Sound

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Sound is a disturbance of mechanical energy that propagates through matter as a wave (through fluids as a compression wave, and through solids as both compression and shear waves). Sound is further characterized by the generic Wave#Physical description of a wave, which are frequency, wavelength, period, amplitude, speed of sound, and direction (sometimes speed and direction are combined as a velocity Vector (spatial), or wavelength and direction are combined as a wave vector).

Humans perceive sound by the sense of hearing (sense). By sound, we commonly mean the vibrations that travel through air and are audible to people. However, scientists and engineers use a wider definition of sound that includes low and high frequency vibrations in the air that cannot be heard by humans, and vibrations that travel through all forms of matter, gases, liquids, solids, and plasma (physics)s.

The matter that supports the sound is called the Transmission medium. Sound propagates as waves of alternating pressure, causing local regions of physical compression and rarefaction. Particles in the medium are displaced by the wave and oscillate. The scientific study of the absorption and reflection of sound waves is called acoustics.

Noise is often used to refer to an unwanted sound. In science and engineering, noise is an undesirable component that obscures a wanted signal.

Perception of sound . Yellow: cochlea. Green: stereocilia. Purple: frequency spectrum of hearing response. Orange: nerve impulse)

Sound is perceived through the sense of hearing (sense). Humans and many animals use their ears to hear sound, but loud sounds and low-frequency sounds can be perceived as vibrations by other parts of the body via the tactition. Sounds are used in several ways, notably for communication through Speech communication and music. They can also be used to acquire information about properties of the surrounding environment such as spatial characteristics and presence of other animals or objects. For example, bats use animal echolocation, ships and submarines use sonar and most humans acquire some spatial information by the way in which they perceive sounds. Elephants and alligators use very low frequency sounds to communicate, and mice, bats, cetaceans, and some insects use high frequency sounds, both outside the human hearing range.

Humans can generally hear sounds with frequencies between 20 Hertz and 20 kHz (the audio range) although this range varies significantly with age, occupational hearing damage, and gender; nearly all people in the developed world can no longer hear 20,000 Hz by the time they are teenagers, and progressively lose the ability to hear both higher frequencies and low level sounds as they get older. Most human speech communication takes place between 200 and 8,000 Hz and the human ear is most sensitive to frequencies around 1000-3,500 Hz. Sound above the hearing range is known as ultrasound, and that below the hearing range as infrasound.

The amplitude of a sound wave is specified in terms of its pressure. The human ear can detect sounds with a very wide range of amplitudes and so a logarithmic decibel amplitude scale is used. The quietest sounds that humans can hear have an amplitude of approximately 20 µPa (micropascals) or a sound pressure level (SPL) of 0 dB re 20 µPa (often incorrectly abbreviated as 0 dB SPL). Prolonged exposure to sound pressure levels exceeding 85 dB can permanently damage the ear, resulting in tinnitus and hearing impairment. Sound levels in excess of 130 dB are more than the human ear can safely withstand and can result in serious pain and permanent damage. At very high amplitudes, sound waves exhibit nonlinear effects, including shock wave.

Just how sound travels, or propagates, is difficult to imagine for many, as sound is invisible. Sound is an oscillating pressure wave, in which air is compressed, then decompressed, as sound moves away from its origin. Imagine a tube exposed to air whereby sound travels longitudinally through it. The air acts rather like a Slinky spring would if confined to the tube. As sound is generated at one end, a pressure wave will begin to travel through the air in the tube. Watching an earth worm move by pulsating its long body may help the imagination. The cycle length (i.e., the distance between successive 'bunched up parts of the slinky') is a particular sound's wave length, though most real world sounds are a mixture of many wave lengths. Low frequency sounds (eg, low organ or piano notes, bass guitars, etc) have large wave lengths, on the order of 10-50 feet long. High frequency sounds (eg, some parts of the noise associated with transient sounds as in many percussion instruments), have wave lengths as small as 1/2 inch.

Speed of sound The speed at which sound travels depends on the medium through which the waves are passing, and is often quoted as a fundamental property of the material. In general, the speed of sound is proportional to the square root of the ratio of the elastic modulus (stiffness) of the medium and its density. Those physical properties and the speed of sound change with ambient conditions. For example, the speed of sound in gases depends on temperature. In air at sea level, the speed of sound is approximately 769.5 mph (1,238.3 km/h) at 68 °F (20 °C), Speed of Sound in water 3,315.1 mph (5,335.1 km/h) at 20 °C (68 °F), Speed of Sound in Water and in steel 13,332.1 mph (21,446 km/h) The Soundry: The Physics of Sound . The speed of sound is also slightly sensitive (a second order effect) to the sound amplitude, which means that there are nonlinear propagation effects, such as the production of harmonics and mixed tones not present in the original sound. (see parametric array).

Sound pressure Sound pressure is the pressure deviation from the local ambient pressure caused by a sound wave. Sound pressure can be measured using a microphone in air and a hydrophone in water. The SI unit for sound pressure is the pascal (unit) (symbol: Pa). The instantaneous sound pressure is the deviation from the local ambient pressure caused by a sound wave at a given location and given instant in time. The effective sound pressure is the root mean square of the instantaneous sound pressure averaged over a given interval of time. In a sound wave, the complementary variable to sound pressure is the particle velocity. For small amplitudes, sound pressure and particle velocity are linearly related and their ratio is the acoustic impedance. The acoustic impedance depends on both the characteristics of the wave and the Transmission medium. The local instantaneous sound intensity is the product of the sound pressure and the acoustic particle velocity and is, therefore, a vector quantity.

The loudest sound ever in air reported was the 1883 volcanic eruption of Krakatoa, whereby sound pressure levels reached 180 dB re 20 µPa at a distance of 100 Mile#Statute miles (160 km).

Sound pressure level As the human ear can detect sounds with a very wide range of amplitudes, sound pressure is often measured as a level on a logarithmic decibel scale.

The sound pressure level (SPL) or Lp is defined as L_\mathrm{p}=10\, \log_{10}\left(\frac{{p}^2}{{p_0}^2}\right) =20\, \log_{10}\left(\frac{p}{p_0}\right)\mbox{ dB} where p is the root-mean-square sound pressure and p0 is a reference sound pressure. Commonly used reference sound pressures, defined in the standard American National Standards Institute S1.1-1994, are 20 micropascal in air and 1 micropascal in water. Without a specified reference level, a value expressed in decibels cannot represent a sound pressure level.

Since the human ear does not have a flat spectral response, sound pressure levels are often frequency weighted so that the measured level will match perceived levels more closely. The International Electrotechnical Commission (IEC) has defined several weighting schemes. A-weighting attempts to match the response of the human ear to noise and A-weighted sound pressure levels are labeled dBA. C-weighting is used to measure peak levels.

===Examples of sound pressure and sound pressure levels===See also Sound pressure#Examples of sound pressure and sound pressure levels.

{| class="wikitable"! Source of sound !! root mean square sound pressure !! sound pressure level|-! !! align="center" | Pa !! align="center" | dB re 20 µPa|-|immediate soft tissue damage || align="right" | 50000 || align="right" | approx. 185|-|rocket launch equipment acoustic tests || align="right" | || align="right" | approx. 165|-|threshold of pain ], 100 m distant || align="right" | 6–200 || align="right" | 110–140|-|jack hammer, 1 m distant / discotheque ] from long-term exposure || align="right" | 0.6 || align="right" | approx. 85|-|traffic noise on major road, 10 m distant || align="right" | 0.2–0.6 || align="right" | 80–90|-|moving passenger car, 10 m distant ] at 2 kHz -- undamaged human ears || align="right" | 0.00002 || align="right" | 0|}

Equipment for dealing with sound Equipment for generating or using sound includes musical instruments, hearing aids, sonar systems and sound reproduction and broadcasting equipment. Many of these use electro-acoustic transducers such as microphones and loudspeakers.

References

Sound measurement

Decibel, sone, Mel scale, phon, hertz
Sound pressure level
Particle velocity, acoustic velocity
Particle displacement, particle amplitude, particle acceleration
Sound power, acoustic power, sound power level
Sound energy flux
Sound intensity, acoustic intensity, sound intensity level
Acoustic impedance, sound impedance, characteristic impedance
Speed of sound, sound velocity, amplitude

See also Template:Sound measurements