Sources of Musical Sound — Question 3

Section 17-6 · Physics pages 2736–2737

Question 3 End corrections prevent an exact octave after closing one end A tube has physical length L = 0.500 m and radius r = 0.010 m. Use an end correction e = 0.60r for each open end and zero correction at a rigid closure. Take c = 340 m/s. L open open Open tube; pressure nodes lie slightly beyond the physical ends in the supplied correction model. (a) Find the fundamental when both ends are open and when one end is closed. (b) Find their frequency ratio and compare with the ideal ratio of two. Explain the direction of the discrepancy.
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Question 3 - Solution End corrections prevent an exact octave after closing one end L open open (a) Method and calculation The effective lengths are Loo = L + 2e = 0.512 m and Lco = L + e = 0.506 m. Therefore foo = 340 2(0.512) = 332.031 Hz, fco = 340 4(0.506) = 167.984 Hz. (b) Interpretation and further calculation The ratio is foo fco = 2(L + e) L + 2e = 1.97656 < 2. Closing one end removes one end correction as well as changing the boundary condition. The closed-open effective length is slightly shorter, making its fundamental slightly higher than exactly half the open-open frequency. Physical check As e/L →0, the ratio approaches two. The correction coefficient is supplied rather than treated as universal for every opening geometry.

Question 3

End corrections prevent an exact octave after closing one end

A tube has physical length L=0.500mL=0.500\,\mathrm m and radius r=0.010mr=0.010\,\mathrm m. Use an end correction e=0.60re=0.60r for each open end and zero correction at a rigid closure. Take c=340m/sc=340\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Find the fundamental when both ends are open and when one end is closed.

  2. Find their frequency ratio and compare with the ideal ratio of two. Explain the direction of the discrepancy.

Question 3 - Solution

End corrections prevent an exact octave after closing one end

Diagram shown in the original SVG worksheet.

(a) Method and calculation

The effective lengths are Loo=L+2e=0.512mL_{oo}=L+2e=0.512\,\mathrm m and Lco=L+e=0.506mL_{co}=L+e=0.506\,\mathrm m. Thereforefoo=3402(0.512)=332.031Hz,fco=3404(0.506)=167.984Hz.f_{oo}=\frac{340}{2(0.512)}=332.031\,\mathrm{Hz},\qquad f_{co}=\frac{340}{4(0.506)}=167.984\,\mathrm{Hz}.

(b) Interpretation and further calculation

The ratio isfoofco=2(L+e)L+2e=1.97656<2.\frac{f_{oo}}{f_{co}}=\frac{2(L+e)}{L+2e}=1.97656<2.Closing one end removes one end correction as well as changing the boundary condition. The closed-open effective length is slightly shorter, making its fundamental slightly higher than exactly half the open-open frequency.

Physical check

As e/L→0e/L\to0, the ratio approaches two. The correction coefficient is supplied rather than treated as universal for every opening geometry.