Marine Acoustics: Direct and Inverse Problems

In this section we consider the acoustic imaging problem in a homogeneous, shallow-water wave guide. The shallow-water wave guide is denoted by
, where h is the depth of the ocean. Let ? be a bounded obstacle imbedded in the wave guide. The total acoustic field u from a point source x s = ( x s 1, x s 2) satisfies
u also satisfies the outgoing radiation condition
where x s 1 is the location of the acoustic source, k > 0 is the wavenumber, and u n is the nth normal propagation mode; i.e., if
then u has representation
On the boundary of ?, denoted by ??, u satisfies some unknown boundary condition of the Dirichlet, Neumann, and impedence types. We denote the boundary conditions as
We consider the total wave u as the combination of a prime field u i and a scattered field u s, u = u i + u s where u i is the Green's function for the parallel wave guide without any obstacle:
where
From (3.44) (3.47), we have
On ??, u s satisfies some unspecified boundary condition
where (3.55) may be data of the following types, namely Dirichlet:
Neumann:
Robin (impedence):
where ? > 0. We assume that ??