replace '<A NAME=' with '<A ID='
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node77.html
60
node77.html
@@ -30,43 +30,43 @@ original version by: Nikos Drakos, CBLU, University of Leeds
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<BODY >
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<!--Navigation Panel-->
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<A NAME="tex2html1697"
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<A ID="tex2html1697"
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HREF="node78.html">
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<IMG WIDTH="37" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="next"
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SRC="next.png"></A>
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<A NAME="tex2html1691"
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<A ID="tex2html1691"
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HREF="node75.html">
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<IMG WIDTH="26" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="up"
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SRC="up.png"></A>
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<A NAME="tex2html1685"
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<A ID="tex2html1685"
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HREF="node76.html">
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<IMG WIDTH="63" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="previous"
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SRC="prev.png"></A>
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<A NAME="tex2html1693"
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<A ID="tex2html1693"
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HREF="node4.html">
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<IMG WIDTH="65" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="contents"
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SRC="contents.png"></A>
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<A NAME="tex2html1695"
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<A ID="tex2html1695"
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HREF="node201.html">
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<IMG WIDTH="43" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="index"
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SRC="index.png"></A>
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<BR>
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<B> Next:</B> <A NAME="tex2html1698"
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<B> Next:</B> <A ID="tex2html1698"
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HREF="node78.html">Waveshaping</A>
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<B> Up:</B> <A NAME="tex2html1692"
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<B> Up:</B> <A ID="tex2html1692"
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HREF="node75.html">Modulation</A>
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<B> Previous:</B> <A NAME="tex2html1686"
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<B> Previous:</B> <A ID="tex2html1686"
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HREF="node76.html">Taxonomy of spectra</A>
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<B> <A NAME="tex2html1694"
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<B> <A ID="tex2html1694"
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HREF="node4.html">Contents</A></B>
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<B> <A NAME="tex2html1696"
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<B> <A ID="tex2html1696"
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HREF="node201.html">Index</A></B>
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<BR>
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<BR>
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<!--End of Navigation Panel-->
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<H1><A NAME="SECTION00920000000000000000"></A>
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<A NAME="sect5.ringmod"></A>
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<H1><A ID="SECTION00920000000000000000"></A>
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<A ID="sect5.ringmod"></A>
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<BR>
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Multiplying audio signals
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</H1>
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@@ -78,7 +78,7 @@ Chapter 1. For a full understanding of the algebra of audio
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signals we must also consider the situation where two audio signals,
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neither of which may be assumed to change slowly, are multiplied. The key to understanding
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what happens is the Cosine Product Formula:
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<A NAME="eq-cosinemultiplication"></A>
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<A ID="eq-cosinemultiplication"></A>
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<BR><P></P>
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<DIV ALIGN="CENTER">
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<!-- MATH
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@@ -182,16 +182,16 @@ one at the sum of the two original frequencies, and one at their difference.
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ALT="$\alpha-\beta$"> happens to be negative, simply switch the
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original two sinusoids and the difference will then be positive.) These
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two new components are called
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<A NAME="5635"></A><I>sidebands</I>.
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<A ID="5635"></A><I>sidebands</I>.
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<P>
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This gives us a technique for shifting the component frequencies
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of a sound, called
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<A NAME="5637"></A><A NAME="5638"></A><I>ring modulation</I>, which is shown in its simplest form in Figure
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<A ID="5637"></A><A ID="5638"></A><I>ring modulation</I>, which is shown in its simplest form in Figure
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<A HREF="#fig05.02">5.2</A>. An oscillator provides a
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<A NAME="5641"></A><I>carrier signal</I>, which
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<A ID="5641"></A><I>carrier signal</I>, which
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is simply multiplied by the input. In this context the input is called the
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<A NAME="5643"></A><I>modulating signal</I>.
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<A ID="5643"></A><I>modulating signal</I>.
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The term "ring modulation" is often used
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more generally to mean multiplying any two signals together, but here we'll
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just consider using a sinusoidal carrier signal. (The technique of ring
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@@ -202,7 +202,7 @@ ring modulator.)
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<P>
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<DIV ALIGN="CENTER"><A NAME="fig05.02"></A><A NAME="5649"></A>
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<DIV ALIGN="CENTER"><A ID="fig05.02"></A><A ID="5649"></A>
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<TABLE>
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<CAPTION ALIGN="BOTTOM"><STRONG>Figure 5.2:</STRONG>
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Block diagram for ring modulating an input signal with a sinusoid.</CAPTION>
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@@ -267,7 +267,7 @@ each at an amplitude of <IMG
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<P>
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<DIV ALIGN="CENTER"><A NAME="fig05.03"></A><A NAME="5655"></A>
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<DIV ALIGN="CENTER"><A ID="fig05.03"></A><A ID="5655"></A>
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<TABLE>
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<CAPTION ALIGN="BOTTOM"><STRONG>Figure 5.3:</STRONG>
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Sidebands arising from multiplying two sinusoids of frequency
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@@ -521,7 +521,7 @@ result are changed according to relatively simple rules.
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<P>
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<DIV ALIGN="CENTER"><A NAME="fig05.04"></A><A NAME="5669"></A>
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<DIV ALIGN="CENTER"><A ID="fig05.04"></A><A ID="5669"></A>
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<TABLE>
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<CAPTION ALIGN="BOTTOM"><STRONG>Figure 5.4:</STRONG>
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Result of ring modulation of a complex signal by a pure sinusoid:
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@@ -579,36 +579,36 @@ is the shift in spectral envelope.
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<P>
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<HR>
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HREF="node78.html">
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SRC="next.png"></A>
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<A NAME="tex2html1691"
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HREF="node75.html">
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<A NAME="tex2html1693"
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<A ID="tex2html1693"
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HREF="node4.html">
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<IMG WIDTH="65" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="contents"
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SRC="contents.png"></A>
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<A NAME="tex2html1695"
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<A ID="tex2html1695"
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HREF="node201.html">
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<IMG WIDTH="43" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="index"
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SRC="index.png"></A>
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<BR>
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<B> Next:</B> <A NAME="tex2html1698"
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<B> Next:</B> <A ID="tex2html1698"
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HREF="node78.html">Waveshaping</A>
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<B> Up:</B> <A NAME="tex2html1692"
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<B> Up:</B> <A ID="tex2html1692"
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HREF="node75.html">Modulation</A>
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<B> Previous:</B> <A NAME="tex2html1686"
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<B> Previous:</B> <A ID="tex2html1686"
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HREF="node76.html">Taxonomy of spectra</A>
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<B> <A NAME="tex2html1694"
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<B> <A ID="tex2html1694"
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HREF="node4.html">Contents</A></B>
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<B> <A NAME="tex2html1696"
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<B> <A ID="tex2html1696"
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HREF="node201.html">Index</A></B>
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<ADDRESS>
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