Course:PHYS341/2018/Calendar/Lecture 10

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Phys341 Lecture 10: Summary and web references

2018.01.24

Textbook: 9.2-9.6 (minus the math)

Slide List

  1. Sound intensity
    • Sound power is the sound energy emitted in unit time
    • Normally measured in watts (W - joules per second)
    • What matters more for detection and hearing is the intensity, the power incident on a unit area
    • Which is why sound appear quieter the further you get from the source; the sound power is spread over a larger area (and may also get absorbed by intervening walls etc.)
    • Normally measured in W/m2
    • We can hear an enormous range of sound intensities (dynamic range) without discomfort
    • In the middle of the audio frequency range (~ 1 kHz) we can easily hear (but seldom experience) a billionth (10-9) of a W/m2
    • 1 W/m2 is usually considered to be at the threshold of pain
  2. Intensity in English, music and physics
  3. The decibel scale
  4. The effect of distance on sound level
    • The way distance affects sound level is generally complicated unless the sound is radiating from a small source into an open space, in which case:
    • Double the distance, sound level drops 6 dB
    • e.g. a siren in an open field produces a SPL of 90 dB at 10 m, 84 dB at 20 m, 78 dB at 40 m etc.
    • If you want to see the math, its all in chapter 9 of Physics and Music
    • This is an example of physicists’ beloved inverse square law but is seldom observed in the real world, because of:
    • Inside: reflections and absorption due to walls, ceiling, audience, etc.
    • Outside: obstructions (buildings etc.), ground surface, wind, atmospheric effects...
  5. A musical example
    • A solo violin produces about 1 mW of audible sound.
    • At a distance of 4 m, standing on a hard floor, this is sound is spread over an area of 100 m2.
    • So the sound intensity if 1/100 mW/m2 or 10-5 W/m2.
    • This translates into 70 dB, forte.
  6. loudness
    • The decibel scale attempts to encompass the dynamic range of the human ear
    • It does not take into account the strong frequency dependence of our hearing
    • e.g. 120 dB at 1 kHz is intensely annoying and verging on deafening
    • 120 dB at 10 Hz we can feel but not hear
    • 120 dB at 100 kHz we can neither hear nor feel
    • Nominally we can hear sounds from 20 Hz to 20 kHz (10 kHz if you are 60+)
    • Understanding and appreciation of speech and music depends on range 125 Hz to 8 kHz
    • This is the range an audiologist tests
  7. Phons
    • “Phons” are a modification of the dB scale intended to take into account our perception of loudness.
    • Phons were originally defined by Fletcher and Munson in the 30s.
    • In 2003 the International Standards Organization redefined phons to take into account the large amount of high-quality data now available.
    • The loudness in phons is defined to be equal to the SPL in dB at 1 kHz
    • At much lower and higher frequencies the loudness in phons is generally less than the SPL in dB, because here our ears are not so acute as at 1 kHz.
    • The standard is called ISO 226:2003 https://en.wikipedia.org/wiki/Equal-loudness_contour (Horizontal axis is frequency!)
    • How to read this plot:
    • At a frequency of 1 kHz at 60 dB sound has a loudness of 60 phons (by definition).
    • At a low frequency of 100 Hz, a SPL of 78 dB has a loudness of 60 phons.
    • At a high frequency of 10 kHz, a SPL of 74 dB has a loudness of 60 phons.
    • At an ultra-low frequency of 10 Hz, a SPL of 108 dB has a loudness of 60 phons.
    • At an ultra-high frequency of 15 kHz, a SPL of 70 dB has a loudness of 60 phons if you are young and healthy, but if you are over 50 you probably cannot hear it at all.
  8. Music and speech
    • Adding sounds of equal frequency
    • The decibel/phon scale addresses a simple question:
    • If I can easily hear one violin:
    • Why doesn’t a pair of violins playing in unison sound twice as loud?
    • Why doesn’t the whole violin section of an orchestra deafen me?
    • Answer:
    • The decibel (and phon) scale is not simply scalable (not linear, but logarithmic)
    • Rule: double the sound, add 3 dB to the original SPL.
    • Two violins each individually playing produce an SPL of 90 dB at your ear.
    • Two such violins playing together produce 93 dB at your ear.
    • How many such violins would it take to hurt your ears (120 dB)?
    • Answer: to add 30 dB requires 10 doublings, i.e. 210 = 1024 (hard to get this many fiddlers in the same physical location).
  9. Sones
    • Just when you thought this was getting too complicated:
    • To address the problem of perceived loudness, another new measure was developed:
    • Let’s not go there; enough is enough for one lecture.
  10. Noise
    • One person’s music is another person’s noise -
    • Sound-induced stress depends on a lot more than dB
    • What can make it worse:
    • Identifiable pitch (e.g. whining fans)
    • Information content (e.g. phone conversations)
    • Antipathy to the source (e.g. wind turbines)
    • “dBA” means dB frequency-weighted for human hearing.
    • Permitted noise exposure in the workplace https://www.worksafebc.com