Last lecture Introduction to materials science and engineering Atoms / electron configuration.

Slides:



Advertisements
Similar presentations
Fundamental Concepts Crystalline: Repeating/periodic array of atoms; each atom bonds to nearest neighbor atoms. Crystalline structure: Results in a lattice.
Advertisements

Nanochemistry NAN 601 Dr. Marinella Sandros
CRYSTAL STRUCTURE- Chapter 3 (atomic arrangement) Why study this?
THE STRUCTURE OF CRYSTALLINE SOLIDS
How do atoms ARRANGE themselves to form solids? Unit cells
Lecture 2.1 Crystalline Solids. Poly-crystalline solids - Grains Mono-crystalline solids- Whiskers, Wafers.
CRYSTAL STRUCTURE.
When dealing with crsytalline materials, it is often necessary to specify a particular point within a unit cell, a particular direction or a particular.
Wigner-Seitz Cell The Wigner–Seitz cell around a lattice point is defined as the locus of points in space that are closer to that lattice point than to.
Miller indices and crystal directions
The Muppet’s Guide to: The Structure and Dynamics of Solids 6. Crystal Growth & Defects.
Crystallography and Structure
Introduction to Solids. 3 Classes of Solids Amorphous – No long range order Polycrystalline – Order within grains Single Crystal – Regular, repeated pattern.
The indeterminate situation arises because the plane passes through the origin. After translation, we obtain intercepts. By inverting them, we get.
THE STRUCTURE OF CRYSTALLINE SOLIDS
Chapter 1 The Crystal Structure of Solids Describe three classifications of solids— amorphous, polycrystalline, and single crystal. Discuss the concept.
Recall Engineering properties are a direct result of the structure of that material. Microstructure: –size, shape and arrangement of multiple crystals.
PX431 Structure and Dynamics of Solids PART 2: Defects and Disorder Diane
Structure of Solids Objectives By the end of this section you should be able to: Calculate atomic packing factors (HW) Compare bcc, fcc and hcp crystal.
ENG2000: R.I. Hornsey Crystal: 1 ENG2000 Chapter 3 Crystals.
L03A: Chapter 3 Structures of Metals & Ceramics The properties of a material depends on the arrangement of atoms within the solid. In a single crystal.
Instructor: Dr. Upali Siriwardane
Discussion Notes Farzana Ansari Feb 14 & 16, 2012.
CE 336 Material Properties Atomic Structure determines: Physical Properties Chemical Properties Biological Properties Electromagnetic Properties.
ME 381R Fall 2003 Micro-Nano Scale Thermal-Fluid Science and Technology Lecture 3: Microstructure of Solids Dr. Li Shi Department of Mechanical Engineering.
Solid State Physics (1) Phys3710
EEE539 Solid State Electronics 1. Crystal Structure Issues that are addressed in this chapter include:  Periodic array of atoms  Fundamental types of.
Chapter 1 Crystal Structures. Two Categories of Solid State Materials Crystalline: quartz, diamond….. Amorphous: glass, polymer…..
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 defect classification point defects self-vacancy, self-interstitial interstitial interstitial and substitutional impurities point defect pairs,
MATERIALS SCIENCE Week 2 STRUCTURE OF MATERIALS. Why Study Crystal Structure of Materials? The properties of some materials are directly related to their.
MSE 630 Introduction to Solid State Physics Topics: Structure of Crystals classification of lattices reciprocal lattices bonding.
W.D. Callister, Materials science and engineering an introduction, 5 th Edition, Chapter 3 MM409: Advanced engineering materials Crystallography.
Crystallographic Points, Directions, and Planes. ISSUES TO ADDRESS... How to define points, directions, planes, as well as linear, planar, and volume densities.
Bravais Lattices in 2D In 2D there are five ways to order atoms in a lattice Primitive unit cell: contains only one atom (but 4 points?) Are the dotted.
Prolog Text Book: C.Kittel, "Introduction to Solid State Physics", 8th ed.,Wiley (2005) Website:
STRUCTURE OF SOLID MATERIALS CLASSIFICATION OF SOLIDS SOLIDS CLASSIFIED AS CRYSTALLINE, AMORPHOUS OR A COMBINATION OF THE TWO. CRYSTALLINE - BUILT UP OF.
CRYSTAL STRUCTURE.
The Structure and Dynamics of Solids
Crystalline Solids BLB 12 th Chapter 12 Sections 1-3, 5.
Properties of engineering materials
ENGINEERING REQUIREMENTS OF MATERIAL Fabrication RequirementsService RequirementsEconomics Requirements.
MS – Module I.
Engg Physics Crystal Structure
STRUCTURE OF MATERIALS. The make up of an atom The simple idea of an atom is that an atom has a nucleus and negatively charged electrons whirling around.
STRUCTURE OF MATERIALS. Three types of atomic bonds: Covalent bonds Ionic bonds Metallic bonds.
ME 330 Engineering Materials
Scanning Electron Microscopy Image of a Ruthenium-Palladium-Aluminium-Alloy MSE 250 Friday, Jan 10, 2003 Quiz next Friday Crystal Structure Professor Dave.
MATERIALS SCIENCE Materials science investigates the relationships between the structures and properties of materials.
Materials Engineering
Crystal Structure and Crystallography of Materials
Properties of engineering materials
Crystallographic Points, Directions, and Planes.
THE SPACE LATTICE AND UNIT CELLS CRYSTAL SYSTEMS AND BRAVAIS LATTICES.
CHAPTER 3: STRUCTURE OF CRYSTALLINE SOLIDS
Concepts of Crystal Geometry
Structure and manufacturing Properties of Metals
Semiconductor Processing Single Crystal Silicon
Lecture 2.1 Crystalline Solids.
Crystallographic Points, Directions, and Planes.
Crystal and Amorphous Structure in Materials
Lecture 2.1 Crystalline Solids.
Chapter 1 Crystallography
Crystal and Amorphous Structure
IMPERFECTIONS IN SOLIDS
MSE420/514: Session 1 Crystallography & Crystal Structure
MODULE 2 - Introduction to Basic Crystallography
Crystal Structure Acknowledgement: This slides are largely obtained from Dr.Neoh Siew Chin UniMAP on the subject Material Engineering.
Chapter 3: Crystal & Amorphous structure in materials Part 1
Crystalline Solids (고체의 결정구조)
Presentation transcript:

last lecture Introduction to materials science and engineering Atoms / electron configuration

today Bonding in solids Structure of crystal solids

Bonding Forces and Energies distance r

The Periodic Table METALS NONMETALS INTERMEDIATE increasing electronegativity

Ionic Bonding Covalent Bonding Ionic Bonding Covalent Bonding e.g. sodium chloride e.g. methane

Metallic Bonding

Bonding Energies low high

Crystalline Structures

amorphouscrystalline

Example: Glass quartz (crystalline) quartz glass (amorphous) Si 4+ O 2- glass (amorphous)

Crystalline Structures simple cubic body-centered cubic (bcc) bcc fcc

Hexagonal Crystal Structures hcp unit cell

Stacking Sequence of Close-Packed Structures first plane A first plane A and second plane B first plane A, second plane B and third plane C: fcc first plane A, second plane B and third plane A: hcp

FCC and BCC Solid Sphere Model fcc unit cell bcc unit cell R R = atomic radius a = unit cell length / lattice constant a a

Crystalline Structures of Materials

Lattice Parameters

Crystal Systems

How to define a direction Vector of convenient length (pass through origin) Project the vector to the axes (and measure in a, b, and c) Multiply or divide these numbers by common factor to get smallest set of integers Write them down as [uvw]

Miller Indices: Crystallographic Directions

Miller Indices: Crystallographic Directions (Miller Bravais)

How to define a plane Plane may not include origin! Determine the intercepts with appropriate axes as a, b, and c Take reciprocals (no intercept means infinity  reciprocal of infinity = 0) Multiply or divide these numbers by common factor to get smallest set of integers Write them down as (hkl)

Miller Indices: Lattice Planes intersection points: 1/2 a, 1/2b, 1/2c reciprocal values: (222)

Defects Point defects Linear defects 2-dimensional defects

Point Defects self-interstitial vacancy

Impurity Atoms interstitial substitutional

Dislocations: Edge Dislocation Burgers vector inserted half plane dislocation line

Dislocations: Screw Dislocation Burgers vector dislocation line

Grain Boundaries Ni-Base Superalloy Waspalloy 50µm high-angle grain boundary (  >15°) low-angle grain boundary

next Properties of materials