Fully non‐linear free‐surface simulations by a 3D viscous numerical wave tank

A finite difference scheme using a modified marker-and-cell (MAC) method is applied to investigate the characteristics of non-linear wave motions and their interactions with a stationary three-dimensional body inside a numerical wave tank (NWT). The Navier-Stokes (NS) equation is solved for two fluid layers, and the boundary values are updated at each time step by a finite difference time marching scheme in the frame of a rectangular co-ordinate system. The viscous stresses and surface tension are neglected in the dynamic free-surface condition, and the fully non-linear kinematic free-surface condition is satisfied by the density function method developed for two fluid layers. The incident waves are generated from the inflow boundary by prescribing a velocity profile resembling flexible flap wavemaker motions, and the outgoing waves are numerically dissipated inside an artificial damping zone located at the end of the tank. The present NS-MAC NWT simulations for a vertical truncated circular cylinder inside a rectangular wave tank are compared with the experimental results of Mercier and Niedzwecki, an independently developed potential-based fully non-linear NWT, and the second-order diffraction computation

[1]  Hamm-Ching Chen,et al.  Time-Domain Simulation of a Berthing DDG-51 Ship By a Domain Decomposition Approach , 1997 .

[2]  J. Niedzwecki,et al.  EXPERIMENTAL MEASUREMENT OF SECOND-ORDER DIFFRACTION BY A TRUNCATED VERTICAL CYLINDER IN MONOCHROMATIC WAVES , 1994 .

[3]  C. W. Hirt,et al.  Improved free surface boundary conditions for numerical incompressible-flow calculations , 1971 .

[4]  J. N. Newman Second-harmonic wave diffraction at large depths , 1990, Journal of Fluid Mechanics.

[5]  Dick K. P. Yue,et al.  Numerical simulations of nonlinear axisymmetric flows with a free surface , 1987, Journal of Fluid Mechanics.

[6]  Moo-Hyun Kim,et al.  The complete second-order diffraction solution for an axisymmetric body Part 1. Monochromatic incident waves , 1989, Journal of Fluid Mechanics.

[7]  M. Longuet-Higgins A theory of the origin of microseisms , 1950, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[8]  M. S. Celebi,et al.  Fully Nonlinear 3-D Numerical Wave Tank Simulation , 1998 .

[9]  Robert F. Beck,et al.  Time-domain computations for floating bodies , 1994 .

[10]  R. Eatock Taylor,et al.  Finite element analysis of two-dimensional non-linear transient water waves , 1994 .

[11]  Michael Selwyn Longuet-Higgins,et al.  The deformation of steep surface waves on water - I. A numerical method of computation , 1976, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[12]  Keisuke Sawada,et al.  A numerical investigation on wing/nacelle interferences of USB configuration , 1987 .

[13]  Ming Zhu,et al.  On the accuracy of numerical wave making techniques , 1993 .

[14]  J. N. Newman,et al.  THE COMPUTATION OF SECOND-ORDER WAVE LOADS , 1991 .

[15]  Robert L. Street,et al.  A computer study of finite-amplitude water waves , 1970 .

[16]  A. Clément Coupling of Two Absorbing Boundary Conditions for 2D Time-Domain Simulations of Free Surface Gravity Waves , 1996 .

[17]  宮田 秀明,et al.  Numerical Study of Some Wave-Breaking Problems by a Finite-Difference Method , 1987 .

[18]  H. Miyata,et al.  A finite difference method for 3D flows about bodies of complex geometry in rectangular co-ordinate systems , 1992 .