Slow crack growth, its modeling and crack-layer approach: A review

A review of empirical equations for slow crack growth under fatigue and creep conditions is presented. The crack propagation rate is commonly expressed as a function of stress intensity factor or energy release rate. A concept of crack driving force and crack stability analysis is employed to predic...

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Published in:International journal of engineering science Vol. 83; pp. 6 - 41
Main Author: Chudnovsky, A.
Format: Journal Article
Language:English
Published: Elsevier Ltd 01-10-2014
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Abstract A review of empirical equations for slow crack growth under fatigue and creep conditions is presented. The crack propagation rate is commonly expressed as a function of stress intensity factor or energy release rate. A concept of crack driving force and crack stability analysis is employed to predict crack behavior under different loading conditions; the concept of crack growth resistance, such as an effective surface energy, is used. It is shown that for a stable crack propagation (the energy release rate is a decreasing function of crack length) crack growth equation results from the crack equilibrium condition, if the crack resistance is assumed to be constant. Experimental studies demonstrate that crack growth resistance is not constant, but changes with crack propagation. Formation of the so-called process zone appears to be responsible for the changes. Process zone (PZ) is a material reaction to stress concentration at crack tip and it is commonly observed under fatigue and creep conditions in most engineering materials. For an unstable crack growth (the energy release rate is an increasing function of crack length) the effect of PZ even more dramatic; for example, in a perfectly homogeneous elastic solid slow crack growth would be impossible without the stabilizing effect of PZ. A system of a crack and PZ is referred to as crack-layer (CL). CL driving forces that are thermodynamic forces associated with crack and PZ growth are introduced. CL growth equations are employed to explain the observed variations of crack growth resistance commonly known as R-curve behavior. The evolution of the process zone in a complex stress field is illustrated by an experiment demonstrating how process zone accelerates and decelerates crack growth. Modeling of the crack–process zone interaction is a challenging problem; recent advances in computational techniques make it solvable. The CL approach is illustrated on an example of engineering thermoplastics. Applications to lifetime prediction of structural components, as well as toughness and durability of materials are discussed.
AbstractList A review of empirical equations for slow crack growth under fatigue and creep conditions is presented. The crack propagation rate is commonly expressed as a function of stress intensity factor or energy release rate. A concept of crack driving force and crack stability analysis is employed to predict crack behavior under different loading conditions; the concept of crack growth resistance, such as an effective surface energy, is used. It is shown that for a stable crack propagation (the energy release rate is a decreasing function of crack length) crack growth equation results from the crack equilibrium condition, if the crack resistance is assumed to be constant. Experimental studies demonstrate that crack growth resistance is not constant, but changes with crack propagation. Formation of the so-called process zone appears to be responsible for the changes. Process zone (PZ) is a material reaction to stress concentration at crack tip and it is commonly observed under fatigue and creep conditions in most engineering materials. For an unstable crack growth (the energy release rate is an increasing function of crack length) the effect of PZ even more dramatic; for example, in a perfectly homogeneous elastic solid slow crack growth would be impossible without the stabilizing effect of PZ. A system of a crack and PZ is referred to as crack-layer (CL). CL driving forces that are thermodynamic forces associated with crack and PZ growth are introduced. CL growth equations are employed to explain the observed variations of crack growth resistance commonly known as R-curve behavior. The evolution of the process zone in a complex stress field is illustrated by an experiment demonstrating how process zone accelerates and decelerates crack growth. Modeling of the crack-process zone interaction is a challenging problem; recent advances in computational techniques make it solvable. The CL approach is illustrated on an example of engineering thermoplastics. Applications to lifetime prediction of structural components, as well as toughness and durability of materials are discussed.
Author Chudnovsky, A.
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  organization: Civil & Materials Engineering Department, Fracture Mechanics and Materials Durability Laboratory, The University of Illinois at Chicago, 842 West Taylor Street, Chicago, IL 60607-7023, United States
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Keywords Crack-layer
Process zone
Crack growth
Fracture propagation
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  ident: 10.1016/j.ijengsci.2014.05.015_b0205
  article-title: Continuum model of medium with cracks
  publication-title: Journal of the Engineering Mechanics Division
  doi: 10.1061/JMCEA3.0002642
  contributor:
    fullname: Kachanov
– start-page: 531
  year: 1972
  ident: 10.1016/j.ijengsci.2014.05.015_b0075
  article-title: Spectrum loading and crack growth
  contributor:
    fullname: Wheeler
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Snippet A review of empirical equations for slow crack growth under fatigue and creep conditions is presented. The crack propagation rate is commonly expressed as a...
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SubjectTerms Constants
Crack growth
Crack propagation
Crack-layer
Cracks
Energy release rate
Fatigue failure
Fracture mechanics
Fracture propagation
Mathematical analysis
Mathematical models
Process zone
Title Slow crack growth, its modeling and crack-layer approach: A review
URI https://dx.doi.org/10.1016/j.ijengsci.2014.05.015
https://search.proquest.com/docview/1642216285
Volume 83
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