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

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16.4.1 First-Order High-Pass Filter<br />

Active Filter Design Techniques<br />

High-Pass Filter Design<br />

Figure 16–25 and 16–26 show a first-order high-pass filter <strong>in</strong> <strong>the</strong> non<strong>in</strong>vert<strong>in</strong>g and <strong>the</strong> <strong>in</strong>vert<strong>in</strong>g<br />

configuration.<br />

V IN<br />

Figure 16–25. First-Order Non<strong>in</strong>vert<strong>in</strong>g High-Pass Filter<br />

V IN<br />

Figure 16–26. First-Order Invert<strong>in</strong>g High-Pass Filter<br />

<strong>The</strong> transfer functions of <strong>the</strong> circuits are:<br />

A(s) <br />

1 R2 R3 1 1<br />

· cR1C1 1 s<br />

C 1<br />

C 1<br />

R 1<br />

R 1<br />

R 3<br />

R 2<br />

R 2<br />

and<br />

V OUT<br />

V OUT<br />

A(s) <br />

R2 R1 1 1<br />

· cR1C1 1 s<br />

<strong>The</strong> negative sign <strong>in</strong>dicates that <strong>the</strong> <strong>in</strong>vert<strong>in</strong>g amplifier generates a 180° phase shift from<br />

<strong>the</strong> filter <strong>in</strong>put to <strong>the</strong> output.<br />

<strong>The</strong> coefficient comparison between <strong>the</strong> two transfer functions and Equation 16–6 provides<br />

two different passband ga<strong>in</strong> factors:<br />

A 1 R 2<br />

R 3<br />

and<br />

A R 2<br />

R 1<br />

while <strong>the</strong> term for <strong>the</strong> coefficient a 1 is <strong>the</strong> same for both circuits:<br />

a 1 <br />

1<br />

cR 1 C 1<br />

16-23

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