SlideShare a Scribd company logo
Lab 8
Experiment 17
A Differentiator Circuit
Note Comment in Lab Manual
• All of the diagrams use a uA741 op amp.
– You are to construct your circuits using an
LM 356 op amp.
• There is a statement that values for R1, R2, and
C2 should be limited by what is in your kit.
– You may combine multiple resistors (capacitors) to
obtain a desired resistance (or capacitance).
Ideal Circuit
Capacitors
)
(
)
(
1
)
(
)
(
1
o
C
t
t
C
C
C
C
t
v
dt
t
i
C
t
v
dt
dv
C
t
i
o




iC
i = 0
iR iR + iC + i =0
where i = 0mA
iC =C1 dV3/dt
iR = [0V – Vo]/R1
Vo = -R1C1 dV3/dt
Practical Circuit
Why Two Different Circuits
• If the input contains electronic noise with high
frequency components, the magnitude of the
high frequency components will be amplified
significantly over the signal of interest and the
system likely will become unstable.
– It is thus necessary to modify the circuit to reduce
or eliminate such effects.
Modifications to Ideal Circuit
• Two modifications to the circuit – both of which
results in the formation of frequency filters.
– First, a series resistor is inserted before the negative
input terminal of op amp. The effect of this resistor is
to act as an attenuator for the high frequency
components.
– Second, a capacitor is placed in the feedback network.
This capacitor provides more feed-back for the high
frequency components than for the low frequency
components and also acts to stabilize the circuit.
Practical Circuit
Capacitors
)
(
)
(
1
)
(
)
(
1
o
C
t
t
C
C
C
C
t
v
dt
t
i
C
t
v
dt
dv
C
t
i
o




From these equations:
• When the voltage across the capacitor doesn’t
change (i.e., d.c. voltage), the capacitor’s current
is equal to zero.
– The capacitor acts like an open circuit.
• When the voltage across the capacitor is
changing rapidly (e.g., high frequency sine wave),
the capacitor’s current is large and also changes
with time.
– The capacitor acts like a short circuit. The current
through the circuit is limited by the other components
in the circuit (i.e., the resistors).
Practical Circuit
R2 with C1 forms a high pass filter.
If V3 is a d.c. voltage source, C1 acts like an open circuit
and all of the input voltage (V3) is dropped across the
capacitor (VC1) and the current through R2 and C1 will
be determined primarily by the first derivative of the
V3.
If V3 is a high frequency a.c. voltage source, C1 acts like
a short circuit and the current through R2 and C1 will
be determined primarily by V3 divided by R2.
Practical Circuit
R1 with C2 forms a low pass filter.
If the difference in the voltage between the negative input
terminal on the op amp and Vo is relatively constant, C1
acts like an open circuit and all of the current through R2
and C1 will flow through R1.
If the difference in the voltage between the negative input
terminal on the op amp and Vo varies a lot with time, C1
acts like a short circuit and all of the current through R2
and C1 will flow through C2 and the output voltage will be
approximately equal to the voltage on the negative input
terminal, which will be 0 V.
Operation as a Function of Frequency
Design Constraints
f
C
R
C
R
C
R
C
R
f
C
R
f
C
R
f
unity
H
C






2
1
1
1
2
1
2
1
and
2
1
2
1
1
2
1
1
1
1
2
1
1
2







Design Constraints
F
C
Hz
f
Hz
f
Hz
f
unity
H
C

1
.
0
1500
5000
3000
1 



dB
• dB is an abbreviation for decibels
V
V
log
20
dB
P
P
log
10
dB
in
out
in
out


















0.707
2
2
V
V
when
occurs
3dB
-
2
1
P
P
when
occurs
3dB
-
in
out
in
out



















Follow the Directions in the Lab
Manual
• Except:
– Use the function generator on the Velleman
oscilloscope
• Remember that you have to set the Amplitude to 10V to
have 5V sin(t) outputted.
– Do not use the 10X probes with the Velleman
oscilloscope when performing the oscilloscope
measurements.
• Just use the standard BNC-to-alligator or BNC-to-IC clip
cables.
– All plots should be made using MatLAB.
PSpice Simulation:
AC Sweep
Differentiator Gain Integrator
Phase Shift
--Dt --












2
f
1
T
is
wave
sine
the
of
period
the
where
degrees
360
angle.
phase
the
is
where
)
sin(
)
90
sin(
)
cos(
)
sin(


D
-






T
t
t
t
t
dt
t
d o
Measurement of Phase Angle
• There are two sets of instructions in the Lab 8
folder under resources
– Phase Delay.pdf, which explains how to make a phase
angle calculation using the information displayed
when the Oscilloscope function of the Velleman
oscilloscope is used.
• You should become familiar with this technique.
– Magnitude and Phase.pdf, which explains how to use
the automated measurement tools on the Velleman
scope to obtain the magnitude and phase of a signal
at a single frequency and over a range of frequencies.
Phase Shift as a Function of Frequency
• The phase shift between the input voltage and
the output voltage of the op amp will change
from 90o to 180o to 270o as the operation of
the circuit changes from a differentiator to
inverting amplifier to integrator.
Caution:
PSpice Transient Analysis Issue
Information in first half cycle is incorrect because
the initial charge on the capacitor is zero.

More Related Content

PPT
Differentiator
PDF
Oscillators
PDF
Analog and Digital Electronics Lab Manual
PPTX
Engeneering Model Traffic Lights Circuit
PPTX
Testing
PPT
08_electronics.basics and introduction12
PPT
08_electronics.basics and introduction23
PPTX
UNIT-3 OPAMP.pptx
Differentiator
Oscillators
Analog and Digital Electronics Lab Manual
Engeneering Model Traffic Lights Circuit
Testing
08_electronics.basics and introduction12
08_electronics.basics and introduction23
UNIT-3 OPAMP.pptx

Similar to Differentiator.ppt (20)

PPT
BJT Amplifiers it works on bjt circuits.
DOCX
Electronic circuit design lab manual
PDF
Transistors handout
PDF
Electrónica: Probador de LOPT/FBT Flyback
PDF
PDF
NEET coaching class in Mumbai
PPT
Ajal op amp
PPT
Ch2.ppt
PPT
Bjt amplifiers
PPTX
Operational Amplifire.pptx
PPTX
project
PDF
5 experiment -_characteristics_of_bipolar_junction_transistors
PPTX
10 lm 555 timer
PPTX
oscillators.pptx
PPTX
Voltage Controlled Oscillator Design - Short Course at NKFUST, 2013
PPTX
High-Efficiency RF Power Amplifiers.pptx
PDF
Lic lab manual
PDF
Electric+Circuit+and+Simulation+Op+amp.pdf
PPT
Power supplies without transformers lightweight
DOCX
Assignment 1 Description Marks out of Wtg() Due date .docx
BJT Amplifiers it works on bjt circuits.
Electronic circuit design lab manual
Transistors handout
Electrónica: Probador de LOPT/FBT Flyback
NEET coaching class in Mumbai
Ajal op amp
Ch2.ppt
Bjt amplifiers
Operational Amplifire.pptx
project
5 experiment -_characteristics_of_bipolar_junction_transistors
10 lm 555 timer
oscillators.pptx
Voltage Controlled Oscillator Design - Short Course at NKFUST, 2013
High-Efficiency RF Power Amplifiers.pptx
Lic lab manual
Electric+Circuit+and+Simulation+Op+amp.pdf
Power supplies without transformers lightweight
Assignment 1 Description Marks out of Wtg() Due date .docx
Ad

Recently uploaded (20)

PPTX
OOP with Java - Java Introduction (Basics)
PPTX
MCN 401 KTU-2019-PPE KITS-MODULE 2.pptx
PPTX
Internet of Things (IOT) - A guide to understanding
PPTX
Lesson 3_Tessellation.pptx finite Mathematics
PPTX
Geodesy 1.pptx...............................................
PDF
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk
PDF
Operating System & Kernel Study Guide-1 - converted.pdf
PPTX
Engineering Ethics, Safety and Environment [Autosaved] (1).pptx
PPTX
Lecture Notes Electrical Wiring System Components
PPTX
additive manufacturing of ss316l using mig welding
PDF
composite construction of structures.pdf
PDF
Model Code of Practice - Construction Work - 21102022 .pdf
PDF
The CXO Playbook 2025 – Future-Ready Strategies for C-Suite Leaders Cerebrai...
PDF
Structs to JSON How Go Powers REST APIs.pdf
PPTX
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
PPTX
FINAL REVIEW FOR COPD DIANOSIS FOR PULMONARY DISEASE.pptx
PPTX
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
PPTX
M Tech Sem 1 Civil Engineering Environmental Sciences.pptx
PDF
PRIZ Academy - 9 Windows Thinking Where to Invest Today to Win Tomorrow.pdf
PDF
Well-logging-methods_new................
OOP with Java - Java Introduction (Basics)
MCN 401 KTU-2019-PPE KITS-MODULE 2.pptx
Internet of Things (IOT) - A guide to understanding
Lesson 3_Tessellation.pptx finite Mathematics
Geodesy 1.pptx...............................................
keyrequirementskkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkkk
Operating System & Kernel Study Guide-1 - converted.pdf
Engineering Ethics, Safety and Environment [Autosaved] (1).pptx
Lecture Notes Electrical Wiring System Components
additive manufacturing of ss316l using mig welding
composite construction of structures.pdf
Model Code of Practice - Construction Work - 21102022 .pdf
The CXO Playbook 2025 – Future-Ready Strategies for C-Suite Leaders Cerebrai...
Structs to JSON How Go Powers REST APIs.pdf
CARTOGRAPHY AND GEOINFORMATION VISUALIZATION chapter1 NPTE (2).pptx
FINAL REVIEW FOR COPD DIANOSIS FOR PULMONARY DISEASE.pptx
Infosys Presentation by1.Riyan Bagwan 2.Samadhan Naiknavare 3.Gaurav Shinde 4...
M Tech Sem 1 Civil Engineering Environmental Sciences.pptx
PRIZ Academy - 9 Windows Thinking Where to Invest Today to Win Tomorrow.pdf
Well-logging-methods_new................
Ad

Differentiator.ppt

  • 1. Lab 8 Experiment 17 A Differentiator Circuit
  • 2. Note Comment in Lab Manual • All of the diagrams use a uA741 op amp. – You are to construct your circuits using an LM 356 op amp. • There is a statement that values for R1, R2, and C2 should be limited by what is in your kit. – You may combine multiple resistors (capacitors) to obtain a desired resistance (or capacitance).
  • 5. iC i = 0 iR iR + iC + i =0 where i = 0mA iC =C1 dV3/dt iR = [0V – Vo]/R1 Vo = -R1C1 dV3/dt
  • 7. Why Two Different Circuits • If the input contains electronic noise with high frequency components, the magnitude of the high frequency components will be amplified significantly over the signal of interest and the system likely will become unstable. – It is thus necessary to modify the circuit to reduce or eliminate such effects.
  • 8. Modifications to Ideal Circuit • Two modifications to the circuit – both of which results in the formation of frequency filters. – First, a series resistor is inserted before the negative input terminal of op amp. The effect of this resistor is to act as an attenuator for the high frequency components. – Second, a capacitor is placed in the feedback network. This capacitor provides more feed-back for the high frequency components than for the low frequency components and also acts to stabilize the circuit.
  • 11. From these equations: • When the voltage across the capacitor doesn’t change (i.e., d.c. voltage), the capacitor’s current is equal to zero. – The capacitor acts like an open circuit. • When the voltage across the capacitor is changing rapidly (e.g., high frequency sine wave), the capacitor’s current is large and also changes with time. – The capacitor acts like a short circuit. The current through the circuit is limited by the other components in the circuit (i.e., the resistors).
  • 12. Practical Circuit R2 with C1 forms a high pass filter. If V3 is a d.c. voltage source, C1 acts like an open circuit and all of the input voltage (V3) is dropped across the capacitor (VC1) and the current through R2 and C1 will be determined primarily by the first derivative of the V3. If V3 is a high frequency a.c. voltage source, C1 acts like a short circuit and the current through R2 and C1 will be determined primarily by V3 divided by R2.
  • 13. Practical Circuit R1 with C2 forms a low pass filter. If the difference in the voltage between the negative input terminal on the op amp and Vo is relatively constant, C1 acts like an open circuit and all of the current through R2 and C1 will flow through R1. If the difference in the voltage between the negative input terminal on the op amp and Vo varies a lot with time, C1 acts like a short circuit and all of the current through R2 and C1 will flow through C2 and the output voltage will be approximately equal to the voltage on the negative input terminal, which will be 0 V.
  • 14. Operation as a Function of Frequency
  • 17. dB • dB is an abbreviation for decibels V V log 20 dB P P log 10 dB in out in out                   0.707 2 2 V V when occurs 3dB - 2 1 P P when occurs 3dB - in out in out                   
  • 18. Follow the Directions in the Lab Manual • Except: – Use the function generator on the Velleman oscilloscope • Remember that you have to set the Amplitude to 10V to have 5V sin(t) outputted. – Do not use the 10X probes with the Velleman oscilloscope when performing the oscilloscope measurements. • Just use the standard BNC-to-alligator or BNC-to-IC clip cables. – All plots should be made using MatLAB.
  • 21. Measurement of Phase Angle • There are two sets of instructions in the Lab 8 folder under resources – Phase Delay.pdf, which explains how to make a phase angle calculation using the information displayed when the Oscilloscope function of the Velleman oscilloscope is used. • You should become familiar with this technique. – Magnitude and Phase.pdf, which explains how to use the automated measurement tools on the Velleman scope to obtain the magnitude and phase of a signal at a single frequency and over a range of frequencies.
  • 22. Phase Shift as a Function of Frequency • The phase shift between the input voltage and the output voltage of the op amp will change from 90o to 180o to 270o as the operation of the circuit changes from a differentiator to inverting amplifier to integrator.
  • 23. Caution: PSpice Transient Analysis Issue Information in first half cycle is incorrect because the initial charge on the capacitor is zero.