A swell of period and deep-water height approaches a coast whose depth contours are…

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

Signal Speeds in Fluids, Ch Waves of finite height: Stokes waves, shoaling and breaking

Problem

A swell of period T=10 sT=10\,\mathrm{s} and deep-water height H0=1.5 mH_0=1.5\,\mathrm{m} approaches a coast whose depth contours are straight and parallel. In deep water its rays make θ0=40∘\theta_0=40^\circ with the normal to the contours. Take the bottom as slowly varying, with no reflection. ((a)) At h=5.0 mh=5.0\,\mathrm{m}, find the ray angle θ\theta, the coefficients KsK_{\rm s} and KrK_{\rm r}, and the wave height HH. ((b)) Find, by bisection, the depth hbh_{\rm b} at which KsKrH0=0.78hK_{\rm s}K_{\rm r}H_0=0.78h, and compare it with the breaking depth of the same swell arriving straight onshore. ((c)) At h=5.0 mh=5.0\,\mathrm{m}, compare the finite-depth second harmonic, 14ka2cosh⁡kh (2+cosh⁡2kh)/sinh⁡3kh\tfrac14ka^2\cosh kh\,(2+\cosh2kh)/\sinh^3kh with a=H/2a=H/2, with the first harmonic aa. Can the Stokes expansion be trusted there, and what does that say about the depth found in part (b)?

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