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An experimental and numerical study of floating breakwaters

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TLDR
In this article, the effect of two different damping mechanisms of a floating breakwater was analyzed in 2D and three basic cross-sections of breakwaters were tested and analyzed in two-dimensional (2D) space.
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This article is published in Coastal Engineering.The article was published on 2018-07-01 and is currently open access. It has received 48 citations till now. The article focuses on the topics: Breakwater.

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Ship roll damping control

TL;DR: The technical feasibility of roll motion control devices has been amply demonstrated for over 100 years as mentioned in this paper, however, performance can still fall short of expectations due to fundamental performance limitations and large variations of the spectral characteristics of wave-induced roll motion.
Journal ArticleDOI

Review of developments in porous membranes and net-type structures for breakwaters and fish cages

TL;DR: In this paper, a literature review is presented on the theoretical, numerical, and experimental progress made in the application of porous membranes and net-type structures to breakwaters and fish cages.
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Numerical studies of submerged moored box-type floating breakwaters with different shapes of cross-sections using SPH

TL;DR: In this article, the wave-attenuation performances and hydrodynamics of moored box-type floating breakwaters with the same weight, same wall thickness, and six different cross-sections, i.e. circular, triangle-down, triangle up, rectangular, trapezoid-down and trapezoidal-up, are investigated numerically using the smoothed particle hydrodynamic (SPH) method.
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Numerical study of the interaction between peregrine breather based freak waves and twin-plate breakwater

TL;DR: In this paper, a 2D numerical wave tank is built in which the simulations are conducted using computational fluid dynamics (CFD) approach, while a strong-coupled fluid-structure interaction (FSI) algorithm is applied to consider the hydroelastic effects.
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Validation of a combined dynamic mesh strategy for the simulation of body's large amplitude motion in wave

TL;DR: A dynamic mesh strategy, which combines the sliding interface technique and the dynamic layering technique, was adopted to handle the mesh update due to the body motion in the simulation to simulate the flow field of the body-wave interaction.
References
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Journal ArticleDOI

Volume of fluid (VOF) method for the dynamics of free boundaries

TL;DR: In this paper, the concept of a fractional volume of fluid (VOF) has been used to approximate free boundaries in finite-difference numerical simulations, which is shown to be more flexible and efficient than other methods for treating complicated free boundary configurations.
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Sea Loads on Ships and Offshore Structures

TL;DR: In this paper, linear-wave induced motions and loads on floating structures were modeled as Second-order nonlinear problems. But the authors did not consider the effects of the wind and current on the floating structures.
Journal ArticleDOI

A wave generation toolbox for the open‐source CFD library: OpenFoam®

TL;DR: OpenFoam as discussed by the authors is a CFD library for solving free surface Newtonian flows using the Reynolds averaged Navier-Stokes equations coupled with a volume of fluid method.
Journal ArticleDOI

2-D numerical analysis of near-field flow at low-crested permeable breakwaters

TL;DR: In this article, Liu et al. proposed a numerical model named COrnell BReaking waves And Structures (COBRAS) based on the Reynolds Averaged Navier-Stokes (RANS) equations to simulate the most relevant hydrodynamic near field processes that take place in the interaction between waves and low-crested breakwaters.
Related Papers (5)
Frequently Asked Questions (11)
Q1. What are the contributions in this paper?

In this paper, Wang et al. used a 2DV elliptical model to study the hydrodynamic behavior of fixed and heave motion floating breakwaters. 

While the added viscous damping 696 removes energy from the motion response and, thus the waves radiated by the body motion, it has 697 no effect on the diffraction problem, i.e. the waves scattered by the fixed body. 

In the numerical set-up it was possible to include a linear external damping coefficient as a 494 supplement to the wave damping. 

In deep water, the appropriate measure of nonlinearity is the wave 265steepness, /S H L , which has a maximum value of max 14.2%S . 

Decay tests 403Traditionally, the damping force is divided into three types; structural, material and fluid 404 damping, see for instance (Sumer and Fredsøe, 2006). 

The damping ratio originating from viscous damping can be difficult to compare directly 514 between cross sections, as the restoring coefficients also changed between the cross sections, as a 515 consequence of the volume of porous media, and due to different non-linear processes. 

335 When adding the porous media to the sides of the FB, the reflection decreased significantly as the 336 porous media reduced the reflection coefficient from around 0.7 to around 0.3 for the largest wave 337frequencies. 

It is desirable to keep the nonlinearity of the waves generated in the flume at a uniform level over 264 the entire range of frequencies. 

The cross 754 section with porous sides (WP P100) showed significantly smaller reflection and transmission 755 coefficients for wave frequencies larger than 0.8 

The damping ratio, total ,was found from decay tests, 524WAMIT was the damping ratio estimated from the numerical modelling without introducing external 525damping. 

The case that 434 included porous sides (WP P100) had the largest damping ratio in heave, which might be related to 435 water filling and emptying the porous media.