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Op Amps for Everyone - The Repeater Builder's Technical ...

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Low-Pass Filter Design<br />

<strong>The</strong> multiplication of the denominator terms with each other yields an n th order polynomial<br />

of S, with n being the filter order.<br />

While n determines the gain rolloff above f C with n·20 dBdecade, a i and b i determine<br />

the gain behavior in the passband.<br />

In addition, the ratio<br />

bi<br />

a i<br />

more a filter inclines to instability.<br />

Q is defined as the pole quality. <strong>The</strong> higher the Q value, the<br />

16.3 Low-Pass Filter Design<br />

Equation 16–1 represents a cascade of second-order low-pass filters. <strong>The</strong> transfer function<br />

of a single stage is:<br />

A i<br />

(s) <br />

A 0<br />

1 ai s b i<br />

s 2 <br />

(16–2)<br />

For a first-order filter, the coefficient b is always zero (b 1 =0), thus yielding:<br />

A(s) A 0<br />

1 a 1<br />

s<br />

(16–3)<br />

<strong>The</strong> first-order and second-order filter stages are the building blocks <strong>for</strong> higher-order filters.<br />

Often the filters operate at unity gain (A 0 =1) to lessen the stringent demands on the op<br />

amp’s open-loop gain.<br />

Figure 16–11 shows the cascading of filter stages up to the sixth order. A filter with an even<br />

order number consists of second-order stages only, while filters with an odd order number<br />

include an additional first-order stage at the beginning.<br />

Active Filter Design Techniques<br />

16-11

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