e&i _unit5 ppt
TRANSCRIPT
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UNIT-5
Primary sensing elements andsignal conditioning
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The General Measurement System (GMS)
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3
ExamplePressure Gauge
Measured Medium / Quantity:
Primary Element:
Variable Conversion Elements:
Variable Manipulation (Gain)
Data Transmission:
Data Presentation:
Air Pressure
Piston
Spring (F x)
Piston Rod
Pointer/Scale
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4
The primary sensing element
which first receives energy from the measured medium andproduces an output depending on the way of measured quantity(measurand").
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5
Signal conditioning
Signal Conditioning is the manipulation of theoutput of a sensor, probe, or transducer toperform one or more of these functions:
Signal level change - amplification orreduction
Filtering
Impedance matching A/D conversion
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Transducers Transducer
a device that converts a primary form of energy into a corresponding
signal with a different energy form
Primary Energy Forms: mechanical, thermal, electromagnetic, optical,
chemical, etc.
Sensor(e.g., thermometer) a device that detects/measures a signal or stimulus
acquires information from the real world
Actuator(e.g., heater)
a device that generates a signal or stimulus
real
world
sensor
actuator
intelligent
feedback
system
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Advantages of electrical transducers
Amplification & attenuation
Mass-inertiaeffects are minimized
Effects of frictionare minimized
Controlled using small power level
Output can be easily used ,transmittedandprocessed .
Telemetry & remote controlExplosive development in field of electronic
components and devices
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Classification of transducers
On the basis of transduction form used.
Primary & secondary transducers
Active & passive transducers
Analog & Digital transducers
Transducers & inverse transducers
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On the basis of transduction
Variation of resistance
Variation of inductance
Variation of capacitance Piezo-electric effect
Magnetostrictive effect
Elastic effect
Hall effect
Thermo electric effect
Piezo-resistive effect
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On the basis of transduction
Resistance transducers
-change in resistance due to change in physical quantity.
Example
Potentiometer
RTD
Strain gauges Photoconductive cells
Thermistor
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On the basis of transduction
Inductive transducers
-any of these quantity changes L=f(N,fr,A,L) theinductance changes.
ExampleLVDT
Synchro
Reluctance pickupEddy-current pickup
Velocity transducer
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On the basis of transduction
Capacitive Transducers
C =orA/d
Any one of these quantity changes the capacitancealso changes
Example
Variable capacitance pressure gaugeCapacitor microphone
Dielectric gauge
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Active and Passive transducers
Active transducers
-no need of any external power source
Ex:photovolatic,thermoelectric,piezoelectric
Passive transducers
Do not generate energy for conversion
Need of external power source
Types
Variable resistance
Opto electronic
Variable reactance
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Variable resistance
Photo conductors
Strain gauge
Thermistor
Opto electronic
Photo- emissive cellPhoto junctions
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Variable reactance
Inductive
Variable reluctance
Variable permeability
LvdtEddy current
Capacitive
Variable area
Variable separation
Variable permittivity
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Analog & digital transducers
Analog-output continuous function of time
Example
Thermocouple
ThermistorLVDT
Digitaloutput in pulses-discrete function of time
Digital tachometer
Push button switch
Television set tuner
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Direct and Inverse Transducers
Direct-one form to electrical
Example :microphone [sound-electrical]
Inverse-electrical into non-electrical
Example:loudspeaker[electrical-sound]
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Characteristics of transducers
Input characteristics
Type of input & operating range
Loading effects
Transfer characteristics
Transfer function Error
response of transducer to environmental influences
Output characteristics
Type of electrical output Output impedence
Useful range
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Factors influencing the choice of
transducers Operating principle
Sensitivity
Operating range
Accuracy
Error
Transient & frequency response
Loading effects
Environmental compatibility
Insensitive to unwanted signals
Usage & ruggedness Electrical aspects
Stability & reliability
Static characteristics
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Operational Amplifiers
An amplifier which not only perform amplification of signal
but also Some mathematical functions like,
adding signals
subtracting signals
integrating signals,
dttx )(The applications of operational amplifiers ( shortened
to op amp ) have grown beyond those listed above.
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Operational Amplifiers
inverting input
noninverting input
output
V-
V+
The basic op amp with supply voltage included is shown
in the diagram below.
Figure : Basic op am diagram with supply voltage and IC configuration
+
1
2
3
4
8
7
6
5
OFFSET
NULL
-IN
+IN
V
N.C.
V+
OUTPUT
OFFSET
NULL
DIP-741
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OPERATIONAL AMPLIFIER
Vd
+
Vo
Rin~inf Rout
Input 1
Input 2
+Vcc
-Vcc
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Operational Amplifier
Definition
Operational amplifier is basically a differentialamplifier whose basic function is to amplify the
difference between two input signals.op-ampalso called as difference amplifier.
Terminal ais known as inverting input terminal.
The signal which is applied at the inverting
terminal(v1) is inverted at the output.Thenegative sign indicates the polarity change atoutput
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OPERATIONAL AMPLIFIER
Terminal bis known as non-inverting input
terminal.
The signal which is applied at the non-
inverting terminal(v2) is not- inverted at the
output.The positive sign indicates the no
polarity change at output
The output voltage V out directly proportional
to the difference of the input volteges(V1~V2)
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Operational Amplifier
Operational amplifier is a direct coupled high gaindifferential input amplifier.
They are used in voltage regulators, activefilters,Instrumentation,A/D ,D/A converters
The performance of the op-amp is well controlled anddetermined by the application of negative feedback.
Usually the feedback elements are passive. So theoperation of the ckt can be made very stable.
The advantage of using differential amplifier in op-ampis due to its rejection capability of unwanted signals.
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Ref:080114HKN Operational Amplifier 27
Common-Mode and Differential
Mode Operation
+
Vo
Vi ~
Same voltage source is applied
at both terminals
Ideally, two input are equally
amplified
Output voltage is ideally zero
due to differential voltage is
zero
Practically, a small output
signal can still be measured
Note for differential circuits:
Opposite inputs : highly amplified
Common inputs : slightly amplified
Common-Mode Rejection
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Ref:080114HKN Operational Amplifier 28
Common-Mode Rejection Ratio (CMRR)
Differential voltage input :
VVVd
Common voltage input :
)(21 VVVc
Output voltage :
ccddo VGVGV Gd: Differential gain
Gc: Common mode gain
)dB(log20CMRR 10c
d
c
d
G
G
G
G
Common-mode rejection ratio:
Note:
When Gd>> Gc or CMRR
Vo= GdVd
+
NoninvertingInput
InvertingInput
Output
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Operational Amplifier 29
CMRR ExampleWhat is the CMRR?
Solution :
dBCMRRand
V(2)From
V(1)From
VV
VV
40)10/1000log(20101000
607007060
806006080
702
4010060
2
20100
60401008020100
21
21
cd
cdo
cdo
cc
dd
GG
GGV
GGV
VV
VV
+
100V
20V
80600V
+
100V
40V
60700V
(1) (2)
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Operational Amplifier 30
Op-Amp Properties(1) Infinite Open Loop gain
- The gain without feedback
- Equal to differential gain
- Zero common-mode gain
- Pratically, Gd= 20,000 to 200,000
(2) Infinite Input impedance
- Input current ii
~0A
- T-in high-grade op-amp
- m-A input current in low-grade op-
amp
(3) Zero Output Impedance
- act as perfect internal voltage source
- No internal resistance
- Output impedance in series with load
- Reducing output voltage to the load
- Practically, Rout~ 20-100
4. Bandwidth infinite
+
V1
V2 Vo
+
Vo
i1~0
i2~0
+
Rout
Vo'Rload
outload
loadoload
RR
RVV
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Operational Amplifier 31
Ideal Vs Practical Op-Amp
Ideal Practical
Open Loop gainA 105
BandwidthBW 10-100Hz
Input ImpedanceZin >1M
Output ImpedanceZout 0 10-100
Output Voltage Vout Depends onlyon Vd= (V+V)
Differential
mode signal
Depends slightly
on average input
Vc= (V++V)/2
Common-Mode
signal
CMRR 10-100dB
+
~
AVin
Vin Vout
Zout=0
I deal op-amp
+
AVinVin Vout
Zout
~
Zin
Practical op-amp
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Op-amp Amplications Voltage Comparator
digitize input
Voltage Follower
buffer
Non-Inverting Amp Inverting Amp
M O C fi i
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More Op-amp Configurations
Summing Amp
Differential Amp
Integrating Amp
Differentiating Amp
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Converting Configuration
Current-to-Voltage
Voltage-to-Current
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FILTERS
Need of filters
-eliminate unwanted signals
- to improve Sample/Noise ratio.
Purpose of filters in circuits
-to passthe signals of wanted frequencies
-to reject the signals of unwanted frequencies
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TYPES OF FILTERS
Any physical form
-mechanical,electrical,pneumatic,hydraulic
The most commonly used types are electricaltype.They are
Passive filters
Active filters
Passive filters
Filters use only passive circuit elements(R,L,C)Active filters
PE+Op-amp
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ATTENUATORS
Attenuators are devices used in bringing down
the voltage conducted between the circuits
that are connected to its input and output
Types of attenuators
resistance attenuators
symmetrical attenuators( T shape)
L type attenuators
pi type attenuators
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MODULATION
Introduction
modulation means modify or to change
The transduced signal is super-imposedon a
high frequency waveform (called carrier) .Sothat the original signal can be recovered anddisplayed.
The high frequency waveform is then said tobe modulated by the transduced signal. Theprocess of recovery is called demodulation
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MODULATION
The process of changing some characteristics(amplitude,frequency,phase) of a carrier wavein accordance with the intensity of the signal
is known as modulation.The resultant wave iscalled modulated wave.
Types of modulation
AM-Radio broadcasting
FM-television sound signal
PM
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AM
When the amplitude of high frequency carrier
waveis changed in accordance with the
intensity of the signal, it is called amplitude
modulation
Three signals
audio signal
carrier wave
modulated signal
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Modulation Factor
determines strength and quality of thetransmitted signal
It is the ratio of the amplitude change of carrierwave to normal carrier wave.
DEMODULATION
The process required for recovery of originalsignal from modulated waveform is calleddemodulation
It involves rectificationof the modulated signalfollowed by elimination of carrier frequency.
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Analog to Digital Converters
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AnalogSignals
Analog signalsdirectly measurable quantitiesin terms of some other quantity
Examples:
Thermometermercury height rises astemperature rises
Car SpeedometerNeedle moves farther
right as you accelerate StereoVolume increases as you turn the
knob.
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Digital Signals
Digital Signalshave only two states. For digital
computers, we refer to binary states, 0 and 1.
1 can be on, 0 can be off.
Examples:
Light switch can be either on or off
Door to a room is either open or closed
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Examples of A/D Applications
Microphones - take your voice varying pressure waves in the airand convert them into varying electrical signals
Strain Gages - determines the amount of strain (change indimensions) when a stress is applied
Thermocoupletemperature measuring device convertsthermal energy to electric energy
Voltmeters
Digital Multimeters
J t h t d
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Just what does an
A/D converter DO?
Converts analog signals into binary words
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AnalogDigital Conversion
2-Step Process:
Quantizing - breaking down analog value is a
set of finite states
Encoding - assigning a digital word or number
to each state and matching it to the input
signal
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Step 1: Quantizing
Example:
You have 0-10V signals.
Separate them into a set
of discrete states with1.25V increments. (How
did we get 1.25V? See
next slide)
Output
States
Discrete Voltage
Ranges (V)
0 0.00-1.25
1 1.25-2.50
2 2.50-3.75
3 3.75-5.00
4 5.00-6.25
5 6.25-7.50
6 7.50-8.75
7 8.75-10.0
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Quantizing
The number of possible states that the converter canoutput is:
N=2n
where n is the number of bits in the AD converter
Example: For a 3 bit A/D converter, N=23=8.
Analog quantization size:Q=(Vmax-Vmin)/N = (10V0V)/8 = 1.25V
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Encoding
Here we assign the
digital value (binary
number) to each state
for the computer toread.
Output
States
Output Binary Equivalent
0 000
1 001
2 010
3 011
4 100
5 101
6 110
7 111
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Accuracy of A/D Conversion
There are two ways to best improve accuracy of A/Dconversion:
increasing the resolution which improves theaccuracy in measuring the amplitude of the analogsignal.
increasing the sampling rate which increases themaximum frequency that can be measured.
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Resolution
Resolution (number of discrete values the converter can
produce) = Analog Quantization size (Q)
(Q) = Vrange / 2^n, where Vrange is the range of analog
voltages which can be represented
limited by signal-to-noise ratio (should be around 6dB)
In our previous example: Q = 1.25V, this is a high resolution. A
lower resolution would be if we used a 2-bit converter, then
the resolution would be 10/2^2 = 2.50V.
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Sampling Rate
Frequency at which ADC evaluates analog signal. As we see in
the second picture, evaluating the signal more often more
accurately depicts the ADC signal.
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Aliasing
Occurs when the input signal is changing much fasterthan the sample rate.
For example, a 2 kHz sine wave being sampled at 1.5kHz would be reconstructed as a 500 Hz (the aliasedsignal) sine wave.
Nyquist Rule: Use a sampling frequency at least twice as high as
the maximum frequency in the signal to avoidaliasing.
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Overall Better Accuracy
Increasing both the sampling rate and the resolution you
can obtain better accuracy in your AD signals.
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A/D Converter Types
Converters
Flash ADC
Delta-Sigma ADC
Dual Slope (integrating) ADC
Successive Approximation ADC
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Flash ADC
Consists of a series of comparators, each one
comparing the input signal to a unique
reference voltage.
The comparator outputs connect to the inputs
of a priority encoder circuit, which produces a
binary output
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Flash ADC Circuit
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How Flash Works
As the analog input voltage exceeds the
reference voltage at each comparator, the
comparator outputs will sequentially saturate
to a high state. The priority encoder generates a binary
number based on the highest-order active
input, ignoring all other active inputs.
Flash
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Flash
Advantages
Simplest in terms ofoperational theory
Most efficient in terms ofspeed, very fast
limited only in terms ofcomparator and gatepropagation delays
Disadvantages
Lower resolution
Expensive
For each additionaloutput bit, the number ofcomparators is doubled
i.e. for 8 bits, 256
comparators needed
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Delta Sigma ADC
Over sampled input signal
goes to the integrator
Output of integration is
compared to GND Integraters to produce a
serial bit stream
Output is serial bit stream
with # of 1s proportionalto Vin
Outputs of Delta Sigma
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p g
Sigma Delta
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Sigma-Delta
Advantages
High resolution
No precision external
components needed
Disadvantages
Slow due to oversampling
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Dual Slope Converter
The sampled signal charges a capacitor for a fixedamount of time
By integrating over time, noise integrates out of the
conversion Then the ADC discharges the capacitor at a fixed rate
with the counter counts the ADCs output bits. A longerdischarge time results in a higher count
t
VintFIX tmeas
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Dual Slope Converter
Advantages
Input signal is averaged
Greater noise immunity
than other ADC types High accuracy
Disadvantages
Slow
High precision external
components required toachieve accuracy
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Successive Approximation ADC
A Successive Approximation Register (SAR) isadded to the circuit
Instead of counting up in binary sequence,
this register counts by trying all values of bitsstarting with the MSB and finishing at the LSB.
The register monitors the comparators outputto see if the binary count is greater or lessthan the analog signal input and adjusts thebits accordingly
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Successive Approximation ADC Circuit
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Output
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Successive Approximation
Advantages
Capable of high speed andreliable
Medium accuracy compared
to other ADC types Good tradeoff between speed
and cost
Capable of outputting the
binary number in serial (onebit at a time) format.
Disadvantages
Higher resolution successiveapproximation ADCs will beslower
Speed limited to ~5Msps
ADC Types Comparison
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ADC Resolution Comparison
0 5 10 15 20 25
Sigma-Delta
Successive Approx
Flash
Dual Slope
Resolution (Bits)
Type Speed (relative) Cost (relative)
Dual Slope Slow Med
Flash Very Fast High
Successive Appox Medium Fast Low
Sigma-Delta Slow Low
ADC Types Comparison
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