Acoustic Principles: Exercises & Solutions for Exam Preparation

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SUMMARY

The discussion focuses on acoustic principles related to string vibrations and resonance, specifically addressing pre-exam exercises in physics. Key calculations include determining the frequency of the third harmonic for a string with a density of 0.01 kg/m and a length of 60 cm under a tension of 576 Newtons, resulting in a frequency of approximately 619.67 Hz. The discussion also explores the resonance effect when a tuning fork at 440 Hz is struck near a closed tube, emphasizing the importance of tube length for sound amplification. Additionally, it explains how striking a lower D on a piano while holding down G produces an upper D note due to resonance.

PREREQUISITES
  • Understanding of harmonic frequencies in string instruments
  • Knowledge of resonance and standing waves
  • Familiarity with the wave equation and tension in strings
  • Basic principles of sound propagation in closed tubes
NEXT STEPS
  • Study the wave equation and its application in string theory
  • Explore the concept of resonance in musical acoustics
  • Learn about the harmonic series and its implications for string instruments
  • Investigate the effects of tube length on sound frequency and resonance
USEFUL FOR

Students preparing for exams in physics, music educators, acoustics researchers, and anyone interested in the principles of sound and vibration in musical instruments.

Sarah_L
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:shy: Any help will be apreciated. These are some pre-exam exercises that were given to my daughter I would like to be able to check the answers and help her with any difficulties.

1) A string, whose density is 0.01 kg/m, and whose length is of 60
cm is stretched with a tension of 576 Newtons.
a) What is the frequency of the third harmonic?
b) At what point was the string plucked?

2) A tuning fork sounds the note A (440 Hz). What would you expect
to happen if it was struck near the mouth of the closed tube (closed
at one end).
Explain why this happens. Would the sound of a tuning fork tuned an
octave higher have the same effect?

3)If you hold down (without playin) the G on the piano, and then
strike the lower D sharply, you will hear a note corresponding to
the upper D. This can't come from the string that was hammered, as
it stops vibrating as soon as you release the key, so where does it come from? Explain this, from what you know about string vibrations.
Both this phenomenon, and the one discussed in question 2 are
examples of a particular acoustic mechanism. What is it?

Thanks a lot!
 
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Sarah_L said:
1) A string, whose density is 0.01 kg/m, and whose length is of 60 cm is stretched with a tension of 576 Newtons.
a) What is the frequency of the third harmonic?
b) At what point was the string plucked?
The string will vibrate with a fundamental frequency:
[tex]\lambda \nu = \sqrt{T/(m/l)}[/tex]

Since [itex]\lambda/2 = 60 cm[/itex] for the fundamental frequency:
[tex]\nu = (2/.6)*\sqrt{576/(.01/.6)} = 619.67 Hz[/tex]
How many times the fundamental is the third harmonic?

In order to excite the third harmonic you cannot have a node (place of 0 motion) in the middle of the string, so it would have to be plucked in the middle I would think.

2) A tuning fork sounds the note A (440 Hz). What would you expect
to happen if it was struck near the mouth of the closed tube (closed
at one end).
Explain why this happens. Would the sound of a tuning fork tuned an
octave higher have the same effect?
How long is the tube? It matters.
The sound will travel down the tube and reflect back from the closed end and constructively interfere with the incident wave. If the tube is 1/4 of a wavelength, it will reflect back from the opening and constructively interfere with both the wave from the tuning fork and the wave reflected from the closed end and you will have resonance (standing wave) - loud sound.

3)If you hold down (without playin) the G on the piano, and then
strike the lower D sharply, you will hear a note corresponding to
the upper D. This can't come from the string that was hammered, as
it stops vibrating as soon as you release the key, so where does it come from? Explain this, from what you know about string vibrations.
Both this phenomenon, and the one discussed in question 2 are
examples of a particular acoustic mechanism. What is it?
Resonance.

AM
 
Sarah_L said:
[..]
3)If you hold down (without playin) the G on the piano, and then
strike the lower D sharply, you will hear a note corresponding to
the upper D. This can't come from the string that was hammered, as
it stops vibrating as soon as you release the key, so where does it come from? Explain this, from what you know about string vibrations.
Both this phenomenon, and the one discussed in question 2 are
examples of a particular acoustic mechanism. What is it?

Thanks a lot!

Hard to say in english ;-)
But i'll try it.

When you press an key on a piano, you will hear all tunes, which length of the waves is a multiple of the tune you hit sharp.

Octave - > double frequence
Quint -> 3/2 frequence
Quart -> 4/3 frequence

so when you hit g', you must hear g'', d'', g'', and so on...


greets
soeren
 

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