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{{Sound measurements}} |
{{Sound measurements}} |
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In [[physics]], '''sound energy''' is a form of |
In [[physics]], '''sound energy''' is a form of energy that can be [[hearing|heard]] by living things. Only those waves that have a frequency of 16 Hz to 20 kHz are audible to humans. However, this range is an average and will slightly change from individual to individual. Sound waves that have frequencies below 16 Hz are called [[infrasound|infrasonic]] and those above 20 kHz are called [[ultrasound|ultrasonic]]. [[Sound]] is a [[mechanical wave]] and as such consists physically in [[oscillation|oscillatory]] elastic [[compression (physics)|compression]] and in oscillatory displacement of a [[fluid]]. Therefore, the [[transmission medium|medium]] acts as [[energy storage|storage]] for both [[potential energy|potential]] and [[kinetic energy]].<ref>{{cite book |
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|title=Handbook of Engineering Acoustics |
|title=Handbook of Engineering Acoustics |
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|last1=Möser|first1=M. |
|last1=Möser|first1=M. |
Revision as of 04:31, 10 May 2024
Sound measurements | |
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Characteristic | Symbols |
Sound pressure | p, SPL, LPA |
Particle velocity | v, SVL |
Particle displacement | δ |
Sound intensity | I, SIL |
Sound power | P, SWL, LWA |
Sound energy | W |
Sound energy density | w |
Sound exposure | E, SEL |
Acoustic impedance | Z |
Audio frequency | AF |
Transmission loss | TL |
In physics, sound energy is a form of energy that can be heard by living things. Only those waves that have a frequency of 16 Hz to 20 kHz are audible to humans. However, this range is an average and will slightly change from individual to individual. Sound waves that have frequencies below 16 Hz are called infrasonic and those above 20 kHz are called ultrasonic. Sound is a mechanical wave and as such consists physically in oscillatory elastic compression and in oscillatory displacement of a fluid. Therefore, the medium acts as storage for both potential and kinetic energy.[1]
Consequently, the sound energy in a volume of interest is defined as the sum of the potential and kinetic energy densities integrated over that volume:
where
- V is the volume of interest;
- p is the sound pressure;
- v is the particle velocity;
- ρ0 is the density of the medium without sound present;
- ρ is the local density of the medium; and
- c is the speed of sound. Sound energy is energy that can be heard.
See also
References
- ^ Möser, M.; Müller, G. (2012). Handbook of Engineering Acoustics. Springer. p. 7. ISBN 9783540694601.