Sources of Musical Sound — Question 1

Section 17-6 · Physics pages 2732–2733

Question 1 Pressure boundary conditions select the organ-pipe spectrum Consider ideal tubes of length L = 0.85 m with sound speed c = 340 m/s. An open end is a pressure node; a closed end is a particle-velocity node and therefore px = 0. Neglect end corrections. L closed open Ideal straight tube; end corrections are stated when used. (a) Derive the allowed frequencies for an open-open tube and for a closed-open tube. (b) List the first three frequencies for each and identify the first overtone of the closed-open tube.
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Question 1 - Solution Pressure boundary conditions select the organ-pipe spectrum L closed open (a) Method and calculation For open-open ends, a pressure mode p ∝sin kx obeys sin kL = 0, giving kn = nπ/L and fn = nc/(2L). For a closed left end, p ∝cos kx automatically has px(0) = 0. The open right end requires cos kL = 0, km = (2m + 1)π 2L , fm = (2m + 1)c 4L . (b) Interpretation and further calculation The open-open fundamental is 340/(2 × 0.85) = 200 Hz, giving 200, 400, 600 Hz. The closed-open fundamental is 100 Hz, giving 100, 300, 500 Hz. Its first overtone is 300 Hz, the third harmonic; overtone order counts allowed modes, not every integer multiple. Physical check The ideal closed-open tube lacks even harmonics. Pressure and displacement nodes exchange roles at either type of end.

Question 1

Pressure boundary conditions select the organ-pipe spectrum

Consider ideal tubes of length L=0.85mL=0.85\,\mathrm m with sound speed c=340m/sc=340\,\mathrm{m/s}. An open end is a pressure node; a closed end is a particle-velocity node and therefore px=0p_x=0. Neglect end corrections.

Diagram shown in the original SVG worksheet.

  1. Derive the allowed frequencies for an open-open tube and for a closed-open tube.

  2. List the first three frequencies for each and identify the first overtone of the closed-open tube.

Question 1 - Solution

Pressure boundary conditions select the organ-pipe spectrum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

For open-open ends, a pressure mode p∝sin⁡kxp\propto\sin kx obeys sin⁡kL=0\sin kL=0, giving kn=nπ/Lk_n=n\pi/L and fn=nc/(2L)f_n=nc/(2L). For a closed left end, p∝cos⁡kxp\propto\cos kx automatically has px(0)=0p_x(0)=0. The open right end requirescos⁡kL=0,km=(2m+1)π2L,fm=(2m+1)c4L.\cos kL=0,\quad k_m=\frac{(2m+1)\pi}{2L},\quad f_m=\frac{(2m+1)c}{4L}.

(b) Interpretation and further calculation

The open-open fundamental is 340/(2×0.85)=200Hz340/(2\times0.85)=200\,\mathrm{Hz}, giving 200,400,600Hz200,400,600\,\mathrm{Hz}. The closed-open fundamental is 100Hz100\,\mathrm{Hz}, giving 100,300,500Hz100,300,500\,\mathrm{Hz}. Its first overtone is 300Hz300\,\mathrm{Hz}, the third harmonic; overtone order counts allowed modes, not every integer multiple.

Physical check

The ideal closed-open tube lacks even harmonics. Pressure and displacement nodes exchange roles at either type of end.