4.4 Article

A finite volume cell-centered Lagrangian hydrodynamics approach for solids in general unstructured grids

Journal

Publisher

WILEY-BLACKWELL
DOI: 10.1002/fld.3770

Keywords

Lagrangian; hydrodynamics; compatible formulation; cell-centered; Godunov; elasto-plastic; hypo-elastic model; second-order; predictor-corrector algorithm; GCL; tensor viscosity; Verney shell collapse

Funding

  1. US Department of Energy's National Nuclear Security Administration by Los Alamos National Security, LLC, at Los Alamos National Laboratory [DE-AC52-06NA25396]
  2. US DOE NNSA's Advanced Simulation and Computing (ASC) Program
  3. US DOE Office of Science Advanced Scientific Computing Research (ASCR) Program in Applied Mathematics Research
  4. US Department of Energy through the LANL LDRD Program

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A finite volume cell-centered Lagrangian hydrodynamics approach, formulated in Cartesian frame, is presented for solving elasto-plastic response of solids in general unstructured grids. Because solid materials can sustain significant shear deformation, evolution equations for stress and strain fields are solved in addition to mass, momentum, and energy conservation laws. The total stress is split into deviatoric shear stress and dilatational components. The dilatational response of the material is modeled using the Mie-Gruneisen equation of state. A predicted trial elastic deviatoric stress state is evolved assuming a pure elastic deformation in accordance with the hypo-elastic stress-strain relation. The evolution equations are advanced in time by constructing vertex velocity and corner traction force vectors using multi-dimensional Riemann solutions erected at mesh vertices. Conservation of momentum and total energy along with the increase in entropy principle are invoked for computing these quantities at the vertices. Final state of deviatoric stress is effected via radial return algorithm based on the J-2 von Mises yield condition. The scheme presented in this work is second-order accurate both in space and time. The suitability of the scheme is evinced by solving one- and two-dimensional benchmark problems both in structured grids and in unstructured grids with polygonal cells. Copyright (c) 2013 John Wiley & Sons, Ltd.

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