The purpose of this numerical simulation is to validate the Six-Degree-of-Freedom (6-DoF) solver with a case of “Free heave motion of a floating cylinder”. The main objective was to achieve the following:
Transient heave decay response after initial displacement.
The numerical simulation type was a Transient, multiphase with laminar flow and a dynamic mesh 6-DoF free body motion. The numerical simulation results of SimScale were compared to the experimental and theoretical results as shown in  and .
The geometry of the study is a 2D straight cylindrical body in a water tank (see Fig.1.). The details of the cylinder and tank dimensions are provided by the table below.
0.1524 m(6 inch)
20 m(65.5 feet)
2.4384 m(8 feet)
The flow domain is the Tank with the cylinder body. For a 2D analysis, it was required to have 1 cell in the width (Z-dir) dimension (see Fig.2.). A 2D structured hexahedral mesh was created with the open source ‘BlockMesh’.
The grid nodes are distributed by a geometric grading in the vicinity of the cylinder. Further, the nodes are clustered near the water line to better resolve the water-air interface. This was critical to achieve the accurate equilibrium floating level and base value of the free heave motion.
The complete details of the mesh are listed in the following table:
Mesh and Element types :
Number of nodes
Number of cells
The numerical analysis performed is detailed as follows:
Tool Type : OPENFOAM®
Analysis Type : Transient Multi-Phase Flow (incompressible)
Turbulence model : Laminar
Advanced Concepts : Six-Degree of Freedom
Air: – Kinematic viscosity(ν
– Density (ρ
Water: – Kinematic viscosity(ν
– Density (ρ
Surface tension =0.07kg.s−2
In the experiments , the cylinder is initially displaced by 1 inch below the water level (with initial level of half immersed cylinder) and then released to move freely in the heave direction only. To replicate the same effect, the initial water depth taken for the numerical simulation was a baseline value of 1.2192 m for a half immersed body ( or 4 ft as was in the experiment ) plus a water level increment of 0.0254 m (1 inch) at the start of the simulation. This initialized the flow domain (water level) similar to the experimental setup.
The water tank surfaces were taken as frictionless walls. The cylinder surfaces were taken as viscous No-slip walls. The top surface was defined as an open-boundary. The following table provides the further details.
Body Motion: 6 Degree of freedom
The 6-DoF model constraints applied are given by table below:
Center of rotation
plane normal (0,0,1)
The mass of the cylinder body is such that at equilibrium exactly a half-immersed body is achieved.
The numerical simulation results of ‘Transient heave decay response’ are compared with experimental data provided by Soichi Ito  and theoretical data by Maskell and Ursell . Similar to the experiment , the numerical setup constrains the rotation of the cylinder and allows only a pure heave motion (1 DOF) for the 2D case. A ‘Mesh independence’ study was done with 3 meshes, coarse, moderate and fine to see the effects on the results. Moreover, a 2D case was analysed using 3 degrees of freedom with free translation in 2 directions and rotation about 1 axis. The result comparison between the 1 DOF and 3 DOF case is also presented.
Firstly, a comparison of the Heave response from different meshes is given in Fig.3. The figure shows that with the coarse mesh, the baseline heave displacement deviates a lot from the zero line. The moderate mesh also has minor deviations, while the fine mesh attains the best oscillation behaviour about the baseline due to high resolution of the Water-Air interface.
The comparison of numerical simulation (fine mesh) with theoretical and experimental data is presented by the Fig. 4 below.
The comparison of the numerical simulation results of 1 DOF (as in experiment) and 3 DOF cases is given in Fig. 5 below.
A visualization of the phase fraction and motion of the body at different times is shown by Fig.6A and Fig.6B.
Fig.6. Phase fraction and motion of body at different times.
(1, 2, 3, 4) Soichi Ito, STUDY OF THE TRANSIENT HEAVE OSCILLATION OF A FLOATING CYLINDER, MASSACHUSETTS INSTITUTE OF TECHNOLOGY May, 1977
Maskell, S. J., and Ursell, F., “The transient motion of a floating body,” J. Fluid Mech., 44, pp. 303-313, 1970.
This offering is not approved or endorsed by OpenCFD Limited, producer and distributor of the OpenFOAM software and owner of the OPENFOAM® and OpenCFD® trade marks. OPENFOAM® is a registered trade mark of OpenCFD Limited, producer and distributor of the OpenFOAM software.
Last updated: January 29th, 2019
Did you find this article helpful?
How can we do better?
We appreciate and value your feedback.
Strictly Necessary Cookies
Strictly Necessary Cookie should be enabled at all times so that we can save your preferences for cookie settings.
If you disable this cookie, we will not be able to save your preferences. This means that every time you visit this website you will need to enable or disable cookies again.