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ANALOG SENSORS FOR MOTION MEASUREMENT

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Title: ANALOG SENSORS FOR MOTION MEASUREMENT


1
ANALOG SENSORS FOR MOTION MEASUREMENT
  • Presented By
  • Vikram Maduri
  • Avinash Reddy Yerva

2
TOPICS
  • Introduction
  • Motion transducers
  • Potentiometers
  • Variable inductance transducers
  • Permanent magnet transducers
  • Eddy current transducers
  • Variable capacitance transducers
  • Piezoelectric transducers
  • Design criterion for control systems

3
INTRODUCTION
  • Measurement of plant outputs and feedback signals
    are very important.
  • The measurement subsystem in a control system
    contains sensors and transducers that detect
    measurands and convert them into acceptable
    signals- typically voltages
  • Sensor A device for measuring some quantity. The
    sensor usually converts the measurement space to
    an electrical signal.
  • Transducer It is a device, that converts one
    type of energy to another.
  • Transducers are used for compensation in
    different plants and systems.
  • Help in reducing the sensitivity of a system to
    parameter change.
  • Several analog sensor-transducer devices are
    commonly used in control system instrumentation
  • We will deal with several analog motion
    transducers.

4
MOTION TRANSDUCERS
  • Motion here means the four kinematics variables
  • Displacement
  • Velocity
  • Acceleration
  • Jerk
  • Each variable is a time derivation of the
    preceding one.
  • Motion measurement is extremely important for
    systems or plant proper functioning.

5
Examples
  • Proximity sensors (to measure displacement) and
    accelerometers are the two most common types of
    measuring devices used in machine protection
    systems for condition monitoring, fault
    detection, control of large machinery.
  • Strain gages are used in measuring strains, they
    can be adopted to measure displacement by using
    auxiliary sensor element i.e. cantilever
    (spring), Resolver provides angular displacement.
  • Pulse generating transducers like digital
    tachometers can serve as both displacement and
    velocity transducer depending on absolute number
    of pulses generated is counted or the pulse rate
    is measured.

6
Motion Transducers
  • Motion transducers will be limited mainly to
    following types of devices
  • Potentiometers
  • Variable inductance transducers
  • Eddy current transducers
  • Variable capacitance transducers
  • Piezoelectric transducers

7
Potentiometers
  • Uniform coil of wire or a film of high resistive
    material carbon, platinum or conductive plastic
  • Resistance is proportional to its length.

Resistive

Element

Wiper

Arm

v




ref

v
x
ref

v
(Supply)

Load


o

(Measurand)
v

Z


(Measurement)


Impedance

o


i


i

-
-
No Current

Nonzero

Current

FIG 1
FIG 2
  • Slider displacement x is proportional to the
    output voltage

8
  • This relationship is valid only if the output
    terminals are open circuit (no current) as shown
    in FIG 1.
  • The output voltage drops when a load with a
    finite impedance is connected which is shown in
    FIG 2.
  • Because of this loading effect the linear
    relationship will no longer be valid
  • Loading can also affect the supply (reference)
    voltage
  • To minimize loading effects
  • Use a stabilized power supply with low output
    impedance
  • Signal conditioning circuitry with high input
    impedance
  • An element with high resistance will have reduced
    power dissipation and less thermal effects
  • However, increased resistance increases the
    output impedance resulting in loading
    non-linearity error
  • FIG 3 shows the linear motion of the translatory
    potentiometer whereas the FIG 4 shows the angular
    motion of Rotatory potentiometer.

9
Translatory and Rotatory potentiometers
Resistive Element
(Measurand)
vo (output)
Wiper
Wiper
vo (output)
x (Measurand)
vref
FIG 3
Translatory for Rectilinear Motions
vref
FIG 4
Rotatory for Angular Motions
10
VARIABLE-INDUCTANCE TRANSDUCERS
  • These motion transducers employ the principle of
    electromagnetic induction
  • Types of variable inductance transducers include
  • Mutual induction transducers
  • Self-induction transducers
  • Permanent magnet transducers
  • An AC excitation in the primary winding induces
    an AC voltage in the secondary winding as
    indicated in FIG 5.
  • The amplitude of the induced voltage depends on
    the flux linkage between the two coils
  • In mutual induction transducers change in the
    flux is effected by either
  • Moving a ferromagnetic material on the flux path
    LVDT, RVDT, mutual induction proximity probe
  • Moving one coil with respect to the other
    resolver, synchro-transformer

FIG 5
11
MUTUAL INDUCTANCE TRANSDUCER(Linear variable
differential transformer (LVDT))
  • An LVDT transducer shown in FIG 6 comprises a
    coil former on to which three coils are wound.
  • The primary coil is excited with an AC current,
    the secondary coils are wound such that when a
    ferrite core is in the central linear position,
    an equal voltage is induced in to each coil.
  • The secondary are connected in opposite so that
    in the central position the outputs of the
    secondary cancels each other out.

FIG 6
12
LINEAR VARIABLE DIFFERENTIAL TRANSFORMER
  • When the armature is in the central position
    there is an equal voltage induced in to both
    secondary coils. The sum of secondary outputs
    cancels each other out resulting in a zero
    output.
  • As the armature moves in to sec1,the result is
    that sum of sec1 and sec2 favors sec1.
  • As the armature moves in to sec2,the sum favors
    sec2.
  • The output is an AC waveform
  • which is indicated in FIG 7

FIG 7
13
LINEAR VARIABLE DIFFERENTIAL TRANSFORMER
  • Signal conditioning associated with differential
    transformers includes rectification and
    demodulation.
  • FIG 8 shows Rectification.
  • FIG 9 shows Demodulation.

FIG 8
FIG 9
14
Self Induction Transducers
  • Based on the principle of self induction.
  • Only a single coil is employed as shown in FIG
    10.
  • Self Induction transducers are usually
    variable-reluctance devices.
  • This can be used as a displacement sensor

FIG 10
15
Permanent Magnet Transducers
  • A permanent magnet is used to generate a uniform
    and steady magnetic field.
  • Permanent magnet transducers are used in
    measuring speed.
  • Two types of speed are measured.
  • Rectilinear speed
  • Rectilinear velocity transducer shown in FIG 11
    is used to measure rectilinear speed
  • Angular speed.
  • DC tachometer-generator in FIG 12 and AC
    tachometer-generator are used in measuring
    angular speed.

16
  • Rectilinear velocity transducer

DC Tachometer-generator
FIG 12
FIG 11
17
Eddy Current Transducers
  • Principle of Eddy current
  • An eddy current is caused by a moving magnetic
    field intersecting a conductor or vice-versa.
  • The relative motion causes a circulating flow of
    electrons, or current, within the conductor.
  • These circulating eddies of current create
    electromagnets with magnetic fields that oppose
    the change in the external magnetic field.
  • The stronger the magnetic field, or greater the
    electrical conductivity of the conductor, the
    greater the currents developed and the greater
    the opposing force.
  • This principle is used in eddy current proximity
    sensor
  • FIG 13 illustrates concept of Eddy current

FIG 13
18
Eddy current proximity sensor
  • The Eddy Current Transducer uses the effect of
    eddy (circular) currents to sense the proximity
    of non-magnetic but conductive materials.
  • A typical eddy current transducer contains two
    coils an active coil (main coil) and a balance
    coil as shown in FIG 14.
  • The active coil senses the presence of a nearby
    conductive object, and balance coil is used to
    balance the output bridge circuit and for
    temperature compensation.

FIG 14
19
Schematic diagram of eddy current proximity sensor
  • FIG 15
  • Active coil and compensating coil forms arms of
    inductance bridge.
  • When a measurand brought to near to active coil,
    due to eddy current which produces eddy current
    magnetic field that opposes active coil field
    causes change in inductance and thus creates
    imbalance in inductance bridge.
  • This change is noted in calibrated unit.

20
Variable capacitance transducers
  • A variable capacitor is a capacitor whose
    capacitance may be intentionally and repeatedly
    changed mechanically or electronically.
  • Capacitance of two plate capacitor is given by
  • CKA / x
  • A change in anyone of K,A,x may be used in
    sensing process.
  • Variable capacitance is used to convert physical
    phenomena into electrical signals
  • Types of capacitor sensors
  • capacitive rotation sensor
  • capacitive displacement sensor
  • capacitive liquid level sensor

21
Variable capacitance transducers
  • Capacitive rotation sensor
  • Angular displacement of one of the plates
    causes the a change in A (area of plate) which is
    shown in FIG 16.

FIG 16
22
Variable capacitance transducers
  • Capacitive Displacement sensor
  • Transverse displacement of one of the plates
    changes x (distance between plates) as shown in
    FIG 17.

FIG 17
23
Variable capacitance transducers
  • Capacitive liquid level sensor
  • A change in K (depends on dielectric
    properties of medium between two plates) is
    produced as the fluid level between the capacitor
    plate changes
  • The advantage of capacitance transducer is
    negligible loading effects.
  • FIG 18 shows change in K value used to measure
    the displacement

FIG 18
24
Piezoelectric transducers
  • Piezoelectric materials Barium titanate, single
    crystal quartz.
  • Piezoelectric Effect
  • When mechanical stress or strain is applied to
    the piezoelectric material, generates an electric
    charge and associated potential difference.
  • The direct application of piezoelectric effect is
    used in pressure and strain measuring devices

25
The Piezoelectric Effect
Crystal material at rest No forces applied (as
shown in FIG 19), so net current flow is 0
Crystal
- - -
Current Meter 0
Charges cancel each other, so no current flow
- - -
FIG 19
26
The Piezoelectric Effect
Crystal material with forces applied in
direction of arrows (FIG 20).
Crystal
- - -
Current Meter deflects in direction
Force

Due to properties of symmetry, charges are net
on one side net - on the opposite side
crystal gets thinner and longer
FIG 20
27
The Piezoelectric Effect
Changing the direction of the applied
force..(FIG 21)
Crystal

Current Meter deflects in - direction
Force
- - - - -
. Changes the direction of current flow, and
the crystal gets shorter and fatter.
FIG 21
28
Piezoelectric accelerometer
  • Piezoelectric velocity transducer
  • It uses piezoelectric accelerometer and an
    integrating amplifier along with impedance
    matching amplifier which is show in FIG 22.
  • Piezoelectric displacement transducer
  • It is obtained by using a double integration of
    piezoelectric accelerometer.

FIG 22
29
Piezoelectric Sensor
  • It may be represented as a charge source with a
    series capacitive impedance Z as shown in FIG 23
  • Z 1/jwc
  • Piezoelectric sensors have a limitation on the
    useful lower frequency.

Fig 23
30
Piezoelectric accelerometer
  • Accelerometers are acceleration measuring
    devices.
  • The piezoelectric accelerometer is a
    piezoelectric motion transducer.
  • It is based on d Alemberts principle which
    states that
  • If a force of magnitude Ma were applied to the
    accelerating mass in the direction opposing the
    acceleration, then the system could be analyzed
    using static equilibrium considerations.

FIG 24
31
DESIGN CRITERION FOR CONTROL SYSTEM
  • Accuracy is affected by parameter changes in the
    control system components and by the influence of
    external disturbances
  • Consider general feedback control as shown in FIG
    25 system to parameter changes and to external
    disturbances.
  • GP(s) Transfer function of the plant ( Of the
    system to be controlled)
  • Gc(s) Transfer function of the controller (
    Including Compensators)
  • H(s) Transfer function of the output feedback
    system ( Including the measurement system)
  • u System input command
  • ud External disturbance input
  • y system output

FIG 25
32
  • After analyzing the feedback back control system
    we can stipulate the following design criterion
    for the system.
  • Make the measurement system (H) very accurate and
    stable
  • Increase the loop gain to reduce the sensitivity
    of the control system to changes in the plant and
    controller .
  • Increase the gain of GcH to reduce the influence
    of external disturbances

33
Conclusion
  • Analog Transducers play a very important part in
    insuring proper functioning of the systems.
  • They are simple, user friendly and reliable.
  • But with increase in complexity and need for
    accuracy in modern day plants use of analog
    transducers is very limited. Newly developed
    Digital and Optical Transducers are more apt for
    use in these plants.

34
References
  • Sensors and Actuators by C W Desilva.
  • http//en.wikipedia.org/wiki/Sensor
  • http//en.wikipedia.org/wiki/Eddy_current
  • http//www.infoplease.com/ce6/sci/A0839004.html
  • http//www.encyclopedia.com/doc/1E1-piezoele.html

35
Discussions
  • Discuss briefly Eddy current Proximity sensor.
  • How does linear displacement is measured using
    potentiometer ?
  • Explain how different motions are measured using
    Variable capacitance transducers ?

36
Questions and comments
37
  • Thanks to one and everyone
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