experiment 8
DESCRIPTION
Experiment 8. * Op Amp Circuits Review * Voltage Followers and Adders * Differentiators and Integrators * Analog Computers. Op Amp Circuits Review. Inverting Amplifier Non-inverting Amplifier Differential Amplifier Op Amp Analysis. Inverting Amplifier. Non Inverting Amplifier. - PowerPoint PPT PresentationTRANSCRIPT
![Page 1: Experiment 8](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56814749550346895db486e8/html5/thumbnails/1.jpg)
Electronic InstrumentationExperiment 8
* Op Amp Circuits Review
* Voltage Followers and Adders
* Differentiators and Integrators
* Analog Computers
![Page 2: Experiment 8](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56814749550346895db486e8/html5/thumbnails/2.jpg)
Op Amp Circuits Review
Inverting Amplifier Non-inverting Amplifier Differential Amplifier Op Amp Analysis
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Inverting Amplifier
in
f
in
out
R
R
V
V
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Non Inverting Amplifier
1
1R
R
V
V f
in
out
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Differential Amplifier
in
fout
R
R
VV
V
21
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Op Amp Analysis Golden Rules of Op Amp Analysis
• 1) The current at the inputs is 0• 2) The voltage at the two inputs is the same
These are theoretical assumptions which allow us to analyze the op-amp circuit to determine what it does.
These rules essentially allow us to remove the op amp from the circuit.
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General Analysis Example(1)
Assume we have the circuit above, where Zf and Zin represent any combination of resistors, capacitors and inductors.
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We remove the op amp from the circuit and write an equation for each input voltage.
Note that the current through Zin and Zf is the same, because equation 1 is a series circuit.
General Analysis Example(2)
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Since I=V/Z, we can write the following:
But VA = VB = 0, therefore:
General Analysis Example(3)
f
outA
in
Ain
Z
VV
Z
VVI
]1
in
f
in
out
f
out
in
in
Z
Z
V
V
Z
V
Z
V
![Page 10: Experiment 8](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56814749550346895db486e8/html5/thumbnails/10.jpg)
For any op amp circuit where the positive input is grounded, as pictured above, the equation for the behavior is given by:
General Analysis Conclusion
in
f
in
out
Z
Z
V
V
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Voltage Followers and Adders
What is a voltage follower? Why is it useful? Voltage follower limitations Adders
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What is a voltage follower?
inoutBA
inBoutA
VVthereforeVV
VVVV
analysis
,
]2]1
:
1in
out
V
V
![Page 13: Experiment 8](https://reader035.vdocuments.mx/reader035/viewer/2022081419/56814749550346895db486e8/html5/thumbnails/13.jpg)
Why is it useful?
In this voltage divider, we get a different output depending upon the load we put on the circuit.
Why?
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We can use a voltage follower to convert this real voltage source into an ideal voltage source.
The power now comes from the +/- 15 volts to the op amp and the load will not affect the output.
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Voltage follower limitations Voltage followers will not work if
their voltage or current limits are exceeded.
Voltage followers are also called buffers and voltage regulators.
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Adders
12121
2
2
1
1
R
R
VV
VthenRRif
R
V
R
VRV
fout
fout
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Weighted Adders Unlike differential amplifiers, adders are
also useful when R1<>R2.
This is called a “Weighted Adder” A weighted adder allows you to combine
several different signals with a different gain on each input.
You can use weighted adders to build audio mixers and digital-to-analog converters.
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Analysis of weighted adder
I2
I1
If
2
2
1
1
2
2
1
1
2
2
1
1
2
22
1
1121
0
R
V
R
VRV
R
V
R
V
R
V
VVR
VV
R
VV
R
VV
R
VVI
R
VVI
R
VVIIII
foutf
out
BAAA
f
outA
f
outAf
AAf
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Differentiators and Integrators
Ideal Differentiator Ideal Integrator Miller (non-ideal) Integrator Comparison of Integration and
Differentiation
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Ideal Differentiator
inf
in
f
in
f
in
out CRj
Cj
R
Z
Z
V
V
analysis
1
:
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Analysis in time domain
dt
dVCRVtherefore
VVR
VV
dt
VVdCI
IIIRIVdt
dVCI
ininfout
BAf
outAAinin
RfCinfRfRfCin
inCin
,
0)(
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Problem with ideal differentiator
Circuits will always have some kind of input resistance, even if it is just the 50 ohms from the function generator.
RealIdeal
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ininin Cj
RZ
1
Analysis of real differentiator
11
inin
inf
inin
f
in
f
in
out
CRj
CRj
CjR
R
Z
Z
V
V
Low Frequencies High Frequencies
infin
out CRjV
V
ideal differentiator
in
f
in
out
R
R
V
V
inverting amplifier
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Comparison of ideal and non-ideal
Both differentiate in sloped region.Both curves are idealized, real output is less well behaved.A real differentiator works at frequencies below c=1/RinCin
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Ideal Integrator
finfinin
f
in
f
in
out
CR
j
CRjR
Cj
Z
Z
V
V
analysis
1
1
:
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Analysis in time domain
)(11
0)(
DCinfin
outinfin
out
BAoutA
fin
Ain
RinCfCf
fCfinRinRin
VdtVCR
VVCRdt
dV
VVdt
VVdC
R
VVI
IIIdt
dVCIRIV
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Problem with ideal integrator (1)
No DC offset.Works ok.
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Problem with ideal integrator (2)
With DC offset.Saturates immediately.What is the integration of a constant?
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Miller (non-ideal) Integrator
If we add a resistor to the feedback path, we get a device that behaves better, but does not integrate at all frequencies.
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Low Frequencies High Frequencies
in
f
in
f
in
out
R
R
Z
Z
V
V 0
0
inin
f
in
out
RZ
Z
V
V
inverting amplifier signal disappears
The influence of the capacitor dominates at higher frequencies. Therefore, it acts as an integrator at higher frequencies, where it also tends to attenuate (make less) the signal.
Behavior of Miller integrator
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11
1
ff
f
ff
ff
f CRj
R
CjR
CjR
Z
Analysis of Miller integrator
inffin
f
in
ff
f
in
f
in
out
RCRRj
R
R
CRj
R
Z
Z
V
V
1
Low Frequencies High Frequencies
in
f
in
out
R
R
V
V
inverting amplifier
finin
out
CRjV
V
1
ideal integrator
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Comparison of ideal and non-ideal
Both integrate in sloped region.Both curves are idealized, real output is less well behaved.A real integrator works at frequencies above c=1/RfCf
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Problem solved with Miller integrator
With DC offset.Still integrates fine.
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Why use a Miller integrator? Would the ideal integrator work on a signal with
no DC offset? Is there such a thing as a perfect signal in real
life?• noise will always be present
• ideal integrator will integrate the noise
Therefore, we use the Miller integrator for real circuits.
Miller integrators work as integrators at > c where c=1/RfCf
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Comparison Differentiaion Integration original signal
v(t)=Asin(t) v(t)=Asin(t)
mathematically
dv(t)/dt = Acos(t) v(t)dt = -(A/cos(t)
mathematical phase shift
+90 (sine to cosine) -90 (sine to –cosine)
mathematical amplitude change
1/
H(j H(j jRC H(j jRC = j/RC electronic phase shift
-90 (-j) +90 (+j)
electronic amplitude change
RC RC
The op amp circuit will invert the signal and modify the mathematical amplitude by RC (differentiator) or 1/RC (integrator)
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Analog Computers (circa. 1970)
Analog computers use op-amp circuits to do real-time mathematical operations.
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Using an Analog Computer
Users would hard wire adders, differentiators, etc. using the internal circuits in the computer to perform whatever task they wanted in real time.
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Analog vs. Digital Computers In the 60’s and 70’s analog and digital computers
competed. Analog
• Advantage: real time
• Disadvantage: hard wired
Digital• Advantage: more flexible, could program jobs
• Disadvantage: slower
Digital wins• they got faster
• they became multi-user
• they got even more flexible and could do more than just math
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Now analog computers live in museums with old digital computers:
Mind Machine Web Museum: http://userwww.sfsu.edu/%7Ehl/mmm.htmlAnalog Computer Museum: http://dcoward.best.vwh.net/analog/index.html