![Page 1: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/1.jpg)
We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational amplifier could be
•1. Class A amplifier.•2. Source follower.•3. Push-Pull amplifier ( inverting and follower).•4. Bipolar Output
![Page 2: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/2.jpg)
![Page 3: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/3.jpg)
![Page 4: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/4.jpg)
![Page 5: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/5.jpg)
![Page 6: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/6.jpg)
![Page 7: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/7.jpg)
Let us now get back to the factors characterizing an operational amplifiers.
Gain; Gain Bandwidth product; CMRR; PSRR;
CMR; Output Swing; Input Offset; Noise
Settling Time; Slew Rate;.
![Page 8: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/8.jpg)
![Page 9: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/9.jpg)
Power Supply Rejection ratio (PSRR)
)0v(vv
)0v(vv
A
AA
V
VPSRR
inps
out
psin
out
ps
dd
OUT
DD
This gives a measure of noise introduced at the output due to fluctuations in the power supply.
![Page 10: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/10.jpg)
![Page 11: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/11.jpg)
Frequency Response:
Assuming that all the inter electrode capacitances are negligibly small it is evident to see that the operational amplifier structure will have three poles contributed by the capacitances CM, C1 and CL.
Predominantly the poles will be due to C1 and CL
![Page 12: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/12.jpg)
In all operational amplifier application they are used in a feedback mode. For the stability of the amplifier configuration we desire that the loop gain be less than unity when the phase shift nears 180º (normally) at 135º.
![Page 13: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/13.jpg)
![Page 14: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/14.jpg)
Depending on the relative values of 1 and 2 will determine whether the loop gain will reach unity before the phase shift reaches 0º. The closer the two frequencies 1 and 2 the less stable will the circuit be. We define two quantities here namely Gain Margin and Phase Margin. Gain margin is the loop gain when the phase is 0º and Phase Margin is the difference from 0º, then phase when the loop gain is unity.
![Page 15: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/15.jpg)
![Page 16: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/16.jpg)
![Page 17: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/17.jpg)
2
6m
c12c21
c6m2
c6m
7d6d3d1d1
c12c21212
c216m2c2211
6m2212m1m
in
out
C
g
CCCCCC
Cgp;
Cg
ggggp
ionapproximatpoleantmindobygiving
CCCCCCRRsCRRgCCRCCRs1
gCs1RRgg
vv
c
2m
c
6m1 C
gGBand
C
gz
![Page 18: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/18.jpg)
![Page 19: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/19.jpg)
The requirement that phase margin should be atleast 60º means that
GBat60
|z|tan
|p|tan
|p|tan180
1
1
2
1
1
1M
This gives us far large gain, |p2| 2.2 GB. Demanding z1 >> p1 gives along with p2| 2.2 GB
2c2m6m C22.0Candg10g
![Page 20: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/20.jpg)
![Page 21: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/21.jpg)
![Page 22: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/22.jpg)
2
6m
c12c21
c6m2
1z3
c6m
7d6d3d1d1
C
g
CCCCCC
Cgp
CR1
p;Cg
ggggp
To remove the zero and have the second pole still farther away, we do pole zero cancellation i.e put z1 = p2. This gives
6mc
2cz g
1C
CCR
![Page 23: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/23.jpg)
Power Supply Rejection Ratio (PSRR):
)0v(vv
)0v(vv
PSRR;)0v(
vv
)0v(vv
PSRR
inss
out
ssin
out
indd
out
ddin
out
![Page 24: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/24.jpg)
ddddd
dddd
d
ddout v
PSRR1
vA
Av
A1
Av
![Page 25: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/25.jpg)
![Page 26: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/26.jpg)
![Page 27: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/27.jpg)
out
dd
6ds3ds1ds
c6m
c6m
2
1m
c
6ds3ds1ds
6m1m
6ds3ds1ds
c6m
c6m
122c1c
1m
c
6ds3ds1ds
6m1m
v
v
1g)gg(
Cgs
1Cg
Cs1
gCs
g)gg(
gg
1g)gg(
Cgs
1Cg
)CCCCCC(s1
gCs
g)gg(
ggPSRR
![Page 28: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/28.jpg)
![Page 29: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/29.jpg)
![Page 30: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/30.jpg)
1)gg(
Cs
1gCs
1gCs
g)gg(
ggPSRR
3ds1ds
c
6m
2
1m
c
6ds3ds1ds
6m1m
![Page 31: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/31.jpg)
![Page 32: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/32.jpg)
1)gg(
Cs1
g
Cs
1g
Cs1
g
Cs
g)gg(
ggPSRR
3ds1ds
c
7ds
7gd
6m
2
1m
c
7ds3ds1ds
6m1m
![Page 33: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/33.jpg)
![Page 34: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/34.jpg)
gm1 = gm2 = gm1 , (gds2 + gds3)-1 = R1 , and (gds6 + gds7)-1 = R2
Slew rate = CC/I5 ; Settling time: 5(VDD - VSS)/I5
c
1m
766
1m
7d6d
6m
315
1m
3d1d
1m
C
goductPrbandwidthGain
I
g2
gg
gGainStageSecond
I
g2
gg
gGainStageFirst
![Page 35: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/35.jpg)
1m6mc
1m
c
6m1
L
6m2
g10g)e.i(C
g10GB10
C
gzZero
;60PMforGB2.2C
g|p|PoleOutput
1T5DS1
5SS1G VV
IVminV
|V|I
VVmaxV 3TO3
51TDD1G
![Page 36: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/36.jpg)
![Page 37: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/37.jpg)
Gain at mid frequency > 5000;
Gain Bandwidth Product: 5MHz;
Input Common Mode Range: -1 to 2V;
Load Capacitance: 10pF;
Slew Rate: 10V/s;
Output Voltage Swing: ± 2V and
Power Dissipation: 2mW
V85.0V,VV55.0m/fF43.2C
04.0;05.0;V/A110K;V/A50K
03T1T2
ox
PN2'
N2'
P
![Page 38: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/38.jpg)
To start with we choose an appropriate value of Cc. Assuming a phase margin of > 60º choose Cc = 3pF.
Given a slew rate of 10V/s we have A3010x1010x3CSRI 612
c5
426
6
2
1T03T1GDD'P
5
3
LW
1555.085.025.210x50
10x30
minVmaxVmaxVVK
I
LW
![Page 39: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/39.jpg)
Pole due to mirror capacitance gm3/(2Cgs3) where Cgs = 0.67 W3 L3 Cox. Assuming a channel length of 1m we get |p3| 448 MHz >> GB.
Using the expression for GB we have
gm1 = GB x Cc = (5 x 106) 2 (3 x 10-12) = 94.25 S
0.3)15()50()2(
)25.94(
IK2
g
LW
LW 2
1'N
22m
21
![Page 40: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/40.jpg)
We have from VDS5
5.4
35.010x110
10x32
VK
I2
LW
26
6
25DS
'5
5
5
To obtain W/L ratio for M6 we take gm6 = 10 gm1 = 942.5 Since we know (W/L)3 = 15 and I3 = 15A we have gm3 = 150. Hence we have
V35.0maxVI
VminVV 1T1
5SS1G5DS
From the expression for VG1 min
![Page 41: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/41.jpg)
From the expression for gm we obtain I6 as
A95
)94(10x502
10x5.942
6WK2
gI
6
26
6'6
26m
6
1410x30
10x955.4
I
I
LW
LW
5
5
5
6
57
Using the values of (W/L)6 = 94 and (W/L)7 = 14 we get VDS7(sat) = 0.351V and VDS6(sat) =0.201V
94150
5.94215
g
g
LW
LW
3m
6m
46
![Page 42: We have so far seen the structure of a differential amplifier, the input stage of an operational amplifier. The second stage of the simplest possible operational](https://reader030.vdocuments.us/reader030/viewer/2022032517/56649caf5503460f949729b8/html5/thumbnails/42.jpg)
The total Power Dissipation is given by
mW625.0)A95A30(V5Pdiss
The over all gain is given by
7696)05.004.0(10x95)05.004.0(10x30
)10x5.924()10x45.92()2(A
66
66
v