Designing Circuits – Synthesis -...
Transcript of Designing Circuits – Synthesis -...
MAE140 Linear Circuits190
Designing Circuits – Synthesis - Lego
Port = a pair of terminals to a cctOne-port cct; measure I(s) and V(s) at same port
Driving-point impedance = input impedance = equiv impedance =Z(s)
Two-portsTransfer function; measure input at one port, output at
another
I(s)
V(s)+
-sCR
sLsIsVsZ
++==
!11
)()()(
I1(s)
V1(s)+
-V2(s)
I2(s)+
-
InputsOutputs
MAE140 Linear Circuits191
Example 11-2, T&R, 6th ed
!
TV(s) =
V2(s)
V1(s)
=R
1
R1+1sC
1
=s
s+1R
1C
1
Transfer function?
Input impedance?
!
Z(s) =V
1(s)
I1(s)
= R1+1sC
1
MAE140 Linear Circuits192
Cascade Connections
We want to apply a chain rule of processing
When can we do this by cascade connection of OpAmp ccts?Cascade means output of ccti is input of ccti+1
This makes the design and analysis much easier
This rule works if stage i+1 does not load stage iVoltage is not changed because of next stage
EitherOutput impedance of source stage is zero
OrInput impedance of load stage is infinite
Works well if Zout,source<<Zin,load
)(...)()()()( 321 sTsTsTsTsT VkVVVV !!!!=
MAE140 Linear Circuits193
Cascade Connections
Look for chain rule+_ R1V1(s)R2
2
1sC
1
1sC
V2(s) V3(s)
+++
Mesh analysis
!
TVtotal(s)=?T
V 1(s)"T
V 2(s) =
R1C
1s
R1C
1s+1
"1
R2C
2s+1
=R
1C
1s
R1R
2C
1C
2( )s 2 + R1C
1+ R
2C
2( )s+1
I2(s)I1(s)
0)(1)(
)()()(1
22
2111
121111
=!!"
#$$%
&+++'
='!!"
#$$%
&+
sIsC
RRsIR
sVsIRsIRsC
!"
#$%
&
!!!!
"
#
$$$$
%
&
++'
'+=!!
"
#$$%
&
'
0)(
1
1
)()( 1
1
212
1
111
2
1 sV
RRsC
R
RRsC
sIsI
( ) ( )
( ) ( ))(
1)(1)(
)(1
)(
1222111
22121
112
23
1221211
22121
1212
2
sVsCRCRCRsCCRR
sCRsIsC
sV
sVsRCRCRCsCCRR
RCCssI
++++==
++++=
No! Why?
MAE140 Linear Circuits194
Cascade Connections – OpAmp ccts
OpAmps can be used to achieve the chain ruleproperty for cascade connectionsThe input to the next stage needs to be driven by the
OpAmp outputConsider standard configurations
Noninverting amplifierNo current drawn from V1 – no load
Inverting amplifierCurrent provided by V1(s)
Need to make sure that stage isdriven by OpAmp output toavoid loading V1(s)
V1(s)+-
V2(s)+
Z2+
Z1
V1(s) +-
Z1 Z2
V2(s)
++I(s)
)()()(
11sZsVsI =
MAE140 Linear Circuits195
OpAmp Ccts and transfer functionsNode B:
Node B:
+_V1(s) +-
Z1 Z2
V2(s)
+A B C
)()(
)()()(0)(
0)()()(
)()()(
12
12
22
11
sZsZ
sVsVsTsV
sZsVsV
sZsVsV
VB
BB
!=="=
=!
+!
+_V1(s)
-+
V2(s)+A
B
C
Z2
Z1
)()()()()()(
0)()(
)()()(
121
1
122
sZsZsZsTsVsV
sZsV
sZsVsV
VB
BB
+=!=
=+"
MAE140 Linear Circuits196
Example 11-4, T&R, 5th ed, p511
Find the transfer function from V1(s) to V2(s)
111
11
11)(sCCsR
sCRsZ1
+=+=
2211 )1)(1()( 12
++−=
CsRCsRCsRsTV
R2
R1
V1(s)
+-
1
1sC
2
1sC
V2(s)
++
11)(222
22
22
2 +=
+=
sCRR
sCRsC
RsZ
MAE140 Linear Circuits197
Circuits as Signal Processors
Design a circuit with transfer function
R1=R2=100Ω, C1=C2=1µF, C3=100µF, L=70mH, R3=1Ω
( )( )
( )24842
52
10101021042.1
+
−+=
+×+
×+
s
jsjsss
s 408408
VO(s)
R2
R1
VI(s)
+-1
1sC
2
1sC
V2(s)
+
+-+
3
1sC
R3
sL
( )( )( )LssLCR
CsRCsRCsRsTV
111
)(2
332211
12 +−×
++−
=
MAE140 Linear Circuits198
Transfer Function Design – OpAmp Stages
First order stages
α
+-
1 Κγ Κ
αγ
++
−=ssKsTV )(
Series RL design
Series RC design
1
+-
Κ !K1
!1
MAE140 Linear Circuits199
First-order stages
αγ
++
−=ssKsTV )(
1
+-
!K1
!1
K1
Parallel RL design
1
+-
!K1
!1
Κ
Parallel RC design
MAE140 Linear Circuits200
Design Example 11-20, T&R, 5th ed, p 542
Design two ccts to realize
Unrealistic component values – scaling needed
)4000)(1000(3000)( ++
=ssssTV
1000µF
+-
1Ω1Ω
+-250µF
1Ω 3Ω
Stage 1 Stage 2
[ ]100010001
1011101
)( 1
3
31 +
!=
"""
#
$
%%%
&
'
+!= !
!
!
ss
ssTV [ ][ ]40003400013)(
12 +
!=+!=
!
ss
ssTV
MAE140 Linear Circuits201
Design Example 11-19, T&R, 5th ed, p 539
Non-inverting amplifier design
Less OpAmps but more difficult designThree stage: last stage not driven
Unrealistic component values still – scaling needed
1Ω+-
1000µF
1Ω2Ω
250µF
1Ω
Stage 1VoltageDivider
Stage 2OpAmp
Stage 3VoltageDivider
)4000)(1000(3000)(
++=
ssssTV
MAE140 Linear Circuits202
Scaled Design Example 11-21, T&R, 5th ed, p 544
More realistic values for components
Need to play games with elements to scaleThe ratio formulas for TV help permit this scaling
It certainly is possible to demand a design TV which isunrealizable with sensible component values
Like a pole at 10-3 Hz
100nF
+-
10ΚΩ10ΚΩ
+-25nF
10ΚΩ 30ΚΩ
MAE140 Linear Circuits203
Second-order Stage Design
Circuit stages to yield
02!"=R 1=L KC
!= 20
11
"
KC 12=2
0!"K
+-
120!
"
K1Ω Ω
1Η !02"#
F20
1
! +-
!02
1"#
H20
1
!
F1HK1
!
TV(s) =
Ks 2 + 2"#
0s+#
0
2
MAE140 Linear Circuits204
Circuit Synthesis
Given a stable transfer function TV(s), realize it via acct using first-order and second-order stages
We are limited to stable transfer functions to keep within thelinear range of the OpAmpsThere is an exception
When the unstable TV(s) is part of a stable feedbacksystem
Come to MAE143B to find out
Transistor cct design is conceptually similar
cbsassssTV++
++= 2
2)( !"#
basssTV ++
=!")(