Theoretical and numerical comparison of hyperelastic and hypoelastic formulations for Eulerian non-linear elastoplasticity
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Michael Dumbser | Raphaël Loubère | Walter Boscheri | Ilya Peshkov | Evgeniy Romenski | M. Dumbser | R. Loubère | W. Boscheri | I. Peshkov | E. Romenski
[1] 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..
[2] L. A. Merzhievskii,et al. Shock-wave processes in metals , 1985 .
[3] David H. Sharp,et al. A conservative formulation for plasticity , 1992 .
[4] S. L. Gavrilyuk,et al. Diffuse interface model for compressible fluid - Compressible elastic-plastic solid interaction , 2012, J. Comput. Phys..
[5] D. Steinberg,et al. A constitutive model for metals applicable at high-strain rate , 1980 .
[6] J. Stewart,et al. On transient relativistic thermodynamics and kinetic theory. Il , 1979, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.
[7] S. Gavrilyuk,et al. A Well-posed Hypoelastic Model Derived From a Hyperelastic One , 2015, Dynamic Damage and Fragmentation.
[8] K. Kamrin,et al. Continuum modelling and simulation of granular flows through their many phases , 2014, Journal of Fluid Mechanics.
[9] J. Glimm,et al. A model for rate-dependent plasticity , 1995 .
[10] Raphaël Loubère,et al. High Order Accurate Direct Arbitrary-Lagrangian-Eulerian ADER-MOOD Finite Volume Schemes for Non-Conservative Hyperbolic Systems with Stiff Source Terms , 2017 .
[11] S. K. Godunov,et al. Nonstationary equations of nonlinear elasticity theory in eulerian coordinates , 1972 .
[12] I. Rutkevich. The propagation of small perturbations in a viscoelastic fluid: PMM vol. 34, n≗1, 1970, pp. 41–56 , 1970 .
[13] J. Nye. Some geometrical relations in dislocated crystals , 1953 .
[14] V. Ju,et al. A Conservative Eulerian Formulation of the Equations for Elastic Flow , 2003 .
[15] J. Maxwell,et al. The Dynamical Theory of Gases , 1905, Nature.
[16] J. F. Besseling. A Thermodynamic Approach to Rheology , 1968 .
[17] S. Godunov,et al. Hydrodynamic Effects in Colliding Solids , 1970 .
[18] J. F. Besseling,et al. Mathematical Modelling of Inelastic Deformation , 1994 .
[19] A. I. Leonov. Nonequilibrium thermodynamics and rheology of viscoelastic polymer media , 1976 .
[20] Eleuterio F. Toro,et al. ADER: Arbitrary High Order Godunov Approach , 2002, J. Sci. Comput..
[21] J. Oldroyd. On the formulation of rheological equations of state , 1950, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[22] N. Bourne,et al. Constitutive modeling of fracture waves , 2003 .
[23] H. S. Udaykumar,et al. Simulation of high speed impact, penetration and fragmentation problems on locally refined Cartesian grids , 2013, J. Comput. Phys..
[24] J. Hirschfelder. Kinetic Theory of Liquids. , 1956 .
[25] Stéphane Clain,et al. The Multidimensional Optimal Order Detection method in the three‐dimensional case: very high‐order finite volume method for hyperbolic systems , 2013 .
[26] Michael Dumbser,et al. A sub-cell based indicator for troubled zones in RKDG schemes and a novel class of hybrid RKDG+HWENO schemes , 2004, J. Comput. Phys..
[27] Dimitris Drikakis,et al. An Eulerian finite‐volume scheme for large elastoplastic deformations in solids , 2010 .
[28] D. Eakins,et al. Attenuation of the dynamic yield point of shocked aluminum using elastodynamic simulations of dislocation dynamics. , 2015, Physical review letters.
[29] W. Israel. Nonstationary irreversible thermodynamics: A Causal relativistic theory , 1976 .
[30] Neil J. Balmforth,et al. Yielding to Stress: Recent Developments in Viscoplastic Fluid Mechanics , 2014 .
[31] Michael Dumbser,et al. Cell centered direct Arbitrary-Lagrangian-Eulerian ADER-WENO finite volume schemes for nonlinear hyperelasticity , 2016 .
[32] Michael Dumbser,et al. A direct Arbitrary-Lagrangian-Eulerian ADER-WENO finite volume scheme on unstructured tetrahedral meshes for conservative and non-conservative hyperbolic systems in 3D , 2014, J. Comput. Phys..
[33] Ilya Peshkov,et al. On a pure hyperbolic alternative to the Navier-Stokes equations , 2014 .
[34] Dochan Kwak,et al. Computational Fluid Dynamics Review 2010 , 2010 .
[35] Heng Xiao,et al. Choice of objective rate in single parameter hypoelastic deformation cycles , 2006 .
[36] Michael Dumbser,et al. Arbitrary-Lagrangian-Eulerian Discontinuous Galerkin schemes with a posteriori subcell finite volume limiting on moving unstructured meshes , 2016, J. Comput. Phys..
[37] Michael Dumbser,et al. Central Weighted ENO Schemes for Hyperbolic Conservation Laws on Fixed and Moving Unstructured Meshes , 2017, SIAM J. Sci. Comput..
[38] S. K. Godunov. Symmetric form of the magnetohydrodynamic equation , 1972 .
[39] P. T. Barton. A level-set based Eulerian method for simulating problems involving high strain-rate fracture and fragmentation , 2018, International Journal of Impact Engineering.
[40] E. H. Lee,et al. Finite‐Strain Elastic—Plastic Theory with Application to Plane‐Wave Analysis , 1967 .
[41] I︠A︡kov Ilʹich Frenkelʹ. Kinetic Theory of Liquids , 1955 .
[42] Nathaniel R. Morgan,et al. A cell-centered Lagrangian Godunov-like method for solid dynamics , 2013 .
[43] P. Roe,et al. A Solution-Adaptive Upwind Scheme for Ideal Magnetohydrodynamics , 1999 .
[44] S. K. Godunov,et al. Elements of continuum mechanics , 1978 .
[46] M. Gurtin,et al. The Mechanics and Thermodynamics of Continua , 2010 .
[47] A. Kulikovskii,et al. Mathematical Aspects of Numerical Solution of Hyperbolic Systems , 1998, physics/9807053.
[48] Angelo Iollo,et al. A Cartesian scheme for compressible multimaterial models in 3D , 2016, J. Comput. Phys..
[49] A. D. Resnyansky,et al. DISLOCATION STRUCTURE IN THE MODELS OF DYNAMIC DEFORMATION AND FRACTURE OF METALS , 1985 .
[50] Chi-Wang Shu,et al. The Runge-Kutta Discontinuous Galerkin Method for Conservation Laws V , 1998 .
[51] Angelo Iollo,et al. A Cartesian Scheme for Compressible Multimaterial Hyperelastic Models with Plasticity , 2017 .
[52] Michael Dumbser,et al. Finite volume schemes of very high order of accuracy for stiff hyperbolic balance laws , 2008, J. Comput. Phys..
[53] J. N. Johnson,et al. Dislocation Dynamics and Single‐Crystal Constitutive Relations: Shock‐Wave Propagation and Precursor Decay , 1970 .
[54] Sylvie Benzoni-Gavage,et al. Multi-dimensional hyperbolic partial differential equations , 2006 .
[55] M. Wilkins. Calculation of Elastic-Plastic Flow , 1963 .
[56] E. Kröner,et al. Allgemeine Kontinuumstheorie der Versetzungen und Eigenspannungen , 1959 .
[57] Bruno Despres,et al. A Geometrical Approach to Nonconservative Shocks and Elastoplastic Shocks , 2007 .
[58] I. Rutkevich. On the thermodynamic interpretation of the evolutionary conditions of the equations of the mechanics of finitely deformable viscoelastic media of maxwell type: PMM vol. 36, n≗2, 1972, pp. 306–319 , 1972 .
[59] Michael Dumbser,et al. A New Family of High Order Unstructured MOOD and ADER Finite Volume Schemes for Multidimensional Systems of Hyperbolic Conservation Laws , 2014 .
[60] Michael Dumbser,et al. Arbitrary high order PNPM schemes on unstructured meshes for the compressible Navier–Stokes equations , 2010 .
[61] Nicolas Favrie,et al. Criterion of Hyperbolicity in Hyperelasticity in the Case of the Stored Energy in Separable Form , 2014 .
[62] M. Torrilhon. Modeling Nonequilibrium Gas Flow Based on Moment Equations , 2016 .
[63] J. Marchal,et al. Loss of evolution in the flow of viscoelastic fluids , 1986 .
[64] Claus-Dieter Munz,et al. ADER: A High-Order Approach for Linear Hyperbolic Systems in 2D , 2002, J. Sci. Comput..
[65] S. Godunov,et al. Use of relaxation viscoelastic model in calculating uniaxial homogeneous strains and refining the interpolation equations for maxwellian viscosity , 1975 .
[66] Michael Dumbser,et al. High order ADER schemes for a unified first order hyperbolic formulation of continuum mechanics: Viscous heat-conducting fluids and elastic solids , 2015, J. Comput. Phys..
[67] R. Bullough,et al. Continuous distributions of dislocations: a new application of the methods of non-Riemannian geometry , 1955, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[68] E. I. Romensky,et al. Thermodynamics and Hyperbolic Systems of Balance Laws in Continuum Mechanics , 2001 .
[69] J. Saut,et al. Change of type and loss of evolution in the flow of viscoelastic fluids , 1986 .
[70] Jacques Massoni,et al. Impact simulation by an Eulerian model for interaction of multiple elastic-plastic solids and fluids , 2017 .
[71] B. Wendroff,et al. Cell-centered Lagrangian Lax–Wendroff HLL hybrid method for elasto-plastic flows , 2017 .
[72] Vladimir A. Titarev,et al. Exact and approximate solutions of Riemann problems in non-linear elasticity , 2009, J. Comput. Phys..
[73] Chi-Wang Shu,et al. A Comparison of Troubled-Cell Indicators for Runge-Kutta Discontinuous Galerkin Methods Using Weighted Essentially Nonoscillatory Limiters , 2005, SIAM J. Sci. Comput..
[74] D. S. Wood,et al. Dislocation Mobility in Copper , 1967 .
[75] E. I. Romenskii. Deformation model for brittle materials and the structure of failure waves , 2007 .
[76] Bruno Després,et al. Discretization of hyperelasticity on unstructured mesh with a cell-centered Lagrangian scheme , 2010, J. Comput. Phys..
[77] Nicolas Favrie,et al. Dynamics of shock waves in elastic-plastic solids , 2011 .
[78] G. J. Ball,et al. A free-Lagrange augmented Godunov method for the simulation of elastic-plastic solids , 2002 .
[79] Stéphane Clain,et al. Improved detection criteria for the multi-dimensional optimal order detection (MOOD) on unstructured meshes with very high-order polynomials , 2012 .
[80] Chi-Wang Shu,et al. Monotonicity Preserving Weighted Essentially Non-oscillatory Schemes with Increasingly High Order of Accuracy , 2000 .
[81] Michael Dumbser,et al. A posteriori subcell limiting of the discontinuous Galerkin finite element method for hyperbolic conservation laws , 2014, J. Comput. Phys..
[82] A. D. Resnyansky,et al. The role of numerical simulation in the study of high-velocity impact , 1995 .
[83] Michael Dumbser,et al. A unified framework for the construction of one-step finite volume and discontinuous Galerkin schemes on unstructured meshes , 2008, J. Comput. Phys..
[84] Eleuterio F. Toro,et al. Derivative Riemann solvers for systems of conservation laws and ADER methods , 2006, J. Comput. Phys..
[85] Michael Dumbser,et al. High order ADER schemes for a unified first order hyperbolic formulation of Newtonian continuum mechanics coupled with electro-dynamics , 2016, J. Comput. Phys..
[86] P. Saramito. A new elastoviscoplastic model based on the Herschel–Bulkley viscoplastic model , 2009 .
[87] Manuel Jesús Castro Díaz,et al. Well-Balanced High Order Extensions of Godunov's Method for Semilinear Balance Laws , 2008, SIAM J. Numer. Anal..
[88] Michael Dumbser,et al. Quadrature-free non-oscillatory finite volume schemes on unstructured meshes for nonlinear hyperbolic systems , 2007, J. Comput. Phys..
[89] Michael Dumbser,et al. Direct Arbitrary-Lagrangian-Eulerian ADER-MOOD finite volume schemes for multidimensional hyperbolic conservation laws , 2015, J. Comput. Phys..
[90] Stéphane Clain,et al. A high-order finite volume method for systems of conservation laws - Multi-dimensional Optimal Order Detection (MOOD) , 2011, J. Comput. Phys..
[91] Eleuterio F. Toro,et al. ADER schemes for three-dimensional non-linear hyperbolic systems , 2005 .
[92] J. Oldroyd. A rational formulation of the equations of plastic flow for a Bingham solid , 1947, Mathematical Proceedings of the Cambridge Philosophical Society.
[93] A. Putz,et al. The solid–fluid transition in a yield stress shear thinning physical gel , 2009 .
[94] Manuel Jesús Castro Díaz,et al. On a well-balanced high-order finite volume scheme for shallow water equations with topography and dry areas , 2007, J. Comput. Phys..
[95] A. J. Gil,et al. A first‐order hyperbolic framework for large strain computational solid dynamics: An upwind cell centred Total Lagrangian scheme , 2017 .
[96] Brian J. Edwards,et al. Thermodynamics of flowing systems : with internal microstructure , 1994 .
[97] M. J. Castro,et al. ADER schemes on unstructured meshes for nonconservative hyperbolic systems: Applications to geophysical flows , 2009 .
[98] Jianxian Qiu,et al. An h-adaptive RKDG method with troubled-cell indicator for two-dimensional hyperbolic conservation laws , 2013, Adv. Comput. Math..
[99] Antonio J. Gil,et al. Development of a cell centred upwind finite volume algorithm for a new conservation law formulation in structural dynamics , 2013 .
[100] S. Godunov,et al. Systems of thermodynamically coordinated laws of conservation invariant under rotations , 1996 .
[101] John A. Trangenstein,et al. Numerical algorithms for strong discontinuities in elastic-plastic solids , 1992 .
[102] Ralf Deiterding,et al. Eulerian adaptive finite-difference method for high-velocity impact and penetration problems , 2013, J. Comput. Phys..
[103] Numerical simulation of discontinuous solutions in nonlinear elasticity theory , 2009 .
[104] Phillip Colella,et al. A higher-order Godunov method for modeling finite deformation in elastic-plastic solids , 1991 .
[105] Jerry S. Brock,et al. Benchmark solution of the dynamic response of a spherical shell at finite strain , 2017 .
[106] Walter Noll,et al. On the Continuity of the Solid and Fluid States , 1955 .
[107] Richard Saurel,et al. Modelling wave dynamics of compressible elastic materials , 2008, J. Comput. Phys..
[108] S. Godunov,et al. Elements of Continuum Mechanics and Conservation Laws , 2003, Springer US.
[109] Miroslav Grmela,et al. Dynamics and thermodynamics of complex fluids. I. Development of a general formalism , 1997 .
[110] E. I. Romenskii. Hypoelastic form of equations in nonlinear elasticity theory , 1974 .
[111] Michael Dumbser,et al. Explicit one-step time discretizations for discontinuous Galerkin and finite volume schemes based on local predictors , 2011, J. Comput. Phys..
[112] Miroslav Grmela,et al. Continuum mechanics and thermodynamics in the Hamilton and the Godunov-type formulations , 2017, Continuum Mechanics and Thermodynamics.
[113] V. I. Kondaurov. Equations of elastoviscoplastic medium with finite deformations , 1982 .
[114] Olivier Pouliquen,et al. Granular Media: Between Fluid and Solid , 2013 .
[115] Rogelio Ortigosa,et al. A first order hyperbolic framework for large strain computational solid dynamics. Part I: Total Lagrangian isothermal elasticity , 2015 .
[116] J. Ball. Convexity conditions and existence theorems in nonlinear elasticity , 1976 .
[117] Michael Dumbser,et al. An Efficient Quadrature-Free Formulation for High Order Arbitrary-Lagrangian–Eulerian ADER-WENO Finite Volume Schemes on Unstructured Meshes , 2016, J. Sci. Comput..
[118] Ilya Peshkov,et al. Thermodynamically consistent nonlinear model of elastoplastic Maxwell medium , 2010 .
[119] Miroslav Grmela,et al. Dynamics and thermodynamics of complex fluids. II. Illustrations of a general formalism , 1997 .
[120] Phillip Colella,et al. A high-order Eulerian Godunov method for elastic-plastic flow in solids , 2001 .
[121] Alain Goriely,et al. Riemann–Cartan Geometry of Nonlinear Dislocation Mechanics , 2012 .
[122] I-Shih Liu,et al. Relativistic thermodynamics of gases , 1986 .
[123] Carl Eckart,et al. The Thermodynamics of Irreversible Processes. IV. The Theory of Elasticity and Anelasticity , 1948 .
[124] M. Semplice,et al. Adaptive Mesh Refinement for Hyperbolic Systems Based on Third-Order Compact WENO Reconstruction , 2014, Journal of Scientific Computing.
[125] Michael Dumbser,et al. Space–time adaptive ADER discontinuous Galerkin finite element schemes with a posteriori sub-cell finite volume limiting , 2014, 1412.0081.
[126] C. M. Dafermos,et al. Hyberbolic [i.e. Hyperbolic] conservation laws in continuum physics , 2005 .
[127] L. E. Malvern. Introduction to the mechanics of a continuous medium , 1969 .
[128] A. I. Leonov. On a class of constitutive equations for viscoelastic liquids , 1987 .
[129] Hyun Gyu Kim. A comparative study of hyperelastic and hypoelastic material models with constant elastic moduli for large deformation problems , 2016 .
[130] E. I. Romensky,et al. Hyperbolic systems of thermodynamically compatible conservation laws in continuum mechanics , 1998 .
[131] C. M. Lund,et al. A constitutive model for strain rates from 10−4 to 106 s−1 , 1989 .
[132] Angelo Iollo,et al. A simple Cartesian scheme for compressible multimaterials , 2014, J. Comput. Phys..
[133] Walter Boscheri,et al. High Order Direct Arbitrary-Lagrangian–Eulerian (ALE) Finite Volume Schemes for Hyperbolic Systems on Unstructured Meshes , 2016, Archives of Computational Methods in Engineering.
[134] Sylvie Benzoni-Gavage,et al. Multidimensional hyperbolic partial differential equations : first-order systems and applications , 2006 .
[135] Manuel Jesús Castro Díaz,et al. High order finite volume schemes based on reconstruction of states for solving hyperbolic systems with nonconservative products. Applications to shallow-water systems , 2006, Math. Comput..
[136] Milos Kojic,et al. Studies of finite element procedures—Stress solution of a closed elastic strain path with stretching and shearing using the updated Lagrangian Jaumann formulation , 1987 .
[137] E. Kröner. The Dislocation as a Fundamental New Concept in Continuum Mechanics , 1963 .
[138] Michael Dumbser,et al. A simple robust and accurate a posteriori sub-cell finite volume limiter for the discontinuous Galerkin method on unstructured meshes , 2016, J. Comput. Phys..
[139] S. P. Gill,et al. Physics of Shock Waves and High-Temperature Hydrodynamic Phenomena , 2002 .
[140] Michael Dumbser,et al. Arbitrary-Lagrangian-Eulerian One-Step WENO Finite Volume Schemes on Unstructured Triangular Meshes , 2013, 1302.3076.
[141] Nathaniel R. Morgan,et al. Reduction of dissipation in Lagrange cell-centered hydrodynamics (CCH) through corner gradient reconstruction (CGR) , 2015, J. Comput. Phys..
[142] A. Green. Hypo-elasticity and plasticity , 1956, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[143] J. Stewart. On transient relativistic thermodynamics and kinetic theory , 1977, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.
[144] Feng Wang,et al. A Conservative Eulerian Numerical Scheme for Elastoplasticity and Application to Plate Impact Problems , 1993, IMPACT Comput. Sci. Eng..
[145] William J. Rider,et al. Enhanced Verification Test Suite for Physics Simulation Codes , 2008 .
[146] G. Lebon,et al. Extended irreversible thermodynamics , 1993 .
[147] Chi-Wang Shu,et al. The Runge-Kutta local projection discontinuous Galerkin finite element method for conservation laws. IV. The multidimensional case , 1990 .
[148] Miroslav Grmela,et al. Irreversible mechanics and thermodynamics of two-phase continua experiencing stress-induced solid–fluid transitions , 2015 .
[149] P. T. Barton,et al. On Computational Modelling of Strain-Hardening Material Dynamics , 2012 .
[150] Nicolas Favrie,et al. Multi-solid and multi-fluid diffuse interface model: Applications to dynamic fracture and fragmentation , 2015, J. Comput. Phys..
[151] Geoffrey Ingram Taylor,et al. The use of flat-ended projectiles for determining dynamic yield stress I. Theoretical considerations , 1948, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.
[152] D. Steinberg,et al. Pressure and temperature derivatives of the isotropic polycrystalline shear modulus for 65 elements , 1974 .
[153] Michael Dumbser,et al. A unified hyperbolic formulation for viscous fluids and elastoplastic solids , 2016, 1705.02151.
[154] M. Dumbser,et al. High-Order Unstructured Lagrangian One-Step WENO Finite Volume Schemes for Non-Conservative Hyperbolic Systems: Applications to Compressible Multi-Phase Flows , 2013, 1304.4816.
[155] W. Johnston,et al. Dislocation Velocities, Dislocation Densities, and Plastic Flow in Lithium Fluoride Crystals , 1959 .
[156] L. A. Merzhievskii,et al. Deformation and collapse of hollow conical casing , 1987 .
[157] Michael Dumbser,et al. ADER Schemes for Nonlinear Systems of Stiff Advection–Diffusion–Reaction Equations , 2011, J. Sci. Comput..
[158] C. Parés. Numerical methods for nonconservative hyperbolic systems: a theoretical framework. , 2006 .
[159] Mikhail Shashkov,et al. A finite volume cell‐centered Lagrangian hydrodynamics approach for solids in general unstructured grids , 2013 .
[160] Chi-Wang Shu. Essentially non-oscillatory and weighted essentially non-oscillatory schemes for hyperbolic conservation laws , 1998 .
[161] Michael Dumbser,et al. Solving the relativistic magnetohydrodynamics equations with ADER discontinuous Galerkin methods, a posteriori subcell limiting and adaptive mesh refinement , 2015, 1504.07458.
[162] Stéphane Clain,et al. The MOOD method in the three-dimensional case: Very-High-Order Finite Volume Method for Hyperbolic Systems. , 2012 .
[163] C. Munz,et al. Hyperbolic divergence cleaning for the MHD equations , 2002 .
[164] Nikolaos Nikiforakis,et al. A multi-physics methodology for the simulation of reactive flow and elastoplastic structural response , 2017, J. Comput. Phys..
[165] J. Clayton,et al. Analysis of nonlinear elastic aspects of precursor attenuation in shock-compressed metallic crystals , 2018 .
[166] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[167] Kurt Friedrichs,et al. Symmetric positive linear differential equations , 1958 .