Published online by Cambridge University Press: 17 July 2009
We consider the solution in the time domain of water-wave scattering by arrays of bottom-mounted cylinders. It has already been shown that near trapping occurs for certain arrangements of cylinders and we are especially focused on this phenomenon. We begin with the well-known single-frequency solution to the problem of a group of cylinders, and the extension of this solution to complex frequencies. It has been shown that singularities (scattering frequencies or resonances) occur for certain values of the complex frequency and these singularities are associated with the near-trapped mode. We show that it is possible to approximate the solution near these singularities, and produce a modal shape which is associated with the near-trapped mode. We then consider the time-dependent problem, beginning with the well-known incident plane wave packet solution. We also show how the problem of an arbitrary initial displacement can be found using the single-frequency solutions. This latter result relies on a special inner product which gives a generalized eigenfunction expansion (because the operator has a continuous spectrum). We then consider the approximation of the time-dependent motion using special mode shapes associated with the scattering frequencies. This approximation relies on the scattering frequencies lying close to the real axis. We present numerical results which show that this approximation is accurate for sufficiently large time.
Movie 1. The near trapped mode for four cylinders associated with the scattering frequency at 2.7641 - 0.0122i.
Movie 2. The near trapped mode for nine cylinders associated with the scattering frequency at 2.7114 - 0.0041i
Movie 3. One of the near trapped modes for nine cylinders associated with the scattering frequency at 2.7635 - 0.0086i
Movie 4. One of the near trapped modes for nine cylinders associated with the scattering frequency at 2.7635 - 0.0086i
Movie 5. The near trapped mode for nine cylinders associated with the scattering frequency at 2.8284 - 0.0102i
Movie 6. The true (a) and approximate (b) solution for four cylinders for a plane incident wave given by equation (4.7).
Movie 7. The true (a) and approximate (b) solution for nine cylinders for a plane incident wave given by equation (4.7).
Movie 8. The true (a) and approximate (b) solution for four cylinders for a plane incident wave given by equation (4.8). We do not start the approximate solution until t=0.