Special 2-D and 3-D Geometrically Nonlinear Finite Elements for Analysis of Adhesively Bonded Joints By Raul H. Andruet Dissertation submitted to the Faculty of the Virginia Polytechnic Institute and State University in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Engineering Science and Mechanics APPROVED: __________________________ ____________________________ D. A. Dillard, Chairman S.M. Holzer, Co-chairman __________________________ ____________________________ E. R. Johnson B.J. Love __________________________ R. D. Kriz April, 1998 Blacksburg, Virginia Special 2-D and 3-D Geometrically Nonlinear Finite Elements for Analysis of Adhesively Bonded Joints By Raul H. Andruet David A. Dillard, Chairman Siegfried M. Holzer, Co-chairman Engineering Science and Mechanics (ABSTRACT) Finite element models have been successfully used to analyze adhesive bonds in actual structures, but this takes a considerable amount of time and a high computational cost. The objective of this study is to develop a simple and cost-effective finite element model for adhesively bonded joints which could be used in industry. Stress and durability analyses of crack patch geometries are possible applications of this finite element model. For example, the lifetime of aging aircraft can be economically extended by the application of patches bonded over the flaws located in the wings or the fuselage. Special two and three- dimensional adhesive elements have been developed for stress and displacement analyses in adhesively bonded joints. Both the 2-D and 3-D elements are used to model the whole adhesive system: adherends and adhesive layer. In the 2-D elements, adherends are represented by Bernoulli beam elements with axial deformation and the adhesive layer by plane stress or plane strain elements. The nodes of the plane stress-strain elements that lie in the adherend-adhesive interface are rigidly linked with the nodes of the beam elements. The 3-D elements consist of shell elements that represent the adherends and solid brick elements to model the adhesive. This technique results in smaller models with faster convergence than ordinary finite element models. The resulting mesh can represent arbitrary geometries of the adhesive layer and include cracks. Since large displacements are often observed in adhesively bonded joints, geometric nonlinearity is modeled. ii 2-D and 3-D stress analyses of single lap joints are presented. Important 3-D effects can be appreciated. Fracture mechanics parameters are computed for both cases. A stress analysis of a crack patch geometry is presented. A numerical simulation of the debonding of the patch is also included. iii Acknowledgements I would like to express my sincere appreciation and gratitude to Dr. S.M. Holzer for his teaching, guidance, patience, friendship, and support. I admire him as a teacher, as a leader, and, above all, as a friend. I also want to express my gratitude to Dr. D.A. Dillard for providing me expert advice in the mechanics of adhesives, and for his support and understanding. I want to extend my gratitude to Dr. E.R. Johnson, Dr. B.J. Love, and R.D. Kriz for serving on the dissertation committee, and to Dr R.H. Plaut for serving on my examining committee. Aida Mendez-Delgado for her smile, support, care, and for being always there when I needed her. My infinite gratitude goes to Marcela Ruiz-Funez, Gustavo Maldonado, Daniela Verthelyi and Eduardo Romano for their friendship and hospitality. To them I am forever grateful. I am grateful to all my friends who made my stay in Virginia an unforgettable experience, to Virgilio Centeno, Tatiana Boluarte, Paul Prato, Clara Diaz, Eduardo Miles, Alberto and Patricia Perez Rigau, Juan Sabate, Margarita, Cristina y Mario Sanchez, Diana Rubio, Mercedes Pastor, Luis Moreschi , Guillermo Aberboch, Daniel Quinones, and many other exceptional friends. Very special thanks to Jacem Tissaoui, Samruam Tongtoe, and Amara Loulizi . I learned a great deal and was honored to work with them. My gratitude goes forever to Gail, Siegfried, Mathew, and Michael Holzer for their generosity, friendship, and hospitality, for making me feel at home. iv I would like to thank Gustavo Maldonado and Sergio Preidikman for their friendship and the long conversations we had about this work. Special thanks to Azar Alizadeh for her dedication and patient in helping me with my writing, and for being an unconditional friend. This work was partially supported by CASS, Center for Adhesive and Sealant Sciences. Finally, I would like to dedicate this work to my family; to my parents, Titi and Nene, to my brothers, Carlos, Luis y Mario, to my sisters in law, Ines, Raquel, and Viviana, and to my nieces and nephews, Florencia, Maria Belen, Tomas, Maria Jose, Agustin, Virginia, and Maria Ines. v Table of Contents 1 Introduction 1.1 Background 1 1.2 Objectives 2 1.3 Significance 2 2 Literature Review 2.1 Adhesively Bonded Joints 4 2.1.1 Closed-Form Solutions 5 2.1.2 Numerical Solutions 7 2.1.3 Finite Element Solutions 8 2.1.4 Two-dimensional Solutions 9 2.1.5 Three-dimensional Solutions 11 2.1.6 Nonlinear Finite Element Methods 12 2.2 Crack Analysis Using Finite Elements 17 2.2.1 Two-dimensional Crack Analysis 21 2.2.2 Three-dimensional Crack Analysis 29 2.3 Fatigue Life Prediction of Adhesively-Bonded Joints 32 3 Geometric Nonlinear Finite Element Formulation 3.1 Introduction 37 3.2 Nonlinear Finite Element Analysis 37 3.3 Isoparametric Finite Element Discretization 43 3.4 Solution Technique for Nonlinear Finite Element 45 Analysis 4 Two-Dimensional Adhesive Finite Element 4.1 Introduction 47 4.2 Formulation 47 vi 4.2.1 Adherends 48 4.2.1 Adhesive 50 4.2.3 Thermal and Moisture Effects 54 4.2.5 Single Lap Joint Example 55 4.3 Fracture Mechanics Analysis 60 4.5 Conclusions 37 5 Three-Dimensional Adhesive Finite Element 5.1 Introduction 68 5.2 Adherends 69 5.3 Adhesive 74 5.4 Thermal and Moisture Effects 79 5.5 Examples 80 5.5.1 Single Lap Joint 80 5.5.2 Crack-Patch Geometry 89 5.5.3 Geometrically Nonlinear Single Lap Joint 97 5.6 Conclusions 104 6 Analysis of Fatigue-Crack Growth in Adhesively Bonded Joints 6.1 Introduction 106 6.2 Determination of Load Characteristics 107 6.3 Fracture Mechanics Parameters 108 6.4 Fatigue-Crack-Growth Law 113 6.5 Determination of Crack Extensions 114 6.6 Algorithm to Simulate Debond 115 6.7 Examples 116 6.7.1 Crack Lap Shear Geometry 117 6.7.2 Crack-Patch Repair Geometry 121 vii 6.8 Summary and Conclusions 126 7 Conclusions and Recommendations 7.1 Introduction 128 7.2 Conclusions 130 7.3 Future Work and Recommendations 131 References 133 Appendix A 139 Vita 150 viii List of Figures Figure 2.1. Single lap joint configuration. 5 Figure 2.2. Geometric nonlinearities in a finite element: (a) Large displacements, small strains; (b) Large displacements, large strains. 14 Figure 2.3. Graphical representation of the Newton-Raphson method. 15 Figure 2.4. Graphical representation of the Riks/Wemper method. 16 Figure 2.5. Three fractures modes. 18 Figure 2.6. J-integral notation and parameters. 21 Figure 2.7. Quarter-point two-dimensional continuum finite element. 22 Figure 2.8. Collapsed quarter-point two-dimensional continuum finite element. 23 Figure 2.9. Arbitrary body with a region with stress concentration. 23 Figure 2.10. Modified crack closure integral method parameters and notation. 28 Figure 2.11. Virtual crack extension method (from Nikishkov and Atluri 1987). 31 Figure 2.12. Fatigue crack extension law. 33 Figure 2.13. Crack-Patch repair configuration. 35 Figure 3.1 Large displacements of a body in stationary Cartesian coordinate system. 38 Figure 3.2 Modified Newton-Raphson method. 46 Figure 4.1 Two dimensional adhesive finite element. 48 Figure 4.2 Nonlinear beam, generalized displacements. 49 Figure 4.3 Nonlinear beam, generalized displacements. 50 Figure 4.4 Single lap joint specimen. 55 Figure 4.5 Finite element model of a simple lap joint 56 Figure 4.6. Peel stress distribution for a single lap joint. 57 Figure 4.7 Shear stress distribution for a single lap joint. 57 Figure 4.8 Finite element model of a simple lap joint for a Geometric Nonlinear Analysis. 58 Figure 4.9. Peel stress distribution for a single lap joint. Geometric nonlinearity is included. 58 ix Figure 4.10. Shear stress distribution for a single lap joint. Geometric nonlinearity included. 59 Figure 4.11. Modified Crack Closure Integral Method. 60 Figure 4.12. Double Cantilever Beam (DCB) Specimen. 61 Figure 4.13. Crack Lap Shear (CLS) Specimen. 62 Figure 4.14. Strain energy release rate vs. applied load. 63 Figure 4.15. Total strain energy release rate results of ASTM round-robin crack lap shear specimen including new results from ADH2D approach. 64 Figure 4.16. Mode mix results of ASTM round-robin crack lap shear specimen including new results from ADH2D approach. 65 Figure 4.17. Comparison between different analyses of strain energy release rate values vs. debond length for the equal adherend thickness CLS specimen of the round-robin study (Johnson 1989). 66 Figure 5.1. Configuration of the adhesive element. 68 Figure 5.2. Adherend element configuration. 69 Figure 5.3. Degrees of freedom per node. 70 Figure 5.4. 3-D adhesive finite element configuration. 74 Figure 5.5. Finite and parent elements. 75 Figure 5.6. Adhesive element finite element configuration. 75 Figure 5.7. Three-dimensional single lap joint geometry. 81 Figure 5.8. Single lap joint: symmetry condition. 81 Figure 5.9. Finite element mesh of the single lap joint. 82 Figure 5.10. Displaced finite element mesh of the single lap joint. 83 Figure 5.11. Peel stress (s ) distribution in the midplane of the adhesive layer zz of the single lap joint example. 84 Figure 5.12. Shear stress (t ) distribution in the midplane of the adhesive xz layer of the single lap joint example. 85 Figure 5.13. Shear stress (t ) distribution in the midplane of the adhesive xy layer of the single lap joint example. 86 Figure 5.14. Shear stress (t ) distribution in the midplane of the adhesive yz layer of the single lap joint example. 87 Figure 5.15. Axial stress (s ) distribution in the midplane of the adhesive zz layer of the single lap joint example. 88 x
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