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

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Second Filter<br />

R 1 <br />

1<br />

<br />

2fca1C1 Closest 1% value is 2.1 kΩ.<br />

With C = <strong>10</strong>0nF,<br />

Active Filter Design Techniques<br />

Band-Pass Filter Design<br />

1<br />

2·<strong>10</strong>3Hz·0.756·<strong>10</strong>0·<strong>10</strong>9 2.<strong>10</strong>5 k<br />

F<br />

R1 1<br />

<br />

1<br />

fcCa1 ·<strong>10</strong>3 ·<strong>10</strong>0·<strong>10</strong>9 3.18 k<br />

·0.756<br />

Closest 1% value is 3.16 kΩ.<br />

R 2 <br />

a 1<br />

4fcCb 1<br />

Closest 1% value is 1.65 kΩ.<br />

<br />

Figure 16–30 shows <strong>the</strong> f<strong>in</strong>al filter circuit.<br />

V IN<br />

<strong>10</strong>0n<br />

2.<strong>10</strong>k<br />

0.9996<br />

4·<strong>10</strong>3 ·<strong>10</strong>0·<strong>10</strong>9 1.67 k<br />

·0.4772<br />

<strong>10</strong>0n <strong>10</strong>0n<br />

3.16k<br />

Figure 16–30. Third-Order Unity-Ga<strong>in</strong> Bessel High-Pass<br />

16.5 Band-Pass Filter Design<br />

1.65k<br />

In Section 16.4, a high-pass response was generated by replac<strong>in</strong>g <strong>the</strong> term S <strong>in</strong> <strong>the</strong> lowpass<br />

transfer function with <strong>the</strong> transformation 1/S. Likewise, a band-pass characteristic<br />

is generated by replac<strong>in</strong>g <strong>the</strong> S term with <strong>the</strong> transformation:<br />

1<br />

(16–7)<br />

s 1 s In this case, <strong>the</strong> passband characteristic of a low-pass filter is transformed <strong>in</strong>to <strong>the</strong> upper<br />

passband half of a band-pass filter. <strong>The</strong> upper passband is <strong>the</strong>n mirrored at <strong>the</strong> mid frequency,<br />

f m (Ω=1), <strong>in</strong>to <strong>the</strong> lower passband half.<br />

V OUT<br />

16-27

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