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ACTIVE NETWORK
ACTIVE FILTERS
Passive filters have several limitations
1. Cannot generate gains greater than one
2. Loading effect makes them difficult to interconnect
3. Use of inductance makes them difficult to handle
Using operational amplifiers one can design all basic filters, and more,
with only resistors and capacitors
The linear models developed for operational amplifiers circuits are valid, in a
more general framework, if one replaces the resistors by impedances
Ideal Op-Amp
These currents are
zero
Basic Inverting Amplifier
0V
  VVgainInfinite
0V
0 II-impedanceinputInfinite
1
1 2
0OVV
Z Z
 
2
1
1
O
Z
V V
Z
 
Linear circuit equivalent
0I
1
2
Z
Z
G 
1
1
1
Z
V
I 
EXAMPLE USING INVERTING AMPLIFIER
LOW PASS FILTER
Basic Non-inverting amplifier
1V
1V
0I 
1
1
2
10
Z
V
Z
VV


1
1
12
0 V
Z
ZZ
V


1
2
1
Z
Z
G 
01 I
EXAMPLE USING NON INVERTING CONFIGURATION
EXAMPLE SECON ORDER FILTER
2
( )V s
22 2 2
1 1 2 3
0
1/
OIN
V VV V V V
R C s R R

   
2
2 2
0
1/
O
VV
R C s
  

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Active network

  • 2. ACTIVE FILTERS Passive filters have several limitations 1. Cannot generate gains greater than one 2. Loading effect makes them difficult to interconnect 3. Use of inductance makes them difficult to handle Using operational amplifiers one can design all basic filters, and more, with only resistors and capacitors The linear models developed for operational amplifiers circuits are valid, in a more general framework, if one replaces the resistors by impedances Ideal Op-Amp These currents are zero
  • 3. Basic Inverting Amplifier 0V   VVgainInfinite 0V 0 II-impedanceinputInfinite 1 1 2 0OVV Z Z   2 1 1 O Z V V Z   Linear circuit equivalent 0I 1 2 Z Z G  1 1 1 Z V I 
  • 4. EXAMPLE USING INVERTING AMPLIFIER LOW PASS FILTER
  • 5. Basic Non-inverting amplifier 1V 1V 0I  1 1 2 10 Z V Z VV   1 1 12 0 V Z ZZ V   1 2 1 Z Z G  01 I
  • 6. EXAMPLE USING NON INVERTING CONFIGURATION
  • 7. EXAMPLE SECON ORDER FILTER 2 ( )V s 22 2 2 1 1 2 3 0 1/ OIN V VV V V V R C s R R      2 2 2 0 1/ O VV R C s   