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

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16.2.2 Tschebyscheff Low-Pass Filters<br />

Fundamentals of Low-Pass Filters<br />

<strong>The</strong> Tschebyscheff low-pass filters provide an even higher ga<strong>in</strong> rolloff above f C. However,<br />

as Figure 16–6 shows, <strong>the</strong> passband ga<strong>in</strong> is not monotone, but conta<strong>in</strong>s ripples of<br />

constant magnitude <strong>in</strong>stead. For a given filter order, <strong>the</strong> higher <strong>the</strong> passband ripples, <strong>the</strong><br />

higher <strong>the</strong> filter’s rolloff.<br />

|A| — Ga<strong>in</strong> — dB<br />

<strong>10</strong><br />

0<br />

–<strong>10</strong><br />

–20<br />

–30<br />

–40<br />

–50<br />

9th Order<br />

2nd Order<br />

–60<br />

0.01 0.1 1<br />

Frequency — Ω<br />

<strong>10</strong><br />

Figure 16–6. Ga<strong>in</strong> Responses of Tschebyscheff Low-Pass Filters<br />

4th Order<br />

With <strong>in</strong>creas<strong>in</strong>g filter order, <strong>the</strong> <strong>in</strong>fluence of <strong>the</strong> ripple magnitude on <strong>the</strong> filter rolloff dim<strong>in</strong>ishes.<br />

Each ripple accounts for one second-order filter stage. Filters with even order numbers<br />

generate ripples above <strong>the</strong> 0-dB l<strong>in</strong>e, while filters with odd order numbers create ripples<br />

below 0 dB.<br />

Tschebyscheff filters are often used <strong>in</strong> filter banks, where <strong>the</strong> frequency content of a signal<br />

is of more importance than a constant amplification.<br />

16.2.3 Bessel Low-Pass Filters<br />

<strong>The</strong> Bessel low-pass filters have a l<strong>in</strong>ear phase response (Figure 16–7) over a wide frequency<br />

range, which results <strong>in</strong> a constant group delay (Figure 16–8) <strong>in</strong> that frequency<br />

range. Bessel low-pass filters, <strong>the</strong>refore, provide an optimum square-wave transmission<br />

behavior. However, <strong>the</strong> passband ga<strong>in</strong> of a Bessel low-pass filter is not as flat as that of<br />

<strong>the</strong> Butterworth low-pass, and <strong>the</strong> transition from passband to stopband is by far not as<br />

sharp as that of a Tschebyscheff low-pass filter (Figure 16–9).<br />

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

Active Filter Design Techniques<br />

16-7

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