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<H1><A ID="SECTION00960000000000000000">
Exercises</A>
</H1>
<P>
<OL>
<LI>A sound has fundamental 440. How could it be ring modulated to
give a tone at 110 Hertz with only odd partials? How could you then fill in the
even ones if you wanted to?
<P>
</LI>
<LI>A sinusoid with frequency 400 and unit peak amplitude is squared. What
are the amplitudes and frequencies of the new signal's components?
<P>
</LI>
<LI>What carrier and modulation frequencies would you give a two-operator FM
instrument to give frequencies of 618, 1000, and 2618 Hertz? (This is
a prominent feature of Chowning's <I>Stria</I> [<A
HREF="node202.html#r-dodge85">DJ85</A>].)
<P>
</LI>
<LI>Two sinusoids with frequency 300 and 400 Hertz and peak amplitude
one (so RMS amplitude <IMG
WIDTH="15" HEIGHT="15" ALIGN="BOTTOM" BORDER="0"
SRC="img549.png"
ALT="$\approx$">0.707) are multiplied. What is the RMS
amplitude of the product?
<P>
</LI>
<LI>Suppose you wanted to make FM yet more complicated by modulating the
<I>modulating</I> oscillator, as in:
<BR><P></P>
<DIV ALIGN="CENTER">
<!-- MATH
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SRC="img550.png"
ALT="\begin{displaymath}
\cos( \omega_c n + a \cos( \omega_m n + b \cos( \omega_p n )))
\end{displaymath}">
</DIV>
<BR CLEAR="ALL">
<P></P>
How, qualitatively speaking, would the spectrum differ from that of the simple
two-modulator example (Section <A HREF="node87.html#sect5.example.fm">5.5</A>)?
<P>
</LI>
<LI>A sinusoid at a frequency <IMG
WIDTH="14" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
SRC="img27.png"
ALT="$\omega $"> is ring modulated by another
sinusoid at exactly the same frequency. At what phase differences will the
DC component of the result disappear?
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<ADDRESS>
Miller Puckette
2006-12-30
</ADDRESS>
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