Closed-Open Tube

Displacement waves in tube closed at one end:

Figure 3: Standing waves for displacement in an closed-open tube
\scalebox{0.75}{\includegraphics{eps/closedtube.eps}}

The wavelength of the first harmonic is $ \lambda_1 = 4L$.

Adding an antinode/node creates the next standing wave pattern with wavelength $ \displaystyle{\lambda_3 = \frac{4}{3}L}$

Since $ \lambda_3$ is $ 1/3^{\mbox{rd}}$ the length of $ \lambda_1$, the frequency is 3 times the fundamental and it is the “third” harmonic.

Notice the second harmonic is missing!


``Music 175: Waves'' by Tamara Smyth, Department of Music, University of California, San Diego (UCSD).
Download PDF version (waves175.pdf)
Download compressed PostScript version (waves175.ps.gz)
Download PDF `4 up' version (waves175_4up.pdf)
Download compressed PostScript `4 up' version (waves175_4up.ps.gz)

Copyright © 2020-04-02 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>