replace '<A NAME=' with '<A ID='

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2022-04-12 23:32:40 -03:00
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commit 2f20b9ef0d
202 changed files with 5110 additions and 5110 deletions

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@@ -30,42 +30,42 @@ original version by: Nikos Drakos, CBLU, University of Leeds
<BODY >
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<H1><A NAME="SECTION001330000000000000000">
<H1><A ID="SECTION001330000000000000000">
Fourier analysis of non-periodic signals</A>
</H1>
@@ -110,12 +110,12 @@ Given a signal <IMG
ALT="$N-1$">,
the technique is to envelope the signal before doing the Fourier analysis.
The envelope shape is known as a
<A NAME="12499"></A><I>window function</I>.
<A ID="12499"></A><I>window function</I>.
Given a window function <IMG
WIDTH="33" HEIGHT="32" ALIGN="MIDDLE" BORDER="0"
SRC="img1123.png"
ALT="$w[n]$">, the
<A NAME="12501"></A><I>windowed Fourier transform</I>
<A ID="12501"></A><I>windowed Fourier transform</I>
is:
<BR><P></P>
<DIV ALIGN="CENTER">
@@ -136,7 +136,7 @@ is:
<P></P>
Much ink has been spilled over the design of suitable window functions for
particular situations, but here we will consider the simplest one, named the
<A NAME="12504"></A><A NAME="12505"></A><I>Hann</I>
<A ID="12504"></A><A ID="12505"></A><I>Hann</I>
window function (the name is sometimes corrupted to "Hanning" in DSP circles).
The Hann window is:
<BR><P></P>
@@ -302,7 +302,7 @@ Dirichlet kernel components are also shown separately.
<P>
<DIV ALIGN="CENTER"><A NAME="fig09.05"></A><A NAME="12536"></A>
<DIV ALIGN="CENTER"><A ID="fig09.05"></A><A ID="12536"></A>
<TABLE>
<CAPTION ALIGN="BOTTOM"><STRONG>Figure 9.5:</STRONG>
The magnitude M(k) of the Fourier transform of the Hann
@@ -450,7 +450,7 @@ Reducing the amplitude of the sidelobes reduces this interference.
<P>
<DIV ALIGN="CENTER"><A NAME="fig09.06"></A><A NAME="12558"></A>
<DIV ALIGN="CENTER"><A ID="fig09.06"></A><A ID="12558"></A>
<TABLE>
<CAPTION ALIGN="BOTTOM"><STRONG>Figure 9.6:</STRONG>
The Hann-windowed Fourier transform of a signal with two
@@ -507,36 +507,36 @@ four-period rule may be relaxed to three or even slightly less.
<P>
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<ADDRESS>