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Draft:Chord phenomenon

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Introduction

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The chord phenomenon refers to the occurrence of multiple harmonically related frequency components sounding simultaneously, forming what is perceived as a musical chord. In music, a chord is typically defined as a combination of three or more notes played together, often forming a harmonic structure that is pleasing to the ear. This phenomenon is not only a cornerstone of musical composition but also a subject of interest in the field of Signal processing..[1].

When analyzed in the frequency domain, musical chords reveal a distinctive spectral pattern. Besides the fundamental frequency f₀, the signal often contains multiple harmonics at 2f₀, 3f₀, 4f₀, ..., which correspond to overtones naturally produced by musical instruments or synthesized sounds. These harmonic relationships give chords their characteristic timbre and resonance[2].

As shown in typical spectrograms, strong peaks appear at the fundamental and its harmonics, demonstrating the periodic and structured nature of chordal sounds. Understanding the chord phenomenon is essential for music theory, acoustics, and modern applications like audio signal processing, music information retrieval, and sound synthesis.

Theoretical Basis

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The chord phenomenon can be explained through the principle of resonance (共振) in acoustics. When a musical instrument is played, it creates standing waves within a resonant medium—like a string or air column. These standing waves occur only at specific resonant frequencies governed by the boundary conditions[3].

For a string of length L, the resonant wavelengths and frequencies are:

where:

  • v is the speed of sound in the medium (e.g., ~340 m/s),
  • f₁ is the fundamental frequency f₀,
  • f₂ = 2f₀, f₃ = 3f₀, ... are the harmonics[4].

Harmonic Series and Chords

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This harmonic series, resulting from simultaneous resonance modes, leads to the presence of frequencies at f₀, 2f₀, 3f₀, ... — which are heard together as a chord. Even a single musical note can contain multiple harmonics due to its mode structure[5].

Periodic but Not Sinusoidal

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Although sound signals are periodic, they are not pure sinusoids. Instead, they are sums of harmonics, leading to rich timbres and the formation of complex chords. This explains the chord phenomenon from a signal perspective[6].

Practical Examples

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Musical Instrument Sounds

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When a piano key is pressed or a guitar string is plucked, it produces not just a single tone but a rich set of harmonics. For example, middle C (approximately 261.63 Hz) on a piano also generates frequencies at 523.26 Hz, 784.89 Hz, and higher, forming a natural chordal structure[7].

Major and minor chords involve combinations of notes whose overtones align. This harmonic alignment gives rise to the sense of consonance or dissonance depending on the frequency relationships[8].

Audio Signal Analysis

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Spectrograms generated using the Short-time Fourier transform (STFT) show harmonics stacked above the fundamental frequency. These harmonic stacks directly reflect the chord phenomenon in the frequency domain[9]..

Music Recognition Apps

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Applications like Shazam analyze time-frequency patterns of sound. Chords produce strong harmonic peaks which help identify musical segments even in noisy environments[10].

Notable Phenomena

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Even when the fundamental frequency is absent, listeners perceive it based on the spacing of the harmonics. This auditory illusion is known as the missing fundamental phenomenon and highlights how the brain interprets harmonic patterns[11].

Inharmonicity

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In some instruments, such as pianos or bells, the overtones are not exact integer multiples of the fundamental. This inharmonicity introduces richness or dissonance into the sound and is a key factor in instrument timbre[12]

Auditory Illusions

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Complex chords can give rise to auditory illusions such as phantom tones, comb filtering, or beating effects. These phenomena are often exploited in electronic and experimental music[13]

  1. ^ Smith, J.O. (2010). Introduction to Digital Filters: With Audio Applications.
  2. ^ Juan Gualterio Roederer (2008). The Physics and Psychophysics of Music: An Introduction. Springer.
  3. ^ Rossing, T.D., Moore, F.R., & Wheeler, P.A. (2002). The Science of Sound. Addison Wesley.
  4. ^ Hall, D.E. (2002). Musical Acoustics. Brooks/Cole.
  5. ^ Arthur H. Benade (1990). Fundamentals of Musical Acoustics. Dover Publications.
  6. ^ McClellan, J.H., Schafer, R.W., & Yoder, M.A. (2003). DSP First: A Multimedia Approach. Prentice Hall.
  7. ^ Campbell, M., Greated, C., & Myers, A. (2004). Musical Instruments: History, Technology, and Performance of Instruments of Western Music. Oxford University Press.
  8. ^ Helmholtz, H.L.F. (1954). On the Sensations of Tone. Dover Publications.
  9. ^ Rabiner, L., & Schafer, R.W. (1978). Digital Processing of Speech Signals. Prentice-Hall.
  10. ^ Wang, A. (2003). An industrial-strength audio search algorithm. In Proceedings of the 4th International Conference on Music Information Retrieval (ISMIR).
  11. ^ Plomp, R. (1967). Pitch of complex tones. Journal of the Acoustical Society of America, 41(6), 1526–1533.
  12. ^ Fletcher, N.H., & Rossing, T.D. (1998). The Physics of Musical Instruments. Springer.
  13. ^ Deutsch, D. (2013). The Psychology of Music (3rd ed.). Academic Press.