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Sound power level can be derived by dividing intensity by radiating area

Sound power level can be derived by dividing intensity by radiating area

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Sep 20, 20262 min read

Sound power level can be derived by dividing intensity by radiating area

Related

  • Sound intensity measures power density as watts per unit area (similarity 0.88)
  • The auditory spectrum differs from the physical power spectrum in resolution and shape (similarity 0.87)
  • Sound power level measures total radiated acoustic power referenced to 1 picowatt (similarity 0.85)
  • Sound intensity is a vector describing the directional flow of sound energy. (similarity 0.85)
  • Sound intensity spans a trillion-fold range, forcing a logarithmic scale (similarity 0.85)
  • Speaker power output changes with room dimensions only via their ratios (similarity 0.85)
  • Measurable and audible sound qualities can be shown to correlate reliably (similarity 0.84)
  • Sound intensity measures energy transfer rate per unit area (similarity 0.84)
  • Sound power, unlike intensity, is direction-independent and context-free (similarity 0.84)
  • Low-frequency tones become relatively louder as level increases. (similarity 0.84)
  • Walls must be rough on many scales to scatter sound diffusely (similarity 0.84)
  • High ambient noise forces listeners to raise volume toward hearing-loss levels (similarity 0.84)
  • Sound pressure and intensity are distinct quantities interconvertible by a known relationship (similarity 0.84)
  • Sound’s constant speed across wavelengths is what preserves speech intelligibility (similarity 0.83)
  • Amounts of masking are expressed as dB differences, not absolute dB SPL levels. (similarity 0.83)

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  • Sound power level can be derived by dividing intensity by radiating area
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  • A room's average sound-bounce path length depends only on volume-to-area ratio
  • Adding soft noise can make music subjectively sound more brilliant
  • Amounts of masking are expressed as dB differences, not absolute dB SPL levels.
  • Faster reaction times track louder sounds only at moderate to high levels
  • Measurable and audible sound qualities can be shown to correlate reliably
  • Perforated projection screens reflect sound back toward loudspeakers
  • Pressure nodes in a sound field host maximal air flow which weakens sound intensity
  • Sound intensity measures energy transfer rate per unit area
  • Sound intensity measures power density as watts per unit area
  • Sound power level measures a source independent of surrounding acoustic context
  • Sound pressure amplitude falls off as the inverse of distance from a source
  • Sound pressure and intensity relate through air impedance of roughly 415 rayls
  • Sound's constant speed across wavelengths is what preserves speech intelligibility
  • Speaker power output changes with room dimensions only via their ratios
  • Spectral cue calibration requires visible sound sources
  • The auditory spectrum differs from the physical power spectrum in resolution and shape
  • Transducer resonances radiate widely and thus stay audible in rooms
  • Vocal tract sound transmission is governed by cross-sectional area
  • Warmth in a sound can be produced by two opposite spectral manipulations