PROBABILISTIC NONLOCAL THEORY FOR QUASIBRITTLE FRACTURE INITIATION AND SIZE EFFECT. I: THEORY

The nonlocal generalization of Weibull theory previously developed for structures that are either notched or fail only after the formation of a large crack is extended to predict the probability of failure of unnotched structures that reach the maximum load before a large crack forms, as is typical of the test of modulus of rupture (flexural strength). The probability of material failure at a material point is assumed to be a power function (characterized by the Weibull modulus and scaling parameter) of the average stress in the neighborhood of that point, the size of which is the material characteristic length. This indirectly imposes a spatial correlation. The model describes the deterministic size effect, which is caused by stress redistribution due to strain softening in the boundary layer of cracking with the associated energy release. As a basic check of soundness, it is proposed that for quasibrittle structures much larger than the fracture process zone or the characteristic length of material, the probabilistic model of failure must asymptotically reduce to Weibull theory with the weakest link model. The present theory satisfies this condition, but the classical stochastic finite-element models do not, which renders the use of these models for calculating loads of very small failure probabilities dubious. Numerical applications and comparisons to test results are left for Part II.

[1]  Ek P. Ba Scaling of quasibrittle fracture: hypotheses of invasive and lacunar fractality, their critique and Weibull connection , 1997 .

[2]  Ted Belytschko,et al.  Continuum Theory for Strain‐Softening , 1984 .

[3]  W. Weibull,et al.  The phenomenon of rupture in solids , 1939 .

[4]  Milan Jirásek,et al.  Macroscopic fracture characteristics of random particle systems , 1994 .

[5]  Yunping Xi,et al.  Statistical Size Effect in Quasi-Brittle Structures: I. Is Weibull Theory Applicable? , 1991 .

[6]  C. Bucher,et al.  On Efficient Computational Schemes to Calculate Structural Failure Probabilities , 1989 .

[7]  Drahomír Novák,et al.  ENERGETIC-STATISTICAL SIZE EFFECT IN QUASIBRITTLE FAILURE AT CRACK INITIATION , 2000 .

[8]  Wing Kam Liu,et al.  Random field finite elements , 1986 .

[9]  Z. Bažant Size Effect in Blunt Fracture: Concrete, Rock, Metal , 1984 .

[10]  D. Breysse Probabilistic formulation of damage-evolution law of cementitious composites , 1990 .

[11]  P. E. Roelfstra,et al.  Le béton numérique , 1985 .

[12]  Zdenek P. Bazant,et al.  Modulus of Rupture: Size Effect due to Fracture Initiation in Boundary Layer , 1995 .

[13]  Z. Bažant,et al.  Stability of Structures: Elastic, Inelastic, Fracture, and Damage Theories , 1993 .

[14]  Y. Uchida,et al.  FRACTURE MECHANICS APPROACH TO EVALUATION OF FLEXURAL STRENGTH OF CONCRETE , 1993 .

[15]  Yunping Xi,et al.  Statistical Size Effect in Quasi‐Brittle Structures: II. Nonlocal Theory , 1991 .

[16]  Z. Bažant,et al.  Fracture and Size Effect in Concrete and Other Quasibrittle Materials , 1997 .

[17]  Zdeněk P. Bažant,et al.  Non-local yield limit degradation , 1988 .

[18]  M. Fréchet Sur la loi de probabilité de l'écart maximum , 1928 .

[19]  ZdĚnk P. BaŽant,et al.  Scaling of quasibrittle fracture: hypotheses of invasive and lacunar fractality, their critique and Weibull connection , 1997 .

[20]  Hid N. Grouni,et al.  Methods of structural safety , 1986 .

[21]  R. Ghanem,et al.  Stochastic Finite Elements: A Spectral Approach , 1990 .

[22]  Alberto Carpinteri,et al.  Multifractal scaling law for the nominal strength variation of concrete structures , 1993 .

[23]  R. Fisher,et al.  Limiting forms of the frequency distribution of the largest or smallest member of a sample , 1928, Mathematical Proceedings of the Cambridge Philosophical Society.

[24]  M. Jirásek,et al.  Particle Model for Quasibrittle Fracture and Application to Sea Ice , 1995 .

[25]  Z. Bažant,et al.  SIZE EFFECT IN TENSILE AND COMPRESSION FRACTURE OF CONCRETE STRUCTURES : COMPUTATIONAL MODELING AND DESIGN , 2022 .

[26]  Ek P. Ba Scaling of quasibrittle fracture: asymptotic analysis , 1997 .

[27]  Z. Bažant,et al.  Scaling of quasibrittle fracture: asymptotic analysis , 1997 .

[28]  P. Petersson Crack growth and development of fracture zones in plain concrete and similar materials , 1981 .

[29]  Shinozuka,et al.  Statistical and fractal aspects of size effect in quasibrittle structures : Conspectus of recent results , 2022 .

[30]  Alberto Carpinteri,et al.  Size effects on nominal tensile strength of concrete structures: multifractality of material ligaments and dimensional transition from order to disorder , 1995 .

[31]  D. Fokwa,et al.  Spatial Variability in Concrete: Nature, Structure, and Consequences , 1994 .

[32]  S. Xia,et al.  A nonlocal damage theory , 1987 .

[33]  L. H. C. Tippett,et al.  ON THE EXTREME INDIVIDUALS AND THE RANGE OF SAMPLES TAKEN FROM A NORMAL POPULATION , 1925 .

[34]  Z. Bažant,et al.  Nonlocal Continuum Damage, Localization Instability and Convergence , 1988 .

[35]  Drahomír Novák,et al.  PROBABILISTIC NONLOCAL THEORY FOR QUASIBRITTLE FRACTURE INITIATION AND SIZE EFFECT. II: APPLICATION , 2000 .

[36]  Z. Bažant,et al.  Nonlocal microplane model for fracture, damage, and size effect in structures , 1990 .

[37]  A. Hillerborg,et al.  Analysis of crack formation and crack growth in concrete by means of fracture mechanics and finite elements , 1976 .