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Handbook of Peridynamic Modeling.

This handbook covers the peridynamic modeling of failure and damage. Peridynamics is a reformulation of continuum mechanics based on the integration of interactions rather than the spatial differentiation of displacements. The book extends the classical theory of continuum mechanics to allow unguide...

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Detaylı Bibliyografya
Yazar: Bobaru, Florin
Diğer Yazarlar: Foster, John T., Geubelle, Philippe H., Silling, Stewart A.
Materyal Türü: e-Kitap
Dil:İngilizce
Baskı/Yayın Bilgisi: Milton : CRC Press LLC, 2016.
Edisyon:1st ed.
Seri Bilgileri:Advances in Applied Mathematics Series
Konular:
Online Erişim:Full-text access
OPAC'ta görüntüle
İçindekiler:
  • Cover
  • Half Title
  • Title Page
  • Copyright Page
  • Contents
  • Foreword
  • Preface
  • List of Figures
  • List of Tables
  • Contributors
  • I: The Need for Nonlocal Modeling and Introduction to Peridynamics
  • 1 Why Peridynamics?
  • 1.1 The mixed blessing of locality
  • 1.2 Origins of nonlocality in a model
  • 1.2.1 Long-range forces
  • 1.2.2 Coarsening a fine-scale material system
  • 1.2.3 Smoothing of a heterogeneous material system
  • 1.3 Nonlocality at the macroscale
  • 1.4 The mixed blessing of nonlocality
  • References
  • 2 Introduction to Peridynamics
  • 2.1 Equilibrium in terms of integral equations
  • 2.2 Material modeling
  • 2.2.1 Bond-based materials
  • 2.2.2 Relation between bond densities and flux
  • 2.2.3 Peridynamic states
  • 2.2.4 Ordinary state-based materials
  • 2.2.5 Correspondence materials
  • 2.2.6 Discrete particles as peridynamic bodies
  • 2.2.7 Setting the horizon
  • 2.2.8 Linearized peridynamics
  • 2.3 Plasticity
  • 2.3.1 Bond-based microplastic material
  • 2.3.2 LPS material with plasticity
  • 2.4 Damage and fracture
  • 2.4.1 Damage in bond-based models
  • 2.4.2 Damage in ordinary state-based material models
  • 2.4.3 Damage in correspondence material models
  • 2.4.4 Nucleation strain
  • 2.5 Treatment of boundaries and interfaces
  • 2.5.1 Bond-based materials
  • 2.5.2 State-based materials
  • 2.6 Emu numerical method
  • 2.7 Conclusions
  • References
  • II: Mathematics, Numerics, and Software Tools of Peridynamics
  • 3 Nonlocal Calculus of Variations and Well-Posedness of Peridynamics
  • 3.1 Introduction
  • 3.2 A brief review of well-posedness results
  • 3.3 Nonlocal balance laws and nonlocal vector calculus
  • 3.4 Nonlocal calculus of variations- an illustration
  • 3.5 Nonlocal calculus of variations- further discussions
  • 3.6 Summary
  • References
  • 4 Local Limits and Asymptotically Compatible Discretizations.
  • 4.1 Introduction
  • 4.2 Local PDE limits of linear peridynamic models
  • 4.3 Discretization schemes and discrete local limits
  • 4.4 Asymptotically compatible schemes for peridynamics
  • 4.5 Summary
  • References
  • 5 Roadmap for Software Implementation
  • 5.1 Introduction
  • 5.2 Evaluating the internal force density
  • 5.3 Bond damage and failure
  • 5.4 The tangent stiffness matrix
  • 5.5 Modeling contact
  • 5.6 Meshfree discretizations for peridynamics
  • 5.7 Proximity search for identification of pairwise interactions
  • 5.8 Time integration
  • 5.8.1 Explicit time integration for transient dynamics
  • 5.8.2 Estimating the maximum stable time step
  • 5.8.3 Implicit time integration for quasi-statics
  • 5.9 Example simulations
  • 5.9.1 Fragmentation of a brittle disk resulting from impact
  • 5.9.2 Quasi-static simulation of a tensile test
  • 5.10 Summary
  • References
  • III: Material Models and Links to Atomistic Models
  • 6 Constitutive Modeling in Peridynamics
  • 6.1 Introduction
  • 6.2 Kinematics, momentum conservation, and terminology
  • 6.3 Linear peridynamic isotropic solid
  • 6.3.1 Plane elasticity
  • 6.3.1.1 Plane stress
  • 6.3.1.2 Plane strain
  • 6.3.2 "Bond-based" theories as a special case
  • 6.3.3 On the role of the influence function
  • 6.3.4 Other elasticity theories
  • 6.4 Finite Deformations
  • 6.4.1 Invariants of peridynamic scalar-states
  • 6.5 Correspondence models
  • 6.5.1 Non-ordinary correspondence models for solid mechanics
  • 6.5.2 Ordinary correspondence models for solid mechanics
  • 6.6 Plasticity
  • 6.6.1 Yield surface and flow rule
  • 6.6.2 Loading/unloading and consistency
  • 6.6.3 Discussion
  • 6.7 Non-ordinary models
  • 6.7.1 A non-ordinary beam model
  • 6.7.2 A non-ordinary plate/shell model
  • 6.7.3 Other non-ordinary models
  • 6.8 Final Comments
  • References
  • 7 Links between Peridynamic and Atomistic Models.
  • 7.1 Introduction
  • 7.2 Molecular dynamics
  • 7.3 A meshfree discretization of peridynamic models
  • 7.4 Upscaling molecular dynamics to peridynamics
  • 7.4.1 A one-dimensional nonlocal linear springs model*
  • 7.4.2 A three-dimensional embedded-atom model(Omitted)
  • 7.5 Computational speedup through upscaling
  • 7.6 Concluding remarks
  • References
  • 8 Absorbing Boundary Conditions with Verification
  • 8.1 Introduction
  • 8.2 A PML for state-based peridynamics
  • 8.2.1 Two-dimensional (2D), state-based peridynamics review
  • 8.2.2 Auxiliary field formulation and PML application
  • 8.2.3 Numerical examples
  • 8.3 Verification of cone and center crack problems
  • 8.3.1 Dimensional analysis of Hertzian cone crack development in brittle elastic solids
  • 8.3.2 State-based verification of a cone crack
  • 8.3.3 Bond-based verification of a center crack
  • 8.4 Verification of an axisymmetric indentation problem
  • 8.4.1 Formulation
  • 8.4.2 Analytical verification
  • References
  • IV: Modeling Material Failure and Damage
  • 9 Dynamic Brittle Fracture as an Upscaling of Unstable Mesoscopic Dynamics
  • 9.1 Introduction
  • 9.2 The macroscopic evolution of brittle fracture as a small horizon limit of mesoscopic dynamics
  • 9.3 Dynamic instability and fracture initiation
  • 9.4 Localization of dynamic instability in the small horizon-macroscopic limit
  • 9.5 Free crack propagation in the small horizon-macroscopic limit
  • 9.6 Summary
  • References
  • 10 Crack Branching in Dynamic Brittle Fracture
  • 10.1 Introduction
  • 10.2 A brief review of literature on crack branching
  • 10.2.1 Theoretical models and experimental results on dynamic brittle fracture and crack branching
  • 10.2.2 Computations of dynamic brittle fracture based on FEM
  • 10.2.3 Dynamic brittle fracture results based on atomistic modeling.
  • 10.2.4 Dynamic brittle fracture based on particle and lattice-based methods
  • 10.2.5 Phase-field models in dynamic fracture
  • 10.2.6 Results on dynamic brittle fracture from peridynamic models
  • 10.3 Brief review of the bond-based peridynamic model
  • 10.4 An accurate and efficient quadrature scheme
  • 10.5 Peridynamic results for dynamic fracture and crack branching
  • 10.5.1 Crack branching in soda-lime glass
  • 10.5.1.1 Load case 1: stress on boundaries
  • 10.5.1.2 Load case 2: stress on pre-crack surfaces
  • 10.5.1.3 Load case 3: velocity boundary conditions
  • 10.5.2 Crack branching in homalite
  • 10.5.2.1 Load case 1: stress on boundaries
  • 10.5.2.2 Load case 2: stress on pre-crack surfaces
  • 10.5.2.3 Load case 3: velocity boundary conditions
  • 10.5.3 Influence of sample geometry
  • 10.5.3.1 Load case 1: stress on boundaries
  • 10.5.3.2 Load case 2: stress on pre-crack surfaces
  • 10.5.3.3 Load case 3: velocity boundary conditions
  • 10.6 Discussion of crack branching results
  • 10.7 Why do cracks branch?
  • 10.8 The importance of nonlocal modeling in crack branching
  • 10.9 Conclusions
  • References
  • 11 Relations between Peridynamic and Classical Cohesive Models
  • 11.1 Introduction
  • 11.2 Analytical PD-based normal cohesive law
  • 11.2.1 Case 1- No bonds have reached critical stretch
  • 11.2.2 Case 2- Bonds have exceeded the critical stretch
  • 11.2.3 Numerical approximation of PD-based cohesive law
  • 11.3 PD-based tangential cohesive law
  • 11.3.1 Case 1- No bonds have reached critical stretch
  • 11.3.2 Case 2- Bonds have exceeded the critical stretch
  • 11.4 PD-based mixed-mode cohesive law
  • 11.5 Conclusions
  • References
  • 12 Peridynamic Modeling of Fiber-reinforced Composites
  • 12.1 Introduction
  • 12.2 Peridynamic analysis of a lamina
  • 12.3 Peridynamic analysis of a laminate
  • 12.4 Numerical results
  • 12.5 Conclusions.
  • 12.6 Appendix A: PD material constants of a lamina
  • 12.6.1 Simple shear
  • 12.6.2 Uniaxial stretch in the fiber direction
  • 12.6.3 Uniaxial stretch in the transverse direction
  • 12.6.4 Biaxial stretch
  • 12.7 Appendix B: Surface correction factors for a composite lamina
  • 12.8 Appendix C: PD interlayer and shear bond constants of a laminate
  • 12.9 Appendix D: Critical Stretch Values for Bond Constants
  • References
  • 13 Peridynamic Modeling of Impact and Fragmentation
  • 13.1 Introduction
  • 13.2 Convergence studies and damage models that influence the damage behavior
  • 13.2.1 Damage-dependent critical bond strain
  • 13.2.2 Critical bond strain dependence on compressive strains along other directions
  • 13.2.3 Surface effect in impact problems
  • 13.2.4 Convergence study for impact on a glass plate
  • 13.3 Impact on a multilayered glass system
  • 13.3.1 Model description
  • 13.3.2 A comparison between FEM and peridynamics for the elastic response of a multilayered system to impact
  • 13.4 Computational results for damage progression in the seven-layer glass system
  • 13.4.1 Damage evolution for the cross section
  • 13.4.2 Damage evolution in the first layer
  • 13.4.3 Damage evolution in the second layer
  • 13.4.4 Damage evolution in the fourth layer
  • 13.4.5 Damage evolution in the seventh layer
  • 13.5 Conclusions
  • References
  • V: Multiphysics and Multiscale Modeling
  • 14 Coupling Local and Nonlocal Models
  • 14.1 Introduction
  • 14.2 Energy-based blending schemes
  • 14.2.1 The Arlequin method
  • 14.2.1.1 Description of the coupling model
  • 14.2.1.2 A numerical example
  • 14.2.2 The morphing method
  • 14.2.2.1 Overview
  • 14.2.2.2 Description of the morphing method
  • 14.2.2.3 One-dimensional analysis of ghost forces
  • 14.2.2.4 Numerical examples
  • 14.3 Force-based blending schemes*.
  • 14.3.1 Convergence of peridynamic models to classical models.