Brittle fracture in disordered materials: A spring network model

Author:

Curtin W. A.,Scher H.

Abstract

A model for investigating the influence of distributed disorder on the failure of brittle materials is introduced. The model assumes that microstructural features of a material can be represented by simple linear springs with a failure threshold, and that the entire material can be represented by a connected network of such springs. Distributed disorder is introduced by allowing spring-to-spring variations in spring characteristics such as the modulus and the failure strain. The conditions under which such a spring network model is valid for studying failure are discussed. The consequences of distributed residual stress disorder on macroscopic mechanical behavior are then studied using the network model, and a brittle to ductile-like transition in the stress-strain behavior is observed with increasing disorder. All the qualitative features of the network results can be described theoretically by a statistical analysis of this problem. Finally, notch tests are performed to evaluate the strength and toughness of the ductile-like materials as compared to the uniform (no disorder) material, and the ductile-like material is found to have (i) a larger work of fracture, (ii) comparable strength in the presence of processing flaws, and (iii) the possibility of larger toughness. Based on these results, the possibility of observing such ductile-like behavior in real composite materials is discussed.

Publisher

Springer Science and Business Media LLC

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics,General Materials Science

Reference21 articles.

1. 19 This behavior may be compared to that which prevails in the case of distributed breakdown strengths. There, all nonlinearity is due to accumulated damage with no release of residual strain and so at any point on the macroscopic σ-ε curve, the effective modulus is precisely σ/ε. Therefore, extensive nonlinear regimes in the distributed εc case must be accompanied by considerable modulus reductions.

2. Toughening by Stress-Induced Microcracking in Two-Phase Ceramics

3. VI. The phenomena of rupture and flow in solids

4. Microcracking in Ceramics Induced by Thermal Expansion or Elastic Anisotropy

5. Transformation and Microcrack Toughening as Complementary Processes in ZrO2-Toughened Al2O3

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