CHEMTCAI, SENSOR AND COATING FOR SAME
FIELD OF THE INVENTION The present invention generally relates to systems for
monitoring environmental contaminants and, more particularly, to systems
for monitoring fugitive emissions from process equipment.
BACKGROUND OF THE INVENTION
Industrial plants which handle volatile organic compounds
(VOCs) typically experience unwanted emissions of such compounds into the
atmosphere from point sources, such as smoke stacks, and non-point
sources, such as valves, pumps, and fittings installed in pipes and vessels
containing the VOCs. Such VOCs include, but are not limited to, aromatics
(e.g. , benzene, toluene, ethylbenzene, and xylenes), halogenated
hydrocarbons (e.g. , carbon tetrachloride, 1 ,1,1-trichloroethane, and
trichloroethylene), ketones (e.g. , acetone, and methyl ethyl ketone), alcohols
(e.g. , methanol, ethanol, and propanol), ethers (e.g. , dimethyl ether and
methyl t-butyl ether), and aliphatic hydrocarbons (e.g., natural gas and
gasoline).
Emissions from non-point sources, referred to as fugitive
emissions, typically occur due to the leakage of the VOCs from joints and
seals. Fugitive emissions from control valves can occur as the result of leakage through the packing between the valve stem and the body or bonnet of the valve. Valves employed in demanding service conditions involving frequent movement of the valve stem and large temperature fluctuations typically suffer accelerated deterioration of the valve stem packing, which
results in greater fugitive emissions than valves employed in less demanding
service.
While improvements in valve stem packing materials and designs have reduced fugitive emissions and lengthened the life of valve packing, the monitoring of fugitive emissions has become important as a
means to identify and reduce fugitive emissions, and to comply with the more stringent regulation of emissions. For example, the Environmental
Protection Agency (EPA) has promulgated regulations for specifying the
maximum permitted emission of certain hazardous air pollutants from
control valves, and requires periodic surveys of emissions from control
valves.
Current methods of monitoring fugitive emissions involve manual procedures using a portable organic vapor analyzer. This manual
method is time consuming and expensive to perform, and also can yield
inaccurate results due to ineffective collection of the fugitive emissions from
the equipment being monitored. If measurements are made on a valve
exposed to wind, emissions from the valve may be dissipated before the
analyzer can properly measure the concentration of the emissions. Also, if the
analyzer is not carefully moved around the valve to capture all the emissions from the valve, an inaccurate measurement will result. Manual measurement methods also require plant personnel to dedicate a significant amount of time to making the measurements, thereby distracting plant personnel from other
duties.
Automated monitoring and detection of fugitive emissions can yield significant advantages over existing manual methods. The EPA regulations require surveys of fugitive emissions at periodic intervals. The
length of the survey interval may be monthly, quarterly, semi-annually, or
annually, with the required surveys becoming less frequent if the facility operator can document a sufficiently low percentage of control valves
exhibiting excessive leakage. Thus, achieving a low percentage of leaking
valves reduces the number of surveys required per year. In a large industrial facility, where the total number of survey points can range from 50,000 to
200,000, a reduced number of surveys can result in large cost savings. By
installing automated fugitive emission-sensing systems on valves subject to the
most demanding service conditions, and thus, most likely to develop leaks,
compliance with the EPA regulations can be more readily achieved for the
entire facility.
However, employing chemical sensors in an industrial
environment requires designing sensors that perform satisfactorily in the
presence of high relative humidity over a broad temperature range. The sensors must be able to discriminate between the emissions of interest and other environmental contaminants, while retaining sufficient sensitivity to detect low concentrations of the fugitive emissions. A provision also must be made to enable periodic calibration of the sensors. The output signals from the fugitive emission sensing system must be suitable for input into plant
monitoring and control systems typically found in process plants. This permits simple and inexpensive integration of the sensing system into existing plant
process control systems.
The fugitive emission sensing system must be inexpensive to
manufacture, and use a power source that is readily available in a typical process plant in order to keep installation costs to a minimum. The system must be suitable for use in hazardous areas subject to risk of explosion- requiring electrical equipment to be intrinsically safe or of an explosion-proof design. It also must be able to operate in harsh environments, including areas
subject to spray washing, high humidity, high and low temperatures, and
vibration. The system also must be simple and reliable, in order to minimize
maintenance costs.
In certain applications, the sensors used to detect fugitive
emissions are provided in the form of piezoelectric-based sensors having high
sensitivities to surface mass changes, such that when an alternating potential is applied across the sensors, changes in resulting wave characteristics in the
sensors, specifically the resonant frequency, indicate the presence of the analyte. More specifically, the sensors typically include a quartz crystal substrate with an outer layer made of material selected to most effectively absorb the analyte. Such outer coatings are selected to increase sensitivity, while reducing acoustic wave damping effects. In addition, such materials
should be environmentally robust to accommodate the aforementioned wide
temperature ranges, humidity ranges, and high levels of dust particles and other contaminants.
SUMMARY OF THE INVENTION
In accordance with one aspect of the present invention, a
chemical sensor is provided which includes a substrate, at least two electrodes
connected to the substrate, and a coating positioned over the substrate and at
least one of the electrodes, with the coating comprising polymer beads.
In accordance with another aspect of the present invention, the
polymer beads can be (a) unmodified polymer beads such as polystyrene,
poly(2, 6-dimethyl-p-phenylene oxide), polystyrene cross-linked with
polyvinylbenzene, polystyrene butadiene, polystyrene/vinyltoluene, poly(methyl
methacrylate), poly(vinyltoluene), poly(bromostyrene),
poly(vinylbenzylchloride), poly(vinylnaphthalene), poly(butyl methacrylate), and poly(acrylic acid);
(b) modified polymer beads, such as carboxyl modified polystyrene, hydroxyl modified polystyrene, amino modified polystyrene, protein modified polymer beads, enzyme modified polymer beads, dye-immobilized polymer beads, and magnetic polymer beads; and (c) mixtures of unmodified and modified beads.
In accordance with other aspects of the present invention, the
polymer beads have a diameter of about 0.01 to about 5 microns. In preferred embodiments, the polymer beads have a glass transition temperature of about 25 °C to about 200°C. A sensor of the present invention can detect VOCs in an amount as low as 10 ppb, and operate in a temperature range of about -10°C to about 85 °C. The resulting coating has a thickness ranging from
about 0.5 microns to about 12 microns.
In accordance with yet another aspect of the present invention, a
coating is provided for an acoustic wave-based chemical sensor, wherein the coating comprises polymer beads.
These and other aspects and features of the present invention
will become more apparent from the following detailed description when taken in conjunction with the accompanying drawings.
BRTEF DESCRIPTION OF THE DRAWINGS
Fig. 1 is a block diagram of a fugitive emissions sensing system
employing the present invention;
Fig. 2 is a schematic diagram of a chemical sensor circuit including a chemical sensor embodying the present invention;
Fig. 3 is a graph showing a typical adsorption isotherm of toluene vapor on a polystyrene bead coating at 25 °C; Fig. 4 is a graph plotting the frequency shifts of a sensor built in accordance with the present invention and a sensor built using a
poly(diphenoxy phosphazene) coating vs. time upon exposure to toluene
vapor; and
Fig. 5 is a schematic diagram of an alternative embodiment of a
chemical sensor according to the present invention.
While the invention is susceptible of various modifications and
alternative constructions, certain illustrative embodiments thereof have been shown in the drawings and will be described below in detail. It should be
understood, however, that there is no intention to limit the invention to the specific forms disclosed, but on the contrary, the intention is to cover all
modifications, alternative constructions, and equivalents, falling within the spirit and scope of the invention as defined by the appended claims.
DETAILED DESCRIPTION OF THE INVENTION
Referring now to the drawings, and with specific reference to
Fig. 1, a fugitive emissions sensing system utilizing the present invention is generally depicted by reference numeral 20. However, it is to be understood
that the present invention is primarily directed to a chemical sensor 22 which
can be employed in a variety of applications, including applications separate from the fugitive emissions sensing system 20.
By way of overview, Fig. 1 is a block diagram of an illustrative fugitive emissions sensing system 20 employing the chemical sensor 22. An emission source 24 is shown, from which a sample stream 26 is drawn into sample retrieval system 28. The sample retrieval system 28 includes an
accumulator 30, a sensor chamber 32, and an ejector 34. A chemical sensor
array 36 is located within the sensor chamber 32. The sample stream 26 is
drawn from the accumulator 30 into the sensor chamber 32, exposing the
chemical sensor array 36 to the sample stream 26. The chemical sensor array 36 contains one or more chemical sensors 22 (Fig. 2). The sample stream 26
then passes into the ejector 34. A compressed air source 40 provides compressed air 42 to the ejector 34, creating a pressure drop within the ejector
34 which draws a sample stream 26 through the sensor chamber 32 and into the
ejector 34. The compressed air 42 and sample stream 26 are mixed within the
ejector 34 and exhausted to atmosphere as a mixture 44.
The chemical sensor array 36 is connected to a sensor interface
circuit 50, which processes the signals from the chemical sensor array 36 and provides process signals to a microcontroller 52. The microcontroller 52 stores
the data from the sensors 22 in a memory 54, and uses the sensor data received
from the fugitive emissions sensing system 20 to initiate control actions to
reduce or eliminate the emissions For example, the microcontroller 52 could close a valve upstream from the emissions source 24 to stop the flow of fluid through the emissions source 24 in order to stop emissions caused by the leakage of the fluid. Alternatively, the microcontroller 52 could alter operating conditions of the emissions source 24 itself to reduce or eliminate the fugitive
emissions The microcontroller 52 may use a communication interface circuit
56 to provide control signals to the upstream valve, the emission source 24, or
any other equivalent that may be used to reduce or eliminate the emissions It can therefore be seen that the fugitive emissions sensing
system 20 may be used to detect the presence of, or measure the concentration of, various types of fluids emitted from the emissions source 24. The system
may be used to detect hazardous, toxic or polluting substances emitted from
the source, or to detect leakage of non-hazardous substances, the loss of which
may be a cause of concern The fugitive emission sensing system 20 may be
used to detect emissions from any kind of source, particularly industrial process
equipment from which hazardous substances may leak. Examples include
control valves, block valves, pumps installed on lines carrying hazardous gases,
agitators, screw conveyors, or other equipment installed on process vessels containing hazardous fluids, heat exchanges, reactors, etc When emissions are detected by the fugitive emissions sensing system 20, this data may be used by
the fugitive emissions sensing system 20 to control the process in such a way as
to reduce or eliminate the emissions
As indicated above, the chemical sensor array 36 may include one or more chemical sensors 22 responsive to a particular analyte or fugitive emission being monitored. In the embodiment depicted in Fig. 2, the chemical sensor 22 is a quartz crystal microbalance (QCM) chemical sensor, but can be
another type of piezoelectric acoustic wave devices, including surface acoustic wave (SAW) devices, acoustic plate mode (APM) devices, and flexural plate
wave (FPW) devices. The sensor could also be in the form of a fiber optic sensor or electrochemical sensor.
As shown in Fig. 2, the chemical sensor 22 may be connected to
an oscillator circuit 62 for monitoring gas emissions. In an alternative embodiment, the chemical sensor 22 could be connected to a network analyzer.
More specifically, the oscillator circuit 62 may include NAND gates 64 and 66,
and an AND gate 68, connected in series. A resistor 70 may be connected
between the output of the NAND gate 66 and the circuit power supply voltage
72, and a resistor 74 may be connected between the output of NAND gate 66
and circuit power supply voltage 72 A resistor 75 may be connected across the NAND gate 64, connecting a first input to the output. A select signal 76
may be connected to the second input of the NAND gate 64, and the same
select signals may also be connected to an input of the AND gate 68. An
enable signal 78 may be connected to an input of the NAND gate 66. When
the select signal 76 and the enable signal 78 are both high, the NAND gates 64 and 66 act as high-gain inverting amplifiers and cause an oscillator 80 to
oscillate between high and low voltage, producing an oscillating square wave output. The oscillating voltage from the oscillator output 80 may be transferred through the AND gate 68 and applied across the chemical sensor 22
causing the chemical sensor 22 to physically resonate. In order to appreciate the significance of this resonance, it is first important to understand that the chemical sensor 22 utilizes the converse piezoelectric effect. By way of background, the piezoelectric effect holds that a mechanical stress applied to the surfaces of various crystals, including quartz, affords a corresponding electrical potential across the crystal having a
magnitude proportional to the applied stress. The electrical charge generated
in the quartz crystal under stress is due to the shift of dipoles resulting from the
displacement of atoms in the crystalline material. The converse piezoelectric
effect holds that application of a voltage across certain crystals, including
quartz crystals, results in a corresponding mechanical strain in the crystal. In quartz, this strain or deformation is elastic. It follows that an alternating potential across the crystal causes a vibrational motion in the quartz crystal,
i.e., the aforementioned resonance. The chemical sensor 22 therefore includes
a crystal substrate 82 which interacts with the oscillating circuit 62, and in turn
causes the oscillator circuit 62 to oscillate at the resonant frequency of the
chemical sensor 22. Thus, the frequency of the oscillator output 80 will vary as
the resonant frequency of the chemical sensor 22 varies.
The resonant frequency of the chemical sensor 22 can vary based on a number of parameters, including the mass, size, shape, and cut of the quartz crystal substrate 82 Quartz crystal exhibits a natural resonant frequency that is a function of the mass and structure of the crystal The precise size, type of cut, and thickness of the quartz crystal substrate 82 are selected to result in a particular resonant frequency For example, an AT-cut crystal with a nominal resonant frequency of 8-30 megahertz is suitable for chemical sensor applications Suitable quartz crystal substrates may be obtained from Standard Crystal Corporation of California Other types of
suitable materials to serve as the substrate include lithium niobate (LiNbO3), which is particularly suited for a surface acoustic wave (SAW) based-sensor, and aluminum nitride (A1N), which is particularly suited for a thin film resonator based-sensor
In order to apply the alternating potential across the substrate
82, first and second electrodes 84 and 86 are connected to the crystal substrate
82 and may be constructed of chromium/gold, although other suitable corrosion-resistant and acoustically compatible conductors may be used,
possibly including aluminum, palladium, chromium, gold-on-chromium, and
graphite The electrodes 84 and 86 may serve as both the conductors for
generating the alternating current across the crystal substrate 82, and as
transducers for sensing parameters related to changes in resonant frequencies resulting in the crystal substrate 82
As indicated above, the resonant frequency of the chemical sensor 22 is a function of the total mass of the device. Therefore, the mass of any coating provided around the crystal substrate 82 also affects the total mass of the device, and thereby affects the resonant frequency of the chemical sensor 22. The coatings provided about the crystal substrate 82 are selected to absorb
molecules of the analyte. When analyte molecules are absorbed by the coating, the mass of the coating is slightly increased, which in turn increases the mass of
the entire sensor 22, and thus changes the resonant frequency of the chemical
sensor 22. The resonant frequency of the chemical sensor 22 is also a function
of the viscoelastic properties of the coatings and mechanical stresses caused by temperature effects in the sensor mounting structure. However, these effects are either negligible or can be compensated for. Thus, a very sensitive gas detector may be constructed by selecting a coating that has a chemical affinity
with the particular analyte of interest. The quantity of molecules absorbed and
deposited, and the resulting change in the operating frequency of the oscillator
circuit 62, is a function of the concentration of the chemical being measured in
the environment surrounding the chemical sensor 22. The frequency changes linearly with changes in chemical concentration, within certain limits.
Thus, a change in the concentration of the analyte can be
measured by measuring the change in the frequency of the oscillator output 80.
The chemical sensor 22 can be calibrated by exposing the sensor 22 to known
concentrations of the analyte and recording the resulting frequency of the
oscillator output 80. The chemical sensor 22 then can be used to measure the absolute concentration of the analyte by comparing the measured frequency to the aforementioned recorded values.
The particular coating chosen for the crystal substrate 82 should preferably readily absorb the molecules of the analyte, to provide a high degree
of sensitivity to the analyte, but do so without damping the generated waves. The coating 88 also should be usable over a wide temperature range, and provide fast response and recovery times. The present invention provides such a coating in the form of a polymer bead coating 88.
Low glass transition temperature polymers and some materials
with low melting points are attractive as coating materials for such sensors due
to their selective, rapid, and reversible responses to volatile organic
compounds. However, low glass transition temperature polymers have low shear modulus, and therefore exhibit a relatively large damping effect on
acoustic waves. The damping or attenuation of the acoustic waves increases as
coating thickness increases, or as ambient temperature increases. This combination of features dictates that coatings of low glass transition
temperature polymers be of a limited thickness and be exposed to a limited
temperature range. However, because the chemical detection sensitivity of
acoustic wave-based sensors is generally proportional to coating thickness,
coatings of low glass transition temperature polymers, which are necessarily
thin, are accordingly limited in their detection sensitivity. The performance of
low melting point materials as coatings generally resembles that of low glass transition temperature polymers. Additionally, the operational temperature range of low melting point materials used as coatings is necessarily limited by
the low melting point. High glass transition temperature polymers exhibit characteristics generally opposite to those of low glass transition temperature polymers when used as chemical sensing coatings. More specifically, since high glass transition temperature polymers have relatively large shear moduli, they exhibit less damping or attenuating effects on acoustic waves over a wide
temperature range. Consequently, thicker coatings of high glass transition temperature polymers can be used which in turn increases sensitivity by
allowing mass uptake of the analyte. However, high glass transition
temperature polymers exhibit extremely slow and hysteresis responses unless used as very thin coatings.
The polymer bead coating 88 of the present invention preferably
utilizes a high glass transition temperature polymer to capitalize on the aforementioned acoustic wave benefits of high glass transition temperature polymers. Polymer bead coating 88 comprises small polymer beads, which
increases coating surface area, thus enabling faster responses primarily through
surface absoφtion. Moreover, the small polymer beads, and resulting high
surface area of the coating 88, enable mass uptake of large amounts of VOCs.
The polymer beads also provide detection sensitivity over a wide range of temperatures, e.g., about -10°C to about 85°C.
Many materials can be effectively employed as the polymer bead material including unmodified polymer beads and microspheres, such as, but not limited to, polystyrene (PS), poly(2, 6-dimethyl-p-phenylene oxide),
polystyrene cross-linked with polyvinylbenzene (PS/DVB), polystyrene/butadiene (PS/B), polystyrene/vinyltoluene (PS/NT), poly(methyl
methacrylate) (PMMA), poly(vinyltoluene) (PNT), poly(bromostyrene),
poly(vinylbenzylchloride), poly(vinylnaphthalene), poly butyl methacrylate),
and poly(acrylic acid). Polystyrene (PS) and poly(phenylene oxide) are preferred materials of construction of the polymer beads. Surface modified polymer beads and microspheres wherein the surfaces are modified to tailor the affinity of the analyte to the sensor also can be employed. Such modified polymer beads and microspheres include, but are not limited to, carboxy
modified polystyrene (COOH), hydroxy modified polystyrene (OH), and amino
modified polystryrene (ΝH2), protein and enzyme modified beads and
microspheres for biosensors, dye-immobilized polymer beads and microspheres
for fiber optical sensors, and magnetic beads and microspheres for magnetic
sensors. The polymer beads have a diameter of about 0.01 to about 5
microns, with a diameter of about 0.02 to about 1 micron being preferred, and
a diameter of about 0.02 to about 0.1 microns being most preferred. This small
bead size increases detection sensitivity with regard to VOCs because as the size of the polymer bead decreases, the number of beads in a given volume increases, and thus the surface area of the coating 88 increases. A large surface area allows the uptake of larger amounts of VOC vapor. For example, the coating 88 has a detection limit as low as about 10 ppb for toluene vapor at
25 °C, and an upper detection limit at the saturated vapor pressure for toluene
The polymer beads preferably have a glass transition temperature of about 25 °C to about 200 °C. The coating 88 preferably has a thickness of about 0.5
to about 12 microns. In manufacturing a sensor 22 in accordance with the present
invention, sufficient adhesion of the beads to the substrate 82 and electrodes
84, 86 is important. Conventional methods for applying coatings to sensors, such as dipping, spraying, and spin coating, are not particularly well suited to application of beads. Rather, the sensor 22 is preferably manufactured by
soaking an absorbent fabric, such as a cotton swab, in an aqueous suspension
of beads, typically at a nonlimiting concentration range of about 2 to about
10%, by weight. The beads preferably are applied to the substrate 82 and
electrodes 84 and 86 by rubbing the wet cotton swab against the substrate 82
and the electrodes 84 and 86 In this way, the beads are strongly bonded to the
substrate 82 and electrodes 84, 86, forming uniform adherent coating 88 The
uniformity of the application process was verified using various microscopic techniques including scanning electron microscopy and atomic force
microscopy. The substrate 82 and electrodes 84, 86 can be manufactured from any of the aforementioned types and materials, with a 9-10 MHZ quartz crystal substrate and gold electrodes being preferred.
The resulting coating exhibits a detection capability for toluene
in the sub ppm level, i.e., 10 ppb, at ambient temperature. Sensor response time, i.e., the time needed for the response to attain 90% of its saturation value, is about one to about nine minutes, and is preferably less than eight minutes. The operational temperature range for the sensor is about -10°C to about 85 °C. Figure 4 shows the response curves of a sensor using a polystyrene bead (PSB) coating according to the present invention, and a sensor using a
poly(diphenoxy phosphazene) (PDPP) coating. More specifically, the PSB
coating has a thickness of 8.3 microns, while the PDPP coating has a thickness
of 2.5 microns. The graph shows exposure to toluene vapor at concentration
levels of 100-1000 ppm in the presence of 40% relative humidity at 40 °C. The
data indicate that sensitivity of the PSB coating to toluene is six times larger than that of the commonly used PDPP coating. The response time of the PSB coating is longer than that of PDPP, but is orders of magnitude shorter than that of bulk polystyrene coatings with a thickness of less than 1 micron.
Fig. 3 shows a typical adsorption isotherm of toluene vapor on
the PSB coatings at 25 °C. The linear correlation between the frequency
response and the partial pressure of toluene vapor in log-log scales suggests
that the adsorption follows the Fruedlich adsoφtion isotherm. The low
detection limit for a signal to noise ratio of 5 is estimated to be about 10 ppb. The data also indicate that PSB coatings have a tendency to selectively absorb
aromatic VOCs, and are less sensitive to polar and hydrogen-bonding vapors, including ketones and alcohols. It has been found that humidity has a minimal effect on the detection of aromatic VOCs.
The sensor 22 was tested using a network analyzer. The network analyzer outputs a sine wave signal in a preprogrammed frequency
range, typically from 8.5 to 12.5 MHZ, and enables the sensor 22 to oscillate at its fundamental resonant frequency. From the signal reflected from the sensor under test, its resonant frequency, series resistance, inductance and capacitance
are extracted using the equivalent circuit analysis.
In an alternative embodiment shown in Fig. 5, a second coating
100 can be positioned over the coating 88 of polymer beads. The second
coating 100 is chosen to enhance responsiveness characteristics and detection sensitivity. For example, a second coating that is hydrophobic can reduce
interference of water vapor. A second coating that is hydrophilic or contains
tailored functional groups, such as amines, carboxylates, or OH groups, can
enhance selectivity and specificity in analyte detection. The second coating 100 may be provided at a range of thicknesses, with a thickness of about 0.2 microns to about 1.5 microns being preferred.
From the foregoing, it can therefore be seen that the present
invention provides an improved acoustic-wave based sensor having a coating of
polymer beads, preferably of a high glass transition temperature polymer. Such a coating exhibits excellent acoustic properties which tend not to damp acoustic waves even at relatively large thicknesses and elevated temperatures, and exhibits excellent responsiveness in terms of volumetric uptake capacity, response time, and reversibility.