ACTIVE FILTERS - THE ACTIVE FILTER HANDBOOK BY F. TEDESCHI
USE VCVS TOPOLOGY - VOLTAGE CONTROLLED VOLTAGE SOURCE
CHOOSE A = 1 ... GOOD FOR OP-AMPS AND EMITTER FOLLOWERS
IN A HIGH PASS FILTER:
-----------R1-----
I I
I I
I I
V(IN)----C1--------C2------ A=1 ---- V(OUT)
I
I
R2
I
I
---
BIAS CAN BE SUPPLIED THROUGH R2 ...
IN A LOW PASS FILTER:
-----------C2-----
I I
I I
I I
V(IN)----R1--------R2------ A=1 ---- V(OUT)
I
I
C1
I
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---
BIAS MUST BE SUPPLIED THROUGH SOURCE ...
IN BOTH CASES, THERE IS NO INPUT BUFFER AMP, SO THE SOURCE
IMPEDANCE MUST BE RELATIVELY LOW AND/OR CONSTANT.
THERE IS ALSO NO INVERSION OF THE INPUT SIGNAL.
FOR THE LPF, THE EQUATIONS REDUCE TO
B0 = 1 / (R1*R2*C1*C2) AND B1 = (1/C2)*(1/R1 + 1/R2)
OR
B0 = G1*G2 / (C1*C2) AND B1 = (G1 + G2) / C2
WHERE H(S) = B0 / (S^2 + B1*S + B0)
IS THE SECOND-ORDER LP FILTER RESPONSE TRANSFER FUNCTION.
NOTE: HIGHER ORDER FILTERS CAN BE MADE FROM A CASCADE OF FIRST
AND SECOND ORDER SECTIONS.
IF WE CHOOSE R1 = R2 = R = 1, THEN WE ONLY HAVE TO FIND THE
CAPACITOR VALUES TO GET A FILTER AND RE-NORMALIZE FOR THE RŐS WE
REALLY WANT AND THE FREQUENCIES WE REALLY WANT.
THEN C2 = 2 / B1 AND C1 = B1 / (2*B0)
EXAMPLE 1: 2-POLE BUTTERWORTH LP FILTER (RIPPLE = 0) (W3 = 1)
B1 = 1.414 B0 = 1
SO C2 = 2 / 1.414 = 1.414 AND C1 = 1.414 / 2*1) = 0.707
EXAMPLE 2: 2-POLE CHEBYCHEV LP FILTER (RIPPLE = 0.5 DB) (WR = 1)
B1 = 1.425 B0 = 1.516
SO C2 = 2 / 1.425 = 1.4 AND C1 = 1.425 / (2*1.516) = 0.47
IF R = 10K, THEN C2 = 1.4 E -4 AND C1 = 0.47 E -4
IF F(RIPPLE) = 2.23 KHZ, WR = 14.0 E3, AND C1 = 10 E-9 AND C2 = 3.36 E-9
WE CANNOT JUST CHOOSE THE CAPACITORS, LIKE C1 = C2 = 1 .
A SOLUTION FOR G1:
G1 = B1 / 2 ± (B1^2 - 4*B0)^0.5 / 2.
G1 IS ONLY REAL IF B0 R1 = 20K, R2 = 5K
J. E. MATZ - 28 FEB 97