Traveling Sound Waves — Question 8

Section 17-3 · Physics pages 2686–2687

Question 8 A rigid end doubles pressure while stopping normal motion A rightward incident pressure wave is pi = P cos(kx −ωt) in x < 0. A rigid wall at x = 0 imposes total normal particle velocity u(0, t) = 0. The medium has impedance Z. S, R wall Plane wave and rigid termination; the incident and reflected paths overlap physically. (a) Find the reflected wave and the combined pressure and velocity fields. (b) Locate the nearest pressure node and velocity antinode to the wall. Is p = Zu valid for the combined field?
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Question 8 - Solution A rigid end doubles pressure while stopping normal motion S, R wall (a) Method and calculation The reflected pressure must be pr = P cos(kx + ωt) because its velocity has the opposite impedance sign. Adding gives p = 2P cos kx cos ωt, u = P Z [cos(kx −ωt) −cos(kx + ωt)] = 2P Z sin kx sin ωt. At x = 0, pressure amplitude is 2P and velocity is zero. (b) Interpretation and further calculation The nearest pressure node is at x = −π/(2k) = −λ/4, also a velocity antinode. The relation p = Zu describes one rightward progressive component, not this standing superposition. Indeed, the wall has nonzero pressure even though its normal velocity vanishes. Physical check At the wall the instantaneous power per area pu is zero, consistent with a stationary rigid boundary doing no work.

Question 8

A rigid end doubles pressure while stopping normal motion

A rightward incident pressure wave is pi=Pcos⁡(kx−ωt)p_i=P\cos(kx-\omega t) in x<0x<0. A rigid wall at x=0x=0 imposes total normal particle velocity u(0,t)=0u(0,t)=0. The medium has impedance ZZ.

Diagram shown in the original SVG worksheet.

  1. Find the reflected wave and the combined pressure and velocity fields.

  2. Locate the nearest pressure node and velocity antinode to the wall. Is p=Zup=Zu valid for the combined field?

Question 8 - Solution

A rigid end doubles pressure while stopping normal motion

Diagram shown in the original SVG worksheet.

(a) Method and calculation

The reflected pressure must be pr=Pcos⁡(kx+ωt)p_r=P\cos(kx+\omega t) because its velocity has the opposite impedance sign. Adding givesp=2Pcos⁡kxcos⁡ωt,p=2P\cos kx\cos\omega t,u=PZ[cos⁡(kx−ωt)−cos⁡(kx+ωt)]=2PZsin⁡kxsin⁡ωt.u=\frac PZ[\cos(kx-\omega t)-\cos(kx+\omega t)]=\frac{2P}{Z}\sin kx\sin\omega t.At x=0x=0, pressure amplitude is 2P2P and velocity is zero.

(b) Interpretation and further calculation

The nearest pressure node is at x=−π/(2k)=−λ/4x=-\pi/(2k)=-\lambda/4, also a velocity antinode. The relation p=Zup=Zu describes one rightward progressive component, not this standing superposition. Indeed, the wall has nonzero pressure even though its normal velocity vanishes.

Physical check

At the wall the instantaneous power per area pupu is zero, consistent with a stationary rigid boundary doing no work.