1 Organized Behavior Across the Scale Boundaries Tiara M. Dunigan MicroEP REU July 25, 2007.

Slides:



Advertisements
Similar presentations
(105) Stability and evolution of nanostructure surfaces Brown University MRSEC For the first time, we have established a direct connection among surface.
Advertisements

Lecture 1. How to model: physical grounds
" On trying daring ideas with Herb". P.M.Petroff Professor Emeritus Materials Department, University of California, Santa Barbara.
LECTURER5 Fracture Brittle Fracture Ductile Fracture Fatigue Fracture
3 – Fracture of Materials
This presentation relies on: 1) 2)
Ductile deformational processes
Plasticity, Ductility 4/15/2017 4/15/2017 1
Equilibrium and Elasticity Equilibrium Center of gravity Static Equilibrium Indeterminate Structures Elasticity Tension, Compression and Shearing pps by.
Knives and Steel. Question: If you take a steel paper clip and bend it repeatedly, will it become stiffer or less stiff with each new bend (at least initially)?
ASE324: Aerospace Materials Laboratory Instructor: Rui Huang Dept of Aerospace Engineering and Engineering Mechanics The University of Texas at Austin.
Line Defects And Ductility Ductility in a crystalline structure - the amount of plastic deformation it can undergo without fracturing - is affected by.
Deformation and Strengthening Mechanisms
What is it? What is it? (Quiz)
TEM study of ferroelastic behavior in polycrystalline LaCoO3
PY3090 Preparation of Materials Lecture 3 Colm Stephens School of Physics.
Dislocations and Strengthening
Rheology rheology What is rheology ? From the root work “rheo-” Current: flow Greek: rhein, to flow (river) Like rheostat – flow of current.
Crystallisation from melts  Why do crystals form?  What controls their shape and size?  Three aspects to the growth of a crystal are Nucleation: formation.
The Structure of Metals
Mechanical Properties of Metals
J. H. Woo, Department of Electrical & Computer Engineering Texas A&M University GEOMETRIC RELIEF OF STRAINED GaAs ON NANO-SCALE GROWTH AREA.
DISLOCATION MOVEMENT.
ANELASTICITY Some Background, Mechanisms and Recent Work Aaron Vodnick MSE 610 4/25/06.
Magnetic domain characterization  Lorentz transmission electron microscopy (LTEM) imaging techniques are used to image the magnetic domain structure of.
3 Physical Properties of Biomaterials CHAPTER
Interfaces in Solids. Coherent without strain Schematics of strain free coherent interfaces Same crystal structure (& lattice spacing) but different composition.
Lecture 3.0 Structural Defects Mechanical Properties of Solids.
Stress and Strain Unit 8, Presentation 1. States of Matter  Solid  Liquid  Gas  Plasma.
Anandh Subramaniam & Kantesh Balani
1 Strength and Ductility. 2 Determining Tensile Strength from the stress-strain curve is easy. Just locate the highest point on the curve. TS = 82 ksi.
Crystal-Air surface Interphase boundary Grain boundary Twin Boundary Stacking Faults Crystal Boundary Crystal-Crystal Low angle High angle 2D DEFECTS (Surface.
5/6/2002, Monday Summary: What we learned from this course?
STRUCTURAL IMPERFECTIONS (DEFECTS) IN CRYSTALLINE SOLIDS
Dynamics of Surface Pattern Evolution in Thin Films Rui Huang Center for Mechanics of Solids, Structures and Materials Department of Aerospace Engineering.
CAREER: Microstructure & Size Effects on Metal Plasticity at Limited Length Scale Frederic Sansoz, University of Vermont, DMR Animated snapshots.
Constant stress experiment ductile elastic Constant stress (strain varies) Constant strain (stress varies)
Plastic Deformation Permanent, unrecovered mechanical deformation  = F/A stress Deformation by dislocation motion, “glide” or “slip” Dislocations –Edge,
Deformation and Strengthening Mechanisms of Materials
Mechanical Properties & Reactivity. Review BCC → Body-Centered-Cubic 3 most common type of Crystalline Structures FCC → Face-Centered-Cubic HCP → Hexagonal-Close-Packed.
The Structure and Dynamics of Solids
Interactions of Quasiparticles
4.12 Modification of Bandstructure: Alloys and Heterostructures Since essentially all the electronic and optical properties of semiconductor devices are.
ENGR 107 – Introduction to Engineering Static Equilibrium, and Stress and Strain (Lecture #8)
Phase Field Microelasticity (PFM) theory and model is developed for most general problem of elasticity of arbitrary anisotropic, structurally and elastically.
ENHANCE OUTPUT POWER OF GAN- BASED LEDS WITH NANO-PATTERN SAPPHIRE SUBSTRATE J. J. Chen, Y. K. Su, Fellow, IEEE, C. L. Lin, S. M. Chen, W. L. Li, and C.
Mechanical Properties
© 2009 Al-Abdallat Properties of Eng. Material 1 (3) Interfacial defects Interfacial defects: Types: External surfaces, Grain boundaries, Twin boundaries.
STRUCTURAL GEOLOGY  PRIMARY & NON-TECTONIC STRUCTURES 1) PRINCIPLE OF ORIGINAL HORIZONTALITY (NICOLAS STENO ) – LAYERS OF SEDIMENTS ARE ORIGINALLY.
Namas Chandra and Sirish Namilae
Friday 12:00 Geology Seminar Dr. Lucy Flesch, Purdue University “Integration of Plate Boundary Observatory and USArray Data to Quantify the Forces Driving.
Imperfections in Solids
Ductile Deformation Processes Chapter 9 in Van der Pluijm and Marshak.
Material science & Metallurgy L D College of Engineering Mechanical Engineering 1.
Materials Science Metals and alloys.
MATERIALS SCIENCE Materials science investigates the relationships between the structures and properties of materials.
Nanoarchitecture of Nanoporous Fiber Arrays for Fuel Cell Applications: Micromechanical Stress Analysis, Experimental Fabrication & Characterization of.
L05B: Line defects (dislocations)
Dislocations and Strengthening
Plastic Deformation Permanent, unrecovered mechanical deformation
MECHANICAL PROPERTIES OF MATERIALS
THE NATURE OF MATERIALS
Dislocations Dislocations Dislocations
Description & importance
Kinetic Monte Carlo Simulation of Epitaxial Growth
Fundamental concepts of metals science
Fundamental concepts of metals science
CRYSTAL IMPERFECTIONS
PLASTIC DEFORMATION & DISLOCATIONS
Shifting Sands Desert Key Words.
Presentation transcript:

1 Organized Behavior Across the Scale Boundaries Tiara M. Dunigan MicroEP REU July 25, 2007

2 Objective To explain why the same defect pattern occurs across the scale boundaries To explain why the same defect pattern occurs across the scale boundaries

3 Outline Dislocation Dislocation Deformation Deformation Shear Stress Shear Stress Atomic Scale Atomic Scale Edge Dislocation Edge Dislocation Nanoscale Nanoscale Quantum Dots Quantum Dots Macroscale Macroscale Linear Dunes Linear Dunes Conclusion Conclusion

4 Scale Boundaries Atomic Scale Atomic Scale Nanoscale Nanoscale Macroscale Macroscale

5 Quantum Dots (nanoscale) Linear Dunes (macroscale) Edge Dislocation (atomic scale)

6 Dislocation Linear Defect where some of the atoms in the crystal lattice are misaligned Linear Defect where some of the atoms in the crystal lattice are misaligned Allows deformation to occur at the lowest possible stress level Allows deformation to occur at the lowest possible stress level Allows for elasticity in a material in order to reduce stress Allows for elasticity in a material in order to reduce stress

7 Deformation Deformation occurs when the defect is moving through a material Deformation occurs when the defect is moving through a material There are two types of deformation There are two types of deformation Plastic Plastic The material undergoes a change in shape that is not reversible The material undergoes a change in shape that is not reversible Elastic Elastic Deformation is reversible Deformation is reversible

8 Shear Stress The type of stress observed across the scale boundaries The type of stress observed across the scale boundaries stress is parallel to the face of the material stress is parallel to the face of the material

9 Edge Dislocation Takes place on the atomic scale Takes place on the atomic scale Moves under the application of external stress by the breaking of existing bonds and forming new bonds with neighboring atoms Moves under the application of external stress by the breaking of existing bonds and forming new bonds with neighboring atoms Fault in a crystalline structure Fault in a crystalline structure

10 Edge Dislocation Takes place on the atomic scale Takes place on the atomic scale Moves under the application of external stress by the breaking of existing bonds and forming new bonds with neighboring atoms Moves under the application of external stress by the breaking of existing bonds and forming new bonds with neighboring atoms Fault in a crystalline structure Fault in a crystalline structure

11 Quantum Dots

12 Misfit Dislocation Observed in Quantum Dots Observed in Quantum Dots Quantum Dots Quantum Dots Nanoparticle made from semi conducting material Nanoparticle made from semi conducting material Dislocation degrade the electronic properties of the quantum dots Dislocation degrade the electronic properties of the quantum dots

13 Quantum Dots Lattice Mismatch Lattice Mismatch Two materials featuring different lattice constants are brought together by deposition of one material on top of another Two materials featuring different lattice constants are brought together by deposition of one material on top of another In order to compensate for the lattice mismatch a misfit dislocation will form. In order to compensate for the lattice mismatch a misfit dislocation will form.

14 Linear Dunes

15 Linear Dunes Linear Dunes Linear Dunes Found in deserts around the world Found in deserts around the world When the wind strength is strong enough, individual sand grains are lifted by the direct action of the shear stress exerted by the wind on the sand surface. The change in wind direction causes the reorientation of a bed form thus producing the defect pattern The change in wind direction causes the reorientation of a bed form thus producing the defect pattern

16 Conclusion In each case the defect pattern occurs as a means to relieve stress In each case the defect pattern occurs as a means to relieve stress In each the case the type of stress induced was shear stress In each the case the type of stress induced was shear stress Shear stress causes an angle to form when shifting from the initial state to the final state Shear stress causes an angle to form when shifting from the initial state to the final state

17 Acknowledgments Dr. Ajay Malshe Dr. Ajay Malshe Professor Vickers Professor Vickers Renee Hearon Renee Hearon Dr. Arlene Maclin Dr. Arlene Maclin

18 References Lattice defects in InAs quantum dots on the GaAs(315)B surface; T. Suzuki, Y. Temko, M.C.Xu, K.Jacobi; Physical Review B 69; The American Physical Society (2004) Lattice defects in InAs quantum dots on the GaAs(315)B surface; T. Suzuki, Y. Temko, M.C.Xu, K.Jacobi; Physical Review B 69; The American Physical Society (2004) Defect reduction with quantum dots in GaN grown on sapphire substrates by molecular beam epitaxy; D. Huang, M.A. Reshchikov, F. Yun, T. King, A.A. Baski, H Morkoc; Applied Physics Letters Vol. 80 #2 (2002) Defect reduction with quantum dots in GaN grown on sapphire substrates by molecular beam epitaxy; D. Huang, M.A. Reshchikov, F. Yun, T. King, A.A. Baski, H Morkoc; Applied Physics Letters Vol. 80 #2 (2002) N. Jin-Phillipp, F. Phillipp;(1999) Defect formation in self assembling quantum dots of InGaAs: a case study of direct measurements of local strain from HREM Journal of Microscopy, Vol.194, pt.1 (1999) N. Jin-Phillipp, F. Phillipp;(1999) Defect formation in self assembling quantum dots of InGaAs: a case study of direct measurements of local strain from HREM Journal of Microscopy, Vol.194, pt.1 (1999) Dynamics of Aeolian sand ripples; Z. Csah´ok1,, C. Misbah, F. Rioual, and A. Valance; European Physical Journal Dynamics of Aeolian sand ripples; Z. Csah´ok1,, C. Misbah, F. Rioual, and A. Valance; European Physical Journal Physical Review E; Volume 60, number 1; July 1999; Nonlinear Dynamics of Aeolian Sand Ripples; Leonid Prigozhin Physical Review E; Volume 60, number 1; July 1999; Nonlinear Dynamics of Aeolian Sand Ripples; Leonid Prigozhin Geology; September 1997;Bedform Dynamics: Does the tail wag the dog?, B. Werner, G. Kocurek Geology; September 1997;Bedform Dynamics: Does the tail wag the dog?, B. Werner, G. Kocurek