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

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Fundamentals of Low-Pass Filters<br />

16-2<br />

This chapter covers active filters. It <strong>in</strong>troduces <strong>the</strong> three ma<strong>in</strong> filter optimizations (Butterworth,<br />

Tschebyscheff, and Bessel), followed by five sections describ<strong>in</strong>g <strong>the</strong> most common<br />

active filter applications: low-pass, high-pass, band-pass, band-rejection, and all-pass filters.<br />

Ra<strong>the</strong>r than resembl<strong>in</strong>g just ano<strong>the</strong>r filter book, <strong>the</strong> <strong>in</strong>dividual filter sections are written<br />

<strong>in</strong> a cookbook style, thus avoid<strong>in</strong>g tedious ma<strong>the</strong>matical derivations. Each section<br />

starts with <strong>the</strong> general transfer function of a filter, followed by <strong>the</strong> design equations to calculate<br />

<strong>the</strong> <strong>in</strong>dividual circuit components. <strong>The</strong> chapter closes with a section on practical<br />

design h<strong>in</strong>ts for s<strong>in</strong>gle-supply filter designs.<br />

16.2 Fundamentals of Low-Pass Filters<br />

<strong>The</strong> most simple low-pass filter is <strong>the</strong> passive RC low-pass network shown <strong>in</strong> Figure 16–2.<br />

Figure 16–2. First-Order Passive RC Low-Pass<br />

Its transfer function is:<br />

A(s) <br />

V IN<br />

R<br />

C<br />

1<br />

RC<br />

s 1<br />

<br />

RC<br />

1<br />

1 sRC<br />

where <strong>the</strong> complex frequency variable, s = jω+σ , allows for any time variable signals. For<br />

pure s<strong>in</strong>e waves, <strong>the</strong> damp<strong>in</strong>g constant, σ, becomes zero and s = jω .<br />

For a normalized presentation of <strong>the</strong> transfer function, s is referred to <strong>the</strong> filter’s corner<br />

frequency, or –3 dB frequency, ω C, and has <strong>the</strong>se relationships:<br />

s s<br />

<br />

C j<br />

j<br />

C f<br />

j<br />

fC With <strong>the</strong> corner frequency of <strong>the</strong> low-pass <strong>in</strong> Figure 16–2 be<strong>in</strong>g f C = 1/2πRC, s becomes<br />

s = sRC and <strong>the</strong> transfer function A(s) results <strong>in</strong>:<br />

A(s) 1<br />

1 s<br />

<strong>The</strong> magnitude of <strong>the</strong> ga<strong>in</strong> response is:<br />

|A| <br />

1<br />

1 2 <br />

For frequencies Ω >> 1, <strong>the</strong> rolloff is 20 dB/decade. For a steeper rolloff, n filter stages<br />

can be connected <strong>in</strong> series as shown <strong>in</strong> Figure 16–3. To avoid load<strong>in</strong>g effects, op amps,<br />

operat<strong>in</strong>g as impedance converters, separate <strong>the</strong> <strong>in</strong>dividual filter stages.<br />

V OUT

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