Lecture 9: Two-Dimensional Defects

Slides:



Advertisements
Similar presentations
INTRODUCTION TO CERAMIC MINERALS
Advertisements

L05C: Surface defects CASTING
Physical Metallurgy 17 th Lecture MS&E 410 D.Ast DRAFT UNFINISHED !!!
ChE 553 Lecture 2 Surface Notation 1. Objectives Learn Notation To Describe the Structure Of Surfaces –Bravis Lattices: BCC, FCC, HCP –Miller Indicies:
Lec. (4,5) Miller Indices Z X Y (100).
1. Chapter 4: Imperfections in Solids 2 Introduction Metals Alloys Solid solutions New/second phase Solute (guest) Solvent (host)
CONDENSED MATTER PHYSICS PHYSICS PAPER A BSc. (III) (NM and CSc.) Harvinder Kaur Associate Professor in Physics PG.Govt College for Girls Sector -11, Chandigarh.
Dislocations – Linear Defects –Two-dimensional or line defect –Line around which atoms are misaligned – related to slip Edge dislocation: –extra half-plane.
Crystalline Arrangement of atoms. Chapter 4 IMPERFECTIONS IN SOLIDS The atomic arrangements in a crystalline lattice is almost always not perfect. The.
Crystallographic Aspects of Dislocations
Dislocations zBasic concepts yedge dislocation yscrew dislocation zCharacteristics of Dislocations ylattice strains zSlip Systems yslip in single crystals.
CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality.
Lecture 2: Crystal Structure PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Discussion Notes Farzana Ansari Feb 14 & 16, 2012.
Interfaces in Solids. Coherent without strain Schematics of strain free coherent interfaces Same crystal structure (& lattice spacing) but different composition.
Chapter 5 - Imperfections in Solids
Twinning Dislocation Reactions
Anandh Subramaniam & Kantesh Balani
PHYS 430/603 material Laszlo Takacs UMBC Department of Physics
Crystal Structure A “unit cell” is a subdivision of the lattice that has all the geometric characteristics of the total crystal. The simplest choice of.
Crystal-Air surface Interphase boundary Grain boundary Twin Boundary Stacking Faults Crystal Boundary Crystal-Crystal Low angle High angle 2D DEFECTS (Surface.
Crystal defect classification point defects self-vacancy, self-interstitial interstitial interstitial and substitutional impurities point defect pairs,
Closest Packing of Spheres How do spheres (atoms) pack to best fill space?? The concept of closest packing is important for understanding many solid structures.
PH 0101 UNIT 4 LECTURE 71 PH0101 UNIT 4 LECTURE-7 POINT IMPERFECTIONS LINE IMPERFECTIONS SURFACE IMPERFECTIONS VOLUME IMPERFECTIONS.
IMPERFECTIONS IN SOLIDS
Lecture 22: The mechanism of plastic deformation, part 2
Lecture 20: The mechanism of plastic deformation PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Last lecture Introduction to materials science and engineering Atoms / electron configuration.
Crystal Structure of Solids
Interactions of Quasiparticles
Lecture 7 Lattice Defects, Vacancies PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
© 2009 Al-Abdallat Properties of Eng. Material 1 (3) Interfacial defects Interfacial defects: Types: External surfaces, Grain boundaries, Twin boundaries.
Engg Physics Crystal Structure
Lecture 17: Diffusion PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
ME 330 Engineering Materials
부산대학교 재료공학부 계면공학 연구실 [Mechanical Properties]  Mechanical Properties: mechanical properties of a material are those properties that involve a reaction.
Materials Science Chapter 4 Disorder in solid Phases.
Crystal Structure and Crystallography of Materials
3. Crystal interfaces and microstructure
MATERIALS SCIENCE Materials science investigates the relationships between the structures and properties of materials.
Materials Engineering
Materials Engineering
Simulation methodology
Crystal Structure and Crystallography of Materials
Chapter 26 IMAGING STRAIN FIELDS
SOLID STATE By: Dr.DEPINDER KAUR.
Crystallographic Points, Directions, and Planes.
SOLID STATE By: Dr.Bhawna.
Indira Gandhi Centre for Atomic Research, India
Dislocations and Strengthening
Visualization of Dislocations in a 3-D Nanoindentation Simulation
CHAPTER 4: IMPERFECTIONS IN SOLIDS
Lecture 9/2: Dislocations
Lecture 8: Dislocations
Chapter 3:week 8 Solid State Chemistry Imperfections in Solid Materials Band theory, insulators, semi conductors p-type and n-type semiconductors and.
Lattice Defects.
Dislocations Dislocations Dislocations
Imperfections in Solid Materials
اساسا سه نوع فصل مشترک مهم در فلزات وجود دارد
Crystallographic Points, Directions, and Planes.
Lecture 1: Stacking of atoms
IMPERFECTIONS IN SOLIDS
Description & importance
Instructor: Yuntian Zhu
CRYSTAL IMPERFECTIONS
Crystal Structure and Crystallography 재료구조론
Grains in Metals.
Chapter 3: Crystal & Amorphous structure in materials Part 1
DSC Lattice, Grain Boundary Dislocations - Basics
Presentation transcript:

Lecture 9: Two-Dimensional Defects PHYS 430/603 material Laszlo Takacs UMBC Department of Physics

Surface defects that do not violate nearest neighbor coordination Stacking fault fcc ABCABCACABCABCABCABC hcp ABABABABCABABABABABA ABABABCACACACACACACA Twinning (mirror image) fcc ABCABCABCBACBACBACBA hcp not for a (0 0 0 1) plane, more complex possible Energy: of the order of 0.1 J/m2 ~ 0.6 eV/nm2 - rather small Al Cu (J/m2) Stacking fault 0.2 0.075 Twin 0.12 0.045

Construction of a general grain boundary in 2-d Step 1: Start with two identical copies of the same lattice

Step 2: Rotate one copy of the lattice relative to the other Step 2: Rotate one copy of the lattice relative to the other. The angle of rotation is a characteristic of the boundary.

Step 3: Overlay the two lattices Step 3: Overlay the two lattices. The relative positions (shift) has to be specified

Step 4: Define the position and direction of the grain boundary

Step 5: Remove one or the other copy of the lattice on both sides Step 5: Remove one or the other copy of the lattice on both sides. It is not always clear if an atom should be taken out or left in place. Also, this is a purely geometric procedure, energy relaxation results in local distortions.

Definition of twist and tilt (asymmetric and symmetric) boundaries

Energy of symmetrical tilt boundaries in Al Energy of symmetrical tilt boundaries in Al. The tilt axis is a <1 1 0> direction.

Low angle tilt boundary Low angle tilt boundary. It can be represented by a line of edge dislocations.

Low angle tilt boundary in YBaCuO Low angle tilt boundary in YBaCuO. The numbers indicate the number of lattice planes between dislocations.

A low angle twist boundary produced by a network of screw dislocations

Coincidence Site Lattice, CSL This description is only applicable to certain rotation angles; but these situations are useful as reference and nature tends to favor them as well. Rotation by 26.57° (not 36.87°) Take a 2x1 rectangle diagonal: 5a, sides are 2x and x (5a)2 = (2x)2 + x2 x = a √5 Area of CSL unit cell = = 5 * area of lattice unit cell

Coherent tilt boundary in Cu and in CuBi alloy Coherent tilt boundary in Cu and in CuBi alloy. Notice that the bright Bi atoms are all located in the grain boundary.

DSC (displacement shift complete) lattice DSC (displacement shift complete) lattice. Includes every lattice point of both lattices. The finest grid used to describe grain boundaries.

Shift in the GB can be described as a dislocation in the DSC lattice Shift in the GB can be described as a dislocation in the DSC lattice. Notice that the lattice sites do not change, only how far one or the other grain extends changes.

The Bernal polyhedra. The close-packed structures can be described as a combination of only regular tetrahedra and octahedra.

A semi-coherent phase boundary

Surface forces acting at the edge of a liquid drop

Angles at the boundary of three phases