An upwind vertex centred finite volume algorithm for nearly and truly incompressible explicit fast solid dynamic applications: Total and Updated Lagrangian formulations
暂无分享,去创建一个
Ferdinando Auricchio | A. J. Gil | Javier Bonet | Osama I. Hassan | Ataollah Ghavamian | Chun Hean Lee | Antonio J. Gil | J. Bonet | F. Auricchio | C. Lee | O. Hassan | A. Ghavamian
[1] Yuki Onishi. F-Bar Aided Edge-Based Smoothed Finite Element Method with 4-Node Tetrahedral Elements for Static Large Deformation Elastoplastic Problems , 2019, International Journal of Computational Methods.
[2] Michael A. Puso,et al. A stabilized nodally integrated tetrahedral , 2006 .
[3] R. Courant,et al. Über die partiellen Differenzengleichungen der mathematischen Physik , 1928 .
[4] C. Bailey,et al. Dynamic solid mechanics using finite volume methods , 2003 .
[5] Philip Cardiff,et al. Development of a finite volume contact solver based on the penalty method , 2012 .
[6] Hrvoje Jasak,et al. Application of the finite volume method and unstructured meshes to linear elasticity , 2000 .
[7] C. SimoJ.,et al. The discrete energy-momentum method , 1992 .
[8] S. Osher,et al. One-sided difference approximations for nonlinear conservation laws , 1981 .
[9] J. M. Kennedy,et al. Hourglass control in linear and nonlinear problems , 1983 .
[10] J. Bonet,et al. A simple average nodal pressure tetrahedral element for incompressible and nearly incompressible dynamic explicit applications , 1998 .
[11] B. Carnes,et al. A simple, stable, and accurate linear tetrahedral finite element for transient, nearly, and fully incompressible solid dynamics: a dynamic variational multiscale approach , 2016 .
[12] Rémi Abgrall,et al. A discontinuous Galerkin discretization for solving the two-dimensional gas dynamics equations written under total Lagrangian formulation on general unstructured grids , 2014, J. Comput. Phys..
[13] Nabil H. Abboud,et al. A dynamic variational multiscale method for viscoelasticity using linear tetrahedral elements , 2017 .
[14] C. Bailey,et al. A vertex‐based finite volume method applied to non‐linear material problems in computational solid mechanics , 2003 .
[15] Kenji Amaya,et al. A locking‐free selective smoothed finite element method using tetrahedral and triangular elements with adaptive mesh rezoning for large deformation problems , 2014 .
[16] Bruno Després,et al. Discretization of hyperelasticity on unstructured mesh with a cell-centered Lagrangian scheme , 2010, J. Comput. Phys..
[17] T. Hughes. Generalization of selective integration procedures to anisotropic and nonlinear media , 1980 .
[18] D. Owen,et al. Design of simple low order finite elements for large strain analysis of nearly incompressible solids , 1996 .
[19] Rogelio Ortigosa,et al. A computational framework for polyconvex large strain elasticity for geometrically exact beam theory , 2015, Computational Mechanics.
[20] Bruno Després,et al. A cell-centered Lagrangian hydrodynamics scheme on general unstructured meshes in arbitrary dimension , 2009, J. Comput. Phys..
[21] A. J. Gil,et al. A Total Lagrangian upwind Smooth Particle Hydrodynamics algorithm for large strain explicit solid dynamics , 2019, Computer Methods in Applied Mechanics and Engineering.
[22] Clark R. Dohrmann,et al. A uniform nodal strain tetrahedron with isochoric stabilization , 2009 .
[23] Mikhail Shashkov,et al. A finite volume cell‐centered Lagrangian hydrodynamics approach for solids in general unstructured grids , 2013 .
[24] R. D. Wood,et al. Nonlinear Continuum Mechanics for Finite Element Analysis , 1997 .
[25] Antonio J. Gil,et al. An upwind vertex centred Finite Volume solver for Lagrangian solid dynamics , 2015, J. Comput. Phys..
[26] Xianyi Zeng,et al. A velocity/stress mixed stabilized nodal finite element for elastodynamics: Analysis and computations with strongly and weakly enforced boundary conditions , 2017 .
[27] A. J. Gil,et al. A variationally consistent Streamline Upwind Petrov–Galerkin Smooth Particle Hydrodynamics algorithm for large strain solid dynamics , 2017 .
[28] Thomas J. R. Hughes,et al. Improved numerical dissipation for time integration algorithms in structural dynamics , 1977 .
[29] Tzanio V. Kolev,et al. High order curvilinear finite elements for elastic-plastic Lagrangian dynamics , 2014, J. Comput. Phys..
[30] Rogelio Ortigosa,et al. A first order hyperbolic framework for large strain computational solid dynamics. Part II: Total Lagrangian compressible, nearly incompressible and truly incompressible elasticity , 2016 .
[31] Manuel Torrilhon,et al. Constraint-Preserving Upwind Methods for Multidimensional Advection Equations , 2004, SIAM J. Numer. Anal..
[32] F. Auricchio,et al. A three-dimensional finite-strain phenomenological model for shape-memory polymers: Formulation, numerical simulations, and comparison with experimental data , 2016 .
[33] Ngoc Cuong Nguyen,et al. Hybridizable discontinuous Galerkin methods for partial differential equations in continuum mechanics , 2012, J. Comput. Phys..
[34] Antonio J. Gil,et al. A vertex centred Finite Volume Jameson-Schmidt-Turkel (JST) algorithm for a mixed conservation formulation in solid dynamics , 2014, J. Comput. Phys..
[35] P. Cardiff,et al. A Lagrangian cell‐centred finite volume method for metal forming simulation , 2017 .
[36] Nathaniel R. Morgan,et al. A cell-centered Lagrangian Godunov-like method for solid dynamics , 2013 .
[37] M. Chial,et al. in simple , 2003 .
[38] O. C. Zienkiewicz,et al. An alpha modification of Newmark's method , 1980 .
[39] Clark R. Dohrmann,et al. Uniform Strain Elements for Three-Node Triangular and Four-Node Tetrahedral Meshes , 1999 .
[40] Antonio J. Gil,et al. A coupled hp-finite element scheme for the solution of two-dimensional electrostrictive materials , 2012 .
[41] Nabil H. Abboud,et al. Implicit finite incompressible elastodynamics with linear finite elements: A stabilized method in rate form , 2016 .
[42] John A. Trangenstein,et al. A second-order Godunov algorithm for two-dimensional solid mechanics , 1994 .
[43] Pierre-Henri Maire,et al. A high-order cell-centered Lagrangian scheme for compressible fluid flows in two-dimensional cylindrical geometry , 2009, J. Comput. Phys..
[44] Rémi Abgrall,et al. A nominally second-order cell-centered Lagrangian scheme for simulating elastic-plastic flows on two-dimensional unstructured grids , 2013, J. Comput. Phys..
[45] A. J. Gil,et al. A first‐order hyperbolic framework for large strain computational solid dynamics: An upwind cell centred Total Lagrangian scheme , 2017 .
[46] Antonio J. Gil,et al. Development of a cell centred upwind finite volume algorithm for a new conservation law formulation in structural dynamics , 2013 .
[47] Antonio J. Gil,et al. A stabilised Petrov-Galerkin formulation for linear tetrahedral elements in compressible, nearly incompressible and truly incompressible fast dynamics , 2014 .
[48] Rogelio Ortigosa,et al. On a tensor cross product based formulation of large strain solid mechanics , 2016 .
[49] A. J. Gil,et al. An upwind cell centred Total Lagrangian finite volume algorithm for nearly incompressible explicit fast solid dynamic applications , 2018, Computer Methods in Applied Mechanics and Engineering.
[50] Phillip Colella,et al. A higher-order Godunov method for modeling finite deformation in elastic-plastic solids , 1991 .
[51] Rogelio Ortigosa,et al. A first order hyperbolic framework for large strain computational solid dynamics. Part I: Total Lagrangian isothermal elasticity , 2015 .
[52] Oubay Hassan,et al. An averaged nodal deformation gradient linear tetrahedral element for large strain explicit dynamic applications , 2001 .
[53] J. C. Simo,et al. The discrete energy-momentum method. Conserving algorithms for nonlinear elastodynamics , 1992 .
[54] Bruno Després,et al. Lagrangian Gas Dynamics in Two Dimensions and Lagrangian systems , 2005 .
[55] J. Bonet,et al. Stability and comparison of different linear tetrahedral formulations for nearly incompressible explicit dynamic applications , 2001 .
[56] E. A. de Souza Neto,et al. An assessment of the average nodal volume formulation for the analysis of nearly incompressible solids under finite strains , 2004 .
[57] T. Belytschko,et al. A uniform strain hexahedron and quadrilateral with orthogonal hourglass control , 1981 .
[58] Antonio J. Gil,et al. A two-step Taylor-Galerkin formulation for fast dynamics , 2014 .
[59] Antonio J. Gil,et al. Development of a stabilised Petrov–Galerkin formulation for conservation laws in Lagrangian fast solid dynamics , 2014 .
[60] Rainald Löhner,et al. An improved finite volume scheme for compressible flows on unstructured grids , 1995 .
[61] Pierre-Henri Maire,et al. Multi-scale Godunov-type method for cell-centered discrete Lagrangian hydrodynamics , 2009, J. Comput. Phys..
[62] Nabil H. Abboud,et al. Elastoplasticity with linear tetrahedral elements: A variational multiscale method , 2018 .
[63] Rémi Abgrall,et al. A Cell-Centered Lagrangian Scheme for Two-Dimensional Compressible Flow Problems , 2007, SIAM J. Sci. Comput..
[64] A. Chorin. A Numerical Method for Solving Incompressible Viscous Flow Problems , 1997 .
[65] Philip Cardiff,et al. A large strain finite volume method for orthotropic bodies with general material orientations , 2014 .
[66] A. J. Gil,et al. A new Jameson–Schmidt–Turkel Smooth Particle Hydrodynamics algorithm for large strain explicit fast dynamics , 2016 .
[67] Mark L. Wilkins,et al. Impact of cylinders on a rigid boundary , 1973 .
[68] I. Bijelonja,et al. A finite volume method for incompressible linear elasticity , 2006 .
[69] R. Courant,et al. On the Partial Difference Equations, of Mathematical Physics , 2015 .
[70] J. Peraire,et al. A variationally consistent mesh adaptation method for triangular elements in explicit Lagrangian dynamics , 2010 .
[71] J. Breil,et al. A 3D finite volume scheme for solving the updated Lagrangian form of hyperelasticity , 2017 .