Sound Waves — Question 9

Section 17-1 · Physics pages 2648–2649

Question 9 Diffraction distinguishes acoustic wavelengths at one opening A wall opening has width D = 0.50 m. Compare tones at 170 Hz and 3400 Hz in air with c = 340 m/s. Use the qualitative diffraction criterion: spreading is strong when D/λ ≲1 and weak when D/λ ≫1. D Opening and possible outgoing directions; not a quantitative radiation pattern. (a) Calculate the two wavelength-to-opening comparisons and identify which tone spreads more strongly. (b) For the high-frequency tone, use the supplied far-field slit relation sin θ1 = λ/D to locate the first minimum. Why does this formula yield no first minimum for the lower tone?
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Question 9 - Solution Diffraction distinguishes acoustic wavelengths at one opening D (a) Method and calculation The wavelengths are λlow = 340/170 = 2.00 m, λhigh = 340/3400 = 0.100 m. D/λlow = 0.25, D/λhigh = 5.0. The lower tone spreads broadly; the higher tone has a narrower forward pattern. (b) Interpretation and further calculation For the high tone, θ1 = sin−1(0.100/0.50) = 11.54◦. For the low tone, the equation would require sin θ1 = 4, which is impossible. It predicts no first zero within the forward angular range, consistent with broad spreading. The slit formula assumes a uniformly driven aperture and far-field observation. Physical check The relevant comparison is D/λ, so changing medium speed at fixed frequency also changes diffraction.

Question 9

Diffraction distinguishes acoustic wavelengths at one opening

A wall opening has width D=0.50mD=0.50\,\mathrm m. Compare tones at 170Hz170\,\mathrm{Hz} and 3400Hz3400\,\mathrm{Hz} in air with c=340m/sc=340\,\mathrm{m/s}. Use the qualitative diffraction criterion: spreading is strong when D/λ≲1D/\lambda\lesssim1 and weak when D/λ≫1D/\lambda\gg1.

Diagram shown in the original SVG worksheet.

  1. Calculate the two wavelength-to-opening comparisons and identify which tone spreads more strongly.

  2. For the high-frequency tone, use the supplied far-field slit relation sin⁡θ1=λ/D\sin\theta_1=\lambda/D to locate the first minimum. Why does this formula yield no first minimum for the lower tone?

Question 9 - Solution

Diffraction distinguishes acoustic wavelengths at one opening

Diagram shown in the original SVG worksheet.

(a) Method and calculation

The wavelengths areλlow=340/170=2.00m,λhigh=340/3400=0.100m.\lambda_{\mathrm{low}}=340/170=2.00\,\mathrm m,\qquad\lambda_{\mathrm{high}}=340/3400=0.100\,\mathrm m.D/λlow=0.25,D/λhigh=5.0.D/\lambda_{\mathrm{low}}=0.25,\qquad D/\lambda_{\mathrm{high}}=5.0.The lower tone spreads broadly; the higher tone has a narrower forward pattern.

(b) Interpretation and further calculation

For the high tone,θ1=sin⁡−1(0.100/0.50)=11.54∘.\theta_1=\sin^{-1}(0.100/0.50)=11.54^\circ.For the low tone, the equation would require sin⁡θ1=4\sin\theta_1=4, which is impossible. It predicts no first zero within the forward angular range, consistent with broad spreading. The slit formula assumes a uniformly driven aperture and far-field observation.

Physical check

The relevant comparison is D/λD/\lambda, so changing medium speed at fixed frequency also changes diffraction.