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The nature and properties of sound

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... the sound is generated by a pure sine oscillation and given by the expression ... For a 1 kHz tone this means that the wavelength is 34 cm. ... – PowerPoint PPT presentation

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Title: The nature and properties of sound


1
The nature and properties of sound
  • Jakob Christensen-Dalsgaard,
  • Center for Sound Communication, SDU Odense
    University

2
Definition of sound
  • Sound is a longitudinal wave propagating in an
    elastic medium
  • The sound wave is pressure /medium motion
    oscillations
  • Pressure and particle velocity are in phase in
    the propagating sound wave

3
Properties of the sound wave 1
  • Some definitions
  • Frequency the number of wave cycles/second (f).
  • Angular frequency (?) ?2?f
  • Wavelength The distance (in m) between two wave
    maxima
  • Phase time offset of wave zero crossing compared
    to reference

4
Properties of the sound wave 2
  • In the simplest case (tuning fork), the sound is
    generated by a pure sine oscillation and given by
    the expression
  • Here, f is the frequency and ? is the phase. P0
    is the sound pressure amplitude

5
Properties of the sound wave 3
  • The relationship between frequency (f),
    wavelength (?) and sound velocity (c)
  • The sound velocity in air is 340 m/s. For a 1 kHz
    tone this means that the wavelength is 34 cm. In
    water, where the sound velocity is approximately
    1500 m/s, the wavelength for a 1 kHz tone is 1.5 m

6
Properties of the sound wave 4
  • Sound pressure and particle velocity During
    sound propagation, the acoustic particles
    oscillate around a rest position.
  • Far away from the sound emitter, the particle
    oscillation velocity of the sine tone is given by
  • Here, particle velocity oscillations is in phase
    with pressure oscillations.

7
Pressure, velocity, impedance
  • The relationship between pressure p and particle
    velocity v in the far-field sound wave is given
    by
  • Z is the characteristic impedance of the medium,
    , where c is sound
    velocity in the medium
  • and ? is the density

8
Sound intensity
  • The sound intensity I, the energy flux radiated
    by the far-field sound wave through a unit area,
    is given by

9
The dB scale
  • Sound pressure is usually stated in dB relative
    to a reference pressure
  • The most common reference pressure (in air) is 20
    ?Pa (dB SPL), close to the human threshold of
    hearing at 1 kHz
  • When sound intensities are used, dB values are
    calculated as
  • since I?p2

10
Some useful dB values
  • Doubling of sound pressure
  • Tenfold increase in sound pressure

11
dB values
  • Note that because the dB scale is logarithmic,
    addition means multiplication of the sound
    pressures!
  • For example Two sound sources both emit sound in
    phase at 50 dB SPL. What is the resulting sound
    pressure?

12
The distance law
  • The area that sound is radiated through increases
    with the square of distance, therefore sound
    intensity drops with the square of distance
  • Since intensity is proportional to pressure
    squared, this means that pressure drops with
    distance (usually stated as -6 dB per distance
    doubled)

13
Sound diffraction and reflection
  • Objects interact with the sound wave in the
    following ways
  • Objects that are smaller than 1/6th wavelength
    are transparent to sound
  • Objects with sizes comparable to the wavelength
    scatter or diffract the sound wave
  • Objects with sizes more than 5-10 wavelengths
    reflect the sound wave

14
Exercise
  • Suppose that a new frog species echolocated at
    500 Hz. What would the minimal sizes of objects
    it could detect (approximately)?

15
Sound reflection
  • Sound reflection depends on the difference
    between the characteristic impedance of the
    medium on both sides of the boundary.
  • Large impedance differenceslarge fraction of
    sound energy is reflected, small fraction is
    transmitted

16
Reflection
  • Reflection from a soft-hard boundary
  • Reflection from a hard-soft boundary

17
Temperature and wind effects
  • Since sound velocity depends on temperature,
  • c331 0.6 T in air
  • temperature gradients result in a velocity
    gradient.
  • A velocity gradient produces refraction of the
    sound wave according to Snells law

18
Temperature and velocity gradients
  • An upward oriented velocity gradient (lower
    ground temperatures) produces downward
    deflection
  • A downward oriented gradient (higher ground
    temperatures) produces upward deflection

19
Wind effects, attenuation
  • The effect of wind currents is to bend the sound
    wave
  • In addition to the drop of sound pressure due to
    spreading, sound can be absorbed/scattered by the
    medium
  • Especially humidity effects on ultrasound

20
Doppler shift
  • A moving sound source
  • compress the sound waves in front of the object
    in the motion direction
  • -Increased frequency
  • Rarify the sound waves behind the object
  • -Decreased frequency

21
Some useful webpages
  • Dan Russells acoustics animation page
  • http//www.kettering.edu/drussell/Demos.html
  • An acoustics tutorial by David Worall at
  • http//online.anu.edu.au/ITA/ACAT/drw/PPofM/INDEX.
    html
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