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Potential health risks of exposure to noise from personal music ...

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Health <strong>risks</strong> <strong>from</strong> <strong>exposure</strong> <strong>to</strong> <strong>noise</strong> <strong>from</strong> <strong>personal</strong> <strong>music</strong> players3.3.2. Sound: Physical and technical backgroundSound or Sound waves comprise a wave phenomenon. Sound waves are ‘longitudinal’waves because sound waves consist <strong>of</strong> areas <strong>of</strong> higher and lower local pressure. Thepropagation <strong>of</strong> sound waves occurs in all media, i.e. in gases, liquids and solids as well asin more complex fluids like e.g. organisms and tissues.Fundamentally, sound waves are characterized by their spectrum. A spectrum is thesummation <strong>of</strong> individual frequencies (f) and amplitudes a certain signal has in thesurrounding medium. In daily acoustic settings sound is a complex summation <strong>of</strong> manydifferent sounds <strong>from</strong> different sources. Sound will not propagate through vacuum and itspropagation is influenced by material properties like density and compression / shearstrengths. Characteristic parameters <strong>of</strong> sound waves in a given situation derive <strong>from</strong> thefundamental wave equation which may be <strong>to</strong> challenging <strong>to</strong> evaluate for a given complexscenario.The <strong>exposure</strong> <strong>to</strong> sound in a typical setting is determined by many fac<strong>to</strong>rs which are notalways easy <strong>to</strong> assess. For sound propagation, the geometry <strong>of</strong> the room, the surfacematerials and furnishings as well as its occupation, the materials and media surroundingthe source and the listener play a determining role. Like for any other wave, the soundwave at a specific location depends on interference <strong>from</strong> different sources which dependson the relative phase reaching the location <strong>from</strong> different sources or after travellingdifferent pathways. Thus, the distribution <strong>of</strong> energy and the energy absorption in sound<strong>exposure</strong> scenarios is not necessarily straightforward which leads <strong>to</strong> the many flavours <strong>of</strong>acoustics as subfields <strong>of</strong> physics and engineering, medicine and architecture. Well-knownexamples are the different acoustical characteristics <strong>of</strong> a furnished and unfurnished room,the sound-design <strong>of</strong> commercial products like cars and the engineering <strong>of</strong> anti-soundreflectionsurfaces <strong>to</strong> be used in the prevention <strong>of</strong> sound propagation next <strong>to</strong> highways,railway lines, but also within sound-studios and in other architectural settings. Notablyalso details <strong>of</strong> the ana<strong>to</strong>my <strong>of</strong> the ear, the hair dress and clothing specific <strong>to</strong> one listenermay affect the sound distribution before the sound reaches the sound sensitive cells inthe inner ear <strong>of</strong> a specific observer.To assess the <strong>exposure</strong> <strong>from</strong> different sources in a specific point, it is common use <strong>to</strong>analyse the different contributions by their frequency and <strong>to</strong> provide certainmeasurements related <strong>to</strong> sound (like power, amplitude etc) by their densities in thefrequency spectrum. Depending on whether sound waves are harmonic (‘<strong>to</strong>nes’, ‘hum’)or relate <strong>to</strong> uncorrelated events. Sound with an equal energy distribution acrossfrequencies is called ‘white <strong>noise</strong>’, while most sources <strong>of</strong> sound exhibit dominatingfrequency bands originating <strong>from</strong> resonance phenomena. Typically, the above describedcomplex interaction <strong>of</strong> sound waves with the particular environment and media(absorption, refraction, reflection and interference) leads <strong>to</strong> a changing spectrum <strong>of</strong>sound waves with progressing propagation or the modified position <strong>of</strong> an observer.3.3.3. Units <strong>of</strong> <strong>noise</strong> <strong>exposure</strong>3.3.3.1. Sound pressure level and dB SPLOne parameter <strong>of</strong> the acoustic (sound) wave which is generally used <strong>to</strong> assess sound<strong>exposure</strong> <strong>to</strong> humans is the sound pressure level expressed in µPa or Pa. Human ear’audible sound pressure levels range <strong>from</strong> 20 µPa (hearing threshold) till 20 Pa (painthreshold), resulting in the scale 1:10,000,000. Since using such a large scale is notpractical, a logarithmic scale in decibels (dB) was introduced which is also in agreementwith physiological and psychological hearing sensations.dB <strong>of</strong> sound pressure level (dB SPL) is defined as: 20 log 10 p1/p0 where p1 is actuallymeasured sound pressure level <strong>of</strong> a given sound, and p0 is a reference value <strong>of</strong> 20µPa,which corresponds <strong>to</strong> the lowest hearing threshold <strong>of</strong> the young, <strong>health</strong>y ear. In thelogarithmic scale the range <strong>of</strong> human ear’s audible sounds is <strong>from</strong> 0 dB SPL (hearingthreshold) <strong>to</strong> 120-140 dB SPL (pain threshold) (see table 1 below).16

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