Question on Harmonics involving Air Tube

In summary: Thereforee + L1 = \frac{1}{4}\lambdae + L2 = \frac{3}{4}\lambdaSubtracting the first equation from the second equation givesL2-L1 = \frac{2}{4}\lambda = \frac{1}{2}\lambdaBut L2 - L1 = 0.4 - 0.115 = 0.285 m= \frac{1}{2}\lambdaTherefore \lambda = 2(0.285) = 0.57 mThe speed of sound in air is given as 343 m/s. The frequency is then given asF = \frac{V}{\lambda} = \
  • #1
dgoudie
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0

Homework Statement


A tuning fork is set into vibration above a vertical open tube filled with water, as seen in the figure below.
http://capaserv.physics.mun.ca/giancoli-calc/Graphics/Graph16/dgian1686.gif

The water level is allowed to drop slowly. As it does so, the air in the tube above the water level is heard to resonate with the tuning fork when the distance from the tube opening to the water level is L1 = 0.115 m and L2 = 0.400 m. What is the frequency of the tuning fork? Assume that the speed of sound in air is 343 m/s.



Homework Equations


F=V/wavelength

at first I assumed it was a closed tube and used:

Fn=nv/(4L)



The Attempt at a Solution



I treated it like a closed tube, and tried F= V/4L
but the computer said it was wrong.
I fiddled around a couple of times and tried it as an open tube and still couldn't get the right answer.

Ive tried: 746 Hz, 301 Hz, 1200 Hz, and 1490 Hz.

Can anyone see what I am doing wrong?

Thanks iun advance
 
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  • #2
The tube is an open/closed tube. Have you tried analyzing it by treating one end as open and one as closed? If so, can you please show your work? I can't find what your doing wrong if you don't show your work.
 
  • #3
I tried it as the top being open and the water representing the closed end of the tube.

I used F=V/4L. L being 0.115 m and V 343 m/s

Does L2 need to be used somehow?
 
  • #4
Do you know that L1 is the first resonance point of the wave? If you don't, you can't assume n=1.

If this is the case,

HINT: Let, [tex]n=n_o[/tex] for L=L1 and n = the next odd integer after[tex]n_o[/tex](since this is an open/closed tube) for L=L2. Can you solve for F using the equations you obtain?
 
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  • #5
The standing wave that forms in the air column need to have a antinode (position of maximum displacement of the oscillations of the air molecules) at the open end and a node at the bottom (top of the water). This means that a quarter of the standing wavelength will fit into the air column when the first resonance occurs and three quarters will fit into the air column when the second resonance is heard (antinode at the open end and a node at the bottom).

In this case there is another complication. The top end of the standing is a bit above the mouth of the tube. This distance is normally referred to as the end-correction (e). The formula should therefore be modified as follows

[tex]e + L_n = \frac{n}{4}\lambda[/tex]

in his case we have the first resonance when n = 1 (L1) (quarter of a wavelength fits) and in the second case n = 3 (L2) (three quarters of the wavelength fits in the air column).
 
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Related to Question on Harmonics involving Air Tube

1. What is the concept of harmonics in relation to air tubes?

Harmonics in relation to air tubes refers to the phenomenon of sound waves being produced and resonating within a closed tube of air. When air is enclosed in a tube and a sound wave is introduced, the air molecules vibrate at a specific frequency, creating a standing wave. This standing wave produces a specific pitch or musical note, known as the fundamental frequency.

2. How does the length of an air tube affect harmonics?

The length of an air tube directly affects the harmonics produced. As the length of the tube increases, the wavelength of the standing wave also increases, resulting in a lower fundamental frequency and a lower pitch. Similarly, a shorter tube will produce a higher frequency and pitch.

3. What is the relationship between harmonics and resonance in air tubes?

Harmonics and resonance are closely related in air tubes. In order for a standing wave to be produced, the length of the air tube must be an integer multiple of the wavelength of the sound wave. This is known as resonance. When resonance occurs, the standing wave is reinforced, resulting in a louder and more sustained sound.

4. How can harmonics in air tubes be manipulated?

Harmonics in air tubes can be manipulated by changing the length of the tube, as well as the shape and material of the tube. Different lengths and shapes will produce different harmonics and pitches. Additionally, adjusting the air pressure or temperature within the tube can also alter the harmonics produced.

5. What are some real-world applications of harmonics involving air tubes?

Harmonics involving air tubes have several practical applications. For example, musical instruments such as flutes, organs, and saxophones all utilize harmonics in air tubes to produce different notes and pitches. The acoustics of buildings and concert halls also rely on the principles of harmonics in air tubes for optimal sound quality. Additionally, medical equipment such as stethoscopes use air tubes to amplify and transmit sound waves from the body.

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