3.2. Wave Number Integration or Spectral Methods
The solution of the basic equations of motion (3.3) is greatly simplified when the medium parameters are independent of the horizontal spatial coordinates x and y. Such a laterally homogeneous, or range-invariant, medium is now assumed. The symmetric point source with f(x, t) = −M grad(δ(x − xs)) exp(−iωt) and ω > 0 is stipulated, with xs = (0, 0, zs) in the water. Introducing a cylindrical coordinate system (r, ϕ, z) with r = (x2 + y2)1/2 (for radius) and ϕ (for azimuth) in the horizontal plane, and corresponding basis vectors er, eϕ, ez, the wave field is independent of ϕ. Omitting the time-harmonic factor exp(−iωt), as usual, the displacement vector u and the traction vector at horizontal planes ...
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