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

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All-Pass Filter Design<br />

16-42<br />

2 i<br />

1 bi 2 2 ai 2 ·e<br />

A(s) <br />

ja<br />

2 i<br />

1 bi 2 2 ai 2 ·eja This gives a constant ga<strong>in</strong> of 1, and a phase shift,φ, of:<br />

2 2 i<br />

ai arctan<br />

1 bi2 (16–24)<br />

(16–25)<br />

To transmit a signal with m<strong>in</strong>imum phase distortion, <strong>the</strong> all-pass filter must have a constant<br />

group delay across <strong>the</strong> specified frequency band. <strong>The</strong> group delay is <strong>the</strong> time by which<br />

<strong>the</strong> all-pass filter delays each frequency with<strong>in</strong> that band.<br />

<strong>The</strong> frequency at which <strong>the</strong> group delay drops to 1 2 –times its <strong>in</strong>itial value is <strong>the</strong> corner<br />

frequency, fC. <strong>The</strong> group delay is def<strong>in</strong>ed through:<br />

tgr d<br />

d<br />

(16–26)<br />

To present <strong>the</strong> group delay <strong>in</strong> normalized form, refer t gr to <strong>the</strong> period of <strong>the</strong> corner frequency,<br />

T C, of <strong>the</strong> all-pass circuit:<br />

Tgr tgr<br />

tgr·fc tgr·<br />

Tc<br />

c<br />

2<br />

Substitut<strong>in</strong>g t gr through Equation 16–26 gives:<br />

Tgr 1 d<br />

·<br />

2 d<br />

(16–27)<br />

(16–28)

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