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An in-depth exploration of the nature of sound stimuli, including the properties of sound waves, decibels, and the human hearing threshold. It covers topics such as sound pressure, frequency measurement, and the logarithmic unit decibel (dB). The document also discusses the conversion of sound pressure to power and the use of references in dB calculations.
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“Sound” is the rhythmic compression and decompression of the air around us caused by a vibrating object.
The decibel is a logarithmic unit used to describe a ratio (i.e., log (x/y)) In engineering analyses, it is used to normalize “power” measurements to a known reference and then compresses the resulting ratio using a log 10 operation. This format is convenient for engineering analyses involving wide dynamic ranges (when very small and the very large magnitudes must be considered simultaneously).
The transducers (microphones) on sound level meters measure sound pressure (i.e., N/m 2 or Pascals). Pressure needs to be converted to power prior to calculation of the decibel equivalent….i.e., acoustic power = pressure 2 Finally, we need to agree upon a Reference value. By convention, we use 20 microPa (i.e., the hearing threshold) Thus: dB = 10 log (Observed Pressure 2 / 20 microPa 2 ) However……..
130 Loud hand clapping at 1 m distance 110 Siren at 10 m distance 95 Hand (circular) power saw at 1 m 80 Very loud expressway traffic at 25 m 60 Lawn mower at 10 m 50 Refrigerator at 1 m 40 Talking; Talk radio level at 2 m 35 Very quiet room fan at low speed at 1 m 25 Normal breathing at 1 m 0 Absolute threshold dBSPL
Acoustic energy results from a traveling wave of rhythmic “compression” through a physical medium (e.g., air; water; steel). It is the “compression” that travels not the medium, per se. The characteristic speed of this travelling wave varies as a function of the medium (elasticity; density). The speed of acoustic energy through the air (aka “sound”) is 331 m/sec (or 742 MPH ) at 0-deg C (Faster at higher temperatures).
99.9% of sound energy in the air is reflected at the air:water boundary (10 log(0.1/100)) = - 30 dB loss ) (1/1000x) How does the ear compensate for this loss as sound energy is transmitted from the air to the fluid that filled the cochlea? 2 dB gain via ossicular leverage (1.6x) 25 dB gain via surface area condensation (eardrum stapes) (316x) ~5 dB gain at mid-frequencies (3x) due to pinna and auditory canal resonance
Three rows of Outer Hair Cells One Row of Inner Hair Cells
Auditory Transduction