Unified Lagrangian formulation for solid and fluid mechanics and FSI problems

Abstract We present a Lagrangian monolithic strategy for solving fluid–structure interaction (FSI) problems. The formulation is called Unified because fluids and solids are solved using the same solution scheme and unknown variables. The method is based on a mixed velocity–pressure formulation. Each time step increment is solved via an iterative partitioned two-step procedure. The Particle Finite Element Method (PFEM) is used for solving the fluid parts of the domain, while for the solid ones the Finite Element Method (FEM) is employed. Both velocity and pressure fields are interpolated using linear shape functions. For quasi-incompressible materials, the solution scheme is stabilized via the Finite Calculus (FIC) method. The stabilized elements for quasi-incompressible hypoelastic solids and Newtonian fluids are called VPS/S-element and VPS/F-element, respectively. Other two non-stabilized elements are derived for hypoelastic solids. One is based on a Velocity formulation (V-element) and the other on a mixed Velocity–Pressure scheme (VP-element). The algorithms for coupling the solid elements with the VPS/F fluid element are explained in detail. The Unified formulation is validated by solving benchmark FSI problems and by comparing the numerical solution to the ones published in the literature.

[1]  Carlos A. Felippa,et al.  Consistent pressure Laplacian stabilization for incompressible continua via higher‐order finite calculus , 2011 .

[2]  J. Nagtegaal,et al.  Some computational aspects of elastic-plastic large strain analysis , 1981 .

[3]  Eugenio Oñate,et al.  Melting and spread of polymers in fire with the particle finite element method , 2010 .

[4]  Kristian Krabbenhoft,et al.  Particle finite element analysis of the granular column collapse problem , 2014 .

[5]  Herbert Edelsbrunner,et al.  Three-dimensional alpha shapes , 1992, VVS.

[6]  Eugenio Oñate,et al.  A unified monolithic approach for multi-fluid flows and fluid–structure interaction using the Particle Finite Element Method with fixed mesh , 2015 .

[7]  Carlos A. Felippa,et al.  A family of residual‐based stabilized finite element methods for Stokes flows , 2011 .

[8]  Eugenio Oñate,et al.  The particle finite element method: a powerful tool to solve incompressible flows with free‐surfaces and breaking waves , 2004 .

[9]  Alessandro Franci,et al.  Unified Lagrangian Formulation for Fluid and Solid Mechanics, Fluid-Structure Interaction and Coupled Thermal Problems Using the PFEM , 2016 .

[10]  Eugenio Oñate,et al.  Modeling of ground excavation with the particle finite element method , 2010 .

[11]  Eugenio Oñate,et al.  Updated lagrangian mixed finite element formulation for quasi and fully incompressible fluids , 2014 .

[12]  D. Dinkler,et al.  A monolithic approach to fluid–structure interaction using space–time finite elements , 2004 .

[13]  F. Brezzi On the existence, uniqueness and approximation of saddle-point problems arising from lagrangian multipliers , 1974 .

[14]  Antonio J. Gil,et al.  The Immersed Structural Potential Method for haemodynamic applications , 2010, J. Comput. Phys..

[15]  U. Perego,et al.  A Lagrangian finite element approach for the simulation of water-waves induced by landslides , 2011 .

[16]  E. Oñate,et al.  FIC/FEM Formulation with Matrix Stabilizing Terms for Incompressible Flows at Low and High Reynolds Numbers , 2006 .

[17]  Eugenio Oñate,et al.  A two‐step monolithic method for the efficient simulation of incompressible flows , 2014 .

[18]  Eugenio Oñate,et al.  Finite calculus formulations for finite element analysis of incompressible flows. Eulerian, ALE and Lagrangian approaches , 2006 .

[19]  O. C. Zienkiewicz,et al.  The Finite Element Method: Its Basis and Fundamentals , 2005 .

[20]  Eugenio Oñate,et al.  Improving mass conservation in simulation of incompressible flows , 2012 .

[21]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[22]  E. Oñate,et al.  Nodally exact Ritz discretizations of 1D diffusion–absorption and Helmholtz equations by variational FIC and modified equation methods , 2006 .

[23]  Wing Kam Liu,et al.  Extended immersed boundary method using FEM and RKPM , 2004 .

[24]  W. Prager,et al.  Introduction of Mechanics of Continua , 1962 .

[25]  Massimiliano Cremonesi,et al.  A Lagrangian finite element approach for the analysis of fluid–structure interaction problems , 2010 .

[26]  Eugenio Oñate,et al.  Analysis of multifluid flows with large time steps using the particle finite element method , 2014 .

[27]  Michael H. Scott,et al.  Modeling fluid-structure interaction by the particle finite element method in OpenSees , 2014 .

[28]  Miss A.O. Penney (b) , 1974, The New Yale Book of Quotations.

[29]  Long Chen FINITE ELEMENT METHOD , 2013 .

[30]  E. Oñate,et al.  Possibilities of the particle finite element method for fluid–soil–structure interaction problems , 2011 .

[31]  Tianshu Wang,et al.  Some improvements on free surface simulation by the particle finite element method , 2009 .

[32]  G. Johnson,et al.  A discussion of stress rates in finite deformation problems , 1984 .

[33]  Eugenio Oñate,et al.  Particle finite element method in fluid-mechanics including thermal convection-diffusion , 2005 .

[34]  Eugenio Oñate,et al.  A particle finite element method (PFEM) for coupled thermal analysis of quasi and fully incompressible flows and fluid-structure interaction problems , 2014 .

[35]  Antonia Larese,et al.  Validation of the particle finite element method (PFEM) for simulation of free surface flows , 2008 .

[36]  Eugenio Oñate,et al.  Lagrangian formulation for finite element analysis of quasi‐incompressible fluids with reduced mass losses , 2014 .

[37]  D. Dinkler,et al.  Fluid-structure coupling within a monolithic model involving free surface flows , 2005 .

[38]  E. Oñate,et al.  The particle finite element method. An overview , 2004 .

[39]  Eugenio Oñate,et al.  On the effect of the bulk tangent matrix in partitioned solution schemes for nearly incompressible fluids , 2015 .

[40]  Eugenio Oñate,et al.  Polyhedrization of an arbitrary 3D point set , 2003 .

[41]  Antonio J. Gil,et al.  On continuum immersed strategies for Fluid-Structure Interaction , 2012 .

[42]  G. Meschke,et al.  An ALE–PFEM method for the numerical simulation of two-phase mixture flow , 2014 .

[43]  Eugenio Oñate,et al.  Unified Lagrangian formulation for elastic solids and incompressible fluids: Application to fluid–structure interaction problems via the PFEM , 2008 .

[44]  P. M. Naghdi,et al.  A general theory of an elastic-plastic continuum , 1965 .

[45]  Eugenio Oñate,et al.  Advances in the particle finite element method for the analysis of fluid-multibody interaction and bed erosion in free surface flows , 2008 .

[46]  Wing Kam Liu,et al.  Nonlinear Finite Elements for Continua and Structures , 2000 .

[47]  Eugenio Oñate,et al.  Derivation of stabilized equations for numerical solution of advective-diffusive transport and fluid flow problems , 1998 .

[48]  Eugenio Oñate,et al.  A particle finite element method for analysis of industrial forming processes , 2014 .

[49]  Eugenio Oñate,et al.  Modelling of tunnelling processes and rock cutting tool wear with the particle finite element method , 2013 .

[50]  E. Oñate,et al.  A monolithic Lagrangian approach for fluid–structure interaction problems , 2010 .