Solucionario Teoria de Circuitos y dispositivos electrnicos 10 ed. Boylestad Nashelsky
Chapter 11 Op-Amp Applicationsdartec.com/MIC4120/CHAP11a.pdfRobert L. Boylestad and Louis Nashelsky...
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Transcript of Chapter 11 Op-Amp Applicationsdartec.com/MIC4120/CHAP11a.pdfRobert L. Boylestad and Louis Nashelsky...
Chapter 11pOp-Amp Applications
OpOp--Amp ApplicationsAmp Applications
ConstantConstant--gain multipliergain multiplierConstantConstant gain multipliergain multiplierVoltage summingVoltage summing
Voltage bufferVoltage bufferControlled sourcesControlled sources
Instrumentation circuitsInstrumentation circuitsActive filtersActive filters
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
22
ConstantConstant--Gain AmplifierGain Amplifier
Inverting VersionInverting Version
more…more…
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
33
ConstantConstant--Gain AmplifierGain Amplifier
Noninverting VersionNoninverting Version
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
44
MultipleMultiple--Stage GainsStage Gains
= AAAA 321
The total gain (3-stages) is given by:
⎟⎞
⎜⎛⎟⎞
⎜⎛⎟⎞
⎜⎛ RRR
AAAA
fff
321
or
⎟⎠⎞
⎜⎝⎛−⎟⎠⎞
⎜⎝⎛−⎟⎟⎠
⎞⎜⎜⎝
⎛+=
R3R
R2R
RR1A ff
1
f
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
55
Voltage SummingVoltage Summing
The output is the sum of individual signals times the gain:
⎟⎟⎠
⎞⎜⎜⎝
⎛++−= 3
3
f2
2
f1
1
fo V
RR
VRR
VRR
V
[Formula 14 3]
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
[Formula 14.3]
66
Voltage BufferVoltage BufferAny amplifier with no gain or loss is called a unity gain unity gain amplifieramplifier. Th d t f i it i lifiThe advantages of using a unity gain amplifier:
• Very high input impedance • Very low output impedance
Realistically these circuits
• Very low output impedance
are designed using equal resistors (R1 = Rf) to avoid problems with offset voltages.
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
77
Controlled SourcesControlled Sources
V lV l ll d lll d lVoltageVoltage--controlled voltage sourcecontrolled voltage sourceVoltageVoltage--controlled current sourcecontrolled current sourceCurrentCurrent--controlled voltage sourcecontrolled voltage sourceCurrentCurrent controlled current sourcecontrolled current sourceCurrentCurrent--controlled current sourcecontrolled current source
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
88
VoltageVoltage--Controlled Voltage SourceControlled Voltage Source
The output voltage is the gain times the Noninverting Amplifier VersionNoninverting Amplifier Versionis the gain times the input voltage. What makes an op-amp different from other
Noninverting Amplifier VersionNoninverting Amplifier Version
different from other amplifiers is its impedance characteristics and gain calculations that depend solely on external resistors.
more…more…
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
99
VoltageVoltage--Controlled Voltage SourceControlled Voltage Source
The output voltage is the gain times the Inverting Amplifier VersionInverting Amplifier Versionis the gain times the input voltage. What makes an op-amp different from other
Inverting Amplifier VersionInverting Amplifier Version
different from other amplifiers is its impedance characteristics and gain calculations that depend solely on external resistors.
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1010
VoltageVoltage--Controlled Current SourceControlled Current Source
The output current is:
11
1o kV
RV
I ==
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1111
CurrentCurrent--Controlled Voltage SourceControlled Voltage Source
This is simply another way of applying the op ampof applying the op-amp operation. Whether the input is a current determined by Vi /R1 or asdetermined by Vin/R1 or as I1:
in1
fout V
RR
V−
=
or
L1out RIV −=
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1212
CurrentCurrent--Controlled Current SourceControlled Current Source
This circuit may appear li d hmore complicated than
the others but it is really the same thing.
inin
fout V
RR
V ⎟⎟⎠
⎞⎜⎜⎝
⎛−=
R||RV
I21
ino −=
in
in
f
out
21
in
f
out
RV
RV
R||RV
RV
−=
−=
RRR
RV
I
RRRR
VI
21ino
21
21ino
⎟⎟⎠
⎞⎜⎜⎝
⎛ +−=
⎟⎟⎠
⎞⎜⎜⎝
⎛×+
−=
inf
kIRR
1II
RR
2
1o
21
=⎟⎟⎠
⎞⎜⎜⎝
⎛+−=
⎟⎠
⎜⎝
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1313
Instrumentation CircuitsInstrumentation Circuits
Some examples of instrumentation circuits using op-amps:
• Display driver• Instrumentation amplifier
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1414
Display DriverDisplay Driver
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1515
Instrumentation AmplifierInstrumentation Amplifier
For all Rs at the same value (except R ):For all Rs at the same value (except Rp):
( ) ( )2121P
o VVkVVR2R1V −=−⎟⎟
⎠
⎞⎜⎜⎝
⎛+=
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1616
Active FiltersActive FiltersAdding capacitors to op-amp circuits provides external control of the cutoff frequencies. The op-amp active filter provides controllable
ff f i d ll bl icutoff frequencies and controllable gain.
• Low-pass filter• High pass filter• High-pass filter• Bandpass filter
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1717
LowLow--Pass FilterPass Filter——FirstFirst--OrderOrder
The upper cutoff frequency d lt i i
11OH CRπ2
1f =1
fv R
R1A +=
and voltage gain are given by:
Copyright ©2009 by Pearson Education, Inc.Upper Saddle River, New Jersey 07458 • All rights reserved.
Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1818
LowLow--Pass FilterPass Filter——SecondSecond--OrderOrder
The roll-off can be made steeper by adding more RC networks.
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
1919
HighHigh--Pass FilterPass Filter
1The cutoff frequency is determined by:
11OL CRπ2
1f =
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Electronic Devices and Circuit Theory, 10/eRobert L. Boylestad and Louis Nashelsky
2020
Bandpass Bandpass FilterFilter
There are two cutoff frequencies: upper andfrequencies: upper and lower. They can be calculated using the same low-pass cutoff and high-low pass cutoff and highpass cutoff frequency formulas in the appropriate sections.pp p
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