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<H2><A NAME="SECTION00883000000000000000">
Additive synthesis: Risset's bell</A>
</H2>
<A NAME="4778"></A>
<P>
The abstraction mechanism of Pd, which we used above to make a reusable ADSR
generator, is also useful for making voice banks. Here we will use
abstractions to organize banks of oscillators for additive synthesis. There
are many possible ways of organizing oscillator banks besides
those shown here.
<P>
The simplest and most direct organization of the sinusoids is to form
partials to add up to a note. The result is monophonic, in the sense that
the patch will play only one note at a time, which, however, will consist of
several sinusoids whose individual frequencies and amplitudes might depend both
on those of the note we're playing, and also on their individual placement
in a harmonic (or inharmonic) overtone series.
<P>
Example D07.additive.pd (Figure <A HREF="#fig04.16">4.16</A>) uses a bank of 11 copies
of an abstraction named <TT>partial</TT> (Figure <A HREF="#fig04.17">4.17</A>) in an
imitation of a well-known bell instrument by Jean-Claude Risset. As described
in [<A
HREF="node202.html#r-dodge85">DJ85</A>, p. 94], the bell sound has 11 partials, each with its own
relative amplitude, frequency, and duration.
<P>
<DIV ALIGN="CENTER"><A NAME="fig04.16"></A><A NAME="4890"></A>
<TABLE>
<CAPTION ALIGN="BOTTOM"><STRONG>Figure 4.16:</STRONG>
A Pd realization of Jean-Claude Risset's bell instrument. The
bell sound is made by summing 11 sinusoids, each made by a copy of the
<TT>partial</TT> abstraction.</CAPTION>
<TR><TD><IMG
WIDTH="498" HEIGHT="389" BORDER="0"
SRC="img384.png"
ALT="\begin{figure}\psfig{file=figs/fig04.16.ps}\end{figure}"></TD></TR>
</TABLE>
</DIV>
<P>
<DIV ALIGN="CENTER"><A NAME="fig04.17"></A><A NAME="4891"></A>
<TABLE>
<CAPTION ALIGN="BOTTOM"><STRONG>Figure 4.17:</STRONG>
The <TT>partial</TT> abstraction used by Risset's bell instrument
from Figure <A HREF="#fig04.16">4.16</A>.</CAPTION>
<TR><TD><IMG
WIDTH="487" HEIGHT="376" BORDER="0"
SRC="img385.png"
ALT="\begin{figure}\psfig{file=figs/fig04.17.ps}\end{figure}"></TD></TR>
</TABLE>
</DIV>
<P>
For each note, the <TT>partial</TT> abstraction computes a simple (quartic)
amplitude envelope consisting only of an attack and a decay segment; there is
no sustain or release segment. This is multiplied by a sinusoid, and the
product is added into a summing bus. Two new object classes are introduced
to implement the summing bus:
<P>
<BR><!-- MATH
$\fbox{ \texttt{catch\~}}$
-->
<IMG
WIDTH="69" HEIGHT="39" ALIGN="MIDDLE" BORDER="0"
SRC="img386.png"
ALT="\fbox{ \texttt{catch\~}}">:
<A NAME="4908"></A>define and output a summing bus. The creation argument (``sum-bus" in this example)
gives the summing bus a name so that <TT>throw~</TT> objects below can refer
to it. You may have as many summing busses (and hence <TT>catch~</TT> objects)
as you like but they must all have different names.
<P>
<BR><!-- MATH
$\fbox{ \texttt{throw\~}}$
-->
<IMG
WIDTH="69" HEIGHT="39" ALIGN="MIDDLE" BORDER="0"
SRC="img388.png"
ALT="\fbox{ \texttt{throw\~}}">:
<A NAME="4909"></A>add to a summing bus. The creation argument selects which summing bus to
use.
<P>
The control interface is crude: number boxes control the ``fundamental"
frequency of the bell and its duration. Sending a ``bang" message to
the <TT>s trigger</TT> object starts a note. (The note then decays over
the period of time controlled by the duration parameter; there is no
separate trigger to stop the note). There is no amplitude
control except via the <TT>output~</TT> object.
<P>
The four arguments to each invocation of the <TT>partial</TT> abstraction specify:
<OL>
<LI>amplitude. The amplitude of the partial at its peak, at the
end of the attack and the beginning of the decay of the note.
<P>
</LI>
<LI>relative duration. This is multiplied by the overall note duration
(controlled in the main patch) to
determine the duration of the decay portion of the sinusoid. Individual partials
may thus have different decay times, so that some partials die out faster than
others, under the main patch's overall control.
<P>
</LI>
<LI>relative frequency. As with the relative duration, this controls each
partial's frequency as a multiple of the overall frequency controlled in the
main patch.
<P>
</LI>
<LI>detune. A frequency in Hertz to be added to the product of the global
frequency and the relative frequency.
<P>
</LI>
</OL>
Inside the <TT>partial</TT> abstraction, the amplitude is simply taken
directly from the ``$1" argument (multiplying by 0.1 to adjust for
the high individual amplitudes); the duration is calculated from the
<TT>r duration</TT> object, multiplying it by the ``$2" argument.
The frequency is computed as <IMG
WIDTH="48" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img390.png"
ALT="$fp+d$"> where <IMG
WIDTH="13" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
SRC="img112.png"
ALT="$f$"> is the global frequency (from
the <TT>r frequency</TT> object), <IMG
WIDTH="11" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
SRC="img57.png"
ALT="$p$"> is the relative frequency of the
partial, and <IMG
WIDTH="11" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
SRC="img28.png"
ALT="$d$"> is the detune frequency.
<P>
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<ADDRESS>
Miller Puckette
2006-12-30
</ADDRESS>
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