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OBJECT:
To calculate the velocity of sound from measurement of the
wavelength in air for sound of a certain frequency.
APPARATUS:
Resonance tube with arrangement for varying water level (use
only distilled water); rubber tipped hammer; tuning fork; Hg thermometer.
INTRODUCTION:
For a closed tube, resonance occurs at tube
lengths of an odd multiple of
one-fourth wavelength, i.e. at /4, 3/4,
5/4 etc.
SUGGESTIONS:
- 1.
- Find the positions of the water level in the tube for
the first three of these resonances. Use these readings to calculate the
velocity of sound, v. Initially have enough water that you can
raise the level above the first resonance position. The tuning fork frequency
is on the fork.
Since the effective end of the resonance tube is not at the tube's end,
do not use the position of the tube's top in your calculations,
but rather take differences between the other readings.
- 2.
- Since v = , correct your value of
v to
0oC
(T = 273.16 K) and compare with that accepted
for dry air at 0oC: 331.29 .07 m/s,
[Wong, J. Acoust. Soc. Am., 79, 1559, (1986)]. For humid air see
3. below.
- 3.
- How should the v.p. of water, Pw, in the tube
affect the measured velocity?
An estimate is not difficult from
v = .Use an average /M:
where is the partial pressure of air
and Pw is the v.p. of water; Ma 29 kg
and Mw = 18 kg. Hence
OPTIONAL: Humidity changes will affect tuning of what musical instruments?
- 4.
- What effect does atmospheric pressure have on the velocity of sound
in dry air? (Assume air at these pressures is an ideal gas.)
- 5.
- Viscosity and heat conduction in the tube may reduce v
by 0.1%.
See N. Feather, ``The Physics of Vibrations and Waves'',
Edinburgh Univ. Press, (1961), p. 110-120; this reference also has a
delightful
historical account (including Newton's famous goof).
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Previous: SC-1 Transverse Standing Waves on
Michael Winokur
4/7/2000