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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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Active Filter Design Techniques<br />

Band-Pass Filter Design<br />

Ami is <strong>the</strong> ga<strong>in</strong> at <strong>the</strong> mid frequency, fmi, of each partial filter<br />

Qi is <strong>the</strong> pole quality of each filter<br />

α and 1/α are <strong>the</strong> factors by which <strong>the</strong> mid frequencies of <strong>the</strong> <strong>in</strong>dividual filters, fm1 and fm2, derive from <strong>the</strong> mid frequency, fm, of <strong>the</strong> overall bandpass.<br />

In a fourth-order band-pass filter with high Q, <strong>the</strong> mid frequencies of <strong>the</strong> two partial filters<br />

differ only slightly from <strong>the</strong> overall mid frequency. This method is called staggered tun<strong>in</strong>g.<br />

Factor α needs to be determ<strong>in</strong>ed through successive approximation, us<strong>in</strong>g equation<br />

16–13:<br />

2 <br />

··a 2<br />

1<br />

b 1 1 2 1<br />

<br />

()2<br />

2 0<br />

2 b1 (16–13)<br />

with a 1 and b 1 be<strong>in</strong>g <strong>the</strong> second-order low-pass coefficients of <strong>the</strong> desired filter type.<br />

To simplify <strong>the</strong> filter design, Table 16–2 lists those coefficients, and provides <strong>the</strong> α values<br />

for three different quality factors, Q = 1, Q = <strong>10</strong>, and Q = <strong>10</strong>0.<br />

Table 16–2. Values of α For Different Filter Types and Different Qs<br />

Bessel Butterworth Tschebyscheff<br />

a1 1.3617 a1 1.4142 a1 1.0650<br />

b1 0.6180 b1 1.0000 b1 1.9305<br />

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

∆Ω 0.01 0.1 1 ∆Ω 0.01 0.1 1 ∆Ω 0.01 0.1 1<br />

α 1.0032 1.0324 1.438 α 1.0035 1.036 1.4426 α 1.0033 1.0338 1.39<br />

16-33

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