PDT 153 Materials Structure And Properties

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Presentation transcript:

PDT 153 Materials Structure And Properties Chapter 5: Imperfection In Solids Prepared by: Dr. Tan Soo Jin

Metallic Solid Solutions A metal alloy, or simply an alloy, is a mixture of two or more metals or a metal and nonmetal. Simplest type of alloy is solid solution. Solid solution is a solid that consists of two or more elements atomically dispersed in a single-phase structure. Two types of solid solution: i. Substitutional Ii. Interstitial

Substitutional Solid Solutions Solute atoms substitute for parent solvent atom in a crystal lattice. The structure remains unchanged. Lattice might get slightly distorted due to change in diameter of the atoms. Solute percentage in solvent can vary fraction of a percentage to 100%. Solvent atoms Solute atoms

Substitutional Solid Solutions (Cont..) The solubility of solids is greater if (Hume-Rothery rules) The diameter of atoms not differ by more than 15% Crystal structures are similar. No much difference in electronegativity (else compounds will be formed). Have same valence.

Interstitial Solid Solution Solute atoms fit in between the voids (interstices) of solvent atoms. Solvent atoms should be much larger than solute atoms for interstitial solid solution. Example:- between 1185K and 1667K, interstitial solid solution of carbon in γ iron (FCC) is formed. A maximum of 2.8% of carbon can dissolve interstitially in iron. Carbon atoms r = 0.077nm Iron atoms r = 0.124nm

Crystalline Imperfections No crystal is perfect. Imperfections affect mechanical properties, chemical properties and electrical properties. Imperfections can be classified as Zero dimension point defects. One dimension / line defects (dislocations). Two dimension defects. Three dimension defects (cracks).

Point Defects – Vacancy Vacancy is formed due to a missing atom. Vacancy is formed (one in 10000 atoms) during crystallization or mobility of atoms. Energy of formation is 1 ev. Mobility of vacancy results in cluster of vacancies. Also caused due to plastic defor- -mation, rapid cooling or particle bombardment.

Point Defects - Interstitially Atom in a crystal, sometimes, occupies interstitial site. This does not occur naturally. Can be induced by irradiation. This defects caused structural distortion.

Point Defects in Ionic Crystals Complex as electric neutrality has to be maintained. If two appositely charged particles are missing, cation-anion divacancy is created. This is scohttky imperfection. Frenkel imperfection is created when cation moves to interstitial site. Impurity atoms are also considered as point defects.

Line Defects – (Dislocations) Lattice distortions are centered around a line. Formed during Solidification Permanent Deformation Vacancy condensation Different types of line defects are Edge dislocation Screw dislocation Mixed dislocation

Line Defects - Edge Dislocation Created by insertion of extra half planes of atoms. Positive edge dislocation Negative edge dislocation Burgers vector Shows displa- cement of atoms (slip). Burgers vector

Line Defects - Screw Dislocation Created due to shear stresses applied to regions of a perfect crystal separated by cutting plane. Distortion of lattice in form of a spiral ramp. Burgers vector is parallel to dislocation line.

Dislocation structure of iron deformed Line Defects - Mixed Dislocation Most crystal have components of both edge and screw dislocation. Dislocation, since have irregular atomic arrangement will appear as dark lines when observed in electron microscope. Dislocation structure of iron deformed 14% at –1950C

Planar Defects Include external surface, grain boundaries, twins, low/high angle boundaries, twists and stacking faults Free surface is also a defect : Bonded to atoms on only one side and hence has higher state of energy Highly reactive Nanomaterials have small clusters of atoms and hence are highly reactive.

Grain Boundaries Grain boundaries separate grains. Formed due to simultaneously growing crystals meeting each other. Width = 2-5 atomic diameters. Some atoms in grain boundaries have higher energy. Restrict plastic flow and prevent dislocation movement 3D view of grains Grain Boundaries In 1018 steel

Twin Boundaries Twin: A region in which mirror image of structure exists across a boundary. Formed during plastic deformation and recrystallization. Strengthens the metal. Twin Twin Plane

Other Planar Defects Small angle tilt boundary: Array of edge dislocations tilts two regions of a crystal by < 100 Stacking faults: Piling up faults during recrystallization due to collapsing. Example: ABCABAACBABC FCC fault Volume defects: Cluster of point defects join to form 3-D void.

Single Crystal To observe grain boundaries, the metal sample must be first mounted for easy handling Then the sample should be ground and polished with different grades of abrasive paper and abrasive solution. The surface is then etched chemically. Tiny groves are produced at grain boundaries. Groves do not intensely reflect light. Hence observed by optical microscope.

Atomic Vibration Every atom in a solid material is vibrating very rapidly about its lattice position within the crystal. These atomic vibration thought as imperfections or defects. Many properties and processes in solids are manifestations of this vibrational atomic motion. For example, melting occurs when the vibrations are vigorous enough to rupture large numbers of atomic bonds.

Effect of Etching Etched Brass 200 X Unetched Brass 200 X Etched Steel

Grain Size Affects the mechanical properties of the material The smaller the grain size, more are the grain boundaries. More grain boundaries means higher resistance to slip (plastic deformation occurs due to slip). More grains means more uniform the mechanical properties are.

N = 2 n-1 Measuring Grain Size ASTM grain size number ‘n’ is a measure of grain size. N = 2 n-1 n < 3 – Coarse grained 4 < n < 6 – Medium grained 7 < n < 9 – Fine grained N > 10 – ultrafine grained N = Number of grains per square 2.54 x 10-2 m of a polished and etched specimen at 100 x. n = ASTM grain size number. 200 X 1018 cold rolled steel, n=10 1045 cold rolled steel, n=8

Scanning Electron Microscope Electron source generates electrons. Electrons hit the surface and secondary electrons are produced. The secondary electrons are collected to produce the signal. The signal is used to produce the image. SEM of fractured metal end

Transmission Electron Microscope Electron produced by heated tungsten filament. Accelerated by high voltage (75 - 120 KV) Electron beam passes through very thin specimen. Difference in atomic arrangement change directions of electrons. Beam is enlarged and focused on fluorescent screen. Collagen Fibrils of ligament as seen in TEM

Transmission Electron Microscope (Cont..) TEM needs complex sample preparation Very thin specimen needed ( several hundred nanometers) High resolution TEM (HRTEM) allows resolution of 0.1 nm. 2-D projections of a crystal with accompanying defects can be observed Low angle boundary As seen In HTREM

Scanning Probe Microscopy Scanning Tunneling Microscope (STM) and Atomic Force Microscope (AFM). Sub-nanometer magnification. Atomic scale topographic map of surface. STM uses extremely sharp tip. Tungsten, nickel, platinum - iridium or carbon nanotubes are used for tips.

Scanning Tunneling Microscope Tip placed one atom diameter from surface. Voltage applied across tip and surface. Electrons tunnel the gap and produce current. Current produced is proportional to change in gap. Can be used only for conductive materials. Constant height and current modes Surface of platinum with defects

Atomic Force Microscope Similar to STM but tip attached to cantilever beam. When tip interacts with surface, van der waals forces deflect the beam. Deflection detected by laser and photodetector. Non-conductive materials can be scanned. Used in DNA research and polymer coating technique.