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

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

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Practical Design H<strong>in</strong>ts<br />

V IN<br />

16-50<br />

C C<br />

R 1<br />

V MID<br />

R 2<br />

+V CC<br />

C B<br />

+V CC<br />

R B<br />

V OUT<br />

R B<br />

V IN<br />

V MID<br />

C 1 =C<br />

Figure 16–50. Bias<strong>in</strong>g a Sallen-Key and an MFB High-Pass Filter<br />

16.8.2 Capacitor Selection<br />

<strong>The</strong> tolerance of <strong>the</strong> selected capacitors and resistors depends on <strong>the</strong> filter sensitivity and<br />

on <strong>the</strong> filter performance.<br />

Sensitivity is <strong>the</strong> measure of <strong>the</strong> vulnerability of a filter’s performance to changes <strong>in</strong> component<br />

values. <strong>The</strong> important filter parameters to consider are <strong>the</strong> corner frequency, f C,<br />

and Q.<br />

For example, when Q changes by ± 2% due to a ± 5% change <strong>in</strong> <strong>the</strong> capacitance value,<br />

<strong>the</strong>n <strong>the</strong> sensitivity of Q to capacity changes is expressed as: Q<br />

s <br />

2%<br />

0.4<br />

%<br />

C 5% % . <strong>The</strong><br />

follow<strong>in</strong>g sensitivity approximations apply to second-order Sallen-Key and MFB filters:<br />

s Q<br />

s<br />

Q fc fc<br />

s s 0.5<br />

%<br />

C R C R %<br />

Although 0.5 %/% is a small difference from <strong>the</strong> ideal parameter, <strong>in</strong> <strong>the</strong> case of higher-order<br />

filters, <strong>the</strong> comb<strong>in</strong>ation of small Q and f C differences <strong>in</strong> each partial filter can significantly<br />

modify <strong>the</strong> overall filter response from its <strong>in</strong>tended characteristic.<br />

Figures 16.51 and 16.52 show how an <strong>in</strong>tended eighth-order Butterworth low-pass can<br />

turn <strong>in</strong>to a low-pass with Tschebyscheff characteristic ma<strong>in</strong>ly due to capacitance changes<br />

from <strong>the</strong> partial filters.<br />

Figure 16–51 shows <strong>the</strong> differences between <strong>the</strong> ideal and <strong>the</strong> actual frequency responses<br />

of <strong>the</strong> four partial filters. <strong>The</strong> overall filter responses are shown <strong>in</strong> Figure 16–52.<br />

C 2<br />

C 3 =C<br />

R 2<br />

V MID<br />

R 1<br />

+V CC<br />

V OUT

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