Hydroelastic and hydrodynamic analysis of a uniform rigid and flexible barge using weakly compressible smoothed particle hydrodynamics (WCSPH)
During fluid-structure interaction (FSI) fluid forces acting on the structure result in the structure moving and deforming, which in turn affects the flow boundary conditions, hence fluid motion. This interaction, also known as two-way coupling, has been studied in marine, offshore and coastal en...
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Format: | Conference or Workshop Item |
Language: | English English |
Published: |
2018
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Online Access: | http://irep.iium.edu.my/65850/8/65850%20WCSPH.pdf http://irep.iium.edu.my/65850/9/65850%20abstract.pdf http://irep.iium.edu.my/65850/ https://umconference.um.edu.my/upload/2-16/Publish_Abstract%20Book%20IRIISE%202018.pdf |
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Institution: | Universiti Islam Antarabangsa Malaysia |
Language: | English English |
Summary: | During fluid-structure interaction (FSI) fluid forces acting on the structure result in the structure
moving and deforming, which in turn affects the flow boundary conditions, hence fluid motion.
This interaction, also known as two-way coupling, has been studied in marine, offshore and coastal
engineering. The majority of approaches used are based on potential flow where nonlinear effects
are either ignored or allowed for through various assumptions on the body and free surface
boundary conditions, leading to a range of partly to fully nonlinear methods. However, numerical
models based on potential flow theory are unable to deal with extreme free surface deformations,
as well as FSI problems where the effects of viscosity, turbulence and compressibility are
significant. In order to address such shortcomings, there have been several attempts to solve
nonlinear rigid body FSI and benefitting from rapid progress in Reynolds-averaged Navier-Stokes
(RANS) code development, using either the finite difference method (FDM) or the finite volume
method (FVM). However, most of these methods are Eulerian and, by and large, ineffective in the
case of extreme events of wave breaking and water spray. Therefore, Lagrangian meshless
methods are viewed as alternatives in providing accurate numerical solutions to improve
inadequacy of mesh-based discretization.
Smoothed Particle Hydrodynamics (SPH) is a mesh-free, Lagrangian method whereby the
computational domain is represented by a set of interpolation points called particles where the
fluid medium is discretised by the interaction between particles rather than grid cells. Each particle
carries an individual mass, velocity, position and any other requisite physical characteristics, which
evolve over time through the governing equations. All particles have a kernel function to define
their range of interaction, while the hydrodynamic variables are defined by integral
approximations.
The current works presented are the first step in extending the application of WCSPH (weakly
compressible SPH) to simulate two-way coupling in FSI. Numerical predictions for such
interactions involving rigid and elastic body could provide useful knowledge in the possibility of
implementing particle method in FSI. In the first part, WCSPH is applied to simulate rigid body
motion of barge in regular waves. Vertical displacements of barge under different wave conditions
are calculated and their Response Amplitude Operators (RAOs) and vertical bending moments
(VBMs) are determined. Results are then compared to experimental data and 2 other numerical
data.
Secondly, forced oscillation tests are performed on a uniform flexible barge using WCSPH for
the 3D radiation problem. Hydrodynamic coefficients, namely added mass and damping
coefficients, are obtained for the rigid body motions of heave and pitch, and the 2-node (2VB) and
3-node (3VB) symmetric distortion mode shapes, including coupling terms. These are compared
with potential flow (using 3D hydroelasticity) and RANS (using STAR-CCM+) predictions.
Domain size, particle numbers and damping zones are modified based on different frequencies of
oscillation, allowing the free surface to be well captured by WCSPH. |
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