Building Acoustics
ARE 547
Dpt of Architectural Engineering
College of Environmental Design
KFUPM
Lecture 1
Djamel Ouis
2nd semester 2015
ARE_547_1
Acoustics
The science concerned with the
production, control, transmission,
reception, and effects of sound.
The science of sound and
vibrations.
Acoustics and its involvements:
Lindsay’s ”Wheel of Acoustics”
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Acoustics: Sound and Vibrations
• Physical Acoustics: Wave propagation and vibrations
• Room Acoustics: sound within closed spaces
• Building Acoustics: Transmission of sound in
constructions
• Environmental Acoustics: road, train and air traffic,
industry
• Electroacoustics: Loudspeakers and Microphones
• Underwater Acoustics: Sonars and submarines
• Psychoacoustics: Hearing perception
• Speech and hearing
• Non-linear Acoustics: loud explosions
• Medical and chemical: ultrasounics
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Acoustics
The oldest branch of “Natural Philosophy”?
In the 6th Century BC, the ancient
Greek philosopher Pythagoras wanted
to know why some combinations of
musical sounds seemed more beautiful
than others, and he found answers in
terms of numerical ratios representing
the harmonic overtone series on a string.
He is reputed to have observed that
when the lengths of vibrating strings
are expressible as ratios of integers (e.g. 2 to 3, 3 to 4), the
tones produced will be harmonious, and the smaller the
integers the more harmonious the sounds.
Acoustics
Vitruvius (80/70-15 BC), Roman architect: father of
architectural acoustics, used bronze vessels to control
reverberation (echeia). He made accurate description
of their placement, number, and tuning; desirable for
music but not always for speech.
Gallilei (1564-1642) and French mathematician Marin Mersenne
(1588-1648) studied the vibration of stretched strings, and found
the complete laws of their vibrations.
Colladon and Sturm measured in 1826,
Lake Geneva, the speed of sound in water:
1437 m/s (today’s: 1481 m/s, 3% error)
Acoustics; some great names
H. von Helmholtz
(1821-94)
On the Sensations
of Tone (1863)
Lord Rayleigh
(1842-1919)
The Theory of
Sound (1877)
Collected Papers
on Acoustics (1923)
J. W. Sabine
(1868-1919)
Basics of Sound
 Sound is the result of propagation of a perturbation in a
medium: No sound in a vacuum.
 A sound wave is a longitudinal wave: the particle motion
is in the direction of propagation of the wave (cf EM wave)
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A transversal wave, here a seismic wave
(Rayleigh surface wave): The particles at the
surface move along an elliptical pathway.
Spherical wave
The energy is evenly distributed over the area
of a sphere centered at the sound source.
The particles on the sphere move in phase.
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The wave equation
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P: any of the quantities pressure, velocity or particle displacement.
c: the speed of wave propagation (sound: ρ0v2 = γP0 ; v = 344,2 m/s)
In one dimension: plane
waves, P(x,t).
A standing wave
Example of a sound wave in a
closed tube
Superposition of 2 waves
traveling in opposite directions
Red wave: moving right,
Green wave: moving left
Blue wave: sum of the two;
a standing wave
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Period, frequency and wavelength
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A (harmonic) wave (often) has a double periodicity:
in space (wavelength: l), and in time (period: T)
f
v
Tv l
vair= 340 m/s
vwater= 1400 m/s
vsteel= 5400 m/s
Wave propagation phenomena:
Reflection
Reflection law: The angle of
reflection is equal to the angle
of incidence: θi= θr
String held fixed at one
end: Reflection with
phase shift (180o).
Hard boundary
String with free end:
Reflection with no
phase shift.
Soft boundary
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Wave propagation phenomena:
Refraction
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Change of the direction of
propagation due to a change in
the wave propagation speed.
e.g. wind gradient or
temperature gradient
Medium with lower speed => shorter
wavelength
f
v
l
Wave propagation phenomena:
Diffraction
 Diffraction occurs whenever a wave encounters
an obstacle: The wavefront is influenced.
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From a plane wave to a
spherical wave.
The wavefronts get less deformed for
a wider gap.
Diffraction
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Barrier height: λ Barrier height: 2 λ Barrier height: 4 λ
Diffraction is a low frequency phenomenon:
Wave proceeds indisturbed for obstacles of the size << λ.
We can hear, but not see around a corner!
Interference: here with two sources. Both
interference and diffraction are involved.
Principle of superposition:
The effect of a sum of causes is equal to
the sum of the effects of each cause.
Wave superposition
Beats, amplitude modulation, AM
 Superposition of two harmonic signals with nearby
frequencies. Adjusting musical instruments (piano &
pitch fork)
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The Doppler Effect
The moving sound source
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Stationary sound source Moving sound source
Change of frequency (pitch):

Sound waves and Different Wave Phenomena

  • 1.
    Building Acoustics ARE 547 Dptof Architectural Engineering College of Environmental Design KFUPM Lecture 1 Djamel Ouis 2nd semester 2015 ARE_547_1
  • 2.
    Acoustics The science concernedwith the production, control, transmission, reception, and effects of sound. The science of sound and vibrations.
  • 3.
    Acoustics and itsinvolvements: Lindsay’s ”Wheel of Acoustics” ARE_547_1:1
  • 4.
    Acoustics: Sound andVibrations • Physical Acoustics: Wave propagation and vibrations • Room Acoustics: sound within closed spaces • Building Acoustics: Transmission of sound in constructions • Environmental Acoustics: road, train and air traffic, industry • Electroacoustics: Loudspeakers and Microphones • Underwater Acoustics: Sonars and submarines • Psychoacoustics: Hearing perception • Speech and hearing • Non-linear Acoustics: loud explosions • Medical and chemical: ultrasounics ARE_547_1:2
  • 5.
    Acoustics The oldest branchof “Natural Philosophy”? In the 6th Century BC, the ancient Greek philosopher Pythagoras wanted to know why some combinations of musical sounds seemed more beautiful than others, and he found answers in terms of numerical ratios representing the harmonic overtone series on a string. He is reputed to have observed that when the lengths of vibrating strings are expressible as ratios of integers (e.g. 2 to 3, 3 to 4), the tones produced will be harmonious, and the smaller the integers the more harmonious the sounds.
  • 6.
    Acoustics Vitruvius (80/70-15 BC),Roman architect: father of architectural acoustics, used bronze vessels to control reverberation (echeia). He made accurate description of their placement, number, and tuning; desirable for music but not always for speech. Gallilei (1564-1642) and French mathematician Marin Mersenne (1588-1648) studied the vibration of stretched strings, and found the complete laws of their vibrations. Colladon and Sturm measured in 1826, Lake Geneva, the speed of sound in water: 1437 m/s (today’s: 1481 m/s, 3% error)
  • 7.
    Acoustics; some greatnames H. von Helmholtz (1821-94) On the Sensations of Tone (1863) Lord Rayleigh (1842-1919) The Theory of Sound (1877) Collected Papers on Acoustics (1923) J. W. Sabine (1868-1919)
  • 8.
    Basics of Sound Sound is the result of propagation of a perturbation in a medium: No sound in a vacuum.  A sound wave is a longitudinal wave: the particle motion is in the direction of propagation of the wave (cf EM wave) ARE_547_1:3 A transversal wave, here a seismic wave (Rayleigh surface wave): The particles at the surface move along an elliptical pathway.
  • 9.
    Spherical wave The energyis evenly distributed over the area of a sphere centered at the sound source. The particles on the sphere move in phase. ARE_547_1:4
  • 10.
    The wave equation ARE_547_1:5 P:any of the quantities pressure, velocity or particle displacement. c: the speed of wave propagation (sound: ρ0v2 = γP0 ; v = 344,2 m/s) In one dimension: plane waves, P(x,t).
  • 11.
    A standing wave Exampleof a sound wave in a closed tube Superposition of 2 waves traveling in opposite directions Red wave: moving right, Green wave: moving left Blue wave: sum of the two; a standing wave ARE_547_1:6
  • 12.
    Period, frequency andwavelength ARE_547_1:7 A (harmonic) wave (often) has a double periodicity: in space (wavelength: l), and in time (period: T) f v Tv l vair= 340 m/s vwater= 1400 m/s vsteel= 5400 m/s
  • 13.
    Wave propagation phenomena: Reflection Reflectionlaw: The angle of reflection is equal to the angle of incidence: θi= θr String held fixed at one end: Reflection with phase shift (180o). Hard boundary String with free end: Reflection with no phase shift. Soft boundary ARE_547_1:8
  • 14.
    Wave propagation phenomena: Refraction ARE_547_1:9 Changeof the direction of propagation due to a change in the wave propagation speed. e.g. wind gradient or temperature gradient Medium with lower speed => shorter wavelength f v l
  • 15.
    Wave propagation phenomena: Diffraction Diffraction occurs whenever a wave encounters an obstacle: The wavefront is influenced. ARE_547_1:10 From a plane wave to a spherical wave. The wavefronts get less deformed for a wider gap.
  • 16.
    Diffraction ARE_547_1:11 Barrier height: λBarrier height: 2 λ Barrier height: 4 λ Diffraction is a low frequency phenomenon: Wave proceeds indisturbed for obstacles of the size << λ. We can hear, but not see around a corner! Interference: here with two sources. Both interference and diffraction are involved. Principle of superposition: The effect of a sum of causes is equal to the sum of the effects of each cause.
  • 17.
    Wave superposition Beats, amplitudemodulation, AM  Superposition of two harmonic signals with nearby frequencies. Adjusting musical instruments (piano & pitch fork) ARE_547_1:12
  • 18.
    The Doppler Effect Themoving sound source ARE_547_1:13 Stationary sound source Moving sound source Change of frequency (pitch):