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Gain (dB)
0BW = f cVo
-20Ideal
0.707 -40
f f 0
BW-
f 10f 100f 1000f f
LPF with different roll-off ratesBasic LPF response
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Gain (dB)
0Vo
-20
0.707 -40Passband
f c f 0
-
0.01f 0.1f f f
Basic HPF response HPF with different roll-off rates
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Vout 21 cco f f f =Centre frequency:1
Quality factor: f Q o=.
Q is an indication of the
f
. Narrow BPF: Q > 10.
Wide-band BPF: < 10.oc1 c2
BW = f c2 - f c1Damping Factor: Q DF
1=
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an op er esponse
Gain (dB) Also known as band 0
-3
re ect, or notc ter.Frequencies within a
certain BW are rejected.
f
Useful for filtering
interferin si nals.oc1 c2
BW
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Characteristics
Av Cheb shev
Bessel
Butterworth
f
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CharacteristicsButterworth: very flat amplitude response in the
phase response however is not linear. (A pole is
Chebyshev: rolloff rate > 20 dB/dec/pole;
response. esse : near p ase response, ere ore no
overshoot on the output with a pulse input; roll o ra e s < 20 ec po e.
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Advantages over passive LC filters :
high Zin and low Zout mean good isolation from source
less bulky and less expensive than inductors when dealin with low fre uenceasy to adjust over a wide frequency range without
altering desired responseDisadvantage: requires dc power supply, and could be
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The damping factor (DF)Frequencyselective +Vin Vout
the response characteristicof the filter. _
R 112
R R
DF =
R 2 Its value depends on the
General dia ram of active filter
filter. For example DF =1.414 for 2 nd order
Butterworth, hence, R 1 =0.586R 2
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R 1+ _
Vin VoutC
2 H RC =
R 1 12
1F A R= +R 2 Roll-off rate for a single-pole
filter is -20 dB/decade.Acl is selectable since DF iso tional for sin le- ole LPF
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The RC network behaves as a voltage divider supplied by v i,and hence the voltage at the non-inverting terminal of the op-amp is given as:
C i
C v v R j X +
=
Where1
2 C X
f C =
The equation for v + then reduces to:
1 2 iv
v j f R C +
= +
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We know that the output of an op-amp non-inverting amplifier
is given by: 12
1o R
v v R
+ = +
u s u ng or v rom e prev ous equa on,
i1
Fo v
fRC2 j1
1
R
R1v
+
+=o F v A=
Where,
i H v +
2 H f
R C =
f H = high cut-off frequency of the filter 1
2
1 p a s s - b a n d g a i n o f t h e f i l t e r F R
A R
= + =
obtained as
v A
( )2
1
o
i H
v f f
=
+
1t a n H
f =
and
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The operation of the low-pass filter can be verified from the
gain magnitude equation:o
F i
v A
v1. At very low frequencies, that is f > f H,
Roll-off Rate :From the gain magnitude equation, we see that, if thefrequency is increased 10 fold (1 decade), the voltage gain is
=.log 10) each time the frequency is increased by 10. Hence theroll-off rate of the first order filter in the stop band is 20
.
At cut-off frequency, f H, the gain falls by 3 dB (= 20 log 0.707).
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Example : Design a first order low-pass filter with a cut-off
frequency at 1 KHz and pass-band gain of 2. Draw thefrequency response of the circuit.
1. From the specified cut-off frequency1
Assume, C = 0.01 F2 H R C
= =
3 6H
1 12 f C 2 ( 1 0 H z ) ( 0 . 0 1 1 0 F ) R x = =
=
2. From the specified pass-band gain R
.
2F R
= + =
This implies, R 1/R 2= 1, or R 1 = R 2
Assume, R 1 = R 2 = 10K
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Frequency Response of the designed low pass filter
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Sallen Key 2nd Order LPF A second order low-pass filter provides a 40 dB/decade roll-off ratein the stop-band. The first order low-pass filter can be convertedn o a secon -or er ype s mp y y us ng an a ona ne wor
The ain of the filter is set bC
A R1 and R 2, while the high cut-off frequency (f H) is set by R A,+ _
Vin VoutA B
C A, B B
1 H f =
R 1
A B A B
The voltage gain magnitude
2
equat on s g ven as:
4
o F v A= H
Where, 12
1 p a s s - b a n d g a i n o f t h e f i l t e r F R
A R
= + =
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Filter Design Proceduresignalinputtheof frequencytheisf
1. To simplify design calculations, set R A=R B=R and C A=C B=C.
2. Choose a value of C 1 F3. Calculate the value of R using the equation
2 H R f C =
. , , 1 =0.586R 2. Choose a value of R 2 100K and calculate the
value of R 1.
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Example : Design a second order low-pass butterworth filter at a
high cut-off frequency of 1KHz. Draw the frequency response of the circuit.
1. Let R A=R B=R and C A=C B=C.
Assume C = 0.0047 F
C A = C B = 0.0047 F
3 6H2 f C 2 ( 1 0 H z ) ( 0 . 0 0 4 7 1 0 F )
R x
= =
R = 33.86K
R A = R B = 33.86K
2. For second order butterworth response we need, R1 = 0.586R 2
=, 2
R1 = 0.586R 2 = 15.82K
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Frequency Response of Designed Low Pass Filter
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CA1
Roll-off rate: -60 dB/dec
+Vin
R A1 R B1 R A2 _
R 1CB1 _ CA2 out
R 23
R 2 oles 1 ole
Third-order (3-pole) configuration
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ng e o e g ass er
C Rolloff
rate,
and
+ _
Vin Vout
R
ormu as or c , an AF are similar to
R 1 t ose
or
.Ideally, a HPF passes R 2 all frequencies above
f c. However,
the
op
amp has an upper frequency limit.
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R AAgain, formulas and
+Vin Vout
BA roll-off rate are similar to those for 2nd-order
_
R 1R B
.To obtain higher roll-
R 2
,can be cascaded.
Basic Sallen-Keysecon -or er HPF
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+Vin
A1
VR A2
_
R 1
R A1 _ CA2
R 23
R Av (dB)
0-3
f LP response
oc1 c2
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Cascading a HPF and a LPF to yield a band pass
c1 c2 sufficiently separated. Hence the resulting
Note that f c1 is the critical frequency for the HPF c2
.Another BPF configuration is the multiple
ee ac w c as a narrower an w and needing fewer components
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C1 Making C 1 = C 2 = C,
_ R 1
2C2
321
31
21
R R R R R
C f o
+=
+
_ n out
R 3Q = f o/BW
;2 21
oooC f
Q R
CA f Q
R ==
2 R
Max. gain:
)2(2 23 oo AQC f Q
R
=
12 Ro
A < 2 2
R 1, C 1 - LP sectionR 2, C 2 - HP section
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Filter
C1The multiple-feedback
R 12
C2
its BP counterpart. For fre uencies between f
+
_ n out
and f c2 the op-amp willtreat V in as a pair of
R 4 common-mode signalsthus rejecting themWhen
C = C =C .1
f o =
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er esponse easuremen s
Discrete Point
Measurement:
Feed
a sine
wave
to t e ter nput w t a vary ng requency ut a constant voltage and measure the output
vo tage at
eac
requency
po nt. A faster way is to use the swept frequency method:
Sweep
Generator Filter
Spectrum
analyzer
The sweep generator outputs a sine wave whose frequency.