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Strongly coupled partitioned six degree-of-freedom rigid body motion solver with Aitken's dynamic under-relaxation

  • Chow, Jeng Hei (DHI Water & Environment (S) Pte Ltd.) ;
  • Ng, E.Y.K. (School of Mechanical and Aerospace Engineering, Nanyang Technological University)
  • Received : 2016.04.11
  • Accepted : 2016.04.14
  • Published : 2016.07.30

Abstract

An implicit method of solving the six degree-of-freedom rigid body motion equations based on the second order Adams-Bashforth-Moulten method was utilised as an improvement over the leapfrog scheme by making modifications to the rigid body motion solver libraries directly. The implementation will depend on predictor-corrector steps still residing within the hybrid Pressure Implicit with Splitting of Operators - Semi-Implicit Method for Pressure Linked Equations (PIMPLE) outer corrector loops to ensure strong coupling between fluid and motion. Aitken's under-relaxation is also introduced in this study to optimise the convergence rate and stability of the coupled solver. The resulting coupled solver ran on a free floating object tutorial test case when converged matches the original solver. It further allows a varying 70%-80% reduction in simulation times compared using a fixed under-relaxation to achieve the required stability.

Keywords

References

  1. Aitken, A.C., 1927. Xxv.-on bernoulli's numerical solution of algebraic equations. Proc. R. Soc. Edinb. 46, 289-305. https://doi.org/10.1017/S0370164600022070
  2. Causin, P., Gerbeau, J.F., Nobile, F., 2005. Added-mass effect in the design of partitioned algorithms for fluid-structure problems. Comput. Methods Appl. Mech. Eng. 194 (42-44), 4506-4527. https://doi.org/10.1016/j.cma.2004.12.005
  3. Foerster, C., Wall, W.A., Ramm, E., 2007. Artificial added mass instabilities in sequential staggered coupling of nonlinear structures and incompressible viscous flows. Comput. Methods Appl. Mech. Eng. 196 (7), 1278-1293. https://doi.org/10.1016/j.cma.2006.09.002
  4. Gopala, V.R., van Wachem, B.G.M., 2008. Volume of fluid methods for immiscible-fluid and free-surface flows. Chem. Eng. J. 141 (1-3), 204-221. https://doi.org/10.1016/j.cej.2007.12.035
  5. Higuera, P., Lara, J.L., Losada, I.J., 2013a. Realistic wave generation and active wave absorption for navier-stokes models: application to openfoam$^{(R)}$. Coast. Eng. 71, 102-118. https://doi.org/10.1016/j.coastaleng.2012.07.002
  6. Higuera, P., Lara, J.L., Losada, I.J., 2013b. Simulating coastal engineering processes with openfoam$^{(R)}$. Coast. Eng. 71, 119-134. https://doi.org/10.1016/j.coastaleng.2012.06.002
  7. Issa, R.I., 1986. Solution of the implicitly discretized fluid-flow equations by operator-splitting. J. Comput. Phys. 62 (1), 40-65. https://doi.org/10.1016/0021-9991(86)90099-9
  8. OpenFOAM, 2014. Predictor-corrector Semi-implicit Mules, p. 30 (Mar).
  9. OpenFOAM, 2015. Openfoam User Guide.
  10. Rusche, H., 2002. Computational Fluid Dynamics of Dispersed Two-phase Flows at High Phase Fractions. Imperial College of Science, Technology & Medicine.
  11. Seng, S., Pedersen, P.T., Jensen, J.J., 2012. Slamming and Whipping Analysis of Ships. DTU Mechanical Engineering.
  12. Weller, H.G., Tabor, G., Jasak, H., Fureby, C., 1998. A tensorial approach to computational continuum mechanics using object-oriented techniques. Comput. Phys. 12 (6), 620-631. https://doi.org/10.1063/1.168744

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