Fluid–structure interaction between a two-dimensional mat-type VLFS and solitary waves by the Green–Naghdi theory

The two-dimensional, nonlinear hydroelasticity of a mat-type very large floating structure (VLFS) is studied within the scope of linear beam theory for the structure and the nonlinear, Level I Green–Naghdi (GN) theory for the fluid. The beam equation and the GN equations are coupled through the kine...

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Veröffentlicht in:Journal of fluids and structures 2008-05, Vol.24 (4), p.527-540
Hauptverfasser: Xia, D., Ertekin, R.C., Kim, J.W.
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Kim, J.W.
description The two-dimensional, nonlinear hydroelasticity of a mat-type very large floating structure (VLFS) is studied within the scope of linear beam theory for the structure and the nonlinear, Level I Green–Naghdi (GN) theory for the fluid. The beam equation and the GN equations are coupled through the kinematic and dynamic boundary conditions to obtain a new set of modified GN equations. These equations represent long-wave motion beneath an elastic plate. A set of jump conditions that are necessary for the continuity (or the matching) of the solutions in the open water region and that under the structure is derived through the use of the postulated conservation laws of mass, momentum, and mechanical energy. The resulting governing equations, subjected to the boundary and jump conditions, are solved by the finite-difference method in the time domain. The present model is applicable, for example, to the study of the hydroelastic response of a mat-type VLFS under the action of a solitary wave, or a frontal tsunami wave. Good agreement is observed between the model results and other published theoretical and numerical predictions, as well as experimental data. The results show that consideration of nonlinearity is important for accurate predictions of the bending moment of the floating elastic plate. It is found that the rigidity of the structure greatly affects the bending moment and displacement of the structure in this nonlinear theory.
doi_str_mv 10.1016/j.jfluidstructs.2007.10.009
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The beam equation and the GN equations are coupled through the kinematic and dynamic boundary conditions to obtain a new set of modified GN equations. These equations represent long-wave motion beneath an elastic plate. A set of jump conditions that are necessary for the continuity (or the matching) of the solutions in the open water region and that under the structure is derived through the use of the postulated conservation laws of mass, momentum, and mechanical energy. The resulting governing equations, subjected to the boundary and jump conditions, are solved by the finite-difference method in the time domain. The present model is applicable, for example, to the study of the hydroelastic response of a mat-type VLFS under the action of a solitary wave, or a frontal tsunami wave. Good agreement is observed between the model results and other published theoretical and numerical predictions, as well as experimental data. 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subjects Applied sciences
Beams (radiation)
Bending moment
Bending moments
Buildings. Public works
Classical transport
Elastic plates
Exact sciences and technology
Floating structures
Fluid dynamics
Fundamental areas of phenomenology (including applications)
General theory
Green–Naghdi equations
Hydraulic constructions
Hydroelasticity
Mat-type VLFS
Mathematical analysis
Mathematical models
Nonlinear shallow-water waves
Nonlinearity
Offshore structure (platforms, tanks, etc.)
Physics
Solid mechanics
Solitary waves
Statistical physics, thermodynamics, and nonlinear dynamical systems
Structural and continuum mechanics
Transport processes
Vibration, mechanical wave, dynamic stability (aeroelasticity, vibration control...)
VLF
title Fluid–structure interaction between a two-dimensional mat-type VLFS and solitary waves by the Green–Naghdi theory
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