Traveling Sound Waves — Question 7

Section 17-3 · Physics pages 2684–2685

Question 7 A pressure reflection coefficient differs from a velocity coefficient A normally incident plane sound wave crosses a stationary fluid interface. The impedances are Z1 = 400 and Z2 = 1200 Pa s/m. Incident, reflected and transmitted signed pressure amplitudes are Pi, Pr, Pt. Pressure and normal velocity are continuous. Z1 Z2 Propagation path; the stated distances determine travel time. (a) Derive Pr/Pi and Pt/Pi. (b) For Pi = 1.0 Pa, find the interface velocity on both sides and explain how Pt > Pi is possible.
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Question 7 - Solution A pressure reflection coefficient differs from a velocity coefficient Z1 Z2 (a) Method and calculation At the interface, Pi + Pr = Pt, Pi −Pr Z1 = Pt Z2 . Solving, rp = Z2 −Z1 Z2 + Z1 = 1 2, tp = 2Z2 Z1 + Z2 = 3 2. The minus sign for reflected velocity is essential. (b) Interpretation and further calculation The total normal velocities agree: u1 = 1 −0.5 400 = 0.00125 m/s, u2 = 1.5 1200 = 0.00125 m/s. Pressure amplitude alone is not an energy fraction. The higher-impedance transmitted medium has a smaller velocity for a given pressure; continuity allows a transmitted pressure larger than the incident pressure. Physical check When Z1 = Z2, rp = 0 and tp = 1. The interface then has no reflected plane wave in this ideal model.

Question 7

A pressure reflection coefficient differs from a velocity coefficient

A normally incident plane sound wave crosses a stationary fluid interface. The impedances are Z1=400Z_1=400 and Z2=1200Pas/mZ_2=1200\,\mathrm{Pa\,s/m}. Incident, reflected and transmitted signed pressure amplitudes are Pi,Pr,PtP_i,P_r,P_t. Pressure and normal velocity are continuous.

Diagram shown in the original SVG worksheet.

  1. Derive Pr/PiP_r/P_i and Pt/PiP_t/P_i.

  2. For Pi=1.0PaP_i=1.0\,\mathrm{Pa}, find the interface velocity on both sides and explain how Pt>PiP_t>P_i is possible.

Question 7 - Solution

A pressure reflection coefficient differs from a velocity coefficient

Diagram shown in the original SVG worksheet.

(a) Method and calculation

At the interface,Pi+Pr=Pt,Pi−PrZ1=PtZ2.P_i+P_r=P_t,\qquad\frac{P_i-P_r}{Z_1}=\frac{P_t}{Z_2}.Solving,rp=Z2−Z1Z2+Z1=12,tp=2Z2Z1+Z2=32.r_p=\frac{Z_2-Z_1}{Z_2+Z_1}=\frac12,\qquad t_p=\frac{2Z_2}{Z_1+Z_2}=\frac32.The minus sign for reflected velocity is essential.

(b) Interpretation and further calculation

The total normal velocities agree:u1=1−0.5400=0.00125m/s,u2=1.51200=0.00125m/s.u_1=\frac{1-0.5}{400}=0.00125\,\mathrm{m/s},\quad u_2=\frac{1.5}{1200}=0.00125\,\mathrm{m/s}.Pressure amplitude alone is not an energy fraction. The higher-impedance transmitted medium has a smaller velocity for a given pressure; continuity allows a transmitted pressure larger than the incident pressure.

Physical check

When Z1=Z2Z_1=Z_2, rp=0r_p=0 and tp=1t_p=1. The interface then has no reflected plane wave in this ideal model.