Measuring the relative phase at the two ends of an open tube. Suppose someone
has taken a long hoselike tube, coiled it up in a box, and let one open end
stick out one side of the box and the other out the other. You are not allowed
to see how much of the tube is coiled inside the box. By adding a small tuning
trombone to a protruding end, you find that you get a resonance at \(523.3\) cps
from your tuning fork. That means that the total length is either \(\frac{1}{2}
\lambda\), or \(\lambda\), or \(\frac{A}{2} \lambda\), or \(\ldots . .\) How can you
find out whether the tube is an odd or even number of half-wavelengths? Hold
two vibrating forks at one end of the tube and listen to the beats. Get the
rhythm in your head so that if you remove one fork momentarily and then
replace it (without disturbing the continued vibrations of both forks), you
can tell that the beat maximum comes "on the beat" (in musical jargon) just
where it should be. Practice several times so that you can skip a beat, count
beats in your head, and come back in step when you replace the fork. (You can
adjust the rubber-band loading to get a convenient beat frequency. If you find
all this difficult, you can use a metronome.) Now! This time, instead of
replacing the (momentarily) removed fork at the same end of the tube, carry it
to the other end. Again listen for the beats. (Both forks have continued
vibrating all this time.) Do they come back "on the beat," or do they come
back "on the off-beat"? Depending on the experimental result, you should be
able to decide whether the tube is an odd or even number of half-wavelengths.
Predict the answer; then try the experiment with your half-wavelength tube.
(Make another tube one wavelength long to get the opposite result.)