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MECHANICAL WAVES AND SOUND
CHAPTER 12 MECHANICAL WAVES AND SOUND
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Goals for Chapter 12 To describe mechanical waves.
To study superposition, standing waves and sound. To present sound as a standing longitudinal wave. To study sound intensity and beats. To examine applications of acoustics and musical tones.
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A disturbance that propagates from one place to another is referred to as a wave.
Mechanical waves propagate with well-defined speeds determined by the properties of the material (medium) through which they travel. Waves carry energy, not matter.
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In a transverse wave individual particles move at right angles to the direction of wave propagation.
In a longitudinal wave individual particles move in the same direction as the wave propagation.
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A wave on a string
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As a wave on a string moves horizontally, all points on the string vibrate in the vertical direction.
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Water waves from a disturbance.
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Wavelength, Frequency, and Speed
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Speed of a wave vwave = λ /T λ f = vwave
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REFLECTIONS AND SUPERPOSITION
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A reflected wave pulse: fixed end
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A reflected wave pulse: free end
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The Principle of supperposition:
Whenever two waves overlap, the actual displacement of any point on the string, at any time, is obtained by vector addition of the following two displacements: The displacement the point would have if ONLY the first wave were present 2) The displacement the point would have if ONLY the second wave were present
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Constructive Interference
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Destructive Interference
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Figure 14-22 Interference with Two Sources
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Waves become coherent Depending on the shape and size of the medium transmitting the wave, different standing wave patterns are established as a function of energy.
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Normal modes for a linear resonator
The resonator is fixed at both ends. Wave energy increases as you go down the y axis below.
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Fundamental frequencies
The fundamental frequency depends on the properties of the resonant medium. If the resonator is a string, cord, or wire, the standing wave pattern is a function of tension, linear mass density, and length.
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