Additive synthesis concepts

Overview

Additive synthesis creates complex sounds by adding together individual sinusoidal signals called partials . A partial's frequency and amplitude are each time-varying functions, so a partial is a more flexible version of the harmonic associated with a Fourier series decomposition of a periodic waveform.

In this module you will learn about partials, how to model the timbre of natural instruments, various sources of control information for partials, and how to make a sinusoidal oscillator with an instantaneous frequency that varies with time.

Partials

A partial is a generalization of the harmonic associated with a Fourier series representation of a periodic waveform. The screencast video of introduces important concepts associated with partials.

Modeling timbre of natural instruments

Perception of an instrument's timbre relies heavily on the attack transient of a note. Since partials can effectively enter and leave the signal at any time, additive synthesis is a good way to model physical instruments. The screencast video of discusses three important design requirements for partials necessary to successfully model a physical instrument.

Sources of control information

The time-varying frequency of a partial is called its frequency trajectory , and is best visualized as a track or path on a spectrogram display. Similarly, the time-varying amplitude of a partial is called its amplitude trajectory . Control information for these trajectories can be derived from a number of sources. Perhaps the most obvious source is a spectral analysis of a physical instrument to be modeled. The screencast video of discusses this concept and demonstrates how a trumpet can be well-modeled by adding suitable partials.

The code for the LabVIEW VI demonstrated within the video is available here: trumpet.zip . This VI requires installation of the TripleDisplay front-panel indicator.

Control information can also be derived from other domains not necessarily related to music. The screencast video of provides some examples of non-music control information, and illustrates how an edge boundary from an image can be "auralized" by translating the edge into a partial's frequency trajectory.

Instantaneous frequency

The frequency trajectory of a partial is defined as a time-varying frequency $f(t)$ . Since a constant-frequency and constant-amplitude sinusoid is mathematically described as $y(t)=A\sin (2\pi f_{0}t)$ , intuition perhaps suggests that the partial should be expressed as $y(t)=a(t)\sin (2\pi f(t)t)$ , where $a(t)$ is the amplitude trajectory. However, as shown in the screencast video of this intuitive result is incorrect; the video derives the correct equation to describe a partial in terms of its trajectories $f(t)$ and $a(t)$ .