ece 342 electronic circuits lecture 23 miller effectemlab.illinois.edu/ece342/notes/lec_23.pdf ·...
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ECE 442 – Jose Schutt‐Aine 1
Jose E. Schutt-AineElectrical & Computer Engineering
University of [email protected]
ECE 342Electronic Circuits
Lecture 23Miller Effect
ECE 442 – Jose Schutt‐Aine 2
22 Dm n ox eff n ox D
eff
W W Ig C V C IL L V
MOSFET High-Frequency Model
2 2mb m mF sb
g g gV
1/ds A DD
r V II
23gs ox ov oxC WLC WL C
gd ov oxC WL C
1
sbosb
SB
o
CCVV
1
dbodb
DB
o
CCVV
2
ECE 442 – Jose Schutt‐Aine 3
CS - High-Frequency Response
3
ECE 442 – Jose Schutt‐Aine 4
1 2 GR R R
CS - High-Frequency Response
4
ECE 442 – Jose Schutt‐Aine 5
'sig sig GR R R
'gd gd gs o gd gs m L gsI sC V V sC V g R V
'1gd gd m L gsI sC g R V
CS - High-Frequency Response
' L ds D LR r R R
5
ECE 442 – Jose Schutt‐Aine 6
'1 eq gs gd m L gssC V sC g R V
'1 Miller Capacitance eq gd m LC C g R
g sigin
g sig
R Vv
R R
' o m L gsV g R V
Define Ceq such thatCS – Miller Effect
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ECE 442 – Jose Schutt‐Aine 7
11 /
G siggs
G sig o
R VV
R R jf f
fo is the corner frequency of the STC circuit
'
12
oin sig
fC R
'1 Miller
in gs eq gs gd m LC C C C C g R
CS – Miller Effect
7
ECE 442 – Jose Schutt‐Aine 8
' 11 /
o Gm L
sig G sig o
V R g RV R R jf f
1 /
o M
sig H
V AV jf f
'
12
H oin sig
f fC R
CS – Miller Effect
8
ECE 442 – Jose Schutt‐Aine 9
Rsig = 100 k, RG=4.7 M, RD =15 k, gm=1mA/V, rds=150 k, RL=10 kCgs=1 pF and Cgd=0.4 pF
' 4.7 1 7.14 74.7 0.1
GM m L
G sig
RA g RR R
': 1eq M m L gdMiller Cap C C g R C
Example
' 150 15 15 7.14 L ds D LR r R R k
0.4 1 7.14 3.26MC pF
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ECE 442 – Jose Schutt‐Aine 10
1
2Hin sig G
fC R R
Upper 3 dB frequency is at:
1.0 3.26 4.26 inC pF
12 6
1 3.822 4.26 10 0.1 4.7 10Hf kHz
3.82Hf kHz
Example (cont’)
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ECE 442 – Jose Schutt‐Aine 11
CE High-Frequency Model
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ECE 442 – Jose Schutt‐Aine 12
CE High-Frequency Model
1 2BR R R
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ECE 442 – Jose Schutt‐Aine 13
' B
sig sigB sig x sig B
rRV VR R r r R R
CE High-Frequency Model
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ECE 442 – Jose Schutt‐Aine 14
'L o C LR r R R
'o m LV g v R
'sig x sig BR r r R R
CE High-Frequency Model
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ECE 442 – Jose Schutt‐Aine 15
The left hand side of the circuit at XX’ knows the existence of C only through the current I replace C with Ceq from base to ground
Bipolar Miller Effect
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ECE 442 – Jose Schutt‐Aine 16
'o m LI sC v v sC v g R v
'1 m LI sC g R v
Bipolar Miller Effect
'1eq m LsC v I sC g R v
'1 , Miller capacitance for BJTeq m LC C g R
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ECE 442 – Jose Schutt‐Aine 17
Bipolar Miller Effect
' 11 /sig
o
v vjf f
'
12o
in sig
fC R
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ECE 442 – Jose Schutt‐Aine 18
'1in eq m Lwhere C C C C C g R
' 1
1 /o m LB
sig B sig ox sig B
V r g RRV R R jf fr r R R
Bipolar Miller Effect (cont’)
11 /
oM
sig o
V AV jf f
'
12H o
in sig
f fC R
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ECE 442 – Jose Schutt‐Aine 19
CS – Miller Effect – Exact Analysis
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ECE 442 – Jose Schutt‐Aine 20
ii
1GR
DD
1GR
gg
1GR
dsds
1gr
'i D m gdo
' ' 2 'i i g gs gd gd D i g gd m D gd gs D
G R g sCvv G G s C C sC R G G sC g R s C C R
CS – Miller Effect – Exact Analysis
'D D ds
D ds
1R R rG g
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ECE 442 – Jose Schutt‐Aine 21
2 ' 'gd gs D gd m D gs ms C C R sC g R or sC g
We neglect the terms in s2 since
'
i D m gdo' '
i i g gs gd m D gd D i g
G R g sCvv G G s C C 1 g R C R G G
ii
1RG
If we multiply through by
CS – Miller Effect – Exact Analysis
21
Miller
ECE 442 – Jose Schutt‐Aine 22
'D m gdo
' 'i i g i gs gd m D gd D s g
R g sCvv 1 R G s R C C 1 g R C R 1 R G
i g
H ' 'i gs gd m D gd D i g
1 R Gf
2 R C C 1 g R C R 1 R G
From which we extract the 3-dB frequency point
CS – Miller Effect – Exact Analysis
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ECE 442 – Jose Schutt‐Aine 23
H ' 'i gs gd m D gd D
1f2 R C C 1 g R C R
H 'gd D
1f2 C R
If Gg is negligible
If Ri =0
CS – Miller Effect – Exact Analysis
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ECE 442 – Jose Schutt‐Aine 24
ii
1GR
CC
1GR
1gr
oo
1gr
BJT-CE – Miller Effect – Exact Analysis
'C C o
C o
1R R rG g
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ECE 442 – Jose Schutt‐Aine 25
's C mo
' ' 2 'i i C i m C C
G R g sCvv G g s C C sC R G g sC g R s C C R
BJT-CE – Miller Effect – Exact Analysis
25
ECE 442 – Jose Schutt‐Aine 26
2 ' 'C m C ms C C R sC g R or sC g
'i C mo
' 'i i m C C i
G R g sCvv G g s C C 1 g R C R G g
'C mo
' 'i i i m D C i
R g sCvv 1 R g s R C C 1 g R C R 1 R g
BJT-CE – Miller Effect – Exact Analysis
We neglect the terms in s2 since
If we multiply through by ii
1RG
26
Miller
ECE 442 – Jose Schutt‐Aine 27
i
H ' 'i m C C i
1 R gf2 R C C 1 g R C R 1 R g
H 'C
1f2 C R
If Ri = 0
BJT-CE – Miller Effect – Exact Analysis
27
ECE 442 – Jose Schutt‐Aine 28
Example For the discrete common-source MOSFET amplifier shown, the transistor has VT = 1V, Cox(W/L) = 0.25 mA/V2, = 0, Cgs = 3 pF, Cgd = 2.7 pF and VA = 20 V. Assume that the coupling capacitors are short circuits at midband and high frequencies.
(a) Find the 3dB bandwidth if Ri = 0
(b) Find the 3dB bandwidth if Ri = 10 k
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ECE 442 – Jose Schutt‐Aine 29
If Ri =0, 3 '
12dB
gd D
fC R
20 131.516
Ads
D
Vr k
I
' 13 2 1.736D D dsR R r k
3 12 3
1 33.952 2.7 10 1.736 10dBf MHz
Example – Part (a)
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ECE 442 – Jose Schutt‐Aine 30
If Ri =50 k,
Example Part (b)
'm Dg R 0.870 1.736 1.51
H ' 'i gs gd m D gd D
1f2 R C C 1 g R C R
H1f 32.27 kHz
2 50 3 2.7 1 1.51 2.7 1.736
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