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Particle Finite Element Method

PFEM particleladen
PFEM CIMNE logo

A Powerful Tool for Fluid-Structure Interaction and Large Deformation Problems

The Particle Finite Element Method (PFEM) is a powerful computational technique developed at CIMNE for solving complex engineering problems involving free-surface flows, large deformations, and fluid-structure interaction. PFEM combines the advantages of Lagrangian particle methods with the robustness of finite element techniques, enabling accurate simulation of problems with evolving boundaries, complex contact interactions, and multi-physics coupling.

Applications

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Free-surface Flow

Accurate tracking of fluid free surfaces, including breaking waves and splashes

⚙️

Fluid-Solid Interaction

Free-surface fluid flows with elasto-plastic structures and complex contact

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Industrial Processes

Simulation of manufacturing: machining, forging, extrusion, and casting

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Landslides Runout

3D simulation of geophysical flows and landslide-generated waves

Particle-laden Flow

Multi-component flows with suspended particles using PFEM-DEM coupling

About the PFEM

The Particle Finite Element Method (PFEM) is a numerical technique for solving multi-physics problems involving fluid dynamics, solid mechanics, and fluid-structure interaction. The method uses a Lagrangian framework where the mesh nodes are treated as particles that move with the material flow.

PFEM is particularly well-suited for problems involving:

  • Free-surface flows with large deformations
  • Fluid-structure interaction with moving boundaries
  • Industrial forming processes
  • Geotechnical applications with large strains
  • Multi-fluid and multi-phase flows

Tsunami wave propagation and impact simulation

Icebreaker simulation using PFEM

Wave breaking and fracture front propagation

The PFEM approach consists of the following key steps:

1. Lagrangian Description: The governing equations are written in a Lagrangian framework where the computational mesh moves with the material particles. This naturally handles convection terms and free-surface tracking.

2. Mesh Generation: At each time step, a new finite element mesh is generated using the Delaunay triangulation of the particle positions. This allows the method to handle large deformations without mesh distortion problems.

3. Alpha Shape Method: The boundary of the domain is identified using the alpha shape technique, which automatically detects the free surface and external boundaries.

4. Finite Element Solution: The governing equations are solved using standard finite element procedures with appropriate stabilization techniques for incompressible flows.

PFEM Solution Steps

Fig 1: Solution steps in PFEM methodology

Alpha Shape Steps

Fig 2: Alpha shape boundary detection steps

For fluid dynamics problems, PFEM solves the Navier-Stokes equations in a Lagrangian framework. The method is particularly effective for:

Free-Surface Flows: The Lagrangian description naturally tracks the free surface without the need for special interface capturing techniques. This makes PFEM ideal for simulating wave breaking, splashing, and sloshing phenomena.

Non-Newtonian Fluids: PFEM can handle complex rheological models including Bingham plastics, viscoplastic materials, and shear-thinning fluids. Applications include fresh concrete flow, mudflows, and industrial slurries.

Multi-fluid Flows: The method can simulate problems involving multiple immiscible fluids with different densities and viscosities, including surface tension effects.

PFEM mesh in a free-surface fluid dynamics problem

Fresh concrete slump test with non-Newtonian Bingham model

PFEM has been successfully extended to solid mechanics problems involving large deformations and complex material behavior:

Large Deformation Analysis: The continuous remeshing capability allows PFEM to handle extremely large deformations that would cause severe mesh distortion in standard FEM approaches.

Contact Problems: The method naturally handles contact and friction between deformable bodies, as well as contact with rigid tools. This is essential for manufacturing process simulations.

Fracture and Failure: PFEM can simulate crack propagation and material failure by allowing the mesh to separate along element edges, creating new free surfaces.

Pressing a quarter of a metal cylinder

Orthogonal cutting test with deformable tool

3D machining with continuous chip formation

Machining with rigid tool - segmental chip

Cylindrical steel bar impacting a wall

Fluid-Structure Interaction (FSI) is one of the most powerful capabilities of PFEM. The method can handle:

Fully Coupled Problems: PFEM solves the fluid and solid domains in a fully coupled manner, ensuring accurate transmission of forces and displacements at the interface.

Free-Surface FSI: The method excels at problems where the fluid has a free surface that interacts with structures, such as wave impact on coastal structures or sloshing in tanks.

Large Motion FSI: PFEM can handle problems with large structural displacements and rotations, including floating bodies and inflatable structures.

FSI Applications Overview

Overview of FSI applications with PFEM

Collapse of water column against deformable membrane

Concrete wall collapse due to tsunami impact

PFEM coupled with Abaqus for airbag deployment

PFEM-2 is an enhanced version of the method that allows for larger time steps and improved computational efficiency:

Multi-time-step Strategy: PFEM-2 uses a predictor-corrector scheme that allows using time steps much larger than traditional explicit methods while maintaining accuracy.

Particle Enrichment: The method enriches the solution with particle-based information to capture fine-scale features without requiring excessively fine meshes.

Multi-fluid Capabilities: PFEM-2 excels at simulating multi-fluid problems with large density ratios and complex interface dynamics.

PFEM-2 Figure 1

Fig 1: PFEM-2 methodology schematic

PFEM-2 Figure 2

Fig 2: Multi-time-step integration scheme

Rayleigh-Taylor instability at Atwood number 3 - time-step comparison

Experimental validation: dam break collapse

Liquid jet injection and primary atomization

Rayleigh-Taylor instability simulation

Detailed Applications

The accurate simulation of the fluid free surface, even in the presence of breaking waves and splashes, together with the automatic modeling of fluid convection and the good energy conservation properties, make the PFEM an ideal tool for the analysis of different hydraulic engineering problems.

The first PFEM simulation of hydraulic laboratory tests was presented in validation studies comparing PFEM results against experimental observations on four different free-surface flow configurations. The suitability of PFEM in modeling wave propagation was clearly demonstrated by reproducing accurately different types of propagating waves in laboratory channels.

Recent work used a PFEM-FEM-DEM technique to simulate the propagation of a tsunami wave in a hydraulic laboratory channel, its impact against a concrete wall and the breakage of the solid structure.

Dam Engineering: PFEM has been applied to simulate overtopping and failure of rockfill dams and related seepage phenomena. Studies include 3D air-water interaction for estimating air demand at dam bottom outlets, and analysis of water shock waves at dam spillways.

Tsunami wave propagation and impact against concrete wall

Collapse of tank with water-oil mixture (PFEM-2)

The simulation of manufacturing processes represents one of the relevant areas of applications of the PFEM. The capability of the method to deal with large deformations, complex contact interaction, and constitutive models explains the large number of PFEM works on manufacturing processes. Furthermore, typically, these problems also include coupled thermal effects that can be easily handled with the PFEM.

Metal Forming: PFEM-solid formulation has been used to reproduce industrial metal forging, machining, and powder filling problems. The method can efficiently simulate cutting processes involving friction, adiabatic shear bands, excessive heating, large strains, and high strain rates.

Mold Filling and Casting: For problems involving large deformation of contours, fluid dynamics approaches are generally preferred. Applications include casting problems and glass forming where the heat equation is coupled to the mechanical model through temperature-dependent viscosity.

Cold Massive Forge - Coining of copper piece

Hot bending of steel plate at 800K

Non-orthogonal machining with deformable tool

Machining with rigid tool - segmental chip

Cold shearing of steel plate

The numerical simulation of landslides is a complex task, due to the complex characterization of the landslide bulk material, the highly deforming shape of the sliding bodies, and the large size of the events. The PFEM has shown to have great potential in this field thanks to its capacity of capturing evolving free surfaces and the possibility of using accurate constitutive models for the landslide material.

Various rheological models have been employed including:

  • Plasticity models with Mohr-Coulomb yield criterion
  • Elastic-viscoplastic models for progressive failure
  • Bingham models for flow-like landslides
  • Regularized μ(I)-rheology for dense granular flows

PFEM has been used to simulate landslide-generated waves (the multi-hazard scenario produced by the impact of landslides in water reservoirs), including the reproduction of the Vajont landslide and the consequent impulse wave in the hydroelectric reservoir using a three-dimensional formulation.

Granular flow with μ(I)-rheology

Tsunami wave created by water landslide

Wave generated by impact of granular material

The PFEM has shown great potential for modeling large deformation problems in geotechnics. The method can track in a natural way the deforming shape of the soil body, compute accurately the contact interaction between the soil and external tools, and consider complex constitutive models.

Cone Penetration Test (CPT): PFEM simulations of CPT in potentially liquefiable materials using state-parameter dependent constitutive models (CASM), showing evolution of water pressure, mean effective stress and deviatoric stress during undrained testing.

Biaxial Tests: Simulation of strain-softening materials using non-local regularization techniques, showing evolution of mesh, vertical stress, incremental plastic deviatoric strain and current bonding.

Pile Installation: Analysis of rough pile insertion in soft clay, modeling the complex non-linear problem of soil-structure interaction during penetration.

Cone penetration test in liquefiable materials

Biaxial test on structured soil

Insertion of rough pile in soft clay

Free-falling penetrometer simulation

Particle-laden, or particulate, flow refers to the dynamics of a multi-component medium where at least one component is a continuously connected fluid (the suspending fluid), and at least one remaining phase consists of disconnected sub-domains (the particles).

The PFEM, combined with a discrete element solver such as the Discrete Element Method (DEM), enables the solution of particle-laden flows even in presence of large motions and changes of shape of the fluid domain.

PFEM-DEM Coupling: Recent formulations allow solid particles to move across fluid elements of the PFEM mesh, similar to traditional particle-in-cell schemes. This maintains good mesh quality during analysis at reasonable computational cost.

Mixing process using PFEM-DEM coupled method

Water tank discharge with embedded particles

Bibliography

Selected peer-reviewed publications on PFEM methodology and applications:

  • Idelsohn SR, Oñate E, Pin FD (2004) The particle finite element method: a powerful tool to solve incompressible flows with free-surfaces and breaking waves. Int J Numer Methods Eng 61(7):964–989
  • Oñate E, Idelsohn S, Pin FD, Aubry R (2004) The particle finite element method. An overview. Int J Comput Methods 1:267–307
  • Idelsohn S, Oñate E, Pin FD (2004) The particle finite element method: a powerful tool to solve incompressible flows with free-surfaces and breaking waves. Int J Numer Methods Eng 61(7):964–989
  • Oñate E, Rojek J, Idelsohn S, Pin FD, Aubry R (2006) Advances in stabilized finite element and particle methods for bulk forming processes. Comput Methods Appl Mech Eng 195(48–49):6750–6777
  • Oñate E, Idelsohn S, Celigueta M, Rossi R (2008) Advances in the particle finite element method for the analysis of fluid-multibody interaction and bed erosion in free surface flows. Comput Methods Appl Mech Eng 197(19–20):1777–1800
  • Carbonell JM, Oñate E, Suarez B (2010) Modeling Ground Excavation with the Particle Finite-Element Method. J Eng Mech 136(4):455–463
  • Cremonesi M, Frangi A, Perego U (2011) A Lagrangian finite element approach for the simulation of water-waves induced by landslides. Comput Struct 89(11–12):1086–1093
  • Oñate E, Franci A, Carbonell JM (2014) A particle finite element method for analysis of industrial forming processes. Comput Mech 54(1):85–107
  • Franci A, Oñate E, Carbonell JM (2016) Unified Lagrangian formulation for solid and fluid mechanics and FSI problems. Comput Methods Appl Mech Eng 298:520–547
  • Rodriguez J, Carbonell JM, Cante J, Oliver J (2016) The particle finite element method (PFEM) in thermo-mechanical problems. Int J Numer Methods Eng 107(9):733–785
  • Gimenez J, Ramajo D, Damián S, Nigro N, Idelsohn S (2017) An assessment of the potential of PFEM-2 for solving long real-time industrial applications. Comput Part Mech 4(3):251–267
  • Franci A, Cremonesi M (2019) 3D regularized μ(I)-rheology for Granular flows simulation. J Comput Phys 378:257–277
  • Cremonesi M, Franci A, Idelsohn SR, Oñate E (2020) A state of the art review of the Particle Finite Element Method (PFEM). Archives of Computational Methods in Engineering, 17, 1709-1735
  • Franci A, Cremonesi M, Perego U, Crosta G, Oñate E (2020) 3D simulation of Vajont disaster. Part 1: Numerical formulation and validation. Engineering Geology, 105854
  • Oñate E, Cornejo A, Zárate F, Kashiyama K, Franci A (2022) Combination of the finite element method and particle-based methods for predicting the failure of reinforced concrete structures under extreme water forces. Engineering Structures, 251B, 113510

... and 100+ additional publications. See full list for complete bibliography.

Author Year Title Institution
Del Pin F 2003 The meshless finite element method applied to a lagrangian particle formulation of fluid flows Universidad Nacional del Litoral, Argentina
Aubry R 2006 Incompressible Lagrangian fluid flow with thermal coupling Universitat Politècnica de Catalunya, Spain
Marti J 2008 El método de elementos finitos de partículas en interacción fluido-estructura Universidad Nacional del Litoral, Argentina
Carbonell JM 2009 Modeling of Ground Excavation with the Particle Finite Element Method Universitat Politècnica de Catalunya, Spain
Cremonesi M 2010 A Lagrangian finite element method for the interaction between flexible structures and free surfaces fluid flows Politecnico di Milano, Italy
Ryzhakov P 2010 Lagrangian FE methods for coupled problems in fluid mechanics Universitat Politècnica de Catalunya, Spain
Larese A 2012 Instability analysis of earth dams due to overspills by the particle finite element method Universitat Politècnica de Catalunya, Spain
Rodriguez JM 2013 Numerical modeling of metal cutting processes using the Particle Finite Element Method Universitat Politècnica de Catalunya, Spain
Zhang X 2014 Particle Finite Element Method in Geomechanics The University of Newcastle, Australia
Zhu M 2014 Fluid-structure interaction analysis with the particle finite element method Oregon State University, US
Franci A 2015 Unified Lagrangian formulation for fluid and solid mechanics, fluid-structure interaction and coupled thermal problems using the PFEM Universitat Politècnica de Catalunya, Spain
Becker P 2015 An enhanced Particle Finite Element Method with special emphasis on landslides and debris flows Universitat Politècnica de Catalunya, Spain
Monforte L 2018 Insertion problems in geomechanics with the particle finite element method Universitat Politècnica de Catalunya, Spain
Celigueta MA 2019 A Particle Finite Element Method for fluid-related problems in civil engineering Universitat Politècnica de Catalunya, Spain
Meduri S 2019 A fully explicit Lagrangian finite element method for highly nonlinear fluid–structure interaction problems Politecnico di Milano, Italy
Cornejo A 2020 A fully Lagrangian formulation for fluid-structure interaction between free-surface flows and multi-fracturing solids Universitat Politècnica de Catalunya, Spain
Author Year Title Duration
Cremonesi M 2021 A fully explicit Lagrangian Finite Element Method for highly non-linear fluid-structure interaction problems, CIMNE seminars 55 min
Oñate E 2016 El método de elementos finitos y partículas (PFEM) en Ingeniería 72 min
Oñate E 2015 The Particle Finite Element Method (PFEM) in Engineering 68 min
Idelsohn S 2015 The Particle Finite Element Method - Second Generation. Particles 2015, Barcelona 35 min
Idelsohn S 2014 Particle Methods: The most efficient way to solve fluid mechanics problem. WCCM, Barcelona 44 min

PFEM analysis of fluid dynamics, non-linear solid mechanics and fluid-structure interaction problems can be run with the open-source code Kratos Multiphysics and the user-friendly interface programmed through the pre- and post-processor GiD.

Kratos Multiphysics

Kratos Multiphysics

A framework for building parallel multi-disciplinary simulation software. Modularity, extensibility and HPC are the main objectives. Kratos has BSD license and is written in C++ with extensive Python interface.

GiD

GiD

A pre- and post-processor designed to cover all common needs in numerical simulation: geometrical modeling, definition of analysis data, meshing, data transfer to analysis software, and visualization of numerical results.

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