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<H2><A NAME="SECTION001234000000000000000"></A>
<A NAME="sect8.twopolebandpass"></A>
<BR>
Band-pass filter
</H2>
<P>
Starting with the three filter types shown above, which all have real-valued
poles and zeros, we now transform them to operate on bands located off the real
axis. The low-pass, high-pass, and shelving filters will then become
band-pass, stop-band, and peaking filters. First we develop the band-pass
filter. Suppose we want a center frequency at <IMG
WIDTH="14" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img27.png"
ALT="$\omega $"> radians and a
bandwidth of <IMG
WIDTH="13" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img8.png"
ALT="$\beta $">. We take the low-pass filter with cutoff frequency
<IMG
WIDTH="13" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img8.png"
ALT="$\beta $">; its pole is located, for small values of <IMG
WIDTH="13" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img8.png"
ALT="$\beta $">, roughly at
<IMG
WIDTH="69" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img919.png"
ALT="$p = 1 - \beta$">.
Now rotate this value by <IMG
WIDTH="14" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img27.png"
ALT="$\omega $"> radians in the complex plane, i.e.,
multiply by the complex number <!-- MATH
$\cos \omega + i \sin \omega$
-->
<IMG
WIDTH="98" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img920.png"
ALT="$\cos \omega + i \sin \omega$">. The new pole
is at:
<BR><P></P>
<DIV ALIGN="CENTER">
<!-- MATH
\begin{displaymath}
{P_1} = (1 - \beta) (\cos \omega + i \sin \omega)
\end{displaymath}
-->
<IMG
WIDTH="194" HEIGHT="28" BORDER="0"
SRC="img921.png"
ALT="\begin{displaymath}
{P_1} = (1 - \beta) (\cos \omega + i \sin \omega)
\end{displaymath}">
</DIV>
<BR CLEAR="ALL">
<P></P>
To get a real-valued output, this must be paired with another pole:
<BR><P></P>
<DIV ALIGN="CENTER">
<!-- MATH
\begin{displaymath}
{P_2} = \overline{P_1} = (1 - \beta) (\cos \omega - i \sin \omega)
\end{displaymath}
-->
<IMG
WIDTH="233" HEIGHT="28" BORDER="0"
SRC="img922.png"
ALT="\begin{displaymath}
{P_2} = \overline{P_1} = (1 - \beta) (\cos \omega - i \sin \omega)
\end{displaymath}">
</DIV>
<BR CLEAR="ALL">
<P></P>
The resulting pole-zero plot is as shown in Figure <A HREF="#fig08.15">8.15</A>.
<P>
<DIV ALIGN="CENTER"><A NAME="fig08.15"></A><A NAME="10361"></A>
<TABLE>
<CAPTION ALIGN="BOTTOM"><STRONG>Figure 8.15:</STRONG>
Two-pole band-pass filter: (a) pole-zero diagram; (b)
frequency response.</CAPTION>
<TR><TD><IMG
WIDTH="537" HEIGHT="244" BORDER="0"
SRC="img923.png"
ALT="\begin{figure}\psfig{file=figs/fig08.15.ps}\end{figure}"></TD></TR>
</TABLE>
</DIV>
<P>
The peak is approximately (not exactly) at the desired center frequency
<IMG
WIDTH="14" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img27.png"
ALT="$\omega $">, and the frequency response drops by 3 decibels approximately <IMG
WIDTH="13" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img8.png"
ALT="$\beta $">
radians above and below it. It is often desirable to normalize the filter to
have a peak gain near unity; this is done by multiplying the input or output by
the product of the distances of the two poles to the peak on the circle, or
(very approximately):
<BR><P></P>
<DIV ALIGN="CENTER">
<!-- MATH
\begin{displaymath}
\beta * (\beta + 2 \omega)
\end{displaymath}
-->
<IMG
WIDTH="84" HEIGHT="28" BORDER="0"
SRC="img924.png"
ALT="\begin{displaymath}
\beta * (\beta + 2 \omega)
\end{displaymath}">
</DIV>
<BR CLEAR="ALL">
<P></P>
For some applications it is desirable to add a zero at the points <IMG
WIDTH="11" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img262.png"
ALT="$1$"> and <IMG
WIDTH="23" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
SRC="img401.png"
ALT="$-1$">,
so that the gain drops to zero at angular frequencies <IMG
WIDTH="11" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img179.png"
ALT="$0$"> and <IMG
WIDTH="13" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img41.png"
ALT="$\pi $">.
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<ADDRESS>
Miller Puckette
2006-12-30
</ADDRESS>
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