EDITOR: B. SOMANATHAN NAIR
1. BUTTERWORTH
FILTER STRUCTURES
Figures
1 and 2 show the first- and second-order filter structures called Sallen and Key structures, named after
the originators. These structures are also known as voltage-controlled voltage-source (VCVS) and KRC (constant-gain RC) filter circuits. By cascading these basic
structures, filters of any order can be obtained. We now numerically design a
Butterworth active LPF of the KRC type.
Example 1: Design a Butterworth
first-order LPF of the KRC type, shown in Fig. 1, for cut-off
frequency of 1000 Hz.
Step 1: Determination of C and R
We have the cut-off frequency of an LPF given by
fc
= 1/2πRC (1)
Substituting for fc
= 1000 Hz and C = 0.1 mF (a standard value of
capacitors widely available in the open market) in (1), we find
R
= 1/2πx1000x0.1x10‒6 = 1.59
kW
R can be realized by using a
standard resistor of 1 kW in series with a
potentiometer of 1 kW for precise adjustment of
resistor values.
Step 2: Determination
of amplifier components R1 and R2
For the non-inverting amplifier used, the gain is
given by
A = 1 + (R2/R1)
(2)
Assuming a typical gain of 100, we find
R2/R1 = 99
Choosing arbitrarily
R1 = 1 kW
we obtain
R2 = 99 kW
Use a standard resistor of 82 kW in series with a potentiometer of 22
kW. The designed circuit is
shown in Fig. 2.
Example 2: Design a Butterworth
second-order LPF shown in Fig. 3 for a cut-off frequency fc of 1000 Hz.
Step 1: Determination of C and R
From Example 1, we obtain the values of R and C as 1.59 kΩ and 0.1 mF, respectively, where R is realized by using a standard
resistor of 1 kW in series with a
potentiometer of 1 kW.
Step 2: Determination
of Amplifier components R1 and R2
As in Example 1, for the non-inverting amplifier
used, the gain A is given by
A
= 1 + (R2/R1) (1)
Using the coefficient of s of a second-order filter (see Table 1 in the previous blog), we
have
3
‒ A = 1.414 (2)
From (1) and (2), we get
R2/R1 = 0.586
Choosing
R1 = 1 kW (arbitrarily)
we obtain
R2 = 0.586 kW
In practical cases, we choose a 560 W in series with a pot of 100 W
as R2.
The fully designed second-order low-pass filter is shown in Fig. 4.
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