ISSUES TO ADDRESS... Structures of ceramic materials: How do they differ from those of metals? Point defects: How are they different from those in metals?

Slides:



Advertisements
Similar presentations
Chapter 12: Structures & Properties of Ceramics
Advertisements

ISSUES TO ADDRESS... How do atoms assemble into solid structures? How does the density of a material depend on its structure? When do material properties.
A Properties of Minerals Week 3: cleavage.
Chapter 7 Mechanical Properties of Solids.
Six-sided, pyramidal Quartz Crystals.
Chapter 12-1 CHAPTER 12: STRUCTURE AND PROPERTIES OF CERAMICS How do ceramics differ from metals ? Keramikos ~ burnt stuff –Heat treatment is necessary.
Lecture # 8 Structure and properties of ceramics Application and processing of ceramics Intended learning Outcomes: 1- Structure of ceramic materials.
Unit Cell of Crystal Structure
Explaining Vapor Pressure on the Molecular Level Some of the molecules on the surface of a liquid have enough energy to escape the attraction of the bulk.
Ionic Coordination and Silicate Structures Lecture 4.
L03C: Chapter 3 (Continued) Inorganic Compounds Reminder: Bonding ranges from ionic to covalent depending on relative electronegativity of constituents.
Metallic –Electropositive: give up electrons Ionic –Electronegative/Electropositive Colavent –Electronegative: want electrons –Shared electrons along bond.
Ceramics Term ceramics comes from the greek word keramikos – “burnt stuff” Ceramics are typically formed during high temperature heat treating – “Firing”
Covalent Network Solids. Tro, Chemistry: A Molecular Approach2 Carbon exhibits the most versatile bonding of all the elements diamond structure consists.
Chapter Chapter 12: Structures & Properties of Ceramics ISSUES TO ADDRESS... How do the crystal structures of ceramic materials differ from those.
Bonding in Solids Sovay, Jen and Miranda. Overview Physical properties of crystaline solids, such as melting point and hardness depend on the arrangements.
Structure of Solids Objectives
Chapter 3: Structures of Metals & Ceramics
Ceramics (세라믹) Associate Professor Su-Jin Kim
CHE 333 Class 23. Ceramics. Ceramic Structures Two Criteria for ceramic structures 1.Electrical Neutrality using ionic charge cation (positive charge)
Crystal Binding (Bonding) Overview & Survey of Bonding Types Continued
Chapter Outline: Ceramics
Ionic – Bonding and Crystal Structure. Valence and Lewis Bond Theory metals and non-metals exchange electrons eg. Na 2 O O [He]    2s 2 2p 4 Na [Ne]
Chapter 11: Liquids & Solids CHE 124: General Chemistry II Dr. Jerome Williams, Ph.D. Saint Leo University.
Chapter 3 Metallic and Ceramic Structures
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Section 10.5 CARBON & SILICON: NETWORK ATOMIC SOLIDS NETWORK SOLIDS: SOLIDS CONTAINING.
Chapter Chapter 12: Structures & Properties of Ceramics ISSUES TO ADDRESS... How do the crystal structures of ceramic materials differ from those.
Most common elements on earth are Si & O SiO 2 (silica) crystalline structures include quartz, crystobalite, & tridymite The strong Si-O bond leads to.
Ceramic Material Science © 2013 Su-Jin Kim, GNU Ceramics ( 세라믹 ) Associate Professor Su-Jin KimSu-Jin Kim School of Mechanical Engineering Gyeongsang National.
Ceramic Their Properties and Material Behavior
ENGR-45_Lec-26_Ceramic_Structure-Props.ppt 1 Bruce Mayer, PE Engineering-45: Materials of Engineering Bruce Mayer, PE Licensed.
Lecture 3 (9/13/2006) Crystal Chemistry Part 2: Bonding and Ionic Radii.
Properties of bonding Mrs. Kay.
Ceramics, Glass and Carbon.
Chapter 12- ISSUES TO ADDRESS... Structures of ceramic materials: How do they differ from that of metals? 1 Point defects: How are they different from.
1 Prof C. H. XU School of Materials Science and Engineering Henan University of Science and Technology Chapter 4: Matrix: Ceramics Subject: Composite Materials.
Ceramics and Glasses Chapter 14. History Ceramics were some of the earliest of mankind’s structural materials Pots Bricks Low Tech High Tech.
1 Solids. 2 Structures of Solids Crystalline vs. Amorphous Crystalline solid: well-ordered, definite arrangements of molecules, atoms or ions. –Most solids.
Chapter Lecture 23 Structures and Properties of Ceramics ME 330 Engineering Materials Crystal structures Defects in Ceramics Mechanical properties.
© 2015 Pearson Education, Inc. Chapter 13 Lecture presentation Add image of chapter 13 cover page (pg. 1 of 28) here Phase Diagrams and Crystalline Solids.
Chapter 12: Ceramics Materials - Structures and Properties
CERAMIC STRUCTURE S. CRYSTAL STRUCTURES AX-Type A m X p -Type A m B n X p -Type.
GROUP MEMBERS ABDUL MUHAIMIN BIN ABDUL HAKIM AFIQ ARIF AMINUDDIN JAFRY AHMAD ADLI MOHAMAD HANAFI AZRAAI HAKIMI AHMAD TAMIZI
Structure, Mechanical properties and its applications.
Chapter 12-7 Frenkel Defect -- a cation is out of place. Shottky Defect -- a paired set of cation and anion vacancies. Equilibrium concentration of defects.
Chemical Bonding 1. Types of Chemical Bonding IonicCovalentMetallic 2.
Materials Science Metals and alloys.
Chapter 3 -1 ISSUES TO ADDRESS... How do atoms assemble into solid structures? How does the density of a material depend on its structure? When do material.
Ceramic Crystal Structures. Interstitial sites = small holes between the lattice atoms where smaller atoms may be placed. The smaller atoms should be.
Chapter 111 Copyright © by Houghton Mifflin Company. All rights reserved. Crystalline Solids; Crystal Lattices and Unit Cells Solids can be crystalline.
MASE 542/Chem 442 Ceramics and Glasses.
Materials Engineering
Chapter 12: Structures & Properties of Ceramics
Crystal Structure and Crystallography of Materials
Chapter 12: Structures & Properties of Ceramics
CHAPTER 12: STRUCTURE AND PROPERTIES OF CERAMICS
Lecture on Minerals
CHAPTER 12 & 13: CERAMICS Ceramic materials are inorganic nonmetallic materials which consist of metallic and nonmetallic elements bonded primarily by.
Chapter 10: Liquids and Solids
Ceramic introduction.
Chapter 3: Solid State Chemistry Week 7
Chapter 3: Solid State Chemistry
Intermolecular forces
Unit 1: Structure and Properties of Matter
Ch. 6 Bonding 6.3 Ionic Bonding.
EME 201 Materials Science Ceramics.
Engineering Materials
Intermolecular Forces and
The Solid-State Structure of Metals and Ionic Compounds
Presentation transcript:

ISSUES TO ADDRESS... Structures of ceramic materials: How do they differ from those of metals? Point defects: How are they different from those in metals? Impurities: How are they accommodated in the lattice and how do they affect properties? Mechanical Properties: What special provisions/tests are made for ceramic materials? Chapter 12: Ceramics Materials - Structures and Properties

Bonding: -- Mostly ionic, some covalent. -- % ionic character increases with difference in electronegativity. Large vs small ionic bond character: Ceramic Bonding SiC: small CaF 2 : large

Ionic Bonding & Structure 1. Size - Stable structures: --maximize the # of nearest oppositely charged neighbors unstable Charge Neutrality: --Net charge in the structure should be zero. SiO 2, MgO, SiC, Al 2 O stable CaF 2 : Ca 2+ cation F - F - anions +

Coordination # increases with Coordination # and Ionic Radii 2 r cation r anion Coord # < linear triangular TDTD OHOH cubic ZnS (zincblende) NaCl (sodium chloride) CsCl (cesium chloride) r cation r anion Issue: How many anions can you arrange around a cation?

Site Selection II 2.Stoichiometry –If all of one type of site is full the remainder have to go into other types of sites. Ex: FCC unit cell has 4 O H and 8 T D sites. If for a specific ceramic each unit cell has 6 cations and the cations prefer O H sites 4 in O H 2 in T D

Site Selection III 3.Bond Hybridization – significant covalent bonding –the hybrid orbitals can have impact if significant covalent bond character present –For example in SiC X Si = 1.8 and X C = 2.5 ca. 89% covalent bonding both Si and C prefer sp 3 hybridization Therefore in SiC get T D sites

On the basis of ionic radii, what crystal structure would you predict for FeO? Answer: based on this ratio, --coord # = 6 --structure = NaCl Example: Predicting Structure of FeO Ionic radius (nm) Cation Anion Al 3+ Fe Ca 2+ O 2- Cl - F -

Rock Salt Structure Same concepts can be applied to ionic solids in general. Example: NaCl (rock salt) structure r Na = nm r Na /r Cl =  cations prefer O H sites r Cl = nm

MgO and FeO MgO and FeO also have the NaCl structure O 2- r O = nm Mg 2+ r Mg = nm r Mg /r O =  cations prefer O H sites So each oxygen has 6 neighboring Mg 2+

AX Crystal Structures AX–Type Crystal Structures include NaCl, CsCl, and zinc blende Cesium Chloride structure:  cubic sites preferred So each Cs + has 8 neighboring Cl -

AX Crystal Structures So each Zn 2+ has 4 neighboring S 2- Zinc Blende structure Size arguments predict Zn 2+ in O H sites, In observed structure Zn 2+ in T D sites Why is Zn 2+ in T D sites? –%ionic approx. 18% –bonding hybridization of zinc favors T D sites Ex: ZnO, ZnS, SiC

AX 2 Crystal Structures Fluorite structure Calcium Fluorite (CaF 2 ) cations in cubic sites UO 2, ThO 2, ZrO 2, CeO 2 antifluorite structure – cations and anions reversed

ABX 3 Crystal Structures Perovskite Ex: complex oxide BaTiO 3

Silicate Ceramics Most common elements on earth are Si & O SiO 2 (silica) structures are quartz, crystobalite, & tridymite The strong Si-O bond leads to a strong, high melting material (1710ºC) Si 4+ O 2- crystobalite

Amorphous Silica Silica gels - amorphous SiO 2 –Si 4+ and O 2- not in well- ordered lattice –Charge balanced by H + (to form OH - ) at “dangling” bonds –SiO 2 is quite stable, therefore un-reactive to makes good catalyst support

Silica Glass Dense form of amorphous silica –Charge imbalance corrected with “counter cations” such as Na + –Borosilicate glass is the pyrex glass used in labs better temperature stability & less brittle than sodium glass Si, B - Network former Other Cations - Network modifier

–Combine SiO 4 4- tetrahedra by having them share corners, edges, or faces –Cations such as Ca 2+, Mg 2+, & Al 3+ act to neutralize & provide ionic bonding Silicate elements Mg 2 SiO 4 Ca 2 MgSi 2 O 7

Layered Silicates Layered silicates (clay silicates) –SiO 4 tetrahedra connected together to form 2-D plane (Si 2 O 5 ) 2- So need cations to balance charge =

Kaolinite clay alternates (Si 2 O 5 ) 2- layer with Al 2 (OH) 4 2+ layer Layered Silicates Note: these sheets loosely bound by van der Waal’s forces

Carbon Forms Carbon black Diamond –tetrahedral carbon hard – no good slip planes brittle – can cut it –large diamonds – jewelry –small diamonds often man made - used for cutting tools and polishing –diamond films hard surface coat – tools, medical devices, etc.

Carbon Forms - Graphite layer structure – aromatic layers –weak van der Waal’s forces between layers –planes slide easily, good lubricant

Carbon Forms – Fullerenes and Nanotubes Fullerenes or carbon nanotubes –wrap the graphite sheet by curving into ball or tube –Buckminister fullerenes Like a soccer ball C 60 - also C 70 + others

Frenkel Defect -- a cation is out of place. Shottky Defect -- a paired set of cation and anion vacancies. Defects in Ceramic Structures Shottky Defect: Frenkel Defect

Impurities must also satisfy charge balance = Electroneutrality Ex: NaCl Substitutional cation impurity Impurities Na + Cl - initial geometryCa 2+ impurityresulting geometry Ca 2+ Na + + Ca 2+ cation vacancy Substitutional anion impurity initial geometry O 2- impurity O 2- Cl - anion vacancy Cl - resulting geometry

Ceramic Phase Diagrams

Ternary phase diagram 45% SiO2 34% Al2O3

General properties of ceramics Brittle (very low fracture toughness) Better strength under compressive Flexural strength is the rupture strength achieved from bending test Creep occurs at higher temperature than metal (compressive) Almost good hardness (used as abrasive materials) A little plastic deformation may be observed in crystalline ceramics; slip plane Non-crystalline ceramics; viscous flow Porosity in ceramics decreases the modulus of elasticity and strength High chemical durability

Mechanical Properties We know that ceramics are more brittle than metals. Why? Consider method of deformation –slippage along slip planes in ionic solids this slippage is very difficult too much energy needed to move one anion past another anion Higher strength under compressive stress –Generally utilized when load conditions are compressive

Load and crack origin

Room T behavior is usually elastic, with brittle failure. 3-Point Bend Testing often used. --tensile tests are difficult for brittle materials. Measuring Elastic Modulus F L/2 δ = midpoint deflection cross section R b d rect.circ. Determine elastic modulus according to: F x linear-elastic behavior  F  slope = E = F  L 3 4bd 3 = F  L 3 12  R 4 rect. cross section circ. cross section

3-point bend test to measure room T strength. Measuring Strength F L/2 δ = midpoint deflection cross section R b d rect.circ. location of max tension Flexural strength: Typ. values: Rect.  fs  3F f L 2bd 2  F f L R3R3 Si nitride Si carbide Al oxide glass (soda) Material  fs (MPa) E(GPa) x F FfFf  fs  Cir.

Flexural strength and Modulus of elasticity of Ceramics

Stress-strain behavior / Porosity

Viscosity

Measuring Elevated T Response  time Elevated Temperature Tensile Test (T > 0.4 T m ). creep test   slope =  ss = steady-state creep rate. x

Ceramic materials have covalent & ionic bonding. Structures are based on: -- charge neutrality -- maximizing # of nearest oppositely charged neighbors. Structures may be predicted based on: -- ratio of the cation and anion radii. Defects -- must preserve charge neutrality -- have a concentration that varies exponentially w/T. Room T mechanical response is elastic, but fracture is brittle, with negligible deformation. Elevated T creep properties are generally superior to those of metals (and polymers). Summary