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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

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