M A MM A M I nstitute of M echanics & A dvanced M aterials I Crack growth analysis by a NURBS- based isogeometric boundary element method Xuan Peng, Elena.

Slides:



Advertisements
Similar presentations
Steady-state heat conduction on triangulated planar domain May, 2002
Advertisements

Parameterizing a Geometry using the COMSOL Moving Mesh Feature
An introduction to Computationnal Fracture Mechanics
Finite Elements and Fracture Mechanics Leslie Banks-Sills The Dreszer Fracture Mechanics Laboratory Department of Solid Mechanics, Materials and Systems.
Batura A.S., Orynyak I.V. IPS NASU Pisarenko’ Institute for Problems of Strength, Kyiv, Ukraine National Academy of Sciences of Ukraine Pisarenko’ Institute.
Point-wise Discretization Errors in Boundary Element Method for Elasticity Problem Bart F. Zalewski Case Western Reserve University Robert L. Mullen Case.
Presented by Robert Hurlston UNTF Conference 2011 Characterisation of the Effect of Residual Stress on Brittle Fracture in Pressure Vessel Steel.
EM 388F Term Paper: Discussion of Fracture Criterions under Impermeable and Permeable Crack Surface of Piezoelectric Materials RONG JIAO April 27, 2008.
Eurohaptics 2002 © Interactive Haptic Display of Deformable Surfaces Based on the Medial Axis Transform Jason J. Corso, Jatin Chhugani,
Chapter 17 Design Analysis using Inventor Stress Analysis Module
Sharif Rahman The University of Iowa Iowa City, IA January 2005 STOCHASTIC FRACTURE OF FUNCTIONALLY GRADED MATERIALS NSF Workshop on Probability.
J.Cugnoni, LMAF-EPFL,  Stress based criteria (like Von Mises) usually define the onset of “damage” initiation in the material  Once critical stress.
Japan-US Workshop held at San Diego on April 6-7, 2002 How can we keep structural integrity of the first wall having micro cracks? R. Kurihara JAERI-Naka.
1 Applications of addition theorem and superposition technique to problems with circular boundaries subject to concentrated forces and screw dislocations.
Developments on Shape Optimization at CIMNE October Advanced modelling techniques for aerospace SMEs.
FEM and X-FEM in Continuum Mechanics Joint Advanced Student School (JASS) 2006, St. Petersburg, Numerical Simulation, 3. April 2006 State University St.
95 學年度第 2 學期碩士論文口試 1 Derivation of the Green’s function for Laplace and Helmholtz problems with circular boundaries by using the null-field integral equation.
1 Applications of addition theorem and superposition technique to problems with circular boundaries subject to screw dislocations Reporter: Chou K. H.
Torsion cracked bar problem using BIEM S. K. Kao HR2-307/2008/01/21.
FEA Simulations Usually based on energy minimum or virtual work Component of interest is divided into small parts – 1D elements for beam or truss structures.
Computational Fracture Mechanics
M M S S V V 0 Scattering of flexural wave in a thin plate with multiple inclusions by using the null-field integral equation approach Wei-Ming Lee 1, Jeng-Tzong.
Unit 3: Solid mechanics An Introduction to Mechanical Engineering: Part Two Solid mechanics Learning summary By the end of this chapter you should have.
M M S S V V 0 Free vibration analysis of a circular plate with multiple circular holes by using addition theorem and direct BIEM Wei-Ming Lee 1, Jeng-Tzong.
M M S S V V 0 Scattering of flexural wave in thin plate with multiple holes by using the null-field integral equation method Wei-Ming Lee 1, Jeng-Tzong.
Fracture and Fragmentation of Thin-Shells Fehmi Cirak Michael Ortiz, Anna Pandolfi California Institute of Technology.
M M S S V V 0 Null-field integral equation approach for free vibration analysis of circular plates with multiple circular holes Wei-Ming Lee 1, Jeng-Tzong.
1 Adaptive error estimation of the Trefftz method for solving the Cauchy problem Presenter: C.-T. Chen Co-author: K.-H. Chen, J.-F. Lee & J.-T. Chen BEM/MRM.
Computational Fracture Mechanics
M M S S V V 0 Scattering of flexural wave in thin plate with multiple holes by using the null-field integral equation method Wei-Ming Lee 1, Jeng-Tzong.
M A MM A M I nstitute of M echanics & A dvanced M aterials I An isogeometric boundary element method for fracture modeling Xuan Peng, Cardiff University.
Meshless Animation of Fracturing Solids Mark Pauly Leonidas J. Guibas Richard Keiser Markus Gross Bart Adams Philip Dutré.
WIND ENSEMBLE FORECASTING USING AN ADAPTIVE MASS-CONSISTENT MODEL A. Oliver, E. Rodríguez, G. Montero.
Finite Element Study of Structural Discontinuities Presented By: Ike Lee and Nick Lin Project Advisor: Ioannis Korkolis.
Smooth nodal stress in the XFEM for crack propagation simulations
IMAM Institute of Mechanics and Advanced Materials
Engineering Doctorate – Nuclear Materials Development of Advanced Defect Assessment Methods Involving Weld Residual Stresses If using an image in the.
Material Model Parameter Identification via Markov Chain Monte Carlo Christian Knipprath 1 Alexandros A. Skordos – ACCIS,
École Polytechnique Fédérale de Lausanne (EPFL),
7 th Annual Workshop on Charm++ and its Applications ParTopS: Compact Topological Framework for Parallel Fragmentation Simulations Rodrigo Espinha 1 Waldemar.
Application of the Direct Optimized Probabilistic Calculation Martin Krejsa Department of Structural Mechanics Faculty of Civil Engineering VSB - Technical.
November 14, 2013 Mechanical Engineering Tribology Laboratory (METL) Arnab Ghosh Ph.D. Research Assistant Analytical Modeling of Surface and Subsurface.
By Valeriy Krutiy A Thesis Report Review Faculty of Rensselaer Polytechnic Institute in Partial Fulfillment of the Requirements for the degree of MASTER.
Adaptive Mesh Modification in Parallel Framework Application of parFUM Sandhya Mangala (MIE) Prof. Philippe H. Geubelle (AE) University of Illinois, Urbana-Champaign.
A STUDY OF THE DYNAMIC RESPONSE OF A FRACTURED TUNNEL TO PLANE WAVES Pei-cheng Xu SwRI, SanAntonio,Texas Sept. 7, 2000.
Stress constrained optimization using X-FEM and Level Set Description
Ale with Mixed Elements 10 – 14 September 2007 Ale with Mixed Elements Ale with Mixed Elements C. Aymard, J. Flament, J.P. Perlat.
Finite Element Methods and Crack Growth Simulations Materials Simulations Physics 681, Spring 1999 David (Chuin-Shan) Chen Postdoc, Cornell Fracture Group.
Numerical Simulation of Dendritic Solidification
EiEi New Approach for Efficient Prediction of Brain Deformation and Updating of Preoperative Images Based on the Extended Finite Element Method Lara M.
Ship Computer Aided Design Displacement and Weight.
Finite Element Modelling of Photonic Crystals Ben Hiett J Generowicz, M Molinari, D Beckett, KS Thomas, GJ Parker and SJ Cox High Performance Computing.
1 Rocket Science using Charm++ at CSAR Orion Sky Lawlor 2003/10/21.
CAD and Finite Element Analysis Most ME CAD applications require a FEA in one or more areas: –Stress Analysis –Thermal Analysis –Structural Dynamics –Computational.
A Fully Conservative 2D Model over Evolving Geometries Ricardo Canelas Master degree student IST Teton Dam 1976.
Global Energy Minimization for Multi-crack Growth in Linear Elastic Fracture using the Extended Finite Element Method Danas Sutula Prof. Stéphane Bordas.
4/28/2017 Modeling Carbon Fiber Composite Microstructures Using Optical Microscopy David Leonhardt.
CRACK GROWTH IN NOTCHED SPECIMEN UNDER REPETITIVE IMPACTS Presented By: Gayan Abeygunawardane-Arachchige Gayan Abeygunawardane-Arachchige Prof. Vadim Silberschmidt.
Institute of Mechanics and Advanced Materials An Adaptive Multiscale Method for Modelling of Fracture in Polycrystalline Materials Ahmad Akbari R., Pierre.
Tetrahedral Mesh Optimization Combining Boundary and Inner Node Relocation and Adaptive Local Refinement.
D. Herrero-Adan (1), Rui P.R. Cardoso (2), O.B. Adetoro (1)
Introduction Numerical model
error-driven local adaptivity in elasto-dynamics
Imperial College OF SCIENCE TECHNOLOGY AND MEDICINE Department of Aeronautics Failure Analysis of a Composite Wingbox with Impact Damage:- A Fracture.
CAD and Finite Element Analysis
On calibration of micro-crack model of thermally induced cracks through inverse analysis Dr Vladimir Buljak University of Belgrade, Faculty of Mechanical.
FEA Simulations Boundary conditions are applied
POSTPROCESSING Review analysis results and evaluate the performance
A 2D isogeometric boundary element method for linear elastic fracture
Local Defect Correction for the Boundary Element Method
Presentation transcript:

M A MM A M I nstitute of M echanics & A dvanced M aterials I Crack growth analysis by a NURBS- based isogeometric boundary element method Xuan Peng, Elena Atroshchenko, Robert Simpson, Sivakumar Kulasegaram, Stéphane Bordas Cardiff University, UK July th World Congress on Computational Mechanics WCCM XI, Barcenola, Spain

2 1/18  Background and Motivations  Modeling strategy by IGABEM Dual BEM modeling Crack tip treatment Calculation of stress intensity factors Crack growth algorithm  Numerical examples Outline

3 Motivation 2/18 Fatigue cracking of nozzle sleeve  Fatigue Fracture Failure of Structure Initiation: micro defects Loading : cyclic stress state (temperature, corrosion)  Numerical methods for crack growth Volume methods: FEM, XFEM/GFEM, Meshfree Boundary methods: BEM Bordas & Moran, 2006 XFEM+LEVEL SET

4 Motivation  Challenges in volume-based methods 3/18 Efficiency & Accuracy XFEM adaptive refinement IGABEM Direct CAD used crack direct calculation calculation stress analysis mesh Remeshing (FEM) Local mesh refinement IGA

5 Dual BEM for crack modeling  Displacement BIE: non–crack boundary and one crack surface  Traction BIE: the other crack surface 4/18

6 NURBS discretisation and collocation  Discretised BIEs NURBS(B-Spline) p=2 Discontinous Lagange p=2 5/18 Greville Abscissae:

7 Singular integration Rigid body motion: 6/18 Singularity subtraction technique:

8 Treatment of crack tip singularity 7/18 Partition of unity enrichment: Consecutive knot insertion at crack tip :

9 Evaluation of stress intensity factors  Contour integral based methods: J integral (involving J 1 and J 2 ): M integral (involving J 1 ): Singular in evaluating J 2 8/18

10 Algorithm for crack propagation Space constraint, parametric constraint Maximum hoop stress criterion Localization constraint function Calculate the moving vector 9/18

11 Numerical examples: Edge crack NURBS(B-Spline) p=2 Discontinous Lagange p=2 10/18

12 Edge crack 11/18 Crack tip refinement VS enrichment Crack opening displacementError in displacement L2 norm NURBS VS Langerange: convergence in SIFs, no crack tip treatment

13 Inclined centre crack (SGBEM, Lagrange BEM, IGABEM) IGABEM(r) :Uniform mesh (refined tip element) LBEM: discontinuous Lagrange BEM SGBEM: symmetric Galerkin BEM, Sutrahar&Paulino (2004) m : number of elements in uniform mesh along the crack surface 12/18

14 Arc crack (M integral, J integral) Uniform mesh + refined tip element Splitting parameter in J integral: 13/18 m : number of elements in uniform mesh along the crack surface

15 Crack growth from rivet holes 12 elements for each circle 3 elements for initial cracks with tip refinement 14/18

16 Crack growth through rivet holes 15/18

17 Conclusions 16/18 Dual equations for IGABEM are used to model crack The crack tip is treated by graded knot insertion or PU enrichment J integral and M integral for calculating stress intensity factors A crack growth algorithm combined with graded knot insertion is realized Future work 3D implementation on IGABEM for crack growth Crack-geometry, crack-crack intersection Crack closure Cohesive crack modeling

18 Ongoing work: 3D implementation  Penny-shaped crack under remote tension 17/18

19 thanks for YOUR attention 18/18 Thanks given to the Framework Programme 7 Initial Training Network Funding under grant number "Integrating Numerical Simulation and Geometric Design Technology” (FP7: ITN-INSIST) and RealTcut project ERC Acknowledgements: