Csound

Jean Baptiste Joseph Fourier demonstrated around 1800 that any continuous function can be perfectly described as a sum of sine waves. This in fact means that you can create any sound, no matter how complex, if you know which sine waves to add together.

This concept really excited the early pioneers of electronic music, who imagined that sine waves would give them the power to create any sound imaginable and previously unimagined. Unfortunately, they soon realized that while adding sine waves is easy, interesting sounds must have a large number of sine waves which are constantly varying in frequency and amplitude, which turns out to be a hugely impractical task.

However, additive synthesis can provide unusual and interesting sounds. Moreover both, the power of modern computers, and the ability of managing data in a programming language offer new dimensions of working with this old tool. As with most things in Csound there are several ways to go about it. We will try to show some of them, and see how they are connected with different programming paradigms.

## What are the main parameters of Additive Synthesis?

Before we go into different ways of implementing additive synthesis in Csound, we shall think about the parameters we can consider. As additive synthesis is the addition of several sine generators, we have parameters on two different levels:

• For each sine, we have a frequency and an amplitude with an envelope.
• The frequency is usually a constant value. But of course you are principally free to vary the frequency. Natural sounds usually have very slight changes of partial frequencies.
• The amplitude must at least have a simple envelope like the well-known ADSR. But more complex ways of continuously altering the amplitude will make the sound much more lively.
• For the sound as a whole, these are the relevant parameters:
• The total number of sinusoids. A sound which consists of just three sinusoids is of course "poorer" than a sound which consists of 100 sinusoids.
• The frequency ratios of the sine generators. For a classical harmonic spectrum, the multipliers of the sinusoids are 1, 2, 3, ... (If your first sine is 100 Hz, the others are 200, 300, 400, ... Hz.) For an inharmonic or noisy spectrum, there are probably no simple integer ratios. This frequency ratio is mainly responsible for our perception of timbre.
• The base frequency is the frequency of the first partial. If the partials are showing an harmonic ratio, this frequency (in the example given 100 Hz) is also the overall perceived pitch.
• The amplitude ratios of the sinusoids. This is also very important for the resulting timbre of a sound. If the higher partials are relatively strong, the sound appears more brilliant; if the higher partials are soft, the sound appears dark and soft.
• The duration ratios of the sinusoids. In simple additive synthesis, all single sines have the same duration, but they may also differ. This usually relates to the envelopes: if the envelopes of different partials vary, some partials may die away faster than others.

It is not always the aim of additive synthesis to imitate natural sounds, but we can definitely learn a lot through the task of first analyzing and then attempting to imitate this sound using additive synthesis techniques. This is what a guitar note looks like when spectrally analyzed:

Each partial has its own movement and duration. We may or may not be able to achieve this successfully in additive synthesis. Let us begin with some simple sounds and consider ways of programming this with Csound; later we will look at some more complex sounds and advanced ways of programming this.

## Simple Additions of Sinusoids inside an Instrument

If additive synthesis amounts to the adding sine generators, it is straightforward to create multiple oscillators in a single instrument and to add the resulting audio signals together. In the following example, instrument 1 shows a harmonic spectrum, and instrument 2 an inharmonic one. Both instruments share the same amplitude multipliers: 1, 1/2, 1/3, 1/4, ... and receive the base frequency in Csound's pitch notation (octave.semitone) and the main amplitude in dB.

EXAMPLE 04A01.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;example by Andrés Cabrera
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

giSine    ftgen     0, 0, 2^10, 10, 1

;receive general pitch and volume from the score
ibasefrq  =         cpspch(p4) ;convert pitch values to frequency
ibaseamp  =         ampdbfs(p5) ;convert dB to amplitude
;create 8 harmonic partials
aOsc1     poscil    ibaseamp, ibasefrq, giSine
aOsc2     poscil    ibaseamp/2, ibasefrq*2, giSine
aOsc3     poscil    ibaseamp/3, ibasefrq*3, giSine
aOsc4     poscil    ibaseamp/4, ibasefrq*4, giSine
aOsc5     poscil    ibaseamp/5, ibasefrq*5, giSine
aOsc6     poscil    ibaseamp/6, ibasefrq*6, giSine
aOsc7     poscil    ibaseamp/7, ibasefrq*7, giSine
aOsc8     poscil    ibaseamp/8, ibasefrq*8, giSine
;apply simple envelope
kenv      linen     1, p3/4, p3, p3/4
;add partials and write to output
aOut = aOsc1 + aOsc2 + aOsc3 + aOsc4 + aOsc5 + aOsc6 + aOsc7 + aOsc8
outs      aOut*kenv, aOut*kenv
endin

ibasefrq  =         cpspch(p4)
ibaseamp  =         ampdbfs(p5)
;create 8 inharmonic partials
aOsc1     poscil    ibaseamp, ibasefrq, giSine
aOsc2     poscil    ibaseamp/2, ibasefrq*1.02, giSine
aOsc3     poscil    ibaseamp/3, ibasefrq*1.1, giSine
aOsc4     poscil    ibaseamp/4, ibasefrq*1.23, giSine
aOsc5     poscil    ibaseamp/5, ibasefrq*1.26, giSine
aOsc6     poscil    ibaseamp/6, ibasefrq*1.31, giSine
aOsc7     poscil    ibaseamp/7, ibasefrq*1.39, giSine
aOsc8     poscil    ibaseamp/8, ibasefrq*1.41, giSine
kenv      linen     1, p3/4, p3, p3/4
aOut = aOsc1 + aOsc2 + aOsc3 + aOsc4 + aOsc5 + aOsc6 + aOsc7 + aOsc8
outs aOut*kenv, aOut*kenv
endin

</CsInstruments>
<CsScore>
;          pch       amp
i 1 0 5    8.00      -10
i 1 3 5    9.00      -14
i 1 5 8    9.02      -12
i 1 6 9    7.01      -12
i 1 7 10   6.00      -10
s
i 2 0 5    8.00      -10
i 2 3 5    9.00      -14
i 2 5 8    9.02      -12
i 2 6 9    7.01      -12
i 2 7 10   6.00      -10
</CsScore>
</CsoundSynthesizer>
```

## Simple Additions of Sinusoids via the Score

A typical paradigm in programming: If you find some almost identical lines in your code, consider to abstract it. For the Csound Language this can mean, to move parameter control to the score. In our case, the lines

```aOsc1     poscil    ibaseamp, ibasefrq, giSine
aOsc2     poscil    ibaseamp/2, ibasefrq*2, giSine
aOsc3     poscil    ibaseamp/3, ibasefrq*3, giSine
aOsc4     poscil    ibaseamp/4, ibasefrq*4, giSine
aOsc5     poscil    ibaseamp/5, ibasefrq*5, giSine
aOsc6     poscil    ibaseamp/6, ibasefrq*6, giSine
aOsc7     poscil    ibaseamp/7, ibasefrq*7, giSine
aOsc8     poscil    ibaseamp/8, ibasefrq*8, giSine
```

can be abstracted to the form

```aOsc     poscil    ibaseamp*iampfactor, ibasefrq*ifreqfactor, giSine
```

with the parameters iampfactor (the relative amplitude of a partial) and ifreqfactor (the frequency multiplier) transferred to the score.

The next version simplifies the instrument code and defines the variable values as score parameters:

EXAMPLE 04A02.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;example by Andrés Cabrera and Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

giSine    ftgen     0, 0, 2^10, 10, 1

instr 1
iBaseFreq =         cpspch(p4)
iFreqMult =         p5 ;frequency multiplier
iBaseAmp  =         ampdbfs(p6)
iAmpMult  =         p7 ;amplitude multiplier
iFreq     =         iBaseFreq * iFreqMult
iAmp      =         iBaseAmp * iAmpMult
kEnv      linen     iAmp, p3/4, p3, p3/4
aOsc      poscil    kEnv, iFreq, giSine
outs      aOsc, aOsc
endin

</CsInstruments>
<CsScore>
;          freq      freqmult  amp       ampmult
i 1 0 7    8.09      1         -10       1
i . . 6    .         2         .         [1/2]
i . . 5    .         3         .         [1/3]
i . . 4    .         4         .         [1/4]
i . . 3    .         5         .         [1/5]
i . . 3    .         6         .         [1/6]
i . . 3    .         7         .         [1/7]
s
i 1 0 6    8.09      1.5       -10       1
i . . 4    .         3.1       .         [1/3]
i . . 3    .         3.4       .         [1/6]
i . . 4    .         4.2       .         [1/9]
i . . 5    .         6.1       .         [1/12]
i . . 6    .         6.3       .         [1/15]
</CsScore>
</CsoundSynthesizer>
```

You might say: Okay, where is the simplification? There are even more lines than before! - This is true, and this is certainly just a step on the way to a better code. The main benefit now is flexibility. Now our code is capable of realizing any number of partials, with any amplitude, frequency and duration ratios. Using the Csound score abbreviations (for instance a dot for repeating the previous value in the same p-field), you can do a lot of copy-and-paste, and focus on what is changing from line to line.

Note also that you are now calling one instrument in multiple instances at the same time for performing additive synthesis. In fact, each instance of the instrument contributes just one partial for the additive synthesis. This call of multiple and simultaneous instances of one instrument is also a typical procedure for situations like this, and for writing clean and effective Csound code. We will discuss later how this can be done in a more elegant way than in the last example.

## Creating Function Tables for Additive Synthesis

Before we continue on this road, let us go back to the first example and discuss a classical and abbreviated method of playing a number of partials. As we mentioned at the beginning, Fourier stated that any periodic oscillation can be described as a sum of simple sinusoids. If the single sinusoids are static (no individual envelope or duration), the resulting waveform will always be the same.

You see four sine generators, each with fixed frequency and amplitude relations, and mixed together. At the bottom of the illustration you see the composite waveform which repeats itself at each period. So - why not just calculate this composite waveform first, and then read it with just one oscillator?

This is what some Csound GEN routines do. They compose the resulting shape of the periodic wave, and store the values in a function table. GEN10 can be used for creating a waveform consisting of harmonically related partials. After the common GEN routine p-fields

```<table number>, <creation time>, <size in points>, <GEN number>
```

you have just to determine the relative strength of the harmonics. GEN09 is more complex and allows you to also control the frequency multiplier and the phase (0-360°) of each partial. We are able to reproduce the first example in a shorter (and computational faster) form:

EXAMPLE 04A03.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;example by Andrés Cabrera and Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

giSine    ftgen     0, 0, 2^10, 10, 1
giHarm    ftgen     1, 0, 2^12, 10, 1, 1/2, 1/3, 1/4, 1/5, 1/6, 1/7, 1/8
giNois    ftgen     2, 0, 2^12, 9, 100,1,0,  102,1/2,0,  110,1/3,0,  123,1/4,0,  126,1/5,0,  131,1/6,0,  139,1/7,0,  141,1/8,0

instr 1
iBasFreq  =         cpspch(p4)
iTabFreq  =         p7 ;base frequency of the table
iBasFreq  =         iBasFreq / iTabFreq
iBaseAmp  =         ampdb(p5)
iFtNum    =         p6
aOsc      poscil    iBaseAmp, iBasFreq, iFtNum
aEnv      linen     aOsc, p3/4, p3, p3/4
outs      aEnv, aEnv
endin

</CsInstruments>
<CsScore>
;          pch       amp       table      table base (Hz)
i 1 0 5    8.00      -10       1          1
i . 3 5    9.00      -14       .          .
i . 5 8    9.02      -12       .          .
i . 6 9    7.01      -12       .          .
i . 7 10   6.00      -10       .          .
s
i 1 0 5    8.00      -10       2          100
i . 3 5    9.00      -14       .          .
i . 5 8    9.02      -12       .          .
i . 6 9    7.01      -12       .          .
i . 7 10   6.00      -10       .          .
</CsScore>
</CsoundSynthesizer>
```

As you can see, for non-harmonically related partials, the construction of a table must be done with a special care. If the frequency multipliers in our first example started with 1 and 1.02, the resulting period is acually very long. For a base frequency of 100 Hz, you will have the frequencies of 100 Hz and 102 Hz overlapping each other. So you need 100 cycles from the 1.00 multiplier and 102 cycles from the 1.02 multiplier to complete one period and to start again both together from zero. In other words, we have to create a table which contains 100 respectively 102 periods, instead of 1 and 1.02. Then the table values are not related to 1 - as usual - but to 100. That is the reason we have to introduce a new parameter iTabFreq for this purpose.

This method of composing waveforms can also be used for generating the four standard historical shapes used in a synthesizer. An impulse wave can be created by adding a number of harmonics of the same strength. A sawtooth has the amplitude multipliers 1, 1/2, 1/3, ... for the harmonics. A square has the same multipliers, but just for the odd harmonics. A triangle can be calculated as 1 divided by the square of the odd partials, with changing positive and negative values. The next example creates function tables with just ten partials for each standard form.

EXAMPLE 04A04.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;example by Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

giImp  ftgen  1, 0, 4096, 10, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1
giSaw  ftgen  2, 0, 4096, 10, 1,1/2,1/3,1/4,1/5,1/6,1/7,1/8,1/9,1/10
giSqu  ftgen  3, 0, 4096, 10, 1, 0, 1/3, 0, 1/5, 0, 1/7, 0, 1/9, 0
giTri  ftgen  4, 0, 4096, 10, 1, 0, -1/9, 0, 1/25, 0, -1/49, 0, 1/81, 0

instr 1
asig   poscil .2, 457, p4
outs   asig, asig
endin

</CsInstruments>
<CsScore>
i 1 0 3 1
i 1 4 3 2
i 1 8 3 3
i 1 12 3 4
</CsScore>
</CsoundSynthesizer>
```

## Triggering Subinstruments for the Partials

Performing additive synthesis by designing partial strengths into function tables has the disadvantage that once a note has begun we do not have any way of varying the relative strengths of individual partials. There are various methods to circumvent the inflexibility of table-based additive synthesis such as morphing between several tables (using for example the ftmorf opcode). Next we will consider another approach: triggering one instance of a subinstrument for each partial, and exploring the possibilities of creating a spectrally dynamic sound using this technique.

Let us return to our second instrument (05A02.csd) which already made some abstractions and triggered one instrument instance for each partial. This was done in the score; but now we will trigger one complete note in one score line, not one partial. The first step is to assign the desired number of partials via a score parameter. The next example triggers any number of partials using this one value:

EXAMPLE 04A05.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;Example by Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

giSine    ftgen     0, 0, 2^10, 10, 1

instr 1 ;master instrument
inumparts =         p4 ;number of partials
ibasfreq  =         200 ;base frequency
ipart     =         1 ;count variable for loop
;loop for inumparts over the ipart variable
;and trigger inumpartss instanes of the subinstrument
loop:
ifreq     =         ibasfreq * ipart
iamp      =         1/ipart/inumparts
event_i   "i", 10, 0, p3, ifreq, iamp
loop_le   ipart, 1, inumparts, loop
endin

instr 10 ;subinstrument for playing one partial
ifreq     =         p4 ;frequency of this partial
iamp      =         p5 ;amplitude of this partial
aenv      transeg   0, .01, 0, iamp, p3-0.1, -10, 0
apart     poscil    aenv, ifreq, giSine
outs      apart, apart
endin

</CsInstruments>
<CsScore>
;         number of partials
i 1 0 3   10
i 1 3 3   20
i 1 6 3   2
</CsScore>
</CsoundSynthesizer>
```

This instrument can easily be transformed to be played via a midi keyboard. The next example connects the number of synthesized partials with the midi velocity. So if you play softly, the sound will have fewer partials than if a key is struck with force.

EXAMPLE 04A06.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;Example by Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

giSine    ftgen     0, 0, 2^10, 10, 1
massign   0, 1 ;all midi channels to instr 1

instr 1 ;master instrument
ibasfreq  cpsmidi       ;base frequency
iampmid   ampmidi   20 ;receive midi-velocity and scale 0-20
inparts   =         int(iampmid)+1 ;exclude zero
ipart     =         1 ;count variable for loop
;loop for inumparts over the ipart variable
;and trigger inumpartss instanes of the subinstrument
loop:
ifreq     =         ibasfreq * ipart
iamp      =         1/ipart/inparts
event_i   "i", 10, 0, 1, ifreq, iamp
loop_le   ipart, 1, inparts, loop
endin

instr 10 ;subinstrument for playing one partial
ifreq     =         p4 ;frequency of this partial
iamp      =         p5 ;amplitude of this partial
aenv      transeg   0, .01, 0, iamp, p3-.01, -3, 0
apart     poscil    aenv, ifreq, giSine
outs      apart/3, apart/3
endin

</CsInstruments>
<CsScore>
f 0 3600
</CsScore>
</CsoundSynthesizer>
```

Although this instrument is rather primitive it is useful to be able to control the timbre in this using key velocity. Let us continue to explore other methods of creating parameter variations in additive synthesis.

## User-controlled Random Variations in Additive Synthesis

In natural sounds, there is movement and change all the time. Even the best player or singer will not be able to play a note in the exact same way twice. And inside a tone, the partials have some unsteadiness all the time: slight excitations of the amplitudes, uneven durations, slight frequency movements. In an audio programming language like Csound, we can achieve these movements with random deviations. It is not so important whether we use randomness or not, rather in which way. The boundaries of random deviations must be adjusted as carefully as with any other parameter in electronic composition. If sounds using random deviations begin to sound like mistakes then it is probably less to do with actually using random functions but instead more to do with some poorly chosen boundaries.

Let us start with some random deviations in our subinstrument. These parameters can be affected:

• The frequency of each partial can be slightly detuned. The range of this possible maximum detuning can be set in cents (100 cent = 1 semitone).
• The amplitude of each partial can be altered, compared to its standard value. The alteration can be measured in Decibel (dB).
• The duration of each partial can be shorter or longer than the standard value. Let us define this deviation as a percentage. If the expected duration is five seconds, a maximum deviation of 100% means getting a value between half the duration (2.5 sec) and the double duration (10 sec).

The following example shows the effect of these variations. As a base - and as a reference to its author - we take the "bell-like sound" which Jean-Claude Risset created in his Sound Catalogue.1

EXAMPLE 04A07.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;Example by Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

;frequency and amplitude multipliers for 11 partials of Risset's bell
giFqs     ftgen     0, 0, -11, -2, .56,.563,.92,.923,1.19,1.7,2,2.74,3,3.74,4.07
giAmps    ftgen     0, 0, -11, -2, 1, 2/3, 1, 1.8, 8/3, 1.46, 4/3, 4/3, 1, 4/3
giSine    ftgen     0, 0, 2^10, 10, 1
seed      0

instr 1 ;master instrument
ibasfreq  =         400
ifqdev    =         p4 ;maximum freq deviation in cents
iampdev   =         p5 ;maximum amp deviation in dB
idurdev   =         p6 ;maximum duration deviation in %
indx      =         0 ;count variable for loop
loop:
ifqmult   tab_i     indx, giFqs ;get frequency multiplier from table
ifreq     =         ibasfreq * ifqmult
iampmult  tab_i     indx, giAmps ;get amp multiplier
iamp      =         iampmult / 20 ;scale
event_i   "i", 10, 0, p3, ifreq, iamp, ifqdev, iampdev, idurdev
loop_lt   indx, 1, 11, loop
endin

instr 10 ;subinstrument for playing one partial
;receive the parameters from the master instrument
ifreqnorm =         p4 ;standard frequency of this partial
iampnorm  =         p5 ;standard amplitude of this partial
ifqdev    =         p6 ;maximum freq deviation in cents
iampdev   =         p7 ;maximum amp deviation in dB
idurdev   =         p8 ;maximum duration deviation in %
;calculate frequency
icent     random    -ifqdev, ifqdev ;cent deviation
ifreq     =         ifreqnorm * cent(icent)
;calculate amplitude
idb       random    -iampdev, iampdev ;dB deviation
iamp      =         iampnorm * ampdb(idb)
;calculate duration
idurperc  random    -idurdev, idurdev ;duration deviation (%)
iptdur    =         p3 * 2^(idurperc/100)
p3        =         iptdur ;set p3 to the calculated value
;play partial
aenv      transeg   0, .01, 0, iamp, p3-.01, -10, 0
apart     poscil    aenv, ifreq, giSine
outs      apart, apart
endin

</CsInstruments>
<CsScore>
;         frequency   amplitude   duration
;         deviation   deviation   deviation
;         in cent     in dB       in %
;;unchanged sound (twice)
r 2
i 1 0 5   0           0           0
s
;;slight variations in frequency
r 4
i 1 0 5   25          0           0
;;slight variations in amplitude
r 4
i 1 0 5   0           6           0
;;slight variations in duration
r 4
i 1 0 5   0           0           30
;;slight variations combined
r 6
i 1 0 5   25          6           30
;;heavy variations
r 6
i 1 0 5   50          9           100
</CsScore>
</CsoundSynthesizer>
```

For a midi-triggered descendant of the instrument, we can - as one of many possible choices - vary the amount of possible random variation on the key velocity. So a key pressed softly plays the bell-like sound as described by Risset but as a key is struck with increasing force the sound produced will be increasingly altered.

EXAMPLE 04A08.csd

```<CsoundSynthesizer>
<CsOptions>
-o dac
</CsOptions>
<CsInstruments>
;Example by Joachim Heintz
sr = 44100
ksmps = 32
nchnls = 2
0dbfs = 1

;frequency and amplitude multipliers for 11 partials of Risset's bell
giFqs     ftgen     0, 0, -11, -2, .56,.563,.92,.923,1.19,1.7,2,2.74,3,3.74,4.07
giAmps    ftgen     0, 0, -11, -2, 1, 2/3, 1, 1.8, 8/3, 1.46, 4/3, 4/3, 1, 4/3
giSine    ftgen     0, 0, 2^10, 10, 1
seed      0
massign   0, 1 ;all midi channels to instr 1

instr 1 ;master instrument
;;scale desired deviations for maximum velocity
;frequency (cent)
imxfqdv   =         100
;amplitude (dB)
imxampdv  =         12
;duration (%)
imxdurdv  =         100
;;get midi values
ibasfreq  cpsmidi       ;base frequency
iampmid   ampmidi   1 ;receive midi-velocity and scale 0-1
;;calculate maximum deviations depending on midi-velocity
ifqdev    =         imxfqdv * iampmid
iampdev   =         imxampdv * iampmid
idurdev   =         imxdurdv * iampmid
;;trigger subinstruments
indx      =         0 ;count variable for loop
loop:
ifqmult   tab_i     indx, giFqs ;get frequency multiplier from table
ifreq     =         ibasfreq * ifqmult
iampmult  tab_i     indx, giAmps ;get amp multiplier
iamp      =         iampmult / 20 ;scale
event_i   "i", 10, 0, 3, ifreq, iamp, ifqdev, iampdev, idurdev
loop_lt   indx, 1, 11, loop
endin

instr 10 ;subinstrument for playing one partial
;receive the parameters from the master instrument
ifreqnorm =         p4 ;standard frequency of this partial
iampnorm  =         p5 ;standard amplitude of this partial
ifqdev    =         p6 ;maximum freq deviation in cents
iampdev   =         p7 ;maximum amp deviation in dB
idurdev   =         p8 ;maximum duration deviation in %
;calculate frequency
icent     random    -ifqdev, ifqdev ;cent deviation
ifreq     =         ifreqnorm * cent(icent)
;calculate amplitude
idb       random    -iampdev, iampdev ;dB deviation
iamp      =         iampnorm * ampdb(idb)
;calculate duration
idurperc  random    -idurdev, idurdev ;duration deviation (%)
iptdur    =         p3 * 2^(idurperc/100)
p3        =         iptdur ;set p3 to the calculated value
;play partial
aenv      transeg   0, .01, 0, iamp, p3-.01, -10, 0
apart     poscil    aenv, ifreq, giSine
outs      apart, apart
endin

</CsInstruments>
<CsScore>
f 0 3600
</CsScore>
</CsoundSynthesizer>
```

It will depend on the power of your computer whether you can play examples like this in realtime. Have a look at chapter 2D (Live Audio) for tips on getting the best possible performance from your Csound orchestra.

Additive synthesis can still be an exciting way of producing sounds. The nowadays computational power and programming structures open the way for new discoverings and ideas. The later examples were intended to show some of these potentials of additive synthesis in Csound.

1. Jean-Claude Risset, Introductory Catalogue of Computer Synthesized Sounds (1969), cited after Dodge/Jerse, Computer Music, New York / London 1985, p.94^