A Physically Motivated Internal State Variable Plasticity/Damage Model Embedded With a Length Scale for Hazmat Tank Cars’ Structural Integrity Applications

In this study, we use a physically-motivated internal state variable model containing a mathematical length scale to re present the material behavior in finite element (FE) simulation s of hazmat tank car shell impacts. Two goals motivated the curre nt study: (1) to reproduce with high fidelity finite deformationand temperature histories, damage, and high rate phenomena whi ch arise during the impact, as well as (2) to investigate numeri cal aspects associated with post-bifurcation mesh-dependenc y of the finite element solution. We add the mathematical length scal e to the model by adopting a nonlocal evolution equation for th e damage, as suggested by Pijaudier-Cabot and Bazant (1987) i n a slightly different context. The FE simulations consist ofa moving striker colliding against a stationary hazmat tank car a nd are carried out with the aid of ABAQUS/Explicit. The results of t hese simulations show that accounting for temperature historie s and nonlocal damage effects in the material model satisfactori ly predicts, independently of the mesh size, the failure process o the tank car impact accident.

[1]  W. Johnson Henri Tresca as the originator of adiabatic heat lines , 1987 .

[2]  Z. Bažant,et al.  Nonlocal damage theory , 1987 .

[3]  R. D. Krieg,et al.  Accuracies of Numerical Solution Methods for the Elastic-Perfectly Plastic Model , 1977 .

[4]  Nikolaos Aravas,et al.  Finite element implementation of gradient plasticity models Part I: Gradient-dependent yield functions , 1998 .

[5]  Geoffrey Ingram Taylor,et al.  The Latent Energy Remaining in a Metal after Cold Working , 1934 .

[6]  Yuebin Guo,et al.  An internal state variable plasticity-based approach to determine dynamic loading history effects on material property in manufacturing processes , 2005 .

[7]  N. Aravas On the numerical integration of a class of pressure-dependent plasticity models , 1987 .

[8]  J. Devaux,et al.  Bifurcation Effects in Ductile Metals With Nonlocal Damage , 1994 .

[9]  Jean-Baptiste Leblond,et al.  Numerical implementation and assessment of a phenomenological nonlocal model of ductile rupture , 2007 .

[10]  A. Needleman,et al.  Nonlocal effects on localization in a void-sheet , 1997 .

[11]  Mark F. Horstemeyer,et al.  Micromechanical finite element calculations of temperature and void configuration effects on void growth and coalescence , 2000 .

[12]  Viggo Tvergaard,et al.  Effects of nonlocal damage in porous plastic solids , 1995 .

[13]  A. Gurson Continuum Theory of Ductile Rupture by Void Nucleation and Growth: Part I—Yield Criteria and Flow Rules for Porous Ductile Media , 1977 .

[14]  Jonas A. Zukas,et al.  High velocity impact dynamics , 1990 .

[15]  Jeff Gordon,et al.  FINITE ELEMENT ANALYSES OF RAILROAD TANK CAR HEAD IMPACTS , 2008 .

[16]  N. Takakura,et al.  EFFECTS OF STRAIN RATE AND TEMPERATURE ON DEFORMATION RESISTANCE OF STAINLESS STEEL , 1992 .

[17]  J. Chaboche,et al.  On the creep crack-growth prediction by a non local damage formulation , 1989 .

[18]  Elias C. Aifantis,et al.  A model for finite-deformation plasticity , 1987 .

[19]  R. Borst SIMULATION OF STRAIN LOCALIZATION: A REAPPRAISAL OF THE COSSERAT CONTINUUM , 1991 .

[20]  M. F. Ashby,et al.  Intergranular fracture during power-law creep under multiaxial stresses , 1980 .