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Lesson 29 · Pipes and columns
A quarter wave in a one-eyed pipe
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A quarter wave in a one-eyed pipe

Close a pipe at one end and the rules change. The closed end pins the air still — a node — while the open mouth swings free — an antinode. The simplest wave that manages both is a QUARTER of a wavelength, so λ=4L\lambda = 4L and f1=v4Lf_1 = \dfrac{v}{4L} — read aloud: f-one equals v over four-L, where LL is now the length of the air column in metres, vv the speed of sound in the room in m/s, and f1f_1 the pipe's fundamental in hertz. Same speed, same length: a closed pipe sounds an octave below the both-ends string. The 4 is the whole difference.

Stranger still: a closed pipe plays odd harmonics only: f1,3f1,5f1f_1, 3f_1, 5f_1. The even multiples would need the closed end to move, and it won't. This is the SPH3U resonance-tube lab: a tuning fork over a tube of water, and the column sings when its length hits a quarter wavelength.

fvL

f=v4Lf = \frac{v}{4L}

  • ff= Fundamental frequency (frequency)
  • vv= Speed of sound (speed)
  • LL= Pipe length (length)
Fundamental of a Closed Pipe solver →
f1fnn

fn=nf1f_n = n f_1

  • fnf_n= Harmonic frequency (frequency)
  • nn= Harmonic number
  • f1f_1= Fundamental frequency (frequency)
Harmonic Frequencies solver →
vT

v=331.3+0.606 TCv = 331.3 + 0.606\, T_C

  • vv= Speed of sound (speed)
  • TT= Air temperature (temperature)
Speed of Sound in Air solver →