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FACULTY OF ELECTRICAL ENGINEERING UITM SHAH ALAM

                       CONTROL SYSTEM AND INSTRUMENTATION

                                      ( ESE439 )




                              “LIQUID LEVEL : CAPACITIVE”




               PREPAREDBY :NOORSHAFIKA MOHAMAD NAZER ( 2009710725 )

                       NORAZLIN BT MOHD. RAZALI (2009297332)

                        NUR FATTAHIAH BT HASLAHUDDIN (2009)

GROUP   : EE240 3A

        DATE         : 23 NOV 2011
Introduction

Level sensors can detect the level of substances that flow, including liquids, slurries, granular
materials, and powders. The level measurement can be either continuous or point values.
Continuous level sensors measure level within a specified range and determine the exact
amount of substance in a certain place, while point-level sensors only indicate whether the
substance is above or below the sensing point. Generally the latter detect levels that are
excessively high or low.Currently we are focusing on liquid level capacitive sensor.

Description and Figure




                                       Capacitive Sensor

The first reference to capacitive is found in Nature 1907, but the peneration today is only a
few percent of all sensor types. Capacitive sensors can directly sense a variety of thing such
as motion, chemical composition, electric field and indirectly can senses other variables
which can converted into motion or dielectric constant such as pressure, accelaration, fluid
level and fluid composition.

Capacitive sensors use the electrical property of capacitance to make measurements.
Capacitance is a property that exists between any two conductive surfaces within some
reasonable proximity. Changes in the distance between the surfaces changes the
capacitance. It is this change of capacitance that capacitive sensors use to indicate changes
in position of a target. High-performance displacement sensors use small sensing surfaces
and as result are positioned close to the targets (0.25-2 mm).
Capacitance Liquid Level




They are built with conductive sensing electrodes in a dielectric, with excitation voltages on
the order of 5V and detection circuits which turn a capacitance variation into a voltage,
frequency, or pulse width variation. This technology is low cost and stability with simple
conditioning circuits. Often, the offset and gain adjustments needed the most sensor type are
not required.

Capacitance and Distance




                                              Figure 1

Applying a voltage to conductive objects causes positive and negative chargesto collect on each
object.This creates an electric fieldin the space between the objects.



Noncontact capacitive sensors work by measuring changes in an electrical property called
capacitance. Capacitance describes how two conductive objects with a space between them
respond to a voltage difference applied to them. When a voltage is applied to the conductors,
an electric field is created between them causing positive and negative charges to collect on
each object (Fig. 1). If the polarity of the voltage is reversed, the charges will also reverse.
Figure 2

Applying an alternating voltage causes the charges to move back and forth between the objects,
creating an alternating current which is detected by the sensor.

Capacitive sensors use an alternating voltage which causes the charges to continually
reverse their positions. The moving of the charges creates an alternating electric current
which is detected by the sensor (Fig. 2). The amount of current flow is determined by the
capacitance, and the capacitance is determined by the area and proximity of the conductive
objects. Larger and closer objects cause greater current than smaller and more distant
objects. The capacitance is also affected by the type of nonconductive material in the gap
between the objects.




                                              Figure 3

Capacitance is determined by Area, Distance, and Dielectric (the material between the conductors).
Capacitance increases when Area or Dielectric increase, and capacitance decreases when the
Distance increases.

Technically, the capacitance is directly proportional to the surface area of the objects and the
dielectric constant of the material between them, and inversely proportional to the distance
between them (Fig. 3).


In typical capacitive sensing applications, the probe or sensor is one of the conductive
objects and the target object is the other. The sizes of the sensor and the target are
assumed to be constant as is the material between them. Therefore, any change in
capacitance is a result of a change in the distance between the probe and the target. The
electronics are calibrated to generate specific voltage changes for corresponding changes in
capacitance. These voltages are scaled to represent specific changes in distance. The
amount of voltage change for a given amount of distance change is called the sensitivity. A
common sensitivity setting is 1.0V/100µm. That means that for every 100µm change in
distance, the output voltage changes exactly 1.0V. With this calibration, a +2V change in the
output means that the target has moved 200µm closer to the probe.



Electric Field




                                           Figure 4

                             Capacitive sensor probe components




                                           Figure 5
                 Cutaway view showing an unguarded sensing area electric field




                                           Figure 6
           Cutaway showing the guard field shaping the sensing area electric field


When a voltage is applied to a conductor, the electric field emanates from every surface. In a
capacitive sensor, the sensing voltage is applied to the Sensing Area of the probe (Figs. 4,
5).
For accurate measurements, the electric field from the sensing area needs to be contained
within the space between the probe and the target. If the electric field is allowed to spread to
other items or other areas on the target then a change in the position of the other item will be
measured as a change in the position of the target.


A technique called “guarding is used to prevent this from happening. To create a guard, the
back and sides of the sensing area are surrounded by another conductor that is kept at the
same voltage as the sensing area itself (Fig. 4, 6).


When the voltage is applied to the sensing area, a separate circuit applies the exact same
voltage to the guard. Because there is no difference in voltage between the sensing area and
the guard, there is no electric field between them. Any other conductors beside or behind the
probe form an electric field with the guard instead of the sensing area. Only the unguarded
front of the sensing area is allowed to form an electric field with the target.


The target size is a primary consideration when selecting a probe for a specific application.
When the sensing electric field is focused by guarding, it creates a slightly conical field that is
a projection of the sensing area. The minimum target diameter for standard calibration is
30% of the diameter of the sensing area. The further the probe is from the target, the larger
the minimum target size.


In general, the maximum gap at which a probe is useful is approximately 40% of the
sensor diameter. Standard calibrations usually keep the gap considerably less than
that.

The range in which a probe is useful is a function of the size of the sensing area. The greater
the area, the larger the range. The driver electronics are designed for a certain amount of
capacitance at the probe. Therefore, a smaller probe must be considerably closer to the
target to achieve the desired amount of capacitance. The electronics are adjustable during
calibration but there is a limit to the range of adjustment.In general, the maximum gap at
which a probe is useful is approximately 40% of the sensing area diameter. Standard
calibrations usually keep the gap considerably less than that.




Using multiple probes on the same target requires that the excitation voltages be
synchronized. This is accomplished by configuring one driver as a master and others
as slaves. Frequently, a target is measured simultaneously by multiple probes. Because the
system measures a changing electric field, the excitation voltage for each probe must be
synchronized or the probes would interfere with each other. If they were not synchronized,
one probe would be trying to increase the electric field while another was trying to decrease it
thereby giving a false reading.


Driver electronics can be configured as masters or slaves. The master sets the
synchronization for the slaves in multiple channel systems.


Capacitive sensors measure all conductors: brass, steel, aluminium, or even salt-water, as
the same. The sensing electric field is seeking a conductive surface. Provided that the target
is a conductor, capacitive sensors are not affected by the specific target material. Because
the sensing electric field stops at the surface of the conductor, target thickness does not
affect the measurement. .



Measuring Non-Conductors




                                            Figure 7
 Non-conductors can be measured by passing the electric field through them to a stationary

                                   conductive target behind.




                                            Figure 8
 Without a conductive target behind, a fringe field can form through a nearby non-conductor
                            allowing the non-conductor to be sensed
Capacitive sensors are most often used to measure the change in position of a conductive
target. But capacitive sensors can be very effective in measuring presence, density,
thickness, and location of non-conductors as well. Non-conductive materials like plastic have
a different dielectric constant than air. The dielectric constant determines how a non-
conductive material affects capacitance between two conductors. When a non-conductor is
inserted between the probe and a stationary reference target, the sensing field passes
through the material to the grounded target (Fig. 7). The presence of the non-conductive
material changes the dielectric and therefore changes the capacitance. The capacitance will
change in relationship to the thickness or density of the material.


It is not always feasible to have a reference target in front of the probe. Measurements may
still be possible by a technique called fringing. If there is no conductive reference directly in
front of the probe, the sensing electric field will wrap back to the body of the probe itself. This
is called a fringe field. If a non-conductive material is brought in proximity to the probe, its
dielectric will change the fringe field; this can be used to sense the non-conductive material.
The sensitivity of the sensor to the non-conductive target is directly proportional to the
dielectric constant of the material.


Compared to other noncontact sensing technologies such as optical, laser, eddy-current, and
inductive, high-performance capacitive sensors have some distinct advantages.


       Higher resolutions including subnanometer resolutions
       Not sensitive to material changes: Capacitive sensors respond equally to all
       conductors
       Less expensive and much smaller than laser interferometers.


Meanwhile, this capacitive technology is sensitive to humidity and needs unstable, high
impedance circuits. In fact, as the dielectric constant of humid is only a few ppm higher that
dry air, humidity itself is not a problem. Very high impedance circuit needed. The capacitive
sensor are rugged as any other sensor type. Its can not tolerate immersion or condensing
humidity, but a few circuits can.

Capacitive sensors are not good choice in these conditions:


       Dirty or wet environment (eddy-current sensors are ideal)
       Large gap between sensor and target is required (optical and laser are better)
The design usually consider following steps:

       Design eletcrode plates to measure the desired variable. Maximize capacitance with
       large area, close spaced plates.
       Surround this sensor with appropriate guard or shield electrodes to handle stray
       capacitance and crosstalk from other circuits.
       Calculate sensor capacitance, stray capacitance and output signal swing.
       Specify tranfer function like Eo = C (area-linear), Eo = 1/C (spacing-linear) . Use two
       balanced capacitors for high capacitors for high accuracy with transfer function like
       C1/C2 or (C1-C2)/(C1+C2) .
       Choose an excitation frequency high enough for low noise.As excitation frequency
       increases, external and circuit generated noise decreases.
       Design circuit to meet accuracy specifications and provide immunity to environment
       challenges.
CIRCUITRY AND EQUATION

Devices that have an output in the form of a change in capacitance include a capacitive level
gauge, capacitive displacement sensor, capacitive moisture meter and capacitive
hygrometer. Capacitance is measured in unit of Farad (F). Like inductance, capacitance can
be measured accurately by an AC bridge circuit and various type of Capacitance Bridge is
available commercially.

As an example, dry leather has a loss tangent of 0.045, but with a relative humidity of 15%
the loss tangent increases to 1.4--possibly a good hygrometer. Aviation gas at 100 octane
exhibits a loss tangent at 1 kHz of 0.0001, but at 91 octane loss tangent increases to 0.0004.
Water has a high K (80) and a loss tangent which peaks at low frequencies and again at
1010 Hz. With this high dielectric activity, the loss tangent or the dielectric constant of water
can be used to detect the moisture content of materials.

Another characteristic of capacitor dielectrics which may have some use in detecting material
properties is dielectric absorption. It is measured by charging a capacitor, discharging for 10
s, and measuring the charge which reappears after 15 min. A relatively low-quality dielectric
like metalized paper has a dielectric absorption of 10%.




                          Approximate method of measuring inductance
Approximate method of measuring capacitance

As figure shown above, it consists of connecting the unknown capacitor in series with a
known resistance in a circuit excited at a known frequency. An AC voltmeter is used to
measure the voltage drop across both the resistor and the capacitor. The capacitance value
is then given by:




Where VrandVcare the voltage measured across the resistance and capacitance respectively,
f is the excitation frequency and R is the known resistance.




For non-conducting substance (less than 0.1µmho/cm3), two bare metal capacitor plates in
the form of concentric cylinder are immersed in the substances as shown below.




The substances behave as a dielectric between the plates according to the depth of the
substances. For concentric cylinder plates of radius a and b (b>a) and total height L, the
depth of the substances, h, is related to the measured capacitance C by:




where
The value of the capacitance depends on the permittivity of the liquids and that of the gas or
air above it. The total permittivity changes depending on the liquid level (for non0conducting
liquid application). In the case of conducting substance, the same measurement techniques
are applied but the capacitors plates are encapsulate in an insulating materials. The
relationship between C and h has to modify to allow for the dielectric effect of the insulator.

In a parallel plate condenser which has identical plates each of the area, A (cm3) separated
by a distance, d (cm) and insulating medium with dielectric constant K (K=1 for air) between
them, the expression for the capacitance is given by:




                                       or

Where;

A=area of plates in square inches

D=distance between the plates in inches

K=dielectric constant of material

From the equation we can observe that the capacitance varies directly with the dielectric
constant which is turn varies directly with the liquid level between the plates.

But as the plate spacing increases relative to area, more flux lines connect from the edges
and backs of the plates and the measured capacitance can be much larger than
calculated.Some other simple geometries are




                                    C = 35.4    10-12r    d
C = 55.6     10-12r    d




APPLICATIONS


Capacitive sensing is a technology based on capacitive coupling that is used in many
different types of sensors, including those to detect and measure: proximity, position or
displacement, humidity, fluid level, and acceleration. Capacitive sensing as a human
interface device (HID) technology, for example to replace the computer mouse, is growing
increasingly popular. Capacitive touch sensors are used in many devices such as laptop
track pads, digital audio players, computer displays, mobile phones, mobile devices and
others. More and more design engineers are selecting capacitive sensors for their versatility,
reliability and robustness, unique human-device interface and cost reduction over
mechanical switches.


Capacitive sensors detect anything which is conductive or has a dielectric different than that
of air. While capacitive sensing applications can replace mechanical buttons with capacitive
alternatives, other technologies such as multi-touch and gesture-based touchscreens are
also premised on capacitive sensing.These are some of the applications of capacitive
sensors that show its wide range of uses;


       Fingerprintdetectors and infrared detectors: capacitive technologies which displacing
       piezoresistance in silicon implementations ofaccelerometers and pressure sensorsare
       appearing on silicon with sensor dimensionsin the microns and electrode capacitance
       of 10 fF, with resolution to 5 aF (10-18 F)




       .
Oil refineries: Capacitive sensors used measure the percentage of water in oil.




Grain storage facilities: measure the moisture content of wheat.




Motion detectors: can detect 10-14 m displacements with good stability, high
speed,and wide extremes of environment, and capacitive sensors with large
electrodes can detect an automobile and measure its speed.




Laptop computers: thetwo-dimensional cursor controluse capacitive sensors while
transparent capacitive sensors on computer monitors.




Ice detector: Airplane wing icing can be detected using insulated metal strips in wing
leading edges.
Thickness measurement: Two plates in contact with an insulator will measure
theinsulator thickness if its dielectric constant is known, or the dielectric constant if
thethickness is known.




                             wafer thickness sensor 1



Lamp dimmer switch: The common metal-plate soft-touch lamp dimmer uses 60Hz
excitation and senses the capacitance to a human body.
Limit switch: detect the proximity of a metal machine componentas an increase in
capacitance, or the proximity of a plastic component by virtue of its increased
dielectric constant over air.




Liquid level: Capacitive liquid level detectors sense the liquid level in a reservoirby
measuring changes in capacitance between conducting plates which areimmersed in
the liquid, or applied to the outside of a non-conducting tank.
Capacitive sensor

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Capacitive sensor

  • 1. FACULTY OF ELECTRICAL ENGINEERING UITM SHAH ALAM CONTROL SYSTEM AND INSTRUMENTATION ( ESE439 ) “LIQUID LEVEL : CAPACITIVE” PREPAREDBY :NOORSHAFIKA MOHAMAD NAZER ( 2009710725 ) NORAZLIN BT MOHD. RAZALI (2009297332) NUR FATTAHIAH BT HASLAHUDDIN (2009) GROUP : EE240 3A DATE : 23 NOV 2011
  • 2. Introduction Level sensors can detect the level of substances that flow, including liquids, slurries, granular materials, and powders. The level measurement can be either continuous or point values. Continuous level sensors measure level within a specified range and determine the exact amount of substance in a certain place, while point-level sensors only indicate whether the substance is above or below the sensing point. Generally the latter detect levels that are excessively high or low.Currently we are focusing on liquid level capacitive sensor. Description and Figure Capacitive Sensor The first reference to capacitive is found in Nature 1907, but the peneration today is only a few percent of all sensor types. Capacitive sensors can directly sense a variety of thing such as motion, chemical composition, electric field and indirectly can senses other variables which can converted into motion or dielectric constant such as pressure, accelaration, fluid level and fluid composition. Capacitive sensors use the electrical property of capacitance to make measurements. Capacitance is a property that exists between any two conductive surfaces within some reasonable proximity. Changes in the distance between the surfaces changes the capacitance. It is this change of capacitance that capacitive sensors use to indicate changes in position of a target. High-performance displacement sensors use small sensing surfaces and as result are positioned close to the targets (0.25-2 mm).
  • 3. Capacitance Liquid Level They are built with conductive sensing electrodes in a dielectric, with excitation voltages on the order of 5V and detection circuits which turn a capacitance variation into a voltage, frequency, or pulse width variation. This technology is low cost and stability with simple conditioning circuits. Often, the offset and gain adjustments needed the most sensor type are not required. Capacitance and Distance Figure 1 Applying a voltage to conductive objects causes positive and negative chargesto collect on each object.This creates an electric fieldin the space between the objects. Noncontact capacitive sensors work by measuring changes in an electrical property called capacitance. Capacitance describes how two conductive objects with a space between them respond to a voltage difference applied to them. When a voltage is applied to the conductors, an electric field is created between them causing positive and negative charges to collect on each object (Fig. 1). If the polarity of the voltage is reversed, the charges will also reverse.
  • 4. Figure 2 Applying an alternating voltage causes the charges to move back and forth between the objects, creating an alternating current which is detected by the sensor. Capacitive sensors use an alternating voltage which causes the charges to continually reverse their positions. The moving of the charges creates an alternating electric current which is detected by the sensor (Fig. 2). The amount of current flow is determined by the capacitance, and the capacitance is determined by the area and proximity of the conductive objects. Larger and closer objects cause greater current than smaller and more distant objects. The capacitance is also affected by the type of nonconductive material in the gap between the objects. Figure 3 Capacitance is determined by Area, Distance, and Dielectric (the material between the conductors). Capacitance increases when Area or Dielectric increase, and capacitance decreases when the Distance increases. Technically, the capacitance is directly proportional to the surface area of the objects and the dielectric constant of the material between them, and inversely proportional to the distance between them (Fig. 3). In typical capacitive sensing applications, the probe or sensor is one of the conductive objects and the target object is the other. The sizes of the sensor and the target are assumed to be constant as is the material between them. Therefore, any change in capacitance is a result of a change in the distance between the probe and the target. The electronics are calibrated to generate specific voltage changes for corresponding changes in capacitance. These voltages are scaled to represent specific changes in distance. The amount of voltage change for a given amount of distance change is called the sensitivity. A common sensitivity setting is 1.0V/100µm. That means that for every 100µm change in distance, the output voltage changes exactly 1.0V. With this calibration, a +2V change in the
  • 5. output means that the target has moved 200µm closer to the probe. Electric Field Figure 4 Capacitive sensor probe components Figure 5 Cutaway view showing an unguarded sensing area electric field Figure 6 Cutaway showing the guard field shaping the sensing area electric field When a voltage is applied to a conductor, the electric field emanates from every surface. In a capacitive sensor, the sensing voltage is applied to the Sensing Area of the probe (Figs. 4, 5).
  • 6. For accurate measurements, the electric field from the sensing area needs to be contained within the space between the probe and the target. If the electric field is allowed to spread to other items or other areas on the target then a change in the position of the other item will be measured as a change in the position of the target. A technique called “guarding is used to prevent this from happening. To create a guard, the back and sides of the sensing area are surrounded by another conductor that is kept at the same voltage as the sensing area itself (Fig. 4, 6). When the voltage is applied to the sensing area, a separate circuit applies the exact same voltage to the guard. Because there is no difference in voltage between the sensing area and the guard, there is no electric field between them. Any other conductors beside or behind the probe form an electric field with the guard instead of the sensing area. Only the unguarded front of the sensing area is allowed to form an electric field with the target. The target size is a primary consideration when selecting a probe for a specific application. When the sensing electric field is focused by guarding, it creates a slightly conical field that is a projection of the sensing area. The minimum target diameter for standard calibration is 30% of the diameter of the sensing area. The further the probe is from the target, the larger the minimum target size. In general, the maximum gap at which a probe is useful is approximately 40% of the sensor diameter. Standard calibrations usually keep the gap considerably less than that. The range in which a probe is useful is a function of the size of the sensing area. The greater the area, the larger the range. The driver electronics are designed for a certain amount of capacitance at the probe. Therefore, a smaller probe must be considerably closer to the target to achieve the desired amount of capacitance. The electronics are adjustable during calibration but there is a limit to the range of adjustment.In general, the maximum gap at which a probe is useful is approximately 40% of the sensing area diameter. Standard calibrations usually keep the gap considerably less than that. Using multiple probes on the same target requires that the excitation voltages be synchronized. This is accomplished by configuring one driver as a master and others as slaves. Frequently, a target is measured simultaneously by multiple probes. Because the
  • 7. system measures a changing electric field, the excitation voltage for each probe must be synchronized or the probes would interfere with each other. If they were not synchronized, one probe would be trying to increase the electric field while another was trying to decrease it thereby giving a false reading. Driver electronics can be configured as masters or slaves. The master sets the synchronization for the slaves in multiple channel systems. Capacitive sensors measure all conductors: brass, steel, aluminium, or even salt-water, as the same. The sensing electric field is seeking a conductive surface. Provided that the target is a conductor, capacitive sensors are not affected by the specific target material. Because the sensing electric field stops at the surface of the conductor, target thickness does not affect the measurement. . Measuring Non-Conductors Figure 7 Non-conductors can be measured by passing the electric field through them to a stationary conductive target behind. Figure 8 Without a conductive target behind, a fringe field can form through a nearby non-conductor allowing the non-conductor to be sensed
  • 8. Capacitive sensors are most often used to measure the change in position of a conductive target. But capacitive sensors can be very effective in measuring presence, density, thickness, and location of non-conductors as well. Non-conductive materials like plastic have a different dielectric constant than air. The dielectric constant determines how a non- conductive material affects capacitance between two conductors. When a non-conductor is inserted between the probe and a stationary reference target, the sensing field passes through the material to the grounded target (Fig. 7). The presence of the non-conductive material changes the dielectric and therefore changes the capacitance. The capacitance will change in relationship to the thickness or density of the material. It is not always feasible to have a reference target in front of the probe. Measurements may still be possible by a technique called fringing. If there is no conductive reference directly in front of the probe, the sensing electric field will wrap back to the body of the probe itself. This is called a fringe field. If a non-conductive material is brought in proximity to the probe, its dielectric will change the fringe field; this can be used to sense the non-conductive material. The sensitivity of the sensor to the non-conductive target is directly proportional to the dielectric constant of the material. Compared to other noncontact sensing technologies such as optical, laser, eddy-current, and inductive, high-performance capacitive sensors have some distinct advantages. Higher resolutions including subnanometer resolutions Not sensitive to material changes: Capacitive sensors respond equally to all conductors Less expensive and much smaller than laser interferometers. Meanwhile, this capacitive technology is sensitive to humidity and needs unstable, high impedance circuits. In fact, as the dielectric constant of humid is only a few ppm higher that dry air, humidity itself is not a problem. Very high impedance circuit needed. The capacitive sensor are rugged as any other sensor type. Its can not tolerate immersion or condensing humidity, but a few circuits can. Capacitive sensors are not good choice in these conditions: Dirty or wet environment (eddy-current sensors are ideal) Large gap between sensor and target is required (optical and laser are better)
  • 9. The design usually consider following steps: Design eletcrode plates to measure the desired variable. Maximize capacitance with large area, close spaced plates. Surround this sensor with appropriate guard or shield electrodes to handle stray capacitance and crosstalk from other circuits. Calculate sensor capacitance, stray capacitance and output signal swing. Specify tranfer function like Eo = C (area-linear), Eo = 1/C (spacing-linear) . Use two balanced capacitors for high capacitors for high accuracy with transfer function like C1/C2 or (C1-C2)/(C1+C2) . Choose an excitation frequency high enough for low noise.As excitation frequency increases, external and circuit generated noise decreases. Design circuit to meet accuracy specifications and provide immunity to environment challenges.
  • 10. CIRCUITRY AND EQUATION Devices that have an output in the form of a change in capacitance include a capacitive level gauge, capacitive displacement sensor, capacitive moisture meter and capacitive hygrometer. Capacitance is measured in unit of Farad (F). Like inductance, capacitance can be measured accurately by an AC bridge circuit and various type of Capacitance Bridge is available commercially. As an example, dry leather has a loss tangent of 0.045, but with a relative humidity of 15% the loss tangent increases to 1.4--possibly a good hygrometer. Aviation gas at 100 octane exhibits a loss tangent at 1 kHz of 0.0001, but at 91 octane loss tangent increases to 0.0004. Water has a high K (80) and a loss tangent which peaks at low frequencies and again at 1010 Hz. With this high dielectric activity, the loss tangent or the dielectric constant of water can be used to detect the moisture content of materials. Another characteristic of capacitor dielectrics which may have some use in detecting material properties is dielectric absorption. It is measured by charging a capacitor, discharging for 10 s, and measuring the charge which reappears after 15 min. A relatively low-quality dielectric like metalized paper has a dielectric absorption of 10%. Approximate method of measuring inductance
  • 11. Approximate method of measuring capacitance As figure shown above, it consists of connecting the unknown capacitor in series with a known resistance in a circuit excited at a known frequency. An AC voltmeter is used to measure the voltage drop across both the resistor and the capacitor. The capacitance value is then given by: Where VrandVcare the voltage measured across the resistance and capacitance respectively, f is the excitation frequency and R is the known resistance. For non-conducting substance (less than 0.1µmho/cm3), two bare metal capacitor plates in the form of concentric cylinder are immersed in the substances as shown below. The substances behave as a dielectric between the plates according to the depth of the substances. For concentric cylinder plates of radius a and b (b>a) and total height L, the depth of the substances, h, is related to the measured capacitance C by: where
  • 12. The value of the capacitance depends on the permittivity of the liquids and that of the gas or air above it. The total permittivity changes depending on the liquid level (for non0conducting liquid application). In the case of conducting substance, the same measurement techniques are applied but the capacitors plates are encapsulate in an insulating materials. The relationship between C and h has to modify to allow for the dielectric effect of the insulator. In a parallel plate condenser which has identical plates each of the area, A (cm3) separated by a distance, d (cm) and insulating medium with dielectric constant K (K=1 for air) between them, the expression for the capacitance is given by: or Where; A=area of plates in square inches D=distance between the plates in inches K=dielectric constant of material From the equation we can observe that the capacitance varies directly with the dielectric constant which is turn varies directly with the liquid level between the plates. But as the plate spacing increases relative to area, more flux lines connect from the edges and backs of the plates and the measured capacitance can be much larger than calculated.Some other simple geometries are C = 35.4  10-12r  d
  • 13. C = 55.6  10-12r  d APPLICATIONS Capacitive sensing is a technology based on capacitive coupling that is used in many different types of sensors, including those to detect and measure: proximity, position or displacement, humidity, fluid level, and acceleration. Capacitive sensing as a human interface device (HID) technology, for example to replace the computer mouse, is growing increasingly popular. Capacitive touch sensors are used in many devices such as laptop track pads, digital audio players, computer displays, mobile phones, mobile devices and others. More and more design engineers are selecting capacitive sensors for their versatility, reliability and robustness, unique human-device interface and cost reduction over mechanical switches. Capacitive sensors detect anything which is conductive or has a dielectric different than that of air. While capacitive sensing applications can replace mechanical buttons with capacitive alternatives, other technologies such as multi-touch and gesture-based touchscreens are also premised on capacitive sensing.These are some of the applications of capacitive sensors that show its wide range of uses; Fingerprintdetectors and infrared detectors: capacitive technologies which displacing piezoresistance in silicon implementations ofaccelerometers and pressure sensorsare appearing on silicon with sensor dimensionsin the microns and electrode capacitance of 10 fF, with resolution to 5 aF (10-18 F) .
  • 14. Oil refineries: Capacitive sensors used measure the percentage of water in oil. Grain storage facilities: measure the moisture content of wheat. Motion detectors: can detect 10-14 m displacements with good stability, high speed,and wide extremes of environment, and capacitive sensors with large electrodes can detect an automobile and measure its speed. Laptop computers: thetwo-dimensional cursor controluse capacitive sensors while transparent capacitive sensors on computer monitors. Ice detector: Airplane wing icing can be detected using insulated metal strips in wing leading edges.
  • 15. Thickness measurement: Two plates in contact with an insulator will measure theinsulator thickness if its dielectric constant is known, or the dielectric constant if thethickness is known. wafer thickness sensor 1 Lamp dimmer switch: The common metal-plate soft-touch lamp dimmer uses 60Hz excitation and senses the capacitance to a human body.
  • 16. Limit switch: detect the proximity of a metal machine componentas an increase in capacitance, or the proximity of a plastic component by virtue of its increased dielectric constant over air. Liquid level: Capacitive liquid level detectors sense the liquid level in a reservoirby measuring changes in capacitance between conducting plates which areimmersed in the liquid, or applied to the outside of a non-conducting tank.