→ More efficient than additive synthesis, but offers less spectral control
Simplified schematic of voltage controlled subtractive synthesis.
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Efficiency of FM synthesis
Uses two oscillators (carrier + modulator)
Generates rich, controllable spectra through frequency modulation
Simple algorithm creates both harmonic and inharmonic sounds
→ Achieves rich timbral control with minimal parameters
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IV. FM Theory
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Origins of frequency modulation
Mainly developed by radio broadcasting engineer Edwin Armstrong (1890 - 1954) for transmitting high-fidelity sound over broadcast radio (since the late 1930)
FM Radio - demodulation
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Simple frequency modulation (FM)
In FM synthesis, the instantaneous frequency of a carrier oscillator (C) is varied according to the output of a modulator oscillator (M).
Carrier frequency (C) - Sets the perceived pitch
Modulator frequency (M) - Determines harmonic/inharmonic character
If the carrier is detuned, the entire harmonic spectrum shifts up or down by that same amount.
Detuning the modulator compresses or expands the separation between the sidebands
From left to right: increasing modulator frequency results in wider spacing
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FM synthesis formula
Basic formula:
Parameters:
- Carrier amplitude
(or ) - Carrier frequency (perceived pitch)
(or ) - Modulator frequency (sideband spacing)
- Modulation depth (frequency deviation or amount of modulation)
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Derived FM parameters
Harmonicity ratio:
Determines harmonic (integer) or inharmonic (non-integer) spectrum
Modulation index:
Controls the number of significant frequency components (sidebands)
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Sidebands (spectral components)
New frequency components appear in pairs symmetrically around the carrier frequency and define the timbre of the sound:
is an integer that determines the order of the sidebands
carrier
modulator
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Calculating the sidebands
Each sideband pair has the same amplitude.
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Reflected sidebands and interference
Lower sidebands extending below 0 Hz reflect at zero with a 180° phase shift, potentially interfering with positive-frequency components.
Coincident series (e.g., 1:1, 2:3 ratio):
Reflected sidebands land on existing positive frequencies
→ regular harmonic spacing with interference
Non-coincident series (e.g., 3:5 ratio):
Reflected sidebands fall between positive frequencies
→ irregular spacing, no interference
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Coincident vs. non-coincident series
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Control over a sound's "brightness"
Modulation index
Number of significant (perceivable) frequency components increases with :
→ Increasing the modulation index creates more sidebands with greater amplitudes, redistributing energy across the spectrum and increasing spectral richness.
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Harmonicity ratio and spectral character
The ratio between M and C determines the harmonicity of the resulting spectrum.
Harmonicity ratio: (modulator ÷ carrier)
→ If is rational (), the spectrum contains only harmonic frequencies
→ If is irrational, the spectrum is inharmonic
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Listening examples: FM spectra
Simple (C=260, H=1.0, I=0.5)
Rich harmonic (C=260, H=1.0, I=5.0)
Complex rational (C=260, H=1.3, I=6.0)
Odd harmonics (C=260, H=2.0, I=3.0)
2:3 ratio (C=260, H=1.5, I=3.0)
Inharmonic √2 (C=260, H=1.414, I=3.0)
Sub-harmonic (C=650, H=0.25, I=2.1)
Irrational π (C=100, H=3.14159, I=4.0)
Extreme (C=100, H=1.3, I=9.0)
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Calculating sideband amplitudes
Sideband amplitudes are determined by mathematical scaling factors known as Bessel functions of the first kind:
The amplitude of the -th sideband is calculated as , where is the sideband order and is the modulation index.
Total average power of the signal remains constant, only the spectral distribution of that energy changes.
→ Bessel functions act as a mathematical "lookup table"
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Dynamic timbres
Coupling an envelope to both the carrier amplitude and modulator level creates realistic, brass-like dynamic changes in both loudness and brightness
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Multiple modulators
Parallel modulators (M1→C, M2→C):
Sideband series add together
C ± k·M₁ and C ± k·M₂
Cascaded modulators (M1→M2→C):
Each sideband from M1→M2 acts as a sine wave modulator for the carrier
Result: sidebands of sidebands (exponential spectral growth)
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Feedback in FM
Feedback routes an operator's output back to its own input:
Generates spectral complexity without additional oscillators
Creates additional sideband frequencies beyond standard FM pairs
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Phase modulation (PM)
PM is the derivative of FM. It varies the phase angle rather than frequency, but produces identical sidebands to FM.
Digital FM synthesis uses PM because:
More stable with feedback loops
Easier to implement digitally
Same audible result as true FM
→ All digital FM synthesizers (DX7, etc.) actually use PM
Demonstrates FM's ability to create complex, organic timbres
→ Established FM as legitimate compositional tool
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VII. Artistic Research
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FM Synthesis and artistic research
Discovery emerged from compositional practice (sound spatialization)
Required teaching himself advanced mathematics, programming, and signal processing
Six years of systematic research to make it musically controllable
Continuous artistic application used in his own compositions and widely adopted by other artists
A major patent licensing success for Stanford with significant impact on the music industry
→ Artistic inquiry and scientific understanding enabled genuine innovation
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Appendix
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Determining the fundamental frequency
For rational harmonicity ratios (in lowest terms), the fundamental frequency can be calculated:
Example:, Hz
Fundamental Hz
→ All sideband frequencies are integer multiples of 26 Hz.
Literature
Chowning, John. "Turenas: the realization of a dream." Journées d'Informatique Musicale. Université de Saint-Etienne, 2011.
Chowning, John. "The Synthesis of Complex Audio Spectra by Means of Frequency Modulation." Computer Music Journal. Vol. 1, No. 2 (April, 1977), pp. 46-54.
Chowning, John. "Fifty Years of Computer Music: Ideas of the Past Speak to the Future." Lecture Notes in Computer Science, pp. 1–10, https://doi.org/10.1007/978-3-540-85035-9_1.
Source: Mathews, M. V. "The digital computer as a musical instrument."
Science, vol. 142, no. 3592, Nov. 1963, pp. 553–557.
https://doi.org/10.1126/science.142.3592.553
Audio: Daisy Bell, IBM 7094 (1961)
Public domain
Stanley Kubrick (1928 – 1999), American film director, screenwriter, producer, and photographer
Image: John Chowning at the Vox Festival
Photo: Histeria
Source: Sound on Sound
https://www.soundonsound.com/people/john-chowning
Fair use for educational purposes
METHOD AND APPARATUS FOR SIMULATING LOCATION AND MOVEMENT OF
SOUND, US Pat. 3665105 - Filed Mar 9, 1970 Patented May 23, 1972
no applications (surround sound came later)
**Notable figures:** John Chowning, Julius Smith, Chris Chafe, Jonathan Berger