Implementing IIR/FIR Filters
Implementing IIR/FIR Filters
Implementing IIR/FIR Filters
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V<br />
0<br />
X<br />
L<br />
||R<br />
----- = ------------------------<br />
V<br />
i X<br />
C + X<br />
L<br />
||R<br />
j ΩLR/ ( jΩL + R)<br />
= -------------------------------------------------------<br />
1/jΩC + jΩLR/jΩL<br />
+ R<br />
Ω<br />
=<br />
2<br />
–<br />
Ω 2<br />
------------------------------------------------<br />
– + j Ω /RC + 1/LC<br />
Ω<br />
=<br />
2<br />
–<br />
Ω 2<br />
------------------------------------------<br />
– + jdΩ<br />
c<br />
Ω+ Ω2 c<br />
Let s = jΩ and define H(s) = V o /V i ; then,<br />
V i<br />
MOTOROLA 1-11<br />
C<br />
L R<br />
V 0<br />
X c = 1/jΩC<br />
X L = jΩL<br />
1<br />
Ωc = -----------<br />
LC<br />
L<br />
d =<br />
R 2 -----------<br />
C<br />
( s/Ω<br />
c)<br />
H( s)<br />
2<br />
( s/Ω ) c<br />
2<br />
= ---------------------------------------------------<br />
+ d( s/Ω) + 1<br />
c<br />
which is the s-domain transfer function. The gain, G(Ω), of the filter is:<br />
G( Ω)<br />
≡ H( s)H∗(<br />
s)<br />
s = jω<br />
( Ω/Ω<br />
c)<br />
2<br />
1 Ω 2 2<br />
( – /Ω ) c<br />
2<br />
( dΩ/Ω<br />
c)<br />
2<br />
= ---------------------------------------------------------------<br />
+<br />
where ∗ denotes complex conjugate.<br />
The phase angle, φΩ, is the angle between the imaginary and<br />
φ( Ω)<br />
tan 1 –<br />
≡ [ l{ H( s)<br />
}/R{ H( s)<br />
} ]<br />
– 1 d( Ω/Ωc )<br />
= π– tan<br />
1 ( Ω/Ωc) 2<br />
real components of H(s).<br />
----------------------------for<br />
Ω ≤ Ωc –<br />
– 1 d( Ω/Ωc )<br />
= – tan<br />
1 ( Ω/Ωc) 2<br />
------------------------------<br />
–<br />
Figure 1-3 s-Domain Analysis of Second-Order Highpass Analog Filter<br />
for Ω > Ω c