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

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Band-Rejection Filter Design<br />

16-36<br />

|A| — Ga<strong>in</strong> — dB<br />

5<br />

0<br />

–5<br />

–<strong>10</strong><br />

–15<br />

–20<br />

–25<br />

–30<br />

A1<br />

A2<br />

Q = 1<br />

–35<br />

<strong>10</strong>0 1 k <strong>10</strong> k <strong>10</strong>0 k<br />

f — Frequency — Hz<br />

Q = <strong>10</strong><br />

Figure 16–35. Ga<strong>in</strong> Responses of a Fourth-Order Butterworth Band-Pass and its Partial Filters<br />

16.6 Band-Rejection Filter Design<br />

A band-rejection filter is used to suppress a certa<strong>in</strong> frequency ra<strong>the</strong>r than a range of frequencies.<br />

Two of <strong>the</strong> most popular band-rejection filters are <strong>the</strong> active tw<strong>in</strong>-T and <strong>the</strong> active <strong>Wien</strong>-<br />

Rob<strong>in</strong>son circuit, both of which are second-order filters.<br />

To generate <strong>the</strong> transfer function of a second-order band-rejection filter, replace <strong>the</strong> S<br />

term of a first-order low-pass response with <strong>the</strong> transformation <strong>in</strong> 16–18:<br />

which gives:<br />

<br />

s 1 s<br />

A(s) A 0 1 s 2<br />

1 ·s s 2<br />

1 M<br />

(16–18)<br />

(16–19)<br />

Thus <strong>the</strong> passband characteristic of <strong>the</strong> low-pass filter is transformed <strong>in</strong>to <strong>the</strong> lower passband<br />

of <strong>the</strong> band-rejection filter. <strong>The</strong> lower passband is <strong>the</strong>n mirrored at <strong>the</strong> mid frequency,<br />

f m (Ω=1), <strong>in</strong>to <strong>the</strong> upper passband half (Figure 16–36).

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