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Perceptual Coherence : Hearing and Seeing

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338 <strong>Perceptual</strong> <strong>Coherence</strong><br />

of sound quality between different pitches <strong>and</strong> loudness that can be used to<br />

identify objects.<br />

String <strong>and</strong> Percussion Instruments: Vibrations in Strings<br />

<strong>and</strong> Plates<br />

Vibrations of Strings<br />

Suppose we pluck a string at the midway point. When we release the string<br />

there will be two traveling waves, one moving toward each end of the string.<br />

At the ends, each wave will be reflected back toward the middle of the string.<br />

If the reflections continue, the wave pattern along the string can become stationary.<br />

If we view the motion from the side, the individual points of the<br />

string oscillate up <strong>and</strong> down, but the wave profile does not move laterally.<br />

The original traveling waves have summed to produce a st<strong>and</strong>ing wave. The<br />

overall motion of the string is complex (although each point simply moves up<br />

<strong>and</strong> down in sinusoidal motion), because the motion is actually the sum of<br />

several simple harmonic motions. The simplest harmonic motion is the up<strong>and</strong>-down<br />

movement of the string as a whole. The second harmonic motion<br />

occurs when the string effectively splits into two parts, <strong>and</strong> each half undergoes<br />

an up-<strong>and</strong>-down motion out of phase with each other. The frequency of<br />

each of these vibrations is twice the frequency of the motion of the string as a<br />

whole. The motion of all of the higher harmonics can be understood in exactly<br />

the same fashion. The string breaks up into more <strong>and</strong> more subunits; the<br />

vibratory frequency of each subunit is the number of subunits times the frequency<br />

of the fundamental vibration (F 0 , 2F 0 , 3F 0 , 4F 0 , 5F 0 ...). 3<br />

The fundamental frequency of the string is determined by its physical<br />

construction <strong>and</strong> the amount of tension (equation 8.1). It is not determined<br />

by how the string is excited. However, the position <strong>and</strong> the manner of excitation<br />

do determine the relative amplitudes of the vibration modes. The<br />

maximum amplitude of a resonance mode occurs when the point of excitation<br />

occurs at an antinode (a point of maximum displacement), <strong>and</strong> the<br />

minimum amplitude occurs when the point of excitation occurs at a node<br />

(a stationary point). Thus, if the string is excited at the center point, the<br />

first up-<strong>and</strong>-down resonance will be maximized because that is the point<br />

of maximum movement, but the second resonance will be minimized because<br />

that is the point of zero movement separating the vibration of the<br />

two halves of the string. In general, the overall amplitude of the vibration<br />

3. By convention, F 0 is termed the fundamental, 2F 0 the second harmonic (F 0 being the<br />

first harmonic), 3F 0 the third harmonic, <strong>and</strong> so on. If the vibration modes are not related by integers<br />

(e.g., the vibration modes found for 2-dimensional wooden violin plates), the vibration<br />

modes are termed partials.

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