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

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|A| [dB]<br />

0<br />

–3<br />

|A| [dB]<br />

0<br />

–3<br />

0 1 Ω<br />

0<br />

Figure 16–36. Low-Pass to Band-Rejection Transition<br />

Ω 1<br />

∆Ω<br />

1<br />

Band-Rejection Filter Design<br />

<strong>The</strong> corner frequency of <strong>the</strong> low-pass transforms to <strong>the</strong> lower and upper –3-dB frequencies<br />

of <strong>the</strong> band-rejection filter Ω 1 and Ω 2. <strong>The</strong> difference between both frequencies is <strong>the</strong><br />

normalized bandwidth ∆Ω:<br />

max m<strong>in</strong><br />

Identical to <strong>the</strong> selectivity of a band-pass filter, <strong>the</strong> quality of <strong>the</strong> filter rejection is def<strong>in</strong>ed<br />

as:<br />

Q fm<br />

<br />

1<br />

B <br />

<strong>The</strong>refore, replac<strong>in</strong>g ∆Ω <strong>in</strong> Equation 16–19 with 1/Q yields:<br />

16.6.1 Active Tw<strong>in</strong>-T Filter<br />

A(s) A0 1 s2 1 1<br />

·s s2<br />

Q<br />

Ω 2<br />

Active Filter Design Techniques<br />

Ω<br />

(16–20)<br />

<strong>The</strong> orig<strong>in</strong>al tw<strong>in</strong>-T filter, shown <strong>in</strong> Figure 16–37, is a passive RC-network with a quality<br />

factor of Q = 0.25. To <strong>in</strong>crease Q, <strong>the</strong> passive filter is implemented <strong>in</strong>to <strong>the</strong> feedback loop<br />

of an amplifier, thus turn<strong>in</strong>g <strong>in</strong>to an active band-rejection filter, shown <strong>in</strong> Figure 16–38.<br />

V IN<br />

Figure 16–37. Passive Tw<strong>in</strong>-T Filter<br />

C<br />

R/2<br />

2C<br />

C<br />

R R<br />

V OUT<br />

16-37

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