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9-1
Lecture 9
RC Filters
9-2
Outlines of Filter Design
Filter
input output
Filtering:
Certain desirable features are retained
Other undesirable features are suppressed
9-3
Filters
Filters have the property of removing unwanted frequencies
from our signal.
Classes: Passive (made of capacitors, resistors, inductors)
Active (involving an amplifier)
Types: Low-Pass (remove high frequencies)
High-Pass (remove low frequencies or DC)
Band-Pass (remove a range of frequencies on
two sides)
Notch (removes frequencies in the middle)
9-4
Classification of Filters
Signal Filter
Analog Filter Digital Filter
Element Type Frequency Band
Active Passive Low-Pass
High-Pass
Band-Pass
Band-Reject
All-Pass
9-5
Filters – Type of filters
http://www.ece.eps.hw.ac.uk/~pmr/teaching/ae/lectures/circuits1.htm
Passive
filters
9-6
Terminology in Filter Design
• Signal-To-Noise Ratio (S/N)
• Bandwidth
the range of frequencies of |G(jw)|>0.707
• Cutoff Frequency
the end of pass-band frequency
• Break-point of a filter
the point with a gain of -3dB
dB
W
W
N
S
N
S
⎟⎟
⎠
⎞
⎜⎜
⎝
⎛
⋅= log10
9-7
RC Filters
In combination with a resistor, a capacitor’s variation in reactance with frequency can be
used to construct a simple low-pass or high-pass filter:
R
RC
C
Vin Vout Vin Vout
High-pass filter Low-pass filter
fC
X
XRZ
Z
R
VV
C
C
π2
1
22
inout
=
+=
⋅=
fC
X
XRZ
Z
X
VV
C
C
C
π2
1
22
inout
=
+=
⋅=
9-8
Passive Low-Pass Filter
• The pass-band is from
0 to some frequency
wp.
• Its stop-band extends
form some frequency
ws, to infinity.
• In practical circuit
design, engineers often
choose amplitude gain
of 0.95 for passive RC
filters:
ωωp ωs
)( ωjH
Vout
Vin
C
R
VVoutoutVVinin RL
9-9
Passive High-Pass Filter
• Its stop-band is form 0
to some frequency ws
• The pass-band is from
some frequency wp to
infinity.
• In practical circuit
design, engineers
choose amplitude gain
of 0.95 for passive CR
filters:
ωωs ωp
)( ωjH
Vout
Vin
R
C
VVoutoutVVinin
9-10
Design of Passive Filters
( )
1
1
+
=
ω
ω
jRC
jH
( )
1
1
+
=
RCs
sH
Transfer Function
( )2
1
1
ωRCV
V
in
out
+
=
The amplitude response:
πτπ 2
1
2
1
3 ==
RC
f dB
The 3dB break-point is at:
LF
L
ZZ
Z
G
+
=
The amplitude gain:
C
R
VVoutoutVVinin RL
9-11
Guideline of Pass Filter Design
R
( )
1
1
+
=
s
sH
τ
Transfer Function
C VVoutoutVVinin RL
RC=τ
Time Constant
Select resistor based on amplitude gain:
95.0=
+
=
LF
L
ZZ
Z
G
LLF RZRZ ⋅==≈ 053.0
95.0
05.0
Select capacitor based on cut-off freq:
dBRfR
C
32
1
π
τ
==
9-12
Higher Order Filters
C
R
VVoutoutVVinin
First Order RC Low Pass Second Order RC Low Pass
C2 VVoutoutVVinin
C1
R1 R2
The higher the order of the filter,
the closer it approaches ideal characteristics.
9-13
Active Filters
• Active filters employ Op-Amps to attenuate
select frequencies and amplify signal during
filtering process.
• Q factor of a filter is defined as the ratio of
the center frequency fc to the bandwidth fH -
fL :
( )LH
C
ff
f
Q
−
=
9-14
Active filters- cascading low pass filters
First
order
Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001.
Second order
3rd order
5th order
9-15
Low-Pass Active Filter
+
-
R1
RF
R2
C1
C2
Passive filters take up lots of space in a circuit and
cause signal to be lost. Combining a passive RC
filter with an op amp for amplification creates
what is known as an active filter. By “active”
we mean that the filter requires power
to operate.
Here is an example of an
active low-pass filter. The signal
is provided to the noninverted
input through an RC low-pass filter
made up of R2 and C2. Feedback to
limit gain comes through C1 and RF. The
parallel combination of C1 and RF presents
an impedance which decreases with increasing
frequency, meaning that more negative feedback is provided to the inverting input at
higher frequencies, reducing gain at those frequencies.
9-16
Design of Low Pass Active Filters
Example:
Design a low pass filter with
cut-off frequency of 5 kHz,
and DC gain of 10:
Two equations, three unknowns
-
+
Vin
Vout
R1
RF
A
B
C2
Transfer Function:
0
0
..
ω
ω
+
=
s
KFT LP
( )22
1
CR
f
F
H π=
The -3 dB cut-off frequency:
1R
R
K F
LP −=
The DC gain:
9-17
High-Pass Active Filter
+
-
R1
RF
R2
C1 C2
R3
Here is an example of an active high-pass
filter. C2 and R2 make up an RC high-pass
filter at the input of the op amp. R3 provides
a path for the input when the frequency is
too low for C2 to freely conduct. When the
input signal passes through R3 instead of
into the amplifier, the output is tied directly to the input and the gain is reduced. So, this
amplifier has low gain at low frequencies and higher gain at high frequencies. C1 prevent
any DC at the input from being coupled to the output.
9-18
Design of High Pass Active Filters
Vout
-
+
Vin
R1
RF
A
B
C1
The -3 dB cut-off frequency:
The DC gain:
Two equations, three
unknowns
Select one component based
on other conditions, and
determine the values of the
other two components.
( )112
1
CR
fH π=
1R
R
K F
HP =
Transfer Function:
0
..
ω+
=
s
s
KFT HP
9-19
Filter Class
• A filter of a given order can be made to approximate to
ideal characteristics in a number of ways, depending on
the values of the filter components (or say: depending on
the filter class.
• Two useful classes are Butterworth (maximally flat) and
Chebyshev (equal-ripple) filters (n is the filter order)
n
C
in
out
f
fV
V
2
1
1
⎟
⎠
⎞⎜
⎝
⎛+
=Butterworth Filter
Chebyshev Filter
⎟
⎠
⎞⎜
⎝
⎛+
=
C
n
in
out
f
fCE
V
V
22
1
1
9-20
Higher Order Active Filters
Vout
-
+
Vin
R2
Rb
C1
R1
Ra
C2
Gain=K
Filter Class R1 R2 C1 C2 K
Buterworth
3.01 dB at ωH
1.00 1.00 1.00 1.00 1.59
Chebyshev
1 dB ripple
1.00 1.00 0.94 0.97 2.00
The above list gives the gain and
component valves for one of the
many choices for ωH=1. You may
find more combinations from
filter design handbook(s).
9-21
Active Filters– High Pass Filters
Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001.
High passLow pass
9-22
Active Filters – Band Pass Filter
Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001.
9-23
Active Filters – Band Reject Filter
Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001.
Passive band reject filter
Active band
reject filter
9-24
References
• Op Amp for everyone, Ron Mancini, Ed,
Texas instrument, 2001.

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09 rc filters

  • 1. 9-1 Lecture 9 RC Filters 9-2 Outlines of Filter Design Filter input output Filtering: Certain desirable features are retained Other undesirable features are suppressed
  • 2. 9-3 Filters Filters have the property of removing unwanted frequencies from our signal. Classes: Passive (made of capacitors, resistors, inductors) Active (involving an amplifier) Types: Low-Pass (remove high frequencies) High-Pass (remove low frequencies or DC) Band-Pass (remove a range of frequencies on two sides) Notch (removes frequencies in the middle) 9-4 Classification of Filters Signal Filter Analog Filter Digital Filter Element Type Frequency Band Active Passive Low-Pass High-Pass Band-Pass Band-Reject All-Pass
  • 3. 9-5 Filters – Type of filters http://www.ece.eps.hw.ac.uk/~pmr/teaching/ae/lectures/circuits1.htm Passive filters 9-6 Terminology in Filter Design • Signal-To-Noise Ratio (S/N) • Bandwidth the range of frequencies of |G(jw)|>0.707 • Cutoff Frequency the end of pass-band frequency • Break-point of a filter the point with a gain of -3dB dB W W N S N S ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ ⋅= log10
  • 4. 9-7 RC Filters In combination with a resistor, a capacitor’s variation in reactance with frequency can be used to construct a simple low-pass or high-pass filter: R RC C Vin Vout Vin Vout High-pass filter Low-pass filter fC X XRZ Z R VV C C π2 1 22 inout = += ⋅= fC X XRZ Z X VV C C C π2 1 22 inout = += ⋅= 9-8 Passive Low-Pass Filter • The pass-band is from 0 to some frequency wp. • Its stop-band extends form some frequency ws, to infinity. • In practical circuit design, engineers often choose amplitude gain of 0.95 for passive RC filters: ωωp ωs )( ωjH Vout Vin C R VVoutoutVVinin RL
  • 5. 9-9 Passive High-Pass Filter • Its stop-band is form 0 to some frequency ws • The pass-band is from some frequency wp to infinity. • In practical circuit design, engineers choose amplitude gain of 0.95 for passive CR filters: ωωs ωp )( ωjH Vout Vin R C VVoutoutVVinin 9-10 Design of Passive Filters ( ) 1 1 + = ω ω jRC jH ( ) 1 1 + = RCs sH Transfer Function ( )2 1 1 ωRCV V in out + = The amplitude response: πτπ 2 1 2 1 3 == RC f dB The 3dB break-point is at: LF L ZZ Z G + = The amplitude gain: C R VVoutoutVVinin RL
  • 6. 9-11 Guideline of Pass Filter Design R ( ) 1 1 + = s sH τ Transfer Function C VVoutoutVVinin RL RC=τ Time Constant Select resistor based on amplitude gain: 95.0= + = LF L ZZ Z G LLF RZRZ ⋅==≈ 053.0 95.0 05.0 Select capacitor based on cut-off freq: dBRfR C 32 1 π τ == 9-12 Higher Order Filters C R VVoutoutVVinin First Order RC Low Pass Second Order RC Low Pass C2 VVoutoutVVinin C1 R1 R2 The higher the order of the filter, the closer it approaches ideal characteristics.
  • 7. 9-13 Active Filters • Active filters employ Op-Amps to attenuate select frequencies and amplify signal during filtering process. • Q factor of a filter is defined as the ratio of the center frequency fc to the bandwidth fH - fL : ( )LH C ff f Q − = 9-14 Active filters- cascading low pass filters First order Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001. Second order 3rd order 5th order
  • 8. 9-15 Low-Pass Active Filter + - R1 RF R2 C1 C2 Passive filters take up lots of space in a circuit and cause signal to be lost. Combining a passive RC filter with an op amp for amplification creates what is known as an active filter. By “active” we mean that the filter requires power to operate. Here is an example of an active low-pass filter. The signal is provided to the noninverted input through an RC low-pass filter made up of R2 and C2. Feedback to limit gain comes through C1 and RF. The parallel combination of C1 and RF presents an impedance which decreases with increasing frequency, meaning that more negative feedback is provided to the inverting input at higher frequencies, reducing gain at those frequencies. 9-16 Design of Low Pass Active Filters Example: Design a low pass filter with cut-off frequency of 5 kHz, and DC gain of 10: Two equations, three unknowns - + Vin Vout R1 RF A B C2 Transfer Function: 0 0 .. ω ω + = s KFT LP ( )22 1 CR f F H π= The -3 dB cut-off frequency: 1R R K F LP −= The DC gain:
  • 9. 9-17 High-Pass Active Filter + - R1 RF R2 C1 C2 R3 Here is an example of an active high-pass filter. C2 and R2 make up an RC high-pass filter at the input of the op amp. R3 provides a path for the input when the frequency is too low for C2 to freely conduct. When the input signal passes through R3 instead of into the amplifier, the output is tied directly to the input and the gain is reduced. So, this amplifier has low gain at low frequencies and higher gain at high frequencies. C1 prevent any DC at the input from being coupled to the output. 9-18 Design of High Pass Active Filters Vout - + Vin R1 RF A B C1 The -3 dB cut-off frequency: The DC gain: Two equations, three unknowns Select one component based on other conditions, and determine the values of the other two components. ( )112 1 CR fH π= 1R R K F HP = Transfer Function: 0 .. ω+ = s s KFT HP
  • 10. 9-19 Filter Class • A filter of a given order can be made to approximate to ideal characteristics in a number of ways, depending on the values of the filter components (or say: depending on the filter class. • Two useful classes are Butterworth (maximally flat) and Chebyshev (equal-ripple) filters (n is the filter order) n C in out f fV V 2 1 1 ⎟ ⎠ ⎞⎜ ⎝ ⎛+ =Butterworth Filter Chebyshev Filter ⎟ ⎠ ⎞⎜ ⎝ ⎛+ = C n in out f fCE V V 22 1 1 9-20 Higher Order Active Filters Vout - + Vin R2 Rb C1 R1 Ra C2 Gain=K Filter Class R1 R2 C1 C2 K Buterworth 3.01 dB at ωH 1.00 1.00 1.00 1.00 1.59 Chebyshev 1 dB ripple 1.00 1.00 0.94 0.97 2.00 The above list gives the gain and component valves for one of the many choices for ωH=1. You may find more combinations from filter design handbook(s).
  • 11. 9-21 Active Filters– High Pass Filters Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001. High passLow pass 9-22 Active Filters – Band Pass Filter Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001.
  • 12. 9-23 Active Filters – Band Reject Filter Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001. Passive band reject filter Active band reject filter 9-24 References • Op Amp for everyone, Ron Mancini, Ed, Texas instrument, 2001.