Frequencies of standing waves in a straw

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Discussion Overview

The discussion revolves around the frequencies produced by sound waves in straws used as noise makers, particularly focusing on their behavior as acoustic instruments. Participants explore the theoretical implications of these frequencies, comparing them to those of traditional woodwind instruments like oboes, and consider the effects of the straw's geometry on sound production.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Experimental/applied

Main Points Raised

  • Some participants note that the straws seem to behave like pipes open at both ends, producing all harmonics, which contrasts with the expected behavior of closed tubes that typically only produce odd harmonics.
  • One participant suggests that the fundamental mode of the straw should have a wavelength about four times the length of the tube, indicating a discrepancy in expected speed of sound calculations.
  • Another participant reports measuring frequencies from their straw oboe and finding them significantly lower than expected, raising questions about the underlying physics.
  • Some participants discuss the potential effects of end corrections and the geometry of the straw on the observed frequencies, suggesting that these factors might contribute to the discrepancies in expected results.
  • There is mention of the acoustic impedance of the straw, with one participant proposing that the high aspect ratio could increase the effective mass of the enclosed air, thereby lowering the resonant frequency.
  • Concerns are raised about the assumptions made regarding the ends of the instrument, with a participant questioning whether the mass of the reed could introduce additional end effects that affect the resonance.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the behavior of the straw as an acoustic instrument, with multiple competing views on how it should theoretically function. There is no consensus on the reasons for the observed discrepancies in frequency measurements.

Contextual Notes

Limitations include potential missing assumptions about the geometry of the straw, the effects of end corrections, and the influence of the oscillating reed on the overall sound production. The discussion highlights unresolved mathematical steps in relating the observed frequencies to theoretical predictions.

steven george
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I am a physics teacher and I my class is currently studying sound waves. I had my class make some noise makers with straws as shown here. http://www.physics.org/interact/physics-to-go/straw-oboes/

We measured the frequencies coming from the straws and they seem to act like a pipe open at both ends since all the harmonics are present. The frequencies seem to be much lower than we would expect though. I had students use the length of the straw and the fundamental frequency to find the speed of sound. Most of them were getting answers between 120 and 145 m/s.

We considered the straw length to be half a wavelength and then multiplied the wavelength by the fundamental frequency to find the speed. Am I missing something here, or is there some reason that this behaves differently than a typical open ended air column?

Thanks for any help!
 
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This kind of instrument ("reeds" instruments, like oboe, clarinet) behaves usually like closed tube at the mouth end.
So your fundamental mode has a wavelength which is about 4 times the length of the tube. (With the end correction, the factor is a little more than 4)
So you will get speed values that are not too bad.
 
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Thanks! I had suspected that it would behave like a closed tube at the mouth end but if that was the case I would expect to see only odd numbered harmonics. We saw all the harmonics so I am still a bit puzzled by the whole thing.
 
How did you measure the frequencies?
 
nasu said:
How did you measure the frequencies?
I use a fantastic program called Zelscope.
 
Hi Steven

I repeated your experiment and got similar results.
I used audacity to measure the spectrum of the straw oboe and saw all the harmonics as expected from a tube open at both ends , not the odd harmonics predicted by the physics of oboes.
Then I looked at the fundamental frequency and the resulting speed of sound was extremely low assuming a tube open at both ends and even substantially low assuming a tube closed at one end and open at the other.

I don't see many people posting their spectra, tube lengths and spectra on line.
our 10 cm straw oboe resonated at many frequencies depending on how hard we blow but the lowest frequency at reasonable flow was 344 Hz and the highest was 409 Hz , these frequencies are far lower than the resonance of the straw if we assume either an open or closed end.

I do not know what would cause this.
 
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Thanks for your input. I'm still hoping to find out what the problem is.
 
An oboe air column behaves like that one of an open pipe at both ends, so it should have the even harmonics.

The interesting thing relative to the results you are finding is that an oboe has length 62 cm, but lowest note around 233 Hz.
 
olivermsun said:
An oboe air column behaves like that one of an open pipe at both ends, so it should have the even harmonics.

The interesting thing relative to the results you are finding is that an oboe has length 62 cm, but lowest note around 233 Hz.

Thanks. Do you have any explanation for the discrpencies? The numbers you give would give a wavelength of 1.24 m (a little more than that when you account for end correction. That would give us a speed of under 300 m/s, which is much too low. The results with straws were much, much worse than this.
 
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I don't know ... it's a real mystery to me. :smile:

The oboe numbers don't seem so far off if you give a 10-15% allowance for end effects, the actual geometry of the oboe, maybe viscous effects, etc. There is a more rigorous way to predict the frequencies that is detailed in Plitnick and Strong (1979): http://scitation.aip.org/content/asa/journal/jasa/65/3/10.1121/1.382503

The straw is interesting though. I will think about it some more tomorrow.
 
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  • #11
With the high aspect ratio of a straw, I expect the acoustic impedance to be rather high; increasing the effective mass of the enclosed air. (see: http://press.princeton.edu/chapters/s9912.pdf) The increased effective mass would lower the resonant frequency, as with a spring-and-mass oscillator.

This site may also be of some interest: https://www.nde-ed.org/EducationResources/CommunityCollege/Ultrasonics/Physics/acousticimpedance.htm
 
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  • #12
I'm wondering about the impedance of an oscillating reed. The simple analysis of a vibrating column or string assume that the ends are perfect open or short circuits. Could the substantial mass ( but not infinite) be introducing a further end effect? Woodwind instruments are not high Q resonators so their natural frequencies would probably depend a lot on the oscillating mechanism as well as the resonant air column.
 
  • #13
Tom.G said:
With the high aspect ratio of a straw, I expect the acoustic impedance to be rather high; increasing the effective mass of the enclosed air. (see: http://press.princeton.edu/chapters/s9912.pdf) The increased effective mass would lower the resonant frequency, as with a spring-and-mass oscillator.

This site may also be of some interest: https://www.nde-ed.org/EducationResources/CommunityCollege/Ultrasonics/Physics/acousticimpedance.htm

Thanks for the links the Princeton book does a great job of describing acoustical impedance. Paul Doherty
 

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