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Finite Element Modeling of Nacre
Austen Motily with Dr. Mark Garnich Sponsored by the Department of Mechanical Engineering and EPSCoR
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Nacre Also known as mother of pearl
Composite material found in mollusk shells Two phases Aragonite Organic protein matrix Barthelat et al. [1]
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Nacre Unique periodic arrangement About 95% aragonite
“repeating” structure Hexagonal platelets About 95% aragonite Brittle Doesn’t absorb much energy About 5% organic protein Ductile Easily deformed Barthelat et al. [1]
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Fracture Toughness The amount of energy a material can absorb before it breaks Nacre has a high fracture toughness 95 % of the nacre is not very tough The unique arrangement of nacre results in its increased toughness
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Why is Toughness important?
Materials must be resistant to flaws Tough materials resist rapid crack propagation Energy absorption is important in structural stability Katti et al. [2]
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Finite Element Modeling
Create a model of the structure Separate the model into small elements Use the finite element method to predict material behavior Analyze the results Abaqus® was used for this research Marks, Laurence [3]
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Representative Volume Element (RVE)
Nacre platelets are about one micron thick Would be almost impossible to model thousands of layers of Nacre Create a small volume representative of overall behavior Zuo and Wei [4]
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Representative Volume Element (RVE)
Difficulties Conceptually more difficult Must implement correct boundary conditions Have to achieve symmetry
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Two-Dimensional (2D) Model
Create a model to compare to results of Zuo and Wei Tension test Simplify as much as possible Start with elastic behavior Implement plastic behavior of organic protein phase Zuo and Wei [4]
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Results of 2D Elastic Simulation
Verify correct geometrical behavior Achieve symmetry
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Results of 2D Plastic Simulation
Protein: elastic linear-plastic material Equivalent to model of Zuo and Wei
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Results of 2D Plastic Simulation
Similar general behavior
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Three-Dimensional (3D) Model
Include depth in the model Elastic-plastic behavior of protein Verify correct implementation of boundary conditions Stress-strain behavior should be the same
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Results of 3D Simulation
Same geometrical behavior as 2D simulation
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Results of 3D Simulation
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Results of 3D Simulation
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Comparison of 2D and 3D Simulations
Same stress-strain behavior for the two simulations
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Comparison of Stress-strain curves
Plastic portion slopes are different
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Discrepancy Between Stress Strain Curves
Distribution of stress along vertical axis Protein behavior converted from shear stress/strain Abaqus® requires normal stress-strain behavior for input Difference in slope of plastic portion of stress-strain curve is too large to be attributed to these factors
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Verification Using the Mathematical Model
Solve the differential equation used by Zuo and Wei Use Matlab® to solve the differential equation Create stress-strain curve and compare to results of Zuo and Wei
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Verification Using the Mathematical Model
Similar to Abaqus® simulation results
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Next Steps Simulate nacre under shear loading
Compare with experimental results from Menig et al. The tension test produced a lot of shearing action in model New simulation will contain different boundary conditions indicative of a shear simulation Menig et al. [5]
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Next Steps More advanced models that incorporate the complex hexagonal platelet arrangement Implement a more realistic elastic- plastic model for the organic protein phase Simulate other loading scenarios such as bending or compression Menig et al. [5]
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References Barthelat F, Dastjerdi AK, Rabiei R An improved failure criterion for biological and engineered staggered composites. Journal of The Royal Society Interface 10, 1-10. Katti DR, Katti KS, Sopp JM, Sarikaya M D Finite Element Modeling of Mechanical Response in Nacre-Based Hybrid Nanocomposites. Computational and Theoretical Polymer Science 11, Marks L Bolted Joints in Finite Element Models. SSA Limited. Zuo S, Wei Y Microstructure observation and mechanical behavior modeling for limnetic nacre. Acta Mechanica Sinica 24, Menig R, Meyers MH, Meyers MA, Vecchio KS Quasi-Static and Dynamic Mechanical Response of Haliotis Rufescens (Abalone) Shells. Acta Materialia 48,
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