Traveling Sound Waves — Question 5

Section 17-3 · Physics pages 2680–2681

Question 5 Equal pressure amplitudes can hide unequal displacement amplitudes Two separate progressive plane waves in the same fluid have equal pressure amplitude P = 1.0 Pa but frequencies f1 = 250 Hz and f2 = 1000 Hz. The fluid has Z = 400 Pa s/m and c = 320 m/s. f 250 1000 Separate equal-pressure tones; spectral heights are not displacement amplitudes. (a) Compare particle-velocity and displacement amplitudes, including numerical values. (b) Compare their strain amplitudes ka. Explain why the higher frequency does not make the compression amplitude larger here.
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Question 5 - Solution Equal pressure amplitudes can hide unequal displacement amplitudes f 250 1000 (a) Method and calculation For each wave, um = P/Z and a = um/(2πf). Therefore um1 = um2 = 0.00250 m/s, a1 = 1.592 µm, a2 = 0.3979 µm, a2/a1 = 1/4. (b) Interpretation and further calculation Since k = ω/c, ka = ω c P Zω = P Zc = 7.8125 × 10−6. Both waves have the same strain and density-perturbation amplitudes. Higher k is exactly offset by smaller a when pressure amplitude and medium are fixed. Physical check B = Zc = 128000 Pa, so ka = P/B is independently consistent with the compression law.

Question 5

Equal pressure amplitudes can hide unequal displacement amplitudes

Two separate progressive plane waves in the same fluid have equal pressure amplitude P=1.0PaP=1.0\,\mathrm{Pa} but frequencies f1=250Hzf_1=250\,\mathrm{Hz} and f2=1000Hzf_2=1000\,\mathrm{Hz}. The fluid has Z=400Pas/mZ=400\,\mathrm{Pa\,s/m} and c=320m/sc=320\,\mathrm{m/s}.

Diagram shown in the original SVG worksheet.

  1. Compare particle-velocity and displacement amplitudes, including numerical values.

  2. Compare their strain amplitudes kaka. Explain why the higher frequency does not make the compression amplitude larger here.

Question 5 - Solution

Equal pressure amplitudes can hide unequal displacement amplitudes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

For each wave, um=P/Zu_m=P/Z and a=um/(2πf)a=u_m/(2\pi f). Thereforeum1=um2=0.00250m/s,u_{m1}=u_{m2}=0.00250\,\mathrm{m/s},a1=1.592μm,a2=0.3979μm,a2/a1=1/4.a_1=1.592\,\mu\mathrm m,\qquad a_2=0.3979\,\mu\mathrm m,\qquad a_2/a_1=1/4.

(b) Interpretation and further calculation

Since k=ω/ck=\omega/c,ka=ωcPZω=PZc=7.8125×10−6.ka=\frac{\omega}{c}\frac{P}{Z\omega}=\frac{P}{Zc}=7.8125\times10^{-6}.Both waves have the same strain and density-perturbation amplitudes. Higher kk is exactly offset by smaller aa when pressure amplitude and medium are fixed.

Physical check

B=Zc=128000PaB=Zc=128000\,\mathrm{Pa}, so ka=P/Bka=P/B is independently consistent with the compression law.