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Music 171:

Tamara Smyth, [email protected] Department of Music, University of California, San Diego (UCSD) October 22, 2019

1 Adding Sinusoids at Different

• Adding sinusoids of the same produces another sinusoid at that frequency (with possibly different and/or ).

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Figure 1: Adding 2 sinusoids at different frequencies. • Adding sinusoids with different frequencies results in a signal that is no longer sinusoidal. But is it periodic?

Music 171: Additive Synthesis 2 A Non-Sinusoidal Periodic Signal

• If the frequencies of the added sinusoids are integer multiples of the fundamental, the resulting signal will be periodic.

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Figure 2: Adding sinusoids at 3, 6, 9 Hz produces a periodic signal at 3 Hz.

• Sinusoidal components, or partials that are integer multiples of a fundamental are calle .

Music 171: Additive Synthesis 3 Viewing in the Frequency Domain

• When viewing in the frequency domain, a “spike” at a frequency indicates there is a sinusoid in the signal at that frequency.

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Figure 3: Adding sinusoids at 5, 10, 15 Hz in both time and frequency domain.

• The height of the spike here, indicates the amplitude (thus all sinusoids here have a peak amplitude of 1). • The relationship between the partials can be seen by the even spacing between the “spikes”.

Music 171: Additive Synthesis 4 Periodic

• A periodic corresponds to a harmonic spectrum, one where sinusoidal components are integer multiples of a . • Periodic waveforms, or harmonic sounds, may be thought of as those having a pitch. • “Standard” periodic waveforms: square, triangle and sawtooth, can be created using additive synthesis:

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Music 171: Additive Synthesis 5 Creating Standard Periodic Waveforms

• The following table gives the harmonic number, relative amplitude and phase of the harmonics for standard waveforms.

Table 1: Other Simple Waveforms Synthesized by Adding Sinusoids

Type Harmonics Amplitude Phase Phase (cosine) ()

square n = [1, 3, 5, ..., N] 1/n −π/2 0 (odd)

triangle n = [1, 3, 5, ..., N] 1/n2 0 π/2 (odd)

sawtooth n = [1, 2, 3, ..., N] 1/n −π/2 0 (even and odd)

• Notice that the phase differs depending on whether you use a sine or cosine function.

Music 171: Additive Synthesis 6 Spectra of Standard Waveforms

Square Spectrum 1

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Figure 4: Spectra of complex waveforms

Music 171: Additive Synthesis 7 Harmonics and Pitch

• Notice that even though these new waveforms contain more than one frequency component, they are still periodic. • Because the frequencis of components are integer multiples of some fundamental frequency, they are called harmonics. • Signals with harmonic spectra have a fundamental frequency and therefore have a periodic waveform (the reverse is, of course, also true). • Pitch is our subjective response to the fundamental frequency. • The relative of the harmonics contribute to the of a sound, but do not necessarily alter the pitch.

Music 171: Additive Synthesis 8 Clarinet Analysis

• A clarinet is generally considered to be closed-open. • Its tone (shown here in the steady state) can be viewed in both time and frequency domain.

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0.8 435 Hz 732 Hz 0.6 1171 Hz 0.4 1025 Hz magnitude 0.2

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Figure 5: Frequency analysis of a clarinet note.

• Summing sinusoids at 145, 433 and 732 Hz (as well as others), can approximate a synthesis of the clarinet (in the steady state).

Music 171: Additive Synthesis 9 Additive Synthesis

• Discrete signals (bandlimited by half the sampling rate) may be represented as the sum of N sinusoids of arbitrary amplitudes, phases, AND frequencies: N x(t)= X Ak cos(ωkt + φk) k=0 • We may therefore, synthesize a sound by setting up a bank of oscillators, each set to the appropriate amplitude, phase and frequency. • The output of each oscillator is added to produce a synthesized sound, and thus the synthesis technique is called additive synthesis.

Music 171: Additive Synthesis 10 Additive Synthesis Pros and Cons

Pros • Additive synthesis provides the maximum flexibility in the types of sound that can be synthesized. • In certain cases, it can realize tones that are “indistinguishable from real tones.” Cons • It is often necessary to do signal analysis before using additive synthesis to produce specific sounds. • Often requires many oscillators to produce good quality sounds—computationally demanding! • Attacks difficult. • Many functions are useful only for a limited range of pitch and loudness, e.g.: – the timbre of a played at A4 is different from one played at A2; – the timbre of a trumpet played loudly is quite different from one played softly at the same pitch.

Music 171: Additive Synthesis 11 Modeling Transient Attacks

• It is possible to use some knowledge of to determine functions: – e.g.: higher frequency harmonics are often the last to appear in the attack but the first to decay. – implement using a separate envelope on each harmonic with a steeper attack/decay for lower frequencies. • The duration of the attack and decay greatly influence the quality of a tone: – wind instruments tend to have long attacks, while – percussion instruments tend to have short attacks.

Music 171: Additive Synthesis 12 ADSR Envelope

• Recall the ADSR envelope (attack, decay, sustain, release) is an envelope that attempts to mimic the behaviour of sound produced by acoustic instruments.

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Figure 6: An ADSR envelope.

• Amplitude envelopes can occur on the overal sound or on individual sinusoidal components.

Music 171: Additive Synthesis 13 Sinusoid with an ADSR Envelope

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Figure 7: A sinusoid with an amplitude envelope.

Music 171: Additive Synthesis 14 Pitch and Frequency

• There is a nonlinear relationship between pitch perception and frequency. – e.g., the pitch interval of an octave corresponds to a frequency ratio of 2:1. – thus octaves in higher registers span more frequencies • We will often encounter a pitch notation wich designates a pitch with an octave: C4 is middle C. • The pitch A4 or “A440” is often used as a reference, and is an A at 440 Hz. • What is the frequency one octave below A440? • In equal-tempered tuning, there are 12 evenly spaced tones in an octave, called semi-tones: – The frequency n semitones above A440 is 440 × 2n/12 Hz. – The frequency n semitones below A440 is − 440 × 2 n/12 Hz.

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