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EEE 241
ANALOG ELECTRONICS
CLASS 15&16
DR NORLAILI MOHD NOH
2
GM can also be obtained by inspection of the
circuit. Since for Q2, collector current is the
output current and emitter current is the input
current (CB configuration), then current gain of
Q2 is ≈ 1.
Hence, current gain of the cascode is equal to
the current gain of the CE Q1.
For the CE, ais = β.
From the previous slide, we know that
We know that
Hence, is 1
M m1i π1
a βG = = = g
R r
o oiMis i
ii i
Gvi ia = = =R
vi i
iR = r
r
+
1v m1 1g v
2v
1 2,C ER
m2 2g vo2r
2C
r
2B
+
ov
1E
+iv
o1r
OR
1B
iR
3
At node C2 :
To determine RO :
When vi=0, then v1=0.
Hence, gm1v1=0
t m2 2 ro2i =g v +i
o2t ro2 2
t m2 2 o2t 2
t t o2 m2 2 o2 2
m2 o2t t o2 2
-v +i r -v = 0
-v + i -g v r -v = 0
-v +i r -g v r -v = 0
v =i r - g r +1 v
+2v
m2 2g v o2r
2C
r
2B
+tv
o1r
+
2v ti
1Cro2i
t
ot
v 0i
vR =
i
KVL at the output loop,
r
+
1v m1 1g v
2v
1 2,C ER
m2 2g vo2r
2C
r
2B
+
ov
1E
+iv
o1r
OR
1B
iR
4
+2v
m2 2g v o2r
2C
r
2B
+tv
o1r
+
2v ti
1C ti
m2 o2t t o2 2
2t
o1 π2
m2 o2 t o1 π2t t o2
t m2 o2
O o2t
o1 π2
v =i r - g r +1 v
-vi =
r //r
v = i r - g r +1 -i r //r
v g r +1R = = r +
1 1i+
r r
m2 o2
O o2m2
o1 o2
m2
o2O o2
m2
o1 o2
m2
o2O o2
m2 o1
o1 o2
g r +1R = r +
1 g+
r β
1g +
rR = r 1+
1 g+
r β
1g +
rR = r 1+
1 g r1+
r β
where o
πm
βr =
g
← enough
5
If ro1 = ro2 , m2 o1
O o2m2 o1
o2
g r +1R = r 1+
g r1+
β
If gm2 ro1 >> βo2 ,
m2 o1
O o2m2 o1
o2
o2 m2 o1
O o2m2 o1
g r +1R = r 1+
g r
β
β g r +1R = r 1+
g r
o1m2 o1 m2
o2 o2O o2 o2
m2 o1 m2 o1
o1 o2 o2
1 rg + r g +
r rR = r 1+ = r 1+
1 g r g r1+ 1+
r β β
If βo2 >>1, then gm2 ro1 >> 1,
o2 m2 o1
O o2m2 o1
o2O o2
O o2 o2
β g rR = r 1+
g r
R = r 1+β
R r β
6
Hence, the CE-CB connection displays an output resistance that is
larger by a factor of about βo2 then the CE stage alone (RO of CE is ro
if RC is neglected)
o o ovo O M
i o i
v v ia R G
v i v
Open circuit voltage gain :
Hence, vo o2 o2 m1a = r β g
O o2 o2R r β
For a CE amplifier, if RC is not
included. Thus, the magnitude of the
maximum available voltage gain is higher
by a factor βo2 than for the case of a single
transistor.
v m oa = g r
7
3.4.2.2 The MOS Cascode
s2 ds1
gs1 i
gs2 s2
i
v = v
v = v
v = v
R =
1M
BIASV
2M
R
DDV
OR
iV+
m1 gs1g v
R
o2r
2D2G
+ov
1S
+iv
o1r
oi
1G 1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs1v
+
gs2v
+
8
oM
i v 0o
iG =
v
KCL at node D2,
ds1o m2 ds1
o2
o ds1 m2o2
vi = -g v -
r
1i = v -g -
r
KCL at node D1,
o m1 i
o1 m2
o2
o m1M
i
o1 m2
o2
1i 1+ = g v
1r g +
r
i gG = =
1v1+
1r g +
r
ds1o m1 i
o1
oo m1 i
o1m2
o2
vi = g v +
r
1ii = g v +
1r -g -r
m1 gs1g v
R
o2r
2D2G
+ov
1S
+iv
o1r
oi
1G 1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs1v
+
gs2v
+
m1 gs1g v
o2r
2D2G+o 0v
1S
+iv
o1r
oi
1G 1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs1v
+
gs2v
+
← enough
9
o m1M
i
o1 m2
o2
m1 o1 m2
o2M
o1 m2
o2
o1m1 m2 o1 m1
o2M
o1m2 o1
o2
M m1o1
m2 o1
o2
i gG = =
1v1+
1r g +
r
1g r g +
rG =
1r g + +1
r
rg g r + +1 -g
rG =
rg r + +1
r
1G = g 1-
rg r + +1
r
If ro1 =ro2, then
M m1m2 o1
1G = g 1-
g r +2
If gm2ro1 >>1, then M m1G g
This equation shows that the
transconductance of the cascode is
always < gm1. If gm2ro1>>1, the
difference is small. The main point here
is that the cascode configuration has
little effect on the transconductance
since the overall GM for the CS is gm.
10
Another way of deriving to this
conclusion is by inspecting the circuit.
For CG,
Ri =1/gm.
The current gm1vi will mostly flow
through this Ri rather than ro1 as
1/ gm << ro1 .
For a CG,
ai = 1
Hence, the output current will then be
the same as the input current to the
CG, which is gm1vi.
GM = io /vi = gm1vi /vi = gm . m1 gs1g v
R
o2r
2D2G
+ov
1S
+iv
o1r
oi
1G 1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs1v
+
gs2v
+
11
t
Ot
v 0i
vR =
i
When vi=0, gm1vi=0.
ro2t m2 ds1
o2
r t ds1o2
t ds1m2t ds1
o2
tm2t ds1
o2 o2
vi = -g v +
rv = v -v
v -vi = v -g +
r
1 vi = v -g - +
r r
Determining Ro
KCL at node D2, m1 gs1g v
R
o2r
2D2G
+ov
1S
+iv
o1r
oi
1G 1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs1v
+
gs2v
+
o2r
2D2G
+tv
o1r
ti
1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs2v
+
oR
12
ds1 t o1
tm2t t o1
o2 o2
o1o1 m2t o2 t
o2
O o2 o1 o2 m2 o1
O m2 o1 o2
v =i r
1 vi = i r -g - +
r r
ri 1+r g + r = v
r
R = r +r r g +r
R g r r
KCL at node D2,
o2r
2D2G
+tv
o1r
ti
1 2,D S
ds1v+
m2 gs2
m2 s2
g vg v
gs2v
+
oR
tm2t ds1
o2 o2
1 vi = v -g - +
r r
13
The output resistance can further be increased by using more
than one level of cascoding. However, number of levels of
cascoding is limited by the power supply voltage and signal
swing requirements.
This equation shows that the MOS cascode increases the output
resistance by a factor of about gm2ro as the RO for CS is ro if RD is
not included.
vo M O
vo m1 m2 o1 o2
2m ovo m1 m2 o1 o2
a = -G R
a = -g g r r
a = - g r if g g and r r
O m2 o1 o2R g r r
14
Two-stage Amplifier (Cascade)
BJT Cascade
B1 11 12
B2 21 22
i
C2
C1
π1,2
o1,2
m1,2
R = R //R =5kΩ
R = R //R =5kΩ
R =1kΩ
R = 20kΩ
R =10kΩ
r =1500Ω
r =33.333Ω
g = 26.67mS
Given :
Find : (a)
(b)
(c)
(d)
(e)
ov2
o1
va
v
o1v1
in
va
v
ov
i
va
v
in2Z
in1Z
1T2T
+inv EC
o1v
+
+iv
iR iC
12R C1R
11R ER
2C
22RC2R
ov
+
o1Z
in1Z
in2Z
21R
CCV
15
+
inv
o1v
+
12R
C1R
11R
22R C2R
ov
+
o1Z in2Zin1Z
1r
m1 ing v
o1r 21R 2r
m2 o1g v
o2r
iR1B 1 2,C B o1i
+iv
1E 2E
2C
1T2T
+inv EC
o1v
+
+iv
iR iC
12R C1R
11R ER
2C
22RC2R
ov
+
o1Z
in1Z
in2Z
21R
CCV
16
(a) Final stage voltage gain, v2a
ov2
o1
m2 o1 o2 C2
v2o1
v2
v2
va =
v
-g v r //Ra =
v
a = -26.67m 33.333k//20k
a = -333.37
+
inv
o1v
+
12R
C1R
11R
22R C2R
ov
+
o1Z in2Zin1Z
1r
m1 ing v
o1r 21R 2r
m2 o1g v
o2r
iR1B 1 2,C B o1i
+iv
1E 2E
2C
17
(b) Final stage input impedance, in2Z
// //
// 1.154
o1in2
o1
in2 21 22 2
in2
vZ
i
Z R R r
Z 5k 1500 k
(c) Initial stage voltage gain, v1a
o1v1
in
m1 in o1 C1 21 22 π2
v1in
v1
va =
v
-g v r //R //R //R //ra =
va = -26.76
+
inv
o1v
+
12R
C1R
11R
22R C2R
ov
+
o1Z in2Zin1Z
1r
m1 ing v
o1r 21R 2r
m2 o1g v
o2r
iR1B 1 2,C B o1i
+iv
1E 2E
2C
18
(d) Amplifier input impedance, Zin1
// //
inin1
i
in1 11 12 1
in1
vZ
iZ R R r
Z 5k//1500=1.154k
(e) // //
// //
11 12 1in i
11 12 1 i
in
i
R R rv vR R r R
v 5k//1500=0.5357
v 5k//1500 1k
+
inv
o1v
+
12R
C1R
11R
22R C2R
ov
+
o1Z in2Zin1Z
1r
m1 ing v
o1r 21R 2r
m2 o1g v
o2r
iR1B 1 2,C B o1i
+iv
1E 2E
2C
19
Overall voltage gain of the cascaded amplifier, av
0.5357 4778.97
o in o1 ov
i i in o1
v v1 v2
v v v vav v v v
a a a
The total gain of the cascaded amplifier is the multiplication of the
gain at each stage of the cascaded network.
+
inv
o1v
+
12R
C1R
11R
22R C2R
ov
+
o1Z in2Zin1Z
1r
m1 ing v
o1r 21R 2r
m2 o1g v
o2r
iR1B 1 2,C B o1i
+iv
1E 2E
2C
ii
20
Find (a) Voltage gain ratio
(b) The current gain ratio
Lv
i
vav
Lii
iai
+inv
+iv
12R
D1R11R
CC
22R
D2R
Lv
+
oRinR
21R
1M2M
LR
CC
CCii Li
DDV
MOSFET Cascade
21
+inv
+iv
12R
D1R11R
CC
22R
D2R
Lv
+
oRinR
21R
1M2M
LR
CC
CCii Li
DDV
+gs1v
gs2v
+12R11R 22R
+
oRinR
m1 gs1g v
o1r 21R
m2 gs2g v
o2r
1G o1i
+iv
D1R
Lv
LR
ii Li2G 2D1D
1S
D2R
2S
22
(a) Voltage gain ratio
L m2 gs2 o2 D2 Lv2
gs2 gs2
v2 m2 o2 D2 L
gs2 m1 gs1 o1 D1 21 22v1
gs1 gs1
v1 m1 o1 D1 21 22
v -g v r //R //Ra = =
v v
a = -g r //R //R
v -g v r //R //R //Ra = =
v v
a = -g r //R //R //R
+gs1v
gs2v
+12R11R 22R
+
oRinR
m1 gs1g v
o1r 21R
m2 gs2g v
o2r
1G o1i
+iv
D1R
Lv
LR
ii Li2G 2D1D
1S
D2R
2S
gs1 i
L gs2 L gs1v
i gs1 gs2 i
m1 m2 o1 o2 D1 21 22 D2 L
vo1 D1 21 22 o2 D2 L
v = v
v v v va = = × ×
v v v v
g g r r R //R //R R //Ra =
r + R //R //R r + R //R
23
L 11 12 v 11 12Li
i L i L
m1 m2 o1 o2 D1 21 22 D2 L
vo1 D1 21 22 o2 D2 L
m1 m2 o1 o2 D1 21 22 D2 L 11 12
io1 D1 21 22 o2 D2 L L
v R //R a R //Ria = = =
i R v R
g g r r R //R //R R //Ra =
r + R //R //R r + R //R
g g r r R //R //R R //R R //Ra =
r + R //R //R r + R //R R
(b) The current gain ratio,
+gs1v
gs2v
+12R11R 22R
+
oRinR
m1 gs1g v
o1r 21R
m2 gs2g v
o2r
1G o1i
+iv
D1R
Lv
LR
ii Li2G 2D1D
1S
D2R
2S