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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 />

16-40<br />

mid-frequency:<br />

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

rejection quality: Q <br />

fm 1<br />

2RC<br />

A 0 <br />

1 <br />

1 <br />

3<br />

To calculate <strong>the</strong> <strong>in</strong>dividual component values, establish <strong>the</strong> follow<strong>in</strong>g design procedure:<br />

1) Def<strong>in</strong>e f m and C and calculate R with:<br />

R 1<br />

2fmC<br />

2) Specify Q and determ<strong>in</strong>e α via:<br />

3Q 1<br />

3) Specify A 0 and determ<strong>in</strong>e β via:<br />

A 0 ·3Q<br />

4) Def<strong>in</strong>e R 2 and calculate R 3 and R 4 with:<br />

and<br />

R 3 R 2<br />

<br />

R 4 R 2<br />

<br />

In comparison to <strong>the</strong> tw<strong>in</strong>-T circuit, <strong>the</strong> <strong>Wien</strong>-Rob<strong>in</strong>son filter allows modification of <strong>the</strong><br />

passband ga<strong>in</strong>, A 0, without affect<strong>in</strong>g <strong>the</strong> quality factor, Q.<br />

If f m is not completely suppressed due to component tolerances of R and C, a f<strong>in</strong>e-tun<strong>in</strong>g<br />

of <strong>the</strong> resistor 2R 2 is required.<br />

Figure 16–41 shows a comparison between <strong>the</strong> filter response of a passive band-rejection<br />

filter with Q = 0.25, and an active second-order filter with Q = 1, and Q = <strong>10</strong>.

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