A strong coupling partitioned approach for fluid–structure interaction with free surfaces

Abstract Fluid–structure interaction (FSI) problems are of great relevance to many fields in engineering and applied sciences. One wide spread and complex FSI-subclass is the category that studies the instationary behavior of incompressible viscous flows and thin-walled structures exhibiting large deformations. Free surfaces often present an essential additional challenge for this class of problems. Prominent application areas are fluid sloshing in tanks and numerable problems in offshore engineering and naval architecture. Especially when partitioned strong coupling schemes are used in order to solve the coupled FSI problem the design of an appropriate overall computational approach including free surface effects is not trivial. In this paper a new so-called partitioned implicit free surface approach is introduced and embedded into a strong coupling FSI solver. For complex problem classes this approach is combined with the general elevation equation that is closed through a dimensionally reduced pseudo-structural approach. The presented approach shows the same stability properties as a full implicit approach but is by far more efficient—especially in the partitioned coupled case.

[1]  C. Farhat,et al.  Torsional springs for two-dimensional dynamic unstructured fluid meshes , 1998 .

[2]  S. Mittal,et al.  A finite element study of incompressible flows past oscillating cylinders and aerofoils , 1992 .

[3]  M. Kawahara,et al.  LAGRANGIAN FINITE ELEMENT ANALYSIS APPLIED TO VISCOUS FREE SURFACE FLUID FLOW , 1987 .

[4]  D. P. Mok,et al.  Partitioned Analysis of Transient Nonlinear Fluid Structure Interaction Problems Including Free Surface Effects , 2000 .

[5]  T. Tezduyar,et al.  A parallel 3D computational method for fluid-structure interactions in parachute systems , 2000 .

[6]  F. Harlow,et al.  Numerical Calculation of Time‐Dependent Viscous Incompressible Flow of Fluid with Free Surface , 1965 .

[7]  Yousef Saad,et al.  An arbitrary Lagrangian-Eulerian finite element method for solving three-dimensional free surface flows , 1998 .

[8]  C. W. Hirt,et al.  An Arbitrary Lagrangian-Eulerian Computing Method for All Flow Speeds , 1997 .

[9]  Tayfun E. Tezduyar,et al.  Finite Element Methods for Fluid Dynamics with Moving Boundaries and Interfaces , 2004 .

[10]  Daniel Pinyen Mok Partitionierte Lösungsansätze in der Strukturdynamik und der Fluid-Struktur-Interaktion , 2001 .

[11]  Tayfun E. Tezduyar,et al.  Finite element methods for flow problems with moving boundaries and interfaces , 2001 .

[12]  T. Tezduyar,et al.  A new strategy for finite element computations involving moving boundaries and interfaces—the deforming-spatial-domain/space-time procedure. I: The concept and the preliminary numerical tests , 1992 .

[13]  Tayfun E. Tezduyar,et al.  PARALLEL FINITE ELEMENT SIMULATION OF 3D INCOMPRESSIBLE FLOWS: FLUID-STRUCTURE INTERACTIONS , 1995 .

[14]  J. Szmelter Incompressible flow and the finite element method , 2001 .

[15]  C. K. Thornhill,et al.  Part IV. An experimental study of the collapse of liquid columns on a rigid horizontal plane , 1952, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[16]  Thomas J. R. Hughes,et al.  Encyclopedia of computational mechanics , 2004 .

[17]  E. Laitone,et al.  The second approximation to cnoidal and solitary waves , 1960, Journal of Fluid Mechanics.

[18]  Werner Schiehlen,et al.  Multifield problems : state of the art , 2000 .

[19]  P. Tallec,et al.  Fluid structure interaction with large structural displacements , 2001 .

[20]  Eugenio Oñate,et al.  A finite element method for fluid-structure interaction with surface waves using a finite calculus formulation , 2001 .

[21]  S. Mittal,et al.  Computation of unsteady incompressible flows with the stabilized finite element methods: Space-time formulations, iterative strategies and massively parallel implementations , 1992 .

[22]  Bruce M. Irons,et al.  A version of the Aitken accelerator for computer iteration , 1969 .

[23]  Wolfgang A. Wall Fluid-Struktur-Interaktion mit stabilisierten Finiten Elementen , 1999 .

[24]  P. J. Slikkerveer,et al.  An implicit surface tension algorithm for Picard solvers of surface-tension-dominated free and moving boundary problems , 1996 .

[25]  C. W. Hirt,et al.  A lagrangian method for calculating the dynamics of an incompressible fluid with free surface , 1970 .

[26]  S. Mittal,et al.  A new strategy for finite element computations involving moving boundaries and interfaces—the deforming-spatial-domain/space-time procedure. II: Computation of free-surface flows, two-liquid flows, and flows with drifting cylinders , 1992 .

[27]  Francis H. Harlow,et al.  Numerical Study of Large‐Amplitude Free‐Surface Motions , 1966 .

[28]  Rekha Ranjana Rao,et al.  A Newton-Raphson Pseudo-Solid Domain Mapping Technique for Free and Moving Boundary Problems , 1996 .

[29]  Wing Kam Liu,et al.  Lagrangian-Eulerian finite element formulation for incompressible viscous flows☆ , 1981 .

[30]  Roland W. Lewis,et al.  Finite element modelling of surface tension effects using a Lagrangian-Eulerian kinematic description , 1997 .

[31]  Balasubramaniam Ramaswamy,et al.  Numerical simulation of unsteady viscous free surface flow , 1990 .

[32]  P. A. Sackinger,et al.  A finite element method for free surface flows of incompressible fluids in three dimensions. Part I. Boundary fitted mesh motion , 2000 .

[33]  Marek Behr,et al.  Free-surface flow simulations in the presence of inclined walls , 2002 .

[34]  C. W. Hirt,et al.  Volume of fluid (VOF) method for the dynamics of free boundaries , 1981 .

[35]  M. Ortiz,et al.  Lagrangian finite element analysis of Newtonian fluid flows , 1998 .