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Understanding Sound and Hearing: Amplitude, Frequency, and Decibels, Slides of Advanced Physics

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.

What you will learn

  • What is the decibel (dB) and how is it calculated?
  • How does the human ear convert sound pressure to power for dB calculations?
  • What is the definition of sound?
  • How is sound pressure measured?
  • What is the reference value used in dB calculations and why?

Typology: Slides

2021/2022

Uploaded on 03/31/2022

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Download Understanding Sound and Hearing: Amplitude, Frequency, and Decibels and more Slides Advanced Physics in PDF only on Docsity!

Sound and Hearing

Nature of the Sound Stimulus

“Sound” is the rhythmic compression and decompression of the air around us caused by a vibrating object.

The “decibel” (dB)

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).

dB = 10 log(Observed Power / Reference)

dB

SPL

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……..

Some Typical Sound Amplitude Values

More about those pesky decibels

  • JND for sound intensity is about 1 dB SPL for most of normal range of hearing
  • What does 0 dB SPL mean? Hint: 20 log (20 microPa/20 microPA) = 0 dB SPL
  • If one machine emits 80 dB SPL then how much sound amplitude would be expected from two machines side-by-side? 2 x 80 = 160 dB SPL ??? (That’s pretty intense) Convert from dB SPL back to raw pressure, sum the pressures, then convert sum to dB SPL 80 dB SPL  antiLog(80/20)  10, 20 log (10,000+10,000) = 86 dB SPL (approx.)

A “Better” Sound Amplitude Table?

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

Most Sound Stimuli are Complex

Speed of Sound

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).

Gross Anatomy of the Ear

The “Impedance Problem”

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

The Cochlea

Photomicrograph: Sensory Hair Cells

Three rows of Outer Hair Cells One Row of Inner Hair Cells

Auditory Transduction