CHAPTER 12 STRUCTURE AND PROPERTIES OF CERAMICS How

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CHAPTER 12: STRUCTURE AND PROPERTIES OF CERAMICS How do ceramics differ from metals ?

CHAPTER 12: STRUCTURE AND PROPERTIES OF CERAMICS How do ceramics differ from metals ? • Keramikos ~ burnt stuff – Heat treatment is necessary • Usually a compound between a metal and a non-metal – Bonding displays a mixture of ionic and covalent character • Generally hard and brittle, have high melting temperature – Why ? • Generally thermally and electrically insulating • Can be opaque, semi-transparent or transparent • Traditional ceramics ~ based on clay (china, porcelain, bricks, tiles) and glasses • Hi-tech ceramics => electronic, communication, computer hardware, aerospace industries Chapter 12 - 1

CERAMIC BONDING • Bonding: --Mostly ionic, some covalent. --% ionic character increases with difference

CERAMIC BONDING • Bonding: --Mostly ionic, some covalent. --% ionic character increases with difference in electronegativity. What is electronegativity ? • Large vs small ionic bond character: Adapted from Fig. 2. 7, Callister 6 e. (Fig. 2. 7 is adapted from Linus Pauling, The Nature of the Chemical Bond, 3 rd edition, Copyright 1939 and 1940, 3 rd edition. Copyright 1960 by Cornell University. Chapter 12 - 2

Crystal Structure of Ionicly Bonded Ceramics • Crystal structure is defined by 2 criterions

Crystal Structure of Ionicly Bonded Ceramics • Crystal structure is defined by 2 criterions 1. Magnitude of the electrical charge on each ion. Charge balance dictates chemical formula (Ca 2+ and F- form Ca. F 2). 2. Relative sizes of the cations and anions. Cations wants maximum possible number of anion nearest neighbors and vice-versa. • Stable ceramic crystal structures require anions surrounding a cation to be all in contact with that cation. • For a specific coordination number there is a critical or minimum cation/anion radius ratio r. C/r. A for which this contact can be maintained. Pure geometrical consideration… Chapter 12 -

IONIC BONDING & CRYSTAL STRUCTURE 1. Charge Neutrality: --Net charge in the crystal structure

IONIC BONDING & CRYSTAL STRUCTURE 1. Charge Neutrality: --Net charge in the crystal structure should be zero. --General form: 2. Maximize the # of nearest oppositely charged neighbors --stable structures: Adapted from Fig. 12. 1, Callister 6 e. Chapter 12 - 3

COORDINATION # AND IONIC RADII • Coordination # increases with Adapted from Fig. 12.

COORDINATION # AND IONIC RADII • Coordination # increases with Adapted from Fig. 12. 4, Callister 6 e. Adapted from Fig. 12. 2, Callister 6 e. Adapted from Table 12. 2, Callister 6 e. Adapted from Fig. 12. 3, Callister 6 e. Chapter 12 - 4

EX 1: PREDICTING STRUCTURE OF Fe. O • On the basis of ionic radii,

EX 1: PREDICTING STRUCTURE OF Fe. O • On the basis of ionic radii, what crystal structure would you predict for Fe. O? • Answer: based on this ratio, --coord # = 6 --structure = Na. Cl (rocksalt) Data from Table 12. 3, Callister 6 e. Two penetrating FCC units; other examples are Mg. O, Mn. S, Li. F…. Chapter 12 - 5

EX 2: Am. Xp STRUCTURES • Consider Ca. F 2 : • Based on

EX 2: Am. Xp STRUCTURES • Consider Ca. F 2 : • Based on this ratio, coord # = 8 and structure = Cs. Cl. • Result: Cs. Cl structure w/only half the cation sites occupied. • Only half the cation sites are occupied since #Ca 2+ ions = 1/2 # F- ions. Adapted from Fig. 12. 5, Callister 6 e. Empty Chapter 12 - 6

EX 3: Zn. S - Zinc. Blende Structure • Zn 2+ + S 2

EX 3: Zn. S - Zinc. Blende Structure • Zn 2+ + S 2 • What is the CN ? • What should be the structure ? Chapter 12 -

Ceramic Density Computations n’: number of formula units in unit cell (all ions that

Ceramic Density Computations n’: number of formula units in unit cell (all ions that are included in the chemical formula of the compound = formula unit) ∑AC: sum of atomic weights of cations in the formula unit ∑AA: sum of atomic weights of anions in the formula unit VC: volume of the unit cell NA: Avogadro’s number, 6. 023 X 1023 (formula units)/mol Chapter 12 -

EX 4: Na. Cl density a n’ = 4 in FCC lattice ∑AC= ANa=

EX 4: Na. Cl density a n’ = 4 in FCC lattice ∑AC= ANa= 22. 99 g/mol ∑AA= ACl= 35. 45 g/mol VC= a 3=[2 (r. Na + r. Cl)]3 Chapter 12 -

Silicate Ceramics • Composed mainly of silicon and oxygen, the two most abundant elements

Silicate Ceramics • Composed mainly of silicon and oxygen, the two most abundant elements in earth’s crust (rocks, soils, clays and sand- Si. O 2 silica) • Basic building block: Si. O 44 - tetrahedron: – Si-O bonding is largely covalent, but overall Si. O 4 block has charge of – 4 – Various silicate structures – different ways to arrange Si. O 44 - blocks Chapter 12 -

EX: Crystalline form of Si. O 2 Three polymorphs of Si. O 2 :

EX: Crystalline form of Si. O 2 Three polymorphs of Si. O 2 : Quartz, Crystobalite, Tridymite Not a very closed pack structure low density ~ 2. 65 g/cm 3 3 D networks of Si. O 44 - tetrahedra Each O atom is shared by an adjacent tetrahedron Chapter 12 -

Window Glass • Still Si. O 44 - tetrahedra are the basic building block.

Window Glass • Still Si. O 44 - tetrahedra are the basic building block. • Most common window glasses are produced by adding other oxides (e. g. Ca. O, Na 2 O, B 2 O 3, etc) whose cations are incorporated within Si. O 4 network. • These cations break the tetrahedral network and glasses melt at lower temperature than pure amorphous Si. O 2. • A lower melting point makes it easy to form glass to make, for instance, bottles. • Some other oxides (Ti. O 2, Al 2 O 3) substitute for silicon and become part of the network Chapter 12 -

Carbon/Diamond/Fullerenes/ Nanotubes Read => p 399 -403 • http: //www. nasa. gov/Groups/Sci. Tech/nano/ Chapter

Carbon/Diamond/Fullerenes/ Nanotubes Read => p 399 -403 • http: //www. nasa. gov/Groups/Sci. Tech/nano/ Chapter 12 -

DEFECTS IN CERAMIC STRUCTURES Point defects in ionic crystals are charged. The Coulombic forces

DEFECTS IN CERAMIC STRUCTURES Point defects in ionic crystals are charged. The Coulombic forces that are generated due to defects are very large and any charge imbalance has a strong tendency to balance itself, electroneutrality. To maintain charge neutrality several point defects can be created at the same time: • Frenkel Defect --a cation is out of place. • Shottky Defect --a paired set of cation and anion vacancies. A c Anion interstitials are unlikely, why ? Shottky Defect: Charge neutrality of the crystal is maintained Frenkel Defect - QD / k. T • Equilibrium concentration of defects ~ exp Adapted from Fig. 13. 20, Callister 5 e. (Fig. 13. 20 is from W. G. Moffatt, G. W. Pearsall, and J. Wulff, The Structure and Properties Chapter 12 - of Materials , Vol. 1, Structure, John Wiley and Sons, Inc. , p. 78. ) See Fig. 12. 21, Callister 6 e.

IMPURITIES • Impurities must also satisfy charge balance • Ex: Na. Cl • Substitutional

IMPURITIES • Impurities must also satisfy charge balance • Ex: Na. Cl • Substitutional cation impurity • Substitutional anion impurity Chapter 12 - 8

Stoichiometry • A state for ionic solids where there is an exact ratio of

Stoichiometry • A state for ionic solids where there is an exact ratio of anions to cations defined by the chemical formula unit. – Na. Cl => anion to cation ratio is exactly 1: 1 – Ca 2 F => 1: 2, otherwise it is called nonstoichiometry – Fe. O => wüstite, Fe 2+ or Fe 3+ may exist depending on temperature and O partial pressure. For any Fe 3+, there has to be an extra vacancy so that the charge neutrality is preserved… But then, Fe 1 -x. O for x < 1… Chapter 12 -

Impurities in Ceramics • Impurity atoms can exist as either substitutional or as interstitial

Impurities in Ceramics • Impurity atoms can exist as either substitutional or as interstitial solid solutions in ceramics – Substitutional ions substitute for ions of like type (anion to anion, cation to cation) – Interstitial ions are small compared to host structure – formation of anion interstitials is unlikely (why? ) – Solubility is higher if ion radii and charges match closely – Incorporation of ion with different charge state requires compensation by point defects to preserve charge neutrality Chapter 12 -

Ceramic Phase Diagrams • Al 2 O 3 -Cr 2 O 3 system; often

Ceramic Phase Diagrams • Al 2 O 3 -Cr 2 O 3 system; often they share a common element in their formula, in many cases it is OXYGEN. – Solubility is achieved by Al 3+ substituting Cr 3+ – Binary Isomorphous system Chapter 12 -

Ceramic Phase Diagrams • Al 2 O 3 -Si. O 2 system Chapter 12

Ceramic Phase Diagrams • Al 2 O 3 -Si. O 2 system Chapter 12 -

MEASURING ELASTIC MODULUS • Room T behavior is usually elastic, with brittle failure. •

MEASURING ELASTIC MODULUS • Room T behavior is usually elastic, with brittle failure. • 3 -Point Bend Testing often used. --tensile tests are difficult for brittle materials. Adapted from Fig. 12. 29, Callister 6 e. • Determine elastic modulus according to: Chapter 12 - 9

Mechanical Properties of Ceramics • Ceramics are very brittle. (Fracture Toughness) – For brittle

Mechanical Properties of Ceramics • Ceramics are very brittle. (Fracture Toughness) – For brittle materials fracture stress concentrators are very important. (Chapter 8: measured fracture strengths are significantly smaller than theoretical predictions for perfect materials due to the stress risers) – Fracture strength of ceramic may be greatly enhanced by creating compressive stresses in the surface region (similar to shot peening, case hardening in metals, chapter 8) • Compressive strength is typically ten times the tensile strength. This makes ceramics good structural materials under compression (e. g. , cement, bricks in building apartments, stone blocks in the pyramids). • Generally, tensile test is not used – Hard to machine, grippers may break the piece, fail after 0. 1% strain. – Size is important due impact of # of cracks on strength, why ? Chapter 12 -

MEASURING STRENGTH • 3 -point bend test to measure room T strength. Adapted from

MEASURING STRENGTH • 3 -point bend test to measure room T strength. Adapted from Fig. 12. 29, Callister 6 e. • Flexural strength: • Typ. values: Si nitride 700 -1000 300 Si carbide 550 -860 430 Al oxide 275 -550 390 glass (soda) 69 69 Data from Table 12. 5, Callister 6 e. Chapter 12 - 10

MEASURING ELEVATED T RESPONSE • Elevated Temperature Tensile Test (T > 0. 4 Tmelt).

MEASURING ELEVATED T RESPONSE • Elevated Temperature Tensile Test (T > 0. 4 Tmelt). • Generally, . . . Chapter 12 - 11

SUMMARY • Ceramic materials have mostly covalent & some ionic bonding. • Structures are

SUMMARY • Ceramic materials have mostly covalent & some 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 brittle, with negligible ductility. Elevated T creep properties are generally superior to those of metals (and polymers). Chapter 12 - 12

ANNOUNCEMENTS Reading: Chapter 12 Core Problems: Self-help Problems: Chapter 12 - 0

ANNOUNCEMENTS Reading: Chapter 12 Core Problems: Self-help Problems: Chapter 12 - 0