Paper 1, Section II, 39B

Waves
Part II, 2011

An inviscid fluid with sound speed c0c_{0} occupies the region 0<y<πα,0<z<πβ0<y<\pi \alpha, 0<z<\pi \beta enclosed by the rigid boundaries of a rectangular waveguide. Starting with the acoustic wave equation, find the dispersion relation ω(k)\omega(k) for the propagation of sound waves in the xx-direction.

Hence find the phase speed c(k)c(k) and the group velocity cg(k)c_{g}(k) of both the dispersive modes and the nondispersive mode, and sketch the form of the results for k,ω>0k, \omega>0.

Define the time and cross-sectional average appropriate for a mode with frequency ω\omega. For each dispersive mode, show that the average kinetic energy is equal to the average compressive energy.

A general multimode acoustic disturbance is created within the waveguide at t=0t=0 in a region around x=0x=0. Explain briefly how the amplitude of the disturbance varies with time as tt \rightarrow \infty at the moving position x=Vtx=V t for each of the cases 0<V<c00<V<c_{0}, V=c0V=c_{0} and V>c0V>c_{0}. [You may quote without proof any generic results from the method of stationary phase.]