Sources of Musical Sound — Question 4

Section 17-6 · Physics pages 2738–2739

Question 4 Thermal tuning and length tuning act through different factors An ideal pipe has fundamental 440 Hz at 293 K. At fixed composition, c ∝ √ T. Neglect the thermal expansion of the pipe. It warms uniformly to 303 K. L open open Ideal straight tube; end corrections are stated when used. (a) Find the new fundamental frequency. (b) By what factor must its effective length change to restore 440 Hz at the new temperature? For an original effective length 0.390 m, find the extension.
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Question 4 - Solution Thermal tuning and length tuning act through different factors L open open (a) Method and calculation For a fixed boundary type, f ∝c/L. With unchanged length, f2 f1 = √303 293 = 1.016922, f2 = 447.446 Hz. The pipe becomes sharper because the sound speed increases. (b) Interpretation and further calculation To keep frequency constant, L2/L1 = c2/c1, hence ∆L = L1 (√ 303/293 −1 ) = 0.00660 m. The pipe must lengthen by about 6.60 mm. Shortening would raise the pitch further instead of compensating for warming. Physical check The length correction is about 1.69%, approximately half the fractional absolute-temperature change for this small temperature interval.

Question 4

Thermal tuning and length tuning act through different factors

An ideal pipe has fundamental 440Hz440\,\mathrm{Hz} at 293K293\,\mathrm K. At fixed composition, c∝Tc\propto\sqrt T. Neglect the thermal expansion of the pipe. It warms uniformly to 303K303\,\mathrm K.

Diagram shown in the original SVG worksheet.

  1. Find the new fundamental frequency.

  2. By what factor must its effective length change to restore 440Hz440\,\mathrm{Hz} at the new temperature? For an original effective length 0.390m0.390\,\mathrm m, find the extension.

Question 4 - Solution

Thermal tuning and length tuning act through different factors

Diagram shown in the original SVG worksheet.

(a) Method and calculation

For a fixed boundary type, f∝c/Lf\propto c/L. With unchanged length,f2f1=303293=1.016922,f2=447.446Hz.\frac{f_2}{f_1}=\sqrt{\frac{303}{293}}=1.016922,\qquad f_2=447.446\,\mathrm{Hz}.The pipe becomes sharper because the sound speed increases.

(b) Interpretation and further calculation

To keep frequency constant, L2/L1=c2/c1L_2/L_1=c_2/c_1, henceΔL=L1(303/293−1)=0.00660m.\Delta L=L_1\left(\sqrt{303/293}-1\right)=0.00660\,\mathrm m.The pipe must lengthen by about 6.60mm6.60\,\mathrm{mm}. Shortening would raise the pitch further instead of compensating for warming.

Physical check

The length correction is about 1.69%1.69\%, approximately half the fractional absolute-temperature change for this small temperature interval.