Generalized Eigenfunction Expansion for Water Waves for a Fixed Body

From WikiWaves
Revision as of 05:02, 18 April 2006 by Meylan (talk | contribs) (Started the page)
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)
Jump to navigationJump to search

This page is under construction.


The theory of generalised eigenfunction is described in Hazard and Lenoir 2002 and Meylan 2002 for the case of a rigid body in water of infinite depth and for a thin plate on water of shallow draft respectively. We will present here the theory for a rigid body in water of finite depth.

Outline of the theory

We consider the case of a rigid body in water of finite depth. We can solve the single frequency problem with frequency [math]\displaystyle{ \omega }[/math] for an incident wave travelling from [math]\displaystyle{ -\infty }[/math]

[math]\displaystyle{ \phi^i = e^{i \omega x} }[/math]

to obtain a solution [math]\displaystyle{ \phi(\omega,x) }[/math]. This looks like an incident plus reflected wave as [math]\displaystyle{ x\to\-infty }[/math] and like a transmitted