electric circuits (fall 2016) pingqiang zhou...
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Electric Circuits (Fall 2016) Pingqiang Zhou
Announcements
• No discussion/lab session on Oct. 8 (SAT) & Oct. 9 (SUN)
Lab3 for week 5 (starting from Oct. 10).
Discussion on circuit theorem in week 5.
• Review solutions to first-order ODEs during holiday
1Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
请务必遵守学术道德规范!
• 单次作业或者实验抄袭
抄袭与被抄袭者该次作业/实验均计零分,课程总成绩打九折。
• 累计两次作业或者实验抄袭
抄袭与被抄袭者相应作业/实验计零,课程总成绩均打七折。
• 累计三次作业或实验抄袭者,或者考试作弊者
课程总成绩计零,同时上报信息学院学术委员会公开处理。
Electric Circuits (Fall 2016) Pingqiang Zhou
Lecture 4
- Operational Amplifiers
9/28/2016
Reading: Chapter 5
Lecture 4 3
Electric Circuits (Fall 2016) Pingqiang Zhou
Outline
• Operational amplifier (op amp) model
• Ideal op amp
• Inverting op amp
• Noninverting op amp
Voltage follower
• Difference amplifier
• Application: DAC
Lecture 4 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Brief History
• The Operational Amplifier (op amp) was invented in the
40’s.
Bell Labs filed a patent in 1941.
• Many consider the first practical op amp to be the vacuum
tube K2-W invented in 1952 by George Philbrick.
• Bob Widlar at Fairchild invented the uA702 op amp in
1963.
• Until uA741, released in 1968, op amps became relatively
inexpensive and started on the road to ubiquity.
5Lecture 4
https://en.wikipedia.org/wiki/Operational_amplifier
Electric Circuits (Fall 2016) Pingqiang Zhou
Where do You Use Op AMP?
• Audio amplifiers
• Low dropout regulators
• Active filters
• Medical sensor interface
• Baseband receivers
• A/D converters
• Oscillators
• Signal generators
• Hearing aids
6Lecture 4[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
The Op Amp
• A basic building block used in analog circuits.
• When combined with resistors, capacitors, and inductors,
can perform various functions:amplification/scaling
sign changing
addition/subtraction/multiplication/division
integration
differentiation
analog filtering
nonlinear functions (exponential, log, sqrt)
• Isolate input from output.
Lecture 4 7[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Analog Computer
8Lecture 4[Source: Alexander]
Electric Circuits (Fall 2016) Pingqiang Zhou
What are Inside an Op Amp?
• Origins at Fairchild Semiconductor in 1968.
9
Source: http://www.ibiblio.org/kuphaldt/electricCircuits/Semi/SEMI_8.html#xtocid109742.
Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Op Amp Terminals
• Five important terminals
The inverting input
The noninverting input
The output
The positive (+) power supply
The negative (-) power supply
• The rest three terminals
2 Offset Null (Balance)
–May used in auxiliary circuit to
compensate for performance
degradation due to aging etc.
1 No Connection (NC)
– Unused, not connected to the
amplifier circuit.
Lecture 4 10
Electric Circuits (Fall 2016) Pingqiang Zhou
Powering an Op Amp
• As an active element, the op-amp
requires a power source.
Often in circuit diagrams the power
supply terminals are obscured (ignored).
The supply current cannot be
overlooked.
• Most op-amps use two voltage
sources, with a ground reference
between them.
This gives a positive and negative
supply voltage.
𝑖0 = 𝑖1 + 𝑖2 + 𝑖+ + 𝑖−
Lecture 4 11
Electric Circuits (Fall 2016) Pingqiang Zhou
Output Voltage
• The voltage output of an op-amp is
proportional to the difference between
the noninverting and inverting inputs
Here, A is called the open loop gain.
Ideally A is infinite. In real devices, it is still
high: 105 to 108.
2 1( )o dv Av A v v
Lecture 4 12
𝑣2
𝑣1
Electric Circuits (Fall 2016) Pingqiang Zhou
Voltage Saturation
• Is the output voltage unlimited?
𝑣0 =
−𝑉𝑐𝑐 𝐴𝑣𝑑 < −𝑉𝑐𝑐𝐴𝑣𝑑 −𝑉𝑐𝑐 ≤ 𝐴𝑣𝑑 ≤ +𝑉𝑐𝑐+𝑉𝑐𝑐 𝐴𝑣𝑑 > +𝑉𝑐𝑐
How do we know the op-amp
is operating in linear region?
Lecture 4 13
Electric Circuits (Fall 2016) Pingqiang Zhou
Input-Output Transfer Plot
14[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Application
15
𝑅1𝑉𝑟𝑒𝑓
𝑉𝑜𝑢𝑡
Source: http://www.allaboutcircuits.com/textbook/semiconductors/chpt-8/the-operational-amplifier/
Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Application
16
Source: http://www.allaboutcircuits.com/textbook/semiconductors/chpt-8/the-operational-amplifier/
Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Example
Lecture 4 17[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Example
Lecture 4 18[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Example
Lecture 4 19[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Practice
A 741 op amp has an open-loop voltage gain of 2 × 105, input
resistance of 2𝑀Ω, and output resistance of 50Ω. Find the
closed-loop gain 𝑣𝑜/𝑣𝑠. Determine current 𝑖 when 𝑣𝑠 = 2𝑉.
20Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Correct or Not?
21Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Negative Feedback
𝑉𝑖𝑛 ↑ ⟹ voltage differential ↑ ⟹ 𝑉𝑜𝑢𝑡 ↑⟹ voltage differential ↓ ⟹ 𝑉𝑜𝑢𝑡 ↓⟹ ⋯⟹ 𝑉𝑜𝑢𝑡 → 𝑉𝑖𝑛 but small difference exists
Lecture 4 22
Negative feedback
Electric Circuits (Fall 2016) Pingqiang Zhou
Tradeoff
• Effective input signal
• Circuit gain
• Linear dynamic range
23Lecture 4[Source: Berkeley]
Negative Feedback No Feedback
Electric Circuits (Fall 2016) Pingqiang Zhou
Negative Feedback
• A self-stabilizing system (also true for any dynamic system
in general), giving the op-amp the capacity to work in its
linear (active) mode.
• Op-amp gain A does not have to be precisely set by the
factory in order for the circuit designer to build an amplifier
circuit with precise gain.
Source: http://www.allaboutcircuits.com/textbook/semiconductors/chpt-8/negative-feedback/
Lecture 4 24
Negative feedback
Electric Circuits (Fall 2016) Pingqiang Zhou
Ideal Op Amp
• Attributes of ideal op-amp:
infinite open-loop gain, 𝐴 ⋍ ∞– Implies that 𝑣2 = 𝑣1.
infinite resistance of the two
inputs, 𝑅𝑖 ⋍ ∞
–This means it will not affect any
node it is attached to
– Implies that 𝑖1 = 𝑖2 = 0.
zero output impedance, 𝑅𝑜 ⋍ 0–From Thevenin’s theorem one can
see that this means it is load
independent.
Lecture 4 25
Electric Circuits (Fall 2016) Pingqiang Zhou
Ideal Op-Amp Analysis – Golden Rules
Assumption 1: The potential between the op-amp input terminals, v(+) –
v(-), equals zero.
R2R1
+
V0VIN
EXAMPLE
Assumption 2: The currents flowing into the op-amp’s two input
terminals both equal zero.
No Potential DifferenceNo Currents
Lecture 4 26[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
27Lecture 4
Inverting Amplifier
[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Example
Lecture 4 28[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
29Lecture 4
Practice
• Determine 𝑣𝑜 in the circuit shown below
Electric Circuits (Fall 2016) Pingqiang Zhou
Non-Inverting Amplifier
Lecture 4 30
_
+
vin+-
R2
R1
RL
vo
[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
31Lecture 4
Application: Voltage Follower
_
+
vin+- RL
v2
v0
[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Application of Voltage Follower
“Buffer” sections of Circuit
Lecture 4 32[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Summing Amplifier
• Aside from amplification, the op-amp can be made to do
addition very readily.
Lecture 4 33
Electric Circuits (Fall 2016) Pingqiang Zhou
Example
34Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Practice
• Find 𝑣𝑜 and 𝑖𝑜 in the circuit shown below
35Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Difference Amplifier
Lecture 4 36
Electric Circuits (Fall 2016) Pingqiang Zhou
Example
• Design an op amp circuit with inputs 𝑣1 and 𝑣2 such that
𝑣𝑜 = −5𝑣1 + 3𝑣2.
37Lecture 4
Electric Circuits (Fall 2016) Pingqiang Zhou
Common Mode Rejection
• It is important that a difference amplifier rejects any signal
that is common to the two inputs.
Which implies that when 𝑣1 = 𝑣2, 𝑣𝑜 = 0.
2 1 2 2
2 1
1 3 4 1
1
1o
R R R Rv v v
R R R R
Lecture 4 38
Electric Circuits (Fall 2016) Pingqiang Zhou
Application: Measurement Uncertainty
(T = 21˚C)v2 V0 = V2 ± 1% of V2
21˚C ± 0.21˚CG = 1
± 1%
(T = 21˚C)
Thermistor
Thermistor
Fixed Reference Temp = 20˚C
1˚C ± 0.01˚C
Direct Measurement
G = 11%
v2
v1
V0 = (V2 ‒ V1) ± 1% of (V2 ‒ V1)
Differential Measurement
Much better measurement uncertainty
Lecture 4 39
Electric Circuits (Fall 2016) Pingqiang Zhou
Cascaded Op Amps
• This head to tail configuration is called “cascading”.
Each amplifier is then called a “stage”.
• The gain of a series of amplifiers is the product of the
individual gains:
𝐴 = 𝐴1 ∙ 𝐴2 ∙ 𝐴3
Lecture 4 40
Electric Circuits (Fall 2016) Pingqiang Zhou
Digital Input
0
1
2
3
4
5
6
7
8
0 2 4 6 8 10 12 14 16
An
alo
g O
utp
ut
(V)
111110000100
0000 0001
Application - DAC
[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
DAC
−𝑉𝑜 =𝑅𝑓
𝑅1𝑉1 +
𝑅𝑓
𝑅2𝑉2 +
𝑅𝑓
𝑅3𝑉3 +
𝑅𝑓
𝑅4𝑉4
Lecture 4 42
Electric Circuits (Fall 2016) Pingqiang Zhou
A DAC can be used to convert the digital representation
of an audio signal into an analog voltage that is then
used to drive speakers -- so that you can hear it!
0 0 1 0 10 0 1 10 1 0 0
1.52
0 1 0 10 1 1 00 1 1 11 0 0 0
2.53
3.54
1 0 0 11 0 1 01 0 1 11 1 0 01 1 0 11 1 1 01 1 1 1
4.55
5.56
6.57
7.5
Binarynumber
Analogoutput(−𝑉𝑜)
0 0 0 00 0 0 1
0.5
MSB LSB
S1 closed if LSB =1
S2 " if next bit = 1
S3 " if " " = 1
S4 " if MSB = 1
4-Bit D/A
8V
+ V0
5K
80K
40K
20K
10K
S1
+-
S3
S2
S4
+
DAC
“Weighted-adder D/A converter”
(Transistors are used
as electronic switches)
[Source: Berkeley]
Electric Circuits (Fall 2016) Pingqiang Zhou
Summary
Lecture 4 44
Electric Circuits (Fall 2016) Pingqiang Zhou
New Content for the Discussion Session
• Positive feedback
• Instrumentation amplifier
• Differentiator
• Integrator
45Lecture 4
Positive feedback