### A Simple Method of Designing Multiple Order All Pole Bandpass Filters by Cascading 2nd Order Sections

```Application Note 27A
June 1988
A Simple Method of Designing Multiple Order All Pole
Bandpass Filters by Cascading 2nd Order Sections
Nello Sevastopoulos
Richard Markell
INTRODUCTION
DESIGNING BANDPASS FILTERS
Filter design, be it active, passive, or switched capacitor,
is traditionally a mathematically intensive pursuit. There
are many architectures and design methods to choose
from. Two methods of high order bandpass filter design
are discussed herein. These methods allow the filter
designer to simplify the mathematical design process
and allow LTC’s switched capacitor filters (LTC®1059,
LTC1060, LTC1061,LTC1064) to be utilized as high quality
bandpass filters.
Table 1 was developed to enable anyone to design Butterworth bandpass filters. We will discuss the tables in
more detail later in this paper, but let’s first design a filter.
AN27A is the first of a series of application notes from
LTC concerning our universal filter family. Additional notes
in the series will discuss notch, lowpass and highpass
filters implemented with the universal switched capacitor
filter. An addition to this note will extend the treatment of
bandpass filters to the elliptic or Cauer forms.
This note will first present a finished design example and
proceed to present the design methodology, which relies on
tabular simplification of traditional filter design techniques.
A 4th order 2kHz Butterworth bandpass filter with a –3dB
bandwidth equal to 200Hz is required as shown in Figure 1.
Noting that (foBP/BW) = 10/1 we can go directly to Table 1
for our normalized center frequencies. From Table 1
under 4th order Butterworth bandpass filters, we go to
(foBP/BW) = 10.
L, LT, LTC, LTM, Linear Technology and the Linear logo are registered trademarks of Linear
Technology Corporation. All other trademarks are the property of their respective owners.
0
–3
200Hz
–10
GAIN (dB)
non-identical 2nd order bandpass sections to form the
familiar Butterworth and Chebyshev bandpass filters.
The second method consists of cascading identical 2nd
order bandpass sections. This approach, although “nontextbook,” enables the hardware to be simple and the
mathematics to be straightforward. Both methods will
be described here.
EXAMPLE 1—DESIGN
–20
–30
–40
–50
–60
0.5k 0.7k
1k
2k
3k 4k 5k
FREQUENCY (Hz)
10k
AN27A F01
Figure 1. 4th Order Butterworth BP Filter, foPB = 2kHz
an28f
AN27A-1
Application Note 27A
We find fo1 = 0.965 and fo2 = 1.036 (both normalized to
foBP = 1). To find our desired actual center frequencies,
we must multiply by foBP = 2kHz to obtain fo1 = 1.930kHz
and fo2 = 2.072kHz.
R42 all belong to the second of two 2nd order sections
in our example.
Our requirements are shown in the following table:
The Qs are Q1 = Q2 = 14.2 which is read directly from
Table 1. Also available from the table is K, which is the
product of each individual bandpass gain HoBP. To put it
another way, the value of K is the gain required to make
the gain, H, of the overall filter equal to 1 at foBP. Our filter
parameters are highlighted in the following table:
foBP
fo1
fo2
Qs
K
2kHz
1.93kHz
2.072kHz
Q1 = Q2 = 14.2
2.03
SECTION 2
fo1 = 1.93kHz
Q1 = 14.2
HoBP1 = 1
fo2 = 2.072kHz
Q2 = 14.2
HoBP2 = 2.03
Note that HoBP1 × HoBP2 = K and this is the reason for
choosing HoBP2 = 2.03.
For this example we choose the fo =
fCLK
50
R2
mode,
R4
so we will tie the 50/100/Hold pin on the SCF chip to V+,
generally (5V to 7V). We choose 100kHz as our clock and
calculate resistor values. Choosing the nearest 1% resistor
values we can implement the filter using Figure 3’s topology and the resistor values listed below.
HARDWARE IMPLEMENTATION
Universal switched capacitor filters are simple to implement. A bandpass filter can be built from the traditional
state-variable filter topology. Figure 2 shows this topology
for both switched capacitor and active operational amplifier
implementations. Our example requires four resistors for
each 2nd order section. So eight resistors are required
to build our filter.
2/3 LTC1061 or 1/2 LTC1064), Figure 3.
R11 = 147k
R21 = 10k
R31 = 147k
R41 = 10.7k
R12 = 71.5k
R22 = 10.7k
R32 = 147k
R42 = 10k
Our design is now complete. We have only to generate a
TTL or CMOS compatible clock at 100kHz, which we feed
to the clock pin of the switched capacitor filter, and we
should be “on the air.”
We associate resistors as belonging to 2nd order sections,
so R1x belongs to the x section. Thus R12, R22, R33 and
STATE VARIABLE SCF
SECTION 1
ACTIVE (OP-AMP) STATE VARIABLE
R4
R4
R3
R2
VIN
R1
–
HP
S
–
+
+
AGND
C
R2
BP
LP
VIN
∫
∫
R1
C
–
R
R5
–
+
R
–
+
1/2 LTC1060
1/3 LTC1061
1/4 LTC1064
+
R6
AN27A F02
3/4 LTC1014
f
R2
R3 R2
fo = CLK |
Q= |
HoHP = –R2 / R1 HoBP = –R3 / R1 HoLP = –R4 / R1
100(50) R4
R2 R4
1
R2
fO =
2πRC R4
MODE 3
Figure 2. Switched Capacitor vs Active RC State Variable Topology
an28f
AN27A-2
Application Note 27A
R41
R42
R31
R32
R21
VIN
R11
HP
–
+
+
S1A
–
–
BP
R22
LP
∫
+
fCLK
50
LP
BP
∫
–
1/2 LTC1060
fo =
–
+
∫
S1A
HP
–
R12
∫
BP
OUTPUT
AN27A F03
1/2 LTC1060
R3 R2
R2
;Q=
HoBP = –R3 /R1
R2 R4
R4
Figure 3. Two 2nd Order Sections Cascaded to Form 4th Order BP Filiter
DESIGNING BANDPASS FILTERS—THEORY BEHIND
THE DESIGN
Traditionally, bandpass filters have been designed by laborious calculations requiring some time to complete. At the
present time programs for various personal or laboratory
computers are often used. In either case, no small amount
of time and/or money is involved to evaluate, and later
test, a filter design.
Many designers have inquired as to the feasibility of cascading 2nd order bandpass sections of relatively low Q to
obtain more selective, higher Q, filters. This approach is
ideally suited to the LTC family of switched capacitor filters
(LTC1059, LTC1060, LTC1061 and LTC1064). The clock
to center frequency ratio accuracy of a typical “Mode 1”
design with non “A” parts is better than 1% in a design
that simply requires three resistors of 1% tolerance or
better. Also, no expensive high precision film capacitors
are required as in the active op amp state variable design.
We present here an approach for designing bandpass filters
using the LTC1059, LTC1060, LTC1061 or the LTC1064
which many designers have “on the air” in days instead
of weeks.
with the required characteristics (generally the Qs are too
high). We wish to explore here the use of cascaded identical
2nd order sections for building high Q bandpass filters.
For a 2nd order bandpass filter
Q=
1– G2
f/ fo
×
2
G
1– ( f / fo )
(1)
Where Q is the required filter quality factor
f is the frequency where the filter should have gain, G,
expressed in Volts/V.
fo is at the filter center frequency. Unity gain is assumed
at fo.
Example 2—Design
We wish to design a 2nd order BP filter to pass 150Hz
and to attenuate 60Hz by 50dB. The required Q may be
calculated from Equation (1):
So,Q =
(
1– 3.162×10 –3
3.162×10
–3
)
2
×
60 / 150
1– ( 60 / 150 )
2
= 150.7
Sections
This very high Q dictates a –3dB bandwidth of 1Hz.
When we want to detect single frequency tones and simultaneously reject signals in close proximity, simple 2nd
order bandpass filters often do the job. However, there are
cases where a 2nd order section cannot be implemented
Although the universal switched capacitor filters can
realize such high Qs, their guaranteed center frequency
accuracy of ±0.3%, although impressive, is not enough to
pass the 150Hz signal without gain error. According to the
an28f
AN27A-3
Application Note 27A
previous equation, the gain at 150Hz will be 1 ±26%; the
rejection, however, at 60Hz will remain at –50dB. The gain
inaccuracy can be corrected by tuning resistor R4 when
mode 3, Figure 2, is used. Also, if only detection of the
signal is sought, the gain inaccuracy could be acceptable.
This high Q problem can be solved by cascading two identical 2nd order bandpass sections. To achieve a gain, G, at
frequency f the required Q of each 2nd order section is:
Q=
1– G
f / fo
×
2
G
1– ( f / fo )
(2)
The gain at each bandpass section is assumed unity.
In order to obtain 50dB attenuation at 60Hz, and still pass
150Hz, we will use two identical 2nd order sections.
We can calculate the required Q for each of two 2nd order
sections from Equation (2):
So,Q =
1– 3.162×10 –3
3.162×10 –3
×
60 / 150
1– ( 60 / 150 )
2
= 8.5!!
With two identical 2nd order sections each with a potential error in center frequency, fo, of ±0.3% the gain error
at 150Hz is 1 ±0.26%. If lower cost (non “A” versions
of LTC1060 and LTC1064) 2nd order bandpass sections
are used with an fo tolerance of ±0.8%, the gain error at
150Hz is 1 ±1.8%! The benefits of lower Q sections are
therefore obvious.
Hardware Implementation
Mode 1 Operation of LTC1060, LTC1061, LTC1064
As previously discussed, we associate resistors with each
2nd order section, so R1x belongs to x section. Thus R12,
R22 and R23 belong to the second of the two 2nd order
sections, Figure 4.
Each section has the same requirements as shown:
fo1 = fo2 = 150Hz
Q1 = Q = 8.5
HoBP1 = HoBP2 = 1
Note that we could get gain out of our BP filter structure
by letting the product of the HoBP terms be >1 (within the
performance limits of the filter itself).
For our example using the LTC1060 we will use fo1 = fo2
= fCLK/100. So we input a 15kHz clock and tie the 50/100/
Hold pin to mid-supplies (ground for ±5V supplies).
We can implement this filter using the two sections of an
LTC1060 filter operated in mode 1. Mode 1 is the fastest
operating mode of the switched capacitor filters. It provides
Lowpass, Bandpass and Notch outputs.
Each 2nd order section will perform approximately as
shown in Figure 5, curve (a).
Implementation in mode 1 is simple as only three resistors
are required per section. Since we are cascading identical
sections, the calculations are also simple.
R31
R21
VIN
R32
S
N
–
R11
–
+
+
AGND
fo =
–
1/2 LTC1060
BP
R22
LP
R12
∫
∫
N
–
+
+
AGND
S
–
–
LP
BP
∫
∫
BP
OUTPUT
AN27A F04
1/2 LTC1060
fCLK
–R3
R3
H
=
Q=
100 oBP R1
R2
Figure 4. LTC1060 as BP Filter Operating in Mode 1
an28f
AN27A-4
Application Note 27A
We can calculate the resistor values from the indicated
formulas and then choose 1% values. (Note that we let
our minimum value be 20k.) The required values are:
R11 = R12 = 169k
R21 = R22 = 20k
R31 = R32 = 169k
Our design is complete. The performance of two 2nd order
sections cascaded versus one 2nd order section is shown
in Figure 5, curve (b). We must, however, generate a TTL
or CMOS clock at 15kHz to operate the filter.
Mode 2 Operation of LTC1060 Family
Suppose that we have no 15kHz clock source readily available. We can use what is referred to as mode 2, which
allows the input clock frequency to be less than 50:1 or
If we wish to operate our previous filter from a television
crystal at 14.318MHz we could divide this frequency by
1000 to give us a clock of 14.318kHz. We could then set
up our mode 2 filter as shown in Figure 6.
We can calculate the resistor values from the formulas
shown and then choose 1% values. The required values are:
R11, R12 = 162k
R21, R22 = 20k
R31, R32 = 162k
R41, R42 = 205k
Cascading More Than Two Identical 2Nd Order
Bp Sections
If more than two identical bandpass sections (2nd order)
are cascaded, the required Q of each section may be
shown to be:
0
BANDPASS GAIN (dB)
100:1 [fCLK/fo = 50 or 100]. This still depends on the connection of the 50/100/Hold pin.
–10
(a): ONE SECTION
–20
Q=
–30
–40
G1/n
(b): TWO SECTIONS
×
( f / fo )
2
1– ( f / fo )
(3)
where Q, G, f and fo are as previously defined and n = the
number of cascaded 2nd order sections.
–50
–60
1– G2/n
30
50
100 150
300 500
FREQUENCY (Hz)
1k
AN27A F05
Figure 5. Cascading Two 2nd Order BP Sections for Higher
Q Response
R41
R42
R31
R32
R21
VIN
R11
N
–
+
+
S
–
–
BP
R22
LP
R12
∫
∫
–
+
+
1/2 LTC1060
fo =
N
S
–
–
1/2 LTC1060
LP
BP
∫
∫
BP
OUTPUT
AN27A F06
fCLK
R2
R3
R2
1+
Q=
1+
R4
R2
R4
100
HoBP = R3 /R1
Figure 6. LTC1060 as BP Filter Operating in Mode 2
an28f
AN27A-5
Application Note 27A
The equivalent Q of the overall bandpass filter is then:
Q(identical section )
(4)
1/n
Figure 7 shows the passband curves for Q = 2 cascaded
bandpass sections where n is the number of 2nd order
The benefits can be seen for two and three cascaded sections. Cascading four or more sections increases the Q,
but not as rapidly. Nevertheless for designers requiring
high Q bandpass filters cascading identical sections is a
very real option considering the simplicity.
Simple 2nd Order Bandpass Filters
Gain and Phase Relations
The bandpass output of each 2nd order filter section of
the LTC1059, LTC1060, LTC1061 and LTC1064, closely
approximates the gain and phase response of an ideal
“textbook” filter.
G=
GAIN (dB)
(2 ) – 1
N=1
–10
N=2
–15
–20
–25
–30
N=3
–35
N=4
–40
0.4
0.6
N = NUMBER OF SECOND ORDER
Q = 2, BANDPASS SECTIONS
0.8
1
1.2
1.4
NORMALIZED FREQUENCY
1.6
AN27A F07
Figure 7. Frequency Response of n Cascaded Identical 2nd Order
Bandpass Sections
frequency and Q drift, but for system considerations,
this may not be practical.
BANDPASS OUTPUT
HoBP
GAIN (V/V)
Q equiv =
0
–3
–5
0.707 HoBP
(H oBP ) × ( ffo ) /Q
1/2
2
 2 2 2
+ ( ffo / Q ) 
 fo – f


(
fL fo fH
f(LOG SCALE)
)
Q=
G = filter gain in Volts/V
f0 = the filter’s center frequency
Q = the quality coefficient of the filter
HoBP = the maximum voltage gain of the filter
occurring at fO
fo
= –3dB bandwidth of the filter
Q
2


–1
 1
fL = fo  +   +1


2Q
 2Q

2


1
 1
fH = fo  +   +1
 2Q 
 2Q

Figure 8. Bandpass Filter Parameters
0
–10 Q = 1
BANDPASS GAIN (dB)
Figure 8 illustrates the above definitions. Figure 9 illustrates the bandpass gain, G, for various values of Q. This
figure is very useful for estimating the filter attenuation
when several identical 2nd order bandpass filters are
cascaded. High Qs make the filter more selective, and
at the same time, more noisy and more difficult to realize. Qs in excess of 100 can be easily realized with the
universal switched capacitor filters, LTC1059, LTC1060,
LTC1061 and LTC1064, and still maintain low center
fo
; f = fL fH
fH – fL o
–20
Q=2
Q=3
Q=5
Q = 10
–30
–40
–50
Q = 20
–60
–70
–80
0.1
0.3 0.5 0.7 1
3
5 7 10
NORMALIZED FREQUENCY AN27A F09
Figure 9. Bandpass Gain as a Function of Q
an28f
AN27A-6
Application Note 27A
used in multichannel systems where phase matching is
required. By way of comparison, a state variable active
bandpass filter built with 1% resistors and 1% capacitors
may have center frequency variation of ±2% resulting in
phase variations of ±2% resulting in phase variations of
±33.8° for Q = 20 and ±11.4° for Q = 5.
The phase shift, φ, of a 2nd order bandpass filter is:

 f 2 – f 2 
×Q 
φ = – arctan  o

 ffo 

The phase shift at fo is 0° or, if the filter is inverting,
it is –180°. All the bandpass outputs of the LTC1059,
LTC1060, LTC1061 and LTC1064 universal filters are
inverting. The phase shift, especially in the vicinity of fo,
depends on the value of Q, see Figure 10. By the same
argument, the phase shift at a given frequency varies
from device to device due to the fo tolerance. This is
true especially for high Qs and in the vicinity of fo. For
instance, an LTC1059A, 2nd order universal filter, has a
guaranteed initial center frequency tolerance of ±0.3%.
The ideal phase shift at the ideal fo should be –180°. With
a Q of 20, and without trimming, the worst-case phase
shift at the ideal fo will be –180° ±6.8°. With a Q of 5
the phase shift tolerance becomes –180° ±1.7°. These
are important considerations when bandpass filters are
Constant Q Versus Constant BW
The bandpass outputs of the universal filters are “constant
Q.” For instance, a 2nd order bandpass filter operating
in mode 1 with a 100kHz clock (see LTC1060 data sheet)
ideally has a 1kHz or 2kHz center frequency, and a –3dB
bandwidth equal to (fo/Q). When the clock frequency
varies, the center frequency and bandwidth will vary
at the same rate. In a constant bandwidth filter, when
the center frequency varies, the Q varies accordingly to
maintain a constant (fo/Q) ratio. A constant bandwidth
BP filter could be implemented using 2nd order switched
capacitor filters but this is beyond the scope of this paper.
0
±10°
±20°
Q=1
±30°
±40°
φ
±50°
Q = 10
±60°
±70°
±80°
±90°
0
0.2
0.4
0.6
0.8
1.0
f/fo
1.2
1.4
1.6
1.8
2.0
AN27A F10
Figure 10. Phase Shift, φ, of a 2nd Order BP Filter Section (LTC1059, 1/2 LTC1060, 1/3 LTC1061)
an28f
AN27A-7
Application Note 27A
Tables 1 through 4 were derived from textbook filter theory.
They can be easily applied to the LTC filter family (LTC1059,
LTC1060, LTC1061 and LTC1064) if the Qs are kept relatively
low (<20) and the tuning resistors are at least 1% tolerance. These lower Q designs provide almost textbook BP
filter performance using LTC’s switched capacitor filters.
For higher Q implementations, tuning should be avoided
and the “A” versions of the LTC1059, LTC1060, LTC1061
or LTC1064 should be specified. Also, resistor tolerances
of better than 1% are a necessity.
This is true for any bandwidth, BW, and any set of frequencies. The tables can now be arithmetically scaled as
illustrated.
A2
2BW
A3
3BW
A4
4BW
A5
5BW
Table 1 may be used to find pole positions and Qs for
Butterworth bandpass filters. It should be noted that
the bandpass filters in these tables are geometrically
symmetrical about their center frequencies, foBP. Any
frequency,f3, as shown in Figure 11 has its geometrical
counterpart f4 such that:
f9 f 7
( f1,f2 ) =
Under this condition, for either Butterworth or Chebyshev
bandpass filters:
f –f
foBP ≅ 3 4 + f3
2
foPB ≅
f5 – f6
+ f5
2
•
•
•
AN27A-8
±BW +
f1f2 = foBP
f1 foBP f2
f4
f6
f8 f10
AN27A F11
(BW )2 + 4( foBP )2
2
MORE GENERALLY ( fx ,fx+1) =
±nBW +
(nBW )2 + 4( foBP )2
( VALID FOR ANY fx ,fx+1PAIR,ANYBW )
Additionally, Table 1 illustrates the attenuation at the
frequencies f3, f5, f7 and f9, which correspond to bandwidths 2, 3, 4 and 5 times the passband (see Figure 11).
These values allow the user to get a good estimate of
filter selectivity,
foPB
1
>> , BW = f2 – f1
BW
2
f5 f3
( f2 – f1) = BW
FREQUENCY (LOG SCALE)
f 2
f4 = oBP
f3
2
Figure 11. Generalized Bandpass Butterworth Response
(See Table 1)
BW
0
–2
GAIN (dB)
An important approximation can be made for not only the
Butterworth filters in Table 1, but also for the Chebyshev
filter Tables 2, 3 and 4. Treating Figure 11 (or Figure 12) as
a generalized bandpass filter, the two corner frequencies f2
and f1 can be seen to be nearly arithmetically symmetrical
with respect to foBP provided that:
BW
0
–3
GAIN (dB)
Using The Tables
A2
2BW
A3
3BW
A4
4BW
A5
5BW
f9 f 7
f5 f3
f1 foBP f2
f4
f6
f8 f10
AN27A F12
FREQUENCY (LOG SCALE)
f4 f3 = foPB
( f4,f3 ) =
±2BW +
(2BW )2 + 4( foBP )2
2
FOR ANY ( fx ,fx–1) PAIR AND
ANY CORRESPONDING BANDWIDTH
(2BW, 3BW, ETC.)
FOR EXAMPLE:
( f6,f5 ) =
±3BW +
(3BW )2 + 4( foBP )2
2
Figure 12. Generalized 4th, 6th, and 8th Order Chebyshev
Bandpass Filter with 2dB Passband Ripple (AMAX)
an28f
fo1 (Hz)
fo2 (Hz) fo3 (Hz) fo4 (Hz)
f–3dB (Hz)
f–3dB (Hz)
Q1 = Q2
20
1
0.982
0.965
0.932
0.885
0.836
0.693
1.018
1.036
1.073
1.125
1.195
1.442
0.975
0.951
0.905
0.847
0.781
0.500
1.025
1.051
1.105
1.180
1.281
2.000
28.3
14.2
7.1
4.3
2.9
1.5
10
20
1
1
0.650
0.979
0.958
0.917
0.866
0.805
1.539
1.022
1.044
1.091
1.155
1.242
1.000
1.000
1.000
1.000
1.000
1.000
0.500
0.975
0.951
0.905
0.847
0.781
2.000
1.025
1.051
1.105
1.180
1.281
2.2
40.0
20.0
10.0
6.1
4.1
1.0
20.0
10.0
5.0
3.0
2.0
5
10
20
1
1
3
1
1
1
2
1
1
0.809
0.990
0.981
0.962
0.938
0.907
1.237
1.010
1.019
1.039
1.066
1.103
0.636
0.977
0.955
0.912
0.858
0.795
1.574
1.023
1.047
1.097
1.166
1.259
0.500
0.975
0.951
0.905
0.847
0.781
2.000
1.025
1.051
1.105
1.180
1.281
1.1
21.6
10.8
5.4
3.3
2.2
52.3
26.2
13.1
7.9
5.4
2.9
Q3 = Q4
8th Order Butterworth Bandpass Filter Normalized to its Center Frequency, foBP = 1, and –3dB Bandwidth (BW)
3
5
1
1
1
2
1
1
Q3
6th Order Butterworth Bandpass Filter Normalized to its Center Frequency, foBP = 1, and –3dB Bandwidth (BW)
5
10
1
1
2
3
1
1
1
1
4th Order Butterworth Bandpass Filter Normalized to its Center Frequency, foBP = 1, and –3dB Bandwidth (BW)
foBP (Hz) foBP/BW (Hz)
Table 1. Butterworth Bandpass Filters Normalized to foBP = 1
8.00
8.00
8.05
8.15
8.48
10.14
4.00
4.01
4.03
4.07
4.18
4.79
2.03
2.03
2.04
2.07
2.07
2.28
K
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
f1 (Hz) f3 (Hz)
–24.0
–24.0
–24.0
–24.0
–24.0
–24.0
–18.2
–18.2
–18.2
–18.2
–18.2
–18.2
–12.3
–12.3
–12.3
–12.3
–12.3
–12.3
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
–38.0
–38.0
–38.0
–38.0
–38.0
–38.0
–28.6
–28.6
–28.6
–28.6
–28.6
–28.6
–19.1
–19.1
–19.1
–19.1
–19.1
–19.1
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
–48.1
–48.1
–48.1
–48.1
–48.1
–48.1
–36.1
–36.1
–36.1
–36.1
–36.1
–36.1
–24.0
–24.0
–24.0
–24.0
–24.0
–24.0
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
–55.8
–55.8
–55.8
–55.8
–55.8
–55.8
–41.9
–41.9
–41.9
–41.9
–41.9
–41.9
–28.0
–28.0
–28.0
–28.0
–28.0
–28.0
GAIN AT f3
GAIN AT f5
GAIN AT f7
GAIN AT f9
(dB)-A2 f5 (Hz) (dB)-A3 f7 (dB) (dB)-A4 f9 (Hz) (dB)-A5
Application Note 27A
an28f
AN27A-9
AN27A-10
2
3
5
10
20
1
1
1
1
1
0.966
0.933
0.871
0.793
0.703
0.488
20
1
0.975
0.951
0.904
0.845
0.777
0.602
2
3
5
10
20
1
1
1
1
1
0.978
0.956
0.914
0.861
0.799
0.639
20
1
0.980
0.960
0.922
0.873
0.816
0.668
1.021
1.041
1.085
1.145
1.225
1.496
1.022
1.046
1.094
1.161
1.251
1.564
1.025
1.051
1.106
1.182
1.287
1.660
1.035
1.071
1.148
1.261
1.422
2.050
fo2 (Hz)
18.87
9.35
4.65
2.79
1.86
0.93
16.39
8.20
4.12
2.47
1.64
0.82
14.49
7.19
3.60
2.16
1.44
0.72
10.31
5.15
2.58
1.54
1.03
0.52
0.974
0.948
0.898
0.837
0.767
0.598
0.970
0.941
0.886
0.818
0.741
0.562
0.966
0.933
0.871
0.795
0.711
0.523
0.953
0.908
0.825
0.727
0.626
0.423
1.027
1.055
1.113
1.195
1.304
1.672
1.031
1.063
1.129
1.223
1.349
1.779
1.035
1.072
1.149
1.258
1.406
1.912
1.050
1.102
1.213
1.375
1.597
2.364
49.8
24.9
12.5
7.5
5.1
2.7
36.5
18.2
9.2
5.5
3.7
2.0
28.1
14.1
7.1
4.3
2.9
1.6
16.9
8.5
4.3
2.6
1.8
1.1
foBP/BW2** (Hz) f–3dB (Hz) f–3dB (Hz) Q1 = Q2
*foBP/BW1 – This is the ratio of the bandpass filter center frequency to the ripple bandwidth of the filter.
**foBP/BW2 – This is the ratio of the bandpass filter center frequency to the –3dB filter bandwidth.
5
10
3
1
1
2
1
1
1
1
Passband Ripple AMAX = 2.0dB
1
1
Passband Ripple AMAX = 1.0dB
5
10
3
1
1
2
1
1
1
1
Passband Ripple AMAX = 0.5dB
1
1
Passband Ripple, AMAX = 0.1dB
foBP (Hz) foBP/BW1* (Hz) fo1 (Hz)
5.07
5.13
5.13
5.22
5.30
6.00
3.63
3.70
3.71
3.76
3.85
4.42
2.97
2.98
3.03
3.07
3.17
3.80
2.37
2.38
2.38
2.48
2.66
3.81
K
Table 2. 4th Order Chebyshev Bandpass Filter Normalized to its Center Frequency foBP = 1
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
f1 (Hz)
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
f3 (Hz)
–12.7
–12.7
–12.7
–12.7
–12.7
–12.7
–10.3
–10.3
–10.3
–10.3
–10.3
–10.3
–7.9
–7.9
–7.9
–7.9
–7.9
–7.9
–3.2
–3.2
–3.2
–3.2
–3.2
–3.2
GAIN AT
f3 (dB)-A2
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
f5 (Hz)
–20.3
–20.3
–20.3
–20.3
–20.3
–20.3
–17.7
–17.7
–17.7
–17.7
–17.7
–17.7
–15.0
–15.0
–15.0
–15.0
–15.0
–15.0
–08.7
–08.7
–08.7
–08.7
–08.7
–08.7
GAIN AT
f5 (dB)-A3
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
f7 (Hz)
–25.5
–25.5
–25.5
–25.5
–25.5
–25.5
–23.0
–23.0
–23.0
–23.0
–23.0
–23.0
–20.2
–20.2
–20.2
–20.2
–20.2
–20.2
–13.6
–13.6
–13.6
–13.6
–13.6
–13.6
GAIN AT
f7 (dB)-A4
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
–29.5
–29.5
–29.5
–29.5
–29.5
–29.5
–27.0
–27.0
–27.0
–27.0
–27.0
–27.0
–24.1
–24.1
–24.1
–24.1
–24.1
–24.1
–17.4
–17.4
–17.4
–17.4
–17.4
–17.4
GAIN AT
f9 (Hz) f9 (dB)-A5
Application Note 27A
an28f
20
1
0.970
0.941
0.886
0.818
0.741
0.558
10
20
1
1
0.609
0.975
0.950
0.903
0.844
0.776
20
1
0.976
0.953
0.908
0.852
0.787
0.626
10
20
1
1
0.639
0.977
0.955
0.912
0.858
0.795
1.023
1.047
1.096
1.165
1.257
1.565
1.024
1.050
1.101
1.174
1.271
1.598
1.026
1.052
1.107
1.185
1.288
1.641
1.030
1.062
1.128
1.222
1.349
1.791
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
1.000
19.61
9.71
4.83
2.91
1.94
0.97
18.18
9.17
4.59
2.74
1.83
0.91
16.95
8.55
4.29
2.57
1.72
0.86
14.49
7.19
3.60
2.16
1.44
0.72
0.975
0.950
0.902
0.843
0.775
0.609
0.973
0.947
0.897
0.834
0.763
0.593
0.971
0.943
0.890
0.824
0.750
0.574
0.966
0.933
0.871
0.795
0.711
0.523
1.026
1.053
1.109
1.187
1.291
1.642
1.028
1.056
1.115
1.199
1.310
1.687
1.030
1.060
1.123
1.213
1.333
1.741
1.035
1.072
1.149
1.258
1.406
1.912
108.5
54.3
27.2
16.5
11.1
6.0
81.0
40.5
20.3
12.3
8.3
4.5
63.8
32.0
16.1
9.7
6.6
3.6
41.3
20.6
10.4
6.3
4.3
2.4
*foBP/BW1 – This is the ratio of the bandpass filter center frequency to the ripple bandwidth of the filter.
**foBP/BW2 – This is the ratio of the bandpass filter center frequency to the –3dB filter bandwidth.
3
5
1
1
1
2
1
1
Passband Ripple, AMAX = 2.0dB
5
10
1
1
2
3
1
1
1
1
Passband Ripple, AMAX = 1.0dB
3
5
1
1
1
2
1
1
Passband Ripple, AMAX = 0.5dB
5
10
1
1
2
3
1
1
1
1
Passband Ripple, AMAX = 0.1dB
54.2
27.1
13.6
8.1
5.4
2.7
40.5
20.2
10.1
6.1
4.1
2.0
32.0
16.0
8.0
4.8
3.2
1.6
20.6
10.3
5.2
3.1
2.1
1.0
foBP (Hz) foBP/BW1* (Hz) fo1 (Hz) fo2 (Hz) fo3 (Hz) foBP/BW2** (Hz) f–3dB (Hz) f–3dB (Hz) Q1 = Q2 Q = 3
Table 3. 6th Order Chebychev Bandpass Filter Normalized to its Center Frequency foBP = 1
26.0
26.0
26.2
26.7
27.4
31.7
16.4
16.4
16.4
16.7
17.1
20.1
11.4
11.8
11.8
12.0
12.5
14.8
7.3
7.3
7.4
7.5
7.9
9.9
K
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.975
0.951
0.905
0.847
0.781
0.500
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
0.951
0.905
0.820
0.721
0.618
0.414
–26.0
–26.0
–26.0
–26.0
–26.0
–26.0
–22.5
–22.5
–22.5
–22.5
–22.5
–22.5
–19.2
–19.2
–19.2
–19.2
–19.2
–19.2
–12.2
–12.2
–12.2
–12.2
–12.2
–12.2
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
–37.5
–37.5
–37.5
–37.5
–37.5
–37.5
–34.0
–34.0
–34.0
–34.0
–34.0
–34.0
–30.8
–30.8
–30.8
–30.8
–30.8
–30.8
–23.6
–23.6
–23.6
–23.6
–23.6
–23.6
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
–45.4
–45.4
–45.4
–45.4
–45.4
–45.4
–41.9
–41.9
–41.9
–41.9
–41.9
–41.9
–38.6
–38.6
–38.6
–38.6
–38.6
–38.6
–31.4
–31.4
–31.4
–31.4
–31.4
–31.4
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
–51.3
–51.3
–51.3
–51.3
–51.3
–51.3
–47.8
–47.8
–47.8
–47.8
–47.8
–47.8
–44.5
–44.5
–44.5
–44.5
–44.5
–44.5
–37.3
–37.3
–37.3
–37.3
–37.3
–37.3
GAIN AT
GAIN AT
GAIN AT
GAIN AT
f1 (Hz) f3 (Hz) f3 (dB)-A2 f5 (Hz) f5 (dB)-A3 f7 (Hz) f7 (dB)-A4 f9 (Hz) f9 (dB)-A5
Application Note 27A
an28f
AN27A-11
AN27A-12
2
3
5
10
20
1
1
1
1
1
0.988
0.977
0.954
0.925
0.889
0.785
20
1
0.989
0.979
0.959
0.932
0.900
0.808
2
3
5
10
20
1
1
1
1
1
0.990
0.980
0.960
0.934
0.903
0.814
20
1
0.990
0.980
0.961
0.936
0.905
0.820
1.010
1.020
1.040
1.068
1.104
1.220
1.010
1.020
1.041
1.070
1.107
1.228
1.010
1.021
1.043
1.073
1.111
1.238
1.012
1.023
1.048
1.081
1.125
1.274
0.976
0.953
0.909
0.853
0.789
0.629
0.976
0.952
0.906
0.850
0.784
0.622
0.975
0.950
0.903
0.845
0.777
0.613
0.972
0.945
0.894
0.830
0.757
0.584
1.024
1.049
1.100
1.172
1.268
1.589
1.025
1.050
1.103
1.177
1.275
1.607
1.026
1.052
1.107
1.183
1.286
1.632
1.028
1.058
1.118
1.204
1.320
1.713
19.61
9.80
4.90
2.95
1.96
0.98
18.87
9.52
4.74
2.85
1.90
0.95
18.18
9.17
4.59
2.74
1.83
0.91
16.39
8.20
4.12
2.48
1.65
0.82
0.975
0.950
0.903
0.845
0.777
0.613
0.974
0.949
0.900
0.840
0.771
0.604
0.973
0.947
0.897
0.834
0.763
0.593
0.970
0.941
0.886
0.818
0.742
0.563
1.026
1.052
1.107
1.184
1.287
1.631
1.027
1.054
1.111
1.191
1.297
1.656
1.028
1.056
1.115
1.199
1.310
1.686
1.031
1.063
1.129
1.222
1.348
1.776
*foBP/BW1 – This is the ratio of the bandpass filter center frequency to the ripple bandwidth of the filter.
**foBP/BW2 – This is the ratio of the bandpass filter center frequency to the –3dB filter bandwidth.
5
10
3
1
1
2
1
1
1
1
Passband Ripple, AMAX = 2.0dB
1
1
Passband Ripple, AMAX = 1.0dB
5
10
3
1
1
2
1
1
1
1
Passband Ripple, AMAX = 0.5dB
1
1
Passband Ripple, AMAX = 0.1dB
124.0 0.951 0.905
127.7 0.905 0.820
128.1 0.847 0.721
133.2 0.781 0.618
162.8 0.500 0.414
70.0 0.975 0.951
70.0 0.951 0.905
70.0 0.905 0.820
71.5 0.847 0.721
74.3 0.781 0.618
90.1 0.500 0.414
29.8 0.975 0.951
29.8 0.951 0.905
29.9 0.905 0.820
30.5 0.847 0.721
32.1 0.781 0.618
40.6 0.500 0.414
190.0 302.0 0.975 0.951
79.0
302.0 0.951 0.905
302.0 0.905 0.820
302.0 0.847 0.721
312.6 0.781 0.618
374.8 0.500 0.414
95.4
47.9
29.0
19.6
10.6
-35.4
-35.4
-35.4
-35.4
-35.4
-35.4
-32.9
-32.9
-32.9
-32.9
-32.9
-32.9
-30.2
-30.2
-30.2
-30.2
-30.2
-30.2
-23.4
-23.4
-23.4
-23.4
-23.4
-23.4
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
0.928
0.861
0.744
0.618
0.500
0.303
-50.8
-50.8
-50.8
-50.8
-50.8
-50.8
-48.3
-48.3
-48.3
-48.3
-48.3
-48.3
-45.5
-45.5
-45.5
-45.5
-45.5
-45.5
-38.8
-38.8
-38.8
-38.8
-38.8
-38.8
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
0.905
0.820
0.677
0.535
0.414
0.236
-61.3
-61.3
-61.3
-61.3
-61.3
-61.3
-58.8
-58.8
-58.8
-58.8
-58.8
-58.8
-56.0
-56.0
-56.0
-56.0
-56.0
-56.0
-49.3
-49.3
-49.3
-49.3
-49.3
-49.3
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
0.883
0.781
0.618
0.469
0.351
0.193
-69.2
-69.2
-69.2
-69.2
-69.2
-69.2
-66.6
-66.6
-66.6
-66.6
-66.6
-66.6
-63.9
-63.9
-63.9
-63.9
-63.9
-63.9
-57.1
-57.1
-57.1
-57.1
-57.1
-57.1
GAIN AT
GAIN AT
GAIN AT
GAIN AT
f1 (Hz) f3 (Hz) f3 (dB)-A2 f5 (Hz) f5 (dB)-A3 f7 (Hz) f7 (dB)-A4 f9 (Hz) f9 (dB)-A5
143.0 120.0 0.975 0.951
71.7
36.0
21.8
14.8
8.0
114.0
57.1
28.7
17.4
11.8
6.4
75.7
37.9
19.1
11.6
7.9
4.4
K
39.5
19.7
11.9
7.9
4.0
59.4
29.7
14.9
8.9
6.0
3.0
47.2
23.6
11.8
7.1
4.8
2.4
31.4
15.7
7.9
4.7
3.2
1.6
foBP (Hz) foBP/BW1* (Hz) fo1 (Hz) fo2 (Hz) fo3 (Hz) fo4 (Hz) foBP/BW2** (Hz) f–3dB (Hz) f–3dB (Hz) Q1=Q2 Q3=Q4
Table 4. 8th Order Chebychev Bandpass Filter Normalized to its Center Frequency foBP = 1
Application Note 27A
an28f
Application Note 27A
Chebyshev or Butterworth—A System Designers
Confusion
RdB
The filter designer/mathematician is familiar with terms
such as:
GAIN (dB)
0
KC = tanh A
1
1
A = cosh –1
∈
n
Ripple bandwidth = 1/cosh A
and AdB = 10 log [1 + ∈2(Cn2(Ω)].
–3
f1´–3dB f1ripple
This is all gobbledygook (not to be confused with floobydust) to the system designer. The system designer is
accustomed to –3dB bandwidths and may be tempted
to use only Butterworth filters because they have the
cherished –3dB bandwidths. But specs are specs and
Butterworth bandpass filters are only so good. Chebyshev bandpass filters trade off ripple in the passband for
somewhat steeper rolloff to the stopband. More ripple
translates to a higher “Q” filter. The pain of the filter
designer is sometimes tolerable to the system designer.
Tables 1 through 4 are unique (we think) in that they
present -3dB bandwidths for Chebyshev filters for use
by system designers. Nevertheless we would be amiss
to Mr. Chebyshev if we did not, at least, explain ripple
bandwidth.
Figure 13 shows the Chebyshev bandpass filter at frequencies near the passband.
foBP
f2ripple f2´–3dB
AN27A F13
FREQUENCY
Figure 13. Typical Chebyshev BP Filter—Close-Up of Passband
It can be clearly seen that the ripple bandwidth
(f1ripple – f2ripple) is the band of passband frequencies
where the ripple is less than or equal to a specific value
(RdB). The –3dB bandwidth is seen to be greater than
the ripple bandwidth and that is the subject of much
confusion on the part of the system designer.
Tables 1 through 4 allow the system designer to use
–3dB bandwidths to specify Chebyshev BP filters. The
Chebyshev approximation to the ideal BP filter has
many benefits over the Butterworth filter near the cutoff
frequency.
YOU CAN DESIGN WITH CHEBYSHEV FILTERS!!!
We choose AMAX = 0.1dB. Now we calculate:
Example 3—Design
Use Table 4 to design an 8th order all pole Chebyshev
bandpass filter centered at foBP = 10.2kHz with a
–3dB bandwidth equal to 800Hz as shown in Figure 14.
foBP
fBW(–3dB)
=
10.2kHz
= 12.75
800Hz
We can now extract from Table 4 the following line:
10
0
–3
foBP foBP/BW1 fo1(Hz) fo2(Hz) fo3(Hz) fo4(Hz) foBP/BW2 Q1=Q2 Q3=Q4
800Hz
GAIN (dB)
1
–50
9.000k
12.000k
foBF = 10.2kHz
FREQUENCY (Hz)
10
0.977
1.023
0.945
1.058
8.20
15.7
K
37.9 29.8
Since our bandwidth ratio foBP/BW2 is not exactly on a
chart line, but between two lines, we must arithmetically
scale to obtain our design parameters. Our foBP/BW2 ratio
lies between 8.2 and 16.39. (Remember, this is –3dB BW!)
AN27A F14
Figure 14. Example 3—8th Order Chebyshev BP Filter
foBP = 10.2kHz, BW = 800Hz
an28f
AN27A-13
Application Note 27A
For a symmetrical bandpass filter the poles are symmetrical
8.2 
( fo2 – fo1) = (1.023 – 0.977) ×10.2kHz ×  12.75
 = 302Hz
 8.2  foBP
Scaling Factor
=
Note: 
 12.75  BW
So our first two poles lie symmetrically about fo(10.2kHz)
and are 302Hz apart:
Recalling that:
foBP
= 12.75 and that foBP = 1,
BW2(–3dB)
(Because all the tables are normalized), we calculate
BW2(–3dB) = .0784
Comparing the Table 4 values for AMAX = 0.1dB we note that:
foBP
foBP
≅
× ( Scaling Factor )
BW1(ripple) BW2(–3dB)
fo2 = 10200Hz + 302Hz/2 = 10351Hz
fo1 = 10200Hz – 302Hz/2 = 10049Hz
For AMAX = 0.1dB, 8th order Chebyshev, this factor is approximately 0.82. For other order filters and/or different
values of AMAX we can examine the corresponding chart
values to find our scaling factor.
The Q of these two poles is equal and is also scaled:
Q1= Q2 = 15.7 ×
12.75
= 24.4
8.2
So our ripple BW is:
We calculate the two additional poles:
BW2(–3dB) × (Scaling Factor) = BW1(ripple)
8.2
= 741Hz
( fo4 – fo3 ) = (1.058 – 0.945) ×10.2kHz × 12.75
.0784 × 0.82 = .0643
fo3 = 10200Hz – 741Hz/2 = 9830Hz
fo4 = 10200Hz + 741Hz/2 = 10571Hz
The Qs are:
Q3 = Q4 = 37.9 ×
12.75
= 58.9
8.2
Qs of this magnitude are difficult to realize no matter how
the filter is realized. The filter designer should strive for
Qs no greater than 20 and perhaps no greater than 10 at
frequencies above 20kHz. K, for this example, is not scaled
and will be equal to 29.8 from Table 4.
Example 3—Frequency Response Estimation
Table 4 (and also Tables 1, 2 and 3) may be used by the
filter designer to obtain a good approximation to the overall
shape of the bandpass filter. Referring to Figure 12 for
Chebyshev filters, we may use the charts to find f3, f5,
f7,…. These frequencies define the band edges at 2, 3,
4,…..times the ripple bandwidth of the Chebyshev filter.
Now we can calculate f3, f5, f7,….Notice that once we find
f3, f5, f7,….it does not matter where on the table our filter
falls. The filter bandwidth determines f3, f5, f7,….and once
we know these frequencies we can directly get our gains
at these frequencies.
By formula:
( fx ,fx+1) =
±nBW +
(nBW )2 + 4( foBP )2
2
for our case foBP = 1
Calculating:
2BW = .1286
3BW = .1929
±2BW +
(.1286)2 + 4
2
±3BW +
(.1929)2 + 4
2
= 1.0664, 0.9378
= 1.1011, 0.9082
Example 3 specified a 10.2kHz bandpass filter with an
800Hz –3dB bandwidth. Our task, if we choose to accept
it, is to convert our -3dB bandwidth to the ripple bandwidth
of the filter so that we may use the tables.
an28f
AN27A-14
Application Note 27A
Then we can denormalize to find points for our Bode plot:
(f3, f4) = 0.9378 × foBP = 0.9378 × 10.2kHz = 9.566kHz
1.0664 × foBP = 1.0664 × 10.2kHz = 10.877kHz
Gain = –23.4dB both f3 and f4
(f5, f6) = 0.9082 × foBP = 0.9082 × 10.2kHz = 9.264kHz
1.1011 × foBP = 1.1011 × 10.2kHz = 11.231kHz
Example 3—Implementation
The 10.2kHz (foBP), 8th order bandpass filter can be
implemented with an LTC1064A using three sections in
mode 2 and one section in mode 3. The implementation
is shown briefly in Figures 15 and 16. The calculations are
not shown here, but are similar to the previous hardware
implementations of examples 1 and 2.
Gain = –38.8dB both f5 and f6
R12 = 137k
VIN
R11 = 232k
1
R21 = 10k
2
R31 = 232k
3
R41 = 140k
4
5
6
5V
7
8
FROM PIN 22
R13 = 255k
R43 = 85.6k
9
R33 = 549k
10
R23 = 10k
11
12
INVB
INVC
HPB/NB
HP/NC
BPB
BPC
LPB
LPC
SB
LTC1064
A.GND
+
V
SA
SC
V–
CLK
50/100
LPA
LPD
BPA
BPD
HPA
HPD
INVA
INVD
24
23
R22 = 10k
22
R32 = 243k
TO R13
21
20
19
18
R42 = 1.02M
–5V
1MHz
17
R44 = 10.5k
R34 = 604k
VOUT
R24 = 10.2k
R14 = 78.7k
AN27A F15
Figure 15. LTC1064 Implementation Pinout—10.2kHz 8th Order BPF
an28f
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.
However, no responsibility is assumed for its use. Linear Technology Corporation makes no representation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
AN27A-15
Application Note 27A
R41 = 140k
R31 = 232k
SECTION 1
MODE 2
fo1 = 10.351kHz
Q1 = 24.4
R21 = 10k
VIN
–
R11 = 232k
INVB(1)
HPB/NB(2)
+
+
–
AGND(6)
BPB(3)
∫
LPB(4)
∫
SB(5)
R12 = 137k
R42 = 1.02M
R32 = 243k
R22 = 10k
–
INVC(24)
SECTION 2
MODE 2
fo2 = 10.049kHz
Q2 = 24.4
LPC(21)
HPC/NC(23)
+
+
–
AGND(6)
BPC(22)
∫
∫
SC(20)
R13 = 255k
R43 = 85.6k
5V
V+(7)
R33 = 549k
R23 = 10k
–
INVA(12)
50/100(17)
HPA/NA(11)
+
+
–
BPA(10)
∫
LPA(9)
1MHz
CLK(18)
∫
V–(19)
AGND(6)
SECTION 3
MODE 2
fo = 10.571kHz
Q3 = 58.9
–5V
SA(8)
R14 = 78.7k
R44 = 10.5k
R34 = 604k
R24 = 10.2k
–
INVD(13)
HPD(14)
BPD(15)
∫
+
∫
LPD(16)
SECTION 4
MODE 3
fo = 9.830kHz
Q = 58.9
AN27A F16
VOUT
AGND(6)
NUMBERS IN PARENTHESIS ARE PIN NUMBERS OF LTC1064
ALL RESISTORS 1%
Figure 16. Implementation of 10.2kHz 8th Order BPF—Section by Section for LTC1064
an28f
Linear Technology Corporation
McCarthy Blvd., Milpitas, CA 95035-7417
AN27A-16 1630
(408) 432-1900 FAX: (408) 434-0507 www.linear.com
●
●
IM/GP 988 20K • PRINTED IN USA
 LINEAR TECHNOLOGY CORPORATION 1988
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