Upload
esmaealzadehha
View
214
Download
0
Embed Size (px)
Citation preview
7/29/2019 82168772 Acoustics Presentation JuL
1/47
7/29/2019 82168772 Acoustics Presentation JuL
2/47
ACOUSTICS
For I know the plans I have
for, plan to prosper you andnot to harm you, plan to give
you hope and a future.
Jer. 29:11
7/29/2019 82168772 Acoustics Presentation JuL
3/47
Acoustics
The science of sound, including itsproduction, propagation and effects
The objective study of the physical behavior
of sound in an enclosed space
Sound
A wave motion consisting of a series of
condensations and rarefactions in an elastic
medium produced by a vibrating body
7/29/2019 82168772 Acoustics Presentation JuL
4/47
7/29/2019 82168772 Acoustics Presentation JuL
5/47
7/29/2019 82168772 Acoustics Presentation JuL
6/47
Audible Range: 20 20 000Hz
Infrasonic
frequencies below the audible range
Ultrasonic
frequencies above the audible range
7/29/2019 82168772 Acoustics Presentation JuL
7/47
Human Voice
60 7000 Hz
85 155 Hz ( Adult Male )
165 225 Hz ( Adult Female )
Generation:
1. Lungs
2. Vocal folds within the larynx3. Articulators ( tongue, cheek, palate, lips, etc. )
7/29/2019 82168772 Acoustics Presentation JuL
8/47
General Interpretation of Sound
1. Physical phenomenon consisting of wave
motion in a transmitting medium
(objective)
2. Sensation due to outside simulation
(subjective)
7/29/2019 82168772 Acoustics Presentation JuL
9/47
Requirements to Produce Sounds
1. Presence of vibrating body
2. Presence of transmitting medium
7/29/2019 82168772 Acoustics Presentation JuL
10/47
Physical Properties of Sound
1. Amplitude
2. Period
3. Frequency4. Wavelength
5. Velocity of Propagation
7/29/2019 82168772 Acoustics Presentation JuL
11/47
Velocity of Sounds
A. Solids
Where:E = Youngs Modulus ofelasticity ( N/m2 )
d = density of the medium, ( kg/m3 )
7/29/2019 82168772 Acoustics Presentation JuL
12/47
Velocity of Sounds
B. Liquids
Where:e = Bulks Modulus ofelasticity ( N/m2 )
d= density of the medium ( kg/m3 )
7/29/2019 82168772 Acoustics Presentation JuL
13/47
Velocity of Sounds
C. Gases
Where:
k = ratio of the specific heat at constant volumePo = the steady pressure of the gas (N/m
2 )
o = the steady or average density of the gas ( kg/m3 )
7/29/2019 82168772 Acoustics Presentation JuL
14/47
Velocity of Sounds
D. Dry Air/Air (for TC 200C)
where:TC = temperature in Celsius
7/29/2019 82168772 Acoustics Presentation JuL
15/47
Velocity of Sounds
D. Dry Air/Air (for TC 200C)
where:
TK = temperature in Kelvin
7/29/2019 82168772 Acoustics Presentation JuL
16/47
Velocity of Sounds
Notes
- Sounds travel more slowly in gasesthan in
liquids, and more slowly in liquids than solids.
- Sounds travels slower with an increased
altitude (elevation if you are on solid earth),
primarily as a result and humidity changes.
7/29/2019 82168772 Acoustics Presentation JuL
17/47
Mach Number
Mach Number
- The speed of an object in air, or any fluid
substance, divided by the speed of sound as
it is in that substance.
7/29/2019 82168772 Acoustics Presentation JuL
18/47
Mach Number
Six Categories
Subsonic: M
7/29/2019 82168772 Acoustics Presentation JuL
19/47
Supersonic Transport (SST)
Concorde
7/29/2019 82168772 Acoustics Presentation JuL
20/47
Supersonic Transport (SST)
Tupolev Tu-144
7/29/2019 82168772 Acoustics Presentation JuL
21/47
Sonic Boom
Sonic Boom
This term is commonly used to refer to
the shocks caused by the supersonic flight of
an aircraft.It generates enormous amount of
sound energy, sounding much like an
explosion.
7/29/2019 82168772 Acoustics Presentation JuL
22/47
7/29/2019 82168772 Acoustics Presentation JuL
23/47
Sonic Boom CLoud
7/29/2019 82168772 Acoustics Presentation JuL
24/47
Possibilities when a Propagated
Sound is Obstructed
Sound is Reflected
Becomes apparent to the listener only when the distancefrom the source and the reflecting medium is great and the
difference between the original and reflected sound is greateror equal to 1/17 of a second.
Brought about by a series of rarefactions between twoparallel surfaces resulting to prolongation of sound
Creates listener fatigue
Reflection caused by two parallel surfaces, producingstanding waves
7/29/2019 82168772 Acoustics Presentation JuL
25/47
Possibilities when a Propagated
Sound is Obstructed
Sound is absorbed
Conversion of sound energy to heat energy
Onward transmission through
obstruction
7/29/2019 82168772 Acoustics Presentation JuL
26/47
Physiological Characteristics of
Wave Motion
1) Pitch
2) Tone
3) Loudness
7/29/2019 82168772 Acoustics Presentation JuL
27/47
Physiological Characteristics of
Wave Motion
Pitch
Number of cycles a wave goes through in a
definite interval
The higher the frequency the higher the pitch
Mel unit of pitch
1000 mels pitch of 1000Hz tone at 40dB
Octave pitch interval 2:1; frequency is twice thegiven tone
7/29/2019 82168772 Acoustics Presentation JuL
28/47
Physiological Characteristics of
Wave Motion
Tone
Timbre quality of sound
- The quality of sound related to harmonic structure
- tone quality or tone color
Pure Tone a sound composed of only one
frequency in which the sound pressure varies
sinusoidally with time.
Musical Sounds composed of the fundamental
frequency and its harmonics
7/29/2019 82168772 Acoustics Presentation JuL
29/47
Physiological Characteristics of
Wave Motion
Loudness
Fluctuation of air pressure created by sound waves
Observers auditory impression of the strength of a
sound and is associated with the rate at which energyis transmitted to the ear.
Depends on the amplitude of the sound
Sone unit of loudness
Loudness Level measured by the sound level of astandard pure tone or specified frequency which is
assessed by normal observers as being equally loud
7/29/2019 82168772 Acoustics Presentation JuL
30/47
PHON
Phon is the unit of loudness level when:
The standard pure tone is produced by asensibly plane sinusoidal progressive
sound wave coming from directly in frontof the observer and having the frequencyof 1kHz
The sound pressure level in the freeprogressive wave is expressed in dBabove 2 x 10-5 N/m2
7/29/2019 82168772 Acoustics Presentation JuL
31/47
Sound Levels
A. Sound Pressure (P) and
Sound Pressure Level (SPL)
Sound Pressure
The local pressure deviation from the ambient
(average, or equilibrium) pressure caused by a
soundwave.
The alternating component of the pressure at a
particular point in a sound field
Expressed in N/m2 or Pa
7/29/2019 82168772 Acoustics Presentation JuL
32/47
Sound Levels
Sound Pressure Level Equal to 20 times the logarithm to the base 10 of the
ratio of the RMS sound pressure to the reference
sound pressure
SPL = 20 log (P/Po)Where:
P = rms sound pressurePo = reference sound pressure
Po = 2 x 10-5 N/m2 or Pa
Po = 0.0002 bar
Po = 2.089 lb/ft2
7/29/2019 82168772 Acoustics Presentation JuL
33/47
Sound Pressure Levels
Sound Pressure Level (SPL) at any unit ofpressure in dB
SPL = 20log(P+N)
Where:
PN = rms sound pressure expressed in any of
pressure in dBN = SPL constant corresponding to the unit atwhich sound pressure is expressed
7/29/2019 82168772 Acoustics Presentation JuL
34/47
SPL Constants
Unit of Sound Pressure DesignationSPL Constant
(N)
Microbar bar 74
Pascal N/m2 94
lb/ft2 psf 127.6
mmHg mmHg 136.5
torr torr 136.5lb/in2 psi 170.8
atm (technical) atm 193.8
atm (standard) atm 194.1
7/29/2019 82168772 Acoustics Presentation JuL
35/47
Sound Levels
B. Sound Intensity (I) and
Sound Intensity Level (SIL)
Sound Intensity
Defined as the power per unit area
The basic units are W/m2
The average rate of transmission of sound energy
through a cross-sectional area of 1 m2
at rightangles to a particular motion.
7/29/2019 82168772 Acoustics Presentation JuL
36/47
Sound Levels
Inverse Square Law
The sound intensity from a point source of
sound will obey the inverse square law if there
are no reflections or reverberation.Any physical law stating that a specified
physical quantity or strength is inversely
proportional to the square of the distance from
the source of that physical quantity.
7/29/2019 82168772 Acoustics Presentation JuL
37/47
7/29/2019 82168772 Acoustics Presentation JuL
38/47
Sound Levels
Ground Source:
7/29/2019 82168772 Acoustics Presentation JuL
39/47
Sound Levels
Isotropic Source:
7/29/2019 82168772 Acoustics Presentation JuL
40/47
Sound Levels
Sound Intensity Level
Where:
I = sound intensityIo = threshold intensity, W/m2
Io = 10-12 W/m2 = 10-16 W/cm2
7/29/2019 82168772 Acoustics Presentation JuL
41/47
Sound Levels
C. Sound Power (W) and
Sound Power Level (PWL)
Sound Power (W)
The total energy radiated per unit time.
7/29/2019 82168772 Acoustics Presentation JuL
42/47
Sound Levels
Sound Power Level (PWL)
Where:
W = sound power , W
Wo = reference sound power
Wo = 10-12 W = 10-16 W
7/29/2019 82168772 Acoustics Presentation JuL
43/47
Volume Unit
7/29/2019 82168772 Acoustics Presentation JuL
44/47
Volume Unit Meter
7/29/2019 82168772 Acoustics Presentation JuL
45/47
Sound Fields
Free fieldA region in space where sound maypropagate free from any form of obstruction.
Near fieldA region close to a source where
the sound pressure and acoustic particlevelocity are not in phase.
Far fieldIt begins where the near field endsand extends to infinity.
7/29/2019 82168772 Acoustics Presentation JuL
46/47
Sound Fields
Direct fieldIt is the part of the sound field
which has not suffered any reflection from
any room surfaces or obstacles.
Reverberant fieldIt is the part of the soundfield which has experienced at least onereflection from a boundary of the room orenclosure containing the source.
7/29/2019 82168772 Acoustics Presentation JuL
47/47
End
Thank you!!