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

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Band-Pass Filter Design<br />

16-30<br />

<strong>The</strong> graph shows that <strong>the</strong> frequency response of second-order band-pass filters gets<br />

steeper with ris<strong>in</strong>g Q, thus mak<strong>in</strong>g <strong>the</strong> filter more selective.<br />

16.5.1.1 Sallen-Key Topology<br />

V IN<br />

Figure 16–33. Sallen-Key Band-Pass<br />

R<br />

C<br />

C<br />

2R<br />

R<br />

<strong>The</strong> Sallen-Key band-pass circuit <strong>in</strong> Figure 16–33 has <strong>the</strong> follow<strong>in</strong>g transfer function:<br />

A(s) <br />

R 1<br />

R 2<br />

V OUT<br />

G·RCm·s<br />

1 RCm(3 G)·s R 2 C 2 m 2 ·s 2<br />

Through coefficient comparison with Equation 16–<strong>10</strong>, obta<strong>in</strong> <strong>the</strong> follow<strong>in</strong>g equations:<br />

mid-frequency:<br />

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

ga<strong>in</strong> at f m:<br />

filter quality:<br />

fm 1<br />

2RC<br />

G 1 R 2<br />

R 1<br />

Am G<br />

3 G<br />

Q 1<br />

3 G<br />

<strong>The</strong> Sallen-Key circuit has <strong>the</strong> advantage that <strong>the</strong> quality factor (Q) can be varied via <strong>the</strong><br />

<strong>in</strong>ner ga<strong>in</strong> (G) without modify<strong>in</strong>g <strong>the</strong> mid frequency (fm). A drawback is, however, that Q<br />

and A m cannot be adjusted <strong>in</strong>dependently.<br />

Care must be taken when G approaches <strong>the</strong> value of 3, because <strong>the</strong>n A m becomes <strong>in</strong>f<strong>in</strong>ite<br />

and causes <strong>the</strong> circuit to oscillate.<br />

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

R 1<br />

2fmC

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