Active Filter Circuits: Design and Analysis with Op Amps, Exams of Design

Active filter can produce band-pass and band-reject filter without using inductor. ... active Low-pass filter for gain of 1 and cutoff frequency of 1 rad/s.

Typology: Exams

2021/2022

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Active Filter Circuits
Z. Aliyazicioglu
Electrical and Computer Engineering Department
Cal Poly Pomona
ECE307-10
ECE 307-10 2
Active Filter Circuits
Introduction
Filter circuits with RLC are passive filter circuit
Use op amp to have active filter circuit
Active filter can produce band-pass and band-reject filter without
using inductor.
Passive filter incapable of amplification. Max gain is 1
Active filter capable of amplification
The cutoff frequency and band-pass magnitude of passive filter
can change with additional load resistance
This is not a case for active filters
We look at few active filter with op amps.
We look at that basic op amp filter circuits can be combined to
active specific frequency response and to attain close to ideal
filter response
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pf4
pf5
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pf9
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Active Filter Circuits

Z. Aliyazicioglu

Electrical and Computer Engineering Department Cal Poly Pomona

ECE307-

Active Filter Circuits

Introduction

Filter circuits with RLC are passive filter circuit

Use op amp to have active filter circuit

Active filter can produce band-pass and band-reject filter without

using inductor.

Passive filter incapable of amplification. Max gain is 1

Active filter capable of amplification

The cutoff frequency and band-pass magnitude of passive filter

can change with additional load resistance

This is not a case for active filters

We look at few active filter with op amps.

We look at that basic op amp filter circuits can be combined to

active specific frequency response and to attain close to ideal

filter response

ECE 307-10 3

Active Filter Circuits =

Transfer function of the circuit

First-Order Low-pass Filters

( )

f

i

Z H s Z

2 2 2

1 1

1 || 1 ( )

R R SC sR C H s R R

− −

= =

R

  • OUT

R

C

Vi (^) Vo

Vi

Zf

Vo

Zi

OUT

2

1 2

( ) ( 1)

R H s R sR C

2

1

R

K

R

2

1 c R C

ω =

( ) ( )

c

c

H s K s

ω

ω

= −

The Gain Cutoff frequency

Transfer function in jω

c

H j K

j

Active Filter Circuits

Example

+^ Vo

R

1

C

1F

  • OUT

R

1

Vi

  • Find R 2 and C values in the following

active Low-pass filter for gain of 1

and cutoff frequency of 1 rad/s.

2

1

1

R K R

= =

2

1 c^1 R C

ω = =

1 ( )

(1 ) 1

H j

j

ω ω

=

R 2 (^) = R 1 = Ω 1 From the gain

From the cutoff frequency

2

1 C 1 F R

= =

2

ECE 307-10 7

Example

C

0.1 uF

R

200K

Vi

  • OUT +

R

20 K Vo

2

1

R

K

R

2

c R C

ω = =

Transfer function in jω

  • Find R 2 and R 1 values in the above active High-pass filter

for gain of 10 and cutoff frequency of 500 rad/s.

From the gain

From the cutoff frequency

1

R K

C

R 2 (^) = R 1 10 = 200 K Ω

j

H j

j

1

Active Filter Circuits

Example

>> w=1:10000;

>> h=20log10(10(abs((jw/ )./(1+jw/500)))); >> semilogx(w,h) >> grid on >> xlabel('\omega(rad/s)') >> ylabel('|H(j\omega)| dB') >>

ECE 307-10 9

Scaling

  • In filter design, we can transform RLC values in to realistic

values, this process is called scaling

  • Two types of scaling, magnitude and frequency scaling
  • In magnitude scaling, we multiply all L and R by scaling

factor k m , multiplying all C by 1/k m

m R = k R ' m L = k L '

m

C

C

k

  • k m ,is positive real number

Active Filter Circuits

Scaling

  • frequency scaling, we multiply all L, C by 1/k f where k f is

scaling factor.

R '= R '

f

L

L

k

f

C

C

k

  • A circuit can be scaled in both magnitude and frequency in

simultanously

m R = k R '^

m

f

k L L k

m f

C

C

k k

ECE 307-10 13

  • Three components
  • A unity gain low-pass filter, cutoff frequency is ωc
  • A unity gain high-pass filter , cutoff frequency ωc
  • A gain component to provide the desired level

Op Amp Band-Pass Filters

2

1

c

c

Low-pass filter High-pass filter Inverting amp.

Vi Vo

Active Filter Circuits

  • OUT

Vi

RH

  • OUT

Rf CH Rf

Vo

RL

RH

CL

RL

  • OUT

Op Amp Band-Pass Filters

2

2 1

c f

c c i

s R H s

s s R

2

2 1

c

c c

K s H s s s

2 2 1 2 1 2

c

c c c c

K s H s

s s

0

s H s

s s

c 2 c 1

2

c L L

R C

1

c H

R CH

ω = (^0 )

max

f

i

R

H j K R

ECE 307-10 15

Example:

  • Design a band-pass filter for a graphical equalizer that has

gain 2 within the frequency between 100 and 10,000 Hz.

Use 0.1 μF capacitors

2

c L L

R C

1

c H

R CH

6 2

L c L

R

ω C π

6 1

H c L

R

ω C π

f

i

R

K

R

  • For upper cutoff frequency from LP filter
    • For gain, choose R (^) i=1KΩ

f i

R = R K = = K Ω

  • For Lower cutoff frequency from HP filter

Active Filter Circuits

From transfer function

j H j

j j

 +^   +^  

>> f=10:80000; >> w=2pif; >> H=((- 2pi10000)./(jw+2pi* 10000)).((- jw)./(jw+2pi100))( -2); >> A=20*log10(abs(H)); >> semilogx(f,A) >> grid on; >> ylabel ('A_{dB}') >> xlabel ('F (Hz)')

10 20log | ( ) | dB

A = H j ω

ECE 307-10 19

Example:

  • Design an active band-reject filter that has gain 5 and the

stop frequency between 100 and 2000 Hz. Use 0.5 μF

capacitors

1

c L L

R C

2

c H H

R C

2 1 For c c

1 2

c c F = Hz and F = Hz

6 1

L c L

R K

ω C π

6 2

H c H

R

ω C π

f

i

R

K

R

  • For gain, choose R (^) i=1KΩ

f i

R = R K = = K Ω

Active Filter Circuits

>> f=10:80000; >> w=2pif; >> H=(((- 2pi100)./(jw+2pi100)) +((- jw)./(jw+2pi2000)))(- 5); >> A=20*log10(abs(H)); >> semilogx(f,A) >> grid on; >> xlabel ('F (Hz)') >> ylabel ('A_{dB}')

1

1 2

c f

c c i

j R H j

j j R

10 20log | ( ) | dB

A = H j ω