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"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10

"Chapter 1 - The Op Amp's Place in the World" - HTL Wien 10

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Band-Rejection Filter Design<br />

16-38<br />

V IN<br />

Figure 16–38. Active Tw<strong>in</strong>-T Filter<br />

C<br />

R<br />

R/2<br />

<strong>The</strong> transfer function of <strong>the</strong> active tw<strong>in</strong>-T filter is:<br />

2C<br />

k1 s<br />

A(s) <br />

2<br />

1 2(2 k)·s s2 C<br />

R<br />

R 1<br />

R 2<br />

V OUT<br />

(16–21)<br />

Compar<strong>in</strong>g <strong>the</strong> variables of Equation 16–21 with Equation 16–20 provides <strong>the</strong> equations<br />

that determ<strong>in</strong>e <strong>the</strong> filter parameters:<br />

mid-frequency:<br />

<strong>in</strong>ner ga<strong>in</strong>:<br />

passband ga<strong>in</strong>:<br />

fm 1<br />

2RC<br />

G 1 R 2<br />

R 1<br />

A 0 G<br />

Q <br />

1<br />

rejection quality:<br />

2(2 G)<br />

<strong>The</strong> tw<strong>in</strong>-T circuit has <strong>the</strong> advantage that <strong>the</strong> quality factor (Q) can be varied via <strong>the</strong> <strong>in</strong>ner<br />

ga<strong>in</strong> (G) without modify<strong>in</strong>g <strong>the</strong> mid frequency (f m). However, Q and A m cannot be adjusted<br />

<strong>in</strong>dependently.<br />

To set <strong>the</strong> mid frequency of <strong>the</strong> band-pass, specify fm and C, and <strong>the</strong>n solve for R:<br />

R 1<br />

2fmC<br />

Because of <strong>the</strong> dependency between Q and A m, <strong>the</strong>re are two options to solve for R 2: ei<strong>the</strong>r<br />

to set <strong>the</strong> ga<strong>in</strong> at mid frequency:<br />

R 2 A 0 1R 1

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