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Transcript
Lecture 19:
CMOS Operational Amplifiers
Gu-Yeon Wei
Division of Engineering and Applied Sciences
Harvard University
[email protected]
Wei
1
Overview
•
•
Wei
Reading
– S&S: Chapter 10.7 – 10.8
Background
– In the beginning of the semester, we built circuits that can perform
interesting and useful operations with op amps. Now, we will take
all that we have learned about circuits and devices to see how
operational amplifiers themselves are built. In this lecture, we will
focus on building CMOS op amps. S&S has much more detail in
terms of building operational amplifiers with BJT and JFET devices.
While these technologies are better suited for discrete op amp
devices, because they offer the potential for higher bandwidths and
output drive capabilities, CMOS op amp circuits find use in many
integrated circuit systems. In CMOS implementations, extra output
stages are used to provide the necessary off-chip drive. One can
read more on this topic in Chapter 9 of S&S.
ES154 - Lecture 19
2
General Characteristics
•
Op amps are an important component of modern CMOS IC’s. They used to designed as
general purpose amplifiers that can meet a variety of requirements. The main target was
extremely high gain (>1e5), high input impedance and low output impedance (like an ideal
amplifier). This was done (to some extent) at the expense of different aspects of
performance (e.g., speed, output voltage range, power, etc.). Designs these days are much
more tailored to have (good enough) performance w.r.t. the specific needs of particular
applications. Within an IC, often use Operational Transconductance Amplifiers (OTA).
•
Some performance parameters of op amps
– Gain and Bandwidth
•
–
Output Swing
•
–
Can minimize by trading off other parameters
Supply Rejection
•
Wei
Combat non-linearity with feedback
Noise and Offset
•
–
Maximize w.r.t. power supply (but supply shrinking in modern processes)
Linearity
•
–
Want as large as possible
Strong dependence on current source output resistance
ES154 - Lecture 19
3
Simple One-Stage Op Amps
•
Two differential pair amplifiers that we have already seen can be used as op
amps. The low-frequency, small-signal gain of both is gmN(roN||roP). The
capacitive loads (CL) usually determine their bandwidth.
Vb
Vout
CL
Vout
Vin
Vin
Wei
CL
CL
ES154 - Lecture 19
4
Cascode Op Amps
•
In order to achieve higher gain, one can use cascoding. These amplifiers are
often called ‘telescopic’ cascode amps. While gain increases, the output range
of these devices are limited.
Vb3
Vb2
Vout
Vb
CL
Vout
CL
Vin
Vb1
CL
Vin
– Connecting the in unity-gain feedback configuration results in significant
reduction of output range
Wei
ES154 - Lecture 19
5
Folded Cascode Circuit
•
•
In order to alleviate some of the drawbacks
of telescopic op amps (limited output
range), a “folded cascode” can be used
(we analyzed this circuit in HW7)
– M1 is common-source
transconductance amp and M2 is
common-gate transimpedance amp
– Advantage is M2 no longer stacks on
top of M1
– Possible for either pMOS or nMOS
cascodes
Vout
Vb
M2
Vin
M1
Vin
M1
Vb
M2
The output resistance for cascode and
folded cascode are roughly equivalent
(gmro2)
Wei
ES154 - Lecture 19
Vin
Vout
Vb
M1
M2
Vout
Vin
M1
Vb
Vout
M2
6
Folded Cascode Amplifier
•
Turn a differential telescopic cascode amplifier into a folded cascode amplifier
Vout
Vb
Vout
Vin
Vb
Vin
Wei
ES154 - Lecture 19
7
Full circuit Implementation
of Folded Cascode Amplifier
Vbp2
IREF1
Vout
Vin
Vbn2
•
•
Wei
IREF2
IREF3
– Reference current sources are set: I REF 3 = I REF 2 + I REF1 2
A version with nMOS differential pair inputs also possible (flip upside down)
What sets output common mode?
– Depends on relative output resistances looking up and down
– Can vary with process and reference current mismatches
ES154 - Lecture 19
8
Gain of a Folded-Cascode Amplifier
•
Calculate gain using the differential half-circuit. Gain
can be calculated as GmRout where Gm is the shortcircuit transconductance of the overall circuit and Rout
is the output resistance.
– Short out Vout to ground and solve for Iout/Vin = Gm
– Solve for the output resistance
Vin
M1
| Av |= Gm Rout
Vbp1
M5
Vbp2
M4
ro45
Vout
Vbn2
M3
Vbn1
M2
Gm ≅ g m1
Rout = ro 45 || [g m 3 ro 3 (ro1 || ro 2 )] = g m 4 ro 4 ro 5 || [g m 3ro 3 (ro1 || ro 2 )]
Vout
-gm3Vx
| Av |≅ g m1{g m 4 ro 4 ro 5 || [g m 3 ro 3 (ro1 || ro 2 )]}
-Vx
ro3
ro45
gm1Vin
Vin
Wei
ES154 - Lecture 19
ro1||ro2
9
+Common-Mode Feedback
•
Use feedback to set the output common mode of a folded cascode amplifer,
called common-mode feedback
– Sense the average (common-mode) voltage at the output, compare to a
desired reference voltage (Vref), and use it to set the current source
IREF1
IREF2
IREF2
Vout
Vin
Vb
CM
Sense
This
Thisisisone
oneofof
several
severalmethods
methodsfor
for
implementing
CM
implementing CM
feedback
feedback
•
Wei
IFB
Vref
For Vin=0, feedback sets IFB=IREF2+IREF1/2 and common-mode voltage = Vref
ES154 - Lecture 19
10
Using High-Swing Cascodes
•
We can also use the high-swing cascode circuit as a load to achieve higher
output range in a single-end telescopic amp
Vb2
Vout
Vb
Vin
Wei
CL
Vout
Vb1
CL
Vin
ES154 - Lecture 19
11
Gain Boosting
•
Another method for increasing the output resistance of a cascode circuit is to
use gain boosting
Rout
Vb
M2
Rout
Vb
M2
Rout
Vb
A3
Rout
M2
M2
M3
Vin
M1
ro1
ro1
Gain Boosting Circuit
ro1
Regulated Cascode
– For the gain boosted cascode circuit…
Rout ≈ A3 g m 2 ro 2 ro1
– Similarly, with a regulated cascode
Rout ≈ ( g m 3 ro 3 )( g m 2 ro 2 ro1 )
Wei
ES154 - Lecture 19
12
Two-Stage Op Amps
•
•
In order to implement amplifiers with high gain and high swing, we must resort to
two-stage amplifier designs
High-Gain
High-Swing
– First stage used to generate high gain
Vin
Vout
Stage
Stage
– Second stage to generate high swing
Use any high-gain first stage and high-swing second stage
– two simple examples (differential and single-ended output amplifiers)
Vbp
Vout1
Vin
Vbp
Vout2
Vin
Vout
Vbn
Wei
ES154 - Lecture 19
13
Next Time
•
Wei
We will complete our discussion of Op amp design with a discussion of stability
and frequency compensation. We first see how frequency analysis of the loop
gain of a feedback circuit gives us the ability to determine whether the circuit will
be stable or not. A loop gain transfer function with a single dominant pole can
be shown to be stable. However, with multiple poles, stability can be
compromised. To combat instability, frequency compensation can be used.
ES154 - Lecture 19
14