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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
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Z. Aliyazicioglu
Electrical and Computer Engineering Department Cal Poly Pomona
ECE307-
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
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
R
C
Vi (^) Vo
Vi
Zf
Vo
Zi
OUT
2
1 2
( ) ( 1)
R H s R sR C
2
1
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
Example
+^ Vo
R
1
C
1F
R
1
Vi
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
R
20 K Vo
2
1
2
c R C
ω = =
Transfer function in jω
for gain of 10 and cutoff frequency of 500 rad/s.
From the gain
From the cutoff frequency
1
R 2 (^) = R 1 10 = 200 K Ω
j
H j
j
1
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
values, this process is called scaling
factor k m , multiplying all C by 1/k m
m R = k R ' m L = k L '
m
k
Scaling
scaling factor.
f
k
f
k
simultanously
m R = k R '^
m
f
k L L k
m f
k k
ECE 307-10 13
Op Amp Band-Pass Filters
2
1
c
c
Low-pass filter High-pass filter Inverting amp.
Vi Vo
Vi
RH
Rf CH Rf
Vo
RL
RH
CL
RL
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
1
c H
max
f
i
H j K R
ECE 307-10 15
Example:
gain 2 within the frequency between 100 and 10,000 Hz.
Use 0.1 μF capacitors
2
c L L
1
c H
6 2
L c L
−
6 1
H c L
−
f
i
f i
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
ECE 307-10 19
Example:
stop frequency between 100 and 2000 Hz. Use 0.5 μF
capacitors
1
c L L
2
c H H
2 1 For c c
1 2
c c F = Hz and F = Hz
6 1
L c L
−
6 2
H c H
−
f
i
f i
>> 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