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:: Physics of Sound ::
 
   
 

Sound Intensities

Permissible Noise Exposures

Perception of Changes in Sound

Combining SPL/SIL Calculations

Acoustics

Psychoacoustics / Psychology of music

Absolute, Perfect, and Relative Pitch

Instrument Ranges

 

 

 

Sound Intensities

Decibles Degree Loudness of Feeling
 
225
194
140
130
 
 
 
120
 
110
Deafening
 
 
 
 
 
 
 
 
 
 
 
12" cannon @ 12 ft, in front & below
Saturn rockt, 50# of TNT @ 10'
Artillery fire, jet aircraft, ram jet
Threshold of pain
>130 causes immediate ear damage
Porpeller aircraft at 5 meters
Hydraulic press, pneumatic rock drill
Thunder, diesel engine room
Nearby riviter
Close to a train, ball mill
 
100
 
 
 
90
 
Very Loud
 
 
 
 
 
 
 
Boiler factory, home lawn mower
Car horn at 5 meters, wood saw
Symphony or a band
>90 regularly can cause ear damage
Noisy factory
Truck without muffler
 
80
 
70
 
 
Loud
 
 
 
 
 
 
Inside a high speed auto
Police whistle, electric shaver
Noisy office, alarm clock
Average radio
Normal street noise
 
60
50
45
Moderate
 
 
 
 
Normal conversation, close up
Normal office noise, quiet stream
To awaken a sleeping person
 
40
 
30
Faint
 
 
 
 
Normal private office noise
Residential neighborhood, no cars
Quiet conversation, recording studio
 
20
 
 
 
10
 
 0
Very Faint
 
 
 
 
 
 
 
 
Inside an empty theater
Ticking of a watch
Rustle of leaves
Whisper
Sound proof room
 Threshold of hearing
Absolute silence

Sound intensities are typically measured in decibels (db). A decibel is defined as 10 times the logarithm of the power ratio
(power ratio is the ratio of the intensity of the sound to the intensity of an arbitrary standard point.) Normally a change of 1
db is the smallest volume change detectable by the human ear.
Sound intensity is also defined in terms of energy (erg) transmitted per second over a 1 square centimeter surface.
This energy is proportional to the velocity of propagation of the sound. The energy density in erg/cm³ = 2pi² x density in g/cm³ x frequency² in Hz x amplitutde² in cm.

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Permissible Noise Exposures

Hours Duration
per Day

Sound Level in
Decibels (Slow Response)

8
6.
4
3
2
1.5
1
.5
.25
90
92
95
97
100
102
105
110
115

The above restrictions are based on the Occupational Safety and Health Act of 1970.
That Code basically states that if the above exposures are exceeded, then hearing
protection must be worn. Note that these are based on the "A scale" of a standard
sound level meter at slow response and will change if some other standard is used.
See the OSHA Section 1910.95 for additional details on the differences.


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Perception of Changes in Sound

Sound Level Change
in Decibels

Perception

3
5
10
Barely perceptible
Clearly perceptible
Twice as loud

Note that the sound level scale in decibels is a logarthmic rather than linear scale. A sound level change of 3 decibels is double (or half) of the previous power level. The ear registers this as just noticable. A change in power level of 10 decibels is a power change of 10 times, and the ear judges this as only twice (or half) as loud.
These relationships do not hold true at all power levels or at the frequencies, as the ear is a very non-linear device. See Fletcher-Munson hearing curves published in books on hearing.
Some human ears can hear sounds in the frequency range of 20Hz to 20,000Hz, however, the hearing for most people is limited to about 30Hz to 15,000Hz.

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Combining SPL/SIL Calculations

From SPL to dB
From SIL to dB
From dB to SPL
From dB to SIL
Combining SIL
Combining SPL

           
  Sound Pressure Level (SPL)        
         
  From SPL to dB:        
  If P=0.23        
 
  Divide P by P0:        
  P/P0 = 0.2/2x 10-5 = 11500        
           
  Take Log:        
  Log(11500) = 4.0607        
           
  Multiply by 20 to get Lp:        
  Lp=20 x 4 = 81.2dB        
         
  From dB to SPL:        
 
Lp = 20Log
(
___P___
)  
 
P0
 
           
  if dB = 42        
           
 
42dB = 20Log
( ___P___ )  
 
2x10-5
 
  Divide both sides by 20:        
 
2.1 = Log
(
___P___
)  
 
2x10-5
 
  Remove Log:        
 
102.1
(
___P___
)  
 
2x10-5
 
           
  Multiply result by P0        
 
125.893 x (2x10-5)
 
=
2.52 x 10-3 (.00252)  
           
  Sound Intensity Level (SIL)        
         
  From SIL to dB:        
  If I=3.612 x 10-9 (0.000000003162)        
 
  Divide I by I0:        
  I/I0 = 3.612 x 10-9/10-12 = 3162        
           
  Take Log:        
  Log(3162) = 3.5        
           
  Multiply by 10 to get Li:        
  Li=10 x 3.5 = 35dB        
           
         
From dB to SIL:        
 
LI = 10Log
(
___I___
)  
 
I0
 
           
  if dB = 42        
           
 
42dB = 10Log
( ___I___ )  
 
10-12
 
  Divide both sides by 10:        
 
4.2 = Log
(
___I___
)  
 
10-12
 
  Remove Log:        
 
104.2
(
___I___
)  
 
10-12
 
           
  Multiply result by I0        
 
15848.932 x (10-12)
 
=
1.585 x 10-8 (.00000001585)  
           
         
  Combining SIL        
           
  Uncorrelated I1 + I2 = Itotal        
           
  30dB + 30dB        
           
  Convert to SIL        
  .000000001+.000000001=.000000002        
           
  Convert to dB        
  .000000002 SIL = 33dB        
         
  Combining SPL        
           
  Uncorrelated P12 + P22 = P2total        
           
  30dB + 30dB        
           
  Convert to SPL        
  .0006322+.0006322=.000000798        
           
  Square Root of Ptotal        
  .00000079922=.000893986        
           
  Convert to dB        
  .000893986 SIL = 33dB        
           



sound level 
dB-SPL
 
sound pressure 
Pa
 
sound intensity 
W/m²
         
sound pressure 
Pa  
sound level 
dB-SPL
 
sound level 
dB-SIL
sound intensiy