TOPIC 2: SOLIDIFICATIONS, IMPERFECTIONS IN SOLIDS & DIFFUSIONS

Slides:



Advertisements
Similar presentations
Chapter 5 Defects in solids
Advertisements

Crystal Lattice Imperfections
L05C: Surface defects CASTING
Chapter 5: Imperfections in Solids
CHAPTER 4: IMPERFECTIONS IN SOLIDS
A (0001) plane for an HCP unit cell is show below.
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Imperfections in Solid Materials R. Lindeke ENGR 2110.
CHAPTER 4: IMPERFECTIONS IN SOLIDS
IMPERFECTIONS IN SOLIDS Week Solidification - result of casting of molten material –2 steps Nuclei form Nuclei grow to form crystals – grain structure.
The Muppet’s Guide to: The Structure and Dynamics of Solids 6. Crystal Growth & Defects.
The Muppet’s Guide to: The Structure and Dynamics of Solids 6. Crystal Growth & Defects.
ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect material.
MSE 528 Crystal structures and Defects Fall 2010.
Chapter 3- CRYSTAL SYSTEMS General lattice that is in the shape of a parallelepiped or prism. a, b, and c are called lattice parameters. x, y, and z here.
Solidification and Grain Size Strengthening
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.
Dislocations and Strengthening
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
The Structure of Metals
Solidification and Heat Treatment
Why are we interested IMPERFECTIONS IN SOLIDS ?
Solidification & Crystalline Imperfections
Why are we interested IMPERFECTIONS IN SOLIDS ?
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Schmid's Law F r = F cos λ A 0 = Acos ψ τ r = σ cos ψ cos λ.
ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect material.
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Chapter 4- ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Solidification and Crystalline Imperfections
Types of Materials Metals : –Strong, ductile –high thermal & electrical conductivity –opaque Polymers/plastics : Covalent bonding  sharing of e’s –Soft,
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Chapter 4-15 Grain boundaries: are boundaries between crystals. are produced by the solidification process, for example. have a change in crystal orientation.
Chapter 4- ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Vacancies: -vacant atomic sites in a structure. Self-Interstitials: -"extra" atoms positioned between atomic sites. POINT DEFECTS CHAPTER 4: IMPERFECTIONS.
IMPERFECTIONS IN SOLIDS
STRUCTURAL IMPERFECTIONS (DEFECTS) IN CRYSTALLINE SOLIDS
CHAPTER 3: INELASTIC DEFORMATION. 6 Vacancies: -vacant atomic sites in a structure. Self-Interstitials: -"extra" atoms positioned between atomic.
The Structure and Dynamics of Solids
A (0001) plane for an HCP unit cell is show below.
Imperfections in Solids
Materials Science Chapter 4 Disorder in solid Phases.
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Material science & Metallurgy L D College of Engineering Mechanical Engineering 1.
Materials Science Metals and alloys.
1 Length Scale of Imperfections Vacancies, impurities dislocations Grain and twin boundaries Voids Inclusions precipitates point, line, planar, and volumetric.
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Chapter 6: Imperfections in Solids
Chapter 5: Imperfections in Solids
DR S. & S. S. GHANDHY GOVERNMENT ENGINEERING COLLEGE , SURAT.
Crystal Lattice Imperfections
Imperfections in the Atomic and Ionic Arrangements
CRITICAL RESOLVED SHEAR STRESS
Play movie  LINE DEFECTS Dislocations: • are line defects,
Dislocations and Strengthening
CHAPTER 4: IMPERFECTIONS IN SOLIDS
CHAPTER 4: IMPERFECTIONS IN SOLIDS
CHAPTER 4: IMPERFECTIONS IN SOLIDS
Chapter 3:week 8 Solid State Chemistry Imperfections in Solid Materials Band theory, insulators, semi conductors p-type and n-type semiconductors and.
Imperfections in Solid Materials
Solidification and Crystalline Imperfection
Chapter 6: Imperfections in Solids
CRYSTAL SYSTEMS General lattice that is in the shape of a parallelepiped or prism. a, b, and c are called lattice parameters. x, y, and z here are called.
IMPERFECTIONS IN SOLIDS
CHAPTER 3: CRYSTAL STRUCTURES & PROPERTIES
CHAPTER 4: IMPERFECTIONS IN SOLIDS
TOPIC 2: Diffusion in Solids
Chapter ISSUES TO ADDRESS... What types of defects arise in solids? Can the number and type of defects be varied and controlled? How do defects affect.
Imperfections in Solids
Presentation transcript:

TOPIC 2: SOLIDIFICATIONS, IMPERFECTIONS IN SOLIDS & DIFFUSIONS ISSUES TO ADDRESS... • What are the solidification mechanisms? • What types of defects arise in solids? • Can the number and type of defects be varied and controlled? • How do defects affect material properties? • Are defects undesirable?

Imperfections in Solids Solidification- result of casting of molten material 2 steps Nuclei form (nucleation : formation of stable nuclei) Nuclei grow to form crystals – grain structure (nuclei: small particles of a new phase formed by a phase change (i.e. solidification) which can grow until the phase change is complete). Start with a molten material – all liquid nuclei crystals growing grain structure liquid Adapted from Fig.4.14 (b), Callister 7e. Crystals grow until they meet each other

Solidification: Nucleation Processes Homogeneous nucleation nuclei form in the bulk of liquid metal Heterogeneous nucleation much easier since stable “nucleus” is already present The formation of very small regions of a new solid phase at the interfaces of solid impurities. Could be wall of mold or impurities in the liquid phase

Homogeneous nucleation Simplest case of nucleation Occurs when the metal itself provide the atoms to form nuclei. E.g. : The case of a pure metal solidifying. When a pure liquid metal is cooled below its equilibrium freezing temperature to a sufficient degree, numerous homogeneous nuclei are created by slow-moving atoms bonding together. Requires a considerable amount of undercooling , ~ several hundreds degrees (Undercooling: Cooling a metal below the transformation temperature without obtaining the transformation). . For a nucleus to be stable so that it can grow into a crystal and must reach a critical size**. (the minimum radius which a particle of a new phase formed by nucleation must have to become a stable nucleus).

Heterogeneous nucleation Nucleation that occurs in a liquid on the surfaces of its container, insoluble impurities or other structural material which lower the critical free energy required to form a stable nucleus. Since large amounts of undercooling do not occur during industrial casting operations (usually only ~ 0.1-10oC), thus the nucleation must be heterogeneous and not homogeneous. heterogeneous nucleation takes place more quickly since the foreign particles act as a scaffold for the crystal to grow on, thus eliminating the necessity of creating a new surface and the incipient surface energy requirements.

Cooling curve for pure metal (without impurities) Liquid cools as specific heat is removed (A-B). Undercooling (B-C). Nucleation begins (C). Homogeneous nucleation. Heat is released causing an increase in the temp of the liquid (C-D). Solidification continue at constant temp. until complete at E.

Growth of crystals in liquid metal and formation of grain structure After stable nuclei have been form in a solidifying metal, these nuclei will grow into crystals. When, solidification of the metal is completed, the crystal join together in different orientations and form crystal boundaries. Solidified metal containing many crystals is called polycrystalline.

Polycrystalline Materials Grain Boundaries regions between crystals transition from lattice of one region to that of the other slightly disordered low density in grain boundaries high mobility high diffusivity high chemical reactivity Adapted from Fig. 4.7, Callister 7e.

Solidification Grains can be - equiaxed (roughly same size in all directions) - columnar (elongated grains) ~ 8 cm heat flow Shell of equiaxed grains due to rapid cooling (greater T) near wall Columnar in area with less undercooling Adapted from Fig. 4.12, Callister 7e. Grain Refiner - added to make smaller, more uniform, equiaxed grains.

Equiaxed grains: grains which are approximately equal in all directions and which have random crystallographic orientations. Commonly found adjacent to a cold mold wall Columnar grains: long, thin grains in a solidified polycrystalline structure. These grains are formed in the interior of solidified metal ingots when heat flow is slow and uniaxial during solidification. The columnar grains have grown perpendicular to the mold faces since large thermal gradients were present in those directions.

increase

Dendrite – The treelike structure of the solid that grows as molten metal freezes (when an undercooled liquid solidifies).

Microstructure - dendrites Cross section sample

Effect of cooling rate (solidification rate) Rapid cooling leads to greater nucleation and more smaller grains. Slow cooling leads to slower nucleus formation and larger grains. More grains means more grain boundary.

Solidification defects (casting) Shrinkage: contraction of a casting during solidification Gas porosity – bubbles of gas trapped within a casting during solidification, caused by the lower solubility of the gas in the solid compared with in the liquid. Mold material defects – wrong mold material selection Pouring metal defects – e.g. material freezing before it completely fills the mold cavity. Metallurgical defects – hot tears and hot spots: Hot tears are failures in the casting that occur as the casting cools, because the metal is weak when it is hot and the stresses in the material can cause the casting to fail as it cools. Solution, proper casting design is needed. Hot spots: surface area of the casting that very hard because it chilled more quickly than surrounding. Can be avoided by proper cooling practises or by changing the chemical composition of the metal.

Continuous casting of steel ingots (a) General setup; (b) closed up of the mold arrangement (After H. E. McGannon (ed.), “ The making, shaping and treating of steel” ,United States Steel Corp., 1971.

Defect in the crystalline structure & Diffusion of atom

Defect in the crystalline structure

Imperfections in Solids There is no such thing as a perfect crystal. What are these imperfections? Why are they important? Many of the important properties of materials are due to the presence of imperfections.

Defect in the crystalline structure can have an tremendous effect on a materials behavior. We can modify and improve many of the physical, electrical, magnetic and optical properties of crystalline materials by controlling the imperfections in their lattice structure.

Types of Imperfections • Vacancy atoms • Interstitial atoms • Substitutional atoms Point defects • Dislocations Line defects • Grain Boundaries Area defects Casting defect Volume defect

(1). Point defects Vacancies, Interstitial and substitutional …move by diffusion

Schottky and Frenkel defects in an ionic crystal Schottky: a defect consisting of a cation and anion vacancies pair. Frenkel : In an ionic solid, a cation-vacancy and cation interstitial pair.

Point Defects Vacancy self- interstitial • Vacancies: -vacant atomic sites in a structure. Vacancy distortion of planes • Self-Interstitials: -"extra" atoms positioned between atomic sites. self- interstitial distortion of planes

Point Defects in Alloys Two outcomes if impurity (B) added to host (A): • Solid solution of B in A (i.e., random dist. of point defects) OR Substitutional solid soln. (e.g., Cu in Ni) Interstitial solid soln. (e.g., C in Fe) • Solid solution of B in A plus particles of a new phase (usually for a larger amount of B) Second phase particle --different composition --often different structure.

(2) Line Defects Dislocations: Schematic of Zinc (HCP): slip steps • are line defects, • slip between crystal planes result when dislocations move, • produce permanent (plastic) deformation. Schematic of Zinc (HCP): • before deformation • after tensile elongation slip steps Adapted from Fig. 7.8, Callister 7e.

Imperfections in Solids Linear Defects (Dislocations) Are one-dimensional defects around which atoms are misaligned Edge dislocation: extra half-plane of atoms inserted in a crystal structure b  to dislocation line Screw dislocation: spiral planar ramp resulting from shear deformation b  to dislocation line Burger’s vector, b: measure of lattice distortion. Refer to magnitude and direction of lattice distortion associated with a dislocation.

Imperfections in Solids Edge Dislocation Fig. 4.3, Callister 7e.

Motion of Edge Dislocation • Dislocation motion requires the successive bumping of a half plane of atoms (from left to right here). • Bonds across the slipping planes are broken and remade in succession. Atomic view of edge dislocation motion from left to right as a crystal is sheared. (Courtesy P.M. Anderson)

Imperfections in Solids Screw Dislocation Screw Dislocation b Dislocation line Burgers vector b (b) (a) Adapted from Fig. 4.4, Callister 7e.

Edge, Screw, and Mixed Dislocations Adapted from Fig. 4.5, Callister 7e.

(3) Surface defects (area defects) grain boundaries and material surface The grain boundaries is a narrow zone where the atoms are not properly spaced

Grain boundaries are: Boundaries between crystal Produced by the solidification process (e.g.) Have a change in crystal orientation across them Impede dislocation motion.

Imperfections in Solids Dislocations are visible in electron micrographs Adapted from Fig. 4.6, Callister 7e.

Dislocations & Crystal Structures • Structure: close-packed planes & directions are preferred. view onto two close-packed planes. close-packed directions close-packed plane (bottom) close-packed plane (top) • Comparison among crystal structures: (more slip system: more ductile) FCC: many close-packed planes/directions; HCP: only one plane, 3 directions; • Specimens that were tensile tested. Mg (HCP) tensile direction Al (FCC)

Microscopic Examination Crystallites (grains) and grain boundaries. Vary considerably in size. Can be quite large ex: Large single crystal of quartz or diamond or Si ex: Aluminum light post or garbage can - see the individual grains Crystallites (grains) can be quite small (mm or less) – necessary to observe with a microscope.

Optical Microscopy • Useful up to 2000X magnification. • Polishing removes surface features (e.g., scratches) • Etching changes reflectance, depending on crystal orientation. 0.75mm crystallographic planes Adapted from Fig. 4.13(b) and (c), Callister 7e. (Fig. 4.13(c) is courtesy of J.E. Burke, General Electric Co. Micrograph of brass (a Cu-Zn alloy)

Optical Microscopy Grain boundaries... Fe-Cr alloy N = 2 n -1 • are imperfections, • are more susceptible to etching, • may be revealed as dark lines, • change in crystal orientation across boundary. Fe-Cr alloy (b) grain boundary surface groove polished surface (a) Adapted from Fig. 4.14(a) and (b), Callister 7e. (Fig. 4.14(b) is courtesy of L.C. Smith and C. Brady, the National Bureau of Standards, Washington, DC [now the National Institute of Standards and Technology, Gaithersburg, MD].) ASTM grain size number N = 2 n -1 number of grains/in2 at 100x magnification

Optical Microscopy Polarized light metallographic scopes often use polarized light to increase contrast Also used for transparent samples such as polymers

Microscopy Optical resolution ca. 10-7 m = 0.1 m = 100 nm For higher resolution need higher frequency X-Rays? Difficult to focus. Electrons wavelengths ca. 3 pm (0.003 nm) (Magnification - 1,000,000X) Atomic resolution possible Electron beam focused by magnetic lenses. Optical microscopy good to ca. wavelength of light Higher frequencies X-rays – good idea but difficult to focus Electrons - wavelength proportional to velocity with high voltage (high acceleration) get wavelengths ca. 3pm (0.003nm) (x1,000,000)

Scanning Tunneling Microscopy (STM) • Atoms can be arranged and imaged! Photos produced from the work of C.P. Lutz, Zeppenfeld, and D.M. Eigler. Reprinted with permission from International Business Machines Corporation, copyright 1995. Carbon monoxide molecules arranged on a platinum (111) surface. Iron atoms arranged on a copper (111) surface. These Kanji characters represent the word “atom”.

Summary • Point, Line, Area and volume defects exist in solids. • The number and type of defects can be varied and controlled (e.g., T controls vacancy conc.) • Defects affect material properties (e.g., grain boundaries control crystal slip). • Defects may be desirable or undesirable (e.g., dislocations may be good or bad, depending on whether plastic deformation is desirable or not.)