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McCormick School of Engineering. Outline. Simple 1-D ModelingSMA Multivariant ModelSingle Crystal ModelPolycrystalline modelComparisons with experimental dataRecent Experimental Data Implications for Further Work. McCormick School of Engineering. Basic Shape Memory Phenomena. Shape Memory Effe
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1. McCormick School of Engineering Micromechanics for SMAs & Aging in Polymer Composites Professor Cate Brinson
Dr. Miinshiou Huang
Kathy Issen
Alex Bekker
Xiujie Gao
2. McCormick School of Engineering Outline Simple 1-D Modeling
SMA Multivariant Model
Single Crystal Model
Polycrystalline model
Comparisons with experimental data
Recent Experimental Data
Implications for Further Work
3. McCormick School of Engineering Basic Shape Memory Phenomena Shape Memory Effect
Pseudoelasticity
4. McCormick School of Engineering Simple 1-D SMA Model Phenomenological Constitutive Law
Split Martensite Volume Fraction:
Kinetic Law based on Phase Diagram
Multivalued, path-dependent function
Simple algebraic kinetic description possible
Location and direction of loading path determines kinetics
5. McCormick School of Engineering “Phase Diagram” Kinetics Divide any thermomechanical loading path into segments
6. McCormick School of Engineering Simple 1-D Constitutive Law Robust and accurate
Easy to program
Used in control algorithms
Used in finite element codes
Coupled with Heat Transfer equations
Limited to 1-D, wire response
Need 3D model as convenient!
7. McCormick School of Engineering Finite Element Example - Active Frequency Tuning
8. McCormick School of Engineering SMA Microstructure of Single Crystal Self-accommodated variants (T-induced)
Hierarchical twin microstructure
Reorientation and Detwinning key for single and polycrystal response
Experimental data for 3D severely lacking
9. McCormick School of Engineering A Multivariant SMA Model
10. McCormick School of Engineering A Multivariant SMA Model
11. McCormick School of Engineering Groups of Variants
12. McCormick School of Engineering Multivariant Single Crystal Model
13. McCormick School of Engineering Habit Plane and Correspondence Variants
14. McCormick School of Engineering Conversion Process Under Load
15. McCormick School of Engineering Single Crystal Comparison: Biaxial Load
16. McCormick School of Engineering Orientation Dependence
17. McCormick School of Engineering Orientation Dependence The anisotropy factor in the cubic system is defined as
A = 2 C44 /(C11 - C12) = 12.8 for Cu-14Al-4.1Ni (wt%)
The ratio of the maximum Young’s modulus to the minimum in the same alloy
Emax / Emin = 10
Multivariant Model:
A = 1 Emax / Emin = 1
(assumed A, M isotropic with same modulus)
Strong anisotropy of austenite should be accounted for in modeling different initial moduli, transformation stresses
Difficulty: Eshelby inclusion analysis difficult for anisotropy
CuAlNi has 2H periodic stacking structure model currently optimized for 9R/18R
18. McCormick School of Engineering Orientation Dependence
19. McCormick School of Engineering Polycrystalline Model
20. McCormick School of Engineering Temperature Induced Transformation
21. McCormick School of Engineering Shape Memory Effect
22. McCormick School of Engineering Pseudoelasticity
23. McCormick School of Engineering Pseudoelasticity
24. McCormick School of Engineering Reuss Approximation
25. McCormick School of Engineering Uniaxial and Triaxial Stress States
26. McCormick School of Engineering Experiment & Prediction
27. McCormick School of Engineering Experiment and Prediction
28. McCormick School of Engineering Experiment and Prediction
29. McCormick School of Engineering Model Prediction for DV>0
30. McCormick School of Engineering Multivariant Model Summary Multivariant Model predicts a variety of shape memory phenomena
Multivariant Model can account for:
tension/compression asymmetry
multiaxial stress states
modulus dependent on stress state
Polycrystalline model has trouble with:
transformation stress magnitudes
strain hardening
Anisotropy of material could be key
Modification for 2H/3R crystallography
Code is computationally intensive
More Experiments needed
31. McCormick School of Engineering Recent Experimental Studies Single crystal CuAlNi experiments
Optical Microscopy
SEM
EBSD
All with in situ loading
Experiments designed to provide key modeling information
Experiments on NiTi planned
32. McCormick School of Engineering SEM Experimental Set-Up
33. McCormick School of Engineering SEM Loading Stage
34. McCormick School of Engineering SEM Image Showing Habit Plane, Twins SEM image at 2000x
Uniaxial loading
Variant ID possible when habit plane and twin plane visible
35. McCormick School of Engineering EBSD in Austenite Phase
36. McCormick School of Engineering Digital Camera Observation in MTS
37. McCormick School of Engineering Stress-Strain Response For previous thermal/loading cycle
38. McCormick School of Engineering Implications of Experiments Model criterion for b1’ and g1’ should differ
Resistance gap between b1’ and g1’
Note single M-variant across width of specimen
NiTi: need to account for detwinning (HV CV)
Work best criteria for variant selection (from tension/compression experiments)
Still need biaxial, bending experiments for more complex load states
Need microscopy resolution to ID variants
39. McCormick School of Engineering
40. McCormick School of Engineering Future Modeling Take one step back:
Remove interaction energy
Simplify Calculations
Retain and expand variant structure
Account for CV, HV:
Detwinning possible
Implement resistance gap:
41. McCormick School of Engineering Preliminary Result Interaction Energy removed
Speedy computation
Ultimately, can remove other layers as discover necessary and unnecessary baggage for 3D polycrystalline response
42. McCormick School of Engineering Summary SMA Polycrystalline 1-D Modeling Tractable
SMA Variant structure and response complex
Microscopy Experiments with in situ loading help provide insight
Micromechanics modeling appropriate and promising
Several micromechanics methods under development