A constitutive description of the inelastic response of ceramics

The objective of the article is to present a unified model for the dynamic mechanical response of ceramics under compressive stress states. The model incorporates three principal deformation mechanisms: (i) lattice plasticity due to dislocation glide or twinning; (ii) microcrack extension; and (iii) granular flow of densely packed comminuted particles. In addition to analytical descriptions of each mechanism, prescriptions are provided for their implementation into a finite element code as well as schemes for mechanism transitions. The utility of the code in addressing issues pertaining to deep penetration is demonstrated through a series of calculations of dynamic cavity expansion in an infinite medium. The results reveal two limiting behavioral regimes, dictated largely by the ratio of the cavity pressure p to the material yield strength σY. At low values of p/σY, cavity expansion occurs by lattice plasticity and hence its rate diminishes with increasing σY. In contrast, at high values, expansion occurs by microcracking followed by granular plasticity and is therefore independent of σY. In the intermediate regime, the cavity expansion rate is governed by the interplay between microcracking and lattice plasticity. That is, when lattice plasticity is activated ahead of the expanding cavity, the stress triaxiality decreases (toward more negative values) which, in turn, reduces the propensity for microcracking and the rate of granular flow. The implications for penetration resistance to high-velocity projectiles are discussed. Finally, the constitutive model is used to simulate the quasi-static and dynamic indentation response of a typical engineering ceramic (alumina) and the results compared to experimental measurements. Some of the pertinent observations are shown to be captured by the present model whereas others require alternative approaches (such as those based on fracture mechanics) for complete characterization.

[1]  Michael F. Ashby,et al.  The failure of brittle porous solids under compressive stress states , 1986 .

[2]  M. Ortiz,et al.  Computational modelling of impact damage in brittle materials , 1996 .

[3]  D. C. Drucker,et al.  Soil mechanics and plastic analysis or limit design , 1952 .

[4]  W. Weibull A Statistical Distribution Function of Wide Applicability , 1951 .

[5]  T. Holmquist,et al.  A comparison of ceramic material models , 2002 .

[6]  Rami Masri,et al.  Dynamic spherical cavity expansion in a pressure sensitive elastoplastic medium , 2004 .

[7]  G. R. Johnson,et al.  Fracture characteristics of three metals subjected to various strains, strain rates, temperatures and pressures , 1985 .

[8]  Horacio Dante Espinosa,et al.  A finite deformation continuum\discrete model for the description of fragmentation and damage in brittle materials , 1998 .

[9]  Sikhanda Satapathy,et al.  Dynamic spherical cavity expansion in brittle ceramics , 2001 .

[10]  D. Clarke GRAIN BOUNDARIES IN POLYCRYSTALLINE CERAMICS , 1987 .

[11]  A. Evans,et al.  Mechanisms and Mechanics Governing the Indentation of Polycrystalline Alumina , 2008 .

[12]  Thomas A. Duffey,et al.  Finite cavity expansion method for near-surface effects and layering during earth penetration , 1998 .

[13]  Michael F. Ashby,et al.  The damage mechanics of brittle solids in compression , 1990 .

[14]  Rebecca M. Brannon,et al.  The Use of Sphere Indentation Experiments to Characterize Ceramic Damage Models , 2010 .

[15]  G. R. Johnson,et al.  Response of boron carbide subjected to large strains, high strain rates, and high pressures , 1999 .

[16]  Stephan Bless,et al.  Computational modeling of the penetration response of a high-purity ceramic , 2002 .

[17]  A. Evans,et al.  The Influence of Material Properties and Confinement on the Dynamic Penetration of Alumina by Hard Spheres , 2009 .

[18]  R. Bagnold Experiments on a gravity-free dispersion of large solid spheres in a Newtonian fluid under shear , 1954, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[19]  D. B. Longcope,et al.  Penetration into ductile metal targets with rigid spherical-nose rods , 1995 .

[20]  P. Hazell,et al.  Crack softening damage model for ceramic impact and its application within a hydrocode , 1997 .

[21]  Arunachalam M. Rajendran,et al.  Modeling the shock response of silicon carbide, boron carbide and titanium diboride , 1996 .