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<H1><A NAME="SECTION001220000000000000000">
Elementary filters</A>
</H1>
<P>
We saw in Chapter 7 how to predict the frequency and phase response of delay
networks. The art of filter design lies in finding a delay network whose
transfer function (which controls the frequency and phase response) has a
desired shape. We will develop an approach to building such delay networks
out of the two types of comb filters developed in Chapter 7: recirculating and
non-recirculating. Here we will be interested in the special case where the
delay is only one sample in length. In this situation, the frequency responses
shown in Figures <A HREF="node108.html#fig07.06">7.6</A> and <A HREF="node109.html#fig07.10">7.10</A> no longer look like combs;
the second peak recedes all the way to the sample rate, <IMG
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ALT="$2\pi $"> radians, when
<IMG
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ALT="$d=1$">. Since only frequencies between 0 and the Nyquist frequency (<IMG
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ALT="$\pi $">
radians) are audible, in effect there is only one peak when <IMG
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ALT="$d=1$">.
<P>
In the comb filters shown in Chapter 7, the peaks are situated at DC (zero
frequency), but we will often wish to place them at other, nonzero
frequencies. This is done using delay networks--comb
filters--with complex-valued gains.
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<LI><A NAME="tex2html2549"
HREF="node133.html">Elementary non-recirculating filter</A>
<LI><A NAME="tex2html2550"
HREF="node134.html">Non-recirculating filter, second form</A>
<LI><A NAME="tex2html2551"
HREF="node135.html">Elementary recirculating filter</A>
<LI><A NAME="tex2html2552"
HREF="node136.html">Compound filters</A>
<LI><A NAME="tex2html2553"
HREF="node137.html">Real outputs from complex filters</A>
<LI><A NAME="tex2html2554"
HREF="node138.html">Two recirculating filters for the price of one</A>
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<ADDRESS>
Miller Puckette
2006-12-30
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