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

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Active Filter Design Techniques<br />

High-Pass Filter Design<br />

To simplify <strong>the</strong> circuit design, it is common to choose unity-ga<strong>in</strong> (α = 1), and C 1 = C 2 = C.<br />

<strong>The</strong> transfer function of <strong>the</strong> circuit <strong>in</strong> Figure 16–28 <strong>the</strong>n simplifies to:<br />

A(s) <br />

1<br />

1 2<br />

cR1C · 1 s <br />

1<br />

c 2R1R2C <strong>The</strong> coefficient comparison between this transfer function and Equation 16–5 yields:<br />

A 1<br />

a 1 2<br />

cR 1 C<br />

b 1 <br />

1<br />

c 2 R 1 R 2 C 2<br />

s 2<br />

2 · 1<br />

Given C, <strong>the</strong> resistor values for R 1 and R 2 are calculated through:<br />

R 1 1<br />

R 2 <br />

fcCa1 a1 4fcCb1 16.4.2.2 Multiple Feedback Topology<br />

<strong>The</strong> MFB topology is commonly used <strong>in</strong> filters that have high Qs and require a high ga<strong>in</strong>.<br />

To simplify <strong>the</strong> computation of <strong>the</strong> circuit, capacitors C 1 and C 3 assume <strong>the</strong> same value<br />

(C 1 = C 3 = C) as shown <strong>in</strong> Figure 16–29.<br />

V IN<br />

C 1 =C<br />

C 2<br />

C 3 =C<br />

Figure 16–29. Second-Order MFB High-Pass Filter<br />

<strong>The</strong> transfer function of <strong>the</strong> circuit <strong>in</strong> Figure 16–29 is:<br />

A(s) <br />

R 2<br />

R 1<br />

C<br />

C2 1 2CC2 · cR1CC2 1 s 2CC2 · cR1CC2 1<br />

s2 V OUT<br />

16-25

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