Student Lecture #1: Operational Amplifiers
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Transcript Student Lecture #1: Operational Amplifiers
James Kelly
Nathan Knight
Gustavo Lee
Introduction
Characteristics of Ideal and Real Op-Amps
Basic Circuits of Op-Amps
Applications
Exercise
An Operational Amplifier (known as an “Op-Amp”) is an
integrated circuit that sets an output voltage based on the
input voltages provided.
In a circuit, it is used to perform an operation and an
amplification where the operation may be add, subtract,
filter, integrate, differentiate, etc.
Op-Amps are composed of transistors, resistors,
capacitors, and diodes.
1941: Karl Swartzel of Bell Labs developed the first Op-Amp.
Used 3 vacuum tubes, only one input (inverting), and operated
on + 350 V to achieve 90 dB gain.
1947: Loebe Julie developed the Op-Amp as it is known today, with
two inputs – inverting and non-inverting.
The differential input made a whole range of new functionality
possible.
1953: First commercially available Op-Amp.
George A. Philbrick Researches (GAP-R). GAP-R pioneered the
first reasonable-cost, mass-produced operational amplifier
1961: Advent of solid-state, discrete Op-Amps.
Made possible by the invention of the silicon transistor, which
led to the concept of Integrated Circuits (IC)
Reduced power input to ±15V to ±10V
1962: Op-Amp in a potted module.
Packaging in small black boxes allowed for integration with a
circuit
1963: First monolithic IC Op-Amp, the
μA702, designed by Bob Widlar at Fairchild
Semiconductor.
Monolithic ICs consist of a single chip
1968: Release of the μA741
The μA741 became the canonical Op-Amp, from
which many modern op-amps base their pinout
from, and is still in production today.
Parameter
Range
Frequency Spectrum
5-kHz to beyond 1-GHz GBW
Supply Voltage
0.9 V to a maximum 1000 V
Input Offsets
Approximately Zero
Introduction
Characteristics of Ideal and Real Op-Amps
Basic Circuits of Op-Amps
Applications
Exercise
𝑉𝑆+ : positive power supply
𝑉𝑆− : negative power supply
𝑉+ : non-inverting input terminal
𝑉− : inverting input terminal
𝑉𝑜𝑢𝑡 : output terminal
𝑉+ , 𝑉− , 𝑉𝑜𝑢𝑡 are all referenced to ground
Parameter Name
Symbol
Value
Input impedance
𝑅𝑖𝑛
∞
Output impedance
𝑅𝑜𝑢𝑡
0
Open-loop gain
𝐺
∞
Bandwidth
𝐵
∞
Temperature-independent.
𝑉𝑜𝑢𝑡 = 𝐺 𝑉+ − 𝑉− = 𝐺 ∙ 𝑉𝑖𝑛
The maximum output voltage value is the supply voltage (saturation):
𝑉𝑆− ≤ 𝑉𝑜𝑢𝑡 ≤ 𝑉𝑆+
What this means:
Current flow into the op-amp from either input terminal is zero.
▪ 𝐼− = 𝐼+ = 0
Differential voltage between the two input terminals is zero.
▪ 𝑉+ − 𝑉− = 0
Parameter Name
Symbol
Value
Input impedance
𝑅𝑖𝑛
106 Ω
Output impedance
𝑅𝑜𝑢𝑡
102 Ω
Open-loop gain
𝐺
104 ~107
Bandwidth
𝐵
103 ~109 Hz
Operating temperature range:
Commercial: 0℃~70℃
Industrial: −25℃~85℃
Military: −55℃~125℃
𝑉𝑜𝑢𝑡 = 𝐺 𝑉+ − 𝑉− = 𝐺 ∙ 𝑉𝑖𝑛
Vout
Saturation results when the output
voltage is equal to the power supply’s
voltage
In typical op-amps, the saturation level is
about 80% of the supply voltage.
Vsat+
Slope = G
Vin
Vsat-
Saturation
Cutoff Points
Positive Saturation Cutoff:
𝑉𝑜𝑢𝑡 = 𝑉𝑠𝑎𝑡+ ≈ 𝑉𝑆+
Linear Mode:
𝑉𝑜𝑢𝑡 = 𝐺 𝑉+ − 𝑉−
Negative Saturation Cutoff:
𝑉𝑜𝑢𝑡 = 𝑉𝑠𝑎𝑡− ≈ 𝑉𝑆−
Introduction
Characteristics of Ideal and Real Op-Amps
Basic Circuits of Op-Amps
Applications
Exercise
A closed-loop op-amp has feedback from the
output back to one of the inputs, whereas an
open-loop op-amp does not.
Open-Loop
Closed-Loop
Negative feedback connects the output to the inverting
input (-), whereas positive feedback connects the output to
the non-inverting input (+).
Negative Feedback
Positive Feedback
Negative feedback op-amps can produce any voltage in the
supply power range.
Positive feedback op-amps can only produce the maximum
and minimum voltages of the range.
Vout
Vout
Vsat+
Vsat+
Vin
VsatNegative Feedback
Vin
VsatPositive Feedback
Functionality: to amplify the input voltage to output
voltage with a negative gain.
𝑉+ = 0 𝑉
𝑉𝑖𝑛 = 𝑉− = 𝑅𝑖𝑛 ∙ 𝐼
𝑉𝑜𝑢𝑡 = 𝑅𝑓 ∙ −𝐼
𝑉𝑜𝑢𝑡
𝑉𝑖𝑛
=
−𝐼∙𝑅𝑓
𝐼∙𝑅𝑖𝑛
𝑉𝑜𝑢𝑡 = −
𝑅𝑓
𝑅𝑖𝑛
∙ 𝑉𝑖𝑛
𝐼
Functionality: to amplify the input voltage to output
voltage with a positive gain.
𝑉𝑖𝑛 = 𝑉− = 𝑉+
𝑉− = 𝑅1 ∙ 𝐼
𝑉𝑜𝑢𝑡 = (𝑅1 + 𝑅2 ) ∙ 𝐼
𝑉𝑜𝑢𝑡
𝑉𝑖𝑛
𝐼∙(𝑅1 +𝑅2 )
=
𝐼∙𝑅1
𝑅2
𝑉𝑜𝑢𝑡 = 1 +
𝑅1
∙ 𝑉𝑖𝑛
𝐼
Functionality: takes the summation of input voltages
over time and provides that as the output signal
𝑉+ = 0 𝑉
𝑉− 𝑡 = 𝑅 ∙ 𝐼(𝑡)= 𝑉𝑖𝑛 (𝑡)
𝑉𝑖𝑛 (𝑡)
𝐼 𝑡 =
𝑅
𝑡
1
𝑉𝑜𝑢𝑡 = − ∙
𝐼(𝜏)𝑑𝜏
0
𝐶
𝑡
1
𝑉𝑜𝑢𝑡 = −
∙ 0 𝑉𝑖𝑛 (𝜏)𝑑𝜏
𝑅𝐶
𝐼(𝑡)
Functionality: takes the rate of change of the
inverted input voltage signal and provides that as
the output signal
𝑉+ = 0 𝑉
1
𝑉− 𝑡 = 𝑉𝑖𝑛 (𝑡) = ∙ 𝐼 𝑡 𝑑𝑡
𝑑𝑉𝑖𝑛 (𝑡)
𝑑𝑡
𝐼 𝑡 =𝐶∙
𝑉𝑜𝑢𝑡 = −𝑅 ∙ 𝐼(𝑡)
𝑉𝑜𝑢𝑡 = −𝑅𝐶 ∙
𝐶
𝑑𝑉𝑖𝑛 (𝑡)
𝑑𝑡
Functionality: takes the difference
between two signals and provides that
as the output
𝑉𝑜𝑢𝑡 =
If
𝑅𝑓
𝑅1
=
𝑅𝑔
𝑅2
𝑅𝑔
𝑅1
𝑅𝑔 +𝑅2
:
𝑉𝑜𝑢𝑡 =
𝑅1 +𝑅𝑓
𝑅𝑓
𝑅1
(𝑉2 −𝑉1 )
Moreover, if 𝑅𝑓 = 𝑅1 :
𝑉𝑜𝑢𝑡 = 𝑉2 − 𝑉1
𝑉2 −
𝑅𝑓
𝑉
𝑅1 1
Functionality: takes the sum of two or more input
voltages and provides an output voltage
proportional to the negative of the algebraic sum
𝑉𝑜𝑢𝑡 = −𝑅𝑓
+
𝑉2
𝑅2
+⋯+
𝑉𝑛
𝑅𝑛
If 𝑅1 = 𝑅2 = ⋯ = 𝑅𝑛 :
𝑉𝑜𝑢𝑡 = −
𝑉1
𝑅1
𝑅𝑓
𝑅1
(𝑉1 +𝑉2 + ⋯ + 𝑉𝑛 )
Moreover, if 𝑅𝑓 = 𝑅1 = 𝑅2 = ⋯ = 𝑅𝑛 :
𝑉𝑜𝑢𝑡 = −(𝑉1 +𝑉2 + ⋯ + 𝑉𝑛 )
By setting
𝑅𝑓
𝑅1
1
𝑛
= , the summing op-amp can be
used as an averaging operator:
1
𝑛
𝑉𝑜𝑢𝑡 = − (𝑉1 +𝑉2 + ⋯ + 𝑉𝑛 )
Introduction
Characteristics of Ideal and Real Op-Amps
Basic Circuits of Op-Amps
Applications
Exercise
Active filters
Signal processing
Digital Image processing
Strain gauges
Control circuits
PID controllers for aircraft
PI controllers for temperature measurement circuitry
And much more…
Attenuates frequencies above
the cutoff frequency.
Cutoff frequency (Hz):
𝑓𝑐 =
1
2𝜋𝑅2 𝐶
Gain in the passband:
𝐺=−
𝑅2
𝑅1
Attenuates frequencies below
the cutoff frequency.
Cutoff frequency (Hz):
𝑓𝑐 =
1
2𝜋𝑅1 𝐶
Gain in the passband:
𝐺=−
𝑅2
𝑅1
Strain gauges consist of a pattern
of resistive foil mounted on a
backing material.
As the foil is subjected to stress,
the resistance of the foil changes in
a defined way.
This results in an output signal
directly related to the stress value,
typically a few millivolts.
Op-Amps are utilized to amplify
the output signal level to 5~10 V, a
suitable level for application to
data collection systems.
A proportional-integral-derivative (PID) controller is a generic feedback
mechanism widely used in industrial control systems.
It calculates an “error” value as the difference between a measured process
variable and a desired setpoint.
Using this error, it calculates a control input using tuning parameters 𝐾𝑝 , 𝐾𝑑 ,
and 𝐾𝑖 to drive the error to zero.
𝑡
𝑑
𝑢 𝑡 = 𝐾𝑝 𝑒 𝑡 + 𝐾𝑖
𝑒 𝜏 𝑑𝜏 + 𝐾𝑑 𝑒(𝑡)
𝑑𝑡
0
So where do op-amps come in?
The error is calculated using a Summing Op-Amp.
Using this error voltage:
▪ The derivative of the error is calculated using a Derivative Op-Amp.
▪ The integral of the error is calculated using an Inverting Op-Amp.
The tuning parameters 𝐾𝑝 , 𝐾𝑑 , and 𝐾𝑖 can be selected by
appropriate selection of resistors and capacitors.
Comparators
Detectors
Threshold detector
Zero-level detector
Oscillators
Wien bridge oscillator
Relaxation oscillator
Level shifters
Introduction
Characteristics of Ideal and Real Op-Amps
Basic Circuits of Op-Amps
Applications
Exercise
Consider the circuit above running for 5 seconds. Find
𝑉𝑜𝑢𝑡 (5) when:
𝑉𝑜𝑢𝑡 0 = 0
𝑉𝑖𝑛 t = 3t
𝑅 = 5𝑀Ω, 𝐶 = 5𝜇, 𝑅𝑖𝑛 = 10𝑘Ω, 𝑅𝑓 = 20𝑘Ω
Cetinkunt, Sabri. Mechatronics. Hoboken, NJ: John Wiley & Sons Inc., 2007.
Jung, Walter G. Op Amp Applications Handbook. Analog Devices, Inc., 2005.
“Operational Amplifier.” http://en.wikipedia.org/wiki/Operational_amplifier.
“Operational Amplifier Applications.”
http://en.wikipedia.org/wiki/Operational_amplifier_applications.
“The Strain Gauge.”
http://web.deu.edu.tr/mechatronics/TUR/strain_gauge.htm.
“The PID Controller.” http://en.wikipedia.org/wiki/PID_controller.
“Feedback in Electronic Circuits: An Introduction.”
http://ecee.colorado.edu/~ecen4827/lectures/dm_feedback1.pdf.
“Differentiator and Integrator Circuits”
http://www.allaboutcircuits.com/vol_3/chpt_8/11.html.
“Inverting Op-Amp” http://www.wiringdiagrams21.com/2009/12/17/basicinverting-op-amp-circuit-diagram/
Questions?