
stem
sco
mp
df
hazm
atca
d
OligoSe
nse
CO
ndashA
utom
otiv
eap
plic
atio
nsf
ood
eval
uatio
npa
ckag
ing
eval
uatio
nht
tp
ww
wo
ligos
ense
be
RST
Rostock
Rau
m-fah
rtund
UmweltschatzGmbH
MO
SQ
CM
SAW
6-10
Early
reco
gniti
onof
fires
w
arni
ngin
the
even
tof
esca
peof
haza
rdou
ssu
bsta
nces
le
akde
tect
ion
wor
kpla
cem
onito
ring
AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
Table
VC
hara
cter
istic
sof
com
mer
cial
e-no
ses
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Airsense
analysisGmbH
MO
S10
Food
eval
uatio
nfla
vour
and
frag
ranc
ete
stin
gA
NN
D
C
PCA
Lapt
op
ww
wa
irsen
sec
om
AlphaMOS-Multi
Organ
olepticSystem
s
CP
MO
S
QC
M
SAW
6-24
Ana
lysi
sof
food
type
squ
ality
cont
rolo
ffoo
dst
orag
efr
esh
fish
and
petr
oche
mic
alpr
oduc
ts
pack
agin
gev
alua
tion
anal
ysis
of
dairy
prod
ucts
al
coho
licbe
vera
ges
and
perf
umes
AN
N
DFA
PCA
Des
ktop
ww
wa
lpha
-mos
com
Applied
Sensor
IR
MO
S
MO
SFET
QC
M
22Id
entifi
catio
nof
purit
ypr
oces
san
dqu
ality
cont
rol
envi
ronm
enta
lan
alys
is
med
ical
diag
nosi
s
AN
N
PCA
Lapt
op
ww
wa
pplie
dsen
sorc
om
Uni
vers
ityof
Link
opin
gs
Swed
en
AromaS
canPLC
CP
32En
viro
nmen
tal
mon
itorin
gch
emic
alqu
ality
cont
rol
phar
mac
eutic
alpr
oduc
tev
alua
tion
AN
N
Des
ktop
Uni
vers
ityof
Man
ches
ter
Inst
itute
ofsc
ienc
ean
dte
chno
logy
UK
Array
Tech
QC
M8
Dia
gnos
ing
lung
canc
er
food
anal
ysis
Uni
vers
ityof
Rom
e
Bloodhoundsensors
CP
14Fo
odev
alua
tion
flavo
uran
dfr
agra
nce
test
ing
mic
robi
olog
y
envi
ronm
enta
lm
onito
ring
degr
adat
ion
dete
ctio
n
AN
N
CA
PC
A
DA
Lapt
op
Uni
vers
ityof
Leed
sU
K
Cyran
oScience
Inc
CP
32Fo
odqu
ality
ch
emic
alan
alys
is
fres
hnes
ssp
oila
ge
cont
amin
atio
nde
tect
ion
cons
iste
ncy
info
ods
and
beve
rage
s
PCA
Palm
top
ww
wc
yran
osci
ence
sco
m
Cal
iforn
iain
stitu
teof
Tech
nolo
gy
USA
MarconiApplied
Technologies
QC
M
CP
MO
SSA
W
8-28
AN
N
DA
PC
AU
nive
rsity
ofW
arw
ick
UK
ElectronicSe
nsorTechnology
Inc
GC
SA
W1
Food
and
beve
rage
qual
ity
bact
eria
iden
tifica
tion
expl
osiv
es
and
drug
dete
ctio
nen
viro
nmen
tal
mon
itorin
g
SPR
Des
ktop
ww
we
stca
lcom
Forschungszen
trum
Karlsruhe
MO
SSA
W40
8
Envi
ronm
enta
lpr
otec
tion
indu
stria
lpr
oces
sco
ntro
lai
r
mon
itorin
gin
text
ilem
ills
fire
alar
ms
Qua
lity
cont
rol
info
od
prod
uctio
nA
utom
otiv
eap
plic
atio
ns
PCA
ww
wf
zkd
eFZ
K2
engl
ish
HKR-Sen
sorsystemeGmbH
QC
M6
Food
and
beve
rage
sco
smet
ics
and
perf
umes
or
gani
c
mat
eria
ls
phar
mac
eutic
alin
dust
ry
AN
N
CA
DFA
PC
A
Des
ktop
ww
wh
kr-s
enso
rde
Tech
nica
lU
nive
rsity
ofM
unic
h
Ger
man
y
Illumina
FOndash
Life
scie
nces
fo
odpr
oces
sing
ag
ricul
ture
ch
emic
alde
tect
ion
AN
Nw
ww
illu
min
aco
mTu
fts
Uni
vers
ity
USA
(Con
tinue
d)
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
193
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
SQ
CM
16-4
0Fo
odan
dbe
vera
gepr
oces
sing
per
fum
eoi
lsa
gric
ultu
ralo
dour
s
and
chem
ical
anal
ysis
pr
oces
sco
ntro
l
AN
N
PCA
Des
ktop
ww
wle
nnar
tz-e
lect
roni
cde
PDF_
docu
men
ts
Uni
vers
ityof
Tubi
ngen
Marconitechnologies
MastiffElectronic
System
sLtd
CP
16Sn
iffs
palm
sfo
rpe
rson
alid
entifi
catio
nw
ww
mas
tiffc
ouk
MicrosensorSystem
sSA
W2
Che
mic
alag
ent
dete
ctio
nch
emic
alw
arfa
re(C
W)
agen
tsan
d
toxi
cin
dust
rial
chem
ical
s(T
ICs)
anal
ysis
Palm
top
ww
wm
icro
sens
orsy
stem
sco
mp
df
hazm
atca
d
OligoSe
nse
CO
ndashA
utom
otiv
eap
plic
atio
nsf
ood
eval
uatio
npa
ckag
ing
eval
uatio
nht
tp
ww
wo
ligos
ense
be
RST
Rostock
Rau
m-fah
rtund
UmweltschatzGmbH
MO
SQ
CM
SAW
6-10
Early
reco
gniti
onof
fires
w
arni
ngin
the
even
tof
esca
peof
haza
rdou
ssu
bsta
nces
le
akde
tect
ion
wor
kpla
cem
onito
ring
AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
Table
V
Man
ufacturer
Sensor
type
No
of
sensors
Applications
Pattern
recognition
commen
ts
Web
sitereferen
ceuniversity
backg
round
Lennartz
ElectronicGmbH
MO
SQ
CM
16-4
0Fo
odan
dbe
vera
gepr
oces
sing
per
fum
eoi
lsa
gric
ultu
ralo
dour
s
and
chem
ical
anal
ysis
pr
oces
sco
ntro
l
AN
N
PCA
Des
ktop
ww
wle
nnar
tz-e
lect
roni
cde
PDF_
docu
men
ts
Uni
vers
ityof
Tubi
ngen
Marconitechnologies
MastiffElectronic
System
sLtd
CP
16Sn
iffs
palm
sfo
rpe
rson
alid
entifi
catio
nw
ww
mas
tiffc
ouk
MicrosensorSystem
sSA
W2
Che
mic
alag
ent
dete
ctio
nch
emic
alw
arfa
re(C
W)
agen
tsan
d
toxi
cin
dust
rial
chem
ical
s(T
ICs)
anal
ysis
Palm
top
ww
wm
icro
sens
orsy
stem
sco
mp
df
hazm
atca
d
OligoSe
nse
CO
ndashA
utom
otiv
eap
plic
atio
nsf
ood
eval
uatio
npa
ckag
ing
eval
uatio
nht
tp
ww
wo
ligos
ense
be
RST
Rostock
Rau
m-fah
rtund
UmweltschatzGmbH
MO
SQ
CM
SAW
6-10
Early
reco
gniti
onof
fires
w
arni
ngin
the
even
tof
esca
peof
haza
rdou
ssu
bsta
nces
le
akde
tect
ion
wor
kpla
cem
onito
ring
AN
N
PCA
Des
ktop
Ant
wer
pU
nive
rsity
B
elgi
um
ww
wr
st-r
osto
ckd
e
Shim
adzu
Co
MO
S6
PCA
D
eskt
op
Diag-Nose
Dia
gnos
ing
tube
rcul
osis
bo
wel
canc
ers
infe
ctio
nsin
wou
nds
and
the
urin
ary
trac
t
ww
wn
ose-
netw
ork
org
Cra
nfiel
dU
nive
rsity
B
edfo
rdsh
ire
Engl
and
Notes
MO
Sndash
met
alox
ide
sem
icon
duct
orC
Pndash
cond
uctin
gpo
lym
erQ
CM
ndashqu
artz
crys
talm
onito
rSA
Wndash
surf
ace
acou
stic
wav
eIR
ndashin
fra
red
MO
SFET
ndashm
etal
oxid
ese
mic
ondu
ctor
field
effe
ct
tran
sist
orG
Cndash
gas
chro
mat
ogra
phy
FOndash
fibre
optic
CO
ndashco
nduc
tive
olig
omer
AN
Nndash
artifi
cial
neur
alne
twor
kD
Cndash
dist
ance
clas
sifie
rsP
CA
ndashpr
inci
ple
com
pone
ntan
alys
isD
FAndash
disc
rimin
ant
func
tion
anal
ysis
C
Andash
clus
ter
anal
ysis
D
Andash
disc
rimin
ant
anal
ysis
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
194
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
Table
VI
Sum
mar
yof
the
prop
ertie
sof
each
sens
orty
pere
view
ed
Sensortype
Mea
surand
Fabrication
Exam
plesofsensitivitydetection
rangedetectionlimits(DL)
Advantages
Disad
vantages
Referen
ce
Polymer
composites
Con
duct
ivity
Scre
enpr
intin
g
spin
coat
ing
dipc
oatin
g
spra
yco
atin
g
mic
rofa
bric
atio
n
ppb
for
HV
PGpp
mfo
rLV
PG
1pe
rce
ntD
RR
bp
pm
DL
01-
5pp
m
Ope
rate
atro
omte
mpe
ratu
re
chea
pdi
vers
era
nge
of
coat
ings
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
Mun
ozet
al
(199
9)
Gar
dner
and
Dye
r(19
97)
and
Rya
net
al
(199
9)
Intrinsically
conducting
polymers
Con
duct
ivity
Elec
troc
hem
ical
chem
ical
poly
mer
isat
ion
01-
100
ppm
Sens
itive
topo
lar
anal
ytes
chea
pgo
odre
spon
setim
es
oper
ate
atro
omte
mpe
ratu
re
Sens
itive
tote
mpe
ratu
rean
d
hum
idity
su
ffer
from
base
line
drift
Nag
leet
al
(199
8)
Metal
oxides
Con
duct
ivity
Scre
enpr
intin
g
RF
sput
terin
gth
erm
al
evap
orat
ion
mic
rofa
bric
atio
n
5-50
0pp
mFa
stre
spon
sean
dre
cove
ry
times
ch
eap
Hig
hop
erat
ing
tem
pera
ture
s
suff
erfr
omsu
lphu
rpo
ison
ing
limite
dra
nge
ofco
atin
gs
Nag
leet
al
(199
8)
SAW
Piez
oele
ctric
ityPh
otol
ithog
raph
y
airb
rush
ing
scre
enpr
intin
g
dipc
oatin
gsp
inco
atin
g
1pg
to1
mg
ofva
pour
1pg
mas
s
chan
ge
DLfrac14
2pp
mfo
roc
tane
and
1pp
mN
O2
and
1pp
mH
2S
with
poly
mer
mem
bran
es
Div
erse
rang
eof
coat
ings
high
sens
itivi
ty
good
resp
onse
times
IC
inte
grat
able
Com
plex
inte
rfac
eci
rcui
try
diffi
cult
tore
prod
uce
Nag
leet
al
(199
8)
Alb
ert
and
Lew
in(2
000)
and
Penz
aet
al(
2001
a)
QCM
Piez
oele
ctric
ityM
icro
mac
hini
ng
spin
coat
ing
airb
rush
ing
inkj
etpr
intin
g
dipc
oatin
g
15
Hz
ppm
1
ngm
ass
chan
geD
iver
sera
nge
ofco
atin
gs
good
batc
hto
batc
h
repr
oduc
ibili
ty
Poor
sign
al-t
o-no
ise
ratio
com
plex
circ
uitr
y
Nag
leet
al
(199
8)an
d
Kim
and
Cho
i(2
002)
Optical
devices
Inte
nsity
spec
trum
Dip
coat
ing
Low
ppb
DL
(NH
3)frac14
1pp
mw
ith
poly
anili
neco
atin
g
Imm
une
toel
ectr
omag
netic
inte
rfer
ence
fa
stre
spon
se
times
ch
eap
light
wei
ght
Suff
erfr
omph
otob
leac
hing
com
plex
inte
rfac
eci
rcui
try
rest
ricte
dlig
htso
urce
s
Jin
etal
(2
001)
and
Nag
leet
al
(199
8)
MOSFET
Thre
shol
d
volta
ge
chan
ge
Mic
rofa
bric
atio
n
ther
mal
evap
orat
ion
28m
Vp
pmfo
rto
luen
e
DLfrac14
(am
ines
Su
lphi
des)frac14
01p
pm
Max
imum
resp
onse
frac1420
0m
V
espe
cial
lyfo
ram
ines
Smal
llo
wco
stse
nsor
sC
MO
S
inte
grat
ible
and
repr
oduc
ible
Bas
elin
edr
ift
need
cont
rolle
d
envi
ronm
ent
Cov
ingt
onet
al
(200
1)
and
Kal
man
etal
(20
00)
Notes
HV
PGndash
high
vapo
rpr
essu
rega
sLV
PGndash
low
vapo
rpr
essu
rega
sD
RR b
ndashre
lativ
edi
ffer
entia
lre
sist
ance
chan
ge
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
195
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
the e-nose arrays are altered to provide different
selectivity patterns to different gases (Schaller
et al 1998) and operating temperatures are
usually between 50 and 1708C (Kalman et al
2000)
The factors that affect the sensitivity of
FET-based devices are operating temperature
composition and structure of the catalytic metal
(Lundstrom et al 1995 Schaller et al 1998)
The temperature is increased to decrease the
response and the recovery times (Dickinson
et al 1998) Typical sensitivities of ChemFET
sensors with carbon black-polymer composite
sensitive films was found to be approximately
28mVppm for toluene vapour (Covington
et al 2001) The detection limit of MOSFET
devices for amines and sulphides was 01 ppm
with Pt Ir and Pd gates and the maximum
response was approximately 200mV especially
for amines (Kalman et al 2000) Response time
varies from device to device and response times
from milliseconds up to 300 s have been
reported in the literature (Covington et al 2001
Eisele et al 2001 Wingbrant et al 2003)
MOSFET sensors have a number of
advantages and disadvantages when used in
e-nose arrays Gas sensing MOSFETs are
produced by microfabrication therefore
reproducibility is quite good and the sensor can
be incorporated into CMOS technology
resulting in small low cost sensors (Dickinson
et al 1998 Gu et al 1998 Nagle et al 1998
Pearce et al 2003 Schaller et al 1998 )
The sensors can suffer from baseline drift and
instability depending on the sensing material
used (Nagle et al 1998) If CMOS is used the
electronic components of the chip have to be
sealed because the sensor needs a gas inlet so it
can penetrate the gate (Nagle et al 1998)
The gas flows across the sensor and also the
operating temperature have serious effects on
the sensitivity and selectivity of the sensor so
control of the surrounding environment is
important (Eklov et al 1997 Nagle et al
1998) This does not suit a handheld e-nose
Commercial e-nose systems
Manufacturers of commercial e-nose systems
have become plentiful in recent times and
produce a wide range of products utilising
different sensor types depending mainly on the
applications Many of these systems are
reviewed in Table V
Conclusions
Conducting polymer composite intrinsically
conducting polymer and metal oxide
conductivity gas sensors SAWand QCM
piezoelectric gas sensors optical gas sensors and
MOSFET gas sensors have been reviewed in this
paper These systems offer excellent
discrimination and lead the way for a new
generation of ldquosmart sensorsrdquo which will mould
the future commercial markets for gas sensors
The principle of operation fabrication
techniques advantages disadvantages and
applications of each sensor type in e-nose
systems have been clearly outlined and a
summary of this information is given inTable VI
References
Albert KJ and Lewis NS (2000) ldquoCross reactive chemicalsensor arraysrdquo Chem Rev Vol 100 pp 2595-626
Behr G and Fliegel W (1995) ldquoElectrical properties andimprovement of the gas sensitivity in multiple-dopedsno2rdquo Sensors and Actuators B Chemical Vol 26Nos 1-3 pp 33-7
Briglin SM Freund MS Tokumaru P and Lewis NS(2002) ldquoExploitation of spatiotemporal informationand geometric optimization of signalnoiseperformance using arrays of carbon black-polymercomposite vapor detectorsrdquo Sensors and Actuators BChemical Vol 82 No 1 pp 54-74
Carey PW and Kowalski BR (1986) ldquoChemicalpiezoelectric sensor and sensor array characterisationrdquoAnalytical chemistry Vol 58 pp 3077-84
Carey PW Beebe KR and Kowalski BR (1986)ldquoSelection of adsorbates for chemical sensor arrays bypattern recognitionrdquo Analytical chemistry Vol 58pp 149-53
Carey PW Beebe KR and Kowalski BR (1987)ldquoMulticomponent analysis using an array ofpiezoelectric crystal sensorsrdquo Analytical chemistryVol 59 pp 1529-34
Charlesworth JM Partridge AC and Garrard N (1997)ldquoMechanistic studies on the interactions betweenpoly(pyrrole) and orgaic vaporsrdquo J Phys ChemVol 97 pp 5418-23
Chen JH Iwata H Tsubokawa N Maekawa Y andYoshida M (2002) ldquoNovel vapor sensor from polymer-grafted carbon black effects of heat-treatment andgamma-ray radiation-treatment on the response of
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
196
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
sensor material in cyclohexane vaporrdquo PolymerVol 43 No 8 pp 2201-6
Comyn J (1985) Polymer permeability Elsevier AppliedScience Amsterdam
Corcoran P (1993) ldquoElectronic odor sensing systemsrdquoElectronics and Communication Engineering JournalVol 5 No 5 pp 303-8
Covington JA Gardner JW Briand D and de Rooij NF(2001) ldquoA polymer gate fet sensor array for detectingorganic vapoursrdquo Sensors and Actuators B ChemicalVol 77 Nos 1-2 pp 155-62
Dai G (1998) ldquoA study of the sensing properties of thin filmsensor to trimethylaminerdquo Sensors and Actuators BChemical Vol 53 Nos 1-2 pp 8-12
Dejous C Rebiere D Pistre J Tiret C and Planade R(1995) ldquoA surface acoustic wave gas sensor detectionof organophosphorus compoundsrdquo Sensors andActuators B Chemical Vol 24 Nos 1-3 pp 58-61
Dickinson TA White J Kauer JS and Walt DR (1998)ldquoCurrent trends in lsquoartificial-nosersquo technologyrdquo Trendsin Biotechnology Vol 16 No 6 pp 250-8
Doleman BJ Lonergan MC Severin EJ Vaid TP andLewis NS (1998a) ldquoQuantitative study of theresolving power of arrays of carbon black-polymercomposites in various vapor-sensing tasksrdquo AnalyticalChemistry Vol 70 No 19 pp 4177-90
Doleman BJ Sanner RD Severin EJ Grubbs RH andLewis NS (1998b) ldquoUse of compatible polymerblends to fabricate arrays of carbon black-polymercomposite vapor detectorsrdquo Analytical chemistry Vol70 pp 2560-4
Eisele I Doll T and Burgmair M (2001) ldquoLow power gasdetection with fet sensorsrdquo Sensors and Actuators BChemical Vol 78 No 1-3 pp 19-25
Eklov T Sundgren H and Lundstrom I (1997) ldquoDistributedchemical sensingrdquo Sensors and Actuators B ChemicalVol 45 No 1 pp 71-7
Fang Q Chetwynd DG Covington JA Toh C-S andGardner JW (2002) ldquoMicro-gas-sensor withconducting polymersrdquo Sensors and Actuators BChemical Vol 84 No 1 pp 66-71
Fraden J (1996) Aip Handbook of Modern Sensors AIPNew York
Freund MS and Lewis NS (1995) ldquoA chemically diverseconducting polymer based electronic noserdquo Proc NatlAcad Sci USA Vol 92 pp 2652-6
Galdikas A Mironas A and Setkus A (1995) ldquoCopper-doping level effect on sensitivity and selectivity of tinoxide thin-film gas sensorrdquo Sensors and Actuators BChemical Vol 26 No 1-3 pp 29-32
Gardner JW and Bartlett PN (1995) ldquoApplication ofconducting polymer technology in microsystemsrdquoSensors and Actuators A Physical Vol 51 No 1pp 57-66
Gardner JW and Dyer DC (1997) ldquoHigh-precisionintelligent interface for a hybrid electronic noserdquoSensors and Actuators A Physical Vol 62 No 1-3pp 724-8
George SC and Thomas S (2001) ldquoTransport phenomenathrough polymeric systemsrdquo Progress in PolymerScience Vol 26 No 6 pp 985-1017
Gopel W Hesse J and Zemel JN (Eds) (1989) MagneticSensors VCH Weinheim
Gopel W Hesse J and Zemel JN (Eds) (1992) OpticalSensors VCH Weinheim
Grate WJ and Abraham MH (1991) ldquoSolubilityinteractions and design of chemically selective sorbantcoatings for chemical sensors and arraysrdquo Sensors andActuators B Vol 3 pp 85-111
Grattan KTV and Sun T (2000) ldquoFiber optic sensortechnology an overviewrdquo Sensors and Actuators APhysical Vol 82 Nos 1-3 pp 40-61
Groves WA and Zellers ET (2001) ldquoAnalysis of solventvapors in breath and ambient air with a surfaceacoustic wave sensor arrayrdquo The Annals ofOccupational Hygiene Vol 45 No 8 pp 609-23
Gu C Sun L Zhang T Li T and Zhang X (1998) ldquoHigh-sensitivity phthalocyanine lb film gas sensor based onfield effect transistorsrdquo Thin Solid Films Vol 327-329pp 383-6
Guadarrama A Fernandez JA Iniguez M Souto J andde Saja JA (2000) ldquoArray of conducting polymersensors for the characterisation of winesrdquo AnalyticaChimica Acta Vol 411 No 1-2 pp 193-200
Hamakawa S Li L Li A and Iglesia E (2002) ldquoSynthesisand hydrogen permeation properties of membranesbased on dense srce095yb005o3-[alpha] thin filmsrdquoSolid State Ionics Vol 148 No 1-2 pp 71-81
Harsanyi G (2000) ldquoPolymer films in sensor applicationsa review of present uses and future possibilitiesrdquoSensor Review Vol 20 No 2 pp 98-105
Hatfield JV Covington JA and Gardner JW (2000)ldquoGasfets incorporating conducting polymers as gatematerialsrdquo Sensors and Actuators B ChemicalVol 65 No 1-3 pp 253-6
Haug M Schierbaum KD Gauglitz G and Gopel W(1993) ldquoChemical sensors based upon polysiloxanesComparison between optical quartz microbalancecalorimetric and capacitance sensorsrdquo Sensors andActuators B Chemical Vol 11 No 1-3 pp 383-91
Heeger AJ (2001) ldquoSemiconducting and metallic polymersthe fourth generation of polymeric materialsrdquo CurrentApplied Physics Vol 1 pp 247-67
Hierlemann A Weimar U Kraus G Schweizer-BerberichM and Gopel W (1995) ldquoPolymer-based sensorarrays and multicomponent analysis for the detectionof hazardous organic vapours in the environmentrdquoSensors and Actuators B Chemical Vol 26 Nos 1-3pp 126-34
Jin Z Su Y and Duan Y (2001) ldquoDevelopment of apolyaniline-based optical ammonia sensorrdquo Sensorsand Actuators B Chemical Vol 72 No 1 pp 75-9
Johnson DJ (1997) Process control instrumentationtechnology Prentice-Hall
Kalman E-L Lofvendahl A Winquist F and Lundstrom I(2000) ldquoClassification of complex gas mixtures fromautomotive leather using an electronic noserdquoAnalytica Chimica Acta Vol 403 No 1-2 pp 31-8
Khlebarov ZP Stoyanova AI and Topalova DI (1992)ldquoSurface acoustic wave gas sensorsrdquo Sensors andActuators B Chemical Vol 8 No 1 pp 33-40
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
197
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198
Kim YH and Choi KJ (2002) ldquoFabrication and applicationof an activated carbon coated quartz crystal sensorrdquoSensors and Actuators B Vol 87 pp 196-200
Lonergan MC Severin EJ Doleman BJ Beaber SAGrubb RH and Lewis NS (1996) ldquoArray-based vaporsensing using chemically sensitive carbon black-polymer resistorsrdquo Chemistry of Materials Vol 8 No9 pp 2298-312
Lundstrom I Ederth T Kariis H Sundgren H Spetz Aand Winquist F (1995) ldquoRecent developments infield-effect gas sensorsrdquo Sensors and Actuators BChemical Vol 23 No 2-3 pp 127-33
Matthews B Jing L Sunshine S Lerner L and Judy JW(2002) ldquoEffects of electrode configuration on polymercarbon-black composite chemical vapor sensorperformancerdquo IEEE Sensors Journal Vol 2 No 3pp 160-8
Mirmohseni A and Oladegaragoze A (2003) ldquoConstructionof a sensor for determination of ammonia and aliphaticamines using polyvinylpyrrolidone coated quartz crystalmicrobalancerdquo Sensors and Actuators B ChemicalVol 89 No 1-2 pp 164-72
Munoz BC Steinthal G and Sunshine S (1999)ldquoConductive polymer-carbon black composites-basedsensor arrays for use in an electronic noserdquo SensorReview Vol 19 No 4 pp 300-5
Nagle HT Gutierrez-Osuna R and Schiffman SS (1998)ldquoThe how and why of electronic hosesrdquo IEEESpectrum Vol 35 No 9 pp 22-31
Partridge AC Jansen ML and Arnold WM (2000)ldquoConducting polymer-based sensorsrdquo MaterialsScience and Engineering C Vol 12 No 1-2 pp 37-42
Pearce TC Schiffman SS Nagle HT and Gardner JW(2003) Handbook of Machine Olfaction Wiley-VCHWeinheim
Penza M Cassano G Sergi A Lo Sterzo C and RussoMV (2001a) ldquoSaw chemical sensing using poly-ynesand organometallic polymer filmsrdquo Sensors andActuators B Chemical Vol 81 No 1 pp 88-98
Penza M Cassano G and Tortorella F (2001b) ldquoGasrecognition by activated wo3 thin-film sensors arrayrdquoSensors and Actuators B Chemical Vol 81 No 1pp 115-21
Penza M Cassano G Tortorella F and Zaccaria G(2001c) ldquoClassification of food beverages andperfumes by wo3 thin-film sensors array and patternrecognition techniquesrdquo Sensors and Actuators BChemical Vol 73 No 1 pp 76-87
Ryan MA Buehler MG Homer ML Mannatt KSLau B Jackson S and Zhou H (1999) The SecondInternational Conference on Integrated MicroNanotechnology for Space Applications-EnablingTechnologies for New Space Systems Pasadena CAUSA
Saha M Banerjee A Halder AK Mondal J Sen A andMaiti HS (2001) ldquoEffect of alumina addition onmethane sensitivity of tin dioxide thick filmsrdquo Sensorsand Actuators B Chemical Vol 79 No 2-3 pp 192-5
Sakurai Y Jung H-S Shimanouchi T Inoguchi T MoritaS Kuboi R and Natsukawa K (2002) ldquoNovel array-type gas sensors using conducting polymers and theirperformance for gas identificationrdquo Sensors andActuators B Chemical Vol 83 No 1-3 pp 270-5
Schaller E Bosset JO and Escher F (1998) ldquoElectronicnoses and their application to foodrdquo Lebensmittel-Wissenschaft und-Technologie Vol 31 No 4pp 305-16
Schmid W Barsan N and Weimar U (2003) ldquoSensing ofhydrocarbons with tin oxide sensors possible reactionpath as revealed by consumption measurementsrdquoSensors and Actuators B Chemical Vol 89 No 3pp 232-6
Severin EJ Doleman BJ and Lewis NS (2000) ldquoAninvestigation of the concentration dependence andresponse to analyte mixtures of carbon blackinsulatingorganic polymer composite vapor detectorsrdquoAnalytical chemistry Vol 72 pp 658-68
Severin EJ Sanner RD Doleman BJ and Lewis NS(1998) ldquoDifferential detection of enantiomericgaseous analytes using carbon black-chiral polymercomposite chemically sensitive resistorsrdquo Analyticalchemistry Vol 70 pp 1440-3
Shurmer HV and Gardner JW (1992) ldquoOdourdiscrimination with an electronic noserdquo Sensors andActuators B Vol 8 pp 1-11
Sotzing GA Phend JN and Lewis NS (2000) ldquoHighlysensitive detective and discrimination of biogenicamines ulitizing arrays of polyanalinecarbon blackcomposite vapor detectorsrdquo Chem Mater Vol 12pp 593-5
Steffes H Imawan C Solzbacher F and Obermeier E(2001) ldquoEnhancement of no2 sensing properties ofin2o3-based thin films using an au or ti surfacemodificationrdquo Sensors and Actuators B ChemicalVol 78 No 1-3 pp 106-12
Tao W-H and Tsai C-H (2002) ldquoH2s sensing properties ofnoble metal doped wo3 thin film sensor fabricated bymicromachiningrdquo Sensors and Actuators B ChemicalVol 81 No 2-3 pp 237-47
Vieth WR (1991) Diffusion in and Through PolymersPrinciples and Applications Hanser Publishers Munich
Walt DR Dickinson T White J Kauer J Johnson SEngelhardt H Sutter J and Jurs P (1998) ldquoOpticalsensor arrays for odor recognitionrdquo Biosensors andBioelectronics Vol 13 No 6 pp 697-9
White NM and Turner JD (1997) ldquoThick-film sensors pastpresent and futurerdquo Meas Sci Technology Vol 8pp 1-20
Wingbrant H Lundstrom I and Lloyd Spetz A (2003) ldquoThespeed of response of MISiCFET devicesrdquo Sensors andActuators B Chemical Vol 93 Nos 1-3 pp 286-94
Yasufuku (2001) ldquoElectroconductive polymers and theirapplications in Japanrdquo IEEE Electrical InsulationMagazine Vol 17 Nos 5 pp 14-24
Zee F and Judy JW (2001) ldquoMicromachined polymer-basedchemical gas sensor arrayrdquo Sensors and Actuators BChemical Vol 72 No 2 pp 120-8
A review of gas sensors employed in electronic nose applications
K Arshak E Moore GM Lyons J Harris and S Clifford
Sensor Review
Volume 24 middot Number 2 middot 2004 middot 181ndash198
198