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

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

0<br />

–5<br />

–<strong>10</strong><br />

–15<br />

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

Q = 1<br />

Q = 0.25<br />

–20<br />

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

Frequency — Ω<br />

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

Active Filter Design Techniques<br />

All-Pass Filter Design<br />

Figure 16–41. Comparison of Q Between Passive and Active Band-Rejection Filters<br />

16.7 All-Pass Filter Design<br />

In comparison to <strong>the</strong> previously discussed filters, an all-pass filter has a constant ga<strong>in</strong><br />

across <strong>the</strong> entire frequency range, and a phase response that changes l<strong>in</strong>early with frequency.<br />

Because of <strong>the</strong>se properties, all-pass filters are used <strong>in</strong> phase compensation and signal<br />

delay circuits.<br />

Similar to <strong>the</strong> low-pass filters, all-pass circuits of higher order consist of cascaded first-order<br />

and second-order all-pass stages. To develop <strong>the</strong> all-pass transfer function from a<br />

low-pass response, replace A 0 with <strong>the</strong> conjugate complex denom<strong>in</strong>ator.<br />

<strong>The</strong> general transfer function of an allpass is <strong>the</strong>n:<br />

<br />

i<br />

1 ais bis A(s) <br />

2<br />

<br />

i<br />

1 ais bis2 (16–23)<br />

with a i and b i be<strong>in</strong>g <strong>the</strong> coefficients of a partial filter. <strong>The</strong> all-pass coefficients are listed <strong>in</strong><br />

Table 16–<strong>10</strong> of Section 16.9.<br />

Express<strong>in</strong>g Equation 16–23 <strong>in</strong> magnitude and phase yields:<br />

16-41

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