Two situations bend waves by a gradient in speed.

PHYSICS · Multi-part · Fermi University Physics · Fluids & Continuum Physics · Waves, acoustics and compressible flow · Waves, acoustics and compressible flow

Signal Speeds in Fluids, Ch Sound in a moving, absorbing fluid: sources, refraction and loss

Problem

Two situations bend waves by a gradient in speed. ((a)) A tsunami of period 15 min15\,\mathrm{min} crosses depth contours that run parallel to a straight coast. In water of depth h1=50 mh_1 = 50\,\mathrm{m} its crests make an angle θ1=40∘\theta_1 = 40^\circ with the depth contours. Using the shallow-water wave speed c=ghc=\sqrt{gh} and Snell's law sin⁡θ/c=const\sin\theta/c = \text{const} along the ray, find the angle θ2\theta_2 the crests make with the depth contours in water of depth h2=8 mh_2 = 8\,\mathrm{m}. ((b)) A steady wind blows over flat ground with speed increasing linearly with height at the rate dU/dz=0.15 s−1\mathrm{d}U/\mathrm{d}z = 0.15\,\mathrm{s^{-1}}, while the sound speed c0=343 m s−1c_0 = 343\,\mathrm{m\,s^{-1}} is uniform with height. A source and a listener each stand at height 2 m2\,\mathrm{m} above the ground, the listener directly upwind of the source. Find the radius of curvature RR of a nearly horizontal ray travelling upwind, and the distance beyond which the listener lies in the acoustic shadow.

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